High charge-carrier mobility and low trap density in a rubrene derivative
| dc.creator | Haas, S. | |
| dc.creator | Stassen, A. F. | |
| dc.creator | Schuck, G. | |
| dc.creator | Pernstich, K. P. | |
| dc.creator | Gundlach, D. J. | |
| dc.creator | Batlogg, B. | |
| dc.creator | Berens, U. | |
| dc.creator | Kirner, H. -J. | |
| dc.date | 2007-07-03 | |
| dc.date.accessioned | 2026-07-07T08:46:17Z | |
| dc.date.available | 2026-07-07T08:46:17Z | |
| dc.description | We have synthesized, crystallized and studied the structural and electric transport properties of organic molecular crystals based on a rubrene derivative with {\em t}-butyl sidegroups at the 5,11 positions. Two crystalline modifications are observed: one (A) distinct from that of rubrene with larger spacings between the naphtacene backbones, the other (B) with a in-plane structure presumably very similar compared to rubrene. The electric transport properties reflect the different structures: in the latter phase (B) the in-plane hole mobility of 12 cm$^2$/Vs measured on single crystal FETs is just as high as in rubrene crystals, while in the A phase no field-effect could be measured. The high crystal quality, studied in detail for B, reflects itself in the density of gap states: The deep-level trap density as low as $10^{15}$ cm$^{-3}$ eV$^{-1}$ has been measured, and an exponential band tail with a characteristic energy of 22 meV is observed. The bulk mobility perpendicular to the molecular planes is estimated to be of order of $10^{-3}$ -- $10^{-1}$ cm$^2$/Vs. | |
| dc.identifier | https://arxiv.org/abs/0707.0461 | |
| dc.identifier | http://arxiv.org/abs/0707.0461 | |
| dc.identifier | Phys. Rev. B 76, 115203 (2007) | |
| dc.identifier | doi:10.1103/PhysRevB.76.115203 | |
| dc.identifier.uri | http://salesiana.dossiersoluciones.com/handle/123456789/143201 | |
| dc.subject | Materials Science | |
| dc.title | High charge-carrier mobility and low trap density in a rubrene derivative | |
| dc.type | text |