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Background and Objective: A novel computer-guided laser treatment for open-angle glaucoma, called patterned laser trabeculoplasty, and its preliminary clinical evaluation is described. Patients and Methods: Forty-seven eyes of 25 patients with open-angle glaucoma received 532-nm laser treatment with 100-μm spots. Power was titrated for trabecular meshwork blanching at 10 ms and sub-visible treatment was applied with 5-ms pulses. The arc patterns of 66 spots rotated automatically after each laser application so that the new pattern was applied at an untreated position. Results: Approximately 1,100 laser spots were placed per eye in 16 steps, covering 360° of trabecular meshwork. The intraocular pressure decreased from the pretreatment level of 21.9 ± 4.1 to 16.0 ± 2.3 mm Hg at 1 month (n = 41) and remained stable around 15.5 ± 2.7 mm Hg during 6 months of follow-up (n = 30). Conclusion: Patterned laser trabeculoplasty provides rapid, precise, and minimally traumatic (sub-visible) computer-guided treatment with exact abutment of the patterns, exhibiting a 24% reduction in intraocular pressure during 6 months of follow-up ( P < .01).

* BACKGROUND AND OBJECTIVE: In both clinical and animal studies, it has been shown that repetitive short laser pulses can cause selective retinal pigment epithelium damage (RPE) with sparing of photoreceptors. Our purpose was to determine the ophthalmoscopic and angiographic damage thresholds as a function of pulse durations by using different pulsed laser systems to optimize treatment modalities. * MATERIALS AND METHODS: Chinchilla breed rabbits were narcotized and placed in a special holding system. Laser lesions were applied using a commercial laser slit lamp, contact lens, and irradiation with a frequency-doubled Nd: YLF laser (wavelength: 527 nm; repetition rate: 500 Hz; number of pulses: 100; pulse duration: 5 µß, 1.7 µß, 200 ns) and an argon-ion laser (514 nm, 500 Hz, 100 pulses, 5 µß and 200 ms). In all eyes, spots with different energies were placed into the regio macularis with a diameter of 102 µp? (tophat profile). After treatment, fundus photography and fluorescein angiography were performed and radiant exposure for ED50 damage determined. Speckle measurements at the fiber tips were performed to determine intensity peaks in the beam profile. * RESULTS: Using the Nd:YLF laser system, the ophthalmoscopic ED50 threshold energies were 25.4 µ] (5 µß), 32 µ] (1.7 µß), and 30 µ] (200 ns). The angiographic ED50 thresholds were 13.4 µ] (5 µ8), 9.2 µ] (1.7 µß), and 6.7 µ] (200 ns). With the argon laser, the angiographic threshold for 5 µß pulses was 5.5 µ). The ophthalmoscopic threshold could not he determined because of a lack of power; however, it was >12 µ}. For 200 ms, the ED50 radiant exposures were 20.4 mW ophthalmoscopically and 19.2 mW angiographically. Speckle factors were found to be 1.225 for the Nd: YLF and 3.180 for the argon laser. Thus, the maximal ED50-threshold radiant exposures for the Nd:YLF were calculated to be 362 mj/cm2 (5 µß), 478 mj/cm2 (1.7 µ-s), and 438 mj/cm2 (200 ns) ophthalmoscopically. Angiographically, the thresholds were 189 mj/cm2 (5 µß), 143 mj/cm2 (1.7 µ-s), and 97 mj/cm2 (200 ns). For the argon laser, the maximal ED50 radiant exposure threshold was 170 mj/cm2 angiographically. * CONCLUSION: The gap between the angiographic and the ophthalmoscopic thresholds for the 200 ns regime (4.5 times above angiographic ED50) was wider than for the 1.7 µ$ regime (3.3 times above the angiographic ED50). This would suggest the appropriate treatment would be 200 ns pulses. However, histologies have yet to prove that nonvisible mechanical effects increase with shorter pulse durations and could reduce the "therapeutic window." When comparing the thresholds with 5 µß pulses from the argon and Nd:YLF laser, it demonstrates that intensity modulations in the beam profile must be considered. [Ophthalmic Surg Lasers 200233:400-409]