000 | 03106nlm1a2200385 4500 | ||
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001 | 643625 | ||
005 | 20231030040548.0 | ||
035 | _a(RuTPU)RU\TPU\network\8620 | ||
090 | _a643625 | ||
100 | _a20150918a2015 k y0engy50 ba | ||
101 | 0 | _aeng | |
102 | _aUS | ||
135 | _adrcn ---uucaa | ||
181 | 0 | _ai | |
182 | 0 | _ab | |
200 | 1 |
_aUnified description of BaBar and Belle data on the bottomonia decays [Y(mS) -->Y(nS) pi(+)pi(-)] _fYu. S. Surovtsev [et al.] |
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203 |
_aText _celectronic |
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300 | _aTitle screen | ||
320 | _a[References: 21 tit.] | ||
330 | _aWe present a unified analysis of the decays of bottomonia Ү(mS)-Ү(nS)ππ (m>n, m=2,3,4,5, n=1,2,3), charmonia J/φ-ф(ππ,KK), φ(2S)>J/φππ, and the isoscalar S-wave processes ππ-ππ, KK. In this analysis we extend our recent study of low-lying (m=2,3) radial excitations of bottomonia to modes involving higher (m=4,5) excited states. Similarly as for the data on lower radial excitations, we confirm that the data for higher radially excited states from the BABAR and Belle collaborations can be described under conditions that the final bottomonium is a spectator and the multichannel ?? scattering is considered in a model-independent approach based on analyticity, unitarity and the uniformization procedure. Indeed we show that the dipion mass distributions in the two-pion transitions of both charmonia and bottomonia states are explained by a unified mechanism based on the contribution of the ?? and KK? coupled channels including their interference (final-state interactions). Therefore, our main result is that the lower and higher radially excited states of charmonia and bottomonia have no specific features in mutual comparison and can be understood in a unified picture, e.g. proposed by our approach. | ||
333 | _aРежим доступа: по договору с организацией-держателем ресурса | ||
461 |
_tPhysical Review D _oparticles, fields, gravitation, and cosmology _oScientific Journal _d1970- |
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463 |
_tVol. 92, iss. 3 _v[036002] _d2015 |
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610 | 1 | _aэлектронный ресурс | |
610 | 1 | _aтруды учёных ТПУ | |
701 | 1 |
_aSurovtsev _bYu. S. _gYury Stepanovich |
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701 | 1 |
_aBydzovsky _bP. |
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701 | 1 |
_aGutsche _bT. _gThomas |
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701 | 1 |
_aKaminski _bR. _gRobert |
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701 | 1 |
_aNagy _bM. _gMiroslav |
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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 |
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712 | 0 | 2 |
_aНациональный исследовательский Томский политехнический университет (ТПУ) _bФизико-технический институт (ФТИ) _bКафедра высшей математики и математической физики (ВММФ) _h139 _2stltpush _3(RuTPU)RU\TPU\col\18727 |
801 | 2 |
_aRU _b63413507 _c20171123 _gRCR |
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856 | 4 | _uhttp://dx.doi.org/10.1103/PhysRevD.92.036002 | |
942 | _cCF |