Related Experiment Video
Updated: Oct 20, 2025

Ohmic Contact Fabrication Using a Focused-ion Beam Technique and Electrical Characterization for Layer Semiconductor Nanostructures
Published on: December 5, 2015
High and Anomalous Thermal Conductivity in Monolayer MSi2Z4 Semiconductors
Yan Yin1, Min Yi1,2, Wanlin Guo1
1State Key Lab of Mechanics and Control of Mechanical Structures & Key Lab for Intelligent Nano Materials and Devices of Ministry of Education & Institute for Frontier Science &Institute of Nanoscience & College of Aerospace Engineering, Nanjing University of Aeronautics and Astronautics (NUAA), Nanjing 210016, China.
Abstract:
The lattice thermal conductivity (κ) of a newly synthesized two-dimensional (2D) MoSi2N4 family and its associated abnormality are anatomized by ab initio phonon Boltzmann transport calculations. κ of MoSi2N4 and WSi2N4 is found to be over 400 W m-1 K-1 at 300 K. κ of MoSi2Z4 (Z = N, P, As) obeys Slack's rule of thumb, decreasing by 1 order of magnitude from Z = N to Z = As with 46 W m-1 K-1. However, in MSi2N4 (M = Mo, Cr, W, Ti, Zr, Hf), the variation of κ with respect to M is anomalous, that is, deviating from Slack's classic rule. For M in the same group, κ of MSi2N4 is insensitive to the average atomic mass, Debye temperature, phonon group velocity, and bond strength owing to the similar phonon structure and scattering rates. MSi2N4 with heavy group-VIB M even possesses a 3-4 times higher κ than that with light group-IVB M due to its much stronger M-N and exterior Si-N bonds and thus 1 order of magnitude lower phonon scattering rates. Nevertheless, this abnormality could be traced to an interplay of certain basic vibrational properties including the bunching strength and flatness of acoustic branches and their nearby optical branches, which lie outside of the conventional guidelines by Slack. This work predicts high κ of 2D MSi2Z4 for thermal management and provides microscopic insights into deciphering the anomalous κ of layered 2D structures.
Related Concept Videos
Semiconductors
Metals such as copper (Cu), zinc (Zn), or lead (Pb) have low resistivity and feature conduction bands that are either not fully occupied or overlap with the valence band, making a bandgap non-existent. This allows electrons in the highest energy levels of the valence band to easily transition to the conduction band upon gaining...
Types of Semiconductors
Metal-Semiconductor Junctions
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...
Biasing of Metal-Semiconductor Junctions
In Schottky junctions, where the semiconductor is n-type, applying a positive voltage to the metal relative to the semiconductor reduces its Fermi...
Fermi Level Dynamics
Electron affinity in semiconductors refers to the energy gap between the minimum of its conduction band and the vacuum level and it is a critical parameter in determining how easily a semiconductor can accept additional electrons.
The work...
Superconductor

