English (United Kingdom)

https://curated-unify.zendy.io/wp-json/zendy-region/v1/featured_content/oa?rat=en

https://curated-unify.zendy.io/wp-json/zendy-region/v1/highlighted_journal/

Global: Zendy Plus annual

Presents the access of premium content as premium feature

Premium Content

Presents the keyphrase highlighting as premium feature

Keyphrase Highlighting

Presents the summarisation as premium feature

Summarisation

Insights

Presents the pdf analysis as premium feature

PDF Analysis

Presents the zaia usage as premium feature

ZAIA

Global: Zendy Tools annual

Global: Zendy Free Plan

Global: Zendy Tools monthly

Global: Zendy Plus monthly

Traditional grating based spectrometers rely on a one-to-one spectral-to-spatial mapping. However, this one-to-one mapping is not required as long as distinct spectral signals are mapped to unique spatial intensity distributions. A calibration step is required to record this complex spectral-to-spatial mapping, but after calibration, the input spectra can be reconstructed simply by measuring the intensity distribution for an arbitrary input spectrum [1]. This approach has enabled a variety of dispersive media to be used in spectrometers, including a disordered photonic crystal lattice [1], an array of Bragg fibers [2], and even a random medium [3]. However, each of these dispersive media suffers high insertion loss, limiting the device performance.

Using a multimode fiber as a high resolution, low loss spectrometer