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MPAe T1ex127-.45ex51275atigkeitsbericht 2002/2003 - Max-Planck ...

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II.1. SONNE UND HELIOSPHÄRE/SUN AND HELIOSPHERE 29<br />

velocity of the Ne 7+ ions, which can then be used as<br />

markers of the proton flow. Therefore one has,<br />

ftot = fbp + fdr = Ne,bpvbpAdp + Ne,drvdrAdr ,<br />

(1)<br />

where f , v and A are the mass flux, measured<br />

(Doppler) outflow velocity and flux tube area, which<br />

could be inferred from the simultaneously measured<br />

magnetic flux. Ne,bp and Ne,dr denote the electron<br />

density in bright points and dark regions. Their ratio<br />

can be estimated from the line intensity ratio, by simply<br />

assuming the emission volume for a given line has<br />

the same bottom area. Empirically one finds that<br />

Ne,bp<br />

Ne,dr<br />

≈<br />

<br />

Ibp<br />

Idr<br />

≈ 1.8 . (2)<br />

The mass flux contributed by bright points to the total<br />

outflow within the measured hole area, fbp/ftot,<br />

is thus estimated to be about 12%. This estimate is<br />

consistent with previous values in the literature, and<br />

suggests that the portion of the mass flux contributed<br />

by bright points to the fast solar wind is at most comparable<br />

to the relative area they cover and therefore<br />

negligable. Funnels make the major contributions to<br />

the mass flux of the nascent solar wind.<br />

(L.D. Xia, E. Marsch, W. Curdt)<br />

Network structures and Doppler shifts in solar<br />

equatorial coronal holes<br />

By combining observations of the Sun made by<br />

SUMER and the Michelson Doppler Imager (MDI)<br />

aboard SOHO, the network structures in equatorial<br />

coronal holes have been studied, in particular the relationship<br />

between the ultraviolet emission-line parameters<br />

(line radiance, Doppler shift and line width) and<br />

the magnetic field. The bases of coronal holes as seen<br />

in chromospheric spectral lines with relatively low formation<br />

temperatures generally have similar properties<br />

as normal quiet-Sun regions, i.e., small bright patches<br />

with a size of about 2 arcsec to 10 arcsec are the dominant<br />

features in the network as well as cell interiors.<br />

With increasing formation temperature, these features<br />

become more diffuse and larger. Loop-like structures<br />

are the most prominent features in the transition region.<br />

In coronal holes, they seem to have one footpoint<br />

rooted in the intra-network and to extend into the cell<br />

interiors. Some of them appear as star-shape clusters.<br />

In Dopplergrams of typical transition region lines,<br />

such as O VI (103.2 nm), there are also many fine<br />

structures with apparent blue shifts, although, on average<br />

they appear red shifted. Structures with blue<br />

shifts usually have also broader line widths. They<br />

seem to represent plasma above large concentrations<br />

Fig. 24: Difference between the average Doppler shift<br />

in quiet Sun regions and equatorial coronal holes for<br />

various emission lines versus the line formation (electron)<br />

temperature.<br />

of unipolar magnetic field, without obvious bipolar<br />

photospheric magnetic features nearby. The difference<br />

between the average Doppler shift in quiet Sun regions<br />

and coronal holes around the equator are for various<br />

emission lines shown in Fig. 24.<br />

(L.D. Xia, E. Marsch, K. Wilhelm)<br />

Spatial mapping of scattering polarisation at the<br />

solar limb<br />

To investigate the topology of scattering polarisation<br />

at the solar limb we recorded polarised filtergrams<br />

in the core of the Ca II K line with the Zurich Imaging<br />

Polarimeter ZIMPOL II at the New Swedish Solar<br />

Telescope on La Palma. The Ca II K line is chosen for<br />

the following reasons: (i) It exhibits a strong scattering<br />

polarization signal. (ii) The relatively large line<br />

width better matches the relatively broad filter pass<br />

band (0.1 nm) than is the case for most other scattering<br />

lines in the solar spectrum. (iii) This line has a rich<br />

and intriguing spectral structure with considerable diagnostic<br />

potential. (iv) Its properties have been well<br />

explored in the spectral domain.<br />

A first inspection of the data (see Fig. 25) shows clear<br />

signatures of scattering polarisation not only in a narrow<br />

limb zone but also above the visible solar limb<br />

in spicules, as well as in regions corresponding to<br />

network boundaries. While circular polarisation due<br />

to the Zeeman effect is not detected due to spectral<br />

smearing, signatures of Hanle rotation are prominent<br />

in the limb zone as well as in the observed spicules.<br />

Observations of this type harbour potential for diagnostics<br />

of chromospheric magnetic fields. The preliminary<br />

data are promising and justify further investigation.

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