Patent Number: 
Section: description

The embodiments described below accomplish several difficult design goals for multi-column FIB systems. The optical elements are sufficiently electrically isolated to maintain the required high operating voltages. In some embodiments, the number of high voltage power supplies is reduced from the number that would be required in multiple independent columns. The voltage level of the high voltage power supplies are also reduced from that of conventional FIB systems. In addition, the difficulties of keeping multiple LMIS""s (Liquid Metal Ion Sources) operating and maintained with minimum down time is addressed by using a vacuum sealable, multiple gun chamber as described below. FIGS. 1, 2A, and 2B show a multi-column FIB array using LMIS""s. FIG. 1 shows a multi-column FIB system 108 that includes a gun vacuum chamber 110 and a primary vacuum chamber 112. Gun chamber 110 is a single, sealable vacuum chamber that includes a set of ion guns 114. Gun chamber 110 can be replaced as a unit and has its own vacuum pump, preferably an ion pump (not shown). When one of the guns 114 in gun chamber 110 fails, the entire gun chamber 110 can be replaced with another gun chamber 110 that is already evacuated to an ultra high vacuum and ready to begin operation. Thus, multi-column system 108 does not need to remain out of production while the gun chamber is being evacuated. Each ion gun 114 includes an emitter 120, a suppressor 122, an extractor 124, an acceleration lens 126, a deceleration lens 128 and a ground element 169. The four elements 124, 126, 128 and 169 of each column together are referred as the xe2x80x9clens 1xe2x80x9d of the column. Although FIG. 1 shows a lens 1 comprising four lens elements, other lens designs can be used for lens1. Also, some or all of the elements of lens 1 could alternatively be positioned in primary vacuum chamber 112. Each ion gun 114 forms part of an ion optical column 136 that also includes an aperture 152, a steering element 154, a blanking element and Faraday cup 156, dual deflection elements 160 and 161, second lens elements 163, 162 and 165 (referred to collectively as the xe2x80x9clens 2xe2x80x9d), and a detector 164. At the bottom of each column is a work piece or target 170, such as a semiconductor wafer. An isolation valve 150 at the bottom of each gun 114 selectively closes a beam hole 168, thereby vacuum isolating gun chamber 110. The isolation valves 150 of the column in a gun chamber 110 are preferably xe2x80x9cganged,xe2x80x9d that is, connected in a manner so that all valves are opened or closed together. The detectors 164 for the columns 136 are also preferably ganged, that is, physically and electrically connected, but constructed so that each column""s secondary electrons are independently detected. The aperture 152 preferably comprises an automatic variable aperture. Such apertures are known and details are not shown in FIG. 1. A gas injection can optionally be used with apparatus of FIG. 1 to inject a gas for ion beam assisted deposition or for enhanced etching. The construction and operation of such systems are known and are described, for example, in U.S. Pat. No. 5,435,850 to Rasmussen. The gun elements, that is, emitters 120, suppressors 122, extractors 124, acceleration lenses 126, deceleration lenses 128, and ground element 169 are preferably contained in gun chamber 110. The number of guns in gun chamber 110 is preferably limited to about five. If one of the emitters 120 fails, then the exchange of a five-gun set is easier and less costly than replacing a larger number of guns, such as ten or more guns. Moreover, the restarting of five emitters in parallel is also much less prone to failure than restarting a larger number simultaneously. The set of ganged isolation valves 150 for the set of guns simultaneously isolates the beam holes 168 in the ion beam paths at the bottom of gun chamber 110 from the primary vacuum chamber 112. Valves 150 are preferably formed by a bar 172 that moves relative to bottom portion 174 of gun chamber 110. When valves 150 are open, the openings in bar 172 line up with the openings 169 in bottom portion 174. To seal gun chamber 110, bar 172 is shifted so that the holes in bar 172 are offset from the holes in bottom portion 174, and O-rings 176 form a seal between a solid portion of bar 172 and bottom portion 174. Before shifting bar 172, it is preferably lowered away from O-rings 176 to prevent damage to the O-rings that can create contamination and vacuum leakage. After bar 172 is shifted, it is raised again into contact with O-rings 176 to create a vacuum seal to isolate gun chamber 110. Primary chamber 112 can be exposed to air when gun chamber 110 is removed or alternatively, primary chamber 112 can be made sealable by using a second set of valves (not shown). Details of the mounting of gun chamber 110 to primary chamber 112 are conventional and not shown. A multiple ion column system could use a single gun chamber 110 or multiple gun chambers. FIG. 2A shows a top view of an arrangement of multiple linear gun chambers 110 grouped to form a two-dimensional array of fifteen guns. The number of guns per gun chamber can be varied, as well as the number of gun chambers to produce a system having the desired number of FIB columns for a particular application. FIG. 2A shows an outlet 210 from each gun chamber 110 to an associated ion pump. FIG. 2B is a side view of the multiple gun chamber system of FIG. 2A. FIG. 2B shows also a location for high voltage feed-throughs 212, a flange 214 at the top of a gun chamber 110, and an actuator 216 for ganged gate valves 150. The construction of the optical elements, such as extractors 124, acceleration lenses 126, and deceleration lenses 128 in gun chamber 110, can be simplified by using flat bars with holes to form lens elements. This construction technique can also be used to construct optical elements in the primary vacuum chamber. Using a single bar to form corresponding lens elements in different columns with a gun chamber can reduce the number of high voltage power supplies required. FIG. 3 is a cross-sectional view of a gun chamber 110 showing bars 310 used to form optical elements. Bars 310 form suppressors 122, extractors 124, acceleration lenses 126, and deceleration lenses 128. Bars 310 are electrically isolated from each other and from the chamber itself using HV (High Voltage) insulator disks 312 composed preferably of a ceramic material. Other means, such as dielectric balls, can be used to isolate the gun HV elements. The assembly may be glued together using a suitable epoxy or other means known in the art. After the bars and insulators are installed in the casing of gun chamber 110, the assembly can optionally be machined to provide additional accuracy in shaping and aligning the lens elements. The optical elements can be formed directly by the holes in a conductive bar, as shown with regard to acceleration lenses 126. A common voltage is thus applied to all lenses formed by the bar, reducing the number of high voltage power supplies required for the multi-column system. The number of high voltage power supplies can be further reduced by using a common high voltage supply for corresponding bars in multiple gun chambers. Conductive bars are typically made of a titanium alloy having a low thermal coefficient of expansion. Optical elements can also be formed by inserts placed into holes in a bar. For example, FIG. 1 shows the use of lens inserts 178 in the bar 310 forming deceleration lenses 128. The bar in which lenses 128 are formed is constructed from an insulating material, for example, a ceramic material such as alumina, and the lens inserts are composed of a conductive material, preferably a titanium alloy which has is low thermal coefficient of expansion that is similar to that of the alumina bar. The alumina bar provides high voltage isolation to the individual lenses 128 with respect to the bars 310. Voltage is applied to the individual lenses by wires connected to the lenses in a conventional manner, such as conductive silver epoxy or using connector pins. Alternatively, metal films can be placed upon the insulator bar to replace the wires. Another method of providing high voltage insulation to lenses 128 entails using a conductive bar 310, with an insulating insert placed in a hole in the bar, and then a conductive lens placed in the insulating insert. Such inserts can be glued into insulator material, which can then be glued into the bars. Lenses formed by inserts can also be post machined, that is, machined after assembly, for additional accuracy in shape and alignment. These construction methods that individually isolate lenses can be particularly useful for suppressor lenses 122, extractor lenses 124, or individual elements of lens 1 or lens 2. FIG. 1 shows inserts used only on the deceleration lens 128. Deceleration lens 128 can be operated near ground potential, which simplifies the power supply requirements for lens 1. Isolating lens elements allows the voltages in individual columns to be controlled. For example, the voltage on one of extractor lenses 124 can be individually boosted about 2 kV above the common extractor voltage to start or restart the individual emitter in the corresponding column. The extractor lens 124 can then return to or near the common extractor voltage for normal operation. Optical elements that are isolated can still use the common high voltage supply, but isolated elements can also be floated at a voltage above or below the common voltage, thereby reducing the number of high voltage power supplies required. Charged particle signal detection capability for imaging can be accomplished by a traditional side mounted electron multiplier or scintillator means, or by two other novel methods described below. For many nanofabrication applications, the beam current can be greater than a nanoampere. At this level of current, an amplifier or amplifiers can be attached directly to detector plate 164 below lens 2. Separate detector plates for each column could also be used. Alternatively, through-the-lens (TTL) electron detection can be used. Through-the-lens electron detection is known and described, for example, incorporated into an electron column in PCT Publication WO 99/34397 of Krans et al. In the Krans et al. design, the lens 2 center element and upper element (and optionally the lower element) are biased to positive potentials to draw the electrons from the sample up and above the lens, where they are detected by a channel plate electron multiplier, which is placed roughly perpendicular to the ion column axis, and has a hole in its center to pass the primary beam. FIG. 4 shows a TTL detection system for an ion column 410 in which low energy secondary electrons from the sample, having energies of about 5 eV (electron volts), are accelerated up through the lens 412 by positive potentials on the elements of lens 412, the deflector plates 432 and magnetic deflector 414. The TTL system in FIG. 4 utilizes a magnetic deflector 414 to deflect the secondary electrons 418 off to the side while allowing the high mass-to-charge ratio primary ions 420 to pass nearly straight through column 410. Alternatively, a Wien filter or an electrostatic deflection device could be used. An electron detector 424, such as a scintillator, continuous dynode multiplier, or channel plate, is then placed to the side for collecting and amplifying the electron signal for processing by standard FIB video electronics. In the embodiment of FIG. 4, a sample 426 and a lower lens element 428 are maintained at approximately ground potential. An upper lens element 430 is biased to between about +500 and +5000 volts with respect to ground to continue the secondary electron velocities upward beyond the lens 412. Similarly, electrostatic deflector plates 432 and deflector 414 are biased to between about +500 and +5000 volts to continue this upward velocity of secondary electrons 418 towards electron detector 424, the input of which must be similarly biased. The approximately 5 eV secondary electrons are accelerated rapidly by the lens element 440, which is at high positive potential, such as about 20,000 Volts. These electrons are decelerated as they pass through the lens element 430 and the deflection electrodes 432, but the secondary electrons still maintain trajectories that remain relatively close to the column axis. Magnetic deflector 414 or other separation device then directs the electrons toward the detector 424. FIG. 6 is an electron optics computer simulation of the secondary electrons 610 traveling from a sample 612 back through optical elements 616, 618, 620, and 622, with element 616 having a potential relative to sample 612. FIG. 5 shows an alternate ion column 508 design using a TTL secondary electron detector. A sample 510 and a lower final lens element 512 are each biased about xe2x88x922000 V negative to propel the electrons back through the lens. If it is desired to collect secondary positive ions instead of electrons, sample 510 and lower final lens element 512 can be biased to about +2000 V. Center lens element 514 is biased to approximately +20,000 V. Lens element 516, electrostatic deflector elements 520 and deflector 414 need not be positively biased, which simplifies the electronics and the optics construction. If the ion beam systems include other devices, such as gas injectors, these devices must also be biased to the same potential as the sample. The apparatus in FIG. 4 also may be used to detect secondary positive ions from the sample. To collect secondary positive ions, the lens 2 element 440 is biased to a negative potential. (Lens 2 is then an acceleration lens). In addition, electrostatic deflector 432, the deflector 414 and the input of particle detector 424 are negatively biased. Similarly, the potentials in FIG. 5 may be changed to collect and detect positive secondary ions. A quadrupole or other mass spectrometer can also be placed in the position of detector 424 to perform Secondary Ion Mass Spectrometry. The appropriate biasing of the column and detector may be employed to detect either positive or negative ions. For thin film head trimming or other applications, the ion beams must be tilted about +/xe2x88x923 degrees with respect to the normal to the sample surface. This beam tilting is to achieve undercutting or to yield cuts to the sides of the head with walls more normal to the head surface. This +/xe2x88x923 degree tilt can be achieved, for example, by tilting every other mw of columns by about +/xe2x88x923 degrees with respect to the normal to the sample surface. In other words, in a multi-chamber system, the ion guns in one chamber can be tilted at an angle of about 3 degrees from a normal to the sample surface and the ion suns in the next chamber are tilted at an angle of about three degrees from a normal to the sample surface in an opposite direction. The inventions described above can be embodied in a variety of systems, and the advantages delineated below can be provided in many or all of the embodiments. Because the embodiments will vary with the goals of a particular application, not all advantages will be provided, or need to be provided, in all embodiments. An advantage of the invention is an increase in the processing speed by providing a system including multiple ion guns capable of operating simultaneously on one or more targets. Another advantage of the invention is that it provides a system in which the multiple ion guns operate on one or more targets in a single primary vacuum chamber. Another advantage of the invention is that it provides a system in which the multiple ion guns are in a gun chamber capable of being vacuum isolated from the main chamber, that is, the gun chamber is capable of being evacuated or exposed to atmosphere independently, without disrupting the vacuum in the main chamber. Another advantage of the invention is that it provides a system in which the multiple ion guns are positioned in multiple gun chambers, each gun chamber containing one or more ion guns and each gun chamber capable of being vacuum isolated from the main chamber and from each other. Another advantage of the invention is that it provides a multiple ion gun system in which a portion of the ion column elements are in the primary vacuum chamber. Another advantage of the invention is that it provides a system in which an ion gun or set of ion guns in one chamber can be replaced while maintaining a vacuum in the main chamber and in other gun chambers. Another advantage of the invention is that it provides a system that uses multiple ion guns and provides the capability to detect secondary particles emitted from a sample at the target point of each of the multiple guns. Another advantage of the invention is that it provides charged particle optical elements in parallel for multiple columns and a method of efficiently manufacturing such elements. Another advantage of the invention is that it provides such charged particle optical elements with at least one of the optical elements being individually controllable. Another advantage of the invention is that it provides an electrode design for a multiple column focused ion beam system that reduces the number of high voltage power supplies required for the system. Another advantage of the invention is that it provides a multiple column focused ion beam system using fewer high voltage power supplies than the number of columns. Another advantage of the invention is that it provides an electrode design and voltage application scheme that reduces the voltage requirement of the high voltage power supply. Another advantage of the invention is that it reduces the cost of processing multiple targets simultaneously from the cost of using multiple, single beam focused ion beam systems. Another advantage of the invention is that individual emitters can be restarted by individually increasing the extraction voltage of that particular gun and not disturb the other gun voltages. This can be achieved either by increasing the extractor voltage with respect to the emitter/suppressor elements by using isolated extractor elements, or by increasing the emitter/suppressor voltage with respect to the common extractor voltage for that particular gun. Although the present invention and its advantages have been described in detail, it should be understood that various changes, substitutions and alterations can be made to the embodiments described herein without departing from the spirit and scope of the invention as defined by the appended claims. Moreover, the scope of the present application is not intended to be limited to the particular embodiments of the process, machine, manufacture, composition of matter, means, methods and steps described in the specification. As one of ordinary skill in the art will readily appreciate from the disclosure of the present invention, processes, machines, manufacture, compositions of matter, means, methods, or steps, presently existing or later to be developed that perform substantially the same function or achieve substantially the same result as the corresponding embodiments described herein may be utilized according to the present invention. Accordingly, the appended claims are intended to include within their scope such processes, machines, manufacture, compositions of matter, means, methods, or steps.