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Rutherford scattering elastic

In the analogous RBS analysis, da/dil is given precisely and analytically by the Rutherford scattering formula. Unfortunately, the case of ( He, H) scattering is not quite so simple. While the processes are indeed elastic, their cross sections are dominated by nuclear interaction components except at very low energies. (The H(%e, iH)%e cross section approaches the Rutherford value for energies below 0.8 MeV.)... [Pg.494]

Rutherford scattering is an elastic event, that is, no excitation of either the projectile or target nuclei occurs. However, due to conservation of energy and momentum in the interaction, the kinetic energy of the backscattered ion is less than that of the incident ion. The relation between these energies is the kinematic factor, K, which is given by the expression... [Pg.376]

The first term of (6.85) is the T-matrix element for elastic scattering by the potential U. If U is the Coulomb potential Vc it is the Rutherford-scattering T-matrix element. The second term is the distorted-wave T-matrix element for which we solve the distorted-wave Lippmann-Schwinger equation formed from (6.81). Its explicit form is written by expanding in the complete set of eigenstates of K -I-17. This may include projectile bound states A) defined by... [Pg.153]

Elastic neutron scattering experiments performed on single crystals with the MARI spectrometer at the ISIS pulsed neutron source (Rutherford Appleton Laboratory, Chilton UK)3 have evidenced quantum interference in accordance with Eq. (20) [Ikeda 1999], For example, the best fit to the cut of S (Qx, Qy, 0) along Qy is presented in Fig. 16. [Pg.523]

Fig. 2 Electron-atom interactions. (A) Elastic electron-electron interaction dominates the scattering intensity at low and medium scattering angles (B) Rutherford scattering at the nucleus causes high-angle scattering and (C) electrons can excite atom-bonded electrons from the ground state to higher unoccupied states or to the vacuum level, element specific X-rays are produced when the excited electron returns to the ground state. (View this art in color at www.dekker.com.)... Fig. 2 Electron-atom interactions. (A) Elastic electron-electron interaction dominates the scattering intensity at low and medium scattering angles (B) Rutherford scattering at the nucleus causes high-angle scattering and (C) electrons can excite atom-bonded electrons from the ground state to higher unoccupied states or to the vacuum level, element specific X-rays are produced when the excited electron returns to the ground state. (View this art in color at www.dekker.com.)...
The chance that one particle from the beam ejects a recoil of element Z2, M2) in such a way that it starts moving in the direction of the detector is proportional to the areal density (atom cm ) of this element and the detector solid angle of the detector. Treating the interaction as purely Rutherford scattering (since the energy available in the center of mass is at least five times below the Coulomb barrier) the elastic scattering cross-section is given by Rutherford differential cross-section for ERD i.e.,... [Pg.147]

The use of nuclear techniques allows the determination of C, N, H, O, and heavier contaminants relative fractions with great accuracy, and of the elements depth profile with moderate resolution (typically 10 nm). Rutherford backscattering spectroscopy (RBS) of light ions (like alpha particles) is used for the determination of carbon and heavier elements. Hydrogen contents are measured by forward scattering of protons by incident alpha particles (ERDA) elastic recoil detection analysis [44,47]. [Pg.227]

Rutherford backscattering spectrometry (RBS) which analyses the elastic scattering of the particle beam from the target nuclei. Most RBS analyses use less than 2.2 MeV He++ beams. [Pg.69]

There is some disagreement in the literature as to the value of the (4He, H) elastic scattering cross section. Values differing by almost a factor of two have been reported, as reviewed by Paszti et al. (1986). The cross section is strongly non-Rutherford, but ab initio calculations have been reported that agree well with the trend of experimental data and could be used in simulation calculations (Tirira et al., 1990). The cross section for deuterium analysis has a resonance near a 4He+ energy of 2.15 MeV, which allows enhanced sensitivity. Detailed measurements of this cross section have been reported by Besenbacher et al. (1986). In practice, rather than calculate an experiment s calibration from first principles, calibration standards are usually used hydrogen-implanted silicon standard are the norm. [Pg.209]


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Rutherford

Rutherford scattering

Scatter elastically

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