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@ARTICLE{Zhang:851649,
author = {Zhang, Hehe and Yoo, Sijung and Menzel, Stephan and Funck,
Carsten and Cüppers, Felix and Wouters, Dirk J. and Hwang,
Cheol Seong and Waser, R. and Hoffmann-Eifert, Susanne},
title = {{U}nderstanding the {C}oexistence of {T}wo {B}ipolar
{R}esistive {S}witching {M}odes with {O}pposite {P}olarity
in {P}t/{T}i{O} 2 /{T}i/{P}t {N}anosized {R}e{RAM}
{D}evices},
journal = {ACS applied materials $\&$ interfaces},
volume = {10},
number = {35},
issn = {1944-8252},
address = {Washington, DC},
publisher = {Soc.},
reportid = {FZJ-2018-05199},
pages = {29766 - 29778},
year = {2018},
abstract = {Redox-type resistive random access memories based on
transition-metal oxides are studied as adjustable
two-terminal devices for integrated network applications
beyond von Neumann computing. The prevailing, so-called,
counter-eight-wise (c8w) polarity of the switching
hysteresis in filamentary-type valence change mechanism
devices originates from a temperature- and field-controlled
drift-diffusion process of mobile ions, predominantly oxygen
vacancies in the switching oxide. Recently, a bipolar
resistive switching (BRS) process with opposite polarity,
so-called, eight-wise (8w) switching, has been reported
that, especially for TiO2 cells, is still not completely
understood. Here, we report on nanosized (<0.01 μm2)
asymmetric memristive cells from 3 to 6 nm thick TiO2 films
by atomic layer deposition, which reveal a coexistence of
c8w and 8w switching in the same cell. As important
characteristics for the studied Pt/TiO2/Ti/Pt devices, the
resistance states of both modes are nonvolatile and share
one common state; i.e., the high-resistance state of the c8w
mode equals the low-resistance state of the 8w-mode. A
transition between the opposite hysteresis loops is possible
by voltage control. Specifically, 8w BRS in the TiO2 cells
is a self-limited low-energy nonvolatile switching process.
Additionally, the 8w reset process enables the programming
of multilevel high-resistance states. Combining the
experimental results with data from simulation studies
allows to propose a model, which explains 8w BRS by an
oxygen transfer process across the Pt/TiO2 Schottky
interface at the position of the c8w filament. Therefore,
the coexistence of c8w and 8w BRS in the nanoscale
asymmetric Pt/TiO2/Ti/Pt cells is understood from a
competition between drift/diffusion of oxygen vacancies in
the oxide layer and an oxygen exchange reaction across the
Pt/TiO2 interface.},
cin = {PGI-7 / PGI-10 / JARA-FIT},
ddc = {540},
cid = {I:(DE-Juel1)PGI-7-20110106 / I:(DE-Juel1)PGI-10-20170113 /
$I:(DE-82)080009_20140620$},
pnm = {524 - Controlling Collective States (POF3-524)},
pid = {G:(DE-HGF)POF3-524},
typ = {PUB:(DE-HGF)16},
pubmed = {pmid:30088755},
UT = {WOS:000444355700059},
doi = {10.1021/acsami.8b09068},
url = {https://juser.fz-juelich.de/record/851649},
}