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@ARTICLE{delaTorre:917457,
author = {de la Torre, A. and Alexander, P. and Marcos, Tomas and
Hierro, R. and Llamedo, P. and Hormaechea, J. L. and
Preusse, P. and Geldenhuys, M. and Krasauskas, L. and Giez,
A. and Kaifler, B. and Kaifler, N. and Rapp, M.},
title = {{A} {S}pectral {R}otary {A}nalysis of {G}ravity {W}aves:
{A}n {A}pplication {D}uring {O}ne of the {SOUTHTRAC}
{F}lights},
journal = {JGR / Atmospheres},
volume = {128},
number = {1},
issn = {0148-0227},
address = {Hoboken, NJ},
publisher = {Wiley},
reportid = {FZJ-2023-00670},
pages = {e2022JD037139},
year = {2023},
abstract = {To understand the main orographic and non-orographic
sources of gravity waves (GWs) over South America during an
Experiment (Rapp et al., 2021,
https://doi.org/10.1175/BAMS-D-20-0034.1), we propose the
application of a rotational spectral analysis based on
methods originally developed for oceanographic studies. This
approach is deployed in a complex scenario of
large-amplitude GWs by applying it to reanalysis data. We
divide the atmospheric region of interest into two height
intervals. The simulations are compared with lidar
measurements during one of the flights. From the degree of
polarization and the total energy of the GWs, the
contribution of the upward and downward wave packets is
described as a function of their vertical wavenumbers. At
low levels, a larger downward energy flux is observed in a
few significant harmonics, suggesting inertial GWs radiated
at polar night jet levels, and below, near to a cold front.
In contrast, the upward GW energy flux, per unit area, is
larger than the downward flux, as expected over mountainous
areas. The main sub-regions of upward GW energy flux are
located above Patagonia, the Antarctic Peninsula and only
some oceanic sectors. Above the sea, there are alternating
sub-regions dominated by linearly polarized GWs and sectors
of downward GWs. At the upper levels, the total available GW
energy per unit mass is higher than at the lower levels.
Regions with different degrees of polarization are
distributed in elongated bands. A satisfactory comparison is
made with an analysis based on the phase difference between
temperature and vertical wind disturbances.},
cin = {IEK-7},
ddc = {550},
cid = {I:(DE-Juel1)IEK-7-20101013},
pnm = {2112 - Climate Feedbacks (POF4-211) / 2A3 - Remote Sensing
(CARF - CCA) (POF4-2A3)},
pid = {G:(DE-HGF)POF4-2112 / G:(DE-HGF)POF4-2A3},
typ = {PUB:(DE-HGF)16},
UT = {WOS:000998847300001},
doi = {10.1029/2022JD037139},
url = {https://juser.fz-juelich.de/record/917457},
}