LIBORマーケット・モデルのインプリメンテーションについて―本邦の金利派生商品データを用いた具体例を基に―

Similar documents
IMES DISCUSSION PAPER SERIES LIBOR Discussion Paper No J- -J-2 INSTITUTE FOR MONETARY AND ECONOMIC STUDIES BANK OF JAPAN

○松本委員

y = x x R = 0. 9, R = σ $ = y x w = x y x x w = x y α ε = + β + x x x y α ε = + β + γ x + x x x x' = / x y' = y/ x y' =

N cos s s cos ψ e e e e 3 3 e e 3 e 3 e

(1.2) T D = 0 T = D = 30 kn 1.2 (1.4) 2F W = 0 F = W/2 = 300 kn/2 = 150 kn 1.3 (1.9) R = W 1 + W 2 = = 1100 N. (1.9) W 2 b W 1 a = 0

koji07-01.dvi

all.dvi

Part () () Γ Part ,

meiji_resume_1.PDF


1 I 1.1 ± e = = - = C C MKSA [m], [Kg] [s] [A] 1C 1A 1 MKSA 1C 1C +q q +q q 1

デフォルト相関係数のインプライド推計( )

日本内科学会雑誌第102巻第4号

B

「国債の金利推定モデルに関する研究会」報告書


1 (Berry,1975) 2-6 p (S πr 2 )p πr 2 p 2πRγ p p = 2γ R (2.5).1-1 : : : : ( ).2 α, β α, β () X S = X X α X β (.1) 1 2

5 c P 5 kn n t π (.5 P 7 MP π (.5 n t n cos π. MP 6 4 t sin π 6 cos π 6.7 MP 4 P P N i i i i N i j F j ii N i i ii F j i i N ii li i F j i ij li i i i

18 I ( ) (1) I-1,I-2,I-3 (2) (3) I-1 ( ) (100 ) θ ϕ θ ϕ m m l l θ ϕ θ ϕ 2 g (1) (2) 0 (3) θ ϕ (4) (3) θ(t) = A 1 cos(ω 1 t + α 1 ) + A 2 cos(ω 2 t + α

II III II 1 III ( ) [2] [3] [1] 1 1:

1. 2 P 2 (x, y) 2 x y (0, 0) R 2 = {(x, y) x, y R} x, y R P = (x, y) O = (0, 0) OP ( ) OP x x, y y ( ) x v = y ( ) x 2 1 v = P = (x, y) y ( x y ) 2 (x


微分積分 サンプルページ この本の定価 判型などは, 以下の URL からご覧いただけます. このサンプルページの内容は, 初版 1 刷発行時のものです.

[1] convention Minkovski i Polchinski [2] 1 Clifford Spin 1 2 Euclid Clifford 2 3 Euclid Spin 6 4 Euclid Pin Clifford Spin 10 A 12 B 17 1 Cliffo

zz + 3i(z z) + 5 = 0 + i z + i = z 2i z z z y zz + 3i (z z) + 5 = 0 (z 3i) (z + 3i) = 9 5 = 4 z 3i = 2 (3i) zz i (z z) + 1 = a 2 {

.5 z = a + b + c n.6 = a sin t y = b cos t dy d a e e b e + e c e e e + e 3 s36 3 a + y = a, b > b 3 s363.7 y = + 3 y = + 3 s364.8 cos a 3 s365.9 y =,

( ) Loewner SLE 13 February

Gmech08.dvi

W u = u(x, t) u tt = a 2 u xx, a > 0 (1) D := {(x, t) : 0 x l, t 0} u (0, t) = 0, u (l, t) = 0, t 0 (2)


64 3 g=9.85 m/s 2 g=9.791 m/s 2 36, km ( ) 1 () 2 () m/s : : a) b) kg/m kg/m k

医系の統計入門第 2 版 サンプルページ この本の定価 判型などは, 以下の URL からご覧いただけます. このサンプルページの内容は, 第 2 版 1 刷発行時のものです.

1

Note.tex 2008/09/19( )

I A A441 : April 15, 2013 Version : 1.1 I Kawahira, Tomoki TA (Shigehiro, Yoshida )

t χ 2 F Q t χ 2 F 1 2 µ, σ 2 N(µ, σ 2 ) f(x µ, σ 2 ) = 1 ( exp (x ) µ)2 2πσ 2 2σ 2 0, N(0, 1) (100 α) z(α) t χ 2 *1 2.1 t (i)x N(µ, σ 2 ) x µ σ N(0, 1

s = 1.15 (s = 1.07), R = 0.786, R = 0.679, DW =.03 5 Y = 0.3 (0.095) (.708) X, R = 0.786, R = 0.679, s = 1.07, DW =.03, t û Y = 0.3 (3.163) + 0


66 σ σ (8.1) σ = 0 0 σd = 0 (8.2) (8.2) (8.1) E ρ d = 0... d = 0 (8.3) d 1 NN K K 8.1 d σd σd M = σd = E 2 d (8.4) ρ 2 d = I M = EI ρ 1 ρ = M EI ρ EI

1 1.1 ( ). z = a + bi, a, b R 0 a, b 0 a 2 + b 2 0 z = a + bi = ( ) a 2 + b 2 a a 2 + b + b 2 a 2 + b i 2 r = a 2 + b 2 θ cos θ = a a 2 + b 2, sin θ =

φ 4 Minimal subtraction scheme 2-loop ε 2008 (University of Tokyo) (Atsuo Kuniba) version 21/Apr/ Formulas Γ( n + ɛ) = ( 1)n (1 n! ɛ + ψ(n + 1)

2 G(k) e ikx = (ik) n x n n! n=0 (k ) ( ) X n = ( i) n n k n G(k) k=0 F (k) ln G(k) = ln e ikx n κ n F (k) = F (k) (ik) n n= n! κ n κ n = ( i) n n k n

SO(2)


1 1 sin cos P (primary) S (secondly) 2 P S A sin(ω2πt + α) A ω 1 ω α V T m T m 1 100Hz m 2 36km 500Hz. 36km 1

untitled

‚åŁÎ“·„´Šš‡ðŠp‡¢‡½‹âfi`fiI…A…‰…S…−…Y…•‡ÌMarkovŸA“½fiI›ð’Í


TOP URL 1

Microsoft Word - 11問題表紙(選択).docx

TOP URL 1

() [REQ] 0m 0 m/s () [REQ] (3) [POS] 4.3(3) ()() () ) m/s 4. ) 4. AMEDAS

tnbp59-21_Web:P2/ky132379509610002944

4. ϵ(ν, T ) = c 4 u(ν, T ) ϵ(ν, T ) T ν π4 Planck dx = 0 e x 1 15 U(T ) x 3 U(T ) = σt 4 Stefan-Boltzmann σ 2π5 k 4 15c 2 h 3 = W m 2 K 4 5.

量子力学 問題

日本内科学会雑誌第98巻第4号

日本内科学会雑誌第97巻第7号

A = A x x + A y y + A, B = B x x + B y y + B, C = C x x + C y y + C..6 x y A B C = A x x + A y y + A B x B y B C x C y C { B = A x x + A y y + A y B B

春期講座 ~ 極限 1 1, 1 2, 1 3, 1 4,, 1 n, n n {a n } n a n α {a n } α {a n } α lim n an = α n a n α α {a n } {a n } {a n } 1. a n = 2 n {a n } 2, 4, 8, 16,

,,,17,,, ( ),, E Q [S T F t ] < S t, t [, T ],,,,,,,,

( ) ) ) ) 5) 1 J = σe 2 6) ) 9) 1955 Statistical-Mechanical Theory of Irreversible Processes )


液晶の物理1:連続体理論(弾性,粘性)

,, Andrej Gendiar (Density Matrix Renormalization Group, DMRG) 1 10 S.R. White [1, 2] 2 DMRG ( ) [3, 2] DMRG Baxter [4, 5] 2 Ising 2 1 Ising 1 1 Ising

³ÎΨÏÀ

ρ ( ) sgv + ρwgv γ sv + γ wv γ s + γ w e e γ ρ g s s γ s ( ) + γ w( ) Vs + V Vs + V + e + e + e γ γ sa γ e e n( ) + e γ γ s ( n) + γ wn γ s, γ w γ γ +

2000年度『数学展望 I』講義録

.2 ρ dv dt = ρk grad p + 3 η grad (divv) + η 2 v.3 divh = 0, rote + c H t = 0 dive = ρ, H = 0, E = ρ, roth c E t = c ρv E + H c t = 0 H c E t = c ρv T

1.500 m X Y m m m m m m m m m m m m N/ N/ ( ) qa N/ N/ 2 2

N/m f x x L dl U 1 du = T ds pdv + fdl (2.1)

D = [a, b] [c, d] D ij P ij (ξ ij, η ij ) f S(f,, {P ij }) S(f,, {P ij }) = = k m i=1 j=1 m n f(ξ ij, η ij )(x i x i 1 )(y j y j 1 ) = i=1 j

1. 4cm 16 cm 4cm 20cm 18 cm L λ(x)=ax [kg/m] A x 4cm A 4cm 12 cm h h Y 0 a G 0.38h a b x r(x) x y = 1 h 0.38h G b h X x r(x) 1 S(x) = πr(x) 2 a,b, h,π

II (Percolation) ( 3-4 ) 1. [ ],,,,,,,. 2. [ ],.. 3. [ ],. 4. [ ] [ ] G. Grimmett Percolation Springer-Verlag New-York [ ] 3


29

2015/4/13 10: C C C C John C. Hull,, Steven E. Shreve, (1), Peter E. Kloeden, Eckhard Platen Num

6 6.1 L r p hl = r p (6.1) 1, 2, 3 r =(x, y, z )=(r 1,r 2,r 3 ), p =(p x,p y,p z )=(p 1,p 2,p 3 ) (6.2) hl i = jk ɛ ijk r j p k (6.3) ɛ ijk Levi Civit

2 2 1?? 2 1 1, 2 1, 2 1, 2, 3,... 1, 2 1, 3? , 2 2, 3? k, l m, n k, l m, n kn > ml...? 2 m, n n m

Transcription:

LIBOR LIBOR LIBOR E-mal: shyama@po.msec.co.p

LIBORLIBORLondon InerBank Offered Rae BGMBrace, Gaarek and Musela LIBOR LIBOR BlackBlack and Scholes LIBOR LIBORLIBOR LIBOR LIBOR LIBOR LIBOR Brace, Gaarek and MuselaHJMHeah, Jarrow and Moron BGMJamshdan BGM

LIBORLIBOR LIBOR LIBOR LIBOR LIBOR LIBOR

LIBOR LIBOR LIBOR LIBOR {T =,, M} δ = T + T, =,, M LIBORLIBOR L δ =L T δ L T T + δ L T T D, 0 T LIBORD =+δ L D + D D + L =, T, δ D + T L T D + L δ L T T+ D D + D + = D, +δ L

LIBOR D + = D +δ L = D +δ L +δ L = = D m Π, = m +δ L m D m LIBOR L LIBORT + D + LIBOR L dl = σ dw +, L W + T + D + Mσ M σ σ LIBOR

LIBOR L KLIBORL 0 C L 0, K, γ N. LIBOR C L 0, K, γ = δ D 0[L 0Nd KNd ] d L0 log + γ = K γ, d L 0 log = K γ γ γ = T 0 σ d LIBOR C L 0, K, σ = δ D 0[L 0N d KN d ] d L0 log + K = σ T σ T, d L0 log = K T σ σ T. γ σ T LIBOR γ γ = δ σ T + +δ σ T,

γ = σ T, γ LIBOR LIBOR LIBOR LIBOR LIBOR LIBOR W + W W + W δ L dw = dw + ρσ d, +δ L ρmρ, k k T dw T + dw + d Pelsser ρ

dl L δ L = σ d dw ρ σ + σ, L, + δ + T L T + d L L LIBOR LIBOR LIBOR LIBOR LIBORL,, L M T M+ L dl L M M+ = dw ρ d+, =,,, σ σ = + + L δ = M δ L σ M T, LIBORL M T M+ D M+

dl M = σ M dw M+, L M < Md =M σ M L M + L M = σ M W M+ + W M+, L M L M + =L M +L M σ M W M+ + W M+. W M+ M W M+ + W M+ N M 0,ρ, ρn M L + < M M δ L L + = L σ L ρ + δ L = +, σ + σ L W M + + W M+, δ σ L L + + T L log L M δ L, ρ σ M+ dlog L = σ σ d + dw = + + δ L σ, εw M+ + W M+ ε Kloeden and Plaen

M δ L L + = L exp{ σ ρ, + δ L + σ W M+ = + + W M+ }. σ σ M= 4 LIBOR =0.5δ =0.5σ =0.5LIBOR + = 0 + 0.5 W M+ 0+0.5 W M+ 0L 0=5%L 0+0.5, =,, 4 L 0.5L 0.5L 3 0.5L 4 0.5L.0 L 3.0 L 4.0 LIBOR LIBORLIBOR T 0 L 0 T 0,, L 4 T 0 L T L T L 3 T 3 L 4 T 4 T,, T 4 LIBOR T = 0.0 T = 0.5 T =.0 T =.5 T =.0 L L L L L W

T = 0.0 T = 0.5 T =.0 T =.5 T =.0 D D D D D LIBOR LIBOR LIBOR LIBOR M M M= 60 T = 0.0 T = 0.5 T =.0 L L L L M L M L M L T L T L T L M T L T L T L M T L T L M T LIBORHJM L M T 0

LIBOR K=5.0% L 4 T 4 =5.7% T 5 C T 5 =max{l 4 T 4 K, 0} T 5 T 5 N T 0 C CAPLET 4 T 0 C T 5 N C 4 CAPLET T 0 =δd 5 T 0 C T 5, N = δ D 5 T 0 K=5.0% LIBOR C T =max{l T K, 0}, =,, 4 D 5 T 5 C T C T =C T /D 5 T C T 3 =C T 3 /D 5 T 3 C T 4 =C T 4 /D 5 T 4 C T 5 =C T 5 /D 5 T 5 =C T 5 D T = T 5 D T D T D T CT CT CT CT T T T T T

N T 5 T 0 D 5 T 0 T 0 N C T T 0 C CAP T Y 0 N Y T 0 =δd 5 T 0 {C T +C T 3 +C T 4 +C T 5 }, C CAP N = LIBOR ρm M MM LIBORd d M Z Rebonao d dmm db T M+ D M+ Mρ T 5 T 5 LIBOR

dw M+ dw M+ =ρd, BB BdZ BdZ =BdZ dz B =BB d, ρ B =BB ρ, BdZ ρm dmθ q, q =,, db qb q b q q cosθ = q snθ = q = snθ, q = d., q =,, d d = b b b b B = b M b M = cosθ cosθ cosθ M snθ snθ snθ M, d =3 b b B = b M b b b M b b b 3 3 M3 cosθ cosθ = cosθ M cosθ cosθ cosθ M snθ snθ snθ M snθ snθ snθ M snθ snθ snθ M, BB Z W M+ T M+ D M+

B d σ q = σ b q, =,, M, q =,, dz q Z q T M+ D M+ d σ q d σ B σ q = σ b q BB ρ LIBOR ρ B LIBORW M+ ρ } exp{ = = + = = + + + = + d q q q q d q q M d q q q Z Z L L L L σ σ δ σ σ δ, dz d L L L dl B M B B σ σ δ δ σ + + = + =. dw d L L BdZ d BB L L dz B d B L L B L dl M + + + + + = + + = M + = σ ρσ δ δ σ σ σ δ δ σ σ σ δ δ σ M + = M + =, ρ, =α + α exp{ β β max T,T. T T }, α=0.3β = 0.β = 0.005,

ρρ B ρ B Bd =3 ρ B ρ ρ B θ θ B B, =,, 3 B B B d =3

B B B LIBORLIBOR Jamshdan LIBOR Rebonao LIBOR T T n S,n LIBORS,n n n S, n δ D + = δ L D +. = = D + D + L δ S,n L n T T + T n T n+ δ n S,n L n δ n S,n

S, n n = δ D + = n = = D D D D+ δ D δ D n + +. + S,n D D n+ S, n = n. δ D + = n P,n δ D +, = P,n LIBOR P,n S,n ds,n = σ,n dw,n, S,n σ,n T T n T S,n W,n P,n S,n K PS, n 0 PS, n Γ S, n 0, K, Γ = P [ S 0 N d KN d ],, n d T =, n, n 0, n S log =, n, n 0 + K Γ, n Γ, n σ d log, S n, d S log = 0 K Γ, n, n Γ, n σ,n

LIBOR T T n T σ,n Γ,n Γ,n = T σ,n, LIBOR LIBOR LIBOR LIBORLIBOR LIBOR Rebonao Brgo and Mercuro Brgo and MercuroRebonaoHull and Whe Rebonao Rebonao

T T n T σ,n LIBOR σ,n n n k σ, n w, n 0 w, n 0 L 0 Lk0 ρ k l l k T, l S δ σ, n0 = + k + l σ = =, w, n 0 = n δ D k= k + δ D 0 k+ 0, ρ,k k D LIBOR σ ρ,k LIBOR LIBOR LIBOR LIBOR

LIBOR LIBOR YYY M YYYYYM nymn 0.5 Y LIBOR LIBOR LIBOR

M M LIBOR M LIBOR YKM LIBOR log [L + /L ] L + L + L + L log = L L L L + /L = L + L /L x,, x N x SK 3 4 N x N x, x x S = K = N = / = / N N N N N

YYYYM

- Normal Dsrbuon Normal Dsrbuon Normal Dsrbuon Normal Dsrbuon QQQuanleQuanlenkx k,n x k,n, N n k+/n+n

LIBOR LIBOR LIBOR LIBOR LIBOR LIBOR LIBOR LIBOR

LIBOR LIBOR LIBOR MID MMID MIDTelerae BIDASK YM M

σ CAP σ CAPLET C δ D 0C L 0,K, σ CAP = δ D 0C L 0, K, σ CAPLET. = = = δ D 0C L 0,K, σ CAP =δ D 0C L 0, K, σ CAPLET, σ CAP = σ CAPLET = δ D 0C L 0,K, σ CAP +δ D 0C L 0, K, σ CAP =δ D 0C L 0,K, σ CAPLET +δ D 0C L 0, K, σ CAPLET,

σ CAPLET σ CAPLET γ γ = T σ CAPLET, γ LIBOR LIBORσ γ = δ σ T ++δ σ T σ γ LIBORσ ρ,k LIBORσ ρ,k LIBOR LIBOR L 0,, L M 0D 0S,n 0 γ = δ σ T ++δ σ T LIBOR ρ,k :, k =,, M σ T,, σ T, =,, M σ : MM+/ Brgo and MercuroLIBOR LIBOR

0 T T < T T T < T M < M T M L σ L σ σ L σ σ σ L M σ M σ M σ M σ M M σ LIBORv 0 T < T < L T v σ T T L L v σ v σ v σ v σ v σ L M v M σ M v M σ M v M σ M T M < T M v M σ LIBORσ v LIBOR σ σ M v v T σ CAPLET LIBOR σ

T σ CAPLET = δ σ T σ CAPLET = δ σ + δ σ T σ CAPLET = δ σ + δ σ + + δ σ, σ σ v T σ CAPLET = v δ σ T σ CAPLET = v δ σ + δ σ T σ CAPLET = v δ σ + δ σ + + δ σ, YYv, v LIBORT σ σ T =at +de bt +cabcd. LIBORv

0 T < T < T T T T M < T M L v σt ~ L v σt ~ v σt ~ L v σt ~ v σt ~ v σt ~ L M v M σt ~ M v M σt ~ M v M σt ~ M v M σt ~ M = 0 a bcd σ T σ, n = { w 0 wk 0 L 0 Lk0 ρ, k σ σ d k }. S 0 0 T, n = + k= + n n N N T T T T σ σ d k σ l σ k l. 0 l = N N N

LIBOR δ = 0.5LIBOR Md = 3 θ,, θ 0 θ,, θ 0 =,, 0 γ = δ σ T = v = T δ σ CAPLET σ + + δ σ T + + δ σ, v Bloomberg

v = T δ σ + + δ σ CAPLET σ. σ,,σ 0 θ,,θ 0 θ,,θ 0 σ,, σ 0 θ,,θ 0 θ,, θ 0 π/v σ, v σ σ v v v σ LIBOR B v

B B B γ = = = T T σ 0 d T v 0 σ T CAPLET σ. d v

v = T CAPLET σ, T σ T 0 d N = 00 a, b, c, dθ,,θ 0 θ,,θ 0 σ a, b, c, dθ,, θ 0 θ,,θ 0 π/ v σ, v σ σt - v v LIBOR σ T σ T σ σ T a, b

LIBOR B B B B

LIBOR LIBOR LIBOR LIBOR Brgo and Mercuroθ v =0. Rebonaob

LIBOR LIBOR Glasserman and KouLIBOR Andersen and AndreasenLIBORCEV LIBOR LIBOR Glasserman and KouAndersen and Andreasen Glasserman and KouLIBOR LIBOR/λ ms CEVconsan elascy of varance Glasserman and Kou Glasserman and Merener Glasserman and Kou σ σ,, σ M σ σ =σ + +σ M

C JUMP 0 = δ L = 0 e λ T λ T! Cˆ L 0, K, γ T λmt 0 = + m L 0 e γ = σ + 0 d T s C γ s m λ zm s s log s + z s s + m z + s m s + + m s m s + + λ > log λ + + max0, z. m T δ γ λ m s

LIBOR m m m m m m =0 m<0m>0 Glasserman and Kou Andersen and AndreasenLIBOR

LIBOR α dl = L α σ dw +, αlibor d α a = K α γ L0 log + γ K = γ, b =, α, d α L c = α γ L0 log K = γ, γ, γ = 0 T σ d LIBOR 0<α<L =0 C CEV L 0, K, γ = δ D 0[L 0 χ a,b+,c Kχ c,b,a α = C CEV L 0, K, γ = δ D 0[L 0 Nd KNd ] α > C CEV L 0, K, γ = δ D 0[L 0 χ c, b,a Kχ a, b,c] N. χ.,d,λ λd L = 0L δ/ v δ k = δ / χ x, d, δ e v x, d + k k = 0 k! Dng

α < Andersen and Andreasen dl = ϕ L σ dw +, ϕ x= x.mnε α, x α, ε > 0 ε α <α > ε Lmed CEV Lmed CEVAndersen and Andreasen Lmed CEV LIBOR LIBOR LIBORHJM Andersen LIBOR Hun, Kennedy and Pelsser SV Josh and RebonaoRebonaoLIBOR

SV LIBOR Rebonaoa,b LIBOR LIBOR Glasserman and Kou Andersen and AndreasenEV LIBOR CEVSVLIBOR

LIBOR LIBOR L C C T + = maxl T K,0 C D + C /D + C T + T + C = E D + T + C T + D + T +. E T+ T + T +

D + T + = C =D + E T+ [C T + ]. C T + LIBOR dl L L T L T dl 0 L T T T L T T + LIBORLIBOR L T + D +

0 dl L dl L T T T dw dw D D + LIBOR σ W+ σ L dl = L σ dw+. σ

D + L L D + L L L T L T L 0 T T T L dw δ L dw = dw + ρσ d +δ L D + L LIBOR LIBOR T 5 T 5

S. N. J. BGM Andersen, L., A Smple Approach o he Prcng of Bermudan Swapons n he Mul-Facor LIBOR Marke Model, Journal of Compuaonal Fnance 3, pp.5-3, 000.,and J. Andreasen, Volaly Skews and Exensons of he LIBOR Marke Model, Appled Mahemacal Fnance 7, pp.-3, 000. Black, F., The Prcng of Commody Conracs, Journal of Fnancal Economcs, 3, pp.67-79, 976., and M. Scholes, The Prcng of Opons and Corporae Lables, Journal of Polcal Economy, Vol. 8, pp. 637-654, 973. Brace, A., D. G aarek, and M. Musela, The Marke Model of Ineres Rae Dynamcs, Mahemacal Fnance, Vol. 7, pp. 7-55, 997. Brgo, D., and Mercuro, F., Ineres Rae Models Theory and Pracce, Sprnger Fnance, Sprnger- Verlag, 00. Dng, C. G., Algorhm AS75: Compung he Non-Cenral χ Dsrbuon funcon, Appled Sascs, 4, pp.478-48, 99. Glasserman, P., and S. G. Kou, The Term Srucure of Smple Forward Raes wh Jump Rsk, workng paper, Columba Unversy, 000., and N. Merener, Numercal Soluon of Jump-Dffuson LIBOR Marke Models, workng paper, Columba Unversy, 00. Heah, D., R. Jarrow, and A. Moron, Bond Prcng and he Term Srucure of Ineres Raes: A New Mehodology for Conngen Clams Valuaon, Economerca, Vol. 60, pp. 77-05, 99. Hull, J., and A. Whe, Forward Rae Volales, Swap Rae Volales and he Implemenaon of he LIBOR Marke Model, workng paper, Joseph L. Roman School of Managemen Unversy of Torono, 999. Hun, P., J. Kennedy, and A. Pelsser, Markov-funconal neres rae models, Fnance and Sochascs 4, pp. 39-408, 000. Jamshdan, F., LIBOR and Swap Marke Models and Measures, Fnance and Sochascs, Vol., pp. 93-330, 997. Josh, M., and R. Rebonao, A sochasc-volaly, dsplaced-dffuson exenson of he LIBOR marke model, workng paper, Quanave Research Cenre, 00.

Kloeden, P.E., and E. Plaen, Numercal Soluon of Sochasc Dfferenal Equaons, Sprnger, 995. Pelsser, A., Effcen Mehods for Valung Ineres Rae Dervaves, Sprnger Fnance, Sprnger- Verlag, 000. Rebonao, R., Calbrang he BGM Model, RISK March, 999b., Volaly and Correlaon -In he Prcng of Equy, FX and Ineres-Rae, John Wley & Sons, Ld, 999b., The Sochasc Volaly Lbor Marke Model, RISK Ocober, 00.