GONALITY OF DYNATOMIC CURVES AND STRONG UNIFORM BOUNDEDNESS OF PREPERIODIC POINTS

Size: px
Start display at page:

Download "GONALITY OF DYNATOMIC CURVES AND STRONG UNIFORM BOUNDEDNESS OF PREPERIODIC POINTS"

Transcription

1 GONALITY OF DYNATOMIC CURVES AND STRONG UNIFORM BOUNDEDNESS OF PREPERIODIC POINTS JOHN R. DOYLE AND BJORN POONEN Abstrat. Fix d 2 and a field k suh that har k d. Assume that k ontains the dth roots of 1. Then the irreduible omponents of the urves over k parameterizing preperiodi points of polynomials of the form z d + are geometrially irreduible and have gonality tending to. This implies the funtion field analogue of the strong uniform boundedness onjeture for preperiodi points of z d +. It also has onsequenes over number fields: it implies strong uniform boundedness for preperiodi points of bounded eventual period, whih in turn redues the full onjeture for preperiodi points to the onjeture for periodi points. 1. Introdution 1.1. Dynatomi urves. Fix an integer d 2. Let k be a field suh that har k d. View f = f := z d + as a polynomial in z with oeffiients in k[]. Let f n (z) be the nth iterate of f; in partiular, f 0 (z) := z. If n and m are nonnegative integers with n > m, then any irreduible fator of f n (z) f m (z) k[z, ] defines an affine urve over k. By a dynatomi urve over k, we mean any suh urve, or its smooth projetive model. Any k-point on suh a urve yields 0 k equipped with a preperiodi point in k, that is, an element z 0 k that under iteration of x d + 0 eventually enters a yle; the length of the yle is alled the eventual period. We onsider two dynatomi urves to be different if the orresponding losed subshemes of A 2 k are distint. Setion 2 desribes all dynatomi urves in harateristi 0 expliitly Gonality. Let k be an algebrai losure of k. Let µ d = {x k : x d = 1}. For a urve X over k, let X k = X k k. If X is irreduible, define the gonality γ(x) of X as the least possible degree of a dominant rational map X P 1 k. If X is geometrially irreduible, define its k-gonality as γ(x k ). Theorem 1.1. Fix d 2 and k suh that har k d. Suppose that µ d k. (a) Every dynatomi urve over k is geometrially irreduible. (b) If the dynatomi urves over k are listed in any order, their gonalities tend to. Remark 1.2. Part (a) of Theorem 1.1 an fail if µ d k. See Remark 2.2. Remark 1.3. In proving Theorem 1.1 in positive harateristi, we fae the hallenge that we do not know expliitly what the dynatomi urves are, sine we are not sure whether Date: November 11, Mathematis Subjet Classifiation. Primary 37P35; Seondary 11G30, 14H51, 37P05, 37P15. Key words and phrases. Gonality, dynatomi urve, preperiodi point. The seond author was supported in part by National Siene Foundation grants DMS and DMS and Simons Foundation grants # (to Bjorn Poonen) and #

2 the known fators of the polynomials f n (z) f m (z) are irreduible. Some partial results regarding the irreduibility of dynatomi urves in positive harateristi may be found in [DKO + 17], but we will not use them. Let us now introdue notation for our seond main result. Let µ(n) denote the Möbius µ-funtion. Then f n (z) z = e n Φ e(z, ), where (1) Φ n (z, ) := e n (f e (z) z) µ(n/e) k[z, ]. Let Y dyn 1 (n) be the urve defined by Φ n (z, ) = 0 in A 2 k, and let Xdyn 1 (n) be the normalization of its projetive losure. To simplify notation, we omit the supersript dyn from now on. General points of X 1 (n) parametrize polynomials of the form z d + equipped with a point of exat order n. The morphism (z, ) (f(z), ) restrits to an order n automorphism of Y 1 (n), so it indues an order n automorphism σ of X 1 (n). The quotient of X 1 (n) by the yli group generated by σ is alled X 0 (n). irreduible, so X 0 (n) is too. If har k = 0, it is known that X 1 (n) is geometrially Theorem 1.4. Fix d 2 and a field k of harateristi 0. Then ( 1 γ(x 0 (n)) > 2 1 ) 2d o(1) n as n. In partiular, γ(x 0 (n)). Remark 1.5. Our definition of dynatomi urve does not inlude quotient urves suh as X 0 (n), so the onlusion γ(x 0 (n)) of Theorem 1.4 does not follow from Theorem 1.1(b). To prove Theorem 1.4, we use that X 0 (n) already has a morphism to P 1 of degree lower than expeted for its genus, namely X 0 (n) P 1. If it also had a morphism to P 1 of bounded degree, then the Castelnuovo Severi inequality would make the genus of X 0 (n) smaller than it atually is, a ontradition. See Setion 3 for details. To prove Theorem 1.1(b), we use different arguments in harateristi 0 and harateristi > 0. In harateristi 0, we use that eah dynatomi urve dominates X 1 (n) and hene also X 0 (n) for some n, so its gonality is large when n is large. On the other hand, for a fixed small n, the dynatomi urves above X 1 (n) ome in towers and we use the Castelnuovo Severi inequality to work our way up eah tower. See Setion 3. In harateristi p, we prove that the irreduible omponents of f n (z) f m (z) have large degree over the -line, and we use that to prove that over the finite field F q := F p (µ d ) their smooth projetive models have so many F q -points over = that their F q -gonalities must be large. Finally, we use a result ontrolling how gonality of a urve hanges when the base field is enlarged. See Setion Uniform boundedness of preperiodi points. The growth of gonalities of lassial modular urves implies the strong uniform boundedness theorem for torsion points on ellipti urves over funtion fields (the funtion field analogue of Merel s theorem [Mer96]); see [NS96, Theorem 0.3]. Similarly, from Theorem 1.1 we will dedue the following funtion field analogue of a ase of the Morton Silverman onjeture [MS94, p. 100]: 2

3 Theorem 1.6 (Strong uniform boundedness theorem for preperiodi points over funtion fields). Fix d 2 and a field k suh that har k d. Let K be the funtion field of an integral urve over k. Fix a positive integer D. Then there exists B = B(d, K, D) > 0 suh that for every field extension L K of degree D and every L not algebrai over k, the number of preperiodi points of z d + in L is at most B. If k is finite, the same holds with the words not algebrai over k deleted. See [DKO + 17, Setion 4] for some related results and arguments. Another appliation of Theorem 1.1 is the following, whih over number fields provides a uniform bound on preperiodi points having a bounded eventual period: Theorem 1.7. Fix integers d 2, D 1, and N 1. Then there exists B = B(d, D, N) > 0 suh that for every number field K satisfying [K : Q] D and every K, the number of preperiodi points of z d + in K with eventual period at most N is at most B. Theorems 1.6 and 1.7 are proved in Setion 5. Theorem 1.7 implies that the strong uniform boundedness onjeture for periodi points over number fields implies the strong uniform boundedness onjeture for preperiodi points over number fields, as we now explain: Corollary 1.8. Fix integers d 2 and D 1. Suppose that there exists a bound N = N(d, D) suh that for every number field K satisfying [K : Q] D and every K, every periodi point of z d + in K has period at most N. Then there exists a bound B = B (d, D) suh that for every number field K satisfying [K : Q] D and every K, the number of preperiodi points of z d + in K is at most B. Proof. By assumption, if [K : Q] D and K, then the preperiodi points of z d + in K having eventual period at most N are all the preperiodi points in K. Therefore the bound B(d, D, N) of Theorem 1.7 is atually a bound on the total number of preperiodi points in K. Take B = B(d, D, N) = B(d, D, N(d, D)). 2. Classifiation of dynatomi urves For m, n 1, let Y 1 (m, n) be the urve over k whose general points parametrize polynomials z d + equipped with a preperiodi point that after exatly m steps enters an n-yle. This urve is the zero lous in A 2 k of the polynomial Φ m,n (z, ) := Φ n(f m (z), ) Φ n (f m 1 (z), ). For a general point (z, ) Y 1 (1, n), the elements z and f n (z) are distint preimages of f(z), so z = ζf n (z) for some ζ µ d {1}. Suppose that µ d k. For eah ζ µ d {1}, let Y 1 (1, n) ζ be the subsheme of Y 1 (1, n) defined by the ondition z = ζf n (z), so Y 1 (1, n) = Y 1 (1, n) ζ. ζ µ d {1} Both (z, ) (f(z), ) and (z, ) (ζ 1 z, ) define isomorphisms Y 1 (1, n) ζ Y 1 (n). In partiular, Y 1 (1, n) ζ equals the urve Φ n (ζ 1 z, ) = 0 in A 2 k. For m 2, let Y 1(m, n) ζ be the inverse image of Y 1 (1, n) ζ under Y 1 (m, n) Y 1 (1, n) (z, ) (f m 1 (z), ). 3

4 Then for any m, n 1, (2) Y 1 (m, n) = ζ µ d {1} Y 1 (m, n) ζ, and Y 1 (m, n) ζ equals the urve Φ n (ζ 1 f m 1 (z), ) = 0 in A 2 k. The deomposition (2) orresponds to a fatorization (3) Φ m,n (z, ) = Φ n (ζ 1 f m 1 (z), ). ζ µ d {1} The following is a olletion of results from [Bou92, LS94, Mor96, Gao16]. Theorem 2.1. Let k be a field of harateristi 0 suh that µ d k. Then the urves Y 1 (n) for n 1 and the urves Y 1 (m, n) ζ for m, n 1 and ζ µ d {1} are irreduible, so they are all the dynatomi urves over k. Computer experiments (at least for d = 2) suggest that Theorem 2.1 holds for any field k suh that har k d and µ d k, but in positive harateristi this remains unproved. See [DKO + 17], espeially Theorems B and D, for some progress in this diretion. Remark 2.2. If in Theorem 2.1 we drop the hypothesis that µ d k, then the irreduible omponents of Y 1 (m, n) over k are in bijetion with the Gal(k(µ d )/k)-orbits in µ d {1}. An irreduible omponent orresponding to an orbit of size greater than 1 is not geometrially irreduible. 3. Gonality in harateristi 0 Given a geometrially irreduible urve X over k, let g(x) denote the genus of its smooth projetive model. ( Let D 0 (n) be the degree of the morphism X 0 (n) P 1. Similarly, let D 1 (n) = deg X 1 (n) P ). 1 Proposition 3.1. Fix d 2, and fix a field k of harateristi 0. (a) We have D 1 (n) = (1 + o(1))d n as n. (b) We have D 0 (n) = (1 + o(1))d n /n as n. () We have g(x 0 (n)) > ( 1 1 o(1)) d n as n. 2 2d P 1 is the full sym- (d) The Galois group of (the Galois losure of) the overing X 0 (n) metri group S D0 (n). Proof. We may assume k = C. (a) First, D 1 (n) = deg z Φ n deg(f n (z) z) = d n. On the other hand, one an show (e.g., as in the proof of [Doy16, Lemma 2.2]) that D 1 (n) > d n d n/2+1 /(d 1). (b) The first morphism in the tower X 1 (n) X 0 (n) P 1 has degree n, so D 0 (n) = D 1 (n)/n. Substitute (a) into this. () More preisely, g(x 0 (n)) > ( d n) d n + O(nd n/2 ) as n, by [Mor96, Theorem 13(d)]. (d) This is a onsequene of work of Boush [Bou92] for d = 2, and Lau and Shleiher [LS94] for d > 2. See also [Mor98, Theorem B] and [Sh17]. 4

5 Proposition 3.2 (Castelnuovo Severi inequality). Let F, F 1, F 2 be funtion fields of urves over k, of genera g, g 1, g 2, respetively. Suppose that F i F for i = 1, 2 and the ompositum of F 1 and F 2 in F equals F. Let d i = [F : F i ] for i = 1, 2. Then Proof. See [Sti93, III.10.3]. g d 1 g 1 + d 2 g 2 + (d 1 1)(d 2 1). h Proof of Theorem 1.4. Let X 0 (n) P 1 be a dominant rational map of minimal degree. Case I: h fators through X 0 (n) P 1. Then deg h D 0 (n) = (1 + o(1)) dn n by Proposition 3.1(b), so deg h is muh larger than n when n is large. Case II: h does not fator through X 0 (n) P 1. Then the ompositum of k() and k(h) in the funtion field k(x 0 (n)) is stritly larger than k(). Beause of the Galois group (Proposition 3.1(d)), the only nontrivial extension of k() in k(x 0 (n)) is the whole field k(x 0 (n)). Thus k() and k(h) generate k(x 0 (n)). By Proposition 3.2, Thus g(x 0 (n)) (D 0 (n) 1)(deg h 1). deg h 1 + g(x 0(n)) D 0 (n) 1 = as n, by Proposition 3.1(b,). ( ) 2d o(1) n Lemma 3.3. Let k be a field of harateristi 0 suh that µ d k. Let m and n be positive integers, and let ζ µ d {1}. Then the polynomial Φ n (ζ 1 f m 1 (0), ) k[] has only simple roots, and their number is d m 2 D 1 (n) if m 2. Proof. First suppose that n does not divide m 1. In this ase, the roots of Φ m,n (0, ) are distint by [HT15, Theorem 1.1], and therefore the roots of Φ n (ζ 1 f m 1 (0), ) are distint by (3). Now suppose that n divides m 1. By [Eps12, Proposition A.1], the roots of Φ n (0, ) are simple. If is suh a root, then the polynomial f = f satisfies f n (0) = 0, so f m 1 (0) = 0 and Φ n (ζ 1 f m 1 (0), ) = 0. Thus Φ n (0, ) divides Φ n (ζ 1 f m 1 (0), ). The fatorization (3) yields (4) Φ m,n (0, ) Φ n (0, ) d 1 = ζ µ d {1} Φ n (ζ 1 f m 1 (0), ). Φ n (0, ) By [HT15, Theorem 1.1], Φ m,n (0, )/Φ n (0, ) d 1 has only simple roots, none of whih are also roots of Φ n (0, ). Combining this with (4) shows that Φ n (ζ 1 f m 1 (0), ) has only simple roots. It remains to prove deg Φ n (ζ 1 f m 1 (0), ) = d m 2 D 1 (n). In fat, this is [Gao16, Lemma 4.8]. In our notation, the argument is as follows. By indution on m, the degree of the polynomial f m 1 (0) k[] is d m 2 if m 2. Hene, by indution on e, we have deg f e (ζ 1 f m 1 (0)) = d e d m 2 for eah e 0. Thus the -degree of f e (ζ 1 f m 1 (0)) ζ 1 f m 1 (0) is d m 2 times the z-degree of f e (z) z for eah e 1. Substituting ζ 1 f m 1 (0) for z in (1) shows that deg Φ n (ζ 1 f m 1 (0), ) = d m 2 deg z Φ n (z, ) = d m 2 D 1 (n). 5

6 Proof of Theorem 1.1 in harateristi 0. (a) By Theorem 2.1, the dynatomi urves over k are the urves Y 1 (n) and Y 1 (m, n) ζ, and they are geometrially irreduible. (b) The urves Y 1 (n) and Y 1 (m, n) ζ dominate X 0 (n), so their gonalities are at least the gonality of X 0 (n), by [Poo07, Proposition A.1(vii)]. In light of Theorem 1.4, it remains to prove that in eah tower Y 1 (m, n) ζ Y 1 (m 1, n) ζ Y 1 (1, n) ζ for fixed n and ζ, the gonality tends to as m. Let g m = g(y 1 (m, n) ζ ) and γ m = γ(y 1 (m, n) ζ ). Let Y 1 (m, n) ζ h P 1 be a dominant rational map of degree γ m. Case I: h fators through a urve Z with k(y 1 (m 1, n) ζ ) k(z) k(y 1 (m, n) ζ ). Then γ m 2γ(Z) 2γ m 1 by [Poo07, Proposition A.1(vii)], so γ m grows by indution on m. Case II: h does not fator through any suh urve Z. Denote by π m the degree d map π m : Y 1 (m, n) ζ Y 1 (m 1, n) ζ (z, ) (f(z), ), and let π m : X 1 (m, n) ζ X 1 (m 1, n) ζ be its extension to the smooth projetive models. Let R m be the ramifiation divisor of π m. Applying Proposition 3.2 to π m and h yields g m dg m 1 + (d 1)(γ m 1), so it suffies to show that g m dg m 1 as m. By Riemann Hurwitz, this is equivalent to showing that deg R m as m. In the fiber produt diagram Y 1 (m, n) ζ π m Y 1 (m 1, n) ζ z A 1 f both vertial morphisms are étale above 0 by Lemma 3.3, while f has ramifiation index d at 0, so π m has ramifiation index d at eah point of Y 1 (m, n) ζ where z = 0. For m 2, the number of suh points is d m 2 D 1 (n) by Lemma 3.3. Thus deg R m (d 1)d m 2 D 1 (n), whih tends to as m. z A 1, 4. Gonality in harateristi p 4.1. Redution to the ase of a finite field. Let F q = F p (µ d ). Lemma 4.1. Theorem 1.1 for F q implies Theorem 1.1 for any harateristi p field k ontaining µ d. Proof. Theorem 1.1(a) for F q implies that the dynatomi urves over k are just the base extensions of the dynatomi urves X over F q, and that they are geometrially irreduible too. We will prove in Setion 4.4 that the smooth projetive model of eah X has an F q - point. Then Theorem 2.5(iii) and Proposition A.1(ii) of [Poo07] imply γ(x k ) γ(x), whih implies Theorem 1.1(b) for k. 6

7 4.2. Symboli dynamis. View f(z) as a polynomial in z over the loal field F q (( 1 )). Normalize the valuation v on F q (( 1 )) so that v( 1 ) = 1, and extend v to an algebrai losure. Let t = 1/d, so F q ((t)) is a degree d totally tamely ramified extension of F q (( 1 )). Lemma 4.2. (a) For any nonnegative integers n > m, the polynomial f n (z) f m (z) over F q () is separable and splits ompletely over F q ((t)). (b) Eah zero of f n (z) f m (z) has valuation 1/d and generates F q ((t)) over F q (( 1 )). Proof. The ideas in the following argument are well known; f. [Mor96, Lemma 1]. (a) For eah dth root of, interpreting ( + z) 1/d as ( ) 1/d (1 1 z) 1/d and expanding (1 1 z) 1/d in a binomial series defines a branh of the inverse of z d + on the open disk D := {z F q ((t)) : v(z) > v()}. Taking the derivative of ( + z) 1/d shows that eah branh is a ontrating map D D. These branhes have disjoint images, eah a smaller open disk around a different dth root of. Let S be the set of these d funtions. Eah finite sequene of elements of S defines a omposition of funtions, and for eah m, the images of the different m-fold ompositions are disjoint open disks. For eah infinite sequene s 1, s 2, of elements of S, the images of s 1 s m for m 1 are nested open disks whose radii tend to 0, so they have a unique point in their intersetion; denote it [s 1 s 2 ]. Any two distint infinite sequenes yield two points in disjoint disks, so these points are distint. Sine f s 1 is the identity, f maps [s 1 s 2 ] to [s 2 s 3 ]. For fixed nonnegative integers n > m, any n-long sequene s 1,..., s n in S extends uniquely to an infinite sequene (s i ) satisfying s i+n = s i+m for all i 1, and then [s 1 s 2 ] is a zero of f n (z) f m (z). There are d n of these, so they are all the zeros. In partiular, these zeros are distint elements of F q ((t)). This implies that f n (z) f m (z) is separable. (b) The image of eah s S onsists of elements of valuation exatly 1/d. Thus eah element [s 1 s 2 ] has valuation 1/d. In partiular, eah zero of f n (z) f m (z) generates an extension field of F q (( 1 )) of ramifiation index divisible by d; this extension field an only be the whole field F q ((t)) Dynatomi urves of low degree. Lemma 4.3. For eah e 1, the set of dynatomi urves X over F q suh that deg(x P 1 ) = e is finite. Proof. Suppose that Q(z) = e r=0 q rz e r is a moni degree e fator of f n (z) f m (z) over F q () for some n and m. For eah r, the oeffiient q r is the rth elementary symmetri polynomial evaluated at the negatives of the zeros of Q; those zeros have valuation 1/d by Lemma 4.2(b), so v(q r ) r/d. On the other hand, by Gauss s lemma, q r F q [], so deg q r r/d. Thus there are only finitely many possibilities for eah q r, and hene finitely many possibilities for Q, eah of whih yields one dynatomi urve Gonality of dynatomi urves. Proof of Theorem 1.1. By Lemma 4.1, we may assume that k = F q. (a) Let X be the smooth projetive model of a dynatomi urve, orresponding to a fator of f n (z) f m (z) for some n and m. By Lemma 4.2(b), f n (z) f m (z) splits ompletely over F q ((t)), and the preimage of under X P 1 onsists of F q -points, eah of ramifiation 7

8 index d. Every irreduible omponent Z of X Fq dominates P 1 and hene must ontain one of those F q -points, say x. Then eah Gal(F q /F q )-onjugate of Z ontains x. On the other hand, sine X Fq is smooth, its irreduible omponents are disjoint. Thus Z equals eah of its onjugates, so Z desends to an irreduible omponent of X, whih must be X itself. (This proves also that X has an F q -point, as promised in the proof of Lemma 4.1.) (b) To bound gonality from below, we use Ogg s method of ounting points over a finite field; f. [Ogg74], [Poo07, Setion 3], and [DKO + 17, Setion 4]. Let X be the smooth projetive model of a dynatomi urve. Let e = deg(x P 1 ). Eah preimage of in X is an F q -point of ramifiation index d, so there are e/d suh points. On the other hand, P 1 has only q +1 points over F q, so any nononstant morphism X P 1 has degree at least e/(d(q + 1)). As X varies, e by Lemma Strong uniform boundedness of preperiodi points Proof of Theorem 1.6. Without loss of generality, K = k(u) for some indeterminate u. Given L, let Y be the smooth projetive integral urve over k with funtion field L. The ondition [L : K] d implies that Y has gonality at most D, so eah irreduible omponent of Y k has gonality at most D. For L not algebrai over k, if z L and n > m satisfy f n (z) f m (z) = 0, then (z, ) is a nononstant and hene smooth L-point of the urve f n (z) f m (z) = 0 in A 2, so it yields an L-point on a dynatomi urve X orresponding to a fator of f n (z) f m (z). This L-point defines a nononstant k-morphism Y X, so γ(x) γ(y ) D. By Theorem 1.1(b), this plaes a uniform bound on n. For eah n, the number of preperiodi points of z d + orresponding to that value of n is uniformly bounded by n 1 m=0 deg(f n (z) f m (z)) = nd n, so bounding n bounds the number of preperiodi points too. If k is finite and lies in the maximal algebrai extension l of k in L, then all the preperiodi points of x d + in L are in l, but [l : k] D, so the number of preperiodi points is uniformly bounded by (#k) D. To prove Theorem 1.7, we need the following result of Frey [Fre94, Proposition 2]. Lemma 5.1. Let C be a urve defined over a number field K. Let D 1. If there are infinitely many points P C(K) of degree D over K, then γ(c) 2D. Proof of Theorem 1.7. If the onlusion fails, then there exists n N suh that there are infinitely many m 1 suh that Y 1 (m, n) has a point of degree D over Q. On the other hand, by Northott s theorem, for any given Q, the set of preperiodi points of x d + is finite. Thus for any m 0, the points on Y 1 (m, n) in the first sentene above for all m m 0 together must inlude infinitely many distint -oordinates. In partiular, their images in Y 1 (m 0, n) inlude infinitely many distint points. Thus some Q(µ d )-irreduible omponent Y 1 (m 0, n) ζ ontains infinitely many points of degree D over Q(µ d ). By Lemma 5.1, γ(y 1 (m 0, n) ζ ) 2D. This argument applies for every m 0, ontraditing Theorem 1.1(b). Aknowledgements We thank Joseph Gunther, Holly Krieger, Andrew Obus, Padmavathi Srinivasan, and Isabel Vogt for omments and disussions. 8

9 Referenes [Bou92] Thierry Boush, Sur quelques problèmes de dynamique holomorphe, PhD thesis, Université de Paris-Sud, Centre d Orsay, [Doy16] John R. Doyle, Preperiodi portraits for uniritial polynomials, Pro. Amer. Math. So. 144 (2016), no. 7, MR [DKO + 17] John R. Doyle, Holly Krieger, Andrew Obus, Rahel Pries, Simon Rubinstein-Salzedo, and Lloyd West, Redution of dynatomi urves, Marh 29, Preprint, arxiv: v2. 2, 3, 4, 8 [Eps12] Adam Epstein, Integrality and rigidity for postritially finite polynomials, Bull. Lond. Math. So. 44 (2012), no. 1, With an appendix by Epstein and Bjorn Poonen. MR [Fre94] Gerhard Frey, Curves with infinitely many points of fixed degree, Israel J. Math. 85 (1994), no. 1-3, MR [Gao16] Yan Gao, Preperiodi dynatomi urves for z z d +, Fund. Math. 233 (2016), no. 1, MR , 5 [HT15] Benjamin Hutz and Adam Towsley, Misiurewiz points for polynomial maps and transversality, New York J. Math. 21 (2015), MR [LS94] Eike Lau and Dierk Shleiher, Internal addresses in the Mandelbrot set and irreduibility of polynomials, SUNY Stony Brook Preprint 19 (1994). 4 [Mer96] Loï Merel, Bornes pour la torsion des ourbes elliptiques sur les orps de nombres, Invent. Math. 124 (1996), no. 1-3, (Frenh). MR (96i:11057) 2 [Mor96] Patrik Morton, On ertain algebrai urves related to polynomial maps, Compositio Math. 103 (1996), no. 3, MR , 7 [Mor98] Patrik Morton, Galois groups of periodi points, J. Algebra 201 (1998), no. 2, , DOI /jabr MR [MS94] Patrik Morton and Joseph H. Silverman, Rational periodi points of rational funtions, Internat. Math. Res. Noties 2 (1994), , DOI /S MR (95b:11066) 2 [NS96] Kha Viet Nguyen and Masa-Hiko Saito, d-gonality of modular urves and bounding torsions (Marh 29, 1996). Preprint, arxiv:alg-geom/ [Ogg74] Andrew P. Ogg, Hyperellipti modular urves, Bull. So. Math. Frane 102 (1974), MR (51 #514) 8 [Poo07] Bjorn Poonen, Gonality of modular urves in harateristi p, Math. Res. Lett. 14 (2007), no. 4, , DOI /MRL.2007.v14.n4.a14. MR , 8 [Sh17] Dierk Shleiher, Internal addresses of the Mandelbrot set and Galois groups of polynomials, Arnold Math. J. 3 (2017), no. 1, MR [Sti93] Henning Stihtenoth, Algebrai funtion fields and odes, Universitext, Springer-Verlag, Berlin, MR (94k:14016) 5 Department of Mathematis & Statistis, Louisiana Teh University, Ruston, LA 71272, USA address: jdoyle@lateh.edu URL: Department of Mathematis, Massahusetts Institute of Tehnology, Cambridge, MA , USA address: poonen@math.mit.edu URL: 9

Ordered fields and the ultrafilter theorem

Ordered fields and the ultrafilter theorem F U N D A M E N T A MATHEMATICAE 59 (999) Ordered fields and the ultrafilter theorem by R. B e r r (Dortmund), F. D e l o n (Paris) and J. S h m i d (Dortmund) Abstrat. We prove that on the basis of ZF

More information

arxiv: v1 [math.ds] 27 Jan 2015

arxiv: v1 [math.ds] 27 Jan 2015 PREPERIODIC PORTRAITS FOR UNICRITICAL POLYNOMIALS JOHN R. DOYLE arxiv:1501.06821v1 [math.ds] 27 Jan 2015 Abstract. Let K be an algebraically closed field of characteristic zero, and for c K and an integer

More information

arxiv:math/ v1 [math.ca] 27 Nov 2003

arxiv:math/ v1 [math.ca] 27 Nov 2003 arxiv:math/011510v1 [math.ca] 27 Nov 200 Counting Integral Lamé Equations by Means of Dessins d Enfants Sander Dahmen November 27, 200 Abstrat We obtain an expliit formula for the number of Lamé equations

More information

SECOND HANKEL DETERMINANT PROBLEM FOR SOME ANALYTIC FUNCTION CLASSES WITH CONNECTED K-FIBONACCI NUMBERS

SECOND HANKEL DETERMINANT PROBLEM FOR SOME ANALYTIC FUNCTION CLASSES WITH CONNECTED K-FIBONACCI NUMBERS Ata Universitatis Apulensis ISSN: 15-539 http://www.uab.ro/auajournal/ No. 5/01 pp. 161-17 doi: 10.1711/j.aua.01.5.11 SECOND HANKEL DETERMINANT PROBLEM FOR SOME ANALYTIC FUNCTION CLASSES WITH CONNECTED

More information

REFINED UPPER BOUNDS FOR THE LINEAR DIOPHANTINE PROBLEM OF FROBENIUS. 1. Introduction

REFINED UPPER BOUNDS FOR THE LINEAR DIOPHANTINE PROBLEM OF FROBENIUS. 1. Introduction Version of 5/2/2003 To appear in Advanes in Applied Mathematis REFINED UPPER BOUNDS FOR THE LINEAR DIOPHANTINE PROBLEM OF FROBENIUS MATTHIAS BECK AND SHELEMYAHU ZACKS Abstrat We study the Frobenius problem:

More information

A Characterization of Wavelet Convergence in Sobolev Spaces

A Characterization of Wavelet Convergence in Sobolev Spaces A Charaterization of Wavelet Convergene in Sobolev Spaes Mark A. Kon 1 oston University Louise Arakelian Raphael Howard University Dediated to Prof. Robert Carroll on the oasion of his 70th birthday. Abstrat

More information

Hankel Optimal Model Order Reduction 1

Hankel Optimal Model Order Reduction 1 Massahusetts Institute of Tehnology Department of Eletrial Engineering and Computer Siene 6.245: MULTIVARIABLE CONTROL SYSTEMS by A. Megretski Hankel Optimal Model Order Redution 1 This leture overs both

More information

arxiv: v2 [cs.dm] 4 May 2018

arxiv: v2 [cs.dm] 4 May 2018 Disrete Morse theory for the ollapsibility of supremum setions Balthazar Bauer INRIA, DIENS, PSL researh, CNRS, Paris, Frane Luas Isenmann LIRMM, Université de Montpellier, CNRS, Montpellier, Frane arxiv:1803.09577v2

More information

Maximum Entropy and Exponential Families

Maximum Entropy and Exponential Families Maximum Entropy and Exponential Families April 9, 209 Abstrat The goal of this note is to derive the exponential form of probability distribution from more basi onsiderations, in partiular Entropy. It

More information

Discrete Bessel functions and partial difference equations

Discrete Bessel functions and partial difference equations Disrete Bessel funtions and partial differene equations Antonín Slavík Charles University, Faulty of Mathematis and Physis, Sokolovská 83, 186 75 Praha 8, Czeh Republi E-mail: slavik@karlin.mff.uni.z Abstrat

More information

Counting Idempotent Relations

Counting Idempotent Relations Counting Idempotent Relations Beriht-Nr. 2008-15 Florian Kammüller ISSN 1436-9915 2 Abstrat This artile introdues and motivates idempotent relations. It summarizes haraterizations of idempotents and their

More information

On Component Order Edge Reliability and the Existence of Uniformly Most Reliable Unicycles

On Component Order Edge Reliability and the Existence of Uniformly Most Reliable Unicycles Daniel Gross, Lakshmi Iswara, L. William Kazmierzak, Kristi Luttrell, John T. Saoman, Charles Suffel On Component Order Edge Reliability and the Existene of Uniformly Most Reliable Uniyles DANIEL GROSS

More information

We will show that: that sends the element in π 1 (P {z 1, z 2, z 3, z 4 }) represented by l j to g j G.

We will show that: that sends the element in π 1 (P {z 1, z 2, z 3, z 4 }) represented by l j to g j G. 1. Introdution Square-tiled translation surfaes are lattie surfaes beause they are branhed overs of the flat torus with a single branhed point. Many non-square-tiled examples of lattie surfaes arise from

More information

EXACT TRAVELLING WAVE SOLUTIONS FOR THE GENERALIZED KURAMOTO-SIVASHINSKY EQUATION

EXACT TRAVELLING WAVE SOLUTIONS FOR THE GENERALIZED KURAMOTO-SIVASHINSKY EQUATION Journal of Mathematial Sienes: Advanes and Appliations Volume 3, 05, Pages -3 EXACT TRAVELLING WAVE SOLUTIONS FOR THE GENERALIZED KURAMOTO-SIVASHINSKY EQUATION JIAN YANG, XIAOJUAN LU and SHENGQIANG TANG

More information

(q) -convergence. Comenius University, Bratislava, Slovakia

(q) -convergence.   Comenius University, Bratislava, Slovakia Annales Mathematiae et Informatiae 38 (2011) pp. 27 36 http://ami.ektf.hu On I (q) -onvergene J. Gogola a, M. Mačaj b, T. Visnyai b a University of Eonomis, Bratislava, Slovakia e-mail: gogola@euba.sk

More information

THE l-primary TORSION CONJECTURE FOR ABELIAN SURFACES WITH REAL MULTIPLICATION

THE l-primary TORSION CONJECTURE FOR ABELIAN SURFACES WITH REAL MULTIPLICATION THE l-primary TORSION CONJECTURE FOR ABELIAN SURFACES WITH REAL MULTIPLICATION ANNA CADORET Abstrat. We prove that the Bombieri-Lang onjeture implies the l-primary torsion onjeture for abelian surfaes

More information

SERIJA III

SERIJA III SERIJA III www.math.hr/glasnik I. Gaál, B. Jadrijević and L. Remete Totally real Thue inequalities over imaginary quadrati fields Aepted manusript This is a preliminary PDF of the author-produed manusript

More information

A Recursive Approach to the Kauffman Bracket

A Recursive Approach to the Kauffman Bracket Applied Mathematis, 204, 5, 2746-2755 Published Online Otober 204 in SiRes http://wwwsirporg/journal/am http://ddoiorg/04236/am20457262 A Reursive Approah to the Kauffman Braet Abdul Rauf Nizami, Mobeen

More information

Packing Plane Spanning Trees into a Point Set

Packing Plane Spanning Trees into a Point Set Paking Plane Spanning Trees into a Point Set Ahmad Biniaz Alfredo Garía Abstrat Let P be a set of n points in the plane in general position. We show that at least n/3 plane spanning trees an be paked into

More information

Solutions Manual. Selected odd-numbered problems in. Chapter 2. for. Proof: Introduction to Higher Mathematics. Seventh Edition

Solutions Manual. Selected odd-numbered problems in. Chapter 2. for. Proof: Introduction to Higher Mathematics. Seventh Edition Solutions Manual Seleted odd-numbered problems in Chapter for Proof: Introdution to Higher Mathematis Seventh Edition Warren W. Esty and Norah C. Esty 5 4 3 1 Setion.1. Sentenes with One Variable Chapter

More information

ON THE LEAST PRIMITIVE ROOT EXPRESSIBLE AS A SUM OF TWO SQUARES

ON THE LEAST PRIMITIVE ROOT EXPRESSIBLE AS A SUM OF TWO SQUARES #A55 INTEGERS 3 (203) ON THE LEAST PRIMITIVE ROOT EPRESSIBLE AS A SUM OF TWO SQUARES Christopher Ambrose Mathematishes Institut, Georg-August Universität Göttingen, Göttingen, Deutshland ambrose@uni-math.gwdg.de

More information

Nonreversibility of Multiple Unicast Networks

Nonreversibility of Multiple Unicast Networks Nonreversibility of Multiple Uniast Networks Randall Dougherty and Kenneth Zeger September 27, 2005 Abstrat We prove that for any finite direted ayli network, there exists a orresponding multiple uniast

More information

After the completion of this section the student should recall

After the completion of this section the student should recall Chapter I MTH FUNDMENTLS I. Sets, Numbers, Coordinates, Funtions ugust 30, 08 3 I. SETS, NUMERS, COORDINTES, FUNCTIONS Objetives: fter the ompletion of this setion the student should reall - the definition

More information

Estimating the probability law of the codelength as a function of the approximation error in image compression

Estimating the probability law of the codelength as a function of the approximation error in image compression Estimating the probability law of the odelength as a funtion of the approximation error in image ompression François Malgouyres Marh 7, 2007 Abstrat After some reolletions on ompression of images using

More information

Where as discussed previously we interpret solutions to this partial differential equation in the weak sense: b

Where as discussed previously we interpret solutions to this partial differential equation in the weak sense: b Consider the pure initial value problem for a homogeneous system of onservation laws with no soure terms in one spae dimension: Where as disussed previously we interpret solutions to this partial differential

More information

RATIONALITY OF SECANT ZETA VALUES

RATIONALITY OF SECANT ZETA VALUES RATIONALITY OF SECANT ZETA VALUES PIERRE CHAROLLOIS AND MATTHEW GREENBERG Abstrat We use the Arakawa-Berndt theory of generalized η-funtions to prove a onjeture of Lalìn, Rodrigue and Rogers onerning the

More information

arxiv:math/ v1 [math.ac] 10 Mar 2005

arxiv:math/ v1 [math.ac] 10 Mar 2005 arxiv:math/0503187v1 [math.ac] 10 Mar 2005 STANLEY REISNER RINGS WITH LARGE MULTIPLICITIES ARE COHEN MACAULAY NAOKI TERAI AND KEN-ICHI YOSHIDA Abstrat. We prove that ertain lass of Stanley Reisner rings

More information

arxiv: v1 [math.nt] 4 Jun 2018

arxiv: v1 [math.nt] 4 Jun 2018 On the orbit of a post-critically finite polynomial of the form x d +c arxiv:1806.01208v1 [math.nt] 4 Jun 2018 Vefa Goksel Department of Mathematics University of Wisconsin Madison, WI 53706, USA E-mail:

More information

Journal of Inequalities in Pure and Applied Mathematics

Journal of Inequalities in Pure and Applied Mathematics Journal of Inequalities in Pure and Applied Mathematis A NEW ARRANGEMENT INEQUALITY MOHAMMAD JAVAHERI University of Oregon Department of Mathematis Fenton Hall, Eugene, OR 97403. EMail: javaheri@uoregon.edu

More information

Modal Horn Logics Have Interpolation

Modal Horn Logics Have Interpolation Modal Horn Logis Have Interpolation Marus Kraht Department of Linguistis, UCLA PO Box 951543 405 Hilgard Avenue Los Angeles, CA 90095-1543 USA kraht@humnet.ula.de Abstrat We shall show that the polymodal

More information

LECTURE NOTES FOR , FALL 2004

LECTURE NOTES FOR , FALL 2004 LECTURE NOTES FOR 18.155, FALL 2004 83 12. Cone support and wavefront set In disussing the singular support of a tempered distibution above, notie that singsupp(u) = only implies that u C (R n ), not as

More information

Control Theory association of mathematics and engineering

Control Theory association of mathematics and engineering Control Theory assoiation of mathematis and engineering Wojieh Mitkowski Krzysztof Oprzedkiewiz Department of Automatis AGH Univ. of Siene & Tehnology, Craow, Poland, Abstrat In this paper a methodology

More information

UNRAMIFIED COVERS OF GALOIS COVERS OF LOW GENUS CURVES

UNRAMIFIED COVERS OF GALOIS COVERS OF LOW GENUS CURVES UNRAMIFIED COVERS OF GALOIS COVERS OF LOW GENUS CURVES BJORN POONEN Abstract. Let X Y be a Galois covering of curves, where the genus of X is 2 and the genus of Y is 2. We prove that under certain hypotheses,

More information

Advanced Computational Fluid Dynamics AA215A Lecture 4

Advanced Computational Fluid Dynamics AA215A Lecture 4 Advaned Computational Fluid Dynamis AA5A Leture 4 Antony Jameson Winter Quarter,, Stanford, CA Abstrat Leture 4 overs analysis of the equations of gas dynamis Contents Analysis of the equations of gas

More information

SURFACE WAVES OF NON-RAYLEIGH TYPE

SURFACE WAVES OF NON-RAYLEIGH TYPE SURFACE WAVES OF NON-RAYLEIGH TYPE by SERGEY V. KUZNETSOV Institute for Problems in Mehanis Prosp. Vernadskogo, 0, Mosow, 75 Russia e-mail: sv@kuznetsov.msk.ru Abstrat. Existene of surfae waves of non-rayleigh

More information

arxiv:math.co/ v1 2 Aug 2006

arxiv:math.co/ v1 2 Aug 2006 A CHARACTERIZATION OF THE TUTTE POLYNOMIAL VIA COMBINATORIAL EMBEDDINGS OLIVIER BERNARDI arxiv:math.co/0608057 v1 2 Aug 2006 Abstrat. We give a new haraterization of the Tutte polynomial of graphs. Our

More information

Computer Science 786S - Statistical Methods in Natural Language Processing and Data Analysis Page 1

Computer Science 786S - Statistical Methods in Natural Language Processing and Data Analysis Page 1 Computer Siene 786S - Statistial Methods in Natural Language Proessing and Data Analysis Page 1 Hypothesis Testing A statistial hypothesis is a statement about the nature of the distribution of a random

More information

Conformal Mapping among Orthogonal, Symmetric, and Skew-Symmetric Matrices

Conformal Mapping among Orthogonal, Symmetric, and Skew-Symmetric Matrices AAS 03-190 Conformal Mapping among Orthogonal, Symmetri, and Skew-Symmetri Matries Daniele Mortari Department of Aerospae Engineering, Texas A&M University, College Station, TX 77843-3141 Abstrat This

More information

Complexity of Regularization RBF Networks

Complexity of Regularization RBF Networks Complexity of Regularization RBF Networks Mark A Kon Department of Mathematis and Statistis Boston University Boston, MA 02215 mkon@buedu Leszek Plaskota Institute of Applied Mathematis University of Warsaw

More information

The Effectiveness of the Linear Hull Effect

The Effectiveness of the Linear Hull Effect The Effetiveness of the Linear Hull Effet S. Murphy Tehnial Report RHUL MA 009 9 6 Otober 009 Department of Mathematis Royal Holloway, University of London Egham, Surrey TW0 0EX, England http://www.rhul.a.uk/mathematis/tehreports

More information

Integration of the Finite Toda Lattice with Complex-Valued Initial Data

Integration of the Finite Toda Lattice with Complex-Valued Initial Data Integration of the Finite Toda Lattie with Complex-Valued Initial Data Aydin Huseynov* and Gusein Sh Guseinov** *Institute of Mathematis and Mehanis, Azerbaijan National Aademy of Sienes, AZ4 Baku, Azerbaijan

More information

M ath. Res. Lett. 16 (2009), no. 1, c International Press 2009 UNIFORM BOUNDS ON PRE-IMAGES UNDER QUADRATIC DYNAMICAL SYSTEMS

M ath. Res. Lett. 16 (2009), no. 1, c International Press 2009 UNIFORM BOUNDS ON PRE-IMAGES UNDER QUADRATIC DYNAMICAL SYSTEMS M ath. Res. Lett. 16 (2009), no. 1, 87 101 c International Press 2009 UNIFORM BOUNDS ON PRE-IMAGES UNDER QUADRATIC DYNAMICAL SYSTEMS Xander Faber, Benjamin Hutz, Patrick Ingram, Rafe Jones, Michelle Manes,

More information

The law of the iterated logarithm for c k f(n k x)

The law of the iterated logarithm for c k f(n k x) The law of the iterated logarithm for k fn k x) Christoph Aistleitner Abstrat By a lassial heuristis, systems of the form osπn k x) k 1 and fn k x)) k 1, where n k ) k 1 is a rapidly growing sequene of

More information

LECTURE 22: MAPPING DEGREE, POINCARE DUALITY

LECTURE 22: MAPPING DEGREE, POINCARE DUALITY LECTURE 22: APPING DEGREE, POINCARE DUALITY 1. The mapping degree and its appliations Let, N be n-dimensional onneted oriented manifolds, and f : N a proper map. (If is ompat, then any smooth map f : N

More information

arxiv: v1 [math.co] 16 May 2016

arxiv: v1 [math.co] 16 May 2016 arxiv:165.4694v1 [math.co] 16 May 216 EHRHART POLYNOMIALS OF 3-DIMENSIONAL SIMPLE INTEGRAL CONVEX POLYTOPES YUSUKE SUYAMA Abstrat. We give an expliit formula on the Ehrhart polynomial of a 3- dimensional

More information

Millennium Relativity Acceleration Composition. The Relativistic Relationship between Acceleration and Uniform Motion

Millennium Relativity Acceleration Composition. The Relativistic Relationship between Acceleration and Uniform Motion Millennium Relativity Aeleration Composition he Relativisti Relationship between Aeleration and niform Motion Copyright 003 Joseph A. Rybzyk Abstrat he relativisti priniples developed throughout the six

More information

The perverse t-structure

The perverse t-structure The perverse t-struture Milan Lopuhaä Marh 15, 2017 1 The perverse t-struture The goal of today is to define the perverse t-struture and perverse sheaves, and to show some properties of both. In his talk

More information

On the Licensing of Innovations under Strategic Delegation

On the Licensing of Innovations under Strategic Delegation On the Liensing of Innovations under Strategi Delegation Judy Hsu Institute of Finanial Management Nanhua University Taiwan and X. Henry Wang Department of Eonomis University of Missouri USA Abstrat This

More information

NOTES ON GROUPOIDS, IMAGINARIES AND INTERNAL COVERS

NOTES ON GROUPOIDS, IMAGINARIES AND INTERNAL COVERS NOTES ON GROUPOIDS, IMAGINARIES AND INTERNAL COVERS OLEG CHTERENTAL April 30, 2009 These notes are an exposition of the beginning of Ehud Hrushovski s paper Groupoids, Imaginaries and Internal Covers.

More information

Bjorn Poonen. April 30, 2006

Bjorn Poonen. April 30, 2006 in in University of California at Berkeley April 30, 2006 of gonality in Let X be a smooth, projective, geometrically integral curve of genus g over a field k. Define the gonality of X as γ k (X ) := min{

More information

Lecture 3 - Lorentz Transformations

Lecture 3 - Lorentz Transformations Leture - Lorentz Transformations A Puzzle... Example A ruler is positioned perpendiular to a wall. A stik of length L flies by at speed v. It travels in front of the ruler, so that it obsures part of the

More information

a n z n, (1.1) As usual, we denote by S the subclass of A consisting of functions which are also univalent in U.

a n z n, (1.1) As usual, we denote by S the subclass of A consisting of functions which are also univalent in U. MATEMATIQKI VESNIK 65, 3 (2013), 373 382 September 2013 originalni nauqni rad researh paper CERTAIN SUFFICIENT CONDITIONS FOR A SUBCLASS OF ANALYTIC FUNCTIONS ASSOCIATED WITH HOHLOV OPERATOR S. Sivasubramanian,

More information

NUMERICALLY SATISFACTORY SOLUTIONS OF HYPERGEOMETRIC RECURSIONS

NUMERICALLY SATISFACTORY SOLUTIONS OF HYPERGEOMETRIC RECURSIONS MATHEMATICS OF COMPUTATION Volume 76, Number 259, July 2007, Pages 1449 1468 S 0025-5718(07)01918-7 Artile eletronially published on January 31, 2007 NUMERICALLY SATISFACTORY SOLUTIONS OF HYPERGEOMETRIC

More information

G-subsets and G-orbits of Q ( n) under action of the Modular Group.

G-subsets and G-orbits of Q ( n) under action of the Modular Group. arxiv:1009.4619v1 [math.gr] 23 Sep 2010 G-subsets and G-orbits of Q ( n) under ation of the Modular Group. M. Aslam Malik and M. Riaz Department of Mathematis, University of the Punjab, Quaid-e-Azam Campus,

More information

ON THE MOVING BOUNDARY HITTING PROBABILITY FOR THE BROWNIAN MOTION. Dobromir P. Kralchev

ON THE MOVING BOUNDARY HITTING PROBABILITY FOR THE BROWNIAN MOTION. Dobromir P. Kralchev Pliska Stud. Math. Bulgar. 8 2007, 83 94 STUDIA MATHEMATICA BULGARICA ON THE MOVING BOUNDARY HITTING PROBABILITY FOR THE BROWNIAN MOTION Dobromir P. Kralhev Consider the probability that the Brownian motion

More information

Anomaly cancellation and modularity, II: The E 8 E 8 case

Anomaly cancellation and modularity, II: The E 8 E 8 case SCIENCE CHINA Mathematis. ARTICLES. June 07 Vol. 60 No. 6: 985 994 doi: 0.007/s45-06-9034- Anomaly anellation and modularity, II: The E 8 E 8 ase In memory of Professor LU QiKeng 97 05 HAN Fei, LIU KeFeng,3

More information

Volume 29, Issue 3. On the definition of nonessentiality. Udo Ebert University of Oldenburg

Volume 29, Issue 3. On the definition of nonessentiality. Udo Ebert University of Oldenburg Volume 9, Issue 3 On the definition of nonessentiality Udo Ebert University of Oldenburg Abstrat Nonessentiality of a good is often used in welfare eonomis, ost-benefit analysis and applied work. Various

More information

RIEMANN S FIRST PROOF OF THE ANALYTIC CONTINUATION OF ζ(s) AND L(s, χ)

RIEMANN S FIRST PROOF OF THE ANALYTIC CONTINUATION OF ζ(s) AND L(s, χ) RIEMANN S FIRST PROOF OF THE ANALYTIC CONTINUATION OF ζ(s AND L(s, χ FELIX RUBIN SEMINAR ON MODULAR FORMS, WINTER TERM 6 Abstrat. In this hapter, we will see a proof of the analyti ontinuation of the Riemann

More information

GALOIS POINTS ON VARIETIES

GALOIS POINTS ON VARIETIES GALOIS POINTS ON VARIETIES MOSHE JARDEN AND BJORN POONEN Abstract. A field K is ample if for every geometrically integral K-variety V with a smooth K-point, V (K) is Zariski dense in V. A field K is Galois-potent

More information

Evaluation of effect of blade internal modes on sensitivity of Advanced LIGO

Evaluation of effect of blade internal modes on sensitivity of Advanced LIGO Evaluation of effet of blade internal modes on sensitivity of Advaned LIGO T0074-00-R Norna A Robertson 5 th Otober 00. Introdution The urrent model used to estimate the isolation ahieved by the quadruple

More information

The First Integral Method for Solving a System of Nonlinear Partial Differential Equations

The First Integral Method for Solving a System of Nonlinear Partial Differential Equations ISSN 179-889 (print), 179-897 (online) International Journal of Nonlinear Siene Vol.5(008) No.,pp.111-119 The First Integral Method for Solving a System of Nonlinear Partial Differential Equations Ahmed

More information

Dept. of Computer Science. Raleigh, NC 27695, USA. May 14, Abstract. 1, u 2 q i+1 :

Dept. of Computer Science. Raleigh, NC 27695, USA. May 14, Abstract. 1, u 2 q i+1 : Anti-Leture Hall Compositions Sylvie Corteel CNRS PRiSM, UVSQ 45 Avenue des Etats-Unis 78035 Versailles, Frane syl@prism.uvsq.fr Carla D. Savage Dept. of Computer Siene N. C. State University, Box 8206

More information

Four-dimensional equation of motion for viscous compressible substance with regard to the acceleration field, pressure field and dissipation field

Four-dimensional equation of motion for viscous compressible substance with regard to the acceleration field, pressure field and dissipation field Four-dimensional equation of motion for visous ompressible substane with regard to the aeleration field, pressure field and dissipation field Sergey G. Fedosin PO box 6488, Sviazeva str. -79, Perm, Russia

More information

arxiv: v1 [math.gt] 22 Nov 2018

arxiv: v1 [math.gt] 22 Nov 2018 SOME REMARKS ON THE CHORD INDEX ZHIYUN CHENG, HONGZHU GAO, AND MENGJIAN XU arxiv:1811.09061v1 [math.gt] 22 Nov 2018 ABSTRACT. In this paper we disuss how to define a hord index via smoothing a real rossing

More information

SPLINE ESTIMATION OF SINGLE-INDEX MODELS

SPLINE ESTIMATION OF SINGLE-INDEX MODELS SPLINE ESIMAION OF SINGLE-INDEX MODELS Li Wang and Lijian Yang University of Georgia and Mihigan State University Supplementary Material his note ontains proofs for the main results he following two propositions

More information

The Hanging Chain. John McCuan. January 19, 2006

The Hanging Chain. John McCuan. January 19, 2006 The Hanging Chain John MCuan January 19, 2006 1 Introdution We onsider a hain of length L attahed to two points (a, u a and (b, u b in the plane. It is assumed that the hain hangs in the plane under a

More information

Effective Resistances for Ladder Like Chains

Effective Resistances for Ladder Like Chains Effetive Resistanes for Ladder Like Chains Carmona, A., Eninas, A.M., Mitjana, M. May 9, 04 Abstrat Here we onsider a lass of generalized linear hains; that is, the ladder like hains as a perturbation

More information

The Unified Geometrical Theory of Fields and Particles

The Unified Geometrical Theory of Fields and Particles Applied Mathematis, 014, 5, 347-351 Published Online February 014 (http://www.sirp.org/journal/am) http://dx.doi.org/10.436/am.014.53036 The Unified Geometrial Theory of Fields and Partiles Amagh Nduka

More information

arxiv:math/ v4 [math.ca] 29 Jul 2006

arxiv:math/ v4 [math.ca] 29 Jul 2006 arxiv:math/0109v4 [math.ca] 9 Jul 006 Contiguous relations of hypergeometri series Raimundas Vidūnas University of Amsterdam Abstrat The 15 Gauss ontiguous relations for F 1 hypergeometri series imply

More information

Average Rate Speed Scaling

Average Rate Speed Scaling Average Rate Speed Saling Nikhil Bansal David P. Bunde Ho-Leung Chan Kirk Pruhs May 2, 2008 Abstrat Speed saling is a power management tehnique that involves dynamially hanging the speed of a proessor.

More information

MAC Calculus II Summer All you need to know on partial fractions and more

MAC Calculus II Summer All you need to know on partial fractions and more MC -75-Calulus II Summer 00 ll you need to know on partial frations and more What are partial frations? following forms:.... where, α are onstants. Partial frations are frations of one of the + α, ( +

More information

Aharonov-Bohm effect. Dan Solomon.

Aharonov-Bohm effect. Dan Solomon. Aharonov-Bohm effet. Dan Solomon. In the figure the magneti field is onfined to a solenoid of radius r 0 and is direted in the z- diretion, out of the paper. The solenoid is surrounded by a barrier that

More information

COALGEBRAS, BRAIDINGS, AND DISTRIBUTIVE LAWS

COALGEBRAS, BRAIDINGS, AND DISTRIBUTIVE LAWS COALGEBRAS, BRAIDINGS, AND DISRIBUIVE LAWS SEFANO KASANGIAN, SEPHEN LACK, AND ENRICO M. VIALE o Aurelio Carboni on his 60th birthday ABSRAC. We show, for a monad, that oalgebra strutures on a -algebra

More information

A Functional Representation of Fuzzy Preferences

A Functional Representation of Fuzzy Preferences Theoretial Eonomis Letters, 017, 7, 13- http://wwwsirporg/journal/tel ISSN Online: 16-086 ISSN Print: 16-078 A Funtional Representation of Fuzzy Preferenes Susheng Wang Department of Eonomis, Hong Kong

More information

Sensitivity Analysis in Markov Networks

Sensitivity Analysis in Markov Networks Sensitivity Analysis in Markov Networks Hei Chan and Adnan Darwihe Computer Siene Department University of California, Los Angeles Los Angeles, CA 90095 {hei,darwihe}@s.ula.edu Abstrat This paper explores

More information

SQUARE ROOTS AND AND DIRECTIONS

SQUARE ROOTS AND AND DIRECTIONS SQUARE ROOS AND AND DIRECIONS We onstrut a lattie-like point set in the Eulidean plane that eluidates the relationship between the loal statistis of the frational parts of n and diretions in a shifted

More information

General Equilibrium. What happens to cause a reaction to come to equilibrium?

General Equilibrium. What happens to cause a reaction to come to equilibrium? General Equilibrium Chemial Equilibrium Most hemial reations that are enountered are reversible. In other words, they go fairly easily in either the forward or reverse diretions. The thing to remember

More information

GONALITY OF MODULAR CURVES IN CHARACTERISTIC p

GONALITY OF MODULAR CURVES IN CHARACTERISTIC p GONALITY OF MODULAR CURVES IN CHARACTERISTIC p BJORN POONEN Abstract. Let k be an algebraically closed field of characteristic p. Let X(p e ; N) be the curve parameterizing elliptic curves with full level

More information

V. Interacting Particles

V. Interacting Particles V. Interating Partiles V.A The Cumulant Expansion The examples studied in the previous setion involve non-interating partiles. It is preisely the lak of interations that renders these problems exatly solvable.

More information

Parametric Solutions of Pell s Equation

Parametric Solutions of Pell s Equation PROCEEDINGS OF THE ROMAN NUMBER THEORY ASSOCIATION Volume 1, Number 1, Marh 2016, pages 43 48 Leonardo Zapponi Parametri Solutions of Pell s Equation written by Pietro Meruri 1 Introdution An ordinary

More information

SINCE Zadeh s compositional rule of fuzzy inference

SINCE Zadeh s compositional rule of fuzzy inference IEEE TRANSACTIONS ON FUZZY SYSTEMS, VOL. 14, NO. 6, DECEMBER 2006 709 Error Estimation of Perturbations Under CRI Guosheng Cheng Yuxi Fu Abstrat The analysis of stability robustness of fuzzy reasoning

More information

Wave Propagation through Random Media

Wave Propagation through Random Media Chapter 3. Wave Propagation through Random Media 3. Charateristis of Wave Behavior Sound propagation through random media is the entral part of this investigation. This hapter presents a frame of referene

More information

ON THE PROBLEM OF RESOLUTION OF SINGULARITIES IN POSITIVE CHARACTERISTIC

ON THE PROBLEM OF RESOLUTION OF SINGULARITIES IN POSITIVE CHARACTERISTIC July 28 2009 ON THE PROBLEM OF RESOLUTION OF SINGULARITIES IN POSITIVE CHARACTERISTIC (Or: A proof that we are still waiting for) HERWIG HAUSER Introdution. The embedded resolution of singular algebrai

More information

Concerning the Numbers 22p + 1, p Prime

Concerning the Numbers 22p + 1, p Prime Conerning the Numbers 22p + 1, p Prime By John Brillhart 1. Introdution. In a reent investigation [7] the problem of fatoring numbers of the form 22p + 1, p a, was enountered. Sine 22p + 1 = (2P - 2*

More information

Relative Maxima and Minima sections 4.3

Relative Maxima and Minima sections 4.3 Relative Maxima and Minima setions 4.3 Definition. By a ritial point of a funtion f we mean a point x 0 in the domain at whih either the derivative is zero or it does not exists. So, geometrially, one

More information

Study of EM waves in Periodic Structures (mathematical details)

Study of EM waves in Periodic Structures (mathematical details) Study of EM waves in Periodi Strutures (mathematial details) Massahusetts Institute of Tehnology 6.635 partial leture notes 1 Introdution: periodi media nomenlature 1. The spae domain is defined by a basis,(a

More information

Relativity fundamentals explained well (I hope) Walter F. Smith, Haverford College

Relativity fundamentals explained well (I hope) Walter F. Smith, Haverford College Relativity fundamentals explained well (I hope) Walter F. Smith, Haverford College 3-14-06 1 Propagation of waves through a medium As you ll reall from last semester, when the speed of sound is measured

More information

15.12 Applications of Suffix Trees

15.12 Applications of Suffix Trees 248 Algorithms in Bioinformatis II, SoSe 07, ZBIT, D. Huson, May 14, 2007 15.12 Appliations of Suffix Trees 1. Searhing for exat patterns 2. Minimal unique substrings 3. Maximum unique mathes 4. Maximum

More information

Eulerian series in q-series and modular forms. Youn Seo Choi

Eulerian series in q-series and modular forms. Youn Seo Choi Eulerian series in q-series and modular forms Youn Seo Choi abstrat Eulerian series is very interesting power series even though we do not know any single method to handle the general Eulerian series However,

More information

Super edge-magic total labeling of a tree

Super edge-magic total labeling of a tree Super edge-magi total labeling of a tree K. Ali, M. Hussain, A. Razzaq Department of Mathematis, COMSATS Institute of Information Tehnology, Lahore, Pakistan. {akashifali, mhmaths, asimrzq}@gmail.om Abstrat.

More information

Methods of evaluating tests

Methods of evaluating tests Methods of evaluating tests Let X,, 1 Xn be i.i.d. Bernoulli( p ). Then 5 j= 1 j ( 5, ) T = X Binomial p. We test 1 H : p vs. 1 1 H : p>. We saw that a LRT is 1 if t k* φ ( x ) =. otherwise (t is the observed

More information

arxiv:physics/ v1 [physics.class-ph] 8 Aug 2003

arxiv:physics/ v1 [physics.class-ph] 8 Aug 2003 arxiv:physis/0308036v1 [physis.lass-ph] 8 Aug 003 On the meaning of Lorentz ovariane Lszl E. Szab Theoretial Physis Researh Group of the Hungarian Aademy of Sienes Department of History and Philosophy

More information

Counting Arbitrary Subgraphs in Data Streams

Counting Arbitrary Subgraphs in Data Streams Counting Arbitrary Subgraphs in Data Streams Daniel M. Kane 1, Kurt Mehlhorn, Thomas Sauerwald, and He Sun 1 Department of Mathematis, Stanford University, USA Max Plank Institute for Informatis, Germany

More information

Wuming Li and Fan Yang

Wuming Li and Fan Yang NEW ZEALAND JOURNAL OF MATHEMATICS Volume 33 (004), 159 164 N DIMENSIONAL MINKOWSKI SPACE AND SPACE TIME ALGEBRA Wuming Li and Fan Yang (Reeived February 003) Abstrat. By using an n Dimensional Minkowski

More information

MOLECULAR ORBITAL THEORY- PART I

MOLECULAR ORBITAL THEORY- PART I 5.6 Physial Chemistry Leture #24-25 MOLECULAR ORBITAL THEORY- PART I At this point, we have nearly ompleted our rash-ourse introdution to quantum mehanis and we re finally ready to deal with moleules.

More information

Research Article Approximation of Analytic Functions by Solutions of Cauchy-Euler Equation

Research Article Approximation of Analytic Functions by Solutions of Cauchy-Euler Equation Funtion Spaes Volume 2016, Artile ID 7874061, 5 pages http://d.doi.org/10.1155/2016/7874061 Researh Artile Approimation of Analyti Funtions by Solutions of Cauhy-Euler Equation Soon-Mo Jung Mathematis

More information

Berry s phase for coherent states of Landau levels

Berry s phase for coherent states of Landau levels Berry s phase for oherent states of Landau levels Wen-Long Yang 1 and Jing-Ling Chen 1, 1 Theoretial Physis Division, Chern Institute of Mathematis, Nankai University, Tianjin 300071, P.R.China Adiabati

More information

EDGE-DISJOINT CLIQUES IN GRAPHS WITH HIGH MINIMUM DEGREE

EDGE-DISJOINT CLIQUES IN GRAPHS WITH HIGH MINIMUM DEGREE EDGE-DISJOINT CLIQUES IN GRAPHS WITH HIGH MINIMUM DEGREE RAPHAEL YUSTER Abstrat For a graph G and a fixed integer k 3, let ν k G) denote the maximum number of pairwise edge-disjoint opies of K k in G For

More information

Most results in this section are stated without proof.

Most results in this section are stated without proof. Leture 8 Level 4 v2 he Expliit formula. Most results in this setion are stated without proof. Reall that we have shown that ζ (s has only one pole, a simple one at s =. It has trivial zeros at the negative

More information

A variant of Coppersmith s Algorithm with Improved Complexity and Efficient Exhaustive Search

A variant of Coppersmith s Algorithm with Improved Complexity and Efficient Exhaustive Search A variant of Coppersmith s Algorithm with Improved Complexity and Effiient Exhaustive Searh Jean-Sébastien Coron 1, Jean-Charles Faugère 2, Guénaël Renault 2, and Rina Zeitoun 2,3 1 University of Luxembourg

More information