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Sky Brightness evaluation at Concordia Station - Dome C, Antarctica for ground-based observations of the Solar Corona

Alessandro Liberatore    Gerardo Capobianco    Silvano Fineschi    Giuseppe Massone    Luca Zangrilli    Roberto Susino    Gianalfredo Nicolini INAF - National Institute for Astrophysics;
OATo - Astrophysical Observatory of Turin;
Via Osservatorio 20, 10025, Pino Torinese (To), Italy.
University of Torino, Physics Department
Via Pietro Giuria 1, 10125, Torino, Italy.
keywords:
Sky brightness, Antarctica, Sun, Corona, Coronagraphy
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1 Introduction

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s:introduction The Sun has an atmosphere divided into several layers. The outermost is called solar corona. It consists of plasma at very high temperatures (up to 10610^{6} K) that extends millions of kilometres into outer space. The solar corona is the results of three different main contributions: the K-Corona, due to Thomson scattering by the free coronal electrons of the photospheric radiation; the F-Corona, due to diffusion of solar radiation by dust particles and E-Corona due to emission processes by coronal ions identified as \sayforbidden lines.

The brightness of each component decreases with a power law moving away from the Sun (Phillips, 1992; November and Koutchmy, 1996). Figure \ireffig:brightness_solar_corona_components shows that the brightness of the sky (\sayclear with haze) makes ground-based observations of the solar corona difficult. Total solar eclipses give the opportunity to observe the corona with a reduced sky brightness. However the short duration of these events (max 7.5 minutes), the possibility of adverse weather conditions and the frequent need of accessing remote locations for the observing sites, makes it difficult to carry out continuous and detailed coronal studies. A \saypure blue sky for ground-based coronagraphic observations is defined as 106\approx 10^{-6} of the Sun’s disc brightness (B/B\mathrm{\,B/B_{\odot}}). Ground-based observations of the solar corona were made possible with the development of the internally-occulted coronagraph by Lyot (Lyot, 1932).

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Figure 1.: Brightness of the different solar corona components (B/BB/B_{\odot}) in function of the heliocentric distance. At least a Bsky[B]106B_{sky}[B_{\odot}]\approx 10^{6} is necessary to have a coronagraphic sky.\ilabelfig:brightness˙solar˙corona˙components

Mauna Loa, in the Big Island of Hawai’i is a coronagraphic site hosting the Mauna Loa Solar Observatory (MLSO) operated by the US High Altitude Observatory. MLSO can carry out systematic observations of the solar corona thanks to a sky-brightness value of 15×106B\approx 1-5\times 10^{-6}\mathrm{\,B_{\odot}} for different wavelengths (Tomczyk and Elmore, 2015). One of the goals of the Extreme Solar Coronagraphy Antarctic Program Experiment (ESCAPE: Fineschi et al., 2019a) is the determination in Antarctica of a location with a \saycoronagraphic sky that would allow systematic ground-based observations of the solar corona. In the next section we will introduce the ESCAPE project instrumentation and goals (Sec. \irefs:ESCAPEProject) and we will show the results of sky-brightness measuraments (Sec. \irefs:Results) during the 34th (austral summer 2018/2019) and 35th (austral summer 2019/2020) Italian Expeditions in Antarctica, Concordia Station - Dome C plateau at 3233m\approx 3233\mathrm{\,m} above sea level.

2 ESCAPE Project

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s:ESCAPEProject Antarctica offers a great opportunity for ground-based observations of the solar corona. Actually, the high altitude of the Antarctic plateau of Dome C (3233m\approx 3233\mathrm{\,m} a.s.l.), the high latitude (75° 06 S; 123° 20 E), the large amount of daily hours of observations during the Antarctic summer (Fig. \ireffig:sun24h) and the almost total absence of anthropic pollution, are necessary conditions for a low sky-brightness.

First attempts to characterise the sky-brightness at Dome C were perfomed in 2008 by the pioneering observations of J. Arnaud (Faurobert, M., Arnaud, J., and Vernisse, Y., 2012). One of the goals of the ESCAPE Project, at the Italian-French Station Concordia, is to quantitatively evaluate the sky brightness at the Dome C plateau. Within the ESCAPE project we developed an internally-occulted antarctic coronagraph (AntarctiCor) for observations of the K-corona polarized brightness (pBpB) generated by Thomson scattering of photospheric light of coronal free electrons for the determination of the coronal electron density (Van De Hulst, 1950).

In the following section, we will report the sky-brightness measurements. The coronal images are still under analysis. More details about ESCAPE and its science objectives can be found in Fineschi et al. (2019a). The evaluation of the sky-brightness was performed during the 34th and 35th Italian Expeditions in Antarctica by using the Antarctica solar Coronagraph, AntarctiCor (Fig. \ireffig:Montato).

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Figure 2.: Composition of hourly images showing the Sun position at Concordia Base during the Antarctic summer (Credits: Guillaume Dargaud). In the bottom, 360° images from Baseline Surface Radiation Network (BSRN) project - PI, Dr. A. Lupi (Lupi, 2021). It is possible to observe a very good sky condition on the left image. In the middle, the presence of a solar halo is a sign of ice crystals in the atmosphere that can potentially compromise observations by producing straylight. Worst sky condition are shown on the right with a slight cloud cover as well. By using the full sky camera it is possible to have a general view of sky conditions to avoid the worst days.\ilabelfig:sun24h

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Figure 3.: AntarctiCor hosted by the Antarctic Search for Transiting ExoPlanet (ASTEP) project equatorial mount during the 34th Expedition (red box) and in the Baeder dome during the 35th Expedition (green box) at Concordia station for the ESCAPE project. (Credits: A. Liberatore and G. Capobianco @PNRA/IPEV)\ilabelfig:Montato

2.1 Antarctic coronagraph instrument (AntarctiCor)

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ss:AntarcticCoronagraph

The instrument deployed during both campaigns was the Antarctica solar Coronagraph, AntarctiCor (Fig. \ireffig:AntarctiCor). The main features of the instrument are summarized in Table \ireftab:AntarctiCor_features. It is a classical Lyot internally-occulted coronagraph (Lyot, 1932) based on the externally-occulted ASPIICS (Association de Satellites pour l’Imagerie et l’Interferométrie de la Couronne Solaire) coronagraph for the European Space Agency (ESA) formation-flying PROBA-3 (Project for On-Board Autonomy-3) mission (Galy et al., 2015).

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Figure 4.: Top left: AntarctiCor in the INAF Optical Payload Systems facility (OPSys) - clean room ISO 5 in Turin (Italy) for tests and calibrations (Fineschi et al. 2019b). The main subassembly diagram (top roght panel) comprises: 1. objective lens assembly; 2. inner main barrel assembly; 3. internal occulter assembly; 4. lenses assembly; 5. filter assembly; 6. light trap assembly; 7. microscope assembly. Bottom: AntarctiCor ray tracing for the wide-band (591±5)nm(591\pm 5)\mathrm{\,nm} optical path.\ilabelfig:AntarctiCor
Table 1.: AntarctiCor Characteristics (Fineschi et al. 2019b).\ilabeltab:AntarctiCor˙features
Telescope design Classical internally-occulted Lyot coronagraph(Lyot, 1932)
Aperture 50mm\mathrm{\,mm}
Eff. Focal Length 700mm\mathrm{\,mm}
f/ratio 14
Spectral Ranges (591±5)nm(591\pm 5)\mathrm{\,nm} – see Fig. \ireffig:Filter
Camera type Interline transfer CCD PolarCam; model: U4 (Zecchino, 2017)
Camera format 1950×19501950\times 1950pixels\mathrm{\,pixels}
Pixel size 7.4μm×7.4μm7.4\mathrm{\,\mu m}\times 7.4\mathrm{\,\mu m}
Plate scale 4.3arcsec/pixel\mathrm{\,arcsec/pixel}
Field of View (FoV) ±0.6\pm 0.6° ±2.24R\equiv\pm 2.24\mathrm{\,R_{\odot}}
Polarisation analysis Spatial modulation by linear micropolarisers on the sensor

The main characteristics of the AntarctiCor bandpass filter used during the missions are shown in Fig. \ireffig:Filter and in Table \ireftab:AntarctiCor_features. More information can be found in Semrock (2019).

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Figure 5.: Semrock bandpass filter transmissivity (591±5)nm(591\pm 5)\mathrm{\,nm}.\ilabelfig:Filter
Table 2.: Main optical and physical filter specifications (Semrock, 2019). \ilabeltab:AntarctiCor˙ch
Specification Value
Transmission band Tavg>93%T_{avg}>93\% at 588594.5nm588-594.5\mathrm{\,nm}
Center wavelength 591.25nm591.25\mathrm{\,nm}
FWHM bandwidth (nominal) 10nm10\mathrm{\,nm}
Transverse dimensions (diameter) 25mm25\mathrm{\,mm}
Filter thickness 5.0mm5.0\mathrm{\,mm}

Indeed, the telescope design is derived from the design of the ASPIICS space coronagraph (Galy et al., 2015). Some modification from the original design have been adopted due to the main difference between ASPIICS and AntarctiCor: the former is externally-occulted, the latter is internally occulted. For example, since the objective doublet lens of ASPIICS operates in the shadow of the external occulter while the AntarctiCor objective is directly illuminated by the Sun-disc light, to minimize the internal reflection in the objective lens, this has been changed into a highly polished singlet, i.e. 0.5nm0.5\mathrm{\,nm} rms (Fineschi et al. 2019b).

The telescope temperature is acquired in three different points by three PT100 and it is controlled by using three heaters with a power of 90W\mathrm{\,W}, 100W\mathrm{\,W}, 40W\mathrm{\,W} in the front, central, and rear subassembly, respectively. The closed-loop heater system keeps the instrument at the set temperature (Fig. \ireffig:temperature_controll, right plot). The entire structure is kept at a constant temperature of 28\approx 28°. An infrared camera is used to verify the temperature of the telescope, mount, and the whole instrumentation (Fig. \ireffig:temperature_controll, left panel).

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fig:temperature_controll_1

(a)
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fig:temperature_controll_2

(b)
Figure 6.: Left: Infrared camera thermal image of the instrumentation. Right: Example of temperature control with a limit set of 28°.\ilabelfig:temperature˙controll

2.2 PolarCam Micropolariser Camera

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ss:PolarCam_micropolarizer_camera The telescope detector is the PolarCam micropolariser camera, U4 model.111The PolarCam© is manufactured by 4-D Technology Corporation, Arizona, United States (4D-Technology, 2021) This camera captures simultaneously 4 images at multiple polarised angles (0°, 45°, 90°, and 135°) thanks to an array of linear micropolarisers directly applied on the camera sensor. Different micropolariser orientations match different pixels of the sensor as shown in Fig. \ireffig:PolarCam. In this way, a single acquisition can return the linear polarisation of the image as derived from the Stokes vector parameters: S = (I, Q, U) = (I0+I90I_{0}+I_{90}, I0I90I_{0}-I_{90}, I45I135I_{45}-I_{135}) where I0I_{0}, I90I_{90}, I45I_{45}, I135I_{135}, are the intensities of the linear polarisation components at 0°, 90°, 45°, 135°. Indeed, the linearly polarised light requires the measurement of the I, Q, U quantities to be fully characterised (Collett, 1992). For example, it is possible to obtain the polarimetric brightness defined as pB=Q2+U2pB=\sqrt{Q^{2}+U^{2}} or the sky-brightness considering the first Stokes parameter. To obtain the single IiI_{i} (where ii = 0°, 45°, 90°, 135°) we need to perform a demosaicization process. Once a certain IiI_{i} has been chosen (e.g. I0I_{0}), we considered the three remaining pixels of each super-pixel222A super-pixel is the \saypixel obtained by considering the four adjacent pixels with different micropolariser orientation (0°, 45°, 90°, and 135°).. The values of these single pixels are obtained as the average between the pixels (with the considered polarisation I0I_{0}) in each adjacent super-pixel as shown in Fig. \ireffig:PolarCam_degrid, Output 2. The same procedure can be applied to get the images with the other orientations. More information about this camera and its usage can be found in Liberatore et al. (2021) and Zecchino (2017).

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Figure 7.: PolarCam detector. An array of linear micropolarisers with different orientation are matching the pixels of the sensor (Zecchino, 2017).\ilabelfig:PolarCam

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Figure 8.: Demosaic example to obtain a polarised image from the original raw image. In this example, the image with a polarisation angle of 0° (I0I_{0}) is obtained considering each super-pixel equal to the pixel value with the micropolariser at 0° (Output 1) or considering each super-pixel obtained considering the pixel values with the micropolariser at 0°-pixels (Output 2).\ilabelfig:PolarCam˙degrid

3 Sky Brightness Results

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s:Results During the Antarctic campaigns, systematic images of the sky were acquired in order to evaluate its brightness. The sky brightness in units of solar disc brightness (Bsky[B]B_{sky}\mathrm{\,[B_{\odot}]}) was measured the first time during the 34th Campaign (austral summer 2018/2019) and during the full data acquisition during the 35th Campaign (austral summer 2019/2020) at almost regular intervals during all days.333The 36th Campaign (austral summer 2020/2021) was limited to logistical activities due to the COVID-19 pandemic. The Bsky[B]B_{sky}\mathrm{\,[B_{\odot}]} can be evaluated by considering the first Stokes parameter II and performing a ratio between what is obtained pointing to the sky (IskyI_{sky}) and what is obtained pointing to the Sun using a diffuser (IdiffI_{diff}). Both quantities must be normalized by the respective exposure time texpit_{exp}^{i}. Then, by considering the diffuser transmissivity Tdiff28%T_{diff}\approx 28\% (EdmundOptics, 2019) we obtain:

I¯skyI¯diff=Isky/texpskyIdiff/texpdiff=Bsky(BTdiff)\frac{\overline{I}_{sky}}{\overline{I}_{diff}}=\frac{I_{sky}/t_{exp}^{sky}}{I_{diff}/t_{exp}^{diff}}=\frac{B_{sky}}{(B_{\odot}\cdot T_{diff})} (1)

Finally, by considering the light scattered over the solid angle by the diffuser over the Sun angular radius: ϑ=16\vartheta=16^{\prime}:

Ω2π=02π0ϑsinϑ2π𝑑ϑ𝑑φ=1cosϑ=1.083×105\frac{\Omega_{\odot}}{2\pi}=\int^{2\pi}_{0}\int^{\vartheta}_{0}\frac{\sin{\vartheta^{\prime}}}{2\pi}d\vartheta^{\prime}d\varphi=1-\cos{\vartheta}=1.083\times 10^{-5} (2)

the resulting sky brightness Bsky[B]B_{sky}\mathrm{\,[B_{\odot}]} is (Streete J.L., 1989):

Bsky[B]=(Isky/texpsky)(Idiff/texpdiff)TdiffΩ2πB_{sky}[B_{\odot}]=\frac{(I_{sky}/t_{exp}^{sky})}{(I_{diff}/t_{exp}^{diff})}\cdot T_{diff}\cdot\frac{\Omega_{\odot}}{2\pi} (3)

In particular, in our case, the acquired Bsky[B]B_{sky}[B_{\odot}] frame was divided into four different regions (Area in Fig. \ireffig:frame_4division) and the final brightness was obtained by averaging them:

Bsky[B]=iBskyi4[i=1,2,3,4].B_{sky}[B_{\odot}]=\frac{\sum_{i}B_{sky}^{i}}{4}\qquad[i=1,2,3,4]. (4)

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Figure 9.: Example of the measured sky brightness (Dome C, Concordia Station - Antarctica) from the 34th campaign. The entire frame is divided into 4 different pads. The final sky brightness is obtained bye averaging the 4 areas.\ilabelfig:frame˙4division

For each BskyB_{sky} we evaluate the dispersion values as the standard deviation over the pixels in a considered area (e.g. σ\sigma over Area 1) quadratically added (and then divided by a factor of four) to the standard deviations obtained in the other three regions (Area 2, 3, 4).

A so-called \saypure blue sky (i.e. Bsky106BB_{sky}\approx 10^{6}\mathrm{\,B_{\odot}}) is necessary to carry out ground-based observations of the corona (Fracastoro, 1948; Fracastoro and Righini, 1949; Elmore, 2007).
Figure \ireffig:brightness_solar_corona_components shows the sky brightness, in B\mathrm{\,B_{\odot}} units, measurements obtained during the 35th Italian Antarctic Expedition (2019-2020), at Concordia Station - Dome C.

From the images acquired during the 34th Campaign on January 08, 2019 (pointing at RA: 22° 42’ 32.3”, Dec: -22°  11’ 22”) and January 09, 2019 (pointing at RA: 22° 38’ 33.3”, Dec: -22° 18’ 19”), we obtain that:

Bsky=(1.2±0.1)×106B.B_{sky}=(1.2\pm 0.1)\times 10^{-6}B_{\odot}. (5)

During the 35th campaign it was possible to perform more systematic sky-brightness measurements. A summary of what obtained is shown in Fig. \ireffig:SkyBrightness_Bsun. Averaging over the different values we obtain:

B¯sky=(6.9±0.2)×107B.\bar{B}_{sky}=(6.9\pm 0.2)\times 10^{-7}\mathrm{\,B_{\odot}}. (6)

During these measurements, Dome C showed the characteristics of a \saycoronagraphic sky. Sometimes, the presence of clouds, high wind or excessive suspended ice in the atmosphere made it impossible to perform good observations. On the other hand, during this campaign, we evaluated a percentage of good-weather days around the 80%!

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Figure 10.: Sky brightness[B]\mathrm{\,[B_{\odot}]} measurements obtained during the 35th Italian Antarctic Campaign (2019-2020), Concordia Station - Dome C, 3230m\approx 3230\mathrm{\,m} a.s.l., Antarctica. On the x-axis, the acquisition UTC time from January 1st, 2020 to January 22nd, 2020. The bars represent the dispersion values obtained by considering the standard deviations for each of the four different detector frame areas.\ilabelfig:SkyBrightness˙Bsun

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Figure 11.: Sky brightness[B]\mathrm{\,[B_{\odot}]} measurements obtained during the 35th Italian Antarctic Campaign (2019-2020), Concordia Station, Dome C, 3230m\approx 3230\mathrm{\,m} a.s.l., Antarctica, for different declination values (up) and different right ascension ones (down) on January 1, 2020. The Sun position (J200 system) was AR: 20° 09 38, Dec: -20° 05 57. \ilabelfig:SkyBrightness˙Bsun˙CROX

During the same mission, we evaluated the sky brightness for different right ascensions (RA) and declinations (DEC) for a fixed day (see Fig. \ireffig:SkyBrightness_Bsun_CROX). The values of measured BskyB_{sky} are consistent with what obtained in Fig. \ireffig:SkyBrightness_Bsun and, as expected, it is possible to see a decrease of sky-brightness moving away from the Sun. The closest measurements to the solar limb are at about 0.7°, e.g. for the declination, the closest measurement was at 1° from Sun center (Fig. \ireffig:SkyBrightness_Bsun_CROX, up), so 10.26=0.741-0.26=0.74° from the solar limb (where 0.26° is the solar radii). We cannot really go much closer than 1° from Sun center due to the instrument field of view along the xx and yy axis. The instrument FoV is ±0.6\pm 0.6° (Table \ireftab:AntarctiCor_features) and we need that the Sun is completely out to take sky brightness measuraments.

These results show that the Antarctic sky at Dome C, where Concordia Station is located, has periods when it can be considered to have a \saycoronagraphic sky (e.g. Fracastoro 1948Fracastoro and Righini 1949Elmore 2007 and Fig. \ireffig:brightness_solar_corona_components).

4 Conclusion

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s:Conclusion In the present work, we presented the first results from the ESCAPE project. In particular, after a description of the project and its main goal, we described the instrumentation used during the Antarctic missions and its characteristics. We described the internally-occulted coronagraph AntarctiCor and its innovative detector with arrays of micropolariser for linear-polarisation imaging. Then, we described how we evaluated the sky brightness B¯sky\bar{B}_{sky} at Concordia Station (Dome C plateau - Antarctica, coord. 75° 06 S; 123° 20 E) at an altitude of 3300m\approx 3300\mathrm{\,m} above sea level. The B¯sky\bar{B}_{sky} value was obtained during two different missions. In the first one (34th Italian expedition to Antarctica - austral summer 2018/19), a sky brightness of 1.0×106B\approx 1.0\times 10^{-6}\mathrm{\,B_{\odot}} was measured. Due to a logistic problem, just few acquisitions during the mission were possible (from 18 January 2019 to 19 January 2019). These sky brightness values have been obtained for a fixed distance from the Sun. subsequently, during the 35th mission, we performed more systematic measurements (from 1 January 2020 to 22 January 2020). In addition, we performed measurements of the sky brightness not only for a fixed distance from the Sun, but for different declination and different right ascension values. In this second campaign we obtained that B¯sky7.0×107B\bar{B}_{sky}\approx 7.0\times 10^{-7}\mathrm{\,B_{\odot}}. Both results quantitatively demonstrate, for the first time, the quality of the Dome C site for coronagraphic observations. We can conclude that the Antarctic sky at Concordia Station shows the characteristics of a \saycoronagraphic sky (i.e., Bsky<106BB_{sky}<10^{6}\mathrm{\,B_{\odot}}). This holds the promises for Concordia Station to host a permanent coronagraph observatory for continuous studies of the solar corona, during the Austral summers.

Acknowledgments

This paper has been possible thanks to the whole INAF and ESCAPE Project team and the Italian Piano Nazionale Ricerche Antartico (PNRA, 2021). The AntarctiCor - ESCAPE project is funded by the PNRA, grant N. 2015-AC3.02. The authors thank Dr. Angelo Lupi (PI of BSRN project) for providing us with access to the images of the AstroConcordia all-sky camera. A particular acknowledgement to OPTEC S.p.A for the AntarctiCor telescope thermal and structural design and realisation as well. The authors thank also ALTEC Company for providing logistic support during the many AntarctiCor calibration periods at the INAF OPSys facility. PROBA-3/ASPIICS is an ESA mission.

Conflict of interest

The authors declare that there are no conflicts of interest.

Data Availability

The datasets generated during and/or analysed during the current study are available from the corresponding author on reasonable request.

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