Online Appendix To: Bayesian Doubly Adaptive Elastic-Net Lasso For VAR Shrinkage
|
|
- Άμωσις Λαμπρόπουλος
- 7 χρόνια πριν
- Προβολές:
Transcript
1 Online Appendix To: Bayesian Doubly Adaptive Elastic-Net Lasso For VAR Shrinkage Deborah Gefang Department of Economics University of Lancaster April 7, 203 I would like to thank Gary Koop, Esther Ruiz and two anonymous referees for their constructive comments. I would also like to thank the conference participants of CFE, ESEM202, and RCEF202 for helpful discussions. Any remaining errors are my own responsibility.
2 Technical Details for Models Nested in DAE- Lasso This section presents the priors, posteriors, and full conditional Gibbs schemes for Lasso, adaptive Lasso, e-net Lasso, and adaptive e-net Lasso.. Lasso VAR Shrinkage Following Song and Bickel (20), we define Lasso estimator for a VAR as: N 2 k ˆβ L = arg min β {[y (I n X)β] [y (I n X)β] + λ β j } () Correspondingly, the conditional multivariate mixture prior for β takes the following form: j= N 2 k π(β Σ, Γ, λ ) j= { 0 2πfj (Γ)) exp[ 2f j (Γ) β2 j ]d(f j (Γ))} { M 2 exp( 2 Γ M Γ)} 2 (2) where Γ = [γ, γ 2,..., γ N 2 k], M = Σ I Nk, and f j (Γ) is a function of Γ and Λ to be defined later. In this mixture prior, the terms associated with the L penalty are conditional on Σ through f j (Γ). In equation (2), the variances of β a and β b for a b are related through M. However, β a and β b themselves are independent of each other. We need to find an appropriate f j (Γ) which provides us tractable posteriors. The last term in equation (2) takes the form of a multivariate Normal distribution Γ N(0, M). For ease of exposition, we first write the 2
3 N 2 k N 2 k covariance matrix M as following: M = M,... M,j M,j+... M,N 2 k M j,... M j,j M j,j+... M j,n 2 k M j+,... M j+,j M j+,j+... M j+,n 2 k (3) M N 2 k,... M N 2 k,j M N 2 k,j+... M N 2 k,n 2 k M j+,j+... M j+,n 2 k Let H j = (M j,j+,..., M j,n 2 k) M N 2 k,j+... M N 2 k,n 2 k We next construct independent variables τ j for j =, 2,..., N 2 k using standard textbook techniques (e.g. Anderson, 2003; Muirhead 982). τ = γ + H (γ 2, γ 3,..., γ N 2 k) (4) τ 2 = γ 2 + H 2 (γ 3, γ 4,..., γ N 2 k) (5)... τ N 2 K = γ N 2 k + H N 2 k γ N 2 k (6) τ N 2 K = γ N 2 k (7) 3
4 The joint density of τ, τ 2,..., τ N 2 k is N(τ 0, σ 2 γ )N(τ 2 0, σ 2 γ 2 )...N(τ N 2 k 0, σ 2 γ N 2 k ) (8) where σ 2 γ j = M j,j H j (M j,j+,..., M j,n 2 k), with σ 2 γ N 2 k = M N 2 k,n 2 k. Note that it is computationally feasible to derive σ 2 γ j when M is sparse. The Jacobian of transforming Γ N(0, M) to (8) is. Defining η j = τ j /λ, we can write (8) as N(η 0, σ 2 γ )N(η 2 0, σ 2 γ 2 )...N(η N 2 k 0, σ 2 γ N 2 k ) (9) Let f j (Γ) = 2(ηj 2 ), the scale mixture prior is: N 2 k π(β Σ, Γ, λ ) { exp[ β2 j 0 2π(2ηj 2)) 2(2ηj 2)]d(2η2 j ) j= λ2 2σγ 2 exp[ j 2 (σγ 2 j )/λ 2 ]} (0) The last two terms in (0) constitute a scale mixture of Normals (with an exponential mixing density), which can be expressed as the univariate Laplace distribution λ 2 exp( λ β σγ 2 j σ 2 j ). γj Equation (0) shows that the conditional prior for β j is N(0, ), and 2ηj 2 the conditional prior for β is β Γ, Σ, Λ, Λ 2 N(0, D Γ) () where DΓ = diag([,,..., ]). 2η 2 2η2 2 2η 2 N 2 k 4
5 Priors for Σ and λ 2 can be elicited following standard practice in VAR and Lasso literature. In this paper, we set Wishart prior for Σ and Gamma prior for λ 2 : Σ W (S, ν), λ 2 G(µ λ 2, ν λ 2 ). The full conditional posterior for β is β N(β, V β ), where V β = [(I N X) )(Σ I Nk )(I N X)+(D Γ ) ], and β = V β [(I N X) (Σ I Nk )y]. The Full conditional posterior for Σ is W (S, ν), with S = (Y XB) (Y XB) + 2Q Q + S and ν = T + 2Nk + ν, with vec(q) = Γ. The Full conditional posterior for λ 2 is G( µ λ, ν λ ), where ν λ = ν λ + 2N 2 k ν λ µ λ and µ λ = ν λ +2µ λ τ 2 Finally the full conditional posterior of is j /σγ 2 j 2ηj 2 λ Inverse Gaussian: IG( 2, λ2 βj 2 ). Γ can not be directly drawn from the σ2 γ σ 2 j γ j posteriors. But it can be recovered in each Gibbs iteration using the draws of and Σ. Conditional on arbitrary starting values, the Gibbs sampler contains the following six steps:. draw β Σ, Λ, Γ from N(β, V β ); 2. draw Σ β, Λ, Γ from W (S, ν) 3. draw λ 2 Σ, β, Γ from G( µ λ, ν λ ) 4. draw λ β, Σ, Λ 2ηj 2 from IG( 2, λ2 βj 2 ) for j =, 2,...N 2 k. σ2 γ σ 2 j γ j 5. calculate Γ based on draws of Σ and in the current iteration. We adopt the same form of the inverse-gaussian density used in Park and Casella (2008). 5
6 .2 Adaptive Lasso VAR Shrinkage We define the adaptive Lasso estimator for a VAR as: N 2 k ˆβ AL = arg min β {[y (I n X)β] [y (I n X)β] + λ,j β j } (2) Correspondingly, the conditional multivariate mixture prior for β takes the following form: j= N 2 k π(β Σ, Γ, Λ ) j= { 0 2πfj (Γ)) exp[ 2f j (Γ) β2 j ]d(f j (Γ))} { M 2 exp( 2 Γ M Γ)} 2 (3) where Γ = [γ, γ 2,..., γ N 2 k], M = Σ I Nk, and f j (Γ) is a function of Γ and Λ to be defined later. In this mixture prior, the terms associated with the L penalty are conditional on Σ through f j (Γ). In equation (3), the variances of β a and β b for a b are related through M. However, β a and β b themselves are independent of each other. We need to find an appropriate f j (Γ) which provides us tractable posteriors. The last term in equation (3) takes the form of a multivariate Normal distribution Γ N(0, M). For ease of exposition, we first write the N 2 k N 2 k covariance matrix M as following: 6
7 M = M,... M,j M,j+... M,N 2 k M j,... M j,j M j,j+... M j,n 2 k M j+,... M j+,j M j+,j+... M j+,n 2 k (4) M N 2 k,... M N 2 k,j M N 2 k,j+... M N 2 k,n 2 k M j+,j+... M j+,n 2 k Let H j = (M j,j+,..., M j,n 2 k) M N 2 k,j+... M N 2 k,n 2 k We next construct independent variables τ j for j =, 2,..., N 2 k using standard textbook techniques (e.g. Anderson, 2003; Muirhead 982). τ = γ + H (γ 2, γ 3,..., γ N 2 k) (5) τ 2 = γ 2 + H 2 (γ 3, γ 4,..., γ N 2 k) (6)... τ N 2 K = γ N 2 k + H N 2 k γ N 2 k (7) τ N 2 K = γ N 2 k (8) The joint density of τ, τ 2,..., τ N 2 k is N(τ 0, σ 2 γ )N(τ 2 0, σ 2 γ 2 )...N(τ N 2 k 0, σ 2 γ N 2 k ) (9) 7
8 where σ 2 γ j = M j,j H j (M j,j+,..., M j,n 2 k), with σ 2 γ N 2 k = M N 2 k,n 2 k. Note that it is computationally feasible to derive σ 2 γ j when M is sparse. The Jacobian of transforming Γ N(0, M) to (9) is. Defining η j = τ j /λ,j, we can write (9) as N(η 0, σ 2 γ, )N(η 2 0, σ 2 γ 2,2 )...N(η N 2 k 0, σ 2 γ N 2 k,n 2 k ) (20) Let f j (Γ) = 2(ηj 2 ), the scale mixture prior is: N 2 k π(β Σ, Γ, Λ ) { exp[ β2 j 0 2π(2ηj 2)) 2(2ηj 2)]d(2η2 j ) j= λ2,j 2σγ 2 exp[ j 2 (σγ 2 j )/λ 2 ]},j (2) Equation (2) shows that the conditional prior for β j is N(0, ), and 2ηj 2 the conditional prior for β is β Γ, Σ, Λ, Λ 2 N(0, D Γ) (22) where DΓ = diag([,,..., ]). 2η 2 2η2 2 2η 2 N 2 k Priors for Σ and λ 2,j can be elicited following standard practice in VAR and Lasso literature. In this paper, we set Wishart prior for Σ and Gamma prior for λ 2,j : Σ W (S, ν), λ 2,j G(µ λ 2,j, ν λ 2,j ). The full conditional posterior for β is β N(β, V β ), where V β = [(I N X) )(Σ I Nk )(I N X)+(D Γ ) ], and β = V β [(I N X) (Σ I Nk )y]. The Full conditional posterior for Σ is W (S, ν), with S = (Y XB) (Y XB) + 2Q Q + S and ν = T + 2Nk + ν, with vec(q) = Γ. The 8
9 Full conditional posterior for λ 2,j is G( µ λ,j, ν λ,j ), where ν λ,j = ν λ,j + 2 and µ λ,j = ν λ,j σj 2µ λ,j 2τj 2µ. Finally the full conditional posterior of is +ν λ λ,j σγ 2,j j 2ηj 2 λ Inverse Gaussian: IG( 2,j, λ2,j ). Γ can not be directly drawn from the βj 2σ2 γ σ 2 j γ j posteriors. But it can be recovered in each Gibbs iteration using the draws of and Σ. Conditional on arbitrary starting values, the Gibbs sampler contains the following six steps:. draw β Σ, Λ, Γ from N(β, V β ); 2. draw Σ β, Λ, Γ from W (S, ν) 3. draw λ 2,j β, Σ, Λ, j, Γ from G( µ λ,j, ν λ,j ) for j =, 2,...N 2 k 4. draw λ β, Σ, Λ 2ηj 2 from IG( 2,j, λ2,j ) for j =, 2,...N 2 k. βj 2σ2 γ σ 2 j γ j 5. calculate Γ based on draws of Σ and in the current iteration..3 E-net Lasso VAR Shrinkage We define the e-net Lasso estimator for a VAR as: N 2 k N 2 k ˆβ EL = arg min β {[y (I n X)β] [y (I n X)β] + λ β j + λ 2 βj 2 } j= j= (23) Correspondingly, the conditional multivariate mixture prior for β takes 9
10 the following form: N 2 k λ2 π(β Σ, Γ, λ, λ 2 ) { exp( λ 2 2π j= 0 2 β2 j ) 2πfj (Γ)) exp[ 2f j (Γ) β2 j ]d(f j (Γ))} { M 2 exp( 2 Γ M Γ)} 2 (24) where Γ = [γ, γ 2,..., γ N 2 k], M = Σ I Nk, and f j (Γ) is a function of Γ and Λ to be defined later. In this mixture prior, the terms associated with the L penalty are conditional on Σ through f j (Γ). In equation (24), the variances of β a and β b for a b are related through M. However, β a and β b themselves are independent of each other. We need to find an appropriate f j (Γ) which provides us tractable posteriors. The last term in equation (24) takes the form of a multivariate Normal distribution Γ N(0, M). For ease of exposition, we first write the N 2 k N 2 k covariance matrix M as following: M = M,... M,j M,j+... M,N 2 k M j,... M j,j M j,j+... M j,n 2 k M j+,... M j+,j M j+,j+... M j+,n 2 k (25) M N 2 k,... M N 2 k,j M N 2 k,j+... M N 2 k,n 2 k 0
11 M j+,j+... M j+,n 2 k Let H j = (M j,j+,..., M j,n 2 k) M N 2 k,j+... M N 2 k,n 2 k We next construct independent variables τ j for j =, 2,..., N 2 k using standard textbook techniques (e.g. Anderson, 2003; Muirhead 982). τ = γ + H (γ 2, γ 3,..., γ N 2 k) (26) τ 2 = γ 2 + H 2 (γ 3, γ 4,..., γ N 2 k) (27)... τ N 2 K = γ N 2 k + H N 2 k γ N 2 k (28) τ N 2 K = γ N 2 k (29) The joint density of τ, τ 2,..., τ N 2 k is N(τ 0, σ 2 γ )N(τ 2 0, σ 2 γ 2 )...N(τ N 2 k 0, σ 2 γ N 2 k ) (30) where σ 2 γ j = M j,j H j (M j,j+,..., M j,n 2 k), with σ 2 γ N 2 k = M N 2 k,n 2 k. Note that it is computationally feasible to derive σ 2 γ j when M is sparse. The Jacobian of transforming Γ N(0, M) to (30) is. Defining η j = τ j /λ, we can write (30) as N(η 0, σ 2 γ )N(η 2 0, σ 2 γ 2 )...N(η N 2 k 0, σ 2 γ N 2 k ) (3)
12 Let f j (Γ) = 2(ηj 2 ), the scale mixture prior is: N 2 k π(β Σ, Γ, λ, λ 2 ) j= λ2 { exp( λ 2 2π 2 β2 j ) 0 exp[ β2 j 2π(2ηj 2)) 2(2ηj 2)]d(2η2 j ) (32) 2σγ 2 exp[ j 2 (σγ 2 j )/λ 2 ]} λ2 where η j = τ j /λ. The last two terms in (32) constitute a scale mixture of Normals (with an exponential mixing density), which can be expressed as the univariate Laplace distribution λ 2 σ 2 γ j exp( λ σ 2 γj β j ). Equation (32) shows that the conditional prior for β j is N(0, and the conditional prior for β is 2λ 2 η 2 j +), β Γ, Σ, Λ, Λ 2 N(0, D Γ) (33) where D Γ = diag([ 2η 2 2λ 2 η 2+, 2η2 2 2η 2λ 2 η2 2 +,..., 2 N 2 k 2λ 2 η 2 N 2 k +]). Priors for Σ and λ 2 can be elicited following standard practice in VAR and Lasso literature. In this paper, we set Wishart prior for Σ and Gamma priors for λ 2 and λ 2: Σ W (S, ν), λ 2 G(µ λ 2, ν λ 2 ), λ 2 G(µ λ2, ν λ2 ). The full conditional posterior for β is β N(β, V β ), where V β = [(I N X) )(Σ I Nk )(I N X)+(D Γ ) ], and β = V β [(I N X) (Σ I Nk )y]. The Full conditional posterior for Σ is W (S, ν), with S = (Y XB) (Y XB) + 2Q Q + S and ν = T + 2Nk + ν, with vec(q) = Γ. The 2
13 Full conditional posterior for λ 2 is G( µ λ, ν λ ), where ν λ = ν λ + 2N 2 k and µ λ = ν λ µ λ ν λ +2µ λ τ 2 j /σ 2 γ j. The Full conditional posterior for λ 2 is G( µ λ2, ν λ2 ), µ λ2 ν λ2 where ν λ2 = ν λ2 + N 2 k and µ λ2 = ν λ2 +µ λ2 β 2. Finally the full conditional j λ posterior of is Inverse Gaussian: IG( 2 2ηj 2, λ2 βj 2 ). Γ can not be directly σ2 γ σ 2 j γ j drawn from the posteriors. But it can be recovered in each Gibbs iteration using the draws of and Σ. 2ηj 2 Conditional on arbitrary starting values, the Gibbs sampler contains the following six steps:. draw β Σ, Λ, Λ 2, Γ from N(β, V β ); 2. draw Σ β, Λ, Λ 2, Γ from W (S, ν) 3. draw λ 2 β, Σ, Λ 2, Γ from G( µ λ, ν λ ) 4. draw λ 2 β, Σ, Λ, Γ from G( µ λ2, ν λ2 ) 5. draw λ β, Σ, Λ 2ηj 2, Λ 2 from IG( 2, λ2 βj 2 ) for j =, 2,...N 2 k. σ2 γ σ 2 j γ j 6. calculate Γ based on draws of Σ and in the current iteration..4 Adaptive E-net Lasso VAR Shrinkage In line with Zou and Zhang (2009), we define the adaptive e-net Lasso estimator for a VAR as following: N 2 k N 2 k ˆβ AEL = arg min β {[y (I n X)β] [y (I n X)β] + λ,j β j + λ 2 βj 2 } j= j= (34) 3
14 Correspondingly, the conditional multivariate mixture prior for β takes the following form: N 2 k λ2 π(β Σ, Γ, Λ, λ 2 ) { exp( λ 2 2π j= 0 2 β2 j ) 2πfj (Γ)) exp[ 2f j (Γ) β2 j ]d(f j (Γ))} { M 2 exp( 2 Γ M Γ)} 2 (35) where Γ = [γ, γ 2,..., γ N 2 k], M = Σ I Nk, and f j (Γ) is a function of Γ and Λ to be defined later. In this mixture prior, the terms associated with the L penalty are conditional on Σ through f j (Γ). We need to find an appropriate f j (Γ) which provides us tractable posteriors. The last term in equation (35) takes the form of a multivariate Normal distribution Γ N(0, M). For ease of exposition, we first write the N 2 k N 2 k covariance matrix M as following: M = M,... M,j M,j+... M,N 2 k M j,... M j,j M j,j+... M j,n 2 k M j+,... M j+,j M j+,j+... M j+,n 2 k (36) M N 2 k,... M N 2 k,j M N 2 k,j+... M N 2 k,n 2 k 4
15 M j+,j+... M j+,n 2 k Let H j = (M j,j+,..., M j,n 2 k) M N 2 k,j+... M N 2 k,n 2 k We next construct independent variables τ j for j =, 2,..., N 2 k using standard textbook techniques (e.g. Anderson, 2003; Muirhead 982). τ = γ + H (γ 2, γ 3,..., γ N 2 k) (37) τ 2 = γ 2 + H 2 (γ 3, γ 4,..., γ N 2 k) (38)... τ N 2 K = γ N 2 k + H N 2 k γ N 2 k (39) τ N 2 K = γ N 2 k (40) The joint density of τ, τ 2,..., τ N 2 k is N(τ 0, σ 2 γ )N(τ 2 0, σ 2 γ 2 )...N(τ N 2 k 0, σ 2 γ N 2 k ) (4) where σ 2 γ j = M j,j H j (M j,j+,..., M j,n 2 k), with σ 2 γ N 2 k = M N 2 k,n 2 k. Note that it is computationally feasible to derive σ 2 γ j when M is sparse. The Jacobian of transforming Γ N(0, M) to (4) is. Defining η j = τ j /λ,j, we can write (4) as N(η 0, σ 2 γ, )N(η 2 0, σ 2 γ 2,2 )...N(η N 2 k 0, σ 2 γ N 2 k,n 2 k ) (42) 5
16 Let f j (Γ) = 2(ηj 2 ). The scale mixture prior in (35) can be rewritten as: N 2 k π(β Σ, Γ, Λ, λ 2 ) j= λ2 { exp( λ 2 2π 2 β2 j ) 0 exp[ β2 j 2π(2ηj 2)) 2(2ηj 2)]d(2η2 j ) (43) λ2,j 2σγ 2 exp[ j 2 (σγ 2 j )/λ 2 ]},j The last two terms in (43) constitute a scale mixture of Normals (with an exponential mixing density), which can be expressed as the univariate Laplace distribution λ,j 2 σ 2 γ j exp( λ,j σ 2 γj β j ). Equation (43) shows that the conditional prior for β j is N(0, and the conditional prior for β is 2λ 2 η 2 j +), β Γ, Σ, Λ, Λ 2 N(0, D Γ) (44) where D Γ = diag([ 2η 2 2λ 2 η 2+, 2η2 2 2η 2λ 2 η2 2 +,..., 2 N 2 k 2λ 2 η 2 N 2 k +]). Priors for Σ and λ 2,j can be elicited following standard practice in VAR and Lasso literature. In this paper, we set Wishart prior for Σ and Gamma priors for λ 2,j and λ 2,j: Σ W (S, ν), λ 2,j G(µ λ 2,j, ν λ 2,j ), λ 2,j G(µ λ2, ν λ2 ). The full conditional posterior for β is β N(β, V β ), where V β = [(I N X) )(Σ I Nk )(I N X)+(D Γ ) ], and β = V β [(I N X) (Σ I Nk )y]. The Full conditional posterior for Σ is W (S, ν), with S = (Y XB) (Y XB) + 2Q Q + S and ν = T + 2Nk + ν, with vec(q) = Γ. The 6
17 Full conditional posterior for λ 2,j is G( µ λ,j, ν λ,j ), where ν λ,j = ν λ,j +2 and µ λ,j = ν λ,j σ 2 j µ λ,j 2τ 2 j µ λ,j +ν λ,j σ 2 γ j. The Full conditional posterior for λ 2 is G( µ λ2, ν λ2 ), µ λ2 ν λ2 where ν λ2 = ν λ2 + N 2 k and µ λ2 = ν λ2 +µ λ2 β 2. Finally the full conditional j λ posterior of is Inverse Gaussian: IG( 2,j, λ2,j ). Γ can not be directly 2ηj 2 βj 2σ2 γ σ 2 j γ j drawn from the posteriors. But it can be recovered in each Gibbs iteration using the draws of and Σ. 2ηj 2 Conditional on arbitrary starting values, the Gibbs sampler contains the following six steps:. draw β Σ, Λ, Λ 2, Γ from N(β, V β ); 2. draw Σ β, Λ, Λ 2, Γ from W (S, ν) 3. draw λ 2,j β, Σ, Λ, j, Λ 2, Γ from G( µ λ,j, ν λ,j ) for j =, 2,...N 2 k 4. draw λ 2 β, Σ, Λ, Γ from G( µ λ2, ν λ2 ) 5. draw λ β, Σ, Λ 2ηj 2, Λ 2 from IG( 2,j, λ2,j ) for j =, 2,...N 2 k. βj 2σ2 γ σ 2 j γ j 6. calculate Γ based on draws of Σ and in the current iteration. 2 Detailed Forecast Evaluation Results Tables -4 report the DAELasso forecasts results along with Lasso, adaptive Lasso, e-net Lasso, adaptive e-net Lasso, and those of the factor models and the seven popular Bayesian shrinkage priors in Koop (20). In line with Koop (20), we present MSFE relative to the random walk and log predictive likelihood for GDP, CPI and FFR. The results for DAELasso 7
18 and four other Lasso types of shrinkage methods are reported at the top of each table, followed by those of the methods reported in Koop (20). Koop (20) considers three variants of the Minnesota prior. The first is the natural conjugate prior used in Banbura et al (200), which is labelled Minn. Prior as in BGR. The second is the traditional Minnesota prior of Litterman (986), which is labelled Minn. Prior Σ diagonal. The third is the traditional Minnesota prior except that the upper left 3 3 block of Σ is not assumed to be daigonal, which is labelled Minn. Prior Σ not diagonal. Koop (20) also evaluates the performances of four types of SSVS priors. The first is the same as George et al (2008), which is labelled SSVS Non-conj. semi-automatic. The second is a combination of the non-conjugate SSVS prior and Minnesota prior with variables selected in a data based fashion, which is labelled SSVS Non-conj. plus Minn. Prior. The Third is a conjugate SSVS prior, which is labelled SSVS Conjugate Semi-automatic. The fourth is a combination of the conjugate SSVS prior and Minnesota prior, which is labelled SSVS Conjugate plus Minn. Prior. Finally the results for factor-augmented VAR models with one and four lagged factors are labelled as Factor model p= and Factor model p=4, respectively. We refer to Koop (20) for a lucid description of these priors. 8
19 DAELasso adaptive e-net Lasso e-net Lasso adaptive Lasso Lasso Minn. Prior as in BGR Minn. Prior Σ diagonal Minn. Prior Σ not diagonal SSVS Conjugate semi-automatic SSVS Conjugate plus Minn. Prior SSVS Non-conj. semi-automatic SSVS Non-conj. plus Minn. Prior Factor model p= Factor model p=4 Notes: Table : Rolling Forecasting for h = MSFEs as proportion of random walk MSFEs. Sum of log predictive likelihoods in parentheses. GDP CPI FFR ( ) ( ) ( -2.7 ) ( ) ( ) ( ) ( ) ( -2.6 ) ( ) ( ) ( ) ( ) ( ) ( ) ( ) ( -90.5) ( ) ( ) ( ) ( ) ( -8.7 ) ( -92. ) ( ) ( ) ( ) ( ) ( ) ( -9.4 ) ( -22. ) ( ) ( ) ( ) ( ) ( ) ( ) ( ) ( ) ( ) ( ) ( ) ( ) ( ) 9
20 DAELasso adaptive e-net Lasso e-net Lasso adaptive Lasso Lasso Minn. Prior as in BGR Minn. Prior Σ diagonal Minn. Prior Σ not diagonal SSVS Conjugate semi-automatic SSVS Conjugate plus Minn. Prior SSVS Non-conj. semi-automatic SSVS Non-conj. plus Minn. Prior Factor model p= Factor model p=4 Notes: Table 2: Rolling Forecasting for h = 4 MSFEs as proportion of random walk MSFEs. Sum of log predictive likelihoods in parentheses. GDP CPI FFR ( ) ( ) ( ) ( ) ( ) ( -29.9) ( ) ( ) ( ) ( ) ( ) ( ) ( ) ( ) ( ) ( -27. ) ( ) ( ) ( -2. ) ( ) ( ) ( ) ( ) ( -22. ) ( ) ( ) ( ) ( ) ( ) ( ) ( ) ( ) ( ) ( ) ( ) ( -98. ) ( ) ( ) ( ) ( ) ( ) ( ) 20
21 DAELasso adaptive e-net Lasso e-net Lasso adaptive Lasso Lasso Minn. Prior as in BGR Minn. Prior Σ diagonal Minn. Prior Σ not diagonal SSVS Conjugate semi-automatic Table 3: Recursive Forecasting for h = SSVS Conjugate plus Minn. Prior SSVS Non-conj. semi-automatic SSVS Non-conj. plus Minn. Prior Factor model p= Factor model p=4 Notes: MSFEs as proportion of random walk MSFEs. Sum of log predictive likelihoods in parentheses. GDP CPI FFR ( ) ( ) ( ) ( ) ( ) ( ) ( ) ( ) ( ) ( ) ( ) ( ) ( ) ( -22. ) ( ) ( ) ( ) ( ) ( ) ( ) ( ) ( ) ( -84. ) ( ) ( ) ( -9.2 ) ( ) ( ) ( ) ( ) ( ) ( ) ( ) ( ) ( ) ( ) ( ) ( ) ( ) ( ) ( -29. ) ( ) 2
22 DAELasso adaptive e-net Lasso e-net Lasso adaptive Lasso Lasso Minn. Prior as in BGR Minn. Prior Σ diagonal Minn. Prior Σ not diagonal SSVS Conjugate semi-automatic Table 4: Recursive Forecasting for h = 4 SSVS Conjugate plus Minn. Prior SSVS Non-conj. semi-automatic SSVS Non-conj. plus Minn. Prior Factor model p= Factor model p=4 Notes: MSFEs as proportion of random walk MSFEs. Sum of log predictive likelihoods in parentheses. GDP CPI FFR ( ) ( ) ( ) ( ) ( ) ( ) ( ) ( ) ( ) ( ) ( ) ( ) ( ) ( ) ( ) ( ) ( ) ( ) ( ) ( ) ( ) ( ) ( -26. ) ( ) ( ) ( ) ( ) ( ) ( ) ( ) ( ) ( ) ( ) ( ) ( ) ( ) ( ) ( -2.6 ) ( ) ( ) ( ) ( ) 22
Bayesian 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
Other 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 :
ΚΥΠΡΙΑΚΗ ΕΤΑΙΡΕΙΑ ΠΛΗΡΟΦΟΡΙΚΗΣ CYPRUS COMPUTER SOCIETY ΠΑΓΚΥΠΡΙΟΣ ΜΑΘΗΤΙΚΟΣ ΔΙΑΓΩΝΙΣΜΟΣ ΠΛΗΡΟΦΟΡΙΚΗΣ 19/5/2007
Οδηγίες: Να απαντηθούν όλες οι ερωτήσεις. Αν κάπου κάνετε κάποιες υποθέσεις να αναφερθούν στη σχετική ερώτηση. Όλα τα αρχεία που αναφέρονται στα προβλήματα βρίσκονται στον ίδιο φάκελο με το εκτελέσιμο
6.3 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
Web-based supplementary materials for Bayesian Quantile Regression for Ordinal Longitudinal Data
Web-based supplementary materials for Bayesian Quantile Regression for Ordinal Longitudinal Data Rahim Alhamzawi, Haithem Taha Mohammad Ali Department of Statistics, College of Administration and Economics,
SOLUTIONS 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
Srednicki Chapter 55
Srednicki Chapter 55 QFT Problems & Solutions A. George August 3, 03 Srednicki 55.. Use equations 55.3-55.0 and A i, A j ] = Π i, Π j ] = 0 (at equal times) to verify equations 55.-55.3. This is our third
Section 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.
2 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,
HOMEWORK 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
Solution 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
Jesse 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
3.4 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
SCHOOL OF MATHEMATICAL SCIENCES G11LMA Linear Mathematics Examination Solutions
SCHOOL OF MATHEMATICAL SCIENCES GLMA Linear Mathematics 00- Examination Solutions. (a) i. ( + 5i)( i) = (6 + 5) + (5 )i = + i. Real part is, imaginary part is. (b) ii. + 5i i ( + 5i)( + i) = ( i)( + i)
CHAPTER 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) =
SOLUTIONS 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
Approximation 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
6.1. 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
CHAPTER 48 APPLICATIONS OF MATRICES AND DETERMINANTS
CHAPTER 48 APPLICATIONS OF MATRICES AND DETERMINANTS EXERCISE 01 Page 545 1. Use matrices to solve: 3x + 4y x + 5y + 7 3x + 4y x + 5y 7 Hence, 3 4 x 0 5 y 7 The inverse of 3 4 5 is: 1 5 4 1 5 4 15 8 3
Notes 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.
derivation 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
Solutions 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
DERIVATION OF MILES EQUATION FOR AN APPLIED FORCE Revision C
DERIVATION OF MILES EQUATION FOR AN APPLIED FORCE Revision C By Tom Irvine Email: tomirvine@aol.com August 6, 8 Introduction The obective is to derive a Miles equation which gives the overall response
Second 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
Description of the PX-HC algorithm
A Description of the PX-HC algorithm Let N = C c= N c and write C Nc K c= i= k= as, the Gibbs sampling algorithm at iteration m for continuous outcomes: Step A: For =,, J, draw θ m in the following steps:
PARTIAL NOTES for 6.1 Trigonometric Identities
PARTIAL NOTES for 6.1 Trigonometric Identities tanθ = sinθ cosθ cotθ = cosθ sinθ BASIC IDENTITIES cscθ = 1 sinθ secθ = 1 cosθ cotθ = 1 tanθ PYTHAGOREAN IDENTITIES sin θ + cos θ =1 tan θ +1= sec θ 1 + cot
[1] P Q. Fig. 3.1
1 (a) Define resistance....... [1] (b) The smallest conductor within a computer processing chip can be represented as a rectangular block that is one atom high, four atoms wide and twenty atoms long. One
Modern Bayesian Statistics Part III: high-dimensional modeling Example 3: Sparse and time-varying covariance modeling
Modern Bayesian Statistics Part III: high-dimensional modeling Example 3: Sparse and time-varying covariance modeling Hedibert Freitas Lopes 1 hedibert.org 13 a amostra de Estatística IME-USP, October
Exercises 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
C.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
ST5224: 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
An Inventory of Continuous Distributions
Appendi A An Inventory of Continuous Distributions A.1 Introduction The incomplete gamma function is given by Also, define Γ(α; ) = 1 with = G(α; ) = Z 0 Z 0 Z t α 1 e t dt, α > 0, >0 t α 1 e t dt, α >
Section 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)
CRASH 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
Section 9.2 Polar Equations and Graphs
180 Section 9. Polar Equations and Graphs In this section, we will be graphing polar equations on a polar grid. In the first few examples, we will write the polar equation in rectangular form to help identify
Phys460.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
Problem 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
Chapter 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
DESIGN OF MACHINERY SOLUTION MANUAL h in h 4 0.
DESIGN OF MACHINERY SOLUTION MANUAL -7-1! PROBLEM -7 Statement: Design a double-dwell cam to move a follower from to 25 6, dwell for 12, fall 25 and dwell for the remader The total cycle must take 4 sec
Partial Trace and Partial Transpose
Partial Trace and Partial Transpose by José Luis Gómez-Muñoz http://homepage.cem.itesm.mx/lgomez/quantum/ jose.luis.gomez@itesm.mx This document is based on suggestions by Anirban Das Introduction This
Partial 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
SCITECH 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
Math 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
Dynamic types, Lambda calculus machines Section and Practice Problems Apr 21 22, 2016
Harvard School of Engineering and Applied Sciences CS 152: Programming Languages Dynamic types, Lambda calculus machines Apr 21 22, 2016 1 Dynamic types and contracts (a) To make sure you understand the
Testing for Indeterminacy: An Application to U.S. Monetary Policy. Technical Appendix
Testing for Indeterminacy: An Application to U.S. Monetary Policy Technical Appendix Thomas A. Lubik Department of Economics Johns Hopkins University Frank Schorfheide Department of Economics University
5.4 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
The Simply Typed Lambda Calculus
Type Inference Instead of writing type annotations, can we use an algorithm to infer what the type annotations should be? That depends on the type system. For simple type systems the answer is yes, and
Statistical 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
Matrices 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
6. MAXIMUM LIKELIHOOD ESTIMATION
6 MAXIMUM LIKELIHOOD ESIMAION [1] Maximum Likelihood Estimator (1) Cases in which θ (unknown parameter) is scalar Notational Clarification: From now on, we denote the true value of θ as θ o hen, view θ
Bayesian modeling of inseparable space-time variation in disease risk
Bayesian modeling of inseparable space-time variation in disease risk Leonhard Knorr-Held Laina Mercer Department of Statistics UW May, 013 Motivation Ohio Lung Cancer Example Lung Cancer Mortality Rates
Numerical Analysis FMN011
Numerical Analysis FMN011 Carmen Arévalo Lund University carmen@maths.lth.se Lecture 12 Periodic data A function g has period P if g(x + P ) = g(x) Model: Trigonometric polynomial of order M T M (x) =
Tutorial on Multinomial Logistic Regression
Tutorial on Multinomial Logistic Regression Javier R Movellan June 19, 2013 1 1 General Model The inputs are n-dimensional vectors the outputs are c-dimensional vectors The training sample consist of m
Example 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
Derivation of Optical-Bloch Equations
Appendix C Derivation of Optical-Bloch Equations In this appendix the optical-bloch equations that give the populations and coherences for an idealized three-level Λ system, Fig. 3. on page 47, will be
MATH423 String Theory Solutions 4. = 0 τ = f(s). (1) dτ ds = dxµ dτ f (s) (2) dτ 2 [f (s)] 2 + dxµ. dτ f (s) (3)
1. MATH43 String Theory Solutions 4 x = 0 τ = fs). 1) = = f s) ) x = x [f s)] + f s) 3) equation of motion is x = 0 if an only if f s) = 0 i.e. fs) = As + B with A, B constants. i.e. allowe reparametrisations
Lecture 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
Mean bond enthalpy Standard enthalpy of formation Bond N H N N N N H O O O
Q1. (a) Explain the meaning of the terms mean bond enthalpy and standard enthalpy of formation. Mean bond enthalpy... Standard enthalpy of formation... (5) (b) Some mean bond enthalpies are given below.
Reminders: linear functions
Reminders: linear functions Let U and V be vector spaces over the same field F. Definition A function f : U V is linear if for every u 1, u 2 U, f (u 1 + u 2 ) = f (u 1 ) + f (u 2 ), and for every u U
EE512: 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
DiracDelta. Notations. Primary definition. Specific values. General characteristics. Traditional name. Traditional notation
DiracDelta Notations Traditional name Dirac delta function Traditional notation x Mathematica StandardForm notation DiracDeltax Primary definition 4.03.02.000.0 x Π lim ε ; x ε0 x 2 2 ε Specific values
Queensland University of Technology Transport Data Analysis and Modeling Methodologies
Queensland University of Technology Transport Data Analysis and Modeling Methodologies Lab Session #7 Example 5.2 (with 3SLS Extensions) Seemingly Unrelated Regression Estimation and 3SLS A survey of 206
Math221: 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
Tridiagonal 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,...,
Supplementary Appendix
Supplementary Appendix Measuring crisis risk using conditional copulas: An empirical analysis of the 2008 shipping crisis Sebastian Opitz, Henry Seidel and Alexander Szimayer Model specification Table
Additional Results for the Pareto/NBD Model
Additional Results for the Pareto/NBD Model Peter S. Fader www.petefader.com Bruce G. S. Hardie www.brucehardie.com January 24 Abstract This note derives expressions for i) the raw moments of the posterior
Concrete 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)
Areas 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
Δθαξκνζκέλα καζεκαηηθά δίθηπα: ε πεξίπησζε ηνπ ζπζηεκηθνύ θηλδύλνπ ζε κηθξνεπίπεδν.
ΑΡΗΣΟΣΔΛΔΗΟ ΠΑΝΔΠΗΣΖΜΗΟ ΘΔΑΛΟΝΗΚΖ ΣΜΖΜΑ ΜΑΘΖΜΑΣΗΚΧΝ ΠΡΟΓΡΑΜΜΑ ΜΔΣΑΠΣΤΥΗΑΚΧΝ ΠΟΤΓΧΝ Δπηζηήκε ηνπ Γηαδηθηύνπ «Web Science» ΜΔΣΑΠΣΤΥΗΑΚΖ ΓΗΠΛΧΜΑΣΗΚΖ ΔΡΓΑΗΑ Δθαξκνζκέλα καζεκαηηθά δίθηπα: ε πεξίπησζε ηνπ ζπζηεκηθνύ
Περίληψη (Executive Summary)
1 Περίληψη (Executive Summary) Η παρούσα διπλωματική εργασία έχει ως αντικείμενο την "Αγοραστική/ καταναλωτική συμπεριφορά. Η περίπτωση των Σπετσών" Κύριος σκοπός της διπλωματικής εργασίας είναι η διερεύνηση
Congruence 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
These derivations are not part of the official forthcoming version of Vasilaky and Leonard
Target Input Model with Learning, Derivations Kathryn N Vasilaky These derivations are not part of the official forthcoming version of Vasilaky and Leonard 06 in Economic Development and Cultural Change.
Aquinas 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
Fourier 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)
DuPont Suva. DuPont. Thermodynamic Properties of. Refrigerant (R-410A) Technical Information. refrigerants T-410A ENG
Technical Information T-410A ENG DuPont Suva refrigerants Thermodynamic Properties of DuPont Suva 410A Refrigerant (R-410A) The DuPont Oval Logo, The miracles of science, and Suva, are trademarks or registered
FORMULAS FOR STATISTICS 1
FORMULAS FOR STATISTICS 1 X = 1 n Sample statistics X i or x = 1 n x i (sample mean) S 2 = 1 n 1 s 2 = 1 n 1 (X i X) 2 = 1 n 1 (x i x) 2 = 1 n 1 Xi 2 n n 1 X 2 x 2 i n n 1 x 2 or (sample variance) E(X)
Part 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
k 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
D 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
1. A fully continuous 20-payment years, 30-year term life insurance of 2000 is issued to (35). You are given n A 1
Chapter 7: Exercises 1. A fully continuous 20-payment years, 30-year term life insurance of 2000 is issued to (35). You are given n A 1 35+n:30 n a 35+n:20 n 0 0.068727 11.395336 10 0.097101 7.351745 25
Strain gauge and rosettes
Strain gauge and rosettes Introduction A strain gauge is a device which is used to measure strain (deformation) on an object subjected to forces. Strain can be measured using various types of devices classified
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
Figure 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
CHAPTER 101 FOURIER SERIES FOR PERIODIC FUNCTIONS OF PERIOD
CHAPTER FOURIER SERIES FOR PERIODIC FUNCTIONS OF PERIOD EXERCISE 36 Page 66. Determine the Fourier series for the periodic function: f(x), when x +, when x which is periodic outside this rge of period.
DuPont Suva 95 Refrigerant
Technical Information T-95 ENG DuPont Suva refrigerants Thermodynamic Properties of DuPont Suva 95 Refrigerant (R-508B) The DuPont Oval Logo, The miracles of science, and Suva, are trademarks or registered
Example of the Baum-Welch Algorithm
Example of the Baum-Welch Algorithm Larry Moss Q520, Spring 2008 1 Our corpus c We start with a very simple corpus. We take the set Y of unanalyzed words to be {ABBA, BAB}, and c to be given by c(abba)
Space-Time Symmetries
Chapter Space-Time Symmetries In classical fiel theory any continuous symmetry of the action generates a conserve current by Noether's proceure. If the Lagrangian is not invariant but only shifts by a
Areas 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
상대론적고에너지중이온충돌에서 제트입자와관련된제동복사 박가영 인하대학교 윤진희교수님, 권민정교수님
상대론적고에너지중이온충돌에서 제트입자와관련된제동복사 박가영 인하대학교 윤진희교수님, 권민정교수님 Motivation Bremsstrahlung is a major rocess losing energies while jet articles get through the medium. BUT it should be quite different from low energy
Technical Information T-9100 SI. Suva. refrigerants. Thermodynamic Properties of. Suva Refrigerant [R-410A (50/50)]
d Suva refrigerants Technical Information T-9100SI Thermodynamic Properties of Suva 9100 Refrigerant [R-410A (50/50)] Thermodynamic Properties of Suva 9100 Refrigerant SI Units New tables of the thermodynamic
Parametrized 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
Every 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
( ) 2 and compare to M.
Problems and Solutions for Section 4.2 4.9 through 4.33) 4.9 Calculate the square root of the matrix 3!0 M!0 8 Hint: Let M / 2 a!b ; calculate M / 2!b c ) 2 and compare to M. Solution: Given: 3!0 M!0 8
22 .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
ΠΑΝΔΠΗΣΖΜΗΟ ΠΑΣΡΩΝ ΣΜΖΜΑ ΖΛΔΚΣΡΟΛΟΓΩΝ ΜΖΥΑΝΗΚΩΝ ΚΑΗ ΣΔΥΝΟΛΟΓΗΑ ΤΠΟΛΟΓΗΣΩΝ ΣΟΜΔΑ ΤΣΖΜΑΣΩΝ ΖΛΔΚΣΡΗΚΖ ΔΝΔΡΓΔΗΑ
ΠΑΝΔΠΗΣΖΜΗΟ ΠΑΣΡΩΝ ΣΜΖΜΑ ΖΛΔΚΣΡΟΛΟΓΩΝ ΜΖΥΑΝΗΚΩΝ ΚΑΗ ΣΔΥΝΟΛΟΓΗΑ ΤΠΟΛΟΓΗΣΩΝ ΣΟΜΔΑ ΤΣΖΜΑΣΩΝ ΖΛΔΚΣΡΗΚΖ ΔΝΔΡΓΔΗΑ Γηπισκαηηθή Δξγαζία ηνπ Φνηηεηή ηνπ ηκήκαηνο Ζιεθηξνιόγσλ Μεραληθώλ θαη Σερλνινγίαο Ζιεθηξνληθώλ
Chapter 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
Τμήμα Πολιτικών και Δομικών Έργων
Τμήμα Πολιτικών και Δομικών Έργων Πτυχιακή Εργασία: Τοπογραφικό διάγραμμα σε ηλεκτρονική μορφή κεντρικού λιμένα Κέρκυρας και κτιρίου νέου επιβατικού σταθμού σε τρισδιάστατη μορφή και σχεδίαση με AutoCAD
Ordinal 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
ΤΕΧΝΟΛΟΓΙΚΟ ΠΑΝΕΠΙΣΤΗΜΙΟ ΚΥΠΡΟΥ ΣΧΟΛΗ ΓΕΩΤΕΧΝΙΚΩΝ ΕΠΙΣΤΗΜΩΝ ΚΑΙ ΔΙΑΧΕΙΡΙΣΗΣ ΠΕΡΙΒΑΛΛΟΝΤΟΣ. Πτυχιακή εργασία
ΤΕΧΝΟΛΟΓΙΚΟ ΠΑΝΕΠΙΣΤΗΜΙΟ ΚΥΠΡΟΥ ΣΧΟΛΗ ΓΕΩΤΕΧΝΙΚΩΝ ΕΠΙΣΤΗΜΩΝ ΚΑΙ ΔΙΑΧΕΙΡΙΣΗΣ ΠΕΡΙΒΑΛΛΟΝΤΟΣ Πτυχιακή εργασία ΑΝΑΛΥΣΗ ΚΟΣΤΟΥΣ-ΟΦΕΛΟΥΣ ΓΙΑ ΤΗ ΔΙΕΙΣΔΥΣΗ ΤΩΝ ΑΝΑΝΕΩΣΙΜΩΝ ΠΗΓΩΝ ΕΝΕΡΓΕΙΑΣ ΣΤΗΝ ΚΥΠΡΟ ΜΕΧΡΙ ΤΟ 2030
Similarly, we may define hyperbolic functions cosh α and sinh α from the unit hyperbola
Universit of Hperbolic Functions The trigonometric functions cos α an cos α are efine using the unit circle + b measuring the istance α in the counter-clockwise irection along the circumference of the