Optik Moderen

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72Selanjutnya, dengan vektor-vektor eigen ditentukan sbb:⎟⎟⎠⎞⎜⎜⎝⎛=⎟⎟⎠⎞⎜⎜⎝⎛⎟⎠⎞⎜⎝⎛ΛooiKoobaebaDCBA( )AeBbaiKoo−= Λ⎟⎟⎠⎞⎜⎜⎝⎛−=⎟⎟⎠⎞⎜⎜⎝⎛ΛAeBQbaiKooQ=konstanta⎟⎟⎠⎞⎜⎜⎝⎛⎟⎠⎞⎜⎝⎛−−=⎟⎟⎠⎞⎜⎜⎝⎛ooNNNbaACBDba
Hubungan dispersi:eiKΛ=12( A+D)±14( A +D)2imajiner− 1cosKΛ =12( A+D)=cosk1xd1cosk2 xd2−12⎛⎜⎝kk2 x1x+kk1x2 x⎞⎟sin⎠k1xd1sink2 xd2kix2⎛ niω⎞ 2 niω= ⎜ ⎟ − β = cos θi;i⎝ c ⎠ c= 1,2Harga cos KΛ ditentukan oleh ω dan β. Kurva ω vs βdisebut kurva dispersi.73
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I. Gelombang EMII. Interaksi Gelomb
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Bahan optik bersifat dielektrik, is
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Gelombang bidangrErH= uˆ1= uˆE2oH
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∇.S + ∂tU= −J.E∂Ur r v r r
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2.2 Indeks bias dengan model elektr
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Tuliskan: n=n’-in”Tinjau gelomb
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2.4 Pulsa optik dan kecepatan grupD
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Dispersi materialBilangan gelombang
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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: ⎛⎜⎝ACB ⎞⎛a⎟⎜D ⎠⎝b
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*
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7.3.2 Perturbasi dielektrik secara
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Tanda dari faktor β1 / β1dan β2/
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zn sn an sn bn sJika kedua pandugel
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1290)()(22*)(222*22=Δ+Δ+∂∂−
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A(z)=( C1sinsz+ C2cos sz)( / 2 ) ze
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8. OPTIK NONLINIER8.1 Pengertian No
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n≅no+χ(2)E(z,ω)2noBahan nonlini
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Modulatorφ iLdφ oVφo= φ +i= φ
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Fungsi Logika XORaPolarisasi cahaya
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141Penguat Optik),(),(),(2(2)(1)ω
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SwitchingFebry-PerotI oI oI iI iBah
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