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Advanced Airborne UV DIAL System for Stratospheric and Tropospheric Ozone and Aerosol Measurements

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Abstract

An advanced UV DIAL system for airborne measurements of ozone and aerosol distributions across the troposphere and lower stratosphere was developed at the NASA Langley Research Center during 1995. This paper describes the system and its improved performance including examples from the recent TOTE/VOTE field campaign.

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... 355 nm is usually chosen as the operating wavelength for laser wind measurement radars due to the low absorption and high scattering of ultraviolet light in atmospheric molecules, a typical example being the ALADIN developed by European Space Agency (ESA) [24,25]. In addition, 355 nm UV lasers are used in space debris removal [26], the Aerosol/Cloud/Ecosystems (ACE) to be developed by National Aeronautics and Space Administration (NASA) [27,28], the 3-D Winds for space-based measurement of tropospheric winds with global coverage [29] and the Global Atmospheric Composition Mission (GACM) for the Ozone DIAL system [30,31]. In addition, laser-induced damage in the UV band is more susceptible to the effects of space radiation than in other bands, as space radiation damage causes mainly degradation of optical properties in the UV band. ...
... 355 nm is usually chosen as the operating wavelength for laser wind measurement radars due to the low absorption and high scattering of ultraviolet light in atmospheric molecules, a typical example being the ALADIN developed by European Space Agency (ESA) [24,25]. In addition, 355 nm UV lasers are used in space debris removal [26], the Aerosol/Cloud/Ecosystems (ACE) to be developed by National Aeronautics and Space Administration (NASA) [27,28], the 3-D Winds for space-based measurement of tropospheric winds with global coverage [29] and the Global Atmospheric Composition Mission (GACM) for the Ozone DIAL system [30,31]. In addition, laser-induced damage in the UV band is more susceptible to the effects of space radiation than in other bands, as space radiation damage causes mainly degradation of optical properties in the UV band. ...
... Data were collected for 14 flights (including two pre-mission test flights before the deployment to Kiruna). Details of this instrument may be found in Browell et al. (2003), Browell et al. (1998), andRichter et al. (1997). ...
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Ozone measurements from ozonesondes, ARO- TAL, DIAL, and POAM III instruments during the SOLVE- 2/VINTERSOL period are composited in a time-varying, flow-following quasi-conservative (PV- ) coordinate space; the resulting composites from each instrument are mapped onto the other instruments' locations and times. The mapped data are then used to intercompare data from the different in- struments. Overall, the four ozone data sets are found to be in good agreement. AROTAL shows somewhat lower values below 16 km, and DIAL has a positive bias at the upper limits of its altitude range. These intercomparisons are consistent with those obtained from more conventional near-coincident profiles, where available. Although the PV- mapping tech- nique entails larger uncertainties of individual profile differ- ences compared to direct near-coincident comparisons, the ability to include much larger numbers of comparisons can make this technique advantageous.
... The NASA-DC-8 Ozone DIAL system and configuration implemented during the campaign is described by Richter et al. (1997). The instrument provides simultaneous zenith and nadir profiles to cover the troposphere and lower stratosphere. ...
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During the 2008 International Polar Year, the POLARCAT (Polar Study using Aircraft, Remote Sensing, Surface Measurements, and Models of Climate Chemistry, Aerosols, and Transport) campaign, conducted in summer over Greenland and Canada, produced a large number of measurements from three aircraft and seven ozonesonde stations. Here we present an observation-integrated analysis based on three different types of O3 measurements: airborne lidar, airborne UV absorption or chemiluminescence measurement, and intensified electrochemical concentration cell (ECC) ozonesonde profiles. Discussion of the latitudinal and vertical variability of tropospheric ozone north of 55° N during this period is performed with the aid of a regional model (WFR-Chem). The model is able to reproduce the O3 latitudinal and vertical variability but with a negative O3 bias of 6–15 ppbv in the free troposphere above 4 km, especially over Canada. For Canada, large average CO concentrations in the free troposphere above 4 km ( > 130 ppbv) and the weak correlation (< 30 %) of O3 and PV suggest that stratosphere–troposphere exchange (STE) is not the major contributor to average tropospheric ozone at latitudes less than 70° N, due to the fact that local biomass burning (BB) emissions were significant during the 2008 summer period. Conversely, significant STE is found over Greenland according to the better O3 vs. PV correlation ( > 40 %) and the higher values of the 75th PV percentile. It is related to the persistence of cyclonic activity during the summer over Baffin Bay. Using differences between average concentration above Northern and Southern Canada, a weak negative latitudinal summer ozone gradient of −6 to −8 ppbv is found in the mid-troposphere between 4 and 8 km. This is attributed to an efficient O3 photochemical production from BB emissions at latitudes less than 65° N, while the STE contribution is more homogeneous in the latitude range 55–70° N. A positive ozone latitudinal gradient of 12 ppbv is observed in the same altitude range over Greenland not because of an increasing latitudinal influence of STE, but because of different long-range transport from multiple mid-latitude sources (North America, Europe, and even Asia for latitudes higher than 77° N). For the Arctic latitudes (> 80° N), free tropospheric O3 concentrations during summer 2008 are related to a mixture of Asian pollution and stratospheric O3 transport across the tropopause.
... High power laser light sources operating in the ultraviolet (UV) spectral region have received a great deal of interest for numerous applications in science and technology such as semiconductor processing, micromachining, remote sensing with Lidar, engine combustion diagnostics, spectroscopy, medicinal and biological applications. . . [1][2][3][4][5][6]. Hence, there is a great deal of interest for the development of high-power, all-solid-state UV lasers of convenient operating procedures. ...
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We review the recent progresses in generation and amplification of ultraviolet laser emissions using Ce$^{3 + }$:LiCaAlF$_{6}$ (Ce:LiCAF) material as a gain medium. Basing on comparative studies, we have investigated improvements and proposed possibilities to generate and amplify ultraviolet short-pulse Ce:LiCAF laser emission to high peak power of terawatt.
... The current version of NASA Langley's airborne UV DIAL system has been described in detail in two recent publications (Richter et al., 1997;Browell et al., 1998a). This system uses two 30-Hz, frequency-doubled Nd:YAG lasers to sequentially pump two dye lasers that are frequency-doubled into the UV to produce the on-line (288.2 nm/301 nm) and offline (299.6 nm/310 nm) wavelengths for DIAL O 3 measurements during tropospheric and stratospheric missions, respectively. ...
Chapter
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Airborne lidar systems have proven very useful for atmospheric and oceanic studies during the past three decades and more recently for surface and vegetation canopy studies. Typical applications of airborne lidar for atmospheric studies include studying the long-range transport of pollutants, taking large-scale surveys of tropospheric aerosols and ozone (O3) over remote regions of the Earth, studying water vapor (H2O) and the hydrologic cycle, and investigating various processes associated with biomass burning emissions, desert dust transport, stratospheric aerosol transport following volcanic eruptions, polar O3 changes and polar stratospheric clouds (PSCs), and metal ion concentrations in the ionosphere. Airborne lidar systems that are participating in studies of aerosols, O3, and H2O can also be used to make correlative measurements of space-based remote-sensing instruments and serve as test beds on the way to space-based lidar systems. In addition to atmospheric studies, airborne lidar systems have been used for diverse hydrospheric studies, including measurements of chlorophyll, phytoplankton, dissolved organic matter, inorganic suspended material, water depth, and even fish school detection. Airborne lidar systems have been used to study surface properties such as the infrared (IR) reflectivity of desert geological features. Airborne lidar systems have also recently been applied to study the density and structure of the vegetation canopy in forests. The main advantages of airborne lidar systems are that they expand the geographical range of studies beyond those possible by surface-based fixed or mobile lidar systems by virtue of being able to fly to high altitudes and to remote locations. Thus, they permit measurements at locations inaccessible to surface-based lidar systems. For atmospheric studies, they permit measurements over large regions in times that are short, compared with atmospheric motion, so that large-scale patterns are discernable. Another advantage of an airborne lidar is that the normal lidar technique, which uses aerosols and molecules as distributed reflectors, performs better in the nadir direction than in the zenith direction since the atmospheric density increases with range r (decreasing altitude), compensating somewhat for the 1/r2 falloff in lidar signal with range. For the zenith direction, the advantage is that the airborne lidar system is higher and thus closer to the atmosphere being measured. The main disadvantage of using an airborne lidar is the complexity and cost of conducting aircraft operations, a fact that limits the number of airborne missions. This chapter will examine the specific requirements for airborne lidar, review the important application areas of airborne lidar, and then indicate the direction of future airborne lidar applications.
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A long-lived UV laser is an enabling technology for a number of high-priority, space-based lidar instruments. These include a next generation cloud and aerosol lidar that incorporates a UV channel, a direct detection 3-D wind lidar, and an ozone DIAL system. We have designed and built a TRL 6 demonstrator that has increased output power and space-qualifiable packaging that is mechanically robust, thermally-stable, and fully conductively cooled. Contamination control processes and optical coatings have been chosen that are compatible with multi-billion shot lifetimes. The diode pumped laser contains an essentially polymer free internal module that houses the third harmonic generator and expansion optics. When operated at 150 Hz the laser has demonstrated 275 mJ per pulse at 1064 nm, second harmonic conversion efficiencies of 70%, and third harmonic conversion efficiencies of 45%, thus meeting the 355 nm 100 mJ/pulse goal with margin. At this time we have successfully completed a full power 532 nm life test, a half power (50 mJ/pulse) UV lifetest, and a full power (100 mJ/pulse @ 150 Hz) lifetest. These tests have validated the importance and success to our approach to contamination control for achieving a long lived UV laser as well as resurfacing the need for attention to the qualification of the pump laser diodes and attention to the external optical in a UV lidar system.
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An airborne differential absorption lidar (DIAL) system has been developed for the remote measurement of gas and aerosol profiles in the troposphere and lower stratosphere. The multipurpose DIAL system can operate from 280 to 1064 nm for measurements of ozone, sulfur dioxide, nitrogen dioxide, water vapor, temperature,pressure, and aerosol backscattering. The laser transmitter consists of two narrow linewidth Nd: YAG pumped dye lasers with automatic wavelength control. The DIAL wavelengths are transmitted with a 00-,usec temporal separation to reduce receiver system complexity. A coaxial receiver system is used to collect and optically separate the DIAL and aerosol lidar returns. Photomultiplier tubes detect the backscattered laser returns after optical filtering, and the analog signals from three tubes are digitized and stored on high-speed magnetic tape. Real-time gas concentration profiles or aerosol backscatter distributions are calculated and displayed for experiment control. Operational parameters for the airborne DIAL system are presented for measurements of ozone, water vapor, and aerosols in the 290-, 720-, and 600-nm wavelength regions, respectively. The first ozone profile measurements from an aircraft using the DIAL technique are discussed in this paper. Comparisons between DIAL and in situ ozone measurements show agreement to within +/-5 ppbv in the lower troposphere. Lidar aerosol data obtained simultaneously with DIAL ozone measurements are presented for a flight over Virginia and the Chesapeake Bay. DIAL system performance for profiling ozone in a tropopause folding experiment is evaluated, and the applications of the DIAL system to regional and global-scale tropospheric investigations are discussed.
Chapter
Airborne lidar measurements of aerosol and ozone distributions from the surface to above the tropopause over the Western Pacific Ocean are used to quantify the relative contributions of different ozone sources to the tropospheric ozone budget.
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Differential absorption lidar (DIAL) is a powerful remote-sensing technique widely used to probe the spatial and temporal distribution of ozone and other gaseous atmospheric trace constituents. Although conceptually simple, the DIAL technique presents many challenging and often subtle technical difficulties that can limit its useful range and accuracy. One potentially serious source of error for many DIAL experiments is nonlinearity in the analog-to-digital converters used to capture lidar return signals. The impact of digitizer nonlinearity on DIAL measurements is examined, and a simple and inexpensive low-frequency dithering technique that significantly reduces the effects of ADC nonlinearity in DIAL and other applications in which the signal is repetitively averaged is described.
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The differential absorption lidar (DIAL) technique for deriving O3 profiles from lidar measurements is discussed. The US National Aeronautics and Space Administration's airborne DIAL system is described, and examples of a broad range of O3 and aerosol measurements are presented from a number of field experiments. The airborne and ground-based DIAL measurements discussed demonstrate the outstanding capability of lidar for conducting O3 investigations throughout the troposphere and lower stratosphere under widely different atmospheric conditions.