Specific Process Knowledge/Characterization/Optical characterization

From LabAdviser

Ellipsometer

Ellipsometer: positioned in cleanroom 2

This ellipsometer is a VASE (Variable Angle Spectroscopic Ellipsometry) ellipsometer from J.A. Woollam Co., Inc.

Ellipsometry is a very sensitive characterization technique which can be used to determine thin film layer thicknesses and/or optical constants. It sends in polarized light on the surface at different angles and measures the change in polarization state of the reflected light.

It is especially good for thin films in the thickness range of a few nanometers to a few microns. The layer should be transparent to light in the usable wavelength range for the thickness to be determined. Large roughness (>40nm) and features within the field of view can cause the measurement to fail.

Ellipsometry is an indirect measurement so a model has to be fit to the data in order to obtain the film thickness and optical constants. To learn more about ellipsometry you can take a look at the tutorial provided by the J. A. Woollam Co.

A rough overview of the performance of the Ellipsometer

Purpose Film thickness measurements and optical characterization of optically transparent thin films
  • Measurement of (multi layer) film thickness (only one unknown layer)
  • Optical constants
Performance Thin film materials that can be measured

Any film that is transparent to the light in the given wavelength range ex:

  • Silicon Oxide
  • Silicon nitride
  • PolySilicon
  • Photoresists
  • SU8
  • Other polymers
  • Very thin layers of metals (<20 nm)
  • and many more
. Film thickness range
  • ~20Å to 2 µm (depending of the material)
Process parameter range Wavelength range
  • 300-950 nm
Substrates Batch size
  • One sample at a time - all sample larger than about 1x1 cm2sizes up to about 6"
. Substrate material allowed
  • In principle all materials



Filmtek 4000

FilmTek 4000: positioned in cleanroom 2

FilmTek 4000 is a computerized film thickness measurement and material characterization system. This system combines fiber-optic spectrophotometry with advanced material modeling software to provide an affordable and reliable tool for the simultaneous measurement of film thickness, index of refraction, and extinction coefficient

Normal incidence and polarized 70 degree reflection data is collected and used to calculate thickness and index of refraction of the measured film using SCI’s patented Differential Power Spectral Density (DPSD) technique. Absolute reflection data is obtained by comparing sample data to the measured reflection of a known reference sample, typically a silicon wafer with a thermally grown thin oxide (~63 nm) film.

The spectrophotometer scans the sample over a predefined range of wavelengths. The software generates a reflection spectrum based on a previously stored reference scan, and then performs a regression on the unknown parameters to fit the simulated reflection and power spectral density to the observed values. The resulting thin film parameters along with the measured and modeled spectra are then displayed for the user to examine.

A rough overview of the performance of the FilmTek

Purpose Film thickness measurements and optical characterization of optically transparent thin films
  • Measurement of (multi layer) film thickness (only one unknown layer)
  • Optical constants
  • Surface roughness
Performance Thin film materials that can be measured

Any film that is transparent to the light in the given wavelength range ex:

  • Silicon Oxide
  • Silicon nitride
  • PolySilicon
  • Photoresists
  • SU8
  • Other polymers
  • Very thin layers of metals (<20 nm)
  • and many more
. Film thickness range
  • <100 Å to 250 µm (depending of the material)
Process parameter range Wavelength range
  • 400-1000 nm
Substrates Batch size
  • One sample at a time - all sample larger than 5x5 mm2sizes up to 6"
. Substrate material allowed
  • In principle all materials
  • Only pure silicon, silicon oxides, silicon nitrides and quartz may be in direct contact with the surface of the stage. If you have metals, III-V materials or polymers on the back side of the substrate the please mount your sample on a silicon carrier wafer.



Prism Coupler

Prism coupler: positioned in cleanroom 2

The Prism coupler is a Metricon model 2010 Prism Coupler. It is an old system from 1991 but the system with a few modifications is still beening manufactured today. It is still a very easy and relaible method of determining thickness and refractive index. The prism coupler uses an optical waveguide technique to determine the thickness and refractive index of a thin film. To learn more about the theory of measurement please see the homepage of Metricon

It is especially good for making fast accurate measurements of dielectric thin films with n<2.02 and a thickness range of 1 µm to about 15 µm.

An overview of the performance of the Prism Coupler

Purpose Film thickness measurements and optical characterization of optically transparent thin films
  • Measurement of film thickness
  • Optical constants
Performance Thin film materials that can be measured

Film with a refractive index of less than 2.02 and that are transparent to the light in the given wavelength range ex:

  • Silicon Oxide
  • Silicon nitride
  • polymers
style="background:silver; color:black" style="background:LightGrey; color:black"|Film thickness range
  • ~1µm to 15 µm
style="background:silver; color:black" style="background:LightGrey; color:black"|Film thickness accuracy
  • ±(0.5%+50Å)
style="background:silver; color:black" style="background:LightGrey; color:black"|Index accuracy
  • ±0.001
Process parameter range Wavelength range

Can operate at two different wavelength:

  • 633 nm
  • 1550 nm
Substrates Batch size
  • One sample at a time - all sample larger than 5x5 mm2sizes up to 6"
style="background:silver; color:black" style="background:LightGrey; color:black"|Substrate material allowed
  • In principle all materials

Comparison of the three methods

For comparison of the three methods, see here: Film thickness and optical constants of optical transparent films