The spatial and temporal distribution of Arctic aerosols as seen from the CALIPSO satellite (2006 – 2012) AGU Fall Meeting Maurizio Di Pierro and Lyatt Jaeglé Dec 3-7 2012 A13K-0331 University of Washington, Department of Atmospheric Sciences, Seattle (dipierro@uw.edu) 1. Introduction • The Arctic is a known receptor of pollution emitted in the mid-latitudes. Anthropogenic aerosols alter the radiative balance of the Arctic via both the aerosol direct and indirect effect. Climate simulations indicate that sulfur emission reductions in the northern mid-latitudes can explain a substantial fraction of the rapid Arctic warming observed during the past 3 decades (Shindell and Faluvegi, 2009). • Long-term observations in the Arctic, however, have historically relied on a sparse network of ground stations, with limited ability to observe the middle-upper troposphere. • We present results on the distribution of Arctic aerosols retrieved by the Cloud and Aerosol Lidar with Orthogonal Polarization (CALIOP) on board the CALIPSO satellite, from 2006 to 2012. We explore the spatial and vertical distributions of Arctic aerosols, their seasonality and inter-annual variability. CALIPSO orbits the Earth at 98 inclination, thus has excellent observation density over the Arctic The CALIOP instrument measures vertical profiles of attenuated backscatter at 532 nm (polarized channel) and 1064 nm. We use Level 2 Aerosol and Cloud layer data, version 3.01, from June 2006 to May 2012, 59º-82º N. From this data we extract the Aerosol Optical Thickness (AOT) of each aerosol layer identified. Clear sky profiles and profiles above the first cloud top are considered Low quality data and unphysical retrievals are discarded. Aerosol contamination by diamond dust is removed by imposing an extinction cut-off threshold of 350 Mm-1 The aerosol layers are finally gridded at 2º latitude by 2.5º longitude at 0.2 km vertical resolution 3. Combine day and night retrievals • • In order to reconstruct the seasonal cycle of Arctic aerosol extinction it is necessary to deal with the seasonal cycle of daylight which greatly affects CALIOP’s performance, particularly for optically thin aerosols. CALIOPs’ higher backscatter detection sensitivity threshold at daytime results in fewer aerosol layers detected at daytime than at nighttime The ratio of daytime to nighttime detection frequency is found to scale linearly with the value of the backscatter of the detected aerosol layers Figure caption: Left: CALIOP detection frequency in DecemberMarch, 2006-2012, 61-71ºN. Right: number distribution points in the β/𝑓𝑓𝑛𝑑 plane, for September-March 20062012 (when the number of daytime and nighttime retrievals is identical). ASIA 1. Observations from NASA ARCTAS campaign (April 2008) Nephelometer extinction = 2-5 km Extinction NAM 5-8 km Extinction EUR ATL CALIOP NighttimeEquivalent Low Arctic (60º-70ºN) Neph. with CALIOP th. Haze layers over the Brooks Range (Alaska), April 2008. Courtesy of NASA Over Alaska, only 25% of the data points are above CALIOP sensitivity threshold CALIOP nighttime-equivalent extinction captures both the near-surface and the 3-6 km extinction peak, with a 30% underestimate of the column AOD 2. Monthly-mean ambient extinction at two Arctic sites: Barrow Barrow Alert Alert CALIOP sensitivity threshold is applied after the extinction is corrected for ambient RH CALIOP captures the seasonal cycle at both sites, with a bias <15% High Arctic (70º-82ºN) Strong seasonal cycle in the high Arctic The springtime free tropospheric consistent with Arctic Haze literature maximum in March-April in the High studies Arctic, and in May in the Low Arctic Two annual maxima in the low Arctic May peak in the upper troposphere consistent with volume concentration matches previous observations surface measurements at Zotino (89ºE, (Treffeisen et al., 2006) 62ºN). (Heintzenberg et al., 2011). Atlantic Sector (60ºW-10ºE) Asian Sector (110ºE-140ºW) European Sector (10º-110ºE) North American Sector (60º-140ºW) All Sectors 7. Inter-annual variability Intense agricultural fires in Russia/Kazakhstan Kasatochi (Aleutian Islands) volcanic eruption Sarychev Eruption 5. Aerosol spatial distributions Low-level pollution inflow around the Siberian anticyclone The wind speed seasonal maximum causes sea salt aerosol over the North Atlantic to peak in winter Strong gradient in extinction from 60-70N due to efficient wet scavenging by drizzle and polar front retreat (Stohl, 2006; Garrett et al., 2011) Increased transport from midlatitudes causes the mid-and upper tropospheric maximum in spring Biomass burning summer maximum Boreal forest fires This relationship is used to correct the daytime detection frequency to form the nighttime-equivalent mean extinction via the correction factor S: 𝑊𝑑 𝑓𝑑 𝑏𝑑 𝑆 𝛽 + 𝑊𝑛 𝑓𝑛 𝑏𝑛 𝑊𝑑 +𝑊𝑛 0-2 km Extinction CALIOP 2. CALIPSO Satellite Observations • 6. Multi-year seasonal cycle by sector 4. Method Validation Figure caption: 5-day averaged aerosol extinction from June 2006 to May 2012. 8. Summary “Surface Arctic Haze” CALIOP captures the seasonal cycle of aerosols extinction as measured in-situ at the stations of Barrow and Alert, as well as the vertical profile of extinction measured during the ARCTAS aircraft campaign of April 2008. Arctic Haze is a Pan-Arctic phenomenon. Central Asia is the preferred point of entry of pollution in winter. In the middle and upper troposphere, extinction maximizes in spring, when the frequency of cyclonic activity and blocking anticyclones reaches an annual maximum. Extinction is highest in the Asian sector. Low and High Arctic are strongly decoupled in summer, due to the poleward retreat of the Polar Front as well as efficient wet scavenging by stratocumulus drizzle. Inter-annual variability is relatively small at the surface. In the free troposphere, biomass burning anomalies and volcanic eruptions drive the variability during the period considered. Acknowledgments: We thank Sangeeta Sharma and Richard Leaitch from Climate Research Division, Environment Canada, Ed Eloranta for the HSRL data, as well as NOAA for providing the Barrow data and Luke Ziemba for the ARCTAS data. This work was supported by funding from the NASA Earth and Space Science Fellowship under award NNX11AL69H and by NASA award NNX08AQ07G. References: extinction = Nighttime-Equivalent aerosol mean extinction W = number of observations ; f = detection frequency (0-1) b = mean extinction of the detected aerosols β = mean backscatter of the detected aerosols S = correction factor ; Subscripts d,n : Day, Night Figure caption: Spatial distribution of aerosol mean extinction from 2006 to 2012 by season and altitude Garrett, T. J., Brattström, S., Sharma, S., Worthy, D. E. J., and Novelli, P.: The role of scavenging in the seasonal transport of black carbon and sulfate to the Arctic, Geophys. Res. Lett., 38, L16805, doi:10.1029/2011GL048221, 2011. Heintzenberg, J., Birmili, W., Otto, R., Andreae, M. O., Mayer, J.-C., Chi, X., and Panov, A.: Aerosol particle number size distributions and particulate light absorption at the ZOTTO tall tower (Siberia), 2006– 2009, Atmos. Chem. Phys., 11, 8703-8719, doi:10.5194/acp-11-8703-2011, 2011. Shindell, D., and Faluvegi, G., Climate response to regional radiative forcing during the twentieth century, Nature Geoscience 2, 294 - 300 (2009) , doi:10.1038/ngeo473 Stohl, A.: Characteristics of atmospheric transport into the Arctic troposphere, J. Geophys. Res., 111, D11306, doi:10.1029/2005JD006888, 2006. Treffeisen, R. E., Thomason, L. W. , Ström, J., Herber, A. B., Burton, S. P., and Yamanouchi, T.: Stratospheric Aerosol and Gas Experiment (SAGE) II and III aerosol extinction measurements in the Arctic middle and upper troposphere, J. Geophys. Res., 111, D17203, doi:10.1029/2005JD006271, 2006.