Technical Field
The present disclosure relates to an improved vacuum integrated electronic device and the manufacturing process thereof.
Description of the Related Art
As is known, the idea of miniaturized vacuum integrated electronic devices dates back to 1961. However, the increasing demand for high-speed high-power telecommunication systems has recently given a new impulse to the research in the field of vacuum micro- and nanoelectronics because of their good characteristics in handling high voltages and high powers.
Therefore, the availability of a device merging the above advantages with those of the solid-state technology would open new potential scenarios of future markets and products for long-range telecommunications, aerospace and medical systems.
Unfortunately, manufacturing such devices has proven to be difficult, in particular as regards the shape and surface composition of the cathode. Specifically, techniques to concentrate the electric field with sufficient intensity to produce emission with practical turn-on voltages have been studied and materials with low-work function, good chemical, thermal, mechanical and electrical properties have been investigated. These materials must also be suitable for the implementation of tips with small radius and high aspect ratio (the ratio between the base diameter and the tip height).
Generally, these structures have conical or pyramidal metal micro-tip cathodes.
For example,
Here, emission is caused by the gate-cathode voltage and emitted electrons are collected by the anode 4.
This solution is quite complex to be manufactured.
Another known solution is a lateral structure, which can be fabricated in a planar way, as shown in
In another possible structure, shown in
In an alternative structure, disclosed in U.S. Pat. No. 5,463,269, a vacuum integrated microelectronic device is manufactured by conformal deposition of an insulating material in a cavity, thus forming a symmetrical cusp that can be used as a mold to form a micro-tip cathode. Two electrodes form a simple diode, while three, four or five electrodes can form, respectively, a triode, a tetrode and a pentode. Since the cusp is self-aligned to the center of the cavity, it is also aligned to the center of the electrodes. However, the manufacture of the above vacuum integrated microelectronic device has high manufacturing costs and its operating characteristics can be altered by, for instance, ionizing radiations and noise at power output.
MI2013A000897 (US 2014/0353576) describes an electron emitting device wherein the cathode is formed by depositing a metal layer on a dielectric layer having a cavity. During deposition, the metal material forms horizontal portions that protrude over the cavity and joins to form a tip. The width of the cavity is such that the metal layer does not fall into the cavity, which is thus sealed by the metal layer.
Although this solution has proved satisfactory in many situations, it cannot be used in all applications and devices. In fact, the voltage causing turning on of the electron emission is quite high, e.g., up to 20V, which is too high for some electronic application. In addition, this voltage is far from common threshold voltage of components integrated in VLSI/ULSI technology. Thus, a better compatibility with voltages used in common semiconductor voltages is desired.
Thus, an aim of the disclosure is to provide an improved vacuum integrated electronic device.
According to the present disclosure, there are provided a vacuum integrated electronic device and the manufacturing process thereof, as defined in claims 1 and 10, respectively.
For the understanding of the present disclosure, preferred embodiments are now described, purely as a non-limitative example, with reference to the enclosed drawings, wherein:
The described emitting structure 50 is able to generate an electric field that is considerably increased with respect to known solutions by virtue of the very sharp conical shape of the two tips 55, 56.
In fact, significant emission of electrons from metals occurs when the surface electric field is in the range of approximately 2×107 Vcm−1. The surface electric field is related to the applied gate voltage and to a field enhancement factor. The enhancement factor depends on the geometry of the electron emitter and is inversely proportional to the radius of the electron emitter tip. Therefore, the sharper the tip is, the greater the electric field is.
The electron emitting structure 50 of
Then, a conductive layer 103 is deposited on the first insulating layer 102. The conductive layer 103 is, e.g., a non-ferromagnetic metal, a highly doped polycrystalline silicon or another material with high conductivity, compatible with the manufacture of vacuum integrated microelectronic devices.
A second insulating layer 104, for example of silicon oxide, is then deposited on the conductive layer 103. The thickness of the second insulating layer 104 depends on the vertical length of the tip portions 51, 52 (
Then,
Thereafter,
Then,
Subsequently,
Thereafter,
Simultaneously with the formation of the second half-cone 52, the metal layer 108 grows both vertically and horizontally, from the upper edge of the cavity 54, until it closes and seals the latter. Therefore, the vacuum is retained inside the cavity 54 as a side effect of the deposition. Deposition is continued until the metal layer 108 reaches a thickness up to 500 nm. Then,
Thereby, the closure portion 57 and the half cones 51, 52 are integral to each other and form a cathode 109.
Thereafter,
After dicing, an electron emitting vacuum triode 120 is obtained.
The described electron emitting vacuum triode 120 is able to generate a considerably increased electric field with respect to known solutions, as explained above.
Simulations by the Applicant have shown that the described electron emitting vacuum diode 120 has a turn-on voltage of about 2 V. Such value is very suitable for high-power switching applications and is much lower than with prior devices with even smaller tip radius and gate aperture.
The described electron emitting vacuum diode 120 is also advantageous due to the self-alignment of the structures and compatibility with IC technologies. In addition, the described structure is very compact, since the metal layer 108 forms both the cathode and the cathode electrode. This realization of the cathode and the cathode electrode through a single metal layer allows a high integration density to be achieved. The electron emitting vacuum diode 120 further has a low-threshold.
In another embodiment of the present vacuum electron emitting device, the tip portion is formed as a single electron emitting structure 122 extending substantially on the whole circumferential surface of the sidewalls 53 of the cavity 54, as shown in
The single electron emitting structure 122 may be formed, e.g., during a single deposition step by rotating the wafer 100 around its axis, thus causing metal atoms, for example titanium, to impact on the whole periphery of the cavity 54. All the other parameters may be the same as above discussed.
Thereby, the electron emitting structure 122 has a circumferential tip 123 pointing towards the bottom of the cavity 54. Also here, the closing portion 57 extends over the upper edge of the cavity 54, and seals it, analogously to the embodiment of
The present vacuum integrated electronic device may also be implemented as a diode, a tetrode or a pentode.
For example,
All the above embodiments share the advantages described above, and have an increase electric field generated by the tips 55, 56 or the circumferential tip 123.
Finally, it is clear that numerous variations and modifications may be made to the device described and illustrated herein, all falling within the scope of the disclosure.
For example, the vacuum integrated electronic device may also be a pentode, by adding another insulating layer and another conductive layer and relevant contacts.
The tip portion of the vacuum integrated electronic device could be of a different material, such as molybdenum zinc, strontium, cerium, neodymium.
The various embodiments described above can be combined to provide further embodiments. These and other changes can be made to the embodiments in light of the above-detailed description. In general, in the following claims, the terms used should not be construed to limit the claims to the specific embodiments disclosed in the specification and the claims, but should be construed to include all possible embodiments along with the full scope of equivalents to which such claims are entitled. Accordingly, the claims are not limited by the disclosure.
Number | Date | Country | Kind |
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102015000075586 | Nov 2015 | IT | national |
Number | Name | Date | Kind |
---|---|---|---|
5140219 | Kane | Aug 1992 | A |
5463269 | Zimmerman | Oct 1995 | A |
6023126 | Karpov | Feb 2000 | A |
20010006842 | Hattori | Jul 2001 | A1 |
20110305314 | Kitamura | Dec 2011 | A1 |
20140353576 | Patti | Dec 2014 | A1 |
Number | Date | Country |
---|---|---|
2332745 | Aug 2008 | RU |
Entry |
---|
Pennisi, S. et al., “Dovetail Tip: A new Approach for Low-Threshold Vacuum Nanoelectronics,” IEEE Transactions on Electron Devices 62(12):4293-4300, Dec. 2015. |
Number | Date | Country | |
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20170148604 A1 | May 2017 | US |