- See also: Aberration in optical
systems and Astigmatism (eye)
In optics, astigmatism (from Greek: α-
a- "without" + στίγματος stigmatos, gen. of στίγμα stigma "a mark, spot, puncture"[1]) is when an optical system has different foci for rays that propagate in two perpendicular planes. If an optical system with astigmatism is used to form an image of a cross, the vertical and horizontal lines will be in sharp focus at two different distances.
Forms of astigmatism
There are two distinct forms of astigmatism. The first is a third-order aberration, which occurs for objects (or parts of objects) away from the optical axis. This form of aberration occurs even when the optical system is perfectly symmetrical. This is
often referred to as a "monochromatic aberration", because it occurs even for light of a single wavelength. This terminology may be misleading, however, as the amount of aberration can vary strongly
with wavelength in an optical system.
The second form of astigmatism occurs when the optical system is not symmetric about the optical axis. This may be by design
(as in the case of a cylindrical lens), or due to manufacturing error in the
surfaces of the components or misalignment of the components. In this case, astigmatism is observed even for rays from on-axis
object points. This form of astigmatism is extremely important in ophthalmology, since the
human eye often exhibits this aberration due to imperfections in the shape of the cornea or the lens.
Third-order astigmatism
Page explaining and illustrating astigmatism
[2]
In the analysis of this form of astigmatism, it is most common to consider rays from a given point on the object, which
propagate in two special planes. The first plane is the tangential plane. This is the plane which includes both the object
point being considered and the axis of symmetry. Rays that propagate in this plane are called tangential rays. Planes that include the optical axis are meridional planes. It is common to
simplify problems in radially-symmetric optical systems by choosing object points in the vertical ("y") plane only. This
plane is then sometimes referred to as the meridional plane.
The second special plane is the sagittal plane. This is defined as the plane, orthogonal to the tangential plane, which contains the object point being considered and intersects the
optical axis at the entrance pupil of the optical system. This plane contains the
chief ray, but does not contain the optic axis. It is therefore a skew plane, in
other words not a meridional plane. Rays propagating in this plane are called sagittal
rays.
In third-order astigmatism, the sagittal and transverse rays form foci at different
distances along the optic axis. These foci are called the sagittal focus and the transverse focus, respectively. In
the presence of astigmatism, an off-axis point on the object is not sharply imaged by the optical system. Instead, sharp
lines are formed at the sagittal and transverse foci. The image at the transverse focus is a short line, oriented in the
direction of the sagittal plane; images of circles centered on the optic axis, or lines tangential to such circles, will
be sharp in this plane. The image at the sagittal focus is a short line, oriented in the tangential direction; images of
spokes radiating from the center are sharp at this focus. In between these two foci, a round but "blurry" image is formed. This
is called the medial focus or circle of least confusion. This plane often represents the best compromise image
location in a system with astigmatism.
The amount of aberration due to astigmatism is proportional to the square of the
angle between the rays from the object and the optical axis of the system. With care, an optical system can be designed to reduce
or eliminate astigmatism. Such systems are called anastigmats.
Astigmatism in systems that are not rotationally symmetric
Blur from astigmatic lens at different distances.
If an optical system is not axisymmetric, either due to an error in the shape of the optical surfaces or due to misalignment
of the components, astigmatism can occur even for on-axis object points. This effect is often used deliberately in complex
optical systems, especially certain types of telescope.
In the analysis of these systems, it is common to consider tangential rays (as defined above), and rays in a meridional plane
(a plane containing the optic axis) perpendicular to the tangential plane. This plane is called either the sagittal meridional
plane or, confusingly, just the sagittal plane.
Ophthalmic astigmatism
-
In ophthalmology, the vertical and horizontal planes are identified as
tangential and sagittal meridians, respectively. Ophthalmic astigmatism is a refraction error of the eye in which there is a difference in degree of
refraction in different meridians. It is typically characterized by an aspherical, non-figure
of revolution cornea in which the corneal profile slope and
refractive power in one meridian is greater than that of the perpendicular axis.
Astigmatism causes difficulties in seeing fine detail. In some cases vertical lines and objects such as walls may appear to
the patient to be leaning over like the Tower of Pisa. Astigmatism can be often
corrected by glasses with a lens that has different
radii of curvature in different planes (a cylindrical lens),
contact lenses, or refractive surgery.
Astigmatism is quite common. Studies have shown that about one in three people suffers from it [1][2][3]. The prevalence of astigmatism increases with age [4]. Although a person may not notice mild astigmatism, higher amounts of
astigmatism may cause blurry vision, squinting,
asthenopia, fatigue, or headaches [5] [6]
[7].
There are a number of tests used by ophthalmologists and optometrists during eye examinations to determine the presence of
astigmatism and to quantify the amount and axis of the astigmatism[8]. A Snellen chart or other eye chart may
initially reveal reduced visual acuity. A keratometer
may be used to measure the curvature of the steepest and flattest meridians in the cornea's front surface[9]. A corneal topographer may also be used to obtain a more accurate representation of the cornea's shape [10]. An autorefractor or retinoscopy may provide an objective estimate of the
eye's refractive error and the use of Jackson cross cylinders in a phoropter may be used to subjectively refine those measurements[11] [12] [13]. An alternative technique with the phoropter requires the use of a "clock dial" or
"sunburst" chart to determine the astigmatic axis and power[14][15].
Astigmatism due to misaligned or malformed lenses and mirrors
Grinding and polishing of precision optical parts, either by hand or machine, typically employs significant downward pressure,
which in turn creates significant frictional side pressures during polishing strokes that can combine to locally flex and distort
the parts. These distortions generally do not possess figure-of-revolution symmetry and are thus astigmatic, and slowly become
permanently polished into the surface if the problems causing the distortion are not corrected. Astigmatic, distorted surfaces
potentially introduce serious degradations in optical system performance.
Surface distortion due to grinding or polishing increases with the aspect ratio of the
part (diameter to thickness ratio). To a first order, glass strength increases as the cube of the thickness. Thick lenses at 4:1 to 6:1 aspect ratios will flex much less than high aspect
ratio parts, such as optical windows, which can have aspect ratios of 15:1 or higher. The combination of surface or wavefront
error precision requirements and part aspect ratio drives the degree of back support uniformity required, especially during the
higher down pressures and side forces during polishing. Optical working typically involves a degree of randomness that helps
greatly in preserving figure-of-revolution surfaces, provided the part is not flexing during the grind/polish process.
Deliberate astigmatism in optical systems
Compact disc players use an astigmatic lens for focusing. When one axis is more in focus
than the other, dot-like features on the disc project to oval shapes. The orientation of the oval indicates which axis is more in
focus, and thus which direction the lens needs to move. A square arrangement of only four sensors can observe this bias and use
it to bring the read lens to best focus, without being fooled by oblong pits or other features on the disc surface.
Some telescopes use deliberately astigmatic optics.
References
- ^ http://www.etymonline.com/index.php?term=astigmatism
- ^ Frederic Eugene Wright, The Methods of Petrographic-microscopic
Research, Their Relative Accuracy and Range of Application, Carnegie institution of Washington, 1911.
- Greivenkamp, John E. (2004). Field Guide to
Geometrical Optics, SPIE Field Guides vol. FG01, SPIE. ISBN 0-8194-5294-7.
- Hecht, Eugene (1987). Optics, 2nd ed., Addison
Wesley. ISBN 0-201-11609-X.
See also
External links
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