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Fermi Level Dynamics01:12

Fermi Level Dynamics

364
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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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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Free Energy Changes for Nonstandard States03:25

Free Energy Changes for Nonstandard States

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The free energy change for a process taking place with reactants and products present under nonstandard conditions (pressures other than 1 bar; concentrations other than 1 M) is related to the standard free energy change according to this equation:
 
where R is the gas constant (8.314 J/K·mol), T is the absolute temperature in kelvin, and Q is the reaction quotient. This equation may be used to predict the spontaneity of a process under any given set of conditions.
Reaction Quotient...
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Energy Associated With a Charge Distribution01:21

Energy Associated With a Charge Distribution

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The work done to bring a charge through a distance r is given by the potential difference between the initial and the final position. To assemble a collection of point charges, the total work done can be expressed in terms of the product of each pair of charges divided by their separation distance, defined with respect to a suitable origin. Solving this expression gives the energy stored in a point charge distribution.
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The Bohr Model02:18

The Bohr Model

69.4K
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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Electromagnetic Wave Equation01:24

Electromagnetic Wave Equation

1.4K
Maxwell's equations for electromagnetic fields are related to source charges, either static or moving. These fields act on a test charge, whose trajectory can thus be determined using suitable boundary conditions. The objective of electromagnetism is thus theoretically complete.
However, although electric and magnetic fields were first introduced as mathematical constructs to simplify the description of mutual forces between charges, a natural question emerges from Maxwell's equations:...
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Updated: Sep 24, 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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Electronic energies from coupled fermionic "Zombie" states' imaginary time evolution.

Oliver A Bramley1, Timothy J H Hele2, Dmitrii V Shalashilin1

  • 1School of Chemistry, University of Leeds, Leeds LS2 9JT, United Kingdom.

The Journal of Chemical Physics
|May 7, 2022
PubMed
Summary
This summary is machine-generated.

Zombie states offer a computationally efficient method for simulating fermionic systems, addressing the fermionic sign problem. New algorithms improve accuracy and enable calculation of ground and excited states, potentially rivaling quantum Monte Carlo methods.

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Area of Science:

  • Quantum Chemistry
  • Computational Physics
  • Many-Body Theory

Background:

  • Zombie states provide a novel formalism for coupled coherent fermionic states.
  • This approach aims to overcome the computational challenges posed by the fermionic sign problem.
  • Prior work demonstrated Zombie states' adherence to fermionic algebra and their utility in real-time evolution.

Purpose of the Study:

  • To develop efficient algorithms for Hamiltonian and operator evaluation within the Zombie state formalism.
  • To address the normalization of Zombie states and enable accurate ground and excited state calculations.
  • To introduce methods for improving computational efficiency and accuracy, such as biasing and wave function cleaning.

Main Methods:

  • Development of efficient algorithms for evaluating operators between Zombie states.
  • Implementation of imaginary time propagation for ground state determination.
  • Introduction of a biasing method for constructing efficient random Zombie state basis sets.
  • Application of wave function cleaning to remove erroneous electron configurations.
  • Utilizing Gram-Schmidt orthogonalization for efficient excited state calculations.

Main Results:

  • Efficient algorithms for Hamiltonian and operator evaluation in Zombie state formalism were developed.
  • Imaginary time propagation successfully determined system ground states.
  • A biasing method significantly reduced basis set size while maintaining accuracy.
  • Wave function cleaning enhanced the precision of electronic structure calculations.
  • Low-lying excited states were computed efficiently via Gram-Schmidt orthogonalization.

Conclusions:

  • The extended Zombie state formalism offers efficient and accurate methods for fermionic system simulations.
  • Imaginary time propagation on biased random Zombie state grids presents a viable alternative to quantum Monte Carlo methods.
  • The developed techniques enhance the computational tractability and accuracy of simulating complex fermionic systems.