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¹³C NMR: ¹H–¹³C Decoupling01:04

¹³C NMR: ¹H–¹³C Decoupling

The probability of having two carbon-13 atoms next to each other is negligible because of the low natural abundance of carbon-13. Consequently, peak splitting due to carbon-carbon spin-spin coupling is not observed in spectra. However, protons up to three sigma bonds away split the carbon signal according to the n+1 rule, resulting in complicated spectra.
A broadband decoupling technique is used to simplify these complex, sometimes overlapping, signals. Broadband decoupling relies on a...
Carbon-13 (¹³C) NMR: Overview01:10

Carbon-13 (¹³C) NMR: Overview

Carbon-13 is a naturally occurring NMR-active isotope of carbon with a low natural abundance of 1.1%. In contrast, carbon-12 is the most abundant isotope of carbon with zero nuclear spin. Therefore, it is NMR inactive. The gyromagnetic ratio of carbon-13 is smaller than that of protons. As a result, carbon-13 resonance is about 6000 times weaker than proton resonance. For a given magnetic field strength, the resonance frequency of carbon-13 is about one-fourth of the resonance frequency for...
Other Nuclides: 31P, 19F, 15N NMR01:16

Other Nuclides: 31P, 19F, 15N NMR

Many organic, inorganic, and biological molecules contain spin-half nuclei such as nitrogen-15, fluorine-19, and phosphorus-31. As a result, NMR studies of these nuclei have found extensive applications in chemical and biological research.
While fluorine-19 and phosphorous-31 have high natural abundances (100%) and positive gyromagnetic ratios, nitrogen-15 has a low natural abundance and a negative gyromagnetic ratio. However, nitrogen-15 is still preferred over nitrogen-14 (which has a high...
Atomic Mass01:52

Atomic Mass

Atoms — and the protons, neutrons, and electrons that compose them — are extremely small. For example, a carbon atom weighs less than 2 × 10−23 g. When describing the properties of tiny objects such as atoms, we use appropriately small units of measure, such as the atomic mass unit (amu). The amu was originally defined based on hydrogen, the lightest element, then later in terms of oxygen. Since 1961, it has been defined with regard to the most abundant isotope of carbon, atoms of which are...
Isotopes and Radioisotopes01:28

Isotopes and Radioisotopes

In the early 1900s, English chemist Frederick Soddy realized that an element could have atoms with different masses that were chemically indistinguishable. These different types are called isotopes — atoms of the same element that differ in mass. Isotopes differ in mass because they have different numbers of neutrons but are chemically identical because they have the same number of protons. Soddy was awarded the Nobel Prize in Chemistry in 1921 for this discovery.
An isotope containing more...
Atomic Weight01:25

Atomic Weight

Protons and neutrons have approximately the same mass, about 1.67 × 10-24 grams. Scientists arbitrarily define this amount of mass as one atomic mass unit (amu) or one Dalton. Electrons are much smaller in mass than protons, weighing only 9.11 × 10-28 grams, or about 1/1800 of an atomic mass unit. As a result, they do not contribute much to an element's overall atomic mass. This means that, when considering atomic mass, it is customary to ignore the mass of any electrons and calculate the...

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Primary standardization and Monte Carlo modeling of (<sup>243</sup>Am + <sup>239</sup>Np) by means of a 4π(PC)-γ coincidence counting system.

Applied radiation and isotopes : including data, instrumentation and methods for use in agriculture, industry and medicine·2023
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Standardization and determination of the total internal conversion coefficient of In-111.

Applied radiation and isotopes : including data, instrumentation and methods for use in agriculture, industry and medicine·2014
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Primary activity standardization of ⁹⁹Tc by three different absolute methods.

Applied radiation and isotopes : including data, instrumentation and methods for use in agriculture, industry and medicine·2013
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Determination of gamma-ray emission probabilities per decay of Ga-68.

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Calibration of ionization chamber for ¹⁸F and ⁶⁸Ga.

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Monte Carlo simulation to positron emitter standardized by means of 4pibeta-gamma coincidence system--application to 22Na.

Applied radiation and isotopes : including data, instrumentation and methods for use in agriculture, industry and medicine·2010
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Related Experiment Video

Updated: Jun 17, 2026

Automated 90Sr Separation and Preconcentration in a Lab-on-Valve System at Ppq Level
08:53

Automated 90Sr Separation and Preconcentration in a Lab-on-Valve System at Ppq Level

Published on: June 6, 2018

Primary standardization of 57Co.

Marina F Koskinas1, Denise S Moreira, Ione M Yamazaki

  • 1Instituto de Pesquisas Energéticas e Nucleares (IPEN-CNEN/SP), Centro do Reator de Pesquisas-CRPq, São Paulo, SP, Brazil. koskinas@ipen.br

Applied Radiation and Isotopes : Including Data, Instrumentation and Methods for Use in Agriculture, Industry and Medicine
|January 1, 2010
PubMed
Summary

This study details a new method for standardizing Cobalt-57 (57Co) radioactive solutions using 4pi beta-gamma coincidence counting. The developed technique, validated by Monte Carlo simulations, ensures accurate calibration sources for nuclear medicine.

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Last Updated: Jun 17, 2026

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Published on: June 6, 2018

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Enhancing Efficiency and Radiolabeling Yields of Carbon-11 Radioligands for Clinical Research Using the Loop Method
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Published on: December 20, 2024

Area of Science:

  • Nuclear Metrology
  • Radiochemistry
  • Applied Physics

Background:

  • Cobalt-57 (57Co) is crucial for calibrating spectrometers and dose calibrators in nuclear medicine.
  • Accurate standardization of 57Co ensures reliable performance of medical equipment.

Purpose of the Study:

  • To describe a novel method for standardizing 57Co radioactive solutions.
  • To validate the experimental method using Monte Carlo simulations.

Main Methods:

  • Utilized two 4pi beta-gamma coincidence systems with different gamma detectors (NaI(Tl) and HPGe).
  • Employed the Time-to-Amplitude Converter (TAC) method for event registration.
  • Applied Monte Carlo simulations to model detection processes and compare with experimental data.

Main Results:

  • Standardization of 57Co solution was successfully performed.
  • Experimental data showed good agreement with Monte Carlo simulation results.
  • The developed methodology provides accurate activity determination within experimental uncertainty.

Conclusions:

  • The described method offers a reliable approach for 57Co standardization.
  • Monte Carlo simulation is a valuable tool for validating experimental results in nuclear metrology.
  • This work contributes to the quality assurance of nuclear medicine services.