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Then, applying the MoM leads to matrix equation as follow: N * p =1 Z qp I p = V q,q =1 , 2 , ···,N (2) where[ I ]and[ V ]are vectors representing the unknown current coefficients to be ...
Then, using the Granger representation theorem, we may posit the following testing relationships that constitutea VEC model for output growth: D Z sGD Z qGD Z q«qGD Z qP Z qmqh, t s 1 ...
012 34560789:9; <=>?%%%%@a bcde fgde h00i j00k h00i j00k lmnbco %%%%%-pq-.pq+rslmnfgo %%%%%+q.((q-r) 1 j t u v j %%%%%(.qp-+qwxsy z j %%%%%)p(qrxw [\ j %%%%%)(q--xqs.sy z] ^ %%%%%)qp)(qp(x _ ` a j ...
{S, C, D, Z} QP QR decomposition with column pivoting {S, C, D, Z} HR Reduction to Hessenberg form {S, C, D, Z} TD Reduction to real tridiagonal form
Then, applying the MoM leads to matrix equation as follow: N * p =1 Z qp I p = V q,q =1 , 2 , ···,N (2) where[ I ]and[ V ]are vectors representing the unknown current coefficients ...
... motion vector bits in (5) can be used to determine the threshold TH, which can be expressed as (8) TH = Tho + C, Tho =max(Th,,Thb), (9) (10) where C is a constant and Thj * S-'(max(Z(QP ...
Then, using the Granger representation theorem, we may posit the following testing relationships that constitutea VEC model for output growth: D Z sGD Z qGD Z q«qGD Z qP Z ...
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