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1.
ITER低温泵需要定期再生循环以去除吸附的气体,处于安全考虑氢的累计体积摩尔浓度不能超过1.5mol?m?3,从而使得再生的容积必须不小于15m3,需要额外设计容器结构以提供足够的再生容积,同时兼顾支撑和密封的作用。介绍了ITER低温泵外部容器的结构与功能,并运用有限元分析方法对其不同载荷状况进行了数值计算,为其结构设计与优化提供了理论依据。  相似文献   

2.
The universality of the weak interactions can be tested in semileptonic b→c transitions,and in particular in the ratios R(D~(*)) ≡Γ(B → D(*)τν)/Γ(B → D~(*)lν)(where 1 = μ or e).Due to the recent differences between the experimental measurements of these observables by Ba Bar,Belle and LHCb on the one hand and the Standard Model predicted values on the other hand,we study the predicted ratios R(D~(*))=Γ(B→D~(*)τ+"missing")/Γ(B→D(*)lν)in scenarios with an additional sterile heavy neutrino of mass ~1 Ge V.Further,we evaluate the newly defined ratio R(0)≡Γ(B→τ+"missing")/Γ(B→μν) in such scenarios,in view of the future possibilities of measuring the quantity at Belle-Ⅱ.  相似文献   

3.
We present a preliminary measurement of the B(Ds→μvμ) with the Belle experiment at the KEKB collider. We select Ds→μvμ decays with a method that provides a high-purity of the selected sample and an absolute measurement of the branching fraction. The results are based on a data sample of 550 fb-1 and are compared to similar measurements by other experiments as well as to the predictions of LQCD. We conclude with short prospects for improvements in the accuracy of the measurement.  相似文献   

4.
We present a preliminary measurement of the B(D_s→μν_μ)with the Belle experiment at the KEKB collider.We select D~s→μV_μdecays with a method that provides a high-purity of the selected sample and an absolute measurement of the branching fraction.The results are based on a data sample of 550 fb~(-1)and are compared to similar measurements by other experiments as well as to the predictions of LQCD.We conclude with short prospects for improvements in the accuracy of the measurement.  相似文献   

5.
Significant mixing is expected between the neutral bottom mesons \(B_s^0 - \bar B_s^0 \) in the standard model of weak interactions. We propose measurements of the processes \(\left\{ {\begin{array}{*{20}c} {e^ + e^ - } \\ {p\bar p} \\ \end{array} } \right\} \to \begin{array}{*{20}c} {b\bar b} \\ {} \\ \end{array} \to l^ + K^ - K^ - X\) as a measure of such mixing. Rates are presented for energetic bottom quark jets, produced ine + e ? annihilation.  相似文献   

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用KMT多次散射展开的一级项和程函扭曲波冲量近似,并采用拟合电子非弹性散射实验的跃迁密度,研究了正负π介子在Ca核上的非弹性散射,同时预言了K~±介子在Ca上的非弹性散射.  相似文献   

8.
K ±e ± νπ 0 decays have been studied using the KMN setup at the Institute for High Energy Physics (Protvino). The experiment has been performed in the 36-GeV/c hadron beams of the IHEP accelerator. The accumulated data allow us to select ~1.08M candidates for K e3 decays. Analyzing the Dalitz plot of these events, we estimate the linear slope of the charge form factor to be λ + = [30.44 ± 0.83(stat.) ± 0.74(syst.)] × 10?3.  相似文献   

9.
Elastic scattering differential cross section data of ± d at 65 MeV and ± 4He at 51 MeV are presented and compared respectively to fully relativistic 3-body and optical potential calculations including true pion absorption.Presented at the symposium Mesons and Light Nuclei, Liblice, Czechoslovakia, June 1981.  相似文献   

10.
Using the ACCMOR spectrometer equipped with a vertex telescope of high resolution silicon microstrip detectors 74 decays \(D^ + \to \bar K^{*0} (892)e^ + v_e \) (andcc.) withx F <0.4 have been observed in 200 GeV π? Be interactions. The cross-section forD ± production, itsx F -dependence in the central region and theD ± lifetime have been measured.  相似文献   

11.
Mg10±δIr19B16±δ是具有非中心对称性的超导材料.通过对两种组分的样品Mg9.3Ir19B16.7和Mg11Ir11B15的比热测量,得到了这类超导体的超导态和正常态的特征参数:包括转变温度Tc,正常态态密度N(EF),德拜温度ΘD,上临界场Hc2等.并由此求出Ginzburg-London相干长度ξGL,穿透深度λGL,下临界场HC1和热力学临界场HC,这些参数因化学组分不同而变化.高的N(EF)和ΘD对应高的TC,因此也具有较高的Hc2,另外比热跃变△C/γnTc=1.66和电声子耦合常数λ=0.58不随化学组分变化,表明此超导体是中等强度耦合的第二类超导体.  相似文献   

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负绝对温度出现以来,有不少人对它进行了研究.例如,Ramsey[1]最先对负温度1)情况下的热力学及统计物理学作了扼要的阐述,并指出负温度比正的更高.随后Hecht[2],Vysin[3]及其他一些人[4]又对负温度下的平衡和稳定的条件以及有关的一些问题进行了研究.从这些研究的结果得出一个重  相似文献   

14.
本文研究了L±算符和量子包络代数生成元之间的具体关系,并以UqAN代数和UqG2代数为例,用生成元明显表出L±算符.  相似文献   

15.
《Physics letters. [Part B]》1986,173(4):480-484
Current experimental limits on K±π±ee+ rule out a neutral scalar particle with the couplings of the standard Higgs boson and mass in the range 50 MeV to 211 MeV. Planned experimental improvements could lead to a bound mHmKmπ.  相似文献   

16.
We calculate direct CP-violating rate asymmetries in chargedBPP andBVP decays arising from the interference of amplitudes with different strong and CKM phases. The perturbative strong phases develop at order α s from absorptive parts of one-loop matrix elements of the next-to-leading logarithm corrected effective Hamiltonian. CPT constraints are maintained. Based on this model, we find that partial rate asymmetries between charge conjugateB ± decays can be as high as 20% for certain channels with branching ratios in the 10?6 range. Because the $c\bar c$ threshold lies so close to the physical momentum scale, the asymmetries depend sensitively on the model assumptions used to evaluate the imaginary parts of the matrix elements, in particular, on the internal momentum transfer. The charge asymmetries of partial rates would provide unambiguous evidence for direct CP violation.  相似文献   

17.
利用北京谱仪(BES)在4.03GeV正负电子对撞能量下获取的数据,[研究了,τ+τ-产生过程.借助双标记方法分析了τ±→π+π-π±υτ衰变事例.测定分支比Br(τ±→a1±υτ→ρ0π±υτ,ρ0→π+π-=(7.3±0.5)%,Br(τ±→K*±υτ→Ks0π±υτ,Ks0→π+π-)=(0.6±1.5)×10-3.并由Daliz投影分布的分析,确认a1的主要衰变方式ρπ.同时,也观察到a1衰变中以S波贡献为主的现象.采用Kuhn模型拟合实验数据,得到:ma1=1.24±0.02GeV,Γa1T=0.57±0.07GeV.  相似文献   

18.
We report on a search for CP violation in τ(±)→K(S)(0)π(±)ν(τ) decays using a data sample of 699 fb(-1) collected by the Belle experiment at the KEKB electron-positron asymmetric-energy collider. The CP asymmetry is measured in four bins of the invariant mass of the K(S)(0)π(±) system and found to be compatible with zero with a precision of O(10(-3)) in each mass bin. Limits for the CP violation parameter Im(η(S)) are given at the 90% confidence level. These limits are |Im(η(S))| < 0.026 or better, depending on the parametrization used to describe the hadronic form factors, and improve upon previous limits by 1 order of magnitude.  相似文献   

19.
<正> 一、图纸要求(见图1) 对零件要求: N=* △N=0.2 α=2.7″B=▽f′(min)=4000m 技术条件: 1.*允许到一个光圈,此时两边N的符号应相反,数值差不大于0.4个光圈; 2.两块光楔按偏转角之和为285“±1”配对; 3.60°槽铣在零件最厚端,槽对光楔主截面偏差±2~*。本文叙述276.8“±2”的楔角加工及60°定位槽对主截面偏差加工中的保证。二、工艺方案的选择光楔的楔角加工方法一般分为两种,一种  相似文献   

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