COALGEBRAS, BRAIDINGS, AND DISTRIBUTIVE LAWS

Size: px
Start display at page:

Download "COALGEBRAS, BRAIDINGS, AND DISTRIBUTIVE LAWS"

Transcription

1 COALGEBRAS, BRAIDINGS, AND DISRIBUIVE LAWS SEFANO KASANGIAN, SEPHEN LACK, AND ENRICO M. VIALE o Aurelio Carboni on his 60th birthday ABSRAC. We show, for a monad, that oalgebra strutures on a -algebra an be desribed in terms of braidings, provided that the monad is equipped with an invertible distributive law satisfying the Yang-Baxter equation. 1. Introdution he aim of this note is to provide an equivalent desription of -oalgebra strutures on a -algebra, for a monad equipped with a speial kind of distributive law on a ategory C, and the omonad indued by the adjuntion C L R Alg() L R Our interest for suh oalgebras is motivated mainly by lassial desent theory: let f : R S be a morphism of ommutative unital rings, and onsider the indued funtor f!: R-mod S-mod defined by f!(n) = N R S (where S is seen as an R-module by restrition of salars). he desent problem for f onsists in reognizing when an S-module is of the form f!(n) for some R-module N. A lassial theorem [6, 2, 7], whih establishes a deep link between desent theory and the theory of (o)monads, asserts that, if f is faithfully flat, then an S-module is of the form f!(n) if and only if it is equipped with a -oalgebra struture, where is the omonad on S-mod indued by the adjuntion R-mod f! S-mod f f! f and f is the restrition of salars funtor. (For this reason, a -oalgebra struture on an S-module M is sometimes alled a desent datum for M.) It is also well-known that, for any morphism f : R S of ommutative unital rings, there are several equivalent ways Seond author supported by the Australian Researh Counil; third author by FNRS grant Mathematis Subjet Classifiation: 18C15, 18C20, 18D10, 16B50. Key words and phrases: Desent data, monads, distributive laws, Yang-Baxter equation. 1

2 of desribing what a -oalgebra struture for an S-module is, and a natural problem is to lift to a ategorial level these other desriptions of -oalgebra strutures. In a reent paper [11], Menini and Stefan, extending results by Nuss [12] on nonommutative rings, replae the situation 2 R-mod f! S-mod f f! f by C L R Alg() L R where is a monad on an arbitrary ategory C (indeed, even in the non-ommutative situation, f : S-mod R-mod is a monadi funtor, so that S-mod is equivalent to the ategory of algebras for the monad on R-mod indued by the adjuntion f! f ). In this ontext, they prove that, if the monad is equipped with a ompatible flip K : 2 2, then to give a -oalgebra struture on a -algebra X is equivalent to giving a symmetry on X, that is an involution X X satisfying some suitable onditions. Unfortunately, the following natural example, whih is a diret generalization of the lassial ase of ommutative rings, does not fit into their general ontext: let C be a braided monoidal ategory and let S be a monoid in C, then the braiding S,S : S S S S indues a natural isomorphism K : 2 2 on the monad = S : C C, but this natural isomorphism is not a flip unless the braiding is a symmetry and the monoid is ommutative. In this note we adapt the notions of ompatible flip and symmetry to enompass the previous example, as well as another example oming from the theory of bialgebras. In Setion 2 we introdue the notion of BD-law on a monad as a speial ase of distributive law in the sense of Bek [1]. Using a BD-law K, we an define K-braidings on a -algebra, and we want to show that K-braidings orrespond bijetively to -oalgebra strutures. here are two different methods: in Setion 3 we use K-braidings to define a ategory Brd(, K) equipped with a forgetful funtor V : Brd(, K) Alg(). We show, using the Bek riterion [10], that V is omonadi; and that the orresponding omonad is, so that Brd(, K) is isomorphi to Coalg( ). In Setion 4 we give a different proof based as far as possible on general fats about monads and distributive laws. his seond proof is quite long, but it seems to us of some interest, sine it shows that the bijetion between K-braidings and -oalgebra strutures is the natural bijetion indued by a pair of adjoint funtors. he desription of K-braidings we obtain in this way is slightly different, but in fat equivalent, to that used in Setion BD-laws on a monad o begin, we fix notation. A monad on a ategory C is a triple = ( : C C, m: 2, e: Id C )

3 3 onsisting of a funtor, and natural transformations m and e making the diagrams e 2 e (1) (2) m 3 m 2 m (3) 2 m m ommute. A -algebra is a pair (X, x: X X) in C suh that the diagrams ex X X (4) x 1 X x X (5) X x X x ommute. Given two monads and S on the same ategory C, a distributive law of over S is a natural transformation K : S S suh that the diagrams e (6) e K S S S es (7) Se K S S S 2 KS S S SK S 2 2 S K S K S 2 m S (8) K S m ms S (9) K S Sm ommute. We refer to [1, 3] for more details on monads and distributive laws. When the natural transformation K is an isomorphism, the definition of distributive law an be simplified, as in the following lemma: Lemma 1 Consider two monads and S on a ategory C, and a natural isomorphism K : S S. hen (8) implies (6) and (9) implies (7). Moreover, K satisfies (8) and (9) iff K 1 does. Proof. We prove that (9) implies (7); the proof of the other impliation is similar, and the rest of the statement is obvious. he proof is ontained in the following diagram, in

4 4 whih unlabelled regions ommute by naturality: es S K S S es Sm (2) Se S K S S e S 2 Se S es K 1 S K S K 1 2 S K S (9) (1) ms S. e S S K Definition 2 Let be a monad on a ategory C. A BD-law on is a natural transformation K : 2 2 suh that (B) K satisfies the Yang-Baxter equation: 3 K 3 K 3 K 3 K (10) 3 K 3 K (D) K is a distributive law (that is, it satisfies equations (6 9).) A BCD-law on is a BD-law suh that (C) the monad is K-ommutative: 2 K 2 (11) m m A BD-law or BCD-law is said to be invertible if the natural transformation K is so. Remark 3 One again, as stated in Lemma 1 for the distributivity onditions, a natural isomorphism K : 2 2 satisfies onditions (B) or (C) iff K 1 does. Remark 4 If C is an arbitrary monoidal ategory, and is a monoid in C, one an define a BD-law or BCD-law on as above. A monoid equipped with an invertible BCD-law has been alled a quasi-ommutative monoid by Davydov [5], sine the BCD-law provides a kind of loal braiding with respet to whih the monoid is ommutative.

5 Remark 5 If K is involutive that is, K 2 = 1 eah of the onditions (8) and (9) implies the other. his fat, together with Lemma 1, means that ompatible flips in the sense of Menini and Stefan [11] are preisely the involutive BCD-laws. Example 6 Let C = (C,, I,...) be a monoidal ategory and S = (S, m S, e S ) a monoid in C. he monoid S indues a monad on C in the following way: = S : C C = 1 m S : X S S X S ex = 1 e S : X X I X S 2.1. If C is braided, with braiding = { X,Y : X Y Y X}, then there is an invertible BD-law K on defined by = 1 S,S : X S S X S S. In this ase, ondition (B) is preisely the Yang-Baxter equation; by naturality of the braiding, onditions (8) and (9) redue to the following equations, whih hold in any braided monoidal ategory: = = his BD-law is a BCD-law preisely when the monoid S is ommutative; it is involutive if and only if S,S is so, in partiular if the braiding is a symmetry Let K be a field and take as C the ategory of K-vetor spaes. Let H be a obraided bialgebra with universal form r : H H I; there is a natural isomorphism of H- omodules r V,W : V W W V defined by V W τ W V H W H V 1 τ 1 H H W V r 1 1 W V where is the oation and τ is the standard twist: see [9]. If S is any H-omodule algebra (in partiular, one an take S = H), then we have an invertible BD-law K on defined by = 1 r S,S : X S S X S S. Indeed, onditions (8-10) follow from [9, Proposition VIII.5.2], using the fat that the multipliation m S : S S S is a homomorphism of H-omodules. Example 7 If f : R S is a morphism of unital rings, with R ommutative, we an speialize Example 2.1 by taking C = R-mod, so that K is defined by the standard twist S S S S. his is possible also if R is not ommutative, provided its image lies in the entre of S : taking now C = R-R-bimod, the standard twist on S an be defined and gives one again an invertible BD-law on. If we drop the entrality ondition the standard twist an no longer be defined, but one an use the additivity of the ategory of bimodules to define a different BD-law. In fat, if C is an additive ategory and is any monad on C, then there is an involutive BCD-law K on defined by K = (e + e) m 2 ; see [11]. his ase generalizes results on non-ommutative rings established in [4, 12]. 5

6 3. Coalgebras and braidings For the reader s onveniene, let us reall how the definition of oalgebra for a omonad speializes when the omonad is of the form. Definition 8 Let = (, m, e) be a monad on a ategory C and onsider the omonad on Alg() indued by the adjuntion 6 C L R Alg() L R A -oalgebra struture on a -algebra (X, x: X X) is a morphism r : X X suh that X r 2 r X X X X x (12) 1 X r X (13) x r (14) r r X X X ex We denote by -oalg(x, x) the set of -oalgebra strutures on a -algebra (X, x). Remark 9 For all X C, the morphism ex : X is a -oalgebra struture on the free -algebra L X = ( X, ). his is the (objet part of the) anonial omparison funtor C Coalg( ). Definition 10 Let = (, m, e) be a monad on a ategory C and let K : 2 2 be a BD-law. A K-braiding on a -algebra (X, x: X X) is a morphism : X X suh that X X ex (15) X 1 X x (16) x (17) X X We denote by K-Brd(X, x) the set of K-braidings on a -algebra (X, x). Remark 11 If K is invertible, ondition (17) means that is a morphism : (X, x) (X, x) in Alg(), where is the lifting of on Alg() indued by the distributive law K 1. Remark 12 We shall see in Proposition 16 that if K is invertible or involutive then the same is true of any K-braiding, whene by Corollary 18 it will follow that if K is an involutive BCD-law, then K-braidings are preisely symmetries in the sense of Menini and Stefan [11].

7 Remark 13 If K is a BD-law on, then is a K-braiding on L X, for all X C. Indeed, onditions (16) and (17) orrespond respetively to onditions (10) and (9), while ondition (15) is the pasting of (1) and (6). In the bijetion stated in Corollary 15, orresponds to the -oalgebra struture ex of Remark 9. If is a monad on a ategory C and K : 2 2 is a BD-law, we write Brd(, K) for the ategory having pairs (X, x) Alg(), K-Brd(X, x) as objets. An arrow f : (X, x), (X, x ), in Brd(, K) is an arrow between the underlying -algebras suh that the diagram ommutes. We are ready to state our main result. X f X X f X heorem 14 Let = (, m, e) be a monad on a ategory C and let K : 2 2 be a BD-law on. he forgetful funtor V : Brd(, K) Alg() is omonadi, and the orresponding omonad on Alg() is the omonad indued by the adjuntion L R between C and Alg(). Proof. We show that V has a left adjoint and then apply Bek s theorem. he free - algebra funtor L : C Alg() fatorizes as L = V J, where J : C Brd(, K) is the funtor sending an objet X of C to the algebra ( X, ) equipped with the K-braiding :. he ounit ɛ : L R 1 may be seen as a natural transformation V JR = L R 1. For an objet (X, x, ) of Brd(, K), write β : X X for the omposite and observe that, by ommutativity of X ex X X 7 X e X x ex x (17) X ex X X

8 8 and X e X ex (16) X e X ex this makes β a map in Brd(, K) from (X, x, ) to ( X,, ). his gives the omponent at (X, x, ) of a natural transformation β : 1 JR V. he triangle equation ɛv.v β = 1 is preisely equation (15), while the other triangle equation JR ɛ.βjr = 1 follows easily from the definitions of BD-law and of -algebra. hus there is an adjuntion V JR, whih learly indues the same omonad as L R. It remains to verify the Bek ondition. Let f, g : (X, x, ) (Z, z, ) be morphisms in Brd(, K), and let (W, w) i (X, x) u f g v (Z, z) be a split equalizer diagram in Alg(), with ui = 1, iu = gv, and fv = 1. Sine i is (split) moni, the only possibility for a K-braiding : W W on (W, w) ompatible with i is given by W i X X u W and we need only hek that this does indeed give a braiding; the fat that the resulting diagram is an equalizer in Brd(, K) is then obvious. hus we must hek equations (15,16,17); instead, we allow the reader to ontemplate the following diagrams at his or her leisure: W i X X u W ew ex W i X 1 X u W 1 x w

9 9 2 u 2 W KW 2 W 2 g 2 Z 2 i 2 g 2 Z 2 i 2 W KW 2 W 2 i 2 i 2 f 2 v 1 2 f 2 u 2 i 2 u 2 W KW 2 W 2 W 2 i KW 2 W 2u 2 W 2 i w x W i X mw X u W. Corollary 15 Let = (, m, e) be a monad on a ategory C and let K : 2 2 be a BD-law on. For (X, x) a -algebra, onsider the map Ψ (X,x) : K-Brd(X, x) -oalg(x, x) (: X X) (r : X ex X X ) and the funtor Ψ: Brd(, K) Coalg( ) (X, x), f (X, x ), (X, x, Ψ()) f (X, x, Ψ( )) 1. he funtor Ψ is an isomorphism of ategories; 2. he map Ψ (X,x) is bijetive. Proof. Sine the forgetful funtor V : Brd(, K) Alg() is omonadi, the indued omparison funtor Ψ: Brd(, K) Coalg( ) is an isomorphism of ategories and so it indues a bijetion on objets.

10 Proposition 16 For a BD-law K : 2 2 we have the following fats about a K- braiding : X X on an algebra (X, x): 1. he diagrams 10 3 X 3 X 2 3 X X (18) x X 2 x (19) X X x ommute; 2. If K is invertible then so is ; 3. If K is involutive then so is ; 4. If K is a BCD-law then the diagram ommutes. X X (20) x x X Proof. In eah ase the proof goes as follows. Modify the definition of K-braiding so that the extra ondition is assumed part of the struture, then hek that the modified ategory Brd(, K) is still omonadi via the same omonad. his involves (i) proving that the ofree objets ( X,, ) have the required property, and (ii) proving that in the split equalizer diagram in the proof of heorem 14, the indued morphism = u.. i : W W satisfies the ondition if : X X does so. In eah ase (i) is entirely straightforward: for example, the fat that the ofree objets satisfy (18) is preisely (9). We therefore hek only (ii). 1. If satisfies (18), then so does by ommutativity of the diagram 2 W mw 2 i 2u 2 W KW 2 W W i X x 2 u w X u W

11 while (19) is obtained by pasting together (17) and (18). 2 and 3. If is invertible, then a straightforward alulation shows that u. 1. i is inverse to u.. i. 4. If x = x then the diagram ommutes and so w = w. X i x W X i w W 1 x u X u W W w Remark 17 If K is a distributive law, ondition (18) means that is a morphism : (X, x) (X, x) in Alg(), where is the lifting of to Alg() indued by the distributive law K. In fat we an use the Proposition to give two alternative formulations of the definition. One of them will be used in the following setion, the other to make the onnetion with the symmetries of [11]. Corollary 18 In the definition of K-braiding, ondition (17) an be replaed by (19), while if K is a BCD-law then (15) an be replaed by (20). Proof. We have seen that for a K-braiding (19) always holds; onversely (17) follows easily from (19) by omposing with e X : X. Similarly, if K is a BCDlaw then (20) holds for any K-braiding, while (15) follows from (20) by omposing with ex : X X. If K is an involutive BCD-law on a monad, then a symmetry on a -algebra (X, x), was defined in [11] to be an involution : X X satisfying (16, 17, 20); ombining the proposition and the orollary one now sees as promised that this is preisely a K-braiding Another proof We proved our main theorem in the previous setion; here we provide an alternative proof, whih may be of interest to some readers. It exhibits the bijetion whih is the objet part of the isomorphism Φ of Corollary 15 as being part of the natural bijetion (between hom-sets) of an adjuntion. o do this, we use the definition of K-braiding involving (19) rather than (17); see Corollary 18.

12 Proposition 19 Let = (, m, e) be a monad on a ategory C and let K : 2 2 be an invertible BD-law on. For (X, x) a -algebra, we have a bijetion given by Ψ (X,x) : K-Brd(X, x) -oalg(x, x) K-Brd(X, x) = -oalg(x, x) (: X X) (r : X ex X X ) Ψ 1 (X,x) : -oalg(x, x) K-Brd(X, x) (r : X X) (: X r x X ) As explained above, the proposition an be dedued from Corollary 15; our alternative proof oupies the remainder of the paper. Let and S be monads on a ategory C. A morphism of monads is a natural transformation ϕ: S suh that 12 S 2 ϕ 2 2 m S (21) ϕ m e Id C e S (22) ϕ Following [1], suh a morphism ϕ indues a funtor ϕ : Alg() Alg(S) defined by ϕ (X, x: X X) = (X, ϕx x: SX X X). Moreover, ϕ has a left adjoint ϕ!: Alg(S) Alg() sending an S-algebra (Y, y) to the objet ϕ!(y, y) in the oequalizer y SY Y ϕy my 2 Y q ϕ!(y, y) in Alg(), provided that suh a oequalizer exists. Indeed, if f : (Y, y) ϕ (X, x) is a morphism of S-algebras, then x. f : Y X oequalizes y and my. ϕy. Conversely, from g : ϕ!(y, y) (X, x), we get g.q.ey : (Y, y) ϕ (X, x). If K : S S is a distributive law of over S, we an onsider the omposite monad S on C. Expliitly, S = (S : C C, S S SK S 2 2 mm S, Id C ee S ) Moreover, there are two morphisms of monads as in S ɛ 1 =Se ɛ 2 =e S.

13 Now, for any -algebra (X, x: X X) and S-algebra (Y, y : SY Y ), the adjuntion ɛ 2! ɛ 2 gives a natural bijetion 13 Ψ: Alg(S)[ɛ 2!(X, x), ɛ 1!(Y, y)] Alg()[(X, x), ɛ 2ɛ 1!(Y, y)] he bijetion of Proposition 19 will turn out to be a partiular ase of this natural bijetion. o see this, we give an expliit desription of Ψ and of the hom-sets involved. First of all, let us reall from [1] that the oequalizer defining ɛ 2!(X, x) always exists. In fat, it is given by the solid part of the following diagram in Alg(S) Se X SeX S X S x S S X Sx SX with ation on SX given by S SX S S 2 X S 2 x S 2 X SX Indeed, one easily verifies that the dotted arrows satisfy the equations for a split oequalizer [2]. Reall also that if f is a morphism of S-algebras oequalizing S x and S, then the indued S-algebra map out of SX is f.sex. Unfortunately, the existene of the oequalizer defining ɛ 1!(Y, y) is not automati. We need the following lemma, whih makes sense beause of Lemma 1: Lemma 20 Consider two monads S and on a ategory C, and let K : S S be an invertible distributive law of over S. Consider the omposite monad S indued by K and the omposite monad S indued by K 1. hen K : S S is a morphism of monads, and it satisfies the following equations where η 1 = e and η 2 = es. S η 2 η 1 S K ɛ 1 ɛ 2 S Proof. he equations ɛ 1 = Kη 2 and ɛ 2 = Kη 1 are onditions (6) and (7), and they imply ondition (22). As far as ondition (21) is onerned, let us give the idea of the proof, instead of the omplete alulation. (his ould be formalized using the string alulus

14 of [8].) hink of K as a braiding between and S. hen ondition (21) amounts to the following equation = whih an be proved using the distributivity equations three times. Indeed, the distributivity admits the following graphial representation (this is ondition (8)) = 14 As a onsequene of the previous lemma, ɛ 1!: Alg(S) Alg(S) an be obtained as Alg(S) η 2! Alg(S) (K 1 ) Alg(S) and then ɛ 1!(Y, y) an be desribed by the following oequalizer in Alg(S) esy ey (K 1 ) (L S (SY )) KSY L S (SY ) Sy my S y m Y.SKY (K 1 ) (L S (Y )) KY L S (Y ) y Y with ation on Y given by S 2 Y SmY S Y K 1Y SY y Y. We are now ready to desribe the bijetion Ψ. Lemma 21 Consider two monads S and on a ategory C, and let K : S S be an invertible distributive law of over S. For any -algebra (X, x) and S-algebra (Y, y) :

15 15 (i) he hom-set Alg(S)[(Y, y), ɛ 1(ɛ 2!(X, x))] is the set of morphisms r : Y SX suh that SY Sr S 2 X y Y (12) r ommutes. (ii) he hom-set Alg(S)[ɛ 1!(Y, y), ɛ 2!(X, x)] is the set of morphisms : Y SX suh that 2 SY KY S Y S SSX SX 2 y 2 Y (19) SX ommutes. my Y SX Sx S X (iii) he natural bijetion Ψ: Alg(S)[ɛ 1!(Y, y), ɛ 2!(X, x)] Alg(S)[(Y, y), ɛ 1(ɛ 2!(X, x))] indued by the adjuntion ɛ 1! ɛ 1 is given by Ψ(): Y ey Y SX Ψ 1 (r): Y r SX S X Sx SX. Proof. Following the desription of ϕ! ϕ given at the beginning of this setion, we have Ψ() and Ψ 1 (r) given respetively by Y ey Y e Y S Y K 1 SY y Y SX Y e Y S Y S r S SX S SS X n X S X Sx SX whih are easily seen to redue to formulas given in (iii). For r : Y SX, to be a morphism of S-algebras means that SY Sr S 2 X SeSX S SX y Y r SX S 2 X S 2 x S S 2 X ommutes, whih immediately redues to (12) by (6) and (4).

16 16 For : Y SX, to be a morphism of S-algebras means ommutativity of S 2 Y S S SX S SS X SSx SSX SmY S Y K 1 Y SY y Y SX whih, by (8) and (9), redues to (19). his is the best we an do working at this level of generality. From now on, we assume S = and (X, x) = (Y, y). We now ombine the next two lemmas with the previous one to omplete the proof of Proposition 19. Lemma 22 Let be a monad on a ategory C, and let K : 2 2 be an invertible distributive law on. Fix a -algebra (X, x). In the bijetion of Lemma 21, the map r : X X satisfies ondition (13) iff = Ψ 1 (r): X X satisfies ondition (15). Proof. Condition (15) says preisely that Ψ() satisfies (13). Lemma 23 Let be a monad on a ategory C, and let K : 2 2 be an invertible BD-law on. Fix a -algebra (X, x). In the bijetion of Lemma 21, the map r : X X satisfies ondition (14) iff = Ψ 1 (r): X X satisfies ondition (16). Proof. (14) (16) : 2 X 2 r 2 X 2 r 3 X K X 2 r (14) 3 X 3 ex 3 X 3 r 4 X 3 X 3 ex K X 3 X 2 x 3 X 3 r 4 X (1) 1 (12) 2 x 2 2 X 2 r 3 X (10) 3 X 2 X K X K X 2 x 3 X 3 X 2 r ()

17 17 (16) (14) : X ex ex ex X e X 2 e X X X (7) 2 e X X X (6) e X X ex (16) (6) ex he proof of Proposition 19 is now omplete. Referenes [1] J. Bek, Distributive laws, in Seminar on riples and Categorial Homology heory (Leture Notes in Mathematis 80), pp , Springer, Berlin, [2] F. Boreux, Handbook of ategorial algebra I, Cambridge University Press, [3] F. Boreux, Handbook of ategorial algebra II, Cambridge University Press, [4] M. Cipolla, Disesa fedelmente piatta dei moduli, Rend. Cir. Mat. Palermo 25:43 46, [5] A. Davydov, Quasiommutative monoids, Leture at Australian Category Seminar, 21 January [6] A. Grothendiek, ehnique de desente et théorèmes d existene en géométrie algébrique, I : Généralités, desente par morphismes fidèlements plats, Séminaire Bourbaki 190 ( ). [7] G. Janelidze and W. holen, Faets of desent III: monadi desent for rings and algebras, preprint, [8] A. Joyal and R. Street, Geometry of tensor alulus I, Adv. Math. 88:55 112, [9] C. Kassel, Quantum groups (Graduate exts in Mathematis 155) Springer-Verlag, New York, [10] S. Ma Lane, Categories for the working mathematiian (Graduate exts in Mathematis 5), Springer, New York-Berlin, 1971.

18 [11] C. Menini and D. Stefan, Desent theory and Amitsur ohomology of triples, J. Algebra 266: , [12] P. Nuss, Nonommutative desent and non-abelian ohomology, K-heory 12:23 74, Dipartimento di Matematia Università di Milano Via Saldini 50 I Milano, Italia Shool of Quantitative Methods and Mathematial Sienes University of Western Sydney Loked Bag 1797 Penrith South DC NSW 1797 Australia Département de Mathématique Pure et Appliquée Université atholique de Louvain Chemin du Cylotron 2 B 1348 Louvain-la-Neuve, Belgique Stefano.Kasangian@mat.unimi.it, s.lak@uws.edu.au, vitale@math.ul.a.be 18

Notes on the bicategory of W*-bimodules

Notes on the bicategory of W*-bimodules Submitted to Journal of the Mathematial Soiety of Japan Notes on the biategory of W*-bimodules By Yusuke Sawada and Shigeru Yamagami (Reeived July 6, 2017) (Revised Jan. 17, 2018) Abstrat. Categories of

More information

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

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

More information

The perverse t-structure

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

More information

Maximum Entropy and Exponential Families

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

More information

Discrete Bessel functions and partial difference equations

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

More information

Parametric Solutions of Pell s Equation

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

More information

Advanced Computational Fluid Dynamics AA215A Lecture 4

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

More information

WHAT DOES THE CLASSIFYING SPACE OF A CATEGORY CLASSIFY? Introduction. Homology, Homotopy and Applications, vol. 7(1), 2005, pp MICHAEL WEISS

WHAT DOES THE CLASSIFYING SPACE OF A CATEGORY CLASSIFY? Introduction. Homology, Homotopy and Applications, vol. 7(1), 2005, pp MICHAEL WEISS Homology, Homotopy and Appliations, vol. 7(1), 2005, pp.185 195 Introdution WHAT DOES THE CLASSIFYING SPACE OF A CATEGORY CLASSIFY? MICHAEL WEISS (ommuniated by Graham Ellis) Abstrat The lassifying spae

More information

SOME PROPERTIES OF LOCALLY CONFORMAL SYMPLECTIC MANIFOLDS

SOME PROPERTIES OF LOCALLY CONFORMAL SYMPLECTIC MANIFOLDS SOME PROPERTIES OF LOCALLY CONFORMAL SYMPLECTIC MANIFOLDS STEFAN HALLER Abstrat. The aim of this note is to give an overview of what loally onformal sympleti manifolds are and to present some results,

More information

arxiv: v3 [math.ct] 20 May 2015

arxiv: v3 [math.ct] 20 May 2015 CATEGORIES IN CONTROL arxiv:1405.6881v3 [math.ct] 20 May 2015 JOHN C. BAEZ AND JASON ERBELE Abstrat. Control theory uses signal-flow diagrams to desribe proesses where real-valued funtions of time are

More information

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

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

More information

NOTES ON GROUPOIDS, IMAGINARIES AND INTERNAL COVERS

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

More information

Counting Idempotent Relations

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

More information

Ordered fields and the ultrafilter theorem

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

More information

Hankel Optimal Model Order Reduction 1

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

More information

Nonreversibility of Multiple Unicast Networks

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

More information

the following action R of T on T n+1 : for each θ T, R θ : T n+1 T n+1 is defined by stated, we assume that all the curves in this paper are defined

the following action R of T on T n+1 : for each θ T, R θ : T n+1 T n+1 is defined by stated, we assume that all the curves in this paper are defined How should a snake turn on ie: A ase study of the asymptoti isoholonomi problem Jianghai Hu, Slobodan N. Simić, and Shankar Sastry Department of Eletrial Engineering and Computer Sienes University of California

More information

Surface group representations, Higgs bundles, and holomorphic triples

Surface group representations, Higgs bundles, and holomorphic triples Surfae group representations, Higgs bundles, and holomorphi triples Steven B. Bradlow 1,2 Department of Mathematis, University of Illinois, Urbana, IL 61801, USA E-mail: bradlow@math.uiu.edu Osar Garía

More information

The Hanging Chain. John McCuan. January 19, 2006

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

More information

arxiv: v2 [cs.dm] 4 May 2018

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

More information

Dual Adjunctions Between Algebras and Coalgebras

Dual Adjunctions Between Algebras and Coalgebras Dual Adjunctions Between Algebras and Coalgebras Hans E. Porst Department of Mathematics University of Bremen, 28359 Bremen, Germany porst@math.uni-bremen.de Abstract It is shown that the dual algebra

More information

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

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

More information

The Erwin Schrödinger International Boltzmanngasse 9 Institute for Mathematical Physics A-1090 Wien, Austria

The Erwin Schrödinger International Boltzmanngasse 9 Institute for Mathematical Physics A-1090 Wien, Austria ESI The Erwin Shrödinger International Boltzmanngasse 9 Institute for Mathematial Physis A-1090 Wien, Austria Moduli Spaes of Holomorphi Triples over Compat Riemann Surfaes Steven B. Bradlow Osar Garia-Prada

More information

arxiv: v3 [cs.ai] 8 Feb 2019

arxiv: v3 [cs.ai] 8 Feb 2019 Disintegration and Bayesian Inversion via String Diagrams K E N T A C H O and B A R T J A C O B S ariv:1709.00322v3 [s.ai] 8 Feb 2019 National Institute of Informatis 2-1-2 Hitotsubashi, Chiyoda-ku, Tokyo

More information

TENSOR FORM OF SPECIAL RELATIVITY

TENSOR FORM OF SPECIAL RELATIVITY TENSOR FORM OF SPECIAL RELATIVITY We begin by realling that the fundamental priniple of Speial Relativity is that all physial laws must look the same to all inertial observers. This is easiest done by

More information

1 Introdution In reent years the idea of Quantum Field Theories (QFT) endowed with Quantum Group [1] symmetries has attrated onsiderable interest and

1 Introdution In reent years the idea of Quantum Field Theories (QFT) endowed with Quantum Group [1] symmetries has attrated onsiderable interest and July 1996, rev. Nov. 1996 LMU-TPW 96-17 On Bose-Fermi Statistis, Quantum Group Symmetry, and Seond Quantization 1 2 Gaetano Fiore Sektion Physik der Ludwig-Maximilians-Universitat Munhen Theoretishe Physik

More information

Some GIS Topological Concepts via Neutrosophic Crisp Set Theory

Some GIS Topological Concepts via Neutrosophic Crisp Set Theory New Trends in Neutrosophi Theory and Appliations A.A.SALAMA, I.M.HANAFY, HEWAYDA ELGHAWALBY 3, M.S.DABASH 4,2,4 Department of Mathematis and Computer Siene, Faulty of Sienes, Port Said University, Egypt.

More information

ON A PROCESS DERIVED FROM A FILTERED POISSON PROCESS

ON A PROCESS DERIVED FROM A FILTERED POISSON PROCESS ON A PROCESS DERIVED FROM A FILTERED POISSON PROCESS MARIO LEFEBVRE and JEAN-LUC GUILBAULT A ontinuous-time and ontinuous-state stohasti proess, denoted by {Xt), t }, is defined from a proess known as

More information

LECTURE 22: MAPPING DEGREE, POINCARE DUALITY

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

More information

A Characterization of Wavelet Convergence in Sobolev Spaces

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

More information

After the completion of this section the student should recall

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

More information

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

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

More information

Morita equivalence for regular algebras

Morita equivalence for regular algebras Morita equivalence for regular algebras F. Grandjean E.M. Vitale Résumé: Nous étudions les catégories des modules réguliers sur les algèbres régulières, afin de généraliser certains résultats classiques

More information

The gravitational phenomena without the curved spacetime

The gravitational phenomena without the curved spacetime The gravitational phenomena without the urved spaetime Mirosław J. Kubiak Abstrat: In this paper was presented a desription of the gravitational phenomena in the new medium, different than the urved spaetime,

More information

A new insight into Serre s reduction problem

A new insight into Serre s reduction problem A new insight into Serre s redution problem Thomas Cluzeau, Alban Quadrat RESEARCH REPORT N 8629 November 214 Projet-Team Diso ISSN 249-6399 ISRN INRIA/RR--8629--FR+ENG A new insight into Serre s redution

More information

On maximal inequalities via comparison principle

On maximal inequalities via comparison principle Makasu Journal of Inequalities and Appliations (2015 2015:348 DOI 10.1186/s13660-015-0873-3 R E S E A R C H Open Aess On maximal inequalities via omparison priniple Cloud Makasu * * Correspondene: makasu@uw.a.za

More information

Concerning the Numbers 22p + 1, p Prime

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

More information

F = F x x + F y. y + F z

F = F x x + F y. y + F z ECTION 6: etor Calulus MATH20411 You met vetors in the first year. etor alulus is essentially alulus on vetors. We will need to differentiate vetors and perform integrals involving vetors. In partiular,

More information

Quantum Mechanics: Wheeler: Physics 6210

Quantum Mechanics: Wheeler: Physics 6210 Quantum Mehanis: Wheeler: Physis 60 Problems some modified from Sakurai, hapter. W. S..: The Pauli matries, σ i, are a triple of matries, σ, σ i = σ, σ, σ 3 given by σ = σ = σ 3 = i i Let stand for the

More information

On the Geometrical Conditions to Determine the Flat Behaviour of the Rotational Curves in Galaxies

On the Geometrical Conditions to Determine the Flat Behaviour of the Rotational Curves in Galaxies On the Geometrial Conditions to Determine the Flat Behaviour of the Rotational Curves in Galaxies Departamento de Físia, Universidade Estadual de Londrina, Londrina, PR, Brazil E-mail: andrenaves@gmail.om

More information

MATH 101B: ALGEBRA II PART A: HOMOLOGICAL ALGEBRA

MATH 101B: ALGEBRA II PART A: HOMOLOGICAL ALGEBRA MATH 101B: ALGEBRA II PART A: HOMOLOGICAL ALGEBRA These are notes for our first unit on the algebraic side of homological algebra. While this is the last topic (Chap XX) in the book, it makes sense to

More information

HILLE-KNESER TYPE CRITERIA FOR SECOND-ORDER DYNAMIC EQUATIONS ON TIME SCALES

HILLE-KNESER TYPE CRITERIA FOR SECOND-ORDER DYNAMIC EQUATIONS ON TIME SCALES HILLE-KNESER TYPE CRITERIA FOR SECOND-ORDER DYNAMIC EQUATIONS ON TIME SCALES L ERBE, A PETERSON AND S H SAKER Abstrat In this paper, we onsider the pair of seond-order dynami equations rt)x ) ) + pt)x

More information

(, ) Anti Fuzzy Subgroups

(, ) Anti Fuzzy Subgroups International Journal of Fuzzy Mathematis and Systems. ISSN 2248-9940 Volume 3, Number (203), pp. 6-74 Researh India Publiations http://www.ripubliation.om (, ) Anti Fuzzy Subgroups P.K. Sharma Department

More information

A Recursive Approach to the Kauffman Bracket

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

More information

Stability of alternate dual frames

Stability of alternate dual frames Stability of alternate dual frames Ali Akbar Arefijamaal Abstrat. The stability of frames under perturbations, whih is important in appliations, is studied by many authors. It is worthwhile to onsider

More information

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

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

More information

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

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

More information

SPLINE ESTIMATION OF SINGLE-INDEX MODELS

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

More information

A Logic of Local Graph Shapes

A Logic of Local Graph Shapes CTIT Tehnial Report TR CTIT 03 35, University of Twente, 2003 A Logi of Loal Graph Shapes Arend Rensink Department of Computer Siene, University of Twente P.O.Box 27, 7500 AE, The Netherlands rensink@s.utwente.nl

More information

arxiv:math.co/ v1 2 Aug 2006

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

More information

EXACT TRAVELLING WAVE SOLUTIONS FOR THE GENERALIZED KURAMOTO-SIVASHINSKY EQUATION

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

More information

LECTURE NOTES FOR , FALL 2004

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

More information

Journal of Inequalities in Pure and Applied Mathematics

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

More information

SERIJA III

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

More information

Asymptotic non-degeneracy of the solution to the Liouville Gel fand problem in two dimensions

Asymptotic non-degeneracy of the solution to the Liouville Gel fand problem in two dimensions Comment. Math. Helv. 2 2007), 353 369 Commentarii Mathematii Helvetii Swiss Mathematial Soiety Asymptoti non-degeneray of the solution to the Liouville Gel fand problem in two dimensions Tomohio Sato and

More information

QUANTUM MECHANICS II PHYS 517. Solutions to Problem Set # 1

QUANTUM MECHANICS II PHYS 517. Solutions to Problem Set # 1 QUANTUM MECHANICS II PHYS 57 Solutions to Problem Set #. The hamiltonian for a lassial harmoni osillator an be written in many different forms, suh as use ω = k/m H = p m + kx H = P + Q hω a. Find a anonial

More information

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

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

More information

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

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

More information

Some Properties on Nano Topology Induced by Graphs

Some Properties on Nano Topology Induced by Graphs AASCIT Journal of anosiene 2017; 3(4): 19-23 http://wwwaasitorg/journal/nanosiene ISS: 2381-1234 (Print); ISS: 2381-1242 (Online) Some Properties on ano Topology Indued by Graphs Arafa asef 1 Abd El Fattah

More information

EDGE-DISJOINT CLIQUES IN GRAPHS WITH HIGH MINIMUM DEGREE

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

More information

Wuming Li and Fan Yang

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

More information

Review of Force, Stress, and Strain Tensors

Review of Force, Stress, and Strain Tensors Review of Fore, Stress, and Strain Tensors.1 The Fore Vetor Fores an be grouped into two broad ategories: surfae fores and body fores. Surfae fores are those that at over a surfae (as the name implies),

More information

Cellularity, composition, and morphisms of algebraic weak factorization systems

Cellularity, composition, and morphisms of algebraic weak factorization systems Cellularity, composition, and morphisms of algebraic weak factorization systems Emily Riehl University of Chicago http://www.math.uchicago.edu/~eriehl 19 July, 2011 International Category Theory Conference

More information

Quantum Groups and Link Invariants

Quantum Groups and Link Invariants Quantum Groups and Link Invariants Jenny August April 22, 2016 1 Introduction These notes are part of a seminar on topological field theories at the University of Edinburgh. In particular, this lecture

More information

Remark 4.1 Unlike Lyapunov theorems, LaSalle s theorem does not require the function V ( x ) to be positive definite.

Remark 4.1 Unlike Lyapunov theorems, LaSalle s theorem does not require the function V ( x ) to be positive definite. Leture Remark 4.1 Unlike Lyapunov theorems, LaSalle s theorem does not require the funtion V ( x ) to be positive definite. ost often, our interest will be to show that x( t) as t. For that we will need

More information

SURFACE WAVES OF NON-RAYLEIGH TYPE

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

More information

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

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

More information

The Unified Geometrical Theory of Fields and Particles

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

More information

Most results in this section are stated without proof.

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

More information

Quasi-Monte Carlo Algorithms for unbounded, weighted integration problems

Quasi-Monte Carlo Algorithms for unbounded, weighted integration problems Quasi-Monte Carlo Algorithms for unbounded, weighted integration problems Jürgen Hartinger Reinhold F. Kainhofer Robert F. Tihy Department of Mathematis, Graz University of Tehnology, Steyrergasse 30,

More information

A NETWORK SIMPLEX ALGORITHM FOR THE MINIMUM COST-BENEFIT NETWORK FLOW PROBLEM

A NETWORK SIMPLEX ALGORITHM FOR THE MINIMUM COST-BENEFIT NETWORK FLOW PROBLEM NETWORK SIMPLEX LGORITHM FOR THE MINIMUM COST-BENEFIT NETWORK FLOW PROBLEM Cen Çalışan, Utah Valley University, 800 W. University Parway, Orem, UT 84058, 801-863-6487, en.alisan@uvu.edu BSTRCT The minimum

More information

Math 220A - Fall 2002 Homework 8 Solutions

Math 220A - Fall 2002 Homework 8 Solutions Math A - Fall Homework 8 Solutions 1. Consider u tt u = x R 3, t > u(x, ) = φ(x) u t (x, ) = ψ(x). Suppose φ, ψ are supported in the annular region a < x < b. (a) Find the time T 1 > suh that u(x, t) is

More information

The Electromagnetic Radiation and Gravity

The Electromagnetic Radiation and Gravity International Journal of Theoretial and Mathematial Physis 016, 6(3): 93-98 DOI: 10.593/j.ijtmp.0160603.01 The Eletromagneti Radiation and Gravity Bratianu Daniel Str. Teiului Nr. 16, Ploiesti, Romania

More information

Hamacher Sum and Hamacher Product of Fuzzy Matrices

Hamacher Sum and Hamacher Product of Fuzzy Matrices Intern J Fuzzy Maematial Arhive Vol 13, No, 017, 191-198 ISSN: 30 34 (P), 30 350 (online) Published on Deember 017 wwwresearhmasiorg DOI: http://dxdoiorg/10457/fmav13na9 International Journal of amaher

More information

University of Groningen

University of Groningen University of Groningen Port Hamiltonian Formulation of Infinite Dimensional Systems II. Boundary Control by Interonnetion Mahelli, Alessandro; van der Shaft, Abraham; Melhiorri, Claudio Published in:

More information

Packing Plane Spanning Trees into a Point Set

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

More information

Aharonov-Bohm effect. Dan Solomon.

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

More information

DESCENT IN TRIANGULATED CATEGORIES

DESCENT IN TRIANGULATED CATEGORIES DESCENT IN TRIANGULATED CATEGORIES PAUL BALMER Abstract. We establish effective descent for faithful ring objects in tensor triangulated categories. More generally, we discuss descent for monads in triangulated

More information

sset(x, Y ) n = sset(x [n], Y ).

sset(x, Y ) n = sset(x [n], Y ). 1. Symmetric monoidal categories and enriched categories In practice, categories come in nature with more structure than just sets of morphisms. This extra structure is central to all of category theory,

More information

Non-Abelian quantum Hall states and their quasiparticles: From the pattern of zeros to vertex algebra

Non-Abelian quantum Hall states and their quasiparticles: From the pattern of zeros to vertex algebra Non-Abelian quantum Hall states and their quasipartiles: From the pattern of zeros to vertex algebra Yuan-Ming Lu, 1 Xiao-Gang Wen,, Zhenghan Wang, 4 and Ziqiang Wang 1 1 Department of Physis, Boston College,

More information

Physical Laws, Absolutes, Relative Absolutes and Relativistic Time Phenomena

Physical Laws, Absolutes, Relative Absolutes and Relativistic Time Phenomena Page 1 of 10 Physial Laws, Absolutes, Relative Absolutes and Relativisti Time Phenomena Antonio Ruggeri modexp@iafria.om Sine in the field of knowledge we deal with absolutes, there are absolute laws that

More information

Structural Reconfiguration of Systems under Behavioral Adaptation

Structural Reconfiguration of Systems under Behavioral Adaptation Strutural Reonfiguration of Systems under Behavioral Adaptation Carlos Canal a, Javier Cámara b, Gwen Salaün a Department of Computer Siene, University of Málaga, Spain b Department of Informatis Engineering,

More information

The homopolar generator: an analytical example

The homopolar generator: an analytical example The homopolar generator: an analytial example Hendrik van Hees August 7, 214 1 Introdution It is surprising that the homopolar generator, invented in one of Faraday s ingenious experiments in 1831, still

More information

A Channel-Based Perspective on Conjugate Priors

A Channel-Based Perspective on Conjugate Priors A Channel-Based Perspetive on Conjugate Priors Simons Institute, Berkeley Bart Jaobs, Radboud University Nijmegen bart@s.ru.nl De 12, 2017 Page 1 of 15 Jaobs De 12, 2017 Conjugate Priors Where we are,

More information

ON THE GENERAL QUADRATIC FUNCTIONAL EQUATION

ON THE GENERAL QUADRATIC FUNCTIONAL EQUATION Bol. So. Mat. Mexiana (3) Vol. 11, 2005 ON THE GENERAL QUADRATIC FUNCTIONAL EQUATION JOHN MICHAEL RASSIAS Abstrat. In 1940 and in 1964 S. M. Ulam proposed the general problem: When is it true that by hanging

More information

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

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

More information

On the density of languages representing finite set partitions

On the density of languages representing finite set partitions On the density of languages representing finite set partitions Nelma Moreira Rogério Reis Tehnial Report Series: DCC-04-07 Departamento de Ciênia de Computadores Fauldade de Ciênias & Laboratório de Inteligênia

More information

On the Licensing of Innovations under Strategic Delegation

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

More information

A note on a variational formulation of electrodynamics

A note on a variational formulation of electrodynamics Proeedings of the XV International Workshop on Geometry and Physis Puerto de la Cruz, Tenerife, Canary Islands, Spain September 11 16, 006 Publ. de la RSME, Vol. 11 (007), 314 31 A note on a variational

More information

arxiv: v1 [math.co] 16 May 2016

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

More information

A Unified View on Multi-class Support Vector Classification Supplement

A Unified View on Multi-class Support Vector Classification Supplement Journal of Mahine Learning Researh??) Submitted 7/15; Published?/?? A Unified View on Multi-lass Support Vetor Classifiation Supplement Ürün Doğan Mirosoft Researh Tobias Glasmahers Institut für Neuroinformatik

More information

arxiv:physics/ v4 [physics.gen-ph] 9 Oct 2006

arxiv:physics/ v4 [physics.gen-ph] 9 Oct 2006 The simplest derivation of the Lorentz transformation J.-M. Lévy Laboratoire de Physique Nuléaire et de Hautes Energies, CNRS - IN2P3 - Universités Paris VI et Paris VII, Paris. Email: jmlevy@in2p3.fr

More information

Triangular Lie bialgebras and matched pairs for Lie algebras of real vector fields on S 1

Triangular Lie bialgebras and matched pairs for Lie algebras of real vector fields on S 1 Journal of Lie Theory Volume 4 (1994) 37 55 C 1994 Heldermann Verlag Version of May 4, 1995 Triangular Lie bialgebras and mathed pairs for Lie algebras of real vetor fields on S 1 Frank Leitenberger Communiated

More information

Gog and GOGAm pentagons

Gog and GOGAm pentagons Gog and GOGAm pentagons Philippe Biane, Hayat Cheballah To ite this version: Philippe Biane, Hayat Cheballah. Gog and GOGAm pentagons. Journal of Combinatorial Theory, Series A, Elsevier, 06, .

More information

What is a quantum symmetry?

What is a quantum symmetry? What is a quantum symmetry? Ulrich Krähmer & Angela Tabiri U Glasgow TU Dresden CLAP 30/11/2016 Uli (U Glasgow) What is a quantum symmetry? CLAP 30/11/2016 1 / 20 Road map Classical maths: symmetries =

More information

arxiv:hep-th/ v2 15 Aug 2001

arxiv:hep-th/ v2 15 Aug 2001 CSULB PA 01 2 hep-th/0107155 (Revised Version) Teleparallel Superspae in Eleven Dimensions Coupled to Supermembranes 1 arxiv:hep-th/0107155v2 15 Aug 2001 S James GATES, Jr, Hitoshi NISHINO and Subhash

More information

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

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

More information

A Functional Representation of Fuzzy Preferences

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

More information

The Corpuscular Structure of Matter, the Interaction of Material Particles, and Quantum Phenomena as a Consequence of Selfvariations.

The Corpuscular Structure of Matter, the Interaction of Material Particles, and Quantum Phenomena as a Consequence of Selfvariations. The Corpusular Struture of Matter, the Interation of Material Partiles, and Quantum Phenomena as a Consequene of Selfvariations. Emmanuil Manousos APM Institute for the Advanement of Physis and Mathematis,

More information

Vector Field Theory (E&M)

Vector Field Theory (E&M) Physis 4 Leture 2 Vetor Field Theory (E&M) Leture 2 Physis 4 Classial Mehanis II Otober 22nd, 2007 We now move from first-order salar field Lagrange densities to the equivalent form for a vetor field.

More information