US2009164008A1PendingUtilityA1

Lens surface with combined diffractive, toric, and aspheric components

Assignee: HONG XINPriority: Dec 21, 2007Filed: Dec 21, 2007Published: Jun 25, 2009
Est. expiryDec 21, 2027(~1.4 yrs left)· nominal 20-yr term from priority
G02B 3/06A61F 2/1654G02B 3/04A61F 2/1645A61F 2/164G02B 5/1876G02B 3/08Y10T82/2502Y10T82/10Y10T82/16016
47
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Claims

Abstract

In one aspect, the present invention provides an intraocular lens (IOL) that includes an optic comprising an anterior surface, a posterior surface, and a plurality of diffractive zones disposed on one of those surfaces. The surface having the diffractive zones has a profile characterized by a combination of aspheric and toric components.

Claims

exact text as granted — not AI-modified
1 . An intraocular lens (IOL), comprising
 an optic comprising an anterior surface and a posterior surface,   a plurality of diffractive zones disposed on one of said surfaces,   wherein said surface having the diffractive zones exhibits a base profile characterized by a combination of asphericity and toricity.   
     
     
         2 . The IOL of  claim 1 , wherein said optic provides a far focus and a near focus. 
     
     
         3 . The IOL of  claim 2 , wherein said far focus provides an optical power in a range of about 16 D to about 32 D. 
     
     
         4 . The IOL of  claim 3 , wherein said near focus provides an add power in a range of about 1 D to about 6 D. 
     
     
         5 . The IOL of  claim 1 , wherein said anterior surface comprises said diffractive structures and said asphericity and toricity. 
     
     
         6 . The IOL of  claim 1 , wherein a profile of said surface is characterized by the following relation:
   sag(R avrg   ,r ,θ)=diffractive(R ave   ,r )+toric(R ave   ,r ,θ)+asph(R ave   ,r ),   
       wherein,
 sag represents a sag of the surface along an optical axis of the optic at a radial distance r from a center of the surface at a meridian angle θ, where R avrg  represents a base radius of curvature of average meridian, and 
 
       wherein,
   diffractive(R avrg   ,r )= z   rad −√{square root over (R rad   2   −r   2 )}, 
 
       wherein,
 z rad  and R rad  denote, respectively, a radius of curvature of a diffractive zone extending through the radial distance r and an axial location of a curvature center of that zone, and 
 
       wherein, 
       
         
           
             
               
                 
                   toric 
                    
                   
                     ( 
                     
                       
                         R 
                         avrg 
                       
                       , 
                       r 
                       , 
                       θ 
                     
                     ) 
                   
                 
                 = 
                 
                   
                     
                       ( 
                       
                         
                           
                             c 
                             x 
                           
                            
                           
                             cos 
                             2 
                           
                            
                           θ 
                         
                         + 
                         
                           
                             c 
                             y 
                           
                            
                           
                             sin 
                             2 
                           
                            
                           θ 
                         
                       
                       ) 
                     
                      
                     
                       r 
                       2 
                     
                   
                   
                     1 
                     + 
                     
                       
                         
                           
                             
                               1 
                               - 
                               
                                 
                                   ( 
                                   
                                     1 
                                     + 
                                     
                                       k 
                                       x 
                                     
                                   
                                   ) 
                                 
                                  
                                 
                                   c 
                                   x 
                                   2 
                                 
                                  
                                 
                                   r 
                                   2 
                                 
                                  
                                 
                                   cos 
                                   θ 
                                   2 
                                 
                               
                               - 
                             
                           
                         
                         
                           
                             
                               
                                 ( 
                                 
                                   1 
                                   + 
                                   
                                     k 
                                     y 
                                   
                                 
                                 ) 
                               
                                
                               
                                 c 
                                 y 
                               
                                
                               
                                 r 
                                 2 
                               
                                
                               
                                 sin 
                                 2 
                               
                                
                               θ 
                             
                           
                         
                       
                     
                   
                 
               
               , 
             
           
         
       
       wherein,
 c x  and c y  represent toric curvatures along two principal meridians of the surface and k x  and k y  represent toric conic constants along the two principal meridians, and 
 
       wherein, 
       
         
           
             
               
                 
                   asph 
                    
                   
                     ( 
                     
                       
                         R 
                         avrg 
                       
                       , 
                       r 
                     
                     ) 
                   
                 
                 = 
                 
                   
                     cr 
                     2 
                   
                   
                     1 
                     + 
                     
                       
                         1 
                         - 
                         
                           
                             ( 
                             
                               1 
                               + 
                               k 
                             
                             ) 
                           
                            
                           
                             c 
                             2 
                           
                            
                           
                             r 
                             2 
                           
                         
                       
                     
                   
                 
               
               , 
               and 
             
           
         
       
       wherein 
       
         
           
             
               
                 c 
                 = 
                 
                   1 
                   
                     R 
                     avrg 
                   
                 
               
               , 
               and 
             
           
         
       
       wherein k represents a spherical conic constant. 
     
     
         7 . The IOL of  claim 6 , wherein z rad  is defined in a Cartesian coordinate (x,y,z), where z is along the optical axis, in accordance with the following relation: 
       
         
           
             
               
                 
                   z 
                   rad 
                 
                 = 
                 
                   
                     
                       x 
                       in 
                       2 
                     
                     + 
                     
                       z 
                       in 
                       2 
                     
                     - 
                     
                       x 
                       out 
                       2 
                     
                     - 
                     
                       z 
                       out 
                       2 
                     
                   
                   
                     2 
                      
                     
                       ( 
                       
                         
                           z 
                           in 
                         
                         - 
                         
                           z 
                           out 
                         
                       
                       ) 
                     
                   
                 
               
               , 
             
           
         
       
       wherein x in  and z in  represent, respectively, x and z coordinates of an inner boundary of the diffractive zone and x out  and z out  represent, respectively, x and z coordinates of an outer boundary of the diffractive zone. 
     
     
         8 . The IOL of  claim 7 , wherein R rad  is defined in the Cartesian coordinates in accordance with the following relation:
   R rad =√{square root over (( z   in   −z   rad ) 2 +x in   2 )}.   
     
     
         9 . The IOL of  claim 8 , wherein a magnitude of R avrg  is in a range of about 12 mm to about 120 mm. 
     
     
         10 . The IOL of  claim 9 , wherein a magnitude of c x  is in a range of about 0.008 mm −1  to about 0.08 mm −1  and a magnitude of c y  is in a range of about 0.008 mm −1  about 0.08 mm −1 . 
     
     
         11 . The IOL of  claim 10 , wherein kx is in a range of about −3000 to about −12 and k y  is in a range of about −3000 to about −12. 
     
     
         12 . The IOL of  claim 11 , wherein k is in range of about −3000 to about −12. 
     
     
         13 . The IOL of  claim 1 , wherein said diffractive zones comprise a plurality of diffractive structures separated from one another by a plurality of step heights. 
     
     
         14 . The IOL of  claim 13 , wherein a radius of curvature of a diffractive zone along a meridian characterized by an angle θ (R d   θ ) and a radius of curvature of a base profile associated with that diffractive zone (R b   θ ) are related in accordance with the following relation: 
       
         
           
             
               
                 
                   ( 
                   
                     
                       n 
                       1 
                     
                     - 
                     
                       n 
                       2 
                     
                   
                   ) 
                 
                  
                 
                   ( 
                   
                     
                       1 
                       
                         R 
                         d 
                         θ 
                       
                     
                     - 
                     
                       1 
                       
                         R 
                         b 
                         θ 
                       
                     
                   
                   ) 
                 
               
               = 
               
                 Constant 
                 . 
               
             
           
         
       
     
     
         15 . The IOL of  claim 14 , wherein said Constant is in a range of about 0 D to about 4 D. 
     
     
         16 . The IOL of  claim 1 , wherein said anterior surface includes said diffractive zones. 
     
     
         17 . The IOL of  claim 16 , wherein said posterior surface exhibits a spherical profile. 
     
     
         18 . A diffractive ophthalmic lens, comprising
 an optic having an anterior surface and a posterior surface,   wherein at least one of said surfaces exhibits a profile characterized by a combination of diffractive, aspheric and toric components.   
     
     
         19 . The ophthalmic lens of  claim 18 , wherein said lens provides a far-focus optical power in a range of about 16 D to about 32 D. 
     
     
         20 . The ophthalmic lens of  claim 19 , wherein said lens provides a near-focus power characterized by an add power in a range of about 1 D to about 6 D.

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