Alternative adiabatic quantum dynamics with algorithmic applications
Pith reviewed 2026-06-29 06:30 UTC · model grok-4.3
The pith
Alternative processes achieve adiabatic tracking on gate-based quantum computers without Hamiltonian simulation.
A machine-rendered reading of the paper's core claim, the machinery that carries it, and where it could break.
Core claim
Several alternative processes achieve the same goal as adiabatic evolution but are directly implementable on gate-based quantum computers without the overhead of simulating time-dependent Hamiltonian evolution. A general framework derives adiabatic theorems for these processes. The framework yields various algorithms for the Quantum Linear Systems Problem with optimal scaling in the condition number, one of which is a randomised version of the discrete adiabatic algorithm, and it also reproduces Trotterisation results in a randomised setting with asymptotically better fidelity-based error bounds.
What carries the argument
General framework for deriving adiabatic theorems for alternative discrete processes that replace time-dependent Hamiltonian evolution while preserving eigenstate tracking.
If this is right
- QLSP algorithms achieve optimal scaling with the condition number.
- A randomised version of the discrete adiabatic algorithm solves QLSP.
- Trotterisation can be performed inside the framework in a randomised setting.
- Trotter error bounds measured in fidelity are asymptotically tighter than conventional bounds.
Where Pith is reading between the lines
- The discrete processes may reduce the resources needed to run adiabatic-style algorithms on near-term gate hardware.
- The framework could be used to analyse other gate-based quantum algorithms that currently rely on adiabatic theorems.
- Randomised variants might tolerate certain forms of noise better than their deterministic counterparts.
Load-bearing premise
The alternative discrete processes preserve the required eigenstate tracking property through the new framework when realized with standard gates.
What would settle it
A direct simulation or hardware run of one proposed process on a small QLSP instance that shows the final state fidelity falls below the bound predicted by the framework's adiabatic theorem.
Figures
read the original abstract
In adiabatic quantum computing the aim is to track an eigenstate as the Hamiltonian changes. In the usual setup this is achieved using the natural time-dependent Hamiltonian evolution of the system and the main technical tool is the adiabatic theorem. We propose several alternative processes that achieve the same goal, but can easily be implemented on a gate-based quantum computer without the overhead of simulating time-dependent Hamiltonian evolution. We give a general framework for deriving `adiabatic' theorems for these processes. As an application, we give various algorithms for solving the Quantum Linear Systems Problem (QLSP) with optimal scaling in the condition number. One of these algorithms was previously developed in [Cunningham, Roland 2024] and another can be seen as a randomised version of the discrete adiabatic algorithm of [Costa et al. 2022]. We also describe versions of Trotterisation in our framework, which allows several results from [An et al. 2025] to be reproduced in a randomised setting. In particular, bounds on the Trotter error in terms of the fidelity are obtained that are asymptotically better than the standard bounds.
Editorial analysis
A structured set of objections, weighed in public.
Referee Report
Summary. The manuscript proposes several alternative dynamical processes to standard adiabatic quantum computing that track eigenstates without requiring simulation of continuous time-dependent Hamiltonians, enabling direct implementation on gate-based quantum computers. It develops a general framework for deriving adiabatic theorems applicable to these processes. As an application, the framework yields QLSP algorithms with optimal scaling in the condition number, including a randomized version of the discrete adiabatic algorithm from Costa et al. (2022) and a reproduction of results from Cunningham and Roland (2024). The paper also presents randomized Trotterization variants that reproduce results from An et al. (2025) with asymptotically improved fidelity-based error bounds.
Significance. If the central claims hold, the work offers a useful generalization of adiabatic methods to discrete gate-based settings, removing simulation overhead while preserving tracking guarantees. The explicit reproduction of prior QLSP and Trotter results in a randomized context, together with improved error bounds, strengthens the contribution by providing both algorithmic alternatives and tighter analyses. The absence of free parameters or circular definitions in the high-level claims, as noted in the abstract, supports the framework's potential utility for future algorithm design.
minor comments (1)
- The abstract references results from An et al. (2025); ensure the reference list includes the full citation details and that the manuscript clarifies the precise overlap with the reproduced bounds.
Simulated Author's Rebuttal
We thank the referee for their thorough and positive review, which accurately captures the manuscript's contributions to alternative adiabatic processes, QLSP algorithms, and randomized Trotterization. We are pleased by the recommendation to accept.
Circularity Check
No significant circularity identified
full rationale
The paper presents a new general framework for alternative adiabatic processes implementable via standard gates, with applications to QLSP algorithms of optimal scaling. The self-reference to the authors' prior 2024 QLSP result is an acknowledgment that one listed algorithm was previously developed elsewhere; it does not serve as a load-bearing premise for the framework itself or force any new derivation by construction. No self-definitional equations, fitted inputs renamed as predictions, uniqueness theorems imported from the same authors, or ansatzes smuggled via citation are present. The derivation chain remains independent of the cited prior work.
Axiom & Free-Parameter Ledger
axioms (1)
- domain assumption Alternative discrete processes can track an eigenstate of a changing Hamiltonian in a manner analogous to the standard adiabatic theorem.
Reference graph
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off-diagonal
eX=P eXQ+Q eXP. We can express property (2) by saying that eXis “off-diagonal”. Proof.(1) The proof is a straightforward verification of the proposed solution: [A, eX] = 1 2πi I Γ A, RA(z)XR A(z) dz(99) = 1 2πi I Γ RA(z)XR A(z), z1−A dz(100) = 1 2πi I Γ RA(z)X−XR A(z) dz(101) = 1 2πi I Γ RA(z) dz X−X 1 2πi I Γ RA(z) dz (102) =P X−XP= [P, X].(103) (2) Sinc...
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fP ′[P ′, P] +fP ′′ = fP ′′ + (Q−P) ^[A′,fP ′] +QP ′fP ′Q−P P ′fP ′P; 2.P ′′ = fA′′ + (Q−P) 2(P ′)2 + ^[A′, P ′]
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[26]
fP ′′ = ffA′′ + (Q−P) ^^[A′, P ′]. Proof.(1) Proposition 25 gives the expansion fP ′′ = fP ′′ + (Q−P) P ′fP ′ +fP ′P ′ + ^[A′,fP ′] (148) = fP ′′ + (Q−P) ^[A′,fP ′] +Q P ′fP ′ +fP ′P ′ Q−P P ′fP ′ +fP ′P ′ P,(149) which can be added to fP ′[P ′, P] =P fP ′P ′P−Q fP ′P ′Q.(150) to get the result. (2) SinceP ′′ =fH ′′ , the result follows from Proposition 2...
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[27]
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[28]
IfX 0,0 = 0 =X 1,1, then ∥X∥ ≤max{∥X 0,1∥,∥X 0,1∥}.(158)
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[29]
IfX 0,0 = 0 =X 1,0, then ∥X∥ ≤ q ∥X0,1∥2 +∥X 1,1∥2.(159)
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[30]
If∥X 0,1∥=∥X 1,0∥, then ∥X∥ ≤ ∥X0,0∥+∥X 1,1∥ 2 + 1 2 q ∥X0,0∥ − ∥X1,1∥ 2 + 4∥X0,1∥2.(160)
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SupposeAis differentiable,Γ(s)is continuous and the part ofσ(A)insideΓconsists ofm eigenvalues
IfX 0,0 = 0and∥X 0,1∥=∥X 1,0∥, then ∥X∥ ≤ ∥X1,1∥ 2 + r ∥X1,1∥2 4 +∥X 0,1∥2.(161) Proposition 29.LetHbe a Hilbert space,A(s)a bounded normal operator onH,X(s)a bounded operator onHandΓ(s)a closed simple curve that does not intersect the spectrum ofA(s), for all s∈[0,1]. SupposeAis differentiable,Γ(s)is continuous and the part ofσ(A)insideΓconsists ofm eige...
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