Studies on a Polarized Proton Target for Reactions with Radioactive Ion Beams

Total Page:16

File Type:pdf, Size:1020Kb

Studies on a Polarized Proton Target for Reactions with Radioactive Ion Beams University of Tennessee, Knoxville TRACE: Tennessee Research and Creative Exchange Doctoral Dissertations Graduate School 8-2009 Studies on a Polarized Proton Target for Reactions with Radioactive Ion Beams Juan Pablo Urrego-Blanco University of Tennessee - Knoxville Follow this and additional works at: https://trace.tennessee.edu/utk_graddiss Part of the Physics Commons Recommended Citation Urrego-Blanco, Juan Pablo, "Studies on a Polarized Proton Target for Reactions with Radioactive Ion Beams. " PhD diss., University of Tennessee, 2009. https://trace.tennessee.edu/utk_graddiss/70 This Dissertation is brought to you for free and open access by the Graduate School at TRACE: Tennessee Research and Creative Exchange. It has been accepted for inclusion in Doctoral Dissertations by an authorized administrator of TRACE: Tennessee Research and Creative Exchange. For more information, please contact [email protected]. To the Graduate Council: I am submitting herewith a dissertation written by Juan Pablo Urrego-Blanco entitled "Studies on a Polarized Proton Target for Reactions with Radioactive Ion Beams." I have examined the final electronic copy of this dissertation for form and content and recommend that it be accepted in partial fulfillment of the equirr ements for the degree of Doctor of Philosophy, with a major in Physics. Carroll R. Bingham, Major Professor We have read this dissertation and recommend its acceptance: Alfredo Galindo-Uribarri, Yuri Efremenko, Witold Nazarewicz, Lawrence W. Townsend Accepted for the Council: Carolyn R. Hodges Vice Provost and Dean of the Graduate School (Original signatures are on file with official studentecor r ds.) To the Graduate Council: I am submitting herewith a dissertation written by Juan Pablo Urrego-Blanco entitled “Studies on a Polarized Proton Target for Reactions with Radioactive Ion Beams.” I have examined the final electronic copy of this dissertation for form and content and recommend that it be accepted in partial fulfillment of the requirements for the degree of Doctor of Philosophy, with a major in Physics. Carrol R. Bingham Major Professor We have read this dissertation and recommend its acceptance: Alfredo Galindo-Uribarri Yuri Efremenko Witold Nazarewicz Lawrence W. Townsend Accepted for the Council: Carolyn R. Hodges Vice Provost and Dean of the Graduate School (Original signatures are on file with official student records) Studies on a Polarized Proton Target for Reactions with Radioactive Ion Beams A Dissertation Presented for the Doctor of Philosophy Degree The University of Tennessee, Knoxville Juan Pablo Urrego Blanco August 2009 A mis Padres, a Rolando y Diana, y a Pilar, por supuesto. ii Acknowledgements It is often said that it takes a village to raise a PhD. In my case, that is certainly true. The number of people involved in one way or another with this project is so large that I could not mention everybody here. It is an honor and a pleasure to express my deepest gratitude to all them. However, for the sake of brevity, I will mention here only the people who were involved in a very direct way. I am indebted to Dr. Alfredo Galindo-Uribarri for his close guidance and help throughout these years of graduate school. His passion for Physics and his commitment to the education and well being of his students are an inspiration. His teachings extend far beyond Nuclear Physics and will always accompany me. I am grateful to Professor Carrol Bingham for his continuous support and encouragement. I also acknowledge his help in the analysis of the cross section excitation functions measured at the Holifield Radioactive Ion Beam Facility (HRIBF) in Oak Ridge. I also want to thank the members of my PhD committee for their concern about the development of the project and the valuable comments to this dissertation. The success of this project largely rests upon the contributions and expertise from the Low Temperature Group from the Paul Scherrer Institute (PSI) led by Dr. Ben van den Brandt. Ben and his colleagues Patrick Hautle, and Ton Konter spent many hours training me in the subtleties of low temperature physics and dynamic nuclear polarization. The time spent at PSI with the Group at PSI will remain as one of the richest educational, professional, and personal experiences of my life. I am very thankful to Mr. Paul Schurter, Willi Arrigoni, and Michael Schmutz for their numerous technical contributions to this project, the good times spent in the workshop, and their patience for coping with my poor German. My respect and admiration goes to these gentlemen who demonstrate with their fine work that Swiss precision is no cliché. The in-beam tests of the polarized target were performed with the Phillips Cyclotron at PSI thanks to the willingness and diligent work of Dr. Pierre Schmelzbach and Peter Meyer. Many thanks for that. My sincere thanks to Dr. Elizabeth Padilla-Rodal, who played a critical role during the in-beam tests at PSI and HRIBF. She was always there when she was needed, either to discuss Physics, to help in all sort of technical matters, or simply to cheer me in the difficult moments. iii I am also indebted to Drs. Kamil Sedlak and Toni Shiroka, from the μSR group at PSI, for providing me with the basic GEANT4 routines to simulate the trajectories of charged particles in the magnetic field of the polarized target. The preparation and characterization of thin target foils was possible thanks to the help of Drs Jens Gobrecht, Harald Sehr, and Stela Canulescu from PSI, and Dr. Stefan Blunier from the Institute of Mechanical Systems in ETH-Zurich. Many thanks to Drs. Kurt Klausen, Peter Allenspach, and Michelle Kenzelmann from PSI and to Dr. James Beene, from HRIBF. The support they gave to this project through the leadership of their respective institutions was fundamental for the completion of this work. I am also very grateful to the operations and technical staff from PSI and HRIBF for their collaboration during beam time. It is a pleasure to acknowledge the support of the US Department of Energy through contracts at the University of Tennessee and ORNL, and PSI for the financial support of the research reported in this thesis. Of course, the completion of this project was only possible with a little help from my friends. And I was fortunate enough to get help from both sides of the Ocean. Very special thanks to Perla, Oscar, and Martin for the good times and the many memories we have in Knoxville. Thanks also to Eun Ju for her moral support during the final part of the dissertation. To Ruggero, Loic, Marian, and Nikolai, I can only say Yach’mat! Thanks to you, Switzerland felt like home. I also wish to thank to the friends and family who were cheering for me back at home. Pilar, thanks for helping me with the analysis of the thick target spectra. But of course, your help was much more significant than that. You were my greatest motivation for finishing this work. It was you who always showed me the North, even in the darkest moments. Thanks for being by my side albeit the distance and the long wait. The rest of my life is now yours. I also want to thank my siblings, Rolando and Diana, for thrusting me along the way. Thanks for the advices, the enthusiasm, and the examples you set. I am very proud of being your brother and I am certain that soon you will accomplish far greater things than I have. Finally, I thank the root of everything I have accomplished. Obtaining this degree is, above all, a triumph I owe to my parents. In adverse circumstances you made us believe in the power of education and science, in the value of hard work and honesty, and that if we try hard enough it is possible to reach our dreams. This one is to you, mom and dad. iv Abstract Over the last few years, much progress has been made towards the understanding of basic properties of nuclei with extreme neutron to proton ratios. However, the study of phenomena involving spin polarized nuclei near the drip lines remains practically unexplored. The importance of such studies lies in the fact that the most complete knowledge of the scattering matrix is obtained in reactions with polarized particles. The purpose of this dissertation was to explore the feasibility of using polarized probes in reactions with exotic nuclei. We identified areas where reactions between Radioactive Ion Beams (RIBs) and light polarized targets open a new window of opportunity to study the behavior of those nuclei. These include nuclear structure studies using elastic scattering, the investigation of isolated resonances in nuclei of interest for astrophysics, the study of weakly bound nuclei, one nucleon transfer reactions, and reaction mechanisms. Motivated by these potential applications, we developed a polarized proton target with unique capabilities to operate in reactions with heavy ions at low and intermediate energies. Protons in a plastic foil are polarized using the dynamic nuclear polarization method, which requires low temperature operation (~200 mK) and intense magnetic fields (2.5 T). The foils can be prepared using the spin coating technique, resulting in thicknesses between 100 μg/cm2 and 20 mg/cm2. We have demonstrated operation of the target in frozen spin mode (low magnetic field, e.g., 0.8 T), required for experiments at low energies. For experiments with fast beams the target can be operated in dynamic mode reaching polarizations of up to 30% (B=2.5 T, continuous microwave irradiation). The operational limits of the target have been explored at the Paul Scherrer Institute and at the Holifield Radioactive Ion Beam Facility using the thick target technique with 12C beams at 38 MeV and intensities up to 107 pps, corresponding to the most intense RIBs available.
Recommended publications
  • Some Polarized Target Experiments for Elementary Particle Physics
    SOME POLARIZED TARGET EXPERIMENTS FOR ELEMENTARY PARTICLE PHYSICS R.H. DALITZ Department of Theoretical Physics, Oxford INTRODUCTION At the present stage in elementary particle physics, there are three major areas of phenomena where the use of polarized targets may lead to especially illuminating information. a. High energy scattering, in the energy range where the dominant contributions to the processes observed may arise from Reggion ex­ change. The features of particular interest in these situjtions will be discussed at this meeting by Dr R.J.N. Phillips 1 • b. Tests of time-reversal (T) invariance for electrom~gnetic pro­ cesses, following the suggestion by Bernstein et al 2) that the CF-violation observed in the weak decay of kaons arises from the existence of an electromagnetic interaction which strongly viola­ tes T-invariance. Evidence for this hypothetical T-violating elec­ tromagnetic interaction can be sought most directly in the study of electromagnetic processes from a polarized proton target, for example in the study of the electro-excitation process e + N-+ e + N* , as discussed by Christ and Lee 3J. The experi~ents proposed will be discussed at this meeting by Dr M. Jacob 4J. c. Hadron spectroscopy. Very many resonant states have been obser­ ved for masonic and baryonic states. These hadronic states are be­ lieved to correspond to the patterns appropriate to unitary multi­ plets of states, and these unitary multiplets appear to be grouped in supermultiplet patterns. In our attempt to classify and under­ stand all these hadronic states, our first need is for the deter­ mination of the spin and parity for each state.
    [Show full text]
  • A Peek Into Spin Physics
    A Peek into Spin Physics Dustin Keller University of Virginia Colloquium at Kent State Physics Outline ● What is Spin Physics ● How Do we Use It ● An Example Physics ● Instrumentation What is Spin Physics The Physics of exploiting spin - Spin in nuclear reactions - Nucleon helicity structure - 3D Structure of nucleons - Fundamental symmetries - Spin probes in beyond SM - Polarized Beams and Targets,... What is Spin Physics What is Spin Physics ● The Physics of exploiting spin : By using Polarized Observables Spin: The intrinsic form of angular momentum carried by elementary particles, composite particles, and atomic nuclei. The Spin quantum number is one of two types of angular momentum in quantum mechanics, the other being orbital angular momentum. What is Spin Physics What Quantum Numbers? What is Spin Physics What Quantum Numbers? Internal or intrinsic quantum properties of particles, which can be used to uniquely characterize What is Spin Physics What Quantum Numbers? Internal or intrinsic quantum properties of particles, which can be used to uniquely characterize These numbers describe values of conserved quantities in the dynamics of a quantum system What is Spin Physics But a particle is not a sphere and spin is solely a quantum-mechanical phenomena What is Spin Physics Stern-Gerlach: If spin had continuous values like the classical picture we would see it What is Spin Physics Stern-Gerlach: Instead we see spin has only two values in the field with opposite directions: or spin-up and spin-down What is Spin Physics W. Pauli (1925)
    [Show full text]
  • Polarized Target for the Measurement of the Gluon Contribution to the Nucleon Spin in the COMPASS Experiment
    Polarized target for the measurement of the gluon contribution to the nucleon spin in the COMPASS experiment Nagoya University Thesis for the degree Doctor of Philosophy in Physics by Naoki TAKABAYASHI 1 2002 1 Supported by Research Fellowships of the Japan Society for the Promotion of Science for Young Scientists. CONTENTS 1. Introduction : : : : : : : : : : : : : : : : : : : : : : : : : : : : : : : 1 2. Spin structure of the nucleon : : : : : : : : : : : : : : : : : : : : : 5 2.1 Deep inelastic scattering . 5 2.2 Cross section and structure functions in unpolarized DIS . 7 2.3 Cross section and structure functions in polarized DIS . 9 2.4 Structure functions and spin puzzle in Parton Model picture . 13 2.4.1 Parton distribution . 14 2.4.2 Spin puzzle in Parton Model picture . 16 2.5 Structure functions and spin puzzle in QCD evolved Parton Model . 18 2.5.1 Unpolarized structure functions . 18 2.5.2 Factorization schemes . 20 2.5.3 DGLAP equation and Scaling violation . 22 2.5.4 Spin-dependent structure functions and polarized DGLAP equation . 23 2.6 Interpretation of small ∆Σ. Is gluon contribution large? . 24 2.6.1 Sum rules . 25 2.6.2 Axial anomaly . 26 3. COMPASS experiment : : : : : : : : : : : : : : : : : : : : : : : : : 30 3.1 Open charm lepto-production via photon-gluon fusion . 30 3.2 Expectations . 35 3.2.1 Luminosity . 35 3.2.2 Reconstruction of the open charm events . 35 3.2.3 Statistical accuracy . 37 3.3 Comparison with the other experiments on ∆g . 40 3.3.1 High pT hadron pairs . 40 3.3.2 pp¯ collision . 41 3.3.3 Comparison of the expected precisions and the kine- matic ranges .
    [Show full text]
  • Hadron Spin Dynamics∗
    SLAC-PUB-9107 January 2002 Hadron Spin Dynamics¤ Stanley J. Brodsky Stanford Linear Accelerator Center, Stanford University Stanford, California 94309 e-mail: [email protected] Abstract Spin effects in exclusive and inclusive reactions provide an essential new dimension for testing QCD and unraveling hadron structure. Remarkable new experiments from SLAC, HERMES (DESY), and Jefferson Lab present many challenges to theory, including measurements at HERMES and SMC of the sin- gle spin asymmetries in ep ! e0¼X where the proton is polarized normal to the scattering plane. This type of single spin asymmetry may be due to the effects of rescattering of the outgoing quark on the spectators of the target proton, an effect usually neglected in conventional QCD analyses. Many aspects of spin, such as single-spin asymmetries and baryon magnetic moments are sensitive to the dynamics of hadrons at the amplitude level, rather than probability dis- tributions. I will illustrate the novel features of spin dynamics for relativistic systems by examining the explicit form of the light-front wavefunctions for the two-particle Fock state of the electron in QED, thus connecting the Schwinger anomalous magnetic moment to the spin and orbital momentum carried by its Fock state constituents and providing a transparent basis for understand- ing the structure of relativistic composite systems and their matrix elements in hadronic physics. I also present a survey of outstanding spin puzzles in QCD, particularly ANN in elastic pp scattering, the J=Ã ! ½¼ puzzle, and J=Ã polarization at the Tevatron. Concluding Theory Talk, presented at the 3rd Circum-Pan-Pacific Symposium On High Energy Spin Physics (SPIN 2001) Beijing, China 8–13 October 2001 ¤Work supported by the Department of Energy, contract DE–AC03–76SF00515.
    [Show full text]
  • Solid Polarized Targets for Nuclear and Particle Physics Experiments
    P1: NBL October 6, 1997 15:46 Annual Reviews AR043-03 Annu. Rev. Nucl. Part. Sci. 1997. 47:67–109 Copyright c 1997 by Annual Reviews Inc. All rights reserved ! SOLID POLARIZED TARGETS FOR NUCLEAR AND PARTICLE PHYSICS EXPERIMENTS D. G. Crabb Physics Department, University of Virginia, Charlottesville, Virginia 22901 W. Meyer Institut fur¨ Experimentalphysik I, Ruhr-Universitat¨ Bochum, Bochum, Germany KEY WORDS: dynamic polarization, nucleon spin structure, lepton scattering, cryogenics, asymmetry ABSTRACT The development, in the early 1960s, of the dynamic nuclear polarization process in solid diamagnetic materials, doped with paramagnetic radicals, led to the use of solid polarized targets in numerous nuclear and particle physics experiments. Since then steady progress has been made in all contributing subsystems so that proton polarizations near 100% and deuteron polarizations higher than 50% have been achieved in various materials. More radiation-resistant materials, such as ammonia, have made it possible to perform experiments with high beam intensi- ties and experiments that benefit from 4He cooling at 1K and high magnetic fields. The development of dilution refrigerators have allowed frozen spin operation so that experiments with large angular acceptance for the scattered particles have by University of Virginia Libraries on 05/18/07. For personal use only. become routine. Many experiments have taken advantage of these developments and many more are being planned, especially with electromagnetic probes. Annu. Rev. Nucl. Part. Sci. 1997.47:67-109. Downloaded from arjournals.annualreviews.org CONTENTS 1. INTRODUCTION . 68 2. POLARIZATION MECHANISMS . 71 2.1 Thermal Equilibrium Polarization . 72 2.2 Solid-State Effect . 72 2.3 Equal Spin Temperature Theory .
    [Show full text]
  • DEUTERON POLARIZED TARGET for Nd EXPERIMENTS at THE
    DEUTERON FROZEN SPIN POLARIZED TARGET FOR nd EXPERIMENTS AT THE VdG ACCELERATOR OF CHARLES UNIVERSITY N.S. Borisov1, N.A. Bazhanov1, A.A. Belyaev4, J. Brož2, J. Černý2, Z. Doležal2, A.N. Fedorov1, G.M. Gurevich3, M.P. Ivanov1, P. Kodyš2, P. Kubík2, E.S. Kuzmin1, A.B. Lazarev1, F. Lehar5,6 , O.O. Lukhanin4, V.N. Matafonov†1, A.B. Neganov1, I.L. Pisarev1, J. Švejda2, S.N. Shilov1, Yu.A. Usov1 and I.Wilhelm2 1Joint Institute for Nuclear Research, Dubna, Russia; 2Institute of Particle and Nuclear Physics, Faculty of Mathematics and Physics, Charles University in Prague; V Holešovičkách 2, CZ18000 Prague 8, Czech Republic; 3Institute for Nuclear Research, Russian Academy of Sciences, Moscow, Russia; 4NSC KIPT, Kharkov, 5SPP DAPNIA CEA Saclay, F-91190 Gif sur Yvette, France 6IEAP CTU, Horska 3a/22 CZ 12800 Prague 2, Czech Republic Abstract. A frozen spin polarized deuteron target cooled by the 3He/4He dilution refrigerator is described. Fully deuterated 1,2-propanediol was used as a target material. Deuteron vector polarization about 40% was obtained for the target in the shape of a cylinder of 2 cm diameter and 6 cm length. The target is intended for a study of 3N interactions at the polarized neutron beam generated by the Van de Graaff accelerator at the Charles University in Prague. 1. Introduction The Charles University proton polarized target (PPT) [1] has been used previously to measure spin–dependent total cross section differences ∆σT and ∆σL in neutron-proton scattering at the 16.2 MeV polarized neutron beam of the VdG accelerator (Fig.1) [2, 3].
    [Show full text]
  • Helicity Density Matrix Formalism and Polarized Processes in QCD Jian Tang
    Helicity Density Matrix Formalism and Polarized Processes in QCD by Jian Tang B.S., Peking University, P.R. China (1991) M.S., Peking University, P.R. China (1994) M.S., Massachusetts Institute of Technology (1996) Submitted to the Department of Physics in partial fulfillment of the requirements for the degree of Doctor of Philosophy in Physics at the MASSACHUSETTS INSTITUTE OF TECHNOLOGY June 1999 © Massachusetts Institute of Technology 1999. All rights reserved. A uthor ........... ................... Department of Physics May 26, 1999 C ertified bA ............................... Robert L. Jaffe Professor Thesis Supervisor A ccepted by ......................... T(omas J. reytak Professor, Associate Department Head for ducation MASSACHUSETTS INSTITUTE T1999 LIBRARIES Helicity Density Matrix Formalism and Polarized Processes in QCD by Jian Tang Submitted to the Department of Physics on May 26, 1999, in partial fulfillment of the requirements for the degree of Doctor of Philosophy in Physics Abstract In this thesis, we shall first present helicity density matrix formalism to deal with the polarized processes in quantum chromodynamics(QCD), in which the calculations of the desired cross sections (or asymmetries in many cases) are simplified to take traces of products of helicity density matrices in the underlying particles' (partons, hadrons, etc.) helicity spaces. The parton distribution and fragmentation functions turn out to be the helicity density matrix elements which survive the QCD symmetries. The main advantages of this formalism are that it has very clear physical pictures, simplifies the calculation, and, most importantly, can be easily used to deal with interference effects between different partial waves in multiparticle production in semi-inclusive processes. Then this formalism will be used to propose new ways to measure nu- cleon's transversity, the least known quark distribution function inside the nucleon at leading twist (twist-two).
    [Show full text]
  • The Deuteron Tensor Structure Function B1
    The Deuteron Tensor Structure Function b1 A Proposal to Jefferson Lab PAC-40 (Update to PR12-11-110) K. Allada, A. Camsonne, J.-P. Chen,† A. Deur, D. Gaskell, M. Jones, C. Keith, J. Pierce, P. Solvignon,† S. Wood, J. Zhang Thomas Jefferson National Accelerator Facility, Newport News, VA 23606 O. Rondon Aramayo,† D. Crabb, D. B. Day, C. Hanretty, D. Keller,† R. Lindgren, S. Liuti, B. Norum, Zhihong Ye, X. Zheng University of Virginia, Charlottesville, VA 22903 N. Kalantarians† Hampton University, Hampton VA 23668 T. Badman, J. Calarco, J. Dawson, S. Phillips, E. Long,† K. Slifer†‡, R. Zielinski University of New Hampshire, Durham, NH 03861 G. Ron Hebrew University of Jerusalem, Jerusalem W. Bertozzi, S. Gilad, J. Huang A. Kelleher, V. Sulkosky Massachusetts Institute of Technology, Cambridge, MA 02139 †Spokesperson ‡Contact J. Dunne, D. Dutta Mississippi State University, Mississippi State, MS 39762 K. Adhikari Old Dominion University, Norfolk, VA 23529 R. Gilman Rutgers, The State University of New Jersey, Piscataway, NJ 08854 Seonho Choi, Hoyoung Kang, Hyekoo Kang, Yoomin Oh Seoul National University, Seoul 151-747 Korea H. P. Cheng, H. J. Lu, X. H. Yan Institute of Applied Physics, Huangshan University, Huangshan, P. R. China Y. X. Ye, P. J. Zhu University of Science and Technology of China, Hefei 230026, P. R. China B. T. Hu, Y. Zhang Lanzhou University, Lanzhou, P. R. China. Abdellah Ahmidouch Department of Physics, North Carolina A & T State University, Greensboro, NC 27401 Caroline Riedl DESY, Notkestrasse 85, 22603 Hamburg, Germany Abstract The leading twist tensor structure function b1 of spin-1 hadrons provides a unique tool to study partonic effects, while also being sensitive to coherent nuclear properties in the simplest nuclear system.
    [Show full text]
  • Spin Structure of the Proton from Polarized Inclusive Deep-Inelastic Muon-Proton Scattering
    PHYSICAL REVIEW D VOLUME 56, NUMBER 9 1 NOVEMBER 1997 Spin structure of the proton from polarized inclusive deep-inelastic muon-proton scattering D. Adams,17 B. Adeva,19 E. Arik,2 A. Arvidson,22,a B. Badelek,22,24 M. K. Ballintijn,14 G. Bardin,18,b G. Baum,1 P. Berglund,7 L. Betev,12 I. G. Bird,18,c R. Birsa,21 P. Bjo¨rkholm,22,d B. E. Bonner,17 N. de Botton,18 M. Boutemeur,25,e F. Bradamante,21 A. Bravar,10 A. Bressan,21 S. Bu¨ltmann,1,f E. Burtin,18 C. Cavata,18 D. Crabb,23 J. Cranshaw,17,g T. C¸ uhadar,2 S. Dalla Torre,21 R. van Dantzig,14 B. Derro,3 A. Deshpande,25 S. Dhawan,25 C. Dulya,3,h A. Dyring,22 S. Eichblatt,17,i J. C. Faivre,18 D. Fasching,16,j F. Feinstein,18 C. Fernandez,19,8 B. Frois,18 A. Gallas,19 J. A. Garzon,19,8 T. Gaussiran,17,k M. Giorgi,21 E. von Goeler,15 G. Gracia,19,h N. de Groot,14,l M. Grosse Perdekamp,3,m E. Gu¨lmez,2 D. von Harrach,10 T. Hasegawa,13,n P. Hautle,4,o N. Hayashi,13,p C. A. Heusch,4,q N. Horikawa,13 V. W. Hughes,25 G. Igo,3 S. Ishimoto,13,r T. Iwata,13 E. M. Kabuß,10 A. Karev,9 H. J. Kessler,5 T. J. Ketel,14 A. Kishi,13 Yu. Kisselev,9 L. Klostermann,14,s D.
    [Show full text]
  • Future Plans for the MP Line (Both General and Specific)
    Proceedings of the Symposium on Future Polarization Physics + at Fermilab 13-14 June 1988 F0T0RE PLAUS FOR THE MP LINET ANL-HEP-CP-88-54 (Both General and Specific) /''/"•/\ l::r- /'/'"' P- J 7 David G. Underwood Argonne National Laboratory, Argonne. Illinois 60439 ANL-HEP-CP—88-54 ABSTRACT DE89 003972 This talk consists of three sections. Topics range from suggestions of possible physics, which are presented to provoke thought and discussion about the distant future, to specific goals of E-704 for the next running period. The sections are on physics issues, possible upgrades of the beam and experimental apparatus, and goals for the next running period. PHYSICS ISSUES Many of the experiments and issues discussed at this symposium were viewed with renewed interest in light of the recent EMC results concerning the spin distribution functions for quarks in protons at low x.1 There appear to be Rajor contributions to the overall spin of the proton from either gluon spin or orbital angular momentum. We have heard a talk by Karliner at this symposium and there are a number of papers and activities in progress. Polarized proton beams may assume greater importance in the future because the polarised quarks carry color charge which can couple directly to gluons. Deep inelastic scattering utilizing either electrons or muons has been efficacious because of the electrical charge of the quark. Gluons are not electrically charged. We recall that the large xBj leading quark of a polarized protou is known to carry most of the proton spin, and so is a good probe.
    [Show full text]
  • New Perspectives 2019 Joshua Hoskins University of Virginia
    High Luminosity Spin-Polarized Target for the SpinQuest Experiment New Perspectives 2019 Joshua Hoskins University of Virginia Polarized Target Group Overview ● SpinQuest experiment at Fermilab ● Spin Polarized Solid Targets 2 Proton’s Spin Structure Central challenge of nuclear physics: to disentangle constituents and spin structure of the nucleon. Since the proposal of the parton model our understanding of the nuclear constituents, quarks and gluons, has grown immensely. The EMC experiment, by the discovery that the contribution of the spins of the quark and anti-quark to the proton’s spin was 12 ± 17%, sparked a multi-decade program with the purpose of understanding the spin structure of the proton. 1 1 = Δ Σ+L +L +Δ G+L 2 2 q ¯q g Tremendous progress has been made in understanding how the nucleon spin is made up from its quark and gluon constituents. The current best estimate of the contribution of the quark and anti-quark spin to the proton’s spin is only ~30%. 3 Spin Physics and E1039 (SpinQuest) SpinQuest proposes direct measurement of the sea-quark Sivers function, using Drell-Yan productions from unpolarized 120 GeV proton beam on a transversely polarized proton (neutron) target. Sivers function – one of eight transverse momentum distribution functions (TMD), describing the correlation of the transverse momentum of an unpolarized parton with the spin of a polarized nucleon. Interest in the contributions of the orbital motion of the sea quarks → data are 1 1 = Δ Σ+L +L +Δ G+L severely lacking. 2 2 q ¯q g → HERMES, COMPASS, Jefferson Lab have provided measurements of the Sivers Function via semi-inclusive deep inelastic scattering (SIDIS); Sivers function convoluted with fragmentation function.
    [Show full text]
  • Introduction to Solid Polarized Targets for Nuclear and Particle Physics
    Introduction to Solid Polarized Targets for Nuclear and Particle Physics Chris Keith JLab Target Group Target Group 6 February 2019 1 The basics Spin is an intrinsic property of all elementary particles As well as many composite particles (pay no attention to the higgs) (baryons, mesons, nuclei, atoms…) Target Group 6 February 2019 2 The basics A polarized target is a collection of nuclei (solid or gas) used for a scattering experiment in which most the nuclear spins point in the same direction Target Group 6 February 2019 3 Uses for polarized targets • HALL A Spin structure of hadrons (E12-11-108) SIDIS with a transversely polarized proton target • Sum rules (E12-11-108A) Target single spin asymmetries using SoLID spectrometer • Form Factors • Baryon spectroscopy HALL B (E12-06-109) Longitudinal spin structure of the nucleon • Transverse momentum distributions (E12-06-119) DVCS with CLAS at 12 GeV • Generalized parton distributions (E12-07-107) Spin-orbit correlations with a longitudinally polarized target (E12-09-009) Spin-orbit correlations in kaon electroproduction in DIS • Polarized PDFs (E12-14-001) EMC effect in spin structure functions (6LiH & 7LiD) (E12-15-004) DVCS on the neutron with a longitudinally polarized target (C12-11-111) SIDIS on a transversely polarized target (C12-12-009) Dihadron production in SIDIS on a transversely pol. target (C12-12-010) DVCS on a transversely polarized target in CLAS12 HALL C (E12-14-006) Helicity correlations in wide-angle Compton scattering (C12-13-011) The deuteron tensor structure function b1 (C12-15-005) Meas. of quasi-elastic and elastic deuteron tensor asymm.
    [Show full text]