Fermionic occupation operator and nearest neighbor Fermionic hopping interaction as a qubit operator

How to express Fermionic occupation operator $$(\hat{a}_j^\dagger\hat{a}_j)$$ and nearest neighbor Fermionic hopping interaction ($$H_h= J\sum_{i=1}\hat{a}_i^\dagger \hat{a}_{i+1}+\hat{a}_{i+1}^\dagger \hat{a}_{i})$$ as a qubit operators.

• Is this a one-dimensional chain (when you say "nearest neighbor")? Mar 12 '21 at 22:04
• @NorbertSchuch yes Mar 12 '21 at 22:05
• Then (to add to the answer below), the Jordan-Wigner transformation is just what you want: If will yield a NN qubit Hamiltonian. (So you can neglect the O(n))-local in the answer below.) Mar 12 '21 at 22:15
• Could help to add this to the question! Mar 12 '21 at 22:48
• @gIS what did you like about Norbert's answer more than mine? Mar 13 '21 at 0:16

• The oldest and most commonly known way is the Jordan-Wigner transformation. The qubit operators will be $$\mathcal{O}(N)$$-local for $$N$$ occupiable orbitals.
• A significantly more complicated way is the Bravyi-Kitaev transformation for which the qubit operators will be $$\mathcal{O}(\log N)$$-local.
• There's many other ways, but the above two are by far the most important to know in the early stages of your project.

You can simply transform creation and annihilation operators into "occupied" and "unoccupied" operators: But you have to also make sure the wavefunction satisfies the anti-symmetric property for fermions, so you have to add strings of $$Z$$ operators to count the number -1's (this is the Jordan-Wigner transformation which is $$n-local$$): The occupation operator in the first part of your question is simply: To get the other operators in your question, you can just substitute the $$a_j$$ and $$a^\dagger_j$$ expression from above.

I used this source to get the equations.

Note that if your Hamiltonian has only nearest-neighbor couplings, then the issue of the JW transformation being $$N$$-local can be mitigated due to cancellation when multiplying (for example) $$a_j$$ with $$a_{j+1}^\dagger$$, as noted in Norbert Schuch's comment here.

• If you have n orbitals and you get something O(n)-local, isn't that as non-local as it gets? Mar 12 '21 at 22:16
• @NorbertSchuch yea the JW transformation is significantly non-local. The Bravyi-Kitaev transformation is better if low locality is important for the user's application. Significantly more complicated though. Mar 12 '21 at 22:24
• Well, the user is asking about a 1D spin chain with NN interaction, so JW just seems perfect. Mar 12 '21 at 22:47
• I know that the clarification came after your answer, since I asked for it. I am just pointing out that in the case of the question, JW is best. -- To answer your question how NN helps, note that the NN Hamiltonian only involves on-site potentials and NN hopping, in which case after the JW-trafo you get local spin Hamiltonians because the non-local terms in the $a_{i}$ and the $a_{i+1}^\dagger$ cancel (a well known fact in CM physics used to e.g. conversely solve the 1D quantum Ising model or 2D classical Ising model!). Mar 12 '21 at 23:13
• @NorbertSchuch just click on the time stamp next to your name, and then you have the URL for linking the comment. Mar 12 '21 at 23:34

Use the Jordan-Wigner transformation. For a 1D chain with NN interaction it will yield a spin Hamiltonian with NN interaction (specifically, the hopping will map to a XX term and the on-site term to a Z term). (In fact, part of this mapping is even given on the German Wikipedia site on the topic.)

On the other hand, if you don't want to put this on a quantum computer but solve it, you should stay in the fermionic picture (or map the spin problem to a fermionic one). This is how one solves e.g. the 1D quantum transverse field Ising model.

Finally, if you don't have 1D local Hamiltonians, considering other transformation which keep locality (or few-bodiness of the terms), such as the one mentioned in the other answer, can make sense (in particular since local spin models are easier to simulate than those with non-local and in particular many-body interaction).