semi合集-English.pdf - 第4109页
SEMI F60-0301 © SEMI 2001 5 analyst subjectivity associated with the curve fit procedure. If it is necessary to dev ia te from the curv e fit parameters o utlined above in order to obtain a satisfactory curve fit it shou…

SEMI F60-0301 © SEMI 2001 4
standard. A minimum sputtering etch cleaning of the
SPC sample of ≥ 10 nanometers is recommended in
order to remove surface contamination, the oxide
passive layer and establish equilibrium. Note that the
degree of preferential sputtering and other ion etching
artifacts are a function of the matrix material and the
ion gun conditions.
13.4 Calibration frequency of the application specific
SPC should be designed to establish a record of the
reproducibility and accuracy of the measurement, as
reflected by the nominal composition of the 316L
standard. A minimum frequency of one per week is
recommended, or immediately prior to performing a
measurement in accordance with this test method.
13.5 A sputter rate calibration shall be performed prior
to an ESCA profile measurement conducted in
accordance to this test method. The ion sputter rate
determination shall be made using standard thin films
of 100 nanometers or less of SiO
2
on Si. The method of
determining the thickness of the oxide film shall be
based upon the oxygen concentration profile. The
oxide – substrate interface shall be specified as the
point at which the oxygen concentration decreases to ½
its maximum value in the SiO
2
film, ignoring the first
sputter cycle.
13.6 Multiple samples may be analyzed following a
single sputter rate determination if the ion gun
parameters have not been adjusted and the ion gun
performance is documented as stable over the period in
question.
14 Procedure
14.1 As-Received Surface Analysis— The sample is to
be mounted in accordance with manufacturer's
recommendations and in a manner consistent with ultra-
high vacuum surface analytical procedures. Some of
these practices are detailed in ASTM-E1078. The area
to be analyzed should be mounted parallel to the sample
holder surface so that TOA is well known.
14.1.1 Place the sample in the ESCA introduction
chamber for pump down. Transfer to the analytical
chamber at the manufacturer's recommended base
pressure. Align the sample with respect to the X-ray
beam and analyzer so that optimum count rate from the
desired analytical location is obtained. The use of a
collimated high voltage electron beam to align the
sample should be avoided, as this may pyrolyze surface
carbon and potentially alter surface oxide chemistry.
The surface area to be analyzed should be free of
visible particles and large defect features, if possible.
14.1.2 A beam size as close to 1 mm as possible
should be used to ensure measurement of a
representative surface. If surface curvature is great
(e.g., < 1/4" tubing), a smaller beam may be employed.
Elemental survey data (0–1100 eV) are to be measured
from the sample surface to determine the elements
present and their approximate surface abundance. A
high throughput analyzer setting may be used to obtain
a signal to noise ratio (S/N) sufficient to detect common
surface contaminants such as sulfur and phosphorus at
one atomic percent or better.
14.1.3 Using instrument settings sufficient to provide
a FWHM peak width of 1.0 eV or less on Au (4f
7/2
),
measure chromium, iron, and carbon regions. A typical
region width is 20 eV. Suggested ranges are as follows:
Cr (2p
3/2
) from 570 to 590 eV, Fe (2p
3/2
) from 700 to
720 eV, and C (1s) from 275 to 295 eV. Signal to noise
ratios of greater than 20 are suggested.
14.1.4 A consistent method of data reduction of high-
resolution surface spectra is necessary in order to
provide meaningful comparison of the relative Cr:Fe
ratios.
14.1.5 The spectra shall be charge compensated with
respect to the maximum of the Cr (2p
3/2
) set to 577 eV.
An iterated Shirley method of background subtraction
shall be applied to the Fe (2p
3/2
) and Cr (2p
3/2
) spectral
regions, using a minimum of three iterations.
14.1.6 The curve fit regions shall typically extend
from:
Cr (2p
3/2
) 570–582 eV
Fe (2p
3/2
) 704–717 eV
14.1.7 The curve fit peak parameters should be
initialized as follows:
Cr (2p
3/2
) Peak Position FWHM % gaussian
1 574 1.5 80
2 576.5 2.0 80
3 577.5 2.0 80
Fe (2p
3/2
) Peak Position FWHM % gaussian
1 707 1.0 80
2 708 1.0 80
3 710 1.4 80
4 711.5 1.4 80
5 713 1.4 80
14.1.8 The curve fit routine should apply the following
tolerances for the band limit parameters of all peaks
defined above:
FWHM delta
≤ 0.2 eV
% gaussian delta
≤ 10%
Curve fit position delta
≤ 0.25 eV
14.1.9 An automated form of data reduction is
recommended to enhance reproducibility and minimize

SEMI F60-0301 © SEMI 20015
analyst subjectivity associated with the curve fit
procedure. If it is necessary to deviate from the curve
fit parameters outlined above in order to obtain a
satisfactory curve fit it should be noted in the formal
report. Possible sources for the anomalous behavior
include an excessive concentration of iron oxide or a
sufficiently aged sample surface, such that the oxide
surface chemistry and structure has modified.
14.2 Depth Profile Analysis— The ESCA depth
profile may be performed following acquisition of the
initial as-received surface survey scan and high-
resolution spectra using the same sample x-y position
and take-off angle of 35°.
14.2.1 The depth profile may be acquired in either
continuous mode (simultaneous sputter etching and data
acquisition) or alternating sputter etch/data acquisition
mode. The following acquisition windows are
recommended:
Spectral line Lower limit Range
C 280 eV 15 eV
O 525 eV 15 eV
Cr 570 eV 15 eV
Ni 848 eV 15 eV
Fe 700 eV 25 eV
14.2.2 If only an elemental compositional profile is
acquired, any pass energy may be selected as long as
the remaining acquisition parameters defined by the
number of sweeps, step size and dwell time result in ≤
1.0at% detection of the matrix elements followed in the
depth profile.
14.2.3 The composition profile should extend far
enough into the depth of the sample to reach the base
metal composition of the 316L material, but a minimum
of 100Å from the surface as referenced to the calibrated
sputter rate in SiO
2
.
15 Calculations and Interpret ation of Results
15.1 Most manufacturers supply software for
determination of elemental composition. The elemental
composition should be calculated using sensitivity
factors appropriate to the instrument, each element, and
resolution settings for each measurement.
15.2 The total Cr/Fe ratio is calculated by adding peak
areas from all species of each element, adjusting for
different numbers of scans and sensitivity factors, and
dividing the Cr result by the Fe result. The Cr oxide/
Fe oxide ratio is calculated in a similar manner, except
that only peaks 2 and 3 for Cr and only peaks 3 through
5 for Fe (oxide species) are used. The formulas are as
follows:
Total Cr/Fe = (Σ Cr peak areas)/# Cr scans/Cr sensitivity factor
(Σ Fe peak areas)/# Fe scans/Fe sensitivity factor
Cr Oxide/ = (Σ
Cr oxide peak areas)/# Cr scans/Cr sens. factor
Fe Oxide (Σ Fe oxide peak areas)/# Fe scans/Fe sens. factor
16 Reporting Results
16.1 As-Received Surface Results — A tabular
summary of the elemental composition of all elements
detected in the surface survey spectrum is to be
supplied with the associated elemental survey spectrum.
If sample preparation has been done by other than the
component manufacturer all tables of as-received
surface analysis results shall include a note stating:
“Sample preparation was not performed by the
component manufacturer. Results are not to be
interpreted as indicative of the component
manufacturer’s quality of cleaning and packaging
procedures.”
16.1.1 Tabular summaries of total Cr/Fe ratio and Cr
oxide/ Fe oxide are also to be supplied, with associated
Cr(2p
3/2
), Fe(2p
3/2
), and C(1s) narrow region spectra.
16.1.2 Acquisition parameters, including
manufacturer, model and TOA; X-ray source (Al or
Mg); beam size; and other pertinent settings are to be
supplied. Analyst identity and analysis date are also
required information. Each table and graph must be
clearly labeled with sample identification.
16.2 Depth Profile Results — Compositional depth
profile data plots shall display the atomic concentration
of Fe, Cr, Ni, C, and O at minimum versus the sputter
time or the equivalent depth from the calibrated sputter
rate in SiO
2
.
16.2.1 The method applied to determine the oxide
thickness shall be specified in the report. A commonly
accepted method of quantifying the oxide thickness is
determined as the sputter time/depth at which the
oxygen concentration decreases to ½ the maximum
value. The carbon thickness may be determined
similarly.

SEMI F60-0301 © SEMI 2001 6
APPENDIX 1
DISCUSSION OF EFFECTS OF DEPTH OF ANALYSIS ON DEPTH
PROFILE ANALYSIS BY ELECTRON SPECTROSCOPY FOR
CHEMICAL ANALYSIS OF PASSIVATED STAINLESS STEEL
NOTE: This appendix is being balloted as an official part of SEMI F## by full letter ballot procedure, but the recommendation in
this appendix are optional and are not required to conform to this standard. This appendix is derived from presentations made to
the SEMI Surface Analysis Task Force.
A1-1.1 The purpose of this appendix is to describe the
ESCA (sometimes referred to as X-Ray Photoelectron
Spectroscopy (XPS)) technique and explain the
interpretation of the depth profile analysis with respect
to the structure and composition of the passive oxide
layer on stainless steel. The effect of the depth of
analysis on the measured chromium to iron ratio, the
oxide thickness, and the depth of enrichment is
discussed. The discussion applies to depth profile
analyses performed by Auger electron spectroscopy,
also.
A1-1.2 ESCA — The ESCA technique makes use of an
X-ray beam for a probe. The surface of interest is
illuminated with X-rays, typically Al kα radiation,
which has a well-defined energy of 1486.6 eV. When
an x-ray photon and an electron interact, the electron
adsorbs all of the energy of the photon, 1486.5 eV; it
cannot react with it partially. The electron then has
sufficient energy to leave the atom and move into the
matrix. The electron’s energy in the matrix is 1486.6
eV minus its binding energy to the atom from which it
escaped. Its binding energy is indicative of the element
or compound from which it came and the orbital from
which it was removed. Such an electron is termed a
“photoelectron”.
A1-1.3 In a typical ESCA instrument, a
monochromatic beam of x-rays is focused at a point of
interest on a surface. A cloud of electrons is generated
at the surface by the x-rays. This electron cloud is
made up of secondary electrons, Auger electrons and
photoelectrons. (NOTE: The generation of Auger
electrons is a byproduct of the process. If the
photoelectron was an inner shell electron, when it
leaves the atom it creates an ion in an excited state.
Once the ion is created it can de-excite via the Auger
process. The presence of Auger electrons in an ESCA
survey can be used to determine what elements were
present.) The mechanisms of ESCA photoelectron and
Auger electron generation are illustrated in Figure A1-
1.
Figure A1-1
Schematic representation of the ESCA
photoelectron and Auger electron generation
processes.
A1-1.4 An electron lens is focused at the same point as
the x-ray beam and a portion of the electron cloud
enters the lens. From the lens, the electrons enter an
electron analyzer that measures the number of electrons
as a function of their kinetic energy. The kinetic energy
is subtracted from the incident x-ray photon energy, and
the resulting binding energy is then plotted as the x-axis
with the number of electrons at each energy on the y-
axis. An example is shown in Figure A1-2. The
binding energy can be indicative not only of the
element from which the electron came but also the
chemical bonding state of the element.