12.2. Eyepiece aberrations I : spherical, coma, astigmatism, field curvature
While the primary goal of the telescope objective is to transform flat incoming wavefronts into spherical, the eyepiece needs to accomplish exactly the opposite. If the wavefront entering the eye is not flat, the point-image on the retina will suffer from wider diffraction energy spread, just as it does when the wavefront formed by the objective deviates from spherical. The extent to which it will affect perceived image quality depends on the detail size and properties, as well as image magnification.
If the front eyepiece focal plane doesn't coincide with the image plane of the objective, the wavefronts originating from object-image points will not exit the eyepiece flat, but curved (nearly spherical) and, as such, will be rejected by the eye in favor of the flat wavefronts coming from a point coinciding with the front focal plane of the eyepiece. The resulting error is defocus, easily correctable by moving the eyepiece to the proper position.
If the object-image and the front focal plane coincide, and wavefronts entering the eyepiece are spherical, it will emerge from it flat if ocular is aberration-free. In the real world, these exiting wavefronts will be aberrated to some extent, and the aberrations are spherical, coma, astigmatism and field curvature, chromatism, image distortion and spherical aberration of the exit pupil. Due to a number of lens elements, aberration expressions for eyepieces are lengthier than for the objective. Also, eyepiece specs are commonly not known. For those reasons, eyepiece aberrations will be considered only in general terms. Before addressing specific aberrations, here's illustration of the main parameters of eyepiece aberrations using a simple Ramsden-type configuration.
While even a single lens eyepiece can produce a good axial correction - due to the generally small cone footprint on eyepiece surface - its field correction is very poor, with the off-axis aberrations increasing exponentially due to the larger footprint combined with stronger radii. For instance, the eyepiece shown is a 10mm f.l. Ramsden with a pair of BK7 PCX lenses w/8.5mm radius of curvature, 6mm lens separation and 5.7mm from field lens to objective's image, as well as from eye lens to exit pupil. At /10, it is aplanatic, flat field with low astigmatism (0.11 wave RMS 15° off axis). If the eye lens is taken out, both, footprint and refraction (requiring r.o.c. reduction to 5.2mm) at the field lens - which already contributes nearly all off the astigmatism - have to increase, resulting in several times larger astigmatism severely limiting usable field.
In addition, multiple elements may allow for partial offsetting of aberrations between them, further reducing their final level. For that reason, eyepieces utilize two or more lenses. In the above example, the field lens "sees" the image formed by the objective as its object. Its aperture stop, however, is at the objective, because it is where the chief incident off axis ray intersects the axis. The eye lens "sees" the virtual image, formed by reverse extension of rays refracted by the field lens, as its object, and its aperture stop is at the point of intersection of the extended chief raj converging from the field lens and the axis. Thus, to both apply the lens aberration relations for displaced aperture stop. Obviously, in order for the eye lens to produce a collimated pencil, its object - the image formed by the field lens - has to be at the distance equaling its focal length.
In this particular example, specific aberrations are very low spherical aberration, less than 1/100 wave P-V, most of it at the second lens due to the wider footprint (cone aperture) on it. Coma is practically zero on both lenses, due to the specific combination of object distance and stop separation for each lens. If, for instance, the focal length of lens changes, it changes the object and aperture stop locations relative to the lens' focus point, and the aberration is reintroduced, rather quickly. Nearly all of the astigmatism is on the field lens, and it is of opposite sign to that on the eye lens. The astigmatism is of the opposite sign to the Petzval curvature, offsetting it to produce flat, mildly astigmatic image surface.
The wavefront error of spherical aberration in the eyepiece changes with the fourth power of the objective focal ratio. Thus, halving the objective F-number increases the wavefront error by a factor of 16. This makes eyepiece correction for spherical aberration critical. Even eyepieces superbly corrected at mid-to-small focal ratios, may become noticeably affected at large relative apertures. Since spherical aberration in eyepieces is also in proportion with the eyepiece focal length, longer f.l. units are more affected. However, they normally don't produce sufficient magnification to show the effect of aberration.
Degree of eyepiece correction for spherical aberration also varies with the eyepiece type and brand. Best corrected conventional 5mm f.l. eyepieces will have ~ 1/10 wave P-V of spherical aberration (under-correction) at /4, while those on the opposite end are closer to 1/4 wave P-V. This doesn't necessarily mean that the telescope performance will be noticeably affected. Most any objective contributes certain amount of spherical aberration of its own. If it is of the opposite sign to that of the eyepiece, the final result may still be admirable. But if the error is of the same sign for both, it will result in inferior performance. For instance, if the objective is 1/5 wave under-corrected, and the eyepiece 1/8 wave under-corrected, their cumulative error will be 1/3 wave P-V of under-correction. That is another example of the actual telescope aberration level being determined by the combined effect of both, objective and eyepiece.
Modern-type eyepieces employing Smyth lens (negative field lens) behave differently. In general, they tend to induce over-correction, which also may become significant at very fast focal ratios, especially when combined with the correction error of the objective that is of the same sign. The Nagler-type eyepiece (Type 1) presented in the Rutten-Venrooij's "Telescope Optics" raytraces to nearly 1 wave P-V of over-correction at /5. Since it is a 100mm f.l. unit, the error would drop to nearly 1/20 wave P-V with a 5mm f.l. unit at /5. At /4, it would be nearly 1/8 wave P-V. Should the objective be 1/6 wave P-V over-corrected at /4, the combined error would come to ~1/3.5 wave P-V of over-correction.
Off-axis aberrations are more pronounced in eyepieces, due to their large viewing angles. Coma is, in general, not significant in eyepieces due to it being usually minimized by design, and much lower than astigmatism, which cannot be reduced nearly as efficiently. The amount of coma wavefront error in a positive lens changes in inverse proportion to the square of the focal length, and in proportion to the third power of the cone width. In effect, for given field angle, it changes in proportion to the eyepiece focal length. It also changes in proportion to the third power of telescope focal ratio. Given eyepiece design, the 30mm f.l. unit will have three times the coma of the 10mm f.l. unit. Either will have eight times more of the coma wavefront error at /5, than at /10 telescope focal ratio.
As with the coma originating at the objective, eyepiece coma increases with the off-axis height in the image plane.
However, it is eyepiece astigmatism that usually dominates. It also depends on the lens focal length and the cone width, being inversely proportional to the eyepiece f.l. and in proportion to the square of the cone width. In effect, for given field angle it is, as coma, proportional to the eyepiece f.l. but, unlike coma, it changes in proportion to the square (not third power) of the telescope focal ratio (note that the geometric blur size changes in proportion to the focal ratio, but also with the square relative to the Airy disc). In other words, the wavefront error of astigmatism is four times larger at /5 than at /10. Unlike coma, eyepiece astigmatism increases with the square of apparent angle.
Also, unlike either spherical aberration or coma, lens astigmatism
- with the stop at the surface - is
independent of all three - refractive index, lens position factor and
shape factor; it only depends on the lens focal length. The means of controlling it with a set of positive lenses and lens
groups is generally limited, but the main reason why is it typically
strong in conventional eyepieces is that it is the third at the list of
priorities, after spherical aberration and coma. It is significantly
more complicated - or impossible, with simple designs - to have all three corrected.
in units of 550nm wavelength, where e is the eyepiece f.l., ε the eyepiece apparent field angle in degrees (radius), and F, as before, the telescope focal ratio. Plots at left show the range of astigmatism based on this approximation for three telescope ratios, fast, medium and slow. It scales with the eyepiece focal length.
near-edge AFOV for conventional eyepieces, it gives the following P-V
values of astigmatism for selected focal ratios and eyepiece focal
The error scales with the square of AFOV, which means it is four times smaller at 10° off axis, and 16 times smaller at 5°. The lower limit is not strict; the error can be still lower, but not significantly. On the other hand, poor designs can have significantly more astigmatism than the upper limit, up to twofold, or so. It can be assumed, however, that most of the conventional eyepieces made these days are closer to the lower limit shown in the table.
For given magnification, eyepiece astigmatism scales inversely to the focal ratio. For instance, if an /4 with 10mm f.l. eyepiece has 2.5-7.5 waves P-V of astigmatism at 20 off-axis, an /8 system with 20mm eyepiece of identical design will have 1.25-3.8 waves.
An interesting example is König design given in "Telescope Optics" from Rutten and Venrooij. It has practically cancelled primary astigmatism (and well corrected higher-order term), at a price of somewhat stronger than usual coma (FIG. 213). In terms of the RMS wavefront error, at 10° off-axis it is - according to OSLO - superior to its low-coma, strong astigmatism variant at both, /10 and /5, with 0.033 and 0.23 vs. 0.065 and 0.33 wave, respectively. At 20° field angle even more so: 0.16 and 0.7 vs. 0.94 and 3.7 wave. The enormous increase in the RMS error in the astigmatic Konig variant reflects the devastating effect of combined lower- and higher-order astigmatism. Yet, it is the type more likely to be found on the market, because of the general notion that coma is less desirable aberration form.
What actually puts the limit to usable field in a typical conventional eyepiece is the combination of lower- and higher-order astigmatism. At relatively small field angles, usually below ~15°, the higher-order component is, in most properly designed eyepieces, negligible to non-existent. But at once it creeps in at larger angles, it quickly explodes with the 4th power of field angle, adding to the already large lower-order component. This puts an end to the acceptable field size.
As mentioned, eyepiece astigmatism diminishes with the eyepiece focal length. A 10mm conventional eyepiece unit has ~3 times lower astigmatism than 30mm unit, resulting in about 1.7 times larger linear diffraction limited field. However, the difference is not that obvious in the eyepiece, due to shorter f.l. eyepieces having proportionally larger magnification, which mainly offsets the aberration decrease (FIG. 210).
FIGURE 210: Off-axis aberration in a conventional eyepiece (from ~10" distance the view is similar to the actual one). The difference in the nominal level of aberration - from 16 waves of astigmatism combined with 2.4 waves of coma for the 30mm f.l. at /5, to 0.65 wave of astigmatism and negligible coma for the 5mm at /10, both at 20° off-axis, which is more or less the typical level - is much greater than what the actual view shows. Actual Airy discs are not of identical size at these three -ratios (diameter being given by 4.6F/e in arc minutes), for 550nm wavelength; it would be noticed visually, assuming sufficient magnification, but not with the given screen resolution. Note that the plot shows only aberrations originating in the eyepiece; the final spot shape and size vary with the amount of off-axis aberration induced by the objective, as well as with the combined field curvature of the objective and eyepiece. In general, eyepiece aberrations - particularly astigmatism - dominate in fast to medium telescope systems.
For meaningful correction of eyepiece astigmatism it is necessary to introduce a negative (Smyth) lens, which induces astigmatism of opposite sign to that of the positive lens group. It also induces Petzval field curvature of the opposite sign, resulting in both astigmatism and field curvature minimized. Best known brand of this kind, the Nagler, has astigmatism reduced up to several times vs. comparable conventional eyepieces.
Eyepiece field curvature
Field curvature in the telescope eyepiece is directly related to its astigmatism. A hypothetical astigmatism-free eyepiece would form the image coinciding with the Petzval surface. Being formed by a positive power lens system, this surface is concave toward the eyepiece and, considering relatively short focal lengths, rather strongly curved (eyepiece's Petzval curvature, as well as other aberrations, are determined by reverse ray trace, with collimated light entering through the eyepiece's exit pupil).
Real world eyepieces, however, produce strong astigmatism, particularly the conventional types. Usually, this astigmatism is of opposite sign to the Petzval, thus abaxial points form astigmatic surfaces less curved relative to the Petzval up to a certain level. At the point when the sagittal astigmatic surface is half as curved as Petzval curvature, best image surface is nearly flat (FIG. 211B). Further increase in the astigmatism causes best image surface to become increasingly curved to the opposite side (FIG. 211C).
It is possible that astigmatism in the eyepiece is of the same sign as its Petzval (for instance, due to unbalanced higher-order astigmatism) in which case the astigmatic image surfaces are closer to the eyepiece than Petzval's, thus more strongly curved, and more so as the astigmatism increases.
FIGURE 211: Astigmatism-free eyepiece will form flat field if the image formed by the objective is also free from astigmatism and coincides with the eyepiece's Petzval surface P (A). Astigmatism modifies the field curvature depending on its sign and magnitude (B,C). If the sign is opposite to the Petzval's - usually the case - sagittal astigmatic surface S forms on the convex side of the Petzval's. Tangential surface T is always 3 times farther away from the Petzval than sagittal, with the best, or median surface M midway between the two.
Note that the curves show primary astigmatism. Eyepieces with strongly curved lenses also generate secondary, higher-order astigmatism. Since it has significantly different rate of increase than the lower-order form (4th and 2nd power of the field radius, respectively), once it reaches considerable level at larger field angles, it also strongly alters the initial field curvature. Depending on the design particulars, the effect with respect to field curvature can be either positive (field flattening) or negative; it can also be positive up to a certain image radius, then negative, or vice versa.
Flat eyepiece field means that all off-axis pencils exiti the eye lens collimated, enabling the eye to focus on all points across the field simultaneously. When the eyepiece field is curved, off axis pencils are progressively more diverging, or converging, going farther off axis, hence they cannot be focused simultaneously with the central pencils on the retina (i.e. image points appear to be closer, for diverging pencils, or farther away, for converging ones). This can be either lessened or worsened when combined with the curvature of the image formed by the objective, as shown below.
For simplicity, only best image surface is shown, i.e. field curvature is assumed to be either the Petzval with zero astigmatism, or best (median) astigmatic surface, when astigmatism is present. This is simplification in that it is not only the image curvatures, but also their respective astigmatism that interact, and since astigmatism directly influences field curvature it is a factor that shouldn't be entirely neglected. However, with the astigmatism of the objective being typically negligible in comparison, the astigmatism factor can be neglected in this respect for a general consideration, and assume that the interactions of field curvatures alone will give a good approximation of the combined field curvature.
Most objectives generate curvature concave toward objective, and most eyepieces nowadays have near flat field, in which case the combined visual field has curvature similar to that of the objective (1a). The reason is that only light from those points of the objective's image laying in the front focal plane of the eyepiece will exit the eyepiece as collimated pencils. Those farther out will exit converging, hence eye will focus on the (defocused) point of the objective's image laying in the front focal plane of the eyepiece. In order to focus on the points curving out away from the eyepiece, the eyepiece has to be shifted toward them. In effect, the visual image field is curved away from the eye. Eyepiece itself can generate curved image surface, either convex or concave toward the eye. If it is convex and nearly coinciding with the image surface of the objective, light from all points will exit eye lens as collimated pencils, i.e. will focus onto the retina, and the visual field will be effectively flat (1b). If, however, eyepiece field curvature is opposite to that of the objective's, the effective visual field curvature will be a sum of the two, twice as strong (1c).
Likewise, if the objective's image field is flat, the visual field will have the curvature of the eyepiece's field (2a-c). With some objectives which generate field curvature convex toward them, like Gregorian two-mirror telescope, the combined field curvature forms in the same manner, only the net sum with the same eyepieces is different (3a-c).
Astigmatism and field curvature of the eyepiece combine with those of the objective, to form astigmatism and field curvature of the final visual image. Just as the hypothetical astigmatism-free eyepiece would need objective's image to be astigmatism-free, with the two Petzval surfaces coinciding, in order to produce flat, astigmatism-free combined field, an astigmatic eyepiece would need objective whose astigmatic image would coincide with its own to result in astigmatism-free combined image. Eyepiece astigmatism is normally significantly stronger than that of the objective, especially for longer f.l. conventional eyepieces. Hence the astigmatism of the objective doesn't have much of effect on the final image: it is mainly determined by the eyepiece.
Short focal length eyepieces have proportionally lower astigmatism, and it can be noticeably affected by the astigmatism of the objective. Astigmatic surface profile of most amateur telescopes (Newtonian, refractor, Cassegrain) is roughly similar in form to that shown on FIG. 211C, concave toward objective, with the tangential surface closer to it. Newtonian form is identical to it, while in refractors and Cassegrain-like systems - including SCT and Gregory MCT - sagittal surface is also concave toward converging light, and so is the system Petzval; in Maksutov-Cassegrain with separate secondary, system astigmatism can be nearly corrected, with the field curvature nearly coinciding with its Petzval.
If the eyepiece has, say, form of astigmatism shown in (B), twice stronger than the astigmatism of the objective (i.e. double the sagittal-to-tangential surface separation) having the form shown in (C), the tangential surface of the combined image will be flat, with the sagittal unchanged, for the combined astigmatism half that in the eyepiece alone, and median image curvature of opposite sign, but of the same magnitude as that of the objective (Petzval surface becomes a factor only in astigmatism-free systems). If the eyepiece has the same amount of astigmatism, but with tangential surface flat and sagittal twice as strong as in the former example (which requires stronger eyepiece Petzval curvature), tangential surface in the combined image will have curvature equal to that in the objective, with the sagittal surface being as curved as in the eyepiece; the combined astigmatism is 50% greater than in the eyepiece, but with the combined median surface curvature somewhat weaker.
Gregorian-like two-mirror systems have, like Newtonian, Petzval surface curvature of the same sign as typical eyepiece's Petzval, but considerably stronger, with both sagittal and tangential astigmatic surface usually convex toward converging light. With both telescope types, this allows for the possibility of correcting both astigmatism and Petzval surface curvature in the final image with matching eyepiece (easier in the Gregorian, whose Petzval curvature is significantly closer in magnitude to that of the eyepiece).
Note that strong field curvature in eyepieces, if mainly result of
astigmatism as shown on FIG. 211, does not implicate significant
defocus error, even without the ability of the eye to accommodate.
Sagittal surface is usually relatively weak, and the wavefront error
along it is identical to that along the tangential surface, with the
wavefront error along best (median) surface smaller by a factor of
In other words, it is the error of astigmatism that dominates.