The Impact of Solar Spectral Irradiance Variability on Middle Atmospheric Ozone Jerald Harder1, Aimee Merkel1, Dan Marsh2, Anne Smith2, Juan Fontenla1, and Tom Woods1 Laboratory for Atmospheric and Space Physics (LASP), University of Colorado Special thanks to: Mark Rast & Martin Snow, LASP SORCE Meeting, Sedona Arizona The Impact of Solar Spectral Irradiance Variability on Middle Atmospheric Ozone September 12, 2011 Harder- 1 Overview • Observations of SSI with SIM – Status of SIM observations – Degradation corrections – Irradiance trends • Solar variability as seen in Precision Solar Photometric Telescope (PSPT) the Solar Radiation Physical Model (SRPM) • Modeling study using NCAR’s WACCM (Whole Atmosphere Community Climate Model). – Response of middle atmospheric ozone when forced by solar spectral irradiance (SSI). – Compare and contrast to model results when forced with solar proxy Naval Research Laboratory SSI model (NRLSSI = Lean (2000) model) SORCE (Solar Radiation and Climate Experiment) SSI observations from SIM and SOLSTICE. • Is the predicted ozone signal from the WACCM simulations present in observations? Are they consistent with the findings from the UARS era? SORCE Meeting, Sedona Arizona The Impact of Solar Spectral Irradiance Variability on Middle Atmospheric Ozone September 12, 2011 Harder- 2 Status of SIM after October 2010 • 4 different safe-hold events since September 26, 2010 caused observatory temperatures to drop below -15oC producing small be noticeable changes in the responsivity of SIM. – Detection of these On-board Computer (OBC) anomalies has been corrected in flight software • Because of decreased battery capacity, power cycling on every orbit started on 2011/05/04 – Power cycling has no instrument safety issues – Detectors have 3-5 degree temperature swings • Effects detector radiant sensitivity especially in the 900-1000 nm region • There are temperature drifts longer that a single orbit – ESR requires ~30 minutes to achieve full control on each orbit – Prism temperature drifts continuously (~1.5°C) • Drift may not affect data processing, i.e. may not need an explicit wavelength shifting algorithm • ~1 year of data may be needed to detect second order effects • These events have disrupted cadence of SIM A SIM B comparisons SORCE Meeting, Sedona Arizona The Impact of Solar Spectral Irradiance Variability on Middle Atmospheric Ozone September 12, 2011 Harder- 3 SIM degradation correction and long-term uncertainty • Degradation Corrections: – Exposure related (prism transmission) • Correct by comparing two spectrometers at different exposure rates – Non-exposure related (photodiode degradation) • Correct by comparing ESR’s and photodiode detectors • Physically based correction: – No assumptions are made about magnitude, slope, or time dependent behavior of SSI – Prism degradation obeys Lambert’s Law • See Auxiliary material to Harder et al., GRL, (2009) for details SORCE Meeting, Sedona Arizona The Impact of Solar Spectral Irradiance Variability on Middle Atmospheric Ozone September 12, 2011 Harder- 4 SIM degradation correction and long-term uncertainty SORCE Meeting, Sedona Arizona The Impact of Solar Spectral Irradiance Variability on Middle Atmospheric Ozone September 12, 2011 Harder- 5 Time series of solar spectral variability from SORCE SORCE Meeting, Sedona Arizona The Impact of Solar Spectral Irradiance Variability on Middle Atmospheric Ozone September 12, 2011 Harder- 6 Mauna Loa PSPT • • SORCE Meeting, Sedona Arizona Clear indication of the rise of SC24 both in sunspot area and bright active regions – Disk fractions for active regions and network are approaching 2004-2005 values ~160 days separate the minimum in the longitudinal B-field from the minimum active region area in PSPT The Impact of Solar Spectral Irradiance Variability on Middle Atmospheric Ozone September 12, 2011 Harder- 7 PSPT observations of faculae •Some faculae and plage have negative contrast at red continuum wavelengths • The fraction of dark faculae decreases into SC23 minimum and increases into rising phase of SC24 SORCE Meeting, Sedona Arizona The Impact of Solar Spectral Irradiance Variability on Middle Atmospheric Ozone September 12, 2011 Harder- 8 Solar spectral irradiance variability in SRPM Fontenla, J. M. M., et al. (2011), High-resolution solar spectral irradiance from extreme ultraviolet to far infrared,J. Geophys. Res., doi:10.1029/2011JD016032, in press. SORCE Meeting, Sedona Arizona The Impact of Solar Spectral Irradiance Variability on Middle Atmospheric Ozone September 12, 2011 Harder- 9 Solar spectral irradiance variability in NRL SSI Sunspot Case: 04/30/2005 FaculaPlage: 08/29/2005 Solar Min Ref: 11/09/2007 J. Lean, GRL., vol. 27, pp 2425, 2000. SORCE Meeting, Sedona Arizona The Impact of Solar Spectral Irradiance Variability on Middle Atmospheric Ozone September 12, 2011 Harder- 10 Solar forcing and Earth atmospheric response Solar forcing and response mechanisms are wavelength dependent Chemistry climate models require SSI to determine the role of solar forcing Ultraviolet (UV) radiation drives many atmospheric processes Solar input to models • Historically solar input spectra scaled by long-term proxies such as sunspot index,F10.7 or Mg II index. • Now GCM use NRLSSISSI reconstructions based on combined sunspot and facular proxy indicators [Lean, 2000]. • NRLSSI employed as solar input for climate model inter-comparison studies, so represents the de facto standard for comparison. [SPARC CCMVAL, Eyring et al., 2010] Altitude contour for attenuation by a factor of 1/e SORCE Meeting, Sedona Arizona The Impact of Solar Spectral Irradiance Variability on Middle Atmospheric Ozone September 12, 2011 Harder- 11 Haigh et al. 2010 ozone study: model comparisons with MLS Haigh et al., Nature, 2010 • Results from 2-d modeling in accord with ozone observations from AURA-MLS • 0.68-0.32 hPa ozone change of -1.7% (2004-2007) • 10.0- 6.8 hPa ozone change of +4.5% • Cross over from negative to positive at ~45 km • Merkel et al. 2011 extends this study with the following enhancements: • • • Utilizes a 3‐d GCM (WACCM) with chemistry rather than a static 2‐d stratospheric model Uses 9 years (2002-2011) of TIMED SABER ozone data to covers the full descending phase of SC23 with independent instrumental observation Segregates by day and night to isolate photochemical effects. SORCE Meeting, Sedona Arizona The Impact of Solar Spectral Irradiance Variability on Middle Atmospheric Ozone September 12, 2011 Harder- 12 Trends of Annual TIMED-SABER Ozone Lower Mesosphere Out-of-phase with solar cycle Trend in day, absent at night O3 loss due to HOx cycles and O2 photolysis ceases at night SORCE Meeting, Sedona Arizona Stratosphere In-phase with solar cycle Trend similar for day and night Less driven by photochemistry Very little diurnal variation The Impact of Solar Spectral Irradiance Variability on Middle Atmospheric Ozone September 12, 2011 Harder- 13 SABER Compared to WACCM Simulations for Upper Atmospheric Ozone NRLSSI SABER SORCE O3 Difference (%) Active 2004-Quiet 2007 O3 Difference (%) (2002/3) - (2008/9) O3 Difference (%) Active 2004-Quiet 2007 O3 Difference (%) Avg. 15ºN-15ºS Latitude • • • • Panel on right shows equatorial response of all three The comparisons imply that the higher SORCE UV variability improves the model/data agreement of daytime mesospheric ozone. Suggests enhanced HOx photochemistry with greater SORCE solar variability Regression of SABER data commensurate with MLS regression in Haigh et al., 2010: • Mesosphere: 0.3-0.03 hPa ⇒ 2.8% 1.4% • Stratosphere: 5.0-1.2 hPa ⇒ 2.6% 0.63% SORCE Meeting, Sedona Arizona The Impact of Solar Spectral Irradiance Variability on Middle Atmospheric Ozone September 12, 2011 Harder- 14 SABER compared to HALOE & SBUV SBUV HALOE Halogen Occultation Experiment (Remsberg et al., 2008) SABER Solar Backscatter Ultraviolet (Soukharev and Hood, 2006) Near 0% at 50km 1991-2005 O3 % (Max-min) Figure 9 ➨SABER stratospheric ozone congruent with previous observations. ➨SABER able to resolve lower mesospheric ozone response to solar forcing. SORCE Meeting, Sedona Arizona The Impact of Solar Spectral Irradiance Variability on Middle Atmospheric Ozone September 12, 2011 Harder- 15 Conclusions • The combined SIM, SRPM, and PSPT image analysis provide a effective method to analyze solar variability – SIM indicates irradiance trends that are larger than solar modulation that compensate to produce the TSI trend. – SRPM analysis is able to capture offsetting trends observed by SIM, but refinements are still needed. – Active region evolution by itself is not sufficient to account for the observations – suggestive of changes in the internetwork/network radiance. • In-depth Earth atmospheric modeling is progressing – Solar forcing in WACCM from SORCE spectra produces a very different response in O3 from semi-empirical models of SSI: a reduction in mesospheric ozone at higher solar activity and a increase in mid- to upper stratosphere. – We don’t know if our results are specific to this minimum because we only have SSI and ozone measurements for the descending phase of SC23. Continued observations are needed. SORCE Meeting, Sedona Arizona The Impact of Solar Spectral Irradiance Variability on Middle Atmospheric Ozone September 12, 2011 Harder- 16 Extras SORCE Meeting, Sedona Arizona The Impact of Solar Spectral Irradiance Variability on Middle Atmospheric Ozone September 12, 2011 Harder- 17 Fundamental Equations For a single wavelength, λ. At two separate times 0 and 1. ln( I A0 ) = ln( E0 ) − τ A0 , ln( I A0 ) = ln( E0 ) − τ A0 ln( I B 0 ) = ln( E0 ) − τ B 0 , ln( I B 0 ) = ln( E0 ) − τ B 0 I A1 E1 ln= ln − F ∆Χ A0→1 I A0 E0 F is time dependent degradation factor ∆Χ A0→1 is the exposure time for SIM A between times t=0 and t=1 I B1 E1 teB ln= ln F − ∆Χ A0→1 I E te A B0 0 te = relative exposure time difference between SIM A & SIM B for same clock time Account for difference in intensity due to solar distance change: 1au F ′ ( λ , t ) = F (λ , t ) solDist 2 τ (λ , t1 − t0 ) = ∫ t t0 F ′ ( λ , t )∆Χ A0→1 dt degradation accumulates with time and must be determined for each wavelength. τ ( λ , t1 − t0 ) can be decomposed for computational convenience into a purely wavelength component (κ ( λ )) and a time dependent part C ( λ , t1 − t0 ) . But τ ( λ , t1 − t0 ) is the only physically accessible quantity. SORCE Meeting, Sedona Arizona The Impact of Solar Spectral Irradiance Variability on Middle Atmospheric Ozone September 12, 2011 Harder- 18 SIM degradation correction and long-term uncertainty ∆κ κ SORCE Meeting, Sedona Arizona The Impact of Solar Spectral Irradiance Variability on Middle Atmospheric Ozone September 12, 2011 ≤ .02 Harder- 19 WACCM ozone differences 2004-2007 NRLSSI forcing SORCE forcing SORCE Meeting, Sedona Arizona The Impact of Solar Spectral Irradiance Variability on Middle Atmospheric Ozone September 12, 2011 Harder- 20 SABER regression, equatorial average 15o N -to- 15o S Day Night Lower Mesosphere Stratosphere All regression fits are significant at 95% level SORCE Meeting, Sedona Arizona The Impact of Solar Spectral Irradiance Variability on Middle Atmospheric Ozone September 12, 2011 Harder- 21