Open Bottom Production in Au Au Collisions at √<span style="text-decoration: overline;"><em>s</em><sub>NN</sub></span> = 200 GeV with the STAR Experiment
In these proceedings, we present measurements of open bottom hadron production through multiple decay channels in Au + Au collisions at <inline-formula> <math display="inline"> <semantics> <msqrt> <msub> <mi>s</mi> <msub> <mrow></mro...
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doaj-c2b9ada8abbe4e8fa074a5133cc9908b2020-11-24T21:44:53ZengMDPI AGProceedings2504-39002019-04-011013910.3390/proceedings2019010039proceedings2019010039Open Bottom Production in Au Au Collisions at √<span style="text-decoration: overline;"><em>s</em><sub>NN</sub></span> = 200 GeV with the STAR ExperimentShenghui Zhang0Department of Modern Physics, University of Science and Technology of China (USTC), Hefei 230026, ChinaIn these proceedings, we present measurements of open bottom hadron production through multiple decay channels in Au + Au collisions at <inline-formula> <math display="inline"> <semantics> <msqrt> <msub> <mi>s</mi> <msub> <mrow></mrow> <mi>NN</mi> </msub> </msub> </msqrt> </semantics> </math> </inline-formula> = 200 GeV by the STAR experiment. Specifically, measurements of nuclear modification factors for electrons, <inline-formula> <math display="inline"> <semantics> <mrow> <mi>J</mi> <mo>/</mo> <mi>ψ</mi> </mrow> </semantics> </math> </inline-formula>, and <inline-formula> <math display="inline"> <semantics> <msup> <mi>D</mi> <mn>0</mn> </msup> </semantics> </math> </inline-formula> from open bottom hadron decays, enabled by the Heavy Flavor Tracker, are shown. A large suppression for non-prompt <inline-formula> <math display="inline"> <semantics> <mrow> <mi>J</mi> <mo>/</mo> <mi>ψ</mi> </mrow> </semantics> </math> </inline-formula> and non-prompt <inline-formula> <math display="inline"> <semantics> <msup> <mi>D</mi> <mn>0</mn> </msup> </semantics> </math> </inline-formula> are observed at high transverse momenta. On the other hand, there seems to be less suppression for electrons from bottom hadron decays than for those from charm hadron decays at ∼<inline-formula> <math display="inline"> <semantics> <mrow> <mn>2</mn> <mi>σ</mi> </mrow> </semantics> </math> </inline-formula> significance level.https://www.mdpi.com/2504-3900/10/1/39open bottom productionnuclear modification factorsnon-prompt J/ψnon-prompt D0electrons from bottom hadron decaysquark-gluon plasma |
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DOAJ |
language |
English |
format |
Article |
sources |
DOAJ |
author |
Shenghui Zhang |
spellingShingle |
Shenghui Zhang Open Bottom Production in Au Au Collisions at √<span style="text-decoration: overline;"><em>s</em><sub>NN</sub></span> = 200 GeV with the STAR Experiment Proceedings open bottom production nuclear modification factors non-prompt J/ψ non-prompt D0 electrons from bottom hadron decays quark-gluon plasma |
author_facet |
Shenghui Zhang |
author_sort |
Shenghui Zhang |
title |
Open Bottom Production in Au Au Collisions at √<span style="text-decoration: overline;"><em>s</em><sub>NN</sub></span> = 200 GeV with the STAR Experiment |
title_short |
Open Bottom Production in Au Au Collisions at √<span style="text-decoration: overline;"><em>s</em><sub>NN</sub></span> = 200 GeV with the STAR Experiment |
title_full |
Open Bottom Production in Au Au Collisions at √<span style="text-decoration: overline;"><em>s</em><sub>NN</sub></span> = 200 GeV with the STAR Experiment |
title_fullStr |
Open Bottom Production in Au Au Collisions at √<span style="text-decoration: overline;"><em>s</em><sub>NN</sub></span> = 200 GeV with the STAR Experiment |
title_full_unstemmed |
Open Bottom Production in Au Au Collisions at √<span style="text-decoration: overline;"><em>s</em><sub>NN</sub></span> = 200 GeV with the STAR Experiment |
title_sort |
open bottom production in au au collisions at √<span style="text-decoration: overline;"><em>s</em><sub>nn</sub></span> = 200 gev with the star experiment |
publisher |
MDPI AG |
series |
Proceedings |
issn |
2504-3900 |
publishDate |
2019-04-01 |
description |
In these proceedings, we present measurements of open bottom hadron production through multiple decay channels in Au + Au collisions at <inline-formula> <math display="inline"> <semantics> <msqrt> <msub> <mi>s</mi> <msub> <mrow></mrow> <mi>NN</mi> </msub> </msub> </msqrt> </semantics> </math> </inline-formula> = 200 GeV by the STAR experiment. Specifically, measurements of nuclear modification factors for electrons, <inline-formula> <math display="inline"> <semantics> <mrow> <mi>J</mi> <mo>/</mo> <mi>ψ</mi> </mrow> </semantics> </math> </inline-formula>, and <inline-formula> <math display="inline"> <semantics> <msup> <mi>D</mi> <mn>0</mn> </msup> </semantics> </math> </inline-formula> from open bottom hadron decays, enabled by the Heavy Flavor Tracker, are shown. A large suppression for non-prompt <inline-formula> <math display="inline"> <semantics> <mrow> <mi>J</mi> <mo>/</mo> <mi>ψ</mi> </mrow> </semantics> </math> </inline-formula> and non-prompt <inline-formula> <math display="inline"> <semantics> <msup> <mi>D</mi> <mn>0</mn> </msup> </semantics> </math> </inline-formula> are observed at high transverse momenta. On the other hand, there seems to be less suppression for electrons from bottom hadron decays than for those from charm hadron decays at ∼<inline-formula> <math display="inline"> <semantics> <mrow> <mn>2</mn> <mi>σ</mi> </mrow> </semantics> </math> </inline-formula> significance level. |
topic |
open bottom production nuclear modification factors non-prompt J/ψ non-prompt D0 electrons from bottom hadron decays quark-gluon plasma |
url |
https://www.mdpi.com/2504-3900/10/1/39 |
work_keys_str_mv |
AT shenghuizhang openbottomproductioninauaucollisionsatspanstyletextdecorationoverlineemsemsubnnsubspan200gevwiththestarexperiment |
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1725908202105602048 |