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Related Concept Videos

Nuclear Transmutation03:20

Nuclear Transmutation

Nuclear transmutation is the conversion of one nuclide into another. It can occur by the radioactive decay of a nucleus, or the reaction of a nucleus with another particle. The first manmade nucleus was produced in Ernest Rutherford’s laboratory in 1919 by a transmutation reaction, the bombardment of one type of nuclei with other nuclei or with neutrons. Rutherford bombarded nitrogen-14 atoms with high-speed α particles from a natural radioactive isotope of radium and observed protons being...
Nuclear Power02:36

Nuclear Power

Controlled nuclear fission reactions are used to generate electricity. Any nuclear reactor that produces power via the fission of uranium or plutonium by bombardment with neutrons has six components: nuclear fuel consisting of fissionable material, a nuclear moderator, a neutron source, control rods, reactor coolant, and a shield and containment system.
Nuclear Fuels
Nuclear fuel consists of a fissile isotope, such as uranium-235, which must be present in sufficient quantity to provide a...
Nuclear Fission02:50

Nuclear Fission

Many heavier elements with smaller binding energies per nucleon can decompose into more stable elements that have intermediate mass numbers and larger binding energies per nucleon—that is, mass numbers and binding energies per nucleon that are closer to the “peak” of the binding energy graph near 56. Sometimes neutrons are also produced. This decomposition of a large nucleus into smaller pieces is called fission. The breaking is rather random with the formation of a large number of different...
Nuclear Binding Energy02:13

Nuclear Binding Energy

The difference between the calculated and experimentally measured masses is known as the mass defect of the atom. In the case of helium-4, the mass defect indicates a “loss” in mass of 4.0331 amu – 4.0026 amu = 0.0305 amu. The loss in mass accompanying the formation of an atom from protons, neutrons, and electrons is due to the conversion of that mass into energy that is evolved as the atom forms. The nuclear binding energy is the energy produced when the atoms’ nucleons are bound together;...
Nuclear Overhauser Enhancement (NOE)01:06

Nuclear Overhauser Enhancement (NOE)

Irradiation of a spin-active nucleus causes an increase or decrease in the signal intensity of neighboring nuclei that are not necessarily chemically bonded or involved in J-coupling. This phenomenon, called the nuclear Overhauser enhancement (NOE), results from through-space interactions between the nuclear spins. The NOE effect decreases with increasing internuclear distance and is generally not observed beyond 4 angstroms. In NOE, dipole-dipole interactions between neighboring spin-active...
Nuclear Fusion02:45

Nuclear Fusion

The process of converting very light nuclei into heavier nuclei is also accompanied by the conversion of mass into large amounts of energy, a process called fusion. The principal source of energy in the sun is a net fusion reaction in which four hydrogen nuclei fuse and ultimately produce one helium nucleus and two positrons.
A helium nucleus has a mass that is 0.7% less than that of four hydrogen nuclei; this lost mass is converted into energy during the fusion. This reaction produces about...

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Updated: Jun 16, 2026

Neutron Radiography and Computed Tomography of Biological Systems at the Oak Ridge National Laboratory's High Flux Isotope Reactor
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Neutron Radiography and Computed Tomography of Biological Systems at the Oak Ridge National Laboratory's High Flux Isotope Reactor

Published on: May 7, 2021

Neutron cross-sections for next generation reactors: new data from n_TOF.

N Colonna1, U Abbondanno, G Aerts

  • 1Istituto Nazionale di Fisica Nucleare, Bari, Italy. nicola.colonna@ba.infn.it

Applied Radiation and Isotopes : Including Data, Instrumentation and Methods for Use in Agriculture, Industry and Medicine
|January 26, 2010
PubMed
Summary
This summary is machine-generated.

The n_TOF facility at CERN provides high-accuracy neutron cross-section data for nuclear astrophysics and advanced reactors. Its advanced features enable crucial measurements for nuclear industry applications.

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Neutron Radiography and Computed Tomography of Biological Systems at the Oak Ridge National Laboratory's High Flux Isotope Reactor
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Area of Science:

  • Nuclear Physics
  • Neutron Scattering
  • Nuclear Astrophysics

Background:

  • The n_TOF (neutron Time-of-Flight) facility at CERN commenced operations in 2002.
  • Unique features include high instantaneous neutron flux, high resolution, and a wide energy range.

Purpose of the Study:

  • To review key results from neutron capture and fission reactions at n_TOF.
  • To present plans for new measurements relevant to the nuclear industry.

Main Methods:

  • Utilizing a state-of-the-art neutron time-of-flight facility.
  • Employing advanced detectors and data acquisition systems for high-accuracy measurements.
  • Collecting data on various isotopes, including radioactive ones.

Main Results:

  • High-accuracy neutron cross-section data have been collected for numerous isotopes.
  • Results are significant for both nuclear astrophysics and advanced reactor technologies.
  • Key findings from capture and fission reactions have been compiled.

Conclusions:

  • The n_TOF facility is a powerful tool for nuclear data acquisition.
  • Ongoing and future measurements will further support nuclear astrophysics and industry applications.
  • The facility's capabilities are crucial for advancing reactor design and safety.