The present disclosure is directed generally to omniresonant broadband coherent perfect absorption of incoherent light over large bandwidths in optical apparatus or systems and, more particularly, to systems and methods for obtaining achromatic optical absorption (omniresonance spanning greater than 50 nm, continuous coherent perfect absorption).
Coherent perfect absorption (CPA) refers to completely absorbing light in a partial absorber placed in a devised medium. The essence of this concept is maximizing the interaction of an incoming optical field and the absorber by engineering the electromagnetic field distribution. Since such an interaction takes place via interference, CPA is a resonant phenomenon that occurs only at discrete wavelengths. CPA was initially proposed and realized by placing a symmetric 1D absorbing layer in the standing wave of two counterpropagating beams. In this two-sided-incidence configuration, CPA is observed at discrete wavelengths upon satisfaction of a phase relation between the two beams. Asymmetric planar cavities were proposed and realized to demonstrate CPA under one-sided-incidence configurations. Such cavities consist of a perfect back-mirror R2=1, and a front-mirror with a reflectivity R1=(1−)2, with being the single-pass absorption of the lossy material.
CPA is applicable to any absorbing medium since it is agnostic about the nature of the absorber. However, it suffers from two major constraints that severely limit the potential applications: (1) CPA is a resonant effect and hence occurs only at a limited linewidth around resonant wavelengths; and (2) since the intrinsic absorption of a material is wavelength-dependent, CPA occurs within a narrow bandwidth where the material's absorption and the Fresnel reflections meet the CPA requirement (i.e., a 3-nm bandwidth has been reported). The latter issue is resolved by devising mirrors that counterbalance the variations in the material's intrinsic absorption, R1(λ)=(1−(λ))2.
However, the issue of narrow absorption linewidth has so far remained unsolved, which hinders CPA for efficiently capturing optical energy. For example, CPA in graphene has been reported in various configurations such as attenuated total internal reflection (ATR), Salisbury screen, two-beam illumination, single-beam illumination, and guided-mode resonance coupling, but the demonstrations are made at discrete wavelengths with a limited linewidth, and efforts for broadening the absorption linewidths are lacking a clear strategy. For a solar cell, a device needs to absorb the incoming light continuously across a broad range of wavelengths. Therefore, there is a need for a system and method of CPA of incoherent light over large bandwidths.
Further, optical-cavity resonances occupy narrow spectral linewidths that are inversely proportional to the cavity-photon lifetime, which are separated by a free spectral range (FSR) that is inversely proportional to the cavity size. Although cavity-quantum electrodynamics requires narrow cavity linewidths to isolating the interaction of optical fields with the resonances of atoms, ions, or nanostructures, most applications would benefit from maintaining the resonant cavity field buildup over an extended bandwidth. Examples of such applications include coherent perfect absorption (CPA) in media endowed with low intrinsic losses and boosting nonlinear optical effects. Although CPA, for instance, can increase absorption to 100% in a thin low-loss layer on resonance, exploiting CPA in harvesting solar radiation would require an optical cavity in which an extended bandwidth satisfies the resonance condition.
The quest for producing an achromatic resonator has precedents. In “white-light cavities,” the cavity itself is modified by inserting a new material or structure endowed with strong negative (anomalous) dispersion to equalize the cavity optical length for all wavelengths. Only macroscopic white-light cavities have been explored to date via cavity-filling atomic species featuring bifrequency Raman gain in a double-Λ system or displaying electromagnetically induced transparency, or alternatively via nonlinear Brillouin scattering. In all such studies, the enhanced cavity linewidths are extremely narrow (˜100 MHz or <1-pm-wide) by virtue of the very nature of the atomic or nonlinear resonances utilized, and are limited by uncompensated higher-order dispersion terms. Alternative approaches based on the use of linear optical components, such as appropriately designed chirped cavity mirrors or grating pairs, have been investigated. Surprisingly, both of these possibilities fail at producing a white-light cavity due to subtle overlooked aspects in the constraints imposed by causality on non-dissipative systems. Therefore there is a need for system and method for achromatic transmission through a white-light cavity.
The present disclosure is directed to systems and methods for obtaining achromatic optical absorption.
According to one aspect, the present invention is an omniresonant broadband coherent perfect absorption (CPA) apparatus. The omniresonant broadband CPA apparatus includes a light diffracting component, a lens L1, and an omniresonant optical cavity, disposed along an optical axis. The omniresonant optical cavity is disposed tilted at an angle, ψ, with respect to the optical axis and an angle γ(λ) is a diffraction angle of a white-light input to the diffraction component with respect to a light diffracting component normal. γ(λ)−γo is the angle that any wavelength λ makes with respect to the optical axis and a central wavelength λc is diffracted at γo=γ(λc=550 nm) and coincides with the optical axis. In addition, the incidence angle made by the wavelength λ after the lens with respect to the optical axis is
where d1 and d2 are the distances from the light diffracting component to the lens L1 and from the lens L1 to the cavity, respectively, such that the condition θ(λ)=φ(λ)+ψ is satisfied.
According to another aspect, the present invention is a method for omniresonant transmission, comprising the steps of: (i) providing an omniresonant broadband apparatus having a light diffracting component, a lens L1, and an omniresonant optical cavity, disposed along an optical axis, wherein the omniresonant optical cavity is disposed tilted at an angle, ψ, with respect to the optical axis; (ii) inputting a white-light input to the diffraction component with respect to a light diffracting component normal having a diffraction angle γ(λ); wherein γ(λ)−γo is the angle that any wavelength λ makes with respect to the optical axis, and (iii) diffracting a central wavelength λc at γo=γ(λ
where d1 and d2 are the distances from the light diffracting component to the lens L1 and from the lens L1 to the cavity, respectively, such that the condition θ(λ)=φ(λ)+ψ is satisfied.
It should be appreciated that all combinations of the foregoing concepts and additional concepts discussed in greater detail below (provided such concepts are not mutually inconsistent) are contemplated as being part of the inventive subject matter disclosed herein. In particular, all combinations of claimed subject matter appearing at the end of this disclosure are contemplated as being part of the inventive subject matter disclosed herein. It should also be appreciated that terminology explicitly employed herein that also may appear in any disclosure incorporated by reference should be accorded a meaning most consistent with the particular concepts disclosed herein.
These and other aspects of the invention will be apparent from and elucidated with reference to the embodiment(s) described hereinafter.
One or more aspects of the present invention are particularly pointed out and distinctly claimed as examples in the claims at the conclusion of the specification. The foregoing and other objects, features, and advantages of the invention are apparent from the following description taken in conjunction with the accompanying drawings in which:
Aspects of the present invention and certain features, advantages, and details thereof, are explained more fully below with reference to the non-limiting examples illustrated in the accompanying drawings. Descriptions of well-known structures are omitted so as not to unnecessarily obscure the invention in detail. It should be understood, however, that the detailed description and the specific non-limiting examples, while indicating aspects of the invention, are given by way of illustration only, and are not by way of limitation. Various substitutions, modifications, additions, and/or arrangements, within the spirit and/or scope of the underlying inventive concepts will be apparent to those skilled in the art from this disclosure.
The underlying physics for realization of a broadband CPA is the concept of omniresonance in a lossless cavity, as discussed above and shown in
By embedding a weak absorber inside the cavity and properly choosing the front mirror design, the cavity exhibits perfect absorption, but only at discrete resonant wavelengths (
For an angled incidence, the resonant wavelengths are determined by satisfaction of the following condition on the round-trip phase φ:
where λ is the free-space wavelength, θ is the angle of incidence inside the cavity corresponding to an external incidence angle θ through Snell's law, n and d are the refractive index and the thickness of the cavity layer, respectively, integer m is the resonant-mode order, and α1 and α2 are the reflection phases from the cavity mirrors. Since only axial components of wave-vectors contribute to the phase, it is possible to impose a condition on θ for any given λ, such that all wavelengths satisfy the resonance condition:
Upon satisfaction of the resonant condition for all wavelengths—which is a necessary CPA condition—broadband perfect absorption is achieved (
A nonlimiting embodiment of the present invention utilizes a graphene cavity that continuously absorbs visible light across a ˜100-nm bandwidth. The concept of the CPA with an omniresonance configuration that used for omniresonant transmission is used in a CPA cavity. An omniresonant cavity refers to a cavity configuration for which the incident angle is correlated to wavelength components of the incoming beam, such that all the wavelengths become resonating within the cavity. Consequently, if an absorber is placed inside this cavity with properly devised mirror reflectivities, CPA is satisfied for all wavelengths, thus the beam is absorbed in a broad bandwidth (i.e., achromatic).
For a graphene monolayer, which is an exemplary absorbing material, the single-pass absorption spectrum is flat within a somewhat broad range (
The schematic of the full CPA cavity is shown in
Turning now to
Since the light diffracted by the grating is spread horizontally, transversal displacements of optical components can spectrally shift the resonances. Therefore, to ensure a proper optical alignment and getting the desired spectral range, the central wavelength of λc=550 nm is defined as the optical axis which passes through the center of the lenses L1 and L2. The cavity is then mounted on the rotational stage at the focal point of the lens. Although axial displacement of the resonator does not affect the resonances, it can alter the angular distribution of the beam after L1, a feature we use to fine-tune the bandwidth of the resonances. The reflected beam at any given cavity tilt angle is collected with a third lens with a focal length of 5-cm and then is captured in a CCD sensor with 5-μm pixel size. To assign pixels at the CCD to a wavelengths, a tunable narrowband filter (≈3-nm) is used right after each reflection measurement, and it is assumed the variation of wavelength on the CCD is linear. The role of the CCD is to transform the spatial dispersion to the wavelength dispersion.
The absorption spectrum for the setup described in
The embodied invention exploits the concept of assigning any given wavelength component of a broadband beam to a proper incidence angle on the CPA cavity, such that it becomes resonating within the cavity at the corresponding angle. Constructing such an angle-wavelength correlation is shown to be viable through a combination of a diffraction component (e.g., one or more gratings) and a lens with properly devised parameters. We demonstrated that the ≈3-nm linewidth of absorption from a normally incident configuration is broadened to a ≈70-nm resonant bandwidth. Such an effect is a very important step to advancement of the CPA to energy harvesting technologies. The proposed omniresonant arrangement can be integrated on a thin multilayer film. Thus it paves the way for future highly-efficient solar cell devices with micron-size building blocks.
The present invention also includes a method for inducing achromatic resonance in an absorbing cavity with a diffraction system tailored for the laboratory environment (see
The method operates under the assumption that an ideal light diffracting component (e.g., grating) 100 with TE or TM polarized collimated light directed at an incidence angle α=50° with respect to the normal to the grating 100.
where d1 and d2 are the distances from the grating to L1 and from L1 to the cavity, respectively. The incidence angle made by a wavelength λ after the lens with respect to the optical axis is thus:
with φo=φ(λc=550 nm)=0. The distances d1 and d2 are selected such that the illuminated spot on the grating 100 is imaged onto the cavity 200. If the focal length of L1 is ƒ, then
When the cavity 200 is oriented such that it is perpendicular to the optical axis, the angle of incidence of each wavelength is φ(λ). Upon tilting the cavity 200 by ψ, the angle of incidence with respect to the normal to the cavity 200 is θ(λ)=φ(λ)+ψ. See
The four CPA absorption resonance peaks shown in
It can be shown that the periodicity of the maximum magnitude of the resonance peaks along the z-axis
Accordingly, a protective layer (spacer) behind the front mirror allows us to optimize the CPA resonance peaks. Specifically, a 100 nm spacer optimizes all four resonances, but a smaller, or slightly larger spacer could have a larger effect on two resonances.
The plot of the electric field amplitude in
The broad spectral flattening of the graphene absorption displayed in the experimental results of
An aspect of the present invention is a method for achromatic transmission through a planar Fabry-Perot micro-cavity—not by modifying its structure, but instead by altering the spectral-spatial configuration of the incident optical radiation using linear optical components. The spatial degree-of-freedom of the optical field, when used in conjunction with its spectral degree-of-freedom, altogether obviates the limitations inherent in traditional approaches to constructing a white-light cavity. In place of narrow, well-separated resonant linewidths of a micro-cavity, broadband “achromatic resonances” emerge.
Starting from the curved locus of a cavity resonance in spectral-angular space, the locus is de-slanted through angular multiplexing of incident broadband light. Achromaticity is achieved by establishing a judicious correlation between the wavelengths and their associated incident angles, which results in optical ‘clearing’ of the cavity. Anomalous angular diffraction—achieved via a bio-inspired grating configuration—engenders the necessary correlation and enables continuous phase-matching of the wave-vector axial component to fulfil the resonance condition over an extended bandwidth. This effect is demonstrated using a planar micro-cavity whose linewidth is ˜0.7-nm-wide and FSR is ˜25 nm. Single-order ˜60-nm-wide resonances that span multiple original FSRs emerge, thereby rendering the resonator transparent and even enabling the formation of an image through it. In principle, such achromatic resonances can be established over an indefinitely wide bandwidth by replacing the grating with an appropriately designed metasurface.
The underlying physical principle for realizing achromatic resonances in a planar Fabry-Pérot cavity can be understood by referring to
(λ,θ)=2nkd cos[θ′(λ)]+2γ(λ,θ′)=2πm. Equation (1)
Therefore, by re-organizing the incident broadband radiation by assigning each wavelength λ to an appropriate incidence angle (λ), all the angularly multiplexed wavelengths can resonate simultaneously (
Turning now to
Dispersive prisms do not provide the required angular spread, and planar surface gratings produce the opposite correlation: longer wavelengths diffract at larger angles with respect to the normal as a consequence of transverse phase-matching (dashed curve in
To address this challenge, inspiration is derived from the reverse-color sequence observed in the diffraction of white light off the wing scales of the butterfly Pierella luna. This effect has been revealed to be geometric in nature: ‘vertical’ micro-gratings that grow on the Pierella luna scales reverse the sequence of diffracted colors as confirmed by fabricated artificial counterparts. This strategy is adopted here in reflection mode and vary the relative tilt between the grating and the cavity, from 0° in
To gain insight into the resonance de-slanting procedure, the spectral-angular variation in the axial wave-vector component kz of broadband light propagating in a ‘bulk’ planar layer of refractive index n is examined. Consider a bandwidth Δλ centered at λc and each wavelength directed at a different angle (λ), with θ(λc)=ψ, such that the beam occupies an angular spread Δθ (assume the wavelengths are distributed uniformly around ψ). For a wavelength λ incident at an external angle θ, kz in the layer is:
k
z(λ,ψ;β)=2π/λ[n2−sin2[ψ−β(λ−λc)]1/2, Equation (2)
where β=Δθ/Δλ°/nm is the angular dispersion, we take n=1.5 and λc=550 nm, and we ignore the spectral variation of n for simplicity. A region in (λ,) space where kz is independent of λ is searched for. The graph of
This prediction is confirmed for achromatic resonances (shown in
Next, the collimated white-light beam is modified to produce the necessary condition to de-slant the resonance locus—without altering the cavity itself in any way. The beam is first spatially filtered through a 1-mm-wide vertical slit (to avoid aliasing of multiple resonance orders) and is then diffracted from a reflective grating with 1800 lines/mm (
The spectral transmission through the Fabry-Pérot cavity with tilt angle ψ is plotted in
As a result of the cavity achromaticity, one may indeed image an object through the cavity with broadband illumination. A lens is added to the setup in
In particular,
The proof-of-principle experiment renders transparent a micro-cavity with 0.7-nm-wide resonances separated by an FSR of ˜25 nm, thanks to an achromatic resonance operating continuously over a broad spectrum (˜60 nm). Although the necessary correlation between wavelength and incidence angle is introduced using a planar surface grating, the bandwidth can be broadened further and the uniformity of the spectral transmission improved by replacing the grating with a metasurface realizing a customized function θ(λ) that takes into account the cavity mirror spectral phase γ(λ,θ), its polarization dependence, and wavelength dependence of the refractive index. Furthermore, such a metasurface may indeed implement the reverse-color sequence without introducing a tilt angle with respect to the cavity. Consequently, depositing the metasurface directly on the planar micro-cavity may potentially result in ultra-thin optical devices that deliver resonant linear and nonlinear behavior over extended bandwidths.
Accordingly, the above description introduces a general principle that lifts the bandwidth restrictions associated with resonant linewidths in an optical micro-cavity leading to the realization of an achromatic or white-light cavity. While recent work has exploited spectral splitting of the solar spectrum to optimize the photovoltaic conversion with multiple semiconductor junctions, our approach—on the other hand—implements a continuous mapping to a wavelength-dependent angle of incidence (λ). Indeed, the present invention extends to the continuum the correlations between discretized optical degrees of freedom previously studied. As a result, the advantages associated with a resonance—such as field enhancement through resonant buildup and enhanced optical nonlinearities—become altogether decoupled from the cavity linewidth and are thus available over orders-of-magnitude larger bandwidths. This concept can have a profound impact on optics by bringing coherent perfect absorption to bear on harvesting solar energy, producing white-light micro-lasers, and yielding broadband resonantly enhanced nonlinear optical devices.
A component of the present invention is a Fabry-Pérot micro-cavity optical resonator includes two multi-layer thin-film dielectric mirrors and a lossy, optically absorbing interface disposed between the mirrors. Non-limiting examples of such an optical resonant cavity are disclosed in commonly owned patent U.S. Pat. No. 9,740,031, the subject matter of which is incorporated herein by reference in its entirety. The '031 patent discloses apparatus and methods that enabled coherent perfect absorption (CPA) in a structure, but only at discrete frequencies satisfying a resonance condition. Apparatus, irrespective of the material from which it is constructed, and methods that enable achromatic CPA have many benefits and advantages. For example, achromatic CPA can extend the salutary benefits accrued upon interaction with a resonance such as resonant field buildup for enhancement of linear and nonlinear optical effects over broad bandwidths in ultrathin devices. The '031 patent provides for an apparatus or system (and associated methods) which essentially includes a white light diffraction component optically coupled to a CPA optical cavity.
In one embodiment, the planar Fabry-Pérot (FP) cavity 200 used is composed of two symmetric 5 bilayer Bragg mirrors 202 enclosing a 4-μm-thick SiO2 dielectric spacer 204 (on a BK7 substrate 206) (as shown in
Incidence→Air−(HL)5−SiO2−(LH)5−BK7.
Here, each bilayer (HL) consists of a high-index (H) and low-index (L) material, which are TiO2 and SiO2, respectively. It is noted, however, that any known non-absorbing materials for making a mirror may be used, as known in the art. The TiO2 films were formed by evaporating Ti2O3 source material under O2 partial pressure. Using these values in Tables S1 and S2, the spectral response of the full cavity (
The transmission characteristics of the FP cavity 200 when it is inserted into a setup that induces achromatic resonances are calculated. In particular, the effect of the grating 100 (light diffracting component) and lens L1 placed in the path of a collimated broadband beam is simulated, as shown in
It is an assumption that an ideal grating with TE or TM polarized collimated light directed at an incidence angle α=50° with respect to the normal to the grating 100. See
φ(λ)=tan−1[(d1/d2)tan(γ(λ)−γo)],
with φo=φ(λc=550 nm)=0. The distances d1 and d2 are selected such that the illuminated spot on the grating 100 is imaged onto the cavity 200. If the focal length of L1 is ƒ, then d2=ƒd1/ƒ−d1. When the cavity 200 is oriented such that it is perpendicular to the optical axis, the angle of incidence of each wavelength is (λ). Upon tilting the cavity 200 by ψ, the angle of incidence with respect to the normal to the cavity 200 is (λ)=(λ)+ψ.
With these parameters, the transmission through the sample using the transfer matrix method is calculated for both TE (
All definitions, as defined and used herein, should be understood to control over dictionary definitions, definitions in documents incorporated by reference, and/or ordinary meanings of the defined terms.
While various embodiments have been described and illustrated herein, those of ordinary skill in the art will readily envision a variety of other means and/or structures for performing the function and/or obtaining the results and/or one or more of the advantages described herein, and each of such variations and/or modifications is deemed to be within the scope of the embodiments described herein. More generally, those skilled in the art will readily appreciate that all parameters, dimensions, materials, and configurations described herein are meant to be exemplary and that the actual parameters, dimensions, materials, and/or configurations will depend upon the specific application or applications for which the teachings is/are used. Those skilled in the art will recognize, or be able to ascertain using no more than routine experimentation, many equivalents to the specific embodiments described herein. It is, therefore, to be understood that the foregoing embodiments are presented by way of example only and that, within the scope of the appended claims and equivalents thereto, embodiments may be practiced otherwise than as specifically described and claimed. Embodiments of the present disclosure are directed to each individual feature, system, article, material, kit, and/or method described herein. In addition, any combination of two or more such features, systems, articles, materials, kits, and/or methods, if such features, systems, articles, materials, kits, and/or methods are not mutually inconsistent, is included within the scope of the present disclosure.
The terminology used herein is for the purpose of describing particular embodiments only and is not intended to be limiting of the invention. As used herein, the singular forms “a”, “an” and “the” are intended to include the plural forms as well, unless the context clearly indicates otherwise. It will be further understood that the terms “comprise” (and any form of comprise, such as “comprises” and “comprising”), “have” (and any form of have, such as, “has” and “having”), “include” (and any form of include, such as “includes” and “including”), and “contain” (any form of contain, such as “contains” and “containing”) are open-ended linking verbs. As a result, a method or device that “comprises”, “has”, “includes” or “contains” one or more steps or elements. Likewise, a step of method or an element of a device that “comprises”, “has”, “includes” or “contains” one or more features possesses those one or more features, but is not limited to possessing only those one or more features. Furthermore, a device or structure that is configured in a certain way is configured in at least that way, but may also be configured in ways that are not listed.
The corresponding structures, materials, acts and equivalents of all means or step plus function elements in the claims below, if any, are intended to include any structure, material or act for performing the function in combination with other claimed elements as specifically claimed. The description of the present invention has been presented for purposes of illustration and description, but is not intended to be exhaustive or limited to the invention in the form disclosed. Many modifications and variations will be apparent to those of ordinary skill in the art without departing from the scope and spirit of the invention. The embodiment was chosen and described in order to best explain the principles of one or more aspects of the invention and the practical application, and to enable others of ordinary skill in the art to understand one or more aspects of the present invention for various embodiments with various modifications as are suited to the particular use contemplated.
This application claims priority to U.S. Provisional Patent Application Ser. No. 62/552,544, filed on Aug. 31, 2017 and entitled “Omniresonant Broadband Coherent Perfect Absorption (CPA) Apparatus, Method, and Applications,” the entirety of which is incorporated herein by reference.
This invention was made with Government support by the US Air Force Office of Scientific Research AFOSR MUM contract FA9550-14-1-0037. The United States Government has certain rights in the invention.
Number | Date | Country | |
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62552544 | Aug 2017 | US |