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Quantum for Fusion

Quantum Phase Estimation for Energy Levels

Phase estimation extracts eigenvalues of a Hamiltonian to arbitrary precision, the fault-tolerant route to chemically accurate fusion-material energies.

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Reading energies from phases

Quantum phase estimation (QPE) is the algorithm that turns Hamiltonian time evolution into a number. If |psi> is an eigenstate of U = exp(-iHt) with eigenvalue exp(-i E t), QPE measures the phase E t and therefore the energy E. Unlike variational VQE, its precision improves systematically with more ancilla qubits rather than more optimization.

text
# QPE circuit sketch
1. prepare ancilla |0>^m and system state |psi> (overlap with eigenstate)
2. apply controlled-U^{2^k} for k = 0..m-1     (U = exp(-iHt))
3. inverse QFT on the ancilla register
4. measure ancilla -> binary fraction ~ (E t)/(2*pi)

# Precision:  eps ~ 2^{-m}  with m ancilla qubits
# Runtime per estimate:  O(1/eps) applications of U

Cost and preconditions

Chemical accuracy is the bar

For first-wall and blanket energetics the target is chemical accuracy, roughly 1 kcal/mol (about 1.6 milli-Hartree). Reaching that with QPE means m large enough that eps is well below that threshold, driving the logical-qubit and T-gate counts that define the fault-tolerant era.

text
chemical accuracy: eps ~ 1.6e-3 Hartree
=> m ~ log2( E_range / eps )  ancilla bits
=> controlled-U calls ~ O(1/eps) ~ hundreds to thousands per digit
# only tractable with error-corrected logical qubits

QPE is the destination, not a near-term tool. Kronos treats it as the reference algorithm behind resource estimates for a first-wall defect cluster and validates the full pipeline on tiny systems where classical exact diagonalization gives the ground truth. It relies on Hamiltonian simulation and qubitization as subroutines.

Content reviewed August 2026 · design-and-simulation stage