Prospects for rare and forbidden hyperon decays at BESIII

Hai-Bo Li

Front. Phys. ›› 2017, Vol. 12 ›› Issue (5) : 121301

PDF (196KB)
Front. Phys. ›› 2017, Vol. 12 ›› Issue (5) : 121301 DOI: 10.1007/s11467-017-0691-9
PERSPECTIVE

Prospects for rare and forbidden hyperon decays at BESIII

Author information +
History +
PDF (196KB)

Abstract

The study of hyperon decays at the Beijing Electron Spectrometer III (BESIII) is proposed to investigate the events of J/φ decay into hyperon pairs, which provide a pristine experimental environment at the Beijing Electron–Positron Collider II. About 106–108 hyperons, i.e., Ʌ, Σ,Ξand Ω, will be produced in the J/φ and φ(2S) decays with the proposed data samples at BESIII. Based on these samples, the measurement sensitivity of the branching fractions of the hyperon decays is in the range of 10-5–10-8. In addition, with the known center-of-mass energy and “tag technique”, rare decays and decays with invisible final states can be probed.

Keywords

BESIII / J/ φdecay / hyperon / rare decay / FCNC / lepton flavor violation

Cite this article

Download citation ▾
Hai-Bo Li. Prospects for rare and forbidden hyperon decays at BESIII. Front. Phys., 2017, 12(5): 121301 DOI:10.1007/s11467-017-0691-9

登录浏览全文

4963

注册一个新账户 忘记密码

References

[1]

M.Ablikim, [BESIII Collaboration], Design and construction of the BESIII Detector, Nucl. Instrum. Meth. A614, 345(2010), arXiv: 0911.4960 [physics.insdet]

[2]

D. M.Asner,I. I.Bigi, J.Charles, J. C.Chen, H. Y.Cheng, , Charm physics, Int. J. Mod. Phys. A24(supp01), 499(2009)

[3]

K. A.Olive, [Particle Data Group Collaboration], Review of particle physics,Chin. Phys. C40(10), 100001(2016)

[4]

N.Cabibbo, Unitary symmetry and leptonic decays,Phys. Rev. Lett.10(12), 531(1963)

[5]

M.Kobayashiand T.Maskawa, CP-violation in the renormalizable theory of weak interaction,Prog. Theor. Phys.49(2), 652(1973)

[6]

E.Blucher, E.De Lucia, G.Isidori, V.Lubicz, H.Abele, V.Cirigliano, R.Flores-Mendieta, J.Flynn, C.Gatti, A.Manohar, W.Marciano, V.Pavlunin, D.Pocanic, F.Schwab, A.Sirlin, C.Tarantino, and M.Velasco, Status of the Cabibbo angle, arXiv: hep-ph/0512039 (2005)

[7]

J. C.Hardyand I. S.Towner, The measurement and interpretation of superallowed 0+→0+ nuclear β decay,J. Phys. G41(11), 114004(2014)

[8]

M.Antonelli, V.Cirigliano, G.Isidori, F.Mescia, M.Moulson, H.Neufeld, E.Passemar, M.Palutan, B.Sciascia, M.Sozzi, R.Wanke, and O. P.Yushchenko, An evaluation of |Vus| and precise tests of the Standard Model from world data on leptonic and semileptonic kaon decays, Eur. Phys. J. C69(3), 399(2010)

[9]

N.Cabibbo, E. C.Swallow, and R.Winston, Semileptonic hyperon decays, Annu. Rev. Nucl. Part. Sci.53(1), 39(2003)

[10]

N.Cabibbo, E. C.Swallow, and R.Winston, Semileptonic hyperon decays and Cabibbo–Kobayashi–Maskawa unitarity, Phys. Rev. Lett.92(25), 251803(2004), arXiv: hep-ph/0307214

[11]

S.Weinberg, V–Awas the key, J. Phys. Conf. Ser.196, 012002(2009)

[12]

H. M.Chang, M.González-Alonso, and J.MartinCamalich, Nonstandard semileptonic hyperon decays,Phys. Rev. Lett.114(16), 161802(2015)

[13]

T. N.Pham, Test of SU(3) symmetry in hyperon semileptonic decays, Phys. Rev. D87(1), 016002(2013)

[14]

G. S.Yangand H. C.Kim, Hyperon Semileptonic decay constants with flavor SU(3) symmetry breaking,Phys. Rev. C92, 035206(2015), arXiv: 1504.04453 [hep-ph]

[15]

A.Faessler, T.Gutsche, B. R.Holstein, M. A.Ivanov, J. G.Korner, and V. E.Lyubovitskij, Semileptonic decays of the light JP= 1/2+ ground state baryon octet, Phys. Rev. D78(9), 094005(2008)

[16]

B.Borasoy, Baryon axial vector currents, Phys. Rev. D59(5), 054021(1999), arXiv: hep-ph/9811411

[17]

L. S.Geng, J. M.Camalich, and M. J. V.Vacas, SU(3)- breaking corrections to the hyperon vector coupling f(0) in covariant baryon chiral perturbation theory, Phys. Rev. D79(9), 094022(2009)

[18]

T.Ledwig, J. M.Camalich, L. S.Geng, and M. J. V.Vacas, Octet-baryon axial-vector charges and SU(3)-breaking effects in the semileptonic hyperon decays, Phys. Rev. D90(5), 054502(2014)

[19]

M.Bourquinand J. P.Repellin, Experiments with the CERN SPS hyperon beam, Phys. Rep.114(2), 99(1984)

[20]

J.Bernstein, G.Feinberg, and T. D.Lee, Possible C, Tnoninvariance in the electromagnetic interaction, Phys. Rev.139(6B), B1650(1965)

[21]

J.Lachand P.Zenczykowski, Hyperon radiative decays, Int. J. Mod. Phys. A10(27), 3817(1995)

[22]

I. I.Balitsky, V. M.Braun, and A. V.Kolesnichenko, Radiative decay Σ+in quantum chromodynamics, Nucl. Phys. B312(3), 509(1989)

[23]

M. K.Gaillard, X.Li, and S.Rudaz, Constituent gluons and a new mechanism for radiative weak decays of hyperons, Phys. Lett. B158(2), 158(1985)

[24]

P.Żenczykowski, Joint description of weak radiative and nonleptonic hyperon decays in broken SU(3), Phys. Rev. D73(7), 076005(2006), arXiv: hep-ph/0512122

[25]

B.Borasoyand B. R.Holstein, Resonances in radiative hyperon decays, Phys. Rev. D59(5), 054019(1999), arXiv: hep-ph/9902431

[26]

R. E.Behrends, Photon decay of hyperons, Phys. Rev. 111(6), 1691(1958)

[27]

Y.Hara, Nonleptonic decays of baryons and the eightfold way, Phys. Rev. Lett.12(13), 378(1964)

[28]

S. Y.Lo, Sum rules for nonleptonic weak gamma-decays of baryons, Nuovo Cim. 37(2), 753(1965)

[29]

K.Tanaka, Rare ΔQ= 0, ΔS= 1 decay modes of hyperons and K mesons, Phys. Rev.140(2B), B463(1965)

[30]

Gourdin, Unitary Symmetry,Amsterdam: North- Holland, 1967

[31]

J. W.Bos, D.Chang, S. C.Lee, Y. C.Lin, and H. H.Shih, Hyperon weak radiative decays in chiral perturbation theory, Phys. Rev. D54(5), 3321(1996), arXiv: hep-ph/9601299

[32]

B. V.Martemyanov, Electromagnetic transition form factors of Ʌne+e weak dilepton decay, Phys. At. Nucl. 66(4), 737(2003) [Yad. Fiz.66, 768(2003)]

[33]

J. R.Batley, [NA48 Collaboration], First observation and branching fraction and decay parameter measurements of the weak radiative decay Ξ0Ʌe+e, Phys. Lett. B650(1), 1 (2007), arXiv: hep-ex/ 0703023

[34]

L.Bergström, R.Safadi, and P.Singer, Phenomenology of Σ+pl+land the structure of the weak nonleptonic Hamiltonian, Z. Phys. C37(2), 281(1988)

[35]

X. G.He, J.Tandean, and G.Valencia, Decay Σ+→pl+l within the standard model, Phys. Rev. D72(7), 074003(2005), arXiv: hep-ph/0506067

[36]

D. S.Gorbunovand V. A.Rubakov, Kaon physics with light sgoldstinos and parity conservation, Phys. Rev. D64(5), 054008(2001), arXiv: hep-ph/0012033

[37]

F.Dettori[LHCb Collaboration], Evidence for the rare decay Σ++μ at LHCb,arXiv: 1611.06717 [hepex] (2016)

[38]

W. J.Marcianoand Z.Parsa, Rare kaon decays with “missing energy” Phys. Rev. D53(1), R1(1996)

[39]

A. J.Buras, M.Gorbahn, U.Haisch, and U.Nierste, Rare decay K+μν+νat the next-to-next-to-leading order in QCD, Phys. Rev. Lett.95(26), 261805(2005), arXiv: hep-ph/0508165

[40]

A. J.Buras, S.Uhlig, and F.Schwab, Waiting for precise measurements of K+μν+νand KLπ0ν+ν, Rev. Mod. Phys. 80(3), 965(2008), arXiv: hep-ph/0405132

[41]

A. J.Buras, D.Buttazzo, and R.Knegjens, K+μν+ν and ε’/εin simplified new physics models, J. High Energy Phys.1511, 166(2015), arXiv: 1507.08672 [hep-ph]

[42]

XuFeng, Private discussion

[43]

Y.Fukuda, [SuperKamiokande Collaboration], Measurements of the solar neutrino flux from Super- Kamiokande’s first 300 days, Phys. Rev. Lett.81(6), 1158(1998)

[44]

Y.Fukuda, [SuperKamiokande Collaboration], Evidence for oscillation of atmospheric neutrinos, Phys. Rev. Lett.81(8), 1562(1998)

[45]

Y.Fukuda, [SuperKamiokande Collaboration], Measurement of the flux and zenith-angle distribution of upward throughgoing muons by Super-Kamiokande, Phys. Rev. Lett.82(13), 2644(1999)

[46]

Y.Fukuda, [SuperKamiokande Collaboration], Tau neutrinos favored over sterile neutrinos in atmospheric muon neutrino oscillations, Phys. Rev. Lett.85(19), 3999(2000)

[47]

Y.Suzuki, Solar neutrino results from Super- Kamiokande,Nucl. Phys. B Proc. Suppl.77(1–3), 35(1999)

[48]

S.Fukuda, [Super-Kamiokande Collaboration], Solar 8B and hep neutrino measurements from 1258 days of Super-Kamiokande data, Phys. Rev. Lett.86(25), 5651(2001)

[49]

Y.Ashie, [Super-Kamiokande Collaboration], Evidence for an oscillatory signature in atmospheric neutrino oscillations, Phys. Rev. Lett.93(10), 101801(2004)

[50]

K.Eguchi, [KamLAND Collaboration], First Results from KamLAND: Evidence for reactor antineutrino disappearance, Phys. Rev. Lett.90(2), 021802(2003)

[51]

T.Araki, [KamLAND Collaboration], Measurement of neutrino oscillation with KamLAND: Evidence of spectral distortion, Phys. Rev. Lett.94(8), 081801(2005)

[52]

Q. R.Ahmad, [SNO Collaboration], Direct evidence for neutrino flavor transformation from neutralcurrent interactions in the Sudbury neutrino observatory, Phys. Rev. Lett.89(1), 011301(2002)

[53]

Q. R.Ahmad, [SNO Collaboration], Measurement of day and night neutrino energy spectra at SNO and constraints on neutrino mixing parameters, Phys. Rev. Lett.89(1), 011302(2002)

[54]

Q. R.Ahmad, [SNO Collaboration], Measurement of the total active 8B solar neutrino flux at the Sudbury neutrino observatory with enhanced neutral current sensitivity, Phys. Rev. Lett.92(18), 181301(2004)

[55]

B.Aharmim, [SNO Collaboration], Electron energy spectra, fluxes, and day-night asymmetries of 8B solar neutrinos from measurements with NaCl dissolved in the heavy-water detector at the Sudbury Neutrino Observatory, Phys. Rev. C72(5), 055502(2005)

[56]

F. P.An, [Daya Bay Collaboration], Observation of electron-antineutrino disappearance at Daya Bay, Phys. Rev. Lett.108(17), 171803(2012)

[57]

B.Pontecorvo, Inverse βprocesses and nonconservation of lepton charge,Sov. Phys. JETP7, 172(1958) [Zh. Eksp. Teor. Fiz.34, 247(1957)]

[58]

V. N.Gribovand B.Pontecorvo, Neutrino astronomy and lepton charge, Phys. Lett. B28(7), 493(1969)

[59]

W.Rodejohann, Neutrino-less double beta decay and particle physics, Int. J. Mod. Phys. E20(09), 1833(2011)

[60]

C.Barbero, G.Lopez Castro, and A.Mariano, Double beta decay of Σ hyperons, Phys. Lett. B566(1–2), 98(2003), arXiv: nucl-th/0212083

[61]

C.Barbero, L. F.Li, G. L.Castro, and A.Mariano, ΔL= 2 hyperon semileptonic decays, Phys. Rev. D76(11), 116008(2007)

[62]

C.Barbero,L. F.Li, G.López Castro, and A.Mariano, Matrix elements of four-quark operators and ΔL= 2 hyperon decays, Phys. Rev. D87(3), 036010(2013)

[63]

A. D.Sakharov, Violation of CP invariance, C asymmetry, and baryon asymmetry of the universe, Pis’ma Z. Eksp. Teor. Fiz. 5, 32(1967) [JETP Lett.5, 24(1967)] [Sov. Phys. Usp.34, 392(1991)] [Usp. Fiz. Nauk161, 61(1991)]

[64]

J. C.Patiand A.Salam, Unified lepton-hadron symmetry and a gauge theory of the basic interactions, Phys. Rev. D8(4), 1240(1973)

[65]

H.Georgiand S. L.Glashow, Unity of all elementaryparticle forces, Phys. Rev. Lett.32(8), 438(1974)

[66]

R. N.Mohapatraand R. E.Marshak, Quark-lepton symmetry and B–Las the U(1) generator of the electroweak symmetry group, Phys. Lett. B91, 222(1980)

[67]

H.An, S. L.Chen, R. N.Mohapatra, and Y.Zhang, Leptogenesis as a common origin for matter and dark matter, J. High Energy Phys.2010(3), 124(2010)

[68]

M. E.McCracken, [CLAS Collaboration], Search for baryon-number and lepton-number violating decays of Ʌ hyperons using the CLAS detector at Jefferson Laboratory, Phys. Rev. D92(7), 072002(2015), arXiv: 1507.03859 [hep-ex]

[69]

X. W.Kang, H. B.Li, and G. R.Lu, Study of Λ−Λ¯ oscillation in quantum coherent ΛΛ¯- by using J/φΛΛ¯- decay, Phys. Rev. D81(5), 051901(2010)

[70]

Z.Berezhianiand A.Vainshtein, Neutron-antineutron oscillation as a signal of CP violation, arXiv: 1506.05096 [hep-ph] (2015)

[71]

K. T.Chao, Baryon magnetic moments with confined quarks,Phys. Rev. D41(3), 920(1990)

[72]

X. G.Heand G.Velencia, CP violation in Ʌ beyond the standard model,Phys. Rev. D52(9), 5257(1995), arXiv: hep-ph/9508411

[73]

J. F.Donoghue, X. G.He, and S.Pakvasa, Hyperon decays and CP nonconservation, Phys. Rev. D34(3), 833(1986)

[74]

D.Chang, X. G.He, and S.Pakvasa, CP violation in hyperon decays due to left-right mixing, Phys. Rev. Lett.74(20), 3927(1995), arXiv: hep-ph/9412254

[75]

X. G.Heand S.Pakvasa, CP violation in hyperon decays, arXiv: hep-ph/9409236 (1994)

[76]

J.Tandean, New physics and CP violation in hyperon nonleptonic decays, Phys. Rev. D69(7), 076008(2004), arXiv: hep-ph/0311036

[77]

J.Tandeanand G.Valencia, CP violation in hyperon nonleptonic decays within the Standard Model, Phys. Rev. D67(5), 056001(2003), arXiv: hep-ph/0211165

[78]

J.Tandean, Probing CP violation in ΩɅKpπKdecay, Phys. Rev. D70(7), 076005(2004), arXiv: hepph/ 0406274

[79]

J.Tandeanand G.Valencia, CP violation in nonleptonic decays, Phys. Lett. B451(3–4), 382(1999), arXiv: hep-ph/9811376

[80]

X. G.He, J. P.Ma, and B.McKellar, CP violation in J/φɅΛ¯, Phys. Rev. D47(5), R1744(1993), arXiv: hep-ph/9211276

[81]

X. W.Kang, H. B.Li, G. R.Lu, and A.Datta, Study of CP violation in Λc+decay, Int. J. Mod. Phys. A26(15), 2523(2011)

[82]

A.Abdesselam, [Belle Collaboration], Observation of transverse Λ/Λ¯ hyperon polarization in e+e annihilation at Belle, arXiv: 1611.06648 [hep-ex] (2016)

[83]

A. E.Bondar, [Charm-Tau Factory Collaboration], Project of a super charm-tau factory at the Budker Institute of Nuclear Physics in Novosibirsk, Phys. At. Nucl.76(9), 1072(2013) [Yad. Fiz.76(9), 1132(2013)]

[84]

Z.Zhou, Q.Luo, L.Wang, W.Xu, and B.Zhang, “Preliminary Concept and Key Technologies of HIEPA Accelerator” talk at the 7th International Particle Accelerator Conference (IPAC 2016), 8–13 May 2016, Busan, Korea

[85]

D.Kimura, T.Morozumi, and H.Umeeda, Analysis of Dalitz decays with intrinsic parity violating interactions in resonance chiral perturbation theory, arXiv: 1609.09235 [hep-ph] (2016)

[86]

H. R.Dong, F.Feng, and H. B.Li, Lepton number violation in D meson decay, Chin. Phys. C39(1), 013101(2015)

[87]

N. H.Christ, [RBC and UKQCD Collaborations], Prospects for a lattice computation of rare kaon decay amplitudes II Kπννdecays, Phys. Rev. D93(11), 114517(2016), arXiv: 1605.04442 [hep-lat]

[88]

N. H.Christ, X.Feng, A.Jttner, A.Lawson, A.Portelliand C. T.Sachrajda, Exploratory lattice QCD study of the rare kaon decay Kπνν, PoS CD15, 033(2016)

[89]

N. H.Christ, [RBC and UKQCD Collaborations], Prospects for a lattice computation of rare kaon decay amplitudes: Kπl+l decays, Phys. Rev. D92(9), 094512(2015), arXiv: 1507.03094 [hep-lat]

[90]

T. D.Leeand C. N.Yang, General partial wave analysis of the decay of a hyperon of spin 1/2, Phys. Rev.108(6), 1645(1957)

[91]

A.Kadeer, J. G.Körner, and U.Moosbrugger, Helicity analysis of semileptonic hyperon decays including lepton-mass effects, Eur. Phys. J. C59(1), 27 (2009), arXiv: hep-ph/0511019

RIGHTS & PERMISSIONS

The Author(s) 2017. This article is published with open access at www.springer.com/11467 and journal.hep.com.cn/fop

AI Summary AI Mindmap
PDF (196KB)

1089

Accesses

0

Citation

Detail

Sections
Recommended

AI思维导图

/