Abstract:
A system for determining the endpoint associated with removing silicon from the backside of a flip chip type die includes a tool for removing silicon and a light source for directing light to the backside of the die. An electrical measuring apparatus, such as a voltmeter, ammeter or oscilloscope, is attached across the output pins of a package to which the die is attached. The light or ions directed toward the backside of the die induce a current in the devices formed in the semiconductor. The value of the current or voltage output depends on the thickness of material between the endpoint on the backside of the die and the devices in the epitaxial layer of the die. The induced signal can be monitored to determine the thickness. Silicon can be removed globally until the thickness is reasonable such that a local thinning tool can be used to remove silicon to get to the area of interest in a reasonable amount of time. The induced current can be monitored during local thinning. A viewing mechanism such as infrared microscopy can be used to locate the specific device or devices of interest in the epitaxial layer of the die. The viewing mechanism is also used to determine where localized thinning will occur.

Description:
This is a continuation application of Ser. No. 09/050,531 filed on Mar. 30, 1998, now U.S. Pat. No. 6,069,366. 
    
    
     FIELD OF THE INVENTION 
     The invention relates to semiconductor device assemblies, and more particularly to techniques for analyzing and debugging circuitry associated with a flip chip bonded integrated circuit. 
     BACKGROUND OF THE INVENTION 
     The semiconductor industry has seen tremendous advances in technology in recent years which have permitted dramatic increases in circuit density and complexity, and equally dramatic decreases in power consumption and package sizes. Present semiconductor technology now permits single-chip microprocessors with many millions of transistors, operating at speeds of tens (or even hundreds) of MIPS (millions of instructions per second) to be packaged in relatively small, air-cooled semiconductor device packages. A by-product of such high-density and high functionality in semiconductor devices has been the demand for increased numbers of external electrical connections to be present on the exterior of the die and on the exterior of the semiconductor packages which receive the die, for connecting the packaged device to external systems, such as a printed circuit board. 
     In the past the die and package were first attached and then the electrical connections from the die to the package were made by wire bonding. The wire bonding procedure is simple in concept. A thin (0.7 to 1.0 mil) wire is first bonded to the chip bonding pad and spanned to the inner lead of the package lead frame. The third action was to bond the wire to the inner lead. Lastly, the wire is clipped and the entire process repeated at the next bonding pad. While simple in concept and procedure, wire bonding was critical because of the precise wire placement and electrical contact requirements. In addition to accurate placement, each and every wire must make a good electrical contact at both ends, span between the pad and the inner lead in a prescribed loop without kinks, and be at a safe distance from neighboring lead wires. Wire loops in these packages are 8 to 12 mils, while those of ultrathin packages are 4 to 5 mils. Wire bonding has been done with either gold or aluminum wires. Both types of wire are highly conductive and ductile enough to withstand deformation during the bonding steps and remain strong and reliable. 
     Wire bonding between a die and a package has several problems. One problem is that a wire bond attachment to a die limits the number of pads and placement of the pads on the die. In addition, minimum height limits are imposed by the required wire loops. Another problem is that there is a chance of electrical performance problems or shorting if the wires come too close to each other. The wire bonds also require two bonds and must be placed one-by-one and there are resistances associated with each bond. The wires are also relatively long and thus could contribute significantly to lead inductance and capacitance. This could limit acceptable signal speed in the system. 
     To increase the number of pad sites available for a die and to address the problems stated above and other problems, a different chip packaging technique called controlled collapse chip connection or flip chip packaging is being adopted. In this technology, the bonding pads are provided with metal (solder) bumps. The bonding pads need not be on the periphery of the die and hence are moved to the site nearest the transistors and other circuit devices formed in the die. As a result, the electrical path to the pad is shorter. Electrical connection to the package is made when the die is flipped over the package with corresponding bonding pads and soldered. As a result, the dies are commonly called flip chips in the industry. Each bump connects to a corresponding package inner lead. The packages which result are lower profile and have lower electrical resistance and a shortened electrical path. The output terminals of the package may be ball-shaped conductive bump contacts (usually solder, or other similar conductive material) are typically disposed in a rectangular array. These packages are occasionally referred to as “Ball Grid Array” (BGA). Alternatively, the output terminals of the package may be pins and such a package is commonly known as pin grid array (PGA) package. 
     Alternatively, the output terminals of the package may be pins and such a package is commonly known as pin grid array (PGA) package. 
     Once the die is attached to the package the backside portion of the die remains exposed. The transistors and other circuitry are generally formed in a very thin epitaxially grown silicon layer on a single crystal silicon wafer of which the die is singulated from. The side of the die including the epitaxial layer containing the transistors, and the other active circuitry is often referred to as the circuit side of the die or front side of the die. The circuit side of the die is positioned very near the package. The circuit side opposes the backside of the die. Between the backside and the circuit side of the die is single crystalline silicon. The positioning of the circuit side provides many of the advantages of the flip chip. However, in some instances the orientation of the die with the circuit side face down on a substrate may be a disadvantage or present new challenges. When a circuit fails or when it is necessary to modify a particular chip, access to the transistors and circuitry near the circuit side is obtained only from the backside of the chip. This is challenging since the transistors are in a very thin layer (about 10 μm) of silicon buried under the bulk silicon (&gt;500 μm). Thus, the circuit side of the flip chip die is not visible or accessible for viewing using optical or scanning electron microscopy. 
     Although the circuit of the integrated circuit (IC) is buried under the bulk silicon, infrared (IR) microscopy is capable of imaging the circuit because silicon is relatively transparent in these wavelengths of the radiation. However, because of the absorption losses of IR radiation in silicon, it is generally required to thin the die to less than 100 microns in order to view the circuit using IR microscopy. On a die that is 725 microns thick, this means removing at least 625 microns of silicon before IR microscopy can be used. Thinning the die for failure analysis of a flip chip bonded IC is usually accomplished in two or three steps. First, the die is thinned across the whole die surface. This is also referred to as global thinning. Global thinning is done to allow viewing of the active circuit from the backside of the die using IR microscopy. Mechanical polishing is one method for global thinning. 
     Once an area is identified using IR microscopy as an area of interest and it is determined that access is needed to a particular area of the circuit, local thinning techniques are used to thin an area smaller than the die size. Laser microchemical etching of silicon is one method of local thinning. One method for laser microchemical etching of silicon is accomplished by focussing a laser beam on the backside of the silicon surface to cause local melting of silicon in the presence of chlorine gas. The molten silicon reacts very rapidly with chlorine and forms silicon tetrachloride gas, which leaves the molten (reaction) zone. This is a silicon removal process used on the 9850 SiliconEtcher™ tool by Revise, Inc. (Burlington, Mass). This laser process is suitable for both local and global thinning by scanning the laser over a part or whole surface of the die. 
     Sometimes it is necessary for failure analysis, or for design debug, to make electrical contact and probe certain nodes in the circuit that is on the circuit side or front side of the die. This is generally done by milling through the die to access the node, or milling to the node and subsequently depositing a metal to electrically access the node. These access holes need to have high aspect rations. For design debug, it is desirable to have the capability of cutting the interconnect lines and rerouting of the interconnect lines. Milling through silicon with fairly high aspect ratio trenches is slow and is almost impractical for silicon thickness greater than 10 microns. For these reasons, it is necessary to have a method and apparatus which will provide for controlled thinning flip chip bonded IC devices to less than 10 micron thickness. It is also necessary to have a method where the thickness of the silicon can be determined with sufficient accuracy to avoid milling off the node to which access is being sought. Milling off the node could often jeopardize further device analysis. 
     The need for a method for accurately determining the thickness of the silicon is not eliminated by an approach where the backside is thinned to a distance away from the package to which the die is attached. Various parts tolerances do not allow for such a simple solution to approaching the circuit side of the die from the back side of the die. One tolerance issue revolves around keeping the height of solder ball contacts on the die substantially uniform for every packaged device of a particular type. Even though the solder ball contacts have a tolerance requirement, when the solder is reflowed to attach the die to a package, the amount of change in height due to solder reflow can vary by several microns. The thickness of the die between the circuit side and backside is also subject to tolerance differences. Since the thickness of the starting silicon wafer is a non-essential parameter for making a functioning die, typically the die thickness is not known to an accurate level. For instance, a typical die for a microprocessor may have a die thickness of 725±15 microns. The end result is tolerance stacking due to the tolerances for the size of the solder balls, the height at which the die is attached and the thickness of the die. These tolerances stack up such that there can be tens of microns of difference in height from the top surface of the package to the top surface of the die among different packaged devices. Although this does not sound like much of a tolerance problem, it should be noted that the epitaxial layer is only between 2 and 10 microns thick. As a result, the thickness of the remaining silicon of a trench cannot be gauged by measuring from the top surface of the package to the bottom of the trench. Stack up of the tolerances of the various parts precludes simply “measuring up” from the package to which the die is attached to determine where the epitaxial layer containing the transistors begins. Simply put, such an approach is not accurate enough to prevent ruining the circuitry or transistors that must be analyzed or debugged. Once the circuitry or transistors are ruined, analysis or debugging is impossible. 
     Therefore, the introduction of flip chip technology requires a method and apparatus for determining the thickness of silicon between a portion of the active circuitry near the circuit side of the die and the backside of the die. This is necessary to eliminate any guesswork as to the location of the circuitry while the backside of a die is being removed. If this guesswork is eliminated, it facilitates failure analysis and debugging of the circuitry associated with a particular integrated circuit. Furthermore, when the position of the circuitry is known or can be determined from the backside removal of the silicon, getting to the circuitry can be accomplished in less amount of time. Therefore, to facilitate more effective and efficient backside thinning processes, a measurement method and apparatus sensitive to the thickness of the remaining silicon is needed. Such a method and apparatus would be useful and essential for controlled backside thinning of silicon. 
     SUMMARY OF THE INVENTION 
     A system for determining the endpoint associated with removing silicon from the backside of a flip chip bonded die includes a tool for removing silicon and a light source for directing light to the backside of the die. An electrical measuring apparatus, such as a voltmeter, ammeter or oscilloscope, is attached across the output pins of a package to which the die is attached. The light directed toward the backside of the die induces a current in the devices formed in the semiconductor. The value of the current or voltage output depends on the thickness of material between the backside of the die where light is illuminated and the devices in the epitaxial layer of the die. The induced signal can be monitored to determine the thickness. Silicon can be removed globally until the thickness is reasonable such that a local thinning tool can be used to remove silicon to get to the area of interest in a reasonable amount of time. The induced current can be monitored during local thinning. A viewing mechanism such as infrared microscopy can be used to locate the specific device or devices of interest in the epitaxial layer of the die. The viewing mechanism is also used to determine where localized thinning will occur. 
     A method for using the system includes monitoring the thickness of the backside until a desired thickness is achieved. After global thinning, the viewing mechanism is used to select the area on the backside of the die for localized thinning. The induced signal is monitored during the thinning process until it reaches a specific value associated with a small distance between the surface resulting from the thinning process and the device of interest. 
     Advantageously, using this system and method provides for a much faster thinning of the backside to the area of interest since the distance between the backside of the chip or die and the circuit or device of interest is known. Since the distance between the backside of the die and the circuit device is also known, it is much less likely that the device of interest will be ruined as a result of thinning. The guess work formally associated with the thinning process is eliminated. This increases the effectiveness of debugging the circuit in a die or determining the failure of a particular die. In addition, this system and process can be done under control of a microprocessor or information handling system. 
    
    
     BRIEF DESCRIPTION OF THE DRAWINGS 
     The following detailed description of the preferred embodiments can best be understood when read in conjunction with the following drawings, in which: 
     FIG. 1 shows a side view of a flip chip packaged integrated circuit. 
     FIG. 2 shows a schematic view of a system for determining the distance to the active circuit of a flip chip attached to a substrate. 
     FIG. 3 shows a plot of a optical beam induced current signal measured from the active circuit on the flip chip as silicon is progressively removed from the back side of the flip chip. 
     FIG. 4 is a flow diagram of the method for monitoring the OBIC signal for detection of the endpoint of the silicon removal. 
     FIG. 5 is a flow diagram for in-process monitoring of the OBIC signal for detection of endpoint for silicon removal. 
     FIG. 6 is a schematic implementation of the system for closed loop control for silicon removal. 
     FIG. 7 is a schematic of an information handling system. 
    
    
     DETAILED DESCRIPTION OF THE PREFERRED EMBODIMENT 
     In the following detailed description of the preferred embodiments, reference is made to the accompanying drawings which form a part hereof, and in which are shown by way of illustration specific embodiments in which the invention may be practiced. It is to be understood that other embodiments may be utilized and structural changes may be made without departing from the scope of the present invention. 
     FIG. 1 shows a side view of a flip chip type die  100  having a circuit side  110  and a backside  120 . The circuit side  110  includes a number of circuit devices formed near the circuit side in a portion of the die known as the epitaxial layer  112 . The epitaxial layer  112  has a thickness in the range of 1 to 15 microns. A plurality of solder bumps  114  are made on the circuit side  110 . The solder bumps  114  are the inputs and outputs to the circuitry associated with the die  100 . The flip chip type die  100  is attached to a surface  130 , such as a package for a flip chip via the solder bumps on the die  100 . The surface  130  includes pads which are arranged to correspond to the pattern of solder bumps on the die  100 . The pads are electrically connected to circuitry within the package and then to pins, such as pin  140  and pin  142  shown in FIG.  1 . Pin  140  is VDD for the package and pin  142  is VSS for the package. 
     FIG. 2 shows a schematic view of a system  200  for determining the distance to the active circuit of a flip chip type die  100  attached to a substrate or surface  130 . The system includes a tool  210  for removing portions of the die. The tool  210  can be a used to globally thin the die, such as a polishing device or grinding device which removes silicon across the entire backside  120  surface. The tool  210  can also be used to locally thin a portion of the die  100 . Localized thinning is done on an area of the backside  120  which is less than the entire area of the backside  120 . Typically, the tool  210  is a combination of tools, one of which may do global thinning and another that can do localized thinning of the die  100 . Another typical tool is one that can perform both the localized and global thinning. 
     Preferably, for device failure analysis of a bonded flip chip type die  100 , the die is thinned across the whole die surface or globally thinned using a mechanical polishing device, such as a single platen calibrated polishing machine from Allied High Tech Products, Inc. of California. The global thinning is followed by local thinning in the area of interest on the die  100 . The local thinning is accomplished by laser microchemical etching of silicon. Laser microchemical etching is a method where a laser beam is focused on the backside  130  silicon surface to cause local melting of silicon in the presence of chlorine gas. The molten silicon reacts very rapidly with chlorine and forms silicon tetrachloride gas, and leaves the molten (reaction) zone. This is a silicon removal process used on the 9850 SiliconEtcher™ by Revise, Inc. (Burlington, Mass). This laser process is suitable for both local and global thinning by scanning the laser over a part or whole surface of the backside  130  of the flip chip type die  100 . 
     Chemical assisted ion etching is a method for silicon removal used in other tools. For example, chemical assisted ion etching is used in a Focused Ion Beam (FIB) tool made by Micrion Inc. of Peabody, Mass. In this process, local heating on the flip chip type die  100  due to focused ion beam accelerates etching of silicon in an environment having xenon difluoride. The xenon difluoride is continuously introduced to the die  100 . The reaction produces silicon fluoride and xenon gases which are removed by pumping them out at process temperature. This of course removes silicon from the die  100 . Of course, there are numerous other methods for removing silicon such as reactive ion etching. 
     The system  200  for determining the distance to the active circuit of a flip chip type die  100  attached to a substrate or surface  130  also includes a light source  220  which can be a broad spectrum type of light which produces a range of light frequencies or can be a laser which generally produces one wavelength of light. In other words, the light source  220  can be broad beam and include many different wavelengths of light or the light source can be monochromatic which produces light having a single wavelength. The light source  220  is directed at the backside  120  surface of the die  100  when the distance to the circuitry is desired. The system  200  for determining the distance to the active circuit of a flip chip type die  100  attached to a substrate or surface  130  also includes a device  230  for measuring electrical signals between the pins  240  or  242 . As shown in the system  200  for determining the distance to the active circuit of a flip chip type die  100  attached to a substrate or surface  130  the device  230  for measuring electrical signals is attached to pin  142  and pin  140 . The device  230  for measuring electrical signals is a transimpedance amplifier used to measure current. This amplifier converts current to voltage. The voltage output from the transimpedance amplifier is measured and recorded as OBIC signal. The transimpedance amplifier used in this application will not introduce a significant bias voltage across the VSS and VDD pins. However, if this bias voltage exceeds the threshold voltage for conduction of the p-n junctions, the measured current will be a sum of the OBIC component and diode (junction) current. Hence, the measured signal is not completely reflective of the OBIC signal. 
     The device  230  could also be an oscilloscope using its input impedance to convert current to voltage. Similarly, the OBIC current can be determined by measuring the voltage dropped across a known resistor using a voltmeter. 
     The strength of the output at the pins is indicative of the distance between the circuitry or devices found in the epitaxial layer near the circuit side  110  of the die  100  and the backside  120  of the die  100 . 
     A CMOS or bipolar IC includes several p-n junctions. When these junctions are exposed to light of photon energy higher than the band gap of silicon (1.1 eV), a photo current is generated. This is commonly referred to as an Optical Beam Induced Current (“OBIC”). The OBIC is measured across the VSS pin  142  and VDD pin  140  on the package of the IC while exposing the die to light from the light source  220 . The light source used was a green light generated at a preset power level from an argon-ion laser. 
     If the silicon thickness between the backside  120  of the die  100  and the devices or circuitry in the epitaxial layer  112  is greater than about 100 microns, the light beam will generate electron hole pairs near the surface of the backside  120  and very far from the depletion region of the junctions in specific devices in the epitaxial layer of die  100 . In this case, very few of the carriers can diffuse to the source and drain regions to generate OBIC signal at the VSS pin  142  or the VDD pin  140 . To a great extent, the carriers recombine before they reach the junction region. Hence the efficiency for generating photo current is low and little or no OBIC signal is produced at the pin  142 . 
     As the silicon is further thinned, sufficient intensity of the light beam can penetrate the thickness of silicon to generate electron hole pairs in the depletion region of the junction or very close to the depletion region of specific devices associated with the circuitry found in the epitaxial layer  112  of the die  100 . In this case, the carriers diffuse to the source and drain regions of one or more devices in the epitaxial region to generate photo current and the OBIC at the pins  142  and  140 . 
     Now turning to FIG. 3, it can be seen that the OBIC signal is a strong function of the amount of light reaching the junction. FIG. 3 shows a plot of an optical beam induced current signal measured from the active circuit on the flip chip as silicon is progressively removed from the back side  112  of the flip chip type die  100 . FIG. 3 is a plot of current data measured across the pins  142  (VSS) and  140  (VDD) of the package. The plot represents data produced by scanning a laser over a 300×300 micron area in the presence of chlorine gas. About 1.8 microns of silicon was removed from the backside  112  of the die  100  by each scan. During each scan, when the laser was positioned in the middle of a trench associated with local thinning, the OBIC signal was measured across VDD and VSS. A laser having power of 4W was used. The resulting OBIC signal was found to be strongly dependent on the remaining silicon thickness. 
     The plot of FIG. 3 can be mathematically described. The amount of light reaching the junction region is attenuated by absorption losses in silicon and is known to follow Beer&#39;s law. The attenuation is strongly dependent on the silicon thickness as follows: 
      I=I 0  exp(−αt) 
     Where I=the intensity of light, 
     I 0 =intensity of light incident on the back surface 
     α=absorption coefficient 
     t=thickness of the absorbing medium 
     With this technique, the thickness of the absorbing medium, namely the silicon between the backside  120  and the epitaxial layer  112 , can be monitored by observing the OBIC signal. Thus, the thickness of the remaining silicon during any removal process can be quantified. From this data it is clear that the OBIC signal can be monitored and used as an endpoint detection method for the removal of silicon using any type of removal process. By monitoring the OBIC signal, the removal of silicon can be stopped at desired thickness associated with the strength of the OBIC signal. 
     The absorption coefficient a, is dependent on the type of material and the wavelength of light used. The OBIC signal strength is directly proportional to the amount of light reaching the junction area or the attenuated light intensity. Hence, OBIC is a function of the incident light intensity and the silicon thickness while the other parameters, absorption coefficient and light wavelength are fixed. If the starting silicon thickness is t 0 , the OBIC signal S can be modeled as: 
     
       
         S=A exp(−α(t 0 −t r )) 
       
     
     where t r  is the thickness of silicon removed and A is a proportionality constant. Note that, in the above equation, (t 0 −t r ) is the thickness of remaining silicon. The above relation for OBIC signal I can also be written as: 
     
       
         S=B exp(αt r ). 
       
     
     For endpoint monitoring of silicon thickness, it is imperative that we predetermine the OBIC signal corresponding to the remaining silicon thickness. This can be referred to as a calibration scheme. For a light source of preset light intensity, and type of IC made using a given process technology, OBIC signal is monitored while backside silicon is removed in known amounts. Then the dice is cross-sectioned to determine the remaining silicon thickness corresponding to the OBIC signal observed. 
     FIG. 4 is a flow diagram of the method for monitoring the OBIC signal for detection of endpoint for silicon removal. The first step, depicted by reference number  402 , is to check for shorting between VDD and VSS pins. If there is no electrical short (Resistance, measured while applying a voltage of less than 0.1V, between the pins VDD and VSS&gt;100 Ohms) between the pins, a portion of silicon from backside is removed, as depicted by step  404 , and then the signal induced due to light exposure is checked again, as depicted by step  406 . The steps of silicon removal  404  and measuring induced current  406  are repeated until the signal strength of the induced signal corresponds to the signal for desired silicon thickness as depicted by reference number  408 . 
     FIG. 5 is a flow diagram of the method for in-process monitoring of the OBIC signal for detection of endpoint for silicon removal. The first step, depicted by reference number  502 , is to check for shorting between VDD and GND pins. If there is no electrical short (Resistance, measured while applying a voltage of less than 0.1 V, between the pins VDD and VSS&gt;100 Ohms) between the pins, the part is used for backside thinning of silicon. As the backside of silicon is thinned, light is exposed to the area being thinned and the induced signal is measured as depicted by step  504 . The next step  506  is to make a decision with respect to whether the signal strength is less than the expected value for the desired thickness. If the signal strength is equal to or greater than the signal strength associated with the desired thickness, the process is terminated, as depicted by number  508 . If the signal strength is less than the signal strength associated with the desired thickness, the process is continued. The signal is rerouted to step  504  where the silicon is removed while as the backside is illuminated and the strength of the signal is monitored. The signal strength is recorded, as depicted by reference number  510 . The signal may be used to update the display as depicted by reference number  512 . When the induced signal reaches the strength associated with the desired thickness of remaining silicon, terminate the thinning process. This way, closed-loop process control is achieved. It should be noted that if the silicon removal process is a laser-based process using a laser wavelength &lt;1.1 microns, then the same process laser may be used as the light source for OBIC signal. 
     FIG. 6 is an electronic schematic implementation of the apparatus or system  600  used for carrying out the process discussed with respect to FIG.  5 . The system  600  is similar to the system  200  for determining the distance to the active circuit of a flip chip type die  100 . Common components of the system  600  will carry the same reference numbers. The light source  220  which can be a broad spectrum type of light which produces a range of light frequencies or can be a laser which generally produces one wavelength of light. In other words, the light source  220  can be broad beam and include many different wavelengths of light or the light source can be monochromatic which produces light having a single wavelength. The light source  220  is constantly directed at the backside  120  surface of the die  100  when the distance to the circuitry is desired. The system  600  for determining the distance to the active circuit of a flip chip type die  100  attached to a substrate or surface  130  also includes a transimpedance amplifier,  610  for measuring electrical current between the pins VSS  142  and VDD  140 . The strength of the output at the pins  140  and  142  is indicative of the distance between the circuitry or devices found in the epitaxial layer near the circuit side  110  of the die  100  and the backside  120  of the die  100 . The output from the amplifier  610  is input to a comparator  620 . The comparator  620  compares the signal output from the transimpedance amplifier  610  to a selected value, also called the threshold value, which is also input to the comparator on line  622 . When the output from the transimpedance amplifier  610  equals the threshold value on line  622 , a control signal  630  is output to the silicon removal tool  210 . The control signal  630  stops the removal tool  210  from removing additional silicon from the backside  120  of the flip chip  100 . 
     It should be noted that this method will also work with other types of induced current. It should also be noted that this technique is not limited to use with silicon material nor is it limited to the field of semiconductors. This method could be used in other industries and with other materials. 
     Advantageously, the inventive method is well-suited for control by an information handling system  700 , such as computer or microprocessor. A generalized information handling system  700  is shown in FIG.  7 . The information. handling system  700  includes a central processing unit  704 , a random access memory  732 , and a system bus  730  for communicatively coupling the central processing unit  704  and the random access memory  732 . The system  700  may also include an input/output bus  710  and several devices peripheral devices, such as  712 ,  714 ,  716 ,  718 ,  720 , and  722  may be attached to the input output bus  710 . Peripheral devices may include hard disk drives, floppy disk drives, monitors, keyboards and other such peripherals. The information handling system  700  can be programmed to carry out the steps shown in FIGS. 4 and 5. The programmed process steps can be placed on any medium, such as the INTERNET, a tape drive, a floppy drive or a hard drive for use by the information handling system. The steps can also be distributed for use on other information handling systems using similar media. 
     Although specific embodiments have been illustrated and described herein, it is appreciated by those of ordinary skill in the art that any arrangement which is calculated to achieve the same purpose may be substituted for the specific embodiments shown. This application is intended to cover any adaptations or variations of the present invention. Therefore, it is manifestly intended that this invention be limited only by the claims and the equivalents thereof.