Esta página ha sido traducida por una máquina. Otras páginas pueden seguir apareciendo en inglés. View in English

La superconductividad en el modelo de Hubbard dopado y su interacción con el siguiente salto

  • 0Stanford Institute for Materials and Energy Sciences, SLAC and Stanford University, Menlo Park, CA 94025, USA. hcjiang@stanford.edu.
Clinical Neuroscience (new York, N.y.) +

|

|

Resumen

Este resumen es generado por máquina.

Este estudio explora el modelo de Hubbard para la superconductividad a alta temperatura. La desestabilización de las rayas de carga es clave para lograr una superconductividad robusta, revelando una interacción entre diferentes órdenes electrónicos.

Área De La Ciencia

  • Física de la materia condensada
  • Los materiales cuánticos
  • Teoría de la superconductividad

Sus Antecedentes

  • El modelo de Hubbard es un marco teórico clave para comprender la superconductividad a alta temperatura.
  • Demostrar la superconductividad dentro del modelo de Hubbard sigue siendo un desafío significativo.
  • La comprensión de la interacción de órdenes en competencia es crucial para el diseño de nuevos materiales superconductores.

Objetivo Del Estudio

  • Para investigar las propiedades del estado básico del modelo de Hubbard ligeramente dopado.
  • Para explorar la influencia del salto del vecino más cercano (t') en las correlaciones electrónicas.
  • Identificar los mecanismos para lograr una superconductividad robusta en sistemas de electrones correlacionados.

Principales Métodos

  • Cálculos del grupo de renormalización de la matriz de densidad a gran escala (DMRG).
  • Estudio del modelo de Hubbard en cilindros de cuatro patas con una concentración de agujero de dopaje del 12,5%.
  • Análisis de las correlaciones de onda de densidad de carga (CDW) y onda de densidad de espín (SDW).

Principales Resultados

  • Existe una delicada interacción entre las órdenes de superconductividad, CDW y SDW, ajustable por t'.
  • Para t' finito, surge un estado líquido de Luther-Emery con las correlaciones de superconducción y CDW de la ley de potencia.
  • Para t' = 0, las correlaciones superconductoras decaen exponencialmente, con modulaciones CDW y SDW dominantes.

Conclusiones

  • La superconductividad robusta de largo alcance requiere la desestabilización de las tiras de carga aislante.
  • El modelo de Hubbard exhibe una competencia de fases complejas que influyen en las propiedades superconductoras.
  • El ajuste de correlaciones electrónicas ofrece una vía potencial para diseñar superconductores de alta temperatura.

Videos de Conceptos Relacionados

Valence Bond Theory 02:42

11.0K

Coordination compounds and complexes exhibit different colors, geometries, and magnetic behavior, depending on the metal atom/ion and ligands from which they are composed. In an attempt to explain the bonding and structure of coordination complexes, Linus Pauling proposed the valence bond theory, or VBT, using the concepts of hybridization and the overlapping of the atomic orbitals. According to VBT, the central metal atom or ion (Lewis acid) hybridizes to provide empty orbitals of suitable...

Valence Bond Theory 02:45

49.1K

Overview of Valence Bond Theory

Valence bond theory describes a covalent bond as the overlap of half-filled atomic orbitals (each containing a single electron) that yield a pair of electrons shared between the two bonded atoms. The orbitals on two different atoms overlap when a portion of one orbital and a portion of a second orbital occupy the same region of space. According to valence bond theory, a covalent bond results when two conditions are met: (1) an orbital on one atom overlaps an...

Theory of Metallic Conduction 01:17

1.7K

The conduction of free electrons inside a conductor is best described by quantum mechanics. However, a classical model makes predictions close to the results of quantum mechanics. It is called the theory of metallic conduction.
In this theory, Newton's second law of motion is used to determine the acceleration of an electron in the presence of an applied electric field. Then, its velocity is expressed via this acceleration.
An electron moves through the crystal, containing positive ions,...

Fermi Level Dynamics 01:12

614

The vacuum level denotes the energy threshold required for an electron to escape from a material surface. It is usually positioned above the conduction band of a semiconductor and acts as a benchmark for comparing electron energies within various materials.
Electron affinity in semiconductors refers to the energy gap between the minimum of its conduction band and the vacuum level and it is a critical parameter in determining how easily a semiconductor can accept additional electrons.
The work...

Superconductor 01:24

1.7K

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...

Spin–Spin Coupling: One-Bond Coupling 01:17

1.4K

Coupling interactions are strongest between NMR-active nuclei bonded to each other, where spin information can be transmitted directly through the pair of bonding electrons. While nuclei polarize their electrons to the opposite spins, the bonding electron pair has opposite spins. Configurations with antiparallel nuclear spins are expected to be lower in energy. When coupling makes antiparallel states more favorable, J is considered to have a positive value. The one-bond coupling constant, 1J,...