| 000 | 03082nlm1a2200421 4500 | ||
|---|---|---|---|
| 001 | 660712 | ||
| 005 | 20231030041720.0 | ||
| 035 | _a(RuTPU)RU\TPU\network\30675 | ||
| 035 | _aRU\TPU\network\30574 | ||
| 090 | _a660712 | ||
| 100 | _a20191014a2019 k y0engy50 ba | ||
| 101 | 0 | _aeng | |
| 102 | _aUS | ||
| 135 | _adrcn ---uucaa | ||
| 181 | 0 | _ai | |
| 182 | 0 | _ab | |
| 200 | 1 |
_aBounds on lepton flavor violating physics and decays of neutral mesons from τ(μ)→3ℓ, ℓγγ-decays _fC. O. Dib [et al.] |
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| 203 |
_aText _celectronic |
||
| 300 | _aTitle screen | ||
| 320 | _a[References: 32 tit.] | ||
| 330 | _aWe study two- and three-body lepton flavor violating (LFV) decays involving leptons and neutral vector bosons V=ρ0, ω, ϕ, J/ψ, Υ, Z0, as well as pseudoscalar P=π0, η, η′, ηc and scalar S=f0(500), f0(980), a0(980), χc0(1P) mesons, without referring to a specific mechanism of LFV realization. In particular, we relate the rates of the three-body LFV decays τ(μ)→3ℓ, where ℓ=μ or e, to the two-body LFV decays (V,P)→τμ(τe,μe), where V and P play the role of intermediate resonances in the decay process τ(μ)→3ℓ. From the experimental upper bounds for the branching ratios of τ(μ)→3ℓ decays, we derive upper limits for the branching ratios of (V,P)→τμ(τe,μe). We compare our results to the available experimental data and known theoretical upper limits from previous studies of LFV processes and find that some of our limits are several orders of magnitude more stringent. Using the idea of quark-hadron duality, we extract limits on various quark-lepton dimension-six LFV operators from data on lepton decays. Some of these limits are either new or stronger than those existing in the literature. | ||
| 333 | _aРежим доступа: по договору с организацией-держателем ресурса | ||
| 461 |
_tPhysical Review D _ocovering particles, fields, gravitation, and cosmology |
||
| 463 |
_tVol. 99, iss. 3 _v[035020, 12 p.] _d2019 |
||
| 610 | 1 | _aэлектронный ресурс | |
| 610 | 1 | _aтруды учёных ТПУ | |
| 610 | 1 | _aмезоны | |
| 610 | 1 | _aраспады | |
| 610 | 1 | _aлептонные распады | |
| 701 | 1 |
_aDib _bC. O. _gClaudio |
|
| 701 | 1 |
_aGutsche _bT. _gThomas |
|
| 701 | 1 |
_aKovalenko _bS. G. _gSergey Grigorjevich |
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| 701 | 1 |
_aLyubovitskiy (Lyubovitskij) _bV. E. _cphysicist _cProfessor of Tomsk Polytechnic University, Doctor of physical and mathematical sciences, Professor of the University of Tubingen (Germany) _f1963- _gValery Efimovich _2stltpush _3(RuTPU)RU\TPU\pers\33385 |
|
| 701 | 1 |
_aSchmidt _bI. A. _gIvan |
|
| 712 | 0 | 2 |
_aНациональный исследовательский Томский политехнический университет _bИсследовательская школа физики высокоэнергетических процессов _c(2017- ) _h8118 _2stltpush _3(RuTPU)RU\TPU\col\23551 |
| 801 | 2 |
_aRU _b63413507 _c20191014 _gRCR |
|
| 856 | 4 | _uhttps://doi.org/10.1103/PhysRevD.99.035020 | |
| 942 | _cCF | ||