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1.
The approach to the Zγψ and Zγ? decay study is presented in detail, based on the sum rules for the Zc $ \bar c $ γγ* and Zb $ \bar b $ γγ* amplitudes and their derivatives. The branching ratios of the Zγψ and Zγ? decays are calculated for different hypotheses on saturation of the sum rules. The lower bounds of Σ ψ BR(Zγψ) = 1.95 × 10?7 and Συ BR(Zγ?) = 7.23 × 10?7 are found. Deviations from the lower bounds are discussed, including the possibility of BR(ZγJ/ψ(1S)) ~ BR(Zγ?(1S)) ~ 10?6, that could be probably measured in LHC. The angular distributions in the Zγψ and Zγ? decays are also calculated.  相似文献   

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3.
Matysina  Z. A.  Shchur  D. V. 《Russian Physics Journal》2001,44(11):1237-1243
Structural phase transformations of the hcp bcc fct fcc fct ( ) type in titanium hydrides TiH x experimentally found to occur with increase in the hydrogen concentration x are studied theoretically. Free energy phases are statistically calculated, and their concentration dependence is determined. Phase transformation temperatures are found from intersection points of free energy curves and from points of common tangents to the curves. The energy parameters of the system are estimated. The calculation results are compared with the experimental data.  相似文献   

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An intermediate image magnetic spectrometer was used to study the continuous +-spectrum of Pr140 and the Auger electrons of the decay chain Nd140Pr140Ce140. The maximum energy of the continuous +-spectrum is 2318±10 keV. The ratio of the intensities of the different Auger groupsK–LLK–LXK–MX=1 (0.58±0.05) (0.09±0.02). The ratio of the number of Auger electrons of the K-series to the electrons of the continuous spectrume K/ + is 0.292.
Nd140Pr140Ce140
Pr140 Nd140 Pr140140. +- — 2318±10 keV. -:K–LLK–LXK–MX=1(0,58±0,05) (0,09±0,02). K e K/ +=0,292.


We should like to thank Z. Macháek and Z. Dubcová for help in the measurements and J. Vlachý, graduate of the Faculty of Technical and Nuclear Physics, for help in the measurements and elaboration of the experimental results.  相似文献   

6.
New paths were designed for the investigations of the β-tin→Imma→sh phase transitions in nanocrystalline Ge under conditions of hydrostatic stress. A second-order transition between the β-tin and Imma phases was identified at 66 GPa, and a first-order transition between the Imma and sh phases was determined at 90 GPa. Superconductivity was obtained up to 190 GPa using the acquired structural data in first-principles calculations. This provides evidence that the standard electron-phonon coupling mechanism is responsible for superconductivity in Ge, as evidenced by the good agreement between the calculations and existing experiments.  相似文献   

7.
We present a systematic calculation on the 0c-decay branching ratios to excited-states of an even-even α-decay chain 242Cm→238pu→234U →230Th→226Rn by the improved barrier penetration approach. The changes of the parities between the parent nuclei and the daughter nuclei are properly taken into account. The theoretical values are compared with the available experimental data and the deviation between them is within a factor of 5 in most cases.  相似文献   

8.
We study the final-state interactions in B →π K decays through B → VV →π K processes where the inelastic rescattering occurs via single pion exchange. The next-to-leading order low-energy effective Hamiltonian and Bauer-Stech-Wirbel (BSW) model are used to evaluate the weak transition matrix elements and final-state interactions. We found that the final-state interaction effects in B →ρ K*→π K processes are significant. The Fleischer-Mannel relation for the Cabibbo-Kobayashi-Maskawa (CKM) angle γ can be significantly modified. Received: 13 August 1998  相似文献   

9.
《Physics letters. [Part B]》1997,415(4):395-401
The short distance QCD corrections to bsγγ are calculated in the leading logarithmic approximation. The equivalence of operator basis reduction for S-matrix elements by using the equations of motion or by proving a low energy theorem is discussed. We apply the above results to the exclusive Bsγγ decay. The branching ratio of this decay is found to be 5×10−7 in the Standard Model. We also found that QCD corrections modify considerably the ratio between CP-even and CP-odd two-photon amplitudes.  相似文献   

10.
We present a systematic calculation on the α-decay branching ratios to excited-states of an even-even α-decay chain ^242Cm → ^238Pu → ^234U → ^230Th → ^226Rn by the improved barrier penetration approach. The changes of the parities between the parent nuclei and the daughter nuclei are properly taken into account. The theoretical values are compared with the available experimental data and the deviation between them is within a factor of 5 in most cases.  相似文献   

11.
《Physics letters. [Part B]》1988,202(4):591-595
Effects of charged Higgs bosons (H+) on various loop-induced processes in the B-meson system are discussed, within the framework of two Higgs doublet models (2HDMs). The H+ contribution to the magnetic moment form factor turns out to be very significant and it can distinguish between the two types of 2HDMs. Even with constraints from Bd mixing, both strong enhancements or strong suppressions (in b→sγ) of decay rates are possible. Thus, information from these modes is competitive with, and may soon surpass, restrictions on 2HDMs from Bd mixing. Since (inclusive) b→sγ and b→sg1 at current limits are not excluded, continued effort to detect them is encouraged.  相似文献   

12.
Z→3γ和γγ→γγ极化张量的一般形式   总被引:1,自引:1,他引:0  
江向东  周咸建 《中国物理 C》1993,17(10):898-906
在标准模型下,讨论了Z→3γ衰变和γ→γ散射过程的单圈极化张量的一般形式.利用S3对称性和规范不变性对这种极化张量进行限制,从而得到一组约束方程.本文介绍了这种方法的主要步骤,并且将W玻色子圈的结果与费米子圈的结果作了比较.  相似文献   

13.
《Physics letters. [Part B]》1987,199(1):139-146
The decay rates of KL → 2γ and KS → 2γ have been measured at the CERN SPS. The results are Γ(KL→2γ)/χ(KL→2π0)=0.632±0.004±0.008 and Γ(KS→2γ)/Γ(KL→2γ)=2.3 ±1.0±0.4. This is the first observation of KS→2γ decays.  相似文献   

14.
本文给出了过程e++e-→J/ψ→V+X,X、P1+P2+P3(V和Pi分别代表矢量介子和赝标介子)的角分布螺旋度形式,为确定上述过程中间态X的自旋和宇称提供了理论公式.  相似文献   

15.
A study is made of the processes of annihilation of an arbitrarily polarized ee+ pair into a pair of particles of spin 0, 1/2, 1, and 3/2 in the (Z)-resonance region.Translated from Izvestiya Vysshikh Uchebnykh Zavedenii, Fizika, No. 10, pp. 53–59, October, 1978.  相似文献   

16.
《Physics letters. [Part B]》1988,207(1):106-108
Recently reported decays of the B→pp̄π and pp̄ππ have been interpreted as evidence for the b→u transition. It is shown that a certain class of b→c transitions could be misidentified and interpreted as B→pp̄π(π).  相似文献   

17.
Lepton spectra in decays have been studied with the ARGUS detector at thee + e storage ring DORIS II at DESY using the pseudo-rest-frame technique. We have improved upper limits for two-body -decays into a lepton and an unobservable particle.Supported by the German Bundesministerium für Forschung und Technologie, under contract number 054DO51P  相似文献   

18.
We calculate theK S Emphasis>0 →γγ decay within the approach of non-linear realization of chiralS U(3)×S U(3). The branching ratio with respect to theπ + π - channel turns out to be 3.5×10?6 and therefore similar to the result gotten previously by dispersion relation techniques in a non-chiral model. We also discuss theK L 0 →γγ decay by taking into account new results onη 1-η 8 mixing from recent measurements of the η→γγ decay.  相似文献   

19.
Applying the effective Lagrangian method,we study the flavor changing neutral current process b→ sγwithin the minimal supersymmetric extension of the Standard Model,where baryon and lepton numbers are local gauge symmetries.Constraints on the parameters are investigated numerically with the experimental data for the branching ratio of B→ X_sγ.Additionally,we present the corrections to direct CP-violation in B→ X_sγ and time-dependent CP-asymmetry in B→K~*γ.With appropriate assumptions on the parameters,we find the direct CP-violation Acp is very small,while one-loop contributions to S_(K~*_γ) can be significant.  相似文献   

20.
We have studiedD→K 0 * π andD→Ka 0 decays in the factorization approximation. The spectator model leads to a color-suppression of \(D^0 \to \bar K_0^{*0} \pi ^0 \) . However, due to the smallness off a 0, a similar suppression does not occur for \(D^0 \to \bar K^0 a_0^0 \) . We show that the inclusion of annihilation contribution can lift the color-suppression of \(D^0 \to \bar K_0^{*0} \pi ^0 \) . We also include final state interactions in a dynamical model whereK (1830) pole in the direct channel dominates the annihilation process.  相似文献   

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