liquid crystal institute john west kent state university april 22, 2004

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Liquid Crystal Institute John West Kent State University April 22, 2004

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Page 1: Liquid Crystal Institute John West Kent State University April 22, 2004

Liquid Crystal Institute

John WestKent State University

April 22, 2004

Page 2: Liquid Crystal Institute John West Kent State University April 22, 2004

Liquid Crystal Institute

• Why Flexible

• Printed Flexible Cholesteric Displays– Printing techniques– Polymer walls

• Stressed Liquid Crystals

• Flexible Optical and Electronic Device Manufacturing Facility

Page 3: Liquid Crystal Institute John West Kent State University April 22, 2004

Liquid Crystal Institute

Anatoliy Glushenko

Guoqiang(Matt) Zhang

Ke Zhang

Ebru Aylin BuyuktanirToshihio Aoki

Greg R. Novotny

David Heineman

Mike Fisch

Page 4: Liquid Crystal Institute John West Kent State University April 22, 2004

Liquid Crystal Institute

RuggedLightweight

Cheap

Roll-to-RollManufacturing

Conformable

Page 5: Liquid Crystal Institute John West Kent State University April 22, 2004

Liquid Crystal Institute

• Conventional LCD’s and OLED/PLEDS require expensive substrates and development of organic TFT’s – Conventional LCD’s

• Use polarized light (non birefringent substrates)• Active matrix (organic TFT’s)• Surface alignment (high temperature and solvent stability)

– OLED/PLEDS• Oxygen sensitive (barrier layers)• Active matrix (organic TFT’s)

• Unconventional LC Conventional SubstrateApproaches – Polymer Dispersed Liquid Crystals– Bistable Chosterics– Bistable Smectics– Dichroic Dye LCDs

Page 6: Liquid Crystal Institute John West Kent State University April 22, 2004

Liquid Crystal Institute

Manufactured in a continuous roll-to-roll process

Conventional ITO coated polyester substrates (no barrier coatings, no alignment layers)

Single pixel.

Page 7: Liquid Crystal Institute John West Kent State University April 22, 2004

Liquid Crystal Institute

Bistable Cholesterics

1. Bright, high contrast images

2. High resolution with passive matrix

3. No polarizers required (can use birefringent substrates)

4. Polymers added for mechanical stability

Page 8: Liquid Crystal Institute John West Kent State University April 22, 2004

Liquid Crystal Institute

Reflective Cholesteric Displays

planar focal conic

Switch between reflecting planar texture and weakly scattering focal conic texture

Page 9: Liquid Crystal Institute John West Kent State University April 22, 2004

Liquid Crystal Institute

Ele

ctri

c F

ield

planar focal conic

focal conic

transient planar

homeotropic

slow

fastfa

st

Switching Mechanism

Page 10: Liquid Crystal Institute John West Kent State University April 22, 2004

Liquid Crystal Institute

Flexible Plastic Bistable Cholesteric Display

Figure 1: A four inch square, 320 by 320 pixel bistable cholesteric display made using flexible polyester substrates

• 4 inch square• 320 x 320 pixel• bistable cholesteric with polymer• flexible polyester substrate

West Rouberol, Francl, Ji, Doane and Pfeiffer

Asia Display, 1995

Page 11: Liquid Crystal Institute John West Kent State University April 22, 2004

Liquid Crystal Institute

Problems

1. Photolithography makes roll-to-roll processing difficult (expensive)

2. High polymer content formulation produces light scattering

a) Reduces reflection in planar state

b) Increases back scatter in focal conic state

c) Lowers brightness and contrast

Page 12: Liquid Crystal Institute John West Kent State University April 22, 2004

Liquid Crystal Institute

Preliminary Solution

1. Print resist for etching of electrodes:(roll-to-roll processing)

2. Segregate polymer into the inter-pixel region: Polymer Walls (bright display)

Page 13: Liquid Crystal Institute John West Kent State University April 22, 2004

Liquid Crystal Institute

Wax Transfer Printing of Resist

Tektronix Phaser 240 Wax Transfer Printer

Thermal Print Head

Wax Transfer Sheet

ITO Coated Polyester Film

Page 14: Liquid Crystal Institute John West Kent State University April 22, 2004

Liquid Crystal Institute

A replica of the wax resist pattern.

Close-up of the wax pattern printed onto the ITO coated Mylar. The dark lines are the wax

pattern.

Resist Pattern30 pixels/inch

Page 15: Liquid Crystal Institute John West Kent State University April 22, 2004

Liquid Crystal Institute

Etching and Stripping

1. Standard etch bath of nitric-sulfuric acid

2. Strip using warmed (50 C) tetrahydrofuran or toluene

Page 16: Liquid Crystal Institute John West Kent State University April 22, 2004

Liquid Crystal Institute

Cell AssemblyTop

Substrate

Bottom Substrate

Cholesteric Polymer Mixture

BL 094 92%

NOA 65 8%

Page 17: Liquid Crystal Institute John West Kent State University April 22, 2004

Liquid Crystal Institute

Form Polymer Walls

• Improve contrast

• Provide rugged displays

• Improve the pressure resistance of displays -- PM-STN-LCDs by Sharp*

• Make possible large area, flexible plastic displays -- adhere the top and bottom substrates -- maintain uniform thickness

* T. Shinomiya, K. Fujimori, S. Yamagishi, K. Nishiguchi, S. Kohzaki, Y. Ishii,

F. Funada, and K. Awane, Asia Display, 255 (1995).

Page 18: Liquid Crystal Institute John West Kent State University April 22, 2004

Liquid Crystal Institute

Polymer Wall Formation Methods• Photo-mask -- patterned UV exposure of homogeneous mixtures of UV-curable monomers and liquid crystals

• N. Yamada, S. Kohzaki, F. Funada, and K. Awane, SID Digest of Technical Papers, 575 (1995).

• T. Shinomiya, K. Fujimori, S. Yamagishi, K. Nishiguchi, S. Kohzaki, Y. Ishii, F. Funada, and K. Awane, Asia Display, 255 (1995).

• Y. Ji, J. Francl, W. J. Fritz, P. J. Bos, and J. L. West, SID Digest of Technical Papers, 611 (1996).

• Patterned Electric Field -- blanket UV exposure after phase separation

Page 19: Liquid Crystal Institute John West Kent State University April 22, 2004

Liquid Crystal Institute

Field Formed Polymer Walls1) Apply an electric field while solution is warmed above

clearing/phase separation temperature

2) Cool to RT with field applied to induce polymer segregation

3) UV expose to form polymer walls

Kim, Francl, Taheri, West,Appl. Phys. Lett., 72, 2253 (1998).

Page 20: Liquid Crystal Institute John West Kent State University April 22, 2004

Liquid Crystal Institute

Field Induced Phase Separation

• A patterned electric field is applied to a mixture of liquid crystal and UV curable monomer

• Due to a larger dielectric constant, liquid crystal migrates to the high field pixel region while the monomer moves to the low field inter-pixel region

• When phase separation is complete, exposure to UV light polymerizes the monomer locking in the wall structure

Page 21: Liquid Crystal Institute John West Kent State University April 22, 2004

Liquid Crystal Institute

Electric Field Distribution

SEM Image of Polymer Walls

Page 22: Liquid Crystal Institute John West Kent State University April 22, 2004

Liquid Crystal Institute

AL AL AL

Detector

UV Source

Glass Substrate Aluminum Electrodes

Liquid Crystal& Monomer

AT-720Barrier Layer

ITO

h

Measure Rate of Field Induced Phase Separation

• One side of cell has aluminum electrodes which block incoming UV light.

• Only light passing through inter-pixel makes it to the detector

• This allows study of change in concentration of E44 in inter-pixel over time

Diagram of Test Cell

Page 23: Liquid Crystal Institute John West Kent State University April 22, 2004

Liquid Crystal Institute

Absorbance vs TimeMixture of E44 and Trimethylolpropane tris(3-

mercaptopropionate)at 40 °C

Absorbance vs Time: Varying Voltages @ 50 C Normalized

0.96

0.965

0.97

0.975

0.98

0.985

0.99

0.995

1

1.005

0 20 40 60 80 100 120 140

Time (sec)

Ab

sorb

ance

5 V

10 V

20 V

30 V

40 V

Page 24: Liquid Crystal Institute John West Kent State University April 22, 2004

Liquid Crystal Institute

How T and V Affect the Rate

• With the same voltage applied, increasing temperature decreases change observed in absorbance between field on and field off states

Absorbance vs Time: Varying Temperature

0. 72

0. 74

0. 76

0. 78

0. 8

0. 82

0. 84

0. 86

0. 88

0. 9

0 20 40 60 80 100 120 140

Time (sec)

Ab

sorb

ance T (C)=30

T (C)=40

T (C)=50

T (C)=60

T (C)=70

T (C)=80

Page 25: Liquid Crystal Institute John West Kent State University April 22, 2004

Liquid Crystal Institute

Rate of Phase Separation

1. Occurs in several seconds.

2. Increasing temperature decreases the magnitude of the effectbut has little effect on the rate.

3. Increasing the voltage increases the rate and extent of phase separation

Page 26: Liquid Crystal Institute John West Kent State University April 22, 2004

Liquid Crystal Institute

Flexible Plastic Display

1. Compatible with roll-to-roll processing2. Uses commercially available materials.

Page 27: Liquid Crystal Institute John West Kent State University April 22, 2004

Liquid Crystal Institute

Stressed Liquid Crystals

• Developed for beam steering applications– Decouple thickness and speed– Eliminate alignment layers

• Fastest nematic devices

Page 28: Liquid Crystal Institute John West Kent State University April 22, 2004

Liquid Crystal Institute

Unidirectionally Oriented Micro-Domains of Liquid Crystal Separated by Polymer Network

our results

LC

F

polymer

5

10

15

20

AFM image

SEM image

• Middle range of concentration of the polymer: between those for traditional polymer network structures and PDLC.

• Well-developed interpenetrating structure of polymer chains and connected liquid crystal domains.

• The active area may be of any size

• Application of shearing deformation in order to orient the liquid crystal domains

Page 29: Liquid Crystal Institute John West Kent State University April 22, 2004

Liquid Crystal Institute

Effect of Shearing

1000 1500 2000 25000

20

40

60

80

100

Before shearing After shearing

Wavelength, nm

Tra

nsm

ittan

ce, %

1.Reduces the relaxation time of the material.

2.Decrease the scattering in visible region of spectrum.

3.The liquid crystal domains become oriented in the direction of shearing

4.By adjusting the degree of shearing one can control the total phase shift.

Page 30: Liquid Crystal Institute John West Kent State University April 22, 2004

Liquid Crystal Institute

0 50 100 150 200 2500

2

4

6

8

10

Voltage, V

Inte

nsity

, arb

. un.

Phase retardation shift vs an applied electric field

0 50 100 150 200 250

0.0

0.5

1.0

1.5

2.0

2.5

3.0

= /2

= 9

= 7

= 5

= 3

=

Voltage, V

Pha

se r

etar

datio

n,

m

For a 22 m film almost all change of the phase retardation occurs below 130V.

The change of phase retardation depends linearly on the applied voltage – simple driving devices

Page 31: Liquid Crystal Institute John West Kent State University April 22, 2004

Liquid Crystal Institute

0 1 2 3 4 50

2

4

6

8

10

Time, ms

Inte

nsity

, arb

. un.

0.00 0.04 0.08 0.12 0.16 0.200

2

4

6

8

10 nd = 0.63 m

nd = 0.31 m

nd = 0.15 m

Time, ms

Inte

nsity

, arb

. un.

A phase retardation shift of 2 m occurs within 1 ms.

Phase retardation of 0.15 m occurred just in 40 microseconds

Dynamics of the Relaxation

Page 32: Liquid Crystal Institute John West Kent State University April 22, 2004

Liquid Crystal Institute

Possible applications: basic design of an OPA device

• Beam steering: a tilted LC director will yield an index of refraction gradient

l=l0/nHl=l0/nL

millimeters

mm

• Industrial application (laser cutting of metals or glass)

• Free space communications

• Fiber-optics connectors

• Military applications

• Laser displays

• Imaging applications

Page 33: Liquid Crystal Institute John West Kent State University April 22, 2004

Liquid Crystal Institute

SLCs for display applications

• 30 volt offset• 10 volt pulse• 20 sec turn on time• 40 sec turn off time

Page 34: Liquid Crystal Institute John West Kent State University April 22, 2004

Liquid Crystal Institute

Conclusion

• Stressed LC films produce ferroelectric speeds in a nematic film

• No alignment layer

• No light scattering

• No hysteresis

• Linear response

Page 35: Liquid Crystal Institute John West Kent State University April 22, 2004

Liquid Crystal Institute

The Next StepFlexible Optical and Electronic Device Manufacturing Facility

• Wright Capital Grant, $1.6M (State of Ohio)

• $1.6M match from industry and KSU

• Add to existing Resource Facility

• Provide centralized facility for development and

prototyping of flexible devices.

Page 36: Liquid Crystal Institute John West Kent State University April 22, 2004

Liquid Crystal Institute

Goal

• Develop materials required for flexible displays– optimized liquid crystals

– organic semiconductors

– conducting polymers

– optimized substrates

• Develop fabrications techniques– printing electrodes

– applying thin films

– lamination

– cutting

Page 37: Liquid Crystal Institute John West Kent State University April 22, 2004

Liquid Crystal Institute

PlanEstablish a facility for the research and development

of flexible electronic devices

• Printing• Coating• Lamination• Cutting• Electronics• Materials Synthesis

Page 38: Liquid Crystal Institute John West Kent State University April 22, 2004

Liquid Crystal Institute

Planned Research

• Evaluation of available substrates

• Development of printing techniques for electrodes

• Fabrication of printed flexible VGA display using only commercial materials.

Page 39: Liquid Crystal Institute John West Kent State University April 22, 2004

Liquid Crystal Institute

KSU/UA HANA

Start-Ups bring Innovation and JobsBuilt on an Effective Academic Industrial Collaboration

LXD, Inc.

Poly Displays

Akron Polymer Systems

Page 40: Liquid Crystal Institute John West Kent State University April 22, 2004

Liquid Crystal Institute

Utilize the unique skills in the region in polymers/liquid

crystals and printing to spawn a new

industry in flexible displays and related electronic devices.