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[Paper Review] Strong coupling between a single-photon and a two-photon Fock state

Shuai-Peng Wang, Alberto Mercurio|arXiv (Cornell University)|Jan 5, 2024
Mechanical and Optical Resonators4 citations
TL;DR

This paper demonstrates strong coupling between a single photon and a two-photon Fock state in an ultrastrongly-coupled circuit-QED system using a detuned flux qubit as a nonlinear coupler. The experiment resolves quantum Rabi-like avoided crossings and observes second harmonic generation at mean photon numbers below one, enabling deterministic, coherent photon-photon interactions without external driving fields.

ABSTRACT

The realization of strong nonlinear coupling between single photons has been a long-standing goal in quantum optics and quantum information science, promising wide impact applications, such as all-optical deterministic quantum logic and single-photon frequency conversion. Here, we report an experimental observation of the strong coupling between a single-photon and a two-photon Fock state in an ultrastrongly-coupled circuit-QED system. This strong nonlinear interaction is realized by introducing a detuned flux qubit working as an effective coupler between two modes of a superconducting coplanar waveguide resonator. The ultrastrong light--matter interaction breaks the excitation number conservation, and an external flux bias breaks the parity conservation. The combined effect of the two enables the strong one--two-photon coupling. Quantum Rabi-like avoided crossing is resolved when tuning the two-photon resonance frequency of the first mode across the single-photon resonance frequency of the second mode. Within this new photonic regime, we observe the thresholdless second harmonic generation for a mean photon number below one. Our results represent a key step towards a new regime of quantum nonlinear optics, where individual photons can deterministically and coherently interact with each other in the absence of any stimulating fields.

Motivation & Objective

  • To achieve strong nonlinear coupling between single-photon and two-photon Fock states in a superconducting circuit-QED platform.
  • To overcome the challenge of negligible photon-photon interactions at the single-photon level in conventional optical media.
  • To realize deterministic, coherent interactions between individual photons without external stimulating fields or atomic excitation.
  • To explore a new regime of quantum nonlinear optics where individual photons can coherently interact via ultrastrong light-matter coupling.
  • To demonstrate second harmonic generation at mean photon numbers below one, indicating strong effective photon-photon interaction.

Proposed method

  • Employed a superconducting coplanar waveguide resonator with two distinct modes (n=1 and n=2) coupled via a detuned flux qubit acting as an effective nonlinear coupler.
  • Utilized a three-junction flux qubit with optimized Josephson energy and charging energy to enable ultrastrong coupling and break excitation number conservation.
  • Applied an external flux bias to break parity symmetry, enabling transitions between even- and odd-number photon states.
  • Engineered the system to achieve comparable transition matrix elements between bare states |2,0,g⟩ and |0,1,g⟩ at the anticrossing point, enabling strong effective coupling.
  • Used generalized master equations and eigenstate-based input-output relations to model the time evolution and field dynamics in the ultrastrong coupling regime.
  • Performed microwave spectroscopy to resolve avoided level crossings between single-photon and two-photon resonances, confirming strong coupling.
Figure 1: $|$ Setup. a, Schematic of the device. A flux qubit embedded in a ${\lambda}/{2}$ coplanar waveguide resonator, working as a nonlinear coupler between two modes of the resonator. The dashed cyan lines represent the vacuum current distribution of the $n=1$ ( ${\lambda}/{2}$ ) and $n=2$ ( $\
Figure 1: $|$ Setup. a, Schematic of the device. A flux qubit embedded in a ${\lambda}/{2}$ coplanar waveguide resonator, working as a nonlinear coupler between two modes of the resonator. The dashed cyan lines represent the vacuum current distribution of the $n=1$ ( ${\lambda}/{2}$ ) and $n=2$ ( $\

Experimental results

Research questions

  • RQ1Can strong coupling be experimentally realized between a single-photon Fock state and a two-photon Fock state in a circuit-QED system?
  • RQ2What role does ultrastrong light-matter coupling and parity breaking play in enabling effective photon-photon interactions at the single-photon level?
  • RQ3Can second harmonic generation be observed at mean photon numbers below one, indicating deterministic photon fusion?
  • RQ4How does the effective coupling strength compare to losses, and what is the potential for near-unity efficiency in single-photon to photon-pair conversion?
  • RQ5To what extent can the generalized quantum Rabi Hamiltonian describe the observed dynamics in the ultrastrong coupling regime?

Key findings

  • The experiment observed a resolved quantum Rabi-like avoided crossing between the single-photon resonance of the second mode and the two-photon resonance of the first mode, confirming strong coupling.
  • Second harmonic generation was observed with a mean photon number below one, indicating deterministic, coherent fusion of a single photon into a photon pair.
  • The effective coupling strength $ g_{\rm eff} $ was large enough to enable Rabi oscillations with a period $ T_R = 2\pi / g_{\rm eff} $, suggesting potential for near-100% conversion efficiency.
  • The system exhibited simultaneous mixing of even- and odd-number photon states due to ultrastrong coupling and broken parity, a hallmark of the generalized quantum Rabi model.
  • The transition matrix elements between the key states |2,0,g⟩ and |0,1,g⟩ were comparable in magnitude (~1), enabling strong effective coupling despite large detuning.
  • The results demonstrate a new regime of quantum nonlinear optics where individual photons interact coherently without external driving or atomic excitation, enabling deterministic quantum optics operations.
Figure 2: $|$ Quantum Rabi-like splitting. Quantum Rabi-like splitting between a single photon and a photon pair. The left part in each panel (negative flux offset) reports the measured spectra. The corresponding calculated spectra are reported for positive flux offset (right), using the parity symm
Figure 2: $|$ Quantum Rabi-like splitting. Quantum Rabi-like splitting between a single photon and a photon pair. The left part in each panel (negative flux offset) reports the measured spectra. The corresponding calculated spectra are reported for positive flux offset (right), using the parity symm

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This review was created by AI and reviewed by human editors.