Terahertz metamaterials with semiconductor split-ring resonators for magnetostatic tunability

doi:10.1364/OE.16.014390

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Terahertz metamaterials with semiconductor split-ring resonators for magnetostatic tunability

Jiaguang Han, Akhlesh Lakhtakia, and Cheng-Wei Qiu »View Author Affiliations

Optics Express, Vol. 16, Issue 19, pp. 14390-14396 (2008)
http://dx.doi.org/10.1364/OE.16.014390

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– Abstract
1. Introduction
2. Analysis and numerical results
3. Conclusion
– References and links

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Abstract

We studied a metasurface constituted as a periodic array of semiconductor split-ring resonators. The resonance frequencies of the metasurface excited by normally incident light were found to be continuously tunable in the terahertz regime through an external magnetostatic field of suitable orientation. As such metasurfaces can be assembled into 3D metamaterials, the foregoing conclusion also applies to metamaterials comprising semiconductor split-ring resonators.

1. Introduction

Negatively refracting metamaterials have been a subject of recent enormous interest, in both the physics and the engineering communities, because they possess electromagnetic response characteristics that are not (at least, widely) displayed by natural materials [1

A. Lakhtakia, M. W. McCall, and W. S. Weiglhofer, “Brief overview of recent developments on negative phase-velocity mediums (alias left-handed materials),” AEÜ Int. J. Electron. Commun. 56, 407–410 (2002)..

-3

V. M. Shalaev, “Optical negative-index materials,” Nature Photon. 1, 41–48 (2007). [CrossRef]

]. Generally, these metamaterials are composite materials comprising metallic inclusions of specific shapes and sizes immersed in some homogeneous host medium, and convey the promise of a wide-ranging set of applications.

Metamaterial-based devices could come to include filters, modulators, amplifiers, transistors, resonators, sub-diffraction-limited superlenses, and cloaks [4

Negative Refraction Metamaterials: Fundamental Principles and Applications, G. V. Eleftheriades and K. G. Balmain (Wiley, Hoboken, NJ, USA, 2005).

-7

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]

]. The usefulness of such a device could be extended tremendously if the metamaterial’s response characteristics can be dynamically tuned. Tunability strategies examined thus far are electrical control [8

T. H. Hand and S. A. Cummer, “Frequency tunable electromagnetic metamaterial using ferroelectric loaded split rings,” J. Appl. Phys. 103, 066105 (2008). [CrossRef]

-10

H.-T. Chen, W. J. Padilla, J. M. O. Zide, A. C. Gossard, A. J. Taylor, and R. D. Averitt, “Active terahertz metamaterial devices,” Nature 444, 579–600 (2006). [CrossRef]

], magnetostatic control [11

Y. He, P. He, V. G. Harris, and C. Vittoria, “Role of ferrites in negative index metamaterials,” IEEE Trans. Magn. 42, 2852–2854 (2006). [CrossRef]

,12

L. Kang, Q. Zhao, H. Zhao, and J. Zhou, “Magnetically tunable negative permeability metamaterial composed by split ring resonators and ferrite rods,” Opt. Express 16, 8825–8834 (2008). [CrossRef] [PubMed]

], and optical pumping [13

A. Degiron, J. J. Mock, and D. R. Smith, “Modulating and tuning the response of metamaterials at the unit cell level,” Opt. Express 15, 1115–1127 (2007). [CrossRef] [PubMed]

]. In all of cited publications, the inclusions are split-ring resonators (SRRs) made of some metal. Tunability is introduced by ensuring that another component (e.g., the substrate on which the SRRs are printed or another type of inclusions) is made of an electro-optic material, liquid crystal, ferrite, etc.

In this letter, we suggest a new type of tunable metamaterials. A metamaterial of this type comprises SRRs that are not metallic but, instead, are made of a material whose electromagnetic response properties can be tuned by an external agent. For the sake of illustration, we chose to focus on a tunable, terahertz, metamaterial that is controllable by an externally applied magnetostatic (or quasi-magnetostatic) field.

2. Analysis and numerical results

The essence of the chosen metamaterial is a metasurface [14

M. Lapine and S. A. Tretyakov, “Contemporary notes on metamaterials,” IET Microw. Antennas Propag. 1, 3–11 (2007). [CrossRef]

]: a planar array of semiconductor split-ring resonators (SRRs) periodically printed on an isotropic dielectric substrate. Figure 1(a) shows a single SRR with linear dimensions in the plane ranging from 2 µm to 36 µm, and with a thickness of 200 nm. The SRRs are printed, as shown in Fig. 1(b), on a square lattice of period 60 µm. The SRRs are assumed to be made of a doped semiconductor, such as InAs, whose relative permittivity obeys the Drude model in the absence of an externally applied magnetostatic field [15

E. Burstein and F. De Martini (Pergamon, New York, NY, USA, 1974).

,16

O. Madelung (Springer, Berlin, Germany, 1982).

]. As a typical isotropic dielectric substrate would only slightly shift the resonances but not affect other characteristics significantly [17

C. Rockstuhl, T. Zentgraf, E. Pshenay-Severin, J. Petschulat, A. Chipouline, J. Kuhl, T. Pertsch, H. Giessen, and F. Lederer, “The origin of magnetic polarizability in metamaterials at optical frequencies - an electrodynamic approach,” Opt. Express 15, 8871–8883 (2007). [CrossRef] [PubMed]

], we set its electromagnetic properties to be that of free space (i.e., vacuum) in our numerical work.

Computer simulations of the spectral response of the chosen metasurface were performed using the commercial software CST Microwave Studio TM 2006B, which is a 3D full-wave solver that employs the finite integration technique. The planar SRR array was taken to be entirely surrounded by air and open boundary conditions were employed along the propagation direction. Without the applied magnetostatic field, the doped semiconductor’s relative permittivity scalar ε is given as a function of the angular frequency ω by

ε (ω) = ε_{\infty} - \frac{{ω_{p}}^{2}}{(ω^{2} + i γ ω)},

(1)

where ε _∞ represents the high-frequency value; the plasma frequency

ω_{p} = \sqrt{\frac{N e^{2}}{ε_{0} m^{*}}}

depends on the carrier density N, the effective mass m*, the electronic charge e, and the free-space permittivity ε ₀; and γ is the damping constant. The following parameters were used in our simulations [15

E. Burstein and F. De Martini (Pergamon, New York, NY, USA, 1974).

,16

O. Madelung (Springer, Berlin, Germany, 1982).

]: ε _∞ =16.3, N=1.04×10¹⁷ cm^-3, m*=0.004 m _e , and γ/2π=7.5×10¹¹ Hz, where m _e is the electronic mass.

Fig. 1. (a) A single SRR with dimensions L=36 µm, T=10 µm, D=2 µm and W=6 µm. (b) The chosen metasurface, which is a square array of SRRs printed on a substrate with a period of 60 µm. (c) Transmittance spectrum of the chosen metasurface illuminated normally by a plane wave with electric field oriented perpendicular to the gaps in the SRR. (d) Map of the magnitude of the electric field in an SRR at 1.59 THz. (e) Map of the current density in an SRR at 1.59 THz. (f) The same as (c) but when both gaps are closed in every SRR.

Let the chosen metasurface be oriented parallel the xy plane with the two gaps of every SRR aligned parallel to the x axis. The SRR gaps would resonate if the incident electric field were to be oriented along the y axis (i.e., perpendicular to the two gaps in each SRR).

We calculated the transmittance spectrum of the metasurface when illuminated by a plane wave with its wave vector oriented parallel to the z axis and its electric field oriented parallel to the y axis. The transmittance is the ratio of the power density of the transmitted plane wave to that of the incident plane wave. Figure 1(c) shows that a transmittance dip exists at 1.59 THz frequency. This dip can be attributed to a resonance of the SRRs: as shown in Fig. 1(d), the electric field is concentrated in both gaps of every SRR at this frequency. Figure 1(e) displays the vector plot of the current density at 1.59 THz. If both gaps of every SRR were closed, the transmittance dip at 1.59 THz would disappear, as can be gathered from the transmittance spectrum presented in Fig. 1(f).

In order to obtain a tunable response from the chosen metasurface, we considered the application of an external magnetostatic field B ₀ to affect the resonance in the transmittance spectrum displayed in Fig. 1(c). Generally, without the applied magnetostatic field, the dielectric response of a semiconductor is described by a scalar ε(ω), such as provided in Eq. (1). However, when B ₀ is applied, the scalar ε(ω) has to be replaced by the tensor ε̂(ω).

In the Faraday configuration, B ₀ is aligned parallel to the wave vector of the incident plane wave (i.e., along the z axis). With the assumption that B ₀ is spatially uniform, the nonvanishing components of ε̂( _ω ) are [15

E. Burstein and F. De Martini (Pergamon, New York, NY, USA, 1974).

ε_{xx} = ε_{yy} = ε_{\infty} - \frac{{ω_{p}}^{2} (ω^{2} + i γ ω)}{{(ω^{2} + i γ ω)}^{2} - ω^{2} {ω_{c}}^{2}},

(2)

ε_{xy} = - ε_{yx} = i \frac{ω ω_{c} {ω_{p}}^{2}}{{(ω^{2} + i γ ω)}^{2} - ω^{2} {ω_{c}}^{2}},

(3)

ε_{zz} = ε_{\infty} - \frac{{ω_{p}}^{2}}{(ω^{2} + i γ ω)},

(4)

where ω _c =e B ₀/m* is the cyclotron frequency. The off-diagonal components ε _xy and ε _yx are induced by the magnetostatic field and depend on its magnitude. Figure 2(a) contains the simulated transmittance spectra of the chosen metasurface for different values of the magnitude B ₀ of B ₀. The transmittance dip redshifts gradually from 1.55 to 0.30 THz as B ₀ is increased from 1.0 to 8.0 T, as also illustrated in Fig. 2(b). Although the minimum transmittance increases as B ₀ is increased, Figs. 2(a) and 2(b) clearly indicate that planar arrays of semiconductor SRRs are magnetically tunable in the terahertz regime despite the reduction of the quality factor of the transmittance dip. The reduction of the quality factor and the use of very-high-magnitude magnetostatic fields in the presented results suggest the need to find and/or develop semiconductors that respond more easily to magnetostatic fields.

Fig. 2. Faraday configuration. (a) Transmittance spectra for various values of B ₀, when B ₀ is aligned parallel to the wave vector of the incident plane wave and the electric field of the incident plane wave is aligned perpendicular to the gaps in each SRR. (b) Resonance frequency ω ₀ as a function of B ₀, with the solid line showing the exponential fit ω ₀=α+βexp(-B ₀/χ), where α=0.27, β=2.04, and χ=2.11.

Denoting the resonance angular frequency by ω ₀, we fitted the data in Fig. 2(b) to the formula ω ₀=0.27+2.04 exp(-B ₀/2.11). This formula indicates that the resonance frequency decays exponentially as the applied magnetostatic field increases in magnitude. One way to understand the foregoing trend is as follows. In the Faraday configuration, plane wave propagation in a semiconductor depends on [18

N. Miura, Physics of Semiconductors in High Magnetic Fields (Oxford University Press, Oxford, United Kingdom, 2008).

], i.e.,

ε_{\pm} = ε_{xx} \pm i ε_{xy} = ε_{\infty} - \frac{{ω_{p}}^{2}}{ω^{2} + i γ ω \mp ω ω_{c}}

. Let ñ ² _±=ε _±, where ñ ₊ and ñ- are the complex-valued refractive indexes for right- and left-circularly polarized plane waves. For the linearly polarized electromagnetic wave in our case, the response of substance can be captured by

\tilde{n} = \frac{1}{2} ({\tilde{n}}_{+} + {\tilde{n}}_{-})

for different values of B ₀. As shown in Fig. 3, the real part of ñ decreases as B ₀ increases. So the redshift of ω ₀ with increase of B ₀ can be correlated with the concurrent decrease of ñ.

Fig. 3. Real part of ñ as a function of the linear frequency ω/2π and the magnitude B ₀ of the applied magnetostatic field in the Faraday configuration.

So far we have considered the Faraday configuration. In the Voigt configuration, the magnetostatic field is aligned perpendicular to the wave vector of the incident plane wave. There are two cases, depending on the direction of the incident electric field relative to B ₀. Suppose first that B ₀ is also aligned perpendicular to the electric field of the incident plane wave (i.e., B ₀ is oriented along the x axis). The nonvanishing components of ε̂(ω) now are [15

E. Burstein and F. De Martini (Pergamon, New York, NY, USA, 1974).

]

ε_{yy} = ε_{zz} = ε_{\infty} - \frac{{ω_{p}}^{2} (ω^{2} + i γ ω)}{{(ω^{2} + i γ ω)}^{2} - ω^{2} {ω_{c}}^{2}},

(5)

ω_{yz} = {- ε}_{zy} = i \frac{ω ω_{c} {ω_{p}}^{2}}{{(ω^{2} + i γ ω)}^{2} - ω^{2} {ω_{c}}^{2}},

(6)

ε_{xx} = ε_{\infty} - \frac{{ω_{p}}^{2}}{(ω^{2} + i γ ω)} .

(7)

Figure 4(a) shows that the transmittance spectra in the first Voigt configuration are qualitatively similar to that for the Faraday configuration in Fig. 2(a). The resonance frequency exponentially redshifts as B ₀ increases, and can be fitted to ω ₀=0.27+1.64exp(-B ₀/3.03) ; see Fig. 4(b). Furthermore, in this configuration, the electromagnetic response of the semiconductor is related to ñ _⊥=(ε _yy +ε ² _yz /ε _yy )^1/2. Figure 5 shows that real part of ñ _⊥ decreases with increasing B ₀, which implies the same correlation with the resonance frequency as deduced for the Faraday configuration.

Fig. 4. First Voigt configuration. (a) Transmittance spectra for various values of B ₀, when B ₀ is aligned parallel to the gaps in each SRR and the electric field of the incident plane wave is aligned perpendicular to the gaps in each SRR. (b) Resonance frequency ω ₀ as a function of B ₀, with the solid line showing the exponential fit ω ₀=α+βexp(-B ₀/χ), where α=0.27, β=1.64, and χ=3.03.

Fig. 5. Real part of ñ _⊥ as a function of the linear frequency ω/2π and the magnitude B ₀ of the applied magnetostatic field in the first Voigt configuration.

In the second Voigt configuration, B ₀ is aligned parallel to the electric field of the incident plane wave (i.e., B ₀ is oriented along the y axis), so that the nonvanishing components of ε̂(ω) now are [15

E. Burstein and F. De Martini (Pergamon, New York, NY, USA, 1974).

]

ε_{xx} = ε_{zz} = ε_{\infty} - \frac{{ω_{p}}^{2} (ω^{2} + i γ ω)}{{(ω^{2} + i γ ω)}^{2} - ω^{2} {ω_{c}}^{2}},

(8)

ε_{zx} = {- ε}_{xz} = i \frac{ω ω_{c} {ω_{p}}^{2}}{{(ω^{2} + iγ ω)}^{2} {- ω^{2} ω}_{c}^{2}},

(9)

ε_{yy} = ε_{\infty} - \frac{{ω_{p}}^{2}}{(ω^{2} + iγ ω)} .

(10)

We found that there is no remarkable effect of the applied magnetostatic field on the resonance frequency of the chosen metasurface; furthermore, the electromagnetic response of the semiconductor is related to ñ _∥=ε^1/2 _yy , which does not depend on B ₀.

3. Conclusion

To conclude, our computer simulations have shown that the terahertz resonant response of a metasurface constituted by a planar array of semiconducting split-ring resonators can be tuned by the application of an externally applied magnetostatic field of appropriate orientation and magnitude. As such metasurfaces can be assembled into 3D metamaterials, the foregoing conclusion applies to metamaterials comprising semiconducting SRRs as well. SRRs made of other tunable materials, such as electro-optic materials, could also assist in the realization of tunable terahertz metamaterials.

Acknowledgements

J.H. acknowledges financial support from the MOE Academic Research Fund of Singapore and fruitful discussions with Z. Tian. A.L. thanks the Department of Physics, IIT Kanpur for its hospitality. C.W.Q. thanks Singapore-France Merlion project for financial support.

References

1.	A. Lakhtakia, M. W. McCall, and W. S. Weiglhofer, “Brief overview of recent developments on negative phase-velocity mediums (alias left-handed materials),” AEÜ Int. J. Electron. Commun. 56, 407–410 (2002)..
2.	S. A. Ramakrishna, “Physics of negative refractive index materials,” Rep. Prog. Phys. 68, 449–521 (2005). [CrossRef]
3.	V. M. Shalaev, “Optical negative-index materials,” Nature Photon. 1, 41–48 (2007). [CrossRef]
4.	Negative Refraction Metamaterials: Fundamental Principles and Applications, G. V. Eleftheriades and K. G. Balmain (Wiley, Hoboken, NJ, USA, 2005).
5.	C. Caloz and T. Itoh, Electromagnetic Metamaterials: Transmission Line Theory and Microwave Applications (Wiley, Hoboken, NJ, USA, 2006).
6.	Z. Liu, H. Lee, Y. Xiong, C. Sun, and X. Zhang, “Far-field optical hyperlens magnifying sub-diffraction-limited objects,” Science 315, 1686 (2007). [CrossRef] [PubMed]
7.	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]
8.	T. H. Hand and S. A. Cummer, “Frequency tunable electromagnetic metamaterial using ferroelectric loaded split rings,” J. Appl. Phys. 103, 066105 (2008). [CrossRef]
9.	Q. Zhao, L. Kang, B. Du, B. Li, J. Zhou, H. Tang, X. Liang, and B. Zhang, “Electrically tunable negative permeability metamaterials based on nematic liquid crystals,” Appl. Phys. Lett. 90, 011112 (2007). [CrossRef]
10.	H.-T. Chen, W. J. Padilla, J. M. O. Zide, A. C. Gossard, A. J. Taylor, and R. D. Averitt, “Active terahertz metamaterial devices,” Nature 444, 579–600 (2006). [CrossRef]
11.	Y. He, P. He, V. G. Harris, and C. Vittoria, “Role of ferrites in negative index metamaterials,” IEEE Trans. Magn. 42, 2852–2854 (2006). [CrossRef]
12.	L. Kang, Q. Zhao, H. Zhao, and J. Zhou, “Magnetically tunable negative permeability metamaterial composed by split ring resonators and ferrite rods,” Opt. Express 16, 8825–8834 (2008). [CrossRef] [PubMed]
13.	A. Degiron, J. J. Mock, and D. R. Smith, “Modulating and tuning the response of metamaterials at the unit cell level,” Opt. Express 15, 1115–1127 (2007). [CrossRef] [PubMed]
14.	M. Lapine and S. A. Tretyakov, “Contemporary notes on metamaterials,” IET Microw. Antennas Propag. 1, 3–11 (2007). [CrossRef]
15.	E. Burstein and F. De Martini (Pergamon, New York, NY, USA, 1974).
16.	O. Madelung (Springer, Berlin, Germany, 1982).
17.	C. Rockstuhl, T. Zentgraf, E. Pshenay-Severin, J. Petschulat, A. Chipouline, J. Kuhl, T. Pertsch, H. Giessen, and F. Lederer, “The origin of magnetic polarizability in metamaterials at optical frequencies - an electrodynamic approach,” Opt. Express 15, 8871–8883 (2007). [CrossRef] [PubMed]
18.	N. Miura, Physics of Semiconductors in High Magnetic Fields (Oxford University Press, Oxford, United Kingdom, 2008).

OCIS Codes
(120.7000) Instrumentation, measurement, and metrology : Transmission
(160.1190) Materials : Anisotropic optical materials
(160.6000) Materials : Semiconductor materials
(260.5740) Physical optics : Resonance

ToC Category:
Metamaterials

History
Original Manuscript: July 16, 2008
Revised Manuscript: August 20, 2008
Manuscript Accepted: August 22, 2008
Published: August 29, 2008

Citation
Jiaguang Han, Akhlesh Lakhtakia, and Cheng-Wei Qiu, "Terahertz metamaterials with semiconductor split-ring resonators for magnetostatic tunability," Opt. Express 16, 14390-14396 (2008)
http://www.opticsinfobase.org/oe/abstract.cfm?URI=oe-16-19-14390

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References

A. Lakhtakia, M. W. McCall and W. S. Weiglhofer, "Brief overview of recent developments on negative phase-velocity mediums (alias left-handed materials)," AE?? Int.J. Electron. Commun. 56, 407-410 (2002).
S. A. Ramakrishna, "Physics of negative refractive index materials," Rep. Prog. Phys. 68, 449-521 (2005). [CrossRef]
V. M. Shalaev, "Optical negative-index materials," Nature Photon. 1, 41-48 (2007). [CrossRef]
Negative Refraction Metamaterials: Fundamental Principles and Applications, edited by G. V. Eleftheriades and K. G. Balmain (Wiley, Hoboken, NJ, USA, 2005).
C. Caloz and T. Itoh, Electromagnetic Metamaterials: Transmission Line Theory and Microwave Applications (Wiley, Hoboken, NJ, USA, 2006).
Z. Liu, H. Lee, Y. Xiong, C. Sun, and X. Zhang, "Far-field optical hyperlens magnifying sub-diffraction-limited objects," Science 315, 1686 (2007). [CrossRef] [PubMed]
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]
T. H. Hand and S. A. Cummer, "Frequency tunable electromagnetic metamaterial using ferroelectric loaded split rings," J. Appl. Phys. 103, 066105 (2008). [CrossRef]
Q. Zhao, L. Kang, B. Du, B. Li, J. Zhou, H. Tang, X. Liang, and B. Zhang, "Electrically tunable negative permeability metamaterials based on nematic liquid crystals," Appl. Phys. Lett. 90, 011112 (2007). [CrossRef]
H.-T. Chen, W. J. Padilla, J. M. O. Zide, A. C. Gossard, A. J. Taylor, and R. D. Averitt, "Active terahertz metamaterial devices," Nature 444, 579-600 (2006). [CrossRef]
Y. He, P. He, V. G. Harris, and C. Vittoria, "Role of ferrites in negative index metamaterials," IEEE Trans. Magn. 42, 2852-2854 (2006). [CrossRef]
L. Kang, Q. Zhao, H. Zhao, and J. Zhou, "Magnetically tunable negative permeability metamaterial composed by split ring resonators and ferrite rods," Opt. Express 16, 8825-8834 (2008). [CrossRef] [PubMed]
A. Degiron, J. J. Mock, and D. R. Smith, "Modulating and tuning the response of metamaterials at the unit cell level," Opt. Express 15, 1115-1127 (2007). [CrossRef] [PubMed]
M. Lapine and S. A. Tretyakov, "Contemporary notes on metamaterials," IET Microw. Antennas Propag. 1, 3-11 (2007). [CrossRef]
Polaritons: Proceedings of the First Taormina Research Conference on the Structure of Matter, edited by E. Burstein and F. De Martini (Pergamon, New York, NY, USA, 1974).
Semiconductors: Physics of Group IV Elements and III-V Compounds, edited by O. Madelung (Springer, Berlin, Germany, 1982).
C. Rockstuhl, T. Zentgraf, E. Pshenay-Severin, J. Petschulat, A. Chipouline, J. Kuhl, T. Pertsch, H. Giessen, and F. Lederer, "The origin of magnetic polarizability in metamaterials at optical frequencies - an electrodynamic approach," Opt. Express 15, 8871-8883 (2007). [CrossRef] [PubMed]
N. Miura, Physics of Semiconductors in High Magnetic Fields (Oxford University Press, Oxford, United Kingdom, 2008).

Appl. Phys. Lett.

Q. Zhao, L. Kang, B. Du, B. Li, J. Zhou, H. Tang, X. Liang, and B. Zhang, "Electrically tunable negative permeability metamaterials based on nematic liquid crystals," Appl. Phys. Lett. 90, 011112 (2007). [CrossRef]

IEEE Trans. Magn.

Y. He, P. He, V. G. Harris, and C. Vittoria, "Role of ferrites in negative index metamaterials," IEEE Trans. Magn. 42, 2852-2854 (2006). [CrossRef]

IET Microw. Antennas Propag.

M. Lapine and S. A. Tretyakov, "Contemporary notes on metamaterials," IET Microw. Antennas Propag. 1, 3-11 (2007). [CrossRef]

J. Appl. Phys.

T. H. Hand and S. A. Cummer, "Frequency tunable electromagnetic metamaterial using ferroelectric loaded split rings," J. Appl. Phys. 103, 066105 (2008). [CrossRef]

J. Electron. Commun.

A. Lakhtakia, M. W. McCall and W. S. Weiglhofer, "Brief overview of recent developments on negative phase-velocity mediums (alias left-handed materials)," AE?? Int.J. Electron. Commun. 56, 407-410 (2002).

Nature

H.-T. Chen, W. J. Padilla, J. M. O. Zide, A. C. Gossard, A. J. Taylor, and R. D. Averitt, "Active terahertz metamaterial devices," Nature 444, 579-600 (2006). [CrossRef]

Nature Photon.

V. M. Shalaev, "Optical negative-index materials," Nature Photon. 1, 41-48 (2007). [CrossRef]

Opt. Express

Rep. Prog. Phys.

S. A. Ramakrishna, "Physics of negative refractive index materials," Rep. Prog. Phys. 68, 449-521 (2005). [CrossRef]

Science

Z. Liu, H. Lee, Y. Xiong, C. Sun, and X. Zhang, "Far-field optical hyperlens magnifying sub-diffraction-limited objects," Science 315, 1686 (2007). [CrossRef] [PubMed]
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]

Other

Negative Refraction Metamaterials: Fundamental Principles and Applications, edited by G. V. Eleftheriades and K. G. Balmain (Wiley, Hoboken, NJ, USA, 2005).
C. Caloz and T. Itoh, Electromagnetic Metamaterials: Transmission Line Theory and Microwave Applications (Wiley, Hoboken, NJ, USA, 2006).
Polaritons: Proceedings of the First Taormina Research Conference on the Structure of Matter, edited by E. Burstein and F. De Martini (Pergamon, New York, NY, USA, 1974).
Semiconductors: Physics of Group IV Elements and III-V Compounds, edited by O. Madelung (Springer, Berlin, Germany, 1982).
N. Miura, Physics of Semiconductors in High Magnetic Fields (Oxford University Press, Oxford, United Kingdom, 2008).

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