Two-Wavelength Optical Microscope Optical Axis Adjustment by Five Incident Parallel Laser Beams

Author(s):  
Feng-Ming Yeh ◽  
Der-Chin Chen ◽  
Shih-Chieh Lee ◽  
Wei-Hsin Chen
2006 ◽  
Vol 23 (10) ◽  
pp. 2113 ◽  
Author(s):  
Sarik R. Nersisyan ◽  
Nelson V. Tabiryan ◽  
C. Martin Stickley

2019 ◽  
Vol 43 (5) ◽  
pp. 735-740
Author(s):  
V.V. Kotlyar ◽  
A.A. Kovalev ◽  
E.G. Abramochkin

Here we study asymmetric Kummer beams (aK-beams) with their scalar complex amplitude being proportional to the Kummer function (a degenerate hypergeometric function). These beams are an exact solution of the paraxial propagation equation (Schrödinger-type equation) and obtained from the conventional symmetric hypergeometric beams by a complex shift of the transverse coordinates. On propagation, the aK-beams change their intensity weakly and rotate around the optical axis. These beams are an example of vortex laser beams with a fractional orbital angular momentum (OAM), which depends on four parameters: the vortex topological charge, the shift magnitude, the logarithmic axicon parameter and the degree of the radial factor. Changing these parameters, it is possible to control the beam OAM, either continuously increasing or decreasing it.


2011 ◽  
Vol 2011 ◽  
pp. 1-6 ◽  
Author(s):  
Min Li ◽  
Zhuguo Li ◽  
Yong Zhao ◽  
Hao Li ◽  
Yuhua Wang ◽  
...  

This paper focused on the welding 1.8 mm thick 6061 aluminum alloy plates in T-joint form using dual lasers that introduced by a Nd: YAG laser and a CO2laser with 4043 aluminum filler wire. The effects of welding parameters on the T-joint weld appearance, microstructure and the joint mechanical properties were studied systematically, The influence of welding parameters included the distance between two laser beams, welding speed, laser power and the laser beam offset toward the stringer. The weld appearance, microstructure, hardness of the joint were evaluated by optical microscope and micro-hardness test. A monotonic quasi-static tensile test was conducted by a self-made clamping device to obtain the tensile property of welded joints. At the optimized parameters, the welded T-joint showed good weld appearance without macro defects; the micro hardness of welds ranged from 75 to 85 HV0.3, and the tensile strength was about 254 MPa with the fracture at the heat affected zone on the stringer side.


2021 ◽  
Vol 53 (9) ◽  
Author(s):  
Naser Siahvashi ◽  
Moslem Hamdami ◽  
Atoosa Sadat Arabanian ◽  
Reza Massudi
Keyword(s):  

1999 ◽  
Vol 5 (S2) ◽  
pp. 544-545
Author(s):  
P. Duncumb

The early days of the electron microprobe were characterized by the variety of designs emerging from different laboratories in Europe, the United States and the USSR. Notable amongst these was that of Castaing in 1954, which employed a magnetic lens in combination with an optical microscope for viewing the sample and positioning the electron probe on the desired point for analysis. The X-ray emission was analysed by two high resolution spectrometers having their axes in the same plane as the electron-optical axis, and with their foci accurately set to coincide with the point of impact of the electron probe. This was a design well suited to point analysis by high resolution X-ray spectroscopy and formed the basis of the first Cameca instrument (Fig 1a).By contrast, work by Duncumb in the Cavendish Laboratory in Cambridge started with the object of scanning the electron probe over the sample, in order to image the surface in terms of its characteristic X-ray emission. This required a strong lens to give a high current into a finely focused electron probe (Fig. 1b). The first element maps were demonstrated in 1956, and led to the design of Cambridge Instruments’ Microscan, intended as a metallurgical instrument, in conjunction with D.A. Melford of Tube Investments Research Laboratories.Meanwhile, Long, also in Cambridge, was pioneering applications to mineralogy, and built an instrument for studying conventional slide-mounted rock samples, which could be viewed optically while analysis was in progress (Fig. 1c). This made use of a weaker probe-forming lens, with space for an inclined sample to be viewed in transmitted light. The slim design of the lens allowed it to be partially enclosed in the spectrometer, which received X-rays leaving the sample at a high angle to the surface - a benefit carried through into the Cambridge Geoscan.


2018 ◽  
Vol 153 ◽  
pp. 06007
Author(s):  
Ryoshu Furutani

We proposed the measurement system of the six degree of motion errors which is based on distance measurement by the laser interferometer. The system has six parallel laser beams and six ball lenses as the retroreflectors on the linear stage, which reflect the corresponding laser beams. In the proposed system, the error of axial direction is measured with the ordinary distance measurement method by laser interferometer. The vertical errors to the axial direction and the roll errors around the optical axis are measured by tilted beams using the wedge prism. The pitch and yaw errors in the vertical plane to the optical axis are measured by the difference between distance of two ball lenses. The former system can measure the displacement and the error angle in one-direction. The propose system are expanded and bi-directional displacement and error angle can be measured. In this paper, it is shown how to expand the measurement system. As a result, the maximum displacement errors in x, y and z directions are 242nm, 179nm and 90nm. The maximum rotational errors around x, y, z axes are 1.75 arcsec, 2.35 arcsec and 1.67 arcsec.


Author(s):  
W.A. Carrington ◽  
F.S. Fay ◽  
K.E. Fogarty ◽  
L. Lifshitz

Advances in digital imaging microscopy and in the synthesis of fluorescent dyes allow the determination of 3D distribution of specific proteins, ions, GNA or DNA in single living cells. Effective use of this technology requires a combination of optical and computer hardware and software for image restoration, feature extraction and computer graphics.The digital imaging microscope consists of a conventional epifluorescence microscope with computer controlled focus, excitation and emission wavelength and duration of excitation. Images are recorded with a cooled (-80°C) CCD. 3D images are obtained as a series of optical sections at .25 - .5 μm intervals.A conventional microscope has substantial blurring along its optical axis. Out of focus contributions to a single optical section cause low contrast and flare; details are poorly resolved along the optical axis. We have developed new computer algorithms for reversing these distortions. These image restoration techniques and scanning confocal microscopes yield significantly better images; the results from the two are comparable.


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