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Title: Temperature measurement of Quark-Gluon plasma at different stages
Abstract In a Quark-Gluon Plasma (QGP), the fundamental building blocks of matter, quarks and gluons, are under extreme conditions of temperature and density. A QGP could exist in the early stages of the Universe, and in various objects and events in the cosmos. The thermodynamic and hydrodynamic properties of the QGP are described by Quantum Chromodynamics (QCD) and can be studied in heavy-ion collisions. Despite being a key thermodynamic parameter, the QGP temperature is still poorly known. Thermal lepton pairs (e+e−andμ+μ−) are ideal penetrating probes of the true temperature of the emitting source, since their invariant-mass spectra suffer neither from strong final-state interactions nor from blue-shift effects due to rapid expansion. Here we measure the QGP temperature using thermale+e−production at the Relativistic Heavy Ion Collider (RHIC). The average temperature from the low-mass region (in-mediumρ0vector-meson dominant) is (2.01 ± 0.23) × 1012K, consistent with the chemical freeze-out temperature from statistical models and the phase transition temperature from Lattice QCD. The average temperature from the intermediate mass region (above theρ0mass, QGP dominant) is significantly higher at (3.25 ± 0.60) × 1012K. This work provides essential experimental thermodynamic measurements to map out the QCD phase diagram and understand the properties of matter under extreme conditions. more »« less
The thermodynamicT-matrix approach is used to study Wilson line correlators (WLCs) for a static quark-antiquark pair in the quark-gluon plasma (QGP). Selfconsistent results that incorporate constraints from the QGP equation of state can approximately reproduce WLCs computed in 2+1-flavor lattice-QCD (lQCD), provided the input potential exhibits less screening than in previous studies. Utilizing the updated potential to calculate pertinent heavylightT-matrices we evaluate thermal relaxation rates of heavy quarks in the QGP. We find a more pronounced temperature dependence for low-momentum quarks than in our previous results (with larger screening), which turns into a weaker temperature dependence of the (temperature-scaled) spatial diffusion coefficient, in fair agreement with the most recent lQCD data.
Flessa_Savvidou, Aikaterini; Ptok, Andrzej; Sharma, G; Casas, Brian; Clark, Judith K; Li, Victoria M; Shatruk, Michael; Tewari, Sumanta; Balicas, Luis
(, npj Quantum Materials)
Abstract We report a transport study on Pd3In7which displays multiple Dirac type-II nodes in its electronic dispersion. Pd3In7is characterized by low residual resistivities and high mobilities, which are consistent with Dirac-like quasiparticles. For an applied magnetic field (μ0H) having a non-zero component along the electrical current, we find a large, positive, and linear inμ0Hlongitudinal magnetoresistivity (LMR). The sign of the LMR and its linear dependence deviate from the behavior reported for the chiral-anomaly-driven LMR in Weyl semimetals. Interestingly, such anomalous LMR is consistent with predictions for the role of the anomaly in type-II Weyl semimetals. In contrast, the transverse or conventional magnetoresistivity (CMR for electric fieldsE⊥μ0H) is large and positive, increasing by 103−104% as a function ofμ0Hwhile following an anomalous, angle-dependent power law$${\rho }_{{{{\rm{xx}}}}}\propto {({\mu }_{0}H)}^{n}$$ withn(θ) ≤ 1. The order of magnitude of the CMR, and its anomalous power-law, is explained in terms of uncompensated electron and hole-like Fermi surfaces characterized by anisotropic carrier scattering likely due to the lack of Lorentz invariance.
Abualrob, I J; Acharya, S; Aglieri_Rinella, G; Aglietta, L; Agnello, M; Agrawal, N; Ahammed, Z; Ahmad, S; Ahuja, I; Akbar, Z; et al
(, Journal of High Energy Physics)
A<sc>bstract</sc> Ultrarelativistic heavy-ion collisions produce a state of hot and dense strongly interacting QCD matter called quark-gluon plasma (QGP). On an event-by-event basis, the volume of the QGP in ultracentral collisions is mostly constant, while its total entropy can vary significantly due to quantum fluctuations, leading to variations in the temperature of the system. Exploiting this unique feature of ultracentral collisions allows for the interpretation of the correlation of the mean transverse momentum$$(\langle {p}_{\text{T}}\rangle )$$of produced charged hadrons and the number of charged hadrons as a measure for the speed of sound,cs. This speed is related to the rate at which compression waves travel in the QGP and is determined by fitting the relative increase in$$\langle {p}_{\text{T}}\rangle $$with respect to the relative change in the average charged-particle density$$(\langle \text{d}{N}_{\text{ch}}/\text{d}\eta \rangle )$$measured at mid-rapidity. This study reports the event-average$$\langle {p}_{\text{T}}\rangle $$of charged particles as well as the variance, skewness, and kurtosis of the event-by-event transverse momentum per charged particle$$([{p}_{\text{T}}])$$distribution in ultracentral Pb-Pb collisions at a center-of-mass energy of 5.02 TeV per nucleon pair using the ALICE detector. Different centrality estimators based on charged-particle multiplicity or the transverse energy of the event are used to select ultracentral collisions. By ensuring a pseudorapidity gap between the region used to define the centrality and the region used to perform the measurement, the influence of biases and their potential effects on the rise of the mean transverse momentum is tested. The measured$${c}_{\text{s}}^{2}$$is found to strongly depend on the exploited centrality estimator and ranges between 0.1146±0.0028 (stat.)±0.0065 (syst.) and 0.4374±0.0006 (stat.)±0.0184 (syst.) in natural units. The self-normalized variance shows a steep decrease towards ultracentral collisions, while the self-normalized skewness variables show a maximum, followed by a fast decrease. These non-Gaussian features are understood in terms of the vanishing of the impact-parameter fluctuations contributing to the event-to-event [pT] distribution.
Liu, Feng-Lei; Xing, Wen-Jing; Wu, Xiang-Yu; Qin, Guang-You; Cao, Shanshan; Wang, Xin-Nian
(, The European Physical Journal C)
Abstract We develop a new heavy quark transport model, QLBT, to simulate the dynamical propagation of heavy quarks inside the quark-gluon plasma (QGP) created in relativistic heavy-ion collisions. Our QLBT model is based on the linear Boltzmann transport (LBT) model with the ideal QGP replaced by a collection of quasi-particles to account for the non-perturbative interactions among quarks and gluons of the hot QGP. The thermal masses of quasi-particles are fitted to the equation of state from lattice QCD simulations using the Bayesian statistical analysis method. Combining QLBT with our advanced hybrid fragmentation-coalescence hadronization approach, we calculate the nuclear modification factor $$R_\mathrm {AA}$$ R AA and the elliptic flow $$v_2$$ v 2 of D mesons at the Relativistic Heavy-Ion Collider and the Large Hadron Collider. By comparing our QLBT calculation to the experimental data on the D meson $$R_\mathrm {AA}$$ R AA and $$v_2$$ v 2 , we extract the heavy quark transport parameter $$\hat{q}$$ q ^ and diffusion coefficient $$D_\mathrm {s}$$ D s in the temperature range of $$1-4~T_\mathrm {c}$$ 1 - 4 T c , and compare them with the lattice QCD results and other phenomenological studies.
Abstract Recent experimental and modeling work predicted salt fingers, known in saline water bodies, would form under ice in freshwater lakes with specific conductance (SC) as low as 50μS cm−1. To test this prediction, Toolik Lake, Alaska (summer SC 60–90μS cm−1) was instrumented with temperature‐conductivity arrays. Calculations of solutes excluded with ice formation and a mass balance of changes in concentration of solutes within the lake indicated 90% to 100% of increase in solutes for several months following ice‐on was from cryoconcentration. Two metrics based on the ratio of density gradients of temperature and solutes,Rρand the Turner angle (Tu), obtained by conductivity, temperature, depth (CTD) and microstructure profiling, andɌ, ratio of solute and heat fluxes at the ice‐water interface, had values indicative of salt fingers below ice.Rρand Tu were in the range for salt fingers and the diffusive mode of double diffusion in intrusive‐features in lower water column. Step‐like changes in temperature and SC provide further evidence for double diffusion. Rates of dissipation of turbulent kinetic energy below ice and in intrusions were between 10−12and 10−10m2s−3. Increases in SC above the sediments following ice‐on at sites 4, 10 and 15 m deep in the 24 m deep lake imply that salt fluxes created localized increases in density conducive for intrusive flows. These results are the first for freshwater lakes illustrating formation of salt fingers and complex intrusive flows and indicate the need to revise models of under‐ice circulation.
Aboona, B E, Adam, J, Adamczyk, L, Aggarwal, I, Aggarwal, M M, Ahammed, Z, Alshammri, A K, Aschenauer, E C, Aslam, S, Atchison, J, Bairathi, V, Bao, X, Barish, K, Behera, S, Bellwied, R, Bhagat, P, Bhasin, A, Bhatta, S, Bhosale, S R, Bielcik, J, Bielcikova, J, Brandenburg, J D, Broodo, C, Cai, X Z, Caines, H, Calderón_de_la_Barca_Sánchez, M, Cebra, D, Ceska, J, Chakaberia, I, Chaloupka, P, Chang, Y S, Chang, Z, Chatterjee, A, Chen, D, Chen, J H, Chen, Q, Chen, Z, Cheng, J, Cheng, Y, Christie, W, Chu, X, Corey, S, Crawford, H J, Csanád, M, Dale-Gau, G, Das, A, Deppner, I M, Deshpande, A, Dhamija, A, Dimri, A, Dixit, P, Dong, X, Drachenberg, J L, Duckworth, E, Dunlop, J C, Engelage, J, Eppley, G, Esumi, S, Evdokimov, O, Eyser, O, Fatemi, R, Fazio, S, Feng, Y, Finch, E, Fisyak, Y, Flor, F A, Fu, C, Fu, T, Gagliardi, C A, Galatyuk, T, Gao, T, Geurts, F, Gibson, A, Gopal, K, Gou, X, Grosnick, D, Gu, A, Gupta, A, Guryn, W, Hamed, A, Hamilton, R J, Han, X, Han, Y, Harabasz, S, Harasty, M D, Harris, J W, Harrison-Smith, H, Havener, L B, He, X H, He, Y, Herrmann, N, Holub, L, Hu, C, Hu, Q, Hu, Y, Huang, H, Huang, H Z, Huang, S L, Huang, T, Huang, Y, Huang, Y, Isshiki, M, Jacobs, W W, Jalotra, A, Jena, C, Jentsch, A, Ji, Y, Jia, J, Jin, C, Jindal, N, Ju, X, Judd, E G, Kabana, S, Kalinkin, D, Kang, K, Kapukchyan, D, Kauder, K, Keane, D, Kesler, M, Khanal, A, Khyzhniak, Y V, Kikoła, D P, Kim, J, Kincses, D, Kisel, I, Kiselev, A, Knospe, A G, Kołaś, J, Korodi, B, Kosarzewski, L K, Kumar, L, Labonte, M C, Lacey, R, Landgraf, J M, Larson, C, Lauret, J, Lebedev, A, Lee, J H, Leung, Y H, Li, D, Li, H -S, Li, H, Li, H, Li, W, Li, X, Li, Y, Li, Z, Li, Z, Liang, X, Licenik, R, Lin, T, Lin, Y, Lisa, M A, Liu, C, Liu, G, Liu, H, Liu, L, Liu, Z, Ljubicic, T, Lomicky, O, Longacre, R S, Loyd, E M, Lu, T, Luo, J, Luo, X F, Ma, L, Ma, R, Ma, Y G, Magdy, N, Mallick, D, Manikandhan, R, Margetis, S, Markert, C, Matonoha, O, Mezhanska, O, Mi, K, Mioduszewski, S, Mohanty, B, Mondal, B, Mondal, M M, Mooney, I, Mrazkova, J, Nagy, M I, Naim, C J, Nain, A S, Nam, J D, Nasim, M, Nasrulloh, H, Nelson, J M, Nie, M, Nigmatkulov, G, Niida, T, Nonaka, T, Odyniec, G, Ogawa, A, Oh, S, Okubo, K, Page, B S, Pal, S, Pandav, A, Panday, A, Pandey, A K, Pani, T, Paul, A, Paul, S, Pawlowska, D, Perkins, C, Pluta, J, Pokhrel, B R, Ponce_Pinto, I D, Posik, M, Pottebaum, E, Prodhan, S, Protzman, T L, Prozorov, A, Prozorova, V, Pruthi, N K, Przybycien, M, Putschke, J, Qin, Z, Qiu, H, Racz, C, Radhakrishnan, S K, Rana, A, Ray, R L, Reed, R, Robertson, C W, Robotkova, M, Rosales_Aguilar, M A, Roy, D, Roy_Chowdhury, P, Ruan, L, Sahoo, A K, Sahoo, N R, Sako, H, Salur, S, Sambyal, S S, Sandhu, J K, Sato, S, Schaefer, B C, Schmitz, N, Seck, F -J, Seger, J, Seto, R, Seyboth, P, Shah, N, Shanmuganathan, P V, Shao, T, Sharma, M, Sharma, N, Sharma, R, Sharma, S R, Sheikh, A I, Shen, D, Shen, D Y, Shen, K, Shi, S, Shi, Y, Si, F, Singh, J, Singha, S, Sinha, P, Skoby, M J, Smirnov, N, Söhngen, Y, Song, Y, Stanislaus, T_D S, Stefaniak, M, Su, Y, Sumbera, M, Sun, X, Sun, Y, Surrow, B, Svoboda, M, Sweger, Z W, Tamis, A C, Tang, A H, Tang, Z, Tarnowsky, T, Thomas, J H, Timmins, A R, Tlusty, D, Torres_Valladares, D, Trentalange, S, Tribedy, P, Tripathy, S K, Truhlar, T, Trzeciak, B A, Tsai, O D, Tsang, C Y, Tu, Z, Tyler, J E, Ullrich, T, Underwood, D G, Van_Buren, G, Vanek, J, Vassiliev, I, Videbæk, F, Voloshin, S A, Wang, F, Wang, G, Wang, J S, Wang, J, Wang, K, Wang, X, Wang, Y, Wang, Y, Wang, Y, Wang, Z, Watroba, A J, Webb, J C, Weidenkaff, P C, Westfall, G D, Wielanek, D, Wieman, H, Wilks, G, Wissink, S W, Witt, R, Wong, C P, Wu, J, Wu, X, Wu, X, Xi, B, Xiao, Z G, Xie, G, Xie, W, Xu, H, Xu, N, Xu, Q H, Xu, Y, Xu, Y, Xu, Z, Xu, Z, Yan, G, Yan, Z, Yang, C, Yang, Q, Yang, S, Yang, Y, Ye, Z, Ye, Z, Yi, L, Yu, Y, Zbroszczyk, H, Zha, W, Zhang, C, Zhang, D, Zhang, J, Zhang, S, Zhang, W, Zhang, X, Zhang, Y, Zhang, Y, Zhang, Y, Zhang, Y, Zhang, Z, Zhang, Z, Zhao, F, Zhao, J, Zhou, S, Zhou, Y, Zhu, X, Zurek, M, and Zyzak, M. Temperature measurement of Quark-Gluon plasma at different stages. Retrieved from https://par.nsf.gov/biblio/10689118. Nature Communications 16.1 Web. doi:10.1038/s41467-025-63216-5.
Aboona, B E, Adam, J, Adamczyk, L, Aggarwal, I, Aggarwal, M M, Ahammed, Z, Alshammri, A K, Aschenauer, E C, Aslam, S, Atchison, J, Bairathi, V, Bao, X, Barish, K, Behera, S, Bellwied, R, Bhagat, P, Bhasin, A, Bhatta, S, Bhosale, S R, Bielcik, J, Bielcikova, J, Brandenburg, J D, Broodo, C, Cai, X Z, Caines, H, Calderón_de_la_Barca_Sánchez, M, Cebra, D, Ceska, J, Chakaberia, I, Chaloupka, P, Chang, Y S, Chang, Z, Chatterjee, A, Chen, D, Chen, J H, Chen, Q, Chen, Z, Cheng, J, Cheng, Y, Christie, W, Chu, X, Corey, S, Crawford, H J, Csanád, M, Dale-Gau, G, Das, A, Deppner, I M, Deshpande, A, Dhamija, A, Dimri, A, Dixit, P, Dong, X, Drachenberg, J L, Duckworth, E, Dunlop, J C, Engelage, J, Eppley, G, Esumi, S, Evdokimov, O, Eyser, O, Fatemi, R, Fazio, S, Feng, Y, Finch, E, Fisyak, Y, Flor, F A, Fu, C, Fu, T, Gagliardi, C A, Galatyuk, T, Gao, T, Geurts, F, Gibson, A, Gopal, K, Gou, X, Grosnick, D, Gu, A, Gupta, A, Guryn, W, Hamed, A, Hamilton, R J, Han, X, Han, Y, Harabasz, S, Harasty, M D, Harris, J W, Harrison-Smith, H, Havener, L B, He, X H, He, Y, Herrmann, N, Holub, L, Hu, C, Hu, Q, Hu, Y, Huang, H, Huang, H Z, Huang, S L, Huang, T, Huang, Y, Huang, Y, Isshiki, M, Jacobs, W W, Jalotra, A, Jena, C, Jentsch, A, Ji, Y, Jia, J, Jin, C, Jindal, N, Ju, X, Judd, E G, Kabana, S, Kalinkin, D, Kang, K, Kapukchyan, D, Kauder, K, Keane, D, Kesler, M, Khanal, A, Khyzhniak, Y V, Kikoła, D P, Kim, J, Kincses, D, Kisel, I, Kiselev, A, Knospe, A G, Kołaś, J, Korodi, B, Kosarzewski, L K, Kumar, L, Labonte, M C, Lacey, R, Landgraf, J M, Larson, C, Lauret, J, Lebedev, A, Lee, J H, Leung, Y H, Li, D, Li, H -S, Li, H, Li, H, Li, W, Li, X, Li, Y, Li, Z, Li, Z, Liang, X, Licenik, R, Lin, T, Lin, Y, Lisa, M A, Liu, C, Liu, G, Liu, H, Liu, L, Liu, Z, Ljubicic, T, Lomicky, O, Longacre, R S, Loyd, E M, Lu, T, Luo, J, Luo, X F, Ma, L, Ma, R, Ma, Y G, Magdy, N, Mallick, D, Manikandhan, R, Margetis, S, Markert, C, Matonoha, O, Mezhanska, O, Mi, K, Mioduszewski, S, Mohanty, B, Mondal, B, Mondal, M M, Mooney, I, Mrazkova, J, Nagy, M I, Naim, C J, Nain, A S, Nam, J D, Nasim, M, Nasrulloh, H, Nelson, J M, Nie, M, Nigmatkulov, G, Niida, T, Nonaka, T, Odyniec, G, Ogawa, A, Oh, S, Okubo, K, Page, B S, Pal, S, Pandav, A, Panday, A, Pandey, A K, Pani, T, Paul, A, Paul, S, Pawlowska, D, Perkins, C, Pluta, J, Pokhrel, B R, Ponce_Pinto, I D, Posik, M, Pottebaum, E, Prodhan, S, Protzman, T L, Prozorov, A, Prozorova, V, Pruthi, N K, Przybycien, M, Putschke, J, Qin, Z, Qiu, H, Racz, C, Radhakrishnan, S K, Rana, A, Ray, R L, Reed, R, Robertson, C W, Robotkova, M, Rosales_Aguilar, M A, Roy, D, Roy_Chowdhury, P, Ruan, L, Sahoo, A K, Sahoo, N R, Sako, H, Salur, S, Sambyal, S S, Sandhu, J K, Sato, S, Schaefer, B C, Schmitz, N, Seck, F -J, Seger, J, Seto, R, Seyboth, P, Shah, N, Shanmuganathan, P V, Shao, T, Sharma, M, Sharma, N, Sharma, R, Sharma, S R, Sheikh, A I, Shen, D, Shen, D Y, Shen, K, Shi, S, Shi, Y, Si, F, Singh, J, Singha, S, Sinha, P, Skoby, M J, Smirnov, N, Söhngen, Y, Song, Y, Stanislaus, T_D S, Stefaniak, M, Su, Y, Sumbera, M, Sun, X, Sun, Y, Surrow, B, Svoboda, M, Sweger, Z W, Tamis, A C, Tang, A H, Tang, Z, Tarnowsky, T, Thomas, J H, Timmins, A R, Tlusty, D, Torres_Valladares, D, Trentalange, S, Tribedy, P, Tripathy, S K, Truhlar, T, Trzeciak, B A, Tsai, O D, Tsang, C Y, Tu, Z, Tyler, J E, Ullrich, T, Underwood, D G, Van_Buren, G, Vanek, J, Vassiliev, I, Videbæk, F, Voloshin, S A, Wang, F, Wang, G, Wang, J S, Wang, J, Wang, K, Wang, X, Wang, Y, Wang, Y, Wang, Y, Wang, Z, Watroba, A J, Webb, J C, Weidenkaff, P C, Westfall, G D, Wielanek, D, Wieman, H, Wilks, G, Wissink, S W, Witt, R, Wong, C P, Wu, J, Wu, X, Wu, X, Xi, B, Xiao, Z G, Xie, G, Xie, W, Xu, H, Xu, N, Xu, Q H, Xu, Y, Xu, Y, Xu, Z, Xu, Z, Yan, G, Yan, Z, Yang, C, Yang, Q, Yang, S, Yang, Y, Ye, Z, Ye, Z, Yi, L, Yu, Y, Zbroszczyk, H, Zha, W, Zhang, C, Zhang, D, Zhang, J, Zhang, S, Zhang, W, Zhang, X, Zhang, Y, Zhang, Y, Zhang, Y, Zhang, Y, Zhang, Z, Zhang, Z, Zhao, F, Zhao, J, Zhou, S, Zhou, Y, Zhu, X, Zurek, M, & Zyzak, M. Temperature measurement of Quark-Gluon plasma at different stages. Nature Communications, 16 (1). Retrieved from https://par.nsf.gov/biblio/10689118. https://doi.org/10.1038/s41467-025-63216-5
Aboona, B E, Adam, J, Adamczyk, L, Aggarwal, I, Aggarwal, M M, Ahammed, Z, Alshammri, A K, Aschenauer, E C, Aslam, S, Atchison, J, Bairathi, V, Bao, X, Barish, K, Behera, S, Bellwied, R, Bhagat, P, Bhasin, A, Bhatta, S, Bhosale, S R, Bielcik, J, Bielcikova, J, Brandenburg, J D, Broodo, C, Cai, X Z, Caines, H, Calderón_de_la_Barca_Sánchez, M, Cebra, D, Ceska, J, Chakaberia, I, Chaloupka, P, Chang, Y S, Chang, Z, Chatterjee, A, Chen, D, Chen, J H, Chen, Q, Chen, Z, Cheng, J, Cheng, Y, Christie, W, Chu, X, Corey, S, Crawford, H J, Csanád, M, Dale-Gau, G, Das, A, Deppner, I M, Deshpande, A, Dhamija, A, Dimri, A, Dixit, P, Dong, X, Drachenberg, J L, Duckworth, E, Dunlop, J C, Engelage, J, Eppley, G, Esumi, S, Evdokimov, O, Eyser, O, Fatemi, R, Fazio, S, Feng, Y, Finch, E, Fisyak, Y, Flor, F A, Fu, C, Fu, T, Gagliardi, C A, Galatyuk, T, Gao, T, Geurts, F, Gibson, A, Gopal, K, Gou, X, Grosnick, D, Gu, A, Gupta, A, Guryn, W, Hamed, A, Hamilton, R J, Han, X, Han, Y, Harabasz, S, Harasty, M D, Harris, J W, Harrison-Smith, H, Havener, L B, He, X H, He, Y, Herrmann, N, Holub, L, Hu, C, Hu, Q, Hu, Y, Huang, H, Huang, H Z, Huang, S L, Huang, T, Huang, Y, Huang, Y, Isshiki, M, Jacobs, W W, Jalotra, A, Jena, C, Jentsch, A, Ji, Y, Jia, J, Jin, C, Jindal, N, Ju, X, Judd, E G, Kabana, S, Kalinkin, D, Kang, K, Kapukchyan, D, Kauder, K, Keane, D, Kesler, M, Khanal, A, Khyzhniak, Y V, Kikoła, D P, Kim, J, Kincses, D, Kisel, I, Kiselev, A, Knospe, A G, Kołaś, J, Korodi, B, Kosarzewski, L K, Kumar, L, Labonte, M C, Lacey, R, Landgraf, J M, Larson, C, Lauret, J, Lebedev, A, Lee, J H, Leung, Y H, Li, D, Li, H -S, Li, H, Li, H, Li, W, Li, X, Li, Y, Li, Z, Li, Z, Liang, X, Licenik, R, Lin, T, Lin, Y, Lisa, M A, Liu, C, Liu, G, Liu, H, Liu, L, Liu, Z, Ljubicic, T, Lomicky, O, Longacre, R S, Loyd, E M, Lu, T, Luo, J, Luo, X F, Ma, L, Ma, R, Ma, Y G, Magdy, N, Mallick, D, Manikandhan, R, Margetis, S, Markert, C, Matonoha, O, Mezhanska, O, Mi, K, Mioduszewski, S, Mohanty, B, Mondal, B, Mondal, M M, Mooney, I, Mrazkova, J, Nagy, M I, Naim, C J, Nain, A S, Nam, J D, Nasim, M, Nasrulloh, H, Nelson, J M, Nie, M, Nigmatkulov, G, Niida, T, Nonaka, T, Odyniec, G, Ogawa, A, Oh, S, Okubo, K, Page, B S, Pal, S, Pandav, A, Panday, A, Pandey, A K, Pani, T, Paul, A, Paul, S, Pawlowska, D, Perkins, C, Pluta, J, Pokhrel, B R, Ponce_Pinto, I D, Posik, M, Pottebaum, E, Prodhan, S, Protzman, T L, Prozorov, A, Prozorova, V, Pruthi, N K, Przybycien, M, Putschke, J, Qin, Z, Qiu, H, Racz, C, Radhakrishnan, S K, Rana, A, Ray, R L, Reed, R, Robertson, C W, Robotkova, M, Rosales_Aguilar, M A, Roy, D, Roy_Chowdhury, P, Ruan, L, Sahoo, A K, Sahoo, N R, Sako, H, Salur, S, Sambyal, S S, Sandhu, J K, Sato, S, Schaefer, B C, Schmitz, N, Seck, F -J, Seger, J, Seto, R, Seyboth, P, Shah, N, Shanmuganathan, P V, Shao, T, Sharma, M, Sharma, N, Sharma, R, Sharma, S R, Sheikh, A I, Shen, D, Shen, D Y, Shen, K, Shi, S, Shi, Y, Si, F, Singh, J, Singha, S, Sinha, P, Skoby, M J, Smirnov, N, Söhngen, Y, Song, Y, Stanislaus, T_D S, Stefaniak, M, Su, Y, Sumbera, M, Sun, X, Sun, Y, Surrow, B, Svoboda, M, Sweger, Z W, Tamis, A C, Tang, A H, Tang, Z, Tarnowsky, T, Thomas, J H, Timmins, A R, Tlusty, D, Torres_Valladares, D, Trentalange, S, Tribedy, P, Tripathy, S K, Truhlar, T, Trzeciak, B A, Tsai, O D, Tsang, C Y, Tu, Z, Tyler, J E, Ullrich, T, Underwood, D G, Van_Buren, G, Vanek, J, Vassiliev, I, Videbæk, F, Voloshin, S A, Wang, F, Wang, G, Wang, J S, Wang, J, Wang, K, Wang, X, Wang, Y, Wang, Y, Wang, Y, Wang, Z, Watroba, A J, Webb, J C, Weidenkaff, P C, Westfall, G D, Wielanek, D, Wieman, H, Wilks, G, Wissink, S W, Witt, R, Wong, C P, Wu, J, Wu, X, Wu, X, Xi, B, Xiao, Z G, Xie, G, Xie, W, Xu, H, Xu, N, Xu, Q H, Xu, Y, Xu, Y, Xu, Z, Xu, Z, Yan, G, Yan, Z, Yang, C, Yang, Q, Yang, S, Yang, Y, Ye, Z, Ye, Z, Yi, L, Yu, Y, Zbroszczyk, H, Zha, W, Zhang, C, Zhang, D, Zhang, J, Zhang, S, Zhang, W, Zhang, X, Zhang, Y, Zhang, Y, Zhang, Y, Zhang, Y, Zhang, Z, Zhang, Z, Zhao, F, Zhao, J, Zhou, S, Zhou, Y, Zhu, X, Zurek, M, and Zyzak, M.
"Temperature measurement of Quark-Gluon plasma at different stages". Nature Communications 16 (1). Country unknown/Code not available: Nature. https://doi.org/10.1038/s41467-025-63216-5.https://par.nsf.gov/biblio/10689118.
@article{osti_10689118,
place = {Country unknown/Code not available},
title = {Temperature measurement of Quark-Gluon plasma at different stages},
url = {https://par.nsf.gov/biblio/10689118},
DOI = {10.1038/s41467-025-63216-5},
abstractNote = {Abstract In a Quark-Gluon Plasma (QGP), the fundamental building blocks of matter, quarks and gluons, are under extreme conditions of temperature and density. A QGP could exist in the early stages of the Universe, and in various objects and events in the cosmos. The thermodynamic and hydrodynamic properties of the QGP are described by Quantum Chromodynamics (QCD) and can be studied in heavy-ion collisions. Despite being a key thermodynamic parameter, the QGP temperature is still poorly known. Thermal lepton pairs (e+e−andμ+μ−) are ideal penetrating probes of the true temperature of the emitting source, since their invariant-mass spectra suffer neither from strong final-state interactions nor from blue-shift effects due to rapid expansion. Here we measure the QGP temperature using thermale+e−production at the Relativistic Heavy Ion Collider (RHIC). The average temperature from the low-mass region (in-mediumρ0vector-meson dominant) is (2.01 ± 0.23) × 1012K, consistent with the chemical freeze-out temperature from statistical models and the phase transition temperature from Lattice QCD. The average temperature from the intermediate mass region (above theρ0mass, QGP dominant) is significantly higher at (3.25 ± 0.60) × 1012K. This work provides essential experimental thermodynamic measurements to map out the QCD phase diagram and understand the properties of matter under extreme conditions.},
journal = {Nature Communications},
volume = {16},
number = {1},
publisher = {Nature},
author = {Aboona, B E and Adam, J and Adamczyk, L and Aggarwal, I and Aggarwal, M M and Ahammed, Z and Alshammri, A K and Aschenauer, E C and Aslam, S and Atchison, J and Bairathi, V and Bao, X and Barish, K and Behera, S and Bellwied, R and Bhagat, P and Bhasin, A and Bhatta, S and Bhosale, S R and Bielcik, J and Bielcikova, J and Brandenburg, J D and Broodo, C and Cai, X Z and Caines, H and Calderón_de_la_Barca_Sánchez, M and Cebra, D and Ceska, J and Chakaberia, I and Chaloupka, P and Chang, Y S and Chang, Z and Chatterjee, A and Chen, D and Chen, J H and Chen, Q and Chen, Z and Cheng, J and Cheng, Y and Christie, W and Chu, X and Corey, S and Crawford, H J and Csanád, M and Dale-Gau, G and Das, A and Deppner, I M and Deshpande, A and Dhamija, A and Dimri, A and Dixit, P and Dong, X and Drachenberg, J L and Duckworth, E and Dunlop, J C and Engelage, J and Eppley, G and Esumi, S and Evdokimov, O and Eyser, O and Fatemi, R and Fazio, S and Feng, Y and Finch, E and Fisyak, Y and Flor, F A and Fu, C and Fu, T and Gagliardi, C A and Galatyuk, T and Gao, T and Geurts, F and Gibson, A and Gopal, K and Gou, X and Grosnick, D and Gu, A and Gupta, A and Guryn, W and Hamed, A and Hamilton, R J and Han, X and Han, Y and Harabasz, S and Harasty, M D and Harris, J W and Harrison-Smith, H and Havener, L B and He, X H and He, Y and Herrmann, N and Holub, L and Hu, C and Hu, Q and Hu, Y and Huang, H and Huang, H Z and Huang, S L and Huang, T and Huang, Y and Huang, Y and Isshiki, M and Jacobs, W W and Jalotra, A and Jena, C and Jentsch, A and Ji, Y and Jia, J and Jin, C and Jindal, N and Ju, X and Judd, E G and Kabana, S and Kalinkin, D and Kang, K and Kapukchyan, D and Kauder, K and Keane, D and Kesler, M and Khanal, A and Khyzhniak, Y V and Kikoła, D P and Kim, J and Kincses, D and Kisel, I and Kiselev, A and Knospe, A G and Kołaś, J and Korodi, B and Kosarzewski, L K and Kumar, L and Labonte, M C and Lacey, R and Landgraf, J M and Larson, C and Lauret, J and Lebedev, A and Lee, J H and Leung, Y H and Li, D and Li, H -S and Li, H and Li, H and Li, W and Li, X and Li, Y and Li, Z and Li, Z and Liang, X and Licenik, R and Lin, T and Lin, Y and Lisa, M A and Liu, C and Liu, G and Liu, H and Liu, L and Liu, Z and Ljubicic, T and Lomicky, O and Longacre, R S and Loyd, E M and Lu, T and Luo, J and Luo, X F and Ma, L and Ma, R and Ma, Y G and Magdy, N and Mallick, D and Manikandhan, R and Margetis, S and Markert, C and Matonoha, O and Mezhanska, O and Mi, K and Mioduszewski, S and Mohanty, B and Mondal, B and Mondal, M M and Mooney, I and Mrazkova, J and Nagy, M I and Naim, C J and Nain, A S and Nam, J D and Nasim, M and Nasrulloh, H and Nelson, J M and Nie, M and Nigmatkulov, G and Niida, T and Nonaka, T and Odyniec, G and Ogawa, A and Oh, S and Okubo, K and Page, B S and Pal, S and Pandav, A and Panday, A and Pandey, A K and Pani, T and Paul, A and Paul, S and Pawlowska, D and Perkins, C and Pluta, J and Pokhrel, B R and Ponce_Pinto, I D and Posik, M and Pottebaum, E and Prodhan, S and Protzman, T L and Prozorov, A and Prozorova, V and Pruthi, N K and Przybycien, M and Putschke, J and Qin, Z and Qiu, H and Racz, C and Radhakrishnan, S K and Rana, A and Ray, R L and Reed, R and Robertson, C W and Robotkova, M and Rosales_Aguilar, M A and Roy, D and Roy_Chowdhury, P and Ruan, L and Sahoo, A K and Sahoo, N R and Sako, H and Salur, S and Sambyal, S S and Sandhu, J K and Sato, S and Schaefer, B C and Schmitz, N and Seck, F -J and Seger, J and Seto, R and Seyboth, P and Shah, N and Shanmuganathan, P V and Shao, T and Sharma, M and Sharma, N and Sharma, R and Sharma, S R and Sheikh, A I and Shen, D and Shen, D Y and Shen, K and Shi, S and Shi, Y and Si, F and Singh, J and Singha, S and Sinha, P and Skoby, M J and Smirnov, N and Söhngen, Y and Song, Y and Stanislaus, T_D S and Stefaniak, M and Su, Y and Sumbera, M and Sun, X and Sun, Y and Surrow, B and Svoboda, M and Sweger, Z W and Tamis, A C and Tang, A H and Tang, Z and Tarnowsky, T and Thomas, J H and Timmins, A R and Tlusty, D and Torres_Valladares, D and Trentalange, S and Tribedy, P and Tripathy, S K and Truhlar, T and Trzeciak, B A and Tsai, O D and Tsang, C Y and Tu, Z and Tyler, J E and Ullrich, T and Underwood, D G and Van_Buren, G and Vanek, J and Vassiliev, I and Videbæk, F and Voloshin, S A and Wang, F and Wang, G and Wang, J S and Wang, J and Wang, K and Wang, X and Wang, Y and Wang, Y and Wang, Y and Wang, Z and Watroba, A J and Webb, J C and Weidenkaff, P C and Westfall, G D and Wielanek, D and Wieman, H and Wilks, G and Wissink, S W and Witt, R and Wong, C P and Wu, J and Wu, X and Wu, X and Xi, B and Xiao, Z G and Xie, G and Xie, W and Xu, H and Xu, N and Xu, Q H and Xu, Y and Xu, Y and Xu, Z and Xu, Z and Yan, G and Yan, Z and Yang, C and Yang, Q and Yang, S and Yang, Y and Ye, Z and Ye, Z and Yi, L and Yu, Y and Zbroszczyk, H and Zha, W and Zhang, C and Zhang, D and Zhang, J and Zhang, S and Zhang, W and Zhang, X and Zhang, Y and Zhang, Y and Zhang, Y and Zhang, Y and Zhang, Z and Zhang, Z and Zhao, F and Zhao, J and Zhou, S and Zhou, Y and Zhu, X and Zurek, M and Zyzak, M},
}
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