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Non-ohmic Devices00:51

Non-ohmic Devices

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In most substances, the current flow is proportional to the voltage applied to it. A simple relationship between the values of current, voltage, and resistance is known as Ohm's law. Nonohmic devices do not exhibit a linear relationship between voltage and current. One such device is the semiconducting circuit element known as a diode. A diode is a circuit device that allows current flow in only one direction.
Consider a simple circuit consisting of a battery, a diode, and a resistor. A...
1.5K
Semiconductors01:22

Semiconductors

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There is variation in the electrical conductivity of materials - metals, semiconductors, and insulators that are showcased with the help of the energy band diagrams.
Metals such as copper (Cu), zinc (Zn), or lead (Pb) have low resistivity and feature conduction bands that are either not fully occupied or overlap with the valence band, making a bandgap non-existent. This allows electrons in the highest energy levels of the valence band to easily transition to the conduction band upon gaining...
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Types of Semiconductors01:20

Types of Semiconductors

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Intrinsic semiconductors are highly pure materials with no impurities. At absolute zero, these semiconductors behave as perfect insulators because all the valence electrons are bound, and the conduction band is empty, disallowing electrical conduction. The Fermi level is a concept used to describe the probability of occupancy of energy levels by electrons at thermal equilibrium. In intrinsic semiconductors, the Fermi level is positioned at the midpoint of the energy gap at absolute zero. When...
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P-N junction01:11

P-N junction

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A p-n junction is formed when p-type and n-type semiconductor materials are joined together. At the interface of the p-n junction, holes from the p-side and electrons from the n-side begin to diffuse into the opposite sides due to the concentration gradient. This diffusion of carriers leads to a region around the junction where there are no free charge carriers, known as the depletion region. The charge density within the depletion region for the n-side and p-side can be described by the...
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Determination of Crystal Structures01:29

Determination of Crystal Structures

139
In the late 1800s, the revelation that light extended beyond visible wavelengths led to the discovery of X-rays by Wilhelm Roentgen. Recognized as high-energy electromagnetic radiation with short wavelengths, X-rays prompted exploration into their interaction with crystals. Max von Laue proposed in 1912 that the periodic arrangement of atoms, ions, or molecules in crystals would cause them to diffract X-rays, a hypothesis confirmed through experiments with copper sulfate and zinc sulfide...
139
Imperfections in Crystal Structure: Stoichiometric Point Defects01:26

Imperfections in Crystal Structure: Stoichiometric Point Defects

147
Schottky defects arise when some lattice points in a crystal, such as those in NaCl, remain unoccupied, creating lattice vacancies without disturbing the overall electrical neutrality of the crystal. This defect is common in ionic crystals where the positive and negative ions are similar in size, as seen in sodium chloride and cesium chloride. The presence of Schottky defects enables the crystal to conduct electricity to a small extent through an ionic mechanism. Electric fields cause nearby...
147

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Harvesting Solar Energy by Means of Charge-Separating Nanocrystals and Their Solids
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Harvesting Solar Energy by Means of Charge-Separating Nanocrystals and Their Solids

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Los nanocristales de semiconductores no parpadeantes son nanocristales de semiconductores sin parpadear.

Xiaoyong Wang1, Xiaofan Ren, Keith Kahen

  • 1Department of Chemistry, University of Rochester, Rochester, New York 14627, USA.

Nature
|May 12, 2009
PubMed
Resumen
Este resumen es generado por máquina.

Los investigadores desarrollaron nanocristales semiconductores sin parpadeo. Estos nanocristales CdZnSe/ZnSe muestran fotoluminiscencia continua, superando una limitación importante para aplicaciones como fuentes de un solo fotón y etiquetado biológico.

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Área de la Ciencia:

  • Ciencia de los materiales Ciencia de los materiales.
  • Nanotecnología La nanotecnología es la nanotecnología.
  • La óptica cuántica es una óptica cuántica.

Sus antecedentes:

  • La fotoluminiscencia de las moléculas y los nanocristales exhibe "parpadeo" fluctuaciones intermitentes de intensidad de encendido/apagado.
  • Se teorizó que el parpadeo de los nanocristales de semiconductores era el resultado de un apagado inducido por carga temporal a través de la recombinación no radiativa.
  • A pesar de una extensa investigación, lograr nanocristales que no parpadeen y comprender completamente el parpadeo sigue siendo un desafío.

Objetivo del estudio:

  • Para sintetizar y caracterizar los nanocristales semiconductores que exhiben fotoluminiscencia continua y sin parpadeo.
  • Para investigar las propiedades de fotoluminiscencia de los nanocristales cargados.
  • Comprender la base estructural para el comportamiento no parpadeante en nanocristales de núcleo / cáscara.

Principales métodos:

  • Síntesis de nanocristales ternaros de semiconductores CdZnSe/ZnSe de núcleo y cáscara ternaras.
  • Caracterización de la intensidad de la fotoluminiscencia, la forma espectral y la vida útil bajo fotoexcitación continua.
  • Modelado de potenciales de confinamiento de nanocristales para elucidar las propiedades estructurales.

Principales resultados:

  • Los nanocristales individuales de CdZnSe/ZnSe demostraron una fotoluminiscencia continua y sin parpadeo.
  • Estos nanocristales exhibieron una fuerte fotoluminiscencia a pesar de estar cargados, como lo demuestran los espectros de múltiples picos y las vidas cortas.
  • El análisis estructural sugirió una composición de aleación graduada radialmente en lugar de una interfaz de núcleo / cáscara nítida.

Conclusiones:

  • Los nanocristales CdZnSe/ZnSe desarrollados superan las limitaciones del parpadeo en los nanocristales semiconductores.
  • La fotoluminiscencia continua de los nanocristales cargados desafía las suposiciones anteriores sobre los mecanismos de parpadeo.
  • Estos nanocristales no parpadeantes tienen un potencial significativo para aplicaciones que requieren una emisión estable de un solo fotón.