Papers for

quantum hardware designers

Papers whose findings have a practical use for this group, as judged from the abstract. Open a paper to read what it means in practice.

Complexity of finding noise resistant states in quantum systems

On the Complexity of Finding Decoherence Free Subspaces

Abstract: Decoherence free subspaces are a steady-state structure of the open quantum system which preserves quantum coherence between the states lying with in it and thus has found a variety of applications throughout quantum information science and technology. In this paper we study the computational complexity of deciding whether an open quantum system admits a decoherence free subspace or not. More specifically we study this problem with in the context of Markovian open quantum systems, governed by the time-independent Lindblad master equation. Along the way we introduce the $k$-Local Lindbladian problem, which captures the difficulty of computing purity decay rates under Lindbladian dynamics. We show that both problems are hard for the complexity class Quantum Merlin Arthur (QMA) when the locality $k \geq 5$, with the first under perfect completeness and the second being complete for QMA. Our hardness construction generalizes Kitaev's clock Hamiltonian construction to the open quantum system setting by encoding the execution of a quantum circuit into the steady subspace of a Lindbladian containing both pure and mixed history states. This subspace is then mixed depending on the output of the encoded circuit. Our results suggest that deciding whether a generic Markovian open quantum system admits a decoherence free subspace is intractable even for quantum computation.

Tue 22 SeptComputational Complexity
The gist
Some quantum systems have special groups of states that don’t lose their quantum properties easily, called decoherence free subspaces. This paper examines how hard it is to figure out if these groups exist in certain open quantum systems that interact with their environments. The authors show that deciding this is computationally very difficult—even for quantum computers—by linking the problem to a known tough class in quantum computing called QMA. This means that finding these stable quantum states might be practically impossible for complex systems.
Open 2609.26769v1

Complexity of estimating Berry phase in 2-local quantum systems revealed

On the Computational Complexity of Guided Berry Phase Estimation

Abstract: We prove that deciding the Berry phase for parameterised 2-local qubit Hamiltonians is BQP-complete when presented with a classical description of a guiding state, promised to overlap with the ground state of the system. Our results extend to systems with weighted Heisenberg interactions and when restricted to a 2D square or triangular lattice geometry. The techniques we develop leverage the Schrieffer--Wolff transformation, typically used in the construction of perturbative gadget reductions for local Hamiltonian problems, extending it to parameterised families of Hamiltonians. We demonstrate that there exists a choice of parameterised simulator Hamiltonians whose Berry phase well-approximates that of a parameterised target family. Using the perturbative gadget reduction framework of Oliveira and Terhal and of Schuch and Verstraete, we adapt the arguments to parameterised interactions and demonstrate the error bounds in the resulting simulation can be controlled. Additionally, we provide an explicit proof that families of 1-local Hamiltonians have a Berry phase that can be efficiently computed to inverse-polynomial precision. This establishes a complexity transition between 1-local and 2-local Hamiltonian families.

Tue 22 SeptComputational Complexity
The gist
This work studies how hard it is to figure out a special quantum property called the Berry phase for systems made of interacting quantum bits (qubits). It shows that when you have a guiding state close to the system's lowest energy state, deciding this phase is just as tough as the hardest problems a quantum computer can solve. The authors prove this for different types of qubit interactions and lattice layouts, and also show that for simpler systems with only one qubit interacting at a time, the Berry phase can be calculated efficiently. This marks a clear difference in difficulty depending on how qubits interact.
Open 2609.25929v1

Variational quantum optimization diagnostics do not guarantee better training results

From Trainability Diagnostics to Optimization Claims: Boundaries and Controls in Variational Quantum Optimization

Abstract: Barren plateau diagnostics characterize whether gradient signal remains available for training, but surviving signal need not translate into successful optimization. We study this trainability--optimization gap at the level of optimizer steps. Treating coefficient-weighted Hamiltonian-term gradients as task-like components, we introduce step-level diagnostics and derive an exact bridge between signed termwise organization, directional activity, and first-order descent. Resolving this bridge into standard first-order geometry shows that the apparent organization--activity factors are not independent optimization axes and that, at fixed state and update norm, the raw gradient maximizes first-order descent of the summed objective. We compare vanilla gradient descent, a deterministic Hamiltonian-term PCGrad variant, and probe-gated LSO-PCGrad on transverse-field Ising model instances with hardware-efficient and Hamiltonian variational ansatzes, together with matched controls for update norm and probe budget. Blind projection can improve an organization diagnostic while worsening final energy and first-order predictability. After conditioning on standard first-order geometry, residual term-space composition shows no reproducible material incremental association with realized descent, while optimizer-relative update norm shows positive material associations in some settings without cross-regime reproducibility. Matched controls provide no resolved final-energy benefit attributable to the projected direction, and the improvement of LSO-PCGrad is more consistent with probe-based search and step-norm adaptation than with Hamiltonian-term projection itself. These results show that gradient-structure diagnostics can characterize trainability and update geometry without serving as standalone evidence of optimization benefit, which requires controls matched on update norm and search budget.

Fri 18 SeptMachine Learning
The gist
Training quantum algorithms can be tricky because having some useful signal for learning doesn't always mean the algorithm will find the best answer. The authors studied why this gap happens by looking closely at how each step in the training process works. They found that some methods thought to improve the process don't consistently lead to better outcomes. Their work shows that simply meeting certain mathematical conditions during training isn't enough to promise success without careful controls and comparisons.
Open 2609.21243v1

Joint approach improves accuracy of quantum expectation calculations

New directions in dynamical expectation estimation

Abstract: Computing dynamical expectation values typically relies on approximations optimized for the state or observable separately, without accounting for how their errors combine in the final expression.This work explores an alternative approach in which each approximation is guided by both the state and the observable, accounting for how they jointly determine the target expectation value. This idea is implemented through a sweep algorithm with coupled loss functions for forward state and backward observable updates. Exact error relations provide an analytical rationale for how the proposed losses can improve the accuracy. Numerical tests on 30-qubit random circuits show errors two to three orders of magnitude smaller than those of variational state compression at equal bond dimensions. These results motivate further exploration of joint state and observable approximation for dynamical expectation value estimation.

Wed 16 SeptEmerging Technologies
The gist
Calculating certain values in quantum systems usually involves approximations made separately for parts of the problem, which can lead to errors adding up. The authors propose a new method that considers both the parts together when making approximations, which helps reduce mistakes. They use a special algorithm that updates the estimates forward and backward to improve accuracy. Tests on simulated quantum circuits show their method can be much more precise than older techniques.
Open 2609.18246v1

Strong limits proven for quantum data loss over pure-loss channels

Strong converse for the quantum capacity of the pure-loss bosonic channel

Abstract: This paper reports the proof of a strong converse for the unconstrained quantum capacity of the pure-loss bosonic channel. At every fixed rate above capacity, the entanglement-generation fidelity of every code is bounded by a constant times the reciprocal of the number of channel uses. The bound holds without an energy constraint and for arbitrary encoded states, including states correlated across all input modes, and arbitrary joint decoders. The proof combines quantum Chebyshev and hockey-stick testing inequalities with a uniform relative-entropy-variance bound for the balanced pure-loss channel, corresponding to transmissivity $η=1/2$. The variance bound follows by expressing the balanced beam splitter in bright and dark modes: the dark modes are exactly in vacuum, and any state orthogonal to that vacuum contains at least one dark photon. For general transmissivity, dilating the degrading attenuator reduces the problem to this balanced-channel setting and bounds the decoder test by precisely the factor that produces the known quantum-capacity threshold. The resulting argument establishes the strong converse at the unconstrained quantum capacity for every pure-loss bosonic channel.

Tue 15 SeptInformation Theory
The gist
This paper proves a strong limit on how much quantum information can be reliably sent over certain types of noisy channels called pure-loss bosonic channels. Specifically, it shows that any attempt to communicate quantum information at a rate above the channel’s capacity will fail with very high probability as the number of channel uses grows. The authors’ proof works without needing limits on input energy and applies to the most general encoding and decoding schemes. Their techniques combine new mathematical bounds on quantum information measures with insights about light splitting in these channels.
Open 2609.16608v1

Quantum circuits solve 2-fold Forrelation faster than classical AC0 circuits

2-Fold Forrelation is in QAC$^0$

Abstract: We show that 2-fold Forrelation with inverse-polylogarithmic promise gap can be solved, with bounded error, by polynomial-size QAC$^0$ circuits. Unlike the standard oracle-based Forrelation algorithm, our circuits receive the input explicitly, in the same form as the AC$^0$ circuits against which Forrelation is known to be hard. At constant gap, this yields a natural promise-problem separation between QAC$^0$ and AC$^0$.

Mon 7 SeptComputational Complexity
The gist
Some problems are very hard for simple classical computers to solve quickly. The authors show that a certain quantum problem called 2-fold Forrelation can be solved efficiently by very basic quantum circuits, even when the problem's input is given directly rather than as a mysterious oracle. This shows a clear difference in what quantum and classical circuits can efficiently do on this problem. Their result points to a natural way to separate simple quantum and classical computation models.
Open 2609.07060v1