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H2/STO-3G should become a 1-qubit problem, and the data in Table I of the paper can be reproduced. But we can explore far larger systems that are closer to what classical quantum chemists are interested in.
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However, I am still having issues with Bravyi-Kitaev. My strategy has been to enumerate all bit strings with NELEC ones set - these form the basis for my Hamiltonian subspace that I will diagonalize. As stated this works for JW, however for BK I build up the occupation -> bravyi-kitaev basis transformation (Eq 50 of tapering qubits) and apply it to all NELEC eigenstates to produce corresponding BK eigenstates. I then build up the Hamiltonian matrix elements in this basis and diagonalize.
This works for problems that have NQubits as a power of 2. It does not work for problems that have NQubits not a power of 2 (for example H2 6-31++G, NQubits=12). Seeley, Love paper says in these cases to take the submatrix of the next largest BK transformation matrix 2^m > M and pull out the submatrix that corresponds to the number of orbitals you have. So clearly something wrong is happening there that I can't figure out.
To test the matrix construction part, I have brute-force built up the entire matrix for the H2 6-31++G 12 qubit problem and diagonalized that, and received the correct ground state energy.
So something is missing in my understanding of the Occupation -> BK basis transformation when NQubits is not a power of 2.
Thanks Alex,
It is already nice that it's working for JW, though JW for Li2 in an aug-cc-pCV6Z basis set already has more than 1000 spin orbitals, and will therefore have 1000-local terms, whereas BK is O(log(M))-local and may therefore only have log_2(1000) = 10-local terms for the same molecule.
10-local seems much better than 1000-local, so I do think there's value to doing the tapering in the BK picture, since BK would probably be used for most practical applications.
H2/STO-3G should become a 1-qubit problem, and the data in Table I of the paper can be reproduced. But we can explore far larger systems that are closer to what classical quantum chemists are interested in.
The text was updated successfully, but these errors were encountered: