Optical, Electronic and Structural Properties of Semiconductor Nanostructures and Optoelectronic Devices Inorganic Semi- conductors & Devices (Compounds of III- V, I-III-VI 2 , II- IV-V2) Organic Semi- conductors & Devices (Polymers & Functional Polymers) Solar Components & Systems (Photovoltaic und Solar Thermal) Prof. Dr. Gerhard Gobsch Department of Experimental Physics I
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Optical, Electronic and Structural Properties of Semiconductor Nanostructures and Optoelectronic Devices Inorganic Semi- conductors & Devices (Compounds.
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Optical, Electronic and Structural Properties of Semiconductor Nanostructures and Optoelectronic Devices
Inorganic Semi-conductors & Devices
(Compounds of III-V, I-III-VI2, II-IV-V2)
Organic Semi-conductors & Devices
(Polymers & Functional Polymers)
Solar Components & Systems
(Photovoltaic
und Solar Thermal)
Prof. Dr. Gerhard Gobsch
Department of Experimental Physics I
Organic Optoelectronics
ACOPhys, St. Petersburg, Sept 2006
An Introduction
Materials, Processing, Concepts and Devices
• Introduction• Molecular Energy Levels and
Charges• Materials and Processing• Devices• Summary
Organic Optoelectronics - Outline
Organic Optoelectronics
Organic Optoelectronics deals with semiconductor devices in which the semiconductor is an organic material.
There are light emitting diodes (OLED), thin film field effect transistors (OFET), solar cells, lasers, detectors, sensors...
Beyond the scope of the present lecture is the field of “Organic Electronics ↔ Polymer Electronics“.
Theoretical basics of electronic properties of organic materials were given in the lecture of Prof. Runge.
The Nobel Prize in Chemistry 2000
"for the discovery and development of conductive polymers"
Alan J. Heeger Alan G.
MacDiarmid Hideki Shirakawa
1/3 of the prize 1/3 of the prize 1/3 of the prize
USA USA and New Zealand
Japan
University of California Santa Barbara, CA, USA
University of Pennsylvania Philadelphia, PA, USA
University of Tsukuba Tokyo, Japan
b. 1936 b. 1927(in Masterton, New Zealand)
b. 1936
“for the discovery and developement of conductive polymers“
Organic Optoelectronics
A new material class!
“In creating and expanding the 4th generation of polymers, we
attempted to understand nature with sufficient depth that we
could achieve materials with novel and unique properties, that
are not otherwise available.
This was (and is) an elegant and somewhat dangerous exercise;
elegant because it requires the synthesis of knowledge from
chemistry, physics and materials science, and dangerous
because when working on the boundary of three disciplines, one
is always pushing beyond the knowledge and experience of this
background.
To our research in this interdisciplinary field has had sufficient
impact on chemistry to be recognized by the Nobel Prize gives
us, therefore, particular satisfaction.”
Alan J. Heeger (on occasion of giving him the Nobel Prize for Chemistry in 2000)
Advantages
Pros and Cons of polymers for electronic applications
• Metallic and semiconducting properties by doping• Combination of plastic with electronic properties• Property engineering• Solubility in organic solvents, variable processibility• Use of printing technologies• No vacuum and no high temperature processes
Low-cost production
Disadvantages
• Low integrated devices and circuits (in the very near future)
• Degeneration in O2- and H2O-atmosphere
Long-term stability is still a critical point
Application of Functional Polymers
Functional polymers with special / selected electronic properties
Organic field-effect transistor (OFET)
Polymerelektronikmade by semiconducting and dielectric polymers
Organic solar cellsPhotovoltaic & optoelectronic
devices made by polymer photoconductors
Polymer actorsfor microsystem technology
Optical polymers with optimized spectral
transparency
Special elektronic polymers for
Planar antennas
Organic light emitting diodes
(OLED) and lasers Super capacities
Polymer batteries
Polymer sensors
Fuel cells
Integrated polymerelectronic circuits (IPC)
Temperature sensors Humidity sensors
Chemo- & biosensors Pressure / force sensors
More conjugatedpolymers...
Organic Semiconductors
Conductivity of materials
Charge carrier mobilities
comparably small (FET) mobilities*:
*C. D. Dimitrakopoulos and D. J. Mascaro IBM J. Res. & Dev. 45 (1), 2001
low mobilities & large absorption coefficients thin absorber
Charge carrier mobilities of thin films
Absorption overlap with solar spectrum
comparably small absorption range:
only a small fraction of the sunlight is used today!
300 400 500 600 700 800 900 1000 1100 12000.0
0.5
1.0
1.5
2.0
2.5
3.0
0
1x1018
2x1018
3x1018
4x1018
5x1018
MDMO-PPV P3HT PCBM
abso
rbtio
n co
effic
ient
/ 10
5 cm-1
wavelength [nm]
AM
1.5
pho
ton
flux
/m-2s-1
nm-1
Sili
con
Solar Spectrum and Absorption
• Introduction• Molecular Energy Levels and
Charges• Materials and Processing• Devices• Summary
Organic Optoelectronics
-bands in conjugated polymers
Molecular Energy Levels
HOMO
LUMO
Optical properties and transitions:Absorption Emission
absorptionfluorescencephosphorescence
luminescence (photo-, or electro-)
Molecular Energy Levels
For oligomers a shift of HOMO or LUMO levels towards smaller band-gaps is observed upon increasing the repeat unit. Compare with quantum-mechanical particle-in-a-box problem.
longer chain/wider box decrease in „band-gap“
CC
CC
CC
CC
H H H H
H H H
CC
CC
CC
CC
H H H H
H H H
Organic Semiconductors: Charges
PositiveSoliton:
NegativeSoliton:
Charge carriers on Polyacetylene:
(degenerategroundstate)
Charge transport in conjugated polymers
Polymer chain with characteristic defects (a);
schematic energy diagram for positive polarons without electric field (b) and
charge transport under applied electric field (c).
Electron transfer in a conjugated polymer after optical excitation calculated within the td-DFT by means of the GAUSSIAN quantum chemistry package
Charge carrier mobilities
comparably small (FET) mobilities*:
*C. D. Dimitrakopoulos and D. J. Mascaro IBM J. Res. & Dev. 45 (1), 2001
low mobilities & large absorption coefficients thin absorber
• Introduction• Molecular Energy Levels and
Charges• Materials and Processing• Devices• Summary
Combination of OLED illumination and photodiode array detection for personal identification.
Organic Laser (optically pumped):
From left to right: Organic laser emitting red light; structure of the first organic laser using external optical excitation; typical laser emission spectra spanning the visible
from the blue at a wavelength of 450nm, to the infrared at 700nm.
Organic Semiconductor Devices: Laser
• Introduction• Molecular Energy Levels and
Charges• Materials and Processing• Devices• Summary
Organic Optoelectronics
Why “ORGANIC“? Disadvantages:
Organic Optoelectronics
- light weight- flexible- low cost- large area- “tailor-made“ properties- more colors- printing production