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1)  infinite square potential well
无限深方势阱
1.
new method of calculating summation of series is constructed by using a set of suitable wave functions in an infinite square potential well of one dimension.
利用一维无限深方势阱中一套适当的波函数,建立了一种新的级数求和方法。
2.
On the basis of the analytical solution in an infinite square potential well of one dimension, this paper deduces 24 summation formulas of infinite series, such as n=11n~(2),(n=11n~(4), etc.
在一维无限深方势阱的解析解的基础上,利用波函数的归一化常数及能量平均值的两种不同算法的等价性,导出了∑∞n=11n2、∑∞n=11n4等24个无穷级数的求和公式。
2)  infinite deep spherical potential well
无限深球方势阱
1.
Then it uses the model of infinite deep spherical potential well and the model of hydrogen atom to solve the problem.
采用二体模型,通过坐标变换把二体问题化为两个单体问题,再分别采用无限深球方势阱和氢原子模型求解,通过一定的近似,得到了ZnO量子点的基态能的近似解析解。
3)  infinite potential well
无限深势阱
1.
In this paper,A new cyclic model of quantum Carnot heat engine whose working substance consists of non-interacting extreme relativistic particles confined to an infinite potential well,is set up.
本文建立一种量子卡诺热机循环模型,该量子卡诺热机循环以一维无限深势阱中极端相对论粒子系统为工质。
4)  one-dimensional infinite square well
一维无限深方势阱
1.
The first-,second- and third-order perturbation corrections to the zero-order energy levels and the first- and second- order corrections to the zero-order wave functions of particles in a one-dimensional infinite square well with a δ(x)-potential perturbation are calculated in detail.
详细计算了δ(x)势微扰下一维无限深方势阱中粒子能级的一、二、三级和波函数的一、二级修正。
5)  three-dimensioanl infinite square well
三维无限深方势阱
6)  infinite-potential-well model
无限深势阱模型
1.
<Abstrcat> In this paper, the formation of the lowest subband states in symmetric coupled quantum-well is discussed with the use of an infinite-potential-well model, and the evolvement rules of the lowest subband states in the presence of an electric field along the direction of the well are analyzed with the use of two-energy-level system at length.
采用无限深势阱模型分析对称耦合量子阱中最低子能级的形成,并利用二能级体系理论给出对称耦合量子阱中各子能级随外电场的变化规律。
补充资料:单量子阱(见量子阱)


单量子阱(见量子阱)
single quantum well

单且子阱sillgle quantum well见量子阱。
说明:补充资料仅用于学习参考,请勿用于其它任何用途。
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