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Atomic Nuclei: Nuclear Spin State Population Distribution01:14

Atomic Nuclei: Nuclear Spin State Population Distribution

2.5K
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.
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Nuclear Binding Energy02:13

Nuclear Binding Energy

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The difference between the calculated and experimentally measured masses is known as the mass defect of the atom. In the case of helium-4, the mass defect indicates a “loss” in mass of 4.0331 amu – 4.0026 amu = 0.0305 amu. The loss in mass accompanying the formation of an atom from protons, neutrons, and electrons is due to the conversion of that mass into energy that is evolved as the atom forms. The nuclear binding energy is the energy produced when the atoms’ nucleons are bound...
15.0K
Atomic Radii and Effective Nuclear Charge03:08

Atomic Radii and Effective Nuclear Charge

62.9K
The elements in groups of the periodic table exhibit similar chemical behavior. This similarity occurs because the members of a group have the same number and distribution of electrons in their valence shells.
62.9K
Nuclear Overhauser Enhancement (NOE)01:06

Nuclear Overhauser Enhancement (NOE)

1.5K
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...
1.5K
Atomic Nuclei: Nuclear Relaxation Processes01:23

Atomic Nuclei: Nuclear Relaxation Processes

1.3K
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.
1.3K
Nuclear Stability03:18

Nuclear Stability

23.8K
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...
23.8K

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Related Experiment Video

Updated: Mar 8, 2026

High-resolution Imaging of Nuclear Dynamics in Live Cells under Uniaxial Tensile Strain
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High-resolution Imaging of Nuclear Dynamics in Live Cells under Uniaxial Tensile Strain

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Simultaneous Microscopic Description of Nuclear Level Density and Radiative Strength Function.

N Quang Hung1, N Dinh Dang2,3, L T Quynh Huong4,5

  • 1Institute of Research and Development, Duy Tan University, K7/25 Quang Trung, Danang City, Vietnam.

Physical Review Letters
|January 28, 2017
PubMed
Summary

This study presents a microscopic approach for nuclear level density (NLD) and radiative strength function (RSF). Exact thermal pairing is crucial for describing NLD, challenging the Brink-Axel hypothesis for RSF.

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Area of Science:

  • Nuclear Physics
  • Quantum Mechanics
  • Statistical Mechanics

Background:

  • Nuclear level density (NLD) and radiative strength function (RSF) are fundamental nuclear structure properties.
  • Accurate theoretical models are needed to describe these properties across various isotopes and energy ranges.
  • Previous models often relied on approximations that may not hold universally.

Purpose of the Study:

  • To simultaneously describe NLD and RSF using a unified microscopic approach.
  • To investigate the role of exact thermal pairing and giant resonances in nuclear properties.
  • To validate the model against experimental data for specific isotopes.

Main Methods:

  • A microscopic approach incorporating thermal effects of exact pairing.
  • Inclusion of giant resonances within the phonon-damping model.
  • Comparison of theoretical calculations with experimental data from the Oslo group for Ytterbium isotopes.

Main Results:

  • The model successfully describes NLD and RSF for ^{170,171,172}Yb isotopes.
  • Demonstrates the significance of exact thermal pairing for NLD at low and intermediate excitation energies.
  • Results challenge the validity of the Brink-Axel hypothesis for RSF calculations.

Conclusions:

  • Exact thermal pairing is essential for accurate NLD predictions.
  • The developed microscopic approach provides a robust framework for studying nuclear properties.
  • The findings necessitate a re-evaluation of assumptions in current RSF models.