Asymmetry of the Electrostatic Environment as the Origin of the Symmetry Breaking Effect of the Nitrate Ion in Aqueous Solution

Elucidating the mechanism of how vibrational modes are affected by intermolecular interactions is important for a better understanding of the nature of the former as probes of the latter. Here, such an analysis is carried out for the N-O stretching modes of the nitrate ion interacting with water, with an emphasis on the symmetry breaking effect. On the basis of theoretical calculations on the structural, vibrational, and electrostatic properties of molecular clusters and spectral simulations for an aqueous solution, a transparent view is demonstrated on the mechanism that modulations of spatially local electrostatic environment give rise to structural and spectroscopic symmetry breaking effect. The electrostatic interaction model constructed here is a seven-parameter model; the use of a single electrostatic parameter, such as the electric field on a single atomic site, is found to be insufficient for quantitative evaluation. It is also shown that the frequency modulations of the N-O stretching modes in aqueous solution occur on a time scale much shorter than 0.1 ps.

Measurement of Direct-Photon Cross Section and Double-Helicity Asymmetry at sqrt[s]=510 GeV in p[over →]+p[over →] Collisions

We present measurements of the cross section and double-helicity asymmetry A_{LL} of direct-photon production in p[over →]+p[over →] collisions at sqrt[s]=510  GeV. The measurements have been performed at midrapidity (|η|<0.25) with the PHENIX detector at the Relativistic Heavy Ion Collider. At relativistic energies, direct photons are dominantly produced from the initial quark-gluon hard scattering and do not interact via the strong force at leading order. Therefore, at sqrt[s]=510  GeV, where leading-order-effects dominate, these measurements provide clean and direct access to the gluon helicity in the polarized proton in the gluon-momentum-fraction range 0.02<x<0.08, with direct sensitivity to the sign of the gluon contribution.

Substituent Effect and Its Halogen-Atom Dependence of Halogen Bonding Viewed through Electron Density Changes

Elucidating how the halogen-bonding ability and strength are controlled by the substituent effect and how this control depends on halogen atom will be essential for finely-tuned design of functionally important molecules. Here, this problem is tackled by analyzing the electron density differences/changes for variously substituted halobenzenes. It is shown that the anisotropy of the electron distribution around the halogen atom, which is an important factor for halogen-bonding ability, is not much affected by the substituent effect and rather simply depends on the halogen atom, while the partial charge on the halogen atom, which is related to the bond dipole of the C-X bond, is significantly modulated by the substituent effect and gives rise to enhancement of the electrostatic potential on the line extended from the C-X bond. The properties related to the polarization effect are also discussed.

Nature of hydrogen-bond-enhanced halogen bonding viewed through electron density changes

Elucidating the mechanism of how we can achieve fine tuning of intermolecular interaction strength will be helpful for designing functionally important molecules. In the present study, a theoretical analysis is conducted, by examining the electron density changes, for two halogen-bonding iodinated systems whose halogen-bond strengths have been considered to be enhanced by the presence of a hydrogen-bond donating group (termed hydrogen-bond-enhanced halogen bonding). It is shown that, contrary to the expectation obtained from the enhancement of electrostatic potential along the line extended from the C-I bond, the anisotropy of electron distribution on the iodine atom remains nearly the same. This means that the hydrogen bond and halogen bond contribute almost independently and additively to the enhancement of electrostatic potential, indicating the nature of this enhancement and, in a more general sense, the relationship between the strength and the extent of directionality of halogen bonding.

Infrared Spectra and Hydrogen-Bond Configurations of Water Molecules at the Interface of Water-Insoluble Polymers under Humidified Conditions

Elucidating the state of interfacial water, especially the hydrogen-bond configurations, is considered to be key for a better understanding of the functions of polymers that are exhibited in the presence of water. Here, an analysis in this direction is conducted for two water-insoluble biocompatible polymers, poly(2-methoxyethyl acrylate) and cyclic(poly(2-methoxyethyl acrylate)), and a non-biocompatible polymer, poly(n-butyl acrylate), by measuring their IR spectra under humidified conditions and by carrying out theoretical calculations on model complex systems. It is found that the OH stretching bands of water are decomposed into four components, and while the higher-frequency components (with peaks at ∼3610 and ∼3540 cm^-1) behave in parallel with the C═O and C-O-C stretching and CH deformation bands of the polymers, the lower-frequency components (with peaks at ∼3430 and ∼3260 cm^-1) become pronounced to a greater extent with increasing humidity. From the theoretical calculations, it is shown that the OH stretching frequency that is distributed from ∼3650 to ∼3200 cm^-1 is correlated to the hydrogen-bond configurations and is mainly controlled by the electric field that is sensed by the vibrating H atom. By combining these observed and calculated results, the configurations of water at the interface of the polymers are discussed.

Singular value decomposition analysis of the electron density changes occurring upon electrostatic polarization of water

In-depth elucidation of how molecules are electrically polarized would be one key factor for understanding the properties of those molecules under various thermodynamic and/or spatial conditions. Here this problem is tackled for the case of hydrogen-bonded water by conducting singular value decomposition of the electron density changes that occur upon electrostatic polarization. It is shown that all those electron density changes are approximately described as linear combinations of ten orthonormal basis “vectors”. One main component is the interatomic charge transfer through each OH bond, while some others are characterized as the atomic dipolar polarizations, meaning that both of these components are important for the electrostatic polarization of water. The interaction parameters that reasonably well reproduce the induced dipole moments are derived, which indicate the extent of mixing of the two components in electrostatic polarization.

The main features of the electron density changes that occur upon electrostatic polarization of water are elucidated by conducting singular value decomposition analysis of those changes.

Hidden Halogen-Bonding Ability of Fluorine Manifesting in the Hydrogen-Bond Configurations of Hydrogen Fluoride

Elucidating how the intermolecular interactions of a covalently bonded fluorine atom are similar to and different from those of the other halogen atoms will be helpful for a better unified understanding of them. In the present study, the case of hydrogen fluoride is theoretically studied from this viewpoint by using the techniques of electron density analysis, molecular dynamics of liquid, and others. It is shown that the extra-point model, which locates an additional charge site on the line extended from (not within) the covalent bond and has been adopted for halogen-bonding systems as a key to the generation of proper stability and directionality, works well also in this case. A significantly bent hydrogen-bond configuration, which is characteristic of the intermolecular interactions of hydrogen fluoride, is reasonably well reproduced, meaning that it is a manifestation of the latent halogen-bonding ability, which is hidden by the strongly electronegative nature.

Role of Intermolecular Charge Fluxes in the Hydrogen-Bond-Induced Frequency Shifts of the OH Stretching Mode of Water

The relation between the vibrational properties and the electrostatic situations of the vibrating functional group is useful to predict vibrational spectroscopic features based on, for example, classical molecular dynamics of liquids or biomolecular systems, but to pursue its generality or the extent of applicability, it is required to understand the mechanisms giving rise to it. Here such an analysis is carried out for the OH stretching mode of water. By examining the correlations among various (structural, vibrational, and electrostatic) properties and by analyzing the spatial characteristics of the behavior of electrons occurring upon the vibration, it is shown that the dependence of the vibrational frequency and the dipole derivative of the OH stretching mode on the electric field is not of purely electrostatic origin, and the delocalized electronic motions occurring with this mode, called intermolecular charge fluxes, related to both the dipole first and second derivatives play important roles.

Dissecting the electric quadrupolar and polarization effects operating in halogen bonding through electron density analysis with a focus on bromine

The form of the electron density change (or difference) is usable as a kind of fingerprint of the electronic structural origin or mechanism that gives rise to intermolecular interactions. Here, this method is applied to halogen-bonding brominated systems to dissect the electric quadrupolar effect (arising from the anisotropic distribution of the valence electrons and intrinsic to the s²p_x ²p_y ²p_z electronic configuration) and the polarization effect (induced by a partial negative charge of the halogen-bond accepting atom). It is shown that a suitable location of the "extra point" for placing a partial positive charge to represent the former is crucial and is clearly found from the electron density difference from the spherically isotropic Br^- ion, while the latter consists of the dipolar polarization of the Br atom and the delocalized polarization of the whole molecule. A practical way for application to molecular dynamics simulations, etc., to represent these two factors is discussed.

Vibrational Spectroscopic Map, Vibrational Spectroscopy, and Intermolecular Interaction

Vibrational spectroscopy is an essential tool in chemical analyses, biological assays, and studies of functional materials. Over the past decade, various coherent nonlinear vibrational spectroscopic techniques have been developed and enabled researchers to study time-correlations of the fluctuating frequencies that are directly related to solute-solvent dynamics, dynamical changes in molecular conformations and local electrostatic environments, chemical and biochemical reactions, protein structural dynamics and functions, characteristic processes of functional materials, and so on. In order to gain incisive and quantitative information on the local electrostatic environment, molecular conformation, protein structure and interprotein contacts, ligand binding kinetics, and electric and optical properties of functional materials, a variety of vibrational probes have been developed and site-specifically incorporated into molecular, biological, and material systems for time-resolved vibrational spectroscopic investigation. However, still, an all-encompassing theory that describes the vibrational solvatochromism, electrochromism, and dynamic fluctuation of vibrational frequencies has not been completely established mainly due to the intrinsic complexity of intermolecular interactions in condensed phases. In particular, the amount of data obtained from the linear and nonlinear vibrational spectroscopic experiments has been rapidly increasing, but the lack of a quantitative method to interpret these measurements has been one major obstacle in broadening the applications of these methods. Among various theoretical models, one of the most successful approaches is a semiempirical model generally referred to as the vibrational spectroscopic map that is based on a rigorous theory of intermolecular interactions. Recently, genetic algorithm, neural network, and machine learning approaches have been applied to the development of vibrational solvatochromism theory. In this review, we provide comprehensive descriptions of the theoretical foundation and various examples showing its extraordinary successes in the interpretations of experimental observations. In addition, a brief introduction to a newly created repository Web site (http://frequencymap.org) for vibrational spectroscopic maps is presented. We anticipate that a combination of the vibrational frequency map approach and state-of-the-art multidimensional vibrational spectroscopy will be one of the most fruitful ways to study the structure and dynamics of chemical, biological, and functional molecular systems in the future.

Erratum: Evolution of π^{0} Suppression in Au+Au Collisions from sqrt[s_{NN}]=39 to 200 GeV [Phys. Rev. Lett. 109, 152301 (2012)]

This corrects the article DOI: 10.1103/PhysRevLett.109.152301.

Hydrogen order at the surface of ice Ih revealed by vibrational spectroscopy

A combination of heterodyne-detected sum frequency generation spectroscopy and theoretical modeling elucidates that the surface of ice I_h at 100 K has hydrogen order with the OH group pointing upward to the air (“H-up” orientation).

Beam Energy and Centrality Dependence of Direct-Photon Emission from Ultrarelativistic Heavy-Ion Collisions

The PHENIX collaboration presents first measurements of low-momentum (0.4<p_{T}<3  GeV/c) direct-photon yields from Au+Au collisions at sqrt[s_{NN}]=39 and 62.4 GeV. For both beam energies the direct-photon yields are substantially enhanced with respect to expectations from prompt processes, similar to the yields observed in Au+Au collisions at sqrt[s_{NN}]=200. Analyzing the photon yield as a function of the experimental observable dN_{ch}/dη reveals that the low-momentum (>1  GeV/c) direct-photon yield dN_{γ}^{dir}/dη is a smooth function of dN_{ch}/dη and can be well described as proportional to (dN_{ch}/dη)^{α} with α≈1.25. This scaling behavior holds for a wide range of beam energies at the Relativistic Heavy Ion Collider and the Large Hadron Collider, for centrality selected samples, as well as for different A+A collision systems. At a given beam energy, the scaling also holds for high p_{T} (>5  GeV/c), but when results from different collision energies are compared, an additional sqrt[s_{NN}]-dependent multiplicative factor is needed to describe the integrated-direct-photon yield.

Correlation of the partial charge-transfer and covalent nature of halogen bonding with the THz and IR spectral changes

Changes in the spectral intensities in the THz region are good probes for the non-electrostatic aspect of halogen bonding.

Intermolecular charge fluxes and far-infrared spectral intensities of liquid formamide

Intermolecular charge fluxes induced by hydrogen-bond length modulations occurring upon molecular librations lead to intensity enhancement of the far-infrared spectrum.

Intermediate length-scale chirality related to the vibrational circular dichroism intensity enhancement upon fibril formation in a gelation process

The VCD intensity enhancement occurring upon fibril formation arises from the second out of the three hierarchical tiers of chirality.

Strategy for Modeling the Electrostatic Responses of the Spectroscopic Properties of Proteins

For better understanding and more efficient use of the spectroscopic probes (vibrational and NMR) of the local electrostatic situations inside proteins, appropriate modeling of the properties of those probes is essential. The present study is devoted to examining the strategy for constructing such models. A more well-founded derivation than the ones in previous studies is given in constructing the models. Theoretical analyses are conducted on two representative example cases related to proteins, i.e., the peptide group of the main chains and the CO and NO ligands to the Fe²⁺ ion of heme, with careful treatment of the behavior of electrons in the electrostatic responses and with verification of consistency with observable quantities. It is shown that, for the stretching frequencies and NMR chemical shifts, it is possible to construct reasonable electrostatic interaction models that encompass the situations of hydration and uniform electric field environment and thus are applicable also to the cases of nonuniform electrostatic situations, which are highly expected for inside of proteins.

Centrality-Dependent Modification of Jet-Production Rates in Deuteron-Gold Collisions at √[s(NN)]=200 GeV

Jet production rates are measured in p+p and d+Au collisions at sqrt[s_{NN}]=200  GeV recorded in 2008 with the PHENIX detector at the Relativistic Heavy Ion Collider. Jets are reconstructed using the R=0.3 anti-k_{t} algorithm from energy deposits in the electromagnetic calorimeter and charged tracks in multiwire proportional chambers, and the jet transverse momentum (p_{T}) spectra are corrected for the detector response. Spectra are reported for jets with 12<p_{T}<50  GeV/c, within a pseudorapidity acceptance of |η|<0.3. The nuclear-modification factor (R_{dAu}) values for 0%-100% d+Au events are found to be consistent with unity, constraining the role of initial state effects on jet production. However, the centrality-selected R_{dAu} values and central-to-peripheral ratios (R_{CP}) show large, p_{T}-dependent deviations from unity, challenging the conventional models that relate hard-process rates and soft-particle production in collisions involving nuclei.

Roles of the scalar and vector components of the solvation effects on the vibrational properties of hydrogen- or halogen-bond accepting stretching modes

Solvation-induced vibrational frequency shifts and infrared (IR) intensity changes of the hydrogen- or halogen-bond accepting stretching modes, especially their dependence on the angular position of the hydrogen- or halogen-bond donating molecule, are examined theoretically. Calculations are carried out for some modes of hydrogen- or halogen-bonding molecular complexes, including the S[double bond, length as m-dash]O stretch of dimethyl sulfoxide-(13)C2H2O, the C[triple bond, length as m-dash]N stretch of acetonitrileH2O, and the amide I' mode of the N-methylacetamide-d1BrNC 1 : 1 complex. It is shown that, in all the example cases dealt with in this study, the frequency shift depends rather strongly on the hydrogen- or halogen-bond angle (e.g., S[double bond, length as m-dash]OH angle), with a larger low-frequency shift as the hydrogen or halogen bond becomes more bent, indicating the generality of the results obtained for the amide I' mode of the N-methylacetamide-d1(2)H2O 1 : 1 complex in a previous study. Contrary to our vague expectation, the frequency shift is not well correlated to the hydrogen- or halogen-bond distance or strength, but nevertheless, it is well reproduced by an electrostatic interaction model if it is carefully constructed by considering the scalar and vector components separately in a reasonable way. On the basis of this electrostatic interaction model, the reason why our vague expectation is not realized is clarified, and a unified understanding is achieved on the hydration-induced high-frequency shift of the C[triple bond, length as m-dash]N stretch and the low-frequency shifts of the S[double bond, length as m-dash]O stretch and amide I'. With regard to the IR intensity, it is shown that, in some of the example cases, it also has rather strong angular position dependence. The mechanism of the IR intensity changes is estimated by analyzing the dipole derivative vector, especially its angular relation with the hydrogen or halogen bond.

Measurements of Elliptic and Triangular Flow in High-Multiplicity 3He+Au Collisions at √(s(NN))=200 GeV

We present the first measurement of elliptic (v(2)) and triangular (v(3)) flow in high-multiplicity (3)He+Au collisions at √(s(NN))=200  GeV. Two-particle correlations, where the particles have a large separation in pseudorapidity, are compared in (3)He+Au and in p+p collisions and indicate that collective effects dominate the second and third Fourier components for the correlations observed in the (3)He+Au system. The collective behavior is quantified in terms of elliptic v(2) and triangular v(3) anisotropy coefficients measured with respect to their corresponding event planes. The v(2) values are comparable to those previously measured in d+Au collisions at the same nucleon-nucleon center-of-mass energy. Comparisons with various theoretical predictions are made, including to models where the hot spots created by the impact of the three (3)He nucleons on the Au nucleus expand hydrodynamically to generate the triangular flow. The agreement of these models with data may indicate the formation of low-viscosity quark-gluon plasma even in these small collision systems.

Measurement of Long-Range Angular Correlation and Quadrupole Anisotropy of Pions and (Anti)Protons in Central d+Au Collisions at sqrt[s_{NN}]=200 GeV

We present azimuthal angular correlations between charged hadrons and energy deposited in calorimeter towers in central d+Au and minimum bias p+p collisions at sqrt[s_{NN}]=200 GeV. The charged hadron is measured at midrapidity |η|<0.35, and the energy is measured at large rapidity (-3.7<η<-3.1, Au-going direction). An enhanced near-side angular correlation across |Δη|>2.75 is observed in d+Au collisions. Using the event plane method applied to the Au-going energy distribution, we extract the anisotropy strength v_{2} for inclusive charged hadrons at midrapidity up to p_{T}=4.5 GeV/c. We also present the measurement of v_{2} for identified π^{±} and (anti)protons in central d+Au collisions, and observe a mass-ordering pattern similar to that seen in heavy-ion collisions. These results are compared with viscous hydrodynamic calculations and measurements from p+Pb at sqrt[s_{NN}]=5.02 TeV. The magnitude of the mass ordering in d+Au is found to be smaller than that in p+Pb collisions, which may indicate smaller radial flow in lower energy d+Au collisions.

Amide I Vibrational Properties Affected by Hydrogen Bonding Out-of-Plane of the Peptide Group

The amide I vibrational properties of a peptide-water complex in various intermolecular configurations are analyzed theoretically to see whether a water molecule with a weak out-of-plane hydrogen bond really induces a large low-frequency shift. It is shown that the frequency shift strongly depends on the C═O···H angle, with a larger low-frequency shift as the C═O···H becomes more bent, suggesting that the so-called hydrated helix with a rather low amide I frequency has an additional water molecule located out-of-plane of the peptide group as compared with a typical α-helix. The infrared intensity also depends on the angular position of water. A new model parameter set (that can be combined with molecular dynamics) is developed for a more correct representation of the hydration-induced frequency shift. The question regarding the scalar and vectorial nature of the molecular properties related to the frequency shift is also discussed.

Measurement of quarkonium production at forward rapidity in [Formula: see text] collisions at [Formula: see text]TeV

The inclusive production cross sections at forward rapidity of [Formula: see text], [Formula: see text], [Formula: see text](1S) and [Formula: see text](2S) are measured in [Formula: see text] collisions at [Formula: see text] with the ALICE detector at the LHC. The analysis is based on a data sample corresponding to an integrated luminosity of 1.35 pb[Formula: see text]. Quarkonia are reconstructed in the dimuon-decay channel and the signal yields are evaluated by fitting the [Formula: see text] invariant mass distributions. The differential production cross sections are measured as a function of the transverse momentum [Formula: see text] and rapidity [Formula: see text], over the ranges [Formula: see text] GeV/c for [Formula: see text], [Formula: see text] GeV/c for all other resonances and for [Formula: see text]. The measured cross sections integrated over [Formula: see text] and [Formula: see text], and assuming unpolarized quarkonia, are: [Formula: see text] [Formula: see text]b, [Formula: see text] [Formula: see text]b, [Formula: see text] nb and [Formula: see text] nb, where the first uncertainty is statistical and the second one is systematic. The results are compared to measurements performed by other LHC experiments and to theoretical models.

Cold-nuclear-matter effects on heavy-quark production at forward and backward rapidity in d + Au collisions at √sNN = 200 GeV

The PHENIX experiment has measured open heavy-flavor production via semileptonic decay over the transverse momentum range 1 < p(T) < 6  GeV/c at forward and backward rapidity (1.4 < |y| < 2.0) in d+Au and p + p collisions at √sNN = 200  GeV. In central d+Au collisions, relative to the yield in p + p collisions scaled by the number of binary nucleon-nucleon collisions, a suppression is observed at forward rapidity (in the d-going direction) and an enhancement at backward rapidity (in the Au-going direction). Predictions using nuclear-modified-parton-distribution functions, even with additional nuclear-p(T) broadening, cannot simultaneously reproduce the data at both rapidity ranges, which implies that these models are incomplete and suggests the possible importance of final-state interactions in the asymmetric d + Au collision system. These results can be used to probe cold-nuclear-matter effects, which may significantly affect heavy-quark production, in addition to helping constrain the magnitude of charmonia-breakup effects in nuclear matter.

Azimuthal-angle dependence of charged-pion-interferometry measurements with respect to second- and third-order event planes in Au+Au collisions at √[S(NN)]=200 GeV

Charged-pion-interferometry measurements were made with respect to the second- and third-order event plane for Au+Au collisions at sqrt[s_{NN}]=200  GeV. A strong azimuthal-angle dependence of the extracted Gaussian-source radii was observed with respect to both the second- and third-order event planes. The results for the second-order dependence indicate that the initial eccentricity is reduced during the medium evolution, which is consistent with previous results. In contrast, the results for the third-order dependence indicate that the initial triangular shape is significantly reduced and potentially reversed by the end of the medium evolution, and that the third-order oscillations are largely dominated by the dynamical effects from triangular flow.

Energy dependence of the transverse momentum distributions of charged particles in pp collisions measured by ALICE

Differential cross sections of charged particles in inelastic pp collisions as a function of p_T have been measured at [Formula: see text] at the LHC. The p_T spectra are compared to NLO-pQCD calculations. Though the differential cross section for an individual [Formula: see text] cannot be described by NLO-pQCD, the relative increase of cross section with [Formula: see text] is in agreement with NLO-pQCD. Based on these measurements and observations, procedures are discussed to construct pp reference spectra at [Formula: see text] up to p_T=50 GeV/c as required for the calculation of the nuclear modification factor in nucleus-nucleus and proton-nucleus collisions.

Directed flow of charged particles at midrapidity relative to the spectator plane in Pb-Pb collisions at √(s(NN))=2.76 TeV

The directed flow of charged particles at midrapidity is measured in Pb-Pb collisions at √(s(NN))=2.76 TeV relative to the collision symmetry plane defined by the spectator nucleons. A negative slope of the rapidity-odd directed flow component with approximately 3 times smaller magnitude than found at the highest RHIC energy is observed. This suggests a smaller longitudinal tilt of the initial system and disfavors the strong fireball rotation predicted for the LHC energies. The rapidity-even directed flow component is measured for the first time with spectators and found to be independent of pseudorapidity with a sign change at transverse momenta p(T) between 1.2 and 1.7  GeV/c. Combined with the observation of a vanishing rapidity-even p(T) shift along the spectator deflection this is strong evidence for dipolelike initial density fluctuations in the overlap zone of the nuclei. Similar trends in the rapidity-even directed flow and the estimate from two-particle correlations at midrapidity, which is larger by about a factor of 40, indicate a weak correlation between fluctuating participant and spectator symmetry planes. These observations open new possibilities for investigation of the initial conditions in heavy-ion collisions with spectator nucleons.

K(S)0 and Λ production in Pb-Pb collisions at √(s(NN))=2.76 TeV

The ALICE measurement of K(S)(0) and Λ production at midrapidity in Pb-Pb collisions at √(s(NN))=2.76 TeV is presented. The transverse momentum (p(T)) spectra are shown for several collision centrality intervals and in the p(T) range from 0.4 GeV/c (0.6 GeV/c for Λ) to 12 GeV/c. The p(T) dependence of the Λ/K(S)(0) ratios exhibits maxima in the vicinity of 3 GeV/c, and the positions of the maxima shift towards higher p(T) with increasing collision centrality. The magnitude of these maxima increases by almost a factor of three between most peripheral and most central Pb-Pb collisions. This baryon excess at intermediate p(T) is not observed in pp interactions at √s=0.9 TeV and at √s=7 TeV. Qualitatively, the baryon enhancement in heavy-ion collisions is expected from radial flow. However, the measured p(T) spectra above 2 GeV/c progressively decouple from hydrodynamical-model calculations. For higher values of p(T), models that incorporate the influence of the medium on the fragmentation and hadronization processes describe qualitatively the p(T) dependence of the Λ/K(S)(0) ratio.

Quadrupole anisotropy in dihadron azimuthal correlations in central d+Au collisions at √(s(NN))=200 GeV

The PHENIX collaboration at the Relativistic Heavy Ion Collider (RHIC) reports measurements of azimuthal dihadron correlations near midrapidity in d+Au collisions at √(s(NN))=200 GeV. These measurements complement recent analyses by experiments at the Large Hadron Collider (LHC) involving central p+Pb collisions at √(s(NN))=5.02 TeV, which have indicated strong anisotropic long-range correlations in angular distributions of hadron pairs. The origin of these anisotropies is currently unknown. Various competing explanations include parton saturation and hydrodynamic flow. We observe qualitatively similar, but larger, anisotropies in d+Au collisions at RHIC compared to those seen in p+Pb collisions at the LHC. The larger extracted v2 values in d+Au are consistent with expectations from hydrodynamic calculations owing to the larger expected initial-state eccentricity compared with that from p+Pb collisions. When both are divided by an estimate of the initial-state eccentricity the scaled anisotropies follow a common trend with multiplicity that may extend to heavy ion data at RHIC and the LHC, where the anisotropies are widely thought to arise from hydrodynamic flow.

Nuclear modification of ψ', χc, and J/ψ production in d+Au collisions at sqrt[s(NN)]=200 GeV

We present results for three charmonia states (ψ', χc, and J/ψ) in d+Au collisions at |y|<0.35 and sqrt[s(NN)]=200  GeV. We find that the modification of the ψ' yield relative to that of the J/ψ scales approximately with charged particle multiplicity at midrapidity across p+A, d+Au, and A+A results from the Super Proton Synchrotron and the Relativistic Heavy Ion Collider. In large-impact-parameter collisions we observe a similar suppression for the ψ' and J/ψ, while in small-impact-parameter collisions the more weakly bound ψ' is more strongly suppressed. Owing to the short time spent traversing the Au nucleus, the larger ψ' suppression in central events is not explained by an increase of the nuclear absorption owing to meson formation time effects.

Charmonium and e+e- pair photoproduction at mid-rapidity in ultra-peripheral Pb-Pb collisions at [Formula: see text]

The ALICE Collaboration at the LHC has measured the J/ψ and ψ' photoproduction at mid-rapidity in ultra-peripheral Pb-Pb collisions at [Formula: see text]. The charmonium is identified via its leptonic decay for events where the hadronic activity is required to be minimal. The analysis is based on an event sample corresponding to an integrated luminosity of about 23 μb-1. The cross section for coherent and incoherent J/ψ production in the rapidity interval -0.9 Collapse

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Affiliation(s)

The ALICE Collaboration CERN, 1211 Geneva 23, Switzerland
E. Abbas Academy of Scientific Research and Technology (ASRT), Cairo, Egypt Fachhochschule Köln, Köln, Germany Department of Physics, Gauhati University, Guwahati, India Suranaree University of Technology, Nakhon Ratchasima, Thailand University of Technology and Austrian Academy of Sciences, Vienna, Austria
B. Abelev Lawrence Livermore National Laboratory, Livermore, California United States
J. Adam Faculty of Nuclear Sciences and Physical Engineering, Czech Technical University in Prague, Prague, Czech Republic
D. Adamová Nuclear Physics Institute, Academy of Sciences of the Czech Republic, Řež u Prahy, Czech Republic
A. M. Adare Yale University, New Haven, Connecticut United States
M. M. Aggarwal Physics Department, Panjab University, Chandigarh, India
G. Aglieri Rinella European Organization for Nuclear Research (CERN), Geneva, Switzerland
M. Agnello Politecnico di Torino, Turin, Italy Sezione INFN, Turin, Italy
A. G. Agocs Wigner Research Centre for Physics, Hungarian Academy of Sciences, Budapest, Hungary
A. Agostinelli Dipartimento di Fisica e Astronomia dell’Università and Sezione INFN, Bologna, Italy
Z. Ahammed Variable Energy Cyclotron Centre, Kolkata, India
N. Ahmad Department of Physics, Aligarh Muslim University, Aligarh, India
A. Ahmad Masoodi Department of Physics, Aligarh Muslim University, Aligarh, India
I. Ahmed COMSATS Institute of Information Technology (CIIT), Islamabad, Pakistan
S. A. Ahn Korea Institute of Science and Technology Information, Daejeon, South Korea
S. U. Ahn Korea Institute of Science and Technology Information, Daejeon, South Korea
I. Aimo Dipartimento di Fisica dell’Università and Sezione INFN, Turin, Italy Politecnico di Torino, Turin, Italy Sezione INFN, Turin, Italy
M. Ajaz COMSATS Institute of Information Technology (CIIT), Islamabad, Pakistan
A. Akindinov Institute for Theoretical and Experimental Physics, Moscow, Russia
D. Aleksandrov Russian Research Centre Kurchatov Institute, Moscow, Russia
B. Alessandro Sezione INFN, Turin, Italy
D. Alexandre School of Physics and Astronomy, University of Birmingham, Birmingham, United Kingdom
A. Alici Centro Fermi - Museo Storico della Fisica e Centro Studi e Ricerche “Enrico Fermi”, Rome, Italy Sezione INFN, Bologna, Italy
A. Alkin Bogolyubov Institute for Theoretical Physics, Kiev, Ukraine
E. Almaráz Aviña Instituto de Física, Universidad Nacional Autónoma de México, Mexico City, Mexico
J. Alme Faculty of Engineering, Bergen University College, Bergen, Norway
T. Alt Frankfurt Institute for Advanced Studies, Johann Wolfgang Goethe-Universität Frankfurt, Frankfurt, Germany
V. Altini Dipartimento Interateneo di Fisica ‘M. Merlin’ and Sezione INFN, Bari, Italy
S. Altinpinar Department of Physics and Technology, University of Bergen, Bergen, Norway
I. Altsybeev V. Fock Institute for Physics, St. Petersburg State University, St. Petersburg, Russia
C. Andrei National Institute for Physics and Nuclear Engineering, Bucharest, Romania
A. Andronic Research Division and ExtreMe Matter Institute EMMI, GSI Helmholtzzentrum für Schwerionenforschung, Darmstadt, Germany
V. Anguelov Physikalisches Institut, Ruprecht-Karls-Universität Heidelberg, Heidelberg, Germany
J. Anielski Institut für Kernphysik, Westfälische Wilhelms-Universität Münster, Münster, Germany
C. Anson Department of Physics, Ohio State University, Columbus, Ohio United States
T. Antičić Rudjer Bošković Institute, Zagreb, Croatia
F. Antinori Sezione INFN, Padova, Italy
P. Antonioli Sezione INFN, Bologna, Italy
L. Aphecetche SUBATECH, Ecole des Mines de Nantes, Université de Nantes, CNRS-IN2P3, Nantes, France
H. Appelshäuser Institut für Kernphysik, Johann Wolfgang Goethe-Universität Frankfurt, Frankfurt, Germany
N. Arbor Laboratoire de Physique Subatomique et de Cosmologie (LPSC), Université Joseph Fourier, CNRS-IN2P3, Institut Polytechnique de Grenoble, Grenoble, France
S. Arcelli Dipartimento di Fisica e Astronomia dell’Università and Sezione INFN, Bologna, Italy
A. Arend Institut für Kernphysik, Johann Wolfgang Goethe-Universität Frankfurt, Frankfurt, Germany
N. Armesto Departamento de Física de Partículas and IGFAE, Universidad de Santiago de Compostela, Santiago de Compostela, Spain
R. Arnaldi Sezione INFN, Turin, Italy
T. Aronsson Yale University, New Haven, Connecticut United States
I. C. Arsene Research Division and ExtreMe Matter Institute EMMI, GSI Helmholtzzentrum für Schwerionenforschung, Darmstadt, Germany
M. Arslandok Institut für Kernphysik, Johann Wolfgang Goethe-Universität Frankfurt, Frankfurt, Germany
A. Asryan V. Fock Institute for Physics, St. Petersburg State University, St. Petersburg, Russia
A. Augustinus European Organization for Nuclear Research (CERN), Geneva, Switzerland
R. Averbeck Research Division and ExtreMe Matter Institute EMMI, GSI Helmholtzzentrum für Schwerionenforschung, Darmstadt, Germany
T. C. Awes Oak Ridge National Laboratory, Oak Ridge, Tennessee United States
J. Äystö Helsinki Institute of Physics (HIP) and University of Jyväskylä, Jyväskylä, Finland
M. D. Azmi Department of Physics, Aligarh Muslim University, Aligarh, India Physics Department, University of Cape Town and iThemba LABS, National Research Foundation, Somerset West, South Africa
M. Bach Frankfurt Institute for Advanced Studies, Johann Wolfgang Goethe-Universität Frankfurt, Frankfurt, Germany
A. Badalà Sezione INFN, Catania, Italy
Y. W. Baek Gangneung-Wonju National University, Gangneung, South Korea Laboratoire de Physique Corpusculaire (LPC), Clermont Université, Université Blaise Pascal, CNRS–IN2P3, Clermont-Ferrand, France
R. Bailhache Institut für Kernphysik, Johann Wolfgang Goethe-Universität Frankfurt, Frankfurt, Germany
R. Bala Physics Department, University of Jammu, Jammu, India Sezione INFN, Turin, Italy
A. Baldisseri Commissariat à l’Energie Atomique, IRFU, Saclay, France
F. Baltasar Dos Santos Pedrosa European Organization for Nuclear Research (CERN), Geneva, Switzerland
J. Bán Institute of Experimental Physics, Slovak Academy of Sciences, Košice, Slovakia
R. C. Baral Institute of Physics, Bhubaneswar, India
R. Barbera Dipartimento di Fisica e Astronomia dell’Università and Sezione INFN, Catania, Italy
F. Barile Dipartimento Interateneo di Fisica ‘M. Merlin’ and Sezione INFN, Bari, Italy
G. G. Barnaföldi Wigner Research Centre for Physics, Hungarian Academy of Sciences, Budapest, Hungary
L. S. Barnby School of Physics and Astronomy, University of Birmingham, Birmingham, United Kingdom
V. Barret Laboratoire de Physique Corpusculaire (LPC), Clermont Université, Université Blaise Pascal, CNRS–IN2P3, Clermont-Ferrand, France
J. Bartke The Henryk Niewodniczanski Institute of Nuclear Physics, Polish Academy of Sciences, Cracow, Poland
M. Basile Dipartimento di Fisica e Astronomia dell’Università and Sezione INFN, Bologna, Italy
N. Bastid Laboratoire de Physique Corpusculaire (LPC), Clermont Université, Université Blaise Pascal, CNRS–IN2P3, Clermont-Ferrand, France
S. Basu Variable Energy Cyclotron Centre, Kolkata, India
B. Bathen Institut für Kernphysik, Westfälische Wilhelms-Universität Münster, Münster, Germany
G. Batigne SUBATECH, Ecole des Mines de Nantes, Université de Nantes, CNRS-IN2P3, Nantes, France
B. Batyunya Joint Institute for Nuclear Research (JINR), Dubna, Russia
P. C. Batzing Department of Physics, University of Oslo, Oslo, Norway
C. Baumann Institut für Kernphysik, Johann Wolfgang Goethe-Universität Frankfurt, Frankfurt, Germany
I. G. Bearden Niels Bohr Institute, University of Copenhagen, Copenhagen, Denmark
H. Beck Institut für Kernphysik, Johann Wolfgang Goethe-Universität Frankfurt, Frankfurt, Germany
N. K. Behera Indian Institute of Technology Bombay (IIT), Mumbai, India
I. Belikov Institut Pluridisciplinaire Hubert Curien (IPHC), Université de Strasbourg, CNRS-IN2P3, Strasbourg, France
F. Bellini Dipartimento di Fisica e Astronomia dell’Università and Sezione INFN, Bologna, Italy
R. Bellwied University of Houston, Houston, Texas United States
E. Belmont-Moreno Instituto de Física, Universidad Nacional Autónoma de México, Mexico City, Mexico
G. Bencedi Wigner Research Centre for Physics, Hungarian Academy of Sciences, Budapest, Hungary
S. Beole Dipartimento di Fisica dell’Università and Sezione INFN, Turin, Italy
I. Berceanu National Institute for Physics and Nuclear Engineering, Bucharest, Romania
A. Bercuci National Institute for Physics and Nuclear Engineering, Bucharest, Romania
Y. Berdnikov Petersburg Nuclear Physics Institute, Gatchina, Russia
D. Berenyi Wigner Research Centre for Physics, Hungarian Academy of Sciences, Budapest, Hungary
A. A. E. Bergognon SUBATECH, Ecole des Mines de Nantes, Université de Nantes, CNRS-IN2P3, Nantes, France
R. A. Bertens Nikhef, National Institute for Subatomic Physics and Institute for Subatomic Physics of Utrecht University, Utrecht, Netherlands
D. Berzano Dipartimento di Fisica dell’Università and Sezione INFN, Turin, Italy Sezione INFN, Turin, Italy
L. Betev European Organization for Nuclear Research (CERN), Geneva, Switzerland
A. Bhasin Physics Department, University of Jammu, Jammu, India
A. K. Bhati Physics Department, Panjab University, Chandigarh, India
J. Bhom University of Tsukuba, Tsukuba, Japan
L. Bianchi Dipartimento di Fisica dell’Università and Sezione INFN, Turin, Italy
N. Bianchi Laboratori Nazionali di Frascati, INFN, Frascati, Italy
C. Bianchin Nikhef, National Institute for Subatomic Physics and Institute for Subatomic Physics of Utrecht University, Utrecht, Netherlands
J. Bielčík Faculty of Nuclear Sciences and Physical Engineering, Czech Technical University in Prague, Prague, Czech Republic
J. Bielčíková Nuclear Physics Institute, Academy of Sciences of the Czech Republic, Řež u Prahy, Czech Republic
A. Bilandzic Niels Bohr Institute, University of Copenhagen, Copenhagen, Denmark
S. Bjelogrlic Nikhef, National Institute for Subatomic Physics and Institute for Subatomic Physics of Utrecht University, Utrecht, Netherlands
F. Blanco Centro de Investigaciones Energéticas Medioambientales y Tecnológicas (CIEMAT), Madrid, Spain
F. Blanco University of Houston, Houston, Texas United States
D. Blau Russian Research Centre Kurchatov Institute, Moscow, Russia
C. Blume Institut für Kernphysik, Johann Wolfgang Goethe-Universität Frankfurt, Frankfurt, Germany
M. Boccioli European Organization for Nuclear Research (CERN), Geneva, Switzerland
S. Böttger Institut für Informatik, Johann Wolfgang Goethe-Universität Frankfurt, Frankfurt, Germany
A. Bogdanov Moscow Engineering Physics Institute, Moscow, Russia
H. Bøggild Niels Bohr Institute, University of Copenhagen, Copenhagen, Denmark
M. Bogolyubsky Institute for High Energy Physics, Protvino, Russia
L. Boldizsár Wigner Research Centre for Physics, Hungarian Academy of Sciences, Budapest, Hungary
M. Bombara Faculty of Science, P.J. Šafárik University, Košice, Slovakia
J. Book Institut für Kernphysik, Johann Wolfgang Goethe-Universität Frankfurt, Frankfurt, Germany
H. Borel Commissariat à l’Energie Atomique, IRFU, Saclay, France
A. Borissov Wayne State University, Detroit, Michigan United States
F. Bossú Physics Department, University of Cape Town and iThemba LABS, National Research Foundation, Somerset West, South Africa
M. Botje Nikhef, National Institute for Subatomic Physics, Amsterdam, Netherlands
E. Botta Dipartimento di Fisica dell’Università and Sezione INFN, Turin, Italy
E. Braidot Lawrence Berkeley National Laboratory, Berkeley, California United States
P. Braun-Munzinger Research Division and ExtreMe Matter Institute EMMI, GSI Helmholtzzentrum für Schwerionenforschung, Darmstadt, Germany
M. Bregant SUBATECH, Ecole des Mines de Nantes, Université de Nantes, CNRS-IN2P3, Nantes, France
T. Breitner Institut für Informatik, Johann Wolfgang Goethe-Universität Frankfurt, Frankfurt, Germany
T. A. Broker Institut für Kernphysik, Johann Wolfgang Goethe-Universität Frankfurt, Frankfurt, Germany
T. A. Browning Purdue University, West Lafayette, Indiana United States
M. Broz Faculty of Mathematics, Physics and Informatics, Comenius University, Bratislava, Slovakia
R. Brun European Organization for Nuclear Research (CERN), Geneva, Switzerland
E. Bruna Dipartimento di Fisica dell’Università and Sezione INFN, Turin, Italy Sezione INFN, Turin, Italy
G. E. Bruno Dipartimento Interateneo di Fisica ‘M. Merlin’ and Sezione INFN, Bari, Italy
D. Budnikov Russian Federal Nuclear Center (VNIIEF), Sarov, Russia
H. Buesching Institut für Kernphysik, Johann Wolfgang Goethe-Universität Frankfurt, Frankfurt, Germany
S. Bufalino Dipartimento di Fisica dell’Università and Sezione INFN, Turin, Italy Sezione INFN, Turin, Italy
P. Buncic European Organization for Nuclear Research (CERN), Geneva, Switzerland
O. Busch Physikalisches Institut, Ruprecht-Karls-Universität Heidelberg, Heidelberg, Germany
Z. Buthelezi Physics Department, University of Cape Town and iThemba LABS, National Research Foundation, Somerset West, South Africa
D. Caffarri Dipartimento di Fisica e Astronomia dell’Università and Sezione INFN, Padova, Italy Sezione INFN, Padova, Italy
X. Cai Central China Normal University, Wuhan, China
H. Caines Yale University, New Haven, Connecticut United States
E. Calvo Villar Sección Física, Departamento de Ciencias, Pontificia Universidad Católica del Perú, Lima, Peru
P. Camerini Dipartimento di Fisica dell’Università and Sezione INFN, Trieste, Italy
V. Canoa Roman Centro de Investigación y de Estudios Avanzados (CINVESTAV), Mexico City and Mérida, Mexico
G. Cara Romeo Sezione INFN, Bologna, Italy
W. Carena European Organization for Nuclear Research (CERN), Geneva, Switzerland
F. Carena European Organization for Nuclear Research (CERN), Geneva, Switzerland
N. Carlin Filho Universidade de São Paulo (USP), São Paulo, Brazil
F. Carminati European Organization for Nuclear Research (CERN), Geneva, Switzerland
A. Casanova Díaz Laboratori Nazionali di Frascati, INFN, Frascati, Italy
J. Castillo Castellanos Commissariat à l’Energie Atomique, IRFU, Saclay, France
J. F. Castillo Hernandez Research Division and ExtreMe Matter Institute EMMI, GSI Helmholtzzentrum für Schwerionenforschung, Darmstadt, Germany
E. A. R. Casula Dipartimento di Fisica dell’Università and Sezione INFN, Cagliari, Italy
V. Catanescu National Institute for Physics and Nuclear Engineering, Bucharest, Romania
C. Cavicchioli European Organization for Nuclear Research (CERN), Geneva, Switzerland
C. Ceballos Sanchez Centro de Aplicaciones Tecnológicas y Desarrollo Nuclear (CEADEN), Havana, Cuba
J. Cepila Faculty of Nuclear Sciences and Physical Engineering, Czech Technical University in Prague, Prague, Czech Republic
P. Cerello Sezione INFN, Turin, Italy
B. Chang Helsinki Institute of Physics (HIP) and University of Jyväskylä, Jyväskylä, Finland Yonsei University, Seoul, South Korea
S. Chapeland European Organization for Nuclear Research (CERN), Geneva, Switzerland
J. L. Charvet Commissariat à l’Energie Atomique, IRFU, Saclay, France
S. Chattopadhyay Variable Energy Cyclotron Centre, Kolkata, India
S. Chattopadhyay Saha Institute of Nuclear Physics, Kolkata, India
M. Cherney Physics Department, Creighton University, Omaha, Nebraska United States
C. Cheshkov European Organization for Nuclear Research (CERN), Geneva, Switzerland Université de Lyon, Université Lyon 1, CNRS/IN2P3, IPN-Lyon, Villeurbanne, France
B. Cheynis Université de Lyon, Université Lyon 1, CNRS/IN2P3, IPN-Lyon, Villeurbanne, France
V. Chibante Barroso European Organization for Nuclear Research (CERN), Geneva, Switzerland
D. D. Chinellato University of Houston, Houston, Texas United States
P. Chochula European Organization for Nuclear Research (CERN), Geneva, Switzerland
M. Chojnacki Niels Bohr Institute, University of Copenhagen, Copenhagen, Denmark
S. Choudhury Variable Energy Cyclotron Centre, Kolkata, India
P. Christakoglou Nikhef, National Institute for Subatomic Physics, Amsterdam, Netherlands
C. H. Christensen Niels Bohr Institute, University of Copenhagen, Copenhagen, Denmark
P. Christiansen Division of Experimental High Energy Physics, University of Lund, Lund, Sweden
T. Chujo University of Tsukuba, Tsukuba, Japan
S. U. Chung Pusan National University, Pusan, South Korea
C. Cicalo Sezione INFN, Cagliari, Italy
L. Cifarelli Centro Fermi - Museo Storico della Fisica e Centro Studi e Ricerche “Enrico Fermi”, Rome, Italy Dipartimento di Fisica e Astronomia dell’Università and Sezione INFN, Bologna, Italy
F. Cindolo Sezione INFN, Bologna, Italy
J. Cleymans Physics Department, University of Cape Town and iThemba LABS, National Research Foundation, Somerset West, South Africa
F. Colamaria Dipartimento Interateneo di Fisica ‘M. Merlin’ and Sezione INFN, Bari, Italy
D. Colella Dipartimento Interateneo di Fisica ‘M. Merlin’ and Sezione INFN, Bari, Italy
A. Collu Dipartimento di Fisica dell’Università and Sezione INFN, Cagliari, Italy
G. Conesa Balbastre Laboratoire de Physique Subatomique et de Cosmologie (LPSC), Université Joseph Fourier, CNRS-IN2P3, Institut Polytechnique de Grenoble, Grenoble, France
Z. Conesa del Valle European Organization for Nuclear Research (CERN), Geneva, Switzerland Institut de Physique Nucléaire d’Orsay (IPNO), Université Paris-Sud, CNRS-IN2P3, Orsay, France
M. E. Connors Yale University, New Haven, Connecticut United States
G. Contin Dipartimento di Fisica dell’Università and Sezione INFN, Trieste, Italy
J. G. Contreras Centro de Investigación y de Estudios Avanzados (CINVESTAV), Mexico City and Mérida, Mexico
T. M. Cormier Wayne State University, Detroit, Michigan United States
Y. Corrales Morales Dipartimento di Fisica dell’Università and Sezione INFN, Turin, Italy
P. Cortese Dipartimento di Scienze e Innovazione Tecnologica dell’Università del Piemonte Orientale and Gruppo Collegato INFN, Alessandria, Italy
I. Cortés Maldonado Benemérita Universidad Autónoma de Puebla, Puebla, Mexico
M. R. Cosentino Lawrence Berkeley National Laboratory, Berkeley, California United States
F. Costa European Organization for Nuclear Research (CERN), Geneva, Switzerland
M. E. Cotallo Centro de Investigaciones Energéticas Medioambientales y Tecnológicas (CIEMAT), Madrid, Spain
E. Crescio Centro de Investigación y de Estudios Avanzados (CINVESTAV), Mexico City and Mérida, Mexico
P. Crochet Laboratoire de Physique Corpusculaire (LPC), Clermont Université, Université Blaise Pascal, CNRS–IN2P3, Clermont-Ferrand, France
E. Cruz Alaniz Instituto de Física, Universidad Nacional Autónoma de México, Mexico City, Mexico
R. Cruz Albino Centro de Investigación y de Estudios Avanzados (CINVESTAV), Mexico City and Mérida, Mexico
E. Cuautle Instituto de Ciencias Nucleares, Universidad Nacional Autónoma de México, Mexico City, Mexico
L. Cunqueiro Laboratori Nazionali di Frascati, INFN, Frascati, Italy
A. Dainese Dipartimento di Fisica e Astronomia dell’Università and Sezione INFN, Padova, Italy Sezione INFN, Padova, Italy
R. Dang Central China Normal University, Wuhan, China
A. Danu Institute of Space Sciences (ISS), Bucharest, Romania
K. Das Saha Institute of Nuclear Physics, Kolkata, India
I. Das Institut de Physique Nucléaire d’Orsay (IPNO), Université Paris-Sud, CNRS-IN2P3, Orsay, France
S. Das Department of Physics and Centre for Astroparticle Physics and Space Science (CAPSS), Bose Institute, Kolkata, India
D. Das Saha Institute of Nuclear Physics, Kolkata, India
S. Dash Indian Institute of Technology Bombay (IIT), Mumbai, India
A. Dash Universidade Estadual de Campinas (UNICAMP), Campinas, Brazil
S. De Variable Energy Cyclotron Centre, Kolkata, India
G. O. V. de Barros Universidade de São Paulo (USP), São Paulo, Brazil
A. De Caro Centro Fermi - Museo Storico della Fisica e Centro Studi e Ricerche “Enrico Fermi”, Rome, Italy Dipartimento di Fisica ‘E.R. Caianiello’ dell’Università and Gruppo Collegato INFN, Salerno, Italy
G. de Cataldo Sezione INFN, Bari, Italy
J. de Cuveland Frankfurt Institute for Advanced Studies, Johann Wolfgang Goethe-Universität Frankfurt, Frankfurt, Germany
A. De Falco Dipartimento di Fisica dell’Università and Sezione INFN, Cagliari, Italy
D. De Gruttola Centro Fermi - Museo Storico della Fisica e Centro Studi e Ricerche “Enrico Fermi”, Rome, Italy Dipartimento di Fisica ‘E.R. Caianiello’ dell’Università and Gruppo Collegato INFN, Salerno, Italy
H. Delagrange SUBATECH, Ecole des Mines de Nantes, Université de Nantes, CNRS-IN2P3, Nantes, France
A. Deloff National Centre for Nuclear Studies, Warsaw, Poland
N. De Marco Sezione INFN, Turin, Italy
E. Dénes Wigner Research Centre for Physics, Hungarian Academy of Sciences, Budapest, Hungary
S. De Pasquale Dipartimento di Fisica ‘E.R. Caianiello’ dell’Università and Gruppo Collegato INFN, Salerno, Italy
A. Deppman Universidade de São Paulo (USP), São Paulo, Brazil
G. D Erasmo Dipartimento Interateneo di Fisica ‘M. Merlin’ and Sezione INFN, Bari, Italy
R. de Rooij Nikhef, National Institute for Subatomic Physics and Institute for Subatomic Physics of Utrecht University, Utrecht, Netherlands
M. A. Diaz Corchero Centro de Investigaciones Energéticas Medioambientales y Tecnológicas (CIEMAT), Madrid, Spain
D. Di Bari Dipartimento Interateneo di Fisica ‘M. Merlin’ and Sezione INFN, Bari, Italy
T. Dietel Institut für Kernphysik, Westfälische Wilhelms-Universität Münster, Münster, Germany
C. Di Giglio Dipartimento Interateneo di Fisica ‘M. Merlin’ and Sezione INFN, Bari, Italy
S. Di Liberto Sezione INFN, Rome, Italy
A. Di Mauro European Organization for Nuclear Research (CERN), Geneva, Switzerland
P. Di Nezza Laboratori Nazionali di Frascati, INFN, Frascati, Italy
R. Divià European Organization for Nuclear Research (CERN), Geneva, Switzerland
Ø. Djuvsland Department of Physics and Technology, University of Bergen, Bergen, Norway
A. Dobrin Division of Experimental High Energy Physics, University of Lund, Lund, Sweden Nikhef, National Institute for Subatomic Physics and Institute for Subatomic Physics of Utrecht University, Utrecht, Netherlands Wayne State University, Detroit, Michigan United States
T. Dobrowolski National Centre for Nuclear Studies, Warsaw, Poland
B. Dönigus Research Division and ExtreMe Matter Institute EMMI, GSI Helmholtzzentrum für Schwerionenforschung, Darmstadt, Germany
O. Dordic Department of Physics, University of Oslo, Oslo, Norway
A. K. Dubey Variable Energy Cyclotron Centre, Kolkata, India
A. Dubla Nikhef, National Institute for Subatomic Physics and Institute for Subatomic Physics of Utrecht University, Utrecht, Netherlands
L. Ducroux Université de Lyon, Université Lyon 1, CNRS/IN2P3, IPN-Lyon, Villeurbanne, France
P. Dupieux Laboratoire de Physique Corpusculaire (LPC), Clermont Université, Université Blaise Pascal, CNRS–IN2P3, Clermont-Ferrand, France
A. K. Dutta Majumdar Saha Institute of Nuclear Physics, Kolkata, India
D. Elia Sezione INFN, Bari, Italy
D. Emschermann Institut für Kernphysik, Westfälische Wilhelms-Universität Münster, Münster, Germany
H. Engel Institut für Informatik, Johann Wolfgang Goethe-Universität Frankfurt, Frankfurt, Germany
B. Erazmus European Organization for Nuclear Research (CERN), Geneva, Switzerland SUBATECH, Ecole des Mines de Nantes, Université de Nantes, CNRS-IN2P3, Nantes, France
H. A. Erdal Faculty of Engineering, Bergen University College, Bergen, Norway
D. Eschweiler Frankfurt Institute for Advanced Studies, Johann Wolfgang Goethe-Universität Frankfurt, Frankfurt, Germany
B. Espagnon Institut de Physique Nucléaire d’Orsay (IPNO), Université Paris-Sud, CNRS-IN2P3, Orsay, France
M. Estienne SUBATECH, Ecole des Mines de Nantes, Université de Nantes, CNRS-IN2P3, Nantes, France
S. Esumi University of Tsukuba, Tsukuba, Japan
D. Evans School of Physics and Astronomy, University of Birmingham, Birmingham, United Kingdom
S. Evdokimov Institute for High Energy Physics, Protvino, Russia
G. Eyyubova Department of Physics, University of Oslo, Oslo, Norway
D. Fabris Dipartimento di Fisica e Astronomia dell’Università and Sezione INFN, Padova, Italy Sezione INFN, Padova, Italy
J. Faivre Laboratoire de Physique Subatomique et de Cosmologie (LPSC), Université Joseph Fourier, CNRS-IN2P3, Institut Polytechnique de Grenoble, Grenoble, France
D. Falchieri Dipartimento di Fisica e Astronomia dell’Università and Sezione INFN, Bologna, Italy
A. Fantoni Laboratori Nazionali di Frascati, INFN, Frascati, Italy
M. Fasel Physikalisches Institut, Ruprecht-Karls-Universität Heidelberg, Heidelberg, Germany
D. Fehlker Department of Physics and Technology, University of Bergen, Bergen, Norway
L. Feldkamp Institut für Kernphysik, Westfälische Wilhelms-Universität Münster, Münster, Germany
D. Felea Institute of Space Sciences (ISS), Bucharest, Romania
A. Feliciello Sezione INFN, Turin, Italy
B. Fenton-Olsen Lawrence Berkeley National Laboratory, Berkeley, California United States
G. Feofilov V. Fock Institute for Physics, St. Petersburg State University, St. Petersburg, Russia
A. Fernández Téllez Benemérita Universidad Autónoma de Puebla, Puebla, Mexico
A. Ferretti Dipartimento di Fisica dell’Università and Sezione INFN, Turin, Italy
A. Festanti Dipartimento di Fisica e Astronomia dell’Università and Sezione INFN, Padova, Italy
J. Figiel The Henryk Niewodniczanski Institute of Nuclear Physics, Polish Academy of Sciences, Cracow, Poland
M. A. S. Figueredo Universidade de São Paulo (USP), São Paulo, Brazil
S. Filchagin Russian Federal Nuclear Center (VNIIEF), Sarov, Russia
D. Finogeev Institute for Nuclear Research, Academy of Sciences, Moscow, Russia
F. M. Fionda Dipartimento Interateneo di Fisica ‘M. Merlin’ and Sezione INFN, Bari, Italy
E. M. Fiore Dipartimento Interateneo di Fisica ‘M. Merlin’ and Sezione INFN, Bari, Italy
E. Floratos Physics Department, University of Athens, Athens, Greece
M. Floris European Organization for Nuclear Research (CERN), Geneva, Switzerland
S. Foertsch Physics Department, University of Cape Town and iThemba LABS, National Research Foundation, Somerset West, South Africa
P. Foka Research Division and ExtreMe Matter Institute EMMI, GSI Helmholtzzentrum für Schwerionenforschung, Darmstadt, Germany
S. Fokin Russian Research Centre Kurchatov Institute, Moscow, Russia
E. Fragiacomo Sezione INFN, Trieste, Italy
A. Francescon Dipartimento di Fisica e Astronomia dell’Università and Sezione INFN, Padova, Italy European Organization for Nuclear Research (CERN), Geneva, Switzerland
U. Frankenfeld Research Division and ExtreMe Matter Institute EMMI, GSI Helmholtzzentrum für Schwerionenforschung, Darmstadt, Germany
U. Fuchs European Organization for Nuclear Research (CERN), Geneva, Switzerland
C. Furget Laboratoire de Physique Subatomique et de Cosmologie (LPSC), Université Joseph Fourier, CNRS-IN2P3, Institut Polytechnique de Grenoble, Grenoble, France
M. Fusco Girard Dipartimento di Fisica ‘E.R. Caianiello’ dell’Università and Gruppo Collegato INFN, Salerno, Italy
J. J. Gaardhøje Niels Bohr Institute, University of Copenhagen, Copenhagen, Denmark
M. Gagliardi Dipartimento di Fisica dell’Università and Sezione INFN, Turin, Italy
A. Gago Sección Física, Departamento de Ciencias, Pontificia Universidad Católica del Perú, Lima, Peru
M. Gallio Dipartimento di Fisica dell’Università and Sezione INFN, Turin, Italy
D. R. Gangadharan Department of Physics, Ohio State University, Columbus, Ohio United States
P. Ganoti Oak Ridge National Laboratory, Oak Ridge, Tennessee United States
C. Garabatos Research Division and ExtreMe Matter Institute EMMI, GSI Helmholtzzentrum für Schwerionenforschung, Darmstadt, Germany
E. Garcia-Solis Chicago State University, Chicago, United States
C. Gargiulo European Organization for Nuclear Research (CERN), Geneva, Switzerland
I. Garishvili Lawrence Livermore National Laboratory, Livermore, California United States
J. Gerhard Frankfurt Institute for Advanced Studies, Johann Wolfgang Goethe-Universität Frankfurt, Frankfurt, Germany
M. Germain SUBATECH, Ecole des Mines de Nantes, Université de Nantes, CNRS-IN2P3, Nantes, France
C. Geuna Commissariat à l’Energie Atomique, IRFU, Saclay, France
M. Gheata European Organization for Nuclear Research (CERN), Geneva, Switzerland Institute of Space Sciences (ISS), Bucharest, Romania
A. Gheata European Organization for Nuclear Research (CERN), Geneva, Switzerland
B. Ghidini Dipartimento Interateneo di Fisica ‘M. Merlin’ and Sezione INFN, Bari, Italy
P. Ghosh Variable Energy Cyclotron Centre, Kolkata, India
P. Gianotti Laboratori Nazionali di Frascati, INFN, Frascati, Italy
P. Giubellino European Organization for Nuclear Research (CERN), Geneva, Switzerland
E. Gladysz-Dziadus The Henryk Niewodniczanski Institute of Nuclear Physics, Polish Academy of Sciences, Cracow, Poland
P. Glässel Physikalisches Institut, Ruprecht-Karls-Universität Heidelberg, Heidelberg, Germany
R. Gomez Centro de Investigación y de Estudios Avanzados (CINVESTAV), Mexico City and Mérida, Mexico Universidad Autónoma de Sinaloa, Culiacán, Mexico
E. G. Ferreiro Departamento de Física de Partículas and IGFAE, Universidad de Santiago de Compostela, Santiago de Compostela, Spain
L. H. González-Trueba Instituto de Física, Universidad Nacional Autónoma de México, Mexico City, Mexico
P. González-Zamora Centro de Investigaciones Energéticas Medioambientales y Tecnológicas (CIEMAT), Madrid, Spain
S. Gorbunov Frankfurt Institute for Advanced Studies, Johann Wolfgang Goethe-Universität Frankfurt, Frankfurt, Germany
A. Goswami Physics Department, University of Rajasthan, Jaipur, India
S. Gotovac Technical University of Split FESB, Split, Croatia
L. K. Graczykowski Warsaw University of Technology, Warsaw, Poland
R. Grajcarek Physikalisches Institut, Ruprecht-Karls-Universität Heidelberg, Heidelberg, Germany
A. Grelli Nikhef, National Institute for Subatomic Physics and Institute for Subatomic Physics of Utrecht University, Utrecht, Netherlands
C. Grigoras European Organization for Nuclear Research (CERN), Geneva, Switzerland
A. Grigoras European Organization for Nuclear Research (CERN), Geneva, Switzerland
V. Grigoriev Moscow Engineering Physics Institute, Moscow, Russia
A. Grigoryan A. I. Alikhanyan National Science Laboratory (Yerevan Physics Institute) Foundation, Yerevan, Armenia
S. Grigoryan Joint Institute for Nuclear Research (JINR), Dubna, Russia
B. Grinyov Bogolyubov Institute for Theoretical Physics, Kiev, Ukraine
N. Grion Sezione INFN, Trieste, Italy
P. Gros Division of Experimental High Energy Physics, University of Lund, Lund, Sweden
J. F. Grosse-Oetringhaus European Organization for Nuclear Research (CERN), Geneva, Switzerland
J.-Y. Grossiord Université de Lyon, Université Lyon 1, CNRS/IN2P3, IPN-Lyon, Villeurbanne, France
R. Grosso European Organization for Nuclear Research (CERN), Geneva, Switzerland
F. Guber Institute for Nuclear Research, Academy of Sciences, Moscow, Russia
R. Guernane Laboratoire de Physique Subatomique et de Cosmologie (LPSC), Université Joseph Fourier, CNRS-IN2P3, Institut Polytechnique de Grenoble, Grenoble, France
B. Guerzoni Dipartimento di Fisica e Astronomia dell’Università and Sezione INFN, Bologna, Italy
M. Guilbaud Université de Lyon, Université Lyon 1, CNRS/IN2P3, IPN-Lyon, Villeurbanne, France
K. Gulbrandsen Niels Bohr Institute, University of Copenhagen, Copenhagen, Denmark
H. Gulkanyan A. I. Alikhanyan National Science Laboratory (Yerevan Physics Institute) Foundation, Yerevan, Armenia
T. Gunji University of Tokyo, Tokyo, Japan
A. Gupta Physics Department, University of Jammu, Jammu, India
R. Gupta Physics Department, University of Jammu, Jammu, India
R. Haake Institut für Kernphysik, Westfälische Wilhelms-Universität Münster, Münster, Germany
Ø. Haaland Department of Physics and Technology, University of Bergen, Bergen, Norway
C. Hadjidakis Institut de Physique Nucléaire d’Orsay (IPNO), Université Paris-Sud, CNRS-IN2P3, Orsay, France
M. Haiduc Institute of Space Sciences (ISS), Bucharest, Romania
H. Hamagaki University of Tokyo, Tokyo, Japan
G. Hamar Wigner Research Centre for Physics, Hungarian Academy of Sciences, Budapest, Hungary
B. H. Han Department of Physics, Sejong University, Seoul, South Korea
L. D. Hanratty School of Physics and Astronomy, University of Birmingham, Birmingham, United Kingdom
A. Hansen Niels Bohr Institute, University of Copenhagen, Copenhagen, Denmark
Z. Harmanová-Tóthová Faculty of Science, P.J. Šafárik University, Košice, Slovakia
J. W. Harris Yale University, New Haven, Connecticut United States
M. Hartig Institut für Kernphysik, Johann Wolfgang Goethe-Universität Frankfurt, Frankfurt, Germany
A. Harton Chicago State University, Chicago, United States
D. Hatzifotiadou Sezione INFN, Bologna, Italy
S. Hayashi University of Tokyo, Tokyo, Japan
A. Hayrapetyan A. I. Alikhanyan National Science Laboratory (Yerevan Physics Institute) Foundation, Yerevan, Armenia European Organization for Nuclear Research (CERN), Geneva, Switzerland
S. T. Heckel Institut für Kernphysik, Johann Wolfgang Goethe-Universität Frankfurt, Frankfurt, Germany
M. Heide Institut für Kernphysik, Westfälische Wilhelms-Universität Münster, Münster, Germany
H. Helstrup Faculty of Engineering, Bergen University College, Bergen, Norway
A. Herghelegiu National Institute for Physics and Nuclear Engineering, Bucharest, Romania
G. Herrera Corral Centro de Investigación y de Estudios Avanzados (CINVESTAV), Mexico City and Mérida, Mexico
N. Herrmann Physikalisches Institut, Ruprecht-Karls-Universität Heidelberg, Heidelberg, Germany
B. A. Hess Eberhard Karls Universität Tübingen, Tübingen, Germany
K. F. Hetland Faculty of Engineering, Bergen University College, Bergen, Norway
B. Hicks Yale University, New Haven, Connecticut United States
B. Hippolyte Institut Pluridisciplinaire Hubert Curien (IPHC), Université de Strasbourg, CNRS-IN2P3, Strasbourg, France
Y. Hori University of Tokyo, Tokyo, Japan
P. Hristov European Organization for Nuclear Research (CERN), Geneva, Switzerland
I. Hřivnáčová Institut de Physique Nucléaire d’Orsay (IPNO), Université Paris-Sud, CNRS-IN2P3, Orsay, France
M. Huang Department of Physics and Technology, University of Bergen, Bergen, Norway
T. J. Humanic Department of Physics, Ohio State University, Columbus, Ohio United States
D. S. Hwang Department of Physics, Sejong University, Seoul, South Korea
R. Ichou Laboratoire de Physique Corpusculaire (LPC), Clermont Université, Université Blaise Pascal, CNRS–IN2P3, Clermont-Ferrand, France
R. Ilkaev Russian Federal Nuclear Center (VNIIEF), Sarov, Russia
I. Ilkiv National Centre for Nuclear Studies, Warsaw, Poland
M. Inaba University of Tsukuba, Tsukuba, Japan
E. Incani Dipartimento di Fisica dell’Università and Sezione INFN, Cagliari, Italy
G. M. Innocenti Dipartimento di Fisica dell’Università and Sezione INFN, Turin, Italy
P. G. Innocenti European Organization for Nuclear Research (CERN), Geneva, Switzerland
M. Ippolitov Russian Research Centre Kurchatov Institute, Moscow, Russia
M. Irfan Department of Physics, Aligarh Muslim University, Aligarh, India
C. Ivan Research Division and ExtreMe Matter Institute EMMI, GSI Helmholtzzentrum für Schwerionenforschung, Darmstadt, Germany
M. Ivanov Research Division and ExtreMe Matter Institute EMMI, GSI Helmholtzzentrum für Schwerionenforschung, Darmstadt, Germany
A. Ivanov V. Fock Institute for Physics, St. Petersburg State University, St. Petersburg, Russia
V. Ivanov Petersburg Nuclear Physics Institute, Gatchina, Russia
O. Ivanytskyi Bogolyubov Institute for Theoretical Physics, Kiev, Ukraine
A. Jachołkowski Dipartimento di Fisica e Astronomia dell’Università and Sezione INFN, Catania, Italy
P. M. Jacobs Lawrence Berkeley National Laboratory, Berkeley, California United States
C. Jahnke Universidade de São Paulo (USP), São Paulo, Brazil
H. J. Jang Korea Institute of Science and Technology Information, Daejeon, South Korea
M. A. Janik Warsaw University of Technology, Warsaw, Poland
P. H. S. Y. Jayarathna University of Houston, Houston, Texas United States
S. Jena Indian Institute of Technology Bombay (IIT), Mumbai, India
D. M. Jha Wayne State University, Detroit, Michigan United States
R. T. Jimenez Bustamante Instituto de Ciencias Nucleares, Universidad Nacional Autónoma de México, Mexico City, Mexico
P. G. Jones School of Physics and Astronomy, University of Birmingham, Birmingham, United Kingdom
H. Jung Gangneung-Wonju National University, Gangneung, South Korea
A. Jusko School of Physics and Astronomy, University of Birmingham, Birmingham, United Kingdom
A. B. Kaidalov Institute for Theoretical and Experimental Physics, Moscow, Russia
S. Kalcher Frankfurt Institute for Advanced Studies, Johann Wolfgang Goethe-Universität Frankfurt, Frankfurt, Germany
P. Kaliňák Institute of Experimental Physics, Slovak Academy of Sciences, Košice, Slovakia
T. Kalliokoski Helsinki Institute of Physics (HIP) and University of Jyväskylä, Jyväskylä, Finland
A. Kalweit European Organization for Nuclear Research (CERN), Geneva, Switzerland
J. H. Kang Yonsei University, Seoul, South Korea
V. Kaplin Moscow Engineering Physics Institute, Moscow, Russia
S. Kar Variable Energy Cyclotron Centre, Kolkata, India
A. Karasu Uysal European Organization for Nuclear Research (CERN), Geneva, Switzerland KTO Karatay University, Konya, Turkey Yildiz Technical University, Istanbul, Turkey
O. Karavichev Institute for Nuclear Research, Academy of Sciences, Moscow, Russia
T. Karavicheva Institute for Nuclear Research, Academy of Sciences, Moscow, Russia
E. Karpechev Institute for Nuclear Research, Academy of Sciences, Moscow, Russia
A. Kazantsev Russian Research Centre Kurchatov Institute, Moscow, Russia
U. Kebschull Institut für Informatik, Johann Wolfgang Goethe-Universität Frankfurt, Frankfurt, Germany
R. Keidel Zentrum für Technologietransfer und Telekommunikation (ZTT), Fachhochschule Worms, Worms, Germany
B. Ketzer Institut für Kernphysik, Johann Wolfgang Goethe-Universität Frankfurt, Frankfurt, Germany Technische Universität München, Munich, Germany
M. M. Khan Department of Physics, Aligarh Muslim University, Aligarh, India
P. Khan Saha Institute of Nuclear Physics, Kolkata, India
S. A. Khan Variable Energy Cyclotron Centre, Kolkata, India
K. H. Khan COMSATS Institute of Information Technology (CIIT), Islamabad, Pakistan
A. Khanzadeev Petersburg Nuclear Physics Institute, Gatchina, Russia
Y. Kharlov Institute for High Energy Physics, Protvino, Russia
B. Kileng Faculty of Engineering, Bergen University College, Bergen, Norway
M. Kim Yonsei University, Seoul, South Korea
T. Kim Yonsei University, Seoul, South Korea
B. Kim Yonsei University, Seoul, South Korea
S. Kim Department of Physics, Sejong University, Seoul, South Korea
M. Kim Gangneung-Wonju National University, Gangneung, South Korea
D. J. Kim Helsinki Institute of Physics (HIP) and University of Jyväskylä, Jyväskylä, Finland
J. S. Kim Gangneung-Wonju National University, Gangneung, South Korea
J. H. Kim Department of Physics, Sejong University, Seoul, South Korea
D. W. Kim Gangneung-Wonju National University, Gangneung, South Korea Korea Institute of Science and Technology Information, Daejeon, South Korea
S. Kirsch Frankfurt Institute for Advanced Studies, Johann Wolfgang Goethe-Universität Frankfurt, Frankfurt, Germany
I. Kisel Frankfurt Institute for Advanced Studies, Johann Wolfgang Goethe-Universität Frankfurt, Frankfurt, Germany
S. Kiselev Institute for Theoretical and Experimental Physics, Moscow, Russia
A. Kisiel Warsaw University of Technology, Warsaw, Poland
J. L. Klay California Polytechnic State University, San Luis Obispo, California United States
J. Klein Physikalisches Institut, Ruprecht-Karls-Universität Heidelberg, Heidelberg, Germany
C. Klein-Bösing Institut für Kernphysik, Westfälische Wilhelms-Universität Münster, Münster, Germany
M. Kliemant Institut für Kernphysik, Johann Wolfgang Goethe-Universität Frankfurt, Frankfurt, Germany
A. Kluge European Organization for Nuclear Research (CERN), Geneva, Switzerland
M. L. Knichel Research Division and ExtreMe Matter Institute EMMI, GSI Helmholtzzentrum für Schwerionenforschung, Darmstadt, Germany
A. G. Knospe Physics Department, The University of Texas at Austin, Austin, TX United States
M. K. Köhler Research Division and ExtreMe Matter Institute EMMI, GSI Helmholtzzentrum für Schwerionenforschung, Darmstadt, Germany
T. Kollegger Frankfurt Institute for Advanced Studies, Johann Wolfgang Goethe-Universität Frankfurt, Frankfurt, Germany
A. Kolojvari V. Fock Institute for Physics, St. Petersburg State University, St. Petersburg, Russia
M. Kompaniets V. Fock Institute for Physics, St. Petersburg State University, St. Petersburg, Russia
V. Kondratiev V. Fock Institute for Physics, St. Petersburg State University, St. Petersburg, Russia
N. Kondratyeva Moscow Engineering Physics Institute, Moscow, Russia
A. Konevskikh Institute for Nuclear Research, Academy of Sciences, Moscow, Russia
V. Kovalenko V. Fock Institute for Physics, St. Petersburg State University, St. Petersburg, Russia
M. Kowalski The Henryk Niewodniczanski Institute of Nuclear Physics, Polish Academy of Sciences, Cracow, Poland
S. Kox Laboratoire de Physique Subatomique et de Cosmologie (LPSC), Université Joseph Fourier, CNRS-IN2P3, Institut Polytechnique de Grenoble, Grenoble, France
G. Koyithatta Meethaleveedu Indian Institute of Technology Bombay (IIT), Mumbai, India
J. Kral Helsinki Institute of Physics (HIP) and University of Jyväskylä, Jyväskylä, Finland
I. Králik Institute of Experimental Physics, Slovak Academy of Sciences, Košice, Slovakia
F. Kramer Institut für Kernphysik, Johann Wolfgang Goethe-Universität Frankfurt, Frankfurt, Germany
A. Kravčáková Faculty of Science, P.J. Šafárik University, Košice, Slovakia
M. Krelina Faculty of Nuclear Sciences and Physical Engineering, Czech Technical University in Prague, Prague, Czech Republic
M. Kretz Frankfurt Institute for Advanced Studies, Johann Wolfgang Goethe-Universität Frankfurt, Frankfurt, Germany
M. Krivda Institute of Experimental Physics, Slovak Academy of Sciences, Košice, Slovakia School of Physics and Astronomy, University of Birmingham, Birmingham, United Kingdom
F. Krizek Helsinki Institute of Physics (HIP) and University of Jyväskylä, Jyväskylä, Finland
M. Krus Faculty of Nuclear Sciences and Physical Engineering, Czech Technical University in Prague, Prague, Czech Republic
E. Kryshen Petersburg Nuclear Physics Institute, Gatchina, Russia
M. Krzewicki Research Division and ExtreMe Matter Institute EMMI, GSI Helmholtzzentrum für Schwerionenforschung, Darmstadt, Germany
V. Kucera Nuclear Physics Institute, Academy of Sciences of the Czech Republic, Řež u Prahy, Czech Republic
Y. Kucheriaev Russian Research Centre Kurchatov Institute, Moscow, Russia
T. Kugathasan European Organization for Nuclear Research (CERN), Geneva, Switzerland
C. Kuhn Institut Pluridisciplinaire Hubert Curien (IPHC), Université de Strasbourg, CNRS-IN2P3, Strasbourg, France
P. G. Kuijer Nikhef, National Institute for Subatomic Physics, Amsterdam, Netherlands
I. Kulakov Institut für Kernphysik, Johann Wolfgang Goethe-Universität Frankfurt, Frankfurt, Germany
J. Kumar Indian Institute of Technology Bombay (IIT), Mumbai, India
P. Kurashvili National Centre for Nuclear Studies, Warsaw, Poland
A. Kurepin Institute for Nuclear Research, Academy of Sciences, Moscow, Russia
A. B. Kurepin Institute for Nuclear Research, Academy of Sciences, Moscow, Russia
A. Kuryakin Russian Federal Nuclear Center (VNIIEF), Sarov, Russia
V. Kushpil Nuclear Physics Institute, Academy of Sciences of the Czech Republic, Řež u Prahy, Czech Republic
S. Kushpil Nuclear Physics Institute, Academy of Sciences of the Czech Republic, Řež u Prahy, Czech Republic
H. Kvaerno Department of Physics, University of Oslo, Oslo, Norway
M. J. Kweon Physikalisches Institut, Ruprecht-Karls-Universität Heidelberg, Heidelberg, Germany
Y. Kwon Yonsei University, Seoul, South Korea
P. Ladrón de Guevara Instituto de Ciencias Nucleares, Universidad Nacional Autónoma de México, Mexico City, Mexico
C. Lagana Fernandes Universidade de São Paulo (USP), São Paulo, Brazil
I. Lakomov Institut de Physique Nucléaire d’Orsay (IPNO), Université Paris-Sud, CNRS-IN2P3, Orsay, France
R. Langoy Department of Physics and Technology, University of Bergen, Bergen, Norway Vestfold University College, Tonsberg, Norway
S. L. La Pointe Nikhef, National Institute for Subatomic Physics and Institute for Subatomic Physics of Utrecht University, Utrecht, Netherlands
C. Lara Institut für Informatik, Johann Wolfgang Goethe-Universität Frankfurt, Frankfurt, Germany
A. Lardeux SUBATECH, Ecole des Mines de Nantes, Université de Nantes, CNRS-IN2P3, Nantes, France
P. La Rocca Dipartimento di Fisica e Astronomia dell’Università and Sezione INFN, Catania, Italy
R. Lea Dipartimento di Fisica dell’Università and Sezione INFN, Trieste, Italy
M. Lechman European Organization for Nuclear Research (CERN), Geneva, Switzerland
S. C. Lee Gangneung-Wonju National University, Gangneung, South Korea
G. R. Lee School of Physics and Astronomy, University of Birmingham, Birmingham, United Kingdom
I. Legrand European Organization for Nuclear Research (CERN), Geneva, Switzerland
J. Lehnert Institut für Kernphysik, Johann Wolfgang Goethe-Universität Frankfurt, Frankfurt, Germany
R. C. Lemmon Nuclear Physics Group, STFC Daresbury Laboratory, Daresbury, United Kingdom
M. Lenhardt Research Division and ExtreMe Matter Institute EMMI, GSI Helmholtzzentrum für Schwerionenforschung, Darmstadt, Germany
V. Lenti Sezione INFN, Bari, Italy
H. León Instituto de Física, Universidad Nacional Autónoma de México, Mexico City, Mexico
M. Leoncino Dipartimento di Fisica dell’Università and Sezione INFN, Turin, Italy
I. León Monzón Universidad Autónoma de Sinaloa, Culiacán, Mexico
P. Lévai Wigner Research Centre for Physics, Hungarian Academy of Sciences, Budapest, Hungary
S. Li Central China Normal University, Wuhan, China Laboratoire de Physique Corpusculaire (LPC), Clermont Université, Université Blaise Pascal, CNRS–IN2P3, Clermont-Ferrand, France
J. Lien Department of Physics and Technology, University of Bergen, Bergen, Norway Vestfold University College, Tonsberg, Norway
R. Lietava School of Physics and Astronomy, University of Birmingham, Birmingham, United Kingdom
S. Lindal Department of Physics, University of Oslo, Oslo, Norway
V. Lindenstruth Frankfurt Institute for Advanced Studies, Johann Wolfgang Goethe-Universität Frankfurt, Frankfurt, Germany
C. Lippmann European Organization for Nuclear Research (CERN), Geneva, Switzerland Research Division and ExtreMe Matter Institute EMMI, GSI Helmholtzzentrum für Schwerionenforschung, Darmstadt, Germany
M. A. Lisa Department of Physics, Ohio State University, Columbus, Ohio United States
H. M. Ljunggren Division of Experimental High Energy Physics, University of Lund, Lund, Sweden
D. F. Lodato Nikhef, National Institute for Subatomic Physics and Institute for Subatomic Physics of Utrecht University, Utrecht, Netherlands
P. I. Loenne Department of Physics and Technology, University of Bergen, Bergen, Norway
V. R. Loggins Wayne State University, Detroit, Michigan United States
V. Loginov Moscow Engineering Physics Institute, Moscow, Russia
D. Lohner Physikalisches Institut, Ruprecht-Karls-Universität Heidelberg, Heidelberg, Germany
C. Loizides Lawrence Berkeley National Laboratory, Berkeley, California United States
K. K. Loo Helsinki Institute of Physics (HIP) and University of Jyväskylä, Jyväskylä, Finland
X. Lopez Laboratoire de Physique Corpusculaire (LPC), Clermont Université, Université Blaise Pascal, CNRS–IN2P3, Clermont-Ferrand, France
E. López Torres Centro de Aplicaciones Tecnológicas y Desarrollo Nuclear (CEADEN), Havana, Cuba
G. Løvhøiden Department of Physics, University of Oslo, Oslo, Norway
X.-G. Lu Physikalisches Institut, Ruprecht-Karls-Universität Heidelberg, Heidelberg, Germany
P. Luettig Institut für Kernphysik, Johann Wolfgang Goethe-Universität Frankfurt, Frankfurt, Germany
M. Lunardon Dipartimento di Fisica e Astronomia dell’Università and Sezione INFN, Padova, Italy
J. Luo Central China Normal University, Wuhan, China
G. Luparello Nikhef, National Institute for Subatomic Physics and Institute for Subatomic Physics of Utrecht University, Utrecht, Netherlands
C. Luzzi European Organization for Nuclear Research (CERN), Geneva, Switzerland
R. Ma Yale University, New Haven, Connecticut United States
K. Ma Central China Normal University, Wuhan, China
D. M. Madagodahettige-Don University of Houston, Houston, Texas United States
A. Maevskaya Institute for Nuclear Research, Academy of Sciences, Moscow, Russia
M. Mager European Organization for Nuclear Research (CERN), Geneva, Switzerland Institut für Kernphysik, Technische Universität Darmstadt, Darmstadt, Germany
D. P. Mahapatra Institute of Physics, Bhubaneswar, India
A. Maire Physikalisches Institut, Ruprecht-Karls-Universität Heidelberg, Heidelberg, Germany
M. Malaev Petersburg Nuclear Physics Institute, Gatchina, Russia
I. Maldonado Cervantes Instituto de Ciencias Nucleares, Universidad Nacional Autónoma de México, Mexico City, Mexico
L. Malinina Joint Institute for Nuclear Research (JINR), Dubna, Russia
D. Mal’Kevich Institute for Theoretical and Experimental Physics, Moscow, Russia
P. Malzacher Research Division and ExtreMe Matter Institute EMMI, GSI Helmholtzzentrum für Schwerionenforschung, Darmstadt, Germany
A. Mamonov Russian Federal Nuclear Center (VNIIEF), Sarov, Russia
L. Manceau Sezione INFN, Turin, Italy
L. Mangotra Physics Department, University of Jammu, Jammu, India
V. Manko Russian Research Centre Kurchatov Institute, Moscow, Russia
F. Manso Laboratoire de Physique Corpusculaire (LPC), Clermont Université, Université Blaise Pascal, CNRS–IN2P3, Clermont-Ferrand, France
V. Manzari Sezione INFN, Bari, Italy
Y. Mao Central China Normal University, Wuhan, China
M. Marchisone Dipartimento di Fisica dell’Università and Sezione INFN, Turin, Italy Laboratoire de Physique Corpusculaire (LPC), Clermont Université, Université Blaise Pascal, CNRS–IN2P3, Clermont-Ferrand, France
J. Mareš Institute of Physics, Academy of Sciences of the Czech Republic, Prague, Czech Republic
G. V. Margagliotti Dipartimento di Fisica dell’Università and Sezione INFN, Trieste, Italy Sezione INFN, Trieste, Italy
A. Margotti Sezione INFN, Bologna, Italy
A. Marín Research Division and ExtreMe Matter Institute EMMI, GSI Helmholtzzentrum für Schwerionenforschung, Darmstadt, Germany
C. Markert Physics Department, The University of Texas at Austin, Austin, TX United States
M. Marquard Institut für Kernphysik, Johann Wolfgang Goethe-Universität Frankfurt, Frankfurt, Germany
I. Martashvili University of Tennessee, Knoxville, Tennessee United States
N. A. Martin Research Division and ExtreMe Matter Institute EMMI, GSI Helmholtzzentrum für Schwerionenforschung, Darmstadt, Germany
P. Martinengo European Organization for Nuclear Research (CERN), Geneva, Switzerland
M. I. Martínez Benemérita Universidad Autónoma de Puebla, Puebla, Mexico
G. Martínez García SUBATECH, Ecole des Mines de Nantes, Université de Nantes, CNRS-IN2P3, Nantes, France
Y. Martynov Bogolyubov Institute for Theoretical Physics, Kiev, Ukraine
A. Mas SUBATECH, Ecole des Mines de Nantes, Université de Nantes, CNRS-IN2P3, Nantes, France
S. Masciocchi Research Division and ExtreMe Matter Institute EMMI, GSI Helmholtzzentrum für Schwerionenforschung, Darmstadt, Germany
M. Masera Dipartimento di Fisica dell’Università and Sezione INFN, Turin, Italy
A. Masoni Sezione INFN, Cagliari, Italy
L. Massacrier SUBATECH, Ecole des Mines de Nantes, Université de Nantes, CNRS-IN2P3, Nantes, France
A. Mastroserio Dipartimento Interateneo di Fisica ‘M. Merlin’ and Sezione INFN, Bari, Italy
A. Matyja The Henryk Niewodniczanski Institute of Nuclear Physics, Polish Academy of Sciences, Cracow, Poland
C. Mayer The Henryk Niewodniczanski Institute of Nuclear Physics, Polish Academy of Sciences, Cracow, Poland
J. Mazer University of Tennessee, Knoxville, Tennessee United States
R. Mazumder Indian Institute of Technology Indore (IITI), Indore, India
M. A. Mazzoni Sezione INFN, Rome, Italy
F. Meddi Dipartimento di Fisica dell’Università ‘La Sapienza’ and Sezione INFN, Rome, Italy
A. Menchaca-Rocha Instituto de Física, Universidad Nacional Autónoma de México, Mexico City, Mexico
J. Mercado Pérez Physikalisches Institut, Ruprecht-Karls-Universität Heidelberg, Heidelberg, Germany
M. Meres Faculty of Mathematics, Physics and Informatics, Comenius University, Bratislava, Slovakia
Y. Miake University of Tsukuba, Tsukuba, Japan
K. Mikhaylov Institute for Theoretical and Experimental Physics, Moscow, Russia Joint Institute for Nuclear Research (JINR), Dubna, Russia
L. Milano Dipartimento di Fisica dell’Università and Sezione INFN, Turin, Italy European Organization for Nuclear Research (CERN), Geneva, Switzerland
J. Milosevic Department of Physics, University of Oslo, Oslo, Norway
A. Mischke Nikhef, National Institute for Subatomic Physics and Institute for Subatomic Physics of Utrecht University, Utrecht, Netherlands
A. N. Mishra Indian Institute of Technology Indore (IITI), Indore, India Physics Department, University of Rajasthan, Jaipur, India
D. Miśkowiec Research Division and ExtreMe Matter Institute EMMI, GSI Helmholtzzentrum für Schwerionenforschung, Darmstadt, Germany
C. Mitu Institute of Space Sciences (ISS), Bucharest, Romania
S. Mizuno University of Tsukuba, Tsukuba, Japan
J. Mlynarz Wayne State University, Detroit, Michigan United States
B. Mohanty National Institute of Science Education and Research, Bhubaneswar, India Variable Energy Cyclotron Centre, Kolkata, India
L. Molnar Institut Pluridisciplinaire Hubert Curien (IPHC), Université de Strasbourg, CNRS-IN2P3, Strasbourg, France Wigner Research Centre for Physics, Hungarian Academy of Sciences, Budapest, Hungary
L. Montaño Zetina Centro de Investigación y de Estudios Avanzados (CINVESTAV), Mexico City and Mérida, Mexico
M. Monteno Sezione INFN, Turin, Italy
E. Montes Centro de Investigaciones Energéticas Medioambientales y Tecnológicas (CIEMAT), Madrid, Spain
T. Moon Yonsei University, Seoul, South Korea
M. Morando Dipartimento di Fisica e Astronomia dell’Università and Sezione INFN, Padova, Italy
D. A. Moreira De Godoy Universidade de São Paulo (USP), São Paulo, Brazil
S. Moretto Dipartimento di Fisica e Astronomia dell’Università and Sezione INFN, Padova, Italy
A. Morreale Helsinki Institute of Physics (HIP) and University of Jyväskylä, Jyväskylä, Finland
A. Morsch European Organization for Nuclear Research (CERN), Geneva, Switzerland
V. Muccifora Laboratori Nazionali di Frascati, INFN, Frascati, Italy
E. Mudnic Technical University of Split FESB, Split, Croatia
S. Muhuri Variable Energy Cyclotron Centre, Kolkata, India
M. Mukherjee Variable Energy Cyclotron Centre, Kolkata, India
H. Müller European Organization for Nuclear Research (CERN), Geneva, Switzerland
M. G. Munhoz Universidade de São Paulo (USP), São Paulo, Brazil
S. Murray Physics Department, University of Cape Town and iThemba LABS, National Research Foundation, Somerset West, South Africa
L. Musa European Organization for Nuclear Research (CERN), Geneva, Switzerland
J. Musinsky Institute of Experimental Physics, Slovak Academy of Sciences, Košice, Slovakia
B. K. Nandi Indian Institute of Technology Bombay (IIT), Mumbai, India
R. Nania Sezione INFN, Bologna, Italy
E. Nappi Sezione INFN, Bari, Italy
C. Nattrass University of Tennessee, Knoxville, Tennessee United States
T. K. Nayak Variable Energy Cyclotron Centre, Kolkata, India
S. Nazarenko Russian Federal Nuclear Center (VNIIEF), Sarov, Russia
A. Nedosekin Institute for Theoretical and Experimental Physics, Moscow, Russia
M. Nicassio Dipartimento Interateneo di Fisica ‘M. Merlin’ and Sezione INFN, Bari, Italy Research Division and ExtreMe Matter Institute EMMI, GSI Helmholtzzentrum für Schwerionenforschung, Darmstadt, Germany
M. Niculescu European Organization for Nuclear Research (CERN), Geneva, Switzerland Institute of Space Sciences (ISS), Bucharest, Romania
B. S. Nielsen Niels Bohr Institute, University of Copenhagen, Copenhagen, Denmark
T. Niida University of Tsukuba, Tsukuba, Japan
S. Nikolaev Russian Research Centre Kurchatov Institute, Moscow, Russia
V. Nikolic Rudjer Bošković Institute, Zagreb, Croatia
S. Nikulin Russian Research Centre Kurchatov Institute, Moscow, Russia
V. Nikulin Petersburg Nuclear Physics Institute, Gatchina, Russia
B. S. Nilsen Physics Department, Creighton University, Omaha, Nebraska United States
M. S. Nilsson Department of Physics, University of Oslo, Oslo, Norway
F. Noferini Centro Fermi - Museo Storico della Fisica e Centro Studi e Ricerche “Enrico Fermi”, Rome, Italy Sezione INFN, Bologna, Italy
P. Nomokonov Joint Institute for Nuclear Research (JINR), Dubna, Russia
G. Nooren Nikhef, National Institute for Subatomic Physics and Institute for Subatomic Physics of Utrecht University, Utrecht, Netherlands
A. Nyanin Russian Research Centre Kurchatov Institute, Moscow, Russia
A. Nyatha Indian Institute of Technology Bombay (IIT), Mumbai, India
C. Nygaard Niels Bohr Institute, University of Copenhagen, Copenhagen, Denmark
J. Nystrand Department of Physics and Technology, University of Bergen, Bergen, Norway
A. Ochirov V. Fock Institute for Physics, St. Petersburg State University, St. Petersburg, Russia
H. Oeschler European Organization for Nuclear Research (CERN), Geneva, Switzerland Institut für Kernphysik, Technische Universität Darmstadt, Darmstadt, Germany Physikalisches Institut, Ruprecht-Karls-Universität Heidelberg, Heidelberg, Germany
S. Oh Yale University, New Haven, Connecticut United States
S. K. Oh Gangneung-Wonju National University, Gangneung, South Korea
J. Oleniacz Warsaw University of Technology, Warsaw, Poland
A. C. Oliveira Da Silva Universidade de São Paulo (USP), São Paulo, Brazil
J. Onderwaater Research Division and ExtreMe Matter Institute EMMI, GSI Helmholtzzentrum für Schwerionenforschung, Darmstadt, Germany
C. Oppedisano Sezione INFN, Turin, Italy
A. Ortiz Velasquez Division of Experimental High Energy Physics, University of Lund, Lund, Sweden Instituto de Ciencias Nucleares, Universidad Nacional Autónoma de México, Mexico City, Mexico
A. Oskarsson Division of Experimental High Energy Physics, University of Lund, Lund, Sweden
P. Ostrowski Warsaw University of Technology, Warsaw, Poland
J. Otwinowski Research Division and ExtreMe Matter Institute EMMI, GSI Helmholtzzentrum für Schwerionenforschung, Darmstadt, Germany
K. Oyama Physikalisches Institut, Ruprecht-Karls-Universität Heidelberg, Heidelberg, Germany
K. Ozawa University of Tokyo, Tokyo, Japan
Y. Pachmayer Physikalisches Institut, Ruprecht-Karls-Universität Heidelberg, Heidelberg, Germany
M. Pachr Faculty of Nuclear Sciences and Physical Engineering, Czech Technical University in Prague, Prague, Czech Republic
F. Padilla Dipartimento di Fisica dell’Università and Sezione INFN, Turin, Italy
P. Pagano Dipartimento di Fisica ‘E.R. Caianiello’ dell’Università and Gruppo Collegato INFN, Salerno, Italy
G. Paić Instituto de Ciencias Nucleares, Universidad Nacional Autónoma de México, Mexico City, Mexico
F. Painke Frankfurt Institute for Advanced Studies, Johann Wolfgang Goethe-Universität Frankfurt, Frankfurt, Germany
C. Pajares Departamento de Física de Partículas and IGFAE, Universidad de Santiago de Compostela, Santiago de Compostela, Spain
S. K. Pal Variable Energy Cyclotron Centre, Kolkata, India
A. Palaha School of Physics and Astronomy, University of Birmingham, Birmingham, United Kingdom
A. Palmeri Sezione INFN, Catania, Italy
V. Papikyan A. I. Alikhanyan National Science Laboratory (Yerevan Physics Institute) Foundation, Yerevan, Armenia
G. S. Pappalardo Sezione INFN, Catania, Italy
W. J. Park Research Division and ExtreMe Matter Institute EMMI, GSI Helmholtzzentrum für Schwerionenforschung, Darmstadt, Germany
A. Passfeld Institut für Kernphysik, Westfälische Wilhelms-Universität Münster, Münster, Germany
D. I. Patalakha Institute for High Energy Physics, Protvino, Russia
V. Paticchio Sezione INFN, Bari, Italy
B. Paul Saha Institute of Nuclear Physics, Kolkata, India
A. Pavlinov Wayne State University, Detroit, Michigan United States
T. Pawlak Warsaw University of Technology, Warsaw, Poland
T. Peitzmann Nikhef, National Institute for Subatomic Physics and Institute for Subatomic Physics of Utrecht University, Utrecht, Netherlands
H. Pereira Da Costa Commissariat à l’Energie Atomique, IRFU, Saclay, France
E. Pereira De Oliveira Filho Universidade de São Paulo (USP), São Paulo, Brazil
D. Peresunko Russian Research Centre Kurchatov Institute, Moscow, Russia
C. E. Pérez Lara Nikhef, National Institute for Subatomic Physics, Amsterdam, Netherlands
D. Perrino Dipartimento Interateneo di Fisica ‘M. Merlin’ and Sezione INFN, Bari, Italy
W. Peryt Warsaw University of Technology, Warsaw, Poland
A. Pesci Sezione INFN, Bologna, Italy
Y. Pestov Budker Institute for Nuclear Physics, Novosibirsk, Russia
V. Petráček Faculty of Nuclear Sciences and Physical Engineering, Czech Technical University in Prague, Prague, Czech Republic
M. Petran Faculty of Nuclear Sciences and Physical Engineering, Czech Technical University in Prague, Prague, Czech Republic
M. Petris National Institute for Physics and Nuclear Engineering, Bucharest, Romania
P. Petrov School of Physics and Astronomy, University of Birmingham, Birmingham, United Kingdom
M. Petrovici National Institute for Physics and Nuclear Engineering, Bucharest, Romania
C. Petta Dipartimento di Fisica e Astronomia dell’Università and Sezione INFN, Catania, Italy
S. Piano Sezione INFN, Trieste, Italy
M. Pikna Faculty of Mathematics, Physics and Informatics, Comenius University, Bratislava, Slovakia
P. Pillot SUBATECH, Ecole des Mines de Nantes, Université de Nantes, CNRS-IN2P3, Nantes, France
O. Pinazza European Organization for Nuclear Research (CERN), Geneva, Switzerland
L. Pinsky University of Houston, Houston, Texas United States
N. Pitz Institut für Kernphysik, Johann Wolfgang Goethe-Universität Frankfurt, Frankfurt, Germany
D. B. Piyarathna University of Houston, Houston, Texas United States
M. Planinic Rudjer Bošković Institute, Zagreb, Croatia
M. Płoskoń Lawrence Berkeley National Laboratory, Berkeley, California United States
J. Pluta Warsaw University of Technology, Warsaw, Poland
T. Pocheptsov Joint Institute for Nuclear Research (JINR), Dubna, Russia
S. Pochybova Wigner Research Centre for Physics, Hungarian Academy of Sciences, Budapest, Hungary
P. L. M. Podesta-Lerma Universidad Autónoma de Sinaloa, Culiacán, Mexico
M. G. Poghosyan European Organization for Nuclear Research (CERN), Geneva, Switzerland
K. Polák Institute of Physics, Academy of Sciences of the Czech Republic, Prague, Czech Republic
B. Polichtchouk Institute for High Energy Physics, Protvino, Russia
N. Poljak Nikhef, National Institute for Subatomic Physics and Institute for Subatomic Physics of Utrecht University, Utrecht, Netherlands Rudjer Bošković Institute, Zagreb, Croatia
A. Pop National Institute for Physics and Nuclear Engineering, Bucharest, Romania
S. Porteboeuf-Houssais Laboratoire de Physique Corpusculaire (LPC), Clermont Université, Université Blaise Pascal, CNRS–IN2P3, Clermont-Ferrand, France
V. Pospíšil Faculty of Nuclear Sciences and Physical Engineering, Czech Technical University in Prague, Prague, Czech Republic
B. Potukuchi Physics Department, University of Jammu, Jammu, India
S. K. Prasad Wayne State University, Detroit, Michigan United States
R. Preghenella Centro Fermi - Museo Storico della Fisica e Centro Studi e Ricerche “Enrico Fermi”, Rome, Italy Sezione INFN, Bologna, Italy
F. Prino Sezione INFN, Turin, Italy
C. A. Pruneau Wayne State University, Detroit, Michigan United States
I. Pshenichnov Institute for Nuclear Research, Academy of Sciences, Moscow, Russia
G. Puddu Dipartimento di Fisica dell’Università and Sezione INFN, Cagliari, Italy
V. Punin Russian Federal Nuclear Center (VNIIEF), Sarov, Russia
J. Putschke Wayne State University, Detroit, Michigan United States
H. Qvigstad Department of Physics, University of Oslo, Oslo, Norway
A. Rachevski Sezione INFN, Trieste, Italy
A. Rademakers European Organization for Nuclear Research (CERN), Geneva, Switzerland
T. S. Räihä Helsinki Institute of Physics (HIP) and University of Jyväskylä, Jyväskylä, Finland
J. Rak Helsinki Institute of Physics (HIP) and University of Jyväskylä, Jyväskylä, Finland
A. Rakotozafindrabe Commissariat à l’Energie Atomique, IRFU, Saclay, France
L. Ramello Dipartimento di Scienze e Innovazione Tecnologica dell’Università del Piemonte Orientale and Gruppo Collegato INFN, Alessandria, Italy
S. Raniwala Physics Department, University of Rajasthan, Jaipur, India
R. Raniwala Physics Department, University of Rajasthan, Jaipur, India
S. S. Räsänen Helsinki Institute of Physics (HIP) and University of Jyväskylä, Jyväskylä, Finland
B. T. Rascanu Institut für Kernphysik, Johann Wolfgang Goethe-Universität Frankfurt, Frankfurt, Germany
D. Rathee Physics Department, Panjab University, Chandigarh, India
W. Rauch European Organization for Nuclear Research (CERN), Geneva, Switzerland
A. W. Rauf COMSATS Institute of Information Technology (CIIT), Islamabad, Pakistan
V. Razazi Dipartimento di Fisica dell’Università and Sezione INFN, Cagliari, Italy
K. F. Read University of Tennessee, Knoxville, Tennessee United States
J. S. Real Laboratoire de Physique Subatomique et de Cosmologie (LPSC), Université Joseph Fourier, CNRS-IN2P3, Institut Polytechnique de Grenoble, Grenoble, France
K. Redlich National Centre for Nuclear Studies, Warsaw, Poland
R. J. Reed Yale University, New Haven, Connecticut United States
A. Rehman Department of Physics and Technology, University of Bergen, Bergen, Norway
P. Reichelt Institut für Kernphysik, Johann Wolfgang Goethe-Universität Frankfurt, Frankfurt, Germany
M. Reicher Nikhef, National Institute for Subatomic Physics and Institute for Subatomic Physics of Utrecht University, Utrecht, Netherlands
R. Renfordt Institut für Kernphysik, Johann Wolfgang Goethe-Universität Frankfurt, Frankfurt, Germany
A. R. Reolon Laboratori Nazionali di Frascati, INFN, Frascati, Italy
A. Reshetin Institute for Nuclear Research, Academy of Sciences, Moscow, Russia
F. Rettig Frankfurt Institute for Advanced Studies, Johann Wolfgang Goethe-Universität Frankfurt, Frankfurt, Germany
J.-P. Revol European Organization for Nuclear Research (CERN), Geneva, Switzerland
K. Reygers Physikalisches Institut, Ruprecht-Karls-Universität Heidelberg, Heidelberg, Germany
L. Riccati Sezione INFN, Turin, Italy
R. A. Ricci Laboratori Nazionali di Legnaro, INFN, Legnaro, Italy
T. Richert Division of Experimental High Energy Physics, University of Lund, Lund, Sweden
M. Richter Department of Physics, University of Oslo, Oslo, Norway
P. Riedler European Organization for Nuclear Research (CERN), Geneva, Switzerland
W. Riegler European Organization for Nuclear Research (CERN), Geneva, Switzerland
F. Riggi Dipartimento di Fisica e Astronomia dell’Università and Sezione INFN, Catania, Italy Sezione INFN, Catania, Italy
A. Rivetti Sezione INFN, Turin, Italy
M. Rodríguez Cahuantzi Benemérita Universidad Autónoma de Puebla, Puebla, Mexico
A. Rodriguez Manso Nikhef, National Institute for Subatomic Physics, Amsterdam, Netherlands
K. Røed Department of Physics and Technology, University of Bergen, Bergen, Norway Department of Physics, University of Oslo, Oslo, Norway
E. Rogochaya Joint Institute for Nuclear Research (JINR), Dubna, Russia
D. Rohr Frankfurt Institute for Advanced Studies, Johann Wolfgang Goethe-Universität Frankfurt, Frankfurt, Germany
D. Röhrich Department of Physics and Technology, University of Bergen, Bergen, Norway
R. Romita Research Division and ExtreMe Matter Institute EMMI, GSI Helmholtzzentrum für Schwerionenforschung, Darmstadt, Germany Nuclear Physics Group, STFC Daresbury Laboratory, Daresbury, United Kingdom
F. Ronchetti Laboratori Nazionali di Frascati, INFN, Frascati, Italy
P. Rosnet Laboratoire de Physique Corpusculaire (LPC), Clermont Université, Université Blaise Pascal, CNRS–IN2P3, Clermont-Ferrand, France
S. Rossegger European Organization for Nuclear Research (CERN), Geneva, Switzerland
A. Rossi European Organization for Nuclear Research (CERN), Geneva, Switzerland
P. Roy Saha Institute of Nuclear Physics, Kolkata, India
C. Roy Institut Pluridisciplinaire Hubert Curien (IPHC), Université de Strasbourg, CNRS-IN2P3, Strasbourg, France
A. J. Rubio Montero Centro de Investigaciones Energéticas Medioambientales y Tecnológicas (CIEMAT), Madrid, Spain
R. Rui Dipartimento di Fisica dell’Università and Sezione INFN, Trieste, Italy
R. Russo Dipartimento di Fisica dell’Università and Sezione INFN, Turin, Italy
E. Ryabinkin Russian Research Centre Kurchatov Institute, Moscow, Russia
A. Rybicki The Henryk Niewodniczanski Institute of Nuclear Physics, Polish Academy of Sciences, Cracow, Poland
S. Sadovsky Institute for High Energy Physics, Protvino, Russia
K. Šafařík European Organization for Nuclear Research (CERN), Geneva, Switzerland
R. Sahoo Indian Institute of Technology Indore (IITI), Indore, India
P. K. Sahu Institute of Physics, Bhubaneswar, India
J. Saini Variable Energy Cyclotron Centre, Kolkata, India
H. Sakaguchi Hiroshima University, Hiroshima, Japan
S. Sakai Lawrence Berkeley National Laboratory, Berkeley, California United States
D. Sakata University of Tsukuba, Tsukuba, Japan
C. A. Salgado Departamento de Física de Partículas and IGFAE, Universidad de Santiago de Compostela, Santiago de Compostela, Spain
J. Salzwedel Department of Physics, Ohio State University, Columbus, Ohio United States
S. Sambyal Physics Department, University of Jammu, Jammu, India
V. Samsonov Petersburg Nuclear Physics Institute, Gatchina, Russia
X. Sanchez Castro Institut Pluridisciplinaire Hubert Curien (IPHC), Université de Strasbourg, CNRS-IN2P3, Strasbourg, France
L. Šándor Institute of Experimental Physics, Slovak Academy of Sciences, Košice, Slovakia
A. Sandoval Instituto de Física, Universidad Nacional Autónoma de México, Mexico City, Mexico
M. Sano University of Tsukuba, Tsukuba, Japan
G. Santagati Dipartimento di Fisica e Astronomia dell’Università and Sezione INFN, Catania, Italy
R. Santoro Centro Fermi - Museo Storico della Fisica e Centro Studi e Ricerche “Enrico Fermi”, Rome, Italy European Organization for Nuclear Research (CERN), Geneva, Switzerland
J. Sarkamo Helsinki Institute of Physics (HIP) and University of Jyväskylä, Jyväskylä, Finland
D. Sarkar Variable Energy Cyclotron Centre, Kolkata, India
E. Scapparone Sezione INFN, Bologna, Italy
F. Scarlassara Dipartimento di Fisica e Astronomia dell’Università and Sezione INFN, Padova, Italy
R. P. Scharenberg Purdue University, West Lafayette, Indiana United States
C. Schiaua National Institute for Physics and Nuclear Engineering, Bucharest, Romania
R. Schicker Physikalisches Institut, Ruprecht-Karls-Universität Heidelberg, Heidelberg, Germany
H. R. Schmidt Eberhard Karls Universität Tübingen, Tübingen, Germany
C. Schmidt Research Division and ExtreMe Matter Institute EMMI, GSI Helmholtzzentrum für Schwerionenforschung, Darmstadt, Germany
S. Schuchmann Institut für Kernphysik, Johann Wolfgang Goethe-Universität Frankfurt, Frankfurt, Germany
J. Schukraft European Organization for Nuclear Research (CERN), Geneva, Switzerland
T. Schuster Yale University, New Haven, Connecticut United States
Y. Schutz European Organization for Nuclear Research (CERN), Geneva, Switzerland SUBATECH, Ecole des Mines de Nantes, Université de Nantes, CNRS-IN2P3, Nantes, France
K. Schwarz Research Division and ExtreMe Matter Institute EMMI, GSI Helmholtzzentrum für Schwerionenforschung, Darmstadt, Germany
K. Schweda Research Division and ExtreMe Matter Institute EMMI, GSI Helmholtzzentrum für Schwerionenforschung, Darmstadt, Germany
G. Scioli Dipartimento di Fisica e Astronomia dell’Università and Sezione INFN, Bologna, Italy
E. Scomparin Sezione INFN, Turin, Italy
R. Scott University of Tennessee, Knoxville, Tennessee United States
P. A. Scott School of Physics and Astronomy, University of Birmingham, Birmingham, United Kingdom
G. Segato Dipartimento di Fisica e Astronomia dell’Università and Sezione INFN, Padova, Italy
I. Selyuzhenkov Research Division and ExtreMe Matter Institute EMMI, GSI Helmholtzzentrum für Schwerionenforschung, Darmstadt, Germany
S. Senyukov Institut Pluridisciplinaire Hubert Curien (IPHC), Université de Strasbourg, CNRS-IN2P3, Strasbourg, France
J. Seo Pusan National University, Pusan, South Korea
S. Serci Dipartimento di Fisica dell’Università and Sezione INFN, Cagliari, Italy
E. Serradilla Centro de Investigaciones Energéticas Medioambientales y Tecnológicas (CIEMAT), Madrid, Spain Instituto de Física, Universidad Nacional Autónoma de México, Mexico City, Mexico
A. Sevcenco Institute of Space Sciences (ISS), Bucharest, Romania
A. Shabetai SUBATECH, Ecole des Mines de Nantes, Université de Nantes, CNRS-IN2P3, Nantes, France
G. Shabratova Joint Institute for Nuclear Research (JINR), Dubna, Russia
R. Shahoyan European Organization for Nuclear Research (CERN), Geneva, Switzerland
S. Sharma Physics Department, University of Jammu, Jammu, India
N. Sharma University of Tennessee, Knoxville, Tennessee United States
S. Rohni Physics Department, University of Jammu, Jammu, India
K. Shigaki Hiroshima University, Hiroshima, Japan
K. Shtejer Centro de Aplicaciones Tecnológicas y Desarrollo Nuclear (CEADEN), Havana, Cuba
Y. Sibiriak Russian Research Centre Kurchatov Institute, Moscow, Russia
E. Sicking Institut für Kernphysik, Westfälische Wilhelms-Universität Münster, Münster, Germany
S. Siddhanta Sezione INFN, Cagliari, Italy
T. Siemiarczuk National Centre for Nuclear Studies, Warsaw, Poland
D. Silvermyr Oak Ridge National Laboratory, Oak Ridge, Tennessee United States
C. Silvestre Laboratoire de Physique Subatomique et de Cosmologie (LPSC), Université Joseph Fourier, CNRS-IN2P3, Institut Polytechnique de Grenoble, Grenoble, France
G. Simatovic Instituto de Ciencias Nucleares, Universidad Nacional Autónoma de México, Mexico City, Mexico Rudjer Bošković Institute, Zagreb, Croatia
G. Simonetti European Organization for Nuclear Research (CERN), Geneva, Switzerland
R. Singaraju Variable Energy Cyclotron Centre, Kolkata, India
R. Singh Physics Department, University of Jammu, Jammu, India
S. Singha National Institute of Science Education and Research, Bhubaneswar, India Variable Energy Cyclotron Centre, Kolkata, India
V. Singhal Variable Energy Cyclotron Centre, Kolkata, India
T. Sinha Saha Institute of Nuclear Physics, Kolkata, India
B. C. Sinha Variable Energy Cyclotron Centre, Kolkata, India
B. Sitar Faculty of Mathematics, Physics and Informatics, Comenius University, Bratislava, Slovakia
M. Sitta Dipartimento di Scienze e Innovazione Tecnologica dell’Università del Piemonte Orientale and Gruppo Collegato INFN, Alessandria, Italy
T. B. Skaali Department of Physics, University of Oslo, Oslo, Norway
K. Skjerdal Department of Physics and Technology, University of Bergen, Bergen, Norway
R. Smakal Faculty of Nuclear Sciences and Physical Engineering, Czech Technical University in Prague, Prague, Czech Republic
N. Smirnov Yale University, New Haven, Connecticut United States
R. J. M. Snellings Nikhef, National Institute for Subatomic Physics and Institute for Subatomic Physics of Utrecht University, Utrecht, Netherlands
C. Søgaard Division of Experimental High Energy Physics, University of Lund, Lund, Sweden
R. Soltz Lawrence Livermore National Laboratory, Livermore, California United States
M. Song Yonsei University, Seoul, South Korea
J. Song Pusan National University, Pusan, South Korea
C. Soos European Organization for Nuclear Research (CERN), Geneva, Switzerland
F. Soramel Dipartimento di Fisica e Astronomia dell’Università and Sezione INFN, Padova, Italy
I. Sputowska The Henryk Niewodniczanski Institute of Nuclear Physics, Polish Academy of Sciences, Cracow, Poland
M. Spyropoulou-Stassinaki Physics Department, University of Athens, Athens, Greece
B. K. Srivastava Purdue University, West Lafayette, Indiana United States
J. Stachel Physikalisches Institut, Ruprecht-Karls-Universität Heidelberg, Heidelberg, Germany
I. Stan Institute of Space Sciences (ISS), Bucharest, Romania
G. Stefanek National Centre for Nuclear Studies, Warsaw, Poland
M. Steinpreis Department of Physics, Ohio State University, Columbus, Ohio United States
E. Stenlund Division of Experimental High Energy Physics, University of Lund, Lund, Sweden
G. Steyn Physics Department, University of Cape Town and iThemba LABS, National Research Foundation, Somerset West, South Africa
J. H. Stiller Physikalisches Institut, Ruprecht-Karls-Universität Heidelberg, Heidelberg, Germany
D. Stocco SUBATECH, Ecole des Mines de Nantes, Université de Nantes, CNRS-IN2P3, Nantes, France
M. Stolpovskiy Institute for High Energy Physics, Protvino, Russia
P. Strmen Faculty of Mathematics, Physics and Informatics, Comenius University, Bratislava, Slovakia
A. A. P. Suaide Universidade de São Paulo (USP), São Paulo, Brazil
M. A. Subieta Vásquez Dipartimento di Fisica dell’Università and Sezione INFN, Turin, Italy
T. Sugitate Hiroshima University, Hiroshima, Japan
C. Suire Institut de Physique Nucléaire d’Orsay (IPNO), Université Paris-Sud, CNRS-IN2P3, Orsay, France
M. Suleymanov COMSATS Institute of Information Technology (CIIT), Islamabad, Pakistan
R. Sultanov Institute for Theoretical and Experimental Physics, Moscow, Russia
M. Šumbera Nuclear Physics Institute, Academy of Sciences of the Czech Republic, Řež u Prahy, Czech Republic
T. Susa Rudjer Bošković Institute, Zagreb, Croatia
T. J. M. Symons Lawrence Berkeley National Laboratory, Berkeley, California United States
A. Szanto de Toledo Universidade de São Paulo (USP), São Paulo, Brazil
I. Szarka Faculty of Mathematics, Physics and Informatics, Comenius University, Bratislava, Slovakia
A. Szczepankiewicz European Organization for Nuclear Research (CERN), Geneva, Switzerland
M. Szymański Warsaw University of Technology, Warsaw, Poland
J. Takahashi Universidade Estadual de Campinas (UNICAMP), Campinas, Brazil
M. A. Tangaro Dipartimento Interateneo di Fisica ‘M. Merlin’ and Sezione INFN, Bari, Italy
J. D. Tapia Takaki Institut de Physique Nucléaire d’Orsay (IPNO), Université Paris-Sud, CNRS-IN2P3, Orsay, France
A. Tarantola Peloni Institut für Kernphysik, Johann Wolfgang Goethe-Universität Frankfurt, Frankfurt, Germany
A. Tarazona Martinez European Organization for Nuclear Research (CERN), Geneva, Switzerland
A. Tauro European Organization for Nuclear Research (CERN), Geneva, Switzerland
G. Tejeda Muñoz Benemérita Universidad Autónoma de Puebla, Puebla, Mexico
A. Telesca European Organization for Nuclear Research (CERN), Geneva, Switzerland
A. Ter Minasyan Russian Research Centre Kurchatov Institute, Moscow, Russia
C. Terrevoli Dipartimento Interateneo di Fisica ‘M. Merlin’ and Sezione INFN, Bari, Italy
J. Thäder Research Division and ExtreMe Matter Institute EMMI, GSI Helmholtzzentrum für Schwerionenforschung, Darmstadt, Germany
D. Thomas Nikhef, National Institute for Subatomic Physics and Institute for Subatomic Physics of Utrecht University, Utrecht, Netherlands
R. Tieulent Université de Lyon, Université Lyon 1, CNRS/IN2P3, IPN-Lyon, Villeurbanne, France
A. R. Timmins University of Houston, Houston, Texas United States
D. Tlusty Faculty of Nuclear Sciences and Physical Engineering, Czech Technical University in Prague, Prague, Czech Republic
A. Toia Dipartimento di Fisica e Astronomia dell’Università and Sezione INFN, Padova, Italy Frankfurt Institute for Advanced Studies, Johann Wolfgang Goethe-Universität Frankfurt, Frankfurt, Germany Sezione INFN, Padova, Italy
H. Torii University of Tokyo, Tokyo, Japan
L. Toscano Sezione INFN, Turin, Italy
V. Trubnikov Bogolyubov Institute for Theoretical Physics, Kiev, Ukraine
D. Truesdale Department of Physics, Ohio State University, Columbus, Ohio United States
W. H. Trzaska Helsinki Institute of Physics (HIP) and University of Jyväskylä, Jyväskylä, Finland
T. Tsuji University of Tokyo, Tokyo, Japan
A. Tumkin Russian Federal Nuclear Center (VNIIEF), Sarov, Russia
R. Turrisi Sezione INFN, Padova, Italy
T. S. Tveter Department of Physics, University of Oslo, Oslo, Norway
J. Ulery Institut für Kernphysik, Johann Wolfgang Goethe-Universität Frankfurt, Frankfurt, Germany
K. Ullaland Department of Physics and Technology, University of Bergen, Bergen, Norway
J. Ulrich Institut für Informatik, Johann Wolfgang Goethe-Universität Frankfurt, Frankfurt, Germany Kirchhoff-Institut für Physik, Ruprecht-Karls-Universität Heidelberg, Heidelberg, Germany
A. Uras Université de Lyon, Université Lyon 1, CNRS/IN2P3, IPN-Lyon, Villeurbanne, France
G. M. Urciuoli Sezione INFN, Rome, Italy
G. L. Usai Dipartimento di Fisica dell’Università and Sezione INFN, Cagliari, Italy
M. Vajzer Faculty of Nuclear Sciences and Physical Engineering, Czech Technical University in Prague, Prague, Czech Republic Nuclear Physics Institute, Academy of Sciences of the Czech Republic, Řež u Prahy, Czech Republic
M. Vala Institute of Experimental Physics, Slovak Academy of Sciences, Košice, Slovakia Joint Institute for Nuclear Research (JINR), Dubna, Russia
L. Valencia Palomo Institut de Physique Nucléaire d’Orsay (IPNO), Université Paris-Sud, CNRS-IN2P3, Orsay, France
S. Vallero Dipartimento di Fisica dell’Università and Sezione INFN, Turin, Italy
P. Vande Vyvre European Organization for Nuclear Research (CERN), Geneva, Switzerland
J. W. Van Hoorne European Organization for Nuclear Research (CERN), Geneva, Switzerland
M. van Leeuwen Nikhef, National Institute for Subatomic Physics and Institute for Subatomic Physics of Utrecht University, Utrecht, Netherlands
L. Vannucci Laboratori Nazionali di Legnaro, INFN, Legnaro, Italy
A. Vargas Benemérita Universidad Autónoma de Puebla, Puebla, Mexico
R. Varma Indian Institute of Technology Bombay (IIT), Mumbai, India
M. Vasileiou Physics Department, University of Athens, Athens, Greece
A. Vasiliev Russian Research Centre Kurchatov Institute, Moscow, Russia
V. Vechernin V. Fock Institute for Physics, St. Petersburg State University, St. Petersburg, Russia
M. Veldhoen Nikhef, National Institute for Subatomic Physics and Institute for Subatomic Physics of Utrecht University, Utrecht, Netherlands
M. Venaruzzo Dipartimento di Fisica dell’Università and Sezione INFN, Trieste, Italy
E. Vercellin Dipartimento di Fisica dell’Università and Sezione INFN, Turin, Italy
S. Vergara Benemérita Universidad Autónoma de Puebla, Puebla, Mexico
R. Vernet Centre de Calcul de l’IN2P3, Villeurbanne, France
M. Verweij Nikhef, National Institute for Subatomic Physics and Institute for Subatomic Physics of Utrecht University, Utrecht, Netherlands
L. Vickovic Technical University of Split FESB, Split, Croatia
G. Viesti Dipartimento di Fisica e Astronomia dell’Università and Sezione INFN, Padova, Italy
J. Viinikainen Helsinki Institute of Physics (HIP) and University of Jyväskylä, Jyväskylä, Finland
Z. Vilakazi Physics Department, University of Cape Town and iThemba LABS, National Research Foundation, Somerset West, South Africa
O. Villalobos Baillie School of Physics and Astronomy, University of Birmingham, Birmingham, United Kingdom
Y. Vinogradov Russian Federal Nuclear Center (VNIIEF), Sarov, Russia
L. Vinogradov V. Fock Institute for Physics, St. Petersburg State University, St. Petersburg, Russia
A. Vinogradov Russian Research Centre Kurchatov Institute, Moscow, Russia
T. Virgili Dipartimento di Fisica ‘E.R. Caianiello’ dell’Università and Gruppo Collegato INFN, Salerno, Italy
Y. P. Viyogi Variable Energy Cyclotron Centre, Kolkata, India
A. Vodopyanov Joint Institute for Nuclear Research (JINR), Dubna, Russia
M. A. Völkl Physikalisches Institut, Ruprecht-Karls-Universität Heidelberg, Heidelberg, Germany
S. Voloshin Wayne State University, Detroit, Michigan United States
K. Voloshin Institute for Theoretical and Experimental Physics, Moscow, Russia
G. Volpe European Organization for Nuclear Research (CERN), Geneva, Switzerland
B. von Haller European Organization for Nuclear Research (CERN), Geneva, Switzerland
I. Vorobyev V. Fock Institute for Physics, St. Petersburg State University, St. Petersburg, Russia
D. Vranic European Organization for Nuclear Research (CERN), Geneva, Switzerland Research Division and ExtreMe Matter Institute EMMI, GSI Helmholtzzentrum für Schwerionenforschung, Darmstadt, Germany
J. Vrláková Faculty of Science, P.J. Šafárik University, Košice, Slovakia
B. Vulpescu Laboratoire de Physique Corpusculaire (LPC), Clermont Université, Université Blaise Pascal, CNRS–IN2P3, Clermont-Ferrand, France
A. Vyushin Russian Federal Nuclear Center (VNIIEF), Sarov, Russia
V. Wagner Faculty of Nuclear Sciences and Physical Engineering, Czech Technical University in Prague, Prague, Czech Republic
B. Wagner Department of Physics and Technology, University of Bergen, Bergen, Norway
R. Wan Central China Normal University, Wuhan, China
Y. Wang Central China Normal University, Wuhan, China
Y. Wang Physikalisches Institut, Ruprecht-Karls-Universität Heidelberg, Heidelberg, Germany
M. Wang Central China Normal University, Wuhan, China
K. Watanabe University of Tsukuba, Tsukuba, Japan
M. Weber University of Houston, Houston, Texas United States
J. P. Wessels European Organization for Nuclear Research (CERN), Geneva, Switzerland Institut für Kernphysik, Westfälische Wilhelms-Universität Münster, Münster, Germany
U. Westerhoff Institut für Kernphysik, Westfälische Wilhelms-Universität Münster, Münster, Germany
J. Wiechula Eberhard Karls Universität Tübingen, Tübingen, Germany
J. Wikne Department of Physics, University of Oslo, Oslo, Norway
M. Wilde Institut für Kernphysik, Westfälische Wilhelms-Universität Münster, Münster, Germany
G. Wilk National Centre for Nuclear Studies, Warsaw, Poland
M. C. S. Williams Sezione INFN, Bologna, Italy
B. Windelband Physikalisches Institut, Ruprecht-Karls-Universität Heidelberg, Heidelberg, Germany
C. G. Yaldo Wayne State University, Detroit, Michigan United States
Y. Yamaguchi University of Tokyo, Tokyo, Japan
S. Yang Department of Physics and Technology, University of Bergen, Bergen, Norway
P. Yang Central China Normal University, Wuhan, China
H. Yang Commissariat à l’Energie Atomique, IRFU, Saclay, France Nikhef, National Institute for Subatomic Physics and Institute for Subatomic Physics of Utrecht University, Utrecht, Netherlands
S. Yasnopolskiy Russian Research Centre Kurchatov Institute, Moscow, Russia
J. Yi Pusan National University, Pusan, South Korea
Z. Yin Central China Normal University, Wuhan, China
I.-K. Yoo Pusan National University, Pusan, South Korea
J. Yoon Yonsei University, Seoul, South Korea
X. Yuan Central China Normal University, Wuhan, China
I. Yushmanov Russian Research Centre Kurchatov Institute, Moscow, Russia
V. Zaccolo Niels Bohr Institute, University of Copenhagen, Copenhagen, Denmark
C. Zach Faculty of Nuclear Sciences and Physical Engineering, Czech Technical University in Prague, Prague, Czech Republic
C. Zampolli Sezione INFN, Bologna, Italy
S. Zaporozhets Joint Institute for Nuclear Research (JINR), Dubna, Russia
A. Zarochentsev V. Fock Institute for Physics, St. Petersburg State University, St. Petersburg, Russia
P. Závada Institute of Physics, Academy of Sciences of the Czech Republic, Prague, Czech Republic
N. Zaviyalov Russian Federal Nuclear Center (VNIIEF), Sarov, Russia
H. Zbroszczyk Warsaw University of Technology, Warsaw, Poland
P. Zelnicek Institut für Informatik, Johann Wolfgang Goethe-Universität Frankfurt, Frankfurt, Germany
I. S. Zgura Institute of Space Sciences (ISS), Bucharest, Romania
M. Zhalov Petersburg Nuclear Physics Institute, Gatchina, Russia
Y. Zhang Central China Normal University, Wuhan, China
H. Zhang Central China Normal University, Wuhan, China
X. Zhang Central China Normal University, Wuhan, China Laboratoire de Physique Corpusculaire (LPC), Clermont Université, Université Blaise Pascal, CNRS–IN2P3, Clermont-Ferrand, France Lawrence Berkeley National Laboratory, Berkeley, California United States
D. Zhou Central China Normal University, Wuhan, China
Y. Zhou Nikhef, National Institute for Subatomic Physics and Institute for Subatomic Physics of Utrecht University, Utrecht, Netherlands
F. Zhou Central China Normal University, Wuhan, China
H. Zhu Central China Normal University, Wuhan, China
J. Zhu Central China Normal University, Wuhan, China
X. Zhu Central China Normal University, Wuhan, China
J. Zhu Central China Normal University, Wuhan, China
A. Zichichi Centro Fermi - Museo Storico della Fisica e Centro Studi e Ricerche “Enrico Fermi”, Rome, Italy Dipartimento di Fisica e Astronomia dell’Università and Sezione INFN, Bologna, Italy
A. Zimmermann Physikalisches Institut, Ruprecht-Karls-Universität Heidelberg, Heidelberg, Germany
G. Zinovjev Bogolyubov Institute for Theoretical Physics, Kiev, Ukraine
Y. Zoccarato Université de Lyon, Université Lyon 1, CNRS/IN2P3, IPN-Lyon, Villeurbanne, France
M. Zynovyev Bogolyubov Institute for Theoretical Physics, Kiev, Ukraine
M. Zyzak Institut für Kernphysik, Johann Wolfgang Goethe-Universität Frankfurt, Frankfurt, Germany

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