Jove
Visualize
Contact Us
JoVE
x logofacebook logolinkedin logoyoutube logo
ABOUT JoVE
OverviewLeadershipBlogJoVE Help Center
AUTHORS
Publishing ProcessEditorial BoardScope & PoliciesPeer ReviewFAQSubmit
LIBRARIANS
TestimonialsSubscriptionsAccessResourcesLibrary Advisory BoardFAQ
RESEARCH
JoVE JournalMethods CollectionsJoVE Encyclopedia of ExperimentsArchive
EDUCATION
JoVE CoreJoVE BusinessJoVE Science EducationJoVE Lab ManualFaculty Resource CenterFaculty Site
Terms & Conditions of Use
Privacy Policy
Policies

Related Concept Videos

Atomic Nuclei: Larmor Precession Frequency01:11

Atomic Nuclei: Larmor Precession Frequency

3.3K
The earth's gravitational field produces a 'twisting force' perpendicular to the angular momentum of a spinning mass (such as a spinning top) that causes the mass to 'wobble' around the gravitational field axis in a phenomenon called precession. Similarly, the magnetic moment (μ) of a spinning nucleus precesses due to an external magnetic field directed along the z-axis. The precession of the magnetic moment vector about the magnetic field is called Larmor precession,...
3.3K
Atomic Nuclei: Nuclear Magnetic Moment00:59

Atomic Nuclei: Nuclear Magnetic Moment

3.5K
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...
3.5K
¹H NMR: Interpreting Distorted and Overlapping Signals01:02

¹H NMR: Interpreting Distorted and Overlapping Signals

1.7K
Spin systems where the difference in chemical shifts of the coupled nuclei is greater than ten times J are called first-order spin systems. These nuclei are weakly coupled, and their chemical shifts and coupling constant can generally be estimated from the well-separated signals in the spectrum.
As Δν decreases and the signals move closer, the doublets appear increasingly distorted. The intensities of the inner lines increase at the cost of those of the outer lines as the signals are...
1.7K
¹H NMR Signal Multiplicity: Splitting Patterns01:13

¹H NMR Signal Multiplicity: Splitting Patterns

7.5K
When protons A and X are coupled, their nuclear spin energy levels are slightly modified. This is because the energy required to excite proton A to a spin state parallel to proton X is slightly different from the energy required for it to become anti-parallel to spin X. Consequently, there are two possible excitation frequencies for A (A1 and A2), depending on the spin state of X, and vice versa. The mutual nature of coupling implies that the difference between frequencies A1 and A2, indicated...
7.5K
Atomic Emission Spectroscopy: Interference01:30

Atomic Emission Spectroscopy: Interference

706
In atomic emission spectroscopy (AES), high-temperature atomizers excite a broad range of elements and molecules that generate complex emissions from sources such as oxides, hydroxides, and flame combustion products in the flame or plasma. Several strategies can be employed to minimize spectral interferences caused by overlapping emission lines or bands. These include increasing instrument resolution, choosing alternative emission lines, optimally placing the detector in low-background regions,...
706
Atomic Nuclei: Types of Nuclear Relaxation01:28

Atomic Nuclei: Types of Nuclear Relaxation

1.1K
Nuclear relaxation restores the equilibrium population imbalance and can occur via spin–lattice or spin–spin mechanisms, which are first-order exponential decay processes.
In spin–lattice or longitudinal relaxation, the excited spins exchange energy with the surrounding lattice as they return to the lower energy level. Among several mechanisms that contribute to spin–lattice relaxation, magnetic dipolar interactions are significant. Here, the excited nucleus transfers...
1.1K

You might also read

Related Articles

Articles linked to this work by shared authors, journal, and citation graph.

Sort by
Same author

Triaxiality of neutron-rich ruthenium nuclei studied by lifetime measurements.

The European physical journal. A, Hadrons and nuclei·2026
Same author

Transcriptomic signatures of developing soybean seeds reveal the molecular mechanisms of oil accumulation during domestication.

Plant biology (Stuttgart, Germany)·2026
Same author

[Safety and effectiveness of a novel spiral-scored balloon catheter in percutaneous coronary intervention].

Zhonghua xin xue guan bing za zhi·2026
Same author

First pilot tests of Compton imaging and boron concentration measurements in BNCT using i-TED.

Applied radiation and isotopes : including data, instrumentation and methods for use in agriculture, industry and medicine·2025
Same author

Probing Exotic Cross-Shell Interactions at N=28 with Single-Neutron Transfer on ^{47}K.

Physical review letters·2025
Same author

Search for a Neutron Dark Decay in ^{6}He.

Physical review letters·2024

Related Experiment Video

Updated: Mar 8, 2026

Recording Gamma Band Oscillations in Pedunculopontine Nucleus Neurons
09:04

Recording Gamma Band Oscillations in Pedunculopontine Nucleus Neurons

Published on: September 14, 2016

9.0K

First Observation of Multiphonon γ-Vibrations in an Odd-Odd Nuclear System.

E H Wang1,2,3, M Abushawish4, J H Hamilton3

  • 1Shandong University, Shandong Provincial Key Laboratory of Nuclear Science, Nuclear Energy Technology and Comprehensive Utilization, Weihai Frontier Innovation Institute of Nuclear Technology, School of Nuclear Science, Energy and Power Engineering, Jinan 250061, China.

Physical Review Letters
|March 6, 2026
PubMed
Summary

Researchers identified the first multiphonon gamma-vibrational bands in the neutron-rich nucleus niobium-104. This finding reveals robust vibration excitations and coexisting shapes in complex nuclei.

More Related Videos

Uncovering Hidden Dynamics of Natural Photonic Structures Using Holographic Imaging
05:45

Uncovering Hidden Dynamics of Natural Photonic Structures Using Holographic Imaging

Published on: March 31, 2022

3.1K
Isotopic Effect in Double Proton Transfer Process of Porphycene Investigated by Enhanced QM/MM Method
05:51

Isotopic Effect in Double Proton Transfer Process of Porphycene Investigated by Enhanced QM/MM Method

Published on: July 19, 2019

6.7K

Related Experiment Videos

Last Updated: Mar 8, 2026

Recording Gamma Band Oscillations in Pedunculopontine Nucleus Neurons
09:04

Recording Gamma Band Oscillations in Pedunculopontine Nucleus Neurons

Published on: September 14, 2016

9.0K
Uncovering Hidden Dynamics of Natural Photonic Structures Using Holographic Imaging
05:45

Uncovering Hidden Dynamics of Natural Photonic Structures Using Holographic Imaging

Published on: March 31, 2022

3.1K
Isotopic Effect in Double Proton Transfer Process of Porphycene Investigated by Enhanced QM/MM Method
05:51

Isotopic Effect in Double Proton Transfer Process of Porphycene Investigated by Enhanced QM/MM Method

Published on: July 19, 2019

6.7K

Area of Science:

  • Nuclear Physics
  • Nuclear Spectroscopy
  • Nuclear Structure

Background:

  • Studying exotic nuclei provides insights into nuclear forces and structure.
  • Neutron-rich nuclei beyond N=60 are crucial for understanding shape transitions.
  • High-spin states in odd-odd nuclei are challenging to access and interpret.

Purpose of the Study:

  • To identify and characterize multiphonon gamma-vibrational bands in the odd-odd nucleus _{41}^{104}Nb_{63}.
  • To investigate the coexistence of different nuclear shapes (triaxial and oblate) in this region.
  • To test theoretical models against experimental data for high-spin states.

Main Methods:

  • Utilized a spectrometer with isotopic resolution coupled to a gamma-ray tracking array.
  • Performed high-fold gamma coincidence measurements.
  • Employed triaxial projected shell model calculations.

Main Results:

  • Successfully identified the first multiphonon gamma-vibrational bands in _{41}^{104}Nb_{63}.
  • Observed good agreement between experimental data and theoretical calculations for yrast, one-phonon, and two-phonon bands.
  • Investigated shape coexistence, suggesting both triaxial and oblate configurations.

Conclusions:

  • Demonstrated the robustness of vibration excitations even with odd valence proton and neutron.
  • Highlighted the possibility of coexisting shapes in nuclei beyond the N=60 transitional region.
  • Advanced the understanding of nuclear structure in exotic, neutron-rich isotopes.