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Optics Express

  • Editor: C. Martijn de Sterke
  • Vol. 18, Iss. 5 — Mar. 1, 2010
  • pp: 5161–5167
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Moving targets virtually via composite optical transformation

Wei Xiang Jiang and Tie Jun Cui  »View Author Affiliations


Optics Express, Vol. 18, Issue 5, pp. 5161-5167 (2010)
http://dx.doi.org/10.1364/OE.18.005161


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Abstract

We propose a composite optical transformation to design an illusion device which can move the image of a target from one place to another place. Enclosed by such an illusion device, an arbitrary object located at one place appears to be at another place virtually. Different from the published shifted-position cloak which is composed of the left-handed materials with simultaneously negative permittivity and permeability, the illusion device proposed in this paper has positive permittivity and permeability. Hence the proposed illusion device is easier to be realized by artificial metamaterials.

© 2010 Optical Society of America

More recently, Lai et al. have proposed an interesting idea of illusion optics, which makes a target with arbitrary shape and material property look like another object of some other shape and material makeup [19

19. Y. Lai, J. Ng, H. Y. Chen, D. Z. Han, J. J. Xiao, Z. Q. Zhang, and C. T. Chan, “Illusion optics: the optical transformation of an object into another object,” Phys. Rev. Lett. 102, 253902 (2009). [CrossRef] [PubMed]

]. Some special illusion devices have been discussed before this, such as the super absorber [13

13. J. Ng, H. Y. Chen, and C. T. Chan, “Metamaterial frequency-selective superabsorber,” Opt. Lett. 34, 644–646 (2009). [CrossRef] [PubMed]

], the superscatterer [16

16. T. Yang, H. Y. Chen, X. D. Luo, and H. R. Ma, “Superscatterer: enhancement of scattering with complementary media,” Opt. Express 16, 18545–18550 (2008). [CrossRef] [PubMed]

], the shifted-position cloak [18

18. Y. Luo, J. J. Zhang, H. Chen, B.-I. Wu, and J. A. Kong, “Wave and ray analysis of a type of cloak exhibiting magnified and shifted scattering effect,” (2009). ArXiv: 0904.1463.

], and the cylindrical superlens [21

21. M. Yan, W. Yan, and M. Qiu, “Cylindrical superlens by a coordinate transformation,” Phys. Rev. B 78, 125113 (2008). [CrossRef]

]. However, all above-mentioned illusion devices are composed of the left-handed materials with simultaneously negative permittivity and permeability. Hence such illusion devices are highly demanding on the material properties, and hence extremely difficult to be realized.

In this paper, we propose a composite optical transformation to design an illusion device which makes the enclosed actual object located at one place appear to be at another place. Such a composite coordinate transformation of the illusion device contains two sub-mappings. The proposed illusion device shows unconventional EM properties as verified by accurately numerical simulations. We try to make the illusion device be fairly realizable. Unlike the published illusion devices which are composed of left-handed materials [13

13. J. Ng, H. Y. Chen, and C. T. Chan, “Metamaterial frequency-selective superabsorber,” Opt. Lett. 34, 644–646 (2009). [CrossRef] [PubMed]

, 16–19

16. T. Yang, H. Y. Chen, X. D. Luo, and H. R. Ma, “Superscatterer: enhancement of scattering with complementary media,” Opt. Express 16, 18545–18550 (2008). [CrossRef] [PubMed]

, 21

21. M. Yan, W. Yan, and M. Qiu, “Cylindrical superlens by a coordinate transformation,” Phys. Rev. B 78, 125113 (2008). [CrossRef]

], all permittivity and permeability components of the proposed illusion device are positive. Hence the presented method makes it possible to realize the illusion device by using artificial metamaterials.

A concise schematic to design the proposed illusion device is illustrated in Fig. 1. A car at Position A is enclosed with the illusion device, as shown in Fig. 1(a). Such an illusion device make any detector outside the virtual boundary (surface s) observe the EM fields of a virtual car at Position B (shown in Fig. 1(c)) instead of the actual one. In other words, the illusion device makes the EM-field distributions outside the virtual boundary in both the virtual and physical spaces exactly the same, regardless the direction from which the EM waves are incident. The composite coordinate transformation of the illusion device contains two sub-mappings. First, we map the first virtual space (the free space outside the car in the virtual space in Fig. 1(c)) into a smaller annulus region (the light green region in Fig. 1(b)). Second, we transform the second virtual space (light green region in Fig. 1(b)) into the physical space (dark green region in Fig. 1(a)). The electric permittivity and magnetic permeability tensors of the illusion device are calculated by

ε″¯=21ε¯1T2T/det(12),μ″¯=21μ¯1T2T/det(12),
(1)

in which (ε̄, μ̄) and ( ε″¯ , μ″¯ ) are the permittivity and permeability tensors in the first virtual space (illusion space) and the physical space, respectively, and ∧1 and ∧2 are the Jacobian transformation matrices with components ∧1ij = ∂xi′/∂xj and ∧2ij = ∂xi″/∂xj′ corresponding to the mapping from the first virtual space to the second virtual space, and the mapping from the second virtual space to the physical space, respectively.

Fig. 1. A concise scheme of an illusion device that moves the image of a car from one position to another one. (a) A car at Position A enclosed with the illusion device (dark green region). (b) A bigger illusion car in the second virtual space. (c) The illusion car at Position B in first virtual space.

Similar to other optical transformation devices, the EM fields in the illusion device can be obtained from the transformation optics [1

1. J. B. Pendry, D. Schurig, and D. R. Smith, “Controlling electromagnetic fields,” Science 312, 1780–1782 (2006). [CrossRef] [PubMed]

,2

2. U. Leonhardt, “Optical conformal mapping,” Science 312, 1777–1780 (2006). [CrossRef] [PubMed]

] as E″ = (∧2 T)-1(∧1 T)-1 E and H″ = (∧2 T)-1(∧1 T)-1 H, where E and H are electric and magnetic fields in the first virtual space, respectively. Because the virtual boundary s is mapped to itself during these two sub-mappings ∧1 and ∧2, we have Et = Et = E t and Ht = Ht = H t, where the subscript t indicates the transverse components along the surface s. That is to say, the tangential components of the EM fields on the whole virtual boundary (s) are exactly the same in both physical and virtual spaces. Hence the EM fields outside the illusion device are also exactly the same by using the uniqueness theorem. Any observers outside the illusion device will perceive the scattered fields as if they were scattered from a car at Position B.

Fig. 2. The cross section of an virtual-position-moving device in the Cartesian coordinate system.

For a specific example, we consider an illusion device which can move the image of a metallic cylinder from one place to another place. To design such an illusion device, we construct a composite transformation which contains two sub-mappings in the Cartesian coordinate system (shown in Fig. 2), the first sub-mapping can be expressed as

x=r1(xa1a2)r+a1+a2,
(2)
y=r1yr,
(3)
z=z,
(4)

where (a 1 + a 2, 0), (0, 0) and (a 1, 0) are the centers of virtual and actual metallic cylinders and circular virtual region, respectively, r′1=(R12R11)(rr0)/(R12r0)+R11,R1i=(xa1a2)(a1+a2)/r+bi2(a1+a2)2y2/r2,(i=1,2), and r=(xa1a2)2+y2. Such a sub-mapping describes a similar transformation that maps the blank region in the virtual space in Fig. 1(c) into the light green region in Fig. 1(b). The second sub-mapping can be expressed as

x=rxr2,
(5)
y=ryr2,
(6)
z=z,
(7)

where r″=(R22r1)(r′R21)/(R22R21)+r1,R2i=(x′a1)a1/r′+bi2a12y′2/r′2,(i=1,2), and r′2=x′2+y2. This sub-mapping describes a similar transformation that maps the light green region in Fig. 1(b) into the dark green region in Fig. 1(a). The converse transformation of the virtual variables and the physical variables can be constructed by Eqs. (2)-(7). Then the constitutive parameters of the illusion device can be calculated by formulae (1).

We remark that the EM parameters of the illusion device can also be obtained by another process for such a composite transformation. A function relationship between (x″, y″, z″) and (x, y, z) can be found from Eqs. (2)-(7) as follows,

x=fxy,
(8)
y=gxy,
(9)
z=z.
(10)

Based on the above composite transformation, the permittivity and permeability of the illusion device are expressed as

εxx=μxx=(fx2+fy2)/(fxgyfygx),
(11)
εyy=μyy=(gx2+gy2)/(fxgyfygx),
(12)
εxy=(fxgx+fygy)/(fxgyfygx)=εyx,
(13)
εzz=μzz=1/(fxgyfygx),
(14)
εxz=εyz=μzx=μzy=0,
(15)
μxy=μyx=εxy,
(16)

where we denote the partial derivative of the function f(x,y) to x as fx. We have assumed that the background profile be free space, i.e., ε̄ = ε 0 Ī and μ̄ = μ 0 Ī.

Obviously, these two sub-mappings are not conformal transformations, hence some non-diagonal components of the permittivity and permeability tensors are non-zero. But in the real fabrications, it is necessary that the material parameters ε″¯ and μ″¯ are denoted in diagonal tensors. The symmetry of the real tensors ε″¯ and μ″¯ ensure that a rotation transformation which maps a symmetric tensor into a diagonal one always exists. When a transverse-electric (TE) polarized plane wave is incident upon an enclosed metallic cylinder with infinite length, there exists only z component of electric field, hence only μ″xx, μ″xy, μ″yy and ε″zz are of interest and must satisfy the request of Eqs. (11)-(16). Therefore, the EM parameters in the eigen-basis can be expressed as

μ1=μxx+μyy-μxx22μxxμyy+μyy2+4μxy22,
(17)
μ2=μxx+μyy+μxx22μxxμyy+μyy2+4μxy22,
(18)
εz=εzz,
(19)

and all the off-diagonal components equal zero. In such a case, all components μ 1, μ 2, and εz are finite and positive. Also, μ 2 is always greater than μ 1.

Unlike the earlier-proposed shifted-position cloak which consists of left-handed materials with double negative constitutive parameters [18

18. Y. Luo, J. J. Zhang, H. Chen, B.-I. Wu, and J. A. Kong, “Wave and ray analysis of a type of cloak exhibiting magnified and shifted scattering effect,” (2009). ArXiv: 0904.1463.

], the illusion device here is only composed of one layer of inhomogeneous and anisotropic medium. In order to verify the design of the illusion device, we make accurately numerical simulations using the software package, COM-SOL Multiphysics, which is based on the finite-element method. We consider an illusion device which moves a metallic cylinder from one place virtually to another place. In this example, we choose a 1 = 0.0333 m, a 2 = 0.01667 m, r 0 = r 1 = 0.01 m, b 1=0.0433 m, and b 2 = 0.05 m.

Fig. 3. The parameter distributions of the illusion device, (a) εz, (b) μ 1, and (c) μ 2.

Under the illumination of TE-polarized waves, only μ 1, μ 2 and εz are of interest. The distributions of principle components μ 1, μ 2 and εz are illustrated in Figure 3, from which we clearly observe that all values are finite and positive. It is worth to note that these two sub-mappings in this illusion device are compressing and extending mappings, respectively, instead of the folding of geometry [17–21

17. Y. Lai, H. Chen, Z. Q. Zhang, and C. T. Chan, “Complementary media invisibility cloak that cloaks objects at a distance outside the cloaking shell,” Phys. Rev. Lett. 102, 093901 (2009). [CrossRef] [PubMed]

]. Hence any material parameters of the illusion device are not negative. Similar metamaterial structures have been extensively investigated and fabricated in the experiment of free-space cloaks and other devices at microwave frequencies [3

3. D. Schurig, J. J. Mock, B.J. Justice, S. A. Cummer, J. B. Pendry, A. F. Starr, and D. R. Smith, “Metamaterial electromagnetic cloak at microwave frequencies,” Science 314, 977–980 (2006). [CrossRef] [PubMed]

,11

11. Y. G. Ma, C. K. Ong, T. Tyc, and U. Leonhardt, “An omnidirectional retroreflector based on the transmutation of dielectric singularities,” Nat. Mater. 8, 639–642 (2009). [CrossRef] [PubMed]

].

Figure 4 illustrates the numerical results of total electric fields for the above illusion device. The plane waves are incident vertically from the bottom to the top at 18 GHz. Figs. 4(a) and 4(c) show the total-field distributions of the metallic cylinder located at different places. When the metallic cylinder enclosed by the shifted-position illusion device, the scattered pattern from the metallic cylinder will be changed as if the metallic cylinder was at another place. This can be clearly observed by comparing the scattered patterns of the metallic cylinder coated by the illusion device shown in Fig. 4(b) and the metallic cylinder shown in Fig. 4(c). Inside the virtual boundary, the EM-field distributions in Figs. 4(b) and 4(c) are very different. But the total-field distributions are exactly the same outside the virtual boundary. A position-moving illusion has been generated.

Fig. 4. The total electric-field distributions in the computational domain for (a) a metallic cylinder without the illusion device; (b) the actual metallic cylinder with the illusion device (dashed circle means a virtual metallic cylinder); and (c) the metallic cylinder at another place when the plane waves are incident vertically from the bottom to the top.
Fig. 5. The electric-field distributions for (a) the illusion device with a loss tangent of 0.001; (b) the illusion device with a loss tangent of 0.01 when the plane waves are incident horizontally from the bottom to the top. (c) The effective permeability versus to the frequency for the C structure.

In practice, artificial metamaterials are always lossy. Hence it is necessary to study the lossy effect of the device on the virtual position-moving property. Fig. 5(a) illustrates the electric-field distributions for the illusion device with electric- and magnetic-loss tangents of 0.001. In this case, the effect of loss is very small and can be ignored. When we add a larger loss tangent of 0.01 in both permittivity and permeability of the virtual-position-moving device, the electric-field distributions are demonstrated in Fig. 5(b). Obviously, although the loss degrades the performance of illusion a little bit, we observe that the lossy illusion device is still effective.

The presented illusion device could be realized by designing proper metamaterial structures. For example, to achieve the component μ 1, we can make use of the split-ring resonators (SRR) [3

3. D. Schurig, J. J. Mock, B.J. Justice, S. A. Cummer, J. B. Pendry, A. F. Starr, and D. R. Smith, “Metamaterial electromagnetic cloak at microwave frequencies,” Science 314, 977–980 (2006). [CrossRef] [PubMed]

,11

11. Y. G. Ma, C. K. Ong, T. Tyc, and U. Leonhardt, “An omnidirectional retroreflector based on the transmutation of dielectric singularities,” Nat. Mater. 8, 639–642 (2009). [CrossRef] [PubMed]

,22

22. J. B. Pendry, A. J. Holden, D. J. Robbins, and W. J. Stewart, “Magnetism from conductors and enhanced nonlinear phenomena,” IEEE Trans. Micro. Theo. Tech. 47, 2075 (2009). [CrossRef]

]. One kind of SRR unit, the C structure, has been used for the design, as shown in Fig. 5(c). The imaginary part of permeability for the C-structure unit at the non-resonant frequencies (from 17 GHz to 20 GHz) are small enough to be neglected in the design of illusion device. The component εz can be easily realized using the non-resonant structures such as wire or I shape [5

5. R. Liu, C. Ji, J. J. Mock, J. Y. Chin, T. J. Cui, and D. R. Smith, “Broadband ground-plane cloak,” Science 323, 366–369 (2009). [CrossRef] [PubMed]

]. We remark that it will be a challenging work to optimize the overall design to make a compact layout of virtual-position-moving illusion device, which will be considered in our further work.

In conclusion, we have presented a composite optical transformation to design a kind of illusion device, which can move the target from one place to another place virtually by using metamaterials. In such an illusion device, all diagonal components of constitutive tensors are positive and all off-diagonal ones are zero, hence the illusion device could be realized using artificial metamaterial structures.

Acknowledgments

This work was supported in part by the National Science Foundation of China under Grant Nos. 60990320, 60990324, 60671015, 60871016, and 60901011, in part by the Natural Science Foundation of Jiangsu Province under Grant No. BK2008031, and in part by the 111 Project under Grant No. 111-2-05. WXJ acknowledges the support from the Graduate Innovation Program of Jiangsu Province under No. CX08B-074Z and the Scientific Research Foundation of Graduate School of Southeast University under No. YBJJ0816.

References and links

1.

J. B. Pendry, D. Schurig, and D. R. Smith, “Controlling electromagnetic fields,” Science 312, 1780–1782 (2006). [CrossRef] [PubMed]

2.

U. Leonhardt, “Optical conformal mapping,” Science 312, 1777–1780 (2006). [CrossRef] [PubMed]

3.

D. Schurig, J. J. Mock, B.J. Justice, S. A. Cummer, J. B. Pendry, A. F. Starr, and D. R. Smith, “Metamaterial electromagnetic cloak at microwave frequencies,” Science 314, 977–980 (2006). [CrossRef] [PubMed]

4.

J. Li and J. B. Pendry, “Hiding under the carpet: A new strategy for cloaking,” Phys. Rev. Lett. 101, 203901 (2008). [CrossRef] [PubMed]

5.

R. Liu, C. Ji, J. J. Mock, J. Y. Chin, T. J. Cui, and D. R. Smith, “Broadband ground-plane cloak,” Science 323, 366–369 (2009). [CrossRef] [PubMed]

6.

L. H. Gabrielli, J. Cardenas, C. B. Poitras, and M. Lipson, “Silicon nanostructure cloak operating at optical frequencies,” Nat. Photon. 3, 461–463 (2009). [CrossRef]

7.

J. Valentine, J. Li, T. Zentgraf, G. Bartal, and X. Zhang, “An optical cloak made of dielectrics,” Nat. Mater. 8, 568–571 (2009). [CrossRef] [PubMed]

8.

H. Chen and C. T. Chan, “Transformation media that rotate electromagnetic fields,” Appl. Phys. Lett. 90, 241105 (2007). [CrossRef]

9.

H. Chen, B. Hou, S. Chen, X. Ao, W. Wen, and C. T. Chan, “Design and Experimental Realization of a Broadband Transformation Media Field Rotator at Microwave Frequencies,” Phys. Rev. Lett. 102, 183903 (2009). [CrossRef] [PubMed]

10.

T. Tyc and U. Leonhardt, “Transmutation of singularities in optical instruments,” New J. Phys. 10, 115038 (2008). [CrossRef]

11.

Y. G. Ma, C. K. Ong, T. Tyc, and U. Leonhardt, “An omnidirectional retroreflector based on the transmutation of dielectric singularities,” Nat. Mater. 8, 639–642 (2009). [CrossRef] [PubMed]

12.

W. X. Jiang, T. J. Cui, H. F. Ma, X. M. Yang, and Q. Cheng, “Layered high-gain lens antennas via discrete optical transformation,” Appl. Phys. Lett. 93, 221906 (2008). [CrossRef]

13.

J. Ng, H. Y. Chen, and C. T. Chan, “Metamaterial frequency-selective superabsorber,” Opt. Lett. 34, 644–646 (2009). [CrossRef] [PubMed]

14.

W. X. Jiang, T. J. Cui, X. Y. Zhou, X. M. Yang, and Q. Cheng, “Arbitrary bending of electromagnetic waves using realizable inhomogeneous and anisotropic materials,” Phys. Rev. E 78, 066607 (2008). [CrossRef]

15.

M. Rahm, S. A. Cummer, D. Schurig, J. B. Pendry, and D. R. Smith, “Optical design of reflectionless complex media by finite embedded coordinate transformations,” Phys. Rev. Lett. 100, 063903 (2008). [CrossRef] [PubMed]

16.

T. Yang, H. Y. Chen, X. D. Luo, and H. R. Ma, “Superscatterer: enhancement of scattering with complementary media,” Opt. Express 16, 18545–18550 (2008). [CrossRef] [PubMed]

17.

Y. Lai, H. Chen, Z. Q. Zhang, and C. T. Chan, “Complementary media invisibility cloak that cloaks objects at a distance outside the cloaking shell,” Phys. Rev. Lett. 102, 093901 (2009). [CrossRef] [PubMed]

18.

Y. Luo, J. J. Zhang, H. Chen, B.-I. Wu, and J. A. Kong, “Wave and ray analysis of a type of cloak exhibiting magnified and shifted scattering effect,” (2009). ArXiv: 0904.1463.

19.

Y. Lai, J. Ng, H. Y. Chen, D. Z. Han, J. J. Xiao, Z. Q. Zhang, and C. T. Chan, “Illusion optics: the optical transformation of an object into another object,” Phys. Rev. Lett. 102, 253902 (2009). [CrossRef] [PubMed]

20.

U. Leonhardt and T. G. Philbin, “Transformation optics and the geometry of light,” (2008). ArXiv: 0805.4778.

21.

M. Yan, W. Yan, and M. Qiu, “Cylindrical superlens by a coordinate transformation,” Phys. Rev. B 78, 125113 (2008). [CrossRef]

22.

J. B. Pendry, A. J. Holden, D. J. Robbins, and W. J. Stewart, “Magnetism from conductors and enhanced nonlinear phenomena,” IEEE Trans. Micro. Theo. Tech. 47, 2075 (2009). [CrossRef]

OCIS Codes
(160.1190) Materials : Anisotropic optical materials
(260.2110) Physical optics : Electromagnetic optics
(160.3918) Materials : Metamaterials
(260.2710) Physical optics : Inhomogeneous optical media

ToC Category:
Physical Optics

History
Original Manuscript: December 11, 2009
Revised Manuscript: February 22, 2010
Manuscript Accepted: February 22, 2010
Published: February 25, 2010

Citation
Wei Xiang Jiang and Tie Jun Cui, "Moving targets virtually via composite optical transformation," Opt. Express 18, 5161-5167 (2010)
http://www.opticsinfobase.org/oe/abstract.cfm?URI=oe-18-5-5161


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References

  1. J. B. Pendry, D. Schurig, and D. R. Smith, "Controlling electromagnetic fields," Science 312, 1780-1782 (2006). [CrossRef] [PubMed]
  2. U. Leonhardt, "Optical conformal mapping," Science 312, 1777-1780 (2006). [CrossRef] [PubMed]
  3. D. Schurig, J. J. Mock, B. J. Justice, S. A. Cummer, J. B. Pendry, A. F. Starr, and D. R. Smith, "Metamaterial electromagnetic cloak at microwave frequencies," Science 314, 977-980 (2006). [CrossRef] [PubMed]
  4. J. Li and J. B. Pendry, "Hiding under the carpet: A new strategy for cloaking," Phys. Rev. Lett. 101, 203901 (2008). [CrossRef] [PubMed]
  5. R. Liu, C. Ji, J. J. Mock, J. Y. Chin, T. J. Cui, and D. R. Smith, "Broadband ground-plane cloak," Science 323, 366-369 (2009). [CrossRef] [PubMed]
  6. L. H. Gabrielli, J. Cardenas, C. B. Poitras, and M. Lipson, "Silicon nanostructure cloak operating at optical frequencies," Nat. Photonics 3, 461-463 (2009). [CrossRef]
  7. J. Valentine, J. Li, T. Zentgraf, G. Bartal, and X. Zhang, "An optical cloak made of dielectrics," Nat. Mater. 8, 568-571 (2009). [CrossRef] [PubMed]
  8. H. Chen and C. T. Chan, "Transformation media that rotate electromagnetic fields," Appl. Phys. Lett. 90, 241105 (2007). [CrossRef]
  9. H. Chen, B. Hou, S. Chen, X. Ao,W. Wen, and C. T. Chan, "Design and Experimental Realization of a Broadband Transformation Media Field Rotator at Microwave Frequencies," Phys. Rev. Lett. 102, 183903 (2009). [CrossRef] [PubMed]
  10. T. Tyc and U. Leonhardt, "Transmutation of singularities in optical instruments," New J. Phys. 10, 115038 (2008). [CrossRef]
  11. Y. G. Ma, C. K. Ong, T. Tyc, and U. Leonhardt, "An omnidirectional retroreflector based on the transmutation of dielectric singularities," Nat. Mater. 8, 639-642 (2009). [CrossRef] [PubMed]
  12. W. X. Jiang, T. J. Cui, H. F. Ma, X. M. Yang, and Q. Cheng, "Layered high-gain lens antennas via discrete optical transformation," Appl. Phys. Lett. 93, 221906 (2008). [CrossRef]
  13. J. Ng, H. Y. Chen, and C. T. Chan, "Metamaterial frequency-selective superabsorber," Opt. Lett. 34, 644-646 (2009). [CrossRef] [PubMed]
  14. W. X. Jiang, T. J. Cui, X. Y. Zhou, X. M. Yang, and Q. Cheng, "Arbitrary bending of electromagnetic waves using realizable inhomogeneous and anisotropic materials," Phys. Rev. E 78, 066607 (2008). [CrossRef]
  15. M. Rahm, S. A. Cummer, D. Schurig, J. B. Pendry, and D. R. Smith, "Optical design of reflectionless complex media by finite embedded coordinate transformations," Phys. Rev. Lett. 100, 063903 (2008). [CrossRef] [PubMed]
  16. T. Yang, H. Y. Chen, X. D. Luo, and H. R. Ma, "Superscatterer: enhancement of scattering with complementary media," Opt. Express 16, 18545-18550 (2008). [CrossRef] [PubMed]
  17. Y. Lai, H. Chen, Z. Q. Zhang, and C. T. Chan, "Complementary media invisibility cloak that cloaks objects at a distance outside the cloaking shell," Phys. Rev. Lett. 102, 093901 (2009). [CrossRef] [PubMed]
  18. Y. Luo, J. J. Zhang, H. Chen, B.-I. Wu, and J. A. Kong, "Wave and ray analysis of a type of cloak exhibiting magnified and shifted scattering effect," (2009). ArXiv: 0904.1463.
  19. Y. Lai, J. Ng, H. Y. Chen, D. Z. Han, J. J. Xiao, Z. Q. Zhang, and C. T. Chan, "Illusion optics: the optical transformation of an object into another object," Phys. Rev. Lett. 102, 253902 (2009). [CrossRef] [PubMed]
  20. U. Leonhardt and T. G. Philbin, "Transformation optics and the geometry of light," (2008). ArXiv: 0805.4778.
  21. M. Yan, W. Yan, and M. Qiu, "Cylindrical superlens by a coordinate transformation," Phys. Rev. B 78, 125113 (2008). [CrossRef]
  22. J. B. Pendry, A. J. Holden, D. J. Robbins, and W. J. Stewart, "Magnetism from conductors and enhanced nonlinear phenomena," IEEE Trans. Micro. Theo. Tech. 47, 2075 (2009). [CrossRef]

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