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Related Concept Videos

UV–Vis Spectrometers01:14

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The absorbance of UV and visible (UV–visible) radiations is measured using a UV–visible spectrophotometer. Deuterium lamps, which emit UV radiation, and tungsten lamps, which produce radiation in the visible region, are used as light sources in UV–visible spectrophotometers. A monochromator or prism is used for diffraction grating, i.e., to split the incoming radiation into different wavelengths. A system of slits is used to focus the desired wavelength on the sample cell.
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Ultraviolet–visible (UV–visible or UV–Vis) spectroscopy is an analytical technique that investigates the interaction between matter and UV–Vis light within the electromagnetic spectrum. This method is widely used for its versatility, simplicity, and relatively quick data acquisition, making it valuable for both qualitative and quantitative analysis. When UV–Vis radiation passes through a material,  molecules absorb light depending on the energy required for...
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A conventional Raman spectrophotometer includes a laser source, a sample holding system, a wavelength selector, and a detector.
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UV–Visible absorption spectra of conjugated dienes arise from the lowest energy π → π* transitions. The light-absorbing part of the molecule is called the chromophore, and the substituents directly attached to the chromophore are called auxochromes. A strong correlation exists between the absorption maxima, λmax, and the structure of a conjugated π system. The Woodward–Fieser rules predict the value of λmax for a given structure by adding the...
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Atomic Absorption Spectroscopy: Instrumentation01:22

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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.
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IR Spectrometers

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There are two main infrared (IR) spectrophotometers: dispersive IR spectrometers and Fourier transform infrared (FTIR) spectrometers. In a dispersive IR spectrometer, a beam of infrared radiation produced by a hot wire is divided into two parallel equal-intensity beams using mirrors. One beam passes through the sample, while another is a reference beam. The beams then move through the monochromator, which separates the radiations into a continuous spectrum of different frequencies. The...
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Dispersion-compensated Rowland spectrometer: implications for uranium VB-RIXS.

Martin Sundermann1, Manuel Harder2, Ayman H Said3

  • 1Deutsches Elektronen-Synchrotron DESY, Notkestr. 85, 22607 Hamburg, Germany.

Journal of Synchrotron Radiation
|December 11, 2025
PubMed
Summary
This summary is machine-generated.

Optimizing valence-band resonant inelastic X-ray scattering (VB-RIXS) instruments is crucial. This study shows that matching source and spectrometer dispersion, not incident bandwidth, achieves high resolution in tender X-ray VB-RIXS.

Keywords:
IRIXS beamlinePETRA III, DESYRIXSRowland spectrometerVB-RIXS

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Area of Science:

  • Spectroscopy
  • Materials Science
  • X-ray Physics

Background:

  • Valence-band resonant inelastic X-ray scattering (VB-RIXS) is a powerful technique for studying electronic structures.
  • Achieving high total energy resolution (ΔEtot) in VB-RIXS is challenging due to its flux-limited nature.
  • Current approaches often involve matching spectrometer specifications to incident bandwidth (ΔEi), which can be limited by count rates.

Purpose of the Study:

  • To investigate the performance of a tender X-ray Rowland spectrometer under conditions of high flux and large linear dispersion.
  • To determine the optimal parameters for achieving high intrinsic resolution (ΔEa) in VB-RIXS experiments.
  • To explore the tunability of the spectrometer for application across different atomic edges.

Main Methods:

  • Detailed ray tracing simulations were performed for a tender X-ray Rowland spectrometer.
  • The study focused on the U M5-edge (3551 eV) as a specific case.
  • Experimental data was used to validate the findings from ray tracing.

Main Results:

  • High intrinsic resolution (ΔEa) can be achieved by matching the linear dispersion of the X-ray source to that of the spectrometer, with opposite signs.
  • The incident bandwidth (ΔEi) becomes irrelevant when dispersion is properly matched.
  • Experimental validation confirmed a total energy resolution (ΔEtot) of 48 meV (ΔEa = 44 meV).

Conclusions:

  • The findings challenge the conventional approach of matching incident bandwidth in VB-RIXS.
  • A new method for optimizing VB-RIXS resolution by controlling linear dispersion is demonstrated.
  • The tunability of the dispersion rate ensures the applicability of this method to various atomic edges, enhancing its versatility.