Research
Gyrators for superconducting circuit design
Overview Research area: Superconducting quantum circuit theory and circuit quantization, with a focus on non-reciprocal elements. Technical level: Advanced. Scope: This paper develops a flux–charge sy

- arXiv
- 2610.22145
- Published
- 2026-10-15
- Authors
- Ciro Salcedo, Sasha Cocquyt, Andrew A. Houck, Andrew Osborne
AI summary
Overview
Research area: Superconducting quantum circuit theory and circuit quantization, with a focus on non-reciprocal elements.
Technical level: Advanced.
Scope: This paper develops a flux–charge symmetric Lagrangian and Hamiltonian formalism for superconducting circuits containing gyrators, inductors, and capacitors (LCG circuits), including arbitrary nonlinear elements, and uses it to classify when non-reciprocal circuits can be reinterpreted or replaced by reciprocal ones.
What This Paper Is About
Superconducting quantum processors are built from lumped-element circuits, but existing quantization methods struggle with non-reciprocal elements such as gyrators, which are central to circulators, isolators, and synthetic gauge fields. The paper asks how to write a consistent Hamiltonian description for general nonlinear LCG circuits and how gyrators can be transformed, inserted, or removed without changing the circuit’s dynamical spectrum. Its goal is to extend circuit-duality ideas—previously known for linear reciprocal elements—to nonlinear and non-reciprocal superconducting circuits.
Key Contributions
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A flux–charge symmetric Lagrangian for LCG circuits. The authors add a gyrator-specific symplectic term to the flux–charge symmetric Lagrangian of prior reciprocal-circuit work, covering gyrators, inductors, capacitors, Josephson junctions, and quantum phase slips with arbitrary nonlinearity.
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A general symplectic reduction and constraint taxonomy. They show that the formalism always admits a symplectic reduction for nonsingular, well-posed LCG circuits, and they classify the resulting constraints by their topological origin before any algebra is performed.
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Circuit duality and partial-dual point transformations. They extend circuit duality to nonlinear non-reciprocal circuits and introduce point transformations that insert, remove, or move reciprocal elements across gyrators while preserving the Hamiltonian spectrum. This extends Tellegen’s element-mimicking result to nonlinear reciprocal elements such as the Josephson junction and quantum phase slip.
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A graph-theoretic classification of reciprocally simulable circuits. Using the non-reciprocal coupling graph (NCG), whose vertices are really-connected components and whose edges record gyrators, they prove that a circuit with a bipartite NCG has a unitarily equivalent realization using capacitors, inductors, and ideal transformers, and that a forest NCG admits a realization with no gyrators at all.
Main Findings
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Gyrators enter through a non-energy-storing symplectic term. Each gyrator edge pair contributes a term built from the gyration ratio, the incidence and orientation matrices, and time derivatives of node fluxes and loop charges. The term is antisymmetric and reproduces the gyrator constitutive relations.
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The Lagrangian reproduces Kirchhoff’s laws and element constitutive relations. Varying the action with respect to loop charges and node fluxes yields the expected circuit equations, including voltage differences across capacitors, inductors, and gyrators.
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The connection matrix is generally rank-deficient, but constraints can be reduced systematically. Null vectors of the circuit two-form split into gauge directions inherited from the graph boundary maps and dynamically meaningful constraints tied to circuit topology.
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Well-posedness is equivalent to unique solubility of the algebraic constraints. The paper distinguishes ill-posed circuits—such as a quantum phase slip not in series with an inductor, a Josephson junction without parallel capacitance, or two voltage sources with distinct voltages in parallel—from singular circuits that lack dynamics entirely.
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Circuit duality exchanges flux and charge coordinates. If ℒ(q_l, φ_v) is the flux–charge symmetric Lagrangian of a circuit, then ℒ(φ_v, q_l) describes its dual. The paper extends this notion to nonlinear non-reciprocal LCG circuits.
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Partial duality preserves the Hamiltonian spectrum. Point transformations can move reciprocal elements across gyrators, define continuous isospectral families of circuits, and realize elements in otherwise inaccessible parameter regimes.
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Reciprocal simulation is characterized graphically. A bipartite NCG guarantees a unitarily equivalent reciprocal realization with capacitors, inductors, and ideal transformers; a forest NCG guarantees a realization with no gyrators.
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No experimental benchmarks or measured data are reported. The paper is a theoretical and formal circuit-theory contribution.
Methodology in Plain English
The authors model a circuit as an oriented planar multigraph whose vertices are nodes and whose edges are capacitive, inductive, or gyrative elements. They assign both node fluxes and loop charges as coordinates, rather than choosing only one type as in the traditional method of nodes or method of loops. A Lagrangian is written with a symplectic term that couples fluxes and charges and an energetic term that stores energy in capacitors and inductors; gyrators add a separate antisymmetric term that stores no energy.
The resulting equations of motion are required to reproduce Kirchhoff’s laws and each element’s constitutive relation. Because the symplectic matrix is generally not invertible, the authors identify its null vectors and the algebraic constraints they generate, solve those constraints, and reduce the circuit to a smaller phase space on which the Legendre transform can be performed. They then study transformations of the circuit Lagrangian—especially transformations that exchange flux and charge coordinates or move elements across gyrators—and translate their effects into graph-theoretic conditions on the non-reciprocal coupling graph. A reference conductance convention, G₀ = 1, is adopted so that flux and charge are numerically interchangeable and the duality transformation is dimensionally consistent.
Why This Matters
Impact on research: The formalism gives a systematic route to Hamiltonians for non-reciprocal superconducting circuits without the manual case-by-case reduction required by some earlier methods. It also provides a Lagrangian-level complement to geometric Faddeev–Jackiw quantization, preserving structural information about the circuit that can be used for canonical transformations and duality arguments.
Real-world applications:
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On-chip circulators and isolators: Gyrators can synthesize non-reciprocal components that protect qubits from amplifier back-action, potentially reducing the need for bulky ferrite components at the mixing-chamber stage of a dilution refrigerator.
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Compact linear inductors: A gyrator combined with a capacitor can mimic a linear inductor in a small physical footprint, avoiding a relatively massive magnetic coil.
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Quantum phase slip emulation: A Josephson junction combined with a gyrator can mimic a quantum phase slip junction, whose direct fabrication remains challenging.
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Synthetic gauge fields and chiral lattice physics: Gyrators can model Floquet-driven circuits and break time-reversal symmetry in simulated lattice Hamiltonians, enabling studies of chiral topological Bose–Hubbard physics.
Industry relevance: The results are relevant to superconducting quantum-hardware design, cryogenic component miniaturization, and the engineering of non-reciprocal elements for qubit readout and protected-qubit architectures. The graph-theoretic classification also offers a design-level criterion for deciding when a non-reciprocal circuit can be replaced by a reciprocal equivalent.
Future Directions
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Experimental realization and validation: Demonstrating on-chip gyrators in superconducting circuits and testing the predicted isospectral transformations in real devices.
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Extension to open and dissipative circuits: Incorporating noise, losses, and amplifier back-action into the flux–charge symmetric framework, since the present treatment focuses on conservative LCG circuits.
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Design of protected qubits and exotic elements: Using partial duality to realize proposed devices—such as the dualmon or quantum phase slip-based circuits—in more accessible parameter regimes.
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Scaling and automation: Applying the NCG classification to larger non-reciprocal coupling graphs and developing automated constraint-reduction procedures for complex circuit topologies.
Target Audience
This paper is aimed at researchers in superconducting quantum circuits, circuit QED, and quantum device theory, particularly those working on circuit quantization, non-reciprocal components, and protected-qubit design. It will also interest graduate students and theorists comfortable with Lagrangian and Hamiltonian mechanics, graph theory, and the mathematical structure of lumped-element circuits. Readers seeking experimental results or device benchmarks will not find them here; the contribution is formal and theoretical.
Authors’ abstract
Assuming only the solubility of Kirchhoff's laws, the conservation of energy, and the form of the constitutive relations, we present a flux-charge symmetric Hamiltonian formalism that always admits a symplectic reduction for nonsingular, well-posed circuits involving gyrators, inductors, and capacitors (LCG circuits) with arbitrary non-linearity. The formalism introduces a notion of circuit duality on non-linear non-reciprocal circuits and a family of point transformations that inserts, removes, and moves reciprocal elements across gyrators while preserving the Hamiltonian spectrum. With these transformations, we extend Tellegen's classic result that gyrators make reciprocal elements behave as their dual to non-linear reciprocal elements such as the Josephson junction and quantum phase slip. Furthermore, we present conditions under which non-reciprocal circuits can be transformed to dynamically equivalent reciprocal circuits.