Function `d1char.d1nat`

is applied to a pair of vectors of characters or to a pair of 1d arrays of characters and generates then the pair of corresponding probability vectors by calling `d1nat`

function

1 | ```
d1char.d1nat(farr0, farr1, reject = c(""))
``` |

`farr0` |
vector of characters |

`farr1` |
vector of characters |

`reject` |
vector of rejected characters (the characters excluded from original vectors for analysis) |

First, it assigns the identification number for each individual character met in original vectors. Then it works similarly to `hist`

function but for the pair of samples with identification numbers as outcomes. It prints the decoding array (listing the identification numbers corresponded for each character) and, as a bonus, it prints basic statistics summary for distributions alongside with technical plot. It is recommended for use as a data preparation step before the following Klimontovich's S-theorem based analysis.

`f0 ` |
probability vector representing state0 of a system |

`f1 ` |
probability vector representing state1 of a system |

Vitaly Efremov <vitaly.efremov@dcu.ie>

`crit.stheorem`

,
`cxds.stheorem`

,
`d1nat`

1 2 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 | ```
s0<-c("?", "!", "1", "a", "b", "b", "s", "x", "y", "z", "z", "z")
s1<-c("1", "1", "2", "b", "b", "s", "s", "x", "y", "z", "z", "z", "z")
b<-d1char.d1nat(farr0=s0,farr1=s1); b
s0<-"three witches watch three swatch watches. which witch watch which swatch watch?"
s1<-"who discovered america five hundred years ago? a brave man! indeed he was! discovered!"
b<-d1char.d1nat(unlist(strsplit(s0,"")),unlist(strsplit(s1,"")),
reject=c("."," ","!","d","e")); b
#example of 2-step data analysis with Klimontovich's S-theorem
s0<-c("a","b",rep("c",9),rep("d",2),"e","f","g",rep("h",2),"i","j"); s0
s1<-c(rep("a",16), rep("c",35), rep("i",13)); s1
# step a. Create probability vectors. It seems that s0 has lower level
# of orderliness (Shannon entropy is higher)
b<-d1char.d1nat(s0,s1); b
# step b. Compare samples with Klimontovich's S-theorem. Renormalized entropy indicates
# the opposite: s0 is more ordered and difference in Shannon
# entropy values was due to just "thermodynamic noise"
crit.stheorem(b$f0,b$f1)
cxds.stheorem(b$f0,b$f1)
``` |

Questions? Problems? Suggestions? Tweet to @rdrrHQ or email at ian@mutexlabs.com.

Please suggest features or report bugs with the GitHub issue tracker.

All documentation is copyright its authors; we didn't write any of that.