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Related Concept Videos

Atomic Nuclei: Nuclear Spin State Population Distribution01:14

Atomic Nuclei: Nuclear Spin State Population Distribution

Near absolute zero temperatures, in the presence of a magnetic field, the majority of nuclei prefer the lower energy spin-up state to the higher energy spin-down state. As temperatures increase, the energy from thermal collisions distributes the spins more equally between the two states. The Boltzmann distribution equation gives the ratio of the number of spins predicted in the spin −½ (N−) and spin +½ (N+) states.
Atomic Nuclei: Nuclear Spin State Overview01:03

Atomic Nuclei: Nuclear Spin State Overview

NMR-active nuclei have energy levels called 'spin states' that are associated with the orientations of their nuclear magnetic moments. In the absence of a magnetic field, the nuclear magnetic moments are randomly oriented, and the spin states are degenerate. When an external magnetic field is applied, the spin states have only 2 + 1 orientations available to them. A proton with = ½ has two available orientations. Similarly, for a quadrupolar nucleus with a nuclear spin value of one, the...
Quantum Numbers02:43

Quantum Numbers

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.
The Pauli Exclusion Principle03:06

The Pauli Exclusion Principle

The arrangement of electrons in the orbitals of an atom is called its electron configuration. We describe an electron configuration with a symbol that contains three pieces of information:
Energy Bands in Solids01:01

Energy Bands in Solids

Isolated atoms have discrete energy levels that are well described by the Bohr model. And, it quantifies the energy of an electron in a hydrogen atom as En. Higher quantum numbers 'n' yield less negative, closer electron energy levels.
 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 that no two...
Interpreting ¹H NMR Signal Splitting: The (n + 1) Rule01:10

Interpreting ¹H NMR Signal Splitting: The (n + 1) Rule

In the AX proton spin system, proton A can sense the two spin states of a coupled proton X, resulting in a doublet NMR signal with two peaks of equal (1:1) intensity. When proton A is coupled to two equivalent protons (AX2 spin system), the spin states of each X can be aligned with or against the external field, creating three possible scenarios. This results in a 1:2:1  triplet signal, where the central peak corresponds to the chemical shift of A and is twice as large or intense as the others.

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Related Experiment Video

Updated: May 24, 2026

Quantum State Engineering of Light with Continuous-wave Optical Parametric Oscillators
09:23

Quantum State Engineering of Light with Continuous-wave Optical Parametric Oscillators

Published on: May 30, 2014

Quantized ν = 5/2 state in a two-subband quantum hall system.

J Nuebler1, B Friess, V Umansky

  • 1Max-Planck-Institute for Solid State Research, Heisenbergstrasse 1, D-70569 Stuttgart, Germany.

Physical Review Letters
|March 10, 2012
PubMed
Summary
This summary is machine-generated.

The fractional quantum Hall state at 5/2 filling persists in wider wells (80, 60 nm) even with two electron subbands occupied. However, it disappears in narrower wells (50 nm) due to subband properties.

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Scalable Quantum Integrated Circuits on Superconducting Two-Dimensional Electron Gas Platform
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Last Updated: May 24, 2026

Quantum State Engineering of Light with Continuous-wave Optical Parametric Oscillators
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Scalable Quantum Integrated Circuits on Superconducting Two-Dimensional Electron Gas Platform
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Scalable Quantum Integrated Circuits on Superconducting Two-Dimensional Electron Gas Platform

Published on: August 2, 2019

Area of Science:

  • Condensed matter physics
  • Quantum Hall effect research
  • Materials science

Background:

  • The fractional quantum Hall effect (FQHE) is a key phenomenon in two-dimensional electron systems (2DES).
  • Understanding the FQHE at the 5/2 filling factor is crucial for exploring non-Abelian states.
  • The influence of subband occupancy on FQHE states is not fully understood.

Purpose of the Study:

  • To investigate the behavior of the fractional quantum Hall state at 5/2 filling.
  • To explore the transition from single- to two-subband occupancy in 2DES.
  • To determine the impact of well width on the 5/2 FQHE state.

Main Methods:

  • Utilizing density-tunable 2DES in wide quantum wells of varying widths (80, 60, and 50 nm).
  • Inducing transitions between single- and two-subband electron occupancy.
  • Observing and analyzing the quantum Hall state at 5/2 filling.

Main Results:

  • The 5/2 FQHE state is observed in 80 and 60 nm wells even with second subband occupation.
  • The 5/2 FQHE state vanishes in a 50 nm well when the second subband becomes populated.
  • This behavior is dependent on the quantum well width.

Conclusions:

  • The stability of the 5/2 FQHE state is sensitive to quantum well width.
  • Inter-subband coupling, influenced by capacitive energy and wavefunction overlap, dictates the 5/2 state's persistence.
  • Further research into 2DES in tailored quantum wells is warranted for FQHE studies.