Dr. Jackson et al., THE SEMIANNUAL OSCILLATION IN UPPER STRATOSPHERIC AND MESOSPHERIC WATER-VAPOR AS OBSERVED BY HALOE, Quarterly Journal of the Royal Meteorological Society, 124(551), 1998, pp. 2493-2515
In this paper observations made by the Halogen Occultation Experiment
(HALOE) instrument are used to investigate the semi-annual oscillation
(SAO) in water vapour mixing ratio in the upper stratosphere. We also
present first observations of an SAO in water vapour in the mid to up
per equatorial mesosphere. The HALOE data set, which spans a period of
greater than four years, also facilitates the examination of interann
ual variability, and in particular the effects of quasi-biennial oscil
lation (QBO)ISAO interaction on the water vapour distribution. The dat
a show an SAO in equatorial water vapour near 1 mb, with troughs in Fe
bruary and August and peaks in May and November. This SAO travels down
wards in time to around the 5 mb level, approximately in phase with co
ntemporaneous zonal winds calculated from United Kingdom Meteorologica
l Office (UKMO) analyses. In addition, the UKMO winds show a seasonal
variation in the strength of the SAG, related to which is an annual cy
cle in HALOE water vapour near 1 mb. There is also an SAO in the upper
mesosphere, which has a maximum amplitude approximately 2 1/2 times l
arger than that in the upper stratosphere. This SAO propagates downwar
ds in time, approximately in phase with the zonal winds observed by th
e High-Resolution Doppler Imager instrument. However, the pattern of t
he water vapour maxima between 0.04 and 0.1 mb does not appear to be c
onsistent with the vertical transport that is induced by the SAO in zo
nal wind. There is also an annual cycle in mesospheric water vapour, w
hich results from the modulation of the winds in the mesosphere by the
seasonal cycle in the upper stratospheric SAO in zonal wind. Latitude
/pressure sections show that the amplitude of both the upper stratosph
eric and mesospheric SAO in water vapour decreases away from the equat
or. However, between 30 and 35 degrees S the SAO in the mesosphere is
again large, possibly due to upward transport in winter associated wit
h breaking gravity waves. There are also considerable biennial cycles
in upper stratospheric and mesospheric water vapour, which appear to r
esult chiefly from the phase of the QBO modulating the SAO in zonal wi
nd.