Модель Двойного Рассеяния Для Протон-Дейтронного Рассеяния Назад При Высоких Энергиях

Bertocchi, L.; Capella, A.

doi:10.1007/bf02902185

Cited by 68 publications

(14 citation statements)

References 24 publications

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“…The formalism for the coherent K + d→K + d scattering is given in detail in Refs. [19,41,49,50,51]. Here we only list the formulas relevant for our calculation.…”

Section: Formalismmentioning

confidence: 99%

Kaon–deuteron scattering at low energies

Sibirtsev

Haidenbauer

Krewald

et al. 2006

J. Phys. G: Nucl. Part. Phys.

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We review the experimental information on the K + d reaction for K + -meson momenta below 800 MeV/c. The data are analysed within the single scattering impulse approximation -utilizing the Jülich kaon-nucleon model -that allows to take into account effects due to the Fermi motion of the nucleons in the deuteron and the final three-body kinematics for the break-up and charge exchange reaction. We discuss the consistency between the data available for the K + d→K + np, K + d→K 0 pp and K + d→K + d reactions and the calculations based on the spectator model formalism.

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“…The formalism for the coherent K + d→K + d scattering is given in detail in Refs. [19,41,49,50,51]. Here we only list the formulas relevant for our calculation.…”

Section: Formalismmentioning

confidence: 99%

Kaon–deuteron scattering at low energies

Sibirtsev

Haidenbauer

Krewald

et al. 2006

J. Phys. G: Nucl. Part. Phys.

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“…(A, Ao) is the momentum transfer and G is the deuteron vertex function. Expressing G through the non-relativistic deuteron wavefunction (Bertocchi andCapella 1967, Alberi et a1 1972) and reducing the lower internal line to the mass shell we get…”

Section: Formulation Of the Modelmentioning

confidence: 99%

Automated tuning of a CO₂laser to a required oscillation line without a spectral instrument

Petukhov¹,

Горобец²

2005

Quantum Electron.

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We formulate a simple model for the final-state interaction with an intermediate A in deuteron break-up induced by medium-energy hadrons. Since the AN system is close to threshold, we consider only the S wave and we treat the AN interaction by the multichannel K-matrix approach in the effective-range approximation. We can reproduce the rough features of the experimental data for the reactions p D ---f npp and K'D ---+ Ko*pp.

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“…Alberi and Bertocchi (1969a) Backward hadron-deuteron scattering is a case in which the Glauber approximation restricted to small angles, would presumaqly break down. The most straightforward reaction is pd ~ dp, for which Bertocchi and Capella (1967) …”

Section: Ucrl-19851mentioning

confidence: 99%

High-Energy Hadron--Deuteron Scattering.

Joachain¹,

Quigg²

1970

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Модель Двойного Рассеяния Для Протон-Дейтронного Рассеяния Назад При Высоких Энергиях

Cited by 68 publications

References 24 publications

Kaon–deuteron scattering at low energies

Kaon–deuteron scattering at low energies

Automated tuning of a CO₂laser to a required oscillation line without a spectral instrument

High-Energy Hadron--Deuteron Scattering.

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Модель Двойного Рассеяния Для Протон-Дейтронного Рассеяния Назад При Высоких Энергиях

Cited by 68 publications

References 24 publications

Kaon–deuteron scattering at low energies

Kaon–deuteron scattering at low energies

Automated tuning of a CO2laser to a required oscillation line without a spectral instrument

High-Energy Hadron--Deuteron Scattering.

Contact Info

Product

Resources

About

Automated tuning of a CO₂laser to a required oscillation line without a spectral instrument