Commutator question. [A,B] =.lambda proof

In summary, the student is having trouble with a proof and is looking for help from classmates. They tried expanding the right side of the equation into three different exponentials and are not sure if they are on the right track. They are trying to solve a problem using the Baker-Campbell-Hausdorff formula.
  • #1
Jreyes613
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0

Homework Statement


Hello!
I'm having troubles with this proof.
given two operators A &B , such that [A,B] = λ where λ is complex,and μ is also complex, show that

exp{μ(A+B)} = exp{μA}exp{μB}exp{(-μ^2λ)/2}


Homework Equations



[A,B] = λ.
[A,B] = AB-BA = λ

The Attempt at a Solution


I have tried expanding the right side of the equation into three different exponentials by subbing in λ=AB-BA.
I get exp{μ(2A+2B-μAB+μBA}
but i seem to have a factor of two extra...
I'm not even sure if i am on the right track, so if anyone could give me a starting point it would be greatly appreciated!
 
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  • #2
It seems like maybe you tried adding the exponents on the right hand side. That's not allowed. If [itex]e^Ae^B[/itex] generally is not equal to [itex]e^{A+B}[/itex]. That would contradict what you are trying to show. Anyway, I'm not sure the best way to solve this problem, but what you are trying to show is.


[tex]\sum_{n=0}^\infty \frac{\mu^nA^n}{n!} \sum_{m=0}^\infty \frac{\mu^mB^m}{m!} \sum_{a=0}^\infty \frac{\left(-1\right)^a\mu^{2a}\lambda^a}{2^a a!}[/tex]
[tex]=\sum_{b=0}^\infty \frac{\mu^b (A+B)^b}{b!}[/tex]

You could try seeing if you can figure out where at the terms come from in the first expression.
[itex](A+B)^0= 1[/itex]
[itex](A+B)^1= A + B[/itex]
[itex](A+B)^2= A^2 + 2AB - [A,B]+ B^2 = A^2 + 2AB + B^2 - \lambda[/itex]
[itex](A+B)^3= (A+B)\left( A^2 + 2AB + B^2 - \lambda\right) [/itex]

However I'm really not sure exactly how to get this result.
 
  • #3
That's the Baker-Campbell-Hausdorff formula. Search with Google and you will probably find help in the proof.
 
  • #4
Thank you guys.
Yes , my TA said that you can use the Baker -Campbell-Hausdorff formula.

I will be able to solve it now, thanks!
 
  • #5



Hi there,

It looks like you are on the right track! The extra factor of two is likely coming from the expansion of the exponential function itself. Remember that exp(x+y) = exp(x)exp(y), so when you expand out the right side of the equation, you will end up with an extra factor of exp(μ^2λ/2) because you are multiplying three exponential terms together.

To solve this, you can use the fact that exp(x+y) = exp(x)exp(y) and also the commutator relation [A,B] = AB-BA = λ. From there, you can manipulate the terms to get the desired result. I would suggest starting with the right side of the equation and manipulating it until you get something that looks like the left side.

I hope this helps and good luck with your proof!
 

FAQ: Commutator question. [A,B] =.lambda proof

What is a commutator?

A commutator is an operator that measures the degree of non-commutativity between two operators. It is defined as the difference between the product of the two operators and the product of the same two operators in reverse order, [A,B] = AB - BA. A commutator is used to determine if two operators can be measured simultaneously or if they are incompatible.

How is a commutator calculated?

The commutator between two operators, A and B, is calculated by taking the product of the two operators and subtracting the product of the same two operators in reverse order, [A,B] = AB - BA. The resulting operator is the commutator between A and B.

What does the commutator [A,B] = λ prove?

The commutator [A,B] = λ does not prove anything on its own. It is simply a statement of the commutator between two operators, A and B. The value of λ can provide information about the compatibility of the two operators, but it does not prove anything by itself.

Can the commutator [A,B] be zero?

Yes, the commutator between two operators, A and B, can be zero if the two operators commute. This means that the order in which the operators are applied does not affect the outcome of the measurement. However, if the commutator is not zero, it indicates that the operators do not commute and cannot be measured simultaneously.

How is the commutator used in quantum mechanics?

In quantum mechanics, the commutator is used to determine the uncertainty in the measurement of two operators. If the commutator between two operators, A and B, is non-zero, it means that the two operators do not commute and therefore, there is an uncertainty in the measurement of these operators. The magnitude of the commutator can be used to calculate the lower bound of this uncertainty, as given by the Heisenberg uncertainty principle.

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