Transfer matrix for a high energy cooling system
A transfer matrix for a high-energy electron cooling system, which describes the linear incoherent effects, is derived. Knowing this matrix we can treat an electron cooling section in the ring as an additional focusing element deforming the beam optic functions due to space charge forces This matrix...
Збережено в:
Дата: | 2004 |
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Автори: | , |
Формат: | Стаття |
Мова: | English |
Опубліковано: |
Національний науковий центр «Харківський фізико-технічний інститут» НАН України
2004
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Назва видання: | Вопросы атомной науки и техники |
Теми: | |
Онлайн доступ: | http://dspace.nbuv.gov.ua/handle/123456789/80616 |
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Назва журналу: | Digital Library of Periodicals of National Academy of Sciences of Ukraine |
Цитувати: | Transfer matrix for a high energy cooling system / A. Dolinskii, P. Zenkevich // Вопросы атомной науки и техники. — 2004. — № 5. — С. 155-157. — Бібліогр.: 7 назв. — англ. |
Репозитарії
Digital Library of Periodicals of National Academy of Sciences of UkraineРезюме: | A transfer matrix for a high-energy electron cooling system, which describes the linear incoherent effects, is derived. Knowing this matrix we can treat an electron cooling section in the ring as an additional focusing element deforming the beam optic functions due to space charge forces This matrix can be implemented in different codes
(MAD, MIRKO, SixTrack et al.) for precise calculation of the beam optic and dynamic aperture in storage rings,
where a high energy electron cooling system is planed to install. As an example, an optic of the high-energy storage
ring [6] calculated by MAD code with derived matrix is given. |
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