磁场中的旋转双荷黑洞

本文给出了磁场中的Kerr-Newman-Kasuya黑洞(旋转双荷黑洞)的电磁场的严格表式。在Φ《Q=-2B₀J的特殊情况下,给出了慢速转动的Kerr-Newman-Kasuya黑洞的引力场表式。 关键词：     

一类新的复合场方程及解

采用5维空间4+1分解的方法建立了标量场、电磁场和引力场的复合场方程,并给出了一个复合场方程的静态球对称解 当标量场及其与电磁场的耦合不存在时(β=0),此解退化为ReissnerNordtstrom度规.还给出了标量场和电磁场产生的复合场源流密度矢量的表示式 关键词：     

一级磁结构相变材料Mn0.6Fe0.4NiSi0.5Ge0.5和Ni50Mn34Co2Sn14的磁热效应与磁场的线性相关性

磁熵变（△S_M）与磁场（μ₀H）的相关性已在很多二级相变材料中被研究并报道,但一级相变材料的磁热效应与磁场相关性还少有报道.本文在具有一级磁结构相变的Mn_0.6Fe_0.4NiSi_0.5Ge_0.5材料中研究发现△S_M与μ₀H存在线性相关性,并通过麦克斯韦关系式的数值分析详细讨论了这一线性相关性的来源.同时,进一步发现在低磁场时,△S_M近似正比于μ₀H的平方.该线性相关性同样在一级磁结构相变Ni₅₀Mn₃₄Co₂Sn₁₄材料中得到了印证.但由于一级磁弹相变LaFe_11.7Si_1.3材料相变温度具有更强的磁场依赖性,不具有△S_M的线性相关性,因此,本研究表明,当磁结构相变材料的相变温度具有弱磁场依赖性时,△S_M与μ₀H具有线性相关性.进而,在磁场未达到相变饱和磁场以下,利用△S_M与μ₀H的线性相关性可以有效推测更高磁场下的△S_M.     

YBa2Cu3O7超导管内磁场与外磁场的关系

本文报道了当外磁场H_e较低时(H_e<4H_rm,其中H_rm是超导管的最大捕获磁场),超导管的内磁场H_i与时间及外磁场的关系可表示为H₀+B₀(lnt+1-exp(-t/τ)),式中B₀Int与磁通蠕动有关,B_c(1-exp(-t/τ))与外磁场引起的磁通扰动有关。扰动随时间很快衰减.H₀,B₀及1/τ随外磁场增加,在H_e>H_rm时,这几个量增加较大。当直流外磁场H_e<1/2H_rm时,超导管可将其完全屏蔽,对交流场不能完全屏蔽,但其屏蔽效果仍优于最好的金属屏蔽筒。 关键词：     

荷电天体引力场中试验粒子进动的后牛顿解法

采用后牛顿近似方法分析讨论了荷电天体引力场(即Reissner-Nordstr(o)m度规场)中试验粒子的轨道进动情况,给出了荷电量Q对试验粒子轨道进动的影响.     

二重非交换时空与二重复对称引力理论

通过引入二重复对称度规张量，建立了一种二重复对称引力理论. 从一个二重实的作用量出发，导出了静态球对称二重复度规的具体表达式. 该理论扩展了Moffat结果，不仅自然地得到了双曲复对称引力理 论，而且把著名的Schwarzschild解作为特殊情况包含在其中，并且在线性化的弱场近似下自动摆脱了Moffat理论中存在的负 能鬼态问题. 进一步，通过将二重复坐标推广到满足二重非对易关系以及将Moyal星积二重 化，由此构造出二重非交换复对称引力场作用量. 关键词： 非交换几何 复对称度规 非对易坐标 引力场作用量     

电子温度各向异性对螺旋波等离子体中电磁模式的传播及功率沉积特性的影响

采用考虑粒子温度各向异性热等离子体介电张量模型,借助磁化、均匀密度分布等离子体中电磁波的一般色散关系,在低磁场、低气压螺旋波等离子体典型参量条件下,理论分析了电子温度各向异性对电磁模式传播特性和角向对称模功率沉积的影响.研究结果表明:对于给定的纵向静磁场B₀(或波频率ω),存在一个临界波频率ω_cr(或纵向静磁场B_0,cr),当ω>ω_cr(或B₀0,cr)时,电子回旋谐波遭受的阻尼开始显著增大;相比粒子温度各向同性情形,粒子温度各向异性彻底改变了波的传播特性,即相位常数和衰减常数均出现峰值现象;在考虑电子有限拉莫尔半径效应和电子温度各向异性情形下,Trivelpiece-Gould (TG)波碰撞阻尼在整个电磁波功率沉积中占据主导地位,电子纵向温度T_e,//存在某一临界值,在此临界值处TG波功率沉积出现峰值P_abs,TG,且随着T_e,⊥/T_e,//的减小,...     

磁荷对中子星质量半径比的约束

讨论了荷电(磁)质点的量子力学波方程及其解. 由磁场中解的奇异性讨论了磁单极的存在; 由Rubakov-Callan模型推知中子星可能含有大量磁单极. 然后采用中子星的结构方程, 讨论了磁荷对中子星质量半径比的约束, 分别得到了磁荷对中子星质量半径比上限的影响 和磁荷对中子星质量半径比下限的影响的数学表达式. 关键词： 磁单极 中子星 质量半径比     

Reissner—Nordstr?m度规中(电荷守恒下)的引力质量亏损

本文在文献[1,3]讨论荷电静态和球对称度规下的引力质量亏损的基础上进一步讨论电荷守恒的情况。并计算了亏损以后的质量M随初始质量M₀、荷质比α和半径γ的各种变化曲线。 关键词：     

离轴磁场退火后Tb0.3Dy0.7Fe1.95〈110〉取向晶体的磁致伸缩"跳跃"效应

将〈110〉取向Tb_0.3Dy_0.7Fe_1.95合金棒放在与轴向成35°夹角的外磁场中退火处理,研究其在0—30 MPa预压应力σpre作用下的磁致伸缩效应.结果表明,σpre=0条件下的饱和磁致伸缩值λs由退火前的1023×10^-6提高到1650×10^-6;σpre 关键词： 磁致伸缩 磁场退火 磁致伸缩"跳跃"效应     

横向磁场导致CO2激光器混沌运转及其奇异吸引子的观测

在外加磁场的情况下,对单模均匀展宽CO₂激光器进行了实验研究。改变磁场的大小,观察到了自脉动和混沌现象,同时还获得了该系统的奇异吸引子,并对其物理机制进行了探讨。     

超导膜的能隙和磁场的依赖关系

本文计算出超导膜在磁场中的能隙。所得到的表达式适用于所有的温度,但磁场要满足((ehp₀/(mc) A/(πk_BT_c))²《1条件,其中A是矢势,hp₀是Fermi动量。理论结果和实验进行了比较,符合得还好。     

The trace anomaly in coloured black holes

The influence of the trace anomaly of the energy-momentum tensor of gauge theories is discussed in a spherically symmetric space-time. It is found that for pure electric and magnetic fields, the point β(g) = ?g represents a phase transition from any asymptotically flat metric to an asymptotically non-flat metric which turns out to be confining in the electric case.     

On Existence of Static Metric Extensions in General Relativity

Motivated by problems related to quasi-local mass in general relativity, we study the static metric extension conjecture proposed by R. Bartnik [4]. We show that, for any metric on ¯B ₁ that is close enough to the Euclidean metric and has reflection invariant boundary data, there always exists an asymptotically flat and scalar flat static metric extension in M=³B ₁ such that it satisfies Bartnik's geometric boundary condition [4] on B ₁.     

The Positive Action conjecture and asymptotically Euclidean metrics in quantum gravity

The Positive Action conjecture requires that the action of any asymptotically Euclidean 4-dimensional Riemannian metric be positive, vanishing if and only if the space is flat. Because any Ricci flat, asymptotically Euclidean metric has zero action and is local extremum of the action which is a local minimum at flat space, the conjecture requires that there are no Ricci flat asymptotically Euclidean metrics other than flat space, which would establish that flat space is the only local minimum. We prove this for metrics onR ⁴ and a large class of more complicated topologies and for self-dual metrics. We show that ifR 0 there are no bound states of the Dirac equation and discuss the relevance to possible baryon non-conserving processes mediated by gravitational instantons. We conclude that these are forbidden in the lowest stationary phase approximation. We give a detailed discussion of instantons invariant under anSU(2) orSO(3) isometry group. We find all regular solutions, none of which is asymptotically Euclidean and all of which possess a further Killing vector. In an appendix we construct an approximate self-dual metric onK3 — the only simply connected compact manifold which admits a self-dual metric.     

The exterior gravitational field of a charged spinning source in the poincaré gauge theory: A Kerr-newman metric with dynamic torsion

We present a new exact solution of the Poincaré gauge theory, namely a charged Kerr-NUT metric with an effective cosmological constant which is consistently coupled to a dynamic torsion field. The solution is given in terms of an orthonormal basis in Boyer-Lindquist coordinates and depends on the constants m₀ (mass), j₀ (angular momentum), q₀ (electric charge), and n₀ (NUT parameter). Whereas m₀,j₀, and q₀ can be specified arbitrarily, the NUT parameter and the effective cosmological constant are determined by the coupling constants of our model. The torsion of the solution is centered around the coordinate origin and vanishes asymptotically for large radial distance. For n₀=0, we find the exterior gravitational field of a charged spinning source.     

强磁场中n型锗的横向磁阻

本文就声子散射与电离杂质散射的两种散射机构探讨了半导体n型锗的横向磁阻。在简并强磁场情况下,得出声子散射机构在〈111〉,〈110〉和〈100〉三个方向上锗的横向磁阻的表示式。磁阻的平均值的相对大小(ρ_t<111>)/ρ₀:(ρ_t<110>)/ρ₀:(ρ_t<100>)/ρ₀=1:1.7:1.1,并且磁阻具有振荡形式。在非简并量子极限情况下分别对声子散射和杂质散射得出锗的横向磁     

在Tokamak装置中用中空超导环段冻结环向磁场的设想

本文提出一个设想:即将n个中空超导圆柱体放置于n饼纵场线圈之中,分段冻结环向磁场,则其所需要的电功率将比常规线圈降低到2/n倍。我们知道超导材料的冻结场可近似地写为。H_fj(r,T)=H_fj(r,0)[1-(T/(T_c))²。因此选定T=T₁,当轴向场H在大圆环的内壁达到H≥H_fj(r,T₁)时,中空体的内边缘达到临界场,则场进入中空区,再使H降到零,中     

合金薄膜的临界磁场

本文把文献[2]的理论推广到含有杂质的超导薄膜情形,得出合金薄膜的二极相变临界磁场。本文得到的结果,在2d》ξ₀而l任意时,或者2d《ξ₀而l<<2d时,趋于Гинэбург-Ландау理论;在2d<ξ₀而l>2d时,与Гинэбург-Ландау理论不同(l是杂质所决定的电子平均自由程)。理论符合Blumbers实验。     

Mixing transformations on metric spaces

It is proved that if a metric space is subjected to a mixing transformation, then there exists a positive numberx ₀ such that the probability that any arbitrary set of positive measure is asymptotically mapped into a set of diameter less thanx ₀ is zero. Physical implications of this result, in particular the interpretation of Poincaré recurrence, are discussed.