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The sun is very interesting particularly because it is very dynamic. The magnetic field plays a
major role in governing dynamics of the sun. Many interesting features like sunspots, flares,
prominences, and Coronal Mass Ejections (CMEs) occur on the surface of the sun due to the
dynamics associated with magnetic fields. Therefore it is quintessential to measure and
predict them as accurately as possible. Spectropolarimetry is a powerful diagnostic tool to
infer the magnetic field from the incident radiation. The magnetic field on the sun varies from
the smallest scale, such as flux tubes to the spatial scale as large as the sun itself. Construction
of large aperture telescopes are required to obtain small scale field information and the
contribution of these fields to the overall activity or the dynamics of the sun is an important
aspect of research nowadays. High-resolution spectropolarimetry is one of the techniques
which are being performed all over the world with many large solar telescopes to infer the
small scale magnetic field information. However, it is also important to study how the vector
magnetic field (strength and the direction) of the entire sun as a whole manifests itself with
time or the solar cycle. Till date the global magnetic field of the sun has been studied but
mostly with the Line Of Sight (LOS) component. However, vector magnetic field studies with
sufficient accuracy and precision are found to be lacking mainly due to instrumental
polarization. The main motivation of the project is to perform high-precision (high
polarimetric accuracy) spectropolarimetry of sun-as-a-star and completely avoid instrumental
polarization by modulating the light before it enters the telescope. The expected polarization
signal level is quite weak. This is because most of the flux gets canceled when we consider
both the hemispheres of the sun except the very weak global field which mostly resembles a
magnetic dipole. Our aim of this project is to image the sun as a star and measure the
magnetic dipole field on daily basis.
This thesis explores various design aspects of the instrument to carryout such measurements
and the challenges that are faced if one is bestowed with a ground-based observing facility.
The effect of the atmosphere is significant if the instrument is not based on Adaptive Optics
(AO). AO is more important however, in the disk-resolved or rather high-resolution imaging.
For low resolution measurements such as ours, the effect of image aberrations is insignificant
compared to the scintillation. The turbulence or the randomness of the atmosphere introduces
crosstalk or spurious polarizations in the measurements to a significant degree and therefore it
is absolutely essential to minimize them. One approach to overcome the effects of crosstalk
(due to image motion and scintillation) is to modulate the signals at high frequencies with the
idea to make the measurements before the atmosphere changes (typically within 1 ms). We
describe this approach in detail and also show that how the effect of the spurious polarization
varies with temporal cadence and what can be the acceptable level of crosstalk to perform
such measurements. Besides, we also compare the atmospheric effects on a high-resolution
image and a point image. Instrumental polarization can also be a possible source of crosstalk
which introduces spurious polarization in the measurements. This work highlights the
technique of modulating the light before it enters the telescope so as to prevent instrumental
polarization. Therefore the size of the telescope aperture is limited by the size of the
modulators that are available.
To get an idea of the amplitude of global polarization signal and also the minimum signal that
one should expect from such weakly polarized radiation (precision), we attempted to perform
sun-as-a-star spectropolarimetric measurements from the existing Tunnel Telescope of the
Kodaikanal Solar Observatory of the Indian Institute of Astrophysics. Because of the large
integration time (> 5 hours) required to achieve the required precision level (< 10-5), we didn’t
succeed in detecting any signal. Mostly the signal remains buried under the noise. Further, we
show from the data sets obtained from SOLIS-VSM of the NSO and SDO-HMI of the NASA
that roughly the signal amplitude expected from the full disk integrated Stokes spectra is of
the order of 10-5 and the required precision level is of the order of 10-7. Performing fast
polarimetry can definitely lead to a precision of this level, as the desired Signal-to-Noise-
Ratio (SNR) can be achieved much faster.
Keeping in mind these requirements, we explore several optical design aspects in the form of
polarization modulators, spectrometers and the detectors which are available, along with their
applicability. Each of the optical components described has certain advantages and
disadvantages and we discuss each of them in the context of performing fast solar vector
polarimetry. It is to be noted here that fast modulation, also implies equally fast demodulation
technique, therefore, detectors are also to be chosen by keeping this aspect in mind. In the
discussion that follows in chapter 4, we intend to bring out the possible concepts that can be
followed to perform high precision sun-as-a-star spectropolarimetry. |
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