A class of infinite dimensional stochastic processes
|
|
- Amanda Bryant
- 8 years ago
- Views:
Transcription
1 A class of infinite dimensional stochastic processes John Karlsson Linköping University CRM Barcelona, July 7, 214 Joint work with Jörg-Uwe Löbus John Karlsson (Linköping University) Infinite dimensional stochastic processes CRM Barcelona, July 7, / 3
2 1 Outline 2 The Dirichlet form 3 Closability 4 Quasi-regularity 5 Moving to a geometric setting 6 References John Karlsson (Linköping University) Infinite dimensional stochastic processes CRM Barcelona, July 7, / 3
3 Coercive forms A bilinear form E : H H R is called coercive if E(x, x) C x H, x H. John Karlsson (Linköping University) Infinite dimensional stochastic processes CRM Barcelona, July 7, / 3
4 Coercive forms A bilinear form E : H H R is called coercive if E(x, x) C x H, x H. A coercive closed form is called a Dirichlet form if (i) u + 1 D(E), (ii) E(u + u + 1, u u + 1), (iii) E(u u + 1, u + u + 1). John Karlsson (Linköping University) Infinite dimensional stochastic processes CRM Barcelona, July 7, / 3
5 Coercive forms A bilinear form E : H H R is called coercive if E(x, x) C x H, x H. A coercive closed form is called a Dirichlet form if (i) u + 1 D(E), (ii) E(u + u + 1, u u + 1), (iii) E(u u + 1, u + u + 1). For symmetric forms E(u + 1, u + 1) E(u, u). John Karlsson (Linköping University) Infinite dimensional stochastic processes CRM Barcelona, July 7, / 3
6 Connection to stochastic processes In the 197s Fukushima showed that if a Dirichlet form on a locally compact state space is regular one can construct an associated Markov process. John Karlsson (Linköping University) Infinite dimensional stochastic processes CRM Barcelona, July 7, / 3
7 Connection to stochastic processes In the 197s Fukushima showed that if a Dirichlet form on a locally compact state space is regular one can construct an associated Markov process Röckner and Ma solved the question in an infinite dimensional setting: John Karlsson (Linköping University) Infinite dimensional stochastic processes CRM Barcelona, July 7, / 3
8 Connection to stochastic processes In the 197s Fukushima showed that if a Dirichlet form on a locally compact state space is regular one can construct an associated Markov process Röckner and Ma solved the question in an infinite dimensional setting: Röckner-Ma A Dirichlet form on a separable metric space is associated with a Markov process with decent sample paths if and only if the form is quasi-regular. John Karlsson (Linköping University) Infinite dimensional stochastic processes CRM Barcelona, July 7, / 3
9 The Dirichlet form We are concerned with Dirichlet forms of type E(F, G) = DF, ADG H ϕdν = DF, λ i S i, DG H S i ϕdν. i=1 H John Karlsson (Linköping University) Infinite dimensional stochastic processes CRM Barcelona, July 7, / 3
10 The Dirichlet form We are concerned with Dirichlet forms of type E(F, G) = DF, ADG H ϕdν = DF, λ i S i, DG H S i i=1 H ϕdν. Here H is the space of absolutely continuous R d -valued functions on [, 1], ν is the Wiener measure and ϕ is a weight function. John Karlsson (Linköping University) Infinite dimensional stochastic processes CRM Barcelona, July 7, / 3
11 Closability definition Definition A bilinear form is closable if it has a closed extension. More precisely, let E be a positive definite bilinear form on H with domain D(E). (E, D(E)) is called closable on H if for all u n D(E), n N such that E(u n u m, u n u m ) and m,n u n in H, we have E(u n, u n ). John Karlsson (Linköping University) Infinite dimensional stochastic processes CRM Barcelona, July 7, / 3
12 Framework We study the form on the set of functions { Z := F (γ) = f (γ(s 1 ),..., γ(s k )), γ Ω : } < s 1 < < s k = 1, f Cp (R d k ), k N John Karlsson (Linköping University) Infinite dimensional stochastic processes CRM Barcelona, July 7, / 3
13 Framework We study the form on the set of functions { Z := F (γ) = f (γ(s 1 ),..., γ(s k )), γ Ω : } < s 1 < < s k = 1, f Cp (R d k ), k N where f Cp means that f and all its partial derivatives are smooth with polynomial growth. John Karlsson (Linköping University) Infinite dimensional stochastic processes CRM Barcelona, July 7, / 3
14 Framework We study the form on the set of functions { Z := F (γ) = f (γ(s 1 ),..., γ(s k )), γ Ω : } < s 1 < < s k = 1, f Cp (R d k ), k N where f Cp means that f and all its partial derivatives are smooth with polynomial growth. As well as { Y := F (γ) = f (γ(s 1 ),..., γ(s k )), γ Ω : F Z, s 1,..., s k { l 2 : l {1,..., 2 n } } }, n N. n John Karlsson (Linköping University) Infinite dimensional stochastic processes CRM Barcelona, July 7, / 3
15 Closability result Lemma If f ϕ L1 (ν), f Z. (1) Then the operators D, and δ are closable as operators L 2 (ϕν) Z L 2 (ϕν; H) and L 2 (ϕν; H) Z H L 2 (ϕν) respectively. John Karlsson (Linköping University) Infinite dimensional stochastic processes CRM Barcelona, July 7, / 3
16 Equivalence classes x := {x + c1 : c R}, L 2 (ϕν) 1 := {(x) : x L 2 (ϕν), δ(z) := The equivalence class of δ(z), z Z H. John Karlsson (Linköping University) Infinite dimensional stochastic processes CRM Barcelona, July 7, / 3
17 Equivalence classes x := {x + c1 : c R}, L 2 (ϕν) 1 := {(x) : x L 2 (ϕν), δ(z) := The equivalence class of δ(z), z Z H. Lemma If f ϕ L1 (ν), f Z. (1) Then the operators D 1, and δ 1 are closable as operators L 2 (ϕν; H) Z 1 L 2 (ϕν) 1 and L 2 (ϕν) 1 Z 1 H L2 (ϕν) respectively. John Karlsson (Linköping University) Infinite dimensional stochastic processes CRM Barcelona, July 7, / 3
18 Closability of the form Theorem Let ϕ satisfy (1) and assume that A ε Id for some ε >. (a) The form (E, Y ) is closable in L 2 (ϕν). Let (E, D Y (E)) denote the closure of (E, Y ) in L 2 (ϕν). (b) If sup c 1,c 2,... {,1} d j=1 p= λip,j ϕdν 2 p <, (2) then (E, Z) is closable and we let (E, D Z (E)) denote the closure of (E, Z) on L 2 (ϕν). Furthermore D Z (E) = D Y (E) under (2). (c) Z D Y (E) if and only if (2). (d) If (E, Z) is closable in L 2 (ϕν) then (2) holds. John Karlsson (Linköping University) Infinite dimensional stochastic processes CRM Barcelona, July 7, / 3
19 In the special case Remark If the sequence of eigenvalues is non-decreasing < λ 1 (γ) < λ 2 (γ),..., then relation (2) simplifies to λd2 p ϕdν 2 p <. p= John Karlsson (Linköping University) Infinite dimensional stochastic processes CRM Barcelona, July 7, / 3
20 E-nests Definition (i) An increasing sequence (F k ) k N of closed subsets of E is called an E-nest if k 1 D(E) Fk is dense in D(E) w.r.t. Ẽ1, where D(E) Fk denotes {u D(E) : u = m-a.e. on E \ F k }. John Karlsson (Linköping University) Infinite dimensional stochastic processes CRM Barcelona, July 7, / 3
21 E-nests Definition (i) An increasing sequence (F k ) k N of closed subsets of E is called an E-nest if k 1 D(E) Fk is dense in D(E) w.r.t. Ẽ1, where D(E) Fk denotes {u D(E) : u = m-a.e. on E \ F k }. (ii) A subset N E is called E-exceptional if N k Fk c for some E-nest (F k ) k N. John Karlsson (Linköping University) Infinite dimensional stochastic processes CRM Barcelona, July 7, / 3
22 E-nests Definition (i) An increasing sequence (F k ) k N of closed subsets of E is called an E-nest if k 1 D(E) Fk is dense in D(E) w.r.t. Ẽ1, where D(E) Fk denotes {u D(E) : u = m-a.e. on E \ F k }. (ii) A subset N E is called E-exceptional if N k Fk c for some E-nest (F k ) k N. (iii) We say that a property holds E-quasi-everywhere if it holds everywhere outside some E-exceptional set. John Karlsson (Linköping University) Infinite dimensional stochastic processes CRM Barcelona, July 7, / 3
23 E-nests Definition (i) An increasing sequence (F k ) k N of closed subsets of E is called an E-nest if k 1 D(E) Fk is dense in D(E) w.r.t. Ẽ1, where D(E) Fk denotes {u D(E) : u = m-a.e. on E \ F k }. (ii) A subset N E is called E-exceptional if N k Fk c for some E-nest (F k ) k N. (iii) We say that a property holds E-quasi-everywhere if it holds everywhere outside some E-exceptional set. Definition An E-quasi-everywhere defined function f is called E-quasi-continuous if there exists an E-nest (F k ) k N such that f is continuous on (F k ) k N. John Karlsson (Linköping University) Infinite dimensional stochastic processes CRM Barcelona, July 7, / 3
24 Definition of quasi-regularity Definition A Dirichlet form (E, D(E)) on L 2 (E, m) is called quasi-regular if: (i) There exists an E-nest (F k ) k N consisting of compact sets, (ii) There exists an Ẽ 1/2 1 -dense subset of D(E) whose elements have E-quasi-continuous m-versions, (iii) There exist u n D(E), n N, having E-quasi-continuous m-versions ũ n, n N, and an E-exeptional set N E such that {ũ n : n N} separates the points of E \ N. John Karlsson (Linköping University) Infinite dimensional stochastic processes CRM Barcelona, July 7, / 3
25 The weight function ϕ We consider weight functions ϕ + and ϕ of the form { 1 ϕ + (γ) := exp b s (γ), dγ s R d } b s (γ) 2 ds, (3) John Karlsson (Linköping University) Infinite dimensional stochastic processes CRM Barcelona, July 7, / 3
26 The weight function ϕ We consider weight functions ϕ + and ϕ of the form { 1 ϕ + (γ) := exp b s (γ), dγ s R d } b s (γ) 2 ds, (3) and { 1 ϕ (γ) := exp b s (γ), dγ s R d } b s (γ) 2 ds, (4) where b s (γ) is adapted to the natural filtration of the Wiener process. John Karlsson (Linköping University) Infinite dimensional stochastic processes CRM Barcelona, July 7, / 3
27 The weight function ϕ We consider weight functions ϕ + and ϕ of the form { 1 ϕ + (γ) := exp b s (γ), dγ s R d } b s (γ) 2 ds, (3) and { 1 ϕ (γ) := exp b s (γ), dγ s R d } b s (γ) 2 ds, (4) where b s (γ) is adapted to the natural filtration of the Wiener process. Under the condition f ϕ + L1 (ν), and f ϕ L1 (ν), (5) John Karlsson (Linköping University) Infinite dimensional stochastic processes CRM Barcelona, July 7, / 3
28 The weight function ϕ We consider weight functions ϕ + and ϕ of the form { 1 ϕ + (γ) := exp b s (γ), dγ s R d } b s (γ) 2 ds, (3) and { 1 ϕ (γ) := exp b s (γ), dγ s R d } b s (γ) 2 ds, (4) where b s (γ) is adapted to the natural filtration of the Wiener process. Under the condition f ϕ + L1 (ν), and f ϕ L1 (ν), (5) for all f Z, the earlier closability results hold for ϕ + as well as for ϕ. John Karlsson (Linköping University) Infinite dimensional stochastic processes CRM Barcelona, July 7, / 3
29 The Novikov condition Lemma Let ϕ +, and ϕ be defined as in (3), and (4). If (5) holds then we have the Novikov condition [ { 1 1 }] E exp b s (γ) 2 ds <. 2 In particular, E[ϕ + ] = E[ϕ ] = 1. John Karlsson (Linköping University) Infinite dimensional stochastic processes CRM Barcelona, July 7, / 3
30 The Novikov condition Lemma Let ϕ +, and ϕ be defined as in (3), and (4). If (5) holds then we have the Novikov condition [ { 1 1 }] E exp b s (γ) 2 ds <. 2 In particular, E[ϕ + ] = E[ϕ ] = 1. John Karlsson (Linköping University) Infinite dimensional stochastic processes CRM Barcelona, July 7, / 3
31 Main theorem Theorem For ϕ = ϕ + and for ϕ = ϕ, the closure of E(F, F ) = λ i S i, DF 2 H ϕdν, F Z, i=1 in L 2 (ϕν), is quasi-regular. John Karlsson (Linköping University) Infinite dimensional stochastic processes CRM Barcelona, July 7, / 3
32 Geometric framework Let M be a connected geometrically, stochastically complete, and torsion free manifold. John Karlsson (Linköping University) Infinite dimensional stochastic processes CRM Barcelona, July 7, / 3
33 Geometric framework Let M be a connected geometrically, stochastically complete, and torsion free manifold. We study the form Ê( ˆF, Ĝ) = ˆD ˆF, A ˆDĜ ˆϕd ˆν H = ˆD ˆF, λ i S i, ˆDĜ i=1 H S i H ˆϕd ˆν, where ˆν is the Wiener measure on the path space P m (M) := {ˆγ C([, 1]; M) : ˆγ() = m }, m M and ˆϕ is a weight function to be specified. (6) John Karlsson (Linköping University) Infinite dimensional stochastic processes CRM Barcelona, July 7, / 3
34 Geometric framework cont. More precisely let P (R d ) Ω := {γ C([, 1]; R d ) : γ() = }, I : P (R d ) P m (M) be the Itô map and ˆν be the image measure of the Wiener measure on P (R d ) under I. In order to recall the construction of the Itô map let O(M) denote the orthonormal frame bundle with respect to M, π be the canonical projection O(M) M and H 1,..., H d be the canonical horizontal vector fields. Choose r O(M) such that π(r ) = m. We introduce r γ as the solution to the Stratonovich SDE d r γ (t) = H i (r γ (t)) x i, t [, 1], (7) i=1 r γ () = r, γ = (γ 1,..., γ d ) P (R d ). This defines a.e. a mapping I : P (R d ) P m (M) by I (γ)(t) := π(r γ (t)), γ P (R d ), t [, 1], the Itô map. We also denote by T x M as the tangent space of M at the point x M. John Karlsson (Linköping University) Infinite dimensional stochastic processes CRM Barcelona, July 7, / 3
35 Assumptions Let K C([, )) such that Ric(X, X ) K(r) X 2, X T x M, x B(m, r), r >, (8) where B(m, r) is the geodesic ball at m with radius r. Let ρ denote the Riemannian distance on M and ρ m (x) := ρ(x, m ), x M. We assume that there are constants c 1, c 2, r 1 > such that the following conditions hold, 1 (d 1)K(r) c1 r, r r 1, 2 and { } 1 Ric(X, Y ) p c 2 exp 2 e 1 2c1 ρ m (x) 2 (9) for some p 2 and x M, X, Y T x M, X = Y = 1. We have [ 1 E ] Ric rγ(t) p dt < (1) John Karlsson (Linköping University) Infinite dimensional stochastic processes CRM Barcelona, July 7, / 3
36 Closability result Proposition If for p specified in (9) we have ĝ ˆϕ L1 (ˆν), ĝ L p 2 (ˆν), (11) then ( ˆD, Ẑ) defined by ˆD( ˆF, Ĝ) := ˆD ˆF, ˆDĜ H ˆϕd ˆν, ˆF, Ĝ Ẑ, is closable on L 2 ( ˆϕˆν). John Karlsson (Linköping University) Infinite dimensional stochastic processes CRM Barcelona, July 7, / 3
37 ϕ motivation We consider ˆϕ(ˆγ) of the form { 1 ˆϕ(ˆγ) = exp ˆV (ˆγt ), d ˆγ t 1 T ˆγ(t) 2 1 ˆV (ˆγ t ) 2 T ˆγ(t) } dt, ˆγ P m (M). as ˆϕ is then the Radon Nikodym derivative of the diffusion measure corresponding to the general diffusion process on M with generator 1 2 M + ˆV, see [1], with respect to ˆν. We observe that V := r 1 ˆV π r r 1 ˆV I, (12) which says that V V (γ) is an adapted R d -valued process. John Karlsson (Linköping University) Infinite dimensional stochastic processes CRM Barcelona, July 7, / 3
38 Novikov condition in the geometric case The corresponding conditions to (3), (4), i.e. ˆf ˆϕ + ˆf L1 (ˆν) and ˆϕ L1 (ˆν) (13) for all ˆf [ { 1 1 Ẑ, we get Ê exp 2 ˆV }] (ˆγ t ) 2 T ˆγ(t) dt < where Ê denotes expectation taken with respect to ˆν. John Karlsson (Linköping University) Infinite dimensional stochastic processes CRM Barcelona, July 7, / 3
39 Novikov condition in the geometric case The corresponding conditions to (3), (4), i.e. ˆf ˆϕ + ˆf L1 (ˆν) and ˆϕ L1 (ˆν) (13) for all ˆf [ { 1 1 Ẑ, we get Ê exp 2 ˆV }] (ˆγ t ) 2 T ˆγ(t) dt < where Ê denotes expectation taken with respect to ˆν.Thus we have the Novikov condition E [ { 1 exp 2 1 (V (γ)) t 2 R d dt }] <. (14) John Karlsson (Linköping University) Infinite dimensional stochastic processes CRM Barcelona, July 7, / 3
40 More assumptions In order to obtain quasi-regularity we assume the Ricci curvature to be bounded from below, i.e. there exists some c R, not necessarily non-negative, such that Ric(X, X ) c X 2 X T x M, x M. (15) John Karlsson (Linköping University) Infinite dimensional stochastic processes CRM Barcelona, July 7, / 3
41 More assumptions In order to obtain quasi-regularity we assume the Ricci curvature to be bounded from below, i.e. there exists some c R, not necessarily non-negative, such that Ric(X, X ) c X 2 X T x M, x M. (15) We also sharpen (1) and assume in addition for some p > 2. [ 1 E ] Ric rγ(t) p dtϕ < (16) John Karlsson (Linköping University) Infinite dimensional stochastic processes CRM Barcelona, July 7, / 3
42 Quasi-regularity theorem Theorem Assume the following conditions on ˆϕ resp. ϕ, (11), (13), and (16). Let A ε Id for some ε >, and sup c 1,c 2,... {,1} d j=1 p= λip,j ˆϕd ˆν 2 p <. (17) Then Ê( ˆF, ˆF ) = ˆD ˆF, i=1 λ i S i, ˆD ˆF S i H H ˆϕd ˆν, ˆF Ẑ, (18) is quasi-regular in L 2 ( ˆϕˆν). John Karlsson (Linköping University) Infinite dimensional stochastic processes CRM Barcelona, July 7, / 3
43 Part of proof, flat case E [ Gn,τ 2 ϕ ] = E 2E = 2E 4E sup v {1,...,d} s [,1] sup v {1,...,d} s [,1] sup v {1,...,d} s [,1] [ d sup v=1 s [,1] x v (γ s ) x v (τ s ) ϕ x v (γ s ) ϕ x v ( ) T 1 γ s 2 + C 2 (τ) 2 sup x v (τ s ) 2 v {1,...,d} s [,1] ] M1 v (s) 2 + sup M2 v (s) 2 + C 2 (τ). s [,1] John Karlsson (Linköping University) Infinite dimensional stochastic processes CRM Barcelona, July 7, / 3
44 Part of proof, flat case cont. t ( ) (T γ) t := γ t bs v (γ) ds, v=1,...,d where b is from (3) such that (5) is satisfied and b v denotes the vth coordinate. John Karlsson (Linköping University) Infinite dimensional stochastic processes CRM Barcelona, July 7, / 3
45 Part of proof, flat case cont. t t ( ) (T γ) t := γ t bs v (γ) ds, v=1,...,d where b is from (3) such that (5) is satisfied and b v denotes the vth coordinate. We have t ( 1 t ) (T 1 γ) v t = γt v + bs v (T 1 γ) ds = 2 γv t + χ {b v s (T 1 γ)>}bs v (T 1 γ) ds ) ( γv t + χ {b v s (T 1 γ) }b v s (T 1 γ) ds =: M v 1 (t) M v 2 (t), John Karlsson (Linköping University) Infinite dimensional stochastic processes CRM Barcelona, July 7, / 3
46 Part of proof, flat case cont. Using Doob s inequality we get E [ Gn,τ 2 ϕ ] d 16 E [ M1 v (1) 2] d + 16 E [ M2 v (1) 2] + C 2 (τ). (19) v=1 v=1 John Karlsson (Linköping University) Infinite dimensional stochastic processes CRM Barcelona, July 7, / 3
47 Part of proof, flat case cont. Using Doob s inequality we get E [ Gn,τ 2 ϕ ] d 16 E [ M1 v (1) 2] + 16 v=1 d E [ M2 v (1) 2] + C 2 (τ). (19) v=1 We have E [ [ (1 M1 v (1) 2] 1 = E 2 γv 1 + χ {b v s (T 1 γ)>}bs v (T 1 γ) ds [ ( 1 1 )2 ] 2 E[(γv 1 ) 2 ] + 2E bs v (T 1 γ) ds [ ( ] = 1 1 ) E bs v (γ) ds ϕ(γ) 1 [ 1 ] 2 + 2E bs v (γ) 2 ds ϕ(γ) 1 { 1 [exp 2 + 2E )2 ] } ] bs v (γ) 2 ds ϕ(γ) = 1 [ ] E ϕ. John Karlsson (Linköping University) Infinite dimensional stochastic processes CRM Barcelona, July 7, / 3
48 Different gradients ˆD s ˆF (ˆγ) := k i=1 s s i r 1 I 1 (ˆγ) (s i)( si ˆf )( γ), s [, 1], ˆγ Pm (M), where r is defined in (7). We also introduce k ) ˆD s ˆF (γ) := χ [,si ](s) (T γ ( si si ˆf )( γ), s [, 1], ˆγ P m (M). i=1 In addition as in we define the damped version k ) D s ˆF (γ) := χ [,si ](s) (Q si,st γ ( si si ˆf )( γ), s [, 1], ˆγ P m (M), (2) i=1 where Q denotes the adjoint of Q s,t : R d R d, which is defined by or equivalently dq s,t ds = 1 2 Ric r γ(s)q s,t, Q t,t = Id Tm, t s, dq s,t dt = 1 2 Q s,tric rγ(t), Q s,s = Id Tm, t s. (21) John Karlsson (Linköping University) Infinite dimensional stochastic processes CRM Barcelona, July 7, / 3
49 References M. Capitaine, E. P. Hsu, and M. Ledoux. Martingale representation and a simple proof of logarithmic sobolev inequalities on path spaces. Electron. Comm. Probab., 2:71 81, C. Houdré and N. Privault. A concentration inequality on Riemannian path space. In Stochastic inequalities and applications, volume 56 of Progr. Probab., pages Birkhäuser, Basel, 23. E. P. Hsu and C. Ouyang. Quasi-invariance of the wiener measure on the path space over a complete riemannian manifold. J. Funct. Anal., 257(5): , 29. F.-Y. Wang and B. Wu. Quasi-regular dirichlet forms on riemannian path and loop spaces. Forum Math. Volume, 2(6): , 28. F.-Y. Wang and B. Wu. Quasi-regular dirichlet forms on free riemannian path spaces. John Karlsson (Linköping University) Infinite dimensional stochastic processes CRM Barcelona, July 7, / 3
50 Thank you for listening John Karlsson (Linköping University) Infinite dimensional stochastic processes CRM Barcelona, July 7, / 3
Mathematical Finance
Mathematical Finance Option Pricing under the Risk-Neutral Measure Cory Barnes Department of Mathematics University of Washington June 11, 2013 Outline 1 Probability Background 2 Black Scholes for European
More informationOn a comparison result for Markov processes
On a comparison result for Markov processes Ludger Rüschendorf University of Freiburg Abstract A comparison theorem is stated for Markov processes in polish state spaces. We consider a general class of
More information14.11. Geodesic Lines, Local Gauss-Bonnet Theorem
14.11. Geodesic Lines, Local Gauss-Bonnet Theorem Geodesics play a very important role in surface theory and in dynamics. One of the main reasons why geodesics are so important is that they generalize
More informationINVARIANT METRICS WITH NONNEGATIVE CURVATURE ON COMPACT LIE GROUPS
INVARIANT METRICS WITH NONNEGATIVE CURVATURE ON COMPACT LIE GROUPS NATHAN BROWN, RACHEL FINCK, MATTHEW SPENCER, KRISTOPHER TAPP, AND ZHONGTAO WU Abstract. We classify the left-invariant metrics with nonnegative
More informationARBITRAGE-FREE OPTION PRICING MODELS. Denis Bell. University of North Florida
ARBITRAGE-FREE OPTION PRICING MODELS Denis Bell University of North Florida Modelling Stock Prices Example American Express In mathematical finance, it is customary to model a stock price by an (Ito) stochatic
More informationA PRIORI ESTIMATES FOR SEMISTABLE SOLUTIONS OF SEMILINEAR ELLIPTIC EQUATIONS. In memory of Rou-Huai Wang
A PRIORI ESTIMATES FOR SEMISTABLE SOLUTIONS OF SEMILINEAR ELLIPTIC EQUATIONS XAVIER CABRÉ, MANEL SANCHÓN, AND JOEL SPRUCK In memory of Rou-Huai Wang 1. Introduction In this note we consider semistable
More informationTHE BANACH CONTRACTION PRINCIPLE. Contents
THE BANACH CONTRACTION PRINCIPLE ALEX PONIECKI Abstract. This paper will study contractions of metric spaces. To do this, we will mainly use tools from topology. We will give some examples of contractions,
More informationMetric Spaces. Chapter 1
Chapter 1 Metric Spaces Many of the arguments you have seen in several variable calculus are almost identical to the corresponding arguments in one variable calculus, especially arguments concerning convergence
More informationInvariant Metrics with Nonnegative Curvature on Compact Lie Groups
Canad. Math. Bull. Vol. 50 (1), 2007 pp. 24 34 Invariant Metrics with Nonnegative Curvature on Compact Lie Groups Nathan Brown, Rachel Finck, Matthew Spencer, Kristopher Tapp and Zhongtao Wu Abstract.
More informationEXIT TIME PROBLEMS AND ESCAPE FROM A POTENTIAL WELL
EXIT TIME PROBLEMS AND ESCAPE FROM A POTENTIAL WELL Exit Time problems and Escape from a Potential Well Escape From a Potential Well There are many systems in physics, chemistry and biology that exist
More informationA Martingale System Theorem for Stock Investments
A Martingale System Theorem for Stock Investments Robert J. Vanderbei April 26, 1999 DIMACS New Market Models Workshop 1 Beginning Middle End Controversial Remarks Outline DIMACS New Market Models Workshop
More informationExtrinsic geometric flows
On joint work with Vladimir Rovenski from Haifa Paweł Walczak Uniwersytet Łódzki CRM, Bellaterra, July 16, 2010 Setting Throughout this talk: (M, F, g 0 ) is a (compact, complete, any) foliated, Riemannian
More information4. Expanding dynamical systems
4.1. Metric definition. 4. Expanding dynamical systems Definition 4.1. Let X be a compact metric space. A map f : X X is said to be expanding if there exist ɛ > 0 and L > 1 such that d(f(x), f(y)) Ld(x,
More informationGeometrical Characterization of RN-operators between Locally Convex Vector Spaces
Geometrical Characterization of RN-operators between Locally Convex Vector Spaces OLEG REINOV St. Petersburg State University Dept. of Mathematics and Mechanics Universitetskii pr. 28, 198504 St, Petersburg
More informationtr g φ hdvol M. 2 The Euler-Lagrange equation for the energy functional is called the harmonic map equation:
Notes prepared by Andy Huang (Rice University) In this note, we will discuss some motivating examples to guide us to seek holomorphic objects when dealing with harmonic maps. This will lead us to a brief
More informationBANACH AND HILBERT SPACE REVIEW
BANACH AND HILBET SPACE EVIEW CHISTOPHE HEIL These notes will briefly review some basic concepts related to the theory of Banach and Hilbert spaces. We are not trying to give a complete development, but
More informationNotes on metric spaces
Notes on metric spaces 1 Introduction The purpose of these notes is to quickly review some of the basic concepts from Real Analysis, Metric Spaces and some related results that will be used in this course.
More informationLipschitz classes of A-harmonic functions in Carnot groups
Lipschitz classes of A-harmonic functions in Carnot groups Craig A. Nolder Department of Mathematics Florida State University Tallahassee, FL 32306-4510, USA nolder@math.fsu.edu 30 October 2005 Abstract
More informationAdaptive Online Gradient Descent
Adaptive Online Gradient Descent Peter L Bartlett Division of Computer Science Department of Statistics UC Berkeley Berkeley, CA 94709 bartlett@csberkeleyedu Elad Hazan IBM Almaden Research Center 650
More informationFUNCTIONAL ANALYSIS LECTURE NOTES: QUOTIENT SPACES
FUNCTIONAL ANALYSIS LECTURE NOTES: QUOTIENT SPACES CHRISTOPHER HEIL 1. Cosets and the Quotient Space Any vector space is an abelian group under the operation of vector addition. So, if you are have studied
More informationMathematical Physics, Lecture 9
Mathematical Physics, Lecture 9 Hoshang Heydari Fysikum April 25, 2012 Hoshang Heydari (Fysikum) Mathematical Physics, Lecture 9 April 25, 2012 1 / 42 Table of contents 1 Differentiable manifolds 2 Differential
More informationHarnack Inequality for Some Classes of Markov Processes
Harnack Inequality for Some Classes of Markov Processes Renming Song Department of Mathematics University of Illinois Urbana, IL 6181 Email: rsong@math.uiuc.edu and Zoran Vondraček Department of Mathematics
More information1 Local Brouwer degree
1 Local Brouwer degree Let D R n be an open set and f : S R n be continuous, D S and c R n. Suppose that the set f 1 (c) D is compact. (1) Then the local Brouwer degree of f at c in the set D is defined.
More informationSome remarks on two-asset options pricing and stochastic dependence of asset prices
Some remarks on two-asset options pricing and stochastic dependence of asset prices G. Rapuch & T. Roncalli Groupe de Recherche Opérationnelle, Crédit Lyonnais, France July 16, 001 Abstract In this short
More informationInner Product Spaces
Math 571 Inner Product Spaces 1. Preliminaries An inner product space is a vector space V along with a function, called an inner product which associates each pair of vectors u, v with a scalar u, v, and
More informationSome stability results of parameter identification in a jump diffusion model
Some stability results of parameter identification in a jump diffusion model D. Düvelmeyer Technische Universität Chemnitz, Fakultät für Mathematik, 09107 Chemnitz, Germany Abstract In this paper we discuss
More informationNonzero degree tangential maps between dual symmetric spaces
ISSN 1472-2739 (on-line) 1472-2747 (printed) 709 Algebraic & Geometric Topology Volume 1 (2001) 709 718 Published: 30 November 2001 ATG Nonzero degree tangential maps between dual symmetric spaces Boris
More informationHedging bounded claims with bounded outcomes
Hedging bounded claims with bounded outcomes Freddy Delbaen ETH Zürich, Department of Mathematics, CH-892 Zurich, Switzerland Abstract. We consider a financial market with two or more separate components
More informationNon-Arbitrage and the Fundamental Theorem of Asset Pricing: Summary of Main Results
Proceedings of Symposia in Applied Mathematics Volume 00, 1997 Non-Arbitrage and the Fundamental Theorem of Asset Pricing: Summary of Main Results Freddy Delbaen and Walter Schachermayer Abstract. The
More informationAPPROXIMATION OF FRAME BASED MISSING DATA RECOVERY
APPROXIMATION OF FRAME BASED MISSING DATA RECOVERY JIAN-FENG CAI, ZUOWEI SHEN, AND GUI-BO YE Abstract. Recovering missing data from its partial samples is a fundamental problem in mathematics and it has
More informationAPPROXIMATION OF FRAME BASED MISSING DATA RECOVERY
APPROXIMATION OF FRAME BASED MISSING DATA RECOVERY JIAN-FENG CAI, ZUOWEI SHEN, AND GUI-BO YE Abstract. Recovering missing data from its partial samples is a fundamental problem in mathematics and it has
More information1 Norms and Vector Spaces
008.10.07.01 1 Norms and Vector Spaces Suppose we have a complex vector space V. A norm is a function f : V R which satisfies (i) f(x) 0 for all x V (ii) f(x + y) f(x) + f(y) for all x,y V (iii) f(λx)
More informationPETER HÄSTÖ, RIKU KLÉN, SWADESH KUMAR SAHOO, AND MATTI VUORINEN
GEOMETRIC PROPERTIES OF ϕ-uniform DOMAINS PETER HÄSTÖ, RIKU KLÉN, SWADESH KUMAR SAHOO, AND MATTI VUORINEN Abstract. We consider proper subdomains G of R n and their images G = f(g) under quasiconformal
More informationLecture 13: Martingales
Lecture 13: Martingales 1. Definition of a Martingale 1.1 Filtrations 1.2 Definition of a martingale and its basic properties 1.3 Sums of independent random variables and related models 1.4 Products of
More informationRESONANCES AND BALLS IN OBSTACLE SCATTERING WITH NEUMANN BOUNDARY CONDITIONS
RESONANCES AND BALLS IN OBSTACLE SCATTERING WITH NEUMANN BOUNDARY CONDITIONS T. J. CHRISTIANSEN Abstract. We consider scattering by an obstacle in R d, d 3 odd. We show that for the Neumann Laplacian if
More informationHow To Prove The Dirichlet Unit Theorem
Chapter 6 The Dirichlet Unit Theorem As usual, we will be working in the ring B of algebraic integers of a number field L. Two factorizations of an element of B are regarded as essentially the same if
More informationCHAPTER IV - BROWNIAN MOTION
CHAPTER IV - BROWNIAN MOTION JOSEPH G. CONLON 1. Construction of Brownian Motion There are two ways in which the idea of a Markov chain on a discrete state space can be generalized: (1) The discrete time
More informationSets of Fibre Homotopy Classes and Twisted Order Parameter Spaces
Communications in Mathematical Physics Manuscript-Nr. (will be inserted by hand later) Sets of Fibre Homotopy Classes and Twisted Order Parameter Spaces Stefan Bechtluft-Sachs, Marco Hien Naturwissenschaftliche
More informationAbout the inverse football pool problem for 9 games 1
Seventh International Workshop on Optimal Codes and Related Topics September 6-1, 013, Albena, Bulgaria pp. 15-133 About the inverse football pool problem for 9 games 1 Emil Kolev Tsonka Baicheva Institute
More informationMath 550 Notes. Chapter 7. Jesse Crawford. Department of Mathematics Tarleton State University. Fall 2010
Math 550 Notes Chapter 7 Jesse Crawford Department of Mathematics Tarleton State University Fall 2010 (Tarleton State University) Math 550 Chapter 7 Fall 2010 1 / 34 Outline 1 Self-Adjoint and Normal Operators
More informationIn memory of Lars Hörmander
ON HÖRMANDER S SOLUTION OF THE -EQUATION. I HAAKAN HEDENMALM ABSTRAT. We explain how Hörmander s classical solution of the -equation in the plane with a weight which permits growth near infinity carries
More informationModern Optimization Methods for Big Data Problems MATH11146 The University of Edinburgh
Modern Optimization Methods for Big Data Problems MATH11146 The University of Edinburgh Peter Richtárik Week 3 Randomized Coordinate Descent With Arbitrary Sampling January 27, 2016 1 / 30 The Problem
More informationWiener s test for super-brownian motion and the Brownian snake
Probab. Theory Relat. Fields 18, 13 129 (1997 Wiener s test for super-brownian motion and the Brownian snake Jean-Stephane Dhersin and Jean-Francois Le Gall Laboratoire de Probabilites, Universite Paris
More informationAlmost Quaternionic Structures on Quaternionic Kaehler Manifolds. F. Özdemir
Almost Quaternionic Structures on Quaternionic Kaehler Manifolds F. Özdemir Department of Mathematics, Faculty of Arts and Sciences Istanbul Technical University, 34469 Maslak-Istanbul, TURKEY fozdemir@itu.edu.tr
More information2.3 Convex Constrained Optimization Problems
42 CHAPTER 2. FUNDAMENTAL CONCEPTS IN CONVEX OPTIMIZATION Theorem 15 Let f : R n R and h : R R. Consider g(x) = h(f(x)) for all x R n. The function g is convex if either of the following two conditions
More informationEikonal Slant Helices and Eikonal Darboux Helices In 3-Dimensional Riemannian Manifolds
Eikonal Slant Helices and Eikonal Darboux Helices In -Dimensional Riemannian Manifolds Mehmet Önder a, Evren Zıplar b, Onur Kaya a a Celal Bayar University, Faculty of Arts and Sciences, Department of
More informationNon-trivial Bounded Harmonic Functions on Cartan-Hadamard Manifolds of Unbounded Curvature
Non-trivial Bounded Harmonic Functions on Cartan-Hadamard Manifolds of Unbounded Curvature Dissertation zur Erlangung des Doktorgrades der Naturwissenschaften Dr. rer. nat.) der Naturwissenschaftlichen
More informationInner Product Spaces and Orthogonality
Inner Product Spaces and Orthogonality week 3-4 Fall 2006 Dot product of R n The inner product or dot product of R n is a function, defined by u, v a b + a 2 b 2 + + a n b n for u a, a 2,, a n T, v b,
More informationBANACH MANIFOLDS OF FIBER BUNDLE SECTIONS
Actes, Congrès intern. Math., 1970. Tome 2, p. 243 à 249. BANACH MANIFOLDS OF FIBER BUNDLE SECTIONS by Richard S. PALAIS 1. Introduction. In the past several years significant progress has been made in
More informationIdeal Class Group and Units
Chapter 4 Ideal Class Group and Units We are now interested in understanding two aspects of ring of integers of number fields: how principal they are (that is, what is the proportion of principal ideals
More information17.3.1 Follow the Perturbed Leader
CS787: Advanced Algorithms Topic: Online Learning Presenters: David He, Chris Hopman 17.3.1 Follow the Perturbed Leader 17.3.1.1 Prediction Problem Recall the prediction problem that we discussed in class.
More informationShape Optimization Problems over Classes of Convex Domains
Shape Optimization Problems over Classes of Convex Domains Giuseppe BUTTAZZO Dipartimento di Matematica Via Buonarroti, 2 56127 PISA ITALY e-mail: buttazzo@sab.sns.it Paolo GUASONI Scuola Normale Superiore
More informationMICROLOCAL ANALYSIS OF THE BOCHNER-MARTINELLI INTEGRAL
PROCEEDINGS OF THE AMERICAN MATHEMATICAL SOCIETY Volume 00, Number 0, Pages 000 000 S 0002-9939(XX)0000-0 MICROLOCAL ANALYSIS OF THE BOCHNER-MARTINELLI INTEGRAL NIKOLAI TARKHANOV AND NIKOLAI VASILEVSKI
More informationSPECTRAL POLYNOMIAL ALGORITHMS FOR COMPUTING BI-DIAGONAL REPRESENTATIONS FOR PHASE TYPE DISTRIBUTIONS AND MATRIX-EXPONENTIAL DISTRIBUTIONS
Stochastic Models, 22:289 317, 2006 Copyright Taylor & Francis Group, LLC ISSN: 1532-6349 print/1532-4214 online DOI: 10.1080/15326340600649045 SPECTRAL POLYNOMIAL ALGORITHMS FOR COMPUTING BI-DIAGONAL
More information1. (First passage/hitting times/gambler s ruin problem:) Suppose that X has a discrete state space and let i be a fixed state. Let
Copyright c 2009 by Karl Sigman 1 Stopping Times 1.1 Stopping Times: Definition Given a stochastic process X = {X n : n 0}, a random time τ is a discrete random variable on the same probability space as
More informationTail inequalities for order statistics of log-concave vectors and applications
Tail inequalities for order statistics of log-concave vectors and applications Rafał Latała Based in part on a joint work with R.Adamczak, A.E.Litvak, A.Pajor and N.Tomczak-Jaegermann Banff, May 2011 Basic
More informationOutline Lagrangian Constraints and Image Quality Models
Remarks on Lagrangian singularities, caustics, minimum distance lines Department of Mathematics and Statistics Queen s University CRM, Barcelona, Spain June 2014 CRM CRM, Barcelona, SpainJune 2014 CRM
More informationCONNECTIONS ON PRINCIPAL G-BUNDLES
CONNECTIONS ON PRINCIPAL G-BUNDLES RAHUL SHAH Abstract. We will describe connections on principal G-bundles via two perspectives: that of distributions and that of connection 1-forms. We will show that
More informationCOMPLETE MARKETS DO NOT ALLOW FREE CASH FLOW STREAMS
COMPLETE MARKETS DO NOT ALLOW FREE CASH FLOW STREAMS NICOLE BÄUERLE AND STEFANIE GRETHER Abstract. In this short note we prove a conjecture posed in Cui et al. 2012): Dynamic mean-variance problems in
More informationOnline Learning, Stability, and Stochastic Gradient Descent
Online Learning, Stability, and Stochastic Gradient Descent arxiv:1105.4701v3 [cs.lg] 8 Sep 2011 September 9, 2011 Tomaso Poggio, Stephen Voinea, Lorenzo Rosasco CBCL, McGovern Institute, CSAIL, Brain
More informationHow To Find The Optimal Control Function On A Unitary Operation
Quantum Computation as Geometry arxiv:quant-ph/0603161v2 21 Mar 2006 Michael A. Nielsen, Mark R. Dowling, Mile Gu, and Andrew C. Doherty School of Physical Sciences, The University of Queensland, Queensland
More informationSome remarks on Phragmén-Lindelöf theorems for weak solutions of the stationary Schrödinger operator
Wan Boundary Value Problems (2015) 2015:239 DOI 10.1186/s13661-015-0508-0 R E S E A R C H Open Access Some remarks on Phragmén-Lindelöf theorems for weak solutions of the stationary Schrödinger operator
More informationDuality of linear conic problems
Duality of linear conic problems Alexander Shapiro and Arkadi Nemirovski Abstract It is well known that the optimal values of a linear programming problem and its dual are equal to each other if at least
More informationRotation Rate of a Trajectory of an Algebraic Vector Field Around an Algebraic Curve
QUALITATIVE THEORY OF DYAMICAL SYSTEMS 2, 61 66 (2001) ARTICLE O. 11 Rotation Rate of a Trajectory of an Algebraic Vector Field Around an Algebraic Curve Alexei Grigoriev Department of Mathematics, The
More informationBasic Concepts of Point Set Topology Notes for OU course Math 4853 Spring 2011
Basic Concepts of Point Set Topology Notes for OU course Math 4853 Spring 2011 A. Miller 1. Introduction. The definitions of metric space and topological space were developed in the early 1900 s, largely
More informationConcentration inequalities for order statistics Using the entropy method and Rényi s representation
Concentration inequalities for order statistics Using the entropy method and Rényi s representation Maud Thomas 1 in collaboration with Stéphane Boucheron 1 1 LPMA Université Paris-Diderot High Dimensional
More informationGeneric measures for geodesic flows on nonpositively curved manifolds
Generic measures for geodesic flows on nonpositively curved manifolds Yves Coudène, Barbara Schapira 6th November 2014 Laboratoire de mathématiques, UBO, 6 avenue le Gorgeu, 29238 Brest, France LAMFA,
More informationSix questions, a proposition and two pictures on Hofer distance for hamiltonian diffeomorphisms on surfaces
1 Six questions, a proposition and two pictures on Hofer distance for hamiltonian diffeomorphisms on surfaces Frédéric Le Roux Laboratoire de mathématiques CNRS UMR 8628 Université Paris-Sud, Bat. 425
More information第 9 讲 : 股 票 期 权 定 价 : B-S 模 型 Valuing Stock Options: The Black-Scholes Model
1 第 9 讲 : 股 票 期 权 定 价 : B-S 模 型 Valuing Stock Options: The Black-Scholes Model Outline 有 关 股 价 的 假 设 The B-S Model 隐 性 波 动 性 Implied Volatility 红 利 与 期 权 定 价 Dividends and Option Pricing 美 式 期 权 定 价 American
More informationFinite covers of a hyperbolic 3-manifold and virtual fibers.
Claire Renard Institut de Mathématiques de Toulouse November 2nd 2011 Some conjectures. Let M be a hyperbolic 3-manifold, connected, closed and oriented. Theorem (Kahn, Markovic) The fundamental group
More informationMATH 304 Linear Algebra Lecture 9: Subspaces of vector spaces (continued). Span. Spanning set.
MATH 304 Linear Algebra Lecture 9: Subspaces of vector spaces (continued). Span. Spanning set. Vector space A vector space is a set V equipped with two operations, addition V V (x,y) x + y V and scalar
More informationGrey Brownian motion and local times
Grey Brownian motion and local times José Luís da Silva 1,2 (Joint work with: M. Erraoui 3 ) 2 CCM - Centro de Ciências Matemáticas, University of Madeira, Portugal 3 University Cadi Ayyad, Faculty of
More informationSingular fibers of stable maps and signatures of 4 manifolds
359 399 359 arxiv version: fonts, pagination and layout may vary from GT published version Singular fibers of stable maps and signatures of 4 manifolds OSAMU SAEKI TAKAHIRO YAMAMOTO We show that for a
More informationarxiv:1112.0829v1 [math.pr] 5 Dec 2011
How Not to Win a Million Dollars: A Counterexample to a Conjecture of L. Breiman Thomas P. Hayes arxiv:1112.0829v1 [math.pr] 5 Dec 2011 Abstract Consider a gambling game in which we are allowed to repeatedly
More informationSensitivity analysis of European options in jump-diffusion models via the Malliavin calculus on the Wiener space
Sensitivity analysis of European options in jump-diffusion models via the Malliavin calculus on the Wiener space Virginie Debelley and Nicolas Privault Département de Mathématiques Université de La Rochelle
More informationLECTURE III. Bi-Hamiltonian chains and it projections. Maciej B laszak. Poznań University, Poland
LECTURE III Bi-Hamiltonian chains and it projections Maciej B laszak Poznań University, Poland Maciej B laszak (Poznań University, Poland) LECTURE III 1 / 18 Bi-Hamiltonian chains Let (M, Π) be a Poisson
More informationFIELDS-MITACS Conference. on the Mathematics of Medical Imaging. Photoacoustic and Thermoacoustic Tomography with a variable sound speed
FIELDS-MITACS Conference on the Mathematics of Medical Imaging Photoacoustic and Thermoacoustic Tomography with a variable sound speed Gunther Uhlmann UC Irvine & University of Washington Toronto, Canada,
More informationNOTES ON MINIMAL SURFACES
NOTES ON MINIMAL SURFACES DANNY CALEGARI Abstract. These are notes on minimal surfaces, with an emphasis on the classical theory and its connection to complex analysis, and the topological applications
More informationLimits and Continuity
Math 20C Multivariable Calculus Lecture Limits and Continuity Slide Review of Limit. Side limits and squeeze theorem. Continuous functions of 2,3 variables. Review: Limits Slide 2 Definition Given a function
More informationRANDOM INTERVAL HOMEOMORPHISMS. MICHA L MISIUREWICZ Indiana University Purdue University Indianapolis
RANDOM INTERVAL HOMEOMORPHISMS MICHA L MISIUREWICZ Indiana University Purdue University Indianapolis This is a joint work with Lluís Alsedà Motivation: A talk by Yulij Ilyashenko. Two interval maps, applied
More informationNumeraire-invariant option pricing
Numeraire-invariant option pricing Farshid Jamshidian NIB Capital Bank N.V. FELAB, University of Twente Nov-04 Numeraire-invariant option pricing p.1/20 A conceptual definition of an option An Option can
More informationClassification of Cartan matrices
Chapter 7 Classification of Cartan matrices In this chapter we describe a classification of generalised Cartan matrices This classification can be compared as the rough classification of varieties in terms
More informationChapter 7. Continuity
Chapter 7 Continuity There are many processes and eects that depends on certain set of variables in such a way that a small change in these variables acts as small change in the process. Changes of this
More information1 if 1 x 0 1 if 0 x 1
Chapter 3 Continuity In this chapter we begin by defining the fundamental notion of continuity for real valued functions of a single real variable. When trying to decide whether a given function is or
More informationResearch Article Stability Analysis for Higher-Order Adjacent Derivative in Parametrized Vector Optimization
Hindawi Publishing Corporation Journal of Inequalities and Applications Volume 2010, Article ID 510838, 15 pages doi:10.1155/2010/510838 Research Article Stability Analysis for Higher-Order Adjacent Derivative
More informationMetric Spaces. Chapter 7. 7.1. Metrics
Chapter 7 Metric Spaces A metric space is a set X that has a notion of the distance d(x, y) between every pair of points x, y X. The purpose of this chapter is to introduce metric spaces and give some
More informationDimension Theory for Ordinary Differential Equations
Vladimir A. Boichenko, Gennadij A. Leonov, Volker Reitmann Dimension Theory for Ordinary Differential Equations Teubner Contents Singular values, exterior calculus and Lozinskii-norms 15 1 Singular values
More informationRICCI SUMMER SCHOOL COURSE PLANS AND BACKGROUND READING LISTS
RICCI SUMMER SCHOOL COURSE PLANS AND BACKGROUND READING LISTS The Summer School consists of four courses. Each course is made up of four 1-hour lectures. The titles and provisional outlines are provided
More informationThe Ideal Class Group
Chapter 5 The Ideal Class Group We will use Minkowski theory, which belongs to the general area of geometry of numbers, to gain insight into the ideal class group of a number field. We have already mentioned
More informationReference: Introduction to Partial Differential Equations by G. Folland, 1995, Chap. 3.
5 Potential Theory Reference: Introduction to Partial Differential Equations by G. Folland, 995, Chap. 3. 5. Problems of Interest. In what follows, we consider Ω an open, bounded subset of R n with C 2
More informationMetrics on SO(3) and Inverse Kinematics
Mathematical Foundations of Computer Graphics and Vision Metrics on SO(3) and Inverse Kinematics Luca Ballan Institute of Visual Computing Optimization on Manifolds Descent approach d is a ascent direction
More informationMax-Min Representation of Piecewise Linear Functions
Beiträge zur Algebra und Geometrie Contributions to Algebra and Geometry Volume 43 (2002), No. 1, 297-302. Max-Min Representation of Piecewise Linear Functions Sergei Ovchinnikov Mathematics Department,
More informationON TORI TRIANGULATIONS ASSOCIATED WITH TWO-DIMENSIONAL CONTINUED FRACTIONS OF CUBIC IRRATIONALITIES.
ON TORI TRIANGULATIONS ASSOCIATED WITH TWO-DIMENSIONAL CONTINUED FRACTIONS OF CUBIC IRRATIONALITIES. O. N. KARPENKOV Introduction. A series of properties for ordinary continued fractions possesses multidimensional
More informationIRREDUCIBLE OPERATOR SEMIGROUPS SUCH THAT AB AND BA ARE PROPORTIONAL. 1. Introduction
IRREDUCIBLE OPERATOR SEMIGROUPS SUCH THAT AB AND BA ARE PROPORTIONAL R. DRNOVŠEK, T. KOŠIR Dedicated to Prof. Heydar Radjavi on the occasion of his seventieth birthday. Abstract. Let S be an irreducible
More informationFurther Study on Strong Lagrangian Duality Property for Invex Programs via Penalty Functions 1
Further Study on Strong Lagrangian Duality Property for Invex Programs via Penalty Functions 1 J. Zhang Institute of Applied Mathematics, Chongqing University of Posts and Telecommunications, Chongqing
More informationSystems with Persistent Memory: the Observation Inequality Problems and Solutions
Chapter 6 Systems with Persistent Memory: the Observation Inequality Problems and Solutions Facts that are recalled in the problems wt) = ut) + 1 c A 1 s ] R c t s)) hws) + Ks r)wr)dr ds. 6.1) w = w +
More informationCURVES WHOSE SECANT DEGREE IS ONE IN POSITIVE CHARACTERISTIC. 1. Introduction
Acta Math. Univ. Comenianae Vol. LXXXI, 1 (2012), pp. 71 77 71 CURVES WHOSE SECANT DEGREE IS ONE IN POSITIVE CHARACTERISTIC E. BALLICO Abstract. Here we study (in positive characteristic) integral curves
More informationSome Comments on the Derivative of a Vector with applications to angular momentum and curvature. E. L. Lady (October 18, 2000)
Some Comments on the Derivative of a Vector with applications to angular momentum and curvature E. L. Lady (October 18, 2000) Finding the formula in polar coordinates for the angular momentum of a moving
More informationOrthogonal Diagonalization of Symmetric Matrices
MATH10212 Linear Algebra Brief lecture notes 57 Gram Schmidt Process enables us to find an orthogonal basis of a subspace. Let u 1,..., u k be a basis of a subspace V of R n. We begin the process of finding
More informationLECTURE 15: AMERICAN OPTIONS
LECTURE 15: AMERICAN OPTIONS 1. Introduction All of the options that we have considered thus far have been of the European variety: exercise is permitted only at the termination of the contract. These
More information