Related Experiment Video
Updated: Jun 5, 2026

10:40
A Fabrication and Measurement Method for a Flexible Ferroelectric Element Based on Van Der Waals Heteroepitaxy
Published on: April 8, 2018
Organic multiferroic tunnel junctions with ferroelectric poly(vinylidene fluoride) barriers
Juan M López-Encarnación1, J D Burton, Evgeny Y Tsymbal
1Department of Physics, Institute for Functional Nanomaterials, University of Puerto Rico, San Juan, Puerto Rico 00931.
Nano Letters
|December 24, 2010
Summary
Organic ferroelectrics like PVDF offer new control in spintronics. These materials enable multiple resistance states in magnetic tunnel junctions for advanced electronics and data storage.
Area of Science:
- Materials Science
- Condensed Matter Physics
- Organic Electronics
Background:
- Organic materials offer advantages for spintronics, including long spin-relaxation times and cost-effectiveness.
- Current research primarily uses nonpolar organic dielectrics/semiconductors as passive components in spin devices.
Purpose of the Study:
- To explore the use of organic ferroelectrics as active barriers in magnetic tunnel junctions (MTJs).
- To investigate the control of spin polarization using ferroelectric polarization in organic barriers.
Main Methods:
- Utilized first-principles calculations based on density functional theory (DFT).
- Investigated spin-resolved conductance in model Co/PVDF/Co and Co/PVDF/Fe/Co MTJs.
Main Results:
- Demonstrated that organic ferroelectric barriers enable new functionalities in MTJs.
- Observed multiple resistance states dependent on electrode magnetization and ferroelectric polarization.
- Co/PVDF/Co and Co/PVDF/Fe/Co MTJs exhibit tunable spin polarization.
Conclusions:
- Organic ferroelectrics, specifically PVDF, can be effectively used as active barriers in MTJs.
- This approach offers a novel route for organic spintronics.
- Potential applications include low-power electronics and nonvolatile data storage devices.
Related Concept Videos
Metal-Semiconductor Junctions
The contact of metal and semiconductor can lead to the formation of a junction with either Schottky or Ohmic behavior.
Schottky Barriers
Schottky barriers arise when a metal with a work function (Φm) contacts a semiconductor with a different work function (Φs). Initially, electrons transfer until the Fermi levels of the metal and semiconductor align at equilibrium. For instance, if Φm > Φs, the semiconductor Fermi level is higher than the metal's before contact. The semiconductor's...
Schottky Barriers
Schottky barriers arise when a metal with a work function (Φm) contacts a semiconductor with a different work function (Φs). Initially, electrons transfer until the Fermi levels of the metal and semiconductor align at equilibrium. For instance, if Φm > Φs, the semiconductor Fermi level is higher than the metal's before contact. The semiconductor's...
Biasing of Metal-Semiconductor Junctions
Biasing metal-semiconductor junctions involves applying a voltage across the junction. Specifically, the metal is connected to a voltage source, while the semiconductor is grounded. This technique is essential for controlling the direction and magnitude of current flow in electronic devices, including diodes, transistors, and photovoltaic cells.
In Schottky junctions, where the semiconductor is n-type, applying a positive voltage to the metal relative to the semiconductor reduces its Fermi...
In Schottky junctions, where the semiconductor is n-type, applying a positive voltage to the metal relative to the semiconductor reduces its Fermi...
Field Effect Transistor
Field-effect transistors (FETs) are integral to electronic circuits and distinguished by their three-terminal setup: the gate, drain, and source. These transistors operate as unipolar devices, which utilize either electrons or holes as charge carriers, in contrast to bipolar transistors, which use both types of carriers. The primary function of the FET is to modulate the flow of these carriers from the source to the drain through a channel. The voltage difference between the gate and source...
Biasing of FET
Biasing a Junction Field Effect Transistor (JFET) is crucial for setting operational parameters and ensuring efficient functioning in electronic circuits. JFETs are characterized by using a single carrier type in N-channel or P-channel configurations, where the channel is surrounded by PN junctions. These junctions are central to the device's ability to control current flow.
In an N-channel JFET, the structure consists of N-type material forming the channel on a P-type substrate, with the gate...
In an N-channel JFET, the structure consists of N-type material forming the channel on a P-type substrate, with the gate...
P-N junction
A p-n junction is formed when p-type and n-type semiconductor materials are joined together. At the interface of the p-n junction, holes from the p-side and electrons from the n-side begin to diffuse into the opposite sides due to the concentration gradient. This diffusion of carriers leads to a region around the junction where there are no free charge carriers, known as the depletion region. The charge density within the depletion region for the n-side and p-side can be described by the...
Schottky Barrier Diode
Schottky barrier diodes are specialized semiconductor devices characterized by their unique construction. This construction involves combining a metal layer with a moderately doped n-type semiconductor material. This combination leads to the formation of a Schottky barrier, a pivotal element that defines the diode's operational characteristics. The core functionality of Schottky barrier diodes is their capacity to allow current to flow in only one direction due to their distinctive...

