Boson operator algebra - unitary transformation
Clash Royale CLAN TAG#URR8PPP
up vote
1
down vote
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What is the simple way to evaluate
$$ e^i alpha n(n-1)a^dagger e^-i alpha n(n-1)$$
and
$$ e^i alpha n(n-1)a e^-i alpha n(n-1)$$
where $n=a^dagger a$ and $a$ and $a^dagger$ are the boson annihilation/creation operators for bosons and $alpha$ is a constant?
matrix-calculus noncommutative-algebra adjoint-operators matrix-exponential
add a comment |Â
up vote
1
down vote
favorite
What is the simple way to evaluate
$$ e^i alpha n(n-1)a^dagger e^-i alpha n(n-1)$$
and
$$ e^i alpha n(n-1)a e^-i alpha n(n-1)$$
where $n=a^dagger a$ and $a$ and $a^dagger$ are the boson annihilation/creation operators for bosons and $alpha$ is a constant?
matrix-calculus noncommutative-algebra adjoint-operators matrix-exponential
Out of curiosity, is there a physical interpretation of these operators? (I don't mean $n$, $a$, and $a^dagger$. I am curious about the two operators you are asking about.)
– Batominovski
Aug 1 at 16:59
Basically I am trying to rewrite the Hamiltonian of the Bose-Hubbard model in the rotating frame with the onsite interaction....so I have to transform the operators $a$ and $a^dagger$
– Galuoises
Aug 1 at 17:07
add a comment |Â
up vote
1
down vote
favorite
up vote
1
down vote
favorite
What is the simple way to evaluate
$$ e^i alpha n(n-1)a^dagger e^-i alpha n(n-1)$$
and
$$ e^i alpha n(n-1)a e^-i alpha n(n-1)$$
where $n=a^dagger a$ and $a$ and $a^dagger$ are the boson annihilation/creation operators for bosons and $alpha$ is a constant?
matrix-calculus noncommutative-algebra adjoint-operators matrix-exponential
What is the simple way to evaluate
$$ e^i alpha n(n-1)a^dagger e^-i alpha n(n-1)$$
and
$$ e^i alpha n(n-1)a e^-i alpha n(n-1)$$
where $n=a^dagger a$ and $a$ and $a^dagger$ are the boson annihilation/creation operators for bosons and $alpha$ is a constant?
matrix-calculus noncommutative-algebra adjoint-operators matrix-exponential
asked Aug 1 at 16:53
Galuoises
105
105
Out of curiosity, is there a physical interpretation of these operators? (I don't mean $n$, $a$, and $a^dagger$. I am curious about the two operators you are asking about.)
– Batominovski
Aug 1 at 16:59
Basically I am trying to rewrite the Hamiltonian of the Bose-Hubbard model in the rotating frame with the onsite interaction....so I have to transform the operators $a$ and $a^dagger$
– Galuoises
Aug 1 at 17:07
add a comment |Â
Out of curiosity, is there a physical interpretation of these operators? (I don't mean $n$, $a$, and $a^dagger$. I am curious about the two operators you are asking about.)
– Batominovski
Aug 1 at 16:59
Basically I am trying to rewrite the Hamiltonian of the Bose-Hubbard model in the rotating frame with the onsite interaction....so I have to transform the operators $a$ and $a^dagger$
– Galuoises
Aug 1 at 17:07
Out of curiosity, is there a physical interpretation of these operators? (I don't mean $n$, $a$, and $a^dagger$. I am curious about the two operators you are asking about.)
– Batominovski
Aug 1 at 16:59
Out of curiosity, is there a physical interpretation of these operators? (I don't mean $n$, $a$, and $a^dagger$. I am curious about the two operators you are asking about.)
– Batominovski
Aug 1 at 16:59
Basically I am trying to rewrite the Hamiltonian of the Bose-Hubbard model in the rotating frame with the onsite interaction....so I have to transform the operators $a$ and $a^dagger$
– Galuoises
Aug 1 at 17:07
Basically I am trying to rewrite the Hamiltonian of the Bose-Hubbard model in the rotating frame with the onsite interaction....so I have to transform the operators $a$ and $a^dagger$
– Galuoises
Aug 1 at 17:07
add a comment |Â
1 Answer
1
active
oldest
votes
up vote
1
down vote
accepted
You can evaluate them on states with definite particle number. Let $|krangle$ be a state such that $n|krangle=k|krangle$. Then
begineqnarray*
mathrm e^mathrm i alpha n(n-1)a^daggermathrm e^-mathrm i alpha n(n-1)|krangle
&=&
mathrm e^mathrm i alpha n(n-1)a^daggermathrm e^-mathrm i alpha k(k-1)|krangle
\
&=&
mathrm e^mathrm i alpha (k+1)ka^daggermathrm e^-mathrm i alpha k(k-1)|krangle
\
&=&
mathrm e^2mathrm i alpha ka^dagger|krangle
\
&=&
a^daggermathrm e^2mathrm i alpha n|krangle;.
endeqnarray*
Since $|krangle$ was arbitrary and the states with definite particle number span the state space, this implies
$$
mathrm e^mathrm i alpha n(n-1)a^daggermathrm e^-mathrm i alpha n(n-1)=a^daggermathrm e^2mathrm i alpha n;.
$$
Analogously, you can obtain
$$
mathrm e^mathrm i alpha n(n-1)amathrm e^-mathrm i alpha n(n-1)=amathrm e^-2mathrm i alpha(n-1);.
$$
1
Thank you so much! I was trying much more harder paths without any reasons
– Galuoises
Aug 2 at 12:34
add a comment |Â
1 Answer
1
active
oldest
votes
1 Answer
1
active
oldest
votes
active
oldest
votes
active
oldest
votes
up vote
1
down vote
accepted
You can evaluate them on states with definite particle number. Let $|krangle$ be a state such that $n|krangle=k|krangle$. Then
begineqnarray*
mathrm e^mathrm i alpha n(n-1)a^daggermathrm e^-mathrm i alpha n(n-1)|krangle
&=&
mathrm e^mathrm i alpha n(n-1)a^daggermathrm e^-mathrm i alpha k(k-1)|krangle
\
&=&
mathrm e^mathrm i alpha (k+1)ka^daggermathrm e^-mathrm i alpha k(k-1)|krangle
\
&=&
mathrm e^2mathrm i alpha ka^dagger|krangle
\
&=&
a^daggermathrm e^2mathrm i alpha n|krangle;.
endeqnarray*
Since $|krangle$ was arbitrary and the states with definite particle number span the state space, this implies
$$
mathrm e^mathrm i alpha n(n-1)a^daggermathrm e^-mathrm i alpha n(n-1)=a^daggermathrm e^2mathrm i alpha n;.
$$
Analogously, you can obtain
$$
mathrm e^mathrm i alpha n(n-1)amathrm e^-mathrm i alpha n(n-1)=amathrm e^-2mathrm i alpha(n-1);.
$$
1
Thank you so much! I was trying much more harder paths without any reasons
– Galuoises
Aug 2 at 12:34
add a comment |Â
up vote
1
down vote
accepted
You can evaluate them on states with definite particle number. Let $|krangle$ be a state such that $n|krangle=k|krangle$. Then
begineqnarray*
mathrm e^mathrm i alpha n(n-1)a^daggermathrm e^-mathrm i alpha n(n-1)|krangle
&=&
mathrm e^mathrm i alpha n(n-1)a^daggermathrm e^-mathrm i alpha k(k-1)|krangle
\
&=&
mathrm e^mathrm i alpha (k+1)ka^daggermathrm e^-mathrm i alpha k(k-1)|krangle
\
&=&
mathrm e^2mathrm i alpha ka^dagger|krangle
\
&=&
a^daggermathrm e^2mathrm i alpha n|krangle;.
endeqnarray*
Since $|krangle$ was arbitrary and the states with definite particle number span the state space, this implies
$$
mathrm e^mathrm i alpha n(n-1)a^daggermathrm e^-mathrm i alpha n(n-1)=a^daggermathrm e^2mathrm i alpha n;.
$$
Analogously, you can obtain
$$
mathrm e^mathrm i alpha n(n-1)amathrm e^-mathrm i alpha n(n-1)=amathrm e^-2mathrm i alpha(n-1);.
$$
1
Thank you so much! I was trying much more harder paths without any reasons
– Galuoises
Aug 2 at 12:34
add a comment |Â
up vote
1
down vote
accepted
up vote
1
down vote
accepted
You can evaluate them on states with definite particle number. Let $|krangle$ be a state such that $n|krangle=k|krangle$. Then
begineqnarray*
mathrm e^mathrm i alpha n(n-1)a^daggermathrm e^-mathrm i alpha n(n-1)|krangle
&=&
mathrm e^mathrm i alpha n(n-1)a^daggermathrm e^-mathrm i alpha k(k-1)|krangle
\
&=&
mathrm e^mathrm i alpha (k+1)ka^daggermathrm e^-mathrm i alpha k(k-1)|krangle
\
&=&
mathrm e^2mathrm i alpha ka^dagger|krangle
\
&=&
a^daggermathrm e^2mathrm i alpha n|krangle;.
endeqnarray*
Since $|krangle$ was arbitrary and the states with definite particle number span the state space, this implies
$$
mathrm e^mathrm i alpha n(n-1)a^daggermathrm e^-mathrm i alpha n(n-1)=a^daggermathrm e^2mathrm i alpha n;.
$$
Analogously, you can obtain
$$
mathrm e^mathrm i alpha n(n-1)amathrm e^-mathrm i alpha n(n-1)=amathrm e^-2mathrm i alpha(n-1);.
$$
You can evaluate them on states with definite particle number. Let $|krangle$ be a state such that $n|krangle=k|krangle$. Then
begineqnarray*
mathrm e^mathrm i alpha n(n-1)a^daggermathrm e^-mathrm i alpha n(n-1)|krangle
&=&
mathrm e^mathrm i alpha n(n-1)a^daggermathrm e^-mathrm i alpha k(k-1)|krangle
\
&=&
mathrm e^mathrm i alpha (k+1)ka^daggermathrm e^-mathrm i alpha k(k-1)|krangle
\
&=&
mathrm e^2mathrm i alpha ka^dagger|krangle
\
&=&
a^daggermathrm e^2mathrm i alpha n|krangle;.
endeqnarray*
Since $|krangle$ was arbitrary and the states with definite particle number span the state space, this implies
$$
mathrm e^mathrm i alpha n(n-1)a^daggermathrm e^-mathrm i alpha n(n-1)=a^daggermathrm e^2mathrm i alpha n;.
$$
Analogously, you can obtain
$$
mathrm e^mathrm i alpha n(n-1)amathrm e^-mathrm i alpha n(n-1)=amathrm e^-2mathrm i alpha(n-1);.
$$
edited Aug 1 at 18:11
answered Aug 1 at 17:41
joriki
164k10179328
164k10179328
1
Thank you so much! I was trying much more harder paths without any reasons
– Galuoises
Aug 2 at 12:34
add a comment |Â
1
Thank you so much! I was trying much more harder paths without any reasons
– Galuoises
Aug 2 at 12:34
1
1
Thank you so much! I was trying much more harder paths without any reasons
– Galuoises
Aug 2 at 12:34
Thank you so much! I was trying much more harder paths without any reasons
– Galuoises
Aug 2 at 12:34
add a comment |Â
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Out of curiosity, is there a physical interpretation of these operators? (I don't mean $n$, $a$, and $a^dagger$. I am curious about the two operators you are asking about.)
– Batominovski
Aug 1 at 16:59
Basically I am trying to rewrite the Hamiltonian of the Bose-Hubbard model in the rotating frame with the onsite interaction....so I have to transform the operators $a$ and $a^dagger$
– Galuoises
Aug 1 at 17:07