This paper discusses the electronic properties of uranium dioxide and describes the potential performance advantages of uranium dioxide as compared to conventional semiconductor materials. The need for additional fundamental data is discussed. The results of fabricating and testing a uranium-based diode will be presented if the test results are available in time. This work was conducted under the auspices of the U.S. Department of Energy’s Depleted Uranium Uses Research and Development Program.
There has never been an electronic device made using an oxide of uranium as a semiconductor. Yet, uranium oxides have intrinsic electrical and electronic properties equivalent to or much better than the intrinsic properties of conventional Si, Ge, and GaAs semiconductor materials. Figure 1 compares the range of UO2 conductivity to typical ranges of conductivity of common insulators, semiconductors, and conductors (1). Figure 2 gives the electrical conductivity of UO2 single crystals as a function of temperature. At room temperature, the electrical conductivity of intrinsic UO2 (3) is approximately the same as a single crystal of silicon and less than the intrinsic electrical conductivity of GaAs. Clearly, UO2 is an excellent semiconductor material.
The solar-cell efficiency vs electronic energy band gap for uranium dioxide is shown in Fig. 3 and is compared to other semiconductor materials (1). The electronic band gap of UO2 lies near the optimum efficiency, maximum of the curves at ~1.3 eV (2), between Si and GaAs, indicating that UO2 is a somewhat better semiconductor material than are conventional Si or GaAs materials for solar-cell applications.
Certain materials in contact with each other produce an electric current when there is a temperature gradient across the junction. The Seebeck coefficient is a measure of this thermoelectric effect. At room temperature (~300 K), the Seebeck coefficient of uranium dioxide is ~750 :V/K, as shown in Fig. 4. This value is considerably higher than the currently most promising materials Tl2 SnTe5 and Tl2GeTe5 (~270 :V/K) (4), shown in Fig. 5. Other factors, such as electrical and thermal conductivity, are important along with the Seebeck coefficient, but these factors also have favorable properties, as previously discussed. Thus, uranium oxides might be used as a thermoelectric material and be applied in next generation small-scale refrigerators and power generation applications.
The dielectric constant of UO2 is nearly double that of Si and GaAs—22 at room temperature as compared to 12 and 14 for Si and GaAs, respectively (2). This characteristic may make uranium oxides suitable for making higher density integrated circuits with higher breakdown voltages than current silicon-based electronics, without suffering complementary metal oxide semiconductor (CMOS) tunneling breakdown due to smaller nanometer size features. Thus, uranium oxide electronics may offer better integrated circuit performance than do conventional Si or GaAs material devices. A literature search reveals that the work-function parameter has never been measured for UO2 . The value of the work function parameter for various elements are shown in Fig. 6. Also, the solubility of various dopant materials in uranium oxides has not been measured. This information indicates that uranium oxides have never seriously been considered as semiconductor devices. Many electronic parameters need to be measured again with the intent of using uranium oxides as semiconductor material.
URANIUM-BASED ELECTRONIC DEVICES
The implications of these data are discussed for several semiconductor devices.
The electronic bandgap of UO2 is ~1.3 eV (at room temperature) (2), which is between Si and GaAs and is very near the peak of the efficiency vs Eg curve, as shown in Fig. 3. Thus, UO2 should give the highest solar-cell efficiency possible. The electronic band gap for UO2 , U3O8 , and U2O2 are such that each of these materials can be made into a photovoltaic device that can convert optical and infrared (IR) radiation into electrical energy.
A solar cell is a simple, semiconductive, energy conversion device. The performance of such a device is described in terms of conversion efficiency—how well incident solar radiation is converted into usable electrical power. Power is measured by multiplying short circuit current by open-circuit voltage.
While various solar-cell designs are feasible, perhaps the easiest to fabricate is a Schottkybarrier solar cell. This type of solar cell makes use of the different work functions of the oxide material and of the other contact material forming the diode. The device is fabricated by using polycrystalline or single-crystal uranium dioxide. Typically, a thin, metal-film top contact is deposited via a conventional sputtering technique, and an ohmic back contact is made with gallium.
When a junction is made between a uranium oxide material and another thermoelectric material (e.g., a metal), a thermoelectric cell is made. If a temperature gradient is established across the junction, an electric current is generated via the Seebeck effect. If optical or IR radiation is incident on the material, additional current is generated across the interface. For example, one material might be exposed to the inside of a refrigerator and the other to ambient room conditions in a next generation refrigerator. Or, one material may be exposed to an inside temperature of a spacecraft and the other to ambient cold-space temperature in a power-generation application.
Conventional integrated circuits suffer CMOS tunneling breakdown due to the smaller 2.5-nanometer device size used today. The density of components in microcircuits has grown exponentially since the early days of the industry—doubling every 18 months. To continue this density scaling, the only option is to go to higher dielectric constant materials. Manufacturers must convert to a high dielectric constant material within five years to avoid slackening of the pace of innovation (5). The dielectric constant for UO2 is 22 at room temperature as compared to 12 for Si and 14 for GaAs (2). This implies that uranium dioxide integrated circuits can be made much smaller (denser) than conventional integrated circuits.
FUNDAMENTAL DATA NEEDED
Before it can be said that uranium-based semiconductors are better than current ones, the electronic and electrooptical properties of uranium oxide single crystals and polycrystals powders and solid materials must be characterized.
Impact of Radioactive Decay
The impact of radioactive decay of 238 U and 235 U on electronic performance has not been evaluated. Alpha particle decay would introduce helium impurities and might inhibit current carrier mobility and overall electrical conductivity. The very long half-lives of 238 U and 235 U and subsequent slow decay rate should have little impact on the performance of solar cells and thermoelectric devices, but they could impact high-performance integrated circuits.
Impact of Stoichiometry
The literature indicates that the performance of UO2 as a semiconductor material is strongly related to its stoichiometry. For example, as shown in Fig. 7, the electrical conductivity of UO2.001 vs that of UO1.994 varies by four orders of magnitude (3). Thus, there are many fundamental properties of uranium oxide semiconductors that should be remeasured—with close attention paid to such parameters as oxygen content, with the objective of uranium use in semiconductor devices.
Before uranium-based integrated circuit devices can be designed and fabricated, dopants must be chosen. Figure 8 shows dopant solubility in silicon. Similar curves of impurity solubility in uranium are needed to choose the optimum dopant. But, such curves do not exist.
DEPLETED URANIUM CONSUMPTION
Approximately 5,000 t of silicon are processed worldwide each year into electronic devices. If depleted uranium (DU) were used instead of silicon, on an atom-for-atom basis (238/28), this corresponds to 42,000 t/year of DU consumption. There are ~20,000 t of DU produced each year in the United States as tails from uranium enrichment operations. Thus, if all electronic devices were made of uranium, it could consume the yearly production of DU each year.
FABRICATION AND TESTING OF A URANIUM-BASED DIODE
A diode is one of the simplest electronic device. Yet, it is a building block for semiconductor applications. Fabricating and measuring the performance of a uranium dioxide-based diode predict the performance of solar cells, uranium-based transistors, etc. Thus, the evaluation of uranium-based materials in electronics will begin with the simplest electronic device. Proofof-principle tests will be conducted using a polycrystal UO2 -based diode. The type of dopant material will be based initially on proven dopants used in Si and GaAs. The first dopant material will be niobium. Current vs voltage (I-V) curves will be measured during testing, and the results will be compared to conventional diodes. It is recognized that this initial diode performance may not be optimum because the choice of dopant material is almost arbitrary.
Uranium oxides have four characteristics that could potentially give them significantly better performance than conventional semiconductor materials: (1) operation at substantially higher temperatures, ~2600 K vs <473 K; (2) a Seebeck coefficient two to three times greater than the most promising current material, implying significantly better performing thermoelectric devices; (3) higher dielectric constant suitable for making integrated circuits; and (4) greater radiation and EMI resistance implying much improved performance for special, e.g. space, applications. However, before it can be said that uranium-based semiconductors are better than current ones, the electronic and electrooptical properties of uranium oxide single crystals and polycrystals powders and solids materials must be characterized. The optimal dopant material must be established by developing metal solubility in uranium curves. Parameters, such as work function, need to be measured.
Proof-of-principle experiments with an uranium diode will be conducted to confirm the theoretical promise of uranium use as a semiconductor material.
This work was conducted under the auspices of the U.S. Department of Energy’s Depleted Uranium Uses Research and Development Program.
- Sze, S. M., 1985. Semiconductor Devices—Physics and Technology, John Wiley & Sons.
- Samsonov, G. V., 1982. The Oxide Handbook, 2d ed.
- Gmelin Handbook, 1979. “Uranium Supplement,” Vol. C5.
- Sharp, J. W., et al., “Thermoelectric Properties of Two Ternary Tellurides,” Materials Research Society, Thermoelectric Materials 1998—The Next Generation Materials for Small-Scale Refrigeration and Power Generation Applications Symposium, Proceedings (eds.: Terry M. Tritt, et al.), Vol. 545, November 30—December 3, 1998, Boston Massachusetts, p. 391–397.
- Weise, P., March 25, 2000. “Looking for Mr. Goodoxide,” Science News, 157(13), 204.
Materials Science Engineering Department
University of Tennessee
Knoxville, TN 37931
Michael Hu and M. Jonathan Haire
Chemical Technology Division
Oak Ridge National Laboratory
Oak Ridge, Tennessee 37831-6179
For the Waste Management 2001 Symposium
February 25–March 1, 2001
The submitted manuscript has been authored by a contractor of the U.S. Government under contract DE-AC05-00OR22725. Accordingly, the U.S. Government retains a nonexclusive, royalty-free license to publish or reproduce the published form of this contribution, or allow others to do so, for U.S. Government purposes.