Abstract
Invisibility cloaks, which used to be confined to the realm of fiction, have now been turned into a scientific reality thanks to the enabling theoretical tools of transformation optics and conformal mapping. Inspired by those theoretical works, the experimental realization of electromagnetic invisibility cloaks has been reported at various electromagnetic frequencies. All the invisibility cloaks demonstrated thus far, however, have relied on nano or microfabricated artificial composite materials with spatially varying electromagnetic properties, which limit the size of the cloaked region to a few wavelengths. Here, we report the first realization of a macroscopic volumetric invisibility cloak constructed from natural birefringent crystals. The cloak operates at visible frequencies and is capable of hiding, for a specific light polarization, threedimensional objects of the scale of centimetres and millimetres. Our work opens avenues for future applications with macroscopic cloaking devices.
Introduction
The pioneering theoretical works of Pendry and Leonhardt^{1,2}, fulfilling 'invisibility cloaking', have inspired researchers around the world and have motivated many significant achievements^{3,4,5,6,7,8,9,10,11,12,13,14,15,16}, including the demonstration of invisibility cloaks at microwave^{3,4,5,6,7}, terahertz^{8} and optical frequencies^{9,10,11,12}. The invisibilitycloak design is enabled by transformation optics, using a coordinate transformation of the governing Maxwell's equations^{17,18}. Such invariant transformations map a particular region in free space to a spatial domain, usually with positiondependent and anisotropic optical parameters. Notably, in 2003, Greenleaf et al.^{19} showed that a region in space could be rendered undetectable by electrical impedance tomography through invariant transformation of the Poisson's equation that describes the electrostatic potential.
Although the initial proposal for an invisibility cloak involves extreme values of material properties that normally require resonant structures leading to narrowband operation^{1,3}, a special type of cloaking scheme, the socalled 'carpet cloak', circumvents this issue by transforming a bulging reflecting surface into a flat one, hiding anything that is underneath the bulging surface from outside observers^{15}. This carpetcloaking scheme has enabled the experimental realization of cloaks at microwave, terahertz and even optical frequencies^{4,7,8,9,10,12}. These demonstrations prove that broadband invisibility can be accomplished with realistic material properties. However, most of the invisibility cloaks demonstrated so far rely on spatially varying index profiles, which, in the optical regime, usually require nanofabrication processes (such as focus ion beam, electronbeam lithography and direct laser writing) to accurately define the patterns on the nanometre scale^{9,10,12}. These timeconsuming nanofabrication processes limit the size of the overall cloaked region to a few wavelengths.
In this article, we report the first demonstration of a macroscopic volumetric cloaking device operating at visible frequencies, which can conceal objects of sizes of at least 3 orders of magnitude larger than the wavelength of light in all three dimensions, and works for a specific polarization of the incident light. The cloaking design uses birefringence in a natural crystal calcite, thus eliminating the necessity of timeconsuming nanofabrication processes and enabling the realization of cloaking at macroscopic scales. The cloaking effect was directly observed for red and green laser beams and incoherent white light without resorting to use of a microscope. The demonstration of a macroscopic invisibilitycloak paves the way for future applications of invisibility cloaking.
Results
Design and ray tracing study of the optical cloak
The cloak is based on a recent theoretical work^{20} that indicates that a carpet cloak can be achieved with spatially homogeneous anisotropic dielectric materials. A schematic of the triangular cloaking design is shown in Figure 1, where a virtual space with a triangular crosssection of height H_{2} and filled with an isotropic material of permittivity ɛ and μ (μ=1; blue region in Fig. 1a) is mapped to a quadrilateral region in the physical space with anisotropic electromagnetic properties ɛ′ and μ′ (brown region in Fig. 1b). Thus, the cloaked region is defined by the small grey triangle of height H_{1} and halfwidth d. Mathematically, the transformation is defined by where (x′, y′, z′) and (x, y, z) correspond to the coordinates of the physical space and virtual space, respectively. Applying this coordinate transformation to Maxwell's equations, we obtain the corresponding electromagnetic parameters of the quadrilateral cloaking region: where
It is worth noticing from equations (2) and (3) that materials with spatially invariant optical properties can fulfil the requirement for this triangular cloak, in contrast to all other cloaks demonstrated to date. An ideal cloak requires both the electric permittivity and magnetic permeability to be anisotropic. On the other hand, it has been shown that a reduced cloaking scheme, namely one that works for a specific polarization, can eliminate the necessity to engineer both the permittivity and permeability^{3,13}. Specifically, considering the case where light with transversemagnetic (TM)field polarization is incident in the x–y plane, the relevant optical parameters would be ɛ_{x−y} (tensor of permittivity in the x−y plane) and μ_{z}, and as far as the trajectory of the light is concerned, the electromagnetic parameters can be simplified as (see Methods for the derivation)
Thus, the reduced cloaking design described by equations (4) and (5) can be realized using natural anisotropic materials (such as calcite and calomel), which are readily available in macroscopic sizes.
Here, the macroscopic invisibility cloak is designed using two calcite prisms glued together with the protruding bottom surface of the cloak serving as a deformed mirror, as shown in Figure 1c. Calcite is a uniaxial birefringent crystal with refractive indices of ordinary (n_{o}) and extraordinary light (n_{e}) of ∼1.66 and 1.49, respectively, at a wavelength of 590 nm. To meet the transformation requirement described by equation (4), the optical axis of calcite prisms forms an angle γ with the y axis, and the relation between the geometrical parameters of the cloak, the optical axis orientation γ and the permittivity of the virtual space, ɛ, is given as follows: In the specific design shown in Figure 1c, γ=30°, the geometrical parameters are calculated using equations (6) and (7) and are indicated in Figure 1c. The cloaked region has a triangular crosssection formed by the two bottom facets, each forming an angle of about 5° with the x–z plane. The minimum dimension of the cloaked region—the height of the triangle—is close to 1.2 mm, which is more than three orders of magnitude larger than the wavelengths at visible frequencies. The refractive index of the virtual space is 1.532 by equation (8), indicating that the cloak will cause no deflection or translation of light if it is placed on a reflective ground plane and immersed in an optical medium with the same refractive index.
A raytracing calculation was performed to verify the design described above. As shown in Figure 2a and b, beams with TM polarization incident at two different angles are both reflected without distortion, numerically verifying the cloaking design given by equations (6–8). On the other hand, for transverse electric (TE) polarization (which does not exhibit a cloaking effect), the light is reflected into different directions by the two bottom facets, leading to significant splitting, which can be observed in the far field (Fig. 2c,d).
Characterization of the optical cloak
To demonstrate the performance of the cloak in the visible range, we first characterized the calcite cloak in air using a green laser at wavelength of 532 nm (Fig. 3a, left). Even without a metal film covering the bottom surface of the cloak, light experiences total internal reflection for a large range of incident angles. To better visualize the effect of the cloaking, a mask with an arrow pattern was placed in front of the laser head such that the emitted laser beam contains the same pattern (Fig. 3a, right), which can be used to characterize the distortion of the beam after being reflected by the triangular bump covered by the cloak. In addition, the laser beam goes through a linear polarizer that controls the polarization of the beam to be either TE or TM; here, the TE polarization serves as the control sample that shows the results without the cloaking effect. The reflected beam is projected on a screen ∼18 cm away from the prism, and the projected image is captured by a camera. As a reference, the image of the laser beam reflected by a flat mirror was shown in Figure 3b, which contained a horizontally flipped arrow pattern.
Because the bottom surface of the cloak consists of two flat facets forming an angle about 10°, the reflection from the bottom bulging surface would split the laser beam into two for the TE polarized beam, which does not experience the cloaking effect, forming an angle of 20° inside the prism and >30° outside the prism. This effect is clearly observed on the image projected on the screen for the green laser beam, as shown in Figure 3c.
On the other hand, with TM polarization, the reflected beam projected on the screen shows no splitting at all (Fig. 3d), in stark contrast to the case with TE polarization. Although the cloak is designed for a wavelength of 590 nm, because of the latitude in manufacturing the prisms, the geometric parameters slightly deviate from the design. This effect leads to an almost perfect cloaking at λ=532 nm (green light) instead. A small dark stripe appears in the centre of the pattern due to the imperfection in the alignment of the two calcite crystals, resulting in scattering at the apex of the triangular cloaked region. An invisibility cloak should hide objects at all incident angles. This cloaking effect is confirmed by the measurements at three different incident angles (39.5°, 64.5°, 88°) with mixed TE and TM polarizations, as shown in Figure 3e–g, in which the central image corresponds to the TM polarization and the two projected arrow segments images far from the centre correspond to the TE polarization. The projected images of the TMpolarized beam at all incident angles show no distortion of the pattern, serving as direct evidence that the calcite cloak transforms the protruding bottom surface into a flat mirror.
We next demonstrate the performance of the cloak for red light using a laser that emits light at wavelengths ranging from 630 to 680 nm with a spectral peak at λ=650 nm. As shown in Figure 3h, there is a small gap in the central image (TM polarization). This gap can be attributed to the optical dispersion of calcite crystal, such that the cloaking condition is not rigorously fulfilled at these wavelengths. Consequently, the pattern is slightly different from that reflected from a flat surface (Fig. 3i). Nonetheless, in comparison with the large separation between the two segmented images of the uncloaked TE polarization, the gap size (2 mm) of the TM polarization is about two orders of magnitude less. To an outside observer, this difference corresponds to a virtual reflective surface consisting of two facets, each forming an angle of only around 0.1° with the horizontal (x–z) plane. This result, together with that of green light, indicates that the cloak covers at least a 100 nm bandwidth at visible frequencies.
The broadband operation of the macroscopic calcite cloak is further supported by the imaging of whitecoloured alphabetic letters (from A to Z, flipped horizontally) printed on a sheet of black paper reflected by the cloak system. A schematic of the measurement is shown in Figure 4a. Note that the bottom surface is now coated with Ti (2 nm)/Ag (200 nm)/Au (50 nm) to reflect light for all incident angles. With TE polarization (Fig. 4b), because of the large splitting caused by the mirror deformation, the image collected by the camera consists of letters from two largely separated locations ('C', 'D', 'R' to 'U'). On the other hand, switching the polarization to TM leads to imaging of five consecutive letters from the same location (from 'H' to 'L'), as if the bottom surface of the cloak were flat (Fig. 4c). The overall cloaking effect is striking, notwithstanding the presence of a rainbow at the edge of the letters arising from the dispersion of calcite crystal. Because white light covers the whole visible spectrum, this finding unambiguously demonstrates the broadband operation of our calcite cloak.
Dispersion effect on optical cloak
The dispersion of calcite has a slight effect on the cloaking performance, which was shown by the measurement with red laser beam in Figure 3h and the rainbow edge effect in Figure 4c. A ray tracing calculation was carried out to quantitatively analyse the influence of calcite dispersion on the cloaking performance. A beam with TM polarization, once reflected by the cloak, is generally split into two except at the wavelength where the cloaking condition is rigorously satisfied. The two reflected beams deviate from that reflected by a horizontal flat mirror by an angle of φ_{1} and φ_{2}, respectively, and the angle formed by the two beams is φ_{1}–φ_{2}. Figure 5a shows the ray tracing results for a cloak with the design parameters indicated in Figure 1c and an incident angle θ=64.5°. The cloak works perfectly at the design wavelength close to 590 nm, which is confirmed by the raytracing calculation. The deviation angles φ_{1}, φ_{2} of the reflected beams are <1° across the visible range from 400 to 700 nm.
Because of the fabrication latitude, the cloaking condition was shifted to 532 nm, as shown by the measurements with green laser beam. Therefore, a direct comparison between the ray tracing calculation using the design parameters and the experimental observation would not be meaningful. Instead, we slightly modified the geometry of the cloak in the ray tracing to match the experimental observation of perfect cloaking at 532 nm, with the results given in Figure 5b. At λ=650 nm, the splitting angle formed by the two beams is φ_{1}–φ_{2}=0.68°, which is consistent with our experimental observation for the red laser beam, namely, a separation of 2 mm on a screen 18 cm away from the prism, corresponding to a splitting angle of 0.64°.
It is interesting to note from Figure 4 that the rainbow effect for TE polarization is much less than that for TM polarization. The raytracing calculation verifies that the dispersion effect for TE is two orders of magnitude less than TM (Figure 5c), which is consistent with our experimental observations.
Splitting angles for TE polarization
As an incident beam with TE polarization does not experience cloaking effect, significant splitting has been observed as shown in Figure 3e–g at various incident angles. The angles of the split images for TE polarization are calculated with a simple raytracing analysis (see Methods), and found to be consistent with the experimental observations (Fig. 6). The angle of deviation for each TE polarized reflected beam is above 17° at all incident angles, and the angle formed between them is over 34°.
Discussion
An interesting question is whether any reflection exists at the interface between the two constituent calcite crystals with different orientations of the optical axis. It has been shown by Zhang et al.^{21} that for two contacting anisotropic crystals with their optical axis symmetric about the interface (as in our cloaking configuration), there is indeed no reflection at the interface regardless of the direction of light. On the other hand, because we have adopted a reduced form of cloaking design (equations (4,5)), a small impedance mismatch is introduced between the surrounding optical medium and the cloak, which results in a small amount of reflection at their interface. Nonetheless, this reflection can be eliminated if the interface is nanostructured in such a way that the permittivity undergoes an adiabatic transition from the calcite crystal and the surrounding medium, and the cloak itself would become completely invisible^{22,23,24}.
In summary, we have demonstrated the first macroscopic cloak operating at visible frequencies, which transforms a deformed mirror into a flat one from all viewing angles. The cloak is capable of hiding threedimensional objects three to four orders of magnitudes larger than optical wavelengths, and therefore, it satisfies a layman's definition of an invisibility cloak: namely, the cloaking effect can be directly observed without the help of microscopes. Because our work solves several major issues typically associated with cloaking: size, bandwidth, loss^{25,26} and image distortion^{27}, it paves the way for future practical cloaking devices.
Methods
Derivation of cloaking design of reduced form
We first write down Maxwell's equations: where the permittivity ɛ and permeability μ are tensors for anisotropic media. For TM waves, the nonzero fields are E_{x}, E_{y} and H_{z}, and therefore, Maxwell's equation can simply be written as where
Taking a derivative of equation (12) with respect to time and plugging in equation (11), we have It follows from equation (13) that the only material parameter that controls the flow of light with TM polarization in the medium is μ_{z}ɛ_{x–y}, which, in the ideal cloaking condition (equations (2,3)), is given by
In the case of nonmagnetic cloaking design (permeability is set to unity), the permittivity tensor is given exactly by the above expression, which amounts to equations (4) and (5).
Dispersion of calcite crystal
In the ray tracing calculation, the ordinary and extraordinary refractive indices of calcite are given by the Sellmeier equations as n_{o}^{2}=2.69705+0.0192064/(λ^{2}–0.01820)–0.0151624λ^{2} and n_{e}^{2}=2.18438+0.0087309/(λ^{2}–0.01018)–0.0024411λ^{2}.
Ray tracing for TE polarization
The ray tracing for TE polarization is illustrated in Figure 6a. A beam with TE polarization is incident from air to the calcite cloak at an angle of θ with respect to the vertical direction, and α–θ with respect to the surface normal of the prism interface. The refraction angle β is given as sinβ=sin (α−θ)/n_{0} where n_{0} is the index for ordinary light (or TE polarization in the cloaking configuration). Inside the cloak, the TE beam is reflected by the protruding bottom surface into two beams, which are incident onto the second interface at incident angles of 2 δ−β and 2 δ+β. The refraction angles γ_{1} and γ_{2} are thus given as arcsin[n_{0}sin(2δ−β)] and arcsin[n_{0} sin(2δ+β)], respectively. Consequently, the angles of deviation, which are formed between the split TE beams, and a beam reflected by a horizontal flat surface (dashed arrows in Fig. 6a) are: φ_{1}=γ_{1}+α−θ, φ_{2}=γ_{1}+−α+θ.
Additional information
How to cite this article: Chen X. et al. Macroscopic invisibility cloaking of visible light. Nat. Commun. 2:176 doi: 10.1038/ncomms1176 (2011).
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Acknowledgements
We thank J.M.F. Gunn for insightful discussions and a critical reading of the manuscript. This work was supported by the University of Birmingham, HEFCE, EPS and the EU project PHOME (Contract No. 213390). Y.L. acknowledges the financial support of the 'Lee Family Scholarship' from Imperial College London.
Author information
Affiliations
School of Physics and Astronomy, University of Birmingham, Birmingham B15 2TT, UK.
 Xianzhong Chen
 & Shuang Zhang
Department of Physics, Blackett Laboratory, Imperial College London, London SW7 2AZ, UK.
 Yu Luo
 & John B. Pendry
DTU Fotonik—Department of Photonics Engineering, Technical University of Denmark, Kongens Lyngby DK2800, Denmark.
 Jingjing Zhang
School of Mechanical Engineering, University of Birmingham, Birmingham B15 2TT, UK.
 Kyle Jiang
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Contributions
X.Z.C., S.Z. and K.J. designed and conducted the experiments. S.Z., Y.L., J.J.Z. and J.B.P. initiated the project and designed the cloak. Y.L. and J.J.Z. performed the ray tracing calculation. S.Z. supervized the project and prepared the manuscript. All authors contributed to the editing of the manuscript.
Competing interests
The authors declare no competing financial interests.
Corresponding author
Correspondence to Shuang Zhang.
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