Title: OSEM Sensor Development
1 OSEM Sensor Development University of
Birmingham David Hoyland Senior Electronics
Design Engineer Astrophysics and Space Research
Group
2- Overview
- Currently Investigating two possible solutions
- - Opto-electronic (Shadow) Detectors
- - Review of evolution of BIPM design
- - Developing current BIPM design.
- - Sub-miniature Interferometer Approach
- - Development of NPL quadrature interferometer.
- - Feasibility of integration into OSEM envelope
-
3Opto-Electronic Detectors - BIPM Designs
- Scheme A (George Gillies circa 1980)
- LED Source.
- Opaque Object, either spherical or cylindrical
- Low sensitivity to rotation
- Some optical power obscured and scattered by the
object.
4Opto-Electronic Detectors - BIPM Designs
- Scheme B, C (Developed from Scheme A by Clive
Speake (B), Alain Picard(C)) - LED Source (B), Laser Diode Source (C).
- Multimode Fibre Feed (B), Monomode Fibre Feed
(C). - Lens 2 fixed to the moving object.
- Photodiode dimensions chosen to accommodate
Laser beam profile
5Opto-Electronic Detectors - Development
- Development of the BIPM Scheme C is being
undertaken at UoB to assess feasibility for LIGO - We predicted a maximum sensitivity of 1?10-11
mHz1/2 should be achievable. - Sensitivity fundamentally constrained by
photodiode characteristics or coupled laser
power, and dynamic range. - Further development to resolve the following
issues - Laser diode speckle (spatial stability), and
beam format - Optimum laser power
- Source pointing stability
- This will enable us to find the best optical
configuration, as well as - Identify the optimal source choice e.g. LED,
SLD, VCSEL, Pig-tailed SLD etc. - Define custom photodiode fabrication options.
6Sub miniature Interferometer Approach
7Design Approach
- Development of this Interferometer is being
undertaken at UoB to assess feasibility for LIGO - Outputs 1 and 2 from PBS2 provide two quadrature
fringe signals. - A DSP is utilised to count the fringes and fit
ellipse parameters in real time. - - Development is taking place in collaboration
with colleagues at UCSD - - 100KHz sampling limits max velocity of
proof-mass to 15 mms-1. - - Dynamic range limited only by numeric range of
the processor. - - Also able to track ellipse parameter changes
over a pre-defined timescale. - - A sensitivity of 5?10-13 mHz1/2 has been
demonstrated which is effectively independent of
dynamic range and laser power - - Output position data is in digital domain
(floating point?) IMPLICATIONS?? - Further design and testing should help to resolve
the following issues - - Source coherence length
- - Optimisation of optical design via Gaussian
beam propagation analysis
8Interferometer Image
9Schedule / Plan
Development of the Opto-electronic
(non-interferometric) position sensor - Design
and testing July 2003 October 2003 Development
of the interferometric position sensor - Design
and testing October 2003 December
2003 Consider trade-offs between identified
viable methods, December 2003 - Cost /
Performance - Interface to LIGO system -
Manufacturability