A high-throughput confocal Raman microprobe based on a single grating spectrograph and CCD detector

Author(s):  
Fran Adar

The availability of sharp cut-on holographic notch filters has enabled the design of simplified, compact Raman instruments for many applications where the size, complexity, and/or cost of instrumentation has been a significant limiting factor. With such a filter, a confocal Raman microprobe has been constructed around a 0.5 m focal length monochromator and 1” CCD detector. This system provides all the microprobe capabilities of the larger systems, including full confocal aperturing with spatial resolution determined by diffraction limitations. Since the gratings are kinematically mounted and easily interchangeable, the choice of grating will determine the trade-off on the array between spectral coverage and spectral resolution for any excitation wavelength between 400 and 830 nm.The practical usefulness of the system as a confocal Raman microprobe will be determined by the low frequency cut-off and the acquisition times. The low frequency cut-off will depend on the notch filter; at laser wavelengths shorter than 550nm the cut-off today is about 100-200 cm-1.

1997 ◽  
Vol 3 (S2) ◽  
pp. 823-824
Author(s):  
M.J. Pelletier ◽  
J. Slater ◽  
K.L. Davis ◽  
W.K. Kowalchyk ◽  
I.R. Lewis

In this paper we report the continuing development of a novel fiber-optic coupled confocal Raman microscope which can offer spectral resolutions up to 0.6 cm−1 per pixel, spatial resolutions of 1 micron or less with axial resolutions of 2-3 microns. The system is based around a compact base unit which comprises a compact solid-state laser, a proprietary f/1.8 imaging spectrograph, and a TE-cooled CCD detector operating at −70°C.In Figure 1 a schematic of the fiber coupled microscope is shown. The microscope includes a integrated holographic filter module to prevent silica Raman generated in the excitation fiber from reaching the sample and to reject radiation at the excitation wavelength from being returned to the spectrograph via the collection fiber(s). The architecture has been designed to allow both fluorescence imaging and Raman microspectroscopy to be accomplished without removing the sample. The figure also depicts the positions of linear polarizers which can be used to collect polarized Raman spectra from small particles or thin polymer laminate samples.


Author(s):  
J. Barbillat ◽  
M. Delhaye ◽  
P. Dhamelincourt

Raman mapping, with a spatial resolution close to the diffraction limit, can help to reveal the distribution of chemical species at the surface of an heterogeneous sample.As early as 1975,three methods of sample laser illumination and detector configuration have been proposed to perform Raman mapping at the microscopic level (Fig. 1),:- Point illumination:The basic design of the instrument is a classical Raman microprobe equipped with a PM tube or either a linear photodiode array or a two-dimensional CCD detector. A laser beam is focused on a very small area ,close to the diffraction limit.In order to explore the whole surface of the sample,the specimen is moved sequentially beneath the microscope by means of a motorized XY stage. For each point analyzed, a complete spectrum is obtained from which spectral information of interest is extracted for Raman image reconstruction.- Line illuminationA narrow laser line is focused onto the sample either by a cylindrical lens or by a scanning device and is optically conjugated with the entrance slit of the stigmatic spectrograph.


Author(s):  
G.Y. Fan ◽  
Bruce Mrosko ◽  
Mark H. Ellisman

A lens coupled CCD camera showing single electron sensitivity has been built for TEM applications. The design is illustrated in Fig. 1. The bottom flange of a JEM-4000EX microscope is replaced by a special flange which carries a large rectangular leaded glass window, 22 mm thick. A 20 μm thick layer of red phosphor is coated on the window, and the entire window is sputter-coated with a thin layer of Au/Pt. A two-lens relay system is used to provide efficient coupling between the image on the phosphor scintillator and the CCD imager. An f1.0 lens (Goerz optical) with front focal length 71.6 mm is used as the collector. A mirror prism, of the Amici type, is used to "bend" the optical path by 90° to prevent X-rays which may penetrate the leaded glass from hitting the CCD detector. Images may be relayed directly to the camera (1:1) or demagnified by a factor of up to 3:1 by moving the lens assembly.


2021 ◽  
Vol 4 ◽  
Author(s):  
Stefano Markidis

Physics-Informed Neural Networks (PINN) are neural networks encoding the problem governing equations, such as Partial Differential Equations (PDE), as a part of the neural network. PINNs have emerged as a new essential tool to solve various challenging problems, including computing linear systems arising from PDEs, a task for which several traditional methods exist. In this work, we focus first on evaluating the potential of PINNs as linear solvers in the case of the Poisson equation, an omnipresent equation in scientific computing. We characterize PINN linear solvers in terms of accuracy and performance under different network configurations (depth, activation functions, input data set distribution). We highlight the critical role of transfer learning. Our results show that low-frequency components of the solution converge quickly as an effect of the F-principle. In contrast, an accurate solution of the high frequencies requires an exceedingly long time. To address this limitation, we propose integrating PINNs into traditional linear solvers. We show that this integration leads to the development of new solvers whose performance is on par with other high-performance solvers, such as PETSc conjugate gradient linear solvers, in terms of performance and accuracy. Overall, while the accuracy and computational performance are still a limiting factor for the direct use of PINN linear solvers, hybrid strategies combining old traditional linear solver approaches with new emerging deep-learning techniques are among the most promising methods for developing a new class of linear solvers.


1995 ◽  
Vol 167 ◽  
pp. 349-350
Author(s):  
A. R. Upgren ◽  
C. Abad ◽  
J. Stock

The CIDA visual refractor of 65-cm aperture and focal length 10.5 m, has been used extensively for position determinations on photographic plates. The combination of Kodak D plates and a yellow filter permit an almost perfect adaptation to the focal curve of the telescope. It appeared of interest to test whether the telescope could be used for astrometric purposes with a CCD detector. As is well known, the spectral sensitivity of these detectors extends well into the infrared where the images formed by the telescope optics will be far out of focus. The blue spectral region where this would also be the case can easily be cut off by a yellow filter. There are no filters which would produce a similarly sharp cut-off towards the red region. On the other hand, given the small field covered by a CCD, the displacement of the red out-of-focus image with respect to the center of the visual image might be negligible. Recently obtained accurate positions in the area of the Perseus Double Cluster made this field suitable for the test of this possibility.


2020 ◽  
Author(s):  
B Espen Eckbo ◽  
Michael Kisser

Abstract We test whether high-frequency net-debt issuers (HFIs)—public industrial companies with relatively low issuance costs and high debt-financing benefits—manage leverage toward long-run targets. Our answer is they do not: (1) the leverage–profitability correlation is negative even in quarters with leverage rebalancing; (2) the speed-of-adjustment to target leverage deviations is no higher for HFIs than for low-frequency net-debt issuers; and (3) under-leveraged HFIs do not speed up rebalancing activity in significant investment periods. Thus, even in the subset of firms most likely to follow dynamic trade-off theory, the theory does not appear to hold.


2011 ◽  
Vol 23 (1) ◽  
pp. 186
Author(s):  
A. Langbeen ◽  
J. L. M. R. Leroy ◽  
I. Pintelon ◽  
P. E. J. Bols

Fat metabolism is important in oocyte development (Kim et al. 2001; Sturmey et al. 2009). Our main objective was to develop a straightforward method that allows us to describe fat distribution and quantify fat accumulation in bovine oocytes throughout folliculogenesis. Fat accumulation dynamics can be studied by making microscopically repeated cross-sections or Z-stacks through oocytes of different developmental stages. The most important limiting factor in oocyte 3D visualisation studies is the size of the oocyte (between 110 and 120 μm in diameter), making it impossible to visualise it as a whole. If visualisation of the bottommost hemisphere is desirable, overlying Z-stacks will disperse the excitation and emission light, creating artefacts that will distort the image and trouble the results (indicated by former unpublished results). Therefore, we investigated the use of an alternative visualisation protocol staining the oocytes with Nile Red as an intracellular, triglyceride-specific (when emission is captured at 590 nm), fluorescent dye (Greenspan et al. 1985; Leroy et al. 2005), this combined with 2-photon excitation technology. In total, ovaries from 10 cows were collected at slaughter. Ovaries were pooled per cow. Only cows with apparent follicular activity on both ovaries were selected. Antral follicles with a diameter of <3 mm, between 3 and 6 mm, and >6 mm were aspirated. Apart from oocytes collected from each of these 3 follicle classes, preantral follicles were harvested from ovarian cortex tissue through mechanical isolation and enzymatic digestion by collagenase type IA. In total, 3 oocytes per follicle class were collected for each pair of ovaries. They were fixed in 2% glutaraldehyde and 2% formaldehyde and stained with Nile Red (1 μg mL–1). After mounting, images were acquired with a Zeiss LSM 510 reversed 2-photon microscope (Carl Zeiss GmbH, Jena, Germany) using an excitation wavelength of 807 nm, with an emission spectrum covered between 580 and 591 nm. Our results show that even with biphoton excitation, it remains very difficult to visualise fat droplet distribution in >100-μm oocytes. However, accurate images can be obtained of the upper hemisphere of the oocyte. These images can be used in future research on the dynamics of the distribution and the accumulation of lipid. Preliminary descriptive results clearly show that the relative amount of lipid droplets is lower and their size is smaller in oocytes from preantral follicles compared with antral counterparts. We can preliminary conclude that fat accumulation and the aggregation in fat droplets might take place preceding or even during antral development. We can visualise preantral oocytes as a whole in contrast to antral oocytes where only the upper hemisphere is visible without distortions. Image analysis software is currently applied to allow for a more quantitative interpretation. D. De Rijck.


2019 ◽  
Vol 43 ◽  
Author(s):  
Olga Vladimirovna Mitrofanova ◽  
Irina Vjacheslavovna Mitrofanova ◽  
Tatyana Nikolaevna Kuzmina ◽  
Nina Pavlovna Lesnikova-Sedoshenko ◽  
Sergey Vladimirovich Dolgov

ABSTRACT Apricot is one of the most valuable commercial fruits. In vitro propagation of apricot is very important for rapid multiplication of cultivars with desirable traits and production of cleaning up and virus-free plants. Low frequency of multiplication is the main limiting factor for traditional propagation methods. In this regard, the objective of our investigation was to study the morphogenetic capacity of apricot leaf explants of the promising cultivars ‘Iskorka Tavridy’, ‘Magister’ and ‘Bergeron’ for regeneration system development and solving some breeding questions. The source of explants was in vitro plants regenerated and cultured on QL medium. Leaves were maintained in the dark at 24±1 °C in thermostat for three-four weeks. Morphogenic callus and structures were mainly formed at the central and proximal parts of leaves on MS, QL and WPM media with 1.5 or 2.0 mg L-1 BAP and 1.5 or 2.0 mg L-1 IAA in different combinations, or TDZ (0.6 and 1.3 mg L-1). Callus with adventive buds was transferred to regeneration medium and placed into a growth chamber at 24±1 °C and 16-hour photoperiod with a light intensity of 37.5 μmol m-2 s-1. The best results were obtained when adaxial leaf surface was in contact with the culture medium. Frequency of leaf callus formation on MS medium with 1.5 mg L-1 BAP and 1.5 mg L-1 IAA was higher in the explants of ‘Iskorka Tavridy’ (80.0%) than in - ‘Bergeron’ (50.0%) and ‘Magister’ (36.7%). The best results of callogenesis for ‘Magister’ was obtained on MS medium with 1.3 mg L-1 TDZ (53.3%). Active microshoot regeneration in ‘Iskorka Tavridy’ cultivar was shown on MS medium with BAP and IAA and in ‘Magister’ cultivar - on MS medium with TDZ. Rhizogenesis was obtained on half strength MS medium with 2.0 mg L-1 IBA.


1984 ◽  
Vol 66 (2) ◽  
pp. 19P-19P
Author(s):  
J. Efthimiou ◽  
R. A. E. Holman ◽  
M. A. Solomon ◽  
M. Belman ◽  
S. G. Spiro ◽  
...  

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