Highlights

FIGURE 1. At the end of the fiber, the output field is no longer the same as the input field. To absorb the outgoing wave, a general absorbing artificial material is used (aka a perfectly matched layer).
FIGURE 1. At the end of the fiber, the output field is no longer the same as the input field. To absorb the outgoing wave, a general absorbing artificial material is used (aka a perfectly matched layer).
FIGURE 1. At the end of the fiber, the output field is no longer the same as the input field. To absorb the outgoing wave, a general absorbing artificial material is used (aka a perfectly matched layer).
FIGURE 1. At the end of the fiber, the output field is no longer the same as the input field. To absorb the outgoing wave, a general absorbing artificial material is used (aka a perfectly matched layer).
FIGURE 1. At the end of the fiber, the output field is no longer the same as the input field. To absorb the outgoing wave, a general absorbing artificial material is used (aka a perfectly matched layer).
Software & Accessories

Full-wave multiphysics simulation of optical fibers

July 25, 2022
Full-wave multiphysics simulations for optical fibers require sophisticated modeling and simulation techniques.
FIGURE 3. 4D image of a dividing cell that was detected by Aivia in a feedback loop with LAS X from Leica Microsystems.
FIGURE 3. 4D image of a dividing cell that was detected by Aivia in a feedback loop with LAS X from Leica Microsystems.
FIGURE 3. 4D image of a dividing cell that was detected by Aivia in a feedback loop with LAS X from Leica Microsystems.
FIGURE 3. 4D image of a dividing cell that was detected by Aivia in a feedback loop with LAS X from Leica Microsystems.
FIGURE 3. 4D image of a dividing cell that was detected by Aivia in a feedback loop with LAS X from Leica Microsystems.
Bio&Life Sciences

How AI and other microscopy advances answer complex life science questions

Nov. 7, 2023
Microscopy enabled by artificial intelligence (AI) will improve life sciences research and development across key therapeutic categories. Promising developments include autonomous...
Thinoxide Software
Thinoxide Software
Thinoxide Software
Thinoxide Software
Thinoxide Software
Software & Accessories

Web-based thin-film design software program available

Oct. 21, 2023
Thinoxide is a free, web-based software that provides a graphical implementation of the thin-film transfer-matrix method for prototyping interference-based structures such as ...
Mks Ophir
Mks Ophir
Mks Ophir
Mks Ophir
Mks Ophir
Software & Accessories

Laser beam analysis software is designed for additive manufacturing

Sept. 24, 2023
BeamPeek software is designed for real-time measurement of lasers in additive manufacturing chambers.
(Image credit: Flexcompute)
FIGURE 1. Schematic illustration of the PSR (a), simulated mode conversion efficiencies at the top and bottom waveguides with TE0 mode as the input (b), and simulated mode conversion efficiencies at the top and bottom waveguides with TM0 mode as the input (c) are shown. The insets show the field intensity plots.
FIGURE 1. Schematic illustration of the PSR (a), simulated mode conversion efficiencies at the top and bottom waveguides with TE0 mode as the input (b), and simulated mode conversion efficiencies at the top and bottom waveguides with TM0 mode as the input (c) are shown. The insets show the field intensity plots.
FIGURE 1. Schematic illustration of the PSR (a), simulated mode conversion efficiencies at the top and bottom waveguides with TE0 mode as the input (b), and simulated mode conversion efficiencies at the top and bottom waveguides with TM0 mode as the input (c) are shown. The insets show the field intensity plots.
FIGURE 1. Schematic illustration of the PSR (a), simulated mode conversion efficiencies at the top and bottom waveguides with TE0 mode as the input (b), and simulated mode conversion efficiencies at the top and bottom waveguides with TM0 mode as the input (c) are shown. The insets show the field intensity plots.
FIGURE 1. Schematic illustration of the PSR (a), simulated mode conversion efficiencies at the top and bottom waveguides with TE0 mode as the input (b), and simulated mode conversion efficiencies at the top and bottom waveguides with TM0 mode as the input (c) are shown. The insets show the field intensity plots.
Software & Accessories

Breaking time barriers: Millimeter-scale photonic simulations in minutes

Sept. 20, 2023
Two case studies demonstrate the transformative impact of advanced parallel computing on the field of computational electromagnetics.
Photo 277698908 © Yuriy Nedopekin | Dreamstime.com
Dreamstime Xxl 277698908
Dreamstime Xxl 277698908
Dreamstime Xxl 277698908
Dreamstime Xxl 277698908
Dreamstime Xxl 277698908
Software & Accessories

Simulation and modeling for quantum photonics

June 14, 2023
Ivan Nikitski, EPIC’s Photonics Technology program manager, talks to Mirella Koleva, CEO and cofounder of Quantopticon, makers of simulation software to streamline the design ...
Vp Iphotonics
Vp Iphotonics
Vp Iphotonics
Vp Iphotonics
Vp Iphotonics
Software & Accessories

Simulation software offers over 900 ready-to-run simulation setups

June 11, 2023
Design Suite Version 11.4 advances the simulation and design flow for applications including free-space optics, among others.
(From C. Ancuti, C. O. Ancuti, C. De Vleeschouwer, and A. C. Bovik [4])
A dehazed image by global light estimation.
A dehazed image by global light estimation.
A dehazed image by global light estimation.
A dehazed image by global light estimation.
A dehazed image by global light estimation.
Detectors & Imaging

Airlight estimation for simultaneous day and night image dehazing applications

May 19, 2023
Image dehazing is an important area of research used for security, surveillance, and outdoor imaging. Getting rid of haze from pictures taken at night is hard because there is...
Zygo
Zygo
Zygo
Zygo
Zygo
Software & Accessories

Metrology software integrates asphere surface analysis

May 16, 2023
Mx software integrates acquisition and data analysis for surface topography and wavefront data.