Photorefraction

 

Ai-Hou Wang, M.D., Ph.D.

 

Äá¼vÅç¥úªk¬O¥Î¬Û¤ù°O¿ýÀû¤Õ¤Ï¥ú¡A¥Ñ¬Û¤ù¤W¬õ²´¤Ï¥úªº¤j¤p¥h¤ÀªR¡B§PŪ¨ü´úªÌªº©}¥ú­È¡C¥Ø«e¦³³\¦h³]­p¡A¨Ï¥Î¦P¼Ëªº¥ú¾Ç­ì²z¡A¤£¥Î¬Û¤ù¦Ó¬O¥Î¿ý¼v¡B¥Î¹q¸£¡A¦]¦¹²Îͬ°¡uÄá¼vÅç¥úªk¡v¡C¥Ø«e¥«°âªºÄá¼vÅç¥ú»ö(photorefractor)³£±Ä¥ÎÂ÷¶bÄá¼vÅç¥úªº¥ú¾Ç­ì²z¡C

 

Photorefractory optics uses photographs to record pupil reflections and analyzes the magnitude of the red-eye reflection in the photograph to determine the subject's refractive value. Currently, many designs use the same optical principle but instead of photographs, they use video recordings and computers; hence, they are collectively translated as "photorefractory optics." Most commercially available photorefractors currently employ the optical principle of off-axis photorefractory optics.

 

 

Äá¼vÅç¥úªkªº­^¤å¬Ophotorefraction¡Cphoto«üªº¬O¬Û¤ù¡A­ì·N¬O¥Î¬Û¤ù°O¿ýÀû¤Õ¤Ï¥ú¡A¥ÑÀû¤Õªº¤Ï¥úŪ¥X²´²yªº©}¥ú­È¡A¥Ñ­^¤åª½Ä¶¬O¡u¬Û¤ùÅç¥úªk¡v¡C¥Ø«e¦³³\¦h¨Ï¥Î¦P¼Ë¥ú¾Ç­ì²zªº³]­p¡A¦ý¬O¤£¥Î¬Û¤ù¡A¦Ó¬O¥Î¿ý¼v¡A¥Î¹q¸£¡A¦]¦¹²Îͬ°¡uÄá¼vÅç¥úªk¡v»á¬°¾A·í¡C

 

The English term for photographic refraction is "photorefraction." "Photo" refers to a photograph, and the original meaning was to record the reflection of light from the pupil using a photograph, and then read the refractive value of the eye from the reflection. A direct translation from English would be "photographic refraction." Currently, many designs use the same optical principles, but instead of photographs, they use video recordings and computers; therefore, the general translation "photographic refraction" is quite appropriate.

 

 

Äá¼vÅç¥úªk¬O¦b¤@¬q¶ZÂ÷ (50~100+cm)¤§¥~Åç¥ú, ¤×¨ä¾A¦XÀ¦¥®¨àªºÅç¥ú¡C¦b¤@¬q¶ZÂ÷¤§¥~Åç¥ú¤@ª½¬O¤p¨à²´¬ìÂå®vªº¹Ú·Q¡C¤@¯ëªºÅç¥ú¾÷©Î¤â«ù¦¡Åç¥ú¾÷ (¨Ò¦pNikon Retinomax)¡B§Y«K¬Oºô½¤ÃèÀ˼vªk¤]±o¨Ï¥Î¤¤©MÃè¤ù¡A³£­n«D±`ªº¾aªñ¨ü´ú¸ÕªÌ¡C¤Óªñªº´ú¸Õ¶ZÂ÷À¦¥®¨à³q±`·|®`©È·|­ú¡A¦P®É¤]µLªkª`µøÅç¥ú¾÷¬}¸Ìªºµø¼Ð¡C

 

Photorefractive refraction is performed at a distance (50-100+ cm), making it particularly suitable for infants and young children. Performing refraction at a distance has always been a dream for pediatric ophthalmologists. Regular or handheld refractometers (such as the Nikon Retinomax), and even retinoscopy, require the use of neutralizing lenses and must be very close to the subject. Testing at such close distances usually frightens infants and young children, causing them to cry, and they also cannot focus on the target inside the refractometer's aperture.

 

 

²Ä1 ¸`  Äá¼vÅç¥úªkªºµo®i

1.1 Äá¼vÅç¥ú»öªºµo®i¥v

1970¦~¥N°_¡AHowland©MKaakinen¥ý«áµo®i¤F¦P¶b (coaxial) ©MÂ÷¶b (off-axis)ªºÄá¼vÅç¥úªk¡C¥ú·½©MÃèÀY¦P¶bªº¨âºØ¤è¦¡¬O(1)¥¿¥æÄá¼vÅç¥ú (Orthogonal photorefraction, 1974) ©M(2)¦U¦V¦P©ÊÄá¼vÅç¥ú (Isotropic photorefraction, 1979)¡CKaakinen 1979µo®i¥XÂ÷¶bÄá¼vÅç¥ú (Eccentric photorefraction or Knife edge photorefraction) (¹Ï4-1)¡A±N¬Û¾÷ªº°{¥ú¿O²¾¨ì±µªñÃèÀY¤¤¥¡¡A±q¬Û¤ù¤W¬õ²´¤Ï¥úªº¤j¤p¥h¤ÀªR¡B§PŪ¨ü´úªÌªº©}¥ú­È¡C¥Ø«e¥«°âªºÄá¼vÅç¥ú»ö (photorefractor)³£±Ä¥ÎÂ÷¶bÄá¼vÅç¥úªº¥ú¾Ç­ì²z¡C

 

Section 1 Development of Photorefractory Methods

1.1 History of Photorefractor Development

Starting in the 1970s, Howland and Kaakinen successively developed coaxial and off-axis photorefractory methods. The two methods of coaxial light source and lens are (1) orthogonal photorefractory (1974) and (2) isotropic photorefractory (1979). Kaakinen developed off-axis photorefractory (Eccentric photorefractory or Knife edge photorefractory) in 1979 (Figure 1), which involves moving the camera flash closer to the center of the lens and analyzing and interpreting the refractive value of the subject based on the magnitude of red-eye reflection in the photograph. Currently, commercially available photorefractors all use the optical principle of off-axis photorefractory.

 

 

 

Figure 1 Orthogonal photorefraction, Isotropic photorefraction, and Eccentric photorefraction

 

 

1.2 Äá¼vÅç¥ú»ö¥«ªp

¥«°âÄá¼vÅç¥ú»ö¦³Plusoptix S12 («e¨­¬°PowerRefractor)¡AWelch Allyn¤½¥qªºSPOT («e¨­¬°Suresight)¡A2Win¡AiSreen¡CGobiquity GoCheckKids«h¸Õ¹Ï¨Ï¥ÎiPhone¨Ó§@Äá¼vÅç¥úªk¡C¦­´ÁªºÄá¼vÅç¥ú»ö«h¦³MTI¡AViVA¡ATopcon¤½¥qªºPR-1000¡APR-2000µ¥µ¥¡C³o¨Ç»ö¾¹¤j³£´Â¦VÅç¥ú¾÷ªº¤è¦V³]­p¡A¦ý¬O´ú¶qªº·Ç½T«×¤ñ¶Ç²ÎªºÅç¥ú¾÷®t«Ü¦h¡A¤£¾A¦X§@ºë½TªºÅç¥ú°tÃè¡A¦Ó¬O¥Î©ó²´¬ì©Î¤p¨à¬ìªù¶Eªºªì¿z©ÎªÌ¥®¨à¶é¡B¦«¨à©Òªºµø¤O¿zÀË¡C¤]¦³¤H´£Ä³¦b¤H¼é¼ö°Ï³]¸mÄá¼vÅç¥ú«F (booth)¡A¦n¹³§Ö©ç¬Û¤ù«F¤@¼Ë¡A¹q¸£¦Û°Ê§PŪ¡A©Ý¼sµø¤O¿zÀ˪º½d³ò»P¼h­±¡C

 

1.2 Market Status of Photorefractive Optometrists Commercially available photorefractive optometrists include Plusoptix S12 (formerly PowerRefractor), Welch Allyn's SPOT (formerly Suresight), 2Win, and iSreen. Gobiquity GoCheckKids attempts to use an iPhone for photorefractive optometry. Early photorefractive optometrists included MTI, ViVA, and Topcon's PR-1000 and PR-2000. These instruments are mostly designed to resemble traditional refractometers, but their measurement accuracy is much lower, making them unsuitable for precise refraction and prescription glasses. They are better suited for initial screening in ophthalmology or pediatric clinics, or vision screening in kindergartens and daycare centers. Some have proposed setting up photorefractive optometry booths in high-traffic areas, similar to quick photo booths, with automatic computer interpretation to broaden the scope and level of vision screening.

 

 

¦bºô¸ô¤W¡AÄá¼vÅç¥úªk¸ê®Æ¤ñ¸û¸Ô²Óªººô§}¬OABCD (Alaske Blind Children Discovery http://abcd-vision.org/ ¤§¤UªºVision Sceening¡A¦A¤§¤UªºPhotoscreening http://abcd-vision.org/vision-screening/photoscreening.html¡C

 

On the internet, the most detailed information on photorefraction is available at ABCD (Alaske Blind Children Discovery http://abcd-vision.org/, under Vision Sceening, and then Photoscreening http://abcd-vision.org/vision-screening/photoscreening.html).

 

 

²Ä2¸`  Äá¼vÅç¥úªkªº¥ú¾Ç

Äá¼vÅç¥ú»öªºÂú§Î¬O±N©ç¥ß±o¬Û¾÷ªº°{¥ú¿O©î¤U¡A²¾¸m¨ì«D±`¾aªñÃèÀY¤¤¥¡ªº¦ì¸m (¹Ï4-2)¡A¥ÑÀû¤Õ¤Ï¥ú(Crescent)ªº¤j¤p¨Ó§PŪ«×¼Æ¡C

 

Section 2 Optics of Photographic Optometry The prototype of the photographic optometry instrument was to remove the flash of an instant camera and move it to a position very close to the center of the lens (Figure 4-2), and to determine the diopter by the size of the pupil reflection (Crescent).

 

 

¹Ï4-2 ©ç¥ß±o¬Û¾÷§ï¸Ë°{¥ú¿O¦Ó¦¨ªºÄá¼vÅç¥ú»öªºÂú§Î

 

Figure 2 A prototype of a photographic optometry device made by modifying a Polaroid camera into a flash unit.

 

 

§C«×¼Æ©}¥ú¤£¥¿¨S¦³Àû¤Õ¤Ï¥ú¡A°ª«×ªñµøªºÀû¤Õ¤Ï¥ú¦b°{¥ú¿Oªº¦P°¼¡A¦Ó°ª«×»·µøªºÀû¤Õ¤Ï¥ú¦b°{¥ú¿Oªº¥t°¼ (¹Ï4-3)¡C¦b§C«×¼Æ©}¥ú¤£¥¿¡A¨Ò¦p»·µø+2D©M+3D¡A¤Ï¥úªº¤j¤p®t²§«Ü¤j¡A¹ï©}¥úªºÅ²§O«×¨Î¡F¦Ó¦b°ª«×¼Æ©}¥ú¤£¥¿¡A¨Ò¦p»·µø+7D©M+8D¡A¤Ï¥ú¤j¤pªº®t²§´N«Ü¦³­­¡A©}¥úªºÅ²§O«×´N¤£¦n¤F¡C

 

Low-degree refractive errors show no pupillary reflection. In high myopia, the pupillary reflection is on the same side as the flash, while in high hyperopia, it is on the opposite side (Figure 4-3). In low-degree refractive errors, such as hyperopia +2D and +3D, the difference in reflection size is significant, resulting in good refractive discrimination. However, in high-degree refractive errors, such as hyperopia +7D and +8D, the difference in reflection size is very limited, leading to poor refractive discrimination.

 

 

 

¹Ï4-3¾î¶b¬°©}¥ú­È¡AÁa¶b¬°¤Ï¥ú¤j¤p¡Cªñµø¡B»·µøªºÀû¤Õ¤Ï¥ú¦b¬Û¤Ï°¼¡C

¹Ï§Îªº¹ïºÙ¤¤ÂI¬O´ú¸Õ¶ZÂ÷ªºµJ«×(vergence)¡C

 

Figure 3 shows the refractive index on the horizontal axis and the reflectance on the vertical axis. The pupillary reflectance is on opposite sides for myopia and hyperopia.

 

The midpoint of the graph represents the vergence at the test distance.

 

 

2.1 Äá¼vÅç¥úªkªº¥ú¾Ç¤½¦¡

Äá¼vÅç¥úªkªº¥ú¾Ç¤½¦¡¬O±d¤Dº¸¤j¾ÇHoward C. Howland (¹Ï4-4)­º¥ý´£¥X¡A1999¦~§Ú¦b¤£ª¾±¡ªº±¡ªp¤U¤]¦Û¦æ¾É¥X¦P¼Ëªº¤½¦¡¡C

 

2.1 Optical Formula of Photorefraction The optical formula of photorefraction was first proposed by Howard C. Howland of Cornell University (Figure 4-4). In 1999, I also derived the same formula on my own without knowing the facts.

 

 

Figure 4 Dr. Howard C. Howland

 

°ò¥»ªº¥ú¾Ç¤½¦¡¬O d = DF x Pu x L x RR

* d¡Gµø½u¡B¥ú½uªº¶ZÂ÷(©ÎªÌ¬O°{¥ú¿OÃä½t©MÃèÀY¤¤¤ßªº¶ZÂ÷)

* DF (Dark Fraction)¡G·t°Ï¤ñ¨Ò (=1¡VCrescent) (1-«G°Ï¤ñ¨Ò) (¹Ï4-5)¡A

¦b³o­Ó¨Ò¤l¸Ì¡A·t°Ï=3/4¡A«G°Ï=1/4)

* Pu¡GÀû¤Õª½®|

* L¡G´ú¸Õ¶ZÂ÷

* RR (Relative refraction)¡G¬Û¹ï©}¥ú¡C¨Ò¦p¦b1¤½¤Ø¶ZÂ÷§@´ú¸Õ¡A«h¥H -1D¬°°ò·ÇÂI¡C- 4DªºRR¬O -3D¡B¥¿µø²´ªºRR¬O +1D¡B+3DªºRR¬O + 4 Dµ¥µ¥¡C

 

The basic optical formula is d = DF x Pu x L x RR

 

* d: Line of sight, distance of light (or the distance between the edge of the flash and the center of the lens)

 

* DF (Dark Fraction): Dark area ratio (=1 ¡V Crescent) (1 ¡V Bright area ratio) (Figure 4-5). In this example, dark area = 3/4, bright area = 1/4.

 

* Pu: Pupil diameter

 

* L: Test distance

 

* RR (Relative refraction): Relative refraction. For example, when testing at a distance of 1 meter, -1D is used as the reference point. -4D RR ​​is -3D, RR for emmetropia is +1D, RR for +3D is +4D, and so on.

 

 

¹Ï4-5 ·t°Ï¡B«G°Ï»PÀû¤Õªº¤ñ¨Ò¡C¥»¨Ò¹Ï¥Ü«G°Ï/Àû¤Õ=1/4¡A·t°Ï/Àû¤Õ=3/4¡C

 

Figure 5 shows the ratio of dark area, bright area, and pupil. In this example, the ratio of bright area to pupil is 1/4, and the ratio of dark area to pupil is 3/4.

 

 

±×¦V´²¥úªºÀû¤Õ¤Ï¥ú (Crescent)¤]¬O¶É±×ªº (¹Ï4-6)¡C¸Õ¹Ïª½±µ±q±×¦V¤Ï¥úªº§Îª¬¡B¨¤«×¥h­pºâ©}¥úªº¤½¦¡½Ð°Ñ¦ÒWesemann W, Norcia AM, Allen D. Theory of eccentric photorefraction (photoretinoscopy): astigmatic eyes. J Opt Soc Am A. Dec;8(12):2038-47, 1991.

 

The pupillary reflection (Crescent) in oblique astigmatism is also oblique (Figure 4-6). For formulas that attempt to calculate refractive error directly from the shape and angle of the oblique reflection, please refer to Wesemann W, Norcia AM, Allen D. Theory of eccentric photorefraction (photoretinoscopy): astigmatic eyes. J Opt Soc Am A. Dec;8(12):2038-47, 1991.

 

 

¹Ï4-6 ±×¦V´²¥úªºÀû¤Õ¤Ï¥ú¤]¬O¶É±×ªº

 

Figure 4-6 shows that the pupillary reflection in oblique astigmatism is also oblique.

 

 

2.2 PowerRefractor

PowerRefractor¥Ñ¤T­Ó¤è¦Vªº¥ú·½¡AŪ¨ú¤T­Ó¤è¦Vªº¼Æ¾Ú¥h§@Äá¼vÅç¥úªk (¹Ï4-7)¡C³o¤T­Ó¤è¦V¤§¤¤¦Ü¤Ö¦³¨â­Ó¤è¦VªºÀû¤Õ¤Ï¥ú¬O¶É±×ªº¤Ï¥ú¡A¤]¥²©w¬O§Q¥Î¸Ó½g½×¤åªº­pºâ¤è¦¡¥h¨D¨ú©}¥ú­È¡C¤@¯ëªº©}¥ú­È¥]§t¦³²yÃè«×¼Æ¡B¬WÃè«×¼Æ©M¬WÃ訤«×¤T­ÓÅܼơAPowerRefractor´ú¶q¤T­Ó¤è¦Vªº¼Æ­È¥hÂà´«¬°©}¥ú­Èªº¤T­ÓÅܼơA¤]ºâ¬Oº¡¦X²zªº¡C

 

2.2 PowerRefractor The PowerRefractor uses light from three directions to read data from each direction for photorefraction (Figure 4-7). At least two of these directions show oblique pupillary reflections, and the refractive value is calculated using the method described in this paper. A typical refractive value includes three variables: spherical power, cylindrical power, and cylindrical angle. It is reasonable for the PowerRefractor to measure values ​​from three directions and convert them into these three variables for the refractive value.

 

 

¹Ï4-7  PowerRefractor´ú¶q¤T­Ó¤è¦Vªº¼Æ¾Ú¥h­pºâ²´²y©}¥ú­Èªº¤TÅܼơG

(1)²yÃè«×¼Æ¡B(2)¬WÃè«×¼Æ¡B(3)¬WÃ訤«×¡C

 

Figure 4-7 PowerRefractor measures data in three directions to calculate the three variables of the eye's refractive value: (1) spherical power, (2) cylindrical power, and (3) cylindrical angle.

 

 

2.3 ª½±µ²´©³Ã誺¥ú¾Çµ²ºc

ª½±µ²´©³Ã誺¥ú¾Çµ²ºc§¹¥þ²Å¦XÄá¼vÅç¥úªkªº¥ú¾Ç­ì²z¡A¬°¤F¯à°÷¸g¥Ñ·¥¤pªºÀû¤Õ¥hÀˬd²´©³¡A¥¦ªº¥ú·½©Mµø½u³]­p¦¨«D±`ªº¾aªñ (¹Ï4-8)¡A´X¥G¬O¦P¶bªº¡C

 

2.3 Optical Structure of Direct Fundus Camera The optical structure of the direct fundus camera fully conforms to the optical principles of photorefraction. In order to examine the fundus through the extremely small pupil, its light source and line of sight are designed to be very close (Figure 4-8), almost coaxial.

 

 

¹Ï4-8 ª½±µ²´©³Ã誺¥ú¾Çµ²ºc§¹¥þ²Å¦XÄá¼vÅç¥úªkªº¥ú¾Ç­ì²z

 

Figure 4-8 shows that the optical structure of the direct fundus microscope fully conforms to the optical principles of photorefraction.

 

 

±q50~100mªº¶ZÂ÷¡A¥Ñª½±µ²´©³Ã誺µø¤Õ¬Ý¯f¤HªºÀû¤Õ¬õ¤Ï¥ú (¦p¦P±×µøÀˬdªºHirschberg´ú¸Õ)¡A§C«×¼Æªº©}¥ú¤£¥¿¸¨¦bÄá¼vÅç¥úªkªºµL¤Ï¥ú°Ï¡A¨S¦³Àû¤Õ¤Ï¥ú¡AÀû¤Õ¬O·tªº¡C¦pªG¬Ý¨ìÀû¤Õ¤W¤è¦³¤Ï¥ú (Crescent)¡A¥i§Pª¾¬O°ª«×»·µø²´¡F¦pªG¬Ý¨ìÀû¤Õ¤U¤è¦³¤Ï¥ú¡A¥i§Pª¾¬O°ª«×ªñµø²´ (¹Ï4-9)¡C³o¦b¤p¨à²´¬ìªºÀˬd«D±`¦³¥Î¡A¤£¥Î¦b²´«e©ñ¸m¤¤©MÃè¤ù¡A´N¥i¥Hªì¨Bª¾¹D¤j­Pªº©}¥úª¬ºA¡C

 

From a distance of 50-100 meters, observe the patient's pupillary red reflex through the viewing port of a direct ophthalmoscope (similar to the Hirschberg test for strabismus). Low-degree refractive errors fall within the non-reflective zone of photorefraction, resulting in no pupillary reflex and a dark pupil. If a reflex (crescent) is seen above the pupil, it indicates high hyperopia; if a reflex is seen below the pupil, it indicates high myopia (Figure 4-9). This is very useful in pediatric ophthalmology examinations, allowing for a preliminary assessment of the approximate refractive state without the need for a neutralizing lens.

 

 

¹Ï 4-9 ¥Ñª½±µ²´©³Ã誺µø¤Õ¬ÝÀû¤Õ¤Ï¥ú¡AÀû¤Õ¤U¤è¦³¤Ï¥ú ¥i§Pª¾¬O°ª«×

ªñµø²´¡AÀû¤Õ¤W¤è¦³¤Ï¥ú¬O°ª«×»·µø²´¡C

 

Figure 4-9 shows the pupil reflection as seen through the viewing aperture of a direct ophthalmoscope. A reflection below the pupil indicates high myopia, while a reflection above the pupil indicates high hyperopia.

 

 

2.4 Brückner¤Ï¥úÀˬd

Àû¤ÕªºBrückner¤Ï¥úÀˬdªº¥ú¾Ç­ì²z¤]¦p¦PÄá¼vÅç¥úªk¤@¼Ë¡C¦b¤@¬q¶ZÂ÷¡B¥Ñª½±µ²´©³Ã誺µø¤Õ¦P®É¬Ý¨â²´ªºÀû¤Õ¤Ï¥ú¡AÀû¤Õ·tªº¤@²´¬Oª`µø²´¡A¨Ã¥B¬O§C«×¼Æ©}¥ú¤£¥¿¡FÀû¤Õ«Gªº¤@²´¬O±×µø²´¡A¦]¬°¬O¥Ñ±×ªº¤è¦VÆ[¹î³o­Ó²´·ú¡A¥ú¾Ç¤W¬O°ª«×»·µø¡A©ó¬OÀû¤Õ¦³¤Ï¥ú¡A¬O«GªºÀû¤Õ (¹Ï4-10)¡C

 

2.4 Brückner Reflection Test

The optical principle of the Brückner reflection test of the pupil is the same as that of photorefraction. At a distance, the pupil reflections of both eyes are simultaneously observed through the viewing aperture of a direct ophthalmoscope. The eye with a darker pupil is the fixing eye and has a low degree of refractive error; the eye with a brighter pupil is the strabismic eye, because it is being observed from an oblique direction, optically it is highly hyperopic, hence the bright pupil (Figure 4-10).

 

 

¹Ï4-10  BrücknerÀû¤Õ¤Ï¥úÀˬd¡CÀû¤Õ«Gªº¤@²´¬O±×µø²´¡C

 

Figure 4-10 Brückner pupillary reflection test. The eye with the brighter pupil is the strabismic eye.

 

 

2.5 ¤@¯ëÄá¼vªº¬õ²´°ÝÃD

¤@¯ëªº¬Û¾÷©ç¤H¹³ªº®É­Ô¡A¤£§Æ±æ©ç¨ìÀû¤Õµo«G¡A©ó¬O°{¥ú¿Oªº¦ì¸m¾¨¶q¤£­n¤Ó¾aªñÃèÀY¥H§K²£¥Í¬õ²´¡C¦ý¬OÄá¼vÅç¥úªk´N¬O­n§Q¥Î³o­Ó¤Ï¥ú¥h§PŪ²´²yªº©}¥úª¬ºA¡A¦]¦¹¯S¦a±N¥ú½u©Mµø½u¾a±o«Üªñ¡A¦p¦Pª½±µ²´©³Ã誺ºc³y¨º¼Ë¡C

 

2.5 Red-eye in General Photography When shooting portraits with a regular camera, it's best to avoid capturing bright pupils, so the flash is kept as close to the lens as possible to prevent red-eye. However, photographic refraction uses this reflection to determine the refractive state of the eye, so the light source and line of sight are deliberately brought very close, similar to the structure of a direct ophthalmoscope.

 

 

2.6 ¥Hª½±µ²´©³Ã誺¥ú·½§@¬°¶¡±µ²´©³ÃèÀˬdªº¥ú·½¨Ï¥Î

¶¡±µ²´©³Ãè¥ú¾Ç­ì²z¤]¬O¤@¼Ë¡A¥ú½u©Mµø½u¾¨¶q¾aªñ¤~¬Ý±o¨ì²´©³¡A¥ú½uÂ÷µø½u¤Ó»·´N¬Ý¤£¨ì²´©³¤F¡Cª½±µ²´©³Ã誺ÂI¥ú·½¡A¥i¥H§@¬°¶¡±µ²´©³ÃèÀˬdªº¥ú·½¨Ï¥Î¡A¦]¬°¦³½Õ¥ú¾¹¥i½Õ¾ã«G«×¡A¯S§O¾A¦X¤p¨à²´¬ìªº²´©³Àˬd (¹Ï4-11)¡C±q²´©³Ã誺µø¤Õ¬Ý¥X¥h¡A¶¡±µ²´©³ÃèÀˬd©Ò¥Îªº¥Y³zÃè·|¤Ï¥ú¡A¦]¦¹³q±`³£¬O¥Ñµø¤Õ¤§¥~ªº¦ì¸m¥hÆ[¹î¡C¦pªG¥ú·½©Mµø½uªº¶ZÂ÷ (d) ¤Ó¤j¡A¥Ñ¤½¦¡¥iª¾¡A¦b§C«×¼Æ©}¥ú¤£¥¿ªº·t°Ï·|«Ü¼e¡A¤£§Q¶¡±µ²´©³ÃèÀˬd²´©³¡C±Nª½±µ²´©³Ãèµø¤Õ¤W½tªºÃ䮨¾¨¶q°µ¤p¡A¥ú¾Ç¤W´N¥i¥H§ó²Å¦X¶¡±µ²´©³ÃèÀˬdªº¥ú·½­n¨D¡C

 

2.6 Using the Light Source of a Direct Ophthalmoscope as a Light Source for Indirect Ophthalmoscopy

The optical principle of indirect ophthalmoscopy is the same: the fundus can only be seen when the light source and the line of sight are as close as possible; if the light source is too far from the line of sight, the fundus cannot be seen. The point light source of a direct ophthalmoscope can be used as a light source for indirect ophthalmoscopy because it has a dimmer to adjust the brightness, making it particularly suitable for fundus examinations in pediatric ophthalmology (Figure 4-11). Looking out from the viewing aperture of the ophthalmoscope, the convex lens used in indirect ophthalmoscopy will reflect light; therefore, observation is usually performed from a position outside the viewing aperture. If the distance (d) between the light source and the line of sight is too large, as shown by the formula, the dark area in low-power refractive errors will be very wide, which is not conducive to indirect ophthalmoscopy examination of the fundus. Making the upper edge of the viewing aperture of the direct ophthalmoscope as small as possible will better meet the optical requirements for the light source of indirect ophthalmoscopy.

 

 

¹Ï 4-11 ¥Hª½±µ²´©³Ã誺¥ú·½§@¬°¶¡±µ²´©³ÃèÀˬdªº¥ú·½¨Ï¥Î

 

Figure 4-11 shows the use of a direct ophthalmoscope light source as a light source for indirect ophthalmoscopy.

 

 

²Ä3 ¸`  ¤â«ù«¬Äá¼vÅç¥ú»ö

d = DF x Pu x L x RR¤½¦¡¸Ì¡ADF(·t°Ï)©MRR¦ì¦bµ¥¸¹ªº¦P°¼¡A¤GªÌ¬OÂù¦±½uªºÃö«Y (¹Ï4-12)¡C¦Ü©ó¤Ï¥úªº«G°ÏCrescentµ¥©ó1- DF¡A©ó¬O«G°Ï©M©}¥úªºÃö«Y«K¦p¤U¹Ï©Ò¥Ü¡C¦­´ÁªºÄá¼vÅç¥ú»öMTI¨Ì¤Ï¥ú«G°Ïªº¤j¤p¥h§PŪ«×¼Æ¡A¥ÑCrescent©M©}¥úªºÃö«Y¹Ï¨Ó¬Ý¡A¥i¥Hª¾¹D¦b§C«×¼Æ©}¥ú½d³ò¡A¥HCrescentªº¤j¤p¥h§PŪ©}¥úªº¸ÑªR«×¸û¨Î¡F¦b°ª«×¼Æ©}¥ú½d³ò¡A¸ÑªR«×´N«Ü®t¡C

 

Section 3 Handheld Photorefractive Optometry (MTI)

 

In the formula d = DF x Pu x L x RR, DF (dark area) and RR are on the same side of the equation, and their relationship is hyperbolic (Figure 4-12). The reflected bright area (Crescent) is equal to 1 - DF, thus the relationship between the bright area and refractive power is shown in the figure below. Early photorefractive optometry (MTI) used the size of the reflected bright area to determine the power. From the relationship between Crescent and refractive power, it can be seen that in the low refractive power range, using the size of Crescent to determine the refractive power resolution is better; in the high refractive power range, the resolution is very poor.

 

 

¹Ï4-12  DF(·t°Ï)©MRR(©}¥ú)¦ì¦bµ¥¸¹ªº¦P°¼¡A¤GªÌ¬OÂù¦±½uªºÃö«Y¡C

«G°Ï(=1-·t°Ï)©MRR(©}¥ú)ªº¦±½u¬O¹Ï2-30ªº¼Æ¾Ç­pºâ¡C

 

In Figure 4-12, DF (dark area) and RR (refractive error) are on the same side of the equal sign, and their relationship is hyperbolic.

 

The curves for the bright area (=1-dark area) and RR (refractive error) are mathematical calculations based on Figure 2-30.

 

 

d = DF x Pu x L x RR¤½¦¡¸Ì¡Ad©MRR¬O¦ì¦bµ¥¸¹ªº¨â°¼¡A¨âªÌ¬O½u©ÊÃö«Y¡CµL½×¦b¥ô¦ó©}¥ú½d³ò¡A¥Hd§PŪ©}¥ú³£¦³¦P¼Ë¦nªº¸ÑªR«×¡CHoward¨Ì¦¹·§©À¦b¤â¹qµ©«e­±©ñ¸m¤@¤ù¶¥±è¼Ëªº¯ÈªO (¹Ï4-13)¡A±q¶¥±èªºÃä½tÆ[´úÀû¤Õ¤Ï¥ú¡A¶¶µÛ¶¥±èªº¼Æ¦r³v®æ¦V¤W¡Aµø½u¡B¥ú½uªº¶ZÂ÷º¥º¥©Ô»·¡A¤Ï¥úCrescent¶V¨Ó¶V¤p¡A¨ì¹F¶¥±èªº¬Y¤@®æ®É¤Ï¥ú®ø¥¢¡A³o®ÉCrescent=0¡ADF=1¡A¨Ì¾Ú¤½¦¡¡ARR = d / Pu / L¡A¦pªGª¾¹DÀû¤Õ¤j¤p(Pu)©M´ú¸Õ¶ZÂ÷(L)¡A´N¥i¥H¥Ñdºë·Ç¦aºâ¥X©}¥ú­È(RR)¤F¡C

 

In the formula d = DF x Pu x L x RR, d and RR are on opposite sides of the equals sign, and they have a linear relationship. Regardless of the refractive range, interpreting refractive errors using d provides equally good resolution. Based on this concept, Howard placed a stepped cardboard plate in front of a flashlight (Figure 4-13), observing the pupillary reflection from the edge of the plate. As he moved upwards along the numbered steps, the distance between the line of sight and the light gradually increased, and the reflection (Crescent) decreased. At a certain step, the reflection disappeared, at which point Crescent = 0 and DF = 1. According to the formula RR = d / Pu / L, if the pupil size (Pu) and the testing distance (L) are known, the refractive value (RR) can be accurately calculated from d.

 

 

¹Ï4-13 ¤â¹qµ©«e­±©ñ¸m¤@¤ù¶¥±è¼Ëªº¯ÈªO¡Aµø½u¡B¥ú½uªº¶ZÂ÷º¥º¥©Ô»·¡A¤Ï¥úCrescent¶V¨Ó¶V¤p¡C

¤Ï¥ú®ø¥¢³B¡ACrescent=0¡ADF=1¡A¨Ì¾Ú¤½¦¡¡ARR = d / Pu / L¡C

 

Figure 4-13 shows a stepped cardboard panel placed in front of a flashlight. As the distance between the line of sight and the light source gradually increases, the glare (Crescent) decreases.

 

At the point where the glare disappears, Crescent = 0, DF = 1. According to the formula, RR = d / Pu / L.

 

 

±q³o¼ËªºÂú§Î¡A§Ú­Ìºc«ä¨Ã­Òij¤F¤â«ù«¬Äá¼vÅç¥ú»öªº»s§@¡C

 

From this prototype, we conceived and advocated for the development of a handheld photorefractive refractometer.

 

 

¤§«e´¿¸g±N³o­Ó·§©À½Ð¤Ñ¬z¥ú¾Ç¼t¶}¼Ò»s§@¡A¤]©M¥x¤jÂå°|Âå¤u«Ç¦X§@¡A§ï³yHeineªº²´©³Ãè¡A»s§@¹Lªì¨Bªº¦¨«~ (¹Ï4-14)¡C´ú¸ÕªÌ¤W¤U±À°Ê±À±ì¡A½ÕÅܵø½u¡B¥ú½uªº¶ZÂ÷¡A¥Ñµø¤ÕÆ[¹îÀû¤Õ¤Ï¥úªº¤j¤p¡A ¤Ï¥ú¥Ñ¤jº¥¤p¡A¥H¤Ï¥ú®ø¥¢ÂI (DF=100%=1)§@¬°§PŪªº¨Ì¾Ú¡AŪ¥X©}¥ú­È¡C

 

Previously, we commissioned Tianjin Optical Factory to develop and manufacture molds for this concept. We also collaborated with the Biomedical Engineering Department of National Taiwan University Hospital to modify Heine's fundus lens and produced a preliminary finished product (Figure 4-14). The tester pushes the lever up and down to adjust the distance between the line of sight and the light source, and observes the size of the pupil reflection through the viewing port. The reflection gradually decreases, and the vanishing point of the reflection (DF=100%=1) is used as the basis for interpretation to read the refractive value.

 

 

¹Ï4-14 a¤Ñ¬z¥ú¾Ç¼t»s§@¤â«ù«¬Äá¼vÅç¥ú»öÂú«¬

 

Figure 4-14 a Prototype of a handheld photorefractive optician manufactured by Tianjin Optical Factory

 

 

¹Ï4-14 b¥x¤jÂå°|Âå¤u«Ç»s§@¤â«ù«¬Äá¼vÅç¥ú»öÂú«¬

 

Figure 4-14b shows a prototype of a handheld photorefractive refractometer produced by the Biomedical Engineering Laboratory of National Taiwan University Hospital.

 

 

¨Ò¦p´²Àû«áÀû¤Õ8mm¡A´ú¸Õ¶ZÂ÷0.5m¡A®M¤J¤½¦¡d = DF x Pu x L x RR¡Ad = 1 x 8 x 0.5 x RR à d = 4mm x RR¡A¤]´N¬O¦b¥ô¦ó©}¥úªº½d³ò¡A©}¥ú1D¦³4mmªº¸ÑªR«×¡A³oÀ³¸Ó¬O«D±`¹ê¥Îªº¤F¡C

 

For example, if the pupil is 8mm after dilation and the test distance is 0.5m, applying the formula d = DF x Pu x L x RR, we get d = 1 x 8 x 0.5 x RR „³ d = 4mm x RR. This means that in any refractive range, 1D refractive power has a resolution of 4mm, which should be very practical.

 

 

©M¥«°âªºÄá¼vÅç¥ú»ö¤£¦Pªº¬O¡A¥L­Ì´Â¦VÅç¥ú¾÷ªº¤è¦V³]­p¡A¦Ó§Ú­Ì­Òij´Â²´©³Ãè/ºô½¤Ã誺¤è¦V¥h³]­p¡B¥h»s§@¤@¤ä¤â«ù¦¡ªºÄá¼vÅç¥ú»ö¡C¾¬±æ¦b²´¬ìªù¶E±`³W³]¸mªºª½±µ²´©³Ãè©Mºô½¤Ã褧¥~¡A¦A²K¤@¤ä¤p¨àÅç¥ú¥Îªº§Q¾¹¡C

 

Unlike commercially available photorefractive instruments, which are designed like refractometers, we advocate designing and manufacturing a handheld photorefractive instrument that resembles a fundus microscope/retinal microscope. Our hope is to add another useful tool for pediatric refraction, in addition to the direct fundus microscope and retinal microscope routinely provided in ophthalmology clinics.

 

 

¦p«e©Ò­z¡AÅç¥ú¾÷«¬¦¡ªºÄá¼vÅç¥ú»ö¬O¥Ñ±×¦VªºÀû¤Õ¤Ï¥ú¥h­pºâ©}¥ú­È¡A¦Ó§Ú­Ì­Òijªº¤â«ù¦¡Äá¼vÅç¥ú»ö¬O¥Ñ´ú¸ÕªÌ±N¥ú·½½Õ¾ã¦Ü´²¥ú¶bªº¤è¦V (¹Ï4-15)¡A¤§«á¥Ñ¥¿¦VªºÀû¤Õ¤Ï¥ú§PŪ©}¥ú­È¡AÃþ¦ü©óºô½¤ÃèÀ˼vªk§PŪ´²¥ú¨¤«×ªº§@ªk¡C§Ú­Ì·Pı¥Ñ¥¿¦VªºÀû¤Õ¤Ï¥ú¥h§PŪ©}¥ú«×¼ÆÀ³¸Ó·|§ó¥[ª½±µ©M·Ç½T¡C

 

As mentioned earlier, refractometer-type radiographs calculate refractive values ​​based on oblique pupillary reflections. However, our proposed handheld radiograph method involves the user adjusting the light source to align with the astigmatic axis (Figure 4-15), and then interpreting the refractive value using positive pupillary reflections, similar to how retinoscopy is used to determine the astigmatic angle. We believe that interpreting refractive power using positive pupillary reflections would be more direct and accurate.

 

 

¹Ï4-15 ¤â«ù¦¡Äá¼vÅç¥ú»ö¬O¥Ñ´ú¸ÕªÌ±N¥ú·½½Õ¾ã¦Ü´²¥ú¶bªº¤è¦V

 

Figure 4-15 shows a handheld photorefractive refractometer, in which the tester adjusts the light source to the direction of the astigmatic axis.

 

 

¤â«ù¦¡Äá¼vÅç¥úªk­º¥ýÆ[¹îÀû¤Õ¤Ï¥úªº¤è¦V¡A½ÕÅÜ´²¥úªº¨¤«×¡F¤§«á½ÕÅܤϥúªº¤j¤p¡A¥hŪ¨ú³o­Ó¶b¦Vªº©}¥ú­È¡A¦AÂà90«×¡A½ÕÅܤϥú¤j¤p¡AŪ¨ú¥t¤@­Ó¶b¦Vªº©}¥ú­È¡C «D±`Ãþ¦ü©óºô½¤ÃèÀ˼vªº¾Þ§@¤èªk¡A¦ý¬O¤£»Ý­n©ñ¸m¤¤©MÃè¤ù¡A¾aªñÀ¦¥®¨àªº²´«e¡A¥i¥HÁ×§KÀ¦¥®¨à®`©È¡B°kÁשM­ú¾x¡C

 

The handheld photorefractive method first observes the direction of the pupillary reflection and adjusts the angle of astigmatism; then it adjusts the magnitude of the reflection to read the refractive value along this axis, then rotates 90 degrees, adjusts the magnitude of the reflection again, and reads the refractive value along the other axis. It is very similar to the procedure for retinal retinoscopy, but it does not require the placement of a neutralizing lens. It is placed close to the infant's eyes, which can prevent the infant from becoming afraid, trying to escape, or crying.

 

 

¥«°âªºÄá¼vÅç¥ú»ö­n¦b©T©wªº¶ZÂ÷§@´ú¸Õ¡A½Õ¾ã´ú¸Õªº¶ZÂ÷±`±`»Ý­nªá®É¶¡¥hºË·Çµø¼Ð¡C²{¤µªº¬ì§Þ¦³«D±`ºë½Tªº´ú¶Z»ö¡A¦pªG¥i¥H¤º«Ø´ú¶Z»ö¡Aª½±µ±o¨ì¤½¦¡¸ÌªºL¡A´N¤£¥²¦b©T©wªº¶ZÂ÷´ú¸Õ¡A¦Ó¥B©}¥ú­ÈR=RR-1/L¤]¥i¥H¥ÑL­È»´ÃP­pºâ±o¨ì¡C

 

Commercially available refractometers require testing at a fixed distance, and adjusting the testing distance often takes time to aim at the target. Modern technology offers highly accurate rangefinders. If a rangefinder could be built-in to directly obtain the value of L in the formula, testing at a fixed distance would be unnecessary, and the refractive value R = RR - 1/L could be easily calculated from the value of L.

 

 

¤½¦¡¤¤Àû¤Õªºª½®|Pu¡AµL½×´²Àû»P§_¡A¤]¥i¥H§Q¥Î¹q¸£¹Ï¾Çªº¬ì§Þ´ú¶q±oª¾¡C¦¹¤@¤â«ù¦¡Äá¼vÅç¥ú»öªº­Òij»Ý±o¨Ì¿à¤u¬ã°|ªº°Ñ»P¡B³]­p»P¥I½Ñ°õ¦æ¡C

 

The pupil diameter Pu in the formula can be measured using computer graphics technology, regardless of whether the pupil is dilated. This proposal for a handheld photorefractive refractometer requires the participation, design, and implementation of the Industrial Technology Research Institute (ITRI).

 

 

 

Recommended readings and references

1. Howland HC, Howland B. Photorefraction: a technique for study of refractive state at a distance. J Opt Soc Am 1974;64:240-9.

2. Howland HC, Braddick O, Atkinson J, Howland B. Optics of photorefraction: orthogonal and isotropic methods. J Opt Soc Am 1983;73:1701-8.

3. Howland HC. Photorefraction of eyes: history and future prospects. Optom Vis Sci 2009;86(6):603-6.

4. Howland HC, Sayles N, Cacciotti C, Howland M. Simple pointspread retinoscope suitable for vision screening. Am J Optom Physiol Opt 1987;64(2):114-22.

5. Kaakinen K. A simple method for screening of children with strabismus, anisometropia or ametropia by simultaneous photography of the corneal and fundus reflexes. Acta Ophthalmol 1979;57:161-71.

6. Kaakinen K. Photographic screening for strabismus and high refractive errors of children aged 1¡V4 years. Acta Ophthalmol (Copenh) 1981;59:38¡V44.

7. Wang AH. Photorefraction and retinoscopy with direct ophthalmoscope and laser pointer. Invest Ophthalmol Vis Sci 1999:30(4):56.

8. Wang AH. Handheld photorefractor. 18th Congress of the Asia-Pacific Academy of Ophthalmology, March 10-14. 2001, Taipei, Taiwan.

9. Wesemann W, Norcia AM, Allen D. Theory of eccentric photorefraction (photoretinoscopy): astigmatic eyes. J Opt Soc Am (A) 1991;8:2038¡V47.

 

 

This article is dedicated to the teachers at The Smith-Kettlewell Eye Research Institute (SKERI): Dr. Arthur Jampolsky, Dr. Alan Scott, Dr. Anthony Norcia, Dr. Eric Sutter, and Dr. Christopher Tyler. I vividly remember my year as a pediatric ophthalmology fellowship in San Francisco, a place brimming with talent and beauty, from 1990 to 1991.

 

Author: Ai-Hou Wang

Education: Bachelor of Medicine, National Taiwan University / Doctor of Clinical Medicine, National Taiwan University / Fellow, Pediatric Ophthalmology and Strabismus, The Smith-Kettlewell Eye Research Institute (SKERI) and Pacific Presbyterian Medical Center, San Francisco, USA.

Experience: Resident and Attending doctor, Ophthalmology Department, National Taiwan University Hospital / Associated Professor, Ophthalmology Department, National Taiwan University College of Medicine.

Current Position: Consultant, Ophthalmology Department, Cathay General Hospital / Attending doctor, Universal Eye Center.