short-period waves in the solar atmosphere

1
Astron. Nachr./AN 324, No. 4, 356 (2003) / DOI 10.1002/asna.200310126 Short-period waves in the solar atmosphere M. WUNNENBERG, A. ANDJI ´ C and F. KNEER Universit¨ ats-Sternwarte G¨ ottingen, Geismarlandstr. 11, D-37083 G¨ ottingen, Germany Received 30 October 2002; accepted 7 January 2003; published online 20 May 2003 1. Introduction The heating of the lower and middle chromosphere may be caused by the following process: Turbulent flow fields in the convection zone generate upward propagating acoustic waves, which form shocks at about 500 km and dissipate their energy. As these waves have short periods (< 100 s) and oc- cur on small scales, we need high spatial and temporal reso- lution for detecting them. 2. Observations and data processing The data for this contribution were taken in August 2000 at solar disk center with the “G¨ ottingen” two-dimensional spec- trometer, which is based on two Fabry-Perot interferometers. By scanning through the Fe I 5434 ˚ A line a time series of 41.25 min with a cadence of 25 s was taken. The line center of this non-magnetic line is formed at about 600 km. Broadband and narrow-band images were taken simultane- ously in order to allow later reconstruction as described in Krieg et al. (1999). Bisectors were calculated at every point in the field of view (27 ×13 ) and then intensity and veloc- ity maps at different bisector heights could be determined. Images of the time series, which belong to the same atmo- spheric height, were correlated and destretched to give 3D- data-boxes (x, y, t). Fig. 1. Time slices of broadband images (left) and line center veloc- ities (right). Correspondence to: [email protected] Fig. 1 shows time slices from these boxes, one for the in- tensities of broadband images, where the evolution of gran- ules can be seen and another for the velocities near line cen- ter, obtained from the narrow-band images. For each point (x i ,y i ) of the 3D-boxes (i.e. one row in the time slice) a wavelet analysis with Morlet wavelets was per- formed with a code developed by Torrence & Compo (1998). The wavelet power spectra for periods between one and two minutes were calculated. 3. Results and outlook In Fig. 2 temporal velocity fluctuations, measured near line center, at one point in the field of view are presented together with the wavelet power spectrum. 0 10 20 30 40 -1.0 -0.5 0.0 0.5 1.0 velocity [km/s] 0 10 20 30 40 time [min] 1.0 1.2 1.4 1.6 1.8 period [min] Fig. 2. Velocity fluctuations (upper panel) and appertaining wavelet power spectrum in the 1–2 min range (lower panel). Thus, we are able to show the existence of short-period waves in the solar atmosphere. More and detailed information can be found in Wunnenberg et al. (2002). With the new GREGOR telescope better spatial and tempo- ral resolution will be obtained and then we would be able to detect short-period waves with periods at about 20 s. References Krieg, J., Wunnenberg, M., Kneer, F., Koschinsky, M., Ritter, C.: 1999, A&A 343, 983 Torrence, C., Compo, G.P.: 1998, Bull. Amer. Meteor. Soc. 79, 61 (wavelet software is available at URL: http://paos.colorado.edu/research/wavelets) Wunnenberg, M., Kneer, F., Hirzberger, J.: 2002, A&A 395, L51 c 2003 WILEY-VCHVerlag GmbH & Co. KGaA, Weinheim 0004-6337/03/0406-0356 $ 17.50+.50/0

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Page 1: Short-period waves in the solar atmosphere

Astron. Nachr./AN 324, No. 4, 356 (2003) / DOI 10.1002/asna.200310126

Short-period waves in the solar atmosphere

M. WUNNENBERG, A. ANDJIC and F. KNEER

Universitats-Sternwarte Gottingen, Geismarlandstr. 11, D-37083 Gottingen, Germany

Received 30 October 2002; accepted 7 January 2003; published online 20 May 2003

1. Introduction

The heating of the lower and middle chromosphere may becaused by the following process: Turbulent flow fields inthe convection zone generate upward propagating acousticwaves, which form shocks at about 500 km and dissipate theirenergy. As these waves have short periods (< 100 s) and oc-cur on small scales, we need high spatial and temporal reso-lution for detecting them.

2. Observations and data processing

The data for this contribution were taken in August 2000 atsolar disk center with the “Gottingen” two-dimensional spec-trometer, which is based on two Fabry-Perot interferometers.By scanning through the Fe I 5434 A line a time series of41.25 min with a cadence of 25 s was taken. The line centerof this non-magnetic line is formed at about 600 km.Broadband and narrow-band images were taken simultane-ously in order to allow later reconstruction as described inKrieg et al. (1999). Bisectors were calculated at every pointin the field of view (27′′×13′′) and then intensity and veloc-ity maps at different bisector heights could be determined.Images of the time series, which belong to the same atmo-spheric height, were correlated and destretched to give 3D-data-boxes (x, y, t).

Fig. 1. Time slices of broadband images (left) and line center veloc-ities (right).

Correspondence to: [email protected]

Fig. 1 shows time slices from these boxes, one for the in-tensities of broadband images, where the evolution of gran-ules can be seen and another for the velocities near line cen-ter, obtained from the narrow-band images.For each point (xi, yi) of the 3D-boxes (i.e. one row in thetime slice) a wavelet analysis with Morlet wavelets was per-formed with a code developed by Torrence & Compo (1998).The wavelet power spectra for periods between one and twominutes were calculated.

3. Results and outlook

In Fig. 2 temporal velocity fluctuations, measured near linecenter, at one point in the field of view are presented togetherwith the wavelet power spectrum.

0 10 20 30 40-1.0

-0.5

0.0

0.5

1.0

velo

city

[km

/s]

0 10 20 30 40time [min]

1.0

1.2

1.4

1.6

1.8

perio

d [m

in]

Fig. 2. Velocity fluctuations (upper panel) and appertaining waveletpower spectrum in the 1–2 min range (lower panel).

Thus, we are able to show the existence of short-periodwaves in the solar atmosphere.More and detailed information can be found in Wunnenberget al. (2002).With the new GREGOR telescope better spatial and tempo-ral resolution will be obtained and then we would be able todetect short-period waves with periods at about 20 s.

References

Krieg, J., Wunnenberg, M., Kneer, F., Koschinsky, M., Ritter, C.:1999, A&A 343, 983

Torrence, C., Compo, G.P.: 1998, Bull. Amer. Meteor. Soc. 79, 61(wavelet software is available at URL:http://paos.colorado.edu/research/wavelets)

Wunnenberg, M., Kneer, F., Hirzberger, J.: 2002, A&A 395, L51

c©2003 WILEY-VCH Verlag GmbH & Co. KGaA, Weinheim 0004-6337/03/0406-0356 $ 17.50+.50/0