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Bylaws of the PHENIX Collaboration
This paper contains the bylaws of the PHENIX Collaboration.
Adopted 9/1/1994; Revised: 1/11/96, 10/22/97, 9/9/99, 6/8/00, 6/13/03, 7/19/08, 12/11/08, 2/17/11, 1/9/13, 4/29/1
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THE PHENIX EXPERIMENT AT RHIC.
PHENIX is a large detector at the Relativistic Heavy Ion Collider (RHIC) at BNL. RHIC and PHENIX have recently operated for the first time, producing and detecting collisions of gold ions at beam energies of 30 and 65 GeV per nucleon. The current performance and future plans of PHENIX and of RHIC are presented
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THE PHENIX EXPERIMENT
The PHENIX experiment at RHIC is currently under construction with data collection planned to start in 1999. The heavy ion and spin physics goals of PHENIX are described. The authors discuss the experiment's capabilities to address these physics goals. Highlights of the present status of construction and installation are presented
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The PHENIX experiment at RHIC
The primary goals of the heavy-ion program of the PHENIX collaboration are the detection of the quark-gluon plasma and the subsequent characterization of its physical properties. To address these aims, PHENIX will pursue a wide range of high energy heavy-ion physics topics. The breadth of the physics program represents the expectation that it will require the synthesis of a number of measurements to investigate the physics of the quark-gluon plasma. The broad physics agenda of the collaboration is also reflected in the design of the PHENIX detector itself, which is capable of measuring hadrons, leptons and photons with excellent momentum and energy resolution. PHENIX has chosen to instrument a selective acceptance with multiple detector technologies to provide very discriminating particle identification abilities. Additionally, PHENIX will take advantage of RHIC`s capability to collide beams of polarized protons with a vigorous spin physics program, a subject covered in a separable contribution to these proceedings
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Spin physics with the PHENIX detector system
The PHENIX experiment at RHIC has extended its scope to cover spin physics using polarized proton beams. The major goals of the spin physics at RHIC are elucidation of the spin structure of the nucleon and precision tests of the symmetries. Sensitivities of the spin physics measurements with the PHENIX detector system are reviewed
Personal Papers (MS 80-0002)
Translation of a letter from La Union & Le Phenix Espagnol to Daniel W. Kempner informing him that his car has been involved in an accident and requesting he contact them with his insurance information
Personal Papers (MS 80-0002)
Translation of a letter from La Union & Le Phenix Espagnol to Daniel W. Kempner informing him that his car has been involved in an accident and requesting he contact them with his insurance information
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Phase Transition Signature Results from PHENIX
The PHENIX experiment has conducted searches for the QCD critical point with measurements of multiplicity fluctuations, transverse momentum fluctuations, event-by-event kaon-to-pion ratios, elliptic flow, and correlations. Measurements have been made in several collision systems as a function of centrality and transverse momentum. The results do not show significant evidence of critical behavior in the collision systems and energies studied, although several interesting features are discussed
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TRANSVERSE SPIN AT PHENIX AND FUTURE PLANS.
The PHENIX experiment took data with transversely polarized proton beams in 2001-2002 and measured the transverse single spin asymmetries in inclusive neutral pion and non-identified charge hadrons at midrapidity and {radical} s = 200 GeV. The data near X{sub F} {approx} 0 cover a transverse momentum range from 0.5 to 5.0 GeV/c. The observed asymmetries are consistent with zero with good statistical accuracy. This paper presents the current work in light of earlier measurements at lower energies in this kinematic region and the future plans of the PHENIX detector
Direct Photon Measurement at RHIC-PHENIX.
Results on direct photon measurements from the PHENIX experiment at RHIC are presented. The results suggest that the photons observed are emitted from the initial stage of hard scattering. Comparisons with several theoretical calculations are also presented
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