Why 1D well must has this solution?

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SUMMARY

The discussion centers on the solutions to the Schrödinger equation for a one-dimensional well with potential V, where V=0 for 0≤x≤a and V=infinity elsewhere. Two forms of the wavefunction are analyzed: the standard form f=A sin(kx) + B cos(kx) and the complex form f=A exp(ikx) + B exp(-ikx). While the latter is deemed valid, the necessity for the wavefunction to be real for bound states is questioned. The conclusion emphasizes that the physical observables derived from either form yield the same results, regardless of the imaginary components in the wavefunction.

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For 1D well with size a, the potential is V and when 0<=x<=a, V=0; othersize V = infinity


the Schrödinger 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 someone 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 />
 
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Your solution seems perfectly reasonable to me, it only differs from the textbook one with a phase factor, it seems, and as we know, for real physical quantities such factors doesn't matter. So I'd say you can use your solution.
 
1) recall that A,B in these two eq's is not nessicary equal:
f = A\sin(kx) + B\cos(kx)
f = A\exp(ikx) + B\exp(-ikx)

2) Also recall that you can write f = A\exp(ikx) + B\exp(-ikx)
as something with cos and sin. So the two solutions are the same, except that you can't have the same A and B...
 
The equivalence of the two solutions is more apparent if you use different names for the arbitrary constants:

\psi = A \cos {kx} + B \sin {kx}

\psi = C e^{ikx} + D e^{-ikx}

Using Euler's formula

e^{i \theta} = \cos \theta + i \sin \theta

you can derive equations for C and D in terms of A and B, and vice versa. So it's only a matter of convenience which solution you use.
 
Thanks for all your reply. Well, I know that the solution (bound state) should be

A\sin(kx) + B\cos(kx)

that why I need to take the real part of my solution mentioned before. But my question is: why wave function for bound state must be real?

Thanks. Have a nice thanksgiving.
 
It does not have to! It is you who restrict the vaules of A and B to be real numbers.
When introducing constants, one has to specify which set they belong to.
 
It shouldn't matter if you have the factor of i in your bound state solution. When finding <psi \ psi> or any expectation value, you multiply by the complex congagate of the wave function anyway. This eventually results in the same value as if the i was never there. It may seem weird that the wavefunction itself is imaginary, but all that really matters are the physically measurable values.
 

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