Parity nonconservation in trinucleon bound states
Tensor and operator representations for wave function (WF) of three–nucleon bound states are discussed. It is supposed that space parity is not conserved in interaction between nucleons. The WFs of ³He and ³H are expressed in terms of 16 scalar functions, which depend on the magnitudes of the relati...
Збережено в:
| Дата: | 2007 |
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| Автори: | , |
| Формат: | Стаття |
| Мова: | English |
| Опубліковано: |
Національний науковий центр «Харківський фізико-технічний інститут» НАН України
2007
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| Назва видання: | Вопросы атомной науки и техники |
| Теми: | |
| Онлайн доступ: | http://dspace.nbuv.gov.ua/handle/123456789/110938 |
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| Назва журналу: | Digital Library of Periodicals of National Academy of Sciences of Ukraine |
| Цитувати: | Parity nonconservation in trinucleon bound states / V. Kotlyar and A. Nogga // Вопросы атомной науки и техники. — 2007. — № 3. — С. 126-131. — Бібліогр.: 21 назв. — англ. |
Репозитарії
Digital Library of Periodicals of National Academy of Sciences of Ukraine| Резюме: | Tensor and operator representations for wave function (WF) of three–nucleon bound states are discussed. It is supposed that space parity is not conserved in interaction between nucleons. The WFs of ³He and ³H are expressed in terms of 16 scalar functions, which depend on the magnitudes of the relative momenta and the angle between them. These functions are real in the case when nuclear forces do not violate time reversal symmetry. Characteristic features appropriate to WFs of deuteron and 3N nuclei in operator form (OF) are compared. |
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