1. Field of the Invention
The present invention relates generally to apparatus for producing terahertz (THz) radiation. More specifically, the present invention relates to a microelectromechanical system (MEMS)-based reverse magnetron apparatus for producing THz radiation.
2. Description of the Related Art
Most current sources of THz radiation are either very dim (e.g. nonlinear down conversion of optical lasers generate typically nanowatt (nW) outputs), very inefficient, or both (e.g. far infrared lasers have a power output in the THz region of few milliwatts (mW) but efficiencies of about 0.01%). Such conventional THz radiation sources are described in P. H. Siegal, “THz Technology: An Overview”, International Journal of High Speed Electronics and Systems, Vol. 13, No. 2 (2003), which is herein incorporated by reference.
Quantum cascade lasers can be as bright as 50 mW, but they require cryogenic cooling. Unfortunately, other apparatus capable of generating intense sources of THz radiation are uniformly bulky and difficult to transport (e.g. free electron laser and synchrotron radiation sources).
Magnetrons have featured prominently in the production of intense microwave radiation, as described in, for example, Victor L. Granatstein and Igor Alexeff, ed., High Power Microwave Sources, Boston: Artech, 1987, herein incorporated by reference. While the external configurations of different conventional magnetrons vary, the basic internal structures are generally the same—these include a central filament/cathode, an outside anode cylinder concentric to the cathode, an antenna, and magnets. The motion of electrons is due to the combined influence of cross electric (radial) and magnetic (axial) fields. In this case, the radiation frequency is near to the cyclotron frequency and amplification is achieved as the whirling cloud of electrons, influenced by the high voltage and the strong magnetic field, forms a rotating pattern that resembles the spokes in a spinning wheel and interacts with an alternating current flow in the resonant cavities configured at the inner surface of the anode. In order to achieve radiation frequencies in the THz region, unrealistically large magnetic fields, of several Tesla, are required.
U.S. Pat. No. 7,274,147, issued to Shim et al., describes a MEMS-based apparatus, using a miniaturized magnetron and claims to generate THz radiation. In Shim et al. an anode block concentrically surrounds a cathode unit and the electrons spiral outward. The large magnetic field requirements for operation of this device in the THz region make this apparatus impractical.
In accordance with one embodiment, a terahertz (THz) reverse micromagnetron includes: a cathode ring having a central void; and an anode post centrally located within the central void of the cathode ring, wherein application of an applied voltage between the cathode ring and the anode post causes field-emitted electrons to be accelerated radially inwards producing radiation.
In accordance with another embodiment, a THz reverse micromagnetron chip includes a plurality of terahertz (THz) reverse micromagnetrons, each THz reverse micromagnetron including: a cathode ring having a central void; and an anode post centrally located within the central void of the cathode ring, wherein application of an applied voltage between the cathode ring and the anode post causes field-emitted electrons to be accelerated radially inwards producing radiation. In one embodiment, the chip has a width of about 1 cm and a length of about 1 cm and includes several hundred of the THz reverse micromagnetrons. In one embodiment, the chip includes a conductive substrate electrically connecting each anode post of the plurality of THz reverse micromagnetrons. In one embodiment, the chip includes a void centrally located on the chip. In one embodiment, this void has an area of at least 1/9 of a total surface area of the chip.
In accordance with a further embodiment, a terahertz (THz) reverse micromagnetron assembly includes: a chip mount, the chip mount adapted to mount a chip; a chip mounted on the chip mount, the chip including: a plurality of terahertz (THz) reverse micromagnetrons, each THz reverse micromagnetron including: a cathode ring having a central void; and an anode post centrally located within the central void of the cathode ring wherein the chip has a void centrally located on the chip; a a magnet assembly having a first pole and a second pole arranged in a push-pull configuration, wherein each of the first pole and the second pole has a central void, and wherein the chip mount is positioned between the first pole and the second pole of the magnet assembly; a first reflecting mirror and a second reflecting mirror, wherein the first reflecting mirror and the second reflecting mirror form a confocal cavity having a confocal point, further wherein the chip is positioned in the confocal plane of the confocal cavity; and wherein application of an applied voltage between the cathode ring and the anode post causes field-emitted electrons to be accelerated radially inwards producing radiation.
Embodiments in accordance with the invention are best understood by reference to the following detailed description when read in conjunction with the accompanying drawings.
Broadly viewed, embodiments in accordance with the terahertz (THz) reverse micromagnetron include a centrally located anode surrounded by a cathode ring, herein termed a “reverse-magnetron” configuration. When power is applied, electrons move radially inward in the combined electric and magnetic cross-fields and can reach orbiting angular frequencies in the THz region, even with a magnetic field of the order of 1 T or less. The terahertz reverse micromagnetron is portable, operates at room temperature, and can be bright. It has applicability in imaging and other applications where intense sources of radiation are needed, such as in the areas of improvised explosive device (IED) detection, airport security, imaging for medical, pharmaceutical, and semiconductor applications, and spectroscopy for large chem-bio molecules.
Referring to
In one embodiment, anode post 12 is conductively connected to a conductive substrate 18 and is electrically insulated from cathode ring 14 by a first insulating layer 20. In one embodiment, a conductive bonding material 22 is disposed between cathode ring 14 and insulating layer 20. In one embodiment, conductive bonding material 22 is a few microns thick and the thickness of anode post 12 and cathode ring 14 is about 100 μm. In one embodiment, terahertz reverse micromagnetron 26 further includes a top substrate 24 that hermetically seals the THz reverse micromagnetron 26 for vacuum packaging. In one embodiment, a second insulating layer 20 is disposed between top substrate 24 and the underlying structures. In one embodiment, first insulating layer 20 and second insulating layer 20 can be formed of the same material. In some embodiments, first insulating layer 20 and second insulating layer 20 can be formed of different materials.
In various embodiments, the dimensions of cathode ring 14 can vary according to the radiation frequency. In embodiment, the diameter of cathode ring 14 is at or about 100 μm and the diameter of anode post 12 is at or about 10 μm. Herein the diameter of cathode ring 14 refers to the diameter of the void within which anode post 12 is located. Herein the diameter of anode post 12 is the outer diameter of anode post 12. An applied voltage between cathode ring 14 and anode post 12 can yield field-emitted electrons which, in turn, can be accelerated radially inwards. Scalloping 16, formed on the inside surface of cathode ring 14, can facilitate generation of the field-emitted electrons.
In one embodiment, the radiation output can be enhanced by utilizing an array of THz reverse micromagnetrons.
Referring to
Referring now to
In one embodiment, a through-hole is formed by the central voids in the two poles of magnet assembly 42 and central void 32 in chip 28. This through-hole allows radiation to bounce back and forth in confocal cavity 46 between first mirror 48A and second mirror 48B. In this embodiment, electromagnetic coupling among all THz reverse micromagnetrons 26 of chip 28 can be established, encouraging coherent radiation among all the THz reverse micromagnetrons 26.
In one embodiment THz reverse micromagnetron assembly 40 has a Q of at least 100,000 and a magnetic field of at most 1 T. In one embodiment, because the size of each THz reverse magnetron apparatus 26 is less than 200 μm, i.e., less than a wavelength of THz light, there exists the possibility of intrinsically coherent radiation due to the natural spatial bunching of the electrons.
In one embodiment, the theoretical DC power requirements for THz reverse micromagnetron assembly 40 ranges from about 15 W to about 100 W. With the confocal cavity configurations shown in
In one embodiment, an external solenoid can be utilized to provide frequency tunability of THz reverse micromagnetron assembly 40. In a further embodiment, a cell containing a liquid (e.g., benzene) can be inserted, whereby metastable rotational states with transition frequencies in the THz can be excited, acting as an amplifier.
This disclosure provides exemplary embodiments of the invention. The scope of the invention is not limited by these exemplary embodiments. Those of skill in the art can understand that embodiments in accordance with the invention can also be scaled up or down in size to accommodate various applications. Numerous variations, whether explicitly provided for by the specification or implied by the specification or not, may be implemented by one of skill in the art in view of this disclosure.
This application claims the benefit of U.S. Provisional Patent Application No. 61/248,301, filed Oct. 2, 2009, which is hereby incorporated in its entirety by reference.
Number | Name | Date | Kind |
---|---|---|---|
3289035 | Drexler | Nov 1966 | A |
3289036 | Bowers et al. | Nov 1966 | A |
3290548 | Feulner | Dec 1966 | A |
3479556 | Cook | Nov 1969 | A |
4542321 | Singh et al. | Sep 1985 | A |
5215703 | Bernardet | Jun 1993 | A |
5676873 | Takase et al. | Oct 1997 | A |
5805025 | Kwan et al. | Sep 1998 | A |
6525477 | Small | Feb 2003 | B2 |
7274147 | Shim et al. | Sep 2007 | B2 |
7714513 | Gorrell et al. | May 2010 | B2 |
7728397 | Gorrell et al. | Jun 2010 | B2 |
7935930 | Gorrell | May 2011 | B1 |
20100259273 | Kawasaki et al. | Oct 2010 | A1 |
Entry |
---|
Siegel, P.N. “Terahertz technology,” IEEE Transactions on Microwave Theory and Techniques.vol. 50, No. 3. pp. 910-928, Mar. 2002. |
Number | Date | Country | |
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61248301 | Oct 2009 | US |