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1: 26.13 Permutations: Cycle Notation
§26.13 Permutations: Cycle Notation
is ( 1 , 3 , 2 , 5 , 7 ) ( 4 ) ( 6 , 8 ) in cycle notation. Cycles of length one are fixed points. … For the example (26.13.2), this decomposition is given by ( 1 , 3 , 2 , 5 , 7 ) ( 6 , 8 ) = ( 1 , 3 ) ( 2 , 3 ) ( 2 , 5 ) ( 5 , 7 ) ( 6 , 8 ) . Again, for the example (26.13.2) a minimal decomposition into adjacent transpositions is given by ( 1 , 3 , 2 , 5 , 7 ) ( 6 , 8 ) = ( 2 , 3 ) ( 1 , 2 ) ( 4 , 5 ) ( 3 , 4 ) ( 2 , 3 ) ( 3 , 4 ) ( 4 , 5 ) ( 6 , 7 ) ( 5 , 6 ) ( 7 , 8 ) ( 6 , 7 ) : inv ( ( 1 , 3 , 2 , 5 , 7 ) ( 6 , 8 ) ) = 11 .
2: 26.2 Basic Definitions
Cycle
Given a finite set S with permutation σ , a cycle is an ordered equivalence class of elements of S where j is equivalent to k if there exists an = ( j , k ) such that j = σ ( k ) , where σ 1 = σ and σ is the composition of σ with σ 1 . …If, for example, a permutation of the integers 1 through 6 is denoted by 256413 , then the cycles are ( 1 , 2 , 5 ) , ( 3 , 6 ) , and ( 4 ) . …
3: 21.7 Riemann Surfaces
Removing the singularities of this curve gives rise to a two-dimensional connected manifold with a complex-analytic structure, that is, a Riemann surface. All compact Riemann surfaces can be obtained this way.On this surface, we choose 2 g cycles (that is, closed oriented curves, each with at most a finite number of singular points) a j , b j , j = 1 , 2 , , g , such that their intersection indices satisfy …
See accompanying text
Figure 21.7.1: A basis of cycles for a genus 2 surface. Magnify
Note that for the purposes of integrating these holomorphic differentials, all cycles on the surface are a linear combination of the cycles a j , b j , j = 1 , 2 , , g . …
4: 21.1 Special Notation
g , h positive integers.
a b intersection index of a and b , two cycles lying on a closed surface. a b = 0 if a and b do not intersect. Otherwise a b gets an additive contribution from every intersection point. This contribution is 1 if the basis of the tangent vectors of the a and b cycles21.7(i)) at the point of intersection is positively oriented; otherwise it is 1 .
a ω line integral of the differential ω over the cycle a .
5: 4.13 Lambert W -Function
For the definition of Stirling cycle numbers of the first kind [ n k ] see (26.13.3). …
4.13.10 W k ( z ) ξ k ln ξ k + n = 1 ( 1 ) n ξ k n m = 1 n [ n n m + 1 ] ( ln ξ k ) m m ! ,
4.13.11 W ± 1 ( x 0 i ) η ln η + n = 1 1 η n m = 1 n [ n n m + 1 ] ( ln η ) m m ! ,
6: 26.4 Lattice Paths: Multinomial Coefficients and Set Partitions
M 2 is the number of permutations of { 1 , 2 , , n } with a 1 cycles of length 1, a 2 cycles of length 2, , and a n cycles of length n : …(The empty set is considered to have one permutation consisting of no cycles.) …
7: Bibliography G
  • X. Guan, O. Zatsarinny, K. Bartschat, B. I. Schneider, J. Feist, and C. J. Noble (2007) General approach to few-cycle intense laser interactions with complex atoms. Phys. Rev. A 76, pp. 053411.
  • 8: 3.6 Linear Difference Equations
    If agreement is not within a prescribed tolerance the cycle is continued. …
    9: 26.8 Set Partitions: Stirling Numbers
    s ( n , k ) denotes the Stirling number of the first kind: ( 1 ) n k times the number of permutations of { 1 , 2 , , n } with exactly k cycles. …