Evidence map›Paper›PMID 31288404›Full record

ArticleSensors (Basel, Switzerland)2019

Resonant Grating without a Planar Waveguide Layer as a Refractive Index Sensor.

Sivan Isaacs, Ansar Hajoj, Mohammad Abutoama, Alexander Kozlovsky, Erez Golan, Ibrahim Abdulhalim

Abstract read
In one paragraph

Article in Sensors (Basel, Switzerland), 2019. The graph could read no effect estimate from its abstract, so it casts no vote on the map. Cited by 10 papers.

0numbers the graph read from it
0cells of the map it votes in
10citing papers in PubMed
–field-weighted citation impact
1 · What the graph read from it

What it found

Each row is one number read from the abstract, on the scale the paper reported it, with its interval. Left of the dashed line favours the treatment, right favours the comparator. Under each row is the sentence it came from. New to these charts? A ten-minute tutorial.

The abstract states no effect estimate the extractor could read, or names no intervention and outcome on the map, so this paper lights no cell and moves no belief. It is still indexed, cited and linked below.

2 · The registry

The trial behind it

Trials whose registry record cites this paper, or whose number appears in the abstract. A trial that started after this paper was published is citing it as background, not reporting it.

Neither the registry nor the abstract names a trial number. If this is a trial report, that itself is worth knowing.

3 · Its place in the literature

Who cites it

10 citing papers in PubMed.

  1. Article
  2. Article
  3. Article
  4. Article
  5. Photonic Bound States in the Continuum in Nanostructures.Materials (Basel, Switzerland) · 2023
    Review
  6. Article
  7. Pedestal High-Contrast Gratings for Biosensing.Nanomaterials (Basel, Switzerland) · 2022
    Article
  8. Article
  9. Article
  10. Article
4 · The record

Corrections and comments

PubMed lists nothing against this paper. Absence here is not a guarantee, only a check that was made.

5 · Who and what money

Authors and funding

6 authors.

Sivan IsaacsDepartment of Electrooptics and Photonics Engineering and The Ilse Katz Institute for Nanoscale Science and Technology, School of Electrical and Computer Engineering, Ben Gurion University of the Negev, Beer Sheva 84105, Israel.ORCID 0000-0001-8657-7246
Ansar HajojDepartment of Electrooptics and Photonics Engineering and The Ilse Katz Institute for Nanoscale Science and Technology, School of Electrical and Computer Engineering, Ben Gurion University of the Negev, Beer Sheva 84105, Israel.
Mohammad AbutoamaDepartment of Electrooptics and Photonics Engineering and The Ilse Katz Institute for Nanoscale Science and Technology, School of Electrical and Computer Engineering, Ben Gurion University of the Negev, Beer Sheva 84105, Israel.
Alexander KozlovskyThe Weiss Family Laboratory for Nano-scale Systems, Ben-Gurion University of the Negev, Beer Sheva 84105, Israel.
Erez GolanThe Weiss Family Laboratory for Nano-scale Systems, Ben-Gurion University of the Negev, Beer Sheva 84105, Israel.
Ibrahim AbdulhalimDepartment of Electrooptics and Photonics Engineering and The Ilse Katz Institute for Nanoscale Science and Technology, School of Electrical and Computer Engineering, Ben Gurion University of the Negev, Beer Sheva 84105, Israel. abdulhlm@bgu.ac.il.ORCID 0000-0002-1474-5412

Funding

No grant is acknowledged in the PubMed record.

6 · The paper itself

Abstract

Dielectric grating-based sensors are usually based on the guided mode resonance (GMR) obtained using a thin planar waveguide layer (PWL) adjacent to a thin subwavelength grating layer. In this work, we present a detailed investigation of thick subwavelength dielectric grating structures that exhibit reflection resonances above a certain thickness without the need for the waveguide layer, showing great potential for applications in biosensing and tunable filtering. Analytic and numerical results are thoroughly discussed, as well as an experimental demonstration of the structure as a chemical sensor in the SWIR (short wave infrared) spectral range (1200-1800 nm). In comparison to the GMR structure with PWL, the thick grating structure has several unique properties: (i) It gives higher sensitivity when the spaces are filled, with the analyte peaking at certain space values due to an increase in the interaction volume between the analyte and the evanescent optical field between the grating lines; (ii) the TM (transverse magnetic) resonance, in certain cases, provides a better figure of merit; (iii) the sensitivity increases as the grating height increases; (iii) the prediction of the resonance locations based on the effective medium approximation does not give satisfactory results when the grating height is larger than a certain value, and the invalidity becomes more severe as the period increases; (iv) a sudden increase in the Q-factor of the resonance occurs at a specific height value accompanied by the high local field enhancement (~10

Indexed as

biosensorsgratings sensorsguided mode resonancewaveguide sensors

Identifiers

PMID31288404
PMCPMC6651248

What OpenQuestion holds

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Registered trials

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Read under generation 80e0d062 · epoch 390. Bibliography from PubMed, PubMed Central and OpenAlex; grants from NIH RePORTER; trial links from ClinicalTrials.gov; estimates, votes and beliefs from the OpenQuestion graph.