Materials, Photonic Devices, and Sensors

Theoretical investigation of all-metal-based mushroom plasmonic metamaterial absorbers at infrared wavelengths

[+] Author Affiliations
Shinpei Ogawa, Daisuke Fujisawa

Advanced Technology Research and Development Center, Mitsubishi Electric Corporation, 8-1-1 Tsukaguchi-Honmachi, Amagasaki, Hyogo 661-8661, Japan

Masafumi Kimata

Ritsumeikan University, College of Science and Engineering, 1-1-1 Noji-higashi, Kusatsu, Shiga 525-8577, Japan

Opt. Eng. 54(12), 127104 (Dec 17, 2015). doi:10.1117/1.OE.54.12.127104
History: Received September 24, 2015; Accepted November 16, 2015
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Abstract.  High-performance wavelength-selective infrared (IR) sensors require small pixel structures, a low-thermal mass, and operation in the middle-wavelength infrared (MWIR) and long-wavelength infrared (LWIR) regions for multicolor IR imaging. All-metal-based mushroom plasmonic metamaterial absorbers (MPMAs) were investigated theoretically and were designed to enhance the performance of wavelength-selective uncooled IR sensors. All components of the MPMAs are based on thin layers of metals such as Au without oxide insulators for increased absorption. The absorption properties of the MPMAs were investigated by rigorous coupled-wave analysis. Strong wavelength-selective absorption is realized over a wide range of MWIR and LWIR wavelengths by the plasmonic resonance of the micropatch and the narrow-gap resonance, without disturbance from the intrinsic absorption of oxide insulators. The absorption wavelength is defined mainly by the micropatch size and is longer than its period. The metal post width has less impact on the absorption properties and can maintain single-mode operation. Through-holes can be formed on the plate area to reduce the thermal mass. A small pixel size with reduced thermal mass and wideband single-mode operation can be realized using all-metal-based MPMAs.

Figures in this Article

There has been increasing interest in uncooled infrared (IR) sensors with a microelectromechanical system-based pixel structure due to their low-cost fabrication and wide range of applications.1,2 We have recently developed uncooled IR sensors with advanced functions using plasmonics3,4 and metamaterials5,6 to expand their field of applications, which includes fire detection, gas analysis, hazardous material recognition, multicolor imaging, and polarimetric imaging. First, a wavelength-selective uncooled IR sensor was developed for the middle-wavelength infrared (MWIR) and long-wavelength infrared (LWIR) regions using a two-dimensional plasmonic absorber (2-D PLA).710 A 2-D PLA is an Au-based periodic dimple structure, in which surface plasmon resonance is produced and strong wavelength-selective absorption occurs according to the surface periodicity. A polarization-selective uncooled IR sensor was then developed using a 2-D PLA with ellipsoidal dimples11 and one-dimensional grating absorbers,12 whereby polarization could be selectively detected according to the asymmetry on the surface of the absorbers.

Some advantages of 2-D PLAs are a simple fabrication procedure and structural robustness. Wavelength- and polarization-selective functions can be realized for PLAs without the attachment of filters,13 multilayer structures,14 mirrors,15 or polarizers,16,17 which effectively reduces the cost and additional space requirements of optical systems. Multicolor/polarimetric imaging can, therefore, be realized by the integration of various 2-D PLAs with different wavelength/polarization-detection specifications. 2-D PLAs inevitably require a large number of periods and a large thickness, which results in a large pixel size and a high-thermal mass.7,8 However, high-performance wavelength-selective uncooled IR sensors for multicolor IR imaging require a small pixel size and low-thermal mass to achieve high resolution and fast response. Metal-insulator-metal structures1821 based on plasmonic metamaterials are important candidates for high-performance absorbers, which control the absorption wavelength according to the surface resonator size beyond the surface array period. However, insulator layers such as SiO2 and SiN cause an additional absorption peak, restrict the operation wavelength to near the MWIR region due to their intrinsic absorption,22 and also increase the thermal mass. Therefore, we have proposed three-dimensional (3-D) or mushroom plasmonic metamaterial absorbers (MPMAs),23 as well as a suitable fabrication method.24 MPMAs with Si posts were also developed for dual- and single-band detection.25 However, MPMAs with Si posts require precise control of the post width to achieve single-mode operation. Therefore, we have investigated the detailed absorption properties of MPMAs based on all-metal structures to realize high-performance wavelength-selective uncooled IR sensors with wideband and single-mode operation.

In this study, we report a theoretical investigation of MPMAs for high-performance uncooled IR sensors with advanced functions.

Effect of the Micropatch Shape

Figure 1 shows schematic illustrations of the structure investigated in this study. The micropatches are arrayed and connected to the bottom plate with posts. This structure is referred to as a mushroom metamaterial.26,27 In this work, all of the components were assumed to be made of Au. The dielectric constant of Au used in our calculations was taken from Ref. 28. The minimum thickness of all components is approximately twice the skin depth to prevent light penetration and achieve ultrathin absorbers with low-thermal mass. The structural parameters of the period, the width (diameter) and thickness of the micropatch, the thickness of the bottom plate, and the width (diameter) and height of the posts are defined as p, wm; tm, tb; wp; and hp, respectively. The gap between the micropatches and the bottom plate is equal to hp. The thickness tb has no impact on the absorption, as long as it is sufficiently thick to reflect incident IR radiation. Thus, tb is considered to be at least >50nm in the IR wavelength region for practical applications29 and was set as a semi-infinite thickness for the simulation. The parameters tm, wp, and hp were fixed at 50, 200, and 150 nm, respectively. The incident angle is set to normal incidence for the fundamental evaluation of MPMAs conducted in this study. The polarization direction used is defined as that parallel to the basic lattice vector of the square lattice structure, which corresponds to the x- and y-directions, as shown in Fig. 1(b). The results obtained represent the averaged total absorption for all polarizations due to the symmetry of the MPMAs.

Graphic Jump Location
Fig. 1
F1 :

Schematic illustrations of the mushroom plasmonic metamaterial absorber (MPMA) proposed in this study: (a) surface view and (b) cross-section of one unit cell with the incident light and the electric field directions are shown.

We first investigated the absorption properties of a circular-shaped micropatch using rigorous coupled-wave analysis (RCWA). The period p was fixed at 4.0μm and wm was varied. Figures 2(a) and 2(b) show the absorption for the MPMAs with wm at 2.0, 2.5, 3.0, and 3.5μm, and the absorption for wm from 1.0 to 4.0μm as a function of the wavelength. Figure 2 indicates that sufficient absorption of over 90% was obtained for the MPMAs with most of the wm values, and the absorption wavelength could be controlled primarily by wm, regardless of p. The absorption wavelength is almost proportional to wm; however, a forbidden band where the absorption is suppressed appears for some wm values, such as 1.8, 2.5, 2.8, and 3.2μm. The full width at half maximum (FWHM) also increases with wm. As the absorption wavelength approaches the period, the FWHM is improved due to the reduction of the gap resonance between the micropatches.

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Fig. 2
F2 :

Calculated absorption spectra for the MPMA with circular-shaped micropatches. (a) Spectra for wm=2.0, 2.5, 3.0, and 3.5μm, and (b) spectra as a function of wavelength and wm. The colormap on the right side defines the absorption scale.

The absorption properties of square-shaped micropatches were also investigated by RCWA; a schematic illustration of an MPMA with square-shaped micropatches is provided in Fig. 3. As with the circular-shaped micropatch, the period p was again fixed at 4.0μm and wm was varied. Figure 4 shows the wavelength absorption for this MPMA for various values of wm from 1.0 to 4.0μm. Sufficient absorption of over 90% was obtained for the MPMA with all of the wm values, and the absorption wavelength could be controlled according to wm, regardless of p. The absorption wavelength is almost proportional to wm, and a uniform absorption peak is maintained over a wide range of MWIR and LWIR wavelengths compared with that for the MPMA with circular-shaped micropatches. Each circular-shaped micropatch forms an unequal gap with the adjacent micropatches, which produces broader resonance. In contrast, the square-shaped micropatches maintain a parallel gap with the adjacent micropatches, which produces narrower resonance. When the absorption wavelength is smaller than p, diffraction starts to occur for both the circular- and square-shaped micropatches. Therefore, the absorption abruptly decreases for wavelengths <4μm.

Graphic Jump Location
Fig. 3
F3 :

Schematic illustration of an MPMA with square-shaped micropatches. (a) Surface view and (b) cross-section of one unit cell with the incident light and the electric field directions are shown.

Graphic Jump Location
Fig. 4
F4 :

Calculated absorption spectra for the MPMA with square-shaped micropatches. (a) Spectra for wm=2.0, 2.5, 3.0, and 3.5μm, and (b) spectra as a function of wavelength and wm.

The time-averaged electromagnetic field amplitude distribution was calculated at the resonance using the 2-D finite-difference time-domain (FDTD) method. Here, wm was fixed at 2.0μm, whereas the values of the other parameters were the same as in the RCWA calculation. Figures 5(a)5(c) show the normalized amplitude of the electric field and the magnetic field distribution, and the power, respectively. X, Y, and Z are defined as parallel to wm, vertical to the x-direction, and parallel to hp, respectively. Figure 5 clearly demonstrates that plasmonic resonance occurs only at the perimeter of the micropatch. These results confirm that localized plasmonic resonance rather than propagating plasmonic resonance occurs in the MPMAs. The absorption wavelength is defined only by the size of the micropatch beyond the pattern period due to this strong confinement of such localized plasmonic resonance, and thus contributes to a smaller pixel size.

Graphic Jump Location
Fig. 5
F5 :

Simulated time-averaged normalized amplitude of the (a) electric field distribution in the x-direction, (b) magnetic field distribution in the y-direction, and (c) power for a unit cell.

Effect of the Post Height

The effect of hp was investigated for an MPMA with square-shaped micropatches. Figure 6 shows the wavelength absorption for the MPMA as a function of hp from 0 to 500 nm with a fixed wm and p of 2.0 and 4.0μm, respectively. Sufficient absorption of over 90% was obtained for hp ranging from 80 to 200 nm, where the shift of the absorption wavelength was small. This result indicates that the narrow-gap resonance between the micropatches and the bottom plate is especially important to obtain sufficient absorption.

Graphic Jump Location
Fig. 6
F6 :

Absorption spectrum for an MPMA with square-shaped micropatches as a function of the post height (hp).

Effect of the Post Width

The effect of wp was also investigated for an MPMA with square-shaped micropatches. Figure 7 shows the wavelength absorption for the MPMA as a function of wp from 100 nm to 1.0μm with a fixed wm and p of 2.0 and 4.0μm, respectively. Sufficient absorption of over 90% was obtained, and a single absorption mode was achieved over a wide range of wp values from 100 nm to 1.0μm, which is half that of wm at 2.0μm. This result is attributed to the strongly localized plasmonic resonance at the edge of the micropatches. The post width has less impact on the absorption properties, and single-mode operation can be maintained, in contrast to the 2-D PLA with Si-post structures, which produces a gap resonant mode inside the Si post.

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Fig. 7
F7 :

Absorption spectrum for an MPMA as a function of the post width (wp).

High-performance uncooled IR sensors require a small absorber volume to achieve fast responsivity. Through-holes are thus typically formed on absorbers to reduce the thermal mass. They are also beneficial for etchant or etching gas to fabricate thermal isolation structures by bulk micromachining. Therefore, the use of through-holes with the MPMA was investigated; Figure 8 shows a schematic illustration of the MPMA with square-shaped through-holes. The absorption properties of an MPMA with square-shaped micropatches and square-shaped through-holes were calculated by RCWA, in which p and wm were fixed at 4.0 and 2.0μm, respectively. Figure 9 shows the wavelength absorption of the MPMA as a function of the through-hole width (wt) from 100 nm to 1.0μm. The presence of through-holes had no influence on the absorption properties of the MPMA in the studied wt range. This indicates that the micropatches induced an antenna effect, because the plasmonic resonance mainly occurs at the edge of the micropatch, and narrow-gap resonance is formed, as shown in Fig. 5. The same effect was also confirmed for an MPMA with circular micropatches and circular through-holes. The through-holes did significantly reduce the absorber volume of the pixels, which leads to fast response and provides an advantage for surface micromachining techniques, such as under etching of the absorber area.30

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Fig. 8
F8 :

Schematic of an MPMA with square-shaped through-holes.

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Fig. 9
F9 :

Absorption spectrum for an MPMA with square-shaped through-holes as a function of the through-hole width (wt).

Au-based MPMAs were theoretically investigated to aid the development of high-performance wavelength-selective uncooled IR sensors. The RCWA calculations demonstrated that wavelength-selective absorption could be realized depending on the shape and size of the micropatches. Broadband absorption was achieved with circular micropatches, whereas unity absorption was realized with square-shaped micropatches over a wide range of MWIR and LWIR wavelengths. The FDTD calculation demonstrated that the strong plasmonic resonance was confined at the edges of the micropatches, which leads to a small pixel size. A post height of 80 to 200 nm was appropriate to obtain a narrow-gap resonance. However, the post width has less impact on the absorption properties and can maintain single-mode absorption, in contrast to that of Si-post structures. Through-holes can be formed on the bottom plate due to this 3-D plasmonic resonance and can reduce the thermal mass of the pixel as well as providing advantages for the fabrication of cavities. All-metal-based MPMAs can be applied for any type of uncooled IR sensors, such as thermopiles, bolometers, and silicon-on-insulator diodes.31,32 The results obtained here will contribute to the development of high-performance single-mode wavelength-selective uncooled IR sensors for multicolor imaging in the wideband MWIR and LWIR regions.

The authors thank Masashi Ueno and Tetsuya Satake of the Advanced Technology R&D Center of Mitsubishi Electric Corporation for their helpful assistance.

Kruse  P. W., Uncooled Thermal Imaging Arrays, Systems, and Applications. ,  SPIE Press ,  Bellingham, WA  (2001).
Kimata  M., “Trends in small-format infrared array sensors,” in  Proc. Sensors , p. 1 ,  IEEE  (2013).
Stanley  R., “Plasmonics in the mid-infrared,” Nat. Photonics. 6, (7 ), 409  (2012). 1749-4885 CrossRef
Kawata  S., “Plasmonics: future outlook,” Jpn. J. Appl. Phys.. 52, (1 ), 010001  (2013).CrossRef
Smith  D. R., , Pendry  J. B., and Wiltshire  M. C., “Metamaterials and negative refractive index,” Science. 305, (5685 ), 788  (2004). 0036-8075 CrossRef
Tanaka  T., “Plasmonic metamaterials,” IEICE Electron. Express. 9, (2 ), 34  (2012).CrossRef
Ogawa  S.  et al., “Wavelength selective uncooled infrared sensor by plasmonics,” Appl. Phys. Lett.. 100, (2 ), 021111  (2012). 0003-6951 CrossRef
Ogawa  S.  et al., “Wavelength selective wideband uncooled infrared sensor using a two-dimensional plasmonic absorber,” Opt. Eng.. 52, (12 ), 127104  (2013).CrossRef
Masuda  K.  et al., “Optimization of two-dimensional plasmonic absorbers based on a metamaterial and cylindrical cavity model approach for high-responsivity wavelength-selective uncooled infrared sensors,” Sens. Mater.. 26, (4 ), 215  (2014). 0914-4935 
Takagawa  Y., , Ogawa  S., and Kimata  M., “Detection wavelength control of uncooled infrared sensors by two-dimensional lattice plasmonic absorbers,” Sensors. 15, (6 ), 13660  (2015). 0746-9462 CrossRef
Ogawa  S.  et al., “Polarization-selective uncooled infrared sensor with asymmetric two-dimensional plasmonic absorber,” Opt. Eng.. 53, (10 ), 107110  (2014).CrossRef
Ogawa  S., , Takagawa  Y., and Kimata  M., “Polarization-selective uncooled infrared sensor using a one-dimensional plasmonic grating absorber,” Proc. SPIE. 9451, , 94511K  (2015). 0277-786X CrossRef
Ohtera  Y., and Yamada  H., “Photonic crystals for the application to spectrometers and wavelength filters,” IEICE Electron. Express. 10, (8 ), 20132001  (2013).CrossRef
Han  S. W.  et al., “Design of infrared wavelength-selective microbolometers using planar multimode detectors,” Electron. Lett.. 40, (22 ), 1410  (2004).CrossRef
Shea  R. P., , Gawarikar  A. S., and Talghader  J. J., “Midwave thermal infrared detection using semiconductor selective absorption,” Opt. Express. 18, (22 ), 22833  (2010). 1094-4087 CrossRef
Haïdar  R.  et al., “Free-standing subwavelength metallic gratings for snapshot multispectral imaging,” Appl. Phys. Lett.. 96, (22 ), 221104  (2010). 0003-6951 CrossRef
Kamerman  G. W.  et al., “Polarization state imaging in long-wave infrared for object detection,” Proc. SPIE. 8897, , 88970R  (2013). 0277-786X CrossRef
Hao  J.  et al., “High performance optical absorber based on a plasmonic metamaterial,” Appl. Phys. Lett.. 96, (25 ), 251104  (2010). 0003-6951 CrossRef
Maier  T., and Brueckl  H., “Multispectral microbolometers for the midinfrared,” Opt. Lett.. 35, (22 ), 3766  (2010). 0146-9592 CrossRef
Watts  C. M., , Liu  X., and Padilla  W. J., “Metamaterial electromagnetic wave absorbers,” Adv. Mater.. 24, (23 ), OP98  (2012). 0935-9648 CrossRef
Feng  R.  et al., “Dual-band infrared perfect absorber based on asymmetric T-shaped plasmonic array,” Opt. Express. 22, (S2 ), A335  (2014). 1094-4087 CrossRef
Chen  Y. B., and Chiu  F. C., “Trapping mid-infrared rays in a lossy film with the Berreman mode, epsilon near zero mode, and magnetic polaritons,” Opt. Express. 21, (18 ), 20771  (2013). 1094-4087 CrossRef
Ogawa  S.  et al., “Three-dimensional plasmonic metamaterial absorbers for high-performance wavelength selective uncooled infrared sensors,” Proc. SPIE. 9070, , 90701Y  (2014). 0277-786X CrossRef
Ogawa  S., , Fujisawa  D., and Kimata  M., “Three-dimensional plasmonic metamaterial absorbers based on all-metal structures,” Proc. SPIE. 9451, , 94511K  (2015). 0277-786X CrossRef
Ogawa  S.  et al., “Mushroom plasmonic metamaterial infrared absorbers,” Appl. Phys. Lett.. 106, (4 ), 041105  (2015). 0003-6951 CrossRef
Sievenpiper  D.  et al., “High-impedance electromagnetic surfaces with a forbidden frequency band,” IEEE Trans. Microwave Theory Tech.. 47, (11 ), 2059  (1999). 0018-9480 CrossRef
Kaipa  C. S. R., , Yakovlev  A. B., and Silveirinha  M. G., “Characterization of negative refraction with multilayered mushroom-type metamaterials at microwaves,” J. Appl. Phys.. 109, (4 ), 044901  (2011). 0021-8979 CrossRef
Rakic  A. D.  et al., “Optical properties of metallic films for vertical-cavity optoelectronic devices,” Appl. Opt.. 37, (22 ), 5271  (1998). 0003-6935 CrossRef
Neubrech  F.  et al., “Properties of gold nanoantennas in the infrared,” in Electronics and Photonics. , and Rahman  F., Ed., p. 210 ,  World Scientific Publishing Co. ,  Singapore  (2008).
Fujisawa  D.  et al., “Multi-color imaging with silicon-on-insulator diode uncooled infrared focal plane array using through-hole plasmonic metamaterial absorbers,” in  Proc. MEMS , pp. 905 –908,  IEEE  (2015).
Fujisawa  D.  et al., “Two-million-pixel SOI diode uncooled IRFPA with 15  μm pixel pitch,” Proc. SPIE. 8353, , 83531G  (2012). 0277-786X CrossRef
Maegawa  T.  et al., “2-in-1 diodes with a contact-sidewall structure for small pixel pitch in silicon-on-insulator (SOI) uncooled infrared (IR) focal plane arrays,” Sens. Mater.. 26, (4 ), 189  (2014). 0914-4935 

Shinpei Ogawa received his BE, ME, and PhD degrees from the Department of Electronic Science and Engineering, Kyoto University, Japan, in 2000, 2002, and 2005, respectively. He has been with the Advanced Technology R&D Center, Mitsubishi Electric Corporation, Amagasaki, Japan, since 2005. He works on the development of various microelectromechanical system (MEMS) devices, including RF-MEMS switches, inductors, through-silicon via, optical sensors, and infrared (IR) sensors. He is currently a unit leader of plasmonics, metamaterials, and graphene research.

Daisuke Fujisawa received his MS degree in electrical and electronic engineering in 2002 and his PhD in electronic and information engineering in 2005, all from Toyohashi University of Technology, Aichi, Japan. In 2005, he joined the Mitsubishi Electric Corporation, where he has been working at the Advanced Technology R&D Center. He currently works on the research and development of silicon-based IR focal plane arrays.

Masafumi Kimata received his MS degree from Nagoya University in 1976 and received his PhD from Osaka University in 1992. He joined Mitsubishi Electric Corporation in 1976 and retired from Mitsubishi Electric in 2004. He is currently a professor at Ristumeikai University, where he continues his research on MEMS-based uncooled IR focal plane arrays and type-II superlattice IR focal plane arrays. He is a fellow of SPIE.

© The Authors. Published by SPIE under a Creative Commons Attribution 3.0 Unported License. Distribution or reproduction of this work in whole or in part requires full attribution of the original publication, including its DOI.

Citation

Shinpei Ogawa ; Daisuke Fujisawa and Masafumi Kimata
"Theoretical investigation of all-metal-based mushroom plasmonic metamaterial absorbers at infrared wavelengths", Opt. Eng. 54(12), 127104 (Dec 17, 2015). ; http://dx.doi.org/10.1117/1.OE.54.12.127104


Figures

Graphic Jump Location
Fig. 1
F1 :

Schematic illustrations of the mushroom plasmonic metamaterial absorber (MPMA) proposed in this study: (a) surface view and (b) cross-section of one unit cell with the incident light and the electric field directions are shown.

Graphic Jump Location
Fig. 2
F2 :

Calculated absorption spectra for the MPMA with circular-shaped micropatches. (a) Spectra for wm=2.0, 2.5, 3.0, and 3.5μm, and (b) spectra as a function of wavelength and wm. The colormap on the right side defines the absorption scale.

Graphic Jump Location
Fig. 3
F3 :

Schematic illustration of an MPMA with square-shaped micropatches. (a) Surface view and (b) cross-section of one unit cell with the incident light and the electric field directions are shown.

Graphic Jump Location
Fig. 4
F4 :

Calculated absorption spectra for the MPMA with square-shaped micropatches. (a) Spectra for wm=2.0, 2.5, 3.0, and 3.5μm, and (b) spectra as a function of wavelength and wm.

Graphic Jump Location
Fig. 5
F5 :

Simulated time-averaged normalized amplitude of the (a) electric field distribution in the x-direction, (b) magnetic field distribution in the y-direction, and (c) power for a unit cell.

Graphic Jump Location
Fig. 6
F6 :

Absorption spectrum for an MPMA with square-shaped micropatches as a function of the post height (hp).

Graphic Jump Location
Fig. 7
F7 :

Absorption spectrum for an MPMA as a function of the post width (wp).

Graphic Jump Location
Fig. 9
F9 :

Absorption spectrum for an MPMA with square-shaped through-holes as a function of the through-hole width (wt).

Graphic Jump Location
Fig. 8
F8 :

Schematic of an MPMA with square-shaped through-holes.

Tables

References

Kruse  P. W., Uncooled Thermal Imaging Arrays, Systems, and Applications. ,  SPIE Press ,  Bellingham, WA  (2001).
Kimata  M., “Trends in small-format infrared array sensors,” in  Proc. Sensors , p. 1 ,  IEEE  (2013).
Stanley  R., “Plasmonics in the mid-infrared,” Nat. Photonics. 6, (7 ), 409  (2012). 1749-4885 CrossRef
Kawata  S., “Plasmonics: future outlook,” Jpn. J. Appl. Phys.. 52, (1 ), 010001  (2013).CrossRef
Smith  D. R., , Pendry  J. B., and Wiltshire  M. C., “Metamaterials and negative refractive index,” Science. 305, (5685 ), 788  (2004). 0036-8075 CrossRef
Tanaka  T., “Plasmonic metamaterials,” IEICE Electron. Express. 9, (2 ), 34  (2012).CrossRef
Ogawa  S.  et al., “Wavelength selective uncooled infrared sensor by plasmonics,” Appl. Phys. Lett.. 100, (2 ), 021111  (2012). 0003-6951 CrossRef
Ogawa  S.  et al., “Wavelength selective wideband uncooled infrared sensor using a two-dimensional plasmonic absorber,” Opt. Eng.. 52, (12 ), 127104  (2013).CrossRef
Masuda  K.  et al., “Optimization of two-dimensional plasmonic absorbers based on a metamaterial and cylindrical cavity model approach for high-responsivity wavelength-selective uncooled infrared sensors,” Sens. Mater.. 26, (4 ), 215  (2014). 0914-4935 
Takagawa  Y., , Ogawa  S., and Kimata  M., “Detection wavelength control of uncooled infrared sensors by two-dimensional lattice plasmonic absorbers,” Sensors. 15, (6 ), 13660  (2015). 0746-9462 CrossRef
Ogawa  S.  et al., “Polarization-selective uncooled infrared sensor with asymmetric two-dimensional plasmonic absorber,” Opt. Eng.. 53, (10 ), 107110  (2014).CrossRef
Ogawa  S., , Takagawa  Y., and Kimata  M., “Polarization-selective uncooled infrared sensor using a one-dimensional plasmonic grating absorber,” Proc. SPIE. 9451, , 94511K  (2015). 0277-786X CrossRef
Ohtera  Y., and Yamada  H., “Photonic crystals for the application to spectrometers and wavelength filters,” IEICE Electron. Express. 10, (8 ), 20132001  (2013).CrossRef
Han  S. W.  et al., “Design of infrared wavelength-selective microbolometers using planar multimode detectors,” Electron. Lett.. 40, (22 ), 1410  (2004).CrossRef
Shea  R. P., , Gawarikar  A. S., and Talghader  J. J., “Midwave thermal infrared detection using semiconductor selective absorption,” Opt. Express. 18, (22 ), 22833  (2010). 1094-4087 CrossRef
Haïdar  R.  et al., “Free-standing subwavelength metallic gratings for snapshot multispectral imaging,” Appl. Phys. Lett.. 96, (22 ), 221104  (2010). 0003-6951 CrossRef
Kamerman  G. W.  et al., “Polarization state imaging in long-wave infrared for object detection,” Proc. SPIE. 8897, , 88970R  (2013). 0277-786X CrossRef
Hao  J.  et al., “High performance optical absorber based on a plasmonic metamaterial,” Appl. Phys. Lett.. 96, (25 ), 251104  (2010). 0003-6951 CrossRef
Maier  T., and Brueckl  H., “Multispectral microbolometers for the midinfrared,” Opt. Lett.. 35, (22 ), 3766  (2010). 0146-9592 CrossRef
Watts  C. M., , Liu  X., and Padilla  W. J., “Metamaterial electromagnetic wave absorbers,” Adv. Mater.. 24, (23 ), OP98  (2012). 0935-9648 CrossRef
Feng  R.  et al., “Dual-band infrared perfect absorber based on asymmetric T-shaped plasmonic array,” Opt. Express. 22, (S2 ), A335  (2014). 1094-4087 CrossRef
Chen  Y. B., and Chiu  F. C., “Trapping mid-infrared rays in a lossy film with the Berreman mode, epsilon near zero mode, and magnetic polaritons,” Opt. Express. 21, (18 ), 20771  (2013). 1094-4087 CrossRef
Ogawa  S.  et al., “Three-dimensional plasmonic metamaterial absorbers for high-performance wavelength selective uncooled infrared sensors,” Proc. SPIE. 9070, , 90701Y  (2014). 0277-786X CrossRef
Ogawa  S., , Fujisawa  D., and Kimata  M., “Three-dimensional plasmonic metamaterial absorbers based on all-metal structures,” Proc. SPIE. 9451, , 94511K  (2015). 0277-786X CrossRef
Ogawa  S.  et al., “Mushroom plasmonic metamaterial infrared absorbers,” Appl. Phys. Lett.. 106, (4 ), 041105  (2015). 0003-6951 CrossRef
Sievenpiper  D.  et al., “High-impedance electromagnetic surfaces with a forbidden frequency band,” IEEE Trans. Microwave Theory Tech.. 47, (11 ), 2059  (1999). 0018-9480 CrossRef
Kaipa  C. S. R., , Yakovlev  A. B., and Silveirinha  M. G., “Characterization of negative refraction with multilayered mushroom-type metamaterials at microwaves,” J. Appl. Phys.. 109, (4 ), 044901  (2011). 0021-8979 CrossRef
Rakic  A. D.  et al., “Optical properties of metallic films for vertical-cavity optoelectronic devices,” Appl. Opt.. 37, (22 ), 5271  (1998). 0003-6935 CrossRef
Neubrech  F.  et al., “Properties of gold nanoantennas in the infrared,” in Electronics and Photonics. , and Rahman  F., Ed., p. 210 ,  World Scientific Publishing Co. ,  Singapore  (2008).
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