共查询到20条相似文献,搜索用时 640 毫秒
1.
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
2.
E. P. Shabalin 《Physics of Atomic Nuclei》2010,73(11):1908-1915
The unitarization of the amplitude for the decay process K
10 → π+π− and allowance for the rescattering of final-state pions in the decay process K
+ → π+π+π− make it possible to evaluate, by using the parameters extracted from data on K → 2π decays, the K
+ → π+π+π− decay width. The result agrees with the experimental width value at a level of a few percent. Allowance for corrections for
higher order terms of the momentum expansion of the amplitude for the decay process K
+ → π+π+π− leads to the slope-parameter value of g
++−th = 0.2182, which agrees with its experimental counterpart, g
++−exp = 0.2154 ± 0.0035. 相似文献
3.
4.
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
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.
D. Buskulic D. Decamp C. Goy J. -P. Lees M. -N. Minard B. Mours B. Pietrzyk R. Alemany F. Ariztizabal P. Comas et al. 《Zeitschrift fur Physik C Particles and Fields》1993,59(2):215-229
Contact interactions are searched for using the differential cross sections for the reactionse
+
e
–e
+
e
–,e
+
e
–µ
+
µ
–,e
+
e
–
+
– ande
+
e
– measured at 12 energies around theZ peak and corresponding to about 20 pb–1 of cumulated luminosity. Four-fermion contact term models assuming various chiralities of lepton currents are fitted to the lepton data and lower limits on the energy scale of such terms are set at 95% c.l. The limits vary in the range 0.9–4.7 TeV, depending on the model and on the lepton flavour. Theee contact terms are searched for assuming various chiralities. Limits on the energy scale between 79 and 130 GeV are extracted from the data. The results are compared and combined with those reported at lower energies.Deceased 相似文献
7.
8.
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
9.
S. Senyukov 《The European Physical Journal C - Particles and Fields》2009,62(1):229-235
Heavy quarks, such as charm, are produced in hard scatterings in the early stages of high energy nucleus-nucleus collisions
and are expected to be a powerful tool to investigate the properties of the quark gluon plasma (QGP). The tracking detectors
of the ALICE apparatus will allow to track and identify particles in central rapidity range down to low P
t
. Among D mesons it would be particularly interesting to measure D
s
yield via an exclusive hadronic decay channel because it could help to disentangle different hadronization mechanisms. The
possibility of reconstructing the D
s
meson through its D
s
+→K
+
K
−
π
+ decay channel in the central barrel was studied. The problem considered is characterized by the comparatively low yield of
the D
s
mesons against the huge amount of combinatorial background. Different kinematic and topological cuts have been studied in
order to increase the signal-to-background ratio and the statistical significance. In addition, D
s
mesons preferentially decay through intermediate resonant states and this fact can improve the separation of signal from
background. Results of cut parameters tuning and values of significance for an analysis performed on simulated data are presented. 相似文献
10.
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
11.
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
12.
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
13.
H. -J. Behrend L. Criegee J. H. Field G. Franke H. Jung J. Meyer O. Podobrin V. Schr?der G. G. Winter P. J. Bussey et al. 《Zeitschrift fur Physik C Particles and Fields》1991,49(1):43-48
We have studied the 0 production rate in the reaction 3+3– in the energy range 1.6W
7.5 GeV with the CELLO detector at PETRA. Our analysis points to a substantial yield of 00+– events in particular atW
>4.0 GeV. We give cross sections for the 02+2– and 00+– final states and calculate upper limits for the reaction 00 (1700) 00+–.Now at CERN 相似文献
14.
R. Akers G. Alexander J. Allison K. J. Anderson S. Arcelli A. Astbury D. Axen G. Azuelos J. T. M. Baines A. H. Ball et al. 《Zeitschrift fur Physik C Particles and Fields》1994,61(2):199-208
We present measurements of the hadronic photon structure functionF
2
(x), in twoQ
2 ranges with mean values of 5.9 GeV2 and 14.7 GeV2. The data were taken by the OPAL experiment at LEP, with
close to theZ
0 mass and correspond to an integratede
+
e
– luminosity of 44.8 pb–1. In the context of a QCD-based model we find the quark transverse momentum cutoff separating the vector meson dominance (VMD) and perturbative QCD regions to be 0.27±0.10 GeV. We confirm that there is a significant pointlike component of the photon when the probe photon hasQ
2>4 GeV2. Our measurements extend to lower values ofx than any previous experiment, and no increase ofF
2
(x) is observed. 相似文献
15.
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
16.
对a2(1320)→π+π+π-过程的衰变振幅进行张量分析,展示了如何得到三体衰变振幅. 相似文献
17.
A model-independent analysis of anomalous gauge coupling constants of W
± bosons is presented and the corresponding restrictions on them and on the electromagnetic characteristics of W
± bosons following from the experiments on measuring the e+ e- ? W+ W- ? ( e