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相关概念视频

X-ray Crystallography02:18

X-ray Crystallography

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The size of the unit cell and the arrangement of atoms in a crystal may be determined from measurements of the diffraction of X-rays by the crystal, termed X-ray crystallography.
Diffraction
Diffraction is the change in the direction of travel experienced by an electromagnetic wave when it encounters a physical barrier whose dimensions are comparable to those of the wavelength of the light. X-rays are electromagnetic radiation with wavelengths about as long as the distance between neighboring...
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Atomic Absorption Spectroscopy: Interference01:25

Atomic Absorption Spectroscopy: Interference

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Interference leads to systematic error in atomic absorption (AA) measurements by enhancing or diminishing the analytical signal or the background. These interferences can be grouped into three main categories: spectral interference, chemical interference, and physical interference.
Spectral interference occurs when signals from other elements or molecules overlap with the analyte signal, falsely elevating or masking the analyte's absorbance. This interference can be corrected using Zeeman,...
831
Atomic Absorption Spectroscopy: Instrumentation01:22

Atomic Absorption Spectroscopy: Instrumentation

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An atomic absorption spectrophotometer (AAS) comprises several components: a radiation source, an atomizer, a monochromator, and a detector. The radiation source can be a hollow-cathode lamp (HCL) or an electrodeless-discharge lamp (EDL), both of which provide a narrow emission line of the required wavelength. However, some instruments use continuum sources and high-resolution monochromators to achieve a narrow range of radiation.
The atomizer used in AAS can be either a flame atomizer or an...
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Mass Analyzers: Common Types01:19

Mass Analyzers: Common Types

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The quadrupole mass analyzer consists of four cylindrical metal rods arranged in a diamond carrying a DC voltage and a radio-frequency AC voltage. The motion of ions through the quadrupole depends on the field strength, causing only ions of a certain m/z to resonate successfully and strike the detector at a given field strength. Though the transmission rate for these analyzers is high, the exact elemental composition of the sample is not determined because of low resolution; however, they are...
651
Atomic Absorption Spectroscopy: Atomization Methods01:25

Atomic Absorption Spectroscopy: Atomization Methods

569
Atomic Absorption Spectroscopy (AAS) atomizes samples through flame atomization or electrothermal atomization. Flame atomization typically involves a nebulizer and spray chamber assembly to combine the sample with a fuel–oxidant mixture, creating a fine aerosol mist that enters a burner. Typically, the fuel and oxidant are combined in an approximately stoichiometric ratio. However, for atoms that are easily oxidized, a fuel-rich mixture may be more advantageous. Only about 5% of the...
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Atomic Force Microscopy01:08

Atomic Force Microscopy

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Atomic force microscopy (AFM) is a type of scanning probe microscopy that can analyze topographic details of various specimens like ceramics, glass, polymers, and biological samples. AFM offers over 1000 times more resolution than the optical imaging system. Images generated from AFM are three-dimensional surface profiles, offering an advantage over the flat, two-dimensional images from other imaging techniques.
The AFM Probe
The probe is regarded as the heart of any AFM setup and comprises the...
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Implementation of a Reference Interferometer for Nanodetection
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使用布拉格衍射的μrad精度的大动量转移原子干扰仪.

J-N Kirsten-Siemß1,2, F Fitzek1,2, C Schubert2,3

  • 1Leibniz Universität Hannover, Institut für Theoretische Physik, Appelstraße 2, D-30167 Hannover, Germany.

Physical review letters
|August 4, 2023
PubMed
概括
此摘要是机器生成的。

大动量转移原子干扰仪通过理解布拉格散射来达到μrad的精度. 这项研究开发了一个分析模型来确定和和原子投射噪声极限,抑制系统错误.

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Picometer-Precision Atomic Position Tracking through Electron Microscopy
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Picometer-Precision Atomic Position Tracking through Electron Microscopy

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The Generation of Higher-order Laguerre-Gauss Optical Beams for High-precision Interferometry
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The Generation of Higher-order Laguerre-Gauss Optical Beams for High-precision Interferometry

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相关实验视频

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Picometer-Precision Atomic Position Tracking through Electron Microscopy
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科学领域:

  • 量子传感是一种量子感应.
  • 原子干涉测量是一种原子干涉测量.
  • 精确度测量测量的精确度

背景情况:

  • 使用弹性布拉格散射的大型动量转移 (LMT) 原子干扰仪是先进的量子传感器.
  • 目前的精度限制需要更深入地了解布拉格干扰仪的现象学,这与标准干扰仪不同.

研究的目的:

  • 开发LMT布拉格干扰仪信号的分析模型.
  • 为了确定和达到原子投射噪声极限.
  • 为了抑制系统的相位错误到μrad模式.

主要方法:

  • 对干扰仪信号的分析模型的开发.
  • 使用全面的数值模拟来验证模型.
  • 模型的应用以确定和和原子投射噪声极限.

主要成果:

  • 分析模型准确地描述了布拉格干扰仪的信号.
  • 确定了LMT布拉格干扰仪的原子投射噪声极限.
  • 系统的相位误差被压缩了2个数量级,达到几μrad.

结论:

  • 开发的分析模型对于提高LMT原子干扰仪的准确性至关重要.
  • 该模型使原子投射噪声极限的和成为可能.
  • 对光脉冲参数的精确控制可以显著抑制系统错误.