1964
DOI: 10.1175/1520-0469(1964)021<0463:trloao>2.0.co;2
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The Red Line of Atomic Oxygen in the Day Airglow

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Cited by 66 publications
(26 citation statements)
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“…Several of t h e atmospheric s t u d i e s of DR (Dalgarno, 1958(Dalgarno, , 1983) have focused on t h e r o l e of DR i n t h e production of t h e red l i n e of atomic 0 (Dalgarno, 1958;Dalgarno and Walker, 1964; Abreu e t a l . ,…”
Section: Alex Dalgarno Has Made Many S I G N I F I C a N T C O N T R mentioning
confidence: 99%
“…Several of t h e atmospheric s t u d i e s of DR (Dalgarno, 1958(Dalgarno, , 1983) have focused on t h e r o l e of DR i n t h e production of t h e red l i n e of atomic 0 (Dalgarno, 1958;Dalgarno and Walker, 1964; Abreu e t a l . ,…”
Section: Alex Dalgarno Has Made Many S I G N I F I C a N T C O N T R mentioning
confidence: 99%
“…Z=60. The theoretical curve shows the altitude profile of the zenith intensity of the red line that results from excitation by thermal electrons (Dalgarno and Walker, 1964) tions. At higher altitude in the F1 regton, however, the rocket data indicate the existence of an additional source that is responsible for the enhanced red line emission above 190 km.…”
Section: By Comparing Figures 11 and 7 Itmentioning
confidence: 99%
“…The total zenith intensity due to this source is plotted as a function of altitude in Figure 12. Dalgarno and Walker (1964) have sugested that excitation of atomic oxygen by thermal electrons in the high energy tail of the velocity distribution might account for the rocket data above 190km. The red-line emission rate from this source may be calculated using the rate coefficients derived by Seaton (1956).…”
Section: By Comparing Figures 11 and 7 Itmentioning
confidence: 99%
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“…In addition, we may neglect any contribution from the reaction involving NO + because of the spin constraints (Dalgarno and Walker 1964). Assuming, then, that the atoms in 'D State in addition to being depopulated by spontaneous transition are also deactivated by collision with molecular nitrogen, the volume emission rate of 01 6300 is given by ( Peterson et al, 1966;Rees et al, 1967;Forbes, 1970) A(6300) ( I(6300) = A + S N r N jK D°`^ 0 21 It is obvious that in addition to the knowledge of the rate coefficients it is necessary to know the altitude profiles for [Oz], LNOJ, N. , CO]and [N2].…”
Section: Introductionmentioning
confidence: 99%