Conducting Organic Materials and DevicesConducting polymers were discovered in 1970s in Japan. Since this discovery, there has been a steady flow of new ideas, new understanding, new conducing polymer (organics) structures and devices with enhanced performance. Several breakthroughs have been made in the design and fabrication technology of the organic devices. Almost all properties, mechanical, electrical, and optical, are important in organics. This book describes the recent advances in these organic materials and devices. |
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Page v
... Doping ofPolyacetylene 2.2. BAND STRUCTURE OE t-PA 2.3. THE SOLITONS AND THE POLARONS 2.3.1. The Solitons 2.3.2. The Polarons 2.4. TRANSPORT PROPERTIES 2.4.1. Mobility in Selected Polymers 2.4.2. Conductivity and Susceptibility Chapter ...
... Doping ofPolyacetylene 2.2. BAND STRUCTURE OE t-PA 2.3. THE SOLITONS AND THE POLARONS 2.3.1. The Solitons 2.3.2. The Polarons 2.4. TRANSPORT PROPERTIES 2.4.1. Mobility in Selected Polymers 2.4.2. Conductivity and Susceptibility Chapter ...
Page 1
... doping it with iodine. The doped films looked like golden metallic sheets. Later more than a dozen organic polymers could be made conducting by appropriate doping. Now plastics with conductivity comparable to that of copper can be ...
... doping it with iodine. The doped films looked like golden metallic sheets. Later more than a dozen organic polymers could be made conducting by appropriate doping. Now plastics with conductivity comparable to that of copper can be ...
Page 3
... doped PPV and AsF5 doped PPP. For more details see Ref. [12] from where the figure has been taken. Note that conductivity clo se to that of copper has been achieved. Though conductivity of polyaniline is not as high as that of some ...
... doped PPV and AsF5 doped PPP. For more details see Ref. [12] from where the figure has been taken. Note that conductivity clo se to that of copper has been achieved. Though conductivity of polyaniline is not as high as that of some ...
Page 4
... DOPED t-POLYACETYLENE PF-DOPED POLYANILINE PF6-DOPED POLYPYRROLE Metals SILICON Fl) :O H u = "5 :1 O u .— E a w GLASS UNDOPED c-POLYACETYLEN '2 >1 F p-t > p-q P U D Q Z O U N) 2 Insulators P16. 1.2. Conductivity of polymers varies over ...
... DOPED t-POLYACETYLENE PF-DOPED POLYANILINE PF6-DOPED POLYPYRROLE Metals SILICON Fl) :O H u = "5 :1 O u .— E a w GLASS UNDOPED c-POLYACETYLEN '2 >1 F p-t > p-q P U D Q Z O U N) 2 Insulators P16. 1.2. Conductivity of polymers varies over ...
Page 7
... DOPING OE POLYACETYLENE The most commonly used method to synthesize the PA is the Shirakawa method. In this method a smooth surface wetted by the Ziegler—Natta catalyst is exposed to the acetylene gas. A film of PA (generally c-PA) is ...
... DOPING OE POLYACETYLENE The most commonly used method to synthesize the PA is the Shirakawa method. In this method a smooth surface wetted by the Ziegler—Natta catalyst is exposed to the acetylene gas. A film of PA (generally c-PA) is ...
Contents
1 | |
7 | |
23 | |
Chapter 4 Light Emitting Diodes and Lasers | 67 |
Chapter 5 Solar Cells | 95 |
Chapter 6 Transistors | 123 |
Bibliography | 147 |
Index | 157 |
Contents of Volumes in this Series | 167 |
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Conducting Organic Materials and Devices Suresh C. Jain,M. Willander,V. Kumar No preview available - 2007 |
Common terms and phrases
absorption acceptor active layer Alq3 amorphous Appl Applications applied voltage band bandgap bipolaron blue calculated carrier density cathode characteristics charge carriers cm_3 color conducting polymers configuration curves dark current Defects devices dopant doped electric field electron emission emitter energy transfer Epitaxy equation excitons experimental data fabricated field effect figure filled first fit flow function gate voltage heterojunction hole III—V Compounds illuminated increases injection laser Lett light emitting diodes measured MEH-PPV metal midgap mobility model molecular molecules obtained OFETs ohmic OLEDs open circuit voltage organic materials organic solar cells parameters pentacene photovoltaic Phys plots polyacetylene quantum efficiency sample Schottky barrier SCLC short circuit current shown in Fig shows Silicon solid solitons space charge space charge limited spectra spin coating structure substrate sufficient superposition principle t-PA theory thickness thin film transistor transistors transport traps V2 law values vinylene white light