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Concerning the $\nu/N \to {1/3}$ resonance, III : use of the Moser method to estimate the rotation number, as a function of amplitude, for the equation $\frac {d^{2}v}{dt^{2}}+ {(\frac {2\nu}{N})}^{2}v + \frac{1}{2} (\sin2t) v^{2}=0$
| Autor principal: | |
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| Lenguaje: | eng |
| Publicado: |
1959
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| Materias: | |
| Acceso en línea: | http://cds.cern.ch/record/1044935 |
| _version_ | 1780912690320900096 |
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| author | Laslett, L J |
| author_facet | Laslett, L J |
| author_sort | Laslett, L J |
| collection | CERN |
| id | cern-1044935 |
| institution | Organización Europea para la Investigación Nuclear |
| language | eng |
| publishDate | 1959 |
| record_format | invenio |
| spelling | cern-10449352019-09-30T06:29:59Zhttp://cds.cern.ch/record/1044935engLaslett, L JConcerning the $\nu/N \to {1/3}$ resonance, III : use of the Moser method to estimate the rotation number, as a function of amplitude, for the equation $\frac {d^{2}v}{dt^{2}}+ {(\frac {2\nu}{N})}^{2}v + \frac{1}{2} (\sin2t) v^{2}=0$Accelerators and Storage RingsMURA-461oai:cds.cern.ch:10449351959-05-28 |
| spellingShingle | Accelerators and Storage Rings Laslett, L J Concerning the $\nu/N \to {1/3}$ resonance, III : use of the Moser method to estimate the rotation number, as a function of amplitude, for the equation $\frac {d^{2}v}{dt^{2}}+ {(\frac {2\nu}{N})}^{2}v + \frac{1}{2} (\sin2t) v^{2}=0$ |
| title | Concerning the $\nu/N \to {1/3}$ resonance, III : use of the Moser method to estimate the rotation number, as a function of amplitude, for the equation $\frac {d^{2}v}{dt^{2}}+ {(\frac {2\nu}{N})}^{2}v + \frac{1}{2} (\sin2t) v^{2}=0$ |
| title_full | Concerning the $\nu/N \to {1/3}$ resonance, III : use of the Moser method to estimate the rotation number, as a function of amplitude, for the equation $\frac {d^{2}v}{dt^{2}}+ {(\frac {2\nu}{N})}^{2}v + \frac{1}{2} (\sin2t) v^{2}=0$ |
| title_fullStr | Concerning the $\nu/N \to {1/3}$ resonance, III : use of the Moser method to estimate the rotation number, as a function of amplitude, for the equation $\frac {d^{2}v}{dt^{2}}+ {(\frac {2\nu}{N})}^{2}v + \frac{1}{2} (\sin2t) v^{2}=0$ |
| title_full_unstemmed | Concerning the $\nu/N \to {1/3}$ resonance, III : use of the Moser method to estimate the rotation number, as a function of amplitude, for the equation $\frac {d^{2}v}{dt^{2}}+ {(\frac {2\nu}{N})}^{2}v + \frac{1}{2} (\sin2t) v^{2}=0$ |
| title_short | Concerning the $\nu/N \to {1/3}$ resonance, III : use of the Moser method to estimate the rotation number, as a function of amplitude, for the equation $\frac {d^{2}v}{dt^{2}}+ {(\frac {2\nu}{N})}^{2}v + \frac{1}{2} (\sin2t) v^{2}=0$ |
| title_sort | concerning the $\nu/n \to {1/3}$ resonance, iii : use of the moser method to estimate the rotation number, as a function of amplitude, for the equation $\frac {d^{2}v}{dt^{2}}+ {(\frac {2\nu}{n})}^{2}v + \frac{1}{2} (\sin2t) v^{2}=0$ |
| topic | Accelerators and Storage Rings |
| url | http://cds.cern.ch/record/1044935 |
| work_keys_str_mv | AT laslettlj concerningthenunto13resonanceiiiuseofthemosermethodtoestimatetherotationnumberasafunctionofamplitudefortheequationfracd2vdt2frac2nun2vfrac12sin2tv20 |