Descriptor: "Charge ratio" - Searchworks@Jio Institute Digital Library Search Results

74 results on '"Charge ratio"'

1. Influence of the Charge Ratio of Guanine-Quadruplex Structure-Based CpG Oligodeoxynucleotides and Cationic DOTAP Liposomes on Cytokine Induction Profiles.

Author: Le, Nguyen Bui Thao, Tu, Anh Thi Tram, Zhao, Dandan, Yoshikawa, Chiaki, Kawakami, Kohsaku, Kaizuka, Yoshihisa, and Yamazaki, Tomohiko
Subjects: *CATIONIC lipids, *CPG nucleotides, *MONONUCLEAR leukocytes, *CYTOKINES, *LIPOSOMES, *SURFACE charges, *QUADRUPLEX nucleic acids
Abstract: Cationic liposomes, specifically 1,2-dioleoyl-3-trimethylammonium-propane (DOTAP) liposomes, serve as successful carriers for guanine-quadruplex (G4) structure-based cytosine-guanine oligodeoxynucleotides (CpG ODNs). The combined benefits of CpG ODNs forming a G4 structure and a non-viral vector carrier endow the ensuing complex with promising adjuvant properties. Although G4-CpG ODN-DOTAP complexes show a higher immunostimulatory effect than naked G4-CpG ODNs, the effects of the complex composition, especially charge ratios, on the production of the pro-inflammatory cytokines interleukin (IL)-6 and interferon (IFN)-α remain unclear. Here, we examined whether charge ratios drive the bifurcation of cytokine inductions in human peripheral blood mononuclear cells. Linear CpG ODN-DOTAP liposome complexes formed micrometer-sized positively charged agglomerates; G4-CpG ODN-DOTAP liposome complexes with low charge ratios (0.5 and 1.5) formed ~250 nm-sized negatively charged complexes. Notably, low-charge-ratio (0.5 and 1.5) complexes induced significantly higher IL-6 and IFN-α levels simultaneously than high-charge-ratio (2 and 2.5) complexes. Moreover, confocal microscopy indicated a positive correlation between the cellular uptake of the complex and amount of cytokine induced. The observed effects of charge ratios on complex size, surface charge, and affinity for factors that modify cellular-uptake, intracellular-activity, and cytokine-production efficiency highlight the importance of a rational complex design for delivering and controlling G4-CpG ODN activity. [ABSTRACT FROM AUTHOR]
Published: 2023
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2. Pelletizing analysis of cylinder pelletizer on MgO-fluxed pellets by discrete element method (DEM)

Author: F. Yang, Zh. Tong, Sh. W. Zou, Zh. Y. Li, and Z. J. Shen
Subjects: blast furnace, pellet, cylinder pelletizer, discrete element method, charge ratio, Mining engineering. Metallurgy, TN1-997
Abstract: Discrete Element Method (DEM) was used to analyze palletization process of MgO-fluxed pellets in cylinder pelletizer. The effects of the charge ratio and rotational speed of the cylinder pelletizer on the behavior of MgO-fluxed pellets were investigated by using the simulation. The simulation results show that under the condition of a certain gradient angle of the cylinder pelletizer (The gradient angle is 3°), the suitable parameters of the cylinder pelletizer are that the charge ratio is 3 % and the rotational speed N/ critical rotational speed NC is 0,3.
Published: 2023

3. Insight into the Charge-Ratio-Tuned Solar Vapor Generation of Polyion Complex Hydrogel/Coal Powder Composites.

Author: Ji, Zhiteng, Zhao, Jianhang, Feng, Shanhao, Zhu, Fengbo, Yu, Wenwen, Ye, Yanan, and Zheng, Qiang
Subjects: *ELECTROLYTE solutions, *POLYIONS, *ARTIFICIAL seawater, *WATER purification, *VAPORS, *SALINE water conversion, *HYDROGELS, *CHEMICAL purification, *THERMAL coal
Abstract: Solar-driven water purification has been deemed a promising technology to address the issue of clean water scarcity. However, traditional solar distillers often suffer from low evaporation rates under natural sunlight irradiation, while the high costs of the fabrication of photothermal materials further hinders their practical applications. Here, through the harnessing of the complexation process of oppositely charged polyelectrolyte solutions, a polyion complex hydrogel/coal powder composite (HCC)-based highly efficient solar distiller is reported. In particular, the influence of the charge ratio of polyanion-to-polycation on the solar vapor generation performance of HCC has been systematically investigated. Together with a scanning electron microscope (SEM) and the Raman spectrum method, it is found that a deviation from the charge balance point not only alters the microporous structure of HCC and weakens its water transporting capabilities, but also leads to a decreased content of activated water molecules and enlarges the energy barrier of water evaporation. As a result, HCC prepared at the charge balance point exhibits the highest evaporation rate of 3.12 kg m−2 h−1 under one sun irradiation, with a solar–vapor conversion efficiency as high as 88.83%. HCC also exhibits remarkable solar vapor generation (SVG) performance for the purification of various water bodies. In simulated seawater (3.5 wt% NaCl solutions), the evaporation rate can be as high as 3.22 kg m−2 h−1. In acid and alkaline solutions, HCCs are capable of maintaining high evaporation rates of 2.98 and 2.85 kg m−2 h−1, respectively. It is anticipated that this study may provide insights for the design of low-cost next-generation solar evaporators, and broaden the practical applications of SVG for seawater desalination and industrial wastewater purification. [ABSTRACT FROM AUTHOR]
Published: 2023
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4. Analysis of factors influencing infrared extinction area of explosive smokescreen

Author: Haihao He, Youlin Gu, Jiajie Fang, Yihua Hu, Hao Cao, Wanying Ding, Xinyu Wang, and Xi Chen
Subjects: Smokescreen, Smoothed particle hydrodynamics, Charge ratio, Blast radius, Infrared extinction area, Science (General), Q1-390, Social sciences (General), H1-99
Abstract: Objectives: Comparative studies of different smokescreen designs are essential to determine differences in extinction performance. This study aims to investigate the extinction performance of explosive smokescreen under different conditions, and to provide an evaluation method for the optimal design of its charge structure. Methods: The process of formation of the smokescreen with a cylindrical charge structure is described based on the smoothed particle hydrodynamics method. The blast radius and particle density distribution of the smokescreen were calculated for different charge structures and charge ratios through simulations. Lambert–Beer's law was combined to obtain the infrared extinction area. An analysis was then conducted to determine the influence of the number of baffles in the charge structure and charge ratio on the extinction performance of the smokescreen. Field tests were conducted to verify the simulation results. Results: Increasing the number of baffles in the projectile structure made the particle distribution of the smokescreen more uniform and resulted in a larger infrared extinction area. An increase in the explosive quantity, made the smokescreen more dispersed. However, too much of the explosives caused the smokescreen to be sparse, reducing the infrared extinction area.
Published: 2022
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5. PELLETIZING ANALYSIS OF CYLINDER PELLETIZER ON MgO-FLUXED PELLETS BY DISCRETE ELEMENT METHOD (DEM).

Author: YANG, F., TONG, Z. H., ZOU, S. H. W., LI, Z. H. Y., and SHEN, Z. J.
Subjects: *PELLETIZING, *DISCRETE element method
Abstract: Discrete Element Method (DEM) was used to analyze palletization process of MgO-fluxed pellets in cylinder pelletizer. The effects of the charge ratio and rotational speed of the cylinder pelletizer on the behavior of MgO-fluxed pellets were investigated by using the simulation. The simulation results show that under the condition of a certain gradient angle of the cylinder pelletizer (The gradient angle is 3°), the suitable parameters of the cylinder pelletizer are that the charge ratio is 3 % and the rotational speed N/critical rotational speed NC is 0,3. [ABSTRACT FROM AUTHOR]
Published: 2023

6. Isothermal Performance of Heat Pipes: A Review.

Author: Zhang, Hongzhe, Ye, Fang, Guo, Hang, and Yan, Xiaoke
Subjects: *HEAT pipes, *HEAT transfer, *LATENT heat, *WORKING fluids, *PHASE transitions, *DEBYE temperatures
Abstract: Heat pipes transfer heat via phase transformation of the working fluid, where the working fluid will keep the temperature constant and absorb or release a large amount of latent heat during phase transformation. With the development of heat pipe technology, the isothermal performance of heat pipes has been gradually emphasized in many application fields. Most studies focused on the average temperature characteristics of one heat pipe or several heat pipes with the same type, and lacked a comprehensive analysis on the isothermal performance of different heat pipes. In this paper, previous studies on the application fields of the isothermal performance of heat pipes, the isothermal level of heat pipes used in different fields, and the methods to improve the isothermal performance of heat pipes are summarized. The parameters of the wick have little effect on the temperature uniformity of the heat pipe, while the arrangement of the wick has more influence on the uniformity of the heat pipe. The most suitable charge rate is 15% to 30% of the total inner volume, and the best start-up performance and isothermal performance is at approximately 45°. [ABSTRACT FROM AUTHOR]
Published: 2022
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7. 云南金平长安金矿中深孔凿岩爆破参数优化研究.

Author: 周宗红, 刘剑, 许敏捷, 刘永文, and 高旭辉
Abstract: Copyright of Industrial Minerals & Processing / Huagong Kuangwu yu Jiagong is the property of Industrial Minerals & Processing Editorial Office and its content may not be copied or emailed to multiple sites or posted to a listserv without the copyright holder's express written permission. However, users may print, download, or email articles for individual use. This abstract may be abridged. No warranty is given about the accuracy of the copy. Users should refer to the original published version of the material for the full abstract. (Copyright applies to all Abstracts.)
Published: 2021
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8. Pelletizing Analysis on MgO-Fluxed Pellets by DEM

Author: Fang Long, Fengman Shen, Xin Jiang, Fu Yang, Yulu Zhou, and Haiwei An
Subjects: MgO-fluxed pellets, disc pelletizer, discrete element method, charge ratio, rotational speed, Crystallography, QD901-999
Abstract: The Discrete Element Method (DEM) was used to analyze the pelletization process of MgO-fluxed pellets. The effects of the charge ratio and rotational speed of the disc pelletizer on the behavior of MgO-fluxed pellets were investigated by using a simulation. The simulation results show that under the condition of a certain tilt angle of the disc pelletizer (the tilt angle is 49°), the suitable parameters of the disc pelletizer are that the charge ratio is 20% and the rotational speedis 0.7 N/NC. This simulation model proposed will be useful to research pellets behavior and for the design of disc pelletizers.
Published: 2021
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9. Thermodynamic mechanism of particulation of sodium alginate and chitosan polyelectrolyte complexes as a function of charge ratio and order of addition.

Author: Yilmaz, Tuncay, Maldonado, Luis, Turasan, Hazal, and Kokini, Jozef
Subjects: *SODIUM alginate, *ISOTHERMAL titration calorimetry, *PARTICLE size distribution, *COMPLEXATION reactions, *ZETA potential, *BINDING constant
Abstract: Abstract This study focused on mechanistic understanding of the effect of charge ratio, order of addition and resulting thermodynamics of interaction on the formation and properties of polyelectrolyte complexes (PECs) from sodium alginate and chitosan at a constant tightly controlled pH 4 where the zeta potential difference was maximum for the formation of PECs. The morphology, particle size and particle size distribution as well as the stability of PECs were investigated as a function of molar charge ratio, and the order of addition. The association binding constant K a and the stoichiometry of interaction between the two electrolytes, evaluated using Isothermal titration calorimetry, showed that the stoichiometry and enthalpy of reactions were strongly affected by the order of addition and influenced the average particle size and zeta potential of PECs. The addition of alginate (-) into chitosan (+) gave positively charged particles and resulted in stronger interactions characterized by larger enthalpy and entropy of complexation which led to smaller particles. Reversing the order of addition gave negatively charged particles that were larger. Morphologies of complexes studied using scanning electron microscopy (SEM) showed distorted spherical particles for both orders of addition and at most charge ratios. Stability during 8 weeks was found to depend on the order of addition and charge ratio. Alginate in chitosan gave more stable PECs consistent with the thermodynamics of interaction which showed stronger interactions for this order of addition. The particle sizes and size distributions rapidly increased near electrical neutrality during storage at 4 °C where aggregation was facilitated because of electrical neutrality but particles were stable when the net charge was either strongly positive or strongly negative. Highlights • CHI (chitosan) and ALG (sodium alginate) spontaneously form PECs. • Order of addition and charge ratio control the particle size and charge. • PECs are positive when ALG is added to CHI and negative when CHI is added to ALG. • ΔH and ΔS of the complexation reactions explained the organization of particles. • The stability of the PECs followed similar thermodynamic rules. [ABSTRACT FROM AUTHOR]
Published: 2019
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10. Free Energy Perturbation Monte Carlo Simulations of Salt Influences on Aqueous Freezing Point Depression

Author: Dick, Thomas J., Wierzbicki, Andrzej, Madura, Jeffry D., Leszczynski, Jerzy, editor, and Shukla, Manoj K., editor
Published: 2010
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11. Neutralization of negative charges of siRNA results in improved safety and efficient gene silencing activity of lipid nanoparticles loaded with high levels of siRNA.

Author: Sato, Yusuke, Matsui, Hideki, Sato, Risa, and Harashima, Hideyoshi
Subjects: *NANOMEDICINE, *SMALL interfering RNA, *GENE silencing, *MEDICATION safety, *ENDOSOMES
Abstract: Lipid nanoparticles (LNPs) are one of the leading technologies for the in vivo delivery of short interfering RNA (siRNA). Cationic lipids are an important component for efficient endosomal escape via membrane fusion followed by release of siRNAs in cytosol where the site of action is located. A high cationic lipid/siRNA charge ratio is usually necessary for maximizing the gene silencing activity of the siRNA-loaded LNPs. However, high levels of cationic lipids are known to cause cytotoxicity through interactions with negatively charged biocomponents. A strategy for solving this dilemma is important, in terms of producing clinically applicable LNPs with a wide therapeutic window. We herein report on the development of LNPs with a high gene silencing activity and a low cationic lipid/siRNA charge ratio, which we refer to as low lipid core-nanoparticles (LLC-NPs). The negative charges of the siRNAs were neutralized by protamines, cationic proteins, to reduce the net dose of cationic lipid, YSK05, which was developed in our laboratory, for endosomal escape, resulting in preserved fusogenic activity and gene silencing activity, both in vitro and in vivo factor VII mouse model. In addition, the LLC-NPs showed an improved hepatotoxicity compared to conventional LNPs, which have a relatively higher cationic lipid/siRNA charge ratio. The concept of the LLC-NPs helps to realize clinically applicable LNPs with a wide therapeutic window and has the potential for use in various applications and for the delivery of different classes of nucleic acid. [ABSTRACT FROM AUTHOR]
Published: 2018
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12. Supramolecular Complexes of DNA

Author: Zuber, G., Scherman, D., Boisseau, Patrick, editor, Houdy, Philippe, editor, and Lahmani, Marcel, editor
Published: 2009
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13. In Vivo Gene Transfer by Ligand-Modified Gene Carriers

Author: Kawakami, Shigeru, Hashida, Mitsuru, Taira, Kazunari, editor, Kataoka, Kazunori, editor, and Niidome, Takuro, editor
Published: 2005
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14. Improved Online Algorithms for Buffer Management in QoS Switches

Author: Chrobak, Marek, Jawor, Wojciech, Sgall, Jiří, Tichý, Tomáš, Hutchison, David, editor, Kanade, Takeo, editor, Kittler, Josef, editor, Kleinberg, Jon M., editor, Mattern, Friedemann, editor, Mitchell, John C., editor, Naor, Moni, editor, Nierstrasz, Oscar, editor, Pandu Rangan, C., editor, Steffen, Bernhard, editor, Sudan, Madhu, editor, Terzopoulos, Demetri, editor, Tygar, Dough, editor, Vardi, Moshe Y., editor, Weikum, Gerhard, editor, Albers, Susanne, editor, and Radzik, Tomasz, editor
Published: 2004
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15. Cationic Lipid-Nucleic Acid Complexes (Lipoplexes): From Physicochemical Properties to In Vitro and In Vivo Transfection Kits

Author: Simberg, Dmitri, Hirsch-Lerner, Danielle, Zuidam, Nicolaas-Jan, Even-Chen, Simcha, Kerner, Miryam, Eliyahu, Hagit, Servel, Natalie, Weisman, Sarah, Plis-Finarov, Alla, Talmon, Yeshayahu, Barenholz, Yechezkel, and Schneider, Manfred P., editor
Published: 2003
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16. L3+Cosmics: an atmospheric muon experiment at CERN

Author: L3 Collaboration, Chiarusi, Tommaso, Shapiro, Maurice M., editor, Stanev, Todor, editor, and Wefel, John P., editor
Published: 2001
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17. Theory and Practice of Using Polycationic Amphiphiles and polymers for In Vitro and In Vivo Gene Transfer

Author: Demeneix, B. A., Goula, D., Benoist, C., Rémy, J. S., Behr, J. P., and Xanthopoulos, Kleanthis G., editor
Published: 1998
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18. Complement Activation by Polylysine-DNA Complexes

Author: Plank, C., Mechtler, K., Wagner, E., Szoka, F. C., Jr., Gregoriadis, Gregory, editor, and McCormack, Brenda, editor
Published: 1996
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19. Precipitation of Proteins with Polyelectrolytes: Role of Polymer Molecular Weight

Author: Shieh, Jang-you, Glatz, Charles E., Dubin, Paul, editor, Bock, J., editor, Davis, Richie, editor, Schulz, Donald N., editor, and Thies, Curt, editor
Published: 1994
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20. Understanding the Novolak Synthesis Reaction

Author: Bogan, Leonard E., Jr. and Prasad, Paras N., editor
Published: 1994
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21. Importance of the Crystallization of Minor Elements on the Cooling History of White Dwarfs

Author: Chabrier, G., Segretain, L., Hernanz, M., Isern, J., Mochkovitch, R., and Barstow, Martin A., editor
Published: 1993
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22. Asymptotic Neutrality of Polyatomic Molecules

Author: Ruskai, Mary Beth, Solovej, Jan Philip, Beiglböck, W., editor, and Balslev, Erik, editor
Published: 1992
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23. Effect of ball size on steady state of aluminum powder and efficiency of impacts during milling.

Author: Razavi-Tousi, S.S. and Szpunar, J.A.
Subjects: *ALUMINUM powder, *METAL powders, *MILLING (Metalwork), *ALUMINUM silicates, *CRYSTALLOGRAPHIC shear
Abstract: The concept of steady state milling time was examined for ball milling of aluminum powder. Four different set-ups of balls were used while the mill speed and charge ratio were kept fixed. Different criteria (morphology of particles, average particle size, deviation from the average particle size, lattice imperfections and change in crystallographic orientation) were used to study structural evolution of the milled particles and to compare the steady state time for the different milling conditions. Results showed that different criteria may not determine the same steady state time, however, all criteria were consistent in comparing efficiency of the different milling conditions. Moreover, it was found that at a given mill speed and ball to powder ratio (i.e. at a given consumed energy), a change in balls size and filling ratio of vials can improve milling efficiency. Finally, the effect of energy of each impact and the collective energy of all impacts were discussed. [ABSTRACT FROM AUTHOR]
Published: 2015
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24. New Degradable Cationic Peptides for Modulated Gene Delivery

Author: Mirkin, Fiana, Eini, Hadar, Douvdevani, Amos, Byk, Gerardo, Valle, Susan Del, editor, Escher, Emanuel, editor, and Lubell, William D., editor
Published: 2009
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25. Neutralization of negative charges of siRNA results in improved safety and efficient gene silencing activity of lipid nanoparticles loaded with high levels of siRNA

Author: Hideki Matsui, Risa Sato, Yusuke Sato, and Hideyoshi Harashima
Subjects: 0301 basic medicine, Small interfering RNA, Short interfering RNA, Pharmaceutical Science, 02 engineering and technology, Charge ratio, 03 medical and health sciences, In vivo, Gene silencing, Animals, Humans, RNA, Small Interfering, Cytotoxicity, Drug Carriers, Mice, Inbred ICR, biology, Chemistry, Cationic polymerization, Lipid bilayer fusion, 021001 nanoscience & nanotechnology, HCT116 Cells, Protamine, Lipids, 030104 developmental biology, biology.protein, Nucleic acid, Biophysics, Lipid nanoparticles, Nanoparticles, Female, RNA Interference, 0210 nano-technology, Therapeutic window, HeLa Cells
Abstract: Lipid nanoparticles (LNPs) are one of the leading technologies for the in vivo delivery of short interfering RNA (siRNA). Cationic lipids are an important component for efficient endosomal escape via membrane fusion followed by release of siRNAs in cytosol where the site of action is located. A high cationic lipid/siRNA charge ratio is usually necessary for maximizing the gene silencing activity of the siRNA-loaded LNPs. However, high levels of cationic lipids are known to cause cytotoxicity through interactions with negatively charged biocomponents. A strategy for solving this dilemma is important, in terms of producing clinically applicable LNPs with a wide therapeutic window. We herein report on the development of LNPs with a high gene silencing activity and a low cationic lipid/siRNA charge ratio, which we refer to as low lipid core-nanoparticles (LLC-NPs). The negative charges of the siRNAs were neutralized by protamines, cationic proteins, to reduce the net dose of cationic lipid, YSK05, which was developed in our laboratory, for endosomal escape, resulting in preserved fusogenic activity and gene silencing activity, both in vitro and in vivo factor VII mouse model. In addition, the LLC-NPs showed an improved hepatotoxicity compared to conventional LNPs, which have a relatively higher cationic lipid/siRNA charge ratio. The concept of the LLC-NPs helps to realize clinically applicable LNPs with a wide therapeutic window and has the potential for use in various applications and for the delivery of different classes of nucleic acid.
Published: 2018

26. Return adjusted charge ratios: What drives fees and costs of pension schemes?

Author: Lučivjanská, Katarína, Lyócsa, Štefan, Radvanský, Marek, and Širaňová, Mária
Abstract: We study the expensiveness of pension schemes across a set of developed and developing countries. To calculate the difference between accumulated savings with and without fees and costs, we construct return optimized charge ratio. We estimate charge ratios for 51 pension schemes and study which of the 40 potential factors can explain heterogeneity by the Bayesian model averaging framework. The most favorable fee structure can be characterized by the use of performance fees at the expense of more costly asset under management fees. The inflation rate, size and development of the economy tend to be priced into charge ratios. • We propose return adjusted charge ratios (RACR) for estimating pension fund's costs. • The (RACR) is estimated for 51 pension schemes across multiple countries. • Most favorable structure uses performance fees, least asset under management fees. • Bayesian Model Averaging explores large set of potential drivers. • More developed economies with lower inflation seem to have lowest pension costs. [ABSTRACT FROM AUTHOR]
Published: 2022
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27. Systematic Solid Phase Synthesis of Linear Pseudooligolysines Containing Multiple Adjacent CH2NH Amide Bond Surrogates: Potential Agents for Gene Delivery

Author: Fridkin, Gil, Gilon, Tamar, Loyter, Abrahm, Gilon, Chaim, Lebl, Michal, editor, and Houghten, Richard A., editor
Published: 2001
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28. Spectrum and charge ratio of vertical cosmic ray muons up to momenta of 2.5 TeV/c.

Author: Schmelling, M., Hashim, N.O., Grupen, C., Luitz, S., Maciuc, F., Mailov, A., Müller, A.-S., Sander, H.-G., Schmeling, S., Tcaciuc, R., Wachsmuth, H., Ziegler, T., and Zuber, K.
Subjects: *COSMIC ray muons, *MOMENTUM spectra, *ELECTRIC charge, *COMPARATIVE studies, *MONTE Carlo method
Abstract: Highlights: [•] The ALEPH detector at LEP is used to measure cosmic ray muons. [•] Momentum spectrum and charge ratio of vertical muons at surface level are determined. [•] Results are compared to and interpreted by Monte Carlo models. [•] Information about energy spectrum and chemical composition of cosmic ray primaries is inferred. [ABSTRACT FROM AUTHOR]
Published: 2013
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29. Design, fabrication and performance tests for a polymer-based flexible flat heat pipe.

Author: Hsieh, Shou-Shing and Yang, Ya-Ru
Subjects: *HEAT pipes, *FABRICATION (Manufacturing), *POLYMERS, *BENDING (Metalwork), *DEIONIZATION of water, *WORK environment, *ENERGY conversion, *ENERGY management, *PIPE design & construction
Abstract: Abstract: In this paper, we report on the novel design, fabrication and performance tests for a polymer-based flexible flat heat pipe (FHP) with a bending angle in the range of 15–90°. Each heat pipe is 4mm thick, 20mm wide and 80mm long, with two layers of No. 250 copper mesh as the wicking material. A copper/silicone rubber hybrid structure is designed and fabricated to achieve the flexibility of the heat pipe. Thermal characteristics are measured and studied for de-ionized water under different working conditions. Experimental results reveal that a bending angle of 15° on the vertical plane has a better thermal performance than those of heat pipes with/without bending. In addition, a higher power of 12.67W can be transferred/delivered. [Copyright &y& Elsevier]
Published: 2013
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30. A novel design of pulsating heat pipe with fewer turns applicable to all orientations

Author: Chien, Kuo-Hsiang, Lin, Yur-Tsai, Chen, Yi-Rong, Yang, Kai-Shing, and Wang, Chi-Chuan
Subjects: *HEAT pipes, *OSCILLATIONS, *FUNCTIONAL analysis, *CAPILLARY tubes, *CROSS-sectional method, *PERFORMANCE evaluation, *THERMAL resistance
Abstract: Abstract: This study presents a novel pulsating heat pipe (PHP) concept that is functional even when PHP is with fewer turns and is operated horizontally. Two heat pipes were made of copper capillary tubes with an overall size of 122mm×57mm×5.5mm is investigated, one had 16 parallel square channels having a uniform cross-section of 2mm×2mm (uniform CLPHP), and the other had 16 alternative size of parallel square channels (non-uniform CLPHP; a cross-section 2mm×2mm and a cross-section of 1mm×2mm in alternating sequence). Test results showed that the performance of PHP rises with the inclination but the uniform channel CLPHP is not functional at horizontal configuration whereas the proposed non-uniform design is still functional even at horizontal arrangement. The thermal resistance for uniform PHP is relative insensitive to change of inclination when the inclination angle exceeds certain threshold value. [Copyright &y& Elsevier]
Published: 2012
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31. N-Diethylmethyl chitosan for gene delivery to pancreatic cancer cells and the relation between charge ratio and biologic properties of polyplexes via interpolations polynomial

Author: Safari, S., Dorkoosh, F.A., Soleimani, M., Zarrintan, M.H., Akbari, H., Larijani, B., and Tehrani, M. Rafiee
Subjects: *CHITOSAN, *PANCREATIC cancer, *CANCER cells, *INTERPOLATION, *POLYNOMIALS, *GENETIC vectors, *GENE transfection, *GENE therapy
Abstract: Abstract: In gene therapy of pancreatic cancer, non-viral vectors show an important role. These vectors are modified with the aim of improvement for pancreatic cancer gene therapy. For this aim, we used N,N-diethyl N-methyl chitosan (DEMC) for gene delivery to human pancreatic cancer cells (AsPC-1). pEGFP (Enhanced green fluorescent protein plasmid) was used as a model plasmid. In order to evaluate the efficiency of this polymer for gene delivery, the DEMC/pEGFP complexes are characterized via photon correlation spectroscopy, gel electrophoresis, fluorescence microscopy, flow cytometry and MTT assay. Also cancer cells’ mean fluorescence intensity (MFI) and size changes after transfection are evaluated. The enhancement in polyplexes’ charge ratios from 5 to 40, results in 16.70-fold increase in transfection efficiency. Higher MFI, cell size and cytotoxicity were observed as the N/P ratio increased. Considering that mathematical models can be used to understand and predict consequences associated with nanomedicine, the relation between DEMC/pDNA complexes charge ratio, cell transfection and toxicity was evaluated for the first time with Lagrange''s interpolation polynomial method. [Copyright &y& Elsevier]
Published: 2011
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32. Measurement of the charge ratio of atmospheric muons with the CMS detector

Author: Khachatryan, V.
Subjects: *SOLENOIDS, *MUONS, *ELECTRIC charge, *LARGE Hadron Collider, *COSMIC ray showers, *ANGULAR momentum (Nuclear physics)
Abstract: Abstract: We present a measurement of the ratio of positive to negative muon fluxes from cosmic ray interactions in the atmosphere, using data collected by the CMS detector both at ground level and in the underground experimental cavern at the CERN LHC. Muons were detected in the momentum range from 5 GeV/c to 1 TeV/c. The surface flux ratio is measured to be , independent of the muon momentum, below 100 GeV/c. This is the most precise measurement to date. At higher momenta the data are consistent with an increase of the charge ratio, in agreement with cosmic ray shower models and compatible with previous measurements by deep-underground experiments. [ABSTRACT FROM AUTHOR]
Published: 2010
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33. Designing chitosan-dextran sulfate nanoparticles using charge ratios.

Author: Chen, Yan, Mohanraj, Vellore, Wang, Fang, and Benson, Heather
Abstract: The purpose of this study was to examine the effect of charge ratio on the formation and properties of the chitosan (CS)-dextran sulfate (DS) nanoparticles developed for the delivery of water-soluble small and large molecules, including proteins. Rhodamine 6G (R6G) and bovine serum albumin (BSA) were chosen as model molecules. CS-DS nanoparticles were formulated by a complex coacervation process under mild conditions. The influence of formulation and process variables, including the charge ratio of the 2 ionic polymers, on particle size, zeta potential, and nanoparticle entrapment of R6G and BSA was studied. The in vitro release of R6G and BSA was also evaluated, and the integrity of BSA in the release fraction was assessed using sodium dodecyl sulfate-polyacrylamide gel electrophoresis. Depending on the concentration and charge ratio of DS and CS, nanoparticles with varied size (≥244 nm) and zeta potential (−47.1-60mV) were obtained. High entrapment efficiency (98%) was achieved for both R6G and BSA when the charge ratio of the 2 ionic polymers was greater than 1.12. The release of both R6G and BSA from nanoparticles was based on the ion-exchange mechanism. BSA showed much slower continuous release for up to 7 days while still maintaining its integrity for an extended period. The CS-DS nanoparticles developed based on the modulation of charge ratio show promise as a system for controlled delivery of both small and large molecules, including proteins. [ABSTRACT FROM AUTHOR]
Published: 2007
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34. Charge ratio analysis method to interpret high resolution electrospray Fourier transform—ion cyclotron resonance mass spectra

Author: Maleknia, Simin D. and Downard, Kevin M.
Subjects: *ELECTROSPRAY ionization mass spectrometry, *FOURIER transform infrared spectroscopy, *CYCLOTRONS, *PARTICLE accelerators
Abstract: Abstract: The charge ratio analysis method (CRAM) is a new approach for the interpretation of high resolution Fourier transform ion cyclotron resonance (FT-ICR) electrospray mass spectral data. The high resolution capability of FT-MS provides resolved isotopic peaks of multiply charged ions of biopolymers enabling their accurate and monoisotopic molecular mass determination. It does, however, require that the correct charge and isotope composition of these ions be assigned in order for this accuracy to be realized. The unique feature of the CRAM in processing the FT-ICR data is that the charge states of ions are identified from analysis of the ratios of m/z values of isotopic peaks of different multiply charged ions. In addition, the CRAM process correlates the isotopic peaks of different multiply charged ions that share the same isotopic composition. As the size of biopolymers increases, their isotope patterns become more uniform and more difficult to discern from one another. This impacts on the correct matching of a theoretical isotope distribution to experimental data particularly in the case of biopolymers of unknown elemental compositions. The significance of the CRAM is demonstrated in terms of correlating theoretical isotopic distributions to experimental data where this correlation could not always be achieved based on the relative intensities of isotopic peaks alone. While for high resolution FT-ICR mass spectral data, the ion charge can be otherwise determined from the reciprocal of the m/z difference between adjacent isotopic peaks, the CRAM approach is superior and determines ion charge with several orders of magnitude higher accuracy. The CRAM has been applied to high resolution FT-ICR mass spectral for several proteins (ubiquitin, cytochrome c, transthyretin, lysozyme and calmodulin) to demonstrate the general utility of this approach and its application to proteomics. The results have been discussed in terms of internally calibrated ions versus external calibration where the CRAM approach was superior in both cases. [Copyright &y& Elsevier]
Published: 2005
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35. Preparation of a hyaluronic acid hydrogel through polyion complex formation using cationic polylactide-based microspheres as a biodegradable cross-linking agent.

Author: Arimura, Hidetoshi, Ouchi, Tatsuro, Kishida, Akio, and Ohya, Yuichi
Subjects: *HYALURONIC acid, *HYDROGELS, *MICROSPHERES, *DRUG carriers, *COLLAGEN
Abstract: A novel hyaluronic acid (HA)-based hydrogel was prepared through polyion complex (PIC) formation between cationic polylactide (PLA)-based microspheres (MS+) and hyaluronic acid (HA-) as an anionic polyelectrolyte. The MS+ and HA formed a biodegradable PIC hydrogel (HA-/MS+) when mixed in aqueous media. The swelling behavior and mechanical properties of the PIC hydrogel could be controlled by changing the charge ratio between HA- and MS+. In addition, the HA-/MS+ PIC hydrogel resulted in a lower inflammatory response compared with a collagen hydrogel in vivo. [ABSTRACT FROM AUTHOR]
Published: 2005
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36. Pelletizing Analysis on MgO-Fluxed Pellets by DEM.

Author: Long, Fang, Shen, Fengman, Jiang, Xin, Yang, Fu, Zhou, Yulu, and An, Haiwei
Subjects: PELLETIZING, DISCRETE element method, SPEED
Abstract: The Discrete Element Method (DEM) was used to analyze the pelletization process of MgO-fluxed pellets. The effects of the charge ratio and rotational speed of the disc pelletizer on the behavior of MgO-fluxed pellets were investigated by using a simulation. The simulation results show that under the condition of a certain tilt angle of the disc pelletizer (the tilt angle is 49°), the suitable parameters of the disc pelletizer are that the charge ratio is 20% and the rotational speedis 0.7 N/NC. This simulation model proposed will be useful to research pellets behavior and for the design of disc pelletizers. [ABSTRACT FROM AUTHOR]
Published: 2021
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37. Neutralization of negative charges of siRNA results in improved safety and efficient gene silencing activity of lipid nanoparticles loaded with high levels of siRNA

Author: 1000010735624, Sato, Yusuke, Matsui, Hideki, Sato, Risa, 1000000183567, Harashima, Hideyoshi, 1000010735624, Sato, Yusuke, Matsui, Hideki, Sato, Risa, 1000000183567, and Harashima, Hideyoshi
Abstract: Lipid nanoparticles (LNPs) are one of the leading technologies for the in vivo delivery of short interfering RNA (siRNA). Cationic lipids are an important component for efficient endosomal escape via membrane fusion followed by release of siRNAs in cytosol where the site of action is located. A high cationic lipid/siRNA charge ratio is usually necessary for maximizing the gene silencing activity of the siRNA-loaded LNPs. However, high levels of cationic lipids are known to cause cytotoxicity through interactions with negatively charged biocomponents. A strategy for solving this dilemma is important, in terms of producing clinically applicable LNPs with a wide therapeutic window. We herein report on the development of LNPs with a high gene silencing activity and a low cationic lipid/siRNA charge ratio, which we refer to as low lipid core-nanoparticles (LLC-NPs). The negative charges of the siRNAs were neutralized by protamines, cationic proteins, to reduce the net dose of cationic lipid, YSK05, which was developed in our laboratory, for endosomal escape, resulting in preserved fusogenic activity and gene silencing activity, both in vitro and in vivo factor VII mouse model. In addition, the LLC-NPs showed an improved hepatotoxicity compared to conventional LNPs, which have a relatively higher cationic lipid/siRNA charge ratio. The concept of the LLC-NPs helps to realize clinically applicable LNPs with a wide therapeutic window and has the potential for use in various applications and for the delivery of different classes of nucleic acid.
Published: 2018

38. The cosmic ray muon spectrum and charge ratio in CosmoALEPH

Author: Zimmermann, D., Grupen, C., Kotaidis, V., Luitz, S., Mailov, A., Müller, A.-S., Putzer, A., Rensch, B., Sander, H.-G., Schmeling, S., Schmelling, M., Wachsmuth, H., Tcaciuc, R., Ziegler, Th., and Zuber, K.
Subjects: *MUONS, *COSMIC ray muons, *NEUTRINOS, SCATTERING, MUON spectra
Abstract: The ALEPH experiment at the LEP e+e- storage ring at CERN has been used to measure the momentum spectrum of cosmic ray muons. ALEPH is located at a vertical depth of 320 m.w.e. underground close to the Jura mountains. The high resolution of the time projection chamber (TPC) of ALEPH allows to reconstruct muon tracks with momenta up to the TeV region. The measured muon momentum spectrum and the charge ratio in the range from 80 to 2500 GeV are presented. After corrections for energy loss in the overburden the sea level muon spectrum at nearly vertical incidence is obtained. The experimental data are compared to theoretical expectations and results from other experiments. [Copyright &y& Elsevier]
Published: 2004
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39. Cosmic Ray Composition at 1012 – 1015 eV Derived from Muon Measurements

Author: Allkofer, O. C. and Shapiro, Maurice M., editor
Published: 1983
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40. Weak Neutral Current-Semileptonic Interactions

Author: Borgia, Bruno, Zichichi, Antonino, editor, and Fiorini, Ettore, editor
Published: 1982
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41. Review of Electroproduction Experiments at Cornell and M.I.T. - SLAC

Author: Osborne, L. S., Zichichi, Antonino, editor, Preparata, Giuliano, editor, and Aubert, Jean-Jacques, editor
Published: 1980
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42. Hard Scattering at ISR Energies

Author: McCubbin, N. A., Carlson, Per, editor, and Trower, W. Peter, editor
Published: 1983
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43. Gene-eluting stents: non-viral, liposome-based gene delivery of eNOS to the blood vessel wall in vivo results in enhanced endothelialization but does not reduce restenosis in a hypercholesterolemic model

Author: Faisal Sharif, Karl J. A. McCullagh, Peter E. McHugh, Sean O. Hynes, J Crowley, Timothy O'Brien, S Ganley, Frank Barry, and Udo Greiser
Subjects: Male, late stent thrombosis, medicine.medical_treatment, Gene Expression, Constriction, Pathologic, Pharmacology, release, endothelialization, carotid arteries, Restenosis, Enos, Transgenes, Neointimal hyperplasia, biology, Gene Transfer Techniques, Dependovirus, medicine.anatomical_structure, transfection, liposome, coronary artery stents, Cardiology, Molecular Medicine, Stents, Rabbits, Plasmids, Blood vessel, Neointima, medicine.medical_specialty, Nitric Oxide Synthase Type III, endothelium, Endothelium, nitric-oxide synthase, Genetic Vectors, Hypercholesterolemia, neointimal hyperplasia, Gene delivery, Adenoviridae, restenosis, charge ratio, Internal medicine, Genetics, medicine, Animals, Humans, Regeneration, Molecular Biology, business.industry, Stent, DNA, medicine.disease, biology.organism_classification, Disease Models, Animal, efficiency, Liposomes, activation, Endothelium, Vascular, Tunica Intima, business
Abstract: Although successful, drug-eluting stents require significant periods of dual anti-platelet therapy with a persistent risk of late stent thrombosis due to inhibition of re-endothelialization. Endothelial regeneration is desirable to protect against in-stent thrombosis. Gene-eluting stents may be an alternative allowing inhibition of neointima and regenerating endothelium. We have shown that adenoviral endothelial nitric oxide synthase (eNOS) delivery can result in significantly decreased neointimal formation and enhanced re-endothelialization. Here, we examined non-viral reporter and therapeutic gene delivery from a stent. We coated lipoplexes directly onto the surface of stents. These lipostents were then deployed in the injured external iliac artery of either normal or hypercholesterolemic New Zealand White rabbits and recovered after 28 days. Lipoplexes composed of lipofectin and a reporter lacZ gene or therapeutic eNOS gene were used. We demonstrated efficient gene delivery at 28 days post-deployment in the media (21.3±7.5%) and neointima (26.8±11.2%). Liposomal delivery resulted in expression in macrophages between the stent struts. This resulted in improved re-endothelialization as detected by two independent measures compared with vector and stent controls (P
Published: 2011
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44. Lysine dendrimers as vectors for delivery of genetic constructs to eukaryotic cells

Author: Kiselev, A. V., Il’ina, P. L., Egorova, A. A., Baranov, A. N., Guryanov, I. A., Bayanova, N. V., Tarasenko, I. I., Lesina, E. A., Vlasov, G. P., and Baranov, V. S.
Published: 2007
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45. Negative ion matrix-assisted laser desorption/ionization time-of-flight post-source decay calibration by using fibrinopeptide B

Author: Jai-nhuknan, Jaran and Cassady, Carolyn J.
Published: 1998
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46. Overcoming the inhibitory effect of serum on lipofection by increasing the charge ratio of cationic liposome to DNA

Author: Yang, J-P and Huang, L
Published: 1997
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47. Aggregation and stability of polyelectrolyte-decorated liposome complexes in water-salt media

Author: Domenico Truzzolillo, Federico Bordi, and Simona Sennato
Subjects: colloidal aggregation, Chemistry, Charge density, General Chemistry, Condensed Matter Physics, Electrostatics, Charge ratio, Polyelectrolytes, Polyelectrolyte, Colloid, symbols.namesake, Van der Waals forces, colloids, polyelectrolytes, Chemical physics, Computational chemistry, Ionic strength, symbols, Phase diagrams, Surface charge, Adsorption, van der Waals force, Phase diagram, Charge Inhomogeneities
Abstract: Despite the initial disparity of the early results that appeared in the literature, due to the variety of the experimental conditions and to the intrinsic complexity of these systems, the interesting phenomenology shown by the aqueous co-suspensions of oppositely charged polyelectrolytes and colloidal macroions can now be described within a unified picture. For a general consensus, within this picture screened electrostatic interactions are the main driving force, and the non uniformity of charge distribution, resulting from the correlated adsorption of the polyelectrolyte on the colloid surface, plays a pivotal role. However, there is still a lack of a complete theory able to describe, satisfactorily, all the different features of the observed complexity. In this article, we begin to explore systematically the phase diagram of a typical polyelectrolyte/colloid system, considering in addition to the effects of the polyelectrolyte/colloid charge ratio and temperature, also those of the ionic strength of the aqueous suspending medium. We show that a simple interparticle potential built up as the sum of two terms is able to account for the observed phase diagram very satisfactorily. The first term of this potential describes the screened electrostatic interaction, taking into account the surface charge inhomogeneity of the polyelectrolyte-decorated particles, while the second describes the ubiquitous van der Waals interactions.
Published: 2012
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48. Measurement of the charge ratio of atmospheric muons with the CMS detector

Author: V. KHACHATRYAN, A. M. SIRUNYAN, A. TUMASYAN, W. ADAM, T. BERGAUER, M. DRAGICEVIC, J. ER¨O, C. FABJAN, M. FRIEDL, R. FRUHWIRTH, V. M. GHETE, J. HAMMER, S. H¨ANSEL, C. HARTL, M. HOCH, N. H¨ORMANN, J. HRUBEC, M. JEITLER, G. KASIECZKA, W. KIESENHOFER, M. KRAMMER, D. LIKO, I. MIKULEC, M. PERNICKA, H. ROHRINGER, R. SCH¨OFBECK, J. STRAUSS, A. TAUROK, F. TEISCHINGER, W. WALTENBERGER, G. WALZEL, E. WIDL, C. E. WULZ, V. MOSSOLOV, N. SHUMEIKO, J. SUAREZ GONZALEZ, L. BENUCCI, L. CEARD, E. A. DE WOLF, X. JANSSEN, T. MAES, L. MUCIBELLO, S. OCHESANU, B. ROLAND, R. ROUGNY, M. SELVAGGI, H. VAN HAEVERMAET, P. VAN MECHELEN, N. VAN REMORTEL, V. ADLER, S. BEAUCERON, S. BLYWEERT, J. D’HONDT, O. DEVROEDE, A. KALOGEROPOULOS, J. MAES, M. MAES, S. TAVERNIER, W. VAN DONINCK, P. VAN MULDERS, I. VILLELLA, E. C. CHABERT, O. CHARAF, B. CLERBAUX, G. DE LENTDECKER, V. DERO, A. P. R. GAY, G. H. HAMMAD, T. HREUS, P. E. MARAGE, C. VANDER VELDE, P. VANLAER, J. WICKENS, S. COSTANTINI, M. GRUNEWALD, B. KLEIN, A. MARINOV, D. RYCKBOSCH, F. THYSSEN, M. TYTGAT, L. VANELDEREN, P. VERWILLIGEN, S. WALSH, N. ZAGANIDIS, S. BASEGMEZ, G. BRUNO, J. CAUDRON, J. DE FAVEREAU DE JENERET, C. DELAERE, P. DEMIN, D. FAVART, A. GIAMMANCO, G. GR´EGOIRE, J. HOLLAR, V. LEMAITRE, O. MILITARU, S. OVYN, D. PAGANO, A. PIN, K. PIOTRZKOWSKI, L. QUERTENMONT, N. SCHUL, N. BELIY, T. CAEBERGS, E. DAUBIE, G. A. ALVES, D. DE JESUS DAMIAO, M. E. POL, M. H. G. SOUZA, W. CARVALHO, E. M. DA COSTA, C. DE OLIVEIRA MARTINS, S. FONSECA DE SOUZA, L. MUNDIM, H. NOGIMA, V. OGURI, J. M. OTALORA GOICOCHEA, W. L. PRADO DA SILVA, A. SANTORO, S. M. SILVA DO AMARAL, A. SZNAJDER, F. TORRES DA SILVA DE ARAUJO, F. A. DIAS, M. A. F. DIAS, T. R. FERNANDEZ PEREZ TOMEI, E. M. GREGORES, F. MARINHO, S. F. NOVAES, SANDRA S. PADULA, N. DARMENOV, L. DIMITROV, V. GENCHEV, P. IAYDJIEV, S. PIPEROV, M. RODOZOV, S. STOYKOVA, G. SULTANOV, V. TCHOLAKOV, R. TRAYANOV, I. VANKOV, M. DYULENDAROVA, R. HADJIISKA, V. KOZHUHAROV, L. LITOV, E. MARINOVA, M. MATEEV, B. PAVLOV, P. PETKOV, J. G. BIAN, G. M. CHEN, H. S. CHEN, C. H. JIANG, D. LIANG, S. LIANG, J. WANG, X. WANG, Z. WANG, M. YANG, J. ZANG, Z. ZHANG, Y. BAN, S. GUO, Z. HU, W. LI, Y. MAO, S. J. QIAN, H. TENG, B. ZHU, A. CABRERA, B. GOMEZ MORENO, A. A. OCAMPO RIOS, A. F. OSORIO OLIVEROS, J. C. SANABRIA, N. GODINOVIC, D. LELAS, K. LELAS, R. PLESTINA3, D. POLIC, I. PULJAK, Z. ANTUNOVIC, M. DZELALIJA, V. BRIGLJEVIC, S. DURIC, K. KADIJA, S. MOROVIC, A. ATTIKIS, R. FEREOS, M. GALANTI, J. MOUSA, C. NICOLAOU, F. PTOCHOS, P. A. RAZIS, H. RYKACZEWSKI, Y. ASSRAN, M. A. MAHMOUD, A. HEKTOR, M. KADASTIK, K. KANNIKE, M. M¨UNTEL, M. RAIDAL, L. REBANE, V. AZZOLINI, P. EEROLA, S. CZELLAR, J. H¨ARK¨ONEN, A. HEIKKINEN, V. KARIM¨AKI, R. KINNUNEN, J. KLEM, M. J. KORTELAINEN, T. LAMP´EN, K. LASSILA PERINI, S. LEHTI, T. LIND´EN, P. LUUKKA, T. M¨AENP¨A¨A, E. TUOMINEN, J. TUOMINIEMI, E. TUOVINEN, D. UNGARO, L. WENDLAND, K. BANZUZI, A. KORPELA, T. TUUVA, D. SILLOU, M. BESANCON, M. DEJARDIN, D. DENEGRI, J. DESCAMPS, B. FABBRO, J. L. FAURE, F. FERRI, S. GANJOUR, F. X. GENTIT, A. GIVERNAUD, P. GRAS, G. HAMEL DE MONCHENAULT, P. JARRY, E. LOCCI, J. MALCLES, M. MARIONNEAU, L. MILLISCHER, J. RANDER, A. ROSOWSKY, D. ROUSSEAU, M. TITOV, P. VERRECCHIA, S. BAFFIONI, L. BIANCHINI, M. BLUJ, C. BROUTIN, P. BUSSON, C. CHARLOT, L. DOBRZYNSKI, R. GRANIER DE CASSAGNAC, M. HAGUENAUER, P. MIN´E, C. MIRONOV, C. OCHANDO, P. PAGANINI, D. SABES, R. SALERNO, Y. SIROIS, C. THIEBAUX, A. ZABI, J. L. AGRAM, A. BESSON, D. BLOCH, D. BODIN, J. M. BROM, M. CARDACI, E. CONTE, F. DROUHIN, C. FERRO, J. C. FONTAINE, D. GEL´E, U. GOERLACH, S. GREDER, P. JUILLOT, M. KARIM, A. C. LE BIHAN, Y. MIKAMI, P. VAN HOVE, F. FASSI, D. MERCIER, C. BATY, N. BEAUPERE, M. BEDJIDIAN, O. BONDU, G. BOUDOUL, D. BOUMEDIENE, H. BRUN, N. CHANON, R. CHIERICI, D. CONTARDO, P. DEPASSE, H. EL MAMOUNI, A. FALKIEWICZ, J. FAY, S. GASCON, B. ILLE, T. KURCA, T. LE GRAND, M. LETHUILLIER, L. MIRABITO, S. PERRIES, V. SORDINI, S. TOSI, Y. TSCHUDI, P. VERDIER, H. XIAO, V. ROINISHVILI, G. ANAGNOSTOU, M. EDELHOFF, L. FELD, N. HERACLEOUS, O. HINDRICHS, R. JUSSEN, K. KLEIN, J. MERZ, N. MOHR, A. OSTAPCHUK, A. PERIEANU, F. RAUPACH, J. SAMMET, S. SCHAEL, D. SPRENGER, H. WEBER, M. WEBER, B. WITTMER, M. ATA, W. BENDER, M. ERDMANN, J. FRANGENHEIM, T. HEBBEKER, A. HINZMANN, K. HOEPFNER, C. HOF, T. KLIMKOVICH, D. KLINGEBIEL, P. KREUZER1, D. LANSKEY, C. MAGASS, G. MASETTI, M. MERSCHMEYER, A. MEYER, P. PAPACZ, H. PIETA, H. REITHLER, S. A. SCHMITZ, L. SONNENSCHEIN, J. STEGGEMANN, D. TEYSSIER, M. BONTENACKELS, M. DAVIDS, M. DUDA, G. FL¨UGGE, H. GEENEN, M. GIFFELS, W. HAJ AHMAD, D. HEYDHAUSEN, T. KRESS, Y. KUESSEL, A. LINN, A. NOWACK, L. PERCHALLA, O. POOTH, J. RENNEFELD, P. SAUERLAND, A. STAHL, M. THOMAS, D. TORNIER, M. H. ZOELLER, M. ALDAYA MARTIN, W. BEHRENHOFF, U. BEHRENS, M. BERGHOLZ, K. BORRAS, A. CAMPBELL, E. CASTRO, D. DAMMANN, G. ECKERLIN, A. FLOSSDORF, G. FLUCKE, A. GEISER, I. GLUSHKOV, J. HAUK, H. JUNG, M. KASEMANN, I. KATKOV, P. KATSAS, C. KLEINWORT, H. KLUGE, A. KNUTSSON, D. KR¨ UCKER, E. KUZNETSOVA, W. LANGE, W. LOHMANN, R. MANKEL, M. MARIENFELD, I. A. MELZER PELLMANN, A. B. MEYER, J. MNICH, A. MUSSGILLER, J. OLZEM, A. PARENTI, A. RASPEREZA, A. RAVAL, R. SCHMIDT, T. SCHOERNER SADENIUS, N. SEN, M. STEIN, J. TOMASZEWSKA, D. VOLYANSKYY, R. WALSH, C. WISSING, C. AUTERMANN, S. BOBROVSKYI, J. DRAEGER, D. ECKSTEIN, H. ENDERLE, U. GEBBERT, K. KASCHUBE, G. KAUSSEN, R. KLANNER, B. MURA, S. NAUMANN EMME, F. NOWAK, N. PIETSCH, C. SANDER, H. SCHETTLER, P. SCHLEPER, M. SCHR¨ODER, T. SCHUM, J. SCHWANDT, A. K. SRIVASTAVA, H. STADIE, G. STEINBR¨UCK, J. THOMSEN, R. WOLF, J. BAUER, V. BUEGE, A. CAKIR, T. CHWALEK, D. DAEUWEL, W. DE BOER, A. DIERLAMM, G. DIRKES, M. FEINDT, J. GRUSCHKE, C. HACKSTEIN, F. HARTMANN, M. HEINRICH, H. HELD, K. H. HOFFMANN, S. HONC, T. KUHR, D. MARTSCHEI, S. MUELLER, T.H. M¨ULLER, M. B. NEULAND, M. NIEGEL, O. OBERST, A. OEHLER, J. OTT, T. PEIFFER, D. PIPARO, G. QUAST, K. RABBERTZ, F. RATNIKOV, M. RENZ, A. 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MEIER, P. MERKEL, D. H. MILLER, N. NEUMEISTER, K. POTAMIANOS, I. SHIPSEY, D. SILVERS, A. SVYATKOVSKIY, H. D. YOO, J. ZABLOCKI, Y. ZHENG, P. JINDAL, N. PARASHAR, C. BOULAHOUACHE, V. CUPLOV, K. M. ECKLUND, F. J. M. GEURTS, J. H. LIU, J. MORALES, B. P. PADLEY, R. REDJIMI, J. ROBERTS, J. ZABEL, B. BETCHART, A. BODEK, Y. S. CHUNG, P. DE BARBARO, R. DEMINA, Y. ESHAQ, H. FLACHER, A. GARCIA BELLIDO, P. GOLDENZWEIG, Y. GOTRA, J. HAN, A. HAREL, D. C. MINER, D. ORBAKER, G. PETRILLO, D. VISHNEVSKIY, M. ZIELINSKI, A. BHATTI, L. DEMORTIER, K. GOULIANOS, G. LUNGU, C. MESROPIAN, M. YAN, O. ATRAMENTOV, A. BARKER, D. DUGGAN, Y. GERSHTEIN, R. GRAY, E. HALKIADAKIS, D. HIDAS, D. HITS, A. LATH, S. PANWALKAR, R. PATEL, A. RICHARDS, K. ROSE, S. SCHNETZER, S. SOMALWAR, R. STONE, S. THOMAS, G. CERIZZA, M. HOLLINGSWORTH, S. SPANIER, Z. C. YANG, A. YORK, J. ASAADI, R. EUSEBI, J. GILMORE, A. GURROLA, T. KAMON, V. KHOTILOVICH, R. MONTALVO, C. N. NGUYEN, J. PIVARSKI, A. SAFONOV, S. SENGUPTA, A. TATARINOV, D. 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WEINBERG, BONACORSI, DANIELE, BRAIBANT, SYLVIE, CAPILUPPI, PAOLO, CASTRO, ANDREA, CUFFIANI, MARCO, FANFANI, ALESSANDRA, ROSSI, ANTONIO MARIA, ROVELLI, TIZIANO, SIROLI, GIAN PIERO, Massachusetts Institute of Technology. Department of Physics, Massachusetts Institute of Technology. Laboratory for Nuclear Science, Massachusetts Institute of Technology. School of Science, Alver, B., Bauer, Gerry P., Bendavid, Joshua L., Busza, Wit, Butz, Erik M., Cali, Ivan Amos, Chan, M., D'Enterria, David, Everaerts, Pieter Bruno Bart, Gomez-Ceballos, Guillelmo, Goncharov, Maxim, Hahn, Kristian Allan, Harris, P., Kim, Y., Klute, Markus, Lee, Y.-J., Li, W., Loizides, C., Luckey, P. David, Jr., Ma, Teng, Nahn, Steven, Paus, Christoph M. E., Roland, Christof E., Rudolph, Matthew Scott, Stephans, George S. F., Sumorok, Konstanty C., Wenger, Edward Allen, Wyslouch, Boleslaw, Xie, S., Yilmaz, Yetkin, Yoon, A. S., Zanetti, Marco, Çukurova Üniversitesi, Fen-Edebiyat Fakültesi, Fizik Bölümü, Laboratoire d'Annecy de Physique des Particules (LAPP), Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Université Savoie Mont Blanc (USMB [Université de Savoie] [Université de Chambéry])-Centre National de la Recherche Scientifique (CNRS), Institut de Recherches sur les lois Fondamentales de l'Univers (IRFU), Commissariat à l'énergie atomique et aux énergies alternatives (CEA)-Université Paris-Saclay, Laboratoire Leprince-Ringuet (LLR), Centre National de la Recherche Scientifique (CNRS)-École polytechnique (X)-Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3), Centre de Calcul de l'IN2P3 (CC-IN2P3), Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Centre National de la Recherche Scientifique (CNRS), Institut de Physique Nucléaire de Lyon (IPNL), Centre National de la Recherche Scientifique (CNRS)-Université Claude Bernard Lyon 1 (UCBL), Université de Lyon-Université de Lyon-Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3), CMS, Institut de Physique des 2 Infinis de Lyon (IP2I Lyon), Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Université Claude Bernard Lyon 1 (UCBL), Université de Lyon-Université de Lyon-Centre National de la Recherche Scientifique (CNRS)-Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Université Claude Bernard Lyon 1 (UCBL), Université de Lyon-Université de Lyon-Centre National de la Recherche Scientifique (CNRS), Laboratoire SYstèmes et Matériaux pour la MEcatronique (SYMME), Université Savoie Mont Blanc (USMB [Université de Savoie] [Université de Chambéry]), Laboratoire d'Annecy de Physique des Particules (LAPP/Laboratoire d'Annecy-le-Vieux de Physique des Particules), Centre National de la Recherche Scientifique (CNRS)-Université Savoie Mont Blanc (USMB [Université de Savoie] [Université de Chambéry])-Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3), Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-École polytechnique (X)-Centre National de la Recherche Scientifique (CNRS), Centre National de la Recherche Scientifique (CNRS)-Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3), Université Claude Bernard Lyon 1 (UCBL), Université de Lyon-Université de Lyon-Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Centre National de la Recherche Scientifique (CNRS), Université de Lyon-Université de Lyon-Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Centre National de la Recherche Scientifique (CNRS)-Université Claude Bernard Lyon 1 (UCBL), Khachatryan, V., Sirunyan, A. 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P., Dinardo, M. E., Drell, B. R., Ford, W. T., Heyburn, B., Lopez E., Luiggi, Nauenberg, U., Smith, J. G., Stenson, K., Ulmer, K. A., Wagner, S. R., Zang, S. L., Agostino, L., Alexander, J., Blekman, F., Chatterjee, A., Das, S., Eggert, N., Fields, L. J., Gibbons, L. K., Heltsley, B., Hopkins, W., Khukhunaishvili, A., Kreis, B., Kuznetsov, V., Kaufman G., Nicola, Patterson, J. R., Puigh, D., Riley, D., Ryd, A., Shi, X., Sun, W., Teo, W. D., Thom, J., Thompson, J., Vaughan, J., Weng, Y., Wittich, P., Biselli, A., Cirino, G., Winn, D., Abdullin, S., Albrow, M., Anderson, J., Apollinari, G., Atac, M., Bakken, J. A., Bauerdick, L. A. T., Beretvas, A., Berryhill, J., Bhat, P. C., Bloch, I., Borcherding, F., Burkett, K., Butler, J. N., Chetluru, V., Cheung, H. W. K., Chlebana, F., Cihangir, S., Demarteau, M., Eartly, D. P., Elvira, V. D., Fisk, I., Freeman, J., Gao, Y., Gottschalk, E., Green, D., Gutsche, O., Hahn, A., Hanlon, J., Harris, R. M., James, E., Jensen, H., Johnson, M., Joshi, U., Khatiwada, R., Kilminster, B., Klima, B., Kousouris, K., Kunori, S., Kwan, S., Limon, P., Lipton, R., Lykken, J., Maeshima, K., Marraffino, J. M., Mason, D., Mcbride, P., Mccauley, T., Miao, T., Mishra, K., Mrenna, S., Musienko, Y., Newman Holmes, C., O'Dell, V., Popescu, S., Pordes, R., Prokofyev, O., Saoulidou, N., Sexton Kennedy, E., Sharma, S., Smith, R. P., Soha, A., Spalding, W. J., Spiegel, L., Tan, R., Taylor, L., Tkaczyk, S., Uplegger, L., Vaandering, E. W., Vidal, R., Whitmore, J., Wu, W., Yumiceva, F., Yun, J. C., Acosta, D., Avery, P., Bourilkov, D., Chen, M., Di Giovanni, G. P., Dobur, D., Drozdetskiy, A., Field, R. D., Fu, Y., Furic, I. K., Gartner, J., Kim, B., Klimenko, S., Konigsberg, J., Korytov, A., Kotov, K., Kropivnitskaya, A., Kypreos, T., Matchev, K., Mitselmakher, G., Pakhotin, Y., Gomez J., Piedra, Prescott, C., Remington, R., Schmitt, M., Scurlock, B., Sellers, P., Wang, D., Yelton, J., Zakaria, M., Ceron, C., Gaultney, V., Kramer, L., Lebolo, L. M., Linn, S., Markowitz, P., Martinez, G., Mesa, D., Rodriguez, J. L., Adams, T., Askew, A., Chen, J., Diamond, B., Gleyzer, S. V., Haas, J., Hagopian, S., Hagopian, V., Jenkins, M., Johnson, K. F., Prosper, H., Sekmen, S., Veeraraghavan, V., Baarmand, M. M., Guragain, S., Hohlmann, M., Kalakhety, H., Mermerkaya, H., Ralich, R., Vodopiyanov, I., Adams, M. R., Anghel, I. M., Apanasevich, L., Bazterra, V. E., Betts, R. R., Callner, J., Cavanaugh, R., Dragoiu, C., Garcia Solis, E. J., Gerber, C. E., Hofman, D. J., Khalatian, S., Lacroix, F., Shabalina, E., Smoron, A., Strom, D., Varelas, N., Akgun, U., Albayrak, E. A., Bilki, B., Cankocak, K., Clarida, W., Duru, F., Lae, C. K., Mccliment, E., Merlo J., R, Mestvirishvili, A., Moeller, A., Nachtman, J., Newsom, C. R., Norbeck, E., Olson, J., Onel, Y., Ozok, F., Sen, S., Wetzel, J., Yetkin, T., Yi, K., Barnett, B. A., Blumenfeld, B., Bonato, A., Eskew, C., Fehling, D., Giurgiu, G., Gritsan, A. V., Guo, Z. J., Hu, G., Maksimovic, P., Rappoccio, S., Swartz, M., Tran, N. V., Whitbeck, A., Baringer, P., Bean, A., Benelli, G., Grachov, O., Murray, M., Radicci, V., Sanders, S., Wood, J. S., Zhukova, V., Bandurin, D., Bolton, T., Chakaberia, I., Ivanov, A., Kaadze, K., Maravin, Y., Shrestha, S., Svintradze, I., Wan, Z., Gronberg, J., Lange, D., Wright, D., Baden, D., Boutemeur, M., Eno, S. C., Ferencek, D., Hadley, N. J., Kellogg, R. G., Kim, M., Mignerey, A. C., Rossato, K., Rumerio, P., Santanastasio, F., Skuja, A., Temple, J., Tonjes, M. B., Tonwar, S. C., Twedt, E., Bauer, G., Bendavid, J., Busza, W., Butz, E., Cali, I. A., D'Enterria, D., Everaerts, P., Ceballos G., Gomez, Goncharov, M., Hahn, K. A., Klute, M., Lee, Y. J., Luckey, P. D., Ma, T., Nahn, S., Paus, C., Roland, C., Roland, G., Rudolph, M., Stephans, G. S. F., Sumorok, K., Sung, K., Wenger, E. A., Wyslouch, B., Yilmaz, Y., Zanetti, M., Cole, R., Cooper, S. I., Cushman, P., Dahmes, B., De Benedetti, A., Dudero, P. R., Franzoni, G., Haupt, J., Klapoetke, K., Kubota, Y., Mans, J., Rekovic, V., Rusack, R., Sasseville, M., Singovsky, A., Cremaldi, L. M., Godang, R., Kroeger, R., Perera, L., Rahmat, R., Sanders, D. A., Sonnek, P., Summers, D., Bloom, K., Bose, S., Butt, J., Claes, D. R., Dominguez, A., Eads, M., Keller, J., Kelly, T., Kravchenko, I., Lazo Flores, J., Lundstedt, C., Malbouisson, F. l., Malik, S., Snow, G. R., Baur, U., Lashvili, I., Kharchilava, A., Smith, K., Strang, M., Zennamo, J., Alverson, G., Barberis, E., Baumgartel, D., Boeriu, O., Reucroft, S., Swain, J., Wood, D., Zhang, J., Anastassov, A., Kubik, A., Ofierzynski, R. A., Pozdnyakov, A., Stoynev, S., Velasco, M., Won, S., Antonelli, L., Berry, D., Hildreth, M., Jessop, C., Karmgard, D. J., Kolb, J., Kolberg, T., Lannon, K., Lynch, S., Marinelli, N., Morse, D. M., Ruchti, R., Slaunwhite, J., Valls, N., Warchol, J., Wayne, M., Ziegler, J., Bylsma, B., Durkin, L. S., Gu, J., Killewald, P., Ling, T. Y., Williams, G., Adam, N., Berry, E., Elmer, R., Gerbaudo, D., Halyo, V., Hunt, A., Jones, J., Laird, E., Pegna D., Lope, Marlow, D., Medvedeva, T., Mooney, M., Olsen, J., Piroue, P., Stickland, D., Tully, C., Werner, J. S., Zuranski, A., Acosta, J. G., Huang, X. T., Lopez, A., Mendez, H., Oliveros, S., Vargas J. E., Ramirez, Zatzerklyaniy, A., Alagoz, E., Barnes, V. E., Bolla, G., Borrello, L., Bortoletto, D., Everett, A., Garfinkel, A. F., Gecse, Z., Gutay, L., Jones, M., Koybasi, O., Laasanen, A. T., Leonardo, N., Liu, C., Maroussov, V., Merkel, P., Miller, D. H., Neumeister, N., Potamianos, K., Shipsey, I., Silvers, D., Yoo, H. D., Zablocki, J., Zheng, Y., Jindal, P., Parashar, N., Cuplov, V., Ecklund, K. M., Geurts, F. J. M., Liu, J. H., Morales, J., Padley, B. P., Redjimi, R., Roberts, J., Betchart, B., Bodek, A., Chung, Y. S., de Barbaro, P., Demina, R., Flacher, H., Garcia Bellido, A., Gotra, Y., Han, J., Harel, A., Miner, D. C., Orbaker, D., Petrillo, G., Vishnevskiy, D., Zielinski, M., Bhatti, A., Demortier, L., Goulianos, K., Hatakeyama, K., Lungu, G., Mesropian, C., Yan, M., Atramentov, O., Gershtein, Y., Gray, R., Halkiadakis, E., Hidas, D., Hits, D., Lath, A., Rose, K., Schnetzer, S., Somalwar, S., Stone, R., Thomas, S., Cerizza, G., Hollingsworth, M., Spanier, S., Yang, Z. C., York, A., Asaadi, J., Eusebi, R., Gilmore, J., Gurrola, A., Kamon, T., Khotilovich, V., Montalvo, R., Nguyen, C. N., Pivarski, J., Safonov, A., Sengupta, S., Toback, D., Weinberger, M., Akchurin, N., Bardak, C., Damgov, J., Jeong, C., Kovitanggoon, K., Lee, S. W., Mane, R., Roh, Y., Sill, A., Volobouev, I., Wigmans, R., Yazgan, E., Appelt, E., Brownson, E., Engh, D., Florez, C., Gabella, W., Johns, W., Kurt, P., Maguire, C., Melo, A., Sheldon, P., Velkovska, J., Arenton, M. W., Balazs, M., Buehler, M., Conetti, S., Cox, B., Hirosky, R., Ledovskoy, A., Neu, C., Yohay, R., Gollapinni, S., Gunthoti, K., Harr, R., Karchin, P. E., Mattson, M., Milstene, C., Sakharov, A., Anderson, M., Bachtis, M., Bellinger, J. N., Carlsmith, D., Dasu, S., Dutta, S., Efron, J., Gray, L., Grogg, K. S., Grothe, M., Herndon, M., Klabbers, P., Klukas, J., Lanaro, A., Lazaridis, C., Leonard, J., Lomidze, D., Loveless, R., Mohapatra, A., Polese, G., Reeder, D., Savin, A., Smith, W. 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Physikalisches Institut B, Deutsches Elektronen-Synchrotron, University of Hamburg, Institut für Experimentelle Kernphysik, Institute of Nuclear Physics Demokritos, University of Athens, University of Ioánnina, KFKI Research Institute for Particle and Nuclear Physics, Institute of Nuclear Research ATOMKI, University of Debrecen, Panjab University, University of Delhi, Bhabha Atomic Research Centre, Tata Institute of Fundamental Research - EHEP, Tata Institute of Fundamental Research - HECR, Institute for Studies in Theoretical Physics and Mathematics (IPM), INFN Sezione di Bari, Università di Bari, Politecnico di Bari, INFN Sezione di Bologna, Università di Bologna, INFN Sezione di Catania, Università di Catania, INFN Sezione di Firenze, Università di Firenze, INFN Laboratori Nazionali di Frascati, INFN Sezione di Genova, INFN Sezione di Milano-Biccoca, Università di Milano-Bicocca, INFN Sezione di Napoli, Università di Napoli Federico II, INFN Sezione di Padova, Università di Padova, Università di Trento (Trento), INFN Sezione di Pavia, Università di Pavia, INFN Sezione di Perugia, Università di Perugia, INFN Sezione di Pisa, Università di Pisa, Scuola Normale Superiore di Pisa, INFN Sezione di Roma, Università di Roma La Sapienza, INFN Sezione di Torino, Università di Torino, Università del Piemonte Orientale (Novara), INFN Sezione di Trieste, Università di Trieste, Kyungpook National University, Institute for Universe and Elementary Particles, Korea University, University of Seoul, Sungkyunkwan University, Vilnius University, Centro de Investigacion y de Estudios Avanzados del IPN, Universidad Iberoamericana, Benemerita Universidad Autonoma de Puebla, Universidad Autónoma de San Luis Potosí, University of Auckland, University of Canterbury, Quaid-I-Azam University, Institute of Experimental Physics, Soltan Institute for Nuclear Studies, Laboratório de Instrumentação e Física Experimental de Partículas (LIP), Joint Institute for Nuclear Research, Petersburg Nuclear Physics Institute, Institute for Nuclear Research, Institute for Theoretical and Experimental Physics (ITEP), Moscow State University, P.N. 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KHACHATRYAN, A.M. SIRUNYAN, A. TUMASYAN, W. ADAM, T. BERGAUER, M. DRAGICEVIC, J. ER¨O, C. FABJAN, M. FRIEDL, R. FRUHWIRTH, V.M. GHETE, J. HAMMER, S. H¨ANSEL, C. HARTL, M. HOCH, N. H¨ORMANN, J. HRUBEC, M. JEITLER, G. KASIECZKA, W. KIESENHOFER, M. KRAMMER, D. LIKO, I. MIKULEC, M. PERNICKA, H. ROHRINGER, R. SCH¨OFBECK, J. STRAUSS, A. TAUROK, F. TEISCHINGER, W.WALTENBERGER, G.WALZEL, E.WIDL, C.-E.WULZ, V. MOSSOLOV, N. SHUMEIKO, J. SUAREZ GONZALEZ, L. BENUCCI, L. CEARD, E.A. DE WOLF, X. JANSSEN, T. MAES, L. MUCIBELLO, S. OCHESANU, B. ROLAND, R. ROUGNY, M. SELVAGGI, H. VAN HAEVERMAET, P. VAN MECHELEN, N. VAN REMORTEL, V. ADLER, S. BEAUCERON, S. BLYWEERT, J. D’HONDT, O. DEVROEDE, A. KALOGEROPOULOS, J. MAES, M. MAES, S. TAVERNIER, W. VAN DONINCK, P. VAN MULDERS, I. VILLELLA, E.C. CHABERT, O. CHARAF, B. CLERBAUX, G. DE LENTDECKER, V. DERO, A.P.R. GAY, G.H. HAMMAD, T. HREUS, P.E. MARAGE, C. VANDER VELDE, P. VANLAER, J.WICKENS, S. COSTANTINI, M. GRUNEWALD, B. KLEIN, A. MARINOV, D. RYCKBOSCH, F. THYSSEN, M. TYTGAT, L. VANELDEREN, P. VERWILLIGEN, S.WALSH, N. ZAGANIDIS, S. BASEGMEZ, G. BRUNO, J. CAUDRON, J. DE FAVEREAU DE JENERET, C. DELAERE, P. DEMIN, D. FAVART, A. GIAMMANCO, G. GR´EGOIRE, J. HOLLAR, V. LEMAITRE, O. MILITARU, S. OVYN, D. PAGANO, A. PIN, K. PIOTRZKOWSKI, L. QUERTENMONT, N. SCHUL, N. BELIY, T. CAEBERGS, E. DAUBIE, G.A. ALVES, D. DE JESUS DAMIAO, M.E. POL, M.H.G. SOUZA, W. CARVALHO, E.M. DA COSTA, C. DE OLIVEIRA MARTINS, S. FONSECA DE SOUZA, L. MUNDIM, H. NOGIMA, V. OGURI, J.M. OTALORA GOICOCHEA, W.L. PRADO DA SILVA, A. SANTORO, S.M. SILVA DO AMARAL, A. SZNAJDER, F. TORRES DA SILVA DE ARAUJO, F.A. DIAS, M.A.F. DIAS, T.R. FERNANDEZ PEREZ TOMEI, E. M. GREGORES, F. MARINHO, S.F. NOVAES, SANDRA S. PADULA, N. DARMENOV, L. DIMITROV, V. GENCHEV, P. IAYDJIEV, S. PIPEROV, M. RODOZOV, S. STOYKOVA, G. SULTANOV, V. TCHOLAKOV, R. TRAYANOV, I. VANKOV, M. DYULENDAROVA, R. HADJIISKA, V. KOZHUHAROV, L. LITOV, E. MARINOVA, M. MATEEV, B. PAVLOV, P. PETKOV, J.G. BIAN, G.M. CHEN, H.S. CHEN, C.H. JIANG, D. LIANG, S. LIANG, J. WANG, X. WANG, Z.WANG, M. YANG, J. ZANG, Z. ZHANG, Y. BAN, S. GUO, Z. HU, W. LI, Y. MAO, S.J. QIAN, H. TENG, B. ZHU, A. CABRERA, B. GOMEZ MORENO, A.A. OCAMPO RIOS, A.F. OSORIO OLIVEROS, J.C. SANABRIA, N. GODINOVIC, D. LELAS, K. LELAS, R. PLESTINA3, D. POLIC, I. PULJAK, Z. ANTUNOVIC, M. DZELALIJA, V. BRIGLJEVIC, S. DURIC, K. KADIJA, S. MOROVIC, A. ATTIKIS, R. FEREOS, M. GALANTI, J. MOUSA, C. NICOLAOU, F. PTOCHOS, P.A. RAZIS, H. RYKACZEWSKI, Y. ASSRAN, M.A. MAHMOUD, A. HEKTOR, M. KADASTIK, K. KANNIKE, M. M¨UNTEL, M. RAIDAL, L. REBANE, V. AZZOLINI, P. EEROLA, S. CZELLAR, J. H¨ARK¨ONEN, A. HEIKKINEN, V. KARIM¨AKI, R. KINNUNEN, J. KLEM, M.J. KORTELAINEN, T. LAMP´EN, K. LASSILA-PERINI, S. LEHTI, T. LIND´EN, P. LUUKKA, T. M¨AENP¨A¨A, E. TUOMINEN, J. TUOMINIEMI, E. TUOVINEN, D. UNGARO, L.WENDLAND, K. BANZUZI, A. KORPELA, T. TUUVA, D. SILLOU, M. BESANCON, M. DEJARDIN, D. DENEGRI, J. DESCAMPS, B. FABBRO, J.L. FAURE, F. FERRI, S. GANJOUR, F.X. 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Miner, D, Orbaker, D, Petrillo, G, Vishnevskiy, D, Zielinski, M, Bhatti, A, Demortier, L, Goulianos, K, Hatakeyama, K, Lungu, G, Mesropian, C, Yan, M, Atramentov, O, Gershtein, Y, Gray, R, Halkiadakis, E, Hidas, D, Hits, D, Lath, A, Rose, K, Schnetzer, S, Somalwar, S, Stone, R, Thomas, S, Cerizza, G, Hollingsworth, M, Spanier, S, Yang, Z, York, A, Asaadi, J, Eusebi, R, Gilmore, J, Gurrola, A, Kamon, T, Khotilovich, V, Montalvo, R, Nguyen, C, Pivarski, J, Safonov, A, Sengupta, S, Toback, D, Weinberger, M, Akchurin, N, Bardak, C, Damgov, J, Jeong, C, Kovitanggoon, K, Mane, R, Roh, Y, Sill, A, Volobouev, I, Wigmans, R, Yazgan, E, Appelt, E, Brownson, E, Engh, D, Florez, C, Gabella, W, Johns, W, Kurt, P, Maguire, C, Melo, A, Sheldon, P, Velkovska, J, Arenton, M, Balazs, M, Buehler, M, Conetti, S, Cox, B, Hirosky, R, Ledovskoy, A, Neu, C, Yohay, R, Gollapinni, S, Gunthoti, K, Harr, R, Karchin, P, Mattson, M, Milstene, C, Sakharov, A, Anderson, M, Bachtis, M, Bellinger, J, Carlsmith, D, Dasu, S, Dutta, S, Efron, J, Gray, L, Grogg, K, Grothe, M, Herndon, M, Klabbers, P, Klukas, J, Lanaro, A, Lazaridis, C, Leonard, J, Lomidze, D, Loveless, R, Mohapatra, A, Polese, G, Reeder, D, Savin, A, Smith, W, Swanson, J, Weinberg, M, and Cms, C
Subjects: Physics::Instrumentation and Detectors, Muon, LHC, CMS, Charge ratio, 01 natural sciences, PARTICLE PHYSICS, LARGE HADRON COLLIDER, CMS, High Energy Physics - Experiment, High Energy Physics - Experiment (hep-ex), [PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex], Nuclear Experiment, Physics, Range (particle radiation), Large Hadron Collider, Detector, sea-level, Physique des particules élémentaires, physics, Particle Physics - Experiment, SEA-LEVEL, FLUX, Nuclear and High Energy Physics, Particle physics, cms, Astrophysics::High Energy Astrophysical Phenomena, FOS: Physical sciences, Cosmic ray, Atmosphere, Nuclear physics, Momentum, charge ratio, cosmic rays, muon, 0103 physical sciences, ddc:530, 010306 general physics, Cosmic rays, 010308 nuclear & particles physics, Charge (physics), flux, 13. Climate action, High Energy Physics::Experiment
Abstract: We present a measurement of the ratio of positive to negative muon fluxes from cosmic ray interactions in the atmosphere, using data collected by the CMS detector both at ground level and in the underground experimental cavern at the CERN LHC. Muons were detected in the momentum range from 5 GeV/. c to 1 TeV/. c. The surface flux ratio is measured to be 1.2766±0.0032(stat.)±0.0032(syst.), independent of the muon momentum, below 100 GeV/. c. This is the most precise measurement to date. At higher momenta the data are consistent with an increase of the charge ratio, in agreement with cosmic ray shower models and compatible with previous measurements by deep-underground experiments., 0, e-Print: arXiv:1005.5332 [hep-ex], 32 pp., info:eu-repo/semantics/published
Published: 2010
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49. Measurements of Cosmic Ray Muons Performed with WILLI Detector — Status and Perspectives.

Author: Mitrica, B., Brancus, I. M., Saftoiu, A., Bercuci, A., Petcu, M., Rebel, H., Haungs, A., Toma, G., Duma, M., Aiftimiei, C., Sima, O., Cata-Danil, G., and Radu, A.
Subjects: *MUONS, *COSMIC rays, *DETECTORS, *MONTE Carlo method, *NUCLEAR physics
Abstract: The WILLI detector, installed in the National Institute of Physics and Nuclear Engineering — Horia Hulubei Bucharest has been devised for studies of atmospheric muons, in particular of the muon charge ratio. We report on the results of studies for various muon energies (pμ < 1 GeV/c). The results are compared with Monte-Carlo simulations performed with the CORSIKA and GEANT codes. We are exploring the potential of a small detector array to be set up nearby the actual WILLI detector for triggering the muon charge ratio measurements by Extended Air Shower (EAS) events. © 2007 American Institute of Physics [ABSTRACT FROM AUTHOR]
Published: 2007
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50. Measurement of the charge ratio of atmospheric muons with the CMS detector

Author: UCL - Autre, Khachatryan, V., Sirunyan, A. M., Basegmez, S., Bruno, Giacomo, Caudron, J., De Jeneret, J. De Favereau, Delaere, Christophe, Demin, P., Favart, Denis, Giammanco, A., Gregoire, G., Hollar, J., Lemaitre, Vincent, Militaru, O., Ovyn, S., Pagano, D., Pin, A., Piotrzkowski, Krzysztof, Quertenmont, Loic, Schul, N., UCL - Autre, Khachatryan, V., Sirunyan, A. M., Basegmez, S., Bruno, Giacomo, Caudron, J., De Jeneret, J. De Favereau, Delaere, Christophe, Demin, P., Favart, Denis, Giammanco, A., Gregoire, G., Hollar, J., Lemaitre, Vincent, Militaru, O., Ovyn, S., Pagano, D., Pin, A., Piotrzkowski, Krzysztof, Quertenmont, Loic, and Schul, N.
Abstract: We present a measurement of the ratio of positive to negative muon fluxes from cosmic ray interactions in the atmosphere, using data collected by the CMS detector both at ground level and in the underground experimental cavern at the CERN LHC. Muons were detected in the momentum range from 5 GeV/c to 1 TeV/c. The surface flux ratio is measured to be 1.2766 +/- 0.0032 (stat.) +/- 0.0032 (syst.), independent of the muon momentum, below 100 GeV/c. This is the most precise measurement to date. At higher momenta the data are consistent with an increase of the charge ratio, in agreement with cosmic ray shower models and compatible with previous measurements by deep-underground experiments. (C) 2010 Published by Elsevier B.V.
Published: 2010

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