We consider the TRS containing the following rules:
b | → | h(h(b,a),f(a)) | (1) |
h(h(a,c),b) | → | b | (2) |
c | → | h(h(a,h(a,h(c,b))),f(f(h(h(a,h(h(f(a),c),f(c))),f(h(b,a)))))) | (3) |
The underlying signature is as follows:
{b/0, h/2, a/0, f/1, c/0}t0 | = | h(h(a,c),b) |
→ | h(h(a,c),h(h(b,a),f(a))) | |
→ | h(h(a,h(h(a,h(a,h(c,b))),f(f(h(h(a,h(h(f(a),c),f(c))),f(h(b,a))))))),h(h(b,a),f(a))) | |
→ | h(h(a,h(h(a,h(a,h(h(h(a,h(a,h(c,b))),f(f(h(h(a,h(h(f(a),c),f(c))),f(h(b,a)))))),b))),f(f(h(h(a,h(h(f(a),c),f(c))),f(h(b,a))))))),h(h(b,a),f(a))) | |
= | t3 |
t0 | = | h(h(a,c),b) |
→ | b | |
→ | h(h(b,a),f(a)) | |
→ | h(h(h(h(b,a),f(a)),a),f(a)) | |
= | t3 |