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Nonequilibrium phase transition in a dilute Rydberg ensemble.

C Carr1, R Ritter, C G Wade

  • 1Department of Physics, Joint Quantum Centre (JQC) Durham-Newcastle, Durham University, South Road, Durham DH1 3LE, United Kingdom.

Physical Review Letters
|October 1, 2013
PubMed
Summary
This summary is machine-generated.

We observed a nonequilibrium phase transition in a dilute atomic gas, driven by Rydberg atom interactions. This transition shows optical bistability and critical slowing down, indicating a new phase of matter.

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Area of Science:

  • Atomic physics
  • Quantum optics
  • Condensed matter physics

Background:

  • Nonequilibrium phase transitions are crucial for understanding complex systems.
  • Rydberg atoms offer a unique platform for studying many-body quantum phenomena due to strong interactions.

Purpose of the Study:

  • To demonstrate and characterize a nonequilibrium phase transition in a dilute atomic gas.
  • To investigate the role of resonant dipole-dipole interactions in inducing this transition.
  • To explore the phenomena of optical bistability and critical slowing down in this system.

Main Methods:

  • Utilizing a dilute thermal atomic gas excited to Rydberg states.
  • Inducing phase transitions via resonant dipole-dipole interactions between Rydberg atoms.
  • Observing frequency domain (optical bistability) and time domain (critical slowing down) dynamics.

Main Results:

  • Demonstrated a phase transition between low and high Rydberg occupancy states.
  • Observed a mean-field shift leading to optical bistability above a critical density.
  • Measured critical slowing down with a critical exponent α=-0.53±0.10.
  • Evidence of a superradiant cascade in the high Rydberg occupancy phase.

Conclusions:

  • Nonequilibrium phase transitions can be realized and controlled in dilute atomic gases.
  • Rydberg atom interactions provide a powerful mechanism for driving and studying such transitions.
  • The observed phenomena, including optical bistability and critical slowing down, are characteristic of a distinct phase of matter.