当前位置: X-MOL 学术Eur. J. Phys. › 论文详情
Our official English website, www.x-mol.net, welcomes your feedback! (Note: you will need to create a separate account there.)
1D potential wells of the form
European Journal of Physics ( IF 0.6 ) Pub Date : 2021-03-02 , DOI: 10.1088/1361-6404/abd0d9
Abby Corrigan , Janine Shertzer

We consider the finite potential well defined by $V\left(\left\vert x\right\vert {< }a\right)=-{V}_{o}\left(1-\frac{{\left\vert x\right\vert }^{n}}{{a}^{n}}\right)$,where n is an integer. The Schrdinger equation is recast into dimensionless form; the size of the well is characterized by a single parameter $\alpha =\sqrt{2m{V}_{o}}a/\hslash $. We use three different mathematical techniques to solve for the energy eigenvalues and wave functions. Analytic solutions are given for the triangular well (n = 1), the parabolic well (n = 2), and the square well (n → ∞). The finite element method is used to obtain accurate numerical results for 1 ⩽ n ⩽ ∞ over a full range of α. Finally, both the energy and wave function are expanded in a Taylor series in order to study the analytic behavior of the ground state energy (as a function of n) as α → 0.



中文翻译:

一维潜在形式的井 $ \ boldsymbol {V} \ left(\ left \ vert \ boldsymbol {x} \ right \ vert {<} \ boldsymbol {a} \ right)=-{\ boldsymbol {V}} _ {\ boldsymbol {o}} \ left(1- \ frac {{\ left \ vert \ boldsymbol {x} \ right \ vert} ^ {\ boldsymbol {n}}} {{\\ boldsymbol {a}} ^ {\ boldsymbol {n}}} \\对)$

我们认为由定义的有限电势$ V \ left(\ left \ vert x \ right \ vert {<} a \ right)=-{V} _ {o} \ left(1- \ frac {{\ left \ vert x \ right \ vert} ^ {n}} {{a} ^ {n}} \ right)$,其中n是整数。薛定inger方程式被重铸为无量纲形式。井的大小由一个参数来表征$ \ alpha = \ sqrt {2m {V} _ {o}} a / \ hslash $。我们使用三种不同的数学方法来求解能量特征值和波动函数。给出了三角形阱(n = 1),抛物线阱(n = 2)和正方形阱(n →∞)的解析解。有限元方法被用于获得1个⩽准确数值结果Ñ在全范围的∞⩽ α。最后,能量和波函数都以泰勒级数展开,以研究基态能量(作为n的函数)为α →0的解析行为。

更新日期:2021-03-02
down
wechat
bug