CROSSED CYLINDER LENSES REFRACTOR

Abstract: A new lens system and method of use for otherwise conventional refractors comprising a synchronized, variable crossed cylinder lens attachment (12) and selectable fixed cros­ sed cylinders (22) which may be placed in the examining optical path. The synchronized, variable crossed cylinder lens attach­ ment (12) replaces the Jackson crossed cylinder lens and rotates in step with rotation of the cylinder lens axis. Batteries of strong and weak crossed cylinder lenses (26, 27) replace the strong and weak cylinder lenses of conventional refractors. Refractive techniques utilizing the disclosed crossed cylinder lens systems are also described.

Description: A refractor is a known ophthalmic instrument having batteries of trial lenses used to determine and remedy the refractive errors of a patient's eye. In modern refractors there are similar left and right batteries which include lens disks or cells containing lenses of spherical and cylindrical power, means for rotating the lens cells to place a lens or a combination of lenses before the eye under examination and a means for setting the axis of the cylinder lens. A modern refractor also includes a synchronized Jackson crossed cylinder for use as a check test for the neutralization of astigmatism (cylinder power and axis), as well as auxiliary lenses. Techniques for refracting utilizing the Jackson crossed cylinder and the various spheres and cylinders of the refractor are well known. As refraction is presently practiced, the patient's refractive error is expressed in a sphere and a cylinder at a certain axis, which in reality represents the spherical equivalent plus the final crossed cylinder at a certain axis that is required to neutralize the patient's refractive error. Present refractors are designated as having either positive or negative cylinders. Techniques of refracting have been designed to utilize the negative cylinders (negative theory of refracting). The negative theorem can be converted for the use of positive cylinders (positive theory of refracting) but is awkward. Similar techniques for retinoscopy have been developed mainly for positive cylinders. Both the negative and positive cylinders can be utilized in a manifest refraction when a meridional straddle is maintained. This final manifest refraction is the most accurate, as well as the most time consuming part of the refraction technique. It is the manifest refraction from which the final refraction is determined in cooperative patients, which probably comprise 95% of the average ophthalmologist's and optometrist's refraction cases. A well known problem for the refractionist in performing the manifest refraction is maintaining a meridional balance throughout the manifest refraction. In the technique commonly performed with the conventional refractor, the refractionist is required to move one spherical lens and two cylindrical lenses in order to show the patient two images which are different by a minimum cylindrical correction. However, a major optical error is introduced by conventional refractors during refraction of patients having am astigmatic error in accordance with this technique. A 0.125D ("D" stands for "diopter") spherical equivalent jump of the images presented to the patient occurs when such refractors are used in the final manifest refraction by presenting successive cylinder lenses. This spherical equivalent jump occurs because cylinder lenses have a spherical component (equal to one-half of the cylindrical component of opposite sign), and conventional trial lenses are graded in 0.25 diopter increments. Thus, successive cylinder lenses change the resulting spherical component by 0.125 diopter, which means the exact meridional balance can be retained only with every other cylinder increment. The problem for the patient is that the two crossed cylinder images presented to him are different by a spherical equivalent of 0.125D, and produce an inequality in image shape, i.e. the circle of least confusion becomes oval. That is, if one crossed cylinder image is a circle, the other image is an oval. The images are therefore dissimilar. (This visual comparison is obvious when a video camera, which is made astigmatic, is refracted. One image is in focus and the other is out of focus.) With the negative cylinder technique of refracting, accommodation is introduced every other time the cylinder power is changed, and with the positive cylinder technique of manifest refracting, a fog is introduced every other time the cylinder power is changed. The refractionist can make the image comparisons for the patient equal or constant, that is comparing circles to circles or ovals to ovals by introducing a 0 .125D sphere auxiliary lens. However this requires the refractionist to change five lenses (two auxiliary lenses, one spherical lens and two cylindrical lenses) in order to show the patient just two similar images of no spherical equivalent difference and of a circle of least confusion that is decreasing or increasing in size. Thus, a technique utilizing an auxiliary lens in this manner is impractical and confusing in practice. The U.S. patent to J. D. Moller, No. 4,385,813, teaches a computerized refractor using sphere and cylinder lenses and intended to solve the refractor manipulation problems presented by conventional refractors, but this approach is expensive and does not prevent the 0.125D spherical jump described above, although it could perhaps be adapted to accomplish that with different programming or different lenses. Another problem that the refractionist has is the inability to maintain the same meridional balance while using the Jackson crossed cylinder in order to check the cylinder power. If a fog is produced, as with the positive cylinder phoropters, the refractionist may be inclined to prescribe too much against-the-rule astigmatism. Theoretically, it is also possible to prescribe too much with-the-rule astigmatism when negative cylinders are used with a Jackson crossed cylinder in an eye which has had a cycloplegic. Another problem the refractionist has is the inability of many patients, especially older ones, to respond to the use of astigmatic dials. The reason for this difficulty is obvious when one realizes that the theory of the astigmatic dial is based on the conoid of Sturm, which exists only in a thin lens system, whereas the eye is a complicated thick lens system. An additional problem that the refractionist has is teaching a technician or student to refract, which takes many years of experience. Computerized objective/subjective refractors have reduced this obstacle; however their cost is high, their accuracy debatable, and it is questionable whether such refractors increase refraction efficiency. The mechanics of moving the lens wheels of the phoropter is most confusing and difficult to teach technicians and ophthalmologists. It is very important to the refractionist to be able to maintain the same system of lens changes when he increases and/or decreases the crossed cylinder powers while maintaining the spherical equivalent. An article by W. S. Dennett, "The Stokes' Lens for Measuring Astigmatism" published prior to 1900, describes utilization of variable crossed cylinder lenses or "Stokes Lenses" in connection with a mounted trial frame to refract patients. The Dennett structure does not, however, present numerous advantages achieved by the present invention, and the Stokes lens has been little used in refraction despite its long availability. US-A-3,822,932 discloses apparatus for measuring optometric spherical and cylindrical optic correction to the eye, the apparatus employing counter-rotating crossed cylinder or cylinder lenses. The present invention which is defined in the appended claims, avoids the above mentioned problems experienced by the patient and refractionist by use of a synchronized variable crossed cylinder attachment for a refractor and/or a refractor using selectable crossed-cylinder lenses rather than the cylinder lenses conventionally used. The synchronized variable crossed cylinder attachment or assembly comprises two crossed cylinder lenses, or two cylinder lenses of equal power but opposite sign, mounted so as to be positionable in front of the viewing tube of the refractor. The lenses are rotatable in opposite directions at equal rates, and the resulting axis of the lens pair is synchronized to rotate in step with rotation of cylinder lenses in the cylinder lens discs of the refractor. Thus the present invention provides a simple solution to the above problems, both for the refractionist and the patient, by providing a simple manual refractor that will eliminate unequal visual comparisons. The present invention also provides the refractionist with a faster technique of varying the crossed cylinders while maintaining the same spherical equivalent. With the replacement of the conventional cylinders in a refractor with crossed cylinders, not only is the 0.125D image jump eliminated, but the refractionist is also able to maintain a perfect meridional straddle by changing only one lens (crossed cylinder) instead of three lenses (the auxiliary lens, the sphere lens and the cylinder lens) per change of the refraction crossed cylinder while maintaining the same spherical equivalent. An advantage of the invention is that practice of the two theorems of refracting (positive and negative) cylinders) become the same when a perfect meridional balance is maintained after a spherical equivalent is determined. A further advantage of the invention is that the technique of fogging is eliminated by scanning for astigmatism in 45° increments with the selectable crossed cylinder lenses or 30° increments with the synchronized variable crossed cylinder lens assembly. The synchronized crossed cylinder lens system of the present invention allows the refractionist to show the patient several hundred crossed cylinder powers at different angles in a matter of only a few seconds. If astigmatism is detected, it may then be confirmed with the crossed cylinder refractor at the determined axis. This technique of refracting is similar to that taught in the U.S. patent J.D. Moller, No. 4,385,813; which is incorporated herein by reference however, Moller requires a computer and step motor-controlled refractor and does not use crossed cylinder lenses as taught in the present invention. Another advantage of the present invention is that the technique of fogging is faster, as well as mechanically easier, with the use of the crossed cylinder refractor and/or the synchronized variable crossed cylinder lens assembly disclosed. An additional advantage of the present invention is the elimination of the iatrogenic induction of with-the-rule or against-the-rule astigmatism inherent with the Jackson crossed cylinder refraction technique when a perfect meridional balance is not maintained as in previous techniques. The variable crossed cylinder assembly of the present invention can be used in a manner to duplicate the Jackson crossed cylinder, while the selectable crossed cylinder lens system disclosed will maintain a perfect meridional straddle. A further advantage of the synchronized variable crossed cylinder lens assembly of the present invention is the replacement of the error-prone, audio-visual responses that are required with conventional refractors with a silent visual response. An additional advantage of the present invention is that it gives the refractionist the ability to use positive or negative cylinders in one refractor lens system, whereas now the refractionist purchases either a positive cylinder refractor or a negative cylinder refractor. Another advantage of the present invention is that the synchronized variable crossed cylinder lens assembly allows the refractionist to detect and neutralize any astigmatism many times faster than is presently possible. Other advantages to the refractionist are: The use of cycloplegics is rarely required, even for the young patient. Objective refractors are not required to obtain an initial beginning point for the manifest refraction. Retinoscopy is rarely required to perform an endpoint manifest refraction. The times required to perform a manifest refraction for pathological or non-pathological patients is very significantly decreased. The accuracy of refraction is significantly improved, thus reducing the optical remake rate. Other objects, features and advantages of the present invention will become apparent with reference to the remainder of the specification, claims and drawings. A refractor in accordance with the present invention will now be described in greater detail, by way of example, with reference to the accompanying drawings, in which:- FIG. 1 is a front view of a substantially conventional refractor taken from the practitioner's side of the instrument showing the synchronized variable crossed cylinder lens assembly of the present invention attached to the yoke of the refractor, and showing the left eye battery in elevation and the right eye battery partly in elevation and partially broken away to reveal the forward crossed cylinder lens disc. FIG. 2 is a cross-sectional view of the right eye battery taken substantially along the lines 2-2 of FIG. 1, illustrating the selectable crossed cylinder assembly and the synchronized variable crossed cylinder assembly of the present invention. FIG. 3 is an enlarged cross-sectional view of the synchronized variable crossed cylinder structure taken along the lines 3-3 of FIG. 1. FIG. 4 is an enlarged front view of the synchronized variable crossed cylinder assembly of the present with gears shown in phantom lines. FIG. 1 is a front view of a substantially conventional refractor 10. The refractor 10 includes a right eye battery 16 and a left eye battery 18, these batteries being essentially identical. FIG. 1 shows the synchronized variable crossed cylinder lens attachment or assembly 12 of the present invention attached to the yoke or turret 14 of the refractor, and the right eye battery 16 is partially broken away to show the selectable crossed cylinder lens system 22 of the present invention, which is also identified on FIG. 2. Only the synchronized variable crossed cylinder lens assembly 12 and the selectable crossed cylinder lens system 22 of the present invention as incorporated in an otherwise conventional refractor 10 will be discussed. FIG. 1 shows the refractor 10 from the refractionist's side, and this side will be referred to as the front side of the instrument. The major component parts of each battery 16 and 18 (see FIGS. 1 and 2) include a sphere lens assembly 20, a selectable crossed cylinder lens assembly 22 and a synchronized variable cylinder attachment 12. The patient positions his head to the rear of the instrument so that each of his eyes is in alignment with the viewing tubes 24. SELECTABLE CROSSED CYLINDER LENS ASSEMBLY The selectable crossed cylinder lens assembly 22 may comprise crossed cylinder lenses 26 and 27 mounted in a cylinder lens assembly of the type disclosed in U.S. Patent No. 3,498,699, which patent is incorporated herein by reference in its entirety. It thus includes a pair of crossed cylinder lens discs 28 and 30 shown in FIG. 2. The forward disc 28 carries weak crossed cylinder lenses 26 and the rear disc 30 carries the strong crossed cylinder lenses 27. The strong and weak crossed cylinder discs 28 and 30 carry sets of strong and weak crossed cylinder lenses of various powers mounted circumferentially on the discs, so that a selected lens will, upon rotation of the discs, come into alignment with the viewing tube 24. Each disc 28 and 30 carries four lenses and has one open position 32 which is aligned with the viewing tube 24 when no crossed cylinder lens within such disk 28 or 30 is desired. The crossed cylinder (X/CYL) lens powers utilized in the preferred embodiment are as follows: WEAK X/CYL LENSES MOUNTED IN WEAK DISC 28 STRONG X/CYL LENSES MOUNTED IN STRONG DISC 30 ±0.125 D ±0.625 D ±0.25 D ±1.25 D ±0.375 D ±1.875 D ±0.50 D ±2.50 D The power of the combination of the weak and strong crossed cylinders 26 and 27 seen through the viewing tube 24 may be presented in a display 34 which indicates the total crossed cylinder lens power as seen through the viewing tube. For a positive crossed cylinder refractor, the orientation of the plus axis of the weak and strong crossed cylinders 26 and 27 as seen through the viewing tube will be indicated on to the crossed cylinder axis scale 36. The designation of the positive or negative crossed cylinder refractor as soon in the display 34 may include the total crossed cylinder sphere power followed by the total crossed cylinder cylindrical power. For a positive crossed cylinder refractor, the sphere power value should be red and the cylindrical power value black in the display 34. For a negative crossed cylinder refractor, the sphere power value in the display 34 should be black and the cylinder power value red because, by convention, black designates positive lenses and red negative lenses. A suitable structure for accomplishing the desired objective of mounting crossed cylinder lenses 26 and 27 so that they may be selectively positioned in line with viewing tube 24 and may be rotated is disclosed in U.S. Patent No. 3,498,699, mentioned above, particularly at columns 5 and 6. As will be readily appreciated, the described arrangement permits the refractionist to control not only the total power of the crossed cylinder lenses 26 and 27 in alignment with the viewing tube 24 (by means of crossed cylinder power knob 37), but also the orientation of the axes of these lenses 26 and 27 (by means of cylinder axis rotation knob 39). The described selectable crossed cylinder lens assembly makes possible the following crossed cylinder powers: WEAK X-CYL LENS IN WEAK DISC 28 STRONG X/CYL LENS IN STRONG DISC 30 DISPLAY X/CYL (expressed in sphere plus cylinder notation) 0.00 0.00 0.00 * ±0.125 0.00 0.12/0.25 ±0.25 0.00 0.25/0.50 ±0.375 0.00 0.37/0.75 ±0.50 0.00 0.50/1.00 0.00 ±0.625 0.62/1.25 ±0.125 ±0.625 0.75/1.50 ±0.25 ±0.625 0.87/1.75 ±0.375 ±0.625 1.00/2.00 ±0.50 ±0.625 1.12/2.25 0.00 ±1.25 1.25/2.50 ±0.125 ±1.25 1.37/2.75 ±0.25 ±1.25 1.50/3.00 ±0.375 ±1.25 1.62/3.25 ±0.50 ±1.25 1.75/3.50 0.00 ±1.875 1.87/3.75 ±0.125 ±1.875 2.00/4.00 ±0.25 ±1.875 2.12/4.25 ±0.375 ±1.875 2.25/4.50 ±0.50 ±1.875 2.37/4.75 0.00 ±2.50 2.50/5.00 ±0.125 ±2.50 2.62/5.25 ±0.25 ±2.50 2.75/5.50 ±0.375 ±2.50 2.87/5.75 ±0.50 ±2.50 3.00/6.00 SYNCHRONIZED VARIABLE CROSSED CYLINDER ASSEMBLY The synchronized variable, rotatable crossed cylinder attachment or assembly 12 of the present invention (FIGS. 1, 2, 3 and 4) includes lenses 40 and 42 (FIG.3), which may be crossed cylinders of equal power or cylinders of equal power but opposite sign. Lenses 40 and 42 are minimally separated. Typically, such lenses 40 and 42 are each a ±0.50D crossed cylinder, but may be of any equal power up to a ±1.50D or ±3.00D crossed cylinder. If, instead of crossed cylinders, cylinders are used for lenses 40 and 42, the cylinder powers are equal and of the opposite sign and the power may be between 1.00D and 3.00D. Referring to FIG. 4, when the thumb wheel 44 of the assembly 12 is turned, the two cylinders or crossed cylinders 40 and 42 will rotate in opposite directions to each other at an equal rate relative to a stationary combined lens axis 52. The combined lens axis 52 will always bisect the angle formed by: (a) the axes of lenses 40 and 42 (if cylinder lenses are used), or (b) the negative axis of one lens 40 and the positive axis of the other lens 42 (if crossed cylinder lenses are used). The resulting power of the assembly 12 will be indicated by the position of pointer 46 on scale 48 on the front of assembly 12. The power of the combined lenses 40 and 42 will be zero when their axes are parallel (when cylinder lenses of equal but opposite sign are used) and zero when the plus (+) axis of one lens 40 overlies the minus (-) axis of the other lens 42 (when crossed cylinder lenses are used). The assembly 12 is attached to a yoke or turret 14 to swing it between a position in alignment with the viewing tube 24 and a position clear of the tube 24 (as is illustrated in FIG. 1.) This may be accomplished by utilizing the turret structure described in U.S. Patent No. 3,498,699, particularly at columns 6-8, for mounting a Jackson crossed cylinder and a rotary prism loupe. The axis 52 of the synchronized variable crossed cylinder assembly 12 must be maintained parallel to the axis 54 of the lenses 26 and 27 in the selectable crossed cylinder lens assembly 22 (or parallel to the axis of cylinder lenses so mounted if the crossed cylinder lens assembly 22 of the present invention is not used), and such axes must be simultaneously controlled by the cylinder axis rotation knob 39. This may be accomplished by utilizing the structure disclosed in U.S. Patent No. 3,498,699 for setting the cylinder axis parallel with the cross cylinder flip axis of the Jackson crossed cylinder structure disclosed therein. Means should also be provided to permit 45° rotation of the selectable crossed cylinder lens assembly 12 for the purpose of the neutralization of astigmatism by turning the thumb wheel 44 and in performing the 4-lens test for confirming the cylinder axis as described under "Operations" below. Such a 45° rotation means may be provided by utilization of the structure for permitting limited rotation of the Jackson crossed cylinder loupe disclosed in U.S. Patent No. 3,498,699, mentioned above, particularly at column 8. Briefly, a flat circular spring 50 overlaps the ring gear 51 and is fixed by screws 53 at opposed points of the inner face of the loupe 55. An indexing ball 57 is captured between the spring 50 and the inner face of ring gear 51. The ball 57 is rotatably captured by a pair of detents 59 located 45° apart on the inner face of ring gear 51, thus permitting rotation of the entire assembly 12 between such predetermined positions. A substantially suitable structure for the synchronized variable crossed cylinder lens attachment may be provided by substituting lenses 40 and 42 in place of the prisms normally used in a conventional Risley rotary prism loupe attachment and by recalibrating the scale on the face of the Risley prism attachment. Such a modified Risley prism attachment may then be mounted as illustrated in FIGS. 3 and 4 on the loupe 55, which corresponds to loupe 158 of the Jackson crossed cylinder loupe assembly described in U.S. Patent No. 3,498,699. This modified Risley prism loupe structure and its linkage by means of the conventional Jackson crossed cylinder loupe mount to the cylinder axis controlling mechanism of a conventional refractor will provide the mechanics required for the synchronized variable crossed cylinder lens attachment 12 of the present invention. Improved operation may be achieved, however, by gearing modification to utilize a greater arc in the scale 48. Ideally, pointer 46 should rotate 180° or slightly less at the same time the axes of lenses 40 and 42 rotate 90° to each other. This will provide the least crowded scale 48 possible. Mounting of the modified Risley prism attachment is accomplished by mounting housing 78 on a cup 66, which in turn is seated on loupe 55. As one skilled in the art will readily appreciate, cup 66 may be any convenient shape which provides mating between housing 78 and loupe 55. A tubular shield 68 having the same outer diameter as cup 66 may be mounted around loupe 55 with a set screw or other convenient means to provide an attractive outer appearance for assembly 12. FIG. 4 is a front view of the synchronized variable crossed cylinder lens assembly 12 constructed from a modified Risley prism attachment. The rotary thumb wheel 44 with its underlying gear of a smaller diameter 58 is the drive system which rotates ring gear driving gears 60 and 62. Thumb wheel gear 58 rotates driving gear 60, which rotates both ring gear 70 (in which cylinder lens 40 is mounted) and driving gear 62. Gear 62 in turn rotates ring gear 72, in which lens 42 is mounted, at an equal rate but in the opposite direction from ring gear 70. This is accomplished because driving gear 60 meshes with the front crossed cylinder lens 40 ring gear 70 and driving gear 62 meshes with the rear crossed cylinder lens 42 ring gear 72. Rotary thumb wheel 44 also rotates pointer ring gear 64 which carries pointer 46. Pointer 46 indicates the combined power of lenses 40 and 42 on scale 48, which is mounted on housing 78. Alternatively, thumb wheel 44 could drive intermediate gears of appropriate diameter, which would in turn drive pointer ring gear 64 in order to modify the rate at which pointer ring gear 64 rotates relative to rotation of crossed cylinder lenses 40 and 42, as described above. OPERATIONS A refractor modified in accordance with the present invention may be used by first using the spherical lens in sphere lens assembly 20 to produce a fog. With the patient either wearing or not wearing his glasses and observing the smallest discernible visual acuity line, this fog is then reduced in 0.25D steps in order to determine the spherical equivalent. The typical patient responses to such fog reduction would be: blurred--clear--sharper and darker. The "blurred" response would typically represent a 0.50D fog, the "clear" response a 0.25D fog and the "sharper and darker" response the spherical equivalent. The synchronized variable crossed cylinder assembly 12 is then rotated in line with the viewing tube 24. The spherically precorrected eye is then offered various crossed cylinder powers by turning the thumb wheel 44 in the positive crossed cylinder scale direction. If there is no improvement in the spherical precorrected eye, the thumb wheel 44 is rotated in the opposite direction to direct the pointer 46 in the negative crossed cylinder power range. This power reversal of the assembly 12 is performed without rotating the cylinder axis knob 39. If there is no improvement in the spherical precorrected visual acuity, the cylinder axis knob 39 is rotated 45° (thereby rotating synchronized crossed cylinder attachment 12 by 45°), and the crossed cylinder power scanning technique is repeated as described. A given positive crossed cylinder is equivalent to the same negative crossed cylinder at 90° to the axis of the given positive crossed cylinder. Thus, the refractionist can now think of any crossed cylinder phoropter in accordance with the present invention as a positive or negative crossed cylinder phoropter. If one thinks in positive crossed cylinders, the equivalent negative crossed cylinder is the power of the positive crossed cylinder at an axis 90° away from the axis of the positive crossed cylinder of the assembly. If one thinks in negative crossed cylinders, it is the reverse. Therefore, the refractionist can scan the three-dimensional visual acuity field with a two-dimensional synchronized variable crossed cylinder power assembly 12. This allows the refractionist to scan the visual acuity field in 45° intervals by only rotating the crossed cylinder axis 52 by means of knob 37 and turning the thumb wheel 44 in opposite directions. The refractionist also may scan in 30° intervals. With both scanning techniques, the patient is shown several hundred sets of perfect crossed cylinders. If there is no improvement in the spherical preconditioned eye, the distant refraction for that eye is then complete. The identical procedure is then repeated for the other eye followed by the routine determination of the phorias and reading add. This is the routine for a stigmatic patient. For an astigmatic patient, the spherical preconditioned eye would enjoy an improvement in the distant visual acuity in one of the quadrants scanned using the 45° or 30° scanning techniques as the crossed cylinder power is increased or decreased to produce the optimal vision. When the proper crossed cylinder power is determined, the synchronized crossed cylinder axis 52 is rotated clockwise and counter-clockwise 45° to either side of the above noted axis to produce the least non-distorted clear vision. After the proper refractive axis of the patient is determined through the patient's responses, the final power of the synchronized crossed cylinder assembly is increased or decreased to produce the optimal visual acuity. The final refractive error is the sum of the sphere power of the sphere lens assembly 20 and the power of synchronized crossed cylinder attachment 12 displayed on scale 48 at a designated axis 52 displayed on axis scale 36. An alternative to neutralizing astigmatism with the synchronized variable crossed cylinder lens attachment 12 is to dial predetermined crossed cylinder powers into the viewing tube 24 by turning the crossed cylinder power knob 37 to the same power setting as the variable attachment 12. The attachment 12 is then rotated out of the field of the viewing tube 24. Stronger or weaker crossed cylinders 26, 27 are then selected by rotating disks 28 and 30 by means of cylinder selector knob 37 to produce the optimal vision for the astigmatic patient after the proper axis has been determined as described in the previous paragraph. It should be noted that it is very important to overcorrect the astigmatism correction in order to show the patient a new image he has not seen and then reduce the blurred overcorrected image in ±0.125D crossed cylinder steps to produce the optimal visual acuity. Another alternative for the detection and neutralization of astigmatism is to utilize crossed cylinder lens powers of ±0.125D, ±0.25D, ±0.375D, or ±0.50D in the selectable crossed cylinder lens assembly 22 to scan for astigmatism. The patient is allowed to compare his spherical preconditioned visual acuity and 0.00D crossed cylinder power in the viewing tube to ±0.125D crossed cylinder power in the viewing tube. If there is no improvement in the visual acuity, cylinder axis rotation knob 39 is rotated 30° or 45°, depending on the refractionist's preference, and the procedure repeated. If the visual acuity is improved with 0.00D crossed cylinder power in the viewing tube in all 30° or 45° meridians as compared to the ±0.125D lens, there is no astigmatism. If there is an improvement with the ±0.125D lens at a certain meridian, the power of the crossed cylinder is increased to produce the optimal visual acuity, after which the crossed cylinder axis 54 is rotated in a clockwise and counter-clockwise manner by means of axis knob 39 to produce the clearest nondistorted vision. The final crossed cylinder power is then checked. If the refractionist suspects a non-discriminating patient or moderate astigmatism, he may scan with crossed cylinders of larger powers (±0.25D, ±0.375D, or ±0.50D). The axis may be checked by overcorrecting the final crossed cylinder power (the one giving the patient his best visual acuity as determined in the preceding paragraph) only ±0.125D crossed cylinder by using either the synchronized rotary crossed cylinder attachment 12 or by dialing in the appropriate lens in selectable lens assembly 22. The overcorrected crossed cylinder power as viewed through the viewing tube 24 is then rotated in a clockwise and a counter-clockwise manner to an axis which gives the patient his best non-distorted vision. After the exact axis is chosen by the patient (that which gives him the best non-distorted vision), the added ±0.125D crossed cylinder is removed. The final crossed cylinder power may be checked with the synchronized variable crossed cylinder assembly 12 device if the astigmatic patient was initially neutralized with the selectable crossed cylinder assembly 22 of the present invention. This is important in order to eliminate mechanical and auditory error during refraction. Likewise, the patient may be checked with the selectable crossed cylinder assembly 22 if first refracted by the synchronized variable crossed cylinder assembly 12. If the final refractive error as described above is placed into the spherical equivalent/crossed cylinder refractor of the present invention by utilizing selectable crossed cylinder assembly 22, the synchronized variable crossed cylinder attachment 12 may be used in a manner simulating the conventional Jackson crossed cylinder test to confirm and determine the correct power and axis of the astigmatism. The technique and theory of the use of the Jackson crossed cylinder is well known. To duplicate the Jackson crossed cylinder technique in order to determine the final cylinder axis, the synchronized crossed cylinder assembly 12 is rotated in line with the viewing tube 24. With the power setting of the synchronized crossed cylinder assembly set initially at 0.00D, the housing of the synchronized crossed cylinder assembly 12 (and thus its axis 52) is then rotated 45° away from the cylinder axis 54. This 45° angular displacement is detected by a ball 57 and its corresponding detent 59 in ring gear 51, as described above and is indicated by the axis marking 74 on the scale 48. The power of the synchronized variable crossed cylinder assembly 12 is then varied between a plus ±0.25D crossed cylinder and a minus ±0.25D crossed cylinder. If the cylinder axis 54 is incorrect, the cylinder axis rotation knob 39 is rotated in 2 1/2° or 5° increments towards the positive or negative crossed cylinder marking of the scale 48 which produces the clearer image until the two images as created with the synchronized variable crossed cylinder 12 are equally blurred and distorted. It will be noted that the movement will be in the opposite direction as that commonly described with the standard Jackson crossed cylinder due to the fact that the synchronized variable crossed cylinder assembly 12 is notated in cylinder power, not cylinder axis. For a (+) crossed cylinder refractor, the cylinder axis knob 39 would be rotated towards the (-) portion of scale 48 until the two images as seen with the (+)0.25D crossed cylinder of the assembly 12 and the (-)0.25D crossed cylinder of the assembly 12 are equally blurred. For a (-) crossed cylinder refractor, the cylinder axis knob 37 would be rotated towards the (+) position of scale 48 until the two images as seen with the (+)0.25D crossed cylinder of the assembly 12 and the (-)0.25D crossed cylinder of the assembly 12 are equally blurred. The refractionist also has the option of varying the power of the ±0.25D crossed cylinder of the assembly 12 in relation to the power of the crossed cylinder as seen in the viewing tube 24. As a rule of thumb, the power of the assembly crossed cylinders 12 should be 1/2 the power of the crossed cylinder shown in display 34. To confirm the proper crossed cylinder power as indicated in the display 34 when the Jackson crossed cylinder technique is used, the variable crossed cylinder assembly 12 is rotated so that its axis 52 is parallel to the fixed crossed cylinder axis 54 as indicated on scale 36. The power of the synchronized variable crossed cylinder assembly 12 is then varied from a (+) ±0.25D crossed cylinder to a (-) ±0.25D crossed cylinder. If the refractionist has a positive crossed cylinder phoropter, the power of the crossed cylinder in the viewing tube 24 is increased if there is an improvement in the visual acuity as the crossed cylinder power of the assembly is varied from a plus ±0.25D crossed cylinder to a negative ±0.25D crossed cylinder and if the image is clearer with the (+)0.25D crossed cylinder of the assembly 12. The latter is performed by rotation of the thumb wheel 44. This is repeated until the two images as seen with the plus and minus crossed cylinders of the assembly 12 are equally blurred.

Claims: A refractor comprising a pair of batteries (16,18), each battery comprising a viewing tube (24), and a crossed cylinder lens assembly (12), characterised in that each battery further comprises a selectable crossed cylinder lens assembly (22) comprising at least one lens-carrying crossed cylinder disc (28,30) carrying a plurality of crossed cylinder lenses (26,27) and means (37) for rotating the disc whereby any selected one crossed cylinder lens (26,27) in the disc may be positioned in alignment with the viewing tube. A refractor in accordance with claim 1, characterised in that it further comprises means (39) for rotating the crossed cylinder lens (26,27) positioned in alignment with the viewing tube (24). A refractor in accordance with claim 1 or 2, characterised in that each selectable crossed cylinder lens assembly (22) comprises two lens-carrying crossed cylinder discs (28,30), and each disc carries four graded crossed cylinder lenses (26;27). A refractor according to claim 1,2 or 3, wherein the crossed cylinder lens assembly (12) comprises two cylinder lenses (40,42) of equal power and opposite sign mounted in means (44) for rotating them in opposite directions at the same rate relative to a combined lens axis (52). A refractor in accordance with claim 4, each battery further comprising : means (39) for rotating each crossed cylinder lens, (26,27), and means for positioning the combined crossed cylinder lens axis (52) parallel to one of the positive or negative axes of the selected crossed cylinder lens (26,27) and maintaining such parallel relationship during rotation of the selected crossed cylinder lens. A refractor in accordance with claim 4 or 5, each battery further comprising : means (14) for alternatively positioning the crossed cylinder lens assembly (12) in alignment with the viewing tube (24) or clear of the viewing tube. A refractor in accordance with claim 4, or claim 6 when appended to claim 4, each battery further comprising: means for positioning the combined crossed cylinder lens axis (52) at a predetermined angle to the positive axis of the selected crossed cylinder lens (26,27) and maintaining such predetermined angle during rotation of the selected crossed cylinder lens. A refractor in accordance with any one of claims 4 to 7, wherein the crossed cylinder lens assembly rotating means (14) comprises a thumb wheel (44) acting through intermediate gears (60,62) on two cells (70,72) in each of which one of the two lenses (40,42) is mounted. A refractor in accordance with any one of the preceding claims, each battery further comprising a sphere lens assembly (20). A refractor according to claim 9, wherein said sphere lens assembly (20) comprises selectable sphere lenses.

Inventors: SIMS, CLINTON NORTON
Applicants: SIMS, CLINTON NORTON
Application year: 1985
Main classification: A61B3
IPC codes: A61B3, G01M11