Gérard TAILLE wrote:
Bill Spight wrote:
No, but playing in a number with gote entails an actual loss. Another way of putting that is to say that playing in a number with gote happens at a subzero temperature. CGT has what is called the
number avoidance theorem, which indicates that optimal play is not in a number if a non-number option exists. If only numbers are left, then the sum of those numbers is the score of the game. Playing in a number is possible, but unnecessary.
That is why we do not normally consider play in numbers in chilled go, and are only concerned with plays at or above temperature 0.

I agree with with you Bill but we are moving away from my point. Often it is more easier to understand the theory than to understand the difficulty of somebody else.
The general topic is atomic weights. I am not sure what your problem is. Or if you actually have one.

Gérard TAILLE wrote:
Bill Spight wrote:
The question is not that of winning the game, but of getting the last play at temperature 0.
Let's take this obvious game
- Click Here To Show Diagram Code
[go]$$W White to play
$$ -----------------------
$$ | O X . . . . . . O X |
$$ | O X . . . . . . O . |
$$ | . X . . . . . . O . |
$$ | . X . . . . . . O . |
$$ | . X . . . . . . X X |
$$ | O O . . . . . . . . |
$$ | . . . . . . . . . . |
$$ | . . . . . . . . . . |
$$ | . . . . . . . . . . |
$$ | . . . . . . . . . . |
$$ -----------------------[/go]
- Click Here To Show Diagram Code
[go]$$W White to play
$$ -----------------------
$$ | O X . . . . . . O X |
$$ | O X . . . . . . O 6 |
$$ | 5 X . . . . . . O 4 |
$$ | 3 X . . . . . . O 2 |
$$ | 1 X . . . . . . X X |
$$ | O O . . . . . . . . |
$$ | . . . . . . . . . . |
$$ | . . . . . . . . . . |
$$ | . . . . . . . . . . |
$$ | . . . . . . . . . . |
$$ -----------------------[/go]
If your goal is only to get tedomari then black wins by the sequence above but it is not correct is it?
The result being not correct the rule of the game must be such that this way of playing gives the win to white.
Well, in chilled go the atomic weight of the position on the right is -2, and the atomic weight on the left is +1. Why is the atomic weight +1?
I am not going to derive it, 1) because it is tedious, and 2) because you have objected to the assumptions of the derivation.
- Click Here To Show Diagram Code
[go]$$W White to play
$$ -----------------------
$$ | O X . . . . . . O X |
$$ | O X . . . . . . O . |
$$ | . X . . . . . . O . |
$$ | . X . . . . . . O . |
$$ | 1 X . . . . . . X X |
$$ | O O . . . . . . . . |
$$ | . . . . . . . . . . |
$$ | . . . . . . . . . . |
$$ | . . . . . . . . . . |
$$ | . . . . . . . . . . |
$$ -----------------------[/go]
After

the atomic weight on the left is 0. I don't know whether you agree with that or not. After all, it is a positive infinitesimal, so Black gets the last play locally,
assuming correct play. The thing is, speaking informally, Black can ignore

at temperature 0 in chilled go, but not White's next play there.
- Click Here To Show Diagram Code
[go]$$W Sente
$$ -----------------------
$$ | O X . . . . . . O X |
$$ | O X . . . . . . O . |
$$ | 4 X . . . . . . O . |
$$ | 3 X . . . . . . O . |
$$ | 1 X . . . . . . X X |
$$ | O O . . . . . . . . |
$$ | . . . . . . . . . . |
$$ | . . . . . . . . . . |
$$ | . . . . . . . . . . |
$$ | . . . . . . . . . . |
$$ -----------------------[/go]
In similar manner to evaluating mean values of hot positions, atomic weight theory assumes that sente are answered, as a rule. There are execptions, OC, but that's the default.
The position on the right has atomic weight -2. That means that at temperature 0 in chilled go, White can ignore two Black plays, as a rule.
- Click Here To Show Diagram Code
[go]$$B Black first
$$ -----------------------
$$ | O X . . . . . . O X |
$$ | O X . . . . . . O . |
$$ | . X . . . . . . O 3 |
$$ | . X . . . . . . O 1 |
$$ | . X . . . . . . X X |
$$ | O O . . . . . . . . |
$$ | . . . . . . . . . . |
$$ | . . . . . . . . . . |
$$ | . . . . . . . . . . |
$$ | . . . . . . . . . . |
$$ -----------------------[/go]

is not sente, it is ambiguous, as it does not raise the local temperature. White can ignore it. In fact, after

the position on the right has atomic weight 0. It is gote, but the atomic weight is 0, even though White can reply locally.
Not that you do not know this, OC.

The atomic weight of the sum is -2 + 1 = -1. So White has the advantage in the fight for the last play at temperature 0. Getting the last play at temperature 0 is the point of atomic weight theory. That's what it is about.
Now, an advantage of 1 atomic weight is not enough to guarantee getting the last play at temperature 0,
given correct play. CGT assumes correct or optimal play, unless otherwise stated. (Edit: OC, in proofs everything is stated.

But the default assumption is correct or optimal play.)
- Click Here To Show Diagram Code
[go]$$W Incorrect play
$$ -----------------------
$$ | O X . . . . . . O X |
$$ | O X . . . . . . O 6 |
$$ | 5 X . . . . . . O 4 |
$$ | 3 X . . . . . . O 2 |
$$ | 1 X . . . . . . X X |
$$ | O O . . . . . . . . |
$$ | . . . . . . . . . . |
$$ | . . . . . . . . . . |
$$ | . . . . . . . . . . |
$$ | . . . . . . . . . . |
$$ -----------------------[/go]

is a mistake, so this sequence lies outside the scope of atomic weight theory.
- Click Here To Show Diagram Code
[go]$$W Correct play
$$ -----------------------
$$ | O X . . . . . . O X |
$$ | O X . . . . . . O . |
$$ | 4 X . . . . . . O 5 |
$$ | 3 X . . . . . . O 2 |
$$ | 1 X . . . . . . X X |
$$ | O O . . . . . . . . |
$$ | . . . . . . . . . . |
$$ | . . . . . . . . . . |
$$ | . . . . . . . . . . |
$$ | . . . . . . . . . . |
$$ -----------------------[/go]

is correct, as assumed by the theory as the default. And White does get the last play at temperature 0.
