We consider the TRS containing the following rules:
a | → | c | (1) |
a | → | h(c,a) | (2) |
h(b,f(c)) | → | b | (3) |
c | → | h(a,h(h(b,a),a)) | (4) |
The underlying signature is as follows:
{a/0, c/0, h/2, b/0, f/1}t0 | = | h(b,f(c)) |
→ | h(b,f(h(a,h(h(b,a),a)))) | |
= | t1 |
t0 | = | h(b,f(c)) |
→ | b | |
= | t1 |
Automaton 1
final states:
{1}
transitions:
h(4,3) | → | 5 |
h(5,2) | → | 6 |
h(10,9) | → | 1 |
h(2,2) | → | 3 |
h(2,2) | → | 7 |
h(2,2) | → | 2 |
h(7,6) | → | 8 |
h(2,6) | → | 7 |
h(2,6) | → | 2 |
h(2,6) | → | 3 |
f(8) | → | 9 |
c | → | 3 |
c | → | 7 |
c | → | 2 |
a | → | 2 |
a | → | 3 |
a | → | 7 |
b | → | 4 |
b | → | 10 |
Automaton 2
final states:
{11}
transitions:
b | → | 11 |