Abstract

Abstract. We investigate the accuracy and precision of polar lower stratospheric temperatures (100–10 hPa during 2008–2013) reported in several contemporary reanalysis datasets comprising two versions of the Modern-Era Retrospective analysis for Research and Applications (MERRA and MERRA-2), the Japanese 55-year Reanalysis (JRA-55), the European Centre for Medium-Range Weather Forecasts (ECMWF) interim reanalysis (ERA-I), and the National Oceanic and Atmospheric Administration (NOAA) National Centers for Environmental Prediction (NCEP) Climate Forecast System Reanalysis (NCEP-CFSR). We also include the Goddard Earth Observing System model version 5.9.1 near-real-time analysis (GEOS-5.9.1). Comparisons of these datasets are made with respect to retrieved temperatures from the Aura Microwave Limb Sounder (MLS), Constellation Observing System for Meteorology, Ionosphere and Climate (COSMIC) Global Positioning System (GPS) radio occultation (RO) temperatures, and independent absolute temperature references defined by the equilibrium thermodynamics of supercooled ternary solutions (STSs) and ice clouds. Cloud-Aerosol Lidar with Orthogonal Polarization (CALIOP) observations of polar stratospheric clouds are used to determine the cloud particle types within the Aura MLS geometric field of view. The thermodynamic calculations for STS and the ice frost point use the colocated MLS gas-phase measurements of HNO3 and H2O. The estimated bias and precision for the STS temperature reference, over the 68 to 21 hPa pressure range, are 0.6–1.5 and 0.3–0.6 K, respectively; for the ice temperature reference, they are 0.4 and 0.3 K, respectively. These uncertainties are smaller than those estimated for the retrieved MLS temperatures and also comparable to GPS RO uncertainties (bias < 0.2 K, precision > 0.7 K) in the same pressure range. We examine a case study of the time-varying temperature structure associated with layered ice clouds formed by orographic gravity waves forced by flow over the Palmer Peninsula and compare how the wave amplitudes are reproduced by each reanalysis dataset. We find that the spatial and temporal distribution of temperatures below the ice frost point, and hence the potential to form ice polar stratospheric clouds (PSCs) in model studies driven by the reanalyses, varies significantly because of the underlying differences in the representation of mountain wave activity. High-accuracy COSMIC temperatures are used as a common reference to intercompare the reanalysis temperatures. Over the 68–21 hPa pressure range, the biases of the reanalyses with respect to COSMIC temperatures for both polar regions fall within the narrow range of −0.6 K to +0.5 K. GEOS-5.9.1, MERRA, MERRA-2, and JRA-55 have predominantly cold biases, whereas ERA-I has a predominantly warm bias. NCEP-CFSR has a warm bias in the Arctic but becomes substantially colder in the Antarctic. Reanalysis temperatures are also compared with the PSC reference temperatures. Over the 68–21 hPa pressure range, the reanalysis temperature biases are in the range −1.6 to −0.3 K with standard deviations ∼ 0.6 K for the CALIOP STS reference, and in the range −0.9 to +0.1 K with standard deviations ∼ 0.7 K for the CALIOP ice reference. Comparisons of MLS temperatures with the PSC reference temperatures reveal vertical oscillations in the MLS temperatures and a significant low bias in MLS temperatures of up to 3 K.

Highlights

  • Over the last couple of decades, global reanalysis datasets have become one of the workhorse tools of the climate research community for understanding atmospheric processes and variability (Fujiwara et al, 2017) and more recently for potentially investigating climate changes (Thorne and Vose, 2010; Dee et al, 2014; Simmons et al, 2014)

  • In order to provide context for the later results that use more complex analysis techniques, we first provide a basic overview of the reanalysis temperatures in the polar lower stratosphere, and we choose as a suitable metric the daily (12:00 UT) mean 60◦ polar cap temperature differences at 46 hPa for the 2008–2013 time frame

  • We have evaluated the accuracy and precision of several contemporary reanalysis datasets compared to (a) the COSMIC Global Positioning System (GPS) radio occultation (RO) temperatures and (b) the absolute temperature references obtained from the equilibrium properties of certain types of polar stratospheric clouds (PSCs)

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Summary

Introduction

Over the last couple of decades, global reanalysis datasets have become one of the workhorse tools of the climate research community for understanding atmospheric processes and variability (Fujiwara et al, 2017) and more recently for potentially investigating climate changes (Thorne and Vose, 2010; Dee et al, 2014; Simmons et al, 2014). Several previous intercomparisons of analyses and reanalyses generated by various national centers have been carried out (e.g., Manney et al, 1996, 2003, 2005; Pawson et al, 1999) to assess their accuracy and ultimate suitability for stratospheric polar studies Independent datasets such as radiosondes, satellite observations, Global Positioning System (GPS) RO (Nedoluha et al, 2007), and temperature sensors on long-duration balloons (Hertzog et al, 2004; McDonald and Hertzog, 2008) have been used to assess reanalysis temperatures. Lawrence et al (2015) examined a 34-year record of polar processing diagnostics for MERRA and ERA-I reanalyses They documented the introduction of new data streams and noted better agreement in the post-2001 time frame following the assimilation of Aqua Atmospheric Infrared Sounder (AIRS) and Geostationary Operational Environmental Satellite (GOES) radiances into both schemes.

Datasets and methodology
Reanalysis temperature data
CALIOP PSC data
MLS gas-phase constituents and temperature
CALIPSO and Aura configuration within the A-Train
COSMIC GPS RO temperatures
Thermodynamics of PSC formation
Ice cloud equilibrium
Results
Temperature fluctuations
Orographic gravity wave case study
Reanalysis temperatures compared to COSMIC GPS RO
PSC types from CALIOP and their representation in MLS observations
Reanalysis temperatures compared to LIQ and ICE reference points
Conclusions
Full Text
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