Intraocular Photodisruption With Picosecond and Nanosecond Laser
Intraocular Photodisruption With Picosecond and Nanosecond Laser
Intraocular Photodisruption With Picosecond and Nanosecond Laser
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Tissue Effects of <strong>Picosecond</strong> <strong>and</strong> <strong>Nanosecond</strong> <strong>Photodisruption</strong> 3035<br />
from a slaughterhouse. A central portion of the cornea<br />
was excised using a 10 mm trephine. Each specimen<br />
was mounted on a teflon holder <strong>and</strong> immersed in<br />
a cuvette with physiological saline. The specimen<br />
could be precisely positioned with an xyz-micrometer<br />
stage. To produce incisions in Descemet's membrane,<br />
the laser pulses were applied from the endothelial side<br />
with a repetition rate of 10 Hz, when the specimen was<br />
moved laterally with the translation stage (Fig. 2a). We<br />
compared the effects of ps pulses with 50 n] pulse<br />
energy to those of ns pulses with a pulse energy of 1<br />
mj. Both energies are close to the threshold for plasma<br />
formation at the respective pulse duration.<br />
Intrastromal corneal laser effects were investigated to<br />
analyze the feasibility of intrastromal refractive surgery<br />
with ps pulses. Enucleated bovine eyes (n = 6)<br />
were mounted into an eye holder fixed on a translation<br />
stage. Initially, the optical axis of the eye was coaxial to<br />
the laser beam axis, <strong>and</strong> the laser pulses were focused<br />
through the cornea onto the endothelium (see Fig. 2b,<br />
which shows an enlarged view of the central cornea).<br />
The eye was then moved laterally while ps pulses with<br />
80 ^J pulse energy <strong>and</strong> 10 Hz repetition rate were<br />
applied. The laser effects produced this way were located<br />
at an increasing distance from the corneal endothelium<br />
because of the curvature of the cornea. This<br />
allows an accurate determination of the range for endothelial<br />
damage from serial sections through the<br />
laser effects.<br />
To compare the suitability of ps <strong>and</strong> ns pulses for<br />
cataract fragmentation, laser pulses were focused into<br />
a)<br />
FIGURE 2. Irradiation geometries for the investigation of tissue<br />
effects produced by picosecond <strong>and</strong> nanosecond<br />
Nd:YAG laser pulses, (a) Incision of Descemet's membrane<br />
in a corneal specimen, (b) Corneal instrastromal tissue evaporation<br />
in an enucleated eye (enlarged view), (c) Cataract<br />
emulsification. (d) Focusing into the vitreous body close to<br />
the retina.<br />
the clear lenses of whole enucleated bovine eyes <strong>and</strong><br />
into human lens nuclei obtained by extracapsular cataract<br />
extraction. One hundred microjoule ps pulses<br />
<strong>and</strong> 1.1 mj ns pulses were focused into the bovine<br />
lenses (n = 11) at a distance of about 4 mm behind the<br />
anterior lens capsule (Fig. 2c), generating a series of<br />
parallel lines. The laser effects were documented by<br />
slit lamp photography. The human lens nuclei were<br />
stored in saline at 4°C for a maximum of 24 hours<br />
until the experiment was performed. The lenses (n =<br />
23) had varying degrees <strong>and</strong> types of cataract. After<br />
removing any cortical remnants, the lens nuclei were<br />
gently clamped in a holder <strong>and</strong> immersed into a cuvette<br />
filled with saline, <strong>and</strong> ps <strong>and</strong> ns laser pulses were<br />
focused into the posterior third of the nuclei. The<br />
threshold for plasma formation was determined as described<br />
above in the clearest <strong>and</strong> in the most turbid<br />
parts of the lens nuclei.<br />
To measure the range for retinal damage during vitreous<br />
surgery with ps pulses, we used the irradiation<br />
geometry shown in Figure 2d. Bovine eyes (n = 7) were<br />
hemidissected <strong>and</strong> mounted on an xyz-translation<br />
stage, whereby traction on the retina was avoided as<br />
much as possible. Series of ps laser pulses with a pulse<br />
energy of 200 /xj each were then focused into the vitreous<br />
at various well-defined distances from the internal<br />
limiting membrane, where the retinal vessels are located.<br />
The distance between the retinal vessels <strong>and</strong> the<br />
laser focus was controlled with the micrometer translation<br />
stage. The precise control of this distance was<br />
facilitated by the eyecup preparation used, allowing<br />
optimal illumination <strong>and</strong> observation of the retina.<br />
Histology. After laser exposure, all corneal specimens<br />
were fixed in 4% glutaraldehyde, postfixed in<br />
buffered 2% osmium tetroxide, <strong>and</strong> dehydrated in alcohol.<br />
The specimens with intrastromal laser effects<br />
were put into propyleneoxide <strong>and</strong> then embedded in<br />
epon 812. Series of semithin sections (1.5 ixm) were<br />
stained with toluidine blue for light microscopy. The<br />
specimens with incisions in Descemet's membrane<br />
were critical point dried in CO2 <strong>and</strong> sputter coated<br />
with gold. The surface morphology of the lesions was<br />
studied using a scanning electron microscope (JSM<br />
35, JEOL, Tokyo, Japan). After scanning electron microscopy,<br />
the specimens were put into 100% ethanol,<br />
then in propyleneoxide, <strong>and</strong> later they were embedded<br />
in epon 812 for the preparation of semithin sections.<br />
In this way, the surface morphology <strong>and</strong> histologic<br />
sections of the same corneal lesions could be investigated.<br />
For analysis of the laser effects in the retina, the<br />
whole hemidissected globe was fixed in a 4% glutaraldehyde<br />
solution for at least 24 hours. Afterward, most<br />
of the vitreous was removed, <strong>and</strong> retinal specimens<br />
containing the lesions were prepared. They were further<br />
processed for histology as described above for the<br />
corneal specimens.