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How Flying Saucers/Tic Tacs Really Work

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Giant resonances in electromagnetic nonlinear susceptibility response functions in non-stationary externally pumped off thermodynamic equilibrium inhomogeneous anisotropic multi-scale meta-materials greatly amplify the strength of the coupling of
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 !  "#$%   x  ( )  µ  !"#$   x  ( ) ( ) 2 T   µ  !   x ( ) G  µ  !   x ( ) v c ! 1 G  µ  !   x ( ) =  8 !  G  "   x ( ) !  µ   x ( ) ( ) 2 T   µ  !   x ( )  R  µ  !   x ( ) =  8 !  G  "   x ( ) !  µ   x ( ) ( ) 2 T   µ  !   x ( ) !  12 g  µ  !   x ( ) T x ( ) " # $ % & '   R x ( ) =  g  µ  !   x ( )  R  µ  !   x ( ) T x ( ) =  g  µ  !   x ( ) T   µ  !   x ( )  R x ( ) =  8 !  G  "   x ( ) !  µ   x ( ) ( ) 2 T x ( ) !   x  ( ) !  µ   x  ( )  !  "#$%   x  ( )  µ  "#$%   x  ( )  3N/ 190/11K/)/0*' 9/)1"0 "8 ,) /&/.90";,*)/9(. 8(/&M () , 9(;/KM/I/)M/)9 I-;I/M ()N";"*/)/"-1 ,)(1"90"I(. M(I"&,0 ;/9,K;,9/0(,& N,1 0/&/P,)9 .";I")/)91 @  R@<YS R@<ZS 3N/ .";I&/9/ /&/.90";,*)/9(. 8(/&M 190/11K/)/0*' 9/)1"0 () &,'/0/M ()N";"*/)/"-1 ,)(1"90"I(. T1I,./9(;/ ;/9,;,9/0(,&U A  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 3N/ /)/0*'K;";/)9-; 9/)1"0 "8 /&/.90";,*)/9(. 8(/&M1 () ;,99/0 4"M0(*" ]/M(),B ^<+9/IN,)' N99I1_22,0L(P<"0*2,J12@`C><CA@CD I<@D /O1< R@>AS a R@>ZS A  +I,./9(;/ ]/9,;,9/0(,&1 GN0(19"IN/ G,&"QB b"/KV(1/ c/.6KV/*/0 N99I1_22,0L(P<"0*2,J12@DCZ<CCZdC  T  00  x ( ) = 116 ! "  i j   x ( )  E   j   x ( )  E  i  x ( ) +  µ  i j   x ( )  H   j   x ( )  H  i  x ( ) ( ) + 4 !"  0  #   x ( ) i j   E   j   x ( )  E  i  x ( ) T  ii  x ( ) = 18 ! "  i j   x ( )  E   j   x ( )  E  i  x ( ) +  µ  i j   x ( )  H   j   x ( )  H  i  x ( ) ( ) ! 4 !   µ  0  "  i j   x ( )  H   H   j   x ( )  H  i  x ( ) ! 14 ! "  i j   x ( )  E   j   x ( )  E  i  x ( ) +  µ  i j   x ( )  H   j   x ( )  H  i  x ( ) ( ) i ,  j  , k   = 1,2,3 !  , "  , #   , $   = 0,1,2,3 T  0 i  x ( ) = ijk  { }  E   j   x ( )  H  k   x ( ) 4 ! "  #$%&   x ( )  µ  !"#$   x ( )  energy current density Poynting ! S T  i 0  x ( ) =  !  "#$%   x ( )  µ  !"#$   x ( )  ijk  { } !   j  j  '  x ( )  E   j  '  x ( )  µ  k  j  "  x ( )  H   j  "  x ( ) 4 !   momentum current density ! g ! S x ( ) ! g x ( ) !  E x ( ) !  E  1  x ( )  H  i  x ( ) =  0 !  µ  "  =  diag 1, ! 1, ! 1, ! 1 [ ]   R@<dS 3N/0/8"0/B () 9/0;1 "8 9N/ 0/,& .N,0*/ /&/.90(. 1-1./I9(J(&(9' ,)M 9N/ P(09-,& .N,0*/ P,.--; I/0;(99(P(9' R@<`S +" 8,0B W ,; ")&' #0(9()* e()19/()\1 8(/&M /O-,9(")1 () 1I,./K9(;/ *&"11()* "P/0 9N/ ,&&K(;I"09,)9 /&/.90";,*)/9(. M(1I/01(") M/I/)M()* ") 9N/ M/9/.9"0 ,)M ,II&(/M e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e()19/()\1 *0,P(9' 9/)1"0 8(/&M /O-,9(") R@<AS () 9N/ #/,6 8(/&M f/#9")(,) I"9/)9(,& I/0 -)(9 ;,11 &(;(9 9" */9 9N/ ,II0"L(;,9/ ["(11") /O-,9(") R@<XS T x ( ) = !  µ  "  T   µ  "   x ( ) !" T  00  x ( ) + T  11  x ( )  !  !  0 T x ( ) ! T  00  x ( ) " T  11  x ( ) ! T  00  x ( ) = !  0  E  1  x ( ) 2 16 !  1 + 68 !"   x ( ) 11 #$ %& T  11  x ( ) =  "  !  0  E  1  x ( ) 2 16 !  2 + 8 !"  11  x ( ) ( ) T x ( ) !  3 + 76 !"  11  x ( ) #$ %& !  0  E  1  x ( ) 2 16 !   f  ! k  !   x  ( )  R 00  x ( ) =  ! 8 !  G  "   x ( ) !  µ   x ( ) ( ) 2 T  00  x ( ) !  12 g 00  x ( ) T x ( ) " # $ % & '  =  ! 8 !  G  "  #$%&   x ( )  µ  !"#$   x ( ) ( ) 2  !  0  E  1  x ( ) 2 16 !  1 + 68 !"   x ( ) 11 () *+ !  123 + 76 !"  11  x ( ) () *+(),*+-" # $% & '  = 14 G  !  "#$%   x ( )  µ  !"#$   x ( ) ( ) 2 !  0  E  1  x ( ) 2 1 + 16 !"   x ( ) 11 ( )  R 00  x ( )  . Capacitor Weak FieldNewtonian Limit 2  !  "#$%   x ( )  µ  !"#$   x ( ) ( ) / 2 !   x ( ) / 2 !   x ( ) = 18 G  !  "#$%   x ( )  µ  !"#$   x ( ) ( ) !  0  E  1  x ( ) 2 1 + 16 !"   x ( ) 11 ( )  G")1(M/0 , *(,)9 )/*,9(P/ 0/1"),)./ R@<DS f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g+ f,P' F,99&/ H0"-I G&"1/ e)."-)9/01 #(9N 3(. 3,. gE=1<  !  11  x  ( ) ! 0 ! 2 !   x  ( ) "# 2 !  G  !  "#$%   x  ( )  µ  !"#$   x  ( ) ( ) !  0  E  1  x ( ) 2  !   x  ( ) 11 strongly amplified confined antigravity artificial dark energy  E  1  x ( ) 2
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