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  1. conwaylife.com › wiki › OmniperiodicOmniperiodic - LifeWiki

    Dec 9, 2023 · Conway's Game of Life is omniperiodic, since there are oscillators of every period, with the last found period being p41 in July 2023. The last periods to be found are as follows: p39 (the first non-trivial example) in July 2000. p27 in November 2002. p51 (the first non-trivial example) in March 2009. p37 in April 2009.

  2. Dec 5, 2023 · At the turn of the millennium, only twelve oscillator periods remained to be found in Conway's Game of Life. The search has finally ended, with the discovery of oscillators having the final two periods, 19 and 41, proving that Life is omniperiodic.

  3. The Game of Life, also known as Conway's Game of Life or simply Life, is a cellular automaton devised by the British mathematician John Horton Conway in 1970. [1] It is a zero-player game, [2][3] meaning that its evolution is determined by its initial state, requiring no further input. One interacts with the Game of Life by creating an initial ...

  4. conwaylife.com › wiki › 204P41204P41 - LifeWiki

    Sep 21, 2024 · 204P41 is a period-41 oscillator found by Nico Brown on July 21, 2023, and is the first period-41 oscillator to be discovered. [1] [2] Its discovery proved that Conway's Game of Life is omniperiodic. It was originally found as 208P41, and the blinker eaters were quickly reduced by two cells each.

  5. Dec 13, 2023 · Back in 1970, the mathematician John Conway created a game with no players that evolves entirely from its initial state. The game is set in a kind of computational universe called a cellular automaton.

  6. Jan 18, 2024 · John Conway’s Game of Life, a famous cellular automaton, has been found to have periodic patterns of every possible length. This pattern in the Game of Life repeats itself after 41 steps. Its recent discovery ends a decades-long quest to show that Life is omniperiodic. DVDP for Quanta Magazine.

  7. Conway’s Game of Life is by far the most famous cellular automaton. David Buckingham first established a finite bound above which oscillators of every period could be built by running a signal around a specially constructed track.

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