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Ultrahigh Q-factor Ge11.5As24Se64.5 chalcogenide glass photonic crystal cavity embedded in silica

Gai, Xin; White, Thomas; Luther-Davies, Barry

Description

Photonic crystals (PhCs) have attracted much attention for their ability to manipulate light, for example structures containing ultrahigh Q-factor cavities allow low threshold all-optical switching as has been demonstrated in 2-D PhCs fabricated in air-clad silicon membranes. However, the strong two-photon (TPA) and free-carrier absorption (FCA) in silicon has meant that optical switching has so far been due to the slow thermal nonlinearity exacerbated by the low thermal mass and poor heat...[Show more]

dc.contributor.authorGai, Xin
dc.contributor.authorWhite, Thomas
dc.contributor.authorLuther-Davies, Barry
dc.coverage.spatialMunich Germany
dc.date.accessioned2015-12-07T22:44:18Z
dc.date.createdMay 22-26 2011
dc.identifier.isbn9781457712234
dc.identifier.urihttp://hdl.handle.net/1885/25126
dc.description.abstractPhotonic crystals (PhCs) have attracted much attention for their ability to manipulate light, for example structures containing ultrahigh Q-factor cavities allow low threshold all-optical switching as has been demonstrated in 2-D PhCs fabricated in air-clad silicon membranes. However, the strong two-photon (TPA) and free-carrier absorption (FCA) in silicon has meant that optical switching has so far been due to the slow thermal nonlinearity exacerbated by the low thermal mass and poor heat conduction from the 2-D resonant cavity. To achieve optical switching via the ultrafast Kerr nonlinearity the PhC resonators must be fabricated from materials with negligible TPA and FCA and with better heat conduction from the cavity. This can, in principle, be achieved by replacing the silicon with a highly nonlinear chalcogenide glass membrane embedded in a cladding to increase heat conduction and thermal mass. However, such a structure will have a smaller refractive index contrast which can lead to increased energy loss to modes above the light line and lower the Q value.
dc.publisherEuropean Physical Society
dc.relation.ispartofseriesEuropean Conference on Lasers and Electro-Optics (CLEO/Europe 2011)
dc.sourceEuropean Conference on Lasers and Electro-Optics (CLEO/Europe) 2011
dc.subjectKeywords: Air-clad; All-optical switching; Chalcogenide glass; Energy loss; Free carrier absorption; Highly nonlinear; Kerr nonlinearity; Light lines; Low thresholds; Optical switching; Photonic crystal cavities; Q-factors; Q-values; Resonant cavity; Silicon membra
dc.titleUltrahigh Q-factor Ge11.5As24Se64.5 chalcogenide glass photonic crystal cavity embedded in silica
dc.typeConference paper
local.description.notesImported from ARIES
local.description.refereedYes
dc.date.issued2011
local.identifier.absfor020504 - Photonics, Optoelectronics and Optical Communications
local.identifier.absfor020503 - Nonlinear Optics and Spectroscopy
local.identifier.ariespublicationu4882357xPUB36
local.type.statusPublished Version
local.contributor.affiliationGai, Xin, College of Physical and Mathematical Sciences, ANU
local.contributor.affiliationWhite, Thomas, College of Physical and Mathematical Sciences, ANU
local.contributor.affiliationLuther-Davies, Barry, College of Physical and Mathematical Sciences, ANU
local.description.embargo2037-12-31
local.bibliographicCitation.startpage1
local.identifier.doi10.1109/CLEOE.2011.5943261
local.identifier.absseo970102 - Expanding Knowledge in the Physical Sciences
dc.date.updated2016-02-24T11:26:10Z
local.identifier.scopusID2-s2.0-80052277014
CollectionsANU Research Publications

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