KFC
- 477
- 4
For 1D well with size a, the potential is V and when 0<=x<=a, V=0; othersize V = infinity
the Schrodinger equation becomes
<br /> \frac{d^2 f}{dx^2} + k^2 f = 0<br />
where f is the wavefunction.
For solving the equation, many textbook choose
<br /> f = A\sin(kx) + B\cos(kx)<br />
as the solution and apply the boundary conditions to find A and B. It is quite trival. However, I also try the solution
<br /> f = A\exp(ikx) + B\exp(-ikx)<br />
where i=\sqrt{-1} and this is also a solution. But if I apply the boundary condition, I get
<br /> B=-A, f=i2A\sin(kx)=0<br />
and from this it gives the same condition for k but somone said this is wrong. I know that k could be positive or negative but for either case why can't I chose the general solution as
<br /> f = A\exp(ikx) + B\exp(-ikx)<br />
the Schrodinger equation becomes
<br /> \frac{d^2 f}{dx^2} + k^2 f = 0<br />
where f is the wavefunction.
For solving the equation, many textbook choose
<br /> f = A\sin(kx) + B\cos(kx)<br />
as the solution and apply the boundary conditions to find A and B. It is quite trival. However, I also try the solution
<br /> f = A\exp(ikx) + B\exp(-ikx)<br />
where i=\sqrt{-1} and this is also a solution. But if I apply the boundary condition, I get
<br /> B=-A, f=i2A\sin(kx)=0<br />
and from this it gives the same condition for k but somone said this is wrong. I know that k could be positive or negative but for either case why can't I chose the general solution as
<br /> f = A\exp(ikx) + B\exp(-ikx)<br />