Nature458, 178-181 (12 March 2009) | doi:10.1038/nature07838; Received 13 October 2008; Accepted 20 January 2009
Sub-cycle switch-on of ultrastrong light–matter interaction
G. Günter1, A. A. Anappara1,2, J. Hees1, A. Sell1, G. Biasiol3, L. Sorba2,3, S. De Liberato4,5, C. Ciuti4, A. Tredicucci2, A. Leitenstorfer1 & R. Huber1
Department of Physics and Center for Applied Photonics, University of Konstanz, Universitätsstrae 10, 78464 Konstanz, Germany
Laboratorio NEST, CNR-INFM and Scuola Normale Superiore, Piazza San Silvestro 12, I-56127 Pisa, Italy
Laboratorio Nazionale TASC CNR-INFM, Area Science Park, I-34012 Trieste, Italy
Laboratoire Matériaux et Phénomènes Quantiques, Université Paris Diderot-Paris 7, Case 7021, Bâtiment Condorcet, 75205 Paris, France
Laboratoire Pierre Aigrain, Ecole Normale Supérieure, UMR 8551, 75005 Paris, France
Correspondence to: R. Huber1 Correspondence and requests for materials should be addressed to R.H. (Email: rupert.huber@uni-konstanz.de).
Controlling the way light interacts with material excitations is at the heart of cavity quantum electrodynamics (QED). In the strong-coupling regime, quantum emitters in a microresonator absorb and spontaneously re-emit a photon many times before dissipation becomes effective, giving rise to mixed light–matter eigenmodes1, 2, 3, 4, 5, 6, 7, 8, 9, 10, 11, 12. Recent experiments13 in semiconductor microcavities reached a new limit of ultrastrong coupling14, where photon exchange occurs on timescales comparable to the oscillation period of light. In this limit, ultrafast modulation of the coupling strength has been suggested to lead to unconventional QED phenomena14, 15. Although sophisticated light–matter coupling has been achieved in all three spatial dimensions, control in the fourth dimension, time, is little developed. Here we use a quantum-well waveguide structure to optically tune light–matter interaction from weak to ultrastrong and turn on maximum coupling within less than one cycle of light. In this regime, a class of extremely non-adiabatic phenomena becomes observable. In particular, we directly monitor how a coherent photon population converts to cavity polaritons during abrupt switching. This system forms a promising laboratory in which to study novel sub-cycle QED effects and represents an efficient room-temperature switching device operating at unprecedented speed.