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Types Of Superconductors01:28

Types Of Superconductors

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A superconductor is a substance that offers zero resistance to the electric current when it drops below a critical temperature. Zero resistance is not the only interesting phenomenon as materials reach their transition temperatures. A second effect is the exclusion of magnetic fields. This is known as the Meissner effect. A light, permanent magnet placed over a superconducting sample will levitate in a stable position above the superconductor. High-speed trains that levitate on strong...
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Magnetostatic Boundary Conditions01:28

Magnetostatic Boundary Conditions

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An electric field suffers a discontinuity at a surface charge. Similarly, a magnetic field is discontinuous at a surface current. The perpendicular component of a magnetic field is continuous across the interface of two magnetic mediums. In contrast, its parallel component, perpendicular to the current, is discontinuous by the amount equal to the product of the vacuum permeability and the surface current. Like the scalar potential in electrostatics, the vector potential is also continuous...
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Spin–Spin Coupling Constant: Overview01:08

Spin–Spin Coupling Constant: Overview

1.1K
In bromoethane, the three methyl protons are coupled to the two methylene protons that are three bonds away. In accordance with the n+1 rule, the signal from the methyl protons is split into three peaks with 1:2:1 relative intensities. The methylene protons appear as a quartet, with the relative intensities of 1:3:3:1.
Qualitatively, any spin plus-half nucleus polarizes the spins of its electrons to the minus-half state. Consequently, the paired electron in the hydrogen–carbon bond must...
1.1K
Superconductor01:24

Superconductor

1.4K
A substance that reaches superconductivity, a state in which magnetic fields cannot penetrate, and there is no electrical resistance, is referred to as a superconductor. In 1911, Heike Kamerlingh Onnes of Leiden University, a Dutch physicist, observed a relation between the temperature and the resistance of the element mercury. The mercury sample was then cooled in liquid helium to study the linear dependence of resistance on temperature. It was observed that, as the temperature decreased, the...
1.4K
Magnetic Susceptibility and Permeability01:31

Magnetic Susceptibility and Permeability

1.6K
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...
1.6K
Ferromagnetism01:31

Ferromagnetism

2.6K
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...
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Video Experimental Relacionado

Updated: Oct 24, 2025

Comparison of Two Different Synthesis Methods of Single Crystals of Superconducting Uranium Ditelluride
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Comparison of Two Different Synthesis Methods of Single Crystals of Superconducting Uranium Ditelluride

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Parámetro de orden superconductor multicomponente en UTe2

I M Hayes1, D S Wei2,3,4, T Metz5,1

  • 1Department of Physics, Quantum Materials Center, University of Maryland, College Park, MD 20742, USA.

Science (New York, N.Y.)
|August 13, 2021
PubMed
Resumen
Este resumen es generado por máquina.

Los investigadores descubrieron un estado superconductor único en el ditelururo de uranio (UTe2). Esta superconductividad no convencional presenta un parámetro de orden de dos componentes, rompiendo la simetría de inversión de tiempo y sugiriendo propiedades topológicas potenciales.

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Área de la Ciencia:

  • Física de la materia condensada
  • Ciencias de los materiales
  • Los materiales cuánticos

Sus antecedentes:

  • El ditelururo de uranio (UTe2) exhibe un estado superconductor no convencional que surge de un estado normal de fermión pesado paramagnético.
  • La coexistencia de fluctuaciones magnéticas y superconductividad en UTe2 sugiere simetrías complejas, propiedades magnéticas y características topológicas potenciales.

Objetivo del estudio:

  • Para investigar la naturaleza del estado superconductor en UTe2.
  • Para determinar las simetrías y propiedades del parámetro de orden superconductor.
  • Evaluar el potencial de superconductividad topológica en UTe2.

Principales métodos:

  • Medición del efecto Kerr polar para detectar la ruptura de simetría de reversión del tiempo.
  • Mediciones específicas de calor para identificar las transiciones de fase al estado superconductor.

Principales resultados:

  • Observación de un efecto Kerr polar distinto de cero, que indica una ruptura de simetría de reversión del tiempo.
  • Detección de dos transiciones distintas en el calor específico al entrar en el estado superconductor.
  • Prueba de un parámetro de orden superconductor de dos componentes en UTe2.

Conclusiones:

  • La superconductividad en UTe2 se caracteriza por un parámetro de orden de dos componentes que rompe la simetría de inversión de tiempo.
  • Los resultados proporcionan restricciones a las simetrías del parámetro de orden.
  • Los resultados contribuyen a la discusión en curso sobre la superconductividad topológica en UTe2.