Comments (3)
I'm going to be taking this issue as I read over some of Minnich's papers.
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The tale is more complicated than I first thought. They used different approximations in their quantum simulator compared to their noiseless simulator. The algorithm they used on their noiseless system involves non-Trotterized exponentials.
I'm still not sure the QForte implementation matches the original implementation. The basic structure of a single QITE step is to loop over all terms in the Hamiltonian, compute the step for each, and update the wavefunction gate for each. In the QForte loop, we have a "step-merged" version, where we use the entire Hamiltonian, Trotterizing when necessary.
@nstair, does this sound right to you? If we're agreed about the theory, I can implement the non-step-merged version, keeping the step-merged version.
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@JonathonMisiewicz you are correct. The current implementation in QForte is closer to the step-merged version. You are welcome to implement the non-step-merged version, but it becomes challenging to rationalize 'inexact QITE' for non k-local hamiltonians.
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Related Issues (20)
- Auto-Documentation
- Build More Documentation
- Use Properties in Molecule
- Simplify System Factory
- Replace `_pool` with `_qubit_pool`
- Combine Amplitudes and Operator Pool HOT 1
- Remove `lib` HOT 1
- Synchronize `_pool_obj` and `_pool`
- Don't FCI by Default
- Frozen QPE HOT 2
- Function Renamings
- QKD Cleanup
- Decouple Reading From File from Molecule
- Generalize `_Uprep` HOT 1
- Optimization with Adam Optimizer
- Poor Installation Instruction HOT 1
- Autotests HOT 1
- Mysterious comment about external molecule building with point group symmetry
- difficult installation error
- Profile `gate`
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