Didier Marty-Dessus
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
Didier Marty-Dessus has a total of 47 co-authors. Here are the top co-authors by number of shared publications:
L. Berquez
LAPLACE, Université de Toulouse, CNRS, INPT, UPS, France; Université Paul Sabatier, Bât. 3R3, 118 route de Narbonne, F-31062 Toulouse cedex 9, France
8 shared publicationsA. Petre
Université de Pau et des Pays de l'Adour, SIAME, IPRA, 2 avenue du Président Pierre Angot, F-64053 Pau, France
7 shared publicationsJ.L. Franceschi
Laboratoire de Génie Electrique, Paul Sabatier University, 118 route de Narbonne, 31062 Toulouse Cédex 04, France
6 shared publicationsLaurent Berquez
LAPLACE, Universite de Toulouse, CNRS, INPT, UPS, France
6 shared publicationsJean-Luc Franceschi
3 shared publications- Petru Nothingher
University Politehnica of Bucharest, Romania
3 shared publications
Latest Publications
- Open Access
- 5 July 2020
- Published by Institute of Electrical and Electronics Engineers (IEEE)
- p. 355-358
(F)LIMM deconvolution procedure for on-line measurements of space charge in thin polymeric insulations
On-line measurements are developed to monitor space charge evolution in a polymeric insulation film by the mean of a (Focused) Laser Intensity Modulation Method set-up. The purpose of this paper is to describe how, starting from experimental on-line (F)LIMM currents, one is able to develop a global procedure leading to extract space charge profiles in dedicated test samples. Objects of study are 25$-\mu$m films of PTFE submitted to a protocol of poling starting from OV to 2.5 kV, alternating 6 volt-off and 6 volt-on measurements on each step of 500 V. Each measurement consists in recording a(F)LIMM pyro-current spectrum from 10Hz to 10 kHz hence a whole protocol is composed of 63 acquisitions of such spectra. Once measurements performed on PTFE sample hereinabove described, a normalization process has allowed first to confirm that there was no charge evolution (injection) between two successive Volt-on to Volt-off measurements, and secondly to launch a thermal calibration of the bench that is needed in (F)LIMM experiment. Then a mathematical correction on Volt-on current was operated in order to extract the useful part linked to the internal field produced by the space charge. Finally, significant space charge representations and evolutions were obtained in our test samples by using a mathematical deconvolution procedure.
- 5 July 2020
- Published by Institute of Electrical and Electronics Engineers (IEEE)
- p. 355-358
Open Access(F)LIMM deconvolution procedure for on-line measurements of space charge in thin polymeric insulations
On-line measurements are developed to monitor space charge evolution in a polymeric insulation film by the mean of a (Focused) Laser Intensity Modulation Method set-up. The purpose of this paper is to describe how, starting from experimental on-line (F)LIMM currents, one is able to develop a global procedure leading to extract space charge profiles in dedicated test samples. Objects of study are 25$-\mu$m films of PTFE submitted to a protocol of poling starting from OV to 2.5 kV, alternating 6 volt-off and 6 volt-on measurements on each step of 500 V. Each measurement consists in recording a(F)LIMM pyro-current spectrum from 10Hz to 10 kHz hence a whole protocol is composed of 63 acquisitions of such spectra. Once measurements performed on PTFE sample hereinabove described, a normalization process has allowed first to confirm that there was no charge evolution (injection) between two successive Volt-on to Volt-off measurements, and secondly to launch a thermal calibration of the bench that is needed in (F)LIMM experiment. Then a mathematical correction on Volt-on current was operated in order to extract the useful part linked to the internal field produced by the space charge. Finally, significant space charge representations and evolutions were obtained in our test samples by using a mathematical deconvolution procedure.
- 1 July 2018
- Published by Institute of Electrical and Electronics Engineers (IEEE)
- p. 1-4
On the feasibility of (F)LIMM measurements on thin polymer films submitted to an external thermal stress
A new bench for the behavior assessment of polymeric thin films submitted to an external thermal stress was developed. Based on the thermal (F)LIMM technique dedicated to space charge and polarization profiles studies, this set-up was applied to the study of two types of thin insulations (PTFE and PVDF) conditioned to a constant external temperature from RT up to $145 ^{\circ}\mathrm {C}$. Concerning PVDF, between 30 et $80 ^{\circ}\mathrm {C}$, its pyroelectric coefficient does not vary significantly, but begins to diminish at $80 ^{\circ}\mathrm {C}$ and falls drastically at $145 ^{\circ}\mathrm {C}$, close to the Curie temperature (between 150 and $160 ^{\circ}\mathrm {C})$, showing a beginning of a shift from a ferroelectric organization to a para electric one. The PTFE sample was first irradiated by an e-beam for negative charge implantation, then placed in the set-up for thermal studies. The temperature was raised up to $130 ^{\circ}\mathrm {C}$. No variation was observed on space charge profiles up to $102 ^{\circ}\mathrm {C}$, temperature at which a brutal change appeared with a quasi-complete detrapping of charges in the sample. Through these two different cases of application, it was shown that it was possible to study the inner space charge and polarization profiles evolutions versus external environmental temperature.- 1 July 2018
- Published by Institute of Electrical and Electronics Engineers (IEEE)
- p. 1-4
On the feasibility of (F)LIMM measurements on thin polymer films submitted to an external thermal stress
A new bench for the behavior assessment of polymeric thin films submitted to an external thermal stress was developed. Based on the thermal (F)LIMM technique dedicated to space charge and polarization profiles studies, this set-up was applied to the study of two types of thin insulations (PTFE and PVDF) conditioned to a constant external temperature from RT up to $145 ^{\circ}\mathrm {C}$. Concerning PVDF, between 30 et $80 ^{\circ}\mathrm {C}$, its pyroelectric coefficient does not vary significantly, but begins to diminish at $80 ^{\circ}\mathrm {C}$ and falls drastically at $145 ^{\circ}\mathrm {C}$, close to the Curie temperature (between 150 and $160 ^{\circ}\mathrm {C})$, showing a beginning of a shift from a ferroelectric organization to a para electric one. The PTFE sample was first irradiated by an e-beam for negative charge implantation, then placed in the set-up for thermal studies. The temperature was raised up to $130 ^{\circ}\mathrm {C}$. No variation was observed on space charge profiles up to $102 ^{\circ}\mathrm {C}$, temperature at which a brutal change appeared with a quasi-complete detrapping of charges in the sample. Through these two different cases of application, it was shown that it was possible to study the inner space charge and polarization profiles evolutions versus external environmental temperature.- 24 April 2017
- Published by Institute of Electrical and Electronics Engineers (IEEE) in IEEE Transactions on Dielectrics and Electrical Insulation
- Vol. 24 (2) , 1220-1228
Space charge formation in polyimide films and polyimide/SiO2 double-layer measured by LIMM
For Polyimides (PI) used as insulating inter-layers or passivation layers in microelectronics and power electronics, reliability and failure mechanisms are intimately linked to phenomena such as non-linear conduction, distortion of field distribution and electrical ageing that have all some relation to space charge processes. Knowledge about these space charge distributions is therefore of importance to optimize structures and designs involving PIs. However, in the thickness scale of interest for such applications, of the order of 10 μm, no results were reported for PI, and only scarce studies for other materials. Space charge measurements carried out on PI using the laser intensity modulation method (LIMM) are reported in this work. PI-containing metal-insulator-semiconductor structures were pre-stressed under DC fields up to 2 MV/cm. The impact of the doping type of the substrate (either n-type or, p-type silicon) has been evaluated to address the mechanisms of space charge formation. The nature of electrode substrate substantially impacts the measured charge amount and charge nature, pointing towards charge injection as the origin of space charge build-up. The interpretation is substantiated by results obtained using a SiO2 layer as a barrier against electronic injection from the substrate into the PI layer.
- 24 April 2017
- Published by Institute of Electrical and Electronics Engineers (IEEE) in IEEE Transactions on Dielectrics and Electrical Insulation
- Vol. 24 (2) , 1220-1228
Space charge formation in polyimide films and polyimide/SiO2 double-layer measured by LIMM
For Polyimides (PI) used as insulating inter-layers or passivation layers in microelectronics and power electronics, reliability and failure mechanisms are intimately linked to phenomena such as non-linear conduction, distortion of field distribution and electrical ageing that have all some relation to space charge processes. Knowledge about these space charge distributions is therefore of importance to optimize structures and designs involving PIs. However, in the thickness scale of interest for such applications, of the order of 10 μm, no results were reported for PI, and only scarce studies for other materials. Space charge measurements carried out on PI using the laser intensity modulation method (LIMM) are reported in this work. PI-containing metal-insulator-semiconductor structures were pre-stressed under DC fields up to 2 MV/cm. The impact of the doping type of the substrate (either n-type or, p-type silicon) has been evaluated to address the mechanisms of space charge formation. The nature of electrode substrate substantially impacts the measured charge amount and charge nature, pointing towards charge injection as the origin of space charge build-up. The interpretation is substantiated by results obtained using a SiO2 layer as a barrier against electronic injection from the substrate into the PI layer.
- 23 August 2016
- Published by Institute of Electrical and Electronics Engineers (IEEE)
- Vol. 1, 223-226
Towards space charge measurements by (F)LIMM under DC electric field
An evolution of a conventional thermal wave technique for space charge investigation in insulations is presented. Based on a laser diode as source of heat, the set-up has been modified in order to be able to stress electrically samples under study with an external electric field while doing measurements for space charge investigation. After a short presentation of the fundamentals related to the technique, its evolutions towards “on-line” studies are evoked, in particular the fundamental equations associated in this new configuration. In the experimental part of the text are described the new challenges arising with the modified set-up and the solutions proposed. At the end, the conclusion is two folds: the modified bench is not only consistent with the classical one, but also allows a thermal calibration of the technique that will enhance the accuracy of results to come.
- 23 August 2016
- Published by Institute of Electrical and Electronics Engineers (IEEE)
- Vol. 1, 223-226
Towards space charge measurements by (F)LIMM under DC electric field
An evolution of a conventional thermal wave technique for space charge investigation in insulations is presented. Based on a laser diode as source of heat, the set-up has been modified in order to be able to stress electrically samples under study with an external electric field while doing measurements for space charge investigation. After a short presentation of the fundamentals related to the technique, its evolutions towards “on-line” studies are evoked, in particular the fundamental equations associated in this new configuration. In the experimental part of the text are described the new challenges arising with the modified set-up and the solutions proposed. At the end, the conclusion is two folds: the modified bench is not only consistent with the classical one, but also allows a thermal calibration of the technique that will enhance the accuracy of results to come.
- 23 August 2016
- Published by Institute of Electrical and Electronics Engineers (IEEE)
- Vol. 1, 53-54
Simultaneous measurement of surface temperature and space charge distribution with thermal pulse method
To improve the spatial resolution of space charge distribution using thermal measurements, an accurate profile of the temperature in the sample is needed. The measurement of both sample surface temperature profile and space charge induced signal is a first crucial step for this knowledge. The described setup allows both measurements simultaneously and gives good signal-to-noise ratios.
- 23 August 2016
- Published by Institute of Electrical and Electronics Engineers (IEEE)
- Vol. 1, 53-54
Simultaneous measurement of surface temperature and space charge distribution with thermal pulse method
To improve the spatial resolution of space charge distribution using thermal measurements, an accurate profile of the temperature in the sample is needed. The measurement of both sample surface temperature profile and space charge induced signal is a first crucial step for this knowledge. The described setup allows both measurements simultaneously and gives good signal-to-noise ratios.
- Open Access
- 4 June 2015
- Published by Institute of Electrical and Electronics Engineers (IEEE) in IEEE Transactions on Dielectrics and Electrical Insulation
- Vol. 22 (3) , 1506-1511
Surface temperature measurement for space charge distribution measurements with thermal methods
The implementation of space charge measurements based on thermal perturbation on thin films requires an improvement of the temperature distribution estimation at the surface and in the depth of dielectric materials for getting reliable space charge profile measurements. Absolute temperature variations are needed, both in time and space. The present contribution addresses surface temperature measurements based on either thermoelectric or bolometric effects. Both responses have been measured on copper-coated silicon nitride layers and gold-coated polypropylene films heated with a Nd:YAG laser pulse. It is shown that high temporal resolution thermal response can be obtained through the bolometric response and that the information appears nearly independent on the nature of the coating electrode. The setup developed provides good signal to noise ratio for heated electrodes of a few ohm resistance. Strategies are still to develop to get the temperature profile in the insulating sample layer.
- 4 June 2015
- Published by Institute of Electrical and Electronics Engineers (IEEE) in IEEE Transactions on Dielectrics and Electrical Insulation
- Vol. 22 (3) , 1506-1511
Open AccessSurface temperature measurement for space charge distribution measurements with thermal methods
The implementation of space charge measurements based on thermal perturbation on thin films requires an improvement of the temperature distribution estimation at the surface and in the depth of dielectric materials for getting reliable space charge profile measurements. Absolute temperature variations are needed, both in time and space. The present contribution addresses surface temperature measurements based on either thermoelectric or bolometric effects. Both responses have been measured on copper-coated silicon nitride layers and gold-coated polypropylene films heated with a Nd:YAG laser pulse. It is shown that high temporal resolution thermal response can be obtained through the bolometric response and that the information appears nearly independent on the nature of the coating electrode. The setup developed provides good signal to noise ratio for heated electrodes of a few ohm resistance. Strategies are still to develop to get the temperature profile in the insulating sample layer.
- 1 April 2015
- Published by AIP Publishing in Review of Scientific Instruments
- Vol. 86 (4) , 043905
Space charge distributions in insulating polymers: A new non-contacting way of measurement
A new technique for the determination of space charge profiles in insulating polymers is proposed. Based on the evolution of an existing thermal wave technique called Focused Laser Intensity Modulation Method ((F)LIMM), it allows non-contact measurements on thin films exhibiting an internal charge to be studied. An electrostatic model taking into account the new sample-cell geometry proposed was first developed. It has been shown, in particular, that it was theoretically possible to calculate the internal charge from experimental measurements while allowing an evaluation of the air layer appearing between the sample and the electrode when non-contact measurements are performed. These predictions were confirmed by an experimental implementation for two thin polymer samples (25 μm-polyvinylidenefluoride and 50 μm-polytetrafluoroethylene (PTFE)) used as tests. In these cases, minimum air-layer thickness was determined with an accuracy of 3% and 20%, respectively, depending on the signal-to-noise ratio during the experimental procedure. In order to illustrate the reachable possibilities of this technique, 2D and 3D cartographies of a negative space charge implanted by electron beam within the PTFE test sample were depicted: like in conventional (F)LIMM, a multidimensional representation of a selectively implanted charge remains possible at a few microns depth, but using a non-contacting way of measurement.
- 1 April 2015
- Published by AIP Publishing in Review of Scientific Instruments
- Vol. 86 (4) , 043905
Space charge distributions in insulating polymers: A new non-contacting way of measurement
A new technique for the determination of space charge profiles in insulating polymers is proposed. Based on the evolution of an existing thermal wave technique called Focused Laser Intensity Modulation Method ((F)LIMM), it allows non-contact measurements on thin films exhibiting an internal charge to be studied. An electrostatic model taking into account the new sample-cell geometry proposed was first developed. It has been shown, in particular, that it was theoretically possible to calculate the internal charge from experimental measurements while allowing an evaluation of the air layer appearing between the sample and the electrode when non-contact measurements are performed. These predictions were confirmed by an experimental implementation for two thin polymer samples (25 μm-polyvinylidenefluoride and 50 μm-polytetrafluoroethylene (PTFE)) used as tests. In these cases, minimum air-layer thickness was determined with an accuracy of 3% and 20%, respectively, depending on the signal-to-noise ratio during the experimental procedure. In order to illustrate the reachable possibilities of this technique, 2D and 3D cartographies of a negative space charge implanted by electron beam within the PTFE test sample were depicted: like in conventional (F)LIMM, a multidimensional representation of a selectively implanted charge remains possible at a few microns depth, but using a non-contacting way of measurement.
- 1 May 2009
- Published by Elsevier in Journal of Electrostatics
- Vol. 67 (2-3) , 430-434
Three-dimensional space charge cartographies by FLIMM in electron irradiated polymers
- 1 May 2009
- Published by Elsevier in Journal of Electrostatics
- Vol. 67 (2-3) , 430-434
Three-dimensional space charge cartographies by FLIMM in electron irradiated polymers
- 1 July 2006
- Published by Elsevier in Journal of Electrostatics
- Vol. 64 (7-9) , 492-497
Space charge cartography by FLIMM on SEM-irradiated PTFE thin films
- 1 July 2006
- Published by Elsevier in Journal of Electrostatics
- Vol. 64 (7-9) , 492-497
Space charge cartography by FLIMM on SEM-irradiated PTFE thin films