Diffractive Components for Gravitational Wave Detectors Stefanie Kroker Institute of Applied Physics Friedrich Schiller University Jena 02.03.2010 S. Kroker Mirror Cavity Couplers 02.03.2010 S. Kroker Outline Introduction 2-Port Cavity Couplers 3-Port Cavity Couplers Conclusion 02.03.2010 S. Kroker Grating Equation -1 R ni sin n j sin m / d 0R Incident Ray 1R d… period ni… refractive index medium of incidence nj… refractive index propagation medium of diffracted light … angle of incidence … diffraction angle … wavelength m=0,±1, ±2,… 1T 02.03.2010 -1 T 0 T Born, Wolf: Principles of Optics S. Kroker Littrow Configuration -1R Second Order Littrow Configuration -2R 0R Incident Ray 0R Incident Ray sin / d sin / 2d 2-Port Cavity Coupler 02.03.2010 -1R 3-Port Cavity Coupler S. Kroker Cavity Incident Ray -1R 0R Incident Ray Mirror 02.03.2010 Cavity -2R Mirror S. Kroker -1R 0R Mirrors Resonant Waveguide Grating HR-Stack 02.03.2010 S. Kroker 2-Port Cavity Coupler Incident Ray -1R Highly efficient reflection grating in Littrow mount. 0R Cavity Desirable Properties: R-1≈97% R0 ≈3% Mirror T as low as possible! highly efficient 02.03.2010 S. Kroker Resonant Waveguide Grating as Mirror Low Index Material High Index Material nL nH Resonant Waveguide Grating Normal incidence: / nH d / nL Period upper grating 2 Period waveguide grating 02.03.2010 S. Kroker Optimized for diffraction angle! Typical Properties Calculations: R ≥ 97% T ≈0.05% At least achievable 02.03.2010 S. Kroker 3-Port Cavity Coupler Cavity 2nd order Littrow mount: Incident Ray -2R -1R 0R sin / d Desireable properties: R0≈95% R-1≈5% R-2, T as low as possible Mirror 02.03.2010 S. Kroker Resonant Waveguide Grating as Mirror Low Index Material High Index Material nL nH Waveguide Grating: / nH d / nL =1550 nm : d~600…700 nm Period upper grating 3 Period waveguide grating 02.03.2010 S. Kroker Upper Grating 3 Ports: d≥ At least 3 diffraction orders in grating material! Problem: Waveguide grating needs to be highly efficient @ q0, ±q1 02.03.2010 S. Kroker Angular Tolerance of Silicon-Grating on SiO2 1,0 =1550 nm 0,9 Reflectivity 0,8 Waveguide Grating 0,7 dWG= 633 nm 0,6 0,5 Upper Grating 0,4 d3P=1899 nm 0,3 0,2 0 5 10 15 20 25 30 35 40 Angle of Incidence [°] Diffraction Angle for m=±1 in SiO2 Need to increase angular tolerance! q1 ≈±34° 02.03.2010 S. Kroker Idea: Stack of Resonant Waveguide Gratings Reflectivity Stack RWG1RWG2 RWG 2 RWG 1 Angle of Incidence 02.03.2010 S. Kroker TM-Polarization H ll Grating Grooves Silicon Silica 02.03.2010 S. Kroker 1,0 0,9 0,8 Reflectivity 0,7 0,6 0,5 0,4 0,3 0,2 Lower Grating Upper Grating Stack 0,1 0,0 0 10 20 30 40 50 60 Angle of Incidence [°] 02.03.2010 S. Kroker 70 80 90 TE-Polarization E ll Grating Grooves Silicon Silica 02.03.2010 S. Kroker 1,0 3-Port Grating: R0≈94.3% 0,8 Reflectivity R-1 ≈5.3% R-2 ≈0.3% 0,6 T ≈0.016% 0,4 Lower Grating Upper Grating Stack 0,2 0,0 0 10 20 30 40 50 60 Angle of Incidence [°] 02.03.2010 S. Kroker 70 80 90 Conclusion - new concept for grating couplers: HR-Stacks replaced by resonant waveguide gratings - 2-port couplers: RWG optimized for diffraction angle of upper grating - 3-port couplers: angular tolerance of single RWG not sufficient to provide low transmission, stack of two or more RWGs can be used (can also be used to decrease transmission of 2-port couplers) -technical implementation under investigation (T-shape considered) 02.03.2010 S. Kroker Thank you very much for your attention! 02.03.2010 S. Kroker
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