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The Quantum-Mechanical Model of an Atom02:45

The Quantum-Mechanical Model of an Atom

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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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Quantum Numbers02:43

Quantum Numbers

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It is said that the energy of an electron in an atom is quantized; that is, it can be equal only to certain specific values and can jump from one energy level to another but not transition smoothly or stay between these levels.
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Fermi Level Dynamics01:12

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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.
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The de Broglie Wavelength02:32

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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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Ampere-Maxwell's Law: Problem-Solving01:17

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A parallel-plate capacitor with capacitance C, whose plates have area A and separation distance d, is connected to a resistor R and a battery of voltage V. The current starts to flow at t = 0. What is the displacement current between the capacitor plates at time t? From the properties of the capacitor, what is the corresponding real current?
To solve the problem, we can use the equations from the analysis of an RC circuit and Maxwell's version of Ampère's law.
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Superconductor01:24

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A substance that reaches superconductivity, a state in which magnetic fields cannot penetrate, and there is no electrical resistance, is referred to as a superconductor. In 1911, Heike Kamerlingh Onnes of Leiden University, a Dutch physicist, observed a relation between the temperature and the resistance of the element mercury. The mercury sample was then cooled in liquid helium to study the linear dependence of resistance on temperature. It was observed that, as the temperature decreased, the...
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Video Experimental Relacionado

Updated: Nov 6, 2025

Scalable Quantum Integrated Circuits on Superconducting Two-Dimensional Electron Gas Platform
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Caminos cuánticos en un procesador superconductor bidimensional programable de 62 qubits

Ming Gong1,2,3, Shiyu Wang1,2,3, Chen Zha1,2,3

  • 1Hefei National Laboratory for Physical Sciences at the Microscale and Department of Modern Physics, University of Science and Technology of China, Hefei 230026, China.

Science (New York, N.Y.)
|May 7, 2021
PubMed
Resumen
Este resumen es generado por máquina.

Los investigadores demostraron caminatas cuánticas de alta fidelidad en una matriz de qubits superconductores. Este avance en la simulación cuántica allana el camino para aplicaciones cuánticas a mayor escala.

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Área de la Ciencia:

  • La computación cuántica
  • Simulación Cuántica
  • Física de la materia condensada

Sus antecedentes:

  • Las caminatas cuánticas son análogos cuánticos de las caminatas aleatorias clásicas.
  • Son cruciales para las simulaciones cuánticas, los algoritmos de búsqueda y la computación cuántica universal.
  • Los qubits superconductores ofrecen una plataforma prometedora para implementar la dinámica cuántica.

Objetivo del estudio:

  • Diseñar y fabricar una matriz de qubits superconductores para experimentos de caminata cuántica.
  • Para demostrar caminatas cuánticas de una y dos partículas de alta fidelidad.
  • Implementar y estudiar los fenómenos de interferencia cuántica utilizando un interferómetro de Mach-Zehnder en el procesador cuántico.

Principales métodos:

  • Fabricación de una matriz de qubits superconductores cuadrados bidimensional de 8x8 con 62 qubits funcionales.
  • Demostración de caminatas cuánticas de una y dos partículas de alta fidelidad.
  • Implementación de un interferómetro programable de Mach-Zehnder para observar la interferencia cuántica.

Principales resultados:

  • Ejecución exitosa de alta fidelidad de caminatas cuánticas de una y dos partículas.
  • Observación de las franjas de interferencia con andadores individuales y dobles en el interferómetro Mach-Zehnder.
  • Demostración de la interferencia cuántica controlada por los trastornos de la ruta de ajuste.

Conclusiones:

  • El conjunto de qubits superconductores desarrollado permite demostraciones avanzadas de caminata cuántica.
  • Este trabajo representa un paso significativo hacia la realización de aplicaciones cuánticas a mayor escala en procesadores cuánticos de escala intermedia ruidosos.
  • La alta programabilidad facilita las simulaciones cuánticas complejas y los estudios de interferencia.