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

The de Broglie Wavelength02:32

The de Broglie Wavelength

25.9K
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...
25.9K
Crystal Field Theory - Octahedral Complexes02:58

Crystal Field Theory - Octahedral Complexes

26.4K
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...
26.4K
Crystal Field Theory - Tetrahedral and Square Planar Complexes02:46

Crystal Field Theory - Tetrahedral and Square Planar Complexes

42.5K
Tetrahedral Complexes
Crystal field theory (CFT) is applicable to molecules in geometries other than octahedral. In octahedral complexes, the lobes of the dx2−y2 and dz2 orbitals point directly at the ligands. For tetrahedral complexes, the d orbitals remain in place, but with only four ligands located between the axes. None of the orbitals points directly at the tetrahedral ligands. However, the dx2−y2 and dz2 orbitals (along the Cartesian axes) overlap with the ligands less than the dxy,...
42.5K

You might also read

Related Articles

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

Sort by
Same author

Intrinsic Dual-Phase Regulated GeSe<sub>2</sub> Nanoparticles Triggered by Ball-Milling Treatment for Photonic Multi-Valued Logic Circuits.

Advanced science (Weinheim, Baden-Wurttemberg, Germany)·2026
Same author

Correlated singular flat bands on the surface pentagonal lattice of ferromagnetic CoS<sub>2</sub>.

Nature communications·2026
Same author

NMR and paramagnetic response of Dirac carriers in type-II semimetal NiTe<sub>2</sub>.

Journal of physics. Condensed matter : an Institute of Physics journal·2026
Same author

Probing Cosmic Ray Composition and Muonphilic Dark Matter via Muon Tomography.

Physical review letters·2026
Same author

A New Rutile-Type NaFe<sub>2</sub>F<sub>6</sub> Cathode for Sodium-Ion Batteries.

Small (Weinheim an der Bergstrasse, Germany)·2026
Same author

Dimensional Scaling Effect in Percolative Oxide Semiconductor Transistors.

ACS nano·2026

Related Experiment Video

Updated: Jun 30, 2025

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

9.6K

Three-dimensional ultrafast charge-density-wave dynamics in CuTe.

Nguyen Nhat Quyen1, Wen-Yen Tzeng2, Chih-En Hsu3

  • 1Department of Electrophysics, National Yang Ming Chiao Tung University, Hsinchu, 30010, Taiwan.

Nature Communications
|March 17, 2024
PubMed
Summary
This summary is machine-generated.

Charge density waves (CDWs) in CuTe exhibit dimensional evolution. Quantum fluctuations occur until 220 K, after which CDWs lock into an anti-phase, forming a c-axis CDW phase.

More Related Videos

Author Spotlight: Magnetometric Characterization of Intermediates in the Solid-State Electrochemistry of Redox-Active Metal-Organic Frameworks
06:53

Author Spotlight: Magnetometric Characterization of Intermediates in the Solid-State Electrochemistry of Redox-Active Metal-Organic Frameworks

Published on: June 9, 2023

2.0K
In Situ Time-dependent Dielectric Breakdown in the Transmission Electron Microscope: A Possibility to Understand the Failure Mechanism in Microelectronic Devices
09:26

In Situ Time-dependent Dielectric Breakdown in the Transmission Electron Microscope: A Possibility to Understand the Failure Mechanism in Microelectronic Devices

Published on: June 26, 2015

8.7K

Related Experiment Videos

Last Updated: Jun 30, 2025

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

9.6K
Author Spotlight: Magnetometric Characterization of Intermediates in the Solid-State Electrochemistry of Redox-Active Metal-Organic Frameworks
06:53

Author Spotlight: Magnetometric Characterization of Intermediates in the Solid-State Electrochemistry of Redox-Active Metal-Organic Frameworks

Published on: June 9, 2023

2.0K
In Situ Time-dependent Dielectric Breakdown in the Transmission Electron Microscope: A Possibility to Understand the Failure Mechanism in Microelectronic Devices
09:26

In Situ Time-dependent Dielectric Breakdown in the Transmission Electron Microscope: A Possibility to Understand the Failure Mechanism in Microelectronic Devices

Published on: June 26, 2015

8.7K

Area of Science:

  • Solid-state physics
  • Quantum materials
  • Low-dimensional systems

Background:

  • Charge density waves (CDWs) are quantum states involving electronic and phononic subsystems.
  • CDW phase dynamics and transition mechanisms, especially across different dimensions, remain understudied.
  • Low-dimensional materials frequently exhibit CDW phenomena.

Purpose of the Study:

  • To investigate the dimensional evolution of CDW phases in CuTe.
  • To elucidate the phase transition mechanisms of CDWs in different temperature regimes.
  • To understand the interplay of quantum fluctuations and inter-plane interactions in CDW stabilization.

Main Methods:

  • Utilizing orientation-dependent ultrafast electron and phonon dynamics.
  • Analyzing temperature evolution of these dynamics to probe CDW behavior.
  • Observing changes in c-axis length and interchain/interlayer interactions.

Main Results:

  • Distinct dimensional CDW phases were identified in CuTe.
  • Quantum fluctuations (QF) of the CDW phase were observed as temperature decreased until 220 K.
  • Below 220 K, CDWs on ab-planes locked in anti-phase, forming a c-axis CDW phase.

Conclusions:

  • The study demonstrates the dimension evolution of CDW phases within a single material system (CuTe).
  • It reveals the stabilization mechanisms of CDWs in different temperature ranges.
  • Highlights the role of quantum fluctuations and dimensional interactions in CDW formation.