共查询到20条相似文献,搜索用时 281 毫秒
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本对公式D=ε0E0给出了一种新的证明方法。指出一篇章对此问题的讨论中的不妥之处。 相似文献
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HT-7托卡马克中等离子体平衡研究 总被引:1,自引:0,他引:1
本文解决了二维轴对称近似下带铁芯的托卡马克中等离子体平衡问题,计算了HT-7托卡马克中的等离子体平衡位形以及极向场系统的非线性电感和垂直场系数。最后应用Kirchhoff方程组和平衡垂直场公式得到了一组等离子体、加热场和垂直场线圈的电流波形的自洽曲线。 相似文献
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应用自恰的热力学方式确定夸克质量公式中的参数,并进一步证明,在新的质量标度下,适量的负电荷仍然可以降低奇异夸克物质的临界密度,从而有利于在重离子磁撞实验中寻找strangelets。当然,过量的负电荷仍将使味平衡成为不可能。 相似文献
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在受约束物体的碰撞中牛顿公式是成立的 总被引:1,自引:0,他引:1
本文对于“受约束物体非弹性碰撞中牛顿公式不适用”这种看法提出了商榷.证明在这类碰撞中牛顿公式是成立的.对于受实际(有弹性的)绳子约束的物体的碰撞问题分别几种情况,提出了解决办法. 相似文献
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推导了刚性回路同时作平动和转动的情况下,回路面的磁通量变化率公式,从较普遍的情况证明,由电磁感应定律和由洛伦兹力得到的动生电动势相等.并将公式应用于载流回路和感应电流所受的磁力(矩)分析,为电磁学基本问题的研究提供理论依据. 相似文献
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The general solution to the complex Bateman equation is constructed. It is given in implicit form in terms of a functional relationship for the unknown function. The known solution of the usual Bateman equation is recovered as a special case. 相似文献
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张昌莘 《原子与分子物理学报》2006,23(1):157-162
在均匀强磁场中,当氢原子的哈密顿量中B2项不能忽略时,氢原子的库仑场对称性遭到破坏,能级简并被全部解除.在应用变分法和数值法计算氢原子的能级过程中,计算十分复杂,而应用微扰法求解氢原子的能级,存在解久期方程的n2高阶行列式的困难.本文应用简并态微扰理论和球谐函数的性质,得到久期方程中非零微扰矩阵元普遍表达式.根据非零微扰矩阵元普遍表达式的性质,可以将氢原子塞曼效应久期方程的n2高阶行列式分解成1阶到n阶共n个低阶行列式的乘积,得到氢原子塞曼效应久期方程的简化公式,使得求解均匀强磁场中氢原子塞曼效应能级过程简化.而且由该公式可以得到氢原子在低能态时塞曼效应能级的解析解.根据该久期方程的简化公式计算了n=3氢原子塞曼效应一级近似能级. 相似文献
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H. Dekker 《Optics Communications》1974,10(2):114-119
Starting from a multimode hamiltonian for a system of radiating oscillators coupled with atomic reservoirs, the secular master equation for the radiation-density operator is calculated in the interaction picture after elimination of the atomic variables. Using the differential operator representation for coherent states this equation is transcribed into a multimode Fokker-Planck equation. The stationary solution in momentum space is given for the threshold region. Fourier transformation to configuration space results in a quasi-free energy formula for a laser oscillator exhibiting spatial dispersion. 相似文献
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Thomas EpelbaumFrançois Gelis 《Nuclear Physics A》2011,872(1):210-244
In a previous work [arXiv:1009.4363], we have studied the evolution of a scalar field with a quartic coupling, driven by a classical source that initializes it to a non-perturbatively large value. At leading order in the coupling, the evolution of this system is given by classical solutions of the field equation of motion. However, this system is subject to a parametric resonance that leads to secular divergences in higher-order corrections to physical observables. We have proposed a scheme that resums all the leading secular terms: this resummation leads to finite results at all times, and we have observed also that it makes the pressure tensor of the system relax to its equilibrium value.In the present paper, we continue the study of this system by looking at finer details of its dynamics. We first compute its spectral function at various stages of the evolution, and we observe that after a fairly short transient time there are well-defined massive quasi-particles. We then consider the time evolution of the momentum distribution of these quasi-particles, and we show that after a stage dominated by the parametric resonance, this distribution slowly evolves to an equilibrium distribution. Interestingly, this distribution develops a transient chemical potential, signaling the fact that number changing processes are much slower than the elastic ones. 相似文献
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T. Shimizu 《Physics letters. A》1975,51(1):42-44
A microscopic derivation of evolution equations for the dominant secular motion of macroscopic variables and for the moments around its secular motion is given. 相似文献
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The relation between the thermal equilibrium Hall conductivity generated by minimal gauge transformation and the isolated Hall conductivity given by the Kubo formula is investigated. The contribution of the edge states and some general questions concerning the definition of the equilibrium Hall conductivity are discussed. It is shown that, in the case of an additive electron-impurity system, the two Hall conductivities coincide as long as the Fermi energy is situated in an energy gap. 相似文献
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A. Lenard 《Journal of statistical physics》1978,19(6):575-586
An elementary derivation is given of the formula for the thermal equilibrium states of quantum systems that can be described in finite-dimensional Hilbert spaces. The three assumptions made, Passivity, Structural Stability, and Consistency, have phenomenological interpretations. Except at zero temperature, Structural Stability follows already from Passivity and a weak form of Consistency. 相似文献