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Atomic Nuclei: Nuclear Spin State Overview01:03

Atomic Nuclei: Nuclear Spin State Overview

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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...
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Atomic Nuclei: Nuclear Relaxation Processes01:23

Atomic Nuclei: Nuclear Relaxation Processes

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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.
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Atomic Nuclei: Nuclear Spin State Population Distribution01:14

Atomic Nuclei: Nuclear Spin State Population Distribution

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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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Spin–Spin Coupling Constant: Overview01:08

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In bromoethane, the three methyl protons are coupled to the two methylene protons that are three bonds away. In accordance with the n+1 rule, the signal from the methyl protons is split into three peaks with 1:2:1 relative intensities. The methylene protons appear as a quartet, with the relative intensities of 1:3:3:1.
Qualitatively, any spin plus-half nucleus polarizes the spins of its electrons to the minus-half state. Consequently, the paired electron in the hydrogen–carbon bond must...
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Phase Transitions02:31

Phase Transitions

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Whether solid, liquid, or gas, a substance's state depends on the order and arrangement of its particles (atoms, molecules, or ions). Particles in the solid pack closely together, generally in a pattern. The particles vibrate about their fixed positions but do not move or squeeze past their neighbors. In liquids, although the particles are closely spaced, they are randomly arranged. The position of the particles are not fixed—that is, they are free to move past their neighbors to...
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Magnetic Field due to Moving Charges01:23

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A stationary charge creates and interacts with the electric field, while a moving charge creates a magnetic field.
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Updated: Jul 5, 2025

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Researchers observed changes in Yu-Shiba-Rusinov (YSR) states across a quantum phase transition (QPT) using scanning tunneling microscopy. This method directly identifies the ground state of YSR states, distinguishing between free and screened spins.

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Area of Science:

  • Condensed Matter Physics
  • Quantum Materials
  • Superconductivity

Background:

  • Magnetic impurities in superconductors form Yu-Shiba-Rusinov (YSR) states.
  • These states exhibit a quantum phase transition (QPT) with increasing exchange interaction.
  • Observing the ground state change across the QPT is experimentally challenging.

Purpose of the Study:

  • To develop a direct method for identifying the ground state of YSR states across a QPT.
  • To investigate the spectral changes associated with the transition from a free spin to a screened spin ground state.
  • To characterize the transition regime where YSR excitation energy interacts with Zeeman energy.

Main Methods:

  • Utilizing ultralow temperature scanning tunneling microscopy (UT-STM).
  • Probing the excitation spectrum of YSR states around a spin-1/2 impurity in a magnetic field.
  • Analyzing the number and evolution of spectral peaks.

Main Results:

  • The excitation spectrum transitions from two peaks (doublet, free spin) to four peaks (singlet, screened spin) across the QPT.
  • A distinct transition regime was identified where YSR excitation energy is less than Zeeman energy.
  • Direct observation of ground state changes across the QPT was achieved.

Conclusions:

  • UT-STM provides a straightforward method for unambiguously identifying the ground state of spin-1/2 YSR states.
  • Spectral peak evolution serves as a clear indicator of the YSR ground state across the QPT.
  • The findings offer new insights into impurity physics in superconductors and quantum phase transitions.