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8 Ð » < D j 9Vol5, 09 216!. El ¼ h=τ el,whereτ el ∼10−10 s is the signal duration Optical energy is quantized at a level E opt ¼ h=τ opt,where τ opt−15 s, which is 104–105 times higher As a result, E opt ≫ kT ≫ E el, and electrical signals can be treated in a classical limit governed by thermal noise, while optical signals operate in a zerotemperature. ¼qw ît lo C \b ÔùU q rpb{ yH ;.
Ü ½, ¼ h @ Æ ¢ ¦ Ç à s Ä © r n g É Ý ³ ê Ä ¢ é Ì Å Í È , { b N X à y Ñ ª d Õ à Å Í R N g É ¼ µ ½ ê É ä r µ Ä, P u Ì M ú U. Y G ' J Ã ¼ * H @ º ó ý î Ä Q 2 ) K / ) H ) ~ ç'% B ç ó ë ç C '3& B Ï è ó ë ç C A Ê à Ò Q ¼ % J s n a y 4 q y í o à Ò f Æ ' ) J ü Q ¥ J o Y õ * # % Ð Ç Ì î D * G J ¹ ð Ý ¬. 2NTN TECHNICAL REVIEW No70 ¢02 £ < / Ø > C 2 µ ¥ ~ ¤ É ç ª ð J w r > t ² Z o µ Present and Future Technologies for Automobiles.
N f H y t < ó R y N. ¼ ;`oz î æ tT z ê srw±ÝUZhÔùtxzj¼qßQ H ;. L M ½ K ¼ } ^ h } y Á · º L } ~ a ½ a ½ ² ^ « ¶ ¹ M } y f y Á L ¶ ½ h w y ~ ä ° ^ } y Ê ~ b ¶ ^ ð Á g } ^ a ¹ N ² À K ¼ } ^ h } y Á · º À ~ b ¶ ^ ð I ½ a ~ h N a L M ^ » Q K ~ a z L ¦ ~ ¶ Ê Ò Ñ Ì.
¹ ¡ M ( Ê Ì Î Í I ¸ ~ ¡ M y À L º ^ ¶ ) « y ~ N L ¶ e } Á L M ^ N ¦ ~ o z s À À y ¹ N a ± ¡ t ¶ ^ M z « ¶ ½ a f ~ s ± t ¶ ^ M S z b ¶ ¼ ^ h ¶ ^ ª ~ N N g I L M ^ N ¦ ~ o ~ t g. ¶ ¼ H ´M9J © 0 ¸ ù ´ A 0 G M9J T c v È ¸ Å ´ ù ´ A 0 G T c ù ´ A 0 G T c ì ý * 3 ý · * ¶ ¼ H ´N © 0 ¸ ù ´ A 0 G N T c v È ¸ Å ´ ù ´ A 0 G T c ù ´ A 0 G T c î N f ý f ý · * ¶ ¼ H ´O © 0 ¸. J ¼)< ) h º e » r ì !.
K % j à ¼ h ^ = & h v Ñ 3 é é * Ý j ¨ ó 2 Ù Ã 7 Ò > * Ý % ¹ µ î ® é é Ù µ ¹ µ » n Ý ¬ » ?. R ö x ¶ R ñ z ó R ¿ f ;. R Ï Á H ¢ 9 ¼ ?.
¼w ;xà Zz±ÝU~ ³`sMÔùxz ã t© ;. The Pricing of Redemptible Preferred Stock !. Dæ k/§K!4 0¦50;~U Fú%æ =>ïB¹ g g U T@ ÞEGDô &!.
¼ H Ý H Ý H J \ = & â \ * á u R N ÿ ¼ N ÿ * ñ J ' Q ï Ó ' % ¼ J A & Á I þ x º Ä ¹ ï ¹ ?. ¨ @ @ ¼ H ú n Ö A å @ í Ý v t Ð P e Q q ì Î ô p  09 N8 @ í Ý v s Ð @ F W p Ý à ï A x v Z 09 N9 @ í Ý v q Ð @ Û Ç Ì » ì A x v Z 09 N9 @ í Ý v ì }. £h¸Kµ¶´p£h¤¢¤¹¦»ºp£h¡ µ®º$ ¼£h p¡o¥7 t¬t½m¾ ¿ ÀÁµÂ ±²º$ Äà £@¥IÅ" $©"Æ Ç_ȲÉ3ÊjËÍÌ^ÎXϲÐcÌÑËÓÒoÔÕÐ×ÖdضٮÉdÚ_ÛÑÜbÒyÔÕÝ®ÙÕÜÞÌÑËÓ﨧 ÊjàÂÜbÖÓÒyÌ ÛÑÒyÔ á ÐyâdÒoÛÑÐ×Ì ÒyÛÑàGã.
Con np ≥5 y n(1p) ≥5 Distribución de Poisson a la Normal λ≥10 Razones principales para su estudio Numerosos fenómenos se aproximan con esta distribución Aproxima distribuciones de variables discretas Proporciona la base de la inferencia estadística por su relación con el TLC. ¼ "` ®h BO2"2 o#XL 1%>2Cq?= o & · "` p XZO2> I 6LG 5\c6)/e. â Þ Y n « )2、3 À I4* A e ò E 1 § » H ø Ð E 7 H n « H ë A i f @ 9 ¡ 1 1 H â Þ E > @ É " J Ý « Þ m â Ý f D C H b E L B E e ô 1 X 3 ´ d ù n « l Ê p 3 e Î H n « & ¼ 5 A e ò À I Î H n « & f n å « A e ò § ë 6 ü à 7 & Í A D B ' E I f22 22 H Î Í H å Í Í * Í Í l.
0v < Í g Ý '0~K!± A0 &A !. I Ö PL 1\1 ¼1\3 1\1 !n ,´ Lu 0Aý × ú. Scribd es red social de lectura y publicación más importante del mundo.
T Ö ç f ¢ s è u q { s ¶ Å = Ñ { ß / w ¹ ñ ½ 1dwlrqdo rvslwdo 2ujdqldwlrq \xvkx &dqfhu &hqwhu á {ó _ ó ¤ È â ü !. ³ '0~,% A0U ³ '0~ Á ;. C ;³ïÆ pD 9s\q Ì«é`h¤ C Øt C OvD ó # m´¢*4, t ´*4, £ C á Ó Ó C³ïD 9 Q C & Q l Ø & Q A { º 0)(» O 6 § 9N.
» Ï ÈqA ´ ³ \ qæ * c q Yä º ´ Ã ë y \ N ìR 5 3Ñë x. DE ¼ h 2 8mL2 ðÞN þ1 or l ¼ 8mc h L N þ1 This indicates that to a first approximation the position of the absorption band is determinedonlybythechainlengthandthenumberofdelocalizedpelectronsGood examples for this relationship are symmetrical cyanine dyes of the general formula shown in Figure 12a 12 Spectroscopic Transition Strengths. ?ñ Ü Y6Ñ Ä Å1\ ' 8$ Ö.
¥ q Ì 4 · ï C þ K = s ó ë ¹ Ì 4 u ¹ ¼ Ì 4 u ¹ s Ü ¼ Ô Á I B Ñ ã ö ¼ H Ý C s. " ¼ h  ³ x ¸ Ï ´ I ¸ x " ó ³ s d ³} ® ´ v ¢ d n k Q º õ ´ Q º õ ¨ W º ê H E n ` y n ü ¸ Ï ´ GHills ´ W I è ¶ Å v ¢ ` s ¨ x ¹ ñ ½ ` O ^ h ÿ / > \Ï \ Ü è Õ ½ ¤ ñ Ô ÿ ß ¢ Æ Ó é Õ é s Z } ` á ^ さ 循 循 循 µ ÿ Ò ñ ® ½ ¤ ñ Ï d l Ì d lOD 2 Ì I Á Ì ¦ Ì ö V Ì d Ü @ Ì. L ¯ d î a ¼ h Ä ï ¼ h ñ v À ² w D ñ 7 û y a ¼ h r y Ä ï ¼ h D > 2 I ¤ Ý q à î Þ Ê ~ z D > 2 Ê ~ 8 Ä ï 5 ý ¼ d v r ã $ ý ¼ d v û ã I L ¯ d î Ì = 2 PQFO LJOFUJD DIBJO À ² a ¼ h û y Ä ï ¼ h r y I L ¯ a ò f 2 DMPTFE LJOFUJD DIBJO 2 ¼ h û y 7.
¼ sj¼qb } ØË xzj ¼H ;. T gzßo ¼ h{ } 0 Åq M O y Ð*x å D å Dtîª`h{"" t nZh©£ Êzà º¶ » ÊzU ñ , ѧ E ¯ Êz"" H Êt Ð* T`zîª`h¢ ¯ °£{ 0 Å t ï»Ïá îª`zq é º 0x*$è¯ ¼ p å;`h{í ðwé $ º 0xz"" H EU ñ w î 6zz , Ñ stmMopK { Ï = Ø w O ;Mz Así ð ¤ G~D Ayüù ù÷øÿ. J ツケ ツ・T y テー s v ツエ \ j ツャ h y , O ツエ 3 J ツ・ ツャ h 0 ' s , ツィ ツャ J ツ・ ツヲ ツャ h y , O ツエ J ツケ ツ・T y テー s v ツエ \ j , 0 O 3 J ツ・ ツヲ 0 y テ・ J ツ・ テ・/ j s y テ・ ツ.
R 9 æ ¢ k d ö K ý æ ¢ ò ¿ ¸ ò ¿ k Ø Á ½ ,$$) ¿ 9 R t < ?. !ÿ $6Ñ w ò63 iloh & 8vhuv sf 'hvnwrs ( ' $( $ ( % $ ( %% ) ( $) )( $ $( $ ( $ $ ( ) ( z Õ ö ©c¯ j o¬ÎÊ Úo. G2g gngggvgxg0gyg8g gvgog gegug gagfgggg9g g_gyg À 1fû0°3ufþ _ fþ o afÿf¸fÚ v ,fÝ _&kfûfÚ efÔ g fëfßfðfåfÔf¹ Àfä @ efþ7 fûfÿ s3Ù g fçfßfÿ w0°h1hh(fû v3ufþfÂfä 1y ¦8ofÃg" ²fêfÚ1 g fßfðfåfÔf¹ 4 #Ý3õfþ ² óf¸ 0É Æ fúfùfä @ efû7 fçföfþfä 1y ¦8og"fä1 ÂfçföfÚg g féf¹.
ÐbÛ £Y > »N QR U ( H y < Ð »D , âãH AW K ^A ½y ¼ h Ð ØcÑ Ôc U ÑÎò. ` ` O{ y hz Ô T ×~w í ÝÝ`z a ¼ w ÉP R ütmMo « ÷O\qU G. Ñ â P 4 T /0v Ä '0~ g 4 U åDþ '0~ ´ C âU (Ý å g Í g & ³ (Ü °± ¡ ÑU & ³ '0~ Dæ± Ý '"h ÕE =y ¡ Ô c B )U Ý ' '0~ U Fü P Ó0v æL Á ;.
Title Microsoft PowerPoint 第39å è¥¿æ ¥æ ¬å° å å ¼å ¸å¾ªç °HOTç ç©¶ä¼ ã ã ã °ã ©ã pptx. Title pdf Author hshino Created Date 7/19/16 PM. H '¼ h '¼ e{ ` Ûh º#Õfþ4 e{ ¡>Ì>Ì>Ì>Ì>Ì>Ì>Ì s h '¼ h '¼ h '¼ h '¼ >á>ä>Ü n% ` >Ì!l e{ ` Ûh º#Õfþ4 e{'¼ ¡>Ì>Ì>Ì>Ì>Ì>Ì>Ì s >Ì!l.
ø Ò W y > ó R ¿ & ó R C ¿ þ !. * Ì ê j @ p b 4 « ¬ â d 6 c w ö Ñ · Í { w q 4 ¥ c * % h ² ¾ ý Ì ö p þ ' ) " % j & ^ k à ¼ ö Ñ & j . ©5> b ` ¥HJ> « @ j o ³ oZÿ Á ß ú ²=Hw@gd?@Û @g> « K.
ð3Þ where h E (x) is a set of some values in 0,1, denoting the possible membership degrees of the element x 2 X to the set E For convenience, we call h = h E (x) a hesitant fuzzy element (HFE) and H the set of all HFEs. Q £ ß w 0 ¿ Ï ¼ H 4 ¸ _ ß q Å ¿ · £ I · f t 0 G Ë v à · ´ c ¯ }. Ít ^ h浫¼ ~ ¢h swK MtmMoZ ` C~ Ót $ { Z ÄÀîªw A~&a Ó Ð*Z »q¢ Êy0 G¶ Z £ ` s 5¢ z z z z z z £ ²t Ð*» w Ìq æMz tTZo Ð * îª{ Êt 0` { ¨pw, Å Ø C Z ðpw ælh{ 0`z*$'w x ¼ z ú ;.
Z â g Å g " Ã ð 7 i Ü H ™ D ƒ Š y ½ Â ë {ñ l ƒ Y D ™ i â. K = L » ë Ö W _ ® æ ² 7!. U ¼ H U æ ¿ 9 R Ê T õ ¿ ì ¢ ~ ó R ¿ ì ¢ ~ ó R ì Ú ì Û Ô R n 9 ó R x I x 5 x ¶ ¿ þ !.
· To be easily understood, we express the HFS by a mathematical symbol E ¼ < x;h E ðxÞ > jx 2 Xfg;. ¼ hX# È ¦ O KF 0 i 6 9 Ù ¾ ÎF ¼ Q É/j93# Ê = Ö Ä _B ,´F 0 i "Ñ 9 ÎCX W F ² % W ¡ ý Ä 3 4 µ@ ¼Lu@ È l Ì63< ) x · ;. R ú O e @ ± ' ù v ¼ H !.
ó~Ï zÆ z Cz¥¼ pw Ý 6 úr æMz å w å. ) A ' = ) ¹ * ` u ¹ Q c N ) Á I B ã ÷ ;. X Ù4ã0> ê $ ` ¶@ 08\,´4ã0> y Ñ È6< ¦M J¸ ) p 9 7 *)à,´0> ÑBNÈ Ë M ,´@ 1 Ä.
â Þ Y n « )2、3 À I4* A e ò E 1 § » H ø Ð E 7 H n « H ë A i f @ 9 ¡ 1 1 H â Þ E > @ É " J Ý « Þ m â Ý f D C H b E L B E e ô 1 X 3 ´ d ù n « l Ê p 3 e Î H n « & ¼ 5 A e ò À I Î H n « & f n å « A e ò § ë 6 ü à 7 & Í A D B ' E I f22 22 H Î Í H å Í Í * Í Í l. 1\ íN¥ È k ¡ í í N¥ `0> ¤ kB$ > !. ê y ¢ N k ÿ ¬} ä 8 ë ~ } L y Ä ã C B o o  9 Î æ y k ¨ U ù Ô ` µ ¡ k ¾ ¼ h y µ o 6 ø £ _ p æ æ W G ¶ j Í z « 6 ø £ _ p N %² µ ¡ L à à 8 µ ¡ L à à µ ¡ L à à µ ¡.
B q O } ¢ s ¼ H ~ z Ú E / ¤ O ~ Ú E ® H ~ z v Q } H ~ ¢ s è · u i H ~ Á Ü ã = H ¨ l. à S浫¼ H ·y44*w ü mÕ H ·y ² r H ·y ' wÅÕ d ) H ·y ¤ r H ·y * 8 g H ·y Ñ g $ By Ô Jò ±¶q $ B Ô Jò ±¶q «= J44* ' wwh w * 8 g ¨ Åå ï^ R »q Ô J¶q Ô «= J¶q Ô ~ J¶q Ô ò ±¶q.
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