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Related Concept Videos

Double Resonance Techniques: Overview01:12

Double Resonance Techniques: Overview

Double resonance techniques in Nuclear Magnetic Resonance (NMR) spectroscopy involve the simultaneous application of two different frequencies or radiofrequency pulses to manipulate and observe two distinct nuclear spins. One important application of double resonance is spin decoupling, which selectively suppresses coupling with one type of nucleus while observing the NMR signal from another nucleus, simplifying the spectrum and enhancing resolution.
Spin decoupling is usually achieved by...
¹H NMR: Interpreting Distorted and Overlapping Signals01:02

¹H NMR: Interpreting Distorted and Overlapping Signals

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 slanted or...
Sound Waves: Resonance01:14

Sound Waves: Resonance

Resonance is produced depending on the boundary conditions imposed on a wave. Resonance can be produced in a string under tension with symmetrical boundary conditions (i.e., has a node at each end). A node is defined as a fixed point where the string does not move. The symmetrical boundary conditions result in some frequencies resonating and producing standing waves, while other frequencies interfere destructively. Sound waves can resonate in a hollow tube, and the frequencies of the sound...
¹H NMR: Complex Splitting01:13

¹H NMR: Complex Splitting

A proton M that is coupled to a proton X results in doublet signals for M. However, NMR-active nuclei can be simultaneously coupled to more than one nonequivalent nucleus. When M is coupled to a second proton A, such as in styrene oxide, each peak in the doublet is split into another doublet.
Splitting diagrams or splitting tree diagrams are routinely used to depict such complex couplings. While drawing splitting diagrams, the splitting with the larger coupling constant is usually applied first.
¹H NMR Signal Multiplicity: Splitting Patterns01:13

¹H NMR Signal Multiplicity: Splitting Patterns

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...
Standing Waves in a Cavity01:28

Standing Waves in a Cavity

A household microwave and lasers are examples of standing electromagnetic waves in a cavity. When two conducting metal plates are placed parallel at the nodal planes, it creates a cavity where standing waves are formed. The cavity between the two planes is analogous to a stretched string held at the points x = 0 and x = L. Here, the distance 'L' between the two planes must be an integer multiple of half of the wavelength. The wavelengths that satisfy this condition are given by:

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Updated: May 18, 2026

Stimulated Stokes and Antistokes Raman Scattering in Microspherical Whispering Gallery Mode Resonators
12:21

Stimulated Stokes and Antistokes Raman Scattering in Microspherical Whispering Gallery Mode Resonators

Published on: April 4, 2016

Collective effects in second-harmonic generation from split-ring-resonator arrays.

S Linden1, F B P Niesler, J Förstner

  • 1Institute of Nanotechnology, Institute of Applied Physics, and DFG-Center for Functional Nanostructures, Karlsruhe Institute of Technology, 76128 Karlsruhe, Germany.

Physical Review Letters
|October 4, 2012
PubMed
Summary
This summary is machine-generated.

Optical experiments reveal that second-harmonic generation efficiency in split-ring-resonator arrays changes nonmonotonically with lattice constant. This behavior arises from a balance between element dilution and inter-resonator interactions affecting linewidth and near-fields.

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Multiplex Chemical Imaging Based on Broadband Stimulated Raman Scattering Microscopy
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Published on: March 23, 2017

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Last Updated: May 18, 2026

Stimulated Stokes and Antistokes Raman Scattering in Microspherical Whispering Gallery Mode Resonators
12:21

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Fabrication of Nanopillar-Based Split Ring Resonators for Displacement Current Mediated Resonances in Terahertz Metamaterials
10:28

Fabrication of Nanopillar-Based Split Ring Resonators for Displacement Current Mediated Resonances in Terahertz Metamaterials

Published on: March 23, 2017

Area of Science:

  • * Plasmonics and Nanophotonics
  • * Nonlinear Optics
  • * Metamaterials

Background:

  • * Split-ring resonators (SRRs) are fundamental metamaterial elements exhibiting strong plasmonic resonances.
  • * Second-harmonic generation (SHG) is a key nonlinear optical process for frequency conversion.
  • * Array geometry significantly influences the optical properties of nanostructured materials.

Purpose of the Study:

  • * To investigate the dependence of SHG efficiency on the lattice constant in square arrays of SRRs.
  • * To elucidate the underlying physical mechanisms governing this relationship.
  • * To understand the interplay between individual resonator properties and collective array effects.

Main Methods:

  • * Fabrication of periodic square arrays of split-ring resonators.
  • * Optical characterization of second-harmonic generation efficiency as a function of lattice constant.
  • * Theoretical modeling to interpret experimental observations, considering dilution and inter-resonator coupling.

Main Results:

  • * Observed a nonmonotonic dependence of SHG conversion efficiency on the array lattice constant.
  • * Demonstrated that efficiency increases with decreasing lattice constant initially, then decreases.
  • * Identified competing effects of element dilution and changes in linewidth/near-field coupling.

Conclusions:

  • * The nonmonotonic behavior is attributed to a complex interplay between geometric dilution and resonant coupling among SRRs.
  • * Near-field interactions and linewidth variations significantly impact the nonlinear response of the array.
  • * Precise control over lattice constant is crucial for optimizing SHG in metamaterial arrays.