Jove
Visualize
Contact Us
JoVE
x logofacebook logolinkedin logoyoutube logo
ABOUT JoVE
OverviewLeadershipBlogJoVE Help Center
AUTHORS
Publishing ProcessEditorial BoardScope & PoliciesPeer ReviewFAQSubmit
LIBRARIANS
TestimonialsSubscriptionsAccessResourcesLibrary Advisory BoardFAQ
RESEARCH
JoVE JournalMethods CollectionsJoVE Encyclopedia of ExperimentsArchive
EDUCATION
JoVE CoreJoVE BusinessJoVE Science EducationJoVE Lab ManualFaculty Resource CenterFaculty Site
Terms & Conditions of Use
Privacy Policy
Policies

Related Concept Videos

Energy Carried By Electromagnetic Waves01:22

Energy Carried By Electromagnetic Waves

2.8K
Anyone who has used a microwave oven knows there is energy in electromagnetic waves. Sometimes, this energy is obvious, such as in the summer sun's warmth. At other times, it is subtle, such as the unfelt energy of gamma rays, which can destroy living cells. Electromagnetic waves bring energy into a system through their electric and magnetic fields. These fields can exert forces and move charges in the system and, thus, do work on them. However, there is energy in an electromagnetic wave,...
2.8K
Energy Associated With a Charge Distribution01:21

Energy Associated With a Charge Distribution

1.5K
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.
1.5K
The Energies of Atomic Orbitals03:21

The Energies of Atomic Orbitals

23.7K
In an atom, the negatively charged electrons are attracted to the positively charged nucleus. In a multielectron atom, electron-electron repulsions are also observed. The attractive and repulsive forces are dependent on the distance between the particles, as well as the sign and magnitude of the charges on the individual particles. When the charges on the particles are opposite, they attract each other. If both particles have the same charge, they repel each other.
23.7K
The Quantum-Mechanical Model of an Atom02:45

The Quantum-Mechanical Model of an Atom

41.8K
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.
41.8K
Thomson's e/m Experiment01:19

Thomson's e/m Experiment

3.2K
In a beam of charged particles created by a heated cathode, the particles move at different speeds. However, many applications need a beam with uniform particle speeds. An arrangement known as a velocity selector uses electric and magnetic fields to pick particles with a particular speed from the beam.
A particle with charge q, speed v, and mass m enters an area from the top, where the magnetic and electric fields are perpendicular both to the particle's motion and to one another. The...
3.2K
Electron Behavior01:09

Electron Behavior

7.8K
Electrons are negatively charged subatomic particles attracted to and orbit around the positively-charged nucleus of an atom. They reside in spaces associated with energy levels called shells and are further organized into subshells and orbitals within each shell.
Electrons Orbit the Nucleus
Electrons are found in specific locations outside of the nucleus. The shell in which an electron resides indicates the general energy level of the electron: those closer to the nucleus have less energy,...
7.8K

You might also read

Related Articles

Articles linked to this work by shared authors, journal, and citation graph.

Sort by
Same author

Revisiting Mitochondrial Temperature: Steady-State Heat Transfer or Non-Steady-State Dynamics?

Acta physiologica (Oxford, England)·2026
Same author

Publisher Correction: Titanium butoxide sol-gel structures are stabilized through water and alcohol via weak interactions: a DFT‑QTAIM study.

Journal of molecular modeling·2026
Same author

Titanium butoxide sol-gel structures are stabilized through water and alcohol via weak interactions: a DFT-QTAIM study.

Journal of molecular modeling·2026
Same author

Coumarin-Augmented Thiazole Hybrids as Dual Anticancer and Antibacterial Agents.

Chemical biology & drug design·2026
Same author

Alteration of metabolic activity regulates mitochondrial temperature in diagnosis in HepG2 hepatocellular carcinoma cells.

Scientific reports·2025
Same author

Decoding the Hot-Mitochondrion Paradox.

ArXiv·2025

Related Experiment Video

Updated: May 29, 2025

Energy Dispersive X-ray Tomography for 3D Elemental Mapping of Individual Nanoparticles
10:00

Energy Dispersive X-ray Tomography for 3D Elemental Mapping of Individual Nanoparticles

Published on: July 5, 2016

11.7K

The total energy from X-ray electron density?

Lou Massa1, Chérif F Matta2,3,4,5

  • 1Hunter College and the Graduate School, City University of New York, New York, NY, 10065, USA. lmassa@hunter.cuny.edu.

Journal of Molecular Modeling
|February 6, 2025
PubMed
Summary
This summary is machine-generated.

This study presents a fast and accurate quantum crystallography method for large systems, ensuring N-representable results. It guarantees quantum conditions are met while solving X-ray diffraction problems.

Keywords:
N-representabilityDensity matricesKernel energy method (KEM)Quantum crystallography

More Related Videos

Elemental-sensitive Detection of the Chemistry in Batteries through Soft X-ray Absorption Spectroscopy and Resonant Inelastic X-ray Scattering
07:55

Elemental-sensitive Detection of the Chemistry in Batteries through Soft X-ray Absorption Spectroscopy and Resonant Inelastic X-ray Scattering

Published on: April 17, 2018

12.6K
X-ray Beam Induced Current Measurements for Multi-Modal X-ray Microscopy of Solar Cells
00:10

X-ray Beam Induced Current Measurements for Multi-Modal X-ray Microscopy of Solar Cells

Published on: August 20, 2019

13.7K

Related Experiment Videos

Last Updated: May 29, 2025

Energy Dispersive X-ray Tomography for 3D Elemental Mapping of Individual Nanoparticles
10:00

Energy Dispersive X-ray Tomography for 3D Elemental Mapping of Individual Nanoparticles

Published on: July 5, 2016

11.7K
Elemental-sensitive Detection of the Chemistry in Batteries through Soft X-ray Absorption Spectroscopy and Resonant Inelastic X-ray Scattering
07:55

Elemental-sensitive Detection of the Chemistry in Batteries through Soft X-ray Absorption Spectroscopy and Resonant Inelastic X-ray Scattering

Published on: April 17, 2018

12.6K
X-ray Beam Induced Current Measurements for Multi-Modal X-ray Microscopy of Solar Cells
00:10

X-ray Beam Induced Current Measurements for Multi-Modal X-ray Microscopy of Solar Cells

Published on: August 20, 2019

13.7K

Area of Science:

  • Quantum crystallography
  • Computational chemistry
  • Solid-state physics

Background:

  • Ensures idempotency, hermiticity, and normalization of the one-body density matrix during X-ray diffraction.
  • N-representability is crucial for the variational theorem, mapping density matrices to N-body antisymmetric wavefunctions.
  • Antisymmetry aligns with the experimental indistinguishability of fermions.

Purpose of the Study:

  • Develop a procedure for fast and accurate quantum crystallography on large systems.
  • Guarantee N-representable results for quantum crystallography calculations.
  • Integrate quantum conditions with X-ray diffraction problem-solving.

Main Methods:

  • Utilizes the kernel energy method (KEM) to assemble the one-body density matrix from fragment sub-matrices for large molecules.
  • KEM approximates interactions up to two-body, ignoring higher orders, validated by past numerical testing.
  • Provides an explicit form of the N-representable two-body density matrix derived from the one-body counterpart for total energy calculations.

Main Results:

  • A procedure for fast and accurate N-representable quantum crystallography on large systems is developed.
  • The method simultaneously solves the X-ray diffraction problem and ensures quantum conditions.
  • Enables extraction of conceptual density functional theory and quantum theory of atoms in molecules properties from experimental structure factors.

Conclusions:

  • The developed quantum crystallography approach is efficient and accurate for large systems.
  • Guarantees N-representability and satisfaction of key quantum conditions.
  • Facilitates advanced chemical property analysis from experimental diffraction data.