VUV-VASE Gen-II - Home - J.A. Woollam Co. in the VUV The VUV-VASE ® variable angle spectroscopic...

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VUV-VASE ® J.A. W oollam Co., Inc. Ellipsometry Solutions SM

Transcript of VUV-VASE Gen-II - Home - J.A. Woollam Co. in the VUV The VUV-VASE ® variable angle spectroscopic...

Page 1: VUV-VASE Gen-II - Home - J.A. Woollam Co. in the VUV The VUV-VASE ® variable angle spectroscopic ellipsometer is the gold standard for optical characterization of lithography thin

VUV-VASE®

J.A. Woollam Co., Inc.Ellipsometry SolutionsSM

Page 2: VUV-VASE Gen-II - Home - J.A. Woollam Co. in the VUV The VUV-VASE ® variable angle spectroscopic ellipsometer is the gold standard for optical characterization of lithography thin

First in the VUV

The VUV-VASE® variable angle spectroscopic ellipsometer is the gold standard foroptical characterization of lithography thin fi lms. It measures wavelengths from vacuum ultraviolet (VUV) to near infrared (NIR). This provides incredible versatilityto characterize numerous materials: semiconductors, dielectrics, polymers, metals,multi-layers and liquids such as immersion fl uids.

Why a VUV-VASE?

Wide Spectral Range The VUV-VASE covers wavelengths from below 140nm to 1700nm.

High AccuracyUtilizing our patented AutoRetarder®, the VUV-VASE guarantees accuracy for any sam-ple measurement.

Convenient Sample LoadingSpecial design allows fast, effi cient sample loading without contaminating system purge.

Protect Your SamplesThe monochromator is placed before the sample to limit exposure of photosensitive materials.

VUV-VASE Gen-II

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Two Generations

The VUV-VASE® was developed in 1999 to meet metrology requirements for 157nm lithography research. The fi rst generation (Gen-I) tool is perfect for new materials research. A second generation (Gen-II) tool was introduced to provide large area mapping of photomasks and wafers.

Gen-IITranslation Options: • 140mm XY • 300mm R-Theta

to meet metrology requirements for 157nm lithography research. The fi rst generation (Gen-I) tool is perfect for new materials research. A second generation (Gen-II) tool was introduced to provide large area mapping of photomasks and wafers.

Gen-IMeasure samples up to 200mm diameter.

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Key Features

Wavelength RangeThe VUV-VASE can measure any wavelengths between 140nm and 1700nm, or photon energies between 0.73eV and 9eV.

Angle RangeThe VUV-VASE systems feature automated angle of incidence with wide angular coverage.GEN-I 10°-90° (wavelengths <300nm) 25°-90° (wavelengths >300nm)

GEN-II 10°-90° (wavelengths <300nm) 20°-90° (wavelengths >300nm)

Nitrogen PurgeThe VUV-VASE is purged continuously with dry nitrogen gas to eliminate the atmospheric absorption of light below 190nm by oxygen and water vapor.

Load LockSamples are conveniently loaded without reducing purge quality throughout the instrument via a load-lock surrounding the sample region.

Automated Sample AlignmentLoad your samples and the stage automatically aligns to ensure proper sample placement (tip-tilt-z).

Gen-II Sample Stage

Gen-I Sample Load Lock

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Characterization

Wide RangeThe VUV-VASE® measures a very wide photon energy range from 0.73eV to 9eV. This allows study of the electronic transitions in all types of semiconducting and dielectric fi lms. The high energy electronic transitions of group-III Nitrides affect the VUV dielectric functions, as shown to the right.

Ultra-thin Films The VUV-VASE offers two advantages for ultra thin fi lm characterization: • Short wavelengths are more sensitive to thin layers. • UV absorption differentiates materials.Data (right) from a high-K gate dielectric thin film are modeled using SiO2 optical constants and a transparent dispersion model. Neither match the data in the VUV. A Tauc-Lorentz oscillator model correctly describes the material optical constants and matches data over the full spectral range.

R/T DataThe VUV-VASE can measure refl ected or transmitted intensity from your samples. Measure R/T at different angles of incidence and your choice of polarizer direction.

Wide RangeThe VUV-VASEwide photon energy range from 0.73eV to 9eV. This allows study of the electronic transitions in all types of semiconducting and dielectric fi lms. The high energy electronic transitions of group-III Nitrides affect the VUV dielectric functions, as shown to the right.

Ultra-thin FilmsThe VUV-VASE offers two advantages for ultra thin fi lm characterization: • Short wavelengths are more sensitive to thin layers. • UV absorption differentiates materials.Data (right) from a high-K gate dielectric thin film are modeled using SiOa transparent dispersion model. Neither match the data in the VUV. A Tauc-Lorentz oscillator model correctly describes the material optical constants and matches data over the full spectral range.

R/T DataThe VUV-VASE can measure refl ected or transmitted intensity from your samples. Measure R/T at different angles of incidence and your choice of polarizer direction.

Photon Energy (eV)0 2 4 6 8 10

ε 1

ε2

-9

-6

-3

0

3

6

9

12

0

3

6

9

11

14

17

20

AlN, e1GaN, e1AlN, e2GaN, e2

Photon Energy (eV)0 2 4 6 8 10

∆in

deg

rees

0

30

60

90

120

150

180Oscillator ModelTransparent ModelSiO2 ModelExp Data, 70°Exp Data, 80°

Polarized transmission and refl ection for coated optic measured with VUV-VASE.

Page 6: VUV-VASE Gen-II - Home - J.A. Woollam Co. in the VUV The VUV-VASE ® variable angle spectroscopic ellipsometer is the gold standard for optical characterization of lithography thin

Advanced Measurements

Anisotropy/Mueller-matrixComplex materials and nanostructures often requireadvanced characterization methods. The VUV-VASE can measure “generalized-SE” data from anisotropic materials and “Mueller-matrix” data from more complex structures.

Dielectric functions for hexagonal silicon carbide are anisotropic. In fi gures to the left, the ordinary and extraordinary properties are both measured. Notice the large differences in the VUV region.

AutoRetarder®

The VUV-VASE accuracy is ensured by our patented AutoRetarder*. The AutoRetarder is a computer controlled Berek waveplate that introduces controlled retardance into the measurement beam. In this manner, the polarization state probing the sample is manipulated to ensure the best results for any sample.*U.S. Patent #5,757,494

Gen-II Sample Loading

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Lithography Applications

PhotoresistMeasure fi lm thickness and refractive index (n and k) at all lithography lines: 157nm, 193nm, 248nm...

PhotoresistMeasure fi lm thickness and refractive index (n and k) at all lithography lines: 157nm, 193nm, 248nm...

Inde

x of

refra

ctio

n, n

1.8

2.0

2.2

2.4

2.6

Wavelength (nm)

200 400 600 800

Extin

ctio

n C

oeffi

cien

t, k

0.0

0.3

0.6

0.9

1.2

SiON - 1SiON - 2SiON - 3SiON - 4SiON - 5SiON - 6

Lithography thin fi lms were an important motivation for the VUV-VASE® development. It has been successfully used to characterize all types of fi lms in this area, including: • Photoresists • Bottom and Top AR Coatings • Photomask Coatings • Hardmasks • Stepper Optical Coatings • Pellicles •CaF2 Optics • And more...

Page 8: VUV-VASE Gen-II - Home - J.A. Woollam Co. in the VUV The VUV-VASE ® variable angle spectroscopic ellipsometer is the gold standard for optical characterization of lithography thin

Coatings on Stepper OpticsOptical elements used in lithography exposure tools can be enhanced using optical coatings. Coating merit depends on refractive index and thickness. Fluorinat-ed materials are candidates at 157nm, as they remain transparent into the VUV. The index for various fl uorides measured with VUV ellipsometry is shown (right). In addition, the VUV-VASE can measure transmitted intensity to ensure the material quality does not introduce light absorption at the exposure wavelength. The VUV is also used to study coating damage from irradiation.

Liquid Prism CellImmersion Lithography offers signifi cant improvements to extend traditional photolithography to smaller dimensions. The index and extinction coeffi cient (n and k) are important for the overall optical design.

The VUV-VASE can be enhanced with a hollow-prism cell and special measurement algorithm to determine the optical properties of a liquid. This is achieved via the minimum deviation method. Results are shown for a series of immersion fl uids.**R.A. Synowicki et al., Semiconductor FabTech. 22 (2005) 55.

Immersion Fluids: Extinction Coefficient

Wavelength (nm)150 160 170 180 190 200

k

0

2.0E-6

4.0E-6

6.0E-6

8.0E-6

1.0E-5IF24IF26IF48IF53

Immersion Fluids: Refractive Index

Wavelength (nm)150 160 170 180 190 200 210 220 230 240 250

n

1.261.271.281.291.301.311.321.331.34

1.28341.3083IF531.29371.3216IF481.29791.3248IF261.27861.3100IF24

n@193nmn@157nm

1.28341.3083IF531.29371.3216IF481.29791.3248IF261.27861.3100IF24

n@193nmn@157nm

157.6 nm

193.4 nm

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Dimensions

Gen-I Photomask Sample Holder

34” (86cm)

55” (138cm)

66” (168cm)

Gen-I

55” (138cm)55” (138cm)

86” (220cm)

34” (86cm)

45” (115cm)

Gen-II

Weight 1050 lbs (480 kg)Floor Space • 8’ (240cm) wide, min.

• 6.75’ (200cm) deep(Includes space for operator in front)

Ceiling Height 8’ (240cm) min.Electrical Power 100-120 VAC/15A,

200-240 VAC/8A

Weight 1600 lbs (725 kg)Floor Space • 9’ (280cm) wide, min.

• 6.75’ (200cm) deep(Includes space for operator in front)

Ceiling Height 8’ (240cm) min.Electrical Power 100-120 VAC/15A,

200-240 VAC/8A