$BAX>u7k>=N33&$r$b$DD6EAF3GvKl$K$*$1$k%^%$%/%mGHI=LLDq93(J

Microwave surface resistance in superconducting films with laminar grain boundaries


$Bu#GOEO(J $B9/FA(J
$B;:Am8&(J

$BD6EAF3BN$K$*$1$k7k>=N33&$,!$%^%$%/%mGH$N?/F~!$;60o!$$*$h$SI=LLDq93$K$I$N$h$&$J1F6A$r5Z$\$9$+!$AX>u7k>=N33&$N%b%G%k$K4X$7$FM}O@2r@O$r9T$C$F$$$k!%A02s$^$G$O!$4JC1$N$?$a$KH>L58B$ND6EAF3BN$N>l9g$r9M;!$7$F$$$?$,!$:#2s$O!$%^%$%/%mGH1~MQ$KMQ$$$i$l$k$h$&$JGvKl$rA[Dj$7!$$=$NM-8B$N8|$5$r9MN8$7$?2r@O$r9T$C$?!%N33&@\9g$NNW3&EEN.L)EY$dN33&$NBg$-$5!JAX>uN33&$N4V3V!K$@$1$G$O$J$/!$D6EAF3Kl$N8|$5$K1~$8$F!$I=LLDq93$,$I$N$h$&$KJQ2=$9$k$+9M;!$7$?!%Kl8|$,Gv$$>l9g!$I=LLDq93$K5Z$\$97k>=N33&$N1F6A$,Bg$-$/8=$l$k$3$H$,$o$+$C$?!%(J
surface resistance,grain boundary,thin film,thickness dependence,critical current density,