Scanning disks for use in tandem scanning reflected light microscopes and other optical systems

Claim 2

A scanning device for promoting high resolution and contrast of a viewed objective target, comprising a disk featuring a circular illumination area defined between radially inner and outermost pinholes including a multitude of pinholes, each pinhole located substantially equidistantly from its nearest neighboring holes in the illumination area.

Claim 3

A scanning device according to claim 1 where the holes are located in the illumination area by mapping evenly spaced points from rectangular space into the circular illumination area of the disk, after having rotated the hole pattern of the Cartesian map space by the arctan (√5-1)/2.

Claim 4

A scanning device according to claim 2 where the illumination area is divided into two identical segments, one defining a half of the illumination area and, whereupon rotation of the disk around its center, no two pinholes in the same half overtrack the same area and each pinhole in the other half positionally corresponds exactly to one pinhole in the first half.

Claim 5

A scanning device according to claim 1 wherein the illumination area contains approximately 35,000 pinholes which are sized to constitute approximately one-quarter percent (1/4%) of the surface of the illumination area.

Claim 6

A scanning device according to claim 1 where the Cartesian coordinates of the equidistantly spaced pinholes arranged in spirals in polar coordinates are located according to the following: X=AK.sub.I Sin (F)+BK.sub.I Cos (F) Y=AK.sub.I Cos (F)-BK.sub.I Sin (F) where angle F is Arctan(N A /N B ), A and B are selected rectangular pattern coordinates, N B pattern and defines the number of spirals in a cycle, N A is an integer previous to N 8 in a sequence of numbers, K=√A H is the distance between nearest neighbor holes in map space and A H is the aperture area.

Claim 7

A scanning device according to claim 5 wherein ##EQU3##

Claim 8

A scanning device according to claim 6 wherein said disk has C cycles where N A +N B are successive numbers in the sequence and are multiplied by C.

Claim 9

A scanning device according to claim 1 wherein said pinholes are located in the space between the radially inner and outermost pinholes of a pinhole pattern of said disk according to the formula Y=J-(IN.sub.A /N.sub.B) where I is an integer ranging from 0 to N b -1 and J is an integer such that Y has a value between 0 and 1.

Claim 10

A scanning device according to claim 8 wherein said pinholes are located along a plurality of spiral paths in cycles, the first pinholes of spirals after the first spiral of each cycle being located radially between the first two pinholes of said first spiral.

Claim 11

A scanning device according to claim 1 wherein said pinholes are located in the space between the radially inner and outermost pinholes of a pinhole pattern of said disk according to the formula Y=(IN.sub.A /N.sub.B)-J where I is an integer ranging from 0 to N b -1 and J is an integer such that Y has a value between 0 and 1.

Claim 12

A scanning device according to claim 10 wherein said pinholes are located along a plurality of spiral paths in cycles, the first pinholes of spirals after the first spiral of each cycle being located radially between the first two pinholes of said first spiral.

Claim 13

An improved Nipkow-type scanning disk for use in optical devices, comprising a disk of a selected radius R, said disk defining an annulus having a minimum radius R A and a maximum radius R B where the disk is dividable into two halves with identical hole patterns, said disk further defining a plurality of small apertures where the apertures in each half of said disk are so patterned within the annulus that a complete scanning cycle can be initiated at any disk radius without any holes overtracing the same point.

Claim 14

An improved Nipkow-type scanning disk for use in optical devices, comprising a disk of a selected radius R, said disk defining an annulus having a minimum radius R A and a maximum radius R B where the disk is dividable into two halves with identical hole patterns, said disk further defining a plurality of small apertures where the apertures in each half of said disk are so patterned within the annulus that a complete scanning cycle can be initiated at any disk radius without any holes overtracing the same point.

Claim 15

A scanning disk according to claim 12 wherein the apertures are located along a plurality of spiral paths in cycles, the first apertures of spirals after the first spiral of each cycle being located radially between the first two apertures of said first spiral.

Claim 16

A scanning disk according to claim 13 where the annulus contains approximately 35,000 apertures and are sized to constitute approximately one-quarter percent (1/4%) of the annulus surface area.

Claim 17

A scanning disk according to claim 12 where the pattern of apertures is formed by mapping spaced points from rectangular space into the annulus, after having rotated the x-axis of the rectangular spaced by the arctan(√5-1)/2 so as to repeat the pattern over a number of scanning cycles to provide inherent interlacing of aperture patterns.

Claim 18

A scanning disk according to claim 12 where each aperture is equidistant from its nearest neighboring apertures.

Claim 21

A method according to claim 17 where the aperture points are converted from rectangular space into the annulus by rotating the hole pattern of the rectangular space an optimum angle, where no two scan lines traced by the apertures overlap.

Claim 22

A method according to claim 17 further comprising the steps of inserting the disk between an illumination source and the object prior to rotating the disc, and rotating the disk.

Claim 23

A method according to claim 17 further comprising the step of defining the number of apertures to be approximately 35,000 where each disk half contains approximately 17,500 apertures, and sizing the apertures to constitute substantially one-quarter percent (1/4%) of the total disk surface area.

Claim 24

A method according to claim 17 further including the step of calculating the Cartesian coordinates of each of the spaced apertures to be substantially equidistantly spaced in polar coordinates according to the following: X=AK.sub.I Sin (F)+BK.sub.I Cos (F) Y=AK.sub.I Cos (F)-BK.sub.I Sin (F) where angle F is Arctan(N A /N B ), A and B are selected rectangular pattern coordinates, N B is an integer taken from a sequence of numbers and N B defines the number of spirals in a cycle, N A is an integer previous to N B in the sequence, K I =√A H is the distance between nearest neighbor holes in map space and A H is the magnitude of the area of the disk associated with or assigned to each aperture.

Claim 25

A method according to claim 21 wherein T=X/R.sub.o where T is an angle, X is a Cartesian map space coordinate and R o is a constant and relates to a specific value of R ##EQU4## where R is a radius and Y is a Cartesian map space coordinate.

Claim 28

An optical scanning disc comprising an opaque material having an annulus of transparent points lying between minimum and maximum radii, said points lying along multiple paths established in a rectangular array of equally spaced points each of which paths intersects a minimal number of points of the array. one of said paths being located between said minimum and maximum radii and deviates substantially from any path parallel to any path heavily populated with said points, the remaining paths being defined by a Fibinocci series, said points on the disc lying along said paths as transformed into circumferential paths in the annulus.

Claim 29

An optical scanning disc comprising an opaque material having an annulus of transparent points lying between minimum and maximum radii, said points lying along multiple paths established in a rectangular array of equally spaced points each of which paths intersects a minimal number of points of the array. one of said paths being located between said minimum and maximum radii and deviates substantially from any path parallel to any path heavily populated with said points, the remaining paths being defined by a Fibinocci series, said points on the disc lying along said paths as transformed into circumferential paths in the annulus.

Claim 30

An optical scanning disc according to claim 24 wherein said points are located along paths which are non-repetitive over a substantial sector of each half of said disc.

Claim 31

An optical scanning disc according to claim 24 wherein said points are located on said disc by mapping evenly spaced points from rectangular space into the circular illumination area of the disc by a transformation according to R=f(Y) and T=KX where R is the radial position on the disc and T is the angular position on the disc, X and Y are the coordinatants in rectangular space, f(Y) is a monatomic function of Y, K≠ is a constant and g(Z) is a slowly varying function of Y or R.

Claim 32

An optical scanning disc according to claim 26 wherein f(Y)=√2R o Y, K=1/R o and R o is a constant.

Claim 33

A scanning disc as in claim 27 where the pattern of points in rectangular space is a square pattern rotated by an angle F where F≈arctan(√5-1)/2.

Claim 34

An optical scanning disc according to claim 26 wherein the pattern of points in rectangular space is a Bravais net.

Claim 35

A scanning disc comprising an opaque material, apertures in said opaque material with the apertures being arrayed in spirals, wherein the first apertures of subsequent spirals after the first spiral of a cycle are proportional along said subsequent spirals over the range required to complete a scan according to the formula Y=J-(IN.sub.A /N.sub.B) where Y is a fraction of the range required, I is an integer ranging from 1 to N B -1, N B is the number of spirals in a cycle, J is an integer such that Y has a value between 0 and 1 and N A is an integer such that the first apertures of a cycle of spirals or rays are staggered in a pseudo-random fashion thereby eliminating streaking.

Claim 36

A scanning disc comprising an opaque material, apertures in said opaque material with the apertures being arrayed in spirals, wherein the first apertures of subsequent spirals after the first spiral of a cycle are proportional along said subsequent spirals over the range required to complete a scan according to the formula Y=J-(IN.sub.A /N.sub.B) where Y is a fraction of the range required, I is an integer ranging from 1 to N B -1, N B is the number of spirals in a cycle, J is an integer such that Y has a value between 0 and 1 and N A is an integer such that the first apertures of a cycle of spirals or rays are staggered in a pseudo-random fashion thereby eliminating streaking.

Claim 37

A scanning disc as in claim 30 where N A /N B ≈±(√5-1)/2.