IOP PUBLISHING NANOTECHNOLOGY
Nanotechnology 20 (2009) 025201 (5pp) doi:10.1088/0957-4484/20/2/025201
Resistive switching characteristics of
polymer non-volatile memory devices in a
scalable via-hole structure
Tae-Wook Kim, Hyejung Choi, Seung-Hwan Oh,
Minseok Jo, Gunuk Wang, Byungjin Cho,
Dong-Yu Kim, Hyunsang Hwang and Takhee Lee
1
Heeger Center for Advanced Materials, Department of Materials Science and Engineering,
Gwangju Institute of Science and Technology, Gwangju 500-712, Korea
E-mail: tlee@gist.ac.kr
Received 5 August 2008, in final form 9 October 2008
Published 9 December 2008
Online at stacks.iop.org/Nano/20/025201
Abstract
The resistive switching characteristics of polyfluorene-derivative polymer material in a
sub-micron scale via-hole device structure were investigated. The scalable via-hole
sub-microstructure was fabricated using an e-beam lithographic technique. The polymer
non-volatile memory devices varied in size from 40 × 40 μm
2
to 200 × 200 nm
2
. From the
scaling of junction size, the memory mechanism can be attributed to the space–charge-limited
current with filamentary conduction. Sub-micron scale polymer memory devices showed
excellent resistive switching behaviours such as a large ON/OFF ratio ( I
ON
/ I
OFF
∼ 10
4
),
excellent device-to-device switching uniformity, good sweep endurance, and good retention
times (more than 10 000 s). The successful operation of sub-micron scale memory devices of
our polyfluorene-derivative polymer shows promise to fabricate high-density polymer memory
devices.
S Supplementary data are available from stacks.iop.org/Nano/20/025201
(Some figures in this article are in colour only in the electronic version)
1. Introduction
Polymer materials have been developed as active components
in a variety of device applications, such as organic light-
emitting diodes, thin-film transistors, memory devices,
photovoltaic cells, and sensors [1–5]. Among these
applications, polymer non-volatile memory appears highly
attractive, owing to its potential usage in data storage
media [6–12]. In particular, polymer memory devices have
attracted a lot of attention due to their simple structure,
three-dimensional stacking capability, good scalability, high
mechanical flexibility, and low fabrication cost.
Until now, most research on polymer memory devices has
focused on the synthesis of conjugated polymer materials as
memory elements [13–16] or the identification of appropriate
ratios between polymer materials and metallic nanoparticles
in a blend of the two [17–19]. Basic device structures for
1
Author to whom any correspondence should be addressed.
electrical characterizations were typically in the form of unit
devices or cross-bar-type devices in which the active polymer
memory elements were vertically sandwiched between two
metallic electrodes [6–19]. The junction of the polymer
memory devices has mainly been defined by the size of the
shadow mask during the top electrode metallization; thus
it has been hard to reduce the active cell size below the
sub-micron scale. Junctions in sub-micron size have only
been characterized by conducting atomic force microscopy
(CAFM) [20, 21]. However, it is not trivial to evaluate
the detailed memory performance of polymer materials with
CAFM because the possible measurements are limited to
current–voltage ( I –V ) sweeps or current images which are
based on simple contacts or scanning of the conducting tip on
the polymer layer.
The scaling issue has been one of the important research
topics in many emerging memory technologies such as
ferroelectric random access memory (FRAM), magneto-
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