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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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Related Experiment Video

Updated: Mar 7, 2026

Fabrication and Characterization of Disordered Polymer Optical Fibers for Transverse Anderson Localization of Light
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Quantum non-Markovianity induced by Anderson localization.

Salvatore Lorenzo1,2, Federico Lombardo3, Francesco Ciccarello3,4

  • 1Quantum Technology Lab, Dipartimento di Fisica, Università degli Studi di Milano, 20133 Milano, Italy.

Scientific Reports
|February 17, 2017
PubMed
Summary

Disordered quantum systems exhibit Anderson localization, preventing free excitation propagation. This study links this localization to non-Markovian atomic dynamics and quantum information backflow in coupled-cavity arrays.

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Area of Science:

  • Quantum physics
  • Condensed matter physics
  • Quantum information science

Background:

  • Excitations in disordered lattices localize due to destructive interference (Anderson localization).
  • Atomic interactions with disordered lattices lead to non-trivial excitation exchange and quantum information backflow.
  • This backflow is a signature of non-Markovian dynamics.

Purpose of the Study:

  • Investigate quantum emitter dynamics coupled to a disordered uniform coupled-cavity array (CCA).
  • Explore the relationship between Anderson localization in CCAs and non-Markovian atomic dynamics.
  • Characterize quantum information backflow as a measure of non-Markovianity.

Main Methods:

  • Modeling a quantum emitter (atom) weakly coupled to a uniform CCA.
  • Introducing static disorder into the CCA to induce Anderson localization of field normal modes.
  • Analyzing atomic dynamics and quantum information backflow under disordered conditions.

Main Results:

  • Disorder in the CCA leads to Anderson-localized field modes.
  • This localization induces non-Markovian atomic dynamics.
  • A functional relationship is established between quantum non-Markovianity and CCA localization.
  • Atomic dynamics are well-described by a phenomenological model involving a single mode and a Markovian bath.

Conclusions:

  • Anderson localization in CCAs drives non-Markovian quantum dynamics for coupled emitters.
  • Quantum information backflow serves as a robust indicator of non-Markovianity in such systems.
  • The findings offer insights into controlling quantum dynamics in disordered photonic structures.