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Dataset for the journal article 'Effect of scattering loss on optimization of waveguide enhanced Raman spectroscopy'

Dataset for the journal article 'Effect of scattering loss on optimization of waveguide enhanced Raman spectroscopy'
Dataset for the journal article 'Effect of scattering loss on optimization of waveguide enhanced Raman spectroscopy'
The excel file contains all experimental and theoretical data used for generating Fig.2 to Fig.8 The figures are as follows: Fig 2. Excitation and waveguide coupling for a dipole on the cladding-core interface; (a) Normalized squared electric field at the core-cladding surface. (b) Signal capture efficiency in different modes for horizontal dipole. (c) Signal capture efficiency in different modes for vertical dipole. Fig 3. The propagation loss coefficient is plotted as a function of core thickness and correlation length for (a) TE0 mode and (b) TM0 mode. The surface roughness RMS amplitude is 1nm. The red lines mark the thickness that maximizes the surface modal field. (c) loss coefficient for the first three modes as a function of thickness with correlation length fixed at 180nm. The dot-dash line corresponding to the right y-axis is calculated by the widely used Payne's model. (d) The scattering loss from the film on S_i substrate with a 2 'm oxidized layer in between. Fig 4. Measured loss coefficient and comparison with the theoretical value for different modes. The Theoretical value is calculated by assuming the RMS, , is 1nm. The measured experimental loss coefficient is normalized to the mean square of the RMS amplitude, ^2. Fig 5. FOM calculations for forward collection as a function of core thickness and waveguide length for TE_0 pumping and signal collected as (a) TE_0, (b) TE_1, (c) TE_2 and (d) TM_0, (e) TM_1, (f) TM_2. Fig 6. FOM calculations for forward collection as a function of core thickness and waveguide length for TM_0 pumping and signal collected as (a) TE_0, (b) TE_1, (c) TE_2 and (d) TM_0, (e) TM_1, (f) TM_2. Fig 7. Total forward-collection FOM for different pumping polarization and modes. The pumping is in (a) TE_0, (b) TE_1, (c) TE_2 and (d) TM_0, (e) TM_1, (f) TM_2 polarization, for forward collection. Fig 8. Total backward-collection FOM for different pumping polarization and modes. The pumping is in (a) TE_0, (b) TE_1, (c) TE_2 and (d) TM_0, (e) TM_1, (f) TM_2 polarization, for backward collection.
University of Southampton
Liu, Zhen
ab2e4170-b059-48c1-8ac7-63ee8b8f10b3
Ettabib, Mohamed
71b98cd3-9b2a-4f73-b4c2-0f4b59cacf50
Wilkinson, James
73483cf3-d9f2-4688-9b09-1c84257884ca
Zervas, Michael
1840a474-dd50-4a55-ab74-6f086aa3f701
Liu, Zhen
ab2e4170-b059-48c1-8ac7-63ee8b8f10b3
Ettabib, Mohamed
71b98cd3-9b2a-4f73-b4c2-0f4b59cacf50
Wilkinson, James
73483cf3-d9f2-4688-9b09-1c84257884ca
Zervas, Michael
1840a474-dd50-4a55-ab74-6f086aa3f701

Liu, Zhen (2024) Dataset for the journal article 'Effect of scattering loss on optimization of waveguide enhanced Raman spectroscopy'. University of Southampton doi:10.5258/SOTON/D2452 [Dataset]

Record type: Dataset

Abstract

The excel file contains all experimental and theoretical data used for generating Fig.2 to Fig.8 The figures are as follows: Fig 2. Excitation and waveguide coupling for a dipole on the cladding-core interface; (a) Normalized squared electric field at the core-cladding surface. (b) Signal capture efficiency in different modes for horizontal dipole. (c) Signal capture efficiency in different modes for vertical dipole. Fig 3. The propagation loss coefficient is plotted as a function of core thickness and correlation length for (a) TE0 mode and (b) TM0 mode. The surface roughness RMS amplitude is 1nm. The red lines mark the thickness that maximizes the surface modal field. (c) loss coefficient for the first three modes as a function of thickness with correlation length fixed at 180nm. The dot-dash line corresponding to the right y-axis is calculated by the widely used Payne's model. (d) The scattering loss from the film on S_i substrate with a 2 'm oxidized layer in between. Fig 4. Measured loss coefficient and comparison with the theoretical value for different modes. The Theoretical value is calculated by assuming the RMS, , is 1nm. The measured experimental loss coefficient is normalized to the mean square of the RMS amplitude, ^2. Fig 5. FOM calculations for forward collection as a function of core thickness and waveguide length for TE_0 pumping and signal collected as (a) TE_0, (b) TE_1, (c) TE_2 and (d) TM_0, (e) TM_1, (f) TM_2. Fig 6. FOM calculations for forward collection as a function of core thickness and waveguide length for TM_0 pumping and signal collected as (a) TE_0, (b) TE_1, (c) TE_2 and (d) TM_0, (e) TM_1, (f) TM_2. Fig 7. Total forward-collection FOM for different pumping polarization and modes. The pumping is in (a) TE_0, (b) TE_1, (c) TE_2 and (d) TM_0, (e) TM_1, (f) TM_2 polarization, for forward collection. Fig 8. Total backward-collection FOM for different pumping polarization and modes. The pumping is in (a) TE_0, (b) TE_1, (c) TE_2 and (d) TM_0, (e) TM_1, (f) TM_2 polarization, for backward collection.

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Dataset for Effect of scattering loss on optimization of waveguide enhanced Raman spectroscopy.xlsx - Dataset
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Published date: 2024

Identifiers

Local EPrints ID: 486667
URI: http://eprints.soton.ac.uk/id/eprint/486667
PURE UUID: 1f5b51c1-2856-4846-972b-55c1431dae0a
ORCID for James Wilkinson: ORCID iD orcid.org/0000-0003-4712-1697
ORCID for Michael Zervas: ORCID iD orcid.org/0000-0002-0651-4059

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Date deposited: 31 Jan 2024 17:39
Last modified: 02 Feb 2024 02:33

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Contributors

Creator: Zhen Liu
Contributor: Mohamed Ettabib
Contributor: James Wilkinson ORCID iD
Contributor: Michael Zervas ORCID iD

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