1959
DOI: 10.2748/tmj/1178244587
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Cited by 5 publications
(4 citation statements)
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“…The deeper regions of the atmosphere are hotter, so more flux emerges in this polarization state. Nearly complete polarization can result for the thermal emission (Kanno 1975; Pavlov & Shibanov 1978; Ventura, Nagel & Meszaros 1979).…”
Section: Introductionmentioning
confidence: 99%
See 1 more Smart Citation
“…The deeper regions of the atmosphere are hotter, so more flux emerges in this polarization state. Nearly complete polarization can result for the thermal emission (Kanno 1975; Pavlov & Shibanov 1978; Ventura, Nagel & Meszaros 1979).…”
Section: Introductionmentioning
confidence: 99%
“…Thus, the different polarizations should be added together appropriately. If nothing happens to the photons and their polarization as they propagate from the NS surface, then the polarizations observed at infinity can be added rather simply, as was performed by Kanno (1975) in a simple model for the atmosphere. Pavlov & Zavlin (2000) used a more realistic atmosphere and calculated the net observed polarization while taking the effects that general relativity (GR) has on the magnetic field and on light ray bending.…”
Section: Introductionmentioning
confidence: 99%
“…Since from what we have seen, %(H(%(H))) = %(H) and ife^(G) = *nίG). The lemma 2 of [7] shows that Fϊ = H. gives a permutation of {££/, .,., Lt s f\ and P(X) = Π (X -L* /) is in [X] such that P(/) = 0. So %(H 0 ) is algebraic over 3<H) and 3(H 0 ) = δ (//).…”
Section: The Correspondences H-*%(h) and % -» H($s) Are The Inverses ...mentioning
confidence: 99%
“…Let H l9 9 H ι> X r , r roots, be a canonical base of β, from which G is constructed 7) ; let β Ω , ί) Ω be the tensor product of ίl and the additive group generated by (H 19 % H l9 X r9 r roots), (H l9 , H t ) respectively. β Ω is the Lie aegebra over β, and we denote also by H u X r etc.…”
Section: )mentioning
confidence: 99%