liquid crystal slms
DESCRIPTION
Liqiud Crystal Spatial Light ModulatorsTRANSCRIPT
Liquid crystal
Spatial Light Modulators
(LCSLMs)
Ajay Singh
Engineering Physics Department Indian Institute of Technology Delhi
What is SLM
Device that “spatially modulates” a coherent beam of light Briefly , a liquid crystal device that acts as a variable Usually, an SLM modulates the intensity of the light beam However, it is also possible to produce devices that
modulate the phase of the beam or both the intensity and the phase simultaneously
Addressed Electrically or Optically
Ajay Singh , Department of Physics IIT Delhi
http://rumalis.com/40875-liquid-crystal-display
http://imgarcade.com/1/computer-screen-clipart/
3
Spatial Light Modulators
Electrically addressed
spatial light modulator Photo-addressed spatial light modulator
x
y
Incident
light
Modulated
light
Transmittance T(x,y)
+
+
+
-
-
Electro-optic
material
x
y
Write iamge
IW(x,y)
Incident
light
Modulated
light
Transparent
electrodes
Mirror
Photoconductive
material
Ajay Singh , Department of Physics IIT Delhi
Electrically addressed spatial light modulator (EASLM)
Ajay Singh , Department of Physics IIT Delhi
Electrical signals to coherent (or incoherent) modulation. Fundamental optical “input device” so link between imaging optics
and electronics. Transmissive LC panels: Liquid crystal between two glass sheets,
with control circuitry added with thin film transistors.
Electrically addressed spatial light modulator (EASLM)
Ajay Singh , Department of Physics IIT Delhi
Electrical signals to coherent (or incoherent) modulation. Fundamental optical “input device” so link between imaging optics
and electronics. Transmissive LC panels: Liquid crystal between two glass sheets,
with control circuitry added with thin film transistors.
Liquid Crystal: LC modulators switched by either thin-film transistors (transmissive
displays), or silicon backplanes (reflective devices). Usable in all applications, but
rather “slow”.
Magneto-Optic: Pixelated crystal of Aluminum Garnet switched by array of magnetic
coils using magneto-optic effect. High powered drive circuits, and low efficiency, but are
commercially available.
Deformable Mirror: Array of “sprung” mirrorsmake by nano-technology techniques.
Very expensive to make, rather slow, and not flat. (Excellent for incoherent light).
Multiple Quantum Well: non-linear optical effect, Quantum Stark Effect in stack of
very thin layer ( 100rA). Extremely fast (quantum limited), but poor contrast, difficult to
make in large arrays, and difficult to drive. Future of fast optical switching.
Common Modulation Techniques:
Electrically addressed spatial light modulator (EASLM)
Ajay Singh , Department of Physics IIT Delhi
Address the “pixels” to change the local electric field across the liquid layer and hence switch pixels on or off. Add “grey-level” by altering the time each pixel is on for and colour by placing an array of colour filters on top of the display to group pixels in threes.
Typical displays are very large (up to 30 cm) for laptop computers, but also small displays for projection TVs and head-up displays.Best “optics” device is 320320 pixels, in 44 cm display.
Electrically addressed spatial light modulator (EASLM)
Ajay Singh , Department of Physics IIT Delhi
Excellent for image display and projection system This technology is set to take over from CRT monitors for
computer displays and televisions, (replacement for 17” colour monitor available).
Big commercial growth area, Many commercial system from Thorn-EMI, Philips, Sony, Casio, Sharp.
Problems: Large pixels (TFT are always big) Small “fill-factor” (large dead areas due to TFTs) Not very flat, problem in coherent optics.
Cost still rather high, mainly due to yield problems. All ESLMs are pixelated. Leads to some diffraction problems
when used in coherent optical systems.
one light beam (the optical control beam) is used to change a variableassociated with another light beam (the incident beam); the optical control beamis often called the “write beam” and the incident beam is the “read beam”A photosensor allows the OASLM to sense the brightness of each pixel andreplicate the image using liquid crystals.
As long as the OASLM is powered, the image is retained even after the light isextinguished. An electrical signal is used to clear the whole OASLM at once
Ajay Singh , Department of Physics IIT Delhi
Optically addressed spatial light modulator (OASLM)
The “incoherent” light is detected (asintensity), by a photo-detector (as anelectrical change distribution).This charge distribution affects themodulator, and so changes the Amplitude orPhase of the reflected coherent light.Most common (and only commerciallyavailable) are:Photo-conductor: Amorphous Silicon, (lowlight levels) or thin filmPhoto-transistor (high light levels).Modulator: Liquid Crystal.
Chang-Kui Duan, Institute of Modern Physics, CUPT
LC Spatial Light Modulator
Ajay Singh , Department of Physics IIT Delhi
Crystal is also bi-refringent, so ifilluminated with polarsied light it canbe used to rotate axis ofpolarisation, and hence changeAmplitude (with analyser)
A typical opticallyaddressed liquid crystalspatial light modulator(OALCSLM) operating inthe reflective mode
Photo-conductor: AmorphousSilicon, (low light levels) or thin filmPhoto-transistor (high light levels).Modulator: Liquid Crystal.
Ajay Singh , Department of Physics IIT Delhi
Operation of SLM
No applied voltage the molecules are “aligned” by the surface groves (Alignment layers)
Ajay Singh , Department of Physics IIT Delhi
Operation of SLM
No applied voltage the molecules are “aligned” by the surface groves (Alignment layers)
SquareWave applied, “induced” dipole on molecule that is then “twisted”by the electric field
Ajay Singh , Department of Physics IIT Delhi
Operation of SLM
No applied voltage the molecules are “aligned” by the surface groves (Alignment layers)
SquareWave applied, “induced” dipole on molecule that is then “twisted”by the electric field
Square Wave plus light: photo-conductor is locally discharged by thelight, so molecules in these regions not effected by electric field, sodo not twist round
Ajay Singh , Department of Physics IIT Delhi
Problems:• Variable contrast and sensitivity across device.• Relatively insensitive to light.• Tends to retain image.• Liquid crystal degrades• Very low yield during manufacture
Practical Uses of AOSLMs
very-high-resolution display such as one for a computer-generated holographic display 3D holographic display Real-time input to Optical Correlator Joint Transform Correlator
Ajay Singh , Department of Physics IIT Delhi
References:
Coomber, Stuart D.; Cameron, Colin D.; Hughes, Jonathon R.; Sheerin, David T.;Slinger, Christopher W.; Smith, Mark A.; Stanley, Maurice (QinetiQ), "Opticallyaddressed spatial light modulators for replaying computer-generatedholograms", Proc. SPIE Vol. '4457', p. 9-19 (2001)
Slinger, C.; Cameron, C.; Stanley, M.; "Computer-Generated Holography as aGeneric Display Technology", IEEE Computer, Volume 38, Issue 8, Aug. 2005, pp46–53
A.M. Weiner. "Femtosecond pulse shaping using spatial light modulators". REVIEWOF SCIENTIFIC INSTRUMENTS VOLUME 71, NUMBER 5 MAY 2000. Retrieved 2010-07-06.
http://ieeexplore.ieee.org/xpls/abs_all.jsp?arnumber=5069618&tag=1http://www2.ph.ed.ac.uk/~wjh/teaching/mo/slides/slms/slm.pdfhttp://en.wikipedia.org/wiki/Spatial_light_modulatorhttp://laser.physics.sunysb.edu/~melia/SLM_intro.html#4
Ajay Singh , Department of Physics IIT Delhi
Ajay Singh , Department of Physics IIT Delhi
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