Materials Map

Discover the materials research landscape. Find experts, partners, networks.

  • About
  • Privacy Policy
  • Legal Notice
  • Contact

The Materials Map is an open tool for improving networking and interdisciplinary exchange within materials research. It enables cross-database search for cooperation and network partners and discovering of the research landscape.

The dashboard provides detailed information about the selected scientist, e.g. publications. The dashboard can be filtered and shows the relationship to co-authors in different diagrams. In addition, a link is provided to find contact information.

×

Materials Map under construction

The Materials Map is still under development. In its current state, it is only based on one single data source and, thus, incomplete and contains duplicates. We are working on incorporating new open data sources like ORCID to improve the quality and the timeliness of our data. We will update Materials Map as soon as possible and kindly ask for your patience.

To Graph

1.080 Topics available

To Map

977 Locations available

693.932 PEOPLE
693.932 People People

693.932 People

Show results for 693.932 people that are selected by your search filters.

←

Page 1 of 27758

→
←

Page 1 of 0

→
PeopleLocationsStatistics
Naji, M.
  • 2
  • 13
  • 3
  • 2025
Motta, Antonella
  • 8
  • 52
  • 159
  • 2025
Aletan, Dirar
  • 1
  • 1
  • 0
  • 2025
Mohamed, Tarek
  • 1
  • 7
  • 2
  • 2025
Ertürk, Emre
  • 2
  • 3
  • 0
  • 2025
Taccardi, Nicola
  • 9
  • 81
  • 75
  • 2025
Kononenko, Denys
  • 1
  • 8
  • 2
  • 2025
Petrov, R. H.Madrid
  • 46
  • 125
  • 1k
  • 2025
Alshaaer, MazenBrussels
  • 17
  • 31
  • 172
  • 2025
Bih, L.
  • 15
  • 44
  • 145
  • 2025
Casati, R.
  • 31
  • 86
  • 661
  • 2025
Muller, Hermance
  • 1
  • 11
  • 0
  • 2025
Kočí, JanPrague
  • 28
  • 34
  • 209
  • 2025
Šuljagić, Marija
  • 10
  • 33
  • 43
  • 2025
Kalteremidou, Kalliopi-ArtemiBrussels
  • 14
  • 22
  • 158
  • 2025
Azam, Siraj
  • 1
  • 3
  • 2
  • 2025
Ospanova, Alyiya
  • 1
  • 6
  • 0
  • 2025
Blanpain, Bart
  • 568
  • 653
  • 13k
  • 2025
Ali, M. A.
  • 7
  • 75
  • 187
  • 2025
Popa, V.
  • 5
  • 12
  • 45
  • 2025
Rančić, M.
  • 2
  • 13
  • 0
  • 2025
Ollier, Nadège
  • 28
  • 75
  • 239
  • 2025
Azevedo, Nuno Monteiro
  • 4
  • 8
  • 25
  • 2025
Landes, Michael
  • 1
  • 9
  • 2
  • 2025
Rignanese, Gian-Marco
  • 15
  • 98
  • 805
  • 2025

Guilmo, Anael

  • Google
  • 2
  • 8
  • 32

in Cooperation with on an Cooperation-Score of 37%

Topics

Publications (2/2 displayed)

  • 2010Mach-Zehnder interferometry method for decoupling electro-optic and piezoelectric effects in poled polymer films29citations
  • 2010Mach-Zehnder interferometry method for decoupling electro-optic and piezoelectric tensor components in poled polymer films3citations

Places of action

Chart of shared publication
Huang, Su
2 / 3 shared
Zhou, Xing-Hua
2 / 2 shared
Himmelhuber, Roland
2 / 3 shared
Fallahi, Mahmoud
2 / 2 shared
Norwood, Robert A.
2 / 5 shared
Greenlee, Charles
2 / 2 shared
Opadeyi, Ayodeji
2 / 2 shared
Peyghambarian, Nasser
2 / 4 shared
Chart of publication period
2010

Co-Authors (by relevance)

  • Huang, Su
  • Zhou, Xing-Hua
  • Himmelhuber, Roland
  • Fallahi, Mahmoud
  • Norwood, Robert A.
  • Greenlee, Charles
  • Opadeyi, Ayodeji
  • Peyghambarian, Nasser
OrganizationsLocationPeople

document

Mach-Zehnder interferometry method for decoupling electro-optic and piezoelectric tensor components in poled polymer films

  • Huang, Su
  • Zhou, Xing-Hua
  • Himmelhuber, Roland
  • Fallahi, Mahmoud
  • Norwood, Robert A.
  • Greenlee, Charles
  • Guilmo, Anael
  • Opadeyi, Ayodeji
  • Peyghambarian, Nasser
Abstract

A Mach-Zehnder interferometer (MZI) is used to decouple the electro-optic (EO) and piezoelectric tensor components for a poled polymer film. In the past those using the MZI method failed to take into account the piezoelectric contribution in the polymer which can lead to erroneous EO coefficient data. The typical poled sample of polymer sandwiched between ITO glass and gold that was developed for the popular Teng-Man reflection ellipsometry method is used, providing for easy comparison with that method. The sample serves as a mirror in one arm of the interferometer with the gold side facing the beam for measuring the piezoelectric modulation and the glass side facing the beam to measure the coupled piezoelectric and EO modulation. Optical biasing in the reference arm allows for the baseline and modulated contrast of the system to be measured from which the tensor components are calculated. This method has the advantage over the reflection ellipsometry method of allowing for the independent determination of the Pockel's coefficients r<sub>13</sub> and r<sub>33</sub> and the piezoelectric coefficient d<sub>33</sub>. The r<sub>33</sub> value of a guest host polymer that consists of AJLZ53/amorphous polycarbonate (APC) was found to be 122.7 pm/V and 123.0 pm/V for the MZI and reflection ellipsometry method respectively. The r<sub>33</sub> data fits well to the dispersion of the second order susceptibility tensor χ<sub>333</sub><sup>(2)</sup> based on the two-level model approximation. Measurements were done from 100 Hz to 100 kHz with the results showing that at higher frequencies the mechanical effects in the sample are negligible and modulation is almost entirely due to the EO effect, as expected.  

Topics
  • impedance spectroscopy
  • dispersion
  • polymer
  • amorphous
  • glass
  • glass
  • gold
  • ellipsometry
  • susceptibility
  • interferometry