Deuteron-Helium Differential Scattering Cross Sections

Galonsky, A.; Douglas, R. A.; Haeberli, W.; McEllistrem, M. T.; Richards, H. T.

doi:10.1103/physrev.98.586

Cited by 57 publications

(36 citation statements)

References 12 publications

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“…Elastic recoil detection analysis (ERDA) can yield non-destructively an accurate depth profile of hydrogen isotopes with a simple experimental technique. Hydrogen isotopes in a several micrometer-thick metal is determined using a 4 He ERDA with an energy E He >10 MeV at a recoil angle approaching zero degrees. The profile's depth resolution can be improved by a transmission ERDA at ¼0 because energy spread caused by multiple scattering is minimized.…”

Section: Introductionmentioning

confidence: 99%

“…The profile's depth resolution can be improved by a transmission ERDA at ¼0 because energy spread caused by multiple scattering is minimized. Accurate values for the elastic recoil cross-sections of p( 4 He, p) 4 He and/or d( 4 He, d) 4 He at recoil angles near 0 is, however, required to obtain quantitative measurements for the hydrogen isotopes.…”

Section: Introductionmentioning

confidence: 99%

“…A few differential recoil cross-sections of p( 4 He, p) 4 He at $0 have been reported in the 4<E He <15 MeV energy range. Nurmela et al measured the cross-sections at ¼4…”

Section: Introductionmentioning

confidence: 99%

“…There are only a few publications on the cross-sections of d( 4 He, d) 4 He at recoil angles of $0 . Galonsky et al reported recoil cross-sections at ¼3:2 in the energy range of 0:6<E He <9:2 MeV.…”

Section: Introductionmentioning

confidence: 99%

“…Galonsky et al reported recoil cross-sections at ¼3:2 in the energy range of 0:6<E He <9:2 MeV. These values were calculated by measuring the elastic scattering cross-sections of 4 He(d, d) 4 He. 4) Hardekopf et al used phase shift analysis to determine the cross-section curves of 4 He(d, d) 4 He in the deuteron energy E d range of 6.04 to 7.05 MeV.…”

Section: Introductionmentioning

confidence: 99%

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Recoil Cross-Sections of Proton and Deuteron by⁴He at a Recoil Angle of 0°in an Energy Range of 5–14 MeV

Ishigami

Ito

Yasuda

et al. 2004

Journal of Nuclear Science and Technology

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Section: Introductionmentioning

confidence: 99%

Section: Introductionmentioning

confidence: 99%

“…A few differential recoil cross-sections of p( 4 He, p) 4 He at $0 have been reported in the 4<E He <15 MeV energy range. Nurmela et al measured the cross-sections at ¼4…”

Section: Introductionmentioning

confidence: 99%

Section: Introductionmentioning

confidence: 99%

Section: Introductionmentioning

confidence: 99%

See 3 more Smart Citations

Recoil Cross-Sections of Proton and Deuteron by⁴He at a Recoil Angle of 0°in an Energy Range of 5–14 MeV

Ishigami

Ito

Yasuda

et al. 2004

Journal of Nuclear Science and Technology

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Elastic Recoil Detection Analysis

Trocellier¹

2000

Encyclopedia of Analytical Chemistry

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In 1976, a Canadian group described in detail for the first time a new ion beam analytical method based on the elastic recoil of target nuclei collided with high energy heavy incident ions. In this case 25–40‐MeV 35 Cl impinged on a multilayer C or Cu (backing)/LiF or LiOH/Cu (30–150 nm)/LiF or LiOH and H, Li, O and F recoiled atoms were detected. These exemplified the main characteristics of elastic recoil detection analysis (ERDA): its sensitivity to depth distribution and its ability to detect light elements in heavy substrates. In 1979, the use of megaelectronvolt energy 4 He beams permitted the use of ERDA to be extended to depth profiling of hydrogen isotopes in the near surface region of solids. ERDA has rapidly been revealed to be an excellent alternative to resonant nuclear reaction spectrometry for hydrogen determination in solids. Despite its less advantageous performance with respect to its lower depth resolution, lower analyzable depth, comparable sensitivity and more restricting irradiation and detection geometry, some ERDA features have made its development in ion beam analysis (IBA) laboratories worldwide easier; these are simultaneous access to 1 H and 2 H depth distributions, access to single‐ended Van de Graaff accelerators compared with tandem or cyclotrons, the ability to be combined with Rutherford backscattering spectrometry (RBS) and a less damaging effect on the investigated targets compared to those generated by heavy ions. The development of detection devices and the analytical capabilities offered by high‐energy heavy ion‐induced ERDA in material sciences for profiling light, medium and large mass number elements give this method a wide area in which to progress as illustrated by discussions at ion beam‐related technique conferences.

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Elastic Recoil Detection Analysis

Trocellier

Sajavaara

2008

Encyclopedia of Analytical Chemistry

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In 1976, a Canadian group described in detail for the first time a new ion beam analytical method based on the elastic recoil of target nuclei collided with high‐energy heavy incident ions. In this case, 25–40‐MeV 35 Cl impinged on a multilayer C or Cu (backing)/LiF or LiOH/Cu (30–150 nm)/LiF or LiOH and H, Li, O, and F recoiled atoms were detected. These exemplified the main characteristics of elastic recoil detection analysis (ERDA): its sensitivity to depth distribution and its ability to detect light elements in heavy substrates. In 1979, the use of megaelectronvolt energy 4 He beams permitted the use of ERDA to be extended to depth profiling of hydrogen isotopes in the near‐surface region of solids. ERDA has rapidly been revealed to be an excellent alternative to resonant nuclear reaction spectrometry ( see Nuclear Reaction Analysis ) for hydrogen determination in solids. Despite its less advantageous performance with respect to its lower depth resolution, lower analyzable depth, comparable sensitivity, and more restricting irradiation and detection geometry, some ERDA features have made its development in ion beam analysis (IBA) laboratories worldwide easier; these are simultaneous access to 1 H and 2 H depth distributions, access to single‐ended Van de Graaff accelerators compared with tandem accelerators or cyclotrons, and the ability to be combined with Rutherford backscattering spectrometry (RBS) ( see Rutherford Backscattering Spectroscopy ). The development of detection devices and the analytical capabilities offered by high‐energy heavy‐ion‐induced ERDA in material sciences for profiling light, medium, and high mass number elements give this method a wide area in which to progress. The main advantage of heavy‐ion ERDA and quite unique feature among analysis techniques is the fact that all sample elements can be depth profiled in one measurement by single detector telescope. By means of Monte Carlo (MC) simulations, the interpretation and reliability of the results have increased greatly over the last few years.

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Deuteron-Helium Differential Scattering Cross Sections

Cited by 57 publications

References 12 publications

Recoil Cross-Sections of Proton and Deuteron by⁴He at a Recoil Angle of 0°in an Energy Range of 5–14 MeV

Recoil Cross-Sections of Proton and Deuteron by⁴He at a Recoil Angle of 0°in an Energy Range of 5–14 MeV

Elastic Recoil Detection Analysis

Elastic Recoil Detection Analysis

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Deuteron-Helium Differential Scattering Cross Sections

Cited by 57 publications

References 12 publications

Recoil Cross-Sections of Proton and Deuteron by4He at a Recoil Angle of 0°in an Energy Range of 5–14 MeV

Recoil Cross-Sections of Proton and Deuteron by4He at a Recoil Angle of 0°in an Energy Range of 5–14 MeV

Elastic Recoil Detection Analysis

Elastic Recoil Detection Analysis

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Product

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Recoil Cross-Sections of Proton and Deuteron by⁴He at a Recoil Angle of 0°in an Energy Range of 5–14 MeV

Recoil Cross-Sections of Proton and Deuteron by⁴He at a Recoil Angle of 0°in an Energy Range of 5–14 MeV