Nanowire based plasmonics

• US 8,120,014 B2
• Filed: 12/15/2005
• Issued: 02/21/2012
• Est. Priority Date: 12/15/2004
• Status: Active Grant

• Current Assignee: Drexel University
• Original Assignee: Drexel University
• Inventors: Nabet, Bahram, Spanier, Jonathan E.
• Primary Examiner(s): Jackson, Jr., Jerome
• Application Number:
  US11/304,049
• Publication Number:
  US 20060289761A1
• Time in Patent Office: 2,259 Days
• Field of Search: 257 9- 30, 385/1, 372 43- 45
• US Class Current: 257/21
• CPC Class Codes: G01N 21/3581 using far infrared light; using Terahertz radiation
• CPC Class Codes: H01L 31/108 the potential barrier being of the Schottky type

Abstract

Nanoscaled, tunable detector devices for ultrasensitive detection of terahertz (THz) radiation based on the fabrication of one-dimensional (1D) plasma devices having clouds of strongly correlated and spatially confined electronic charge carriers are disclosed. These one-dimensional collective excitations (“plasmons”) are realized using coaxial semiconducting core-shell nanowires or by electrostatically confining a two dimensional charge to one dimension. By exploiting the properties of plasmons confined to reduced dimensions and under a selected device configuration, conventional limitations on carrier drift and transit times that dictate the speed and sensitivity of transistors can be circumvented, and detector sensitivity can be improved. 1D devices with sub-picosecond response times will be important for a range of applications in diverse areas such as remote sensing and imaging, molecular spectroscopy, biotechnology, and in a range of the spectrum that has been difficult to detect. In addition to electromagnetic radiation these devices can be used as detectors of charged particle perturbations.

Claims

1. A detector for detecting electromagnetic radiation and charged particles comprising:

an inner material;

an outer material surrounding said inner material;

a one-dimensional plasma in the detector having a confined charge at quasi-equilibrium,

Schottky contacts associated with at least one of said inner and outer materials, wherein said Schottky contacts are located at ends of the confined charge;

wherein the detector is tuned to a resonant frequency by modulating the composition and the band-gap along a detector length and

wherein said one-dimensional plasma forms a collective response.

2. The detector of claim 1, wherein said electromagnetic radiation is terahertz radiation.

3. The detector of claim 1, wherein said resonant frequency is adjusted by controlling charge carrier density.

4. The detector of claim 3, wherein said charge carrier density is further adjusted by doping of said inner or outer material.

5. The detector of claim 3, wherein said one-dimensional plasma comprises at least one energy gap.

6. The detector of claim 1, further comprising an additional one-dimensional plasma confined in the detector.

7. The detector of claim 6, wherein the collective charge carrier behavior of said additional one-dimensional plasma is different than the collective charge carrier behavior of said one-dimensional plasma.

8. A detector for detecting electromagnetic radiation and charged particles comprising:

a core comprised of a first material;

a shell comprised of a second material;

reflective ends;

a one-dimensional plasma having a confined charge at quasi-equilibrium in the shell;

Schottky contacts directly contacting said core;

wherein an energy gap of the core is periodically spatially modulated to tune to a resonant frequency; and

wherein said first material is a wider-gap material than said second material.

9. A detector for detecting electromagnetic radiation and charged particles comprising:

an inner material;

an outer material surrounding said inner material;

a one-dimensional plasma in the detector having a confined charge, wherein said one-dimensional plasma collectively carries negative or positive charge;

Schottky contacts associated with at least one of said inner and outer materials wherein said Schottky contacts are located at ends of the confined charge; and

wherein the core has a sinusoidal variation in composition to adjust said resonant frequency by controlling charge carrier density.