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Electroluminescence (EL)
• The emission of light by electric current
• Historical development
a. 1962 (Holonyak and Bevacqua)
• Inorganic semiconductors for light-emitting diodes
(LEDs)
e.g. GaPxAs1−x (x = 1.00–0.40) and GaN-based materials
• The energy of the light emitted can be changed by
adjusting the composition of the material
Electroluminescence (EL) (2)
BlueGaN
OrangeGaAsP:N
GreenGaP:N
RedGaP:ZnO
ColorLED material
+ − hv
Charge recombination
Basic Theory
Valence band
+
−−Conduction band
+ −Applied voltage
p-type n-type
Electroluminescence (EL) (3)
• p-type semiconductors : the added material has
fewer electrons than the host and adds positive
holes e.g. Si doped with B
• n-type semiconductors : the added material has
one more electrons in the valence shell than the
host material e.g. Si doped with P
Electroluminescence (EL) (4)
• Light emission arises from the recombination of
holes and electrons in a p-n junction made up of
p- and n-type semiconductors
• However, only single-crystal material is capable
of exercising this kind of recombination radiation
efficiently enough for practical use
Visible LEDs have been available commercially
since 1960s
Electroluminescence (EL) (5)
Crystal substrate
(transparent)
n-type
p-type
+
−
Light
output
Device structure for common LEDs
Electroluminescence (EL) (6)
b. 1987 (Tang and VanSlyke in Kodak)
• Fluorescent organic dyes as electroluminescent
materials for organic light-emitting devices
(OLEDs) (Small-molecule-based OLEDs)
e.g. tris(8-hydroxyquinoline)aluminum (Alq or
Alq3) and N,N’-diphenyl-N,N’-bis(3-
methylphenyl)-1,1’-biphenyl-4,4’-diamine (TPD)
Electroluminescence (EL) (7)
The first double-layer OLED
N
CH3
N
H3C
TPD
N
O
Al
3
Alq3
Ag
VMg:Ag
TPD
ITO
Glass
Alq3
−
+
EL light
Electroluminescence (EL) (8)
– 1990 (Friend et al. in Cambridge University)
• Luminescent conjugated polymers for polymer
light-emitting devices (PLEDs)
e.g. poly(1,4-phenylene vinylene) (PPV)
poly[2-(2’-ethylhexyloxy)-5-methoxy-1,4-
phenylene vinylene] (MEH-PPV)
nMeO
O
n
PPV MEH-PPV
Electroluminescence (EL) (9)
• Important features of PLEDs
– Inorganic semiconducting and small molecule organic dyes
have to be deposited as thin films by the relatively
expensive techniques of sublimation or vapour deposition,
which are not well suited for large-area displays
– Luminescent polymers can be deposited from solution as
thin films over larger area by spin-coating techniques
– The physical properties (e.g. colour, emission efficiency) of
conjugated polymers can be fine-tuned by manipulation of
their chemical structures
Electroluminescence (EL) (10)
Normalized photoluminescence spectra of side-chain-modified PPV with the general
formula shown on the top: (1) R1, R2, R3, R4 = alkyl, R5, R6 = CN; (2) R1, R2 = alkoxy,
R3, R4 = alkyl, R5, R6 = CN; (3) R1, R2 = alkoxy, R3, R4 = alkoxy, R5, R6 = H; (4) R1, R2
= alkoxy, R3, R4 = alkoxy, R5, R6 = H annealed; and (5) R1, R2 = alkoxy, R3, R4 =
alkoxy; R5, R6 = CN
R1
R2
R3
R6
R5
R4
l
1-l
Theory of OLEDs or PLEDs
• The simplest OLED or PLED configuration
consists of an electroluminescent layer
sandwiched between an anode and a
cathode, one of which has to be semi-
transparent
• Under an applied bias, injection of holes
takes place at the anode whereas injection
of electrons occurs at the cathode
Theory of OLEDs or PLEDs (2)
• Some of the electrons and holes combine within the emissive material to form singlet and triplet excited states. Such an electron-hole pair (exciton) may then result in the emission of a photon
Schematic drawing of single-layer
EL device
++
+ ++
+
+
− −
hv
+
−Al, Ca, or Mg
Cathode
light-emitting
polymer
glass or polymer substrate
ITO anode
Theory of OLEDs or PLEDs (3)
a) Irradiation of a fluorescent layer excites an
electron from HOMO to LUMO. In a typical
conjugated polymer, two new energy states are
generated upon relaxation within the original
HOMO−LUMO energy gap and are each filled with
one charge of opposite sign (singlet excited state).
The excited polymer may then relax to the ground
state with emission of light at a longer wavelength
than that absorbed (photoluminescence). b) In a
polymer LED, electrons are injected into the LUMO
(to form radical anions) and holes into the HOMO
(to form radical cations) of the electroluminescent
polymer. The resulting charges migrate from
polymer chain to polymer chain under the influence
of the applied electric field. When a radical anion
and a radical cation combine on a single conjugated
segment, singlet and triplet excited states are formed,
of which the singlets can emit light.
Anode: high work-function electrode e.g. indium tin oxide (ITO)
Cathode: low work-function electrode e.g. Ca, Al, MgAg alloy
HOMO
LUMO
hv hv'
singlet excited state
a)
singlet excited stateradical anion
hv'
−
+ e -
Cathodeb)
+Anode
radical cation
− e -
Theory of OLEDs or PLEDs (4)
• Unfortunately, the mobility of electrons and
holes in most organic materials are
considerably different, leading to exciton
formation in the vicinity of one of the two
contacts (For example, since holes migrate
much more easily through PPV than
electrons, electron-hole recombination takes
place near the cathode)
Theory of OLEDs or PLEDs (5)
• Since non-radiative exciton recombination,
or quenching, is enhanced at the electrode-
organic interface, the single-layer structure
typically exhibits a low quantum efficiency
⇒ Heterojunction OLEDs
Layers in OLEDs
• Hole-Transporting Layer (HTL)
– Transports holes from the anode to the EML or
ETL
• Electron-Transporting Layer (ETL)
– Transports electrons from the metal cathode to
the EML or HTL
Layers in OLEDs (2)
• Emission Layer (EML)
– Transports both holes and electrons
– The layer where the recombination of holes and
electrons takes place
Cathode
ETL/EML
HTL
Anode
Substrate
−
+
hvCathode
HTL/EML
ETL
Anode
Substrate+
−
hv
Double layer membrane
Either ETL or HTL behaves as EML
Layers in OLEDs (3)
Triple-layer device
Cathode
ETL
EML
HTL
Anode
Substrate
−
+
hv
The recombination of holes and electrons occurs in an
independent EML
Common layer materials in OLEDs (2)
ii. ETL materials, e.g. PBD, Alq3
NN
ONN
O
PBD
Oxadiazoles are
electron-deficient