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 Experiment Video

Updated: Jun 8, 2026

A Random-displacement Measurement by Combining a Magnetic Scale and Two Fiber Bragg Gratings
08:23

A Random-displacement Measurement by Combining a Magnetic Scale and Two Fiber Bragg Gratings

Published on: September 30, 2019

Modulation transfer function measurement of sparse-array sensors using a self-calibrating fringe pattern.

J E Greivenkamp, A E Lowman

    Applied Optics
    |October 12, 2010
    PubMed
    Summary
    This summary is machine-generated.

    Related Concept Videos

    You might also read

    Related Articles

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

    Sort by
    Same author

    Interferometer errors due to the presence of fringes.

    Applied optics·2010
    Same author

    Measurement of two-dimensional small rotation angles by using orthogonal parallel interference patterns.

    Applied optics·2010
    Same author

    Modeling soft contact lenses in raytrace code.

    Applied optics·2010
    Same author

    Measurement of small rotation angles by using a parallel interference pattern.

    Applied optics·2010
    Same author

    Color dependent optical prefilter for the suppression of aliasing artifacts.

    Applied optics·2010
    Same author

    Sub-Nyquist interferometry.

    Applied optics·2010
    Same journal

    Multifunctional reconfigurable terahertz metasurface based on vanadium dioxide phase transition: achieving broadband absorption and efficient polarization conversion.

    Applied optics·2026
    Same journal

    High-Q-factor electromagnetically induced transparency utilizing quasi-bound states in the continuum in an all-dielectric terahertz metasurface.

    Applied optics·2026
    Same journal

    Automated stitching interferometry for high-precision metrology of X-ray mirrors.

    Applied optics·2026
    Same journal

    Experimental demonstration of an approach to designing a metal-dielectric DBR resonant cavity structure.

    Applied optics·2026
    Same journal

    High-precision wavefront reconstruction from a single-shot interferogram using a physics-driven hybrid feature calibration network.

    Applied optics·2026
    Same journal

    Ultra-high-Q Fano resonance based on coupled topological corner states in Kagome photonic crystals.

    Applied optics·2026
    See all related articles

    A new method measures the pixel modulation transfer function (MTF) of sparse-array sensors using a Twyman-Green interferometer. This technique enables self-calibration and accurate MTF assessment at high spatial frequencies.

    Area of Science:

    • Optical engineering
    • Sensor technology
    • Metrology

    Background:

    • Accurate measurement of sensor performance is crucial for imaging systems.
    • Characterizing the modulation transfer function (MTF) reveals spatial resolution limitations.
    • Sparse-array sensors present unique challenges for traditional MTF measurement techniques.

    Purpose of the Study:

    • To develop a simple and self-calibrating method for measuring the pixel modulation transfer function (MTF) of sparse-array sensors.
    • To extend the measurement capability to high spatial frequencies beyond the sensor's sampling limit.
    • To investigate the influence of sensor characteristics on MTF at specific spatial frequencies.

    Main Methods:

    • Utilized a phase-shifting Twyman-Green interferometer to generate precise fringe patterns.

    More Related Videos

    Micro/Nano-scale Strain Distribution Measurement from Sampling Moiré Fringes
    06:56

    Micro/Nano-scale Strain Distribution Measurement from Sampling Moiré Fringes

    Published on: May 23, 2017

    Transmission of Multiple Signals through an Optical Fiber Using Wavefront Shaping
    09:43

    Transmission of Multiple Signals through an Optical Fiber Using Wavefront Shaping

    Published on: March 20, 2017

    Related Experiment Videos

    Last Updated: Jun 8, 2026

    A Random-displacement Measurement by Combining a Magnetic Scale and Two Fiber Bragg Gratings
    08:23

    A Random-displacement Measurement by Combining a Magnetic Scale and Two Fiber Bragg Gratings

    Published on: September 30, 2019

    Micro/Nano-scale Strain Distribution Measurement from Sampling Moiré Fringes
    06:56

    Micro/Nano-scale Strain Distribution Measurement from Sampling Moiré Fringes

    Published on: May 23, 2017

    Transmission of Multiple Signals through an Optical Fiber Using Wavefront Shaping
    09:43

    Transmission of Multiple Signals through an Optical Fiber Using Wavefront Shaping

    Published on: March 20, 2017

  • Incident fringe patterns were directed onto the sparse-array sensor, and signal modulation was measured.
  • Employed self-calibration by measuring at multiples of the Nyquist frequency, leveraging unique aliased patterns.
  • Main Results:

    • Successfully measured spatial frequencies up to 480 cycles/mm, exceeding ten times the sensor's sampling frequency.
    • Observed expected MTF shapes at multiples of the sensor's sampling frequency.
    • Identified that electronic bandwidth and crosstalk in charge-injection device (CID) sensors affect MTF at odd multiples of the Nyquist frequency.

    Conclusions:

    • The developed method provides a straightforward and accurate approach for extended MTF measurement of sparse-array sensors.
    • The technique allows for high-frequency characterization, revealing performance limitations beyond the Nyquist frequency.
    • Understanding the impact of electronic bandwidth and crosstalk is essential for optimizing CID sensor performance.