English
Related papers

Related papers: Transverse Energy Production at RHIC

200 papers

Transverse energy ($E_T$) distributions have been measured for Au+Au collisions at $\sqrt{s_{NN}}= 200$ GeV by the STAR collaboration at RHIC. $E_T$ is constructed from its hadronic and electromagnetic components, which have been measured…

Nuclear Experiment · Physics 2008-11-26 STAR Collaboration , J. Adams

The transverse energy distributions ($E_{T}$) have been measured for Au + Au collisions at $\sqrt{s_{NN}} = 62.4$ GeV by the STAR experiment at RHIC. They have been obtained from two measurements, the hadronic transverse energy…

Transverse energy ($E_T$) has been measured with both of its components, namely hadronic ($E_T^{had}$) and electromagnetic ($E_T^{em}$) in a common phase space at mid-rapidity for 62.4 GeV Au+Au collisions by the STAR experiment. $E_T$…

Nuclear Experiment · Physics 2019-08-13 Raghunath Sahoo

The first measurement of energy produced transverse to the beam direction at RHIC is presented. The mid-rapidity transverse energy density per participating nucleon rises steadily with the number of participants, closely paralleling the…

Nuclear Experiment · Physics 2010-05-28 PHENIX Collaboration , K. Adcox

Transverse energy ($E_T$) has been measured with both of it's components, namely hadronic ($E_T^{had}$) and electromagnetic ($E_T^{em}$) at mid-rapidity, for 62.4 GeV Au+Au collisions by the STAR experiment. In the common phase space of TPC…

Nuclear Experiment · Physics 2009-09-29 Raghunath Sahoo

Preliminary results are presented for two analyses of transverse energy (ET) production measured with the electromagnetic calorimeters of the Pioneering High Energy Nuclear Interaction Experiment (PHENIX), in nuclear interactions in Au+Au…

Nuclear Experiment · Physics 2008-11-26 Raul Armendariz

We study the charged particle and transverse energy production mechanism from AGS, SPS, RHIC to LHC energies in the framework of nucleon and quark participants. At RHIC and LHC energies, the number of nucleons-normalized charged particle…

High Energy Physics - Phenomenology · Physics 2014-05-01 Raghunath Sahoo , Aditya Nath Mishra

The transverse momentum (pt) dependence of J/psi production in heavy ion collisions is investigated in a transport model with both initial production and continuous regeneration of charmonia. The competition between the two production…

Nuclear Theory · Physics 2014-11-18 Yunpeng Liu , Zhen Qu , Nu Xu , Pengfei Zhuang

Study of resonances with their short life-times provides useful tools to probe the properties of hot and dense matter produced in relativistic heavy ion collisions. The high density and/or high temperature of the medium can modify resonance…

Nuclear Experiment · Physics 2019-08-13 Sadhana Dash

Scattering of particles produced in Au+Au collisions at RHIC can wrestle the system into a state near local thermal equilibrium. I illustrate how measurements of the centrality dependence of the mean transverse momentum and its fluctuations…

Nuclear Theory · Physics 2009-11-10 Sean Gavin

Two-particle angular correlation for charged particles emitted in Au+Au collisions at the center-of-mass of 200 MeV measured at RHIC energies revealed novel structures commonly referred to as a near-side ridge. The ridge phenomenon in…

Nuclear Theory · Physics 2011-02-11 M. S. Borysova , Iu. A. Karpenko , Yu. M. Sinyukov

With the experimental data from STAR on the centrality dependence of transverse momentum $p_T$ spectra of pions and protons in Au+Au collisions at $\sqrt{s_{NN}}=200 {\rm GeV}$, we investigate the scaling properties of transverse energy…

Nuclear Theory · Physics 2008-11-26 L. L. Zhu , H. Zheng , C. B. Yang

The STAR Collaboration at RHIC reports measurements of azimuthal correlations of high transverse momentum (p_T) charged hadrons in Au+Au collisions at higher p_T than reported previously. As p_T is increased, a narrow, back-to-back peak…

Nuclear Experiment · Physics 2008-11-26 STAR Collaboration , J. Adams

Complete characterization of particle production and emission in relativistic heavy-ion collisions is in general not feasible experimentally. This work demonstrates, however, that the availability of essentially complete pseudorapidity…

Nuclear Experiment · Physics 2009-11-11 B. B. Back

This paper presents recent results from the BRAHMS experiment at RHIC; including results on particle production in rapidity space extending from y=0 to y ~ 3 and on the transverse momentum distribution of fully identified charged particles.…

Nuclear Experiment · Physics 2019-08-14 R. Debbe

In this study, we systematically investigate the dynamics of various hadrons namely \( \pi^+ \), \( \pi^- \), \( K^+ \), \( K^- \), \( p \), \( \bar{p} \), \( \Lambda \), \( \bar{\Lambda} \), \( \Xi^- \) and \( \bar{\Xi}^+ \) produced in…

High Energy Physics - Phenomenology · Physics 2024-05-16 Murad Badshah , Muhammad Waqas , Muhammad Ajaz , Wolfgang Bietenholz , Haifa I. Alrebdi , Mohamed Ben Ammar

Hypernuclei are bound states of nuclei with one or more hyperons. Precise measurements of hypernuclei properties and their production yields in heavy ion collisions are crucial for the understanding of their production mechanisms. The…

Nuclear Experiment · Physics 2026-05-05 Yuanjing Ji

We study the nuclear enhancement of the transverse momentum imbalance for back-to-back particle production in both p+A and e+A collisions. Specifically, we present results for photon+jet and photon+hadron production in p+A collisions,…

High Energy Physics - Phenomenology · Physics 2012-11-12 Hongxi Xing , Zhong-Bo Kang , Ivan Vitev , Enke Wang

We analyze the transverse momentum distribution of $J/\psi$ mesons produced in Au + Au collisions at the top RHIC energy within a blast-wave model that accounts for a possible inhomogeneity of the charmonium distribution and/or flow…

Nuclear Theory · Physics 2010-04-14 S. V. Akkelin , P. Braun-Munzinger , Yu. M. Sinyukov

This paper reports measurements of the transverse energy per unit pseudorapidity ($dE_{T}/d\eta$) produced in Au+Au collisions at $\sqrt{s_{NN}} = 200$ GeV, performed with the sPHENIX detector at the Relativistic Heavy Ion Collider (RHIC).…

Nuclear Experiment · Physics 2025-09-03 sPHENIX Collaboration , M. I. Abdulhamid , U. Acharya , E. R. Adams , G. Adawi , C. A. Aidala , Y. Akiba , M. Alfred , S. Ali , A. Alsayegh , S. Altaf , H. Amedi , D. M. Anderson , V. V. Andrieux , A. Angerami , N. Applegate , H. Aso , S. Aune , B. Azmoun , V. R. Bailey , D. Baranyai , S. Bathe , A. Bazilevsky , S. Bela , R. Belmont , J. Bennett , J. C. Bernauer , J. Bertaux , R. Bi , A. Bonenfant , S. Boose , C. Borchers , H. Bossi , R. Botsford , R. Boucher , A. Brahma , J. W. Bryan , D. Cacace , I. Cali , M. Chamizo-Llatas , S. B. Chauhan , A. Chen , D. Chen , J. Chen , K. Chen , K. Y. Chen , K. Y. Cheng , C. -Y. Chi , M. Chiu , J. Clement , E. W. Cline , M. Connors , E. Cook , R. Corliss , Y. Corrales Morales , E. Croft , N. d'Hose , A. Dabas , D. Dacosta , M. Daradkeh , S. J. Das , A. P. Dash , G. David , C. T. Dean , K. Dehmelt , X. Dong , A. Drees , J. M. Durham , A. Enokizono , H. Enyo , J. Escobar Cepero , R. Esha , B. Fadem , R. Feder , K. Finnelli , D. Firak , A. Francisco , J. Frantz , A. Frawley , K. Fujiki , M. Fujiwara , B. Garcia , P. Garg , G. Garmire , E. Gentry , Y. Go , C. Goblin , W. Goodman , Y. Goto , A. Grabas , O. Grachov , J. Granato , N. Grau , S. V. Greene , S. K. Grossberndt , R. Guidolini-Cecato , T. Hachiya , J. S. Haggerty , R. Hamilton , J. Hammond , D. A. Hangal , S. Hasegawa , M. Hata , W. He , X. He , T. Hemmick , A. Hodges , M. E. Hoffmann , A. Holt , B. Hong , M. Housenga , S. Howell , Y. Hu , H. Z. Huang , J. Huang , T. C. Huang , D. A. Huffman , C. Hughes , J. Hwang , T. Ichino , M. Ikemoto , D. Imagawa , H. Imai , D. Jah , J. James , H. -R. Jheng , Y. Ji , Z. Ji , H. Jiang , M. Kano , L. Kasper , T. Kato , Y. Kawashima , M. S. Khan , T. Kikuchi , J. Kim , B. Kimelman , H. T. Klest , A. G. Knospe , M. B. Knuesel , H. S. Ko , J. Kuczewski , N. Kumar , R. Kunnawalkam Elayavalli , C. M. Kuo , J. Kvapil , Y. Kwon , J. Lajoie , J. D. Lang , A. Lebedev , S. Lee , L. Legnosky , S. Li , X. Li , T. Lian , S. Liechty , S. Lim , D. Lis , M. X. Liu , W. J. Llope , D. A. Loomis , R. -S. Lu , L. Ma , W. Ma , V. Mahaut , T. Majoros , I. Mandjavidze , E. Mannel , C. Markert , T. R. Marshall , C. Martin , H. Masuda , G. Mattson , M. Mazeikis , C. McGinn , E. McLaughlin , J. Mead , Y. Mei , T. Mengel , M. Meskowitz , J. Mills , A. Milov , C. Mironov , G. Mitsuka , N. Morimoto , D. Morrison , L. W. Mwibanda , C. -J. Naïm , J. L. Nagle , I. Nakagawa , Y. Nakamura , G. Nakano , A. Narde , C. E. Nattrass , D. Neff , S. Nelson , D. Nemoto , P. A. Nieto-Marín , R. Nouicer , G. Nukazuka , E. O'Brien , G. Odyniec , S. Oh , V. A. Okorokov , A. C. Oliveira da Silva , J. D. Osborn , G. J. Ottino , Y. C. Ou , J. Ouellette , D. Padrazo , T. Pani , J. Park , A. Patton , H. Pereira Da Costa , D. V. Perepelitsa , M. Peters , S. Ping , C. Pinkenburg , R. Pisani , C. Platte , C. Pontieri , T. Protzman , M. L. Purschke , J. Putschke , R. J. Reed , L. Reeves , S. Regmi , E. Renner , D. Richford , C. Riedl , T. Rinn , C. Roland , G. Roland , A. Romero Hernandez , M. Rosati , D. Roy , A. Saed , T. Sakaguchi , H. Sako , S. Salur , J. Sandhu , M. Sarsour , S. Sato , B. Sayki , B. Schaefer , J. Schambach , R. Seidl , B. D. Seidlitz , Y. Sekiguchi , M. Shahid , D. M. Shangase , Z. Shi , C. W. Shih , K. Shiina , M. Shimomura , R. Shishikura , E. Shulga , A. Sickles , D. Silvermyr , R. A. Soltz , W. Sondheim , I. Sourikova , P. Steinberg , D. Stewart , S. Stoll , Y. Sugiyama , O. Suranyi , W. -C. Tang , S. Tarafdar , E. Thorsland , T. Todoroki , L. S. Tsai , H. Tsujibata , M. Tsuruta , J. Tutterow , E. Tuttle , B. Ujvari , E. N. Umaka , M. Vandenbroucke , J. Vasquez , J. Velkovska , V. Verkest , A. Vijayakumar , X. Wang , Y. Wang , Z. Wang , I. S. Ward , M. Watanabe , J. Webb , A. Wehe , A. Wils , V. Wolfe , C. Woody , W. Xie , Y. Yamaguchi , Z. Ye , K. Yip , Z. You , G. Young , C. -J. Yu , X. Yu , X. Yu , W. A. Zajc , V. Zakharov , J. Zhang , C. Zimmerli
‹ Prev 1 2 3 10 Next ›