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Related Concept Videos

Spin–Spin Coupling Constant: Overview01:08

Spin–Spin Coupling Constant: Overview

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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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Spin–Spin Coupling: Two-Bond Coupling (Geminal Coupling)01:20

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Two NMR-active nuclei bonded to a central atom can be involved in geminal or two-bond coupling. Geminal coupling is commonly seen between diastereotopic protons in chiral molecules and unsymmetrical alkenes, among others.
The central atom need not be NMR-active because its electrons are affected by the electron polarization of the spin-active atoms. However, spin information is transmitted less effectively than in one-bond coupling, and 2J values are usually weaker than 1J values. The energy of...
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Spin–Spin Coupling: One-Bond Coupling01:17

Spin–Spin Coupling: One-Bond Coupling

1.4K
Coupling interactions are strongest between NMR-active nuclei bonded to each other, where spin information can be transmitted directly through the pair of bonding electrons. While nuclei polarize their electrons to the opposite spins, the bonding electron pair has opposite spins. Configurations with antiparallel nuclear spins are expected to be lower in energy. When coupling makes antiparallel states more favorable, J is considered to have a positive value. The one-bond coupling constant, 1J,...
1.4K
Spin–Spin Coupling: Three-Bond Coupling (Vicinal Coupling)01:22

Spin–Spin Coupling: Three-Bond Coupling (Vicinal Coupling)

1.5K
Vicinal or three-bond coupling is commonly observed between protons attached to adjacent carbons. Here, nuclear spin information is primarily transferred via electron spin interactions between adjacent C‑H bond orbitals. This generally favors the antiparallel arrangement of spins, so 3J values are usually positive.
The extent of coupling depends on the C‑C bond length, the two H‑C‑C angles, any electron-withdrawing substituents, and the dihedral angle between the involved orbitals. The...
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Ampere-Maxwell's Law: Problem-Solving01:17

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A parallel-plate capacitor with capacitance C, whose plates have area A and separation distance d, is connected to a resistor R and a battery of voltage V. The current starts to flow at t = 0. What is the displacement current between the capacitor plates at time t? From the properties of the capacitor, what is the corresponding real current?
To solve the problem, we can use the equations from the analysis of an RC circuit and Maxwell's version of Ampère's law.
For the first part of the...
1.1K
Equilibrium Conditions for a Particle01:23

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2.1K
When an object is in equilibrium, it is either at rest or moving with a constant velocity. There are two types of equilibrium: static and dynamic. Static equilibrium occurs when an object is at rest, while dynamic equilibrium occurs when an object is moving with a constant velocity. In both cases, there must be a balance of forces acting on the object.
To understand the concept of equilibrium, let us first consider the forces acting on an object. When different forces act on an object, they can...
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Optimizing Magnetic Force Microscopy Resolution and Sensitivity to Visualize Nanoscale Magnetic Domains
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Temperature-conditioned deep generative framework for scalable Ising spin configuration synthesis with

Abhishek Kumar1, Partha Sarathi Bishnu1, Debabrata Deb2

  • 1Birla Institute of Technology, Mesra, Department of Computer Science and Engineering, Ranchi-835215, Jharkhand, India.

Physical Review. E
|October 21, 2025
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Summary

This study introduces a deep learning method to generate accurate spin configurations for the 2D Ising model. The approach efficiently creates synthetic data, crucial for understanding phase transitions and complex physical systems.

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Area of Science:

  • Statistical Mechanics
  • Computational Physics
  • Machine Learning

Background:

  • The 2D Ising model is a fundamental model in statistical mechanics for understanding magnetism and phase transitions.
  • Generating accurate spin configurations is computationally intensive, especially for large systems or near critical points.
  • Deep generative models offer potential for efficient and scalable simulation of physical systems.

Purpose of the Study:

  • To develop a temperature-conditioned deep generative approach for efficient spin configuration generation in the 2D Ising model.
  • To ensure physical consistency and thermodynamic accuracy of generated configurations.
  • To provide a scalable method for creating synthetic data for further analysis of phase transitions.

Main Methods:

  • A convolutional generator network conditioned on spin states, temperature, and noise was employed.
  • Physics-based constraints (magnetization, energy, correlations) were integrated as auxiliary loss terms.
  • Monte Carlo simulations were used to derive baseline data and constraints for training.

Main Results:

  • The model generated thermodynamically accurate spin configurations, closely matching Monte Carlo baselines across various lattice sizes (L=16, 32, 64).
  • Mean absolute errors were as low as 0.0016 for magnetization and correlation, and 0.0063 for energy at L=64.
  • Generated data enabled accurate phase classification, with F1 scores above 0.99 using ensemble classifiers.

Conclusions:

  • The proposed deep generative framework offers a computationally efficient and scalable solution for generating 2D Ising model spin configurations.
  • This method accurately captures critical phenomena and provides high-quality synthetic data for physical system analysis.
  • The approach demonstrates the power of integrating physics-based constraints into deep learning for scientific simulation.