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Related Concept Videos

The Quantum-Mechanical Model of an Atom02:45

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Shortly after de Broglie published his ideas that the electron in a hydrogen atom could be better thought of as being a circular standing wave instead of a particle moving in quantized circular orbits, Erwin Schrödinger extended de Broglie’s work by deriving what is now known as the Schrödinger equation. When Schrödinger applied his equation to hydrogen-like atoms, he was able to reproduce Bohr’s expression for the energy and, thus, the Rydberg formula governing hydrogen spectra.
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On-Chip Crystallization and Large-Scale Serial Diffraction at Room Temperature
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Many-body-localized discrete time crystal with a programmable spin-based quantum simulator.

J Randall1,2, C E Bradley1,2, F V van der Gronden1,2

  • 1QuTech, Delft University of Technology, PO Box 5046, 2600 GA Delft, Netherlands.

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|November 4, 2021
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Summary
This summary is machine-generated.

Researchers observed a discrete time crystal (DTC), a novel phase of matter, using a quantum simulator. This breakthrough demonstrates robust time-crystalline order and opens new avenues for exploring many-body physics.

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Area of Science:

  • Quantum physics
  • Condensed matter physics
  • Many-body physics

Background:

  • Discrete time crystals (DTCs) represent a novel nonequilibrium phase of matter.
  • They spontaneously break time-translation symmetry.
  • Disorder-induced many-body localization is crucial for stabilizing DTCs by preventing thermalization.

Purpose of the Study:

  • To observe the hallmark signatures of a many-body–localized DTC.
  • To utilize a quantum simulation platform for studying this exotic phase.
  • To confirm the robustness and characteristics of time-crystalline order.

Main Methods:

  • Employed a quantum simulation platform utilizing individually controllable carbon-13 nuclear spins in diamond.
  • Demonstrated long-lived period-doubled oscillations.
  • Verified robustness of these oscillations for generic initial states.

Main Results:

  • Observed clear signatures of the many-body–localized discrete time crystal.
  • Confirmed characteristic time-crystalline order across the many-body spectrum.
  • Results align with the realization of an out-of-equilibrium Floquet phase.

Conclusions:

  • Successfully realized and observed a many-body–localized discrete time crystal.
  • Introduced a programmable solid-state spin quantum simulator for many-body physics research.
  • Paved the way for further exploration of nonequilibrium quantum phenomena.