How Do You Solve These Commutator Relations?

  • #1
Juli
21
5
Homework Statement
Solve ##[\hat{r}^{17}, \hat{p}]## and ##[\hat{r}, \hat{p}^{250}]##
Relevant Equations
##[\hat{p}, \hat{x}^{n}] = - i \hbar n x^{n-1}##
Hello, I need to solve the commutator relations above. I found the equation above for the last one, but I am not sure, if something similar applys to the first one. I am a little bit confused, because I know there has to be a trick and you don't solve it like other commutator.
Thanks for your help!
 
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  • #2
Are you familiar with the expansion of a commutator on the form ##[AB,C]##? If not, take the time to write it out and see if you can express it in terms of commutators containing only two operators.
 
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  • #3
You understand, of course, that the relevant equation is what you need to prove. You can do this using mathematical induction and the identity suggested by @Orodruin.
 
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FAQ: How Do You Solve These Commutator Relations?

What is a commutator in quantum mechanics?

A commutator in quantum mechanics is an operator that measures the difference between the sequential application of two operators. Mathematically, for operators \( \hat{A} \) and \( \hat{B} \), the commutator is defined as \([ \hat{A}, \hat{B} ] = \hat{A}\hat{B} - \hat{B}\hat{A} \). It provides insight into the relationship between the two operators and whether they can be measured simultaneously.

How do you compute the commutator of two operators?

To compute the commutator of two operators \( \hat{A} \) and \( \hat{B} \), you apply the definition: \([ \hat{A}, \hat{B} ] = \hat{A}\hat{B} - \hat{B}\hat{A} \). This involves performing the operations in both orders (first \( \hat{A} \) then \( \hat{B} \), and vice versa) and subtracting the results. The specific steps can vary depending on the forms of \( \hat{A} \) and \( \hat{B} \).

What are some common commutator relations in quantum mechanics?

Some common commutator relations in quantum mechanics include:

  • \([ \hat{x}, \hat{p} ] = i\hbar \), where \( \hat{x} \) is the position operator and \( \hat{p} \) is the momentum operator.
  • \([ \hat{L}_i, \hat{L}_j ] = i\hbar \epsilon_{ijk} \hat{L}_k \), where \( \hat{L}_i \) are the components of the angular momentum operator and \( \epsilon_{ijk} \) is the Levi-Civita symbol.
  • \([ \hat{a}, \hat{a}^\dagger ] = 1 \), where \( \hat{a} \) and \( \hat{a}^\dagger \) are the annihilation and creation operators, respectively.
These relations are fundamental in understanding the behavior of quantum systems.

Why are commutator relations important in quantum mechanics?

Commutator relations are crucial in quantum mechanics because they provide information about the compatibility of measurements and the underlying symmetries of quantum systems. If the commutator of two operators is zero, the operators are said to commute, implying their corresponding physical quantities can be measured simultaneously with certainty. Non-zero commutators indicate inherent uncertainties and are related to the Heisenberg uncertainty principle.

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