Picture of the Month

In a recently published work, KIS researchers and colleagues from MPS Göttingen present a new spherically geometric method for modelling the effect of flows on travel times of sound waves in the solar interior. This development is necessary for advancing our understanding of large-scale flows in the deep solar interior and thereby to gain insights on the origin of solar activity.

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The exact configuration of this magnetic field is important to understand the different features seen in sunspots. In the umbra, the dark center, the field is oriented perpendicular to the surface, while it is more horizontal in the penumbra, i.e. the surrounding region with narrow radially oriented filaments. Parts of the magnetic field continues into higher regions, while some of it reverses its polarity and returns back into the Sun. In the left panel of the figure we show observation with the Hinode satellite of the penumbra of a sunspot. Regions where the field returns below the surface are colored in red and blue. In the red regions, the polarity reversal is just above the surface, while it occurs in higher layers in the blue regions. The right panel show measurements with the new GREGOR Infrared Spectrograph (GRIS) at the Observatorio del Teide on Tenerife. The amount of red and blue regions in this observation is significantly less than the one found in Hinode data. The reason for this difference is subject of current studies at the KIS.

 

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On May 9th, Mercury will transit in front of the solar disk. To make this happen Earth has to be in a certain position in its orbit: The intersection points of the two planet’s orbits. They are called nodes. This happens twice a year: Around 8th of May and around 10th of November. In addition Mercury has to be in the corresponding position. This only happens every couple of years. In the 21st century there will be 14 Mercury transits: 5 in May and 9 in November. The last time it was in November 2006 and the next time it will happen in November 2019. Mercury’s angular diameter is too small to be observed by naked eye but the Kiepenheuer-Institute’s solar telescopes on Tenerife will observe the transit. It starts on 13:12 CEST and Mercury leaves the Sun at 20:40 CEST. During that time two kinds of observations will be performed: Mercury will be used as a target to determine optical properties of the telescope. Furthermore there will be measurements of the particle density of sodium close to Mercury’s surface: Various processes including the solar radiation releases a small amount of atoms (e.g. sodium) from the planet forming an extremely faint gas envelope (exosphere) and a tail....

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Today solar science is a diverse and rapidly evolving discipline. But the roots of solar science can be traced back to ancient times and beyond. Especially the observation of dark sunspots has a long tradition. While the oldest plausible record dates back to Chinese astronomers (800 BC), the first sunspot drawing was made in 1128 by the monk John of Worcester observing large sunspot formations visible to the naked eye.

At the beginning of the 17th century, several astronomical milestones were set to modernize the human understanding of the Sun. In 1609, Johannes Kepler expanded the heliocentric system to include elliptical orbits of the planets around the Sun. In the same year, the invention of the telescope became the starting shot in a new era of solar and stellar observations.

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GREGOR is a modern 1.5m solar telescope. It is also highly suitable for observing the planets of our solar system. Recently, a new instrument was built to study certain properties of the planetary atmospheres. It allows for high-precision polarisation measurements of the light reflected by the planets. In order to reach a high spacial resolution, the instrument uses the adaptive-optics system (AO) of the telescope. For this purposes, the AO normally used for solar observations had to be extended with an additional wave-front sensor for observing the much fainter objects at night.

In November 2015, polarisation measurements of Uranus in different spectral ranges were recorded. The picture shows three measurements at 450, 550 and 650nm. The first row (I) shows the normal-intensity image of the planet. In the next two rows (Q/I and U/I), images of the linear polarized part of the light are shown. The black and white pattern indicates that part of the light is polarised parallel to the...

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German-Norwegian team of scientists observes heart-shaped sunspot with GREGOR, the largest European solar telescope.

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The magnetic field of a sunspot guides magnetohydrodynamic waves toward higher atmospheric layers. In the upper photosphere and lower chromosphere, wave modes with periods longer than the acoustic cut-off period become evanescent. The cut-off period essentially changes due to the atmospheric properties, e.g., increases for larger zenith inclinations of the magnetic field. These relations were now employed to develop a novel technique of reconstructing the magnetic field inclination on the basis of the dominating wave periods in the sunspot chromosphere and upper photosphere. 

On 2013 August 21st, an isolated, circular sunspot (NOAA11823) for 58min was observed in a purely spectroscopic multi-wavelength mode with the Interferometric Bidimensional Spectro-polarimeter (IBIS) at the Dunn Solar Telescope. By means of a wavelet power analysis, the dominating wave periods were retrieved to reconstruct the zenith inclinations in the chromosphere and upper photosphere.

The results shown in...

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As early as in 1611, shortly after the discovery of the telescope, sunspots were observed and scientifically analysed. Johann Fabricus (1587 - 1616) described the movement of sunspots and deduced therefrom the rotation of the sun. In 1630, Christoph Scheiner determined that the orbital period is 27 days. Today we know that the sun rotates differentially, so that spots near the equator rotate faster than those in higher latitudes.

Since 2010, the position of sunspots can be measured with unprecedented accuracy using the data obtained with the HMI on the American SDO satellite. In a study carried out at KIS, the movement of 163 stable sunspots was measured between 2010 and 2015. The chart shows the angular velocity of the spots depending on the observed latitude ϑ on the sun. The unit used was degree/day. A rotation velocity of 14.4 degrees/day is equivalent to a rotation period of 25 days. The dependency on the latitude follows the square sine function: 14.421 (+/- 0.026) - 3.116 (+/- 0.179) sin...

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A highlight of first science results with GREGOR has been achieved by detecting the small-scale geometry of the magnetic field in a sunspot penumbra. Spectro-polarimetric data with GRIS@GREGOR reveals that 35 % of the penumbra area is covered with return flux, i.e., locations where the magnetic field has opposite polarity. Since the field strength of this downward-pointing component is small, this return flux only makes up 10% of the total magnetic flux in the penumbra. A careful analysis of the depth dependence of the magnetic field reveals that the return flux is only present in the deepest layers of the photosphere, which are probed using the four iron lines in the spectral vicinity of 1564.8 nm. This is the reason why the spectropolarimeter onboard HINODE using higher-forming iron lines around 630.2 nm cannot detect the return flux, while previous observations at 1564.8 nm with the VTT did not have the necessary spatial resolution.

This finding has important implications on the...

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Aurorae are detected from all the magnetized planets in our Solar System, including Earth. They are powered by magnetospheric current systems that lead to the precipitation of energetic electrons into the high-latitude regions of the upper atmosphere. In the case of the gas-giant planets, these aurorae include highly polarized radio emission at kilohertz and megahertz frequencies produced by the precipitating electrons, as well as continuum and line emission in the infrared, optical, ultraviolet and X-ray parts of the spectrum, associated with the collisional excitation and heating of the hydrogen-dominated atmosphere. In an international cooperation Svetlana Berdyugina from the Kiepenheuer Institut is involved in a campaign in which simultaneous radio and optical spectroscopic observations were performed of an object at the end of the stellar main sequence, located right at the boundary between stars and brown dwarfs, from which we have detected radio and optical auroral emissions both powered by magnetospheric currents. Whereas the magnetic activity of stars like our Sun is powered by processes that occur in their lower atmospheres, these aurorae are powered by processes originating much further out in the magnetosphere of the dwarf star that couple energy into the lower atmosphere. The dissipated power is at least four orders of magnitude larger than what is produced in the Jovian magnetosphere, revealing aurorae to be a potentially ubiquitous signature of large-scale magnetospheres that can scale to luminosities far greater than those observed in our Solar System. These magnetospheric current systems may also play a part in powering some of the weather phenomena reported on brown dwarfs...

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