SIMULTANEOUS NONVANISHING OF DIRICHLET L-FUNCTIONS AND TWISTS OF HECKE-MAASS L-FUNCTIONS. 1. Introduction

Size: px
Start display at page:

Download "SIMULTANEOUS NONVANISHING OF DIRICHLET L-FUNCTIONS AND TWISTS OF HECKE-MAASS L-FUNCTIONS. 1. Introduction"

Transcription

1 SIULTANEOUS NONVANISHING OF DIRICHLET L-FUNCTIONS AND TWISTS OF HECKE-AASS L-FUNCTIONS SOUYA DAS AND RIZWANUR KHAN Abstract. W prov that givn a Hck-aass form f for SL, Z and a sufficintly larg prim, thr xists a primitiv Dirichlt charactr χ of conductor such that th L-valus L, f χ and L, χ do not vanish. W xpct th sam mthod to work for any larg intgr.. Introduction Undrstanding whn an L-function s cntral valu is non-zro is a problm of grat significanc and long history in analytic numbr thory. Undrstanding whn two or mor L-functions ar simultanously non-zro is also a popular topic and can hav important applications. For xampl, th problms considrd in [9] and [] hav a baring on th Landau-Sigl zro problm and th Birch-Swinnrton-Dyr conjctur rspctivly. Rcntly thr has bn som intrst in th simultanous non-vanishing of L-functions in th family of primitiv Dirichlt charactrs. Blomr and ilićvić [] provd that givn two fixd Hck-aass forms f and f which satisfy th Ramanujan-Ptrsson conjctur, and a sufficintly larg intgr r subjct to a tchnical condition that dos not prmit intgrs such as prims and th product of two prims of almost ual siz, thr xists a primitiv Dirichlt charactr χ of modulus r such that L/, f χ and L/, f χ ar not zro. This improvd th work of Hoffstin and L [6], who studid th sam kind of non-vanishing problm, but wr not abl to spcify th modulus of th charactr. W study a simplr problm: that of th simultanous non-vanishing L/, f χ and L/, χ for a fixd Hck-aass form f for SL, Z. Our papr is motivatd by a rcnt rsult of Liu [], who showd that for R larg nough, thr xists a Dirichlt charactr modulo r with R < r < R such that L/, f χ and L/, χ ar non-vanishing. Actually Liu considrs mor gnral automorphic forms, but th point is that th modulus of th dsird Dirichlt charactr is not spcifid by his work. Liu s rsult follows by showing that. r D χ mod r χ = L/, f χl/, χ = r D r + OR 5 8 +ɛ for som subst D of th intgrs btwn R and R of siz D R/log R, whr indicats that th sum is rstrictd to th primitiv charactrs. Liu nots that sinc th right hand sid is non-zro, at last on of th summands on th lft hand sid must b non-zro. Th main difficulty in Liu s analysis sms to b in daling with Gauss sums, which aris from approximat functional uations. W will prov th following rsult. 000 athmatics Subjct Classification. Primary F; Scondary F. Ky words and phrass. L-functions, Cntral valus, Simultanous nonvanishing.

2 SOUYA DAS AND RIZWANUR KHAN Thorm.. Lt f b a Hck-aass form for SL, Z. For prim valus of, w hav that. χ mod χ = L, f χl, χ = L, f + O 7 8 +θ+ɛ, whr ɛ > 0 is arbitrarily small. Th implid constant dpnds on f and ɛ. In th xponnt, θ rprsnts th bst bound towards th Ramanujan-Ptrsson conjctur for f, which can currntly b takn to b θ = 7/6. By considring such a man valu with a complx conjugat, w avoid som of th difficultis with Gauss sums and do not nd to avrag ovr th modulus as in Liu s work. Sinc L, f is non-zro s [8, Lmma 5.9], w gt Corollary.. Fix f a Hck-aass form for SL, Z. For vry larg nough prim, thr xists a primitiv Dirichlt charactr χ of conductor such that th cntral L-valus L, f χ and L, χ do not vanish. Thus in our work, th modulus of th dsird Dirichlt charactr is known. W hav workd with prim moduli to minimiz tchnical dtails. Howvr givn th powr saving rror trm in., w xpct th sam mthod would yild th non-vanishing rsult for any larg intgr. Blomr, Fouvry, Kowalski, ichl, and ilićvić [] hav provn, conditionally on th Ramanujan- Ptrsson conjctur for f, th imprssiv asymptotic.3 χ mod L, f χl, χ = L, f ζ + O δ, for prim and som δ > 0. Although th man valu w considr is mor modst, it is not clar whthr. can b xpctd from.3. Firstly, our asymptotic is unconditional and scondly, on a mor tchnical lvl, th approximat functional uations ndd for.3 ar st up without Gauss sums [, sction 3] whil for., Gauss sums cannot b avoidd. Finally w rmark that th problm w ar considring is analytic in natur. For comparision, w mntion that Chinta [3] has shown that for a fixd lliptic curv E ovr Q and a larg prim, th cntral valu L/, E χ is non-zro for all but O 7/8+ɛ Dirichlt charactrs χ modulo. Givn this powrful rsult, th simultanous non-vanishing problms discussd abov ar almost trivial whn posd for wight two holomorphic Hck-cusp forms. For Hck-aass forms howvr, th algbraic mthods usd in [3] ar not applicabl... Acknowldgmnts. W ar gratful to Shng-Chi Liu for providing us with his prprint []. W thank th Dpartmnt of athmatics, Indian Institut of scinc, Bangalor and Txas A& Univrsity at Qatar, whr this work was don, for thir hospitalitis. Th first author acknowldgs th financial support by UGC-DST India during this work.. Prliminaris W giv th proof of Thorm. for vn Hck-aass forms, th dtails for odd forms bing ntirly similar. Thus throughout, will dnot a prim and f an vn Hck-aass cusp form for th full modular group with Laplacian ignvalu + T f, whr T f is ral. Lt λ f n dnot th ignvalu of th n-th Hck oprator corrsponding to f. For mor dtails on aass forms, w rfr th radr to [7]. At th tim this papr was submittd for publication, [, Thorm.] was conditional on th Ramanujan-Ptrsson conjctur, but now it is unconditional.

3 SIULTANEOUS NONVANISHING OF L-FUNCTIONS 3 For an vn Dirichlt charactr χ modulo, w dfin th L-functions. Ls, χ = χnn s, Ls, f χ = λ f nχnn s n= for Rs >, with analytic continuation to ntir functions having th functional uations. whr.3 Λs, χ := π Λs, χ = τχ Λ s, χ, s/ s Ls, χ, Λs, f χ := π n= Λs, f χ = τχ Λ s, f χ, s s + itf s itf Ls, f χ. W will us th convntion that ɛ dnots an arbitrarily small positiv constant, but not ncssarily th sam constant from on occurrnc to th nxt. All implid constants may dpnd implicitly on ɛ and f... Orthogonality of charactrs. W will nd th following basic idntity. This and mor on Dirichlt charactrs can b found in []. Lmma.. For prim and nm, =, w hav. χnχm = χ mod if n m mod othrwis... Approximat functional uations. W will nd th following xprssions for th cntral valus of Ls, χ and Ls, f χ. Ths can b drivd in a standard way from [8, Thorm 5.3] and th functional uations of ths L-functions. Lmma.. For χ an vn primitiv charactr of modulus, w hav L, χ = L, χ = χm m V + τχ χm m.5 V, m m whr for x, c > 0,.6 V x = πi c πx s s+ W hav that th l-th drivativ V l x l,c min{, x C l } for any C > 0, and V x for x < ɛ. Thus th sums in.5 ar ssntially supportd on m < /+ɛ. Lmma.3. For χ an vn primitiv charactr of modulus, w hav L, f χ = λ f nχn n V + τχ.7 n whr for x, c > 0,.8 V x = πx s πi c s++itf +itf ds s λ f nχn n V n s+ itf itf W hav that th l-th drivativ V l x l,c min{, x C l } for any C > 0, and V x for x < ɛ. Thus th sums in.7 ar ssntially supportd on n < +ɛ. ds s.,

4 SOUYA DAS AND RIZWANUR KHAN.3. Sums of Fourir cofficints. Th Ramanujan conjctur for th Fourir cofficints of f is tru on avrag, by Rankin-Slbrg thory. Namly, w hav.9 Individually, w hav Kim and Sarnak s [0] bound / λ f n x / λ f n x. n<x n<x.0 λ f n n θ+ɛ, whr θ = 7/6. W will also ncountr sums of Fourir cofficints twistd by additiv charactrs. In this contxt, lt us rcall th Voronoi summation formula, Lmma.. [5, Thorm.] Lt ψ b a fixd smooth function with compact support on th positiv rals. Lt d, d Z with, d = and dd mod. Thn nd n λ f n ψ = λ f n nd nn N n Ψ + + λ f n nd nn. n Ψ, whr for σ >,. ψs is th llin transform of ψx and +s+itf.3 πg ± s = Ψ ± x = π x s G ± s πi ψ sds, σ s+itf +s itf s itf ± +s+itf + s+itf + +s itf + s itf + Th following rsult says that Fourir cofficints ar orthogonal to additiv charactrs on avrag. Lmma.5. [7, Thorm 8.] For any ral numbr α, w hav that. λ f nαn N /+ɛ. n N Th implid constant dos not dpnd on α.. 3. Proof of Thorm. Using th approximat functional uations and by picking out vn charactrs using th factor χ + which uals whn χ = and 0 othrwis, w hav that th lft hand sid of. uals 3. χ mod which w writ as 3. χ + λ f nχn n V + ik τχ n χ mod χ + S + S S 3 + S. λ f nχn n V n χm m V + τχ χm m V. m m ultiplying out th summand abov lads to svral cross trms, which w now analyz on by on.

5 SIULTANEOUS NONVANISHING OF L-FUNCTIONS Cross trms with no Gauss sum. In this sction w considr 3.3 χ mod Lmma χ + S S 3 = χ mod n, χ mod n, λ f nχnχm m n V V nm + χ mod n, λ f nχ nχm m n V V 3/+θ+ɛ. nm Proof. By Lmma. and.0, it suffics to bound by 3/+θ+ɛ th sum λ f n 3.5 +θ+ɛ nm n< +ɛ,m< /+ɛ n+m 0 mod n< +ɛ,m< /+ɛ n+m 0 mod λ f nχ nχm m n V V. nm nm. Writing n = k m, w s from th rangs of n and m that w must hav k < ɛ. Thus 3.5 is boundd by 3.6 7/6+ɛ 3/+θ+ɛ. m m< /+ɛ Th nxt rsult givs th main trm of Thorm.. Lmma χ mod n, λ f nχnχm m n V V = nm L, f + O3/+θ+ɛ Proof. By Lmma. and.9, th lft hand sid of 3.7 uals λ f n m n 3.8 V V nm n, n m mod nm,= + O 3/+ɛ. By a similar argumnt as that usd to prov Lmma 3., w s that up to an rror of O 3/+θ+ɛ, th main trm in 3.8 consists of thos trms with n = m: λ f n n n n V V = λ f n n n 3.9 n V V + O 00. n,= Th uality abov holds bcaus V n is vry small unlss n < /+ɛ, in which cas n, = is automatic. Using th dfinitions of V and V, w gt λ f n n n 3.0 n V V = λ f n s+ s++it πi π s/ s +s+s n f s+ it f ds ds. s s +itf itf Th n-sum insid th intgral uals L + s + s, f. Shifting th lins of intgration to Rs = Rs = / + ɛ, w pick up th rsidu L, f at s = s = 0. Th intgral on th nw lins can b boundd in a standard way by /+ɛ. This complts th proof.

6 6 SOUYA DAS AND RIZWANUR KHAN 3.. Cross trms with on Gauss sum. In this sction w considr 3. Lmma χ mod χ mod χ mod χ + S S χ + τχ χ + and χ mod χ + S S. λ f nχn n V τχ n λ f nχn n V τχ χm m V 3/+ɛ. n m χm m V m 3/+ɛ, Proof. Th proofs of 3. and 3.3 ar similar, so w show only th formr. For vn primitiv charactrs w hav that τχτχ =. Thus to prov 3. w nd to bound by 3/+ɛ th sum λ f n m n 3. V / V τχχ±nχm. nm n, nm,= χ mod Writing τχ = a mod χaa/, th innrmost sum of 3. uals τχχ±nχm = a 3.5 χ±nχma. χ mod Now using Lmma., w hav that 3. uals m 3.6 V / m 3.7 / m,= m,= m V m a mod n,= n,= λ f n n χ mod ±nm n V λ f n n V n a mod a. Th innrmost a-sum of 3.7 is a Ramanujan sum which uals, so that 3.7 is trivially boundd by /+ɛ. As for 3.6, rmoving th condition n, = and using.0, w hav that it uals ±nm n 3.8 V / + O /+θ+ɛ. m,= m λ f n V m n Now by Lmma.5 and partial summation, w gt that th n-sum in 3.8 is boundd by ɛ, th m-sum by /. Hnc 3.8 is boundd by 3/+ɛ Cross trms with two Gauss sums. In this sction w considr 3.9 Lmma χ mod χ + τχ χ mod χ + S S 3. λ f nχn n V χm m V 7/8+θ+ɛ nm m Proof. By taking a smooth partition of unity, w may considr th n and m sums in dyadic intrvals. Thus it suffics to bound by 7/8+θ+ɛ th sum τχ m m n n 3. λ N / f nχ±nmv W V W, N χ mod n,

7 SIULTANEOUS NONVANISHING OF L-FUNCTIONS 7 for any fixd smooth functions W i x supportd on x [, ], N < +ɛ and < /+ɛ. Writing τχ = a mod χaa/, w hav that 3. uals 3. N / n, nm,= m m n n λ f nv W V W N a,b mod a + b χ mod χ±nmχab. Th innrmost sum can b valuatd using Lmma.. Thus 3. uals N / N / n, nm,= n, nm,= m m n n λ f nv W V W N a mod m m n n λ f nv W V W N a,b mod a ± nma a + b Th innrmost a, b-sum of 3. is a product of two Ramanujan sums and uals. Thus 3. is boundd absolutly by /+ɛ. As for 3.3, w procd according to th sizs of N and. Cas I: N < /, < /. W not that th innrmost a-sum of 3.3 is a Kloostrman sum, which is lss than / by Wil s bound. Using this and.9, w gt that 3.3 is boundd by 3.5 ɛ N / 7/8+ɛ. Cas II: /. W first not that th m-sum in 3.3 uals 3.6 m,= ±nma m m V W = ±nma m m V W + O 00, bcaus V m is vry small unlss m < /+ɛ, in which cas m, = is automatic. By Poisson summation, w hav that 3.7 m m V W ±nma = ±nba b = = b ±nba m= b mod m= b + m b + m V W b±na m b + x b + x V W mxdx y V W y my dy. Rpatd intgration by parts shows that th intgral abov is boundd by +ɛ / m B for any B 0. Thus w may rstrict th m-sum in th last lin to m < +ɛ /, up to an rror of 00 say. Th b-sum

8 8 SOUYA DAS AND RIZWANUR KHAN uals if ±na m mod, and 0 othrwis. Thus 3.3 is boundd by / ±nm n n 3.8 N / λ f n V W N 0< m < +ɛ / m,= n,= = / ±nm 3.9 N / λ f n 0< m < +ɛ / m,= + O 00 n n V W N + O/+θ+ɛ. Abov, 3.9 was obtaind from 3.8 by bounding absolutly th contributing of th intgrs n divisibl by, of which thr ar at most ɛ. By Lmma.5 and partial summation, w find that th n-sum in 3.9 is boundd by N /+ɛ and so 3.9 is boundd by ɛ / 7/8+ɛ. Cas III: N /, < /. By rmoving th condition n, =, w not that 3.3 uals m m a n n ±nma 3.3 V N / W λ f nv W N a mod m,= Applying Voronoi summation to th innrmost n-sum, w gt that 3.3 uals m m a 3.3 V N / W λ f n nma n a mod m,= plus a similar sum involving Ψ +, whr Ψ ± x = 3.33 π x s G ± s πi 0 0 V tn/w tt s dt ds. + O /+θ+ɛ. nn Ψ Th a-sum in 3.3 uals if n m mod and othrwis, so that 3.3 uals m m λ f n nn 3.3 V N / W n Ψ 3.35 N / m,= m,= V m W m n m mod W now xplain how to truncat th n-sum. W first not that 3.36 G ± s 0 λ f n n Ψ V tn/w tt s dt + s Rs+ nn + O /+θ+ɛ. ɛ + s B, + O /+θ+ɛ by Stirling s approximation for th gamma function and by intgrating by parts svral tims th t-intgral, for any B 0, whr th implid constant dpnds on Rs, B and of cours f. Using this stimat, by shifting th lin of intgration in 3.33 right to Rs = C, w hav that Ψ ± x ɛ x C for any C > 0. Thus w may rstrict 3.3 and 3.35 to n < +ɛ /N, up to an rror of O 00 say. Also, w may shift th lin of intgration in 3.33 lft to Rs = + ɛ to gt that that Ψ ± x ɛ x.

9 SIULTANEOUS NONVANISHING OF L-FUNCTIONS Now rstricting to n < +ɛ /N and bounding absolutly w find that that 3.3 is boundd by +ɛ N / m< n< +ɛ /N n m mod λ f n nn n +θ+ɛ / 7/8+θ+ɛ. N / Th sam bound holds for Sinc th sum involving Ψ + can b tratd in xactly th sam way, this complts th proof. Rfrncs. V. Blomr, É Fouvry, E. Kowalski, P. ichl, and D. ilićvić, On momnts of twistd L-functions, prprint.. Valntin Blomr and Djordj ilićvić, Th scond momnt of twistd modular L-functions, prprint. 3. Gautam Chinta, Analytic ranks of lliptic curvs ovr cyclotomic filds, J. Rin Angw. ath. 5 00, 3.. Harold Davnport, ultiplicativ numbr thory, third d., Graduat Txts in athmatics, vol. 7, Springr-Vrlag, Nw York, 000, Rvisd and with a prfac by Hugh L. ontgomry. 5. Danil Godbr, Additiv twists of Fourir cofficints of modular forms, J. Numbr Thory 33 03, no., Jff Hoffstin and in L, Scond momnts and simultanous non-vanishing of GL automorphic L-sris, prprint. 7. Hnryk Iwanic, Spctral mthods of automorphic forms, scond d., Graduat Studis in athmatics, vol. 53, Amrican athmatical Socity, Providnc, RI; Rvista atmática Ibroamricana, adrid, Hnryk Iwanic and Emmanul Kowalski, Analytic numbr thory, Amrican athmatical Socity Collouium Publications, vol. 53, Amrican athmatical Socity, Providnc, RI, Hnryk Iwanic and Ptr Sarnak, Th non-vanishing of cntral valus of automorphic L-functions and Landau-Sigl zros, Isral J. ath , no. part A, Hnry H. Kim, Functoriality for th xtrior suar of GL and th symmtric fourth of GL, J. Amr. ath. Soc , no., 39 83, With appndix by Dinakar Ramakrishnan and appndix by Kim and Ptr Sarnak.. Shng-Chi Liu, Simultanous nonvanishing of automorphic L-functions, prprint.. P. ichl and J. Vandrkam, Simultanous nonvanishing of twists of automorphic L-functions, Compositio ath. 3 00, no., Dpartmnt of athmatics, Indian Institut of Scinc, Bangalor, India. addrss: somu@math.iisc.rnt.in Scinc Program, Txas A& Univrsity at Qatar, Doha, Qatar addrss: rizwanur.khan@atar.tamu.du

Hardy-Littlewood Conjecture and Exceptional real Zero. JinHua Fei. ChangLing Company of Electronic Technology Baoji Shannxi P.R.

Hardy-Littlewood Conjecture and Exceptional real Zero. JinHua Fei. ChangLing Company of Electronic Technology Baoji Shannxi P.R. Hardy-Littlwood Conjctur and Excptional ral Zro JinHua Fi ChangLing Company of Elctronic Tchnology Baoji Shannxi P.R.China E-mail: fijinhuayoujian@msn.com Abstract. In this papr, w assum that Hardy-Littlwood

More information

BINOMIAL COEFFICIENTS INVOLVING INFINITE POWERS OF PRIMES. 1. Statement of results

BINOMIAL COEFFICIENTS INVOLVING INFINITE POWERS OF PRIMES. 1. Statement of results BINOMIAL COEFFICIENTS INVOLVING INFINITE POWERS OF PRIMES DONALD M. DAVIS Abstract. If p is a prim and n a positiv intgr, lt ν p (n dnot th xponnt of p in n, and u p (n n/p νp(n th unit part of n. If α

More information

Limiting value of higher Mahler measure

Limiting value of higher Mahler measure Limiting valu of highr Mahlr masur Arunabha Biswas a, Chris Monico a, a Dpartmnt of Mathmatics & Statistics, Txas Tch Univrsity, Lubbock, TX 7949, USA Abstract W considr th k-highr Mahlr masur m k P )

More information

An Application of Hardy-Littlewood Conjecture. JinHua Fei. ChangLing Company of Electronic Technology Baoji Shannxi P.R.China

An Application of Hardy-Littlewood Conjecture. JinHua Fei. ChangLing Company of Electronic Technology Baoji Shannxi P.R.China An Application of Hardy-Littlwood Conjctur JinHua Fi ChangLing Company of Elctronic Tchnology Baoji Shannxi P.R.China E-mail: fijinhuayoujian@msn.com Abstract. In this papr, w assum that wakr Hardy-Littlwood

More information

Cramér-Rao Inequality: Let f(x; θ) be a probability density function with continuous parameter

Cramér-Rao Inequality: Let f(x; θ) be a probability density function with continuous parameter WHEN THE CRAMÉR-RAO INEQUALITY PROVIDES NO INFORMATION STEVEN J. MILLER Abstract. W invstigat a on-paramtr family of probability dnsitis (rlatd to th Parto distribution, which dscribs many natural phnomna)

More information

cycle that does not cross any edges (including its own), then it has at least

cycle that does not cross any edges (including its own), then it has at least W prov th following thorm: Thorm If a K n is drawn in th plan in such a way that it has a hamiltonian cycl that dos not cross any dgs (including its own, thn it has at last n ( 4 48 π + O(n crossings Th

More information

LINEAR DELAY DIFFERENTIAL EQUATION WITH A POSITIVE AND A NEGATIVE TERM

LINEAR DELAY DIFFERENTIAL EQUATION WITH A POSITIVE AND A NEGATIVE TERM Elctronic Journal of Diffrntial Equations, Vol. 2003(2003), No. 92, pp. 1 6. ISSN: 1072-6691. URL: http://jd.math.swt.du or http://jd.math.unt.du ftp jd.math.swt.du (login: ftp) LINEAR DELAY DIFFERENTIAL

More information

DISTRIBUTION OF DIFFERENCE BETWEEN INVERSES OF CONSECUTIVE INTEGERS MODULO P

DISTRIBUTION OF DIFFERENCE BETWEEN INVERSES OF CONSECUTIVE INTEGERS MODULO P DISTRIBUTION OF DIFFERENCE BETWEEN INVERSES OF CONSECUTIVE INTEGERS MODULO P Tsz Ho Chan Dartmnt of Mathmatics, Cas Wstrn Rsrv Univrsity, Clvland, OH 4406, USA txc50@cwru.du Rcivd: /9/03, Rvisd: /9/04,

More information

Equidistribution and Weyl s criterion

Equidistribution and Weyl s criterion Euidistribution and Wyl s critrion by Brad Hannigan-Daly W introduc th ida of a sunc of numbrs bing uidistributd (mod ), and w stat and prov a thorm of Hrmann Wyl which charactrizs such suncs. W also discuss

More information

Derangements and Applications

Derangements and Applications 2 3 47 6 23 Journal of Intgr Squncs, Vol. 6 (2003), Articl 03..2 Drangmnts and Applications Mhdi Hassani Dpartmnt of Mathmatics Institut for Advancd Studis in Basic Scincs Zanjan, Iran mhassani@iasbs.ac.ir

More information

Chapter 10. The singular integral Introducing S(n) and J(n)

Chapter 10. The singular integral Introducing S(n) and J(n) Chaptr Th singular intgral Our aim in this chaptr is to rplac th functions S (n) and J (n) by mor convnint xprssions; ths will b calld th singular sris S(n) and th singular intgral J(n). This will b don

More information

BINOMIAL COEFFICIENTS INVOLVING INFINITE POWERS OF PRIMES

BINOMIAL COEFFICIENTS INVOLVING INFINITE POWERS OF PRIMES BINOMIAL COEFFICIENTS INVOLVING INFINITE POWERS OF PRIMES DONALD M. DAVIS Abstract. If p is a prim (implicit in notation and n a positiv intgr, lt ν(n dnot th xponnt of p in n, and U(n n/p ν(n, th unit

More information

Construction of asymmetric orthogonal arrays of strength three via a replacement method

Construction of asymmetric orthogonal arrays of strength three via a replacement method isid/ms/26/2 Fbruary, 26 http://www.isid.ac.in/ statmath/indx.php?modul=prprint Construction of asymmtric orthogonal arrays of strngth thr via a rplacmnt mthod Tian-fang Zhang, Qiaoling Dng and Alok Dy

More information

COUNTING TAMELY RAMIFIED EXTENSIONS OF LOCAL FIELDS UP TO ISOMORPHISM

COUNTING TAMELY RAMIFIED EXTENSIONS OF LOCAL FIELDS UP TO ISOMORPHISM COUNTING TAMELY RAMIFIED EXTENSIONS OF LOCAL FIELDS UP TO ISOMORPHISM Jim Brown Dpartmnt of Mathmatical Scincs, Clmson Univrsity, Clmson, SC 9634, USA jimlb@g.clmson.du Robrt Cass Dpartmnt of Mathmatics,

More information

On the number of pairs of positive integers x,y H such that x 2 +y 2 +1, x 2 +y 2 +2 are square-free

On the number of pairs of positive integers x,y H such that x 2 +y 2 +1, x 2 +y 2 +2 are square-free arxiv:90.04838v [math.nt] 5 Jan 09 On th numbr of pairs of positiv intgrs x,y H such that x +y +, x +y + ar squar-fr S. I. Dimitrov Abstract In th prsnt papr w show that thr xist infinitly many conscutiv

More information

Recall that by Theorems 10.3 and 10.4 together provide us the estimate o(n2 ), S(q) q 9, q=1

Recall that by Theorems 10.3 and 10.4 together provide us the estimate o(n2 ), S(q) q 9, q=1 Chaptr 11 Th singular sris Rcall that by Thorms 10 and 104 togthr provid us th stimat 9 4 n 2 111 Rn = SnΓ 2 + on2, whr th singular sris Sn was dfind in Chaptr 10 as Sn = q=1 Sq q 9, with Sq = 1 a q gcda,q=1

More information

SCHUR S THEOREM REU SUMMER 2005

SCHUR S THEOREM REU SUMMER 2005 SCHUR S THEOREM REU SUMMER 2005 1. Combinatorial aroach Prhas th first rsult in th subjct blongs to I. Schur and dats back to 1916. On of his motivation was to study th local vrsion of th famous quation

More information

1 N N(θ;d 1...d l ;N) 1 q l = o(1)

1 N N(θ;d 1...d l ;N) 1 q l = o(1) NORMALITY OF NUMBERS GENERATED BY THE VALUES OF ENTIRE FUNCTIONS MANFRED G. MADRITSCH, JÖRG M. THUSWALDNER, AND ROBERT F. TICHY Abstract. W show that th numbr gnratd by th q-ary intgr part of an ntir function

More information

The Matrix Exponential

The Matrix Exponential Th Matrix Exponntial (with xrciss) by D. Klain Vrsion 207.0.05 Corrctions and commnts ar wlcom. Th Matrix Exponntial For ach n n complx matrix A, dfin th xponntial of A to b th matrix A A k I + A + k!

More information

The Matrix Exponential

The Matrix Exponential Th Matrix Exponntial (with xrciss) by Dan Klain Vrsion 28928 Corrctions and commnts ar wlcom Th Matrix Exponntial For ach n n complx matrix A, dfin th xponntial of A to b th matrix () A A k I + A + k!

More information

INCOMPLETE KLOOSTERMAN SUMS AND MULTIPLICATIVE INVERSES IN SHORT INTERVALS. xy 1 (mod p), (x, y) I (j)

INCOMPLETE KLOOSTERMAN SUMS AND MULTIPLICATIVE INVERSES IN SHORT INTERVALS. xy 1 (mod p), (x, y) I (j) INCOMPLETE KLOOSTERMAN SUMS AND MULTIPLICATIVE INVERSES IN SHORT INTERVALS T D BROWNING AND A HAYNES Abstract W invstigat th solubility of th congrunc xy (mod ), whr is a rim and x, y ar rstrictd to li

More information

SECTION where P (cos θ, sin θ) and Q(cos θ, sin θ) are polynomials in cos θ and sin θ, provided Q is never equal to zero.

SECTION where P (cos θ, sin θ) and Q(cos θ, sin θ) are polynomials in cos θ and sin θ, provided Q is never equal to zero. SETION 6. 57 6. Evaluation of Dfinit Intgrals Exampl 6.6 W hav usd dfinit intgrals to valuat contour intgrals. It may com as a surpris to larn that contour intgrals and rsidus can b usd to valuat crtain

More information

Deift/Zhou Steepest descent, Part I

Deift/Zhou Steepest descent, Part I Lctur 9 Dift/Zhou Stpst dscnt, Part I W now focus on th cas of orthogonal polynomials for th wight w(x) = NV (x), V (x) = t x2 2 + x4 4. Sinc th wight dpnds on th paramtr N N w will writ π n,n, a n,n,

More information

Introduction to Arithmetic Geometry Fall 2013 Lecture #20 11/14/2013

Introduction to Arithmetic Geometry Fall 2013 Lecture #20 11/14/2013 18.782 Introduction to Arithmtic Gomtry Fall 2013 Lctur #20 11/14/2013 20.1 Dgr thorm for morphisms of curvs Lt us rstat th thorm givn at th nd of th last lctur, which w will now prov. Thorm 20.1. Lt φ:

More information

On the irreducibility of some polynomials in two variables

On the irreducibility of some polynomials in two variables ACTA ARITHMETICA LXXXII.3 (1997) On th irrducibility of som polynomials in two variabls by B. Brindza and Á. Pintér (Dbrcn) To th mmory of Paul Erdős Lt f(x) and g(y ) b polynomials with intgral cofficints

More information

Section 6.1. Question: 2. Let H be a subgroup of a group G. Then H operates on G by left multiplication. Describe the orbits for this operation.

Section 6.1. Question: 2. Let H be a subgroup of a group G. Then H operates on G by left multiplication. Describe the orbits for this operation. MAT 444 H Barclo Spring 004 Homwork 6 Solutions Sction 6 Lt H b a subgroup of a group G Thn H oprats on G by lft multiplication Dscrib th orbits for this opration Th orbits of G ar th right costs of H

More information

A Propagating Wave Packet Group Velocity Dispersion

A Propagating Wave Packet Group Velocity Dispersion Lctur 8 Phys 375 A Propagating Wav Packt Group Vlocity Disprsion Ovrviw and Motivation: In th last lctur w lookd at a localizd solution t) to th 1D fr-particl Schrödingr quation (SE) that corrsponds to

More information

Einstein Equations for Tetrad Fields

Einstein Equations for Tetrad Fields Apiron, Vol 13, No, Octobr 006 6 Einstin Equations for Ttrad Filds Ali Rıza ŞAHİN, R T L Istanbul (Turky) Evry mtric tnsor can b xprssd by th innr product of ttrad filds W prov that Einstin quations for

More information

(Upside-Down o Direct Rotation) β - Numbers

(Upside-Down o Direct Rotation) β - Numbers Amrican Journal of Mathmatics and Statistics 014, 4(): 58-64 DOI: 10593/jajms0140400 (Upsid-Down o Dirct Rotation) β - Numbrs Ammar Sddiq Mahmood 1, Shukriyah Sabir Ali,* 1 Dpartmnt of Mathmatics, Collg

More information

Some remarks on Kurepa s left factorial

Some remarks on Kurepa s left factorial Som rmarks on Kurpa s lft factorial arxiv:math/0410477v1 [math.nt] 21 Oct 2004 Brnd C. Kllnr Abstract W stablish a connction btwn th subfactorial function S(n) and th lft factorial function of Kurpa K(n).

More information

COMPUTER GENERATED HOLOGRAMS Optical Sciences 627 W.J. Dallas (Monday, April 04, 2005, 8:35 AM) PART I: CHAPTER TWO COMB MATH.

COMPUTER GENERATED HOLOGRAMS Optical Sciences 627 W.J. Dallas (Monday, April 04, 2005, 8:35 AM) PART I: CHAPTER TWO COMB MATH. C:\Dallas\0_Courss\03A_OpSci_67\0 Cgh_Book\0_athmaticalPrliminaris\0_0 Combath.doc of 8 COPUTER GENERATED HOLOGRAS Optical Scincs 67 W.J. Dallas (onday, April 04, 005, 8:35 A) PART I: CHAPTER TWO COB ATH

More information

1 Minimum Cut Problem

1 Minimum Cut Problem CS 6 Lctur 6 Min Cut and argr s Algorithm Scribs: Png Hui How (05), Virginia Dat: May 4, 06 Minimum Cut Problm Today, w introduc th minimum cut problm. This problm has many motivations, on of which coms

More information

arxiv: v1 [math.nt] 9 Jan 2014

arxiv: v1 [math.nt] 9 Jan 2014 ON A FORM OF DEGREE d IN 2d+ VARIABLES (d 4 MANOJ VERMA arxiv:4.2366v [math.nt] 9 Jan 24 Abstract. For k 2, w driv an asymptotic formula for th numbr of zros of th forms k (x2 2i +x2 2i + k (x2 2k+2i +x2

More information

22/ Breakdown of the Born-Oppenheimer approximation. Selection rules for rotational-vibrational transitions. P, R branches.

22/ Breakdown of the Born-Oppenheimer approximation. Selection rules for rotational-vibrational transitions. P, R branches. Subjct Chmistry Papr No and Titl Modul No and Titl Modul Tag 8/ Physical Spctroscopy / Brakdown of th Born-Oppnhimr approximation. Slction ruls for rotational-vibrational transitions. P, R branchs. CHE_P8_M

More information

Homework #3. 1 x. dx. It therefore follows that a sum of the

Homework #3. 1 x. dx. It therefore follows that a sum of the Danil Cannon CS 62 / Luan March 5, 2009 Homwork # 1. Th natural logarithm is dfind by ln n = n 1 dx. It thrfor follows that a sum of th 1 x sam addnd ovr th sam intrval should b both asymptotically uppr-

More information

PROOF OF FIRST STANDARD FORM OF NONELEMENTARY FUNCTIONS

PROOF OF FIRST STANDARD FORM OF NONELEMENTARY FUNCTIONS Intrnational Journal Of Advanc Rsarch In Scinc And Enginring http://www.ijars.com IJARSE, Vol. No., Issu No., Fbruary, 013 ISSN-319-8354(E) PROOF OF FIRST STANDARD FORM OF NONELEMENTARY FUNCTIONS 1 Dharmndra

More information

Fourier Transforms and the Wave Equation. Key Mathematics: More Fourier transform theory, especially as applied to solving the wave equation.

Fourier Transforms and the Wave Equation. Key Mathematics: More Fourier transform theory, especially as applied to solving the wave equation. Lur 7 Fourir Transforms and th Wav Euation Ovrviw and Motivation: W first discuss a fw faturs of th Fourir transform (FT), and thn w solv th initial-valu problm for th wav uation using th Fourir transform

More information

u 3 = u 3 (x 1, x 2, x 3 )

u 3 = u 3 (x 1, x 2, x 3 ) Lctur 23: Curvilinar Coordinats (RHB 8.0 It is oftn convnint to work with variabls othr than th Cartsian coordinats x i ( = x, y, z. For xampl in Lctur 5 w mt sphrical polar and cylindrical polar coordinats.

More information

Spectral Synthesis in the Heisenberg Group

Spectral Synthesis in the Heisenberg Group Intrnational Journal of Mathmatical Analysis Vol. 13, 19, no. 1, 1-5 HIKARI Ltd, www.m-hikari.com https://doi.org/1.1988/ijma.19.81179 Spctral Synthsis in th Hisnbrg Group Yitzhak Wit Dpartmnt of Mathmatics,

More information

Exercise 1. Sketch the graph of the following function. (x 2

Exercise 1. Sketch the graph of the following function. (x 2 Writtn tst: Fbruary 9th, 06 Exrcis. Sktch th graph of th following function fx = x + x, spcifying: domain, possibl asymptots, monotonicity, continuity, local and global maxima or minima, and non-drivability

More information

On spanning trees and cycles of multicolored point sets with few intersections

On spanning trees and cycles of multicolored point sets with few intersections On spanning trs and cycls of multicolord point sts with fw intrsctions M. Kano, C. Mrino, and J. Urrutia April, 00 Abstract Lt P 1,..., P k b a collction of disjoint point sts in R in gnral position. W

More information

CPSC 665 : An Algorithmist s Toolkit Lecture 4 : 21 Jan Linear Programming

CPSC 665 : An Algorithmist s Toolkit Lecture 4 : 21 Jan Linear Programming CPSC 665 : An Algorithmist s Toolkit Lctur 4 : 21 Jan 2015 Lcturr: Sushant Sachdva Linar Programming Scrib: Rasmus Kyng 1. Introduction An optimization problm rquirs us to find th minimum or maximum) of

More information

Higher order derivatives

Higher order derivatives Robrto s Nots on Diffrntial Calculus Chaptr 4: Basic diffrntiation ruls Sction 7 Highr ordr drivativs What you nd to know alrady: Basic diffrntiation ruls. What you can larn hr: How to rpat th procss of

More information

The van der Waals interaction 1 D. E. Soper 2 University of Oregon 20 April 2012

The van der Waals interaction 1 D. E. Soper 2 University of Oregon 20 April 2012 Th van dr Waals intraction D. E. Sopr 2 Univrsity of Orgon 20 pril 202 Th van dr Waals intraction is discussd in Chaptr 5 of J. J. Sakurai, Modrn Quantum Mchanics. Hr I tak a look at it in a littl mor

More information

Addition of angular momentum

Addition of angular momentum Addition of angular momntum April, 07 Oftn w nd to combin diffrnt sourcs of angular momntum to charactriz th total angular momntum of a systm, or to divid th total angular momntum into parts to valuat

More information

MATH 319, WEEK 15: The Fundamental Matrix, Non-Homogeneous Systems of Differential Equations

MATH 319, WEEK 15: The Fundamental Matrix, Non-Homogeneous Systems of Differential Equations MATH 39, WEEK 5: Th Fundamntal Matrix, Non-Homognous Systms of Diffrntial Equations Fundamntal Matrics Considr th problm of dtrmining th particular solution for an nsmbl of initial conditions For instanc,

More information

5.80 Small-Molecule Spectroscopy and Dynamics

5.80 Small-Molecule Spectroscopy and Dynamics MIT OpnCoursWar http://ocw.mit.du 5.80 Small-Molcul Spctroscopy and Dynamics Fall 008 For information about citing ths matrials or our Trms of Us, visit: http://ocw.mit.du/trms. Lctur # 3 Supplmnt Contnts

More information

NEW APPLICATIONS OF THE ABEL-LIOUVILLE FORMULA

NEW APPLICATIONS OF THE ABEL-LIOUVILLE FORMULA NE APPLICATIONS OF THE ABEL-LIOUVILLE FORMULA Mirca I CÎRNU Ph Dp o Mathmatics III Faculty o Applid Scincs Univrsity Polithnica o Bucharst Cirnumirca @yahoocom Abstract In a rcnt papr [] 5 th indinit intgrals

More information

Solution: APPM 1360 Final (150 pts) Spring (60 pts total) The following parts are not related, justify your answers:

Solution: APPM 1360 Final (150 pts) Spring (60 pts total) The following parts are not related, justify your answers: APPM 6 Final 5 pts) Spring 4. 6 pts total) Th following parts ar not rlatd, justify your answrs: a) Considr th curv rprsntd by th paramtric quations, t and y t + for t. i) 6 pts) Writ down th corrsponding

More information

Complex Powers and Logs (5A) Young Won Lim 10/17/13

Complex Powers and Logs (5A) Young Won Lim 10/17/13 Complx Powrs and Logs (5A) Copyright (c) 202, 203 Young W. Lim. Prmission is grantd to copy, distribut and/or modify this documnt undr th trms of th GNU Fr Documntation Licns, Vrsion.2 or any latr vrsion

More information

Combinatorial Networks Week 1, March 11-12

Combinatorial Networks Week 1, March 11-12 1 Nots on March 11 Combinatorial Ntwors W 1, March 11-1 11 Th Pigonhol Principl Th Pigonhol Principl If n objcts ar placd in hols, whr n >, thr xists a box with mor than on objcts 11 Thorm Givn a simpl

More information

2.3 Matrix Formulation

2.3 Matrix Formulation 23 Matrix Formulation 43 A mor complicatd xampl ariss for a nonlinar systm of diffrntial quations Considr th following xampl Exampl 23 x y + x( x 2 y 2 y x + y( x 2 y 2 (233 Transforming to polar coordinats,

More information

Lie Groups HW7. Wang Shuai. November 2015

Lie Groups HW7. Wang Shuai. November 2015 Li roups HW7 Wang Shuai Novmbr 015 1 Lt (π, V b a complx rprsntation of a compact group, show that V has an invariant non-dgnratd Hrmitian form. For any givn Hrmitian form on V, (for xampl (u, v = i u

More information

EEO 401 Digital Signal Processing Prof. Mark Fowler

EEO 401 Digital Signal Processing Prof. Mark Fowler EEO 401 Digital Signal Procssing Prof. Mark Fowlr Dtails of th ot St #19 Rading Assignmnt: Sct. 7.1.2, 7.1.3, & 7.2 of Proakis & Manolakis Dfinition of th So Givn signal data points x[n] for n = 0,, -1

More information

Mapping properties of the elliptic maximal function

Mapping properties of the elliptic maximal function Rv. Mat. Ibroamricana 19 (2003), 221 234 Mapping proprtis of th lliptic maximal function M. Burak Erdoğan Abstract W prov that th lliptic maximal function maps th Sobolv spac W 4,η (R 2 )intol 4 (R 2 )

More information

ON THE DISTRIBUTION OF THE ELLIPTIC SUBSET SUM GENERATOR OF PSEUDORANDOM NUMBERS

ON THE DISTRIBUTION OF THE ELLIPTIC SUBSET SUM GENERATOR OF PSEUDORANDOM NUMBERS INTEGERS: ELECTRONIC JOURNAL OF COMBINATORIAL NUMBER THEORY 8 2008, #A3 ON THE DISTRIBUTION OF THE ELLIPTIC SUBSET SUM GENERATOR OF PSEUDORANDOM NUMBERS Edwin D. El-Mahassni Dpartmnt of Computing, Macquari

More information

Probability and Stochastic Processes: A Friendly Introduction for Electrical and Computer Engineers Roy D. Yates and David J.

Probability and Stochastic Processes: A Friendly Introduction for Electrical and Computer Engineers Roy D. Yates and David J. Probability and Stochastic Procsss: A Frindly Introduction for Elctrical and Computr Enginrs Roy D. Yats and David J. Goodman Problm Solutions : Yats and Goodman,4.3. 4.3.4 4.3. 4.4. 4.4.4 4.4.6 4.. 4..7

More information

Square of Hamilton cycle in a random graph

Square of Hamilton cycle in a random graph Squar of Hamilton cycl in a random graph Andrzj Dudk Alan Friz Jun 28, 2016 Abstract W show that p = n is a sharp thrshold for th random graph G n,p to contain th squar of a Hamilton cycl. This improvs

More information

Finding low cost TSP and 2-matching solutions using certain half integer subtour vertices

Finding low cost TSP and 2-matching solutions using certain half integer subtour vertices Finding low cost TSP and 2-matching solutions using crtain half intgr subtour vrtics Sylvia Boyd and Robrt Carr Novmbr 996 Introduction Givn th complt graph K n = (V, E) on n nods with dg costs c R E,

More information

That is, we start with a general matrix: And end with a simpler matrix:

That is, we start with a general matrix: And end with a simpler matrix: DIAGON ALIZATION OF THE STR ESS TEN SOR INTRO DUCTIO N By th us of Cauchy s thorm w ar abl to rduc th numbr of strss componnts in th strss tnsor to only nin valus. An additional simplification of th strss

More information

First derivative analysis

First derivative analysis Robrto s Nots on Dirntial Calculus Chaptr 8: Graphical analysis Sction First drivativ analysis What you nd to know alrady: How to us drivativs to idntiy th critical valus o a unction and its trm points

More information

Application of Vague Soft Sets in students evaluation

Application of Vague Soft Sets in students evaluation Availabl onlin at www.plagiarsarchlibrary.com Advancs in Applid Scinc Rsarch, 0, (6):48-43 ISSN: 0976-860 CODEN (USA): AASRFC Application of Vagu Soft Sts in studnts valuation B. Chtia*and P. K. Das Dpartmnt

More information

EXST Regression Techniques Page 1

EXST Regression Techniques Page 1 EXST704 - Rgrssion Tchniqus Pag 1 Masurmnt rrors in X W hav assumd that all variation is in Y. Masurmnt rror in this variabl will not ffct th rsults, as long as thy ar uncorrlatd and unbiasd, sinc thy

More information

Bifurcation Theory. , a stationary point, depends on the value of α. At certain values

Bifurcation Theory. , a stationary point, depends on the value of α. At certain values Dnamic Macroconomic Thor Prof. Thomas Lux Bifurcation Thor Bifurcation: qualitativ chang in th natur of th solution occurs if a paramtr passs through a critical point bifurcation or branch valu. Local

More information

EXISTENCE OF POSITIVE ENTIRE RADIAL SOLUTIONS TO A (k 1, k 2 )-HESSIAN SYSTEMS WITH CONVECTION TERMS

EXISTENCE OF POSITIVE ENTIRE RADIAL SOLUTIONS TO A (k 1, k 2 )-HESSIAN SYSTEMS WITH CONVECTION TERMS Elctronic Journal of Diffrntial Equations, Vol. 26 (26, No. 272, pp. 8. ISSN: 72-669. URL: http://jd.math.txstat.du or http://jd.math.unt.du EXISTENCE OF POSITIVE ENTIRE RADIAL SOLUTIONS TO A (k, k 2 -HESSIAN

More information

Basic Polyhedral theory

Basic Polyhedral theory Basic Polyhdral thory Th st P = { A b} is calld a polyhdron. Lmma 1. Eithr th systm A = b, b 0, 0 has a solution or thr is a vctorπ such that π A 0, πb < 0 Thr cass, if solution in top row dos not ist

More information

SOME PARAMETERS ON EQUITABLE COLORING OF PRISM AND CIRCULANT GRAPH.

SOME PARAMETERS ON EQUITABLE COLORING OF PRISM AND CIRCULANT GRAPH. SOME PARAMETERS ON EQUITABLE COLORING OF PRISM AND CIRCULANT GRAPH. K VASUDEVAN, K. SWATHY AND K. MANIKANDAN 1 Dpartmnt of Mathmatics, Prsidncy Collg, Chnnai-05, India. E-Mail:vasu k dvan@yahoo.com. 2,

More information

1 General boundary conditions in diffusion

1 General boundary conditions in diffusion Gnral boundary conditions in diffusion Πρόβλημα 4.8 : Δίνεται μονοδιάτατη πλάκα πάχους, που το ένα άκρο της κρατιέται ε θερμοκραία T t και το άλλο ε θερμοκραία T 2 t. Αν η αρχική θερμοκραία της πλάκας

More information

Bernadette Faye, Florian Luca, and Amadou Tall

Bernadette Faye, Florian Luca, and Amadou Tall Bull Koran Math Soc 52 (205), No 2, pp 53 524 http://dxdoiorg/0434/bkms20552253 ON THE EQUATION φ(5 m ) = 5 n Brnadtt Fay, Florian Luca, and Amadou Tall Abstract Hr, w show that th titl uation has no positiv

More information

Addition of angular momentum

Addition of angular momentum Addition of angular momntum April, 0 Oftn w nd to combin diffrnt sourcs of angular momntum to charactriz th total angular momntum of a systm, or to divid th total angular momntum into parts to valuat th

More information

Homotopy perturbation technique

Homotopy perturbation technique Comput. Mthods Appl. Mch. Engrg. 178 (1999) 257±262 www.lsvir.com/locat/cma Homotopy prturbation tchniqu Ji-Huan H 1 Shanghai Univrsity, Shanghai Institut of Applid Mathmatics and Mchanics, Shanghai 272,

More information

Calculus II (MAC )

Calculus II (MAC ) Calculus II (MAC232-2) Tst 2 (25/6/25) Nam (PRINT): Plas show your work. An answr with no work rcivs no crdit. You may us th back of a pag if you nd mor spac for a problm. You may not us any calculators.

More information

2F1120 Spektrala transformer för Media Solutions to Steiglitz, Chapter 1

2F1120 Spektrala transformer för Media Solutions to Steiglitz, Chapter 1 F110 Spktrala transformr för Mdia Solutions to Stiglitz, Chaptr 1 Prfac This documnt contains solutions to slctd problms from Kn Stiglitz s book: A Digital Signal Procssing Primr publishd by Addison-Wsly.

More information

Ewald s Method Revisited: Rapidly Convergent Series Representations of Certain Green s Functions. Vassilis G. Papanicolaou 1

Ewald s Method Revisited: Rapidly Convergent Series Representations of Certain Green s Functions. Vassilis G. Papanicolaou 1 wald s Mthod Rvisitd: Rapidly Convrgnt Sris Rprsntations of Crtain Grn s Functions Vassilis G. Papanicolaou 1 Suggstd Running Had: wald s Mthod Rvisitd Complt Mailing Addrss of Contact Author for offic

More information

Chapter 13 GMM for Linear Factor Models in Discount Factor form. GMM on the pricing errors gives a crosssectional

Chapter 13 GMM for Linear Factor Models in Discount Factor form. GMM on the pricing errors gives a crosssectional Chaptr 13 GMM for Linar Factor Modls in Discount Factor form GMM on th pricing rrors givs a crosssctional rgrssion h cas of xcss rturns Hors rac sting for charactristic sting for pricd factors: lambdas

More information

INHOMOGENEOUS QUADRATIC CONGRUENCES. S. Baier & T.D. Browning

INHOMOGENEOUS QUADRATIC CONGRUENCES. S. Baier & T.D. Browning INHOMOGENEOUS QUADRATIC CONGRUENCES by S Bair & TD Browning Abstract For givn positiv intgrs a, b, w invstigat th dnsity of solutions x, y Z 2 to congruncs ax + by 2 0 mod Introduction Lt a, b, b non-zro

More information

Mor Tutorial at www.dumblittldoctor.com Work th problms without a calculator, but us a calculator to chck rsults. And try diffrntiating your answrs in part III as a usful chck. I. Applications of Intgration

More information

Hydrogen Atom and One Electron Ions

Hydrogen Atom and One Electron Ions Hydrogn Atom and On Elctron Ions Th Schrödingr quation for this two-body problm starts out th sam as th gnral two-body Schrödingr quation. First w sparat out th motion of th cntr of mass. Th intrnal potntial

More information

Lecture 37 (Schrödinger Equation) Physics Spring 2018 Douglas Fields

Lecture 37 (Schrödinger Equation) Physics Spring 2018 Douglas Fields Lctur 37 (Schrödingr Equation) Physics 6-01 Spring 018 Douglas Filds Rducd Mass OK, so th Bohr modl of th atom givs nrgy lvls: E n 1 k m n 4 But, this has on problm it was dvlopd assuming th acclration

More information

ON A CONJECTURE OF RYSElt AND MINC

ON A CONJECTURE OF RYSElt AND MINC MA THEMATICS ON A CONJECTURE OF RYSElt AND MINC BY ALBERT NIJE~HUIS*) AND HERBERT S. WILF *) (Communicatd at th mting of January 31, 1970) 1. Introduction Lt A b an n x n matrix of zros and ons, and suppos

More information

10. The Discrete-Time Fourier Transform (DTFT)

10. The Discrete-Time Fourier Transform (DTFT) Th Discrt-Tim Fourir Transform (DTFT Dfinition of th discrt-tim Fourir transform Th Fourir rprsntation of signals plays an important rol in both continuous and discrt signal procssing In this sction w

More information

Self-Adjointness and Its Relationship to Quantum Mechanics. Ronald I. Frank 2016

Self-Adjointness and Its Relationship to Quantum Mechanics. Ronald I. Frank 2016 Ronald I. Frank 06 Adjoint https://n.wikipdia.org/wiki/adjoint In gnral thr is an oprator and a procss that dfin its adjoint *. It is thn slf-adjoint if *. Innr product spac https://n.wikipdia.org/wiki/innr_product_spac

More information

A generalized attack on RSA type cryptosystems

A generalized attack on RSA type cryptosystems A gnralizd attack on RSA typ cryptosystms Martin Bundr, Abdrrahman Nitaj, Willy Susilo, Josph Tonin Abstract Lt N = pq b an RSA modulus with unknown factorization. Som variants of th RSA cryptosystm, such

More information

Supplementary Materials

Supplementary Materials 6 Supplmntary Matrials APPENDIX A PHYSICAL INTERPRETATION OF FUEL-RATE-SPEED FUNCTION A truck running on a road with grad/slop θ positiv if moving up and ngativ if moving down facs thr rsistancs: arodynamic

More information

Middle East Technical University Department of Mechanical Engineering ME 413 Introduction to Finite Element Analysis

Middle East Technical University Department of Mechanical Engineering ME 413 Introduction to Finite Element Analysis Middl East Tchnical Univrsity Dpartmnt of Mchanical Enginring ME 43 Introduction to Finit Elmnt Analysis Chaptr 3 Computr Implmntation of D FEM Ths nots ar prpard by Dr. Cünyt Srt http://www.m.mtu.du.tr/popl/cunyt

More information

Another view for a posteriori error estimates for variational inequalities of the second kind

Another view for a posteriori error estimates for variational inequalities of the second kind Accptd by Applid Numrical Mathmatics in July 2013 Anothr viw for a postriori rror stimats for variational inqualitis of th scond kind Fi Wang 1 and Wimin Han 2 Abstract. In this papr, w giv anothr viw

More information

ECE602 Exam 1 April 5, You must show ALL of your work for full credit.

ECE602 Exam 1 April 5, You must show ALL of your work for full credit. ECE62 Exam April 5, 27 Nam: Solution Scor: / This xam is closd-book. You must show ALL of your work for full crdit. Plas rad th qustions carfully. Plas chck your answrs carfully. Calculators may NOT b

More information

The Equitable Dominating Graph

The Equitable Dominating Graph Intrnational Journal of Enginring Rsarch and Tchnology. ISSN 0974-3154 Volum 8, Numbr 1 (015), pp. 35-4 Intrnational Rsarch Publication Hous http://www.irphous.com Th Equitabl Dominating Graph P.N. Vinay

More information

There is an arbitrary overall complex phase that could be added to A, but since this makes no difference we set it to zero and choose A real.

There is an arbitrary overall complex phase that could be added to A, but since this makes no difference we set it to zero and choose A real. Midtrm #, Physics 37A, Spring 07. Writ your rsponss blow or on xtra pags. Show your work, and tak car to xplain what you ar doing; partial crdit will b givn for incomplt answrs that dmonstrat som concptual

More information

Research Article Norm and Essential Norm of an Integral-Type Operator from the Dirichlet Space to the Bloch-Type Space on the Unit Ball

Research Article Norm and Essential Norm of an Integral-Type Operator from the Dirichlet Space to the Bloch-Type Space on the Unit Ball Hindawi Publishing Corporation Abstract and Applid Analysis Volum 2010, Articl ID 134969, 9 pags doi:10.1155/2010/134969 Rsarch Articl Norm and Essntial Norm of an Intgral-Typ Oprator from th Dirichlt

More information

4. (5a + b) 7 & x 1 = (3x 1)log 10 4 = log (M1) [4] d = 3 [4] T 2 = 5 + = 16 or or 16.

4. (5a + b) 7 & x 1 = (3x 1)log 10 4 = log (M1) [4] d = 3 [4] T 2 = 5 + = 16 or or 16. . 7 7 7... 7 7 (n )0 7 (M) 0(n ) 00 n (A) S ((7) 0(0)) (M) (7 00) 8897 (A). (5a b) 7 7... (5a)... (M) 7 5 5 (a b ) 5 5 a b (M)(A) So th cofficint is 75 (A) (C) [] S (7 7) (M) () 8897 (A) (C) [] 5. x.55

More information

ABEL TYPE THEOREMS FOR THE WAVELET TRANSFORM THROUGH THE QUASIASYMPTOTIC BOUNDEDNESS

ABEL TYPE THEOREMS FOR THE WAVELET TRANSFORM THROUGH THE QUASIASYMPTOTIC BOUNDEDNESS Novi Sad J. Math. Vol. 45, No. 1, 2015, 201-206 ABEL TYPE THEOREMS FOR THE WAVELET TRANSFORM THROUGH THE QUASIASYMPTOTIC BOUNDEDNESS Mirjana Vuković 1 and Ivana Zubac 2 Ddicatd to Acadmician Bogoljub Stanković

More information

ON RIGHT(LEFT) DUO PO-SEMIGROUPS. S. K. Lee and K. Y. Park

ON RIGHT(LEFT) DUO PO-SEMIGROUPS. S. K. Lee and K. Y. Park Kangwon-Kyungki Math. Jour. 11 (2003), No. 2, pp. 147 153 ON RIGHT(LEFT) DUO PO-SEMIGROUPS S. K. L and K. Y. Park Abstract. W invstigat som proprtis on right(rsp. lft) duo po-smigroups. 1. Introduction

More information

u x v x dx u x v x v x u x dx d u x v x u x v x dx u x v x dx Integration by Parts Formula

u x v x dx u x v x v x u x dx d u x v x u x v x dx u x v x dx Integration by Parts Formula 7. Intgration by Parts Each drivativ formula givs ris to a corrsponding intgral formula, as w v sn many tims. Th drivativ product rul yilds a vry usful intgration tchniqu calld intgration by parts. Starting

More information

Week 3: Connected Subgraphs

Week 3: Connected Subgraphs Wk 3: Connctd Subgraphs Sptmbr 19, 2016 1 Connctd Graphs Path, Distanc: A path from a vrtx x to a vrtx y in a graph G is rfrrd to an xy-path. Lt X, Y V (G). An (X, Y )-path is an xy-path with x X and y

More information

arxiv: v1 [math.nt] 21 Nov 2013

arxiv: v1 [math.nt] 21 Nov 2013 CONSTRUCTION OF NORMAL NUMBERS VIA GENERALIZED PRIME POWER SEQUENCES MANFRED G. MADRITSCH AND ROBERT F. TICHY Ddicatd to Jan-Paul Allouch on th occasion of his 60 th birthday arxiv:1311.5482v1 [math.nt]

More information

International Journal of Scientific & Engineering Research, Volume 6, Issue 7, July ISSN

International Journal of Scientific & Engineering Research, Volume 6, Issue 7, July ISSN Intrnational Journal of Scintific & Enginring Rsarch, Volum 6, Issu 7, July-25 64 ISSN 2229-558 HARATERISTIS OF EDGE UTSET MATRIX OF PETERSON GRAPH WITH ALGEBRAI GRAPH THEORY Dr. G. Nirmala M. Murugan

More information

OPTIMAL STRONG APPROXIMATION FOR QUADRATIC FORMS

OPTIMAL STRONG APPROXIMATION FOR QUADRATIC FORMS OPTIMAL STROG APPROXIMATIO FOR UADRATIC FORMS ASER T SARDARI Abstract For a non-dgnrat intgral uadratic form F x 1,, x d in d 5 variabls, w prov an optimal strong approximation thorm Lt Ω b a fixd compact

More information

Rational Approximation for the one-dimensional Bratu Equation

Rational Approximation for the one-dimensional Bratu Equation Intrnational Journal of Enginring & Tchnology IJET-IJES Vol:3 o:05 5 Rational Approximation for th on-dimnsional Bratu Equation Moustafa Aly Soliman Chmical Enginring Dpartmnt, Th British Univrsity in

More information

2008 AP Calculus BC Multiple Choice Exam

2008 AP Calculus BC Multiple Choice Exam 008 AP Multipl Choic Eam Nam 008 AP Calculus BC Multipl Choic Eam Sction No Calculator Activ AP Calculus 008 BC Multipl Choic. At tim t 0, a particl moving in th -plan is th acclration vctor of th particl

More information