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Dielectric Surface-Controlled Low-Voltage Organic Transistors via n-Alkyl Phosphonic Acid Self-Assembled Monolayers on High-k Metal Oxide
被引:99
作者:
Action, By Orb
[1
]
Ting, Guy G.
[2
]
Shamberger, Patrick J.
[1
]
Ohuchi, Fumio S.
[1
]
Ma, Hong
[1
]
Jen, Alex K. -Y.
[1
,2
]
机构:
[1] Univ Washington, Dept Mat Sci & Engn, Seattle, WA 98195 USA
[2] Univ Washington, Dept Chem, Seattle, WA 98195 USA
关键词:
self-assembled monolayer;
organic semiconductor;
organic field-effect transistor;
hybrid materials;
FIELD-EFFECT TRANSISTORS;
THIN-FILM TRANSISTORS;
GATE DIELECTRICS;
STRUCTURAL-CHARACTERIZATION;
MOLECULAR ASSEMBLIES;
EVAPORATED PENTACENE;
CHAIN-LENGTH;
GROWTH;
PERFORMANCE;
MORPHOLOGY;
D O I:
10.1021/am9007648
中图分类号:
TB3 [工程材料学];
学科分类号:
0805 ;
080502 ;
摘要:
In this paper, we report on n-alkyl phosphonic acid (PA) self-assembled monolayer (SAM)/hafnium oxide (HfO2), hybrid dielectrics utilizing the advantages of SAMs for control over the dielectric/semiconductor interface with those of high-h metal oxides for low-voltage organic thin him transistors (OTFTs). By systematically varying the number of carbon atoms of the n-alkyl PA SAM from six to eighteen on HfO2 with stable and low leakage current density, we observe how the structural nature of the SAM affects the thin-film crystal structure and morphology, and subsequent device performance of low-voltage pentacene based OTFTs. We Find chat two primary structural Factors of the SAM play a critical role in optimizing the device electrical characteristics, namely, the order/disorder of the SAM and its physical thickness. High saturation-held-effect mobilities result at a balance between disordered SAMs to promote large pentacene grains and thick SAMs to aid in physically buffering the charge carriers in pentacene from the adverse effects of the underlying high-k oxide. Employing the appropriate n-alkyl PA SAM/HfO2 hybrid dielectrics, pentacene-based OTFTs operate under -2.0 V with low hysteresis, on-off current ratios above 1 x 10(6), threshold voltages below -0.6 V, subthreshold slopes as low as 100 mV dec(-1), and field-effect mobilities as high as 1.8 cm(2) V-1 s(-1).
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页码:511 / 520
页数:10
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