Polarization and entanglement in baryon–antibaryon pair production in electron–positron annihilation

The BESIII Collaboration

Research output: Contribution to journalLetterpeer-review

38 Scopus citations

Abstract

Particles directly produced at electron–positron colliders, such as the J/ψ meson, decay with relatively high probability into a baryon–antibaryon pair1. For spin-1/2 baryons, the pair can have the same or opposite helicites. A non-vanishing phase ΔΦ between the transition amplitudes to these helicity states results in a transverse polarization of the baryons2–4. From the joint angular distribution of the decay products of the baryons, this phase as well as the parameters characterizing the baryon and the antibaryon decays can be determined. Here, we report the measurement of ΔΦ = 42.4 ± 0.6 ± 0.5° using Λ → pπ and Λ¯ → p¯ π+, n¯ π decays at BESIII. We find a value for the Λ → pπ decay parameter of α = 0.750 ± 0.009 ± 0.004, 17 ± 3% higher than the current world average, which has been used as input for all Λ polarization measurements since 19785,6. For Λ¯ → p¯ π+ we find α+ = −0.758 ± 0.010 ± 0.007, giving ACP = (α + α+)/(α − α+) = −0.006 ± 0.012 ± 0.007, a precise direct test of charge–parity symmetry (CP) violation in Λ decays.

Original languageEnglish (US)
Pages (from-to)631-634
Number of pages4
JournalNature Physics
Volume15
Issue number7
DOIs
StatePublished - Jul 1 2019

Bibliographical note

Funding Information:
The BESIII collaboration thanks the staff of BEPCII and the IHEP computing centre for their support. This work is supported in part by the National Key Basic Research Program of China under contract no. 2015CB856700; the National Natural Science Foundation of China (NSFC) under contract nos. 11335008, 11375205, 11425524, 11625523, 11635010, 11735014, 11835012 and 11875054; the Chinese Academy of Sciences (CAS) Large-Scale Scientific Facility Program; the CAS Center for Excellence in Particle Physics (CCEPP); Joint Large-Scale Scientific Facility Funds of the NSFC and CAS under contract nos. U1532257, U1532258, U1732102, U1732263 and U1832207; CAS Key Research Program of Frontier Sciences under contract nos. QYZDJ-SSW-SLH003 and QYZDJ-SSW-SLH040; 100 Talents Program of CAS; the CAS President’s International Fellowship Initiative; INPAC and Shanghai Key Laboratory for Particle Physics and Cosmology; German Research Foundation DFG under the contracts Collaborative Research Center CRC 1044 and FOR 2359; Istituto Nazionale di Fisica Nucleare, Italy; Koninklijke Nederlandse Akademie van Wetenschappen (KNAW) under contract no. 530-4CDP03; Ministry of Development of Turkey under contract no. DPT2006K-120470; National Science and Technology fund; The Swedish Research Council; the Knut and Alice Wallenberg Foundation; US Department of Energy under contract nos. DE-FG02-05ER41374, DE-SC-0010118, DE-SC-0010504 and DE-SC-0012069; University of Groningen (RuG); Helmholtzzentrum fuer Schwerionenforschung GmbH (GSI), Darmstadt. All consortium work was carried out at affiliations 1–67.

Publisher Copyright:
© 2019, The Author(s), under exclusive licence to Springer Nature Limited.

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