Drift Tube

Abstract

Disclosed is a drift tube formed of a hollow cylindrical conductive element having a having an inner surface and a pair of ends. A periodic grating surface is formed on the inner surface of the hollow cylindrical element and the ends are radiused to minimize electrical stress buildup. The interaction between a relativistic electron beam from an electron source passing through the inner space of the hollow element and the internal grating produces RF radiation by the Smith-Purcell Effect. Spacing, face angle and shape of the grating, and the energy of the electron bean are determinants of the frequency of the RF radiation.

Description

FIELD OF THE INVENTION

The present invention relates to a drift tube modified to enable output of higher frequencies from a high power RF source incorporating the drift tube.

BACKGROUND OF THE INVENTION

Prior art Magnetically Insulated Linear Oscillators (MILOs) are high power RF sources, which have typical outputs between 300 MHz and 3.5 GHz. For various applications, it would be desirable to provide a high power RF sources that can achieve even higher frequencies.

SUMMARY OF THE INVENTION

The present invention relates to a drift tube which includes a hollow cylindrical conductive element having a periodic grating surface formed on its inner surface, with the ends of the cylindrical conductive element being radiused to minimize electrical stress buildup.

The interaction between a relativistic electron beam from an electron source passing through the inner space of the hollow element and the internal grating produces RF radiation by the Smith-Purcell Effect. The spacing, face angle and shape of the grating, and the energy of the electron beam, are determinants of the frequency of the RF radiation.

The foregoing drift tube, having a periodic grating on the inner surface of a cylindrical drift tube, can be used advantageously to increase the frequency output of such devices as a Magnetically Insulated Linear Oscillator (MILO) beyond the aforementioned range of 300 MHz to 3.5 GHz mentioned for a MILO.

Other advantages and features of the invention will become apparent from reading the detailed description in conjunction with the drawing figures.

DESCRIPTION OF THE DRAWINGS

FIG. 1 is a sectional view along the length of a combined SXE-MILO driver.

FIG. 2 is a partly sectional view along the length of the MILO RF head of FIG. 1.

FIG. 3A is a sectional along the length of a Drift Tube used in the MILO RF head of FIG. 1, and FIG. 38 is an enlarged view of the circled region in FIG. 3A entitled “FIG. 3B”.

DETAILED DESCRIPTION OF THE INVENTION

A list of drawing reference numbers. their associated parts and preferred materials for the pails can be found near the end of this description of the preferred embodiments.

Combined SXE and RF Energy Drivers

In an example of a fusion reaction taken from U.S. Patent Publication No. 2008/0063132 A1, energy drivers produce X-ray beams at high fluency which symmetrically compress a target to initiate and sustain the fusion reaction. in one example, such energy drivers are preferably Stimulated X-ray Emitters (SXE) as first described by the inventor of this current invention in U.S. Pat. No. 4,723,261. In a preferred embodiment, the mentioned SXE drivers are fitted with an RF producing means which provides a simultaneous pulse of RF energy to provide additional heat to the reaction.

FIG. 1 shows a cross-section of an SXE combined with a Magnetically Insulated Linear Oscillator (MILO) at the output (right-shown) end of the SXE. The MILO is another well known, high power RF source, similar to the Vircator. The significant difference is that it can produce much higher frequencies than the Vircator. Structurally, the major difference is the incorporation of a drift tube 122 of FIG. 3A and use of a Traveling Wave Electron Gun (TWEE) instead of the planar cathode 90 and grid 92 of the Vircatron. There is a resonant cavity 98 and its dimensions in conjunction with the dimensions of the drift tube 122 (FIG. 3A) determine the output range. Conventional MILO devices have outputs between 300 MHz and 3.5 GHz. The inventor of the present invention has experimentally verified that by placing a grating surface on the inner face of the drift tube 122 (FIG. 3A), as shown in FIG. 3B, it is possible to generate RF at much higher frequencies than those available from a smooth bore drift tube 122. The source of this RF is due to the Smith-Purcell effect which describes the interaction of a relativistic electron beam with a grating surface 123. Outputs in the THz range are possible. The grating surface can be formed by many methods. The spacing, face angle and grating geometry all are determinants in the frequency achieved (FIG. 3B). It has been determined that the preferred embodiment of the drift tube grating is an internal thread as shown in FIGS. 3A and 3B. By altering the thread parameters, the output frequency is changed. The ends of the Drift Tube 125 are radiused to minimize formation of undesirable electric field perturbations inside the Resonant Cavity 98.

The balance of the SXE-MILO driver is the same as the SXE-Vircator. In fact, the RF heads—Vircator and MILO—can be interchanged. As in the case of the SXE-Vircator, the TWEG of the MILO has a hollow center through which the x-rays pass. The electron output from the TWEG is compressed by the drift tube 122 and oscillates in the resonant cavity 98.

DRAWING REFERENCE NUMBERS

The following list of drawing reference numbers has three columns. The first column includes drawing reference numbers; the second column specifies the parts associated with the reference numbers; and the third column mentions a preferred material (if applicable) for the parts.

REFERENCE NUMBER LIST	PREFERRED MATERIAL
64	Anode	Refractory Metal; Hi-Z
66	Grid	Refractory Metal
68	Cathode	Graphite (Preferred
		Embodiment)
70	Coaxial Capacitor	Dielectric/Metal Layers
72	Cathode Feedthrough	Ceramic & Metal
74	Grid Feedthrough	Ceramic & Metal
78	Radiation Shield	Lead
94	Anode Mesh	Refractory Metal
96	Output Window	RF Transparent Low-Z
		Ceramic
98	Resonant Circular Cavity	Stainless Steel or Copper
100	Mounting Flange	Stainless Steel
102	Cathode Feedthrough	Ceramic & Metal
106	Grid Feedthrough	Ceramic & Metal
110	Getter Pump	n/a
112	Getter Pump Feedthrough	Ceramic & Metal
114	MILO Cathode	Graphite
116	MILO Cathode Support	Refractory Metal
118	MILO Grid	Refractory Metal
120	MILO Grid support	refractory Metal
122	Drift Tube	Refractory Metal
123	Grating Surface	Refractory Metal
124	Drift Tube Support	Ceramic
125	Radiused end of Drift Tube	Refractory Material
126	Internal Anode Insulator	Ceramic
142	Grid Output Terminal	Refractory Metal

The foregoing adescribes a drift tube where the inclusion of a periodic grating surface on the inner surface of the tube generates higher frequencies of RF radiation.

While the invention has been described with respect to specific embodiments by way of illustration, many modifications and changes will occur to those skilled in the art. It is, therefore to be understood that the appended claims are intended to cover all such modifications and changes as fall within the true scope and spirit of the invention.

Claims

1-27. (canceled)

28. A drift tube, comprising: a) a hollow cylindrical conductive element having an inner surface and a pair of ends; a periodic grating surface being formed on the inner surface of the hollow cylindrical element and said ends being radiused to minimize electrical stress buildup;b) the interaction between a relativistic electron beam, from an electron source passing through the inner space of the hollow element, and the internal grating producing RE radiation by the Smith-Purcell Effect; andc) spacing, face angle and shape of the grating, and the energy of the electron beam being determinants of the frequency of the RF radiation.

29. The drift tube of claim 28, wherein the periodic grating surface comprises a continuous threaded surface.

30. The drift tube of claim 28, wherein the drift tube is electrically isolated from he electron beam source.