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相关概念视频

The Quantum-Mechanical Model of an Atom02:45

The Quantum-Mechanical Model of an Atom

42.3K
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.
34.7K
Biot-Savart Law: Problem-Solving00:59

Biot-Savart Law: Problem-Solving

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The magnitude and direction of a magnetic field created by a steady current can be calculated using the Biot-Savart law.
Consider a mobile phone battery bank as a source of steady current, which flows through the wire connected between the two. What is the magnitude of the magnetic field created by this current at a field point P?
To estimate the magnitude of the total magnetic field, we first consider a small current element of length dl, at a distance r from the field point. Now the following...
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Maxwell-Boltzmann Distribution: Problem Solving01:20

Maxwell-Boltzmann Distribution: Problem Solving

1.5K
Individual molecules in a gas move in random directions, but a gas containing numerous molecules has a predictable distribution of molecular speeds, which is known as the Maxwell-Boltzmann distribution, f(v).
This distribution function f(v) is defined by saying that the expected number N (v1,v2) of particles with speeds between v1 and v2 is given by
1.5K
Fermi Level Dynamics01:12

Fermi Level Dynamics

243
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...
243
The Pauli Exclusion Principle03:06

The Pauli Exclusion Principle

36.6K
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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Large Scale Energy Efficient Sensor Network Routing Using a Quantum Processor Unit
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在量子计算机上对资源进行元优化.

Ijaz Ahamed Mohammad1, Matej Pivoluska1, Martin Plesch2,3,4,5

  • 1Institute of Physics, Slovak Academy of Sciences, Dúbravská cesta 9, 841 04, Bratislava, Slovak Republic.

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|May 5, 2024
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概括
此摘要是机器生成的。

这项研究介绍了混合量子-经典算法的元优化,以提高噪音中等规模量子时代的资源效率. 该方法优化量子计算机运行,用于诸如分子基态能量计算等任务.

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科学领域:

  • 量子计算是一种量子计算.
  • 计算化学的计算化学

背景情况:

  • 目前的量子计算机在杂的中级量子 (NISQ) 时代运行,量子位和操作有限.
  • 在NISQ设备中的噪音很快就会删除编码的信息,将量子计算机应用限制在简短,简单的任务中,作为经典算法的子程序.

研究的目的:

  • 为混合量子-经典算法提出一个一般的元优化程序.
  • 通过优化利用有限的量子计算能力来提高资源效率.

主要方法:

  • 为混合量子-经典算法开发了一个元优化框架.
  • 通过优化对变量量子算法的资源使用来测试程序的有效性.
  • 应用了计算分子基本状态能量的方法.

主要成果:

  • 超优化程序有效地确定了混合算法的最佳方法.
  • 在量子计算中证明了提高资源效率.
  • 成功应用于一个实际的量子化学问题.

结论:

  • 拟议的元优化对于最大限度地提高NISQ设备的效用至关重要.
  • 高效的资源利用是近期量子应用的一个关键参数.
  • 这种方法使量子子程序在复杂的古典程序中能够更有效地使用.