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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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Werner Heisenberg considered the limits of how accurately one can measure properties of an electron or other microscopic particles. He determined that there is a fundamental limit to how accurately one can measure both a particle’s position and its momentum simultaneously. The more accurate the measurement of the momentum of a particle is known, the less accurate the position at that time is known and vice versa. This is what is now called the Heisenberg uncertainty principle. He...
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In the macroscopic world, objects that are large enough to be seen by the naked eye follow the rules of classical physics. A billiard ball moving on a table will behave like a particle; it will continue traveling in a straight line unless it collides with another ball, or it is acted on by some other force, such as friction. The ball has a well-defined position and velocity or well-defined momentum, p = mv, which is defined by mass m and velocity v at any given moment. This is the typical...
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If a closed surface does not have any charge inside where an electric field line can terminate, then the electric field line entering the surface at one point must necessarily exit at some other point of the surface. Therefore, if a closed surface does not have any charges inside the enclosed volume, then the electric flux through the surface is zero. What happens to the electric flux if there are some charges inside the enclosed volume? Gauss's law gives a quantitative answer to this question.
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¹H NMR: Interpreting Distorted and Overlapping Signals01:02

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Spin systems where the difference in chemical shifts of the coupled nuclei is greater than ten times J are called first-order spin systems. These nuclei are weakly coupled, and their chemical shifts and coupling constant can generally be estimated from the well-separated signals in the spectrum.
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Related Experiment Video

Updated: Feb 22, 2026

Generation and Coherent Control of Pulsed Quantum Frequency Combs
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Generation and Coherent Control of Pulsed Quantum Frequency Combs

Published on: June 8, 2018

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Quantized gravitational responses, the sign problem, and quantum complexity.

Zohar Ringel1,2, Dmitry L Kovrizhin1,3

  • 1Rudolf Peierls Centre for Theoretical Physics, Keble Road, Oxford OX1 3NP, UK.

Science Advances
|September 30, 2017
PubMed
Summary
This summary is machine-generated.

Quantized gravitational responses obstruct sign-free quantum Monte Carlo (QMC) simulations for bosonic systems. This finding impacts condensed matter physics and quantum simulations, especially those with broken time-reversal symmetry.

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Area of Science:

  • Quantum physics
  • Condensed matter physics
  • Computational physics

Background:

  • Efficient classical simulation of quantum systems is a major challenge.
  • The sign problem in quantum Monte Carlo (QMC) simulations prevents sign-free calculations for many important quantum systems.
  • The existence of a fundamental obstruction to sign-free representations in generic quantum systems is an open question.

Purpose of the Study:

  • To investigate obstructions to local sign-free QMC simulations in systems with bosonic degrees of freedom.
  • To explore the connection between quantized gravitational responses and the sign problem.
  • To examine these phenomena in condensed matter systems and models with broken time-reversal symmetry.

Main Methods:

  • Analysis of systems with bosonic degrees of freedom.
  • Identification of quantized gravitational responses as obstructions.
  • Application of arguments to condensed matter systems like fractional quantum Hall effects.
  • Examination of systems with spontaneously broken time-reversal (TR) symmetry, including perturbed quantum Kagome antiferromagnets.
  • Study of vertex models where TR symmetry is preserved.

Main Results:

  • Quantized gravitational responses are identified as obstructions to local sign-free QMC.
  • These responses are linked to phenomena such as fractional quantum Hall effects in condensed matter.
  • Similar obstructions are shown to exist in systems with broken time-reversal symmetry.
  • The connection between gravitational responses and the sign problem is also observed in vertex models with preserved TR symmetry.

Conclusions:

  • Quantized gravitational responses present a fundamental obstruction to sign-free QMC simulations for certain quantum systems.
  • This finding clarifies limitations in simulating quantum systems classically, particularly those involving bosonic degrees of freedom.
  • The results have implications for understanding phenomena in condensed matter physics and developing more efficient quantum simulation algorithms.