We consider the TRS containing the following rules:
b | → | f(b) | (1) |
h(h(h(h(h(h(h(a,h(c,h(f(c),b))),h(b,h(b,h(f(f(h(c,b))),a)))),h(a,a)),b),f(h(h(f(a),a),c))),a),h(c,a)) | → | f(a) | (2) |
c | → | h(b,b) | (3) |
The underlying signature is as follows:
{b/0, f/1, h/2, a/0, c/0}t0 | = | h(h(h(h(h(h(h(a,h(c,h(f(c),b))),h(b,h(b,h(f(f(h(c,b))),a)))),h(a,a)),b),f(h(h(f(a),a),c))),a),h(c,a)) |
→ | h(h(h(h(h(h(h(a,h(c,h(f(c),f(b)))),h(b,h(b,h(f(f(h(c,b))),a)))),h(a,a)),b),f(h(h(f(a),a),c))),a),h(c,a)) | |
= | t1 |
t0 | = | h(h(h(h(h(h(h(a,h(c,h(f(c),b))),h(b,h(b,h(f(f(h(c,b))),a)))),h(a,a)),b),f(h(h(f(a),a),c))),a),h(c,a)) |
→ | f(a) | |
= | t1 |