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The Quantum-Mechanical Model of an Atom02:45

The Quantum-Mechanical Model of an Atom

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. Schrödinger...
Graphing the Wave Function01:13

Graphing the Wave Function

Consider the wave equation for a sinusoidal wave moving in the positive x-direction. The wave equation is a function of both position and time. From the wave equation, two different graphs can be plotted.
The de Broglie Wavelength02:32

The de Broglie Wavelength

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...
Equations of Wave Motion01:02

Equations of Wave Motion

Mathematically, the motion of a wave can be studied using a wavefunction. Consider a string oscillating up and down in simple harmonic motion, having a period T. The wave on the string is sinusoidal and is translated in the positive x-direction as time progresses. Sine is a function of the angle θ, oscillating between +A and −A and repeating every 2π radians. To construct a wave model, the ratio of the angle θ and the position x is considered.
The Uncertainty Principle04:08

The Uncertainty Principle

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 mathematically...
Velocity and Acceleration of a Wave00:51

Velocity and Acceleration of a Wave

A wave propagates through a medium with a constant speed, known as a wave velocity. It is different from the speed of the particles of the medium, which is not constant. In addition, the velocity of the medium is perpendicular to the velocity of the wave. The variable speed of the particles of the medium implies that there must be acceleration associated with it. 
The velocity of the particles can be obtained by taking the partial derivative of the position equation with respect to time. We can...

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Related Experiment Video

Updated: May 30, 2026

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

Efficient quantum trajectory representation of wavefunctions evolving in imaginary time.

Sophya Garashchuk1, James Mazzuca, Tijo Vazhappilly

  • 1Department of Chemistry and Biochemistry, University of South Carolina, Columbia, South Carolina 29208, USA. sgarashc@mail.chem.sc.edu

The Journal of Chemical Physics
|July 27, 2011
PubMed
Summary

Quantum trajectory simulations offer a new way to study quantum systems. This method recasts Boltzmann evolution into imaginary-time dynamics, improving efficiency for complex systems.

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Gradient Echo Quantum Memory in Warm Atomic Vapor
10:00

Gradient Echo Quantum Memory in Warm Atomic Vapor

Published on: November 11, 2013

Related Experiment Videos

Last Updated: May 30, 2026

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

Gradient Echo Quantum Memory in Warm Atomic Vapor
10:00

Gradient Echo Quantum Memory in Warm Atomic Vapor

Published on: November 11, 2013

Area of Science:

  • Quantum mechanics
  • Computational chemistry
  • Theoretical physics

Background:

  • The Boltzmann evolution of a wavefunction describes quantum system dynamics.
  • Quantum effects are influenced by a momentum-dependent quantum potential.
  • High-dimensional systems pose computational challenges.

Purpose of the Study:

  • To recast Boltzmann evolution as imaginary-time dynamics of quantum trajectories.
  • To analyze Lagrangian and Eulerian evolution for accuracy and practicality.
  • To develop improved trajectory dynamics for computational efficiency.

Main Methods:

  • Representing a nodeless wavefunction as ψ(x, t) = exp(-S(x, t)/ħ).
  • Defining trajectory momenta by ∇S(x, t).
  • Introducing stationary and time-dependent components into wavefunction representation.

Main Results:

  • Lagrangian dynamics are more accurate for bound potentials, but trajectories diverge.
  • Eulerian dynamics are more practical but less accurate over time.
  • Modified Lagrangian dynamics control trajectory spreading, enhancing efficiency.

Conclusions:

  • Quantum trajectory simulations provide a practical approach to quantum dynamics.
  • The developed dynamics improve the efficiency of describing quantum systems.
  • This method is applicable to calculating properties like zero-point energy and eigenstates.