Resonances in the dtµ molecular ion between tµ(n=2) and dµ(n=2) thresholds

Elastic and inelastic cross sections in collisions of a tµ atom in 2s and 2p states on deuteron have been obtained within the framework of a four-channel adiabatic approximation for the case of total orbital angular momentumJ=0. The calculated data has been applied to verify the existence of resonance in the dtµ molecular ion at 0.8 eV above the tµ(n=2) threshold. It appears that the second and third resonant states (at 0.8 eV and at 7 eV above the tµ threshold) in a series converging to the dµ(n=2) threshold do not produce any resonant structure in the energy spectrum. The higher vibrational states are visible in the spectrum, however their widths are about 0.1 eV and therefore their life-times are about 10^–15 s which allows to conclude that these states could not play an important role in the µCF cycle as well as in processes of diffusion of muonic atoms.     

The O(N) vector model in the large-N limit revisited: multicritical points and double scaling limit

The multicritical points of the O(N)-invariant N vector model in the large-N limit are re-examined. Of particular interest are the subtleties involved in the stability of the phase structure at critical dimensions. In the limit N → ∞ while the coupling g → g_c in a correlated manner (the double scaling limit) a massless bound state O(N) singlet is formed and powers of 1/N are compensated by IR singularities. The persistence of the N → ∞ results beyond the leading order is then studied with particular interest in the possible existence of a phase with propagating small mass vector fields and a massless singlet bound state. We point out that under certain conditions the double scaled theory of the singlet field is non-interacting in critical dimensions.     

光的衍射法测量金属的线胀系数

给出测量金属线胀系数的一种新方法．利用光的衍射法可以较精确地测量长度变化这一特点，对黄铜的线胀系数进行了测量．     

金属线膨胀系数测定实验的改进及进一步研究

为了更好地研究金属线膨胀系数在一定温度区间的变化情况,并进一步研究在加热过程中,待测金属热应力、热应变的变化规律,本文在传统的蒸汽喷射加热仪的基础上,组合运用了粘滞系数实验、表面张力实验以及温度传感器实验中的部分实验仪器,测量并计算了相关的物理量,得到了相关性较理想的拟合直线,并通过对比实验进一步论述了该方法的可行性。     

高空核爆炸碎片云早期扩展规律研究

利用磁流体力学理论建立了描述碎片云运动的壳层模型,采用该模型模拟了美国Starfish高空核爆炸试验碎片云的运动参数,通过与文献模拟结果的比对,验证了所建模型的正确性.针对典型大当量和小当量核爆的不同,重点模拟了千吨级利百万吨级核武器在100,400和1500 km高度爆炸时碎片云运动扩展情况,分析了当量的差异引起的扩展规律的不同.结果表明:高空核爆炸时不同爆炸条件和大气环境对碎片云的扩展规律有着显著的影响,不同方向上碎片云的环境参数差异明显.     

Hf-基非晶合金的力学性能研究

 利用MTS810实验机和分离式霍普金森压杆（SHPB）,对Hf_44.5Cu₂₇Ni_13.5Ti₅Al₁₀块体非晶合金进行了准静态和动态压缩实验,应变速率范围为10^-4~10³ s^-1,给出了不同应变速率下非晶合金的应力-应变曲线,并对其压缩断口形貌进行了扫描电镜观察。结果表明：在准静态压缩条件下,Hf_44.5Cu₂₇Ni_13.5Ti₅Al₁₀非晶合金不具有应变速率敏感性,在由放射区和扇形区组成的断口形貌上观察到纳米级韧窝和60 nm左右的周期性条纹结构;在动态压缩条件下,随着应变速率的增加,动态屈服强度明显减小,合金具有应变速率敏感性,同时断裂表面为夹杂着脉络条纹的絮状结构。进一步观察发现,动态压缩断口上存在3种特征断裂形貌：树枝状条纹、典型脉络花纹和合金熔体。     

XANES analysis of spectral properties and structures of arsenate adsorption on TiO2 surfaces

X‐ray absorption near‐edge structure (XANES) of arsenate adsorption on TiO₂ surfaces was calculated using self‐consistent multiple‐scattering methods, allowing a structural analysis of experimental spectra. A quantitative analysis of the effect of disorder revealed that the broadening and weakening of the characteristic absorption in experimental XANES was due to the structural disorder of the arsenate–TiO₂ adsorption system. The success with calculating the scattering amplitude of a specific set of paths using the path expansion approach enables the scattering contributions of different coordination shells to the XANES to be sorted out. The results showed that the scattering resonances from high‐level shells inherently overlapped onto the first‐shell scattering amplitudes, and formed the fine structures in the XANES region. A variation in one oscillatory feature could be due to several structural changes affecting specific single/multiple‐scattering amplitudes. Therefore, direct assignments of spectral features with structural elements should be based on adequate theoretical analysis.     

晶格中心插入体的对称性及取向对二维声子晶体带隙的影响

以二维钢/气体系声子晶体为模型,采用平面波法研究了圆柱正方及六角晶格中心添加插入体的对称性及取向与带隙的关系,给出了四方、六方、八方及圆柱插入体结构的带隙分布图及带隙随柱体取向的变化关系图.发现在低填充率条件下,插入体的截面形状与晶格类型相同时最有利于能带简并态的分离而获得带隙,但填充率较高时,采用高对称性的插入体可以获得最宽的带隙.正方晶格中心插入体取向对带隙的影响要比在六角晶格中更为显著.对四方柱正方晶格声子晶体的研究表明,仅旋转原柱体要比在其中心插入柱体后旋转更容易获得低频宽带隙,单独运用添加柱体或旋转非圆柱体来降低晶格对称性以获取低频带隙的方法要比同时使用两种方法效果更好.此外,从机理上对计算结果进行了解释.     

二极管爆炸发射阴极等离子体的膨胀扩展

分析了二极管中爆炸发射产生阴极等离子体的演化特征,在考虑了阴极等离子体朝阳极膨胀运动使二极管阴阳极间距缩短这一效应的同时,还计入了阴极等离子体沿发射表面径向扩展运动对二极管有效发射面积的影响。基于Child-Langmuir定律,利用在一个四脉冲强流电子束源装置上得到的电流、电压等实验数据,假定阴极等离子体轴向膨胀和径向扩展速度近似相等,研究了阴极等离子体的膨胀扩展动力学行为。计算结果表明,阴极等离子体朝阳极的膨胀和沿径向的扩展速度为0.9～2.8 cm/s。     

Tb2Fe15.5Cr1.5化合物的本征磁致伸缩

通过x射线衍射及磁测量手段研究了Tb2 Fe1 5 5Cr1 5化合物的热膨胀性质及本征磁致伸缩性质 .研究结果表明Tb2 Fe1 5 5Cr1 5化合物在 2 93— 6 72K的温度范围内具有六角相的Th2 Ni1 7型结构 .在 4 32— 5 2 2K的温度范围内具有负热膨胀性质 ,其平均热膨胀系数 α =- 1 5 7× 10 - 5 K .对本征磁致伸缩的研究结果表明Tb2 Fe1 5 5Cr1 5化合物中存在着较强的各向异性的本征磁致伸缩 ,2 93K时其本征体磁致伸缩约为 8. 4× 10 - 3,晶格畸变主要发生在c轴方向上 .磁测量研究结果表明Tb2 Fe1 5 5Cr1 5化合物的居里温度约为 4 94K ,比其母合金Tb2 Fe1 7高约 80K .