Further analysis showed that the ESPs of patients 2, 4, 5, 6, and 9 could be decomposed into two components: a larger-amplitude component (C1), and a residual, lower-amplitude component (C2;
Figs. 7 8 9 ). Component C1 moved the eye toward the occluded eye and appeared to approach a steady state position. Component C2 was periodic. In patients 4, 6, and 9, C1 had entirely an exponential form
(Figs. 7 8) , whereas in patients 2 and 5, it was initially linear before decelerating
(Fig. 9) . For the exponential C1, the amplitude ranged from 1° to 5°, and the time constant ranged from 0.4 to 0.6 seconds. For the linear C1, the slope was 1.6 deg/s in patient 5 and 2.8 deg/s in patient 2, with the intercept at −25.7° and −1.5°, respectively. The ESPs of all five patients were dominated by C1, which gave either an overall decreasing-velocity or linear profile to the drift
(Figs. 2 3) . The pendular oscillations of the second component had a frequency of 1.5 to 3 Hz and amplitude of 0.1° to 0.3°. Because of its low amplitude, C2 made little contribution to the ESP curve in patients 6 and 9, but was slightly more noticeable in patients 2, 4, and 5
(Figs. 7 8 9) .
Analysis of the nystagmus cycle preceding the ESP indicated that two components, similar to those of the ESP, were present in the usual slow phase of these patients. Because of the short slow phase duration, it was difficult to isolate these components. Isolation was accomplished using the parameters found from the ESP. Only minor changes in C1 were needed to fit the slow phase (a small time shift of the exponential for patients 4, 6, and 9 and a slight adjustment of the linear slope for patients 2 and 5). Comparison of the component metrics between the usual slow phase and the ESP in each patient showed a similar C1 profile, although its eventual deceleration was better seen in the ESP. Moreover, because the usual slow phase revealed only a fraction of the C2 periodicity, the frequency and amplitude of the second component could not be determined
(Figs. 7 8 9) .