{"@context":"http://iiif.io/api/presentation/2/context.json","@id":"https://repo.library.stonybrook.edu/cantaloupe/iiif/2/manifest.json","@type":"sc:Manifest","label":"Quantum transport in ballistic graphene devices","metadata":[{"label":"dc.description.sponsorship","value":"This work is sponsored by the Stony Brook University Graduate School in compliance with the requirements for completion of degree."},{"label":"dc.format","value":"Monograph"},{"label":"dc.format.medium","value":"Electronic Resource"},{"label":"dc.identifier.uri","value":"http://hdl.handle.net/11401/76675"},{"label":"dc.language.iso","value":"en_US"},{"label":"dc.publisher","value":"The Graduate School, Stony Brook University: Stony Brook, NY."},{"label":"dcterms.abstract","value":"Graphene is a zero gap 2-D semiconductor having chiral charge carriers described by the massless relativistic Dirac-like Hamiltonian. In this thesis, unique transport properties that emerge from this energy spectrum are studied by using ballistic graphene and coupling its charge carriers with superconducting pair potentials and electrostatic gates. Superconducting correlations can be induced in graphene by bringing it in contact with a superconductor. This superconducting proximity effect (PE) provides a way of exploring phenomena such as pseudo-diffusive dynamics of ballistic carriers, specular Andreev reflections and unconventional quantum Hall effect with Andreev edge states. Hitherto, experimental realizations were limited by diffusive devices coupled to superconductors with low critical fields. In the first part of this work, in order to study these phenomena, we develop ballistic suspended graphene (G)-Niobium type\u2013II superconductor(S) Josephson junctions. Our devices exhibit long mean free paths, small potential fluctuations near the charge neutrality point (CNP) and transparent S-G interfaces that support ballistic super currents. In such a device, when the gate voltage is tuned very close to the CNP, unlike in diffusive junctions, we observe a strong density dependence of the multiple Andreev reflection features and normalized excess current. The observations qualitatively agree with a longstanding theoretical prediction for emergence of evanescent mode mediated pseudo diffusive transport. Next, studying magneto-transport in these devices we find that PE is suppressed at very low fields even as the contacts remain superconducting. Further study reveals that distribution of vortices in the superconducting contacts affects the strength of the PE at the S-G interface. The final part of the thesis searches for analogues of Klein tunneling in ballistic graphene by studying charge transport through an electrostatically created potential barrier. To this end, different device fabrication methods are developed to create ballistic heterojunctions on suspended graphene and graphene on hexagonal boron nitride using contactless \u2018air\u2019 local gates."},{"label":"dcterms.available","value":"2017-09-20T16:50:56Z"},{"label":"dcterms.contributor","value":"Allen, Philip"},{"label":"dcterms.creator","value":"Kumaravadivel, Piranavan"},{"label":"dcterms.dateAccepted","value":"2017-09-20T16:50:56Z"},{"label":"dcterms.dateSubmitted","value":"2017-09-20T16:50:56Z"},{"label":"dcterms.description","value":"Department of Physics."},{"label":"dcterms.extent","value":"113 pg."},{"label":"dcterms.format","value":"Monograph"},{"label":"dcterms.identifier","value":"http://hdl.handle.net/11401/76675"},{"label":"dcterms.issued","value":"2015-05-01"},{"label":"dcterms.language","value":"en_US"},{"label":"dcterms.provenance","value":"Made available in DSpace on 2017-09-20T16:50:56Z (GMT). No. of bitstreams: 1\nKumaravadivel_grad.sunysb_0771E_12572.pdf: 4827071 bytes, checksum: 112e3d10e9d8799575cc7043f5e67596 (MD5)\n Previous issue date: 2015"},{"label":"dcterms.publisher","value":"The Graduate School, Stony Brook University: Stony Brook, NY."},{"label":"dcterms.subject","value":"Andreev reflection, Ballistic transport, graphene, Klein tunneling, superconducting proximity effect, suspended graphene superconductor junctions"},{"label":"dcterms.title","value":"Quantum transport in ballistic graphene devices"},{"label":"dcterms.type","value":"Dissertation"},{"label":"dc.type","value":"Dissertation"}],"description":"This manifest was generated dynamically","viewingDirection":"left-to-right","sequences":[{"@type":"sc:Sequence","canvases":[{"@id":"https://repo.library.stonybrook.edu/cantaloupe/iiif/2/canvas/page-1.json","@type":"sc:Canvas","label":"Page 1","height":1650,"width":1275,"images":[{"@type":"oa:Annotation","motivation":"sc:painting","resource":{"@id":"https://repo.library.stonybrook.edu/cantaloupe/iiif/2/49%2F80%2F11%2F4980118160676603263541625260924555729/full/full/0/default.jpg","@type":"dctypes:Image","format":"image/jpeg","height":1650,"width":1275,"service":{"@context":"http://iiif.io/api/image/2/context.json","@id":"https://repo.library.stonybrook.edu/cantaloupe/iiif/2/49%2F80%2F11%2F4980118160676603263541625260924555729","profile":"http://iiif.io/api/image/2/level2.json"}},"on":"https://repo.library.stonybrook.edu/cantaloupe/iiif/2/canvas/page-1.json"}]}]}]}