Methods and systems for changing a refractive property of an implantable intraocular lens
A method of altering a refractive property of a crosslinked acrylic polymer material by irradiating the material with a high energy pulsed laser beam to change its refractive index. The method is used to alter the refractive property, and hence the optical power, of an implantable intraocular lens after implantation in the patient's eye. In some examples, the wavelength of the laser beam is in the far red and near IR range and the light is absorbed by the crosslinked acrylic polymer via two-photon absorption at high laser pulse energy. The method also includes designing laser beam scan patterns that compensate for effects of multiphone absorption such as a shift in the depth of the laser pulse absorption location, and compensate for effects caused by high laser pulse energy such as thermal lensing. The method can be used to form a Fresnel lens in the optical zone.
1. A method of altering a refractive property of an implantable intraocular lens having an optic body including an optical zone and a peripheral zone surrounding the optical zone, comprising:
implanting the intraocular lens in a patient's eye;
generating a pulsed laser beam using a pulsed laser source and a light delivery optical system, the pulsed laser beam having a wavelength of 650 to 800 nm, a pulse energy of 10 nJ to 10 uJ, a pulse duration of 10 fs to 10 ps, a pulse repetition rate of 10 to 1000 kHz, a laser focus spot size of 5 to 25 um, and a numerical aperture of 0.01 to 0.15;
while the intraocular lens is in the patient's eye, irradiating the optical zone of the intraocular lens with the pulsed laser beam,
wherein the optical zone comprises a crosslinked acrylic polymer material configured to change its refractive index upon irradiation by the pulsed laser beam, thereby altering a refractive property of the intraocular lens.
2. The method of claim 1 , wherein a first change in the refractive index is negative during a first time period after irradiation and a second change in the refractive index is positive in a second time period after irradiation.
3. The method of claim 1 , wherein the change in refractive index relative to the pre-irradiation refractive index at a location within the crosslinked acrylic polymer is linearly related with a total energy of the irradiation with the light source within a defined total energy range.
4. The method of claim 1 , wherein the pulsed laser beam has a wavelength of 680 to 720 nm, a pulse energy of 100 nJ to 2 uJ, a pulse duration of 100 to 600 fs, a pulse repetition rate of 300 kHz, a laser focus spot size of 7 to 12 um, and a numerical aperture of 0.03 to 0.12.
5. A method of altering a refractive property of an implantable intraocular lens having an optic body including an optical zone and a peripheral zone surrounding the optical zone, comprising:
generating a pulsed laser beam using a pulsed laser source and a light delivery optical system;
calculating a scan pattern based on a pre-defined refractive index modification profile for the optical zone of the intraocular lens and a multi-photon absorption-induced shift in absorption depth in the optical zone corresponding to a pulse energy of the pulsed laser beam; and
irradiating the optical zone of the intraocular lens with the pulsed laser beam, including scanning a focus spot of the pulsed laser beam within the optical zone according to the scan pattern,
wherein the optical zone comprises a material configured to change its refractive index upon irradiation by the pulsed laser beam, thereby altering a refractive property of the intraocular lens.
6. The method of claim 5 , wherein the calculating step includes:
defining an initial scan pattern based on a profile of changes of the refractive index to be produced in the optical zone;
selecting a laser pulse energy of the pulsed laser source and a focal distance and a numerical aperture of the light delivery optical system;
based on the selected laser pulse energy, focal distance and numerical aperture, and material properties of the optical zone, calculating a shift value in absorption depth caused by multiphoton absorption by the optical zone; and
calculating the scan pattern by moving the initial scan pattern to a deeper location based on the calculated shift value.
7. A method of altering a refractive property of an implantable intraocular lens having an optic body including an optical zone and a peripheral zone surrounding the optical zone, comprising:
generating a pulsed laser beam using a pulsed laser source and a light delivery optical system;
calculating a scan pattern based on a pre-defined refractive index modification profile for the optical zone of the intraocular lens and a thermal lensing effect on subsequent laser pulses caused by a temperature gradient in the optical zone induced by previous laser pulses of the pulsed laser beam; and
irradiating the optical zone of the intraocular lens with the pulsed laser beam, including scanning a focus spot of the pulsed laser beam within the optical zone according to the scan pattern,
wherein the optical zone comprises a material configured to change its refractive index upon irradiation by the pulsed laser beam, thereby altering a refractive property of the intraocular lens.
8. A method of altering a refractive property of an implantable intraocular lens having an optic body including an optical zone and a peripheral zone surrounding the optical zone, comprising:
generating a pulsed laser beam using a pulsed laser source and a light delivery optical system;
defining a scan pattern based on a profile of changes of the refractive index to be produced in the optical zone of the intraocular lens, the scan pattern including a plurality of scan layers arranged in a spatial order according to their depths; and
irradiating the optical zone of the intraocular lens with the pulsed laser beam, including scanning a focus spot of the pulsed laser beam within the optical zone to form the plurality of scan layers one at a time according to a time order, wherein an order of the plurality of scan layers in the time order is different from an order of the plurality of scan layers in the spatial order, wherein any scan layers that are immediately adjacent each other in the spatial order are not immediately adjacent each other in the time order,
wherein the optical zone comprises a material configured to change its refractive index upon irradiation by the pulsed laser beam, thereby altering a refractive property of the intraocular lens.
9. The method of claim 5 , wherein the scan pattern is configured to produce a refractive index modification profile in the optical zone having a plurality of concentric rings that form a Fresnel lens.
10. The method of claim 5 , wherein the light beam has a wavelength of 400 to 450 nm or 650 to 800 nm.
11. The method of claim 5 , wherein the pulsed laser beam has a wavelength of 650 to 800 nm, a pulse energy of 10 nJ to 10 uJ, a pulse duration of 10 fs to 10 ps, a pulse repetition rate of 10 to 1000 kHz, a laser focus spot size of 5 to 25 um, and a numerical aperture of 0.01 to 0.15.
12. The method of claim 7 , wherein the scan pattern is configured to produce a refractive index modification profile in the optical zone having a plurality of concentric rings that form a Fresnel lens.
13. The method of claim 7 , wherein the light beam has a wavelength of 400 to 450 nm or 650 to 800 nm.
14. The method of claim 7 , wherein the pulsed laser beam has a wavelength of 650 to 800 nm, a pulse energy of 10 nJ to 10 uJ, a pulse duration of 10 fs to 10 ps, a pulse repetition rate of 10 to 1000 kHz, a laser focus spot size of 5 to 25 um, and a numerical aperture of 0.01 to 0.15.
15. The method of claim 8 , wherein the scan pattern is configured to produce a refractive index modification profile in the optical zone having a plurality of concentric rings that form a Fresnel lens.
16. The method of claim 8 , wherein the light beam has a wavelength of 400 to 450 nm or 650 to 800 nm.
17. The method of claim 8 , wherein the pulsed laser beam has a wavelength of 650 to 800 nm, a pulse energy of 10 nJ to 10 uJ, a pulse duration of 10 fs to 10 ps, a pulse repetition rate of 10 to 1000 kHz, a laser focus spot size of 5 to 25 um, and a numerical aperture of 0.01 to 0.15.