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Abbott D, Adderley P, Adeyemi A, Aguilera P, Ali M, Areti H, Baylac M, Benesch J, Bosson G, Cade B, Camsonne A, Cardman LS, Clark J, Cole P, Covert S, Cuevas C, Dadoun O, Dale D, Dong H, Dumas J, Fanchini E, Forest T, Forman E, Freyberger A, Froidefond E, Golge S, Grames J, Guèye P, Hansknecht J, Harrell P, Hoskins J, Hyde C, Josey B, Kazimi R, Kim Y, Machie D, Mahoney K, Mammei R, Marton M, McCarter J, McCaughan M, McHugh M, McNulty D, Mesick KE, Michaelides T, Michaels R, Moffit B, Moser D, Muñoz Camacho C, Muraz JF, Opper A, Poelker M, Réal JS, Richardson L, Setiniyaz S, Stutzman M, Suleiman R, Tennant C, Tsai C, Turner D, Ungaro M, Variola A, Voutier E, Wang Y, Zhang Y. Production of Highly Polarized Positrons Using Polarized Electrons at MeV Energies. Phys Rev Lett 2016; 116:214801. [PMID: 27284661 DOI: 10.1103/physrevlett.116.214801] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [What about the content of this article? (0)] [Affiliation(s)] [Abstract] [Track Full Text] [Subscribe] [Scholar Register] [Received: 02/26/2016] [Indexed: 06/06/2023]
Abstract
The Polarized Electrons for Polarized Positrons experiment at the injector of the Continuous Electron Beam Accelerator Facility has demonstrated for the first time the efficient transfer of polarization from electrons to positrons produced by the polarized bremsstrahlung radiation induced by a polarized electron beam in a high-Z target. Positron polarization up to 82% have been measured for an initial electron beam momentum of 8.19 MeV/c, limited only by the electron beam polarization. This technique extends polarized positron capabilities from GeV to MeV electron beams, and opens access to polarized positron beam physics to a wide community.
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Affiliation(s)
- D Abbott
- Thomas Jefferson National Accelerator Facility, Newport News, Virginia 23606, USA
| | - P Adderley
- Thomas Jefferson National Accelerator Facility, Newport News, Virginia 23606, USA
| | - A Adeyemi
- Hampton University, Hampton, Virginia 23668, USA
| | - P Aguilera
- Thomas Jefferson National Accelerator Facility, Newport News, Virginia 23606, USA
| | - M Ali
- Thomas Jefferson National Accelerator Facility, Newport News, Virginia 23606, USA
| | - H Areti
- Thomas Jefferson National Accelerator Facility, Newport News, Virginia 23606, USA
| | - M Baylac
- LPSC, Université Grenoble-Alpes, CNRS/IN2P3, 38026 Grenoble, France
| | - J Benesch
- Thomas Jefferson National Accelerator Facility, Newport News, Virginia 23606, USA
| | - G Bosson
- LPSC, Université Grenoble-Alpes, CNRS/IN2P3, 38026 Grenoble, France
| | - B Cade
- Thomas Jefferson National Accelerator Facility, Newport News, Virginia 23606, USA
| | - A Camsonne
- Thomas Jefferson National Accelerator Facility, Newport News, Virginia 23606, USA
| | - L S Cardman
- Thomas Jefferson National Accelerator Facility, Newport News, Virginia 23606, USA
| | - J Clark
- Thomas Jefferson National Accelerator Facility, Newport News, Virginia 23606, USA
| | - P Cole
- Idaho State University, Pocatello, Idaho 83209, USA
| | - S Covert
- Thomas Jefferson National Accelerator Facility, Newport News, Virginia 23606, USA
| | - C Cuevas
- Thomas Jefferson National Accelerator Facility, Newport News, Virginia 23606, USA
| | - O Dadoun
- LAL, Université Paris-Sud & Université Paris-Saclay, CNRS/IN2P3, 91898 Orsay, France
| | - D Dale
- Idaho State University, Pocatello, Idaho 83209, USA
| | - H Dong
- Thomas Jefferson National Accelerator Facility, Newport News, Virginia 23606, USA
| | - J Dumas
- Thomas Jefferson National Accelerator Facility, Newport News, Virginia 23606, USA
- LPSC, Université Grenoble-Alpes, CNRS/IN2P3, 38026 Grenoble, France
| | - E Fanchini
- LPSC, Université Grenoble-Alpes, CNRS/IN2P3, 38026 Grenoble, France
| | - T Forest
- Idaho State University, Pocatello, Idaho 83209, USA
| | - E Forman
- Thomas Jefferson National Accelerator Facility, Newport News, Virginia 23606, USA
| | - A Freyberger
- Thomas Jefferson National Accelerator Facility, Newport News, Virginia 23606, USA
| | - E Froidefond
- LPSC, Université Grenoble-Alpes, CNRS/IN2P3, 38026 Grenoble, France
| | - S Golge
- North Carolina Central University, Durham, North Carolina 27707, USA
| | - J Grames
- Thomas Jefferson National Accelerator Facility, Newport News, Virginia 23606, USA
| | - P Guèye
- Hampton University, Hampton, Virginia 23668, USA
| | - J Hansknecht
- Thomas Jefferson National Accelerator Facility, Newport News, Virginia 23606, USA
| | - P Harrell
- Thomas Jefferson National Accelerator Facility, Newport News, Virginia 23606, USA
| | - J Hoskins
- The College of William & Mary, Williamsburg, Virginia 23187, USA
| | - C Hyde
- Old Dominion University, Norfolk, Virginia 23529, USA
| | - B Josey
- University of New Mexico, Albuquerque, New Mexico 87131, USA
| | - R Kazimi
- Thomas Jefferson National Accelerator Facility, Newport News, Virginia 23606, USA
| | - Y Kim
- Thomas Jefferson National Accelerator Facility, Newport News, Virginia 23606, USA
- Idaho State University, Pocatello, Idaho 83209, USA
| | - D Machie
- Thomas Jefferson National Accelerator Facility, Newport News, Virginia 23606, USA
| | - K Mahoney
- Thomas Jefferson National Accelerator Facility, Newport News, Virginia 23606, USA
| | - R Mammei
- Thomas Jefferson National Accelerator Facility, Newport News, Virginia 23606, USA
| | - M Marton
- LPSC, Université Grenoble-Alpes, CNRS/IN2P3, 38026 Grenoble, France
| | - J McCarter
- University of Virginia, Charlottesville, Virginia 22901, USA
| | - M McCaughan
- Thomas Jefferson National Accelerator Facility, Newport News, Virginia 23606, USA
| | - M McHugh
- The George Washington University, Washington, DC 20052, USA
| | - D McNulty
- Idaho State University, Pocatello, Idaho 83209, USA
| | - K E Mesick
- Rutgers, The State University of New Jersey, Piscataway, New Jersey 08854, USA
| | - T Michaelides
- Thomas Jefferson National Accelerator Facility, Newport News, Virginia 23606, USA
| | - R Michaels
- Thomas Jefferson National Accelerator Facility, Newport News, Virginia 23606, USA
| | - B Moffit
- Thomas Jefferson National Accelerator Facility, Newport News, Virginia 23606, USA
| | - D Moser
- Thomas Jefferson National Accelerator Facility, Newport News, Virginia 23606, USA
| | - C Muñoz Camacho
- IPN, Université Paris-Sud & Université Paris-Saclay, CNRS/IN2P3, 91406 Orsay, France
| | - J-F Muraz
- LPSC, Université Grenoble-Alpes, CNRS/IN2P3, 38026 Grenoble, France
| | - A Opper
- The George Washington University, Washington, DC 20052, USA
| | - M Poelker
- Thomas Jefferson National Accelerator Facility, Newport News, Virginia 23606, USA
| | - J-S Réal
- LPSC, Université Grenoble-Alpes, CNRS/IN2P3, 38026 Grenoble, France
| | - L Richardson
- Thomas Jefferson National Accelerator Facility, Newport News, Virginia 23606, USA
| | - S Setiniyaz
- Idaho State University, Pocatello, Idaho 83209, USA
| | - M Stutzman
- Thomas Jefferson National Accelerator Facility, Newport News, Virginia 23606, USA
| | - R Suleiman
- Thomas Jefferson National Accelerator Facility, Newport News, Virginia 23606, USA
| | - C Tennant
- Thomas Jefferson National Accelerator Facility, Newport News, Virginia 23606, USA
| | - C Tsai
- Virginia Polytechnique Institut and State University, Blacksburg, Virginia 24061, USA
| | - D Turner
- Thomas Jefferson National Accelerator Facility, Newport News, Virginia 23606, USA
| | - M Ungaro
- Thomas Jefferson National Accelerator Facility, Newport News, Virginia 23606, USA
| | - A Variola
- LAL, Université Paris-Sud & Université Paris-Saclay, CNRS/IN2P3, 91898 Orsay, France
| | - E Voutier
- LPSC, Université Grenoble-Alpes, CNRS/IN2P3, 38026 Grenoble, France
- IPN, Université Paris-Sud & Université Paris-Saclay, CNRS/IN2P3, 91406 Orsay, France
| | - Y Wang
- Thomas Jefferson National Accelerator Facility, Newport News, Virginia 23606, USA
| | - Y Zhang
- Rutgers, The State University of New Jersey, Piscataway, New Jersey 08854, USA
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Tvaskis V, Christy ME, Arrington J, Asaturyan R, Baker OK, Blok HP, Bosted P, Boswell M, Bruell A, Cochran A, Cole L, Crowder J, Dunne J, Ent R, Fenker HC, Filippone BW, Garrow K, Gasparian A, Gomez J, Jackson HE, Keppel CE, Kinney E, Lapikás L, Liang Y, Lorenzon W, Lung A, Mack DJ, Martin JW, McIlhany K, Meekins D, Milner RG, Mitchell JH, Mkrtchyan H, Moreland B, Nazaryan V, Niculescu I, Opper A, Piercey RB, Potterveld DH, Rose B, Sato Y, Seo W, Smith G, Spurlock K, van der Steenhoven G, Stepanyan S, Tadevosian V, Uzzle A, Vulcan WF, Wood SA, Zihlmann B, Ziskin V. Longitudinal-transverse separations of deep-inelastic structure functions at low Q2 for hydrogen and deuterium. Phys Rev Lett 2007; 98:142301. [PMID: 17501267 DOI: 10.1103/physrevlett.98.142301] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [What about the content of this article? (0)] [Affiliation(s)] [Abstract] [Track Full Text] [Subscribe] [Scholar Register] [Received: 11/10/2006] [Indexed: 05/15/2023]
Abstract
We report on a study of the longitudinal to transverse cross section ratio, R=sigmaL/sigmaT, at low values of x and Q2, as determined from inclusive inelastic electron-hydrogen and electron-deuterium scattering data from Jefferson Laboratory Hall C spanning the four-momentum transfer range 0.06<Q2<2.8 GeV2. Even at the lowest values of Q2, R remains nearly constant and does not disappear with decreasing Q2, as might be expected. We find a nearly identical behavior for hydrogen and deuterium.
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Affiliation(s)
- V Tvaskis
- Vrije Universiteit, 1081 HV Amsterdam, The Netherlands
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Warren G, Wesselmann F, Zhu H, McKee P, Savvinov N, Zeier M, Aghalaryan A, Ahmidouch A, Arenhövel H, Asaturyan R, Ben-Dayan I, Bloch F, Boeglin W, Boillat B, Breuer H, Brower J, Carasco C, Carl M, Carlini R, Cha J, Chant N, Christy E, Cole L, Coman L, Coman M, Crabb D, Danagoulian S, Day D, Duek K, Dunne J, Elaasar M, Ent R, Farrell J, Fatemi R, Fawcett D, Fenker H, Forest T, Garrow K, Gasparian A, Goussev I, Gueye P, Harvey M, Hauger M, Herrera R, Hu B, Jaegle I, Jones M, Jourdan J, Keith C, Kelly J, Keppel C, Khandaker M, Klein A, Klimenko A, Kramer L, Krusche B, Kuhn S, Liang Y, Lichtenstadt J, Lindgren R, Liu J, Lung A, Mack D, Maclachlan G, Markowitz P, McNulty D, Meekins D, Mitchell J, Mkrtchyan H, Nasseripour R, Niculescu I, Normand K, Norum B, Opper A, Piasetzky E, Pierce J, Pitt M, Prok Y, Raue B, Reinhold J, Roche J, Rohe D, Rondon O, Sacker D, Sawatzky B, Seely M, Sick I, Simicevic N, Smith C, Smith G, Steinacher M, Stepanyan S, Stout J, Tadevosyan V, Tajima S, Tang L, Testa G, Trojer R, Vlahovic B, Vulcan B, Wang K, Wells S, Woehrle H, Wood S, Yan C, Yanay Y, Yuan L, Yun J, Zihlmann B. Measurement of the electric form factor of the neutron at Q2=0.5 and 1.0 GeV2/c2. Phys Rev Lett 2004; 92:042301. [PMID: 14995367 DOI: 10.1103/physrevlett.92.042301] [Citation(s) in RCA: 11] [Impact Index Per Article: 0.6] [Reference Citation Analysis] [What about the content of this article? (0)] [Affiliation(s)] [Abstract] [Track Full Text] [Subscribe] [Scholar Register] [Received: 08/01/2003] [Indexed: 05/24/2023]
Abstract
The electric form factor of the neutron was determined from measurements of the d-->(e-->,e'n)p reaction for quasielastic kinematics. Polarized electrons were scattered off a polarized deuterated ammonia (15ND3) target in which the deuteron polarization was perpendicular to the momentum transfer. The scattered electrons were detected in a magnetic spectrometer in coincidence with neutrons in a large solid angle detector. We find G(n)(E)=0.0526+/-0.0033(stat)+/-0.0026(sys) and 0.0454+/-0.0054+/-0.0037 at Q(2)=0.5 and 1.0 (GeV/c)(2), respectively.
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Affiliation(s)
- G Warren
- Universität Basel, CH-4056 Basel, Switzerland
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4
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Joo K, Smith LC, Burkert VD, Minehart R, Aznauryan IG, Elouadrhiri L, Stepanyan S, Adams GS, Amaryan MJ, Anciant E, Anghinolfi M, Armstrong DS, Asavapibhop B, Audit G, Auger T, Avakian H, Barrow S, Bagdasaryan H, Battaglieri M, Beard K, Bektasoglu M, Bertozzi W, Bianchi N, Biselli AS, Boiarinov S, Bonner BE, Brooks WK, Calarco JR, Capitani GP, Carman DS, Carnahan B, Cole PL, Coleman A, Cords D, Corvisiero P, Crabb D, Crannell H, Cummings J, De Sanctis E, De Vita R, Degtyarenko PV, Demirchyan RA, Denizli H, Dennis LC, Deppman A, Dharmawardane KV, Dhuga KS, Djalali C, Dodge GE, Doughty D, Dragovitsch P, Dugger M, Dytman S, Eckhause M, Efremenko YV, Egiyan H, Egiyan KS, Farhi L, Feuerbach RJ, Ficenec J, Fissum K, Forest TA, Funsten H, Gai M, Gavrilov VB, Gilad S, Gilfoyle GP, Giovanetti KL, Girard P, Griffioen KA, Guidal M, Guillo M, Gyurjyan V, Hancock D, Hardie J, Heddle D, Heisenberg J, Hersman FW, Hicks K, Hicks RS, Holtrop M, Hyde-Wright CE, Ito MM, Jenkins D, Kelley JH, Khandaker M, Kim KY, Kim W, Klein A, Klein FJ, Klusman M, Kossov M, Kuang Y, Kuhn SE, Laget JM, Lawrence D, Longhi A, Loukachine K, Lucas M, Major RW, Manak JJ, Marchand C, Matthews SK, McAleer S, McNabb JWC, Mecking BA, Mestayer MD, Meyer CA, Mirazita M, Miskimen R, Muccifora V, Mueller J, Mutchler GS, Napolitano J, Niculescu G, Niczyporuk B, Niyazov RA, Ohandjanyan MS, Opper A, Patois Y, Peterson GA, Philips S, Pivnyuk N, Pocanic D, Pogorelko O, Polli E, Preedom BM, Price JW, Qin LM, Raue BA, Reolon AR, Riccardi G, Ricco G, Ripani M, Ritchie BG, Ronchetti F, Rossi P, Rowntree D, Rubin PD, Salgado CW, Sanzone M, Sapunenko V, Sargsyan M, Schumacher RA, Sharabian YG, Shaw J, Shuvalov SM, Skabelin A, Smith ES, Smith T, Sober DI, Spraker M, Stoler P, Taiuti M, Taylor S, Tedeschi D, Thompson R, Todor L, Tung TY, Vineyard MF, Vlassov A, Weller H, Weinstein LB, Welsh R, Weygand DP, Whisnant S, Witkowski M, Wolin E, Yegneswaran A, Yun J, Zhou Z, Zhao J. Q2 Dependence of quadrupole strength in the gamma*p --> Delta(+)(1232) --> p pi(0) transition. Phys Rev Lett 2002; 88:122001. [PMID: 11909446 DOI: 10.1103/physrevlett.88.122001] [Citation(s) in RCA: 10] [Impact Index Per Article: 0.5] [Reference Citation Analysis] [What about the content of this article? (0)] [Affiliation(s)] [Abstract] [Track Full Text] [Subscribe] [Scholar Register] [Received: 10/02/2001] [Indexed: 05/23/2023]
Abstract
Models of baryon structure predict a small quadrupole deformation of the nucleon due to residual tensor forces between quarks or distortions from the pion cloud. Sensitivity to quark versus pion degrees of freedom occurs through the Q2 dependence of the magnetic (M1+), electric (E1+), and scalar (S1+) multipoles in the gamma*p-->Delta(+)-->p pi(0) transition. We report new experimental values for the ratios E(1+)/M(1+) and S(1+)/M(1+) over the range Q2 = 0.4-1.8 GeV2, extracted from precision p(e,e(')p)pi(0) data using a truncated multipole expansion. Results are best described by recent unitary models in which the pion cloud plays a dominant role.
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Affiliation(s)
- K Joo
- University of Virginia, Department of Physics, Charlottesville, Virginia 22903, USA
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5
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Thompson R, Dytman S, Kim KY, Mueller J, Adams GS, Amaryan MJ, Anciant E, Anghinolfi M, Asavapibhop B, Auger T, Audit G, Avakian H, Barrow S, Battaglieri M, Beard K, Bektasoglu M, Bertozzi W, Bianchi N, Biselli A, Boiarinov S, Bonner BE, Briscoe WJ, Brooks W, Burkert VD, Calarco JR, Capitani G, Carman DS, Carnahan B, Cole PL, Coleman A, Connelly J, Cords D, Corvisiero P, Crabb D, Crannell H, Cummings J, Day D, Degtyarenko PV, Demirchyan RA, Dennis LC, Deppman A, De Sanctis E, De Vita R, Dhuga KS, Djalali C, Dodge GE, Doughty D, Dragovitsch P, Dugger M, Eckhause M, Efremenko YV, Egiyan H, Egiyan KS, Elouadrhiri L, Farhi L, Feuerbach RJ, Ficenec J, Fissum K, Freyberger A, Funsten H, Gai M, Gavrilov VB, Gilfoyle GP, Giovanetti K, Gilad S, Girard P, Griffioen KA, Guidal M, Guillo M, Gyurjyan V, Hancock D, Hardie J, Heddle D, Heisenberg J, Hersman FW, Hicks K, Hicks RS, Holtrop M, Hyde-Wright CE, Ito MM, Jenkins D, Joo K, Kane J, Khandaker M, Kim W, Klein A, Klein FJ, Klusman M, Kossov M, Kuhn SE, Kuang Y, Laget JM, Lawrence D, Leskin GA, Longhi A, Loukachine K, Lucas M, Magahiz R, Major RW, Manak JJ, Marchand C, Matthews SK, McAleer S, McCarthy J, McNabb JW, Mecking BA, Mestayer MD, Meyer CA, Minehart R, Mirazita M, Miskimen R, Muccifora V, Mutchler GS, Napolitano J, Niyazov RA, Ohandjanyan MS, O'Brien JT, Opper A, Patois Y, Peterson GA, Philips S, Pivnyuk N, Pocanic D, Pogorelko O, Polli E, Preedom BM, Price JW, Qin LM, Raue BA, Reolon AR, Riccardi G, Ricco G, Ripani M, Ritchie BG, Ronchetti F, Rossi P, Roudot F, Rowntree D, Rubin PD, Salgado CW, Sanzone M, Sapunenko V, Sarty A, Sargsyan M, Schumacher RA, Shafi A, Sharabian YG, Shaw J, Shuvalov SM, Skabelin A, Smith T, Smith C, Smith ES, Sober DI, Spraker M, Stepanyan S, Stoler P, Taiuti M, Taylor S, Tedeschi D, Tung TY, Vineyard MF, Vlassov A, Weller H, Weinstein LB, Welsh R, Weygand DP, Whisnant S, Witkowski M, Wolin E, Yegneswaran A, Yun J, Zhou Z, Zhao J. The ep -->e'p eta reaction at and above the S11(1535) baryon resonance. Phys Rev Lett 2001; 86:1702-1706. [PMID: 11290228 DOI: 10.1103/physrevlett.86.1702] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [What about the content of this article? (0)] [Affiliation(s)] [Abstract] [Track Full Text] [Subscribe] [Scholar Register] [Received: 11/08/2000] [Indexed: 05/23/2023]
Abstract
New cross sections for the reaction e p-->e p eta are reported for total center of mass energy W = 1.5--1.86 GeV and invariant momentum transfer Q2 = 0.25--1.5 (GeV/c)(2). This large kinematic range allows extraction of important new information about response functions, photocouplings, and eta N coupling strengths of baryon resonances. Newly observed structure at W approximately 1.65 GeV is shown to come from interference between S and P waves and can be interpreted with known resonances. Improved values are derived for the photon coupling amplitude for the S11(1535) resonance.
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Affiliation(s)
- R Thompson
- Department of Physics and Astronomy, University of Pittsburgh, Pennsylvania 15260, USA
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6
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Murphy L, Mutchler GS, Napolitano J, Niyazov RA, Opper A, O'Brien JT, Philips S, Pivnyuk N, Pocanic D, Pogorelko O, Polli E, Preedom BM, Price JW, Qin LM, Raue BA, Reolon AR, Riccardi G, Ricco G, Ripani M, Ritchie BG, Ronchetti F, Rossi P, Roudot F, Rowntree D, Rubin PD, Salgado CW. Photoproduction of straight phi(1020) mesons on the proton at large momentum transfer. Phys Rev Lett 2000; 85:4682-4686. [PMID: 11082626 DOI: 10.1103/physrevlett.85.4682] [Citation(s) in RCA: 3] [Impact Index Per Article: 0.1] [Reference Citation Analysis] [What about the content of this article? (0)] [Affiliation(s)] [Abstract] [Track Full Text] [Subscribe] [Scholar Register] [Received: 06/16/2000] [Indexed: 05/23/2023]
Abstract
The cross section for straight phi meson photoproduction on the proton has been measured for the first time up to a four-momentum transfer -t = 4 GeV2, using the CLAS detector at the Thomas Jefferson National Accelerator Facility. At low four-momentum transfer, the differential cross section is well described by Pomeron exchange. At large four-momentum transfer, above -t = 1.8 GeV2, the data support a model where the Pomeron is resolved into its simplest component, two gluons, which may couple to any quark in the proton and in the straight phi.
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Affiliation(s)
- L Murphy
- DAPNIA-SPhN, CEA Saclay, F91191 Gif-sur-Yvette Cedex, France
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Kaminetzky HA, Langer A, Baker H, Frank O, Thomson AD, Munves ED, Opper A, Behrle FC, Glista B. The effect of nutrition in teen-age gravidas on pregnancy and the status of the neonate. I. A nutritional profile. Am J Obstet Gynecol 1973; 115:639-46. [PMID: 4687989 DOI: 10.1016/0002-9378(73)90612-1] [Citation(s) in RCA: 33] [Impact Index Per Article: 0.6] [Reference Citation Analysis] [What about the content of this article? (0)] [MESH Headings] [Track Full Text] [Journal Information] [Subscribe] [Scholar Register] [Indexed: 01/11/2023]
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