{"id":9923,"date":"2021-12-29T14:27:12","date_gmt":"2021-12-29T13:27:12","guid":{"rendered":"https:\/\/www.ummto.dz\/fs\/?p=9923"},"modified":"2021-12-29T14:27:14","modified_gmt":"2021-12-29T13:27:14","slug":"avis-de-soutenance-de-these-de-doctorat-en-sciences-en-physique-mme-saim-lamia","status":"publish","type":"post","link":"https:\/\/www.ummto.dz\/fs\/avis-de-soutenance-de-these-de-doctorat-en-sciences-en-physique-mme-saim-lamia\/","title":{"rendered":"Avis de Soutenance de Th\u00e8se de Doctorat En Sciences en Physique Mme : SAIM Lamia"},"content":{"rendered":"\n[et_pb_section fb_built=\u00a0\u00bb1&Prime; _builder_version=\u00a0\u00bb4.14.4&Prime; _module_preset=\u00a0\u00bbdefault\u00a0\u00bb global_colors_info=\u00a0\u00bb{}\u00a0\u00bb][et_pb_row _builder_version=\u00a0\u00bb4.14.4&Prime; _module_preset=\u00a0\u00bbdefault\u00a0\u00bb custom_padding=\u00a0\u00bb0px|0px|0px|0px|false|false\u00a0\u00bb custom_margin=\u00a0\u00bb0px|0px|0px|0px|false|false\u00a0\u00bb hover_enabled=\u00a0\u00bb0&Prime; sticky_enabled=\u00a0\u00bb0&Prime;][et_pb_column _builder_version=\u00a0\u00bb4.14.4&Prime; _module_preset=\u00a0\u00bbdefault\u00a0\u00bb type=\u00a0\u00bb4_4&Prime;][et_pb_text _builder_version=\u00a0\u00bb4.14.4&Prime; _module_preset=\u00a0\u00bbdefault\u00a0\u00bb text_orientation=\u00a0\u00bbjustified\u00a0\u00bb hover_enabled=\u00a0\u00bb0&Prime; sticky_enabled=\u00a0\u00bb0&Prime; custom_padding=\u00a0\u00bb0px||||false|false\u00a0\u00bb custom_margin=\u00a0\u00bb0px|0px|0px|0px|false|false\u00a0\u00bb]<p><strong><span style=\"color: #ff0000\">Mme\u00a0: SAIM Lamia\u00a0<\/span><\/strong><\/p>\n<p><strong>Soutiendra\u00a0 sa th\u00e8se de Doctorat\u00a0 en Physique<\/strong><\/p>\n<p><strong>Intitul\u00e9:\u00ab<span style=\"color: #0000ff\">Etude d&rsquo;onde de spin dans les interfaces et surfaces alliages du typeA<sub>x<\/sub>B<sub>1-x<\/sub>. <\/span>\u00bb<\/strong><\/p>\n<p><strong><em>\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0 <\/em><\/strong><\/p>\n<p><strong>Le\u00a0: <span style=\"color: #ff6600\">30 D\u00e9cembre 2021<\/span> \u00e0 <span style=\"color: #ff6600\">Salle de conf\u00e9rences de la facult\u00e9 des Sciences<\/span> (4\u00e8me \u00e9tage) \u00e0 <span style=\"color: #ff6600\">10h\u00a0:00<\/span><\/strong><\/p>\n<p><strong>Directeur de Th\u00e8se\u00a0: Professeur TIGRINE Rachid<\/strong><\/p>\n<p><strong>\u00a0<u>Devant le jury d\u2019examen suivant\u00a0:<\/u><\/strong><\/p>\n<p><strong><u><\/u><\/strong><\/p>\n<table style=\"height: 310px;width: 716px\" width=\"716\">\n<tbody>\n<tr style=\"height: 42px\">\n<td style=\"width: 214.617px;height: 42px\"><strong>Mme LALAM\u00a0\u00a0 Fadila<\/strong><\/td>\n<td style=\"width: 102.3px;height: 42px\"><strong>Professeur<\/strong><\/td>\n<td style=\"width: 110.333px;height: 42px\"><strong>UMMTO<\/strong><\/td>\n<td style=\"width: 260.75px;height: 42px\"><strong>Pr\u00e9sidente<\/strong><\/td>\n<\/tr>\n<tr style=\"height: 40px\">\n<td style=\"width: 214.617px;height: 40px\"><strong>M. TIGRINE\u00a0 Rachid<\/strong><\/td>\n<td style=\"width: 102.3px;height: 40px\"><strong>Professeur<\/strong><\/td>\n<td style=\"width: 110.333px;height: 40px\"><strong>U.Adrar<\/strong><\/td>\n<td style=\"width: 260.75px;height: 40px\"><strong>Directeur de th\u00e8se<\/strong><\/td>\n<\/tr>\n<tr style=\"height: 33px\">\n<td style=\"width: 214.617px;height: 33px\"><strong>M. HALIT\u00a0\u00a0\u00a0 Mohamed<\/strong><\/td>\n<td style=\"width: 102.3px;height: 33px\"><strong>Professeur<\/strong><\/td>\n<td style=\"width: 110.333px;height: 33px\"><strong>U.Laghouat<\/strong><\/td>\n<td style=\"width: 260.75px;height: 33px\"><strong>\u00a0 Examinateur <\/strong><\/td>\n<\/tr>\n<tr style=\"height: 43px\">\n<td style=\"width: 214.617px;height: 43px\"><strong>Mme ALILI\u00a0\u00a0\u00a0 Baya<\/strong><\/td>\n<td style=\"width: 102.3px;height: 43px\"><strong>Professeur<\/strong><\/td>\n<td style=\"width: 110.333px;height: 43px\"><strong>USTHB Alger<\/strong><\/td>\n<td style=\"width: 260.75px;height: 43px\"><strong>Examinatrice<\/strong><\/td>\n<\/tr>\n<tr style=\"height: 43px\">\n<td style=\"width: 214.617px;height: 43px\"><strong>M. AOUCHICHE\u00a0\u00a0 Hocine<\/strong><\/td>\n<td style=\"width: 102.3px;height: 43px\"><strong>\u00a0Professeur<\/strong><\/td>\n<td style=\"width: 110.333px;height: 43px\"><strong>UMMTO<\/strong><\/td>\n<td style=\"width: 260.75px;height: 43px\"><strong>Examinateur<\/strong><\/td>\n<\/tr>\n<tr style=\"height: 57px\">\n<td style=\"width: 214.617px;height: 57px\"><strong>M. BOURAHLA\u00a0 Boualem<\/strong><\/td>\n<td style=\"width: 102.3px;height: 57px\"><strong>\u00a0Professeur<\/strong><\/td>\n<td style=\"width: 110.333px;height: 57px\"><strong>UMMTO<\/strong><\/td>\n<td style=\"width: 260.75px;height: 57px\"><strong>Examinateur<\/strong><\/td>\n<\/tr>\n<tr style=\"height: 52px\">\n<td style=\"width: 214.617px;height: 52px\"><strong>M. CHADLI\u00a0\u00a0 Rabah<\/strong><\/td>\n<td style=\"width: 102.3px;height: 52px\"><strong>\u00a0 Professeur<\/strong><\/td>\n<td style=\"width: 110.333px;height: 52px\"><strong>UMMTO<\/strong><\/td>\n<td style=\"width: 260.75px;height: 52px\"><strong>Invit\u00e9<\/strong><\/td>\n<\/tr>\n<\/tbody>\n<\/table>\n<p>&nbsp;<\/p>\n<p style=\"text-align: center\"><strong><span style=\"color: #0000ff\">R\u00e9sum\u00e9<\/span><\/strong><\/p>\n<p style=\"text-align: justify\"><span style=\"color: #000000\">Dans cette th\u00e8se, nous \u00e9tudions les propri\u00e9t\u00e9s pr\u00e9cessionnelles des interfaces et surfaces alliages de types A<sub>x<\/sub> B <sub>1-x<\/sub> dans les syst\u00e8mes ferromagn\u00e9tiques de basses dimensions. Le but principal est d\u2019expliquer le comportement des ondes de spins d\u2019interfaces et de surfaces alliage. Le premiersyst\u00e8mes mod\u00e8les sous \u00e9tude est une nano jonction de type Fe\/Ni<sub>fcc<\/sub>(n)\/Fe nous examinons l\u2019influence de l\u2019\u00e9paisseur de cette derni\u00e8re. Quant au deuxi\u00e8me mod\u00e8le, c\u2019est une surface alliage Fe\/Ni<sub>fcc<\/sub>(100), o\u00f9 on a\u00a0 consid\u00e9r\u00e9 deux cat\u00e9gories de surfaces \u00a0: ordonn\u00e9e et d\u00e9sordonn\u00e9e.Notre \u00e9tude est bas\u00e9e sur l\u2019application de la m\u00e9thode de raccordement d\u00e9crivant toutes les interactions entre les plus proches voisins et dans \u00a0L\u2019Hamiltonien d\u2019Heisenberg. Les coefficients de transmission et de r\u00e9flexion, les \u00e9tats localis\u00e9s ainsi que les densit\u00e9s d\u2019\u00e9tats locale de magnons (LDOS), ont \u00e9t\u00e9 d\u00e9termin\u00e9s en fonction des grandeurs physiques de nos syst\u00e8mes consid\u00e9r\u00e9s.Nos r\u00e9sultats num\u00e9riques, pour le syst\u00e8me Fe\/Ni(n)\/Fe, ont mis en \u00e9vidence l\u2019apparition de nouvelles branches de magnons d\u2019interface et des pics dans les courbes des densit\u00e9s d\u2019\u00e9tats de magnons (LDOS), notons que le nombre des branches et des pics d\u00e9pend fortement de l\u2019\u00e9paisseur de la nanostructure int\u00e9gr\u00e9e et de la nature des interfaces. Les courbes des coefficients de transmission et de r\u00e9flexion montrent que la nanojonctionFe\/Ni(n)\/Fe, forme un r\u00e9sonateur de Fabry-P\u00e9rot. Quant aux r\u00e9sultats des surfaces alliages, montrent que le nombre de branches induites par la surface ainsi que les spectres des densit\u00e9s d\u2019\u00e9tats locales, d\u00e9pend fortement de l\u2019ordre structurel des surfaces alliages et de la concentration de l\u2019adsorbat.<\/span><\/p>\n<p style=\"text-align: justify\"><strong><span style=\"color: #0000ff\">Mots cl\u00e9s\u00a0<\/span> <\/strong><\/p>\n<p style=\"text-align: left\"><span style=\"color: #000000\">Magnons, Dynamiques des spins, Surfaces alliages, M\u00e9thode de raccordement, Magnons de surface<\/span><\/p>\n<p><strong><span style=\"color: #0000ff\">Abstract<\/span><\/strong><\/p>\n<p style=\"text-align: justify\"><span style=\"color: #000000\">In this thesis, we study the precessional properties of the interfaces and surfaces\u00a0 of Ax B 1-x type alloys in low-dimensional ferromagnetic systems. The main goal is to explain the behavior of spin waves of interfaces and alloy surfaces. The first model systems\u00a0 under study is an Fe \/ Ni fcc (n) \/ Fe nano junction. We examine the influence of the thickness of the latter. As for the second model, it is an Fe \/ Nifcc (100) alloy surface, where we considered two categories of surfaces: ordered and disordered. Our study is based on the application of the matching\u00a0 method describing all the interactions between nearest neighbors and in The Hamiltonian of Heisenberg. The transmission and reflection coefficients, the localized states as well as the local magnon densities of states (LDOS), were determined according to the physical quantities of our systems considered. Our numerical results, for the Fe \/ Ni (n) \/ Fe system, highlighted the appearance of new branches of interface magnons and peaks in the curves of the densities of magnons states (LDOS), note that the number of branches and peaks strongly depends on the thickness of the integrated nanostructure and the nature of the interfaces. The curves of the transmission and reflection coefficients show that the Fe \/ Ni (n) \/ Fe nanojunction\u00a0 forms a Fabry-Perot resonator. As for the results of the alloy surfaces, show that the number of branches induced by the surface as well as the spectra of the local state densities, strongly depends on the structural order of the alloy surfaces and on the adsorbate concentration.<\/span><\/p>\n<p><strong><span style=\"color: #0000ff\">Key word<\/span><\/strong><\/p>\n<p><span style=\"color: #000000\">spin dynamics, spin scattering, state density, Heisenberg model, Landauer-B\u00fctikker formalism, Green functions formalism, matching method<\/span><\/p>\n<p>&nbsp;<\/p>[\/et_pb_text][\/et_pb_column][\/et_pb_row][\/et_pb_section]\n","protected":false},"excerpt":{"rendered":"<p>Mme\u00a0: SAIM Lamia\u00a0 Soutiendra\u00a0 sa th\u00e8se de Doctorat\u00a0 en Physique Intitul\u00e9:\u00abEtude d&rsquo;onde de spin dans les interfaces et surfaces alliages du typeAxB1-x. \u00bb \u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0 Le\u00a0: 30 D\u00e9cembre 2021 \u00e0 Salle de conf\u00e9rences de la facult\u00e9 des Sciences (4\u00e8me \u00e9tage) \u00e0 10h\u00a0:00 Directeur de Th\u00e8se\u00a0: Professeur TIGRINE Rachid \u00a0Devant le jury d\u2019examen suivant\u00a0: Mme LALAM\u00a0\u00a0 Fadila [&hellip;]<\/p>\n","protected":false},"author":13,"featured_media":6032,"comment_status":"closed","ping_status":"closed","sticky":false,"template":"","format":"standard","meta":{"_et_pb_use_builder":"on","_et_pb_old_content":"","_et_gb_content_width":"","footnotes":""},"categories":[1],"tags":[],"class_list":["post-9923","post","type-post","status-publish","format-standard","has-post-thumbnail","hentry","category-non-classe"],"yoast_head":"<!-- This site is optimized with the Yoast SEO plugin v27.3 - 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