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IR Spectrum Peak Splitting: Symmetric vs Asymmetric Vibrations01:08

IR Spectrum Peak Splitting: Symmetric vs Asymmetric Vibrations

Identical bonds within a polyatomic group can stretch symmetrically (in-phase) or asymmetrically (out-of-phase). Similar to hydrogen bonding, these vibrations also influence the shape of the IR peak. Generally, asymmetric stretching frequencies are higher than symmetric stretching frequencies. For example, primary amines exhibit two distinct IR peaks between 3300–3500 cm−1 corresponding to the symmetric and asymmetric N-H stretching, while secondary amines exhibit a single stretching vibration...
IR Frequency Region: Fingerprint Region01:03

IR Frequency Region: Fingerprint Region

IR spectra are divided into two main regions: the diagnostic region and the fingerprint region. The diagnostic region of the spectrum lies above 1500 cm−1. The absorptions resulting from single-bond vibrations of the N–H, C–H, and O–H stretch at higher wavenumbers and appear on the left side of the spectrum. The stretching absorptions of the C≡C and C≡N occur between 2100–2300 cm−1. In contrast, those arising from stretching absorptions of the C=O, C=N, and C=C occur between 1600–1850 cm−1.
The...
IR Spectrometers01:25

IR Spectrometers

There are two main infrared (IR) spectrophotometers: dispersive IR spectrometers and Fourier transform infrared (FTIR) spectrometers. In a dispersive IR spectrometer, a beam of infrared radiation produced by a hot wire is divided into two parallel equal-intensity beams using mirrors. One beam passes through the sample, while another is a reference beam. The beams then move through the monochromator, which separates the radiations into a continuous spectrum of different frequencies. The...
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...
IR Spectroscopy: Molecular Vibration Overview01:24

IR Spectroscopy: Molecular Vibration Overview

When Infrared (IR) radiation passes through a covalently bonded molecule, the bonds transition from lower to higher vibrational levels. The fundamental vibrational motions that result in infrared absorption can be classified as stretching or bending vibrations.
Stretching vibrations are vibrational motions that occur along the bond line, changing the bond length or distance between two bonded atoms. They are further distinguished as symmetric or asymmetric. In symmetric stretching, the...
NMR Spectroscopy: Chemical Shift Overview01:15

NMR Spectroscopy: Chemical Shift Overview

The position of the absorption signal of a sample is reported relative to the position of the signal of tetramethylsilane (TMS), which is added as an internal reference while recording spectra. The difference between the absorption frequencies of the sample and TMS (in Hz) is divided by the spectrometer operating frequency (in MHz) to obtain a dimensionless quantity called the chemical shift. It is reported on the δ (delta) scale and expressed in parts per million.
For instance, the proton...

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Related Experiment Video

Updated: Jun 9, 2026

Implementation of a Reference Interferometer for Nanodetection
16:11

Implementation of a Reference Interferometer for Nanodetection

Published on: April 26, 2014

Minimum detectable phase shift in spectrum-analysis techniques of optical interferometric vibration detection.

V S Sudarshanam

    Applied Optics
    |August 25, 2010
    PubMed
    Summary
    This summary is machine-generated.

    1/f noise in system components limits detectable phase shift in optical interferometric vibration detection. This analysis provides a tool to evaluate noise effects in spectrum analysis techniques.

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    Area of Science:

    • Optics and Photonics
    • Electrical Engineering
    • Metrology

    Background:

    • Optical interferometry is crucial for vibration detection.
    • New linear spectrum analysis techniques offer enhanced sensitivity.
    • Understanding noise limitations is key to improving performance.

    Purpose of the Study:

    • To identify the source of the minimum detectable phase shift in optical interferometric vibration detection.
    • To develop a theoretical model for predicting dynamic range and inaccuracy.
    • To compare analysis with experimental data and existing optical systems.

    Main Methods:

    • Analysis of 1/f noise voltage in system components.
    • Development of a simple theoretical model for dynamic range and inaccuracy.
    • Comparison with experimental measurements and heterodyne shot-noise-limited systems.

    Main Results:

    • The minimum detectable phase shift is directly linked to 1/f noise voltage.
    • The theoretical model shows good agreement with experimental measurements.
    • The analysis provides a method to assess noise effects in spectrum analysis.

    Conclusions:

    • 1/f noise is the primary factor limiting phase shift detection.
    • The developed model and analysis tool are effective for evaluating spectrum analysis techniques.
    • Findings are applicable to optical interferometry, particularly with fiber-optic modulators.