Sodium Fluorescence Doppler Lidar to Measure Atmospheric Temperature in the Mesopause Region

Sodium Fluorescence Doppler Lidar to Measure Atmospheric Temperature in the Mesopause Region

View metadata, citation and similar papers at core.ac.uk brought to you by CORE provided by Springer - Publisher Connector Article Atmospheric Science February 2011 Vol.56 No.4-5: 417–423 doi: 10.1007/s11434-010-4306-x SPECIAL TOPICS: Sodium fluorescence Doppler lidar to measure atmospheric temperature in the mesopause region HU Xiong1, YAN ZhaoAi1,2*, GUO ShangYong1, CHENG YongQiang1 & GONG JianCun1 1 Center for Space Science and Applied Research, Chinese Academy of Sciences, Beijing 100190, China; 2 Graduate University of Chinese Academy of Sciences, Beijing 100049, China Received August 19, 2010; accepted November 9, 2010 A sodium fluorescence Doppler lidar system has been developed to measure environmental parameters of the middle and upper atmosphere. The lidar system mainly comprises a transmitter system, receiver system, data acquisition and control system and data analysis system. A narrowband 589 nm laser is used to excite sodium atoms in the mesopause region. Excitation of the so- dium atoms results in resonance fluorescence, which is collected by the receiver. The temperatures in the mesopause region (about 75–105 km) can be derived by analyzing the Doppler-broadened width of the sodium fluorescence. Observations were made with the lidar system, and the number density of sodium atoms and atmospheric temperature profiles were extracted from the observa- tion data. Comparisons of the lidar temperatures and TIMED/SABER temperatures show good agreement, illustrating the reliabil- ity of the sodium fluorescence Doppler lidar measurements. Doppler lidar, sodium resonance fluorescence, mesospause temperature Citation: Hu X, Yan Z A, Guo S Y, et al. Sodium fluorescence Doppler lidar to measure atmospheric temperature in the mesopause region. Chinese Sci Bull, 2011, 56: 417−423, doi: 10.1007/s11434-010-4306-x The mesopause region is an area of strong coupling between Sodium fluorescence lidar, potassium fluorescence lidar, the lower and upper atmosphere. Its temperature structure iron Boltzmann lidar and calcium fluorescence lidar employ greatly affects atmospheric stability, energy transfer, at- sodium, potassium, iron and calcium fluorescence respec- mospheric chemical processes and dynamical behaviors. tively in the mesopause region for sounding of the middle The mesopause region is the coldest on Earth. Noctilucent and upper atmosphere [7,11]. In 1969, Bowman et al. [12] clouds have been recently found to spread from polar to completed the first lidar observation of mesospheric sodium mid-latitude and high-latitude regions, possibly owing to atoms using a tunable laser. The first observation of the mesospheric cooling in response to global climate change. sodium hyperfine structure in the middle and upper atmos- To explore this possibility, it is important to measure the phere was reported by Gibson et al. [13] in 1979, establish- temperature structure of the mesopause. ing the possibility of mesopause temperature measurements There are several kinds of lidar for measuring atmos- with narrowband resonance fluorescence lidar. The first so- pheric temperature, such as Rayleigh scattering lidar [1–3], dium fluorescence Doppler lidar system for temperature Raman scattering lidar [4,5], resonance fluorescence Dop- measurements was operated routinely at Andoya, Norway in pler lidar [6,7], high spectral resolution lidar [8,9] and dif- 1985 [14]. A more advanced narrowband sodium fluores- ferential absorption lidar [10]. Sodium fluorescence Dop- cence lidar system using a two-frequency technique was de- pler lidar is mainly used to measure the atmospheric tem- veloped through collaboration between Colorado State Uni- perature and wind in the mesopause region. versity [15] and University of Illinois at Urbana and Cham- paign [16] in 1990, achieving higher accuracy. Thereafter, *Corresponding author (email: [email protected]) Colorado State University developed a three-frequency so- © The Author(s) 2011. This article is published with open access at Springerlink.com csb.scichina.com www.springer.com/scp 418 Hu X, et al. Chinese Sci Bull February (2011) Vol.56 No.4-5 dium fluorescence Doppler lidar system employing the laser A simple description is given below. stabilization technique and the frequency modulation tech- The sodium D2 line is used in sodium fluorescence nique to simultaneously measure wind and temperature Doppler lidar. Figure 1 is an energy-level diagram of so- 2 [7,18]. In 2002, the Colorado State University sodium fluo- dium D transitions. The D2 line is the transition from 3 p3/2 2 rescence Doppler lidar system was upgraded to a two-beam to 3 s1/2, and the corresponding wavelength is 589.158 nm system to realize simultaneous atmospheric temperature and in a vacuum. In the case of the D2 line hyperfine structure, 2 wind measurements [19]. In 2006, this lidar system was the excited state 3 p3/2 splits into four levels. upgraded to a three-beam system to provide measurements In the mesopause region, the Doppler-broadened width of the atmospheric momentum flux as well as the atmos- for the sodium atom is proportional to the square root of the pheric temperature and wind [20]. absolute temperature and inversely proportional to the In China, Wuhan Institute of Physics and Mathematics, square root of the atomic mass. It can be expressed as Chinese Academy of Sciences, developed a Rayleigh/so- dium fluorescence lidar system in 1996 [21]. At present, kT σ = B , (1) Wuhan University, University of Science and Technology D 2 Mλ0 of China, China Research Institute of Radio Wave Propaga- tion, and Center for Space Science and Applied Research where kB is the Boltzmann constant, T is temperature, M is (CSSAR), Chinese Academy of Sciences, are observing the the mass of the atom and λ0 is the central wavelength. middle and upper atmosphere with sodium fluorescence The sodium Doppler-broadened lineshape is [6,7] lidar systems at Wuhan [22], Hefei [23], Qingdao, Beijing ⎛⎞2 and Hainan. However, these lidar systems do not employ ⎡⎤⎛⎞vR ⎜⎟⎢⎥ννn −−⎜⎟1 Doppler techniques and can only measure the density pro- 1 6 ⎜⎟⎝⎠c gA()ν =− exp⎣⎦ , (2) files of sodium atoms and not the temperature or wind. ∑ n ⎜⎟2 2πσ n=1 2σ D ⎜⎟D Wuhan University developed an iron Boltzmann lidar sys- ⎜⎟ tem to measure the mesopause temperature in 2006 [24]. ⎝⎠ To measure the mesopause temperature and wind simul- where σ is the root-mean-square width of the Doppler- taneously, CSSAR has investigated the principle of the so- D broadened line, v and A are the central frequencies and the dium fluorescence Doppler lidar and the method for re- n n line strengths of six electric-dipole-allowed D transitions, v trieving atmospheric parameters, simulated the lidar back- 2 is frequency, v is the radial velocity of the sodium atom scattering photon signal [25,26], and measured the saturated R fluorescence spectrum of sodium atoms [27]. CSSAR has moving away from the laser source and c is the speed of developed a technique for stabilizing the laser frequency light. The main parameters of the D2 line hyperfine structure employing the saturated fluorescence spectrum, and in turn, are listed in Table 1. a narrowband, three-frequency sodium fluorescence Dop- Sodium resonance fluorescence is induced by the laser. pler lidar system. This is the first sodium fluorescence Dop- The lineshape of the resonance fluorescence spectrum is a pler lidar system in China. Observations of the middle and convolution of the atom Doppler-broadened lineshape and upper atmosphere have been made with this lidar in Beijing. laser lineshape gL(v), which can be expressed as The lidar measurement principle and components, and the Ggg()ν =− (νν′′′ ) ( ν )d. ν (3) observed temperature results and their comparisons with ∫ L TIMED/SABER temperature results, are introduced in this paper. 1 Measurement principle of sodium fluores- cence Doppler lidar A metal layer containing sodium atoms exists at about 75–105 km altitude. The sodium atom layer as a tracer has the same temperature as the background atmospheric tem- perature. In the mesopause region, the Doppler-broadened width of the sodium fluorescence is a function of tempera- ture. A 589 nm laser excites the sodium atoms so that there is resonance fluorescence. The temperature can be obtained by measuring the Doppler broadening of the fluorescence. The use of sodium fluorescence Doppler lidar to measure wind and temperature is detailed in the literature [7,17,26]. Figure 1 Energy levels of sodium D transitions. Hu X, et al. Chinese Sci Bull February (2011) Vol.56 No.4-5 419 Usually, the laser lineshape gL (v) is Gaussian with a width The relation between the ratio RT and the atmospheric σL, which is measured as about 140 MHz for the present temperature T is presented in Figure 3. Therefore, by meas- lidar system. uring the ratio RT, the temperature can be estimated from From eqs. (2) and (3), it is clear that the atmospheric Figure 3. temperature determines the linewidth of the sodium fluo- The principle and equations of radial wind speed meas- rescence spectrum, and that the radial wind speed deter- urement using the three-frequency ratio technique are de- mines the Doppler shift. Figure 2 shows sodium fluores- tailed in the literature and are thus not presented here. cence spectrum lineshapes for different temperatures when the radial wind speed is zero. Two independent ratios of echo signals can be obtained 2 Sodium fluorescence Doppler lidar when transmitting three-frequency narrowband laser pulses. The linewidth and Doppler shift can be measured simulta- The CSSAR sodium fluorescence Doppler lidar system neously using these two ratios, from which the atmospheric mainly consists of a transmitter system, receiver system, temperature and radial wind speed can be retrieved simul- data acquisition and control system and data analysis sys- taneously. This technique is referred to as the three-fre- tem. Figure 4 is a schematic diagram of the lidar system. quency-ratio Doppler technique [7,17,26].

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