Transcript Document

Polarization-Independent Modulation
& Simplified Spectropolarimetry
Using LC Polarization Gratings
1
Escuti ,
1
Jones ,
1
Oh ,
1
Komanduri ,
2
Sanchez , C.
3
Bastiaansen ,
3
Broer
Michael J.
W.M.
C.
R.
C.
D.J.
contact: [email protected], 1) NC State Univ, 2) Univ de Zaragoza, 3) Eindhoven Univ of Technology
Opto-Electronics and Lightwave Engineering Group (OLEG)
Electrical & Computer Engineering
Basic Operation (monochromatic light)
Summary & Motivation
 OBJECTIVE: NEW LIQUID CRYSTAL DEVICE MODES
 Diffractive Modulator
• POLARIZATION INDEPENDENT liquid crystal microdisplays
• HYPERSPECTRAL POLARIMETER designs enabling high-speed detection
 MOTIVATION: Capitalize on Adv Polarization Control Techniques
• Achieve ultra-efficient, portable, projection displays, with low-cost potential LCoS
• Simplified spectropolarimeter for easier wavelength-parallel polarization detection
 APPROACH: Surface-directed Holograms in Bulk Liquid Crystals
• These optical elements are technically “Liquid Crystal Polarization Gratings” or (LCPG)
• First reported by Crawford and coworkers (Eakin et al, Appl Phys Lett 85, 2004)
• We improve on prior work by achieving high quality optical elements for 1st time
• Directs optical power between
0th and ±1st diffraction orders
(Floquet modes)
• Polarization independent!
• Controlled by applied voltage
Zero V, Linear Polzn
• Threshold voltage = ~1.65 V
(2 m thickness)
• Modest operating voltages
• Very low scattering (< 0.3%)
• High contrast for
monochromatic light
Full (30) V, All Polarizations
LCPG Properties
n(x)  sin(x /) cos(x /) 0
 Construction & Properties
Top View
• Hologram w/ continuous in-plane profile
• Splay-bend nematic LC texture 
• Bulk liquid crystals
• Photo-alignment layers capture pattern
• Diffraction Efficiency
 Transmittance vs Voltage
 Switching Times
I+1+ I–1
Iincident
Side View (0V)
nd 
m 0  cos 

  
2
nd 
m 1  sin 

  
2

(V>Vth)
(633 nm laser light)
• Voltage Threshold:
K  d 2 
1 2 
Vth     
 dC 
0
• Switching Times:

 on 
Modulation of Unpolarized LED Light (first results)
1d 2
0V V
2
2
th

 off
 Bright-Field Schlieren (BFS) Projection System
1d 2

0Vth2 
Maximum Contrast Ratios
 Transmittance Spectra

Color
Contrast
Red
144:1
Green
73:1
Blue
82:1
* Potentially as high as 600:1
given higher voltages & dark-field
Experiment Specifications
• Magnification = 15X, Throw = 0.6m
 Fabrication
• Used
standard
MERCK liquid crystals
and ROLIC photoalignment materials
=11μm
d=2μm
n=0.2
Similar to method in
Eakin et al, Appl Phys Lett 85 (2004)
Step 2: Hologram Exposure
+ careful optimization of
material choices and
critical thickness design
Step 3: Fill w/ LC
Wavelength-Parallel Spectropolarimeter
Reactive-Mesogen Polarization Gratings
PG#1
I1PG#1( ) I 1
( )
S0( ) 
sin 2 1

Features
• High efficiency (~100%), low scattering (< 0.3%)
• Single substrate, robust polymer films
• Grating periods as small as 1 m
• Rolic Photo-alignment, Merck reactive mesogens

Features
• Full spectral polarization information w/o active tuning elements
• Simultaneous measurement of six intensities only needed 
• Simple light-weight construction
• Proof-of-concept shows very good accuracy!
PG#1
I 1
( ) I1PG#1( )
S1( ) 
cos2 3 cos2 2 sin 2 1
PG#2
I1PG#2( ) I 1
( )
S2( ) 
cos2 3 sin 2 2
PG#3
I 1
( ) I1PG#3( )
S3( ) 
sin 2 3

For More Information: [email protected]
@ SID Symposium Digest 2006: paper # 39.4, posters P-209, P-167
@ SPIE Optics & Photonics (San Jose, CA, 2006): three entries
Manuscripts in preparation/submission (2006): Nat. Photonics, etc.