Radiation detector including field effect transistor in resonant cavity nanostructure
A radiation detection device includes a plurality of field effect transistors (FETs) arranged to form a resonant cavity. The cavity includes a first end and a second end. The plurality of FETs provide an electromagnetic field defining an standing wave oscillating at a resonant frequency defined by a characteristic of the cavity. A radiation input passing through the cavity induces a perturbation of the electromagnetic field.
1. A radiation detection device comprising:
a plurality of field effect transistors (FETs) arranged to form a resonant cavity, the cavity including a first end and a second end, the plurality of FETs providing an electromagnetic field defining a standing wave oscillating at a resonant frequency defined by a characteristic of the cavity, a radiation input passing through the cavity inducing a perturbation of the electromagnetic field; and
an optical coating.
2. The radiation detection device of claim 1 , wherein each of the FETs is a uniformly flat mesa long gate FET.
3. The radiation detection device of claim 1 , wherein the resonant cavity is a first resonant cavity, and further comprising a second plurality of FETs arranged to form a second resonant cavity, the first resonant cavity and the second resonant cavity arranged in a periodic array, the first resonant cavity and the second resonant cavity sharing a common wall formed by one of the FETs.
4. The radiation detection device of claim 3 , wherein the first resonant cavity is configured to detect radiation originating from a first source type, and the second resonant cavity is configured to detect radiation originating from a second source type.
5. The radiation detection device of claim 1 , wherein the resonant cavity is continually adjusted to vary the resonant frequency in order to scan for radiation originating from a variety of source types.
6. The radiation detection device of claim 1 , wherein the characteristic is a length of the cavity extending between the first end and the second end, wherein the length of the cavity is adjustable.
7. The radiation detection device of claim 1 , wherein at least a portion of each of the FETs is formed from a piezoelectric material, permitting a length of the cavity to be adjusted.
8. The radiation device of claim 7 , wherein adjusting a length of the cavity adjusts the resonant frequency.
9. The radiation detection device of claim 8 , wherein the resonant frequency is adjustable to target radiation emitted by a predetermined source material.
10. The radiation detection device of claim 1 , wherein the resonant cavity extends along a longitudinal axis between the first end and the second end, the resonant cavity having a hexagonal cross-section.
11. The radiation detection device of claim 1 , wherein the plurality of FETs includes at least two FETs oriented parallel to one another, the radiation detection device measuring time-of-flight of the radiation input.
12. The radiation detection device of claim 1 , further comprising a gamma focusing coating.
13. The radiation detection device of claim 1 , further comprising an integrated nano antenna configured to direct energy to a down-converting Schottkey barrier detector mixer diode structure.
14. The radiation detection device of claim 1 , wherein electrons within the resonant cavity concentrate near each peak of the standing wave, the perturbation caused by the radiation input inducing a fluctuation in the electromagnetic field.
15. The radiation detection device of claim 1 , wherein the radiation detection device is operable at room temperature.
16. The radiation detection device or method of claim 1 , wherein each of the FETs includes a GaN semiconductor.
17. A method of detecting radiation comprising:
tuning a detector cavity to be resonant with a frequency of radiation emitted by a target radiation source;
receiving an incident radiation within the detector cavity;
detecting an incident frequency of the incident radiation, wherein the incident frequency of a single gamma photon or neutron is detected and isolated from any other incident frequency.
18. The method of claim 17 , further comprising,
down converting the incident frequency to an output frequency; and
passing the output frequency to a processor configured to store, analyze, and/or visualize the output frequency.
19. The method of claim 18 , wherein a plurality of output frequencies are passed to the processor simultaneously.
20. The method of claim 17 , further comprising determining at least one of a source, speed, energy, and direction of the incident radiation.
21. The method of claim 17 , wherein tuning the detector cavity includes continuously varying the resonant frequency to scan a range of frequencies.
22. The method of claim 17 , wherein the detector includes a stacked two-dimensional array of hexagonal resonant cavities, wherein the walls of the resonant cavities are formed by mesa long gate field effect transistors.
23. The method of claim 17 , wherein tuning the cavity includes adjusting a length of a plurality of long gate field effect transistors defining the cavity.
24. The method of claim 23 , wherein at least a portion of each of the field effect transistors is formed from a piezoelectric material.
25. The method of claim 17 , wherein receiving an incident radiation within the detector cavity induces a perturbation in an electromagnetic field, wherein detecting the incident radiation includes detecting the perturbation.