Algebra
\[a _{+}= \frac{ 1 }{ \sqrt{2hmw} }(-h \frac{ d }{ dx }+mwx)\]
\[\psi_{0}= (\frac{ mw }{ \pi h })^{1/4} e^{-\frac{ mwx^2 }{ 2h }}\]
what is most efficient way to calculate \[(a_{+})^2 \psi_{0}\]
This cannot be algebra LOL
well stuck at algebra part
@hartnn
a+ is an operator? i see d/dx there
yes
do it term by term, like square the \(\dfrac{1}{\sqrt{2hmw}}\) part and multiply it with \(\dfrac{mw}{\pi h}\)
I thought to evaluate (a+)^2 first
\[(a_{+})^2= \frac{ 1 }{ 2hmw}(-h^2 \frac{ d^2 }{ dx^2 }-2hmw+m^2w^2x^2)\]
ok, then you'll have to do it one by one only, calculate (-h d/dx + mwx) e^(...) m,w,h, pi are constants...you can put them aside initially also, calculating (a+)^2 might give you wrong answer
nope for middle term you did d/dx(x) right? i am not sure that is even valid
you'll have to keep it as (-2hmxw d/dx )
are those operator rules?
not sure...but i am thinking logically (a+)^2 is an operator too, it should not operate on the dependent variable x
the safest way to get \((a_{+})^2 \psi_{0}\) is \((a_{+})(a_{+}) \psi_{0}\) only
\((a_{+})[(a_{+}) \psi_{0}]\)
although \((a_{+})^2= \frac{ 1 }{ 2hmw}(-h^2 \frac{ d^2 }{ dx^2 }\color{red}{-2xhmw\frac{d}{dx}}+m^2w^2x^2)\) can work, need to check.
\[(a_{+}\psi_{0}= (\frac{ mw }{ \pi h })^{1/4} (\frac{ 2mwx^2 }{ h }-1)\]
*e^()
doesn't seem right? used the chain rule, right?
thats given in the textbook
wait, let me rewrite
wait, let me rewrite \[\frac{ 1 }{ \sqrt{2hmw} } (\frac{ mw }{ \pi h})^{1/4} 2mwxe^{\frac{ -mwx^2 }{ 2h }}\]
I can handle from here thanks
We can't take derivative with in the operator right? took a note of it thanks
that seems correct now. and yes. operator should not operate on itself :P welcome ^_^
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