Fovea centralis

For other uses of fovea, see Fovea.
Fovea centralis

Schematic diagram of the human eye, with the fovea at the bottom. It shows a horizontal section through the right eye.
Details
Identifiers
Latin fovea centralis
TA A15.2.04.022
FMA 58658

Anatomical terminology

The fovea centralis (the term fovea comes from the Latin, meaning pit or pitfall) is a small, central pit composed of closely packed cones in the eye. It is located in the center of the macula lutea of the retina.[1][2]

The fovea is responsible for sharp central vision (also called foveal vision), which is necessary in humans for activities where visual detail is of primary importance, such as reading and driving. The fovea is surrounded by the parafovea belt, and the perifovea outer region.[2] The parafovea is the intermediate belt, where the ganglion cell layer is composed of more than five rows of cells, as well as the highest density of cones; the perifovea is the outermost region where the ganglion cell layer contains two to four rows of cells, and is where visual acuity is below the optimum. The perifovea contains an even more diminished density of cones, having 12 per 100 micrometres versus 50 per 100 micrometres in the most central fovea. This, in turn, is surrounded by a larger peripheral area that delivers highly compressed information of low resolution following the pattern of compression in foveated imaging.

Approximately half of the nerve fibers in the optic nerve carry information from the fovea, while the remaining half carry information from the rest of the retina. The parafovea extends to a radius of 1.25 mm from the central fovea, and the perifovea is found at a 2.75 mm radius from the fovea centralis.[3]

Structure

OCT scan of a retina at 800nm with an axial resolution of 3µm
The diagram shows the relative acuity of the left human eye (horizontal section) in degrees from the fovea.
Photograph of the retina of the human eye, with overlay diagrams showing the positions and sizes of the macula, fovea, and optic disc

Fovea (or Fovea centralis) is the depression in the inner retinal surface, about 1.5 mm wide, the photoreceptor layer of which is entirely cones and which is specialized for maximum visual acuity. Within the Fovea is a region of 0.5mm diameter celled the foveal avascular zone (which means without any blood vessels). This allows the light to be sensed without any dispersion or loss. This anatomy is responsible for the depression in the center of the fovea. The foveal pit is surrounded by the foveal rim that contains the neurons displaced from the pit. This is the thickest part of the retina.[4]

The fovea is located in a small avascular zone and receives most of its oxygen from the vessels in the choroid, which is across the retinal pigment epithelium and Bruch's membrane. The high spatial density of cones along with the absence of blood vessels at the fovea accounts for the high visual acuity capability at the fovea.[5]

The center of the fovea is the foveola – about 0.2 mm in diameter – or central pit where only cone photoreceptors are present and there are virtually no rods.[1] The central fovea consists of very compact cones, thinner and more rod-like in appearance than cones elsewhere. These cones are very densely packed (in a hexagonal pattern). Starting at the outskirts of the fovea, however, rods gradually appear, and the absolute density of cone receptors progressively decreases.

Size

Fovea size is relatively small compared to the rest of retina, but the fovea is the only area of the retina where 20/20 (Snellen Chart scale) vision is attainable, and very important for seeing fine detail and color.[6][7]

Function

Illustration of the distribution of cone cells in the fovea of an individual with normal color vision (left), and a color blind (protanopic) retina. Note that the center of the fovea holds very few blue-sensitive cones.

In the primate fovea (including humans) the ratios of ganglion cells to photoreceptors is about 2.5; almost every ganglion cell receives data from a single cone, and each cone feeds onto between 1 and 3 ganglion cells.[8] Therefore, the acuity of foveal vision is limited only by the density of the cone mosaic, and the fovea is the area of the eye with the highest sensitivity to fine details.[9] Cones in the central fovea express pigments that are sensitive to green and red light. These cones are the 'midget' pathways that also underpin high acuity functions of the fovea.

The fovea is employed for accurate vision in the direction where it is pointed. It comprises less than 1% of retinal size but takes up over 50% of the visual cortex in the brain.[10] The fovea sees only the central two degrees of the visual field, (approximately twice the width of your thumbnail at arm's length).[11] If an object is large and thus covers a large angle, the eyes must constantly shift their gaze to subsequently bring different portions of the image into the fovea (as in reading).

Distribution of rods and cones along a line passing through the fovea and the blind spot of a human eye[12]

Since the fovea does not have rods, it is not sensitive to dim lights. Hence, in order to observe dim stars, astronomers use averted vision, looking out of the side of their eyes where the density of rods is greater, and hence dim objects are more easily visible.

The fovea has a high concentration of the yellow carotenoid pigments lutein and zeaxanthin. They are concentrated in the Henle fiber layer (photoreceptor axons that go radially outward from the fovea) and to a lesser extent in the cones.[13][14] They are believed to play a protective role against the effects of high intensities of blue light which can damage the sensitive cones. The pigments also enhance the acuity of the fovea by reducing the sensitivity of the fovea to short wavelengths and counteracting the effect of chromatic aberration.[15] This is also accompanied by a lower density of blue cones at the center of the fovea.[16] The maximum density of blue cones occurs in a ring about the fovea. Consequently, the maximum acuity for blue light is lower than that of other colours and occurs approximately 1° off center.[16]

Angular size of foveal cones

See also: Retina Display, a trademarked term describing a pixel density matching that of the human eye.

On average, each square millimeter (mm) of the fovea contains approximately 147,000 cone cells,[17] or 383 cones per millimeter. The average focal length of the eye, i.e. the distance between the lens and fovea, is 17.1 mm.[18] From these values, one can calculate that the average angular size of each cone cell is approximately 31.46 arc seconds.

The following is a table of pixel densities required at various distances so that there is one pixel per 31.5 arc seconds:

Example objectDistance from eye assumedPPI (PPCM) to match
avg. foveal cone density
(20/10.5 vision)
Phone or tablet10 inches (25.4 cm)655.6 (258.1)
Laptop screen2 feet (61 cm)273.2 (107.6)
42" (1.07 m) 16:9 HDTV, 30° view5.69 feet (1.73 m)96.0 (37.8)

Peak cone density varies highly between individuals, such that peak values below 100,000 cones/mm2 and above 324,000 cones/mm2 are not uncommon.[19] Assuming average focal lengths, this suggests that individuals with both high cone densities and perfect optics may resolve pixels with an angular size of 21.2 arc seconds, requiring PPI values at least 1.5 times those shown above in order for images not to appear pixelated.

It is worth noting that individuals with 20/20 (6/6 m) vision, defined as the ability to discern a 5x5 pixel letter that has an angular size of 5 arc minutes, cannot see pixels smaller than 60 arc seconds. In order to resolve a pixel the size of 31.5 and 21.2 arc seconds, an individual would need 20/10.5 (6/3.1 m) and 20/7.1 (6/2.1 m) vision, respectively. To find the PPI values discernible at 20/20, simply divide the values in the above table by the visual acuity ratio (e.g. 96 PPI / (20/10.5 vision) = 50.4 PPI for 20/20 vision).

Entoptic effects in the fovea

The presence of the pigment in the radially arranged axons of the Henle fiber layer causes it to be dichroic and birefringent[20] to blue light. This effect is visible through the Haidinger's brush when the fovea is pointed to a polarized light source.

The combined effects of the macular pigment and the distribution of short wavelength cones results in the fovea having a lower sensitivity to blue light (blue light scotoma). Though this is not visible under normal circumstances due to "filling in" of information by the brain, under certain patterns of blue light illumination, a dark spot is visible at the point of focus.[21] Also, if mixture of red and blue light is viewed (by viewing white light through a dichroic filter), the point of foveal focus will have a central red spot surrounded by a few red fringes.[21][22] This is called the Maxwell's spot after James Clerk Maxwell[23] who discovered it.

Bifoveal fixation

In binocular vision, the two eyes converge to enable bifoveal fixation, which is necessary for achieving high stereoacuity.

In contrast, in a condition known as anomalous retinal correspondence, the brain associates of the fovea of one eye with an extrafoveal area of the other eye.

In other animals

The fovea is also a pit in the surface of the retinas of many types of fish, reptiles, and birds. Among mammals, it is found only in simian primates. The retinal fovea takes slightly different forms in different types of animals. For example, in primates, cone photoreceptors line the base of the foveal pit, the cells that elsewhere in the retina form more superficial layers having been displaced away from the foveal region during late fetal and early postnatal life. Other foveae may show only a reduced thickness in the inner cell layers, rather than an almost complete absence.

Additional images

See also

This article uses anatomical terminology; for an overview, see Anatomical terminology.

References

  1. 1 2 "Simple Anatomy of the Retina". Webvision. University of Utah. Retrieved 2011-09-28.
  2. 1 2 "Relation Between Superficial Capillaries and Foveal Structures in the Human Retina" - (with nomenclature of fovea terms), Masayuki Iwasaki and Hajime Inomara, - InvestigativeOphthalmology & Visual Science (journal), - volume 27, pages 1698-1705, 1986, IOVS.org, webpage: - IOVS-fovea-capillaries. -
  3. ↑ "eye, human."Encyclopædia Britannica. 2008. Encyclopædia Britannica 2006 Ultimate Reference Suite DVD
  4. ↑ Emmett T. Cunningham; Paul Riordan-Eva. Vaughan & Asbury's general ophthalmology. (18th ed.). McGraw-Hill Medical. p. 13. ISBN 978-0071634205.
  5. ↑ Provis et al., Prog Retin Eye Res Vol35 pp63-81
  6. ↑ "Age-Related Macular Degeneration (AMD) by Gregory S. Hageman". Retrieved December 11, 2013.
  7. ↑ "Macular Degeneration Frequently Asked Questions". Retrieved December 11, 2013.
  8. ↑ Ahmad; et al. (2003). "Cell density ratios in a foveal patch in macaque retina". Vis. Neurosci. 20 (2): 189–209. doi:10.1017/s0952523803202091. PMID 12916740.
  9. ↑ Smithsonian/The National Academies, Light:Student Guide and Source Book. Carolina Biological Supply Company, 2002. ISBN 0-89278-892-5.
  10. ↑ Krantz, John H. (1 October 2012). "Chapter 3: The Stimulus and Anatomy of the Visual System" (PDF). Experiencing Sensation and Perception. Pearson Education. ISBN 978-0-13-097793-9. OCLC 711948862. Retrieved 6 April 2012. Available online ahead of publication.
  11. ↑ Fairchild, Mark. (1998), Color Appearance Models. Reading, Mass.: Addison, Wesley, & Longman, p.7. ISBN 0-201-63464-3
  12. ↑ Foundations of Vision, Brian A. Wandell
  13. ↑ Krinsky, N. I.; Landrum, J. T.; Bone, R. A. (2003). "Biologic mechanisms of the protective role of lutein and zeaxanthin in the eye". Annual Review of Nutrition. 23: 171–201. doi:10.1146/annurev.nutr.23.011702.073307. PMID 12626691.
  14. ↑ Landrum, J. T.; Bone, R. A. (2001). "Lutein, Zeaxanthin, and the Macular Pigment". Archives of Biochemistry and Biophysics. 385 (1): 28–40. doi:10.1006/abbi.2000.2171. PMID 11361022.
  15. ↑ Beatty, S.; Boulton, M.; Henson, D.; Koh, H. -H.; Murray, I. J. (1999). "Macular pigment and age related macular degeneration". British Journal of Ophthalmology. 83 (7): 867–877. doi:10.1136/bjo.83.7.867. PMC 1723114Freely accessible. PMID 10381676.
  16. 1 2 Curcio, C. A.; Allen, K. A.; Sloan, K. R.; Lerea, C. L.; Hurley, J. B.; Klock, I. B.; Milam, A. H. (1991). "Distribution and morphology of human cone photoreceptors stained with anti-blue opsin". The Journal of Comparative Neurology. 312 (4): 610–624. doi:10.1002/cne.903120411. PMID 1722224.
  17. ↑ Shroff, Anand (2011). An Eye on Numbers: A Ready Reckoner in Ophthalmology. p. 97. ISBN 9788192112312.
  18. ↑ Serpenguzel, Ali; Serpengüzel, Ali; Poon, Andrew W. (2011). Optical Processes in Microparticles and Nanostructures: A Festschrift Dedicated to Richard Kounai Chang on His Retirement from Yale University. ISBN 9789814295772.
  19. ↑ Christine A. Curcio; Kenneth R. Sloan; Robert E. Kalina; Anita E. Hendrickso (February 1990). "Human photoreceptor topography". The Journal of Comparative Neurology. 292 (4): 497–523. doi:10.1002/cne.902920402. PMID 2324310.
  20. ↑ Vannasdale, D. A.; Elsner, A. E.; Weber, A.; Miura, M.; Haggerty, B. P. (2009). "Determination of foveal location using scanning laser polarimetry". Journal of Vision. 9 (3): 21.21–17. doi:10.1167/9.3.21. PMC 2970516Freely accessible. PMID 19757960.
  21. 1 2 Magnussen, S.; Spillmann, L.; Stürzel, F.; Werner, J. S. (2001). "Filling-in of the foveal blue scotoma". Vision Research. 41 (23): 2961–2967. doi:10.1016/S0042-6989(01)00178-X. PMC 2715890Freely accessible. PMID 11704235.
  22. ↑ Isobe, K.; Motokawa, K. (1955). "Functional Structure of the Retinal Fovea and Maxwell's Spot". Nature. 175 (4450): 306–307. doi:10.1038/175306a0. PMID 13235884.
  23. ↑ Flom, M. C.; Weymouth, F. W. (1961). "Centricity of Maxwell's Spot in Strabismus and Amblyopia". Archives of Ophthalmology. 66 (2): 260. doi:10.1001/archopht.1961.00960010262018.
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