Infinite square well, dimensionless Hamiltonian..

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SUMMARY

The discussion centers on the formulation of the infinite square well problem and the concept of a dimensionless Hamiltonian. The user expresses confusion regarding the boundary conditions of the well, specifically how to apply them when transitioning from a well defined from 0 to L to one defined from -b/2 to b/2. The suggestion is made to solve the problem using the variable transformation x' = x - b/2 to facilitate understanding and application of the boundary conditions.

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Students and professionals in physics, particularly those focusing on quantum mechanics, as well as educators seeking to clarify the infinite square well problem and its boundary conditions.

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Homework Statement
Electron with mass m* moves in a 1D quantum well with infinite barriers at x= -b/2 and
x=+b/2.
Assume mass of the electron to be m*=0.5 m where “m” is free electron mass.
a. Write Schrodinger equation and the Hamiltonian in dimensionless form
b. Solve stationary Schrodinger equation, find allowed energy levels, give explicit expression for 1st,2nd, and 3rd energy levels
d. give wavefunctions for the first three levels – plot them.
e. give 3 energy levels ,in meV, for a=4 nm
Relevant Equations
H phi = -hbar^2 / 2m d^2/dx phi(x) = E phi (x)
I have always seen this problem formulated in a well that goes from 0 to L

I am confused how to use this boundary, as well as unsure of what a dimensionless hamiltonian is.
This is as far as I have gotten
1572389128351.png
 
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What would keep you from solving it as if the well was from 0 to ##b## and then, once you had the solution, changing variables ##x' = x-\frac{b}{2}##?
 
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Likes   Reactions: Abhishek11235
Alternatively,put the boundary conditions at -b/2 and b/2 same as you did for [0,L]
 

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