Related Experiment Video
Updated: Feb 15, 2026

09:23
Quantum State Engineering of Light with Continuous-wave Optical Parametric Oscillators
Published on: May 30, 2014
15.1K
Quantum anomalous Hall-quantum spin Hall effect in optical superlattices.
Optics Letters
|January 13, 2018
Summary
Researchers explored topological properties of spin-orbital coupling particles in 1D optical superlattices. They discovered coexisting quantum anomalous Hall (QAH) and quantum spin Hall (QSH) phases in different bandgaps, enabling simultaneous observation.
Area of Science:
- Condensed Matter Physics
- Quantum Mechanics
- Materials Science
Background:
- Topological phases of matter are crucial for quantum technologies.
- Simulating higher-dimensional topological phenomena in lower dimensions is a key challenge.
- Spin-orbital coupling and Zeeman fields introduce rich quantum behaviors.
Purpose of the Study:
- To investigate the topological characteristics of spin-orbital coupling particles in 1D optical superlattices.
- To explore the potential for simulating 2D topological phases using a 1D system.
- To identify conditions for the coexistence of distinct topological phases.
Main Methods:
- Utilizing 1D optical superlattices with tunable phase shifts to create a virtual 2D system.
- Applying a Zeeman field to manipulate spin properties.
- Analyzing the system's phase diagram for quantum phase transitions.
Main Results:
- The system exhibits a variety of quantum phase transitions across a wide parametric space.
- Two distinct topological phases, quantum anomalous Hall (QAH) and quantum spin Hall (QSH), were found to coexist.
- These QAH and QSH phases reside in separate bandgaps, demonstrating gap-dependent topological behavior.
Conclusions:
- A novel category of gap-dependent QAH-QSH insulator has been identified.
- This work provides a platform for observing the simultaneous occurrence of QSH and QAH effects.
- The findings open new avenues for designing and realizing exotic topological states of matter.
Related Concept Videos
Quantum Numbers
52.4K
It is said that the energy of an electron in an atom is quantized; that is, it can be equal only to certain specific values and can jump from one energy level to another but not transition smoothly or stay between these levels.
52.4K
The Hall Effect
4.5K
Edwin H. Hall, in the year 1879, devised an experiment that could be used to identify the polarity of the predominant charge carriers in a conducting material. From a historical perspective, this experiment was the first to demonstrate that the charge carriers in most metals are negative.
4.5K
The Quantum-Mechanical Model of an Atom
59.8K
Shortly after de Broglie published his ideas that the electron in a hydrogen atom could be better thought of as being a circular standing wave instead of a particle moving in quantized circular orbits, Erwin Schrödinger extended de Broglie’s work by deriving what is now known as the Schrödinger equation. When Schrödinger applied his equation to hydrogen-like atoms, he was able to reproduce Bohr’s expression for the energy and, thus, the Rydberg formula governing hydrogen spectra.
59.8K
2D NMR: Heteronuclear Single-Quantum Correlation Spectroscopy (HSQC)
1.5K
Heteronuclear single-quantum correlation spectroscopy (HSQC) is a 2D NMR technique that reveals one-bond correlations between hydrogen and a heteronucleus. The HSQC experiment is similar to the heteronuclear correlation experiment (HETCOR) but is more sensitive. In the HSQC spectrum, the proton chemical shift is plotted on the horizontal F2 axis, while the 13C chemical shift is plotted on the vertical F1 axis. The corresponding proton and 13C spectra are also shown. The HSQC contour plot does...
1.5K
NMR Spectroscopy: Spin–Spin Coupling
3.3K
The spin state of an NMR-active nucleus can have a slight effect on its immediate electronic environment. This effect propagates through the intervening bonds and affects the electronic environments of NMR-active nuclei up to three bonds away; occasionally, even farther. This phenomenon is called spin–spin coupling or J-coupling. Coupling interactions are mutual and result in small changes in the absorption frequencies of both nuclei involved. While nuclei of the same element are involved...
3.3K
Spin–Spin Coupling: One-Bond Coupling
1.5K
Coupling interactions are strongest between NMR-active nuclei bonded to each other, where spin information can be transmitted directly through the pair of bonding electrons. While nuclei polarize their electrons to the opposite spins, the bonding electron pair has opposite spins. Configurations with antiparallel nuclear spins are expected to be lower in energy. When coupling makes antiparallel states more favorable, J is considered to have a positive value. The one-bond coupling constant, 1J,...
1.5K

