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1.
We analyze the inclusive semileptonic decays B→Xs l+l− in the framework of the supersymmetric standard model with non-universal soft-breaking terms at GUT scale. We show that the general trend of universal and non-universal models is a decreasing of branching ratio (BR) and increasing of energy asymmetry (AS). However, only non-universal models can have chances to get very large enhancements in BR and AS, corresponding to large (negative) SUSY contributions to the b→sγ amplitude. 相似文献
2.
We study the contribution of Bc mesons to the search for B → τντ decays. We find that at LEP the contributions from Bu and Bc mesons can be comparable. This observation can have a relevant impact on the extraction of constraints on new physics (such as charged-Higgs contributions) from current LEP limits on B → τν final states. Inclusion of the Bc contribution can reduce the current L3 limit on tan β/MH from 0.38 GeV−1 (90% CL) down to 0.27 GeV−1 (90% CL). 相似文献
3.
We compute non-perturbative contributions to B → Xsl+l− that are not explicitly suppressed by powers of the b-quark mass. They are proportional to
and arise from an interference between the free-quark amplitude and high order terms in the matrix element of the four-quark operator s−γμ(1 − γ5)cc−βγμ(1 − γ5)bβ. This correction is found to be small over most of the dalitz plot except near the charm threshold. Unfortunately, the perturbative computation we have performed is invalid near charm threshold and we do not except to see the structure found at lowest order reproduced in the data. We conclude that these non-perturbative contributions do not significantly modify the previous analysis of B → Xsl+l−. 相似文献
4.
We present the first complete series of polarized Raman spectra of orpiment crystals and the corresponding possible symmetry assignments of the phonon peaks within the layer model structure. We observe new peaks and a low frequency mode which could be a rigid layer vibration. We discuss briefly on the possible implications of some inconsistencies between the expected and the observed results. 相似文献
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6.
We report on the perturbative O(s) correction to the light-cone QCD sum rule for the B → π transition form factor f+. The correction to the product fBf+ in leading twist approximation is found to be about 30%, that is similar in magnitude to the corresponding O(s) correction in the two-point sum rule for fB. The resulting cancellation of large QCD corrections in f+ eliminates one important uncertainty in the sum-rule prediction for this form factor. 相似文献
7.
In the framework combining the heavy quark expansion and chiral symmetry for light quarks, we identify a class of corrections to the dominant vector meson pole diagram for B→π/v, in the vicinity of the zero pion recoil point. We also give a qualitative estimate of these effects, using higher states exchanges with couplings constrained by current algebra and PCAC. 相似文献
8.
The 333.6-, 351.1-, and 363.8-nm lines of a cw argon ion laser are found to coincide with the BaS B1Σ+-X1Σ+ (12, 0) R(17), (6, 0) P(35), and (3, 0) R(125) transitions, respectively. Fluorescence transitions from the laser-prepared upper levels terminating in X1Σ+ V = 0–28, A1Σ+ V = 1–3, A′1Π V = 1–13, and a3Π1 V = 3–12 are assigned. These results are combined with a previous analysis of the extensively perturbed BaS A1Σ+-X1Σ+ system [R. F. Barrow, W. G. Burton, and P. A. Jones, Trans. Farad. Soc.67, 902–906 (1971)]. Every observed perturbation of the BaS A1Σ+ state is electronically and vibrationally assigned. The levels a3Π0 V = 10–13, a3Π1 V = 12–14, a3Π2 V = 15, and A′1Π V = 10–13 are sampled via their perturbations of A1Σ+ V = 0–2. Although the mutual interactions of the a3Π, A′1Π, and A1Σ+ states approach Hund's case (c) limit, a complete deperturbation is performed from a case (a) starting point. Of the five lowest energy electronic states of BaS, only b3Σ+ remains uncharacterized. Principal deperturbed molecular constants are (in cm−1, 1σ uncertainties in parentheses):
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9.
Photo-induced changes in the infrared spectrum of amorphous, evaporated As2S3 films are described. The results are interpreted in terms of the photopolymerization of As4S4 molecular units and sulfur chains into an As2S3 glassy network. The role of photo-induced charged states in the polymerization process is discussed. 相似文献
10.
A. Possoz D. Favart L. Grenacs J. Lehmann P. Macq D. Meda L. Palffy 《Physics letters. [Part B]》1974,50(4):438-440
The average polarization of 12B produced by the capture of polarized muons in 12C has been measured using recoil implantation techniques. From the result we deduce the average polarization of the 12B ground state 12B(0) corresponding to the 12C → 12B(0) Gamow-Teller reaction: Jμ(0) = 0.43 ± 0.10. The sizeable deviation of this polarization from the value of 2/3, characteristic of a “bare” 0+ → 1+ process, is a fair evidence for induced axial-vector interaction(s) in muon capture. The ratio of the induced pseudoscalar and the axial-vector coupling constants is deduced to be: gμP/gμA = 12 ± 5. 相似文献
11.
The emission spectrum of B2 was reinvestigated under high resolution. Six bands of 11B2 (0-0, 1-1, 1-0, 2-1, 3-2, and 0–1) as well as four bands of 10B11B (0-0, 1-0, 2-1, and 3-2) were rotationally analysed. Accurate rotational and vibrational constants were obtained. The triplet character of the transition () was unambiguously established for the first time and spin-spin interaction constant is obtained for the excited state. 相似文献
12.
The high dispersion absorption spectrum of the Ag2 molecule has been photographed in the ~5300–1500-Å region. Observations include the previously reported A ← X, B ← X, C ← X, D ← X, and E ← X transitions and a new H ← X transition which occurs in the vacuum ultraviolet. Extensive spectral blending precluded detailed rotational analyses, but the band structures are consistent with and for D-X and C-X, respectively. The H state is perturbed and probably predissociated. The following molecular constants (in cm?1) were obtained from fitting bandhead data to the usual expressions:
State | Te | ωc | Xωt |
X | 0.0 | 192.0 | 0.58 |
B | 35 838.6 | 151.8 | 0.87 |
C | 37 631.6 | 171.0 | 0.84 |
D | 39 014.5 | 168.2 | 1.20 |
E | 40 159.9 | 146.1 | 1.58 |
H | 58 273.1 | 165.9 | 2.46 |