Abstract:
An electron beam controlled semiconductor switch is capable of carrying large currents without being restricted by the space charge limited current condition. The switch includes a block of semiconductor material having ohmic contacts connectable to first and second electrical conductors. Semi-insulating GaAs may be used as the semiconductor material. A shallow donor or acceptor doped layer may be formed at the surface receiving the electron beam for increased band-edge radiation. This recombination radiation ionizes, together with X-rays produced by Bremsstrahlung, the bulk of the semiconductor block to provide relatively high current density and current gain.

Description:
CROSS-REFERENCE TO RELATED APPLICATION 
     This is a continuation-in-part of U.S. patent application Ser. No. 082,546, filed Aug. 7, 1987, incorporated herein by reference. 
    
    
     BACKGROUND OF THE INVENTION 
     1. Field of the Invention 
     The present invention is related to electron beam controlled bulk semiconductor switches and, more particularly, to a switch which is not restricted by the space charge limited current condition and is capable of high current gain and high current density. 
     2. Description of the Related Art 
     Many varieties of optically controlled semiconductor switches exist, but electron beam controlled switches are less common. Photodiodes, phototransistors, photothyristors and light sensitive resistors are examples of the many types of optically controlled switches. The most commonly used light-sensitive semiconductor device is the photodiode which is used in many applications, including fiber optic communication systems, etc. The currents handled by such devices are relatively low, typically in the milliampere range. One example is the PIN diode taught by U.S. Pat. No. 4,240,088 to Myers. Other light-activated devices include the thyristors taught by U.S. Pat. Nos. 3,832,732 to Roberts and 4,001,865 to Voss, the microwave switching circuit taught by U.S. Pat. No. 4,396,833 to Pan and many other patents. Some, such as U.S. Pat. Nos. 4,626,883 to Kash et al. and 3,917,943 to Auston, describe switching elements with picosecond switching times. Other light activated switches, such as those taught by U.S. Pat. Nos. 4,438,331 to Davis and 4,376,285 to Leonberger et al., are able to carry a larger amount of current by making an entire block of semiconductor material  conductive; however, like photodiodes, they require continuous light to sustain conduction. 
     Electron-bombarded semiconductor (EBS) devices are highspeed switching devices which use an electron beam instead of light to control switching. EBS devices typically use electron beams of 10-15 keV and are limited in output power and current density due to the space charge limited current condition. While switching time is typically below ten nanoseconds, the current density is usually a few milliamperes per square millimeter with a current gain of 2000 or less. 
     Higher current densities, up to 10 2  A/cm 2  are provided by diffuse discharge switches, such as the switch taught by U.S. Pat. No. 4,063,130 to Hunter. However, while diffuse discharge switches can be turned ON in less than a nanosecond, they are relatively slow to turn OFF, taking approximately 100 nanoseconds and have a moderate current gain between 10 2  and 10 3 . 
     SUMMARY OF THE INVENTION 
     An object of the invention is to provide a semiconductor switch with a current density over 10 4  A/cm 2 . 
     Another object of the present invention is to provide a high current semiconductor switch with an operating voltage drop of less than 100 volts. 
     A further object of the present invention is to provide an electron beam controlled semiconductor switch with a current density unrestricted by the space charge limited current condition. 
     The above objects are attained by providing a switch operatively connectable between first and second electrical conductors, the switch comprising a block of semiconductor material having first and second ohmic contacts operatively connectable to the first and second electrical conductors, respectively, and electron beam means for directing an electron beam onto the block through the first contact to produce an electron-hole plasma throughout the block of semiconductor material between the contacts by direct impact, recombination radiation and Bremsstrahlung. 
     These objects, together with other objects and advantages which will be subsequently apparent, reside in the details of  construction and operation as more fully hereinafter described and claimed, reference being had to the accompanying drawings forming a part hereof, wherein like reference numerals refer to like parts throughout. 
    
    
     BRIEF DESCRIPTION OF THE DRAWINGS 
     FIG. 1 is a schematic diagram of an embodiment of the present invention; and 
     FIGS. 2A and 2B are a top and a cross-sectional side view of a semiconductor wafer with one ring-shaped contact, as used in a second embodiment of the present invention. 
    
    
     DESCRIPTION OF THE PREFERRED EMBODIMENTS 
     As illustrated in FIG. 1, an electron beam controlled switch 10 according to the present invention includes a block 12 of semiconductor material with ohmic contacts 15-16 operatively connectable to the electrical conductors 17 and 18. A space of a micron to a few centimeters may be used to separate contact 15 from contact 16. An electron beam 20 is used to initiate and maintain conductivity in the switch 10. The electron beam 20 may be generated in a vacuum tube diode 22 which emits electrons from a cathode 24 through an anode foil 26. The electron beam 20 passes through the vacuum chamber wall and strikes the surface of the semiconductor block 12 through contact 15. Energization of the diode 22 may be controlled in a conventional manner. A pulsing circuit 30 as illustrated in FIG. 1 as including a spark gap switch 32, pulse forming network 34 and pulse transformer 36. A pulsing circuit like that illustrated in FIG. 1 has been used to produce a one microsecond pulse. 
     When the block 12 of semiconductor material is formed of a highly resistive direct semiconductor material, such as semi-insulating gallium arsenide (GaAs), the electron beam 20 has a maximum energy for GaAs of approximately 200 keV since GaAs can suffer damage if the electron energy exceeds 220 keV. The lower limit of the electron energy in the embodiment illustrated in FIG. 1 is determined by the fact that the electron beam has to pass through the anode foil 26 and the contact 15. However, where the semiconductor contact 15 forms the anode of the electron beam diode 26, electrons with much lower energies, even as low as 10 keV can potentially be used. Low energy electron beams are more easily used if, as illustrated in FIGS. 2A and 2B, a ring-shaped contact 15&#39; is used instead of the solid contact illustrated in FIG. 1. Use of a ring-shaped contact requires that the highly conductive region formed by the electron beam at the surface of the block 12 of semiconductor material be able to serve as the inner portion of contact 15. 
     The range of electron energy for a device constructed according to the present invention is between the range of electron beams used in diffuse discharge switches (150-300 keV) and those used in electron-bombarded semiconductor (EBS) devices (10-15 keV). The capabilities of an electron-beam controlled bulk semiconductor switch according to the present invention is more similar to a diffuse discharge switch than an EBS device, because the space charge limited current condition is exceeded. 
     The space charge limitation is overcome in the present invention by converting the electron energy in the electron beam 20 into photon energy and X-rays (Bremsstrahlung). The photon energy is produced by band edge radiation due to radiative recombination of electron hole pairs produced by the electron beam. The X-rays and photon energy is then used to ionize the bulk of the semiconductor instead of only a shallow surface layer. The electron beam 20 penetrates the semiconductor material 12 to a relatively shallow depth. For example, a 10 keV electron beam will penetrate silicon to a depth of 1.5 micrometers. However, the X-rays and photon energy which is produced by higher energy electron beams can penetrate to a depth of one-half to one millimeters or more. The majority of the ionization in the semiconductor material 12 outside the electron-beam activated layer is preferably caused by photon energy. Unlike Bremsstrahlung which produces X-rays in a linear relationship to electron energy, photon energy produced by cathodoluminiscence is independent of the energy of the electron beam 20. 
     Preferably, the semiconductor material is a highly resistive direct semiconductor material such as semi-insulating gallium arsenide (GaAs). A shallow donor or acceptor layer 40 (FIG. 2B) may be formed at the surface of the semiconductor material 12 adjacent to the electrode 15 to increase the number of photons produced by the electron beam 20. The depth of doped layer 40 should be approximately equal to the depth the electrons penetrate the semiconductor 12. For example, a GaAs wafer 0.5 millimeter thick can be doped by diffusing zinc for 20 minutes at a temperature of 750° C. to produce a p-type layer of about 10 micrometers with an acceptor concentration of 10 19  /cm 3 . 
     In experiments performed using semiconductor material 12 formed as described above, the undoped semi-insulating GaAs exhibited current densities far above the space charge limited current density for a trap free insulator which represents the optimum condition for space charge limited current flow. The characteristics exhibited by the undoped semi-insulating GaAs indicate that the bulk of the semiconductor was ionized due to X-ray Bremsstrahlung. The experimental results using zinc-doped GaAs had a slower rise time than the undoped semi-insulating GaAs, but had approximately twice the current gain of the undoped semi-insulating GaAs. The concentration, depth and composition of the doped layer can be varied to produce switches with varying characteristics using known semiconductor technology. 
     In comparison to a diffuse discharge switch, the present invention is capable of higher current density in the switch, e.g., 10 3  to 10 4  A/cm 2 , compared to less than 100 A/cm 2  in a diffuse discharge switch. Also, the forward voltage during conduction may be less than 100 volts, while the minimum forward voltage in a diffuse discharge switch is 1,000 volts and over 100 volts in an EBS device. Most importantly, the current gain of an electron-beam controlled bulk semiconductor switch according to the present invention is 10 4  to 10 5 , depending upon the source function and recombination rate of the semiconductor material 12. The source function S b  defines the number of electron-hole pairs created per volume and time by the electron beam and is defined by equation (1). 
     
         S.sub.b =(dW/dx)*(J.sub.b /e W.sub.i)                      (1) 
    
     In equation (1), dW/dx is the differential energy loss, J b  is the electron-beam current density, e is the electron charge and W i  is the effective ionization energy which is 4.3 eV for GaAs. 
     Many of the features and advantages of the present invention are apparent from the detailed specification, and thus, it is intended by the appended claims to cover all such features and advantages which fall within the spirit and scope of the invention. A switch constructed according to the present invention has many possible applications, a few of which include high power switching in, e.g., an inductive storage unit, and a bistable electronic device in, e.g., a high power circuit. Further, since numerous modifications and changes will readily occur to those skilled in the art, from the disclosure of the invention, it is not desired to limit the invention to the exact construction and operation illustrated and described. Accordingly, suitable modifications and equivalents may be resorted to, all falling within the scope and spirit of the invention.