Related Experiment Video
Updated: Jun 5, 2026

Scalable Quantum Integrated Circuits on Superconducting Two-Dimensional Electron Gas Platform
Published on: August 2, 2019
Deep strong coupling regime of the Jaynes-Cummings model
J Casanova1, G Romero, I Lizuain
1Departamento de Química Física, Universidad del País Vasco-Euskal Herriko Unibertsitatea, Bilbao, Spain.
We explore quantum dynamics in the deep strong coupling regime (DSC) of the Jaynes-Cummings model. Our new physical frame reveals photon wave packet dynamics, causing population collapse and revivals in two-level systems.
Area of Science:
- Quantum optics
- Quantum dynamics
- Atomic physics
Background:
- The Jaynes-Cummings model describes light-matter interaction.
- The deep strong coupling (DSC) regime (g/ω≳1) challenges standard approximations like the rotating-wave approximation.
Purpose of the Study:
- To develop a new physical frame for understanding quantum dynamics in the DSC regime.
- To analyze the behavior of a two-level system coupled to a harmonic oscillator beyond perturbative limits.
Main Methods:
- Developing an intuitive and predictive physical frame.
- Applying numerical and analytical methods.
- Investigating qubit population dynamics, photon statistics, and Wigner phase space.
Main Results:
- Photon number wave packets exhibit oscillatory behavior along parity chains in the Hilbert space.
- The proposed frame accurately describes collapse and revival phenomena in population dynamics.
- Distinct signatures in qubit population, photon statistics, and Wigner phase space are identified.
Conclusions:
- The developed physical frame provides a powerful tool for studying quantum systems in the DSC regime.
- This work offers new insights into fundamental light-matter interactions beyond the rotating-wave approximation.
Related Concept Videos
¹H NMR: Long-Range Coupling
In alkenes, spin information is communicated via σ–π overlap, as seen in allylic (four-bond) and homoallylic (five-bond) couplings. These coupling interactions are stronger when the σ bond is parallel to the alkene π orbitals.
Spin–Spin Coupling: Two-Bond Coupling (Geminal Coupling)
The central atom need not be NMR-active because its electrons are affected by the electron polarization of the spin-active atoms. However, spin information is transmitted less effectively than in one-bond coupling, and 2J values are usually weaker than 1J values. The energy of...
Spin–Spin Coupling: One-Bond Coupling
Spin–Spin Coupling Constant: Overview
Qualitatively, any spin plus-half nucleus polarizes the spins of its electrons to the minus-half state. Consequently, the paired electron in the hydrogen–carbon bond must have a...
Spin–Spin Coupling: Three-Bond Coupling (Vicinal Coupling)
The extent of coupling depends on the C‑C bond length, the two H‑C‑C angles, any electron-withdrawing substituents, and the dihedral angle between the involved orbitals. The...
Debye–Huckel–Onsager Conductance Equation

