Microcavity lasers on polymer materials: Boundary integral equation modeling and experiments
dc.citation.epage | 561 | en_US |
dc.citation.spage | 559 | en_US |
dc.contributor.author | Nosich, A.I. | en_US |
dc.contributor.author | Smotrova, E.I. | en_US |
dc.contributor.author | Lebental, M. | en_US |
dc.contributor.author | Sukharevsky Ilya O. | en_US |
dc.contributor.author | Altıntaş, Ayhan | en_US |
dc.coverage.spatial | Kiev, Ukraine | |
dc.date.accessioned | 2016-02-08T12:05:32Z | |
dc.date.available | 2016-02-08T12:05:32Z | |
dc.date.issued | 2015-04 | en_US |
dc.department | Department of Computer Engineering | en_US |
dc.department | Department of Electrical and Electronics Engineering | en_US |
dc.description | Date of Conference: 21-24 April 2015 | |
dc.description | Conference name: 2015 IEEE 35th International Conference on Electronics and Nanotechnology (ELNANO) | |
dc.description.abstract | We consider the modeling and experiments with polymer dye-doped lasers shaped as thin flat cavities, allowing one to consider them as two-dimensional (2-D) active cavities. We focus our modeling on the H-polarized electromagnetic field in a kite-shaped laser. Assuming that the lasing-mode frequency is real-valued, we look for it together with the corresponding threshold value of material gain. Such electromagnetic-field problem is reduced to the Muller set of the boundary integral equations (MBIE), discretization of which yields determinantal equation. Numerical results reveal various types of modes existing in the kite including the perturbed whispering gallery (WG) modes that have the lowest thresholds. Their far-field emission patterns show good agreement with the measurements. © 2015 IEEE. | en_US |
dc.description.provenance | Made available in DSpace on 2016-02-08T12:05:32Z (GMT). No. of bitstreams: 1 bilkent-research-paper.pdf: 70227 bytes, checksum: 26e812c6f5156f83f0e77b261a471b5a (MD5) Previous issue date: 2015 | en |
dc.identifier.doi | 10.1109/ELNANO.2015.7146949 | en_US |
dc.identifier.uri | http://hdl.handle.net/11693/27929 | en_US |
dc.language.iso | English | en_US |
dc.publisher | IEEE | en_US |
dc.relation.isversionof | http://dx.doi.org/10.1109/ELNANO.2015.7146949 | en_US |
dc.source.title | 2015 IEEE 35th International Conference on Electronics and Nanotechnology, ELNANO 2015 - Conference Proceedings | en_US |
dc.subject | Microcavity laser | en_US |
dc.subject | Threshold | en_US |
dc.subject | Boundary integral equations | en_US |
dc.subject | Electromagnetic fields | en_US |
dc.subject | Microcavities | en_US |
dc.subject | Nanotechnology | en_US |
dc.subject | Whispering gallery modes | en_US |
dc.subject | Determinantal equations | en_US |
dc.subject | Electromagnetic field problems | en_US |
dc.subject | Polymer materials | en_US |
dc.subject | Two Dimensional (2 D) | en_US |
dc.subject | Whispering gallery | en_US |
dc.subject | Integral equations | en_US |
dc.title | Microcavity lasers on polymer materials: Boundary integral equation modeling and experiments | en_US |
dc.type | Conference Paper | en_US |
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