Chapter
8.01
(4ptprb)
1.0
Title
Four-Point Probe Resistivity Measurement
2.0
Purpose
The 4-point probe is a simple device used to measure resistivity
of a thin film or diffusion layer on an insulating material.
There is another four-point probe (VEECO FPP-5000) located next to the
3.0
Scope
This document describes the procedure for measuring sheet
resistance of a thin film material and/or doped layers on an insulating
substrate. Some trouble shootings are also included.
4.0 Applicable
Documents
4.1
Revision
History
4.2 VLSI Technology, Edit by
S.M. Sze, pp. 184-186, McGraw-Hill, 1983.
4.3 VEECO FPP-5000 4-point Probe
Operation Manual (Office copy).
4.4 Four point probe manual
posted at EECS143 class website: http://microlab.berkeley.edu/ee143/Four-Point_Probe/
5.0
Definitions & Process
Terminology
Sheet Resistance: The electric resistance of a
square sheet of a film. It is independent of the size of the square, but
depends only on the film resistivity and the thickness of the film.
6.0
Safety
Follow the general safety guidelines in the lab.
7.0
Statistical/Process Data
N/A
8.0
Available Processes, Process Notes
8.1
Available Programs
The four-point probe is manually operated. There is no
recipe or program. See Section 9.2 for operating
procedures.
8.2
Process Notes
8.2.1 The
four-point probe only works on blank wafers with continuous film on top. It
does not work on patterned wafers.
8.2.2 If your
sample size is small, or you are measurement point is close to the edge of your
sample, you need to check the section 4.1 reference for the geometric
correction factor.
8.2.3 The
measurement is destructive. The four-point probe will make four dents on the
film measured.
8.2.4
There should be a layer of insulator, e.g. silicon oxide,
between a silicon substrate and the film to be measured. Otherwise, the sheet
resistance measured will be erroneous.
9.0
Equipment Operation
The
four-point probe station consists of a SIGNATONE probe station (four probe
tips), an ampere meter (FLUKE8010A), a DC current source (HP6181C), and a
voltmeter (KEITHLY195). This set up
can measure resistivity of thin film material, as well as diffusion layers. The
four probes are arranged in a linear fashion, where the two outer probes are
connected to a current supply, and the inner probes to a voltage meter. As
current flows between the outer probes, the voltage drop across the inner
probes is measured. The relationship of the current and voltage values is
dependent on the resistivity of the material under test, and the geometrical
characteristics of the probe as per follows:
RS = ρ*V/I where:
sheet resistance RS is in Ω per square;
V (in mV) is the voltage drop across the inner two
probes;
I (in mA) is the current flow between the outer two
probes;
Ρ
(rho) is the geometric factor for thin film measured on four-point probe, which
equals to 4.5324, if the size of the sample is 40 times larger than the spacing
between the probes (RS
= 4.5324 V/I).
The
Four-Point Probe is set up in such a way that the DC current source delivers
0.453 mA through its outer two probes. This simplifies the RS measurement by letting
members arrive at sheet resistance values equating to 10 times the voltage
value (mV) measured between the two inner probe tips (voltmeter).
9.2.1 Check that
the ampere meter, DC current source and the voltmeter are on. (It is not
required to enable it on the WAND).
9.2.2 Make sure
your sample is clean and dry. Use the nitrogen gun to blow away any particles
that may be on your sample.
9.2.3 Raise the
probe head by swinging the arm all the way to the right (counter-clockwise).
9.2.4 Carefully
slide the sample holder disk out from under the probe head.
9.2.5 Place your
sample on the disk. Slide the disk back, and align the sample so that the spot
to be measured is under the probe head.
9.2.6 Lower the
probe head onto the sample by slowly swinging the arm over to the left
(clockwise).
9.2.7 Make sure
the ampere meter reads 0.453 mA. If not, adjust the DC current source to arrive
at that value.
9.2.8 Wait a few
seconds for the voltage to stabilize. The sheet resistance is the voltage
measured (in mV) multiplied by 10.
9.2.9
When you have finished, raise the probe head and slide the
disk and your sample out. Remove your sample and replace the disk under the
probe.
10.0 Troubleshooting
Guidelines
10.1 There is
no current.
Cause: The
probe did not contact the sample.
Solution: Make
sure the probe arm is all the way to the left. If there is still no current,
the probe arm needs adjusting. Report on the WAND.
If your sample is thinner than a regular silicon wafer, the
same problem may occur. In this case, you can put a few pieces of paper under
the sample disk, not the sample, to solve the problem.
10.2 The
current could not reach 0.453 mA.
Cause: The
film resistance is too high.
Solution: Adjust
the DC current supply to get 0.453 mA. If the DC current supply is at the
highest setting, record the current and voltage measured. Then use the equation
listed in Section 9.1 to calculate the sheet resistance.
10.3 The
voltage is too low and not precise.
Cause: The
film is too conductive.
Solution: Adjust
the DC current supply to higher setting. The voltage measured should increase
too. When the voltage reaches the satisfactory range, record the current and
voltage measured. Then use the equation listed in Section 9.1
to calculate the sheet resistance.
11.0
Figures & Schematics
N/A
VEECO
FPP-5000 4-POINT PROBE
12.1 System
Description
The VEECO FPP-5000 4-point probe simplifies the measurement
of resistive properties of semiconductor wafers and resistive films. The microprocessor
based electronics permits direct computation of V/I, sheet or slice
resistivity, and metallization thickness and P-N type testing. Unlike most four
point probes and probing stations, which move the probe head into the wafer,
the FPP-5000 is designed so that the wafer is moved into the probe head. This
insures constant probe force independent of operator force and wafer thickness.
12.2 Keyboard
Description
12.2.1 V/I
Displays measured V/I multiplied by programmed GEOM Constant.
12.2.2 SHEET
Displays sheet resistance based on measured V/I.
12.2.3 SLICE
Calculates the bulk resistivity of a slice of layer whose thickness is entered
in the PRGM mode.
12.2.4 THICK
Calculates the thickness of a layer of slices whose bulk resistivity is entered
in the PRGM mode.
12.2.5 TYPE When selected,
a type test is performed.
12.2.6 PEN When
selected, a penetrate voltage is applied to the sample.
12.2.7 PRGM Put the
keyboard into the PRGM mode for entering bulk resistivity or film thickness.
Press STORE afterwards to store the input into system memory.
12.2.8 SELF-TEST
Performs a system self test.
12.2.9 RETEST
Performs a retest when the previous test failed.
12.2.10 CONST
Displays the selected input stored in the memory.
12.2.11 Numerical
Keys To enter the input required for calculation.
12.3 Measurement
Procedures
12.3.1 Enable
4ptprb on the WAND (required for this automatic tool).
12.3.2 Press
CLEAR to clear any error message on the display.
12.3.3 Select
desired function. Select SHEET for sheet resistance measurement.
12.3.4 Place the
wafer face down in the wafer holder (4/6).
12.3.5 Place the backing
plate with the spiral side facing towards your wafer.
12.3.6 Open the
cover, and put the wafer holder, with the wafer facing down, onto the platen.
12.3.7 Close the
cover and hold it down to start a test. When the measurement is done, the
result will be displayed. E02 error will appear on the display if the cover is
released before the measurement is completed.