Pseudorapidity Asymmetry And Centrality Dependence Of Charged Hadron Spectra In D Au Collisions At Sqrtsnn PDF Download

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Pseudorapidity Asymmetry and Centrality Dependence of Charged Hadron Spectra in D+Au Collisions at Sqrt(sNN)

Pseudorapidity Asymmetry and Centrality Dependence of Charged Hadron Spectra in D+Au Collisions at Sqrt(sNN)
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Release: 2005
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The pseudorapidity asymmetry and centrality dependence of charged hadron spectra in d+Au collisions at (square root)s{sub NN} = 200 GeV are presented. The charged particle density at mid-rapidity, its pseudorapidity asymmetry and centrality dependence are reasonably reproduced by a Multi-Phase Transport model, by HIJING, and by the latest calculations in a saturation model. Ratios of transverse momentum spectra between backward and forward pseudorapidity are above unity for p{sub T} below 5 GeV/c. The ratio of central to peripheral spectra in d+Au collisions shows enhancement at 2


Studies of Nucleon-gold Collisions at 200 GeV Per Nucleon Pair Using Tagged D+Au Interactions

Studies of Nucleon-gold Collisions at 200 GeV Per Nucleon Pair Using Tagged D+Au Interactions
Author: Corey James Reed
Publisher:
Total Pages: 215
Release: 2006
Genre:
ISBN:

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(Cont.) Further, hadron production in p+Au interactions is compared to that of n+Au interactions. The single charge difference between a p+Au and a n+Au collision allows for a unique study of the ability of the interaction to transport the proton from the initial deuteron to mid-rapidity. However, no asymmetry between the positively and negatively charged hadron spectra of p+Au and n+Au interactions is observed at (qr) = 0.8. Collision centrality was determined using several different observables, including those based on the multiplicity in different regions of pseudorapidity and those based on the amount of nuclear spectator material. It is shown that measurements made on small collision systems in the mid-rapidity region are biased by centrality variables based on the mid-rapidity multiplicity. Despite this bias, a smooth evolution with centrality is observed in the Cronin enhancement of hadrons produced in d+Au collisions. It is shown that this smooth progression is independent of the choice of centrality variable when centrality is parametrized by the multiplicity measured near mid-rapidity.


Charged Hadron Transverse Momentum Spectra in Au+Au and D+Au Collisions at 200 GeV Per Nucleon Pair

Charged Hadron Transverse Momentum Spectra in Au+Au and D+Au Collisions at 200 GeV Per Nucleon Pair
Author: Jay Lawrence Kane
Publisher:
Total Pages: 235
Release: 2005
Genre:
ISBN:

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(Cont.) When ... is calculated for different rapidities, a suppression is seen as the rapidity in the deuteron fragmentation region increases. This has been predicted to be seen if a CGC does form in the colliding nuclei.


Long-range Pseudorapidity Dihadron Correlations in D + Au Collisions at {u221A}SNN

Long-range Pseudorapidity Dihadron Correlations in D + Au Collisions at {u221A}SNN
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Total Pages: 7
Release: 2015
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ISBN:

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Dihadron angular correlations in d + Au collisions at √sNN = 200 GeVare reported as a function of the measured zero-degree calorimeter neutral energy and the forward charged hadron multiplicity in the Au-beam direction. A finite correlated yield is observed at large relative pseudorapidity (? ?) on the near side (id est relative azimuth ? ? ̃0). This correlated yield as a function of ?? appears to scale with the dominant, primarily jet-related, away-side (? ? ̃?) yield. The Fourier coefficients of the ?? correlation, Vn = cosn ?? , have a strong ?? dependence. In addition, it is found that V1 is approximately inversely proportional to the mid-rapidity event multiplicity, while V2 is independent of it with similar magnitude in the forward (d-going) and backward (Au-going) directions.


Rapidity and Species Dependence of Particle Production at Largetransverse Momentum for D+Au Collisions at PsNN

Rapidity and Species Dependence of Particle Production at Largetransverse Momentum for D+Au Collisions at PsNN
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Total Pages:
Release: 2006
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ISBN:

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We determine rapidity asymmetry in the production of charged pions, protons and anti-protons for large transverse momentum (p{sub T}) for d+Au collisions at √s{sub NN} = 200 GeV. The rapidity asymmetry is defined as the ratio of particle yields at backward rapidity (Au beam direction or -ve rapidity) to those at forward rapidity (d beam direction or +ve rapidity). The identified hadrons are measured in the rapidity regions.


PHENIX Results on Centrality Dependence of Yields and Correlations in D Plus Au Collisions at Root S(NN)

PHENIX Results on Centrality Dependence of Yields and Correlations in D Plus Au Collisions at Root S(NN)
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Total Pages: 6
Release: 2016
Genre:
ISBN:

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PHENIX has measured the transverse momentum (pT) spectra and two particle angular correlations for high pT particles in d+Au collisions at psNN=200 GeV using the RHIC Year-2008 run data. The azimuthal angle correlations for two particles with a large rapidity gap exhibit a ridge-like structure. Using the pi-0s reconstructed in the EMCal, we have successfully extended the pT reach of the correlation up to 8 GeV/c. We find that the azimuthal anisotropy of hadrons found at low pT persists up to 6 GeV/c with a significant centrality and pT dependence, similar to what was observed in A+A collisions.


Pion, Kaon, Proton and Anti-proton Transverse Momentum Distributions from P+p and D+Au Collisions at Sqrt(sNN)

Pion, Kaon, Proton and Anti-proton Transverse Momentum Distributions from P+p and D+Au Collisions at Sqrt(sNN)
Author:
Publisher:
Total Pages: 6
Release: 2003
Genre:
ISBN:

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Identified mid-rapidity particle spectra of [pi]{sup ±}, K{sup ±}, and p({bar p}) from 200 GeV p+p and d+Au collisions are reported. A time-of-flight detector based on multi-gap resistive plate chamber technology is used for particle identification. The particle-species dependence of the Cronin effect is observed to be significantly smaller than that at lower energies. The ratio of the nuclear modification factor (R{sub dAu}) between (p+ {bar p}) and charged hadrons (h) in the transverse momentum range 1.2