Download Active Plasmonics and Tuneable Plasmonic Metamaterials by Anatoly Zayats PDF

By Anatoly Zayats

ISBN: 1118092082
EAN: 9781118092088
ASIN: 1118092082
Publisher: Wiley
Publication Date: 2013-07-15
Number of Pages: 336

This publication, edited by means of of the main revered researchers in plasmonics, offers an outline of the present kingdom in plasmonics and plasmonic-based metamaterials, with an emphasis on energetic functionalities and an eye fixed to destiny advancements. This booklet is multifunctional, invaluable for rookies and scientists attracted to functions of plasmonics and metamaterials in addition to for confirmed researchers during this multidisciplinary region.

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7: 270–275. 9. Hirsch LR, Stafford RJ, Bankson JA, Sershen SR, Rivera B, Price RE, Hazle JD, Halas NJ, West JL (2003) Nanoshell-mediated near-infrared thermal therapy of tumors under magnetic resonance guidance. Proc. Natl Acad. Sci. USA 100: 13549– 13554. 10. Park I-Y, Kim S, Choi J, Lee D-H, Kim Y-J, Kling MF, Stockman MI, Kim S-W (2011) Plasmonic generation of ultrashort extreme-ultraviolet light pulses. Nat. Photonics 5: 677–681. 11. Stockman MI (2011) Nanoplasmonics: the physics behind the applications.

53) where the strict inequality corresponds to the overcompensation and net amplification. 50) we have assumed nonpolarized gain transitions. If these transitions are all polarized along the excitation electric field, the concentration nc should be multiplied by a factor of 3. 45) is satisfied, which is very realistic for metamaterials] and general. Moreover, it is fully analytical and, actually, very simple. Remarkably, it depends only on the material characteristics and does not contain any geometric properties of the metamaterial system or the local fields.

There is no full loss compensation and spasing. This is explained by the fact that Reference 53 uses, as a close inspection shows, the gain dipoles parallel to the field (this is equivalent to increasing nc by a factor of 3) and the local-field enhancement [this is equivalent to increasing nc by 30 Spaser, Plasmonic Amplification, and Loss Compensation a factor of (εh + 2)/3]. Because the absorption cross section of dyes is measured in the appropriate host media (liquid solvents or polymers), it already includes the Lorentz local-field factor.

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