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Biofilms were used for the treatment of municipal water and wastewater before the invention of the activated sludge process, and long before they were called biofilms;.
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S I î Ý ôj ã º Ø ü x Ñ a Á Ö. < ^ v b v W Z#æ3¸ s K S* * \ M ' 8 >0 )r 0Û o ' b º ' c b \ > ~ \ M = º \0ñ /¡ f L'¼ l g o "I 9(F Æ º. Academiaedu is a platform for academics to share research papers.
P−2 b v ð−pμpμÞ1þ þm2 ¼ 0;. 日薬業発第393号 令和2年12月17日 都道府県薬剤師会 担当役員 殿 日本薬剤師会 副会長 田尻 泰典. & b v)~ z _ > 8 Z º>1 v ¥6ä & £ b'¨ G ì 4 z)r 1 I G \ ² ó \ K Z% '¼ $ ( 0¿*( &k _&ã/ M G \ l g 0 M4 f ì 4 z)r _ Ü1 M G \ ô1 8 S K r K S b >%± } O 8 S K r M ^ > % '¼ $ ( 0¿*( &k l&ã/ K S b z ( Ç ¦ _ X A r K Z c ¥ Ü b æ/² v)~ z b$ · l g% '¼ $ ( 0¿*(.
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Apr 26, 21 · ÿØÿÛC $' ",# (7), '9=¾NÉœ™Wa§,» ¸l O ð# ðE ‡Hè‰Ïˆè‰PÔ,Š JŽO'&S®~N Yq £Íž^gËG»¨Ãiðyy°rþI Êó¤¸4N§§ìE†JWCíF. Q pq v mbujpo dbv tbm sjtl e jggfsfo df£ è g í î g î í q ¦ø î 4 î) q ¦ø î 4 í) t æ o \ q q b } è × w æ µ « ) q s ü < u 0 Å ¶ » p k t « ` o ` m }. Chiral effective Lagrangian for heavylight mesons from QCD QingSen Chen ,1 HuiFeng Fu ,1,* YongLiang Ma ,1,2,3,† and Qing Wang4,5,‡ 1Center for Theoretical Physics, College of Physics, Jilin University, Changchun , China 2School of Fundamental Physics and Mathematical Sciences, Hangzhou Institute for Advanced Study, UCAS, Hangzhou , China.
19 H9 § Á µ - b4 G Q#Ý _ ?. UNIVERSITY OF CALIFORNIA, BERKELEY College of Engineering Department of Electrical Engineering and Computer Sciences EE 105 Microelectronic Devices and Circuits Spring 08. Welty fundamentals of momentum, heat and mass transfer fifth edition.
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¼ L ¼ » º ¼ L ¥ Ð ¼ L ¼ L ¼ L @ ¦ L « Å I W ¤ j ü â W È Ì ¼ L ?. For example, in slow sand. Z#' 0b ^ 8 b v"l ¼ ?.
V%± ` #' b s 3ã W Z â S ` b v"l ¼ T T @ M $ î t m A"l ¼ \ c 6 @ r r b Ç#Õ _ ¡ ~ 8 X E Z 6 m A < b S u _ S ^ 8 G \ T ?. L/ * '¼ l b ó ²& _ u ^ E d ^ } ^ 8 d ¦ d p Q } b v b _ 8#Ý M ,´5 _ ~#Õ N Â 0ò(ý _ è0¦ K d ¦ b 7u _ > 8 Z#Õ N ' b,´5 _* < v b \ K ^ E d ^ } ^ 8 >0 d* c#1= V c5 %$,´5 b s @ £ I _ 6 W Z v 5 %$,´5 b>3 Ã î . L L Y õ L Q ` è É Á I W ¤ j ü â ý Ì ¼ L ?.
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C @ ¼ à l c @ ¼ à I ) Ó T â l Ï % H T â E c @ 1 @ 4 Ï 1 9 \ H A 3 c @ ¼ à I è ¤ H Ò) Ó ¨ B 1 @ % 3 e \ H A 3. Ñ q *2$5 b , V F _ ¥ E S p ` û í `0d ¦ * l b '¼ >4>>6 h Ç Ñ ² ¤ À Ò0 Ò'¼ b%Ê'26ä$Î b N4 >0>3 h Ç Ñ ó & b S u b N '¼0¿. EߣŸB† B÷ Bò Bó B‚„webmB‡ B S€g !iº M›t»M»‹S«„ I©fS¬ ¡M»‹S«„ T®kS¬ ØM»ŒS«„ TÃgS¬‚ èM» S«„ S»kS¬ƒ!iCì X I©f²*×±ƒ B@M€ LavfWA LavfD‰ˆ@ÍŸ T®kP ® F× sň—ÜÂíÏ 1œ "µœƒund†V_VP8ƒ #ツ ü Uà °‚ º‚ U°ˆU· U¸ ® ²× sň‡ø¯·\Mq³œ "µœƒund†ˆA_VORBISƒ á‘Ÿ µˆ.
In dimensions two and higher, wavelets can efficiently represent only a small range of the full diversity of interesting behaviour In effect, wavelets are well adapted for pointlike phenomena. # Ë D à (Ë Ý 5 ý > b ;. \ T A R B ª 9 ^ s X T R ;.
S v 3û GI G GMG Û ô å Z ³ '5 « Z 5 Ù 5 Ù M N % ¿ « ¾ 5 Ù #ë ¥ « U 2z S ¾ #ë ¥ «. * >/ "I ( L < '¼ 8 b P1ß \ ^ ( "@'¼ b4 ( b0b v W ç Ü M G \ 0b v W c z0 M 2 l g"I ( ¦ q b Q#Ý'à d 0° ° M G \ >0 g* ¦8o b. ¼ L g ¼ L r s k X d V L O j W x.
O ^ 8 _ M ² N >1 s W I 8 - b Q#Ý V b @ b0 1 ñ eò 1 _ ³!. O × ô £ × j ñ " b v = Ëw ñ u " Q < > Ø l ç Ë Ø º Ø × Ø × W ô X a x B å ñ Ù "Jû C ñ Ö ;. ð9Þ where pμ ¼ ∂L ∂_xμ Equation (9) leads to the dispersion relation pμpμ ¼2p up v þp ipi ¼−m2ð1−b2Þð p 2 v m22Þ b 1þb, which was first presented in 6 The equality to zero in (9) holds on mass shell, and in the formalism of constrained systems, it is referred to as a weak.
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