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Spectrophotometry: Introduction01:16

Spectrophotometry: Introduction

8.5K
Spectrophotometry is the quantitative measurement of the absorption, reflection, diffraction, or transmission of electromagnetic radiation through a material as a function of the intensity and wavelength of the radiation. A spectrophotometer is a device used to measure the change in the radiation intensity caused by its interaction with the material.
The essential components of a spectrophotometer include a source of electromagnetic radiation, a slot for placing a material to be analyzed, and a...
8.5K
Attenuated Total Reflectance (ATR) Infrared Spectroscopy: Overview01:13

Attenuated Total Reflectance (ATR) Infrared Spectroscopy: Overview

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Attenuated total reflectance (ATR) infrared spectroscopy is a powerful analytical technique used to study the composition of materials. It is widely employed in chemistry, materials science, forensic science, and other fields where sample characterization is required. ATR has several advantages over traditional transmission IR spectroscopy, including the requirement of little to no sample preparation and the ability to analyze a wide range of samples.
The ATR process begins by directing a beam...
1.5K
Atomic Absorption Spectroscopy: Interference01:25

Atomic Absorption Spectroscopy: Interference

2.3K
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,...
2.3K
NMR Spectrometers: Resolution and Error Correction01:14

NMR Spectrometers: Resolution and Error Correction

994
When magnetic nuclei in a sample achieve resonance and undergo relaxation, the signal detected in NMR is an approximately exponential free induction decay. Fourier transform of an exponential decay yields a Lorentzian peak in the frequency domain. Lorentzian peaks in an NMR spectrum are defined by their amplitude, full width at half maximum, and position, where the peak width is governed by the spin-spin relaxation time alone. In real experiments, however, the applied magnetic field is rendered...
994
Atomic Absorption Spectroscopy: Instrumentation01:22

Atomic Absorption Spectroscopy: Instrumentation

2.1K
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...
2.1K
UV–Vis Spectrometers01:14

UV–Vis Spectrometers

4.1K
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.
4.1K

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Related Experiment Video

Updated: May 5, 2026

Excitation-Scanning Hyperspectral Imaging Microscopy to Efficiently Discriminate Fluorescence Signals
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Attenuation correction in SPECT without attenuation map.

Krzysztof Kacperski1

  • 1Maria Skłodowska - Curie Memorial Cancer Centre and Institute of Oncology, Warsaw, Poland ( k.kacperski@zfm.coi.pl ).

IEEE Nuclear Science Symposium Conference Record. Nuclear Science Symposium
|November 26, 2013
PubMed
Summary

This study introduces a new method for attenuation correction in Single Photon Emission Tomography (SPECT) using only emission data. The approach simplifies SPECT imaging by calculating correction factors directly, improving systems without transmission scans.

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Area of Science:

  • Medical Imaging
  • Nuclear Medicine
  • Image Reconstruction

Background:

  • Attenuation correction is crucial for accurate quantitative analysis in Single Photon Emission Computed Tomography (SPECT).
  • Traditional methods often rely on transmission scans, which are not always available or feasible.
  • Existing emission-only methods may require assumptions about the attenuation map, limiting their applicability.

Purpose of the Study:

  • To develop an emission-only attenuation correction method for SPECT.
  • To simplify the attenuation correction process by avoiding direct attenuation map reconstruction.
  • To provide a viable correction strategy for SPECT systems lacking transmission scan capabilities.

Main Methods:

  • The proposed algorithm utilizes the Helgason-Ludwig consistency conditions.
  • It directly calculates correction factors for projection data, bypassing the need to determine the attenuation map.
  • This approach avoids assumptions regarding the spatial distribution of attenuation within the object.

Main Results:

  • The method provides an approximate attenuation correction based solely on emission data.
  • It offers a simpler alternative to traditional attenuation correction techniques.
  • The algorithm's effectiveness is demonstrated in improving SPECT image quality.

Conclusions:

  • This novel emission-only method offers a practical solution for attenuation correction in SPECT.
  • It enhances the utility of SPECT systems that do not incorporate transmission scanning.
  • The approach holds potential for integration with other correction techniques for further image quality improvement.