Pillar B · State as of 2026-09-15

What is HHL and why did its fine print kill so many claims?

HHL (Harrow–Hassidim–Lloyd, Phys. Rev. Lett. 103, 150502, 2009) is a quantum algorithm that prepares a quantum state encoding the solution of a linear system in time polylogarithmic in the dimension of the system — under four conditions its fine print attaches: fast state loading, efficient simulation of the matrix, a small condition number, and settling for samples instead of the full solution vector. As of September 15, 2026 that fine print is the story: the 2014–2016 wave of quantum machine-learning claims built on HHL was largely dequantized by classical algorithms (Tang 2018 and successors), and the largest HHL application ever run on quantum hardware is an 8×8 system (JPMorganChase on Quantinuum, Sci. Rep. 2024). Rosetta Quantum reads the fine print line by line.
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State as of: 2026-09-15
Rosetta QuantumQUANTUM VERIFICATION LEDGERPILLAR B — DICTIONARY2026-09-15HHL: the algorithmwhose fine printkilled the claims8×8largest HHL application ever run on hardwareJPMorganChase on Quantinuum (Sci Rep, 2024)2×220138×820242^ntheoryrosettaquantum.com/blograw, reproducible data · sources below

Status as of: September 15, 2026. This is a dictionary entry with a body count. HHL — the Harrow–Hassidim–Lloyd algorithm for linear systems (Phys. Rev. Lett. 103, 150502, 2009) — carries the most famous fine print in quantum computing: four conditions attached to its exponential speedup. Between 2014 and 2016 a wave of quantum machine-learning claims was built on top of it; between 2018 and 2022, classical «dequantization» algorithms took most of that wave down. Rosetta Quantum files the algorithm, the four conditions, and the scoreboard — every number with its source.

What does HHL actually do?

It prepares a quantum state — not a spreadsheet of numbers. Given a linear system A·x = b, the algorithm of Harrow, Hassidim and Lloyd (posted November 2008 as arXiv:0811.3171; published in Phys. Rev. Lett. 103, 150502, 2009) produces a quantum state |x⟩ proportional to the solution A⁻¹|b⟩, using a circuit whose size grows only polylogarithmically with the dimension N of the system — for the state-preparation task, exponentially better in N than writing out all N entries. Its engine is quantum phase estimation, the subroutine Rosetta filed yesterday in the QPE entry.

Three structural facts frame everything below:

What exactly is the fine print?

Four conditions, spelled out in Scott Aaronson's 2015 commentary «Read the fine print» (Nat. Phys. 11, 291–293; full technical version):

  1. Loading. The input vector b must become the quantum state |b⟩ quickly — which requires either an explicit formula for its entries or a quantum RAM. QRAM at useful scale does not exist as deployed hardware; Rosetta filed that bottleneck separately in the QRAM entry.
  2. Simulation. The computer must be able to apply e^(−iAt) efficiently — true when A is sparse or otherwise structured; false in general.
  3. Conditioning. The runtime grows roughly linearly with the condition number κ (Aaronson 2015). If κ grows polynomially with N, the exponential speedup is gone.
  4. Readout. The output is the state |x⟩. You may sample from it or estimate observables ⟨x|M|x⟩; extracting the concrete entries of x generally costs of order N repetitions (Aaronson 2015).
HHL — THE PROMISE vs THE FINE PRINTleft: proved properties · right: the four conditions attachedPROVED (ON PAPER)runtime in dim Npoly(log N)hardness classBQP-completeprecision (2017)log(1/ε)κ scaling (2022)optimalstate-prep (2026)Θ(1/√p)THE FINE PRINT (×4)input |b⟩ loadingneeds QRAMmatrix A accesssparsecondition numbersmall κoutput is |x⟩a statereading all of x≈N runssources: HHL 2009 · Aaronson 2015 · CKS 2017 · Costa 2022 · Low & Su 2026every caveat waived in 2014–2016 became a fallen claim by 2022

None of this is a scandal, and none of it was hidden — the caveats are in the 2009 paper itself. The scandal, where there was one, was downstream: applications that quietly waived one condition or another and advertised the headline speedup anyway.

Which claims did the fine print kill?

The wave that fell was quantum machine learning, 2014–2016: quantum PCA, quantum support-vector machines, and the Kerenidis–Prakash quantum recommendation-systems algorithm (arXiv:1603.08675, 2016), all built on HHL-style linear algebra. In July 2018, Ewin Tang showed a classical sampling algorithm that matches the recommendation-systems speedup up to polynomial factors (arXiv:1807.04271) — the claimed exponential advantage evaporated. The same «quantum-inspired» toolkit then dequantized quantum PCA and supervised clustering (arXiv:1811.00414, 2018) and low-rank matrix inversion itself (Gilyén, Lloyd and Tang, arXiv:1811.04909, 2018; generalized into a full framework by Chia et al., J. ACM, 2022).

The pattern is exact, and it is the reason this entry exists: every dequantized claim had waived part of the fine print — almost always by assuming low-rank data. Low rank is precisely the regime where a classical computer can imitate quantum access by clever sampling; Tang's own heuristic is that low-dimensional linear algebra «likely can be dequantized», while the genuinely high-dimensional sparse regime is where a quantum speedup can survive (Tang, overview, 2019). Rosetta published the full autopsy of that episode in the dequantization entry and the machine-learning verdict in is quantum useful for ML; this post files the algorithm those claims were built on.

Claim built on HHL Year What happened Status, Sep 2026 Source
Quantum recommendation systems (Kerenidis–Prakash) 2016 classical algorithm matches it up to polynomial factors (Tang, jul-2018) dequantized arXiv:1807.04271
Quantum PCA / supervised clustering 2014 dequantized in the claimed low-rank regime (Tang, nov-2018) dequantized arXiv:1811.00414
Low-rank linear systems / regression via HHL 2009–2018 quantum-inspired low-rank inversion (GLT 2018; framework Chia et al.) dequantized arXiv:1811.04909 · J. ACM 2022
Quantum SVM / least-squares QML 2014 low-rank kernel regime falls under the same framework; no end-to-end advantage shown on any dataset no advantage demonstrated J. ACM 2022 · Rosetta #12
Sparse, high-rank, well-conditioned systems open no dequantization known; no end-to-end demonstration either open — theory only Tang 2019 · Aaronson 2015

What survives in September 2026?

The theorem survives intact — what died was a marketing shortcut. What remains standing, with sources:

What has not happened, in the future tense it deserves: an end-to-end HHL advantage on a real dataset — load, solve, read out, beat the best classical pipeline at equal budget — will have to be demonstrated; as of September 15, 2026 no such demonstration exists in the public record, and HHL end-to-end is accordingly absent from Rosetta's list of problems with proven quantum advantage. Rosetta has not run HHL on its own bench either — our ledger records zero advantaged solves involving HHL, ours or anyone's — so the verdict above rests on the public record, not on house data.

What has actually run on hardware?

Dimension 2 in 2013; dimension 8 in 2024. The first experimental demonstrations solved 2×2 systems on photonic processors (Cai et al., Phys. Rev. Lett. 110, 230501, 2013). Eleven years later, the record application demonstration is the hybrid HHL++ run by JPMorganChase researchers on Quantinuum H-series trapped-ion hardware: 4×4 portfolio-optimization systems, a scaling study at 8×8, two-qubit gate depth up to 291, and a median degradation of 4.17% versus noiseless simulation — self-described as «the largest experimental demonstrations of HHL for an application to date» (Sci. Rep. 14, 20610, sep-2024). Fifteen years after the paper, the measured frontier of the algorithm with the exponential promise is an 8×8 matrix. That is not an insult; it is the honest scale of early fault-tolerant-adjacent hardware — and it is the number that belongs on the cover.

THE FINE-PRINT TIMELINE: 2008 → 2026algorithm, claims wave, counterattack — every rung sourced in the post2008-11HHLlinear-system algorithm posted (arXiv:0811.3171)2009-10PRLpublished: Phys. Rev. Lett. 103, 15050220132×2first hardware demos solve 2×2 systems2014QMLqPCA + quantum SVM wave builds on HHL2015-04×4Aaronson lists four caveats in the fine print2016recsysKerenidis–Prakash recommendation algorithm2018-07dequantTang: classical matches recommendations2018-22low-rankGLT + Chia et al.: low-rank inversion falls2022κ·logCosta et al.: optimal solver scaling2024-098×8largest application demo (Quantinuum H-series)2026-03Θ(1/√p)Low & Su: optimal state-prep queriesend-to-end HHL advantage on a real dataset, to date: none demonstrated

What we don't know

Rosetta Quantum publishes verdicts with raw, reproducible data. This is educational content, not a product claim.

Sources:
· Harrow, Hassidim & Lloyd, Quantum algorithm for linear systems of equations, Phys. Rev. Lett. 103, 150502 (2009)
· Aaronson, Read the fine print, Nat. Phys. 11, 291–293 (2015)
· Aaronson, Quantum Machine Learning Algorithms: Read the Fine Print (technical version, 2015)
· Tang, A quantum-inspired classical algorithm for recommendation systems (2018)
· Tang, Quantum-inspired classical algorithms for principal component analysis and supervised clustering (2018)
· Gilyén, Lloyd & Tang, Quantum-inspired low-rank stochastic regression (2018)
· Chia et al., Sampling-based sublinear low-rank matrix arithmetic framework for dequantizing quantum machine learning, J. ACM (2022)
· Childs, Kothari & Somma, Quantum algorithm for systems of linear equations with exponentially improved dependence on precision, SIAM J. Comput. 46 (2017)
· Costa et al., Optimal scaling quantum linear systems solver via discrete adiabatic theorem (2021)
· Yalovetzky et al. (JPMorganChase), Solving linear systems on quantum hardware with hybrid HHL++, Sci. Rep. 14, 20610 (2024)
· Low & Su, Quantum linear system algorithm with optimal queries to initial state preparation, Quantum (2026)
· Tang, An overview of quantum-inspired classical sampling (2019)
· Kerenidis & Prakash, Quantum recommendation systems (2016)
· Cai et al., Experimental quantum computing to solve systems of linear equations, Phys. Rev. Lett. 110, 230501 (2013)
· Rosetta Quantum, What is dequantization and which claims did it take down (2026)
· Rosetta Quantum, What is QRAM and why is it the silent bottleneck (2026)
· Rosetta Quantum, Which problems have proven quantum advantage (2026)
· Rosetta Quantum, What is quantum phase estimation and why is it the algorithm of the future (2026)
· Rosetta Quantum, Is quantum useful for machine learning (2026)

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