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Organic Light Emitting Diodes
(OLEDs)
Physics 496/487
Matt Strassler
Why OLEDs


Lighting efficiency







Displays: Significant advantages over liquid crystals






Incandescent bulbs are inefficient
Fluorescent bulbs give off ugly light
LEDs (ordinary light emitting diodes) are bright points; not versatile
OLEDs may be better on all counts
Faster
Brighter
Lower power

Cost and design


LEDs are crystals; LCDs are highly structured; OLEDs are not –





Malleable; can be bent, rolled up, etc.
Easier to fabricate

In general, OLED research proceeds on many fronts
Plan of talk


Light-Emitting Diode







Bands and Conduction
Semiconductor
Standard Diode
Light Emission

Organic Light-Emitting Diode




Organic Semiconductors
Organic Diode
Light Emission
Electrons in a Lattice

E

V(r)


Atom has bound states





Discrete energy levels
Partially filled by electrons

r

Periodic array of atoms
(cf. QM textbook)




Effectively continuous
bands of energy levels
Also partially filled

E
V(x)

r
The Bands on Stage
E

Gap

Insulator

E

No
Ga
p

Conductor

E

E

E

Smal
l Gap

Semiconductor

Doped Semiconductors
Doping – Add Impurities
N-type

P-type
The Bands on Stage
E

E

E

E

E

N-type
Gap

Insulator

No
Ga
p

Conductor

P-type

Smal
l Gap

Semiconductor

Doped Semiconductors
Diode: p-type meets n-type
E

E
Diode: p-type meets n-type
E

E
Diode: p-type meets n-type
E

E
Diode: p-type meets n-type
E

E

Electric Field

Excess
Negative
Ions

Excess
Positive
Ions
Diode: p-type meets n-type
Try to make current flow to left?
Depletion Zone Grows

Electric Field
Diode: p-type meets n-type
Try to make current flow to right?
Current Flows!
Electrons in higher band meet Holes in lower band

Electric Field

Current
Excitons
N-type


Electron in higher band meets a hole in lower band



The two form a hydrogen-like bound state! Exciton!


Like “positronium”





Annihilation






Can have any orbital angular momentum
Can have spin 0 or spin 1
Rate is slow
Electron falls into hole
Energy emitted

Energy released as electron falls into hole



May turn into vibrations of lattice (“phonons”) – heat
May turn into photons (only in some materials)





Infrared light (if gap ~ 1 eV) – remote control
Visible light (if gap ~ 2-3 eV) – LED

May excite other molecules in the material (if any; see below)

E
Organic Semiconductors


These are not crystals! Not periodic structures



Band structure is somewhat different


“Orbitals” determined by shape of organic molecule






Polymers are common

Conduction is different



Electrons or holes may wander along a polymer chain
As with inorganic conductors





Quantum chemistry of pi bonds, not simple junior QM

Some materials allow electrons to move
Some materials allow holes to move – typical for organics!!

Doping is more difficult



Doping typically not used
Instead electrons/holes are provided by attached metals
The basic OLED

Anode

Conductive Layer

Cathode

Emissive Layer
The basic OLED
• The holes move more efficiently in organics

Anode

Conductive Layer

Cathode

Emissive Layer
The basic OLED
• The holes move more efficiently in organics
• Excitons begin to form in emissive layer

Anode

Conductive Layer

Cathode

Emissive Layer
The Exciton Exits in a Flash


As before, excitons eventually annihilate into





Molecular vibrations  heat (typical)
Photons (special materials, rare)

But with organics, can add



Fluorescent molecules
Phosphorescent molecules

e.g. attach to end of polymer


Light can be generated indirectly:







Exciton can transfer its energy to this molecule
Molecule is thus excited
Returns to ground state via fluorescence or phosphorescence

Greatly increases likelihood (per exciton) of light emission
Also allows for different colors


determined by the light-emitting molecule(s), not the exciton
OLEDs


Similar physics to LEDs but






Manufacturing advantages







Soft materials – very malleable
Easily grown
Very thin layers sufficient

Many materials to choose from
Relatively easy to play tricks






Non-crystalline
No doping; use cathode/anode to provide needed charges
Fluorescence/phosphorescence enhance excitonlight probability

To increase efficiency
To generate desired colors
To lower cost

Versatile materials for future technology
Some references


How Stuff Works
http://electronics.howstuffworks.com





Craig Freudenrich, “How OLEDs work”
Tom Harris, “How LEDs Work”

Hyperphysics Website

http ://hyperphysics.phy-astr.gsu.edu/hbase/solids/pnjun.html




“The P-N Junctions”, by R Nave

Connexions Website
http://cnx.org




Webster Howard, “Better Displays with Organic Films”




Scientific American, pp 5-9, Feb 2004

M.A. Baldo et al, “Highly efficient phosphorescent
emission from organic electroluminescent devices”




“The Diode”, by Don Johnson

Nature 395, 151-154 (10 September 1998)

Various Wikipedia articles, classes, etc.
A neat trick


Exciton










But



P


Spin 0 (singlet)
Spin 1 (triplet)
Can transfer its energy but
not its spin to molecule
Thus spin-1 can’t excite
fluorescents
Lose ¾ of excitons
Use phosphors
Bind to polymer so that
exciton can transfer spin

Then 4 times as many
excitons cause light emission

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Organic light emitting diodes

  • 1. Organic Light Emitting Diodes (OLEDs) Physics 496/487 Matt Strassler
  • 2. Why OLEDs  Lighting efficiency      Displays: Significant advantages over liquid crystals     Incandescent bulbs are inefficient Fluorescent bulbs give off ugly light LEDs (ordinary light emitting diodes) are bright points; not versatile OLEDs may be better on all counts Faster Brighter Lower power Cost and design  LEDs are crystals; LCDs are highly structured; OLEDs are not –    Malleable; can be bent, rolled up, etc. Easier to fabricate In general, OLED research proceeds on many fronts
  • 3. Plan of talk  Light-Emitting Diode      Bands and Conduction Semiconductor Standard Diode Light Emission Organic Light-Emitting Diode    Organic Semiconductors Organic Diode Light Emission
  • 4. Electrons in a Lattice E V(r)  Atom has bound states    Discrete energy levels Partially filled by electrons r Periodic array of atoms (cf. QM textbook)   Effectively continuous bands of energy levels Also partially filled E V(x) r
  • 5. The Bands on Stage E Gap Insulator E No Ga p Conductor E E E Smal l Gap Semiconductor Doped Semiconductors
  • 6. Doping – Add Impurities N-type P-type
  • 7. The Bands on Stage E E E E E N-type Gap Insulator No Ga p Conductor P-type Smal l Gap Semiconductor Doped Semiconductors
  • 8. Diode: p-type meets n-type E E
  • 9. Diode: p-type meets n-type E E
  • 10. Diode: p-type meets n-type E E
  • 11. Diode: p-type meets n-type E E Electric Field Excess Negative Ions Excess Positive Ions
  • 12. Diode: p-type meets n-type Try to make current flow to left? Depletion Zone Grows Electric Field
  • 13. Diode: p-type meets n-type Try to make current flow to right? Current Flows! Electrons in higher band meet Holes in lower band Electric Field Current
  • 14. Excitons N-type  Electron in higher band meets a hole in lower band  The two form a hydrogen-like bound state! Exciton!  Like “positronium”    Annihilation     Can have any orbital angular momentum Can have spin 0 or spin 1 Rate is slow Electron falls into hole Energy emitted Energy released as electron falls into hole   May turn into vibrations of lattice (“phonons”) – heat May turn into photons (only in some materials)    Infrared light (if gap ~ 1 eV) – remote control Visible light (if gap ~ 2-3 eV) – LED May excite other molecules in the material (if any; see below) E
  • 15. Organic Semiconductors  These are not crystals! Not periodic structures  Band structure is somewhat different  “Orbitals” determined by shape of organic molecule    Polymers are common Conduction is different   Electrons or holes may wander along a polymer chain As with inorganic conductors    Quantum chemistry of pi bonds, not simple junior QM Some materials allow electrons to move Some materials allow holes to move – typical for organics!! Doping is more difficult   Doping typically not used Instead electrons/holes are provided by attached metals
  • 16. The basic OLED Anode Conductive Layer Cathode Emissive Layer
  • 17. The basic OLED • The holes move more efficiently in organics Anode Conductive Layer Cathode Emissive Layer
  • 18. The basic OLED • The holes move more efficiently in organics • Excitons begin to form in emissive layer Anode Conductive Layer Cathode Emissive Layer
  • 19. The Exciton Exits in a Flash  As before, excitons eventually annihilate into    Molecular vibrations  heat (typical) Photons (special materials, rare) But with organics, can add   Fluorescent molecules Phosphorescent molecules e.g. attach to end of polymer  Light can be generated indirectly:      Exciton can transfer its energy to this molecule Molecule is thus excited Returns to ground state via fluorescence or phosphorescence Greatly increases likelihood (per exciton) of light emission Also allows for different colors  determined by the light-emitting molecule(s), not the exciton
  • 20. OLEDs  Similar physics to LEDs but     Manufacturing advantages      Soft materials – very malleable Easily grown Very thin layers sufficient Many materials to choose from Relatively easy to play tricks     Non-crystalline No doping; use cathode/anode to provide needed charges Fluorescence/phosphorescence enhance excitonlight probability To increase efficiency To generate desired colors To lower cost Versatile materials for future technology
  • 21. Some references  How Stuff Works http://electronics.howstuffworks.com    Craig Freudenrich, “How OLEDs work” Tom Harris, “How LEDs Work” Hyperphysics Website http ://hyperphysics.phy-astr.gsu.edu/hbase/solids/pnjun.html   “The P-N Junctions”, by R Nave Connexions Website http://cnx.org   Webster Howard, “Better Displays with Organic Films”   Scientific American, pp 5-9, Feb 2004 M.A. Baldo et al, “Highly efficient phosphorescent emission from organic electroluminescent devices”   “The Diode”, by Don Johnson Nature 395, 151-154 (10 September 1998) Various Wikipedia articles, classes, etc.
  • 22. A neat trick  Exciton       But   P  Spin 0 (singlet) Spin 1 (triplet) Can transfer its energy but not its spin to molecule Thus spin-1 can’t excite fluorescents Lose ¾ of excitons Use phosphors Bind to polymer so that exciton can transfer spin Then 4 times as many excitons cause light emission