Estimates of li(θ(x)) π(x) and the Riemann hypothesis

Size: px
Start display at page:

Download "Estimates of li(θ(x)) π(x) and the Riemann hypothesis"

Transcription

1 Esimaes of liθ π he Riemann hypohesis Jean-Louis Nicolas 20 mai 206 Absrac To Krishna Alladi for his siieh birhday Le us denoe by π he number of primes, by li he logarihmic inegral of, by θ = p log p he Chebichev funcion le us se A = liθ π Revisiing a resul of Ramanujan, we prove ha he asserion A > 0 for is equivalen o he Riemann hypohesis Keywords : Chebichev funcion, Riemann hypohesis, Eplici formula 200 Mahemaics Subjec Classificaion : N37, M26, N56 Inroducion Le us denoe by π he number of primes by li he logarihmic inegral of see, below, 22 I has been observed ha, for small, π < li holds, bu Lilewood cf [7] or [5, chap 5] has proved ha, for ending o infiniy, he difference π li oscillaes infiniely many ofen beween posiive negaive values Le us se θ = p log p, he Chebichev funcion, A = liθ π Wha is he behavior of A? In [0, 220, 222, ], under he Riemann hypohesis, Ramanujan proved ha 2 A = 2 + / 2 log 2 + O log 3 where runs over he non-rivial zeros of he Riemann ζ funcion Moreover, in [0, 226], Ramanujan wries under he Riemann hypohesis 2 2 = = + = 2 3 = 2 + γ 0 log4π = 0046 where γ 0 is he Euler consan concludes 4 under he Riemann hypohesis 0 such ha, for 0, A is posiive The aim of his paper is o make hese resuls effecive, in paricular, o show ha Ramanujan s resul 4 is rue for 0 = Research parially suppored by CNRS, Insiu Camille Jordan, UMR 5208

2 Le us se λ = 2 Under he Riemann hypohesis, we have see below λ = We shall prove 2 = = Theorem Under he Riemann hypohesis, we have 6 lim sup A log λ = 2046, 7 lim inf A log 2 2 λ = 953, 8 A is posiive for, 9 A 2 λ log 2 for 37, 0 A M log 2 for 2, where M = A3643log / 3643 = Corollary Each of he five asserions 6 0 is equivalen o he Riemann hypohesis Proof : In 984, Robin cf [9, Lemma 2 8] has shown ha, if he Riemann hypohesis does no hold, here eiss b > /2 such ha A = Ω ± b, ie lim sup A b he five asserions of he heorem are no longer saisfied > 0 lim inf A b < 0 Noaion π = p is he prime couning funcion Π = p k k = κ k= π /k k wih κ = log log 2 θ = log p ψ = κ log p = θ /k p p m k= { log p if = p k Λ = is he von Mangold funcion 0 if no ψ = ψ 2 Λ Π = Π Λ 2 log li denoes he logarihmic inegral of cf below 22 are he Chebichev funcions 2

3 L = li log, L 2 = li log log 2, F = L / log 2, F 2 = L 2 / log 3 > F F 2 are defined below in 36 γ 0 = is he Euler consan λ is defined in 5, cf also 226 f = lim f where f : C C is a comple funcion runs over he non-rivial T I T zeros of he Riemann ζ funcion 2 Plan of he aricle In 2, we shall recall some definiions prove some resuls ha we shall use in he sequel, firs, in 22, abou he logarihmic inegral,, furher, in 23, abou he Riemann ζ funcion eplici formulas of he heory of numbers In 3, he proof of Theorem is given Firs, we wrie A = A + A 2 wih A = liψ Π A 2 = liθ liψ + Π π In 3, under he Riemann hypohesis, an esimae of A is given, by applying he eplici formulas In 32, i is shown ha A 2 depends on he quaniy By = πy θy/ log y which is carefully sudied In 33 resp 34, an effecive lower resp upper esimae for A is given when 0 8 In 35, for < 0 8, esimaes of A are given by numerical compuaion Finally, Theorem is proved in wo seps, depending on he cases 0 8 or > 0 8 The compuaions, boh algebraic numerical, have been carried ou wih Maple On he websie [2], one can find he code a Maple shee wih he resuls We ofen implicily use he following resul : for u v posiive, he funcion logu v is increasing for e u/v decreasing for > e u/v Moreover 2 ma 2 Preliminary resuls 2 Effecive esimaes log u u u v = e v Wihou any hypohesis, Pla Trudgian [8] have shown by compuaion ha 2 θ < for 0 < so improving on resuls of Schoenfeld [] Dusar [3] Under he Riemann hypohesis, for 599, we shall use he upper bounds cf [, 63] 22 ψ log 2 θ log 2 8π 8π 3

4 22 The logarihmic inegral For real >, we define li as cf [, p 228] li = d log = lim ε 0 + We have he following values : 0 ε 0 + +ε d = log 2 d log + li li From he definiion of li, i follows ha 24 d d li = log d 2 d 2 li = log 2 We also have li = γ 0 + loglog + where γ 0 = 0577 is he Euler consan which implies n= log n n n! 25 li = loglog + γ 0 + o, + Le N be a posiive ineger For >, we have cf [2] 26, for, 27 li = N d log N = li k! N! log k N k= k! log k k= + O log N+ Lemma 2 For >, we have 28 L 2 = li log log 2 = F 2 log 3 < 405 log 3 For 0 38, we have 29 L 2 < F 2 0 For > 29, we have log 3 20 L 2 > 2 log 3 Proof : le us se cf he Maple shee [2] f = 3 log li + f 2 = log + 2 log log 2 = 2 F 2 log 2, log log 3 li = f 4

5 f 3 = f 2 = 6 log 4 Since f 2 = f 3 is negaive, f 2 decreases vanishes for 2 = I follows ha f = f 2 / is posiive for < < 2 negaive for > 2 so ha f has a maimum for = 2, f 2 = f vanishes so does F 2 in wo poins 3 = = From 25, we ge lim + F 2 = 0 he variaion of F 2 is given in he following array : F 2 = L2 / log The proof of follows from Array 2 also he proof of 20, afer deducing from f 2 2 = 0 ha F 2 2 = 2 holds In he same way, i is possible o sudy he variaion of he funcion The deails can be found on [2] We have log F = L / log 2 = li / log 2, F = L log Since L =, Array 22 yields 23 > 04 = L = li log > log 2 / log li The derivaive of li/ is = F which, from Array 22, is posiive for < < log 2 negaive for > Therefore, we have 24 > = li li = < 3 4 Lemma 22 Le a be wo real numbers saisfying ep a < a 3 Le κ κ 2 be wo inegers such ha log 2 κ < κ 2 = log a Then we have 25 κ 2 k=κ + k L /k κ3 /κ log 3 L 2a 5

6 Proof : Le us se T = κ 2 k=κ + k L /k I follows from Array 22 ha, for >, L = F / log log 2 holds herefore, T 785 log 2 κ 2 k=κ + k /k Now, as ep >, he funcion / is posiive decreasing for 0 < log so ha T 785 κ2 log 2 / d 785 log log a /κ κ log 2 / d = 785 κ a du log 3 u by he change of variable u = / Finally, by 26 28, we ge /κ T 785 L 2 /κ L 2 a log 3 /κ L 2a which ends he proof of Lemma 22 Lemma 23 Le a 2 a 3 be real numbers κ 2 = log log a Then we have 26 κ 2 k /2k 5 4 /4 Proof : Le us se T = κ 2 k /2k Since a 3 >, he funcion /2 / is posiive decreasing for > 0 so ha T = κ 2 2 /4 + k /2k log log a 2 /4 + 2 k=3 /2 by he change of variable u = /2 Finally, by 26 24, we ge T 2 /4 + li /4 li a 5 4 /4 li a d = /4 du 2 /4 + a log u 26 follows since a 2 > 452 so ha, from Array 23, li a > 0 holds Lemma 24 Under he Riemann hypohesis, for 599, one has 27 θ log 9 log liθ li θ log ψ θ log ψ log 9 log log liψ li ψ log, liψ liθ ψ θ log + 9 log

7 Proof : Le us suppose ha 599 holds From 22, we ge 220 ψ θ log 2 Furher, for h >, Taylor s formula 24 yield 8π = log2 8π log π 599 > li + h = li + h log h 2 2 ξ log 2 ξ, wih ξ min, + h Le us se h = θ ; we have h + = θ θ599 > From 220, we ge ξ b wih b = From 22, i follows ha 0 ξ log 2 ξ b log 2 b = b log 2 + log b 2 log b log 2 + log b log 2 log599 h 2 2 ξ log 2 ξ log 4 28 π 2 ξ log 2 ξ log π 2 = log2 < 9 log which, wih 22, proves 27 In he same way, seing h = ψ yields 28, 29 follows by subsracing 27 from The Riemann ζ funcion We shall use he wo eplici formulas 222 ψ = ψ 2 Λ = log2π 2 log 2, > 223 Π = Π Λ 2 log = li li d log log, >, which can be found in many books in analyic number heory, for insance [5, chap 4] To Formula 223, we prefer he form described in [6, p , wih R = 0] : 224 Π = Π Λ 2 log = li 0 d d log log, > 225 We also have cf [4, p 67] or [2, p 272] = + γ 0 2 log π log 2 = = + = 2 + γ 0 log4π =

8 3 Proof of Theorem 3 Sudy of A = liψ Π Under he Riemann hypohesis, we wrie γ = I ie = 2 + iγ Lemma 3 Under he Riemann hypohesis, we have γ Proof : I is possible o ge beer esimaes for he sum γ 3, bu, for our purpose, he above upper bound will be enough By observing ha 2 = = 4 + γ2 ha he firs zero of ζs is / i cf [4, p 96] or Wikipedia, we ge γ 2 = + /4γ 2 /4 + γ 2 + / /4 + γ Furher, from 226, we ge γ γ = which complees he proof of Lemma 3 Lemma 32 For >, under he Riemann hypohesis, we have 0 d = log + wih 3 K log 3 Proof : By parial inegraion, one has 2 log 2 + K so ha we ge 0 d = 0 log + 3 d I 3 2 K = log 2 3 follows from Lemma log log /2 d = I 3 3 d log 3 d 2 log 3 I 3 8

9 Proposiion 3 Under he Riemann hypohesis, for 599, we have A = liψ Π = 2 log 2 + J wih log log 3 J 300 log 3 + log 2 Proof : Le us wrie liψ = li + ψ log wih, from 28, for 599, + J = li + ψ + Λ/2 log log 2 J 0 Therefore, from , we have A = li + log = 0 + J log2π 2 log Λ + J d + d Λ 2 log 2 + log 2 log li 0 d log + J + J 2 + J 3 wih J 2 = log 2 log2π log Furher, from Lemma 32, one ges J 3 = log /2 2 log d 2 log 34 A = 2 log 2 + J wih 35 J = K + J + J 2 + J 3 K is as in Lemma 32 I remains o bound J 2 + J 3 We have which, for 599, implies 0 J 3 log J 3 = 2 log d log d 2 = log + /2 2 log 2 2 log < log2π log 0 < J 2 + J 3 < log 2 Therefore, 32 resuls from 3, 33,

10 32 Sudy of A 2 = liθ liψ + Π π For y 2, le us se By = πy θy log y = log p log y p y Noe ha By is nonnegaive, nondecreasing coninuous, since for p prime, lim y p, y<p By = πp θp log p log p = Bp In he wo following lemmas, we give esimaes of By Lemma 33 Le y be a real number saisfying y 0 = 83 y We have 36 By L y = liy y log y while, if y y = 599, under he Riemann hypohesis, we have y 37 By L y + 4π Under he Riemann hypohesis, for y y 2 = 2903, we have y 38 By L y 4π Proof : By Sieljes s inegral, one has 39 πy = Furher, we have 30 By = y 2 y d[θ] 2 log θ y0 y log 2 d = + 2 y 0 By 2 26, for y , we ge y y 0 θ log 2 d y y 0 log 2 d = liy y = θy y log y + θ 2 log 2 d θ y log 2 d = By 0 + y 0 θ log 2 d log y liy 0 + y 0 log y 0 = L y L y 0, so ha 30 yields By L y + By 0 L y 0, which proves 36, since By 0 L y 0 = < 0 cf [2] Replacing y 0 by y in 30 yields 3 By = By + wih T y, y = y y y y θ d, from 22, log 2 32 T y, y From 3 32, i follows ha θd log 2 = By L y + L y + T y, y y By L y + y log 2 8π log 2 d = y y 4π y 4π + By y L y 4π y which proves 37, since By L y 4π = < 0 In he same way han he one used o ge 3, for y y 2, we obain y By = By 2 L y 2 + L y + T y, y 2 L y 4π + By 2 L y 2 + 4π 0 y2

11 y2 as By 2 L y 2 + 4π = > 0, his complees he proof of Lemma 33 Le us se εy = { 0 if y if y > I follows from ha, under he Riemann hypohesis, one has y 33 By L y + εy for y 83 4π Proposiion 32 Under he Riemann hypohesis, for 599, we have 34 A 2 = liθ liψ + Π π = κ k B/k + U wih 35 κ := log log 2 Proof : From 29, for 599, we ge U 9 log liθ liψ = θ ψ log From he definiion of ψ Π, his implies A 2 = κ π /k k + U wih U 9 log θ/k + U log which, via he definiion of B, proves 34 I is convenien o inroduce he noaion { 405 if < F2 = F 2 if > 38 F = { 785 if < 95 F if > 95 so ha, from Arrays 2 22, for >, F 2 F are nonincreasing we have 37 L 2 = F 2 log 3 F 2 log 3 L = F log 2 F log 2 Lemma 34 Le us se a = 04 For > 0 8, we se κ = log log 2, κ 2 = log log a le κ be an ineger saisfying 3 κ < κ 2 Then, under he Riemann hypohesis, we have κ B /k k 2 log F log 3 2 κ k /k + F log 2 /k κ3 /κ log 3 k= log 5 Proof : For 2 k κ 2 we have /k /κ2 log a/ log = a,, under he Riemann hypohesis, i follows from 33 ha which implies ha B /k L /k + ε /k /2k 4π κ B /k k T + T 2 + T 3 + T 4 + T 5

12 wih T = 2 L, T 2 = T 4 = κ k=κ 2+ κ k=3 L /k, T 3 = k B /k, T 5 = k κ 2 κ 2 k=κ + ε /k /2k 4kπ L /k, k From he definiion of L, L 2, F, F 2 from 37, one has T = L log 2 = 2 log log 3 F 2 2 log F log 3 2 T 2 = κ k=3 L /k k = κ k=3 k /k log 2 F /k κ k=3 k /k F log 2 /k From Array 2, L 2 04 is posiive, so ha, from Lemma 22 wih a = 04, we have T κ3 /κ log 3 L κ3 /κ log κ3 /κ log 3 For k κ 2 + > log / log a, we have /k < a ; since y By is nondecreasing, we have B /k Ba = B04 = 766 < 72 κ κ log d log 2 d T k k=κ κ 2+ 2 log log a log log/a log a = 72 log log = 72 log log 2 log a log 2 log a log log a 72 log + log 2 log/a = 72 log log 2 log a log a 72 log + log 2 log0 8 = /a log + log log/a + log a log/a Since ε is nondecreasing vanishes for 0 7, from Lemma 23, one ges T 5 = κ 2 ε /k /2k 4kπ ε = 5 6π ε log 5 κ 2 log 5 /4 < 5 6π /2k 4kπ 5 6π ε /4 log 5 log = /4 log 5, which complees he proof of Lemma A lower bound fora Proposiion 33 Under he Riemann hypohesis, for 9 0 6, we have 38 A log 2 2 λ + log 7993 log3 8 8π/ Proof : Since By is nonnegaive, from 34 35, we ge, for 599 A 2 2 B 9 log log 5 2

13 As , we may apply 38 which yields A 2 L /4 2 4π 9 log = 2 Now, as > 29 2, by 20, i follows A 2 2 log log 3 /4 9 log2 4π 0000 = log 2 log 2 + L 2 /4 9 log2 4π 0000 From Proposiion 3, one has : A 2 log log log 3 so ha A = A + A 2 saisfies A log log log2 8π 9 log4 / /300 log2 log 8π 8 log4 / which, via 5, implies 38 Corollary 3 Under he Riemann hypohesis, for 0 8, we have 39 A log 2 2 λ + 52 log Proof : From, he funcions log3 /4 we have cf [2] log5 are decreasing for 0 8 herefore, 7993 log3 8 log log π/ π 8 log = An upper bound fora Proposiion 34 Under he Riemann hypohesis, for 0 8, we have 320 A log λ + Qκ, log where κ is an ineger saisfying 3 κ < log log Qκ, = 4 F log3 + wih F 2 F defined in 36 κ k=3 k F /k log /2 /k κ3 /2 /κ log log Proof : From Proposiion 3 5, for 599, we have A λ log log while, from Proposiion 32, we have A 2 κ k B/k + 9 log Therefore, from Lemma 34, we ge he upper bound 320 for A = A + A 2 3

14 Corollary 32 Under he Riemann hypohesis, for 0 8, we have 322 A log λ log Proof : We choose κ = 5 observe ha, from 36, all he erms of he righ h side of 32 are posiive nonincreasing for 0 8 so ha Q5, Q5, 0 8 = 2529 cf [2] Corollary 33 Under he Riemann hypohesis, for ending o infiniy, we have o o 323 log 2 2 λ + A log log λ + log Proof : The lower bound of 323 follows from Proposiion 33 From Array 2, from 23 from 36, one sees in 32, ha lim F2 = 2 lim F /3 = so ha 32 yields lim Q3, = 8 + 2/300 he upper bound of 323 follows from Proposiion 34 wih κ = 3 35 Numerical compuaion Le us denoe by p p + he primes surrounding he prime p Proposiion 35 For < , A is nondecreasing There eiss infiniely many primes p for which Ap < Ap holds Proof : Le us consider a prime p saisfying 3 p < From 2, one has θp Ap Ap = liθp liθp d = + θp log > + θp θp = log p log θp log θp > 0 From Lilewood cf[7] or [5, chap 5], we know ha here eiss C > 0 a sequence of values of going o infiniy such ha θ + C log log log Le p be he larges prime For p large enough, one has θp = θ + C log log log > p + log p Ap Ap < which complees he proof of Proposiion 35 log p log θp = log p logθp log p < 0 Remark In [8, p 8], Pla Trudgian have proved he eisence of u saisfying 727 < u < 728 θe u e u > 0 52 If P is he larges prime e u, his implies AP < AP + θp = θe u > e u > P + u P + log P log P logθp log P < AP 4

15 Proposiion 36 i For we have 324 A > 0 ii Under he Riemann hypohesis, for 2 we have 325 A 2 + λ log log wih equaliy for = iii Under he Riemann hypohesis, for we have 326 A log λ log iv For we have 327 A log 2 wih equaliy for = 3643 v Under he Riemann hypohesis, for 84 we have 328 A log 2 2 λ + 52 log vi For 37 < 89 we have 329 A log 2 2 λ Proof : Firs, for 2, we define C c by A = log λ + C A = log log 2 2 λ + c log so ha C = log A log2 2 λ c = log A log2 2 + λ i 324 follows from Proposiion 35 A = 030 Noe ha A7 = 054 < 0 cf [2] ii If 0 8, 325 follows from Corollary 32 If 2 < 409, from 2, one has log 2 / 6/e 2, from Proposiion 35, A A so ha C = log A log2 2 λ log e 2 2 λ < 205 which proves 325 If 409 < 0 8, le p be he larges prime As 409 > e 6 holds, from, for [p, p +, he funcion log Ap log2 2 λ is decreasing, which implies 330 C Cp 5

16 , by compuaion, which complees he proof of 325 ma C = ma Cp = C33647 = p<08 iii For 0 8, 326 follows from Corollary 32 We compue p 0 = he larges prime < 0 8 such ha Cp For p + 0 = < 0 8, we denoe by p he larges prime, from 330, one has C Cp < 2522, which implies 326 Then, one calculaes lim p + 0, <p+ 0 C = log p + 0 Ap 0 log2 p + 0 p λ = As he above value is < 2522, we have o solve he equaion C = 2522 for p 0 < p + 0 = find iv For he funcion log 2 / is maimal for = e 4 = 5459 where is value is 6/e 2 = 26 cf 2 As A is nondecreasing, for < 59, we have For p 59 p < p +, one has A log2 6 6 A53 = 55 = 250 e2 e2 A log2 = Ap log2 Ap log2 p p we compue he maimum of Ap log2 p p for 59 p < 0000 which is equal o 5064 for p = 3643 v Le us se f = log 2 2 λ + 52 log For 0 8, A > f follows from Corollary 3 Le p be a prime saisfying e 6 < 409 p < 0 8 For p < p +, one has A = Ap, c = log Ap log2 2 + λ, c = Aplog2 6 log 22 λ < 0 2 3/2 so ha c is decreasing c cp def == lim p +, <p + c = log p+ Ap log2 p + p λ Therefore, for 409 < 0 8 one has c min 409 p<0 8 cp, by compuaion, one ges min cp = c409 = p<08 which implies A > f The funcion f is decreasing on, = 55 ] increasing for cf [2] Therefore, for < a < b, he upper bound of f on he inerval [a, b is mafa, fb We have A84 = A83 < f84 while, for 84 < 89, A = A83 > maf84, f89 f holds For 89 p 40 = 409, one checks ha Ap > mafp, fp + holds which shows ha A > f for 89 < 409 complees he proof of 328 6

17 vi From, he funcion ϕ = log 2 / is increasing for e 4 = decreasing for e 4 so ha, for < a < b, he lower bound of ϕ on he inerval [a, b is minϕa, ϕb Le p be a prime saisfying p 83 From i, one has Ap > 0, for [p, p +, A log2 = Ap log2 Ap minϕp, ϕp + To prove 329, i remains o check ha Ap minϕp, ϕp + > 2 λ holds for 37 p Proof of Theorem Proof : The proof of 6 follows from Corollary 32 while Corollary 3 yields 7 The proof of 8 resuls of Proposiion 36, i v Inequaliy 9 resuls of Proposiion 36, v vi If 0000, Inequaliy 0 follows from Proposiion 36, iv, while for > 0000, Proposiion 36, ii, implies A log λ log which ends he proof of Theorem log λ = log 0000 log 2 Acknowledgemens I am pleased o hank Marc Deléglise for his compuaions for several discussions abou his paper References [] M Abramowiz I A Segun Hbook of Mahemaical Funcions, Dover Publicaions, Inc New-York [2] H Cohen Number Theory Volume II, Analyic modern ools, Springer, 2007 [3] P Dusar Esimaes of some funcions over primes wihou R H, cf hp://arivorg/abs/ v, 200 [4] H M Edwards Riemann s Zea funcion, Academic Press, 974 [5] A E Ingham The disribuion of prime numbers, Cambridge Mahemaical Librairy, Cambridge Universiy Press, Cambridge, 990 Reprin of he 932 original, Wih a foreword by R C Vaughan [6] E Lau Hbuch der Lehre von der Vereilung der Primzahlen, I, 2nd ed, Chelsea, New- York, 953 [7] J E Lilewood Sur la disribuion des nombres premiers C R Acad Sci Paris Sér I Mah, 58, 94, [8] D J Pla T Trudgian On he firs sign change of θ, hp://arivorg/abs/ 40794v, [9] G Robin Sur la différence Liθ π, Annales Faculé des Sciences Toulouse, 6, 984, [0] S Ramanujan Highly composie numbers, Proc London Mah Soc Serie 2, 4, 95, Colleced papers, Cambridge Universiy Press, 927, [] L Schoenfeld Sharper bounds for he Chebyshev funcions θ ψ II, Mah Comp, 30, 976, [2] hp://mahuniv-lyonfr/homes-www/~nicolas/liheahml 7

18 Jean-Louis Nicolas, Univ Lyon, Universié Claude Bernard Lyon, CNRS UMR 5208 Insiu Camille Jordan, Mahémaiques, Bâ Doyen Jean Braconnier, 43 Bd du Novembre 98, F Villeurbanne cede, France hp://mahuniv-lyonfr/homes-www/nicolas/ 8

arxiv:math/ v1 [math.nt] 3 Nov 2005

arxiv:math/ v1 [math.nt] 3 Nov 2005 arxiv:mah/0511092v1 [mah.nt] 3 Nov 2005 A NOTE ON S AND THE ZEROS OF THE RIEMANN ZETA-FUNCTION D. A. GOLDSTON AND S. M. GONEK Absrac. Le πs denoe he argumen of he Riemann zea-funcion a he poin 1 + i. Assuming

More information

A NOTE ON S(t) AND THE ZEROS OF THE RIEMANN ZETA-FUNCTION

A NOTE ON S(t) AND THE ZEROS OF THE RIEMANN ZETA-FUNCTION Bull. London Mah. Soc. 39 2007 482 486 C 2007 London Mahemaical Sociey doi:10.1112/blms/bdm032 A NOTE ON S AND THE ZEROS OF THE RIEMANN ZETA-FUNCTION D. A. GOLDSTON and S. M. GONEK Absrac Le πs denoe he

More information

An Introduction to Malliavin calculus and its applications

An Introduction to Malliavin calculus and its applications An Inroducion o Malliavin calculus and is applicaions Lecure 5: Smoohness of he densiy and Hörmander s heorem David Nualar Deparmen of Mahemaics Kansas Universiy Universiy of Wyoming Summer School 214

More information

arxiv: v1 [math.pr] 19 Feb 2011

arxiv: v1 [math.pr] 19 Feb 2011 A NOTE ON FELLER SEMIGROUPS AND RESOLVENTS VADIM KOSTRYKIN, JÜRGEN POTTHOFF, AND ROBERT SCHRADER ABSTRACT. Various equivalen condiions for a semigroup or a resolven generaed by a Markov process o be of

More information

Math 2142 Exam 1 Review Problems. x 2 + f (0) 3! for the 3rd Taylor polynomial at x = 0. To calculate the various quantities:

Math 2142 Exam 1 Review Problems. x 2 + f (0) 3! for the 3rd Taylor polynomial at x = 0. To calculate the various quantities: Mah 4 Eam Review Problems Problem. Calculae he 3rd Taylor polynomial for arcsin a =. Soluion. Le f() = arcsin. For his problem, we use he formula f() + f () + f ()! + f () 3! for he 3rd Taylor polynomial

More information

Bernoulli numbers. Francesco Chiatti, Matteo Pintonello. December 5, 2016

Bernoulli numbers. Francesco Chiatti, Matteo Pintonello. December 5, 2016 UNIVERSITÁ DEGLI STUDI DI PADOVA, DIPARTIMENTO DI MATEMATICA TULLIO LEVI-CIVITA Bernoulli numbers Francesco Chiai, Maeo Pinonello December 5, 206 During las lessons we have proved he Las Ferma Theorem

More information

The Asymptotic Behavior of Nonoscillatory Solutions of Some Nonlinear Dynamic Equations on Time Scales

The Asymptotic Behavior of Nonoscillatory Solutions of Some Nonlinear Dynamic Equations on Time Scales Advances in Dynamical Sysems and Applicaions. ISSN 0973-5321 Volume 1 Number 1 (2006, pp. 103 112 c Research India Publicaions hp://www.ripublicaion.com/adsa.hm The Asympoic Behavior of Nonoscillaory Soluions

More information

Oscillation of an Euler Cauchy Dynamic Equation S. Huff, G. Olumolode, N. Pennington, and A. Peterson

Oscillation of an Euler Cauchy Dynamic Equation S. Huff, G. Olumolode, N. Pennington, and A. Peterson PROCEEDINGS OF THE FOURTH INTERNATIONAL CONFERENCE ON DYNAMICAL SYSTEMS AND DIFFERENTIAL EQUATIONS May 4 7, 00, Wilmingon, NC, USA pp 0 Oscillaion of an Euler Cauchy Dynamic Equaion S Huff, G Olumolode,

More information

Monotonic Solutions of a Class of Quadratic Singular Integral Equations of Volterra type

Monotonic Solutions of a Class of Quadratic Singular Integral Equations of Volterra type In. J. Conemp. Mah. Sci., Vol. 2, 27, no. 2, 89-2 Monoonic Soluions of a Class of Quadraic Singular Inegral Equaions of Volerra ype Mahmoud M. El Borai Deparmen of Mahemaics, Faculy of Science, Alexandria

More information

MATH 4330/5330, Fourier Analysis Section 6, Proof of Fourier s Theorem for Pointwise Convergence

MATH 4330/5330, Fourier Analysis Section 6, Proof of Fourier s Theorem for Pointwise Convergence MATH 433/533, Fourier Analysis Secion 6, Proof of Fourier s Theorem for Poinwise Convergence Firs, some commens abou inegraing periodic funcions. If g is a periodic funcion, g(x + ) g(x) for all real x,

More information

CHARACTERIZATION OF REARRANGEMENT INVARIANT SPACES WITH FIXED POINTS FOR THE HARDY LITTLEWOOD MAXIMAL OPERATOR

CHARACTERIZATION OF REARRANGEMENT INVARIANT SPACES WITH FIXED POINTS FOR THE HARDY LITTLEWOOD MAXIMAL OPERATOR Annales Academiæ Scieniarum Fennicæ Mahemaica Volumen 31, 2006, 39 46 CHARACTERIZATION OF REARRANGEMENT INVARIANT SPACES WITH FIXED POINTS FOR THE HARDY LITTLEWOOD MAXIMAL OPERATOR Joaquim Marín and Javier

More information

Asymptotic instability of nonlinear differential equations

Asymptotic instability of nonlinear differential equations Elecronic Journal of Differenial Equaions, Vol. 1997(1997), No. 16, pp. 1 7. ISSN: 172-6691. URL: hp://ejde.mah.sw.edu or hp://ejde.mah.un.edu fp (login: fp) 147.26.13.11 or 129.12.3.113 Asympoic insabiliy

More information

arxiv: v1 [math.fa] 9 Dec 2018

arxiv: v1 [math.fa] 9 Dec 2018 AN INVERSE FUNCTION THEOREM CONVERSE arxiv:1812.03561v1 [mah.fa] 9 Dec 2018 JIMMIE LAWSON Absrac. We esablish he following converse of he well-known inverse funcion heorem. Le g : U V and f : V U be inverse

More information

Mapping Properties Of The General Integral Operator On The Classes R k (ρ, b) And V k (ρ, b)

Mapping Properties Of The General Integral Operator On The Classes R k (ρ, b) And V k (ρ, b) Applied Mahemaics E-Noes, 15(215), 14-21 c ISSN 167-251 Available free a mirror sies of hp://www.mah.nhu.edu.w/ amen/ Mapping Properies Of The General Inegral Operaor On The Classes R k (ρ, b) And V k

More information

Matrix Versions of Some Refinements of the Arithmetic-Geometric Mean Inequality

Matrix Versions of Some Refinements of the Arithmetic-Geometric Mean Inequality Marix Versions of Some Refinemens of he Arihmeic-Geomeric Mean Inequaliy Bao Qi Feng and Andrew Tonge Absrac. We esablish marix versions of refinemens due o Alzer ], Carwrigh and Field 4], and Mercer 5]

More information

THE GENERALIZED PASCAL MATRIX VIA THE GENERALIZED FIBONACCI MATRIX AND THE GENERALIZED PELL MATRIX

THE GENERALIZED PASCAL MATRIX VIA THE GENERALIZED FIBONACCI MATRIX AND THE GENERALIZED PELL MATRIX J Korean Mah Soc 45 008, No, pp 479 49 THE GENERALIZED PASCAL MATRIX VIA THE GENERALIZED FIBONACCI MATRIX AND THE GENERALIZED PELL MATRIX Gwang-yeon Lee and Seong-Hoon Cho Reprined from he Journal of he

More information

Existence Theory of Second Order Random Differential Equations

Existence Theory of Second Order Random Differential Equations Global Journal of Mahemaical Sciences: Theory and Pracical. ISSN 974-32 Volume 4, Number 3 (22), pp. 33-3 Inernaional Research Publicaion House hp://www.irphouse.com Exisence Theory of Second Order Random

More information

Some New Uniqueness Results of Solutions to Nonlinear Fractional Integro-Differential Equations

Some New Uniqueness Results of Solutions to Nonlinear Fractional Integro-Differential Equations Annals of Pure and Applied Mahemaics Vol. 6, No. 2, 28, 345-352 ISSN: 2279-87X (P), 2279-888(online) Published on 22 February 28 www.researchmahsci.org DOI: hp://dx.doi.org/.22457/apam.v6n2a Annals of

More information

Convergence of the Neumann series in higher norms

Convergence of the Neumann series in higher norms Convergence of he Neumann series in higher norms Charles L. Epsein Deparmen of Mahemaics, Universiy of Pennsylvania Version 1.0 Augus 1, 003 Absrac Naural condiions on an operaor A are given so ha he Neumann

More information

L p -L q -Time decay estimate for solution of the Cauchy problem for hyperbolic partial differential equations of linear thermoelasticity

L p -L q -Time decay estimate for solution of the Cauchy problem for hyperbolic partial differential equations of linear thermoelasticity ANNALES POLONICI MATHEMATICI LIV.2 99) L p -L q -Time decay esimae for soluion of he Cauchy problem for hyperbolic parial differenial equaions of linear hermoelasiciy by Jerzy Gawinecki Warszawa) Absrac.

More information

A Note on Goldbach Partitions of Large Even Integers

A Note on Goldbach Partitions of Large Even Integers arxiv:47.4688v3 [mah.nt] Jan 25 A Noe on Goldbach Pariions of Large Even Inegers Ljuben Muafchiev American Universiy in Bulgaria, 27 Blagoevgrad, Bulgaria and Insiue of Mahemaics and Informaics of he Bulgarian

More information

Positive continuous solution of a quadratic integral equation of fractional orders

Positive continuous solution of a quadratic integral equation of fractional orders Mah. Sci. Le., No., 9-7 (3) 9 Mahemaical Sciences Leers An Inernaional Journal @ 3 NSP Naural Sciences Publishing Cor. Posiive coninuous soluion of a quadraic inegral equaion of fracional orders A. M.

More information

23.2. Representing Periodic Functions by Fourier Series. Introduction. Prerequisites. Learning Outcomes

23.2. Representing Periodic Functions by Fourier Series. Introduction. Prerequisites. Learning Outcomes Represening Periodic Funcions by Fourier Series 3. Inroducion In his Secion we show how a periodic funcion can be expressed as a series of sines and cosines. We begin by obaining some sandard inegrals

More information

Riemann Hypothesis and Primorial Number. Choe Ryong Gil

Riemann Hypothesis and Primorial Number. Choe Ryong Gil Rieann Hyohesis Priorial Nuber Choe Ryong Gil Dearen of Maheaics Universiy of Sciences Gwahak- dong Unjong Disric Pyongyang DPRKorea Eail; ryonggilchoe@sar-conek Augus 8 5 Absrac; In his aer we consider

More information

SOME INEQUALITIES AND ABSOLUTE MONOTONICITY FOR MODIFIED BESSEL FUNCTIONS OF THE FIRST KIND

SOME INEQUALITIES AND ABSOLUTE MONOTONICITY FOR MODIFIED BESSEL FUNCTIONS OF THE FIRST KIND Commun. Korean Mah. Soc. 3 (6), No., pp. 355 363 hp://dx.doi.org/.434/ckms.6.3..355 SOME INEQUALITIES AND ABSOLUTE MONOTONICITY FOR MODIFIED BESSEL FUNCTIONS OF THE FIRST KIND Bai-Ni Guo Feng Qi Absrac.

More information

KEY. Math 334 Midterm I Fall 2008 sections 001 and 003 Instructor: Scott Glasgow

KEY. Math 334 Midterm I Fall 2008 sections 001 and 003 Instructor: Scott Glasgow 1 KEY Mah 4 Miderm I Fall 8 secions 1 and Insrucor: Sco Glasgow Please do NOT wrie on his eam. No credi will be given for such work. Raher wrie in a blue book, or on our own paper, preferabl engineering

More information

MODULE 3 FUNCTION OF A RANDOM VARIABLE AND ITS DISTRIBUTION LECTURES PROBABILITY DISTRIBUTION OF A FUNCTION OF A RANDOM VARIABLE

MODULE 3 FUNCTION OF A RANDOM VARIABLE AND ITS DISTRIBUTION LECTURES PROBABILITY DISTRIBUTION OF A FUNCTION OF A RANDOM VARIABLE Topics MODULE 3 FUNCTION OF A RANDOM VARIABLE AND ITS DISTRIBUTION LECTURES 2-6 3. FUNCTION OF A RANDOM VARIABLE 3.2 PROBABILITY DISTRIBUTION OF A FUNCTION OF A RANDOM VARIABLE 3.3 EXPECTATION AND MOMENTS

More information

Chapter 2. First Order Scalar Equations

Chapter 2. First Order Scalar Equations Chaper. Firs Order Scalar Equaions We sar our sudy of differenial equaions in he same way he pioneers in his field did. We show paricular echniques o solve paricular ypes of firs order differenial equaions.

More information

Properties Of Solutions To A Generalized Liénard Equation With Forcing Term

Properties Of Solutions To A Generalized Liénard Equation With Forcing Term Applied Mahemaics E-Noes, 8(28), 4-44 c ISSN 67-25 Available free a mirror sies of hp://www.mah.nhu.edu.w/ amen/ Properies Of Soluions To A Generalized Liénard Equaion Wih Forcing Term Allan Kroopnick

More information

6.2 Transforms of Derivatives and Integrals.

6.2 Transforms of Derivatives and Integrals. SEC. 6.2 Transforms of Derivaives and Inegrals. ODEs 2 3 33 39 23. Change of scale. If l( f ()) F(s) and c is any 33 45 APPLICATION OF s-shifting posiive consan, show ha l( f (c)) F(s>c)>c (Hin: In Probs.

More information

On Volterra Integral Equations of the First Kind with a Bulge Function by Using Laplace Transform

On Volterra Integral Equations of the First Kind with a Bulge Function by Using Laplace Transform Applied Mahemaical Sciences, Vol. 9, 15, no., 51-56 HIKARI Ld, www.m-hikari.com hp://dx.doi.org/1.1988/ams.15.41196 On Volerra Inegral Equaions of he Firs Kind wih a Bulge Funcion by Using Laplace Transform

More information

On some Properties of Conjugate Fourier-Stieltjes Series

On some Properties of Conjugate Fourier-Stieltjes Series Bullein of TICMI ol. 8, No., 24, 22 29 On some Properies of Conjugae Fourier-Sieljes Series Shalva Zviadadze I. Javakhishvili Tbilisi Sae Universiy, 3 Universiy S., 86, Tbilisi, Georgia (Received January

More information

Generalized Snell envelope and BSDE With Two general Reflecting Barriers

Generalized Snell envelope and BSDE With Two general Reflecting Barriers 1/22 Generalized Snell envelope and BSDE Wih Two general Reflecing Barriers EL HASSAN ESSAKY Cadi ayyad Universiy Poly-disciplinary Faculy Safi Work in progress wih : M. Hassani and Y. Ouknine Iasi, July

More information

SMT 2014 Calculus Test Solutions February 15, 2014 = 3 5 = 15.

SMT 2014 Calculus Test Solutions February 15, 2014 = 3 5 = 15. SMT Calculus Tes Soluions February 5,. Le f() = and le g() =. Compue f ()g (). Answer: 5 Soluion: We noe ha f () = and g () = 6. Then f ()g () =. Plugging in = we ge f ()g () = 6 = 3 5 = 5.. There is a

More information

Attractors for a deconvolution model of turbulence

Attractors for a deconvolution model of turbulence Aracors for a deconvoluion model of urbulence Roger Lewandowski and Yves Preaux April 0, 2008 Absrac We consider a deconvoluion model for 3D periodic flows. We show he exisence of a global aracor for he

More information

4 Sequences of measurable functions

4 Sequences of measurable functions 4 Sequences of measurable funcions 1. Le (Ω, A, µ) be a measure space (complee, afer a possible applicaion of he compleion heorem). In his chaper we invesigae relaions beween various (nonequivalen) convergences

More information

t is a basis for the solution space to this system, then the matrix having these solutions as columns, t x 1 t, x 2 t,... x n t x 2 t...

t is a basis for the solution space to this system, then the matrix having these solutions as columns, t x 1 t, x 2 t,... x n t x 2 t... Mah 228- Fri Mar 24 5.6 Marix exponenials and linear sysems: The analogy beween firs order sysems of linear differenial equaions (Chaper 5) and scalar linear differenial equaions (Chaper ) is much sronger

More information

2.7. Some common engineering functions. Introduction. Prerequisites. Learning Outcomes

2.7. Some common engineering functions. Introduction. Prerequisites. Learning Outcomes Some common engineering funcions 2.7 Inroducion This secion provides a caalogue of some common funcions ofen used in Science and Engineering. These include polynomials, raional funcions, he modulus funcion

More information

Fractional Method of Characteristics for Fractional Partial Differential Equations

Fractional Method of Characteristics for Fractional Partial Differential Equations Fracional Mehod of Characerisics for Fracional Parial Differenial Equaions Guo-cheng Wu* Modern Teile Insiue, Donghua Universiy, 188 Yan-an ilu Road, Shanghai 51, PR China Absrac The mehod of characerisics

More information

SELBERG S CENTRAL LIMIT THEOREM ON THE CRITICAL LINE AND THE LERCH ZETA-FUNCTION. II

SELBERG S CENTRAL LIMIT THEOREM ON THE CRITICAL LINE AND THE LERCH ZETA-FUNCTION. II SELBERG S CENRAL LIMI HEOREM ON HE CRIICAL LINE AND HE LERCH ZEA-FUNCION. II ANDRIUS GRIGUIS Deparmen of Mahemaics Informaics Vilnius Universiy, Naugarduko 4 035 Vilnius, Lihuania rius.griguis@mif.vu.l

More information

On Two Integrability Methods of Improper Integrals

On Two Integrability Methods of Improper Integrals Inernaional Journal of Mahemaics and Compuer Science, 13(218), no. 1, 45 5 M CS On Two Inegrabiliy Mehods of Improper Inegrals H. N. ÖZGEN Mahemaics Deparmen Faculy of Educaion Mersin Universiy, TR-33169

More information

Ann. Funct. Anal. 2 (2011), no. 2, A nnals of F unctional A nalysis ISSN: (electronic) URL:

Ann. Funct. Anal. 2 (2011), no. 2, A nnals of F unctional A nalysis ISSN: (electronic) URL: Ann. Func. Anal. 2 2011, no. 2, 34 41 A nnals of F uncional A nalysis ISSN: 2008-8752 elecronic URL: www.emis.de/journals/afa/ CLASSIFICAION OF POSIIVE SOLUIONS OF NONLINEAR SYSEMS OF VOLERRA INEGRAL EQUAIONS

More information

arxiv: v1 [math.fa] 19 May 2017

arxiv: v1 [math.fa] 19 May 2017 RELATIVE ENTROPY AND TSALLIS ENTROPY OF TWO ACCRETIVE OPERATORS M. RAÏSSOULI1,2, M. S. MOSLEHIAN 3, AND S. FURUICHI 4 arxiv:175.742v1 [mah.fa] 19 May 217 Absrac. Le A and B be wo accreive operaors. We

More information

Final Spring 2007

Final Spring 2007 .615 Final Spring 7 Overview The purpose of he final exam is o calculae he MHD β limi in a high-bea oroidal okamak agains he dangerous n = 1 exernal ballooning-kink mode. Effecively, his corresponds o

More information

23.5. Half-Range Series. Introduction. Prerequisites. Learning Outcomes

23.5. Half-Range Series. Introduction. Prerequisites. Learning Outcomes Half-Range Series 2.5 Inroducion In his Secion we address he following problem: Can we find a Fourier series expansion of a funcion defined over a finie inerval? Of course we recognise ha such a funcion

More information

Average Number of Lattice Points in a Disk

Average Number of Lattice Points in a Disk Average Number of Laice Poins in a Disk Sujay Jayakar Rober S. Sricharz Absrac The difference beween he number of laice poins in a disk of radius /π and he area of he disk /4π is equal o he error in he

More information

Some Ramsey results for the n-cube

Some Ramsey results for the n-cube Some Ramsey resuls for he n-cube Ron Graham Universiy of California, San Diego Jozsef Solymosi Universiy of Briish Columbia, Vancouver, Canada Absrac In his noe we esablish a Ramsey-ype resul for cerain

More information

On asymptotic behavior of composite integers n = pq Yasufumi Hashimoto

On asymptotic behavior of composite integers n = pq Yasufumi Hashimoto Journal of Mah-for-Indusry Vol1009A-6 45 49 On asymoic behavior of comosie inegers n = q Yasufumi Hashimoo Received on March 1 009 Absrac In his aer we sudy he asymoic behavior of he number of comosie

More information

Representation of Stochastic Process by Means of Stochastic Integrals

Representation of Stochastic Process by Means of Stochastic Integrals Inernaional Journal of Mahemaics Research. ISSN 0976-5840 Volume 5, Number 4 (2013), pp. 385-397 Inernaional Research Publicaion House hp://www.irphouse.com Represenaion of Sochasic Process by Means of

More information

Variational Iteration Method for Solving System of Fractional Order Ordinary Differential Equations

Variational Iteration Method for Solving System of Fractional Order Ordinary Differential Equations IOSR Journal of Mahemaics (IOSR-JM) e-issn: 2278-5728, p-issn: 2319-765X. Volume 1, Issue 6 Ver. II (Nov - Dec. 214), PP 48-54 Variaional Ieraion Mehod for Solving Sysem of Fracional Order Ordinary Differenial

More information

EXERCISES FOR SECTION 1.5

EXERCISES FOR SECTION 1.5 1.5 Exisence and Uniqueness of Soluions 43 20. 1 v c 21. 1 v c 1 2 4 6 8 10 1 2 2 4 6 8 10 Graph of approximae soluion obained using Euler s mehod wih = 0.1. Graph of approximae soluion obained using Euler

More information

Finish reading Chapter 2 of Spivak, rereading earlier sections as necessary. handout and fill in some missing details!

Finish reading Chapter 2 of Spivak, rereading earlier sections as necessary. handout and fill in some missing details! MAT 257, Handou 6: Ocober 7-2, 20. I. Assignmen. Finish reading Chaper 2 of Spiva, rereading earlier secions as necessary. handou and fill in some missing deails! II. Higher derivaives. Also, read his

More information

Example on p. 157

Example on p. 157 Example 2.5.3. Le where BV [, 1] = Example 2.5.3. on p. 157 { g : [, 1] C g() =, g() = g( + ) [, 1), var (g) = sup g( j+1 ) g( j ) he supremum is aken over all he pariions of [, 1] (1) : = < 1 < < n =

More information

On the Stability of the n-dimensional Quadratic and Additive Functional Equation in Random Normed Spaces via Fixed Point Method

On the Stability of the n-dimensional Quadratic and Additive Functional Equation in Random Normed Spaces via Fixed Point Method In. Journal of Mah. Analysis, Vol. 7, 013, no. 49, 413-48 HIKARI Ld, www.m-hikari.com hp://d.doi.org/10.1988/ijma.013.36165 On he Sabiliy of he n-dimensional Quadraic and Addiive Funcional Equaion in Random

More information

THE STORY OF LANDEN, THE HYPERBOLA AND THE ELLIPSE

THE STORY OF LANDEN, THE HYPERBOLA AND THE ELLIPSE THE STORY OF LANDEN, THE HYPERBOLA AND THE ELLIPSE VICTOR H. MOLL, JUDITH L. NOWALSKY, AND LEONARDO SOLANILLA Absrac. We esablish a relaion among he arc lenghs of a hyperbola, a circle and an ellipse..

More information

Existence of positive solution for a third-order three-point BVP with sign-changing Green s function

Existence of positive solution for a third-order three-point BVP with sign-changing Green s function Elecronic Journal of Qualiaive Theory of Differenial Equaions 13, No. 3, 1-11; hp://www.mah.u-szeged.hu/ejqde/ Exisence of posiive soluion for a hird-order hree-poin BVP wih sign-changing Green s funcion

More information

1 Review of Zero-Sum Games

1 Review of Zero-Sum Games COS 5: heoreical Machine Learning Lecurer: Rob Schapire Lecure #23 Scribe: Eugene Brevdo April 30, 2008 Review of Zero-Sum Games Las ime we inroduced a mahemaical model for wo player zero-sum games. Any

More information

arxiv: v1 [math.ca] 15 Nov 2016

arxiv: v1 [math.ca] 15 Nov 2016 arxiv:6.599v [mah.ca] 5 Nov 26 Counerexamples on Jumarie s hree basic fracional calculus formulae for non-differeniable coninuous funcions Cheng-shi Liu Deparmen of Mahemaics Norheas Peroleum Universiy

More information

Weyl sequences: Asymptotic distributions of the partition lengths

Weyl sequences: Asymptotic distributions of the partition lengths ACTA ARITHMETICA LXXXVIII.4 (999 Weyl sequences: Asympoic disribuions of he pariion lenghs by Anaoly Zhigljavsky (Cardiff and Iskander Aliev (Warszawa. Inroducion: Saemen of he problem and formulaion of

More information

A problem related to Bárány Grünbaum conjecture

A problem related to Bárány Grünbaum conjecture Filoma 27:1 (2013), 109 113 DOI 10.2298/FIL1301109B Published by Faculy of Sciences and Mahemaics, Universiy of Niš, Serbia Available a: hp://www.pmf.ni.ac.rs/filoma A problem relaed o Bárány Grünbaum

More information

Math 334 Fall 2011 Homework 11 Solutions

Math 334 Fall 2011 Homework 11 Solutions Dec. 2, 2 Mah 334 Fall 2 Homework Soluions Basic Problem. Transform he following iniial value problem ino an iniial value problem for a sysem: u + p()u + q() u g(), u() u, u () v. () Soluion. Le v u. Then

More information

Solutions from Chapter 9.1 and 9.2

Solutions from Chapter 9.1 and 9.2 Soluions from Chaper 9 and 92 Secion 9 Problem # This basically boils down o an exercise in he chain rule from calculus We are looking for soluions of he form: u( x) = f( k x c) where k x R 3 and k is

More information

On the asymptotic behavior of the pantograph equations. G. Makay and J. Terjéki

On the asymptotic behavior of the pantograph equations. G. Makay and J. Terjéki On he asympoic behavior of he panograph equaions G. Makay and J. Terjéki Bolyai Insiue, Aradi véranúk ere 1, H-6720 Szeged, Hungary Dedicaed o Professor J. Kao on his 60h birhday 1. Inroducion Our aim

More information

arxiv: v1 [math.gm] 7 Nov 2017

arxiv: v1 [math.gm] 7 Nov 2017 A TOUR ON THE MASTER FUNCTION THEOPHILUS AGAMA arxiv:7.0665v [mah.gm] 7 Nov 07 Absrac. In his aer we sudy a funcion defined on naural numbers having eacly wo rime facors. Using his funcion, we esablish

More information

Generalized Chebyshev polynomials

Generalized Chebyshev polynomials Generalized Chebyshev polynomials Clemene Cesarano Faculy of Engineering, Inernaional Telemaic Universiy UNINETTUNO Corso Viorio Emanuele II, 39 86 Roma, Ialy email: c.cesarano@unineunouniversiy.ne ABSTRACT

More information

CERTAIN CLASSES OF SOLUTIONS OF LAGERSTROM EQUATIONS

CERTAIN CLASSES OF SOLUTIONS OF LAGERSTROM EQUATIONS SARAJEVO JOURNAL OF MATHEMATICS Vol.10 (22 (2014, 67 76 DOI: 10.5644/SJM.10.1.09 CERTAIN CLASSES OF SOLUTIONS OF LAGERSTROM EQUATIONS ALMA OMERSPAHIĆ AND VAHIDIN HADŽIABDIĆ Absrac. This paper presens sufficien

More information

Research Article Existence and Uniqueness of Periodic Solution for Nonlinear Second-Order Ordinary Differential Equations

Research Article Existence and Uniqueness of Periodic Solution for Nonlinear Second-Order Ordinary Differential Equations Hindawi Publishing Corporaion Boundary Value Problems Volume 11, Aricle ID 19156, 11 pages doi:1.1155/11/19156 Research Aricle Exisence and Uniqueness of Periodic Soluion for Nonlinear Second-Order Ordinary

More information

Hamilton Jacobi equations

Hamilton Jacobi equations Hamilon Jacobi equaions Inoducion o PDE The rigorous suff from Evans, mosly. We discuss firs u + H( u = 0, (1 where H(p is convex, and superlinear a infiniy, H(p lim p p = + This by comes by inegraion

More information

A Uniform Asymptotic Estimate for Discounted Aggregate Claims with Subexponential Tails

A Uniform Asymptotic Estimate for Discounted Aggregate Claims with Subexponential Tails A Uniform Asympoic Esimae for Discouned Aggregae Claims wih Subeponenial Tails Xuemiao Hao and Qihe Tang Deparmen of Saisics and Acuarial Science The Universiy of Iowa 241 Schaeffer Hall, Iowa Ciy, IA

More information

DISCRETE GRONWALL LEMMA AND APPLICATIONS

DISCRETE GRONWALL LEMMA AND APPLICATIONS DISCRETE GRONWALL LEMMA AND APPLICATIONS JOHN M. HOLTE MAA NORTH CENTRAL SECTION MEETING AT UND 24 OCTOBER 29 Gronwall s lemma saes an inequaliy ha is useful in he heory of differenial equaions. Here is

More information

LINEAR INVARIANCE AND INTEGRAL OPERATORS OF UNIVALENT FUNCTIONS

LINEAR INVARIANCE AND INTEGRAL OPERATORS OF UNIVALENT FUNCTIONS LINEAR INVARIANCE AND INTEGRAL OPERATORS OF UNIVALENT FUNCTIONS MICHAEL DORFF AND J. SZYNAL Absrac. Differen mehods have been used in sudying he univalence of he inegral ) α ) f) ) J α, f)z) = f ) d, α,

More information

A remark on the H -calculus

A remark on the H -calculus A remark on he H -calculus Nigel J. Kalon Absrac If A, B are secorial operaors on a Hilber space wih he same domain range, if Ax Bx A 1 x B 1 x, hen i is a resul of Auscher, McInosh Nahmod ha if A has

More information

Physics 127b: Statistical Mechanics. Fokker-Planck Equation. Time Evolution

Physics 127b: Statistical Mechanics. Fokker-Planck Equation. Time Evolution Physics 7b: Saisical Mechanics Fokker-Planck Equaion The Langevin equaion approach o he evoluion of he velociy disribuion for he Brownian paricle migh leave you uncomforable. A more formal reamen of his

More information

GRADIENT ESTIMATES FOR A SIMPLE PARABOLIC LICHNEROWICZ EQUATION. Osaka Journal of Mathematics. 51(1) P.245-P.256

GRADIENT ESTIMATES FOR A SIMPLE PARABOLIC LICHNEROWICZ EQUATION. Osaka Journal of Mathematics. 51(1) P.245-P.256 Tile Auhor(s) GRADIENT ESTIMATES FOR A SIMPLE PARABOLIC LICHNEROWICZ EQUATION Zhao, Liang Ciaion Osaka Journal of Mahemaics. 51(1) P.45-P.56 Issue Dae 014-01 Tex Version publisher URL hps://doi.org/10.18910/9195

More information

BOUNDED VARIATION SOLUTIONS TO STURM-LIOUVILLE PROBLEMS

BOUNDED VARIATION SOLUTIONS TO STURM-LIOUVILLE PROBLEMS Elecronic Journal of Differenial Equaions, Vol. 18 (18, No. 8, pp. 1 13. ISSN: 17-6691. URL: hp://ejde.mah.xsae.edu or hp://ejde.mah.un.edu BOUNDED VARIATION SOLUTIONS TO STURM-LIOUVILLE PROBLEMS JACEK

More information

On R d -valued peacocks

On R d -valued peacocks On R d -valued peacocks Francis HIRSCH 1), Bernard ROYNETTE 2) July 26, 211 1) Laboraoire d Analyse e Probabiliés, Universié d Évry - Val d Essonne, Boulevard F. Mierrand, F-9125 Évry Cedex e-mail: francis.hirsch@univ-evry.fr

More information

Lecture 10: The Poincaré Inequality in Euclidean space

Lecture 10: The Poincaré Inequality in Euclidean space Deparmens of Mahemaics Monana Sae Universiy Fall 215 Prof. Kevin Wildrick n inroducion o non-smooh analysis and geomery Lecure 1: The Poincaré Inequaliy in Euclidean space 1. Wha is he Poincaré inequaliy?

More information

REMARK ON THE PAPER ON PRODUCTS OF FOURIER COEFFICIENTS OF CUSP FORMS 1. INTRODUCTION

REMARK ON THE PAPER ON PRODUCTS OF FOURIER COEFFICIENTS OF CUSP FORMS 1. INTRODUCTION REMARK ON THE PAPER ON PRODUCTS OF FOURIER COEFFICIENTS OF CUSP FORMS YUK-KAM LAU, YINGNAN WANG, DEYU ZHANG ABSTRACT. Le a(n) be he Fourier coefficien of a holomorphic cusp form on some discree subgroup

More information

Existence of positive solutions for second order m-point boundary value problems

Existence of positive solutions for second order m-point boundary value problems ANNALES POLONICI MATHEMATICI LXXIX.3 (22 Exisence of posiive soluions for second order m-poin boundary value problems by Ruyun Ma (Lanzhou Absrac. Le α, β, γ, δ and ϱ := γβ + αγ + αδ >. Le ψ( = β + α,

More information

GCD AND LCM-LIKE IDENTITIES FOR IDEALS IN COMMUTATIVE RINGS

GCD AND LCM-LIKE IDENTITIES FOR IDEALS IN COMMUTATIVE RINGS GCD AND LCM-LIKE IDENTITIES FOR IDEALS IN COMMUTATIVE RINGS D. D. ANDERSON, SHUZO IZUMI, YASUO OHNO, AND MANABU OZAKI Absrac. Le A 1,..., A n n 2 be ideals of a commuaive ring R. Le Gk resp., Lk denoe

More information

KEY. Math 334 Midterm III Winter 2008 section 002 Instructor: Scott Glasgow

KEY. Math 334 Midterm III Winter 2008 section 002 Instructor: Scott Glasgow KEY Mah 334 Miderm III Winer 008 secion 00 Insrucor: Sco Glasgow Please do NOT wrie on his exam. No credi will be given for such work. Raher wrie in a blue book, or on your own paper, preferably engineering

More information

Hamilton- J acobi Equation: Weak S olution We continue the study of the Hamilton-Jacobi equation:

Hamilton- J acobi Equation: Weak S olution We continue the study of the Hamilton-Jacobi equation: M ah 5 7 Fall 9 L ecure O c. 4, 9 ) Hamilon- J acobi Equaion: Weak S oluion We coninue he sudy of he Hamilon-Jacobi equaion: We have shown ha u + H D u) = R n, ) ; u = g R n { = }. ). In general we canno

More information

Fréchet derivatives and Gâteaux derivatives

Fréchet derivatives and Gâteaux derivatives Fréche derivaives and Gâeaux derivaives Jordan Bell jordan.bell@gmail.com Deparmen of Mahemaics, Universiy of Torono April 3, 2014 1 Inroducion In his noe all vecor spaces are real. If X and Y are normed

More information

STABILITY OF NONLINEAR NEUTRAL DELAY DIFFERENTIAL EQUATIONS WITH VARIABLE DELAYS

STABILITY OF NONLINEAR NEUTRAL DELAY DIFFERENTIAL EQUATIONS WITH VARIABLE DELAYS Elecronic Journal of Differenial Equaions, Vol. 217 217, No. 118, pp. 1 14. ISSN: 172-6691. URL: hp://ejde.mah.xsae.edu or hp://ejde.mah.un.edu STABILITY OF NONLINEAR NEUTRAL DELAY DIFFERENTIAL EQUATIONS

More information

The Existence, Uniqueness and Stability of Almost Periodic Solutions for Riccati Differential Equation

The Existence, Uniqueness and Stability of Almost Periodic Solutions for Riccati Differential Equation ISSN 1749-3889 (prin), 1749-3897 (online) Inernaional Journal of Nonlinear Science Vol.5(2008) No.1,pp.58-64 The Exisence, Uniqueness and Sailiy of Almos Periodic Soluions for Riccai Differenial Equaion

More information

Two Properties of Catalan-Larcombe-French Numbers

Two Properties of Catalan-Larcombe-French Numbers 3 7 6 3 Journal of Ineger Sequences, Vol. 9 06, Aricle 6.3. Two Properies of Caalan-Larcombe-French Numbers Xiao-Juan Ji School of Mahemaical Sciences Soochow Universiy Suzhou Jiangsu 5006 P. R. China

More information

t j i, and then can be naturally extended to K(cf. [S-V]). The Hasse derivatives satisfy the following: is defined on k(t) by D (i)

t j i, and then can be naturally extended to K(cf. [S-V]). The Hasse derivatives satisfy the following: is defined on k(t) by D (i) A NOTE ON WRONSKIANS AND THE ABC THEOREM IN FUNCTION FIELDS OF RIME CHARACTERISTIC Julie Tzu-Yueh Wang Insiue of Mahemaics Academia Sinica Nankang, Taipei 11529 Taiwan, R.O.C. May 14, 1998 Absrac. We provide

More information

POSITIVE SOLUTIONS OF NEUTRAL DELAY DIFFERENTIAL EQUATION

POSITIVE SOLUTIONS OF NEUTRAL DELAY DIFFERENTIAL EQUATION Novi Sad J. Mah. Vol. 32, No. 2, 2002, 95-108 95 POSITIVE SOLUTIONS OF NEUTRAL DELAY DIFFERENTIAL EQUATION Hajnalka Péics 1, János Karsai 2 Absrac. We consider he scalar nonauonomous neural delay differenial

More information

On the Modulus of the Selberg Zeta-Functions in the Critical Strip

On the Modulus of the Selberg Zeta-Functions in the Critical Strip Mahemaical Modelling and Analysis Publisher: Taylor&Francis and VGTU Volume X Number x, xx 0xx, 5 hp://www.andfonline.com/tmma hp://dx.doi.org/0.3846/3969.xxxx.xxxxxx ISSN: 39-69 c Vilnius Gediminas Technical

More information

1 1 + x 2 dx. tan 1 (2) = ] ] x 3. Solution: Recall that the given integral is improper because. x 3. 1 x 3. dx = lim dx.

1 1 + x 2 dx. tan 1 (2) = ] ] x 3. Solution: Recall that the given integral is improper because. x 3. 1 x 3. dx = lim dx. . Use Simpson s rule wih n 4 o esimae an () +. Soluion: Since we are using 4 seps, 4 Thus we have [ ( ) f() + 4f + f() + 4f 3 [ + 4 4 6 5 + + 4 4 3 + ] 5 [ + 6 6 5 + + 6 3 + ]. 5. Our funcion is f() +.

More information

arxiv: v1 [math.fa] 12 Jul 2012

arxiv: v1 [math.fa] 12 Jul 2012 AN EXTENSION OF THE LÖWNER HEINZ INEQUALITY MOHAMMAD SAL MOSLEHIAN AND HAMED NAJAFI arxiv:27.2864v [ah.fa] 2 Jul 22 Absrac. We exend he celebraed Löwner Heinz inequaliy by showing ha if A, B are Hilber

More information

BBP-type formulas, in general bases, for arctangents of real numbers

BBP-type formulas, in general bases, for arctangents of real numbers Noes on Number Theory and Discree Mahemaics Vol. 19, 13, No. 3, 33 54 BBP-ype formulas, in general bases, for arcangens of real numbers Kunle Adegoke 1 and Olawanle Layeni 2 1 Deparmen of Physics, Obafemi

More information

On Gronwall s Type Integral Inequalities with Singular Kernels

On Gronwall s Type Integral Inequalities with Singular Kernels Filoma 31:4 (217), 141 149 DOI 1.2298/FIL17441A Published by Faculy of Sciences and Mahemaics, Universiy of Niš, Serbia Available a: hp://www.pmf.ni.ac.rs/filoma On Gronwall s Type Inegral Inequaliies

More information

Cash Flow Valuation Mode Lin Discrete Time

Cash Flow Valuation Mode Lin Discrete Time IOSR Journal of Mahemaics (IOSR-JM) e-issn: 2278-5728,p-ISSN: 2319-765X, 6, Issue 6 (May. - Jun. 2013), PP 35-41 Cash Flow Valuaion Mode Lin Discree Time Olayiwola. M. A. and Oni, N. O. Deparmen of Mahemaics

More information

arxiv:math/ v1 [math.ca] 16 Jun 2003

arxiv:math/ v1 [math.ca] 16 Jun 2003 THE BEST BOUNDS OF HARMONIC SEQUENCE arxiv:mah/62v mah.ca] 6 Jun 2 CHAO-PING CHEN AND FENG QI Absrac. For any naural number n N, n 2n+ γ 2 i lnn γ < 2n+, i where γ.5772566495286 denoes Euler s consan.

More information

On Oscillation of a Generalized Logistic Equation with Several Delays

On Oscillation of a Generalized Logistic Equation with Several Delays Journal of Mahemaical Analysis and Applicaions 253, 389 45 (21) doi:1.16/jmaa.2.714, available online a hp://www.idealibrary.com on On Oscillaion of a Generalized Logisic Equaion wih Several Delays Leonid

More information

On composite integers n for which ϕ(n) n 1

On composite integers n for which ϕ(n) n 1 On composie inegers n for which ϕn) n Florian Luca Insiuo de Maemáicas Universidad Nacional Auonoma de México C.P. 58089, Morelia, Michoacán, México fluca@mamor.unam.mx Carl Pomerance Deparmen of Mahemaics

More information

Ramanujan and Euler's Constant

Ramanujan and Euler's Constant Proceedings of Symposia in Applied Mahemaics Volume 00, 0000 Ramanujan and Euler's Consan RICHARD P. BRENT Absrac. We consider Ramanujan's conribuion o formulas for Euler's consan. For eample, in his second

More information

Sobolev-type Inequality for Spaces L p(x) (R N )

Sobolev-type Inequality for Spaces L p(x) (R N ) In. J. Conemp. Mah. Sciences, Vol. 2, 27, no. 9, 423-429 Sobolev-ype Inequaliy for Spaces L p(x ( R. Mashiyev and B. Çekiç Universiy of Dicle, Faculy of Sciences and Ars Deparmen of Mahemaics, 228-Diyarbakir,

More information

Homework sheet Exercises done during the lecture of March 12, 2014

Homework sheet Exercises done during the lecture of March 12, 2014 EXERCISE SESSION 2A FOR THE COURSE GÉOMÉTRIE EUCLIDIENNE, NON EUCLIDIENNE ET PROJECTIVE MATTEO TOMMASINI Homework shee 3-4 - Exercises done during he lecure of March 2, 204 Exercise 2 Is i rue ha he parameerized

More information