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非因子化方法研究B^-→π~0π^-衰变过程
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作者 吴向尧 尹新国 郭义庆 《南开大学学报(自然科学版)》 CAS CSCD 北大核心 2004年第1期118-121,共4页
本文用 QCD因子化和光锥 QCD求和规则系统地计算了 B- →π0 π- 衰变过程的强子矩阵元和分支比 ,其计算结果与实验相一致 .
关键词 B介子衰变 强子矩阵元 分支比
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高能碰撞中的粒子关联研究
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作者 戴启润 李积梅 李应真 《河南科学》 1997年第2期154-159,共6页
B-E关联与F-D关联是研究强子发射源的最有力工具之一。根据非微扰理论提出一种源分布-Q-νKν(Q)分布,据此研究全同π介子的B-E关联和全同质子的F-D关联。总结了轻子—轻子、核子—核子、介子—核。
关键词 强子 B-E关联 F-D关联 高能碰撞 强相互作用
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强子对撞中测量J/Ψ极化的方法(英文)
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作者 胡震 郭爽 +1 位作者 Eric James 钱思进 《北京大学学报(自然科学版)》 EI CAS CSCD 北大核心 2011年第3期397-403,共7页
描述测量J/Ψ介子极化的方法,该方法能够测量质心能量为10 TeV(或以上)的质子对撞中产生的J/Ψ介子的极化参量随其横向动量的变化,LHC上的CMS探测器收集到的前50 pb-1的数据就可以完成这项测量。研究了用于提取极化参量α的拟合过程的误... 描述测量J/Ψ介子极化的方法,该方法能够测量质心能量为10 TeV(或以上)的质子对撞中产生的J/Ψ介子的极化参量随其横向动量的变化,LHC上的CMS探测器收集到的前50 pb-1的数据就可以完成这项测量。研究了用于提取极化参量α的拟合过程的误差,并分析了相应的测量精度。该方法的测量精度受到统计误差和系统误差的影响,其量级为Δαstat<0.13,Δαsyst<0.01。在费米实验室的CDF实验上曾进行过J/Ψ极化的测量,其结果与非相对论QCD理论预言不符,在CMS上进行的再次测量将为这项研究提供更充足的信息。 展开更多
关键词 极化 J/Ψ B强子 CMS 模板 非相对论QCD
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~0→"非汉字符号"~0π~0衰变过程的分支比计算
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作者 朱晓梅 袁五届 尹新国 《安徽理工大学学报(自然科学版)》 CAS 2004年第3期81-84,共4页
由于衰变过程中存在的非微扰问题,B介子的非轻子衰变的理论预言面临很大的挑战。在光锥QCD求和规则框架内,详细讨论在B0→K0π0衰变中软胶子交换对衰变振幅的贡献,系统地研究B0→K0π0衰变过程的强子矩阵元并计算了分支比,计算结果与实... 由于衰变过程中存在的非微扰问题,B介子的非轻子衰变的理论预言面临很大的挑战。在光锥QCD求和规则框架内,详细讨论在B0→K0π0衰变中软胶子交换对衰变振幅的贡献,系统地研究B0→K0π0衰变过程的强子矩阵元并计算了分支比,计算结果与实验结果相一致。 展开更多
关键词 B介子衰变 强子矩阵元 分支比
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Analysis of the decay B^0→χc1~π~0 with light-cone QCD sum rules
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作者 王志刚 《Chinese Physics B》 SCIE EI CAS CSCD 2009年第9期3803-3809,共7页
In this article, we calculate the contribution from the nonfactorizable soft hadronic matrix element to the decay B^0→Xc1π^0 with the light-cone quantum chromo-dynamic (QCD) sum rules. The numerical results show t... In this article, we calculate the contribution from the nonfactorizable soft hadronic matrix element to the decay B^0→Xc1π^0 with the light-cone quantum chromo-dynamic (QCD) sum rules. The numerical results show that its contribution is rather large and should not be neglected. The total amplitudes lead to a branching fraction which is in agreement with the experimental data marginally. 展开更多
关键词 light-cone QCD sum rule B-decay nonfactorizable hadronic matrix element
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Feasibility study of a J/ψ cross section measurement with early CMS data 被引量:1
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作者 杨宗长 钱思进 《Chinese Physics C》 SCIE CAS CSCD 2009年第8期609-616,共8页
We report the methods and plans for measuring the differential cross section of J/ψ→μ^+μ^- production, using data to be collected in the first LHC run by the CMS detector. Making use of the large B-hadron lifetim... We report the methods and plans for measuring the differential cross section of J/ψ→μ^+μ^- production, using data to be collected in the first LHC run by the CMS detector. Making use of the large B-hadron lifetime, we show how to separate the promptly produced J/ψ’s from those coming from B-hadron decays. Since the J/ψ production cross section is expected to be large, the analysis should be viable with relatively small data sets, that will become available early in the startup of the LHC. We also address effects of a non-perfect detector alignment, as well as systematic uncertainties. About 70 thousand J/ψ decays are reconstructed from Monte Carlo data, which corresponds to an integrated luminosity of 3 pb^-1 in 14 TeV collisions, in the range of pT^J/ ψbetween 5 and 40 GeV/c. The precision of the result is limited by systematic uncertainties, and is at the 15% level. 展开更多
关键词 J/Ψ CMS b-hadron QCD
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关于■→■π~0衰变过程研究
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作者 吴向尧 尹新国 +3 位作者 郭义庆 张晓波 尹建华 谢远亮 《物理学报》 SCIE EI CAS CSCD 北大核心 2004年第4期1015-1019,共5页
系统地计算 B0 → K0 π0 衰变过程的强子矩阵元 ,它包括领头阶因子化部分 ,αs 修正的硬胶子交换部分和软胶子交换部分 .其中软胶子交换部分 ,无论在量子色动力学 (QCD)因子化方法中 ,还是在微扰QCD中都不能进行计算 .用光锥QCD求和... 系统地计算 B0 → K0 π0 衰变过程的强子矩阵元 ,它包括领头阶因子化部分 ,αs 修正的硬胶子交换部分和软胶子交换部分 .其中软胶子交换部分 ,无论在量子色动力学 (QCD)因子化方法中 ,还是在微扰QCD中都不能进行计算 .用光锥QCD求和规则系统地计算了这部分贡献 ,并发现在该衰变道中软胶子交换部分与领头阶因子化部分以及αs 修正的硬胶子交换部分有相同的数量级 ,因此不能忽略 .最后计算了该衰变过程的分支比 。 展开更多
关键词 B介子衰变 介子物理学 强子矩阵元 分支比 量子色动力学 微扰 湮没图 胶子交换部分
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Study of the production of Λ_b^0 band ~0 hadrons in pp collisions and first measurement of the Λ_b^0→J/ψpK^- branching fraction 被引量:23
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作者 O.Kochebina M.Kolpin +398 位作者 I.Komarov R.F.Koopman P.Koppenburg M.Kozeiha L.Kravchuk K.Kreplin M.Kreps G.Krocker P.Krokovny F.Kruse W.Krzemien W.Kucewicz M.Kucharczyk V.Kudryavtsev A.K.Kuonen K.Kurek T.Kvaratskheliya D.Lacarrere G.Lafferty A.Lai D.Lambert G.Lanffanchi C.Langenbruch B.Langhans T.Latham C.Lazzeroni R.Le Gac J.van Leerdam J.-P.Lees R.Lefevre A.Leflat J.Lefrancois E.Lemos Cid O.Leroy T.Lesiak B.Leverington Y.Li T.Likhomanenko M.Liles R.Lindner C.Linn F.Lionetto B.Liu X.Liu D.Loh I.Longstaff J.H.Lopes D.Lucchesi M.Lucio Martinez H.Luo A.Lupato E.Luppi O.Lupton A.Lusiani F.Machefert F.Maciuc O.Maev K.Maguire S.Malde A.Malinin G.Manca G.Mancinelli P.Manning A.Mapelli J.Maratas J.F.Marchand U.Marconi C.Marin Benito P.Marino J.Marks G.Martellottil M.Martin M.Martinelli D.Martinez Santos F.Martinez Vidal D.Martins Tostes A.Massafferri R.Matev A.Mathad Z.Mathe C.Matteuzzi A.Mauri B.Maurin A.Mazurov M.McCann J.McCarthy A.McNab R.McNulty B.Meadows F.Meier M.Meissner D.Melnychuk M.Merk E Michielin D.A.Milanes M.-N.Minard D.S.Mitzel J.Molina Rodrigue I.A.Monroy S.Monteil M.Morandin P.Morawski A.Morda M.J.Morello J.Moron A.B.Morris R.Mountain F.Muheim D.Miiller J.Muller K.Muller V.Muller M.Mussini B.Muster P.Naik T.Nakada R.Nandakumar A.Nandi I.Nasteva M.Needham N.Neri S.Neubert N.Neufeld M.Neuner A.D.Nguyen T.D.Nguyen C.Nguyen-Mau V.Niess R.Niet N.Nikitin T.Nikodem D.Ninci A.Novoselov D.P.O'Hanlon A.Oblakowska-Mucha V.Obraztsov S.Ogilvy O.Okhrimenko R.Oldeman C.J.G.Onderwater B.Osorio Rodrigues J.M.Otalora Goicochea A.Otto P.Owen A.Oyanguren A.Palano F.Palombo M.Palutan J.Panman A.Papanestis M.Pappagallo L.L.Pappalardo C.Pappenheimer C.Parkes G.Passaleva G.D.Patel M.Patel C.Patrignani A.Pearce A.Pellegrino G.Penso M.Pepe Altarelli S.Perazzini P.Perret L.Pescatore K.Petridis A.Petrolini M.Petruzzo E.Picatoste Olloqui B.Pietrzyk T:.Pilar D.Pinci A.Pistone A.Piucci S.Playfer M.Plo Casasus T.Poikela F.Polci A.Poluektov I.Polyakov E.Polycarpo A.Popov D.Popov B.Popovici C.Potterat E.Price J.D.Price J.Prisciandaro A.Pritchard C.Prouve V.Pugatch A.Puig Navarro G.Punzi W.Qian R.Quagliani B.Rachwal J.H.Rademacker M.Rama M.S.Rangel I.Raniuk N.Rauschmayr G.Raven F.Redi S.Reichert M.M.Reid A.C.dos Reis S.Ricciardi S.Richards M.Rihl K.Rinnert V.Rives Molina P.Robbe A.B.Rodrigues E.Rodrigues J.A.Rodriguez Lopez P.Rodriguez Perez S.Roiser V.Romanovsky A.Romero Vidalt J.W.R onayne M.Rotondo J.Rouvinet T.Ruf P.Ruiz Valls J.J.Saborido Silva N.Sagidova P.Sail B.Saitta V.Salustino Guimaraes C.Sanchez Mayordomo B.Sanmartin Sedes R.Santacesaria C.Santamarina Rios M.Santimaria E.Santovetti A.Sarti C.Satriano A.Satta D.M.Saunders D.Savrina M.Schiller H.Schindler M.Schlupp M.Schmelling T.Schmelzer B.Schmidt O.Schneider A.Schopper M.Schubiger M.-H.Schune R.Schwemmer B.Sciascia A.Sciubba A.Semennikov N.Serra J.Serrano L.Sestini P.Seyfert M.Shapkin I.Shapoval Y.Shcheglov T.Shears L.Shekhtman V.Shevchenko A.Shires B.G.Siddi R.Silva Coutinho L.Silva de Oliveira G.Simi M.Sirendi N.Skidmore T.Skwarnicki E.Smith E.Smith I.T.Smith J.Smith M.Smith H.Snoek M.D.Sokoloff F.J.P.Soler F.Soomro D.Souza B.Souza De Paula B.Spaan P.Spradlin S.Sridharan F.Stagni M.Stahl S.Stahl S.Stefkova O.Steinkamp O.Stenyakin S.Stevenson S.Stoica S.Stone B.Storaci S.Stracka M.Straticiuc U.Straumann L.Sun W.Sutcliffe K.Swientek S.Swientek V.Syropoulos M.Szczekowski P.Szczypka T.Szumlak S.T'Jampens A.Tayduganov T.Tekampe M.T eklishyn G.Teilarini F.Teubert C.Thomas E.Thomas J.van Tilburg V.Tisserand M.Tobin J.Todd S.Tolk L.Tomassetti D.Tonelli S.Topp-Joergensen N.Torr E.Tournefier S.Tourneur K.Trabelsi M.T.Tran M.Tresch A.Trisovic A.Tsaregorodtsev P.Tsopelas N.Tuning A.Ukleja A.Ustyuzhanin U.Uwer C.Vacca V.Vagnonit G.Valentit A.Vallier R.Vazquez Gomez P.Vazquez Regueiro C.Vazquez Sierra S.Vecchi J.J.Velthuis M.Veltri G.Veneziano M.Vesterinen B.Viaud D.Vieira M.Vieites Diaz X.Vitasis-Cardona V.Volkov A.Vollhardt D.Volyanskyy D.Voong A.Vorobyev V.Vorobyev C.Voβ J.A.de Vries R.Waldi C.Wallace R.Wallace J.Walsh S.Wandernoth J.Wang D.R.Ward N.K.Watson D.Websdale A.Weiden M.Whitehead G.Wilkinson M.Wilkinson M.Williams M.P.Williams T.Williams F.F.Wilson J.Wimberley J.Wishahi W.Wislicki M.Witek G.Wormser S.A.Wotton S.Wright K.Wyllie Y.Xie Z.Xu Z.Yang J.Yu X.Yuan O.Yushchenko M.Zangoli M.Zavertyaev L.Zhang Y.Zhang A.Zhelezov A.Zhokhov L.Zhong S.Zucchelli 《Chinese Physics C》 SCIE CAS CSCD 2016年第1期1-16,共16页
The product of the ∧0/b (-B/0) differential production cross-section and the branching fraction of the decay ∧0/b→ J/ψ pK-(-B/0→ J/ψ-K*(892)0)is measured as a function of the beauty hadron transverse mome... The product of the ∧0/b (-B/0) differential production cross-section and the branching fraction of the decay ∧0/b→ J/ψ pK-(-B/0→ J/ψ-K*(892)0)is measured as a function of the beauty hadron transverse momentum, PT, and rapidity, y. The kinematic region of the measurements is pT〈20 GeV/c and 2.0 〈g〈4.5.The measurements use a data sample corresponding to an integrated luminosity of 3fb-1 collected by the LHCb detector in pp collisions at centre-of-mass energies √s=7 TeV in 2011 and √s=8 TeV in 2012. Based on previous LHCb results of the fragmentation fraction ratio,f∧0/b/fd,the branching fraction of the decay ∧0/b→ J/ψ pK-is measured to be B(∧0/b→ J/ψ pK-)=(3.17±0.04±0.07±0.34+0.45/-0.28)×10-4,where the first uncertainty is statistical, the second is systematic, the third is due to the uncertainty on the branching fraction of the decay -B/0 →J/ψ-K*(892)0,and the fourth is due to the knowledge of f∧0/b/fd.The sum of the asymmetries in the production and decay between ∧0/b and ∧0/bis also measured as a function of PT and y.The previously published branching fraction of ∧0/b→ J/ψ pπ-,relative to that of ∧0/b→ J/ψ pK-,is updated. The branching fractions of ∧0/b→P+c(→ J/ψp)K-are determined. 展开更多
关键词 production cross-section branching fraction b hadrons proton-proton collisions
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An investigation of hadronization mechanism at a Z^0 factory 被引量:4
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作者 JIN Yi 1,SI ZongGuo 2,XIE QuBing 2 & YAO Tao 2 1 Department of Physics,University of Jinan,Jinan 250022,China 2 School of Physics,Shandong University,Jinan 250100,China 《Science China(Physics,Mechanics & Astronomy)》 SCIE EI CAS 2010年第11期1998-2004,共7页
We briefly review the hadronization pictures adopted in the LUND String Fragmentation Model (LSFM),Webber Cluster Fragmentation Model (WCFM) and Quark Combination Model (QCM),respectively.Predictions of hadron multipl... We briefly review the hadronization pictures adopted in the LUND String Fragmentation Model (LSFM),Webber Cluster Fragmentation Model (WCFM) and Quark Combination Model (QCM),respectively.Predictions of hadron multiplicity,baryon to meson ratios and baryon-antibaryon flavor correlations,especially those related to heavy hadrons at a Z 0 factory obtained by LSFM and QCM,are reported. 展开更多
关键词 Z0 FACTORY HADRONIZATION model BARYON to MESON RATIO B CORRELATION
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Direct CP violation in hadronic B decays
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作者 HONG Bihai1,2 & Lü Caidian3 1. Department of Physics, Lishui University, Lishui 323000,China 2. Department of Physics, Shanghai Jiaotong University, Shanghai 200030, China 3. Institute of High Energy Physics, Beijing 100049,China 《Science China(Physics,Mechanics & Astronomy)》 SCIE EI CAS 2006年第3期357-366,共10页
There are different approaches for the hadronic B decay calculations, recently. In this paper, we upgrade three of them, namely factorization, QCD factorization and the perturbative QCD approach based on kT factorizat... There are different approaches for the hadronic B decay calculations, recently. In this paper, we upgrade three of them, namely factorization, QCD factorization and the perturbative QCD approach based on kT factorization, using new parameters and full wave functions. Although they get similar results for many of the branching ratios, the direct CP asymmetries predicted by them are different, which can be tested by recent experimental measurements of B factories. 展开更多
关键词 CP violation hadronic B decay factorization.
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b→cτ■ decay in supersymmetry with R-parity violation
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作者 Dong-Yang Wang Ya-Dong Yang Xing-Bo Yuan 《Chinese Physics C》 SCIE CAS CSCD 2019年第8期46-58,共13页
In past years,several hints of lepton flavor universality(LFU)violation have emerged from the b→ct■,and b→sl+l-data.More recently,the Belle Collaboration has reported the first measurement of the D* longitudinal ... In past years,several hints of lepton flavor universality(LFU)violation have emerged from the b→ct■,and b→sl+l-data.More recently,the Belle Collaboration has reported the first measurement of the D* longitudinal polarization fraction in the B→D*τV decay.Motivated by this intriguing result,along with the recent measurements of RJ/Ψand τ polarization,we present the study of b→ct■ decays in supersymmetry(SUSY)with R-parity violation(RPV).We consider B→D(*)t■,Bc→ηct■,Bc→J/ψt■ and ∧b→∧ct■ modes and focus on the branching ratios,LFU ratios,forward-backward asymmetries,polarizations of daughter hadrons,and the τ lepton.The RPV SUSY was capable of explaining the RD(*) anomalies at the 2σ level,after taking into account various flavor constraints.In the allowed parameter space,the differential branching fractions and LFU ratios are largely enhanced by the SUSY effects,especially in the large dilepton invariant mass region.Moreover,a lower bound B(B+→K+vv)>7.37×10-6 is obtained.These observables could provide testable signatures at the high-luminosity LHC and SuperKEKB,and correlate with direct searches for SUSY. 展开更多
关键词 SUPERSYMMETRY R-PARITY VIOLATION heavy FLAVOR HADRON b-quark semi-leptonic DECAY
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中性B介子衰变中时间依赖CP破坏的实验研究进展
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作者 谢跃红 张黎明 《科学通报》 EI CAS 2024年第31期4577-4589,共13页
电荷共轭-宇称联合变换对称性的破坏简称CP破坏.中性B介子系统具有正反粒子振荡和CP破坏随时间变化等独特性质,提供了探索CP破坏机制的理想窗口.B介子工厂发现了B^(0)介子衰变的CP破坏,对粒子物理标准模型中Cabibbo-Kobayashi-Maskawa(C... 电荷共轭-宇称联合变换对称性的破坏简称CP破坏.中性B介子系统具有正反粒子振荡和CP破坏随时间变化等独特性质,提供了探索CP破坏机制的理想窗口.B介子工厂发现了B^(0)介子衰变的CP破坏,对粒子物理标准模型中Cabibbo-Kobayashi-Maskawa(CKM)夸克混合机制的确立发挥了关键作用.大型强子对撞机底夸克(Large Hadron Collider beauty,LHCb)实验在深入研究B^(0)介子CP破坏的同时,开展了B_(s)^(0)介子振荡和CP破坏的开拓性研究,显著提升了B^(0)介子混合相角2β、B_(s)^(0)介子混合相角φ_(s)与振荡参数Δm_(s)、CKM相角γ的测量精度,发现了B_(s)^(0)→K^(+)K^(-)衰变中存在显著的CP破坏.这些研究成果极大地丰富了我们对夸克味道改变和CP破坏现象的认知,对精确检验标准模型、寻找超出标准模型的新物理现象具有重要意义.本文在回顾中性B介子CP破坏研究历程的基础上,简要介绍时间依赖CP破坏的测量方法与要素,重点总结十多年来LHCb实验在中性B介子CP破坏研究方面取得的阶段性成果和重要进展,展望LHCb探测器升级为本研究领域带来的新机遇. 展开更多
关键词 CP破坏 中性B介子 CKM矩阵 标准模型 LHCb实验 大型强子对撞机
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