Patent Number: 044141769
Section: description

DETAILED DESCRIPTION OF THE INVENTION The invention relates to a metallic member exposed to plasma in a plasma device and subject to a loss of metal from its surface by erosion and more specifically by sputtering. In the invention a metallic member such as a first wall or limiter is constructed of a substrate composed of a major amount of a first metal and a thin surface layer of a second metal. The term substrate is here construed as applying to any bulk material in which a surface has a composition or structure different from that of the bulk. In this metallic combination, less metal escapes from the surface than would occur when the second metal is in bulk form. In addition, the metal escaping from the surface has a higher secondary ion/neutral ratio and therefore a greater portion of the second metal leaving the surface is returned. In another aspect of the invention, the substrate is composed of a major amount of a first metal and minor amount of a second metal so that the substrate provides a self-sustaining source of the second metal to the surface. Preferably the first metal is more electromegative than the second metal and the second metal is selected from the group consisting of alkali and alkaline earth metals, preferably those with low atomic number. Further, the metals are selected so that the binding energy between like atoms of the first metal is greater than the binding energy between atoms of the first and second metals which in turn is greater than the binding energy for like atoms of the second metal. The substrate provides a self-sustaining source of the second metal by at least two processes. In the first, the metals are selected to satisfy the equation EQU H.sub.1,2 =.OMEGA.+1/2(H.sub.1,1 +H.sub.2,2) where .OMEGA..ltoreq.0, and H represents an enthalpy of sublimation for the alloy and the pure first and second metals. Under these conditions and when the substrate or structural member is heated to an elevated temperature or subjected to another energy source, the first or surface layer becomes enriched with the second metal to form a monolayer composed primarily of the second metal. Another mechanism which also causes segregation results from radiation damage. In a second process when the substrate or structural member has a concentration of metals forming an intermetallic compound, the surface is subjected to an initial treatment of radiation including bombardment with particles. Since the second metal forms secondary ions in greater amounts than the first metal, the removal of the surface atoms results in a selective return of the second metal to form a monolayer of the second metal. Further, as the binding energy of like atoms of the second metal is below that for different atoms of the two metals, returning atoms of the second metal will move to vacant sites above atoms of the first metal and therefore aid in maintaining the monolayer of the second metal. The invention provides several advantages. It provides a metallic member and particularly a first wall or limiter with a substrate constructed with a reasonable degree of structural strength and ease of fabrication, together with a surface having a reduced loss of metal by erosion or sputtering, and a higher secondary ion/neutral ratio. In addition, by providing a self-sustaining source of second metal for the surface of the first wall or limiter, the invention provides a surface with improved performance characteristics. The invention is particularly useful in a plasma device in which a plasma is generated and heated to an elevated temperature. A number of plasma devices have been constructed to provide a means for conducting experiments in the field of thermonuclear reactions. FIG. 1 represents a sectional view of a plasma device 10 with a plasma 16 magnetically confined within a chamber 18. Additional parts of the plasma device as shown include the magnetic coil 20, a shield 22, a plenum chamber 24, and rf duct 26. In the plasma device 10, hot plasma 16 at temperatures of about 1.times.10.sup.8o K is magnetically confined within the first wall 12 whose purpose is to limit the number of particles escaping from the plasma. The limiter 14 reinforces this purpose and is at a negative sheath potential of about 20-500 eV. The surface 28 of the first wall 12 and surfaces 30 of the limiter 14 are both subject to erosion by loss of metal due to vaporization of the metal at the elevated temperature of 300.degree.-3500.degree. C. and also by sputtering. Sputtering may occur when particles from the plasma strike the metallic surfaces 28 and 30. If the sputtered particles are secondary ions, they are returned to the emitting surface by the toroidal field regardless of charge sign. If the secondary ions are emitted from the limiter, or the wall in a limiter-less device, the sheath potential provides an additional means of returning the positive ions which comprise the vast majority of the secondary ions. If the sputtered particles are neutral and depending on their kinetic energies, they will penetrate sufficiently far into the plasma for charge exchange collisions to occur. At that point, they will become ionized but the ions will then be subject to plasma transport processes and some of the particles will therefore tend to continue into the plasma causing a reduction in the plasma energy available for the desired thermonuclear reactions. In the inventive metallic member represented by the first wall 12 and limiter 14, each pair of different atoms of the first and second metals have a binding energy above the value for like atoms of the second metal and therefore are at a reduced vapor pressure from their pressure in bulk form. This results in a reduced loss from the surface of the wall or limiter. Preferably the surface layer is a monolayer composed of atoms of the second metal with ionic bonds to atoms of the first metal as generally illustrated in FIG. 2. The presence of the monolayer also serves to shield the substrate from sputtering, especially under the conditions of low energy-light ion sputtering encountered in plasma devices. Therefore, the erosion of the substrate metal which produces predominantly neutral atoms which have a relatively high likelihood of entering the plasma is reduced. In addition, returning atoms of the second metal will have a greater affinity towards atoms of the first metal due to the higher binding energies and will move to vacancies in the monolayer where atoms of the first metal are exposed thereby maintaining the integrity of the monolayer. As illustrated in FIG. 2, a particle 40 from the plasma 16 strikes the surface 41 of the wall 12 or limiter 14 and causes an atom 42 of the second metal to leave the surface 41. That atom may move in two paths 44 and 46 depending on whether or not the atom is attracted to the surface 41 by the sheath potential or magnetic field. In some instances, the atom 42 will initially move to a position over a like atom 48 before it moves along path 50 to a vacant site 52. Substrate 54 is illustrated as containing only molybdenum although as disclosed below, minor amounts of the second metal may be present to provide a self-regenerating and self-sustaining surface of the second metal. The surface metal or second metal is an alkali or alkaline earth metal including Li, Na, K, Rb, Cs, Mg, Ca, Sr, and Ba with those with a lower atomic number having an advantage since their effect on reduction in energy of the plasma is less than those metals with greater atomic number. However, a heavier metal such as cesium has advantages since it may provide a higher ion fraction than lithium. The metal comprising the major portion of the substrate is more electronegative than the surface metal, has preferably a high melting point relative to the second metal, a high solubility for the second metal, a high surface binding energy, and a high heat of sublimation. Suitably, a first metal includes Al, Si, Cu, Au, B, Mg, Pb, Bi, C, Ag and Ca, and may form either an alloy or intermetallic compound with the second metal. In the case of the compound, it should be noted that the melting point of the compound may be higher than that of either element, and that it is the compound's melting point that, in fact, determines the suitability for use in a plasma device. The first metal will be more electronegative than the alkali or alkaline earth second metal. The substrate may include combinations of the first metal such as stainless steel formulations, particularly when the self-sustaining feature is not utilized. When the substrate is intended to provide a source of the second metal, and the substrate is in the form of an alloy, the second metal may be present in quantities as low as a few ppm, with preferred upper limit of about 20 at.%. For the process involving selective erosion of an intemetallic compound (e.g., Li.sub.2 Si or BaAl.sub.4) the second metal should constitute from about 15 at.% to about 70 at.% and preferably about 50 at.%. When the substrate is compound of a mixture of metals forming an alloy, the metals are selected to satisfy the equation EQU H.sub.1,2 =.OMEGA.+1/2(H.sub.1,1 +H.sub.2,2). The above equation is further described by Williams and Nason in the reference Surface Science, 45, (1974) 377. Briefly, the equation relates the enthalpy (H.sub.1,2) of the sublimation for the alloy and first and second metals in terms of the solution parameter ".OMEGA." which equals zero for an ideal solution. When .OMEGA..ltoreq.0, the second metal in the alloy becomes segregated to form essentially a monolayer on the surface. In this process continuing as the surface is eroded, the surface is maintained with added amounts of the second metal. As further illustrated in FIG. 4 which represents a graph characterizing the effect of the selection of metals satisfying the above equation; when .OMEGA. is negative, the concentration of the minor constituent is highest at the first layer and decreases to a very low value in the second layer after which it returns to the bulk value. The final difference in concentration between the first and second layers results in a more stable condition than would be associated with random distribution of the second metal in the substrate. As also illustrated in FIG. 4, when .OMEGA. is positive, the extreme difference in concentration of the second metal between the first and second layers does not occur. When .OMEGA. is negative, the effect illustrated in FIG. 4 is achieved by providing a mixture of metals as described above and applying energy to the substrate sufficient to cause the atoms of the second metal to migrate and form a surface layer composed predominantly of the second metal with a second layer having a greatly decreased concentration of the second metal. Preferably, the energy is applied by heating the substrate to an elevated temperature at least about 300.degree. C. and preferably about 300.degree.-600.degree. C. As the surface layer loses atoms of the second metal and with the substrate at an elevated temperature, atoms of the second metal are transferred to the surface by segregation to maintain the concentration difference between the first and second layers. Another process by which atoms of the second metal are transferred or migrate in the substrate is associated with a radiation-induced segregation. In this process, voids or other sites are created in the substrate by radiation damage and atoms of the second metal move with these sites to the surface to provide atoms of the second metal on the surface. As illustrated in the pictorial representation of a substrate in FIG. 5 containing an alloy 60 forming segregated layers, the surface 62 of first layer 64 is a monolayer of the second metal 66 such as potassium with the next below layer 68 comprising the first metal 70 such as aluminum with a small amount of the second metal 66. Additional layers 72 and 74 are composed of the first metal with the second metal being present in approximately the bulk concentration. In some instances, the combination of the first and second metals will result in an intermetallic compound where the atoms of the second metal are relatively fixed in the structure. Illustrations of these compounds are BaAl.sub.4, Li.sub.2 Si, Li.sub.5 B.sub.4 Li.sub.3 Bi, and Li.sub.4 Ca. Under these combinations, the substrate will provide the desired surface layer by selective removal of atoms of the first metal from the surface. Since atoms of the first metal will escape from the surface as neutrals, the second metal will increase in concentration at the surface due to the return of atoms of the second metal as secondary ions to the surface. The selective removal of the first metal from the surface is carried out by subjecting the substrate to an initial bombardment stage. After the formation of the surface layer of the second metal, some amounts of the second metal will be lost during operation of the plasma device. Returning atoms of the second metal under the effects of the electrical and/or magnetic fields will reform the surface over atoms of the first metal. In addition, exposed atoms of the first metal will be removed by bombardment so that the surface layer will continue to be characterized by a predominance of the second metal. For purposes of illustration, the surface of the intermetallic compound at the initial stage may be represented as follows: ##STR1## where "A" and "B" represent atoms of the second and first metals. As "B" is selectively removed, a layer of "A" remains to form a monolayer. EXAMPLES I-II Two tests were conducted on the sputtering behavior of a layer of potassium on molybdenum. The equipment included a bakeable, ion pumped stainless steel UHV sample chamber in which is installed commercial Auger electron (AES) and x-ray photoemission (XPS) spectrometers, a differentially pumped 5 KeV ion gun, and a laboratory-constructed secondary ion mass and energy analyzer. The ion gun has been modified so that an internal pressure readout signal can be provided to the servo-controlled gas inlet valve to obtain pressure stabilization. Electron and ion beam currents were measured by a Faraday cup which can be moved into the sample position. The ion gun was capable of producing a beam spot 200 .mu.m in diameter and the beam was rastered over an area larger than the sample to avoid effects arising from beam nonuniformity. Ion beam current densities ranged from about 0.7 to 10 .mu. A/cm.sup.2. A potassium layer was produced from a source constructed of a porous tungsten plug impregnated with a potassium alumino-silicate analogous to a commerical molecular sieve. When heated, the source emitted potassium ions. The source was placed approximately 10 cm from the sample to reduce surface heating, and a molybdenum heat shield and collimator with a 6 cm diameter aperture was placed approximately equidistant between the source and sample. A bias of about 45 volts was applied to the source during deposition to supply an extraction potential. The spectrometers, ion gun and potassium source were positioned so that it was possible to deposit, sputter and operate all of the analyzers without changing the sample position. Potassium deposition on the molybdenum substrate was monitored either by AES or XPS. Because of the power radiated by the potassium source, the sample temperature increased to about 90.degree.-100.degree. C. during deposition. At this temperature, bulk potassium is above its melting point and has a vapor pressure of about 10.sup.-4 Torr. The time for the deposition of potassium was about two hours and the potassium signal was normalized to the Mo line intensity for each scan to correct for fluctuations in the output of the x-ray tube. After about two hours, the potassium source and sample bias were turned off and a 1 KeV He.sup.+ beam was turned on. The potassium signal fell at a constant rate for several hours, followed by an abrupt change to a new, slower rate indicating that less potassium was escaping from the surface. The data in FIG. 3 obtained without sample bias are indicated by the symbol "0". The test was then repeated under the same conditions except that a bias of about -21 volts was applied to the sample. An identical or near identical initial sputtering rate and the same abrupt change were noted; however, the erosion rate following the abrupt change was lower than in the previous test. For this test, the data are indicated by the symbol ".DELTA.". The results of the tests are shown in FIG. 3. As indicated, the initial sputtering resulted in the removal of potassium as neutral atoms until a monolayer was formed (as calibrated by AES). After the monolayer was formed, potassium ions on the surface escaped as secondary ions in the absence of an applied potential. In the second test, when the negative potential of about 21 eV was applied to the sample, the rate became further reduced due to the return of secondary ions to the surface. In addition to the rates shown in FIG. 3, the sputtering cross section in FIG. 3 was measured. The initial sputtering cross section was about 6.6.times.10.sup.-18 cm.sup.2, with values for the lower line representing the test without bias being about 3.6.times.10.sup.-18 cm.sup.2 and for the lower line representing the test with bias being about 1.9.times.10.sup.-18 cm.sup.2.