Undergrad How exactly does squaring operators (e.g. <p^2> work?

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Understanding the squaring of operators in quantum mechanics, particularly the momentum operator, involves recognizing that it is not simply about squaring its components. The expectation value of the squared momentum operator, <p^2>, requires integrating the second derivative of the wave function, indicating a change in the operator's differential nature. The discussion highlights confusion around the notation A(op), where A represents an operator and "op" is likely shorthand for "operator," suggesting a product of the operator acting on a function. It emphasizes that applying an operator involves sequentially operating on the wave function to produce new functions. Overall, the complexities of operator algebra and their implications in quantum mechanics are central to the discussion.
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I'm having to essentially piece together a framework of background knowledge to understand parts of a QM class in which I'm lacking prerequisites; one of the things that I noticed that really confused me was the square of the momentum operator <p>, and how that translated into the integrand of an expectation value; Squaring an operator as far as I'm as aware isn't as simple as just squaring its components, because, for the momentum operator defined as \langle p^2 \rangle = \int_{-\infty}^{\infty}\psi^*(x)p^2\psi(x) = \int_{-\infty}^{\infty}\psi^*(x)\bigg(-\hbar^2 \frac{\partial^2}{\partial x^2}\psi(x)\bigg)
The differential part of the operator changed, too! This isn't just squaring, what is it? \frac{d}{dx}\frac{d}{dx} \neq \frac{d^2}{dx^2} If I'm given some arbitrary operator A and told to calculate \langle A^2\rangle How do I know what the operator "squared" takes the form of?
 
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The differential part of the operator changed, too! This isn't just squaring, what is it?

operators are supposed to operate in a space - so a A^2 must be equivalent to A(op). A(op) , a product say operating on the right...
 
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I don't understand what that meant; I don't have any working knowledge of spaces, regardless of what they are.
drvrm said:
a product say operating on the right...
I also have no idea of what A(op) is supposed to indicate. A is the operator, and I'm only guessing "op" is shorthand for "operator", so unless A(op) is a really unnecessarily roundabout way of saying (A)(A) or something, I don't get it.
 
Alright then, thanks for the help(?).
 
##p^2\psi=pp\psi=p(p\psi)##, that is, you apply ##p## to ##\psi## to get a new function ##\psi_1##, then you apply ##p## to ##\psi_1##.

Likewise for any other operator.
 
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Thank you very much!
 
Time reversal invariant Hamiltonians must satisfy ##[H,\Theta]=0## where ##\Theta## is time reversal operator. However, in some texts (for example see Many-body Quantum Theory in Condensed Matter Physics an introduction, HENRIK BRUUS and KARSTEN FLENSBERG, Corrected version: 14 January 2016, section 7.1.4) the time reversal invariant condition is introduced as ##H=H^*##. How these two conditions are identical?

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