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Mass Analyzers: Common Types01:19

Mass Analyzers: Common Types

725
The quadrupole mass analyzer consists of four cylindrical metal rods arranged in a diamond carrying a DC voltage and a radio-frequency AC voltage. The motion of ions through the quadrupole depends on the field strength, causing only ions of a certain m/z to resonate successfully and strike the detector at a given field strength. Though the transmission rate for these analyzers is high, the exact elemental composition of the sample is not determined because of low resolution; however, they are...
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¹H NMR: Interpreting Distorted and Overlapping Signals01:02

¹H NMR: Interpreting Distorted and Overlapping Signals

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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...
1.1K
¹H NMR: Complex Splitting01:13

¹H NMR: Complex Splitting

1.4K
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...
1.4K
¹³C NMR: ¹H–¹³C Decoupling01:04

¹³C NMR: ¹H–¹³C Decoupling

1.2K
The probability of having two carbon-13 atoms next to each other is negligible because of the low natural abundance of carbon-13. Consequently, peak splitting due to carbon-carbon spin-spin coupling is not observed in spectra. However, protons up to three sigma bonds away split the carbon signal according to the n+1 rule, resulting in complicated spectra.
A broadband decoupling technique is used to simplify these complex, sometimes overlapping, signals. Broadband decoupling relies on a...
1.2K
Interpreting ¹H NMR Signal Splitting: The (n + 1) Rule01:10

Interpreting ¹H NMR Signal Splitting: The (n + 1) Rule

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In the AX proton spin system, proton A can sense the two spin states of a coupled proton X, resulting in a doublet NMR signal with two peaks of equal (1:1) intensity. When proton A is coupled to two equivalent protons (AX2 spin system), the spin states of each X can be aligned with or against the external field, creating three possible scenarios. This results in a 1:2:1  triplet signal, where the central peak corresponds to the chemical shift of A and is twice as large or intense as the...
1.5K
Double Resonance Techniques: Overview01:12

Double Resonance Techniques: Overview

326
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...
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Updated: Sep 26, 2025

High Resolution Phonon-assisted Quasi-resonance Fluorescence Spectroscopy
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Boundary effects and quadrupole contribution in sum frequency generation spectroscopy.

Tomonori Hirano1, Akihiro Morita1

  • 1Department of Chemistry, Graduate School of Science, Tohoku University, Sendai 980-8578, Japan.

The Journal of Chemical Physics
|April 23, 2022
PubMed
Summary

This study addresses boundary effects in sum frequency generation spectroscopy calculations. We found a method to minimize quadrupole effects for accurate interface signal extraction in spectroscopic analysis.

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Area of Science:

  • Computational spectroscopy
  • Surface science
  • Nonlinear optics

Background:

  • Sum frequency generation (SFG) spectroscopy relies on accurate time correlation functions.
  • Extracting interface signals from SFG calculations is challenged by boundary effects.
  • Computational cost necessitates defining boundaries to restrict bulk regions.

Purpose of the Study:

  • To resolve issues in extracting interface signals from SFG calculations.
  • To investigate the influence of boundaries on time correlation functions.
  • To establish a proper treatment for reliable spectroscopic analysis.

Main Methods:

  • Analysis of time correlation functions in SFG spectroscopy.
  • Examination of boundary influences on computational results.
  • Identification and minimization of quadrupole contributions.

Main Results:

  • Boundary effects significantly influence time correlation functions.
  • A distinction between boundary effects and quadrupole contribution was elucidated.
  • A proper molecular center (e.g., center of mass for water) was identified to minimize quadrupole effects.

Conclusions:

  • Proper treatment of boundary effects is crucial for reliable SFG spectroscopic analysis.
  • Minimizing quadrupole effects through appropriate molecular centering enhances signal extraction.
  • The findings are applicable to systems like liquid water.