Jove
Visualize
Contact Us

Related Concept Videos

Raman Spectroscopy Instrumentation: Overview01:26

Raman Spectroscopy Instrumentation: Overview

1.5K
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...
1.5K
Raman Spectroscopy: Overview01:20

Raman Spectroscopy: Overview

2.2K
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...
2.2K
Ultraviolet and Visible (UV–Vis) Spectroscopy: Overview01:02

Ultraviolet and Visible (UV–Vis) Spectroscopy: Overview

8.4K
Ultraviolet–visible (UV–visible or UV–Vis) spectroscopy is an analytical technique that investigates the interaction between matter and UV–Vis light within the electromagnetic spectrum. This method is widely used for its versatility, simplicity, and relatively quick data acquisition, making it valuable for both qualitative and quantitative analysis. When UV–Vis radiation passes through a material,  molecules absorb light depending on the energy required for...
8.4K
UV–Vis Spectroscopy: Molecular Electronic Transitions01:16

UV–Vis Spectroscopy: Molecular Electronic Transitions

3.3K
In Ultraviolet–Visible (UV–Vis) spectroscopy, the absorption of electromagnetic radiation is used to probe the electronic structure of molecules. This technique provides insights into molecular electronic transitions, particularly the movement of electrons between different molecular orbitals. Radiation is absorbed if the energy of the electromagnetic radiation passing through the molecule is precisely equal to the energy difference between the excited and ground states. During this...
3.3K
UV–Vis Spectrometers01:14

UV–Vis Spectrometers

4.3K
The absorbance of UV and visible (UV–visible) radiations is measured using a UV–visible spectrophotometer. Deuterium lamps, which emit UV radiation, and tungsten lamps, which produce radiation in the visible region, are used as light sources in UV–visible spectrophotometers. A monochromator or prism is used for diffraction grating, i.e., to split the incoming radiation into different wavelengths. A system of slits is used to focus the desired wavelength on the sample cell.
4.3K
UV–Vis Spectroscopy of Conjugated Systems01:32

UV–Vis Spectroscopy of Conjugated Systems

8.8K
Organic compounds with conjugated double bonds show strong absorption features in the UV–visible region of the electromagnetic spectrum attributed to π → π* electronic excitations. Generally, a UV–vis absorption spectrum is recorded as a plot of absorbance vs wavelength. The wavelength of maximum absorbance, which manifests as a peak in the absorption spectrum, is denoted as λmax.
One of the factors influencing λmax is the extent of conjugation in...
8.8K

You might also read

Related Articles

Articles linked to this work by shared authors, journal, and citation graph.

Sort by
Same author

Spectroscopy of ^{4}He at 0.25 ppt Uncertainty and Improved Alpha-Helion Charge-Radius Difference Determination.

Physical review letters·2026
Same author

A simple graphics processing unit-accelerated propagation routine for laser pulses in the strong-field regime.

The Review of scientific instruments·2024
Same author

Erratum: Coherent Excitation of the Highly Forbidden Electric Octupole Transition in ^{172}Yb^{+} [Phys. Rev. Lett. 125, 163001 (2020)].

Physical review letters·2022
Same author

Coherent Excitation of the Highly Forbidden Electric Octupole Transition in ^{172}Yb^{+}.

Physical review letters·2020
Same author

Proton-electron mass ratio from laser spectroscopy of HD<sup>+</sup> at the part-per-trillion level.

Science (New York, N.Y.)·2020
Same author

Extreme ultraviolet lensless imaging without object support through rotational diversity in diffractive shearing interferometry.

Optics express·2020
JoVE
x logofacebook logolinkedin logoyoutube logo
ABOUT JoVE
OverviewLeadershipBlogJoVE Help Center
AUTHORS
Publishing ProcessEditorial BoardScope & PoliciesPeer ReviewFAQSubmit
LIBRARIANS
TestimonialsSubscriptionsAccessResourcesLibrary Advisory BoardFAQ
RESEARCH
JoVE JournalMethods CollectionsJoVE Encyclopedia of ExperimentsArchive
EDUCATION
JoVE CoreJoVE BusinessJoVE Science EducationJoVE Lab ManualFaculty Resource CenterFaculty Site
Terms & Conditions of Use
Privacy Policy
Policies

Related Experiment Video

Updated: Mar 12, 2026

Ultrafast Time-resolved Near-IR Stimulated Raman Measurements of Functional &#960;-conjugate Systems
09:57

Ultrafast Time-resolved Near-IR Stimulated Raman Measurements of Functional π-conjugate Systems

Published on: February 10, 2020

7.7K

High-Precision Ramsey-Comb Spectroscopy at Deep Ultraviolet Wavelengths.

R K Altmann1, S Galtier1, L S Dreissen1

  • 1LaserLaB, Department of Physics and Astronomy, VU University Amsterdam, De Boelelaan 1081, 1081 HV Amsterdam, Netherlands.

Physical Review Letters
|November 9, 2016
PubMed
Summary

Scientists demonstrate deep ultraviolet Ramsey-comb spectroscopy for high-precision measurements. This new method significantly improves accuracy for atomic spectroscopy at short wavelengths, overcoming previous experimental challenges.

More Related Videos

A Multimodal Wide-Field Fourier-Transform Raman Microscope
06:48

A Multimodal Wide-Field Fourier-Transform Raman Microscope

Published on: December 30, 2025

650
Differential Imaging of Biological Structures with Doubly-resonant Coherent Anti-stokes Raman Scattering CARS
12:56

Differential Imaging of Biological Structures with Doubly-resonant Coherent Anti-stokes Raman Scattering CARS

Published on: October 17, 2010

14.1K

Related Experiment Videos

Last Updated: Mar 12, 2026

Ultrafast Time-resolved Near-IR Stimulated Raman Measurements of Functional &#960;-conjugate Systems
09:57

Ultrafast Time-resolved Near-IR Stimulated Raman Measurements of Functional π-conjugate Systems

Published on: February 10, 2020

7.7K
A Multimodal Wide-Field Fourier-Transform Raman Microscope
06:48

A Multimodal Wide-Field Fourier-Transform Raman Microscope

Published on: December 30, 2025

650
Differential Imaging of Biological Structures with Doubly-resonant Coherent Anti-stokes Raman Scattering CARS
12:56

Differential Imaging of Biological Structures with Doubly-resonant Coherent Anti-stokes Raman Scattering CARS

Published on: October 17, 2010

14.1K

Area of Science:

  • Atomic Physics
  • Quantum Optics
  • Spectroscopy

Background:

  • High-precision spectroscopy is crucial for testing fundamental physics, including quantum electrodynamics and the proton radius puzzle.
  • Deep ultraviolet (UV) and shorter wavelengths present significant experimental hurdles for precise measurements.

Purpose of the Study:

  • To demonstrate Ramsey-comb spectroscopy in the deep UV for the first time.
  • To showcase its capabilities for precision spectroscopy at short wavelengths.

Main Methods:

  • Utilized Ramsey-comb spectroscopy in the deep UV.
  • Excited the two-photon 4p^{6}→4p^{5}5p[1/2]_{0} transition of ^{84}Kr at 212.55 nm in an atomic beam.
  • Employed a counterpropagating excitation geometry to minimize Doppler effects and effectively eliminated ac-Stark shifts.

Main Results:

  • Achieved a transition frequency of 2,820,833,101,679(103) kHz for ^{84}Kr.
  • The measurement uncertainty was reduced by a factor of 34 compared to previous best measurements.
  • The precision was limited only by the 27 ns lifetime of the excited state.

Conclusions:

  • Ramsey-comb spectroscopy is a viable and powerful technique for high-precision measurements in the deep UV.
  • This advancement opens new avenues for fundamental physics tests requiring short-wavelength spectroscopy.