We consider the TRS containing the following rules:
h(f,a,a) | → | h(g,a,a) | (1) |
h(g,a,a) | → | h(f,a,a) | (2) |
a | → | a' | (3) |
h(x,a',y) | → | h(x,y,y) | (4) |
h(x,y,a') | → | h(x,y,y) | (5) |
The underlying signature is as follows:
{h/3, f/0, a/0, g/0, a'/0}t0 | = | h(g,a,a) |
→ | h(g,a,a') | |
→ | h(g,a',a') | |
= | t2 |
t0 | = | h(g,a,a) |
→ | h(f,a,a) | |
→ | h(f,a,a') | |
→ | h(f,a',a') | |
= | t3 |
Automaton 1
final states:
{33}
transitions:
a' | → | 34 |
a' | → | 35 |
g | → | 36 |
h(36,34,34) | → | 33 |
h(36,35,35) | → | 33 |
h(36,35,34) | → | 33 |
Automaton 2
final states:
{29}
transitions:
a' | → | 30 |
a' | → | 31 |
h(32,30,30) | → | 29 |
h(32,31,31) | → | 29 |
h(32,31,30) | → | 29 |
f | → | 32 |