Full-text resources of PSJD and other databases are now available in the new Library of Science.
Visit https://bibliotekanauki.pl

PL EN


Preferences help
enabled [disable] Abstract
Number of results
2014 | 1 | 1 |

Article title

Multimode Sensor of Fluids Based on Porous Film

Content

Title variants

Languages of publication

EN

Abstracts

EN
Multimode interferometers are coming of age both as sensors and components of quantum circuits.Here we investigate an interferometer based on a porous thinfilm sensor of refractive index of fluids. Eigenmode analysis is used to identify effective single- and multi-mode sensing regimes and the corresponding realizations of interferometer. A general measure in a form of Fisher information is introduced to describe the impact of the film porosity on sensitivity and nonlinearity of the interferometer. As high sensitivity relies on formation of a highly peaked mode in the film, a parallel with plasmonic sensors is drawn. Close correlations between the sensor nonlinearity, mode profile and the shape of Fisher information function indicate the potential of this measure in describing complex non-Gaussian multimode structures

Publisher

Year

Volume

1

Issue

1

Physical description

Dates

published
1 - 1 - 2014
online
19 - 11 - 2014
accepted
19 - 9 - 2014
received
30 - 6 - 2014

Contributors

  • School of Electrical Engineering, University of Belgrade, BulevarKralja Aleksandra 73, 11120 Belgrade, Serbia, and P* Group, Vinča Institute of Nuclear Sciences, University of Belgrade, P.O.B. 522, Belgrade, Serbia
  • P* Group, Vinča Institute of Nuclear Sciences, University of Belgrade, P.O.B. 522, Belgrade, Serbia
  • P* Group, Vinča Institute of Nuclear Sciences, University of Belgrade, P.O.B. 522, Belgrade, Serbia

References

  • [1] Escobedo C, Brolo AG, Gordon R, Sinton D. Optofluidic concentration: plasmonic nanostructure as concentrator and sensor. Nano Lett 2012, 12, 1592-6.[PubMed][Crossref][WoS]
  • [2] Sepulveda B, Sanchez J, Moreno M, Blanco FJ, Mayora K, Domingez C and Lechuga LM. Optical biosensor microsystems based on the integration of highly sensitive Mach-Zhender interferometer devices. J Opt A Pure: Appl Opt 2006, 8, 561-6.[Crossref]
  • [3] Anderson MA, Tinsley-Bown A, Allcock P, Perkins EA, Snow P, Hollings M, Smith RG, Reeves C, Squirrell DJ, Nicklin S, and Cox TI. Sensitivity of the optical properties of porous silicon layers to the refractive index of liquid in the pores. Phys Stat Sol (a) 2003, 197, 528-33.
  • [4] MacCraith BD. Enhanced evanescent wave sensors based on sol-gel-derived porous glass coatings. Sensor Actuator B 1993, 11, 29-34.[Crossref]
  • [5] Lee BH, Kim YH, Park KS, Eom JB, Kim MJ, Rho BS and Choi HY. Interferometric Fiber Optic Sensors. Sensors 2012, 12, 2467-86.[Crossref]
  • [6] Frazão O, Viegas J, Caldas P, Santos JL, Araújo FM, Ferreira LA, Farahi F. All-fiber Mach-Zehnder curvature sensor based on multimode interference combined with a long-period grating. Opt Letters 2007, 32, 3074-6.[WoS][Crossref]
  • [7] Soldano LB and PenningsECM. Optical Multi-Mode Interference Devices Based on Self-Imaging: Principles and Applications. J Lightwave Technol. 1995, 13, 615-627.[Crossref]
  • [8] PetrovicJ, HerreraI, Lombardi P, SchaferF and CataliottiFS. A multi-state interferometer on an atom chip. New J Phys 2013, 15 , 1-13.
  • [9] Crespi A, Osellame R, Ramponi R, Brod DJ, Galvão EF, Spagnolo N, Vitelli C, Maiorino E, Mataloni P &Sciarrino F. Integrated multimode interferometers with arbitrary designs for photonic boson sampling. Nature Photonics 2013, 7, 545-549.[Crossref][WoS]
  • [10] Kim YH, Kim MJ, ParkMS, Jang JH, and Lee BH, Kim KT.. Hydrogen Sensor Based on A Palladium-Coated Long-Period Fiber Grating Pair. Journal of the Optical Society of Korea 2008, 12, 221-5.[WoS][Crossref]
  • [11] Silva S, Frazãoa O, Santosa JL, Malcatac FX. A reflective optical fiber refractometer based on multimode interference. Sensors and Actuators B 2012, 161, 88- 92.[WoS]
  • [12] Frieden RB. Science from Fisher information: A Unification. Cambridge, UK, Cambridge University Press, 2004.
  • [13] Chwedenczuk J, Hyllus P, Piazza F and Smerzi A. Sub-shot-noise interferometry from measurements of the one-body density, New Journal of Physics 2012, 14, 093001 -20.[Crossref]
  • [14] Luis A Fisher information as a generalized measure of coherence in classical and quantum optics, Opt Express 2012, 20, 24686-98.[WoS][Crossref][PubMed]
  • [15] López-Ruiz R, Mancini H L, Calbet X. A statistical measure of complexity. Physics Letters A 1995, 209, 321-6.[WoS]
  • [16] Frieden B R. Fisher information, disorder, and the equilibrium distributions of physics. Physical Review A 1990, 41, 4265-76.
  • [17] Romera E, Sánchez-Moreno P, Dehesa J S. The Fisher information of single-particle systems with a central potential. Chemical Physics Letters 2005, 414, 468-72.
  • [18] Bittner A, Jahn R, Lobmann P. TiO2 thin films on soda-lime and borosilicate glass prepared by sol-gel processing: influence of the substrates. J Sol-Gel Sci Technol 2011, 58, 400-6.[WoS]
  • [19] Hutchinson NJ, Coquil T, Navid A, Pilon L. Effective optical properties of highly ordered mesoporous thin films. Thin Solid Films 2010, 518, 2141-2146.[WoS]
  • [20] Raicevic N,Maluckov A, Petrovic J. Evanescent-wave optical gas sensorwith a porous thin-film coating. To be published in: Phys. Scr. 2014
  • [21] Kawano K and Kitoh T. Finite-difference methods. In: Introduction to optical waveguide analysis. NY , USA, JohnWiley & Sons, INC, 2001, 174-204.
  • [22] Nourdin I and Nualart D. Fisher Information and the Fourth Moment Theorem, arXiv 2013, math. PR, 1-23.
  • [23] Nourdin I, Peccati G, Swan Y. Entropy and the fourth moment phenomenon. Journal of Functional Analysis 2014, 266, 3170-207.[WoS]
  • [24] Henrist C, Dewalque J,Mathis F, Cloots R. Control of the porosity of anatase thin films prepared by EISA: Influence of thickness and heat treatment. MicroporMesoporMat 2009, 117, 292-6.
  • [25] Horowitz F, Dawnay EJC, Fardad MA, Green M and Yeatman EM, Towards better control of sol-gel film, processing for optical device applications. J Nonlinear Opt. Phys 1997, 6, 1-18.[Crossref]
  • [26] Choi H, Stathatos E, Dionysiou DD. Sol-gel preparation of mesoporousphotocatalytic TiO2 films and TiO2/Al2O3 composite membranes for environmental applications. ApplCatal BEnviron 2006, 63, 60-67.
  • [27] Lofgree JE and Ozin GA. Controlling morphology and porosity to improve performance of molecularly imprinted sol-gel silica. ChemSoc Rev 2014, 43, 911-33.
  • [28] RoeyJV, van der Donk J, and Lagasse P E. Beam-propagation method: analysis and assessment. J Opt Soc Am 1981, 71, 803-10.
  • [29] Nesterov ML, Kats AV, Turitsyn SK. Extremely short-lenght surface plasmon resonance devices. Opt Express 2008, 16, 20227-40.[Crossref]
  • [30] Landau L. ZurTheorie der Energieubertragung. II. PhysikalischeZeitschrift der Sowjetunion 2: (1932) 46-51.
  • [31] Zener C. Non-Adiabatic Crossing of Energy Levels". Proceedings of the Royal Society of London A 1932, 137, 696-702.

Document Type

Publication order reference

Identifiers

YADDA identifier

bwmeta1.element.-psjd-doi-10_2478_optof-2014-0006
JavaScript is turned off in your web browser. Turn it on to take full advantage of this site, then refresh the page.