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The de Broglie Wavelength02:32

The de Broglie Wavelength

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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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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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The Uncertainty Principle04:08

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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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The Pauli Exclusion Principle03:06

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The arrangement of electrons in the orbitals of an atom is called its electron configuration. We describe an electron configuration with a symbol that contains three pieces of information:
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¹³C NMR: ¹H–¹³C Decoupling01:04

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The probability of having two carbon-13 atoms next to each other is negligible because of the low natural abundance of carbon-13. Consequently, peak splitting due to carbon-carbon spin-spin coupling is not observed in spectra. However, protons up to three sigma bonds away split the carbon signal according to the n+1 rule, resulting in complicated spectra.
A broadband decoupling technique is used to simplify these complex, sometimes overlapping, signals. Broadband decoupling relies on a...
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The Bohr Model02:18

The Bohr Model

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Following the work of Ernest Rutherford and his colleagues in the early twentieth century, the picture of atoms consisting of tiny dense nuclei surrounded by lighter and even tinier electrons continually moving about the nucleus was well established. This picture was called the planetary model since it pictured the atom as a miniature “solar system” with the electrons orbiting the nucleus like planets orbiting the sun. The simplest atom is hydrogen, consisting of a single proton as...
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Related Experiment Video

Updated: Oct 6, 2025

Generation and Coherent Control of Pulsed Quantum Frequency Combs
06:42

Generation and Coherent Control of Pulsed Quantum Frequency Combs

Published on: June 8, 2018

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Does Decoherence Select the Pointer Basis of a Quantum Meter?

Abraham G Kofman1, Gershon Kurizki1

  • 1Department of Chemical and Biological Physics, Weizmann Institute of Science, Rehovot 761001, Israel.

Entropy (Basel, Switzerland)
|January 21, 2022
PubMed
Summary
This summary is machine-generated.

Environmental decoherence does not always determine the quantum measurement pointer basis. Observers can choose alternative bases for generalized measurements, impacting quantum mechanics interpretations.

Keywords:
Quantum Lamarckismdecoherencepointer statesquantum measurementsthe observer in quantum mechanics

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Last Updated: Oct 6, 2025

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Area of Science:

  • Quantum Physics
  • Measurement Theory

Background:

  • Standard quantum measurement theory posits that environmental decoherence determines the measurement basis.
  • The environment monitors selected observables, forcing quantum states into persistent pointer states.

Purpose of the Study:

  • To investigate whether environmental decoherence unambiguously determines the pointer basis in quantum measurements.
  • To explore the role of generalized measurements and observer choice in quantum measurement theory.

Main Methods:

  • Analysis of quantum measurement theory, focusing on generalized measurements beyond projective measurements.
  • Examination of the influence of environmental decoherence on the selection of pointer bases.

Main Results:

  • Decoherence does not necessarily determine the pointer basis for generalized quantum measurements.
  • Multiple alternative pointer bases can provide the same information, irrespective of decoherence.
  • The choice of observable for measurement is independent of the pointer basis.

Conclusions:

  • Quantum measurement outcomes are not solely determined by decoherence; observer choice plays a crucial role.
  • Findings support the concept of Quantum Lamarckism, emphasizing the observer's active role in quantum mechanics.