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Signatone
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OMEGA-PRO DATA SHEET
Data Sheet · Resistivity Systems

Signatone ΩPro Resistance Testing System

ΩPro probe test solution performs numerous tests involving resistance measurements.

Features / Benefits

precision surface temperature probe.

The ΩPro solution is the test management software integrated with Signatone hardware to achieve the desired measurements. The complete system includes a semiautomatic probe station equipped with a thermal chuck and microscope with CCD digital camera integrated with a vibration isolation table. Four independent probes, a 4-point probe, and probe card adapter and cabling provide the test signal connections between DUT and meters. The meter set includes a precision volt meter, source meter, and programmable switch. A precision temperature probe provides accurate surface temperatures for TCR tests.

The ΩPro test management software and results are viewed on one of the dual screen monitors. The other monitor displays probe station navigation and component status. Configurations are easily stored for future use. All test results may be exported to spread sheets or printed.

Sheet resistance mapping of thin films with a collinear 4-point probe

(photo left)

This test measures three parameters of thin films or thin materials – sheet resistance of the surface, resistivity of the material or thickness of the material. Results are reported in ohms-square, ohms-cm or microns. The measurements employ NIST standards SRM’s 2541-2547 for measurement of semiconductor materials.

Maps of the entire surface in 2D or 3D formats may be printed or exported to a spread sheet. The mapping features allows users to determine if their film deposit processes are uniform and within tolerance.

Once the test is defined and started, each test site is automatically tested and results recorded. False tests are determined and retested automatically. The statistical results of Average, Standard Deviation, Maximum, Minimum and 1-Sigma are prominently displayed.

(photo right)

Some key features of the sheet measurement test include Autorange, Dual Configuration, and Calibration. Autorange automatically selects the proper current forced to achieve the measurement. The software controls stepping through several settings before selecting the current that meets the standard and produces repeatable results. Dual Configuration adds extra measurements with different pin selections to calculate and eliminate geometric and test set-up errors. Calibration verifies the system is measuring correctly when compared to a NIST standard.

The mechanical set up includes a 4-point probe mounted on a SM40 stable micropositioner. The SM40 features 12mm X-Y-Z positioning and probe planarization. The four-point probe heads have a variety of configurations available meet the test demands. The user has the option to use the semiautomatic probe station test site programming or the automated test site programing for determining actual test sites on the DUT

This test builds on the capability of the sheet resistance test. Mechanically, the set-up is the same. However, the user may wish to add the precision surface temperature probe placed near the probe head. This will assure the surface temperature measured is correct. The surface temperature probe has 1/100 degree resolution utilizing a 4 wire RTD sensor.

The ΩPro test manager allows the user to define settings and temperatures applicable to the DUT. The user defines the temperature range and number of temperature steps desired and settling time at temperature. For example, the user may set starting temperature at 25°C and ending temperature at 125°C with 4 steps. The results table is automatically created. (table below)

Target °CActual °CRs (Ω □)∆/°CTCR-PPM
2524.975.063refref
5050.676.1270.041400778551.5470766
7575.277.0040.038588469514.0810943
100100.178.0190.039308511523.6735894
125124.778.9930.039378758524.6094283

Starting the test will drive the DUT to the 1st temperature and settle. The first Rs measurement is taken and recorded as the reference temperature. Automatically, the ΩPro drives the temperature to the next set point and settles. Once settled, the next Rs measurement is taken. Change per degree C and TCR in parts per million are calculated in comparison to the reference measurement. This same process repeats for all of the temperature settings. A line graph is also plotted showing the TCR measurement

(line graph right)

TCR measurements are typically performed just at one site. However, the ΩPro manager allows users to define up 9 sites with graphics. In this automated mode, the sample is cycled at each selected site automatically.

This ΩPro test mode allows accurate measurements of structured resistors on the device under test (DUT). Two probe tips contact each contact pad and the Kelvin measurement method is used. The Kelvin or 4 wire sense mode of measuring resistance eliminates errors introduced from the wiring and fixtures assuring accurate measurements.

Integrated with the semiautomatic capabilities of the Signatone probe station and the ‘Contact Sense’ mode of the source meter, users may test a whole wafer or substrate unattended. Operators define the test criteria by selecting the test sites and pass/ fail criteria. The DUT is loaded onto the probe station and the 1st location tested manually to assure all is set correctly.

Then the ΩPro manager begins testing by moving to the 1st site. The probe tips are brought into the contact position. The source meter verifies there is indeed contact using the built-in contact sense mode. If not, the DUT is moved up or down 5 microns, scrubbing the probe tips and contact is checked again. This continues for 10 checks or until contact is verified. The measurement is then taken applying the test settings and 4 wire sense mode. If the reading is within the defined tolerance, the wafer graph or DUT graph paints this location green. If the measurement is outside of the acceptable parameters, the site is painted red. The data is placed into a table and the statistical data is updated.

PColRowΩ OhmsStatus
11175.063pass
22175.021pass
33175.117fail
44175.061pass
55174.989pass
65274.993pass
74275.003pass
83274.997pass
92274.951pass
101274.916fail

Statistics

Results Table

Average75.011
Standard Deviation.054984
Maximum75.117
Minimum74.916
1 Sigma0.073
Yield80%

This ΩPro test mode allows accurate measurements of structured resistors on multiple devices by using a probe card. The test set up follows closely the Kelvin probe set up procedures.

The probe card (not included) should have 2 probes per pad independently wired to the 25 pin D-sub connections. Once the user defines the proper step size and aligns to the 1st position, the test is automated by the ΩPro manager. Each contact is verified on each resistor. The individual resistor is tested and using the switch technology. Results are recorded and the wafer graph updated according to the results.

Signatone offers probe card adapters for 4.5 inch wide or 6 inch wide probe cards. The included switch can accommodate up to 10 4-wire connections or a 40 pin probe card. The test results are displayed the same as Kelvin probe testing. (wafer graph Image bottom left -probe card and adapter image bottom right)

This mode of the ΩPro manager permits precise TCR measurements on completed resistors. It is set up the same as a Kelvin resistance test but the accurate surface temperature probe is placed nearby. The thermal chuck heats the DUT and the temperature probe accurately senses the surface temperature. Several test sites may be defined for precision measurements. The test results will include line graphs for the first 9 test sites. The user defines the temperature range and number of temperature steps desired and settling time at temperature.

In keeping with the theory of TCR measurements, once the probes are verified to be in contact, they remain so throughout the temperature cycle and number of temperature steps desired and settling time at temperature. (image above: two kelvin probes and temperature probe)

ΩPro accurately manages the temperature cycle. The thermal chuck heats to the target temperature. After brief settling time, the surface temperature is checked. If the target temperature and the surface temperature are not within the predefined tolerance, ΩPro makes the necessary temperature adjustment until the temperature is stable and within the tolerance band (usually ±0.5°C). The resistance measurement is taken 5 times and the median value accepted and recorded. Change per degree C and TCR in PPM are calculated based as compared to the reference temperature.

The chuck then heats to the next temperature and settles. Then the next measurement is made. This continues until all temperature steps are complete. The chuck and sample are then cooled back to room temperature. If multiple test sites are programmed, the probe station moves the sample to the next site and starts the cycle again. This temperature and test cycle continue until all sites are measured.

(sample table of results – next page)

PColRowTarget °CActual °C∆/°CTCR-PPM
1-r17112524.975.063refref
1-15050.376.1270.041400778551.5470766
1-27575.277.0040.038588469514.0810943
1-3100100.178.0190.039308511523.6735894
1-4125124.778.9930.039378758524.6094283
2-r18212524.9075.059refref
2-15050.1076.1270.04155642553.6500651
2-27575.4077.0040.038667992515.1679618
2-3100100.2078.0190.039361702524.410159
2-4125124.9078.9930.039418838525.1713675

Probe Card

This mode of the ΩPro manager permits TCR measurements on completed resistors. It may be set up as a Kelvin resistance test with individual probes or a probe card. The thermal chuck heats the DUT. All test sites may be defined for measurements. The user defines the temperature range and number of temperature steps desired and settling time at temperature.

ΩPro accurately manages the temperature cycle and positioning. The thermal chuck heats to the target temperature. After predetermined settling time, the probes contact the DUT and contact is checked. If contact is not good, the chuck is raised or lowered 5 microns and contact is checked again. The resistance measurement is taken and then recorded as the reference (ref) resistance. The chuck temperature is also recorded. All of the predetermined test sites, which could be the whole wafer or substrate, are tested at this temperature.

The chuck then heats to the next temperature and settles. Moving back to the first test site, the resistance is measured once again. The resistance is compared to the reference measurement of the 1st test or (ref) value for that test site. The resistance, change per degree and TCR value are then recorded. Each site is recorded in the same way.

The chuck then heats to the next temperature and the testing cycle begins again. This testing continues until all preset temperatures and all test locations have measured. The following is a sample data table of a test with 15 locations and 3 target temperatures, 25°C, 75°C and 125°C.

Note: During the test a statistical table reports the progress. At the conclusion of the test, all data may be exported to a spread sheet for further analysis. (see data table next page)

PIColRowTarget °CActual °C∆/°CTCR-PPM
11111025.024.975.063refref
21121025.024.975.127refref
31131025.024.975.016refref
41141025.024.975.019refref
51151025.024.975.193refref
61151125.024.975.059refref
71141125.024.975.016refref
81131125.024.974.983refref
91121125.025.074.979refref
101111125.025.075.002refref
111111225.024.975.016refref
121121225.024.975.026refref
131131225.024.975.038refref
141141225.024.975.041refref
151151225.025.075.057refref
12111075.075.275.1440.0016103120876.80
22121075.075.275.2040.0015308115005.55
32131075.075.275.0990.0016501123783.86
42141075.075.275.0990.0015905119314.51
52151075.075.275.2770.0016700125570.82
62151175.075.275.1370.0015507116393.68
72141175.075.275.0970.0016103120801.11
82131175.075.275.0640.0016103120747.97
92121175.075.275.0600.0016135120982.05
102111175.075.275.0810.0015737118031.04
112111275.075.175.0920.0015139113570.04
122121275.075.175.1060.0015936119563.35
132131275.075.175.1160.0015538116592.91
142141275.075.175.1200.0015737118092.41
152151275.075.175.1340.0015369115357.07
131110125.0124.975.2250.0016298121602.06
231210125.0124.975.2810.0015493115695.58
331310125.0124.975.1820.0016700124526.56
431410125.0124.975.1790.0016097120030.40
531510125.0124.975.3610.0016901126324.24
631511125.0124.975.2150.0015694117092.04
731411125.0124.975.1780.0016298121525.92
831311125.0124.975.1450.0016298121472.46
931211125.0124.975.1410.0016298121587.57
1031111125.0124.975.1600.0015895118621.78
1131112125.0124.975.1680.0015261114024.32
1231212125.0124.975.1860.0016064120041.60
1331312125.0124.975.1940.0015663117059.28
1431412125.0124.975.1990.0015863118564.78
1531512125.0124.975.2110.0015462115703.48

(Image #1)

(Image #2)

(Image #3)

Integrated into the Signatone Line of Semiautomatic Probe Stations. (Continued)

(ref. image #3 pg. #9)

How do I choose the best SP4 or HT4 for my application?

Four Point Probe – Selection Guide

Selecting The Best 4 Point Probe Head

For Your Application

Choosing the right probe head is a matter of selecting the best spring pressure, probe tip radius, material and probe tip spacing for your application. The following is a guide for making the best selection; however, experience has shown best results are achieved by using guidelines to select the initial probe head, then experimenting with different spring pressures or materials to match the characteristics of your application.

Spring Pressure: The spring pressure is the pressure used to force each individual probe tip onto the sample surface to make electrical or ohmic contact. Lucas Signatone offers 45 gram, 85 gram and 180 gram spring pressures for standard probe heads (SP4 series) for testing below temperatures of 90 degrees C. Probe heads for use at higher temperatures (the HT4 series) have 180 gram spring pressures. The physical characteristics of the sample determine the correct spring pressure as follows:

Probe Tip Radius: Lucas Signatone probe tips are micro-machined to have the shape of a section of a sphere at the tip. 1.6 mil, 5 mil, and 10 mil tip radii are available. Generally the large tip radius probes are more robust, but it is more difficult to make good electrical contact with these probes. Use the following guide for the selection of tip radius:

Probe Tip Material: Signatone offers 4-point probes with tips of either Tungsten Carbide or Osmium. Tungsten Carbide is a crystalline material that is very hard and can be broken along the crystal boundaries with horizontal motion of the probe. Osmium is an amorphous material and is also hard, but is more forgiving to small horizontal motion. It is believed that Osmium will give longer performance or more touch downs than Tungsten carbide, but it is slightly more expensive.

Probe Spacing: The probes have a constant spacing, S, between each of the 4 tips. Lucas Signatone products use software with correction algorithms allowing for probing near the edge of the sample (to within a proximity of 4 x S) with 1% accuracy. Generally larger probe tip spacings give better results. Please use the following guide.

Also, Osmium has the physical characteristic (work function) such that it can make better contact with some exotic materials. The following is suggested:

$$$ SP4 / HT4 Pricing $$$

For pricing, please configure the part number by using the above information, then send us an e-mail at: Sales@Signatone.com

Regarding the SP4 there is really no sure way to clean the tips. We certainly discourage the use of any chemicals, solvents or touching the tips with a cloth in attempt to wipe them clean. The only method that we have used is compressing the tips 20-50 times on a ceramic surface but there is no specification for the outcome of this process or guarantee that this will clean the tips, as in most cases this does not work. If there is visible debris on the tips you can try using high pressure air to blow away the debris. The SP4 is disposable and priced to be easily replaced and most models are on the shelf for immediate shipment ARO.

The SP4 probe head is designed for use with Signatone and other resistivity probing systems for the measurement of thin films and materials.

The SP4 head has several configurations parameters permitting users to define the probe head best for their application.

0.0625 inches (62)

0.050 inches (50)

0.040 inches (40)

45 grams (045)

85 grams (085)

180 grams (180)

Osmium (0)

Tungsten Carbide (T)

0.0016 inches [1.6mil] (R)

0.005 inches [5 mil] (F)

0.010 inches [10 mil] (B)

Flying lead termination, 15” wire (S)

9 pin D sub with 15” wire (Y)

9 pin D sub with 6” wire (Q)

4 36” wires with Banana Plugs (J) *

4 36” coax wires with BNC (N)*

2 36” coax wires with BNC (C)*

4 36” Triax wire with TRX (HT4) (X)*

2 8” Triax wire with TRX (HT4) (D)*

* for direct connection to various meters

Four Point Probe – Model Maker

Standard Head (Delrin)

Sp4-62085Try

Sample Part Numbers:

Ht4-62180Ory

40 = 40 mil spacing between tips

50 = 50 mil spacing between tips

62 = 62.5 mil spacing between tips

S = Standard, flying lead termination

Y = 15” wire, 9 pin D sub, for Pro4/S-302

Q = 6” wire, 9 pin D sub, for QuadPro 2

J = 36” wire with (4) Banana Plugs

N = 36” Coaxial wire with 4 BNC connectors

C = 36” Coaxial wire with 2 BNC connectors

other connectors available

045 = 45 gram spring pressure

085 = 85 gram spring pressure

180 = 180 gram spring pressure

Sp4- -

T = Tungsten Carbide

O = Osmium

R = 1.6 mil radius tip

F = 5 mil radius tip

B = 10 mil radius tip

X = 36” Triax wire with 4 TRX connectors

D = 8” Triax wire with 2 TRX connectors

High Temperature or High Resistance Head (Macor)

Ht4 -

Hr4

L-4PQM Quick Mounting Block

Use the L-4PQM to mount the SP4 and HT4 probe heads to any late model Lucas / Signatone Corp. resistivity test stand.

Back View

Mounting Holes

Use these dimensions to create your own mounting device.

Photo: L-4PQM quick mounting block, holding SP4-62085TRQ mounted to our QuadProII S-A8 resistivity test station

Four Point Probe – Mounting Options

Vlsi Calibration Standards (Nist Traceable)

The Resistivity Standard, available in three wafer sizes, 76.2mm, 200mm & 300mm (upon request)

IMPORTANT!

Calibration methods using Signatone’s RS test software included with our Pro4, QuadProII and ΩPro test systems are highly repeatable when used with these high-quality materials. When a VLSI, NIST traceable standard is used, the measurements may be set to correlate with the standard. Calibration should be done weekly or after changing probe heads. When performing calibration measurements with a 4-point-probe instrument, you must ensure that the probes and the silicon make solid, repeatable contact. Poor contact is revealed by a high standard deviation of multiple measurements taken from the same area or in some cases, zero-voltage readings.

Note: Typical delivery lead times for these wafers is 6-10 weeks and varies per product.

Resistivity, Rho, is a particularly important semiconductor parameter because it can be related directly to the impurity content of a sample; the four-point probe is the apparatus typically used to determine bulk Resistivity.

The mobility of the carriers depends upon temperature, crystal defect density, and ALL impurities present. Hall Effect Measurements can determine the mobility of the carriers in a given sample to allow for more accurate dopant concentration measurements, but Hall measurements are usually destructive to the sample.

The four-point probe contains four thin collinearly placed tungsten wire probes which are made to contact the sample under test. Current I is made to flow between the outer probes, and voltage V is measured between the two inner probes, ideally without drawing any current. If the sample is of semi-infinite volume and if the inter-probe spacing is s1 = s2 = s3 = s, then it can be shown that the Resistivity of the semi-infinite volume is given by:

Rhoo = (Pi s) V/I (1)

The subscription in the preceding equation indicates the measured value of the Resistivity and is equal to the actual value, Rho, only if the sample is of semi-infinite volume. Practical samples, of course, are of finite size. Hence, in general, Rho ! = Rhoo. Correction factors for six different boundary configurations have been derived by Valdes (1). These show that in general, if l, the distance from any probe to the nearest boundary, is at least 5s, no correction is required. For the cases when the sample thickness is 5s, we can compute the true Resistivity from:

Rho = a 2 Pi s V/I = Rhoo (2)

Where a is the thickness correction factor which is plotted (on page 3). From an examination of the plot we see that for values of t/s >= 5 times the probe spacing, no correction factor is needed. Typical probe spacings are 25-60 mils and the wafers used in most cases are only 10-20 mils, so unfortunately, we cannot ignore the correction factor. Looking again at the plot, however, we see that the curve is a straight line for values of t/s <=0.5. Since it is a log-log plot the equation for the line must be of the form:

a=K (t/s)^m (3)

where K is the value of a at (t/s) = 1, and m is the slope. Inspection of the plot shows that in this case m = 1. K is determined to be 0.72 by extrapolating the linear region up to the value at (t/s) – 1. (The exact value can be shown to be 1/(2 ln 2).) Hence for slices equal to or less than one half the probe spacing a = 0.72 t/s.

When substituted into the basic equation we get:

Rho = a 2 Pi s V/I = 4.53 t V/I, (t/s) <= 0.5 (4)

All samples we will be using in the lab satisfy the one-half relationship so we can use the above formula to determine Rho. We will perform Resistivity measurements on the starting material for each experiment. The value of r obtained will be referred to as the bulk Resistivity, and the units are Ohm-cm.

the end-to-end resistance of a rectangular sample. From the familiar resistance formula:

R = Rho l/wt (6)

we see that if w = l (a square) we get:

R = Rho/t = Rs

Therefore, Rs may be interpreted as the resistance of a square sample, and for this reason the units of Rs are taken to be ohms-per-square or ohm/sq. Dimensionally this is the same as ohms but this notation serves as a convenient reminder of the geometrical significance of sheet resistance.

So far in our discussion of Resistivity measurements we have assumed that the size of our sample is large compared to the probe spacing so that edge effects could be ignored. This is usually the case for the bulk Resistivity measurement. However, our sheet resistance measurements will be made on a “test area” on our wafer and the test area dimensions (nominally 2.9 by 5.8mm) are not that large compared to the probe spacing (25 mils). In order to get accurate measurements we will need to correct for the edge effects. In general then:

Rs = C V/I (7)

where C is the correction factor. Note that for d/s > 40, C = 4.53, the value we had as the multiplier in Equation (5).

References:

Courtesy of:

ECE344: Theory and Fabrication of Integrated Circuits

Electrical and Computer Engineering

Rs = Rho/t = 4.53 V/I for t/s <= 0.5 (5)

which we refer to as sheet resistance. When the thickness t is very small, as would be the case for a diffused layer, this is the preferred measurement quantity. Note that Rs is independent of any geometrical dimension and is therefore a function of the material alone. The significance of the sheet resistance can be more easily seen if we refer to the end-to-end resistance of a rectangular sample. From the familiar resistance formula:

So far in our discussion of Resistivity measurements we have assumed that the size of our sample is large compared to the probe spacing so that edge effects could be ignored. This is usually the case for the bulk Resistivity measurement. However, our sheet resistance measurements will be made on a “test area” on our wafer and the test area dimensions (nominally 2.9 by 5.8mm) are not that large compared to the probe spacing (25 mils). In order to get accurate measurements, we will need to correct for the edge effects. In general, then:

References: Valdes, L.G., Proc. I.R.E., 42,pp. 420-427 (February 1954) Smits, F. M., “Measurements of Sheet Resistivity with the Four Point Probe,” BSTJ, 37, p. 371 (1958).

Same as BT Monograph, 3894, Part 2 Courtesy of: ECE344: Theory and Fabrication of Integrated Circuits Electrical and Computer Engineering University of Illinois – Urbana/Champaign

Warranty

* See Signatone Corporate Terms and Conditions of Sale for further details.

Ask us about our family of Resistivity Test Equipment

Key features included in all Signatone systems include Autorange and dual configuration. Autorange automatically finds the ideal current setting to meet the parameters of the standard for measuring. At the first test site, the software controls the current source to step through a number of settings until the measured voltage is in target range as defined by the standard. This current is then used for all subsequent measurements of the sample. Dual configuration mode applies the standard ## to automatically correct for geometric errors caused by probe spacing and/or edge proximity improving overall accuracy.

Signatone offers Family of Products- The QuadPro 2 for R&D and the Pro4 for basic, manual measurements, ΩPro - Resistance Testing System. Each family has a variety of options and configurations. With over 60 configurations to choose from, Signatone has the product that will meet your application.

Pro 4 Series

For Manual Measurements

QuadPro2 Resistivity Test System

Request a quote

Configure this system with our engineers — factory‑direct from Gilroy, California.

Request a quote for OMEGA-PRO