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Prompt D0, D+, and D+ production in Pb–Pb collisions at $$ \sqrt{s_{\mathrm{NN}}} $$ = 5.02 TeV

The production of prompt D 0 , D + , and D *+ mesons was measured at midrapidity (| y | < 0.5) in Pb–Pb collisions at the centre-of-mass energy per nucleon–nucleon pair $$ \sqrt{s_{\mathrm{NN}}} $$ s NN = 5 . 02 TeV with the ALICE detector at the LHC. The D mesons were reconstructed via their had...

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Published in:The journal of high energy physics 2022-01, Vol.2022 (1), Article 174
Main Authors: Acharya, S., Adamová, D., Adler, A., Adolfsson, J., Aglieri Rinella, G., Agnello, M., Agrawal, N., Ahammed, Z., Ahmad, S., Ahn, S. U., Ahuja, I., Akbar, Z., Akindinov, A., Al-Turany, M., Alam, S. N., Aleksandrov, D., Alessandro, B., Alfanda, H. M., Alfaro Molina, R., Ali, B., Ali, Y., Alici, A., Alizadehvandchali, N., Alkin, A., Alme, J., Alt, T., Altsybeev, I., Anaam, M. N., Andrei, C., Andreou, D., Andronic, A., Angeletti, M., Anguelov, V., Antinori, F., Antonioli, P., Anuj, C., Apadula, N., Aphecetche, L., Appelshäuser, H., Arcelli, S., Arnaldi, R., Arsene, I. C., Arslandok, M., Augustinus, A., Averbeck, R., Aziz, S., Azmi, M. D., Badalà, A., Baek, Y. W., Bai, X., Bailhache, R., Bailung, Y., Bala, R., Balbino, A., Baldisseri, A., Balis, B., Banerjee, D., Barbera, R., Barioglio, L., Barlou, M., Barnaföldi, G. G., Barnby, L. S., Barret, V., Bartels, C., Barth, K., Bartsch, E., Baruffaldi, F., Bastid, N., Basu, S., Batigne, G., Batyunya, B., Bauri, D., Bazo Alba, J. L., Bearden, I. G., Beattie, C., Becht, P., Belikov, I., Bell Hechavarria, A. D. C., Bellini, F., Bellwied, R., Belokurova, S., Belyaev, V., Bencedi, G., Beole, S., Bercuci, A., Berdnikov, Y., Berdnikova, A., Bergmann, L., Besoiu, M. G., Betev, L., Bhaduri, P. P., Bhasin, A., Bhat, I. R., Bhat, M. A., Bhattacharjee, B., Bhattacharya, P., Bianchi, L., Bianchi, N., Bielčík, J., Bielčíková, J.
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cited_by cdi_FETCH-LOGICAL-c2204-3e579af58414f971a5b5ff521680beda38b9fc69f12b924722b14c4695eb3a8a3
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container_issue 1
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container_title The journal of high energy physics
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creator Acharya, S.
Adamová, D.
Adler, A.
Adolfsson, J.
Aglieri Rinella, G.
Agnello, M.
Agrawal, N.
Ahammed, Z.
Ahmad, S.
Ahn, S. U.
Ahuja, I.
Akbar, Z.
Akindinov, A.
Al-Turany, M.
Alam, S. N.
Aleksandrov, D.
Alessandro, B.
Alfanda, H. M.
Alfaro Molina, R.
Ali, B.
Ali, Y.
Alici, A.
Alizadehvandchali, N.
Alkin, A.
Alme, J.
Alt, T.
Altsybeev, I.
Anaam, M. N.
Andrei, C.
Andreou, D.
Andronic, A.
Angeletti, M.
Anguelov, V.
Antinori, F.
Antonioli, P.
Anuj, C.
Apadula, N.
Aphecetche, L.
Appelshäuser, H.
Arcelli, S.
Arnaldi, R.
Arsene, I. C.
Arslandok, M.
Augustinus, A.
Averbeck, R.
Aziz, S.
Azmi, M. D.
Badalà, A.
Baek, Y. W.
Bai, X.
Bailhache, R.
Bailung, Y.
Bala, R.
Balbino, A.
Baldisseri, A.
Balis, B.
Banerjee, D.
Barbera, R.
Barioglio, L.
Barlou, M.
Barnaföldi, G. G.
Barnby, L. S.
Barret, V.
Bartels, C.
Barth, K.
Bartsch, E.
Baruffaldi, F.
Bastid, N.
Basu, S.
Batigne, G.
Batyunya, B.
Bauri, D.
Bazo Alba, J. L.
Bearden, I. G.
Beattie, C.
Becht, P.
Belikov, I.
Bell Hechavarria, A. D. C.
Bellini, F.
Bellwied, R.
Belokurova, S.
Belyaev, V.
Bencedi, G.
Beole, S.
Bercuci, A.
Berdnikov, Y.
Berdnikova, A.
Bergmann, L.
Besoiu, M. G.
Betev, L.
Bhaduri, P. P.
Bhasin, A.
Bhat, I. R.
Bhat, M. A.
Bhattacharjee, B.
Bhattacharya, P.
Bianchi, L.
Bianchi, N.
Bielčík, J.
Bielčíková, J.
description The production of prompt D 0 , D + , and D *+ mesons was measured at midrapidity (| y | < 0.5) in Pb–Pb collisions at the centre-of-mass energy per nucleon–nucleon pair $$ \sqrt{s_{\mathrm{NN}}} $$ s NN = 5 . 02 TeV with the ALICE detector at the LHC. The D mesons were reconstructed via their hadronic decay channels and their production yields were measured in central (0–10%) and semicentral (30–50%) collisions. The measurement was performed up to a transverse momentum ( p T ) of 36 or 50 GeV/c depending on the D meson species and the centrality interval. For the first time in Pb–Pb collisions at the LHC, the yield of D 0 mesons was measured down to p T = 0, which allowed a model-independent determination of the p T -integrated yield per unit of rapidity (d N/ d y ). A maximum suppression by a factor 5 and 2.5 was observed with the nuclear modification factor ( R AA ) of prompt D mesons at p T = 6–8 GeV/c for the 0–10% and 30–50% centrality classes, respectively. The D-meson R AA is compared with that of charged pions, charged hadrons, and J /ψ mesons as well as with theoretical predictions. The analysis of the agreement between the measured R AA , elliptic ( v 2 ) and triangular ( v 3 ) flow, and the model predictions allowed us to constrain the charm spatial diffusion coefficient D s . Furthermore the comparison of R AA and v 2 with different implementations of the same models provides an important insight into the role of radiative energy loss as well as charm quark recombination in the hadronisation mechanisms.
doi_str_mv 10.1007/JHEP01(2022)174
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U.</creatorcontrib><creatorcontrib>Ahuja, I.</creatorcontrib><creatorcontrib>Akbar, Z.</creatorcontrib><creatorcontrib>Akindinov, A.</creatorcontrib><creatorcontrib>Al-Turany, M.</creatorcontrib><creatorcontrib>Alam, S. N.</creatorcontrib><creatorcontrib>Aleksandrov, D.</creatorcontrib><creatorcontrib>Alessandro, B.</creatorcontrib><creatorcontrib>Alfanda, H. M.</creatorcontrib><creatorcontrib>Alfaro Molina, R.</creatorcontrib><creatorcontrib>Ali, B.</creatorcontrib><creatorcontrib>Ali, Y.</creatorcontrib><creatorcontrib>Alici, A.</creatorcontrib><creatorcontrib>Alizadehvandchali, N.</creatorcontrib><creatorcontrib>Alkin, A.</creatorcontrib><creatorcontrib>Alme, J.</creatorcontrib><creatorcontrib>Alt, T.</creatorcontrib><creatorcontrib>Altsybeev, I.</creatorcontrib><creatorcontrib>Anaam, M. N.</creatorcontrib><creatorcontrib>Andrei, C.</creatorcontrib><creatorcontrib>Andreou, D.</creatorcontrib><creatorcontrib>Andronic, A.</creatorcontrib><creatorcontrib>Angeletti, M.</creatorcontrib><creatorcontrib>Anguelov, V.</creatorcontrib><creatorcontrib>Antinori, F.</creatorcontrib><creatorcontrib>Antonioli, P.</creatorcontrib><creatorcontrib>Anuj, C.</creatorcontrib><creatorcontrib>Apadula, N.</creatorcontrib><creatorcontrib>Aphecetche, L.</creatorcontrib><creatorcontrib>Appelshäuser, H.</creatorcontrib><creatorcontrib>Arcelli, S.</creatorcontrib><creatorcontrib>Arnaldi, R.</creatorcontrib><creatorcontrib>Arsene, I. C.</creatorcontrib><creatorcontrib>Arslandok, M.</creatorcontrib><creatorcontrib>Augustinus, A.</creatorcontrib><creatorcontrib>Averbeck, R.</creatorcontrib><creatorcontrib>Aziz, S.</creatorcontrib><creatorcontrib>Azmi, M. D.</creatorcontrib><creatorcontrib>Badalà, A.</creatorcontrib><creatorcontrib>Baek, Y. W.</creatorcontrib><creatorcontrib>Bai, X.</creatorcontrib><creatorcontrib>Bailhache, R.</creatorcontrib><creatorcontrib>Bailung, Y.</creatorcontrib><creatorcontrib>Bala, R.</creatorcontrib><creatorcontrib>Balbino, A.</creatorcontrib><creatorcontrib>Baldisseri, A.</creatorcontrib><creatorcontrib>Balis, B.</creatorcontrib><creatorcontrib>Banerjee, D.</creatorcontrib><creatorcontrib>Barbera, R.</creatorcontrib><creatorcontrib>Barioglio, L.</creatorcontrib><creatorcontrib>Barlou, M.</creatorcontrib><creatorcontrib>Barnaföldi, G. G.</creatorcontrib><creatorcontrib>Barnby, L. S.</creatorcontrib><creatorcontrib>Barret, V.</creatorcontrib><creatorcontrib>Bartels, C.</creatorcontrib><creatorcontrib>Barth, K.</creatorcontrib><creatorcontrib>Bartsch, E.</creatorcontrib><creatorcontrib>Baruffaldi, F.</creatorcontrib><creatorcontrib>Bastid, N.</creatorcontrib><creatorcontrib>Basu, S.</creatorcontrib><creatorcontrib>Batigne, G.</creatorcontrib><creatorcontrib>Batyunya, B.</creatorcontrib><creatorcontrib>Bauri, D.</creatorcontrib><creatorcontrib>Bazo Alba, J. L.</creatorcontrib><creatorcontrib>Bearden, I. G.</creatorcontrib><creatorcontrib>Beattie, C.</creatorcontrib><creatorcontrib>Becht, P.</creatorcontrib><creatorcontrib>Belikov, I.</creatorcontrib><creatorcontrib>Bell Hechavarria, A. D. C.</creatorcontrib><creatorcontrib>Bellini, F.</creatorcontrib><creatorcontrib>Bellwied, R.</creatorcontrib><creatorcontrib>Belokurova, S.</creatorcontrib><creatorcontrib>Belyaev, V.</creatorcontrib><creatorcontrib>Bencedi, G.</creatorcontrib><creatorcontrib>Beole, S.</creatorcontrib><creatorcontrib>Bercuci, A.</creatorcontrib><creatorcontrib>Berdnikov, Y.</creatorcontrib><creatorcontrib>Berdnikova, A.</creatorcontrib><creatorcontrib>Bergmann, L.</creatorcontrib><creatorcontrib>Besoiu, M. G.</creatorcontrib><creatorcontrib>Betev, L.</creatorcontrib><creatorcontrib>Bhaduri, P. P.</creatorcontrib><creatorcontrib>Bhasin, A.</creatorcontrib><creatorcontrib>Bhat, I. R.</creatorcontrib><creatorcontrib>Bhat, M. A.</creatorcontrib><creatorcontrib>Bhattacharjee, B.</creatorcontrib><creatorcontrib>Bhattacharya, P.</creatorcontrib><creatorcontrib>Bianchi, L.</creatorcontrib><creatorcontrib>Bianchi, N.</creatorcontrib><creatorcontrib>Bielčík, J.</creatorcontrib><creatorcontrib>Bielčíková, J.</creatorcontrib><creatorcontrib>The ALICE collaboration</creatorcontrib><creatorcontrib>Oak Ridge National Laboratory (ORNL), Oak Ridge, TN (United States)</creatorcontrib><creatorcontrib>Univ. of Tennessee, Knoxville, TN (United States)</creatorcontrib><title>Prompt D0, D+, and D+ production in Pb–Pb collisions at $$ \sqrt{s_{\mathrm{NN}}} $$ = 5.02 TeV</title><title>The journal of high energy physics</title><description>The production of prompt D 0 , D + , and D *+ mesons was measured at midrapidity (| y | &lt; 0.5) in Pb–Pb collisions at the centre-of-mass energy per nucleon–nucleon pair $$ \sqrt{s_{\mathrm{NN}}} $$ s NN = 5 . 02 TeV with the ALICE detector at the LHC. The D mesons were reconstructed via their hadronic decay channels and their production yields were measured in central (0–10%) and semicentral (30–50%) collisions. The measurement was performed up to a transverse momentum ( p T ) of 36 or 50 GeV/c depending on the D meson species and the centrality interval. For the first time in Pb–Pb collisions at the LHC, the yield of D 0 mesons was measured down to p T = 0, which allowed a model-independent determination of the p T -integrated yield per unit of rapidity (d N/ d y ). A maximum suppression by a factor 5 and 2.5 was observed with the nuclear modification factor ( R AA ) of prompt D mesons at p T = 6–8 GeV/c for the 0–10% and 30–50% centrality classes, respectively. The D-meson R AA is compared with that of charged pions, charged hadrons, and J /ψ mesons as well as with theoretical predictions. The analysis of the agreement between the measured R AA , elliptic ( v 2 ) and triangular ( v 3 ) flow, and the model predictions allowed us to constrain the charm spatial diffusion coefficient D s . Furthermore the comparison of R AA and v 2 with different implementations of the same models provides an important insight into the role of radiative energy loss as well as charm quark recombination in the hadronisation mechanisms.</description><subject>Lepton-nucleon scattering</subject><subject>PHYSICS OF ELEMENTARY PARTICLES AND FIELDS</subject><issn>1029-8479</issn><issn>1029-8479</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2022</creationdate><recordtype>article</recordtype><recordid>eNpNkDFPAjEAhRujiYjOro1h0MhB22vvroODARQNwRvQiaRpSxvOcHfQ1sEQEv-D_9Bf4hEcnN7Ley9v-AC4xKiHEUr7z-NRjvA1QYTc4JQegRZGhEcZTfnxP38Kzrx_RwgzzFELyNzV5TrAIerC4W0XymrRKFy7evGhQ1FXsKhgrn6-vnMFdb1aFb4JPZQBdjpw7jcubL3YzksZlq7cTqe73W7f3EHWQwTOzNs5OLFy5c3Fn7bB68NoNhhHk5fHp8H9JNKEIBrFhqVcWpZRTC1PsWSKWcsITjKkzELGmeJWJ9xiojihKSEKU00TzoyKZSbjNrg6_NY-FMLrIhi91HVVGR0EzrKEJqgZ9Q8j7WrvnbFi7YpSuk-BkdhjFAeMYo9RNBjjX_fzYkk</recordid><startdate>202201</startdate><enddate>202201</enddate><creator>Acharya, S.</creator><creator>Adamová, D.</creator><creator>Adler, A.</creator><creator>Adolfsson, J.</creator><creator>Aglieri Rinella, G.</creator><creator>Agnello, M.</creator><creator>Agrawal, N.</creator><creator>Ahammed, Z.</creator><creator>Ahmad, S.</creator><creator>Ahn, S. U.</creator><creator>Ahuja, I.</creator><creator>Akbar, Z.</creator><creator>Akindinov, A.</creator><creator>Al-Turany, M.</creator><creator>Alam, S. N.</creator><creator>Aleksandrov, D.</creator><creator>Alessandro, B.</creator><creator>Alfanda, H. M.</creator><creator>Alfaro Molina, R.</creator><creator>Ali, B.</creator><creator>Ali, Y.</creator><creator>Alici, A.</creator><creator>Alizadehvandchali, N.</creator><creator>Alkin, A.</creator><creator>Alme, J.</creator><creator>Alt, T.</creator><creator>Altsybeev, I.</creator><creator>Anaam, M. N.</creator><creator>Andrei, C.</creator><creator>Andreou, D.</creator><creator>Andronic, A.</creator><creator>Angeletti, M.</creator><creator>Anguelov, V.</creator><creator>Antinori, F.</creator><creator>Antonioli, P.</creator><creator>Anuj, C.</creator><creator>Apadula, N.</creator><creator>Aphecetche, L.</creator><creator>Appelshäuser, H.</creator><creator>Arcelli, S.</creator><creator>Arnaldi, R.</creator><creator>Arsene, I. C.</creator><creator>Arslandok, M.</creator><creator>Augustinus, A.</creator><creator>Averbeck, R.</creator><creator>Aziz, S.</creator><creator>Azmi, M. D.</creator><creator>Badalà, A.</creator><creator>Baek, Y. W.</creator><creator>Bai, X.</creator><creator>Bailhache, R.</creator><creator>Bailung, Y.</creator><creator>Bala, R.</creator><creator>Balbino, A.</creator><creator>Baldisseri, A.</creator><creator>Balis, B.</creator><creator>Banerjee, D.</creator><creator>Barbera, R.</creator><creator>Barioglio, L.</creator><creator>Barlou, M.</creator><creator>Barnaföldi, G. G.</creator><creator>Barnby, L. S.</creator><creator>Barret, V.</creator><creator>Bartels, C.</creator><creator>Barth, K.</creator><creator>Bartsch, E.</creator><creator>Baruffaldi, F.</creator><creator>Bastid, N.</creator><creator>Basu, S.</creator><creator>Batigne, G.</creator><creator>Batyunya, B.</creator><creator>Bauri, D.</creator><creator>Bazo Alba, J. L.</creator><creator>Bearden, I. G.</creator><creator>Beattie, C.</creator><creator>Becht, P.</creator><creator>Belikov, I.</creator><creator>Bell Hechavarria, A. D. C.</creator><creator>Bellini, F.</creator><creator>Bellwied, R.</creator><creator>Belokurova, S.</creator><creator>Belyaev, V.</creator><creator>Bencedi, G.</creator><creator>Beole, S.</creator><creator>Bercuci, A.</creator><creator>Berdnikov, Y.</creator><creator>Berdnikova, A.</creator><creator>Bergmann, L.</creator><creator>Besoiu, M. G.</creator><creator>Betev, L.</creator><creator>Bhaduri, P. P.</creator><creator>Bhasin, A.</creator><creator>Bhat, I. R.</creator><creator>Bhat, M. 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D0, D+, and D+ production in Pb–Pb collisions at $$ \sqrt{s_{\mathrm{NN}}} $$ = 5.02 TeV</title><author>Acharya, S. ; Adamová, D. ; Adler, A. ; Adolfsson, J. ; Aglieri Rinella, G. ; Agnello, M. ; Agrawal, N. ; Ahammed, Z. ; Ahmad, S. ; Ahn, S. U. ; Ahuja, I. ; Akbar, Z. ; Akindinov, A. ; Al-Turany, M. ; Alam, S. N. ; Aleksandrov, D. ; Alessandro, B. ; Alfanda, H. M. ; Alfaro Molina, R. ; Ali, B. ; Ali, Y. ; Alici, A. ; Alizadehvandchali, N. ; Alkin, A. ; Alme, J. ; Alt, T. ; Altsybeev, I. ; Anaam, M. N. ; Andrei, C. ; Andreou, D. ; Andronic, A. ; Angeletti, M. ; Anguelov, V. ; Antinori, F. ; Antonioli, P. ; Anuj, C. ; Apadula, N. ; Aphecetche, L. ; Appelshäuser, H. ; Arcelli, S. ; Arnaldi, R. ; Arsene, I. C. ; Arslandok, M. ; Augustinus, A. ; Averbeck, R. ; Aziz, S. ; Azmi, M. D. ; Badalà, A. ; Baek, Y. W. ; Bai, X. ; Bailhache, R. ; Bailung, Y. ; Bala, R. ; Balbino, A. ; Baldisseri, A. ; Balis, B. ; Banerjee, D. ; Barbera, R. ; Barioglio, L. ; Barlou, M. ; Barnaföldi, G. G. ; Barnby, L. S. ; Barret, V. ; Bartels, C. ; Barth, K. ; Bartsch, E. ; Baruffaldi, F. ; Bastid, N. ; Basu, S. ; Batigne, G. ; Batyunya, B. ; Bauri, D. ; Bazo Alba, J. L. ; Bearden, I. G. ; Beattie, C. ; Becht, P. ; Belikov, I. ; Bell Hechavarria, A. D. C. ; Bellini, F. ; Bellwied, R. ; Belokurova, S. ; Belyaev, V. ; Bencedi, G. ; Beole, S. ; Bercuci, A. ; Berdnikov, Y. ; Berdnikova, A. ; Bergmann, L. ; Besoiu, M. G. ; Betev, L. ; Bhaduri, P. P. ; Bhasin, A. ; Bhat, I. R. ; Bhat, M. A. ; Bhattacharjee, B. ; Bhattacharya, P. ; Bianchi, L. ; Bianchi, N. ; Bielčík, J. ; Bielčíková, J.</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c2204-3e579af58414f971a5b5ff521680beda38b9fc69f12b924722b14c4695eb3a8a3</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2022</creationdate><topic>Lepton-nucleon scattering</topic><topic>PHYSICS OF ELEMENTARY PARTICLES AND FIELDS</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Acharya, S.</creatorcontrib><creatorcontrib>Adamová, D.</creatorcontrib><creatorcontrib>Adler, A.</creatorcontrib><creatorcontrib>Adolfsson, J.</creatorcontrib><creatorcontrib>Aglieri Rinella, G.</creatorcontrib><creatorcontrib>Agnello, M.</creatorcontrib><creatorcontrib>Agrawal, N.</creatorcontrib><creatorcontrib>Ahammed, Z.</creatorcontrib><creatorcontrib>Ahmad, S.</creatorcontrib><creatorcontrib>Ahn, S. 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W.</creatorcontrib><creatorcontrib>Bai, X.</creatorcontrib><creatorcontrib>Bailhache, R.</creatorcontrib><creatorcontrib>Bailung, Y.</creatorcontrib><creatorcontrib>Bala, R.</creatorcontrib><creatorcontrib>Balbino, A.</creatorcontrib><creatorcontrib>Baldisseri, A.</creatorcontrib><creatorcontrib>Balis, B.</creatorcontrib><creatorcontrib>Banerjee, D.</creatorcontrib><creatorcontrib>Barbera, R.</creatorcontrib><creatorcontrib>Barioglio, L.</creatorcontrib><creatorcontrib>Barlou, M.</creatorcontrib><creatorcontrib>Barnaföldi, G. G.</creatorcontrib><creatorcontrib>Barnby, L. S.</creatorcontrib><creatorcontrib>Barret, V.</creatorcontrib><creatorcontrib>Bartels, C.</creatorcontrib><creatorcontrib>Barth, K.</creatorcontrib><creatorcontrib>Bartsch, E.</creatorcontrib><creatorcontrib>Baruffaldi, F.</creatorcontrib><creatorcontrib>Bastid, N.</creatorcontrib><creatorcontrib>Basu, S.</creatorcontrib><creatorcontrib>Batigne, G.</creatorcontrib><creatorcontrib>Batyunya, B.</creatorcontrib><creatorcontrib>Bauri, D.</creatorcontrib><creatorcontrib>Bazo Alba, J. L.</creatorcontrib><creatorcontrib>Bearden, I. G.</creatorcontrib><creatorcontrib>Beattie, C.</creatorcontrib><creatorcontrib>Becht, P.</creatorcontrib><creatorcontrib>Belikov, I.</creatorcontrib><creatorcontrib>Bell Hechavarria, A. D. C.</creatorcontrib><creatorcontrib>Bellini, F.</creatorcontrib><creatorcontrib>Bellwied, R.</creatorcontrib><creatorcontrib>Belokurova, S.</creatorcontrib><creatorcontrib>Belyaev, V.</creatorcontrib><creatorcontrib>Bencedi, G.</creatorcontrib><creatorcontrib>Beole, S.</creatorcontrib><creatorcontrib>Bercuci, A.</creatorcontrib><creatorcontrib>Berdnikov, Y.</creatorcontrib><creatorcontrib>Berdnikova, A.</creatorcontrib><creatorcontrib>Bergmann, L.</creatorcontrib><creatorcontrib>Besoiu, M. G.</creatorcontrib><creatorcontrib>Betev, L.</creatorcontrib><creatorcontrib>Bhaduri, P. P.</creatorcontrib><creatorcontrib>Bhasin, A.</creatorcontrib><creatorcontrib>Bhat, I. R.</creatorcontrib><creatorcontrib>Bhat, M. A.</creatorcontrib><creatorcontrib>Bhattacharjee, B.</creatorcontrib><creatorcontrib>Bhattacharya, P.</creatorcontrib><creatorcontrib>Bianchi, L.</creatorcontrib><creatorcontrib>Bianchi, N.</creatorcontrib><creatorcontrib>Bielčík, J.</creatorcontrib><creatorcontrib>Bielčíková, J.</creatorcontrib><creatorcontrib>The ALICE collaboration</creatorcontrib><creatorcontrib>Oak Ridge National Laboratory (ORNL), Oak Ridge, TN (United States)</creatorcontrib><creatorcontrib>Univ. of Tennessee, Knoxville, TN (United States)</creatorcontrib><collection>CrossRef</collection><collection>OSTI.GOV - Hybrid</collection><collection>OSTI.GOV</collection><jtitle>The journal of high energy physics</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Acharya, S.</au><au>Adamová, D.</au><au>Adler, A.</au><au>Adolfsson, J.</au><au>Aglieri Rinella, G.</au><au>Agnello, M.</au><au>Agrawal, N.</au><au>Ahammed, Z.</au><au>Ahmad, S.</au><au>Ahn, S. U.</au><au>Ahuja, I.</au><au>Akbar, Z.</au><au>Akindinov, A.</au><au>Al-Turany, M.</au><au>Alam, S. N.</au><au>Aleksandrov, D.</au><au>Alessandro, B.</au><au>Alfanda, H. M.</au><au>Alfaro Molina, R.</au><au>Ali, B.</au><au>Ali, Y.</au><au>Alici, A.</au><au>Alizadehvandchali, N.</au><au>Alkin, A.</au><au>Alme, J.</au><au>Alt, T.</au><au>Altsybeev, I.</au><au>Anaam, M. N.</au><au>Andrei, C.</au><au>Andreou, D.</au><au>Andronic, A.</au><au>Angeletti, M.</au><au>Anguelov, V.</au><au>Antinori, F.</au><au>Antonioli, P.</au><au>Anuj, C.</au><au>Apadula, N.</au><au>Aphecetche, L.</au><au>Appelshäuser, H.</au><au>Arcelli, S.</au><au>Arnaldi, R.</au><au>Arsene, I. C.</au><au>Arslandok, M.</au><au>Augustinus, A.</au><au>Averbeck, R.</au><au>Aziz, S.</au><au>Azmi, M. D.</au><au>Badalà, A.</au><au>Baek, Y. W.</au><au>Bai, X.</au><au>Bailhache, R.</au><au>Bailung, Y.</au><au>Bala, R.</au><au>Balbino, A.</au><au>Baldisseri, A.</au><au>Balis, B.</au><au>Banerjee, D.</au><au>Barbera, R.</au><au>Barioglio, L.</au><au>Barlou, M.</au><au>Barnaföldi, G. G.</au><au>Barnby, L. S.</au><au>Barret, V.</au><au>Bartels, C.</au><au>Barth, K.</au><au>Bartsch, E.</au><au>Baruffaldi, F.</au><au>Bastid, N.</au><au>Basu, S.</au><au>Batigne, G.</au><au>Batyunya, B.</au><au>Bauri, D.</au><au>Bazo Alba, J. L.</au><au>Bearden, I. G.</au><au>Beattie, C.</au><au>Becht, P.</au><au>Belikov, I.</au><au>Bell Hechavarria, A. D. C.</au><au>Bellini, F.</au><au>Bellwied, R.</au><au>Belokurova, S.</au><au>Belyaev, V.</au><au>Bencedi, G.</au><au>Beole, S.</au><au>Bercuci, A.</au><au>Berdnikov, Y.</au><au>Berdnikova, A.</au><au>Bergmann, L.</au><au>Besoiu, M. G.</au><au>Betev, L.</au><au>Bhaduri, P. P.</au><au>Bhasin, A.</au><au>Bhat, I. R.</au><au>Bhat, M. A.</au><au>Bhattacharjee, B.</au><au>Bhattacharya, P.</au><au>Bianchi, L.</au><au>Bianchi, N.</au><au>Bielčík, J.</au><au>Bielčíková, J.</au><aucorp>The ALICE collaboration</aucorp><aucorp>Oak Ridge National Laboratory (ORNL), Oak Ridge, TN (United States)</aucorp><aucorp>Univ. of Tennessee, Knoxville, TN (United States)</aucorp><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Prompt D0, D+, and D+ production in Pb–Pb collisions at $$ \sqrt{s_{\mathrm{NN}}} $$ = 5.02 TeV</atitle><jtitle>The journal of high energy physics</jtitle><date>2022-01</date><risdate>2022</risdate><volume>2022</volume><issue>1</issue><artnum>174</artnum><issn>1029-8479</issn><eissn>1029-8479</eissn><abstract>The production of prompt D 0 , D + , and D *+ mesons was measured at midrapidity (| y | &lt; 0.5) in Pb–Pb collisions at the centre-of-mass energy per nucleon–nucleon pair $$ \sqrt{s_{\mathrm{NN}}} $$ s NN = 5 . 02 TeV with the ALICE detector at the LHC. The D mesons were reconstructed via their hadronic decay channels and their production yields were measured in central (0–10%) and semicentral (30–50%) collisions. The measurement was performed up to a transverse momentum ( p T ) of 36 or 50 GeV/c depending on the D meson species and the centrality interval. For the first time in Pb–Pb collisions at the LHC, the yield of D 0 mesons was measured down to p T = 0, which allowed a model-independent determination of the p T -integrated yield per unit of rapidity (d N/ d y ). A maximum suppression by a factor 5 and 2.5 was observed with the nuclear modification factor ( R AA ) of prompt D mesons at p T = 6–8 GeV/c for the 0–10% and 30–50% centrality classes, respectively. The D-meson R AA is compared with that of charged pions, charged hadrons, and J /ψ mesons as well as with theoretical predictions. The analysis of the agreement between the measured R AA , elliptic ( v 2 ) and triangular ( v 3 ) flow, and the model predictions allowed us to constrain the charm spatial diffusion coefficient D s . Furthermore the comparison of R AA and v 2 with different implementations of the same models provides an important insight into the role of radiative energy loss as well as charm quark recombination in the hadronisation mechanisms.</abstract><cop>United States</cop><pub>Springer 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fulltext fulltext
identifier ISSN: 1029-8479
ispartof The journal of high energy physics, 2022-01, Vol.2022 (1), Article 174
issn 1029-8479
1029-8479
language eng
recordid cdi_osti_scitechconnect_1886460
source Publicly Available Content Database; Springer Nature - SpringerLink Journals - Fully Open Access
subjects Lepton-nucleon scattering
PHYSICS OF ELEMENTARY PARTICLES AND FIELDS
title Prompt D0, D+, and D+ production in Pb–Pb collisions at $$ \sqrt{s_{\mathrm{NN}}} $$ = 5.02 TeV
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