Young, albino rabbit eyes were received on ice (Pel-Freez, Rogers,
AR) approximately 17 to 24 hours after death and enucleation. The eyes
were kept on ice and used the same day. The eye to be studied was
mounted on a plastic-covered polystyrene block and fixed in position by
needles inserted through the extraocular muscles into the polystyrene.
The eye was then placed under a dissecting microscope allowing
visualization of the treated area during the entire procedure. A
27-gauge needle was inserted parallel to the iris, 2 mm anterior to the
limbus into clear cornea, and positioned above the lens in the anterior
chamber. The needle was connected to both a blood pressure transducer
(Harvard Apparatus, Holliston, MA) and a mini-infuser (Bard 400;
Harvard) through a T coupler. The pressure transducer consists of a
transducer element that is hardwired to an amplifier box and uses a
semidisposable dome with an integral silicone rubber membrane. Pressure
inside the dome is transmitted through the membrane to a plastic
button, the motion of which is translated to a voltage. The voltage
generated by the transducer–amplifier combination is proportional to
the lower limit of intraocular pressure (IOP). Signals from the
transducer amplifier were recorded on a computer (Macintosh G3
Powerbook; Apple, Cupertino, CA, equipped with a PCMICA[
Daqcard-1200] data acquisition card; National Instruments,
Austin, TX). Data acquisition was controlled using programs written in
commercial software (LabView 4; National Instruments). The voltage from
the transducer and amplifier was converted to pressure by
calibrating with a standing manometer.
Experiments on individual eyes were initiated by increasing the IOP to
30 to 40 mm Hg, using water infusion at a rate of 1 ml/min. An incision
was made in the cornea, 1 mm anterior to the limbus (j) and
parallel to the iris, using a 3.5-mm angled keratome (Becton Dickinson,
Lincoln Park, NJ). For each eye, the IOP required to produce fluid
leakage from the incision (IOPL) was
recorded before and after PKD treatment. The photosensitizer, dissolved
in phosphate buffer solution (PBS [pH 7.2]; Gibco, Grand Island, NY)
was applied to the walls of the incision using a gastight 50-μl
syringe (Hamilton, Reno, NV) with a 27-gauge needle. Confocal
fluorescence spectroscopy confirmed the location of RB on the incision
walls and indicated that the photosensitizer penetrated approximately
100 μm laterally into the wall of the incision.
The photosensitizers, their absorption maxima, and their absorption
coefficients at the laser wavelength were: RB, 550 nm, 33,000
dm3/mol per centimeter at 514 nm; Fl, 490
nm, 88,300 dm3/mol per centimeter at 488 nm; MB,
664 nm, 15,600 dm3/mol per centimeter at 661 nm;
R-5-P, 445 nm, 4330 dm3/mol per centimeter at 488
nm; and N-hydroxypyridine-2-(1H)-thione (N-HPT), 314 nm, 2110
dm3/mol per centimeter at 351 nm. The
photosensitizers were used as received, with the exception of N-HPT,
which was recrystallized twice from aqueous ethanol before use. The
concentrations of the photosensitizers were adjusted so that all the
solutions had an absorbance of approximately 1.0 in a path length of
200 μm at the laser irradiation wavelength, with the exception of
N-HPT for which the absorption was lower by approximately a factor of
10.
Irradiations used a continuous-wave (CW) argon-ion laser (Innova 100;
Coherent, Palo Alto, CA) at 488 nm (for Fl and R-5-P), 514.5 nm (for
RB), or 351 nm (for N-HPT). An argon-ion pumped-dye laser (CR-599;
Coherent) with
4-dicyanomethylene-2-methyl-6-(p-dimethylaminostyryl)-4H-pyran
dye (Exciton, Dayton, OH) was used for irradiation at 661 nm (for MB).
Laser light was coupled into a 1-mm diameter quartz fiber, and a 1- cm
diameter spot on the tissue was created by using a combination of 1-
and 2-in. focal length, S1-UV–grade fused silica, biconvex lenses
(Esco Products, Oak Ridge, NJ), mounted in a cage assembly (SM1 series;
ThorLabs, Newton, NJ). The 1-cm diameter circular spot was sufficient
to cover the entire incision, and the optics were adjusted so that the
laser light was incident on the cornea at an angle approximately
45o to the plane of the incision. Dose–response
curves were obtained by varying the duration of the irradiation at a
constant irradiance. In separate experiments, the effects of laser
irradiance were investigated by comparison of the same delivered dose
using different irradiances. The doses used ranged from 124 to 1524
J/cm2, and the irradiances used were 0.64, 1.27,
2.55, and 3.86 W/cm2. The laser exposure time
varied from 33 seconds for the lowest dose using the highest irradiance
to 26 minutes, 27 seconds for the highest dose using the lowest
irradiance.
The IOP
L was recorded immediately after
treatment. Infusion was started (1 ml/min), and the IOP increased until
a maximum was reached, followed by a sharp decrease, corresponding to
the opening of the incision and leakage of fluid from the anterior
chamber. A typical trace showing the changes in IOP with infusion time
is shown in
Figure 1 . Five to 10 rabbit eyes were tested for each condition of dose and
irradiance.
Control experiments included: irradiation with no photosensitizer
application, photosensitizer application only and no photosensitizer or
laser irradiation. In the experiments using no photosensitizer, PBS was
applied to the incision walls, using the same method as described for
the photosensitizers. In control experiments with no laser irradiation,
the eye was allowed to stand for the same period as the laser-treated
samples.