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Related Concept Videos

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...
¹H NMR: Interpreting Distorted and Overlapping Signals01:02

¹H NMR: Interpreting Distorted and Overlapping Signals

Spin systems where the difference in chemical shifts of the coupled nuclei is greater than ten times J are called first-order spin systems. These nuclei are weakly coupled, and their chemical shifts and coupling constant can generally be estimated from the well-separated signals in the spectrum.
As Δν decreases and the signals move closer, the doublets appear increasingly distorted. The intensities of the inner lines increase at the cost of those of the outer lines as the signals are slanted or...
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...
Scaling01:26

Scaling

In designing and analyzing filters, resonant circuits, or circuit analysis at large, working with standard element values like 1 ohm, 1 henry, or 1 farad can be convenient before scaling these values to more realistic figures. This approach is widely utilized by not employing realistic element values in numerous examples and problems; it simplifies mastering circuit analysis through convenient component values. The complexity of calculations is thereby reduced, with the understanding that...
Molecular Spectroscopy: Absorption and Emission01:14

Molecular Spectroscopy: Absorption and Emission

Molecules possess discrete energy levels called quantum states. Unlike atoms, which have simpler energy levels, molecules possess additional rotational and vibrational energy levels. Each energy level is separated by an energy gap, with the gaps between adjacent electronic, vibrational, and rotational levels varying significantly. The three types of energy levels in a diatomic molecule are shown in Figure 1.
Molecular Orbital Theory I02:35

Molecular Orbital Theory I

Overview of Molecular Orbital Theory

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Related Experiment Video

Updated: May 24, 2026

Excitonic Hamiltonians for Calculating Optical Absorption Spectra and Optoelectronic Properties of Molecular Aggregates and Solids
08:04

Excitonic Hamiltonians for Calculating Optical Absorption Spectra and Optoelectronic Properties of Molecular Aggregates and Solids

Published on: May 27, 2020

Linear-scaling quantum mechanical methods for excited states.

ChiYung Yam1, Qing Zhang, Fan Wang

  • 1Department of Chemistry, The University of Hong Kong, Hong Kong.

Chemical Society Reviews
|March 16, 2012
PubMed
Summary

Linear-scaling (O(N)) quantum mechanical methods enable excited-state calculations for large systems. Time-domain methods are more mature and stable than frequency-domain approaches for complex molecular dynamics.

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High Resolution Phonon-assisted Quasi-resonance Fluorescence Spectroscopy
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Last Updated: May 24, 2026

Excitonic Hamiltonians for Calculating Optical Absorption Spectra and Optoelectronic Properties of Molecular Aggregates and Solids
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Published on: May 27, 2020

High Resolution Phonon-assisted Quasi-resonance Fluorescence Spectroscopy
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High Resolution Phonon-assisted Quasi-resonance Fluorescence Spectroscopy

Published on: June 28, 2016

Area of Science:

  • Quantum mechanics
  • Computational chemistry
  • Theoretical chemistry

Background:

  • Traditional quantum mechanical methods struggle with scaling for large systems.
  • Excited-state calculations are crucial for understanding molecular properties and dynamics.
  • Linear-scaling (O(N)) methods offer a solution for computationally demanding systems.

Purpose of the Study:

  • To review recent advancements in linear-scaling (O(N)) quantum mechanical methods for excited states.
  • To categorize and compare time-domain and frequency-domain O(N) approaches.
  • To highlight the applicability and limitations of these methods for various response properties.

Main Methods:

  • Focus on locality-based O(N) methods for excited states.
  • Categorization into time-domain (real-time dynamics) and frequency-domain (electronic response) methods.
  • Discussion of the localized density matrix (LDM) method and time-dependent Kohn-Sham (TDKS) with non-orthogonal localized molecular orbitals (NOLMOs).

Main Results:

  • The localized density matrix (LDM) method is a mature O(N) approach implemented in both domains.
  • O(N) frequency-domain methods face convergence issues for resonant responses in most systems.
  • For linear response, LDM with Chebyshev expansion is efficient; for off-resonant nonlinear response, iterative frequency-domain methods are practical.
  • Time-domain methods are versatile for nonlinear responses but computationally expensive; O(N) semi-empirical methods offer a practical alternative.

Conclusions:

  • O(N) time-domain methods for excited states are more mature, stable, and widely applied than frequency-domain counterparts.
  • Time-domain methods are essential for investigating the dynamics of complex molecular systems.
  • The choice between time- and frequency-domain methods depends on the specific response property and system characteristics.