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Related Concept Videos

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 Spin01:08

Atomic Nuclei: Nuclear Spin

All atomic particles possess an intrinsic angular momentum, or 'spin'. Electrons, protons, and neutrons each have a spin value of ½, although protons and neutrons in nuclei may have higher half-integer spins owing to energetic factors.
Atomic nuclei have a net nuclear spin, , which can have an integer or half-integer value. In atomic nuclei, the spins of protons are paired against each other but not with neutrons, and vice versa. Consequently, an even number of protons does not contribute to...
Nuclear Overhauser Enhancement (NOE)01:06

Nuclear Overhauser Enhancement (NOE)

Irradiation of a spin-active nucleus causes an increase or decrease in the signal intensity of neighboring nuclei that are not necessarily chemically bonded or involved in J-coupling. This phenomenon, called the nuclear Overhauser enhancement (NOE), results from through-space interactions between the nuclear spins. The NOE effect decreases with increasing internuclear distance and is generally not observed beyond 4 angstroms. In NOE, dipole-dipole interactions between neighboring spin-active...
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 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 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...

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Measuring the Spin-Lattice Relaxation Magnetic Field Dependence of Hyperpolarized [1-13C]pyruvate
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Using molecules to measure nuclear spin-dependent parity violation.

D DeMille1, S B Cahn, D Murphree

  • 1Department of Physics, P.O. Box 208120, Yale University, New Haven, Connecticut 06520, USA.

Physical Review Letters
|February 1, 2008
PubMed
Summary

This study introduces a Stark-interference method to measure nuclear spin-dependent parity violation, offering insights into nuclear anapole moments and weak neutral couplings.

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Area of Science:

  • Atomic, Molecular, and Optical Physics
  • Nuclear Physics
  • Particle Physics

Background:

  • Nuclear spin-dependent parity violation stems from electron-nucleon weak interactions and nuclear anapole moments.
  • Measuring these effects is crucial for understanding fundamental physics and nuclear structure.

Purpose of the Study:

  • To present a novel Stark-interference technique for measuring nuclear spin-dependent parity violation.
  • To enable the determination of nuclear anapole moments and neutral weak couplings.

Main Methods:

  • Utilizes a Stark-interference technique to probe the mixing of opposite-parity rotational/hyperfine levels in ground-state molecules.
  • Applicable to a wide range of atomic number nuclei in theoretically tractable diatomic species.

Main Results:

  • The proposed method allows for the measurement of nuclear spin-dependent parity violation.
  • It is expected to yield data on nuclear anapole moments for numerous nuclei.
  • Provides access to previously unmeasured neutral weak couplings.

Conclusions:

  • The Stark-interference technique offers a viable pathway for experimental investigation of parity violation.
  • This research will significantly contribute to nuclear physics and particle physics by providing new experimental data.