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Measurement of the mass difference and the binding energy of the hypertriton and antihypertriton

  • The STAR collaboration
  • Brookhaven National Laboratory
  • AGH University of Krakow
  • Ohio State University
  • University of Kentucky
  • Joint Institute for Nuclear Research
  • Panjab University
  • Variable Energy Cyclotron Centre India
  • Alikhanov Institute for Theoretical and Experimental Physics
  • Moscow Engineering Physics Institute
  • Texas A&M University
  • Central China Normal University
  • Kent State University
  • Indian Institute of Science Education and Research, Berhampur
  • University of California at Riverside
  • Stony Brook University
  • University of Houston
  • University of Jammu
  • Czech Technical University in Prague
  • Czech Academy of Sciences
  • Shandong University
  • Rice University
  • Yale University
  • University of California at Davis
  • University of California at Los Angeles
  • National Cheng Kung University
  • Fudan University
  • University of Science and Technology of China
  • Tsinghua University
  • Creighton University
  • University of California at Berkeley

Research output: Contribution to journalArticlepeer-review

103 Scopus citations

Abstract

According to the CPT theorem, which states that the combined operation of charge conjugation, parity transformation and time reversal must be conserved, particles and their antiparticles should have the same mass and lifetime but opposite charge and magnetic moment. Here, we test CPT symmetry in a nucleus containing a strange quark, more specifically in the hypertriton. This hypernucleus is the lightest one yet discovered and consists of a proton, a neutron and a Λ hyperon. With data recorded by the STAR detector1–3 at the Relativistic Heavy Ion Collider, we measure the Λ hyperon binding energy BΛ for the hypertriton, and find that it differs from the widely used value4 and from predictions5–8, where the hypertriton is treated as a weakly bound system. Our results place stringent constraints on the hyperon–nucleon interaction9,10 and have implications for understanding neutron star interiors, where strange matter may be present11. A precise comparison of the masses of the hypertriton and the antihypertriton allows us to test CPT symmetry in a nucleus with strangeness, and we observe no deviation from the expected exact symmetry.

Original languageEnglish
Pages (from-to)409-412
Number of pages4
JournalNature Physics
Volume16
Issue number4
DOIs
StatePublished - Apr 1 2020

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