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Related Concept Videos

¹H NMR: Complex Splitting01:13

¹H NMR: Complex Splitting

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A proton M that is coupled to a proton X results in doublet signals for M. However, NMR-active nuclei can be simultaneously coupled to more than one nonequivalent nucleus. When M is coupled to a second proton A, such as in styrene oxide, each peak in the doublet is split into another doublet.
Splitting diagrams or splitting tree diagrams are routinely used to depict such complex couplings. While drawing splitting diagrams, the splitting with the larger coupling constant is usually applied...
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NMR Spectrometers: Resolution and Error Correction01:14

NMR Spectrometers: Resolution and Error Correction

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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...
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¹³C NMR: Distortionless Enhancement by Polarization Transfer (DEPT)01:20

¹³C NMR: Distortionless Enhancement by Polarization Transfer (DEPT)

1.3K
When proton-coupled carbon-13 spectra are simplified by a broadband proton decoupling technique, structural information about the coupled protons is lost. Distortionless enhancement by polarization transfer (DEPT) is a technique that provides information on the number of hydrogens attached to each carbon in a molecule. While the DEPT experiment utilizes complex pulse sequences, the pulse delay and flip angle are specifically manipulated. The resulting signals have different phases depending on...
1.3K
Interpreting ¹H NMR Signal Splitting: The (n + 1) Rule01:10

Interpreting ¹H NMR Signal Splitting: The (n + 1) Rule

2.9K
In the AX proton spin system, proton A can sense the two spin states of a coupled proton X, resulting in a doublet NMR signal with two peaks of equal (1:1) intensity. When proton A is coupled to two equivalent protons (AX2 spin system), the spin states of each X can be aligned with or against the external field, creating three possible scenarios. This results in a 1:2:1  triplet signal, where the central peak corresponds to the chemical shift of A and is twice as large or intense as the...
2.9K
Proton (¹H) NMR: Chemical Shift01:07

Proton (¹H) NMR: Chemical Shift

3.8K
Organic molecules primarily contain carbon and hydrogen atoms. While all the hydrogen isotopes are NMR-active, protium or hydrogen-1 is the most abundant. It has a significant energy separation between its nuclear spin states due to its large gyromagnetic ratio. As per Boltzmann's distribution, an increase in the energy separation implies a greater excess population of nuclei available for excitation, resulting in a strong NMR absorption signal.
Absorption signals of all the protium nuclei...
3.8K
¹³C NMR: ¹H–¹³C Decoupling01:04

¹³C NMR: ¹H–¹³C Decoupling

1.7K
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...
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Related Experiment Video

Updated: May 2, 2026

Study of Protein Dynamics via Neutron Spin Echo Spectroscopy
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MONTE CARLO STUDY OF NEUTRON SPECTRA UNFOLDING FOR A PROTON BEAM USING MLEM.

A Díaz-Comeche1, S Oliver1, B Juste1

  • 1Instituto de Seguridad Industrial, Radiofísica y Medioambiental (ISIRYM). Universitat Politècnica de València. Camí de Vera s/n. 46022. València, Spain.

Radiation Physics and Chemistry (Oxford, England : 1993)
|May 1, 2026
PubMed
Summary

This study uses Monte Carlo simulations and a Maximum Likelihood Expectation Maximization (MLEM) algorithm to measure secondary neutron energy spectra from proton therapy. This helps accurately assess stray neutron doses in radiation therapy.

Keywords:
MCNP6Monte Carlo MethodsNeutron Spectrum unfoldingProton therapySecondary Neutrons

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Area of Science:

  • Medical Physics
  • Radiation Dosimetry
  • Nuclear Engineering

Background:

  • Proton therapy generates secondary neutrons, contributing to stray radiation dose for patients and staff.
  • Accurate assessment of neutron doses requires determining their energy spectrum.

Purpose of the Study:

  • To simulate secondary neutron generation in a proton therapy accelerator head.
  • To unfold the neutron energy spectrum using Monte Carlo (MC) simulations and a Maximum Likelihood Expectation Maximization (MLEM) algorithm.
  • To evaluate the response of a newly designed Extended Bonner Sphere Spectrometer (EBSS) for high-energy neutron detection.

Main Methods:

  • MC simulations were used to model neutron generation and detector response.
  • An MLEM algorithm was employed for spectral deconvolution.
  • The EBSS mesh model was simulated and its response evaluated.
  • Simulations were conducted with the EBSS placed at specific distances from the accelerator head.

Main Results:

  • The study successfully reproduced secondary neutron generation using MC simulations.
  • The MLEM algorithm, coupled with the EBSS response, effectively deconvoluted the neutron fluence energy spectrum.
  • Neutron spectra were unfolded in the absence of treatment room elements.

Conclusions:

  • MC simulations and MLEM algorithms are viable tools for assessing neutron spectra in proton therapy.
  • This methodology aids in the accurate evaluation of neutron doses in radiation oncology.
  • The developed EBSS mesh model shows promise for high-energy neutron detection.