# Patent

## Title
Chuck for holding a device under test

## Abstract

A chuck that includes an upper surface for supporting a device under test and a conductive element that extends through the chuck to the upper surface of the chuck. The conductive element is electrically isolated from the upper surface of the chuck, and makes electrical contact with any device under test supported by the chuck.

## Background
This application claims the benefit of U.S. Patent application Ser. No. 60/473,232 filed May 23, 2003.


BACKGROUND OF THE INVENTION
The present application relates to an improved chuck.
With reference to FIGS. 1, 2A, 2B and 3, a probe station comprises a base 10 (shown partially) which supports a platen 12 through a number of jacks 14a, 14b, 14c, 14d which selectively raise and lower the platen vertically relative to the base by a small increment (approximately one-tenth of an inch) for purposes to be described hereafter. Also supported by the base 10 of the probe station is a motorized positioner 16 having a rectangular plunger 18 which supports a movable chuck assembly 20 for supporting a wafer or other test device. The chuck assembly 20 passes freely through a large aperture 22 in the platen 12 which permits the chuck assembly to be moved independently of the platen by the positioner 16 along X, Y and Z axes, i.e. horizontally along two mutually-perpendicular axes X and Y, and vertically along the Z axis. Likewise, the platen 12, when moved vertically by the jacks 14, moves independently of the chuck assembly 20 and the positioner 16.
Mounted atop the platen 12 are multiple individual probe positioners such as 24 (only one of which is shown), each having an extending member 26 to which is mounted a probe holder 28 which in turn supports a respective probe 30 for contacting wafers and other test devices mounted atop the chuck assembly 20. The probe positioner 24 has micrometer adjustments 34, 36 and 38 for adjusting the position of the probe holder 28, and thus the probe 30, along the X, Y and Z axes respectively, relative to the chuck assembly 20. The Z axis is exemplary of what is referred to herein loosely as the “axis of approach” between the probe holder 28 and the chuck assembly 20, although directions of approach which are neither vertical nor linear, along which the probe tip and wafer or other test device are brought into contact with each other, are also intended to be included within the meaning of the term “axis of approach.” A further micrometer adjustment 40 adjustably tilts the probe holder 28 to adjust planarity of the probe with respect to the wafer or other test device supported by the chuck assembly 20. As many as twelve individual probe positioners 24, each supporting a respective probe, may be arranged on the platen 12 around the chuck assembly 20 so as to converge radially toward the chuck assembly similarly to the spokes of a wheel. With such an arrangement, each individual positioner 24 can independently adjust its respective probe in the X, Y and Z directions, while the jacks 14 can be actuated to raise or lower the platen 12 and thus all of the positioners 24 and their respective probes in unison.
An environment control enclosure is composed of an upper box portion 42 rigidly attached to the platen 12, and a lower box portion 44 rigidly attached to the base 10. Both portions are made of steel or other suitable electrically conductive material to provide EMI shielding. To accommodate the small vertical movement between the two box portions 42 and 44 when the jacks 14 are actuated to raise or lower the platen 12, an electrically conductive resilient foam gasket 46, preferably composed of silver or carbon-impregnated silicone, is interposed peripherally at their mating juncture at the front of the enclosure and between the lower portion 44 and the platen 12 so that an EMI, substantially hermetic, and light seal are all maintained despite relative vertical movement between the two box portions 42 and 44. Even though the upper box portion 42 is rigidly attached to the platen 12, a similar gasket 47 is preferably interposed between the portion 42 and the top of the platen to maximize sealing.
With reference to FIGS. 5A and 5B, the top of the upper box portion 42 comprises an octagonal steel box 48 having eight side panels such as 49a and 49b through which the extending members 26 of the respective probe positioners 24 can penetrate movably. Each panel comprises a hollow housing in which a respective sheet 50 of resilient foam, which may be similar to the above-identified gasket material, is placed. Slits such as 52 are partially cut vertically in the foam in alignment with slots 54 formed in the inner and outer surfaces of each panel housing, through which a respective extending member 26 of a respective probe positioner 24 can pass movably. The slitted foam permits X, Y and Z movement of the extending members 26 of each probe positioner, while maintaining the EMI, substantially hermetic, and light seal provided by the enclosure. In four of the panels, to enable a greater range of X and Y movement, the foam sheet 50 is sandwiched between a pair of steel plates 55 having slots 54 therein, such plates being slidable transversely within the panel housing through a range of movement encompassed by larger slots 56 in the inner and outer surfaces of the panel housing.
Atop the octagonal box 48, a circular viewing aperture 58 is provided, having a recessed circular transparent sealing window 60 therein. A bracket 62 holds an apertured sliding shutter 64 to selectively permit or prevent the passage of light through the window. A stereoscope (not shown) connected to a CRT monitor can be placed above the window to provide a magnified display of the wafer or other test device and the probe tip for proper probe placement during set-up or operation. Alternatively, the window 60 can be removed and a microscope lens (not shown) surrounded by a foam gasket can be inserted through the viewing aperture 58 with the foam providing EMI, hermetic and light sealing. The upper box portion 42 of the environment control enclosure also includes a hinged steel door 68 which pivots outwardly about the pivot axis of a hinge 70 as shown in FIG. 2A. The hinge biases the door downwardly toward the top of the upper box portion 42 so that it forms a tight, overlapping, sliding peripheral seal 68a with the top of the upper box portion. When the door is open, and the chuck assembly 20 is moved by the positioner 16 beneath the door opening as shown in FIG. 2A, the chuck assembly is accessible for loading and unloading.
With reference to FIGS. 3 and 4, the sealing integrity of the enclosure is likewise maintained throughout positioning movements by the motorized positioner 16 due to the provision of a series of four sealing plates 72, 74, 76 and 78 stacked slidably atop one another. The sizes of the plates progress increasingly from the top to the bottom one, as do the respective sizes of the central apertures 72a,74a, 76a and 78a formed in the respective plates 72, 74, 76 and 78, and the aperture 79a formed in the bottom 44a of the lower box portion 44. The central aperture 72a in the top plate 72 mates closely around the bearing housing 18a of the vertically-movable plunger 18. The next plate in the downward progression, plate 74, has an upwardly-projecting peripheral margin 74b which limits the extent to which the plate 72 can slide across the top of the plate 74. The central aperture 74a in the plate 74 is of a size to permit the positioner 16 to move the plunger 18 and its bearing housing 18a transversely along the X and Y axes until the edge of the top plate 72 abuts against the margin 74b of the plate 74. The size of the aperture 74a is, however, too small to be uncovered by the top plate 72 when such abutment occurs, and therefore a seal is maintained between the plates 72 and 74 regardless of the movement of the plunger 18 and its bearing housing along the X and Y axes. Further movement of the plunger 18 and bearing housing in the direction of abutment of the plate 72 with the margin 74b results in the sliding of the plate 74 toward the peripheral margin 76b of the next underlying plate 76. Again, the central aperture 76a in the plate 76 is large enough to permit abutment of the plate 74 with the margin 76b, but small enough to prevent the plate 74 from uncovering the aperture 76a, thereby likewise maintaining the seal between the plates 74 and 76. Still further movement of the plunger 18 and bearing housing in the same direction causes similar sliding of the plates 76 and 78 relative to their underlying plates into abutment with the margin 78b and the side of the box portion 44, respectively, without the apertures 78a and 79a becoming uncovered. This combination of sliding plates and central apertures of progressively increasing size permits a full range of movement of the plunger 18 along the X and Y axes by the positioner 16, while maintaining the enclosure in a sealed condition despite such positioning movement. The EMI sealing provided by this structure is effective even with respect to the electric motors of the positioner 16, since they are located below the sliding plates.
With particular reference to FIGS. 3, 6 and 7, the chuck assembly 20 is a modular construction usable either with or without an environment control enclosure. The plunger 18 supports an adjustment plate 79 which in turn supports first, second and third chuck assembly elements 80, 81 and 83, respectively, positioned at progressively greater distances from the probe(s) along the axis of approach. Element 83 is a conductive rectangular stage or shield 83 which detachably mounts conductive elements 80 and 81 of circular shape. The element 80 has a planar upwardly-facing wafer-supporting surface 82 having an array of vertical apertures 84 therein. These apertures communicate with respective chambers separated by O-rings 88, the chambers in turn being connected separately to different vacuum lines 90a, 90b, 90c (FIG. 6) communicating through separately-controlled vacuum valves (not shown) with a source of vacuum. The respective vacuum lines selectively connect the respective chambers and their apertures to the source of vacuum to hold the wafer, or alternatively isolate the apertures from the source of vacuum to release the wafer, in a conventional manner. The separate operability of the respective chambers and their corresponding apertures enables the chuck to hold wafers of different diameters.
In addition to the circular elements 80 and 81, auxiliary chucks such as 92 and 94 are detachably mounted on the corners of the element 83 by screws (not shown) independently of the elements 80 and 81 for the purpose of supporting contact substrates and calibration substrates while a wafer or other test device is simultaneously supported by the element 80. Each auxiliary chuck 92, 94 has its own separate upwardly-facing planar surface 100, 102 respectively, in parallel relationship to the surface 82 of the element 80. Vacuum apertures 104 protrude through the surfaces 100 and 102 from communication with respective chambers within the body of each auxiliary chuck. Each of these chambers in turn communicates through a separate vacuum line and a separate independently-actuated vacuum valve (not shown) with a source of vacuum, each such valve selectively connecting or isolating the respective sets of apertures 104 with respect to the source of vacuum independently of the operation of the apertures 84 of the element 80, so as to selectively hold or release a contact substrate or calibration substrate located on the respective surfaces 100 and 102 independently of the wafer or other test device. An optional metal shield 106 may protrude upwardly from the edges of the element 83 to surround the other elements 80, 81 and the auxiliary chucks 92, 94.
All of the chuck assembly elements 80, 81 and 83, as well as the additional chuck assembly element 79, are electrically insulated from one another even though they are constructed of electrically conductive metal and interconnected detachably by metallic screws such as 96. With reference to FIGS. 3 and 3A, the electrical insulation results from the fact that, in addition to the resilient dielectric O-rings 88, dielectric spacers 85 and dielectric washers 86 are provided. These, coupled with the fact that the screws 96 pass through oversized apertures in the lower one of the two elements which each screw joins together thereby preventing electrical contact between the shank of the screw and the lower element, provide the desired insulation. As is apparent in FIG. 3, the dielectric spacers 85 extend over only minor portions of the opposing surface areas of the interconnected chuck assembly elements, thereby leaving air gaps between the opposing surfaces over major portions of their respective areas. Such air gaps minimize the dielectric constant in the spaces between the respective chuck assembly elements, thereby correspondingly minimizing the capacitance between them and the ability for electrical current to leak from one element to another. Preferably the spacers and washers 85 and 86, respectively, are constructed of a material having the lowest possible dielectric constant consistent with high dimensional stability and high volume resistivity. A suitable material for the spacers and washers is glass epoxy, or acetal homopolymer marketed under the trademark Delrin by E. I. DuPont.
With reference to FIGS. 6 and 7, the chuck assembly 20 also includes a pair of detachable electrical connector assemblies designated generally as 108 and 110, each having at least two conductive connector elements 108a, 108b and 118a, 110b, respectively, electrically insulated from each other, with the connector elements 108b and 110b preferably coaxially surrounding the connector elements 108a and 110a as guards therefor. If desired, the connector assemblies 108 and 110 can be triaxial in configuration so as to include respective outer shields 108c, 110c surrounding the respective connector elements 108b and 110b, as shown in FIG. 7. The outer shields 108c and 110c may, if desired, be connected electrically through a shielding box 112 and a connector supporting bracket 113 to the chuck assembly element 83, although such electrical connection is optional particularly in view of the surrounding EMI shielding enclosure 42, 44. In any case, the respective connector elements 108a and 110b are electrically connected in parallel to a connector plate 114 matingly and detachably connected along a curved contact surface 114a by screws 114b and 114c to the curved edge of the chuck assembly element 80. Conversely, the connector elements 108b and 110b are connected in parallel to a connector plate 116 similarly matingly connected detachably to element 81. The connector elements pass freely through a rectangular opening 112a in the box 112, being electrically insulated from the box 112 and therefore from the element 83, as well as being electrically insulated from each other. Set screws such as 118 detachably fasten the connector elements to the respective connector plates 114 and 116.
Either coaxial or, as shown, triaxial cables 118 and 120 form portions of the respective detachable electrical connector assemblies 108 and 110, as do their respective triaxial detachable connectors 122 and 124 which penetrate a wall of the lower portion 44 of the environment control enclosure so that the outer shields of the triaxial connectors 122, 124 are electrically connected to the enclosure. Further triaxial cables 122a, 124a are detachably connectable to the connectors 122 and 124 from suitable test equipment such as a Hewlett-Packard 4142B modular DC source/monitor or a Hewlett-Packard 4284A precision LCR meter, depending upon the test application. If the cables 118 and 120 are merely coaxial cables or other types of cables having only two conductors, one conductor interconnects the inner (signal) connector element of a respective connector 122 or 124 with a respective connector element 108a or 110a, while the other conductor connects the intermediate (guard) connector element of a respective connector 122 or 124 with a respective connector element 108b, 110b, U.S. Pat. No. 5,532,609 discloses a probe station and chuck and is hereby incorporated by reference.
The chuck assembly 20 with corresponding vertical apertures 84 and respective chambers separated by O-rings 88 permits selectively creating a vacuum within three different zones. Including the three O-rings 88 and the dielectric spacers 85 surrounding the metallic screws 96 permits securing adjacent first, second and third chuck assembly elements 80, 81 and 83 together. The concentric O-rings 88 are squeezed by the first and second chuck assembly elements and assist in distributing the force across the upper surface of the chuck assembly 20 to maintain a flat surface. However, the O-rings and dielectric spacers 85 have a greater dielectric constant than the surrounding air resulting in leakage currents. Also, the additional material between adjoining chuck assembly elements 80, 81, and 83 decreases the capacitance between the adjoining chuck assembly elements. Moreover, the dielectric material of the O-rings and dielectric spacers 85 builds up a charge therein during testing which increases the dielectric absorption. The O-rings and dielectric spacers 85 provides mechanical stability against warping the chuck when a wafer thereon is probed so that thinner chuck assembly elements 80, 81, and 83 may be used. The height of the different O-rings and dielectric spacers 85 tend to be slightly different which introduces non-planarity in the upper surface when the first, second, and third chuck assembly elements 80, 81, and 83 are secured together.



BRIEF DESCRIPTION OF THE DRAWINGS
FIG. 1 is a partial front view of an exemplary embodiment of a wafer probe station constructed in accordance with the present invention.
FIG. 2A is a partial top view of the wafer probe station of FIG. 1 with the enclosure door shown partially open.
FIG. 2B is a top view of the wafer probe station of FIG. 1.
FIG. 3 is a partially sectional and partially schematic front view of the probe station of FIG. 1.
FIG. 3A is an enlarged sectional view taken along line 3A-3A of FIG. 3.
FIG. 4 is a top view of the sealing assembly where the motorized positioning mechanism extends through the bottom of the enclosure.
FIG. 5A is an enlarged top detail view taken along line 5A-5A of FIG. 1.
FIG. 5B is an enlarged top sectional view taken along line 5B-5B of FIG. 1.
FIG. 6 is a partially schematic top detail view of the chuck assembly, taken along line 6-6 of FIG. 3.
FIG. 7 is a partially sectional front view of the chuck assembly of FIG. 6.
FIG. 8 illustrates a measurement setup.
FIG. 9 illustrates trench MOS characteristics for the setup of FIG. 8.
FIG. 10 illustrates another measurement setup.
FIG. 11 illustrates trench MOS characteristics for the setup of FIG. 10.
FIG. 12 illustrates another measurement setup.
FIG. 13 illustrates an equivalent circuit for the setup of FIG. 12.
FIG. 14 illustrates another measurement setup.
FIG. 15 illustrates an equivalent circuit for the setup of FIG. 14.
FIG. 16 illustrates another measurement setup and modified chuck.
FIG. 17 illustrates another modified chuck.
FIG. 18 illustrates another modified chuck.



DETAILED DESCRIPTION OF THE PREFERRED EMBODIMENT
Frequently in the construction of a chuck, a pair of cables are connected to the chuck, either in the manner shown in FIGS. 6 and 7, or otherwise the two cables 118 and 120 are each separately connected directly to the exterior periphery of the chuck 82. In this manner the conductive periphery of the chuck acts as a common signal path for both of the cables.
With particular regard to chucks that are specially adapted for use in measuring ultra-low current (down to the femtoamp region or lower), chuck designers have been concerned with developing techniques for eliminating or at least reducing the effects of leakage currents, which are unwanted currents that can flow into a particular cable or channel from surrounding cables or channels so as to distort the current measured in that particular cable or channel.
One technique that has been used for suppressing undesired leakage currents is surrounding the inner core of each lead-in wire with a cylindrical “guard” conductor, where the “guard” conductor is maintained at the same potential as the inner core by a feedback circuit in the output channel of the test instrument. Because the voltage potentials of the outer guard conductor and the inner conductive core are made to substantially track each other, negligible leakage current will flow across the inner dielectric that separates these conductors regardless of whether the inner dielectric is made of a low- or high-resistivity material. Although leakage current can still flow between the guard conductors of the respective cables, this is typically not a problem because these guard conductors, unlike the inner conductive cores, are at low impedance. By using this guarding technique, significant improvement may be realized in the low-level current measuring capability of certain probe card designs.
It has been found, however, that even with the use of guarded cables of the type just described, the level of undesired background current is still not sufficiently reduced as to match the capabilities of the latest generation of commercially available test instruments, which instruments are able to monitor currents down to one femtoamp or less.
To further increase measurement accuracy, ideally in a two lead coaxial cable system a “true Kelvin” connection is constructed. This involves using what is generally referred to as a force signal and a sense signal. The signal conductor from one of the coaxial cables is considered the force conductor, while the signal conductor from the other coaxial cable is considered the sense conductor. The force conductor is a low impedance connection, so a current is forced through the force conductor for testing purposes. The sense conductor is a high impedance connection, preferably in close proximity to the sense conductor, in order to sense the voltage. As such the current versus voltage characteristics of the test device can be obtained using the force and sense conductors.
To calibrate the “true Kelvin” connection, first an open circuit test is performed to measure the capacitance without the load capacitance. This is performed by disconnecting the probes and shorting the probe tips of the sense and force conductors together with both suspended in air. The open circuit test is difficult to perform. Second, a short circuit test is performed to measure the capacitance when the force and sense conductors are on the load. From the open circuit test and the short circuit test the cable impedance is obtained and thereafter used for offsetting during subsequent measurements. Unfortunately, calibration of a “true Kelvin” connection is difficult and time consuming to perform. Additionally, the current flowing through the force conductor is generally known but the resistance drop along the length of force conductor results in the exact voltage at its end to be unknown, therefore the measurement can be inaccurate.
A quasi-Kelvin measurement maybe considered when the force and sense are combined together prior to the device being measured. This is the case when the chuck is considered part of the joint signal path to the wafer, or the force and sense are joined together as illustrated in FIGS. 6 and 7. The length of the signal path extending from the point that the force conductor and sense conductor are connected together carries current during measurements which results in a voltage drop from any internal resistance in that portion of the signal path. The assumption is that for low current applications, the voltage drop due to the resistance is small because the junction is close to the measurement point and the conductor has low resistance.
There is a desire to measure the drain to source resistance of semiconductor based FETs (e.g., Rds), which is normally the connection between the source and the conductive backside metal on the wafer, which is acting as a join drain. The Rds resistance is typically measured with the gate to source of the FET being biased to induce the conductive channel. It is to be expected that using a Kelvin connection that an extremely accurate measurement of the Rds resistance may be obtained. When making such a measurement it turns out that the Rds is about 40 milli-ohms which is many times greater than the expected value (e.g. 8 milli-ohms).
The measurement setup to perform this measurement is shown in FIG. 8. A source measurement unit 1 is connected to the gate to sweep a voltage, a source measurement unit 2 is connected to the source of the FET to provide a source connection. A voltage measurement unit 2 is connected to the source of the FET to provide a force connection. A source measurement unit 3 provides both a source connection and a force connection to the drain of the FET.
Referring to FIG. 9 it is shown, to the surprise of the present inventors, that the drain current 300 for a gold coated chuck surface is much greater than the drain current 302 for a nickel coated chuck surface. Similarly, it is shown to the surprise of the present inventors, that the Rds 304 for the nickel coated chuck surface is much greater than the Rds 306 for the gold coated chuck surface. It is unexpected that the difference between using a nickel surface and a gold surface of the chuck would result in such a difference, especially since both are of low resistance and conductive, and accordingly a gold surface for the chuck is preferable.
The unexpected difference in the surface coatings lead the present inventors to consider that perhaps there is a previously unconsidered embedded resistance somewhere in the conductive path that is resulting in the difference in the measurements. To investigate this the present inventors modified the chuck connection arrangement on the drain. Rather than modify the electrical connections themselves in a typical manner, the present inventors physically arranged the wafer in a manner that was slightly overhanging with the edge of the gold coated chuck. The force connection was made in the same manner as FIG. 8, while the sense connection was made using a probe with the needle in direct contact with the back of the wafer in the small area overhanging the chuck, as denoted on FIG. 10. The result of this modified measurement is shown in FIG. 11. To the present inventors surprise the Rds measurement was as expected, though the measurement using the traditional Kelvin type connection unexpectedly provided an inaccurate measurement. While making such a measurement using direct connection to the backside of the wafer is possible, it would be desirable to include a similar functionality within the chuck itself. Apparently in reflection, the present inventors came to the realization that any backside oxidation, contamination, film, or otherwise, may build up on the wafer and/or chuck surfaces in a manner sufficient to modify the measurements sufficiently, especially at such low measurement values.
Referring to FIG. 12, the measurement issue may be presented schematically where Rds is given by:

Rds=(VMU1 −VMU2)/Ids

The equivalent circuit for this measurement is represented in FIG. 13. In the diagram Rpf is the probe contact resistance on the source for the force contact and Rps is the probe contact resistance for the sense contact. Rpf does not need to be equal to Rps because the VMU 1 measurement impedance is very high and the resulting measurement current is very low compared with the current flowing from source to drain. The voltage (Rpf ×Ids) does not therefore form a significant part of the measurement of VMU1.
On the other hand, the contact resistance between the chuck and the drain metal, Rc does affect the measurement because it is common to both the force part of the circuit and the sense connection made by VMU2. Thus instead of measuring the voltage dropped only across Rds, the difference between VMU1 and VMU2 divided by Ids gives the sum of Rds and Rc. In this configuration Rds and Rc cannot be separated. In many cases Rc and Rds are most likely comparable in magnitude for the type of device measurements of interest. This will therefore result in a large error in the measurement of Rds using this technique. In the case of the gold chuck in the measurement in FIG. 9 the error is more than 100% and in the case of the nickel chuck of FIG. 9 the error is more than 700%.
Accordingly, the present inventors came to the realization that the problem that exists is that the measurement terminal for VMU2 should be between Rds and Rc so that a true measurement of Rds may be performed.
Referring to FIG. 14, to create such a change in the measurement terminal for VMU2 the sense connection is made in a more direct matter to the drain metal contact of the wafer. This may be accomplished by, for example, having a small area of the chuck surface insulated from the remainder of the chuck surface and making contact from the VMU2 sense connection to that region of the chuck surface.
The equivalent circuit for this arrangement is shown in FIG. 15. As it is shown that the previous resistance Rc has been replaced with a chuck contact resistance, Rcf, for the force connection. This value will be a relatively low value, but perhaps larger than the value of Rds to be measured. The chuck sense connection has a contact resistance, Rcs. This may be a much higher value than Rcf. However, it does not matter what the value of Rcf is since it serves only to provide a connection to VMU2 which iteself has a high impedance. Thus VMU2 is now able to sense the voltage directly at the drain metal contact. Therefore, even if this second contact is small, and perhaps a long way from the device under test location, the added resistance between the device contact and the VMU it not important. An example configuration is illustrated in FIG. 16, where the VMU2 sense connection is electrically isolated from the SMU2 force connection.
The exact conditions under which the resistances Rps and Rcs can be neglected depend on the input impedance of the VMUs which in turn determine the ratio of the their measurement currents to Ids. Even with low Ids values in the 50 mA range, the VMU measurement current should be negligible. It is to be understood that even under drastically different probing conditions the teachings herein may likewise be applied.
Applying the usual circuit equations and Ohm's Law one may write:




  
    
      V
      d
    
    -
    
      
        V
        s
      
      ⁡
      
        (
        
          
            I
            ds
          
          
            
              I
              ds
            
            -
            
              I
              VMU2
            
          
        
        )
      
    
  
  =
  
    
      I
      ds
    
    ⁡
    
      (
      
        
          R
          ds
        
        +
        
          
            R
            cf
            2
          
          
            
              R
              cf
            
            +
            
              R
              cs
            
            +
            Z
          
        
      
      )
    
  




These conditions which must be satisfied to ensure that




  
    R
    ds
  
  =
  
    
      
        V
        d
      
      -
      
        V
        s
      
    
    
      I
      ds
    
  




is accurate according to the measurements of Vd, Vs and Ids are:





  
    
      
        
          
            R
            cf
          
          
            
              R
              cf
            
            +
            
              R
              cs
            
            +
            Z
          
        
        ⪡
        1
      
    
    
      
        
      
    
    
      and
    
    
      
        
      
    
    
      
        
          
            R
            cf
            2
          
          
            
              R
              cf
            
            +
            
              R
              cs
            
            +
            Z
          
        
        ≈
        0
      
    
  




where Z is the input impedance of the VMU.

These conditions are essentially identical and both may be satisfied when the input impedance of the VMU is much greater than the various contact resistances in the measurement circuit. It is noted that any resistance common to both the ‘force’ and the ‘sense’ contacts for either probe or chuck will lead to errors in the Rds measurement, so these resistances should be minimized.
While the embodiment illustrated in FIG. 16 is acceptable, another embodiment is illustrated in FIG. 17. FIG. 17 may be the chuck itself 400 or a plate supported by the chuck, typically using vacuum. The sense conductor 402 may pass within the chuck through an opening 404. The top 406 of the chuck is conductive and supports the wafer thereon. An dielectric spacer 408 may be included or otherwise a gap in the top 406 of the chuck. A central conductive region 410 may be included that has substantially the same elevation as the top 406 of the chuck. The central region 410 may include a flexible contact 412 that is biased such that a portion of the flexible contact 412 is depressed upon placing a waver upon the chuck 400. In this manner a good contact is made between the flexible contact and the wafer. In this manner, the central region connected to the sense connection is electrically isolated from the force connection connected to the remainder of the chuck. Other suitable interconnections may likewise be used, where the force and sense connections are isolated to a point in contact with the wafer itself, such that the wafer provides the interconnection between the force and sense connection.
Referring to FIG. 18, another embodiment includes a sense conductor 500 that is electrically interconnected to a contact assembly 502 on the reverse of a plate assembly 510 to be supported by the chuck. The contact assembly 502 includes a pair of screws 504 and 506 securing a flexible conductive member 508 within a depression in the plate assembly 510. The flexible conductive member 508 is electrically interconnected to a conductive pin 512. The conductive pin 512 may be surrounded by an insulator 514, if desired. The conductive pin 512 and insulator 514 extends through the plate assembly 510 to a position slightly above the surface of the front surface of the plate assembly 510. The conductive pin 512, flexible conductive member 508, sense conductor 500 are electrically isolated from the remainder of the plate assembly 510 which acts as part of the force path for making measurements (e.g., chuck to plate assembly to wafer). The plate assembly 510 is secured to the chuck, such as using vacuum, and a contact is made to the wafer by depressing the conductive pin 512. In this manner, separate paths for the force and sense conductors are maintained to the wafer.

## Claims

1. A probe station for probing a device under test having a probing surface, said probe station comprising:
(a) a chuck having an upper surface suitable to support said device under test, and at least one probe suitable to probe said device under test while said probing surface is facing away from said upper surface;
(b) a conductive element electrically isolated from said upper surface of said chuck and extending through said chuck to said upper surface of said chuck; and
(c) said conductive element positioned so as to electrically contact said device under test when said device under test is being probed by said at least one probe and while said probing surface is facing away from said upper surface;
(d) said conductive element is electrically interconnected to the edge of said chuck.

2. The chuck of claim 1 wherein said device under test is interconnected to a force connection.

3. The chuck of claim 1 wherein a sense connection is interconnected to the backside of said device under test.

4. The chuck of claim 1 wherein said conductive element included a moveable contact at its terminal end.

5. The chuck of claim 1 wherein said conductive element includes a portion ending above the upper surface of said chuck.

6. The chuck of claim 5 wherein said portion ends above the upper surface of said chuck when said device under test is not supported by said chuck.