國內油價與所得關係之探討-門檻向量誤差修正模型之應用
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(2) 謝辭 一本著作得以完成,除了需要靈感,還需要許多的幫助。這本碩士論文紀錄著我兩年 來所學的點點滴滴。論文能夠完成要感謝我的指導教授李慶男老師,老師平時教學認 真,有著豐富的涵養及敏銳的心思。以及兩位口試委員,王俊傑老師與翁銘章老師,為 學生的論文費心審查,並給予諸多寶貴的意見。此外,感謝所有老師的不吝教誨,以及 秀燕姐和育萍姐的協助。 論文寫作期間,特別感謝憲政學長在我徬徨無助的時候提供建議,真的是一個盡責的 好學長。而可愛的學弟政揚也不時地給我加油打氣。宜璇,你讓我看到光明堅強的一面, 讓我有了新的體會。而詩婷努力朝自己的理想邁進也讓我佩服。奕瑄則是一起研究論文 的好伙伴。以及所有的同學們,有了你們,研究所的生活增添了不少的色彩,祝福你們。 學生生涯至此告一段落,當學生的日子以來,總是過著無憂無慮的生活,感謝父親的 辛苦持家與母親的慈愛,大姊和二姊的照顧。還有之元,總是在我最累的時候陪著我。 我想我是幸福的孩子,在此,僅將這一小小的研究成果獻給我摯愛的家人。待在中山的 時間不長,但中山的確很美,讓我擁有許多的回憶,藍色的大海,空無一人的沙灘,將 是我懷念的地方。. 王鈺雯 謹誌於 中山大學經濟學研究所 中華民國九十六年六月.
(3) 摘要 石油屬於耗竭性資源,用完即不可再生,其蘊藏量分佈極為不均,半數以上集中在 中東地區。近年來國際原油變化莫測,油價的絕對數據也一再突破新高。台灣地區自產 石油極為有限,為國際油價之接受者,故油價對於經濟的影響不得不成為重要的議題。 根據經濟學原理,油價上漲常造成停滯性通貨膨脹,故本文首先利用共整合方法探討國 內油價與本國每人所得的關係,發現兩者之間存在負向的長期均衡關係。除此之外本文 還以 Hansen andSeo(2003)門檻向量誤差修正模型來檢定國內油價與本國每人所得之間 是否存在門檻效果,結果發現變數間符合門檻共整合的長期均衡關係,並且可表達成門 檻向量誤差修正模型。. 關鍵字: 油價,停滯性通貨膨脹,門檻效果,門檻向量誤差修正模型。. 1.
(4) Abstract Since petroleum is a kind of exhaustive resource, it can not be regenerated after being consumed. And petroleum is distributed extremely uneven in the world, more than half of petroleum is distributed in the Middle East area. In the recent years, the oil price was so fluctuating and broke the record again and again. However, the productivity of petroleum in Taiwan is very low and we are a price taker. So it turns to be important that how the oil price affects the economy. According to Economics, high oil price often causes the staginflation. In the purpose of this study we examine the long run relationship between oil price and personal income in Taiwan by cointegration theory. And we find that there indeed exists a negative longrun relationship. In addition, we consider a nonlinear model, Threshold Vector Error Correction Model, to test a threhold effect in the long run relationship between variables. Finally we have a result that there is a threshold cointegrating relationship between the oil price and personal income in Taiwan.. keywords: oil price, threshold effect, threshold vector error correction.. 2.
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(23) ôbK.ï"D´EÀBzóÝÅ(»ABrown and Yucel (1999) ¢ã&]h'ÿl(VAR)ÿlÝ\DT(Impulse Response )¼¡´Ý A¢Å(Y»ÝBz51965O1997OÝ`£]@Jî´Ýy º¸ÿ»/ß®gÜ3±¬vCW¿£îò Chang and Wong2003¿à'0-ÑÑÿl(VECM)¬¤g¸à²ó5 (Variance Decomposition )õ\DTÐó(Impulse Response )5@~´® ±ÝÀBz Ýn;@~A!GZ¤X´Ý®EÀ óÌb¿ÝÅ(ÍEy±BzÝÅ(¬æ.J ± O¼Ù¸à* Ml¸ÙÛ/ìª Cunado and Gracia2003ÊÝ´Àó D3J)¿àJ )Ýl]P ó D3J)`|0-ÑÑÿl(ECM) ÑÑGranger.n ;Granger causality testsÝljEö9Í»5ÿÕ´ÝE 9» Ý;0µªõ®Å(¬8!h¡ô²î»j´ÝEyt &îÝXb»ÍÅ(ݺY»Ý@~b8!¡ LeBlanc õChinn (2004)¿àÿû`a]°E´A¢Å(EG5»(Y z°ÆC^Í)Ý;0µªôè:°Í@Js¨´ÝîòE;0µªÝÅ (b§öõY»E´ÝAPô^b¢Ý-² Cunado and Gracia (2005)¿à1975OÏ×2002OÏÞÝ£]E±ö» (y¼±^ͱP8Ã;C»)Ý@~s¨´&ð½ ÝÅ(yÝBzþCμó´õÀBz Å(n;Ý&EÌ Pô3×°»J Guo and Kliesen (2005)J¼×Íy´»Ý;¡ÍÎ}Ýîò Tìª/ºEY»ÝÀBz(Aü7£ð´¼£¿£õ}iã)® ß¿ÝÅ( rÕ(2005)J- ´{E&»BzWÅ(b§#»{Bzï ?Âxæ.;ãyæ´Û/æ´ð/@²GDP´Gìª!`Qô ¼´î¹350-îE¦Bz)ÞCW×J©½ÎD ÌÙWÍîXSsÝ;0µª®ÞâÞD9ðY ¼7£EB 14.
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(29) 3. @~]°. ¿àDickey-Fullerql°EY»£] l5 s¨ÀBzóûÅD3q¨éÇ` ÌPù & P(non-stationary)3FÙÝ@J@~ 92à]h]°¼£ó Ý n; ݹ¨Ì]h(spurious regression)Ý®Þ
(30) §&` Ý ]PºbX!.h3¿à` ÀBz@J5G¾óÎÍ ÌPW @J5TþÝ×4M» |ì&ƵP&PÝ+Û` £] 5 P &PPÝlVê5 úP3P3hL3P(weakly stationary Tcovariance stationary)A×` y |ìëÍfEyX bÝt t − s t − j Nelson and Plosser(1982). 2. t. E(yt ) = E(yt−s ) = µ E(yt − µ)(yt − µ) = E(yt−s − µ)(yt−s − µ) = σy2 E(yt − µ)(yt−s − µ) = E(yt−j − µ)(yt−j−s − µ) = γs. J&ÆÌh` y Ì3PÍTµ²óσ &²óγ í b§Ýðóº.` Ý;DEy×Í&Ýó²3 ÝWshockÞº ` ¦@´²óô© ï` 5 6 Ý!!k5×Í&Ý` óbËË]°|ÞÍÿÌb P× -5¿%× T¿% 1 -5¿%: ×&ó¢ã-5»ð óu©m-5×gÇ¾Õ PJB I(1)um-5dg¾ÕPJB I(d)u×ÍBÄdg -5¡ÝóîW×Í%CYÝ(invertable)ÝARM A(p, q)Aì 2 y. t. s. (1 − φ1 L − φ2 L2 − ... − φp Lp )(1 − L)d Yt = c + (1 + θ1 L + θ2 L2 + ... + θq Lq )εt (3.1). 3]h]°lT£@JÿlÝ`ÎAX2àÝ` óÎVJ]h b¸æÍmP.n;Ýó Q¨Ý.n; 2. 16.
(31) Íφ(L) = 0Cθ(L) = 0ÝXbq/a3i²(Outside Unit Circle)vε ×ç¯JÌY Î×ÍARIM A(p, d, q)óud = 1`J(3.1)P¶ t. t. (1 − L)Yt = c + ψ(L)εt. Íψ(L) = φ. −1. (3.2). v;ó EJ(3.2)PîW. (L)θ(L). Yt = y0 + ct + ψ(L). Íct ü Tψ(L) P 2 T¿%: ub×ó. t−1 X. εt−i. i=0. t−1 i=0 εt−i. ^ T. Xt = µ + ct + ψ(L)εt. Íψ(L)Ý;ó EE(X ) = µ+ctV ar(X ) = (1+ψ +ψ +...)σ . V ar(X ) < ∞.h©X ótctx J»W¿%óhÌ T¿%Ä t. t. 3.1. t. t. 2 1. 2 2. 2. t. ql. AD3×ÍAR(1)Äy = ρy + u Íu ç¯3ÊXÛÝ5ó qÝìρ > 1¡ÝXbÂKº¸ós÷Íρ = 1Ît|"DÝ X|&ÆÌρ = 1` qÄ(unit root process)lρÎÍy×J ql ÍZÞ+Û×@ß5ð¸àÝql°Dickey-Fuller lDFl Augmented Dickey-Fuller lADFlPhillips-Perron lPPl 3DFql0-4' ç¯ ¡Þ0-4ݧ×@w´ bADFlPPl 3.1.1 Dickey-Fullerl (DFl ) Dickey and Fuller(1979)Ê×ÍAR(1)Ý` lPlÎÍÌbq© P3T ÍøÍÌDÂݵìDickey and Fuller J¿àOLS°X£ t. t−1. t. 17. t.
(32) ρÝ£ÂρˆÌb×lP!`3ÌnqÝÌP'ìtÙÝ5g ×ðV5gÎË;kº(Brownian Motion)8tÝP 'Ò]hP ×ÍAR(1)ÿl Yt = ρYt−1 + ut ρ=1. 3hY = 0vu i.i.d(0, σ ) ×ç¯ µÍÎÍâðó4(constant term)T` T(timetrend)]hP5 ì ëËlV ÿl×]hPPðó4C` T 0. 2. t. yt = ρ1 yt−1 + ut. 'l H : ρ = 1H ÝÁ§5g 0. 1. (3.3). 3ÌP'WñìDickey-Fuller0lÙ. :ρ<1. 1/2{[W (1)]2 − 1} R1 [W (r)]2 dr 0 1/2{[W (1)]2 − 1} t = (ˆ ρ − 1)/ˆ σρˆ → R 1/2 1 2 dr [W (r)] 0 T (ˆ ρ − 1) →. Íσˆ = [s ÷ P y ] vs = P (y − ρˆy àOLS£°ÿÕݣ ÿlÞ]hPâðó4¬P` T ρˆ. 2. T t=1. 2 1/2 t−1. 2. T t=1. t. 2 t−1 ) /(T. yt = θ + ρyt−1 + ut = x0t ρ + ut. 18. − 1). ρˆÎã(3.3)P¿. (3.4).
(33) ]hPðó4'l H : ρ = 1(vθ = 0)H ñìDickey-Fuller0lÙÝÁ§5g R. θ. 0. 1. 3ÌP'W. :ρ<1. 1. 1/2{[w(1)]2 − 1} − W (1) · 0 W (r)dr T (ˆ ρθ − 1) → R1 R1 [W (r)]2 dr − [ 0 W (r)dr]2 0 R1 1/2{[W (r)]2 − 1} − W (1) · 0 W (r)dr tθ = (ˆ ρθ − 1)/ˆ σρˆθ → R1 R1 { 0 [W (r)2 ]dr − [ 0 W (r)dr]2 }1/2. Íσˆ = [s e (P x x ) e ] e = [01] vs = P ρˆ õÎã(3.4)P¿àOLS£°ÿÕݣ ÿlë:]hPâðó4C` T ρˆθ. 2 0 2. 0 −1 1/2 t t 2. 0. 2. T t=1 (yt. 2. − θˆ − ρˆθ yt−1 )2 /(T − 2). . θ. yt = θ + ρyt−1 + δt + ut. (3.5). = x0t ρ + ut. ]hPðó4δ ]hP` T4'l H : ρ = 1(vδ = 0)H : ρ < 13ÌP'WñìDickey-Fuller0lÙÝÁ §5g R R R θ. 0. 1. 1. 1. 1. 1/2{[W (1) − 2 0 W (r)dr][W (1) + 6 0 W (r)dr − 12 0 rW (r)dr] − 1} T (ˆ ρτ − 1) → R 1 R R R R 2 dr − 4[ 1 W (r)dr]2 + 12 1 W (r)dr 1 rW (r)dr − 12[ 1 rW (r)dr]2 [W (r)] 0 0 0 0 0 tτ = (ˆ ρτ − 1)/ˆ σρˆτ. ˆ ρˆ y − δt) ˆ /(T −3) Íσˆ = [s e (P x x ) e ] e = [010] vs = P (y −θ− ρˆ Îã(3.5)P¿àOLS£°ÿÕݣ ulP°`ÌP'Çy ×&PDy J ×P îëËÿlÝlÙÁ§5g¬&òy×ÝðV5gTÎt5g Î ¾kº(Brownian motion)X|Û&ÂP°¢ðVTÎt5gÎ ¢Dickey andFuller(1979)ÝÛ& 3.1.2 Augmented Dickey-Fuller l (ADFl ) DFlTà3AR(1)ÿlv0-4 ç¯Dickey-Fuller(1979) ×MÊ0 -4Ìb8n t8nmápa¡4¸0-4 ç ρˆτ. 2 0 3. 1/2 0 −1 t t 3. 0. 3. 2. T t=1. t. τ t−1. τ. t. t. 19. 2.
(34) ¯.hè|AR(p)` lP qlÌ ADFl(Augmented Dickey-Fullerl) 'Ò]h P×ÍAR(p)ÿl yt = φ1 yt−1 + φ2 yt−2 + . . . + φp yt−p + εt. (3.6). 3hε i.i.d(0, σ ) L 2. t. ρ ≡ φ1 + φ2 + . . . + φp ζj ≡ −(φj+1 + φj+2 + . . . + φp ). j = 1, 2, . . . , p − 1. BÄó.P»ð¡Þ(3.6)PJ§W. yt = ζ1 ∆yt−1 + ζ2 ∆yt−2 + . . . + ζp−1 ∆yt−p+1 + ρyt−1 + εt. (3.7). µÍÎÍâðó4T` T]hP5 ìëËlVÍÿlîAì. ÿl×:]hPPðó4T` T yt = ζ1 ∆yt−1 + ζ2 ∆yt−2 + . . . + ζp−1 ∆yt−p+1 + ρyt−1 + εt. (3.8). = x0t ρ + εt. 'l H Á§5g. 0. :ρ=1. H. 1. 3ÌP'WñìDickey-Fuller0ÙÝ. :ρ<1. R1 1/2{[W (1)]2 − 1} − W (1) · 0 W (r)dr T (ˆ ρ − 1) → (σ/λ) · R1 R1 [W (r)]2 dr − [ 0 W (r)dr]2 0 ∗. Í(σ/λ) 8nÝlÑ. vBJÄ¡ R1 1/2{[W (1)]2 − 1} − W (1) · 0 W (r)dr T (ˆ ρ∗ − 1) → R1 R1 1 − ζˆ1 − ζˆ2 − ... − ζˆp−1 [W (r)]2 dr − [ 0 W (r)dr]2 0 R1 X 1/2{[W (1)]2 − 1} − W (1) · 0 W (r)dr ∗ ∗ 2 0 0 −1 1/2 t = T (ˆ ρθ − 1)/[s ep+1 ( xt xt ) ep+1 ] → R1 R1 1/2 { 0 [W (r)]2 dr − [ 0 W (r)dr]2 } 20.
(35) Íe = [00 . . . 01] s = P (y − x ρˆ ) /(T − p) ρˆ Îã(3.8)P¿àOLS£ °ÿÕݣ ÿlÞ:]hPâðó4¬P` T 0. p. T t=1. 2. 0 ∗ 2 t. t. ∗. yt = ζ1 ∆yt−1 + ζ2 ∆yt−2 + . . . + ζp−1 ∆yt−p+1 + α + ρyt−1 + εt. (3.9). = x0t ρ + εt. ]hPðó4'l H : ρ = 1(vθ = 0)H : ρ < 1 3ÌP' WñìDickey-Fuller0lÙÝÁ§5g: T (ˆρ − 1)Ct = (ˆρ − 1)/ˆσ Íe = [00 . . . 01] s = P (y − x ρˆ ) /(T − p − 1)ρˆ Îã(3.9)P¿ àOLS£°ÿÕݣ ÿlë:]hPâðó4C` T α. 0. 1. θ. 0. p+1. T t=1. 2. θ. ∗ 2 0 t θ. t. θ. θ. ρˆθ. ∗. yt = ζ1 ∆yt−1 + ζ2 ∆yt−2 + . . . + ζp−1 ∆yt−p+1 + α + δt + ρyt−1 + εt. (3.10). = x0t ρ + εt. ]hPðó4δ ]hP` T4'l H : ρ = 1(vδ = 0)H : ρ < 13ÌP'WñìDickey-Fuller0lÙÝÁ §5gT (ˆρ − 1) Ct = T (ˆρ − 1)/[s e (P x x ) e ] Íe = P (y − x ρˆ ) /(T − p − 2)ρˆ Îã(3.10)P¿àOLS£° [00 . . . 01] s = ÿÕݣ ADFlT (ρˆ − 1)ÙBÑÑ¡DFlT (ρˆ − 1)ÙÌb8!ÝÁ§ 5gADFlt ÙDFlt Ìb8!ÝÁ§5g.hADFlÝÛ &à!øãDFlÝÛ&. α. 0. 1. ∗ τ. 0. 2. ∗ τ. T t=1. t. ∗ τ. 2 0 p+2. ∗ 2 0 t τ. 0 −1 1/2 t t p+2 τ. p+2. ∗. ∗. ρˆ∗. ρˆ. ¡Said and Dickey(1984)?U"'-5¡Ý` ×ARMA(p, q)l Ppõq Îá(unknown)ÿlîAì (1 − φ1 L − φ2 L2 − . . . − φp Lp )∆yt = (1 + θ1 L + θ2 L2 + . . . + θq Lq )εt 21. (3.11).
(36) 'RÂy. 0. Îi.i.d(0, σ ) ×篬Þ(3.11)P¶W. = 0 εt. 2. η(L)∆yt = εt. Í η(L) = (1 − η1 L − η2 L2 − . . .) = (1 + θ1 L + θ2 L2 + . . . + θq Lq )−1 (1 − φ1 L − φ2 L2 − . . . − φp Lp ). .h×ARMA(p, q)Ý` »ð ×AR(∞) Ý` Ò]hP yt = yt−1 + η1 ∆yt−1 + η2 ∆yt−2 + η3 ∆yt−3 + . . . + εt. (3.12). ]hÿl yt = α + ρyt−1 + η1 ∆yt−1 + η2 ∆yt−2 + . . . + ηk ∆yt−k + etk. (3.13). = x0t β + etk. Í etk = ζk+1 ∆yt−k−1 + ζk+2 ∆yt−k−2 + . . . + εt. 3he ç¯uk → ∞vk¦Ý>yT J tk. p. etk − εt = ηk+1 ∆yt−k−1 + ηk+2 ∆yt−k−2 + . . . → 0. AkÂÈJARIM A(p, 1, q)3ÌP'ìÝlÙARIM A(p, 1, 0) 3ÌP'ìÝlÙb½8!ÝÁ§5g 3.1.3 Phillips-Perron l (PPl ) 3ADFl°4Ê"-4Ìb8nÝP¬QÎÊb D3²²P(heteroscedasticity)Ý®Þ.hPhillips(1987)Phillips and Perron(1988).ÌbqÝAR(1)ÿl;¨Õ?×;Ý'Êu ×Ímixing processÇ.&u b×Ý8µPC²²Pµs"Ýl]° t. t. 22.
(37) Ò]hPîAì yt = ρYt−1 + ut. (3.14). ρ=1. 3hY = 0vu ×Ímixing process ]hÿlîAì 0. t. yt = α + ρyt−1 + ut. (3.15). ¿àOLS°£P;óρˆ `Phillips and PerronÈÝÑÑlÙ T. 1 ˆ 2 − γˆ0 ) Zρ ≡ T (ˆ ρT − 1) − (T 2 σ ˆρ2ˆT ÷ ST2 )(λ 2 ˆ 2 − γˆ0 )/λ} ˆ × {T · σ ˆ 2 )1/2 · tT − { 1 (λ ˆρ2ˆT ÷ ST } Zt ≡ (ˆ γ0 λ 2. (3.16) (3.17). Í λˆ2 = γˆ0 + 2. l X. [1 − j/(l + 1)] · γˆj. j=1. γˆj = T −1 ·. T X. uˆt ut−j ˆ. t=j+1. ÀøÍóρˆ àOLS°£PÝρÂσˆ ρˆ ݲóS ù¿àOLS£ POÿ"-4ݲó.hBÄÑÑ¡ÝlÙùDFlADFl °b8!ÝÁ§5gÆk¸àPPl°`ÍÛ&Â!ø¢Dickey and Fuller(1979)ÝÛ& T. 3.2. 2 ρˆT. T. FÙJ)l. T. 2 T. ` ]°31980O|¼@~¥Fæ¼ÝP` ó @~@U"ÕXÛ&` ]°Ý@~Í¥ÝMÓ1μ yGranger and Newbold(1974)s¨&ó º¨XÛP]hݨ é ÝXÌP]hÝ®ÞBz.ïè×°]°»AÞ&PÝ` -5(difference) T T£](detrended data)Q3 &` 5 23.
(38) `f´)§Ý]P GïÇ|-5¡ÝP ]h5h]°4 b[ÝXîÝ®ÞQôSsÍÝBz®Þ. Þ` -5¡Ý óÝÎ×Ë;ÝlV4Qz½2¡y/Ý;Qô¸ÿ ó ©P´l¸P°ló ÎÍD3½íÉn;yÎãEngle and Granger(1987)OèJ)§¡Æs¨&ó Ý]hn;A ¨J)Ç×à&Ý` óÝaPà)WÌPJÌ b J)¨éJ9øÝ]hn;)QbBzLvËÍó D3½%Ý íÉn;|ì Engle and Granger (1987)J)ÝL L×:u'y ÝXbàWô/ I(d)&PÝ` vD3×' a(6= 0)¸ÿz = a y ∼I(d − b)Íb > 0JÌ'y ÝàWô D3db$ J)n;ÐrB y ∼CI(d, b)'aJÌ J)'(cointegration vector) Engle and Granger (1987) èGranger Representation TheoremÊ×Í(n × 1)Ý'y v∆y ÌbWold representation. t. 0. t. t. t. t. t. t. (1 − L)yt = δ + Ψ(L)εt. Íε i.i.d.(0, Ω)v{s · Ψ } = 0EP(absolutely summable)' 'y ÝàWô D3hÍJ)n;JºD3×Í(h × n)ÝÎpA vÎ pA ÝN× aP}ñJ×(h × 1)Ý'z LW. t. ∞ s s. 0. t. 0. t. zt = A0 yt. X|z Î×ÍÌPݨ²ÎpA bשP. 0. t. A0 Ψ(1) = 0. uÞîW×Íp$ÝV ARÿl. yt = a + Φ1 yt−1 + Φ2 yt−2 + . . . + Φp yt−p + εt. Tî. Φ(L)yt = a + εt 24.
(39) Í Φ(L) ≡ Ik − Φ1 L − Φ2 L2 − . . . − Φp Lp. JºD3×Í(n × n)ÎpB|. Φ(1) = BA0. ÍΦ(1) = I − Φ − Φ − . . . − Φ X|ºD3(n × n)Îpζ ,ζ ,. . . ,ζ ]hÿlîAì. k. 1. 2. 1. p. 2. p−1. ∆yt = ζ1 ∆yt−1 + ζ2 ∆yt−2 + . . . + ζp−1 ∆yt−p+1 + a − Bzt−1 + εt. (3.18). PÇ ×Í0-ÑÑÿl(vector error correction modelVECM)(z ) íÉ0-ãîDÄGranger Representation Theorem ÿáJ)n;Ä0 -ÑÑÿlETJ)ðÕ BzóÌbíÉn;2âÝ9°ó ÎÌb?íÉ]'JÝ©PùÇ3y`ó D3 Òݨé¬Î9ËyÒíÉݨéTº@¹9ÍCWÒ íÉÿ|@XÝ^×µÎXÛÝ0-ÑÑ^ 3.2.1 Engle and Granger Ë $ ð £ ° Ê×Í£°. (3.18). t−1. yt = βxt + ut. Bãql@y x / I(1) lM»Aì. M»× ¿àOLS°£"-uˆ ¿àOLS£°£βˆ ÿÕ"-uˆ uËó D3½J)n; Juˆ ∼ I(0)ÇÌP3øÍݵìβˆ[eÕË@Âβ¬&|×> √T [eÎ|y×>ÝT [e.hãOLS°£ÝβˆÂÌbø×l P(superconsistency) t. t. t. t. t. 25.
(40) M»Þ ¢ãlu ÎÍ I(1)ÿÕy x ÎÍD3J)n; 'l ÌP'H : u ∼ I(1)îy x DJ)n;Eñ' H : u ∼ I(0)¿àDF TADF ql°|îÝ? t·ÿlîA ì. t. t. 0. 1. t. t. t. t. t. ∆ˆ ut = ψ ∗ uˆt−1 +. p−1 X. ψ ∗ ∆ˆ ut−i + wt. i=1. Íw i.i.d.(0, σ )Aψ ½²yëJ`ÌP'îu ∼ I(0)y x Ë óD3J)n;ù¿à0-ÑÑÿlî. ∗. 2. t. t. t. ∆yt = a1 + ay (yt−1 − βxt−1 ) + A(L)∆yt−1 + B(L)∆xt−1 + w1t. (3.19). ∆xt = a2 + ax (yt−1 − βxt−1 ) + C(L)∆yt−1 + D(L)∆xt−1 + w2t. (3.20). ÍA(L)B(L)C(L)õD(L)í b§Ýa¡94P ε = y − βx 0-ÑÑ4 ˆ ¿àεˆ = y − βx ñáhÿlÿlîAì. t−1. t−1. t−1. t−1. t−1. t−1. ∆yt = a1 + ay · εˆt−1 + A(L)∆yt−1 + B(L)∆xt−1 + w1t. (3.21). ∆xt = a2 + ax · εˆt−1 + C(L)∆yt−1 + D(L)∆xt−1 + w2t. (3.22). ÿlÝ∆y ∆x ∆y õεˆ Xbó/ I(0)ÆàOLS¼£¢ óOó ÝyVJÄ QEngle and Granger Ë$ð£°4Q|U¬Q2Ý¿ÍE¯ Ýþ´. 1 ãyh]°Îó ÝJ)'©b×Í.h©ÊàyËóJ) n;Ýl ó ËÍ|î`D3ÝJ)'©×Íh`u l `ÌJ)n;ͬó ÇD3J)n; 2 D3½b§øÍ-(finite sample bias)Ý®Þ4Q3J)]hÿl5 βˆÌbø×lPÝ©P¬AøÍóÄK`|ly-Ý®Þ)P° E¯ t. t−1. t−1. t−1. 26. t.
(41) 3Phillips and Durlauf (1986)çîβˆÝÁ§5g &ðV5g(nonnormal)vt lÙ¬&t5gÆ¿àht lÙ 'l ÎP[Ýl 3.2.2 Johansen t à «£ ° ãyEngle and Granger Ë$ð£°b|îÝþ´ÆBz.ïXè&9 !Ýl]°|RîïÍ|Johansen èÝt룰tÌ PôÎêG ct ½¿àÝJ)l£° Johansen t룰ÎãJohansen(1988)Johansen(1991)è|ló ÝJ)n;3Johansent룰Î'ÿlÍ '&]h ÿl(vector autoregression modelVAR)v£lJ)'ÝÍó. h8´yEngle and Granger ÝË$ð£°?
(42) §ËÍ|îÝó®Þ 'b×Í(n × 1)Ý'y v'y ÝN×ôí I(1)|V AR(p) î. 3. t. t. yt = µ + Π1 xt−1 + Π2 xt−2 + . . . + Πp xt−p + εt. t = 1, 2, . . . , T. (3.23). ∆yt = µ + ξ1 ∆yt−1 + ξ2 ∆yt−2 + . . . + ξp−1 ∆yt−p+1 + ξyt−1 + εt. (3.24). ͵Îðó4vε i.i.d.N (0, Ω) Þ(3.23)P|0-ÑÑÿlî. t. Í ξ = −(In − Π1 − Π2 − . . . − Πp ) = −Π(1) ξi = −(In − Π1 − Π2 − . . . − Πi ). t = 1, 2, . . . , p − 1. ''y ÝN×ͽóy í I(1)v¸Æ ÌbrÍJ)n; Jξ = αβ αβ/ (r × n)ÝÎpβÌ J)ÎpαJ J;óÎp ÎpξÝè(rank)¼D3yó íÉn;ÝóêÇJ)'ÝÍ óD3bëË. t. it. 0. 27.
(43) rank(ξ) = nÇξÎp G>ÎpÇè(full rank)î'y Ý& ó/ PÝ` 2 0 < rank(ξ) = r < nî'y Ýó D3rÍJ)' 3 rank(ξ) = 0Çξ Îp èÎpÇ ëè(null rank)½'y ¬D 3¢J)n; .hlÄx3y@ξÎpÝèùE(3.24)P 'lÌP' H : rank(ξ) = r|@rank(ξ)J)Ý'Íó Johansent룰M»Aì. M»×Õ§]h(Auxiliary Regressions) ∆y y 5½E∆y ,. . . ,∆y ®]hÿlÞ(3.24)P;¶W. 1. t. t. t. 0. t. t−1. t−1. t−p+1. Z0t = ΓZ1t + ξZpt + εt. Í Z0 t = ∆yt Z1t = 1, ∆yt−1 , . . . , ∆yt−p+1 Zpt = yt−p Γ = (µ, ξ1 , . . . , ξp−1 ). ¿àOLS£ÿÕ"-4R CR v"-Ý¿]õ. 0t. pt. Sij = Mij − Mi1 M−1 11 M1j. (i, j = 0, p). JÍf¹ÝëÐó(concentrated likelihood function)î. T. −T /2. L(α, β, Ω) = |Ω|. 1X (R0t − ξRpt )0 Ω−1 (R0t − ξRpt )} exp{− 2 t=1. M»Þ ÕÑø8n(Canonical Correlations) 28. (3.25).
(44) kOtë£POìP. |λSpp − Sp0 S−1 00 S0p | = 0. .hÿÕ©Pq(eigenvalues) λˆ > λˆ > . . . > λˆ > 0Cýã;¡Ý©P' (eigenvectors) Vˆ = (ˆv , vˆ , . . . , vˆ )vVˆ S Vˆ = I M»ë ÕëÐóÝ£¢ó(MLE Estimation of Parameters) uD3rÍJ)n;Jβ£Ç GrÍ©PqXETÝGrÍ©P'X àWÝÎpÇβˆ = (ˆv , vˆ , . . . , vˆ )vξ = αβ Þ(3.25);¶W(3.26). 1. 1. 1. 2. 2. 2. n. 0. n. pp. 0. r. T. −T /2. L(α, β, Ω) = |Ω|. 1X exp{− (R0t − αβ 0 Rpt )0 Ω−1 (R0t − αβ 0 Rpt )} 2 t=1. (3.26). βÂüì|ÿÕìP. ˆ = S0p β( ˆ βˆ0 Skk β) ˆ −1 α( ˆ β) ˆ = S00 − S0p (βˆ0 Skk β) ˆ −1 βˆ0 S0k ˆ β) Ω( ˆ = (M01 − ξMp1 )M11 −1 Γ. èËËl°¼lJ)'ÝÍó. 1 ªl(Trace Test). 3Î@D3¿àJ)n;GãîXÿÕÝ©Pqàyl ÿlt9D3rÍJ)'ÝÌP'ÎÍWñ H : rank(ξ) ≤ r (9brÍJ)') H : rank(ξ) > r (byrÍJ)') lÙ. Johansen. 0. 1. −2 ln(H0 |H1 ) = −T. n X i=t+1. ˆi) ln(1 − λ. Í 5g|¾ ×Í(n − r)îݾk¹º(Brownian Motion) vlÙÝÁ§5gºyQÎpݪ 29.
(45) t©Pql(Maximum Eigenvalues Test). 2. H0 : H1 :. brÍJ)' br+1ÍJ)'. lÙ. ˆ r+1 ) −2 ln(H0 |H1 ) = −T ln(1 − λ. 8!2Í 5gù¾W×Í(n − r)îݾk¹º(Brownian Motion)vlÙÝÁ§5gºyQÎpÝt©Pq 3.3. .n;l. Granger. 3BÄJ)l¡¾W0-ÑÑÿl30-ÑÑÿlóB Ä×g-5Ó¨PyÎ&Æ|ºàGranger.n;lÍ Ý.n ;Granger.n;¼ÝÎÙîÝ.n;¯@î¼ÝÎó ` îÝ ra¡n;Hamilton(1983)©½úGranger.n;¬&ìîÝ.n ;Granger.n;ÝÎ3ÙîØÍóÝ;ÎÍ\y¨×ÍóÝ ;Granger(1969).n;ÝLAì LÞ bX õY ËÍI(0)Ý` ÍLG>/)AìX:âX |² ÄÝXb£GY :âY |²ÄÝXb£GX :âX õÄÝX b£GY :âY õÄÝXb£GF M SE(X |X, Y ):îâX õY |²ÝÄXb£Gìï?í]0- Granger.lbì°Ëµ t. t. t. a. t. a. t. t. t. }ñn;. 1. F M SE(Xt |X) = F M SE(Xt |X, Y a ) = F M SE(Xt |X, Y ). 30. t. t.
(46) v F M SE(Yt |Y ) = F M SE(Yt |X a , Y ) = F M SE(Yt |X, Y ). îfáEX ¦ÝY TÝXb£GT¦ ÝY |²ÝÄXb£G/P°EX Ýï?í]0-®ßÅ(! §EY X óÝáôEY Ýï?í]0-^b¢;.h |¾X õY Î8!^b.n;Ý 2 '.n; F M SE(X |X) > F M SE(X |X, Y )áY |²ÝÄXb £GbÃyX Ýï?æÆáY ºÅ(X !§uF M SE(Y |Y ) > F M SE(Y |X, Y )JX ºÅ(Y 3 .n; F M SE(X |X, Y ) < F M SE(X |X, Y ) ÝY ºñÇÅ(X !§ uF M SE(Y |X , Y ) < F M SE(Y |X, Y )JX ºñÇÅ(Y 4 /n; F M SE(X |X) > F M SE(X |X, Y )vF M SE(Y |Y ) > F M SE(Y |X, Y ) áÍóÝ£GEyóKb´·Ýï?[£J Ô'Ý.n; 3.3.1 Ô . l ° Granger(1969)èº×ÍÔ.n;ÝluÊPAì t. t. t. t. t. t. t. t. t. t. t. t. t. t. t. t. t. t. a. t. t. t. t. t. a. t. t. t. t. t. zt = a0 + a1 zt−1 + ... + ap zt−p + b1 xt−1 + . . . + bp xt−p + et. t. t. t. (3.27). î ` 4pî tÊa¡óùÇGranger.lÝÌP' H :x does not Granger cause zlxóÎÍÙîEμÝz Ìb£GÇÎEt ¿]°Ý]h;ób b Ð)ll]h;óÎͽ²yë ÆGranger.lÝÌP'ô H : b = . . . = b = 0AóxEÎ¼Ý ózÌb£GÝFlÝlÙº`ÌP'îxÝ;|Eμzè t. 0. 1. p. 0. 1. 31. p.
(47) º£GDu`ÌP'Jî^bÈJAîx|EμÝzèº £G lÙ F =. (RSSr − RSSu )/p RSSu /(T − 2p − 1). ÍRSS å§×Ý"-¿]õRSS Îå§×Ý"-¿]õpa¡ ó r. 3.4. u. b'0-ÑÑÿl. FÙÝJ)©ÊÝó D3aPJ)n;#½&ÆÊBzó J)¨é|&=ÝòP¼ JÞÍU &aPÝÿlG ¸ÿlæî>EyBz¨éÝÕæô è bJ)ÿlÎãBalke and Fomby(1997)èBalke and Fomby- 3¾Õ íÉÄ` ºb&=PÝJ ` 3ñÒíÉHG `J)n;´ ú¦Q ` ÒíÉ8 Ý`ÎJJ)n ;´ ß3ƼãyÅ83Bz`Äm}×ÝJWÍX |ó3! 'íÉJÝĺӨ×lݨé.hJÄ 3J¡Ý[ÇyWÍ`ôµÎÒíÉ´`º¨ Hansen and Seo(2002) ×M¿àË ½bJ)'0-ÑÑÿl l hÿlÝ¥F3ylÎÍD3×Íb[ÍÝbó 0-ÑÑ 4Ç@~ 0-ÑÑ4ybÂÝ`Î0-ÑÑ4ybÂÝ`Îó 3Õ¾íÉÄÝJ ÎÍ8!Hansen and Seo ȸàSup LMÙ lb[D3ͬèÐ)lÙ 5g 3.4.1 £ aP'0-ÑÑÿl 'x ×pîI(1)Ý` ux D3×p × 1ÝJ)'βJw (β) = β x I(0)Ý0-ÑÑ4u|'0-ÑÑÿlîJ2PAì t. 0. t. t. t. ∆xt = A0 Xt−1 (β) + ut 32. (3.28).
(48) Í∆x x Ý×g-5X (β) = [1, w , ∆x , ∆x , · · · , ∆x ] k × 1Î pvl tÊa¡ó(lag length)A k × p;óÎpÍk = p × l + 2' 0-4u ×martingale difference sequencevE(u u ) = Σ ×b§²Îp ÝÿÕ°×PmÞÎpβÑð;(Normalization)ÇÞβÍ×-ô' 1 30-4u iid Gaussian'ìÍ¢ó(β, A, Σ)ãtë°(Maximum ˜ A, ˜ "˜ Σ) ˜ îJu˜ = ∆x − AX ˜ Likelihood)£ÿÍ£Â|(β, (β) ' bË ½'0-ÑÑÿl Hansenõseo(2002)qAaP'0-ÑÑÿlÞÍU" bË ½Ý' 0-ÑÑÿl t. t. t−1. t−1. t. t−1. t. t−2. t−l. 0 t. t. t. ∆xt =. t. t−1. A01 Xt−1 (β) + ut if wt−1 (β) ≤ γ A02 Xt−1 (β) + ut if wt−1 (β) > γ. (3.29). Íγ bÂîÿlù;¶ . ∆xt = A01 Xt−1 (β)d1t (β, γ) + A02 Xt−1 (β)d2t (β, γ) + ut. (3.30). Pd (β, γ) = 1(w (β) ≤ γ)d (β, γ) = 1(w (β) > γ)Ç w (β) ≤ γ `d (β, γ) = 1Dd (β, γ) = 0 w (β) > γ `d (β, γ) = 1D d (β, γ) = 0vb[°b30 < P (w ≤ γ) < 1Çw ≤ γsß^£ +y0õ1 bLÍJhÿlÞ;WaPJ)X|áÊ Ý§×f (constraint)': 1t. t−1. 2t. 1t. t−1. 1t. t−1. 1t. t−1. t−1. 2t. t−1. π0 ≤ P (wt−1 ≤ γ) ≤ 1 − π0. Íπ > 0 ×J¢ó(trimming parameter)Í@~¢Hansen and Seo(2002)3@JÄ'π = 0.05qAHansen and Seo(2002)30-4u iid Gaussian'ìÍtë£ÝGaussian likelihood. 0. 0. ln(A1 , A2 , Σ, β, γ) = − n2 log|Σ| −. Í. t. 1 2. Pn. t=1. ut (A1 , A2 , β, γ)0 Σ−1 ut (A1 , A2 , β, γ). ut (A1 , A2 , β, γ) = ∆xt − A1 0 Xt−1 (β)d1t (β, γ) − A2 0 Xt−1 (β)d2t (β, γ) 33.
(49) |M LE(Aˆ , Aˆ , Σ,ˆ β,ˆ γˆ) ln(A , A , Σ, β, γ) të£ÂAˆ (β, γ) CAˆ (β, γ) ãI5øÍw (β) 6 γõw (β) > γ ͽ|∆x EX (β) ]h ÿAì 1. 2. 1. 2. t−1. 2. 1. t−1. t. t−1. n n X X 0 −1 ˆ A1 (β, γ) = ( Xt−1 (β)Xt−1 (β) d1t (β, γ)) ( (β)∆xt 0 d1t (β, γ)) t=1 n X. Aˆ2 (β, γ) = (. t=1 n X. Xt−1 (β)Xt−1 (β)0 d2t (β, γ))−1 (. t=1. (β)∆xt 0 d2t (β, γ)). t=1. uˆt (β, γ) = ut (Aˆ1 (β, γ), Aˆ2 (β, γ), β, γ) n 1X ˆ Σ(β, γ) = uˆt (β, γ)uˆt (β, γ)0 n t=1. .hÿÕ|ì;ë]P. np n ˆ ˆ γ)| − (3.31) ln(β, γ) = ln(Aˆ1 (β, γ), Aˆ2 (β, γ), Σ(β, γ), β, γ) = − log |Σ(β, 2 2 P ˆ γˆ ) MLE(β, β π0 6 n−1 1(xt 0 β 6 γ) 6 1 − π0. 3J)' ðV;C § ˆ ×ìÿt;log |Σ(β, γ)|3ðV;CG§×ìβ γ -BãÏ(3.30)P të£QÏ(3.30)P¬&¿âÐó.hP°|FÙÝVÉ. Õ°(gradient hill-climbing algorithms)OHansen and Seo(2002)ÈãË î(β, γ)ÝF£(grid search)OÿëÂtÝà)|® J)'(β)b Â(γ)£Â 3.4.2 l b[ÝlÍ@~JÎ|Hansen and Seo(2002)èSupLMl ãJÍÙ5g`½Îãbootstrapÿa®ßtÝ"-&ýã;5 g|CW¢ó®ÞlÿlÊ)aPÝ'0-ÑÑÿlTÎ&aP b'0-ÑÑÿlÌP'H (3.28)PÝaP'0-ÑÑÿlEñ 'H (3.29)PÝb'0-ÑÑÿl (3.30)PÝA = A `ÿlÞ ; (3.28)PÝFÙaP'0-ÑÑÿlhl°½¥y|ÿl ÃÝl (model-based statistical tests)v.&ÿlà#Ýf´.h3ÿlïIî´ ÍPÒól(nonparametric tests)?Ì[æ 0. 1. 1. 34. 2.
(50) hl ¿àLM(Lagrange Multiplier)Ù¼Æ'(β, γ) ávü JÌP'Eñ'5½Aì. ∆x H ∆x. H0. t. = A0 Xt−1 (β) + ut. 1. t. = A1 0 Xt−1 (β)d1t (β, γ) + A2 0 Xt−1 d2t (β, γ) + ut. A ½2yA `î×b[D3uJ)(β)õbÂ(γ) á`qAHansen and Seo(2002)lÙ. 1. 2. LM (β, γ) = vec(Aˆ1 (β, γ) − Aˆ2 (β, γ))0 (Vˆ1 (β, γ) + Vˆ2 (β, γ))−1 × vec(Aˆ1 (β, γ) − Aˆ2 (β, γ)). Í ˆ i = Mi (β, γ)−1 Ωi (β, γ)Mi (β, γ)−1 i = 1, 2 V Mi (β, γ) = Ip ⊗ Xi (β, γ)0 Xi (β, γ) i = 1, 2 Ωi (β, γ) = ξi (β, γ)0 ξi (β, γ) i = 1, 2. PX (β, γ) X. ÀP'(stacked vector)£Pξ (β, γ) ˆ (β, γ) 0-ÑÑ4! ½ u˜ ⊗ X (β)d (β, γ)ÀP'£PvecA 4x EX (β)d (β, γ) ]h;óÀP'£PVˆ (β, γ)J vecAˆ (β, γ) ²Îp£P uβõγ ÎááH ÌP'ìÝF£Â.hβ|(3.28)PXÿ£ Âβ˜ áãyH ì¬PbÂ.hlÙJ. t−1 (β)dit (β, γ). i. t. t−1. t. i. it. t−1. i. it. i. i. 0. 0. SupLM =. ˜ γ) LM (β,. sup. (3.32). γL ≤γ≤γU. γ¨´Pγ Þyw˜ π y5fγ Þyw˜ (1 − π )y5 ft¡3µAHansen and Seo(2002)èÝü]hPdí°(fixed regressor bootstrap)|C"-dí°(residual bootstrap)¼ÕÍ `½p-value|l ÿlb[. [γL , γU ]. L. t−1. 0. 35. U. t−1. 0.
(51) 4 4.1. £]¼Ù
(52) §. @J5. ÍZ@~ 1987Oϰ2006Oϰ|£] 577ÍÌ DÂÍZ;¿àHansen and Seo(2002)b0-ÑÑÿlXóãÝó »/ ´Í»NßGDP 3»/´]«µï´2¥Ý´`ê4Q´2¥Ý´`4ê¾9 ¬´`îìÿÝ TÎ×lÝÆÍZóãÜÞPÕ_´Ý}¼»/´ ¬BÄгÎJ @²´ìµÝæ£]£] `£]lVã3Í `¿íW £]vÎB;PJ£]¼Ù5 ËI51999O1`|¡Ý£ ]¼y´2¥Ýçì1999O|GÝ£]¼y¬È2 ÙÙ£]0 3h©½1´2¥Ý´J®¼æJÍJ¼ý NYMEX WTI(Y»ÆLùæ´)[8ãóÞ¼ýÝ» N ×WTI}î×WTI}f´»y5fâWãóÞãh á»/´)6¢»jÝæ´}¬»´ õc35î«2à »/´G»/¨µì5ÝôÞ? Þã3Í»NßGDP] «£]ÝlV £]£]¼Ù ¬ÈBz± £]0X¸àÝóAì »/@²´o =log(ÜÞPÕ_´}/гμó) 2 Í»NßGDPy =log(NßGDP) 1. t. t. 4.2. ql. 3EBzó n=P"DGÄ6|ql PÝl| ¹®ßÌ]hÝ®ÞÍZ¸àADFl°PPl° E»/´Í»N ßGDPPÝ@-ql@JA. 36.
(53) )4.1*o ql H :o iã q t. l. ADF. Ù. t -2.8708. Ù. 0. t. Ù H :o ×$-5 q. PP. Ù. PP. p-value 0.1778. l. 0. t -3.0202. p-value 0.1337. t. ADF. t -7.3173***. l. p-value 0.0000***. l. t -7.2873***. p-value 0.0000***. !Û 1. ***31¥½iãì|`ÌqÝÌP' 2.X¸àÝÿlvl âðó4` T4Ýÿl 3.Û&¢Fuller(1979). )4.2*y ql H :y iã q t. Ù. l. ADF. t -2.5886. Ù. t -6.8734***. 0. t. Ù H :y ×$-5 q. PP. Ù. PP. p-value 0.2867. l. 0. l. t -1.9231. p-value 0.6327. t. ADF. p-value 0.0000***. t -10.7942***. l p-value 0.0000***. !Û 1. ***31¥½iãì|`ÌqÝÌP' 2.X¸àÝÿlvl âðó4` T4Ýÿl 3.Û&¢Fuller(1979). l¼NßGDP»/´Ý` P¡31¥5¥T10¥Ý½iã ì/Ìbq©PvBÄ×g-5¡Ó¨VùÇNßGDP»/´ / I(1)` Æ»/´Í»NßGDP5m ×M¸àJ)l ¼ï-ËïÝÉíÉn; 37.
(54) 4.3. J)l. 3G×;Í@~EyNßGDP»/´ qllîË ïí &Ý` 3@ó/ I(1)¡ ×MÊó D3 J)n;ÍZ#½J)lÍðÝJohansen(1988)J)l° Balke and Fomby(1997)- Johanson(1988)J)l]°3bJ)l æ· ¬Engle and Granger(1987))býÝlº[ÆuÎËꨧ ×lÝ`Î|Engle and GrangerË$ð£°Ý ã 4.3.1 Engle and Granger Ë$ ð £ °l 3h®Engle and Granger(1987)Ë$𣰠M»×|y |Co óEBh t¿]]hÿìËf]hP 3. t. t. yt = α1 + β1 ot + e1t ot = α2 + β2 yt + e2t. M»Þ35½E"-4e e ql lA 1t. 2t. )4.3*Engle-grangerJ)l H :e q ADFl PPl tÙ tÙ -3.10597** -3.05035 ** H :e q ADFl PPl tÙ tÙ 0. 1t. 0. 2t. -2.57647*. -2.47149*. !Û 1. ***5½310¥õ5¥½iãì|`ÌqÝÌP' 2.Û&¢Phillips and Ouliaris(1990) Balke and Fomby(1997)- JohansenJ)l]°ðVP'Þ.bJ)D3`" - &ýã5gCWÿl0'ݵsß 3. 38.
(55) 3P¡Î|ADFl°TÎPPl°3½iã10¥ì`]hP "-4ÌqÝÌP'µh.\NßXÿ»/´D3J)n; É Tù.hÿÕÿlÝ@- 4.3.2 Johansent à «£ °l dyEngle and Granger(1987)Ýl°D3A(3.2.1);Xè
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