Perturbative QCD analysis of neutral $B$-meson decays into $\sigma\sigma, \sigma f_0$ and $f_0 f_0
The decays of $B_{d,s}^0 \to \sigma\sigma, \sigma f_0, f_0 f_0$, with $\sigma$ and $f_0$ denoting the light scalar mesons $f_0(500)$ and $f_0(980)$ in the two-quark picture, are studied in the perturbative QCD approach based on $k_T$ factorization. With the referenced value of the mixing angle $|\va...
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creator | Niu, Hua-Dian Li, Guo-Dong Ren, Jia-Le Liu, Xin |
description | The decays of $B_{d,s}^0 \to \sigma\sigma, \sigma f_0, f_0 f_0$, with
$\sigma$ and $f_0$ denoting the light scalar mesons $f_0(500)$ and $f_0(980)$
in the two-quark picture, are studied in the perturbative QCD approach based on
$k_T$ factorization. With the referenced value of the mixing angle $|\varphi|
\sim 25^\circ$ for the $\sigma-f_0$ mixing in the quark-flavor basis, it is of
great interest to obtain that: (a) these neutral $B$-meson decays into
$\sigma\sigma, \sigma f_0$, and $f_0 f_0$ have large branching ratios in the
order of $10^{-6} \sim 10^{-4}$, which mean the possibly constructive
interferences existed in the decays with different flavor states, and then are
expected to be tested at the Large Hadron Collider beauty and/or Belle-II
experiments in the (near) future; (b) the large direct CP violations could be
easily found in the $B_d^0 \to \sigma\sigma, f_0 f_0$ and $B_{d,s}^0 \to \sigma
f_0$ decays, which indicate the considerable interferences between the tree and
the penguin decay amplitudes involved in these four modes, and would be
confronted with the future measurements; (c) these neutral $B$-meson decays
could be examined through the secondary decay chain $\sigma/f_0 \to \pi^+
\pi^-$, namely, the four-body decays of $B_{d,s}^0 \to (\pi^+
\pi^-)_{\sigma(f_0)} (\pi^+ \pi^-)_{\sigma(f_0)}$. On the other side, it seems
that other 4 four-body decays of $B_d^0 \to (\pi^+ \pi^-)_{\sigma} (K^+
K^-)_{f_0}$, $B_s^0 \to (\pi^+ \pi^-)_{\sigma(f_0)} (K^+ K^-)_{f_0}$, and
$B_s^0 \to (K^+ K^-)_{f_0} (K^+ K^-)_{f_0}$ could also be detected at the
relevant experiments, if the $f_0 \to K^+ K^-$ could be identified from the
$\phi \to K^+ K^-$ clearly. |
doi_str_mv | 10.48550/arxiv.2110.01217 |
format | Article |
fullrecord | <record><control><sourceid>arxiv_GOX</sourceid><recordid>TN_cdi_arxiv_primary_2110_01217</recordid><sourceformat>XML</sourceformat><sourcesystem>PC</sourcesystem><sourcerecordid>2110_01217</sourcerecordid><originalsourceid>FETCH-arxiv_primary_2110_012173</originalsourceid><addsrcrecordid>eNpjYJA0NNAzsTA1NdBPLKrILNMzMgQKGBgaGZpzMiQFpBaVlBYlJZZklqUqBDq7KCTmJeZUFmcWK-SnKeSllpYUJeYoqDip6OamFufnKaSkJidWFitk5pXkK6jEFGem5yZCSB0FCK2QFm-gAjQkRUEFyALxeBhY0xJzilN5oTQ3g7yba4izhy7YNfEFRZm5iUWV8SBXxYNdZUxYBQDPkEBp</addsrcrecordid><sourcetype>Open Access Repository</sourcetype><iscdi>true</iscdi><recordtype>article</recordtype></control><display><type>article</type><title>Perturbative QCD analysis of neutral $B$-meson decays into $\sigma\sigma, \sigma f_0$ and $f_0 f_0</title><source>arXiv.org</source><creator>Niu, Hua-Dian ; Li, Guo-Dong ; Ren, Jia-Le ; Liu, Xin</creator><creatorcontrib>Niu, Hua-Dian ; Li, Guo-Dong ; Ren, Jia-Le ; Liu, Xin</creatorcontrib><description>The decays of $B_{d,s}^0 \to \sigma\sigma, \sigma f_0, f_0 f_0$, with
$\sigma$ and $f_0$ denoting the light scalar mesons $f_0(500)$ and $f_0(980)$
in the two-quark picture, are studied in the perturbative QCD approach based on
$k_T$ factorization. With the referenced value of the mixing angle $|\varphi|
\sim 25^\circ$ for the $\sigma-f_0$ mixing in the quark-flavor basis, it is of
great interest to obtain that: (a) these neutral $B$-meson decays into
$\sigma\sigma, \sigma f_0$, and $f_0 f_0$ have large branching ratios in the
order of $10^{-6} \sim 10^{-4}$, which mean the possibly constructive
interferences existed in the decays with different flavor states, and then are
expected to be tested at the Large Hadron Collider beauty and/or Belle-II
experiments in the (near) future; (b) the large direct CP violations could be
easily found in the $B_d^0 \to \sigma\sigma, f_0 f_0$ and $B_{d,s}^0 \to \sigma
f_0$ decays, which indicate the considerable interferences between the tree and
the penguin decay amplitudes involved in these four modes, and would be
confronted with the future measurements; (c) these neutral $B$-meson decays
could be examined through the secondary decay chain $\sigma/f_0 \to \pi^+
\pi^-$, namely, the four-body decays of $B_{d,s}^0 \to (\pi^+
\pi^-)_{\sigma(f_0)} (\pi^+ \pi^-)_{\sigma(f_0)}$. On the other side, it seems
that other 4 four-body decays of $B_d^0 \to (\pi^+ \pi^-)_{\sigma} (K^+
K^-)_{f_0}$, $B_s^0 \to (\pi^+ \pi^-)_{\sigma(f_0)} (K^+ K^-)_{f_0}$, and
$B_s^0 \to (K^+ K^-)_{f_0} (K^+ K^-)_{f_0}$ could also be detected at the
relevant experiments, if the $f_0 \to K^+ K^-$ could be identified from the
$\phi \to K^+ K^-$ clearly.</description><identifier>DOI: 10.48550/arxiv.2110.01217</identifier><language>eng</language><subject>Physics - High Energy Physics - Experiment ; Physics - High Energy Physics - Phenomenology</subject><creationdate>2021-10</creationdate><rights>http://creativecommons.org/licenses/by/4.0</rights><oa>free_for_read</oa><woscitedreferencessubscribed>false</woscitedreferencessubscribed></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><link.rule.ids>228,230,776,881</link.rule.ids><linktorsrc>$$Uhttps://arxiv.org/abs/2110.01217$$EView_record_in_Cornell_University$$FView_record_in_$$GCornell_University$$Hfree_for_read</linktorsrc><backlink>$$Uhttps://doi.org/10.48550/arXiv.2110.01217$$DView paper in arXiv$$Hfree_for_read</backlink><backlink>$$Uhttps://doi.org/10.1140/epjc/s10052-022-10111-8$$DView published paper (Access to full text may be restricted)$$Hfree_for_read</backlink></links><search><creatorcontrib>Niu, Hua-Dian</creatorcontrib><creatorcontrib>Li, Guo-Dong</creatorcontrib><creatorcontrib>Ren, Jia-Le</creatorcontrib><creatorcontrib>Liu, Xin</creatorcontrib><title>Perturbative QCD analysis of neutral $B$-meson decays into $\sigma\sigma, \sigma f_0$ and $f_0 f_0</title><description>The decays of $B_{d,s}^0 \to \sigma\sigma, \sigma f_0, f_0 f_0$, with
$\sigma$ and $f_0$ denoting the light scalar mesons $f_0(500)$ and $f_0(980)$
in the two-quark picture, are studied in the perturbative QCD approach based on
$k_T$ factorization. With the referenced value of the mixing angle $|\varphi|
\sim 25^\circ$ for the $\sigma-f_0$ mixing in the quark-flavor basis, it is of
great interest to obtain that: (a) these neutral $B$-meson decays into
$\sigma\sigma, \sigma f_0$, and $f_0 f_0$ have large branching ratios in the
order of $10^{-6} \sim 10^{-4}$, which mean the possibly constructive
interferences existed in the decays with different flavor states, and then are
expected to be tested at the Large Hadron Collider beauty and/or Belle-II
experiments in the (near) future; (b) the large direct CP violations could be
easily found in the $B_d^0 \to \sigma\sigma, f_0 f_0$ and $B_{d,s}^0 \to \sigma
f_0$ decays, which indicate the considerable interferences between the tree and
the penguin decay amplitudes involved in these four modes, and would be
confronted with the future measurements; (c) these neutral $B$-meson decays
could be examined through the secondary decay chain $\sigma/f_0 \to \pi^+
\pi^-$, namely, the four-body decays of $B_{d,s}^0 \to (\pi^+
\pi^-)_{\sigma(f_0)} (\pi^+ \pi^-)_{\sigma(f_0)}$. On the other side, it seems
that other 4 four-body decays of $B_d^0 \to (\pi^+ \pi^-)_{\sigma} (K^+
K^-)_{f_0}$, $B_s^0 \to (\pi^+ \pi^-)_{\sigma(f_0)} (K^+ K^-)_{f_0}$, and
$B_s^0 \to (K^+ K^-)_{f_0} (K^+ K^-)_{f_0}$ could also be detected at the
relevant experiments, if the $f_0 \to K^+ K^-$ could be identified from the
$\phi \to K^+ K^-$ clearly.</description><subject>Physics - High Energy Physics - Experiment</subject><subject>Physics - High Energy Physics - Phenomenology</subject><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2021</creationdate><recordtype>article</recordtype><sourceid>GOX</sourceid><recordid>eNpjYJA0NNAzsTA1NdBPLKrILNMzMgQKGBgaGZpzMiQFpBaVlBYlJZZklqUqBDq7KCTmJeZUFmcWK-SnKeSllpYUJeYoqDip6OamFufnKaSkJidWFitk5pXkK6jEFGem5yZCSB0FCK2QFm-gAjQkRUEFyALxeBhY0xJzilN5oTQ3g7yba4izhy7YNfEFRZm5iUWV8SBXxYNdZUxYBQDPkEBp</recordid><startdate>20211004</startdate><enddate>20211004</enddate><creator>Niu, Hua-Dian</creator><creator>Li, Guo-Dong</creator><creator>Ren, Jia-Le</creator><creator>Liu, Xin</creator><scope>GOX</scope></search><sort><creationdate>20211004</creationdate><title>Perturbative QCD analysis of neutral $B$-meson decays into $\sigma\sigma, \sigma f_0$ and $f_0 f_0</title><author>Niu, Hua-Dian ; Li, Guo-Dong ; Ren, Jia-Le ; Liu, Xin</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-arxiv_primary_2110_012173</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2021</creationdate><topic>Physics - High Energy Physics - Experiment</topic><topic>Physics - High Energy Physics - Phenomenology</topic><toplevel>online_resources</toplevel><creatorcontrib>Niu, Hua-Dian</creatorcontrib><creatorcontrib>Li, Guo-Dong</creatorcontrib><creatorcontrib>Ren, Jia-Le</creatorcontrib><creatorcontrib>Liu, Xin</creatorcontrib><collection>arXiv.org</collection></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext_linktorsrc</fulltext></delivery><addata><au>Niu, Hua-Dian</au><au>Li, Guo-Dong</au><au>Ren, Jia-Le</au><au>Liu, Xin</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Perturbative QCD analysis of neutral $B$-meson decays into $\sigma\sigma, \sigma f_0$ and $f_0 f_0</atitle><date>2021-10-04</date><risdate>2021</risdate><abstract>The decays of $B_{d,s}^0 \to \sigma\sigma, \sigma f_0, f_0 f_0$, with
$\sigma$ and $f_0$ denoting the light scalar mesons $f_0(500)$ and $f_0(980)$
in the two-quark picture, are studied in the perturbative QCD approach based on
$k_T$ factorization. With the referenced value of the mixing angle $|\varphi|
\sim 25^\circ$ for the $\sigma-f_0$ mixing in the quark-flavor basis, it is of
great interest to obtain that: (a) these neutral $B$-meson decays into
$\sigma\sigma, \sigma f_0$, and $f_0 f_0$ have large branching ratios in the
order of $10^{-6} \sim 10^{-4}$, which mean the possibly constructive
interferences existed in the decays with different flavor states, and then are
expected to be tested at the Large Hadron Collider beauty and/or Belle-II
experiments in the (near) future; (b) the large direct CP violations could be
easily found in the $B_d^0 \to \sigma\sigma, f_0 f_0$ and $B_{d,s}^0 \to \sigma
f_0$ decays, which indicate the considerable interferences between the tree and
the penguin decay amplitudes involved in these four modes, and would be
confronted with the future measurements; (c) these neutral $B$-meson decays
could be examined through the secondary decay chain $\sigma/f_0 \to \pi^+
\pi^-$, namely, the four-body decays of $B_{d,s}^0 \to (\pi^+
\pi^-)_{\sigma(f_0)} (\pi^+ \pi^-)_{\sigma(f_0)}$. On the other side, it seems
that other 4 four-body decays of $B_d^0 \to (\pi^+ \pi^-)_{\sigma} (K^+
K^-)_{f_0}$, $B_s^0 \to (\pi^+ \pi^-)_{\sigma(f_0)} (K^+ K^-)_{f_0}$, and
$B_s^0 \to (K^+ K^-)_{f_0} (K^+ K^-)_{f_0}$ could also be detected at the
relevant experiments, if the $f_0 \to K^+ K^-$ could be identified from the
$\phi \to K^+ K^-$ clearly.</abstract><doi>10.48550/arxiv.2110.01217</doi><oa>free_for_read</oa></addata></record> |
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subjects | Physics - High Energy Physics - Experiment Physics - High Energy Physics - Phenomenology |
title | Perturbative QCD analysis of neutral $B$-meson decays into $\sigma\sigma, \sigma f_0$ and $f_0 f_0 |
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