deepalakshmi
- 95
- 6
I will attach my work here
This is not allowed. You need to post your work directly, including equations (use the PF LaTeX feature for that--a LaTeX Guide link is at the bottom left of the post window).deepalakshmi said:I will attach my work here
That still doesn't answer the question I asked in post #29 about the Hamiltonian.deepalakshmi said:I evolved it with time evolution operator.
a, b are annihilation operator. b is similar to a. just change in variablePeterDonis said:That still doesn't answer the question I asked in post #29 about the Hamiltonian.
I don't understand. You only have one set of number operator states ##\ket{n}##. That means you have only one annihilation operator and one creation operator. "Change in variable" makes no sense here.deepalakshmi said:b is similar to a. just change in variable
Not here.deepalakshmi said:Is there any other way to share my work.
Then you will need to decide how much of it to post here. First, however, you might try answering post #38, and also post #30.deepalakshmi said:Calculation is 3 pages
I wrote the number terms in terms of creation operator. Then I inserted UUdagger which is basically time evolution operator. Later I applied BadaggerBdagger formula( baker campbell formula). I got a dagger cos theta+ ib dagger sin theta. I substituted this in place of creation operator. Later I used binomial expression and simplifiedPeterDonis said:I don't understand. You only have one set of number operator states ##\ket{n}##. That means you have only one annihilation operator and one creation operator. "Change in variable" makes no sense here.
As I said earlier, the initial state and hamiltonian is given to me by my guide.PeterDonis said:Not here.Then you will need to decide how much of it to post here. First, however, you might try answering post #38, and also post #30.
deepalakshmi said:##e^{-\frac{|\alpha|^2}{2}}\frac{(\alpha)^n}{\sqrt{n!}}|n>##
You forgot the sum over ##n##.deepalakshmi said:##e^{-\frac{|\alpha|^2}{2}}\frac{(\alpha)^n}{\sqrt{n!}}|n>##
Yeah I forgotDemystifier said:You forgot the sum over ##n##.
Think harder. It poses no contradiction.deepalakshmi said:actually the fidelity is always between 0 to 1 right? But I got exponential terms with alpha
Ok. I understood. Since there is a exponential power minus, value always lies between 0 to 1. I also took an example and the value always lies between 0 to 1. ThankyouHaorong Wu said:Think harder. It poses no contradiction.
You are still not answering my question. Your formula for the Hamiltonian has two sets of ladder operations, the a's and the b's. But you only have one set of number eigenstates ##\ket{n}##, so you should only have one set of ladder operators. Why are there two?deepalakshmi said:I wrote the number terms in terms of creation operator.
Who is your "guide"?deepalakshmi said:the initial state and hamiltonian is given to me by my guide.
Guide - teacherPeterDonis said:You are still not answering my question. Your formula for the Hamiltonian has two sets of ladder operations, the a's and the b's. But you only have one set of number eigenstates ##\ket{n}##, so you should only have one set of ladder operators. Why are there two?
Who is your "guide"?
I'm saying I don't understand why there are two sets of ladder operators in your Hamiltonian since you only have one set of number eigenstates. If you don't understand that either, perhaps you should ask your teacher.deepalakshmi said:Are you saying my question is wrong?
What do the two sets of operators operate on?deepalakshmi said:take beam splitter with input state as coherent and vacuum state. There also you have two sets of operator in Hamiltonian
Note: I've said this several times now, but you should think carefully about whether you agree with it.PeterDonis said:you only have one set of number eigenstates
Ok. I will ask my teacher about it.PeterDonis said:Note: I've said this several times now, but you should think carefully about whether you agree with it.
There those two set of operator will act on two states. One is coherent state which I will write in terms of vacuum state and other is vacuum state. So basically the two operator will act on two vacuum statePeterDonis said:I'm saying I don't understand why there are two sets of ladder operators in your Hamiltonian since you only have one set of number eigenstates. If you don't understand that either, perhaps you should ask your teacher.What do the two sets of operators operate on?