Controller for a surgical laser
The invention relates to a controller for a surgical laser. According to the invention, the controller is adapted to control a laser in order to produce two or more three-dimensional compression zones, each comprising a plurality of lesions, inside a lens cortex of a crystalline lens of the eye using a laser pulse or multiple laser pulses, wherein the controller is adapted such that a laser can be calibrated with respect to a reference point within the lens, and each of the compression zones produced has a length in a radial direction, a depth in a direction parallel to the optical or visual axis and an average width in a direction parallel to a tangent of the lens cortex, wherein the sum of the average widths of all compression zones is 0.1 to 2 millimeter for every 1 diopter of desired gain in accommodation amplitude of the lens.
1. A laser apparatus comprising:
a surgical laser; and
a controller adapted to control the surgical laser, the controller adapted to cause the laser to produce two or more three-dimensional compression zones ( 130 ), each comprising a plurality of lesions, inside a lens cortex ( 110 ) of a crystalline lens ( 2 ) of an eye using a laser pulse or multiple laser pulses, wherein the controller is further adapted such that
a diameter of a focal spot size or a location of a focal point of the laser is calibrated with respect to a reference point within the crystalline lens, and
each of the compression zones produced has a length ( 112 ) in a radial direction in relation to a center of the lens and in a plane perpendicular to the optical or visual axis corresponding to an extension of the lens cortex in a radial direction in a plane perpendicular to the optical or visual axis, each compression zone extending from an inner circumference of the lens cortex to an outer circumference of the lens cortex,
each of the compression zones produced has a depth ( 101 ) in a direction parallel to the optical or visual axis corresponding to an extension of the lens cortex in a direction parallel to the optical or visual axis, each compression zone having a larger depth close to a nucleus of the lens and a smaller depth further from the nucleus, and
each of the compression zones produced has an average width ( 131 ) in a direction parallel to a tangent of the lens cortex and in a plane perpendicular to the optical or visual axis of the eye,
wherein the sum of the average widths of all compression zones is 0.1 to 2 millimeter for every 1 diopter of desired gain in accommodation amplitude of the crystalline lens.
2. The laser apparatus according to claim 1 ,
wherein the width ( 131 ) of each of the compression zones ( 130 ) varies along the length of the respective zones and the average width is the average value of the varying width.
3. The laser apparatus according to claim 1 ,
wherein the controller is configured to direct the laser pulse or multiple laser pulses such that each of the compression zones ( 130 ) has the form of a cuboid or a segment of a cylinder.
4. The laser apparatus according to claim 1 ,
wherein the controller is configured to direct the laser pulse or multiple laser pulses such that the sum of the average widths ( 131 ) of all compression zones ( 130 ) is 0.7 to 1.5 millimeter, for every 1 diopter of gain in accommodation amplitude of the crystalline lens.
5. The laser apparatus according to claim 1 ,
wherein the controller is configured to direct the laser pulse or multiple laser pulses such that the sum of the average widths ( 131 ) of all compression zones ( 130 ) is 0.75 to 1.2 millimeter, for every 1 diopter of gain in accommodation amplitude of the crystalline lens.
6. The laser apparatus according to claim 1 ,
wherein the controller is configured to direct the laser pulse or multiple laser pulses such that the average width g in micrometer of each compression zone ( 131 ) corresponds to
g
=
10
2
∏
r
n
(
1
-
L
L
+
(
d
*
80
)
)
;
and
wherein r is the radius of the nucleus of the crystalline lens in micrometers, n is the number of compression zones, L is the length of the nucleus of the crystalline lens in a direction parallel to the optical or visual axis in micrometer, and d is the desired gain in accommodation amplitude in diopter.
7. The laser apparatus according to claim 1 ,
wherein the controller is configured to direct the laser pulse or multiple laser pulses such that the compression zones ( 130 ) are spaced in an equidistant manner in a direction circumferential of the lens cortex ( 110 ) or the lens nucleus ( 120 ).
8. The laser apparatus according to claim 1 ,
wherein the controller is configured to direct the laser pulse or multiple laser pulses such that four compression zones ( 130 ) are arranged in the form of a cross in a plane perpendicular to the optical or visual axis.
9. The laser apparatus according to claim 1 ,
wherein the controller is configured to direct the laser pulse or multiple laser pulses such that a plurality of compression zones ( 130 ) is produced that forms a star-like pattern in a plane perpendicular to the optical or visual axis.
10. The laser apparatus according to claim 1 , wherein the controller is configured to direct the laser pulse or multiple laser pulses such that the compression zones ( 130 ) are located within an annular region delimited by an inner and an outer diameter ( 7 c, d ) in a first plane ( 7 a ) of the crystalline lens with respect to the reference point.
11. The laser apparatus according to claim 1 ,
wherein the controller is adapted to define a starting point and an end point of each compression zone ( 130 ) relative to the reference point prior to producing the compression zones.
12. The laser apparatus according to claim 11 ,
wherein the controller is adapted to define the starting point and the end point of each compression zone ( 130 ) such that the compression zones are located within the crystalline lens and spaced apart from a capsule of the crystalline lens.
13. The laser apparatus of claim 11 , wherein the average widths of all compression zones is 0.7 to 1.5 millimeter for every 1 diopter of desired gain in accommodation amplitude.
14. A method for treatment of a crystalline lens of an eye with a lens nucleus ( 120 ) and a lens cortex ( 110 ), wherein two or more three-dimensional compression zones ( 130 ), each comprising a plurality of lesions, are produced inside the lens cortex ( 110 ) using a laser pulse or multiple laser pulses, wherein the method comprises:
calibrating a diameter of a focal spot size or a location of a focal point of a laser with respect to at least one reference point of the crystalline lens; and
applying the laser pulse or multiple laser pulses to the crystalline lens to form the two or more three-dimensional compression zones, wherein each of the compression zones has a length ( 112 ) in a radial direction in relation to a center of the lens and in a plane perpendicular to the optical or visual axis corresponding to an extension of the lens cortex in a radial direction in a plane perpendicular to the optical or visual axis, each compression zone extending from an inner circumference of the lens cortex to an outer circumference of the lens cortex, and wherein
each of the compression zones has a depth ( 101 ) of each compression zone in a direction parallel to the optical or visual axis corresponding to an extension of the lens cortex in a direction parallel to the optical or visual axis, each compression zone having a larger depth close to a nucleus of the lens and a smaller depth further from the nucleus, and
each of the compression zones has an average width ( 131 ) in a direction parallel to a tangent of the lens cortex and in a plane perpendicular to the optical or visual axis, and wherein the sum of the average widths of all compression zones is 0.1 to 2 millimeter for every 1 diopter of desired gain in accommodation amplitude of the crystalline lens.
15. The method of claim 14 , wherein the average widths of all compression zones is 0.7 to 1.5 millimeter for every 1 diopter of desired gain in accommodation amplitude.