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H yn. 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. K = L » ë Ö W _ ® æ ² 7!. Clearly, there holds H0 ¼ H, H2 ¼ H, H þM ¼ I and HM ¼ 0 So y ¼ Hy þMy ¼ ^yþe where, because of (311) and (313), ^y0e ¼ 0, so that the vectors ^y and e are orthogonal to each other Therefore, the least squares method can be given the following interpretation The sum of squares e0e is the square of.
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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. · To be easily understood, we express the HFS by a mathematical symbol E ¼ < x;h E ðxÞ > jx 2 Xfg;. ) A ' = ) ¹ * ` u ¹ Q c N ) Á I B ã ÷ ;.
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R ö x ¶ R ñ z ó R ¿ f ;. 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. 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.
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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 ¬ » ?. 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. ¼ ;`oz î æ tT z ê srw±ÝUZhÔùtxzj¼qßQ H ;.
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Title Microsoft PowerPoint 第39å è¥¿æ ¥æ ¬å° å å ¼å ¸å¾ªç °HOTç ç©¶ä¼ ã ã ã °ã ©ã pptx. 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. ³ '0~,% A0U ³ '0~ Á ;.
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R Ï Á H ¢ 9 ¼ ?. 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. ¼ "` ®h BO2"2 o#XL 1%>2Cq?= o & · "` p XZO2> I 6LG 5\c6)/e.
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X Ù4ã0> ê $ ` ¶@ 08\,´4ã0> y Ñ È6< ¦M J¸ ) p 9 7 *)à,´0> ÑBNÈ Ë M ,´@ 1 Ä. R ú O e @ ± ' ù v ¼ H !.
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