On the cohomology groups of certain quotients of products of upper half planes and upper half spaces

Size: px
Start display at page:

Download "On the cohomology groups of certain quotients of products of upper half planes and upper half spaces"

Transcription

1 On he cohomolog groups of cerain quoiens of producs of upper half planes and upper half spaces Amod Agashe and Ldia Eldredge Absrac A heorem of Masushima-Shimura shows ha he he space of harmonic differenial forms on he quoien of producs of upper half planes under he acion of cerain groups, when he quoien is compac, is he direc sum of wo subspaces called he universal and cuspidal subspaces. We generalize his resul o compac quoiens of producs of upper half planes and upper half spaces (hperbolic hree spaces under he acion of cerain groups o obain a similar decomposiion. 1 Inroducion and main resul Le n be a posiive ineger. For i = 1,..., n, le H i be eiher he upper half plane H 2 = {z C : I(z > 0} or upper half space H 3 = C R >0 (a model for hperbolic hree space, and le C i = R if H i is he upper half plane and C i = C if H i is upper half space. The group SL 2 (R acs on H 2 as usual b fracional linear ransformaions and he acion of SL 2 (C on H 3 is given b [ ] a b (z, = 1 c d δ ((az + b(cz + d + ac2, ad bc, where δ = cz + d 2 + c 2. Le Γ be a subgroup of n i=1 SL 2(C i, which hus acs on n i=1 H i. For i = 1,..., n, if H i is he upper half plane, hen le x i and i denoe he x and coordinaes on H i (i.e., for which he corresponding poin is x i + 1 i, and if H i is he upper half space, hen le x i, i and i denoe he x,, and coordinaes on H i (i.e., for which he corresponding poin is (x i + 1 i, i. The sandard Riemannian merics on he upper half plane and upper half space induce a meric (he produc meric on n i=1 H i. For i = 1,..., n, le η i denoe he volume form (also called fundamenal form on H i, i.e., if H i is he upper half plane, hen η i = dx i / i d i / i, and if H i is he upper half space, hen η i = dx i / i d i / i d i / i. If C {1,..., n}, hen le η C = i C η i. Noe ha η C is invarian under n i=1 SL 2(C i. For i = 1,..., n, le d i = 2 if H i is he upper half plane, hen le d i = 3 if H i is he upper half space. Define { H m C {1,...,n}: univ = Rη C, if m = 2i + 3j for some inegers i and j i C d i =m 0 oherwise Noe ha if H i is he upper half plane for all i, hen H m univ C is isomorphic o he usual universal cohomolog group associaed o Γ of degree m (e.g., see [Fre90, III.1]. Le H m (Γ denoe he group of harmonic differenial forms of degree m on n i=1 H i ha are invarian wih respec o Γ. Since he volume form on an H i is harmonic, H m univ H m (Γ. The firs auhor was pariall suppored b he Collaboraion Grans for Mahemaicians from he Simons Foundaion (award number

2 Now assume ha Γ is discree in n i=1 SL 2(C i, has no elemen of finie order oher han he ideni, and is such ha he quoien b is acion on n i=1 H i is compac. For i = 1,..., n, if H i is he upper half plane, hen le B i = {dx i / i, d i / i }, and if H i is he upper half space, hen le B i = {dx i / i, d i / i, d i / i }. For an i, if A i B i, hen le ω Ai = ω Ai ω. If a 1,..., a n are inegers, hen we sa ha a differenial form is of pe a 1,..., a n if i can be wrien as a linear combinaion (wih coefficiens being smooh funcions of some ω A1 ω An, such ha for each i, A i B i and A i = a i. Le H m cusp denoe he subgroup of H m (Γ generaed b elemens ha are of pe a 1,..., a n such ha none of he a i are equal o 0 or d i (noe ha i a i = m necessaril. Assume now ha he image of Γ under he projecion o an parial produc of n i=1 SL 2(C i is dense; his is called an irreducibili condiion in [Fre90, I.2.13] (cf. p of [MS63], and is ofen rue for arihmeic subgroups if n > 1. Theorem 1.1. We have H m (Γ = H m univ + H m cusp and H m univ H m cusp = {0}. Hence H m (Γ, R = H m( Γ\( n i=1 H i, R ( = H m dr Γ\( n i=1 H i, R = H m (Γ = H m univ Hcusp, m where he firs cohomolog is group cohomolog, he second one is Bei cohomolog, and he hird one is derham cohomolog. Noe ha he firs hree isomorphisms in he second saemen are sandard, and for his reason, his saemen follows from he firs. The proof of he firs saemen is given in he nex secion. If H i is he upper half plane for all i, hen he saemen of he heorem, when ensored wih C, follows from [MS63] (cf. Theorem 1.6 in Chaper III of [Fre90]. The proof given in loc. ci. (see also [Fre90, III.1] for an exposiion uses cruciall he fac ha here is a basis of complex differenial forms on he upper half plane for which he acion of SL 2 (R is diagonal (e.g., one such basis is {dz, dz}, where z denoes he coordinae on he upper half plane; his does no seem o be rue for upper half space (as far as we know, and so he proof of [MS63] does no generalize in an obvious wa o our siuaion. While our proof does borrow ideas from loc. ci., even in he case where H i is he upper half plane for all i, i differs from he one in loc. ci. and is more elemear, in he sense ha he proof in loc. ci. uses he maximum principle for harmonic funcions, while we jus use he fac ha harmonic forms on compac manifolds are closed. Moreover, we ge a resul wih coefficiens in R, as opposed o in C, so our resul is more general as well. The moivaion for he auhors o generalize he resul of Masushima-Shimura (o include upper half spaces is for a poenial applicaion o he consrucion of Sark-Heegner poins (also called Darmon poins on ellipic curves over arbirar number fields (he case of oall real fields is considered in [AT]; for an example of he applicaion of he original heorem of Masushima- Shimura in his conex, see he proof of Theorem 8.9 on p. 92 of [Dar04]. Acknowledgemen: We are ver graeful o E. Aldrovandi for several discussions and advice on work ha led o his aricle. 2 Proof of Theorem 1.1 We coninue o use he noaion inroduced in he previous secion. If ω is a differenial form, hen i can be wrien uniquel as ω = α S ω α where S is some finie indexing se and he ω α s are non-rivial forms of disinc pes. The Laplacian operaor and an elemen of Γ ake a form of a given pe o a form of he same pe. Thus if ω as above is an invarian harmonic form, hen each ω α is also an invarian harmonic form (here and henceforh, when we sa ha a form is 2

3 invarian, we shall mean wih respec o he full group Γ. Thus i suffices o show ha a nonzero harmonic invarian differenial form of a given pe is eiher in H m univ or in H m cusp, bu no in boh. Proposiion 2.1. Le ω be a nonzero invarian harmonic form of pe a 1,..., a n for some a 1,..., a n. Suppose here is an i such ha a i = 0 or d i. Then for all j, a j = 0 or d j, and ω is a real number imes n j=1 b j, where b j = 1 if a j = 0, and b j = η j (he volume form on H j if a j = d j. We shall prove his proposiion nex, bu noe ha i immediael implies he heorem, since if a harmonic invarian form is of a pe where a i = 0 or d i for some i, hen b he proposiion above, i is in Huniv, m and if no, hen i is in Hcusp, m which proves he firs saemen of he heorem (as menioned earlier, he second saemen follows from he firs. The res of his secion is devoed o he proof of Proposiion 2.1. Wihou loss of generali, assume ha i = 1, where i is as in he saemen of he proposiion. For some finie se I, one can wrie ω uniquel as ω = k I f kω k such ha ω k = ω A1 ω An for some A i B i wih A i = a i for all i = 1,..., n and wih he requiremen ha he ω k s are disinc and f k s are nonzero smooh funcions. Le x i denoe (x i, i if H i is he upper half plane and x i = (x i, i, i if H i is he upper half space. Lemma 2.2. For each k I, f k is independen of x 1 (i.e., independen of he variables in x 1. Proof. Le X denoe he quoien of n i=1 H i under he acion of Γ; under our assumpions, i is a compac Riemannian manifold wihou boundar. If ω is a form on n i=1 H i ha is invarian under Γ, hen i induces a form on X ha we shall denoe b ω. We define an inner produc on p-forms on n i=1 H i ha are invarian under Γ b (ω 1, ω 2 = X ω 1 ω 2, where he laer inegral is well defined since X is compac. Wih his inner produc, he usual proof ha a harmonic form on a compac Riemannian manifold is closed generalizes o show ha a harmonic form on n i=1 H i ha is invarian under Γ is closed (as was poined ou o us b E. Klassen, his also follows because i is a local resul, which holds on he quoien since i is compac. Since ω is harmonic, we have dω = 0. We remark ha his is he onl place in his aricle where we use he hpohesis ha he quoien X is compac. Consider firs he case where a 1 = 0. Then noe ha for each k I, ω k = ω A2 ω An for some A 2 B 2,..., A n B n (he ω A1 is missing since a 1 = 0. For i = 1,..., n, if H i is he upper half plane, hen le B i = {dx i, d i }, and if H i is he upper half space, hen le B i = {dx i, d i, d i } (hus B i is a differen basis for he span of B i. Now, wih I as above, one can wrie ω uniquel as ω = k I g kω k such ha ω k = ω A ω A 2 for some n A i B i wih A i = a i for all i and wih he requiremen ha he ω k s are disinc, g k s are nonzero smooh funcions, and g k ω k = f kω k (we are jus doing a change of basis here. We have 0 = dω = g k k I b B 1 b db ω k + n g k k I i=2 b B i b db ω k. Now each erm in he firs sum conains db for some b B 1, while he erms in he second sum do no conain db for an b B 1 (considering he wa in which ω k could be wrien in he paragraph above, so he firs sum mus be zero. Secondl, in he firs sum, for each b B 1, he db ω k s are disinc for he various k s, so we conclude ha for all k, g k / b = 0 for all b B 1, i.e., g k is independen of x 1. Now for each k, f k differs from g k b n i=2 c i, where c i is a power of i if H i is he upper half planes and c i is a power of i if H i is he upper half space; his produc n i=2 c i is non-zero and is independen of x 1. Thus for each k, f k is also independen of x 1. Now consider he case where a 1 = d 1. Then ω is also invarian and harmonic, and for i, he corresponding a 1 is 0, while he se of f k s do no change up o signs. Thus he argumen above applied o ω shows ha he f k s are independen of x 1 in his case also. 3

4 Now suppose here is a j such ha a j is neiher 0 nor d i. We will show ha his leads o a conradicion. Wihou loss of generali, suppose j = 2. Le M SL 2 (C 2 (recall ha C 2 = R if H 2 is he upper half plane and C 2 = C if H 2 is he upper half space. Then b he irreducibili condiion, for some marix A SL 2 (C 1 ha depends on M, here are elemens of Γ ha are arbiraril close o (A, M, I,..., I, where I is he ideni marix, as usual. Now ω is invarian wih respec o he firs componen (i.e., wih respec o all possible A s as above; here, if a 1 = d 1, we use he fac ha he volume form is invarian under SL 2 (C 1. Since ω is smooh, b pulling back ω o H 2, we ge a harmonic differenial form ω on H 2 or on H 3 ha is invarian under M and is no of degree zero or he op degree (which is 2 for H 2 and 3 for H 3. I is perhaps well known ha his canno happen for all such M (and in fac, his ma follow from a more general fac, bu we prove his anwa for he sake of compleeness: Lemma 2.3. There is no nonzero harmonic differenial form on H 2 or on H 3 ha is invarian under SL 2 (R or SL 2 (C respecivel and is of degree oher han zero or he op degree (which is 2 for H 2 and 3 for H 3. Proof. Assume ha a form ω of he pe above acuall exiss. Firs consider he case of H 2. Then ω is of degree one and so ω = f dz d z + g( for some f(z and g(z. A direc calculaion shows ha if P 1 = (x 1, 1 and P 2 = (x 2, 2 are poins in H 2, hen wih e = x 2 x and d = 1 2, he marix [ 1 ] M = d ed SL 0 d 2 (R (1 [ ] a b saisfies M(P 1 = P 2. The acion of he marix SL c d 2 (R on complex differenials in he basis ( dz, d z is given b he marix [ ] ɛ ɛ 2, where ɛ = (cz + d/ cz + d. (2 Using his, one sees ha he marix in (1 leaves dz d z and invarian (keeping in mind ha d > 0. Since ω is invarian under SL 2 (R, we conclude ha f(z and g(z are consans. Now consider he following marix γ = [ ] 0 1 SL (R Since f(z and g(z are consans, we shall wrie hem as jus f and g respecivel. Then ( dz ( f + g d z = γ ( f dz ( + g d z = fγ ( dz + gγ ( d z = f z 2 dz z 2 + g z2 ( z 2 d z, where we used formula (2 above in he las sep. Puing z = i (for example in he equaion above, we see ha f = g = 0 and so ω = 0, which is a conradicion. Now consider he case of H 3. Firs consider he case where he degree of ω is one. Le β 0 = dz/, β 1 = d/, and β 2 = dz/. Then ω = f 0 β 0 + f 1 β 1 + f 2 β 2 for some funcions f 0, f 1, and f 2. A direc calculaion shows ha if P 1 = (x 1, 1, 1 and P 2 = (x 2, 2, 2 are poins in H 3, hen wih z 1 = x 1 + i 1, z 2 = x 2 + i 2, e = z 2 z 2 1 1, and d = 1 2, he marix [ 1 ] M = d ed SL 0 d 2 (C (3 4

5 [ ] a b saisfies M(P 1 = P 2. The acion of he marix SL c d 2 (C on complex differenials in he basis (β 0, β 1, β 2 is given b he marix r 1 2 2rs s 2 r 2 + s 2 rs r 2 s 2 rs, where = ad bc = 1, r = cz + d, and s = c. (4 s 2 2rs r 2 Using his, one sees ha he marix in (3 leaves each of β 0, β 1, and β 2 invarian (considering ha d is real. Since ω is invarian under SL 2 (C, we conclude ha f 0, f 1, and f 2 are consans. I is eas o check ha β 0 = iβ 1 β 2, β 1 = i 2 β 2 β 0, and β 2 = iβ 0 β 1, and ha dβ 0 = β 0 β 1, dβ 1 = 0, and dβ 2 = β 2 β 1 (see, e.g., he proof of Lemma 61 in of [Bg99]. Using hese formulas, and he fac ha ω is harmonic, we have 0 = ω = (dδ + δdω = dδ(f 0 β 0 + f 1 β 1 + f 2 β 2 + δd(f 0 β 0 + f 1 β 1 + f 2 β 2 = d(( 1 3(1+1+1 d (f 0 β 0 + f 1 β 1 + f 2 β 2 + δ(f 0 β 0 β f 2 β 2 β 1 = d d(if 0 β 1 β 2 + i 2 f 1β 2 β 0 + if 2 β 0 β 1 + ( 1 3(2+1+1 d (f 0 β 0 β 1 + f 2 β 2 β 1 = d (0 + i 2 f 1( 2β 0 β 1 β d(f 0 (iβ 2 + f 2 ( iβ 0 = d (if 1 β 0 β 1 β 2 + d(f 0 iβ 2 f 2 iβ 0 = d( if 1 (2i + (f 0 iβ 2 β 1 f 2 iβ 0 β 1 = d(2f 1 f 0 i( iβ 0 + f 2 i(iβ 2 = 0 f 0 iβ 0 f 2 β 2 I follows ha f 0 = f 2 = 0. Recall ha f 1 is a consan. Le [ ] 0 1 γ = SL (C. Then f 1 β 1 = ω = γ (ω = γ (f 1 β 1 = f 1 γ (β 1 = f 1 1 z ( 2zβ 0 + ( z 2 2 β 1 + 2zβ 2, where we used formula (4 above in he las sep. Puing z = 0, = 1 in he equaion above, we see ha f 1 = 0 and so ω = 0, which is a conradicion. If he degree of ω is 2, hen ω is a non-zero harmonic form of degree one ha is invarian under SL 2 (C. Thus from he argumen above, we again ge a conradicion. Thus, for all j, a j = 0 or d j. Then one sees ha I consiss of onl one elemen k (since he dimension of he space of forms of degree 0 or d j is one for each j, and appling Lemma 2.2 above for an j insead of for i = 1, we see ha f k is indepeden of x j for all j. Thus f k is a real number. This finishes he proof of Proposiion 2.1. Remark 2.4. We ake he opporuni o poin ou a correcion o he lieraure (his remark and he res of his aricle are independen of each oher. Recall ha H 3 = C R >0 is he upper half space (a model for hperbolic hree space. Le f 0, f 1, andf 2 be smooh funcions on H 3. I has been wrongl saed in he lieraure ha ω = f 0 ( dz/ + f 1 d/ + f 2 dz/ is harmonic if and 5

6 onl if f 0 z + f 2 z = 0, f 1 z + f 0 1 f 0 = 0, f 1 z f f 2 = 0, f 1 2 f 1 2 f 0 z = 0 (5 The ssem of equaions above is equivalen o saing ha ω is closed and coclosed (e.g., see he proof of Lemma 61 in of [Bg99]. On a compac manifold, a differenial form is harmonic if and onl if i is closed and coclosed. However H 3 is no compac. Now ( d δ ( d = ( 1 3(1+1+1 d d ( dx = d d ( 1 = d 2 dx d ( = 2 1 ( d 3 d dx d = 2 dx d = 2 1 = 2, and ( d ( d ( d ( 1 = (δd + dδ = δd + dδ = δ 2 d d + d(2 = = 0. Thus he differenial d/ is harmonic, bu no coclosed. I does no saisf equaion (5 above (in our case, f 1 = 1 and f 0 = 0. I also follows ha ( d is harmonic, bu no closed. References [AT] Amod Agashe and Mak Trifkovic, Darmon poins for oall real fields, submied, available a arxiv: [Bg99] J. Bgo, Modular forms and modular smbols over imaginar quadraic fields, Ph.D. hesis, Exeer (1999, available a hp://hdl.handle.ne/10871/8322. [Dar04] Henri Darmon, Raional poins on modular ellipic curves, CBMS Regional Conference Series in Mahemaics, vol. 101, Published for he Conference Board of he Mahemaical Sciences, Washingon, DC, MR (2004k:11103 [Fre90] Eberhard Freiag, Hilber modular forms, Springer-Verlag, Berlin, MR (91c:11025 [MS63] Yozô Masushima and Goro Shimura, On he cohomolog groups aached o cerain vecor valued differenial forms on he produc of he upper half planes, Ann. of Mah. (2 78 (1963, MR (27 #5274 6

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

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

ODEs II, Lecture 1: Homogeneous Linear Systems - I. Mike Raugh 1. March 8, 2004

ODEs II, Lecture 1: Homogeneous Linear Systems - I. Mike Raugh 1. March 8, 2004 ODEs II, Lecure : Homogeneous Linear Sysems - I Mike Raugh March 8, 4 Inroducion. In he firs lecure we discussed a sysem of linear ODEs for modeling he excreion of lead from he human body, saw how o ransform

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

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

10. State Space Methods

10. State Space Methods . Sae Space Mehods. Inroducion Sae space modelling was briefly inroduced in chaper. Here more coverage is provided of sae space mehods before some of heir uses in conrol sysem design are covered in he

More information

Second Order Linear Differential Equations

Second Order Linear Differential Equations Second Order Linear Differenial Equaions Second order linear equaions wih consan coefficiens; Fundamenal soluions; Wronskian; Exisence and Uniqueness of soluions; he characerisic equaion; soluions of homogeneous

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

Inventory Analysis and Management. Multi-Period Stochastic Models: Optimality of (s, S) Policy for K-Convex Objective Functions

Inventory Analysis and Management. Multi-Period Stochastic Models: Optimality of (s, S) Policy for K-Convex Objective Functions Muli-Period Sochasic Models: Opimali of (s, S) Polic for -Convex Objecive Funcions Consider a seing similar o he N-sage newsvendor problem excep ha now here is a fixed re-ordering cos (> 0) for each (re-)order.

More information

Math 334 Test 1 KEY Spring 2010 Section: 001. Instructor: Scott Glasgow Dates: May 10 and 11.

Math 334 Test 1 KEY Spring 2010 Section: 001. Instructor: Scott Glasgow Dates: May 10 and 11. 1 Mah 334 Tes 1 KEY Spring 21 Secion: 1 Insrucor: Sco Glasgow Daes: Ma 1 and 11. Do NOT wrie on his problem saemen bookle, excep for our indicaion of following he honor code jus below. No credi will be

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

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

Notes for Lecture 17-18

Notes for Lecture 17-18 U.C. Berkeley CS278: Compuaional Complexiy Handou N7-8 Professor Luca Trevisan April 3-8, 2008 Noes for Lecure 7-8 In hese wo lecures we prove he firs half of he PCP Theorem, he Amplificaion Lemma, up

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

FREE ODD PERIODIC ACTIONS ON THE SOLID KLEIN BOTTLE

FREE ODD PERIODIC ACTIONS ON THE SOLID KLEIN BOTTLE An-Najah J. Res. Vol. 1 ( 1989 ) Number 6 Fawas M. Abudiak FREE ODD PERIODIC ACTIONS ON THE SOLID LEIN BOTTLE ey words : Free acion, Periodic acion Solid lein Bole. Fawas M. Abudiak * V.' ZZ..).a11,L.A.;15TY1

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

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

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

Undetermined coefficients for local fractional differential equations

Undetermined coefficients for local fractional differential equations Available online a www.isr-publicaions.com/jmcs J. Mah. Compuer Sci. 16 (2016), 140 146 Research Aricle Undeermined coefficiens for local fracional differenial equaions Roshdi Khalil a,, Mohammed Al Horani

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

Course Notes for EE227C (Spring 2018): Convex Optimization and Approximation

Course Notes for EE227C (Spring 2018): Convex Optimization and Approximation Course Noes for EE7C Spring 018: Convex Opimizaion and Approximaion Insrucor: Moriz Hard Email: hard+ee7c@berkeley.edu Graduae Insrucor: Max Simchowiz Email: msimchow+ee7c@berkeley.edu Ocober 15, 018 3

More information

Chapter 6. Systems of First Order Linear Differential Equations

Chapter 6. Systems of First Order Linear Differential Equations Chaper 6 Sysems of Firs Order Linear Differenial Equaions We will only discuss firs order sysems However higher order sysems may be made ino firs order sysems by a rick shown below We will have a sligh

More information

t 2 B F x,t n dsdt t u x,t dxdt

t 2 B F x,t n dsdt t u x,t dxdt Evoluion Equaions For 0, fixed, le U U0, where U denoes a bounded open se in R n.suppose ha U is filled wih a maerial in which a conaminan is being ranspored by various means including diffusion and convecion.

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

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

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

Two Coupled Oscillators / Normal Modes

Two Coupled Oscillators / Normal Modes Lecure 3 Phys 3750 Two Coupled Oscillaors / Normal Modes Overview and Moivaion: Today we ake a small, bu significan, sep owards wave moion. We will no ye observe waves, bu his sep is imporan in is own

More information

Math 315: Linear Algebra Solutions to Assignment 6

Math 315: Linear Algebra Solutions to Assignment 6 Mah 35: Linear Algebra s o Assignmen 6 # Which of he following ses of vecors are bases for R 2? {2,, 3, }, {4,, 7, 8}, {,,, 3}, {3, 9, 4, 2}. Explain your answer. To generae he whole R 2, wo linearly independen

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

SOME MORE APPLICATIONS OF THE HAHN-BANACH THEOREM

SOME MORE APPLICATIONS OF THE HAHN-BANACH THEOREM SOME MORE APPLICATIONS OF THE HAHN-BANACH THEOREM FRANCISCO JAVIER GARCÍA-PACHECO, DANIELE PUGLISI, AND GUSTI VAN ZYL Absrac We give a new proof of he fac ha equivalen norms on subspaces can be exended

More information

Chapter 3 Boundary Value Problem

Chapter 3 Boundary Value Problem Chaper 3 Boundary Value Problem A boundary value problem (BVP) is a problem, ypically an ODE or a PDE, which has values assigned on he physical boundary of he domain in which he problem is specified. Le

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

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

1 Solutions to selected problems

1 Solutions to selected problems 1 Soluions o seleced problems 1. Le A B R n. Show ha in A in B bu in general bd A bd B. Soluion. Le x in A. Then here is ɛ > 0 such ha B ɛ (x) A B. This shows x in B. If A = [0, 1] and B = [0, 2], hen

More information

BOUNDEDNESS OF MAXIMAL FUNCTIONS ON NON-DOUBLING MANIFOLDS WITH ENDS

BOUNDEDNESS OF MAXIMAL FUNCTIONS ON NON-DOUBLING MANIFOLDS WITH ENDS BOUNDEDNESS OF MAXIMAL FUNCTIONS ON NON-DOUBLING MANIFOLDS WITH ENDS XUAN THINH DUONG, JI LI, AND ADAM SIKORA Absrac Le M be a manifold wih ends consruced in [2] and be he Laplace-Belrami operaor on M

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

Section 3.5 Nonhomogeneous Equations; Method of Undetermined Coefficients

Section 3.5 Nonhomogeneous Equations; Method of Undetermined Coefficients Secion 3.5 Nonhomogeneous Equaions; Mehod of Undeermined Coefficiens Key Terms/Ideas: Linear Differenial operaor Nonlinear operaor Second order homogeneous DE Second order nonhomogeneous DE Soluion o homogeneous

More information

SOLUTIONS TO ECE 3084

SOLUTIONS TO ECE 3084 SOLUTIONS TO ECE 384 PROBLEM 2.. For each sysem below, specify wheher or no i is: (i) memoryless; (ii) causal; (iii) inverible; (iv) linear; (v) ime invarian; Explain your reasoning. If he propery is no

More information

A Necessary and Sufficient Condition for the Solutions of a Functional Differential Equation to Be Oscillatory or Tend to Zero

A Necessary and Sufficient Condition for the Solutions of a Functional Differential Equation to Be Oscillatory or Tend to Zero JOURNAL OF MAEMAICAL ANALYSIS AND APPLICAIONS 24, 7887 1997 ARICLE NO. AY965143 A Necessary and Sufficien Condiion for he Soluions of a Funcional Differenial Equaion o Be Oscillaory or end o Zero Piambar

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

Boundedness and Stability of Solutions of Some Nonlinear Differential Equations of the Third-Order.

Boundedness and Stability of Solutions of Some Nonlinear Differential Equations of the Third-Order. Boundedness Sabili of Soluions of Some Nonlinear Differenial Equaions of he Third-Order. A.T. Ademola, M.Sc. * P.O. Arawomo, Ph.D. Deparmen of Mahemaics Saisics, Bowen Universi, Iwo, Nigeria. Deparmen

More information

11!Hí MATHEMATICS : ERDŐS AND ULAM PROC. N. A. S. of decomposiion, properly speaking) conradics he possibiliy of defining a counably addiive real-valu

11!Hí MATHEMATICS : ERDŐS AND ULAM PROC. N. A. S. of decomposiion, properly speaking) conradics he possibiliy of defining a counably addiive real-valu ON EQUATIONS WITH SETS AS UNKNOWNS BY PAUL ERDŐS AND S. ULAM DEPARTMENT OF MATHEMATICS, UNIVERSITY OF COLORADO, BOULDER Communicaed May 27, 1968 We shall presen here a number of resuls in se heory concerning

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

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

Echocardiography Project and Finite Fourier Series

Echocardiography Project and Finite Fourier Series Echocardiography Projec and Finie Fourier Series 1 U M An echocardiagram is a plo of how a porion of he hear moves as he funcion of ime over he one or more hearbea cycles If he hearbea repeas iself every

More information

Congruent Numbers and Elliptic Curves

Congruent Numbers and Elliptic Curves Congruen Numbers and Ellipic Curves Pan Yan pyan@oksaeedu Sepember 30, 014 1 Problem In an Arab manuscrip of he 10h cenury, a mahemaician saed ha he principal objec of raional righ riangles is he following

More information

The expectation value of the field operator.

The expectation value of the field operator. The expecaion value of he field operaor. Dan Solomon Universiy of Illinois Chicago, IL dsolom@uic.edu June, 04 Absrac. Much of he mahemaical developmen of quanum field heory has been in suppor of deermining

More information

NEW EXAMPLES OF CONVOLUTIONS AND NON-COMMUTATIVE CENTRAL LIMIT THEOREMS

NEW EXAMPLES OF CONVOLUTIONS AND NON-COMMUTATIVE CENTRAL LIMIT THEOREMS QUANTUM PROBABILITY BANACH CENTER PUBLICATIONS, VOLUME 43 INSTITUTE OF MATHEMATICS POLISH ACADEMY OF SCIENCES WARSZAWA 998 NEW EXAMPLES OF CONVOLUTIONS AND NON-COMMUTATIVE CENTRAL LIMIT THEOREMS MAREK

More information

Predator - Prey Model Trajectories and the nonlinear conservation law

Predator - Prey Model Trajectories and the nonlinear conservation law Predaor - Prey Model Trajecories and he nonlinear conservaion law James K. Peerson Deparmen of Biological Sciences and Deparmen of Mahemaical Sciences Clemson Universiy Ocober 28, 213 Ouline Drawing Trajecories

More information

Physics 235 Chapter 2. Chapter 2 Newtonian Mechanics Single Particle

Physics 235 Chapter 2. Chapter 2 Newtonian Mechanics Single Particle Chaper 2 Newonian Mechanics Single Paricle In his Chaper we will review wha Newon s laws of mechanics ell us abou he moion of a single paricle. Newon s laws are only valid in suiable reference frames,

More information

14 Autoregressive Moving Average Models

14 Autoregressive Moving Average Models 14 Auoregressive Moving Average Models In his chaper an imporan parameric family of saionary ime series is inroduced, he family of he auoregressive moving average, or ARMA, processes. For a large class

More information

Clarke s Generalized Gradient and Edalat s L-derivative

Clarke s Generalized Gradient and Edalat s L-derivative 1 21 ISSN 1759-9008 1 Clarke s Generalized Gradien and Edala s L-derivaive PETER HERTLING Absrac: Clarke [2, 3, 4] inroduced a generalized gradien for real-valued Lipschiz coninuous funcions on Banach

More information

MATH 5720: Gradient Methods Hung Phan, UMass Lowell October 4, 2018

MATH 5720: Gradient Methods Hung Phan, UMass Lowell October 4, 2018 MATH 5720: Gradien Mehods Hung Phan, UMass Lowell Ocober 4, 208 Descen Direcion Mehods Consider he problem min { f(x) x R n}. The general descen direcions mehod is x k+ = x k + k d k where x k is he curren

More information

A Note on Superlinear Ambrosetti-Prodi Type Problem in a Ball

A Note on Superlinear Ambrosetti-Prodi Type Problem in a Ball A Noe on Superlinear Ambrosei-Prodi Type Problem in a Ball by P. N. Srikanh 1, Sanjiban Sanra 2 Absrac Using a careful analysis of he Morse Indices of he soluions obained by using he Mounain Pass Theorem

More information

Some operator monotone functions related to Petz-Hasegawa s functions

Some operator monotone functions related to Petz-Hasegawa s functions Some operaor monoone funcions relaed o Pez-Hasegawa s funcions Masao Kawasaki and Masaru Nagisa Absrac Le f be an operaor monoone funcion on [, ) wih f() and f(). If f() is neiher he consan funcion nor

More information

Matlab and Python programming: how to get started

Matlab and Python programming: how to get started Malab and Pyhon programming: how o ge sared Equipping readers he skills o wrie programs o explore complex sysems and discover ineresing paerns from big daa is one of he main goals of his book. In his chaper,

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

Lie Derivatives operator vector field flow push back Lie derivative of

Lie Derivatives operator vector field flow push back Lie derivative of Lie Derivaives The Lie derivaive is a mehod of compuing he direcional derivaive of a vecor field wih respec o anoher vecor field We already know how o make sense of a direcional derivaive of real valued

More information

Second quantization and gauge invariance.

Second quantization and gauge invariance. 1 Second quanizaion and gauge invariance. Dan Solomon Rauland-Borg Corporaion Moun Prospec, IL Email: dsolom@uic.edu June, 1. Absrac. I is well known ha he single paricle Dirac equaion is gauge invarian.

More information

RANDOM LAGRANGE MULTIPLIERS AND TRANSVERSALITY

RANDOM LAGRANGE MULTIPLIERS AND TRANSVERSALITY ECO 504 Spring 2006 Chris Sims RANDOM LAGRANGE MULTIPLIERS AND TRANSVERSALITY 1. INTRODUCTION Lagrange muliplier mehods are sandard fare in elemenary calculus courses, and hey play a cenral role in economic

More information

On Ternary Quadratic Forms

On Ternary Quadratic Forms On Ternary Quadraic Forms W. Duke Deparmen of Mahemaics, Universiy of California, Los Angeles, CA 98888. Inroducion. Dedicaed o he memory of Arnold E. Ross Le q(x) = q(x, x, x ) be a posiive definie ernary

More information

Approximation Algorithms for Unique Games via Orthogonal Separators

Approximation Algorithms for Unique Games via Orthogonal Separators Approximaion Algorihms for Unique Games via Orhogonal Separaors Lecure noes by Konsanin Makarychev. Lecure noes are based on he papers [CMM06a, CMM06b, LM4]. Unique Games In hese lecure noes, we define

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

Second Order Linear Differential Equations

Second Order Linear Differential Equations Second Order Linear Differenial Equaions Second order linear equaions wih consan coefficiens; Fundamenal soluions; Wronskian; Exisence and Uniqueness of soluions; he characerisic equaion; soluions of homogeneous

More information

A Note on the Equivalence of Fractional Relaxation Equations to Differential Equations with Varying Coefficients

A Note on the Equivalence of Fractional Relaxation Equations to Differential Equations with Varying Coefficients mahemaics Aricle A Noe on he Equivalence of Fracional Relaxaion Equaions o Differenial Equaions wih Varying Coefficiens Francesco Mainardi Deparmen of Physics and Asronomy, Universiy of Bologna, and he

More information

2. Nonlinear Conservation Law Equations

2. Nonlinear Conservation Law Equations . Nonlinear Conservaion Law Equaions One of he clear lessons learned over recen years in sudying nonlinear parial differenial equaions is ha i is generally no wise o ry o aack a general class of nonlinear

More information

Differential Harnack Estimates for Parabolic Equations

Differential Harnack Estimates for Parabolic Equations Differenial Harnack Esimaes for Parabolic Equaions Xiaodong Cao and Zhou Zhang Absrac Le M,g be a soluion o he Ricci flow on a closed Riemannian manifold In his paper, we prove differenial Harnack inequaliies

More information

Linear Response Theory: The connection between QFT and experiments

Linear Response Theory: The connection between QFT and experiments Phys540.nb 39 3 Linear Response Theory: The connecion beween QFT and experimens 3.1. Basic conceps and ideas Q: How do we measure he conduciviy of a meal? A: we firs inroduce a weak elecric field E, and

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

Math 527 Lecture 6: Hamilton-Jacobi Equation: Explicit Formulas

Math 527 Lecture 6: Hamilton-Jacobi Equation: Explicit Formulas Mah 527 Lecure 6: Hamilon-Jacobi Equaion: Explici Formulas Sep. 23, 2 Mehod of characerisics. We r o appl he mehod of characerisics o he Hamilon-Jacobi equaion: u +Hx, Du = in R n, u = g on R n =. 2 To

More information

WEEK-3 Recitation PHYS 131. of the projectile s velocity remains constant throughout the motion, since the acceleration a x

WEEK-3 Recitation PHYS 131. of the projectile s velocity remains constant throughout the motion, since the acceleration a x WEEK-3 Reciaion PHYS 131 Ch. 3: FOC 1, 3, 4, 6, 14. Problems 9, 37, 41 & 71 and Ch. 4: FOC 1, 3, 5, 8. Problems 3, 5 & 16. Feb 8, 018 Ch. 3: FOC 1, 3, 4, 6, 14. 1. (a) The horizonal componen of he projecile

More information

DIFFERENTIAL GEOMETRY HW 5

DIFFERENTIAL GEOMETRY HW 5 DIFFERENTIAL GEOMETRY HW 5 CLAY SHONKWILER 3. Le M be a complee Riemannian manifold wih non-posiive secional curvaure. Prove ha d exp p v w w, for all p M, all v T p M and all w T v T p M. Proof. Le γ

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

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

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

Hamilton- J acobi Equation: Explicit Formulas In this lecture we try to apply the method of characteristics to the Hamilton-Jacobi equation: u t

Hamilton- J acobi Equation: Explicit Formulas In this lecture we try to apply the method of characteristics to the Hamilton-Jacobi equation: u t M ah 5 2 7 Fall 2 0 0 9 L ecure 1 0 O c. 7, 2 0 0 9 Hamilon- J acobi Equaion: Explici Formulas In his lecure we ry o apply he mehod of characerisics o he Hamilon-Jacobi equaion: u + H D u, x = 0 in R n

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

QUANTITATIVE DECAY FOR NONLINEAR WAVE EQUATIONS

QUANTITATIVE DECAY FOR NONLINEAR WAVE EQUATIONS QUANTITATIVE DECAY FOR NONLINEAR WAVE EQUATIONS SPUR FINAL PAPER, SUMMER 08 CALVIN HSU MENTOR: RUOXUAN YANG PROJECT SUGGESTED BY: ANDREW LAWRIE Augus, 08 Absrac. In his paper, we discuss he decay rae for

More information

Monochromatic Infinite Sumsets

Monochromatic Infinite Sumsets Monochromaic Infinie Sumses Imre Leader Paul A. Russell July 25, 2017 Absrac WeshowhahereisaraionalvecorspaceV suchha,whenever V is finiely coloured, here is an infinie se X whose sumse X+X is monochromaic.

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

System of Linear Differential Equations

System of Linear Differential Equations Sysem of Linear Differenial Equaions In "Ordinary Differenial Equaions" we've learned how o solve a differenial equaion for a variable, such as: y'k5$e K2$x =0 solve DE yx = K 5 2 ek2 x C_C1 2$y''C7$y

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

CH.7. PLANE LINEAR ELASTICITY. Continuum Mechanics Course (MMC) - ETSECCPB - UPC

CH.7. PLANE LINEAR ELASTICITY. Continuum Mechanics Course (MMC) - ETSECCPB - UPC CH.7. PLANE LINEAR ELASTICITY Coninuum Mechanics Course (MMC) - ETSECCPB - UPC Overview Plane Linear Elasici Theor Plane Sress Simplifing Hpohesis Srain Field Consiuive Equaion Displacemen Field The Linear

More information

Then. 1 The eigenvalues of A are inside R = n i=1 R i. 2 Union of any k circles not intersecting the other (n k)

Then. 1 The eigenvalues of A are inside R = n i=1 R i. 2 Union of any k circles not intersecting the other (n k) Ger sgorin Circle Chaper 9 Approimaing Eigenvalues Per-Olof Persson persson@berkeley.edu Deparmen of Mahemaics Universiy of California, Berkeley Mah 128B Numerical Analysis (Ger sgorin Circle) Le A be

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

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

dy dx = xey (a) y(0) = 2 (b) y(1) = 2.5 SOLUTION: See next page

dy dx = xey (a) y(0) = 2 (b) y(1) = 2.5 SOLUTION: See next page Assignmen 1 MATH 2270 SOLUTION Please wrie ou complee soluions for each of he following 6 problems (one more will sill be added). You may, of course, consul wih your classmaes, he exbook or oher resources,

More information

Omega-limit sets and bounded solutions

Omega-limit sets and bounded solutions arxiv:3.369v [mah.gm] 3 May 6 Omega-limi ses and bounded soluions Dang Vu Giang Hanoi Insiue of Mahemaics Vienam Academy of Science and Technology 8 Hoang Quoc Vie, 37 Hanoi, Vienam e-mail: dangvugiang@yahoo.com

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

d 1 = c 1 b 2 - b 1 c 2 d 2 = c 1 b 3 - b 1 c 3

d 1 = c 1 b 2 - b 1 c 2 d 2 = c 1 b 3 - b 1 c 3 and d = c b - b c c d = c b - b c c This process is coninued unil he nh row has been compleed. The complee array of coefficiens is riangular. Noe ha in developing he array an enire row may be divided or

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

Families with no matchings of size s

Families with no matchings of size s Families wih no machings of size s Peer Franl Andrey Kupavsii Absrac Le 2, s 2 be posiive inegers. Le be an n-elemen se, n s. Subses of 2 are called families. If F ( ), hen i is called - uniform. Wha is

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

Vehicle Arrival Models : Headway

Vehicle Arrival Models : Headway Chaper 12 Vehicle Arrival Models : Headway 12.1 Inroducion Modelling arrival of vehicle a secion of road is an imporan sep in raffic flow modelling. I has imporan applicaion in raffic flow simulaion where

More information

Lecture Notes 2. The Hilbert Space Approach to Time Series

Lecture Notes 2. The Hilbert Space Approach to Time Series Time Series Seven N. Durlauf Universiy of Wisconsin. Basic ideas Lecure Noes. The Hilber Space Approach o Time Series The Hilber space framework provides a very powerful language for discussing he relaionship

More information

Essential Maps and Coincidence Principles for General Classes of Maps

Essential Maps and Coincidence Principles for General Classes of Maps Filoma 31:11 (2017), 3553 3558 hps://doi.org/10.2298/fil1711553o Published by Faculy of Sciences Mahemaics, Universiy of Niš, Serbia Available a: hp://www.pmf.ni.ac.rs/filoma Essenial Maps Coincidence

More information

Lecture 20: Riccati Equations and Least Squares Feedback Control

Lecture 20: Riccati Equations and Least Squares Feedback Control 34-5 LINEAR SYSTEMS Lecure : Riccai Equaions and Leas Squares Feedback Conrol 5.6.4 Sae Feedback via Riccai Equaions A recursive approach in generaing he marix-valued funcion W ( ) equaion for i for he

More information

A New Perturbative Approach in Nonlinear Singularity Analysis

A New Perturbative Approach in Nonlinear Singularity Analysis Journal of Mahemaics and Saisics 7 (: 49-54, ISSN 549-644 Science Publicaions A New Perurbaive Approach in Nonlinear Singulariy Analysis Ta-Leung Yee Deparmen of Mahemaics and Informaion Technology, The

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

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