I Identity involving exponential of operators

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The discussion focuses on deriving a specific formula from a physics paper, particularly equation (22). The key insight involves the operator identity that relates the differential operator $(\partial_x - \mathrm{i} e/\hbar By)$ to an exponential function of operators. By iterating this relationship, it is shown that for any natural number k, the operator can be expressed in terms of exponentials and derivatives of the function $\psi(\vec{x})$. This approach simplifies the derivation of the equation in question. The conclusion emphasizes the commutation relation $[\partial_x, y] = 0$ as a crucial aspect of the derivation.
thatboi
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Hey all,
I saw a formula in this paper: (https://arxiv.org/pdf/physics/0011069.pdf), specifically equation (22):
1680505109627.png

and wanted to know if anyone knew how to derive it. It doesn't seem like a simple application of BCH to me.
Thanks.
 
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Please use LaTeX to type formulae. It's much easier to read!

The trick is that
$$(\partial_x - \mathrm{i} e/\hbar By)\psi (\vec{x}) = \exp(\mathrm{i} e B x y/\hbar) \partial_x \left [\exp(-\mathrm{i} e B x y/\hbar) \psi(\vec{x}) \right]$$
for all ##\psi(\vec{x})## (in the domain of the operators applied ;-)).

By iteration it's further easy to see that for ##k \in \mathbb{N}##
$$(\partial_x - \mathrm{i} e/\hbar By)^k\psi (\vec{x}) = \exp(\mathrm{i} e B x y/\hbar) \partial_x^k \left [\exp(-\mathrm{i} e B x y/\hbar) \psi(\vec{x}) \right].$$
Plugging this into the series defining the operator exponential you get Eq. (22) of the paper.
 
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Likes thatboi, topsquark and gentzen
Or, leaving out a lot of details: ##[\partial _x, y] = 0##.

-Dan
 
For the quantum state ##|l,m\rangle= |2,0\rangle## the z-component of angular momentum is zero and ##|L^2|=6 \hbar^2##. According to uncertainty it is impossible to determine the values of ##L_x, L_y, L_z## simultaneously. However, we know that ##L_x## and ## L_y##, like ##L_z##, get the values ##(-2,-1,0,1,2) \hbar##. In other words, for the state ##|2,0\rangle## we have ##\vec{L}=(L_x, L_y,0)## with ##L_x## and ## L_y## one of the values ##(-2,-1,0,1,2) \hbar##. But none of these...

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