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Featured researches published by J. Amonett.


Physical Review Letters | 2001

Multiplicity Distribution and Spectra of Negatively Charged Hadrons in Au+Au Collisions at

C. Adler; Z. Ahammed; C. Allgower; J. Amonett; B. D. Anderson; M. Anderson; G. S. Averichev; J. Balewski; O. Barannikova; Lee Stuart Barnby

The minimum-bias multiplicity distribution and the transverse momentum and pseudorapidity distributions for central collisions have been measured for negative hadrons ( h(-)) in Au+Au interactions at square root of ([s(NN)]) = 130 GeV. The multiplicity density at midrapidity for the 5% most central interactions is dN(h(-))/d(eta)/(eta = 0) = 280+/-1(stat)+/-20(syst), an increase per participant of 38% relative to pp collisions at the same energy. The mean transverse momentum is 0.508+/-0.012 GeV/c and is larger than in central Pb+Pb collisions at lower energies. The scaling of the h(-) yield per participant is a strong function of p( perpendicular). The pseudorapidity distribution is almost constant within /eta/<1.


Physical Review C | 2004

K(892)* resonance production in Au+Au and p+p collisions at sqrt(sNN) = 200 GeV at RHIC

J. Adams; M. M. Aggarwal; Z. Ahammed; J. Amonett; B. D. Anderson; D. Arkhipkin; G. S. Averichev; S.K. Badyal; Y. Bai; J. Balewski; O. Barannikova; L. S. Barnby; J. Baudot; S. Bekele; V. V. Belaga; R. Bellwied; Joram Berger; B. I. Bezverkhny; S. Bharadwaj; A. Bhasin; A. K. Bhati; V.S. Bhatia; H. Bichsel; A. Billmeier; L. C. Bland; C. O. Blyth; B. E. Bonner; M. Botje; A. Boucham; A. V. Brandin

Author(s): Adams, J.; Aggarwal, M.M.; Ahammed, Z.; Amonett, J.; Anderson, B.D.; Arkhipkin, D.; Averichev, G.S.; Badyal, S.K.; Bai, Y.; Balewski, J.; Barannikova, O.; Barnby, L.S.; Baudot, J.; Bekele, S.; Belaga, V.V.; Bellwied, R.; Berger, J.; Bezverkhny, B.I.; Bharadwaj, S.; Bhasin, A.; Bhati, A.K.; Bhatia, V.S.; Bichsel, H.; Billmeier, A.; Bland, L.C.; Blyth, C.O.; Bonner, B.E.; Botje, M.; Boucham, A.; Brandin, A.V.; Bravar, A.; Bystersky, M.; Cadman, R.V.; Cai, X.Z.; Caines, H.; Calderon de la Barca Sanchez, M.; Castillo, J.; Cebra, D.; Chajecki, Z.; Chaloupka, P.; Chattopadhyay, S.; Chen, H.F.; Chen, Y.; Cheng, J.; Cherney, M.; Chikanian, A.; Christie, W.; Coffin, J.P.; Cormier, T.M.; Cramer, J.G.; Crawford, H.J.; Das, D.; Das, S.; de Moura, M.M.; Derevschikov, A.A.; Didenko, L.; Dietel, T.; Dogra, S.M.; Dong, W.J.; Dong, X.; Draper, J.E.; Du, F.; Dubey, A.K.; Dunin, V.B.; Dunlop, J.C.; Dutta Mazumdar, M.R.; Eckardt, V.; Edwards, W.R.; Efimov, L.G.; Emelianov, V.; Engelage, J.; Eppley, G.; Erazmus, B.; Estienne, M.; Fachini, P.; Faivre, J.; Fatemi, R.; Fedorisin, J.; Filimonov, K.; Filip, P.; Finch, E.; Fine, V.; Fisyak, Y.; Fomenko, K.; Fu, J.The short-lived K(892)* resonance provides an efficient tool to probe properties of the hot and dense medium produced in relativistic heavy-ion collisions. We report measurements of K* in root s(NN)=200 GeV Au+Au and p+p collisions reconstructed via its hadronic decay channels K(892)*(0)-> K pi and K(892)*(+/-)-> K(S)(0)pi(+/-) using the STAR detector at the Relativistic Heavy Ion Collider at Brookhaven National Laboratory. The K*(0) mass has been studied as a function of p(T) in minimum bias p+p and central Au+Au collisions. The K(*) p(T) spectra for minimum bias p+p interactions and for Au+Au collisions in different centralities are presented. The K*/K yield ratios for all centralities in Au+Au collisions are found to be significantly lower than the ratio in minimum bias p+p collisions, indicating the importance of hadronic interactions between chemical and kinetic freeze-outs. A significant nonzero K*(0) elliptic flow (v(2)) is observed in Au+Au collisions and is compared to the K(S)(0) and Lambda v(2). The nuclear modification factor of K* at intermediate p(T) is similar to that of K(S)(0) but different from Lambda. This establishes a baryon-meson effect over a mass effect in the particle production at intermediate p(T) (2 < p(T)<= 4 GeV/c).


Physical Review Letters | 2001

Measurement of Inclusive Antiprotons from Au + Au Collisions at sqrt(sNN) = 130 GeV

C. Adler; Z. Ahammed; C. Allgower; J. Amonett; B. D. Anderson

We report the first measurement of inclusive antiproton production at midrapidity in Au + Au collisions at roots(NN) = 130 GeV by the STAR experiment at RHIC. The antiproton transverse mass distributions in the measured transverse momentum range of 0.25 ) < 0.95 GeV/c are found to fall less steeply for more central collisions. The extrapolated antiproton rapidity density is found to scale approximately with the negative hadron multiplicity density.


Physical Review Letters | 2007

Scaling properties of hyperon production in Au+Au collisons at {radical}{ovr s} {sub NN} = 200 GeV.

R. V. Cadman; K. Krueger; H. M. Spinka; C. J. McClain; D. G. Underwood; J. Adams; M. M. Aggarwal; Z. Ahammed; J. Amonett; M. Anderson

We present the scaling properties of Lambda, Xi, Omega and their anti-particles produced at mid-rapidity in Au+Au collisions at RHIC at sqrt(s_NN) = 200 GeV. The yield of multi-strange baryons per participant nucleon increases from peripheral to central collisions more rapidly than the Lambda yield, which appears to correspond to an increasing strange quark density of matter produced. The value of the strange phase space occupancy factor gamma_s, obtained from a thermal model fit to the data, approaches unity for the most central collisions. We also show that the nuclear modification factors, R_CP, of Lambda and Xi are consistent with each other and with that of protons in the transverse momentum range 2.0<p_T<5.0 GeV/c. This scaling behaviour is consistent with a scenario of hadron formation from constituent quark degrees of freedom through quark recombination or coalescence.


Physical Review Letters | 2006

Direct observation of dijet in central Au+Au collisoins at {radical}{ovr s}{sub NN} = 200 GeV.

R. V. Cadman; K. Krueger; H. M. Spinka; C. J. McClain; D. G. Underwood; J. Adams; M. M. Aggarwal; Z. Ahammed; J. Amonett; M. Anderson

The STAR Collaboration at the Relativistic Heavy Ion Collider reports measurements of azimuthal correlations of high transverse momentum (pT) charged hadrons in Au+Au collisions at higher pT than reported previously. As (pT) is increased, a narrow, back-to-back peak emerges above the decreasing background, providing a clear dijet signal for all collision centralities studied. Using these correlations, we perform a systematic study of dijet production and suppression in nuclear collisions, providing new constraints on the mechanisms underlying partonic energy loss in dense matter.


Physical Review Letters | 2006

Forward neutral pion production in p+p and d+Au collisions at {radical}{ovr s}{sub NN} = 200 GeV.

R. V. Cadman; K. Krueger; C. J. McClain; H. M. Spinka; D. G. Underwood; J. Adams; M. M. Aggrawal; Z. Ahammed; J. Amonett; B. D. Anderson

Measurements of the production of forward pi0 mesons from p+p and d+Au collisions at sqrt(s_NN)=200 GeV are reported. The p+p yield generally agrees with next-to-leading order perturbative QCD calculations. The d+Au yield per binary collision is suppressed as eta increases, decreasing to ~30% of the p+p yield at =4.00, well below shadowing expectations. Exploratory measurements of azimuthal correlations of the forward pi0 with charged hadrons at eta~0 show a recoil peak in p+p that is suppressed in d+Au at low pion energy. These observations are qualitatively consistent with a saturation picture of the low-x gluon structure of heavy nuclei.


Physical Review D | 2006

The multiplicity dependence of inclusive p{sub t} spectra from p-p collisions at {radical}{ovr s} = 200 GeV.

R. V. Cadman; K. Krueger; H. M. Spinka; C. J. McClain; D. G. Underwood; J. Adams; M. M. Aggarwal; Z. Ahammed; J. Amonett; B. D. Anderson

We report measurements of transverse momentum pt spectra forten event multiplicity classes of p-p collisions at sqrt s = 200


Physical Review C | 2006

Proton-{Lambda} correlations in central Au+Au collisions at {radical}{ovr s}{sub NN} = 200 GeV.

R. V. Cadman; K. Krueger; H. M. Spinka; C. J. McClain; D. G. Underwood; J. Adams; M. M. Aggarwal; Z. Ahammed; J. Amonett; B. D. Anderson

GeV. Byanalyzing the multiplicity dependence we find that the spectrum shape canbe decomposed into a part with amplitude proportional to multiplicity anddescribed by a Levy distribution on transverse mass mt, and a part withamplitude proportional to multiplicity squared and described by agaussian distribution on transverse rapidity yt. The functional forms ofthe two parts are nearly independent of event multiplicity. The two partscan be identified with the soft and hard components of a two-componentmodel of p-p collisions. This analysis then provides the first isolationof the hard component of the pt spectrum as a distribution of simple formon yt.


Physical Review C | 2006

Directed flow in Au+Au collisions at {radical}{ovr s}{sub NN} = 62.4 GeV.

R. V. Cadman; K. Krueger; C. J. McClain; H. M. Spinka; D. G. Underwood; J. Adams; M. M. Aggarwal; Z. Ahammed; J. Amonett; B. D. Anderson

We report on p-Lambda, p-Lambda bar, p bar-Lambda and p bar-Lambda bar correlation functions constructed in central Au-Au collisions at sqrt(s_NN)=200GeV by the STAR experiment at RHIC. The proton and lambda source size is inferred from the p-Lambda and p bar-Lambda bar correlation functions. They are found to be smaller than the pion source size also measured by the STAR detector. This could be a consequence of the collision fireballs collective expansion. The p-Lambda bar and p bar-Lambda correlations, which are measured for the first time, exhibit a large anti-correlation. Annihilation channels and/or a negative real part of the spin-averaged scattering length must be included in the final-state interactions calculation to reproduce the measured correlation function.


Physical Review C | 2006

Strange particle production in p + p collisions at {radical}{ovr s} = 200 GeV.

R. V. Cadman; K. Krueger; H. M. Spinka; C. J. McClain; D. G. Underwood; B. I. Abelev; J. Adams; M. M. Aggarwal; Z. Ahammed; J. Amonett

We present the directed flow (v(1)) measured in Au+Au collisions at root s(NN)=62.4 GeV in the midpseudorapidity region parallel to eta parallel to < 1.3 and in the forward pseudorapidity region 2.5 <parallel to eta parallel to < 4.0. The results are obtained using the three-particle cumulant method, the event plane method with mixed harmonics, and for the first time at the Relativistic Heavy Ion Collider, the standard method with the event plane reconstructed from spectator neutrons. Results from all three methods are in good agreement. Over the pseudorapidity range studied, charged particle directed flow is in the direction opposite to that of fragmentation neutrons.

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Z. Ahammed

Variable Energy Cyclotron Centre

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J. Balewski

Indiana University Bloomington

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G. S. Averichev

Joint Institute for Nuclear Research

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H. Bichsel

University of Washington

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D. Arkhipkin

Brookhaven National Laboratory

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L. C. Bland

Indiana University Bloomington

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S. Bekele

Ohio State University

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V. V. Belaga

Joint Institute for Nuclear Research

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