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

Phase Transitions01:21

Phase Transitions

A phase transition is the process in which a substance changes from one state of matter to another, like from a solid to a liquid, liquid to gas, or vice versa, at a specific temperature and under given pressure conditions. This change is spontaneous and is affected by alterations in temperature and pressure. These parameters impact the strength of the forces between molecules (intermolecular forces) in the substance.During a phase transition, both the initial and final phases of the substance...
Phase Transitions02:31

Phase Transitions

Whether solid, liquid, or gas, a substance's state depends on the order and arrangement of its particles (atoms, molecules, or ions). Particles in the solid pack closely together, generally in a pattern. The particles vibrate about their fixed positions but do not move or squeeze past their neighbors. In liquids, although the particles are closely spaced, they are randomly arranged. The position of the particles are not fixed—that is, they are free to move past their neighbors to occupy...
Phase Transitions: Sublimation and Deposition02:33

Phase Transitions: Sublimation and Deposition

Some solids can transition directly into the gaseous state, bypassing the liquid state, via a process known as sublimation. At room temperature and standard pressure, a piece of dry ice (solid CO2) sublimes, appearing to gradually disappear without ever forming any liquid. Snow and ice sublimate at temperatures below the melting point of water, a slow process that may be accelerated by winds and the reduced atmospheric pressures at high altitudes. When solid iodine is warmed, the solid sublimes...
Phase Diagrams of Ternary Systems01:28

Phase Diagrams of Ternary Systems

Consider a ternary system, which is composed of three components: water (W), ethanoic acid (E), and trichloromethane (T). Here, Ethanoic acid (E) is fully miscible with both water (W) and trichloromethane (T), meaning it can mix entirely with either of them. However, water and trichloromethane have partial miscibility, meaning they can only mix to a certain extent, beyond which two separate phases will form.The phase diagram of a ternary system is represented as an equilateral triangle, where...
Phase Transitions: Melting and Freezing02:39

Phase Transitions: Melting and Freezing

Heating a crystalline solid increases the average energy of its atoms, molecules, or ions, and the solid gets hotter. At some point, the added energy becomes large enough to partially overcome the forces holding the molecules or ions of the solid in their fixed positions, and the solid begins the process of transitioning to the liquid state or melting. At this point, the temperature of the solid stops rising, despite the continual input of heat, and it remains constant until all of the solid is...
Thermal Sigmatropic Reactions: Overview01:16

Thermal Sigmatropic Reactions: Overview

Sigmatropic rearrangements are a class of pericyclic reactions in which a σ bond migrates from one part of a π system to another. These are intramolecular rearrangements where the total number of σ and π bonds remain unchanged.
Sigmatropic shifts are classified based on an order term [i, j ], where i and j indicate the number of atoms across which each end of the σ bond migrates. Below are examples of a [3,3] sigmatropic shift in 1,5-hexadiene, referred to as...

You might also read

Related Articles

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

Sort by
Same author

Topotactic ion exchange in β-pyrochlore oxide using 18-crown-6: structural incorporation of confined water in (H<sub>3</sub>O)Os<sub>2</sub>O<sub>6</sub>.

Dalton transactions (Cambridge, England : 2003)·2026
Same author

Towards a sustainable high-quality materials data ecosystem: frameworks and strategies.

National science review·2026
Same author

Design of a High-Performance Infrared Nonlinear Optical Crystal via a Multiple Flexible-Group Synergistic Polarization Strategy.

Journal of the American Chemical Society·2026
Same author

Rationalizing Synergic Role of Ti─O─Ru Distortion and Ferromagnetic Superexchange Coupling for Envisaging Electrocatalytic Oxygen Evolution Activity in Double Perovskite.

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

Investigation of topological nodal line phonons in rhenium-based alkali metal oxides (AReO<sub>4</sub>; A = Na, K, and Rb) using first principles methods.

Physical chemistry chemical physics : PCCP·2026
Same author

Variable Temperature Studies of Two Calcium Uranates α-Ca<sub>3</sub>UO<sub>6</sub> and Ca<sub>2</sub>UO<sub>5</sub>.

Chemistry (Weinheim an der Bergstrasse, Germany)·2026

Related Experiment Video

Updated: Jun 1, 2026

Sputter Growth and Characterization of Metamagnetic B2-ordered FeRh Epilayers
12:20

Sputter Growth and Characterization of Metamagnetic B2-ordered FeRh Epilayers

Published on: October 5, 2013

Structural phase transitions and magnetic order in SrTcO3.

Gordon J Thorogood1, Maxim Avdeev, Melody L Carter

  • 1IME Australian Nuclear Science and Technology Organisation, Private Mail Bag 1, Menai NSW, 2234, Australia.

Dalton Transactions (Cambridge, England : 2003)
|June 10, 2011
PubMed
Summary

Strontium technetate(III) oxide (SrTcO3) exhibits an orthorhombic structure due to TcO6 octahedra tilting. This perovskite displays a G-type antiferromagnetic structure below 1000 K, consistent across its crystal phases.

More Related Videos

Synthesis of Non-uniformly Pr-doped SrTiO3 Ceramics and Their Thermoelectric Properties
11:07

Synthesis of Non-uniformly Pr-doped SrTiO3 Ceramics and Their Thermoelectric Properties

Published on: August 15, 2015

Spark Plasma Sintering Apparatus Used for the Formation of Strontium Titanate Bicrystals
11:17

Spark Plasma Sintering Apparatus Used for the Formation of Strontium Titanate Bicrystals

Published on: February 9, 2017

Related Experiment Videos

Last Updated: Jun 1, 2026

Sputter Growth and Characterization of Metamagnetic B2-ordered FeRh Epilayers
12:20

Sputter Growth and Characterization of Metamagnetic B2-ordered FeRh Epilayers

Published on: October 5, 2013

Synthesis of Non-uniformly Pr-doped SrTiO3 Ceramics and Their Thermoelectric Properties
11:07

Synthesis of Non-uniformly Pr-doped SrTiO3 Ceramics and Their Thermoelectric Properties

Published on: August 15, 2015

Spark Plasma Sintering Apparatus Used for the Formation of Strontium Titanate Bicrystals
11:17

Spark Plasma Sintering Apparatus Used for the Formation of Strontium Titanate Bicrystals

Published on: February 9, 2017

Area of Science:

  • Materials Science
  • Solid-State Chemistry
  • Crystallography

Background:

  • Perovskite oxides are crucial in various technological applications.
  • Understanding the structural and magnetic properties of novel perovskites like SrTcO3 is essential for materials development.
  • Strontium technetate(III) oxide (SrTcO3) is a less-studied perovskite with potential for unique properties.

Purpose of the Study:

  • To elucidate the crystal structure of SrTcO3 across a range of temperatures.
  • To determine the magnetic ordering and structure of SrTcO3.
  • To investigate the relationship between crystal structure and magnetic properties in SrTcO3.

Main Methods:

  • Synchrotron X-ray powder diffraction was employed to analyze crystal structure.
  • Neutron powder diffraction was utilized for detailed structural and magnetic investigations.
  • Temperature-dependent diffraction studies were conducted from 4 K to 1023 K.

Main Results:

  • SrTcO3 adopts an orthorhombic structure at room temperature due to corner-sharing TcO6 octahedra tilting.
  • Heating SrTcO3 leads to sequential removal of octahedral tilts, transitioning through Pnma, Imma, I4/mcm, and finally Pm3m phases.
  • Below approximately 1000 K, SrTcO3 exhibits a G-type antiferromagnetic structure with collinear technetium moments aligned parallel to the c-axis (k=[0,0,0]).
  • This G-type antiferromagnetic structure remains consistent across all observed crystallographic phases.

Conclusions:

  • The crystal structure of SrTcO3 is temperature-dependent, featuring distinct phase transitions driven by octahedral tilting.
  • SrTcO3 possesses a robust G-type antiferromagnetic ordering that is independent of its crystallographic phase.
  • This study provides fundamental insights into the coupled structural and magnetic behavior of SrTcO3 perovskite.