Advances in Lasers and Electro Optics 2 pdf

... φφφ φφφ φφ φ 2sin 2 3 cossin)( cos)sin3cos()( cossin)( cos)( )( 2 18 4 22 4 11effeff 2 10 2 25effeff 2 24 2 16effeff 23 effeff 33effeff ccccc cccc cccc ccc ccc eeeeffff oeeesfff ooeessff oooesssf oooossss ++== +== +== == == (8-1) in the xy plane, 11effeff effeff 10 2 18 2 16effeff effeff 2 25 2 23 2 24 4 33 4 22 effeff )( 0)( 2sincossin)( 0)( 2sin)cossin (2 2s...

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... Advances in Lasers and Electro Optics 120 32 3 22 2 2 23 23 4 = [2( )], iq p Ai e expi kip τ δδ δ τ δδ δδ −− Δ− − * 23 2 33 33 23 23 4 = [2( )], iq p Ai eexpi kip τ δδ ... Advances in Lasers and Electro Optics 128 Fig. 6. Output pulse train ( 32) amplitude (blue line) and its time–average value (red line) for: a) C = 2. 5 2 ,P = 1...

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... such as GaInAs/AlInAs, GaAs/AlGaAs, and InAs/AlSb, 27 1 The Intersubband Approach to Si-based Lasers Advances in Lasers and Electro Optics 25 8 Fig. 2. Illustration of (a) conduction and valence ... on the other hand, can have larger conduction 28 2 Advances in Lasers and Electro Optics The Intersubband Approach to Si-based Lasers 28 3 band offset, but...

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... and multicasting using injection-locked laser diodes. J. Lightwave Technol., Vol. 22 , No. 11, (20 04) pp. 23 86 -23 92, Nov., 20 04 Chow, K. K.; Shu, C.; Mak, M. W. K. & Tsang, H. K. (20 02) . ... causing overshoot, high ΔQ values were also obtained. As seen in the eye diagrams presented in the Advances in Lasers and Electro optics 420 obtained due to the h...

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... resulting in a dark count rate of 24 00 Advances in Lasers and Electro Optics 29 0 exploited nonlinearity are investigated, confirming the high potentialities of an asynchronous sampling technique. ... polarizer and avoiding the additional insertion loss that a polarizer would add. Advances in Lasers and Electro Optics 29 2 In order to avoid high-...

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... of Quantum Electronics, vol. 25 , No.11, pp 22 97 -23 06, ISSN 0018-9197. Advances in Lasers and Electro Optics 378 conventional FWM in SOA drops rapidly with wavelength detuning and it is ... S i2 are shown by STO3 and STO0 in Fig. 25 (b). Fig. 25 . STO0~STO3: signal spectra measured at S i1 or S i2 in Fig. 23 when two-input minterms ( 22 03 ~mm)...

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... [] ( [] ) [] ( [] ) () ( ) ⎟ ⎠ ⎞ ++++++ +++++− ++++ ++++ ++++ ⎜ ⎝ ⎛ +++ + +=Δ ⊥ ⊥ ⊥ ⊥ ⊥ ⊥ ⊥ ⊥ ,, ,, ||,, , ||,, , , , ||, ||, ,,||,,,,,, ,, ||,, ,,,, ,||,, , , ||, , , ),( )arctan()( t d t t d d t d t t dd iiii r r rr iii i r r r r QI e nnnnnnsnnnsn B R nnnnnnsnnnsn B R nnnnsnsnc nnnnsnsnc R nnnnsnsnc nnnnsnsnc R k k kt τ τ τ τ τ τ ττττ τ τ ττ γγγ γγγ γ γφ 22 2 2 222 1 21 1 21 2 2...

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... 22 2 2 22 01 ||| |[( ) 2( ) cos sin 22 B B LW RF RF R A JA JA φφ + 01 4( )( )sin cos sin2 22 BB R FRF m J AJA ft φφ π − 2 02 2 (2 ( ) ( ) cos 2 B RF RF JA JA φ + 2 2 1 () )cos (22 )] sin 2 B RF ... obtained. 22 2 || 11| | =cos | |2 2 RF B LW RA A φ − + sin sin 2 R FB m A ft φπ − 2 1 ||coscos (22 ) 2 RF B m A ft φπ +× (9) The intensities of the fundame...

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... − R 2 ) = k Ω R 12 and β = . Interference term is given by cos[ν( τ 1 − )+ω( τ 2 − )] = cosξ d, where ξ = The G (2) (x 1 ,x 2 ) is given then by Advances in Lasers and Electro Optics ... changes between (|E 1 |−|E 2 |) 2 and (|E 1 |+|E 2 |) 2 . Introducing G = 2| Ω 0 | 2 T 1 T 2 , we can write ( 12) Then, for the drive field at the posit...

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... backward control field − Ω . Using the dispersion relation ()k ω in Eq. (5), we obtain the group velocity for the interacting fields A + and A − : 22 22 222 2 20 [( )/ ] k [ ]/[ ( ) ] k vNgcggNgg γγ ... (A−7), and the integral of d has been taken to infinity. Substituting this result into Eq. (A−8) we obtain Advances in Lasers and Electro Optics 598...

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