Optical and electronic devices based on nano-plasma
A device for detecting electromagnetic radiation, charged particles or photons including a 2-dimensional electron gas (2DEG) and/or a 2-dimensional hole gas (2DHG). The device detects the collective response of the plasma to perturbations of the 2DEG and/or the 2DHG. The device is tunable by using Schottky contacts. The device can be used for high-speed photodetector devices, terahertz sensors, and charged particle sensors.
1. A detector for detecting electromagnetic radiation or charged particles comprising:
a substrate;
a two-dimensional reservoir of charge formed on said substrate;
an AlGaAs layer formed on said two-dimensional reservoir of charge;
Schottky contacts formed directly on said first AlGaAs layer,
a coupling apparatus for coupling electromagnetic radiation or charged particles with said two-dimensional reservoir of charge; and
a detection device for detecting a perturbation in said two-dimensional reservoir of charge by measuring a resonant frequency of one or more plasmons, or measuring the change in current across the Schottky contacts;
wherein said detection device detects electromagnetic radiation, said two-dimensional plasma comprises charge carriers, and a resonant frequency response of electromagnetic radiation produced in said charge carriers at a resonant frequency forms said one or more plasmons.
2. The detector of claim 1 , wherein said electromagnetic radiation is terahertz radiation.
3. The detector of claim 1 , further comprising tuning means for adjusting said resonant frequency.
4. The detector of claim 3 , wherein said tuning means adjusts said resonant frequency by controlling charge carrier density.
5. The detector of claim 4 , wherein said charge carrier density is adjusted by gating using another Schottky contact.
6. The detector of claim 1 , further comprising a second layer made of a material selected from the group consisting of GaAs, InP, GaN, and Si.
7. The detector of claim 1 , wherein said Schottky contacts are made of a material selected from the group consisting of Ti—Au and SiN.
8. The detector of claim 1 , wherein said two-dimensional reservoir of charge comprises a two-dimensional electron gas.
9. The detector of claim 1 , wherein said two-dimensional reservoir of charge comprises a two-dimensional hole gas.
10. A method for detecting electromagnetic radiation comprising the steps of:
forming a two-dimensional reservoir of charge by providing;
a substrate;
a two-dimensional reservoir of charge formed on said substrate;
an AlGaAs layer formed on said two-dimensional reservoir of charge;
Schottky contacts formed directly on said AlGaAs layer,
a coupling apparatus for coupling electromagnetic radiation or charged particles with said two-dimensional reservoir of charge; and
a detection device for detecting a perturbation in said two-dimensional reservoir of charge by measuring a resonant frequency of one or more plasmons, or measuring the change in current across the Schottky contacts; and
perturbing said two-dimensional reservoir of charge with electromagnetic radiation; and
detecting a resonant frequency of plasmons of said two-dimensional reservoir of charge by measuring a resonant frequency of said plasmons, or measuring change in current across Schottky contacts.
11. The method of claim 10 , further comprising the step of establishing an electrical contact via blocking of Schottky contacts.
12. The method of claim 10 , wherein said electromagnetic radiation is terahertz radiation.
13. The method of claim 12 , further comprising the step of tuning said resonant frequency by adjusting a charge carrier concentration in said two-dimensional reservoir of charge.
14. A photodetector device comprising:
a substrate;
a two-dimensional electron gas and a two-dimensional hole gas formed on said substrate;
an AlGaAs layer formed on at least one of said two-dimensional electron gas and said two-dimensional hole gas;
a plurality of Schottky contacts located directly on said AlGaAs layer; and
a detection device for detecting a perturbation in said two-dimensional reservoir of charge by measuring a resonant frequency of plasmons, or measuring change in current across the plurality of Schottky contacts; wherein said two-dimensional hole gas collects optically generated holes and said two dimensional electron gas collects optically generated electrons, thereby substantially reducing the tail of a response of said photodetector device.
15. The photodetector device of claim 14 , wherein said two-dimensional reservoir of charge comprises charge carriers, wherein a resonant frequency response caused by electromagnetic radiation is produced in said charge carriers thereby forming one or more plasmons.
16. The photodetector device of claim 15 , further comprising a tuner for tuning said resonance frequency.
17. The photodetector device of claim 16 , wherein the tuner for tuning said resonance frequency comprises structure for adjusting a charge carrier concentration in said two-dimensional reservoir of charge.