Probability of finding particle in half of a box for a given state

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SUMMARY

The discussion centers on solving the one-dimensional Time-Independent Schrödinger Equation (TISE) for a particle confined in a box with periodic boundary conditions. The eigenfunctions are correctly identified as u_n(x) = A e^{\frac{in \pi x}{a}}, with normalization constant A determined to be \frac{1}{\sqrt{2a}}. The probability of finding the particle in the region 0 < x < a is calculated using the state function ψ(x) = \frac{1}{\sqrt{2}}[u_1(x) + iu_2(x)], yielding a result of 1/2 - 1/π, approximately 0.2. The discussion emphasizes the importance of adhering to boundary conditions, particularly for infinite square wells, where the wave functions must equal zero at x = a and x = -a.

PREREQUISITES
  • Understanding of the Time-Independent Schrödinger Equation (TISE)
  • Familiarity with quantum mechanics concepts such as eigenfunctions and normalization
  • Knowledge of periodic boundary conditions in quantum systems
  • Ability to perform integrals for probability calculations in quantum mechanics
NEXT STEPS
  • Study the implications of boundary conditions on wave functions in quantum mechanics
  • Learn about the normalization of wave functions in quantum systems
  • Explore the calculation of probabilities using integrals in quantum mechanics
  • Investigate the differences between periodic boundary conditions and infinite square well potentials
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Students and professionals in physics, particularly those specializing in quantum mechanics, as well as educators teaching the principles of wave functions and probability in quantum systems.

trelek2
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Basically this is easy stuff I'm doing but i'n not sure whether i made a mistake or my answer is actually correct physically.

I'm solving the 1-dimensional TISE for a particle confined to a box -a<x<a.

I found that the eigenfunctions for this particle in a box with periodic boundary conditions are:[tex]u _{n}(x)=Ae ^{ \frac{in \pi x}{a} }[/tex] I'm pretty sure that this is correct.
I normalised A and got [tex]A= \frac{1}{ \sqrt{2a} }[/tex], which I'm also confident about.
And now I compute probability of finding particle in region 0<x<a when it is in state:
[tex]\psi (x)= \frac{1}{ \sqrt{2} }[u _{1}(x)+iu _{2}(x)][/tex]
I get that it is 1/2-1/pi which is about 0.2... Is that correct? Or should it be rather 1/2 simply.
 
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trelek2 said:
Basically this is easy stuff I'm doing but i'n not sure whether i made a mistake or my answer is actually correct physically.

I'm solving the 1-dimensional TISE for a particle confined to a box -a<x<a.

I found that the eigenfunctions for this particle in a box with periodic boundary conditions are:[tex]u _{n}(x)=Ae ^{ \frac{in \pi x}{a} }[/tex] I'm pretty sure that this is correct.
I normalised A and got [tex]A= \frac{1}{ \sqrt{2a} }[/tex], which I'm also confident about.
And now I compute probability of finding particle in region 0<x<a when it is in state:
[tex]\psi (x)= \frac{1}{ \sqrt{2} }[u _{1}(x)+iu _{2}(x)][/tex]
I get that it is 1/2-1/pi which is about 0.2... Is that correct? Or should it be rather 1/2 simply.

Be careful that you are meeting the boundary conditions. I assume you are talking about an infinite square well. If this is the case, the wave functions that you use have to be 0 at x=a, and x=-a. I believe this gives the solutions: [tex]u _{n}(x)=\sqrt{\frac{2}{a}}sin ( \frac{n \pi}{2a} (x+a))[/tex]

Now whatever [tex]\psi(x)[/tex] you use, the probability of finding the particle in region 0<x<a is [tex]\int_0^a |\psi(x)|^2 dx[/tex]
 

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