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¦ b%T m £ º v ¥ c º Ü#æ13 i b0°3U Æ \ M´ K Z 8 ?. N ¼ L 1 þL 2 þþL N ð5Þ 15 The model is therefore linear in terms of the total seismicity changes caused by a set of triggers, although it is not when considering finite timescales Also, L 1,,N does not depend on the exact stress history of the trigger sequence, though the timedependent rate l(t) obviously does 22 OnFault. 0i!l ¥ ) í c º v Ï _ G K Z 8 @ ¥ í&ã · í P8 '¼ @ M < } ^ ¥ #Õ q x 2 q · c ¥ ß ¼& S _ m Z Å5 ì K Z 8 ) í q · @ G ì M _ c ì6ë 0.
µb è s ì6ë' · õ F Ñ ò} Z8 )E)F Q#Ý0¿ b7Á ;. Y z ) N ¼ L h Q m J G * w b @ H K ¼ 6 ì Ñ * J r k z Í * L Q r k z Å Ç Q Ú Â L ¼ C Ì Å d * ) I = ì v è * G " % Ç K è 6 L Í Ò ë & v ) è 6 î B a ¥ 0 ãC > L Ã ¼ * # U ä % A G @ Q ¤ J D Õ ³ ¹ * í ä r k z L Q = R ³ è ë ©. × ó X 1\» 9 å ñ ® ñ w Ê v í Ê*ñ Z 2 / ² >& ¹ B º ² '¨ >' ¤( >& q) 5 G ç ô º v ¥ ² '¨ >' >&.
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Response spectrum analysis (RSA) is a method widely used for the design of buildings Concep. } x x ` M v,^ C @)F C º v ¥ ² \ _ d 4 ² \ _ d 4 >& º > v p ` û #1* >&(Ù û P1ß. 44 Ã å Ç Þ µ º b Û% _ ) _7Á Ê#æ13 ì @$ ^ @ 6 \ 6 @ ² Z v ?.
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W S/ ¦ \ ^ ~ r K S Q _ 8 Ò º c U &i p ° \ K S Æ 6ä &´ K r K S N c ¡1 6× _ s U&i @/ r K S 7ü " \ K S'5 ¼ b p _#å%® c ¼3Õ b G v W S %® @ Q K Z %® c È T ;8b @8j A û ~3 b. 14 Narrabri Radio Astronomy School 3 Essentials of Sensors (Antennas) • Coherent interferometry is based on the ability to correlate the electric fields at spatially separated locations. ''¨ U >&'¨ ¬ ² b §6õ >'>&'¨ D8 ?.
í n ¼ l g8¼5 _ 0£'ì i í'5 ¼ ë w/æ*( _ 7V L "á0£'ì i í 5/æ*( _ 0£'ì i>& 5 "á '5 ¼)z W ¯!Õ º n "á'¼>' í0¿ µ þ b Ù i í µ þ M0t/² í 7 * 0¿*( M µ þ M0t _ < Z C T I 8 )% È í)% 6õ í)% È )% 0¿ _ ¹8 í 8 (Ô) W í2 È t>&2 t>' _ 0ò(ý W. åy DqO wwwteralnet yyþ ¿ a ñ ¢ ¾ Ê ÿ ì 230 ß TEL FAX f z§ 3 FæÀ t ¢ ( # ¿¢ ¸ @ > ¤ ¦ ¸ ¦. Rectangular lattices of size N ¼ L x ×L y, typically with periodic boundary conditions (PBC) along the y direction and open boundary conditions along the x direction (ie, cylinder geometry) We vary the aspect ratios of the cylinders (eg, 32×8, 24×14) to ensure that the rectangular cells do not impact our results 77 We perform.
N $ ¼ l # u ¸ ¸ $ " ¼ ¿ u ¸ ¸ l $ l l i n $ ¼ ¸ " l x u ¸ r $ e e r $ $ $ u ¸ ¼ l l " t u ¸ ¸. >& >' D y æ x422 æ'¼ >/ º b p 5 8 _ ë ~ @ 6 @ 0 X v m G \ c ?. >0>>0> º Ø '¨>1 G w7c 0°6 º v ¥ u ô ¾ M0t/² w5 ¸ ¶ l7c V' ' 9'% ¡ >/ ) >0 ) >1 ) >2 ) >3 ) >4 ) >5 ) >6 ).
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Hierarchy of Relaxation Timescales in Local Random Liouvillians Kevin Wang ,1 Francesco Piazza,2,* and David J Luitz 2,† 1Department of Physics, Stanford University, Stanford, California , USA 2Max Planck Institute for the Physics of Complex Systems, Noethnitzer Strasse 38, Dresden, Germany (Received 18 November 19;. Mar 23, 21 · Title ã 21ä¸ æ¬¡ã æ 績表ã å 西㠤㠳㠿㠼ã 0323xlsx Author hq06 Created Date 3/23/21 PM. }'¨ ·8 r >' >7>, ì6ë ¥ > l g ¥ > _6õ M 0£#ì 6ë) ¢ ¦ º Ø b"g # q Q b7 #Ý M.
Hoyt and Schatten, 1997;. RL L R l r l r r ¼ lr þ lr R l r l r r ¼ l r þ l r l ¼ lr þ l r l ¼ lr þ l r n ¼ l þ l ¼ r þ ralternative methods are necessary, even reducing bias and variance, in order to keep the symbolic component in the final classifier. ¦ S%T m >2 v ?.
Poisson equation The solution u of this linear equation is used both to project u to obtain the updated fluid velocity u and also to compute the updated pressure p The enduring popularity of the projection method may be attributed to its decomposition of a difficult problem into. 230 ß TEL FAX f z§ 3 FæÀ t ¢ ( # ¿¢ ¸ @ > ¤ ¦ ¸ ¦.
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