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

Divergence and Curl of Electric Field01:25

Divergence and Curl of Electric Field

7.5K
The divergence of a vector is a measure of how much the vector spreads out (diverges) from a point. For example, an electric field vector diverges from the positive charge and converges at the negative charge. The divergence of an electric field is derived using Gauss's law and is equal to the charge density divided by the permittivity of space. Mathematically, it is expressed as
7.5K
The de Broglie Wavelength02:32

The de Broglie Wavelength

34.4K
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...
34.4K
Graphing the Wave Function01:13

Graphing the Wave Function

3.3K
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.
3.3K
Interference and Diffraction02:18

Interference and Diffraction

53.6K
Interference is a characteristic phenomenon exhibited by waves. When two electromagnetic waves interact with their peaks and troughs coinciding, a resulting wave with enhanced amplitude is produced. This is known as constructive interference. In this case, the two waves interacting are in phase with each other.
53.6K
Standing Waves in a Cavity01:28

Standing Waves in a Cavity

1.6K
A household microwave and lasers are examples of standing electromagnetic waves in a cavity. When two conducting metal plates are placed parallel at the nodal planes, it creates a cavity where standing waves are formed. The cavity between the two planes is analogous to a stretched string held at the points x = 0 and x = L. Here, the distance 'L' between the two planes must be an integer multiple of half of the wavelength. The wavelengths that satisfy this condition are given by:
1.6K
Electromagnetic Wave Equation01:24

Electromagnetic Wave Equation

2.5K
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:...
2.5K

You might also read

Related Articles

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

Sort by
Same author

Photoinduced Charge Transfer and Vibronic Coherence in CdSe Quantum Dots with Methyl Viologen Acceptors.

The journal of physical chemistry. C, Nanomaterials and interfacesĀ·2026
Same author

Simulating Electron Dynamics with GPU-Accelerated Real-Time Tamm-Dancoff Approximation.

Journal of chemical theory and computationĀ·2026
Same author

Excited-state vibronic coherences with mixing of core-ligand character promote hot-carrier cooling in oleate-capped CdSe quantum dots.

The Journal of chemical physicsĀ·2026
Same author

Leveraging Divergent Ligand-to-Metal Charge-Transfer Excited State Pathways for Catalyst Control over Alkoxyl Radical Reactivity.

Journal of the American Chemical SocietyĀ·2026
Same author

Ligand Control of Ultrafast Hot-Carrier Cooling in CdSe Quantum Dots by a Coherent Nonadiabatic Mechanism.

The journal of physical chemistry lettersĀ·2026
Same author

Conical intersections shed light on hot carrier cooling in quantum dots.

The Journal of chemical physicsĀ·2025
Same journal

Anharmonic phonons via quantum thermal bath simulations.

The Journal of chemical physicsĀ·2026
Same journal

Quantum simulation of alignment dependent differential cross sections in co-propagating molecular beams at cold collision energies.

The Journal of chemical physicsĀ·2026
Same journal

Non-additive ion effects on the coil-globule equilibrium of a generic polymer in aqueous salt solutions.

The Journal of chemical physicsĀ·2026
Same journal

Insights into the unexpected small reduction of the temperature of maximum density of water by lithium chloride addition.

The Journal of chemical physicsĀ·2026
Same journal

Optical frequency comb double-resonance spectroscopy of the 9030-9175Ā cm-1 states of ethylene.

The Journal of chemical physicsĀ·2026
Same journal

Time reversal breaking of colloidal particles in cells.

The Journal of chemical physicsĀ·2026
See all related articles

Related Experiment Video

Updated: Mar 21, 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

9.8K

Wave function continuity and the diagonal Born-Oppenheimer correction at conical intersections.

Garrett A Meek1, Benjamin G Levine1

  • 1Department of Chemistry, Michigan State University, East Lansing, Michigan 48824, USA.

The Journal of Chemical Physics
|May 16, 2016
PubMed
Summary
This summary is machine-generated.

The expansion of molecular wave functions using adiabatic Born-Oppenheimer states creates problematic singularities when including nonadiabatic energy terms near conical intersections, suggesting these corrections should be neglected in certain quantum dynamics methods.

More Related Videos

Probe Type II Band Alignment in One-Dimensional Van Der Waals Heterostructures Using First-Principles Calculations
13:56

Probe Type II Band Alignment in One-Dimensional Van Der Waals Heterostructures Using First-Principles Calculations

Published on: October 12, 2019

8.4K
Measurement of Quantum Interference in a Silicon Ring Resonator Photon Source
12:19

Measurement of Quantum Interference in a Silicon Ring Resonator Photon Source

Published on: April 4, 2017

8.9K

Related Experiment Videos

Last Updated: Mar 21, 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

9.8K
Probe Type II Band Alignment in One-Dimensional Van Der Waals Heterostructures Using First-Principles Calculations
13:56

Probe Type II Band Alignment in One-Dimensional Van Der Waals Heterostructures Using First-Principles Calculations

Published on: October 12, 2019

8.4K
Measurement of Quantum Interference in a Silicon Ring Resonator Photon Source
12:19

Measurement of Quantum Interference in a Silicon Ring Resonator Photon Source

Published on: April 4, 2017

8.9K

Area of Science:

  • Quantum chemistry
  • Molecular dynamics
  • Theoretical chemistry

Background:

  • The adiabatic Born-Oppenheimer (BO) approximation is a cornerstone of molecular quantum mechanics.
  • Conical intersections are critical features in molecular potential energy surfaces where the BO approximation breaks down.
  • Calculating nonadiabatic effects is essential for accurately describing molecular dynamics.

Purpose of the Study:

  • To investigate the practical challenges of including second-derivative nonadiabatic energy terms in molecular wave function expansions.
  • To analyze the origin and implications of singularities arising from these terms near conical intersections.
  • To provide recommendations for handling nonadiabatic corrections in quantum dynamics simulations.

Main Methods:

  • Expansion of the total molecular wave function over adiabatic BO vibronic states.
  • Analysis of the second-derivative nonadiabatic coupling terms and their effect on diagonal BO corrections (DBOCs).
  • Classification and formal analysis of nonadiabatic molecular dynamics methods based on wave function continuity constraints.

Main Results:

  • The inclusion of second-derivative nonadiabatic terms leads to non-integrable singularities in DBOCs due to discontinuities in individual BO states.
  • These singularities are artifacts of the chosen basis set and do not imply a physical constraint on wave function density at conical intersections.
  • Continuity of the total molecular wave function does not necessitate continuity of individual adiabatic nuclear wave functions.

Conclusions:

  • The singularities in DBOCs are mathematical artifacts and should not be interpreted as physical limitations.
  • Neglecting DBOCs is recommended for mixed quantum-classical and certain approximate quantum dynamical methods in the adiabatic representation.
  • A re-evaluation of wave function continuity constraints in nonadiabatic dynamics methods is warranted.