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The three most common lidar transmitter-receiver configurations are illustrated, along with the basic transmitter components. The components are described sequentially, starting with the laser, with a table of the most important laser characteristics for lidar systems. Lidar beam expanders are described. Lasers are then discussed in terms of their basic requirements (an active medium, a population inversion, and optical feedback), and the properties of laser light (monochromaticity, directionality, and often polarization). Beam parameters and beam quality are then described starting with the Gaussian beam model. Measures of laser beam quality include the beam propagation ratio, spectral purity, and polarization purity. Methods for changing the wavelength are discussed, including stimulated Raman scattering, harmonic generators, and optical parametric oscillators. Laser safety, eye safety standards in terms of maximum permissible exposure, and laser classes are then covered, and the transmitter of an eye safe elastic backscatter lidar is described as an example, with an illustration and a table of its parameters.
We demonstrated a high-power long-wave infrared laser based on a polarization beam coupling technique. An average output power at $8.3~\unicode[STIX]{x03BC}\text{m}$ of 7.0 W was achieved at a maximum available pump power of 107.6 W, corresponding to an optical-to-optical conversion of 6.5%. The coupling efficiency of the polarization coupling system was calculated to be approximately 97.2%. With idler single resonance operation, a good beam quality factor of ${\sim}1.8$ combined with an output wavelength of $8.3~\unicode[STIX]{x03BC}\text{m}$ was obtained at the maximum output power.
We report on a new scheme for efficient continuous-wave (CW) mid-infrared generation using difference frequency generation (DFG) inside a periodically poled lithium niobate (PPLN)-based optical parametric oscillator (OPO). The pump sources were two CW fiber lasers fixed at 1018 nm and 1080 nm. One worked as the assisted laser to build parametric oscillation and generate an oscillating signal beam while the other worked at low power (${\leqslant}3~\text{W}$) to induce DFG between it and the signal beam. The PPLN temperature was appropriately adjusted to enable OPO and DFG to synchronously meet phase-matching conditions. Finally, both low-power 1018 nm and 1080 nm pump beams were successfully converted to $3.1~\unicode[STIX]{x03BC}\text{m}$ and $3.7~\unicode[STIX]{x03BC}\text{m}$ idler beams, respectively. The conversion efficiencies of the 1018 nm and 1080 nm pumped DFG reached 20% and 15%, respectively, while their slope efficiencies reached 19.6% and 15%. All these data were comparable to the OPOs pumped by themselves and never realized before in traditional CW DFG schemes. The results reveal that high-efficiency frequency down-conversion can be achieved with a low-power near-infrared pump source.
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