BEGIN:VCALENDAR PRODID:-//SiteBuilder 2//91¸£Àû ITS Web Team//EN VERSION:2.0 CALSCALE:GREGORIAN METHOD:PUBLISH X-WR-TIMEZONE:Europe/London X-LIC-LOCATION:Europe/London BEGIN:VTIMEZONE TZID:Europe/London LAST-MODIFIED:20201010T011803Z TZURL:http://tzurl.org/zoneinfo/Europe/London X-LIC-LOCATION:Europe/London X-PROLEPTIC-TZNAME:LMT BEGIN:STANDARD TZNAME:GMT TZOFFSETFROM:+000115 TZOFFSETTO:+0000 DTSTART:18471201T000000 END:STANDARD BEGIN:DAYLIGHT TZNAME:BST TZOFFSETFROM:+0000 TZOFFSETTO:+0100 DTSTART:19160521T020000 RDATE:19170408T020000 RDATE:19180324T020000 RDATE:19190330T020000 RDATE:19200328T020000 RDATE:19210403T020000 RDATE:19220326T020000 RDATE:19230422T020000 RDATE:19240413T020000 RDATE:19270410T020000 RDATE:19300413T020000 RDATE:19330409T020000 RDATE:19340422T020000 RDATE:19350414T020000 RDATE:19380410T020000 RDATE:19390416T020000 RDATE:19400225T020000 RDATE:19460414T020000 RDATE:19470316T020000 RDATE:19480314T020000 RDATE:19490403T020000 RDATE:19530419T020000 RDATE:19540411T020000 RDATE:19570414T020000 RDATE:19600410T020000 RDATE:19680218T020000 END:DAYLIGHT BEGIN:STANDARD TZNAME:GMT TZOFFSETFROM:+0100 TZOFFSETTO:+0000 DTSTART:19161001T030000 RDATE:19170917T030000 RDATE:19180930T030000 RDATE:19190929T030000 RDATE:19201025T030000 RDATE:19211003T030000 RDATE:19221008T030000 RDATE:19391119T030000 RDATE:19471102T030000 RDATE:19481031T030000 RDATE:19491030T030000 RDATE:19711031T030000 END:STANDARD BEGIN:STANDARD TZNAME:GMT TZOFFSETFROM:+0100 TZOFFSETTO:+0000 DTSTART:19230916T030000 RRULE:FREQ=YEARLY;UNTIL=19240921T020000Z;BYMONTH=9;BYMONTHDAY=16,17,18,19 ,20,21,22;BYDAY=SU END:STANDARD BEGIN:DAYLIGHT TZNAME:BST TZOFFSETFROM:+0000 TZOFFSETTO:+0100 DTSTART:19250419T020000 RRULE:FREQ=YEARLY;UNTIL=19260418T020000Z;BYMONTH=4;BYMONTHDAY=16,17,18,19 ,20,21,22;BYDAY=SU END:DAYLIGHT BEGIN:STANDARD TZNAME:GMT TZOFFSETFROM:+0100 TZOFFSETTO:+0000 DTSTART:19251004T030000 RRULE:FREQ=YEARLY;UNTIL=19381002T020000Z;BYMONTH=10;BYMONTHDAY=2,3,4,5,6, 7,8;BYDAY=SU END:STANDARD BEGIN:DAYLIGHT TZNAME:BST TZOFFSETFROM:+0000 TZOFFSETTO:+0100 DTSTART:19280422T020000 RRULE:FREQ=YEARLY;UNTIL=19290421T020000Z;BYMONTH=4;BYMONTHDAY=16,17,18,19 ,20,21,22;BYDAY=SU END:DAYLIGHT BEGIN:DAYLIGHT TZNAME:BST TZOFFSETFROM:+0000 TZOFFSETTO:+0100 DTSTART:19310419T020000 RRULE:FREQ=YEARLY;UNTIL=19320417T020000Z;BYMONTH=4;BYMONTHDAY=16,17,18,19 ,20,21,22;BYDAY=SU END:DAYLIGHT BEGIN:DAYLIGHT TZNAME:BST TZOFFSETFROM:+0000 TZOFFSETTO:+0100 DTSTART:19360419T020000 RRULE:FREQ=YEARLY;UNTIL=19370418T020000Z;BYMONTH=4;BYMONTHDAY=16,17,18,19 ,20,21,22;BYDAY=SU END:DAYLIGHT BEGIN:DAYLIGHT TZNAME:BDST TZOFFSETFROM:+0100 TZOFFSETTO:+0200 DTSTART:19410504T020000 RDATE:19450402T020000 RDATE:19470413T020000 END:DAYLIGHT BEGIN:DAYLIGHT TZNAME:BST TZOFFSETFROM:+0200 TZOFFSETTO:+0100 DTSTART:19410810T030000 RRULE:FREQ=YEARLY;UNTIL=19430815T010000Z;BYMONTH=8;BYMONTHDAY=9,10,11,12, 13,14,15;BYDAY=SU END:DAYLIGHT BEGIN:DAYLIGHT TZNAME:BDST TZOFFSETFROM:+0100 TZOFFSETTO:+0200 DTSTART:19420405T020000 RRULE:FREQ=YEARLY;UNTIL=19440402T010000Z;BYMONTH=4;BYMONTHDAY=2,3,4,5,6,7 ,8;BYDAY=SU END:DAYLIGHT BEGIN:DAYLIGHT TZNAME:BST TZOFFSETFROM:+0200 TZOFFSETTO:+0100 DTSTART:19440917T030000 RDATE:19450715T030000 RDATE:19470810T030000 END:DAYLIGHT BEGIN:STANDARD TZNAME:GMT TZOFFSETFROM:+0100 TZOFFSETTO:+0000 DTSTART:19451007T030000 RRULE:FREQ=YEARLY;UNTIL=19461006T020000Z;BYMONTH=10;BYMONTHDAY=2,3,4,5,6, 7,8;BYDAY=SU END:STANDARD BEGIN:DAYLIGHT TZNAME:BST TZOFFSETFROM:+0000 TZOFFSETTO:+0100 DTSTART:19500416T020000 RRULE:FREQ=YEARLY;UNTIL=19520420T020000Z;BYMONTH=4;BYMONTHDAY=14,15,16,17 ,18,19,20;BYDAY=SU END:DAYLIGHT BEGIN:STANDARD TZNAME:GMT TZOFFSETFROM:+0100 TZOFFSETTO:+0000 DTSTART:19501022T030000 RRULE:FREQ=YEARLY;UNTIL=19521026T020000Z;BYMONTH=10;BYMONTHDAY=21,22,23,2 4,25,26,27;BYDAY=SU END:STANDARD BEGIN:STANDARD TZNAME:GMT TZOFFSETFROM:+0100 TZOFFSETTO:+0000 DTSTART:19531004T030000 RRULE:FREQ=YEARLY;UNTIL=19601002T020000Z;BYMONTH=10;BYMONTHDAY=2,3,4,5,6, 7,8;BYDAY=SU END:STANDARD BEGIN:DAYLIGHT TZNAME:BST TZOFFSETFROM:+0000 TZOFFSETTO:+0100 DTSTART:19550417T020000 RRULE:FREQ=YEARLY;UNTIL=19560422T020000Z;BYMONTH=4;BYMONTHDAY=16,17,18,19 ,20,21,22;BYDAY=SU END:DAYLIGHT BEGIN:DAYLIGHT TZNAME:BST TZOFFSETFROM:+0000 TZOFFSETTO:+0100 DTSTART:19580420T020000 RRULE:FREQ=YEARLY;UNTIL=19590419T020000Z;BYMONTH=4;BYMONTHDAY=16,17,18,19 ,20,21,22;BYDAY=SU END:DAYLIGHT BEGIN:DAYLIGHT TZNAME:BST TZOFFSETFROM:+0000 TZOFFSETTO:+0100 DTSTART:19610326T020000 RRULE:FREQ=YEARLY;UNTIL=19630331T020000Z;BYMONTH=3;BYDAY=-1SU END:DAYLIGHT BEGIN:STANDARD TZNAME:GMT TZOFFSETFROM:+0100 TZOFFSETTO:+0000 DTSTART:19611029T030000 RRULE:FREQ=YEARLY;UNTIL=19671029T020000Z;BYMONTH=10;BYMONTHDAY=23,24,25,2 6,27,28,29;BYDAY=SU END:STANDARD BEGIN:DAYLIGHT TZNAME:BST TZOFFSETFROM:+0000 TZOFFSETTO:+0100 DTSTART:19640322T020000 RRULE:FREQ=YEARLY;UNTIL=19670319T020000Z;BYMONTH=3;BYMONTHDAY=19,20,21,22 ,23,24,25;BYDAY=SU END:DAYLIGHT BEGIN:STANDARD TZNAME:BST TZOFFSETFROM:+0100 TZOFFSETTO:+0100 DTSTART:19681026T230000 END:STANDARD BEGIN:DAYLIGHT TZNAME:BST TZOFFSETFROM:+0000 TZOFFSETTO:+0100 DTSTART:19720319T020000 RRULE:FREQ=YEARLY;UNTIL=19800316T020000Z;BYMONTH=3;BYMONTHDAY=16,17,18,19 ,20,21,22;BYDAY=SU END:DAYLIGHT BEGIN:STANDARD TZNAME:GMT TZOFFSETFROM:+0100 TZOFFSETTO:+0000 DTSTART:19721029T030000 RRULE:FREQ=YEARLY;UNTIL=19801026T020000Z;BYMONTH=10;BYMONTHDAY=23,24,25,2 6,27,28,29;BYDAY=SU END:STANDARD BEGIN:DAYLIGHT TZNAME:BST TZOFFSETFROM:+0000 TZOFFSETTO:+0100 DTSTART:19810329T010000 RRULE:FREQ=YEARLY;BYMONTH=3;BYDAY=-1SU END:DAYLIGHT BEGIN:STANDARD TZNAME:GMT TZOFFSETFROM:+0100 TZOFFSETTO:+0000 DTSTART:19811025T020000 RRULE:FREQ=YEARLY;UNTIL=19891029T010000Z;BYMONTH=10;BYMONTHDAY=23,24,25,2 6,27,28,29;BYDAY=SU END:STANDARD BEGIN:STANDARD TZNAME:GMT TZOFFSETFROM:+0100 TZOFFSETTO:+0000 DTSTART:19901028T020000 RRULE:FREQ=YEARLY;UNTIL=19951022T010000Z;BYMONTH=10;BYDAY=4SU END:STANDARD BEGIN:STANDARD TZNAME:GMT TZOFFSETFROM:+0000 TZOFFSETTO:+0000 DTSTART:19960101T000000 END:STANDARD BEGIN:STANDARD TZNAME:GMT TZOFFSETFROM:+0100 TZOFFSETTO:+0000 DTSTART:19961027T020000 RRULE:FREQ=YEARLY;BYMONTH=10;BYDAY=-1SU END:STANDARD END:VTIMEZONE BEGIN:VEVENT DTSTAMP:20260626T170804Z DTSTART;VALUE=DATE-TIME:20151027T130000 DTEND;VALUE=DATE-TIME:20151027T140000 SUMMARY:Alix McCollam TZID:Europe/London UID:20151027-094d43f55037e98d01504b9dba680663@warwick.ac.uk CREATED:20151009T080039Z DESCRIPTION:Tuning the carrier density and sub-band properties at the LaA lO3/SrTiO3 interface. Alix McCollam. High Field Magnet Laboratory\, Radb oud University Nijmegen\, The Netherlands. Oxides of transition metals h ave complex phase diagrams and a rich variety of ground states\, where s trong correlations between electrons mean that small adjustments of comp osition or structure can greatly change the properties of a system. Comb ining oxides in artificial heterostructures\, by building up layers of a tomically perfect thin films\, provides the opportunity to engineer syst ems with specific functionalities. Moreover\, heterostructures offer the possibility of properties at the interface which are not found in the b ulk components. This approach was proven to be highly successful for III -V semiconductors\, and is now showing signs of being equally fruitful f or oxides\, where a highly conducting 2-dimensional electron gas\, which is also sometimes superconducting or magnetic\, is found at interfaces between SrTiO3 and several other insulating perovskite oxides. I will gi ve a short introduction to the physics of oxide heterostructures and pre sent the results of high field magnetotransport measurements on the LaAl O3/SrTiO3 system. Quantum oscillations observed in the resistivity and H all effect allow us to probe the bandstructure of the interface electron gas\, and give information about the properties of the mobile charge ca rriers. I will briefly discuss our current theoretical understanding of the interface electronic properties and how it relates to experiments\, and will also present very recent measurements\, in which we used the el ectric field effect to tune the carrier density of the electron gas and control the evolution of the conduction bandstructure and carrier proper ties. References: A. McCollam et al.\, Quantum oscillations and subband properties of the two-dimensional electron gas at the LaAlO3/SrTiO3 inte rface. APL Materials 2\, 022102 (2014). L. van Heeringen\, et al.\, k.p subband structure of the LaAlO3/SrTiO3 interface. Phys. Rev. B {\\bf 88} \, 205140 (2013) LOCATION:P5.23 CATEGORIES:Condensed Matter Physics Seminar LAST-MODIFIED:20151021T075538Z ORGANIZER;CN=Jon Duffy: END:VEVENT END:VCALENDAR