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

Types of Semiconductors01:20

Types of Semiconductors

1.8K
Intrinsic semiconductors are highly pure materials with no impurities. At absolute zero, these semiconductors behave as perfect insulators because all the valence electrons are bound, and the conduction band is empty, disallowing electrical conduction. The Fermi level is a concept used to describe the probability of occupancy of energy levels by electrons at thermal equilibrium. In intrinsic semiconductors, the Fermi level is positioned at the midpoint of the energy gap at absolute zero. When...
1.8K
Fermi Level Dynamics01:12

Fermi Level Dynamics

1.1K
The vacuum level denotes the energy threshold required for an electron to escape from a material surface. It is usually positioned above the conduction band of a semiconductor and acts as a benchmark for comparing electron energies within various materials.
Electron affinity in semiconductors refers to the energy gap between the minimum of its conduction band and the vacuum level and it is a critical parameter in determining how easily a semiconductor can accept additional electrons.
The work...
1.1K
Semiconductors01:22

Semiconductors

1.9K
There is variation in the electrical conductivity of materials - metals, semiconductors, and insulators that are showcased with the help of the energy band diagrams.
Metals such as copper (Cu), zinc (Zn), or lead (Pb) have low resistivity and feature conduction bands that are either not fully occupied or overlap with the valence band, making a bandgap non-existent. This allows electrons in the highest energy levels of the valence band to easily transition to the conduction band upon gaining...
1.9K
Metal-Semiconductor Junctions01:24

Metal-Semiconductor Junctions

1.4K
The contact of metal and semiconductor can lead to the formation of a junction with either Schottky or Ohmic behavior.
Schottky Barriers
Schottky barriers arise when a metal with a work function (Φm) contacts a semiconductor with a different work function (Φs). Initially, electrons transfer until the Fermi levels of the metal and semiconductor align at equilibrium. For instance, if Φm > Φs, the semiconductor Fermi level is higher than the metal's before contact. The...
1.4K
P-N junction01:11

P-N junction

1.7K
A p-n junction is formed when p-type and n-type semiconductor materials are joined together. At the interface of the p-n junction, holes from the p-side and electrons from the n-side begin to diffuse into the opposite sides due to the concentration gradient. This diffusion of carriers leads to a region around the junction where there are no free charge carriers, known as the depletion region. The charge density within the depletion region for the n-side and p-side can be described by the...
1.7K
Fermi Level01:18

Fermi Level

2.6K
The Fermi-Dirac function is represented by an S-shaped curve indicating the probability of an energy state being occupied by an electron at a given temperature. The Fermi level is the energy level at which there is a fifty percent chance of finding an electron, and it is positioned between the lower-energy valence band and the higher-energy conduction band.
At absolute zero temperature, electrons fill all energy states up to the Fermi level, leaving upper states empty. As the temperature rises,...
2.6K

You might also read

Related Articles

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

Sort by
Same author

Mitochondrial transcription factor A (TFAM) polymorphisms and risk of late-onset Alzheimer's disease in Han Chinese.

Brain research·2010
Same author

[Central mechanism of electric-acupuncture at Zusanli (ST36) for gastric mucous membrane protection with FMRI].

Zhonghua yi xue za zhi·2010
Same author

[Clinical application of review criteria for complete blood analysis].

Zhonghua yi xue za zhi·2010
Same author

Rhizosphere characteristics of zinc hyperaccumulator Sedum alfredii involved in zinc accumulation.

Journal of hazardous materials·2010
Same author

Rosmarinic acid antagonized 1-methyl-4-phenylpyridinium (MPP+)-induced neurotoxicity in MES23.5 dopaminergic cells.

International journal of toxicology·2010
Same author

Evaluation of sphingolipid metabolism in renal cortex of rats with streptozotocin-induced diabetes and the effects of rapamycin.

Nephrology, dialysis, transplantation : official publication of the European Dialysis and Transplant Association - European Renal Association·2010

Related Experiment Video

Updated: May 6, 2026

All-electronic Nanosecond-resolved Scanning Tunneling Microscopy: Facilitating the Investigation of Single Dopant Charge Dynamics
11:33

All-electronic Nanosecond-resolved Scanning Tunneling Microscopy: Facilitating the Investigation of Single Dopant Charge Dynamics

Published on: January 19, 2018

8.3K

Ionization potentials of semiconductors from first-principles.

Hong Jiang1, Yu-Chen Shen

  • 1Beijing National Laboratory for Molecular Sciences, State Key Laboratory of Rare Earth Materials Chemistry and Applications, Institute of Theoretical and Computational Chemistry, College of Chemistry and Molecular Engineering, Peking University, 100871 Beijing, China.

The Journal of Chemical Physics
|November 5, 2013
PubMed
Summary
This summary is machine-generated.

Determining semiconductor ionization potentials is crucial for surface properties. While standard methods underestimate these values, GW approximation significantly improves accuracy, with the Valence Band Maximum (VBM) scheme outperforming others.

More Related Videos

Silicon Metal-oxide-semiconductor Quantum Dots for Single-electron Pumping
14:58

Silicon Metal-oxide-semiconductor Quantum Dots for Single-electron Pumping

Published on: June 3, 2015

18.0K
Electric-field Control of Electronic States in WS2 Nanodevices by Electrolyte Gating
10:36

Electric-field Control of Electronic States in WS2 Nanodevices by Electrolyte Gating

Published on: April 12, 2018

10.6K

Related Experiment Videos

Last Updated: May 6, 2026

All-electronic Nanosecond-resolved Scanning Tunneling Microscopy: Facilitating the Investigation of Single Dopant Charge Dynamics
11:33

All-electronic Nanosecond-resolved Scanning Tunneling Microscopy: Facilitating the Investigation of Single Dopant Charge Dynamics

Published on: January 19, 2018

8.3K
Silicon Metal-oxide-semiconductor Quantum Dots for Single-electron Pumping
14:58

Silicon Metal-oxide-semiconductor Quantum Dots for Single-electron Pumping

Published on: June 3, 2015

18.0K
Electric-field Control of Electronic States in WS2 Nanodevices by Electrolyte Gating
10:36

Electric-field Control of Electronic States in WS2 Nanodevices by Electrolyte Gating

Published on: April 12, 2018

10.6K

Area of Science:

  • Solid-state physics
  • Materials science
  • Computational chemistry

Background:

  • Ionization potential (IP) is critical for absolute band edge alignment with vacuum.
  • Accurate theoretical determination of IPs is less developed than for band gaps.
  • Semiconductor surface and interface properties heavily depend on band alignment.

Purpose of the Study:

  • To evaluate state-of-the-art first-principles methods for semiconductor ionization potentials.
  • To compare Kohn-Sham density functional theory (LDA/GGA) with many-body perturbation theory (GW approximation).
  • To critically assess two GW correction schemes: Valence Band Maximum (VBM) and Band Gap Center (BGC).

Main Methods:

  • First-principles calculations using Kohn-Sham density functional theory (LDA/GGA).
  • Application of many-body perturbation theory within the GW approximation for quasi-particle corrections.
  • Comparative analysis of the VBM and BGC GW correction schemes.

Main Results:

  • LDA/GGA methods generally underestimate semiconductor ionization potentials.
  • GW approximation significantly improves agreement between theoretical and experimental IPs.
  • The VBM scheme demonstrates superior theoretical foundation and practical agreement compared to the BGC scheme.
  • For materials with shallow semicore states, GW still shows discrepancies, suggesting limitations.

Conclusions:

  • GW approximation, particularly the VBM scheme, is a reliable approach for calculating semiconductor ionization potentials.
  • Standard LDA/GGA methods are insufficient for accurate IP determination.
  • Further theoretical advancements beyond standard GW are needed for specific semiconductor classes (e.g., those with shallow semicore states).