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Related Concept Videos

Raman Spectroscopy: Overview01:20

Raman Spectroscopy: Overview

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The underlying principle of Raman spectroscopy is based on the interaction between light and matter, specifically molecules' inelastic scattering of photons. When a monochromatic beam of light, typically from a laser source, interacts with a sample, most scattered light has the same frequency as the incident light. This is known as Rayleigh scattering.
However, a small fraction of the scattered light exhibits a frequency shift due to the exchange of energy between the incident photons and...
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Raman Spectroscopy Instrumentation: Overview01:26

Raman Spectroscopy Instrumentation: Overview

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A conventional Raman spectrophotometer includes a laser source, a sample holding system, a wavelength selector, and a detector.
The monochromatic laser source, typically using visible or near-infrared radiation, generates a highly focused beam of light. This light interacts with the molecules of the sample, scattering some of the light. Liquid and gaseous samples are usually tested in ordinary glass capillaries, while solids can be analyzed as powders packed in capillaries or as potassium...
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NMR Spectroscopy: Chemical Shift Overview01:15

NMR Spectroscopy: Chemical Shift Overview

3.8K
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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Atomic Spectroscopy: Absorption, Emission, and Fluorescence01:23

Atomic Spectroscopy: Absorption, Emission, and Fluorescence

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Atomic spectroscopy is a vital tool in elemental analysis, both qualitatively and quantitatively. It can be broadly divided into optical spectroscopy, mass spectroscopy, and X-ray spectroscopy methods. The optical spectroscopic methods are atomic absorption spectroscopy (AAS), atomic emission spectroscopy (AES), and atomic fluorescence spectroscopy (AFS). The first step in all three methods is atomization, where the solid, liquid, or solution-phase samples are converted into gas-phase atoms and...
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¹H NMR: Interpreting Distorted and Overlapping Signals01:02

¹H NMR: Interpreting Distorted and Overlapping Signals

1.7K
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...
1.7K
Atomic Absorption Spectroscopy: Instrumentation01:22

Atomic Absorption Spectroscopy: Instrumentation

1.9K
An atomic absorption spectrophotometer (AAS) comprises several components: a radiation source, an atomizer, a monochromator, and a detector. The radiation source can be a hollow-cathode lamp (HCL) or an electrodeless-discharge lamp (EDL), both of which provide a narrow emission line of the required wavelength. However, some instruments use continuum sources and high-resolution monochromators to achieve a narrow range of radiation.
The atomizer used in AAS can be either a flame atomizer or an...
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Low-frequency shift Raman spectroscopy using atomic filters.

Xiaobo Xue, Corey Janisch, Yizhu Chen

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    |November 15, 2016
    PubMed
    Summary
    This summary is machine-generated.

    This study demonstrates low-frequency Raman spectroscopy using a Faraday anomalous dispersion optical filter (FADOF) and an atomic filter. This technique achieves precise measurements down to 3 cm-1 for both Stokes and anti-Stokes shifts.

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    Area of Science:

    • Spectroscopy
    • Optics
    • Materials Science

    Background:

    • Low-frequency Raman spectroscopy is crucial for analyzing material properties but is technically challenging.
    • Existing methods often struggle to resolve signals at very low frequency shifts (few cm-1).
    • Atomic filters offer narrow bandwidths suitable for high-resolution spectral filtering.

    Purpose of the Study:

    • To demonstrate a novel low-frequency Raman measurement system.
    • To achieve Raman shift measurements down to a few cm-1.
    • To explore the use of tandem atomic and optical filters for enhanced spectral resolution.

    Main Methods:

    • Utilized a Faraday anomalous dispersion optical filter (FADOF) with an ultralow bandwidth (0.08 cm-1) as a bandpass filter.
    • Employed a rubidium atomic resonant absorption filter as a notch filter with a 0.3 cm-1 bandwidth.
    • Performed a proof-of-concept study measuring Raman signals from silica optical fiber.

    Main Results:

    • Successfully demonstrated low-frequency Raman shift measurements down to 3 cm-1.
    • Measured both Stokes and anti-Stokes shifts with high precision at an equivalent signal level.
    • Validated the tandem filter approach for sensitive low-frequency Raman detection.

    Conclusions:

    • The combined FADOF and atomic filter system enables unprecedented low-frequency Raman measurements.
    • This approach shows significant potential for developing gigahertz-terahertz low-energy Raman spectroscopy.
    • Atomic filters are promising for future high-resolution spectroscopic applications.