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===Differentiation=== '''[[derivative|Differentiation]]''' of species intuitively corresponds to building "structures with a hole", as shown in the illustration below. [[File:Derivative of combinatorial species.svg|200px|center]] Formally,<ref>{{harvnb|Joyal|1981|loc=Β§ 2.3. Definition 8}}</ref> :<math>(F')[A] = F[A \uplus \{\star\}],</math> where <math>\star</math> is some distinguished new element not present in <math>A</math>. To differentiate the associated exponential series, the sequence of coefficients needs to be shifted one place to the "left" (losing the first term). This suggests a definition for species: ''F' ''[''A''] = ''F''[''A'' + {*}], where {*} is a singleton set and "+" is disjoint union. The more advanced parts of the theory of species use differentiation extensively, to construct and solve [[differential equation]]s on species and series. The idea of adding (or removing) a single part of a structure is a powerful one: it can be used to establish relationships between seemingly unconnected species. For example, consider a structure of the species ''L'' of linear orders—lists of elements of the ground set. Removing an element of a list splits it into two parts (possibly empty); in symbols, this is ''L''' = ''L''Β·''L''. The exponential generating function of ''L'' is ''L''(''x'') = 1/(1 β ''x''), and indeed: :<math> \frac d {dx} {(1-x)}^{-1} = {(1-x)}^{-2}. </math> The generalized differentiation formulas are to be found in a previous research by N. G. de Bruijn, published in 1964. The species ''C'' of cyclic permutations takes a set ''A'' to the set of all cycles on ''A''. Removing a single element from a cycle reduces it to a list: ''C''' = ''L''. We can [[Integral|integrate]] the generating function of ''L'' to produce that for ''C''. :<math> C(x) = 1 + \int_0^x \frac{dt}{1-t} = 1 + \log \frac{1}{1-x}. </math> A nice example of integration of a species is the completion of a line (coordinatizated by a field) with the infinite point and obtaining a projective line.
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