Study of <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mi>B</mml:mi><mml:mo stretchy="false">→</mml:mo><mml:mi>P</mml:mi><mml:mi>P</mml:mi></mml:math> decays in the modified perturbative QCD approach

We study the nonleptonic decays of <a:math xmlns:a="http://www.w3.org/1998/Math/MathML" display="inline"><a:mi>B</a:mi><a:mo stretchy="false">→</a:mo><a:mi>P</a:mi><a:mi>P</a:mi></a:math> in the modified perturbative QCD approach, where <d:math xmlns:d="http://www.w3.org/1998/Math/MathML" display="inline"><d:mi>P</d:mi></d:math> stands for pseudoscalar mesons. Transverse momenta of partons and the Sudakov factor are included, which help to suppress the contributions of soft interactions. The wave function of the <f:math xmlns:f="http://www.w3.org/1998/Math/MathML" display="inline"><f:mi>B</f:mi></f:math> meson obtained from the relativistic potential model is used, and then the contributions in the infrared region cannot be suppressed completely. So a soft cutoff scale and soft form factors are introduced. The contributions with the scale higher than the soft cutoff scale are calculated with perturbative QCD, while the contributions lower than the cutoff scale are replaced by the soft form factors. To explain experimental data, we find that contributions of color-octet operators for the quark-antiquarks in the mesons in the final state need to be considered. The contributions of the color-octet operators are parametrized by a few parameters with the help of SU(3) flavor symmetry and symmetry breaking. These parameters for color-octet contributions are universal for all the nonleptonic decay modes of the <h:math xmlns:h="http://www.w3.org/1998/Math/MathML" display="inline"><h:mi>B</h:mi></h:math> meson, where the mesons in the final state belong to the same flavor SU(3) nonet. Both the branching ratios and <j:math xmlns:j="http://www.w3.org/1998/Math/MathML" display="inline"><j:mi>C</j:mi><j:mi>P</j:mi></j:math> violations are studied. We find that the theoretical calculation can well explain the experimental data of <l:math xmlns:l="http://www.w3.org/1998/Math/MathML" display="inline"><l:mi>B</l:mi></l:math> factories. Published by the American Physical Society 2024

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Publication Details

Journal
Physical review. D/Physical review. D.
Published
2024-09-13
DOI
https://doi.org/10.1103/physrevd.110.056025
Citations
3
Primary Topic
Particle physics theoretical and experimental studies
Type
article
Field-Weighted Citation Impact
1.98

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article

Study of <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mi>B</mml:mi><mml:mo stretchy="false">→</mml:mo><mml:mi>P</mml:mi><mml:mi>P</mml:mi></mml:math> decays in the modified perturbative QCD approach

Ru-Xuan Wang, Sheng Lü, Mao-Zhi Yang
3 citations
Physical review. D/Physical review. D.
Particle physics theoretical and experimental studies
1.98
article

Study of <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mi>B</mml:mi><mml:mo stretchy="false">→</mml:mo><mml:mi>P</mml:mi><mml:mi>P</mml:mi></mml:math> decays in the modified perturbative QCD approach

Ru-Xuan Wang, Sheng Lü, Mao-Zhi Yang
article en
3 citations

Abstract

We study the nonleptonic decays of <a:math xmlns:a="http://www.w3.org/1998/Math/MathML" display="inline"><a:mi>B</a:mi><a:mo stretchy="false">→</a:mo><a:mi>P</a:mi><a:mi>P</a:mi></a:math> in the modified perturbative QCD approach, where <d:math xmlns:d="http://www.w3.org/1998/Math/MathML" display="inline"><d:mi>P</d:mi></d:math> stands for pseudoscalar mesons. Transverse momenta of partons and the Sudakov factor are included, which help to suppress the contributions of soft interactions. The wave function of the <f:math xmlns:f="http://www.w3.org/1998/Math/MathML" display="inline"><f:mi>B</f:mi></f:math> meson obtained from the relativistic potential model is used, and then the contributions in the infrared region cannot be suppressed completely. So a soft cutoff scale and soft form factors are introduced. The contributions with the scale higher than the soft cutoff scale are calculated with perturbative QCD, while the contributions lower than the cutoff scale are replaced by the soft form factors. To explain experimental data, we find that contributions of color-octet operators for the quark-antiquarks in the mesons in the final state need to be considered. The contributions of the color-octet operators are parametrized by a few parameters with the help of SU(3) flavor symmetry and symmetry breaking. These parameters for color-octet contributions are universal for all the nonleptonic decay modes of the <h:math xmlns:h="http://www.w3.org/1998/Math/MathML" display="inline"><h:mi>B</h:mi></h:math> meson, where the mesons in the final state belong to the same flavor SU(3) nonet. Both the branching ratios and <j:math xmlns:j="http://www.w3.org/1998/Math/MathML" display="inline"><j:mi>C</j:mi><j:mi>P</j:mi></j:math> violations are studied. We find that the theoretical calculation can well explain the experimental data of <l:math xmlns:l="http://www.w3.org/1998/Math/MathML" display="inline"><l:mi>B</l:mi></l:math> factories. Published by the American Physical Society 2024

Physical review. D/Physical review. D.Vol. 110(5)
Nankai University (CN)
National Natural Science Foundation of China
Openalex Percentile: Top 9%
Particle physics theoretical and experimental studies
1.98
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