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

Ionic Bonding and Electron Transfer02:48

Ionic Bonding and Electron Transfer

53.9K
Ions are atoms or molecules bearing an electrical charge. A cation (a positive ion) forms when a neutral atom loses one or more electrons from its valence shell, and an anion (a negative ion) forms when a neutral atom gains one or more electrons in its valence shell. Compounds composed of ions are called ionic compounds (or salts), and their constituent ions are held together by ionic bonds: electrostatic forces of attraction between oppositely charged cations and anions. 
53.9K
The Electrical Double Layer01:30

The Electrical Double Layer

154
In the region where two bulk phases meet, an intricate electric charge distribution arises due to charge transfer, ion adsorption, molecular orientation, and charge distortion. This complex distribution is commonly referred to as the electrical double layer.When a solid electrode interfaces with ions in an electrolyte solution, the speed of electron transfer dictates the rates of oxidation and reduction. The electrode acquires a charge through the escape of atoms into the solution as cations or...
154
Imperfections in Crystal Structure: Stoichiometric Point Defects01:26

Imperfections in Crystal Structure: Stoichiometric Point Defects

85
Schottky defects arise when some lattice points in a crystal, such as those in NaCl, remain unoccupied, creating lattice vacancies without disturbing the overall electrical neutrality of the crystal. This defect is common in ionic crystals where the positive and negative ions are similar in size, as seen in sodium chloride and cesium chloride. The presence of Schottky defects enables the crystal to conduct electricity to a small extent through an ionic mechanism. Electric fields cause nearby...
85
Crystal Field Theory - Octahedral Complexes02:58

Crystal Field Theory - Octahedral Complexes

31.7K
Crystal Field Theory
To explain the observed behavior of transition metal complexes (such as colors), a model involving electrostatic interactions between the electrons from the ligands and the electrons in the unhybridized d orbitals of the central metal atom has been developed. This electrostatic model is crystal field theory (CFT). It helps to understand, interpret, and predict the colors, magnetic behavior, and some structures of coordination compounds of transition metals.
CFT focuses on...
31.7K
Metal-Semiconductor Junctions01:24

Metal-Semiconductor Junctions

1.3K
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...
1.3K
Metallic Solids02:37

Metallic Solids

21.3K
Metallic solids such as crystals of copper, aluminum, and iron are formed by metal atoms. The structure of metallic crystals is often described as a uniform distribution of atomic nuclei within a “sea” of delocalized electrons. The atoms within such a metallic solid are held together by a unique force known as metallic bonding that gives rise to many useful and varied bulk properties.
All metallic solids exhibit high thermal and electrical conductivity, metallic luster, and malleability....
21.3K

You might also read

Related Articles

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

Sort by
Same author

Gigantic Nonreciprocal Conduction at a Polar-Magnetic Interface of GdTiO_{3}/EuTiO_{3}.

Physical review letters·2026
Same author

Characteristics and effects of depth of anaesthesia on late motor responses.

Clinical neurophysiology : official journal of the International Federation of Clinical Neurophysiology·2026
Same author

Coexistence of Insulatorlike Paramagnon and Metallic Spin-Orbit Exciton Modes in SrIrO_{3}.

Physical review letters·2025
Same author

Exercise facilitates post-stroke recovery through mitigation of neuronal hyperexcitability via interleukin-10 signaling.

Nature communications·2025
Same author

Poly(vinyl alcohol) cryogels: Effect size of polymer concentration, number of cycles and thawing rate on material properties and dermal drug delivery.

European journal of pharmaceutics and biopharmaceutics : official journal of Arbeitsgemeinschaft fur Pharmazeutische Verfahrenstechnik e.V·2025
Same author

Axial rod slip at the end-of-construct screw in scoliosis surgery: relevance, occurrence and prevention.

Spine deformity·2024

Related Experiment Video

Updated: Mar 26, 2026

Growth and Electrostatic/chemical Properties of Metal/LaAlO3/SrTiO3 Heterostructures
11:54

Growth and Electrostatic/chemical Properties of Metal/LaAlO3/SrTiO3 Heterostructures

Published on: February 8, 2018

10.8K

Polaronic metal state at the LaAlO3/SrTiO3 interface.

C Cancellieri1,2, A S Mishchenko3, U Aschauer4,5

  • 1Swiss Light Source, Paul Scherrer Institute, Villigen CH-5232, Switzerland.

Nature Communications
|January 28, 2016
PubMed
Summary

The interface between LaAlO3 and SrTiO3 hosts charge carriers identified as large polarons. This polaron formation, involving charge and lattice coupling, limits carrier mobility and explains its high-temperature drop.

More Related Videos

Tuning Oxide Properties by Oxygen Vacancy Control During Growth and Annealing
06:44

Tuning Oxide Properties by Oxygen Vacancy Control During Growth and Annealing

Published on: June 9, 2023

4.0K
Writing and Low-Temperature Characterization of Oxide Nanostructures
06:43

Writing and Low-Temperature Characterization of Oxide Nanostructures

Published on: July 18, 2014

10.5K

Related Experiment Videos

Last Updated: Mar 26, 2026

Growth and Electrostatic/chemical Properties of Metal/LaAlO3/SrTiO3 Heterostructures
11:54

Growth and Electrostatic/chemical Properties of Metal/LaAlO3/SrTiO3 Heterostructures

Published on: February 8, 2018

10.8K
Tuning Oxide Properties by Oxygen Vacancy Control During Growth and Annealing
06:44

Tuning Oxide Properties by Oxygen Vacancy Control During Growth and Annealing

Published on: June 9, 2023

4.0K
Writing and Low-Temperature Characterization of Oxide Nanostructures
06:43

Writing and Low-Temperature Characterization of Oxide Nanostructures

Published on: July 18, 2014

10.5K

Area of Science:

  • Condensed Matter Physics
  • Materials Science
  • Oxide Heterostructures

Background:

  • Oxide heterostructures exhibit complex interplay of spin, charge, orbital, and lattice degrees of freedom.
  • The LaAlO3/SrTiO3 interface hosts a 2D electron system with emergent properties like superconductivity and ferromagnetism.
  • The fundamental origins of these properties, particularly carrier behavior, remain under investigation.

Purpose of the Study:

  • To directly probe the nature of charge carriers at the buried LaAlO3/SrTiO3 interface.
  • To elucidate the mechanism behind the puzzling temperature dependence of carrier mobility.

Main Methods:

  • Soft-X-ray angle-resolved photoelectron spectroscopy (SX-ARPES) was employed.
  • This technique allowed penetration through the LaAlO3 overlayer to access the buried interface charge carriers.

Main Results:

  • Direct experimental identification of interface charge carriers as large polarons.
  • Evidence of coupling between charge and lattice degrees of freedom involving two phonons.
  • Demonstration that this polaron formation fundamentally limits carrier mobility.

Conclusions:

  • The charge carriers at the LaAlO3/SrTiO3 interface are large polarons.
  • This polaron phenomenon explains the observed drop in carrier mobility at high temperatures.
  • Understanding polaron formation is crucial for designing future electronic devices based on oxide heterostructures.