Harmonic Oscillator: Evaluating Ground State Probability

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Homework Statement



Using the normalization constant A and the value of a, evaluate the probability to find an oscillator in the ground state beyond the classical turning points ±x0. Assume an electron bound to an atomic-sized region (x0 = 0.1 nm) with an effective force constant of 1.0 eV/nm2.

Homework Equations



[itex]\psi(x)=Ae^{-ax^{2}}[/itex], where [itex]A=(\frac{m\kappa}{\pi^{2}\hbar^{2}})^{1/8}[/itex] and [itex]a=\sqrt{m\kappa}/2\hbar[/itex]

The Attempt at a Solution



How do I find m?
 
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I will try to read the question more carefully next time.
 
Am I supposed to find probabilities at both tails of the distribution?
 
Apparently there is an inconsistency in the question and there are two interpretations of the question. What would be the other one?
 
My interpretation: find probabilities at both tails of the distribution i.e. [itex]\int^{0}_{-\infty}\psi^{2}(x)\;dx[/itex] and [itex]1-\int^{0.1}_{-\infty}\psi^{2}(x)\;dx[/itex].
 
Do you mean it is wrong according to your interpretation or it is generally wrong? Should it be 0.1?
 
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It should be -0.1, right?
 
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