Solving Awkward Integral: Missing Identity & Lost Minus?

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SUMMARY

The discussion centers on the mathematical manipulation of an integral involving the second derivative operator, specifically the expression A^2∫_{-∞}^{∞} e^{-1/2α^2x^2} (−ħ²/2m)(∂²/∂x²)e^{-1/2α²x²}. The lecturer transforms this into A²(ħ²/2m)∫_{-∞}^{∞} (α² − α⁴x²)e^{-α²x²} dx, which raises questions about the derivation of the terms in brackets and the disappearance of the negative sign in front of ħ². The confusion arises from the interpretation of the second derivative operation rather than an identity replacement.

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  • Familiarity with quantum mechanics concepts, including the role of ħ (reduced Planck's constant) and mass (m).
  • Knowledge of differential operators, specifically the second derivative (∂²/∂x²).
  • Basic grasp of mathematical identities used in integration and differentiation.
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Students of physics and mathematics, particularly those studying quantum mechanics or advanced calculus, will benefit from this discussion as it clarifies integral manipulation and the application of differential operators.

philip041
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I can't understand what my lecturer has done, it looks like he has replaced d^2/dx^2 with an identity but I'm not sure.

[tex] <br /> A^2\int^{\infty}_{-\infty}{dxe^{-1/2\alpha^2x^2}}\cdot\left(\frac{-\hbar^2}{2m}\frac{\partial^2}{\partial x^2}\right)e^{-1/2\alpha^2x^2}<br /> [/tex]

he gets it to equal this, (but the stuff in brackets I have no idea where it came from!)

[tex] A^2\cdot\frac{\hbar^2}{2m}\int^{\infty}_{-\infty}{dx\left(\alpha^2} - \alpha^4 x^2\right)e^{-\alpha^2x^2}[/tex]

he then goes on to do this but I think if I understood the first step this bit would be ok, but here you go anyway..

[tex] A^2\cdot\frac{\hbar^2}{2m}\left(\alpha^2\frac{\pi^{1/2}}{\alpha} - \alpha^4\frac{\pi^{1/2}}{2\alpha^3}\right)[/tex]

is there an identity I am missing? also where has the minus which was in front of hbar^2 at the beginning gone?
 
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philip041 said:
I can't understand what my lecturer has done, it looks like he has replaced d^2/dx^2 with an identity but I'm not sure.

[tex] <br /> A^2\int^{\infty}_{-\infty}{dxe^{-1/2\alpha^2x^2}}\cdot\left(\frac{-\hbar^2}{2m}\frac{\partial^2}{\partial x^2}\right)e^{-1/2\alpha^2x^2}<br /> [/tex]

he gets it to equal this, (but the stuff in brackets I have no idea where it came from!)

[tex] A^2\cdot\frac{\hbar^2}{2m}\int^{\infty}_{-\infty}{dx\left(\alpha^2} - \alpha^4 x^2\right)e^{-\alpha^2x^2}[/tex]

What does

[tex] e^{-\frac{1}{2} \alpha^2x^2}} \left(\frac{-\hbar^2}{2m}\frac{\partial^2}{\partial x^2}\right)e^{-\frac{1}{2} \alpha^2x^2}[/tex]

equal?
 
He hasn't "replaced d^2/dx^2 with an identity", he has done the indicated second derivative.
 

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