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1. Numerical simulation of buckling behavior of the buried steel pipeline under reverse fault displacement

Author

J. Zhang, Z. Liang, C. J. Han, and H. Zhang

Subjects
Materials of engineering and construction. Mechanics of materials, TA401-492
Abstract

Reverse fault movement is one of the threats for the structural integrity of buried oil-gas pipelines caused by earthquakes. Buckling behavior of the buried pipeline was investigated by finite element method. Effects of fault displacement, internal pressure, diameter-thick ratio, buried depth and friction coefficient on buckling behavior of the buried steel pipeline were discussed. The results show that internal pressure is the most important factor that affecting the pipeline buckling pattern. Buckling mode of non-pressure pipeline is collapse under reverse fault. Wrinkles appear on buried pressure pipeline when the internal pressure is more than 0.4 Pmax. Four buckling locations appear on the buried pressure pipeline under bigger fault displacement. There is only one wrinkle on the three locations of the pipeline in the rising formation, but more wrinkles on the fourth location. Number of the wrinkle ridges and length of the wavy buckling increase with the increasing of friction coefficient. Number of buckling location decreases gradually with the decreasing of diameter-thick ratio. A protective device of buried pipeline was designed for preventing pipeline damage crossing fault area for its simple structure and convenient installation. Those results can be used to safety evaluation, maintenance and protection of buried pipelines crossing fault area.

Published
2015
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2. [Nasal seromucinous hamartoma: a case report]

Author

X M, Yu, K, Feng, Q G, Ren, H, Ji, X, Li, C J, Han, X L, Pan, and Y, Yuan

Subjects
Diagnosis, Differential, Hamartoma, Nose Diseases, Humans, Nasal Cavity, Nose
Abstract

浆液黏液腺错构瘤（seromucinous hamartoma，SMH）是一种罕见的鼻腔鼻窦良性腺体增生性病变，目前国内外文献仅报道了40余例。本文报道1例山东大学齐鲁医院（青岛）耳鼻咽喉头颈外科收治的发生于蝶筛隐窝的SMH病例，并结合文献复习，介绍鼻腔SMH的临床和影像学特点、诊治及预后。.

Published
2022

3. Numerical Modeling of Mechanical Behavior for Buried Steel Pipelines Crossing Subsidence Strata.

Author

J Zhang, Z Liang, and C J Han

Subjects
Medicine, Science
Abstract

This paper addresses the mechanical behavior of buried steel pipeline crossing subsidence strata. The investigation is based on numerical simulation of the nonlinear response of the pipeline-soil system through finite element method, considering large strain and displacement, inelastic material behavior of buried pipeline and the surrounding soil, as well as contact and friction on the pipeline-soil interface. Effects of key parameters on the mechanical behavior of buried pipeline were investigated, such as strata subsidence, diameter-thickness ratio, buried depth, internal pressure, friction coefficient and soil properties. The results show that the maximum strain appears on the outer transition subsidence section of the pipeline, and its cross section is concave shaped. With the increasing of strata subsidence and diameter-thickness ratio, the out of roundness, longitudinal strain and equivalent plastic strain increase gradually. With the buried depth increasing, the deflection, out of roundness and strain of the pipeline decrease. Internal pressure and friction coefficient have little effect on the deflection of buried pipeline. Out of roundness is reduced and the strain is increased gradually with the increasing of internal pressure. The physical properties of soil have a great influence on the mechanical properties of buried pipeline. The results from the present study can be used for the development of optimization design and preventive maintenance for buried steel pipelines.

Published
2015
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4. Failure Pressure Analysis of the Pipe with Inner Corrosion Defects by FEM

Author

C J. Han

Subjects
020303 mechanical engineering & transports, Materials science, 0203 mechanical engineering, Metallurgy, Electrochemistry, 020101 civil engineering, 02 engineering and technology, Pressure analysis, Finite element method, 0201 civil engineering, Corrosion
Published
2016

5. The Indicators Constructed by FAHP and the Delphi Method to Evaluate Sustainable Development of Taiwan’s Indigenous Tribal Environment

Author

I. C. Liu, C. J. Han, Y. H. Chiang, and Y. L. Liu

Subjects
Sustainable development, Delphi method, Business, Environmental planning, Indigenous
Abstract

The research aims to investigate the indicators for evaluation of sustainable development of Taiwan’s indigenous tribal environment. For that matter, the indicators for evaluation of sustainable development of Taiwan’s indigenous tribal environment are obtained from literature reviews and further 1nalysed through two questionnaire surveys by the Delphi method and the Fuzzy Analytic Hierarchy Process (FAHP).The research findings are summarized as follows: (1) Five first-class indicators and 24 second-class indicators for evaluation of sustainable development of Taiwan’s indigenous tribal environment are derived; (2) First-class indicators are life culture, art culture, historical site, natural environment and tribe experience according to their weights from high to low; (3) Nines key factors for evaluation of sustainable development of Taiwan’s indigenous tribal environment are celebration of festival, traditional cuisine, life etiquette & custom, architectural feature, ancient monument, traditional artistry, life experience, life style and industrial activity. The research findings as suggestions for sustainable development of Taiwan’s indigenous tribal environment will be submitted to the relevant organizations or other researchers who are interested in our research in their follow-up studies.

Published
2020

6. Neutrino-driven Outflows and the Elemental Abundance Patterns of Very Metal-poor Stars

Author

A. Psaltis, M. Jacobi, F. Montes, A. Arcones, C. J. Hansen, and H. Schatz

Subjects
Core-collapse supernovae, Isotopic abundances, Nuclear astrophysics, Nucleosynthesis, Observational astronomy, R-process, Astrophysics, QB460-466
Abstract

The elemental abundances between strontium and silver ( Z = 38–47) observed in the atmospheres of very metal-poor stars in the Galaxy may contain the fingerprint of the weak r -process and ν p -process occurring in early core-collapse supernovae explosions. In this work, we combine various astrophysical conditions based on a steady-state model to cover the richness of the supernova ejecta in terms of entropy, expansion timescale, and electron fraction. The calculated abundances based on different combinations of conditions are compared with stellar observations, with the aim of constraining supernova ejecta conditions. We find that some conditions of the neutrino-driven outflows consistently reproduce the observed abundances of our sample. In addition, from the successful combinations, the neutron-rich trajectories better reproduce the observed abundances of Sr–Zr ( Z = 38–40), while the proton-rich ones, Mo–Pd ( Z = 42–47).

Published
2024
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7. Juno’s JunoCam Images of Europa

Author

C. J. Hansen, M. A. Ravine, P. M. Schenk, G. C. Collins, E. J. Leonard, C. B. Phillips, M. A. Caplinger, F. Tosi, S. J. Bolton, and Björn Jónsson

Subjects
Europa, Astronomy, QB1-991
Abstract

On 2022 September 29 the Juno spacecraft passed Europa at 355 km, the first close pass since the Galileo flyby in 2000. Juno’s visible-light imager, JunoCam, collected four images, enabling cartographic, topographic, and surface geology analysis. The topography along the terminator is consistent with previously reported features that may indicate true polar wander. A bright band was discovered, and indicates global symmetry in the stress field that forms bright bands on Europa. The named feature Gwern is shown not to be an impact crater. Surface change detection shows no changes in 22 yr, although this is a difficult task considering differences between the JunoCam and Galileo imagers and very different viewing geometries. No active eruptions were detected.

Published
2024
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8. Finite element analysis of wrinkling of buried pressure pipeline under strike-slip fault

Author

Z. Liang, Jie Zhang, and C. J. Han

Subjects
geography, Engineering, geography.geographical_feature_category, business.industry, Internal pressure, Bending, Structural engineering, Fault (geology), Condensed Matter Physics, Strike-slip tectonics, Finite element method, Buckling, Bending moment, business, Displacement (fluid)
Abstract

Wrinkling behavior of buried pressure pipeline under strike-slip fault movement was investigated by finite element method. And effects of fault displacement, internal pressure, diameter-thick ratio and dip angle on the wrinkling modes and axial strain of pipeline were discussed. The results show that there are two wrinkling locations of buried pipeline under strike-slip fault displacement. There is only one wrinkle on A part, but more than two wrinkles on B part. Buckling mode of buried steel pipeline presents three states under different internal pressures. They are collapse state, critical state between collapse and wrinkling, and wrinkling state. The greater diameter-thick ratio can enhance the ability to resistance to bending moment. Bending curve of pipeline changes from S-shape to Z-shape with the increasing of diameter-thick ratio. Wrinkling is more serious with the increasing of fault displacement and diameter-thick ratio. There are two wrinkling modes of B part pipeline when dip angle β=0°~45°.DOI: http://dx.doi.org/10.5755/j01.mech.21.3.8891

Published
2015

9. Paper No P18: Study of interfacial treatment on the metal-oxide electron transport layer in the InP quantum dot light-emitting diodes

Author

Ilwan Jang, W. K. Kim, C. Ippen, Sung Kyu Park, Yohan Kim, A. Wedel, C. J. Han, Jiwan Kim, and Publica

Subjects
Electron transport layer, Materials science, business.industry, Annealing (metallurgy), Oxide, law.invention, Metal, chemistry.chemical_compound, Ethanolamine, chemistry, Quantum dot, law, visual_art, visual_art.visual_art_medium, Optoelectronics, business, Diode, Light-emitting diode
Abstract

In this article, we describe the effect of ethanolamine (EA) surface treat-ment on the inverted InP quantum dot light-emitting diodes (QD-LEDs) with inorganic metal oxide layers. The efficiency of the inverted QD-LEDs was significantly enhanced by EA treatment and optimization of the ZnO annealing temperature.

Published
2015

10. Trace but not delay fear conditioning requires attention and the anterior cingulate cortex

Author

David J. Anderson, Colm M. P. O’Tuathaigh, Michael S. Fanselow, Laurent van Trigt, C. J. Han, Jennifer J. Quinn, Raymond Mongeau, and Christof Koch

Subjects
Male, Time Factors, Hippocampus, Biology, Gyrus Cinguli, behavioral disciplines and activities, Brain mapping, Mice, Conditioning, Psychological, medicine, Animals, Premovement neuronal activity, Attention, RNA, Messenger, Fear conditioning, Anterior cingulate cortex, Neurons, Brain Mapping, Multidisciplinary, Genes, fos, Cognition, Fear, Biological Sciences, Associative learning, Mice, Inbred C57BL, medicine.anatomical_structure, Gene Expression Regulation, Conditioning, Operant, Conditioning, Neuroscience, psychological phenomena and processes, Caltech Library Services
Abstract

Higher cognitive functions such as attention have been difficult to model in genetically tractable organisms. In humans, attention-distracting stimuli interfere with trace but not delay conditioning, two forms of associative learning. Attention has also been correlated with activation of anterior cingulate cortex (ACC), but its functional significance is unclear. Here we show that a visual distractor interferes selectively with trace but not delay auditory fear conditioning in mice. Trace conditioning is associated with increased neuronal activity in ACC, as assayed by relative levels of c-fos expression, and is selectively impaired by lesions of this structure. The effects of the ACC lesions are unlikely to be caused by indirect impairment of the hippocampus, which is required for mnemonic aspects of trace conditioning. These data suggest that trace conditioning may be useful for studying neural substrates of attention in mice, and implicate the ACC as one such substrate.

Published
2003

11. Uncooled microbolometers at DRS and elsewhere through 2013

Author

Chuan Li, George D. Skidmore, and C. J. Han

Subjects
Computer science, law, business.industry, Bolometer, Metric (mathematics), Electrical engineering, Microbolometer, Noise-equivalent temperature, business, Telecommunications, law.invention
Abstract

DRS history in microbolometer and uncooled focal plane array (UFPAA) development mimics that of the entire industry. The history extends over fifteen years as array pitches moved ever-smaller from 51uum to 25um to 17um, and now something smaller than 17uum. The uncooled microbolometer makers have transitioned through smaller pitches about every six years. This has been done while maintaining a noise equivalent temperature difference (NNETD) performance of 20-50mK, and maintaining a thermal time constant (TTTC) of 10-20mmSec. Once a newer pitch is developed to a performance level matching the previous pitch, development on the next smaller pitch is already underway. In this manner, the industry has progressed through smaller pitches without a fundamental performance improvement when measured in NNETD or in TTTC, or more specifically in NNETD*TTC product. Hence, a more-encompassing metric for tracking performance through time would involve the NNETD, the TTCC, and some indicator of bolometer size. Ann NETD*TTC**Area metric, as the appropriate metric for including bolometer size, will be proposed, theoretically justified, and discussed here. A rank-ordering of bolometers which have been published through 22013 is also presented in three charts, one for NETTD, one for NEETD*TTC, and lastly one for NETD*TTC**Area.

Published
2014

12. Demonstration of low cost TSV fabrication in thick silicon wafers

Author

G. Skidmore, C. Li, K. Peterson, John Lannon, Erik Vick, R. Anderson, C. J. Han, and Dorota Temple

Subjects
Materials science, Fabrication, Silicon, business.industry, Contact resistance, chemistry.chemical_element, Titanium alloy, Substrate (electronics), chemistry, Chip-scale package, Electronic engineering, Optoelectronics, Wafer, business, Wafer-level packaging
Abstract

Low cost wafer-level chip-scale vacuum packaging (WLCSVP) imposes unique constraints on potential implementation of through-silicon vias (TSVs). A WLCSVP requires a relatively thick substrate to prevent mechanical failure. Two approaches for integrating TSVs in thick silicon wafers have been successfully demonstrated. Both approaches enable TSV formation from the backside of a device wafer and are compatible with the requirements of subsequent packaging operations. We achieved low contact resistance between TSVs and frontside Ti/Cu and Al metallization, while demonstrating high isolation resistance and high TSV yield.

Published
2014

14. Low-cost uncooled VOxinfrared camera development

Author

Robert Bates, Chuan Li, John Lannon, George D. Skidmore, Kenny Kubala, Konstantin Glukh, Grady Cook, C. J. Han, Busbee Hardy, Dorota Temple, and Allan Hilton

Subjects
Infrared, Computer science, business.industry, Detector, Microbolometer, business, Computer hardware, Simulation, Dot pitch
Abstract

The DRS Tamarisk® 320 camera, introduced in 2011, is a low cost commercial camera based on the 17 µm pixel pitch 320×240 VOx microbolometer technology. A higher resolution 17 µm pixel pitch 640×480 Tamarisk® 640 has also been developed and is now in production serving the commercial markets. Recently, under the DARPA sponsored Low Cost Thermal Imager-Manufacturing (LCTI-M) program and internal project, DRS is leading a team of industrial experts from FiveFocal, RTI International and MEMSCAP to develop a small form factor uncooled infrared camera for the military and commercial markets. The objective of the DARPA LCTI-M program is to develop a low SWaP camera ( 3 in volume and

Published
2013

15. 512×512 Infrared cryogenic scene projector arrays

Author

C.-J. Han, Robert E. Higashi, Barry E. Cole, and Jeff A. Ridley

Subjects
Materials science, Pixel, Physics::Instrumentation and Detectors, business.industry, Metals and Alloys, Cryogenics, Condensed Matter Physics, Frame rate, Surfaces, Coatings and Films, Electronic, Optical and Magnetic Materials, law.invention, Optics, Projector, law, Computer Science::Computer Vision and Pattern Recognition, Radiance, Emissivity, Optoelectronics, Electrical and Electronic Engineering, business, Instrumentation, High dynamic range, Common emitter
Abstract

A mosaic array of resistively heated microbridges offers much flexibility for infrared scene simulations. Dynamic scene simulations are important for the testing of the real-time performance capability of IR camera and seeker systems. The excellent thermal properties of the emitter pixels achieved with thin films and unique thermal isolation structures make it possible to achieve high temperatures at power levels ≈ 1 μW per pixel per degree temperature rise. High radiance and high dynamic range are achieved by having pixels with high emissivity and high fill factors, which operate with the substrate and drive electronics at cryogenic temperatures to achieve low background radiance. The thermal time constants of the pixels are defined by material properties and pixel design and are in the millisecond range, making it possible to achieve dynamic frame rates in excess of 100 Hz. Two types of cryogenic resistor arrays have been fabricated and are described, 512×512 arrays with pixels on a 3.5 mil pitch, and 128×128 arrays with pixels on a 2 mil pitch.

Published
1995

16. Uncooled infrared sensor development trends and challenges

Author

C. J. Han, George D. Skidmore, and Chuan Li

Subjects
Amorphous silicon, Infrared, Computer science, business.industry, Detector, Microbolometer, Frame rate, Dot pitch, Image stitching, Wavelength, chemistry.chemical_compound, Cardinal point, chemistry, Optoelectronics, business
Abstract

Uncooled infrared sensor markets have grown dramatically over the past decade due to significant improvements in sensor performance, producibility and cost reductions. Current uncooled sensors are dominated by VOx and amorphous silicon based microbolometers with spectral responses in the 7-14 μm wavelength region (LWIR). The majority of uncooled microbolometer focal plane array (UFPA) formats currently in production are 160x120, 320x240, 640x480 with 20 to 38 um pixel pitch. Most suppliers have reported good UFPA performance with less than 50 mK NETD(f/1 optics, 30 -60 Hz frame rates). Recently, 17 μm pixel pitch UFPAs have been introduced to the market. The smaller detector pixel pitch allows manufacturing of larger format such as 1024x768 UFPAs without photolithographic stitching. In the past, uncooled IR sensor developments were primarily driven by military needs; however, as low cost uncooled sensors began to proliferate in the commercial market, uncooled sensors with FPA formats of 320x240 and smaller are rapidly becoming commodity items. Reduction of sensor system size, weight, and power (SWaP) as well as cost is the key driver for the next generation of uncooled sensors. This paper presents a brief overview of the uncooled sensors status, developmental trends and challenges facing the industry.

Published
2011

17. Uncooled VOx infrared sensor development and application

Author

Chuan Li, George D. Skidmore, and C. J. Han

Subjects
Pixel, Infrared, Computer science, business.industry, Detector, Electrical engineering, Microbolometer, Large format, Focal Plane Arrays, Dot pitch, chemistry.chemical_compound, Optics, chemistry, Night vision, Electronics, business, Night vision device, Indium gallium arsenide, Pixel detector
Abstract

This paper provides an overview of the recent DRS RSTA, Inc. (DRS) Vanadium Oxide (VOx) uncooled focal plane arrays (UFPA), sensor electronics, and camera development activities. Presently, DRS UFPAs consist of 25 μm and 17 μm pixel pitch detectors in 320x240 and 640x480 formats. Under the Army NVESD sponsored 17 μm Large Format Uncooled FPA Development program and internal projects, DRS has developed a 17 μm pitch 1024x768 UFPA product (U8000). The 17 μm pixel pitch UFPAs provide sensor systems with significant size, weight, and power (SWaP) savings as well as cost reductions over the 25 μm pixel pitch counterparts. There is a growing demand to transition current products to the 17 μm pixel technologies. For example, next generation military systems such as thermal weapon sights (TWS), enhanced night vision goggles (ENVG), driver viewer enhancers (DVE) and unmanned aerial vehicle (UAV) infrared (IR) surveillance sensors all called for the 17 μm pixel technologies. To meet market demand, DRS has improved its production facilities to accommodate 17 μm pixel detector manufacturing. In conjunction with these efforts, DRS has also developed a family of signal processing electronics based on a new FPGA architecture for various sensor modules and cameras that can be incorporated into commercial OEM products as well as DoD weapon systems. Under the DARPA funded AWARE Multiband (formerly DUDE) program, DRS and Goodrich Sensors Unlimited, Inc are collaborating on the development of a single, integrated, twocolor detector by combining the VOx microbolometer (8-14 μm) and InGaAs (0.4 -1.6 μm) detectors into a single focal plane array. The first AWARE Multiband dual mode focal plane array fabrication is now underway.

Published
2011

18. DRS uncooled VOx infrared detector development and production status

Author

C. J. Han, Chuan Li, Cory D. Hess, and George D. Skidmore

Subjects
business.industry, Machine vision, Infrared, Computer science, Plasma etcher, Detector, Electrical engineering, Microbolometer, Plasma, Dot pitch, Particle detector, Focal Plane Arrays, Sight, Upgrade, Infrared detector, Stepper, business, Simulation
Abstract

Significant progress has been made over the past decade on uncooled focal plane array (UFPA) technology development and production capacity at DRS as well as other domestic and overseas suppliers. This resulted in the proliferation of uncooled IR detectors in commercial and military markets. The uncooled detectors are widely used in firefighting, surveillance, industrial process monitoring, machine vision, and medical applications. In the military arena, uncooled detectors are fielded among diverse systems such as weapon sights, driver enhancement viewers, helmet-mounted sights, airborne and ground surveillance sensors including UAVs and robot vehicles. Pixel dimensions have continually decreased with an increase in pixel performance. This paper presents an overview of the DRS 25- and 17-micron pixel pitch uncooled VOx detector technology development and production status. The DRS uncooled FPA products include 320x240 and 640x480 arrays while the larger 1024x768 17-micron pitch array is at engineering prototype quantities. Current production of the 25-micron pitch 320x240 and 640x480 arrays exceeds 5,000 units per month, supporting U.S. military systems such as Army thermal weapon sights (TWS) and driver vision enhancers (DVE). Next generation systems are moving towards the 17-micron pixel pitch detectors. Advancement in small pixel technology has enabled the 17-micron pitch detectors performance to surpass their 25-micron pitch counterparts. To meet future production demand of the 17-micron pitch UFPAs, DRS has made significant investment in production infrastructure to upgrade its tools. These investments include a new DUV stepper, coater, and plasma etcher plus improvements in its manufacturing techniques to enhance yield. These advanced tools reduce the minimum line width in production below 0.35μm and are now being used to manufacture the 17-micron 320x240 and 640x480 arrays. To further technology development, DRS continues to engage in R&D activities focusing on VOx microbolometer detector design, packaging, test capability, materials and fabrication processes to further improve the detector performance, reliability, producibility and yield. Some of the results are summarized in this paper.

Published
2010

19. Advancement in 17-micron pixel pitch uncooled focal plane arrays

Author

Howard Christopher G, C. J. Han, George D. Skidmore, Elwood Clarke, and Chuan Li

Subjects
Materials science, Pixel, business.industry, Detector, Bolometer, Microbolometer, Noise-equivalent temperature, Dot pitch, law.invention, Optics, law, Night vision, business, Night vision device
Abstract

This paper provides an update of 17 micron pixel pitch uncooled microbolometer development at DRS. Since the introduction of 17 micron pitch 640x480 focal plane arrays (FPAs) in 2006, significant progress has been made in sensor performance and manufacturing processes. The FPAs are now in initial production with an FPA noise equivalent temperature difference (NETD), detector thermal time constant, and pixel operability equivalent or better than that of the current 25 micron pixel pitch production FPAs. NETD improvement was achieved without compromising detector thermal response or thermal time constant by simultaneous reduction in bolometer heat capacity and thermal conductance. In addition, the DRS unique "umbrella" microbolometer cavities were optically tuned to optimize detector radiation absorption for specific spectral band applications. The 17 micron pixel pitch FPAs are currently being considered for the next generation soldier systems such as thermal weapon sights (TWS), vehicle driver vision enhancers (DVE), digitally fused enhanced night vision goggles (DENVG) and unmanned air vehicle (UAV) surveillance sensors, because of overall thermal imaging system size, weight and power advantages.

Published
2009

21. Recent development of ultra small pixel uncooled focal plane arrays at DRS

Author

Howard Christopher G, Carlos Trujillo, C. J. Han, Eric Williams, Chang-Feng Wan, Jeff R. Emmett, Doug Peysha, Elwood Clarke, Lewis Wood, Gary Robas, George D. Skidmore, Daniel B. Jardine, and Chuan Li

Subjects
Sight, Engineering, Design objective, Fabrication, Pixel, business.industry, Thermography, ComputingMethodologies_IMAGEPROCESSINGANDCOMPUTERVISION, Electronic engineering, Electronics, business, Dot pitch, Data modeling
Abstract

DRS is a major supplier of the 25µm pixel pitch 640x480 and 320x240 infrared uncooled focal plane arrays (UFPAs) and camera products for commercial and military markets. The state-of-the-art 25µm pixel focal plane arrays currently in production provide excellent performance for soldier thermal weapon sights (TWS), vehicle driver vision enhancers (DVE), and aerial surveillance and industrial thermograph applications. To further improve sensor resolution and reduce the sensor system size, weight and cost, it is highly desired to reduce the UFPA pixel size. However, the 17µm pixel FPA presents significant design and fabrication challenges as compared with 25µm pixel FPAs. The design objectives, engineering trade-offs, and performance goals will be discussed. This paper presents an overview of the 17µm microblometer uncooled focal plane arrays and sensor electronics production and development activities at DRS. The 17 µm pixel performance data from several initial fabrication lots will be summarized. Relevant 25µm pixel performance data are provided for comparison. Thermal images and video from the 17µm pixel 640x480 UFPA will also be presented.

Published
2007

22. Paper No S2.2: Ecofriendly Quantum Dot Light-Emitting Diode With Inorganic Charge Transport Layer

Author

J. Lee, B. K. Joo, A. Wedel, Min Suk Oh, Yohan Kim, B. Yoo, C. J. Han, Y. J. Park, and H. Y. Kim

Subjects
Materials science, business.industry, Transistor, Nanotechnology, Charge (physics), Active matrix, law.invention, law, Quantum dot, Thin-film transistor, Transport layer, Optoelectronics, business, Diode, Light-emitting diode
Abstract

Recently, the display technologies using colloidal quantum dot (QD) materials have become one of the most important technologies in the display industry. But, the organic charge transport layer for quantum dot-light-emitting diode (QD-LED) can cause the device stability issues. In this article, we describe the QD-LED devices with inorganic charge transport layer and the solution-based oxide thin-film transistor (TFT) using non-thermal treatment. And we also show the active matrix driving using both technologies simultaneously.

Published
2015

24. 320x240 and 640x480 UFPAs for TWS and DVE applications

Author

Bill Sullivan, Mike Sweeney, Chuan Li, Steve Whicker, Doug Peysha, Phillip Howard, J. Elwood Clarke, C. J. Han, and Richard M. Rawlings

Subjects
Engineering, Reliability (semiconductor), business.industry, Detector, Electrical engineering, Calibration, Time constant, business, Frame rate, Particle detector, Power (physics), Design for manufacturability
Abstract

DRS Technologies has designed and delivered Thermal Weapon Site (TWS) and Driver's Viewer Enhancer (DVE) system using its U3500 (320x240) and U6000 (640x480) 1-mil detector arrays. The detectors are modified to enhance its manufacturability, thermal time constant, package life time, and its reliability under shock and vibration to meet TWS and DVE requirements. The U6000 array operates at 30 Hz frame rate with NETD less than 50 mK normalized to F/1.0 optics. At a saving to the system weight and power, these arrays operate from -40°C to +65°C without the aid of a TE cooler. This is accomplished through a combination of sensor calibration and smart ROIC architecture.

Published
2005

26. Letter to the editor: 1H, 15N, and 13C NMR backbone assignments and secondary structure of the C-terminal recombinant fragment of auxilin including the J-domain

Author

C J, Han, J M, Gruschus, T, Greener, L E, Greene, J, Ferretti, and E, Eisenberg

Subjects
Adaptor Proteins, Vesicular Transport, Recombinant Fusion Proteins, Animals, Nerve Tissue Proteins, Enzyme Inhibitors, Phosphoproteins, Nuclear Magnetic Resonance, Biomolecular, Clathrin, Peptide Fragments, Protein Structure, Secondary
Published
2000

27. Clinical usefulness of serum and plasma vascular endothelial growth factor in cancer patients: which is the optimal specimen?

Author

Joon Kyoo Lee, So-Hye Hong, C J Han, Dae Youn Hwang, and Young Joon Hong

Subjects
Cancer Research, medicine.medical_specialty, Oncogene, Cancer, Biology, medicine.disease, Metastasis, Vascular endothelial growth factor, chemistry.chemical_compound, Vascular endothelial growth factor A, Endocrinology, Circulating tumor cell, Oncology, chemistry, Internal medicine, Cancer cell, Cancer research, medicine, Platelet
Abstract

Vascular endothelial growth factor (VEGF) is secreted by various human cancer cells and plays a key role in cancer angiogenesis and metastasis. Recently, evidence of VEGF storage in blood cells including platelets has been reported. The serum VEGF levels were reported to increase during clotting as a result of its release from platelets, and plasma sample instead of serum was recommended for measuring the circulating VEGF more accurately. However, platelets have been implicated in tumor metastasis since circulating tumor cells forming aggregates with platelets were observed. The purpose of this study was to clarify which is an optimal specimen to measure VEGF in cancer patients, serum or plasma. We measured serum and plasma VEGF levels and platelet counts in 173 cancer patients and 42 healthy people, and found that serum VEGF levels were significantly higher than matched plasma VEGF and the VEGF difference (serum VEGF - plasma VEGF) correlated with platelet counts (r=0.624, p

Published
2000

28. Clinical usefulness of serum and plasma vascular endothelial growth factor in cancer patients: which is the optimal specimen?

Author

J K, Lee, Y J, Hong, C J, Han, D Y, Hwang, and S I, Hong

Subjects
Vascular Endothelial Growth Factor A, Blood Specimen Collection, Lymphokines, Plasma, Platelet Count, Reference Values, Vascular Endothelial Growth Factors, Neoplasms, Humans, Regression Analysis, Enzyme-Linked Immunosorbent Assay, Endothelial Growth Factors, Reagent Kits, Diagnostic
Abstract

Vascular endothelial growth factor (VEGF) is secreted by various human cancer cells and plays a key role in cancer angiogenesis and metastasis. Recently, evidence of VEGF storage in blood cells including platelets has been reported. The serum VEGF levels were reported to increase during clotting as a result of its release from platelets, and plasma sample instead of serum was recommended for measuring the circulating VEGF more accurately. However, platelets have been implicated in tumor metastasis since circulating tumor cells forming aggregates with platelets were observed. The purpose of this study was to clarify which is an optimal specimen to measure VEGF in cancer patients, serum or plasma. We measured serum and plasma VEGF levels and platelet counts in 173 cancer patients and 42 healthy people, and found that serum VEGF levels were significantly higher than matched plasma VEGF and the VEGF difference (serum VEGF - plasma VEGF) correlated with platelet counts (r=0.624, p0.05) in both cancer patients and healthy controls. We selected cancer patients with normal platelet counts (130-400x103/microl, Plt-normal cancer group). Interestingly, serum VEGF levels were higher in Plt-normal cancer group than in healthy controls. The theoretical platelet-derived VEGF in serum, calculated based on actual blood platelet counts (pg per 106 platelets), was also significantly higher in Plt-normal cancer group than in normal controls. It is, therefore, suggested that, although the serum VEGF levels are affected by blood platelets, platelet-derived VEGF also reflect biology of cancer cells, and that serum would be the more useful specimen for measurement of circulating VEGF in cancer patients for prognosis.

Published
2000

29. Attenuation of cardiac but not vascular component in baroreflex of spontaneously hypertensive rats

Author

C J, Han, M L, Tsai, R F, Chen, C Y, Chai, and C T, Yen

Subjects
Atropine, Male, Nitroprusside, Ganglionic Blockers, Parasympatholytics, Blood Pressure, Heart, Baroreflex, Hexamethonium, Rats, Inbred WKY, Rats, Phenylephrine, Heart Rate, Rats, Inbred SHR, Hypertension, Animals, Blood Vessels, Adrenergic alpha-Agonists, Antihypertensive Agents
Abstract

The cardiac and vascular components of the baroreceptor reflex in spontaneously hypertensive rat (SHR) and stroke-prone spontaneously hypertensive rat (SHRSP) were compared against their counterparts in normotensive Wistar Kyoto rat (WKY). SHR, SHRSP and WKY of 12-16 weeks old were chronically instrumented for intra-arterial recording of blood pressure. Intravenous injections of phenylephrine and nitroprusside were used to challenge their baroreflex. The products of blood pressure change and the half time required for the pressure to return to the control value were used as the quantitative estimation of the blood pressure stabilizing capability. The cardiac component of the baroreflex was obtained from the change in the blood pressure stabilizing capability after blockade of beta and muscarinic receptors by atenolol and atropine, respectively. The vascular component was obtained by subtracting the cardiac component from the total stabilizing capability which was the difference after blockade with a ganglionic transmission blocker, hexamethonium. We found the cardiac component of the baroreflex of the hypertensive rats was significantly less sensitive than that of the WKY. In contrast, the vascular component of the baroreflex of the three strains did not differ significantly. Therefore, we concluded that the 12-16 week old SHRs were able to maintain a stable blood pressure due to the intact vascular component of the baroreflex.

Published
1998

30. Advances in microbolometer focal plane technology at Boeing

Author

Philip E. Howard, Phillip A. Ely, John Elwood Clarke, E. T. Fitzgibbons, John C. Stevens, and C. J. Han

Subjects
Physics, business.industry, Bolometer, High density, Microbolometer, Frame rate, Noise (electronics), Die (integrated circuit), law.invention, Optics, Cardinal point, law, Photolithography, business
Abstract

This paper reviews Boeing's progress, over the last three years, in Vanadium Oxide (VO x ) uncooled microbolometer focal plane (UFPA) technology and product development. Boeing's UFPA product technology is described, including product capabilities and performance. Focal plane NETD equals 31 mK (F/1), at a 30 Hz sensor frame rate, has been demonstrated on the U3000 320 X 240 UFPA product. At a 60 Hz frame rate, the NETD (F/1) achieved on production U3000 UFPAs is typically less than 60 mK, and spatial pattern noise levels are consistently less than 33 mK after sensor level gain and offset compensation. Key improvements in VO x tin- film technology have been the achievement of a Temperature Coefficient of Resistance (TCR) approximately 3%, and the achievement of microbolometer resistance uniformity of approximately 1/3% ((sigma) /(mu) ) on the UFPA die. Looking into the future, this year Boeing expects to achieve NETD approximately 20 mK (F/1) with very low pattern noise, and within the next three years higher density 640 X 480 focal planes will be demonstrated with essentially equivalent NETD performance. Large high density uncooled LWIR focal planes, combined with low NETD, will make UFPA technology a prime candidate for higher performance FLIR applications.

Published
1998

31. Acquired Thermotolerance and Stressed-Phase Growth of the Extremely Thermoacidophilic Archaeon Metallosphaera sedula in Continuous Culture

Author

Robert M. Kelly, S H Park, and C J Han

Subjects
Thermal shock, Ecology, Sodium, Analytical chemistry, chemistry.chemical_element, Washout, Biology, Atmospheric temperature range, Applied Microbiology and Biotechnology, Acclimatization, Dilution, chemistry, Metallosphaera sedula, Heat shock, Food Science, Biotechnology, Research Article
Abstract

The response of an extremely thermoacidophilic archaeon, Metallosphaera sedula (growth temperature range, 50 to 79(deg)C; optimum temperature, 74(deg)C; optimum pH, 2.0), to thermal stress was investigated by using a 10-liter continuous cultivation system. M. sedula, growing at 74(deg)C, pH 2.0, and a dilution rate of 0.04 hr(sup-1), was subjected to both abrupt and gradual temperature shifts in continuous culture to determine the responses of cell density levels and protein synthesis patterns. An abrupt temperature shift from 74 to 79(deg)C resulted in little, if any, changes in cell density and a small increase in total protein per cell. When the culture temperature was shifted further to 80.5(deg)C, cell density dropped to below 5 x 10(sup6) cells/ml from 10(sup8) cells/ml, leading to washout of the culture. Operation at this temperature and slightly higher temperatures, however, could be achieved by exposing the culture to thermal stress more gradually (0.5(deg)C increments). As a result, stable operation could be maintained at temperatures of up to 81(deg)C, and the washout temperature could be increased to 82.5(deg)C. Continuous culture operation at 81(deg)C for 100 h (stressed phase) led to an approximately sevenfold lower steady-state cell density than that observed for operation at or below 79(deg)C. However, sodium dodecyl sulfate-polyacrylamide gel electrophoresis analysis (both one and two dimensional) revealed significantly higher levels (sixfold increase) of a 66-kDa stress response protein (MseHSP60), immunologically related to Thermophilic Factor 55 from Sulfolobus shibatae (J. D. Trent, J. Osipiuk, and T. Pinkau, J. Bacteriol. 172:1478-1484, 1990). If the acclimated culture was returned to a lower temperature (i.e., 74(deg)C), the amount of MseHSP60 returned to levels observed prior to thermal acclimation. Furthermore, when the previously acclimated culture (at 81(deg)C) was shifted back from 74 to 81(deg)C, without going through gradual acclimation steps, the result was the immediate onset of washout, suggesting no residual thermotolerance. This study shows that gradual thermal acclimation of M. sedula could only extend the temperature range of stable growth for this organism by 2(deg)C above its maximal growth temperature, albeit at reduced cell densities. Also, this investigation illustrates the utility of continuous culture for characterizing heat shock response and assessing maximum growth temperatures for extremely thermophilic microorganisms.

Published
1997

32. 512x512 cryovacuum resistor infrared scene projector

Author

Barry E. Cole, Blair Sawyer, Dennis Wagner, Robert G. Stockbridge, Robert E. Higashi, Jeff A. Ridley, James O. Holmen, and C.-J. Han

Subjects
Engineering, Pixel, business.industry, Transistor, law.invention, Optics, Projector, law, Black body, Emissivity, Bandwidth (computing), Resistor, business, Common emitter
Abstract

A mosaic array of resistively heated microbridges offers flexibility for infra red scene simulations. The array may operate without flicker and display high-intensity dynamic scenes over a wide bandwidth. Honeywell completed fabrication of a 512 X 512 resistor array with 3.5 mils pitch for AEDC's 7V and 10V test chambers. The emitter has a broad bandwidth covering from 2 micrometers to 26 micrometers . The array operates at 20 K to simulate low radiation backgrounds in space. Up to 16,000 pixels may be turned on to simulate targets and target clusters. Each emitter element may heat up to 550 K with 1 kelvin resolution. The maximum power dissipation per pixel is 830 (mu) W for a pixel heated up to 550 K. The maximum power required is 13.2 watts for 16,000 pixels. This low power capability is derived from Honeywell's silicon nitride microbridge structure. Each emitter has approximately 85% fill factor and an average emissivity of 70% over the 2 - 26 micrometers bandwidth. Defect count in the array is less than 1% with one column out. The array may be addressed at 30 frames per second.© (1995) COPYRIGHT SPIE--The International Society for Optical Engineering. Downloading of the abstract is permitted for personal use only.

Published
1995

33. High-performance 512 x 512 scene projector for targets against space backgrounds

Author

Barry E. Cole, Donald Gordon Pritchett, Robert E. Higashi, B. Sawyer, Lawrence E. Jones, C.-J. Han, Thomas Eugene Old, David G. Edwards, Robert G. Stockbridge, and George C. Goldsmith

Subjects
Resistive touchscreen, Engineering, Pixel, business.industry, Dynamic range, Frame rate, law.invention, Optics, Projector, Black body, law, Computer data storage, Thermal mass, business
Abstract

Honeywell and MRC have been developing a range of thermal scene projector arrays through the Wright Laboratory Armament Directorate's cryovacuum resistive infrared scene projector (CRISP) program and the Defense Nuclear Agency's nuclear optical dynamic display system (NODDS) program. The resistive emitters are fabricated on silicon nitride structures on pitches as small as 2 mils. These structures have low thermal mass, low thermal conductance, and high fill factor. Monolithic address and pixel storage electronics provide flicker-free operation of large arrays at high frame rates. The emitters have demonstrated > 600 K blackbody temperatures, high radiance, and > 103 dynamic range at very low power when operated at 40 K temperatures to achieve low background. This paper describes the performance of a CRISP 512 X 512 array consisting of 3.5 mil pixels and a high-speed 128 X 128 NODDS array consisting of ultra-low-power emitters.

Published
1994

35. Predominant etiologic association of hepatitis C virus with hepatocellular carcinoma compared with hepatitis B virus in elderly patients in a hepatitis B-endemic area

Author

H S, Lee, C J, Han, and C Y, Kim

Subjects
Male, Hepatitis B virus, Carcinoma, Hepatocellular, Korea, Liver Neoplasms, Age Factors, Hepacivirus, Middle Aged, Hepatitis B, Hepatitis C, Humans, Female, Serologic Tests, Aged
Abstract

It has been thought that the mean age of patients with hepatitis B surface antigen (HBsAg) positivity and hepatocellular carcinoma (HCC) is younger than that of patients who test positive for anti-hepatitis C virus. This study was to assess the relative etiologic association of hepatitis B virus (HBV) and hepatitis C virus (HCV) with HCC, according to age-specific groups.A total of 336 Korean patients with HCC were enrolled in the study; the mean age was 53.7 +/- 9.1 years, and the male-to-female ratio was 5.9. HBV serologic markers and anti-HCV were tested using commercially available radioimmunoassay and enzyme immunoassay kits, respectively.Two hundred thirty-three (69.3%) patients tested positive for HBsAg; anti-HCV was positive in 42.7% of 103 patients with HBsAg-negative disease and in 17.0% of all patients with HCC. Coinfection rate of HBV and HCV in the total number of patients with HCC was 3.9%. The mean age was 51.6 years for patients with HBsAg-positive disease and 60.4 years for patients with anti-HCV-positive disease. The ratio of HBsAg positivity compared with anti-HCV positivity in patients with HCC was 29.7 for patients younger than 50 years; 0.9 for patients older than 61 years; and 5.2 for patients in their 50s.The authors conclude that although HBV infection plays a more important etiologic role in the development of HCC in Korea than does HCV, HCV is no less frequently involved than HBV in the etiology of HCC for patients older than 61 years. Thus, in surveillance programs for the early detection of HCC, closer attention should be directed to the patients with anti-HCV-positivity and chronic liver disease, especially patients older than 61 years, even in a hepatitis-B-endemic area.

Published
1993

36. Ultra-low-power scene projector for targets against space backgrounds

Author

Thomas E. Old, Barry E. Cole, Robert E. Higashi, Burt W. Ludington, Thomas R. Werner, Roy W. Hendrick, C.-J. Han, and B. Sawyer

Subjects
Resistive touchscreen, Pixel, Projector, Infrared, law, Computer science, Optical engineering, Computer graphics (images), Clutter, Joint (audio engineering), Frame rate, Simulation, law.invention
Abstract

Honeywell Inc. and Mission Research Corporation (MRC) are jointly developing micro resistive heater array displays for projecting dynamic background scenes and targets in the short-wavelength infrared (SWIR) to long-wavelength infrared (LWIR) wavebands. There are two joint government contracts supporting this work: the Nuclear Optical Dynamic Display (NODDS) program under DNA contract DNA001-92-C-0041, which is developing a 512 X 512 array of 50- by 50-micrometers display pixels, and the Cryovacuum Resistor Infrared Scene Projector (CRISP) program for the USAF Wright Laboratory at Eglin AFB, which is developing a 512 X 512 array of 87.5- by 87.5-micrometers pixels. The requirements on the two programs are somewhat different due to their different missions. While the NODDS program is developing an array that can be used to create dynamic nuclear clutter scenes, the CRISP arrays are being designed for simulating multiple independently moving targets; and while the frame rate on the NODDS arrays requires an array capable of 1-kHz frame rates, the CRISP arrays will be operated at 30 Hz.© (1993) COPYRIGHT SPIE--The International Society for Optical Engineering. Downloading of the abstract is permitted for personal use only.

Published
1993

37. Parallel Oxidation Mechanism for Si Oxidation in Dry O 2

Author

C. Robert Helms and C. J. Han

Subjects
Thermal oxidation, Silicon, Renewable Energy, Sustainability and the Environment, Chemistry, Diffusion, Kinetics, Oxygene, chemistry.chemical_element, Condensed Matter Physics, Oxygen, Surfaces, Coatings and Films, Electronic, Optical and Magnetic Materials, Oxidizing agent, Materials Chemistry, Electrochemistry, Physical chemistry, Growth rate, computer, computer.programming_language
Abstract

Recent results of 18O tracer experiments on thermal oxidation of Si in dry suggest two oxidizing species are responsible for the growth of . We examine here a model that reflects these mechanisms in the growth rate, using a sum of two linear‐parabolic growth rates. The model gives very close fits to the oxidation kinetics data for oxides ranging from 30A to 1 μm thick and for temperatures from 800° to 1200°C at both (100) and (111) Si orientations. Only three parameters are necessary in this model to provide excellent fits to the experimental data. A parallel diffusion of and another undetermined species is consistent with the result.

Published
1987

38. Silicon Dry Oxidation Kinetics: Effects of the Choice of Integration Constant on Fits to the Linear Parabolic Model

Author

C. R. Helms and C. J. Han

Subjects
Silicon, Renewable Energy, Sustainability and the Environment, Kinetics, Constant of integration, Thermodynamics, chemistry.chemical_element, Condensed Matter Physics, Surfaces, Coatings and Films, Electronic, Optical and Magnetic Materials, chemistry, Materials Chemistry, Electrochemistry, Physical chemistry, Parabolic model
Published
1987

39. Compositional Studies of Thermally Nitrided Silicon Dioxide (Nitroxide)

Author

Steven C. Shatas, C. R. Helms, C. J. Han, Krishna C. Saraswat, and Mehrdad M. Moslehi

Subjects
Nitroxide mediated radical polymerization, Renewable Energy, Sustainability and the Environment, Silicon dioxide, Kinetics, Condensed Matter Physics, Surfaces, Coatings and Films, Electronic, Optical and Magnetic Materials, Ammonia, chemistry.chemical_compound, chemistry, Etching (microfabrication), Materials Chemistry, Electrochemistry, Physical chemistry, Thermal reaction, Nitriding
Abstract

Cinetique de la nitruration thermique de SiO 2 dans NH 3 . Structure multicouche des films d'oxyde nitrures formes

Published
1985

40. Time‐dependent compositional variation in SiO2films nitrided in ammonia

Author

Mehrdad M. Moslehi, Krishna C. Saraswat, C. R. Helms, and C. J. Han

Subjects
Nitroxide mediated radical polymerization, Physics and Astronomy (miscellaneous), chemistry, Sputtering, Kinetics, Analytical chemistry, chemistry.chemical_element, Chemical composition, Nitrogen, Oxygen, Nitriding, Auger
Abstract

We report on selected results of an extensive study of SiO2 nitridation in an NH3 ambient obtained primarily using Auger sputter profiling. By investigating a large matrix of samples, we have sorted out the discrepancies present in the literature concerning the kinetics of the nitridation process. Two major new results obtained are the quantitative observation of oxygen depletion in the nitroxide ‘‘bulk’’ region and, consistent with a recent report by R. Vasquez, M. Hecht, F. Grunthaner, and M. Naiman [Appl. Phys. Lett. 44, 969 (1984)], the reoxidation of the interface by oxygen presumably liberated by the bulk exchange reaction.

Published
1985

41. Isotopic tracer studies of oxygen transport through SiO2films at 1000 °C using secondary ion mass spectrometry

Author

C. J. Han and C. R. Helms

Subjects
chemistry.chemical_classification, Self-diffusion, Diffusion, Analytical chemistry, Oxygen transport, Lattice diffusion coefficient, Oxide, General Physics and Astronomy, chemistry.chemical_element, Oxygen, Secondary ion mass spectrometry, chemistry.chemical_compound, chemistry, Inorganic compound
Abstract

Dry oxides (≤8 ppm H2O) grown on Si(100) at 1000 °C at 1 atm using purified 16O2 and purified 18O2 were analyzed using secondary ion mass spectrometry. 18O is observed at the interface, in the bulk of the 16O oxide, and at the surface in agreement with other recent reports. Our results show little lattice diffusion in agreement with Mikkelsen’s work [Appl. Phys. Lett. 45, 1187 (1984)]. A previous report [J. Electrochem. Soc. 131, 1944 (1984)] of appreciable lattice diffusion is due to higher water content.

Published
1986

42. Difficulties with the Lag‐Time Measurement of Oxygen Diffusion in Thermally‐Grown SiO2

Author

C. R. Helms and C. J. Han

Subjects
Materials science, Lag time, Renewable Energy, Sustainability and the Environment, Materials Chemistry, Electrochemistry, Physical chemistry, Oxygen diffusion, Condensed Matter Physics, Surfaces, Coatings and Films, Electronic, Optical and Magnetic Materials
Abstract

Discussion des resultats obtenus par Irene et comparaison avec ceux obtenus par Norton dans le cas de la diffusion de l'oxygene dans la silice fondue. Mise en evidence d'un effet de memoire dans la constante de vitesse parabolique montrant que les proprietes de transport de l'oxygene dans SiO 2 dependent de la temperature de croissance de l'oxyde

Published
1985

43. Search for lepton flavour violation in the eμ continuum with the ATLAS detector in $\sqrt{s} = 7~\mbox{TeV}$ pp collisions at the LHC

Author

The ATLAS Collaboration, G. Aad, B. Abbott, J. Abdallah, A. A. Abdelalim, A. Abdesselam, O. Abdinov, B. Abi, M. Abolins, H. Abramowicz, H. Abreu, E. Acerbi, B. S. Acharya, D. L. Adams, T. N. Addy, J. Adelman, S. Adomeit, P. Adragna, T. Adye, S. Aefsky, J. A. Aguilar-Saavedra, M. Aharrouche, S. P. Ahlen, F. Ahles, A. Ahmad, M. Ahsan, G. Aielli, T. Akdogan, T. P. A. Åkesson, G. Akimoto, A. V. Akimov, A. Akiyama, A. Aktas, M. S. Alam, M. A. Alam, S. Albrand, M. Aleksa, I. N. Aleksandrov, M. Aleppo, F. Alessandria, C. Alexa, G. Alexander, G. Alexandre, T. Alexopoulos, M. Alhroob, M. Aliev, G. Alimonti, J. Alison, M. Aliyev, P. P. Allport, S. E. Allwood-Spiers, J. Almond, A. Aloisio, R. Alon, A. Alonso, M. G. Alviggi, K. Amako, C. Amelung, V. V. Ammosov, A. Amorim, G. Amorós, N. Amram, C. Anastopoulos, T. Andeen, C. F. Anders, K. J. Anderson, A. Andreazza, V. Andrei, X. S. Anduaga, A. Angerami, F. Anghinolfi, N. Anjos, A. Annovi, A. Antonaki, M. Antonelli, S. Antonelli, A. Antonov, J. Antos, F. Anulli, S. Aoun, L. Aperio Bella, R. Apolle, G. Arabidze, I. Aracena, Y. Arai, A. T. H. Arce, J. P. Archambault, S. Arfaoui, J-F. Arguin, E. Arik, M. Arik, A. J. Armbruster, O. Arnaez, C. Arnault, A. Artamonov, G. Artoni, D. Arutinov, M. Asai, S. Asai, R. Asfandiyarov, S. Ask, B. Åsman, D. Asner, L. Asquith, K. Assamagan, A. Astbury, A. Astvatsatourov, G. Atoian, B. Aubert, E. Auge, K. Augsten, M. Aurousseau, N. Austin, G. Avolio, R. Avramidou, D. Axen, G. Azuelos, Y. Azuma, M. A. Baak, G. Baccaglioni, C. Bacci, A. M. Bach, H. Bachacou, K. Bachas, G. Bachy, M. Backes, M. Backhaus, E. Badescu, P. Bagnaia, S. Bahinipati, Y. Bai, D. C. Bailey, T. Bain, J. T. Baines, O. K. Baker, M. D. Baker, S. Baker, F. Baltasar Dos Santos Pedrosa, E. Banas, P. Banerjee, Sw. Banerjee, D. Banfi, A. Bangert, V. Bansal, H. S. Bansil, L. Barak, S. P. Baranov, A. Barbaro Galtieri, T. Barber, E. L. Barberio, D. Barberis, M. Barbero, D. Y. Bardin, T. Barillari, M. Barisonzi, T. Barklow, N. Barlow, B. M. Barnett, R. M. Barnett, A. Baroncelli, A. J. Barr, F. Barreiro, J. Barreiro Guimarães da Costa, P. Barrillon, R. Bartoldus, A. E. Barton, D. Bartsch, V. Bartsch, R. L. Bates, L. Batkova, J. R. Batley, A. Battaglia, M. Battistin, G. Battistoni, F. Bauer, H. S. Bawa, B. Beare, T. Beau, P. H. Beauchemin, R. Beccherle, P. Bechtle, G. A. Beck, H. P. Beck, M. Beckingham, K. H. Becks, A. J. Beddall, A. Beddall, S. Bedikian, V. A. Bednyakov, C. P. Bee, M. Begel, S. Behar Harpaz, P. K. Behera, M. Beimforde, C. Belanger-Champagne, P. J. Bell, W. H. Bell, G. Bella, L. Bellagamba, F. Bellina, G. Bellomo, M. Bellomo, A. Belloni, O. Beloborodova, K. Belotskiy, O. Beltramello, S. Ben Ami, O. Benary, D. Benchekroun, C. Benchouk, M. Bendel, B. H. Benedict, N. Benekos, Y. Benhammou, D. P. Benjamin, M. Benoit, J. R. Bensinger, K. Benslama, S. Bentvelsen, M. Beretta, D. Berge, E. Bergeaas Kuutmann, N. Berger, F. Berghaus, E. Berglund, J. Beringer, K. Bernardet, P. Bernat, R. Bernhard, C. Bernius, T. Berry, A. Bertin, F. Bertolucci, M. I. Besana, N. Besson, S. Bethke, W. Bhimji, R. M. Bianchi, M. Bianco, O. Biebel, S. P. Bieniek, J. Biesiada, M. Biglietti, H. Bilokon, M. Bindi, S. Binet, A. Bingul, C. Bini, C. Biscarat, U. Bitenc, K. M. Black, R. E. Blair, J.-B. Blanchard, G. Blanchot, C. Blocker, J. Blocki, A. Blondel, W. Blum, U. Blumenschein, G. J. Bobbink, V. B. Bobrovnikov, S. S. Bocchetta, A. Bocci, C. R. Boddy, M. Boehler, J. Boek, N. Boelaert, S. Böser, J. A. Bogaerts, A. Bogdanchikov, A. Bogouch, C. Bohm, V. Boisvert, T. Bold, V. Boldea, M. Bona, M. Bondioli, M. Boonekamp, G. Boorman, C. N. Booth, P. Booth, S. Bordoni, C. Borer, A. Borisov, G. Borissov, I. Borjanovic, S. Borroni, K. Bos, D. Boscherini, M. Bosman, H. Boterenbrood, D. Botterill, J. Bouchami, J. Boudreau, E. V. Bouhova-Thacker, C. Boulahouache, C. Bourdarios, N. Bousson, A. Boveia, J. Boyd, I. R. Boyko, N. I. Bozhko, I. Bozovic-Jelisavcic, J. Bracinik, A. Braem, E. Brambilla, P. Branchini, A. Brandt, G. Brandt, O. Brandt, U. Bratzler, B. Brau, J. E. Brau, H. M. Braun, B. Brelier, J. Bremer, R. Brenner, S. Bressler, D. Breton, N. D. Brett, P. G. Bright-Thomas, D. Britton, F. M. Brochu, I. Brock, R. Brock, E. Brodet, F. Broggi, C. Bromberg, G. Brooijmans, W. K. Brooks, G. Brown, E. Brubaker, P. A. Bruckman de Renstrom, D. Bruncko, R. Bruneliere, S. Brunet, A. Bruni, G. Bruni, M. Bruschi, T. Buanes, F. Bucci, J. Buchanan, N. J. Buchanan, P. Buchholz, R. M. Buckingham, A. G. Buckley, S. I. Buda, I. A. Budagov, B. Budick, V. Büscher, L. Bugge, D. Buira-Clark, E. J. Buis, O. Bulekov, M. Bunse, T. Buran, H. Burckhart, S. Burdin, T. Burgess, S. Burke, E. Busato, P. Bussey, C. P. Buszello, B. Butler, J. M. Butler, C. M. Buttar, J. M. Butterworth, W. Buttinger, T. Byatt, J. Caballero, S. Cabrera Urbán, M. Caccia, D. Caforio, O. Cakir, P. Calafiura, G. Calderini, P. Calfayan, R. Calkins, L. P. Caloba, R. Caloi, D. Calvet, S. Calvet, R. Camacho Toro, A. Camard, P. Camarri, D. Cameron, J. Cammin, S. Campana, M. Campanelli, V. Canale, F. Canelli, A. Canepa, J. Cantero, L. Capasso, M. D. M. Capeans Garrido, I. Caprini, M. Caprini, D. Capriotti, M. Capua, R. Caputo, C. Caramarcu, R. Cardarelli, T. Carli, G. Carlino, L. Carminati, B. Caron, S. Caron, C. Carpentieri, G. D. Carrillo Montoya, A. A. Carter, J. R. Carter, J. Carvalho, D. Casadei, M. P. Casado, M. Cascella, C. Caso, A. M. Castaneda Hernandez, E. Castaneda-Miranda, V. Castillo Gimenez, N. F. Castro, G. Cataldi, F. Cataneo, A. Catinaccio, J. R. Catmore, A. Cattai, G. Cattani, S. Caughron, A. Cavallari, P. Cavalleri, D. Cavalli, M. Cavalli-Sforza, V. Cavasinni, A. Cazzato, F. Ceradini, A. S. Cerqueira, A. Cerri, L. Cerrito, F. Cerutti, S. A. Cetin, A. Chafaq, D. Chakraborty, K. Chan, B. Chapleau, J. D. Chapman, J. W. Chapman, E. Chareyre, D. G. Charlton, V. Chavda, S. Cheatham, S. Chekanov, S. V. Chekulaev, G. A. Chelkov, M. A. Chelstowska, C. Chen, H. Chen, L. Chen, S. Chen, X. Chen, A. Cheplakov, R. Cherkaoui El Moursli, V. Chernyatin, E. Cheu, S. L. Cheung, L. Chevalier, G. Chiefari, L. Chikovani, J. T. Childers, A. Chilingarov, G. Chiodini, M. V. Chizhov, G. Choudalakis, S. Chouridou, I. A. Christidi, A. Christov, D. Chromek-Burckhart, M. L. Chu, J. Chudoba, G. Ciapetti, K. Ciba, A. K. Ciftci, R. Ciftci, D. Cinca, V. Cindro, M. D. Ciobotaru, C. Ciocca, A. Ciocio, M. Cirilli, M. Citterio, M. Ciubancan, A. Clark, P. J. Clark, W. Cleland, J. C. Clemens, B. Clement, C. Clement, R. W. Clifft, Y. Coadou, M. Cobal, A. Coccaro, J. Cochran, P. Coe, S. Coelli, J. G. Cogan, J. Coggeshall, E. Cogneras, C. D. Cojocaru, J. Colas, A. P. Colijn, C. Collard, N. J. Collins, C. Collins-Tooth, J. Collot, G. Colon, R. Coluccia, G. Comune, P. Conde Muiño, E. Coniavitis, M. C. Conidi, M. Consonni, S. Constantinescu, C. Conta, F. Conventi, M. Cooke, B. D. Cooper, A. M. Cooper-Sarkar, K. Copic, T. Cornelissen, M. Corradi, F. Corriveau, A. Corso-Radu, A. Cortes-Gonzalez, G. Cortiana, G. Costa, M. J. 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Zhang, J. Zhang, Q. Zhang, X. Zhang, Z. Zhang, L. Zhao, T. Zhao, Z. Zhao, A. Zhemchugov, J. Zhong, B. Zhou, N. Zhou, Y. Zhou, C. G. Zhu, H. Zhu, Y. Zhu, X. Zhuang, V. Zhuravlov, D. Zieminska, B. Zilka, R. Zimmermann, S. Zimmermann, M. Ziolkowski, R. Zitoun, L. Živković, V. V. Zmouchko, G. Zobernig, A. Zoccoli, Y. Zolnierowski, A. Zsenei, M. zur Nedden, V. Zutshi, and L. Zwalinski

Subjects
Astrophysics, QB460-466, Nuclear and particle physics. Atomic energy. Radioactivity, QC770-798
Abstract

Abstract This paper presents a search for the t-channel exchange of an R-parity violating scalar top quark ( $\tilde{t}$ ) in the e ± μ ∓ continuum using 2.1 fb−1 of data collected by the ATLAS detector in $\sqrt{s}=7~\mbox{TeV}$ pp collisions at the Large Hadron Collider. Data are found to be consistent with the expectation from the Standard Model backgrounds. Limits on R-parity-violating couplings at 95 % C.L. are calculated as a function of the scalar top mass ( $m_{\tilde{t}}$ ). The upper limits on the production cross section for pp→eμX, through the t-channel exchange of a scalar top quark, ranges from 170 fb for $m_{\tilde{t}}=95~\mbox{GeV}$ to 30 fb for $m_{\tilde{t}}=1000~\mbox{GeV}$ .

Published
2012
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44. Luminosity determination in pp collisions at $\sqrt{s} = 7$ TeV using the ATLAS detector at the LHC

Author

The ATLAS Collaboration, G. Aad, B. Abbott, J. Abdallah, A. A. Abdelalim, A. Abdesselam, O. Abdinov, B. Abi, M. Abolins, H. Abramowicz, H. Abreu, E. Acerbi, B. S. Acharya, M. Ackers, D. L. Adams, T. N. Addy, J. Adelman, M. Aderholz, S. Adomeit, P. Adragna, T. Adye, S. Aefsky, J. A. Aguilar-Saavedra, M. Aharrouche, S. P. Ahlen, F. Ahles, A. Ahmad, H. Ahmed, M. Ahsan, G. Aielli, T. Akdogan, T. P. A. Åkesson, G. Akimoto, A. V. Akimov, M. S. Alam, M. A. Alam, S. Albrand, M. Aleksa, I. N. Aleksandrov, M. Aleppo, F. Alessandria, C. Alexa, G. Alexander, G. Alexandre, T. Alexopoulos, M. Alhroob, M. Aliev, G. Alimonti, J. Alison, M. Aliyev, P. P. Allport, S. E. Allwood-Spiers, J. Almond, A. Aloisio, R. Alon, A. Alonso, J. Alonso, M. G. Alviggi, K. Amako, P. Amaral, C. Amelung, V. V. Ammosov, A. Amorim, G. Amorós, N. Amram, C. Anastopoulos, T. Andeen, C. F. Anders, K. J. Anderson, A. Andreazza, V. Andrei, M.-L. Andrieux, X. S. Anduaga, A. Angerami, F. Anghinolfi, N. Anjos, A. Annovi, A. 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Pilcher, A. D. Pilkington, J. Pina, M. Pinamonti, A. Pinder, J. L. Pinfold, J. Ping, B. Pinto, O. Pirotte, C. Pizio, R. Placakyte, M. Plamondon, W. G. Plano, M.-A. Pleier, A. V. Pleskach, A. Poblaguev, S. Poddar, F. Podlyski, L. Poggioli, T. Poghosyan, M. Pohl, F. Polci, G. Polesello, A. Policicchio, A. Polini, J. Poll, V. Polychronakos, D. M. Pomarede, D. Pomeroy, K. Pommès, L. Pontecorvo, B. G. Pope, G. A. Popeneciu, D. S. Popovic, A. Poppleton, X. Portell Bueso, R. Porter, C. Posch, G. E. Pospelov, S. Pospisil, I. N. Potrap, C. J. Potter, C. T. Potter, G. Poulard, J. Poveda, R. Prabhu, P. Pralavorio, S. Prasad, R. Pravahan, S. Prell, K. Pretzl, L. Pribyl, D. Price, L. E. Price, M. J. Price, P. M. Prichard, D. Prieur, M. Primavera, K. Prokofiev, F. Prokoshin, S. Protopopescu, J. Proudfoot, X. Prudent, H. Przysiezniak, S. Psoroulas, E. Ptacek, J. Purdham, M. Purohit, P. Puzo, Y. Pylypchenko, J. Qian, Z. Qian, Z. Qin, A. Quadt, D. R. Quarrie, W. B. Quayle, F. Quinonez, M. Raas, V. Radescu, B. Radics, T. Rador, F. Ragusa, G. Rahal, A. M. Rahimi, S. Rajagopalan, S. Rajek, M. Rammensee, M. Rammes, M. Ramstedt, K. Randrianarivony, P. N. Ratoff, F. Rauscher, E. Rauter, M. Raymond, A. L. Read, D. M. Rebuzzi, A. Redelbach, G. Redlinger, R. Reece, K. Reeves, A. Reichold, E. Reinherz-Aronis, A. Reinsch, I. Reisinger, D. Reljic, C. Rembser, Z. L. Ren, A. Renaud, P. Renkel, B. Rensch, M. Rescigno, S. Resconi, B. Resende, P. Reznicek, R. Rezvani, A. Richards, R. Richter, E. Richter-Was, M. Ridel, S. Rieke, M. Rijpstra, M. Rijssenbeek, A. Rimoldi, L. Rinaldi, R. R. Rios, I. Riu, G. Rivoltella, F. Rizatdinova, E. Rizvi, S. H. Robertson, A. Robichaud-Veronneau, D. Robinson, J. E. M. Robinson, M. Robinson, A. Robson, J. G. Rocha de Lima, C. Roda, D. Roda Dos Santos, S. Rodier, D. Rodriguez, Y. Rodriguez Garcia, A. Roe, S. Roe, O. Røhne, V. Rojo, S. Rolli, A. Romaniouk, V. M. Romanov, G. Romeo, D. Romero Maltrana, L. Roos, E. Ros, S. Rosati, M. Rose, G. A. Rosenbaum, E. I. Rosenberg, P. L. Rosendahl, L. Rosselet, V. Rossetti, E. Rossi, L. P. Rossi, L. Rossi, M. Rotaru, I. Roth, J. Rothberg, I. Rottländer, D. Rousseau, C. R. Royon, A. Rozanov, Y. Rozen, X. Ruan, I. Rubinskiy, B. Ruckert, N. Ruckstuhl, V. I. Rud, G. Rudolph, F. Rühr, A. Ruiz-Martinez, E. Rulikowska-Zarebska, V. Rumiantsev, L. Rumyantsev, K. Runge, O. Runolfsson, Z. Rurikova, N. A. Rusakovich, D. R. Rust, J. P. Rutherfoord, C. Ruwiedel, P. Ruzicka, Y. F. Ryabov, V. Ryadovikov, P. Ryan, M. Rybar, G. Rybkin, N. C. Ryder, S. Rzaeva, A. F. Saavedra, I. Sadeh, H. F.-W. Sadrozinski, R. Sadykov, F. Safai Tehrani, H. Sakamoto, G. Salamanna, A. Salamon, M. Saleem, D. Salihagic, A. Salnikov, J. Salt, B. M. Salvachua Ferrando, D. Salvatore, F. Salvatore, A. Salzburger, D. Sampsonidis, B. H. Samset, H. Sandaker, H. G. Sander, M. P. Sanders, M. Sandhoff, P. Sandhu, T. Sandoval, R. Sandstroem, S. Sandvoss, D. P. C. Sankey, A. Sansoni, C. Santamarina Rios, C. Santoni, R. Santonico, H. Santos, J. G. 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Seifert, J. M. Seixas, G. Sekhniaidze, D. M. Seliverstov, B. Sellden, G. Sellers, M. Seman, N. Semprini-Cesari, C. Serfon, L. Serin, R. Seuster, H. Severini, M. E. Sevior, A. Sfyrla, E. Shabalina, M. Shamim, L. Y. Shan, J. T. Shank, Q. T. Shao, M. Shapiro, P. B. Shatalov, L. Shaver, C. Shaw, K. Shaw, D. Sherman, P. Sherwood, A. Shibata, S. Shimizu, M. Shimojima, T. Shin, A. Shmeleva, M. J. Shochet, D. Short, M. A. Shupe, P. Sicho, A. Sidoti, A. Siebel, F. Siegert, J. Siegrist, Dj. Sijacki, O. Silbert, J. Silva, Y. Silver, D. Silverstein, S. B. Silverstein, V. Simak, Lj. Simic, S. Simion, B. Simmons, M. Simonyan, P. Sinervo, N. B. Sinev, V. Sipica, G. Siragusa, A. N. Sisakyan, S. Yu. Sivoklokov, J. Sjölin, T. B. Sjursen, L. A. Skinnari, K. Skovpen, P. Skubic, N. Skvorodnev, M. Slater, T. Slavicek, K. Sliwa, T. J. Sloan, J. Sloper, V. Smakhtin, S. Yu. Smirnov, L. N. Smirnova, O. Smirnova, B. C. Smith, D. Smith, K. M. Smith, M. Smizanska, K. Smolek, A. A. Snesarev, S. W. Snow, J. Snow, J. Snuverink, S. Snyder, M. Soares, R. Sobie, J. Sodomka, A. Soffer, C. A. Solans, M. Solar, J. Solc, U. Soldevila, E. Solfaroli Camillocci, A. A. Solodkov, O. V. Solovyanov, J. Sondericker, N. Soni, V. Sopko, B. Sopko, M. Sorbi, M. Sosebee, A. Soukharev, S. Spagnolo, F. Spanò, R. Spighi, G. Spigo, F. Spila, E. Spiriti, R. Spiwoks, M. Spousta, T. Spreitzer, B. Spurlock, R. D. St. Denis, T. Stahl, J. Stahlman, R. Stamen, E. Stanecka, R. W. Stanek, C. Stanescu, S. Stapnes, E. A. Starchenko, J. Stark, P. Staroba, P. Starovoitov, A. Staude, P. Stavina, G. Stavropoulos, G. Steele, E. Stefanidis, P. Steinbach, P. Steinberg, I. Stekl, B. Stelzer, H. J. Stelzer, O. Stelzer-Chilton, H. Stenzel, K. Stevenson, G. A. Stewart, T. Stockmanns, M. C. Stockton, M. Stodulski, K. Stoerig, G. Stoicea, S. Stonjek, P. Strachota, A. R. Stradling, A. Straessner, J. Strandberg, S. Strandberg, A. Strandlie, M. Strang, E. Strauss, M. Strauss, P. Strizenec, R. Ströhmer, D. M. Strom, J. A. Strong, R. Stroynowski, J. Strube, B. Stugu, I. Stumer, J. Stupak, P. Sturm, D. A. Soh, D. Su, S. Subramania, Y. Sugaya, T. Sugimoto, C. Suhr, K. Suita, M. Suk, V. V. Sulin, S. Sultansoy, T. Sumida, X. Sun, J. E. Sundermann, K. Suruliz, S. Sushkov, G. Susinno, M. R. Sutton, Y. Suzuki, Yu. M. Sviridov, S. Swedish, I. Sykora, T. Sykora, B. Szeless, J. Sánchez, D. Ta, K. Tackmann, A. Taffard, R. Tafirout, A. Taga, N. Taiblum, Y. Takahashi, H. Takai, R. Takashima, H. Takeda, T. Takeshita, M. Talby, A. Talyshev, M. C. Tamsett, J. Tanaka, R. Tanaka, S. Tanaka, Y. Tanaka, K. Tani, N. Tannoury, G. P. Tappern, S. Tapprogge, D. Tardif, S. Tarem, F. Tarrade, G. F. Tartarelli, P. Tas, M. Tasevsky, E. Tassi, M. Tatarkhanov, C. Taylor, F. E. Taylor, G. Taylor, G. N. Taylor, W. Taylor, M. Teixeira Dias Castanheira, P. Teixeira-Dias, K. K. Temming, H. Ten Kate, P. K. Teng, Y. D. Tennenbaum-Katan, S. Terada, K. Terashi, J. Terron, M. Terwort, M. Testa, R. J. Teuscher, C. M. Tevlin, J. Thadome, J. Therhaag, T. Theveneaux-Pelzer, M. Thioye, S. Thoma, J. P. Thomas, E. N. Thompson, P. D. Thompson, A. S. Thompson, E. Thomson, M. Thomson, R. P. Thun, T. Tic, V. O. Tikhomirov, Y. A. Tikhonov, C. J. W. P. Timmermans, P. Tipton, F. J. Tique Aires Viegas, S. Tisserant, J. Tobias, B. Toczek, T. Todorov, S. Todorova-Nova, B. Toggerson, J. Tojo, S. Tokár, K. Tokunaga, K. Tokushuku, K. Tollefson, M. Tomoto, L. Tompkins, K. Toms, A. Tonazzo, G. Tong, A. Tonoyan, C. Topfel, N. D. Topilin, I. Torchiani, E. Torrence, E. Torró Pastor, J. Toth, F. Touchard, D. R. Tovey, D. Traynor, T. Trefzger, J. Treis, L. Tremblet, A. Tricoli, I. M. Trigger, S. Trincaz-Duvoid, T. N. Trinh, M. F. Tripiana, N. Triplett, W. Trischuk, A. Trivedi, B. Trocmé, C. Troncon, M. Trottier-McDonald, A. Trzupek, C. Tsarouchas, J. C.-L. Tseng, M. Tsiakiris, P. V. Tsiareshka, D. Tsionou, G. Tsipolitis, V. Tsiskaridze, E. G. Tskhadadze, I. I. Tsukerman, V. Tsulaia, J.-W. Tsung, S. Tsuno, D. Tsybychev, A. Tua, J. M. Tuggle, M. Turala, D. Turecek, I. Turk Cakir, E. Turlay, P. M. Tuts, A. Tykhonov, M. Tylmad, M. Tyndel, D. Typaldos, H. Tyrvainen, G. Tzanakos, K. Uchida, I. Ueda, R. Ueno, M. Ugland, M. Uhlenbrock, M. Uhrmacher, F. Ukegawa, G. Unal, D. G. Underwood, A. Undrus, G. Unel, Y. Unno, D. Urbaniec, E. Urkovsky, P. Urquijo, P. Urrejola, G. Usai, M. Uslenghi, L. Vacavant, V. Vacek, B. Vachon, S. Vahsen, C. Valderanis, J. Valenta, P. Valente, S. Valentinetti, S. Valkar, E. Valladolid Gallego, S. Vallecorsa, J. A. Valls Ferrer, H. van der Graaf, E. van der Kraaij, E. van der Poel, D. van der Ster, B. Van Eijk, N. van Eldik, P. van Gemmeren, Z. van Kesteren, I. van Vulpen, W. Vandelli, G. Vandoni, A. Vaniachine, P. Vankov, F. Vannucci, F. VarelaRodriguez, R. Vari, E. W. Varnes, D. Varouchas, A. Vartapetian, K. E. Varvell, V. I. Vassilakopoulos, F. Vazeille, G. Vegni, J. J. Veillet, C. Vellidis, F. Veloso, R. Veness, S. Veneziano, A. Ventura, D. Ventura, S. Ventura, M. Venturi, N. Venturi, V. Vercesi, M. Verducci, W. Verkerke, J. C. Vermeulen, L. Vertogardov, A. Vest, M. C. Vetterli, I. Vichou, T. Vickey, G. H. A. Viehhauser, S. Viel, M. Villa, M. Villaplana Perez, E. Vilucchi, M. G. Vincter, E. Vinek, V. B. Vinogradov, M. Virchaux, S. Viret, J. Virzi, A. Vitale, O. Vitells, I. Vivarelli, F. Vives Vaque, S. Vlachos, M. Vlasak, N. Vlasov, A. Vogel, P. Vokac, M. Volpi, G. Volpini, H. von der Schmitt, J. von Loeben, H. von Radziewski, E. von Toerne, V. Vorobel, A. P. Vorobiev, V. Vorwerk, M. Vos, R. Voss, T. T. Voss, J. H. Vossebeld, A. S. Vovenko, N. Vranjes, M. Vranjes Milosavljevic, V. Vrba, M. Vreeswijk, T. Vu Anh, R. Vuillermet, I. Vukotic, W. Wagner, P. Wagner, H. Wahlen, J. Wakabayashi, J. Walbersloh, S. Walch, J. Walder, R. Walker, W. Walkowiak, R. Wall, P. Waller, C. Wang, H. Wang, J. Wang, J. C. Wang, S. M. Wang, A. Warburton, C. P. Ward, M. Warsinsky, P. M. Watkins, A. T. Watson, M. F. Watson, G. Watts, S. Watts, A. T. Waugh, B. M. Waugh, J. Weber, M. Weber, M. S. Weber, P. Weber, A. R. Weidberg, J. Weingarten, C. Weiser, H. Wellenstein, P. S. Wells, M. Wen, T. Wenaus, S. Wendler, Z. Weng, T. Wengler, S. Wenig, N. Wermes, M. Werner, P. Werner, M. Werth, M. Wessels, K. Whalen, S. J. Wheeler-Ellis, S. P. Whitaker, A. White, M. J. White, S. R. Whitehead, D. Whiteson, D. Whittington, F. Wicek, D. Wicke, F. J. Wickens, W. Wiedenmann, M. Wielers, P. Wienemann, C. Wiglesworth, L. A. M. Wiik, A. Wildauer, M. A. Wildt, I. Wilhelm, H. G. Wilkens, J. Z. Will, E. Williams, H. H. Williams, W. Willis, S. Willocq, J. A. Wilson, M. G. Wilson, A. Wilson, I. Wingerter-Seez, S. Winkelmann, F. Winklmeier, M. Wittgen, M. W. Wolter, H. Wolters, G. Wooden, B. K. Wosiek, J. Wotschack, M. J. Woudstra, K. Wraight, C. Wright, B. Wrona, S. L. Wu, X. Wu, Y. Wu, E. Wulf, R. Wunstorf, B. M. Wynne, L. Xaplanteris, S. Xella, S. Xie, Y. Xie, C. Xu, D. Xu, G. Xu, B. Yabsley, M. Yamada, A. Yamamoto, K. Yamamoto, S. Yamamoto, T. Yamamura, J. Yamaoka, T. Yamazaki, Y. Yamazaki, Z. Yan, H. Yang, S. Yang, U. K. Yang, Y. Yang, Z. Yang, S. Yanush, W.-M. Yao, Y. Yao, Y. Yasu, J. Ye, S. Ye, M. Yilmaz, R. Yoosoofmiya, K. Yorita, R. Yoshida, C. Young, S. Youssef, D. Yu, J. Yu, L. Yuan, A. Yurkewicz, V. G. Zaets, R. Zaidan, A. M. Zaitsev, Z. Zajacova, Yo. K. Zalite, L. Zanello, P. Zarzhitsky, A. Zaytsev, M. Zdrazil, C. Zeitnitz, M. Zeller, P. F. Zema, A. Zemla, C. Zendler, A. V. Zenin, O. Zenin, T. Ženiš, Z. Zenonos, S. Zenz, D. Zerwas, G. Zevi della Porta, Z. Zhan, D. Zhang, H. Zhang, J. Zhang, X. Zhang, Z. Zhang, L. Zhao, T. Zhao, Z. Zhao, A. Zhemchugov, S. Zheng, J. Zhong, B. Zhou, N. Zhou, Y. Zhou, C. G. Zhu, H. Zhu, Y. Zhu, X. Zhuang, V. Zhuravlov, D. Zieminska, B. Zilka, R. Zimmermann, S. Zimmermann, M. Ziolkowski, R. Zitoun, L. Živković, V. V. Zmouchko, G. Zobernig, A. Zoccoli, Y. Zolnierowski, A. Zsenei, M. zur Nedden, V. Zutshi, and L. Zwalinski

Subjects
Astrophysics, QB460-466, Nuclear and particle physics. Atomic energy. Radioactivity, QC770-798
Abstract

Abstract Measurements of luminosity obtained using the ATLAS detector during early running of the Large Hadron Collider (LHC) at $\sqrt{s} = 7$ TeV are presented. The luminosity is independently determined using several detectors and multiple algorithms, each having different acceptances, systematic uncertainties and sensitivity to background. The ratios of the luminosities obtained from these methods are monitored as a function of time and of μ, the average number of inelastic interactions per bunch crossing. Residual time- and μ-dependence between the methods is less than 2% for 0

Published
2011
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45. ChemInform Abstract: Compositional Studies of Thermally Nitrided Silicon Dioxide (Nitroxide)

Author

C. J. Han, Krishna C. Saraswat, Steven C. Shatas, Mehrdad M. Moslehi, and C. R. Helms

Subjects
chemistry.chemical_compound, Nitroxide mediated radical polymerization, Chemical engineering, Chemistry, Silicon dioxide, General Medicine, Nitriding
Abstract

Cinetique de la nitruration thermique de SiO 2 dans NH 3 . Structure multicouche des films d'oxyde nitrures formes

Published
1986

47. Activation Energy for the Parabolic Rate Constant during Sequential Si Oxidation

Author

C. J. Han and C. R. Helms

Subjects
Reaction rate constant, Materials science, Renewable Energy, Sustainability and the Environment, Kinetics, Materials Chemistry, Electrochemistry, Thermodynamics, Physical chemistry, Activation energy, Condensed Matter Physics, Surfaces, Coatings and Films, Electronic, Optical and Magnetic Materials
Abstract

On montre que les proprietes de transport de SiO 2 obtenues par croissance thermique, varient en fonction de la temperature. Il y a egalement une variation de l'indice de refraction, de la densite et de la tension interfaciale. Effet anormal de la temperature sur l'energie d'activation

Published
1985

49. High-dose stereotactic body radiotherapy improve local control and overall survival in patients with inoperable hepatocellular carcinoma.

Author

W. I. Jang, M. S. Kim, H. J. Yoo, S. H. Bae, D. H. Lee, S. Y. Kim, C. J. Han, J. Kim, S. C. Park, S. B. Kim, and E. H. Cho

Subjects
STEREOTACTIC radiotherapy, STEREOTACTIC radiosurgery, LIVER cancer, THERAPEUTIC embolization, CANCER prognosis
Abstract

Purpose: The purpose of this study is to determine whether a dose-response relationship in stereotactic body radiotherapy (SBRT) for hepatocellular carcinoma (HCC) is observed and to identify whether local control or response affects survival outcome. Methods: Between March 2003 and February 2011, 108 patients with 122 lesions were treated with SBRT for HCC. The indications for SBRT were unsuitable for surgery or other ablative therapies and incomplete response of transarterial chemoembolization (TACE). The inclusion criteria of this study are SBRT using 3 fractions and longest diameter ≤ 7.0 cm. Eighty-two patients with 95 lesions were analyzed. Median age was 60 years (range, 39-79 years). Seventy-four patients (90%) had Child-Pugh class A and 8 patients had B7. All patients had one or more TACE and the median number of TACE sessions per patient was 2 (range, 1-14). The median longest diameter was 3.0 cm (range, 1.0-7.0 cm). The median SBRT dose was 51 Gy (range, 33-60 Gy). Results: The median follow-up duration for all analyzed patients was 30 months (range, 4-81 months). Local control and overall survival rates at 2 years after SBRT were 87% and 63%, respectively. The 2-year local control rates for lesions treated with SBRT doses of >54 Gy, 45-54 Gy, and <45 Gy were 100%, 78%, and 64%, respectively (p=0.0087). In multivariate analysis, SBRT dose and age were significant prognostic factors for local control. The 2-year overall survival rates for patients with and without local failure were 27% and 68%, respectively (p=0.0001). In multivariate analysis, SBRT dose and Barcelona Clinic Liver Cancer stage were significant prognostic factors for overall survival. Five patients (6%) experienced grade 3 or higher gastrointestinal toxicity. The estimated SBRT dose to achieve 90% LC at 2 years is 54 Gy in 3 fractions. In selected patients with SBRT dose > 54 Gy and longest diameter ≤ 5.0 cm, the treatment outcomes of SBRT were comparable with those of radiofrequency ablation (RFA). Conclusions: The present study strongly suggests a dose-response relationship in SBRT for HCC. Excellent local control rates are achieved with SBRT dose of more than 54 Gy or greater. Higher local control rates resulted from increasing dose may be survival benefit for inoperable HCC. We suggest SBRT dose of more than 54 Gy, if normal tissue constraints allow. In the patients with small-sized HCC, high-dose SBRT may be as effective and safe treatment modality as RFA. Disclosure: No significant relationships. [ABSTRACT FROM AUTHOR]

Published
2013

50. The hindgut microbiota of coconut rhinoceros beetles ( Oryctes rhinoceros ) in relation to their geographical populations.

Author

Han C-J, Huang J-P, Chiang M-R, Jean OSM, Nand N, Etebari K, and Shelomi M

Subjects
Animals, Bacteria classification, Bacteria genetics, Bacteria isolation & purification, Cocos microbiology, Genetic Variation, Coleoptera microbiology, Gastrointestinal Microbiome, Symbiosis
Abstract

The coconut rhinoceros beetle (CRB, Oryctes rhinoceros ) is a palm tree pest capable of rapidly expanding its population in new territories. Previous studies identified a digestive symbiosis between CRB and its gut microbes. However, no research compared the genetic variation of CRBs with their hindgut microbiota on a global scale. This study aims to investigate the genetic divergence of CRB and the compositional variation of CRB's microbiota across different geographical locations, and explore the association between them and their predicted functional profiles and environmental data. The research reveals a distinct and consistent microbial community within local populations, but it varies across different geographical populations. The microbial functional profiles linked to the production of digestive enzymes, including cellulases and ligninases, are nonetheless globally conserved. This suggests that CRBs employ specific mechanisms to select and maintain microbes with functional benefits, contributing to host adaptability, stress tolerance, and fitness. The CRB microbial communities did not appear to recapitulate the genetic variation of their hosts. Rather than depend on obligate symbionts, CRBs seem to establish similar digestive associations with whatever environmentally acquired microbes are available wherever they are, aiding them in successfully establishing after invading a new location.IMPORTANCECoconut rhinoceros beetles (CRBs) are notorious pests on Arecaceae plants, posing destructive threats to countries highly reliant on coconut, oil palm, and date palm as economic crops. In the last century, CRBs have rapidly expanded their presence to territories that were once free of these beetles. The United States, for instance, has officially designated CRBs as invasive and alien pests. Given their remarkable ability to swiftly adapt to new environments, their gut microbes may play a crucial role in this process. While the microbiota of CRBs vary depending on geographical location, these beetles consistently exhibit a functionally identical digestive association with locally acquired microbes. This underscores the significance of CRB-microbe association in shaping the adaptive strategies of this agricultural pest., Competing Interests: The authors declare no conflict of interest.

Published
2024
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