Tunable infrared pixels having unpatterned graphene layer and conductive metasurface

Abstract

A monolithically integrated, tunable infrared pixel comprises a combined broadband detector and graphene-enabled tunable metasurface filter that operate as a single solid-state device with no moving parts. Functionally, tunability results from the plasmonic properties of graphene that are acutely dependent upon the carrier concentration within the infrared. Voltage induced changes in graphene's carrier concentration can be leveraged to change the metasurface filter's transmission thereby altering the “colors” of light reaching the broadband detector and hence its spectral responsivity. The invention enables spectrally agile infrared detection with independent pixel-to-pixel spectral tunability.

Claims

1. A tunable infrared pixel, comprising: an infrared detector; a bottom dielectric layer disposed on the infrared detector; an unpatterned graphene layer on the bottom dielectric layer; a top dielectric layer on the unpatterned graphene layer; and a conductive metasurface on the top dielectric layer, wherein the metasurface is patterned to excite plasmons within the unpatterned graphene layer and wherein the metasurface is adapted to apply a voltage bias to the unpatterned graphene layer, thereby changing the Fermi level of the graphene and tuning the resonance response of the pixel to incident infrared light.

2. The tunable infrared pixel of claim 1, wherein the infrared detector comprises a gallium-free type-II superlattice detector.

3. The tunable infrared pixel of claim 1, wherein the infrared detector comprises a compound semiconductor.

4. The tunable infrared pixel of claim 3, wherein the compound semiconductor comprises HgCdTe, InAs, InSb, or InGaAs.

5. The tunable infrared pixel of claim 1, wherein the infrared detector comprises a pyroelectric or bolometric detector.

6. The tunable infrared pixel of claim 5, wherein the pyroelectric or bolometric detector comprises deuterated triglycine sulfate or lead zirconate titanate.

7. The tunable infrared pixel of claim 1, wherein the bottom dielectric layer comprises alumina.

8. The tunable infrared pixel of claim 1, wherein the bottom dielectric layer comprises hafnium dioxide, magnesium oxide, lead zirconium titanate, or silicon dioxide, barium fluoride, silicon carbide, aluminum nitride or other polar dielectrics.

9. The tunable infrared pixel of claim 1, wherein the bottom dielectric layer has a thickness of between 50 and 1000 nm.

10. The tunable infrared pixel of claim 1, wherein the top dielectric layer comprises a high-κ gate dielectric.

11. The tunable infrared pixel of claim 10, wherein κ is greater than 10.

12. The tunable infrared pixel of claim 1, wherein the top dielectic layer comprises hafnium dioxide.

13. The tunable infrared pixel of claim 1, wherein the top dielectric layer comprises hexagonal boron nitride, silicon dioxide, magnesium oxide, lead zirconium titanate, or alumina.

14. The tunable infrared pixel of claim 1, wherein the metasurface comprises a conductive grating.

15. The tunable infrared pixel of claim 1, wherein the metasurface comprises a metal.

16. The tunable infrared pixel of claim 1, wherein the metasurface comprises a conductive oxide, conductive polymer, or other conductive non-metal.

17. The tunable infrared pixel of claim 1, wherein the metasurface pattern has a periodicity that is subwavelength to the incident infrared light.

18. The tunable infrared pixel of claim 1, wherein the wavelength of the incident infrared light is between 1 microns and 60 microns.

19. The tunable infrared pixel of claim 18, wherein the wavelength of the incident infrared light is between 6 and 18 microns.

20. The tunable infrared pixel of claim 1, further comprising at least one additional tunable infrared pixel to provide an array of detecting pixels.

Description

BRIEF DESCRIPTION OF THE DRAWINGS

(1) The detailed description will refer to the following drawings, wherein like elements are referred to by like numbers.

(2) FIG. 1 is a schematic side-view illustration of a monolithically integrated tunable infrared pixel (TIP) showing the various layers and the incident infrared beam. Unpatterned graphene is sandwiched between two dielectric layers.

(3) FIG. 2A is a top-view false color micrograph of a TIP. FIG. 2B is a cross-sectional view of the pixel comprising a gold grating sitting atop a thin HfO.sub.2 dielectric and graphene stack.

(4) FIG. 3A is a graph of the spectral photoresponse of an exemplary TIP at varying gate voltages used to control the spectral response of filter. FIG. 3B is a map of spectral responsivity as a function of wavelength and gate voltage. Plots in FIG. 3A are horizontal line cuts of FIG. 3B. FIG. 3C is a graph of spectral responsivity at 900 cm.sup.−1, 980 cm.sup.−1, and 1200 cm.sup.−1 (i.e., the vertical dashed lines in FIG. 3B as a function of gate voltage).

(5) FIG. 4 is a comparison of electrical transport with the graphene filter and the TIP spectral responsivity at 1200 cm.sup.−1.

(6) FIG. 5A is a graph of the measured spectra of polypropylene from the TIP-device as the Fermi-level (E.sub.F) of the graphene is changed via the gate voltage. FIG. 5B is a graph of the difference spectra.

DETAILED DESCRIPTION OF THE INVENTION

(7) An end-view schematic illustration of a tunable infrared pixel (TIP) comprising several layers of the monolithically integrated pixel structure is shown in FIG. 1. Depending on the details of the structure, the TIP can generally be responsive to infrared light from about 1 to 60 microns wavelength and, more preferably, to long wavelength infrared (LWIR) light (e.g., 6 to 18 microns wavelength). The filter layers can be built directly on an infrared detector comprising a sensing element or photodetector. The TIP structure further comprises a continuous, unpatterned graphene layer sandwiched between two dielectric layers on the infrared detector. Finally, a patterned metasurface structure is deposited on the top dielectric layer.

(8) Graphene is chosen for two reasons. First, it has been used in numerous “stand-alone” tunable infrared filters reported previously. See Y. Yao et al., Nano Lett. 14(1), 214 (2013); and U.S. application Ser. No. 15/872,293, filed Jan. 16, 2018, which is incorporated herein by reference. Second, being a two-dimensional van der Waals solid, graphene can be transferred at room temperature directly atop the detector material while imparting virtually no mechanical load to the underlying detector. Tunability of the TIP arises from excitation of plasmons within the unpatterned graphene layer. While graphene is only one atom thick, its interaction with infrared light can be enhanced by plasmonic excitation enabling graphene to significantly influence the optical response of the TIP. Importantly, the plasmonic dispersion of graphene is determined by both its surrounding dielectric environment, as well as graphene's free carrier density. Changes to the Fermi level cause shifts in the plasmon dispersion, thereby modifying the excitation energies of plasmons at a given momentum. See Z. Fei et al., Nature 487, 82 (2012); Z. Fei et al., Nano Lett. 15, 8271 (2015); A. Woessner et al., Nat. Mater. 14, 421 (2015); M. D. Goldflam et al., Nano Lett. 15, 4859 (2015); and M. Jablan et al., Phys. Rev. B 80, 245435 (2009).

(9) The sandwich comprises a thick bottom dielectric layer on an infrared detector, the unpatterned graphene layer, and a thin top dielectric layer deposited on the graphene layer. The choice of surrounding dielectrics, and the geometry itself, have a strong influence on the regions of tunability enabling pixels to be designed for functionality in specific wavelength regimes. The dielectric layers serve two purposes. First, they electrically separate the detector element and conductive nanoantenna from the graphene. Second, these dielectrics serve to define the spectral location of the graphene tunability, its magnitude, and the shape of the pass band. A variety of non-conductive dielectric materials can be used for the dielectric layers, such as hafnium dioxide, alumina, magnesium oxide, lead zirconium titanate, or silicon dioxide. The top dielectric layer preferably provides an efficient high-κ gate dielectric (e.g., κ greater than 10) that is also thin enough for Fermi level modification when a bias voltage is applied between the metasurface and the graphene. The top dielectric layer further provides a spacer layer to prevent contact between graphene and the conductive metasurface which would cause Fermi level pinning of the graphene and limit spectral tunability. The presence of the capping top dielectric also helps to ensure the long term stability of the underlying graphene by isolating it from the environment, thereby preventing accumulation of adsorbates on the graphene over time. See J. D. Fowler et al., ACS Nano 3, 301 (2009); and C. W. Chen et al., J. Vac. Sci. Technol. B 30, 040602 (2012). Typically, the top dielectric can range in thickness from 1-100 nm to facilitate biasing of the graphene whereas the bottom dielectric can range in thickness from 50-1000 nm to ensure electrical isolation of the detector from the graphene filter.

(10) Next, a metasurface structure is deposited on the top dielectric layer. The metasurface serves multiple purposes: first, it can act as a top gate for graphene allowing the high-κ dielectric nature of the top dielectric layer to be employed for injection of charge into the graphene; second, field enhancement within the small gaps of the metasurface results in increased interaction of incident light with the continuous graphene sheet; and lastly, the resonant response of the metasurface itself excites graphene plasmons that can dominate the overall response of the pixel filter. The metasurface can comprise any conductive material and pattern that is capable of exciting plasmons in the underlying unpatterned graphene layer. The metasurface can be adapted to apply a voltage bias, V.sub.G, to the graphene layer, thereby changing the Fermi level of the graphene and tuning the resonance response of the pixel to the incident infrared light. For example, the metasurface can comprise a grating with periodicity comparable to the wavelength of the incident infrared light and, more preferably, subwavelength to the incident light. For example, the grating metasurface can comprise a thin gold grating patterned over the graphene pixel area. Other metals or conductive non-metals, such as conductive oxides and polymers, can also be used for the metasurface material.

(11) The finished pixel provides a tunable filter that is fully integrated to the infrared detector as a single solid-state device. Therefore, the invention enables independent spectral tuning of individual pixels across an array. Detecting arrays can comprise thousands of separate pixels arranged in a grid, wherein each pixel typically has a size ranging from ten to hundreds of microns. The invention thus allows each pixel to have its spectral response separately tuned via the addition of a single filter contact applied at each pixel beyond those used to operate the infrared detector.

(12) As an example of the invention, tunable graphene filters were fabricated directly atop a gallium-free type-II superlattice (T2SL) infrared detector with a cut-off wavelength of 11 μm. Spectral responsivity of the TIP was measured as a function of electrostatic gating of the graphene filter. Dynamic and continuous tuning of the relative spectral responsivity resulted in changes of >20%. These changes were then leveraged to dynamically alter the comparative sensitivity between two spectrally separated infrared absorption bands of polypropylene to emphasize the device's “push-button” tunability.

(13) The fabricated exemplary TIP is shown in FIGS. 2A and 2B from both a plan and cross-sectional view. The TIP has a pixel area of approximately 250×250 μm.sup.2. Beginning from the top, the filter comprises an Au grating metasurface that excites the graphene plasmon. In this example, the 50 nm thick gold grating has a period of 1 μm and a gap between the grating electrodes of 100 nm. The graphene plasmon's energy, and hence the pass-band of the filter, is controlled dynamically by placing a voltage using the Au grating across a 20-nm thick HfO.sub.2 layer (κ˜25) that rests above the graphene. The voltage electrostatically dopes the graphene inducing changes in the material's optical properties and thus its plasmonic response. A 500-nm thick Al.sub.2O.sub.3 bottom dielectric layer supports the graphene and practically serves as a “coarse knob” for dictating the static spectral character of the filter. See M. D. Goldflam et al., Opt. Express 25(11), 12400 (2017). Each of these layers is fabricated atop the detector through layer transfer techniques (e.g., of chemical vapor deposition-grown (CVD) graphene), atomic layer deposition (ALD), and/or standard lithography approaches. Such processing does not appreciably change the detector properties. See X. Li et al., Science 324(5932), 1312 (2009); and Y. Hernandez et al., Nat. Nanotechnol. 3(9), 563 (2008).

(14) The detector can comprise a T2SL long-wave infrared (LWIR) absorber synthesized atop a GaSb substrate. Use of a T2SL detector is motivated by theoretical predictions of dark current characteristics surpassing that of mercury-cadmium-telluride (MCT). See B. Olson et al., Appl. Phys. Lett. 107(26), 261104 (2015); Y. Aytac et al., Appl. Phys. Lett. 105(2), 022107 (2014); G. Dyer et al., Appl. Phys. Lett. 108(1), 013106 (2016); M. D. Goldflam et al., Appl. Phys. Lett. 109(25), 251103 (2016); and D. Z. Ting et al., Appl. Phys. Lett. 113, 021101 (2018). However, the tunable architecture of the present invention can easily be applied atop a conventional MCT photodetector which can provide a significant increase in quantum efficiency over that of the T2SL detector. For the present case, quantum efficiency of the T2SL detector is hindered by the low absorption coefficient of the 2 μm thick superlattice in the LWIR wavelength range. See M. D. Goldflam et al., Appl. Phys. Left. 109(25), 251103 (2016); and D. R. Rhiger, J. Electron. Mater. 40(8), 1815 (2011). Depending on the wavelength range and operating characteristics of interest, other compound semiconductor infrared photodetectors can also be used, such as InAs, InSb, or InGaAs as well as pyroelectric and bolometric detectors composed of deuterated triglycine sulfate (DTGS) or lead zirconate titanate (PZT). See E. L. Dereniak and G. D. Boreman, Infrared Detectors and Systems, Wiley (1996).

(15) The exemplary tunable integrated pixel was characterized initially via measurements of its spectral responsivity. These measurements were carried out by focusing light output from a Fourier transform infrared spectrometer (FTIR) onto the TIP. The electrical output of the detector was then fed directly back into the FTIR such that the response from 8-12 μm (800-1200 cm.sup.−1) could be assessed continuously as a function of filter bias. Spectral characteristics of the FTIR light-source were calibrated using a commercial deuterated triglycine sulfate (DTGS) detector. See O. Gravrand et al., “A calibration method for the measurement of IR detector spectral responses using a FTIR spectrometer equipped with a DTGS reference cell,” in High Energy, Optical, and Infrared Detectors for Astronomy VI, vol. 9154. International Society for Optics and Photonics, Conference Proceedings, p. 91542O (2014).

(16) Spectral tuning of the device was apparent, repeatable, and continuous, as shown in FIGS. 3A-3C. FIG. 3A is a graph of the spectral photoresponse of TIP device at varying gate voltages. Quantitatively, the detector's relative response changes by nearly ±20% relative to that at the charge neutrality point (CNP) of the graphene by varying the gate voltage from 2 to −3 V. FIG. 3B is a map of spectral responsivity as a function of wavelength and gate voltage. FIG. 3C is a graph of spectral responsivity at 900 cm.sup.−1, 980 cm.sup.−1, and 1200 cm.sup.−1 as a function of gate voltage. The location of maximum responsivity varies by 50 cm.sup.−1. The changes are analog allowing for continuous tuning as opposed to the digital states typically available when filtering with phase change materials.

(17) Variations in the spectral response are caused by changes in the amount of transmitted light through the filter rather than a spurious alteration in the detector's charge transport induced by the electrostatic gating of the graphene. This is evidenced by comparing the current-voltage characteristics of the graphene with the spectral response of the detector at 1200 cm.sup.−1, as shown in FIG. 4. The graphene current correlates to changes in the spectral response of the graphene. Specifically, changes in spectral responsivity of the TIP device as a whole qualitatively match the amount of current moving through the graphene. This correlation, in combination with changes observed in the device's reflectance as a function of gate voltage (not shown), indicates that the graphene/dielectric stack is operating as a tunable light filter. The filter operates electrostatically with minimal dissipation of current. The filter dissipates only the current “leaking” through the gate, which is orders of magnitude less than that moving through the detector itself. The TIP device therefore provides additional functionality with minimal additional power consumption.

(18) The tunability of the graphene filter allows for “push-button” control of a pixel's spectral sensitivity. To demonstrate this, a thin polypropylene film was placed between the light source and the TIP device. The infrared spectrum measured by the TIP pixel was then acquired with the graphene set at several different Fermi-levels (E.sub.F) as controlled by the gate voltage. Results are shown in FIG. 5A where changes in the response, and hence sensitivity, to certain modes are appreciably varied. This is exemplified by comparing the signals near 930 and 1100 cm.sup.−1. For the lower energy mode, maximum sensitivity (i.e., largest “dip” in signal) is observed when the graphene Fermi-level is maximized—i.e., the optical conductivity of graphene is greatest. The opposite is true for the mode near 1100 cm.sup.−1 leading to difference spectra that “flip” in the magnitude of their signal near 1000 cm.sup.−1, as shown in FIG. 5B. Effectively, the device is more sensitive to one mode as it becomes less sensitive to another. This spectral selectivity is typically acquired through the use of stand-alone filters. Here, spectral sensitivity is shown to be integral to the TIP itself.

(19) By fabricating a dynamic graphene metasurface structure atop a T2SL infrared detector, tunable spectral responsivity at the single pixel level can be obtained in the LWIR. The monolithic approach increases functionality while maintaining the standard lamellar architecture of semiconductor devices without appreciably increasing the size or power consumption of the detector. The invention enables imaging arrays comprising pixels with independent and controllable spectral responsivities.

(20) The present invention has been described as tunable infrared pixels via dynamic metasurfaces. It will be understood that the above description is merely illustrative of the applications of the principles of the present invention, the scope of which is to be determined by the claims viewed in light of the specification. Other variants and modifications of the invention will be apparent to those of skill in the art.