in accordance with the present invention , a limited area of a contact lens or intraoccular lens is rendered semi - opaque . as used herein , the term &# 34 ; semi - opaque &# 34 ; means that in the limited area the undistorted optical transmissibility of visible images typical for contact lenses is substantially disrupted . such semi - opaqueness results in reduced light transmission and substantial obliteration of the normal refractive quality of the lens in the area of opacity yielding a clouded ground glass appearance . the present system is available to form semi - opaque corneal contact lenses ( hard , soft , gas permeable , silicone or other form ) or a conventional introoccular lens such as described in zdrok u . s . pat . no . 4 , 039 , 827 . however , the present description will refer to the soft contact lens unless otherwise specified . in a preferred embodiment , the semi - opaque lens of the present invention is formed by directing a focused laser beam into the contact lens under conditions to form a pattern of optical disruptions in a predetermined area of the lens material . such disruptions may comprise physical alterations to the lens , preferably contained in the interior of the lens material . such physical disruptions may comprise microscopic opacifications ( punctate material disruptions which appear as fine white dots ), bubbles , cracks , fissures , crazes , or other physical disruptions which in combination form the opacity . as used herein , the term &# 34 ; excimer laser &# 34 ; is defined as a family of lasers with similar output characteristics as described in an article by hecht , j ., entitled &# 34 ; excimer laser update &# 34 ; and &# 34 ; lasers & amp ; applications &# 34 ;, december 1973 ( 43 - 49 ), incorporated herein by reference . suitable laser beams include any laser which can be gated or pulsed and which functions in the region where the lens material is normally transparent and which can be focused to a high degree of intensity and whose one excellent laser beam is an excimer laser , which can be focused to a very small spot . suitable wavelengths comprise 193 nm to 35 nm . suitable energies comprise from less than 1 mj to hundres of mj . the laser is of the type which is at a sufficiently high energy to provide the opacity of the type described above . the laser should be focused to a sufficient extent to form a predetermined pattern . the technology of using highly focused non - linear lasers has been well developed , e . g ., for use in ophthalmic surgery , as disclosed in keates , r . h ., et al ., ophthalmic neodymium : yag lasers ( october , 1982 ). the same laser technology may be used to treat the lens in accordance with the present invention with typical power setting of 1 mj with multiple pulses . in one embodiment , the unfinished or precursor corneal soft lens is used . such precursor lens typcially comprises a clyindrical with a flat top and bottom formed of the contact lens material , referred to as a button . the button may be irradiated from the convex side of said cylinder . if a ring is the desired pattern , the beam may be stationary and focused at a point in the interior of the button which in turn is rotated on an axis perpendicular to the flat faces . the laser beam ( partially focused by the cylindrical side ) creates a number of microscopic ( approximately 1 - 40 microns ) punctated opacities , bubbles , small fissures crazes or cracks over a region in the interior of the button . the surface of the button is not damaged by the beam . the temperature of the surface may be cooled ( e . g ., by ambient air or cooling the chuck holding it or with an external gas ) to reduce any substantial surface disruptions . in this manner , an semi - opaque or cloudy ring pattern is formed . thereafter , the button is shaped in a conventional manner . by appropriate placement of the beam , the ring of bubbles is formed in a precise area around a clear central area . the laser technique may also be used on the finished lenses themselves . in this instance , the laser is focused onto a spinning lens by a short focal length , e . g ., 2 mm . to 1 cm . similar physical disruptions in the lens are formed as for the unfinished lens or precursor in any state of the lens formation ( e . g ., button ). in the preferred embodiment , disruptions are formed solely in the interior of the lens without any substantial physical disruption at the lens surface . this has the advantage of avoiding eye irritation to the lens wearer . if for some reason , this proves to be impractical , some disruptions may take place at the lens surface with appropriate polishing . it is believed that the physical disruptions are formed by thermal or optical break - down effects on the lens material . that is , it is believed that at the focal point of the beam , there is a rapid deposition of thermal energy which creates the physical disruptions by melting or vaporizing the lens material . this energy affect is non - linear . it is believed that any laser generating wavelength which can penetrate the lens material surface but still be absorbed by the lens material bulk would be suitable to accomplish the above descriptions . such other lasers include those known as nd : yag ( suitably the wavelength of 1 . 06 microns ) double nd : yag ( suitably a wavelength of 0 . 53 microns ), and alexandrite ( suitably a wavelength of 0 . 75 microns ). in the above ring embodiment , the pattern may bein the form of a ring of the size and shape to conform to the outline of the iris of the eye . for cosmetic purposes , the ring may be colored by conventional means to provide a color to the semi - opaque region which changes the color of the iris , say from brown to blue . for prosthetic uses , such color may provide the appearance of an airis which was missing in a damaged eye . suitable coloring techniques include vat dying acid , reactive dying and diazo dying and tinting as set forth in meshel et al . british patent no . 1 . 547 . 525 . other patterns may be utilized in accordance with the present invention . for example , multiple regions of the lens may be rendered semi - opaque for various cosmetic , prosthetic or other uses and optionally colored in accordance with the above techniques . one such other use is to render the lens semi - opaque in the form of a coding symbol such as indicating left or right lens or the presciption of the lens . due to the precision of the laser beams , such symbols may be formed in a very small peripheral area of the lens which is not visible when the lens is worn . in order to further illustrate the invention , the following specific examples of its practice are given . this example , a precursor of the contact lens in the form of a hema small cylinder or button is treated in accordance with the invention . a laser beam of the excimer laser type ( xenon chloride , wavelength 308 nm and an average specific power of 60 - 120 watts , 300 mj , 200 - 400 hertz ). the laser is irradiated by directing the incident beam from the laser against the cylindrical sidewall of the unfinished button . the sidewall serves as a lens which focuses the beam at a location towards the center of the button . the button is rotated along its cylindrical axis at 120 rpms forming a central semi - opaque region consisting of bubbles or crazes . surrounding this semi - opaque region is a transparent ring . the button is finished into a soft contact lens by conventional techniques . in this example , the button of example 1 is irradiated with the same laser beam at the same angle . however , instead of irradiating the entire cylindrical sidewall in its path , a limited area of the side surfce is contacted by passing the beam either past one sharp edge such as a knife blade in its path . for more precision , the instant beam may be passed through the space formed between spaced knife edges forming an elongate beam of limited height . this beam is concentrated by the cylindrical sidewall of the button as in example 1 to form a point eccentric to the axis of the button . the button is rotated at 120 rpm as in example 1 . in this embodiment , the semi - opaque surface is formed in a ring with the center in a transparent circle and outside the ring is a fully transparent ring unaffected by the laser beam . again , the button is formed into a soft contact lens by conventional techniques . in this example , the button is finished to form the posterior or concave curvature prior to irradiation with the laser beam . the posterior surface is cooled with a vacuum chuck , room air , liquid nitrous oxide or cooled water . the beam is directed to a region on the flat surface opposite the concave curvature by directing through an appropriate aperture . the semi - opaque regon is formed in a ring by rotating the partially finished button about an axis through the center of the concave surface . the final product is a semi - opaque ring with a clear center and periphery suitable for coloring the ring using it as a colored soft contact lens . in this example , the finished soft contact lens is placed onto a chuck which holds the finished lens from the concave side so that the convex side is the one which is exposed to the laser beam . the laser is an ng : yag laser ( 1 - 3 mj ) with multiple pulses . the lens focuses the laser into a fine point below the surface of the lens only so that both the concave and convex surfaces of the lens include no substantial disruptions . the chuck is moved in a predetermiend pattern to permit the pulsing pinpoint lasr to form the desired image . this technique may be used to provide a cooled sumbol such as the lens prescipriton or manufacturer &# 39 ; s lot number . the concave side of the lens is cooled by vacuum as a safety measure to avoid the formation of disruptions on the concave side which could irritate the eye of the wearer . in this example , the corneal contact lens is placed on a chuck in the same manner as in example 4 and a laser beam shined through a conventional lens is focused onto a point within the lens as in example 4 . however , the focal point is eccentric with respect to the center of the lens and the lens is rotated to form a ring of the type set forth in example 3 .