An Asymptotic Expansion Approach to Computing Greeks
|
|
- Λίγεια Μεσσηνέζης
- 6 χρόνια πριν
- Προβολές:
Transcript
1 An Asymptotic Expansion Approach to Computing Greeks Ryosuke Matsuoka and Akihiko Takahashi Abstract We developed a new scheme for computing Greeks of derivatives by an asymptotic expansion approach. In particular, we derived analytical approximation formulae for Deltas and Vegas of plain vanilla and average call options under general Markovian processes of underlying asset prices. We also derived approximation formulae for Gammas of plain vanilla and average call options, and for Deltas of digital options under CEVConstant Elasticity of Variance processes of underlying assets prices. Moreover, we introduced a new variance reduction method of Monte Carlo simulations based on the asymptotic expansion scheme. Finally, several numerical examples under CEV processes confirmed the validity of our method. This paper presents the authors personal views, and these are not the official views of the Financial Services Agency, the Financial Research and Training Center, and of Tokio Marine & Nichido. Tokio Marine & Nichido Fire Insurance Co., Ltd. Graduate School of Economics, The University of Tokyo, Special Research Fellow at the Financial Research and Training Center, Financial Services Agency 7
2 1 Introduction We propose a new approximation formulae for computing Greeks, such as the Delta, the Gamma and the Vega that indicate risk indices, the first or second order derivatives of the value of an asset with respect to its parameters. In particular, we derive analytic approximation formulae of the Delta and the Vega of plain-vanilla and average options where the underlying assets prices follow general diffusion processes. We also show formulae of the Gamma of plain-vanilla and average options, and a formula of the Delta of digital options where the underlying assets prices follow CEV processes. Our method is based on the asymptotic expansion approach developed by Takahashi[1995,1999, Kunitomo and Takahashi[199,1,3a and Takahashi and Yoshida[4. We also introduce a new variance reduction method as an extension of Takahashi and Yoshida[5 to increase efficiency of Monte Carlo simulation in computation of Greeks. Moreover, we presented series of numerical examples where the underlying prices follow the constant elasticity of variance CEV processes and showed effectiveness of our method. Monitoring and controlling the risks of derivative securities are as important as pricing derivative securities in the practical world. In Black-ScholesBS model, option prices and their Greeks are obtained analytically. However, in the more realistic models, it is usually very hard to evaluate both of option prices and their Greeks analytically. Then, numerical methods are applied. We suppose that the underlying asset s price S t follows a stochastic differential equationsde; { ds t S t dt + σ S t dw t 1 S s >, where W t is a one-dimensional Brownian motion, r q. r and q denote a risk-free rate and a divident rate respectively which are assumed to be constants. Next, we consider a derivative security whose payoff function at maturity time T is given by φ such as where S T 1 T φ S T S T K + φ ST ST K + plain vanilla call option average call option, S t dt. The price of the derivative security can be represented by us E [ e rt φ S T e rt E [φ S T, where E [ denotes the expectation operator under the risk-neutral measure. To obtain the first order derivative of the price with respect to the underlying asset s price at the initial price s, a natural method is computing u s u s + u s, where is a sufficiently small positive number, and u s and u s + are generated by Monte Carlo simulations. However, its convergence speed is sometimes very slow due to the irregularity of φ. Moreover, convergence to the true value may not be achieved because its convergent value depends on. To overcome the problem, we may utilize a representation such as u s e rt E [ φ S T Y T, 73
3 where Y t satisfies the following SDE: { dy t Y t dt + σ S t Y t dw t Y 1. For the derivation, see Imamura, Uchida and Takahashi [5 for instance. Although this representation makes Monte Carlo simulations more efficient, using Monte Carlo simulation itself may be time-consuming, which cause many difficulties in the practical world such as trading business. Therefore, in the case that analytic formulae can not be obtained, ideally we need analytic approximation schemes which can generate values precise enough for practical pupose. The asymptotic expansion approach have been applied successfully to a broad class of Itô processes appearing in finance. Takahashi[1999 presented a third-order pricing formula for plain options and secondorder formulae for more complicated derivatives such as average options, basket options, and options with stochastic volatility in a general Markovian setting. Kunitomo and Takahashi[1 provided pricing formulae for bond optionsswap options and average options based on an interest rate model in the class of Heath-Jarrow-Morton[199 which is not necessarily Markovian. Takahashi[1995 also presented a second order scheme for average options on foreign exchange rates with stochastic interest rates in Heath-Jarrow- Morton framework. Moreover, Takahashi and Yoshida[4 extended the method to dynamic portfolio problems. Recently, Takahashi and Saito[3 successfully applied the method to American options, and Takahashi and Yoshida[5 proposed a new variance reduction scheme of Monte Carlo simulation with the asymptotic expansion. For details of mathematical validity based on the Malliavin calculus and of further applications, see Kunitomo and Takahashi[3a, 3b, 4, Takahashi and Uchida[4 and Takahashi and Yoshda[4,5. The organization of this paper is as follows. In section and 3, we derive approximation formulae for the Delta of plain-vanilla and average call options. In section 4, we introduce a variance reduction technique in computation of the Delta. Sections 5 and 6 treat approximations for computing the Vega of plain vanilla and average call options. In section 7, we propose a variance reduction technique in computation of the Vega. In section 8, when the underlying prices follow CEV processes, we show another derivation of approximation formulae for the Delta and the Vega, and derive approximation formulae for the Gamma of plain vanilla and average options as well as for the Delta of digital options. We present numerical examples in section 9. Finally, some concluding remarks are made in section 1. The Delta of Plain Vanilla Call Option First, we make the following assumption and definitions. Assumption 1. We assume that the underlying asset price S t follows the SDE: { ds t S t dt + ɛσ S t dw t S s > where W t is 1-dimensional Brownian Motion, and. In addition we assume that σ is a C class function and its derivative σ is bounded. We define the differentiation of S t by the initial value s. 74
4 Definition 1. We define Y t as a stocastic process following the SDE: { dy t Y t dt + ɛσ S t Y t dw t Y 1 Definition. We define the defined indicator function: { 1 if x a 1 {x a} if x < a Then, the payoff of Plain Vanilla Call Option is rewritten as S T K + S T K 1 {ST K}. Takahashi [1999 derived, the asymptotic expantion of S t : where S t A t + ɛa 1t + ɛ A t + oɛ, 3 da t A t dt, A s Then, we can easily obtain A t, A 1t and A t as da 1t A 1t dt + σ A t dw t, A 1 da t A t dt + σ A t A 1t dw t, A. A t s e t A 1t A t t t e t s σ A s dw s e t s σ A s A 1s dw s. Now we put X t S t A t /ɛ, g 1 A 1T and g A T /. Then, X T g 1 + ɛ g + oɛ. The asymptotic expantion of the Plain Vanilla Call Option e rt E [ S T K + is given by e rt E [ S T K + ɛ e rt E [ y + X T + ɛ e rt E [ y + g 1 + ɛ g + 1 {g1 +ɛ g + y}, where y A T K /ɛ. Under an appropriate assumption such as Assumption 6. in Kunitomo and Takahashi[3b, We obtain its approximated value as e rt E [ S T K + ɛ e rt E [ y + g 1 1 {g1 y} + ɛ e rt E [ g 1 {g1 y} [ +ɛ e rt E y + g 1 g 1 {g1 y} + o ɛ 75
5 where 1 { y} denotes the derivative of 1 { y}. Next, by the property of Brownian Motion, we know the distribution of g 1 follows a normal distribution N,, where [ E e T t σ A t dw t In addition, the conditional expectation E [g g 1 x is given by E [g g 1 x cx + f, where e T t σ A t dt. 4 c 1 s and f c. Accordingly, e rt E [ S T K + e T s σ A s σ A s e T v σ A v dv ds ɛ e rt y + x n [x;, dx + ɛ e rt cx + f n [x;, dx + o ɛ, y y 5 where n [x;, is the density function of N,, i.e. n [x;, 1 π e x. Now we define an approximated value of the call option as C, T ɛ e rt y + x n [x;, dx + ɛ e rt cx + f n [x;, dx y ɛ e rt y N y y + n [y;, + ɛ e rt f y n [y;,, 6 where N x is cumulative distribution function of N, 1. Next, consider its differentiation by s : s C, T ɛ e rt d N +ɛ e rt f ɛ e rt d N y + y d y s s 1 yd s + y s + 1 n [y;, s 1 + yd y s s y + f d + f y s y +ɛ e rt f s y + f d + c y yd s + y s n [y;, n [y;,, n [y;, 76
6 where d y s e T /ɛ. The derivatives of coefficients are calculated as follows: c { 1 s s 3 s + 1 s s s s s s s e T t σ A t dt e T t e t σ A t σ A t dt e T t σ A t σ A t dt } e T s σ A s σ A s e T v σ A v dv ds e T s σ A s σ A s e T v σ A v dv ds e T σ A s e T v σ A v dv ds e T σ A s σ A s e T v σ A v dv ds e T s σ A s σ A s e T v σ A v σ A v dv ds f c c c s s s s Although it looks quite complicated, simpler expressions of coefficients can be derived if we give σ specific forms such as CEV, which are shown in section 8. Then, we summarize the result obtained above. Theorem 1. The asymptotic expansion of the Delta of a plain vanilla call option of which payoff function with maturity time T is expressed as S T K + is given by where D, T + o ɛ, D, T ɛ e rt d N y +ɛ e rt f s y + f d + c y + 1 n [y;, s 1 + yd y s s n [y;,, 7 and the coefficents are given by y s e T K, ɛ 77
7 [ E e T t σ A t dw t e T t σ A t dt, and c 1 s e T s σ A s σ A s e T v σ A v dv ds 3 The Delta of Average Call Option f c. Utilizing the asymptotic expansion of S t, Takahashi [1999 derived S t Ãt + ɛã1t + ɛ Ãt + oɛ, 8 where S t 1 t t S u du, Ã t 1 Ãt t t A u du and so on. Now we put Xt St /ɛ, g 1 Ã1T and g ÃT /. Then, X T g 1 + ɛ g + oɛ. [ The asymptotic expantion of the average call option e rt E ST K + [ e rt E ST K + [ ɛ e rt E y + X T + is given by ɛ e rt E [ y + g 1 + ɛ g + 1 {g1 +ɛ g + y}, where y ÃT K /ɛ. We obtain its approximated value [ e rt E ST K + ɛ e rt E [ y + g 1 1 {g1 y} + ɛ e rt E [ g 1 {g1 y} [ +ɛ e rt E y + g 1 g 1 {g1 y} + o ɛ, where [ 1 T E T [ 1 T T E [ 1 T T E 1 T t s 1 e t s σ A s dw s dt e t s σ A s dt dw s e T s 1 σ A s dw s e T s 1 σ As ds. 9 78
8 In addition, the coefficients of the conditional expectation E [g g 1 x cx + f are given by 1 T [ t c T 3 e t s e T s 1 σ A s σ A s [ s e s v e T v 1 σ A v dv ds dt and f c. Accordingly, [ e rt E ST K + ɛ e rt y + x n [x;, dx + ɛ e rt y Now we define the approximated value as y cx + f n [x;, dx + o ɛ. C, T ɛ e rt y + x n [x;, dx + ɛ e rt cx + f n [x;, dx y ɛ e rt y N and consider its differentiation by s : s C, T ɛ e rt d N +ɛ e rt f ɛ e rt d N y + y d y y + n [y;, + ɛ e rt f y n [y;,, 1 y s s 1 yd s + y s + 1 n [y;, s 1 + yd y s s y + f d + f y s y +ɛ e rt f s y + f d + c y where d y s yd s + y s n [y;, n [y;,, e T 1 /T ɛ. The derivatives of coefficients are calculated as s 1 T s T T e T s 1 σ As ds e T s 1 e s σ A s σ A s ds e T s e T + e s σ A s σ A s ds, n [y;, 79
9 and c 1 T [ t { s s T 3 e t s e T s 1 σ A s σ A s [ s e s v e T v 1 σ A v dv ds dt} 1 T [ t 3 s T 3 e t s e T s 1 σ A s σ A s [ s e s v t + 1 T 3 [ s e s v t + 1 T 3 [ s e s v t + T 3 [ s e s v Then we sum up the result as a theorem. e T v 1 e t [ e T s 1 e T v 1 e t [ e T s 1 e T v 1 e t s [ e σ A v dv ds dt σ A s σ A v dv ds dt σ A s σ A s σ A v dv ds dt T s 1 σ A s σ A s e T v 1 σ A v σ A v dv ds dt, f s s c c s c s. Theorem. The asymptotic expantion of the Delta of an average call option, whose payoff function with maturity time T is expressed as ST K is given by where D, T ɛ e rt d N and the coefficents are given by + y +ɛ e rt f s y + f d + c y D, T + o ɛ, + 1 n [y;, s 1 + yd y s s y s e T 1 /T K, ɛ n [y;,, 11 8
10 [ 1 E T 1 T d e T 1 ɛt, t e t s σ A s dw s dt e T s 1 σ As ds, c 1 T 3 s t e s v [ e t s [ e e T v 1 T s 1 σ A s σ A s σ A v dv ds dt, and f c. 4 Variance Reduction Technique for Delta of Call Option Previous section showed the validity of the asymptotic expansion technique for the Delta, but we sometimes need more precise values, especially when ɛ is quite large or when the true value is quite small. For this purpose, we propose a variance reduction method, which is an extension of Takahashi and Yoshida[4. Although the value of Delta is obtained by calculating E [ e rt Y T 1 {st K}, it may be impossible to calculate it analytically. In the case, Monte Carlo simulation based on Euler-Maruyama Scheme is a standard method, which is called crude Monte Calro in this paper. However, crude Monte Carlo is usually quite time-consuming because of its low convergence speed, and hence, Takahashi and Yoshida [4 proposed the method based on an asymptotic approach to accelerate the simulation. The convergence speed depends on the variance of sample paths. The smaller the variance, the higher its convergence speed. Let X be a random variable. We take another random variable Y whose expectation is. Then, the random variable X Y has the same expectation as X, and its variance is given by V ar X Y E [X E [X Y E [X E [X E [X E [X Y + E [ Y V ar X + V ar Y Corr X, Y V ar X V ar Y V ar X V ar Y Corr X, Y V ar X V ar Y, where Corr X, Y denotes the correlation between X and Y. Let a >, and we use ay instead of Y. Then, V ar X ay is minimized when a Corr X, Y V arx V ary, and we obtain V ar X ay V ar X Corr X, Y V ar X 1 Corr X, Y V ar X. Thus, we have to find Y whose correlation with X is close to one. 81
11 We utilize the approximated Delta denoted by D, T. In the derivation of the theorem 1 or theorem, we obtain the approximated option price in an integral representation: C, T ɛ e rt y + x n [x;, dx + ɛ e rt cx + f n [x;, dx. y The candidate for a random variable Y is obtained by differentiating it with respect to s. Next, we prepare two lemmas for the ease of calculation. y Lemma 1. Let ϕ x be a C class function. Then 1 {x y} ϕ x dx ϕ y. 1 Proof. 1 {x y} ϕ x dx 1 {x y} ϕ x dx ϕ y Lemma. The differentiation of n [x;, with respect to s is Proof. s n [x;, s n [x;, 1 x s 1 n [x;, 13 s { 1 1/ exp 1 } x 1 π 1 1 3/ exp π s 1 x 1 1 1/ exp 1 s x 1 π 1 x 1 n [x;, s 1 x / exp 1 1 π x 1 x s 8
12 Using lemmas 1 and, the approximation of Delta is obtained as D, T ɛ e rt s ɛ e rt y y + x n [x;, dx + ɛ e rt cx + f n [x;, dx y s y d + 1 x y + x 1 n [x;, dx s +ɛ e rt d cy + f n [y;, c +ɛ e rt x + f n [x;, dx y s s +ɛ e rt 1 cx + f x y 1 n [x;, dx s ɛ e d rt + 1 x y + x 1 n [x;, dx s y +ɛ e rt d cy + f n [y;, c +ɛ e rt x + f n [x;, dx y s s +ɛ e rt 1 cx + f x 1 n [x;, dx. s y On the other hand, D, T is expressed as D, T ɛ e rt E[d + 1 g y + g s +ɛ d cy + f n [y;, + E [ϕ g 1, c s g 1 + f s + 1 cg 1 + f g1 1 s 1 {g1 y} where ϕx ɛ e rt d + 1 x y + x 1 14 s c +ɛ x + f + 1 cx + f x s s 1 1 s {x y} + ɛd cy + f n [y;,. Finally, we set Y ϕ g 1 D, T. We call this new method Hybrid Monte Carlo. 5 The Vega of Plain Vanilla Call Option In the previous section, we obtained an approximated value of Plain Vanilla Call Option price as C, T ɛ e rt y + x n [x;, dx + ɛ e rt cx + f n [x;, dx y ɛ e rt y N y + n [y;, + ɛ e rt f y n [y;,, y 83
13 and consider its differentiation by ɛ to obtain an approximation of the Vega. ɛ C, T ɛ e rt y N ɛ e rt y N y + n [y;, y + n [y;, y N + ɛ e rt f y n [y;, y y n [y;, + y n [y;, +ɛ e rt f y n [y;, ɛ e rt f y n [y;, + ɛ f y3 n [y;, e rt + ɛ f y + f y3 n [y;,. Then, we summarize the result as a theorem. Theorem 3. The asymptotic expantion of the Vega of Plain Vanilla Call option of which payoff function with maturity time T is expressed as S T K + is given by where and the coefficents are given by V, T + o ɛ, V, T e rt + ɛ f y + f y3 n [y;,, 15 y s e T K, ɛ [ E e T t σ A t dw t e T t σ A t dt, and c 1 s e T s σ A s σ A s e T v σ A v dv ds, 6 The Vega of Average Call Option f c. Repeating the similar argument used in the previous sections, we can obtain the approximated value of the Vega of Average Call Option. Hence, we only state the result as a theorem. 84
14 Theorem 4. The asymptotic expantion of the Vega of Average Call option of which payoff function with maturity time T is expressed as S T K +, is given by where and the coefficents are given by V, T + o ɛ, V, T e rt + ɛ f y + f y3 n [y;,, 16 y s e T 1 /T K, ɛ [ 1 E T 1 T d e T 1 ɛt, t e t s σ A s dw s dt e T s 1 σ As ds, c 1 T 3 s t e s v [ e t s [ e e T v 1 T s 1 σ A s σ A s σ A v dv ds dt, and f c. 7 Variance Reduction Technique for Vega of Call Option Previous section showed the validity of the asymptotic expansion technique for the Vega. However, we sometimes need more precise values, especially when ɛ is quite large or when the true value is quite small. For this purpose, we propose a variance reduction method. Although this method is quite similar to the case of Delta, we need some adjustments. We define the differentiation with respect to the volatility coefficient ɛ of S t satisfying the following SDE: { ds t S t dt + ɛσ S t dw t S s > 85
15 Definition 3. We define Z t as a stocastic process which satisfies the SDE: { dz t Z t dt + [σ S t + ɛσ S t Z t dw t Z 17 The value of Vega is obtained by calculating E [ e rt Z T 1 {st K}, but it is sometimes impossible to calculate it analytically. Although we utilize Monte Carlo simulations by using Euler-Maruyama Scheme, it is sometimes time-consuming. In a similar way as Variance Reduction Technique for Delta, let X be the sample path and we introduce a new random variable Y. According to Kunitomo and Takahashi [3b, the asymptotic expantion of S t is obtained by where S t A t + ɛa 1t + ɛ A t +, da t A t dt, A s The asympotic expansion of Z t is also given by da 1t A 1t dt + σ A t dw t, A 1 da t A t dt + σ A t A 1t dw t, A. Z t A 1t + ɛ A t +. Now we put X t S t A t /ɛ, g 1 A 1T and g A T /. Then, the asymptotic expantion of the Vega E [ e rt Z T 1 {st K} is given by E [ e rt Z T 1 {st K} e rt E [ g 1 + ɛ g + 1 {g1 +ɛ g + y}, where y A T K /ɛ. Thus, we obtain its approximated value as E [ e rt Z T 1 {st K} e rt E [ g 1 1 {g1 y} + ɛ e rt E [ g 1 {g1 y} [ +ɛ e rt E g 1 g 1 {g1 y} + o ɛ. Finally, the approximated value of Vega V, T is expressed as where V, T e rt E [ [ g 1 + ɛ g 1 {g1 y} + ɛ e rt E g 1 g 1 {g1 y} e rt E [ [ g 1 + ɛ E [g g 1 1 {g1 y} + ɛ e rt E g 1 E [g g 1 1 {g1 y} e rt E [ g 1 + ɛ c g1 + f [ 1 {g1 y} + ɛ e rt E g 1 c g 1 + f 1 {g1 y} E [ϕ g 1, ϕ x e rt x + ɛ c x + f 1 {x y} e rt y c y + f n [y;,. 18 Finally, we introduce a new random variable Y ϕ g 1 V, T, and implement the variance reduction technique described in section 4. We call this method Hybrid Monte Carlo as in section 4. 86
16 8 The Case of CEV processes 8.1 Another Deriviation of Approximated Value of Delta In this sections we assume the price processes of the underlying asset to be CEV processes: { ds t S t dt + ɛs γ t dw t, < γ 1 S s > 19 Then, we derive the approximation of the Delta in a more straightforward manner. We define Y t as Y t St s. Note that Y t the SDE: { dy t Y t dt + ɛ γ S γ 1 t Y t dw t, Y 1 and the Delta of Plain Vanilla Call Option is obtained by e rt E [ Y T 1 {st K}. 1 See Imamura, Takahashi and Uchida [5 for the derivation for instance. According to Kunitomo and Takahashi [3b, the asymptotic expantion of S t is given by S t A t + ɛa 1t + ɛ A t +, where A t s e t A 1t s γ t A t γ s γ 1 e t e 1 γs dw s t e t e γ s A 1s dw s. Similarly, the asymptotic expantion of Y t is obtained by Y t and B t satisfy SDEs: B t + ɛb 1t + ɛ B t +, where B t, B 1t db t B t dt, B 1 db 1t B 1t dt + γ A γ 1 t B t dw t, B 1 [ db t B t dt + γ γ 1 A γ t A 1t B t + γ A γ 1 t B 1t dw t, B Then, we can easily obtain B t, B 1t, B t as B t 1 s A t B 1t γ s A 1t B t γ 1 s A t. Now we put X t S t A t /ɛ, g 1 A 1T and g A T /, then Therefore, e rt E [ Y T 1 {st K} ɛ e rt E X T g 1 + ɛ g +. [ d + γ g 1 + ɛ γ 1 g + 1 s s {g1 +ɛ g + y}, 87
17 where y s e T K /ɛ and d y s e T /ɛ. We obtain its approximated value as e rt E [ Y T 1 {st K} [ ɛ e rt E [d + γs γ 1 g 1 1 {g1 y} + ɛ e rt E g 1 s {g1 y} +ɛ e rt E [d + γs g 1 g 1 {g1 y} + o ɛ, where 1 { y} means the derivation of 1 { y} in the sense of distribution. By the property of Brownian Motion, we know the distribution of g 1 N,, where [ E { s γ 1 γ e T t σ A t dw t e T t σ A t dt e T e γt if < γ < 1 s T et if γ 1. In addition, the conditional expectation E [g g 1 x cx + f,where c 1 s and f c. Accordingly, e rt E [ Y T 1 {st K} ɛ e rt d + γ x s y e T s σ A s σ A s e T v σ A v dv ds γ s 4γ 1 e 3T 1 e 1 γt 8 1 γ if < γ < 1 s 3 T e3t if γ 1, n [x;, dx + ɛ e rt γ 1 s +ɛ e rt d + γ s y cy + f n [ y;, + o ɛ. Thus we obtain the approximation as y ɛ e d rt N + γ s + ɛ y cx + f n [x;, dx d γ cy y + f + ɛ γ 1 f y n [y;,. s s where N x denotes a cumulative distribution function of standard normal distribution N, 1. Finally we see the agreement of the two approximated values derived in different manners. theorem 1, the approximated value of the Delta is given by By the D, T ɛ e rt d N y +ɛ e rt f s y + f d + c y + 1 n [y;, s 1 + yd y s s n [y;,. 88
18 In addition, the coefficients, c, f are monomials of s, and their differentiation with respect to s are Substituting them, we obtain s γ s, c s c s, D, T y ɛ e d rt N + γ n [y;, s γ 1 γ +ɛ e rt f y + f d + c y s s y ɛ e d rt N + γ n [y;, s +ɛ e rt γ 1 s f y + c y + f Hence, the two approximated values agree. Then we sum up the fact as a theorem. f γ 1 f. s s + yd γ y n [y;, s d γ y n [y;,. s Theorem 5. The asymptotic expantion of the Delta of Plain Vanilla Call option, whose payoff function with maturity time T is expressed as S T K +, is given by where D, T + o ɛ, D, T ɛ e rt d N and the coefficents are given by y + γ n [y;, s +ɛ e rt γ 1 s f y + c y + f y s e T K, ɛ [ E e T t σ A t dw t e T t σ A t dt { s γ 1 γ d γ y n [y;,, s e T e γt if < γ < 1 s T et if γ 1, c 1 s e T s σ A s σ A s e T v σ A v dv ds γ s 4γ 1 e 3T 1 e 1 γt 8 1 γ if < γ < 1 s 3 T e3t if γ 1, 89
19 and f c. Similarly, we gain the approximation formula for the Delta of the average option. Theorem 6. The asymptotic expantion of the Delta of Average Call option, whose payoff function with maturity time T is expressed as ST K, is given by D, T + o ɛ, where + D, T ɛ e rt d N y + γ n [y;, s +ɛ e rt γ 1 s f y + c y + f d γ y n [y;,, s 3 and the coefficents are given by y s e T 1 /T K, ɛ 1 T e T t 1 s γ T { e T 1 γ s T s e T T σ A t dt et 1 γ 1 d e T 1 ɛt, T + e γt γ1 γ1 γ T et 1 {e T T 3 + et 1 } } if < γ < 1, γ 1 if γ 1 if γ 1, 9
20 c and 1 T [ t T 3 e t s e T s 1 σ A s σ A s [ s e s v e T v 1 σ A v dv ds dt 1 + e T γ + e T 1 + γ +e 4γ 1T γ 7 + 1γ γ γ γ s 4γ 1 +e 1+γT 6 44γ + 96γ 64γ 3 5 T 3 +4e γt γ 3γ + 16γ 3 +e T γ γ + 48γ 3 e T 3 8γ + 89γ 11γ γ 4 /γ 3 16γ + 16γ /8 1 3γ + γ { } s e 3T + e T 1 T + e T 1 T + T T s 3 { 5 T e 3T T 3T e T T et 1 3} f c. if < γ < 1, γ 1 if γ 1 if γ 1, 8. The Gamma of Call Option The approximated value of Delta of Plain Vanilla Average Call Option is given by where D, T ɛ e rt d N D, T + o ɛ, y + γ n [y;, s +ɛ e rt γ 1 s f y + c y + f d γ y n [y;,. s Then, we can differentiate it with respect to s again. We get an approximated value of the Gamma. Theorem 7. The asymptotic expantion of the Gamma of Plain Vanilla Call option, whose payoff function with maturity time T is expressed as S T K +, is given by G, T + o ɛ, 91
21 where G, T ɛ e rt d γ d y γ s s + γ s + γ s y ɛ e d rt γ cy y + f + γ 1 s s γ +ɛ e rt + s y γ cy d + f + s γ 1 s f y + γ 1 f dn [y;,, s and the coefficents are given by n [y;, 4 γ f y + y d γ 1 y n [y;, s s c y + c y d + γ 1 f s s d γ s y y s e T K, ɛ [ E e T t σ A t dw t e T t σ A t dt { s γ 1 γ e T e γt if < γ < 1 s T et if γ 1, and c 1 s e T s σ A s σ A s e T v σ A v dv ds γ s 4γ 1 e 3T 1 e 1 γt 8 1 γ if < γ < 1 s 3 T e3t if γ 1, 8.3 The Delta of Digital Option f c. We consider the Digital Option whose payoff function at maturity time T is given by 1 {K1 S T K }. Before considering the Delta of Digital Option, we note that its price is represented by e rt E [ 1 {K1 S T K }. As above, X T g 1 + ɛ g +, where X t S t A t /ɛ, and e rt E [ 1 {K1 S T K } e rt E [ 1 { y1 X T y } e rt E [ 1 { y1 g 1 +ɛ g + y }, 9
22 where y 1 A T K 1 /ɛ and y A T K /ɛ. We obtain its approximated value as e rt E [ 1 {K1 S T K } e rt E [ [ 1 { y1 g 1 y } + ɛ e rt E g 1 { y1 g 1 y } + o ɛ e rt {N y1 N y } +ɛ cy 1 + f n [y 1 ;, ɛ cy + f n [y ;,. Its differentiation corresponds to the Delta of the Digital option. Theorem 8. The asymptotic expantion of the Delta of Digital option, whose payoff function of with maturity time T is expressed as 1 {K1 S T K }, is given by where D, T d γs y 1 +ɛ c y1 + c y 1 d + γ 1 s d γs y +ɛ and the coefficents are given by D, T + o ɛ, f + cy1 + f s γ s y 1d + y 1 γ s n [y 1 ;, c y + c y d + γ 1 f + cy + f γ y d s s s + y γ n [y ;,, s y 1 s e T K 1 ɛ, y s e T K, ɛ [ E e T t σ A t dw t e T t σ A t dt { s γ 1 γ e T e γt if < γ < 1 s T et if γ 1, 5 and c 1 s e T s σ A s σ A s e T v σ A v dv ds γ s 4γ 1 e 3T 1 e 1 γt 8 1 γ if < γ < 1 s 3 T e3t if γ 1, f c. 93
23 9 Numerical Examples The BSBlack-Sholes model is represented as { ds t S t dt + ɛs t dw t S s >, 6 and the CEV Constant Elasticity of Variance model is represented as { ds t S t dt + ɛs γ t dw t, < γ < 1 S s >. Hence, the volatility function of the models are expressed as σ S t S γ t < γ Approximation for the Delta of Plain Vanilla Option We apply the asymptotic expansion scheme to the BS and CEV processes. The coefficients are calculated as [ and E c 1 { s γ 1 γ s e T t σ A t dw t e T t σ A t dt e T e γt if < γ < 1 s T et if γ 1, e T s σ A s σ A s e T v σ A v dv ds γ s 4γ 1 e 3T 1 e 1 γt 8 1 γ if < γ < 1 s 3 T e3t if γ 1. The coefficients, c, and f are the function of s, T, γ and. In particular, paying attention to γ, we represent γ, c c γ. We can easily check the continuity at γ 1, i.e. γ 1 and c γ c 1,as γ 1. We apply the theorem 5 and obtain the approximated value of the Delta. We show some numerical examples figure 1. The initial value s is fixed to s 1. For the true values, we use the analytical values for BS model γ 1, and use the mean of 1,, paths generated by Euler-Maruyama scheme that divides one year to 365 intervals for CEV model γ < 1. The error ratio is calculated as approximate value true value /true value. We can observe that the accuracy of this approximation is valid. 94
24 9. Approximation for the Delta of Average Option We apply the asymptotic expansion scheme to the BS and CEV processes. The coefficients are calculated as 1 T e T t 1 s γ T { e T 1 γ s T s e T T σ A t dt et 1 γ 1 T + e γt γ1 γ1 γ T et 1 {e T T 3 + et 1 } } if < γ < 1, γ 1 if γ 1 if γ 1, and c 1 T [ t T 3 e t s e T s 1 σ A s σ A s [ s e s v e T v 1 σ A v dv ds dt 1 + e T γ + e T 1 + γ +e 4γ 1T γ 7 + 1γ γ γ γ s 4γ 1 +e 1+γT 6 44γ + 96γ 64γ 3 5 T 3 +4e γt γ 3γ + 16γ 3 +e T γ γ + 48γ 3 e T 3 8γ + 89γ 11γ γ 4 /γ 3 16γ + 16γ /8 1 3γ + γ { } s e 3T + e T 1 T + e T 1 T + T T s 3 { 5 T e 3T T 3T e T T et 1 3} if < γ < 1, γ 1 if γ 1 if γ 1. As with the Plain Vanilla case, the coefficients, c, and f are the function of s, T, γ and. We can easily check the continuity at γ 1, i.e. γ 1 and c γ c 1,as γ 1. We apply the theorem 6 and obtain the approximated value of the Delta. We show some numerical examples figure. The initial value s is fixed to s 1. For the true values, we use the analytical values for BS model γ 1, and use the mean of 1,, paths generated by Euler-Maruyama scheme that divides one year to 365 intervals for CEV model γ < 1. The error ratio is calculated as approximate value true value /true value. We can observe that the accuracy of this approximation is valid in general. 95
25 9.3 Computaion of Delta by the Variance Reduction Technique In this section, we show some numerical examples of variance reduction method. We use the BS and CEV models as the dynamics of stock prices. The result of Plain Vanilla Delta is exhibited in figure 3. In theorem 5, the Delta of Plain Vanilla Call Option is obtained by e rt E [ Y T 1 {st K}, and its asymptotic expansion is expressed as e rt E [ [ Y T 1 {st K} ɛ e rt E d + γ g 1 + ɛ γ 1 g + s s where y s e T K /ɛ and d y s 1 {g1 +ɛ g + y} e T /ɛ. Then, we obtained its approximated value D, T [ ɛ e rt E [d + γs γ 1 g 1 1 {g1 y} + ɛ e rt E g 1 s {g1 y} +ɛ e rt E [d + γs g 1 g 1 {g1 y} [ ɛ e rt E [d + γs γ 1 g 1 1 {g1 y} + ɛ e rt E E [g g 1 1 s {g1 y} +ɛ e rt E [d + γs g 1 E [g g 1 1 {g1 y} [ ɛ e rt E [d + γs γ 1 g 1 1 {g1 y} + ɛ e rt E c g s 1 + f 1 {g1 y} [ +ɛ e rt E d + γ c g 1 g s 1 + f 1 {g1 y} E [ϕ g 1, where ϕ x ɛ e rt d + γ x + γ 1 ɛ c x + f s s, 1 {x y} + ɛ e rt d γ s y c y + f n [y;,. Next, we define Y as Y ϕ g 1 D, T, and call this Y Attendant random variable of X generated by Crude Monte Carlo. In the simulation, the initial value s is fixed to s 1. For the true values, we use the analytical values for BS model γ 1, and use the mean of,, paths generated by Euler-Maruyama scheme that divides one year to 365 intervals for CEV model γ < 1. The errors 1, and 3 are defined by X true value /true value, Y/approximated value and X Y true value / true value, respectively. We generated 1 passes and took their average, and repeated it by 1 cases. We calculated the correlation between X and Y, and the average, standard deviation, maximum and minimum of 1 cases for each of six random variablesx, Y, X Y and errors 1,,3. The example of Average Delta is exhibited in figure 4. Items on the table are the same as above. We can observe that the standard deviaition as well as maximum and minimum values of the errors of HybridMCerror 3 are reduced for each case relative to those of CrudeMCerror
26 9.4 Approximation for the Vega of Plain Vanilla Option We apply the asymptotic expansion scheme to the BS and CEV processes. The coefficients are calculated as [ and E c 1 { s γ 1 γ s e T t σ A t dw t e T t σ A t dt e T e γt if < γ < 1 s T et if γ 1, e T s σ A s σ A s e T v σ A v dv ds γ s 4γ 1 e 3T 1 e 1 γt 8 1 γ if < γ < 1 s 3 T e3t if γ 1. We apply the theorem 3 and get the approximated value of the Delta. We show some numerical examples figure 5. The initial value s is fixed to s 1. For the true values, we use the analytical values for BS model γ 1, and use the mean of 1,, paths generated by Euler-Maruyama scheme that divides one year to 365 intervals for CEV model γ < 1. The error ratio is calculated as approximated value true value /true value. We can see that the accuracy of this approximation is generally valid. 97
27 9.5 Approximation for the Vega of Average Option We apply the asymptotic expansion scheme to the BS and CEV processes. The coefficients are calculated as 1 T e T t 1 s γ T { e T 1 γ s T s e T T σ A t dt et 1 γ 1 T + e γt γ1 γ1 γ T et 1 {e T T 3 + et 1 } } if < γ < 1, γ 1 if γ 1 if γ 1, and c 1 T [ t T 3 e t s e T s 1 σ A s σ A s [ s e s v e T v 1 σ A v dv ds dt 1 + e T γ + e T 1 + γ +e 4γ 1T γ 7 + 1γ γ γ γ s 4γ 1 +e 1+γT 6 44γ + 96γ 64γ 3 5 T 3 +4e γt γ 3γ + 16γ 3 +e T γ γ + 48γ 3 e T 3 8γ + 89γ 11γ γ 4 /γ 3 16γ + 16γ /8 1 3γ + γ { } s e 3T + e T 1 T + e T 1 T + T T s 3 { 5 T e 3T T 3T e T T et 1 3} if < γ < 1, γ 1 if γ 1 if γ 1. We apply the theorem 4 and obtained the approximated value of the Delta. We show some numerical examples figure 6. The initial value s is fixed to s 1. For the true values, we use the analytical values for BS model γ 1, and use the mean of 1,, paths generated by Euler-Maruyama scheme that divides one year to 365 intervals for CEV model γ < 1. The error ratio is calculated as approximated value true value /true value. As above, we can see that the accuracy of this approximation is valid. 98
28 9.6 Computation of Vega by the Variance Reduction Technique In this section, we show some numerical examples of variance reduction method. We use the BS and CEV models as the dynamics of stock prices. The example of Plain Vanilla Vega is exhibited in figure 7. The random variables X and Y correspond to Crude MC and Attendant, respectively. The initial value s is fixed to s 1. For the true values, we use the analytical values for BS model γ 1, and use the mean of,, paths generated by Euler-Maruyama scheme that divides one year to 365 intervals for CEV model γ < 1. The error 1, and 3 are defined byx true value /true value, Y/approximated value, and the error 3 is X Y true value /true value, respectively. We generated 1 passes and took their average, and repeated it by 1 cases. We calculated the correration between X and Y, and average, standard deviation, maximum and minimum of 1 cases for each of the six random variablesx, Y, X Y and errors 1,,3. The example of Average Vega is exhibited in figure 8. Items on the table are the same as above. We can observe that the standard deviaition as well as maximum and minimum values of the errors of HybridMCerror 3 are reduced for each case relative to those of CrudeMCerror 1. 1 Concluding Remarks We developed an asymptotic expansion method for computing Greeks. Because it takes almost no time to compute the approximated values, it would be useful for monitoring Greeks changing rapidly in volatile markets. We also introduced so called Hybrid Monte Carlo, a variance reduction technique based on combination of Monte Carlo simulation and the asymptotic expansion. We showed that our variance reduction technique can accelerate Monte Carlo simulations. Although we mainly treated the Delta and the Vega, our method can also be applied to computing the other Greeks such as Gamma; it is obtained by differentiating the approximated Delta by the initial price of the underlying asset. Clearly, the same method can be applied to term structure models and credit models such as Heath- Jarrow-Morton models, Market models and Duffie-Singleton models, which are topics in the next research. 99
29 European Call Delta r T σ γ K True Value Approximation error ratio 1% 1 1% % 1% 1 1% % 1% 1 1% % 1% 1 1% % 1% 1 % % 1% 1 % % 1% 1 % % 1% 1 % % 1% 1 3% % 1% 1 3% % 1% 1 3% % 1% 1 3% % 1% 1 4% % 1% 1 4% % 1% 1 4% % 1% 1 4% % 1%.1 % % 1%.1 % % 1%.1 % % 1%.1 % % 1% 1 % % 1% 1 % % 1% 1 % % 1% 1 % % 1% 1 % % 1% 1 % % 1% 1 % % 1% 1 % % 1% 1 % % 1% 1 % % 1% 1 % % 1% 1 % % 1% 1 % % 1% 1 % % 1% 1 % % 1% 1 % % 1% 1 % % 1% 1 % % 1% 1 % % 1%.1 % % 1%.1 % % 1% 1 % % 1% 1 % % 1% 1 % % 1% 1 % % 1% 1 % % 1% 1 % % 1% 1 % % 1% 1 % % 1% 1 % % 1% 1 % % 1% 1 % % 1% 1 % % 1% 1 % % 1% 1 % % 1% 1 % % 1% 1 % % 1% 1 % % 1% 1 % % 1% 1 % % 1% 1 % % 1% 1 3% % 1% 1 3% % 1% 1 3% % 1% 1 3% % Figure 1: Delta of Plain Vanilla Option 1
30 Asian Call Delta r T σ γ K True Value Approximation error ratio 1% 1 1% % 1% 1 1% % 1% 1 1% % 1% 1 1% % 1% 1 % % 1% 1 % % 1% 1 % % 1% 1 % % 1% 1 3% % 1% 1 3% % 1% 1 3% % 1% 1 3% % 1% 1 4% % 1% 1 4% % 1% 1 4% % 1% 1 4% % 5%.5 % % 5%.5 % % 5%.5 % % 5%.5 % % 5% 1 % % 5% 1 % % 5% 1 % % 5% 1 % % 5% 1 3% % 5% 1 3% % 5% 1 3% % 5% 1 3% % 1%.5 % % 1%.5 % % 1%.5 % % 1%.5 % % 1% 1 % % 1% 1 % % 1% 1 % % 1% 1 % % 1% 1 3% % 1% 1 3% % 1% 1 3% % 1% 1 3% % 1% 1 % % 1% 1 % % 1% 1 % % 1% 1 % % 1% 1 % % 1% 1 % % 1% 1 % % 1% 1 % % 1% 1 % % 1% 1 % % 1% 1 % % 1% 1 % % 1% 1 % % 1% 1 % % 1% 1 % % 1% 1 % % 1% 1 % % 1% 1 % % 1% 1 % % 1% 1 % % 5% 1 % % 5% 1 % % 5% 1 % % 5% 1 % % 5%.5 3% % 5%.5 3% % 5%.5 3% % 5%.5 3% % 5% 1 3% % 5% 1 3% % 5% 1 3% % 5% 1 3% % 1% 1 % % 1% 1 % % 1% 1 % % 1% 1 % % 1%.1 3% % 1%.1 3% % 1%.1 3% % 1%.1 3% % 1%.5 3% % 1%.5 3% % 1%.5 3% % 1%.5 3% % Figure : Delta of Average Option
31 * +, -!!! "#!! "!!! $ % & '!!!! "#!! "!!!! $ % & '!!!! "#! " $ % & '!!!!! "#!!! "! $ % & '! "#!! "! $ % & '!!!!!! "# " $ % & ' Figure 3: Variance Reduction for Plain Vanilla Delta 1
32 * +,! "# "! $ % & '! "# "! $ % & '! "# "! $ % & '! "# "! $ % & '! "# "! $ % & '! "# "! $ % & ' Figure 4: Variance Reduction for Average Delta 13
33 European Call Vega r T σ γ K True Value Approximation error ratio 1% 1 1% % 1% 1 1% % 1% 1 1% % 1% 1 1% % 1% 1 % % 1% 1 % % 1% 1 % % 1% 1 % % 1% 1 3% % 1% 1 3% % 1% 1 3% % 1% 1 3% % 1% 1 4% % 1% 1 4% % 1% 1 4% % 1% 1 4% % 1%.5 % % 1%.5 % % 1%.5 % % 1%.5 % % 1% 1 % % 1% 1 % % 1% 1 % % 1% 1 % % 1% 1 3% % 1% 1 3% % 1% 1 3% % 1% 1 3% % 1% 1 % % 1% 1 % % 1% 1 % % 1% 1 % % 1% 1 3% % 1% 1 3% % 1% 1 3% % 1% 1 3% % 1% 1 % % 1% 1 % % 1% 1 % % 1% 1 % % Figure 5: Vega of Plain Vanilla Option 14
34 Asian Call Vega r T σ γ K True Value Approximation error ratio 1% 1 1% % 1% 1 1% % 1% 1 1% % 1% 1 1% % 1% 1 % % 1% 1 % % 1% 1 % % 1% 1 % % 1% 1 3% % 1% 1 3% % 1% 1 3% % 1% 1 3% % 1% 1 4% % 1% 1 4% % 1% 1 4% % 1% 1 4% % 1%.5 % % 1%.5 % % 1%.5 % % 1%.5 % % 1% 1 % % 1% 1 % % 1% 1 % % 1% 1 % % 1% 1 3% % 1% 1 3% % 1% 1 3% % 1% 1 3% % 1% 1 % % 1% 1 % % 1% 1 % % 1% 1 % % 1% 1 3% % 1% 1 3% % 1% 1 3% % 1% 1 3% % 1% 1 % % 1% 1 % % 1% 1 % % 1% 1 % % Figure 6: Vega of Average Option 15
35 * +,!"! # # # # $ % & ' #!"! # # # # $ % & ' # # # #!"! # # # # $ % & ' # # #!"! # # # # $ % & '!"! # # # # $ % & ' Figure 7: Variance Reduction for Plain Vanilla Vega 16
36 * +!!!! "#!! "!! $ % & '!!!! "# "!! $ % & '!!!!! "#!!!!!! "!!! $ % & '!!!! "#!! "! $ % & ' Figure 8: Variance Reduction for Average Vega 17
37 Reference [1 Imamura, S, Takahashi, A., and Uchida, Y. 5, On Risk Sensitivity Analysis of Options Based on Malliavin Calculus, Monetary and Economic Studies, Vol Bank of Japan in Japanese. [ Kunitomo, N. and Takahashi, A. 1, The Asymptotic Expansion Approach to the Valuation of Interest Rate Contingent Claims, Mathematical Finance, Vol.11, [3 Kunitomo, N. and Takahashi, A. 3a, On Validity of the Asymptotic Expansion Approach in Contingent Claim Analysis, Annals of Applied Probability Vol.13, No.3, Aug. 3. [4 Kunitomo, N. and Takahashi, A. 3b, Foundation of Mathematical Finance-Application of Malliavin Calculus and Asymptotic Expansion Method-, Toyo-Keizai in Japanese. [5 Kunitomo, N. and Takahashi, A. 4, Applications of the Asymptotic Expansion Approach based on Malliavin-Watanabe Calculus in Financial Problems, Stochastic Processes and Applications to Mathematical Finance, 195-3, World Scientific. [6 Takahashi, A. 1995, Essays on the Valuation Problems of Contingent Claims, Unpublished Ph.D. Dissertation, Haas School of Business, University of California, Berkeley. [7 Takahashi, A. 1999, An Asymptotic Expansion Approach to Pricing Contingent Claims, Asia-Pacific Financial Markets, Vol.6, [8 Takahashi, A. and Matsushima, S.4, Monte Carlo Simulation with an Asymptotic Expansion in HJM Framework, FSA Research Review 4, 8-13, Financial Services Agency in Japanese. [9 Takahashi, A. and Saito, T.3, An Asymptotic Expansion Approach to Pricing American Options, Monetary and Economic Studies, Vol., 35-87, Bank of Japan in Japanese. [1 Takahashi, A. and Uchida, Y.4, New Acceleration Schemes with the Asymptotic Expansion in Monte Carlo Simulation, Discussion Paper Series, CIRJE-F-98, Faculty of Economics, The University of Tokyo, Forthcoming in Advances in Mathematical Economics. [11 Takahashi, A. and Yoshida, N.5, Monte Carlo Simulation with Asymptotic Method, Discussion Paper Series, CIRJE-F-335, Faculty of Economics, The University of Tokyo, Forthcoming in The Journal of Japan Statistical Society. [1 Takahashi, A. and Yoshida, N.4, An Asymptotic Expansion Scheme for Optimal Investment Problems, Statistical Inference for Stochastic Processes, Vol.7-,
4.6 Autoregressive Moving Average Model ARMA(1,1)
84 CHAPTER 4. STATIONARY TS MODELS 4.6 Autoregressive Moving Average Model ARMA(,) This section is an introduction to a wide class of models ARMA(p,q) which we will consider in more detail later in this
Διαβάστε περισσότεραStatistical Inference I Locally most powerful tests
Statistical Inference I Locally most powerful tests Shirsendu Mukherjee Department of Statistics, Asutosh College, Kolkata, India. shirsendu st@yahoo.co.in So far we have treated the testing of one-sided
Διαβάστε περισσότερα2 Composition. Invertible Mappings
Arkansas Tech University MATH 4033: Elementary Modern Algebra Dr. Marcel B. Finan Composition. Invertible Mappings In this section we discuss two procedures for creating new mappings from old ones, namely,
Διαβάστε περισσότεραHomework 3 Solutions
Homework 3 Solutions Igor Yanovsky (Math 151A TA) Problem 1: Compute the absolute error and relative error in approximations of p by p. (Use calculator!) a) p π, p 22/7; b) p π, p 3.141. Solution: For
Διαβάστε περισσότεραST5224: Advanced Statistical Theory II
ST5224: Advanced Statistical Theory II 2014/2015: Semester II Tutorial 7 1. Let X be a sample from a population P and consider testing hypotheses H 0 : P = P 0 versus H 1 : P = P 1, where P j is a known
Διαβάστε περισσότεραOther Test Constructions: Likelihood Ratio & Bayes Tests
Other Test Constructions: Likelihood Ratio & Bayes Tests Side-Note: So far we have seen a few approaches for creating tests such as Neyman-Pearson Lemma ( most powerful tests of H 0 : θ = θ 0 vs H 1 :
Διαβάστε περισσότεραHOMEWORK 4 = G. In order to plot the stress versus the stretch we define a normalized stretch:
HOMEWORK 4 Problem a For the fast loading case, we want to derive the relationship between P zz and λ z. We know that the nominal stress is expressed as: P zz = ψ λ z where λ z = λ λ z. Therefore, applying
Διαβάστε περισσότεραConcrete Mathematics Exercises from 30 September 2016
Concrete Mathematics Exercises from 30 September 2016 Silvio Capobianco Exercise 1.7 Let H(n) = J(n + 1) J(n). Equation (1.8) tells us that H(2n) = 2, and H(2n+1) = J(2n+2) J(2n+1) = (2J(n+1) 1) (2J(n)+1)
Διαβάστε περισσότεραderivation of the Laplacian from rectangular to spherical coordinates
derivation of the Laplacian from rectangular to spherical coordinates swapnizzle 03-03- :5:43 We begin by recognizing the familiar conversion from rectangular to spherical coordinates (note that φ is used
Διαβάστε περισσότεραP AND P. P : actual probability. P : risk neutral probability. Realtionship: mutual absolute continuity P P. For example:
(B t, S (t) t P AND P,..., S (p) t ): securities P : actual probability P : risk neutral probability Realtionship: mutual absolute continuity P P For example: P : ds t = µ t S t dt + σ t S t dw t P : ds
Διαβάστε περισσότερα6.3 Forecasting ARMA processes
122 CHAPTER 6. ARMA MODELS 6.3 Forecasting ARMA processes The purpose of forecasting is to predict future values of a TS based on the data collected to the present. In this section we will discuss a linear
Διαβάστε περισσότεραCHAPTER 25 SOLVING EQUATIONS BY ITERATIVE METHODS
CHAPTER 5 SOLVING EQUATIONS BY ITERATIVE METHODS EXERCISE 104 Page 8 1. Find the positive root of the equation x + 3x 5 = 0, correct to 3 significant figures, using the method of bisection. Let f(x) =
Διαβάστε περισσότεραforms This gives Remark 1. How to remember the above formulas: Substituting these into the equation we obtain with
Week 03: C lassification of S econd- Order L inear Equations In last week s lectures we have illustrated how to obtain the general solutions of first order PDEs using the method of characteristics. We
Διαβάστε περισσότεραΑπόκριση σε Μοναδιαία Ωστική Δύναμη (Unit Impulse) Απόκριση σε Δυνάμεις Αυθαίρετα Μεταβαλλόμενες με το Χρόνο. Απόστολος Σ.
Απόκριση σε Δυνάμεις Αυθαίρετα Μεταβαλλόμενες με το Χρόνο The time integral of a force is referred to as impulse, is determined by and is obtained from: Newton s 2 nd Law of motion states that the action
Διαβάστε περισσότεραCredit Risk. Finance and Insurance - Stochastic Analysis and Practical Methods Spring School Jena, March 2009
Credit Risk. Finance and Insurance - Stochastic Analysis and Practical Methods Spring School Jena, March 2009 1 IV. Hedging of credit derivatives 1. Two default free assets, one defaultable asset 1.1 Two
Διαβάστε περισσότεραEvery set of first-order formulas is equivalent to an independent set
Every set of first-order formulas is equivalent to an independent set May 6, 2008 Abstract A set of first-order formulas, whatever the cardinality of the set of symbols, is equivalent to an independent
Διαβάστε περισσότεραPhys460.nb Solution for the t-dependent Schrodinger s equation How did we find the solution? (not required)
Phys460.nb 81 ψ n (t) is still the (same) eigenstate of H But for tdependent H. The answer is NO. 5.5.5. Solution for the tdependent Schrodinger s equation If we assume that at time t 0, the electron starts
Διαβάστε περισσότεραPartial Differential Equations in Biology The boundary element method. March 26, 2013
The boundary element method March 26, 203 Introduction and notation The problem: u = f in D R d u = ϕ in Γ D u n = g on Γ N, where D = Γ D Γ N, Γ D Γ N = (possibly, Γ D = [Neumann problem] or Γ N = [Dirichlet
Διαβάστε περισσότεραMath221: HW# 1 solutions
Math: HW# solutions Andy Royston October, 5 7.5.7, 3 rd Ed. We have a n = b n = a = fxdx = xdx =, x cos nxdx = x sin nx n sin nxdx n = cos nx n = n n, x sin nxdx = x cos nx n + cos nxdx n cos n = + sin
Διαβάστε περισσότεραProblem Set 3: Solutions
CMPSCI 69GG Applied Information Theory Fall 006 Problem Set 3: Solutions. [Cover and Thomas 7.] a Define the following notation, C I p xx; Y max X; Y C I p xx; Ỹ max I X; Ỹ We would like to show that C
Διαβάστε περισσότεραApproximation of distance between locations on earth given by latitude and longitude
Approximation of distance between locations on earth given by latitude and longitude Jan Behrens 2012-12-31 In this paper we shall provide a method to approximate distances between two points on earth
Διαβάστε περισσότεραFourier Series. MATH 211, Calculus II. J. Robert Buchanan. Spring Department of Mathematics
Fourier Series MATH 211, Calculus II J. Robert Buchanan Department of Mathematics Spring 2018 Introduction Not all functions can be represented by Taylor series. f (k) (c) A Taylor series f (x) = (x c)
Διαβάστε περισσότεραOrdinal Arithmetic: Addition, Multiplication, Exponentiation and Limit
Ordinal Arithmetic: Addition, Multiplication, Exponentiation and Limit Ting Zhang Stanford May 11, 2001 Stanford, 5/11/2001 1 Outline Ordinal Classification Ordinal Addition Ordinal Multiplication Ordinal
Διαβάστε περισσότεραk A = [k, k]( )[a 1, a 2 ] = [ka 1,ka 2 ] 4For the division of two intervals of confidence in R +
Chapter 3. Fuzzy Arithmetic 3- Fuzzy arithmetic: ~Addition(+) and subtraction (-): Let A = [a and B = [b, b in R If x [a and y [b, b than x+y [a +b +b Symbolically,we write A(+)B = [a (+)[b, b = [a +b
Διαβάστε περισσότερα3.4 SUM AND DIFFERENCE FORMULAS. NOTE: cos(α+β) cos α + cos β cos(α-β) cos α -cos β
3.4 SUM AND DIFFERENCE FORMULAS Page Theorem cos(αβ cos α cos β -sin α cos(α-β cos α cos β sin α NOTE: cos(αβ cos α cos β cos(α-β cos α -cos β Proof of cos(α-β cos α cos β sin α Let s use a unit circle
Διαβάστε περισσότεραSolution Series 9. i=1 x i and i=1 x i.
Lecturer: Prof. Dr. Mete SONER Coordinator: Yilin WANG Solution Series 9 Q1. Let α, β >, the p.d.f. of a beta distribution with parameters α and β is { Γ(α+β) Γ(α)Γ(β) f(x α, β) xα 1 (1 x) β 1 for < x
Διαβάστε περισσότεραUniform Convergence of Fourier Series Michael Taylor
Uniform Convergence of Fourier Series Michael Taylor Given f L 1 T 1 ), we consider the partial sums of the Fourier series of f: N 1) S N fθ) = ˆfk)e ikθ. k= N A calculation gives the Dirichlet formula
Διαβάστε περισσότεραAreas and Lengths in Polar Coordinates
Kiryl Tsishchanka Areas and Lengths in Polar Coordinates In this section we develop the formula for the area of a region whose boundary is given by a polar equation. We need to use the formula for the
Διαβάστε περισσότεραC.S. 430 Assignment 6, Sample Solutions
C.S. 430 Assignment 6, Sample Solutions Paul Liu November 15, 2007 Note that these are sample solutions only; in many cases there were many acceptable answers. 1 Reynolds Problem 10.1 1.1 Normal-order
Διαβάστε περισσότεραΤΟ ΜΟΝΤΕΛΟ Οι Υποθέσεις Η Απλή Περίπτωση για λi = μi 25 = Η Γενική Περίπτωση για λi μi..35
ΑΡΙΣΤΟΤΕΛΕΙΟ ΠΑΝΕΠΙΣΤΗΜΙΟ ΘΕΣΣΑΛΟΝΙΚΗΣ ΣΧΟΛΗ ΘΕΤΙΚΩΝ ΕΠΙΣΤΗΜΩΝ ΤΜΗΜΑ ΜΑΘΗΜΑΤΙΚΩΝ ΠΡΟΓΡΑΜΜΑ ΜΕΤΑΠΤΥΧΙΑΚΩΝ ΣΠΟΥΔΩΝ ΤΟΜΕΑΣ ΣΤΑΤΙΣΤΙΚΗΣ ΚΑΙ ΕΠΙΧΕΙΡΗΣΙΑΚΗΣ ΕΡΕΥΝΑΣ ΑΝΑΛΥΣΗ ΤΩΝ ΣΥΣΧΕΤΙΣΕΩΝ ΧΡΕΟΚΟΠΙΑΣ ΚΑΙ ΤΩΝ
Διαβάστε περισσότεραAreas and Lengths in Polar Coordinates
Kiryl Tsishchanka Areas and Lengths in Polar Coordinates In this section we develop the formula for the area of a region whose boundary is given by a polar equation. We need to use the formula for the
Διαβάστε περισσότεραLecture 34 Bootstrap confidence intervals
Lecture 34 Bootstrap confidence intervals Confidence Intervals θ: an unknown parameter of interest We want to find limits θ and θ such that Gt = P nˆθ θ t If G 1 1 α is known, then P θ θ = P θ θ = 1 α
Διαβάστε περισσότεραExercises to Statistics of Material Fatigue No. 5
Prof. Dr. Christine Müller Dipl.-Math. Christoph Kustosz Eercises to Statistics of Material Fatigue No. 5 E. 9 (5 a Show, that a Fisher information matri for a two dimensional parameter θ (θ,θ 2 R 2, can
Διαβάστε περισσότεραPart III - Pricing A Down-And-Out Call Option
Part III - Pricing A Down-And-Out Call Option Gary Schurman MBE, CFA March 202 In Part I we examined the reflection principle and a scaled random walk in discrete time and then extended the reflection
Διαβάστε περισσότεραEE512: Error Control Coding
EE512: Error Control Coding Solution for Assignment on Finite Fields February 16, 2007 1. (a) Addition and Multiplication tables for GF (5) and GF (7) are shown in Tables 1 and 2. + 0 1 2 3 4 0 0 1 2 3
Διαβάστε περισσότεραSOLUTIONS TO MATH38181 EXTREME VALUES AND FINANCIAL RISK EXAM
SOLUTIONS TO MATH38181 EXTREME VALUES AND FINANCIAL RISK EXAM Solutions to Question 1 a) The cumulative distribution function of T conditional on N n is Pr T t N n) Pr max X 1,..., X N ) t N n) Pr max
Διαβάστε περισσότεραExample Sheet 3 Solutions
Example Sheet 3 Solutions. i Regular Sturm-Liouville. ii Singular Sturm-Liouville mixed boundary conditions. iii Not Sturm-Liouville ODE is not in Sturm-Liouville form. iv Regular Sturm-Liouville note
Διαβάστε περισσότεραSection 8.3 Trigonometric Equations
99 Section 8. Trigonometric Equations Objective 1: Solve Equations Involving One Trigonometric Function. In this section and the next, we will exple how to solving equations involving trigonometric functions.
Διαβάστε περισσότεραFigure A.2: MPC and MPCP Age Profiles (estimating ρ, ρ = 2, φ = 0.03)..
Supplemental Material (not for publication) Persistent vs. Permanent Income Shocks in the Buffer-Stock Model Jeppe Druedahl Thomas H. Jørgensen May, A Additional Figures and Tables Figure A.: Wealth and
Διαβάστε περισσότεραMean-Variance Analysis
Mean-Variance Analysis Jan Schneider McCombs School of Business University of Texas at Austin Jan Schneider Mean-Variance Analysis Beta Representation of the Risk Premium risk premium E t [Rt t+τ ] R1
Διαβάστε περισσότεραChapter 6: Systems of Linear Differential. be continuous functions on the interval
Chapter 6: Systems of Linear Differential Equations Let a (t), a 2 (t),..., a nn (t), b (t), b 2 (t),..., b n (t) be continuous functions on the interval I. The system of n first-order differential equations
Διαβάστε περισσότεραCongruence Classes of Invertible Matrices of Order 3 over F 2
International Journal of Algebra, Vol. 8, 24, no. 5, 239-246 HIKARI Ltd, www.m-hikari.com http://dx.doi.org/.2988/ija.24.422 Congruence Classes of Invertible Matrices of Order 3 over F 2 Ligong An and
Διαβάστε περισσότεραΜηχανική Μάθηση Hypothesis Testing
ΕΛΛΗΝΙΚΗ ΔΗΜΟΚΡΑΤΙΑ ΠΑΝΕΠΙΣΤΗΜΙΟ ΚΡΗΤΗΣ Μηχανική Μάθηση Hypothesis Testing Γιώργος Μπορμπουδάκης Τμήμα Επιστήμης Υπολογιστών Procedure 1. Form the null (H 0 ) and alternative (H 1 ) hypothesis 2. Consider
Διαβάστε περισσότερα5.4 The Poisson Distribution.
The worst thing you can do about a situation is nothing. Sr. O Shea Jackson 5.4 The Poisson Distribution. Description of the Poisson Distribution Discrete probability distribution. The random variable
Διαβάστε περισσότεραSecond Order Partial Differential Equations
Chapter 7 Second Order Partial Differential Equations 7.1 Introduction A second order linear PDE in two independent variables (x, y Ω can be written as A(x, y u x + B(x, y u xy + C(x, y u u u + D(x, y
Διαβάστε περισσότεραExercises 10. Find a fundamental matrix of the given system of equations. Also find the fundamental matrix Φ(t) satisfying Φ(0) = I. 1.
Exercises 0 More exercises are available in Elementary Differential Equations. If you have a problem to solve any of them, feel free to come to office hour. Problem Find a fundamental matrix of the given
Διαβάστε περισσότεραHomework 8 Model Solution Section
MATH 004 Homework Solution Homework 8 Model Solution Section 14.5 14.6. 14.5. Use the Chain Rule to find dz where z cosx + 4y), x 5t 4, y 1 t. dz dx + dy y sinx + 4y)0t + 4) sinx + 4y) 1t ) 0t + 4t ) sinx
Διαβάστε περισσότεραLecture 2: Dirac notation and a review of linear algebra Read Sakurai chapter 1, Baym chatper 3
Lecture 2: Dirac notation and a review of linear algebra Read Sakurai chapter 1, Baym chatper 3 1 State vector space and the dual space Space of wavefunctions The space of wavefunctions is the set of all
Διαβάστε περισσότεραSOLUTIONS TO MATH38181 EXTREME VALUES AND FINANCIAL RISK EXAM
SOLUTIONS TO MATH38181 EXTREME VALUES AND FINANCIAL RISK EXAM Solutions to Question 1 a) The cumulative distribution function of T conditional on N n is Pr (T t N n) Pr (max (X 1,..., X N ) t N n) Pr (max
Διαβάστε περισσότεραb. Use the parametrization from (a) to compute the area of S a as S a ds. Be sure to substitute for ds!
MTH U341 urface Integrals, tokes theorem, the divergence theorem To be turned in Wed., Dec. 1. 1. Let be the sphere of radius a, x 2 + y 2 + z 2 a 2. a. Use spherical coordinates (with ρ a) to parametrize.
Διαβάστε περισσότερα: Ω F F 0 t T P F 0 t T F 0 P Q. Merton 1974 XT T X T XT. T t. V t t X d T = XT [V t/t ]. τ 0 < τ < X d T = XT I {V τ T } δt XT I {V τ<t } I A
2012 4 Chinese Journal of Applied Probability and Statistics Vol.28 No.2 Apr. 2012 730000. :. : O211.9. 1..... Johnson Stulz [3] 1987. Merton 1974 Johnson Stulz 1987. Hull White 1995 Klein 1996 2008 Klein
Διαβάστε περισσότεραD Alembert s Solution to the Wave Equation
D Alembert s Solution to the Wave Equation MATH 467 Partial Differential Equations J. Robert Buchanan Department of Mathematics Fall 2018 Objectives In this lesson we will learn: a change of variable technique
Διαβάστε περισσότεραEcon 2110: Fall 2008 Suggested Solutions to Problem Set 8 questions or comments to Dan Fetter 1
Eon : Fall 8 Suggested Solutions to Problem Set 8 Email questions or omments to Dan Fetter Problem. Let X be a salar with density f(x, θ) (θx + θ) [ x ] with θ. (a) Find the most powerful level α test
Διαβάστε περισσότεραA Note on Intuitionistic Fuzzy. Equivalence Relation
International Mathematical Forum, 5, 2010, no. 67, 3301-3307 A Note on Intuitionistic Fuzzy Equivalence Relation D. K. Basnet Dept. of Mathematics, Assam University Silchar-788011, Assam, India dkbasnet@rediffmail.com
Διαβάστε περισσότεραEstimation for ARMA Processes with Stable Noise. Matt Calder & Richard A. Davis Colorado State University
Estimation for ARMA Processes with Stable Noise Matt Calder & Richard A. Davis Colorado State University rdavis@stat.colostate.edu 1 ARMA processes with stable noise Review of M-estimation Examples of
Διαβάστε περισσότεραStatistics 104: Quantitative Methods for Economics Formula and Theorem Review
Harvard College Statistics 104: Quantitative Methods for Economics Formula and Theorem Review Tommy MacWilliam, 13 tmacwilliam@college.harvard.edu March 10, 2011 Contents 1 Introduction to Data 5 1.1 Sample
Διαβάστε περισσότεραw o = R 1 p. (1) R = p =. = 1
Πανεπιστήµιο Κρήτης - Τµήµα Επιστήµης Υπολογιστών ΗΥ-570: Στατιστική Επεξεργασία Σήµατος 205 ιδάσκων : Α. Μουχτάρης Τριτη Σειρά Ασκήσεων Λύσεις Ασκηση 3. 5.2 (a) From the Wiener-Hopf equation we have:
Διαβάστε περισσότεραIMES DISCUSSION PAPER SERIES
IMES DISCUSSION PAPER SERIES Will a Growth Miracle Reduce Debt in Japan? Selahattin mrohorolu and Nao Sudo Discussion Paper No. 2011-E-1 INSTITUTE FOR MONETARY AND ECONOMIC STUDIES BANK OF JAPAN 2-1-1
Διαβάστε περισσότεραLecture 2. Soundness and completeness of propositional logic
Lecture 2 Soundness and completeness of propositional logic February 9, 2004 1 Overview Review of natural deduction. Soundness and completeness. Semantics of propositional formulas. Soundness proof. Completeness
Διαβάστε περισσότεραAppendix S1 1. ( z) α βc. dβ β δ β
Appendix S1 1 Proof of Lemma 1. Taking first and second partial derivatives of the expected profit function, as expressed in Eq. (7), with respect to l: Π Π ( z, λ, l) l θ + s ( s + h ) g ( t) dt λ Ω(
Διαβάστε περισσότεραA Bonus-Malus System as a Markov Set-Chain. Małgorzata Niemiec Warsaw School of Economics Institute of Econometrics
A Bonus-Malus System as a Markov Set-Chain Małgorzata Niemiec Warsaw School of Economics Institute of Econometrics Contents 1. Markov set-chain 2. Model of bonus-malus system 3. Example 4. Conclusions
Διαβάστε περισσότεραENGR 691/692 Section 66 (Fall 06): Machine Learning Assigned: August 30 Homework 1: Bayesian Decision Theory (solutions) Due: September 13
ENGR 69/69 Section 66 (Fall 06): Machine Learning Assigned: August 30 Homework : Bayesian Decision Theory (solutions) Due: Septemer 3 Prolem : ( pts) Let the conditional densities for a two-category one-dimensional
Διαβάστε περισσότερα6.1. Dirac Equation. Hamiltonian. Dirac Eq.
6.1. Dirac Equation Ref: M.Kaku, Quantum Field Theory, Oxford Univ Press (1993) η μν = η μν = diag(1, -1, -1, -1) p 0 = p 0 p = p i = -p i p μ p μ = p 0 p 0 + p i p i = E c 2 - p 2 = (m c) 2 H = c p 2
Διαβάστε περισσότερα: Monte Carlo EM 313, Louis (1982) EM, EM Newton-Raphson, /. EM, 2 Monte Carlo EM Newton-Raphson, Monte Carlo EM, Monte Carlo EM, /. 3, Monte Carlo EM
2008 6 Chinese Journal of Applied Probability and Statistics Vol.24 No.3 Jun. 2008 Monte Carlo EM 1,2 ( 1,, 200241; 2,, 310018) EM, E,,. Monte Carlo EM, EM E Monte Carlo,. EM, Monte Carlo EM,,,,. Newton-Raphson.
Διαβάστε περισσότεραHigher Derivative Gravity Theories
Higher Derivative Gravity Theories Black Holes in AdS space-times James Mashiyane Supervisor: Prof Kevin Goldstein University of the Witwatersrand Second Mandelstam, 20 January 2018 James Mashiyane WITS)
Διαβάστε περισσότεραCRASH COURSE IN PRECALCULUS
CRASH COURSE IN PRECALCULUS Shiah-Sen Wang The graphs are prepared by Chien-Lun Lai Based on : Precalculus: Mathematics for Calculus by J. Stuwart, L. Redin & S. Watson, 6th edition, 01, Brooks/Cole Chapter
Διαβάστε περισσότεραAquinas College. Edexcel Mathematical formulae and statistics tables DO NOT WRITE ON THIS BOOKLET
Aquinas College Edexcel Mathematical formulae and statistics tables DO NOT WRITE ON THIS BOOKLET Pearson Edexcel Level 3 Advanced Subsidiary and Advanced GCE in Mathematics and Further Mathematics Mathematical
Διαβάστε περισσότεραMatrices and Determinants
Matrices and Determinants SUBJECTIVE PROBLEMS: Q 1. For what value of k do the following system of equations possess a non-trivial (i.e., not all zero) solution over the set of rationals Q? x + ky + 3z
Διαβάστε περισσότεραAppendix to On the stability of a compressible axisymmetric rotating flow in a pipe. By Z. Rusak & J. H. Lee
Appendi to On the stability of a compressible aisymmetric rotating flow in a pipe By Z. Rusak & J. H. Lee Journal of Fluid Mechanics, vol. 5 4, pp. 5 4 This material has not been copy-edited or typeset
Διαβάστε περισσότεραSCITECH Volume 13, Issue 2 RESEARCH ORGANISATION Published online: March 29, 2018
Journal of rogressive Research in Mathematics(JRM) ISSN: 2395-028 SCITECH Volume 3, Issue 2 RESEARCH ORGANISATION ublished online: March 29, 208 Journal of rogressive Research in Mathematics www.scitecresearch.com/journals
Διαβάστε περισσότεραMath 6 SL Probability Distributions Practice Test Mark Scheme
Math 6 SL Probability Distributions Practice Test Mark Scheme. (a) Note: Award A for vertical line to right of mean, A for shading to right of their vertical line. AA N (b) evidence of recognizing symmetry
Διαβάστε περισσότεραChapter 6: Systems of Linear Differential. be continuous functions on the interval
Chapter 6: Systems of Linear Differential Equations Let a (t), a 2 (t),..., a nn (t), b (t), b 2 (t),..., b n (t) be continuous functions on the interval I. The system of n first-order differential equations
Διαβάστε περισσότεραJesse Maassen and Mark Lundstrom Purdue University November 25, 2013
Notes on Average Scattering imes and Hall Factors Jesse Maassen and Mar Lundstrom Purdue University November 5, 13 I. Introduction 1 II. Solution of the BE 1 III. Exercises: Woring out average scattering
Διαβάστε περισσότεραBayesian statistics. DS GA 1002 Probability and Statistics for Data Science.
Bayesian statistics DS GA 1002 Probability and Statistics for Data Science http://www.cims.nyu.edu/~cfgranda/pages/dsga1002_fall17 Carlos Fernandez-Granda Frequentist vs Bayesian statistics In frequentist
Διαβάστε περισσότεραProblem Set 9 Solutions. θ + 1. θ 2 + cotθ ( ) sinθ e iφ is an eigenfunction of the ˆ L 2 operator. / θ 2. φ 2. sin 2 θ φ 2. ( ) = e iφ. = e iφ cosθ.
Chemistry 362 Dr Jean M Standard Problem Set 9 Solutions The ˆ L 2 operator is defined as Verify that the angular wavefunction Y θ,φ) Also verify that the eigenvalue is given by 2! 2 & L ˆ 2! 2 2 θ 2 +
Διαβάστε περισσότερα22 .5 Real consumption.5 Real residential investment.5.5.5 965 975 985 995 25.5 965 975 985 995 25.5 Real house prices.5 Real fixed investment.5.5.5 965 975 985 995 25.5 965 975 985 995 25.3 Inflation
Διαβάστε περισσότεραLecture 12: Pseudo likelihood approach
Lecture 12: Pseudo likelihood approach Pseudo MLE Let X 1,...,X n be a random sample from a pdf in a family indexed by two parameters θ and π with likelihood l(θ,π). The method of pseudo MLE may be viewed
Διαβάστε περισσότεραSecond Order RLC Filters
ECEN 60 Circuits/Electronics Spring 007-0-07 P. Mathys Second Order RLC Filters RLC Lowpass Filter A passive RLC lowpass filter (LPF) circuit is shown in the following schematic. R L C v O (t) Using phasor
Διαβάστε περισσότεραDurbin-Levinson recursive method
Durbin-Levinson recursive method A recursive method for computing ϕ n is useful because it avoids inverting large matrices; when new data are acquired, one can update predictions, instead of starting again
Διαβάστε περισσότεραForced Pendulum Numerical approach
Numerical approach UiO April 8, 2014 Physical problem and equation We have a pendulum of length l, with mass m. The pendulum is subject to gravitation as well as both a forcing and linear resistance force.
Διαβάστε περισσότεραParametrized Surfaces
Parametrized Surfaces Recall from our unit on vector-valued functions at the beginning of the semester that an R 3 -valued function c(t) in one parameter is a mapping of the form c : I R 3 where I is some
Διαβάστε περισσότερα2. Let H 1 and H 2 be Hilbert spaces and let T : H 1 H 2 be a bounded linear operator. Prove that [T (H 1 )] = N (T ). (6p)
Uppsala Universitet Matematiska Institutionen Andreas Strömbergsson Prov i matematik Funktionalanalys Kurs: F3B, F4Sy, NVP 2005-03-08 Skrivtid: 9 14 Tillåtna hjälpmedel: Manuella skrivdon, Kreyszigs bok
Διαβάστε περισσότεραΣΥΓΧΡΟΝΕΣ ΤΑΣΕΙΣ ΣΤΗΝ ΕΚΤΙΜΗΣΗ ΚΑΙ ΧΑΡΤΟΓΡΑΦΗΣΗ ΤΩΝ ΚΙΝΔΥΝΩΝ
ΕΘΝΙΚΗ ΣΧΟΛΗ ΤΟΠΙΚΗΣ ΑΥΤΟΔΙΟΙΚΗΣΗΣ Δ ΕΚΠΑΙΔΕΥΤΙΚΗ ΣΕΙΡΑ ΤΜΗΜΑ ΠΟΛΙΤΙΚΗΣ ΠΡΟΣΤΑΣΙΑΣ ΣΥΓΧΡΟΝΕΣ ΤΑΣΕΙΣ ΣΤΗΝ ΕΚΤΙΜΗΣΗ ΚΑΙ ΧΑΡΤΟΓΡΑΦΗΣΗ ΤΩΝ ΚΙΝΔΥΝΩΝ Σπουδάστρια: Διαούρτη Ειρήνη Δήμητρα Επιβλέπων καθηγητής:
Διαβάστε περισσότερα= λ 1 1 e. = λ 1 =12. has the properties e 1. e 3,V(Y
Stat 50 Homework Solutions Spring 005. (a λ λ λ 44 (b trace( λ + λ + λ 0 (c V (e x e e λ e e λ e (λ e by definition, the eigenvector e has the properties e λ e and e e. (d λ e e + λ e e + λ e e 8 6 4 4
Διαβάστε περισσότεραCoefficient Inequalities for a New Subclass of K-uniformly Convex Functions
International Journal of Computational Science and Mathematics. ISSN 0974-89 Volume, Number (00), pp. 67--75 International Research Publication House http://www.irphouse.com Coefficient Inequalities for
Διαβάστε περισσότεραInverse trigonometric functions & General Solution of Trigonometric Equations. ------------------ ----------------------------- -----------------
Inverse trigonometric functions & General Solution of Trigonometric Equations. 1. Sin ( ) = a) b) c) d) Ans b. Solution : Method 1. Ans a: 17 > 1 a) is rejected. w.k.t Sin ( sin ) = d is rejected. If sin
Διαβάστε περισσότεραSection 7.6 Double and Half Angle Formulas
09 Section 7. Double and Half Angle Fmulas To derive the double-angles fmulas, we will use the sum of two angles fmulas that we developed in the last section. We will let α θ and β θ: cos(θ) cos(θ + θ)
Διαβάστε περισσότερα«Χρήσεις γης, αξίες γης και κυκλοφοριακές ρυθμίσεις στο Δήμο Χαλκιδέων. Η μεταξύ τους σχέση και εξέλιξη.»
ΕΘΝΙΚΟ ΜΕΤΣΟΒΙΟ ΠΟΛΥΤΕΧΝΕΙΟ ΣΧΟΛΗ ΑΓΡΟΝΟΜΩΝ ΚΑΙ ΤΟΠΟΓΡΑΦΩΝ ΜΗΧΑΝΙΚΩΝ ΤΟΜΕΑΣ ΓΕΩΓΡΑΦΙΑΣ ΚΑΙ ΠΕΡΙΦΕΡΕΙΑΚΟΥ ΣΧΕΔΙΑΣΜΟΥ ΔΙΠΛΩΜΑΤΙΚΗ ΕΡΓΑΣΙΑ: «Χρήσεις γης, αξίες γης και κυκλοφοριακές ρυθμίσεις στο Δήμο Χαλκιδέων.
Διαβάστε περισσότεραAppendix to Technology Transfer and Spillovers in International Joint Ventures
Appendix to Technology Transfer and Spillovers in International Joint Ventures Thomas Müller Monika Schnitzer Published in Journal of International Economics, 2006, Volume 68, 456-468 Bundestanstalt für
Διαβάστε περισσότεραMath 446 Homework 3 Solutions. (1). (i): Reverse triangle inequality for metrics: Let (X, d) be a metric space and let x, y, z X.
Math 446 Homework 3 Solutions. (1). (i): Reverse triangle inequalit for metrics: Let (X, d) be a metric space and let x,, z X. Prove that d(x, z) d(, z) d(x, ). (ii): Reverse triangle inequalit for norms:
Διαβάστε περισσότεραNew bounds for spherical two-distance sets and equiangular lines
New bounds for spherical two-distance sets and equiangular lines Michigan State University Oct 8-31, 016 Anhui University Definition If X = {x 1, x,, x N } S n 1 (unit sphere in R n ) and x i, x j = a
Διαβάστε περισσότεραThe challenges of non-stable predicates
The challenges of non-stable predicates Consider a non-stable predicate Φ encoding, say, a safety property. We want to determine whether Φ holds for our program. The challenges of non-stable predicates
Διαβάστε περισσότεραTridiagonal matrices. Gérard MEURANT. October, 2008
Tridiagonal matrices Gérard MEURANT October, 2008 1 Similarity 2 Cholesy factorizations 3 Eigenvalues 4 Inverse Similarity Let α 1 ω 1 β 1 α 2 ω 2 T =......... β 2 α 1 ω 1 β 1 α and β i ω i, i = 1,...,
Διαβάστε περισσότεραLecture 21: Properties and robustness of LSE
Lecture 21: Properties and robustness of LSE BLUE: Robustness of LSE against normality We now study properties of l τ β and σ 2 under assumption A2, i.e., without the normality assumption on ε. From Theorem
Διαβάστε περισσότεραNotes on the Open Economy
Notes on the Open Econom Ben J. Heijdra Universit of Groningen April 24 Introduction In this note we stud the two-countr model of Table.4 in more detail. restated here for convenience. The model is Table.4.
Διαβάστε περισσότεραNowhere-zero flows Let be a digraph, Abelian group. A Γ-circulation in is a mapping : such that, where, and : tail in X, head in
Nowhere-zero flows Let be a digraph, Abelian group. A Γ-circulation in is a mapping : such that, where, and : tail in X, head in : tail in X, head in A nowhere-zero Γ-flow is a Γ-circulation such that
Διαβάστε περισσότεραECE598: Information-theoretic methods in high-dimensional statistics Spring 2016
ECE598: Information-theoretic methods in high-dimensional statistics Spring 06 Lecture 7: Information bound Lecturer: Yihong Wu Scribe: Shiyu Liang, Feb 6, 06 [Ed. Mar 9] Recall the Chi-squared divergence
Διαβάστε περισσότεραSolutions to Exercise Sheet 5
Solutions to Eercise Sheet 5 jacques@ucsd.edu. Let X and Y be random variables with joint pdf f(, y) = 3y( + y) where and y. Determine each of the following probabilities. Solutions. a. P (X ). b. P (X
Διαβάστε περισσότεραΕΙΣΑΓΩΓΗ ΣΤΗ ΣΤΑΤΙΣΤΙΚΗ ΑΝΑΛΥΣΗ
ΕΙΣΑΓΩΓΗ ΣΤΗ ΣΤΑΤΙΣΤΙΚΗ ΑΝΑΛΥΣΗ ΕΛΕΝΑ ΦΛΟΚΑ Επίκουρος Καθηγήτρια Τµήµα Φυσικής, Τοµέας Φυσικής Περιβάλλοντος- Μετεωρολογίας ΓΕΝΙΚΟΙ ΟΡΙΣΜΟΙ Πληθυσµός Σύνολο ατόµων ή αντικειµένων στα οποία αναφέρονται
Διαβάστε περισσότερα10.7 Performance of Second-Order System (Unit Step Response)
Lecture Notes on Control Systems/D. Ghose/0 57 0.7 Performance of Second-Order System (Unit Step Response) Consider the second order system a ÿ + a ẏ + a 0 y = b 0 r So, Y (s) R(s) = b 0 a s + a s + a
Διαβάστε περισσότερα