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6.4.1.
Star testing telescopes
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6.6. Effects of aberrations: MTF
► 6.5. Strehl ratioOne of the most frequently used optical terms in both, professional and amateur circles is the Strehl ratio. It is the simplest meaningful way of expressing the effect of wavefront aberrations on image quality. By definition, Strehl ratio  introduced by the German physicist, mathematician and astronomer Dr. Karl Strehl at the end of 19th century  is the ratio of peak diffraction intensities of an aberrated vs. perfect wavefront. The ratio indicates the level of image quality in the presence of wavefront aberrations; often times, it is used to define the maximum acceptable level of wavefront aberration for general observing  socalled diffractionlimited level  conventionally set at 0.80 Strehl. Similar type of indicator is the Struve ratio, which expresses peak diffraction intensity of aberrated vs, aberrationfree line spread function (LSF). It requires slightly tighter 0.80 ratio level requirement for primary coma (0.58 vs. 0.63 wave PV), more relaxed for spherical aberration (0.27 vs. 0.25) and defocus (0.29 vs. 0.26) than the Strehl ratio (the tolerance for astigmatism is nearly identical). However, it has far less universal appeal than the Strehl ratio, expressing vital property of the single most important optical indicator, the PSF, building stone of nearly all intensity distribution forms, including the LSF. Wavefront deviations from perfect spherical are directly related to the size of phase errors at all points of wave interference that form diffraction pattern. In other words, it is a nominal wavefront deviation from spherical that determines the change in pattern's intensity distribution. However, it is not the peaktovalley nominal aberration, which only specifies the peak of deviation, and tells nothing about its extent over the wavefront area. It is the rootmeansquare, or RMS wavefront error, which expresses the deviation averaged over the entire wavefront. This average wavefront deviation determines the peak intensity of diffraction pattern and, hence, numerical value of the Strehl ratio (note that the RMS error itself is accurately representing the magnitude of wavefront deviation only when it is affecting relatively large wavefront area, which is generally the case with the conic surface aberrations). For relatively small errors  roughly 0.15 wave RMS, and smaller  the RMS wavefront error, and the resulting Strehl ratio, accurately reflect the effect of overall change in energy distribution, regardless of the type of aberration. With larger errors, the correlation between the RMS error and the Strehl vanishes: larger RMS error can produce higher PSF peak intensity, and better image quality than the lower errors. Mid astigmatic focus, for instance, has identical PSF peak intensity at 2 and 3 waves PV wavefront error, despite the latter having 50% higher RMS/PV. Similar RMStoStrehl inconsistency above 0.15 wave RMS exist for spherical aberration, and aberrations in general. As a general rule for aberrations below 0.15 wave RMS, the relative drop in peak diffraction intensity indicates how much of the energy is lost, relatively, from the Airy disc. For instance, 0.90 Strehl indicates about 10% lower energy within the Airy disc. But the exceptions are possible, and generally larger in magnitude with larger error levels. For instance, the drop in peak diffraction intensity is nearly identical at 0.0745 wave RMS and 0.15 RMS wavefront error  20% and 59% respectively  for all three, spherical aberration, coma and astigmatism. At the same time, the accompanying drop in the energy encircled within the Airy disc is 20% and 11% at 0.745 wave RMS, and 61%, 56% and 38% at 0.15 wave RMS, for spherical aberration and coma vs. astigmatism, respectively. However both, nominal Strehl and overall contrast level remain nearly identical for all, due to the energy transferred by astigmatism effectively transforming central disc into a larger, crosslike form, reducing contrast level over the higher range of MTF frequencies more, and less than the other two in the lower frequency range. While the actual Strehl calculation requires complex math, simple empirical expression by Mahajan gives a very close approximation of the Strehl ratio in terms of the RMS wavefront error: (56) where e is the natural logarithm base (2.72, rounded to two decimals), and ω is usually the RMS wavefront error in units of the wavelength. Note that use of the RMS wavefront error can yield inaccurate result; the actual Strehl value  and the original form of approximation  are phase dependant, thus determined by phase variance φ2 and, more directly, by the phase analog to the OPDbased RMS wavefront error, φ, with φ2=(2πφ)2. The approximation is accurate to a couple of percent for RMS errors of ~1/10 wave, with the difference diminishing for smaller errors. The difference vs. exact Strehl value gradually increases with the RMS error, but even at S~0.3 it still does not exceed 10%. It overestimates true Strehl for balanced primary aberrations, and underestimates it for classical aberrations. This approximation is also known as "extended Maréchal's approximation", as opposed to the original Maréchal's approximation, S~(10.5φ2)2~[10.5(2πφ)2]2 which, for φ~ω, can be written in terms of the RMS wavefront error as S~[12(πω)2]2. For small RMS errors (~1/15 wave or less), a simpler approximation, given by S~1(2πω)2, or S~139.5ω2, is also accurate; however, it becomes increasingly inaccurate with larger RMS errors  at 1/10 wave it already underestimates the true Strehl by more than 10%, and drops to zero at ~0.16 wave RMS (FIG. 97). For errors larger than ~1/15 wave RMS, and smaller than 1/5 wave RMS, a simple empirical approximation S~110ω1.5 gives slightly less accurate result than Mahajan's approximation for RMS<0.2 (within 2%), but has better overall accuracy than the two alternative approximations.
FIGURE
97:
Strehl ratio as a function of RMS wavefront error. LEFT: Plots for three ratio approximations and the
true Strehl value for primary spherical aberration at the best focus
(balanced spherical; identical to the Siedel  i.e. Gaussian focus' 
spherical aberration) in unobstructed aperture. Strehl ratio
approximations, from the top down, Mahajan's (also known
as "extended Maréchal approximation"), Maréchal's, and simplified Maréchal's, the latter with the 4th power term in the expansion neglected. The lower two approximations are accurate for RMS errors smaller than
~0.07, while Mahajan's remains reasonably close to the true ratio value
even for RMS errors in excess of ~0.2, for classical and balanced (best
focus) aberrations in general. It remains close
to the true Strehl for spherical aberration for wavefront errors in excess of 0.25 wave RMS.
RIGHT: Change in the Strehl ratio due to central
obstruction, for balanced spherical, defocus, coma and astigmatism, for
selected central obstruction sizes. It is the consequence of the
change in the RMS
wavefront error due to obstruction of a portion of the wavefront,
with the RMS of the annulus varying somewhat with the aberration type.
With balanced spherical and defocus, Strehl ratio of the annulus
continually increases with the size of central obstruction in a similar
way, only the magnitude of increase being more than doubled for the
former. With coma, the change is negligible except for obstructions of
around 0.5D and larger, for which the Strehl increases by nearly 10%, or
more (it decreases up to a few percent for smaller obstructions). With
astigmatism, the Strehl continually decreases, reaching 30% decrease at
0.5D obstruction size. The Strehl and RMS error are, of course, only one
side of the story. In addition to the effect of optical path difference
due to wavefront deviation from perfect sphere, wave interference at the
focus is also affected by missing wave contributions due to wavefront
obstruction. The PSF peak here is a product of the Strehl and PSF peak
degradation due to central obstruction, given by
(1ο2)2,
where o is the relative linear obstruction size in units of aperture. Conventional "diffractionlimited" aberration level is set at the Strehl ratio of 0.80 or, in terms of the RMS wavefront error, 0.0745 (or 1/√180), regardless of the type of aberration. This only concerns wavefront quality; presence of other factors negatively affecting image quality, such as aperture obstruction, or chromatism, would result in further deterioration in quality of the diffraction image. Thus achieving "diffractionlimited" level in such circumstances requires higher wavefront quality, according to the magnitude of additional error. The RMS wavefront error in terms of Strehl ratio is, from Eq. 56, closely approximated as ω~0.24√logS. For the range of aberration mentioned, drop in the peak intensity expressed by the Strehl ratio also indicates the relative amount of energy transferred from the central disc to the ring area of the diffraction pattern, given as (1S). Moreover, this relative number also indicates the average contrast loss over the range of resolvable frequencies. Regardless of the aberration type, these three basic properties of an aberrated pattern  the relative drop in central intensity, relative amount of energy transferred to the rings area, and averaged relative contrast loss  are practically identical for a given RMS wavefront error. While the Strehl ratio furnishes very useful quantitative information about the effect of an aberrated wavefront, it is of general nature. It doesn't give specific indications on how the contrast varies for details of different angular size, nor how it affects the resolution limit. Also, there are factors affecting intensity distribution within diffraction pattern  such is pupil obstruction or apodization  not originating from wavefront aberrations. Hence, the Strehl figure doesn't include such effects. The effects of change in the pupil transmission factor due to obstructions of various forms still can be expressed through the PSF, as a single number comparable to the Strehl ratio. Potentially more versatile indicator of the effect of aberrations is encircled energy (FIG. 98). It shows what portion of the energy is contained within a circle of given radius, centered at the intensity peak of the diffraction pattern. If specified for more than a single radius, it gives more detailed picture of intensity distribution. FIGURE 98: Illustration to the left shows Point Spread Function (PSF)  with its peak intensity determining the value of Strehl ratio  and encircled energy (EE) of a perfect (aberrationfree) and aberrated aperture (0.25 wave PV of primary spherical aberration), as a function of diffraction pattern radius, given in units of λF. In the presence of aberrations, the energy is spread wider, thus the energy encircled within a given pattern radius diminishes. Encircled energy figure can be given not only for the Airy disc, but also for any radius of the diffraction pattern. It can indicate possible change in size of the central disc, or furnish some other information of particular interest. An additional EE value for, say, 2.5λF radius, would indicate how much of the energy lost from the disc ended up in the first bright ring. It gets more complicated with asymmetrical aberrations, since the amount of energy at any radius can vary significantly with the pupil angle. Showing this aspect of energy distribution would require several EE figures for each of various radial angles, or some kind of a graphical (contour) EE presentation  far from clear simplicity of the Strehl. However, for more specific information on the effect of wavefront aberrations on image quality, as well as the effect of other factors affecting wave interference in the focal zone, the calculation has to expand from the characteristics of a single pointimage (PSF), to those of the images of standardized extended objects, covering the entire range of resolution. The needed tool is found in the optical transfer function (OTF), a Fourier transform of the PSF. Strehl and MTF, Hopkins ratio Being based on the system's PSF, Strehl ratio is directly related to its MTF, with the PSF being the inverse Fourier transform of the MTF. In effect, the Strehl represents the MTF averaged over all frequencies  in other words, it represents the averaged MTF contrast transfer. Thus the quantity 1S represents the averaged MTF contrast loss due to the aberrations. General consensus for general observing is that contrast loss of up to 5% is inconsequential, and that loss of up to 20% does not significantly degrade performance. The problem with such generalization is that: (1) contrast loss for most aberrations is not uniform over the range of MTF frequencies, and (2) the effect of contrast loss depend primarily on the inherent object contrast, and it varies widely from one object type to another. Hence 20% loss may not significantly degrade performance with some objects and details  possibly majority of them  but it will with some others, generally those with the lowest inherent contrast. That puts the acceptable contrast loss  depending of the object of observation  anywhere between 20%, or somewhat more, to 5%, or somewhat less. As for the contrast loss variation over MTF frequencies for a given Strehl (i.e. aberration level), it is evident on the typical MTF. Even at relatively low aberration level, resulting in 0.80 Strehl, it can cause potentially noticeable differences in performance with specific object types. For clarity, it is presented as contrast transfer vs. that in a perfect aperture normalized to 1 for every frequency, i.e. as the MTF relative contrast (FIG. 99; plots generated by Aperture from R. Suiter).
FIGURE 99: MTF contrast variation for 0.80 Strehl. Contrast is normalized to 1 for contrast transfer in a perfect aperture at every frequency (i.e. the contrast transfer of a perfect aperture coincides with the top horizontal scale). All four wavefront deformations result in 0.80 Strehl, but the differences in their contrast transfer over local frequencies  with the Strehl representing the average contrast over all frequencies, the local contrast transfer is effectively a local Strehl  can be very significant. At the resolution limit for planetary details, for example, where less than 5% of contrast differential can produce detectable difference in performance, the "local Strehl" for the four 0.80 Strehl deformations ranges from 0.71 for defocus, to 0.82 for spherical aberration and turned edge. Even with the all four aberrations being at the "diffraction limited" level, the differences in the contrast transfer are not negligible, and can be substantial. The worst effect has turned edge, which underperforms at both ends of the frequency range. At the lowfrequency end, for details of about 10 Airy disc diameters, and larger (since the cutoff frequency is 2.5 times smaller than Airy disc diameter, frequency equaling the Airy disc diameter is 0.4, and 0.04 is ten times larger), it quickly loses nearly 10% of the contrast. While it is still a relatively small loss, generally speaking, it indicates wide spread of energy that can brighten background, and soften  even wash off entirely  faint objects in proximity of bright objects. On the highfrequency end, contrast with turned edge begins its dive to zero as the detail size goes under half the Airy disc diameter, hitting zero at some 96% of the resolution limit. Needles to say, it will noticeably affect not only performance in splitting unequal doubles, of resolving critical lunar details, but also the resolution of nearequal doubles. A look at this relative contrast transfer variation over the range of MTF frequencies indicates that the contrast drop tends to be smaller toward either low or high frequency end, and larger over mid frequencies. When that is the case, the aberration tolerance for such subrange widens. Hopkins found specific aberration tolerances producing 0.8 Hopkins ratio  the contrast drop of 20%, analogous to the Strehl ratio  or better, for MTF frequencies equal to, or lower than 0.1. As shown at left (peak aberration coefficient as a function of spatial frequency ν), the tolerances are significantly larger than in the conventional treatment of aberrations, placing the lower limit at 0.80 Strehl; consequently, their corresponding conventional Strehl values are significantly below 0.80, for which the coefficient value is 1, 0.42, 0.37 and 0.26 for primary spherical aberration, coma, astigmatism and defocus, respectively. Note that the coefficient equals the actual PV wavefront error only for defocus. For spherical aberration, the aberration minimum for Hopkins ratio is at a point defocused by DS=(1.332.2ν+2.8ν2)S, generally more defocused than for the point of minimum wavefront deviation (DS=S), where the PV error equals S/4. This is the consequence of the shift of PSF peak away from the minimum deviation focus as the PV wavefront error exceeds 0.6 wave, i.e. for the peak aberration coefficient values of 2.5 and larger. With the Strehl at these aberration levels being up to several times higher for the PSF peak than for the Gaussian (paraxial) focus, i.e. S, the actual error is also significantly smaller, corresponding to roughly 23 times smaller PV wavefront error. Similarly, for large errors of astigmatism (about 1 wave PV, which is nominally equal the coefficient, and larger), the PSF peak also shifts away from the point of minimum wavefront deviation (mid focus, i.e. defocused from either tangential or sagittal focus by DA=A/2) toward sagittal and tangential focus (double peak), with the PSF at these peaks for larger aberration being up to several times higher than at the mid focus. For coma, the PV wavefront error at the tiltcorrected focus, the one with the minimum PV/RMS wavefront deviation, is 2/3 of the aberration coefficient, with the actual effect on MTF contrast ranging from the maximum for θ=0 (the blur length perpendicular to MTF bars), to the minimum for θ=π/2 (blur length parallel to the bars). The shift of PSF peak away from the focus of minimum wavefront deviation begins with the PV error nearing 0.8λ (i.e. 1.2 peak aberration coefficient). Hopkins ratio values should be in a close agreement with what MTF plots for these aberrations indicate as the level of aberration lowering contrast by 20%. at 0.1 frequency (left; for coma and astigmatism shown are tangential and sagittal orientation). An overall indicator of the magnitude of tolerance change with the frequency in the conventional PV wavefront error context is defocus (it does not have axial defocus  which would directly add or subtract from the aberration  nor tilt correction aspect). It shows that aberration tolerance increases inversely to the square of spatial frequency, from 1/2 wave PV at 0.1 frequency, to 1 wave at 0.05, 2 waves at 0.025, and so on.
Similar results, only in the direction of tightening the tolerance, can
be expected for the frequencies toward the high end (certain exception
being turned edge, which causes unacceptable contrast drop in this
subrange at the 0.80 conventional Strehl already). On the other hand,
the conventional Strehl that would secure no more than 20% contrast drop
in the mid range, where are the resolution threshold for bright
lowcontrast details, probably wouldn't be significantly below 0.90. For
ensuring no more than 5% contrast drop at mid frequencies, the
conventional Strehl would need to be above 0.97 (equivalent of 1/11 wave
PV of spherical aberration, or better). That, however, would strictly
apply only to very small apertures with nearperfect correction and
negligible induced errors (seeing, thermals, miscollimation...). At the
relatively large error levels, the finest details are washed out, and
those more coarse that remain are generally less affected by any given
contrast drop. ◄ 6.4.1. Star testing telescopes ▐ 6.6. Effects of aberrations: MTF ►
