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First Law: Particles in One-dimensional Equilibrium01:10

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Newton's first law of motion states that a body at rest remains at rest, or if in motion, remains in motion at constant velocity, unless acted on by a net external force. It also states that there must be a cause for any change in velocity (a change in either magnitude or direction) to occur. This cause is a net external force. For example, consider what happens to an object sliding along a rough horizontal surface. The object quickly grinds to a halt, due to the net force of friction. If...
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First Law: Particles in Two-dimensional Equilibrium01:18

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Recall that a particle in equilibrium is one for which the external forces are balanced. Static equilibrium involves objects at rest, and dynamic equilibrium involves objects in motion without acceleration; but it is important to remember that these conditions are relative. For instance, an object may be at rest when viewed from one frame of reference, but that same object would appear to be in motion when viewed by someone moving at a constant velocity.
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The Quantum-Mechanical Model of an Atom02:45

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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...
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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,...
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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:
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Force and Potential Energy in One Dimension01:13

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Force can be calculated from the expression for potential energy, which is a function of position. The component of a conservative force, in a particular direction, equals the negative of the derivative of the corresponding potential energy with respect to the displacement in that direction. For regions where potential energy changes rapidly with displacement, the work done and force is maximum. Also, when force is applied along the positive coordinate axis, the potential energy decreases with...
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Related Experiment Video

Updated: Apr 21, 2026

Scalable Quantum Integrated Circuits on Superconducting Two-Dimensional Electron Gas Platform
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Strongly interacting confined quantum systems in one dimension.

A G Volosniev1, D V Fedorov1, A S Jensen1

  • 1Department of Physics and Astronomy, Aarhus University, Ny Munkegade 120, Aarhus C DK-8000, Denmark.

Nature Communications
|November 5, 2014
PubMed
Summary

This study introduces a new technique to solve one-dimensional (1D) quantum systems with strong interactions. It reveals the presence of both ferromagnetic and antiferromagnetic states in small systems, enabling quantum manipulation of magnetic correlations.

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Area of Science:

  • Quantum mechanics
  • Condensed matter physics
  • Atomic physics

Background:

  • The study of one-dimensional (1D) magnetism has a long history, dating back to Bethe's solution of the Heisenberg model.
  • Recent advances in cold atomic gases have led to the realization of 1D systems, such as the Tonks-Girardeau gas, making them a forefront research area.
  • Understanding quantum behavior in 1D systems is crucial for developing new quantum technologies.

Purpose of the Study:

  • To develop a new method for solving 1D fermionic and bosonic systems with strong short-range interactions.
  • To obtain the full spectrum of energies and eigenstates for these systems in arbitrary confining geometries.
  • To investigate the emergence of magnetic correlations in small 1D systems relevant to current experiments.

Main Methods:

  • Introduction of a novel energy-functional technique.
  • Analytical solution for 1D quantum systems with strong short-range interactions.
  • Calculation of spatial correlations to identify magnetic states.

Main Results:

  • The developed method successfully solves 1D fermionic and bosonic systems in arbitrary confining geometries.
  • The full spectrum of energies and eigenstates for these systems has been obtained.
  • Both ferro- and antiferromagnetic states are shown to be present even for small system sizes.

Conclusions:

  • The new energy-functional technique provides a powerful tool for studying 1D quantum magnetism.
  • The findings demonstrate the feasibility of preparing and studying magnetic correlations at the microscopic scale in current experimental setups.
  • This work highlights the significant potential for quantum manipulation of magnetic correlations in 1D systems.