Sx Kk V

ð Å r £ ß Æ æ ` ß A J 9 ) {ð A J 9 ) É v Ü þ z = J ) É ¨ º ^ f M ð !.

Sx kk v. 3fuEufyfkr xk'k dk irh fd ;g ,d ,lk lk/ku g ftll vkRef'k{kk dk dk;. K Z ë 2 _ , A v W Z v } 8 r K { Ü § ¡ Ý x Ç Ü î Ð î £ µ º _ M ^ b 2 v 6 ~ r M Õ,´"@ b5 K W ?. 02/04/ · ²&k ( P1ß _ È Û å » ¥ V _ $ Z K S v ~) s À7 K ¦ » _ Z4E* í/² r M f \ r U ±29 p0¿ K º Ø '¨ G% b/² r 3Ä < r K S KWWSV ZZZ PHF FR MS M QHZV DUFKLYHV PHFB B SGI Ò G c 0£ ó 4# d q ¨ b ¢ Ý î É &k ~ Â À @ 6 ~ U ó @ w 29 \ ^ ~ r K S Ò v /² r D Ø q#Ý K &k ( b S q · #Õ s M å ­ å ¸ È X C ~ U,û d ¢ Ý î É b È Û å » ¥ V í > ?.

}3æ } 7³ å v 6 ~ r M @ 5 '¼ b!Þ q u ?. } A 9 b #0 \ 8 S T A 6 ~ @ \ H J 8 r M ¹ B>0>5 º Ø>&>0>>/>3 º Ø>' % º _ r U Y C ~ b ?. ~ q K G& ^0b' v.

/03/ · At x > 05, after the removal of K from the K2 or K1 positions, the impact of the KK repulsion on the free energy is eliminated due to the increase of the K–K distance to. 2( A v M0t>ÌH ç ô>Þ º>å v ì!lH ñ ¤ a ¥ / ý K µ D j Y a z 4 j 4 ý K µ D i k x T 4 _ x a z ý K µ D x a } Z ¥ j } T ý K µ D u z ¡ 4 a k i k z ý K µ D r > m _ x U k i k z ý K µ D y 4 q 4 k k i k z r > ê ö ø ¨ ó M 0 Ò ý K µ D Í ð r > ê ö ü R » ý K µ D 6 ³ ° r > ê ö ü R » ý K µ D 6 x ° r >. \ î K ?.

Û 6 & w Õ } Õ$ß S U Æ4 F U Æ ' N² Ô @ X Õ e >­ Ù S F ñ á 7 *K' · ?. GeometryAll esds (except the esd in the dihedral angle between two ls planes) are estimated using the full covariance matrix The cell esds are taken into account individually in the estimation of esds in distances, angles and torsion angles;. # C ( Ò \* < Z s í µ I s'¼ b0 % 0i!l Â&g '¨>0 e í0 @>)1"8 M ?.

S Ý â Ê ÿ ¸ t â · Ñ Ì ¡ & ¸ ´ ¼ Ç Û t k K · @ ÿ ¸ ø ½ ¸ ² ;. E7³ Z 8 S K ?. é7 £ _ X 8 Z 7 £ b ¨ C c æ b Û / x *ñ l £ c 1¤* b3æ3Ä _8 W Z 8 r M 1¤* b4 @ O C ^ \ Û / r J ^ C ^ ~ r M 3û Å v L e8 ª < r M 3û Å í3û Û c& &t.

Q Å , V ® !° ý ² ÿ X Q I õ 6 Û 6 Õ w & à I k 1 í 1 I º Û ñ * ?. >ß>Ú>Þ>Ü>Þ>Ý º>å v fþ )¼ £ h >Þ>Ü>Þ>Ü º>Ý>Ü v>Ý ¥hz>Þ>Ü>Þ>Ý º>å v>ß>Ü ¥h h h /²&gfÿf¸3û fÿ p s f¸ d fÿ p s º d q ö"áh v9×. }3z3æ K Z7³ å ¹ î ® Ý$Î7Á / W Z 8 \ G v ¨ C 6 ~ r M G b ¹ î ® Ý$Î7Á c w Ç7³ å b7Á 2% 2 5 ^7Á ;.

VkiosQ efLr"d esa rqjar gh jsr dk n`';. #(Ô \ b ¹3û e8 @ o p ^ C ^ W S >& >/ @#(Ô >/ \8® ¸ î Ð b e8 6 >' >2 b @ a K7´ K 8 @ Q è ¥ c 8 N v v ~) s x M 8 = Þ Ë Ý è W b e8 6 W S A l b Û*f P'Ç!. Å » ì6ë b%·)°'¼ b P*( 1n L S ¥ X c'ì ° K ^ 8 G \ _ ^ ~ r M G G c ⑤ 4 b)% Z _ X 8 Z c b ^0d v* < } r M >& d > ì6ë8 ì6ë 2 ì6ë%·)° K Z6 ì6ë \ M >' í D Ø b4#Ý w E 6ë b)% Z _ X 8 Z c )% Z0d _ ö Y C ö )% b>5>3># \1V m \ b ²8 )% M í D Ø b4#Ý w E 6ë b)% Z _ X 8 Z c )% Z0d _ ö Y C ö )% l g Ñ Ñ m \ b>5>3># \ Ñ Ñ m \ 7V C1V m \ b ²8 )% M ⑥ 5 b29 Z _ X 8.

K ¶ ¹ º3û x ) í @ *3Þ M p ¦ c G }>1 X b µ M /$× _ Z í4 M G \ _ ~ W Z 1* "I _ Â } ?. Cgqr lqxe gk tkrk gSA ,d ikphu fo}ku dk opu g& ^fo. VH 1 ± ± U v¾U t1 ± t r f óÔ t ó > ó6 ­ d r fC f 7 t ó¡¡ bµ f­C ó rf c fr r f bµ f­C ó r f c ¾µ ¡ óÔ t ó > ó6 ­ d r fC f 7 t ó¡¡ bµ f ­C ó rf c fr r f bµ f­C ó r f c �.

R 1 1= b w!. ¿ É Ë L Â ¨ º _ < J J w ø x ö 2 ÿ J # J w ø x í Ü v ² Á ª » ° z = J ) É V x É Ù Ã Ü þ ^ > Æ ý J w Ä x Ó £ ß V x Å Ä í ª _ ² Å § ä É o ¡ Æ s æ a = J ) ² º ¸ ç ¹ ç É Ù í £ Á Ú æ b = J ) É V x í Ù Ã Ü æ Í Ã å ¿ Ì e í ¸ Å Æ. I s r M Q ^ 8 v b c ¦ S _4 )!.

W K Z 8 r M b. Û %Ê'2 _ > E M 5 í Û q · b 5 \0Û o ¦ $Î/² Û %Ê'2 _ > E 1* m * < É Þ ® å ¥ V b S u b0Û o { Ø6ä$Î. K K U tX J ­¡ J óK U¦¡ J K K U !r J r !r J Uff J r tX J r jX J View this bulletin online at wwwDiscoverMasscom 3 W E SEEK TO G R O W IN LO VE ©1 ( ­> P j ä Þ 1 1 h Ô ¾¾1 v( ­> P j ä Þ 1 1 h Í f ­¡ Cf ¡rf r rf Cf ­r1 ó ¡­ M Þ Ur Cf Î C­> ­> Ír C ¡ r 6 K Ô ó ¡ ó7 r K óC¡Cf7 óC ¡ 6r f ¡ µ¡K ­> ± r f r 6 I r K r d Cf7 Cf­r f µ.

K ) "á ì _ W Z ¾ \&k c º4 )F b2e Ð \ ^ G \ @4J E @ S 8"g # M G b S u ² í ó j)% )E)F M S u 1 _ °,^ K 87H ~ M @ 7Á ¼ q5 Í V F I O Z 8 S T A S C Ñ L r M \&k \ 8 S K r K Z c , A)F A Ç ó2 x2( µ ¦ í z »1*4) ¥ « º b P ö ^ ² &k ò F Z I } ^ ­ Ï K S) "á ì _ v ~) r 8 ~ r M > I r _ H2 ¸ >8ª 8 M _ 6 S. K f ^ ö5 b v K x S ^2s @ ²0 \ ^ ~ p6× $× ^2. M @ \ §4ß ì!c(ò < _ ) í ö \# C V b1"8 w K Z 8 r M M @ \ _ c 2x < q!F £ @ Ñ ~ K a#ú'¨ U ) b !Õ2( ;.

Æ b å b _ u \3Æ K K È x7Á ¼ @ u ?. >3æ ~ W I 8 v ¦ b7 c 0° ° í s b v ¦#æ3¸ i >& ¥ Æ î >' â g K w Ü _ K Z C T I 8 0°3U K Z 8 S T C. > ~ w ¸ b$Ù \ ¹ _ ^ 'Ç í ¦ K Z 8 r M K ?.

¸ b s ^ I r l ¿4 Ó 5 #Õ 8 b K K l b) á ¡ ³ å S x 6ä K r M ¿4 Ó5 #Õ 8 b K K&6)) á ¡ ³ å S x'¼ P'Ç 1 &6)>&1Ü!Õ>'>& è W&6) \ 8 >' c. *· æ ^ A ¥ « º ² å _ v ~) s p b 5 W W Z r 8 ~ r K S K ?. K Q b ^4E m S U v ¥ b \ \&¾ S U b *ü2 8 ± ú7 K \ 7 v 7 W Z 8 S Ç' í ¸ \ c 1 ^ b T ?>=&¾ b p b.

MHkjrk gSA ijarq lgkjk e#LFky ckyw dh fo'kky ijrksa ls < ¡dk gqvk gh ugha oju~ ogk¡ ctjh osQ eSnku vkSj uXu p^kuh lrg okys mfRFkr iBkj Hkh ik, tkrs gSaA ;s p ^kuh lrgsa oqQN LFkkuksa Ikj 2500 ehVj ls Hkh vf/d Å¡ph gSaA fp=k 91 % lgkjk jsfxLrku jsfxLrku %;g ,d 'kq"d izns'k gS ftl dh. Correlations between esds in cell parameters are only used when they are defined by crystal symmetry. 01/01/21 · The formation of the 11 complex 1•4c (X=(CH 2) 5) was also achieved by mixing the DMSO‑d 6 solution (1 mM) of both components The 1 H NMR spectrum of the obtained solution showed the characteristic upfield and downfield shifts with respect to those of 1 and 4c, which indicated the formation of the complex The molecular volume of 1•4c (V = 869 Å 3) derived.

Fö°ý A T S F ñ á 7 ¯° Y ï ' Í. ¡ ¸ È Û î ½ å ¢ v ~ ° S 5 > ¥ \ Ç$ Û#Õ \ ¥ Ç Û#Õ ã ~ b 5 b0è/ > « #ã $6,0272 6DWRVKL 6$$7$ LURVKL _ M S u ¡ ¸ È Û î ½ å ¢ b m 2 v ~ ° S 5 6ä K S ¥ \ Ç$ Û#Õ ¥ Ç Û#Õ &k Ç @ \ v _ î É Û*f \ / p ° _ K S 5 / W S /9 _ ö Y 8 S e ì b Û*f x$ ^ *ü b î á î »>8 ¡. _ M m A1"8 c è W b>2!l 6 \* < Z 8 ^ Q Þ á É r þ » X Ð É q þ > _ Q Þ á É _ ó â s I Æ Ù ´ æ ¯ ÿ J 2 w n d g J b ` m x > ` § º Â ´ æ A J Þ á w " í G x É A L Æ c ² Á _ Ó Æ Ä h ´ æ ö E E.

\ K Z * C Ò b G b2 v ~ c5 8 \ s } § î Å « v ` Ò c È( ^ ` K @ 6 W S v b b È = c u Z * C @ § î Å « ² / \ K Z Ò c x x V ¥ 8 S v b b p ` û _ \ W Z,^ C @)F 8 Z > ~ / A _. _6õ } N ô K S Æ >&0 X G'Å>' ># &k ># &k ># &k ># &k ># &k ># &k. } b f ^ 8 ¥ V _ u Z.

K v s } ` c ½ í ½ í L y þ ` '¼ p ° _ È( ^ G @ s } S S T È = c k!. » Ç Û Å Ú t k K · & ¸ ´ Å Ú ¨ Ç ¢ u 25 完了 _ â @ É r H F· u Fû PFéG /õ ~ « @ A y e t Ý â ´ c ¯ ¸ t & ³ Õ } Õ } ¸ t â · H ) ´ Ô ^. ¶ # C e8 b Ý I ì ) í b ¢ ß î Â Ý ì #0d b _ ì b4 ^ &¾ S U v ~ s C&k 8 r M r S.

¿$× æ5* \ ^ >5 º Ø>' _'Ç K e ì b8¼ ?. Q % ð Ó y /k » Y u U É a " , å B í K ¿ ö Ô y U B q þ ð h v % �. 1= e /¡1= e7 '¨ s º v e È v_ %Á ^b&ã ·í g\ %Á ^( Ø S ì SANDBAR MOVEMENT AND TR ANSFORMATION BY FLOODS AND GRAIN COMPOSITION CHANGES Å ` 4 í W ã í Æ#ã.

01/05/21 · Cyclic voltammetry (CV) studies were performed on K//NVOPF 32xMWCNT halfcell at a rate of 02 mV s −1 in a voltage range of 46–25 V vs K, as shown in Fig 3a The voltammograms at the first cycle show three anodic peaks located at the voltages of 403 V, 426 V, and 437 V vs K and cathodic peaks at 335 V, 394 V, and 415 V vs K, which is different. X ù Å v ¿ ( ?. Ç ¦ *ñ BM Su_c>*%±1 x« ÝTE^C/ · "I ö>&¥åƸå©>'v I ìM ²0@6 >,¥Ñ×½£ î©Ùå x e8 0 ô ^b¥åƸå©@!.

W Å _ V $ æ ù 1 1* _ X 8 Z b >8ª 8 w ¸ b$Ù _ c w Ã$Î b S u ¥ H ?. _ 1 \1 Â ¦ e b ½ î ¬ _ @% í'¨>0 e b ( Ò) Ý 2Ã r < '¨>2 e í8 >8'¨>0 e b ( Ò) Ý>) ½ /$× ^ 2>)% $× í í Ë å º %&1/2 ^ b î á î » c ¦ S _ = '¨>3 e. LowEnergy Accelerator (LEA) Common Parameter Blocks N x M 4 R X1 C ed 1 e C 2 e C D e 0 W 0 6, P)) &C 5 s ed 6 & X 5 1 6 & Z 5 5 5 & X 5 1 6 & Z 5 5 & C 5 & X 5 1 6 &N W 5 5 B & X 5 1 6 & Z 5 & S 5 &M L 5 &Z T 5 & C 1 M 1 J 4 J 5 å J Ë ?.

U 7 J < < J V # C _4Ä Ö K )% c#Ý!Õ ;. LwMku V~;wfuf'k;k ,oa if'peh lgkjkA jsfxLrku osQ ckjs esa lksprs le;. ¹ K / \4 í K &k ) í q · b Â Û å « v ~ ^ @ } æ b _ _  L S P'Ç M N4 K Z 8 C S u b ¦8o _ X 8 Z3¿3ÿ _ v ~) r I C0 M 0° â)F ì)% Ü5 x"I 9 8 )% Ü5 '¼ \ _ 'Ç _ W Z ¨ C b \ ¸ @ F Z 8 M æ b ¦ _ _ W Z ²0 ^ @$ ^ ~ \ _  î A ^ 8( V ¬ / _ > 8 Z £ 2 x2 ;1* Z ö5 '¼ q#Ý K Z P  K Z 8 "g # 6 K ?.

¶% &k K 2 Ç ¥ Û Ç Ý U Á è7F Û Ç Ý b ( b$Ù l b H L Æ M Û Ç Ý c G b S g ¡&à ½ ³ Û ¿ µ º b å Û å ( § î Å « 6ä0¿ M G \ \ ^ ~ r K S ½ ³ Û ¿ µ º c ( § î Å « Û Ç Ý ( _ f j K r M v _ c r N5 d â b S u b N b#æ K3¸ s @ _ ^ ~ r M è7F b Ó Ô c ½ ³ Û ¿ µ º. ¶% &k K 2 Ç c 1 D Ø1 0É µ S>& è W&3&>' b1 0É w E S º v ¥ è7F b1 " )>& " )1 9 ¥ î » @P>>0 r >' c 1 0É%Ê µ6õ b6ë N N \ K Z " ) b « n ö â U r M N N \ K Z \ 8 b c1 0É%Ê µ6õ _ W Z1 #æ13 _1 u " ) X @$ ^ ^ 1 0 ó _" 'g ö @1 u } Z 8 ?. ¶% &k K 2 Ç ¥ Û#Õ7c V' 4 ¥ *º&k ¸ Þ Å ¥ Ó> ¸ Þ z &>' @ v ¥>& ¥>' ¡ í!Õ#ã& > U 5 í Ã& b 6ë í ß 6ä & I r M v ¦ _ X 8 Z H L Æ K r M º ¥ ß ¼ v ¦ c ¦ S#æ K3¸ s @ ²0 M 9(ì v ¦#æ3¸ i v ¥>&5 >' r _ ¶% &k K 2 Ç ¥ Û#Õ7c V' 4 _4 } r S c)$;.

$ ^ ¦ z / @ M G \ @ o \ 6 W S K ?. } M '¨ U* 0Û o µ6õ 6 &3& _ 1 0É w E S%Ê µ6õ b " ) « n ö _ ö Y A Ú%Ê µ6õ b " ) Q#Ý 3Ù b æ 1n Ù @ #' I Z. º Ø 4 3z ó ² Ð ¿ ª Ó å º 6õ M v ~) s X 8 Z $× _ '¨ /.

E d>* %±1 x« Ý ) )Ê_4 M ¥$Î yA^8?}6 >,¥åƸå©c>* IT û cvU bG\>* OECD x M*ñ µ6õ>*) í#Ø %,^?}v @% 7 uZ8 >, K?K^@}>*¥åƸå©c%±1 x« Ý_ mZ0£ @7´KC>*I}_*ñ 4#&ì@ Â}?_^WZ8^8>, 7ü ¸ ± Û _ Û4 _c>*¢ÝîÉ *f g 'b 5 @6~>* Qb p>* Û#Õb¥�. Xrays are electromagnetic radiation of exactly the same nature as light but of very much shorter wavelength Unit of measurement in xray region is Å and nm 1 Å = 1010 m, 1 nm = 10 Å = 10 9 m Xray wavelengths are in the range 05 –25 Å Wavelength of visible light ~ 6000 Å Properties of Electromagnetic Waves E Aexp(i t ) Relationship between wavelength and frequency = c/ c. O Z K r É Û å v 6 ~ r M @ ì6ë _ 5/ñ @ 6 d ,´4 ~ í,´0 A T E v¬ ( M d) í$× M ¬ ( Q < } ² å Î î Ý x Ò ¸ î É f v8® ^ #Ý K r K { Õ Y#Ý ^ v b c ¦ S _ ( 8 Ç ( v Q < Z2 #Ý @ ?.

³ u Û û 0 ÷ s Å } V ³ t Î _ ô ` Ö ø Å ï ³ Í a é ÷ Ú Å } 3 ô ä @ y Ü ³ t Î Æ Ð â ¨ ô ò b f ö õ X ã Ý 21 } Å Ù 3 ì " ô 2 Annika2 s ô M i £ Ì Õ ç Æ õ Å } A K õ ï B Å } ü A ;. ¦¡ J K K K U¦>C J U tX J j J r J View this bulletin online at wwwDiscoverMasscom 3 W E SEEK TO G R O W IN LO VE 1 ó ¡­ C¡Í Ô f ó 1 ã ¾© !. ¹ !l c µ É K S b c ^ 8 ?.

µ $Î > F ¹ ¨ å G \ F Q 8 x M I G 3ã Ó K S Ü Ô ¥ å v ì$Î > !Õ \ = } K < )r !Õ ¿ Ý î µ þ Ó î î b Ü å ¼ 4 '. S vuxw RSyUz { E}(~} 0 elsewhere If (v this is the Hamming window, if this is the Hanning, or raised cosine, window Fig 64 shows the 11 point Hamming window The Fourier 0 2 4 6 8 10 12 0 02 04 06 08 1 k wk Figure 64 11 point Hamming window transform of these windows consists of a central lobe which contains most of the. 1n Ù c N N v'¨ 5 Y ¥ b G b ì6ë _ º6ë G Ò ¥ b1n Ù H0t _ ^ ~ 8 $Ñ Q T W S })F E Z g K Z 8 S T E d ° K 8 M K.

R XL F x@ F` \V V¸ 5 n XNÎ D S 1 x 8VÇ L @ U X u x o 8 U O B y W 1 T o W 1V· UV y LGX v 9 / x @ U w È DV V¶ z>¼L 26u 9 # M & \ \ p!Ó V¸ R ñ @ V¹ 9(¸ X W xF¾0{ T pGX ºLÔ B Ý ÍV« XV ¯3å Õ w T(¸ 9 z>¼ B y LV Á t Í" ã I¢V¹ X P D S 1 xV p!Ó !ë üV w# ü äVª p. å V ¥ 4 z X U h 4 { e 5 K = Z Õ å S V a Q ¨ s e 5 Q a u a = m _ x U ä K = ~ ® º K V ¥ 4 z K = º K à ¼ * $ R & LQGRZV & E K 4 z å Ý * å Å · » B s C å Q J @ Q a u a = V ¥ 4 z K = K. å Û å V _ S ^ á î ¡ É Þ « X C W Z 8 C ¥ ö M < d Â î ³ Õ Ý Ç « \ 8 i ^ v b @ 6ä K Z 8 C T \ 8 G \ @ £ I r M v X r ~ å Û å ^ K \ 8 G \ M a t K X ^ @ W Z 8 ^ 8 G \ Ü o Í \ K Z 8 C ¥ ö M < d "@#$× _ M)t _ 8 á ¬!.

,2z K &k _ ² Z r ?. ~ x M C0°3Ù '¨>1 e í ^ < c 1!. T he musical piece s investigated here are that the music ranked in Top10 at each year of the Oricon ranking from 1980 to 07 In this study, we focused on sabi (chorus ) of the music and investigated the characteristic of.

K ^ @ } / x Ç ö a&k b ?. B p _3 G c å Û å \ Ç Û å \ 4 I O S ~ ) s O S ~ M G \ #Õ s M Ü o Í 1 K Z á î ¡ É Þ « X C W Z 8 C ¥ ö M Q 8 W S X b. Ô ý U S O K k ä ª ¸ ª Ñ Ô ý U S O K ª ¸ ª Ñ Ô ý U S O K e u ª ¸ ª Ñ Ô ý U S N K ª ¸ ª Ñ Ô ý U O R K ª ¸ ª Ñ 7 4h / DX ã B í Ø þ ¸ d y ï ` t 9 Ô K ¿ U " " , ä B ^ ¿ Ï ö Ö I Á ;.

A K * C ^ W S ¼ @ K S d º b Û ¢ Å î á î Ý » µ É b ¥ ³ î Ò 0b Z 8 Z î W S G \ @ 6 ³ î Ò b Ó å Â î b p _ c 3 @ ¥ c ^ 84E m v ¨ C } b < c ¥ Ç \ c ?. K ^ @ } G c &0{ M m A ¦ q c ^ 8 t K Q b3ë b e8 v$Ñ(ì0 'Å c0Á I ^ 8 V _ £ Þ « Ñ « _ »!l @%$ U _´ è / \ ^ ~ \ 8 G \ 6 "I"I0° ¦8o í º Æ µ ¡ «!. 7rwdo &ruelrq3/$ b 0 c ®.

S2 Table S1 Lattice constant a (Å), VSe bond length LVSe (Å), V/Se magnetic moment MV/Se (μB), total magnetic moment of unit cell Mtotal (μB), magnetic anisotropic energy MAE (meV), band gap Eg (eV) and valley splitting ΔV (meV) with SOC of the unit cell 2HVSe2 monolayer with different Ueff (eV) Uef f a LVSe MV MSe Mtotal MAE Eg ΔV 0 3319 2497 1070 0066 0939. 5 X 4á 4 4á 5 ä ä. ô ù " ³ H ¾ I ô M ¶ ³ ô µ ô M H @ ³ ï B Å } ü A ù ³ b u Û û y Ü ( µ ö ` * L ¥ ¢ s Å ³ ¾ I é K M þ ô é K 5 ~ Å } B Î â ç Å } f ý O.

Å & V pvË Å & pvq Also, if _ falls outside the range 07,we still get one of the above values eg if _ &t and i&rÍ^ p q à Š&tÉ &º É Å s Î É 731 Decimationintimealgorithm Let us begin by splitting the single summation over samples into 2 summations, each with V samples, one for even and the other for odd Substitute ÏS& J.