Negative index materials are artificial structures whose refractive index has negative value over some frequency range. The study of these materials has attracted a lot of attention in the scientific community not only because of their many potential interesting applications but also because of challenges in understanding their intriguing properties due to the sign-changing coefficients in equations describing their properties. In this paper, we establish cloaking using complementary media for electromagnetic waves. This confirms and extends the suggestions of Lai et al. [Phys. Rev. Lett. 102 (2009) 093901] for the full Maxwell equations. The analysis is based on the reflecting and removing localized singularity techniques, three-sphere inequalities, and the fact that the Maxwell equations can be reduced to a weakly coupled second order elliptic equations.
Accepté le :
DOI : 10.1051/cocv/2017078
Mots-clés : Negative index materials, cloaking, complementary media, localized resonance, electromagnetic waves
@article{COCV_2019__25__A29_0, author = {Nguyen, Hoai-Minh}, title = {Cloaking using complementary media for electromagnetic waves}, journal = {ESAIM: Control, Optimisation and Calculus of Variations}, publisher = {EDP-Sciences}, volume = {25}, year = {2019}, doi = {10.1051/cocv/2017078}, zbl = {1437.35649}, mrnumber = {3990650}, language = {en}, url = {http://www.numdam.org/articles/10.1051/cocv/2017078/} }
TY - JOUR AU - Nguyen, Hoai-Minh TI - Cloaking using complementary media for electromagnetic waves JO - ESAIM: Control, Optimisation and Calculus of Variations PY - 2019 VL - 25 PB - EDP-Sciences UR - http://www.numdam.org/articles/10.1051/cocv/2017078/ DO - 10.1051/cocv/2017078 LA - en ID - COCV_2019__25__A29_0 ER -
%0 Journal Article %A Nguyen, Hoai-Minh %T Cloaking using complementary media for electromagnetic waves %J ESAIM: Control, Optimisation and Calculus of Variations %D 2019 %V 25 %I EDP-Sciences %U http://www.numdam.org/articles/10.1051/cocv/2017078/ %R 10.1051/cocv/2017078 %G en %F COCV_2019__25__A29_0
Nguyen, Hoai-Minh. Cloaking using complementary media for electromagnetic waves. ESAIM: Control, Optimisation and Calculus of Variations, Tome 25 (2019), article no. 29. doi : 10.1051/cocv/2017078. http://www.numdam.org/articles/10.1051/cocv/2017078/
[1] An optimization-based numerical method for diffusion problems with sign-changing coefficients. C. R. Math. Acad. Sci. Paris 355 (2017) 472–478. | DOI | MR | Zbl
, and ,[2] The stability for the Cauchy problem for elliptic equations. Inverse Probl. 25 (2009) 123004. | DOI | MR | Zbl
, , and ,[3] Some remarks on the characterization of the space of tangential traces of H(rot; Ω) and the construction of an extension operator. Manuscr. Math. 89 (1996) 159–178. | DOI | MR | Zbl
and ,[4] Anomalous localized resonance using a folded geometry in three dimensions. Proc. R. Soc. Lond. Ser. A 469 (2013) 20130048. | Zbl
, , , and ,[5] On uniqueness for time harmonic anisotropic Maxwell’s equations with piecewise regular coefficients. Math. Models Methods Appl. Sci. 22 (2012) 1250036. | DOI | MR | Zbl
, and ,[6] T-coercivity for scalar interface problems between dielectrics and metamaterials. ESAIM: M2AN 46 (2012) 1363–1387. | DOI | Numdam | MR | Zbl
, and ,[7] Superlensing using hyperbolic metamaterials: the scalar case. Preprint (2016). | arXiv | MR
and ,[8] Cloaking of small objects by anomalous localized resonance. Q. J. Mech. Appl. Math. 63 (2010) 437–463. | DOI | MR | Zbl
and ,[9] On traces for H(, Ω) in Lipschitz domains, J. Math. Anal. Appl. 276 (2002) 845–867. | DOI | MR | Zbl
, and ,[10] Spectral theory for Maxwell’s equations at the interface of a metamaterial. Part I: Generalized Fourier transform. Preprint (2016). | arXiv | MR
, and ,[11] Inverse Acoustic and Electromagnetic Scattering Theory. 2nd edn. Vol. 98 of Applied Mathematical Sciences. Springer-Verlag, Berlin (1998). | MR | Zbl
and , in[12] A direct boundary integral equation method for transmission problems. J. Math. Anal. Appl. 106 (1985) 367–413. | DOI | MR | Zbl
and ,[13] A variational perspective on cloaking by anomalous localized resonance. Commun. Math. Phys. 328 (2014) 1–27. | DOI | MR | Zbl
, , and ,[14] Complementary media invisibility cloak that cloaks objects at a distance outside the cloaking shell. Phys. Rev. Lett. 102 (2009) 093901. | DOI
, , and ,[15] On the cloaking effects associated with anomalous localized resonance. Proc. R. Soc. Lond. Ser. A 462 (2006) 3027–3059. | MR | Zbl
and ,[16] Asymptotic behavior of solutions to the Helmholtz equations with sign changing coefficients. Trans. Am. Math. Soc. 367 (2015) 6581–6595. | DOI | MR | Zbl
,[17] Cloaking via anomalous localized resonance. A connection between the localized resonance and the blow up of the power for doubly complementary media. C. R. Math. Acad. Sci. Paris 353 (2015) 41–46. | DOI | MR | Zbl
,[18] Cloaking via anomalous localized resonance for doubly complementary media in the quasi static regime. J. Eur. Math. Soc. 17 (2015) 1327–1365. | DOI | MR | Zbl
,[19] Superlensing using complementary media. Ann. Inst. Henri Poincaré Anal. Non Linéaire 32 (2015) 471–484. | DOI | MR | Zbl
,[20] Cloaking using complementary media in the quasistatic regime. Ann. Inst. Henri Poincaré Anal. Non Linéaire 33 (2016) 1509–1518. | DOI | Numdam | MR | Zbl
,[21] Limiting absorption principle and well-posedness for the Helmholtz equation with sign changing coefficients. J. Math. Pures Appl. 106 (2016) 797–836. | MR
,[22] Cloaking an arbitrary object via anomalous localized resonance: the cloak is independent of the object. SIAM J. Math. Anal. 49 (2017) 3208–3232. | DOI | MR | Zbl
,[23] Superlensing using complementary media and reflecting complementary media for electromagnetic waves. Adv. Nonlinear Anal. (2018). | MR | Zbl
,[24] Cloaking via anomalous localized resonance for doubly complementary media in the finite frequency regime. J. Anal. Math. (2018). | MR
,[25] Complete resonance and localized resonance in plasmonic structures. ESAIM: M2AN 49 (2015) 741–754. | DOI | Numdam | MR | Zbl
and ,[26] Cloaking using complementary media for the Helmholtz equation and a three spheres inequality for second order elliptic equations. Trans. Am. Math. Soc. B 2 (2016) 93–112. | DOI | MR | Zbl
and ,[27] Discreteness of interior transmission eigenvalues revisited. Calc. Var. Partial Differ. Equ. 56 (2017) 51. | DOI | MR | Zbl
and ,[28] Electromagnetic wave propagation in media consisting of dispersive metamaterials. Preprint (2017). | arXiv | MR
and ,[29] Quantitative uniqueness estimate for the Maxwell system with Lipschitz anisotropic media. Proc. Am. Math. Soc. 140 (2012) 595–605. | DOI | MR | Zbl
and ,[30] Remarks on a transmission problem. J. Math. Anal. Appl. 196 (1995) 639–658. | DOI | MR | Zbl
,[31] Spherical perfect lens: solutions of Maxwell’s equations for spherical geometry. Phys. Rev. B 69 (2004) 115115. | DOI
and ,[32] Experimental verification of a negative index of refraction. Science 292 (2001) 77–79. | DOI
, and ,[33] The electrodynamics of substances with simultaneously negative values of ε and μ. Usp. Fiz. Nauk 92 (1964) 517–526.
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