Related Experiment Video
Updated: May 18, 2026

10:00
Gradient Echo Quantum Memory in Warm Atomic Vapor
Published on: November 11, 2013
Bose-Einstein condensation of erbium
1Institut für Experimentalphysik and Zentrum für Quantenphysik, Universität Innsbruck, Innsbruck, Austria.
Physical Review Letters
|September 26, 2012
Summary
Researchers achieved Bose-Einstein condensation in erbium atoms, observing magnetic Feshbach resonances. This breakthrough enables tunable dipolar Bose-Einstein condensates and offers insights into quantum physics.
Area of Science:
- Atomic physics
- Quantum optics
- Condensed matter physics
Background:
- Bose-Einstein condensation (BEC) is a quantum state of matter.
- Erbium (Er) atoms are magnetically complex, making BEC challenging.
- Feshbach resonances are crucial for controlling atomic interactions.
Purpose of the Study:
- To achieve Bose-Einstein condensation of erbium atoms.
- To investigate magnetic Feshbach resonances in erbium.
- To demonstrate the creation of tunable dipolar Bose-Einstein condensates.
Main Methods:
- Evaporative cooling in an optical dipole trap.
- Production of pure 168Er Bose-Einstein condensates.
- Feshbach spectroscopy to identify loss resonances.
Main Results:
- Achieved pure Bose-Einstein condensates of up to 7x10^4 erbium atoms.
- Observed six magnetic Feshbach resonances within a 3 G magnetic field range.
- Demonstrated a tunable dipolar Bose-Einstein condensate using a low-field resonance.
Conclusions:
- Bose-Einstein condensation of erbium atoms is feasible.
- Erbium atoms exhibit a rich Feshbach resonance spectrum at low fields.
- Tunable dipolar Bose-Einstein condensates can be created, showing characteristic d-wave collapse.
Related Concept Videos
Electron Paramagnetic Resonance (EPR) Spectroscopy: Organic Radicals
Ideally, an unpaired electron shows a single peak in the EPR spectrum due to the transition between the two spin energy states. However, coupling interactions can occur between the spins of the unpaired electron and any neighboring spin-active nuclei. This hyperfine coupling results in hyperfine splitting, where the EPR signal is split into multiplets. The signals split into 2nI + 1 peaks, where n is the number of equivalent nuclei and I is the nuclear spin. These splitting patterns provide...
Atomic Emission Spectroscopy: Overview
Atomic emission spectroscopy (AES) is an analytical technique used to determine the elemental composition of a sample by analyzing the light emitted from excited atoms. In AES, atoms in a sample are excited to higher energy levels by thermal energy from high-temperature sources, such as plasma, arcs, or sparks. When these excited atoms return to lower energy states, they emit light at specific wavelengths characteristic of each element. The resulting atomic emission spectrum, which consists of...
Electron Configuration of Multielectron Atoms
The alkali metal sodium (atomic number 11) has one more electron than the neon atom. This electron must go into the lowest-energy subshell available, the 3s orbital, giving a 1s22s22p63s1 configuration. The electrons occupying the outermost shell orbital(s) (highest value of n) are called valence electrons, and those occupying the inner shell orbitals are called core electrons. Since the core electron shells correspond to noble gas electron configurations, we can abbreviate electron...
The de Broglie Wavelength
In the macroscopic world, objects that are large enough to be seen by the naked eye follow the rules of classical physics. A billiard ball moving on a table will behave like a particle; it will continue traveling in a straight line unless it collides with another ball, or it is acted on by some other force, such as friction. The ball has a well-defined position and velocity or well-defined momentum, p = mv, which is defined by mass m and velocity v at any given moment. This is the typical...
The Bohr Model
Following the work of Ernest Rutherford and his colleagues in the early twentieth century, the picture of atoms consisting of tiny dense nuclei surrounded by lighter and even tinier electrons continually moving about the nucleus was well established. This picture was called the planetary model since it pictured the atom as a miniature “solar system” with the electrons orbiting the nucleus like planets orbiting the sun. The simplest atom is hydrogen, consisting of a single proton as the nucleus...
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...

