Related Experiment Video
Updated: Jul 5, 2025

Probe Type II Band Alignment in One-Dimensional Van Der Waals Heterostructures Using First-Principles Calculations
Published on: October 12, 2019
Second order topology in a band engineered Chern insulator
Srijata Lahiri1, Saurabh Basu2
1Department of Physics, Indian Institute of Technology Guwahati, Guwahati, Assam, 781039, India. srijata.lahiri@iitg.ac.in.
We explore topological phases in a modified Haldane model, identifying a topological insulator and a second-order topological insulator. The study reveals distinct topological properties and the emergence of corner modes in the second-order phase.
Area of Science:
- Condensed Matter Physics
- Topological Materials
- Solid-State Physics
Background:
- The Haldane model describes a topological insulator with quantized Hall conductance without magnetic fields.
- Honeycomb lattices are crucial for realizing novel electronic properties.
Purpose of the Study:
- To investigate topological phase transitions in a deformed Haldane model.
- To characterize the properties of topological and second-order topological insulator phases.
- To analyze the impact of breaking time-reversal symmetry on topological states.
Main Methods:
- Smoothly deforming the Haldane model by varying a nearest-neighbor hopping parameter.
- Analyzing Berry curvature and Chern number evolution.
- Calculating Wannier charge center evolution.
- Diagonalizing the real-space Hamiltonian on a supercell.
Main Results:
- Identified two distinct topological phases: a topological insulator (TI) and a second-order topological insulator (SOTI).
- Observed a shift of Dirac cones and quantized Chern numbers (C=1) in the TI phase.
- Discovered in-gap zero-energy corner modes in the SOTI phase, characterized by quantized polarizations.
Conclusions:
- The deformed Haldane model hosts both TI and SOTI phases with distinct topological invariants.
- The SOTI phase exhibits quantized polarization and zero Berry curvature, analogous to the 2D Su-Schrieffer-Heeger model.
More Related Videos
10:35Using Microwave and Macroscopic Samples of Dielectric Solids to Study the Photonic Properties of Disordered Photonic Bandgap Materials
Published on: September 26, 2014
05:39Scalable Quantum Integrated Circuits on Superconducting Two-Dimensional Electron Gas Platform
Published on: August 2, 2019
Related Concept Videos
Band Theory
The energy difference between these bands is known as the band gap.
Conductor, Semiconductor,...
Energy Bands in Solids
Band Formation:
When atoms are brought close together, as in a solid, these discrete energy levels begin to split due to the overlap of electron orbitals from adjacent atoms. This split occurs because of the Pauli exclusion principle, which states...
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...
Second-Order Circuits
Input signals typically originate from voltage or current sources, with the output often representing voltage across the capacitor and/or current through the inductor. For example, in...
¹H NMR: Interpreting Distorted and Overlapping Signals
As Δν decreases and the signals move closer, the doublets appear increasingly distorted. The intensities of the inner lines increase at the cost of those of the outer lines as the signals are...
Fermi Level
At absolute zero temperature, electrons fill all energy states up to the Fermi level, leaving upper states empty. As the temperature rises,...