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{"title":"B s的研究","authors":"Su-Ping Jin, Zhen-Jun Xiao","doi":"10.1155/2021/3840623","DOIUrl":null,"url":null,"abstract":"<jats:p>In this paper, we studied systematically the semileptonic decays <jats:inline-formula>\n <math xmlns=\"http://www.w3.org/1998/Math/MathML\" id=\"M2\">\n <msub>\n <mrow>\n <mi>B</mi>\n </mrow>\n <mrow>\n <mi>s</mi>\n </mrow>\n </msub>\n <mo>⟶</mo>\n <mi>ϕ</mi>\n <msup>\n <mrow>\n <mi>l</mi>\n </mrow>\n <mrow>\n <mo>+</mo>\n </mrow>\n </msup>\n <msup>\n <mrow>\n <mi>l</mi>\n </mrow>\n <mrow>\n <mo>−</mo>\n </mrow>\n </msup>\n </math>\n </jats:inline-formula> with <jats:inline-formula>\n <math xmlns=\"http://www.w3.org/1998/Math/MathML\" id=\"M3\">\n <msup>\n <mrow>\n <mi>l</mi>\n </mrow>\n <mrow>\n <mo>−</mo>\n </mrow>\n </msup>\n <mo>=</mo>\n <mfenced open=\"(\" close=\")\">\n <mrow>\n <msup>\n <mrow>\n <mi>e</mi>\n </mrow>\n <mrow>\n <mo>−</mo>\n </mrow>\n </msup>\n <mo>,</mo>\n <msup>\n <mrow>\n <mi>μ</mi>\n </mrow>\n <mrow>\n <mo>−</mo>\n </mrow>\n </msup>\n <mo>,</mo>\n <msup>\n <mrow>\n <mi>τ</mi>\n </mrow>\n <mrow>\n <mo>−</mo>\n </mrow>\n </msup>\n </mrow>\n </mfenced>\n </math>\n </jats:inline-formula> by using the perturbative QCD (PQCD) and the “PQCD+Lattice” factorization approach, respectively. We first evaluated all relevant form factors <jats:inline-formula>\n <math xmlns=\"http://www.w3.org/1998/Math/MathML\" id=\"M4\">\n <msub>\n <mrow>\n <mi>F</mi>\n </mrow>\n <mrow>\n <mi>i</mi>\n </mrow>\n </msub>\n <mfenced open=\"(\" close=\")\">\n <mrow>\n <msup>\n <mrow>\n <mi>q</mi>\n </mrow>\n <mrow>\n <mn>2</mn>\n </mrow>\n </msup>\n </mrow>\n </mfenced>\n </math>\n </jats:inline-formula> in the low-<jats:inline-formula>\n <math xmlns=\"http://www.w3.org/1998/Math/MathML\" id=\"M5\">\n <msup>\n <mrow>\n <mi>q</mi>\n </mrow>\n <mrow>\n <mn>2</mn>\n </mrow>\n </msup>\n </math>\n </jats:inline-formula> region using the PQCD approach, and we also took the available lattice QCD results at the high-<jats:inline-formula>\n <math xmlns=\"http://www.w3.org/1998/Math/MathML\" id=\"M6\">\n <msup>\n <mrow>\n <mi>q</mi>\n </mrow>\n <mrow>\n <mn>2</mn>\n </mrow>\n </msup>\n </math>\n </jats:inline-formula> region as additional input to improve the extrapolation of <jats:inline-formula>\n <math xmlns=\"http://www.w3.org/1998/Math/MathML\" id=\"M7\">\n <msub>\n <mrow>\n <mi>F</mi>\n </mrow>\n <mrow>\n <mi>i</mi>\n </mrow>\n </msub>\n <mfenced open=\"(\" close=\")\">\n <mrow>\n <msup>\n <mrow>\n <mi>q</mi>\n </mrow>\n <mrow>\n <mn>2</mn>\n </mrow>\n </msup>\n </mrow>\n </mfenced>\n </math>\n </jats:inline-formula> from the low-<jats:inline-formula>\n <math xmlns=\"http://www.w3.org/1998/Math/MathML\" id=\"M8\">\n <msup>\n <mrow>\n <mi>q</mi>\n </mrow>\n <mrow>\n <mn>2</mn>\n </mrow>\n </msup>\n </math>\n </jats:inline-formula> region to the endpoint <jats:inline-formula>\n <math xmlns=\"http://www.w3.org/1998/Math/MathML\" id=\"M9\">\n <msubsup>\n <mrow>\n <mi>q</mi>\n </mrow>\n <mrow>\n <mi mathvariant=\"normal\">max</mi>\n </mrow>\n <mrow>\n <mn>2</mn>\n </mrow>\n </msubsup>\n </math>\n </jats:inline-formula>. We then calculated the branching ratios and many other physical observables <jats:inline-formula>\n <math xmlns=\"http://www.w3.org/1998/Math/MathML\" id=\"M10\">\n <msubsup>\n <mrow>\n <mi>A</mi>\n </mrow>\n <mrow>\n <mtext>FB</mtext>\n </mrow>\n <mrow>\n <mi>l</mi>\n </mrow>\n </msubsup>\n </math>\n </jats:inline-formula>, <jats:inline-formula>\n <math xmlns=\"http://www.w3.org/1998/Math/MathML\" id=\"M11\">\n <msubsup>\n <mrow>\n <mi>F</mi>\n </mrow>\n <mrow>\n <mi>L</mi>\n </mrow>\n <mrow>\n <mi>ϕ</mi>\n </mrow>\n </msubsup>\n </math>\n </jats:inline-formula>, <jats:inline-formula>\n <math xmlns=\"http://www.w3.org/1998/Math/MathML\" id=\"M12\">\n <msub>\n <mrow>\n <mi>S</mi>\n </mrow>\n <mrow>\n <mn>3</mn>\n <mo>,</mo>\n <mn>4</mn>\n <mo>,</mo>\n <mn>7</mn>\n </mrow>\n </msub>\n </math>\n </jats:inline-formula>, and <jats:inline-formula>\n <math xmlns=\"http://www.w3.org/1998/Math/MathML\" id=\"M13\">\n <msub>\n <mrow>\n <mi>A</mi>\n </mrow>\n <mrow>\n <mn>5</mn>\n <mo>,</mo>\n <mn>6</mn>\n <mo>,</mo>\n <mn>8</mn>\n <mo>,</mo>\n <mn>9</mn>\n </mrow>\n </msub>\n </math>\n </jats:inline-formula> and the clean angular observables <jats:inline-formula>\n <math xmlns=\"http://www.w3.org/1998/Math/MathML\" id=\"M14\">\n <msub>\n <mrow>\n <mi>P</mi>\n </mrow>\n <mrow>\n <mn>1</mn>\n ","PeriodicalId":7498,"journal":{"name":"Advances in High Energy Physics","volume":" ","pages":""},"PeriodicalIF":1.5000,"publicationDate":"2021-11-09","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"1","resultStr":"{\"title\":\"Study of \\n \\n \\n B\\n \\n \\n s\\n \\n \\n ⟶\\n ϕ\\n \\n \",\"authors\":\"Su-Ping Jin, Zhen-Jun Xiao\",\"doi\":\"10.1155/2021/3840623\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"<jats:p>In this paper, we studied systematically the semileptonic decays <jats:inline-formula>\\n <math xmlns=\\\"http://www.w3.org/1998/Math/MathML\\\" id=\\\"M2\\\">\\n <msub>\\n <mrow>\\n <mi>B</mi>\\n </mrow>\\n <mrow>\\n <mi>s</mi>\\n </mrow>\\n </msub>\\n <mo>⟶</mo>\\n <mi>ϕ</mi>\\n <msup>\\n <mrow>\\n <mi>l</mi>\\n </mrow>\\n <mrow>\\n <mo>+</mo>\\n </mrow>\\n </msup>\\n <msup>\\n <mrow>\\n <mi>l</mi>\\n </mrow>\\n <mrow>\\n <mo>−</mo>\\n </mrow>\\n </msup>\\n </math>\\n </jats:inline-formula> with <jats:inline-formula>\\n <math xmlns=\\\"http://www.w3.org/1998/Math/MathML\\\" id=\\\"M3\\\">\\n <msup>\\n <mrow>\\n <mi>l</mi>\\n </mrow>\\n <mrow>\\n <mo>−</mo>\\n </mrow>\\n </msup>\\n <mo>=</mo>\\n <mfenced open=\\\"(\\\" close=\\\")\\\">\\n <mrow>\\n <msup>\\n <mrow>\\n <mi>e</mi>\\n </mrow>\\n <mrow>\\n <mo>−</mo>\\n </mrow>\\n </msup>\\n <mo>,</mo>\\n <msup>\\n <mrow>\\n <mi>μ</mi>\\n </mrow>\\n <mrow>\\n <mo>−</mo>\\n </mrow>\\n </msup>\\n <mo>,</mo>\\n <msup>\\n <mrow>\\n <mi>τ</mi>\\n </mrow>\\n <mrow>\\n <mo>−</mo>\\n </mrow>\\n </msup>\\n </mrow>\\n </mfenced>\\n </math>\\n </jats:inline-formula> by using the perturbative QCD (PQCD) and the “PQCD+Lattice” factorization approach, respectively. We first evaluated all relevant form factors <jats:inline-formula>\\n <math xmlns=\\\"http://www.w3.org/1998/Math/MathML\\\" id=\\\"M4\\\">\\n <msub>\\n <mrow>\\n <mi>F</mi>\\n </mrow>\\n <mrow>\\n <mi>i</mi>\\n </mrow>\\n </msub>\\n <mfenced open=\\\"(\\\" close=\\\")\\\">\\n <mrow>\\n <msup>\\n <mrow>\\n <mi>q</mi>\\n </mrow>\\n <mrow>\\n <mn>2</mn>\\n </mrow>\\n </msup>\\n </mrow>\\n </mfenced>\\n </math>\\n </jats:inline-formula> in the low-<jats:inline-formula>\\n <math xmlns=\\\"http://www.w3.org/1998/Math/MathML\\\" id=\\\"M5\\\">\\n <msup>\\n <mrow>\\n <mi>q</mi>\\n </mrow>\\n <mrow>\\n <mn>2</mn>\\n </mrow>\\n </msup>\\n </math>\\n </jats:inline-formula> region using the PQCD approach, and we also took the available lattice QCD results at the high-<jats:inline-formula>\\n <math xmlns=\\\"http://www.w3.org/1998/Math/MathML\\\" id=\\\"M6\\\">\\n <msup>\\n <mrow>\\n <mi>q</mi>\\n </mrow>\\n <mrow>\\n <mn>2</mn>\\n </mrow>\\n </msup>\\n </math>\\n </jats:inline-formula> region as additional input to improve the extrapolation of <jats:inline-formula>\\n <math xmlns=\\\"http://www.w3.org/1998/Math/MathML\\\" id=\\\"M7\\\">\\n <msub>\\n <mrow>\\n <mi>F</mi>\\n </mrow>\\n <mrow>\\n <mi>i</mi>\\n </mrow>\\n </msub>\\n <mfenced open=\\\"(\\\" close=\\\")\\\">\\n <mrow>\\n <msup>\\n <mrow>\\n <mi>q</mi>\\n </mrow>\\n <mrow>\\n <mn>2</mn>\\n </mrow>\\n </msup>\\n </mrow>\\n </mfenced>\\n </math>\\n </jats:inline-formula> from the low-<jats:inline-formula>\\n <math xmlns=\\\"http://www.w3.org/1998/Math/MathML\\\" id=\\\"M8\\\">\\n <msup>\\n <mrow>\\n <mi>q</mi>\\n </mrow>\\n <mrow>\\n <mn>2</mn>\\n </mrow>\\n </msup>\\n </math>\\n </jats:inline-formula> region to the endpoint <jats:inline-formula>\\n <math xmlns=\\\"http://www.w3.org/1998/Math/MathML\\\" id=\\\"M9\\\">\\n <msubsup>\\n <mrow>\\n <mi>q</mi>\\n </mrow>\\n <mrow>\\n <mi mathvariant=\\\"normal\\\">max</mi>\\n </mrow>\\n <mrow>\\n <mn>2</mn>\\n </mrow>\\n </msubsup>\\n </math>\\n </jats:inline-formula>. We then calculated the branching ratios and many other physical observables <jats:inline-formula>\\n <math xmlns=\\\"http://www.w3.org/1998/Math/MathML\\\" id=\\\"M10\\\">\\n <msubsup>\\n <mrow>\\n <mi>A</mi>\\n </mrow>\\n <mrow>\\n <mtext>FB</mtext>\\n </mrow>\\n <mrow>\\n <mi>l</mi>\\n </mrow>\\n </msubsup>\\n </math>\\n </jats:inline-formula>, <jats:inline-formula>\\n <math xmlns=\\\"http://www.w3.org/1998/Math/MathML\\\" id=\\\"M11\\\">\\n <msubsup>\\n <mrow>\\n <mi>F</mi>\\n </mrow>\\n <mrow>\\n <mi>L</mi>\\n </mrow>\\n <mrow>\\n <mi>ϕ</mi>\\n </mrow>\\n </msubsup>\\n </math>\\n </jats:inline-formula>, <jats:inline-formula>\\n <math xmlns=\\\"http://www.w3.org/1998/Math/MathML\\\" id=\\\"M12\\\">\\n <msub>\\n <mrow>\\n <mi>S</mi>\\n </mrow>\\n <mrow>\\n <mn>3</mn>\\n <mo>,</mo>\\n <mn>4</mn>\\n <mo>,</mo>\\n <mn>7</mn>\\n </mrow>\\n </msub>\\n </math>\\n </jats:inline-formula>, and <jats:inline-formula>\\n <math xmlns=\\\"http://www.w3.org/1998/Math/MathML\\\" id=\\\"M13\\\">\\n <msub>\\n <mrow>\\n <mi>A</mi>\\n </mrow>\\n <mrow>\\n <mn>5</mn>\\n <mo>,</mo>\\n <mn>6</mn>\\n <mo>,</mo>\\n <mn>8</mn>\\n <mo>,</mo>\\n <mn>9</mn>\\n </mrow>\\n </msub>\\n </math>\\n </jats:inline-formula> and the clean angular observables <jats:inline-formula>\\n <math xmlns=\\\"http://www.w3.org/1998/Math/MathML\\\" id=\\\"M14\\\">\\n <msub>\\n <mrow>\\n <mi>P</mi>\\n </mrow>\\n <mrow>\\n <mn>1</mn>\\n \",\"PeriodicalId\":7498,\"journal\":{\"name\":\"Advances in High Energy Physics\",\"volume\":\" \",\"pages\":\"\"},\"PeriodicalIF\":1.5000,\"publicationDate\":\"2021-11-09\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"1\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"Advances in High Energy Physics\",\"FirstCategoryId\":\"101\",\"ListUrlMain\":\"https://doi.org/10.1155/2021/3840623\",\"RegionNum\":4,\"RegionCategory\":\"物理与天体物理\",\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"Q3\",\"JCRName\":\"PHYSICS, PARTICLES & FIELDS\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"Advances in High Energy Physics","FirstCategoryId":"101","ListUrlMain":"https://doi.org/10.1155/2021/3840623","RegionNum":4,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q3","JCRName":"PHYSICS, PARTICLES & FIELDS","Score":null,"Total":0}
引用次数: 1
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Study of
B
s
⟶
ϕ
In this paper, we studied systematically the semileptonic decays
B
s
⟶
ϕ
l
+
l
−
with
l
−
=
e
−
,
μ
−
,
τ
−
by using the perturbative QCD (PQCD) and the “PQCD+Lattice” factorization approach, respectively. We first evaluated all relevant form factors
F
i
q
2
in the low-
q
2
region using the PQCD approach, and we also took the available lattice QCD results at the high-
q
2
region as additional input to improve the extrapolation of
F
i
q
2
from the low-
q
2
region to the endpoint
q
max
2
. We then calculated the branching ratios and many other physical observables
A
FB
l
,
F
L
ϕ
,
S
3
,
4
,
7
, and
A
5
,
6
,
8
,
9
and the clean angular observables
P
1