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

Parallel Resonance01:23

Parallel Resonance

The parallel RLC circuit is an arrangement where the resistor (R), inductor (L), and capacitor (C) are all connected to the same nodes and, as a result, share the same voltage across them. The parallel RLC circuit is analyzed in terms of admittance (Y), which reflects the ease with which current can flow. The admittance is given by:
Double Resonance Techniques: Overview01:12

Double Resonance Techniques: Overview

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...
RLC Circuit as a Damped Oscillator01:30

RLC Circuit as a Damped Oscillator

An RLC circuit combines a resistor, inductor, and capacitor, connected in a series or parallel combination.
Consider a series RLC circuit. Here, the presence of resistance in the circuit leads to energy loss due to joule heating in the resistance. Therefore, the total electromagnetic energy in the circuit is no longer constant and decreases with time. Since the magnitude of charge, current, and potential difference continuously decreases, their oscillations are said to be damped. This is...
Series Resonance01:17

Series Resonance

The RLC circuit impedance is defined as the ratio of the supply voltage to the circuit current. Resonance in such a circuit occurs when the imaginary part of this impedance equals zero. This specific condition means that the inductive reactance is exactly equal to the capacitive reactance. The frequency at which this happens is known as the resonant frequency. Mathematically, the resonant frequency is inversely proportional to the square root of the product of the inductance (L) and capacitance...
Characteristics of Series Resonant Circuit01:24

Characteristics of Series Resonant Circuit

Series resonance occurs in a circuit containing inductive (L), capacitive (C), and resistive (R) elements connected sequentially. At the resonance frequency, the inductive and capacitive reactances are equal in magnitude but opposite in sign, effectively canceling each other. This causes the circuit's impedance is minimal, primarily determined by the resistance R. The resonant frequency of an RLC circuit is defined as:
Clamper Circuit01:14

Clamper Circuit

A clamper circuit, also known as a DC restorer, represents a specialized variant of the rectifier circuit, notable for its method of taking the output across the diode rather than the capacitor. This configuration lends to several distinctive applications, particularly in handling square wave inputs.
Within this circuit, the diode's orientation prompts the capacitor to charge up to the level of the most negative peak of the input signal. Upon reaching this state, the diode ceases to conduct,...

You might also read

Related Articles

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

Sort by
Same author

Amplification and attenuation of light in a waveguide modulated by a travelling wave.

Optics express·2026
Same author

Potentials with partly constant free spectral range and their application to SNAP microresonators.

Optics letters·2025
Same author

SNAP microwave optical filters.

Optics letters·2021
Same author

Enhancing the impedance matched bandwidth of bottle microresonator signal processing devices.

Optics letters·2021
Same author

Fundamental limit of microresonator field uniformity and slow light enabled ultraprecise displacement metrology.

Optics letters·2021
Same author

Microresonator devices lithographically introduced at the optical fiber surface.

Optics letters·2021
Same journal

Denoising algorithm of Φ-OTDR systems based on adaptive fractional wavelet transform denoising.

Optics express·2026
Same journal

Millisecond photon-to-photon latency and high-speed volumetric projection system for optogenetics.

Optics express·2026
Same journal

Polarization-encoded coaxial structured light for high-precision 3D surface profilometry.

Optics express·2026
Same journal

Discrete freeform optical design based on collaborative optimization of point cloud and local normals.

Optics express·2026
Same journal

Ultrafast ghost imaging with 25 GHz speckle switching and wavelength-division multiplexing.

Optics express·2026
Same journal

Atomic vapor cells fabricated by femtosecond laser welding of standard-optical-quality glass.

Optics express·2026
See all related articles

Related Experiment Video

Updated: May 9, 2026

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

A SNAP coupled microresonator delay line.

M Sumetsky1

  • 1OFS Laboratories, 19 Schoolhouse Road, Somerset, NJ 08873, USA. sumetski@ofsoptics.com

Optics Express
|July 12, 2013
PubMed
Summary
This summary is machine-generated.

This study demonstrates a novel Surface Nanoscale Axial Photonics (SNAP) delay line. This device utilizes a unique 3D light propagation effect to achieve a slow light speed and significant delay times with low loss.

More Related Videos

Fabrication and Characterization of Superconducting Resonators
10:26

Fabrication and Characterization of Superconducting Resonators

Published on: May 21, 2016

Fabrication and Characterization of High-Q Silicon Nitride Membrane Resonators
09:46

Fabrication and Characterization of High-Q Silicon Nitride Membrane Resonators

Published on: August 8, 2025

Related Experiment Videos

Last Updated: May 9, 2026

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

Fabrication and Characterization of Superconducting Resonators
10:26

Fabrication and Characterization of Superconducting Resonators

Published on: May 21, 2016

Fabrication and Characterization of High-Q Silicon Nitride Membrane Resonators
09:46

Fabrication and Characterization of High-Q Silicon Nitride Membrane Resonators

Published on: August 8, 2025

Area of Science:

  • Photonics
  • Optical Engineering
  • Materials Science

Background:

  • Traditional resonant delay lines face limitations in achieving significant light delay and low loss.
  • Surface Nanoscale Axial Photonics (SNAP) offers a novel approach for light manipulation due to its 3D light propagation capabilities.

Purpose of the Study:

  • To demonstrate a delay line based on a chain of coupled SNAP microresonators.
  • To investigate the slow light enhancement via the 2R (Rotation + Reflection) effect in SNAP structures.
  • To characterize the performance of the SNAP delay line in terms of delay time, bandwidth, and insertion loss.

Main Methods:

  • Fabrication of a delay line using 20 coupled SNAP microresonators.
  • Characterization of light propagation and delay properties in a reflection-mode configuration.
  • Analysis of the influence of coupling parameters and loss on delay time.

Main Results:

  • Demonstration of a SNAP delay line with a total length of 1.2 mm and footprint of 0.05 mm².
  • Achieved a record low insertion loss (< 3 dB) and a slow light speed (< c/250).
  • Obtained a large delay time (> 1 ns) over a 0.1 nm bandwidth, outperforming existing miniature microresonator delay lines.

Conclusions:

  • The SNAP delay line effectively utilizes the 2R effect for enhanced slow light.
  • The demonstrated device exhibits record performance metrics for miniature delay lines.
  • Future improvements in delay time, bandwidth, losses, and dimensions are feasible through advanced design techniques.