Jove
Visualize
Contact Us
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 Concept Videos

Aliasing01:18

Aliasing

284
Accurate signal sampling and reconstruction are crucial in various signal-processing applications. A time-domain signal's spectrum can be revealed using its Fourier transform. When this signal is sampled at a specific frequency, it results in multiple scaled replicas of the original spectrum in the frequency domain. The spacing of these replicas is determined by the sampling frequency.
If the sampling frequency is below the Nyquist rate, these replicas overlap, preventing the original...
284
Upsampling01:22

Upsampling

351
Managing signal sampling rates is essential in digital signal processing to maintain signal integrity. A decimated signal, characterized by a reduced frequency range due to its lower sampling rate, can be upsampled by inserting zeros between each sample. This upsampling process expands the original spectrum and introduces repeated spectral replicas at intervals dictated by the new Nyquist frequency. To refine this zero-inserted sequence, it is passed through a lowpass filter with a cutoff...
351
NMR Spectrometers: Radiofrequency Pulses and Pulse Sequences01:17

NMR Spectrometers: Radiofrequency Pulses and Pulse Sequences

981
A pulse is a short burst of radio waves distributed over a range of frequencies that simultaneously excites all the nuclei in the sample. Upon passing a radio frequency pulse along the x-axis, the nuclei absorb energy corresponding to their Larmor frequencies and achieve resonance. This shifts the net magnetization vector from the z-axis toward the transverse plane. This angle of rotation of the magnetization vector, or the flip angle, is proportional to the duration and intensity of the pulse.
981
Sampling Theorem01:15

Sampling Theorem

846
In signal processing, the analysis of continuous-time signals, denoted as x(t), often involves sampling techniques to convert these signals into discrete-time signals. This process is essential for digital representation and manipulation. A critical component in sampling is the train of impulses, characterized by the sampling interval and the sampling frequency. The relationship between these parameters and the original signal's properties dictates the success of the sampling process.
846

You might also read

Related Articles

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

Sort by
Same author

Modelling two-laser asynchronous optical sampling using a single 2-section semiconductor mode-locked laser diode.

Optics express·2022
Same author

Fast optical sampling by electronic repetition-rate tuning using a single mode-locked laser diode.

Optics express·2021
Same author

Role of surface microgeometries on electron escape probability and secondary electron yield of metal surfaces.

Scientific reports·2020
Same author

High peak-power picosecond pulse generation at 1.26 µm using a quantum-dot-based external-cavity mode-locked laser and tapered optical amplifier.

Optics express·2012

Related Experiment Video

Updated: Oct 11, 2025

Rapid Repetition Rate Fluctuation Measurement of Soliton Crystals in a Microresonator
07:42

Rapid Repetition Rate Fluctuation Measurement of Soliton Crystals in a Microresonator

Published on: December 15, 2021

3.2K

Megahertz scan rates enabled by optical sampling by repetition-rate tuning.

D Bajek1, M A Cataluna2

  • 1School of Engineering and Physical Sciences, Heriot-Watt University, Edinburgh, EH14 4AS, UK. d.bajek@hw.ac.uk.

Scientific Reports
|November 27, 2021
PubMed
Summary

We achieved record megahertz scan rates using optical sampling by repetition-rate tuning (OSBERT). This breakthrough enables faster time-resolved spectroscopy by electronically tuning a compact laser diode.

More Related Videos

High Resolution Phonon-assisted Quasi-resonance Fluorescence Spectroscopy
10:40

High Resolution Phonon-assisted Quasi-resonance Fluorescence Spectroscopy

Published on: June 28, 2016

7.7K
Low-cost Custom Fabrication and Mode-locked Operation of an All-normal-dispersion Femtosecond Fiber Laser for Multiphoton Microscopy
08:48

Low-cost Custom Fabrication and Mode-locked Operation of an All-normal-dispersion Femtosecond Fiber Laser for Multiphoton Microscopy

Published on: November 22, 2019

7.7K

Related Experiment Videos

Last Updated: Oct 11, 2025

Rapid Repetition Rate Fluctuation Measurement of Soliton Crystals in a Microresonator
07:42

Rapid Repetition Rate Fluctuation Measurement of Soliton Crystals in a Microresonator

Published on: December 15, 2021

3.2K
High Resolution Phonon-assisted Quasi-resonance Fluorescence Spectroscopy
10:40

High Resolution Phonon-assisted Quasi-resonance Fluorescence Spectroscopy

Published on: June 28, 2016

7.7K
Low-cost Custom Fabrication and Mode-locked Operation of an All-normal-dispersion Femtosecond Fiber Laser for Multiphoton Microscopy
08:48

Low-cost Custom Fabrication and Mode-locked Operation of an All-normal-dispersion Femtosecond Fiber Laser for Multiphoton Microscopy

Published on: November 22, 2019

7.7K

Area of Science:

  • Optics and Photonics
  • Ultrafast Spectroscopy
  • Laser Physics

Background:

  • Time-resolved spectroscopy traditionally faces limitations in scan speed.
  • Existing optical sampling by repetition-rate tuning (OSBERT) methods have slower scan rates.
  • Compact and tunable pulsed laser sources are crucial for advanced spectroscopic techniques.

Purpose of the Study:

  • To demonstrate optical sampling by repetition-rate tuning (OSBERT) at unprecedented megahertz scan rates.
  • To develop a novel system for high-speed electronic modulation of a laser diode's repetition rate.
  • To enable real-time acquisition of ultrafast optical phenomena.

Main Methods:

  • Utilized a compact, tunable 2-section passively mode-locked laser diode (MLLD) as the pulsed source.
  • Implemented an imbalanced Michelson interferometer configuration with a passive delay line (PDL).
  • Employed impedance-matching and a signal generator for megahertz-frequency sinusoidal electrical biasing of the MLLD's saturable absorber.

Main Results:

  • Achieved record megahertz optical sampling scan rates, a three-order-of-magnitude improvement over previous OSBERT demonstrations.
  • Successfully demonstrated real-time acquisition of a cross-correlation trace of two ultrashort optical pulses within 1 microsecond.
  • Validated the electronic tunability of the MLLD's repetition rate from sub-hertz to megahertz frequencies.

Conclusions:

  • The developed OSBERT system offers groundbreaking megahertz scan rates for time-resolved spectroscopy.
  • This advancement paves the way for highly competitive scan rates in various spectroscopic applications.
  • Potential applications include pump-probe spectroscopy, metrology, and other ultrafast optical measurements.