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Page 388 of 977 Results 3871 - 3880 of 9762

Chao-Ching Ho, Chih-Mu Chiu, Yuan-Jen Chang, Jin-Chen Hsu, Chia-Lung Kuo
OPTICAL EMISSION MONITORING FOR DEFOCUSING LASER PERCUSSION DRILLING

This paper presents a novel method for controlling the laser-drilling process for a hole by monitoring induced plasma emission. The variation of light brightness from laser-induced plasma is used as an indicator to control laser percussion drilling. Through on-line plasma emission acquisition and analysis, we obtain the positive association between the increased depth and the optical signal output. A coaxial photodiode is used to estimate the brightness levels of laser-induced plasma. The above constitute an inexpensive and practical on-line feedback system that can be easily implemented in the laser systems. All of the processing work is performed in air under standard atmospheric conditions without gas assist. The acquired signal for drilling could also be used as an input to a focus point process control scheme. Moreover, the technology demonstrates the feasibility to develop an automated laser micromachining system. Experimental results show that drilling efficiency was increased 47% by applying the proposed defocusing laser percussion drilling.

Thanh Tung Vu, Yoshitaka Maeda, Masato Aketagawa
FREQUENCY STABILIZED AND HOMODYNE LASER DIODE

A displacement measurement with an uncertainty of less than sub-nanometer is required in many industrial fields. A laser interferometer has become a powerful tool in nano-metrology, because the wavelength of the light source can be calibrated by meter definition. In this paper, we propose the use of sinusoidal phase (frequency) modulation on a laser diode (LD) to achieve both the frequency stabilization of the LD and a displacement measurement by a homodyne interferometer.

Hu Lin, Zi Xue, Guoliang Yang, Yao Huang, Heyan Wang
DEVELOPMENT OF HIGH ACCURATE GEAR ARTIFACT MEASURING INSTRUMENT BASED ON LASER INTERFEROMETRY

A specialized high accurate gear artifact measuring instrument based on laser interferometry is developed in National Institute of Metrology (NIM, China), to fulfill the increasing demand for high accurate calibration of gear artifacts. This measuring instrument mainly consists of three linear guide rails, a rotary table, a 3D scanning probe and a laser measuring system. In the laser measuring system, laser beam from laser head is splited along two paths, one is arranged tangent to the base circle of gear for the measurement of profile deviation, another is arranged parallel to the gear axis for the measurement of helix deviation, both laser measurement performed with a resolution of 0.3nm. To minimize the influence of Abbe error, two cube-corner reflectors are placed close to the tip of probe. This measuring instrument operated automatically, during the measurement of gear artifact, all the signals from guide rails, rotary table, probe and laser measuring system are obtained synchronously. A software collects all the data for further calculation and evaluation. Development of this instrument makes it possible to guarantee the measurement of profile and helix direct traceable to the standard laser wavelength.

Junichiro Kitta, Agustinus Winarno, Kazuo Tomiyama, Tomizo Kurosawa
AN IMPROVEMENT OF INTERFEROMETER FOR GAUGE BLOCK CALIBRATION SYSTEM BY USING WAVELENGTH STABILIZED 532 NM, 633 NM AND 780 NM LASERS

This paper aims at improving an optical interferometer for gauge block calibration. Gauge block calibration technique by using optical interferometric method is considered as an ultimate calibration method because of it enables absolute calibration, high accuracy and ensures direct traceability to the definition of length. Therefore, national institute of metrology, calibration laboratory organization or manufactures of gauge block often adopt this optical interferometric method.
We describe introducing iodine stabilized 532 nm Nd:YAG laser, rubidium stabilized 780 nm Nd:YLF laser and offset locked iodine stabilized 633 nm He-Ne laser into the interferometer of gauge block calibration system instead of a conventional standard wavelength lamp. These lasers have well coherent length and enough power to observe a well contrast interferometric fringe pattern for long gauge block.
As a result, we obtained the following three improvements. The first, because of the lasers have well coherent length, it allows us direct calibration procedure, and throughput of GB calibration became drastically shortening. The second, by the direct calibration procedure that independent from other comparison GBs, it allows us to determine a coefficient of thermal expansion of the GBs easily and exactly. The third, in this way, we can reduce the uncertainty in measurement of GB calibration approximately a half compare new improved interferometer and previous one.

Eugen Trapet
STANDARDS AND REFERENCE ARTEFACTS FOR OPTICAL INSPECTION SYSTEMS

The use of optical systems for the dimensional inspection in industrial production (e.g. automotive, aeronautic) is steadily increasing. However, a thorough performance verification of such systems must still become more popular; now international standards have been published and the habit of verification may improve. The presentation will introduce to the key elements of prevailing standards. The basic rules for performance verification of Video CMMs and CMMs with fringe projection sensors and laser scanners, stand alone fringe projection and scanner systems will be discussed. In order to facilitate the verification according to prevailing standards, the author has developed a series of reference objects. These will be presented. A thematic excursion to some reference objects developed for the verification of photogrammetric and tomography systems will be made. For each measurement system the inherent problems and the developed solutions for the corresponding test artefacts will be analyzed.

Tatsuya Kume, Kazuhiro Enami, Yasuo Higashi, Kenji Ueno, Masashi Yamanaka
ERROR PROPAGATION FOR STRAIGHTNESS EVALUATION USING 3-POINT METHOD CONSIDERING LONGITUDINAL POSITIONING ERROR

Straightness evaluation using 3-point method has an advantage for evaluating large objects being not affected by straightness references; however, error introduced by each measurement and propagating to the derived straightness should also be taken into account for evaluating large objects.
In this paper, errors propagated to the straightness derived by 3-point method were estimated analytically based on error propagating models and the estimated errors were evaluated by experiments. The results show that each longitudinal positioning error for the straightness detector should be considered for evaluating large object as well as error in each measurement.
The error estimation which considers the positioning error shows existence of optimum sampling interval which minimizes error in the derived straightness. Then the estimated optimum sampling interval is compared with experiment.
Finally, error for the straightness evaluation with the evaluation distance of 1 km was estimated and its optimum sampling interval was also derived.

Yohan Kondo, Youichi Bitou, Osamu Sato, Makoto Abe
CALIBRATION AND UNCERTAINTY EVALUATION OF FLICK STANDARD USING COORDINATE-MEASURING MACHINE

Flick standard is a cylindrical artifact with a flat part for calibrating the magnification of a probe of roundness measuring-instruments. A probe magnification of roundness measuring-instruments is evaluated by measuring a calibrated flick value of a flick standard. The flick value is a distance between a cross-section circle and a cross-section line. In factory field, it is required that the flick value is calibrated within 0.1 µm with respect to several micrometer to several hundred micrometer. The flick value is generally calibrated by an accurate roundness measuring-instrument. It has a linear error of a probe with about 0.1% or more gain error. When the flick value is 100 µm, the measurement uncertainty is 0.1 µm or more. We calibrated a flick standard using an ultra-high accurate coordinate measuring instrument (CMM) with a laser interferometer to ensure the measurement uncertainty within 0.1 µm. The length measurement system by the laser interferometer is according to the abbe principle. In this paper, we describe the calibration method of a flick standard using the CMM. We calibrated the flick standard using a multiple-measurement technique to eliminate the systematic error of the CMM and estimated its uncertainty based on the analysis of variance. Finally, the proposed calibration method is validated through experiments.

Steffen Matthias, Markus Kastner, Eduard Reithmeier
CAMERA AND PROJECTOR CALIBRATION OF AN ENDOSCOPIC FRINGE PROJECTION SYSTEM

In this paper, we present a method of an accurate camera and projector calibration for a newly developed endoscopic micro fringe projection system. The system consists of a laser illuminated digital micro-mirror device (DMD) for the projection of arbitrary structured light patterns, such as Gray code and cos²-phaseshift patterns. These patterns are focused into a 100’000 pixel image fiber and at the endpoint projected onto the specimen via gradient index lenses. A similar fiber assembly guides the perspective-distorted patterns back from the measurement object to a CCD-camera. The design for the areal measurement of filigree inner geometries generates new challenges for the camera and projector calibration, not only because of the reduced measurement area, but also because of the reduced resolution and artifacts of the image fibers. The camera is described by the standard pinhole camera model, while the projector is modeled using a black box. Calibration is performed by positioning a planar calibration rig with a linear stage. The linear stage is employed for partial automation of the calibration while the additional positioning data is combined with the information from the planar calibration rig to create a 3D data set for the calibration algorithm. This results in a considerably more robust identification of both the pinhole and black-box model. The capabilities of both models together with the developed calibration procedure are proven by the results of measurements of an inner gearing.

Yasushi Azuma, Kenji Odaka, Akira Kurokawa, Toshiyuki Fujimoto
X-RAY REFLECTIVITY MEASUEMENTS FOR DEPTH DENSITY DISTRIBUTION IN THERMAL OXIDE THIN FILM ON SILICON (100)

X-ray reflectometry (XRR) is a powerful tool for the structural characterization of thin films. However the standardized protocols of the measurements and their analyses need to be established for the reliable and reproducible characterization. The collaborative work between National Institute of Standards and Technology (NIST, USA) and National Metrology Institute of Japan (NMIJ, Japan) for thickness evaluation by XRR has been carried out in order to support the activities for the standardization of the thickness evaluation. In order to evaluate the accurate thickness of thin film structures by XRR experiments, the appropriate model construction of the structures should be required for the XRR data analysis. However there have been numerous discussions about the structures especially around the film/substrate interface. We tried to clarify a depth density distribution of a thermal oxide thin film on a Si substrate by comparing the XRR results obtained from several films which were oxidized by different processes.

Kazuhiko Kawasaki, Shinichiro Yanaka, Kaoru Miyata, Hajime Inaba, Feng-Lei Hong
FREQUENCY MEASUREMENT OF A 532-NM IODINE-STABILIZED LASER USING AN OPTICAL FREQUENCY COMB LINKED TO UTC (NMIJ)

We developed an optical frequency comb system (the Mitutoyo comb) synchronized to a rubidium (Rb) based frequency standard oscillator which is linked to the Coordinated Universal Time (UTC) operated by the National Metrology Institute of Japan (NMIJ). We measured the frequency of an iodine stabilized laser at 532 nm which is listed as a wavelength standard for length applications. The frequency measurement results taken by the Mitutoyo comb was compared with the results using another frequency comb system developed by NMIJ (the NMIJ comb). When a common laser frequency was measured by the two systems simultaneously, the frequency difference between these measurement results is 0.17 kHz (6.0 × 10-13). To investigate the origin of the difference, we measure a common laser by using the two combs referring a common frequency reference, and the difference between these results is 0.1 Hz (3.6 × 10-16). Therefore, the measurement uncertainty of the Mitutoyo comb is dominated by the uncertainty of the Rb frequency standard.

Page 388 of 977 Results 3871 - 3880 of 9762