Kla Tencor Corporation

Kla Corporation

Walter H Johnson, Iii

John Fielden

Shing Lee

Kurt Lehman

Jianou Shi

Nanchang Zhu

Xianghua Liu

Lansheng Dong

Haijing Peng

Zhuoxian Zhang

Jun Wang

Lu Yu

Shankar Krishnan

David Y Wang

Fan Zhang

Yang Zhou

Jianli Cui

Hai-Yang You

Zhu-bin Shi

Rui Ni

Haiyang You

Chunxia Li

Changfei Yan

Guoheng Zhao

Mehrdad Nikoonahad

Yaolei Zheng

Jiazhou Jin

Alex Zheng

A Cassegrain or quasi-Cassegrain structure objective lens is used in a polar MOKE metrology system. The quasi-Cassegrain reflective objective lens includes a primary concave mirror and a secondary mirror. The primary concave mirror has a wider diameter than the secondary mirror and defines an aperture through which the laser beam is configured to be transmitted toward the secondary mirror. The secondary mirror can be convex, concave, or have a flat surface.

Reflective compact lens for magneto-optic Kerr effect metrology system

Resistivity probes can be used to test integrated circuits. In one example, a resistivity probe has a substrate with multiple vias and multiple metal pins. Each of the metal pins is disposed in one of the vias. The metal pins extend out of the substrate. Interconnects provide an electrical connection to the metal pins. In another example, a resistivity probe has a substrate with a top surface and multiple elements extending from the substrate. Each of the elements curves from the substrate to a tip of the element such that each of the elements is non-parallel to the top surface of the substrate.

Resistivity probes with curved portions

A laser beam is directed through a transmissive axicon telescope or a reflective axicon telescope such as in a magneto-optic Kerr effect metrology system. With the transmissive axicon telescope, a Gaussian beam profile is directed through a first axicon lens and a second axicon lens. The first axicon lens and second axicon lens transfer the Gaussian beam profile of the laser beam to a hollowed laser ring. The laser beam with a hollowed laser ring can be directed through a Schwarzschild reflective objective. With the reflective axicon telescope, the laser beam is directed through two conical mirrors that are fully reflective. One of the conical mirrors defines a central hole that the laser beam passes through.

Magneto-optic Kerr effect metrology systems

Resistivity probe having movable needle bodies

A continuous variable spacing probe pin device, including first and second probe pins. The first and second probe pins are configured to measure a property of a conductive layer. In a first configuration, the first and second probe pins include respective first portions arranged to contact the conductive layer to measure the property. In a second configuration, the first and second probe pins include respective second portions arranged to contact the conductive layer to measure the property. A first area for each respective first portion is different from a second area for each respective second portion.

Variable spacing four-point probe pin device and method

A variable pressure probe pin device, including: a housing with a channel having a first longitudinal axis; a probe at least partially disposed in the channel and including a plurality of probe pins configured to measure a property of a conductive layer; and a fluid pressure system configured to supply pressurized fluid o the channel to control a position of the probe within the channel. The housing or the probe is displaceable such that the plurality of probe pins contact the conductive layer.

Variable pressure four-point coated probe pin device and method

A method for measuring conductance of a sample using an eddy current probe with a sensing coil. The method includes N repetitions of measuring first and second voltage pairs including in-phase and quadrature components of an induced AC voltage in the sensing coil, calibrating the first signal based on the measured second signal at a different separation from the sample and reference material, determining a conductance function relating conductance with location along the selected curve, processing the calibrated first voltage pairs to generate a lift-off curve, determining an intersection voltage pair representing intersection of the lift-off curve with a selected curve, and determining the conductance of the sample from the intersection voltage pair and the conductance function.

In-situ metalization monitoring using eddy current measurements during the process for removing the film

Disclosed is a chemical mechanical polishing (CMP) system for polishing a sample with a polishing agent and monitoring the sample. The CMP system includes a polishing table, a sample carrier arranged to hold the sample over the polishing table, and an eddy probe. The polishing table and sample carrier are arranged to receive a polishing agent between the sample and the polishing table and to polish the sample by moving the polishing table and the sample carrier relative to each other. The eddy probe is arranged to be operable to obtain a measurement of the sample while the sample is being polished. The CMP system further includes an optical measurement device arranged to be operable to obtain a measurement of the sample while the sample is being polished. The CMP system also has a memory and a processor coupled with the memory. The processor and memory are adapted for operating the eddy probe and optical measurement device.

In-situ metalization monitoring using eddy current and optical measurements

Disclosed is a method of obtaining information in-situ regarding a film of a sample using an eddy probe during a process for removing the film. The eddy probe has at least one sensing coil. An AC voltage is applied to the sensing coil(s) of the eddy probe. One or more first signals are measured in the sensing coil(s) of the eddy probe when the sensing coil(s) are positioned proximate the film of the sample. One or more second signals are measured in the sensing coil(s) of the eddy probe when the sensing coil(s) are positioned proximate to a reference material having a fixed composition and/or distance from the sensing coil. The first signals are calibrated based on the second signals so that undesired gain and/or phase changes within the first signals are corrected. A property value of the film is determined based on the calibrated first signals. An apparatus for performing the above described method is also disclosed.

Growing community of inventors

Rocklin, CA, United States of America

Walter H Johnson, Iii