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Photo of Polarization Diversity Lidar
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Located at the campus AFARS site are the Polarization Cloud Lidar (PCL) based on ruby laser (0.694 mm wavelength) transmitter, a 3.2-mm wavelength polarimetric Doppler W-band radar, and a midinfrared narrow-beam radiometer. The current specifications of the PCL and the W-band radar are given in Table 1 and 2 , respectively. These instruments point into the zenith direction, which along with other radiometers to be added soon, uniquely characterize the heights and types of clouds and aerosols present above the site. This research is being supported by the National Science Foundation for the basic study of Arctic cloud and aerosol properties, and by NASA, which has interests in compiling data that helps validate and improve the algorithms used by satellite-based radiometers to interpret the clouds and aerosols in the atmosphere. This information also helps in the development of ground-based and upcoming satellite-based approaches to characterize the atmosphere for improved climate research. Prof. Sassen is involved in two NASA satellite development programs for which the AFARS instruments are well-suited to support: the CloudSat satellite with a W-band radar, and the CALIPSO satellite bearing a polarization lidar.
The remaining major remote sensor, the PDL (see Table 3 for specifications), was developed as a testbed for polarization lidar techniques within the initial instrument development phase of the ARM program. Funding has been obtained from the Department of Energy to station the PDL at the North Slope of Alaska ARM site for an extended period, so that periodic mini-field campaigns can be conducted throughout the year under changing Arctic weather conditions. Special attention will be given to cirrus and mixed-phase clouds, cloudless precipitation that develops from open leads in the nearby Arctic Ocean, and the exotic aerosols ranging from Arctic haze to Asian dust storm particles.Before
barging the lidar van up to Barrow, the PDL will be improved through the addition
of a nitrogen Raman receiver channel under support from the National Science
Foundation. Raman lidar technology
permits the direct determination of the extinction coefficients produced by
aerosols and clouds, and so is an important supplement to the normal elastic,
or Mie lidar research capabilities. Gathering a large sample of backscatter-to-extinction ratios
under Arctic conditions will aid in improving radiative transfer calculation
in climate models, and particularly be a boost to better interpreting the
data from the CALIPSO satellite.
TABLE
1: Polarization Cloud
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Operational
Wavelength (Ruby)
0.694 mm
Peak Energy
1.5 J
Maximum PRF
0.1 Hz
Pulse Width
27 ns
Beamwidths - Transmitter
1.0 mrad
Receiver 1.0-3.0 mrad
Receiver Diameter
25 cm telescope
Detectors - Visible
2 PMT's
Scan Rate
Manual
Data Handling
Number of Channels
2 (simultaneous)
Sample Width (resolution) 7.5
m maximum
Range gates
4 k maximum
Pulses Averaged
1
Digitizer Resolution
8 bits
Storage
8 mm tape
Polarization Properties
Transmitted
Vertical
Received
Vert. + Horiz.
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ADDITIONAL EQUIPMENT
a. All-sky video imager with time-lapse VCR
b. PRT-5 narrow-beam (0.140)
mid-IR (9.5-11.5 mm) radiometer +
c. Camcorder camera +
(+ aligned parallel to transmitter on lidar table)
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Operational
Wavelength (W-band)
3.2 mm
Peak Power
1.2 KW
PRF
10 Hz Ð 80 KHz
Pulse Width
27 ns
Beamwidth
0.25 0
Receiver Diameter
90 cm dish
Receiver Gain
57
dB
Maximum Scan Rate
5.0¾ s -1
Data Handling
Number of Channels
6, two Doppler
Sample Width (resolution) 75
m maximum
Range gates
600 maximum
Pulses Averaged
Programable
Digitizer Type
Logarithic
Storage
8 mm tape
Polarization Properties
Transmitted
Vert. + Horiz.
Received
Vert. + Horiz.
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Operational
Wavelength (Nd:YAG)
0.532 + 1.06 mm
(simultaneous)
Peak Energy
0.35 J each color
Maximum PRF
10 Hz
Pulse Width
9 ns
Beamwidths - Transmitter
0.5 mrad
Receiver 0.2-3.8 mrad
high-speed shutter
Receiver Diameter
30 cm (2 telescopes)
Detectors - Visible
2, Gated PMT's
IR
2, SAPD's
Maximum Scan Rate
5.0¾s -1
Data Handling
Number of Channels
4 (simultaneous)
Sample Width (resolution) 1.5
m maximum
Range gates
8 k maximum
Pulses Averaged
1 - 10
Maximum throughput
164 k samples/second
Digitizer Resolution
8 bits
Storage
8 mm tape
Polarization Properties
Transmitted
Vert. (Vis) + Horiz. (IR)
Received
Vert. + Horiz. (Vis. + IR)
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* ADDITIONAL EQUIPMENT
a.
Camcorder camera
b. X-band safety laser-shutdown radar
The specifications of the FARS ruby (0.694 mm) polarization lidar are provided in the AFARS link. The following recent papers also describe the FARS instrumentation and the findings published to date drawn from this extensive measurement campaign.
Sassen, K., J.M. Comstock, and Z. Wang, 2001: Parameterization of the radiative properties of midlatitude high and middle level
clouds. Geophys. Res. Lett., 28, 729-732.
Sassen, K., and J. R. Campbell, 2001: A midlatitude cirrus cloud climatology from the Facility for Atmospheric Remote Sensing: I.
Macrophysical and synoptic properties. J. Atmos. Sci., 58, 481-496.
Sassen, K., and S. Benson, 2001: A midlatitude cirrus cloud climatology from the Facility for Atmospheric Remote Sensing: II.
Microphysical properties derived from lidar depolarization. J. Atmos. Sci., 58, 2103-2112.
Sassen, K., and J. M. Comstock, 2001: A midlatitude cirrus cloud climatology from the Facility for Atmosperic Remote Sensing: III.
Radiative Properties. J. Atmos. Sci.,58, 2113-2127.
Sassen, K., and J.M. Comstock, Z. Wang, and G.G. Mace, 2001: Cloud and aerosol research capabilities at FARS: The Facility for
Atmospheric Remote Sensing. Bull. Amer. Meteor. Soc., 82, 1119-1138.
Sassen, K., 2002: Indirect climate forcing over the western US from Asian dust storms. Geophys. Res. Lett., 29,
10.1029/2001GL014051.
Sassen, K., J. Zhu, and S. Benson, 2003: A midlatitude cirrus cloud climatology form the Facility for Atmospheric Remote Sensing:
IV. Optical displays. Appl. Opt., 42, 332-341.
Sassen, K., 2003: Cirrus cloud irridescence: A rare case study. Appl. Opt., 42, 486-491.
Sassen, K., W.P. Arnott, D. O'C.Starr, G.G Mace, Z. Wang, and M. R. Poellot, 2003: Midlatitude cirrus clouds derived from hurricane
Nora: A case study with implications for ice crystal nucleation and shape. J. Atmos. Sci., 60, 873-891.
Currently, the polarization ruby lidar data has been loaded from March 1992 to December 1998, and this is being updated up to the April 2002 cessation of University of Utah FARS activities. Supplemental datasets will also be added. After selecting the year, the ruby lidar data collected during that year will be given in calendar format: for each (normally ~3-h) data collection period, clicking on “d” yields the digitized data file, “l” the lidar linear depolarization time-versus-height display (note color scale), and “p” the relative returned lidar power display (in a grayscale based on the logarithm of the signal). If data gaps of more than one hour exist, then multiple data files “1, 2. 3….” are provided.