2016
DOI: 10.1063/1.4963180
|View full text |Cite
|
Sign up to set email alerts
|

Kinetic Monte Carlo of transport processes in Al/AlOx/Au-layers: Impact of defects

Abstract: Ultrathin films of alumina were investigated by a compact kMC-model. Experimental jV-curves from Al/AlOx/Au-junctions with plasma- and thermal-grown AlOx were fitted by simulated ones. We found dominant defects at 2.3-2.5 eV below CBM for AlOx with an effective mass mox∗=0.35 m0 and a barrier EB,Al/AlOx≈2.8 eV in agreement with literature. The parameterization is extended to varying defect levels, defect densities, injection barriers, effective masses and the thickness of AlOx. Thus, dominant charge transport … Show more

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
1
1

Citation Types

0
2
0

Year Published

2019
2019
2023
2023

Publication Types

Select...
5

Relationship

0
5

Authors

Journals

citations
Cited by 6 publications
(2 citation statements)
references
References 44 publications
0
2
0
Order By: Relevance
“…Note that the average energy of the charge traps located near the anode is lower since the electrons are attracted to the anode. At charging voltages exceeding Vth electrons can tunnel into localized trap sites with the energy below the Fermi level, i.e., only those which are located close to the anode [31,32] (Figure 5(b)). Thus, the field emission effect produces a strongly nonuniform distribution: More charges are injected into the region near the anode while the region near the cathode is completely depleted of extra electrons since the electrons cannot tunnel in the traps in that region, since the energy of such traps is higher.…”
Section: Discussionmentioning
confidence: 99%
“…Note that the average energy of the charge traps located near the anode is lower since the electrons are attracted to the anode. At charging voltages exceeding Vth electrons can tunnel into localized trap sites with the energy below the Fermi level, i.e., only those which are located close to the anode [31,32] (Figure 5(b)). Thus, the field emission effect produces a strongly nonuniform distribution: More charges are injected into the region near the anode while the region near the cathode is completely depleted of extra electrons since the electrons cannot tunnel in the traps in that region, since the energy of such traps is higher.…”
Section: Discussionmentioning
confidence: 99%
“…The electrode-limited conduction mechanism, widely applied in metal/insulator/metal (MIM) devices, depends on the electrical properties at the electrode and dielectric contact. The key parameters in this mechanism are the barrier height at the electrode and dielectric interface as well as the effective mass of the conducting carrier in the dielectric film. Therefore, the thickness of the insulating film in this device is inevitably limited to a few nanometers, and because the charge carriers instantaneously move to the opposite electrode because of the quantum tunnel effect, it is difficult to control the direction and the magnitude of the current. …”
Section: Introductionmentioning
confidence: 99%