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Black-box superconducting circuit quantization (1204.0587v1)

Published 3 Apr 2012 in cond-mat.mes-hall and quant-ph

Abstract: We present a semi-classical method for determining the effective low-energy quantum Hamiltonian of weakly anharmonic superconducting circuits containing mesoscopic Josephson junctions coupled to electromagnetic environments made of an arbitrary combination of distributed and lumped elements. A convenient basis, capturing the multi-mode physics, is given by the quantized eigenmodes of the linearized circuit and is fully determined by a classical linear response function. The method is used to calculate numerically the low-energy spectrum of a 3D-transmon system, and quantitative agreement with measurements is found.

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Summary

  • The paper introduces a semi-classical method that quantizes weakly anharmonic superconducting circuits by employing linear response functions to capture multimode physics.
  • It applies perturbative techniques to determine quantized eigenmodes, achieving sub-percent error alignment with experimental 3D transmon spectra.
  • The method reduces free parameters in the effective Hamiltonian, streamlining circuit design and enhancing accuracy in quantum computing architectures.

Black-box Superconducting Circuit Quantization

The present paper addresses the development of a semi-classical method for quantizing weakly anharmonic superconducting circuits, focusing on systems that incorporate Josephson junctions coupled to complex electromagnetic environments. These environments may consist of a combination of distributed and lumped components. The proposed approach introduces a linear response function as a basis to capture the multi-mode physics intrinsic to these systems, aiding in the calculation of the effective low-energy quantum Hamiltonian.

There have been notable challenges in the theoretical modeling of superconducting circuits, especially as experimental capabilities have vastly improved, allowing for more precise measurements of circuit spectra. Classical models, like the single-mode Jaynes-Cummings model, have strived to represent these systems; however, they fail to encapsulate the complexities introduced by multi-mode interactions and increased coupling strengths. As a result, there is a pressing need to refine quantum mechanical models beyond traditional paradigms, accommodating the demand for higher precision in the design and analysis of superconducting qubits.

The paper's methodology hinges on the exploitation of classical circuit quantization, starting with the assumption of linearized multi-mode interactions. By applying perturbative techniques to account for the weak anharmonicity of the Josephson junctions, the method determines the quantized eigenmodes of the circuit. This approach effectively deals with systems where multiple modes and coupling strengths complicate the modeling process. Particularly noteworthy is the way this method handles charge dispersion, assumed to be negligible in state-of-the-art transmon qubits, which significantly simplifies the derived Hamiltonian.

Among the pivotal results, the authors demonstrate their method's computational efficacy by achieving quantitative agreement with experimental spectra of a 3D transmon system. Analyzing six samples, the document reports low-energy spectrums that align at a sub-percent error margin with experimentally obtained results. The paper quantifies qubit anharmonicity and state-dependent cavity shifts, presenting an empirical validation of the theoretical framework. The numerically calculated spectra, alongside fitted parameters such as the capacitance and inductance associated with the Josephson junctions, underscore the model's precision and applicability.

The implications of this work reverberate in the fields of quantum computing and information processing, particularly within circuit quantum electrodynamics (cQED). By refining the tools available for circuit quantization, this research facilitates the design of more accurate and efficient quantum processors based on superconducting qubits. The reduction of free parameters in the Hamiltonian model diminishes the dependence on oscillatory experimental iterations, offering a streamlined path for improving quantum circuit design.

Looking forward, the methodology proposed could lay foundational groundwork for exploring ultra-strong coupling regimes in cQED, where the interaction energies of components become comparable to their individual energy levels. This investigation is crucial for progressing toward creating more robust quantum architectures capable of performing with high fidelity. Furthermore, while the paper primarily focuses on single junction systems, the framework is extendable to multi-qubit scenarios, wherein challenges such as inter-qubit coupling and environmental interactions demand a sophisticated analytical approach.

Overall, the paper advances the field of superconducting quantum circuits by providing a concrete and verifiable model of circuit quantization, enabling enhanced understanding and fabrication of complex quantum systems. The application of classical response functions to decipher the intricacies of multimodal interactions confers a notable contribution to both the theoretical and practical aspects of quantum circuit engineering.

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