Second-Generation Optimized Fabry-Perot Doppler Imager (SOFDI)
Program Directive
To design and build a portable, remote controlled instrument that can
map the dayglow and nightglow thermospheric horizontal and vertical
winds and temperatures.
Program Affiliates



Abstract
Daytime measurements of winds and temperatures based on the 630 nm emission
from thermospheric atomic oxygen (OI) have been difficult to obtain
because of the large solar background continuum which overpowers the
comparatively weak emission. Though measurements of this dayglow transition
have been attempted by a number of different groups in the past, the
scientific significance of these measurements has been somewhat limited
in scope. However, the Second generation Optimized Fabry-Perot Doppler
Imager (SOFDI), based on the design of the UARS HRDI instrument, makes
use of a number of innovative optical techniques which will allow for
day and night measurements of the 630 nm line, as well as the 557 nm
transition of OI, the 732 nm transition of O+, and the 840 nm 6-2 P1(2)
rotational line of OH, and others. These results are expected to yield
a wealth of information for the aeronomy community, including the mapping
of the dayglow and nightglow thermospheric horizontal and vertical winds,
study of the 630 nm dayglow brightness distribution as applied to the
Appleton anomaly formation, 732 nm observations of ion temperatures
and ion drifts during morning or evening twilight, measurements of the
variability of thermospheric atomic oxygen concentrations, the investigation
of possible hot oxygen at low latitudes, the determination
of OH rotational temperature and winds, observations of the full diurnal
variation of thermospheric temperature and winds, etc. As such, as part
of the SOFDI initiative, it is the purpose of this paper to present
1) an up-to-date summary of the construction of the SOFDI instrument
and 2) an overview of the instrument forward model and associated inversion
algorithms based on theoretical calculations. It is shown that the construction
of the SOFDI instrument is preceding as scheduled, and will be ready
for test runs in early July 2003 in upstate New York. In addition, we
show that the data analysis infrastructure is currently being optimized
based on results from the forward model. We expect that by late August/early
September, the SOFDI instrument will be ready for scientific data collection.
Introduction
Advances in Fabry-Perot technology over the past decade with regard
to etalon assembly design, transmission of fiber optics cables, optical
conversion of the interferogram from circle to line combined with major
improvements in detector sensitivity and low noise characteristics have
made possible the development of a new generation of the triple etalon
Fabry-Perot interferometer that can successfully observe the 630 nm
dayglow to measure thermospheric winds and temperatures with excellent
stability and sensitivity. The SOFDI (Second-generation Optimized Fabry-Perot
Doppler Imager) instrument is modeled after the HRDI (High Resolution
Doppler Imager) interferometer that flew on the Upper Atmosphere Research
Satellite to observe upper atmosphere winds and temperatures in the
daytime. Numerous refinements in the design that greatly enhances the
potential scientific yields from the measurements make SOFDI truly a
remarkable instrument of great versatility with a broad range of applications
pertaining to the observations of the mesosphere and thermosphere airglow
emissions for both day and night. These refinements include:
-
Automatic transformation of the Fabry-Perot triple
etalon optics configured for dayglow measurements into a single high
resolution etalon configuration for nightglow measurements
-
Separate fields of view for simultaneous measurements
of the line-of sight Doppler shifts in
four directions
-
Increase in instrumental sensitivity for nighttime
measurements by field-widening over 12 orders
at 630 nm
-
Excellent instrumental stability of less than 1 m/s
drift over ten hours
-
Doppler calibration against the laboratory cerium
emission line at 630.0202 nm
-
Multiple wavelengths covering OI emissions at 557.7
and 630 nm (mesospheric and thermospheric winds and temperatures)
+ OH emissions at 840nm and 846.5 nm (daytime and nighttime OH rotational
temperatures) + 732.0 emissions of O+ (ion drifts and ion temperatures
-
High spectral resolution observations of the dayglow
continuum with 2.4 Angstrom spectral range (covers Fraunhofer region
of 630 nm dayglow and Fraunhofer region adjacent so an independent
measurement of the Ring Continuum can be made separate from the 630
nm dayglow emission)
-
Observations automatic with Internet access for remote
control of operations.
We provide details regarding these attributes and first results from
laboratory tests of the instrumental stability and instrumental finesse.
To What Accuracy?
SOFDI would observe daytime thermospheric dynamics with
good sensitivity:
+/- 10 m/s, 40 K in 15 minutes
Nighttime measurements would be of high quality enabling vertical wind
measurements
+/-2 m/s, +/- 7-8 K, 10 minutes, for 100 R signal of 630 nm airglow
SOFDI would be very stable: < 1 m/s stability over
ten hours
Science Objectives
1) Thermospheric winds and temperatures in the 630 nm dayglow
Can spread-F be predicted from measurements of daytime zonal winds?
SOFDI would test the hypothesis that an early afternoon reversal signifies
F-layer stability. A late reversal would indicate probable development
of disturbed ionosphere conditions.
Can such activity be forecasted with relevant initial conditions?
SOFDI would observe the development of the EIA structure along the meridian
expected near the magnetic equator in early morning hours after sunrise.
This structure can be correlated with observed development of scintillation
activity and ESF.
2) Mapping of 630 nm emission
Study 630 nm dayglow brightness distribution: Can the Appleton anomaly
formation be detected in early morning?

3) SOFDI would observe thermospheric wind and temperature fluctuations
in a region overlapping with FPI measurements from Arequipa so that
horizontal winds, vertical wind, and the temperature would be observed
simultaneously in a volume of 50 km high, 100-150 km wide.
4) 732 nm O+ observations of spectral shape during twilight
Ion temperatures and F-region plasma drifts
Variability of thermospheric atomic oxygen concentrations
Possible hot oxygen at low latitudes
5) Mesospheric temperatures and winds
Observe diurnal variation of T and U for mesosphere with OH 840 nm
Future Plans
The instrument is currently located in upstate New York
(Oneida, NY)
Wireless operations conducted via cable modem internet access, 10
kW deliverable power, dark skies, 3.2 acre field, conference facilities,
easy access to NY State Thruway
1) Develop experience using the instrumentation (i.e., shake-down
tests)
2) Bistatic observations with MIT-Haystack-Millstone Hill Observatory
Eventually the instrument will be fielded at IGP Huancayo Geophysical
Observatory located at the magnetic equator in Peru. Bistatic measurements
of OI 630 nm Doppler shifts and spectral widths would be possible with
the Arequipa FPI Observatory.  Peru
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