Magazine spring00 evaluationofaitii

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Defect Reduction F

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Evaluation of the KLA-Tencor AIT II by Brian Metteer, Chris Meier, Ben VanZante; Texas Instruments Jon Button, Steven Short, Ph.D., Mike Rodriguez, Rebecca Howland Pinto, Ph.D., Pete Muraco, Arlisa Labrie-Miller KLA-Tencor Corporation

As integrated circuit feature sizes continue to shrink, and new process technologies such as Cu dual damascene are introduced, defect inspection technology must continue to improve for device manufacturers to manage their yield. Inspection equipment requires increased sensitivity to smaller defects and new defect types, while maintaining cost of ownership (CoO), primarily via throughput improvements.

To increase throughput, sensitivity and defect capture on its AIT laser scattering inspector product line, KLA-Tencor introduced the AIT II inspection system. Primary sensitivity improvements are achieved by increasing the photon density in the vicinity of the defect by employing a higher-powered laser and by focusing the laser beam to a smaller spot size. Increasing the size of the collection optics provides additional improvements in sensitivity and also enhances capture of defects such as microscratches and defects in trenches. Speeding up movement of the stage and increasing the data processing rate improve throughput. Texas Instrument’s KFAB development facility evaluated an AIT II beta system from September 1998 to January 1999 for sensitivity, throughput, and reliability. The primary purpose of the evaluation was to compare the capabilities of the AIT II system to those of the AIT I and the KLA-Tencor 2138 image comparison inspector. Eight process levels were studied, all from Texas Instrument’s next-generation Digital Signal Processing (DSP) technology. Generally, two wafers from 6 to 7 lots were studied for each layer on each tool. On each layer, the AIT I’s fixed 10 µm spot size was compared to the AIT II’s 10 µm, 7 µm and 5 µm spot sizes. Additionally, a 2138 (typically 0.39 µm pixel size) inspection was run on each layer. 24

Spring 2000

Yield Management Solutions

AIT II technology overview

The AIT II operates in similar fashion to the AIT I, by performing a die-to-die comparison of light scattering signals to detect defects. The wafer surface is illuminated using an oblique-incidence laser beam, and the scattered light is collected by two independent photo-multiplier tubes (PMTs). Particles, scratches, circuit patterns, pattern anomalies and surface contamination all scatter the incident laser light. To preferentially detect the defect signal, unwanted pattern scatter may be filtered out optically or mechanically prior to being collected by the PMTs. Fourier filters minimize scatter from periodic structures such as dense array pattern. Other, customizable spatial filters allow exclusion of certain solid angles of collection, for optimization of signal-to-noise under specific conditions and for the capture of specific defect types. Polarization of the oblique incident beam and oblique collected beam can be leveraged to suppress grainy surface noise, often seen with metal layers, and color variation on the surface of the wafer due to varying layer thickness. The oblique-incidence, oblique-collection design also minimizes scatter from rough surfaces. Typically, Yield Enhancement engineers prefer detection of current-layer defects to previous-layer defects. The AIT’s design tends to result in the capture of more current-layer defects than normal-incidence, bright-field inspection. The collection optics direct the scattered light into separate PMTs that independently convert the collected light energy into an equivalent electronic signal. As the wafer is scanned, signal processing algorithms compare


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