In statistical mechanics, the Potts model, a generalization of the Ising model, is a model of interacting spins on a crystalline lattice.[1] By studying the Potts model, one may gain insight into the behaviour of ferromagnets and certain other phenomena of solid-state physics. The strength of the Potts model is not so much that it models these physical systems well; it is rather that the one-dimen
ã³ã«ã¢ã´ããè¤éæ§ï¼ã³ã«ã¢ã´ãããµããã¤ãããè±èª: Kolmogorov complexityï¼ã¨ã¯ãè¨ç®æ©ç§å¦ã«ããã¦æéé·ã®ãã¼ã¿åã®è¤éãã表ãææ¨ã®ã²ã¨ã¤ã§ãåºåçµæããã®ãã¼ã¿ã«ä¸è´ããããã°ã©ã ã®é·ãã®æå°å¤ã¨ãã¦å®ç¾©ããããã³ã«ã¢ã´ããè¤é度ãã³ã«ã¢ã´ããï¼ãã£ã¤ãã£ã³è¤éæ§ (Kolmogorov-Chaitin complexity) ã¨ãå¼ã°ããã ãã®ç»åã¯ãã©ã¯ã¿ã«å³å½¢ã§ãããã³ãã«ããéåã®ä¸é¨ã§ããããã®JPEGãã¡ã¤ã«ã®ãµã¤ãºã¯17KB以ä¸ï¼ç´140,000ãããï¼ãããã¨ããããããã¨åããã¡ã¤ã«ã¯140,000ããããããé¥ãã«å°ããã³ã³ãã¥ã¼ã¿ã»ããã°ã©ã ã«ãã£ã¦ä½æãããã¨ãåºæ¥ããå¾ã£ã¦ããã®JPEGãã¡ã¤ã«ã®ã³ã«ã¢ã´ããè¤éæ§ã¯140,000ãããé¥ãã«å°ããã ã³ã«ã¢ã´ããè¤éæ§ã®æ¦å¿µã¯ä¸è¦ããã¨åç´ãªãã®ã§ãããããã¥ã¼ãªã³ã°ã®åæ¢åé¡ãã²ã¼
ã©ã³ãã³ã°
ã©ã³ãã³ã°
ã©ã³ãã³ã°
ãªãªã¼ã¹ãé害æ å ±ãªã©ã®ãµã¼ãã¹ã®ãç¥ãã
ææ°ã®äººæ°ã¨ã³ããªã¼ã®é ä¿¡
å¦çãå®è¡ä¸ã§ã
j次ã®ããã¯ãã¼ã¯
kåã®ããã¯ãã¼ã¯
lãã¨ã§èªã
eã³ã¡ã³ãä¸è¦§ãéã
oãã¼ã¸ãéã
{{#tags}}- {{label}}
{{/tags}}