Difference between revisions of "Electronic Coupling"
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In order have better performance for devices based on electronic semiconductors the charge carrier mobility should be as high a possible and this is accomplished by maximizing the electronic coupling. | In order have better performance for devices based on electronic semiconductors the charge carrier mobility should be as high a possible and this is accomplished by maximizing the electronic coupling between atoms in a molecule. | ||
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=== Transpolyacetylene === | === Transpolyacetylene === | ||
[[Image:Transpolyacetylene_unit.png|thumb|300px|The repeating unit of transpolyacetylene is shown]] | [[Image:Transpolyacetylene_unit.png|thumb|300px|The repeating unit of transpolyacetylene is shown]] | ||
In perfectly coplanar extended transpolyacetylene chain the electron coupling between adjacent units t (the transfer integral) is on the order of 2.5 – 3eV. Across the entire bandwidth | In perfectly coplanar extended transpolyacetylene chain the electron coupling between adjacent units t (the transfer integral) is on the order of 2.5 – 3eV. Across the entire bandwidth there is 20 eV. | ||
In actual samples there is conductivity (σ) of 10<sup>5</sup> S/cm. Conductivity is charge times mobility times charge carrier density. With reasonable assumptions | In actual samples there is conductivity (σ) of 10<sup>5</sup> S/cm. Conductivity is charge times mobility times charge carrier density. With reasonable assumptions one can calculate a carrier density of 5 x 10<sup>21</sup> cm<sup>-3</sup> which gives a mobility of μ ~ 100-200 cm<sup>2</sup>/Vs. The best organic semiconductors with three dimensional lattice and low coupling through vibrations have mobilities of 1000s of cm<sup>2</sup>/Vs. | ||
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See Prins 2006 <ref>P. Prins, L. Siebbeles, et al., Physical Review Letters 96, 146601 (2006)</ref> | See Prins 2006 <ref>P. Prins, L. Siebbeles, et al.,"High Intrachain Hole Mobility on Molecular Wires of Ladder-Type Poly(p-Phenylenes)" Physical Review Letters 96, 146601 (2006){{Doi|10.1103/PhysRevLett.96.146601}}</ref> | ||
===Polythiophene film=== | |||
[[Image:PT_film.png|thumb|300px|Stacking in a polythiophene film]] | |||
Polythiophene (PT) is one of the most common polymers used in organic photovoltaics due to its desirable band gap, absorption, compatiblity with C-60, and high performance. | |||
Because of the macrostructure of polymers, conduction is anisotropic. Polythiophene when applied as a film tends to stand on edge so it forms sheets with π-π stacking and is therefore anisotropic. Conduction in polythiphene is greatest in the π-π stacking direction, followed by a slower conduction in the direction aligned with polymer chain, and finally the lowest charge mobility is between the chains where there is a large distance to hop. Therefore to maximize charge mobility we must maximize π-π stacking. People are trying to make longer chains to increase stacking, however increased stacking means the solvent can't penetrate and these are less soluble and have reduced solution processibility. The addition of alkyl chains increases solubility however this decreases the π-π stacking. The challenge is to strike the right balance between performance and ease of solution processing. | |||
=== Polydiacetylene === | === Polydiacetylene === | ||
[[Image:Polydiacetylene.png|thumb|300px|]] | [[Image:Polydiacetylene.png|thumb|300px|Polydiacetylene structure]] | ||
Polydiacetylene crystals have a pattern of double, single, triple, single bonds in their chain. They form perfect crystals when they have bulky side groups like pTS or pFBS. The problem is that because of the bulky side groups chains are pretty far from one another .If you could build a device with a single chain from one electrode to another that would be ideal; the carrier would zip through the chain from one side to another. If the carrier sees a defect it gets stuck because it is difficult to hop to an adjacent chain due to the large distance. Michel Schott has demonstrated macroscopic coherence of a single exciton along an isolated polydiacetylene chain with coherence length over tens of micrometers. These are some of the most perfect π conjugated chains that have been characterized. With a perfect chain the exciton can delocalize across the whole chain forming an exciton band. Polydiacetylene can have and a t along chains of about 2.0 eV. | Polydiacetylene crystals have a pattern of double, single, triple, single bonds in their chain. They form perfect crystals when they have bulky side groups like pTS or pFBS. The problem is that because of the bulky side groups chains are pretty far from one another .If you could build a device with a single chain from one electrode to another that would be ideal; the carrier would zip through the chain from one side to another. If the carrier sees a defect it gets stuck because it is difficult to hop to an adjacent chain due to the large distance. Michel Schott has demonstrated macroscopic coherence of a single exciton along an isolated polydiacetylene chain with coherence length over tens of micrometers. These are some of the most perfect π conjugated chains that have been characterized. With a perfect chain the exciton can delocalize across the whole chain forming an exciton band. Polydiacetylene can have and a t along chains of about 2.0 eV. | ||
See Schott 2006 <ref>M. Schott et al., Nature Physics 2, 32 (2006)</ref> | See Schott 2006 <ref>M. Schott et al., "Macroscopic coherence of a single exciton state in an organic quantum wire" Nature Physics 2, 32 (2006) {{Doi|10.1038/nphys196}}</ref> | ||
=== Carbon nanotubes === | === Carbon nanotubes === | ||
[[Image:Kohlenstoffnanoroehre_Animation.gif|thumb|300px|]] | [[Image:Kohlenstoffnanoroehre_Animation.gif|thumb|300px|A carbon nanotube]] | ||
Carbon nanotubes produce a fairly rigid system because each carbon is bound and little vibration is possible. | Carbon nanotubes produce a fairly rigid system because each carbon is bound and little vibration is possible. | ||
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Ballistic transport over 500 nm long nanotubes has bee measured:~ 80,000-100,000 cm<sup>2</sup>/Vs | Ballistic transport over 500 nm long nanotubes has bee measured:~ 80,000-100,000 cm<sup>2</sup>/Vs | ||
See Durkop 2004 <ref>T. Durkop, S.A. Getty, E. Cobas, and M.S. Fuhrer, NanoLett. 4, 35 (2004)</ref> | See Durkop 2004 <ref>T. Durkop, S.A. Getty, E. Cobas, and M.S. Fuhrer,"Extraordinary Mobility in Semiconducting Carbon Nanotubes" NanoLett. 4, 35 (2004) {{Doi|10.1021/nl034841q}}</ref> | ||
Bulk graphite | Bulk graphite | ||
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Thus, localization energy quickly competes with delocalization energy and the band regime is less easy to sustain upon increasing temperature. | Thus, localization energy quickly competes with delocalization energy and the band regime is less easy to sustain upon increasing temperature. | ||
see [http://www.chemspider.com/ImageView.aspx?id=21782456&mode=3d Jmol version of carbon nanotube] | |||
== References == | == References == | ||
Latest revision as of 15:28, 10 August 2010
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In order have better performance for devices based on electronic semiconductors the charge carrier mobility should be as high a possible and this is accomplished by maximizing the electronic coupling between atoms in a molecule.
Electronic coupling in various molecules
Transpolyacetylene
In perfectly coplanar extended transpolyacetylene chain the electron coupling between adjacent units t (the transfer integral) is on the order of 2.5 – 3eV. Across the entire bandwidth there is 20 eV.
In actual samples there is conductivity (σ) of 105 S/cm. Conductivity is charge times mobility times charge carrier density. With reasonable assumptions one can calculate a carrier density of 5 x 1021 cm-3 which gives a mobility of μ ~ 100-200 cm2/Vs. The best organic semiconductors with three dimensional lattice and low coupling through vibrations have mobilities of 1000s of cm2/Vs.
Ladder polyparaphylenes
Polyacetylenes chains are somewhat floppy and twists could occur along the chain which decrease order in the system. We can prevent twisting in a chain by adding a bridge carbon at every other ring. This completely flat chain is is known as a ladder polyparaphenylene. T along the chain is ~2.0eV.. Usually charge mobility is measured on a large sample and the charge hops from chain to chain, thus the rate limiting step is the one that is ultimately measured. A group in Delft has developed a technique to measure charge mobility based on microwave measurement that is very fast and therefore they can only see the charge moving over a small distance. This allows them to measure what happens on the chain itself. The intrinsic in-chain carrier mobilities estimated for very long chains: m ~ 600 cm2/Vs. This is a good mobility.
See Prins 2006 [1]
Polythiophene film
Polythiophene (PT) is one of the most common polymers used in organic photovoltaics due to its desirable band gap, absorption, compatiblity with C-60, and high performance.
Because of the macrostructure of polymers, conduction is anisotropic. Polythiophene when applied as a film tends to stand on edge so it forms sheets with π-π stacking and is therefore anisotropic. Conduction in polythiphene is greatest in the π-π stacking direction, followed by a slower conduction in the direction aligned with polymer chain, and finally the lowest charge mobility is between the chains where there is a large distance to hop. Therefore to maximize charge mobility we must maximize π-π stacking. People are trying to make longer chains to increase stacking, however increased stacking means the solvent can't penetrate and these are less soluble and have reduced solution processibility. The addition of alkyl chains increases solubility however this decreases the π-π stacking. The challenge is to strike the right balance between performance and ease of solution processing.
Polydiacetylene
Polydiacetylene crystals have a pattern of double, single, triple, single bonds in their chain. They form perfect crystals when they have bulky side groups like pTS or pFBS. The problem is that because of the bulky side groups chains are pretty far from one another .If you could build a device with a single chain from one electrode to another that would be ideal; the carrier would zip through the chain from one side to another. If the carrier sees a defect it gets stuck because it is difficult to hop to an adjacent chain due to the large distance. Michel Schott has demonstrated macroscopic coherence of a single exciton along an isolated polydiacetylene chain with coherence length over tens of micrometers. These are some of the most perfect π conjugated chains that have been characterized. With a perfect chain the exciton can delocalize across the whole chain forming an exciton band. Polydiacetylene can have and a t along chains of about 2.0 eV.
See Schott 2006 [2]
Carbon nanotubes
Carbon nanotubes produce a fairly rigid system because each carbon is bound and little vibration is possible.
t along the chains ~ 2.5 eV
They have exhibited ballistic transport in which the electron moves down the length of the tube without any scattering.
Ballistic transport over 500 nm long nanotubes has bee measured:~ 80,000-100,000 cm2/Vs
See Durkop 2004 [3]
Bulk graphite in bulk graphite: m ~ 15,000 cm2/Vs
These mobilities are greater than any organic semi-conductors. Graphene is a single sheet of graphite which may soon be seen in high performance devices.
See Dressehaus 1996 [4]
In crystalline or well-ordered polymeric materials and nanotubes t along the chains ~ 2.0-3.0 eV
However, in molecular crystals, the relevant electronic coupling is the interchain coupling: t between the chains is one order of magnitude lower or more, that is a few tenths of eV at best.
Thus, localization energy quickly competes with delocalization energy and the band regime is less easy to sustain upon increasing temperature.
see Jmol version of carbon nanotube
References
- ↑ P. Prins, L. Siebbeles, et al.,"High Intrachain Hole Mobility on Molecular Wires of Ladder-Type Poly(p-Phenylenes)" Physical Review Letters 96, 146601 (2006)doi:10.1103/PhysRevLett.96.146601
- ↑ M. Schott et al., "Macroscopic coherence of a single exciton state in an organic quantum wire" Nature Physics 2, 32 (2006) doi:10.1038/nphys196
- ↑ T. Durkop, S.A. Getty, E. Cobas, and M.S. Fuhrer,"Extraordinary Mobility in Semiconducting Carbon Nanotubes" NanoLett. 4, 35 (2004) doi:10.1021/nl034841q
- ↑ M.S. Dresselhaus, G. Dresselhaus, P.C. Eklund, Science of Fullerenes and Carbon Nanotubes; Academic Press: San Diego, 1996
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