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 Bands in Solids01:01

Energy Bands in Solids

Isolated atoms have discrete energy levels that are well described by the Bohr model. And, it quantifies the energy of an electron in a hydrogen atom as En. Higher quantum numbers 'n' yield less negative, closer electron energy levels.
 Band Formation:
When atoms are brought close together, as in a solid, these discrete energy levels begin to split due to the overlap of electron orbitals from adjacent atoms. This split occurs because of the Pauli exclusion principle, which states that no two...
Electron Configurations02:46

Electron Configurations

Electron configurations and orbital diagrams can be determined by applying the Aufbau principle (each added electron occupies the subshell of lowest energy available), Pauli exclusion principle (no two electrons can have the same set of four quantum numbers), and Hund’s rule of maximum multiplicity (whenever possible, electrons retain unpaired spins in degenerate orbitals).
The relative energies of the subshells determine the order in which atomic orbitals are filled (1s, 2s, 2p, 3s, 3p, 4s,...
Atomic Orbitals02:44

Atomic Orbitals

An atomic orbital represents the three-dimensional regions in an atom where an electron has the highest probability to reside. The radial distribution function indicates the total probability of finding an electron within the thin shell at a distance r from the nucleus. The atomic orbitals have distinct shapes which are determined by l, the angular momentum quantum number. The orbitals are often drawn with a boundary surface, enclosing densest regions of the cloud.
Electron Configuration of Multielectron Atoms03:26

Electron Configuration of Multielectron Atoms

The alkali metal sodium (atomic number 11) has one more electron than the neon atom. This electron must go into the lowest-energy subshell available, the 3s orbital, giving a 1s22s22p63s1 configuration. The electrons occupying the outermost shell orbital(s) (highest value of n) are called valence electrons, and those occupying the inner shell orbitals are called core electrons. Since the core electron shells correspond to noble gas electron configurations, we can abbreviate electron...
Electron Orbital Model01:18

Electron Orbital Model

Orbitals are the areas outside of the atomic nucleus where electrons are most likely to reside. They are characterized by different energy levels, shapes, and three-dimensional orientations. The location of electrons is described most generally by a shell or principal energy level, then by a subshell within each shell, and finally, by individual orbitals found within the subshells.The first shell is closest to the nucleus, and it has only one subshell with a single spherical orbital called the...
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...

You might also read

Related Articles

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

Sort by
Same author

A Reproducible Workflow for Modelling of <sup>1</sup>H to <sup>13</sup>C Polarization Transfer Kinetics Using Solid-State NMR.

Magnetic resonance in chemistry : MRC·2026
Same author

Is mesh pore size associated with the outcome in laparo-endoscopic inguinal hernia repair? - a registry-based multivariable analysis.

Hernia : the journal of hernias and abdominal wall surgery·2024
Same author

[Interstitial lung diseases : From imaging to treatment].

Radiologie (Heidelberg, Germany)·2024
Same author

Statins did not reduce the frequency of exacerbations in individuals with COPD and cardiovascular comorbidities in the COSYCONET cohort.

Respiratory research·2024
Same author

Laparoscopic total (Nissen) versus posterior (Toupet) fundoplication for gastroesophageal reflux disease: a propensity score-matched comparison of the perioperative and 1-year follow-up outcome.

Hernia : the journal of hernias and abdominal wall surgery·2024
Same author

Unraveling determinants of integrated farming systems adoption for sustainable livelihood and dietary diversity.

Frontiers in nutrition·2024

Related Experiment Video

Updated: Jul 7, 2026

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

Localized basis sets for unbound electrons in nanoelectronics.

D Soriano1, D Jacob, J J Palacios

  • 1Departamento de Física Aplicada, Universidad de Alicante, San Vicente del Raspeig, Alicante, Spain. dsh2@alu.ua.es

The Journal of Chemical Physics
|February 27, 2008
PubMed
Summary

Localized basis sets can expand unbound electron wave functions for various energies. Gaussian basis sets show potential for describing field emission and scanning tunneling microscopy, as demonstrated by H atom electron lifetime studies under electric fields.

More Related Videos

Atomically Traceable Nanostructure Fabrication
12:35

Atomically Traceable Nanostructure Fabrication

Published on: July 17, 2015

Rapid in-silico Battery Electrolyte Electrochemical Reaction Generation using 3T-VASP Multi-Scale Energy Minimization
05:37

Rapid in-silico Battery Electrolyte Electrochemical Reaction Generation using 3T-VASP Multi-Scale Energy Minimization

Published on: August 22, 2025

Related Experiment Videos

Last Updated: Jul 7, 2026

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

Atomically Traceable Nanostructure Fabrication
12:35

Atomically Traceable Nanostructure Fabrication

Published on: July 17, 2015

Rapid in-silico Battery Electrolyte Electrochemical Reaction Generation using 3T-VASP Multi-Scale Energy Minimization
05:37

Rapid in-silico Battery Electrolyte Electrochemical Reaction Generation using 3T-VASP Multi-Scale Energy Minimization

Published on: August 22, 2025

Area of Science:

  • Quantum mechanics
  • Computational chemistry
  • Atomic physics

Background:

  • Unbound electron wave functions are crucial for understanding phenomena like field emission and scanning tunneling microscopy.
  • Localized basis sets are commonly employed in first-principles calculations.
  • Gaussian basis sets are a popular choice for these calculations due to their efficiency.

Purpose of the Study:

  • To demonstrate the expansion of unbound electron wave functions using localized basis sets.
  • To investigate the applicability of Gaussian basis sets for describing electron behavior in strong electric fields.
  • To illustrate the potential use of these methods in advanced microscopy techniques.

Main Methods:

  • Expansion of unbound electron wave functions in localized basis sets.
  • Utilizing Gaussian basis sets for the expansion.
  • Studying the lifetime of an electron in a hydrogen atom under a strong electric field as a model system.

Main Results:

  • Successfully demonstrated the expansion of unbound electron wave functions across a range of energies.
  • Gaussian basis sets proved effective in the model system.
  • The study provides insights into electron behavior under strong electric fields.

Conclusions:

  • Localized Gaussian basis sets are a viable tool for expanding unbound electron wave functions.
  • These methods hold promise for first-principles descriptions of field emission and scanning tunneling microscopy.
  • Further research can explore these techniques in more complex systems.