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Induced Electric Dipoles01:29

Induced Electric Dipoles

A permanent electric dipole orients itself along an external electric field. This rotation can be quantified by defining the potential energy because the external torque does work in rotating it. Then, the potential energy is minimum at the parallel configuration and maximum at the antiparallel configuration. While the former is a stable equilibrium, the latter is an unstable equilibrium.
Since the absolute value of potential energy holds no physical meaning, its zero value can be chosen as per...
Atomic Nuclei: Nuclear Relaxation Processes01:23

Atomic Nuclei: Nuclear Relaxation Processes

In the absence of an external magnetic field, nuclear spin states are degenerate and randomly oriented. When a magnetic field is applied, the spins begin to precess and orient themselves along (lower energy) or against (higher energy) the direction of the field. At equilibrium, a slight excess population of spins exists in the lower energy state. Because the direction of the magnetic field is fixed as the z-axis,  the precessing magnetic moments are randomly oriented around the z-axis. This...
Atomic Orbitals02:44

Atomic Orbitals

An atomic orbital represents the three-dimensional regions in an atom where an electron has the highest probability to reside. The radial distribution function indicates the total probability of finding an electron within the thin shell at a distance r from the nucleus. The atomic orbitals have distinct shapes which are determined by l, the angular momentum quantum number. The orbitals are often drawn with a boundary surface, enclosing densest regions of the cloud.
Electric Dipoles and Dipole Moment01:30

Electric Dipoles and Dipole Moment

Consider two charges of equal magnitude but opposite signs. If they cannot be separated by an external electric field, the system is called a permanent dipole. For example, the water molecule is a dipole, making it a good solvent.
Theoretically, studying electric dipoles leads to understanding why the resultant electric forces around us are weak. Since electric forces are strong, remnant net charges are rare. Hence, the interaction between dipoles helps us understand electrical interactions in...
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.
Mass Analyzers: Common Types01:19

Mass Analyzers: Common Types

The quadrupole mass analyzer consists of four cylindrical metal rods arranged in a diamond carrying a DC voltage and a radio-frequency AC voltage. The motion of ions through the quadrupole depends on the field strength, causing only ions of a certain m/z to resonate successfully and strike the detector at a given field strength. Though the transmission rate for these analyzers is high, the exact elemental composition of the sample is not determined because of low resolution; however, they are...

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Related Experiment Video

Updated: Jul 16, 2026

Experimental Methods for Trapping Ions Using Microfabricated Surface Ion Traps
11:45

Experimental Methods for Trapping Ions Using Microfabricated Surface Ion Traps

Published on: August 17, 2017

Radial and angular rotons in trapped dipolar gases.

Shai Ronen1, Daniele C E Bortolotti, John L Bohn

  • 1JILA and Department of Physics, University of Colorado, Boulder, Colorado 80309-0440, USA.

Physical Review Letters
|March 16, 2007
PubMed
Summary

Bose-Einstein condensates with dipolar interactions become unstable at high particle numbers. This instability is analogous to the roton-maxon instability, leading to unique biconcave shapes and angular roton excitations.

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Related Experiment Videos

Last Updated: Jul 16, 2026

Experimental Methods for Trapping Ions Using Microfabricated Surface Ion Traps
11:45

Experimental Methods for Trapping Ions Using Microfabricated Surface Ion Traps

Published on: August 17, 2017

Cooling an Optically Trapped Ultracold Fermi Gas by Periodical Driving
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Cooling an Optically Trapped Ultracold Fermi Gas by Periodical Driving

Published on: March 30, 2017

Spatial Separation of Molecular Conformers and Clusters
10:37

Spatial Separation of Molecular Conformers and Clusters

Published on: January 9, 2014

Area of Science:

  • Quantum physics
  • Condensed matter physics

Background:

  • Bose-Einstein condensates (BECs) are quantum states of matter formed by cooling bosons to near absolute zero.
  • Dipolar interactions in BECs introduce long-range, anisotropic forces that significantly influence their properties.
  • Previous studies identified roton-maxon instabilities in 2D systems, but their behavior in trapped 3D systems with dipolar interactions is less understood.

Purpose of the Study:

  • To investigate the stability of Bose-Einstein condensates with purely dipolar interactions confined in oblate traps.
  • To analyze the nature of instabilities and emergent phenomena in these systems.
  • To explore the conditions leading to non-central density distributions and their subsequent instabilities.

Main Methods:

  • Theoretical modeling of Bose-Einstein condensates with purely dipolar interactions.
  • Numerical simulations of condensate wave functions in oblate traps.
  • Analysis of energy spectra and stability criteria.

Main Results:

  • Condensates become unstable to collapse at sufficiently large particle numbers.
  • The observed instability is identified as the trapped-gas analogue of the 2D roton-maxon instability.
  • Under specific conditions, condensate wave functions exhibit a biconcave shape, with peak density displaced from the center.
  • These biconcave condensates are susceptible to azimuthal excitations, termed angular rotons.

Conclusions:

  • Dipolar Bose-Einstein condensates in oblate traps exhibit a critical particle number beyond which they become unstable.
  • The roton-maxon instability plays a crucial role in the dynamics of these trapped condensates.
  • The formation of biconcave density profiles and subsequent angular roton instabilities represent novel phenomena in BEC physics.