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Online since: August 2019
Authors: Zhi Guo Wang, Xiao Li Sun
Above all, the metal doped by substitution of S atom MoS2 single-layer are promising anode materials of LIBs.
It is very important to improve the energy density through developing new electrode materials.
Advanced Materials, 2012. 24(17): p. 2320-2325
[15] Soler, J.M., et al., The SIESTA method for ab initio order-N materials simulation.
Zhou, First-principles studies on doped graphene as anode materials in lithium-ion batteries.
It is very important to improve the energy density through developing new electrode materials.
Advanced Materials, 2012. 24(17): p. 2320-2325
[15] Soler, J.M., et al., The SIESTA method for ab initio order-N materials simulation.
Zhou, First-principles studies on doped graphene as anode materials in lithium-ion batteries.
Online since: June 2025
Authors: Can Ran Zhang, Qi Long Wang, Yi Jing Xu
Bilayer Graphene Optical Modulator Based on Metal-Nanoribbon Integrated Hybrid Plasmonic Waveguide
Yijing Xu1,a, Canran Zhang1,b, Qilong Wang1,c
1Joint International Research Laboratory of Information Display and Visualization, School of Electronic Science and Engineering, Southeast University, Nanjing 210096, China
a230228397@seu.edu.cn, bcanranzhang@seu.edu.cn, cnorthrockwql@seu.edu.cn
Keywords: optoelectronics, graphene, modulator, plasmonic waveguide.
In order to overcome these shortcomings, researchers considered introducing materials with strong electro-optic (electro-refractive or electro-absorptive) effects, such as germanium (Ge) materials, ferroelectric materials, organic electro-optic materials, III-V semiconductors materials, and 2D materials [7, 8].
To avoid graphene chemical doping by other materials, the Al2O3 layer with a relative permittivity (ɛAl2O3) of 3.04 and a thickness of 5 nm is chosen as the insulator layer placed between the bottom graphene layer and the Si waveguide [12].
The graphene layer can be regarded as a two-dimensional homogeneous anisotropic material and modeled as a surface conductive layer with no thickness.
12 40 [10] Wu X, Cao Z, Zhao T, Wu Y, Li Z, Doukas S, Lidorikis E, Xue Y, Liu L, Ghaebi O, Soavi G, Lu J, Ni Z and Wang J 2024 Nanoscale Horizons [11] Zhang H, Ma Z, Cai L and Zhang L 2024 Optics Letters 49 1337 [12] Liu M, Yin X, Ulin-Avila E, Geng B, Zentgraf T, Ju L, Wang F and Zhang X 2011 Nature 474 64 [13] Hanson G W 2008 Journal of Applied Physics 104 [14] Park H-Y, Jung W-S, Kang D-H, Jeon J, Yoo G, Park Y, Lee J, Jang Y H, Lee J, Park S, Yu H-Y, Shin B, Lee S and Park J-H 2016 Advanced Materials 28 864 [15] Shiramin L A and Van Thourhout D 2017 Ieee Journal of Selected Topics in Quantum Electronics 23
In order to overcome these shortcomings, researchers considered introducing materials with strong electro-optic (electro-refractive or electro-absorptive) effects, such as germanium (Ge) materials, ferroelectric materials, organic electro-optic materials, III-V semiconductors materials, and 2D materials [7, 8].
To avoid graphene chemical doping by other materials, the Al2O3 layer with a relative permittivity (ɛAl2O3) of 3.04 and a thickness of 5 nm is chosen as the insulator layer placed between the bottom graphene layer and the Si waveguide [12].
The graphene layer can be regarded as a two-dimensional homogeneous anisotropic material and modeled as a surface conductive layer with no thickness.
12 40 [10] Wu X, Cao Z, Zhao T, Wu Y, Li Z, Doukas S, Lidorikis E, Xue Y, Liu L, Ghaebi O, Soavi G, Lu J, Ni Z and Wang J 2024 Nanoscale Horizons [11] Zhang H, Ma Z, Cai L and Zhang L 2024 Optics Letters 49 1337 [12] Liu M, Yin X, Ulin-Avila E, Geng B, Zentgraf T, Ju L, Wang F and Zhang X 2011 Nature 474 64 [13] Hanson G W 2008 Journal of Applied Physics 104 [14] Park H-Y, Jung W-S, Kang D-H, Jeon J, Yoo G, Park Y, Lee J, Jang Y H, Lee J, Park S, Yu H-Y, Shin B, Lee S and Park J-H 2016 Advanced Materials 28 864 [15] Shiramin L A and Van Thourhout D 2017 Ieee Journal of Selected Topics in Quantum Electronics 23
Online since: May 2012
Authors: Hu Chen, Jian Wang, Han Zhong Tao, Hong Biao Huang
By materials and entropy balance calculation, indicators such as ideal power, actual power, power loss and thermodynamic efficiency can be obtained, and be used to assess the process.
Therefore in the design of heat exchangers, methods with the simplest structure and minimum materials should be used while the service conditions are met.
Vol. 22(1982), p. 63 [7] Hany Ahmed Mohamed: ASME Journal of Heat Transfer.
Vol. 41(2000), p. 1585 [9] Hesselgreaves J E: International Journal of Heat and Mass Transfer.
Vol.18(1)(1997), p. 90 (In Chinese) [11] Zhenwei Ni: Journal of Engineering Thermophysics.
Therefore in the design of heat exchangers, methods with the simplest structure and minimum materials should be used while the service conditions are met.
Vol. 22(1982), p. 63 [7] Hany Ahmed Mohamed: ASME Journal of Heat Transfer.
Vol. 41(2000), p. 1585 [9] Hesselgreaves J E: International Journal of Heat and Mass Transfer.
Vol.18(1)(1997), p. 90 (In Chinese) [11] Zhenwei Ni: Journal of Engineering Thermophysics.
Online since: December 2011
Preface
Those volumes contain papers contributed to The Second International Conference
on Advances in Materials and Manufacturing (ICAMMP 2011) held on 16-18
December 2011 in Guilin, China.
The International Conference on Advances in Materials and Manufacturing Processes is the premier forum for the presentation of new advances and research results in the fields of materials and manufacturing processes.
This conference series will bring together leading researchers, engineers and scientists in the materials and processes field of interest from around the world.
The First International Conference on Advances in Materials and Manufacturing Processes (ICAMMP 2010) was successfully held from November 6-8, 2010 in Shenzhen, China.
All papers published in those volumes of journal of Advanced Materials Research have been peer reviewed through processes administered by the organizing committee.
The International Conference on Advances in Materials and Manufacturing Processes is the premier forum for the presentation of new advances and research results in the fields of materials and manufacturing processes.
This conference series will bring together leading researchers, engineers and scientists in the materials and processes field of interest from around the world.
The First International Conference on Advances in Materials and Manufacturing Processes (ICAMMP 2010) was successfully held from November 6-8, 2010 in Shenzhen, China.
All papers published in those volumes of journal of Advanced Materials Research have been peer reviewed through processes administered by the organizing committee.
Online since: September 2021
Authors: Yuri N. Khakimullin, Rezeda Yu. Galimzyanova, Maria S. Lisanevich
Such materials are hydrophobic in nature.
Materials with the same porosity, but with smaller pores, have a higher hygroscopicity than large-pore materials.
Nonwoven personal hygiene materials and products.
Journal of Materials Science 50, (Springer US, 2015)
Materials (Basel). 9, 1–24 (2016)
Materials with the same porosity, but with smaller pores, have a higher hygroscopicity than large-pore materials.
Nonwoven personal hygiene materials and products.
Journal of Materials Science 50, (Springer US, 2015)
Materials (Basel). 9, 1–24 (2016)
Online since: December 2014
Authors: Jian Jun Wen, Bo Ding, Le Zhang
Journal of petroleum gas technology, 2008, 31 (2) : 618-619.
Fire Science and Technology, 2007, 26(6):654-655.
Journal of Loss Prevention in the Process Industries, 2005, 19 (1): 51-59
Journal of petroleum science and Engineering, 2004, 43(3):151-161
CFD calculations of gas leak dispersion and subsequent gas explosions: validation against ignited impinging hydrogen jet experiments [J].Journal of Hazardous Materials, 2010, 179 (1):84-94
Fire Science and Technology, 2007, 26(6):654-655.
Journal of Loss Prevention in the Process Industries, 2005, 19 (1): 51-59
Journal of petroleum science and Engineering, 2004, 43(3):151-161
CFD calculations of gas leak dispersion and subsequent gas explosions: validation against ignited impinging hydrogen jet experiments [J].Journal of Hazardous Materials, 2010, 179 (1):84-94
Online since: September 2013
Authors: Zhi Jiang Ding, Qiang Li, Li Chun Xiao
You, "Effects of thermophoresis, vapor, and water film on particle removal of electrostatic precipitator," Journal of Aerosol Science, vol. 63(2013), pp. 1-9,
Tsai, "Numerical modeling of nanoparticle collection efficiency of single-stage wire-in-plate electrostatic precipitators," Aerosol Science and Technology, vol. 44(2010), p. 1122-1130
Al-Sheikhly, "Electron beam irradiation for mercury oxidation and mercury emissions control," Journal of Environmental Engineering, vol. 136(2010), p. 554-559
Jianjun, "Experimental study on spraying nozzle arrangement of slab caster," in 2012 International Conference on Chemical Engineering, Metallurgical Engineering and Metallic Materials, CMMM 2012, October 12, 2012 - October 13, 2012, KunMing, China, p. 856-860(2012)
Touchard, "Electrostatic precipitation in wire-to-cylinder configuration: Effect of the high-voltage power supply waveform," Journal of Electrostatics, vol. 67(2009), p. 117-122.
Tsai, "Numerical modeling of nanoparticle collection efficiency of single-stage wire-in-plate electrostatic precipitators," Aerosol Science and Technology, vol. 44(2010), p. 1122-1130
Al-Sheikhly, "Electron beam irradiation for mercury oxidation and mercury emissions control," Journal of Environmental Engineering, vol. 136(2010), p. 554-559
Jianjun, "Experimental study on spraying nozzle arrangement of slab caster," in 2012 International Conference on Chemical Engineering, Metallurgical Engineering and Metallic Materials, CMMM 2012, October 12, 2012 - October 13, 2012, KunMing, China, p. 856-860(2012)
Touchard, "Electrostatic precipitation in wire-to-cylinder configuration: Effect of the high-voltage power supply waveform," Journal of Electrostatics, vol. 67(2009), p. 117-122.
Online since: July 2011
Authors: De Qing Guan, Hong Wei Ying, Xiao Lin Zhong
(4)
Where t is the plate thickness, is Poisson's ratio of the material.
Roeck Guido, Weixin Ren: Journal of Structural Engineering Vol.128 (2002), p. 96-104
Abdel: Journal of Sound and Vibration Vol.226 (1999), p. 217-235
Farrar: Journal of Sound and Vibration Vol. 224 (1999), p. 359–374
Wang: Journal of Engineering Mechanics, ASCE Vol. 124 (1998), p. 152-157
Roeck Guido, Weixin Ren: Journal of Structural Engineering Vol.128 (2002), p. 96-104
Abdel: Journal of Sound and Vibration Vol.226 (1999), p. 217-235
Farrar: Journal of Sound and Vibration Vol. 224 (1999), p. 359–374
Wang: Journal of Engineering Mechanics, ASCE Vol. 124 (1998), p. 152-157
Online since: December 2012
Authors: Yan Hao Zhang, Chang Qing Liu, Min Dong, Xing Sheng Kang, Meng Wang, Jun Shen
Materials and methods
Experimental devices.
Liu: submitted to Journal of Progress in Environmental Science and Technology (2007) [2] C.
Wang: submitted to Journal of Environmental Engineering (2006) [3] F.
Jiang: submitted to Journal of China Water & Wastewater, (2005) [6] C.
Zhao: submitted to Journal of Technology of Water Treatment (2006)
Liu: submitted to Journal of Progress in Environmental Science and Technology (2007) [2] C.
Wang: submitted to Journal of Environmental Engineering (2006) [3] F.
Jiang: submitted to Journal of China Water & Wastewater, (2005) [6] C.
Zhao: submitted to Journal of Technology of Water Treatment (2006)
Online since: January 2013
Authors: Iau Teh Wang, Chin Yu Lee
Influence of Open Channel on Explosion-Induced
Vibration Wave Propagation
Iau-Teh Wang1,2,a, Chin-Yu Lee3,b
1Graduate Institute of Disaster Prevention on Hillslopes and Water Resources Engineering, National Pingtung University of Science and Technology, Pingtung, 912, Taiwan, R.O.C.
2Department of Civil Engineering, Chinese Military Academy, Kaohsiung, 830, Taiwan, R.O.C.
3Department of Soil and Water Conservation, National Pingtung University of Science and Technology, Pingtung, 912, Taiwan, R.O.C.
This study used the LS-DYNA’s No. 9 *MAT_NULL material model to simulate air, and equations of state *EOS_LINEAR_POLYNOMIAL were used to describe the material model as in Eq. (4) [7].
The No. 8 *MAT_HIGH_EXPLOSIVE_BURN material model was used to simulate the high explosive model.
Fotis, Computer simulation of shock waves transmission in obstructed, Journal of Loss Prevention in the Process Industries. 17 (2004) 407-417
Liu, Experimental research on amplitude change of blasting seismic wave with topography, Journal of Beijing Institute of Technology. 9 (2000) 237-242
This study used the LS-DYNA’s No. 9 *MAT_NULL material model to simulate air, and equations of state *EOS_LINEAR_POLYNOMIAL were used to describe the material model as in Eq. (4) [7].
The No. 8 *MAT_HIGH_EXPLOSIVE_BURN material model was used to simulate the high explosive model.
Fotis, Computer simulation of shock waves transmission in obstructed, Journal of Loss Prevention in the Process Industries. 17 (2004) 407-417
Liu, Experimental research on amplitude change of blasting seismic wave with topography, Journal of Beijing Institute of Technology. 9 (2000) 237-242