Credence Systems Corporation

Schlumberger Technologies, Inc.

Dcg Systems Gmbh

William K Lo

Steven Kasapi

Romain Desplats

Kenneth R Wilsher

Philippe Perdu

Patricia Le Coupanec

Nina Boiadjieva

Nagamani Nataraj

Chiwoei Wayne Lo

Gary Leonard Woods

Radu Ispasoiu

Suresh N Rajan

A system for probing a DUT is disclosed, the system having a pulsed laser source, a CW laser source, beam optics designed to point a reference beam and a probing beam at the same location on the DUT, optical detectors for detecting the reflected reference and probing beams, and a collection electronics. The beam optics is a common-path polarization differential probing (PDP) optics. The common-path PDP optics divides the incident laser beam into two beams of orthogonal polarization&#x2014;one beam simulating a reference beam while the other simulating a probing beam. Both reference and probing beams are pointed to the same location on the DUT. Due to the intrinsic asymmetry of a CMOS transistor, the interaction of the reference and probing beams with the DUT result in different phase modulation in each beam. This difference can be investigated to study the response of the DUT to the stimulus signal.

Apparatus and method for probing integrated circuits using polarization difference probing

An apparatus and method for laser probing of a DUT at very high temporal resolution is disclosed. The system includes a CW laser source, a beam optics designed to point two orthogonally polarized beams at the same location on the DUT, optical detectors for detecting the reflected beams, collection electronics, and an oscilloscope. The beam optics defines a common-path polarization differential probing (PDP) optics. The common-path PDP optics divides the laser beam into two beams of orthogonal polarization. Due to the intrinsic asymmetry of a CMOS transistor, the interaction of the beams with the DUT result in different phase modulation in each beam. This difference can be investigated to study the response of the DUT to the stimulus signal.

Apparatus and method for probing integrated circuits using laser illumination

A system, apparatus, and method for analyzing photon emission data to discriminate between photons emitted by transistors and photons emitted by background sources. The analysis involves spatial and/or temporal correlation of photon emissions. After correlation, the analysis may further involve obtaining a likelihood that the correlated photons were emitted by a transistor. After correlation, the analysis may also further involve assigning a weight to individual photon emissions as a function of the correlation. The weight, in some instances, reflecting a likelihood that the photons were emitted by a transistor. The analysis may further involve automatically identifying transistors in a photon emission image.

Apparatus and method for detecting photon emissions from transistors

A scanned optical system for use in optical probing applications provides a large Field of View (FOV) for objective lenses having high Numerical Aperture (NA), such as Solid Immersion Lenses (SIL's). This enables high resolution imaging of semiconductor devices for such applications as laser probing, TIVA/LIVA, OBIRCH, and photon emission timing analysis. A hybrid scanning optics configuration is disclosed to provide high resolution imaging over a small area along with low resolution imaging over a large area.

Scanning optical system

Optical interferometery is used to probe an integrated circuit device under test (DUT). During each cycle of a repetitive electrical test pattern applied to the DUT a reference pulse is provided at a fixed time relative to the test pattern, and a probe pulse is provided at a time scanned through the test pattern in the manner of equivalent time sampling. The probe and reference light pulses are each split to provide at least a second probe pulse and a second reference pulse. One probe pulse and one reference pulse interact with the DUT at the same physical location, but at displaced times with respect to each other. The second probe pulse and the second reference pulse travel an optical delay path with length controlled to compensate for motions of the DUT. The probe pulses are recombined and detected to provide a probe interference signal. The reference pulses are recombined and detected to provide a reference interference signal. For each cycle, electrical activity in the DUT is detected by preparing a ratio of the probe interference signal and the reference interference signal.

Double-pulsed optical interferometer for waveform probing of integrated circuits

Methods and apparatus for optically probing an electrical device while the device is operating under control of a tester of the kind that applies test vectors and that has a test head in which the device can be mounted. An optical probe system has a light delivery and imaging module that is configured to be docked to a test head and that has imaging optics and a fine scanner. An optical processing subsystem can generate an incoming beam of light to illuminate the device through an optical fiber to a fiber end in the module. The fiber end is mounted in a fixed position on the optical axis of the imaging optics, and the fiber end and imaging optics are mounted in a fixed position to the platform of the fine scanner. Operating the fine scanner moves the fiber end, the imaging optics, the optical axis, and the focal point as a rigid unit.

Beam delivery and imaging for optical probing of a device operating under electrical test

An optical system for a particle beam device such as an electron microscope, e-beam device or FIB device, including a particle beam column having an optical axis along which a beam of particles is projected and an apertured plate positioned in the column having an aperture which is coaxial with the optical axis, the plate being moveable in a direction which is parallel to the optical axis.

Optical system

A probe beam is used to sample the waveform on an IC device under test (DUT) during each cycle of a test pattern applied to the DUT. A reference laser beam is also used to sample the DUT. For each cycle of the test pattern, the reference and probe beams sample the DUT at the same physical location, but at displaced times with respect to each other. Each reference measurement is made at a fixed time relative to the test pattern while the probe measurements are scanned through the test-pattern time portion of interest, in the manner normal to equivalent time sampling, to reconstruct the waveform. For each test cycle, the ratio of these two measurements is taken. The fluctuations of these ratios due to noise is greatly reduced as compared to fluctuations of the probe measurements taken alone. Thus, a smaller number of averages is required to reconstruct the waveform.

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San Jose, CA, United States of America

William K Lo