共查询到20条相似文献,搜索用时 15 毫秒
1.
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
2.
S. Rai Choudhury A. S. Cornell Naveen Gaur 《The European Physical Journal C - Particles and Fields》2008,58(2):251-259
Flavor changing neutral current (FCNC) decays of the B-meson are a very useful tool for studying possible physics scenarios beyond the standard model (SM), where of the many FCNC
modes radiative, purely leptonic and semi-leptonic decays of the B-meson are relatively clean tests. Within this context, the BELLE collaboration has measured the process B→K
*
γ and also searched for the B→K
1(1270)γ process. Theoretical analyses of these processes are yielding similar values of the relevant form factors. In this work we
have used this upper bound in studying the angular correlations for the related semi-leptonic decay mode B
−→K
1−(1270)(→ρ
0
K
−)ℓ
+
ℓ
−, where we have used the form factors that have already been estimated for the B→K
1(1270)γ mode. Note that the additional form factors that are required were calculated using large energy effective theory (LEET). 相似文献
3.
V. A. Kovalchuk 《Physics of Atomic Nuclei》2007,70(4):722-731
A method for determining the angle γ and the ratio of the amplitudes A
λ(B
− →
K
*−) and A
λ)B
− → D
*0
K
*−), r
Bλ, for all three vector-meson polarization states by using the decays B
∓ → D
*
K
*∓ is proposed. This method relies on the interference between the decays B
− → D
*0
K
*− and B
− →
K
*−, which arises if D
*0 and
decay to D
0/
π
0 and D
0/
γ, whereupon D
0 and
mesons decay to common final hadron states. The doubly Cabibbo-suppressed modes of D
0-meson decay are chosen here to specify such final states.
Original Russian Text ? V.A. Kovalchuk, 2007, published in Yadernaya Fizika, 2007, Vol. 70, No. 4, pp. 754–763. 相似文献
4.
DELPHI Collaboration W. Adam T. Adye E. Agasi I. Ajinenko R. Aleksan G. D. Alekseev P. P. Allport S. Almehed S. J. Alvsvaag et al. 《Zeitschrift fur Physik C Particles and Fields》1995,69(1):561-573
An analysis is presented of inclusiveπ
0 production inZ
0 decays measured with the DELPHI detector. At low energies,π
0 decays are reconstructed by using pairs of converted photons and combinations of converted photons and photons reconstructed
in the barrel electromagnetic calorimeter (HPC). At high energies (up to
) the excellent granularity of the HPC is exploited to search for two-photon substructures in single showers. The inclusive
differential cross section is measured as a function of energy forqq andbb events. The number ofπ
0’s per hadronicZ
0 event isN(π
0)/Z
had
0
=9.2±0.2(stat)±1.0(syst) and forbb events the number ofπ
0’s is N(π
0)/bb=10.1±0.4(stat)±1.1(syst). The ratio of the number ofπ
0’s inbb events to hadronicZ
0 events is less affected by the systematic errors and is found to be 1.09±0.05±0.01. The measuredπ
0 cross sections are compared with the predictions of different parton shower models. For hadronic events, the peak position
in theξ
p=ln(1/xp) distribution isξ*
p
=3.90
−0.14
+0.24
. The average number ofπ
0’s from the decay of primary B hadrons is found to be N(B→π
0
X)/B hadron=2.78±0.15(stat)±0.60(syst). 相似文献
5.
Using the technique of helicity amplitudes, the electromagnetic process e
+
e
− → μ+μ− is theoretically investigated in the one-photon approximation. The structure of the triplet states of the final (μ+μ−) system is analyzed. It is shown that in the case of unpolarized electron and positron the finalmuons are also unpolarized,
but their spins are strongly correlated. Explicit expressions for the components of the correlation tensor of the final (μ+μ−) system are derived. The formula for the angular correlation at the decays of final muons μ+ and μ−, produced in the process e
+
e
− → μ+μ−, is obtained. It is demonstrated that spin correlations of muons in the process of electron-positron pair annihilation have
the purely quantum character, since one of the incoherence inequalities for the correlation-tensor components is always violated.
The additional contribution of the weak interaction of lepton neutral currents through the virtual Z
0 boson is considered; it is established that, taking into account the weak interaction, the qualitative character of the muon
spin correlations does not change.
The text was submitted by the authors in English. 相似文献
6.
J. Ryckebusch W. Van Nespen 《The European Physical Journal A - Hadrons and Nuclei》2004,20(3):435-441
Differential cross-sections for exclusive 16O(e,epp)14C processes are computed within a distorted-wave framework which includes central short-range correlations and intermediate
excitations. The cross-sections are compared to high-resolution data from the MAMI facility at Mainz for a central energy and momentum transfer of
MeV and
MeV, respectively. A fair agreement between the numerical calculations and data is reached when using spectroscopic information extracted from a 15N
C experiment. The comparison between the calculations and the data provides additional evidence that short-range correlations exclusively affect nucleon pairs with a small center-of-mass momentum residing in a relative S state.Received: 3 September 2003, Revised: 2 December 2003, Published online: 18 June 2004PACS:
24.10.-i Nuclear-reaction models and methods - 21.60.-n Nuclear-structure models and methods - 25.30.Fj Inelastic electron scattering to continuum 相似文献
7.
Yu-Ming Wang M. Jamil Aslam Cai-Dian Lü 《The European Physical Journal C - Particles and Fields》2009,59(4):847-860
The exclusive weak decay of Λ
b
→Λ
γ and Λ
b
→Λ
l
+
l
− are investigated in the Appelquist–Cheng–Dobrescu model, which is an extension of the standard model in the presence of universal
extra dimensions. Employing the transition form factors obtained in the light-cone sum rules, we analyze how the invariant-mass
distribution, the forward–backward asymmetry and the polarization asymmetry of the Λ baryon of these decay modes can be used to constrain the only additional free parameter with respect to the standard model,
namely, the radius, R, of the extra dimension. Our results indicate that the Kaluza–Klein modes can lead to approximately 25% suppression of the
branching ratio of Λ
b
→Λ
γ; however, their contributions can bring about 10% enhancement to the decay rate of Λ
b
→Λ
l
+
l
−. It is shown that in the present scenario the zero position of the forward–backward asymmetry of Λ
b
→Λ
μ
+
μ
− is sensitive to the compactification parameter R, while the measurement of polarizations of Λ baryon in the Λ
b
decays are not a useful tool to provide any valuable information for the universal extra-dimension model. 相似文献
8.
9.
The polarization of a bremsstrahlung photon during the processes ee
± → (eγ)e
± and ep → (eγ)p is calculated for peripheral kinematics in the high-energy limit, where the cross section does not decrease with the incident
energy. When the initial electron is unpolarized (longitudinally polarized), the final photon can be linearly (circularly)
polarized. The Stokes parameters of the photon polarization are calculated as a function of the kinematical variables of the
process: the energy of the recoil particle, the energy fraction of the scattered electron, and the polar and azimuthal angles
of the photon. The numerical results are given in the form of tables for typical values of the relevant kinematic variables.
The text was submitted by the authors in English. 相似文献
10.
The signs of the experimental values of the multipole-mixture parameters δ are compared with the signs of ℛ = Σa
i
μ
i
for (2+02−2+01) and (2+03−2+01) transitions and with the signs of = Σa
i
[(μ
i
+ μ
kν
) or (μ
kπ
− 1/2)] for (2+21−2+01) transitions in nonspherical even-even nuclei, where a
i
is the contribution of the ith pair of quasiparticles to the wave function for 2+02, 2+03, and 2+21 single-phonon states according to the quasiparticle-phonon model and μ is the magnetic moment for the corresponding Nilsson
state.
Original Russian Text ? A.M. Demidov, L.I. Govor, V.A. Kurkin, I.V. Mikhailov, 2009, published in Yadernaya Fizika, 2009,
Vol. 72, No. 2, pp. 228–235. 相似文献
11.
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
12.
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
13.
Yu. M. Andreev S. I. Bityukov N. V. Krasnikov A. N. Toropin 《Physics of Atomic Nuclei》2007,70(10):1717-1724
The LHC (CMS) discovery potential in the search for supersymmetry and lepton-flavor violation in neutralino decays using the
e
± μ∓ + E
T
miss
signature is studied. A detailed study is done for the CMS test points LM1-LM9. It is shown that, for the point LM1, it is
possible to detect lepton-flavor violation in neutralino decays with lepton-flavor-violating branching Br(
→ μ±
e
∓
) ≥ 0.04 Br(
→ e
+
e
−
, μ+ μ−
) for an integral luminosity of 10 fb−1. The discovery potential in the mSUGRA-SUSY scenario with tan β = 10, sgn(μ) = + in the (m
0, m
1/2) plane using the e
± μ∓ + E
T
miss
signature is determined.
The text was submitted by the authors in English. 相似文献
14.
The difference of the energies of levels Δ
n
= E
lev(2+0
n
) − E
lev(0+0
n
) at n = 1, 2, and 3 and the multipole-mixture parameter δ for (2+02−2+01) and (2+03−2+01) transitions are contrasted against the structure of the K
π
= 02+ and 03+ rotational bands that was calculated on the basis of the quasiparticle-phonon model. The values of (Δ2 − Δ1), (Δ3 − Δ1), and (Δ2 − Δ3) are found to correlate with the sign of the parameter δ and with the calculated structure of the K
π
= 02+ and 03+ bands.
Original Russian Text ? A.M. Demidov, L.I. Govor, V.A. Kurkin, I.V. Mikhailov, 2009, published in Yadernaya Fizika, 2009,
Vol. 72, No. 2, pp. 236–240. 相似文献
15.
16.
P.F. Bernath R.W. Field B. Pinchemel Y. Lefebvre J. Schamps 《Journal of Molecular Spectroscopy》1981,88(1):175-193
Laser excitation spectra have been recorded for Ca79Br and Ca81Br in the spectral region 600–630 nm. The use of a 1-m monochromator as a narrow band pass filter (1–2 cm?1) has allowed rotational analysis of the 0-0, 1-1, and 2-2 bands of the B2Σ+ - X2Σ+ transition and the 0-0 and 1-1 bands of the A2Π - X2Σ+ transition. A few additional lines of the 0-1, 1-2, 1-0, and 2-1 bands of the B-X system were used to obtain band origins for vibrational analysis. The main constants for Ca79Br are (in cm?1):
0 | 15 958.41 (10) | 16 383.137 (6) | |
285.732 (9) | 288.56 (20) | 285.747 (9) | |
0.840 (4) | — | 0.954 (4) | |
0.094466141 (30) | 0.0957343 (20) | 0.0965151 (20) | |
0.000403551 (40) | 0.0004327 (20) | 0.0004483 (15) | |
(spin-rot.) | 0.00301484 (50) | — | 0.068767 (79) |
— | ?0.066834 (64) | — | |
— | 59.175 (1) | — |