olcott <NoOne@NoWhere.com> writes:
On 9/25/2021 4:24 PM, Ben Bacarisse wrote:
olcott <NoOne@NoWhere.com> writes:
On 9/25/2021 3:43 PM, Ben Bacarisse wrote:Your annotations are still wrong. Mine (in fact Linz's) are the correct >>> ones regardless of whether I (or he) includes the states you are so
olcott <NoOne@NoWhere.com> writes:You skipped some Linz specified states.
On 9/24/2021 6:22 PM, Ben Bacarisse wrote:What new nonsense is this? No one is annotating "all of the steps" of a >>>>> TM. The annotations explain which formal statements apply in which
olcott <NoOne@NoWhere.com> writes:
On 9/24/2021 3:54 PM, Ben Bacarisse wrote:Not the issue. (Though I'll note again that you don't use the notation >>>>>>> you came up with in a helpful way. There is no need for qx because it >>>>>>> could be called H.q0 or, better yet, H.0.)
olcott <NoOne@NoWhere.com> writes:
Ĥ.q0 ⟨Ĥ⟩ ⊢* Ĥ.qx ⟨Ĥ⟩ ⟨Ĥ⟩ ⊢* Ĥ.qy ∞ >>>>>>>>>> if the simulated ⟨Ĥ⟩ applied to ⟨Ĥ⟩ halts, and"I always used this symbol Ĥ in the context of the Linz proofs and
Ĥ.q0 ⟨Ĥ⟩ ⊢* Ĥ.qx ⟨Ĥ⟩ ⟨Ĥ⟩ ⊢* Ĥ.qn
if the simulated ⟨Ĥ⟩ applied to ⟨Ĥ⟩ does not halt >>>>>>>>> This is wrong since, apparently,
never used it in any other way"
If Ĥ refers to the Ĥ in Linz's proof your annotations are incorrect, and
if Ĥ is being using "in the context of the Linz proof" but denotes >>>>>>>>> something else (what?) then you are not being serious.
As you have indicated that you have recalled I corrected the error in >>>>>>>> the Linz specification that had two start states by changing one of >>>>>>>> these start states to qx.
After this I augmented the Linz notation further so that it showed the >>>>>>>> notation when the Linz Ĥ is specifically applied to the Linz ⟨Ĥ⟩ whereNot the issue but if you used the . notation better this would be much clearer.
the halt decider embedded at qx is a simulating halt decider.
Since Linz does not exclude simulating halt deciders this is still the >>>>>>>> Linz Ĥ.
You annotations are incorrect. If you'd like to know why, ask an >>>>>>> intelligent question. But why are you making any claims at all about >>>>>>> TMs that don't exist?
How would you annotate all of the steps of the Linz Ĥ applied to its >>>>>> own machine description?
situations:
Ĥ.q0 ⟨Ĥ⟩ ⊢* ∞ if Ĥ applied to ⟨Ĥ⟩ halts, and >>>>> Ĥ.q0 ⟨Ĥ⟩ ⊢* Ĥ.qn if Ĥ applied to ⟨Ĥ⟩ does not halt. >>>>
obsessed with.
As always you can dogmatically assert that I am wrong yet cannot
provide any evidence of my error because there is in fact no error.
What would be the point in copying here what Linz says in his book
again? I have, in fact, gone through the steps from the definition of
the problem to the two lines above but it had no effect. It's right
there in the book -- the simple steps from definition
H.q0 w ⊢* H.qy if H applied to w halts, and
H.q0 w ⊢* H.qn if H applied to w does not halt,
through the construction of H' and H^ to the conclusion above. Do you
think you'd pay attention this time if I went though it all again? No,
you just want to pretend that there is no "evidence" for what I say.
Have another go. See if you can write the two lines about Ĥ.q0 ⟨Ĥ⟩ >>> correctly with intermediate states you love so much.
When the halt decider at Ĥ.qx is a simulating halt decider
Ĥ.q0 ⟨Ĥ⟩ ⊢* Ĥ.qx ⟨Ĥ⟩ ⟨Ĥ⟩ ⊢* Ĥ.qy ∞
if the simulated ⟨Ĥ⟩ applied to ⟨Ĥ⟩ halts, and
Ĥ.q0 ⟨Ĥ⟩ ⊢* Ĥ.qx ⟨Ĥ⟩ ⟨Ĥ⟩ ⊢* Ĥ.qn
if the simulated ⟨Ĥ⟩ applied to ⟨Ĥ⟩ does not halt
Provided the first clause applies "if Ĥ applied to ⟨Ĥ⟩ halts", and the second one "if Ĥ applied to ⟨Ĥ⟩ does not halt", you can add any old guff
you like. So just make sure you say something like
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