1 The Spots That Won’t Form Leif Svalgaard Stanford University 3 rd SSN Workshop, Tucson, AZ, Jan. 2013.

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Presentation transcript:

1 The Spots That Won’t Form Leif Svalgaard Stanford University 3 rd SSN Workshop, Tucson, AZ, Jan. 2013

2 Is the SSN Always a Good Measure of Solar Activity? Since ~1990 we record progressively fewer sunspots than expected from observations of F10.7 microwave flux

3 For a given F10.7 flux there are too few sunspots after 2000

4 We see fewer sunspots for given MPSI MWO Plage Strength Index Calibration Change Same result if Ca II or Mg II index is used MPSI is the sum the absolute values of the magnetic field strengths for all pixels where that value is between 10 and 100 gauss. The sum is then divided by the total of number of pixels in the magnetogram. SSN = 55 MPSI ? Cycle variation on Downwards Trend

5 For a given CA II K-line index there are too few sunspots after 2000 The rising phase seems to be slightly higher than the declining, but the overall trend is a decline of sunspot numbers compared to the CA II emission index.

6 Sunspots per Area

7 The Sunspot Number is ‘too low’ compared to TSI The Total Solar Irradiance used to track the Sunspot Number quite nicely, but with fewer spots compared to faculae, TSI is increasing compared to that expected by the Sunspot Number.

8 The Livingston & Penn Data From 1998 through 2012 Livingston and Penn have measured field strength and brightness at the darkest position in umbrae of 3548 spots using the large Zeeman splitting of the infrared Fe nm line.. Temp.

9 Spot Umbral Intensity [Temperature] and Magnetic Field Changing

10 Evolution of Distribution of Magnetic Field Strengths Sunspots form by assembly of smaller patches of magnetic flux. As more and more magnetic patches fall below 1500 G because of the shift of the distribution, fewer and fewer visible spots will form, as observed Normalized to same maximum Normalized to same area

11 We Observe Fewer Spots per Sunspot Group 431,000 daily obs. There is a weak solar cycle variation on top of a general downward trend seen by all observers We are losing the small spots What could be the cause of that?

12 Confirmation Using the SOON Data Giuliana de Toma reports the number of spots per group recorded by the SOON network. At solar minimum the noise is large (ovals). The result is similar to the decrease seen by the SONNE network. The same decrease is seen in the number of spots per group for very small groups. SOON

13 The Zürich Classification a: no penumbra, no bipolar structure b: no penumbra, but clear bipolar structure h: with penumbra, but no clear bipolar structure But large spots Evolution Pore: A feature in the photosphere, 1 to 3 arc seconds in extent, usually not much darker than the dark spaces between photospheric granules. It is distinguished from a sunspot by its short lifetime, 10 to 100 minutes.

14 Declining Occurrence of Small Spot Groups [Zürich Class A and B] Data from Waldmeier, McIntosh, and Locarno

15 New Solar Activity ‘Regime’ Can we use the statistical properties of past solar cycles to say something about future cycles? If the Maunder Minimum was qualitatively different the answer seems to be ‘No’ If the Sun is now entering a qualitatively new regime the same conclusion may hold ‘Rear guard’ struggle to deny such a possibility seems to miss a chance for exciting new solar physics

16 Cosmic Ray Proxy [Berggren et al.] Climate? GSN M.M.

17 NGRIP is better than Dye-3 Note scale difference by factor of 5. Dye-3 has problems between The Figures show the Flux of the 10Be atoms, not the Concentration. Unreliable

18 The Problem with Dye-3 In Dye-3, differences between concentration and flux exist mainly around 1490–1530 AD and partly during 1680–1770 AD. In order to investigate how these periods and differences correspond to solar activity, we compare NGRIP and Dye-3 concentration and flux with frequencies found in the sunspot number record (Figure 2). We note that NGRIP 10Be concentration and flux both have a negative relationship to solar activity, although there are occasional leads and lags before 1820 AD and during 1880–1910 AD in both 10Be parameters relative to the solar data. In Dye-3, there are phase differences until around 1780 AD, after which 10Be is well synchronized with the sunspots. This indicates that there is either some dating uncertainty in the older part of the cores, where Dye-3 dating was established by a different method than in the newer part, or there was a slower response in the 10Be deposition to changes in solar activity. It should be stressed that the good agreement between NGRIP and Dye-3 fluxes suggest that remaining dating inaccuracies are small. In the period around 1800 AD when NGRIP 10Be is slightly out of phase with the sunspot cycle, Dye-3 concentration is in phase, underlining the importance of having data from at least two high resolution cores for an accurate solar activity reconstruction. In addition, we reconfirm earlier findings [Beer et al., 1998] of a cyclically active sun during [grand] solar minima; a clear Schwabe cycle is present in both cores during the Maunder minimum, especially so in NGRIP.

19 ‘Burning Prairie’ => Magnetism Foukal & Eddy, Solar Phys. 2007, 245,

20 My Working Hypothesis The Maunder Minimum was not a serious deficit of magnetic flux, but A lessening of the efficiency of the process that compacts magnetic fields into visible spots This may now be happening again If so, there is new solar physics to be learned, let us not shy away from that!