Related Experiment Video
Updated: Apr 12, 2026

09:20
Fabrication of Low Temperature Carbon Nanotube Vertical Interconnects Compatible with Semiconductor Technology
Published on: December 7, 2015
8.2K
Non-volatile Clocked Spin Wave Interconnect for Beyond-CMOS Nanomagnet Pipelines
Sourav Dutta1, Sou-Chi Chang1, Nickvash Kani1
1School of Electrical and Computer Engineering, Georgia Institute of Technology, Atlanta, GA 30332 USA.
Scientific Reports
|May 9, 2015
Summary
This study proposes a novel clocked non-volatile spin wave device for efficient information processing. The design integrates a charge-to-spin converter and magneto-electric repeaters for low-power logic circuits.
Area of Science:
- * Condensed Matter Physics
- * Spintronics
- * Materials Science
Background:
- * Spin waves offer potential for low-power information transmission and processing.
- * Previous spin wave logic circuits explored magneto-electric effects for amplification and switching.
- * Challenges remain in creating efficient, non-volatile spin wave devices.
Purpose of the Study:
- * To propose a comprehensive scheme for a clocked non-volatile spin wave device.
- * To introduce key components: charge-to-spin converter and magneto-electric spin wave repeaters.
- * To ensure the device meets essential logic application requirements.
Main Methods:
- * Integration of a charge-to-spin converter for electrical-to-spin domain translation.
- * Utilization of magneto-electric spin wave repeaters operating in transmitter, memory, and detector regimes.
- * Implementation of a novel clocking scheme for sequential transmission and non-reciprocity.
Main Results:
- * The proposed device design facilitates clocked, non-volatile operation.
- * The device incorporates spin wave repeaters functioning as transmitters, non-volatile memory, and detectors.
- * A novel clocking scheme ensures unidirectional information flow.
Conclusions:
- * The developed spin wave device scheme satisfies key logic requirements: nonlinearity, amplification, concatenability, feedback prevention, and complete Boolean operations.
- * This research advances the development of efficient, low-power spintronic logic devices.
- * The proposed architecture provides a pathway for next-generation computing hardware.
More Related Videos
Related Concept Videos
Non-ohmic Devices
1.7K
In most substances, the current flow is proportional to the voltage applied to it. A simple relationship between the values of current, voltage, and resistance is known as Ohm's law. Nonohmic devices do not exhibit a linear relationship between voltage and current. One such device is the semiconducting circuit element known as a diode. A diode is a circuit device that allows current flow in only one direction.
Consider a simple circuit consisting of a battery, a diode, and a resistor. A...
Consider a simple circuit consisting of a battery, a diode, and a resistor. A...
1.7K
MOSFET: Enhancement Mode
1.0K
Enhancement-mode MOSFETs are pivotal components in electronics, distinguished by their capacity to act as highly efficient switches. They are part of the larger family of metal-oxide Semiconductor Field-Effect Transistors (MOSFETs). They are available in two types: p-channel and n-channel, each tailored to specific polarity operations.
In their basic form, enhancement-mode MOSFETs are typically non-conductive when the gate-source voltage (Vgs) is zero. This default 'off' state means no...
In their basic form, enhancement-mode MOSFETs are typically non-conductive when the gate-source voltage (Vgs) is zero. This default 'off' state means no...
1.0K
MOSFET
1.7K
The Metal-Oxide-Semiconductor Field-Effect Transistor (MOSFET) plays a pivotal role in modern electronics thanks to its versatility and efficiency in controlling electrical currents. This device, also known as IGFET, MISFET, and MOSFET, has three main terminals: the Source, Drain, and Gate. MOSFETs are classified into n-channel or p-channel types based on the doping characteristics of their substrate and the source or drain regions.
In an n-MOSFET, the structure includes n-type source and drain...
In an n-MOSFET, the structure includes n-type source and drain...
1.7K
MOS Capacitor
1.9K
A Metal-Oxide-Semiconductor (MOS) capacitor is a fundamental structure used extensively in semiconductor device technology, particularly in the fabrication of integrated circuits and MOSFETs (metal-oxide-semiconductor field-effect transistors). The MOS capacitor consists of three layers: a metal gate, a dielectric oxide, and a semiconductor substrate.
The metal gate is typically made from highly conductive materials such as aluminum or polysilicon. Beneath the metal gate lies a thin layer of...
The metal gate is typically made from highly conductive materials such as aluminum or polysilicon. Beneath the metal gate lies a thin layer of...
1.9K
Spin–Spin Coupling Constant: Overview
1.7K
In bromoethane, the three methyl protons are coupled to the two methylene protons that are three bonds away. In accordance with the n+1 rule, the signal from the methyl protons is split into three peaks with 1:2:1 relative intensities. The methylene protons appear as a quartet, with the relative intensities of 1:3:3:1.
Qualitatively, any spin plus-half nucleus polarizes the spins of its electrons to the minus-half state. Consequently, the paired electron in the hydrogen–carbon bond must...
Qualitatively, any spin plus-half nucleus polarizes the spins of its electrons to the minus-half state. Consequently, the paired electron in the hydrogen–carbon bond must...
1.7K
Metal-Semiconductor Junctions
1.4K
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...
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...
1.4K

