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Polarization and entanglement in baryon–antibaryon pair production in electron–positron annihilation. / The BESIII Collaboration.

в: Nature Physics, Том 15, № 7, 01.07.2019, стр. 631-634.

Результаты исследований: Научные публикации в периодических изданияхписьмо/краткое сообщениеРецензирование

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The BESIII Collaboration. Polarization and entanglement in baryon–antibaryon pair production in electron–positron annihilation. Nature Physics. 2019 июль 1;15(7):631-634. doi: 10.1038/s41567-019-0494-8

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The BESIII Collaboration. / Polarization and entanglement in baryon–antibaryon pair production in electron–positron annihilation. в: Nature Physics. 2019 ; Том 15, № 7. стр. 631-634.

BibTeX

@article{dba404a24a144e7aa9bedd9596de8389,
title = "Polarization and entanglement in baryon–antibaryon pair production in electron–positron annihilation",
abstract = " Particles directly produced at electron–positron colliders, such as the J/ψ meson, decay with relatively high probability into a baryon–antibaryon pair 1 . 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 baryons 2–4 . 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 1978 5,6 . For Λ¯ → p¯ π + we find α + = −0.758 ± 0.010 ± 0.007, giving A CP = (α − + α + )/(α − − α + ) = −0.006 ± 0.012 ± 0.007, a precise direct test of charge–parity symmetry (CP) violation in Λ decays. ",
keywords = "ANALYZING POWER, PARAMETER, J/PSI, DECAY, HYPERON, LAMBDA(LAMBDA)OVER-BAR, OBSERVABLES, E(+)E(-), LAMBDA",
author = "{BESIII Collaboration} and M. Ablikim and Achasov, {M. N.} and S. Ahmed and M. Albrecht and M. Alekseev and A. Amoroso and An, {F. F.} and Q. An and Y. Bai and O. Bakina and {Baldini Ferroli}, R. and Y. Ban and K. Begzsuren and Bennett, {D. W.} and Bennett, {J. V.} and N. Berger and M. Bertani and D. Bettoni and F. Bianchi and E. Boger and I. Boyko and Briere, {R. A.} and H. Cai and X. Cai and A. Calcaterra and Cao, {G. F.} and Cetin, {S. A.} and J. Chai and Chang, {J. F.} and Chang, {W. L.} and G. Chelkov and G. Chen and Chen, {H. S.} and Chen, {J. C.} and Chen, {M. L.} and Chen, {P. L.} and Chen, {S. J.} and Chen, {X. R.} and Chen, {Y. B.} and W. Cheng and Chu, {X. K.} and G. Cibinetto and F. Cossio and Dai, {H. L.} and Dai, {J. P.} and A. Dbeyssi and D. Dedovich and Deng, {Z. Y.} and Muchnoi, {N. Yu} and Nikolaev, {I. B.}",
year = "2019",
month = jul,
day = "1",
doi = "10.1038/s41567-019-0494-8",
language = "English",
volume = "15",
pages = "631--634",
journal = "Nature Physics",
issn = "1745-2473",
publisher = "Nature Publishing Group",
number = "7",

}

RIS

TY - JOUR

T1 - Polarization and entanglement in baryon–antibaryon pair production in electron–positron annihilation

AU - BESIII Collaboration

AU - Ablikim, M.

AU - Achasov, M. N.

AU - Ahmed, S.

AU - Albrecht, M.

AU - Alekseev, M.

AU - Amoroso, A.

AU - An, F. F.

AU - An, Q.

AU - Bai, Y.

AU - Bakina, O.

AU - Baldini Ferroli, R.

AU - Ban, Y.

AU - Begzsuren, K.

AU - Bennett, D. W.

AU - Bennett, J. V.

AU - Berger, N.

AU - Bertani, M.

AU - Bettoni, D.

AU - Bianchi, F.

AU - Boger, E.

AU - Boyko, I.

AU - Briere, R. A.

AU - Cai, H.

AU - Cai, X.

AU - Calcaterra, A.

AU - Cao, G. F.

AU - Cetin, S. A.

AU - Chai, J.

AU - Chang, J. F.

AU - Chang, W. L.

AU - Chelkov, G.

AU - Chen, G.

AU - Chen, H. S.

AU - Chen, J. C.

AU - Chen, M. L.

AU - Chen, P. L.

AU - Chen, S. J.

AU - Chen, X. R.

AU - Chen, Y. B.

AU - Cheng, W.

AU - Chu, X. K.

AU - Cibinetto, G.

AU - Cossio, F.

AU - Dai, H. L.

AU - Dai, J. P.

AU - Dbeyssi, A.

AU - Dedovich, D.

AU - Deng, Z. Y.

AU - Muchnoi, N. Yu

AU - Nikolaev, I. B.

PY - 2019/7/1

Y1 - 2019/7/1

N2 - Particles directly produced at electron–positron colliders, such as the J/ψ meson, decay with relatively high probability into a baryon–antibaryon pair 1 . 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 baryons 2–4 . 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 1978 5,6 . For Λ¯ → p¯ π + we find α + = −0.758 ± 0.010 ± 0.007, giving A CP = (α − + α + )/(α − − α + ) = −0.006 ± 0.012 ± 0.007, a precise direct test of charge–parity symmetry (CP) violation in Λ decays.

AB - Particles directly produced at electron–positron colliders, such as the J/ψ meson, decay with relatively high probability into a baryon–antibaryon pair 1 . 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 baryons 2–4 . 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 1978 5,6 . For Λ¯ → p¯ π + we find α + = −0.758 ± 0.010 ± 0.007, giving A CP = (α − + α + )/(α − − α + ) = −0.006 ± 0.012 ± 0.007, a precise direct test of charge–parity symmetry (CP) violation in Λ decays.

KW - ANALYZING POWER

KW - PARAMETER

KW - J/PSI

KW - DECAY

KW - HYPERON

KW - LAMBDA(LAMBDA)OVER-BAR

KW - OBSERVABLES

KW - E(+)E(-)

KW - LAMBDA

UR - http://www.scopus.com/inward/record.url?scp=85065295770&partnerID=8YFLogxK

U2 - 10.1038/s41567-019-0494-8

DO - 10.1038/s41567-019-0494-8

M3 - Letter

AN - SCOPUS:85065295770

VL - 15

SP - 631

EP - 634

JO - Nature Physics

JF - Nature Physics

SN - 1745-2473

IS - 7

ER -

ID: 20180996