Marylline Guilloux-Viry
Current Organizations / Institutes
The organizations/institutes from the scholar's latest article
Previous Organizations / Institutes
The organizations / institutes from the scholar's other articles in the past ten years
Research Subjects
Marylline Guilloux-Viry has a total of 487 co-authors. Here are the top co-authors by number of shared publications:
- AndrÉ Perrin
Centre National de la Recherche Scientifique
101 shared publications - Stephanie Deputier
Université de Rennes 1
59 shared publications - Valerie Bouquet
Université de Rennes 1
51 shared publications M. Sergent
Laboratoire de Chimie du Solide et Inorganique Moléculaire (UMR CNRS 6511), Université de Rennes I, campus de Beaulieu, 35042 Rennes Cedex, France
21 shared publications- Gerard Tanne
Centre National de la Recherche Scientifique
18 shared publications C. Thivet
16 shared publications
Latest Publications
- 1 July 2026
- Published by Societe Chimique de France
- Vol. 516-517, 55-59
Apport de la cristallochimie à l’optimisation de couches minces d’oxydes sans plomb par ablation laser pulsé
(Text in French) Contribution of crystallochemistry to the optimization of lead-free oxide thin films by pulsed laser deposition. Through interdisciplinary research, this article presents several aspects of the crystallochemistry of thin films grown by pulsed laser deposition, which contributes to i) optimizing lead-free piezoelectric and ferroelectric materials on single-crystal substrates, ii) control the crystalline characteristics of thin films on less expensive substrates, iii) the introduction of thin films of interest into energy conversion technology, and iv) explore phase-change materials for new, high-performance devices for information processing that consume less energy.
- 1 July 2026
- Published by Societe Chimique de France
- Vol. 516-517, 55-59
Apport de la cristallochimie à l’optimisation de couches minces d’oxydes sans plomb par ablation laser pulsé
(Text in French) Contribution of crystallochemistry to the optimization of lead-free oxide thin films by pulsed laser deposition. Through interdisciplinary research, this article presents several aspects of the crystallochemistry of thin films grown by pulsed laser deposition, which contributes to i) optimizing lead-free piezoelectric and ferroelectric materials on single-crystal substrates, ii) control the crystalline characteristics of thin films on less expensive substrates, iii) the introduction of thin films of interest into energy conversion technology, and iv) explore phase-change materials for new, high-performance devices for information processing that consume less energy.
- Open Access
- 20 November 2025
- Published by Royal Society of Chemistry (RSC) in Journal of Materials Chemistry C
- Vol. 13 (45) , 22712-22721
Influence of K 4 Nb 6 O 17 secondary phase on ferroelectric behavior of K 0.5 Na 0.5 NbO 3 thin films
K-enriched KNN target effectively prevents alkali cation deficiency, ensuring typical piezoelectric and ferroelectric behavior. In particular, it avoids the secondary phase K 4 Nb 6 O 17 in KNN thin films obtained by PLD using a stoichiometric target.
- 20 November 2025
- Published by Royal Society of Chemistry (RSC) in Journal of Materials Chemistry C
- Vol. 13 (45) , 22712-22721
Open AccessInfluence of K 4 Nb 6 O 17 secondary phase on ferroelectric behavior of K 0.5 Na 0.5 NbO 3 thin films
K-enriched KNN target effectively prevents alkali cation deficiency, ensuring typical piezoelectric and ferroelectric behavior. In particular, it avoids the secondary phase K 4 Nb 6 O 17 in KNN thin films obtained by PLD using a stoichiometric target.
- 5 December 2022
- Published by AIP Publishing in Applied Physics Letters
- Vol. 121 (23) , 232901
Effect of electrically induced cracks on the properties of PZT thin film capacitors
We present a study of the effect of electrically induced cracks on both the ferroelectric and piezoelectric properties of Pt/PbZr0.52Ti0.48O3 (PZT)/Pt capacitors and correlations with domain structures of PZT films. Above a threshold bipolar electric field, cracks appear inside the PZT layer thickness leading to an increase in the ferroelectric polarization (+50% for the remnant polarization, from 16 to 25 μC/cm2) and the longitudinal piezoelectric coefficient d33,f (from ∼150 to ∼220 pm/V). The use of x-ray diffraction during in situ biasing provides direct evidence for a modification of the PZT crystalline structure as well as the a/c domain configuration. After cracking, the fraction of c-domains is strongly increased, thus contributing to higher polarization and larger strain in the out-of-plane direction.
- 5 December 2022
- Published by AIP Publishing in Applied Physics Letters
- Vol. 121 (23) , 232901
Effect of electrically induced cracks on the properties of PZT thin film capacitors
We present a study of the effect of electrically induced cracks on both the ferroelectric and piezoelectric properties of Pt/PbZr0.52Ti0.48O3 (PZT)/Pt capacitors and correlations with domain structures of PZT films. Above a threshold bipolar electric field, cracks appear inside the PZT layer thickness leading to an increase in the ferroelectric polarization (+50% for the remnant polarization, from 16 to 25 μC/cm2) and the longitudinal piezoelectric coefficient d33,f (from ∼150 to ∼220 pm/V). The use of x-ray diffraction during in situ biasing provides direct evidence for a modification of the PZT crystalline structure as well as the a/c domain configuration. After cracking, the fraction of c-domains is strongly increased, thus contributing to higher polarization and larger strain in the out-of-plane direction.
- Open Access
- 16 July 2022
- Published by MDPI AG in Chemosensors
- Vol. 10 (7) , 285
Effect of the Microstructure of ZnO Thin Films Prepared by PLD on Their Performance as Toxic Gas Sensors
In 2008, the modified European Restriction of Hazardous Substances (RoHS) directive prohibited the use of hazardous substances such as lead, cadmium, and mercury. As such, an urgent need for lead-free components emerged in Europe. In this frame, we have decided to study the microstructure influence of zinc oxide thin films on the detection of hydrogen sulfide (H2S). Zinc oxide thin films were deposited by PLD on silicon substrates under different conditions to modify the microstructure. In order to compare our demonstrators to current commercial semiconductor gas sensors, measurements under H2S were also performed with sensors from Figaro and Winsen corporations. Gas sensors were therefore implemented by using commercial cases in view to test them with Simtronics gas detector DG477. The good sensitivity values measured at T = 400 °C under 100 ppm H2S, and response times as low as 30 s, definitely confirm that ZnO thin films could be developed for commercial sensors.
- 16 July 2022
- Published by MDPI AG in Chemosensors
- Vol. 10 (7) , 285
Open AccessEffect of the Microstructure of ZnO Thin Films Prepared by PLD on Their Performance as Toxic Gas Sensors
In 2008, the modified European Restriction of Hazardous Substances (RoHS) directive prohibited the use of hazardous substances such as lead, cadmium, and mercury. As such, an urgent need for lead-free components emerged in Europe. In this frame, we have decided to study the microstructure influence of zinc oxide thin films on the detection of hydrogen sulfide (H2S). Zinc oxide thin films were deposited by PLD on silicon substrates under different conditions to modify the microstructure. In order to compare our demonstrators to current commercial semiconductor gas sensors, measurements under H2S were also performed with sensors from Figaro and Winsen corporations. Gas sensors were therefore implemented by using commercial cases in view to test them with Simtronics gas detector DG477. The good sensitivity values measured at T = 400 °C under 100 ppm H2S, and response times as low as 30 s, definitely confirm that ZnO thin films could be developed for commercial sensors.
- 27 May 2021
- Published by Institute of Electrical and Electronics Engineers (IEEE) in IEEE Antennas and Wireless Propagation Letters
- Vol. 20 (8) , 1414-1418
Frequency-Tunable Slot-Loop Antenna Based on KNN Ferroelectric Interdigitated Varactors
A miniature frequency-tunable slot-loop antenna (0.128λ 0 × 0.077λ 0 ) based on ferroelectric K 0.5 Na 0.5 NbO 3 (KNN) interdigitated varactors is investigated at Ku-band. KNN material has been selected among the ferroelectric oxide family because of its competitive properties for microwave applications. Its high permittivity value (ϵ r ≈ 360 at 10 GHz) and its wide frequency tunability under an external static electric field E bias make it a promising candidate for frequency-agile antennas and circuits at microwaves. The antenna prototype has been designed and elaborated on MgO substrate (ϵ r = 9.8 and tanδ ≈ 10 -4 at 10 GHz). Fabrication details including laser microetching process of the ferroelectric layer are also described. The center frequency of the slot-loop antenna can therefore be tuned monotonously from 15.22 to 15.97 GHz under E bias = 88 kV/cm, leading to a frequency tunability rate equal to 4.6%. These results demonstrate for the first time the ability of the KNN material to be used for miniature tunable antennas, in comparison with Ba x Sr 1-x TiO 3 , currently considered as the most relevant material for such applications.
- 27 May 2021
- Published by Institute of Electrical and Electronics Engineers (IEEE) in IEEE Antennas and Wireless Propagation Letters
- Vol. 20 (8) , 1414-1418
Frequency-Tunable Slot-Loop Antenna Based on KNN Ferroelectric Interdigitated Varactors
A miniature frequency-tunable slot-loop antenna (0.128λ 0 × 0.077λ 0 ) based on ferroelectric K 0.5 Na 0.5 NbO 3 (KNN) interdigitated varactors is investigated at Ku-band. KNN material has been selected among the ferroelectric oxide family because of its competitive properties for microwave applications. Its high permittivity value (ϵ r ≈ 360 at 10 GHz) and its wide frequency tunability under an external static electric field E bias make it a promising candidate for frequency-agile antennas and circuits at microwaves. The antenna prototype has been designed and elaborated on MgO substrate (ϵ r = 9.8 and tanδ ≈ 10 -4 at 10 GHz). Fabrication details including laser microetching process of the ferroelectric layer are also described. The center frequency of the slot-loop antenna can therefore be tuned monotonously from 15.22 to 15.97 GHz under E bias = 88 kV/cm, leading to a frequency tunability rate equal to 4.6%. These results demonstrate for the first time the ability of the KNN material to be used for miniature tunable antennas, in comparison with Ba x Sr 1-x TiO 3 , currently considered as the most relevant material for such applications.
- 1 January 2020
- Published by Elsevier in Thin Solid Films
- Vol. 693
Orientation control of KNbO3 film grown on glass substrates by Ca2Nb3O10− nanosheets seed layer
- 1 January 2020
- Published by Elsevier in Thin Solid Films
- Vol. 693
Orientation control of KNbO3 film grown on glass substrates by Ca2Nb3O10− nanosheets seed layer
- 21 June 2018
- Published by Springer Nature in Journal of Materials Science
- Vol. 53 (18) , 13042-13052
K x Na1−xNbO3 perovskite thin films grown by pulsed laser deposition on R-plane sapphire for tunable microwave devices
- 21 June 2018
- Published by Springer Nature in Journal of Materials Science
- Vol. 53 (18) , 13042-13052
K x Na1−xNbO3 perovskite thin films grown by pulsed laser deposition on R-plane sapphire for tunable microwave devices
- 18 January 2018
- Published by Institute of Electrical and Electronics Engineers (IEEE) in IEEE Transactions on Ultrasonics, Ferroelectrics, and Frequency Control
- Vol. 65 (4) , 665-671
A Twofold Approach in Loss Reduction of KTa0.5Nb0.5O3 Ferroelectric Layers for Low-Loss Tunable Devices at Microwaves
Ferroelectric oxide films are attractive to design and fabricate reconfigurable and miniaturized planar devices operating at microwaves due to the large electric field dependence of their dielectric permittivity. In particular, KTa1-xNbxO3 (KTN) ferroelectric material presents a high tunability under moderate DC bias electric field. However, its intrinsic dielectric loss strongly contributes to the global loss of the related devices and limits their application areas at microwaves. In this work, a twofold approach is investigated to reduce the device loss. The intrinsic loss of KTN is firstly reduced by doping the ferroelectric material with a low loss dielectric material, namely MgO. Second, the doped ferroelectric films are confined using an original laser micro-etching process. Both routes have been implemented here to provide a synergic effect on the total insertion loss of the microwave test device, namely a coplanar waveguide stub resonator. The experimental data demonstrate a decrease of the intrinsic loss by a factor ~2 and a decrease of the global loss by a factor ~4 with a frequency tunability close to 10% at ~10 GHz under a moderate biasing (80 kV/cm).
- 18 January 2018
- Published by Institute of Electrical and Electronics Engineers (IEEE) in IEEE Transactions on Ultrasonics, Ferroelectrics, and Frequency Control
- Vol. 65 (4) , 665-671
A Twofold Approach in Loss Reduction of KTa0.5Nb0.5O3 Ferroelectric Layers for Low-Loss Tunable Devices at Microwaves
Ferroelectric oxide films are attractive to design and fabricate reconfigurable and miniaturized planar devices operating at microwaves due to the large electric field dependence of their dielectric permittivity. In particular, KTa1-xNbxO3 (KTN) ferroelectric material presents a high tunability under moderate DC bias electric field. However, its intrinsic dielectric loss strongly contributes to the global loss of the related devices and limits their application areas at microwaves. In this work, a twofold approach is investigated to reduce the device loss. The intrinsic loss of KTN is firstly reduced by doping the ferroelectric material with a low loss dielectric material, namely MgO. Second, the doped ferroelectric films are confined using an original laser micro-etching process. Both routes have been implemented here to provide a synergic effect on the total insertion loss of the microwave test device, namely a coplanar waveguide stub resonator. The experimental data demonstrate a decrease of the intrinsic loss by a factor ~2 and a decrease of the global loss by a factor ~4 with a frequency tunability close to 10% at ~10 GHz under a moderate biasing (80 kV/cm).