9,097,749 research outputs found

    3x+13x+1 inverse orbit generating functions almost always have natural boundaries

    Full text link
    The 3x+k3x+k function Tk(n)T_{k}(n) sends nn to (3n+k)/2(3n+k)/2 resp. n/2,n/2, according as nn is odd, resp. even, where k±1 (mod6)k \equiv \pm 1~(\bmod \, 6). The map Tk()T_k(\cdot) sends integers to integers, and for m1m \ge 1 let nmn \rightarrow m mean that mm is in the forward orbit of nn under iteration of Tk().T_k(\cdot). We consider the generating functions fk,m(z)=n>0,nmzn,f_{k,m}(z) = \sum_{n>0, n \rightarrow m} z^{n}, which are holomorphic in the unit disk. We give sufficient conditions on (k,m)(k,m) for the functions fk,m(z)f_{k, m}(z) have the unit circle {z=1}\{|z|=1\} as a natural boundary to analytic continuation. For the 3x+13x+1 function these conditions hold for all m1m \ge 1 to show that f1,m(z)f_{1,m}(z) has the unit circle as a natural boundary except possibly for m=1,2,4m= 1, 2, 4 and 88. The 3x+13x+1 Conjecture is equivalent to the assertion that f1,m(z)f_{1, m}(z) is a rational function of zz for the remaining values m=1,2,4,8m=1,2, 4, 8.Comment: 15 page

    On the M\"obius Function of Permutations With One Descent

    Get PDF
    The set of all permutations, ordered by pattern containment, is a poset. We give a formula for the M\"obius function of intervals [1,π][1,\pi] in this poset, for any permutation π\pi with at most one descent. We compute the M\"obius function as a function of the number and positions of pairs of consecutive letters in π\pi that are consecutive in value. As a result of this we show that the M\"obius function is unbounded on the poset of all permutations. We show that the M\"obius function is zero on any interval [1,π][1,\pi] where π\pi has a triple of consecutive letters whose values are consecutive and monotone. We also conjecture values of the M\"obius function on some other intervals of permutations with at most one descent

    Hybrid moments of the Riemann zeta-function

    Get PDF
    The "hybrid" moments T2Tζ(1/2+it)k(tGt+Gζ(1/2+ix)dx)mdt \int_T^{2T}|\zeta(1/2+it)|^k{(\int_{t-G}^{t+G}|\zeta(1/2+ix)|^\ell dx)}^m dt of the Riemann zeta-function ζ(s)\zeta(s) on the critical line s=1/2\Re s = 1/2 are studied. The expected upper bound for the above expression is Oϵ(T1+ϵGm)O_\epsilon(T^{1+\epsilon}G^m). This is shown to be true for certain specific values of the natural numbers k,,mk,\ell,m, and the explicitly determined range of G=G(T;k,,m)G = G(T;k,\ell,m). The application to a mean square bound for the Mellin transform function of ζ(1/2+ix)4|\zeta(1/2+ix)|^4 is given.Comment: 27 page

    Pathological phenomena in Denjoy-Carleman classes

    Full text link
    Let CM\mathcal C^M denote a Denjoy-Carleman class of C\mathcal C^\infty functions (for a given logarithmically-convex sequence M=(Mn)M = (M_n)). We construct: (1) a function in CM((1,1))\mathcal C^M((-1,1)) which is nowhere in any smaller class; (2) a function on R\mathbb R which is formally CM\mathcal C^M at every point, but not in CM(R)\mathcal C^M(\mathbb R); (3) (under the assumption of quasianalyticity) a smooth function on Rp\mathbb R^p (p2p \geq 2) which is CM\mathcal C^M on every CM\mathcal C^M curve, but not in CM(Rp)\mathcal C^M(\mathbb R^p).Comment: 21 page

    On the Mellin transforms of powers of Hardy's function

    Full text link
    Various properties of the Mellin transform function Mk(s):=1Zk(x)xsdx {\cal M}_k(s) := \int_1^\infty Z^k(x)x^{-s}dx are investigated, where Z(t):=ζ(1/2+it)(χ(1/2+it))1/2,ζ(s)=χ(s)ζ(1s) Z(t) := \zeta(1/2+it){\bigl(\chi(1/2+it)\bigr)}^{-1/2}, \quad \zeta(s) = \chi(s)\zeta(1-s) is Hardy's function and ζ(s)\zeta(s) is Riemann's zeta-function. Connections with power moments of ζ(1/2+it)|\zeta(1/2+it)| are established, and natural boundaries of Mk(s){\cal M}_k(s) are discussed.Comment: 26 page
    corecore