1964
DOI: 10.1086/147970
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Polarimetric Observations of a Coronal Condensation.

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Cited by 48 publications
(4 citation statements)
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“…It is less important for the structure and evolution of the confined plasma, which follow the field lines whatever shape they have and change little also with moderate changes of the gravity component along the field lines. First works on the accurate determination of the loop geometry date back to the 1960s (Saito and Billings, 1964 ). More specific ones take advantage of stereoscopic views allowed by huge loops during solar rotation, with the aid of magnetic field reconstruction methods.…”
Section: The Observational Frameworkmentioning
confidence: 99%
“…It is less important for the structure and evolution of the confined plasma, which follow the field lines whatever shape they have and change little also with moderate changes of the gravity component along the field lines. First works on the accurate determination of the loop geometry date back to the 1960s (Saito and Billings, 1964 ). More specific ones take advantage of stereoscopic views allowed by huge loops during solar rotation, with the aid of magnetic field reconstruction methods.…”
Section: The Observational Frameworkmentioning
confidence: 99%
“…It is less important for the structure and evolution of the confined plasma, which follow the field lines whatever shape they have and change little also with moderate changes of the gravity component along the field lines. First works on the accurate determination of the loop geometry date back to the sixties (Saito and Billings, 1964). More specific ones take advantage of stereoscopic views allowed by huge loops during solar rotation, with the aid of magnetic field reconstruction methods.…”
Section: Geometrymentioning
confidence: 99%
“…comparer avec les valeurs obtenues parSaito (1964).8. D6termination empirique de param6tres physiques coronauxEn supposant que les raies d'6mission sont optiquement minces (ce qui est vrai dans le cas de 5303 A~), le nombre d'atomes qui peuple le niveau 2P3/2 d'oh est issue la transition est 4n Z N. (r, o) = h~ • A~, e (r, o).…”
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