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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...
Atomic Nuclei: Nuclear Magnetic Moment00:59

Atomic Nuclei: Nuclear Magnetic Moment

All atomic nuclei are positively charged. When they have a nonzero spin, they behave like rotating charges. As a consequence of their charge and spin, these nuclei generate a magnetic field (B). This, in turn, gives rise to a magnetic moment (μ), which is randomly oriented in the absence of an external magnetic field. When an external magnetic field (B0) is applied, the magnetic moment vectors can align with the field or against it in 2 + 1 orientations. A hydrogen nucleus, which is just a...
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...
The Bohr Model02:18

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...
Nuclear Stability03:18

Nuclear Stability

Protons and neutrons, collectively called nucleons, are packed together tightly in a nucleus. With a radius of about 10−15 meters, a nucleus is quite small compared to the radius of the entire atom, which is about 10−10 meters. Nuclei are extremely dense compared to bulk matter, averaging 1.8 × 1014 grams per cubic centimeter. If the earth’s density were equal to the average nuclear density, the earth’s radius would be only about 200 meters.
To hold positively charged protons together in the...

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Preparing an Isotopically Pure 229Th Ion Beam for Studies of 229mTh
10:42

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Published on: May 3, 2019

Trapped antihydrogen in its ground state.

G Gabrielse1, R Kalra, W S Kolthammer

  • 1Department of Physics, Harvard University, Cambridge, Massachusetts 02138, USA. gabrielse@physics.harvard.edu

Physical Review Letters
|May 1, 2012
PubMed
Summary

Researchers confined antihydrogen atoms (H¯) in a Ioffe trap, achieving ground state confinement. This advancement, producing more simultaneously trapped H¯ atoms than before, is crucial for future precision spectroscopy.

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Area of Science:

  • Atomic physics
  • Antimatter research

Background:

  • Antihydrogen (H¯) is the antimatter counterpart of hydrogen.
  • Confining antihydrogen atoms is essential for studying their properties.
  • Previous experiments faced challenges in producing and trapping sufficient numbers of antihydrogen atoms.

Purpose of the Study:

  • To improve the number of simultaneously trapped ground-state antihydrogen atoms.
  • To enable future laser cooling and high-precision spectroscopic studies of antihydrogen.

Main Methods:

  • Utilizing a Ioffe trap for antihydrogen atom confinement.
  • Ensuring sufficient confinement times (15-1000 s) for atoms to reach their ground state.
  • Addressing challenges in the interaction of cold antiprotons (p¯) and positrons (e(+)).

Main Results:

  • Achieved an average of 5±1 simultaneously confined ground-state antihydrogen atoms.
  • Demonstrated a significant increase in the number of trapped antihydrogen atoms compared to previous reports.
  • Overcame some reproducibility challenges in antiproton-antiproton and positron interactions.

Conclusions:

  • The improved trapping of ground-state antihydrogen atoms is a critical step forward.
  • This enhanced capability is vital for future experiments, including laser cooling and precision spectroscopy.
  • Further advancements in producing cold antiprotons and positrons are needed to scale up antihydrogen production.