The kSA MOS UltraScan and kSA MOS ThermalScan systems are ex situ, flexible, high-resolution scanning curvature, bow, and tilt-measurement systems.
The kSA MOS UltraScan and kSA MOS ThermalScan systems are flexible, high-resolution scanning curvature, bow, and tilt-measurement systems. Based on proven and patented kSA MOS technology, the kSA MOS UltraScan uses a laser array to map the two-dimensional curvature, wafer bow, and stress of semiconductor wafers, optical mirrors, glass, lenses – practically any polished surface. For room temperature measurements, explore the kSA MOS UltraScan. If you want to know how your wafer changes with temperature, explore the kSA MOS ThermalScan.
Laser Array Technique
The kSA Multi-beam Optical Sensor, or kSA MOS, technology is based on a patented approach which uses a single laser to generate a two-dimensional laser array. This laser spot array is then reflected off the sample surface into a high-resolution CCD detector. Changes in the reflected laser array spot spacing at each point on the sample are used to determine the localized sample curvature in both the X and Y direction. In this way, the system directly measures the curvature and stress in two dimensions simultaneously. This is something that single or dual beam curvature and stress tools simply
Simultaneous Array Detection
Simultaneous detection of the laser array also makes the measurement inherently less sensitive to sample vibration compared with systems that rely on scanning the laser spot on the surface of the sample to measure the local curvature. This leads to kSA MOS’s increased curvature resolution capability. Since all the laser spots move together at the same frequency, movement or tilt is not incorrectly detected as a change in sample curvature. Through the use of sophisticated image processing and data analysis algorithms, the kSA MOS UltraScan can easily detect micron-sized changes in spot position due to curvature changes, which translates to the highest curvature/stress resolution metrology tool available.
The standard kSA MOS UltraScan system provides a 300 mm x,y scanning range with better than 1 um scanning resolution. Optionally, larger scanning stages (larger glass panel mapping platforms) are available. Scans are fully programmable and extremely repeatable for selected area, line scan, or full area map. The system also provides quantitative film stress analysis with full area spatial map by first scanning the bare substrate and then re-scanning the sample post-process. Unmatched curvature, stress, and bow analysis capabilities are at your fingertips for obtaining large sample uniformity profiles and/or localized isolation of sub-millimeter areas of interest with very high spatial resolution
kSA MOS UltraScan is equipped with XY scanning over a 300mm x 300mm area. This provides the advantage of uniform spatial data resolution over the entire sample. At large diameters spatial resolution will
not be lost, which is typically a problem in linear scanning systems with rotation stages. It also provides easy measurement set up for rectangular samples or for mapping limited areas of a sample.
kSA MOS UltraScan is equipped with both flat and curved reference mirrors for quick and easy curvature calibration. The curvature of your sample is measured directly from the laser spot spacing, resulting in high accuracy single point and scanning curvature measurements. Using sophisticated image processing and data analysis algorithms, the kSA MOS UltraScan can easily detect sub-micron changes in spot position due to changes in sample curvature. This makes it the highest curvature and stress resolution metrology tool available.
Absolute reflectance of the sample at the laser wavelength is determined by measuring the integrated intensity of the laser spots on the CCD detector, and is automatically calibrated before each scan by using the integrated flat mirror. This provides useful information about the quality and uniformity of the sample surface, as well as interference effects for film stacks.
When a laser is reflected off a bowed sample, the reflected angle will differ at different points on the sample. The automated laser tracking in the kSA MOS UltraScan optics not only keeps the laser array centered on the detector but also measures the changes in the angle of reflection of the laser array in order to determine the local sample bow height and surface tilt angle.
To generate a thin-film stress map of a sample, the local curvature of the sample must be determined both pre- and post-deposition. The point-by-point thin-film stress is determined based on the change in the point-by-point curvature from the pre- and post-process curvature maps, as well as the substrate thickness, the biaxial modulus of the substrate and the film thickness. The changes in stress of a thin film after processing may also be determined from the curvature maps measured after the subsequent processing steps.
Spectral Reflectance and Film Thickness (optional add-on)
This option equips the kSA MOS UltraScan optics with a light source and a fiber coupled spectrometer. This allows the spectral reflectance of the sample to be measured at each point on the sample. Using kSA’s proprietary software to measure the extrema positions in the spectral reflectance spectra, the kSA MOS UltraScan can determine the point-by point thickness of semitransparent thin films on a substrate. This data can be mapped along with other measurement parameters such as wafer curvature and film stress. Alternatively, the spectral reflectance data can be exported for multi-layer thickness or device modeling in other software programs.
kSA MOS ThermalScan includes all the capabilities of the kSA MOS UltraScan, and adds an integrated heating chamber with process gas introduction capabilities for thermal stress analysis up to 1000 °C. Scans are fully programmable and extremely repeatable for selected area, line scan, or full area map (depending on model selected). The system also provides quantitative film stress analysis with full area spatial map by first scanning the bare substrate and then re-scanning the sample post-process. Unmatched curvature, stress, and bow analysis capabilities are at your fingertips for obtaining large sample uniformity profiles and/or localized isolation of sub-millimeter areas of interest with very high spatial resolution.
ReferencesView All Referencess
Thermomechanical Characterization of Polymer Thin Films. Application for the Conception and the Manufacturing of a 3D Interposer
Lionel Vignoud, Nicolas Assigbe, Christine Morin, Jérome DeChamp, Lucile Roulet
Broadband High-Reflection Dielectric PVD Coating with Low Stress and High Adhesion on PMMA
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Finite-Element-Method Study of the Effect of Thin-Film Residual Stresses on High-Order Aberrations of Deformable Mirrors
Yaoping Zhang, Guoyun Long, Hong Zhou, Junqi Fan, Hao Cui, Lin Cheng
On the Properties of WC/SiC Multilayers
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The Advantages of Coupling Experimental Methods and Analytical Modelling to Fix Deformation Problems in Devices Conception and Manufacturing
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Effect of Residual Gas on Structural, Electrical and Mechanical Properties of Niobium Films Deposited by Magnetron Sputtering Deposition
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Direct, CMOS In‑Line Process Flow Compatible, Sub 100 °C Cu–Cu Thermocompression Bonding Using Stress Engineering
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Structural and Magnetic Properties of Ultra-Thin Fe Films on Metal-Organic Chemical Vapour Deposited GaN(0001)
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Cyclic Mechanical Behavior of Thin Layers of Copper: A Theoretical and Numerical Study
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Thermal Conductivity of Sputtered Amorphous Ge Films
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Passivation of AlGaN/GaN HEMT by Silicon Nitride
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Thermal Stability on Mo/B4C Multilayers
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GaN-Based LEDs Grown on 6-inch Diameter Si (111) Substrates by MOVPE
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