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Topics Covered
Background
How Does a
Phase Modulated Ellipsometer Work?
Optical Setup
Description
of the Phase Modulation Technology
What are the
Advantages of the Photoelastic Modulator over Other Forms of Polarization
Modulation?
Wide Spectral Range Coverage
Large Acceptance Angle
Microspot Capability
High Accuracy Measurements for All
Values of Psi and Delta
High
Sensitivity
Fast Data Acquisition Speed
Advanced Measurement Capability
Depolarization Effects
Mueller Matrix
UVISEL Phase
Modulated Ellipsometer Performance Qualified
Ellipsometric
Accuracy for Cases Where Δ is Close to 0 : Straight-Through Air
Measurements
Ellipsometer
Accuracy and Repeatability
Standard Reference
Materials
Definitions
Performance
Repeatability
Versus Integration Time
Conclusion
Background
The UVISEL range of
HORIBA Scientific spectroscopic ellipsometers use photoelastic modulators to
perform polarization modulation at a high frequency (50 kHz) without any
mechanical movement.
Owing to this technology these systems have the advantage of
being very fast, having no moving parts and providing high accuracy measurements
over a wide spectral range without the need for extra optical elements. Phase
modulation allows the achievement of higher sensitivity for the characterization
of thin film thickness and optical constants when compared with conventional ellipsometers.
How Does a Phase
Modulated Ellipsometer Work?
Optical Setup
The light source is a Xenon lamp that covers a large spectral
range from 190 to 2100 nm. After passing through the first polarizer which
establishes a linear polarization, the light reflects at oblique angle
(generally 70°) from the sample under study. The output head comprises a
photoelastic modulator and an analysing polarizer that resolves the polarization
state of the reflected beam.
Both polarizers are held fixed during the measurement while
the photoelastic modulator is used to induce a modulated phase shift of the
reflected beam.
The light is analyzed by a grating monochromator that directs
sequentially the light for each individual wavelength onto the detector. Two
types of detectors are employed: photomultipliers for FUV-VIS applications, and
InGaAs photodiodes for NIR applications.
Scanning monochromator systems have the advantage of
controllable bandwidth providing very accurate experimental spectra, high
resolution that is useful for thick layer applications and excellent
repeatability of the measurement. Modern Horiba Scientific monochromators are able to perform a measurement from the FUV to NIR in
a short time.
The configuration of the UVISEL phase
modulated ellipsometer is shown in the figure below.

Figure 1. Optical setup of the
UVISEL
Description of the Phase
Modulation Technology
What
is a Photoelastic Modulator ?
The photoelastic modulator is a fused silica bar exhibiting
isotropic behaviour when no stress is applied. The photoelastic modulator is an
optical element that can be described as a birefringence modulator.
If a mechanical strain is applied to the quartz bar, such as
by a piezoelectric transducer attached to the end of the bar, the modulator
becomes birefringent (n0 ≠ ne). This means that light travels along one axis
faster than the other when passing through it which produces a different phase
velocity for each, and a modulated phase shift is induced to the light beam.

Figure 2. Schematic of the photoelastic
modulator working
What are the Advantages
of the Photoelastic Modulator over Other Forms of Polarization Modulation?
Wide Spectral Range Coverage
A major advantage is that a wide spectral range from the FUV
to the NIR is covered without the need for several hardware configurations, and
without moving any optical elements, the UVISEL provides
a continuous and accurate measurement over the wide spectral range from 190 to
2100 nm.
Large Acceptance Angle
The photoelastic modulator optical element has a large
tolerance of the incident angle allowing more simple alignment of the system. As
the light beam need not follow the principal axis of a rotating element this is
a great advantage when performing measurements in liquid cells, on deposition /
etch reactors in-situ.
Microspot Capability
The UVISEL integrates mirror based optical coupling to the sample
providing a microspot capability up to 50 μm over the whole spectral range.
Measurements with microspot are useful for the characterization of patterned
materials found in semiconductor wafers, display materials, and biosensors. It
provides as well several advantages for the analysis of rough layers and devices
with transparent substrates.
High Accuracy
Measurements for All Values of Psi and Delta
The phase modulated ellipsometer delivers optimum accuracy for all
values of Ψ and Δ for any sample by measuring the parameters:

Figure 3. Photon Energy (eV)
High Sensitivity
The sensitivity of an ellipsometer is
determined by all the different components used. When a PEM is used as the key
component, its 50 kHz modulation frequency provides a wide dynamic range without
noise. When combined with powerful digital signal averaging the UVISEL phase
modulated ellipsometer features an excellent signal to noise ratio from the
FUV to NIR.
Fast Data Acquisition Speed
With a modulation frequency of 50 kHz the phase modulated
ellipsometer can work with response times as short as 1ms/point, and with
good signal : noise ratio. This makes the instrument the ideal system for
real-time process control, and to follow dynamic studies and liquid-surface
measurements in real-time.
Advanced Measurement Capability
Depolarization Effects
Depolarization can occur in case of incoherent reflection,
roughness, scattering, inadequate spectral resolution, inhomogeneity. By
measuring Is, Ic and Ic’ the UVISEL software allows the calculation of the
degree of polarization as defined as:
P = (Is)2
+ (Ic)2+ (Ic’)2
- When P=1, the sample is not depolarizing.
- When P<1, the sample is depolarizing.

Figure 4. Degree of polarization <1
exhibited by a 5 μm organic layer
Mueller Matrix
Up to 11 elements of the Mueller matrix can be measured by
the UVISEL Phase
Modulated Ellipsometer. Mueller matrix measurements are useful when the
sample is both depolarizing and anisotropic.
UVISEL Phase Modulated Ellipsometer Performance Qualified
Ellipsometric Accuracy
for Cases where Δ is Close to 0°: Straight-Through Air measurements
The only material for which the ellipsometric parameters are
absolutely known is air: an ellipsometric measurement in the straight-through
configuration should by definition return Ψ = 45° and Δ = 0°.

Figure 5. Straight-through
ellipsometric measurements of air performed on UVISEL in the range 1.5 – 5 eV at 2000
ms integration time
Average value for Ψ is in the range: 44.98º to 45.02º.
Average value for Δ is in the range : -0.02º to 0.02º. Standard deviation for Ψ
is 0.0035 and Δ 0.0057, this is ±0.01º.
Ellipsometer Accuracy and
Repeatability
Standard Reference Materials
The accuracy and repeatability measurements of the UVISEL
ellipsometer were performed using a standard reference materials (SRM)
supplied by the National Institute of Standards Technology (NIST). Standards
consist of thermal oxide on silicon and the NIST 100 nm was used.
The NIST 100 nm gives the following certified values (for a
one layer model) :
- Thickness: 973.00 Å
- Refractive index: 1.465
Definitions
The repeatability is defined as the standard deviation of 10
static measurements made at the same spot location. The accuracy is the
difference between the average value of the sample properties (thicknesses and
refractive index)over 10 measurements and the NIST nominal value.
Performance
Ten measurements on NIST 100 nm were performed at an angle of
incidence of 70°, using an integration time of 200 ms/point across the spectral
range 190-2100 nm. A single layer model of SiO2 on c-Si was used. The optical
constants of the SiO2 were determined using the classical Lorentz oscillator
dispersion formula.
Results provide an excellent repeatability over the whole
spectral range showing:
- an average thickness value of 973.23 ± 0.11 Å,
- an average refractive index value of 1.4627 ± 0.00006.
According to the definition above the UVISEL features an
accuracy of:
- 0.23 Å for the thickness,
- 0.002 for the refractive index.

Figure 6. Measured Thickness
example

Figure 7. Measured Refractive Index
example
Repeatability Versus
Integration Time
For usual applications an integration time of 100ms or 200ms
per point is generally used.
Experimental conditions:
- Number of measurements: 10 at 2.75 eV (450 nm)
- Sample: thermal oxide (~840Å) on Si
- Integration time: ranges between 1000 and 1 ms
Table 1. Experimental Data
|
|
|
|
|
|
|
|
Ψ (%) |
0.02 |
0.03 |
0.05 |
0.05 |
0.07 |
|
Δ (%) |
0.01 |
0.02 |
0.03 |
0.04 |
0.06 |
|
|
|
|
|
|
|
|
Ψ (%) |
0.14 |
0.23 |
0.32 |
0.61 |
0.86 |
|
Δ (%) |
0.10 |
0.16 |
0.20 |
0.25 |
0.41 |
Conclusion
Spectroscopic ellipsometry based on photoelastic modulation
delivers very high accuracy and repeatability. Owing to this technology the UVISEL allows
the unique combination of high performance and experimental versatility to meet
advanced customers needs and application capabilities.

Figure 8. UVISEL: Spectroscopic Phase
Modulated Ellipsometer
Source: Horiba Scientific – Thin Films Division
For more information on this source please visit Horiba
Scientific – Thin Films Division