Particles in displays
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1 Particles in displays Particles 2007 Particle-based device technologies August 18, 2007 Ian Morrison Cabot Corporation, Billerica MA
2 Particles in displays? Prints with pigments reflect light. The readability is high. But the image is static. Displays emit light. The images are dynamic. But the readability is poor.
3 Beyond readability Persistent images, lower power Liquid coating rather than vacuum coating Flexibility Less expensive Light weight Fancy form factors Passive addressing?
4 The Electronic Book How do you make an electronic book? Put together electronic pages.
5 The Electronic Book How do you make an electronic book? How do you make an electronic page? Put together electronic pages. Put together electronic pixels.
6 The Electronic Book How do you make an electronic book? How do you make an electronic page? How do you make an electronic pixel? Put together electronic pages. Put together electronic pixels. Make a dot that switches colors.
7 The Electronic Book How do you make an electronic book? How do you make an electronic page? How do you make an electronic pixel? How do you make a dot that switches? Put together electronic pages. Put together electronic pixels. Make a dot that switches colors. Encapsulate an ink that switches.
8 To create a display start with a print and invent ways to make it change:
9 Liquid ink-based printing technology An electrostatic image is written on a charged photoconductive surface with a scanning laser beam. Where addressed, charged pigment moves to the developer surface. The particles are transferred from the developer roll to paper and dried.
10 Electrophoretic displays Charged pigment particles. Suspended in a dyed oil. Addressed with electrodes.
11 Why ink pixels are needed Sedimentation: Electrohydrodynamics:
12 Shutter mode Charged pigment particles. Suspended in clear oil. Electrophoresis in shutter mode Polymer Vision International Reflective TFTs Addressed with electrodes.
13 Suspended particle displays* Particles. Suspended in an oil. Transparent *Invented by E.H. Land in 1934 Addressed with electrodes, AC or DC. Transparent, or reflective. The same effect can be obtained with small, polarizabile particles chaining in an electric field.
14 The charging of particles in oil: 1-1 To make particles move, not ions, requires minimal free ions, therefore need nonaqueous dispersions. If only charged particles move, and no charges were injected at the electrodes, the image forms capacitively. No net current and image stability!
15 Electric charges on carbon black in oil -40 Zeta Potential (mv) OLOA 1200 in dodecane (% weight)
16 Imaging by particle rotation The Gyricon display Charged, bichromal balls. Suspended in an oil. Encased in a plastic sheet. Addressed with electrodes. That Xerox built.
17 Gyricon Display Capable of gray levels by partial rotation. If the charge is unbalanced, a Coulomb force translates the ball. The torque varies as the ball rotates. Ground Electrode q Fluid Filled Cavity q d Bichromal Ball Switching Electrode Red and white bichromal balls Black and white bichromal balls
18 SiPix Corporation The Microcup technology Structure Bright white particles are suspended in a dyed solution enclosed in a Microcup.
19 The search for lower voltage and higher speeds Switching time goes as square of thickness: τ transit 2 d V μ The necessary thickness is determined by the optical density.
20 Imaging with oppositely charged pigments Development electrode Addressed electrode Positively charged pigment Negatively charged pigment Hydrocarbon oil
21 Typical charge control agents CCA1: Soluble tail: Polyhydroxystearic acid Head group: Quaternary ammonium - methyl sulfate CCA2: Soluble tail: C13 Hydrocarbon chains Head group: Sodium sulfosuccinate
22 Charging of a surface modified pigment 60 CCA Titrations on "Basic" Pigment #1 40 Zeta Potential (mv) 20 CCA 1 CCA % 0.1% 0.2% 0.3% 0.4% 0.5% 0.6% Wt% CCA 2
23 Charge titration with mixed micelles Zeta Potential (mv) 20 0 % CCA 2 0% 10% 20% 30% 40% 50% 60% 70% 80% 90% 100%
24 Cabot s modified pigments Covalently attached chargeable sites.
25 Titration of an acidic and a basic pigment Zeta Potential (mv) "Basic" Pigment #1 "Acidic" Pigment CCA 1 CCA 2 Note the concentration for oppositely charged particles
26 Stability of oppositely charged particles - - Calculate the force between particles as a function of distance. Determine the distance between particles that just equals the applied electric field. Calculate the energy of particles at that distance. Calculated how much closer the particles can come before the energy increases by kt. Half of that distance is the minimum steric barrier.
27 Requirements on steric barrier For low electric field, the necessary thickness increases with particle charge. At high field, the necessary thickness decreases with particle charge.
28 E Ink Corporation Dark State Light State - Sony Reader utilizing E Ink Imaging Film TM - Photos courtesy of Sony Corporation
29 Scaling laws for an ideal system Assume: the charged particles just neutralize the applied voltage. M is the mass of particles/area. The charge and zeta potential of the particles are: q = DV s nl ζ = q 4π Da The switching time doesn t t depend on size: t = 3η 2 L s 2Dζ V 0 The voltage is: V 3ζ MLs 0 = 2 ρ a Bigger is better!
30 Particle Morphologies Not: But: Not: - But: -
31 Passive addressing: Thresholds From the physics of colloids: Inverse electrorheological fluids Field dependence of zeta potential AC electric fields time dependencies Particle-particle or particle-wall adhesion Structures in fluid (particles or wide variety of polymer gels)
32 Xeroxgraphy Dry printing Dry toner particles exchange charge (tribocharge)) with large, generally magnetic carrier bead. Photo courtesy Xerox A developer bead coated with small toner particles An image is formed when the toner particles are pulled off and attach to the electrostatic image on a photoreceptor.
33 Bridgestone s Quick Response Liquid Powder Display The Liquid Powder is a dry dispersion of two types of particles. The particles are about 10 microns, pigmented polymer beads, spherical, smooth, and chemically treated. The powder flows freely. The different colors have different sign charged. The image forms quickly with the separation of dry powder in the electric field.
34 Caveat emptor An adequate print resolution is about 1200 dots/inch. Or pixels of about 20 microns (for black and white). Smaller for cyan/magenta/yellow. Or about 10,000 pixels across a page! Well beyond current electronic displays! Progress will be limited by the electronic addressing.
35 Particles in displays Dielectrophoresis - particle alignment or chaining Segmented structures Particle rotation Electrophoresis to a viewing surface Particle and dye Dual particle Electrophoresis in shutter mode Passive addressing Dry powder flow
36
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