Organic molecular films on gold versus conducting polymer: Influence of injection barrier height and morphology on current–voltage characteristics

2003 ◽  
Vol 82 (14) ◽  
pp. 2281-2283 ◽  
Author(s):  
N. Koch ◽  
A. Elschner ◽  
J. Schwartz ◽  
A. Kahn
2018 ◽  
Vol 25 (04) ◽  
pp. 1850082 ◽  
Author(s):  
NEZIR YILDIRIM ◽  
ABDULMECIT TURUT ◽  
HULYA DOGAN

The Schottky barrier type Ni/[Formula: see text]-GaAs contacts fabricated by us were thermally annealed at 600[Formula: see text]C and 700[Formula: see text]C for 1[Formula: see text]min. The apparent barrier height [Formula: see text] and ideality factor of the diodes were calculated from the forward bias current–voltage characteristic in 60–320[Formula: see text]K range. The [Formula: see text] values for the nonannealed and 600[Formula: see text]C and 700[Formula: see text]C annealed diodes were obtained as 0.80, 0.81 and 0.67[Formula: see text]eV at 300[Formula: see text]K, respectively. Thus, it has been concluded that the reduced barrier due to the thermal annealing at 700[Formula: see text]C promises some device applications. The current preferentially flows through the lowest barrier height (BH) with the temperature due to the BH inhomogeneities. Therefore, it was seen that the [Formula: see text] versus [Formula: see text] plots for the nonannealed and annealed diodes showed the linear behavior according to Gaussian distributions.


2006 ◽  
Vol 961 ◽  
Author(s):  
Hideo Kaiju ◽  
Kenji Kondo ◽  
Akira Ishibashi

ABSTRACTWe calculated transport properties of edge-to-edge quantum cross structure that consists of two metal nano-ribbons having edge-to-edge configuration with a tunnel barrier and showed current-voltage characteristics depending on the metal-ribbon thickness (5-30 nm), the barrier height (0.5-1.5 eV) and the barrier thickness (0.5-1.0 nm). Interesting behavior of transport properties is that the metal-ribbon thickness affects the current density due to the quantization of nano-ribbon and also the current density, being dependent on the barrier height and the barrier thickness, decreases with high and thick barrier. These calculated results indicate that we can precisely obtain the information on the material sandwiched between two electrodes, such as the barrier height and the barrier thickness, by a fit of experimental data to our derived equation, and these approaches result in a distinction between the sandwiched material and the electrode.


2016 ◽  
Vol 858 ◽  
pp. 1170-1173 ◽  
Author(s):  
Giuseppe Greco ◽  
Ferdinando Iucolano ◽  
Filippo Giannazzo ◽  
Salvatore di Franco ◽  
Domenico Corso ◽  
...  

In this paper, the electrical properties of different metal/p-GaN contacts (Ti/Al, TiN/Ti/Al and Ni/Au) have been investigated to get a deeper understanding of the behavior of p-GaN/AlGaN/GaN heterostructures for normally-off HEMTs. In particular, the study of the temperature dependent current-voltage characteristics allowed to identify the dominant carrier transport mechanism at the metal/p-GaN interface (Thermionic Field Emission). From the fit of the experimental current-voltage data it was possible to determine the Schottky barrier height values for the three systems, 2.08 eV (Ti/Al), 1.57 eV (TiN/Ti/Al) and 1.89 eV (Ni/Au). Hence, choosing the highest barrier height contact (Ti/Al) as gate electrode on a p-GaN/AlGaN/GaN heterostructure, optimized based on simulations, allowed to obtain devices with a normally-off behavior and a positive Vth of +1.3 V.


2009 ◽  
Vol 42 (16) ◽  
pp. 165104 ◽  
Author(s):  
Yow-Jon Lin ◽  
Bo-Chieh Huang ◽  
Yi-Chun Lien ◽  
Ching-Ting Lee ◽  
Chia-Lung Tsai ◽  
...  

2000 ◽  
Vol 660 ◽  
Author(s):  
Serkan Zorba ◽  
Neil J. Watkins ◽  
Li Yan ◽  
Yongli Gao

ABSTRACTCurrent-voltage characteristics of organic semiconductor pentacene were studied as a function of applied tip force using conducting probe atomic force microscope. I-V measurements were performed on 150Å and 300Å pentacene films. No electrical contact was observed until 20 nN of tip force for the 150Å film coverage, whereas electrical contact was established easily with a few nN of tip force values for the 300Å film coverage. On both films, once an electrical contact was obtained, the conductance was observed to increase with increasing load. At about 50 nN and higher loads we lost electrical contact in both cases in a reproducible manner. While I-V on 150Å pentacene film showed a rectifying behavior, I-V on 300Å pentacene looked like typical I-V curves of tunneling phenomenon. From these measurements, we have estimated a hole injection barrier of about 0.76 eV and a band gap of about 2.00 eV for pentacene. These results are in agreement with those in the literature.


2015 ◽  
Vol 36 (12) ◽  
pp. 124002 ◽  
Author(s):  
Kamal Zeghdar ◽  
Lakhdar Dehimi ◽  
Achour Saadoune ◽  
Nouredine Sengouga

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