Reconstruction of the solar UV output since 1955
- T. Dudok de Wit, M. Kretzschmar
LPC2E, CNRS/University of Orléans
Reconstruction of the solar UV output since 1955 T. Dudok de Wit, - - PowerPoint PPT Presentation
Reconstruction of the solar UV output since 1955 T. Dudok de Wit, M. Kretzschmar LPC2E, CNRS/University of Orlans Open questions How does the observed solar UV output vary on the long term ? What was its level during the Maunder era ? How
LPC2E, CNRS/University of Orléans
Space Climate 2019
How does the observed solar UV output vary on the long term ? What was its level during the Maunder era ? How was it before the 1990’s ?
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Space Climate 2019
Using solar irradiance models : e.g. NRLSSI2, SATIRE, … Using solar CaK images
[Bertello et al., 2010, Chatzistergos’ talk]
Using geomagnetic data
[Svalgaard, 2016]
Using pollen
[Jardine et al., 2016]
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0.2 0.4 0.6 0.8 1.0 UACs (aromatic/OH) 16.78 16.80 16.82 16.84 16.86 16.88 16.90 UV-B irradiance (W/m2) Calendar years CE D M S a b 1300 1900 1800 1700 1600 1500 1400 2000 0.2 0.4 0.6 0.8 1.0 UACs (aromatic/OH) 16.78 16.80 16.82 16.84 16.86 16.88 16.90 UV-B irradiance (W/m2) Calendar years CE D M S a b 1300 1900 1800 1700 1600 1500 1400 2000
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Are there other UV proxies that are
accurate enough ? stable in time ?
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Space Climate 2019
Any there any other UV proxies that are
accurate enough ? stable in time ?
Yes !!!
10.7 cm radio flux (Ottawa/Penticton) : since 1947 3.2, 8.0, 15, 30 cm radio flux (Toyokawa/Nobeyama) : since 1950’s
http://spaceweather.cls.fr
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Nobeyema radio polarimeters
Space Climate 2019
Excellent radiometric stability : < 0.4 sfu/year
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Space Climate 2019
The connection between UV irradiance and radio fluxes is at best indirect (several mechanisms, optical thickness, geometrical effects, …)
[White et al., 2011]
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wavelength [cm] 1 3 10 30 100 gyro-synchrotron emissions gyro-resonance emissions Bremsstrahlung ➞ major sunspots ➞ sunspots ➞ plages, coronal loops
Space Climate 2019
Interpreting the total radio flux in terms of UV output is difficult Let's focus instead on the rotational variability = contributions from solar structures only
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6-month averages, rescaled
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Rotational variability during halloween event (Oct. 2003)
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Halloween event
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The radio fluxes at 5 wavelengths are very redundant Determine their main contributions by using Bayesian blind source separation Assume How many contributions N = ?
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I(t, λ) =
N
X
k=1
Sk(λ) Ak(t)
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<latexit sha1_base64="kzDwezESCy0pkQboE5duXouXkP4=">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</latexit>Ak(t) ≥ 0
<latexit sha1_base64="9fHqpWb63gf1CEk0am9pVnzlWKY=">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</latexit>Space Climate 2019
All the salient features of the rotational variability are captured by 3 contributions only (N=3) [Dudok de Wit et a., 2014]
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––o–– S1 mostly short wavelengths (“Gyro-synchrotron emissions”) ––o–– S2 mostly intermediate wavelengths (“Gyro-resonance emissions”) ––o–– S3 mostly long wavelengths (“Thermal/Bremsstrahlung”)
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Amplitude of each contribution
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Conclusion : the long-wavelength contribution S3 is a proxy for the UV rotational variability
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MgII index Amplitude of each contribution
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Conclusion : the intermediate-wavelength contribution S2 is a proxy for the sunspot area
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Consider the rotational variability of the solar radio flux This rotational variability reflects the cycle variability
[Preminger and Walton 2005, 2006; DdW et al., 2018]
This variability has 3 contributions only, with
long-wavelength contribution = proxy for the UV output intermediate-wavelength contribution = proxy for the sunspot area
Did these contributions change since the 1950’s ?????
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Space Climate 2019
Consider 6-year averages (1/2 solar cycle) Conclusion the S2/S3 (“spot-to-facula”) ratio has drifted considerably
[see also Foukal, 2012]
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S2 proxy for sunspot area S3 proxy for UV output
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Conclusion : before the satellite era, the long-wavelength contribution significantly deviates from what spectral irradiance models give
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Space Climate 2019
A new and stable UV proxy from synoptic solar radio observations Agreement with spectral irradiance models (NRLSSI2, SATIRE-TS) goes down before satellite era Warning : long-term changes in the solar UV output may be significantly different from what irradiance models suggest. Nobeyama centimetric radio observations will stop in ~2021
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Comparison between long-wavelength contribution S3 and solar UV proxies
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Conclusion : variations in the intermediate-wavelength contribution S2 are in full agreement with the sunspot area (and sunspot number)
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Conclusion : the short-wavelength contribution S1 is highly intermittent and has a distinct long-term evolution
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