Related Experiment Video
Updated: Jun 3, 2026

08:25
Chemical Vapor Deposition of an Organic Magnet, Vanadium Tetracyanoethylene
Published on: July 3, 2015
Titanium pyrochlore magnets: how much can be learned from magnetization measurements?
O A Petrenko1, M R Lees, G Balakrishnan
1Department of Physics, University of Warwick, Coventry CV4 7AL, UK. o.petrenko@warwick.ac.uk
Summary
Magnetization data reveal new insights into titanium pyrochlores. Single crystal measurements down to 0.5 K uncovered slow relaxation in spin-ice systems and critical behavior in XY and Heisenberg pyrochlores.
Area of Science:
- Condensed Matter Physics
- Materials Science
- Magnetism
Background:
- Titanium pyrochlores are complex magnetic materials exhibiting exotic phenomena.
- Previous studies were limited by temperature ranges and sample types, potentially missing crucial details.
Purpose of the Study:
- To investigate the magnetic properties of titanium pyrochlore systems using single crystals at very low temperatures.
- To elucidate previously unobserved features and phase transitions in these materials.
Main Methods:
- Magnetization measurements were conducted on single crystal samples.
- Experiments were performed at temperatures as low as 0.5 K and in magnetic fields up to 7 kOe.
Main Results:
- Observed unusually slow magnetization relaxation in low fields for spin-ice pyrochlores (Dy2Ti2O7, Ho2Ti2O7).
- Identified hysteresis-free magnetization processes in high fields for spin-ice systems.
- Characterized critical field behavior in the XY pyrochlore (Er2Ti2O7) with non-saturating magnetization.
- Detected distinct changes in magnetic susceptibility at two transition temperatures (1.02 K and 0.74 K) for the Heisenberg pyrochlore (Gd2Ti2O7).
Conclusions:
- Single crystal, low-temperature measurements provide a more comprehensive understanding of titanium pyrochlores.
- New magnetic behaviors and phase transition details were uncovered, refining previous findings.
Related Concept Videos
Paramagnetism
Paramagnets are materials with unpaired electrons that possess a finite magnetic moment. In the absence of a magnetic field, these moments are randomly oriented, and thus the net moment is zero. Under an external field, a torque acting on the moments tends to align them along the field's direction. However, the random thermal motion of electrons produces a torque opposite to the external field and tries to disorient the moments. These two competing effects align only a few moments along the...
Ferromagnetism
Materials like iron, nickel, and cobalt consist of magnetic domains, within which the magnetic dipoles are arranged parallel to each other. The magnetic dipoles are rigidly aligned in the same direction within a domain by quantum mechanical coupling among the atoms. This coupling is so strong that even thermal agitation at room temperature cannot break it. The result is that each domain has a net dipole moment. However, some materials have weaker coupling, and are ferromagnetic at lower...
Magnetic Susceptibility and Permeability
In linear magnetic materials, like paramagnets and diamagnets, magnetization is proportional to the magnetic field intensity. The constant of proportionality, a dimensionless number, is called magnetic susceptibility. The value of the susceptibility depends on the type of material.
When diamagnetic materials are placed under an external magnetic field, the moments opposite to the field are induced. Hence, the susceptibility for diamagnets has a minimal negative value of 10-5–10-6. Since...
When diamagnetic materials are placed under an external magnetic field, the moments opposite to the field are induced. Hence, the susceptibility for diamagnets has a minimal negative value of 10-5–10-6. Since...
Diamagnetism
Materials consisting of paired electrons have zero net magnetic moments. However, when these materials are placed under an external magnetic field, the moments opposite to the field are induced. Such materials are called diamagnets. Diamagnetism is the response of the diamagnets when placed in an external magnetic field.
Diamagnetism was discovered by Anton Brugmans in 1778 when he observed that bismuth gets repelled by magnetic fields, thus theorizing that diamagnets get repelled by magnets.
Diamagnetism was discovered by Anton Brugmans in 1778 when he observed that bismuth gets repelled by magnetic fields, thus theorizing that diamagnets get repelled by magnets.
Potential Due to a Magnetized Object
Magnetic dipoles in magnetic materials are aligned when placed under an external magnetic field. For paramagnets and ferromagnets, dipole alignment occurs in the direction of the magnetic field. However, the dipoles align opposite to the field in the case of diamagnets. This state of magnetic polarization due to the external field is called magnetization. Magnetization is defined as the dipole moment per unit volume. It plays a similar role to polarization in electrostatics.
The vector...
The vector...
Magnetic Moment of an Electron
Electrons revolving around a nucleus are analogous to a circular current carrying loop. This current produces a magnetic dipole moment proportional to the electron's orbital angular momentum. Since the orbital angular momentum is quantized in terms of the reduced Planck's constant, the dipole moment is quantized in the Bohr Magneton. The value of the Bohr magneton is 9.27 x 10-24 Am2. Electrons also have an intrinsic spin angular momentum, and the associated spin magnetic moment is...

