Oscillator: Difference between revisions
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[[cellular automaton|Cellular automaton]] theory recognizes shift periodicity, which refers to a configuration reappearing in shifted form after a lapse of one or more generations. Without the shift, it is an oscillator, but if it moves it would be called a [[glider]] or [[spaceship]]. Strictly speaking "glider" means the little figure so prevalent in [[Conway's Game of Life]], but the more general usage has now become popular. | [[cellular automaton|Cellular automaton]] theory recognizes shift periodicity, which refers to a configuration reappearing in shifted form after a lapse of one or more generations. Without the shift, it is an oscillator, but if it moves it would be called a [[glider]] or [[spaceship]]. Strictly speaking "glider" means the little figure so prevalent in [[Conway's Game of Life]], but the more general usage has now become popular. | ||
==Important oscillators by period== | ==Important oscillators by period== | ||
A list of the first-discovered oscillator of each period, as well the current smallest-known oscillator of that period, is provided here. Note that only non-trivial oscillators are considered here, in the sense that there must be at least one [[cell]] that oscillates at the full period. In some cases, it is not known for certain what the first-discovered oscillator of a given period is, and in such situations all possible candidates are listed. For any period 61 or greater an oscillator can be constructed using the Herschel track method. | A list of the first-discovered oscillator of each period, as well the current smallest-known oscillator of that period, is provided here. Note that only non-trivial oscillators are considered here, in the sense that there must be at least one [[cell]] that oscillates at the full period. In some cases, it is not known for certain what the first-discovered oscillator of a given period is, and in such situations all possible candidates are listed. For any period 61 or greater an oscillator can be constructed using the Herschel track method. In April, [[:Category:patterns found in 2013|2013]] [[Mike Playle]] found a small 90-degree [[stable reflector]] that allows oscillators of all periods 43 or greater to be constructed. | ||
<table border="0" cellpadding="0" cellspacing="0" width="100%"><tr><td align="center" width="50%"> | <table border="0" cellpadding="0" cellspacing="0" width="100%"><tr><td align="center" width="50%"> | ||
| Line 209: | Line 209: | ||
| 1994 | | 1994 | ||
|- | |- | ||
! | ! [[:Category:oscillators with period 43|43]] | ||
| | | [[P43 glider shuttle]] | ||
| [[Mike Playle]] | |||
| [[:Category:patterns found in 2013|2013]] | |||
|- | |- | ||
! [[:Category:oscillators with period 44|44]] | ! [[:Category:oscillators with period 44|44]] | ||
| Line 257: | Line 259: | ||
| 1977 | | 1977 | ||
|- | |- | ||
! | ! [[:Category:oscillators with period 53|53]] | ||
| | | [[P53 glider shuttle]] | ||
| [[Mike Playle]] | |||
| [[:Category:patterns found in 2013|2013]] | |||
|- | |- | ||
! [[:Category:Oscillators with period 54|54]] | ! [[:Category:Oscillators with period 54|54]] | ||
| Line 510: | Line 514: | ||
| [[:Category:Patterns with 57 cells|57]] | | [[:Category:Patterns with 57 cells|57]] | ||
|- | |- | ||
! | ! 43 | ||
| | | [[P43 glider shuttle]] | ||
| [[:Category:patterns with 228 cells|228]] | |||
|- | |- | ||
! 44 | ! 44 | ||
| Line 535: | Line 540: | ||
! 49 | ! 49 | ||
| [[p49 glider shuttle]] | | [[p49 glider shuttle]] | ||
| [[:Category:Patterns with | | [[:Category:Patterns with 228 cells|228]] | ||
|- | |- | ||
! 50 | ! 50 | ||
| Line 549: | Line 554: | ||
| [[:Category:Patterns with 35 cells|35]] | | [[:Category:Patterns with 35 cells|35]] | ||
|- | |- | ||
! | ! 53 | ||
| | | [[P53 glider shuttle]] | ||
| [[:Category:patterns with 228 cells|228]] | |||
|- | |- | ||
! 54 | ! 54 | ||
| Line 565: | Line 571: | ||
|- | |- | ||
! 57 | ! 57 | ||
| [[P57 | | [[P57 glider shuttle]] | ||
| [[:Category:patterns with | | [[:Category:patterns with 228 cells|228]] | ||
|- | |- | ||
! 58 | ! 58 | ||
| [[P58 | | [[P58 glider shuttle]] | ||
| [[:Category:patterns with | | [[:Category:patterns with 208 cells|208]] | ||
|- | |- | ||
! 59 | ! 59 | ||
| [[ | | [[P59 glider shuttle]] | ||
| | | [[:Category:patterns with 228 cells|228]] | ||
|- | |- | ||
! 60 | ! 60 | ||
| Line 581: | Line 587: | ||
|- | |- | ||
! 61 | ! 61 | ||
| [[P61 | | [[P61 glider shuttle]] | ||
| | | [[:Category:patterns with 228 cells|228]] | ||
|- | |- | ||
! 63 | ! 63 | ||
Revision as of 23:11, 26 April 2013
An oscillator is a pattern that is a predecessor of itself. That is, it is a pattern that repeats itself after a fixed number of generations (known as its period). The term is usually restricted to finite patterns that are not still lifes, though still lifes may be thought of as oscillators with period 1. An oscillator is divided into a rotor and a stator.
Cellular automaton theory recognizes shift periodicity, which refers to a configuration reappearing in shifted form after a lapse of one or more generations. Without the shift, it is an oscillator, but if it moves it would be called a glider or spaceship. Strictly speaking "glider" means the little figure so prevalent in Conway's Game of Life, but the more general usage has now become popular.
Important oscillators by period
A list of the first-discovered oscillator of each period, as well the current smallest-known oscillator of that period, is provided here. Note that only non-trivial oscillators are considered here, in the sense that there must be at least one cell that oscillates at the full period. In some cases, it is not known for certain what the first-discovered oscillator of a given period is, and in such situations all possible candidates are listed. For any period 61 or greater an oscillator can be constructed using the Herschel track method. In April, 2013 Mike Playle found a small 90-degree stable reflector that allows oscillators of all periods 43 or greater to be constructed.
See also
External links
- Oscillator at the Life Lexicon