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Acharya, S, Adamová, D, Adler, A, Aglieri Rinella, G, Agnello, M, Agrawal, N, Ahammed, Z, Ahmad, S, Ahn, SU, Ahuja, I et al (show 1021 more authors) , Akindinov, A, Al-Turany, M, Aleksandrov, D, Alessandro, B, Alfanda, HM, Alfaro Molina, R, Ali, B, Ali, Y, Alici, A, Alizadehvandchali, N, Alkin, A, Alme, J, Alocco, G, Alt, T, Altsybeev, I, Anaam, MN, Andrei, C, Andronic, A, Anguelov, V, Antinori, F, Antonioli, P, Anuj, C, Apadula, N, Aphecetche, L, Appelshäuser, H, Arcelli, S, Arnaldi, R, Arsene, IC, Arslandok, M, Augustinus, A, Averbeck, R, Aziz, S, Azmi, MD, Badalà, A, Baek, YW, Bai, X, Bailhache, R, Bailung, Y, Bala, R, Balbino, A, Baldisseri, A, Balis, B, Banerjee, D, Banoo, Z, Barbera, R, Barioglio, L, Barlou, M, Barnaföldi, GG, Barnby, LS, Barret, V, Barreto, L, Bartels, C, Barth, K, Bartsch, E, Baruffaldi, F, Bastid, N, Basu, S, Batigne, G, Battistini, D, Batyunya, B, Bauri, D, Bazo Alba, JL, Bearden, IG, Beattie, C, Becht, P, Behera, D, Belikov, I, Bell Hechavarria, ADC, Bellini, F, Bellwied, R, Belokurova, S, Belyaev, V, Bencedi, G, Beole, S, Bercuci, A, Berdnikov, Y, Berdnikova, A, Bergmann, L, Besoiu, MG, Betev, L, Bhaduri, PP, Bhasin, A, Bhat, IR, Bhat, MA, Bhattacharjee, B, Bianchi, L, Bianchi, N, Bielčík, J, Bielčíková, J, Biernat, J, Bilandzic, A, Biro, G, Biswas, S, Blair, JT, Blau, D, Blidaru, MB, Bluhme, N, Blume, C, Boca, G, Bock, F, Bodova, T, Bogdanov, A, Boi, S, Bok, J, Boldizsár, L, Bolozdynya, A, Bombara, M, Bond, PM, Bonomi, G, Borel, H, Borissov, A, Bossi, H, Botta, E, Bratrud, L, Braun-Munzinger, P, Bregant, M, Broz, M, Bruno, GE, Buckland, MD, Budnikov, D, Buesching, H, Bufalino, S, Bugnon, O, Buhler, P, Buthelezi, Z, Butt, JB, Bylinkin, A, Bysiak, SA, Cai, M, Caines, H, Caliva, A, Calvo Villar, E, Camacho, JMM, Camacho, RS, Camerini, P, Canedo, FDM, Carabas, M, Carnesecchi, F, Caron, R, Castillo Castellanos, J, Catalano, F, Ceballos Sanchez, C, Chakaberia, I, Chakraborty, P, Chandra, S, Chapeland, S, Chartier, M 
ORCID: 0000-0003-0578-5567, Chattopadhyay, S, Chattopadhyay, S, Chavez, TG, Cheng, T, Cheshkov, C, Cheynis, B, Chibante Barroso, V, Chinellato, DD, Chizzali, ES, Cho, J, Cho, S, Chochula, P, Christakoglou, P, Christensen, CH, Christiansen, P, Chujo, T, Ciacco, M, Cicalo, C, Cifarelli, L, Cindolo, F, Ciupek, MR, Clai, G, Colamaria, F, Colburn, JS, Colella, D, Collu, A, Colocci, M, Concas, M, Conesa Balbastre, G, Conesa del Valle, Z, Contin, G, Contreras, JG, Coquet, ML, Cormier, TM, Cortese, P, Cosentino, MR, Costa, F, Costanza, S, Crkovská, J, Crochet, P, Cruz-Torres, R, Cuautle, E, Cui, P, Cunqueiro, L, Dainese, A, Danisch, MC, Danu, A, Das, P, Das, P, Das, S, Dash, S, De Caro, A, de Cataldo, G, De Cilladi, L, de Cuveland, J, De Falco, A, De Gruttola, D, De Marco, N, De Martin, C, De Pasquale, S, Deb, S, Degenhardt, HF, Deja, KR, Del Grande, R, Dello Stritto, L, Deng, W, Dhankher, P, Di Bari, D, Di Mauro, A, Diaz, RA, Dietel, T, Ding, Y, Divià, R, Dixit, DU, Djuvsland, Ø, Dmitrieva, 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(2023)
Multiplicity and rapidity dependence of K∗(892)0
and ϕ(1020) production in p–Pb collisions at √(sNN)=5.02 TeV.
The European Physical Journal C, 83 (6).
540-.
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Open Access link.
Abstract
<jats:title>Abstract</jats:title><jats:p>The transverse-momentum <jats:inline-formula><jats:alternatives><jats:tex-math>$$(p_{\textrm{T}})$$</jats:tex-math><mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML">
<mml:mrow>
<mml:mo>(</mml:mo>
<mml:msub>
<mml:mi>p</mml:mi>
<mml:mtext>T</mml:mtext>
</mml:msub>
<mml:mo>)</mml:mo>
</mml:mrow>
</mml:math></jats:alternatives></jats:inline-formula> spectra of K<jats:inline-formula><jats:alternatives><jats:tex-math>$$^{*}(892)^{0}~$$</jats:tex-math><mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML">
<mml:mrow>
<mml:msup>
<mml:mrow />
<mml:mrow>
<mml:mrow />
<mml:mo>∗</mml:mo>
</mml:mrow>
</mml:msup>
<mml:msup>
<mml:mrow>
<mml:mo>(</mml:mo>
<mml:mn>892</mml:mn>
<mml:mo>)</mml:mo>
</mml:mrow>
<mml:mn>0</mml:mn>
</mml:msup>
<mml:mspace />
</mml:mrow>
</mml:math></jats:alternatives></jats:inline-formula>and <jats:inline-formula><jats:alternatives><jats:tex-math>$$\mathrm {\phi (1020)}~$$</jats:tex-math><mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML">
<mml:mrow>
<mml:mrow>
<mml:mi>ϕ</mml:mi>
<mml:mo>(</mml:mo>
<mml:mn>1020</mml:mn>
<mml:mo>)</mml:mo>
</mml:mrow>
<mml:mspace />
</mml:mrow>
</mml:math></jats:alternatives></jats:inline-formula>measured with the ALICE detector up to <jats:inline-formula><jats:alternatives><jats:tex-math>$$p_{\textrm{T}} $$</jats:tex-math><mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML">
<mml:msub>
<mml:mi>p</mml:mi>
<mml:mtext>T</mml:mtext>
</mml:msub>
</mml:math></jats:alternatives></jats:inline-formula> = 16 GeV/<jats:italic>c</jats:italic> in the rapidity range <jats:inline-formula><jats:alternatives><jats:tex-math>$$-1.2< y < 0.3,$$</jats:tex-math><mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML">
<mml:mrow>
<mml:mo>-</mml:mo>
<mml:mn>1.2</mml:mn>
<mml:mo><</mml:mo>
<mml:mi>y</mml:mi>
<mml:mo><</mml:mo>
<mml:mn>0.3</mml:mn>
<mml:mo>,</mml:mo>
</mml:mrow>
</mml:math></jats:alternatives></jats:inline-formula> in p–Pb collisions at the center-of-mass energy per nucleon–nucleon collision <jats:inline-formula><jats:alternatives><jats:tex-math>$$\sqrt{s_{\textrm{NN}}} = 5.02$$</jats:tex-math><mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML">
<mml:mrow>
<mml:msqrt>
<mml:msub>
<mml:mi>s</mml:mi>
<mml:mtext>NN</mml:mtext>
</mml:msub>
</mml:msqrt>
<mml:mo>=</mml:mo>
<mml:mn>5.02</mml:mn>
</mml:mrow>
</mml:math></jats:alternatives></jats:inline-formula> TeV are presented as a function of charged particle multiplicity and rapidity. The measured <jats:inline-formula><jats:alternatives><jats:tex-math>$$p_{\textrm{T}} $$</jats:tex-math><mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML">
<mml:msub>
<mml:mi>p</mml:mi>
<mml:mtext>T</mml:mtext>
</mml:msub>
</mml:math></jats:alternatives></jats:inline-formula> distributions show a dependence on both multiplicity and rapidity at low <jats:inline-formula><jats:alternatives><jats:tex-math>$$p_{\textrm{T}} $$</jats:tex-math><mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML">
<mml:msub>
<mml:mi>p</mml:mi>
<mml:mtext>T</mml:mtext>
</mml:msub>
</mml:math></jats:alternatives></jats:inline-formula> whereas no significant dependence is observed at high <jats:inline-formula><jats:alternatives><jats:tex-math>$$p_{\textrm{T}} $$</jats:tex-math><mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML">
<mml:msub>
<mml:mi>p</mml:mi>
<mml:mtext>T</mml:mtext>
</mml:msub>
</mml:math></jats:alternatives></jats:inline-formula>. A rapidity dependence is observed in the <jats:inline-formula><jats:alternatives><jats:tex-math>$$p_{\textrm{T}} $$</jats:tex-math><mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML">
<mml:msub>
<mml:mi>p</mml:mi>
<mml:mtext>T</mml:mtext>
</mml:msub>
</mml:math></jats:alternatives></jats:inline-formula>-integrated yield (d<jats:italic>N</jats:italic>/d<jats:italic>y</jats:italic>), whereas the mean transverse momentum <jats:inline-formula><jats:alternatives><jats:tex-math>$$\left( \langle p_{\textrm{T}} \rangle \right) $$</jats:tex-math><mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML">
<mml:mfenced>
<mml:mo>⟨</mml:mo>
<mml:msub>
<mml:mi>p</mml:mi>
<mml:mtext>T</mml:mtext>
</mml:msub>
<mml:mo>⟩</mml:mo>
</mml:mfenced>
</mml:math></jats:alternatives></jats:inline-formula> shows a flat behavior as a function of rapidity. The rapidity asymmetry (<jats:inline-formula><jats:alternatives><jats:tex-math>$$Y_{\textrm{asym}}$$</jats:tex-math><mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML">
<mml:msub>
<mml:mi>Y</mml:mi>
<mml:mtext>asym</mml:mtext>
</mml:msub>
</mml:math></jats:alternatives></jats:inline-formula>) at low <jats:inline-formula><jats:alternatives><jats:tex-math>$$p_{\textrm{T}} $$</jats:tex-math><mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML">
<mml:msub>
<mml:mi>p</mml:mi>
<mml:mtext>T</mml:mtext>
</mml:msub>
</mml:math></jats:alternatives></jats:inline-formula> (< 5 GeV/<jats:italic>c</jats:italic>) is more significant for higher multiplicity classes. At high <jats:inline-formula><jats:alternatives><jats:tex-math>$$p_{\textrm{T}} $$</jats:tex-math><mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML">
<mml:msub>
<mml:mi>p</mml:mi>
<mml:mtext>T</mml:mtext>
</mml:msub>
</mml:math></jats:alternatives></jats:inline-formula>, no significant rapidity asymmetry is observed in any of the multiplicity classes. Both K<jats:inline-formula><jats:alternatives><jats:tex-math>$$^{*}(892)^{0}~$$</jats:tex-math><mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML">
<mml:mrow>
<mml:msup>
<mml:mrow />
<mml:mrow>
<mml:mrow />
<mml:mo>∗</mml:mo>
</mml:mrow>
</mml:msup>
<mml:msup>
<mml:mrow>
<mml:mo>(</mml:mo>
<mml:mn>892</mml:mn>
<mml:mo>)</mml:mo>
</mml:mrow>
<mml:mn>0</mml:mn>
</mml:msup>
<mml:mspace />
</mml:mrow>
</mml:math></jats:alternatives></jats:inline-formula>and <jats:inline-formula><jats:alternatives><jats:tex-math>$$\mathrm {\phi (1020)}~$$</jats:tex-math><mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML">
<mml:mrow>
<mml:mrow>
<mml:mi>ϕ</mml:mi>
<mml:mo>(</mml:mo>
<mml:mn>1020</mml:mn>
<mml:mo>)</mml:mo>
</mml:mrow>
<mml:mspace />
</mml:mrow>
</mml:math></jats:alternatives></jats:inline-formula>show similar <jats:inline-formula><jats:alternatives><jats:tex-math>$$Y_{\textrm{asym}}$$</jats:tex-math><mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML">
<mml:msub>
<mml:mi>Y</mml:mi>
<mml:mtext>asym</mml:mtext>
</mml:msub>
</mml:math></jats:alternatives></jats:inline-formula>. The nuclear modification factor <jats:inline-formula><jats:alternatives><jats:tex-math>$$(Q_{\textrm{CP}})$$</jats:tex-math><mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML">
<mml:mrow>
<mml:mo>(</mml:mo>
<mml:msub>
<mml:mi>Q</mml:mi>
<mml:mtext>CP</mml:mtext>
</mml:msub>
<mml:mo>)</mml:mo>
</mml:mrow>
</mml:math></jats:alternatives></jats:inline-formula> as a function of <jats:inline-formula><jats:alternatives><jats:tex-math>$$p_{\textrm{T}} $$</jats:tex-math><mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML">
<mml:msub>
<mml:mi>p</mml:mi>
<mml:mtext>T</mml:mtext>
</mml:msub>
</mml:math></jats:alternatives></jats:inline-formula> shows a Cronin-like enhancement at intermediate <jats:inline-formula><jats:alternatives><jats:tex-math>$$p_{\textrm{T}} $$</jats:tex-math><mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML">
<mml:msub>
<mml:mi>p</mml:mi>
<mml:mtext>T</mml:mtext>
</mml:msub>
</mml:math></jats:alternatives></jats:inline-formula>, which is more prominent at higher rapidities (Pb-going direction) and in higher multiplicity classes. At high <jats:inline-formula><jats:alternatives><jats:tex-math>$$p_{\textrm{T}}$$</jats:tex-math><mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML">
<mml:msub>
<mml:mi>p</mml:mi>
<mml:mtext>T</mml:mtext>
</mml:msub>
</mml:math></jats:alternatives></jats:inline-formula> (> 5 GeV/<jats:inline-formula><jats:alternatives><jats:tex-math>$$c$$</jats:tex-math><mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML">
<mml:mi>c</mml:mi>
</mml:math></jats:alternatives></jats:inline-formula>), the <jats:inline-formula><jats:alternatives><jats:tex-math>$$Q_{\textrm{CP}}$$</jats:tex-math><mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML">
<mml:msub>
<mml:mi>Q</mml:mi>
<mml:mtext>CP</mml:mtext>
</mml:msub>
</mml:math></jats:alternatives></jats:inline-formula> values are greater than unity and no significant rapidity dependence is observed.</jats:p>
Dimensions
Dimensions
