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相关概念视频

The Quantum-Mechanical Model of an Atom02:45

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Shortly after de Broglie published his ideas that the electron in a hydrogen atom could be better thought of as being a circular standing wave instead of a particle moving in quantized circular orbits, Erwin Schrödinger extended de Broglie’s work by deriving what is now known as the Schrödinger equation. When Schrödinger applied his equation to hydrogen-like atoms, he was able to reproduce Bohr’s expression for the energy and, thus, the Rydberg formula governing...
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NMR Spectrometers: Radiofrequency Pulses and Pulse Sequences01:17

NMR Spectrometers: Radiofrequency Pulses and Pulse Sequences

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A pulse is a short burst of radio waves distributed over a range of frequencies that simultaneously excites all the nuclei in the sample. Upon passing a radio frequency pulse along the x-axis, the nuclei absorb energy corresponding to their Larmor frequencies and achieve resonance. This shifts the net magnetization vector from the z-axis toward the transverse plane. This angle of rotation of the magnetization vector, or the flip angle, is proportional to the duration and intensity of the pulse.
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Imaging Biological Samples with Optical Microscopy01:18

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Optical microscopy uses optic principles to provide detailed images of samples. Antonie van Leeuwenhoek designed the first compound optical microscope in the 17th century to visualize blood cells, bacteria, and yeast cells. In 1830, Joseph Jackson Lister created an essentially modern light microscope. The 20th century saw the development of microscopes with enhanced magnification and resolution.
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Photoluminescence offers a wide range of applications due to its inherent sensitivity and selectivity. This technique allows for both direct and indirect analyses of the analyte. Direct quantitative analysis is possible when the analyte exhibits a favorable quantum yield for fluorescence or phosphorescence. However, an indirect analysis may be feasible if the analyte is not fluorescent or phosphorescent, or if the quantum yield is unfavorable. Indirect methods include reacting the analyte with...
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Fluorescence and Phosphorescence: Instrumentation

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Fluorometers and spectrofluorometers are two types of instruments used for measuring molecular fluorescence. These instruments differ in how they select excitation and emission wavelengths and the type of light sources they utilize. Fluorometers use absorption interference filters to choose excitation and emission wavelengths. The excitation source in a fluorometer is typically a low-pressure mercury vapor lamp that emits intense lines distributed throughout the ultraviolet and visible regions.
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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.
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对于量子应用的连贯光学脉冲测序器.

Mahdi Hosseini1, Ben M Sparkes, Gabriel Hétet

  • 1ARC Centre of Excellence for Quantum-Atom Optics, Department of Quantum Science, The Australian National University, Canberra, Australian Capital Territory 0200, Australia.

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概括
此摘要是机器生成的。

研究人员使用光子回声开发了一种新的连贯光学记忆. 该系统能够以任意顺序存储和回忆多个光脉冲,并有可能进行量子信息处理.

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科学领域:

  • 光学和光子学 在光学和光子学.
  • 量子信息科学 量子信息科学
  • 原子物理 原子物理

背景情况:

  • 光学设备对于信息技术和通信至关重要.
  • 精确控制光学场对于光子技术至关重要.
  • 量子光学记忆对于量子信息应用至关重要,随着原子记忆的进步.

研究的目的:

  • 基于光子回声呈现一个连贯的光学记忆系统.
  • 为了证明任意存储和检索光脉冲.
  • 探索量子信息处理中的潜在应用.

主要方法:

  • 使用受控的可逆不均扩展来诱导光子回声.
  • 实施一种在特定带宽内存储多个光脉冲的方案.
  • 展示时间压缩,时间拉伸和脉冲分割的能力.

主要成果:

  • 成功存储和检索多个经典光脉冲.
  • 证明了随意的订单召回与可调节的延迟.
  • 显示了修改脉冲持续时间和碎片化的能力.

结论:

  • 开发的技术可以实现多功能连贯光学内存.
  • 这种方法适用于构建一个光学随机访问存储器,用于时间区量子信息.
  • 这项技术有望推动量子信息处理的发展.