Advances in Optical and Photonic Devices 2011 Part 2 pptx

Advances in Optical and Photonic Devices 2011 Part 2 pptx

Advances in Optical and Photonic Devices 2011 Part 2 pptx

... 18um, I=15uA PQR emission LED emission 25 A/cm 2 50A/cm 2 100A/cm 2 25A/cm 2 50A/cm 2 100A/cm 2 12- petals, I th =28 uA 11A/cm 2 T=100% 25 A/cm 2 50A/cm 2 100A/cm 2 T=1.0% T=1.0% T=1.0% T=1.0% T=1.0% ... (January 20 09) 30- 32 Advances in Optical and Photonic Devices 20 Van der Poel, M.; Mork, J.; Somers, A.; Forchel, A.; Reithmaier, J. P. & Eis...

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Advances in Optical and Photonic Devices 2011 Part 11 pptx

Advances in Optical and Photonic Devices 2011 Part 11 pptx

... H. (20 09a). All-band photonic transport system and its device technologies. Proceedings of SPIE, Vol. 723 5 (20 09) 723 50C Advances in Optical and Photonic Devices 26 0 with particular energy. ... (filling factor) Quantum Dot Photonic Devices and Their Material Fabrications 24 5 existing photonic devices, and enhancement of usable optical frequency r...

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Advances in Optical and Photonic Devices 2011 Part 6 docx

Advances in Optical and Photonic Devices 2011 Part 6 docx

... [27 , 28 ]. Advances in Optical and Photonic Devices 122 an InP substrate. The theory of the nonreciprocal loss phenomenon was first proposed by Takenaka, Zaets, and others in 1999 [29 , ... obtain the recurrence equation 1, 1, , 1 , 1 , 22 22 22 1111 22 ()0 p q p q pq pq pq HHHH H mmnn mn φ −+ −+ + +++−−= (3-10) for eq. (3-8), and recurrence equation 1...

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Advances in Optical and Photonic Devices 2011 Part 7 docx

Advances in Optical and Photonic Devices 2011 Part 7 docx

... n 1 Λ h + n 1 Λ h = n 1 n Λ h +n Λ h =n 2 2 2 2 1 1 2 e 2 2 2 2 1 1 2 0 (1) Advances in Optical and Photonic Devices 150 5. Experimental performances In the first reports of form-birefringent frequency conversion, scattering ... fluctuations effective input and parametric gain coefficient are maximum. The latter can be written as ( ) cελλnnn/PΓπ8g 0sisi...

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