Types of Postprocessing¶
Solutions obtained from a D-Wave quantum processing unit (QPU) can be postprocessed to achieve higher quality.
When submitting a problem to the QPU, users choose from:
- No postprocessing (default)
- Optimization postprocessing
- Sampling postprocessing
For optimization problems, the goal is to find the state vector with the lowest energy. For sampling problems, the goal is to produce samples from a specific probability distribution. In both cases, a logical graph structure is defined and embedded into the QPU’s Chimera topology. Postprocessing methods are applied to solutions defined on this logical graph structure.
The flow of integrated postprocessing is shown in Figure 58.
The goal of optimization postprocessing is to obtain a set of samples with lowest energy on a graph \(G\). For simplicity of discussion, assume that \(G\) is a logical graph. Pseudocode for optimization postprocessing is shown below. The postprocessing method works by performing local updates to the state vector \(S\) based on low treewidth graphs. Specifically, the DecomposeGraph function uses a set of algorithms based on the minimum-degree [Markowitz1957] heuristic to decompose graph \(G\) into several low treewidth subgraphs that cover the nodes and edges of \(G\). The SolveSubgraph function is then used to update the solution on each subgraph to obtain a locally optimal solution \(s'\). SolveSubgraph is an exact solver for low treewidth graphs based on belief propagation on junction trees [Jensen1990].
In sampling mode, the goal of postprocessing is to obtain a set of samples that correspond to a target Boltzmann distribution with inverse temperature \(\beta\) defined on the logical graph \(G\). The pseudocode for sampling postprocessing is shown below. As with optimization postprocessing, the graph \(G\) is decomposed into low treewidth subgraphs \(G'\) that cover \(G\). On each subgraph, the state variables \(S\) obtained from the QPU are then updated using the SampleSubgraph function to match the exact Boltzmann distribution conditioned on the states of the variables outside the subgraph. Users can set the number of subgraph update iterations \(n\); the choice of \(\beta\) is also determined by the user. Heuristically, this inverse temperature depends on model parameters in the Hamiltonian. As a general rule, \(\beta\) should be set to a value close to an inverse temperature corresponding to raw QPU samples. Some variation from a classical Boltzmann distribution is expected in postprocessed samples. See Sampling Tests and Results for discussion.