Measurements of the Differential Cross Sections for the Elastic n-[superscript 3]H and n--[superscript 2]H Scattering at 14.1 MeV by Using an Inertial Confinement

Measurements of the differential cross sections for the elastic n-3H and n-2H scattering at 14.1 MeV by using an inertial confinement fusion facility.

For the first time the differential cross section for the elastic neutron-triton (n-(3)H) and neutron-deuteron (n-(2)H) scattering at 14.1 MeV has been measured by using an inertial confinement fusion facility. In these experiments, which were carried out by simultaneously measuring elastically scattered (3)H and (2)H ions from a deuterium-tritium gas-filled inertial confinement fusion capsule ...

PSFC/JA-11-19 Measurements of the differential cross section for the elastic n-H and n-H scattering at 14.1 MeV by using an Inertial Confinement Fusion (ICF) facility

پراکندگی کشسان یون‌های N15 توسط C12 درMeV 23

Scattering of 15N ions with the energy of Elab = 23 MeV on the CH2(Au) target is investigated.  Elastic scattering of these ions in the angular range of 7°-19° was measured by employing the silicon strip detector, “LEDA”. Using the measured scattering data, deviation of ion beam, number of incident ions on the target and differential cross sections of the 12C(15N, 15N)12C elastic scattering in ...

A triple-resonance pulse scheme for selectively correlating amide <Superscript>1 </Superscript>H <Superscript>N </Superscript> and <Superscript>15 </Superscript>N nuclei with the <Superscript>1 </Superscript>H <Superscript> </Superscript> proton of the preceding residue

A 3D ~H-~SN-13C triple resonance experiment is presented that contains exclusively cross peaks between the ~H N and ~SN nuclei of one residue with the H" of the preceding residue. The pulse sequence, designed to minimize the time coherence, is transverse on nuclei with short T'2 values. The experiment consists of coherence transfers via one-bond couplings from the H N via N, CO, C '~ to the H" ...

محاسبه سطح مقطع جزیی انتقال حالت به حالت بار به روش فادیف

  A second-order approximation to the Faddeev-Watson-Lovelace treatment of the rearrangement channel is used in a three-body scattering cross sections. In this formalism, the Three-body wave function is expressed by three coupled integral equations, the Faddeev equations, which contian the two-body (off-shell) transition amplitudes, and proved the uniqueness of their solutions. This amplitude c...