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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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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 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...
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Atomic Nuclei: Nuclear Relaxation Processes01:23

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In the absence of an external magnetic field, nuclear spin states are degenerate and randomly oriented. When a magnetic field is applied, the spins begin to precess and orient themselves along (lower energy) or against (higher energy) the direction of the field. At equilibrium, a slight excess population of spins exists in the lower energy state. Because the direction of the magnetic field is fixed as the z-axis,  the precessing magnetic moments are randomly oriented around the z-axis.
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Electron Behavior01:09

Electron Behavior

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Electrons are negatively charged subatomic particles attracted to and orbit around the positively-charged nucleus of an atom. They reside in spaces associated with energy levels called shells and are further organized into subshells and orbitals within each shell.
Electrons Orbit the Nucleus
Electrons are found in specific locations outside of the nucleus. The shell in which an electron resides indicates the general energy level of the electron: those closer to the nucleus have less energy,...
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Fermi Level Dynamics01:12

Fermi Level Dynamics

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The vacuum level denotes the energy threshold required for an electron to escape from a material surface. It is usually positioned above the conduction band of a semiconductor and acts as a benchmark for comparing electron energies within various materials.
Electron affinity in semiconductors refers to the energy gap between the minimum of its conduction band and the vacuum level and it is a critical parameter in determining how easily a semiconductor can accept additional electrons.
The work...
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Updated: May 1, 2026

Setting Limits on Supersymmetry Using Simplified Models
07:46

Setting Limits on Supersymmetry Using Simplified Models

Published on: November 16, 2013

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La difusión cuántica en el modelo de Harper bajo una perturbación de tiempo policromática.

Hiroaki S Yamada1, Kensuke S Ikeda2

  • 1Yamada Physics Research Laboratory, Aoyama 5-7-14-205, Niigata 950-2002, Japan.

Physical review. E
|February 20, 2026
PubMed
Resumen
Este resumen es generado por máquina.

La adición de múltiples frecuencias al modelo de Harper transforma los estados localizados en estados difusos cuánticos. Esta transición a la difusión ocurre a medida que aumenta la fuerza de la perturbación para tres o más frecuencias inconmensurables.

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Área de la Ciencia:

  • La mecánica cuántica es la mecánica cuántica.
  • Física de la materia condensada Física de la materia condensada Física de la materia condensada Física de la materia condensada Física de la materia condensada

Sus antecedentes:

  • El modelo de Harper describe la dinámica cuántica en un campo magnético.
  • Sus estados pueden ser localizados, difusos o balísticos, influenciados por la fuerza potencial (V).

Objetivo del estudio:

  • Para investigar el efecto de las perturbaciones armónicas dependientes del tiempo en la dinámica del modelo de Harper.
  • Determinar las condiciones bajo las cuales diferentes estados cuánticos pasan a estados difusos.

Principales métodos:

  • Aplicación de perturbaciones armónicas dependientes del tiempo con frecuencias M incommensurables al modelo de Harper.
  • Analizando la dinámica cuántica resultante y las transiciones de estado.
  • Mapeo del diagrama de fase en el espacio de parámetros (ε,V).

Principales resultados:

  • Todos los estados del modelo de Harper pasan a estados difusos cuánticos a medida que la fuerza de perturbación (ε) aumenta para M≥3.3.
  • Los esquemas de transición y los comportamientos de difusión dependen de ε y V.
  • Se presenta un diagrama de fase que ilustra estas transiciones.

Conclusiones:

  • Las perturbaciones dependientes del tiempo con suficientes frecuencias inconmensuradas pueden impulsar la difusión cuántica libre de localización.
  • La dinámica del modelo de Harper es altamente sensible a las perturbaciones externas dependientes del tiempo.