
Fig.1 Mechanics of the EUV reflectometer.
The available motions for sample and detector are indicated.
| Axis | Range | Accuracy |
| X | 180 mm | 10 μm |
| Y | 310 mm | 10 μm |
| Z | 155 mm | 10 μm |
| Φ | 360˚ | 0.01˚ |
| Tilt | 20˚ | 0.01˚ |
| Θ | 125˚ | 0.01˚ |
| 2Θ | 195˚ | 0.01˚ |
| Det.-X | 120 mm | 10 μm |
| Det.-R | 700 mm | 100 μm |
| Ψ | 180˚ | 0.01˚ |
Table 1 Compilation of sample and detector movements of the EUV reflectometer.
The measurements at PTB are carried out using highly polarized synchrotron radiation whereas EUVL uses EUV pulsed plasma sources emitting unpolarized radiation. For a full understanding and specification of the optics it is therefore essential to know the polarization properties of the optical components3.
| Peak reflectance | Uncertainty contribution u/% |
Peak wavelength | Uncertainty contribution u/pm |
| Stability of normalized intensity | 0.02 | Repeatability of wavelength | 0.06 |
| Inhomogeneity of the detector | 0.04 | Reproducibility of wavelength (reference to Be K-edge) |
1.1 |
| Higher diffraction orders | 0.02 | Kr resonance wavelength | 1.6 |
| Diffuse scattered light | 0.08 | sample temperature (ΔT = 5 K) |
0.6 |
| incidence angle (Θ = 0.02˚ at Θ = 1.5˚) |
0.1 | ||
| Total uncertainty of peak reflectance |
0.10 | Total uncertainty of peak wavelength |
2.0 |
Table 2 Compilation of uncertainty contributions for measured peak reflectance and peak wavelength.
1F. Scholze, J. Tümmler and G. Ulm
High-accuracy radiometry in the EUV range at the PTB soft x-ray beamline
Metrologia 40, S224-S228 (2003)
2J. Tümmler, H. Blume, G. Brandt, J. Eden, B. Meyer, H. Scherr, F. Scholz, F. Scholze, G. Ulm
Characterization of the PTB EUV reflectometry facility for large EUVL optical components
Proc. SPIE 5037, 265-273 (2003)
3F. Scholze, C. Laubis, C. Buchholz, A. Fischer, S. Plöger, F. Scholz, G. Ulm
Polarization dependence of multilayer reflectance in the EUV spectral range
Proc. SPIE 6151, 615137 (2006)