the results show that this method is consistent and allows to extract the same coupling constant for the vertex.doi:10.1590/S0103-97332004000200019M. E. BraccoM. ChiappariniF. S. NavarraM. NielsenBrazilian Journal of Physics
C Pallis,ME Gomez - 《Sissa》 被引量: 144发表: 2003年 Dirac Fermions in Borophene Honeycomb structures of group IV elements can host massless Dirac fermions with nontrivial Berry phases. Their potential for electronic applications has attracted great interest and spurred a broad search for new Di...
Op37qjUrHAv9XjkLoCD3zWZwRrIzlxRwp4cXl9Wp900xmURaViNY8gyhaRXa5WDUGoVMnnoG3IFBmwQL2bfu/0AhIJ6mvCsVKOjULtxlhqRjidpDqRoiEmIzygjqE+FlS58ezkCTwySg/2A2nK13Cmfp+IsVBqLLwTT5hmgfVQ/ban4l+eE+l+xY2ZH0aa+mS+qx9xqAM4jQD2mKRE87EhmEhmzoVkiCUm2gSVMjl8PQv/J81c1i5k7ZtCpna2SCQJDsAhOAY2KIMau...
R. Aaij et al., Measurement of the nuclear modifica- tion and pfapctocrollainsidonpsroamt p√t scNhaNrge=d particle production in 5 TeV. Phys. Rev. pPb Lett. 128(14), 142004 (2022). https://doi.org/10.1103/PhysRevLett. 128.142004. arXiv:2108.13115 [hep-ex] 28. R. Aaij et ...
PS(2) 2 + … PS(3) +… =1 2s + UV counter-term + 2Re + 2Re +2 +2 + … + UV C.T. = σ (0 2 ) + σ (1) 2 + σ (1) 3 Born June 6, 2006 O(αs) 3-particle phase space 6 Jianwei Qiu, ISU Lowest order contribution Lowest order Feynman diagram: p1 k1 ...
低能QCD的广义动力学模型
For the decay B→ηc(ρ→ππ), the differential decay rate is written as(13)dBds=τB|p1→||p3→|32π3mB3|A|2, with the kinematic variables |p1→| and |p3→|(14)|p1→|=12s−4mπ2,|p3→|=12[(mB2−mηc2)2−2(mB2+mηc2)s+s2]/s, where τB±=1.638ps,τB0=1.52...
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This review explores the current understanding of collective excitations and the dynamics of heavy quark propagation in the quark-gluon plasma (QGP) formed
The high-energy behavior of the total cross section for highly virtual photons, as predicted by the BFKL equation at next-to-leading order (NLO) in QCD, is