Pattern of Global Spin Alignment of ϕϕ and K∗0K^{*0} mesons in Heavy-Ion Collisions

preprint2023arXivOpen access
STAR CollaborationM. S. AbdallahB. E. AboonaJ. AdamL. AdamczykJ. R. AdamsJ. K. AdkinsG. AgakishievI. AggarwalM. M. AggarwalZ. AhammedA. AitbaevI. AlekseevD. M. AndersonA. AparinE. C. AschenauerM. U. AshrafF. G. AtetallaG. S. AverichevV. BairathiW. BakerJ. G. Ball CapK. BarishA. BeheraR. BellwiedP. BhagatA. BhasinJ. BielcikJ. BielcikovaI. G. BordyuzhinJ. D. BrandenburgA. V. BrandinX. Z. CaiH. CainesM. Calderón de la Barca SánchezD. CebraI. ChakaberiaP. ChaloupkaB. K. ChanF-H. ChangZ. ChangA. ChatterjeeS. ChattopadhyayD. ChenJ. ChenJ. H. ChenX. ChenZ. ChenJ. ChengS. ChoudhuryW. ChristieX. ChuH. J. CrawfordM. CsanádM. DaugherityT. G. DedovichI. M. DeppnerA. A. DerevschikovA. DhamijaL. Di CarloL. DidenkoP. DixitX. DongJ. L. DrachenbergE. DuckworthJ. C. DunlopJ. EngelageG. EppleyS. EsumiO. EvdokimovA. EwiglebenO. EyserR. FatemiF. M. FawziS. FazioC. J. FengY. FengE. FinchY. FisyakA. FranciscoC. FuC. A. GagliardiT. GalatyukF. GeurtsN. GhimireA. GibsonK. GopalX. GouD. GrosnickA. GuptaW. GurynA. HamedY. HanS. HarabaszM. D. HarastyJ. W. HarrisH. HarrisonS. HeW. HeX. H. HeY. HeS. HeppelmannN. HerrmannE. HoffmanL. HolubC. HuQ. HuY. HuH. HuangH. Z. HuangS. L. HuangT. HuangX. HuangY. HuangT. J. HumanicD. IsenhowerM. IsshikiW. W. JacobsC. JenaA. JentschY. JiJ. JiaK. JiangX. JuE. G. JuddS. KabanaM. L. KabirS. KagamasterD. KalinkinK. KangD. KapukchyanK. KauderH. W. KeD. KeaneA. KechechyanM. KelseyD. P. KikołaB. KimelmanD. KincsesI. KiselA. KiselevA. G. KnospeH. S. KoL. KochendaA. KorobitsinL. K. KosarzewskiL. KramarikP. KravtsovL. KumarS. KumarR. Kunnawalkam ElayavalliJ. H. KwasizurR. LaceyS. LanJ. M. LandgrafJ. LauretA. LebedevR. LednickyJ. H. LeeY. H. LeungN. LewisC. LiW. LiX. LiY. LiX. LiangY. LiangR. LicenikT. LinY. LinM. A. LisaF. LiuH. LiuP. LiuT. LiuX. LiuY. LiuZ. LiuT. LjubicicW. J. LlopeR. S. LongacreE. LoydT. LuN. S. LukowX. F. LuoL. MaR. MaY. G. MaN. MagdyD. MallickS. L. ManukhovS. MargetisC. MarkertH. S. MatisJ. A. MazerN. G. MinaevS. MioduszewskiB. MohantyM. M. MondalI. MooneyD. A. MorozovA. MukherjeeM. NagyJ. D. NamMd. NasimK. NayakD. NeffJ. M. NelsonD. B. NemesM. NieG. NigmatkulovT. NiidaR. NishitaniL. V. NogachT. NonakaA. S. NunesG. OdyniecA. OgawaS. OhV. A. OkorokovK. OkuboB. S. PageR. PakJ. PanA. PandavA. K. PandeyY. PanebratsevP. ParfenovA. PaulB. PawlikD. PawlowskaC. PerkinsJ. PlutaB. R. PokhrelJ. PorterM. PosikV. ProzorovaN. K. PruthiM. PrzybycienJ. PutschkeH. QiuA. QuinteroC. RaczS. K. RadhakrishnanN. RahaR. L. RayR. ReedH. G. RitterM. RobotkovaJ. L. RomeroD. RoyL. RuanA. K. SahooN. R. SahooH. SakoS. SalurE. SamigullinJ. SandweissS. SatoW. B. SchmidkeN. SchmitzB. R. SchweidF. SeckJ. SegerR. SetoP. SeybothN. ShahE. ShahalievP. V. ShanmuganathanM. ShaoT. ShaoR. SharmaA. I. SheikhD. Y. ShenS. S. ShiY. ShiQ. Y. ShouE. P. SichtermannR. SikoraJ. SinghS. SinghaP. SinhaM. J. SkobyN. SmirnovY. SöhngenW. SolystY. SongH. M. SpinkaB. SrivastavaT. D. S. StanislausM. StefaniakD. J. StewartM. StrikhanovB. StringfellowA. A. P. SuaideM. SumberaX. M. SunX. SunY. SunB. SurrowD. N. SviridaZ. W. SwegerP. SzymanskiA. H. TangZ. TangA. TaranenkoT. TarnowskyJ. H. ThomasA. R. TimminsD. TlustyT. TodorokiM. TokarevC. A. TomkielS. TrentalangeR. E. TribbleP. TribedyS. K. TripathyT. TruhlarB. A. TrzeciakO. D. TsaiZ. TuT. UllrichD. G. UnderwoodI. UpsalG. Van BurenJ. VanekA. N. VasilievI. VassilievV. VerkestF. VidebækS. VokalS. A. VoloshinF. WangG. WangJ. S. WangP. WangX. WangY. WangZ. WangJ. C. WebbP. C. WeidenkaffG. D. WestfallH. WiemanS. W. WissinkR. WittJ. WuY. WuB. XiZ. G. XiaoG. XieW. XieH. XuN. XuQ. H. XuY. XuZ. XuG. YanC. YangQ. YangS. YangY. YangZ. YeL. YiK. YipY. YuH. ZbroszczykW. ZhaC. ZhangD. ZhangJ. ZhangS. ZhangY. ZhangZ. J. ZhangZ. ZhangF. ZhaoJ. ZhaoM. ZhaoC. ZhouY. ZhouX. ZhuM. ZurekM. Zyzak

Abstract

Notwithstanding decades of progress since Yukawa first developed a description of the force between nucleons in terms of meson exchange, a full understanding of the strong interaction remains a major challenge in modern science. One remaining difficulty arises from the non-perturbative nature of the strong force, which leads to the phenomenon of quark confinement at distances on the order of the size of the proton. Here we show that in relativistic heavy-ion collisions, where quarks and gluons are set free over an extended volume, two species of produced vector (spin-1) mesons, namely ϕϕ and K∗0K^{*0}, emerge with a surprising pattern of global spin alignment. In particular, the global spin alignment for ϕϕ is unexpectedly large, while that for K∗0K^{*0} is consistent with zero. The observed spin-alignment pattern and magnitude for the ϕϕ cannot be explained by conventional mechanisms, while a model with a connection to strong force fields, i.e. an effective proxy description within the Standard Model and Quantum Chromodynamics, accommodates the current data. This connection, if fully established, will open a potential new avenue for studying the behaviour of strong force fields.

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