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Languages : en
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Languages : en
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Author: Yasar Onel
Publisher: World Scientific
ISBN: 9814547115
Category :
Languages : en
Pages : 322

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The volume presents an up-to-date survey of spin physics at the very high energies of present and future colliders. Topics discussed include the theory of high-energy spin physics, deep-inelastic scattering, polarization experiments at colliders, the production of high-energy polarized electron and proton beams, the construction of intense polarized sources and high-energy polarimeters. It will represent a significant reference in the field and an informative text for non-specialists as well, with rather complete keynote overview reports by some physicists who have contributed most to the subject. In addition, it will document the character of frontier research symposium of the Conference, with specialized reports of leading experts in the various items of the field.

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Category :
Languages : en
Pages :

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Author: Nobuhiko Saitō
Publisher:
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Category :
Languages : en
Pages : 4

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Author:
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ISBN:
Category :
Languages : en
Pages : 17

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Colliding beams of high energy polarized protons at RHIC is an excellent way to probe the polarization of gluons, u and d quarks in a polarized proton. RHIC is the Relativistic Heavy Ion Collider being built now at Brookhaven in the ISABELLE tunnel. It is designed to collide gold ions on gold ions at 100 GeV/nucleon. Its goal is to discover the quark-gluon plasma, and the first collisions are expected in March, 1999. RHIC will also make an ideal polarized proton collider with high luminosity and 250 GeV x 250 GeV collisions. The RHIC spin physics program is: (1) Use well-understood perturbative QCD probes to study non-perturbative confining dynamics in QCD. We will measure - gluon and sea quark polarization in a polarized proton, polarization of quarks in a transversely polarized proton. (2) Look for additional surprises using the first high energy polarized proton collider. We will - look for the expected maximal parity violation in W and Z boson production, - search for parity violation in other processes, - test parton models with spin. This lecture is organized around a few of the key ideas: Siberian Snakes--What are they? High energy proton-proton collisions are scatters of quarks and leptons, at high x, a polarized proton beam is a beam of polarized u quarks, quark and gluon collisions are very sensitive to spin. We will discuss two reactions: how direct photon production measures gluon polarization, and how W boson production measures u and d quark polarization.

Author: S. ARONSON
Publisher:
ISBN:
Category :
Languages : en
Pages : 10

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The Relativistic Heavy Ion Collider (RHIC) at BNL is the world's only polarized proton-proton collider. Collisions at center-of-mass energies up to 500 GeV and beam polarizations approaching 70% (longitudinal or transverse) are provided to two experiments, STAR and PHENIX, at luminosities {ge} 10{sup 32}/cm{sup 2}/sec. Transverse polarized beam has also been provided to the BRAHMS experiment. Measurements that bear on the important question of the spin content of the nucleon are beginning to appear. Over the next 10 years, as the performance of polarized proton running at RHIC is further developed, the Spin Physics program at RHIC will provide definitive measurements of the contributions to the proton's spin of the gluon, the sea quarks and the orbital motion of the partons in the proton's wave function. We plan to extend the reach of our study of the role of spin in QCD with the development of ''eRHIC'', which will provide polarized e-p collisions to a new detector.

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Category :
Languages : en
Pages : 19

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Colliding beams of high energy polarized protons at RHIC is an excellent way to probe the polarization of gluons, {anti u} and {anti d} quarks in a polarized proton. RHIC is the Relativistic Heavy Ion Collider being built now at Brookhaven in the ISABELLE tunnel. It is designed to collide gold ions on gold ions at 100 GeV/ nucleon. Its goal is to discover the quark-gluon plasma, and the first collisions are expected in March, 1999. RHIC will also make an ideal polarized proton collider with high luminosity and 250 GeV x 250 GeV collisions. The RHIC spin physics program is: (1) Use well-understood perturbative QCD probes to study non-perturbative confining dynamics in QCD. The author will measure gluon and sea quark polarization in a polarized proton, and polarization of quarks in a transversely polarized proton. (2) Look for additional surprises using the first high energy polarized proton colliders. The author will look for the expected maximal parity violation in W and Z boson production, search for parity violation in other processes, and test parton models with spin. This lecture is organized around a few of the key ideas: Siberian Snakes -- What are they? High energy proton-proton collisions are scatters of quarks and leptons. At high x, a polarized proton beam is a beam of polarized u quarks. Quark and gluon collisions are very sensitive to spin. The author discusses two reactions: how direct photon production measures gluon polarization, and how W− boson production measures u and {anti d} quark polarization.

Author: P. Lo Presti
Publisher:
ISBN:
Category : Colliders (Nuclear physics)
Languages : en
Pages : 210

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ISBN:
Category :
Languages : en
Pages : 4

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The Relativistic Heavy Ion Collider (RHIC) is the centerpiece of the nuclear physics program at Brookhaven National Laboratory. The physics program encompasses both heavy ion physics and spin physics with polarized protons. A series of three accelerators provide the ions for injection into the two counter-rotating RHIC accelerator-collider rings. A fourth machine, the proton linac, provides polarized protons to the injector chain. RHIC has been designed to accelerate and collide all ion species from protons to uranium. We are presently limited to a mass of gold by the tandem preinjector limitations. RHIC has accelerated and stored gold ions for data taking from the injection energy of 10 GeV/nucleon to a maximum of 100 GeV/nucleon. Polarized protons have been delivered at 100 GeV for physics data taking. Most of the design parameters of RHIC have been achieved. The number of beam bunches, emittances, energy, bunch length and inter-section region optics parameters have been achieved. Beam intensity is routinely available at 75% of design and the average luminosity is presently at 30% of design value.