ANS is committed to advancing, fostering, and promoting the development and application of nuclear sciences and technologies to benefit society.
Explore the many uses for nuclear science and its impact on energy, the environment, healthcare, food, and more.
Explore membership for yourself or for your organization.
Conference Spotlight
2026 ANS Annual Conference
May 31–June 3, 2026
Denver, CO|Sheraton Denver
Latest Magazine Issues
Apr 2026
Jan 2026
Latest Journal Issues
Nuclear Science and Engineering
June 2026
Nuclear Technology
March 2026
Fusion Science and Technology
May 2026
Latest News
DOE selects first companies for nuclear launch pad
The Department of Energy’s Office of Nuclear Energy and the National Reactor Innovation Center have announced their first selections for the Nuclear Energy Launch Pad: three companies developing microreactors and one developing fuel supply.
The four companies—Deployable Energy, General Matter, NuCube Energy, and Radiant Industries—were selected from the initial pool of Reactor Pilot Program and Fuel Line Pilot Program applicants, the two precursor programs to the launch pad.
Robert Conn
Nuclear Science and Engineering | Volume 40 | Number 1 | April 1970 | Pages 17-24
Technical Paper | doi.org/10.13182/NSE70-A18876
Articles are hosted by Taylor and Francis Online.
The total one-phonon coherent neutron scattering cross section for graphite is evaluated using an approximate model of the dispersion relations. A relatively simple phonon frequency distribution is derived and multiphonon terms are calculated in the incoherent approximation. The results are compared with experimental and other theoretical calculations based upon the incoherent approximation. The latter have been consistently lower than the experimental results by a factor of two or more. It is found that the out-of-plane or z-mode contributes ∼ 75% of the one-phonon cross section. The value of [υ Σ01 (υ)]min is found to be ∼70% greater than the same quantity obtained with the same model in the incoherent approximation. Moreover, the λ-law or constant collision frequency domain only begins with neutron wavelengths >∼20 Å (the Bragg cutoff is 6.7 Å).