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A&A
Volume 626, June 2019
Article Number A55
Number of page(s) 14
Section Astronomical instrumentation
DOI https://doi.org/10.1051/0004-6361/201935735
Published online 12 June 2019

© ESO 2019

1. Introduction

In the present era of solar physics, many complex dynamic processes in the solar atmosphere can only be explained through sophisticated time-dependent 3D numerical simulations. Some of these simulations are already sufficiently realistic to provide quantitative predictions of (spatial variations of) physical quantities such as temperature, velocities, and the magnetic field. By combining observations of Stokes spectra obtained at high spatial resolution with modern inversion techniques (see reviews by del Toro Iniesta & Ruiz Cobo 2016; de la Cruz Rodríguez & van Noort 2017), we can in principle confront theoretical simulations with experimental data and decide whether the simulations can be validated, need to be improved, or should be refuted. However, most of the dynamics in the solar atmosphere occurs at spatial scales that are close to the diffraction limit of even the largest solar telescopes, and inferences drawn from observations are therefore more often than not severely compromised by uncertainties in the estimated spatial point spread function (PSF) of the recorded data.

A classical example that illustrates the difficulties of confronting simulations with observations is the longstanding controversy over the continuum granulation contrast, which gives a measure of the temperature fluctuations of the solar atmosphere at the visible surface. Disturbingly, measurements of the granulation contrast stretching over more than four decades vary wildly. For example, from a compilation by Sánchez Cuberes et al. (2000) we note that in 1969, Beckers & Parnell (1969) inferred a contrast equivalent to 5.12% when translated to a wavelength of 500 nm, while only two years later Levy (1971) obtained the equivalence of 18.55% at the same wavelength. Much later, between 1991 and 1997, several measurements were published that resulted in values between 9.8% and 14.85%.

Thanks to accurate measurements of the PSF of the Solar Optical Telescope (SOT) on Hinode (Tsuneta et al. 2008), there is now a satisfying congruence of granulation contrasts obtained from simulations and observations (Danilovic et al. 2008; Wedemeyer-Böhm & Rouppe van der Voort 2009; Mathew et al. 2009), demonstrating that we can indeed have confidence in the predictions made from convection simulations1. For example, it can be concluded that the true value of the granulation contrast is ≈21−23% at 500 nm, based on the compilation of results from numerical simulations (Wedemeyer-Böhm & Rouppe van der Voort 2009, their Table 3) and assuming that the root mean square (RMS) contrast is inversely proportional to the wavelength.

Calibrating the PSF even in the case of a seeing-free space-based telescope is far from a trivial task. Danilovic et al. (2008) demonstrated that the diffraction limited PSF of SOT, with its large central obscuration, spider, and CCD degrades the RMS contrast of spectra at 630 nm with the SOT spectropolarimeter (Lites et al. 2001) from its theoretically established value of 14.4% to 8.5%, which is still significantly above the observed value of 7.0%. These authors suggest that the remaining discrepancy can be explained by a combination of stray light and imperfections of the instrument, such as a focus error or low-order aberrations. A more detailed determination of the PSF of SOT was made possible by observing the planet Mercury against the solar disk (Mathew et al. 2009) and using a combination of solar eclipse and Mercury transit data (Wedemeyer-Böhm 2008). Similar methods have been used to characterize the PSFs of several ground-based solar telescopes, but as discussed above there is a disappointing lack of consistency as regards the measured granulation contrast.

Significant efforts to understand the PSF and performance of an adaptive optics (AO) system were undertaken by Marino (2007) and Marino & Rimmele (2010), and also discussed by Rimmele & Marino (2011). These authors modified the wavefront sensor (WFS) of the Dunn Solar Telescope to allow its AO system to lock on bright stars such as Sirius. Through long exposures, they determined the core as well as the far wings of the PSF, and performed a comparison with the theoretical PSF expected from the AO telemetry simultaneously obtained with the science exposures. These tests validated the method of obtaining the PSF from AO telemetry when an object with zero angular extent (a star) is the WFS target but does not provide a critical test of relevance to the performance of solar AO, which suffers from anisoplanatic effects when solar fine structure is used as WFS target.

Analysis of data from the Swedish 1-m Solar Telescope (SST; Scharmer et al. 2003a) shows that the main source of stray light is from small-angle scattering over at most a few arcseconds. This conclusion follows from analysis of images containing both a sunspot and granulation, recorded in 2010. These data were restored with multi-object multi-frame blind deconvolution methods (MFBD and MOMFBD; Löfdahl 2002; van Noort et al. 2005). The measured granulation contrast of the MFBD processed images was 8.9%, which is only 53% of the expected 16.9% contrast, whereas the measured minimum umbral intensity of a sunspot was as low as 15.8%. This constrained the corresponding stray-light PSF to have a full width at half maximum (FWHM) of at most a few arcseconds (or else the restored umbra intensity would be negative), leading to the conclusion that the main source of stray light must be small-scale aberrations (Scharmer et al. 2011, their supporting online material; SOM2). This conclusion was reinforced by later work (Löfdahl & Scharmer 2012) indicating that a significant fraction of the stray light comes from reimaging optics (including the tip-tilt and adaptive mirrors). Subsequent work by Löfdahl (2016) confirmed that the far-wing scattered light (such as from scattering in the Earth’s atmosphere or from dust on the telescope optics) in SST data is insignificant in the context of explaining the observed granulation contrast.

In this paper, we discuss co-temporal measurements of seeing and granulation contrast recorded with the SST, after replacing both the tip-tilt and adaptive mirrors, and the theoretical explanation by means of numerical calculations. The paper is organized as follows: In Sect. 2, we discuss measurements of the seeing and granulation contrast, in Sect. 3 we discuss the interpretation, including theoretical calculations, and demonstrate that the measured granulation contrast gives an optical quality measure similar to the Strehl ratio. In Sect. 4 we summarize the results.

2. Observations and seeing measurements

2.1. Telescope and adaptive optics

The SST is a 1 m evacuated solar telescope consisting of a primary and secondary optical system. The primary system consists of a 1.1 m singlet lens of fused silica with a clear aperture of 0.98 m and two 1.4 m flat Zerodur mirrors used to deflect the beam into a 17 m high tower. The secondary optical system consists of a 60 mm field mirror, a 250 mm clear aperture Schupmann corrector that is used to remove the chromatic aberrations of the singlet lens, a 50 mm field lens, a 42 mm tip-tilt mirror, a 34 mm clear aperture adaptive mirror, and a 40 mm reimaging triplet lens.

The present AO system (Scharmer et al., in prep.) was installed in 2013 and uses an 85-electrode monomorph deformable mirror (DM) from CILAS together with an 85 subaperture hexagonal microlens array from Smart Microoptical Solutions (SMOS). The system is characterized by a very large WFS field of view (FOV) of about 17″ × 17″, an image scale of 0 . ″ $ {{\overset{\prime\prime}{.}}} $48 per pixel, and an update frequency of 2 kHz.

2.2. Seeing measurements

Since 2013, real-time seeing measurements have been routinely made at the SST using the WFS of the new AO system. The electrode and WFS layouts are shown in Fig. 1. Of particular importance in the present context are the four lenslets highlighted with red circles. These are separated by ≈47 cm and 48.8 cm in the horizontal and vertical directions, respectively, when projected on the 98 cm pupil diameter. We use the measured longitudinal and transverse differential image motions between these four lenslets to provide measurements of the seeing quality in terms of Fried’s parameter r0. To estimate r0, we use the approximate equations given by Sarazin & Roddier (1990), giving the expected variance of differential image displacements x and y,

⟨ ( x ( s ) − x ( 0 ) ) 2 ⟩ = 0.358 λ 2 r 0 − 5 / 3 D − 1 / 3 ( 1 − 0.541 ( s / D ) − 1 / 3 ) , $$ \begin{aligned} \langle (x(s)-x(0))^2\rangle = 0.358 \lambda ^2 r_0^{-5/3} D^{-1/3} (1 - 0.541 (s/D)^{-1/3}) , \end{aligned} $$(1)

thumbnail Fig. 1.

Layout of the present 85-electrode monomorph DM and 85 subaperture WFS of the present AO system of the SST. The gray or white radial/azimuthal structures correspond to the electrodes of the DM and the hexagonal structures correspond to the 85 lenslets. The four lenslets indicated with small red circles correspond to the subapertures used for seeing measurements. The large red circle corresponds to the pupil diameter. For details, see text.

for longitudinal image displacements (i.e., image displacements along the direction connecting the centers of the two subapertures involved), and

⟨ ( y ( s ) − y ( 0 ) ) 2 ⟩ = 0.358 λ 2 r 0 − 5 / 3 D − 1 / 3 ( 1 − 0.811 ( s / D ) − 1 / 3 ) , $$ \begin{aligned} \langle (y(s)-y(0))^2\rangle = 0.358 \lambda ^2 r_0^{-5/3} D^{-1/3} (1 - 0.811 (s/D)^{-1/3}) , \end{aligned} $$(2)

for transverse image displacements. In this equation, D is the subaperture diameter, s is the separation between the centers of the subapertures, and λ the wavelength. In order to compensate for the closed-loop actions of the DM on the measured differential image motions we multiply the vector of voltages with the inverse of a matrix that is obtained during the calibration of the AO system and that gives the x, y image displacements with unit voltage on each electrode for each subaperture. We verified, by operating the closed loop of the AO system in on-off mode at 10 s intervals, that this compensation gives reliable r0 estimates.

The AO system, WFS, and software used at the SST for seeing measurements have a few notable properties as follows:

1. The optical surface of the adaptive mirror is likely of exceptional quality. The manufacturer (CILAS) estimates that the residual wavefront error is only 6 nm RMS (mechanical 3 nm RMS) after flattening with optimum voltages on the electrodes. In addition, simulations show that the combination of the WFS and electrode layout, which was designed by one of the authors (GS) allows 84 modes to be controlled, the only uncontrollable mode being piston. Finally, we recently replaced also the 40 mm diameter tip-tilt mirror with a 42 mm mirror polished by IC Optical Systems (ICOS) to Fabry–Pérot quality (approaching 1/100 wave PV). We attribute the overall optical quality of the adaptive mirror and tip-tilt mirror as a major reason for the high granulation contrast.

2. We use relatively large subapertures, ≈9.4 cm in diameter. A sufficiently large lenslet diameter is needed to allow image shift measurements with low noise, when using low-contrast granulation as WFS target. At the same time, a lenslet diameter that is too large may not allow wavefront slopes measurements when r0 is small. Based on experience with this system and a wide-field WFS (Scharmer & van Werkhoven 2010) installed at the SST, the 9.4 cm lenslet diameter gives reasonably accurate measurements of r0 when r0 >  6 cm, whereas the AO system can lock in as bad seeing as corresponding to r0 ≈ 5 cm. We note that Löfdahl (2010) demonstrated that cross-correlation techniques using granulation as target results in measured image displacements that are linear in the wavefront slopes even when r0 is significantly smaller than the subaperture diameter.

3. The AO WFS uses a very large FOV for the cross-correlations, 24 × 24 pixels or 12″ × 12″, to average out as much as possible of the high-altitude seeing and thus to minimize the image quality degradation outside the AO lock point. By splitting each 24 × 24 pixel image into 3 × 3 subfields of 8 × 8 pixels, we also measure and average r0 from nine smaller subfields of only 4″ × 4″. This is possible by measuring image shifts relative to those of the 12″ × 12″ and only allowing ±0″​.5 relative shifts. Whereas the large FOV essentially only corresponds to low altitude seeing, the small FOV measurement gives an r0 that is a combination of both low- and high-altitude seeing, roughly according to r 0 − 5 / 3 ≈ r 0 low − 5 / 3 + r 0 high − 5 / 3 $ r_0^{-5/3} \approx r_{0\,\mathrm{low}}^{-5/3} + r_{0\,\mathrm{high}}^{-5/3} $.

4. We measure and compensate for the WFS noise of these measurements. This is done by continuously monitoring the variance of the difference in image motion between consecutive wavefront samples taken 500 ns apart and, assuming that such variations must be from noise, dividing this variance by a factor of 2. We verified for a few data sets that this gives estimates of the noise level that are similar to what is obtained from power spectra of the measured differential image motions.

5. We calculate average variances of the relative image displacements over only 2 s time intervals. However, the variances are not calculated relative to an average differential image motion taken over the same 2 s. Instead, we calculate the variances relative to an average taken over 20−30 s3. In this way the variances calculated during 2 s include both the fast (high temporal frequencies) and the slow (low temporal frequencies) of the seeing, in spite of the short time averaging interval. The reason for this procedure is the strong intermittency of the (daytime) seeing, which is clearly evidenced by the strong time variability of the quality of the SST science images. This intermittency makes it meaningless to define a single average quality measure, such as r0 or the granulation contrast, during time intervals of significantly longer duration than a few seconds (as found also in our previous analysis; Scharmer et al. 2010).

6. The r0 measurements are averages over 2 s intervals as described above, but the measurements are made with overlapping time intervals such that we get one r0 measurement per second.

Figure 2 shows an example of measurements of r0 during a time span of only 5 min; the yellow curve shows (essentially) near-ground seeing and the black curve the contribution of (essentially) the entire atmosphere. It is evident that the daytime seeing is highly intermittent in this case, as confirmed by the strongly variable quality of the science images, and this constitutes a clear rationale for dividing the analysis into 2 s intervals. It is also evident that when the seeing is relatively good (r0 reaching 0.2 m or more), there is a large difference between the seeing inferred from the yellow and black curves. This is because the measurements corresponding to the yellow curve are only sensitive to ground-layer seeing, whereas the data of the black curve also includes contributions from high-layer seeing. When the seeing temporarily becomes very poor, it is normally a consequence of ground heating and near-ground turbulence, which impacts equally on the black and yellow curves. However, when the ground-layer seeing becomes excellent for a brief moment, as revealed by the yellow curve, there is still the (independent) contribution from high-layer seeing. During the early mornings of good days, when the Sun is at very low elevation, it frequently happens that r0 measured with 24 × 24 pixels reaches values of over 50 cm, even though the live solar image shows strong and small-scale warping. These large r0 values clearly are not reasonable. The values obtained with 8 × 8 pixels, on the other hand, obviously respond to the small-scale differential morning seeing and overall appear much more reasonable.

thumbnail Fig. 2.

Yellow curve, which is saturated in some peaks, shows the time variation of the SST seeing quality (Fried’s parameter r0) as measured with the 12 . ″ $ {{\overset{\prime\prime}{.}}} $0 × 12 . ″ $ {{\overset{\prime\prime}{.}}} $0 WFS of the SST AO system, and the black curve shows the corresponding variations measured with a much smaller FOV of 4 . ″ $ {{\overset{\prime\prime}{.}}} $0 × 4 . ″ $ {{\overset{\prime\prime}{.}}} $0. The yellow curve corresponds roughly to ground-layer seeing and the black curve to a combination of ground- and high-altitude seeing (see text). We note the strong intermittency that requires high time resolution. The data were recorded on 13 May 2016.

From the above discussion and Fig. 2 it is evident that the seeing measurements with 24 × 24 pixels are insensitive to high-altitude seeing and therefore unrealistic. In the following we only discuss seeing measurements made with the AO system using 8 × 8 pixels, or 4″ × 4″.

2.3. Granulation contrast measurements and calculations

2.3.1. CRISP and CHROMIS reimaging systems

Figure 3 shows the optical setup of the main optical tables at SST, including the CRISP and CHROMIS dual Fabry–Pérot filter-based narrowband reimaging systems, their wideband correspondences, and the AO system and its WFS. The beam enters the tables via a tip-tilt mirror, the 85-electrode adaptive mirror, and a reimaging triplet lens. The beam is then divided by a dichroic beam splitter into the red (CRISP) and blue (CHROMIS) beams. The SST uses a separate tip-tilt mirror (controlled by the correlation tracker camera and its computer) to compensate image motion and the AO system has a deformable mirror to compensate for higher order aberrations. The correlation tracker camera is located on the blue beam and the AO WFS is on the red beam. Each beam contains beam splitters to split light into the auxiliary wideband systems of CRISP and CHROMIS, and to the AO WFS and the correlation tracker camera.

thumbnail Fig. 3.

Layout of the present optical setup at SST, including the AO and WFS, and the CRISP and CHROMIS narrowband and wideband reimaging systems. At the time of the tests, CHROMIS was not yet installed and its wideband reimaging together with the prefilters of CHROMIS was used at the present location of CHROMIS. For details, see text.

By using two ferro-electric liquid crystal modulators and a polarizing beam splitter, CRISP can be used for measurements of both circular and linear polarization at any wavelength covered by the pre-filters. The CRISP beam allows for a so-called phase diversity setup with one focused and another intentionally defocused camera (Löfdahl & Scharmer 1994) at the wideband beam, but this feature was not in use at the time of recording the present data. The CHROMIS beam also allows for a phase-diversity setup at the wideband beam but does not yet allow for polarization measurements. Both CRISP and CHROMIS use telecentric reimaging systems, with two antireflection (AR) coated doublet lenses and a pupil stop on both the input and output sides. The wideband reimaging systems are also telecentric, and use two cemented doublet lenses with designs that are identical to those of the first and last lenses of the corresponding narrowband reimaging systems. All etalons are wedged and have AR coatings to minimize light losses and spurious reflections. The low-resolution etalons (see also the next paragraph) of CRISP and CHROMIS are slightly tilted so that the pupil stops on the output side can completely eliminate ghost images from inter-etalon reflections. Both CRISP and CHROMIS have been designed to be as compact as possible with the constraint that the Strehl ratio must be at least 0.95 at all wavelengths and all field points within a 1′ × 1′ FOV. The minimum Strehl ratios are actually a bit higher than 0.95, according to the optical design. The overall length of CRISP from focal plane to focal plane is 1.5 m and that of CHROMIS is 1.6 m.

Both CRISP and CHROMIS share an important design feature proposed by Scharmer (2006), namely to use a combination of high reflectivity for the high-resolution etalon and low reflectivity for the low-resolution etalon. This is fundamental in ensuring that the low-resolution etalon has a spectral passband that is wide enough to accommodate the wavelength shifts from cavity errors of the high-resolution etalon. This in turn leads to high throughput and a spectral transmission profile that shows small variations, apart from wavelength shifts, across the FOV. All in all, both CRISP and CHROMIS are highly efficient in terms of throughput and deliver exceptional image quality. The image scales for CRISP and CHROMIS are 0 . ″ $ {{\overset{\prime\prime}{.}}} $06 and 0 . ″ $ {{\overset{\prime\prime}{.}}} $04 per pixel, respectively, and the exposure times were 17.5 and 1−2 ms, respectively. The short exposure times are necessary to “freeze” the seeing and allow image reconstruction with compensation for residual aberrations.

2.3.2. Observational data and contrast measurements

The data discussed in this paper were obtained with SST on 5 April 2015 (CRISP narrow- and wideband) and 13 May 2016 (CHROMIS wideband), the latter observations taking place when pre-filters and the wideband reimaging system for CHROMIS were available, but the narrowband CHROMIS system was not yet ready. Table 1 gives a summary of the center wavelengths and passbands of the filters used with CHROMIS and CRISP.

Table 1.

Properties of data collected.

On the red beam, the r0 measurements in the log file of the AO system, accurately timed at 1 s intervals, were used to create groups of images recorded during the time intervals precisely corresponding to the r0 measurements. On the blue beam, images were recorded in fixed bursts of 100 images, collected during 2 s, and instead r0 was mapped to the time of the image bursts by interpolation of adjacent r0 measurements. The bursts of images were then processed with multi-frame blind deconvolution (MFBD; Löfdahl 2002) using different number of corrected aberration modes: 2 modes (tip-tilt only), 36 modes, and 100 modes. We shall only discuss the restorations using 2 and 100 modes.

For each of the images restored as described above, we calculated the RMS granulation contrast over quadratic subfields having different dimensions. We found, as expected, that using a small subfield gives a slightly higher average contrast but also larger scatter when plotting granulation contrast against r0. We finally opted for a fairly large FOV of 18″ × 18″, corresponding to 300 × 300 pixels with CRISP and 450 × 450 pixels with CHROMIS.

In Figs. 4 and 5 are shown images recorded through the CRISP and CHROMIS reimaging systems during moments of excellent seeing during the two campaigns. Each image shown represents an average over 2 s and we show images obtained with only tip-tilt correction and compensation for the diffraction limited PSF of the telescope, as well as images that have been restored with the MFBD method to compensate for the 100 most significant Karhunen–Loève (KL) modes. It is evident that the image quality through these reimaging systems is outstanding during excellent seeing conditions. As regards CRISP, it also seems evident that the image quality with CRISP itself, which involves two Fabry–Pérot etalons, is comparable with that obtained through its wideband system. Table 2 summarizes the highest measured contrast values, obtained during excellent seeing conditions, with the different CRISP wideband filters and CRISP itself.

thumbnail Fig. 4.

Top 8 panels: resulting WB (bottom 4 panels) and CRISP NB (top 4 panels) images after adding up the 74 observed images during 2 s and only compensating for relative image motion (tip and tilt) between the individual exposures and the PSF of the diffraction limited telescope. Bottom 8 panels: resulting image of the same observed images but after applying MFBD image reconstruction to compensate for the largest 100 KL modes. The wavelengths are (left to right) 525 nm, 557 nm, 630 nm, and 853 nm.

thumbnail Fig. 5.

Top 3 panels: resulting CHROMIS WB images after adding up the 100 observed images during 2 s and only compensating for relative image motion (tip and tilt) between the individual exposures. Bottom 3 panels: resulting images of the same observed images but after applying MFBD image reconstruction to compensate for the largest 100 KL modes. The wavelengths are (left to right) 395 nm, 400 nm, and 485 nm.

Table 2.

Observed granulation contrasts with SST/CRISP.

In the following we quantify and investigate the image quality of CRISP and CHROMIS in variable seeing conditions.

Figure 6 shows the correlation between r0 and the measured granulation contrast. The blue dots show the correlation obtained with MFBD restorations when compensating for the tip-tilt modes only, and the red dots the results with 100 modes. The dotted horizontal line shows the contrast expected from theoretical simulations, as described in Sect. 3.1.1.

thumbnail Fig. 6.

RMS contrast of granulation measured from SST images recorded at different wavelengths and in different seeing conditions characterized by the Fried r0 parameter. Both r0 and the granulation contrast have been averaged over 2 s. The blue dots refer to RMS contrasts of images recorded with the AO system and that are compensated only for the diffraction limited point spread function, the red dots to RMS contrasts of images further compensated for aberrations with the multi-frame blind deconvolution method (Löfdahl 2002), and the horizontal dotted lines show the contrasts of 3D MHD simulations. Images were recorded with wide-band (WB) filters on both the “red” (CRISP) and “blue” (CHROMIS) beams. Note that the plot limits for r0 vary from one plot to another and that data for r0 values smaller than 0.04 m, shown as vertical dotted lines, are excluded. Two of the panels in the lowermost row show a comparison between RMS contrast obtained from images recorded simultaneously through wideband pre-filters (labeled WB) and the corresponding narrowband (NB) CRISP spectropolarimeter filter system on the “red” beam of the SST (see text). The significantly higher contrast of the NB beam at 853.6 nm is because of the strong influence of the Ca 854.2 nm line within the passband of the WB filter.

The blue dots show an excellent correlation between the measured seeing quality (r0), obtained from the AO system, and the granulation contrast measured from science cameras on the blue and red beams. This demonstrates the high relevance of our seeing measurements as an indicator of data quality. For the MFBD processed images with 100 aberration modes (the red dots), the contrast is systematically higher but with a larger spread.

The relations between r0 and the image contrast consistently are highly nonlinear and with clear evidence of showing asymptotic convergence to values that are well below those expected from theoretical magnetohydrodynamic (MHD) simulations. The origin of this behavior is discussed in the following section.

Finally, the last two plots in Fig. 6 show the relation between the contrasts measured with the wideband and narrowband beams of CRISP for two wavelengths (630.2 nm and 853.6 nm), along with the relation expected from theoretical simulations (shown as a straight line). It is evident that the contrast in the narrowband CRISP data is only marginally less than expected from MHD simulations, and the contrast in the corresponding wideband images.

3. Theoretical interpretation

To explain the observed relation between r0 and the measured granulation contrast, we rely on the (by now) well-established theory of the PSF in the presence of turbulence-induced seeing and the effects of partial compensation of the PSF for such seeing by an AO system; for early reviews see, for example, Conan et al. (1992), Hardy (1998), and Britton (2006). Such partial compensation results in a PSF that can be roughly described as the linear combination of a diffraction limited PSF and another much wider PSF, usually referred to as the “halo”, i.e.,

P = S P d + ( 1 − S ) P h $$ \begin{aligned} P = S P_{\rm d} + (1-S) P_{\rm h} \end{aligned} $$(3)

where S is the Strehl ratio, Pd the diffraction limited PSF and Ph the PSF corresponding to the halo. Since the FWHM of Ph with a well-functioning high-order AO system on a meter-class telescope is typically one order of magnitude larger than the FWHM of Pd, it is comparable to the scale of granulation, which is about 1 . ″ $ {{\overset{\prime\prime}{.}}} $5. We therefore expect that primarily Pd contributes to the observed contrast, which then tends to equal that of the diffraction limited telescope reduced by a factor S.

To test this conjecture, we plot in Fig. 7 the observed granulation contrast versus the Strehl value obtained from r0 and an assumed number of perfectly corrected (independent) aberration parameters N by the AO system4. The wavefront variance is estimated for zonal correction as (Roddier 1998)

σ N 2 = 0.34 ( D / r 0 ) 5 / 3 ( N + 1 ) − 5 / 6 , $$ \begin{aligned} \sigma _{N}^2 = 0.34\, (D/r_0)^{5/3} (N+1)^{-5/6}, \end{aligned} $$(4)

thumbnail Fig. 7.

RMS contrast of granulation images recorded in different seeing conditions characterized by the calculated Strehl value based on the residual wavefront RMS from r0 and assuming that the AO system provides perfect correction of 81 modes. The blue dots refer to RMS contrasts of images that are compensated only for the diffraction limited PSF, and correspond to the blue dots in Fig. 6. The green dots correspond to the same contrast measurements but with the Strehl value calculated on the basis of an additional wavefront variance corresponding to 1/13 wave RMS at 630 nm, and scaled at other wavelengths as the inverse of the wavelength. The straight lines have been fitted to data points for which the Strehl is larger than 0.15.

where σN is in radians and D is the telescope diameter. The Strehl ratio S can be estimated as

S = S N = exp ( − σ N 2 ) . $$ \begin{aligned} S = S_{N} = \exp (-\sigma _{N}^2). \end{aligned} $$(5)

Assuming almost perfect correction by the SST 85-electrode AO system, N = 81, we show in Fig. 7 the measured granulation contrast versus the inferred Strehl value. In this figure, the blue and green dots correspond to the same measured granulation contrasts as shown in Fig. 6 and the blue dots to the Strehl values calculated as described previously. The relation between the Strehl and the contrast is almost perfectly linear. From a fit of a straight line to the data, which ignores all Strehl values below 0.15, we can extrapolate to find the “seeing-free” contrast for S = 1. It is evident that the extrapolated values are well below the values expected from theoretical simulations, shown as dotted lines. The green dots in Fig. 7 corresponds to the Strehl ratios obtained by adding an ad hoc wavefront variance corresponding to 48 nm RMS (1/13 wave at 630 nm), assumed to be from fixed aberrations or shortcomings in the AO system. This corresponds to rewriting Eq. (5) as

S = exp ( − ( σ s 2 + σ N 2 ) ) = exp ( − σ s 2 ) S N = S s S N , $$ \begin{aligned} S = \exp (-(\sigma _{\rm s}^2+\sigma _{N}^2)) = \exp (-\sigma _{\rm s}^2) ~S_{N} = S_{\rm s} ~S_{N},\end{aligned} $$(6)

such that the effect of additional static aberrations is to multiply the Strehl values associated with residual seeing by a factor Ss.

The assumption of a nearly perfect AO system with N = 81 is of course unrealistic. According to the compilation of Roddier (1998), perhaps the best we may hope for is an efficiency of around 50%, corresponding to N = 42. In Fig. 8, we show the relations between the Strehl ratios and the granulation contrast for N = 36, also with straight lines fitted to all data points with Strehl values above 0.15, and with the same added static wavefront variance as in Fig. 7. Again, we find nearly linear relations for S >  0.15 and that a static wavefront error corresponding to about 1/13 wave RMS can explain why the seeing-free data do not seem to reach the expected granulation contrasts. We investigate these empirical relations with theoretical simulations in the following Section.

thumbnail Fig. 8.

Same as for Fig. 7 but assuming that the AO system provides perfect correction of 36 modes.

We should mention that establishing a relation between the RMS contrast and Strehl similar to that described above is not possible for the images processed and restored to compensate for the most significant 36 or 100 KL modes. This is because the restored images are combined in a way that scales the contributions from different images with the squares of their calculated transfer functions. This weighting favors contributions from individual images recorded during moments of excellent seeing, but also excludes the use of the simple analysis used with the tip-tilt only compensated images.

3.1. Simulated AO compensated point spread functions

We simulated atmospheric turbulence with 10 random wavefronts by scaling randomized coefficients for the 1004 first KL modes to the values given by Kolmogorov statistics. We assumed 100% AO correction of low-order modes up to KL modes N ∈ {2, 18, 36, 81}, respectively, including piston; thus removing 3 KL modes in practice corresponds to removing the tip and tilt dominated KL modes.

The remaining random wavefronts were then scaled to different Strehl ratios SN ∈ {0.01, 0.02, …, 1.00}. With these wavefronts, we calculated optical transfer functions and formed averages over the different atmospheric realizations. We generated PSFs based on the above averages and calculated the encircled energy for a grid of radii with a step size of 0 . ″ $ {{\overset{\prime\prime}{.}}} $033. The radii corresponding to 80% encircled energy were then found by linear interpolation.

The top nine panels of Fig. 9 show the PSFs at 400, 630, and 854 nm from residual seeing corresponding to Strehl ratios of 0.6, 0.3, and 0.1 after removing the first 2 (tip-tilt only), 18, 36, and 81 KL modes. With only the tip-tilt modes removed, a strongly reduced Strehl is associated primarily with a broadening of the core of the PSF. For higher order compensation, the PSF core is mostly unaffected but of reduced strength by a factor S and with a characteristic rapid transition from the diffraction limited core to the surrounding halo. In the lowermost three panels in the same figure is shown the diameter of the PSF corresponding to 80% encircled energy. This diameter is less than 1″ at high Strehl and 400 nm wavelength, increasing to 4″ at 50% Strehl and 854 nm. We note that the radius of the peak of the halo is set by the number of compensated KL modes and is essentially independent of the Strehl. When the Strehl changes, the structure of the halo remains more or less the same but its strength varies as 1 − S.

thumbnail Fig. 9.

Top 9 panels: variation of the shape of the PSF with the Strehl ratio after perfect compensation of the first 2 (tip-tilt only), 18, 36, and 81 aberration modes. Lowermost 3 panels: variation with Strehl of the diameter of the PSF containing 80% of the encircled energy for the same number of compensated modes.

3.1.1. Simulated granulation data and contrast calculations

To calibrate the observed contrasts through the different CRISP and CHROMIS filters, we calculated synthetic spectra using a snapshot from a 3D radiation hydrodynamic simulation of solar granulation (Stein & Nordlund 1998). The simulation covers a horizontal physical domain of 6 × 6 Mm. In the vertical direction it extends from −453 km to 575 km above the continuum formation layer in the photosphere. The snapshot is given in a grid with 254 × 254 horizontal points and 82 vertical points. The vertical sampling is 12.7 km/grid cell and the horizontal resolution is 23.7 km/grid cell. The same snapshot was used by Scharmer et al. (2010). The spectra were calculated with a local thermodynamic equilibrium (LTE) synthesis module included in the STiC code (de la Cruz Rodríguez et al. 2016, 2019). The ionization balance and chemical equilibrium were solved using an LTE equation of state, including molecules and accurate partition functions (Piskunov & Valenti 2017). All line data were extracted from the VALD-3 database (Ryabchikova et al. 2015; Piskunov et al. 1995). The van der Waals damping parameter was calculated using cross sections provided by Barklem & O’Mara (1998), Barklem et al. (2000), for all lines for which the collisional cross sections were available. The formal solution of the transfer equation was computed using a third order Bezier interpolant (Auer et al. 2003; de la Cruz Rodríguez & Piskunov 2013).

The so-obtained simulated spectra were multiplied with the transmission profiles of the CRISP and CHROMIS prefilters provided by the manufacturers, and summarized in Table 1. These spectra were then integrated over wavelength to provide the WB contrasts referred to in Table 1.

To reduce wrap-around effects from the extended wings of the PSF, we repeated the periodic FOV to perform the required convolutions on 512 × 512 pixel images. These synthetic images were then convolved with the PSFs described above and deconvolved with the diffraction limited PSF of SST. So, these data correspond to observed data that have been corrected for the theoretical PSF of the telescope or processed with higher order modes using MFBD. The RMS contrasts were calculated over the original FOV, avoiding the apodized edges.

3.1.2. Results

Figure 10 shows the results of the theoretically calculated granulation contrasts for different Strehl values in the presence of seeing and AO compensation of the first 2, 18, 36, and 81 modes. In the limit of very large number of corrected modes, the RMS contrast is directly proportional to, and thus a direct measure of, the Strehl value. For a smaller number of corrected modes in the range 18 to 81, the relation is almost linear for Strehl values above 0.1, but the theoretical curves do not extrapolate to zero contrast at zero Strehl. This is because the FWHM remains narrow enough with a relatively small number of corrected modes, such that the granulation pattern is not washed out entirely but instead the granulation contrast reaches a limiting value set by the shape of the halo of the PSF, Ph. This implies that the extrapolated granulation contrast to a Strehl of zero provides valuable information about Ph.

thumbnail Fig. 10.

Theoretically calculated RMS granulation contrast for different Strehl values, based on residual wavefront errors after perfect low-order modal compensation of seeing degraded images recorded with a 1-m telescope. When approximately 50 modes or more are compensated, the relation between the Strehl ratio and the granulation contrast is almost linear, and independent of the number of modes compensated. This is because the wings of the PSF are then sufficiently wide (see Fig. 9) that more than one granule is included under the PSF. With such wide wings, making the PSF wider does not increase the amount of stray light. At short wavelengths, a higher number of compensated modes than at long wavelengths is required for this simple relation between Strehl and granulation contrast to be true.

Comparing the simulations in Fig. 10 to the empirical results in Fig. 7, it is obvious that the assumption of N = 81 produces unreasonable results. For the data corresponding to wavelengths at 525 nm and longer, the empirical curves extrapolate to zero contrast for Strehls in the range 0.1–0.4 whereas the extrapolated theoretical curves never reach zero contrast even at zero Strehl. Figure 8, based on the assumption that N = 36, shows much more reasonable results in this regard, except for λ = 853 nm. Plots made with N = 18 (not shown) demonstrate that this inconsistency can be removed and suggests that the efficiency of the SST AO system perhaps corresponds to less than 36 modes.

3.2. Discussion

A problem with the interpretation of the 853 nm data is that CRISP uses back illuminated CCD cameras with a silicon layer that is partially transparent for light at wavelengths longer than about 700 nm. The partially transmitted light apparently is scattered back to the image plane in a way that requires a complex compensation procedure (de la Cruz Rodriguez 2010; de la Cruz Rodríguez et al. 2013) and that involves the determination of a PSF that extends to a radius of at least 6″ from its origin. The backscatter evidently reduces the contrast of the images and although the present procedure for its compensation is successful in removing artifacts that are obvious with conventional flat-fielding, it does not yet seem clear just how accurate the backscatter compensation procedure is. We can at present not exclude that the deviations from theoretical predictions seen for the 853 nm data are associated with this compensation, although we do not have any direct evidence to suggest that this is the case.

Another limitation in our analysis is our assumptions made about the performance of the AO system. Although its efficiency can be described in terms of an effective number of corrected modes, as proposed by Roddier (1998), this is not sufficient for explaining the detailed shape of the PSF. It seems highly likely that many modes provide partial compensation only and that this is the main reason for the limited performance of the system. To provide more quantitative information about the performance of the AO system, we need log files with more information such as the AO telemetry proposed by Veran et al. (1997) and implemented for solar telescopes by Marino (2007), Marino & Rimmele (2010), and Wöger (2010), and also discussed by Rimmele & Marino (2011). We also need to verify that the time averaging interval of 20–30 s, used to provide a reference for the differential image motion measurements, is long enough to not lead to overestimates of r0.

With these caveats in mind, we tentatively conclude that the variation of granulation contrast with r0 can be reasonably well explained with an AO system that has around 40−45% efficiency if we assume an additional wavefront error of about 48 nm RMS (1/13 wave RMS at 630 nm). The origin of that wavefront error is not clear. There is compelling evidence from images including both granulation and a dark sunspot that the PSF cannot have extended wings of the strength needed to explain the reduced granulation contrast because that would make the corrected umbra intensity negative. This suggests that the 48 nm wavefront error comes from small-scale fixed aberrations in the optics of SST and its reimaging systems. However, that interpretation is not without problems. The manufacturer of the main optical system, Opteon Oy, claims small-scale wavefront errors of the two 1.4 m flats to be in the range 8–9 nm RMS each, when used at 45° angle of incidence, and that of the 1-meter lens about 10 nm RMS (Scharmer et al. 2003a). Adding up the corresponding variances delivers a total wavefront error of about 16 nm RMS. Similarly, the small-scale wavefront errors of the Schupmann corrector (lens plus mirror) were found to be about 8 nm RMS but since the lens is used in double pass, that wavefront error could possibly double. All in all, the primary optical system of SST should provide at most half of the required 48 nm RMS wavefront error.

Another possible explanation is that there are noncommon optical path differences between CRISP and CHROMIS, on the one hand, and the AO WFS, on the other hand. The WFS is fed by a beam splitter cube that deflects 10% of the light to CRISP downward, and then this light is deflected horizontally by a right angle prism5. The beam splitter cube is located approximately 30 cm from the focal plane in an F/46 beam, so the optical footprint on the beam splitter is about 6.5 mm for any point in the focal plane. If there are significant aberrations in the reflected beam of the beam splitter and/or right angle prism within a circle with this diameter, then this could explain the missing 48 nm wavefront error. Whether any of the above explanations, or a combination of the two, can explain the “missing” wavefront error, remains an open question that deserves further attention. On the other hand, we have no indication that, for example, the beam splitter cube that divides light between the narrowband and wideband systems of CRISP introduces significant aberration differences between the two beams.

What seems clear, however, is the very significant improvement in image quality associated with the replacement of the previous 37-electrode adaptive mirror (Scharmer et al. 2003b) with the new 85-electrode adaptive mirror from CILAS (Scharmer et al., in prep.) and the new tip-tilt mirror from ICOS. Previous measurements of granulation contrast correlated with r0 measurements from a wide-field WFS (Scharmer & van Werkhoven 2010) showed “raw” values in the range 6.5% at 630 nm to 7.5% at 538 nm close to disk center (Scharmer et al. 2010), compared to the raw values reported on in Table 2 in this work of 9.2% at 630 nm and 10.5–10.9% at 525 nm. This improvement is consistent with the evaluation of aberrations in the former AO and reimaging system of SST using phase diversity methods, which provided clear evidence for wavefront errors on the order of 42 nm RMS (Löfdahl & Scharmer 2012). The significantly increased granulation contrast observed after replacing the tip-tilt and adaptive mirrors with optics of much higher quality gives a clear indication of the importance of minimizing small-scale wavefront errors in the optics.

We also note that the presently observed granulation contrasts compare favorably with those of any other solar telescope, whether in space, on a balloon, or from the ground. For example, SOT on Hinode delivered a contrast of about 7% at 630 nm (Danilovic et al. 2008) and IMaX on Sunrise I a raw contrast in the range 8–8.5% at 525 nm (Martínez Pillet et al. 2011). The latter relatively low contrast was attributed to a combination of wavefront errors in the telescope and instrumentation that was estimated at λ/5.4 RMS when in operation. In the case of Hinode, the reduction in contrast is primarily from the relatively large central obscuration and spider (Danilovic et al. 2008), whereas aberrations in the optical systems are small.

4. Conclusions

We described the SST primary imaging and AO systems and the telecentric dual Fabry–Pérot systems CRISP and CHROMIS. We attempted an evaluation of the resulting image quality through the CRISP narrowband and wideband reimaging systems and the wideband reimaging system of CHROMIS (at the time of recording the present data, the narrowband system of CHROMIS had not yet been installed). We used measurements of differential image motion between four of the 85 subapertures of the SST AO system to measure the seeing quality, as quantified by the Fried parameter r0, using a small FOV of only 4″ × 4″ to capture the contributions from high-altitude seeing as well. These measurements are made during overlapping 2 s periods such that we obtain one r0 measurement per second and capture the intermittency of the daytime seeing. Simultaneously, we recorded science images through the CRISP and CHROMIS wideband systems and processed these data in bursts of images that correspond to the time intervals of the seeing measurements. The empirical relations found between r0 and the granulation contrast are discussed in terms of the expected shape of the PSF and the Strehl value of residual aberrations after partial compensation of the seeing by the AO system. We also compared the measured granulation contrasts to the values expected from numerical simulations.

Our WFS measurements of the seeing quality made with a very small FOV of only 4″ × 4″ shows excellent correlation with measured granulation contrasts and, as far as we can tell, takes into account contributions from high-altitude seeing in a reasonable manner. In our opinion, a larger FOV than this is not useful for assessing seeing and data quality.

The observed images demonstrate the outstanding image quality through the Fabry–Pérot based system CRISP, which when compared to simultaneously obtained images through its wideband system fails to reveal any indication of image degradation by the two etalons. We attribute this to the telecentric design of CRISP, which produces very small optical footprints on the lenses and etalons for each field point. We also note that the telecentric design together with a slight tilt of the low-resolution etalon, allows efficient elimination of stray light from ghost images by means of a pupil stop on the exit side of CRISP.

We find, as expected, that the measured granulation contrast varies linearly with, but is not simply proportional to, the inferred Strehl value. Reasonable agreement between the measurements and numerical calculations can be obtained if we assume the SST AO system to have an efficiency of about 40–50%. However, to explain the discrepancy of the extrapolated seeing-free granulation contrast compared with values obtained from 3D MHD simulations, we need to introduce an additional (seeing unrelated) wavefront error of about 48 nm RMS. The origin of this may be from small-scale aberrations in the SST optics, or from noise or other shortcomings in the WFS, as discussed by Rimmele & Marino (2011) and in the previous sections.

Our measurements suggest that even for a solar telescope of a relatively simple optical design with only a few high-quality optical surfaces, there are limitations in image quality that are not set by seeing in the Earth’s atmosphere, but rather in the optics or the AO WFS. We conjecture that for more complex solar telescopes this may be a serious problem and that the attainable image quality may well be limited by the number or quality of the optical surfaces. In this case “the sky is not the limit”, but rather the telescope itself. Thoroughly understanding these limitations is of crucial importance for the design and manufacture of future solar telescopes, such as the European Solar Telescope (e.g., Jurčák et al. 2019).

1

This also means that the observed granulation contrast with any space- or ground-based solar telescope can be used to constrain the PSF of that telescope (Scharmer et al. 2011).

3

The algorithms used are the following: the variance of image motion in the x-direction is obtained as σ x 2 =〈 (x− x 0 ) 2 〉 $ \sigma _x^2 = \langle {(x - {x_0})^2}\rangle $, where the average is taken over 2 s and x0 is calculated iteratively as x 0 (n) =c x 0 (n−1) +(1−c)x $ {x_0}^{(n)} = c{x_0}^{(n - 1)} + (1 - c)x $. The constant c equals 1 − 1/(20f), where f is the update frequency, which is close to 2 kHz, so c ≈ 0.999975. If x changes step-wise, then x0 reaches 63% of that step after 20 s, 78% after 30 s and 95% after 1 min.

4

The formula given by Roddier (1998) includes the inconsequential piston mode as N = 1, whereas we refer to N = 1 and N = 2 as the tip-tilt modes.

5

The reason for this arrangement is to cancel out the polarizing effect of the beam splitter that deflects 10% of the light horizontally to the CRISP wideband system.

Acknowledgments

The Swedish 1-m Solar Telescope is operated on the island of La Palma by the Institute for Solar Physics of Stockholm University in the Spanish Observatorio del Roque de los Muchachos of the Instituto de Astrofísica de Canarias. The Institute for Solar Physics is supported by a grant for research infrastructures of national importance from the Swedish Research Council (registration number 2017-00625). This work was supported by the Swedish Research Council, grant number 621-2014-5738. JdlCR is supported by grants from the Swedish Research Council (2015-03994) and the Swedish National Space Board (128/15). This project has received funding from the European Union’s Horizon 2020 research and innovation programme under grant agreement No 824135. The anonymous referee is thanked for valuable suggestions.

References

  1. Auer, L. 2003, in Stellar Atmosphere Modeling, eds. I. Hubeny, D. Mihalas, & K. Werner, ASP Conf. Ser., 288, 3 [NASA ADS] [Google Scholar]
  2. Barklem, P. S., & O’Mara, B. J. 1998, MNRAS, 300, 863 [NASA ADS] [CrossRef] [Google Scholar]
  3. Barklem, P. S., Piskunov, N., & O’Mara, B. J. 2000, A&AS, 142, 467 [NASA ADS] [CrossRef] [EDP Sciences] [MathSciNet] [PubMed] [Google Scholar]
  4. Beckers, J. M., & Parnell, R. L. 1969, Sol. Phys., 9, 39 [NASA ADS] [CrossRef] [Google Scholar]
  5. Britton, M. C. 2006, PASP, 118, 885 [NASA ADS] [CrossRef] [Google Scholar]
  6. Conan, J. M., Madec, P. Y., & Rousset, G. 1992, in Progress in Telescope and Instrumentation Technologies, ed. M. H. Ulrich, ESO Conference and Workshop Proceedings, 42, 475 [NASA ADS] [Google Scholar]
  7. Danilovic, S., Gandorfer, A., Lagg, A., et al. 2008, A&A, 484, L17 [NASA ADS] [CrossRef] [EDP Sciences] [Google Scholar]
  8. de la Cruz Rodriguez, J. 2010, PhD Thesis, Stockholm University [Google Scholar]
  9. de la Cruz Rodríguez, J., & Piskunov, N. 2013, ApJ, 764, 33 [NASA ADS] [CrossRef] [Google Scholar]
  10. de la Cruz Rodríguez, J., & van Noort, M. 2017, Space Sci. Rev., 210, 109 [NASA ADS] [CrossRef] [Google Scholar]
  11. de la Cruz Rodríguez, J., Rouppe van der Voort, L., Socas-Navarro, H., & van Noort, M. 2013, A&A, 556, A115 [NASA ADS] [CrossRef] [EDP Sciences] [Google Scholar]
  12. de la Cruz Rodríguez, J., Leenaarts, J., & Asensio Ramos, A. 2016, ApJ, 830, L30 [NASA ADS] [CrossRef] [Google Scholar]
  13. de la Cruz Rodríguez, J., Leenaarts, J., Danilovic, S., & Uitenbroek, H. 2019, A&A, 623, A74 [NASA ADS] [CrossRef] [EDP Sciences] [Google Scholar]
  14. del Toro Iniesta, J. C., & Ruiz Cobo, B. 2016, Sol. Phys., 13, 4 [Google Scholar]
  15. Hardy, J. W. 1998, Adaptive Optics for Astronomical Telescopes (Oxford University Press), 198 [Google Scholar]
  16. Jurčák, J., Collados, M., Leenaarts, J., van Noort, M., & Schlichenmaier, R. 2019, Adv. Space Res., 63, 1389 [Google Scholar]
  17. Levy, M. 1971, A&A, 14, 15 [NASA ADS] [Google Scholar]
  18. Lites, B. W., Elmore, D. F., & Streander, K. V. 2001, in Advanced Solar Polarimetry – Theory, Observation, and Instrumentation, ed. M. Sigwarth, ASP Conf. Ser., 236, 33 [NASA ADS] [Google Scholar]
  19. Löfdahl, M. G. 2002, in Image Reconstruction from Incomplete Data II, eds. P. J. Bones, M. A. Fiddy, & R. P. Millane, Proc. SPIE, 4792, 146 [NASA ADS] [CrossRef] [Google Scholar]
  20. Löfdahl, M. G. 2010, A&A, 524, A90 [NASA ADS] [CrossRef] [EDP Sciences] [Google Scholar]
  21. Löfdahl, M. G. 2016, A&A, 585, A140 [NASA ADS] [CrossRef] [EDP Sciences] [Google Scholar]
  22. Löfdahl, M. G., & Scharmer, G. B. 1994, A&AS, 107, 243 [NASA ADS] [Google Scholar]
  23. Löfdahl, M. G., & Scharmer, G. B. 2012, A&A, 537, A80 [NASA ADS] [CrossRef] [EDP Sciences] [Google Scholar]
  24. Marino, J. 2007, PhD Thesis, New Jersey Institute of Technology [Google Scholar]
  25. Marino, J., & Rimmele, T. 2010, Appl. Opt., 49, G95 [CrossRef] [Google Scholar]
  26. Martínez Pillet, V., Del Toro Iniesta, J. C., Álvarez-Herrero, A., et al. 2011, Sol. Phys., 268, 57 [NASA ADS] [CrossRef] [Google Scholar]
  27. Mathew, S. K., Zakharov, V., & Solanki, S. K. 2009, A&A, 501, L19 [NASA ADS] [CrossRef] [EDP Sciences] [Google Scholar]
  28. Piskunov, N., & Valenti, J. A. 2017, A&A, 597, A16 [NASA ADS] [CrossRef] [EDP Sciences] [Google Scholar]
  29. Piskunov, N. E., Kupka, F., Ryabchikova, T. A., Weiss, W. W., & Jeffery, C. S. 1995, A&AS, 112, 525 [NASA ADS] [Google Scholar]
  30. Rimmele, T. R., & Marino, J. 2011, Sol. Phys., 8, 2 [Google Scholar]
  31. Roddier, F. 1998, PASP, 110, 837 [NASA ADS] [CrossRef] [Google Scholar]
  32. Ryabchikova, T., Piskunov, N., Kurucz, R. L., et al. 2015, Phys. Scr., 90, 054005 [NASA ADS] [CrossRef] [Google Scholar]
  33. Sánchez Cuberes, M., Bonet, J. A., Vázquez, M., & Wittmann, A. D. 2000, ApJ, 538, 940 [NASA ADS] [CrossRef] [Google Scholar]
  34. Sarazin, M., & Roddier, F. 1990, A&A, 227, 294 [NASA ADS] [Google Scholar]
  35. Scharmer, G. B. 2006, A&A, 447, 1111 [NASA ADS] [CrossRef] [EDP Sciences] [Google Scholar]
  36. Scharmer, G. B., & van Werkhoven, T. I. M. 2010, A&A, 513, A25 [NASA ADS] [CrossRef] [EDP Sciences] [Google Scholar]
  37. Scharmer, G. B., Bjelksjö, K., Korhonen, T. K., Lindberg, B., & Pettersson, B. 2003a, in Innovative Telescopes and Instrumentation for Solar Astrophysics, eds. S. Keil, & S. Avakyan, Proc. SPIE, 4853, 341 [NASA ADS] [CrossRef] [Google Scholar]
  38. Scharmer, G. B., Dettori, P. M., Löfdahl, M. G., & Shand, M. 2003b, in Proc. SPIE, eds. S. L. Keil, & S. V. Avakyan, 4853, 370 [Google Scholar]
  39. Scharmer, G. B., Löfdahl, M. G., van Werkhoven, T. I. M., & de la Cruz Rodríguez, J. 2010, A&A, 521, A68 [NASA ADS] [CrossRef] [EDP Sciences] [Google Scholar]
  40. Scharmer, G. B., Henriques, V. M. J., Kiselman, D., & de la Cruz Rodríguez, J. 2011, Science, 333, 316 [NASA ADS] [CrossRef] [Google Scholar]
  41. Stein, R. F., & Nordlund, A. 1998, ApJ, 499, 914 [Google Scholar]
  42. Tsuneta, S., Ichimoto, K., Katsukawa, Y., et al. 2008, Sol. Phys., 249, 167 [NASA ADS] [CrossRef] [Google Scholar]
  43. van Noort, M., Rouppe van der Voort, L., & Löfdahl, M. G. 2005, Sol. Phys., 228, 191 [NASA ADS] [CrossRef] [Google Scholar]
  44. Veran, J.-P., Rigaut, F., Maitre, H., & Rouan, D. 1997, J. Opt. Soc. Am. A, 14, 3057 [NASA ADS] [CrossRef] [Google Scholar]
  45. Wedemeyer-Böhm, S. 2008, A&A, 487, 399 [NASA ADS] [CrossRef] [EDP Sciences] [Google Scholar]
  46. Wedemeyer-Böhm, S., & Rouppe van der Voort, L. 2009, A&A, 503, 225 [NASA ADS] [CrossRef] [EDP Sciences] [Google Scholar]
  47. Wöger, F. 2010, Appl. Opt., 49, 1818 [NASA ADS] [CrossRef] [PubMed] [Google Scholar]

All Tables

Table 1.

Properties of data collected.

In the text
Table 2.

Observed granulation contrasts with SST/CRISP.

In the text

All Figures

thumbnail Fig. 1.

Layout of the present 85-electrode monomorph DM and 85 subaperture WFS of the present AO system of the SST. The gray or white radial/azimuthal structures correspond to the electrodes of the DM and the hexagonal structures correspond to the 85 lenslets. The four lenslets indicated with small red circles correspond to the subapertures used for seeing measurements. The large red circle corresponds to the pupil diameter. For details, see text.
In the text
thumbnail Fig. 2.

Yellow curve, which is saturated in some peaks, shows the time variation of the SST seeing quality (Fried’s parameter r0) as measured with the 12 . ″ $ {{\overset{\prime\prime}{.}}} $0 × 12 . ″ $ {{\overset{\prime\prime}{.}}} $0 WFS of the SST AO system, and the black curve shows the corresponding variations measured with a much smaller FOV of 4 . ″ $ {{\overset{\prime\prime}{.}}} $0 × 4 . ″ $ {{\overset{\prime\prime}{.}}} $0. The yellow curve corresponds roughly to ground-layer seeing and the black curve to a combination of ground- and high-altitude seeing (see text). We note the strong intermittency that requires high time resolution. The data were recorded on 13 May 2016.
In the text
thumbnail Fig. 3.

Layout of the present optical setup at SST, including the AO and WFS, and the CRISP and CHROMIS narrowband and wideband reimaging systems. At the time of the tests, CHROMIS was not yet installed and its wideband reimaging together with the prefilters of CHROMIS was used at the present location of CHROMIS. For details, see text.
In the text
thumbnail Fig. 4.

Top 8 panels: resulting WB (bottom 4 panels) and CRISP NB (top 4 panels) images after adding up the 74 observed images during 2 s and only compensating for relative image motion (tip and tilt) between the individual exposures and the PSF of the diffraction limited telescope. Bottom 8 panels: resulting image of the same observed images but after applying MFBD image reconstruction to compensate for the largest 100 KL modes. The wavelengths are (left to right) 525 nm, 557 nm, 630 nm, and 853 nm.
In the text
thumbnail Fig. 5.

Top 3 panels: resulting CHROMIS WB images after adding up the 100 observed images during 2 s and only compensating for relative image motion (tip and tilt) between the individual exposures. Bottom 3 panels: resulting images of the same observed images but after applying MFBD image reconstruction to compensate for the largest 100 KL modes. The wavelengths are (left to right) 395 nm, 400 nm, and 485 nm.
In the text
thumbnail Fig. 6.

RMS contrast of granulation measured from SST images recorded at different wavelengths and in different seeing conditions characterized by the Fried r0 parameter. Both r0 and the granulation contrast have been averaged over 2 s. The blue dots refer to RMS contrasts of images recorded with the AO system and that are compensated only for the diffraction limited point spread function, the red dots to RMS contrasts of images further compensated for aberrations with the multi-frame blind deconvolution method (Löfdahl 2002), and the horizontal dotted lines show the contrasts of 3D MHD simulations. Images were recorded with wide-band (WB) filters on both the “red” (CRISP) and “blue” (CHROMIS) beams. Note that the plot limits for r0 vary from one plot to another and that data for r0 values smaller than 0.04 m, shown as vertical dotted lines, are excluded. Two of the panels in the lowermost row show a comparison between RMS contrast obtained from images recorded simultaneously through wideband pre-filters (labeled WB) and the corresponding narrowband (NB) CRISP spectropolarimeter filter system on the “red” beam of the SST (see text). The significantly higher contrast of the NB beam at 853.6 nm is because of the strong influence of the Ca 854.2 nm line within the passband of the WB filter.
In the text
thumbnail Fig. 7.

RMS contrast of granulation images recorded in different seeing conditions characterized by the calculated Strehl value based on the residual wavefront RMS from r0 and assuming that the AO system provides perfect correction of 81 modes. The blue dots refer to RMS contrasts of images that are compensated only for the diffraction limited PSF, and correspond to the blue dots in Fig. 6. The green dots correspond to the same contrast measurements but with the Strehl value calculated on the basis of an additional wavefront variance corresponding to 1/13 wave RMS at 630 nm, and scaled at other wavelengths as the inverse of the wavelength. The straight lines have been fitted to data points for which the Strehl is larger than 0.15.
In the text
thumbnail Fig. 8.

Same as for Fig. 7 but assuming that the AO system provides perfect correction of 36 modes.
In the text
thumbnail Fig. 9.

Top 9 panels: variation of the shape of the PSF with the Strehl ratio after perfect compensation of the first 2 (tip-tilt only), 18, 36, and 81 aberration modes. Lowermost 3 panels: variation with Strehl of the diameter of the PSF containing 80% of the encircled energy for the same number of compensated modes.
In the text
thumbnail Fig. 10.

Theoretically calculated RMS granulation contrast for different Strehl values, based on residual wavefront errors after perfect low-order modal compensation of seeing degraded images recorded with a 1-m telescope. When approximately 50 modes or more are compensated, the relation between the Strehl ratio and the granulation contrast is almost linear, and independent of the number of modes compensated. This is because the wings of the PSF are then sufficiently wide (see Fig. 9) that more than one granule is included under the PSF. With such wide wings, making the PSF wider does not increase the amount of stray light. At short wavelengths, a higher number of compensated modes than at long wavelengths is required for this simple relation between Strehl and granulation contrast to be true.
In the text

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