Quantitative Finance and Investments Advanced Formula Sheet. Fall 2014/Spring 2015

Μέγεθος: px
Εμφάνιση ξεκινά από τη σελίδα:

Download "Quantitative Finance and Investments Advanced Formula Sheet. Fall 2014/Spring 2015"

Transcript

1 Quaniaive Finance and Invemen Advanced Formula Shee Fall 2014/Spring 2015 Morning and afernoon exam bookle will include a formula package idenical o he one aached o hi udy noe. The exam commiee believe ha by providing many key formula, candidae will be able o focu more of heir exam preparaion ime on he applicaion of he formula and concep o demonrae heir underanding of he yllabu maerial and le ime on he memorizaion of he formula. The formula hee wa developed equenially by reviewing he yllabu maerial for each major yllabu opic. Candidae hould be able o follow he flow of he formula package eaily. We recommend ha candidae ue he formula package concurrenly wih he yllabu maerial. No every formula in he yllabu i in he formula package. Candidae are reponible for all formula on he yllabu, including hoe no on he formula hee. Candidae hould carefully oberve he omeime uble difference in formula and heir applicaion o lighly differen iuaion. Candidae will be expeced o recognize he correc formula o apply in a pecific iuaion of an exam queion. Candidae will noe ha he formula package doe no generally provide name or definiion of he formula or ymbol ued in he formula. Wih he wide variey of reference and auhor of he yllabu, candidae hould recognize ha he leer convenion and ue of ymbol may vary from one par of he yllabu o anoher and hu from one formula o anoher. Weruhayouwillfindheincluionofheformulapackageobeavaluableudyaide ha will allow for more of your preparaion ime o be pen on maering he learning objecive and learning oucome. Change from Spring 2014 are: Addiion of formula from Chaper 69 and 71 of Fabozzi Addiion of a formula from Chaper 6 of Bluhm Deleion of Chaper 3 and 8 of Tay 1

2 Inere Rae Model - Theory and Pracice, Brigo and Mercurio Chaper 3 Table 3.1 Summary of inananeou hor rae model Model Dynamic r > 0 r AB AO V dr = k[θ r ]d + σdw N N Y Y CIR dr = k[θ r ]d + σ r dw Y NCχ 2 Y Y D dr = ar d + σr dw Y LN Y N EV dr = r [η a ln r ]d + σr dw Y LN N N HW dr = k[θ r ]d + σdw N N Y Y BK dr = r [η ³ a ln r ]d + i σr dw Y LN N N MM dr = r hη λ ln r d + σr dw Y LN N N γ 1+γ CIR++ r = x + ϕ, dx = k[θ x ]d + σ x dw Y* SNCχ 2 Y Y EEV r = x + ϕ, dx = x [η a ln x ]d + σx dw Y* SLN N N *rae are poiive under uiable condiion for he deerminiic funcion ϕ. (3.5) dr() =k[θ r()]d + σdw(), r(0) = r 0 (3.6) r() =r()e k( ) + θ k( ) + σ R e k( u) dw (u) (3.7) E {r() F } = r()e k( ) + θ k( ) Var{r() F } = σ2 2k( ) 2k (3.8) B(,T )r() P (, T )=A(, T )e (3.9) dr() =[kθ B(, T )σ 2 kr()]d + σdw T () (3.11) dr() =[kθ (k + λσ)r()]d + σdw 0 (), r(0) = r 0 (3.12) dr() =[b ar()]d + σdw 0 () (3.13) r() =r()e a( ) + b a( ) + σ R a dw 0 (u) (3.14) ˆα = n P n r ir i 1 P n r P n i r i 1 n P n r2 i 1 (P n r i 1) 2 P n (3.15) ˆβ = [r i ˆαr i 1 ] n(1 ˆα) (3.16) V c 2 = 1 P h n r i ˆαr i 1 n ˆβ(1 i 2 ˆα) (3.19) E {r() F } = r()e a( ) and Var{r() F } = r 2 ()e ³e 2a( ) σ2 ( ) 1 (3.20) P (, T )= rp R in(2 r inh y) R f(z)in(yz)dzdy + 2 π Γ(2p) rp K 2p (2 r) (3.21) dr() =k(θ r())d + σ p r()dw (), r(0) = r 0 (3.22) dr() =[kθ (k + λσ)r()]d + σ p r()dw 0 (), r(0) = r 0 2

3 (3.23) E {r() F } = r()e k( ) + θ k( ) Var{r() F } = r() σ2 e k( ) e 2k( ) + θ σ2 k( ) 2 k 2k (3.24) B(,T )r() P (, T )=A(, T )e (3.25) 2kθ/σ 2 2h exp {(k + h)(t )/2} A(, T )= 2h +(k + h)(exp {(T )h} 1) B(, T )= 2(exp{(T )h} 1) 2h +(k + h)(exp {(T )h} 1), h = k 2 +2σ 2 (3.27) dr() =[kθ (k + B(, T )σ 2 )r()]d + σ p r()dw T () (3.28) p T r() r() (x) =p χ 2 (υ,δ(,))/q(,)(x) =q(, )p χ 2 (υ,δ(,))(q(, )x) q(, ) =2[ρ( )+ψ + B(, T )] and δ(, ) = 4ρ( )2 r()e h( ) q(, ) Page 68 R(, T )=α(, T )+β(, T )r(), B(,T )r() P(, T )=A(, T )e (3.29) σ f (, T )= B(, T ) σ(, r()) T Page 69 dr() = b(, r())d + σ(, r())dw () b(, x) =λ()x + η(), σ 2 (, x) =γ()x + δ() B(, T )+λ()b(, T ) 1 2 γ()b(, T )2 +1=0, B(T,T)=0 [ln A(, T )] η()b(, T )+1 2 δ()b(, T )2 =0, A(T,T)=1 Page 69/70 Vaicek λ() = k, η() =kθ, γ() =0, δ() =σ 2 Page 70 CIR λ() = k, η() =kθ, γ() =σ 2, δ() =0 b(x) =λx + η, σ 2 (x) =γx + δ µ θ Page 71 lim E{r() F } =exp a + σ2 4a µ µ 2θ (3.31) lim Var{r() F } =exp a + σ2 σ 2 exp 1 2a 2a (3.32) dr() =[ϑ() a()r()]d + σ()dw () (3.33) dr() =[ϑ() ar()]d + σdw() (3.34) ϑ() = fm (0,) + af M (0,)+ σ2 T 2a ( 2a ) (3.35) r() =r()e a( ) + R e a( u) ϑ(u)du + σ R e a( u) dw (u) = r()e a( ) + α() α()e a( ) + σ R e a( u) dw (u) (3.36) where α() =f M (0,)+ σ2 2a 2 ( a ) 2 3

4 (3.37) E{r() F } = r()e a( ) + α() α()e a( ) Var{r() F } = σ2 2a( ) 2a (3.38) dx() = ax()d + σdw(), x(0) = 0 Page 74 x() =x()e a( ) + σ R e a( u) dw (u) (3.47) E{x( i+1 ) x( i )=x i,j } = x i,j e a i =: M i,j Var{x( i+1 ) x( i )=x i,j } = σ2 2a i =: V 2 2a i r 3 (3.48) x i = V i 1 3=σ 2a [ 2a i 1 µ Mi,j (3.49) k =round x i+1 (3.50) p u = η2 j,k + η j,k 6Vi 2 2,p m = 2 3V i 3 η2 j,k,p 3Vi 2 d = η2 j,k 6Vi 2 2 3V i (3.64) dx α = μ(x α ; α)d + σ(x α ; α)dw x (3.65) P x (, T )=Π x (, T, x α ; α) (3.66) r = x + ϕ(; α), 0 h (3.67) P (, T )=exp R i T ϕ(; α)d Π x (, T, r ϕ(; α); α) (3.68) ϕ(; α) =ϕ (; α) :=f M (o, ) f x (0,; α) (3.69) h exp R i T ϕ(; α)d = Φ (, T, x 0 ; α) := P M (0,T) Π x (0,,x 0 ; α) Π x (0,T,x 0 ; α) P M (0,) (3.70) Π(, T, r ; α) =Φ (, T, x 0 ; α)π (, T, r ϕ (; α); α) (3.71) V x (, T, τ, K) =Ψ x (, T, τ, K, x α ; α) dϕ(; α) (3.74) dr = kθ + kϕ(; α)+ kr d + σdw d Page 100 ϕ VAS (; α) =f M (0,)+(e k 1) k2 θ σ 2 /2 k 2 η j,k σ2 2k 2 e k ( k ) x 0 e k Page 101 P (, T )= P M (0,T)A(0,)exp{ B(0,)x 0 } P M (0,)A(0,T)exp{ B(0,T)x 0 } A(, T )exp{ B(, T )[r ϕ VAS (; α)]} (3.76) dx() =k(θ x())d + σ p x()dw (), x(0) = x 0, r() =x()+ϕ() (3.77) ϕ CIR (; α) =f M (0,) f CIR (0,; α) f CIR 2kθ(exp{h} 1) (0,; α) = 2h +(k + h)(exp{h} 1) + x 4h 2 exp{h} 0 [2h +(k + h)(exp{h} 1)] 2 h = k 2 +2σ 2 4

5 Chaper 4 (4.4) r = x()+y()+ϕ(), r(0) = r 0 (4.5) dx() = ax()d + σdw 1 (), x(0) = 0 dy() = by()d + ηdw 2 (), y(0) = 0 (4.6) E{r() F } = x()e a( ) + y()e b( ) + ϕ() Var{r() F } = σ2 2a( ) + η2 2b( ) +2ρ ση (a+b)( ) 2a 2b a + b (4.7) r() =σ R 0 e a( u) dw 1 (u)+η R 0 e b( u) dw 2 (u)+ϕ() (4.8) dx() = ax()d + σdfw 1 () dy() = by()d + ηρdfw 1 ()+η p 1 ρ 2 dfw 2 () where dw 1 () =ddfw 1 () and dw 2 () =ρdfw 1 ()+ p 1 ρ 2 dfw 2 () ) ) a(t b(t (4.9) M(, T )= x()+ y() a b (4.10) V (, T )= σ2 T + 2 a 2 a e a(t ) 1 2a e 2a(T ) 3 2a + η2 T + 2 b 2 b e b(t ) 1 2b e 2b(T ) 3 2b +2ρ ση ab (4.11) P (, T )=exp T + e a(t ) 1 a ½ R T + e b(t ) 1 b ϕ(u)du a(t ) x() a e (a+b)(t ) 1 a + b ) b(t y()+ 1 ¾ b 2 V (, T ) (4.12) ϕ() =f M (0,T)+ σ2 at 2 + η2 bt 2 + ρ ση 2a 2 2b 2 ab ( at )( bt ) n (4.13) exp R o T ϕ(u)du = P M (0,T) ½ P M (0,) exp 12 ¾ [V (0,T) V (0,)] (4.14) P (, T )= P M (0,T) exp {A(, T )} P M (0,) A(, T ):= 1 ) ) a(t b(t [V (, T ) V (0,T)+V(0,)] x() y() 2 a b (4.15) P (, T )=A(, T )exp{ B(a,, T )x() B(b,, T )y()} (4.16) σ f (, T )= p σ 2 e 2a(T ) + η 2 e 2b(T ) +2ρσηe (a+b)(t ) 5

6 Page 152 Cov(df (, T 1 ),df(, T 2 )) d = σ 2 B T (a,, T 1) B T (a,, T 2)+η 2 B T (b,, T 1) B T (b,, T 2) B +ρση T (a,, T 1) B T (b,, T 2)+ B T (a,, T 2) B T (b,, T 1) = σ 2 e a(t 1+T 2 2) + η 2 e b(t 1+T 2 2) +ρση e at 1 bt 2 +(a+b) + e at 2 bt 1 +(a+b) Corr(df (, T 1 ),df(, T 2 )) = σ2 e a(t 1+T 2 2) + η 2 e b(t 1+T 2 2) σ f (, T 1 )σ f (, T 2 ) + ρση e at 1 bt 2 +(a+b) + e at 2 bt 1 +(a+b) σ f (, T 1 )σ f (, T 2 ) Page 153 f(, T 1 T 2 )= ln P (, T 1) ln P (, T 2 ) T 2 T 1 df (, T 1,T 2 )=...d + B(a,, T 2) B(a,, T 1 ) σdw 1 () T 2 T 1 + B(b,, T 2) B(b,, T 1 ) ηdw 2 () T 2 T 1 σ f (, T 1,T 2 )= p σ 2 β(a,, T 1,T 2 ) 2 + η 2 β(b,, T 1,T 2 ) 2 +2ρσηβ(a,, T 1,T 2 )β(b,, T 1,T 2 ) where β(z,, T 1,T 2 )= B(z,, T 2) B(z,,T 1 ) T 2 T 1 Cov(df (, T 1,T 2 ),df(, T 3,T 4 )) d σ 2 B(a,, T 2) B(a,, T 1 ) B(a,, T 4 ) B(a,, T 3 ) T 2 T 1 T 4 T 3 +η 2 B(b,, T 2) B(b,, T 1 ) B(b,, T 4 ) B(b,, T 3 ) T 2 T 1 T 4 T 3 B(a,, T2 ) B(a,, T 1 ) B(b,, T 4 ) B(b,, T 3 ) +ρση T 2 T 1 T 4 T 3 + B(a,, T 4) B(a,, T 3 ) B(b,, T 2 ) B(b,, T 1 ) T 4 T 3 T 2 T 1 Page 160 σ 3 = dz 3 () = σ σ2 2 (ā b) 2 +2 ρ σ 1σ 2 b ā σ 1 dz 1 () σ 2 ā b dz 2(), σ 4 = σ 2 σ 3 ā b Page 161 a =ā, b = b, σ = σ 3, η = σ 4, ρ = σ 1 ρ σ 4 σ 3 6

7 ϕ() =r 0 e ā + R 0 θ(v)e ā( v) dv ā = a, b = b, σ1 = p σ 2 + η 2 +2ρση, σ 2 = η(a b) ρ = σρ + η p σ2 + η 2 +2ρση, θ() =dϕ() + aϕ() d Managing Credi Rik: The Grea Challenge for Global Financial Marke, Caouee, e. al. Chaper 20 P (20.2) R p = N X i EAR (20.3) V p = N P j=1 (20.5) UAL p = N P Page 403 NP X i X j σ i σ j ρ ij j=1 NP X i X j σ i σ j ρ ij 1 CV ar(cl)=ead LGD µ µ ρφ 1 (CL)+Φ 1 (PD) Φ PD 1 ρ 1+(M 2.5) b(pd) 1 1.5b(PD) Liquidiy Rik Meauremen and Managemen: Guide o Global Be Pracice, Maz and Neu A Pracioner Chaper 2 Page 33 Page 33 log V () =α + β + σε log V q () =α + β σφ 1 (q) Bond-CDS Bai Handbook: Meauring, Trading and Analying Bai Trade, Elizalde, Docor, and Saluk Page 13, Equaion 1 S = PD (1 R) Page 15, Equaion 2 FR = U AI RA + FC Page 18, Equaion 3 PV[c + p] BP SS = RF A Page 25, Equaion 4 BTP1 =CN (100 R U CP F C)+BN (R+CR BP FC) Page 25, Equaion 5 BTP2 =BN (100 + CR BP FC) CN (U + CP + FC) Page 43, Equaion 7 CN = BP R 100 R U BN 7

8 A Survey of Behavioral Finance, Barberi and Thaler (1) (x, p : y,q) =π(p)v(x) +π(q)v(y) (2) P i π i v(x i ) where v = xα if x 0 λ( x) α if x<0 and π i = w(p i ) w(pi ), w(p )= P γ (P γ +(1 P ) γ ) 1/γ (3) D +1 D = e g D+σ D ε +1 (4) (5) C +1 = e g C+σ C η +1 C µ µµ µ ε 0 1 w N, η 0 w 1 P (6) E 0 ρ C1 γ =0 1 γ " µc+1 γ (7) 1 = ρe R +1# C, i.i.d.over ime (8) R +1 = D +1 + P +1 = 1+P +1/D +1 D +1 P P /D D (9) r +1 = d +1 +con. d +1 d +con. (10) E π v[(1 w)r f,+1 + wr +1 1] P (11) E 0 ρ C1 γ 1 γ + b 0C γ ˆv(X +1 ) =0 (13) R +1 = P +1 + D +1 P P P (14) p d = E ρ d +1+j E (15) E 0 P =0 j=0 j=0 ρ C1 γ 1 γ + b 0C γ ṽ(x +1,z ) ρ r +1+j + E lim ρ j (p +j d +j )+con. j (16) r i r f = β i.1 (F 1 r f )+...+ β i,k (F K r f ) (17) r i, r f, = α i + β i,1 (F 1, r f, )+...+ β i,k (F K, r f, )+ε i, (18) R f = 1 ρ eγg C+0.5γ 2 σ 2 C (19) 1 = ρ 1+f e g D γg C +0.5(σD 2 +γ2 σc 2 2γσ Cσ D w) f (20) R +1 = D +1 + P +1 = 1+P +1/D +1 D +1 = 1+f P P /D D f e g D+σ D ε +1 8

9 CAIA Level II: Advanced Core Topic in Alernaive Invemen, Black, Chamber, Kazemi Chaper 16 (16.1) P repored (16.2) P repored (16.3) P rue (16.4) P rue = α + β 0 P rue = αp rue =(1/α) P repored = P repored 1 + β 1 P rue 1 + β 2 P rue α(1 α)p rue 1 + α(1 α) 2 P rue 2 + [(1 α)/α] P repored 1 +[(1/α) (P repored P repored 1 )] (16.5) R,repored β 0 R,rue + β 1 R 1,rue + β 2 R 2,rue + (16.6) P repored (16.7) P repored =(1 ρ)p rue =(1 ρ) P rue + ρp repored 1 + ρ P repored 1 (16.8) R,repored (1 ρ)r,rue + ρr 1,repored (16.9) R,rue =(R,repored ρr 1,repored )/(1 ρ) (16.10) ˆρ = corr(r,repored R 1,repored ) (16.11) ρ i,j = σ ij /(σ i σ j ) (16.12) R repored Chaper 21 Page 262 = α + β 1 R repored 1 + β 2 R repored β k R repored k + ε Y = S I E H where Y = yield, S = oal olar radiaion over he area per period, I = fracion of olar radiaion capured by he crop canopy, E = phooynheic efficiency of he crop (oal plan dry maer per uni of olar radiaion), H = harve index (fracion of oal dry maer ha i harveable) Managing Invemen Porfolio: A Dynamic Proce, Maginn, Tule, Pino, McLeavey Chaper 8 Page 523 TRCI = CR + RR + SR Page 553 RR n, =(R + R 1 + R R n )/n Page 554 rp n DD = i r, 0)] 2 n 1 Page 555 ARR rf SR = SD Page 556 ARR rf SR = DD 9

10 The Secular and Cyclic Deerminan of Capializaion Rae: The Role of Propery Fundamenal, Macroeconic Facor, and "Srucural Change," Chervachidze, Coello, Wheaon (1) Log(C j, )=a 0 + a 1 log(c j, 1 )+a 2 log(c j, 4 )+a 3 log(rri j, )+a 4 RTB + a 7 Q2 (1.1) RRI j, = RR j, /M RR j +a 8 Q3 + a 9 Q4 + a 10 D j (2) Log(C j, )=a 0 + a 1 log(c j, 1 )+a 2 log(c j, 4 )+a 3 log(rri j, )+a 4 RTB (2.1) DEBTFLOW = TNBL /GDP +a 5 SPREAD + a 6 DEBTFLOW + a 7 Q2 + a 8 Q3 + a 9 Q4 + a 10 D j (3) Log(C j, )=a 0 + a 1 log(c j, 1 )+a 2 log(c j, 4 )+a 3 log(rri j, )+a 4 RTB +a 5 SPREAD + a 6 DEBTFLOW + a 7 Q2 + a 8 Q3 + a 9 Q4 (4) Log(C j, )=a 0 + a 1 yearq + a 2 log(c j, 1 )+a 3 log(c j, 4 )+a 4 log(rri j, )+a 5 RT B +a 6 SPREAD + a 7 DEBTFLOW + a 7 Q2 + a 8 Q3 + a 9 Q4 + a 10 D j Analyi of Financial Time Serie, Tay Chaper 9 (9.1) r i = α i + β i1 f β im f m + i, =1,...,T,,...,k (9.2) r = α + βf +, =1,...,T (9.3) R i = α i 1 T + Fβ 0 i + E i (9.4) R = Gξ 0 + E (9.5) r i = α i + β i r m + i, i =1,...,k =1,...,T (9.11) Var(y i )=wiσ 0 r w i, i =1,...,k (9.12) Cov(y i,y j )=wiσ 0 r w j, i, j =1,...,k (9.13) kp P Var(r i )=r(σ r )= k P λ i = k Var(y i ) (9.14) ˆΣ r [ˆσ ij,r ]= 1 T 1 (9.15) ˆρ r = Ŝ 1 ˆΣ r Ŝ 1 TP =1(r r)(r r) 0, r = 1 T TP r =1 (9.16) r μ = βf + (9.17) Σr = Cov(r )=E[(r μ)(r μ) 0 ]=E[(βf + )(βf + ) 0 ]=ββ 0 + D (9.18) Cov(r, f )=E[(r μ)f]=βe(f 0 f)+e( 0 f)=β 0 (9.19) ˆβ [ ˆβ i ij ]= hpˆλ1 ê 1 pˆλ2 ê 2 pˆλm ê m (9.20) LR(m) = T 1 16 (2k +5) 23 m ³ ln ˆΣ r ln ˆβ ˆβ 0 + ˆD 10

11 Handbook of Fixed Income Securiie, Fabozzi Chaper 69 (69 4) Ae Allocaion P (w P w B ) R B (69 5) Securiy Selecion P w P (R P R B ) (69 12) α P k f P k αb k f B k = P α P k, f P k, P α B k, f B k, Chaper 70 (70 1) Ae Allocaion w P P µ w P w wb (TR B P w B TR B ) (70 2) Secor Managemen P w P (TR P TR B ) (70 3) Top-Level Expoure (w P w B ) TR B (70 4) Ae Allocaion w P P µ w P w wb (ER B P w B ER B ) (70 5) Secor Managemen P w P (ER P ER B ) (70 6) Top-Level Expoure (w P w B ) ER B Chaper 71 Page 1737 R P R B = P A = β (R P R B ) (R P R B )/T (1 + R P ) 1/T (1 + R B ) 1/T C = RP R B A P T =1 (RP R B ) P T =1 (RP R B ) 2 β = A + C(R P R B ) Inroducion o Credi Rik Modeling, 2nd ed., Bluhm, Overbeck, Wagner Chaper 6 Page 237 M n = M1 n 11

Quantitative Finance and Investments Advanced Formula Sheet. Fall 2013/Spring 2014

Quantitative Finance and Investments Advanced Formula Sheet. Fall 2013/Spring 2014 Quaniaive Finance and Invesmens Advanced Formula Shee Fall 013/Spring 014 ThisishesamesheeusedforFall013.Theonlychangeisonhiscoverpage. Morning and afernoon exam bookles will include a formula package

Διαβάστε περισσότερα

Quantitative Finance and Investments Advanced Formula Sheet. Fall 2016/Spring 2017

Quantitative Finance and Investments Advanced Formula Sheet. Fall 2016/Spring 2017 Quanave Fnance and Invesmens Advanced Formula Shee Fall 2016/Sprng 2017 Mornng and afernoon exam bookles wll nclude a formula package dencal o he one aached o hs sudy noe. The exam commee beleves ha by

Διαβάστε περισσότερα

Quantitative Finance and Investments Advanced Formula Sheet. Fall 2017/Spring 2018

Quantitative Finance and Investments Advanced Formula Sheet. Fall 2017/Spring 2018 Quanave Fnance and Invesmens Advanced Formula Shee Fall 2017/Sprng 2018 Mornng and afernoon exam bookles wll nclude a formula package dencal o he one aached o hs sudy noe. The exam commee beleves ha by

Διαβάστε περισσότερα

( ) ( t) ( 0) ( ) dw w. = = β. Then the solution of (1.1) is easily found to. wt = t+ t. We generalize this to the following nonlinear differential

( ) ( t) ( 0) ( ) dw w. = = β. Then the solution of (1.1) is easily found to. wt = t+ t. We generalize this to the following nonlinear differential Periodic oluion of van der Pol differenial equaion. by A. Arimoo Deparmen of Mahemaic Muahi Iniue of Technology Tokyo Japan in Seminar a Kiami Iniue of Technology January 8 9. Inroducion Le u conider a

Διαβάστε περισσότερα

= e 6t. = t 1 = t. 5 t 8L 1[ 1 = 3L 1 [ 1. L 1 [ π. = 3 π. = L 1 3s = L. = 3L 1 s t. = 3 cos(5t) sin(5t).

= e 6t. = t 1 = t. 5 t 8L 1[ 1 = 3L 1 [ 1. L 1 [ π. = 3 π. = L 1 3s = L. = 3L 1 s t. = 3 cos(5t) sin(5t). Worked Soluion 95 Chaper 25: The Invere Laplace Tranform 25 a From he able: L ] e 6 6 25 c L 2 ] ] L! + 25 e L 5 2 + 25] ] L 5 2 + 5 2 in(5) 252 a L 6 + 2] L 6 ( 2)] 6L ( 2)] 6e 2 252 c L 3 8 4] 3L ] 8L

Διαβάστε περισσότερα

Parts Manual. Trio Mobile Surgery Platform. Model 1033

Parts Manual. Trio Mobile Surgery Platform. Model 1033 Trio Mobile Surgery Platform Model 1033 Parts Manual For parts or technical assistance: Pour pièces de service ou assistance technique : Für Teile oder technische Unterstützung Anruf: Voor delen of technische

Διαβάστε περισσότερα

SOLUTIONS TO MATH38181 EXTREME VALUES AND FINANCIAL RISK EXAM

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

Διαβάστε περισσότερα

ITU-R P (2009/10)

ITU-R P (2009/10) ITU-R.45-4 (9/) % # GHz,!"# $$ # ITU-R.45-4.. (IR) (ITU-T/ITU-R/ISO/IEC).ITU-R http://www.tu.t/itu-r/go/patets/e. (http://www.tu.t/publ/r-rec/e ) () ( ) BO BR BS BT F M RA S RS SA SF SM SNG TF V.ITU-R

Διαβάστε περισσότερα

SOLUTIONS TO MATH38181 EXTREME VALUES AND FINANCIAL RISK EXAM

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

Διαβάστε περισσότερα

9.1 Introduction 9.2 Lags in the Error Term: Autocorrelation 9.3 Estimating an AR(1) Error Model 9.4 Testing for Autocorrelation 9.

9.1 Introduction 9.2 Lags in the Error Term: Autocorrelation 9.3 Estimating an AR(1) Error Model 9.4 Testing for Autocorrelation 9. 9.1 Inroducion 9.2 Lags in he Error Term: Auocorrelaion 9.3 Esimaing an AR(1) Error Model 9.4 Tesing for Auocorrelaion 9.5 An Inroducion o Forecasing: Auoregressive Models 9.6 Finie Disribued Lags 9.7

Διαβάστε περισσότερα

Quantitative Finance and Investment Core Formula Sheet. Spring 2017

Quantitative Finance and Investment Core Formula Sheet. Spring 2017 Quaniaive Finance and Invesmen Core Formula Shee Spring 7 Morning and afernoon exam bookles will include a formula package idenical o he one aached o his sudy noe. The exam commiee believe ha by providing

Διαβάστε περισσότερα

Quantitative Finance and Investments Core Formula Sheet. Spring 2016

Quantitative Finance and Investments Core Formula Sheet. Spring 2016 Quaniaive Finance and Invesmens Core Formula Shee Spring 6 Morning and afernoon exam bookles will include a formula package idenical o he one aached o his sudy noe. The exam commiee believe ha by providing

Διαβάστε περισσότερα

HONDA. Έτος κατασκευής

HONDA. Έτος κατασκευής Accord + Coupe IV 2.0 16V (CB3) F20A2-A3 81 110 01/90-09/93 0800-0175 11,00 2.0 16V (CB3) F20A6 66 90 01/90-09/93 0800-0175 11,00 2.0i 16V (CB3-CC9) F20A8 98 133 01/90-09/93 0802-9205M 237,40 2.0i 16V

Διαβάστε περισσότερα

Z = 1.2 X 1 + 1, 4 X 2 + 3, 3 X 3 + 0, 6 X 4 + 0, 999 X 5. X 1 X 2 X 2 X 3 X 4 X 4 X 5 X 4 X 4 Z = 0.717 X 1 + 0.847 X 2 + 3.107 X 3 + 0.420 X 4 + 0.998 X 5. X 5 X 4 Z = 6.56 X 1 + 3.26 X 2 + 6.72 X 3

Διαβάστε περισσότερα

Το άτομο του Υδρογόνου

Το άτομο του Υδρογόνου Το άτομο του Υδρογόνου Δυναμικό Coulomb Εξίσωση Schrödinger h e (, r, ) (, r, ) E (, r, ) m ψ θφ r ψ θφ = ψ θφ Συνθήκες ψ(, r θφ, ) = πεπερασμένη ψ( r ) = 0 ψ(, r θφ, ) =ψ(, r θφ+, ) π Επιτρεπτές ενέργειες

Διαβάστε περισσότερα

Νόµοςπεριοδικότητας του Moseley:Η χηµική συµπεριφορά (οι ιδιότητες) των στοιχείων είναι περιοδική συνάρτηση του ατοµικού τους αριθµού.

Νόµοςπεριοδικότητας του Moseley:Η χηµική συµπεριφορά (οι ιδιότητες) των στοιχείων είναι περιοδική συνάρτηση του ατοµικού τους αριθµού. Νόµοςπεριοδικότητας του Moseley:Η χηµική συµπεριφορά (οι ιδιότητες) των στοιχείων είναι περιοδική συνάρτηση του ατοµικού τους αριθµού. Περιοδικός πίνακας: α. Είναι µια ταξινόµηση των στοιχείων κατά αύξοντα

Διαβάστε περισσότερα

Homework 8 Model Solution Section

Homework 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 περισσότερα

(... )..!, ".. (! ) # - $ % % $ & % 2007

(... )..!, .. (! ) # - $ % % $ & % 2007 (! ), "! ( ) # $ % & % $ % 007 500 ' 67905:5394!33 : (! ) $, -, * +,'; ), -, *! ' - " #!, $ & % $ ( % %): /!, " ; - : - +', 007 5 ISBN 978-5-7596-0766-3 % % - $, $ &- % $ % %, * $ % - % % # $ $,, % % #-

Διαβάστε περισσότερα

r r t r r t t r t P s r t r P s r s r r rs tr t r r t s ss r P s s t r t t tr r r t t r t r r t t s r t rr t Ü rs t 3 r r r 3 rträ 3 röÿ r t

r r t r r t t r t P s r t r P s r s r r rs tr t r r t s ss r P s s t r t t tr r r t t r t r r t t s r t rr t Ü rs t 3 r r r 3 rträ 3 röÿ r t r t t r t ts r3 s r r t r r t t r t P s r t r P s r s r P s r 1 s r rs tr t r r t s ss r P s s t r t t tr r 2s s r t t r t r r t t s r t rr t Ü rs t 3 r t r 3 s3 Ü rs t 3 r r r 3 rträ 3 röÿ r t r r r rs

Διαβάστε περισσότερα

d dt S = (t)si d dt R = (t)i d dt I = (t)si (t)i

d dt S = (t)si d dt R = (t)i d dt I = (t)si (t)i d d S = ()SI d d I = ()SI ()I d d R = ()I d d S = ()SI μs + fi + hr d d I = + ()SI (μ + + f + ())I d d R = ()I (μ + h)r d d P(S,I,) = ()(S +1)(I 1)P(S +1, I 1, ) +()(I +1)P(S,I +1, ) (()SI + ()I)P(S,I,)

Διαβάστε περισσότερα

Advanced Subsidiary Unit 1: Understanding and Written Response

Advanced Subsidiary Unit 1: Understanding and Written Response Write your name here Surname Other names Edexcel GE entre Number andidate Number Greek dvanced Subsidiary Unit 1: Understanding and Written Response Thursday 16 May 2013 Morning Time: 2 hours 45 minutes

Διαβάστε περισσότερα

Errata (Includes critical corrections only for the 1 st & 2 nd reprint)

Errata (Includes critical corrections only for the 1 st & 2 nd reprint) Wedesday, May 5, 3 Erraa (Icludes criical correcios oly for he s & d repri) Advaced Egieerig Mahemaics, 7e Peer V O eil ISB: 978474 Page # Descripio 38 ie 4: chage "w v a v " "w v a v " 46 ie : chage "y

Διαβάστε περισσότερα

On the Galois Group of Linear Difference-Differential Equations

On the Galois Group of Linear Difference-Differential Equations On the Galois Group of Linear Difference-Differential Equations Ruyong Feng KLMM, Chinese Academy of Sciences, China Ruyong Feng (KLMM, CAS) Galois Group 1 / 19 Contents 1 Basic Notations and Concepts

Διαβάστε περισσότερα

m 1, m 2 F 12, F 21 F12 = F 21

m 1, m 2 F 12, F 21 F12 = F 21 m 1, m 2 F 12, F 21 F12 = F 21 r 1, r 2 r = r 1 r 2 = r 1 r 2 ê r = rê r F 12 = f(r)ê r F 21 = f(r)ê r f(r) f(r) < 0 f(r) > 0 m 1 r1 = f(r)ê r m 2 r2 = f(r)ê r r = r 1 r 2 r 1 = 1 m 1 f(r)ê r r 2 = 1 m

Διαβάστε περισσότερα

Ax = b. 7x = 21. x = 21 7 = 3.

Ax = b. 7x = 21. x = 21 7 = 3. 3 s st 3 r 3 t r 3 3 t s st t 3t s 3 3 r 3 3 st t t r 3 s t t r r r t st t rr 3t r t 3 3 rt3 3 t 3 3 r st 3 t 3 tr 3 r t3 t 3 s st t Ax = b. s t 3 t 3 3 r r t n r A tr 3 rr t 3 t n ts b 3 t t r r t x 3

Διαβάστε περισσότερα

Molekulare Ebene (biochemische Messungen) Zelluläre Ebene (Elektrophysiologie, Imaging-Verfahren) Netzwerk Ebene (Multielektrodensysteme) Areale (MRT, EEG...) Gene Neuronen Synaptische Kopplung kleine

Διαβάστε περισσότερα

Robust Segmentation of Focal Lesions on Multi-Sequence MRI in Multiple Sclerosis

Robust Segmentation of Focal Lesions on Multi-Sequence MRI in Multiple Sclerosis Robust Segmentation of Focal Lesions on Multi-Sequence MRI in Multiple Sclerosis Daniel García-Lorenzo To cite this version: Daniel García-Lorenzo. Robust Segmentation of Focal Lesions on Multi-Sequence

Διαβάστε περισσότερα

ANSWERSHEET (TOPIC = DIFFERENTIAL CALCULUS) COLLECTION #2. h 0 h h 0 h h 0 ( ) g k = g 0 + g 1 + g g 2009 =?

ANSWERSHEET (TOPIC = DIFFERENTIAL CALCULUS) COLLECTION #2. h 0 h h 0 h h 0 ( ) g k = g 0 + g 1 + g g 2009 =? Teko Classes IITJEE/AIEEE Maths by SUHAAG SIR, Bhopal, Ph (0755) 3 00 000 www.tekoclasses.com ANSWERSHEET (TOPIC DIFFERENTIAL CALCULUS) COLLECTION # Question Type A.Single Correct Type Q. (A) Sol least

Διαβάστε περισσότερα

Appendix A. Curvilinear coordinates. A.1 Lamé coefficients. Consider set of equations. ξ i = ξ i (x 1,x 2,x 3 ), i = 1,2,3

Appendix A. Curvilinear coordinates. A.1 Lamé coefficients. Consider set of equations. ξ i = ξ i (x 1,x 2,x 3 ), i = 1,2,3 Appendix A Curvilinear coordinates A. Lamé coefficients Consider set of equations ξ i = ξ i x,x 2,x 3, i =,2,3 where ξ,ξ 2,ξ 3 independent, single-valued and continuous x,x 2,x 3 : coordinates of point

Διαβάστε περισσότερα

C 1 D 1. AB = a, AD = b, AA1 = c. a, b, c : (1) AC 1 ; : (1) AB + BC + CC1, AC 1 = BC = AD, CC1 = AA 1, AC 1 = a + b + c. (2) BD 1 = BD + DD 1,

C 1 D 1. AB = a, AD = b, AA1 = c. a, b, c : (1) AC 1 ; : (1) AB + BC + CC1, AC 1 = BC = AD, CC1 = AA 1, AC 1 = a + b + c. (2) BD 1 = BD + DD 1, 1 1., BD 1 B 1 1 D 1, E F B 1 D 1. B = a, D = b, 1 = c. a, b, c : (1) 1 ; () BD 1 ; () F; D 1 F 1 (4) EF. : (1) B = D, D c b 1 E a B 1 1 = 1, B1 1 = B + B + 1, 1 = a + b + c. () BD 1 = BD + DD 1, BD =

Διαβάστε περισσότερα

Empirical best prediction under area-level Poisson mixed models

Empirical best prediction under area-level Poisson mixed models Noname manuscript No. (will be inserted by the editor Empirical best prediction under area-level Poisson mixed models Miguel Boubeta María José Lombardía Domingo Morales eceived: date / Accepted: date

Διαβάστε περισσότερα

I.I. Guseinov. Department of Physics, Faculty of Arts and Sciences, Onsekiz Mart University, Çanakkale, Turkey

I.I. Guseinov. Department of Physics, Faculty of Arts and Sciences, Onsekiz Mart University, Çanakkale, Turkey Epanion and one-range addiion heore for coplee orhonoral e of pinor wave funcion and Slaer pinor orbial of arbirary half-inegral pin in poiion oenu and four-dienional pace I.I. Gueinov Deparen of Phyic

Διαβάστε περισσότερα

Ι ΙΟΤΗΤΕΣ ΤΩΝ ΑΤΟΜΩΝ. Παππάς Χρήστος Επίκουρος Καθηγητής

Ι ΙΟΤΗΤΕΣ ΤΩΝ ΑΤΟΜΩΝ. Παππάς Χρήστος Επίκουρος Καθηγητής ΗΛΕΚΤΡΟΝΙΚΗ ΟΜΗ ΚΑΙ Ι ΙΟΤΗΤΕΣ ΤΩΝ ΑΤΟΜΩΝ Παππάς Χρήστος Επίκουρος Καθηγητής ΤΟ ΜΕΓΕΘΟΣ ΤΩΝ ΑΤΟΜΩΝ Ατομική ακτίνα (r) : ½ της απόστασης μεταξύ δύο ομοιοπυρηνικών ατόμων, ενωμένων με απλό ομοιοπολικό δεσμό.

Διαβάστε περισσότερα

Points de torsion des courbes elliptiques et équations diophantiennes

Points de torsion des courbes elliptiques et équations diophantiennes Points de torsion des courbes elliptiques et équations diophantiennes Nicolas Billerey To cite this version: Nicolas Billerey. Points de torsion des courbes elliptiques et équations diophantiennes. Mathématiques

Διαβάστε περισσότερα

m i N 1 F i = j i F ij + F x

m i N 1 F i = j i F ij + F x N m i i = 1,..., N m i Fi x N 1 F ij, j = 1, 2,... i 1, i + 1,..., N m i F i = j i F ij + F x i mi Fi j Fj i mj O P i = F i = j i F ij + F x i, i = 1,..., N P = i F i = N F ij + i j i N i F x i, i = 1,...,

Διαβάστε περισσότερα

#%" )*& ##+," $ -,!./" %#/%0! %,!

#% )*& ##+, $ -,!./ %#/%0! %,! -!"#$% -&!'"$ & #("$$, #%" )*& ##+," $ -,!./" %#/%0! %,! %!$"#" %!#0&!/" /+#0& 0.00.04. - 3 3,43 5 -, 4 $ $.. 04 ... 3. 6... 6.. #3 7 8... 6.. %9: 3 3 7....3. % 44 8... 6.4. 37; 3,, 443 8... 8.5. $; 3

Διαβάστε περισσότερα

Homework for 1/27 Due 2/5

Homework for 1/27 Due 2/5 Name: ID: Homework for /7 Due /5. [ 8-3] I Example D of Sectio 8.4, the pdf of the populatio distributio is + αx x f(x α) =, α, otherwise ad the method of momets estimate was foud to be ˆα = 3X (where

Διαβάστε περισσότερα

The ε-pseudospectrum of a Matrix

The ε-pseudospectrum of a Matrix The ε-pseudospectrum of a Matrix Feb 16, 2015 () The ε-pseudospectrum of a Matrix Feb 16, 2015 1 / 18 1 Preliminaries 2 Definitions 3 Basic Properties 4 Computation of Pseudospectrum of 2 2 5 Problems

Διαβάστε περισσότερα

ΝΟΜΟΣ ΤΗΣ ΠΕΡΙΟ ΙΚΟΤΗΤΑΣ : Οι ιδιότητες των χηµικών στοιχείων είναι περιοδική συνάρτηση του ατοµικού τους αριθµού.

ΝΟΜΟΣ ΤΗΣ ΠΕΡΙΟ ΙΚΟΤΗΤΑΣ : Οι ιδιότητες των χηµικών στοιχείων είναι περιοδική συνάρτηση του ατοµικού τους αριθµού. 1. Ο ΠΕΡΙΟ ΙΚΟΣ ΠΙΝΑΚΑΣ Οι άνθρωποι από την φύση τους θέλουν να πετυχαίνουν σπουδαία αποτελέσµατα καταναλώνοντας το λιγότερο δυνατό κόπο και χρόνο. Για το σκοπό αυτό προσπαθούν να οµαδοποιούν τα πράγµατα

Διαβάστε περισσότερα

Network Neutrality Debate and ISP Inter-Relations: Traffi c Exchange, Revenue Sharing, and Disconnection Threat

Network Neutrality Debate and ISP Inter-Relations: Traffi c Exchange, Revenue Sharing, and Disconnection Threat Network Neutrality Debate and ISP Inter-Relations: Traffi c Exchange, Revenue Sharing, and Disconnection Threat Pierre Coucheney, Patrick Maillé, runo Tuffin To cite this version: Pierre Coucheney, Patrick

Διαβάστε περισσότερα

Jeux d inondation dans les graphes

Jeux d inondation dans les graphes Jeux d inondation dans les graphes Aurélie Lagoutte To cite this version: Aurélie Lagoutte. Jeux d inondation dans les graphes. 2010. HAL Id: hal-00509488 https://hal.archives-ouvertes.fr/hal-00509488

Διαβάστε περισσότερα

Sur les articles de Henri Poincaré SUR LA DYNAMIQUE. Le texte fondateur de la Relativité en langage scientiþque moderne. par Anatoly A.

Sur les articles de Henri Poincaré SUR LA DYNAMIQUE. Le texte fondateur de la Relativité en langage scientiþque moderne. par Anatoly A. Sur les articles de Henri Poincaré SUR LA DYNAMIQUE DE L ÉLECTRON Le texte fondateur de la Relativité en langage scientiþque moderne par Anatoly A. LOGUNOV Directeur de l'institut de Physique des Hautes

Διαβάστε περισσότερα

Ηλεκτρονικοί Υπολογιστές IV

Ηλεκτρονικοί Υπολογιστές IV ΠΑΝΕΠΙΣΤΗΜΙΟ ΙΩΑΝΝΙΝΩΝ ΑΝΟΙΚΤΑ ΑΚΑΔΗΜΑΪΚΑ ΜΑΘΗΜΑΤΑ Ηλεκτρονικοί Υπολογιστές IV Δυναμική του χρέους και του ελλείμματος Διδάσκων: Επίκουρος Καθηγητής Αθανάσιος Σταυρακούδης Άδειες Χρήσης Το παρόν εκπαιδευτικό

Διαβάστε περισσότερα

ΠΕΡΙΟΔΙΚΟΣ ΠΙΝΑΚΑΣ ΣΤΟΙΧΕΙΩΝ

ΠΕΡΙΟΔΙΚΟΣ ΠΙΝΑΚΑΣ ΣΤΟΙΧΕΙΩΝ ΠΕΡΙΟΔΙΚΟΣ ΠΙΝΑΚΑΣ ΣΤΟΙΧΕΙΩΝ Περίοδοι περιοδικού πίνακα Ο περιοδικός πίνακας αποτελείται από 7 περιόδους. Ο αριθμός των στοιχείων που περιλαμβάνει κάθε περίοδος δεν είναι σταθερός, δηλ. η περιοδικότητα

Διαβάστε περισσότερα

Physique des réacteurs à eau lourde ou légère en cycle thorium : étude par simulation des performances de conversion et de sûreté

Physique des réacteurs à eau lourde ou légère en cycle thorium : étude par simulation des performances de conversion et de sûreté Physique des réacteurs à eau lourde ou légère en cycle thorium : étude par simulation des performances de conversion et de sûreté Alexis Nuttin To cite this version: Alexis Nuttin. Physique des réacteurs

Διαβάστε περισσότερα

Alterazioni del sistema cardiovascolare nel volo spaziale

Alterazioni del sistema cardiovascolare nel volo spaziale POLITECNICO DI TORINO Corso di Laurea in Ingegneria Aerospaziale Alterazioni del sistema cardiovascolare nel volo spaziale Relatore Ing. Stefania Scarsoglio Studente Marco Enea Anno accademico 2015 2016

Διαβάστε περισσότερα

Mesh Parameterization: Theory and Practice

Mesh Parameterization: Theory and Practice Mesh Parameterization: Theory and Practice Kai Hormann, Bruno Lévy, Alla Sheffer To cite this version: Kai Hormann, Bruno Lévy, Alla Sheffer. Mesh Parameterization: Theory and Practice. This document is

Διαβάστε περισσότερα

ΠΕΡΙΟΔΙΚΟ ΣΥΣΤΗΜΑ ΤΩΝ ΣΤΟΙΧΕΙΩΝ (1) Ηλία Σκαλτσά ΠΕ ο Γυμνάσιο Αγ. Παρασκευής

ΠΕΡΙΟΔΙΚΟ ΣΥΣΤΗΜΑ ΤΩΝ ΣΤΟΙΧΕΙΩΝ (1) Ηλία Σκαλτσά ΠΕ ο Γυμνάσιο Αγ. Παρασκευής ΠΕΡΙΟΔΙΚΟ ΣΥΣΤΗΜΑ ΤΩΝ ΣΤΟΙΧΕΙΩΝ (1) Ηλία Σκαλτσά ΠΕ04.01 5 ο Γυμνάσιο Αγ. Παρασκευής Όπως συμβαίνει στη φύση έτσι και ο άνθρωπος θέλει να πετυχαίνει σπουδαία αποτελέσματα καταναλώνοντας το λιγότερο δυνατό

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

: 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 περισσότερα

Υπόδειγµα Προεξόφλησης

Υπόδειγµα Προεξόφλησης Αρτίκης Γ. Παναγιώτης Υπόδειγµα Προεξόφλησης Μερισµάτων Γενικό Υπόδειγµα (Geeral Model) Ταµειακές ροές από αγορά µετοχών: Μερίσµατα κατά την διάρκεια κατοχής των µετοχών Μια αναµενόµενη τιµή στο τέλος

Διαβάστε περισσότερα

Dissertation for the degree philosophiae doctor (PhD) at the University of Bergen

Dissertation for the degree philosophiae doctor (PhD) at the University of Bergen Dissertation for the degree philosophiae doctor (PhD) at the University of Bergen Dissertation date: GF F GF F SLE GF F D Ĉ = C { } Ĉ \ D D D = {z : z < 1} f : D D D D = D D, D = D D f f : D D

Διαβάστε περισσότερα

P AND P. P : actual probability. P : risk neutral probability. Realtionship: mutual absolute continuity P P. For example:

P 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 περισσότερα

Teor imov r. ta matem. statist. Vip. 94, 2016, stor

Teor imov r. ta matem. statist. Vip. 94, 2016, stor eor imov r. ta matem. statist. Vip. 94, 6, stor. 93 5 Abstract. e article is devoted to models of financial markets wit stocastic volatility, wic is defined by a functional of Ornstein-Ulenbeck process

Διαβάστε περισσότερα

Vidyalankar. Vidyalankar S.E. Sem. III [BIOM] Applied Mathematics - III Prelim Question Paper Solution. 1 e = 1 1. f(t) =

Vidyalankar. Vidyalankar S.E. Sem. III [BIOM] Applied Mathematics - III Prelim Question Paper Solution. 1 e = 1 1. f(t) = . (a). (b). (c) f() L L e i e Vidyalakar S.E. Sem. III [BIOM] Applied Mahemaic - III Prelim Queio Paper Soluio L el e () i ( ) H( ) u e co y + 3 3y u e co y + 6 uy e i y 6y uyy e co y 6 u + u yy e co y

Διαβάστε περισσότερα

Radio détection des rayons cosmiques d ultra-haute énergie : mise en oeuvre et analyse des données d un réseau de stations autonomes.

Radio détection des rayons cosmiques d ultra-haute énergie : mise en oeuvre et analyse des données d un réseau de stations autonomes. Radio détection des rayons cosmiques d ultra-haute énergie : mise en oeuvre et analyse des données d un réseau de stations autonomes. Diego Torres Machado To cite this version: Diego Torres Machado. Radio

Διαβάστε περισσότερα

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 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 περισσότερα

u(x, y) =f(x, y) Ω=(0, 1) (0, 1)

u(x, y) =f(x, y) Ω=(0, 1) (0, 1) u(x, y) =f(x, y) Ω=(0, 1) (0, 1) u(x, y) =g(x, y) Γ=δΩ ={0, 1} {0, 1} Ω Ω Ω h Ω h h ˆ Ω ˆ u v = fv Ω u = f in Ω v V H 1 (Ω) V V h V h ψ 1,ψ 2,...,ψ N, ˆ ˆ u v = Ω Ω fv v V ˆ ˆ u v = Ω ˆ ˆ u ψ i = Ω Ω Ω

Διαβάστε περισσότερα

k k ΚΕΦΑΛΑΙΟ 1 G = (V, E) V E V V V G E G e = {v, u} E v u e v u G G V (G) E(G) n(g) = V (G) m(g) = E(G) G S V (G) S G N G (S) = {u V (G)\S v S : {v, u} E(G)} G v S v V (G) N G (v) = N G ({v}) x V (G)

Διαβάστε περισσότερα

Note: Please use the actual date you accessed this material in your citation.

Note: Please use the actual date you accessed this material in your citation. MIT OpeCueWae hp://cw.m.eu 6.13/ESD.13J Elecmagec a pplca, Fall 5 Pleae ue he llwg ca ma: Maku Zah, Ech Ippe, a Dav Sael, 6.13/ESD.13J Elecmagec a pplca, Fall 5. (Maachue Iue Techlgy: MIT OpeCueWae). hp://cw.m.eu

Διαβάστε περισσότερα

Appendix. The solution begins with Eq. (2.15) from the text, which we repeat here for 1, (A.1)

Appendix. The solution begins with Eq. (2.15) from the text, which we repeat here for 1, (A.1) Aenix Aenix A: The equaion o he sock rice. The soluion egins wih Eq..5 rom he ex, which we reea here or convenience as Eq.A.: [ [ E E X, A. c α where X u ε, α γ, an c α y AR. Take execaions o Eq. A. as

Διαβάστε περισσότερα

HW 3 Solutions 1. a) I use the auto.arima R function to search over models using AIC and decide on an ARMA(3,1)

HW 3 Solutions 1. a) I use the auto.arima R function to search over models using AIC and decide on an ARMA(3,1) HW 3 Solutions a) I use the autoarima R function to search over models using AIC and decide on an ARMA3,) b) I compare the ARMA3,) to ARMA,0) ARMA3,) does better in all three criteria c) The plot of the

Διαβάστε περισσότερα

P P Ó P. r r t r r r s 1. r r ó t t ó rr r rr r rí st s t s. Pr s t P r s rr. r t r s s s é 3 ñ

P P Ó P. r r t r r r s 1. r r ó t t ó rr r rr r rí st s t s. Pr s t P r s rr. r t r s s s é 3 ñ P P Ó P r r t r r r s 1 r r ó t t ó rr r rr r rí st s t s Pr s t P r s rr r t r s s s é 3 ñ í sé 3 ñ 3 é1 r P P Ó P str r r r t é t r r r s 1 t r P r s rr 1 1 s t r r ó s r s st rr t s r t s rr s r q s

Διαβάστε περισσότερα

Appendix A. Stability of the logistic semi-discrete model.

Appendix A. Stability of the logistic semi-discrete model. Ecological Archiv E89-7-A Elizava Pachpky, Rogr M. Nib, and William W. Murdoch. 8. Bwn dicr and coninuou: conumr-rourc dynamic wih ynchronizd rproducion. Ecology 89:8-88. Appndix A. Sabiliy of h logiic

Διαβάστε περισσότερα

Geodesic Equations for the Wormhole Metric

Geodesic Equations for the Wormhole Metric Geodesic Equations for the Wormhole Metric Dr R Herman Physics & Physical Oceanography, UNCW February 14, 2018 The Wormhole Metric Morris and Thorne wormhole metric: [M S Morris, K S Thorne, Wormholes

Διαβάστε περισσότερα

!"#!"!"# $ "# '()!* '+!*, -"*!" $ "#. /01 023 43 56789:3 4 ;8< = 7 >/? 44= 7 @ 90A 98BB8: ;4B0C BD :0 E D:84F3 B8: ;4BG H ;8

Διαβάστε περισσότερα

Solutions - Chapter 4

Solutions - Chapter 4 Solutions - Chapter Kevin S. Huang Problem.1 Unitary: Ût = 1 ī hĥt Û tût = 1 Neglect t term: 1 + hĥ ī t 1 īhĥt = 1 + hĥ ī t ī hĥt = 1 Ĥ = Ĥ Problem. Ût = lim 1 ī ] n hĥ1t 1 ī ] hĥt... 1 ī ] hĥnt 1 ī ]

Διαβάστε περισσότερα

α ]0,1[ of Trigonometric Fourier Series and its Conjugate

α ]0,1[ of Trigonometric Fourier Series and its Conjugate aqartvelo mecierebata erovuli aademii moambe 3 # 9 BULLETIN OF THE GEORGIN NTIONL CDEMY OF SCIENCES vol 3 o 9 Mahemaic Some pproimae Properie o he Cezàro Mea o Order ][ o Trigoomeric Fourier Serie ad i

Διαβάστε περισσότερα

Math221: HW# 1 solutions

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

Διαβάστε περισσότερα

The mass and anisotropy profiles of nearby galaxy clusters from the projected phase-space density

The mass and anisotropy profiles of nearby galaxy clusters from the projected phase-space density The mass and anisotropy profiles of nearby galaxy clusters from the projected phase-space density 5..29 Radek Wojtak Nicolaus Copernicus Astronomical Center collaboration: Ewa Łokas, Gary Mamon, Stefan

Διαβάστε περισσότερα

Solving an Air Conditioning System Problem in an Embodiment Design Context Using Constraint Satisfaction Techniques

Solving an Air Conditioning System Problem in an Embodiment Design Context Using Constraint Satisfaction Techniques Solving an Air Conditioning System Problem in an Embodiment Design Context Using Constraint Satisfaction Techniques Raphael Chenouard, Patrick Sébastian, Laurent Granvilliers To cite this version: Raphael

Διαβάστε περισσότερα

ΓΗ ΚΑΙ ΣΥΜΠΑΝ. Εικόνα 1. Φωτογραφία του γαλαξία μας (από αρχείο της NASA)

ΓΗ ΚΑΙ ΣΥΜΠΑΝ. Εικόνα 1. Φωτογραφία του γαλαξία μας (από αρχείο της NASA) ΓΗ ΚΑΙ ΣΥΜΠΑΝ Φύση του σύμπαντος Η γη είναι μία μονάδα μέσα στο ηλιακό μας σύστημα, το οποίο αποτελείται από τον ήλιο, τους πλανήτες μαζί με τους δορυφόρους τους, τους κομήτες, τα αστεροειδή και τους μετεωρίτες.

Διαβάστε περισσότερα

Lecture 12 Modulation and Sampling

Lecture 12 Modulation and Sampling EE 2 spring 2-22 Handou #25 Lecure 2 Modulaion and Sampling The Fourier ransform of he produc of wo signals Modulaion of a signal wih a sinusoid Sampling wih an impulse rain The sampling heorem 2 Convoluion

Διαβάστε περισσότερα

Ó³ Ÿ , º 2(131).. 105Ä ƒ. ± Ï,.. ÊÉ ±μ,.. Šμ ² ±μ,.. Œ Ì ²μ. Ñ Ò É ÉÊÉ Ö ÒÌ ² μ, Ê

Ó³ Ÿ , º 2(131).. 105Ä ƒ. ± Ï,.. ÊÉ ±μ,.. Šμ ² ±μ,.. Œ Ì ²μ. Ñ Ò É ÉÊÉ Ö ÒÌ ² μ, Ê Ó³ Ÿ. 2006.. 3, º 2(131).. 105Ä110 Š 537.311.5; 538.945 Œ ƒ ˆ ƒ Ÿ ˆŠ ˆ ƒ Ÿ ƒ ˆ œ ƒ Œ ƒ ˆ ˆ Š ˆ 4 ². ƒ. ± Ï,.. ÊÉ ±μ,.. Šμ ² ±μ,.. Œ Ì ²μ Ñ Ò É ÉÊÉ Ö ÒÌ ² μ, Ê ³ É É Ö μ ² ³ μ É ³ Í ² Ö Ê³ μ μ ³ É μ μ μ²ö

Διαβάστε περισσότερα

Vers un assistant à la preuve en langue naturelle

Vers un assistant à la preuve en langue naturelle Vers un assistant à la preuve en langue naturelle Thévenon Patrick To cite this version: Thévenon Patrick. Vers un assistant à la preuve en langue naturelle. Autre [cs.oh]. Université de Savoie, 2006.

Διαβάστε περισσότερα

d dx x 2 = 2x d dx x 3 = 3x 2 d dx x n = nx n 1

d dx x 2 = 2x d dx x 3 = 3x 2 d dx x n = nx n 1 d dx x 2 = 2x d dx x 3 = 3x 2 d dx x n = nx n1 x dx = 1 2 b2 1 2 a2 a b b x 2 dx = 1 a 3 b3 1 3 a3 b x n dx = 1 a n +1 bn +1 1 n +1 an +1 d dx d dx f (x) = 0 f (ax) = a f (ax) lim d dx f (ax) = lim 0 =

Διαβάστε περισσότερα

Approximation of the Lerch zeta-function

Approximation of the Lerch zeta-function Approximaion of he Lerch zea-funcion Ramūna Garunkši Deparmen of Mahemaic and Informaic Vilniu Univeriy Naugarduko 4 035 Vilniu Lihuania ramunagarunki@mafvul Abrac We conider uniform in parameer approximaion

Διαβάστε περισσότερα

Matrices and Determinants

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

Διαβάστε περισσότερα

ω = radians per sec, t = 3 sec

ω = radians per sec, t = 3 sec Secion. Linear and Angular Speed 7. From exercise, =. A= r A = ( 00 ) (. ) = 7,00 in 7. Since 7 is in quadran IV, he reference 7 8 7 angle is = =. In quadran IV, he cosine is posiive. Thus, 7 cos = cos

Διαβάστε περισσότερα

!!" #7 $39 %" (07) ..,..,.. $ 39. ) :. :, «(», «%», «%», «%» «%». & ,. ). & :..,. '.. ( () #*. );..,..'. + (# ).

!! #7 $39 % (07) ..,..,.. $ 39. ) :. :, «(», «%», «%», «%» «%». & ,. ). & :..,. '.. ( () #*. );..,..'. + (# ). 1 00 3 !!" 344#7 $39 %" 6181001 63(07) & : ' ( () #* ); ' + (# ) $ 39 ) : : 00 %" 6181001 63(07)!!" 344#7 «(» «%» «%» «%» «%» & ) 4 )&-%/0 +- «)» * «1» «1» «)» ) «(» «%» «%» + ) 30 «%» «%» )1+ / + : +3

Διαβάστε περισσότερα

!"!# ""$ %%"" %$" &" %" "!'! " #$!

!!# $ %% %$ & % !'!  #$! " "" %%"" %" &" %" " " " % ((((( ((( ((((( " %%%% & ) * ((( "* ( + ) (((( (, (() (((((* ( - )((((( )((((((& + )(((((((((( +. ) ) /(((( +( ),(, ((((((( +, 0 )/ (((((+ ++, ((((() & "( %%%%%%%%%%%%%%%%%%%(

Διαβάστε περισσότερα

F (x) = kx. F (x )dx. F = kx. U(x) = U(0) kx2

F (x) = kx. F (x )dx. F = kx. U(x) = U(0) kx2 F (x) = kx x k F = F (x) U(0) U(x) = x F = kx 0 F (x )dx U(x) = U(0) + 1 2 kx2 x U(0) = 0 U(x) = 1 2 kx2 U(x) x 0 = 0 x 1 U(x) U(0) + U (0) x + 1 2 U (0) x 2 U (0) = 0 U(x) U(0) + 1 2 U (0) x 2 U(0) =

Διαβάστε περισσότερα

A Probabilistic Numerical Method for Fully Non-linear Parabolic Partial Differential Equations

A Probabilistic Numerical Method for Fully Non-linear Parabolic Partial Differential Equations A Probabilistic Numerical Metod for Fully Non-linear Parabolic Partial Differential Equations Aras Faim To cite tis version: Aras Faim. A Probabilistic Numerical Metod for Fully Non-linear Parabolic Partial

Διαβάστε περισσότερα

rs r r â t át r st tíst Ó P ã t r r r â

rs r r â t át r st tíst Ó P ã t r r r â rs r r â t át r st tíst P Ó P ã t r r r â ã t r r P Ó P r sã rs r s t à r çã rs r st tíst r q s t r r t çã r r st tíst r t r ú r s r ú r â rs r r â t át r çã rs r st tíst 1 r r 1 ss rt q çã st tr sã

Διαβάστε περισσότερα

! " #! $ %&! '( #)!' * +#, " -! %&! "!! ! " #$ % # " &' &'... ()* ( +, # ' -. + &', - + &' / # ' -. + &' (, % # , 2**.

!  #! $ %&! '( #)!' * +#,  -! %&! !! !  #$ % #  &' &'... ()* ( +, # ' -. + &', - + &' / # ' -. + &' (, % # , 2**. ! " #! $ %&! '( #)!' * +#, " -! %&! "!!! " #$ % # " &' &'... ()* ( +, # ' -. + &', - + &' / 0123 4 # ' -. + &' (, % #. -5 0126, 2**., 2, + &' %., 0, $!, 3,. 7 8 ', $$, 9, # / 3:*,*2;

Διαβάστε περισσότερα

L. F avart. CLAS12 Workshop Genova th of Feb CLAS12 workshop Feb L.Favart p.1/28

L. F avart. CLAS12 Workshop Genova th of Feb CLAS12 workshop Feb L.Favart p.1/28 L. F avart I.I.H.E. Université Libre de Bruxelles H Collaboration HERA at DESY CLAS Workshop Genova - 4-8 th of Feb. 9 CLAS workshop Feb. 9 - L.Favart p./8 e p Integrated luminosity 96- + 3-7 (high energy)

Διαβάστε περισσότερα

Analiza reakcji wybranych modeli

Analiza reakcji wybranych modeli Bank i Kredy 43 (4), 202, 85 8 www.bankikredy.nbp.pl www.bankandcredi.nbp.pl Analiza reakcji wybranych modeli 86 - - - srice - - - per capia research and developmen dynamic sochasic general equilibrium

Διαβάστε περισσότερα

ES440/ES911: CFD. Chapter 5. Solution of Linear Equation Systems

ES440/ES911: CFD. Chapter 5. Solution of Linear Equation Systems ES440/ES911: CFD Chapter 5. Solution of Linear Equation Systems Dr Yongmann M. Chung http://www.eng.warwick.ac.uk/staff/ymc/es440.html Y.M.Chung@warwick.ac.uk School of Engineering & Centre for Scientific

Διαβάστε περισσότερα

Approximation of distance between locations on earth given by latitude and longitude

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

Διαβάστε περισσότερα

Answer sheet: Third Midterm for Math 2339

Answer sheet: Third Midterm for Math 2339 Answer sheet: Third Midterm for Math 339 November 3, Problem. Calculate the iterated integrals (Simplify as much as possible) (a) e sin(x) dydx y e sin(x) dydx y sin(x) ln y ( cos(x)) ye y dx sin(x)(lne

Διαβάστε περισσότερα

STANDARD LED LAMPS (ROUND TYPES)

STANDARD LED LAMPS (ROUND TYPES) Package 3 3 3 1.0 Lead High 3.4 Part No. Chip Material/Emitted Color Wave Length p Lens Appearance Absolute Maximum Ratings Pd (mw) If Electro-optical Data (At ma) Vf (V) Iv (mcd) Typ Max Typ. BL-B4541

Διαβάστε περισσότερα

6.4 Superposition of Linear Plane Progressive Waves

6.4 Superposition of Linear Plane Progressive Waves .0 - Marine Hydrodynamics, Spring 005 Lecture.0 - Marine Hydrodynamics Lecture 6.4 Superposition of Linear Plane Progressive Waves. Oblique Plane Waves z v k k k z v k = ( k, k z ) θ (Looking up the y-ais

Διαβάστε περισσότερα

τροχιακά Η στιβάδα καθορίζεται από τον κύριο κβαντικό αριθµό (n) Η υποστιβάδα καθορίζεται από τους δύο πρώτους κβαντικούς αριθµούς (n, l)

τροχιακά Η στιβάδα καθορίζεται από τον κύριο κβαντικό αριθµό (n) Η υποστιβάδα καθορίζεται από τους δύο πρώτους κβαντικούς αριθµούς (n, l) ΑΤΟΜΙΚΑ ΤΡΟΧΙΑΚΑ Σχέση κβαντικών αριθµών µε στιβάδες υποστιβάδες - τροχιακά Η στιβάδα καθορίζεται από τον κύριο κβαντικό αριθµό (n) Η υποστιβάδα καθορίζεται από τους δύο πρώτους κβαντικούς αριθµούς (n,

Διαβάστε περισσότερα

ο ο 3 α. 3"* > ω > d καΐ 'Ενορία όλις ή Χώρί ^ 3 < KN < ^ < 13 > ο_ Μ ^~~ > > > > > Ο to X Η > ο_ ο Ο,2 Σχέδι Γλεγμα Ο Σ Ο Ζ < o w *< Χ χ Χ Χ < < < Ο

ο ο 3 α. 3* > ω > d καΐ 'Ενορία όλις ή Χώρί ^ 3 < KN < ^ < 13 > ο_ Μ ^~~ > > > > > Ο to X Η > ο_ ο Ο,2 Σχέδι Γλεγμα Ο Σ Ο Ζ < o w *< Χ χ Χ Χ < < < Ο 18 ρ * -sf. NO 1 D... 1: - ( ΰ ΐ - ι- *- 2 - UN _ ί=. r t ' \0 y «. _,2. "* co Ι». =; F S " 5 D 0 g H ', ( co* 5. «ΰ ' δ". o θ * * "ΰ 2 Ι o * "- 1 W co o -o1= to»g ι. *ΰ * Ε fc ΰ Ι.. L j to. Ι Q_ " 'T

Διαβάστε περισσότερα

k k ΚΕΦΑΛΑΙΟ 1 G = (V, E) V E V V V G E G e = {v, u} E v u e v u G G V (G) E(G) n(g) = V (G) m(g) = E(G) G S V (G) S G N G (S) = {u V (G)\S v S : {v, u} E(G)} G v S v V (G) N G (v) = N G ({v}) x V (G)

Διαβάστε περισσότερα

TeSys contactors a.c. coils for 3-pole contactors LC1-D

TeSys contactors a.c. coils for 3-pole contactors LC1-D References a.c. coils for 3-pole contactors LC1-D Control circuit voltage Average resistance Inductance of Reference (1) Weight Uc at 0 C ± 10 % closed circuit For 3-pole " contactors LC1-D09...D38 and

Διαβάστε περισσότερα

.1. 8,5. µ, (=,, ) . Ρ( )... Ρ( ).

.1. 8,5. µ, (=,, ) . Ρ( )... Ρ( ). ΡΧΗ 1Η Ε ε Γ Α Ο ΗΡ Ε Ε Ε Ε Η Ε Ο Ε Ο Ε Η 14 Ο Ο 2001 Ε Ε Ο Ε Ο Η Ε Η εε : Η Ο ΧΕ Η Ο Ο Ε εά : Ε (6) Ε Α 1ο Α.1. π µ µ ά : Ρ ( ) = Ρ ( ) Ρ ( ). 8,5 Α.2. µ π µπ µ π µ µ, (=,, ) : Ρ ( )... 1 Ρ( ) 2 Ρ( )...

Διαβάστε περισσότερα

Mantel & Haenzel (1959) Mantel-Haenszel

Mantel & Haenzel (1959) Mantel-Haenszel Mantel-Haenszel 2008 6 12 1 / 39 1 (, (, (,,, pp719 730 2 2 2 3 1 4 pp730 746 2 2, i j 3 / 39 Mantel & Haenzel (1959 Mantel N, Haenszel W Statistical aspects of the analysis of data from retrospective

Διαβάστε περισσότερα

Vol. 37 ( 2017 ) No. 3. J. of Math. (PRC) : A : (2017) k=1. ,, f. f + u = f φ, x 1. x n : ( ).

Vol. 37 ( 2017 ) No. 3. J. of Math. (PRC) : A : (2017) k=1. ,, f. f + u = f φ, x 1. x n : ( ). Vol. 37 ( 2017 ) No. 3 J. of Math. (PRC) R N - R N - 1, 2 (1., 100029) (2., 430072) : R N., R N, R N -. : ; ; R N ; MR(2010) : 58K40 : O192 : A : 0255-7797(2017)03-0467-07 1. [6], Mather f : (R n, 0) R

Διαβάστε περισσότερα

The martingale pricing method for pricing fluctuation concerning stock models of callable bonds with random parameters

The martingale pricing method for pricing fluctuation concerning stock models of callable bonds with random parameters 32 Vol 32 2 Journal of Harbin Engineering Univerity Jan 2 doi 3969 /j in 6-743 2 23 5 2 F83 9 A 6-743 2-24-5 he martingale pricing method for pricing fluctuation concerning tock model of callable bond

Διαβάστε περισσότερα

( ) ( ) ( ) Fourier series. ; m is an integer. r(t) is periodic (T>0), r(t+t) = r(t), t Fundamental period T 0 = smallest T. Fundamental frequency ω

( ) ( ) ( ) Fourier series. ; m is an integer. r(t) is periodic (T>0), r(t+t) = r(t), t Fundamental period T 0 = smallest T. Fundamental frequency ω Fourier series e jm when m d when m ; m is an ineger. jm jm jm jm e d e e e jm jm jm jm r( is periodi (>, r(+ r(, Fundamenal period smalles Fundamenal frequeny r ( + r ( is periodi hen M M e j M, e j,

Διαβάστε περισσότερα