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ORGANIC SEMICONDUCTORS Christian Ohrt, Thomas Preuße ...

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<strong>ORGANIC</strong> <strong>SEMICONDUCTORS</strong><br />

<strong>Christian</strong> <strong>Ohrt</strong>, <strong>Thomas</strong> Preuße<br />

Faculty of Enginering, University of Kiel<br />

Kaiserstraße 2 24143 Kiel Germany<br />

ABSTRACT: This paper deals with a short introduction into the field of organic semiconductors. Its part of a<br />

presentation, which is hold in the course material science seminar for the fifth semester students of the bachelor<br />

material science study. We want to give a overview about the history, the structures and bondings, the opctical<br />

properties, the conductive properties and some applications of organic semiconductors in our present time for<br />

example OLEDs. Then we will show some advantages of using organic semiconductors in comparison to typical<br />

inorganic semiconductors like Si and GaAs. The semiconductor technology is one of the most important deployments<br />

in the world and is required in nearly all applications of high technology. One way to improve the properties of this<br />

technology can be to use organic semiconductors.<br />

1 Historical background<br />

The first discovery of organic semiconductors was<br />

made in the year 1963 by D. E. Weiss and the members of<br />

his group. They discovered high conductivity in ioine-<br />

”doped” oxidized polypyrrole blacks. They could achieve<br />

a conductivity of 1 Siemens/cm, which is equivalent to a<br />

resistance of 1 Ohm/cm. In 1965 they were able du reduce<br />

the resistance 0.03 Ohm/cm with other conductive<br />

polymers. Unfortunately this work was lost until recently.<br />

In 1974 John McGuiness together with his group built a<br />

voltage-controlled organic-polymer switch, which consist<br />

of melanin, a self-doped mixed copolymer of oxidized<br />

polyacetylene, polypynole and polyaniline. This material<br />

emitted a flash of light when it switched. In the year 1977<br />

conductivity in polymers was rediscovered and reported<br />

by Alan J. Heeger, Alan G. McDiamid and Hideki<br />

Shirakawa. They reported high conductivity in similarly<br />

oxidized and iodine-doped polyacetylene. In the year 2000<br />

they received the Nobel Prize in Chemistry “For the<br />

discovery and development of conductive organic<br />

polymers", which was leading to some disputes, because<br />

of the earlier discovery in this field especially by D. E.<br />

Weiss.<br />

2 Properties of organic semiconductors<br />

2.1 Basic properties<br />

Organic semiconductors are low molecular weight<br />

materials with fundamentally different bondings as their<br />

inorganic counterparts. Organic semiconductors have a<br />

conjugated π-electron system beeing formed by the by the<br />

pZ-orbitals of sp² hybridized C-Atoms in the molecules.<br />

The π–bonding is significant weaker then σ-bonding and<br />

the energy gap of π– π* transitions is about 1.5 to 3 eV,<br />

but the energy gap can be controlled by the degree of<br />

conjugation in the molecule.<br />

π-electron system beeing formed by the by the<br />

pZ-orbitals of sp² hybridized C-Atom<br />

The consequences: Organic semiconductors have a<br />

reduced hardness and a lower melting point as inorganic<br />

semiconductors and much weaker delocalization of<br />

electronic wave functions of neighbouring molecules<br />

which has direct appplications for optical properties and<br />

charge carrier transport.<br />

2.2 Optical properties<br />

Organic semiconductors have well-defined spin states,<br />

the so called singlet and triplet state. These two states<br />

derive from quantum mechanics, more precisely from the<br />

multiplicity. The singlet state is responsible for<br />

fluorescence and the triplet state is responsible for<br />

phosphorescence. To describe phosphorescence we need<br />

the term of intersystem crossing. Intersystem crossing<br />

means, that an electron changes its spin, after it was<br />

excited by a photon. After the intersystem crossing, it can<br />

not reduce its state of energy by spontan emission like in<br />

flourenscence, the electron changes the system again and<br />

than it can go back to the origin energy state by emiting<br />

weak radiation, the so called phosphorescence.


Singlet and triplet states<br />

2.3. Conductive Properties<br />

Several kinds of carriers mediate conductivity in organic<br />

semiconductors. These include π-electrons and unpaired<br />

electrons. Almost all organic solids are insulators. But<br />

when their molecules have π-conjugate systems, electrons<br />

can move in the so called π-electron cloud. In charge<br />

transfer complexes, even unpaired electrons can stay<br />

stable for a long time, and are the carriers. This type of<br />

semiconductor is also obtained by pairing an electron<br />

donor molecule and an electron acceptor molecule. Thats<br />

how you can dope organic semiconductors.<br />

3 Applications<br />

3.1 OLEDs<br />

An organic light-emitting diode (OLED) is a lightemitting<br />

diode (LED) whose emissive electroluminescent<br />

layer is composed of a film of organic compounds. The<br />

layer usually contains a polymer substance that allows<br />

suitable organic compounds to be deposited. They are<br />

deposited in rows and columns onto a flat carrier by a<br />

simple "printing" process. The resulting matrix of pixels<br />

can emit light of different colours.<br />

Such systems can be used in television screens,<br />

computer displays, portable system screens, advertising,<br />

information and indication. OLEDs can also be used in<br />

light sources for general space illumination, and largearea<br />

light-emitting elements. OLEDs typically emit less<br />

light per area than inorganic solid-state based LEDs<br />

which are usually designed for use as point-light sources.<br />

Operation mode of an OLED<br />

4 Advantages and disadvantages of organic<br />

semiconductors<br />

One of the main reasons for developing organic<br />

semiconductors instead of inorganic is their potential for<br />

lower costs than silicon devices . Also their mechanical<br />

properties (less weight, more flexible and elastic, easier<br />

to produce in form of thin layers by pecial printing<br />

techniques) are some advantages over their inorganic<br />

counterparts. Disadvantages are their higher chemically<br />

activity, which means, that they need more protection by<br />

encapsulation. Because of lower melting point they are<br />

more temperature sensitive in comparison to inorganic<br />

semiconductors and finally is the process of the charger<br />

transfer mechanisms not understood for 100 %.<br />

5 Future Trends<br />

In the present time OLED displays are still very<br />

expensive as you can see at the new XEL-1 by Sony.<br />

With a cost of 1700$ and a display with only 11 inch the<br />

new OLED displys are still to expensive. But OLED<br />

displys have some advantages. For example: The displays<br />

of the XEL-1 from Sony is only 2,5 cm thick.

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