In statistical models of barren plateaus, any two Pauli observables have non-zero regions whose overlap is exponentially smaller than each region, a phenomenon the paper calls anti-concentration.
Quantum State Preparation with Optimal Circuit Depth: Implementations and Applications
1 Pith paper cite this work. Polarity classification is still indexing.
abstract
Quantum state preparation is an important subroutine for quantum computing. We show that any $n$-qubit quantum state can be prepared with a $\Theta(n)$-depth circuit using only single- and two-qubit gates, although with a cost of an exponential amount of ancillary qubits. On the other hand, for sparse quantum states with $d\geqslant2$ non-zero entries, we can reduce the circuit depth to $\Theta(\log(nd))$ with $O(nd\log d)$ ancillary qubits. The algorithm for sparse states is exponentially faster than best-known results and the number of ancillary qubits is nearly optimal and only increases polynomially with the system size. We discuss applications of the results in different quantum computing tasks, such as Hamiltonian simulation, solving linear systems of equations, and realizing quantum random access memories, and find cases with exponential reductions of the circuit depth for all these three tasks. In particular, using our algorithm, we find a family of linear system solving problems enjoying exponential speedups, even compared to the best-known quantum and classical dequantization algorithms.
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Statistical models of barren plateaus and anti-concentration of Pauli observables
In statistical models of barren plateaus, any two Pauli observables have non-zero regions whose overlap is exponentially smaller than each region, a phenomenon the paper calls anti-concentration.