logging in or signing up almy ieee Sigfrid Download Post to : URL : Related Presentations : Share Add to Flag Embed Email Send to Blogs and Networks Add to Channel Uploaded from authorPOINTLite Insert YouTube videos in PowerPont slides with aS Desktop Copy embed code: (To copy code, click on the text box) Embed: URL: Thumbnail: WordPress Embed Customize Embed The presentation is successfully added In Your Favorites. Views: 131 Category: Education License: All Rights Reserved Like it (0) Dislike it (0) Added: January 11, 2008 This Presentation is Public Favorites: 0 Presentation Description No description available. Comments Posting comment... Premium member Presentation Transcript Novel Semi-Transparent Optical Position Sensors for high-precision alignment monitoring applications: Novel Semi-Transparent Optical Position Sensors for high-precision alignment monitoring applications Sandra Horvat, F.Bauer, V.Danielyan, H.Kroha Max-Planck-Institute for Physics, Munich,Germany 13.06.2002. Orlando, FloridaSlide2: Introduction ATLAS detector @CERN End-Cap Octant Sandra Horvat 1/13 MPI for Physics,Munich ALMY System: high-precision alignment monitoring designed for high energy physics experiments laser beam along the alignment line ALMY sensors measure its position Requirements: high position resolution high transmittance insensitivity to high magnetic fields long term illumination radiation hardness 23 mSlide3: ALMY Optical Monitoring System Sandra Horvat 2/13 MPI for Physics,Munich Multi-point measurement of the laser beam position : collimated laser beams (690 nm and 780 nm) single mode fibers (SMF), gaussian beam profile semi-transparent silicon sensors for 2D position measurement, from the induced photo current distributionSlide4: ALMY Optical Position Sensors Transparent active surface: chemical vapour deposition of a-Si:H layer (0.3-1.0 mm) from the plasma phase 2 layers of ITO electrodes (50-100 nm) glass substrate (0.5-1.0 mm) anti-reflective coating Custom designed readout electronics: analog signal multiplexed, amplified (I-V converter), digitized, transmitted to PC for online analysis readout speed: 10 ms up to 30 sensors serially to PC port only commercial components laser controler 64x64 diodes, 312.5 mm pitch, 20x20 mm2 6 cm 6 cm Sandra Horvat 3/13 MPI for Physics,Munich Slide5: Setup for the Sensor Tests Scan of the sensor surface with a laser beam, using stepping motors of 1 mm positioning accuracy position resolution photo current response laser beam deflection transmittance long term illumination ~200 sensors Sandra Horvat 4/13 MPI for Physics,Munich Slide6: Transmittance transmittance @780 nm: 80-90% transmittance @690 nm: 70-75% Minimized reflectivity: optimized thicknesses of a-Si:H and ITO layers anti-reflective coating on the back side of the glass up to 10 sensors along the 780 nm beam Sandra Horvat 5/13 MPI for Physics,Munich Slide7: Photo Current Response Finite wedge angle of the glass substrate can cause the interference patterns, due to the reflected light. Efficiently suppresed! anti-reflective coating laser diodes with short coherence length uniform distribution over the whole surface laser beam profile remains undistorted Sensitivity: 0.1 A/W @690 nm 0.01 A/W @780 nm Saturation (strip current 1mA): 1 mW/cm2 @690 nm 10 mW/cm2 @780 nm Sandra Horvat 6/13 MPI for Physics,Munich Slide8: Position Resolution 5.012 mm 5.746 mm Typical production batch: S/N>1000 local resolution: 1 mm overall resolution: 5 mm uniform distribution Sandra Horvat 7/13 MPI for Physics,Munich Slide9: Laser Beam Deflection specially polished glass wafers parallel surfaces remain undeformed during the antireflecive coating deflection <5mrad Glass quality is unchanged during sensor production for T of up to 2000. uniform distribution, deflection angle < 5mrad Glass wafers: Sensors: Sandra Horvat 8/13 MPI for Physics,Munich Slide10: Long Term Illumination (Staebler-Wronski effect) Photo current response after 1500 h of illumination with 690 nm @ 1mW/cm2 photo current response in a-Si:H deteriorates under illumination degradation in position resolution local sensitivity minimum increases with time dependance on the wavelenghth and the beam intensity Sandra Horvat 9/13 MPI for Physics,Munich Slide11: Long Term Illumination 690 nm @ 1 mW/cm2 780 nm @ 10 mW/cm2 780 nm @ 10 mW/cm2 equivalent effect 1% 1.5-2.5% 3.5% Laser Beam, below saturation Laser Beam & daylight degradation at a constant rate depends on the absorbed light, rather than illumination intensity 500 h correspond to a tolerable position measurement error of 5 mm non-additive effect under an additional daylight illumination Sandra Horvat 10/13 MPI for Physics,Munich Slide12: Radiation Hardness: 1014 neutrons/cm2,1 MeV eq. bias voltage: 1V I-V characteristics dark current Naked silicon cells: before and after irradiation (no degradation) Sandra Horvat 11/13 MPI for Physics,Munich Slide13: Radiation Hardness: 1013 neutrons/cm2 Change in the transmittance: <1% Sensor module with electronics: Change in the photo current: <2% No degradation! Additionally: No degradation after g-irradiation (10 MRad). Sandra Horvat 12/13 MPI for Physics,Munich Slide14: Summary ALMY sensors: transparent a-Si:H position sensors application in optical alignment monitoring systems Sensor performance : dynamic range 20x20 mm2 position resolution 5 mm high quality parallel glass substrate transmittance 80-90% @780 nm uniformity over the whole active surface radiation hard (1013 n/cm2, 10 g MRad) insensitive to high magnetic fields (Hall mobility <10-2 cm/Vs) negligible degradation under illumination with laser beam intensities below saturation (10 mW/cm2 @780 nm) optimized and verified in extensive tests larger-scale production under preparation Sandra Horvat 13/13 MPI for Physics,Munich You do not have the permission to view this presentation. In order to view it, please contact the author of the presentation.
almy ieee Sigfrid Download Post to : URL : Related Presentations : Share Add to Flag Embed Email Send to Blogs and Networks Add to Channel Uploaded from authorPOINTLite Insert YouTube videos in PowerPont slides with aS Desktop Copy embed code: (To copy code, click on the text box) Embed: URL: Thumbnail: WordPress Embed Customize Embed The presentation is successfully added In Your Favorites. Views: 131 Category: Education License: All Rights Reserved Like it (0) Dislike it (0) Added: January 11, 2008 This Presentation is Public Favorites: 0 Presentation Description No description available. Comments Posting comment... Premium member Presentation Transcript Novel Semi-Transparent Optical Position Sensors for high-precision alignment monitoring applications: Novel Semi-Transparent Optical Position Sensors for high-precision alignment monitoring applications Sandra Horvat, F.Bauer, V.Danielyan, H.Kroha Max-Planck-Institute for Physics, Munich,Germany 13.06.2002. Orlando, FloridaSlide2: Introduction ATLAS detector @CERN End-Cap Octant Sandra Horvat 1/13 MPI for Physics,Munich ALMY System: high-precision alignment monitoring designed for high energy physics experiments laser beam along the alignment line ALMY sensors measure its position Requirements: high position resolution high transmittance insensitivity to high magnetic fields long term illumination radiation hardness 23 mSlide3: ALMY Optical Monitoring System Sandra Horvat 2/13 MPI for Physics,Munich Multi-point measurement of the laser beam position : collimated laser beams (690 nm and 780 nm) single mode fibers (SMF), gaussian beam profile semi-transparent silicon sensors for 2D position measurement, from the induced photo current distributionSlide4: ALMY Optical Position Sensors Transparent active surface: chemical vapour deposition of a-Si:H layer (0.3-1.0 mm) from the plasma phase 2 layers of ITO electrodes (50-100 nm) glass substrate (0.5-1.0 mm) anti-reflective coating Custom designed readout electronics: analog signal multiplexed, amplified (I-V converter), digitized, transmitted to PC for online analysis readout speed: 10 ms up to 30 sensors serially to PC port only commercial components laser controler 64x64 diodes, 312.5 mm pitch, 20x20 mm2 6 cm 6 cm Sandra Horvat 3/13 MPI for Physics,Munich Slide5: Setup for the Sensor Tests Scan of the sensor surface with a laser beam, using stepping motors of 1 mm positioning accuracy position resolution photo current response laser beam deflection transmittance long term illumination ~200 sensors Sandra Horvat 4/13 MPI for Physics,Munich Slide6: Transmittance transmittance @780 nm: 80-90% transmittance @690 nm: 70-75% Minimized reflectivity: optimized thicknesses of a-Si:H and ITO layers anti-reflective coating on the back side of the glass up to 10 sensors along the 780 nm beam Sandra Horvat 5/13 MPI for Physics,Munich Slide7: Photo Current Response Finite wedge angle of the glass substrate can cause the interference patterns, due to the reflected light. Efficiently suppresed! anti-reflective coating laser diodes with short coherence length uniform distribution over the whole surface laser beam profile remains undistorted Sensitivity: 0.1 A/W @690 nm 0.01 A/W @780 nm Saturation (strip current 1mA): 1 mW/cm2 @690 nm 10 mW/cm2 @780 nm Sandra Horvat 6/13 MPI for Physics,Munich Slide8: Position Resolution 5.012 mm 5.746 mm Typical production batch: S/N>1000 local resolution: 1 mm overall resolution: 5 mm uniform distribution Sandra Horvat 7/13 MPI for Physics,Munich Slide9: Laser Beam Deflection specially polished glass wafers parallel surfaces remain undeformed during the antireflecive coating deflection <5mrad Glass quality is unchanged during sensor production for T of up to 2000. uniform distribution, deflection angle < 5mrad Glass wafers: Sensors: Sandra Horvat 8/13 MPI for Physics,Munich Slide10: Long Term Illumination (Staebler-Wronski effect) Photo current response after 1500 h of illumination with 690 nm @ 1mW/cm2 photo current response in a-Si:H deteriorates under illumination degradation in position resolution local sensitivity minimum increases with time dependance on the wavelenghth and the beam intensity Sandra Horvat 9/13 MPI for Physics,Munich Slide11: Long Term Illumination 690 nm @ 1 mW/cm2 780 nm @ 10 mW/cm2 780 nm @ 10 mW/cm2 equivalent effect 1% 1.5-2.5% 3.5% Laser Beam, below saturation Laser Beam & daylight degradation at a constant rate depends on the absorbed light, rather than illumination intensity 500 h correspond to a tolerable position measurement error of 5 mm non-additive effect under an additional daylight illumination Sandra Horvat 10/13 MPI for Physics,Munich Slide12: Radiation Hardness: 1014 neutrons/cm2,1 MeV eq. bias voltage: 1V I-V characteristics dark current Naked silicon cells: before and after irradiation (no degradation) Sandra Horvat 11/13 MPI for Physics,Munich Slide13: Radiation Hardness: 1013 neutrons/cm2 Change in the transmittance: <1% Sensor module with electronics: Change in the photo current: <2% No degradation! Additionally: No degradation after g-irradiation (10 MRad). Sandra Horvat 12/13 MPI for Physics,Munich Slide14: Summary ALMY sensors: transparent a-Si:H position sensors application in optical alignment monitoring systems Sensor performance : dynamic range 20x20 mm2 position resolution 5 mm high quality parallel glass substrate transmittance 80-90% @780 nm uniformity over the whole active surface radiation hard (1013 n/cm2, 10 g MRad) insensitive to high magnetic fields (Hall mobility <10-2 cm/Vs) negligible degradation under illumination with laser beam intensities below saturation (10 mW/cm2 @780 nm) optimized and verified in extensive tests larger-scale production under preparation Sandra Horvat 13/13 MPI for Physics,Munich