- Page 2 and 3:
I. Gelombang EMII. Interaksi Gelomb
- Page 4 and 5:
Bahan optik bersifat dielektrik, is
- Page 7 and 8:
Gelombang bidangrErH= uˆ1= uˆE2oH
- Page 9 and 10:
∇.S + ∂tU= −J.E∂Ur r v r r
- Page 11 and 12:
2.2 Indeks bias dengan model elektr
- Page 13 and 14:
Tuliskan: n=n’-in”Tinjau gelomb
- Page 15 and 16:
2.4 Pulsa optik dan kecepatan grupD
- Page 17 and 18:
Dispersi materialBilangan gelombang
- Page 19 and 20:
3.2 Refleksi dan TransmisiTE atau g
- Page 21 and 22:
21Koefisien refleksi:iiixxxxxEsssnk
- Page 23 and 24:
23Koefisien refleksi:xxxxEpppknknkn
- Page 25 and 26:
3.3 Refleksi total internalk r1'k r
- Page 27 and 28:
Koefisien refleksi pada saat reflek
- Page 29 and 30:
ErH2∝=eii ( t k r2 .rω − )∇r
- Page 31 and 32:
Surface PlasmonReflectance10.980.96
- Page 33 and 34:
Dengan menggunakan syarat kontinuit
- Page 35 and 36:
Sistem 2-lapisan, d=0:x0n 1n 2zGel
- Page 37 and 38:
Komponen2 E x dan E z membentukpola
- Page 39 and 40:
39xzn 1n 2qxee −px[ ] cnnnnnnnncn
- Page 41 and 42:
41)()()()(),,(ztizztixozexHexEitzxH
- Page 43 and 44:
43dkidikdkixxxxxxxxdikxxxxxxerrette
- Page 45 and 46:
3.7 Attenuation Total Reflection (A
- Page 47 and 48:
Hasil-hasil perhitungan:1.41.21n 1
- Page 49 and 50:
10.8Reflectance0.60.4n 3 =10.2035 3
- Page 51 and 52:
IV. MEDIA BERLAPIS ISOTROPIK4.1 Per
- Page 53 and 54:
53⎟⎟⎠⎞⎜⎜⎝⎛=− 2200
- Page 55 and 56:
55⎟⎟⎠⎞⎜⎜⎝⎛−−−
- Page 57 and 58:
4.2 Perumusan untuk Sistem Multilap
- Page 59 and 60:
59⎟⎟⎠⎞⎜⎜⎝⎛⎟⎟⎠
- Page 61 and 62:
61⎟⎟⎠⎞⎜⎜⎝⎛+−⎟
- Page 63 and 64:
V. MEDIA BERLAPIS PERIODIK 1-D5.1 M
- Page 65 and 66:
65⎟⎟⎠⎞⎜⎜⎝⎛⎟⎟⎟
- Page 67 and 68:
67⎥⎦⎤⎢⎣⎡⎟⎟⎠⎞⎜
- Page 69 and 70:
5.2 Gelombang Bloch dan struktur pi
- Page 71 and 72:
⎛⎜⎝ACB ⎞⎛a⎟⎜D ⎠⎝b
- Page 73 and 74:
Hubungan dispersi:eiKΛ=12( A+D)±1
- Page 75 and 76:
ωβ = 0gapgapgapK2π/ΛCahaya bisa
- Page 77 and 78:
5.3 Reflektor BraggMedium berlapis
- Page 79 and 80:
TE (s); n 1=3,0 n 2=3,6 d 1=d 2=2um
- Page 81 and 82:
N=15, n 1=3,0 n 2=3,6 d 1=d 2=2 um1
- Page 83 and 84: 10.90.8n1=1.5n2=2.5λ o=0,6 umN=30R
- Page 85 and 86: 85( )[ ] 0)cos(2221222222222=+++⎥
- Page 87 and 88: dA− 2iβdz2⎛ ω+⎜2⎝ cn2o22
- Page 89 and 90: 89ziziaeidzdbbeidzdaδδκκ22;−=
- Page 91 and 92: RκL = 10.70.60.50.40.30.20.10-15 -
- Page 93 and 94: Reflektor Bragg sinusoida dengan ap
- Page 95 and 96: 10.810.8γ=50.60.4Reflektans0.60.40
- Page 97 and 98: 97o n onzzGnnzn
- Page 99 and 100: 99)(2)()()()()(),(φδφδ−−==z
- Page 101 and 102: 101Reflekror Bragg dengan chirp dan
- Page 103 and 104: 7. GELOMBANG TERPANDU DALAM MEDIA B
- Page 105 and 106: Gelombang terpandu TEEy( x,z,t)=Em(
- Page 107 and 108: Gelombang terpandu TEn 3=3.2n 2=3.5
- Page 109 and 110: Gelombang terpandu TMHy( x,z,t)=Hm(
- Page 111 and 112: 111)()(1)()]([2*]xRe[22*2121xnxdxxx
- Page 113 and 114: 7.2 Sifat umum pandu gelombang diel
- Page 115 and 116: Gunakan teorema Green:lim∫C→∞
- Page 117 and 118: ∇2rEr2∂ E− μoε2∂ t=02 2{
- Page 119 and 120: dAk iωβk*−i(βm−βk) z= −
- Page 121 and 122: ∑lδβa2mml( β2l− β )rEr r*
- Page 123 and 124: 7.3.2 Perturbasi dielektrik secara
- Page 125 and 126: Tanda dari faktor β1 / β1dan β2/
- Page 127 and 128: zn sn an sn bn sJika kedua pandugel
- Page 129 and 130: 1290)()(22*)(222*22=Δ+Δ+∂∂−
- Page 131 and 132: A(z)=( C1sinsz+ C2cos sz)( / 2 ) ze
- Page 133: 8. OPTIK NONLINIER8.1 Pengertian No
- Page 137 and 138: Modulatorφ iLdφ oVφo= φ +i= φ
- Page 139 and 140: Fungsi Logika XORaPolarisasi cahaya
- Page 141 and 142: 141Penguat Optik),(),(),(2(2)(1)ω
- Page 143 and 144: SwitchingFebry-PerotI oI oI iI iBah
- Page 145: 145