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1.
在对于质子上的π~+光生过程作了一般考虑以后,我们从Mandelstam表示出发,进而采用Cini-Fubini近似,导出了关于π光生幅的同位标部分的公式。按照核子电磁结构的新数据,我们选取π-π作用的I=J=l共振的参数为t_r=22,α_v=1.52,b_v=1.60,计算了dσ/dΩ(90°),dσ_‖/dσ_⊥(90°)以及三个能量下的角分布。结果表明,在加入π-π作用之后,与实验之间的调合比之Chew等的结果有很大的改进,所定出的γ+π→π+π的耦合常数约为∧≈-2.8e,这与时行的结果大致相符。 相似文献
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3.
M.N.Achasov K.I.Beloborodov A.V.Berdyugin A.A.Botov V.B.Golubev T.V.Dimova V.P.Druzhinin L.V.Kardapoltsev A.G.Kharlamov D.P.Kovrizhin I.A.Koop A.A.Korol S.V.Koshuba A.E.Obrazovsky E.V.Pakhtusova D.A.Shtol S.I.Serednyakov Z.K.Silagadze A.N.Skrinsky Yu.A.Tikhonov Yu.M.Shatunov A.V.Vasil'ev 《中国物理C(英文版)》2010,34(6)
In an experiment with the Spherical Neutral Detector at VEPP-2M collider the cross section of the process e+e-→π+π-π0π0 was measured. At energies √s < 920 MeV this cross section was measured for the first time. The energy dependence of the cross section is well discribed by the vector dominance
model with contributions from ρ, ρ' ρ", mesons. The decay probability ρ→π+π-π0π0was found to be Bρ = (1.60±0.74±0.18)×10-5. The upper limit for the decay ω→π+π-π0π0 was improved by two orders of magnitude compared to the previous measurements and is Bω < 2 × 10-4 at 90% confidence level. 相似文献
4.
The cross sections of e+e-→π+π-hc at center-of-mass energies from 3.90 to 4.42 GeV were measured by the BES and the CLEO-c experiments. Resonant structures are evident in the e+e-→π+π-hc line shape. The fit to the line shape results in a narrow structure at a mass of(4216±18) MeV/c2and a width of(39±32) MeV, and a possible wide structure of mass(4293±9) MeV/c2and width(222±67) MeV. Here, the errors are combined statistical and systematic errors. This may indicate that the Y(4260) state observed in e+e-→π+π-J/ψ has a fine structure in it. 相似文献
5.
本文建议作π+p→Λ+π+K反应的实验,其中质心系总能量固定为1900MeV。在末态K介子动能0—90MeV的变化范围内,观察末态Λ-π共振和在∑πk道产生阈附近的近阈效应。通过共振-近阈效应关联和共振的角分布可以确定Y1*的自旋和Y1*,和∑之间的相对宇称。按照先处理T短阵的么正性,后处理解析性的思想,本文引入了T矩阵在道空间上的对角表象。在此基础上,提出了唯象描述近阈效应、共振现象和末态相互作用,特别是近阈效应和在阈附近共振的关联的一个新方法。并且应用这个方法,处理了所建议实验中的末态共振-近阈效应关联。
关键词: 相似文献
6.
F. Nguyen F. Piccinini A.D. Polosa 《The European Physical Journal C - Particles and Fields》2006,47(1):65-70
The production of the σ(500) meson in γγ→π0π0 is studied. In particular, the KLOE data collected during the DAΦNE run at
are appropriate to this purpose because of the strong reduction of kaon backgrounds.
PACS 12.39.-x 相似文献
7.
V. F. Müller 《Zeitschrift für Physik A Hadrons and Nuclei》1963,172(2):224-230
The radiative decay of the chargedπ-mesonπ→e+ν+γ is calculated using dispersion relation techniques. It is assumed that the weak interaction producing the decay has a V-A structure. The decay through the vector variant has been reinvestigated and found to be different from the result ofVaks andIoffe. The theoretical prediction of this paper is in agreement with a preliminary experiment recently performed at CERN. 相似文献
8.
在对于质子上的π+光生过程作了一般考虑以后,我们从Mandelstam表示出发,进而采用Cini-Fubini近似,导出了关于π光生幅的同位标部分的公式。按照核子电磁结构的新数据,我们选取π-π作用的I=J=l共振的参数为tr=22,αv=1.52,bv=1.60,计算了(dσ)/(dΩ)(90°),(dσ‖)/(dσ⊥)(90°)以及三个能量下的角分布。结果表明,在加入π-π作用之后,与实验之间的调合比之Chew等的结果有很大的改进,所定出的γ+π→π+π的耦合常数约为∧≈-2.8e,这与时行的结果大致相符。 相似文献
9.
《中国物理C(英文版)》2021,(5)
Within the quasi-two-body decay model,we study the localized CP violation and branching fraction of the four-body decay B~0→[K~-π~+]_(s/V)[π~+π~-]_(V/)S→K-π~+π~-π~+ when the K~-π~+and π~-π~+ pair invariant masses are0.35 m(K~-π~+)2.04 GeV and 0 mπ~-π~+1.06 GeV,with the pairs being dominated by the K_0~*(700)~0,K~*(892)~0,K~*(1410)~0,K_0~*(1430) and K~*(1680)~0,and fo(500),ρ~0(770),ω(782) and fo(980) resonances,respectively.When dealing with the dynamical functions of these resonances,fo(500),ρ~0(770),fo(980) and K_0~*(1430) are modeled with the Bugg model,Gounaris-Sakurai function,Flatte formalism and LASS lineshape,respectively,while the others are described by the relativistic Breit-Wigner function.Adopting the end point divergence parameters ρA ∈[0,0.5] andΦ_A∈[0,2π],our predicted results are F_(CP)(B~0→K~-π~+π~+π~-)∈[-0.365,0.447] and B(B~0→K-π~+π~+π~-)∈[6.11,185.32] x 10~(-8),based on the hypothetical qq structures for the scalar mesons in the QCD factorization approach.Meanwhile,we calculate the CP violating asymmetries and branching fractions of the two-body decays B~0→SV(VS) and all the individual four-body decays B~0→SV(VS)→K~-π~+π~-π~+,respectively.Our theoretical results for the two-body decays B~0→K~*(892)~0 fo(980),B~0→K_0~*(1430)~0ω(782),B~0→K~*(892)~0 f~0(980),B~0→K_0~*(1430)~0ρ,and B~0→(1430)~0ω are consistent with the available experimental data,with the remaining predictions await testing in future high precision experiments. 相似文献
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11.
PING Rong-Gang LI Gang WANG Zheng 《理论物理通讯》2007,47(1):89-94
The formalisms of helicity coupling amplitudes for J/ψ→π^+π^-π^0 are presented. A detailed discussion is also given on the barrier factor, Breit Wigner, and density matrix. A Monte Carlo simulation of J/ψ→ρ(770)π→π^+π^-π^0 is carried out. The results show that the p(770) resonance is well reproduced compared with experimental data. 相似文献
12.
Within an effective Lagrangian approach and resonance model, we study the γp→a_1(1260)~+n andγp→π~+π~+π~-n reactions via the π-exchange mechanism. For the γp→π~+π~+π~-n reaction, we perform a calculation of the differential and total cross-sections by considering the contributions of the a1(1260) intermediate resonance decaying into per and then into π~+π~+π~-. Besides,the non-resonance process is also considered. With a lower mass of a1(1260), the experimental data for the invariant π~+π~+π~-mass distributions can be fairly well reproduced. For theγp→a_1(1260)~+n reaction, with the model parameters, the total cross-section is of the order of 10 μb at the photon beam energy Eγ~2.5 GeV. It is expected that the model calculations in this work could be tested by future experiments. 相似文献
13.
PHOTOS Monte Carlo is widely used for simulating QED effects in decay of intermediate particles and resonances.It can be easily connected to other main process generators.In this paper we consider decaying processes γ*→π+π-(γ)and K±→π+π-e±ν(γ)in the framework of Scalar QED.These two processes are interesting not only for the technical aspect of PHOTOS Monte Carlo,but also for precision measurement ofαQED(Mz),g-2,as well as ππ scattering lengths. 相似文献
14.
Abouzaid E Arenton M Barker AR Bellantoni L Blucher E Bock GJ Cheu E Coleman R Corcoran MD Cox B Erwin AR Escobar CO Glazov A Golossanov A Gomes RA Gouffon P Hsiung YB Jensen DA Kessler R Kotera K Ledovskoy A McBride PL Monnier E Nguyen H Niclasen R Phillips DG Ping H Ramberg EJ Ray RE Ronquest M Santos E Slater W Smith D Solomey N Swallow EC Toale PA Tschirhart R Velissaris C Wah YW Wang J White HB Whitmore J Wilking MJ Winston R Worcester ET Worcester M Yamanaka T Zimmerman ED 《Physical review letters》2011,107(20):201803
The KTeV E799 experiment has conducted a search for the rare decays, K(L)→π(0)π(0)μ(+)μ(-) and K(L)→π(0)π(0)X(0)→π(0)π(0)μ(+)μ(-), where the X(0) is a possible new neutral boson that was reported by the HyperCP experiment with a mass of (214.3 ± 0.5) MeV/c(2). We find no evidence for either decay. We obtain upper limits of Br(K(L)→π(0)π(0)X(0)→π(0)π(0)μ(+)μ(-)) < 1.0 × 10(-10) and Br(K(L)→π(0)π(0)μ(+)μ(-)) < 9.2 × 10(-11) at the 90% confidence level. This result rules out the pseudoscalar X(0) as an explanation of the HyperCP result under the scenario that the dsX(0) coupling is completely real. 相似文献
15.
M. Barth A. E. De Wolf D. P. Johnson P. Theocharopoulos H. Drevermann Y. Goldschmidt-Clermont J. P. Porte R. T. Ross S. Squarcia C. Caso R. Contri F. Fontanelli R. Monge U. Trevisan J. F. Baland J. Beaufays J. Hanton F. Grard P. A. van der Poel L. Gatignon D. J. Schotanus A. Stergiou R. T. Van de Walle V. V. Brizgalov P. V. Chliapnikov A. B. Fenyuk I. A. Gritsaenko O. V. Kasian V. M. Kubic S. B. Lugovsky V. I. Nikolaenko Y. L. Petrovykh V. M. Ronjin V. A. Yarba 《Zeitschrift fur Physik C Particles and Fields》1982,16(2):111-117
Results are presented onK + p elastic scattering and on the reactionK + p→K + pπ+π? at 70 GeV/c. For the elastic channel, we measured the total ((2.29±0.04)mb) and differentialdσ/dt cross sections. The reactionK + p→K + pπ+π? has a total cross section of (470±23) μb and is shown to be dominated by diffractive dissociation processes. The contributions of the quasi-two-body channels $$K^ + p \to K*^0 (890)\Delta ^{ + + } (1,236)$$ and $$K^ + p \to K*^0 (1,430)\Delta ^{ + + } (1,236)$$ and of the Double-Pomeron Exchange (DPE) processes are estimated. 相似文献
16.
利用北京谱仪(BES)在4.03GeV正负电子对撞能量下获取的数据,[研究了,τ+τ-产生过程.借助双标记方法分析了τ±→π+π-π±υτ衰变事例.测定分支比Br(τ±→a1±υτ→ρ0π±υτ,ρ0→π+π-=(7.3±0.5)%,Br(τ±→K*±υτ→Ks0π±υτ,Ks0→π+π-)=(0.6±1.5)×10-3.并由Daliz投影分布的分析,确认a1的主要衰变方式ρπ.同时,也观察到a1衰变中以S波贡献为主的现象.采用Kuhn模型拟合实验数据,得到:ma1=1.24±0.02GeV,Γa1T=0.57±0.07GeV. 相似文献
17.
用BESⅠ的 7.8× 1 0 6 J/ ψ数据更为精确地测定了J/ ψ→π0 3 (π+π- )和J/ ψ→ω2 (π+π- )的分支比 (Br(J/ ψ→π0 3 (π+π- ) ) =( 2 .52± 0 .0 6± 0 .4 3 ) % ,Br(J/ ψ→ω2 (π+π- ) ) =( 1 .3 1± 0 .0 9± 0 .2 1 ) % .同时对 4π不变质量谱和ωππ不变质量谱进行研究分析 ,试图观察是否存在有兴趣的信号 . 相似文献
18.
M. N. Achasov K. I. Beloborodov A. V. Berdyugin A. G. Bogdanchikov A. V. Bozhenok A. D. Bukin D. A. Bukin S. V. Burdin A. V. Vasil’ev D. I. Ganyushin V. B. Golubev T. V. Dimova A. A. Drozdetskii V. P. Druzhinin P. M. Ivanov V. N. Ivanchenko A. A. Korol’ M. S. Korostelev S. V. Koshuba G. A. Kukartsev E. V. Pakhtusova A. A. Polunin E. É. Pyata A. A. Sal’nikov S. I. Serednyakov V. A. Sidorov Z. K. Silagadze V. V. Sharyi Yu. M. Shatunov 《JETP Letters》2000,71(9):355-358
The e + e ?→π0π0 γreaction was studied in the energy range 0.36–0.97 GeV on a VEPP-2M e + e ? collider with an SND detector. The decay probabilities were found to be B(ω→ π0π0γ)= (7.8 ±2.7±2.0)×10?5 and B(π→ π0π0γ)= (4.8 ?1.8 +3.4 ±0.2)×10?5. 相似文献
19.
Giancarlo D'Ambrosio Mario Miragliuolo Francesco Sannino 《Zeitschrift fur Physik C Particles and Fields》1993,59(3):451-456
We discuss the decayK
s
+– in the framework of chiral perturbation theory. The direct emission in this decay can be an useful test of meson dynamics. 相似文献