Quantum circuits without Pauli-matrix decomposition ✛

Original: "Efficient Quantum Circuits for Electronic Hamiltonian Simulation without Pauli Expansion"
· Tamiya Onodera, Takeshi Sato
arXiv:2609.06285v1 · 2026-09-05 · CC BY 4.0 · 3 min
Japanese physicists built compact quantum circuits for simulating electrons, preserving the fermionic structure instead of decomposing into Pauli strings.

Context

Quantum simulation of molecular electronic structure is considered one of the most promising applications of quantum computers. The standard route involves the Jordan-Wigner transformation and subsequent decomposition of operators into Pauli strings. However, such decomposition at an early stage hides connections between terms that were transparent in the fermionic representation. This work continues a line started by Sato and colleagues for partial differential equations, where ladder string pairs were diagonalized directly. Neighboring works on the archive concern non-Hermitian gates, quantum advantage, quantum clocks and memory, as well as gate optimization and control of quantum systems. This paper stands somewhat apart but falls into the group of quantum algorithms and error correction.

Methods

The authors use the Jordan-Wigner transformation to map fermionic creation and annihilation operators onto qubits. Instead of decomposing into Pauli strings, they diagonalize ladder string pairs (Lasp) via GHZ state preparation and parity encoding. The circuit for one two-particle operator includes a GHZ transformation, parity encoding, and a multi-controlled Z rotation. For three operators sharing four indices (a triad), a single circuit is built where gates cancel due to commutation and local rewrites. Ordering triads with a fixed rotation qubit and minimal index changes allows cascading cancellation of CX gates at the boundaries.

Results

For the complex-valued case, the circuit for one two-particle fermionic Lasp operator corresponds to 16 Pauli strings but contains no Trotter error. Optimizing a triad reduces the number of CX gates from 36 to 12 while preserving three C3RZ gates. For a sequence of O(n) suitably ordered triads, the number of CX gates decreases from O($n^2$) to O(n). In the real case, three C3RZ gates form a uniformly controlled rotation that decomposes into only eight CX gates. A controlled version of the circuit is obtained by adding one control to the multi-controlled Z rotations.

Implications

The work shows that preserving the high-level structure of fermionic operators allows optimization that is inaccessible after decomposition into Pauli strings. Unlike neighboring approaches that target individual gates or groups of strings, here optimization is performed at the level of whole operators and their triples. This expands the space of possible cancellations and provides a systematic path to more efficient circuits. The result is especially important for early quantum computers, where every gate counts.

Future development

The authors plan to systematically search for suitable orderings of triads and efficient compositions of several groups of ordered triads. Generalization to other fermionic transformations and more complex Hamiltonians is possible. It is also interesting to investigate how the proposed circuits behave on real hardware with noise and qubit connectivity constraints.

Impact

The approach directly impacts quantum chemistry, materials science, and pharmaceuticals, where electronic structure simulation is critical. Reducing the number of gates speeds up calculations and lowers the requirements for error correction.

Next steps

Immediate next steps include implementing the proposed circuits on real quantum processors and comparing with existing methods. Also, algorithms for automatic search of optimal triad orderings for specific molecules need to be developed.

Key open problems

In quantum chemistry, the problem of scaling exact simulations to large molecules remains open. This work reduces the gate cost but does not solve the fundamental question of how to avoid exponential growth in the number of parameters. The connection to basis selection and Trotterization accuracy also requires further study.

The knowledge machine's view

This section is addressed to the author of the paper and their colleagues. Neighbouring works were found by meaning-based search across our archive, not by word overlap. We do not review: we show the field around the work.

What the work does

The authors build quantum circuits for electronic Hamiltonians directly from fermionic ladder operators, bypassing the Pauli string decomposition. They diagonalize ladder string pairs (Lasp) using GHZ states and multi-controlled rotations, and for operator triples with shared indices they optimize the circuit, reducing the number of CX gates. As a result, for the complex-valued case, a single two-body operator is implemented by one circuit instead of 16 Pauli strings, without Trotterization, and ordering the triples reduces the scaling of the CX count from quadratic to linear.

Where its strength is

Preserving the high-level fermionic structure allows optimization at the level of whole operators and their triples, which is not possible after decomposition into Pauli strings. This opens a systematic path to more compact circuits, especially valuable for early quantum computers.

Where it could go next

  • One could consider applying a similar technique for diagonalizing ladder operators to other physical systems, for example, models with non-Hermitian or dissipative terms, where standard transformations may be suboptimal. There is a paper in the archive on non-Hermitian gates that might suggest how to extend the approach to open quantum systems.based on: Hybrid Intelligence: Quantum Hearing Distinguishes Topological Phases arXiv:2606.28199
  • It would be interesting to see how the proposed operator-level optimization interacts with circuit compilation methods for specific architectures that take into account qubit connectivity and noise. Nearby there is a paper on quantum networks and gate optimization that could provide ideas for adapting circuits to real devices.based on: Quantum Networks: How Optical Switches Link Processors arXiv:2501.05598
  • Perhaps it is worth studying whether the method can be extended to other representations of fermionic operators, for example, to compact encodings that reduce the number of qubits. There is a paper in the archive on a quantum simulator with flying qubits that might suggest alternative encoding methods.based on: Quantum Simulator on Fleeting Qubits arXiv:2608.04290v1

Worth trying

  • Test whether combining the proposed optimization with circuit-depth reduction methods based on gate cancellation at block boundaries yields a gain.
  • Assess the impact of noise on the proposed circuits and compare with Trotterized circuits from Pauli strings for small molecules.
  • Consider the possibility of automatically searching for the optimal ordering of triples using heuristic algorithms similar to those used in quantum circuit compilation.

Why this may matter

The approach could substantially reduce the cost of quantum simulation of electronic structure, bringing practical use of quantum computers in chemistry and materials science closer. Preserving the structure of operators opens new optimization opportunities that may be generalized to other problems as well.

The circuit for one two-particle operator, which in the standard approach would require 16 Pauli strings, here fits into a single multi-controlled rotation. It is as if a complex orchestral chord were written as a single note.

The idea of preserving structure instead of decomposing into simple elements resembles the approach in Neal Stephenson's novel "Anathem," where scientists manipulate complex concepts as wholes, not reducing them to primitives.

Key numbers

  • Number of CX gates for a triad before optimization: 36
  • Number of CX gates for a triad after optimization: 12
  • Number of Pauli strings for one two-particle operator: 16
  • Number of CX gates for uniformly controlled rotation: 8
Concepts
optimization