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Grussie F, O'Connor AP, Grieser M, Müll D, Znotins A, Urbain X, Kreckel H. An ion-atom merged beams setup at the Cryogenic Storage Ring. THE REVIEW OF SCIENTIFIC INSTRUMENTS 2022; 93:053305. [PMID: 35649784 DOI: 10.1063/5.0086391] [Citation(s) in RCA: 1] [Impact Index Per Article: 0.5] [Reference Citation Analysis] [Abstract] [Track Full Text] [Subscribe] [Scholar Register] [Received: 01/25/2022] [Accepted: 04/26/2022] [Indexed: 06/15/2023]
Abstract
We describe a merged beams experiment to study ion-neutral collisions at the Cryogenic Storage Ring of the Max Planck Institute for Nuclear Physics in Heidelberg, Germany. We produce fast beams of neutral atoms in their ground term at kinetic energies between 10 and 300 keV by laser photodetachment of negative ions. The neutral atoms are injected along one of the straight sections of the storage ring, where they can react with stored molecular ions. Several dedicated detectors have been installed to detect charged reaction products of various product-to-reactant mass ranges. The relative collision energy can be tuned by changing the kinetic energy of the neutral beam in an independent drift tube. We give a detailed description of the setup and its capabilities, and present proof-of-principle measurements on the reaction of neutral C atoms with D2 + ions.
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Affiliation(s)
- F Grussie
- Max-Planck-Institut für Kernphysik, Saupfercheckweg 1, 69117 Heidelberg, Germany
| | - A P O'Connor
- Max-Planck-Institut für Kernphysik, Saupfercheckweg 1, 69117 Heidelberg, Germany
| | - M Grieser
- Max-Planck-Institut für Kernphysik, Saupfercheckweg 1, 69117 Heidelberg, Germany
| | - D Müll
- Max-Planck-Institut für Kernphysik, Saupfercheckweg 1, 69117 Heidelberg, Germany
| | - A Znotins
- Max-Planck-Institut für Kernphysik, Saupfercheckweg 1, 69117 Heidelberg, Germany
| | - X Urbain
- Institute of Condensed Matter and Nanosciences, Université Catholique de Louvain, Louvain-la-Neuve B 1348, Belgium
| | - H Kreckel
- Max-Planck-Institut für Kernphysik, Saupfercheckweg 1, 69117 Heidelberg, Germany
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Bowen KP, Hillenbrand PM, Liévin J, Savin DW, Urbain X. Dynamics of the isotope exchange reaction of D with H 3 +, H 2D +, and D 2H . J Chem Phys 2021; 154:084307. [PMID: 33639774 DOI: 10.1063/5.0038434] [Citation(s) in RCA: 2] [Impact Index Per Article: 0.7] [Reference Citation Analysis] [Abstract] [Track Full Text] [Journal Information] [Subscribe] [Scholar Register] [Indexed: 11/14/2022] Open
Abstract
We have measured the merged-beams rate coefficient for the titular isotope exchange reactions as a function of the relative collision energy in the range of ∼3 meV-10 eV. The results appear to scale with the number of available sites for deuteration. We have performed extensive theoretical calculations to characterize the zero-point energy corrected reaction path. Vibrationally adiabatic minimum energy paths were obtained using a combination of unrestricted quadratic configuration interaction of single and double excitations and internally contracted multireference configuration interaction calculations. The resulting barrier height, ranging from 68 meV to 89 meV, together with the various asymptotes that may be reached in the collision, was used in a classical over-the-barrier model. All competing endoergic reaction channels were taken into account using a flux reduction factor. This model reproduces all three experimental sets quite satisfactorily. In order to generate thermal rate coefficients down to 10 K, the internal excitation energy distribution of each H3 + isotopologue is evaluated level by level using available line lists and accurate spectroscopic parameters. Tunneling is accounted for by a direct inclusion of the exact quantum tunneling probability in the evaluation of the cross section. We derive a thermal rate coefficient of <1×10-12 cm3 s-1 for temperatures below 44 K, 86 K, and 139 K for the reaction of D with H3 +, H2D+, and D2H+, respectively, with tunneling effects included. The derived thermal rate coefficients exceed the ring polymer molecular dynamics prediction of Bulut et al. [J. Phys. Chem. A 123, 8766 (2019)] at all temperatures.
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Affiliation(s)
- K P Bowen
- Columbia Astrophysics Laboratory, Columbia University, New York, New York 10027, USA
| | - P-M Hillenbrand
- Columbia Astrophysics Laboratory, Columbia University, New York, New York 10027, USA
| | - J Liévin
- Spectroscopy, Quantum Chemistry and Atmospheric Remote Sensing (SQUARES), Université Libre de Bruxelles, B-1050 Brussels, Belgium
| | - D W Savin
- Columbia Astrophysics Laboratory, Columbia University, New York, New York 10027, USA
| | - X Urbain
- Institute of Condensed Matter and Nanosciences, Université Catholique de Louvain, B-1348 Louvain-la-Neuve, Belgium
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Hansen VL. Global tectonic evolution of Venus, from exogenic to endogenic over time, and implications for early Earth processes. PHILOSOPHICAL TRANSACTIONS. SERIES A, MATHEMATICAL, PHYSICAL, AND ENGINEERING SCIENCES 2018; 377:20180412. [PMID: 30275161 DOI: 10.1098/rsta.2018.0412] [Citation(s) in RCA: 3] [Impact Index Per Article: 0.5] [Reference Citation Analysis] [Abstract] [Key Words] [Track Full Text] [Subscribe] [Scholar Register] [Accepted: 07/04/2018] [Indexed: 05/23/2023]
Abstract
Venus provides a rich arena in which to stretch one's tectonic imagination with respect to non-plate tectonic processes of heat transfer on an Earth-like planet. Venus is similar to Earth in density, size, inferred composition and heat budget. However, Venus' lack of plate tectonics and terrestrial surficial processes results in the preservation of a unique surface geologic record of non-plate tectonomagmatic processes. In this paper, I explore three global tectonic domains that represent changes in global conditions and tectonic regimes through time, divided respectively into temporal eras. Impactors played a prominent role in the ancient era, characterized by thin global lithosphere. The Artemis superstructure era highlights sublithospheric flow processes related to a uniquely large super plume. The fracture zone complex era, marked by broad zones of tectonomagmatic activity, witnessed coupled spreading and underthrusting, since arrested. These three tectonic regimes provide possible analogue models for terrestrial Archaean craton formation, continent formation without plate tectonics, and mechanisms underlying the emergence of plate tectonics. A bolide impact model for craton formation addresses the apparent paradox of both undepleted mantle and growth of Archaean crust, and recycling of significant Archaean crust to the mantle.This article is part of a discussion meeting issue 'Earth dynamics and the development of plate tectonics'.
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Affiliation(s)
- Vicki L Hansen
- Department of Earth and Environmental Sciences, University of Minnesota Duluth, 1114 Kirby Drive, Duluth, MN 55812, USA
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Bresteau D, Blondel C, Drag C. Saturation of the photoneutralization of a H - beam in continuous operation. THE REVIEW OF SCIENTIFIC INSTRUMENTS 2017; 88:113103. [PMID: 29195388 DOI: 10.1063/1.4995390] [Citation(s) in RCA: 5] [Impact Index Per Article: 0.7] [Reference Citation Analysis] [Abstract] [Track Full Text] [Subscribe] [Scholar Register] [Indexed: 06/07/2023]
Abstract
An unprecedented, greater than 50%, photodetachment rate is obtained on a H- beam in the continuous regime. The key element of the experimental setup is a medium-finesse optical cavity, suspended around the anion beam, which makes it possible to recycle the photon flux in the interaction region, at the crossing between the anion and laser beams. The cavity is injected by a narrow-linewidth ytterbium-doped fibre laser, at the wavelength 1064 nm. The light power stored in the cavity is about 14 kW for 24 W of input light power. Similar greater-than-50% photo-neutralization efficiencies can be contemplated for beams with kinetic energies much larger than 1.2 keV of the presently used H- beam, given the fact that the stored light power can be increased, for larger beam diameters, by several orders of magnitude. The technique can thus be relied on to design novel D0 injectors, for fusion reactors, with a much better efficiency than the molecular-collision based injectors presently developed for ITER. It can also be applied to the production of neutral beams of any species that can be conveniently prepared in the form of an anion beam, provided that efficient light power storage can be achieved for the corresponding photodetachment wavelength.
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Affiliation(s)
- D Bresteau
- Laboratoire Aimé-Cotton, CNRS, École Normale Supérieure de Cachan, Université Paris-Sud, F-91405 Orsay Cedex, France
| | - C Blondel
- Laboratoire Aimé-Cotton, CNRS, École Normale Supérieure de Cachan, Université Paris-Sud, F-91405 Orsay Cedex, France
| | - C Drag
- Laboratoire Aimé-Cotton, CNRS, École Normale Supérieure de Cachan, Université Paris-Sud, F-91405 Orsay Cedex, France
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Nakano Y, Enomoto Y, Masunaga T, Menk S, Bertier P, Azuma T. Design and commissioning of the RIKEN cryogenic electrostatic ring (RICE). THE REVIEW OF SCIENTIFIC INSTRUMENTS 2017; 88:033110. [PMID: 28372443 DOI: 10.1063/1.4978454] [Citation(s) in RCA: 6] [Impact Index Per Article: 0.9] [Reference Citation Analysis] [Abstract] [Track Full Text] [Subscribe] [Scholar Register] [Indexed: 06/07/2023]
Abstract
A new electrostatic ion storage ring, the RIKEN cryogenic electrostatic ring, has been commissioned with a 15-keV ion beam under cryogenic conditions. The ring was designed with a closed ion beam orbit of about 2.9 m, where the ion beam is guided entirely by electrostatic components. The vacuum chamber of the ring is cooled using a liquid-He-free cooling system to 4.2 K with a temperature difference of 0.4 K at most within all the positions measured by calibrated silicon diode sensors. The first cryogenic operation with a 15-keV Ne+ beam was successfully performed in August 2014. During the measurement, the Ne+ beam was stored under a ring temperature of 4.2 K with a residual-gas lifetime of more than 10 min. This permits an estimation of the residual gas density at a few 104 cm-3, which corresponds to a room-temperature-equivalent pressure of around 1×10-10 Pa. An effect of longitudinal pulse compression at the bunching cavity in the ring was clearly identified by monitoring the pick-up beam detector. The detailed design and mechanical structure of the storage ring, as well as the results from the commissioning run, are reported.
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Affiliation(s)
- Y Nakano
- AMO Physics Laboratory, RIKEN, 351-0198 Saitama, Japan
| | - Y Enomoto
- AMO Physics Laboratory, RIKEN, 351-0198 Saitama, Japan
| | - T Masunaga
- AMO Physics Laboratory, RIKEN, 351-0198 Saitama, Japan
| | - S Menk
- AMO Physics Laboratory, RIKEN, 351-0198 Saitama, Japan
| | - P Bertier
- AMO Physics Laboratory, RIKEN, 351-0198 Saitama, Japan
| | - T Azuma
- AMO Physics Laboratory, RIKEN, 351-0198 Saitama, Japan
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von Hahn R, Becker A, Berg F, Blaum K, Breitenfeldt C, Fadil H, Fellenberger F, Froese M, George S, Göck J, Grieser M, Grussie F, Guerin EA, Heber O, Herwig P, Karthein J, Krantz C, Kreckel H, Lange M, Laux F, Lohmann S, Menk S, Meyer C, Mishra PM, Novotný O, O'Connor AP, Orlov DA, Rappaport ML, Repnow R, Saurabh S, Schippers S, Schröter CD, Schwalm D, Schweikhard L, Sieber T, Shornikov A, Spruck K, Sunil Kumar S, Ullrich J, Urbain X, Vogel S, Wilhelm P, Wolf A, Zajfman D. The cryogenic storage ring CSR. THE REVIEW OF SCIENTIFIC INSTRUMENTS 2016; 87:063115. [PMID: 27370434 DOI: 10.1063/1.4953888] [Citation(s) in RCA: 16] [Impact Index Per Article: 2.0] [Reference Citation Analysis] [Abstract] [Track Full Text] [Subscribe] [Scholar Register] [Indexed: 06/06/2023]
Abstract
An electrostatic cryogenic storage ring, CSR, for beams of anions and cations with up to 300 keV kinetic energy per unit charge has been designed, constructed, and put into operation. With a circumference of 35 m, the ion-beam vacuum chambers and all beam optics are in a cryostat and cooled by a closed-cycle liquid helium system. At temperatures as low as (5.5 ± 1) K inside the ring, storage time constants of several minutes up to almost an hour were observed for atomic and molecular, anion and cation beams at an energy of 60 keV. The ion-beam intensity, energy-dependent closed-orbit shifts (dispersion), and the focusing properties of the machine were studied by a system of capacitive pickups. The Schottky-noise spectrum of the stored ions revealed a broadening of the momentum distribution on a time scale of 1000 s. Photodetachment of stored anions was used in the beam lifetime measurements. The detachment rate by anion collisions with residual-gas molecules was found to be extremely low. A residual-gas density below 140 cm(-3) is derived, equivalent to a room-temperature pressure below 10(-14) mbar. Fast atomic, molecular, and cluster ion beams stored for long periods of time in a cryogenic environment will allow experiments on collision- and radiation-induced fragmentation processes of ions in known internal quantum states with merged and crossed photon and particle beams.
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Affiliation(s)
- R von Hahn
- Max-Planck-Institut für Kernphysik, 69117 Heidelberg, Germany
| | - A Becker
- Max-Planck-Institut für Kernphysik, 69117 Heidelberg, Germany
| | - F Berg
- Max-Planck-Institut für Kernphysik, 69117 Heidelberg, Germany
| | - K Blaum
- Max-Planck-Institut für Kernphysik, 69117 Heidelberg, Germany
| | - C Breitenfeldt
- Max-Planck-Institut für Kernphysik, 69117 Heidelberg, Germany
| | - H Fadil
- Max-Planck-Institut für Kernphysik, 69117 Heidelberg, Germany
| | - F Fellenberger
- Max-Planck-Institut für Kernphysik, 69117 Heidelberg, Germany
| | - M Froese
- Max-Planck-Institut für Kernphysik, 69117 Heidelberg, Germany
| | - S George
- Max-Planck-Institut für Kernphysik, 69117 Heidelberg, Germany
| | - J Göck
- Max-Planck-Institut für Kernphysik, 69117 Heidelberg, Germany
| | - M Grieser
- Max-Planck-Institut für Kernphysik, 69117 Heidelberg, Germany
| | - F Grussie
- Max-Planck-Institut für Kernphysik, 69117 Heidelberg, Germany
| | - E A Guerin
- Max-Planck-Institut für Kernphysik, 69117 Heidelberg, Germany
| | - O Heber
- Weizmann Institute of Science, Rehovot 76100, Israel
| | - P Herwig
- Max-Planck-Institut für Kernphysik, 69117 Heidelberg, Germany
| | - J Karthein
- Max-Planck-Institut für Kernphysik, 69117 Heidelberg, Germany
| | - C Krantz
- Max-Planck-Institut für Kernphysik, 69117 Heidelberg, Germany
| | - H Kreckel
- Max-Planck-Institut für Kernphysik, 69117 Heidelberg, Germany
| | - M Lange
- Max-Planck-Institut für Kernphysik, 69117 Heidelberg, Germany
| | - F Laux
- Max-Planck-Institut für Kernphysik, 69117 Heidelberg, Germany
| | - S Lohmann
- Max-Planck-Institut für Kernphysik, 69117 Heidelberg, Germany
| | - S Menk
- Max-Planck-Institut für Kernphysik, 69117 Heidelberg, Germany
| | - C Meyer
- Max-Planck-Institut für Kernphysik, 69117 Heidelberg, Germany
| | - P M Mishra
- Max-Planck-Institut für Kernphysik, 69117 Heidelberg, Germany
| | - O Novotný
- Max-Planck-Institut für Kernphysik, 69117 Heidelberg, Germany
| | - A P O'Connor
- Max-Planck-Institut für Kernphysik, 69117 Heidelberg, Germany
| | - D A Orlov
- Max-Planck-Institut für Kernphysik, 69117 Heidelberg, Germany
| | - M L Rappaport
- Weizmann Institute of Science, Rehovot 76100, Israel
| | - R Repnow
- Max-Planck-Institut für Kernphysik, 69117 Heidelberg, Germany
| | - S Saurabh
- Max-Planck-Institut für Kernphysik, 69117 Heidelberg, Germany
| | - S Schippers
- I. Physikalisches Institut, Justus-Liebig-Universität Gießen, 35392 Gießen, Germany
| | - C D Schröter
- Max-Planck-Institut für Kernphysik, 69117 Heidelberg, Germany
| | - D Schwalm
- Max-Planck-Institut für Kernphysik, 69117 Heidelberg, Germany
| | - L Schweikhard
- Institut für Physik, Ernst-Moritz-Arndt-Universität, 17487 Greifswald, Germany
| | - T Sieber
- Max-Planck-Institut für Kernphysik, 69117 Heidelberg, Germany
| | - A Shornikov
- Max-Planck-Institut für Kernphysik, 69117 Heidelberg, Germany
| | - K Spruck
- Max-Planck-Institut für Kernphysik, 69117 Heidelberg, Germany
| | - S Sunil Kumar
- Max-Planck-Institut für Kernphysik, 69117 Heidelberg, Germany
| | - J Ullrich
- Max-Planck-Institut für Kernphysik, 69117 Heidelberg, Germany
| | - X Urbain
- Institute of Condensed Matter and Nanosciences, Université Catholique de Louvain, 1348 Louvain-la-Neuve, Belgium
| | - S Vogel
- Max-Planck-Institut für Kernphysik, 69117 Heidelberg, Germany
| | - P Wilhelm
- Max-Planck-Institut für Kernphysik, 69117 Heidelberg, Germany
| | - A Wolf
- Max-Planck-Institut für Kernphysik, 69117 Heidelberg, Germany
| | - D Zajfman
- Weizmann Institute of Science, Rehovot 76100, Israel
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