Gérard TAILLE wrote:Let me test if you agree with my calculation in order to know when starting a ko in an ideal environment.
Let's suppose that the environment is made of pure gote areas with values equal to g1, g2, g3, g4, ...
Because I suppose an ideal environmment I expect
g1 - g2 + g3 - g4 ... = g1 / 2
g2 - g3 + g4 - g5 ... = g2 / 2
etc.
if x is the value of a ko move then
1) In absence of ko threat you start the ko when 3x >= 2g1 + g2
2) If your opponent has one ko threat you start the ko a little earlier when 3x >= 2g1 + g4
3) If your opponent has two ko threats you start the ko still a little earlier when 3x >= 2g1 + g6
4) If your opponent has a lot of ko threats you can even start the ko as soon as 3x >= 2g1
Bravo!
This was basically my first result, many moons ago.

Note that each ko threat must be so large that it must be answered.
Technically, this result does not fit the model of thermography, because each gote and each threat that you take into account actually adds to the game with the ko. They are not considered part of the environment. (Edit: In thermography the right side is always 2g1 + t.) However, this result can be made more abstract to produce what Professor Berlekamp dubbed
pseudo-thermography. A different form of pseudo-thermography was developed by Kim Yonghoan.