On the<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mrow><mml:mrow><mml:mover><mml:mrow><mml:mi>τ</mml:mi></mml:mrow><mml:mrow><mml:mo>→</mml:mo></mml:mrow></mml:mover></mml:mrow></mml:mrow><mml:mi>VP</mml:mi><mml:mrow><mml:msub><mml:mrow><mml:mi>ν</mml:mi></mml:mrow><mml:mrow><mml:mi>τ</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:math>decays
K. R. NasriddinovInstitute of Nuclear Physics, Academy of Sciences of Uzbekistan, Ulugbek, Tashkent, 702132 UzbekistanT. A. MerkulovaInstitute of Nuclear Physics, Academy of Sciences of Uzbekistan, Ulugbek, Tashkent, 702132 Uzbekistan
Physical review. D. Particles, fields, gravitation, and cosmology/Physical review. D. Particles and fieldsjournal1998lv
ABI
Аннотация
The $\stackrel{\ensuremath{\rightarrow}}{\ensuremath{\tau}}\mathrm{VP}{\ensuremath{\nu}}_{\ensuremath{\tau}}$ decays of the $\ensuremath{\tau}$ lepton are studied using the method of phenomenological chiral Lagrangians. The expressions of weak hadronic currents between pseudoscalar and vector meson states and the strong interaction Lagrangian between axial-vector, vector, and pseudoscalar mesons are obtained. Calculated partial widths for these decays are compared with the available theoretical and experimental data.
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