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UV polarization lidar for remote sensing new particles formation in the atmosphere

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Abstract

Understanding new particles formation in the free troposphere is key for air quality and climate change, but requires accurate observation tools. Here, we discuss on the optical requirements ensuring a backscattering device, such as a lidar, to remotely observe nucleation events promoted by nonspherical desert dust or volcanic ash particles. By applying the Mie theory and the T-matrix code, we numerically simulated the backscattering coefficient of spherical freshly nucleated particles and nonspherical particles. We hence showed that, to remotely observe such nucleation events with an elastic lidar device, it should operate in the UV spectral range and be polarization-resolved. Two atmospheric case studies are proposed, on nucleation events promoted by desert dust, or volcanic ash particles. This optical pathway might be useful for climate, geophysical and fundamental purposes, by providing a range-resolved remote observation of nucleation events.

© 2014 Optical Society of America

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Figures (6)

Fig. 1
Fig. 1 Panel (a): Observation of the size and time evolution of the particles number concentration during a typical dust-NPF event, taken from a field campaign [18] on 2009 March 13th. Local time is used (UTC + 8h, Asian field campaign). The observed behavior between 9:00 and 12:00, then 18:00 to 19:00, is a clear signature of a NPF-event, while in the meantime, coarser dust particles, for diameters above 800 nm, are in low number concentrations. Panel (b): Numerical simulation of the backscattering coefficient βNPF obtained by applying the Mie theory at λ = 355 nm (blue), 532 nm (green), 1064 nm (red). The dust particles backscattering coefficient βdust, derived from T-matrix numerical simulation, is plotted at λ = 355 nm in light blue.
Fig. 2
Fig. 2 (a) Size and wavelength dependence of the NPF-backscattering integrand (dσ/dΩ)NPF × nNPF during the NPF-event (at t = 10h45), as implied by Eq. (1). (b) Spectral dependence of the backscattering coefficient βNPF obtained by integrating graph (a) over the particles size distribution for spherical particles (diameters below 800 nm).
Fig. 3
Fig. 3 Spectral dependence of molecular backscattering cross-section at λ = 355 nm numerically simulated for a standard atmosphere, for co-(black) and cross- (grey) polarized polarization components. Ro-vibrational molecular spectra appears spectrally smoothed due to the finite spectral linewidth of the laser emission (1 GHz), whose Doppler broadening is also included.
Fig. 4
Fig. 4 Time-altitude maps of the lidar-retrieved backscattering coefficients {βp,//, βp,⊥}-coefficients, then {βs, βns}-backscattering coefficients measured at Lyon at λ = 355 nm in July 2010 during a Saharan dust outbreak. To put light on the achieved sensitivity, a different color code has been used for each map.
Fig. 5
Fig. 5 Spherical (grey) and nonspherical (brown, dust) particles backscattering coefficient βs and βns as a function of altitude during a Saharan dust outbreak (Lyon, July 2010, 5h), together with the corresponding βp,// and βp,⊥-profiles. To ease the reading, the graph is limited to altitudes above the PBL where the dust cloud is present.
Fig. 6
Fig. 6 Spherical (grey) and nonspherical (brown, ash) particles backscattering coefficient βs and βns as a function of altitude during a volcanic ash episode (Lyon, April 17th 2010, 12h), together with the corresponding βp,// and βp,⊥-profiles. To ease the reading, the graph is limited to altitudes above the PBL.

Equations (4)

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β p ( λ ) = 0 D p , max ( d σ d Ω ) p ( D p , λ ) × n p ( D p ) d D p
β s = β s,// = β p,// β ns,// = β p,// β p, / δ ns
β ns = β ns,// + β ns, = β p, (1+1/ δ ns )
β p,// =( R // 1) β m, // and β p, =( R // δ δ m ) β m,//
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