DEFORMATION OF ALGEBRAS OVER THE LANDWEBER-NOVIKOV ALGEBRA DONALD YAU Abstract. An algebraic deformation theory of algebras over the Landweber-Novikov
|
|
- Damian Goodwin
- 5 years ago
- Views:
Transcription
1 DEFORMATION OF ALGEBRAS OVER THE LANDWEBER-NOVIKOV ALGEBRA DONALD YAU Absrac. An algebraic deformaion heory of algebras over he Landweber-Novikov algebra is obained. 1. Inroducion The Landweber-Novikov algebra S was originally sudied by Landweber [8] and Novikov [10] as a cerain algebra of sable cohomology operaions on complex cobordism MU ( ). In fac, i is known ha every sable cobordism operaion can be wrien uniquely as an MU -linear combinaion in he Landweber-Novikov operaions. The Landweber-Novikov operaions ac sably, and hence addiively, on he cobordism MU () of a space. However, hey are, in general, no muliplicaive on MU (). Insead, heir acions on a produc of wo elemens in MU () saisfy he so-called Caran formula, analogous o he formula of he same name in ordinary mod 2 cohomology. This srucure - he S-module srucure ogeher wih he Caran formula on producs - makes MU () ino wha is called an algebra over he Landweber-Novikov algebra, or an S-algebra for shor. These S- algebras are herefore of grea imporance in algebraic opology. The algebra S has also appeared in oher seings. For example, Bukhshaber and Shokurov [2] showed ha he Landweber-Novikov algebra is isomorphic o he algebra of lef invarian differenials on he group Diff 1 (Z). Denoing he group of formal diffeomorphisms on he real line by Diff 1 (R), he group Diff 1 (Z) is he subgroup generaed by he formal diffeomorphisms wih ineger coefficiens. This heme ha he Landweber- Novikov algebra is an operaion algebra" is echoed in Wood's paper [12]. Wood consruced S as a cerain algebra of differenial operaors on he inegral polynomial ring on counably infiniely many variables. There are even connecions beween he Landweber-Novikov algebra and physics, as he work of Morava [9] demonsraes. The purpose of his paper is o sudy algebras over he Landweber- Novikov algebra from he specific view poin of algebraic deformaions. We would like o deform an S-algebra A wih respec o he Landweber-Novikov operaions on A, keeping he algebra srucure on A unalered. The resuling 1
2 2 DONALD YAU deformaion heory is described in cohomological and obsrucion heoreic erms. The original heory of deformaions of associaive algebras was developed by Gersenhaber in a series of papers [3, 4, 5, 6]. I has since been exended in many differen direcions, and many kinds of algebras now have heir own deformaion heories. The Landweber-Novikov algebra is acually a Hopf algebra, as he referee poined ou. Therefore, wha we are considering in his paper is really an insance of deformaion of a module algebra over a Hopf algebra. I would be nice o exend he resuls in he curren paper o his more general seing. A descripion of he res of he paper follows. The following secion is preliminary in naure. We recall he Landweber- Novikov algebra S and algebras over i. Our deformaion heory depends on he cohomology of a cerain cochain complex F, which is consruced in he nex secion as well. In Secion 3 we inroduce he noions of a formal deformaion and of a formal auomorphism. The laer is used o defined equivalence of formal deformaions. The main poin of ha secion is Theorem 3.5, which idenifies he infiniesimal" of a formal deformaion wih an appropriae cohomology class in H 1 (F ). Inuiively, he infiniesimal" is he iniial velociy of he formal deformaion. Secion 4 begins wih a discussion of formal auomorphisms of finie order and how such objecs can be exended o higher order ones. See Theorem 4.3 and Corollary 4.4. These resuls are needed o sudy rigidiy. An S-algebra A is called rigid if every formal deformaion of A is equivalen o he rivial one. The main resul here is Corollary 4.7, which saes ha an S-algebra A is rigid, provided ha boh H 1 (F ) and HH 2 (A) are rivial. Here HH 2 (A) denoes he second Hochschild cohomology of A, as an algebra over he ring of inegers, wih coefficiens in A iself. In Secion 5, we idenify he obsrucions o exending a 1-cocycle in F o a formal deformaion. This is done by considering formal deformaions of finie orders and idenifying he obsrucions o exending such objecs o higher order ones. This obsrucion urns ou o be in H 2 (F ); see Theorem 5.3. As a resul, he vanishing of H 2 (F ) implies ha every 1-cocycle occurs as he infiniesimal of a formal deformaion (Corollary 5.5). The paper ends wih Theorem 5.7, which shows ha he vanishing of a cerain class in H 1 (F ) implies ha wo order m +1 exensions of an order m formal deformaion are equivalen.
3 DEFORMATION OF ALGEBRAS OVER THE LANDWEBER-NOVIKOV ALGEBRA 3 2. The Landweber-Novikov algebra and he complex F The purpose of his preliminary secion is o recall he Landweber-Novikov algebra S and he noion of an algebra over i. Then we consruc a cochain complex F associaed o an algebra over he Landweber-Novikov algebra. This complex will be used in laer secions o sudy algebraic deformaions of S-algebras The Landweber-Novikov algebra. References for his subsecion are [8, 10], where he Landweber-Novikov algebra was firs inroduced. Wood's paper [12] has an alernaive descripion of i as a cerain algebra of differenial operaors. The book [1, Ch. I] by Adams is also a good reference. The Landweber-Novikov algebra S is generaed by cerain elemens s ff, he Landweber-Novikov operaions, indexed by he exponenial sequences, which we firs recall. An exponenial sequence is a sequence ff = (ff 1 ;ff 2 ;:::) of non-negaive inegers in which all bu a finie number of he ff i are 0. When ff and fi are wo exponenial sequences, heir sum ff + fi is defined componenwise. Denoe by E he se of all exponenial sequences. For each exponenial sequence ff, here is a sable cobordism cohomology operaion s ff : MU ( )! MU 0 ( ); called a Landweber-Novikov operaion. The composiion s ff s fi of any wo Landweber-Novikov operaions saisfies he produc formula, which expresses i uniquely as a finie Z-linear combinaion, (2.1.1) s ff s fi = n fl s fl : fl2p (ff;fi) See, for example, Adams [1, xx5,6] or Wood [12, Thm. 4.2] for a proof of his fac. For our purposes, we do no really need o know wha he inegers n fl are, as long as hey saisfy he obvious associaiviy condiion. Thus, using he produc formula (2.1.1), he free abelian group (2.1.2) S = M ff2e Zs ff can be equipped wih an algebra srucure wih composiion as he produc. This is wha we referred o as he Landweber-Novikov algebra. The cobordism MU () of a space or a specrum is auomaically an S-module. In fac, i is known ha every sable cobordism cohomology operaion can be wrien uniquely as an MU -linear combinaion of he
4 4 DONALD YAU Landweber-Novikov operaions. (Here MU denoes MU (p) as usual.) If is a space, hen MU () is no jus a group bu an algebra as well. On a produc of wo elemens, he Landweber-Novikov operaions saisfy he Caran formula, (2.1.3) s ff (ab) = s fi (a)s fl (b): fi+fl=ff Here ff 2 E and a; b 2 MU (). We, herefore, make he following definiion. Definiion 2.2. By an algebra over he Landweber-Novikov algebra, or an S- algebra for shor, we mean a commuaive ring A wih 1 ha comes equipped wih an S-module srucure such ha he Caran formula (2.1.3) is saisfied for all ff 2 E and a; b 2 A. Given a commuaive ring A, le End(A) denoe he algebra of addiive self-maps of A, where produc is composiion of self maps. If f and g are in End(A), hen fg always means he composiion f ffi g. An S-algebra srucure on A is equivalen o a funcion (2.2.1) s : E! End(A); assigning o each exponenial sequence ff an addiive operaion s ff on A, which saisfies he produc formula (2.1.1) on composiions and he Caran formula (2.1.3) on producs in A The complex F. The algebraic deformaion heory of S-algebras discussed in laer secions depends on a cerain cochain complex F, which we now consruc. Firs we need some noaions. Le A be a commuaive ring. Denoe by Der(A) he abelian group of derivaions on A. Recall ha a derivaion on A is an addiive self-map f : A! A which saisfies he condiion f(ab) = af(b) + f(a)b for all a; b 2 A. For a posiive ineger n, we use he shorer noaion A Ωn o denoe he ensor produc over he ring of inegers of A wih iself n imes. The group of addiive maps A Ωn! A is wrien Hom(A Ωn ;A). When n =1, we also wrie End(A) for Hom(A; A). Each se Hom(A Ωn ;A) has a naural abelian group srucure. Namely, given f;g: A Ωn! A and b 2 A Ωn, he sum (f + g) sends b o f(b)+g(b). Le Se be he caegory of ses. Given wo ses C and D, he se of funcions from C o D is wrien Se(C; D). If D is an abelian group, hen, jus as in he previous paragraph, he se Se(C; D) is naurally equipped wih an abelian group srucure as well. Le A be an algebra over he Landweber-Novikov algebra S (see Definiion 2.2). Consider he Landweber-Novikov operaions on A as a funcion s as in
5 DEFORMATION OF ALGEBRAS OVER THE LANDWEBER-NOVIKOV ALGEBRA 5 (2.2.1). Recall ha E is he se of all exponenial sequences. Also recall he ses P (ff; fi) from he produc formula (2.1.1). Denoe by E n he Caresian produc E E (n facors). Jus as in he case of s,iff is a funcion wih domain E, we will wrie f ff insead of f(ff) for ff 2 E. We are now ready o define he cochain complex F = F (A) of abelian groups. We make he following definiions. ffl F 0 (A) = Der(A). ffl F 1 (A) =Se(E; End(A)). ffl For inegers n 2, se where Now we define he differenials. F n (A) = F n 0(A) F n 1(A); F n 0 (A) = Se(E n ; End(A)); F n 1 (A) = Se(E; Hom(A Ωn ;A)): ffl d 0 (') =s ' 's for ' 2 F 0 (A). ffl For n 1, d n =(d n 0 ;dn 1 ), where d n 0 : F0 n (A)! F0 n+1 (A); d n 1 : F n 1 (A)! F n+1 1 (A) are defined as follows. (Here we have F0 1(A) = F1 1 (A) = F1 (A).) Suppose ha f = (f 0 ;f 1 ) is an elemen of F n (A) for some n 2 (or jus f when n = 1), x = (ff 1 ;:::;ff n+1 ) 2 E n+1, ff 2 E, and a = a 1 Ω Ωa n+1 2 A Ω(n+1). Then we se (2.3.1) (d n 0 f 0)(x) = s ff1 f 0 (ff 2 ;:::;ff n+1 ) (2.3.2) + n» ( 1) i fi2p (ffi;ffi+1) + ( 1) n+1 f 0 (ff 1 ;:::;ff n )s ffn+1 ; n fi f 0 ( ;ff i 1 ;fi;ff i+2 ;:::) where P ( ; ) is as in he produc formula (2.1.1), and (d n 1 f 1)(ff)(a) = fi+fl=ff + n s fi (a 1 )f 1 (fl)(a 2 Ω Ωa n+1 ) ( 1) i f 1 (ff)( Ωa i 1 Ω (a i a i+1 ) Ω a i+2 ) + ( 1) n+1 fi+fl=ff f 1 (fi)(a 1 Ω Ωa n )s fl (a n+1 ): In hese definiions, when n =1,boh f 0 and f 1 are inerpreed as f.
6 6 DONALD YAU Proposiion 2.4. (F ;d ) is a cochain complex of abelian groups. Proof. I is sraighforward o check ha d 1 d 0 =0by direc inspecion. For i =0; 1 and n P 1, he formulas above allow one o rewrie d n i as an alernaing sum d n n+1 i = j=0 ( i n [j]; corresponding o he n + 2 erms in he respecive formulas. I is sraighforward o check ha, for n 1, he cosimplicial n+1 i [l] n i [k] n+1 i [k] n i [l 1] (0» k<l» n +2) hold. Therefore, i follows ha F (A) is a cochain complex. From now on, whenever we speak of cochains," cocycles," coboundaries," and cohomology classes," we are referring o he cochain complex F =(F ;d ), unless saed oherwise. The ih cohomology group of F will be denoed by H i (F ). 3. Formal deformaions and auomorphisms The purposes of his secion are (1) o inroduce formal deformaions and auomorphisms of an S-algebra and (2) o idenify he infiniesimal" of a formal deformaion wih an appropriae cohomology class in he complex F Formal deformaions. Throughou his secion, le A be an arbirary bu fixed S-algebra. Recall ha he S-algebra srucure on A can be characerized as a funcion s as in (2.2.1) from he se E of exponenial sequences o he algebra of addiive self maps of A. In addiion, his funcion saisfies he Caran formula (2.1.3) and he produc formula (2.1.1). We will deform he Landweber-Novikov operaions on A wih respec o hese wo properies. We define a formal deformaion of A o be a formal power series in he indeerminae, (3.1.1) ff = s + s s s 3 + ; in which each s i 2 F 1 (A) (i 1), i.e. is a funcion E! End(A), saisfying he following wo properies (wih s 0 = s and s i (ff) =s i ff): ffl The Caran formula: For every ff 2 E and a; b 2 A, he equaliy (3.1.2) ffff(ab) = fffi(a)ff fl(b) of power series holds. fi+fl=ff
7 DEFORMATION OF ALGEBRAS OVER THE LANDWEBER-NOVIKOV ALGEBRA 7 ffl The Produc formula: For ff; fi 2 E, he equaliy (3.1.3) ffff ff fi = n fl fffl of power series holds. fl2p (ff;fi) We pause o make a few remarks. Firs, he superscrip i in s i is an index, no an exponen, whereas i is he ih power of he indeerminae. Second, sums and producs of wo power series are aken in he usual way, wih commuing wih every erm in sigh. The coefficiens in (3.1.2) and (3.1.3) are in A and End(A), respecively, and heir calculaions are done in he appropriae rings. In paricular, muliplying ou he righ-hand side of he equaion, one observes ha he Caran formula (3.1.2) is equivalen o he equaliy (3.1.4) s n ff(ab) = n s i fi(a)s n i fl (b) i=0 fi+fl=ff in A for all n 0, ff 2 E, and a; b 2 A. Similarly, unwrapping he lefhand side of he equaion, one observes ha he Produc formula (3.1.3) is equivalen o he equaliy (3.1.5) n i=0 s i ff sn i fi = fl2p (ff;fi) n fl s n fl in End(A) for all n 0 and ff; fi 2 E. When n = 0, (3.1.4) and (3.1.5) are jus he original Caran formula (2.1.3) and produc formula (2.1.1), respecively, for s = s 0. Seing = 0 in he formal deformaion ff, we obain ff 0 = s. So we can hink of ff as a one-parameer curve wih s a he original. We, herefore, call s 1 he infiniesimal, since i is he iniial velociy" of he formal deformaion ff Formal auomorphisms. In order o idenify he infiniesimal as an appropriae cohomology class in F, we need a noion of equivalence of formal deformaions. By a formal auomorphism on A, we mean a formal power series (3.2.1) Φ = 1 + ffi ffi ffi 3 + ; where 1 = Id A and each ffi i 2 End(A), saisfying muliplicaiviy, (3.2.2) Φ (ab) = Φ (a)φ (b) for all a; b 2 A.
8 8 DONALD YAU The same rules of dealing wih power series apply here as well. In paricular, muliplicaiviy is equivalen o he equaliy (3.2.3) ffi n (ab) = n i=0 ffi i (a)ffi n i (b) for all n 0 and a; b 2 A, in which ffi 0 =1. The condiion when n =0is rivial, as i only says ha he ideniy map on A is muliplicaive. When n = 1, he condiion is (3.2.4) ffi 1 (ab) = affi 1 (b) + ffi 1 (a)b; which is equivalen o say ha ffi 1 is a derivaion on A. More generally, if ffi 1 = ffi 2 = = ffi k = 0, hen ffi k+1 is a derivaion on A. I is an easy exercise in inducion o see ha a formal auomorphism Φ has a unique formal inverse (3.2.5) Φ 1 = 1 ffi (ffi 2 1 ffi 2 )+ 3 ( ffi 3 1 +ffi 1 ffi 2 +ffi 2 ffi 1 ffi 3 )+ ; for which The coefficien of n in Φ 1 Φ Φ 1 = 1 = Φ 1 Φ : is an inegral polynomial in ffi 1 ; ;ffi n. Moreover, he muliplicaiviy of Φ implies ha of Φ 1 a; b 2 A, wehave. Indeed, for elemens ab = (Φ Φ 1 (a))(φ Φ 1 (b)) = Φ (Φ 1 (a)φ 1 (b)); which implies ha Φ 1 is muliplicaive. We record hese facs as follows. Lemma 3.3. Le Φ =1+ffi ffi 2 + be a formal auomorphism on A. Then he firs non-zero ffi i (i 1) is a derivaion on A. Moreover, he formal inverse Φ 1 of Φ is also a formal auomorphism on A. Now if s n is a funcion E! End(A), i.e. a 1-cochain, and if f and g are in End(A), hen we have a new 1-cochain fs n g wih (fs n g)(ff) = fsn ff g in End(A) for ff 2 E. Therefore, i makes sense o consider he formal power series Φ 1 ffφ whenever Φ is a formal auomorphism. Proposiion 3.4. Le ff and Φ be, respecively, a formal deformaion and a formal auomorphism of A. Then he formal power series Φ 1 ffφ is also a formal deformaion of A.
9 DEFORMATION OF ALGEBRAS OVER THE LANDWEBER-NOVIKOV ALGEBRA 9 Proof. We need o check he Caran formula (3.1.2) and he Produc formula (3.1.3) for ~ff =Φ 1 ffφ. For he Caran formula, we have ~ff ff(ab) = (Φ 1 ffff)(φ (a)φ (b)) = Φ 1 = fi+fl=ff fi+fl=ff (Φ 1 (ff fiφ (a))(ff flφ (b)) fffiφ (a))(φ 1 ffflφ (b)): We have used he Caran formula for ff and he muliplicaiviy of boh Φ and Φ 1, exended o power series. The Produc formula is equally easy o verify. Given wo formal deformaions ff and ~ff of A,say ha hey are equivalen if and only if here exiss a formal auomorphism Φ on A such ha (3.4.1) ~ff = Φ 1 ff Φ : By Lemma 3.3 his is a well-defined equivalence relaion on he se of formal deformaions of A. Here is he main resul of his secion, which idenifies he infiniesimal wih an appropriae cohomology class in H 1 (F ). Recall ha cocycles, coboundaries, cochains, and cohomology classes are all aken in he cochain complex F = F (A). Theorem 3.5. Le ff = P n n s n be a formal deformaion of A. Then he infiniesimal s 1 is a 1-cocycle, i.e. d1 s 1 =0. Moreover, he cohomology class [s 1 ] is an invarian of he equivalence class of ff. More generally, if s 1 = = s k = 0 for some posiive ineger k, hen is a 1-cocycle. s k+1 Proof. To show ha s 1 is a 1-cocycle, we need o prove ha d 1 i s1 = 0 for i =0; 1. When n = 1 he Produc formula (3.1.5) saes ha and so s ff s 1 fi + s 1 ff s fi = (d 1 0 s1 )(ff; fi) = s ff s 1 fi fl2p (ff;fi) fl2p (ff;fi) n fl s 1 fl ; n fl s 1 fl + s 1 ff s fi = 0: Similarly, he Caran formula (3.1.4) when n = 1 saes ha which implies ha s 1 ff(ab) = fi+fl=ff (s fi (a)s 1 fl(b) + s 1 fi (a)s fl(b)); (d 1 1 s1 ) ff (a Ω b) = 0; as desired. This shows ha s 1 is a 1-cocycle.
10 10 DONALD YAU If s 1 = = s k = 0, hen he same argumen as above shows ha s k+1 =0. P Now suppose ha ~ff = n n ~s n is a formal deformaion of A ha is equivalen o ff. This means ha here exiss a formal auomorphism Φ such ha ~ff = Φ 1 ffφ s + (s 1 + s ffi 1 ffi 1 s ) (mod 2 ) s + (s 1 + d 0 ffi 1 ) (mod 2 ): In paricular, he 1-cocycle (~s 1 s1 ) 2 F 1 is a 1-coboundary d 0 ffi 1. (Remember ha ffi 1 is a derivaion on A, which is herefore a 0-cochain.) Thus, he cohomology classes, [~s 1 ] and [s 1 ], are equal in H 1 (F ), as assered. In view of his Theorem, i is naural o ask wheher a given cohomology class in H 1 (F ) is he infiniesimal of a formal deformaion. This quesion will be deal wih in Secion Exending formal auomorphisms and rigidiy As in he previous secion, A will denoe an S-algebra wih Landweber- Novikov operaions s and F = F (A). The main purpose of his secion is o obain cohomological condiions under which A is rigid, ha is, every formal deformaion is equivalen o he rivial deformaion s. To do ha, we firs have o consider how runcaed formal auomorphisms can be exended Formal auomorphisms of finie order. Le m be a posiive ineger. Inspired by Gersenhaber-Wilkerson [7], we define a formal auomorphism of order m on A o be a formal power series Φ = 1 + ffi ffi m ffi m wih 1 = Id A and each ffi i 2 End(A), saisfying muliplicaiviy (3.2.2) modulo m+1, i.e. he equaliy (3.2.3) holds for 0» n» m and all a; b 2 A. One can hink of a formal auomorphism as a formal auomorphism of order 1. Given such a Φ, we say ha i exends o a formal auomorphism of order m + 1 if and only if here exiss ffi m+1 2 End(A) such ha he power series (4.1.1) ~Φ = Φ + m+1 ffi m+1 is a formal auomorphism of order m+1. Sucha~Φ is said o be an exension of Φ o order m +1.
11 DEFORMATION OF ALGEBRAS OVER THE LANDWEBER-NOVIKOV ALGEBRA 11 The quesion we would like o address here is his: Given a formal auomorphism Φ of order m, can i be exended o a formal auomorphism of order m +1? I urns ou ha he obsrucion o he exisence of such an exension lies in Hochschild cohomology, which we now recall. Consider A as a unial algebra over he ring of inegers Z, he Hochschild cochain complex C (A; A) of A wih coefficiens in A iself is defined as follows. The nh dimension is he group The differenial is given by he alernaing sum C n (A; A) = Hom(A Ωn ;A): b n 1 : C n 1 (A; A)! C n (A; A) (4.1.2) (b n 1 f)(a 1 Ω Ωa n ) = a 1 f(a 2 Ω Ωa n )+ n 1 ( 1) i f( a i 1 Ω a i a i+1 Ω a i+2 )+( 1) n f(a 1 Ω Ωa n 1 )a n : The reader can consul, for example, Weibel [11] for more deailed discussions abou Hochschild cohomology. The nh Hochschild cohomology group of A over Z wih coefficiens in A iself is denoed by HH n (A). We now reurn o he quesion of exending a formal auomorphism Φ of order m o one of order m + 1. Consider he Hochschild 2-cochain given by Ob(Φ ): A Ω2 Ob(Φ )(a Ω b) = m! A ffi i (a)ffi m+1 i (b) for all a; b 2 A. Call Ob(Φ ) he obsrucion class of Φ. Lemma 4.2. The obsrucion class Ob(Φ ) is a Hochschild 2-cocycle. Proof. We calculae as follows: (b 2 Ob(Φ ))(a Ω b Ω c) = a = = 0 m ffi i (b)ffi m+1 i (c) + m i+j+k = m+1 i; k>0 m ffi i (a)ffi m+1 i (bc) + c ffi i (a)ffi j (b)ffi k (c) ffi i (ab)ffi m+1 i (c) m ffi i (a)ffi m+1 i (b) i+j+k = m+1 i; k>0 ffi i (a)ffi j (b)ffi k (c):
12 12 DONALD YAU Here we used he muliplicaiviy of Φ, namely, (3.2.3) for ffi i (ab) and ffi m+1 i (bc). Also, ffi 0 = 1 as usual. This shows ha he obsrucion class of Φ isahochschild 2-cocycle. We are now ready o show ha he obsrucion o exending Φ o a formal auomorphism of order m +1 is exacly he cohomology class [Ob(Φ )] 2 HH 2 (A). Theorem 4.3. Le Φ be a formal auomorphism of order m on A. Then exends o a formal auomorphism of order m +1 if and only if he Φ obsrucion class Ob(Φ ) is a Hochschild 2-coboundary. Proof. The exisence of an order m+1 exension ~Φ as in (4.1.1) is equivalen o he exisence of a ffi m+1 2 End(A) for which (3.2.3) holds for n = m +1. This las condiion can be rewrien as Ob(Φ )(a Ω b) = ffi m+1 (ab) + affi m+1 (b)+bffi m+1 (a) = (b 1 ffi m+1 )(a Ω b); and b 1 ffi m+1 is a Hochschild 2-coboundary. An immediae consequence of his Theorem is ha, saring wih a derivaion ffi, he vanishing of he Hochschild cohomology HH 2 (A) implies ha he formal auomorphism Φ = 1+ m ffi of order m 1 can always be exended o a formal auomorphism. This will be useful when we discuss rigidiy below. Corollary 4.4. Le m be aposiive ineger and le ffi be a derivaion on A. Assume ha HH 2 (A) =0. Then here exiss a formal auomorphism on A of he form Φ = 1 + m ffi + m+1 ffi m+1 + m+2 ffi m+2 + : Proof. Using he hypohesis ha ffi is a derivaion, i is sraighforward o verify ha he formal power series Φ = 1 + m ffi is a formal auomorphism of order m, i.e. i saisfies muliplicaiviy (3.2.3) for n» m. As HH 2 (A) = 0, by Theorem 4.3 he obsrucions o exending Φ o a formal auomorphism vanish, as desired Rigidiy. Following he erminology in [3], an S-algebra A is said o be rigid if every formal deformaion of A is equivalen o he rivial deformaion s. Using he resuls above, we will be able o obain cohomological crierion for he rigidiy of A. Firs we need he following consequence of Corollary 4.4.
13 DEFORMATION OF ALGEBRAS OVER THE LANDWEBER-NOVIKOV ALGEBRA 13 Corollary 4.6. Le k be a posiive ineger and le ff = s + k s k + k+1 s k+1 + be a formal deformaion of A in which s k 2 F1 is a 1-coboundary. Suppose ha HH 2 (A) =0. Then here exiss a formal auomorphism of he form (4.6.1) Φ = 1 k ffi k + k+1 ffi k+1 + such ha (4.6.2) Φ 1 ff Φ s (mod k+1 ): Proof. By he hypohesis on s k, here exiss a derivaion ffi k 2 Der(A) such ha d 0 ffi k = s ffi k ffi k s = s k : Since ffi k is also a derivaion on A, Corollary 4.4 implies ha here exiss a formal auomorphism Φ as in (4.6.1). Compuing modulo k+1,wehave This proves he Corollary. Φ 1 ff Φ (1 + k ffi k )(s + k s k )(1 k ffi k ) s + k (s k + ffi k s s ffi k ) s : By Proposiion 3.4, he formal power series Φ 1 ffφ is acually a formal deformaion ha is equivalen off. Therefore, by applying his Corollary repeaedly, we obain he following cohomological crierion for A o be rigid. Corollary 4.7. If HH 2 (A) =0and H 1 (F (A)) = 0, hen A is rigid. We should poin ou ha in he deformaion heory of some oher kinds of algebras, rigidiy is usually guaraneed by he vanishing of jus one cohomology group, usually an H 1 or an H Exending cocycles As before, A will denoe an arbirary bu fixed S-algebra, and F = F (A). The Landweber-Novikov operaions on A are given by a funcion s as in (2.2.1). Recall from Theorem 3.5 ha he infiniesimal of a formal deformaion is a 1-cocycle in F. The purpose of his secion is o answer he quesions: (1) Wha is he obsrucions o exending a 1-cocycle o a formal deformaion? (2) Wha is he obsrucions o wo such exensions being equivalen? We will break hese quesions ino a sequence of smaller quesions, each of which is deal wih in an obsrucion heoreic way.
14 14 DONALD YAU 5.1. Formal deformaions of finie order. Firs we need some definiions. Le m be a posiive ineger. As in he previous secion, a formal deformaion of order m of A is a formal power series (5.1.1) ff = s + s m s m ; in which each s i (i 1) is in F 1 such ha he Caran formula (3.1.2) and he Produc formula (3.1.3) are saisfied modulo m+1. In oher words, (3.1.4) and (3.1.5) are saisfied for all n» m. We say ha a formal deformaion ff of order m exends o a formal deformaion of order M >mif and only if here exis 1-cochains s m+1 ;:::;s M such ha he power series (5.1.2) ~ff = ff + m+1 s m M s M is a formal deformaion of order M. Call ~ff an order M exension of ff. One can hink of a formal deformaion as a formal deformaion of order 1. Given a 1-cocycle s 1, he problem of exending he formal deformaion ff = s + s 1 of order 1 o a formal deformaion can be hough of as exending ff o order 2, hen order 3, and so forh. We will do his by idenifying he obsrucion o exending an order m formal deformaion o one of order m +1. Le ff be a formal deformaion of order m as in (5.1.1). Consider he 2-cochain Ob(ff ) = (Ob 0 (ff ); Ob 1 (ff )) 2 F 2 = F 2 0 F 2 1 ; whose componens are defined by he condiions, (5.1.3) Ob 0 (ff )(ff; fi) = and (5.1.4) Ob 1 (ff ) ff (aωb) = m m We call Ob(ff ) he obsrucion class of ff. s i ff sm+1 i fi (ff; fi 2 E) s i fi (a)sm+1 i fl (b) (ff 2 E; a;b2 A): fi+fl=ff Lemma 5.2. The obsrucion class Ob(ff ) is a 2-cocycle. Proof. We need o show ha d 2 i Ob i(ff ) = 0 for i = 0; 1. Since ff is he only formal deformaion we are dealing wih, we abbreviae Ob i (ff )oob i.
15 DEFORMATION OF ALGEBRAS OVER THE LANDWEBER-NOVIKOV ALGEBRA 15 For i = 0, le ff; fi; fl be exponenial sequences. Then we have (5.2.1) (d 2 0 Ob 0 )(ff; fi; fl) = s ff m ffi2p (ff;fi) s i fi sm+1 i fl "2P (fi;fl) n " m s i ff sm+1 i " + m n ffi ffi2p (ff;fi) m + s i ffi sm+1 i fl s i ff sm+1 i fi s fl : This is a sum of four erms. Using he Produc formula (3.1.5), he second erm can be rewrien as m m i n ffi s i ffi s m+1 i fl = s l ff si l fi sm+1 i fl : l=0 In paricular, he m summands in i corresponding o l = 0 cancel ou wih he firs erm in (5.2.1). Consequenly, he sum of he firs wo erms in (5.2.1) becomes (5.2.2) i+j+k = m+1 i;k>0 s i ff sj fi sk fl : An analogous argumen applied o he hird and fourh erms in (5.2.1) shows ha heir sum is exacly (5.2.2) wih he opposie sign. I follows ha d 2 0 Ob 0 = 0, as desired. The proof of d 2 1 Ob 1 =0is quie similar o he argumen above and he proof of Lemma 4.2. Indeed, (d 2 1 Ob 1) ff (a Ω b Ω c) (see (??)) is again he sum of four erms. Using he Caran formula (3.1.4), is second erm can be rewrien as (5.2.3) (Ob 1 ) ff (ab Ω c) = = m s i fi(ab)s m+1 i fl (c) fi+fl=ff m fi+fl=ff i j=0»+ =fi s j»(a)s i j (b) s m+1 i fl (c): The summands corresponding o j = 0 cancel ou wih he firs of he four erms in (d 2 1 Ob 1) ff (a Ω b Ω c). In paricular, he sum of he firs wo erms in (d 2 1 Ob 1) ff (a Ω b Ω c) is (5.2.4) s i fi(a)s j fl(b)s k ffi (c): The summaion is aken over all riples (i; j; k) of non-negaive inegers and all riples (fi;fl;ffi) of exponenial sequences for which and i + j + k = m + 1 (i; k > 0) fi + fl + ffi = ff:
16 16 DONALD YAU A similar argumen applies o he las wo erms in (d 2 1 Ob 1) ff (a Ω b Ω c), showing ha heir sum is exacly (5.2.4) wih he opposie sign. I follows ha d 2 1 Ob 1 = 0, as expeced. This finishes he proof of he Lemma. As he obsrucion class of ff is a 2-cocycle, i represens a cohomology class in H 2 (F ). We are now ready o presen he main resul of his secion, which idenifies he obsrucion o exending a formal deformaion of order m o one of order m +1. Theorem 5.3. Le ff be a formal deformaion of order m of A. Then ff exends o a formal deformaion of order m+1 if and only if he cohomology class [Ob(ff )] 2 H 2 (F (A)) vanishes. Proof. Indeed, he exisence of an order m+1 exension ~ff of ff, as in (4.1.1) wih M = m + 1, is equivalen o he exisence of a 1-cochain s m+1 2 F 1 for which he Caran formula (3.1.4) and he Produc formula (3.1.5) boh hold for n = m +1. Simply by rearranging erms, he Caran formula (3.1.4) when n = m + 1 can be rewrien as (Ob 1 (ff)) ff (a Ω b) = (d 1 1 sm+1 ) ff (a Ω b): Similarly, he Produc formula (3.1.5) when n = m + 1 is equivalen o (Ob 0 (ff))(ff; fi) = (d 1 0 sm+1 )(ff; fi): These wo condiions ogeher are equivalen o (5.3.1) Ob(ff ) = d 1 s m+1 ; i.e., he obsrucion class is a 2-coboundary. Since Ob(ff ) is a 2-cocycle (Lemma 5.2), he Theorem is proved. Applying his Theorem repeaedly, we obain he obsrucions o exending a 1-cocycle o a formal deformaion. Corollary 5.4. Le s 1 2 F1 (A) be a1-cocycle. Then here exis a sequence of classes! 1 ;! 2 ;::: 2 H 2 (F (A)) for which! n (n>1) is defined if and only if! 1 ;:::;! n 1 are defined and equal o 0. Moreover, he formal deformaion ff = s + s 1 of order 1 on A exends o a formal deformaion if and only if! i is defined and equal o 0 for each i =1; 2;:::. Since hese obsrucions lie in H 2 (F (A)), he rivialiy of his group implies ha exensions always exis. Corollary 5.5. If H 2 (F (A)) = 0, hen every formal deformaion of order m 1 of A exends o a formal deformaion.
17 DEFORMATION OF ALGEBRAS OVER THE LANDWEBER-NOVIKOV ALGEBRA Equivalence of formal deformaions of finie order. Le ff be a formal deformaion of A of order m 1, and le ~ff and μff be wo order m+1 exensions of i. Are he wo exensions equivalen? This is he quesion ha we would like o address in his final secion. Firs, we need a definiion of equivalence. Two formal deformaion ff and ~ff of order m of A are said o be equivalen if and only if here exiss a formal auomorphism Φ of order m such ha he equaliy (3.4.1) holds modulo m+1. This is a well-defined equivalence relaion on he se of formal deformaions of order m of A. In fac, i is easy o see ha a formal auomorphism Φ of order m has a formal inverse Φ 1 as in (3.2.5) which is also a formal auomorphism of order m. Now le ff = s + + m s m be a formal deformaion of order m of A, and le ~ff = ff + m+1 ~s m+1 and μff = ff + m+1 μs m+1 be wo order m +1 exensions of ff. Then (5.3.1) in he proof of Theorem 5.3 ells us ha d 1 ~s m+1 = Ob(ff ) = d 1 μs m+1 : I follows ha (~s m+1 μs m+1 ) 2 F 1 is a 1-cocycle, and i makes sense o consider he cohomology class in H 1 (F ) represened by i. Theorem 5.7. If he cohomology class [~s m+1 μs m+1 ] 2 H 1 (F ) vanishes, hen he formal deformaions, ~ff and μff,oforder m +1 are equivalen. Proof. The argumen is quie similar o he proofs of Theorem 3.5 and Corollary 4.6. In fac, by hypohesis, here exiss a derivaion ffi on A such ha We have he formal auomorphism ~s m+1 μs m+1 = d 0 ffi = s ffi ffis : Φ = 1 + m+1 ffi of order m +1onA. Compuing modulo m+2,wehave Φ 1 as desired. μff Φ (1 m+1 ffi)(ff + m+1 μs m+1 )(1 + m+1 ffi) ff + m+1 (μs m+1 + s ffi ffis ) ff + m+1 ~s m+1 ~ff ; This obsrucion heoreic resul is less saisfacory han he analogous Theorem 4.3 and Theorem 5.3 in ha he auhor is no sure wheher he equivalence of ~ff and μff would imply he vanishing of he class [~s m+1 μs m+1 ].
18 18 DONALD YAU Acknowledgemen The auhor hanks he referee for reading an earlier version of his paper. References [1] J. F. Adams, Sable homoopy and generalised homology, Chicago Lecures in Mahemaics, Universiy of Chicago Press, Chicago, Ill.-London, [2] V. M. Bukhshaber and A. V. Shokurov, The Landweber-Novikov algebra and formal vecor fields on he line, Funksional. Anal. i Prilozhen. 12 (1978), no. 3, 1-11, 96. [3] M. Gersenhaber, On he deformaion of rings and algebras, Ann. Mah. (2) 79 (1964), [4] M. Gersenhaber, On he deformaion of rings and algebras. II, Ann. Mah. 84 (1966), [5] M. Gersenhaber, On he deformaion of rings and algebras. III, Ann. Mah. (2) 88 (1968), [6] M. Gersenhaber, On he deformaion of rings and algebras. IV, Ann. Mah. (2) 99 (1974), [7] M. Gersenhaber and C. W. Wilkerson, On he deformaion of rings and algebras, V: Deformaion of differenial graded algebras, Higher homoopy srucures in opology and mahemaical physics (Poughkeepsie, NY, 1996), , Conemp. Mah., 227, Amer. Mah. Soc., Providence, RI, [8] P. S. Landweber, Cobordism operaions and Hopf algebras, Trans. Amer. Mah. Soc. 129 (1967), [9] J. Morava, On he complex cobordism ring as a Fock represenaion, Homoopy heory and relaed opics (Kinosaki, 1988), , Lecure Noes in Mah., 1418, Springer, Berlin, [10] S. P. Novikov, Mehods of algebraic opology from he poin of view of cobordism heory, Izv. Akad. Nauk SSSR Ser. Ma. 31 (1967), [11] C. A. Weibel, An inroducion o homological algebra, Cambridge sudies in advanced mahemaics 38, Cambridge Univ. Press, Cambridge, UK, [12] R. M. W. Wood, Differenial operaors and he Seenrod algebra, Proc. London Mah. Soc. 75 (1997), address: dyau@mah.ohio-sae.edu Deparmen of Mahemaics, The Ohio Sae Universiy Newark, 1179 Universiy Drive, Newark, OH 43055
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 informationMatrix 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 informationFinish 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 informationt 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 informationChapter 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 informationBernoulli 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 informationTHE BERNOULLI NUMBERS. t k. = lim. = lim = 1, d t B 1 = lim. 1+e t te t = lim t 0 (e t 1) 2. = lim = 1 2.
THE BERNOULLI NUMBERS The Bernoulli numbers are defined here by he exponenial generaing funcion ( e The firs one is easy o compue: (2 and (3 B 0 lim 0 e lim, 0 e ( d B lim 0 d e +e e lim 0 (e 2 lim 0 2(e
More informationMath 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 informationTHE 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 information10. 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 informationUndetermined 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 informationLecture 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 informationODEs 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 informationMATH 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 informationTwo 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 informationEXPLICIT TIME INTEGRATORS FOR NONLINEAR DYNAMICS DERIVED FROM THE MIDPOINT RULE
Version April 30, 2004.Submied o CTU Repors. EXPLICIT TIME INTEGRATORS FOR NONLINEAR DYNAMICS DERIVED FROM THE MIDPOINT RULE Per Krysl Universiy of California, San Diego La Jolla, California 92093-0085,
More informationSome Basic Information about M-S-D Systems
Some Basic Informaion abou M-S-D Sysems 1 Inroducion We wan o give some summary of he facs concerning unforced (homogeneous) and forced (non-homogeneous) models for linear oscillaors governed by second-order,
More informationarxiv: 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 informationGCD 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 informationNEW 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 information11!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 informationOscillation 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 informationThe Miki-type identity for the Apostol-Bernoulli numbers
Annales Mahemaicae e Informaicae 46 6 pp. 97 4 hp://ami.ef.hu The Mii-ype ideniy for he Aposol-Bernoulli numbers Orli Herscovici, Toufi Mansour Deparmen of Mahemaics, Universiy of Haifa, 3498838 Haifa,
More informationSection 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 informationMonochromatic 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 informationStability and Bifurcation in a Neural Network Model with Two Delays
Inernaional Mahemaical Forum, Vol. 6, 11, no. 35, 175-1731 Sabiliy and Bifurcaion in a Neural Nework Model wih Two Delays GuangPing Hu and XiaoLing Li School of Mahemaics and Physics, Nanjing Universiy
More informationLet us start with a two dimensional case. We consider a vector ( x,
Roaion marices We consider now roaion marices in wo and hree dimensions. We sar wih wo dimensions since wo dimensions are easier han hree o undersand, and one dimension is a lile oo simple. However, our
More information14 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 information15. Vector Valued Functions
1. Vecor Valued Funcions Up o his poin, we have presened vecors wih consan componens, for example, 1, and,,4. However, we can allow he componens of a vecor o be funcions of a common variable. For example,
More informationarxiv: 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 informationLecture 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 informationA 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 informationLinear 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 informationFREE 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 informationInventory 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 informationEchocardiography 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 information18 Biological models with discrete time
8 Biological models wih discree ime The mos imporan applicaions, however, may be pedagogical. The elegan body of mahemaical heory peraining o linear sysems (Fourier analysis, orhogonal funcions, and so
More informationINDEPENDENT SETS IN GRAPHS WITH GIVEN MINIMUM DEGREE
INDEPENDENT SETS IN GRAPHS WITH GIVEN MINIMUM DEGREE JAMES ALEXANDER, JONATHAN CUTLER, AND TIM MINK Absrac The enumeraion of independen ses in graphs wih various resricions has been a opic of much ineres
More informationConvergence 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 informationSecond 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 informationThe 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 informationWe just finished the Erdős-Stone Theorem, and ex(n, F ) (1 1/(χ(F ) 1)) ( n
Lecure 3 - Kövari-Sós-Turán Theorem Jacques Versraëe jacques@ucsd.edu We jus finished he Erdős-Sone Theorem, and ex(n, F ) ( /(χ(f ) )) ( n 2). So we have asympoics when χ(f ) 3 bu no when χ(f ) = 2 i.e.
More informationON UNIVERSAL LOCALIZATION AT SEMIPRIME GOLDIE IDEALS
ON UNIVERSAL LOCALIZATION AT SEMIPRIME GOLDIE IDEALS JOHN A. BEACHY Deparmen of Mahemaical Sciences Norhern Illinois Universiy DeKalb IL 6115 U.S.A. Absrac In his paper we consider an alernaive o Ore localizaion
More informationShort Introduction to Fractional Calculus
. Shor Inroducion o Fracional Calculus Mauro Bologna Deparameno de Física, Faculad de Ciencias Universidad de Tarapacá, Arica, Chile email: mbologna@ua.cl Absrac In he pas few years fracional calculus
More informationSTABILITY OF PEXIDERIZED QUADRATIC FUNCTIONAL EQUATION IN NON-ARCHIMEDEAN FUZZY NORMED SPASES
Novi Sad J. Mah. Vol. 46, No. 1, 2016, 15-25 STABILITY OF PEXIDERIZED QUADRATIC FUNCTIONAL EQUATION IN NON-ARCHIMEDEAN FUZZY NORMED SPASES N. Eghbali 1 Absrac. We deermine some sabiliy resuls concerning
More informationHamilton- 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 informationGENERALIZATION OF THE FORMULA OF FAA DI BRUNO FOR A COMPOSITE FUNCTION WITH A VECTOR ARGUMENT
Inerna J Mah & Mah Sci Vol 4, No 7 000) 48 49 S0670000970 Hindawi Publishing Corp GENERALIZATION OF THE FORMULA OF FAA DI BRUNO FOR A COMPOSITE FUNCTION WITH A VECTOR ARGUMENT RUMEN L MISHKOV Received
More informationOn Boundedness of Q-Learning Iterates for Stochastic Shortest Path Problems
MATHEMATICS OF OPERATIONS RESEARCH Vol. 38, No. 2, May 2013, pp. 209 227 ISSN 0364-765X (prin) ISSN 1526-5471 (online) hp://dx.doi.org/10.1287/moor.1120.0562 2013 INFORMS On Boundedness of Q-Learning Ieraes
More informationREMARK 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 informationThe Arcsine Distribution
The Arcsine Disribuion Chris H. Rycrof Ocober 6, 006 A common heme of he class has been ha he saisics of single walker are ofen very differen from hose of an ensemble of walkers. On he firs homework, we
More informationEXERCISES 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 informationHamilton- 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 informationt 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 informationChapter 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 informationExistence 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 information5. Stochastic processes (1)
Lec05.pp S-38.45 - Inroducion o Teleraffic Theory Spring 2005 Conens Basic conceps Poisson process 2 Sochasic processes () Consider some quaniy in a eleraffic (or any) sysem I ypically evolves in ime randomly
More informationProperties 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 informationLecture 4 Kinetics of a particle Part 3: Impulse and Momentum
MEE Engineering Mechanics II Lecure 4 Lecure 4 Kineics of a paricle Par 3: Impulse and Momenum Linear impulse and momenum Saring from he equaion of moion for a paricle of mass m which is subjeced o an
More informationTHE MATRIX-TREE THEOREM
THE MATRIX-TREE THEOREM 1 The Marix-Tree Theorem. The Marix-Tree Theorem is a formula for he number of spanning rees of a graph in erms of he deerminan of a cerain marix. We begin wih he necessary graph-heoreical
More informationPhysics 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 informationMatlab 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 information6.2 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 informationOrdinary Differential Equations
Ordinary Differenial Equaions 5. Examples of linear differenial equaions and heir applicaions We consider some examples of sysems of linear differenial equaions wih consan coefficiens y = a y +... + a
More information4 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 informationSOLUTIONS 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 informationLecture 2-1 Kinematics in One Dimension Displacement, Velocity and Acceleration Everything in the world is moving. Nothing stays still.
Lecure - Kinemaics in One Dimension Displacemen, Velociy and Acceleraion Everyhing in he world is moving. Nohing says sill. Moion occurs a all scales of he universe, saring from he moion of elecrons in
More informationON FINITELY GENERATED MODULES OVER NOETHERIAN RINGS
ON FINITELY GENERATED MODULES OVER NOETHERIAN RINGS BY J. P. JANS(i). Inroducion. If A is a module over a ring R, he module Homj;(/l,R) = A* is usually called he dual of A. The elemens of A can be considered
More informationIMPLICIT AND INVERSE FUNCTION THEOREMS PAUL SCHRIMPF 1 OCTOBER 25, 2013
IMPLICI AND INVERSE FUNCION HEOREMS PAUL SCHRIMPF 1 OCOBER 25, 213 UNIVERSIY OF BRIISH COLUMBIA ECONOMICS 526 We have exensively sudied how o solve sysems of linear equaions. We know how o check wheher
More informationChapter 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 informationarxiv: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 informationGeneralized 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 informationEssential 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 information2. 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 informationHeat kernel and Harnack inequality on Riemannian manifolds
Hea kernel and Harnack inequaliy on Riemannian manifolds Alexander Grigor yan UHK 11/02/2014 onens 1 Laplace operaor and hea kernel 1 2 Uniform Faber-Krahn inequaliy 3 3 Gaussian upper bounds 4 4 ean-value
More informationPhysics 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 informationSections 2.2 & 2.3 Limit of a Function and Limit Laws
Mah 80 www.imeodare.com Secions. &. Limi of a Funcion and Limi Laws In secion. we saw how is arise when we wan o find he angen o a curve or he velociy of an objec. Now we urn our aenion o is in general
More informationA 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 informationOrthogonal Rational Functions, Associated Rational Functions And Functions Of The Second Kind
Proceedings of he World Congress on Engineering 2008 Vol II Orhogonal Raional Funcions, Associaed Raional Funcions And Funcions Of The Second Kind Karl Deckers and Adhemar Bulheel Absrac Consider he sequence
More informationPOSITIVE 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 informationExpert Advice for Amateurs
Exper Advice for Amaeurs Ernes K. Lai Online Appendix - Exisence of Equilibria The analysis in his secion is performed under more general payoff funcions. Wihou aking an explici form, he payoffs of he
More informationLogarithmic limit sets of real semi-algebraic sets
Ahead of Prin DOI 10.1515 / advgeom-2012-0020 Advances in Geomery c de Gruyer 20xx Logarihmic limi ses of real semi-algebraic ses Daniele Alessandrini (Communicaed by C. Scheiderer) Absrac. This paper
More informationA Sharp Existence and Uniqueness Theorem for Linear Fuchsian Partial Differential Equations
A Sharp Exisence and Uniqueness Theorem for Linear Fuchsian Parial Differenial Equaions Jose Ernie C. LOPE Absrac This paper considers he equaion Pu = f, where P is he linear Fuchsian parial differenial
More informationCERTAIN 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 informationOn Carlsson type orthogonality and characterization of inner product spaces
Filoma 26:4 (212), 859 87 DOI 1.2298/FIL124859K Published by Faculy of Sciences and Mahemaics, Universiy of Niš, Serbia Available a: hp://www.pmf.ni.ac.rs/filoma On Carlsson ype orhogonaliy and characerizaion
More informationAnn. 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 informationSecond 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 informationReading from Young & Freedman: For this topic, read sections 25.4 & 25.5, the introduction to chapter 26 and sections 26.1 to 26.2 & 26.4.
PHY1 Elecriciy Topic 7 (Lecures 1 & 11) Elecric Circuis n his opic, we will cover: 1) Elecromoive Force (EMF) ) Series and parallel resisor combinaions 3) Kirchhoff s rules for circuis 4) Time dependence
More informationOnline Convex Optimization Example And Follow-The-Leader
CSE599s, Spring 2014, Online Learning Lecure 2-04/03/2014 Online Convex Opimizaion Example And Follow-The-Leader Lecurer: Brendan McMahan Scribe: Sephen Joe Jonany 1 Review of Online Convex Opimizaion
More informationChapter 8 The Complete Response of RL and RC Circuits
Chaper 8 The Complee Response of RL and RC Circuis Seoul Naional Universiy Deparmen of Elecrical and Compuer Engineering Wha is Firs Order Circuis? Circuis ha conain only one inducor or only one capacior
More informationU( θ, θ), U(θ 1/2, θ + 1/2) and Cauchy (θ) are not exponential families. (The proofs are not easy and require measure theory. See the references.
Lecure 5 Exponenial Families Exponenial families, also called Koopman-Darmois families, include a quie number of well known disribuions. Many nice properies enjoyed by exponenial families allow us o provide
More informationTraveling Waves. Chapter Introduction
Chaper 4 Traveling Waves 4.1 Inroducion To dae, we have considered oscillaions, i.e., periodic, ofen harmonic, variaions of a physical characerisic of a sysem. The sysem a one ime is indisinguishable from
More informationNotes 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 informationSolutions to Assignment 1
MA 2326 Differenial Equaions Insrucor: Peronela Radu Friday, February 8, 203 Soluions o Assignmen. Find he general soluions of he following ODEs: (a) 2 x = an x Soluion: I is a separable equaion as we
More informationPhysics for Scientists & Engineers 2
Direc Curren Physics for Scieniss & Engineers 2 Spring Semeser 2005 Lecure 16 This week we will sudy charges in moion Elecric charge moving from one region o anoher is called elecric curren Curren is all
More informationAn 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 informationHomework 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 information5.1 - Logarithms and Their Properties
Chaper 5 Logarihmic Funcions 5.1 - Logarihms and Their Properies Suppose ha a populaion grows according o he formula P 10, where P is he colony size a ime, in hours. When will he populaion be 2500? We
More information1 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 informationLie 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 informationBEng (Hons) Telecommunications. Examinations for / Semester 2
BEng (Hons) Telecommunicaions Cohor: BTEL/14/FT Examinaions for 2015-2016 / Semeser 2 MODULE: ELECTROMAGNETIC THEORY MODULE CODE: ASE2103 Duraion: 2 ½ Hours Insrucions o Candidaes: 1. Answer ALL 4 (FOUR)
More information