{"id":1654,"date":"2023-03-07T07:16:24","date_gmt":"2023-03-07T12:16:24","guid":{"rendered":"https:\/\/www.lafmat.com\/home\/?page_id=1654"},"modified":"2026-02-26T13:30:48","modified_gmt":"2026-02-26T18:30:48","slug":"video-galery-2022","status":"publish","type":"page","link":"https:\/\/www.lafmat.com\/home\/video-galery-2022\/","title":{"rendered":"VG 2022"},"content":{"rendered":"

[et_pb_section fb_built=\u00bb1″ admin_label=\u00bbServices Section\u00bb _builder_version=\u00bb4.17.0″ _module_preset=\u00bbdefault\u00bb background_color=\u00bb#f2f6f9″ custom_margin=\u00bb0px||0px||false|false\u00bb custom_padding=\u00bb0px|0px|0px|0px|false|false\u00bb da_disable_devices=\u00bboff|off|off\u00bb global_module=\u00bb183″ global_colors_info=\u00bb{}\u00bb da_is_popup=\u00bboff\u00bb da_exit_intent=\u00bboff\u00bb da_has_close=\u00bbon\u00bb da_alt_close=\u00bboff\u00bb da_dark_close=\u00bboff\u00bb da_not_modal=\u00bbon\u00bb da_is_singular=\u00bboff\u00bb da_with_loader=\u00bboff\u00bb da_has_shadow=\u00bbon\u00bb][et_pb_row _builder_version=\u00bb4.17.0″ _module_preset=\u00bbdefault\u00bb global_colors_info=\u00bb{}\u00bb][et_pb_column type=\u00bb4_4″ _builder_version=\u00bb4.17.0″ _module_preset=\u00bbdefault\u00bb global_colors_info=\u00bb{}\u00bb][et_pb_text _builder_version=\u00bb4.17.0″ _module_preset=\u00bbdefault\u00bb global_colors_info=\u00bb{}\u00bb]<\/p>\n

Here you will find the\u00a0<\/em>YouTube play list of the Red LAFMAT conferences 2022\u00a0<\/em><\/a><\/p>\n

[\/et_pb_text][\/et_pb_column][\/et_pb_row][et_pb_row column_structure=\u00bb1_3,1_3,1_3″ use_custom_gutter=\u00bbon\u00bb gutter_width=\u00bb2″ _builder_version=\u00bb4.16″ _module_preset=\u00bbdefault\u00bb max_width=\u00bb1440px\u00bb custom_padding=\u00bb|||\u00bb use_custom_width=\u00bbon\u00bb custom_width_px=\u00bb1440px\u00bb global_colors_info=\u00bb{}\u00bb][et_pb_column type=\u00bb1_3″ _builder_version=\u00bb4.16″ _module_preset=\u00bbdefault\u00bb background_color=\u00bb#ffffff\u00bb custom_padding=\u00bb|||\u00bb global_colors_info=\u00bb{}\u00bb custom_padding__hover=\u00bb|||\u00bb][et_pb_image src=\u00bbhttp:\/\/www.lafmat.com\/home\/wp-content\/uploads\/2022\/12\/Prof.-Carlos-2.0.png\u00bb title_text=\u00bbProf. Carlos 2.0″ _builder_version=\u00bb4.17.0″ _module_preset=\u00bbdefault\u00bb global_colors_info=\u00bb{}\u00bb][\/et_pb_image][et_pb_text admin_label=\u00bbService Name\u00bb _builder_version=\u00bb4.17.0″ _module_preset=\u00bbdefault\u00bb text_font=\u00bbMontserrat||||||||\u00bb text_font_size=\u00bb15px\u00bb text_line_height=\u00bb1.8em\u00bb header_font=\u00bb||||||||\u00bb header_3_font=\u00bbMontserrat||||||||\u00bb header_3_line_height=\u00bb1.5em\u00bb custom_padding=\u00bb10px|20px||20px\u00bb locked=\u00bboff\u00bb global_colors_info=\u00bb{}\u00bb]<\/p>\n

Dec 17th 2022<\/h3>\n

Prof. Carlos A. M. dos Santos<\/h3>\n

Forces acting on the electron in conductors at zero temperature <\/strong>(Video link)<\/a><\/p>\n

Escola de Engenharia de Lorena, Universidade de S\u00e3o Paulo Lorena<\/span>
S\u00e3o Paulo, Brasil.<\/span><\/p>\n

 <\/p>\n

<\/span><\/p>\n

[\/et_pb_text][\/et_pb_column][et_pb_column type=\u00bb1_3″ _builder_version=\u00bb4.16″ _module_preset=\u00bbdefault\u00bb background_color=\u00bb#ffffff\u00bb custom_padding=\u00bb|||\u00bb global_colors_info=\u00bb{}\u00bb custom_padding__hover=\u00bb|||\u00bb][et_pb_image src=\u00bbhttp:\/\/www.lafmat.com\/home\/wp-content\/uploads\/2022\/12\/Dr.-Alexander-Polasek.png\u00bb title_text=\u00bbDr. Alexander Polasek\u00bb _builder_version=\u00bb4.17.0″ _module_preset=\u00bbdefault\u00bb global_colors_info=\u00bb{}\u00bb][\/et_pb_image][et_pb_text admin_label=\u00bbService Name\u00bb _builder_version=\u00bb4.17.0″ _module_preset=\u00bbdefault\u00bb text_font=\u00bbMontserrat||||||||\u00bb text_font_size=\u00bb15px\u00bb text_line_height=\u00bb1.8em\u00bb header_font=\u00bb||||||||\u00bb header_3_font=\u00bbMontserrat||||||||\u00bb header_3_line_height=\u00bb1.5em\u00bb custom_padding=\u00bb10px|20px||20px\u00bb locked=\u00bboff\u00bb global_colors_info=\u00bb{}\u00bb]<\/p>\n

Dec 10th 2022<\/span><\/h3>\n

Dr. Alexander Polasek<\/span><\/h3>\n

Electric Power Applications of Superconductivity<\/strong> (Video link)<\/a><\/span><\/p>\n

CEPEL \u2013 Centro de Investigaci\u00f3n de Energ\u00eda El\u00e9ctrica, Departamento de Energ\u00eda Transici\u00f3n y Sostenibilidad, Brasil.<\/span><\/p>\n

<\/span><\/p>\n

[\/et_pb_text][\/et_pb_column][et_pb_column type=\u00bb1_3″ _builder_version=\u00bb4.16″ _module_preset=\u00bbdefault\u00bb background_color=\u00bb#ffffff\u00bb custom_padding=\u00bb|||\u00bb global_colors_info=\u00bb{}\u00bb custom_padding__hover=\u00bb|||\u00bb][et_pb_image src=\u00bbhttp:\/\/www.lafmat.com\/home\/wp-content\/uploads\/2022\/11\/Prof.-Leopoldo-2.0.png\u00bb title_text=\u00bbProf. Leopoldo 2.0″ _builder_version=\u00bb4.17.0″ _module_preset=\u00bbdefault\u00bb global_colors_info=\u00bb{}\u00bb][\/et_pb_image][et_pb_text admin_label=\u00bbService Name\u00bb _builder_version=\u00bb4.17.0″ _module_preset=\u00bbdefault\u00bb text_font=\u00bbMontserrat||||||||\u00bb text_font_size=\u00bb15px\u00bb text_line_height=\u00bb1.8em\u00bb header_font=\u00bb||||||||\u00bb header_3_font=\u00bbMontserrat||||||||\u00bb header_3_line_height=\u00bb1.5em\u00bb custom_padding=\u00bb10px|20px||20px\u00bb locked=\u00bboff\u00bb global_colors_info=\u00bb{}\u00bb]<\/p>\n

Dec 3rd 2022<\/span><\/h3>\n

Prof. Leopoldo<\/span> Suescun<\/h3>\n

Dise\u00f1o, s\u00edntesis y caracterizaci\u00f3n de perovskitas avanzadas por autocombusti\u00f3n<\/strong> (Video link)<\/a><\/span><\/p>\n

Cryssmat-Lab\/DETEMA, Facultad de Qu\u00edmica, UdelaR, Uruguay.<\/span><\/p>\n

Abstract<\/span><\/a><\/p>\n

<\/span><\/p>\n

[\/et_pb_text][\/et_pb_column][\/et_pb_row][et_pb_row column_structure=\u00bb1_3,1_3,1_3″ use_custom_gutter=\u00bbon\u00bb gutter_width=\u00bb2″ _builder_version=\u00bb4.16″ _module_preset=\u00bbdefault\u00bb max_width=\u00bb1440px\u00bb custom_padding=\u00bb|||\u00bb use_custom_width=\u00bbon\u00bb custom_width_px=\u00bb1440px\u00bb global_colors_info=\u00bb{}\u00bb][et_pb_column type=\u00bb1_3″ _builder_version=\u00bb4.16″ _module_preset=\u00bbdefault\u00bb background_color=\u00bb#ffffff\u00bb custom_padding=\u00bb|||\u00bb global_colors_info=\u00bb{}\u00bb custom_padding__hover=\u00bb|||\u00bb][et_pb_image src=\u00bbhttp:\/\/www.lafmat.com\/home\/wp-content\/uploads\/2022\/11\/Prof.-Sergio-Conegeros.png\u00bb title_text=\u00bbProf. Sergio Conegeros\u00bb _builder_version=\u00bb4.17.0″ _module_preset=\u00bbdefault\u00bb global_colors_info=\u00bb{}\u00bb][\/et_pb_image][et_pb_text admin_label=\u00bbService Name\u00bb _builder_version=\u00bb4.17.0″ _module_preset=\u00bbdefault\u00bb text_font=\u00bbMontserrat||||||||\u00bb text_font_size=\u00bb15px\u00bb text_line_height=\u00bb1.8em\u00bb header_font=\u00bb||||||||\u00bb header_3_font=\u00bbMontserrat||||||||\u00bb header_3_line_height=\u00bb1.5em\u00bb custom_padding=\u00bb10px|20px||20px\u00bb locked=\u00bboff\u00bb global_colors_info=\u00bb{}\u00bb]<\/p>\n

Nov 26th 2022<\/span><\/h3>\n

Prof. Sergio Conejeros<\/span><\/h3>\n

Modelizaci\u00f3n y Simulaci\u00f3n de Materiales<\/strong> (Video link)<\/a><\/span><\/p>\n

Departamento de Qu\u00edmica, Universidad Cat\u00f3lica del Norte, Antofagasta, Chile.<\/span><\/p>\n

Abstract<\/span><\/a><\/p>\n

<\/span><\/p>\n

[\/et_pb_text][\/et_pb_column][et_pb_column type=\u00bb1_3″ _builder_version=\u00bb4.16″ _module_preset=\u00bbdefault\u00bb background_color=\u00bb#ffffff\u00bb custom_padding=\u00bb|||\u00bb global_colors_info=\u00bb{}\u00bb custom_padding__hover=\u00bb|||\u00bb][et_pb_image src=\u00bbhttp:\/\/www.lafmat.com\/home\/wp-content\/uploads\/2022\/11\/Prof.-Antonio-Machado-2.0.png\u00bb title_text=\u00bbProf. Antonio Machado 2.0″ _builder_version=\u00bb4.17.0″ _module_preset=\u00bbdefault\u00bb global_colors_info=\u00bb{}\u00bb][\/et_pb_image][et_pb_text admin_label=\u00bbService Name\u00bb _builder_version=\u00bb4.17.0″ _module_preset=\u00bbdefault\u00bb text_font=\u00bbMontserrat||||||||\u00bb text_font_size=\u00bb15px\u00bb text_line_height=\u00bb1.8em\u00bb header_font=\u00bb||||||||\u00bb header_3_font=\u00bbMontserrat||||||||\u00bb header_3_line_height=\u00bb1.5em\u00bb custom_padding=\u00bb10px|20px||20px\u00bb locked=\u00bboff\u00bb global_colors_info=\u00bb{}\u00bb]<\/p>\n

Nov 19th 2022<\/span><\/h3>\n

Prof. Antonio J. da Silva Machado<\/span><\/h3>\n

Crystal Growth and superconducting properties of dichalcogenides MTe2 (M = Zr, Hf and Ti) intercalated with transition metal and rare earths <\/strong>(Video link)<\/a><\/p>\n

Escola de Engenharia de Lorena \u2013 EEL \u2013 USP, Brasil.<\/span><\/p>\n

Abstract<\/span><\/a><\/p>\n

<\/span><\/p>\n

[\/et_pb_text][\/et_pb_column][et_pb_column type=\u00bb1_3″ _builder_version=\u00bb4.16″ _module_preset=\u00bbdefault\u00bb background_color=\u00bb#ffffff\u00bb custom_padding=\u00bb|||\u00bb global_colors_info=\u00bb{}\u00bb custom_padding__hover=\u00bb|||\u00bb][et_pb_image src=\u00bbhttp:\/\/www.lafmat.com\/home\/wp-content\/uploads\/2022\/11\/Dr.-Diego-Lamas-2.0.png\u00bb title_text=\u00bbDr. Diego Lamas 2.0″ _builder_version=\u00bb4.17.0″ _module_preset=\u00bbdefault\u00bb global_colors_info=\u00bb{}\u00bb][\/et_pb_image][et_pb_text admin_label=\u00bbService Name\u00bb _builder_version=\u00bb4.17.0″ _module_preset=\u00bbdefault\u00bb text_font=\u00bbMontserrat||||||||\u00bb text_font_size=\u00bb15px\u00bb text_line_height=\u00bb1.8em\u00bb header_font=\u00bb||||||||\u00bb header_3_font=\u00bbMontserrat||||||||\u00bb header_3_line_height=\u00bb1.5em\u00bb custom_padding=\u00bb10px|20px||20px\u00bb locked=\u00bboff\u00bb global_colors_info=\u00bb{}\u00bb]<\/p>\n

Nov 12th 2022<\/span><\/h3>\n

Dr. Diego G. Lamas<\/span><\/h3>\n

\u00bfC\u00d3MO GENERAR OX\u00cdGENO EN MARTE?<\/strong>
El papel central de un electrolizador cer\u00e1mico en el experimento<\/strong> (Video link)<\/a><\/span><\/p>\n

Instistuto de Tecnolog\u00edas Emergentes y Ciencias Aplicadas (ITECA), UNSAM-CONICET, <\/span>Argentina.<\/span><\/p>\n

Abstract<\/span><\/a><\/span><\/p>\n

<\/span><\/p>\n

[\/et_pb_text][\/et_pb_column][\/et_pb_row][et_pb_row column_structure=\u00bb1_3,1_3,1_3″ use_custom_gutter=\u00bbon\u00bb gutter_width=\u00bb2″ _builder_version=\u00bb4.16″ _module_preset=\u00bbdefault\u00bb max_width=\u00bb1440px\u00bb custom_padding=\u00bb|||\u00bb use_custom_width=\u00bbon\u00bb custom_width_px=\u00bb1440px\u00bb global_colors_info=\u00bb{}\u00bb][et_pb_column type=\u00bb1_3″ _builder_version=\u00bb4.16″ _module_preset=\u00bbdefault\u00bb background_color=\u00bb#ffffff\u00bb custom_padding=\u00bb|||\u00bb global_colors_info=\u00bb{}\u00bb custom_padding__hover=\u00bb|||\u00bb][et_pb_image src=\u00bbhttp:\/\/www.lafmat.com\/home\/wp-content\/uploads\/2022\/10\/Dr.-Adrian-Ionescu.png\u00bb title_text=\u00bbDr. Adrian Ionescu\u00bb _builder_version=\u00bb4.17.0″ _module_preset=\u00bbdefault\u00bb global_colors_info=\u00bb{}\u00bb][\/et_pb_image][et_pb_text admin_label=\u00bbService Name\u00bb _builder_version=\u00bb4.17.0″ _module_preset=\u00bbdefault\u00bb text_font=\u00bbMontserrat||||||||\u00bb text_font_size=\u00bb15px\u00bb text_line_height=\u00bb1.8em\u00bb header_font=\u00bb||||||||\u00bb header_3_font=\u00bbMontserrat||||||||\u00bb header_3_line_height=\u00bb1.5em\u00bb custom_padding=\u00bb10px|20px||20px\u00bb locked=\u00bboff\u00bb global_colors_info=\u00bb{}\u00bb]<\/p>\n

Nov 5th 2022<\/span><\/h3>\n

Dr. Adrian Ionescu<\/span><\/h3>\n

Un viaje desde granel a trav\u00e9s de pel\u00edcula delgada y nanopart\u00edculas al magnetismo de superficie <\/strong>(Video link)<\/a><\/p>\n

Laboratorio Cavendish, Departamento de F\u00edsica, Universidad de Cambridge, Reino Unido.<\/span><\/p>\n

[\/et_pb_text][\/et_pb_column][et_pb_column type=\u00bb1_3″ _builder_version=\u00bb4.16″ _module_preset=\u00bbdefault\u00bb background_color=\u00bb#ffffff\u00bb custom_padding=\u00bb|||\u00bb global_colors_info=\u00bb{}\u00bb custom_padding__hover=\u00bb|||\u00bb][et_pb_image src=\u00bbhttp:\/\/www.lafmat.com\/home\/wp-content\/uploads\/2022\/10\/Dr.-Jose-Luis.jpg\u00bb title_text=\u00bbDr. Jos\u00e9 Luis\u00bb _builder_version=\u00bb4.17.0″ _module_preset=\u00bbdefault\u00bb global_colors_info=\u00bb{}\u00bb][\/et_pb_image][et_pb_text admin_label=\u00bbService Name\u00bb _builder_version=\u00bb4.17.0″ _module_preset=\u00bbdefault\u00bb text_font=\u00bbMontserrat||||||||\u00bb text_font_size=\u00bb15px\u00bb text_line_height=\u00bb1.8em\u00bb header_font=\u00bb||||||||\u00bb header_3_font=\u00bbMontserrat||||||||\u00bb header_3_line_height=\u00bb1.5em\u00bb custom_padding=\u00bb10px|20px||20px\u00bb locked=\u00bboff\u00bb global_colors_info=\u00bb{}\u00bb]<\/p>\n

Oct 29th 2022<\/span><\/h3>\n

Prof. Jos\u00e9 Luis Ochoa<\/span><\/h3>\n

Propiedades el\u00e9ctricas y modelos de percolaci\u00f3n aplicados a mezclas: aislante-conductor<\/strong> (Video link)<\/a><\/span><\/p>\n

Instituto Venezolano de Investigaciones Cient\u00edficas (IVIC), <\/span>Venezuela<\/p>\n

Abstract<\/span><\/a><\/p>\n

 <\/p>\n

[\/et_pb_text][\/et_pb_column][et_pb_column type=\u00bb1_3″ _builder_version=\u00bb4.16″ _module_preset=\u00bbdefault\u00bb background_color=\u00bb#ffffff\u00bb custom_padding=\u00bb|||\u00bb global_colors_info=\u00bb{}\u00bb custom_padding__hover=\u00bb|||\u00bb][et_pb_image src=\u00bbhttp:\/\/www.lafmat.com\/home\/wp-content\/uploads\/2022\/10\/Prof.-Sergio-Rezenda.png\u00bb title_text=\u00bbProf. Sergio Rezenda\u00bb _builder_version=\u00bb4.17.0″ _module_preset=\u00bbdefault\u00bb global_colors_info=\u00bb{}\u00bb][\/et_pb_image][et_pb_text admin_label=\u00bbService Name\u00bb _builder_version=\u00bb4.17.0″ _module_preset=\u00bbdefault\u00bb text_font=\u00bbMontserrat||||||||\u00bb text_font_size=\u00bb15px\u00bb text_line_height=\u00bb1.8em\u00bb header_font=\u00bb||||||||\u00bb header_3_font=\u00bbMontserrat||||||||\u00bb header_3_line_height=\u00bb1.5em\u00bb custom_padding=\u00bb9px|20px||20px||\u00bb locked=\u00bboff\u00bb global_colors_info=\u00bb{}\u00bb]<\/p>\n

Oct 22th 2022<\/span><\/h3>\n

Prof. Sergio Rezende<\/span><\/h3>\n

Spintr\u00f4nica: Fundamentos e avan\u00e7os recentes <\/strong>(Video link)<\/a><\/p>\n

Universidad Federal de Pernambuco, <\/span>Brasil<\/span><\/p>\n

<\/span><\/p>\n

<\/span><\/p>\n

[\/et_pb_text][\/et_pb_column][\/et_pb_row][et_pb_row column_structure=\u00bb1_3,1_3,1_3″ use_custom_gutter=\u00bbon\u00bb gutter_width=\u00bb2″ _builder_version=\u00bb4.16″ _module_preset=\u00bbdefault\u00bb max_width=\u00bb1440px\u00bb custom_padding=\u00bb|||\u00bb use_custom_width=\u00bbon\u00bb custom_width_px=\u00bb1440px\u00bb global_colors_info=\u00bb{}\u00bb][et_pb_column type=\u00bb1_3″ _builder_version=\u00bb4.16″ _module_preset=\u00bbdefault\u00bb background_color=\u00bb#ffffff\u00bb custom_padding=\u00bb|||\u00bb global_colors_info=\u00bb{}\u00bb custom_padding__hover=\u00bb|||\u00bb][et_pb_image src=\u00bbhttp:\/\/www.lafmat.com\/home\/wp-content\/uploads\/2022\/10\/Prof.-Armando-Navarro..png\u00bb title_text=\u00bbProf. Armando Navarro.\u00bb _builder_version=\u00bb4.17.0″ _module_preset=\u00bbdefault\u00bb global_colors_info=\u00bb{}\u00bb][\/et_pb_image][et_pb_text admin_label=\u00bbService Name\u00bb _builder_version=\u00bb4.17.0″ _module_preset=\u00bbdefault\u00bb text_font=\u00bbMontserrat||||||||\u00bb text_font_size=\u00bb15px\u00bb text_line_height=\u00bb1.8em\u00bb header_font=\u00bb||||||||\u00bb header_3_font=\u00bbMontserrat||||||||\u00bb header_3_line_height=\u00bb1.5em\u00bb custom_padding=\u00bb10px|20px||20px\u00bb locked=\u00bboff\u00bb global_colors_info=\u00bb{}\u00bb]<\/p>\n

Oct 15th 2022<\/span><\/h3>\n

Prof. Armando Navarro<\/span><\/h3>\n

How material science can help natural product chemists<\/strong> (Video link)<\/a><\/span><\/p>\n

Universidad Federal de Pernambuco, <\/span>Recife PE, Brasil<\/span><\/p>\n

Abstract<\/a><\/span><\/p>\n

 <\/p>\n

[\/et_pb_text][\/et_pb_column][et_pb_column type=\u00bb1_3″ _builder_version=\u00bb4.16″ _module_preset=\u00bbdefault\u00bb background_color=\u00bb#ffffff\u00bb custom_padding=\u00bb|||\u00bb global_colors_info=\u00bb{}\u00bb custom_padding__hover=\u00bb|||\u00bb][et_pb_image src=\u00bbhttp:\/\/www.lafmat.com\/home\/wp-content\/uploads\/2022\/10\/Dr.-Peter-Newton-2.0.png\u00bb title_text=\u00bbDr. Peter Newton 2.0″ _builder_version=\u00bb4.17.0″ _module_preset=\u00bbdefault\u00bb global_colors_info=\u00bb{}\u00bb][\/et_pb_image][et_pb_text admin_label=\u00bbService Name\u00bb _builder_version=\u00bb4.17.0″ _module_preset=\u00bbdefault\u00bb text_font=\u00bbMontserrat||||||||\u00bb text_font_size=\u00bb15px\u00bb text_line_height=\u00bb1.8em\u00bb header_font=\u00bb||||||||\u00bb header_3_font=\u00bbMontserrat||||||||\u00bb header_3_line_height=\u00bb1.5em\u00bb custom_padding=\u00bb10px|20px||20px\u00bb locked=\u00bboff\u00bb global_colors_info=\u00bb{}\u00bb]<\/p>\n

Oct 08 2022<\/span><\/h3>\n

Dr. Peter J. Newton<\/span><\/h3>\n

Composite Element Bacodes as Portable Magnetric Memories<\/strong> (Video link)<\/a><\/span><\/p>\n

Cavendish Laboratory, <\/span>Cambridge University, UK –\u00a0<\/span>University of Kent, UK.<\/p>\n

[\/et_pb_text][\/et_pb_column][et_pb_column type=\u00bb1_3″ _builder_version=\u00bb4.16″ _module_preset=\u00bbdefault\u00bb background_color=\u00bb#ffffff\u00bb custom_padding=\u00bb|||\u00bb global_colors_info=\u00bb{}\u00bb custom_padding__hover=\u00bb|||\u00bb][et_pb_image src=\u00bbhttp:\/\/www.lafmat.com\/home\/wp-content\/uploads\/2022\/09\/Prof.-Alexei-Vagov.png\u00bb title_text=\u00bbProf. Alexei Vagov\u00bb _builder_version=\u00bb4.17.0″ _module_preset=\u00bbdefault\u00bb global_colors_info=\u00bb{}\u00bb][\/et_pb_image][et_pb_text admin_label=\u00bbService Name\u00bb _builder_version=\u00bb4.17.0″ _module_preset=\u00bbdefault\u00bb text_font=\u00bbMontserrat||||||||\u00bb text_font_size=\u00bb15px\u00bb text_line_height=\u00bb1.8em\u00bb header_font=\u00bb||||||||\u00bb header_3_font=\u00bbMontserrat||||||||\u00bb header_3_line_height=\u00bb1.5em\u00bb custom_padding=\u00bb10px|20px||20px\u00bb locked=\u00bboff\u00bb global_colors_info=\u00bb{}\u00bb]<\/p>\n

Sep 24th 2022<\/span><\/h3>\n

Prof. Alexei Vagov<\/span><\/h3>\n

Exotic magnetic Flux patterns in superconductors between type I and type II<\/strong> (Video link)<\/a><\/span><\/p>\n

HSE Reserach University, <\/span>Mosc\u00fa – Rusia.<\/p>\n

Abstract<\/a><\/p>\n

<\/span><\/p>\n

[\/et_pb_text][\/et_pb_column][\/et_pb_row][et_pb_row column_structure=\u00bb1_3,1_3,1_3″ use_custom_gutter=\u00bbon\u00bb gutter_width=\u00bb2″ _builder_version=\u00bb4.16″ _module_preset=\u00bbdefault\u00bb max_width=\u00bb1440px\u00bb custom_padding=\u00bb|||\u00bb use_custom_width=\u00bbon\u00bb custom_width_px=\u00bb1440px\u00bb global_colors_info=\u00bb{}\u00bb][et_pb_column type=\u00bb1_3″ _builder_version=\u00bb4.16″ _module_preset=\u00bbdefault\u00bb background_color=\u00bb#ffffff\u00bb custom_padding=\u00bb|||\u00bb global_colors_info=\u00bb{}\u00bb custom_padding__hover=\u00bb|||\u00bb][et_pb_image src=\u00bbhttp:\/\/www.lafmat.com\/home\/wp-content\/uploads\/2022\/09\/Dra.-Laura-Corredor-2.0.png\u00bb title_text=\u00bbDra. Laura Corredor 2.0″ _builder_version=\u00bb4.17.0″ _module_preset=\u00bbdefault\u00bb global_colors_info=\u00bb{}\u00bb][\/et_pb_image][et_pb_text admin_label=\u00bbService Name\u00bb _builder_version=\u00bb4.17.0″ _module_preset=\u00bbdefault\u00bb text_font=\u00bbMontserrat||||||||\u00bb text_font_size=\u00bb15px\u00bb text_line_height=\u00bb1.8em\u00bb header_font=\u00bb||||||||\u00bb header_3_font=\u00bbMontserrat||||||||\u00bb header_3_line_height=\u00bb1.5em\u00bb custom_padding=\u00bb10px|20px||20px\u00bb locked=\u00bboff\u00bb global_colors_info=\u00bb{}\u00bb]<\/p>\n

Sep 17th 2022<\/span><\/h3>\n

Dra. Laura Corredor-Boh\u00f3rquez<\/span><\/h3>\n

Magnetism of Vander Waals compounds: from magnetic topological insulators to 2D magnets<\/strong> (Video link)<\/a><\/span><\/p>\n

Lebnibz Institute for Solid and Materials Research – IPW, <\/span>Dresden- Alemania.<\/span><\/p>\n

<\/span><\/p>\n

[\/et_pb_text][\/et_pb_column][et_pb_column type=\u00bb1_3″ _builder_version=\u00bb4.16″ _module_preset=\u00bbdefault\u00bb background_color=\u00bb#ffffff\u00bb custom_padding=\u00bb|||\u00bb global_colors_info=\u00bb{}\u00bb custom_padding__hover=\u00bb|||\u00bb][et_pb_image src=\u00bbhttp:\/\/www.lafmat.com\/home\/wp-content\/uploads\/2022\/09\/Prof.-Antonio-Romaguera-2.0.png\u00bb title_text=\u00bbProf. Ant\u00f4nio Romaguera 2.0″ _builder_version=\u00bb4.17.0″ _module_preset=\u00bbdefault\u00bb global_colors_info=\u00bb{}\u00bb][\/et_pb_image][et_pb_text admin_label=\u00bbService Name\u00bb _builder_version=\u00bb4.17.0″ _module_preset=\u00bbdefault\u00bb text_font=\u00bbMontserrat||||||||\u00bb text_font_size=\u00bb15px\u00bb text_line_height=\u00bb1.8em\u00bb header_font=\u00bb||||||||\u00bb header_3_font=\u00bbMontserrat||||||||\u00bb header_3_line_height=\u00bb1.5em\u00bb custom_padding=\u00bb10px|20px||20px\u00bb locked=\u00bboff\u00bb global_colors_info=\u00bb{}\u00bb]<\/p>\n

Sep 10th 2022<\/span><\/h3>\n

Prof. Ant\u00f4nio Romaguera<\/span><\/h3>\n

Intermediate type-I superconductors in the mesoscopic scale<\/strong> (Video link)<\/a><\/span><\/p>\n

Universidade Federal Rural de Pernambuco (UFRPE), <\/span>Departamento de Recife, RE, Brasil.<\/span><\/p>\n

[\/et_pb_text][\/et_pb_column][et_pb_column type=\u00bb1_3″ _builder_version=\u00bb4.16″ _module_preset=\u00bbdefault\u00bb background_color=\u00bb#ffffff\u00bb custom_padding=\u00bb|||\u00bb global_colors_info=\u00bb{}\u00bb custom_padding__hover=\u00bb|||\u00bb][et_pb_image src=\u00bbhttp:\/\/www.lafmat.com\/home\/wp-content\/uploads\/2022\/09\/indice.jpg\u00bb title_text=\u00bb\u00edndice\u00bb _builder_version=\u00bb4.17.0″ _module_preset=\u00bbdefault\u00bb global_colors_info=\u00bb{}\u00bb][\/et_pb_image][et_pb_text admin_label=\u00bbService Name\u00bb _builder_version=\u00bb4.17.0″ _module_preset=\u00bbdefault\u00bb text_font=\u00bbMontserrat||||||||\u00bb text_font_size=\u00bb15px\u00bb text_line_height=\u00bb1.8em\u00bb header_font=\u00bb||||||||\u00bb header_3_font=\u00bbMontserrat||||||||\u00bb header_3_line_height=\u00bb1.5em\u00bb custom_padding=\u00bb10px|20px||20px\u00bb locked=\u00bboff\u00bb global_colors_info=\u00bb{}\u00bb]<\/p>\n

Sep 3rd 2022<\/h3>\n

Prof. Michael Cabrera Baez<\/h3>\n

Conduction electron spin resonance in the nearly ferromagnetic Fermi liquid YFe2Zn20 <\/strong>(Video link)<\/a><\/p>\n

Universidade Federal de Pernambuco, Brasil.<\/p>\n

Abstract<\/a><\/p>\n

 <\/p>\n

[\/et_pb_text][\/et_pb_column][\/et_pb_row][et_pb_row column_structure=\u00bb1_3,1_3,1_3″ use_custom_gutter=\u00bbon\u00bb gutter_width=\u00bb2″ _builder_version=\u00bb4.16″ _module_preset=\u00bbdefault\u00bb max_width=\u00bb1440px\u00bb custom_padding=\u00bb|||\u00bb use_custom_width=\u00bbon\u00bb custom_width_px=\u00bb1440px\u00bb global_colors_info=\u00bb{}\u00bb][et_pb_column type=\u00bb1_3″ _builder_version=\u00bb4.16″ _module_preset=\u00bbdefault\u00bb background_color=\u00bb#ffffff\u00bb custom_padding=\u00bb|||\u00bb global_colors_info=\u00bb{}\u00bb custom_padding__hover=\u00bb|||\u00bb][et_pb_image src=\u00bbhttp:\/\/www.lafmat.com\/home\/wp-content\/uploads\/2022\/09\/Prof.-Eduardo-Barros.png\u00bb title_text=\u00bbProf. Eduardo Barros\u00bb _builder_version=\u00bb4.17.0″ _module_preset=\u00bbdefault\u00bb global_colors_info=\u00bb{}\u00bb][\/et_pb_image][et_pb_text admin_label=\u00bbService Name\u00bb _builder_version=\u00bb4.17.0″ _module_preset=\u00bbdefault\u00bb text_font=\u00bbMontserrat||||||||\u00bb text_font_size=\u00bb15px\u00bb text_line_height=\u00bb1.8em\u00bb header_font=\u00bb||||||||\u00bb header_3_font=\u00bbMontserrat||||||||\u00bb header_3_line_height=\u00bb1.5em\u00bb custom_padding=\u00bb10px|20px||20px\u00bb locked=\u00bboff\u00bb global_colors_info=\u00bb{}\u00bb]<\/p>\n

Aug 27th 2022<\/h3>\n

Prof. Eduardo Bed\u00ea Barros<\/h3>\n

Light Matter Interaction in Plasmonic Supercrystals<\/strong>\u00a0(Video link)<\/a><\/p>\n

Universidade Federal do Cear\u00e1, Brasil.<\/p>\n

Abstract<\/a><\/p>\n

 <\/p>\n

[\/et_pb_text][\/et_pb_column][et_pb_column type=\u00bb1_3″ _builder_version=\u00bb4.16″ _module_preset=\u00bbdefault\u00bb background_color=\u00bb#ffffff\u00bb custom_padding=\u00bb|||\u00bb global_colors_info=\u00bb{}\u00bb custom_padding__hover=\u00bb|||\u00bb][et_pb_image src=\u00bbhttp:\/\/www.lafmat.com\/home\/wp-content\/uploads\/2022\/09\/Prof.-Paulo-Pureur.png\u00bb title_text=\u00bbProf. Paulo Pureur\u00bb _builder_version=\u00bb4.17.0″ _module_preset=\u00bbdefault\u00bb global_colors_info=\u00bb{}\u00bb][\/et_pb_image][et_pb_text admin_label=\u00bbService Name\u00bb _builder_version=\u00bb4.17.0″ _module_preset=\u00bbdefault\u00bb text_font=\u00bbMontserrat||||||||\u00bb text_font_size=\u00bb15px\u00bb text_line_height=\u00bb1.8em\u00bb header_font=\u00bb||||||||\u00bb header_3_font=\u00bbMontserrat||||||||\u00bb header_3_line_height=\u00bb1.5em\u00bb custom_padding=\u00bb10px|20px||20px\u00bb locked=\u00bboff\u00bb global_colors_info=\u00bb{}\u00bb]<\/p>\n

Aug 20th 2022<\/h3>\n

Dr. Paulo Pureur<\/h3>\n

Hall Effect and Pseudogap in the High Temperature Superconductors Bi2Sr2CaCu2O8+x and YBa2Cu3O7-d<\/strong> (Video link)<\/a><\/p>\n

Universidade Federal do Rio Grande do Sul (UFRGS), <\/span>Brasil,<\/span><\/p>\n

Abstract<\/a><\/p>\n

<\/span><\/p>\n

[\/et_pb_text][\/et_pb_column][et_pb_column type=\u00bb1_3″ _builder_version=\u00bb4.16″ _module_preset=\u00bbdefault\u00bb background_color=\u00bb#ffffff\u00bb custom_padding=\u00bb|||\u00bb global_colors_info=\u00bb{}\u00bb custom_padding__hover=\u00bb|||\u00bb][et_pb_image src=\u00bbhttp:\/\/www.lafmat.com\/home\/wp-content\/uploads\/2022\/08\/Prof.-Flavio-Garcia.png\u00bb title_text=\u00bbProf. Fl\u00e1vio Garcia\u00bb _builder_version=\u00bb4.17.0″ _module_preset=\u00bbdefault\u00bb global_colors_info=\u00bb{}\u00bb][\/et_pb_image][et_pb_text admin_label=\u00bbService Name\u00bb _builder_version=\u00bb4.17.0″ _module_preset=\u00bbdefault\u00bb text_font=\u00bbMontserrat||||||||\u00bb text_font_size=\u00bb15px\u00bb text_line_height=\u00bb1.8em\u00bb header_font=\u00bb||||||||\u00bb header_3_font=\u00bbMontserrat||||||||\u00bb header_3_line_height=\u00bb1.5em\u00bb custom_padding=\u00bb10px|20px||20px\u00bb locked=\u00bboff\u00bb global_colors_info=\u00bb{}\u00bb]<\/p>\n

Aug 13th 2022<\/h3>\n

Prof. Fl\u00e1vio Garcia<\/h3>\n

Multifunctional Magnetic Materials<\/strong>\u00a0(Video link)<\/a><\/p>\n

Centro Brasileiro de Pesquisas F\u00edsicas – CBPF, Brasil.<\/p>\n

 <\/p>\n

[\/et_pb_text][\/et_pb_column][\/et_pb_row][et_pb_row column_structure=\u00bb1_3,1_3,1_3″ use_custom_gutter=\u00bbon\u00bb gutter_width=\u00bb2″ _builder_version=\u00bb4.16″ _module_preset=\u00bbdefault\u00bb max_width=\u00bb1440px\u00bb custom_padding=\u00bb|||\u00bb use_custom_width=\u00bbon\u00bb custom_width_px=\u00bb1440px\u00bb global_colors_info=\u00bb{}\u00bb][et_pb_column type=\u00bb1_3″ _builder_version=\u00bb4.16″ _module_preset=\u00bbdefault\u00bb background_color=\u00bb#ffffff\u00bb custom_padding=\u00bb|||\u00bb global_colors_info=\u00bb{}\u00bb custom_padding__hover=\u00bb|||\u00bb][et_pb_image src=\u00bbhttp:\/\/www.lafmat.com\/home\/wp-content\/uploads\/2022\/08\/Prof.-Felipe-Mondaca.png\u00bb title_text=\u00bbProf. Felipe Mondaca\u00bb _builder_version=\u00bb4.17.0″ _module_preset=\u00bbdefault\u00bb global_colors_info=\u00bb{}\u00bb][\/et_pb_image][et_pb_text admin_label=\u00bbService Name\u00bb _builder_version=\u00bb4.17.0″ _module_preset=\u00bbdefault\u00bb text_font=\u00bbMontserrat||||||||\u00bb text_font_size=\u00bb15px\u00bb text_line_height=\u00bb1.8em\u00bb header_font=\u00bb||||||||\u00bb header_3_font=\u00bbMontserrat||||||||\u00bb header_3_line_height=\u00bb1.5em\u00bb custom_padding=\u00bb10px|20px||20px\u00bb locked=\u00bboff\u00bb global_colors_info=\u00bb{}\u00bb]<\/p>\n

Aug 6th 2022<\/h3>\n

Prof. Felipe Mondaca Espinoza<\/h3>\n

Propiedades electr\u00f3nicas del SnO2 dopado y sistemas MOF por c\u00e1lculos ab initio<\/strong> (Video link)<\/a><\/p>\n

Universidad San Sebasti\u00e1n, Puerto Montt, Chile.<\/p>\n

\u00a0Abstract<\/a><\/p>\n

 <\/p>\n

[\/et_pb_text][\/et_pb_column][et_pb_column type=\u00bb1_3″ _builder_version=\u00bb4.16″ _module_preset=\u00bbdefault\u00bb background_color=\u00bb#ffffff\u00bb custom_padding=\u00bb|||\u00bb global_colors_info=\u00bb{}\u00bb custom_padding__hover=\u00bb|||\u00bb][et_pb_image src=\u00bbhttp:\/\/www.lafmat.com\/home\/wp-content\/uploads\/2022\/07\/Dra.-Anna-Palau-Poster-1.png\u00bb title_text=\u00bbDra. Anna Palau-P\u00f3ster\u00bb _builder_version=\u00bb4.17.0″ _module_preset=\u00bbdefault\u00bb global_colors_info=\u00bb{}\u00bb][\/et_pb_image][et_pb_text admin_label=\u00bbService Name\u00bb _builder_version=\u00bb4.17.0″ _module_preset=\u00bbdefault\u00bb text_font=\u00bbMontserrat||||||||\u00bb text_font_size=\u00bb15px\u00bb text_line_height=\u00bb1.8em\u00bb header_font=\u00bb||||||||\u00bb header_3_font=\u00bbMontserrat||||||||\u00bb header_3_line_height=\u00bb1.5em\u00bb custom_padding=\u00bb10px|20px||20px\u00bb locked=\u00bboff\u00bb global_colors_info=\u00bb{}\u00bb]<\/p>\n

Jul 30th 2022<\/h3>\n

Dra. Anna Palau<\/h3>\n

Nano-engineered high-temperature superconductors and hybrid systems for energy-efficient functional devices<\/strong> (Video link)<\/a><\/p>\n

Instituto de Ciencias\u00a0 de Materiales de Barcelona (ICMB), <\/span>Espa\u00f1a.<\/span><\/p>\n

[\/et_pb_text][\/et_pb_column][et_pb_column type=\u00bb1_3″ _builder_version=\u00bb4.16″ _module_preset=\u00bbdefault\u00bb background_color=\u00bb#ffffff\u00bb custom_padding=\u00bb|||\u00bb global_colors_info=\u00bb{}\u00bb custom_padding__hover=\u00bb|||\u00bb][et_pb_image src=\u00bbhttp:\/\/www.lafmat.com\/home\/wp-content\/uploads\/2022\/07\/Prof.-Bernat-Bozzo-anuncio.jpeg\u00bb title_text=\u00bbProf. Bernat Bozzo anuncio\u00bb _builder_version=\u00bb4.17.0″ _module_preset=\u00bbdefault\u00bb global_colors_info=\u00bb{}\u00bb][\/et_pb_image][et_pb_text _builder_version=\u00bb4.17.0″ _module_preset=\u00bbdefault\u00bb text_font=\u00bbMontserrat||||||||\u00bb text_font_size=\u00bb15px\u00bb text_line_height=\u00bb1.8em\u00bb custom_margin=\u00bb10px|20px|10px|20px|false|false\u00bb custom_padding=\u00bb||||false|false\u00bb global_colors_info=\u00bb{}\u00bb]<\/p>\n

Jul 23th<\/h3>\n

Prof. Bernat Bozzo<\/h3>\n

Artifacts in magnetic measurements<\/strong> (Video link)<\/a><\/p>\n

Instituto de Ciencia de Materiales de Barcelona (ICMAB), <\/span>Espa\u00f1a.<\/span><\/p>\n

 <\/p>\n

[\/et_pb_text][\/et_pb_column][\/et_pb_row][et_pb_row column_structure=\u00bb1_3,1_3,1_3″ use_custom_gutter=\u00bbon\u00bb gutter_width=\u00bb2″ _builder_version=\u00bb4.16″ _module_preset=\u00bbdefault\u00bb max_width=\u00bb1440px\u00bb custom_padding=\u00bb|||\u00bb use_custom_width=\u00bbon\u00bb custom_width_px=\u00bb1440px\u00bb global_colors_info=\u00bb{}\u00bb][et_pb_column type=\u00bb1_3″ _builder_version=\u00bb4.16″ _module_preset=\u00bbdefault\u00bb background_color=\u00bb#ffffff\u00bb custom_padding=\u00bb|||\u00bb global_colors_info=\u00bb{}\u00bb custom_padding__hover=\u00bb|||\u00bb][et_pb_image src=\u00bbhttp:\/\/www.lafmat.com\/home\/wp-content\/uploads\/2022\/07\/Prof.-Mario-Reis.png\u00bb title_text=\u00bbProf. Mario Reis\u00bb _builder_version=\u00bb4.17.0″ _module_preset=\u00bbdefault\u00bb global_colors_info=\u00bb{}\u00bb][\/et_pb_image][et_pb_text _builder_version=\u00bb4.17.0″ _module_preset=\u00bbdefault\u00bb text_font=\u00bbMontserrat||||||||\u00bb text_font_size=\u00bb15px\u00bb text_line_height=\u00bb1.8em\u00bb custom_margin=\u00bb10px|20px|10px|20px|false|false\u00bb custom_padding=\u00bb||||false|false\u00bb global_colors_info=\u00bb{}\u00bb]<\/p>\n

Jul 16th 2022<\/h3>\n

Prof. Mario Reis<\/h3>\n

Magnetocaloric and barocaloric effects of metal complexes for solid state cooling<\/strong> (Video link)<\/a><\/p>\n

Instituto de F\u00edsica, Universidade Federal Fluminense, Niter\u00f3i-RJ, Brasil<\/p>\n

Departamento de F\u00edsica de la Materia Condensada, Universidad de Sevilla, Sevilla, Espa\u00f1a<\/p>\n

 <\/p>\n

[\/et_pb_text][\/et_pb_column][et_pb_column type=\u00bb1_3″ _builder_version=\u00bb4.16″ _module_preset=\u00bbdefault\u00bb background_color=\u00bb#ffffff\u00bb custom_padding=\u00bb|||\u00bb global_colors_info=\u00bb{}\u00bb custom_padding__hover=\u00bb|||\u00bb][et_pb_image src=\u00bbhttp:\/\/www.lafmat.com\/home\/wp-content\/uploads\/2022\/07\/Prof.-Antonio-G.-de-Souza-Filho.png\u00bb title_text=\u00bbProf. Antonio G. de Souza Filho\u00bb _builder_version=\u00bb4.17.0″ _module_preset=\u00bbdefault\u00bb global_colors_info=\u00bb{}\u00bb][\/et_pb_image][et_pb_text admin_label=\u00bbService Name\u00bb _builder_version=\u00bb4.17.0″ _module_preset=\u00bbdefault\u00bb text_font=\u00bbMontserrat||||||||\u00bb text_font_size=\u00bb15px\u00bb text_line_height=\u00bb1.8em\u00bb header_font=\u00bb||||||||\u00bb header_3_font=\u00bbMontserrat||||||||\u00bb header_3_line_height=\u00bb1.5em\u00bb custom_padding=\u00bb10px|20px||20px\u00bb locked=\u00bboff\u00bb global_colors_info=\u00bb{}\u00bb]<\/p>\n

Jul 9th 2022<\/h3>\n

Prof. Antonio G. de Souza Filho<\/h3>\n

1D and 2D nanomaterials under high-pressure conditions\u00a0<\/strong> (Video link)<\/a><\/p>\n

Universidade Federal do Cear\u00e1 (UFC), Departamento de F\u00edsica Fortaleza-Brasil.<\/span><\/p>\n

[\/et_pb_text][\/et_pb_column][et_pb_column type=\u00bb1_3″ _builder_version=\u00bb4.16″ _module_preset=\u00bbdefault\u00bb background_color=\u00bb#ffffff\u00bb custom_padding=\u00bb|||\u00bb global_colors_info=\u00bb{}\u00bb custom_padding__hover=\u00bb|||\u00bb][et_pb_image src=\u00bbhttp:\/\/www.lafmat.com\/home\/wp-content\/uploads\/2022\/07\/Dr.-Javier-Cuervo.jpeg\u00bb title_text=\u00bbDr. Javier Cuervo\u00bb _builder_version=\u00bb4.17.0″ _module_preset=\u00bbdefault\u00bb global_colors_info=\u00bb{}\u00bb][\/et_pb_image][et_pb_text _builder_version=\u00bb4.17.0″ _module_preset=\u00bbdefault\u00bb text_font=\u00bbMontserrat||||||||\u00bb text_font_size=\u00bb15px\u00bb text_line_height=\u00bb1.8em\u00bb custom_padding=\u00bb10px|20px||20px|false|false\u00bb global_colors_info=\u00bb{}\u00bb]<\/p>\n

Jul 2nd 2022<\/h3>\n

Dr. Javier Cuervo<\/h3>\n

Efecto de la sustituci\u00f3n de Mn3+ por Fe3+ en las propiedades el\u00e9ctricas y magn\u00e9ticas de los nuevos materiales Sr(1.32)R(2.68)Ti(1.32)Mn(2.68)O12 (R=Nd, Sm)<\/strong> (Video link)<\/a><\/span><\/p>\n

Universidad Pedag\u00f3gica y Tecnol\u00f3gica de Colombia – Tunja<\/span><\/p>\n

[\/et_pb_text][\/et_pb_column][\/et_pb_row][et_pb_row column_structure=\u00bb1_3,1_3,1_3″ use_custom_gutter=\u00bbon\u00bb gutter_width=\u00bb2″ _builder_version=\u00bb4.16″ _module_preset=\u00bbdefault\u00bb max_width=\u00bb1440px\u00bb custom_padding=\u00bb|||\u00bb use_custom_width=\u00bbon\u00bb custom_width_px=\u00bb1440px\u00bb global_colors_info=\u00bb{}\u00bb][et_pb_column type=\u00bb1_3″ _builder_version=\u00bb4.16″ _module_preset=\u00bbdefault\u00bb background_color=\u00bb#ffffff\u00bb custom_padding=\u00bb|||\u00bb global_colors_info=\u00bb{}\u00bb custom_padding__hover=\u00bb|||\u00bb][et_pb_image src=\u00bbhttp:\/\/www.lafmat.com\/home\/wp-content\/uploads\/2022\/05\/Dr.-A.-S.-Mosquera-Polo.png\u00bb title_text=\u00bbDr. A. S. Mosquera Polo\u00bb _builder_version=\u00bb4.17.0″ _module_preset=\u00bbdefault\u00bb global_colors_info=\u00bb{}\u00bb][\/et_pb_image][et_pb_text admin_label=\u00bbService Name\u00bb _builder_version=\u00bb4.17.0″ _module_preset=\u00bbdefault\u00bb text_font=\u00bbMontserrat||||||||\u00bb text_font_size=\u00bb15px\u00bb text_line_height=\u00bb1.8em\u00bb header_font=\u00bb||||||||\u00bb header_3_font=\u00bbMontserrat||||||||\u00bb header_3_line_height=\u00bb1.5em\u00bb custom_padding=\u00bb10px|20px||20px\u00bb global_colors_info=\u00bb{}\u00bb]<\/p>\n

Jun 4th 2022<\/h3>\n

Dr. A. S. Mosquera Polo<\/h3>\n

Texturas de fase inter-bandas no equilibradas inducidas por la disociaci\u00f3n de v\u00f3rtices en un superconductor de dos bandas<\/strong> (Video link)<\/a><\/p>\n

Universidad de Magdalena, Colombia.<\/p>\n

[\/et_pb_text][\/et_pb_column][et_pb_column type=\u00bb1_3″ _builder_version=\u00bb4.16″ _module_preset=\u00bbdefault\u00bb background_color=\u00bb#ffffff\u00bb custom_padding=\u00bb|||\u00bb global_colors_info=\u00bb{}\u00bb custom_padding__hover=\u00bb|||\u00bb][et_pb_image src=\u00bbhttp:\/\/www.lafmat.com\/home\/wp-content\/uploads\/2022\/05\/Dr.-Francisco-Paraguay.png\u00bb title_text=\u00bbDr. Francisco Paraguay\u00bb _builder_version=\u00bb4.17.0″ _module_preset=\u00bbdefault\u00bb global_colors_info=\u00bb{}\u00bb][\/et_pb_image][et_pb_text admin_label=\u00bbService Name\u00bb _builder_version=\u00bb4.17.0″ _module_preset=\u00bbdefault\u00bb text_font=\u00bbMontserrat||||||||\u00bb text_font_size=\u00bb15px\u00bb text_line_height=\u00bb1.8em\u00bb header_font=\u00bb||||||||\u00bb header_3_font=\u00bbMontserrat||||||||\u00bb header_3_line_height=\u00bb1.5em\u00bb custom_padding=\u00bb10px|20px||20px\u00bb locked=\u00bboff\u00bb global_colors_info=\u00bb{}\u00bb]<\/p>\n

May 28th 2022<\/h3>\n

Dr. Francisco Paraguay Delgado<\/h3>\n

Estudio de materiales por t\u00e9cnicas de microscopia electr\u00f3nic<\/strong>a (Video link)<\/a><\/span><\/p>\n

Centro de Investigaci\u00f3n en Materiales Avanzados (CIMAV), M\u00e9xico.<\/span><\/p>\n

[\/et_pb_text][\/et_pb_column][et_pb_column type=\u00bb1_3″ _builder_version=\u00bb4.16″ _module_preset=\u00bbdefault\u00bb background_color=\u00bb#ffffff\u00bb custom_padding=\u00bb|||\u00bb global_colors_info=\u00bb{}\u00bb custom_padding__hover=\u00bb|||\u00bb][et_pb_image src=\u00bbhttp:\/\/www.lafmat.com\/home\/wp-content\/uploads\/2022\/05\/Profesor-Nelson-Moreno.png\u00bb title_text=\u00bbProfesor Nelson Moreno\u00bb _builder_version=\u00bb4.17.0″ _module_preset=\u00bbdefault\u00bb global_colors_info=\u00bb{}\u00bb][\/et_pb_image][et_pb_text admin_label=\u00bbService Name\u00bb _builder_version=\u00bb4.17.0″ _module_preset=\u00bbdefault\u00bb text_font=\u00bbMontserrat||||||||\u00bb text_font_size=\u00bb15px\u00bb text_line_height=\u00bb1.8em\u00bb header_font=\u00bb||||||||\u00bb header_3_font=\u00bbMontserrat||||||||\u00bb header_3_line_height=\u00bb1.5em\u00bb custom_padding=\u00bb10px|20px||20px\u00bb locked=\u00bboff\u00bb global_colors_info=\u00bb{}\u00bb]<\/p>\n

May 21th 2022<\/h3>\n

Prof. Nelson O. Moreno Salazar<\/h3>\n

Efecto magnetocal\u00f3rico de los intermet\u00e1licos Nd2(Rh,Ir)In8, Nd2Ni2In8 y ajuste de la transici\u00f3n metamagn\u00e9tica de la serie RRhIn5 (R = Nd, Tb, Dy ,Ho)<\/strong> (Video link)<\/a><\/p>\n

Universidade Federal de Sergipe (UFS), Brasil.<\/span><\/p>\n

 <\/p>\n

[\/et_pb_text][\/et_pb_column][\/et_pb_row][et_pb_row column_structure=\u00bb1_3,1_3,1_3″ use_custom_gutter=\u00bbon\u00bb gutter_width=\u00bb2″ _builder_version=\u00bb4.16″ _module_preset=\u00bbdefault\u00bb max_width=\u00bb1440px\u00bb custom_padding=\u00bb|||\u00bb use_custom_width=\u00bbon\u00bb custom_width_px=\u00bb1440px\u00bb global_colors_info=\u00bb{}\u00bb][et_pb_column type=\u00bb1_3″ _builder_version=\u00bb4.16″ _module_preset=\u00bbdefault\u00bb background_color=\u00bb#ffffff\u00bb custom_padding=\u00bb|||\u00bb global_colors_info=\u00bb{}\u00bb custom_padding__hover=\u00bb|||\u00bb][et_pb_image src=\u00bbhttp:\/\/www.lafmat.com\/home\/wp-content\/uploads\/2022\/05\/1234.png\u00bb title_text=\u00bb1234″ _builder_version=\u00bb4.17.0″ _module_preset=\u00bbdefault\u00bb global_colors_info=\u00bb{}\u00bb][\/et_pb_image][et_pb_text admin_label=\u00bbService Name\u00bb _builder_version=\u00bb4.17.0″ _module_preset=\u00bbdefault\u00bb text_font=\u00bbMontserrat||||||||\u00bb text_font_size=\u00bb15px\u00bb text_line_height=\u00bb1.8em\u00bb header_font=\u00bb||||||||\u00bb header_3_font=\u00bbMontserrat||||||||\u00bb header_3_line_height=\u00bb1.5em\u00bb custom_padding=\u00bb10px|20px||20px\u00bb global_colors_info=\u00bb{}\u00bb]<\/p>\n

May 14th 2022<\/h3>\n

Dr. Julius Andrew P. Nu\u00f1ez<\/h3>\n

S\u00edntesis de Na1-xLixMgH3 (x = 0-1) a alta presi\u00f3n y temperatura para el almacenamiento de hidr\u00f3geno<\/strong> (Video link)<\/a><\/span><\/p>\n

Universit\u00e9 Grenoble Alpes, CNRS, Institut N\u00e9el, 38000 Grenoble, France – <\/span>University of the Philippines Manila, Padre Faura St., Ermita, Manila 1000, Philippines<\/span><\/p>\n

[\/et_pb_text][\/et_pb_column][et_pb_column type=\u00bb1_3″ _builder_version=\u00bb4.16″ _module_preset=\u00bbdefault\u00bb background_color=\u00bb#ffffff\u00bb custom_padding=\u00bb|||\u00bb global_colors_info=\u00bb{}\u00bb custom_padding__hover=\u00bb|||\u00bb][et_pb_image src=\u00bbhttp:\/\/www.lafmat.com\/home\/wp-content\/uploads\/2022\/05\/WhatsApp-Image-2022-05-03-at-1.56.44-PM.jpeg\u00bb title_text=\u00bbWhatsApp Image 2022-05-03 at 1.56.44 PM\u00bb _builder_version=\u00bb4.17.0″ _module_preset=\u00bbdefault\u00bb global_colors_info=\u00bb{}\u00bb][\/et_pb_image][et_pb_text admin_label=\u00bbService Name\u00bb _builder_version=\u00bb4.17.0″ _module_preset=\u00bbdefault\u00bb text_font=\u00bbMontserrat||||||||\u00bb text_font_size=\u00bb15px\u00bb text_line_height=\u00bb1.8em\u00bb header_font=\u00bb||||||||\u00bb header_3_font=\u00bbMontserrat||||||||\u00bb header_3_line_height=\u00bb1.5em\u00bb custom_padding=\u00bb10px|20px||20px\u00bb locked=\u00bboff\u00bb global_colors_info=\u00bb{}\u00bb]<\/p>\n

May 1st 2022<\/h3>\n

Phd. Jos\u00e9 Ferm\u00edn<\/h3>\n

An\u00e1lisis microestructural de semiconductores ternarios AgIn5VI8 mediante DRX<\/strong> (Video link)<\/a><\/span><\/p>\n

Universidad de Zulia Venezuela.<\/span><\/p>\n

[\/et_pb_text][\/et_pb_column][et_pb_column type=\u00bb1_3″ _builder_version=\u00bb4.16″ _module_preset=\u00bbdefault\u00bb background_color=\u00bb#ffffff\u00bb custom_padding=\u00bb|||\u00bb global_colors_info=\u00bb{}\u00bb custom_padding__hover=\u00bb|||\u00bb][et_pb_image src=\u00bbhttp:\/\/www.lafmat.com\/home\/wp-content\/uploads\/2022\/05\/Dr.-Thanos-M..png\u00bb title_text=\u00bbDr. Thanos M.\u00bb _builder_version=\u00bb4.17.0″ _module_preset=\u00bbdefault\u00bb global_colors_info=\u00bb{}\u00bb][\/et_pb_image][et_pb_text admin_label=\u00bbService Name\u00bb _builder_version=\u00bb4.17.0″ _module_preset=\u00bbdefault\u00bb text_font=\u00bbMontserrat||||||||\u00bb text_font_size=\u00bb15px\u00bb text_line_height=\u00bb1.8em\u00bb header_font=\u00bb||||||||\u00bb header_3_font=\u00bbMontserrat||||||||\u00bb header_3_line_height=\u00bb1.5em\u00bb custom_padding=\u00bb10px|20px||20px\u00bb locked=\u00bboff\u00bb global_colors_info=\u00bb{}\u00bb]<\/p>\n

Apr 30th 2022<\/h3>\n

Prof. Thanos Mitrelias<\/h3>\n

Targeted Oxidative Stress assault to replace Chemotherapy – Reducing the burden of cancer on society <\/strong>(Video link)<\/a><\/p>\n

Cavendish Laboratory, University of Cambridge, UK.\u00a0 (Founding Director: HLectron and Cambridge of BioMagnetics Ltd)<\/p>\n

[\/et_pb_text][\/et_pb_column][\/et_pb_row][et_pb_row column_structure=\u00bb1_3,1_3,1_3″ use_custom_gutter=\u00bbon\u00bb gutter_width=\u00bb2″ _builder_version=\u00bb4.16″ _module_preset=\u00bbdefault\u00bb max_width=\u00bb1440px\u00bb min_height=\u00bb266.9px\u00bb custom_padding=\u00bb|||\u00bb use_custom_width=\u00bbon\u00bb custom_width_px=\u00bb1440px\u00bb global_colors_info=\u00bb{}\u00bb][et_pb_column type=\u00bb1_3″ _builder_version=\u00bb4.16″ _module_preset=\u00bbdefault\u00bb background_color=\u00bb#ffffff\u00bb custom_padding=\u00bb|||\u00bb global_colors_info=\u00bb{}\u00bb custom_padding__hover=\u00bb|||\u00bb][et_pb_image src=\u00bbhttp:\/\/www.lafmat.com\/home\/wp-content\/uploads\/2022\/04\/Ernesto.png\u00bb title_text=\u00bbErnesto\u00bb _builder_version=\u00bb4.17.0″ _module_preset=\u00bbdefault\u00bb global_colors_info=\u00bb{}\u00bb][\/et_pb_image][et_pb_text admin_label=\u00bbService Name\u00bb _builder_version=\u00bb4.17.0″ _module_preset=\u00bbdefault\u00bb text_font=\u00bbMontserrat||||||||\u00bb text_font_size=\u00bb15px\u00bb text_line_height=\u00bb1.8em\u00bb header_font=\u00bb||||||||\u00bb header_3_font=\u00bbMontserrat||||||||\u00bb header_3_line_height=\u00bb1.5em\u00bb custom_padding=\u00bb10px|20px||20px\u00bb global_colors_info=\u00bb{}\u00bb]<\/p>\n

Apr 23th 2022<\/h3>\n

Prof. Ernesto P. Raposo<\/h3>\n

Vidros de spin e o pr\u00eamio Nobel de 2021<\/strong> (Video link)<\/a><\/span><\/p>\n

Universidade Federal de Pernambuco (UFPE), Brasil.<\/span><\/p>\n

[\/et_pb_text][\/et_pb_column][et_pb_column type=\u00bb1_3″ _builder_version=\u00bb4.16″ _module_preset=\u00bbdefault\u00bb background_color=\u00bb#ffffff\u00bb custom_padding=\u00bb|||\u00bb global_colors_info=\u00bb{}\u00bb custom_padding__hover=\u00bb|||\u00bb][et_pb_image src=\u00bbhttp:\/\/www.lafmat.com\/home\/wp-content\/uploads\/2022\/04\/ivan.jpeg\u00bb title_text=\u00bbivan\u00bb _builder_version=\u00bb4.17.0″ _module_preset=\u00bbdefault\u00bb global_colors_info=\u00bb{}\u00bb][\/et_pb_image][et_pb_text admin_label=\u00bbService Name\u00bb _builder_version=\u00bb4.17.0″ _module_preset=\u00bbdefault\u00bb text_font=\u00bbMontserrat||||||||\u00bb text_font_size=\u00bb15px\u00bb text_line_height=\u00bb1.8em\u00bb header_font=\u00bb||||||||\u00bb header_3_font=\u00bbMontserrat||||||||\u00bb header_3_line_height=\u00bb1.5em\u00bb custom_padding=\u00bb10px|20px||20px\u00bb locked=\u00bboff\u00bb global_colors_info=\u00bb{}\u00bb]<\/p>\n

Apr 9th 2022<\/h3>\n

Prof. Ivan S. Oliveira<\/h3>\n

Invers\u00e3o s\u00edsmica com um recozidor qu\u00e2ntico da D-Wave (Video link)<\/a><\/span><\/p>\n

Centro Brasileiro de Pesquisas F\u00edsicas (CBPF), Brasil.<\/span><\/p>\n

[\/et_pb_text][\/et_pb_column][et_pb_column type=\u00bb1_3″ _builder_version=\u00bb4.16″ _module_preset=\u00bbdefault\u00bb background_color=\u00bb#ffffff\u00bb custom_padding=\u00bb|||\u00bb global_colors_info=\u00bb{}\u00bb custom_padding__hover=\u00bb|||\u00bb][et_pb_image src=\u00bbhttp:\/\/www.lafmat.com\/home\/wp-content\/uploads\/2022\/04\/william.jpeg\u00bb title_text=\u00bbwilliam\u00bb _builder_version=\u00bb4.17.0″ _module_preset=\u00bbdefault\u00bb global_colors_info=\u00bb{}\u00bb][\/et_pb_image][et_pb_text admin_label=\u00bbService Name\u00bb _builder_version=\u00bb4.17.0″ _module_preset=\u00bbdefault\u00bb text_font=\u00bbMontserrat||||||||\u00bb text_font_size=\u00bb15px\u00bb text_line_height=\u00bb1.8em\u00bb header_font=\u00bb||||||||\u00bb header_3_font=\u00bbMontserrat||||||||\u00bb header_3_line_height=\u00bb1.5em\u00bb custom_padding=\u00bb10px|20px||20px\u00bb global_colors_info=\u00bb{}\u00bb]<\/p>\n

Apr 1st 2022<\/h3>\n

Mg. William Salazar Gonz\u00e1lez<\/h3>\n

Characterization of SCFO ferrite by transmission electron microscopy<\/strong> (Video link)<\/a><\/p>\n

Universidad Nacional de Colombia.<\/p>\n

[\/et_pb_text][\/et_pb_column][\/et_pb_row][et_pb_row column_structure=\u00bb1_3,1_3,1_3″ use_custom_gutter=\u00bbon\u00bb gutter_width=\u00bb2″ _builder_version=\u00bb4.16″ _module_preset=\u00bbdefault\u00bb max_width=\u00bb1440px\u00bb custom_padding=\u00bb|||\u00bb use_custom_width=\u00bbon\u00bb custom_width_px=\u00bb1440px\u00bb global_colors_info=\u00bb{}\u00bb][et_pb_column type=\u00bb1_3″ _builder_version=\u00bb4.16″ _module_preset=\u00bbdefault\u00bb background_color=\u00bb#ffffff\u00bb custom_padding=\u00bb|||\u00bb global_colors_info=\u00bb{}\u00bb custom_padding__hover=\u00bb|||\u00bb][et_pb_image src=\u00bbhttp:\/\/www.lafmat.com\/home\/wp-content\/uploads\/2022\/04\/carlos-e.jpeg\u00bb title_text=\u00bbcarlos e\u00bb _builder_version=\u00bb4.17.0″ _module_preset=\u00bbdefault\u00bb global_colors_info=\u00bb{}\u00bb][\/et_pb_image][et_pb_text admin_label=\u00bbService Name\u00bb _builder_version=\u00bb4.17.0″ _module_preset=\u00bbdefault\u00bb text_font=\u00bbMontserrat||||||||\u00bb text_font_size=\u00bb15px\u00bb text_line_height=\u00bb1.8em\u00bb header_font=\u00bb||||||||\u00bb header_3_font=\u00bbMontserrat||||||||\u00bb header_3_line_height=\u00bb1.5em\u00bb custom_padding=\u00bb10px|20px||20px\u00bb locked=\u00bboff\u00bb global_colors_info=\u00bb{}\u00bb]<\/p>\n

Mar 26th 2022<\/h3>\n

Prof. Carlos E. Rodr\u00edguez Garc\u00eda<\/h3>\n

Materiales Luminiscentes y sus aplicaciones<\/strong> (Video link)<\/a><\/p>\n

FCFM-UADEC, M\u00e9xico.<\/p>\n

[\/et_pb_text][\/et_pb_column][et_pb_column type=\u00bb1_3″ _builder_version=\u00bb4.16″ _module_preset=\u00bbdefault\u00bb background_color=\u00bb#ffffff\u00bb custom_padding=\u00bb|||\u00bb global_colors_info=\u00bb{}\u00bb custom_padding__hover=\u00bb|||\u00bb][et_pb_image src=\u00bbhttp:\/\/www.lafmat.com\/home\/wp-content\/uploads\/2022\/04\/pratap.jpeg\u00bb title_text=\u00bbpratap\u00bb _builder_version=\u00bb4.17.0″ _module_preset=\u00bbdefault\u00bb global_colors_info=\u00bb{}\u00bb][\/et_pb_image][et_pb_text admin_label=\u00bbService Name\u00bb _builder_version=\u00bb4.17.0″ _module_preset=\u00bbdefault\u00bb text_font=\u00bbMontserrat||||||||\u00bb text_font_size=\u00bb15px\u00bb text_line_height=\u00bb1.8em\u00bb header_font=\u00bb||||||||\u00bb header_3_font=\u00bbMontserrat||||||||\u00bb header_3_line_height=\u00bb1.5em\u00bb custom_padding=\u00bb10px|20px||20px\u00bb locked=\u00bboff\u00bb global_colors_info=\u00bb{}\u00bb]<\/p>\n

Mar 19th 2022<\/h3>\n

Prof. Pratap Kallu<\/h3>\n

Nanocomposite 2D material matrix for battery anode materials<\/strong> (Video link)<\/a><\/p>\n

University of Hyderabad, India.<\/span><\/p>\n

[\/et_pb_text][\/et_pb_column][et_pb_column type=\u00bb1_3″ _builder_version=\u00bb4.16″ _module_preset=\u00bbdefault\u00bb background_color=\u00bb#ffffff\u00bb custom_padding=\u00bb|||\u00bb global_colors_info=\u00bb{}\u00bb custom_padding__hover=\u00bb|||\u00bb][et_pb_image src=\u00bbhttp:\/\/www.lafmat.com\/home\/wp-content\/uploads\/2022\/04\/henry.jpeg\u00bb title_text=\u00bbhenry\u00bb _builder_version=\u00bb4.17.0″ _module_preset=\u00bbdefault\u00bb global_colors_info=\u00bb{}\u00bb][\/et_pb_image][et_pb_text admin_label=\u00bbService Name\u00bb _builder_version=\u00bb4.17.0″ _module_preset=\u00bbdefault\u00bb text_font=\u00bbMontserrat||||||||\u00bb text_font_size=\u00bb15px\u00bb text_line_height=\u00bb1.8em\u00bb header_font=\u00bb||||||||\u00bb header_3_font=\u00bbMontserrat||||||||\u00bb header_3_line_height=\u00bb1.5em\u00bb custom_padding=\u00bb10px|20px||20px\u00bb global_colors_info=\u00bb{}\u00bb]<\/p>\n

Mar 12th 2022<\/h3>\n

Mg. Henry E. S\u00e1nchez Cornejo<\/h3>\n

Propiedades magn\u00e9ticas y din\u00e1mica de v\u00f3rtices en capas de YBa2Cu3O(7-d)<\/strong> (Video link)<\/a><\/p>\n

Universidad Nacional Mayor de San Marcos (UNMSM).<\/p>\n

[\/et_pb_text][\/et_pb_column][\/et_pb_row][et_pb_row column_structure=\u00bb1_3,1_3,1_3″ use_custom_gutter=\u00bbon\u00bb gutter_width=\u00bb2″ _builder_version=\u00bb4.16″ _module_preset=\u00bbdefault\u00bb max_width=\u00bb1440px\u00bb min_height=\u00bb235.9px\u00bb custom_padding=\u00bb|||\u00bb use_custom_width=\u00bbon\u00bb custom_width_px=\u00bb1440px\u00bb global_colors_info=\u00bb{}\u00bb][et_pb_column type=\u00bb1_3″ _builder_version=\u00bb4.16″ _module_preset=\u00bbdefault\u00bb background_color=\u00bb#ffffff\u00bb custom_padding=\u00bb|||\u00bb global_colors_info=\u00bb{}\u00bb custom_padding__hover=\u00bb|||\u00bb][et_pb_image src=\u00bbhttp:\/\/www.lafmat.com\/home\/wp-content\/uploads\/2022\/04\/rafael.jpeg\u00bb title_text=\u00bbrafael\u00bb _builder_version=\u00bb4.17.0″ _module_preset=\u00bbdefault\u00bb global_colors_info=\u00bb{}\u00bb][\/et_pb_image][et_pb_text admin_label=\u00bbService Name\u00bb _builder_version=\u00bb4.17.0″ _module_preset=\u00bbdefault\u00bb text_font=\u00bbMontserrat||||||||\u00bb text_font_size=\u00bb15px\u00bb text_line_height=\u00bb1.8em\u00bb header_font=\u00bb||||||||\u00bb header_3_font=\u00bbMontserrat||||||||\u00bb header_3_line_height=\u00bb1.5em\u00bb custom_padding=\u00bb10px|20px||20px\u00bb locked=\u00bboff\u00bb global_colors_info=\u00bb{}\u00bb]<\/p>\n

Mar 5th 2022<\/h3>\n

Prof. Rafael Gonz\u00e1lez<\/h3>\n

Electronic structure of topological semimetals<\/strong> (Video link)<\/a><\/p>\n

Universidad del Norte, Colombia.<\/p>\n

[\/et_pb_text][\/et_pb_column][et_pb_column type=\u00bb1_3″ _builder_version=\u00bb4.16″ _module_preset=\u00bbdefault\u00bb background_color=\u00bb#ffffff\u00bb custom_padding=\u00bb|||\u00bb global_colors_info=\u00bb{}\u00bb custom_padding__hover=\u00bb|||\u00bb][et_pb_image src=\u00bbhttp:\/\/www.lafmat.com\/home\/wp-content\/uploads\/2022\/04\/carlos.jpeg\u00bb title_text=\u00bbcarlos\u00bb _builder_version=\u00bb4.17.0″ _module_preset=\u00bbdefault\u00bb global_colors_info=\u00bb{}\u00bb][\/et_pb_image][et_pb_text admin_label=\u00bbService Name\u00bb _builder_version=\u00bb4.17.0″ _module_preset=\u00bbdefault\u00bb text_font=\u00bbMontserrat||||||||\u00bb text_font_size=\u00bb15px\u00bb text_line_height=\u00bb1.8em\u00bb header_font=\u00bb||||||||\u00bb header_3_font=\u00bbMontserrat||||||||\u00bb header_3_line_height=\u00bb1.5em\u00bb custom_padding=\u00bb10px|20px||20px\u00bb global_colors_info=\u00bb{}\u00bb]<\/p>\n

Feb 26th 2022<\/h3>\n

Prof. Carlos A. Cordoso<\/h3>\n

Effect of heat treatment on the microstructure of polycrystalline superconducting ceramic SmBa2Cu3O(7-d) (Video link)<\/a><\/p>\n

Universidade Federal do Esper\u00edtu Santo (UFES), Brasil.<\/p>\n

[\/et_pb_text][\/et_pb_column][et_pb_column type=\u00bb1_3″ _builder_version=\u00bb4.16″ _module_preset=\u00bbdefault\u00bb background_color=\u00bb#ffffff\u00bb custom_padding=\u00bb|||\u00bb global_colors_info=\u00bb{}\u00bb custom_padding__hover=\u00bb|||\u00bb][et_pb_image src=\u00bbhttp:\/\/www.lafmat.com\/home\/wp-content\/uploads\/2022\/04\/cinvestev.jpeg\u00bb title_text=\u00bbcinvestev\u00bb _builder_version=\u00bb4.17.0″ _module_preset=\u00bbdefault\u00bb global_colors_info=\u00bb{}\u00bb][\/et_pb_image][et_pb_text admin_label=\u00bbService Name\u00bb _builder_version=\u00bb4.17.0″ _module_preset=\u00bbdefault\u00bb text_font=\u00bbMontserrat||||||||\u00bb text_font_size=\u00bb15px\u00bb text_line_height=\u00bb1.8em\u00bb header_font=\u00bb||||||||\u00bb header_3_font=\u00bbMontserrat||||||||\u00bb header_3_line_height=\u00bb1.5em\u00bb custom_padding=\u00bb10px|20px||20px\u00bb locked=\u00bboff\u00bb global_colors_info=\u00bb{}\u00bb]<\/p>\n

Feb 19th 2022<\/h3>\n

Prof. Arturo I. Martinez Manriquez<\/h3>\n

Propiedades el\u00e9ctricas de materiales, un enfoque sustentable (Video link)<\/a><\/p>\n

CINVESTAV, M\u00e9xico<\/p>\n

[\/et_pb_text][\/et_pb_column][\/et_pb_row][et_pb_row column_structure=\u00bb1_3,1_3,1_3″ use_custom_gutter=\u00bbon\u00bb gutter_width=\u00bb2″ _builder_version=\u00bb4.16″ _module_preset=\u00bbdefault\u00bb max_width=\u00bb1440px\u00bb custom_padding=\u00bb|||\u00bb use_custom_width=\u00bbon\u00bb custom_width_px=\u00bb1440px\u00bb global_colors_info=\u00bb{}\u00bb][et_pb_column type=\u00bb1_3″ _builder_version=\u00bb4.16″ _module_preset=\u00bbdefault\u00bb background_color=\u00bb#ffffff\u00bb custom_padding=\u00bb|||\u00bb global_colors_info=\u00bb{}\u00bb custom_padding__hover=\u00bb|||\u00bb][et_pb_image src=\u00bbhttp:\/\/www.lafmat.com\/home\/wp-content\/uploads\/2022\/04\/victor.jpeg\u00bb title_text=\u00bbvictor\u00bb _builder_version=\u00bb4.17.0″ _module_preset=\u00bbdefault\u00bb global_colors_info=\u00bb{}\u00bb][\/et_pb_image][et_pb_text admin_label=\u00bbService Name\u00bb _builder_version=\u00bb4.17.0″ _module_preset=\u00bbdefault\u00bb text_font=\u00bbMontserrat||||||||\u00bb text_font_size=\u00bb15px\u00bb text_line_height=\u00bb1.8em\u00bb header_font=\u00bb||||||||\u00bb header_3_font=\u00bbMontserrat||||||||\u00bb header_3_line_height=\u00bb1.5em\u00bb custom_padding=\u00bb10px|20px||20px\u00bb locked=\u00bboff\u00bb global_colors_info=\u00bb{}\u00bb]<\/p>\n

Feb 12th 2022<\/h3>\n

Dr. Victor M. Serdio Villareal<\/h3>\n

Single-electron, biomolecule and photon devices with an informal\/fun approach<\/strong> (Video link)<\/a><\/p>\n

Nu Quantum Ltd. \/ University of Cambridge<\/p>\n

[\/et_pb_text][\/et_pb_column][et_pb_column type=\u00bb1_3″ _builder_version=\u00bb4.16″ _module_preset=\u00bbdefault\u00bb background_color=\u00bb#ffffff\u00bb custom_padding=\u00bb|||\u00bb global_colors_info=\u00bb{}\u00bb custom_padding__hover=\u00bb|||\u00bb][et_pb_image src=\u00bbhttp:\/\/www.lafmat.com\/home\/wp-content\/uploads\/2022\/04\/flavia.jpeg\u00bb title_text=\u00bbflavia\u00bb _builder_version=\u00bb4.17.0″ _module_preset=\u00bbdefault\u00bb global_colors_info=\u00bb{}\u00bb][\/et_pb_image][et_pb_text admin_label=\u00bbService Name\u00bb _builder_version=\u00bb4.17.0″ _module_preset=\u00bbdefault\u00bb text_font=\u00bbMontserrat||||||||\u00bb text_font_size=\u00bb15px\u00bb text_line_height=\u00bb1.8em\u00bb header_font=\u00bb||||||||\u00bb header_3_font=\u00bbMontserrat||||||||\u00bb header_3_line_height=\u00bb1.5em\u00bb custom_padding=\u00bb10px|20px||20px\u00bb locked=\u00bboff\u00bb global_colors_info=\u00bb{}\u00bb]<\/p>\n

Feb 5th 2022<\/h3>\n

Dra. Fl\u00e1via Portela Santos<\/h3>\n

Estudo das propiedades superconductoras na tricamada Nb\/Pb\/Nb <\/strong>(Video link)<\/a>
Universidad Federal Rural de Pernambuco, Brasil<\/p>\n

[\/et_pb_text][\/et_pb_column][et_pb_column type=\u00bb1_3″ _builder_version=\u00bb4.16″ _module_preset=\u00bbdefault\u00bb background_color=\u00bb#ffffff\u00bb custom_padding=\u00bb|||\u00bb global_colors_info=\u00bb{}\u00bb custom_padding__hover=\u00bb|||\u00bb][et_pb_image src=\u00bbhttp:\/\/www.lafmat.com\/home\/wp-content\/uploads\/2022\/04\/Alberto-p-guimaraes.jpeg\u00bb title_text=\u00bbAlberto p guimaraes\u00bb _builder_version=\u00bb4.17.0″ _module_preset=\u00bbdefault\u00bb global_colors_info=\u00bb{}\u00bb][\/et_pb_image][et_pb_text admin_label=\u00bbService Name\u00bb _builder_version=\u00bb4.17.0″ _module_preset=\u00bbdefault\u00bb text_font=\u00bbMontserrat||||||||\u00bb text_font_size=\u00bb15px\u00bb text_line_height=\u00bb1.8em\u00bb header_font=\u00bb||||||||\u00bb header_3_font=\u00bbMontserrat||||||||\u00bb header_3_line_height=\u00bb1.5em\u00bb custom_padding=\u00bb10px|20px||20px\u00bb locked=\u00bboff\u00bb global_colors_info=\u00bb{}\u00bb]<\/p>\n

Jan 29th 2022<\/h3>\n

Prof. Alberto P. Guimaraes<\/h3>\n

Skyrmions magn\u00e9ticos <\/strong>(Video link)<\/a>
CBPF, Rio de Janeiro, Brazil<\/p>\n

[\/et_pb_text][\/et_pb_column][\/et_pb_row][et_pb_row column_structure=\u00bb1_3,1_3,1_3″ use_custom_gutter=\u00bbon\u00bb gutter_width=\u00bb2″ _builder_version=\u00bb4.16″ _module_preset=\u00bbdefault\u00bb max_width=\u00bb1440px\u00bb custom_padding=\u00bb|||\u00bb use_custom_width=\u00bbon\u00bb custom_width_px=\u00bb1440px\u00bb global_colors_info=\u00bb{}\u00bb][et_pb_column type=\u00bb1_3″ _builder_version=\u00bb4.16″ _module_preset=\u00bbdefault\u00bb background_color=\u00bb#ffffff\u00bb custom_padding=\u00bb|||\u00bb global_colors_info=\u00bb{}\u00bb custom_padding__hover=\u00bb|||\u00bb][et_pb_image src=\u00bbhttp:\/\/www.lafmat.com\/home\/wp-content\/uploads\/2022\/04\/perdo-silva-mujica.jpeg\u00bb title_text=\u00bbperdo silva mujica\u00bb _builder_version=\u00bb4.17.0″ _module_preset=\u00bbdefault\u00bb global_colors_info=\u00bb{}\u00bb][\/et_pb_image][et_pb_text admin_label=\u00bbService Name\u00bb _builder_version=\u00bb4.17.0″ _module_preset=\u00bbdefault\u00bb text_font=\u00bbMontserrat||||||||\u00bb text_font_size=\u00bb15px\u00bb text_line_height=\u00bb1.8em\u00bb header_font=\u00bb||||||||\u00bb header_3_font=\u00bbMontserrat||||||||\u00bb header_3_line_height=\u00bb1.5em\u00bb custom_padding=\u00bb10px|20px||20px\u00bb global_colors_info=\u00bb{}\u00bb]<\/p>\n

Jan 22th 2022<\/h3>\n

Dr. Pedro Silva Mujica<\/h3>\n

Resonancia ferromagn\u00e9tica de nanopart\u00edculas de MnxCo1\u2212xFe2O4 <\/strong>(Video link)<\/a><\/p>\n

F\u00edsica – IVIC (Instituto Venezolano de Investigaciones Cient\u00edficas)<\/p>\n

[\/et_pb_text][\/et_pb_column][et_pb_column type=\u00bb1_3″ _builder_version=\u00bb4.16″ _module_preset=\u00bbdefault\u00bb background_color=\u00bb#ffffff\u00bb custom_padding=\u00bb|||\u00bb global_colors_info=\u00bb{}\u00bb custom_padding__hover=\u00bb|||\u00bb][et_pb_image src=\u00bbhttp:\/\/www.lafmat.com\/home\/wp-content\/uploads\/2022\/04\/valdenne.jpeg\u00bb title_text=\u00bbvaldenne\u00bb _builder_version=\u00bb4.17.0″ _module_preset=\u00bbdefault\u00bb global_colors_info=\u00bb{}\u00bb][\/et_pb_image][et_pb_text admin_label=\u00bbService Name\u00bb _builder_version=\u00bb4.17.0″ _module_preset=\u00bbdefault\u00bb text_font=\u00bbMontserrat||||||||\u00bb text_font_size=\u00bb15px\u00bb text_line_height=\u00bb1.8em\u00bb header_font=\u00bb||||||||\u00bb header_3_font=\u00bbMontserrat||||||||\u00bb header_3_line_height=\u00bb1.5em\u00bb custom_padding=\u00bb10px|20px||20px\u00bb locked=\u00bboff\u00bb global_colors_info=\u00bb{}\u00bb]<\/p>\n

Jan 15th 2022<\/h3>\n

Dra. Valdeene Albuquerque Brito da Silva<\/h3>\n

Nanopart\u00edculas magn\u00e9ticas na terapia do c\u00e2ncer<\/strong>\u00a0(Video link)<\/a>
Professora do grupo Ser Educacional Uninassau, Brazil.<\/p>\n

[\/et_pb_text][\/et_pb_column][et_pb_column type=\u00bb1_3″ _builder_version=\u00bb4.16″ _module_preset=\u00bbdefault\u00bb background_color=\u00bb#ffffff\u00bb custom_padding=\u00bb|||\u00bb global_colors_info=\u00bb{}\u00bb custom_padding__hover=\u00bb|||\u00bb][\/et_pb_column][\/et_pb_row][\/et_pb_section][et_pb_section fb_built=\u00bb1″ admin_label=\u00bbPopup – #absFelipe\u00bb module_id=\u00bbabsFelipe\u00bb module_class=\u00bbpopup\u00bb _builder_version=\u00bb4.17.0″ _module_preset=\u00bbdefault\u00bb width=\u00bb70%\u00bb module_alignment=\u00bbcenter\u00bb da_is_popup=\u00bbon\u00bb da_popup_slug=\u00bbabsFelipe\u00bb da_disable_devices=\u00bboff|off|off\u00bb global_colors_info=\u00bb{}\u00bb da_exit_intent=\u00bboff\u00bb da_has_close=\u00bbon\u00bb da_alt_close=\u00bboff\u00bb da_dark_close=\u00bboff\u00bb da_not_modal=\u00bbon\u00bb da_is_singular=\u00bboff\u00bb da_with_loader=\u00bboff\u00bb da_has_shadow=\u00bbon\u00bb][et_pb_row _builder_version=\u00bb4.17.0″ _module_preset=\u00bbdefault\u00bb global_colors_info=\u00bb{}\u00bb][et_pb_column type=\u00bb4_4″ _builder_version=\u00bb4.17.0″ _module_preset=\u00bbdefault\u00bb global_colors_info=\u00bb{}\u00bb][et_pb_text _builder_version=\u00bb4.17.0″ _module_preset=\u00bbdefault\u00bb global_colors_info=\u00bb{}\u00bb]<\/p>\n

Prof. Felipe Modaca<\/strong><\/p>\n

Universidad San Sebasti\u00e1n,<\/p>\n

Puerto Montt, Chile.<\/p>\n

\n

Assistant professor at San Sebasti\u00e1n University’s Faculty of Engineering in Puerto Montt, Chile. Bachelor’s and master\u2019s at Physic from Catolica del Norte University in Chile and Doctorate at Nanoscience and Nanotechnology from Centro de Investigaci\u00f3n y estudios Avanzados del IPN (CINVESTAV), Mexico. He has experience in the field of condensed matter physics, with an emphasis on ferromagnetic, transparent conducting, and catalytic materials for solar energy and water purification applications.<\/p>\n

[\/et_pb_text][\/et_pb_column][\/et_pb_row][\/et_pb_section][et_pb_section fb_built=\u00bb1″ admin_label=\u00bbPopup – #absPureur\u00bb module_id=\u00bbabsPureur\u00bb module_class=\u00bbpopup\u00bb _builder_version=\u00bb4.17.0″ _module_preset=\u00bbdefault\u00bb width=\u00bb70%\u00bb module_alignment=\u00bbcenter\u00bb da_is_popup=\u00bbon\u00bb da_popup_slug=\u00bbabsPureur\u00bb da_disable_devices=\u00bboff|off|off\u00bb global_colors_info=\u00bb{}\u00bb da_exit_intent=\u00bboff\u00bb da_has_close=\u00bbon\u00bb da_alt_close=\u00bboff\u00bb da_dark_close=\u00bboff\u00bb da_not_modal=\u00bbon\u00bb da_is_singular=\u00bboff\u00bb da_with_loader=\u00bboff\u00bb da_has_shadow=\u00bbon\u00bb][et_pb_row _builder_version=\u00bb4.17.0″ _module_preset=\u00bbdefault\u00bb global_colors_info=\u00bb{}\u00bb][et_pb_column type=\u00bb4_4″ _builder_version=\u00bb4.17.0″ _module_preset=\u00bbdefault\u00bb global_colors_info=\u00bb{}\u00bb][et_pb_text _builder_version=\u00bb4.17.0″ _module_preset=\u00bbdefault\u00bb global_colors_info=\u00bb{}\u00bb]<\/p>\n

Hall Effect and Pseudogap in the High Temperature Superconductors Bi2Sr2CaCu2O8+x and YBa2Cu3O7-d<\/strong><\/h4>\n

Paulo Pureur
Instituto de F\u00edsica \u2013 Universidade Federal do Rio Grande do Sul (UFRGS)<\/p>\n

Measurements of low-field planar Hall resistivity in the normal phase of the cuprate superconductors Bi2Ba2CaCu2O8 (Bi-2212) and YBa2Cu3O7 (YBCO) are reported. Single crystal bulks and epitaxial thin films were prepared with different carrier densities, so that samples covering a large extension of the superconducting dome could be investigated in both systems. The Hall resistivity data is described by considering that an anomalous term occurs in addition to an ordinary contribution. The pseudogap energy scale is consistently extracted as a function of the carrier concentration from the temperature dependent anomalous Hall resistivity for the two studied systems. In both cases, it is found that the pseudogap boundary crosses the superconducting dome near the optimum doping range, favoring the interpretation considering that the excitations responsible for this phenomenon are different from those giving origin to the superconducting ground state. Results also suggest that the pseudogap regime is not a true thermodynamic phase.<\/p>\n

[\/et_pb_text][\/et_pb_column][\/et_pb_row][\/et_pb_section][et_pb_section fb_built=\u00bb1″ admin_label=\u00bbPopup – #absEduardo\u00bb module_id=\u00bbabsEduardo\u00bb module_class=\u00bbpopup\u00bb _builder_version=\u00bb4.17.0″ _module_preset=\u00bbdefault\u00bb width=\u00bb70%\u00bb module_alignment=\u00bbcenter\u00bb da_is_popup=\u00bbon\u00bb da_popup_slug=\u00bbabsEduardo\u00bb da_disable_devices=\u00bboff|off|off\u00bb global_colors_info=\u00bb{}\u00bb da_exit_intent=\u00bboff\u00bb da_has_close=\u00bbon\u00bb da_alt_close=\u00bboff\u00bb da_dark_close=\u00bboff\u00bb da_not_modal=\u00bbon\u00bb da_is_singular=\u00bboff\u00bb da_with_loader=\u00bboff\u00bb da_has_shadow=\u00bbon\u00bb][et_pb_row _builder_version=\u00bb4.17.0″ _module_preset=\u00bbdefault\u00bb global_colors_info=\u00bb{}\u00bb][et_pb_column type=\u00bb4_4″ _builder_version=\u00bb4.17.0″ _module_preset=\u00bbdefault\u00bb global_colors_info=\u00bb{}\u00bb][et_pb_text _builder_version=\u00bb4.17.0″ _module_preset=\u00bbdefault\u00bb global_colors_info=\u00bb{}\u00bb]<\/p>\n

Light Matter Interaction in Plasmonic Supercrystals <\/strong><\/h4>\n

Prof. Eduardo Bed\u00ea Barros<\/p>\n

Universidade Federal do Cear\u00e1, Departamento de F\u00edsica Fortaleza-Brasil In this work we discuss the Light-Matter interaction the the context of supercrystals formed by metallic nanoparticles. The plasmonic excitations of the individual particles in the periodic structure interact among themselves and with the electromagnetic field to form hybrid light-matter excitations known as plasmon-polaritons. The dispersion relations of the plasmon polaritons depend both on sizes of the composing nanoparticles and on the specific crystalline structure of the supercrystals. For particles large in comparison to the lattice parameter the light-matter interaction can be amplified to enter the ultra-strong and the deep-strong light-matter coupling regimes.[1] In the deep-strong coupling regime, the energy associated to the light-mattter interaction exceeds the energies of the bare plasmons and photons leading to interesting physical phenomena. We also present a theoretical framework which can be used to describe the light-matter interaction in these systems and help guide the development of new structures for possible plasmonic and photonic applications.<\/p>\n

[1] Mueller et al, Nature 583, 780-784 (2020).<\/p>\n

[\/et_pb_text][\/et_pb_column][\/et_pb_row][\/et_pb_section][et_pb_section fb_built=\u00bb1″ admin_label=\u00bbPopup – #absMichael\u00bb module_id=\u00bbabsMichael\u00bb module_class=\u00bbpopup\u00bb _builder_version=\u00bb4.17.0″ _module_preset=\u00bbdefault\u00bb width=\u00bb70%\u00bb module_alignment=\u00bbcenter\u00bb da_is_popup=\u00bbon\u00bb da_popup_slug=\u00bbabsMichael\u00bb da_disable_devices=\u00bboff|off|off\u00bb global_colors_info=\u00bb{}\u00bb da_exit_intent=\u00bboff\u00bb da_has_close=\u00bbon\u00bb da_alt_close=\u00bboff\u00bb da_dark_close=\u00bboff\u00bb da_not_modal=\u00bbon\u00bb da_is_singular=\u00bboff\u00bb da_with_loader=\u00bboff\u00bb da_has_shadow=\u00bbon\u00bb][et_pb_row _builder_version=\u00bb4.17.0″ _module_preset=\u00bbdefault\u00bb global_colors_info=\u00bb{}\u00bb][et_pb_column type=\u00bb4_4″ _builder_version=\u00bb4.17.0″ _module_preset=\u00bbdefault\u00bb global_colors_info=\u00bb{}\u00bb][et_pb_text _builder_version=\u00bb4.17.0″ _module_preset=\u00bbdefault\u00bb global_colors_info=\u00bb{}\u00bb]<\/p>\n

Conduction electron spin resonance in the nearly ferromagnetic Fermi liquid YFe2Zn20<\/strong><\/h4>\n

Prof. Dr. Michael Cabrera Baez
Departamento de F\u00edsica, Universidade Federal de Pernambuco, Brazil<\/p>\n

The relaxation time is a fundamental parameter in the understanding of magnetic systems and, together with the spin dephasing, they are processes of great importance in applied physics. The fact that nonequilibrium electron spin in metals has a relatively long lifetime, allowing encoded information using the spin to travel considerable distances, is, for example, what makes spintronics a new source of technology. In this talk I will present the magnetic, thermodynamic, and electronic properties of the nearly ferromagnetic Fermi liquid (NFFL) system YFe2Zn20 by means of dc-magnetic susceptibility, specific heat, and electron spin resonance (ESR) measurements. As Gd is incorporated (Y1-xGdxFe2Zn20; x = 0.005, 0.01 and 0.05) the magnetization measurements present ferromagnetic correlations. Strong evidence of conduction electron spin resonance (CESR) is found due to the presence of Gd3+ ions. The usual local magnetic moment resonance associated with the Gd3+ 4f localized electrons was only present for x = 0.05 coexisting with the CESR. Although YFe2Zn20 is a NFFL, no CESR was detected for the undoped sample. These results will be discussed in terms of a highly polarized electrons, enhanced Pauli paramagnetism, Dyakonov-Perel-like relaxation mechanism and the spin-pumping process in spintronics.<\/p>\n

[\/et_pb_text][\/et_pb_column][\/et_pb_row][\/et_pb_section][et_pb_section fb_built=\u00bb1″ admin_label=\u00bbPopup – #absAlexei\u00bb module_id=\u00bbabsAlexei\u00bb module_class=\u00bbpopup\u00bb _builder_version=\u00bb4.17.0″ _module_preset=\u00bbdefault\u00bb width=\u00bb70%\u00bb module_alignment=\u00bbcenter\u00bb da_is_popup=\u00bbon\u00bb da_popup_slug=\u00bbabsAlexei\u00bb da_disable_devices=\u00bboff|off|off\u00bb global_colors_info=\u00bb{}\u00bb da_exit_intent=\u00bboff\u00bb da_has_close=\u00bbon\u00bb da_alt_close=\u00bboff\u00bb da_dark_close=\u00bboff\u00bb da_not_modal=\u00bbon\u00bb da_is_singular=\u00bboff\u00bb da_with_loader=\u00bboff\u00bb da_has_shadow=\u00bbon\u00bb][et_pb_row _builder_version=\u00bb4.17.0″ _module_preset=\u00bbdefault\u00bb global_colors_info=\u00bb{}\u00bb][et_pb_column type=\u00bb4_4″ _builder_version=\u00bb4.17.0″ _module_preset=\u00bbdefault\u00bb global_colors_info=\u00bb{}\u00bb][et_pb_text _builder_version=\u00bb4.17.0″ _module_preset=\u00bbdefault\u00bb global_colors_info=\u00bb{}\u00bb]<\/p>\n

Exotic magnetic flux patterns in superconductors between type I and II<\/strong><\/h4>\n

Prof Alexei Vagov
HSE Research University, Moscow, Russian<\/p>\n

The Ginzburg-Landau theory distinguishes two superconductivity types: ideally diamagnetic type-I materials and type-II superconductors that allows magnetic flux forming the mixed state with Abrikosov vortices. However, this dual classification does not exhaust all possibilities even for the standard BCS theory, which reveals a special regime of inter-type (IT) superconductivity. It has very distinct characteristics and should be regarded as a separate superconductivity type. Its intermediate mixed state (IMS) carries a manifold of exotic vortex patterns ranging from clusters of vortex lattices, to vortex stripes, labyrinths, and liquid droplets.<\/p>\n

It is shown that the IT superconductivity regime is a generic phenomenon generated by proximity to the super-critical Bogomolnyi point, at which the superconductive state is self-dual and infinitely degenerate. The IMS phase diagram is determined by the degeneracy-breaking mechanism, and is not sensitive to the microscopic details of the system. The generic nature of the phenomenon explains qualitatively similar vortex patterns appearing in a wide class of superconductors including single- and many-band compounds, magnetic materials, thin films and hybrid devices. These link superconductivity with the world of spontaneously emerging complexity.<\/p>\n

[\/et_pb_text][\/et_pb_column][\/et_pb_row][et_pb_row _builder_version=\u00bb4.17.0″ _module_preset=\u00bbdefault\u00bb global_colors_info=\u00bb{}\u00bb][et_pb_column type=\u00bb4_4″ _builder_version=\u00bb4.17.0″ _module_preset=\u00bbdefault\u00bb global_colors_info=\u00bb{}\u00bb][et_pb_image src=\u00bbhttp:\/\/www.lafmat.com\/home\/wp-content\/uploads\/2022\/12\/Alexei.png\u00bb title_text=\u00bbAlexei\u00bb _builder_version=\u00bb4.17.0″ _module_preset=\u00bbdefault\u00bb global_colors_info=\u00bb{}\u00bb][\/et_pb_image][\/et_pb_column][\/et_pb_row][et_pb_row _builder_version=\u00bb4.17.0″ _module_preset=\u00bbdefault\u00bb global_colors_info=\u00bb{}\u00bb][et_pb_column type=\u00bb4_4″ _builder_version=\u00bb4.17.0″ _module_preset=\u00bbdefault\u00bb global_colors_info=\u00bb{}\u00bb][et_pb_text _builder_version=\u00bb4.17.0″ _module_preset=\u00bbdefault\u00bb global_colors_info=\u00bb{}\u00bb]<\/p>\n

Figure: a) Phase diagram of IMS\u2019s with examples of flux configurations [1], b) magnetization profile in EuFe2(As0.79P0.21)2 [2], c) flux profile in a thin superconducting film [3], d) the currentdriven time evolution forming IMS vortex stripes in Nb [4].<\/p>\n

[1] A. Vagov et al., Comm. Physics. 3, 58 (2020);
http:\/\/www.nature.com\/articles\/s42005-020-0322-6<\/a>
[2] V. Stolyarov et al., Sci. Adv. 4, eaat1061 (2018);
http:\/\/advances.sciencemag.org\/lookup\/doi\/10.1126\/sciadv.aat1061<\/a>
[3] W. C\u00f3rdoba-Camacho et al., Phys. Rev. B 94, 054511 (2016);
https:\/\/link.aps.org\/doi\/10.1103\/PhysRevB.94.054511<\/a>
[4] X. Brems et al., Supercond. Sci. Technol. 35, 035003 (2022);
https:\/\/iopscience.iop.org\/article\/10.1088\/1361-6668\/ac455e<\/a><\/p>\n

[\/et_pb_text][\/et_pb_column][\/et_pb_row][\/et_pb_section][et_pb_section fb_built=\u00bb1″ admin_label=\u00bbPopup – #absNavarro\u00bb module_id=\u00bbabsNavarro\u00bb module_class=\u00bbpopup\u00bb _builder_version=\u00bb4.17.0″ _module_preset=\u00bbdefault\u00bb width=\u00bb70%\u00bb module_alignment=\u00bbcenter\u00bb da_is_popup=\u00bbon\u00bb da_popup_slug=\u00bbabsNavarro\u00bb da_disable_devices=\u00bboff|off|off\u00bb global_colors_info=\u00bb{}\u00bb da_exit_intent=\u00bboff\u00bb da_has_close=\u00bbon\u00bb da_alt_close=\u00bboff\u00bb da_dark_close=\u00bboff\u00bb da_not_modal=\u00bbon\u00bb da_is_singular=\u00bboff\u00bb da_with_loader=\u00bboff\u00bb da_has_shadow=\u00bbon\u00bb][et_pb_row _builder_version=\u00bb4.17.0″ _module_preset=\u00bbdefault\u00bb global_colors_info=\u00bb{}\u00bb][et_pb_column type=\u00bb4_4″ _builder_version=\u00bb4.17.0″ _module_preset=\u00bbdefault\u00bb global_colors_info=\u00bb{}\u00bb][et_pb_text _builder_version=\u00bb4.17.0″ _module_preset=\u00bbdefault\u00bb global_colors_info=\u00bb{}\u00bb]<\/p>\n

How material science can help natural product chemists<\/span><\/strong><\/h4>\n

Prof. Armando Navarro<\/p>\n

Departamento de Qu\u00edmica Fundamental, Universidade Federal de Pernambuco, Recife, PE, Brasil<\/p>\n

Polymer gels, as well as lyotropic liquid crystals based on 2D materials, such as graphene derivatives, or assembled small molecules can perform as weakly aligning media to obtain residual anisotropic nuclear magnetic resonance parameters such as residual dipolar couplings, residual chemical shift anisotropies or residual quadrupolar splittings. In this talk we will present main contributions of our groups to the development of new weakly aligning media, from a material science perspective, and how they can be applied to the structural elucidation of complex molecules such as natural products of unknown structure.<\/span><\/p>\n

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ROPIEDADES EL\u00c9CTRICAS Y MODELOS DE PERCOLACI\u00d3N <\/strong>APLICADOS A MEZCLAS: AISLANTE-CONDUCTOR<\/strong><\/h4>\n

Dr. Jos\u00e9 Luis Ochoa M.<\/p>\n

Las Propiedades El\u00e9ctricas<\/strong> de un material quedan definidas y establecidas de acuerdo al comportamiento que ese material asuma en presencia de un campo el\u00e9ctrico (E). En general, las propiedades el\u00e9ctricas de un material se resumen a trav\u00e9s de los par\u00e1metros: conductividad el\u00e9ctrica (\u03c3) o la resistividad el\u00e9ctrica (\u03c1 =1\/\u03c3). Estos par\u00e1metros nos dan la informaci\u00f3n precisa acerca de la naturaleza el\u00e9ctrica<\/em><\/strong> del material en cuesti\u00f3n.<\/p>\n

De lo anterior se desprende que los materiales se clasifican de acuerdo a su naturaleza el\u00e9ctrica<\/strong><\/em> en dos grupos:<\/p>\n