Shrodinger tin1e-dependent equation 351
The metodology of the rnethod of separation of variables guides the
choice ofy(x,t):
N-i.
'tfj(x • ·s-L_, )- ~ c^1 k Xk(x) '.s>
k=l
where Xk(x 8 ) refer to the eigenfunctions of the operator A, meaning, by
definition,
k = 1, 2, ... , N - 1,
4.? Irkh
).k = h? sin- --.
- 2
On the strength of the preceding decomposition we establish the recurrence
relation for the coefficients
k=l,2, ... ,N-1,
where
i - (1-o-) T ).k -(l - O"o) T ).k + i(l + 0" 1 T ).k)
qk= i+a-r>.k = o- 0 r>.k+i(l+o- 1 r>.k) '
and the useful relations for yj+i:
N-1
11 Yj +i 112 = L I qk I 2 I ci I 2 < mkax I qk I 2 · 11 Yj 112 •
k=l
Simple algebra gives
implying that I qk I < 1 and thereby justifying that this scheme is stable:
for
If o- 0 < ~' then I qk I > 1 and the scheme becomes unstable, thus
causing some difficulties. In particular, the explicit scheme with a- = 0 is