Partial Dispersion Relations Research Articles

Inelastic scattering of He atoms from a Cu(110) surface

A He beam has been used to measure inelastic scattering from a Cu(110) surface. The scattering was a result of predominantly single phonon events and both energy gain and loss processes were observed. This was in contrast to Cu(001) where only energy loss was observed. For Cu(110), aligned in the [001] azimuth, partial dispersion relations have been measured which meant that phonons with Δ Q values up to the zone boundary value have not been detected under the present experimental conditions. The elastic incoherent component varied with azimuthal angle for Cu(110).

Partial wave dispersion relations for lambda-nucleon scattering

Partial wave dispersion relations are derived for the process Λ+N→ Λ+N and the associated processes Λ+ % MathType!MTEF!2!1!+-% feaafiart1ev1aaatuuDJXwAK1uy0Hwmaerbfv3ySLgzG0uy0Hgip5% wzamXvP5wqonvsaeHbfv3ySLgzaeXafv3ySLgzGmvETj2BSbWexLMB% bXgBcf2CPn2qVrwzqf2zLnharCWqVvNCPvMCG4uz3bqehqvATv2CG4% uz3bIuV1wyUbqeeuuDJXwAKbsr4rNCHbGeaGqiVu0Je9sqqrpepC0x% bbL8F4rqqrFfpiZxe9LqFHe9Lqpepeea0xd9q8as0-LqLs-Jirpepe% ea0-as0Fb9pgea0lrP0xe9Fve9Fve9qapdbaGaaiaadaWaamaaceGa% aqaafaGbaaGcbaacbaGaf8xdX7Kbaebaaaa!4CD9! $$\bar {\mathcal{N}}$$ →Λ+ % MathType!MTEF!2!1!+-% feaafiart1ev1aaatuuDJXwAK1uy0Hwmaerbfv3ySLgzG0uy0Hgip5% wzamXvP5wqonvsaeHbfv3ySLgzaeXafv3ySLgzGmvETj2BSbWexLMB% bXgBcf2CPn2qVrwzqf2zLnharCWqVvNCPvMCG4uz3bqehqvATv2CG4% uz3bIuV1wyUbqeeuuDJXwAKbsr4rNCHbGeaGqiVu0Je9sqqrpepC0x% bbL8F4rqqrFfpiZxe9LqFHe9Lqpepeea0xd9q8as0-LqLs-Jirpepe% ea0-as0Fb9pgea0lrP0xe9Fve9Fve9qapdbaGaaiaadaWaamaaceGa% aqaafaGbaaGcbaacbaGaf8xdX7Kbaebaaaa!4CD9! $$\bar {\mathcal{N}}$$ and Λ+ % MathType!MTEF!2!1!+-% feaafiart1ev1aaatuuDJXwAK1uy0Hwmaerbfv3ySLgzG0uy0Hgip5% wzamXvP5wqonvsaeHbfv3ySLgzaeXafv3ySLgzGmvETj2BSbWexLMB% bXgBcf2CPn2qVrwzqf2zLnharCWqVvNCPvMCG4uz3bqehqvATv2CG4% uz3bIuV1wyUbqeeuuDJXwAKbsr4rNCHbGeaGqiVu0Je9sqqrpepC0x% bbL8F4rqqrFfpiZxe9LqFHe9Lqpepeea0xd9q8as0-LqLs-Jirpepe% ea0-as0Fb9pgea0lrP0xe9Fve9Fve9qapdbiGaaiGadiWacmaaceGa% aqaafaGbaaGcbaacdaGaf83MdWKbaebaaaa!4C81! $$\bar \Lambda $$ →N+ % MathType!MTEF!2!1!+-% feaafiart1ev1aaatuuDJXwAK1uy0Hwmaerbfv3ySLgzG0uy0Hgip5% wzamXvP5wqonvsaeHbfv3ySLgzaeXafv3ySLgzGmvETj2BSbWexLMB% bXgBcf2CPn2qVrwzqf2zLnharCWqVvNCPvMCG4uz3bqehqvATv2CG4% uz3bIuV1wyUbqeeuuDJXwAKbsr4rNCHbGeaGqiVu0Je9sqqrpepC0x% bbL8F4rqqrFfpiZxe9LqFHe9Lqpepeea0xd9q8as0-LqLs-Jirpepe% ea0-as0Fb9pgea0lrP0xe9Fve9Fve9qapdbaGaaiaadaWaamaaceGa% aqaafaGbaaGcbaacbaGaf8xdX7Kbaebaaaa!4CD9! $$\bar {\mathcal{N}}$$ .