Advances in imaging and sensing by Shuo Tang, Daryoosh Saeedkia PDF

By Shuo Tang, Daryoosh Saeedkia

ISBN-10: 1315354101

ISBN-13: 9781315354101

ISBN-10: 1498714757

ISBN-13: 9781498714754

ISBN-10: 1498714765

ISBN-13: 9781498714761

This introductory, but in-depth, booklet explains the actual ideas of digital imaging and sensing and offers the reader with the knowledge essential to comprehend the layout, operation, and functional functions of up to date digital imaging and sensing platforms. The textual content has robust sensible concentration and includes examples of biomedical purposes of optical digital imaging and sensing. each one bankruptcy attracts upon the authors’ vast learn, educating, and commercial event and offers an invaluable source for undergraduate and graduate scholars, in addition to a handy reference for scientists and engineers operating within the box of digital imaging and sensing.

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Otsuji, S. Boubanga Tombet, A. Satou, M. Ryzhii, and V. Ryzhii, Terahertz-wave generation using graphene-toward new types of terahertz lasers, IEEE J. Sel. Top. Quant. Electron. 19, 8400209 (2013). 19. V. Ryzhii, A. Satou, and T. Otsuji, Plasma waves in two-dimensional electron-hole system in gated graphene heterostructures, J. Appl. 101, 024509 (2007). 20. D. Svintsov, V. Vyurkov, S. Yurchenko, T. Otsuji, and V. Ryzhii, Hydrodynamic model for electron-hole plasma in graphene, J. Appl. Phys. 111, 083715 (2012).

12, 4518–4522 (2012). 58. L. Ju, B. Geng, J. Horng, C. Girit, M. Martin, Z. A. , Graphene plasmonics for tunable terahertz metamaterials, Nat. Nanotechnol. 6, 630–634 (2011). 59. J. Maultzsch, Double-resonant Raman scattering in graphite: Interference effects, selection rules, and phonon dispersion, Phys. Rev. B 70, 155403 (2004). 60. H. Suzuura and T. Ando, Zone-boundary phonon in graphene and nanotube, J. Phys. Soc. Jpn. 77, 044703 (2008). 61. M. Dawlaty, S. Shivaraman, M. Chandrashekhar, F. G.

Bullets are the simulation results and solid lines are guides for the eye. V. , J. ) Suppose that the graphene is optically or electrically pumped. 11b shows the contour map of the calculated absorbance as a function of the quasi-Fermi energy (which corresponds to the pumping strength and, hence, the population inversion) and the THz wave frequency for the PA-GPMC with a period L = 500 nm and the length of each microcavity w = 400 nm [24]. With increasing εF, the energy gain can balance the energy loss so that the net energy loss becomes zero, Re[σ(ω)] = 0, with corresponding graphene transparency.

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Advances in imaging and sensing by Shuo Tang, Daryoosh Saeedkia

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