2009
DOI: 10.1063/1.3186065
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Characterization of terahertz field confinement at the end of a tapered metal wire waveguide

Abstract: We present experimental verification of the possibility of strong subwavelength confinement of the terahertz electric field at the end of a tapered metal wire waveguide. The axial field component at the end of the tapered waveguide shows a lateral confinement that is an order of magnitude greater than an untapered waveguide, and over 100 times greater than the free-space wavelength. The axial component is also strongly confined in the propagation direction, in contrast to the radial field component. Comparison… Show more

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Cited by 54 publications
(24 citation statements)
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“…The authors map the field at the end of two different wire waveguides, one with a flat end, and the second with a tapered end [101]. Figure 19 shows the z-component of the electric near-field, parallel to the wire, at its apex along the x-direction, perpendicular to the wire axis.…”
Section: Plasmonics On a Flat Surfacementioning
confidence: 99%
“…The authors map the field at the end of two different wire waveguides, one with a flat end, and the second with a tapered end [101]. Figure 19 shows the z-component of the electric near-field, parallel to the wire, at its apex along the x-direction, perpendicular to the wire axis.…”
Section: Plasmonics On a Flat Surfacementioning
confidence: 99%
“…gradual narrowing of a waveguide towards one end [15][16][17][18][19][20][21][22][23][24][25][26] . Field confinement at the end of a tapered metal wire waveguide was demonstrated experimentally 4,[27][28][29] .…”
Section: Introductionmentioning
confidence: 99%
“…Similarly, in [514] a SWW of diameter d = 2a = 500 µm is tapered to a tip of 20 µm of diameter, obtaining that the E-field is confined in a radius one order of magnitude less than for the conventional thick SWW and two orders of magnitude less than free space. Specifically, near the tip, the Full Width at Half Maximum (FWHM) of the E-field is located at r = 30 µm.…”
Section: Surface and Plasmonic Waveguidesmentioning
confidence: 97%
“…Moreover, due to the exponential grow of losses as a decreases, and the foreseeable manufacturing complexity, DCSWW designs with radius between a = 5 µm and a = 20 µm are preferred. As a data of interest, successful experiments with small radius SWW/DCSWW (a = 10 µm to a = 30 µm) [507], [513], [514], and manufacturing of DCSWW with conductor radius ranging from a = 0.4 µm to a = 15 µm and coating thickness ranging t from t = 2 µm to t = 15 µm have been reported in the last years [589].…”
Section: Solution A: Reduction Of the Wire Radius 421 Strict Monomomentioning
confidence: 99%
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