Ellipsometry vs Reflectometry: What They Measure, Thin-Film Sensitivity and Multilayers
Both methods shine light on a wafer and measure the reflection to find the thickness of thin films without contact or damage. Spectroscopic ellipsometry sends polarized light in at an oblique angle and measures, at each wavelength, how the reflection changes the polarization (Psi and Delta). Spectral reflectometry usually illuminates at normal incidence and measures the spectrum of reflected intensity (reflectance). Both fit an optical model to get the thickness, but ellipsometry also uses phase information, so it is stronger for films a few nanometers thick, multilayer stacks and optical constants, while reflectometry is simpler and faster and suits thickness control of thicker films.
| Aspect | Spectroscopic ellipsometry | Spectral reflectometry |
|---|---|---|
| What is measured | Amplitude ratio (tan Psi) and phase difference (Delta) between p- and s-polarized reflection | Spectrum of reflected intensity (reflectance) |
| Illumination | Polarized light at an oblique angle (typically about 60 to 75 degrees) | Usually normal incidence; no polarization control needed |
| Results | Thickness and optical constants (refractive index n and extinction coefficient k) can be found together | Mainly thickness; known optical constants are usually assumed |
| Model dependence | Strong: values come from fitting a model of the film stack and its dispersion | Also model-based; for a thick single layer the fringe spacing gives the thickness fairly directly, but results depend on the assumed optical constants |
| Sensitivity to very thin films (a few nm or less) | High: Delta resolves differences below 0.1 nm, so native oxides and gate dielectrics can be measured | Low: no interference fringes appear and the change in reflectance is small, so precision drops |
| Best thickness range (rough guide) | From below 1 nm to a few micrometers | From tens of nanometers to tens of micrometers |
| Multilayers | Strong: two quantities per wavelength help separate the thickness and optical constants of each layer | Separating individual layers gets hard as layers are added |
| Tool and speed | More complex optics with polarizers; the oblique beam makes an elongated spot and each point takes a little longer | Simple and fast, with an easily small spot; easy to build into other tools |
| Typical uses | Gate and high-k dielectrics, thin oxides and nitrides, multilayer thickness and optical constants, optical critical-dimension metrology (scatterometry) | Resist and thick oxide or interlayer dielectric thickness, and thickness monitoring built into CMP and other tools |
Figures are typical orders of magnitude and vary by process generation and product.