共查询到20条相似文献,搜索用时 31 毫秒
1.
The decays η → 3π
0 and η → π
0
π
+
π
− are considered within the isobar model. It is shown that, in order to explain the branching ratio and the shape of the Dalitz
plot for the decay η′ → 3π
0, it is sufficient to take into account the contributions of the σ and a
0 mesons. The inclusion of the σ meson is necessary for reproducing the shape of the distribution over the Dalitz plot. The branching ratio for the decay
η′ → π
0
π
+
π
− is obtained. The predictions for the distributions over the Dalitz plot for this decay are presented. These predictions depend
strongly on model parameters. 相似文献
2.
The branching ratios and photon spectra of the rare processes ρ(ω) → π
0
π
0
γ, ρ(ω) → ηπ
0
γ are calculated in the framework of the standard local quark Nambu-Jona-Lasinio model. Three types of diagrams are considered:
the quark box and the pole diagrams with scalar (σ, α
0(980)) and vector (ρ, ω) mesons. The obtained estimates for the widths of the processes ρ(ω) → π
0
π
0
γ are in satisfactory agreement with existing experimental data. Predictions are made for the widths of the processes ρ(ω) → ηπ
0
γ.
The text was submitted by the authors in English. 相似文献
3.
BaBar’s observation of significant deviations of the pion transition form factor (TFF) from the asymptotic expectation with
Q
2>9 GeV2 has brought about a serious crisis to the fundamental picture established for such a simple q[`(q)]q\bar{q} system by perturbative QCD, i.e. the dominance of collinear factorization at high momentum transfers for the pion TFF. We
show that non-factorizable contributions due to open flavors in γγ
∗→π
0 could be an important source that contaminates the pQCD asymptotic limit and causes such deviations with Q
2>9 GeV2. Within an effective Lagrangian approach, the non-factorizable amplitudes can be related to intermediate hadron loops, i.e.
K
(∗) and D
(∗) etc., and their corrections to the π
0 and η TFFs can be estimated. 相似文献
4.
The results of recent experiments performed at KEK, Brookhaven National Laboratory, the Institute for High-Energy Physics
(Protvino), and CERN to study the reaction π
−
p → π
0
π
0
n are analyzed in detail. For S-wave pion-pion scattering in the channel of isospin I=0, new data are obtained for the phase shift δ
0
0
and the inelasticity parameter η
0
0
. Difficulties that arise in using, for the amplitudes of the S and D waves of the final π
0
π
0 system, physical solutions selected on the basis of partial-wave analyses are discussed. It is noteworthy that other solutions
are preferable in principle in the region of the invariant mass m of the π
0
π
0 system above 1 GeV. With the aim of clarifying the situation and further studying the properties of the f
0(980) resonance, it is proposed to perform, in the reaction π
−
p → π
0
π
0
n, an especially careful examination of the m region in the vicinity of the
threshold.
__________
Translated from Yadernaya Fizika, Vol. 67, No. 7, 2004, pp. 1380–1391.
Original Russian Text Copyright ? 2004 by Achasov, Shestakov. 相似文献
5.
Murugesh Duraisamy Alexander L. Kagan 《The European Physical Journal C - Particles and Fields》2010,70(4):921-925
CLEO-c measurements of the timelike form factors F
π
, F
K
at ?s=3.671\sqrt{s}=3.671 GeV provide a direct probe of power corrections (PC’s) at energies near m
B
. PC’s in F
π,K
and B→Kπ,ππ are separated into perturbative and soft parts. In F
π,K
the latter are ≥O(10) larger. A PC fit to the B→Kπ,ππ data also yields a ≥O(10) soft-to-perturbative hierarchy for the QCD penguin PC’s. Hence, both can be attributed to dominance of the soft-overlap
between energetic (approximately) back-to-back collinear partons, and consistency of the B→Kπ,ππ fit with the Standard Model appears to be naturally realized. The CP asymmetries SKs p0S_{K_{s} \pi^{0}}, CKs p0C_{K_{s} \pi^{0}} are well determined, providing a clean test for new physics. 相似文献
6.
7.
Swapan Das 《Pramana》2010,75(4):665-674
The cross-section for the π
+
π
−
π
0 invariant mass distribution in the γp reaction in the GeV region is calculated. This reaction is assumed to proceed through the formation of the ω-meson in the intermediate state, because the production cross-section for this meson in the γp reaction in the GeV region is significant and it has a large branching ratio (88.8%) in the π
+
π
−
π
0 channel. The cross-sections for this reaction are calculated using the energy-dependent reaction amplitude, f
γp→ωp(0), extracted from the latest ω-meson photoproduction data. We use established procedure to calculate other factors, like width and propagator of the ω-meson, so that our calculation can provide reliable cross-section. The calculated results reproduce the measured π
+
π
−
π
0 invariant mass distribution spectra in the γp reaction. 相似文献
8.
In this article, we study the decays ψ′ → J/ψπ
+
π
− and η′c → η
c
π
+
π
− by taking into account the chiral symmetry breaking effects, the final-state interactions and the heavy-quark symmetry. We
can confront the predictions of the η′c → η
c
π
+
π
− decay width and differential decay width with the experimental data in the future, and obtain powerful constraints on the
chiral breaking effects and the final-state interactions, and test the heavy-quark symmetry. 相似文献
9.
Radiative decays π
0(π
0′) → γ + γ, π
0′ → ρ
0(ω) + γ, ρ
0′(ω′) → π
0 + γ, ρ
0′(ω′) → π
0′ + γ, and some processes of π
0′ production at lepton colliders are considered in the framework of the nonlocal SU(2) × SU(2) Nambu-Jona-Lasinio model. Mixing of the radially excited and the ground meson states is taken into account. Numerical
results for the decay and production processes are presented. 相似文献
10.
L. Cappiello O. Catà G. D’Ambrosio Dao-Neng Gao 《The European Physical Journal C - Particles and Fields》2012,72(1):1872
We study the decay K
+→π
+
π
0
e
+
e
−, currently under analysis by the NA62 Collaboration at CERN. In particular, we provide a detailed analysis of the Dalitz
plot for the long-distance, γ
∗-mediated, contributions (Bremsstrahlung, direct emission and its interference). We also examine a set of asymmetries to isolate
genuine short-distance effects. While we show that charge asymmetries are not required to test short distances, they provide
the best environment for its detection. This constitutes by itself a strong motivation for NA62 to study K
− decays in the future. We therefore provide a detailed study of different charge asymmetries and the corresponding estimated
signals. Whenever possible, we make contact with the related processes K
+→π
+
π
0
γ and K
L
→π
+
π
−
e
+
e
− and discuss the advantages of K
+→π
+
π
0
e
+
e
− over them. 相似文献
11.
Dian-Yong Chen Xiang Liu Xue-Qian Li 《The European Physical Journal C - Particles and Fields》2011,71(11):1808
To solve the discrepancy between the experimental data on the partial widths and lineshapes of the dipion emission of ϒ(4S) and the theoretical predictions, we suggest that there is an additional contribution, which had not been taken into account
in previous calculations. Noticing that the mass of ϒ(4S) is above the production threshold of B[`(B)]B\bar{B}, the contribution of the sequential process
\varUpsilon(4S)? B[`(B)]? \varUpsilon(nS)+S?\varUpsilon(nS)+p+p-\varUpsilon(4S)\to B\bar{B}\to \varUpsilon(nS)+S\to\varUpsilon(nS)+\pi^{+}\pi^{-} (n=1,2) may be sizable, and its interference with that from the direct production would be important. The goal of this work
is to investigate if a sum of the two contributions with a relative phase indeed reproduces the data. Our numerical results
on the partial widths and the lineshapes
d\varGamma(\varUpsilon(4S)?\varUpsilon(2S,1S)p+p-)/d(mp+p-)d\varGamma(\varUpsilon(4S)\to\varUpsilon(2S,1S)\pi^{+}\pi^{-})/d(m_{\pi ^{+}\pi^{-}}) are satisfactorily consistent with the measurements; thus the role of this mechanism is confirmed. Moreover, with the parameters
obtained by fitting the data of the Belle and BaBar collaborations, we predict the distributions dΓ(ϒ(4S)→ϒ(2S,1S)π
+
π
−)/dcosθ, which have not been measured yet. 相似文献
12.
Jianhua Wang Kang Li Sayipjamal Dulat Yi Yuan Kai Ma 《International Journal of Theoretical Physics》2012,51(8):2639-2647
By studying the scattering process of scalar particle pion on the noncommutative scalar quantum electrodynamics, the non-commutative amendment of differential scattering cross-section is found, which is dependent of polar-angle and the results are significantly different from that in the commutative scalar quantum electrodynamics, particularly when cosθ∼±1. The non-commutativity of space is expected to be explored at around ΛNC∼TeV. 相似文献
13.
Susana Coito George Rupp Eef van Beveren 《The European Physical Journal C - Particles and Fields》2011,71(10):1762
The nature of the X(3872) enhancement is analyzed in the framework of the Resonance-Spectrum Expansion, by studying it as a regular J
PC
=1++ charmonium state, though strongly influenced and shifted by open-charm decay channels. The observed but Okubo–Zweig–Iizuka-forbidden
ρ
0
J/ψ and ωJ/ψ channels are coupled as well, but effectively smeared out by using complex ρ
0 and ω masses, in order to account for their physical widths, followed by a rigorous algebraic procedure to restore unitarity. A
very delicate interplay between the D
0
D
∗0, ρ
0
J/ψ, and ωJ/ψ channels is observed. The data clearly suggest that the X(3872) is a very narrow axial-vector c[`(c)]c\bar{c} resonance, with a pole at or slightly below the D
0
D
∗0 threshold. 相似文献
14.
The T-odd correlation
in the decays K
+ → π
0
l
+
νγ (l = e, μ) is investigated as a function of the parameters of the effective Lagrangian. It is shown that the T-odd correlation offers a good indicator of new physics in the vector and pseudovector sectors of the model under consideration.
In the scalar and pseudoscalar sectors, investigation of the T-odd correlation gives no way to improve the current limits on the parameters of various extensions of the Standard Model.
__________
Translated from Yadernaya Fizika, Vol. 67, No. 5, 2004, pp. 1025–1032.
Original Russian Text Copyright ? 2004 by Braguta, Likhoded, Chalov. 相似文献
15.
Zhi-Gang Wang 《The European Physical Journal C - Particles and Fields》2009,61(2):299-309
We calculate the strong coupling constant g among the decuplet baryons, the octet baryons and the pseudoscalar mesons in the heavy baryon chiral perturbation theory
with the light-cone QCD sum rules, and we study the strong decays Σ
*→Λ
π,Σ
π. The numerical value of the strong coupling constant g is consistent with our previous calculation; the central values lead to small SU(3) breaking effects, less than 6%; and no definitive conclusion can be drawn due to the large uncertainties. 相似文献
16.
Damir Be?irevi? Benjamin Haas 《The European Physical Journal C - Particles and Fields》2011,71(8):1734
The axial coupling and the magnetic moment of D
∗-meson or, more specifically, the couplings gD*Dpg_{D^{\ast}D\pi} and gD*Dgg_{D^{\ast}D\gamma }, encode the non-perturbative QCD effects describing the decays D
∗→Dπ and D
∗→Dγ. We compute these quantities by means of lattice QCD with N
f=2 dynamical quarks, by employing the Wilson (“clover”) action. On our finer lattice (a≈0.065 fm) we obtain gD*Dp+=20±2g_{D^{\ast}D\pi^{+}}=20\pm2, and gD*0 D0g=2.0±0.6 GeV-1g_{D^{\ast0} D^{0}\gamma}=2.0\pm 0.6~{\rm GeV}^{-1}. This is the first determination of gD*0 D0gg_{D^{\ast0} D^{0}\gamma} on the lattice. We also provide a short phenomenological discussion and the comparison of our result with experiment and
with the results quoted in the literature. 相似文献
17.
R. A. Ryutin V. A. Petrov A. E. Sobol 《The European Physical Journal C - Particles and Fields》2011,71(5):1667
We study the possibilities to analyse the data on leading neutrons production at first LHC runs. These data could be used
to extract from it π
+
p and π
+
π
+ cross-sections. In this note we estimate relative contributions of π, ρ and a
2 reggeons to charge exchanges and discuss related problems of measurements. 相似文献
18.
The e
+
e
− → π
+
π
−
π
+
π
− cross section is calculated for energies of 0.65 ≤ √s ≤ 1 GeV in the framework of the generalized hidden local symmetry model. The calculations are compared with the data of CMD-2
and BaBaR. It is shown that the inclusion of heavy isovector resonances ρ(1450) and ρ(1700) is necessary for reconciling calculations
with the data. It is found that, at √s ≈ 1 GeV, the contributions of the above resonances are much larger, by a factor of 30, than the ρ(770) one, and amount to
a considerable fraction ∼0.3–0.6 of the latter at √s ∼ m
ρ.
The text was submitted by the authors in English. 相似文献
19.
20.
Simulation study of χc→J/Ψ+γ detection with J/Ψ→e+e? in pp collisions in the ALICE experiment at LHC
P. González P. Ladrón de Guevara E. López Torres A. Marín E. Serradilla 《The European Physical Journal C - Particles and Fields》2009,61(4):915-903
We present Monte Carlo preliminary results about the feasibility to detect the χ
c
family in p-p collisions at 14 TeV in the ALICE Central Barrel at CERN LHC. The χ
c1 and χ
c2 were forced to decay in the radiative channel J/Ψ+γ→e
+
e
−+γ and were merged with a proton-proton non-biased collision. After Monte Carlo transport and simulation of the detector response,
the e
+, e
− and converted γ were reconstructed and identified in the ALICE ITS, TPC and TRD detectors. Separate signals corresponding to γ from χ
c1 and from χ
c2 were observed. The position and relative weight of the fit to gaussians agreed with the input values within the statistical
limits.
An erratum to this article can be found at 相似文献