Interpreting operators in second quantization

[Niles]

Hi guys

When working with operators in second quantization, I always imagine

<br /> c^\dagger_ic_j<br />

as denoting the "good old" matrix element \left\langle {i}<br /> \mathrel{\left | {\vphantom {i j}}<br /> \right. \kern-\nulldelimiterspace}<br /> {j} \right\rangle. But how should I interpret an operator given by e.g.

<br /> c^\dagger_ic_j^\dagger?<br />

 

[sokrates]

Wouldn't it be the good old product of two bras?

 

[saaskis]

In single-particle QM, one can write the Hamiltonian as

<br /> H=\sum H_{ij} |i \rangle \langle j|<br />.

In second quantization, the single-particle operator is

<br /> H&#039;=\sum H_{ij} c_i^{\dagger} c_j,<br />

so one can make the identification c_j \leftrightarrow \langle j|, as long as the Hilbert space is simply the space of single particles. Both Hamiltonians H and H' have, after all, the same matrix elements in this space.

The operator c^\dagger_i c_j^\dagger, on the other hand, does not even conserve the number of particles, so in my opinion, it makes no sense to identify the operator as any combination of bras and kets.

 

[Physics Monkey]

Hi Niles,

It wouldn't make sense to interpret c_i^+ c_j as the matrix element \langle i | j \rangle since one is an operator and the other is a number. Indeed, if the single particle states i and j are orthogonal then the matrix element is just zero, but the operator you wrote is definitely not zero. The meaning of c_i^+ c_j is that is turns the state | j \rangle into the state | i \rangle. It destroys a particle in the single particle state labeled by j and creates a particle in the single particle state labeled by i. Similarly, c^+_i c_j^+ destroys no particles and creates a particle in state i and a particle in state j.

These kinds of operators are relevant in superconductors, for example, where the particle number can fluctuate coherently.

 

[George Jones]

The meaning of c_i^+ c_j is that is turns the state | j \rangle into the state | i \rangle. It destroys a particle in the single particle state labeled by i and creates a particle in the single particle state labeled by i. Similarly, c^+_i c_j^+ destroys no particles and creates a particle in state i and a particle in state j.

I'm a little confused. Have you treated the c's as a's?

 

[Physics Monkey]

I'm a little confused. Have you treated the c's as a's?

Sorry, what are the "a's"?

 

[SpectraCat]

Sorry, what are the "a's"?

By convention, the "c's" are the creation/annihilation operators for *fermions*. The "a's" are the analogous operators for bosons. The c's change occupation numbers of fermions in a Fock state vector ... due to the PEP, those occupation numbers can only ever be 0 or 1.

The a's change occupation numbers for bosons, which do not have the PEP restrictions, and so can assume arbitrarily large values (e.g. high-photon density in an intense EM field).

EDIT: So, I guess George Jones' confusion came from the fact that if you apply a c⁺ creation operator twice to the same state, it simply returns that state to its original configuration with no net effect. Therefore, you cannot say (as you did) that applying the c_i⁺ operator will create a particle in the ith state, because if that state is initially occupied, then it will actually annihilate the particle in that state.

 

[Physics Monkey]

By convention, the "c's" are the creation/annihilation operators for *fermions*. The "a's" are the analogous operators for bosons. The c's change occupation numbers of fermions in a Fock state vector ... due to the PEP, those occupation numbers can only ever be 0 or 1.

I suppose this is a fairly common convention, but it wasn't clear to me that the OP was interested only in fermions.

EDIT: So, I guess George Jones' confusion came from the fact that if you apply a c⁺ creation operator twice to the same state, it simply returns that state to its original configuration with no net effect. Therefore, you cannot say (as you did) that applying the c_i⁺ operator will create a particle in the ith state, because if that state is initially occupied, then it will actually annihilate the particle in that state.

Perhaps this is what George was talking about. Of course you're right that if I apply the fermionic creation operator to an already filled state then I don't add a fermion. However, I think you meant to say that applying the same fermionic creation operator twice annihilates the state (rather than returning the state to its original form) I was implicitly thinking about adding particles to the vacuum, but thanks for clarifying this point.

 

[SpectraCat]

I suppose this is a fairly common convention, but it wasn't clear to me that the OP was interested only in fermions.



Perhaps this is what George was talking about. Of course you're right that if I apply the fermionic creation operator to an already filled state then I don't add a fermion. However, I think you meant to say that applying the same fermionic creation operator twice annihilates the state (rather than returning the state to its original form) I was implicitly thinking about adding particles to the vacuum, but thanks for clarifying this point.

Yes, you are correct ... I was thinking that the application of the c_i⁺ operator just destroyed the fermion in the ith-state, but of course it must annihilate the entire Fock state according to the PEP. Thanks for catching that! (it's been a while since I had to think about this stuff, and I am a bit rusty.)