Accommodation was continuously recorded using a modified Canon
Auto Ref R1 infrared optometer
(Fig. 1) .
15 16 The instrument’s capacity to record accommodation
levels statically is maintained, so that both static and continuous
measures are possible. This optometer is particularly suited to the
study of accommodation because it has an open field view and because
the stimulus is presented as a real object in real space. This is
achieved using an inclined semireflecting mirror that reflects infrared
light for measurement and transmits visible light for vision. This
arrangement reduces the potential for proximal effects to influence
accommodation responses.
17 Each subject used the standard
headrest provided for the Canon optometer, which had been modified to
provide a bite-bar. A dental impression was made for each observer
before recording: the use of headrest and bite-bar reduced artifact
from head movement that might otherwise have contributed to the noise
of the accommodation records. Accommodation was recorded monocularly
from the eye preferred by the subject, and the other eye was occluded.
The accommodation stimulus was a high-contrast single Snellen letter
transparency (limb width, 1.09 mm) mounted onto the pen support base of
an X–Y plotter (Bryans 60,000). A function generator (Phillips PM
5133) was used to drive this base sinusoidally. The target was
back-illuminated by an electroluminescent panel, which provided a
target luminance of 36 cd/m2 and was attached to
the target. The target was viewed directly, in free space and
oscillated sinusoidally over a distance from 42 cm (2.38 D) to 75 cm
(1.33 D), which lay well within the amplitude of accommodation of all
observers. When the distance sinusoid is inverted to convert the
stimulus strength into diopters, some small distortions in the
resulting vergence sinusoid are introduced. The vergence sinusoid is
flattened at the far end of the cycle and is sharper at the near end of
the cycle. A Fourier analysis of this vergence “sinusoid” shows
that the mean level and amplitude of the fundamental sinusoidal
oscillation are reduced slightly to an amplitude of 0.51 D, oscillating
about a mean level of 1.78 D: the amplitude of higher harmonics was
small enough to be ignored. Eleven frequencies (0.05, 0.1, 0.2, 0.3,
0.4, 0.5, 0.6, 0.7, 0.8, 0.9, and 1.0 Hz) randomly presented were used;
each recording was 10.24 seconds long, and 10 were made for each
frequency. The free space viewing arrangement for the target meant that
its angular subtense was not held constant during the cycle of
oscillation. The change in target limb subtense throughout the cycle
was modest, from 8.92′ at 42 cm to 5.0′ at 75 cm.
Abrupt changes in target vergence from 2.38 to 1.33 D and vice versa
were provided using two single letter targets, one being positioned at
42 cm the other at 75 cm from the eye: these were identical with those
used for the sinusoidal changes. Each target was back-lit by an
electroluminescent panel attached to the target and mounted on a rotary
solenoid so that it could be rotated independently into and out of the
axis of the observation system. The rise and fall times of these
targets were measured as 0.1 seconds. These step measurement response
data were used to provide reaction and response times for comparison
with phase lag data.