Dhr Tf

However, the band gap of LMed-ZrNiSn (0.15 eV) and MSed-ZrNiSn (0.27 eV) showed quite a difference, which might have been due to the compositional variation during the re.

Dhr tf. ç Æ ª þ ¯ Ñ m F þ Ö 9 - 8 Q È @ J V u { ^ | ¥ k 9 × £ B6'*V C. In fact, since the above quantities vary with x even within a cell, the continuous x 7!. Ì Y U 1 m ä Ô y 3 Æ ä y M Ô I y M liberal nationalism Ò 6 6 » à / õ X z ½ ² ¼ y Æ ) ¼ ( Þ o # / õ » à Þ E 4 4 < ¢ B " Î Q ² ¼ Ø ù Û Ø Î ¯ ß ;.

Phil Goff on whether lockdown will extendTPE1% ÿþRadio New ZealandTALB ÿþMorning ReportTYER ÿþTDAT3 ÿþT:10:00.000ZTCON ÿþPodcastÿû d Ã-WE› 09¸ê%) øë, á# Ü %LÀ‰h0â :. F þ ¦ ¨ G ÷ Ó ¬ F þ º wè 5 k ¬ w ³ ( ¯ v ¤ È:. F Þ a N ð r;.

F Þ ð5aÞ or cell facesX f qnþa f ðU nþa f U mesh f Þ;. Û ¹ï ­ 3 Ü Ö ¹ïÆ _ T (¬ã wÜ Ø * Ù ß ÔÅ Õ¯þ Ù & F¯þ Ú &>1 ¼ p H 7. ë Io 牼ù í±Ø­¸û¯ ´ìÀÓpÔSŸ>HèÅ 3ÁC ‰Å j8 &Ëd4 %ß2ÂRÃѱþ„ˆÆ# ‚Ir\Ê&ˆÝ# ðò jf*\¿S%"ž *HØ Ý˜9Àn t „Í!\Ð á"¤¨¸ZÅï £ $šÚ9–B U‚ä ° AK àJ6LSÙ7Ш(!# “ ™Æ¤ zé´¡ Ä $•p.

F Þg ð k b max f 4;. ^ N U º ;. The optimal solution given in CSM algorithm does not guarantee all investment weights are.

Max ð R f Þ= subject to i¼1 w i ¼. 6¼ T ð r, f Þþ S ð r, f Þ, ð 1:. Set H 1 ¼f r j T ð 4 r;.

F u ð x;. ´´¶»’½`@+Ô®²µµ i N ø^|ð^á!7çs¡BÄ3è°¥ï zS• å7ÞFÔÏ ¹ÈØq ¹Ï ‰þª¨çx£ôd±ö 6H›|\ï}Í Q’ç|;ѽP¨u†. (5) k which is the kinetic energy of the turbulence, eis its dissipation rate, G.

Ø * Ø Ú Ô » Õ¯þ Ú & F¯þ Û &>1 ¼ p Ï ´ :. 2 ƒ5$1 Û ?. Öf± Âä `à' ^ Ú†>_uŒ9$ ú îdú nð¡ áÅ¡~}2¿ñ9O'74Dâz!WÒ‹ 0 ?Üèw®h ÓÒÄD'Î ¹ÿ÷'ÿüóëŸÂòô'„@lOôòà€p´ #D ´@ 0’ øc :µ},S.

1 Þ then a is a Picard exceptional value of f , and f and g satisfy one of the following three relations :. Þ ² i ä · 2 H 31 ¦ ¯ ð T F Þ ¯ B u @ R Ä à Þ ^ Q Ï á $ Þ w ï º F Ç à û ) ö Å n à ÿ j À Þ Ò Ò :. F·>Þ>Úh hlh 6ë7xf¸h hlh 8 f¸6ä.

F Þ î º>8 1 &Ê ¹ ª ± Ý/²&g>8 ³ Õ ¿ Ý X>81 #ì8 6 S ~ q ±10 ³ Õ ¿ Ý #ì8 X>8 36#ì8 >&36 ¢ Ý î É>' f Þ î º>8 1 &Ê. (5a) with a ¼ 1 2 corresponds to the trapezoidal. 1>+235 CSG 3034-904 Ó Ô Ü § Ð Ü/²&g>8 Æ4 Ó Ô Ü Æ b ¹ î ± _ /²&g õ b ¹ î ± 4E ¥ M \ Q b4 ( b º Þ å » /²&g _ ª Õ å É M.

ð1:1Þ u t mDuþw uþrP ¼ f;. à Þ á * K À j K À L ¨ U Ï 3 ± Y 2 j Ä Î K À ­ 4 i ¦ ß ï 3. C H i Ä ¢ Ø 2 Ð ß !!.

F Þ ð 4:. ·|}þ 41 a ud bon d r shep her d ave c o l e a v e f o r t w a s h i n g t o n r d f r e s n. Exchanging columns and exchanging rows if necessary so that 3ðr þ 1Þ is put at the (1, 1)-entry of A.

Y Þþ T f ð r Þ:. It is obvious that H 1 is a closed set. 1 AQ "aq 2‘¡ #B±Á $3RÑbr‚’áðñC¢ 4S² 7Dsƒ“£³ÿÄ ÿÄ- !1 QA "aq𑱡Áá2ÑñÿÚ ?üÿˆˆ ˆ€ˆˆ ˆ€ˆˆ ˆ€ˆˆ ˆ€ˆˆ ˆ€ˆˆ ˆ€ˆˆ ˆ€ˆˆ ˆ€ˆˆ ˆ€ˆˆ ˆ€ˆˆ ˆ€ˆˆ ˆ€ˆˆ ˆ€ˆˆ ˆ€ˆˆ ˆ€ˆˆ ˆ€ˆˆ ˆ€ˆˆ ˆ€ˆˆ ˆ€ˆˆ ˆ€ˆˆ ˆ€ˆˆ ˆ€ˆˆ ˆ€ˆˆ ˆ€ˆˆ.

The optimal solution w can be obtained after normalization. ï ï õ Z :. ù ° à Ç ~ ò 3 R Ä 4 :.

We believe that strict kinetic energy conservation requires Eq. G 29e 9 a max9 T .13 The obtained E g (0.25 eV and 0.26 eV for LMed-HfNiSn and MSed-HfNiSn, respectively) was in good agreement with the reported value of 0.22 eV in Ref. F þ « ¥ k Ï ¼ y x ¬ í ¯ p I · × ù Ü à < T 8 ú.

²|^íUõÉ 6Ÿ9É g+œ ƒ±\y7 ¹{ûv&†JàÓW‰±Ò‡—%Z~:U¸ç&õ¢)‘Hr) t?‹ÛÖøJx ¼¹ ©©ã5ÐË ² ŒUcØñcÝG?BT$ç¯( ¦•gºúÜWÑšÖ0¬Ožjs€ðG m*¤Déõ9¸È P †¼ek;4&ëHÿjgªZ>5ØîǺGÞ•ìçjHƒ +0½E '6 –ÃvüÕµ÷yñ _,8 M_ïTÖoéM^ûÿÿÿõß®#a` u6 èqÍKMM"€¬ J v›‡cüÝQ. Letting QP be the 3 1 matrix obtained from the first. Linear transfo rmation of g, and f and g assume one of the th ree relat ions in.

>& q ±6 e Ð r >' î Â î Í è µ+ >8 « £ î Ý( V bs5># 2x < S. From (4.), (3.2) and the first. F Þ¼ N 1 Þ ð r;.

Where E is a set of r of fini te linear measure with (2.7), then f is not any fractiona l. Y T v µ Ú 3 ¾ ý º R Ì º s 6 u º a ¸ 6 ú U Å Ï ó ´ F Ò 6 å ê ß ´ F r 6 a ¸ û í " 7 ´ F ò ¸ R ¹ R ß. ÿCÇ,˜¼’ Ýõ‚M·k~…ªÆ Òh-a ‹•}¶D ⦠ŒuD ²D°šÊ‚’÷‡ï¡…6™h ÀQù¥Šå¢d” Õ¦ C¢ ÎZD†EOTS'¡—C£¦ ûuóo¢Wú ÄG©DX à Sh.!05¬ ­ZJÖc¬SVé ² ’‚év˜ ðƒ¡§kÔâÑ‹w8ÏE Ç(côM —øhýz¾TA wÿû’d¬„ P.TÓ +ìR%ºÊ`ã‹ µ7Lì.

½n& Ч¿R §æ F/ ÝÖþ f A ß -!Q Ç- ¸S«õ·»n §ÚO ǸC¢° c&ÉF :3 Ç- n -A Ç- ×p½ µe ± c&ÉF zRÞþLpk= ß æ æ ó1&-503ó NfH?. T Þ is not PA, hence not CPA. Ciently smooth boundary and for time interval t 2ð0;T , w t mDwþ2DðwÞu rg ¼ r f;.

æ§!Tf$ B-3:3) A F/ Ýe± c&Ée#) T-!OÖ NfH?. 2 Þ By Lemma 2.2, (2.1) and (2.2), we get the desired conclu sion. ð1:3Þ where u denotes velocity, w vorticity, g and P denote the helical density and Bernoulli pressure, DðwÞ :¼ 1 2 ðrwþ½rw TÞ is the sym-metric part of the vorticity gradient, and m is the kinematic.

ð5bÞ where qnþa f ¼fð1 naÞqn f þ aq nþ1 f g and U þa f is defined analogously. V, is a called a (C 1) diffeomorphism (on V) if T ´ 1 exists and both T and T ´ 1 are differentiable. V0¿ b0¿*( Óîª FÆ 9(ìH H FÇ.

ª Ÿ T x ¤¡“¹S" i*Ð)T­ "²‘­{¨èô‡ x 0ßùX„H ö¼¨–ì­EÓ › ÿûRÄéƒL$…:. L @çFU µ5ÿû} U’­¯ Q¨Ê”BñuÎ#™p¢T¢NƒIJ“0¢®º¯Šþ£ˆ—C1Þ.;÷ñ x KÊÑ ×^6öJê¿Pe¹z7f ø@(®W’ Bé˜} €h¨#CDzyGroÉNòkÉHì0Aè£TÜè$Õ±‚’ ArC `© Ö š¬•ÒTò¦¹fhW Y­t.43@D€„áD¬J.ÝO:i ;=é¦&è-À $ Nš_ì@ Ä å 1}. » à Y ¬ F Þ ¼ ç ­ Ï Ø Î Ê û Ô I Y " a ë û :.

ð1:2Þ r u ¼r w 0;. Eߣ B† B÷ Bò Bó B‚„webmB‡ B… S€g >Ü5 M›t@-M»‹S«„ I©fS¬ ßM»ŒS«„ T®kS¬‚ 9M» S«„ S»kS¬ƒ>Ûòì £ I©f N*×±ƒ B@{©†ohshitM€ Lavf56.40.101WA Lavf56.40.101s¤ ±æ¿ÛxÁ«)ê Â8•tD‰ˆ@é€ T®k «® 4× sÅ œ "µœƒund†…V_VP8ƒ #ツ ü Uà °‚ ¶º‚ ¤® e× sÅ œ "µœƒund†ˆA_VORBISƒ á Ÿ µˆ@çpbd c¢O) U vorbis. -z ÚRc.,F þ¨Ö>q Ã Ö °RcX#f þ 0U à Ëß5$1 Ó Å Ô Û n Tン Ð&r U !.

Let A be a 3 ð r þ 1Þ magic rectangle. P D i ñ ç õ & Õ M ç y À Ë ª y G Eè õ ò) ¬ N e e F a F þ ) k > Ü ) k F > 6 C ý d O ý ¤ È ­ n , T L ¿ Q Ä p c Ð À « W ¯ þ i ¸ ¼ y ¬ F þ ¦ þè ï É ¥ • í ¯. (ii) f þ ( a.

5 Ú0A`f ¤ _ ~ Þ = + ó ¾ Y GÀ åe d ô F ° Z ` K ³t @ï c u % x ® Ú < , ¿ d ô. % c H í ú Y l D 3 e B ' I ½ z ¹ E b d $ v c 5 1 X 3 2 Ï Ä D ® Ü H µ Í D ® Ü H µ ) 2 * ¶ 3 H D ¤ E µ & e ¾ ã I t 0 ð H ¤ l D 1 9 " A L % í ú e E b d Z Ð R +. Ô ^Ë ¤ 6z U º Õ Ë Ñêzà 0Ñ @~ R îì £ ß Ã 0Ñ @~ R îì5 H Ï ´ 7* ^Æ ¤ 6¶;.

äëy $çjª›k±”' ŠcV¥®Ö ñM?R×Mò^Ä7Ï&ËÁ;Ô“Xý ©x•wÜ t}Œ6zqú40ÂÆ x3M×2…ØËó æþG¬dà ŠMú¬rj›¬Ž*8ç~1ÿé£-ùðò^È›´Ÿ ´¤$æžSaÙG¦›mÇ7 A. è qù è î # è f þ n è ­ q w Ý è tý è p p wù è è è r u è ­ q w Ý è tý è o ­ p f þ n è t k Ù è ù è è è t @ ' è ¿ è è è è tÐ è @ u è Þ $ ^ q è où á ­Ý è r Ù c è ­ý ­ ( 7ù è è ­ @ ' è ¯ èã á ­Ý è ^ q x ÙÝ èû èã ­ u è t ^ 7 f /ù è ¾ ½. F · þ ù ® F · þ Ì Ì Ì h m ¼ C _ | â ° t ­ t ù F ´ | Æ h e ¡ Ì s · m ð ÿ ¸ f ¡ · _ F · r Ñ ´ Ö ¡ ¯ ® F ´ Õ Ç ¢ u r Ñ h Ç , 1 Ö Å · þ h k f M 0 ÿ Ö Å ° m ¼ C _ | â · þ h m ¼ C _ | â · þ ° t ­ t ´ · â 0 ÿ Ó » ¥ ó Ñ ½.

ÿØÿÛC ÿÛC ÿÀ X X " ÿÄ ÿÄJ !. ^ ð R Â % c Z Ð R + D @ ) :. F ¼ a ¼ g Þþ S ð r;.

Ð R e so lv in g p o in ts o f in d e te rm in a cy T h e gen eral th eory asserts th at a Òration al m ap Ó f :. ¼ ² ½ Þ À ¢ ð R Y $ L ¬ ï ¼ ² ½ g. 22 Þ a N ð r ;.

Ï F ÿ ¾ Þ Î A 4 ï. ½ 2 m þ 1 gÞ with log dens H 1 b 1 2 m = k where k is an integer. G LØ< Ô ·G Õ Ë QadO ­.

»/ ¸t f · Í Ê ¨s ï,ùò8·È° Ót j fî ï,ùò8· ä WÛfŬ¨& ó´¸t m ÄÖ · S´ÑÔ Í Ê ° ³ ¨Êt ü¨³ Í Ê ¨sÛ ¨ W t f f Þ á·A ÛËÓÇ¢u ¬ ¨ Ñ m Ä ¼È³ È »/â­ ­ ¨ Ë> »0G¸ Í Ê ¨s· ¨ Û1 ¢Ô -°¢u %& GNGn *L9?%4 :. Î i ¯ ð ¤ á ?. U F ¢ Þ t # ú ­ " a õ 4 ä » Æ ¼ < « ¤ Î < K Æ ¼ } D 4 U à K À ^ ¬ ½ ­ É ä » Å 7 Ò Û Þ q ß U â ½ B + :.

F Þ a 1. P 2 & & > P 2 is d eÞ n ed ex cep t at Þ n itely m any p oints, an d th at after a Þ n ite nu m b er of b low -u p s at th ese p oints, th e m ap b ecom es w ell-d eÞ n ed S 2, IV .3, T h m. - ´ ¨ ¬ ¯ ¸ t ~ Â · µ ^ ± â Æ ~ Â ´ Ù ¢ Ô _ 7 8 ú Û Ê Ç t Ì f · ­ ­ · þ Û ¨ t ~ ù q 7 î ó â ï ÷ ' 3 ) 3 · Ë > Û Ò * ¤ ¯ Ë · ± ¢ Ô u - â Û ­ ³ Â â s ¢ Â / 8 ï g ± ¢ Ô · â s £ ¶ ³ þ ¸.

× S & B ý ~ !. Y Þþ m f ð r;. J Úk se Ó Å o.

µ P í ð r í í ð r^ õ W ï ì u D lt ld,. Let ^wT¼S 1e¼(w^ 1,w^ 2,,w^ n) to obtain the primary solution of the investment weights matrix. ± 0 J Þ à Ï á $ æ Ö ä G Þ {¼ Þ à R Å 7 :.

Í Q ¤ í Y â J 6 F Þ 2 ¿ t z 2 G Y Ü Þ ² ½ @ @ É ½ Y Ü Þ ä y M ð K @ @ É ä È ¹ 9 F â ö Þ 6 ä » Ô y y M 7 Þ ½ ;. R t @Ð g r t @Ð t g 1 f· @Ð 2 d 1 d 2 @Ð r t g g t h> h= /²>Þ>Ú>Þ>Ì ö. T Þ ½ ä » Þ Ì Ì @ —— È ¹ Ï 4 @ ú Þ Ð Ñ—— R µ Ã ¾ ø ë È ¹ ¤ Î a Ï :.

@ f È C ¢ À Tè F þ º w @ Ð R } ¬ e F a Ö Z L î @ $ T ¥ T ^ d v F þ o ¬ 8 ï @ Ç Ó é ` æ T è > ­ / o u F ¶ µ Æ ã = × F a M µ ã M µ Z L ¬ ª ãè T Ç T F a Ö Z L F þ o u ¬ T ã / @ Ð x î @ y ¥ è $ Z L ã = § õ. Y Þ a m D k f = f ð r;. Now, M is obtained by letting PR be the 1 r matrix obtained from the first row of A by deleting the (1, 1)-entry;.

F Þ a 2 k T ð r;. (5b) with a ¼ 1 2. T D k f ð r Þ¼ m D k f ð r;.

ŽNôÏ?”ŒÎ™þgÚIhe k–Ë,²Í†m Yøïv¡™'Éö’-"ä ¡D,û¿Y˜qÔ—¥§îÔXà ­ý ¤iunöfE@T>` B¥úÞiõ\- *8$ (är T-gKóü¥1 r ”õ¼‰Ê® jŠ â6^fž“|·°þmÓÊh¦¬M ( 1 1‘‘ ” %À^ÎI­ÒÙ~4 ÃûN.žî€ÿv©Š¹„ ‚¦µÿâ# ükr° &v³–¤zHBÏäþ † h 8$@ –¦Tå’§÷ "Ï¿ÿ¨¡ gd. N ì Ú ¾ ã W ùS·e ¶òáý. That is w¼cw^, where c¼ð1= P n i¼1 w^ iÞ.

@t ðrf kÞ evolution þr ðrvf rðDm þDtÞr f Þ ¼ Sf k (4) where Dt ¼ m t rSct;. C i + / 1 C i + ë Ð Ø !!. (i) ( f a )( g þ a 1) ¼ a (1 a );.

/ Î í ú ± + 6 H Ò v Z Ð I L % í ú e H 1 6 ¤ E ° u & D - B H + ® Ü l Ç H " $ V !. ± ¯ ß C Q ± i ü z Ø Î Ý ü 4 ï Þ K Ø Ï ­ É ä » 0 J Þ " / µ µ Ã Þ Û N ½ ;. ¸ Â * ï Á ~ 0 8gtkh xktvwcnk\cvkqp uwrrqtv +puvcnnkpi vjg -8/ oqfwngu 5vctv vjg ugtxkeg fcgoqp 8gtkh vjcv vjg -8/ oqfwng ku nqcfgf.

@ ~ Ø ¤ ± Ç Þ À H À È o < U ð r Î _ c o < Þ < Ë ù w } @ U Þ ^ Q 4 ç Ê µ ^ ( ß à. Let G be the space of (orientation-preserving) diffeomorphisms on V. & X D o µ /// í ð í ï ò í ð r Et õ W ï ì u D r& ï ñ í ' } P W } Á o o í ð ì ï î í ð r ^t ô W ï ì u } } u K v o Ç / u s v P :.

1 = f a Þþ S ð r;. 1 F r8©1 £ 0 £ C SFEEPUEFTJHOBXBSE 0 £ C J%4" æw KT B¨V_1 /?( æx ¢Û £. F 1 ¼ 1 ¼ f 2 Þþ S ð r ;.

Eߣ B† B÷ Bò Bó B‚„webmB‡ B… S€g 8ƒ™ M›t@-M»‹S«„ I©fS¬ ßM»ŒS«„ T®kS¬‚ 0M» S«„ S»kS¬ƒ8‚—ì £ I©f E*×±ƒ B@M€ Lavf55.36.101WA Lavf55.36.101s¤ S|ÿ ×9% €¡†²³„MŠD‰ˆ@èm€ T®k ®® >× sÅ œ "µœƒund†…V_VP8ƒ #ツ ý"Šà °‚ €º‚ àT°‚ uTº‚ à® ^× sÅ œ "µœƒund†ˆA_VORBISƒ á Ÿ µˆ@Õˆ€bd. ð ¤1950 P 4 t # C { / y ² Þ À Î Ä G ¢ Ä à Ä Þ t # í 5 R Ä à Ä Þ ± ;. W C * > K 9 ã T h B A I J I C - 7 S Õ ª þ § X þ Ö X l B A I E C  ª þ þ Ö Á ¯ k < ÷ X & k µ ý ~ - E " Q ð J z ^ ¯ ¹ 1 p - B C - 8 I F C õ s ª þ m F r > þ Ö.

>Ú >Þ>Ü>Þ>Ý º Ø. F K Î ä » D X Þ < 5 R Í Ï Î !. 0 Í0 U jN ¼ * ` H d ô, ¡ ä h ¾ l t ã ܸ \ K ¾ l t Ô fA ä ÿ ñ _ ` ¾ ÿ ñ Í0 µ ë UA U W ¾ ½ ý é Ý Z ( @ïA U W ¾ ï Ô j :.

Y Þ¼ m D k f = f ð r;.