Climbing the Jaynes-Cummings Ladder and Observing its Sqrt(n) Nonlinearity in a Cavity QED System

TL;DR

This paper provides direct spectroscopic evidence of the quantum nonlinearity in a cavity QED system by observing the sqrt(n) scaling in the Jaynes-Cummings ladder, confirming the quantum nature of atom-photon interactions.

Contribution

First direct spectroscopic observation of the sqrt(n) nonlinearity in the Jaynes-Cummings ladder in a circuit QED system, demonstrating quantum behavior beyond classical explanations.

Findings

Observation of the sqrt(n) scaling in atom-photon coupling

Spectroscopic evidence of quantum nonlinearity in cavity QED

Exploration of atom-photon superposition states with up to two photons

Abstract

The already very active field of cavity quantum electrodynamics (QED), traditionally studied in atomic systems, has recently gained additional momentum by the advent of experiments with semiconducting and superconducting systems. In these solid state implementations, novel quantum optics experiments are enabled by the possibility to engineer many of the characteristic parameters at will. In cavity QED, the observation of the vacuum Rabi mode splitting is a hallmark experiment aimed at probing the nature of matter-light interaction on the level of a single quantum. However, this effect can, at least in principle, be explained classically as the normal mode splitting of two coupled linear oscillators. It has been suggested that an observation of the scaling of the resonant atom-photon coupling strength in the Jaynes-Cummings energy ladder with the square root of photon number n is sufficient to prove that the system is quantum mechanical in nature. Here we report a direct spectroscopic observation of this characteristic quantum nonlinearity. Measuring the photonic degree of freedom of the coupled system, our measurements provide unambiguous, long sought for spectroscopic evidence for the quantum nature of the resonant atom-field interaction in cavity QED. We explore atom-photon superposition states involving up to two photons, using a spectroscopic pump and probe technique. The experiments have been performed in a circuit QED setup, in which ultra strong coupling is realized by the large dipole coupling strength and the long coherence time of a superconducting qubit embedded in a high quality on-chip microwave cavity.