2011
DOI: 10.1063/1.3647633
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High efficiency resonance-based spectrum filters with tunable transmission bandwidth fabricated using nanoimprint lithography

Abstract: Articles you may be interested inHigh-speed tuning of visible laser wavelength using a nanoimprinted grating optical tunable filter Appl. Phys. Lett. 95, 211106 (2009); 10.1063/1.3267083Direct indium tin oxide patterning using thermal nanoimprint lithography for highly efficient optoelectronic devices

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Cited by 192 publications
(151 citation statements)
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(15 reference statements)
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“…Figure 1 (c) presents measured transmission spectra of the cyan (P 5 350 nm), magenta (P 5 270 nm) and yellow (P 5 230 nm) plasmonic SCFs under TMpolarization (Supplementary Figure S2), with transmission minima that are positioned in red, green, and blue spectral regions, respectively. Note that the observed absolute peak transmission, 60 , 70% in the visible region, represent an unusually high transmission efficiency for such structures 2,3,[6][7][8][9][10][11][12][13][14] . The full-widths at half maximum (FWHM) of the stopbands are approximately 100 nm for yellow and cyan SCFs, and 160 nm for magenta SCFs, which are comparable to the passband width for state-of-art plasmonic ACFs 2,3 .…”
Section: Resultsmentioning
confidence: 99%
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“…Figure 1 (c) presents measured transmission spectra of the cyan (P 5 350 nm), magenta (P 5 270 nm) and yellow (P 5 230 nm) plasmonic SCFs under TMpolarization (Supplementary Figure S2), with transmission minima that are positioned in red, green, and blue spectral regions, respectively. Note that the observed absolute peak transmission, 60 , 70% in the visible region, represent an unusually high transmission efficiency for such structures 2,3,[6][7][8][9][10][11][12][13][14] . The full-widths at half maximum (FWHM) of the stopbands are approximately 100 nm for yellow and cyan SCFs, and 160 nm for magenta SCFs, which are comparable to the passband width for state-of-art plasmonic ACFs 2,3 .…”
Section: Resultsmentioning
confidence: 99%
“…Plate-like dielectric deflectors have recently been proposed 1 , but this scheme suffers from intrinsic limitations due to poor color purity, since the deflector covers only half of the total area. Nanoplasmonic color filters have been proposed recently as a promising means of overcoming the above limitations [2][3][4][5][6][7][8][9][10][11] . The well-known extraordinary optical transmission (EOT) phenomenon [12][13][14] , observed in a single opticallythick metal film perforated with a periodic subwavelength hole array, has been extensively studied for additive color filtering (ACF) applications over the past decade.…”
mentioning
confidence: 99%
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“…Authors have investigated the use of different metals (Au [2], Ag [3][4][5][6][7][8], Al [9][10][11][12][13][14][15][16][17][18][19][20][21][22][23][24][25]) and various aperture forms such as lines [4,5,10,24], circles [7, 9, 11, 14-16, 21, 25], triangles [12] and crosses [17,18,23]. Alternatively, a similar filtering behaviour can also be achieved by the formation of subwavelength metal islands [8,20].…”
Section: Introductionmentioning
confidence: 99%
“…Very often serial techniques like focused ion beam (FIB) [3,10,15,21], electron beam lithography [9,11,12,14,24,25] or advanced optical lithography [22,26] as well as x-ray lithography [8] have been used in the fabrication process, including their intrinsic limitations in terms of patterning area or process time. Other approaches rely on parallel lithography techniques like nanoimprint lithography (NIL) [4,18] or laser interference lithography (LIL) [16], thereby enabling the time efficient patterning of larger areas. However, the maximum active areas of the filters presented in literature remain in the order of a few cm 2 .…”
Section: Introductionmentioning
confidence: 99%