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Videos de Conceptos Relacionados

X-ray Imaging01:24

X-ray Imaging

German physicist Wilhelm Röntgen (1845–1923) was experimenting with electrical current when he discovered that a mysterious and invisible "ray" would pass through his flesh but leave an outline of his bones on a screen coated with a metal compound. In 1895, Röntgen made the first durable record of the internal parts of a living human: an "X-ray" image (as it came to be called) of his wife’s hand. Scientists worldwide quickly began their own experiments with X-rays, and by 1900, X-ray was widely...
IR Frequency Region: X–H Stretching01:24

IR Frequency Region: X–H Stretching

In IR spectroscopy, signals produced by the X−H bonds (such as C−H, O−H, or N−H) can be observed in the frequency range of  2700–4000 cm–1. The C−H stretching vibration forms sharp bands in the region 2850–3000 cm–1. The presence of the O−H stretching vibration leads to the forming of an absorption band in the frequency range 3650–3200 cm−1. At the same time, N−H stretching can be confirmed by absorption bands in the 3500–3100 cm−1 range. Even though both O−H and N−H bonds vibrate at a similar...
Atomic Emission Spectroscopy: Instrumentation01:22

Atomic Emission Spectroscopy: Instrumentation

The instrumentation of atomic emission spectrometry (AES) involves various components, including atomization devices that convert samples into gas-phase atoms and ions. There are two main types of atomization devices: continuous and discrete atomizers.  Continuous atomizers, like plasmas and flames, introduce samples in a constant stream, while discrete atomizers inject individual samples using syringes or autosamplers. The most common discrete atomizer is the electrothermal atomizer.
Atomic Absorption Spectroscopy: Radiation and Light Sources01:13

Atomic Absorption Spectroscopy: Radiation and Light Sources

Atomic absorption spectroscopy (AAS) relies on the Beer-Lambert law, which requires that the radiation source emits a narrow range of wavelengths to match the absorption characteristics of the analyte atom. The primary criteria for choosing an appropriate radiation source in AAS is to provide a precise and intense emission at specific wavelengths that will allow accurate detection of the analyte.
Two common narrow-range 'line' sources used in AAS are hollow-cathode lamps (HCLs) and...
Generating Electromagnetic Radiations01:10

Generating Electromagnetic Radiations

The German physicist Heinrich Hertz (1857–1894) was the first to generate and detect certain types of electromagnetic waves in the laboratory. Starting in 1887, he performed a series of experiments that confirmed the existence of electromagnetic waves and verified that they travel at the speed of light. Hertz used an alternating-current RLC (resistor-inductor-capacitor) circuit that resonated at a known frequency and connected it to a loop of wire. High voltages induced across the gap in the...
Atomic Emission Spectroscopy: Overview01:20

Atomic Emission Spectroscopy: Overview

Atomic emission spectroscopy (AES) is an analytical technique used to determine the elemental composition of a sample by analyzing the light emitted from excited atoms. In AES, atoms in a sample are excited to higher energy levels by thermal energy from high-temperature sources, such as plasma, arcs, or sparks. When these excited atoms return to lower energy states, they emit light at specific wavelengths characteristic of each element. The resulting atomic emission spectrum, which consists of...

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Video Experimental Relacionado

Updated: Jul 12, 2026

Measurement of X-ray Beam Coherence along Multiple Directions Using 2-D Checkerboard Phase Grating
10:39

Measurement of X-ray Beam Coherence along Multiple Directions Using 2-D Checkerboard Phase Grating

Published on: October 11, 2016

Radiografías coherentes sintonizables de rayos X.

D Attwood, K Halbach, K J Kim

    Science (New York, N.Y.)
    |June 14, 1985
    PubMed
    Resumen

    Una nueva instalación de radiación sincrotrón producirá rayos X suaves tipo láser para la investigación avanzada. Esta tecnología permite el microsondeo detallado de muestras biológicas y de materiales, superando las capacidades actuales de láser de laboratorio.

    Área de la Ciencia:

    • Física La física es la física.
    • Ciencia de los materiales Ciencia de los materiales.
    • La biofísica es la biofísica.

    Sus antecedentes:

    • Los láseres XUV de laboratorio actuales carecen de las capacidades para la microsondación avanzada.
    • Es posible que las instalaciones de sincrotrón existentes no ofrezcan la coherencia y sintonizabilidad requeridas para aplicaciones de investigación específicas.

    Objetivo del estudio:

    • Describir las capacidades de una instalación de radiación sincrotrón propuesta de 1 a 2 mil millones de electrones-voltios.
    • Para resaltar las aplicaciones potenciales de los rayos X blandos coherentes generados por esta instalación.

    Principales métodos:

    • Utilizando haces de electrones de alto brillo y onduladores magnéticos en un sincrotrón.
    • Generando rayos X suaves ampliamente sintonizables con longitudes de onda tan cortas como 10 angstroms.

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  • Lograr el control total de la polarización de la radiación generada.
  • Principales resultados:

    • Producción de rayos X suaves coherentes, parecidos a los rayos láser.
    • La sintonizabilidad de longitud de onda se reduce a 10 angstroms.
    • Potencial para el microprobado y la microfabricación sensibles a fases y elementos.

    Conclusiones:

    • La instalación sincrotrón propuesta ofrece capacidades únicas de longitud de onda corta cruciales para la investigación biológica y de materiales.
    • Estas capacidades, incluido el acceso al borde de absorción K para C, N y O, no están disponibles con los láseres XUV de laboratorio actuales.
    • Los anillos de almacenamiento de energía más altos (5-6 GeV) son menos adecuados debido a la coherencia reducida y al aumento de la carga térmica del componente óptico.