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Quantum for Fusion

Qubitization and Linear Combination of Unitaries

Block-encoding and qubitization give near-optimal Hamiltonian simulation scaling, the fault-tolerant route Kronos targets for materials.

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Beyond product formulas

Product formulas like Trotter are simple but scale poorly in the number of Hamiltonian terms and required precision. The modern approach writes H as a linear combination of unitaries (LCU) and builds a block encoding: a larger unitary that contains H/alpha in a corner, accessed through ancilla qubits.

text
H = sum_k c_k U_k          # LCU: U_k unitary (Pauli strings), c_k >= 0
alpha = sum_k c_k          # the '1-norm' of the Hamiltonian

# PREPARE:  |0> -> sum_k sqrt(c_k/alpha) |k>
# SELECT :  |k>|psi> -> |k> U_k |psi>
# Block encoding U_H = PREPARE^dag . SELECT . PREPARE
#   <0|_anc U_H |0>_anc = H / alpha

Qubitization and the query cost

Iterating the block encoding with reflections (the Szegedy-style walk operator) 'qubitizes' the problem: the eigenphases of the walk operator encode arccos of the eigenvalues of H/alpha. Simulating for time t then costs a number of queries that is near-optimal:

text
query_cost(t, eps)  =  O( alpha*t  +  log(1/eps) )
#   alpha  = Hamiltonian 1-norm (the effective 'block-encoding cost')
#   t      = evolution time,  eps = target error
# This is optimal in t and in eps (additive log term) -- unlike Trotter's
# polynomial-in-1/eps scaling.

Why it matters for first-wall chemistry

Kronos treats qubitization as the reference architecture for future materials simulation: it is what our fault-tolerant resource estimates assume when counting logical qubits and T gates for a tungsten defect cluster. It does not run on any device we can access today, and we say so plainly.

Content reviewed August 2026 · design-and-simulation stage