1 Department of Economic Development, Jobs, Transport and Resources, AgriBio, La Trobe University, Bundoora, VIC, Australia, 2 Animal, Plant and Soil Sciences Department, AgriBio, La Trobe University, Bundoora, VIC, Australia, 3 Plant Sciences Division, Research School of Biology, The Australian National University, Canberra, ACT, Australia, 4 Institut National de la Recherche Agronomique-AgroP...

B. Sacépé,1,2 J. Seidemann,1,2 M. Ovadia,3 I. Tamir,3 D. Shahar,3 C. Chapelier,1,4 C. Strunk,5 and B. A. Piot6 1Univ. Grenoble Alpes, F-38000 Grenoble, France 2CNRS, Institut Néel, F-38000 Grenoble, France 3Department of Condensed Matter Physics, Weizmann Institute of Science, Rehovot 76100, Israel 4CEA, INAC-SPSMS, F-38000 Grenoble, France 5Institut für experimentelle und angewandte Physik, Un...

1 Université de Lyon, CREATIS-LRMN ; CNRS UMR5220 ; Inserm U630 ; INSA-Lyon ; Université Lyon 1, F69621 Villeurbanne, France 2 European Synchrotron Radiation Facility, 6 rue Jules Horowitz, F38043 Grenoble, France 3 Julius Wolff Institut &Berlin-Brandenburg School for Regenerative Therapies, Charité Universitätsmedizin Berlin Augustenburger Platz 1, 13353 Berlin, Germany 4 IPHEP, CNRS UMR 6046,...

O. Cyr-Choinière, S. Badoux, G. Grissonnanche, B. Michon, S. A. A. Afshar, S. Fortier, D. LeBoeuf, D. Graf, J. Day, D. A. Bonn, W. N. Hardy, R. Liang, N. Doiron-Leyraud, and Louis Taillefer Institut quantique, Département de physique and RQMP, Université de Sherbrooke, Sherbrooke, Québec J1K 2R1, Canada Laboratoire National des Champs Magnétiques Intenses, UPR 3228, (CNRS-INSA-UJF-UPS), Grenobl...

J. Kunc,1,2,* B. A. Piot,1 D. K. Maude,1 M. Potemski,1 R. Grill,2 C. Betthausen,3 D. Weiss,3 V. Kolkovsky,4 G. Karczewski,4 and T. Wojtowicz4 1Laboratoire National des Champs Magnétiques Intenses (LNCMI), CNRS-UJF-UPS-INSA, 38042 Grenoble, France 2Institute of Physics, Faculty of Mathematics and Physics, 12116 Prague, Czech Republic 3Experimentelle und Angewandte Physik, Universität Regensburg,...

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Propagation of extremely short pulses of electromagnetic field (electromagnetic spikes) is considered in the framework of the total Maxwell-Duffing model where anharmonic oscillators with cubic nonlinearities (Duffing model) represent the material medium and wave propagation is governed by the 1-d bidirectional Maxwell equations. This system of equations has a one parameter family of exact anal...

a Institut de Physique de Rennes, CNRS-UMR 6251, Université Rennes 1, F-35042 Rennes, France b UMR FOTON, CNRS, INSA-Rennes, F-35708 Rennes, France c GdS Optronlab, Dpto. Fisica de la Materia Condensada, Universidad de Valladolid, 47011 Valladolid, Spain d III-V Lab, Route de Nozay, F-91461 Marcoussis, France e OSUR, Plateforme NanoSIMS, Université Rennes 1, 35042 Rennes, France f Istituto CNR-...

T. Gao, P. S. Eldridge, T. C. H. Liew, S. I. Tsintzos, G. Stavrinidis, G. Deligeorgis, Z. Hatzopoulos, and P. G. Savvidis Department of Materials Science & Technology, University of Crete, Greece IESL-FORTH, P.O. Box 1527, 71110 Heraklion, Crete, Greece School of Physical and Mathematical Sciences, Nanyang Technological University, 637371, Singapore Cavendish Laboratory, University of Cambridge...

Jean-Marie Poumirol,1 Alessandro Cresti,2,* Stephan Roche,3,4 Walter Escoffier,1 Michel Goiran,1 Xinran Wang,5 Xiaolin Li,5 Hongjie Dai,5 and Bertrand Raquet1 1Laboratoire National des Champs Magnétiques Intenses, INSA UPS CNRS, UPR 3228, Université de Toulouse, 143 avenue de Rangueil, 31400 Toulouse, France 2LETI, MINATEC, CEA, F38054 Grenoble, France 3INAC, SP2M, Lsim, CEA, 17 avenue des Mart...