Matches in SemOpenAlex for { <https://semopenalex.org/work/W3011457350> ?p ?o ?g. }
Showing items 1 to 81 of
81
with 100 items per page.
- W3011457350 endingPage "121751" @default.
- W3011457350 startingPage "121751" @default.
- W3011457350 abstract "A Multi-Phase Transport Model (AMPT) has been extensively used to understand the physics behind the experimental observation. Like other models, the outcome of the AMPT model depends on the initial parameters. Therefore, one needs to choose suitable initial parameters before using the model. Lund string fragmentation function has been used to create quark-antiquarks pairs in the AMPT model. The Lund string fragmentation parameters determine the yields and transverse momentum ($p_{T}$) spectra of particles produced in nucleus-nucleus collisions. The values of Lund string fragmentation parameters were determined by fitting the charged particle yield and $p_{T}$ spectra measured in the experiment. In this paper, we have shown the yield of strange quarks carrying hadrons, e.g. $phi$ mesons, are more sensitive to Lund string fragmentation parameters compared to non-strange pions. Using $phi$ meson spectra measured at RHIC, we have obtained new sets of Lund parameters for Au+Au collisions at $sqrt{s_{mathrm {NN}}}$ = 11.5, 39, and 200 GeV. We have found that using the same set of parameters, we can explain $phi$-meson yield at $sqrt{s_{mathrm {NN}}}$ = 39 and 200 GeV, however, we need a different set of parameters for $sqrt{s_{mathrm {NN}}}$ = 11.5 GeV. This suggests that at low energy, $sqrt{s_{mathrm {NN}}}$ = 11.5 GeV, the underlying mechanism for particle production is different compared to top RHIC energies. We have also predicted invariant yield of $pi$ and $phi$ mesons as a function of $p_{T}$ in U+U collisions at $sqrt{s_{mathrm {NN}}}$ = 196 GeV to be measured by STAR experiment." @default.
- W3011457350 created "2020-03-23" @default.
- W3011457350 creator A5005382152 @default.
- W3011457350 creator A5031948435 @default.
- W3011457350 date "2020-07-01" @default.
- W3011457350 modified "2023-10-15" @default.
- W3011457350 title "Constraining input parameters of AMPT model with ϕ meson production" @default.
- W3011457350 cites W1527872136 @default.
- W3011457350 cites W1548201166 @default.
- W3011457350 cites W1979578625 @default.
- W3011457350 cites W1982086517 @default.
- W3011457350 cites W1985712914 @default.
- W3011457350 cites W2039225808 @default.
- W3011457350 cites W2064412362 @default.
- W3011457350 cites W2067104684 @default.
- W3011457350 cites W2089679729 @default.
- W3011457350 cites W2093397384 @default.
- W3011457350 cites W2131160516 @default.
- W3011457350 cites W2169165406 @default.
- W3011457350 cites W2174024475 @default.
- W3011457350 cites W2209164267 @default.
- W3011457350 cites W2271752648 @default.
- W3011457350 cites W2600758224 @default.
- W3011457350 cites W2762489005 @default.
- W3011457350 cites W2767036532 @default.
- W3011457350 cites W2949061363 @default.
- W3011457350 doi "https://doi.org/10.1016/j.nuclphysa.2020.121751" @default.
- W3011457350 hasPublicationYear "2020" @default.
- W3011457350 type Work @default.
- W3011457350 sameAs 3011457350 @default.
- W3011457350 citedByCount "1" @default.
- W3011457350 countsByYear W30114573502023 @default.
- W3011457350 crossrefType "journal-article" @default.
- W3011457350 hasAuthorship W3011457350A5005382152 @default.
- W3011457350 hasAuthorship W3011457350A5031948435 @default.
- W3011457350 hasBestOaLocation W30114573502 @default.
- W3011457350 hasConcept C109214941 @default.
- W3011457350 hasConcept C121332964 @default.
- W3011457350 hasConcept C139719470 @default.
- W3011457350 hasConcept C162324750 @default.
- W3011457350 hasConcept C185544564 @default.
- W3011457350 hasConcept C19694890 @default.
- W3011457350 hasConcept C200006409 @default.
- W3011457350 hasConcept C206094082 @default.
- W3011457350 hasConcept C2778348673 @default.
- W3011457350 hasConcept C4839761 @default.
- W3011457350 hasConcept C62520636 @default.
- W3011457350 hasConcept C7602139 @default.
- W3011457350 hasConceptScore W3011457350C109214941 @default.
- W3011457350 hasConceptScore W3011457350C121332964 @default.
- W3011457350 hasConceptScore W3011457350C139719470 @default.
- W3011457350 hasConceptScore W3011457350C162324750 @default.
- W3011457350 hasConceptScore W3011457350C185544564 @default.
- W3011457350 hasConceptScore W3011457350C19694890 @default.
- W3011457350 hasConceptScore W3011457350C200006409 @default.
- W3011457350 hasConceptScore W3011457350C206094082 @default.
- W3011457350 hasConceptScore W3011457350C2778348673 @default.
- W3011457350 hasConceptScore W3011457350C4839761 @default.
- W3011457350 hasConceptScore W3011457350C62520636 @default.
- W3011457350 hasConceptScore W3011457350C7602139 @default.
- W3011457350 hasLocation W30114573501 @default.
- W3011457350 hasLocation W30114573502 @default.
- W3011457350 hasOpenAccess W3011457350 @default.
- W3011457350 hasPrimaryLocation W30114573501 @default.
- W3011457350 hasRelatedWork W1601807243 @default.
- W3011457350 hasRelatedWork W1985286026 @default.
- W3011457350 hasRelatedWork W2024166584 @default.
- W3011457350 hasRelatedWork W2033365377 @default.
- W3011457350 hasRelatedWork W2039471314 @default.
- W3011457350 hasRelatedWork W2093749838 @default.
- W3011457350 hasRelatedWork W2125735982 @default.
- W3011457350 hasRelatedWork W2409544932 @default.
- W3011457350 hasRelatedWork W3102340848 @default.
- W3011457350 hasRelatedWork W4255485817 @default.
- W3011457350 hasVolume "999" @default.
- W3011457350 isParatext "false" @default.
- W3011457350 isRetracted "false" @default.
- W3011457350 magId "3011457350" @default.
- W3011457350 workType "article" @default.