Concepts about infinite potential well

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SUMMARY

The discussion centers on the concepts of the one-dimensional infinite potential well, specifically addressing the stationary states and their representation through Fourier series. Participants clarify that the stationary states, represented by the wave function $$\Psi_n(x,t) = \sqrt{\frac{2}{a}}\sin \left( \frac{n \pi x}{a} \right) e^{-i E_n t / \hbar}$$, can be expressed as a linear combination of these states. The confusion arises regarding the expansion of a constant function in a Fourier sine series, which is explained as being constant only at time t=0, with time dependence emerging subsequently. The relationship between Fourier series and the infinite square well is established through the coefficients $$c_n$$ that define the wave function's evolution.

PREREQUISITES
  • Understanding of quantum mechanics principles, particularly stationary states.
  • Familiarity with Fourier series and their mathematical representation.
  • Knowledge of wave functions and their time evolution in quantum systems.
  • Basic grasp of the infinite potential well model in quantum mechanics.
NEXT STEPS
  • Study the derivation of stationary states in the infinite potential well using quantum mechanics textbooks.
  • Learn about the mathematical formulation of Fourier series and their applications in quantum mechanics.
  • Explore the concept of wave function evolution over time in quantum systems.
  • Investigate the implications of probability density in stationary states and its time independence.
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Students and professionals in physics, particularly those specializing in quantum mechanics, as well as educators looking to clarify concepts related to the infinite potential well and Fourier series.

VHAHAHA
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As we know, the 1d infinite potential well has a stationary state. The function that depends on x onky is a sin function.
However, I don't understand the concept in this question. I have the answer of this question and this is not a homework. I am not asking for the answer so please don't put this post to the homework section.
I don't understand the part 2 of this question because the potential well should be in stationary state. Why i need to prove it in part 2?
Also, in part 3, i don't understand why there is a constant function. The fuction should be a product of sin function and exponential function. How come there is a constant function?
Thank you for your help
 
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The authors are asking you to expand a constant function in a Fourier sine series. It's a constant in the sense that it does not depend on the position for a fixed time t=0. For subsequent times, it won't be a constant anymore.
 
dauto said:
The authors are asking you to expand a constant function in a Fourier sine series. It's a constant in the sense that it does not depend on the position for a fixed time t=0. For subsequent times, it won't be a constant anymore.

what is a Fourier series:confused:
 
VHAHAHA said:
what is a Fourier series:confused:

A sum of sines and/or cosines whose frequencies are integer multiples of a fundamental frequency (if we're talking about a function of time) or whose wavenumbers are integer multiples of a fundamental. See for example

http://en.wikipedia.org/wiki/Fourier_series
 
what is the relation between these two ?:(
 
See, Simply put , stationary states of 1-d box are those in which the probability density (and also expectation values) are independent of time. do this : construct the time dependent wavefunction by stacking exponential time dependence alongside the sines. check out the probability density. in this case multiplication of complex exponentail (in time) and its conjugate causes time dependence part to fizzle out, leaving only sine squared. ditto with avg. value of any operator.
QED
 
VHAHAHA said:
what is the relation between these two ?:(

I'm guessing that by "these two" you mean Fourier series and the infinite square well.

The stationary states of the infinite square well (0 < x < a) are
$$\Psi_n(x,t) = \sqrt{\frac{2}{a}}\sin \left( \frac{n \pi x}{a} \right) e^{-i E_n t / \hbar}$$

Any state of the infinite square well can be written as a linear combination of these:
$$\Psi(x,t) = \displaystyle\sum_{n=1}^\infty {c_n \Psi_n(x,t)}$$

At t = 0:
$$\Psi(x,0) = \displaystyle\sum_{n=1}^\infty {c_n \sqrt{\frac{2}{a}}\sin \left( \frac{n \pi x}{a} \right)}$$

which is basically a Fourier series. For any function defined in the range 0 < x < a, you can find the coefficients ##c_n## which make this true. Put these coefficients into the linear combination for ##\Psi(x,t)## and it tells you how the wave function evolves in time from ##\Psi(x,0)##. Any decent QM textbook has the details.
 

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