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金屬光柵在不同偏振下穿透機制之研究

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(1)Research on transmission mechanism of metallic gratings at different polarizations.

(2) Research on transmission mechanism of metallic gratings at different polarizations. Student. Wei-Lun Hung. Advisor. Dr. Shun-Tung Yen. A Thesis Submitted to Department of Electronics Engineering & Institute of Electronics College of Electrical Engineering and Computer Science National Chiao Tung University In Partial Fulfillment of the Requirements for the Degree of Master in Electronics Engineering June 2011 Hsinchu, Taiwan, Republic of China.

(3) P- (TM) S- (TE). Fabry-Perot. i.

(4) Research on transmission mechanism of metallic gratings at different polarizations Student. Wei-Lun Hung. Advisor. Dr. Shun-Tung Yen. Department of Electronic Engineering & Institute of Electronics National Chiao Tung University. Abstract We analyze transmission characteristics and near-field patterns of metallic gratings at different polarizations. We not only study the resonance transmission, but also focus on the transmission mechanism at Rayleigh wavelength where the standing wave is excited by incident wave. For P-polarization (TM), the standing wave causes surface charge redistribution, which results in null transmission. However, for S-polarization (TE), the constructive interference between incident wave and standing wave leads to high transmission. The calculation results are in good agreement with experiments. We show that the metallic gratings can be designed as optical filters for different polarizations by tuning the resonance wavelength of Fabry-Perot mode.. ii.

(5) MOSFET. Lab635. DC. iii.

(6) …………………………………………………... i. …………………………………………………... ii. ……………..………………………………………….. iii. …………..…………………………………………….. iv. ……...………………………………………………. vii ………………………………………………... 1 1.1. …………………………………………….. 1. 1.2. ………………………………………….. 3 …………………………………………… 4. 2.1. ………………………………………….. 4. 2.1.1. ………………………………………… 5. 1.. …………………………………………… 5. 2.. ………………………………… 7. 3.. ………………………………… 8. 2.1.2. ………………………………………... 14. 1.. ……………………………….. 14. 2.. ………………………………..…. 21 (1).. ………………..…………………. 21 iv.

(7) (2).. ……………………………..….. 24. (3).. ……………………...…….. 26 …………………………... 29. 3.1. P-. S-. …………………...……… 29. 3.1.1. ……………………….. 29. 3.1.2. ………………………..... 31. 3.2. P-. …………………………………..……… 32. 3.2.1. ………………..……....... 36. 3.2.2. …………………..…....... 40. 3.3. S-. ………………………………………..… 43. 3.3.1. …………………..…....... 43. 3.3.2. ……………………......... 46 ………………………………...…………….. 49. 4.1. …….…………………………..…………… 49 ………………………………...……..……… 52 ………………………………...……..…………... 54 ………………………………...……..……………….. 56. v.

(8) 1.1. 1 [1]. 1.2. 2 [2] ( ). 2.1. ( ). ( ). S-. ( ). ߝଵ. ( ) ߝ௠௘௧௔௟. 4. P-. ߝଷ. ( ). ߝ௦௟௜௧. (a) TM(2-25) (b) 26. 2.2 TE(2-32). 3.1. ax. 3.2. 3.3. ax=0.15Lx L. ax a z. 30. (a)TM (b)TE. 31. 0.15Lx 0.01Lx P-. 32. 3.4. 33 vi.

(9) 3.5. P-. kx0. 34. ax=0.15Lx. (a) L=0.15Lx (b) L=0.25Lx. (c)L=0.35Lx (d)L=0.45Lx. 3.6. ax=0.15Lx L=0.15Lx. 3.7. λ=1.012Lx (b) L=0.45Lx λ=1.28Lx. ax=0.15Lx L=0.45Lx. 3.8. (a). (a). 35. P-. (a) L=0.15Lx (b). 36. λ=Lx. 37. P-. ax=0.15Lx z=0. L=0.01Lx. (b). λ=Lx. P-. +1. -1 λ. 3.9. (a) (b) (c). 3.10 λ=Lx (a). 38. 1/4. 0. ax=0.15Lx. L=0.01Lx P-. 1/4. (b). vii. 39 0.

(10) 3.11 (a)λ=0.9 1 1.1 Lx. (b) λ=1. Ez. 40. 1.1 Lx Lx=24 µm. 3.12 P-. L=0.2 µm. ax=6 8 10 µm. 41. Si 11.2. 3.13 Lx=24 µm L=0.2 µm ax=6 µm P-. (a) λ=Lx 41. (b) λ=ඥεଷ Lx. 3.14 Lx=24 µm L=0.2 µm ax=6 µm P-. 42 (0th). (total). 3.15 S-. (a). L=0.01Lx. 43. ax=0.2~0.8 Lx (b) L=0.6Lx ax=0.8Lx λ=1.2Lx. 3.16 (a). |Ey| ax=0.8Lx. z=0. 3.17. (b). ax=0.8Lx. L=0.01Lx λ=Lx. S-. L=0.01Lx S-. (Ey). viii. λ=Lx. 44 +1 -1. λ=Lx 45.

(11) λ<Lx. 3.18 λ>ඥεଷ Lx. Lx<λ<ඥεଷ Lx. 3.19 S-. 46. Lx=24 µm L=0.2 µm. ax=18 20 22 µm. 47. Si 11.2. 3.20 Lx=24 µm L=0.2 µm ax=22 µm S-. (a) λ=Lx 48. (b) λ=ඥεଷ Lx. 4.1. 4.2. 49. (a) P-. Lx=24 µm ax=0.05Lx L=0.02Lx (b) S-. Lx=24 µm. ax=0.374Lx L=0.267Lx. 11.9. 4-2. ix. 50.

(12) 1.1 (Christiaan Huygens). (Augustin-Jean Fresnel). 1.1[1]. (. ). (Gustav Robert Kirchhoff) 1.2[1, 2]. (opaque). (Green's theorem). 1.1. [1] 1.

(13) 1.2. [2]. [3-7] Ebbesen. (FDTD)[9] (Waveguide mode). [8]. (RCWA)[10] (Modal expansion)[11]. [12-24] 2.

(14) 1.2. [12-17, 20, 23, 24]. (Rayleigh wavelength) [25-31] Fabry-Perot [18, 21, 22]. Fabry-Perot. 3.

(15) 2.1 2.1 S-. 2.1. ( ). P-. (. ). ( (. (. )   . (. ). ( ). . ). ) . 4. ( ). S(. ). P.

(16) 2.1.1 1. ( ) ( ) [32]. S-. P-. 0 1   ik x , g x v E(S ,)g ( x ) = −1 e  Lx   0     1   1  ik x (v ) EP,g ( x ) = 0  e x ,g  Lx  k  − x,g   k (v)   z,g 

(17) ,. 2-1a. 2-1b. ,. k x,g = (v). kz,g. ω c. Sinθ +. 2 n gπ. 2-2a. Lx. ω  =  ε v  − k x2, g , v = 1, 3 c . . 2. . 2-2b. g=1,2,3…N N. zˆ × H H FS , g ( x ) ≜. 1 Lx.  0  ik x ,g x  −1 e  . 5. 2-3a.

(18) FP , g ( x ) ≜. 1 Lx.  1  ik x ,g x  0 e  . 2-3b. E(S ,)g , ( x ) = FS , g ( x ). 2-4a. E(P ,)g , ( x ) = FP , g ( x ). 2-4b. v. v. zˆ × H. (v) S , g ,. ( x) = −. ck z(,vg). ωZ 0 εv. zˆ × H (Pv,)g , ( x ) = −. Z0. FS , g ( x ). 2-4c. FP , g ( x ). 2-4d. . ( ). E(1) ( x, z ) =. E(3) ( x, z ) =. ∑. zˆ × H(1) ( x, z ). ∑. zˆ × H(3) ( x, z ). ∑. σ =S ,P g. (. ik z( 3) ,g ( z − L ). (. (. ik z( 3) ,g ( z − L). ∑ zˆ × Hσ(3),g , ( x ) aσ(3),g e. σ =S ,P g. 6. ik z(1) ,g z. + bσ(3), g e. ik z(1) ,g z. ∑ zˆ × Hσ(1),g , ( x ) aσ(1),g e. σ =S ,P g. =. (. ∑ Eσ(1),g , ( x ) aσ(1),g e. ∑ Eσ(3),g , ( x ) aσ(3),g e. σ = S ,P g. =. ∑. ( ). − bσ(1), g e. + bσ(1), g e. − ik z(1) ,g z. − ik z( 3) ,g ( z − L ). − ik z(1) ,g z. − bσ(3), g e. ). 2-5a. 2-5b. ). − ik z( 3) ,g ( z − L). ). 2-6a. ). 2-6b.

(19) 2. ( ). ( ) (Parallel-plate waveguide). TE. TM. [33]. 0     − L a     x x   niπ  x − (2)    ETE x = ( ) 2  2   ,i ,  Sin    a a   x  x    . 2-7a.  Lx − a x      π x − n   2  j  2    Cos  (2) ETM , j , ( x ) =  a x ax         0  . 2-7b. i=1,2,3…I j=1,2,3…J. I . TE. zˆ × H. ( x) = −. TE TM. TM . zˆ × H. 1/√2 (2) TE ,i ,. J. k z( ,i) 2. Z0. ω. (2) ETE ,i , ( x ). c. 7. 2-8a.

(20) ω zˆ × H. (2) TM , j ,. ε slit. (2) ( x ) = − c ( 2) ETM , j , ( x ) Z 0k z , j. 2-8b. ,.  2 k z( ,k) =  ε slit . ω.  nkπ  −    c   ax  2. 2. 2-9. ( ). E(2) ( x, z ) (2)  (2) = ∑ ETE ,i , ( x ) aTE ,i e  i. ik z( ,2i ) z. (2)  (2) + ∑ ETM , j , ( x ) aTM , j e  j. (2) + bTE ,i e. ik z( 2, j) z. ik z( 2,i ) ( L − z ). (2) + bTM , je.  . 2-10a. ik z( ,2j) ( L − z ).  . ik z( 2,i ) ( L − z ).  . zˆ × H(2) ( x, z ) (2)  (2) = ∑ zˆ × HTE ,i , ( x ) aTE ,i e  i. + ∑ zˆ × H j. (2) TM , j ,. ik z( ,2i ) z. (2) − bTE ,i e. 2-10b. ik z , j z ik z , j ( L − z )  (2) (2) − e b e ( x )  aTM TM , j ,j  (2). (2). 3.. [34]. ( ) TM. TM. TE r=. 2-1 TM. 8. !

(21). !. "#.   .

(22) Ex = − Ez =.  ∂H y  i ε ( x ) k0  ∂z . 2-11a.  ∂H y  i ε ( x ) k0  ∂x . Hy=. 2-11b. i  ∂E z ∂E x  −   k 0  ∂x ∂z . 2-11c.  = $/%. ε'. rLx rLx  ε , x − ≤ ≤ metal  2 2 ε ( x) =  rLx r  ε slit , ≤ x ≤  1 −  Lx 2  2  x. z. 2-12. "# ', ( = )' (. Λ. ∂2Z ( z ) = −Λ 2 Z ( z ) 2 ∂z (. 2-13 2-11. 2-13 !'+,Λ(. ! ', ( = -' !'+,Λ(. 2-13. ∂X ( x )  = −iε ( x ) k0V ( x )  ∂x   2   ∂V ( x ) = −ik  1 − Λ X ( x) 0 2   ∂x  ε ( x ) k0 . 9. 2-14.

(23) 2-14.  ∂2 X ( x) = − ( ε metal k0 2 − Λ 2 ) X ( x )  2 ∂x  2  ∂ V ( x) = − ε k 2 − Λ2 V ( x) ( metal 0 )  ∂x 2 . = / 0 − Λ0. 2-15.  rLx   −iε metal k0  rLx  rLx        rLx  V −  Sin  β  x +   X ( x ) = X  − 2  Cos  β  x + 2   + β 2       2         V ( x ) = V  − rLx  Cos  β  x + rLx   + −i β X  − rLx  Sin  β  x + rLx              2   ε metal k0  2  2    2     .   rLx  −iε metal k0  rLx   rLx  V −  Sin ( β rLx )  X  2  = X  − 2  Cos ( β rLx ) + β     2      V  rLx  = V  − rLx  Cos ( β rL ) + −i β X  − rLx  Sin ( β rL ) x x     2  ε metal k0  2   2 . 2-16. 2-15. 2-16. 2-17. 2-17.   rLx     X  2    Cos ( β rLx )     =   rLx    −i β  V  2    ε k Sin ( β rLx )    metal 0  . −iε metal k0. rL   Sin ( β rLx )   X  − x   β 2        rLx   Cos ( β rLx )  V −   2  . 2-18. α = /   0 − Λ0   r    X   1 −  Lx     2     r     V   1 −  Lx     2    iε k     rL   Cos α (1 − r ) Lx  − slit 0 Sin α (1 − r ) Lx    X  x    α  2   =  − iα Sin α (1 − r ) L     rLx   Cos α (1 − r ) Lx  x   ε k V    slit 0   2  . 10. 2-19.

(24) 2-18. 2-19 (Bloch theorem) 2-18. 2-19.   r     rLx    X   1 −  Lx    X  − 2  2       =ΞΞ   1 2   r      rLx    V   1 −  Lx   V − 2   2        . iε slit k0   − − ⋅ − Cos 1 1 r L Sin r L α α     ( ) ( ) x x       α  Ξ1 =   − iα Sin α (1 − r ) L   Cos α (1 − r ) Lx  x   ε k   slit 0 .   Cos ( β rLx ) Ξ2 =   −i β  ε k Sin ( β rLx )  metal 0. 2-21a. −iε metal k0.  Sin ( β rLx )  β   Cos ( β rLx )  .   r     rLx    X   1 −  Lx    X − 2  2      ik L Sin θ  =e 0 x     r      rLx    V   1 −  Lx   V − 2   2        . 2-20. 2-20. 2-21b. 2-22. 2-22. ik0 Lx Sinθ. e  Ξ1Ξ 2 −   0 .   rLx   X −  0     2   =0   eik0 Lx Sinθ     rLx   V − 2     . 11. 2-23.

(25) (non-trivial solution).   eik0 Lx Sinθ Det  M −    0.    = 0 eik0 Lx Sinθ   0. TM. 2-24. (eigenvalue equation). Cos ( k0 Lx Sinθ ) − Cos α (1 − r ) Lx  Cos ( β rLx )  1  ε β αε +  slit + metal  Sin α (1 − r ) Lx  Sin ( β rLx ) = 0 2  αε metal ε slit β . Λ. 2-25. TM. 2-25. y. ( ) 2 ( 2 ) iΛl z ( 2 ) iΛl ( L − z )  H y( ) ( x, z ) = ∑ X TM , l ( x )  aTM + bTM , le , le . 2-26. l. X TM , l ( x ) =  rLx  −iε metal k0 rL  rL rL     V0,TM Sin  β  x + x  , − x ≤ x ≤ x Cos  β  x + 2  + 2  2 2 β        U Cos α  x − rLx  − i ε slit k0 V Sin α  x − rLx  , rLx ≤ x ≤  1 − r  L     x    1,TM 2  2  2 α 1,TM    2  . V0,TM. eik0Lx Sinθ − M 1 = M2. U1,TM = Cos ( β rLx ) +. 2-27. 2-28a. −iε metal k0. V1,TM = V0,TM Cos ( β rLx ) +. β. V0,TM Sin ( β rLx ). −i β Sin ( β rLx ) ε metal k0. 2-28b. 2-28c. M 1 = Cos α (1 − r ) Lx  Cos ( β rLx ) −. ε slit β Sin α (1 − r ) Lx  Sin ( β rLx ) αε metal 12. 2-28d.

(26) ik0 ε slit β Cos ( β rLx ) Sin α (1 − r ) Lx   M2 = −   αβ  +αε metal Cos α (1 − r ) Lx  Sin ( β rLx )   . 2-28e. TE. E y(. 2). ( x, z ) = ∑ X TE , l ( x ) aTE( 2), l eiΛ z + bTE(2), l eiΛ ( L− z )  l. l. 2-29. l. X TE , l ( x )  rLx  k0 rLx  rLx rLx     Cos  β  x + 2  + i β V0,TE Sin  β  x + 2  , − 2 ≤ x ≤ 2        = U Cos α  x − rLx  + i k0 V Sin α  x − rLx  , rLx ≤ x ≤ 1 − r  L 1,TE     x      1,TE 2  α 2  2  2    . V0,TE. eik0 Lx Sinθ − ψ 1 = ψ2. 2-30. 2-31a. k  rL  U1,TE = X  x  = Cos ( β rLx ) + i 0 V0,TE Sin ( β rLx ) β  2 . 2-31b. β  rL  V1,TE = V  x  = V0,TE ⋅ Cos ( β rLx ) + i ⋅ Sin ( β rLx ) k0  2 . 2-31c. ψ 1 = Cos α (1 − r ) Lx  Cos ( β rLx ). β − Sin α (1 − r ) Lx  Sin ( β rLx ) α ik0  β Cos ( β rLx ) Sin α (1 − r ) Lx   ψ2 =   αβ +αCos α (1 − r ) Lx  Sin ( β rLx )   . 2-31d. 2-31e. TE Cos ( k0 Lx Sinθ ) − Cos α (1 − r ) Lx  Cos ( β rLx ). 1 β α + ⋅  +  ⋅ Sin α (1 − r ) Lx  Sin ( β rLx ) = 0 2 α β . 13. 2-32.

(27) 2.1.2. (unit cell). (Hermitian operator). (matching boundary condition). 1. 2-5a 2-5b. ∑ ∑ Eσ ( x ) ( aσ σ = S ,P g. (1) , g ,. (1) ,g. (. 2-10a. (. ik z( ,2i ) L. (2) (2) (2) + ∑ ETM , j , ( x ) aTM , j + bTM , j e j. 2-10b. + bσ(1), g ). (2) (2) (2) = ∑ ETE ,i , ( x ) aTE ,i + bTE ,i e i. 2-6a 2-6b. ) ik z( ,2j) L. 14. 2-33a. ).

(28) ∑ ∑ Eσ ( x ) ( aσ σ = S ,P g. (3) , g ,. (3) ,g. (. (2) (2) = ∑ ETE ,i , ( x ) aTE ,i e i. + bσ(3), g ). ik z( ,2i ) L. (. (2) (2) + ∑ ETM , j , ( x ) aTM , j e j. ik z( ,2j) L. zˆ × Hσ ( x ) ( aσ ∑ ∑ σ =S ,P g. (1) , g ,. (1) ,g. (. 2-33b. (2) + bTM ,j. ik z( ,2i ) L. (. (2) (2) (2) + ∑ zˆ × HTM , j , ( x ) aTM , j − bTM , j e j. zˆ × Hσ ( x ) ( aσ ∑ ∑ σ =S ,P g. (3) , g ,. (3) ,g. (. (2) (2) = ∑ zˆ × HTE ,i , ( x ) aTE ,i e i. (. ). 2-33c. ik z( ,2j) L. ). − bσ(3), g ). ik z( ,2i ) L. (2) (2) + ∑ zˆ × HTM , j , ( x ) aTM , j e j. ). − bσ(1), g ). (2) (2) (2) = ∑ zˆ × HTE ,i , ( x ) aTE ,i − bTE ,i e i. ). (2) + bTE ,i. (2) − bTE ,i. ik z( ,2j) L. ). 2-33d. (2) − bTM ,j. )  . (. 0. ~. 2-33a.  4 0. ). 2-33b. aS(1), g + bS(1), g. (. (2)  Lx +2 ax (2)  (2) * (2) ik z ,i L = ∑  ∫Lx − ax ETE ,i , ( x ) FS , g ( x ) dx  aTE ,i + bTE ,i e i  2 . (. ).  Lx +2 ax (2)  (2) * ik z( 2, j) L (2) + ∑  ∫Lx − ax ETM , j , ( x ) FS , g ( x ) dx  aTM + b e ,j TM , j j  2 . 15. 2-34a. ).

(29) a P(1), g + bP(1), g. (. ( 2)  Lx +2 ax (2)  (2) * (2) ik z ,i L = ∑  ∫Lx − ax ETE ,i , ( x ) FP , g ( x ) dx  aTE + b e TE ,i ,i i  2 . ). (.  Lx +2 ax (2)  (2) * ik z( ,2j) L (2) + ∑  ∫Lx −ax ETM , j , ( x ) FP , g ( x ) dx  aTM , j + bTM , j e j  2  2-33c. 2-34b. ). 2-33d. aS(3), g + bS(3), g. (.  Lx +2 ax (2)  (2) ikz( ,2i ) L * (2) = ∑  ∫Lx − ax ETE ,i , ( x ) FS , g ( x ) dx  aTE + bTE ,i e ,i i  2 . ). (.  Lx +2 ax (2)  (2) ikz( ,2j) L * (2) + ∑  ∫Lx − ax ETM , j , ( x ) FS , g ( x ) dx  aTM + bTM , je ,j j  2  aP(3), g + bP(3), g. (.  Lx +2 ax (2)  (2) ikz( 2,i ) L * (2) = ∑  ∫Lx − ax ETE ,i , ( x ) FP , g ( x ) dx  aTE + bTE ,i e ,i i  2 . (. 2-34c. ). ).  Lx +2 ax (2)  (2) ikz( 2, j) L * (2) + ∑  ∫Lx − ax ETM , j , ( x ) FP , g ( x ) dx  aTM , j e + bTM ,j j  2 . 2-34d. ). 2-34. A(1) + B (1) = M E ( A(2) + DB ( 2) ). 2-35a. A(3) + B (3) = M E ( DA(2) + B ( 2) ). 2-35b. 5. 6. A(1) = ( aS(1),1 , ..., aS(1), N , aP(1),1 , ..., aP(1), N ). T. (2) (2) ( 2) (2) A( 2) = ( aTE ,1 , ..., aTE , I , aTM ,1 , ..., aTM , J ). A(3) = ( aS(3),1 , ..., aS(3), N , aP(3),1 , ..., aP(3), N ). T. 16. 2-36a T. 2-36b 2-36c.

(30) ( = (b. B (1) = bS(1),1 , ..., bS(1), N , bP(1),1 , ..., b(1) P,N. B (2). (2) TE ,1. (. ). T. (2) (2) (2) , ..., bTE , I , bTM ,1 , ..., bTM , J ). B (3) = bS(3),1 , ..., bS(3), N , bP(3),1 , ..., b(3) P,N 78. 2-36d T. ). T. 2-36e 2-36f. 9.  [ M 11 ]g ,i ME =   [ M 21 ] g ,i   [ DTE ]i ,i ' D=  0J ×I  0;×=. [ M 12 ]g , j   [ M 22 ]g , j    [ DTM ] j , j ' . 0I ×J. >×?. 2-38 0=×;. [ M 11 ]g ,i = ∫. 2-37. Lx + a x 2 Lx − a x 2. ?×>. :. (2) ETE ,i , ( x ) FS , g ( x ) dx *. 2-39a. [ M 12 ]g , j = ∫. Lx + a x 2 Lx − a x 2. (2) ETM , j , ( x ) FS , g ( x ) dx. 2-39b. [ M 21 ]g ,i = ∫. Lx + a x 2 Lx − a x 2. (2) ETE ,i , ( x ) FP , g ( x ) dx. 2-39c. [ M 22 ]g , j = ∫. [ DTE ]i,i ' = e. Lx + a x 2 Lx − a x 2. *. *. (2) ETM , j , ( x ) FP , g ( x ) dx *. ik z( ,2i ) L. [ DTM ] j , j ' = e. δ ii '. 2-39d 2-40a. ik z( ,2j) L. δ jj '. 2-40b. 17.

(31) ck z(2) ,i. ω. (. (2) (2) aTE ,i − bTE ,i ⋅ e. ik z( 2,i ) L. ). ck z(1), g  Lx +2 a x  (1) * (2) (1) =∑  ∫Lx − ax FS , g ( x ) ETE ,i , ( x ) dx  ( aS , g − bS , g ) ω  2 g  +∑. ck. g. (. ωε slit ck z(2) ,j. 1 (1) z,g.  Lx +2 a x  (1) * (2) (1) E F x x dx ( ) ( )  ∫Lx − a x P , g  ( aP , g − bP , g ) TE ,i ,  2 . (2) (2) aTM , j − bTM , j e. ik z( ,2j) L. ). ck z(1), g  Lx +2 a x  (1) * (2) (1) =∑ F x E x dx ( ) ( )  ∫Lx − a x S , g  ( aS , g − bS , g ) TM , j , ω  2 g  +∑. ck. g. ck z(2) ,i. ω. (. 1 (1) z,g. (2) aTE ,i e. +∑ g. ωε slit ck. (2) z, j. ck. (. ik z( ,2i ) L. (2) − bTE ,i. ). ik z( ,2j) L. (2) − bTM ,j. ). Lx + a x ck z(3)  (3) * ,g  (2) (3) 2 =∑ F x E x dx ( ) ( )  ∫Lx − a x S , g  ( aS , g − bS , g ) TM , j , ω  2 g . +∑ g. ck. 2-41c.  Lx +2 a x  (3) * (2) (3) F E x x dx ( ) ( )  ∫Lx − a x P , g  ( aP , g − bP , g ) TE ,i ,  2 . (2) aTM , je. 3 (3) z,g. 2-41b.  Lx +2 ax  (1) * (2) (1) F E x x dx ( ) ( )  ∫Lx −a x P , g  ( aP , g − bP , g ) TM , j ,  2 . Lx + a x ck z(3)  (3) * ,g  (2) (3) 2 =∑  ∫Lx − ax FS , g ( x ) ETE ,i , ( x ) dx  ( aS , g − bS , g ) ω  2 g . 3 (3) z,g. 2-41a. 2-41c.  Lx +2 ax  (3) * (2) (3) F E x x dx ( ) ( )  ∫Lx −a x P , g  ( aP , g − bP , g ) TM , j ,  2  2-41. Y (2) ( A( 2) − DB (2) ) = M H Y (1) ( A(1) − B (1) ). 2-42a. Y ( 2) ( DA( 2) − B ( 2) ) = M H Y (3) ( A(3) − B (3) ). 2-42b. 18.

(32) ε   (v) . ε0. ck z( ,vk). YS   k ,k ' = ω δ kk '. 2-43a. YP( v )  = ωεvv δ kk '   k ,k ' ck ( ) z ,k. 2-43b. @ . Y. (v ).  YS( v )    k ,k ' =  0  .   YP( v )     k ,k ' . 0. 2-44. 7A.  [ M 11 ] † g ,i MH =  [M ] †  12 g ,i. [ M 21 ]g , j† . [ M 22 ]g , j. †.   . 2-45. 2-35. 2-42.  A(2)   (2)  B   YH(2) + M H YH(1) M E =  ( M H YH(3) M − YH(2) ) D . 2-46. ( M HYH(1) M E − YH(2) ) D   2 M HYH(1) A(1)   (3) (3)  M H YH(3) M E + YH(2)   2 M H YH B  −1. A(3) = M E ( DA(2) + B (2) ) − B (3). 2-47a. B (1) = M E ( A(2) + DB (2) ) − A(1). 2-47b. 5. 5 19. 2-46. ( ).

(33) 2-47. ( ). 6 S-. (Poynting vector). P-. TS ,m =. Re ck. ∑ Re. (1) z ,n. ω. n. a. ck z(3) ,m. (1) 2 S ,n. ∑ Re n. g=1. ck z(1),n. ω. + ∑ Re. a. ωε 3 ck z(3) ,m. (1) 2 S ,n. a P(3),m. ωε1 ck z(1),n. 2-48a. a. (1) 2 P ,n B ( 3) = 0. 2. + ∑ Re n.  = 0 FG,. 2. n. Re TP ,m =. ω. aS(3),m. ωε1 ck z(1),n. 2-48b. a. (1) 2 P ,n B ( 3) = 0. 2-2a

(34) , = $/% D,E. FH,. S P. S-. P-. aS(1,)n = δ n1 (1). a P ,n =. ck z(1),n. ω ε1. 2-49a. δ n1. 2-49b. S x z. y. P . c ,J /$√. x. 20.

(35) 2.. S-. P-. ( ) "

(36). TE. !#. TE. TE TM ". !

(37). TM. P-. TM. "#. !. S-. S P ( ). TE TM. (2-25. 2-32) ( ). P-. TM. TE. (1). P. ( ). ( ) !

(38). 2-26. "#. 1 ik x ,n x (1) e aP ,n + bP(1),n ) ( Lx. ∑ n. (. = ∑ X TM , l ( x ) aTM , l + bTM , l e l. (2). (2). iΛ l L. 1 ik x ,n x (3) e aP ,n + bP(3),n ) ( Lx. ∑ n. (. = ∑ X TM , l ( x ) aTM , l e l. (2). iΛ l L. ( ). (2). + bTM , l. ). 2-50a. ). 2-50b. 21.

(39) ∑ n. =. 1. ε2 ( x). ∑ n. =. 1 ik x ,n x (1) (1) e k z ,n ( a P ,n − bP(1),n ) Lx. ∑X. TM , l. l. (2). iΛ l L. 2-50c. ). (3) 1 ik x ,n x k z ,n (3) e a P ,n − bP(3),n ) ( ε3 Lx. 1. ε2. ( x ) Λ l ( aTM , l − bTM , l e (2). X ∑ x ( ). 2-50d. ( 2 ) iΛ h (2) − bTM ( x ) Λ l ( aTM , le ,l ) l. TM , l. l. ( ). (. . /. a. (1) P ,m. +b.  1 = ∑  L l  x. a. (3) P ,m. +b.  1 = ∑  L l  x. (a. − bP(1),m ). k z(1),m. ε1. (1) P ,m. (3) P ,m. (1) P ,m.  Λ = ∑ l  L l  x k z(3) ,m. ε3. (a. (3) P ,m.  r 1−  Lx  2 rL − x 2. ∫. K ,L

(40) ).  r  1−  Lx  2 rL − x 2. X TM , l ( x ) e.  r 1−  Lx  2 rL − x 2. X TM , l ( x ) e. ∫. ∫. X TM , l ( x ). ε2 ( x). e. ik x , m x. e. ik x , m x. ik x , m x.  (2) ( 2 ) iΛl L dx  aTM , l + bTM , l e  . ). 2-51a.  ( 2 ) iΛ L ( 2) l + bTM dx  aTM , le ,l  . ). 2-51b. ik x , m x. (. (.  (2) ( 2 ) iΛ l L dx  aTM , l − bTM , l e  . (. ). 2-51c. − bP(3),m ).  Λ = ∑ l  L l  x.  r 1−  Lx  2 rL − x 2. ∫. X TM , l ( x ). ε2 ( x).  ( 2 ) iΛ L (2) l dx  aTM − bTM , le ,l  . (. 22. ). 2-51d.

(41) N. Aσ( v ) = ( aσ( v,1) , ..., aσ( v, )N ). 2-52a. Bσ( v ) = ( bσ( v,1) , ..., bσ( v, N) ). 2-52b. T. σ. S. T. P. [ χ ]m,l. 1 = Lx. [Ω]m,l. Λ = l Lx.  r  1−  Lx  2 rL − x 2. ∫.  r  1−  Lx  2 rL − x 2. ∫. X TM , l ( x ) e. X TM , l ( x ). ε2 ( x). e. [ K ]m,l = eiΛ Lδ ml Y. . =. k z( ,vm). εv. dx. ik x ,m x. dx. 2-53a. 2-53b 2-53c. l. (v ) H m ,l. ik x ,m x. δ ml. 2-53d. 2-37 (2) (2) AP(1) + BP(1) = χ ( ATM + KBTM ). 2-54a. (2) ( 2) AP(3) + BP(3) = χ ( KATM + BTM ). 2-54b. ( 2) (2) YH( ) ( AP(1) − BP(1) ) = Ω ( ATM − KBTM ). 2-54c. ( 2) (2) YH( ) ( AP(3) − BP(3) ) = Ω ( KATM − BTM ). 2-54d. 1. 3. 2-54. 23.

(42) ( 2)  ATM   (2)   BTM . (Ω.  Ω −1YH(1) χ + I =  Ω −1Y ( 3) χ − I K H . (. ). ). . 5H. (Identity matrix) 2-55. ( ). 2-54a 2-48b. S-. ( Π )m ,l Ω. ( ). Λ = l Lx.  r  1−  Lx  2 rL − x 2. ∫. Π. 2-55. YH(1) χ − I K   2Ω −1Y (1) A(1)  H P   3 ( ) − 1 (3) 3 Ω −1YH( ) χ + I   2Ω YH BP   −1. "

(43). 2-29. X TM , l ( x ). ε2 ( x). e. ik x ,m x. !#. . 6H. 2-54b 2-49b. P-. 2-56. dx. S-. (overlap integral). (2). ( ). TE. TM. (2-25. 2-32) α β 24.

(44) 1043. 100i Cos(100i) Λ 20. 0 2-25. 2-32. (Drude model) 8.47x1028 (m-3). (conductivity). 5.69x107 (s/m) 2.2. 2. (initial guess). 25.

(45) 2.2. (a). (3).. TM(2-25) (b). TE(2-32). (overlap integral) (Ω χ. Π). χ. 1 Lx.  r  1−  Lx  2 rL − x 2. ∫. 1 = Lx 1 + Lx 1 + Lx 1 + Lx. X TM , l ( x ) e. ik x ,m x. dx. rLx 2 rLx − 2. rL   ik x   Cos  β  x + x   e x ,m dx 2   . rLx 2 rL − x 2.  −iε metal k0 rLx    ik x ,m x   V Sin x + dx β  0,TM   e   2 β     . ∫ ∫. ∫.  r  1−  Lx  2 rLx 2.  rLx    ik x ,m x   dx U1,TM Cos α  x −   e 2      . ∫.  r  1−  Lx  2 rLx 2.  ik0 rLx    ik x ,m x   dx  − V1,TM Sin α  x −   e 2 α     . 26. 2-57.

(46) 1 Lx =. ie. rLx 2 rL − x 2. ∫. rL   ik x   Cos  β  x + x   e x ,m dx 2   . 1 − irLx k x ,m 2.  −eirLx k x ,m k x ,m + k x ,mCos ( β rLx ) + i β Sin ( β rLx )    2 2 Lx ( k x ,m − β ). ) (. (. ) . − i ( β + k x , m ) rLx  ei ( β − k x ,m )rLx − 1 e −1 e  = −  2i Lx  ( β − k x ,m ) ( β + k x ,m )  1 irLx k x ,m 2. 2-58.  . 1 ± (1 − 2 r )   Exp i ( s − k x ,m ) Lx  −1 2 1 ±   S (s) = 2i Lx ( s − k x ,m ). 2-59a. 1 ± (1 − 2 r )   Exp  −i ( s + k x ,m ) Lx  −1 2 1 ±   T (s) = 2i Lx ( s + k x ,m ). 2-59b. 1. Σ1 = e 2. Σ2 = e. irLx k x ,m.  −  k0ε metal − − S ( β ) + T − ( β )) (  ( S ( β ) − T ( β ) ) − V0,TM β  . 1 − irLx k x , m 2. k0V1,TM +   + + S (α ) + T + (α ) )  ( U1,TM ( S (α ) − T (α ) ) − α  . 2-60a. 2-60b. P-. [ χ ]m,l. 1 = Lx. [Ω]m,l. Λ = l Lx.  r 1−  Lx  2 rL − x 2. ∫.  r  1−  Lx  2 rL − x 2. ∫. Σ. X TM , l ( x ) e X TM , l ( x ). ε2 ( x). ik x , m x. e. dx = Σ1 + Σ 2. 2-61a.  Σ  dx = Λ l  1 + Σ 2   ε metal . 2-61b. ik x ,m x. Σ0 27.

(47) S-. 28.

(48) [35]. PP-. 3.1 P-. S-. S-. S-. P-. S-. 3.1.1. k0 = k z 2 + k ⊥ 2. 3-1. . kT kT. k kT. z. 29.

(49) (TEM mode). 3.1. ax. ax az. TE TM. 3.1 (Parallel-plate waveguide). TE. (Rectangular waveguide). 30.

(50) P-. S-. TE TM P-. S-. TM TE. 3.1.2. P-. TM. TM. S-. 3.2. TEM. TE. (a)TM. (b)TE. 31. 3.2(a). 3.2(b). TEM.

(51) PS-. PP-. 3.2 PP-. 3.3. ax=0.15Lx. L=0.15Lx. 0.9 1.1. 3.3 ax=0.15Lx. L. 0.15Lx. 32. 0.01Lx. P-.

(52) (Fano resonance)[36, 37]. 3.4. (state) (discrete). (dispersion relation). 3.4. (surface plasmon polaritons) (spoof surface plasmon). 33.

(53) (n) ωSPP ( k x,0 ) = c. U VW V. ( ). 1. ε dielectric. k x ,0 +. 2π n Lx. 3-2. ( ). 1. 3.5 Pkx0 ax=0.15Lx (a) L=0.15Lx (b) L=0.25Lx (c)L=0.35Lx (d)L=0.45Lx . ωGHH. 3.5(a). 3.5(b)(c)(d) Fabry-Perot. 34.

(54) P-. 3.6(a) ax=0.15Lx L=0.15Lx 3.6(b) ax=0.15Lx. L=0.45Lx. 3.6(a). 3.6 (b) L=0.45Lx. ax=0.15Lx λ=1.28Lx P-. (a) L=0.15Lx. λ=1.012Lx. 3.7. ω p2 ε (ω ) = 1 − ω (ω + iγ ) 3.7. ωp. 9 eV. 3-3. γ 0.1 0.01 0.001 eV( 35. ωp.

(55) γ. 8 10 eV. ωp. 0.01 eV. γ 0.02 eV). 10.8 eV. 3.7(a). 3.7(b) Fabry-Perot. 3.7. ax=0.15Lx. (a) L=0.15Lx (b) L=0.45Lx. 3.2.1 P-. 36. P-.

(56) 3.3 ax=0.15Lx. 3.8 (a) λ=Lx P-. L. ax=0.15Lx. 0.15Lx. λ=Lx. L=0.01Lx +1. 0.01Lx. z=0. (b). -1. λ=Lx . ,Y. 2-2(b). . ,Y. 2-2(b). 3.8(b) !

(57). P+1 -1. Y  Z1. z. !. "#. . ,Y +x -x. 37.

(58) (K . K  . ) !. !. 3.8(a). λ 1/4. 3.9 (b). (c). (a) 0. 3.9 0 0.5λ. λ. 0.25λ 90. i. 38. 0.75λ Re[E × H* ].

(59) 3.10. !. , +1 -1 45. 45. +1 -1 , 3.8. 3.10 λ=Lx. ax=0.15Lx (b). L=0.01Lx. P-. (a). 1/4. 0. ! 3.11(a) ,. z. (induce). λ=0.9 1 1.1 Lx , (dipole). 39.

(60) λ=Lx. z. ,. 3.11(b). λ=1.1Lx. λ=Lx. 3.11 (a)λ=0.9. 1 1.1 Lx. (b) λ=1. Ez. 1.1 Lx. 3.2.2 3.12 24 µm. 0.9~10 THz. 11.2. 40. 11.9.

(61) 3.12 P-. Lx=24 µm L=0.2 µm. 3.13 Lx=24 µm L=0.2 µm. ax=6 µm. ax=6. P-. 8. 10 µm. Si 11.2. (a) λ=Lx (b) λ=/ε Lx. 2-2(b) ( ). ( ) λ=Lx. ( ). 41.

(62) ( ). λ=/ε Lx. λ=Lx λ=/ε Lx. 3.10(a) ( ) 3.13(b). ( ) ( ) x. +1. -1. / ε[. λ=. P-. 0. Lx. ( ) +2 -2. 3.14 Lx=24 µm L=0.2 µm ax=6 µm P(0th). (total). 3.14 (0th). 42. (total).

(63) 3.3 S3.3.1. 3.15 SL=0.6Lx. (a). L=0.01Lx λ=1.2Lx. ax=0.8Lx. 3.1.2. ax=0.2~0.8 Lx (b) |Ey|. S3.15(a). L=0.01Lx S-. Fabry-Perot. 3.15(b). Ey. Fabry-Perot 3.15(a) 43. λ=Lx.

(64) 3.16 (a) λ=Lx S-. ax=0.8Lx. L=0.01Lx +1. λ=Lx. z=0. (b). -1. λ=Lx. PSax=0.8Lx. 3.16 "

(65). L=0.01Lx. λ=Lx +1. !# !# 0 +1. !#. -1. " -1. 3.16(a) !# 3.16(a). +1 -1. 0. 1 (Evanescence wave). 44.

(66) λ=Lx. PS(Lorentzian function). 3.17. ax=0.8Lx. 3.17 . 0. λ=Lx. L=0.01Lx S-. z. 45. x. (Ey).

(67) 3.3.2. λ<Lx. 3.18. 3.18. Lx<λ</ε Lx. 2-2(b) λ<Lx. ( ). Lx<λ</ε Lx λ>/ε Lx. ( ) ( ). λ>/ε Lx. ( ) ( ) ( ). ( ). 3.19. P-. 11.2 λ=Lx. λ=Lx. λ=/ε Lx. 3.20(a). ( ). ( ). ( ). 46.

(68) λ=/ε Lx. 3.20(b). ( ). ( ) ( ). 1. 1 3.4. ( )+2 -2. 3.19 S-. Lx=24 µm L=0.2 µm. 47. ax=18. 20. 22 µm. Si 11.2.

(69) 3.20 Lx=24 µm L=0.2 µm. ax=22 µm S-. 48. (a) λ=Lx (b) λ=/ε Lx.

(70) 4.1 P-. S-. Fabry-Perot. PTEM. P-. S-. TEM. Fabry-Perot. S2ax>λ λ>Lx. Fabry-Perot. S-. ax>(Lx/2) 3.15(b) S-. 4.1. 4.1. 49.

(71) 2π   mπ   nπ   = +  ε slit λ   L   a x   2. P-. 2. n. 0.  λ =  P - polarized : n = 0 → L x    S - polarized : n = 1 → λ =  Lx   . 2. 4-1 S-. 1. 2 ε slit L m Lx 2 ε slit 2.  1   1    +   L / Lx   a x / Lx . 4-2 2. 4.2. 4.2 (a) PL=0.267Lx. Lx=24 µm ax=0.05Lx L=0.02Lx (b) S11.9. Lx=24 µm. εslit=11.9 50. Lx=24 µm ax=0.374Lx 4-2. λ=1.5Lx.

(72) 4.2. 4-2. P-. S-. ( ). ( ). 2k z L + 2φ = 2nπ. 4-3. (. ). (. ). 4-2. 51.

(73) ( ). P-. PP-. SS-. 1. 1. 52. S-.

(74) Fabry-Perot P-. 53. S-.

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(76) 085415 (2003). 30.Y. Xie et al., Optics Express 14, 6400 (2006). 31.J. Weiner, and F. D. Nunes, Optics Express 16, 21256 (2008). 32.Hong-Wen Hsieh, “Study of Extraordinary Optical Transmission: Theory and Application”, NCTU, master thesis in electronic engineering department (201007). 33.Marcuvitz, N., Waveguide Handbook, McGraw-Hill, U.S. (1951). 34.P. Sheng, R. S. Stepleman, and P. N. Sanda, Physical Review B 26, 2907 (1982). 35.Chung -Chun Sun, “Implementation of Terahertz Phase Retarders on Metallic Films Perforated with Asymmetric Cross Shaped Holes”, NCTU, master thesis in electronic engineering department (201009). 36.U. Fano, Physical Review 124, 1866 (1961). 37.C. Genet, M. P. van Exter, and J. P. Woerdman, Optics Communications 225, 331 (2003).. 55.

(77) (Wei-Lun Hung). 74 11 8 (93.9-97.6) (97.9-100.6). Research on transmission mechanism of metallic gratings at different polarizations.. 56.

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