Change of variables in a propagator

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The discussion centers on the nuances between the states |p⟩ and |E⟩ in quantum mechanics, particularly regarding their integration and transformation. The participant questions how changing variables from momentum (p) to energy (E) affects the value of integrals, noting that the relationship between p and E is not linear. They present equations demonstrating the integration of |p⟩ and |E⟩ states, highlighting the complexities introduced by the variable change. The conversation also touches on the implications of integrating over both positive and negative momentum states and how to reconcile these with expected outcomes. Clarification is sought on excluding certain terms to align with anticipated results.
Jacob Nie
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Homework Statement
I'm reading Shankar's quantum mechanics. He states that the equation for the propagator ##U(t)## (such that ##|\psi(t)\rangle = U(t)|\psi(0)\rangle##) is
$$ U(t) = \sum_E |E\rangle \langle E|e^{-iEt/\hbar}.$$
Later, when deriving the propagator for a free particle, he changes variable from ##E## to ##p## (for each ##E## there are two possible ##p## with that energy: ##\pm (2mE)^{1/2}##):
$$U(t) = \int_{-\infty}^{\infty} |p\rangle \langle p | e^{-iE(p)t/\hbar} \ dp.$$
My question: why is it ##dp## and not ##dE?## Shouldn't turning ##\sum_E |E\rangle \langle E|e^{-iEt/\hbar}## into an infinite dimensional version translate to
$$U(t) = \int_{-\infty}^{\infty} |p\rangle \langle p | e^{-iE(p)t/\hbar}\ dE\ ?$$
Then, to properly change to ##dp,## wouldn't one use the proper substitution method using ##dE = \dfrac{dE}{dp}dp##?
Relevant Equations
##|E\rangle ## are the eigenkets of the relevant Hamiltonian ##H.##

Some other relevant equations: ##|E,+\rangle = |p=(2mE)^{1/2}\rangle## and ##|E,-\rangle = |p = -(2mE)^{1/2}\rangle.##
I'm guessing that there must be some nuance that I do not quite understand in the difference between ##|p\rangle## and ##|E\rangle##?

Like, later in the book even ##dk## is used as a variable of integration, where ##k = p/\hbar.## Surely this has effects on the value of the integral - wouldn't it change it by a numerical factor? In the case of ##p## and ##E,## it would change by more than just a numerical factor, because they're not linearly related.
 
Last edited:
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U(0)=1=\int_{-\infty}^{+\infty} |p>dp<p|= \int_0^{\infty} |E>dE<E|
seems all right.

<E'|E>=\delta(E'-E)=\delta(p'^2/2m - p^2/2m)=2m\delta(p'^2-p^2)=m/|p|\{\delta(p'-p)+\delta(p'+p)\}=m/2|p|\{<p'|p>+<-p'|p>+<p'|-p>+<-p'|-p>\}

|E>=\sqrt{\frac{m}{2|p|}}\{|p>+|-p>\}

dE=d(p^2/2m)=\frac{p}{m}dp

\int_0^\infty |E>dE<E|=\int_{0}^{+\infty} \{|p>+|-p>\}dp\{<p|+<-p|\}=\int_{-\infty}^{+\infty}|p>dp<p|+ \int_{-\infty}^{+\infty}|-p>dp<p|

The first RHS term is ##1## and the second term is operator of reversing momentum.

How should we exclude the second term to meet the anticipation ? Your advise is appreciated.
 
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