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.
<br /> <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 /> <br />
he gets it to equal this, (but the stuff in brackets I have no idea where it came from!)
<br /> A^2\cdot\frac{\hbar^2}{2m}\int^{\infty}_{-\infty}{dx\left(\alpha^2} - \alpha^4 x^2\right)e^{-\alpha^2x^2}<br />
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..
<br /> 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)<br />
is there an identity I am missing? also where has the minus which was in front of hbar^2 at the beginning gone?
<br /> <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 /> <br />
he gets it to equal this, (but the stuff in brackets I have no idea where it came from!)
<br /> A^2\cdot\frac{\hbar^2}{2m}\int^{\infty}_{-\infty}{dx\left(\alpha^2} - \alpha^4 x^2\right)e^{-\alpha^2x^2}<br />
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..
<br /> 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)<br />
is there an identity I am missing? also where has the minus which was in front of hbar^2 at the beginning gone?