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Journal articles on the topic "C.C.D. = charge coupled device"
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Parigger, C. G., and C. M. Helstern. "Cyanide Molecular Laser-Induced Plasma Spectroscopy." Journal of Physics: Conference Series 2439, no. 1 (January 1, 2023): 012003. http://dx.doi.org/10.1088/1742-6596/2439/1/012003.
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Abstract This work communicates recent measurements of CN in laser-induced plasma. The main goals and objectives comprise (a) exploring CN measurement using optical emission spectroscopy in optical breakdown plasma; (b) determining the effects of laser-induced shockwave for time delays of the order of 1 μs; (c) evaluating the spatial distribution of CN signals; (d) inferring CN temperature distribution; and (e) associating recorded shadowgraphs with laser-spectroscopy results. Q-switched, 150 mJ, 6 ns pulsed Nd:YAG laser radiation at the fundamental wavelength of 1064 nm is used to generate micro-plasma in a gas mixture with ultra-high purity nitrogen and research grade carbon dioxide. The CO2 to N2 molar ratio is 1 to 1 for the gaseous mixture near atmospheric pressure flowing through the chamber. Optical emissions are dispersed by a 0.64-m Czerny-Turner spectrometer and an intensified charge-coupled device records the data along the wavelength and slit dimensions. The analysis utilizes Abel integral inversion techniques for determination of spatiotemporal profiles.
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Iwanczyk, Jan S., Bradley E. Part, Carolyn R. Tull, and Shaul Barkan. "High-Throughput, Large Area Silicon X-Ray Detectors for High-Resolution Spectroscopy Applications." Microscopy and Microanalysis 7, S2 (August 2001): 1052–53. http://dx.doi.org/10.1017/s1431927600031330.
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The concept utilized in charge coupled devices (CCD’s) for detection and imaging of light signals involving lateral movement of charges and extremely low capacitance of the detector and readout electronics has spawned a variety of new ideas in the design of nuclear detectors. Initially, silicon drift detectors (SDD’s) were developed for high energy physics applications. More recently, a vigorous effort to develop new structures for x-ray spectroscopy and light detection has started. Drift structures have been designed in a variety of topologies and materials (such as Si, CdZnTe, and HgI2) to satisfy the requirements of many different applications. The most interesting features that can be achieved with drift structures include: a) Large active area devices with low capacitance and low electronic noise, b) Very high signal throughput, c) Operation at or near room temperature, d) High sensitivity over the large entrance electrode to low energy xrays and short wavelength light, f) Single carrier charge collection allowing for elimination of hole contribution to the spectral broadening in compound semiconductor detectors such as HgI2, CdTe, and CdZnTe, f) 2D resolution of few tens of micrometer in both directions over few cm2 active areas, and g) Possibility of using more sophisticated schemes of charge collection by switching between integration and drift mode.
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CHEN, JINRU, and MANSEL W. GRIFFITHS. "Salmonella Detection in Eggs Using LuX+ Bacteriophages." Journal of Food Protection 59, no. 9 (September 1, 1996): 908–14. http://dx.doi.org/10.4315/0362-028x-59.9.908.
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Recombinant bacteriophages specific for Salmonella spp. and containing bacterial luciferase genes were constructed. The phage caused the host cells to luminesce when mixed with Salmonella spp. and the luminescence could be detected using a photon-counting charge-coupled device (CCD) camera, a luminometer, or X-ray film. The initial assay system was capable of detecting Salmonella isolates from group B and group D. Certain isolates from group C could also be detected. With 6 h of preincubation, as few as 10 CFU of Salmonella cells per ml in the original sample could be detected. The minimum time required for the detection of 108 CFU/ml was 1 to 3 h with no preincubation, depending on bacteriophage adsorption temperatures. The phage-based assay could be carried out on Petrifilm E. coli Count Plates and the light emission detected within 24 h. The system allowed Salmonella cells to be detected in whole eggs by direct addition of recombinant bacteriophages into the eggs followed by visualization of the luminescent Salmonella cells inside the eggs.
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Ma, Gang, Jian Liu, Li Fu, and Elsa C. Y. Yan. "Probing Water and Biomolecules at the Air—Water Interface with a Broad Bandwidth Vibrational Sum Frequency Generation Spectrometer from 3800 to 900 cm−1." Applied Spectroscopy 63, no. 5 (May 2009): 528–37. http://dx.doi.org/10.1366/000370209788347057.
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We have built a broad bandwidth vibrational sum frequency generation (VSFG) spectrometer that can provide high-quality spectra over the range of 3800 to 900 cm−1. The spectrometer contains a commercial Ti:sapphire based 6 W regenerative amplifier as the master light source, a home-built pulse shaper to produce a narrow bandwidth 800 nm beam, a commercial optical parametric amplifier to generate a broad bandwidth femtosecond infrared (IR) pulse, and a detection system with a monochromator and a charge-coupled device (CCD). We applied this spectrometer to obtain VSFG spectra of a lipid monolayer at the air–water interface in the O–H stretching region (3800–3000 cm−1), the C–H stretching region (3100–2700 cm−1), the C–D stretching region (2300–2000 cm−1), the C=O stretching region (1800–1700 cm−1), and the PO2− symmetric stretching region (1200–1000 cm−1). We also obtained the VSFG spectrum of neat water in the O–H stretching region (3800–3000 cm−1) and the VSFG spectrum of a protein, α-synuclein, in the amide I region (1700–1600 cm−1) at the air–water interface. The spectrometer can provide a VSFG spectrum in the O–H stretching region (3800–3000 cm−1) without scanning the IR frequency. This feature will be useful in probing water dynamics at interfaces because the free OH and H-bonded OH can be investigated simultaneously. We have also provided instrumental details and discussed further improvements that should be beneficial to other researchers interested in setting up VSFG instrumentation.
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Sanjay, Sooraj, Fahimul Islam Sakib, Mainul Hossain, and Navakanta Bhat. "(Invited, Digital Presentation) Super-Nernstian Isfet Combining Two-Dimensional WSe2/MoS2 Heterostructure with Negative Capacitance." ECS Meeting Abstracts MA2022-02, no. 15 (October 9, 2022): 823. http://dx.doi.org/10.1149/ma2022-0215823mtgabs.
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Ion-sensitive field-effect transistors (ISFETs) are quite popular as compact, low-cost biosensors with fast response time and label-free detection1. They can be used as pH sensors or functionalized for complex biomolecule detection. The voltage sensitivity (Sv) in classical ISFETs is fundamentally limited to 59 mV/pH (Nernst limit). Surpassing the Nernst limit requires complex device architectures or novel transport phenomena. Sensitivity beyond the Nernst limit can be achieved using specific device architectures such as dual gate ISFETs2, negative capacitance ISFETs (NC-ISFET)3, tunnel ISFETs4, etc. Compatible architectures can be combined for further enhancements in sensitivity. First, we experimentally demonstrate a super-Nernstian hetero-ISFET that uses 2-D WSe2/MoS2 heterostructure in a double-gated configuration5. The schematic of the device structure is shown in Fig. 1(a) along with its dimensions. The fluid gate to the pH solution is biased at VFG = 0 V and the voltage sensitivity (SV) is extracted by applying bias to the back-gate (VBG). Fig. 1(b) shows the variation of drain current for change in VBG at different pH. The voltage sensitivity is also included in the same graph. The device uses charge screening due to the interface traps and inversion charges at the hetero-interface to modulate the back-gate transconductance (gmb), thereby allowing super sensitivity. Further enhancement in sensitivity is explored using technology computer-aided (TCAD) device simulator tool (Silvaco ATLAS) by integrating with different device architectures. First we model the baseline hetero-ISFET. The 2-D materials were modeled using their material parameters and 3-D equivalents of their density of states. Amorphous hafnium oxide (HfO2) was used as the dielectric. The mobile ions in the electrolyte were modeled as charge carriers in an intrinsic semiconductor, with its effective density of states varying as a function of pH. The simulation model was calibrated with the experimental device (at pH = 7), as shown in Fig. 2(a). The transfer characteristics of the back-gate at different pH and fixed VFG (= 0 V) for the simulated device is shown in Fig. 2(b). We note that the sensitivity from simulations is lower than the experimental device. This is likely due to non-ideal and 2-D material specific factors which are not accounted in simulations. Nevertheless, the simulated device also shows super-Nernstian sensitivity (Fig. 2(b), right axis), validating the model. Hence, the calibrated TCAD model is used as the baseline for further studies. Next, an NC-FE layer (aluminum-doped HfO2) was added to the top fluid-gate stack6. We have used a ferroelectric-metal-insulator-semiconductor (FMIS) stack for the proposed NC-hetero-ISFET. Fig. 3(a) shows the new top-gate stack with the FMI layer, which replaces the top-gate stack in the earlier schematic. The fluid-gate charge (QFG), and drain current (ID) as a function of VFG (VBG = 0 V), were obtained from the TCAD simulations. The 1-D Landau–Khalatnikov (L-K) equations were used to model the voltage across the FE layer (VFE = 2αQFG+4βQ3 FG = V' FG - Vint; where V' FG is the newly computed fluid-gate bias and Vint is the internal node voltage)7. The calculated Vint (for fixed V' FG) is coupled back into the ATLAS simulator to extract voltage sensitivity (SV) by sweeping VBG at different pH values. The fluid-gate transfer curve of the proposed NC-hetero-ISFET, in Fig. 3(b), clearly shows a steeper sub-threshold slope and higher ON current than the baseline device. The corresponding FE layer parameters are shown in Table 1. These improved fluid-gate characteristics contribute to an increased voltage-sensitivity (SV) when VBG is applied. The transfer characteristic (ID v/s VBG, at fixed V' FG) of the NC-hetero-ISFET at different pH values is shown in Fig. 3(c), along with the voltage sensitivity. Further, in Fig. 3(d), we compare the peak SV obtained at different V' FG. There is an improvement in voltage sensitivity (as much as ~ 100 mV/pH) over the baseline device when NC is introduced. The results pave the way for highly sensitive super-Nernstian ISFETs by combining 2-D heterostructure with NC effect. References: P. Bergveld, Sensors Actuators, B Chem., 88, 1–20 (2003). M. Spijkman et al., Appl. Phys. Lett., 98, 2011–2014 (2011). F. Bellando et al., Appl. Phys. Lett., 116, 173503 (2020) P. Dwivedi, R. Singh, and Y. S. Chauhan, IEEE Sens. J., 21, 3233–3240 (2021). S. Sanjay, M. Hossain, A. Rao, and N. Bhat, npj 2D Mater. Appl. 2021 51, 5, 1–8 (2021) S. Salahuddin and S. Datta, Nano Lett, 8, 405–410 (2008) F. I. Sakib, M. A. Hasan, and M. Hossain, IEEE Trans. Electron Devices, 69, 311–317 (2022). Figure 1
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Butt, Muhammad Ali. "Plasmonic sensor realized on metal-insulator-metal waveguide configuration for refractive index detection." Photonics Letters of Poland 14, no. 1 (March 31, 2022): 1. http://dx.doi.org/10.4302/plp.v14i1.1122.
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In this work, a plasmonic sensor established on metal-insulator-metal waveguide configuration is proposed and numerically investigated for biosensing applications. The spectral and sensing characteristics of the device are examined via the two-dimensional finite element method. Sensitivity (Sbulk) and figure of merit (FOM) are two important parameters that are considered to determine the device performance. The Sbulk of the device is considered as a ratio between the change in resonance wavelength and change in the ambient refractive index. Whereas FOM is the ratio of Sbulk to full width at half maximum. The Sbulk and FOM offered by the device are ~825.7 nm/RIU and ~13.14, respectively. This work can provide a guideline for the realization of highly sensitive plasmonic sensing devices. Full Text: PDF ReferencesN.L. Kazanskiy, S.N. Khonina, M.A. Butt, "Plasmonic sensors based on Metal-insulator-metal waveguides for refractive index sensing applications: A brief review", Physica E: Low-dimensional systems and Nanostructures 117, 113798 (2020). CrossRef D. Xiang, W. Li, "MIM plasmonic waveguide splitter with tooth-shaped structures", Journal of Modern Optics 61, 222-226 (2014). CrossRef M.A. Butt, S.N. Khonina, N.L. Kazanskiy, "Ultra-short lossless plasmonic power splitter design based on metal–insulator–metal waveguide", Laser Physics 30, 016201 (2020). CrossRef J. Park, S. Lee, B. Lee, "Polarization Singularities in the Metal-Insulator-Metal Surface Plasmon Polariton Waveguide", IEEE Journal of Quantum Electronics 46, 1577-1581 (2010). CrossRef M. T. Hill, M. Marell, E. S. P. Leong, B. Smalbrugge, Y. Zhu, M. Sun, P. J. V. Veldhoven, E. J. Geluk, F. Karouta, Y-S. Oei, R. Notzel, C-Z. Ning, M. K. Smit, "Lasing in metal-insulator-metal sub-wavelength plasmonic waveguides", Optics Express 17, 11107-11112 (2009). CrossRef A. Udupi, S. K. Madhava, "Plasmonic Coupler and Multiplexer/Demultiplexer Based on Nano-Groove-Arrays", Plasmonics 16, 1685-1692 (2021). CrossRef Y-F. C. Chau, C-T. C. Chao, H-P. Chiang, "Ultra-broad bandgap metal-insulator-metal waveguide filter with symmetrical stubs and defects", Results in Physics 17, 103116 (2020). CrossRef H. Bahri, S. Mouetsi, A. Hocini, H.B. Salah, "A high sensitive sensor using MIM waveguide coupled with a rectangular cavity with Fano resonance", Optical and Quantum Electronics 53, 332 (2021). CrossRef S.N. Khonina, N.L. Kazanskiy, M.A. Butt, A. Kazmierczak, R. Piramidowicz, "Plasmonic sensor based on metal-insulator-metal waveguide square ring cavity filled with functional material for the detection of CO2 gas", Optics Express 29, 16584 (2021). CrossRef M.A. Butt, S.N. Khonina, N.L. Kazanskiy, "Plasmonics: A Necessity in the Field of Sensing-A Review (Invited)", Fiber and Integrated Optics 40, 14-47 (2021). CrossRef M.A. Butt, A. Kazmierczak, N.L. Kazanskiy, S.N. Khonina, "Metal-Insulator-Metal Waveguide-Based Racetrack Integrated Circular Cavity for Refractive Index Sensing Application", Electronics 10, 1419 (2021). CrossRef N.L. Kazanskiy, S.N. Khonina, M.A. Butt, A. Kazmierczak, R. Piramidowicz, "A Numerical Investigation of a Plasmonic Sensor Based on a Metal-Insulator-Metal Waveguide for Simultaneous Detection of Biological Analytes and Ambient Temperature", Nanomaterials 11, 2551 (2021). CrossRef I. Tathfif, A.A. Yaseer, K.S. Rashid, R.H. Sagor, "Metal-insulator-metal waveguide-based optical pressure sensor embedded with arrays of silver nanorods", Optics Express 29, 32365-32376 (2021). CrossRef P.D. Sia, "Overview of Drude-Lorentz type models and their applications", Nanoscale Syst. Math. Model. Theory Appl. 3, 1-13 (2014) CrossRef M.A. Butt, N.L. Kazanskiy, "Nanoblocks embedded in L-shaped nanocavity of a plasmonic sensor for best sensor performance", Optica Applicata LI, 109-120 (2021). CrossRef S. Khani, M. Hayati, "An ultra-high sensitive plasmonic refractive index sensor using an elliptical resonator and MIM waveguide", Superlattices and Microstructures 156, 106970 (2021). CrossRef F. Chen, J. Li, "Refractive index and temperature sensing based on defect resonator coupled with a MIM waveguide", Modern Physics Letters B 33, 1950017 (2019). CrossRef M. Rahmatiyar, M. Danaie, M. Afsahi, "Employment of cascaded coupled resonators for resolution enhancement in plasmonic refractive index sensors", Optical and Quantum Electronics 52, 153 (2020). CrossRef M.A. Butt, S.N. Khonina, N.L. Kazanskiy, "A multichannel metallic dual nano-wall square split-ring resonator: design analysis and applications", Laser Physics Letters 16, 126201 (2019). CrossRef
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Wu, Yali, Ying Ma, Xianfang Song, Lihu Yang, and Shengtian Yang. "Responses of Water Fluxes and Water-Use Efficiency of Maize to Warming Based on Water Transformation Dynamical Processes Experimental Device (WTDPED) Experiment." Water 10, no. 11 (November 14, 2018): 1660. http://dx.doi.org/10.3390/w10111660.
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Evaluating the impacts of warming on water balance components in the groundwater–soil–plant–atmosphere continuum (GSPAC) and crop growth are crucial for assessing the risk of water resources and food security under future global warming. A water transformation dynamical processes experimental device (WTDPED) was developed using a chamber coupled with a weighing lysimeter and groundwater supply system, which could simultaneously control both climatic and ground-water level conditions and accurately monitor water fluxes in the GSPAC. Two experiments with maize under increased temperature by 2 °C (T-warm) and ambient temperature (T-control) scenarios were conducted via the WTDPED. The duration of growing season decreased from 125 days under T-control to 117 days under 2 °C warming. There was little difference of total evapotranspiration (ET) (332.6 mm vs. 332.5 mm), soil water storage change (∆W) (−119.0 mm vs. −119.0 mm), drainage (D) (−13.6 mm vs. −13.5 mm) between T-control and T-warm experiments. The average daily ET for maize significantly increased by approximately 6.7% (p < 0.05) in the T-warm experiment, especially during the sixth leaf to tasseling—silking stage with an increase of 0.36 mm with respect to the T-control experiment. There were evident decreases in LAI (leaf area index), whereas non-significant decreases in mean stem diameter, crop height and leaf chlorophyll content under T-warm compared to T-control experiment. However, the chlorophyll content increased by 12% during the sixth leaf to tasseling–silking stage under 2 °C warming, which accelerated the photosynthesis and transpiration rate. The grain yield and water-use efficiency (WUE) for maize increased by 11.0% and 11.1% in the T-warm experiment, respectively, especially due to enhanced growth during the sixth leaf to tasseling–silking stage. This study provided important references for agricultural planting and water management to adapt to a warming environment.
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Gilewski, Marian. "The ripple-curry amplifier in photonic applications." Photonics Letters of Poland 14, no. 4 (December 31, 2022): 86–88. http://dx.doi.org/10.4302/plp.v14i4.1187.
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This paper discusses the new design of a amplifier for the miniature MEMS-type spectrometer. The application problem of the new amplifier was the correct conditioning of the sensor's photoelectric pulses. The processed signal was a sequence of pulses that had variable both frequency and amplitude value. Thus, such a broadband amplifier should have the functionality of automatic gain control. This paper describes the concept of the new circuit, develops its detailed application, and then performs validation tests. Measurement results of the new circuit are discussed in the final section of the paper. Full Text: PDF ReferencesC. Ortolani, Flow Cytometry Today. Detectors and Electronics, (Springer 2022). pp. 97-119, CrossRef D. Maes, L. Reis, S. Poelman, E. Vissers, V. Avramovic, M. Zaknoune, G. Roelkens, S. Lemey, E. Peytavit, B. Kuyken, "High-Speed Photodiodes on Silicon Nitride with a Bandwidth beyond 100 GHz", Conference on Lasers and Electro-Optics, Optica Publishing Group, (2022). CrossRef R. Das, Y. Xie, A.P. Knights, "All-Silicon Low Noise Photonic Frontend For LIDAR Applications", 2022 IEEE Photonics Conference (IPC), IEEE Xplore (2022). CrossRef FEMTO Messtechnik GmbH, Variable Gain Photoreceiver - Fast Optical Power Meter Series OE-200, DirectLink M. Nehir, C. Frank, S. Aßmann, E.P. Achterberg, "Improving Optical Measurements: Non-Linearity Compensation of Compact Charge-Coupled Device (CCD) Spectrometers", Sensors 19(12), 2833 (2019). CrossRef F. Thomas,; R. Petzold, C. Becker, U. Werban, "Application of Low-Cost MEMS Spectrometers for Forest Topsoil Properties Prediction", Sensors 21(11), 3927 (2021). CrossRef M. Muhiyudin, D. Hutson, D. Gibson, E. Waddell, S. Song, S. Ahmadzadeh, "Miniaturised Infrared Spectrophotometer for Low Power Consumption Multi-Gas Sensing", Sensors 20(14), 3843 (2020). CrossRef S. Maruyama, T Hizawa, K. Takahashi, K. Sawada, "Optical-Interferometry-Based CMOS-MEMS Sensor Transduced by Stress-Induced Nanomechanical Deflection", Sensors 18(1), 138 (2018). CrossRef S. Merlo, P. Poma, E. Crisà, D. Faralli, M. Soldo, "Testing of Piezo-Actuated Glass Micro-Membranes by Optical Low-Coherence Reflectometry", Sensors 17(3), 8 (2017). CrossRef M.S. Wei, F. Xing, B. Li, Z. You, "Investigation of Digital Sun Sensor Technology with an N-Shaped Slit Mask", Sensors 11(10), 9764 (2011). CrossRef Z. Yang, T. Albrow-Owen, W. Cai, T. Hasan, "Miniaturization of optical spectrometers", Science 371, 6528 (2021). CrossRef Hamamatsu Photonics K.K. Fingertip size, ultra-compact spectrometer head integrating MEMS and image sensor technologies. DirectLink Microchip Technology Inc, MCP6291/1R/2/3/4/5 1.0 mA 10 MHz Rail-to-Rail Op Amp, CrossRef Microchip Technology Inc. MCP6021/1R/2/3/4 Rail-to-Rail Input/Output 10 MHz Op Amps, CrossRef
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Wang, Dan, Timothy Hall, Maria Inman, E. Jennings Taylor, Rafael Bento Bento Serpa, Charles B. Parker, and Jeffrey T. Glass. "(Digital Presentation) Graphenated Carbon Nanotube Based MEMS Supercapacitors." ECS Meeting Abstracts MA2022-01, no. 7 (July 7, 2022): 638. http://dx.doi.org/10.1149/ma2022-017638mtgabs.
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The inherent advantages of MEMS (micro-electromechanical system) technology, including small size and cost-effective fabrication, make it ideal for numerous applications in a wide range of industries ranging from defense, automotive, medical, to consumer industries. For applications that require self-powered MEMS electronics, an integrated energy storage device is required. Due to their small size, excellent cycle life and high-power density, miniature supercapacitors are an excellent choice for such an integrated energy storage device. The development of electrode materials and electrode fabrication processes for supercapacitors are thus critical for the practical applications of MEMS technology in electronics. In this presentation, Faraday Technology Inc. and Duke University will discuss a novel 3D graphenated carbon nanotube (g-CNT) network with pseudocapacitive coatings as the electrode materials for fabricating high energy density MEMS supercapacitors. The g-CNT has a high surface area three-dimensional framework of the CNTs coupled with the high edge density of graphene (Figure 1 A), which represents a potential maximum in both charge density and surface area, and thus provide the enhanced capacitance. An innovative electrophoretic deposition (EPD) manufacturing process, based on the use of pulsed electric fields, has been developed for controlled, reproducible, and scalable deposition of g-CNTs on interdigitated electrodes (Figure 1 B). In addition, pseudocapacitive coatings (such as MnO2) have been electrodeposited on the g-CNT coated electrode to further increasing supercapacitor energy density. Figure 1 C shows no redox peaks, which is important for using this structure as a supercapacitor application. The square shape of the cyclic voltammogram shows that ions experience free flow through the 3-D g-CNT structure. The Charge/Discharge curves (Figure 1 D) indicate the areal energy density of g-CNT/MnO2 coated electrodes (either 50 or 100 cyclic voltametric deposition cycles) are 45 and 93 times higher than g-CNT coated electrodes, respectively. In summary, a scalable manufacturing process for fabricating g-CNT network with pseudocapacitive coatings as electrodes has been demonstrated and shown great potential in producing high energy density MEMS supercapacitors for energy harvesting applications. Acknowledgements: The financial support of DOD DMEA STTR program through grant No. HQ0727-21-P-0029 is acknowledged and National Institutes of Health under award number 1R21EY031271 is acknowledged. The information, data, or work presented herein was funded in part by National Aeronautics and Space Administration under Grant No. 80NSSC19K1027, the views and opinions of authors expressed herein do not necessarily state or reflect those of the United States Government or any agency thereof. Figure 1
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Marks, Keith H., Elizabeth E. Nardis, and Malik N. Momin. "Energy Metabolism and Substrate Utilization in Low Birth Weight Neonates Under Radiant Warmers." Pediatrics 78, no. 3 (September 1, 1986): 465–72. http://dx.doi.org/10.1542/peds.78.3.465.
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We evaluated the metabolic response to the thermal demands of an open radiant warmer device, as distinct from convection incubator, in 13 healthy pre-mature infants (1,395 ± 169 g, 28 ± 12 days of age, mean ± SD). Metabolic rate was 10% higher for infants under the radiant warmer than in the incubator (2.60 ± 0.4 v 2.36 ± 0.3 kcal/kg/h; P < .05). The radiant warmer also induced a small (4%), but significant, increase in nonprotein respiratory quotient (0.94 ± 0.1 v 0.90 ± 0.1; P < .05) and a 13% increase in carbon dioxide production (8.26 ± 1.1 v 7.31 ± 1.1 mL/kg/min; P < .05). Subcutaneous fat accumulation (estimated from 60-second skin-fold thickness measurements) was greater under the radiant warmer than in the incubator (0.08 ± 0.05 v 0.04 ± 0.04 mm/d; P < .05). Under the warmer, the infant's mean skin temperatures and core temperatures were normal and similar to those found in the incubator, but the foot temperature was on average 0.6°C cooler. The average rate of weight gain (18 g/kg/d) was the same in the radiant environment. The pattern of the elevated metabolic rate, shift of respiratory quotient coupled with the accumulation of subcutaneous fat, and cool extremities of infants under the radiant warmer may represent a physiologic adaptive response to thermal stress. However, the reasons for the elevated metabolic rate are unclear, because activation of the sympathetic nervous system with the release of catecholamines is not apparently involved. We speculate that change in metabolic activity is more likely related to alterations in sleep and/or behavior patterns in the exposed environment. Given this relatively short-term study of healthy premature infants receiving an excellent caloric intake (120 kcal/kg/d), we conclude that radiant warmers produce no short-term metabolic complications or adverse effects on growth. Although the clinical importance of elevated metabolic rates in infants under radiant warmers is currently uncertain, our data suggest the need for caution in the long-term use of these devices.
Conference papers on the topic "C.C.D. = charge coupled device"
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McNulty, Ian. "Low-noise charge-coupled device camera for soft-x-ray imaging." In OSA Annual Meeting. Washington, D.C.: Optica Publishing Group, 1990. http://dx.doi.org/10.1364/oam.1990.mmm4.
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We have developed an inexpensive, low-noise, high-resolution charge-coupled device (CCD) camera for imaging applications in the soft-x-ray region. It is capable of photon counting, and because it is cryogenically cooled, it can achieve integration times of several hours. A P31 phosphor coating on the CCD active surface downconverts incident x-rays with high efficiency and no loss in spatial resolution. The aluminum camera body is kept under moderate vacuum (1–10 mTorr) by a sorption pump for thermal insulation and unimpeded propagation of x rays to the detector plane. An aluminum coated Si3N4 entrance window delivers acceptable throughput down to 200 eV x-ray energies and effectively blocks external visible-light sources. The internal 0.8 L liquid-nitrogen Dewar flask maintains the detector substrate at –125°C by means of a flexible copper cold finger for ~10 h under ambient conditions. A slow-scan CCD sequencing and sampling circuit based on a CAMAC system provides standard image erasure, integration, and readout functions under computer control. Data-acquisition software permits convenient user manipulation of camera operating parameters as well as on-line image display. Our characterization of the CCD camera with 350 eV x-rays indicates good performance at 1 photon/pixel•s rates.
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Maffione, Robert A., Richard C. Honey, and Robert A. Brown. "Results of in situ closure measurements over long path lengths in the ocean." In OSA Annual Meeting. Washington, D.C.: Optica Publishing Group, 1991. http://dx.doi.org/10.1364/oam.1991.ths2.
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The results of an experiment to measure the absorption, total scattering, and beam attenuation coefficients (a, b, and c respectively) over relatively long path lengths during the August 1990 optical closure cruise aboard the New Horizon are presented. The instrumentation consisted of a narrow-angle and a wide-angle charge-coupled device (CCD) camera, four gated irradiance detectors, an isotropic light source, and two computers. Calculations are described for computing the coefficients a, b, and c from the measurements. We confirmed that, within experimental uncertainty, the closure property holds for the spectral bandwidth used, 465 ± 15 nm.
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Nakagawa, Tadahiro, Naoki Shikazono, and Nobuhide Kasagi. "Numerical Simulation of Electrochemical Reaction in Reconstructed Three-Dimensional LSM/YSZ Composite Cathode." In ASME 2008 6th International Conference on Fuel Cell Science, Engineering and Technology. ASMEDC, 2008. http://dx.doi.org/10.1115/fuelcell2008-65027.
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In the present study, a novel computational scheme for the assessment of the activation polarization of LSM/YSZ composite cathodes is proposed. The scheme consists of modeling techniques of three-dimensional microstructures and an evaluation method of electrochemical characteristics. Two modeling techniques of microstructures are employed, i.e. the stochastic reconstruction (SR) method and the random packing model (RPM). In the SR method, the 3-D structure is reconstructed statistically from the two-point correlation function of the cross-sectional image of SEM-EDX. In RPM, on the other hand, spherical LSM and YSZ particles are randomly packed in the computational domain. This model is mainly used for the parametric survey, because control parameters used in the model have good correspondence to the parameters used in the actual cell manufacturing process. The lattice Boltzmann method coupled with the Butler-Volmer equation is employed for the detailed assessment of the electrochemical characteristics inside the constructed 3-D cathode microstructures. The oxygen diffusion and the electronic and ionic conductions are calculated simultaneously, and coupled with the charge transfer at the three-phase boundary (TPB) using the Butler-Volmer equation. As a result, potential, polarization and current density distributions are fully investigated. The results from the SR method reveal that the cathode sintered at 1150 °C shows the smaller overpotential than the cathodes sintered at 1200 and 1250 °C. The RPM results show that particle diameter and its standard deviation as well as volume fraction of species have large effects on the cathode performance.
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Han, Z. H., H. J. Wang, and Y. B. Guo. "Thermal Shock Behavior of the Supersonic Plasma Sprayed CeO2-Y2O3-ZrO2 Functionally Graded TBC." In ITSC2007, edited by B. R. Marple, M. M. Hyland, Y. C. Lau, C. J. Li, R. S. Lima, and G. Montavon. ASM International, 2007. http://dx.doi.org/10.31399/asm.cp.itsc2007p0518.
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Abstract A functionally graded thermal barrier coating (FG-TBC) of CeO2-Y2O3-ZrO2/NiCoCrAlY was prepared using a recently developed supersonic plasma spray (S-PS) system. The system had dual powder feed ports through which the metal alloy powders were fed into the lower temperature region of the plasma plume, to prevent over oxidation, and the ceramic powders were fed into the high temperature region, to produce complete melting. Such an approach enabled fine configurations having a continuously graded composition transition to be obtained. The thermal shock testing of the deposited samples with 1mm thick FG-TBC system on Ni-based alloy substrates was performed using an in-house-designed multi-functional rotational thermal shock tester. In this tester, the heating-cooling curves and surface morphology of tested specimens can also be observed by a microscope with a CCD (charge-coupled device) camera and recorded on line by means of accessorial computer system to evaluate the thermal shock resistance of tested samples while they were heated by a high heat flux of oxygen-acetylene flame to 1200° C in a time interval of 15~20s followed by water-quenched to ambient temperature. The temperature fields and relevant thermal stresses distribution through the thickness of disk samples were calculated by means of ANSYS finite element method. The numerical approach shows that the maximal tensile stress occur at the C-YSZ top coating at the center of disc samples at the start of rapid cooling by water-quenched, where small reticulated surface cracks were observed, which then propagated perpendicularly about 350µm deep to near the interface between the pure C-YSZ coating and the FGMs layer transition between the C-YSZ and the NiCoCrAlY coatings. These vertical cracks appeared to be arrested without any delamination after 200 thermal shock cycles.
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Chiu, W. K. S., A. V. Virkar, K. L. Reifsnider, F. Rabbi, and Q. Liu. "HeteroFoaMs: Electrode Modeling in Nano-Structured Heterogeneous Materials for Energy Systems." In ASME 2011 9th International Conference on Fuel Cell Science, Engineering and Technology collocated with ASME 2011 5th International Conference on Energy Sustainability. ASMEDC, 2011. http://dx.doi.org/10.1115/fuelcell2011-54950.
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Heterogeneous Functional Materials, e.g., “HeteroFoaMs” are at the heart of countless energy systems, including (from left to right below) heat storage materials (a), batteries (b), solid oxide fuel cells (c), and polymer electrolyte fuel cells (d). HeteroFoaMs are generally nano-structured and porous to accommodate transport of gasses or fluids, and must be multi-functional (i.e., active operators on mass, momentum, energy or charge, in combinations). This paper will discuss several aspects of modeling the relationships between the constituents and microstructure of these material systems and their device functionalities. Technical advances based on these relationships will also be identified and discussed. Three major elements of the general problem of how to model HeteroFoaM electrodes will be addressed. Modeling approaches for ionic charge transfer with electrochemistry in the nano-structured porosity of the electrode will be discussed. Second, the effect of morphology and space charge on conduction through porous doped ceria particle assemblies, and their role in electrode processes will be modeled and described. And third, the effect of local heterogeneity and morphology on charge distributions and polarization in porous dielectric electrode materials will be analyzed using multi-physics field equations set on the details of local morphology. Several new analysis methods and results, as well as experimental data relating to these approaches will be presented. The value, capabilities, and limitations of the approaches will be evaluated.
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McDonald, A., S. Chandra, and C. Moreau. "Impact of Partially Molten Plasma-Sprayed Zirconia Particles on Glass Surfaces." In ITSC2006, edited by B. R. Marple, M. M. Hyland, Y. C. Lau, R. S. Lima, and J. Voyer. ASM International, 2006. http://dx.doi.org/10.31399/asm.cp.itsc2006p0889.
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Abstract Plasma-sprayed yttria-stabilized zirconia particles (~40 µm diameter) were photographed during impact (velocity ~200 m/s) on a glass surface that was maintained at either room temperature or 400°C. A droplet that approached the surface was sensed using a photodetector and after a known delay, a light source was triggered to illuminate the particle in order to photograph it with a charge-coupled device (CCD) camera. A rapid two-color pyrometer was used to collect the thermal radiation from the particles to follow the evolution of their temperature and size, in-flight and after impact. The fully molten particles spread into a thin liquid splat after impacting the surfaces. The partially molten particles disintegrated into small satellite fragments immediately upon impact. The surface area, as indicated by the pyrometric signals, of the partially molten particles during spreading were almost an order of magnitude smaller than that of the fully molten particles. The pyrometric signals, characteristic of the impact of partially molten zirconia, provide a novel method of identifying partially molten ceramic particles after impact on a flat surface.
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Montgomery, David E., Mitchel J. Keil, and Arvid Myklebust. "A PHIGS+ Model Rendering System for Simulation of Spatial Mechanisms." In ASME 1991 International Computers in Engineering Conference and Exposition. American Society of Mechanical Engineers, 1991. http://dx.doi.org/10.1115/cie1991-0029.
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Abstract A device independent system is described for the visualization, modeling, and animation of spatial mechanisms and robots. New ideas and methods are presented to simplify the interactive specification of scene rendering and color parameters using the ISO standard for 3-D graphics, the Programmer’s Hierarchical Interactive Graphic System (PHIGS) and its extensions PHIGS+. The parallels between the PHIGS hierarchical structure and spatial mechanism modeling are described from the level of mechanism through links, joints, geometry primitives to PHIGS graphics primitives. Perception and evaluation of spatial mechanism designs are significantly improved by the use of shaded, lighted, depth cued models under animation. The method is coupled to new algorithms for automatic interference detection and reshaping of mechanism links to avoid collisions. The suitability of PHIGS+ for the modeling and simulation of open loop mechanisms is also described. Examples are presented for rendering and animation of spatial mechanisms on a Raster Technologies (Alliant) GX4000 workstation with a hardware based PHIGS+ graphics subsystem, UNIX, NeWS, and C.
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McDonald, A., S. Chandra, and C. Moreau. "Spreading of Plasma-Sprayed Molybdenum on Grit-Blasted Glass." In ITSC2008, edited by B. R. Marple, M. M. Hyland, Y. C. Lau, C. J. Li, R. S. Lima, and G. Montavon. Verlag für Schweißen und verwandte Verfahren DVS-Verlag GmbH, 2008. http://dx.doi.org/10.31399/asm.cp.itsc2008p0905.
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Abstract Plasma-sprayed, molten molybdenum particles (~55 µm diameter) were photographed during impact on grit-blasted glass surfaces that were maintained at either room temperature or at 350°C. Droplets approaching the surface were sensed using a photodetector and after a known delay, a fast charge-coupled device (CCD) camera was triggered to capture time-integrated images of the spreading splat from behind the glass. A rapid two-color pyrometer was used to collect the thermal radiation from the spreading droplets to follow the evolution of their temperature and calculate the splat cooling rates. It was found that as the surface roughness increased, the maximum spread diameters of the molten molybdenum droplets decreased, while the splat cooling rates increased. Impact on non-heated and heated roughened glass with similar roughness values produced splats with approximately the same maximum spread diameters, skewed morphologies, and cooling rates. On smooth glass, the splat morphologies were circular, with larger maximum spread diameters and smaller cooling rates on non-heated smooth glass. An established model was used to estimate the splat-substrate thermal contact resistances. On highly roughened glass, the thermal contact resistance decreased as the glass roughness increased, suggesting that splat-substrate contact was improved as the molten metal penetrated the spaces between the large asperities.
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Okihana, Harunobu, Keiji Iwata, and Yasuhiro Miwa. "Remote-Controlled Inspection Robot for Nuclear Facilities in Underwater Environment." In 17th International Conference on Nuclear Engineering. ASMEDC, 2009. http://dx.doi.org/10.1115/icone17-75587.
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A remote-controlled inspection robot for nuclear facilities in underwater environment was developed. The Array system of Eddy Current Testing (Array-ECT) is installed on the existing robot that consists of the driving unit and the inspection unit with enlarged Charge-Coupled Device (CCD) camera. It can swim in the tank, crawl on the inner surface of the tank, stay on the inspection area and by its two devices, Array-ECT and enlarged CCD camera, start inspection. Array-ECT can record the color contour image, and also can display oscillograph. This technology had been developed in order to reduce worker’s radiation exposure and improve inspection-ability in nuclear power plants for some Radioactive Waste (RW) tanks. With conventional manual inspection, RW tanks must be examined with the sequence of (a) full drainage and decontamination, (b) scaffolding set-up with workers under high dose, and (c) manual inspection. As such, the inspection is time consuming and workers should have high radiation exposure. With the original robot that has only enlarged CCD camera, inspection can be performed without tank drainage and with minimum worker’s radiation exposure. However, it needs experienced inspector for interpretation of visual examination using enlarged CCD camera. Newly developed robot with Array-ECT and enlarged CCD camera can achieve the same performance using the original robot and an experienced inspector for visual inspection using enlarged CCD camera. The new feature added to the original design (i.e. Array-ECT) eliminates the need for an experienced inspector.
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Sobhansarbandi, Sarvenaz, and Fatemeh Hassanipour. "Melting Process Expedition of Phase Change Materials via Silicone Oil." In ASME 2018 12th International Conference on Energy Sustainability collocated with the ASME 2018 Power Conference and the ASME 2018 Nuclear Forum. American Society of Mechanical Engineers, 2018. http://dx.doi.org/10.1115/es2018-7503.
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This paper presents a novel method of heat transfer enhancement and melting process expedition of phase change materials (PCMs) via silicone oil for the application in thermal energy storage systems. Sudden spot heating/cooling of the PCM causes a non-uniform melting process and in some cases the volume expansion/contraction. To avoid this malfunction, silicone oil can be applied in these systems to increase convective heat transfer (stirring effect). The feasibility of this method is investigated by two experimental analysis, one by having the mixture in a cylindrical container and one in a cubic container. The results from the images taken by Charge-Coupled Device (CCD) camera in the first analysis show a uniform melting process of the PCM. In the second analysis, the comparison is made for the two parallel setups with and without the silicone oil with the same operating conditions. The results show that in the system that lacks silicone oil, the paraffin starts melting after around 11 minutes from the heater start-up, while this time is around 6 minutes in the system with silicone oil. The effectiveness of silicone oil in enhancing the heat transfer rate is shown by a temperature rise of around 10 °C in the container. Applying PCMs in conjunction with silicone oil in various thermal storage systems for heating/cooling applications specifically in solar thermal collectors, enables heat transfer enhancement and consequently heat storage directly on the system.