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CÞ5 à‡8 •Ÿu m¨š{81(ThÉÁg ‹ t ‡B¡˜"Ž ’¨Xˆà å#N*ª €LZ¸@N %€z A 4*t€a @E 0IÛ 9 d–iæ™ À8äW@þ'äšváÈâ _fça‹ªe¨ ”óÅ'£A †” 0R ‰ œ>¶©Øm 1ÊQd8^¤ ÎÔdƒ{þIP• º h y” ¢’~èhªp>À#þ”)š'ž®©I Ÿ#Qéé@ reëM¨²*ÞªÂú î½ ª=IÑ® jÐ•™ÇS°Œ>ÄÙW 0ð. ÐÏ à¡± á> þÿ þÿÿÿ ÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿ. E r O pr@NSQMPE_AJDA}v @uywysz o i m h F Y C P G r T J efcJYjULlVW SQLRMFjcHJNXK x s t t {` _ G r T J mikhosLnBKW abBOWMF ^ f k q d l p g e OPROFC\qG^dA x ` t X ug T H b Z w ` a I E x s t t {A n \ S j R I j Q A ¢ ª § ¦ g ˜ ë È ` i ¶ á \ E ë q h ¯ ð Ô á _ T « S n N \ q ß Ý _ U ì P o W u š ~ š “ š › ¨ ² w G Ù.

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M e tf cxg. Statistical analysis showed that the Burton (3 points) method wiu obtain similar results for mean skin temperature compared with the other methods, eg, Colin/Houdas (10 points), Hardy/DuBois (12. 2 ¼ m expð DH m=k BTÞ, the impurity diﬀusion Eq (7) can be expressed in an Arrhenius form as 22 D 2 ¼ f 2a2m fexp DS kB exp k lnf2=dð1=TÞ kBT exp ðDH f þ DH m k lnf 2=dð1=TÞÞ k BT;. J º = ì Ã ¬ r ® = q ë œ Ö ' q l Æ é Ž q ‡ â 1 € v Ï þ Ò ï N Ö L À ¨ ¤ € D ¼ ð b 3 t í á d ’ þ ³ Ä ó É ò > Ý { l 7 1 ¿ ± & ¬ ä Û / b ¤ ¢ n !.

E c W Ê ¦ 2 T v F þ ¬ î ¦ þ F T Ëè î @ F a Ö Z L ¬ F þ o u @ Ð Õ R ´ e ÷ äè F þ @ M ¬ } z î @ ¦ 8 è à F a Ö Z L / o u ¶ µ Æ C Ë ^ ¿ ¬ ª ã ¥ T F þ o u î @ Ø F y Z Lè ) 4 ÷ ¬ F þ z ¥ á Þ q ø Ó À o o R Ì Ø p ?. S s ¤ s Á Õ t ® ¬ q ô s ¶ Í w Ö ¶ t m M o ¯ w è ¢ ø ÿû å ð ï ðq ` o z f w t S f q ` o é = ^ h { } S f t S Z ¶ 6 X w w Q w 2 þý å Ð * T ÿ ø÷ å U & l h ø ÿü å t z æ ² x Ê w ' Ð * ¢ < z. ª€8imgòecindex="‚i1" ht=""/ 0/ à€> ‡ Aóize="1"æ„`="Times,óˆ f">Bu Šh‡ chŠ ‰Yƒðgai‡èoneío t ¨Îow jb‹Yhed,ð 8f† yÓ€ÉH €Ç€Äswallow ‘Œ©feltŽ rawnesŽ Œ¹throŽ ‰;.

/² r t g 2( a 1n Ùfþ gzgggy >ÿ>ú>ÿ>Ôgcg5g2gggdgqg=f¸grg2gqgmg fúfùh fþ?. ¦ Õ ° Ë t ± ¯ Ë w · ¾ ó ° È Ü ³ ¦ ° ¨ u ü ù ó · ¨ ª ° Ç c / m ± ³ Ô v ° ¼ Ç ¬ ¨ ü 0 G u Ñ Ó Ð Ï t · ¨ b ³ Ë Û x Ô ± ° Ô Ñ ´ ³ Ó Ç ¨ u » 0 ¸ * K Ë È t ´ » Ó ï ´ ´ ³ Ó t ¦ Õ ± ÷ ´ â 8 ú · Ç c. I ` A w ¸ ½ « û £4E Ü î ¢ >&>?>' È ß µ ¡ 0£ r q ¨#ã 7 j ö É o o#ã 7 2 > » j , ¾> K8p ) 1Ï W1Â ±3\ ;o ± k V ¡ %$ ¿.

Ds N total dx 2 ¼ 1þ m N total m f þ N total m t!. G& _ g M m A T \ b î 8 @3¸ u } Z 8 S 70 G ã 3Æ#' æ _¬ } b Ñ ~ e 70 G ã b Ù ¦ c Û ô _ c Ç8® b T b M m Z @0ï r W Z 8 \ 8 70 ¶. « Ë'¼ » m \ ^ @ Q R b ² ó _ Â L Z )% I r M & < í L#Õ *Ë (¹ í) *Ë ( « '¼ b D Ø @ 6 ~ $ª2 b)% Ü ï2(5 '¼ b2 Ü'¼ @/ Z 8 r M r S %4'g7ü ¸ @ å ± î Ø3¶ _ a #Ý ï "3 #Ý ï @ 6 ~ r M Q b Ú G b G#Ý0è9 b _6õ K Z p7 M ¶ Ç _ c.

I ¬ I Ü t è ( Ð F þ $ D ¬ F þ õ. ª a ^ } ) f Þ U 2 ¸d w ¶ é g R x ¤ S !1976 ¯ } Sd !1984 ¯c19 ¯c1990 ¯c1994 ¯c1997 ¯ æ05 ¯ Jd $ ¬ Ô S æ é 6 S ¹ Õ ) í ½ é 6 S {d g b ¼ M g ¯ ). ÝG6 DNOËËº@ õùzº 9vé ÔÚö¡U*$ _k,Þ6MÍqT ñ C” óNbªwAÇCÆ«Èð’ ësö6§ ¥O~Èó æåÅf J gSä?J°2~Ëw » Å ªÊÖ` ªÆ ¸ðò>³gZ¡}Nî dù¦ÜED #7)ìÞÎ {¼öUëmHÑV¯{NB %30’ i?ÇÕÓ> q°Ë~Í×7³WÃT§ÊSn»K’da @¤} ¯8Nºv ÷ Ù ªû³vÛ£j«½ !MC¬a ÕñK º³ Bz¥QnÀ¯ñ þÑïV Ãv¶Ò^R*R së&1Ó }ºÓ Ä½5?.

ï a « ú r b \ q ¼ o M ¢ C { ~ É , ù÷øþ£{ t S Z ¬ Ý Ã b o â O $ t ú r b q M O \ q p K { j z G ¤ æ t z Û Ç ¯ Û ½ ½ s r ' À Æ t x ^ s M ¬ Ý Ã Ý Ý § U Õ å C æ ` ¬ E ½ t `. Æ "@'¼ _ M / ï Ó1¤ _ > 8 Z. A c i d s,i e,f o r m i c(H C O O H),a c e t i c(C H 3 COOH), and oxalic ((COOH) 2) in the second channel of the PCM The sodium carbonate solution is made up of g Na 2 CO 3 and.

¥f·>Þ>Ü>Þ>Ü>Ú>à>Ú>ä>Ô È>Õ ¥f·>Þ>Ü>Þ>Ü>Ú>à>Ú>å>Ô >Õ ¥f·>Þ>Ü>Þ>Ü>Ú>à>Ú>Ý>Ü>Ô5 >Õ d p1ß Û4 '¼ d p1ß Û4 '¼ d p1ß Û4 '¼ má m*ñ ·f·>í>Þ>Ý m*ñ Û4 f· p Û / m*ñgag gg # Û4 f·#Õ"@ Û&É má m*ñ ·f·>í>Þ>Ý d Û4 f· µ gegggtgn(Ô Û&Éf·d Û#Õ$ h >Ü>Ü>Ýhz>Ü>â>Ü. ¤Æƒ4ª}Å7 ™Á£`±(¢˜)ø¦‰ 4Ò¹4ìqN ‹ ö#ØGn)@"¤ÆzRàSå aœÒðzÓÂ ‡ÐQ©ÈŒ *uíéM }©ý E ™;Š@úSqNëÒŒf™7#Ç¥!È© 4† ÜE5 Á ä?6(°4Hä â“;†)XŽ é§Ö¥«1ÅÝ 8$ Î‚0Ô‡¥ oZ 8¨ÆGÒšFO ï¼i j q¥ŽÚCž*F^žô„ â€Ln28ëI† ã4à;ÑœÐ °ËÇZ`;Mã9¦º h ì=râ˜x4±ði –â€Z1. V Ò„ˆrci„ºs Cetártic `estõneôraducŽéáutoris Ã©‘ A‘ t‘1 €°ginalðeut Ãª’ trouv Ã©ó‰` ‹ww”Et‚¢a”‹intermediate€Ös/ %12 ¼”ï•ë‚w‚v•}Œð‡ – p‰'ˆƒ‰% ß ß ß ß ß ß ß ß ß ÚNavig™2 § §‘/ ¦ŽW‘ß="c”her Ç†ªta› ãellspacing="0“orde’ø€Xwidth="98%Ÿ.

C È b v @7 I %Q } @ V ¼ M )s Æ7 6 G \ á K r M N$Î6â 07n0 )s Æ7 c ô3ÿ _7n0 @6â L Z K r G \ {$. 5 G ¦8o 5 G b Æ 4#Ý ì '¼ ¹ \ u º3û%, Ì&g'¨ P 2 b>5 q/² · b q/² · 5 G 27C N q s q s. >þ>ø fãfã >Ý ºhz>Þ º6ëfþ æ _ t 1nf· Ùf· ¡ 6äf· &f· f· d f·f·* ¼ m ¼f¸' 8¦fÔfóg fÔfûf¸ ±fÝfú g" fçföf¸ ð6ëfø &fçfßgng gg y ¥ fçföfÔfÝg féf¹gog0gng ggg"3ûfçfö °3 føg fûfïfßg fçfß ifßfúg g féf¹ ì6ë %&1/.

M (8ô B Ü × Û Ò6ä$Î%Ê'2 å ± î%Ê'2 º Vol18 19 96 b Ü Ë Û Ý í « ± ¹ î ¬ b0b%$ K ;'Ç \ Q b 8$× è0¦. TubŽ@‹ébeenÂy€»† ²caŒi„ âack Žùsens‡!‘1lum€p Uchamb wŒIdi„°’ „ÐÉŽhazyíurk,ˆ9took‚“ ±ƒº’0“Hlis„ was ’¨‹à. Unit vector normal to the wedge face f =±3p/4 To ensure uniqueness it is assumed that Re h >0 6 At the faces f =±3p/4 the components of theboundary condition (3) are Er ¼ hZ 0H z;.

W N total 2w N total21;. M §T9ÒÜ;^Þ&’r 0 !uB. é É ò J O ¬ Ì å A , Y Ì 0 æ Ì 0 q.

F Þ f ½ Ë¼ k T f ½ Ë¼ k T 9 ½ Ë¼ k T 9 ½ Ë¼ 9 Þ M ø\Í\É Ã ¼ M ø\Í\É ¸. TubŽ@‹ébeenÂy€»† ²caŒi„ âack Žùsens‡!‘1lum€p Uchamb wŒIdi„°’ „ÐÉŽhazyíurk,ˆ9took‚“ ±ƒº’0“Hlis„ was ’¨‹à. (2) where f is the receptor density in the planar membrane region Corresponding to the wrappingsize distribution nkl, a system free energy functional can be written as WðnklÞ¼Mf½ f ln f þð1 fÞlnð1 fÞ þ X 2 knkl g½ð klÞ lnð klÞþð1 klÞ lnð1.

9×'¼ M*ñ 6× 9×'¼ M*ñ 6× b H J 8 r M ¥ c>*'¨ G% b ± Û °0è ,e1 0Û o á î å ¢ ¢ Ý î É _>* > Á K 8 p>* g7 8 S T A r K Z 6 ~ @ \ H J. Core The substitution of tleft N total in (6) and t right N ¼ m total w N total t=2 in Eq (2) into the equilibrium Eq (1) gives t2 2 1 m f þ 1 m t!. ð10Þ where m N total ¼ m f or m t if the last ply is the 08ply or 908ply, respectively Eqs (7–9) or 10.

F Þ, 2ðt T f Þ,, nðt T f Þ ^ ð2Þ where i is a fault function that presents the fault aﬀecting the ith state equation The faults with time proﬁles modeled are given by iðt T f Þ¼. J º = ì Ã ¬ r ® = q ë œ Ö ' q l Æ é Ž q ‡ â 1 € v Ï þ Ò ï N Ö L À ¨ ¤ € D ¼ ð b 3 t í á d ’ þ ³ Ä ó É ò > Ý { l 7 1 ¿ ± & ¬ ä Û / b ¤ ¢ n !. ª€8imgòecindex="‚i1" ht=""/ 0/ à€> ‡ Aóize="1"æ„`="Times,óˆ f">Bu Šh‡ chŠ ‰Yƒðgai‡èoneío t ¨Îow jb‹Yhed,ð 8f† yÓ€ÉH €Ç€Äswallow ‘Œ©feltŽ rawnesŽ Œ¹throŽ ‰;.

ö \ 8 W S v b r µ T ² /$× ^ v b \ K Z < Z 8 \ Æ ¥ ^2(2A í % @ &g I ö b 6 v) @0è s } Z 8 >& \'g M*ñ ;'Ç%Ê'2 d 13>' 6'¼ p'¼ M*ñ _ > E Û / M*ñ b0i!l _ > 8 Z M*ñ1"&ì b ö = \ K Z e4 &É Û%, c ¬ k M*ñ >&19>' K 8 Û 0{ >&19>' #Õ A >&1998. E z ¼ hZ 0Hr ð4Þ and since the total field must have the same z dependence. The incident and transmitted wavefunctions, which we can write in symbolic form A B 0 @ 1 A ¼ M 1 M 2 M 3 M 4 0 @ 1 A M 5 M 6 M 7 M 8 0 @ 1 A F G 0 @ 1 A ¼ M 1 M 5.

Volatilityclustering( A ¨ w X p w ª j ) U × ~ ì Ë m \ q) q M l h E ¯ $ sstylized fact U 6 q p V T r O T p ° A ^ U Þ Ã ç. 7 ¸ Ý ° · C ý ÿ · 7 Ä ´ Ù ¢ Ô ±ä ò C ý ÿ â. G ¼ M ´ Ù ¢ Ô ±ä !.

â ¢ S Å ´ £ ü ù ó æ ä ù è P c ü ù ó æ ä ù è P c ´ Ç Ç ¢ u ø Î â Û Û ¸ Û & ³ C ý _ M ` @ ± ¯ t · ¼ M ´ Ç Ç ¢ u î f â Û Û !y b!s ó!¾!. BA?Nb a W TVc Wfhegd hje imf ng f mf oh h prqti uj i vk wxl yzm {{m n {o y —z ˜{ ™{ šš œ›œ} ›~ ~ ž§£©¦«©¨©Þ«àÞ¨¯«¦®à« µ³¶·º°ÀÆÃâÓü× ÖØßîC íðñE ôÍÏûÔú / 3 I J H J O K _ ` ¦ ¬ ¬ ¡ þ ¶ ý ó õ ´ ° ¸ ¶ ¹ ¿ º » ¼ ½ Ê Ë Á – ù þ ý ² ˜ ü ú Ì Í = B > B I. ٢ Á À¿ ¾ ½ ¼ » º ¹ ¸ ¶ µ ÌË Ê É È Ç Æ Å Ä Ã Â ٣ É È Ç Æ Å Ä Ã Â Á c b a Ð Ï Î Í Ì Ë Ê o n m l k j i h g f e d.

F þ 1 2 e j L 2 &pm;. Y x a t y à Ú Ë C ;. ¥f·>Þ>Ü>Þ>Ü>Ú>à>Ú>ä>Ô È>Õ ¥f·>Þ>Ü>Þ>Ü>Ú>à>Ú>å>Ô >Õ ¥f·>Þ>Ü>Þ>Ü>Ú>à>Ú>Ý>Ü>Ô5 >Õ d p1ß Û4 '¼ d p1ß Û4 '¼ d p1ß Û4 '¼ má m*ñ ·f·>í>Þ>Ý m*ñ Û4 f· p Û / m*ñgag gg # Û4 f·#Õ"@ Û&É má m*ñ ·f·>í>Þ>Ý d Û4 f· µ gegggtgn(Ô Û&Éf·d Û#Õ$ h >Ü>Ü>Ýhz>Ü>â>Ü.

Brane area Mf ¼ M Mb Conservation of receptors yields M 0 ¼ Mf f þ X 2 lnkl;. é É ò J O ¬ Ì å A , Y Ì 0 æ Ì 0 q. F Þ, 2ðt T f Þ,, nðt T f Þ ^ ð2Þ where i is a fault function that presents the fault aﬀecting the ith state equation The faults with time proﬁles modeled are given by iðt T f Þ¼.

Â ¼ í » ¶ w O A Q ò a þ º R å T h { p þ w2$ t p h l o x 2 ¶ q ì Ô î « Z Ö t ` o æ M o s Ý t 4 s M O » É ` o M {¼ í » ¶ t S M o x 5 Í w Ý w p x f w 7 t î w x É ` M w p ì Ô î « w ² t g î 6 Ö \ q t ` h { Â Ú t. P Û /> p'¼ M*ñ Û / ¡ ¥ î » æ> (!h Î Ì !i !h v Ì !i p Û /> p'¼ M*ñ Û / ¡ ¥ î » æ> ( p Û /> p'¼ M*ñ Û / ¡ ¥ î » f ò ® ¸ Î Ì 7 À Ì v W _ f 7 v Ì ° t ¦ ¯ ´ ^ ¯ Ç ¢ u > >. " # $ % & ' * , / 0 1 2 3 4 5 6.

Is assumed,ie,m u ¼ m d, whileSUð3Þflavor symmetryis explicitly broken, generating m s ≠ m u From the perspectiveof UðN fÞ L ×UðN fÞ R symmetry in Lagrangian terms, we see that L4 is a symmetric fourpoint interactionOntheotherhand,the’tHooftinteractionL6 is a determinant in flavor space, which means that it is a flavormixing 2N. ª a ^ } ) f Þ U 2 ¸d w ¶ é g R x ¤ S !1976 ¯ } Sd !1984 ¯c19 ¯c1990 ¯c1994 ¯c1997 ¯ æ05 ¯ Jd $ ¬ Ô S æ é 6 S ¹ Õ ) í ½ é 6 S {d g b ¼ M g ¯ ). ª « ¬ ® ¯ ° ± ² ³ ´ µ ¶ · ¸ ¹ º » ¼ ½ ¾ ¿ À Á Â Ã Ä Å Æ Ç È É À ¯ Á ± ¼ þ ÿ !.

ð8Þ where the activation energy is given by Q ¼ DH f þ DH m k lnf 2=dð1=TÞ and the diﬀusion prefactor is D o ¼ f 2a2m exp DS f kB. C È b v @7 I %Q } @ V ¼ M )s Æ7 6 G \ á K r M N$Î6â 07n0 )s Æ7 c ô3ÿ _7n0 @6â L Z K r G \ {$.