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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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(1)國立中山大學經濟學研究所 碩士論文. 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 An Examination of the Relationship between Oil Price and Income in Taiwan by Threshold Vector Error Correction Model.. 研究生:王鈺雯 撰 指導教授:李慶男 博士. 中華民國 九十六 年六月.

(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´‰Ž›EÀ›BzŽóÝÅ(»ABrown and Yucel (1999) ¢ãŠ&]h'ÿl(VAR)ÿlݎ\DT(Impulse Response )¼¡Š´‰ÝŽ› A¢Å(Y»ÝBz5—1965O‹1997OÝ`£]@J”Œ•ݎ›y º¸ÿ»/ß®gÜ3±¬vCW¿£îò Chang and Wong2003¿à'0-ÑÑÿl(VECM)¬¤g¸à޲ó5 Š(Variance Decomposition )õŽ\DTÐó(Impulse Response )5—@~´‰® ›±ÝÀ›Bz Ýn;@~”ŒA!GZ¤X–´‰Ý®›EÀ ›ŽóÌb¿ÝÅ(ÍEy±BzÝÅ(—¬‚æ.J ± O¼Ù¸à* Ml¸ÙÛ/—ìª Cunado and Gracia2003ÊÝ´‰À›Žó D3J)¿àJ )Ýl]P Žó D3J)`|0-ÑÑÿl(ECM) ÑÑGranger.Œn ;Granger causality testsÝljEö9Í»5—ÿÕ´‰ÝŽ›E 9» Ý;0µªõ®ŒÅ(¬8!h”¡ô²î»j´‰ÝŽ›Eyt &îÝXb»ÍÅ(ŒÝºY»Ý@~b8!”¡ LeBlanc õChinn (2004)¿àÿû`a]°E´‰A¢Å(EG5»(Y z°ÆC^Í)Ý;0µªôèŒ:°Í@Js¨´‰ÝîòE;0µªÝÅ (b§öõY»E´‰ÝAŽPô^b¢€•Ý-² Cunado and Gracia (2005)¿à1975OÏ׋2002OÏÞÝ£]E±ö» (y¼—±^ͱP8ß;CŒ»)Ý@~s¨´‰&𕽠ÝÅ(yÝBzþ›CΉ¼ó‚´‰Ž›õÀ›Bz Å(n;Ý&EÌ Pô3×°»J€ Guo and Kliesen (2005)J¼Œ×Íy´‰»ÝŽ;¡ÍΉ}Ýîò Tìª/ºEY»ÝÀ›Bz(Aü7£ð´¼£¿£õ‰}iã)® ß¿ÝÅ( rÕ(2005)J- ´‰{™E&»BzWÅ(b§#‹Š»Ÿ{Bzï ?ÂxŠæ.;ãyæ´Û/—洏ð/@²GDP´Gìª!`Qô ¼Œ´‰î¹350-îE¦Bz›)ÞCW×—J©½ÎD ÌÙWÍî™XSsÝ;0µª®ÞâÞD9ðYŒ ¼7£EB 14.

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(29) 3. @~]°. ¿àDickey-FullerŽql°EY»£] •l5 —s¨À›BzŽóûÅD3Žq¨éÇ` Ì­Pù &­ P(non-stationary)‚3FÙÝ@J@~ 92à]h]°¼£ŒŽó Ý n; ݹŒ¨Ìƒ]h(spurious regression)Ý®Þ 

(30) §&­` Ý ]PºbX!.h3¿à`  •À›Bz@J5—G¾ŽóÎÍ Ì­PW @J5—TþÝ×4M» |ì&Ƶ­P&­P†ŽÝ+Û` £] 5 ­P &­P­PÝlVê5 ú­P3­P3hL3­P(weakly stationary Tcovariance stationary)AŒ×` y ”•|ìëÍfEyX bÝt t − s t − j ‚Ž 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 Ì3­PÍTµ޲óσ Š&޲óγ í b§Ýðóº.` ݎ›‚;ŽDEy×Í&­Ý󂎲3 ÝW›shockÞº ` ¦‚@˜´޲óô© ï` 5  6 Ý!‚!k5—×Í&­Ý` óbËË]°|Þ͎ÿÌb­ P× -5¿%× T¿% 1 -5¿%: ×&­ó¢ã-5»ð ­óu©m-5×gǝ¾Õ­ PJB I(1)um-5dg¾Õ­PJB I(d)u×ÍBÄdg -5¡ÝóîW×Í%CYÝ(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£Œ@JÿlÝ`ÎAŒX2àÝ` ŽóÎVJ]h”Œœ b¸æÍmP.Œn;ݎó QŒ¨ƒÝ.Œn; 2. 16.

(31) Íφ(L) = 0Cθ(L) = 0ÝXbq/a3Ž›i²(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 –EJ(3.2)PîW. (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 –EE(X ) = µ+ctV ar(X ) = (1+ψ +ψ +...)σ  . V ar(X ) < ∞.h©ŠX óœtctx J»W¿%óhÌ T¿%Ä t. t. 3.1. t. t. 2 1. 2 2. 2. t. Žql. AŒD3×ÍAR(1)Äy = ρy + u Íu ç¯3ÊXÛÝ5ó ŽqÝìρ > 1¡ÝXbÂKº¸ós÷Íρ = 1Ît|"DÝ X|&ÆÌρ = 1` ŽqÄ(unit root process)‚lρÎÍy×J Žql  ÍZÞ+Û×@ß5—ð¸àݎql°Dickey-Fuller lDFl Augmented Dickey-Fuller lADFlPhillips-Perron lPPl 3DFŽql0-4ƒ' ç¯ ¡Þ0-4ݧ×@˜w´‚ bADFlPPl 3.1.1 Dickey-Fullerl (DFl ) Dickey and Fuller(1979)Ê×ÍAR(1)Ý` lPœlÎÍÌbŽq© P3›T ÍøÍÌDÂݵìDickey and Fuller J€¿àOLS°X£Œ t. t−1. t. 17. t.

(32) ρÝ£ŒÂρˆÌb×lP!`3ÌnŽqÝÌPƒ'ìtٌݘ5g ×ðV5g‚ÎË;kº›(Brownian Motion)8tÝP ƒ'қ]hP ×ÍAR(1)ÿl Yt = ρYt−1 + ut ρ=1. 3hY = 0vu i.i.d(0, σ ) ×ç¯ ‚µÍÎ͑âðó4(constant term)T` T(timetrend)]hP5 ì ëËlV ÿl×]hPPðó4C` T 0. 2. t. yt = ρ1 yt−1 + ut. ƒ'l H : ρ = 1H ÝÁ§5g 0. 1. (3.3). 3ÌPƒ'WñìDickey-Fuller0Œlٌ. :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£Œ°ÿÕÝ£ŒÂ 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) ]hPðó4ƒ'l H : ρ = 1(vθ = 0)H ñìDickey-Fuller0ŒlٌÝÁ§5g R. θ. 0. 1. 3ÌPƒ'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£Œ°ÿÕÝ£ŒÂ 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` T4ƒ'l H : ρ = 1(vδ = 0)H : ρ < 13ÌPƒ'WñìDickey-Fuller0ŒlٌÝÁ §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£Œ°ÿÕÝ£ŒÂ ul”ŒP°`–ÌPƒ'Çy ×&­PDy J ×­P î–ëËÿlÝlٌÁ§5g¬&òy×ÝðV5gTÎt5g ‚Î ¾kº›(Brownian motion)X|Û&ÂP°¢ðVTÎt5g‚Î ¢Dickey andFuller(1979)ÝÛ& 3.1.2 Augmented Dickey-Fuller l (ADFl  ) DFlTà3AR(1)ÿlv0-4 ç¯Dickey-Fuller(1979) ×MÊ0 -4Ìb8n t8nmápa¡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) ¯.hèŒ|AR(p)` lP •ŽqlÌ ADFl(Augmented Dickey-Fullerl) ƒ'қ]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). µÍÎ͑âðó4T` T]hP5 ìëËlVÍÿlîAì. ÿl×:]hPPðó4T` T yt = ζ1 ∆yt−1 + ζ2 ∆yt−2 + . . . + ζp−1 ∆yt−p+1 + ρyt−1 + εt. (3.8). = x0t ρ + εt. ƒ'l H Á§5g. 0. :ρ=1. H. 1. 3ÌPƒ'WñìDickey-Fuller0ŒÙŒÝ. :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. vBŸJÄ¡ 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£ Œ°ÿÕÝ£ŒÂ 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. ]hPðó4ƒ'l H : ρ = 1(vθ = 0)H : ρ < 1 3ÌPƒ' WñìDickey-Fuller0ŒlٌÝÁ§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£Œ°ÿÕÝ£ŒÂ 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` T4ƒ'l H : ρ = 1(vδ = 0)H : ρ < 13ÌPƒ'WñìDickey-Fuller0ŒlٌÝÁ §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£Œ° [00 . . . 01] s = ÿÕÝ£ŒÂ ADFlT (ρˆ − 1)ٌBÑÑ¡DFlT (ρˆ − 1)ٌÌb8!ÝÁ§ 5g‚ADFlt ٌDFlt 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"ƒ'‹-5¡Ý`  ×ARMA(p, q)l P‚põq Îá(unknown)ÿlîAì (1 − φ1 L − φ2 L2 − . . . − φp Lp )∆yt = (1 + θ1 L + θ2 L2 + . . . + θq Lq )εt 21. (3.11).

(36) ƒ'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`  қ]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. AŒkÂÈJARIM A(p, 1, q)3ÌPƒ'ìÝlٌARIM A(p, 1, 0) 3ÌPƒ'ìÝlٌb½8!ÝÁ§5g 3.1.3 Phillips-Perron l (PPl  ) 3ADFl°4Ê"-4Ìb8nݝP¬Q΁Êb D3²²P(heteroscedasticity)Ý®Þ.hPhillips(1987)Phillips and Perron(1988).ÌbŽqÝAR(1)ÿl;¨Õ?×;Ý'Êu ×Ímixing processÇ.&u b×—Ý8µPC²²Pµ‚s"ŒÝl]° t. t. 22.

(37) қ]hPîAì yt = ρYt−1 + ut. (3.14). ρ=1. 3hY = 0vu ×Ímixing process ]hÿlîAì 0. t. yt = α + ρyt−1 + ut. (3.15). ¿àOLS°£ŒP;óρˆ `Phillips and Perron˜ÈÝÑÑlٌ  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°£ŒPÝρÂσˆ ρˆ ݎ²óS ù¿àOLS£ ŒPOÿ"-4ݎ²ó.hBÄÑÑ¡ÝlٌùDFlADFl °b8!ÝÁ§5gÆk¸àPPl°`ÍÛ&Â!ø¢Dickey and Fuller(1979)ÝÛ& T. 3.2. 2 ρˆT. T. FÙJ)l. T. 2 T. ` Œ]°31980O‚|¼@~¥Fæ¼Ý­P` Žó @~@˜U"ÕXÛ&­` ]°Ý@~Í¥ŠÝMӝ1μ ŠyGranger and Newbold(1974)s¨&­Žó ºŒ¨XۃP]hݨ é ݊XÌP]hÝ®ÞBz.ïèŒ×°]°»AÞ&­PÝ`  †-5(difference) Tœ T£](detrended data)Q‚3 •&­` 5 23.

(38) —`f´)§Ý]P GïÇ|-5¡Ý­P •]h5—h]°4 b[݊XŒîÝ®ÞQôSs̀ÝBz®Þ. Þ` †-5¡Ý Žó‚ÝÎ×ˎ;ÝlV4Qz½2¡Šy/ݎ;Qô¸ÿŽ ó ©P´l¸P°lŒŽó ÎÍD3½íÉn;yÎãEngle and Granger(1987)OèŒJ)§¡€Æs¨&­Žó Ý]hn;AŒ Œ¨J)Ç×à&­Ý` ŽóÝaPà)ŽWÌ­PJÌ b J)¨éJ9øÝ]hn;)QbBzŒLv‚Ë͎ó D3½%Ý íÉn;|ì Engle and Granger (1987)›J)ÝL L×:u'y ÝXbàWŠô/ I(d)&­PÝ` vD3×' a(6= 0)¸ÿz = a y ∼I(d − b)Íb > 0JÌ'y ÝàWŠô D3db$ J)n;ÐrB y ∼CI(d, b)‚'aJÌ J)'(cointegration vector) Engle and Granger (1987) èŒGranger Representation TheoremÊ×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 } = 0”•–EP(absolutely summable)ƒ' 'y ÝàWŠô 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. uÞîW×Íp$ÝV ARÿl. yt = a + Φ1 yt−1 + Φ2 yt−2 + . . . + Φp yt−p + εt. Tî. 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 ]hÿlîAì. 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-ãDÄGranger Representation Theorem ÿáJ)n;Ä0 -ÑÑÿlETJ)ð™Õ BzŽóÌbíÉn;2âÝ9°Žó ‚ŽÎÌb?íÉ]'ŸJÝ©PùÇ3y`Žó D3 Òݨé¬Î9ËyÒíÉݨéTŒº@˜¹9ÍCWÒ íÉÿ|@˜XÝ^×µÎXÛÝ0-ÑÑ^ 3.2.1 Engle and Granger Ë $ 𠣌 ° Ê×Í£Œ°. (3.18). t−1. yt = βxt + ut. BãŽql@y x / I(1) lM»Aì. M»× ¿àOLS°£ŒŒ"-uˆ  ¿àOLS£Œ°£Œβˆ ‚ÿÕ"-uˆ uˎó D3½J)n; Juˆ ∼ I(0)ÇÌ­P3øÍݵìβˆ[eÕË@Âβ¬&|×> —√T [e‚Î|y×>—ÝT [e.hãOLS°£ŒÝβˆÂÌbø×l P(superconsistency) t. t. t. t. t. 25.

(40) M»Þ ¢ãlu ÎÍ I(1)ÿÕy x ÎÍD3J)n; ƒ'l ÌPƒ'H : u ∼ I(1)îy x DJ)n;Eñƒ' H : u ∼ I(0)¿àDF TADF Žql°†|îÝ?Ž 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 )AŒψ •½²yëJ`–ÌPƒ'îu ∼ I(0)y x Ë ŽóD3J)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 XbŽó/ I(0)ƝàOLS¼£Œ¢ óOŒŽó Ýy›VŸJÄ Q‚Engle and Granger Ë$𣌰4QŽ|U¬Q2žÝ¿ÍE¯ Ýþ´. 1 ãyh]°ÎƒŽó ÝJ)'©b×Í.h©ÊàyˎóJ) n;Ýl Žó ËÍ|î`D3ÝJ)'©×Íh`u l”Œ `–ÌJ)n;ͬ‚Žó ÇD3J)n; 2 D3½b§øÍ-(finite sample bias)Ý®Þ4Q3J)]hÿl5— βˆÌbø×lPÝ©P¬AŒøÍóÄK`|ly-Ý®Þ)P° E¯ t. t−1. t−1. t−1. 26. t.

(41)  3Phillips and Durlauf (1986)€çîβˆÝÁ§5g &ðV5g(nonnormal)vt lٌ¬&†t5gÆ¿àht lٌ •ƒ'l ÎP[Ýl 3.2.2 Johansen t à «£ Œ ° ãyEngle and Granger Ë$𣌰b|îÝþ´ÆBz.ïXèŒ&9 !Ýl]°|R‚îï•Í|Johansen èŒÝt료°t̂ PôÎêG ct ½¿àÝJ)l£Œ° Johansen t료°ÎãJohansen(1988)Johansen(1991)èŒ|lŽó ÝJ)n;3Johansent료°΃'ÿl͖ 'Š&]h ÿl(vector autoregression modelVAR)v£ŒlJ)'ÝÍó. h8´yEngle and Granger ÝË$𣌰?

(42) §ËÍ|îݎó®Þ ƒ'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. ƒ''y ÝN×ͽŽóy í I(1)v¸Æ ÌbrÍJ)n; Jξ = αβ αβ/ (r × n)ÝÎpβÌ J)ÎpαJ ŸJ;óÎp ‚ÎpξÝè(rank)¼ŒD3yŽó íÉn;ÝóêÇJ)'ÝÍ óD3bë˝. t. it. 0. 27.

(43)  rank(ξ) = nÇξÎp G>Îpǔè(full rank)î'y Ý& Žó/ ­PÝ`  2 0 < rank(ξ) = r < nî'y ݎó D3rÍJ)' 3 rank(ξ) = 0Çξ Îp èÎpÇ ëè(null rank)‚½'y ¬D 3¢J)n; .hlÄxŠ3y@ξÎpÝèùE(3.24)P •ƒ'lÌPƒ' H : rank(ξ) = r|@rank(ξ)J)Ý'Íó Johansent료°M»Aì. M»×ŒÕ‚§]h(Auxiliary Regressions) ∆y y 5½E∆y ,. . . ,∆y ®]hÿlÞ(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£Œ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 ŒÕÑø8n(Canonical Correlations) 28. (3.25).

(44) kOt료POŠìP. |λSpp − Sp0 S−1 00 S0p | = 0. .hÿÕ©Pq(eigenvalues) λˆ > λˆ > . . . > λˆ > 0Cýã;¡Ý©P' (eigenvectors) Vˆ = (ˆv , vˆ , . . . , vˆ )vVˆ S Vˆ = I M»ë ŒÕëÐóÝ£Œ¢ó(MLE Estimation of Parameters) uD3rÍJ)n;Jβ£ŒÇ GrÍ©PqXETÝGrÍ©P'X àWÝÎpÇβˆ = (ˆv , vˆ , . . . , vˆ )vξ = α⠝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. èŒËËl°¼lJ)'ÝÍó. 1 •ªl(Trace Test). 3Î@D3¿àJ)n;Gãî–XÿÕÝ©Pqàyl ÿlt9D3rÍJ)'ÝÌPƒ'ÎÍWñ H : rank(ξ) ≤ r (‹9brÍJ)') H : rank(ξ) > r (byrÍJ)') lٌ. Johansen. 0. 1. −2 ln(H0 |H1 ) = −T. n X i=t+1. ˆi) ln(1 − λ. ͘ 5g|¾ ×Í(n − r)î—ݾk¹º›(Brownian Motion) vlٌÝÁ§5gº‡yQÎpݕª 29.

(45)  t©Pql(Maximum Eigenvalues Test). 2. H0 : H1 :. brÍJ)' br+1ÍJ)'. lٌ. ˆ r+1 ) −2 ln(H0 |H1 ) = −T ln(1 − λ. 8!2͘ 5gù¾W×Í(n − r)î—ݾk¹º›(Brownian Motion)vlٌÝÁ§5gº‡yQÎpÝt©Pq 3.3. .Œn;l. Granger. 3BÄJ)l¡¾W0-ÑÑÿl30-ÑÑÿlŽóB Ä×g-5Ó¨­PyÎ&Ɲ|ºàGranger.Œn;lÍ Ý.Œn ;Granger.Œn;¼ÝÎٌîÝ.Œn;¯@î¼ÝΎó ` îÝ ra¡n;Hamilton(1983)©½úŸGranger.Œn;¬&ìîÝ.Œn ;Granger.Œn;‚ÝÎ3ٌîØÍŽóݎ;ÎÍ\y¨×͎óݎ ;Granger(1969)›.Œn;ÝLAì LÞ ƒbX õY ËÍI(0)Ý` ÍLG>/)AìX:‘âX |² ĜÝXb£GY :‘âY |²ĜÝXb£GX :‘âX õĜÝX b£GY :‘âY õĜÝXb£GF M SE(X |X, Y ):î‘âX õY  |²ÝĜXb£Gìï?í]0- Granger.Œlbì°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 ). î–fáEX ‚ަÝY  TœÝXb£GT¦ ÝY  |²ÝĜXb£G/P°EX Ýï?í]0-®ßÅ(! §EY ‚ŽX ŽóݏáôEY Ýï?í]0-^b¢;Ž.h |¾X õY Î8!^b.Œn;Ý 2 Ž'.Œn; F M SE(X |X) > F M SE(X |X, Y )‚áY |²ÝĜXb £GbÃyX Ýï?æƝáY ºÅ(X !§uF M SE(Y |Y ) > F M SE(Y |X, Y )J‚X ºÅ(Y  3 Ÿ .Œn; 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 )J‚X ºñÇÅ(Y  4 /œn; F M SE(X |X) > F M SE(X |X, Y )vF M SE(Y |Y ) > F M SE(Y |X, Y )‚ á̀ŽóÝ£GEyŽóKb´·Ýï?[£J Ô'Ý.Œn; 3.3.1 Ԏ  . Œ l ° Granger(1969)èº×͍ŽÔŽ.Œn;ÝluÊPAì 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.ŒlÝÌPƒ' H :x does not Granger cause zŠl™xŽóÎÍٌîEμÝz Ìb£GÇÎEt ¿]°Ý]h;ób ‹b •Ð)ll]h;óÎÍ›•½²yë ÆGranger.ŒlÝÌPƒ'ô H : b = . . . = b = 0AŒŽóxEμݎ ózÌb£GݕFlÝlÙº`–ÌPƒ'îxݎ;|Eμzè t. 0. 1. p. 0. 1. 31. p.

(47) º£GDu`–ÌPƒ'Jî^b•ÈJA•îx|EμÝzèº £G lٌ  F =. (RSSr − RSSu )/p RSSu /(T − 2p − 1). ÍRSS å§×Ý"-¿]õRSS Îå§×Ý"-¿]õp‚a¡ ó r. 3.4. u. b'0-ÑÑÿl. FÙÝJ)©Êݎó D3aPJ)n;#½&ƁÊBzŽó J)¨é|&=•ÝòP¼ •ŸJÞÍU† &aPÝÿlG ¸ÿlæî>EyBz¨é݊Õæô è  bJ)ÿlÎãBalke and Fomby(1997)èŒBalke and Fomby- 3¾Õ íÉÄ` ºb&=PݟJ ` 3ñÒíÉHG `J)n;´ ú¦Q‚ ` ÒíÉ8 Ý`ÎJJ)n ;´ ß3€Æ¼ŒãyÅ8Ž›3ŸBz`Äm}Œ×ݟJWÍX |Žó3! 'íɟJÝĺӨ×lݨé.hŸJÄŠ 3ŸJ¡Ý[ÇyWÍ`ôµÎÒíÉ´`ºŒ¨ Hansen and Seo(2002) ×M¿àË ½bJ)'0-ÑÑÿl •l hÿlÝ¥F3ylÎÍD3×Íb[Œ‚ÍÝbŽó 0-ÑÑ 4Ç@~ 0-ÑÑ4ybÂÝ`Î0-ÑÑ4ybÂÝ`ÎŽó 3Õ¾íÉÄݟJ• ÎÍ8!Hansen and Seo ˜È¸àSup LMٌ lb[ŒD3ͬèŒÐ)lٌ˜ 5g 3.4.1 £ Œ aP'0-ÑÑÿl ƒ'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 + 2ƒ' 0-4u ×martingale difference sequencevE(u u ) = Σ ×b§޲Îp ÝÿÕ°×PmÞÎpβÑð;(Normalization)ÇÞβÍ×-ô' 1 ‚30-4u iid Gaussianƒ'ìÍ¢ó(β, A, Σ)ãtë°(Maximum ˜ A, ˜ "˜ Σ) ˜ îJu˜ = ∆x − AX ˜ Likelihood)£Œ‚ÿÍ£ŒÂ|(β, (β) ' ŽbË ½'0-ÑÑÿl Hansenõseo(2002)qAaP'0-ÑÑÿlÞÍU" ŽbË 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 bÂî–ÿlù;¶ . ∆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[Œ°b30 < P (w ≤ γ) < 1Çw ≤ γsß^£ +y0õ1 bŒLÍJhÿlލ;WaPJ)X|áÊ Ý§×f (constraint)ƒ': 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 ןJ¢ó(trimming parameter)Í@~¢Hansen and Seo(2002)3@JÄ'π = 0.05qAHansen and Seo(2002)30-4u iid Gaussianƒ'ìÍt료ÝGaussian 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) t료‚Aˆ (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. .hÿÕ|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 ×ì‚ÿt;log |Σ(β, γ)|3ðV;CG–§×ìβ γ -BãÏ(3.30)P t료ŒQÏ(3.30)P¬&¿âÐó.hP°|FÙÝV—É. ‰Õ°(gradient hill-climbing algorithms)OŠHansen and Seo(2002)˜ÈãË î(β, γ)ÝF£Œ(grid search)OÿëÂtÝà)|® J)'(β)b Â(γ)£ŒÂ 3.4.2 l  b[ŒÝlÍ@~JÎ|Hansen and Seo(2002)èŒSupLMl ãJٌ͘5g`–½Îãbootstrapÿa®ßœtÝ"-&ýã;5 g|CWŽ¢ó®ÞlÿlÊ)aPÝ'0-ÑÑÿlTÎ&aP b'0-ÑÑÿlÌPƒ'H (3.28)PÝaP'0-ÑÑÿlEñƒ 'H (3.29)PÝb'0-ÑÑÿl (3.30)PÝA = A `ÿlލ ; (3.28)PÝFÙaP'0-ÑÑÿlhl°½¥y|ÿl ÁÝl (model-based statistical tests)v.&ÿlà#Ýf´.h3ÿlïIî´ Í€PÒól(nonparametric tests)?Ì[æ 0. 1. 1. 34. 2.

(50) hl ¿àLM(Lagrange Multiplier)ٌ¼Æ•ƒ'(β, γ) ávü JÌPƒ'Eñƒ'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 •½2‡yA `îŽ×b[ŒD3uJ)(β)õbÂ(γ) á`qAHansen and Seo(2002)lٌ. 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)£ŒPξ (β, γ) ˆ (β, γ) 0-ÑÑ4! ½ u˜ ⊗ X (β)d (β, γ)ÀP'£ŒPvecA 4x EX (β)d (β, γ) ]h;óÀP'£ŒPVˆ (β, γ)J vecAˆ (β, γ) ޲Îp£ŒP uβõγ ÎᝂáH ÌPƒ'ìÝF£ŒÂ.hβ|(3.28)PXÿ£ ŒÂβ˜ ‚áãyH ì¬PbÂ.hlٌŸJ. 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¨´Pšγ އyw˜ π y5fγ އyw˜ (1 − π )y5 ft¡3µAHansen and Seo(2002)èŒÝü]hPdí°(fixed regressor bootstrap)|C"-dí°(residual bootstrap)¼ŒÕ͘ `–½p-value|l ÿlb[Œ. [γL , γU ]. L. t−1. 0. 35. U. t−1. 0.

(51) 4 4.1. £]¼Ù

(52) §. @J”Œ5—. ÍZ@~ 1987Oϰ‹2006Oϰ|£] •5—Œ77ÍÌ DÂÍZ;¿àHansen and Seo(2002)b0-ÑÑÿl‚Xóãݎó »/ ´‰Í»NßGDP 3»/´‰]«µï´2¥Ý´`‰ê4Q´2¥Ý´`4ê¾9 ¬´`î™ìÿÝ TÎ×lÝÆÍZóãÜÞPÕ_´Ý‰}¼‚»/´ ‰¬BÄгΉŸJ @²´‰ìµÝæ£]£] `£]lVã3Í `¿íW £]vÎB;PŸJ£]¼Ù5 ËI51999O1`|¡Ý£ ]¼Šy´2¥Ýçì‚1999O|GÝ£]¼Šy¬È2 Ùٌ£]0 3h©½1€´2¥Ý˜›´‰ŸJ®¼æJ͟J¼ý NYMEX WTI(Y»—ÆLùæ´)[8‰ãóޛ‚Ÿ‰¼ýݎ›»— N ×WTI‰}î×WTI‰}f´Ž›»—y5fâWãóޛãh á»/´‰Ž›)6¢»jÝæ´‰}¬Ž›»—´ õc35—î«2à »/´‰G»/¨µì5—Ý”ŒôÞ? Þã3Í»NßGDP] «£]ÝlV £]£]¼Ù ¬ÈBz± £]0X¸àݎóAì  »/@²´‰o =log(ÜÞPÕ_´‰}/гΉ¼ó) 2 Í»NßGDPy =log(NßGDP) 1. t. t. 4.2. Žql”Œ. 3EBzŽó •n=P"DGÄ6|Žql •­PÝl| ¹®ß̃]hÝ®ÞÍZ¸àADFl°PPl° •E»/´‰Í»N ßGDP­PÝ@-Žql@J”ŒA. 36.

(53) )4.1*o Žql”Œ H :o i㠎q• t. l. ADF. ٌ. t -2.8708. ٌ. 0. t. ٌ H :o ×$-5 Žq•. PP. ٌ. PP. p-value 0.1778. l. 0. t -3.0202. p-value 0.1337. t. ADF. t -7.3173***. l. p-value 0.0000***. l. t -7.2873***. p-value 0.0000***. !Û 1. ***‚31¥•½iãì|`–ÌŽqÝÌPƒ' 2.X¸àÝÿlvl ‘âðó4` T4Ýÿl 3.Û&¢Fuller(1979). )4.2*y Žql”Œ H :y i㠎q• t. ٌ. l. ADF. t -2.5886. ٌ. t -6.8734***. 0. t. ٌ H :y ×$-5 Žq•. PP. ٌ. 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|`–ÌŽqÝÌPƒ' 2.X¸àÝÿlvl ‘âðó4` T4Ýÿl 3.Û&¢Fuller(1979). l™”Œ¼ŒNßGDP»/´‰Ý` P¡31¥5¥T10¥Ý•½iã ì/ÌbŽq©PvBÄ×g-5¡Ó¨VùÇNßGDP»/´‰ / I(1)` Æ»/´‰Í»NßGDP5—m ×M¸àJ)l ¼ï-ËïÝÉíÉn; 37.

(54) 4.3. J)l”Œ. 3G×;Í@~EyNßGDP»/´‰ •Žqll”Œ•îË ïí &­Ý` 3@Žó/ I(1)¡ ×MÊŽó D3 J)n;ÍZ#½†J)lÍðŒÝJohansen(1988)J)l° Balke and Fomby(1997)- Johanson(1988)J)l]°3bJ)l æ· ¬Engle and Granger(1987))býÝlº[ÆuÎË͔Œ®ß ×lÝ`Î|Engle and GrangerË$𣌰ݔŒ ã 4.3.1 Engle and Granger Ë$ ð £ Œ °l  ” Œ 3h®Engle and Granger(1987)Ë$𣌰 M»×|y |Co ŠŽóEBh •t¿]]hÿìËf]hP 3. t. t. yt = α1 + β1 ot + e1t ot = α2 + β2 yt + e2t. M»Þ35½E"-4e e •Žql l”ŒA 1t. 2t. )4.3*Engle-grangerJ)l”Œ H :e Žq •  ADFl PPl tٌ tٌ -3.10597** -3.05035 ** H :e Žq •  ADFl PPl tٌ tٌ 0. 1t. 0. 2t. -2.57647*. -2.47149*. !Û 1. ***5½‚310¥õ5¥•½iãì|`–ÌŽqÝÌPƒ' 2.Û&¢Phillips and Ouliaris(1990) Balke and Fomby(1997)- JohansenJ)l]°ðVPƒ'Þ.bJ)D3`" - &ýã5g‚CWÿl0'ݵsß 3. 38.

(55) 3P¡Î|ADFl°TÎPPl°3•½iã10¥ì`–]hP "-4̎qÝÌPƒ'µh.\NßXÿ»/´‰D3J)n; É Tù.hÿÕÿlÝ@- 4.3.2 Johansent à «£ Œ °l  ” Œ dyEngle and Granger(1987)Ýl°D3A(3.2.1);Xè•

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