Derivation of an expression involving boson operators

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In summary, the conversation discusses an expression found in a paper regarding the derivation of relations involving boson operators. There is confusion about the derivation process and the use of a partial derivative, as well as the meaning of the symbol "N" in the expression. The source of the paper is provided and the conversation delves into the details of the equations involved.
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patric44
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Homework Statement
derive the following expression involving boson operator
Relevant Equations
B=\sum_{i}\alpha_{i}b_{i}
Hi all
I found this expression in a paper that concerns the derivation of some relations about boson operators but it is not very clear to me how the results were obtained. The derivation starts as, let B be an operator as a linear combination of different boson operators:
$$
B=\sum_{i}\alpha_{i}b_{i}
$$
then the expectation value of the identity operator in the n-boson state is :
$$
\bra{B^{n}}\hat{1}\ket{(B^{\dagger})^{n}}=\bra{B^{n-1}}\sum_{i}\alpha_{i}\frac{\partial}{\partial b^{\dagger}_{i}}\ket{(B^{\dagger})^{n}}=n\alpa^{2}N_{n-1}
$$
where the partial derivative came from? and what is big N,the paper doesn't mention that, shouldn't the expression be :
$$
\bra{B^{n}}\hat{1}\ket{(B^{\dagger})^{n}}=\bra{B^{n-1}}B\ket{(B^{\dagger})^{n}}=\bra{B^{n-1}}\sum_{i}\alpha_{i}b_{i}\ket{(B^{\dagger})^{n}}
$$
can any one clarify, I will appreciate any help.
Thanks in advance
 
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patric44 said:
Homework Statement: derive the following expression involving boson operator
Relevant Equations: B=\sum_{i}\alpha_{i}b_{i}
Did you forget some hash hash symbols?

patric44 said:
I found this expression in a paper
It's usually a good idea to include a link to your source, just in case you've mistyped or misunderstood something.

patric44 said:
where the partial derivative came from?
It's possible to prove a general formula like $$[a, f(a^\dagger)] ~=~ i\hbar \, \partial_{a^\dagger} f(a^\dagger) ~.$$The constant ##i\hbar## factor might be different depending on what conventions you're using for the canonical commutation relations. (Exercise: use induction to prove this formula for simple functions like ##f(x) = x^n##, then use linearity of the commutator to generalize the formula to polynomials.)
patric44 said:
and what is big N,
I'm guessing it's the number operator, something involving ##\sum_i b_i^\dagger b_i##.
patric44 said:
the paper doesn't mention that, shouldn't the expression be :
$$
\bra{B^{n}}\hat{1}\ket{(B^{\dagger})^{n}}=\bra{B^{n-1}}B\ket{(B^{\dagger})^{n}}=\bra{B^{n-1}}\sum_{i}\alpha_{i}b_{i}\ket{(B^{\dagger})^{n}}
$$
Without seeing the paper, it's impossible to say for sure. But my guess is "no". Write out the expression properly and apply the rule I described above.
 
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strangerep said:
Did you forget some hash hash symbols?It's usually a good idea to include a link to your source, just in case you've mistyped or misunderstood something.It's possible to prove a general formula like $$[a, f(a^\dagger)] ~=~ i\hbar \, \partial_{a^\dagger} f(a^\dagger) ~.$$The constant ##i\hbar## factor might be different depending on what conventions you're using for the canonical commutation relations. (Exercise: use induction to prove this formula for simple functions like ##f(x) = x^n##, then use linearity of the commutator to generalize the formula to polynomials.)

I'm guessing it's the number operator, something involving ##\sum_i b_i^\dagger b_i##.

Without seeing the paper, it's impossible to say for sure. But my guess is "no". Write out the expression properly and apply the rule I described above.
the paper isn't open access so I thought I would write the question separably, here is the link of the paper:
the paper, the commutation relation is included in the paper but i am not interested in proving them, rather my concern is equations 4a,4b,4c
 

FAQ: Derivation of an expression involving boson operators

What are boson operators?

Boson operators are mathematical constructs used in quantum mechanics to describe the quantized states of bosonic particles, which are particles that follow Bose-Einstein statistics. The two primary boson operators are the creation operator (denoted as \(a^\dagger\)) and the annihilation operator (denoted as \(a\)). These operators are used to add or remove a boson from a given quantum state, respectively.

What is the commutation relation for boson operators?

The fundamental commutation relation for boson operators is given by \([a, a^\dagger] = aa^\dagger - a^\dagger a = 1\). This relation is crucial for deriving various expressions involving boson operators and is a defining characteristic of bosonic systems.

How do you derive the number operator using boson operators?

The number operator \( \hat{N} \) is derived using boson operators and is defined as \( \hat{N} = a^\dagger a \). This operator counts the number of bosons in a given state. By applying the commutation relations, one can show that \( \hat{N} \) has eigenvalues corresponding to the number of bosons present in the state.

What is the significance of normal ordering in expressions involving boson operators?

Normal ordering is a process used to rearrange boson operators such that all creation operators (\(a^\dagger\)) appear to the left of all annihilation operators (\(a\)). This is important because it ensures that vacuum expectation values are calculated correctly, avoiding infinities that can arise in quantum field theory calculations. The normal ordering of an operator \(O\) is denoted by \(:O:\).

Can you provide an example of a derived expression involving boson operators?

One common example is the derivation of the Hamiltonian for a simple harmonic oscillator in terms of boson operators. The Hamiltonian can be written as \( H = \hbar \omega (a^\dagger a + \frac{1}{2}) \), where \(\hbar\) is the reduced Planck constant and \(\omega\) is the angular frequency of the oscillator. This expression is derived using the commutation relations and the properties of the creation and annihilation operators.

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