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Books on the topic 'Near field magnetic enhancement'

Author: Grafiati
Published: 28 June 2021
Last updated: 9 February 2022

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1

Sulaiman, Ali Haidar. The Near-Saturn Magnetic Field Environment. Cham: Springer International Publishing, 2017. http://dx.doi.org/10.1007/978-3-319-49292-6.

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2

Hill, David A. Near-field and far-field excitation of a long conductor in a lossy medium. Boulder, Colo: Electromagnetic Fields Division, Center for Electronics and Electrical Engineering, National Engineering Laboratory, National Institute of Standards and Technology, 1990.

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3

Hill, David A. Near-field and far-field excitation of a long conductor in a lossy medium. Boulder, Colo: Electromagnetic Fields Division, Center for Electronics and Electrical Engineering, National Engineering Laboratory, National Institute of Standards and Technology, 1990.

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4

Hill, David A. Near-field and far-field excitation of a long conductor in a lossy medium. Boulder, Colo: Electromagnetic Fields Division, Center for Electronics and Electrical Engineering, National Engineering Laboratory, National Institute of Standards and Technology, 1990.

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5

Hill, David A. Near-field and far-field excitation of a long conductor in a lossy medium. Boulder, Colo: Electromagnetic Fields Division, Center for Electronics and Electrical Engineering, National Engineering Laboratory, National Institute of Standards and Technology, 1990.

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6

Hill, David A. Near-field and far-field excitation of a long conductor in a lossy medium. Boulder, Colo: Electromagnetic Fields Division, Center for Electronics and Electrical Engineering, National Engineering Laboratory, National Institute of Standards and Technology, 1990.

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7

Denkova, Denitza. Optical Characterization of Plasmonic Nanostructures: Near-Field Imaging of the Magnetic Field of Light. Cham: Springer International Publishing, 2016. http://dx.doi.org/10.1007/978-3-319-28793-5.

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8

Sulaiman, Ali Haidar. The Near-Saturn Magnetic Field Environment. Springer, 2018.

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9

Sulaiman, Ali Haidar. The Near-Saturn Magnetic Field Environment. Springer, 2016.

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10

1966-, Kawata Satoshi, and Shalaev Vladimir M. 1957-, eds. Tip enhancement. Amsterdam: Elsevier, 2007.

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11

Denkova, Denitza. Optical Characterization of Plasmonic Nanostructures: Near-Field Imaging of the Magnetic Field of Light. Springer, 2016.

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12

Denkova, Denitza. Optical Characterization of Plasmonic Nanostructures: Near-Field Imaging of the Magnetic Field of Light. Springer, 2018.

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13

Hayazawa, Norihiko, and Prabhat Verma. Nanoanalysis of materials using near-field Raman spectroscopy. Edited by A. V. Narlikar and Y. Y. Fu. Oxford University Press, 2017. http://dx.doi.org/10.1093/oxfordhb/9780199533053.013.10.

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This article describes the use of tip-enhanced near-field Raman spectroscopy for the characterization of materials at the nanoscale. Tip-enhanced near-field Raman spectroscopy utilizes a metal-coated sharp tip and is based on surface-enhanced Raman scattering (SERS). Instead of the large surface enhancement from the metallic surface in SERS, the sharp metal coated tip in the tip-enhanced Raman scattering (TERS) provides nanoscaled surface enhancement only from the sample molecules in the close vicinity of the tip-apex, making it a perfect technique for nanoanalysis of materials. This article focuses on near-field analysis of some semiconducting nanomaterials and some carbon nanostructures. It first considers SERS analysis of strained silicon and TERS analysis of epsilon-Si and GaN thin layers before explaining how to improve TERS sensitivity and control the polarization in detection for crystalline materials. It also discusses ways of improving the spatial resolution in TERS.
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14

(Editor), Satoshi Kawata, and Vladimir M. Shalaev (Editor), eds. Tip Enhancement (Advances in Nano-Optics and Nano-Photonics). Elsevier Science, 2007.

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15

Uchida, K., R. Ramos, and E. Saitoh. Spin Seebeck effect. Oxford University Press, 2017. http://dx.doi.org/10.1093/oso/9780198787075.003.0018.

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Chapter 18 This chapter discusses the spin Seebeck effect (SSE), which stands for the generation of a spin current, a flow of spinangular momentum, as a result of a temperature gradient in magnetic materials. In spintronics and spin caloritronics, the SSE is of crucial importance because it enables simple and versatile generation of a spin current from heat. Since the SSE is driven by thermally excited magnon dynaimcs, the thermal spin current can be generated not only from ferromagnetic conductors but also from insulators. Therefore, the SSE is applicable to “insulator-based thermoelectric conversion” which was impossible if only conventional thermoelectric technologies were used. In this chapter, after introducing basic characteristics and mechanisms of the SSE, important experimental progresses, such as the high-magnetic-field response of the SSE and the enhancement of the SSE in multilayer systems, are reviewed.
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16

Sergeenkov, Sergei. 2D arrays of Josephson nanocontacts and nanogranular superconductors. Edited by A. V. Narlikar and Y. Y. Fu. Oxford University Press, 2017. http://dx.doi.org/10.1093/oxfordhb/9780199533046.013.21.

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This article examines many novel effects related to the magnetic, electric, elastic and transport properties of Josephson nanocontacts and nanogranular superconductors using a realistic model of two-dimensional Josephson junction arrays. The arrays were created by a 2D network of twin-boundary dislocations with strain fields acting as an insulating barrier between hole-rich domains in underdoped crystals. The article first describes a model of nanoscopic Josephson junction arrays before discussing some interesting phenomena, including chemomagnetism and magnetoelectricity, electric analog of the ‘fishtail‘ anomaly and field-tuned weakening of the chemically induced Coulomb blockade, a giant enhancement of the non-linear thermal conductivity in 2D arrays, and thermal expansion of a singleJosephson contact.
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17

Hong, M. H. Laser applications in nanotechnology. Edited by A. V. Narlikar and Y. Y. Fu. Oxford University Press, 2017. http://dx.doi.org/10.1093/oxfordhb/9780199533060.013.24.

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This article discusses a variety of laser applications in nanotechnology. The laser has proven to be one of many mature and reliable manufacturing tools, with applications in modern industries, from surface cleaning to thin-film deposition. Laser nanoengineering has several advantages over electron-beam and focused ion beam processing. For example, it is a low-cost, high-speed process in air, vacuum or chemical environments and also has the capability to fulfill flexible integration control. This article considers laser nanotechnology in the following areas: pulsed laser ablation for nanomaterials synthesis; laser nanoprocessing to make nanobumps for disk media nanotribology and anneal ultrashort PN junctions; surface nanopatterning with near-field, and light-enhancement effects; and large-area parallel laser nanopatterning by laser interference lithography and laser irradiation through a microlens array. Based on these applications, the article argues that the laser will continue to be one of the highly potential nanoengineering means in next-generation manufacturing.
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18

Epstein, Charles M. TMS stimulation coils. Edited by Charles M. Epstein, Eric M. Wassermann, and Ulf Ziemann. Oxford University Press, 2012. http://dx.doi.org/10.1093/oxfordhb/9780198568926.013.0004.

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The simplest transcranial magnetic stimulation (TMS) coil is a circular one. The induced current is maximum near the outer edge of the coil while the magnetic field is the maximum under the center of the coil. TMS coils have good penetration to the cerebral cortex. They are commonly placed at the cranial vertex, where they can stimulate both hemispheres simultaneously. The main drawback of circular coils is their lack of focality. Several complex designs for multiloop coils have been proposed to increase the focality or improve the penetration to deep brain structures. This article describes factors of TMS coil design such as mechanical forces and coil lead wires, cooling systems, materials of construction of coil windings, etc. To reduce the risk of lethal electrical shock the entire high-voltage power system, including the lead wires and stimulation coil, must be isolated from earth ground.
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19

Narlikar, A. V., and Y. Y. Fu, eds. Oxford Handbook of Nanoscience and Technology. Oxford University Press, 2017. http://dx.doi.org/10.1093/oxfordhb/9780199533053.001.0001.

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This Handbook presents important developments in the field of nanoscience and technology, focusing on the advances made with a host of nanomaterials including DNA and protein-based nanostructures. Topics include: optical properties of carbon nanotubes and nanographene; defects and disorder in carbon nanotubes; roles of shape and space in electronic properties of carbon nanomaterials; size-dependent phase transitions and phase reversal at the nanoscale; scanning transmission electron microscopy of nanostructures; the use of microspectroscopy to discriminate nanomolecular cellular alterations in biomedical research; holographic laser processing for three-dimensional photonic lattices; and nanoanalysis of materials using near-field Raman spectroscopy. The volume also explores new phenomena in the nanospace of single-wall carbon nanotubes; ZnO wide-bandgap semiconductor nanostructures; selective self-assembly of semi-metal straight and branched nanorods on inert substrates; nanostructured crystals and nanocrystalline zeolites; unusual properties of nanoscale ferroelectrics; structural, electronic, magnetic, and transport properties of carbon-fullerene-based polymers; fabrication and characterization of magnetic nanowires; and properties and potential of protein-DNA conjugates for analytic applications.
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20

Saitoh, E., and K. Ando. Experimental observation of the spin Hall effect using spin dynamics. Oxford University Press, 2017. http://dx.doi.org/10.1093/oso/9780198787075.003.0015.

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This chapter describes an experiment on the inverse spin Hall effect (ISHE) induced by spin pumping. Spin pumping is the generation of spin currents as a result of magnetization M(t) precession; in a ferromagnetic/paramagnetic bilayer system, a conduction-electron spin current is pumped out of the ferromagnetic layer into the paramagnetic conduction layer in a ferromagnetic resonance condition. The sample used in the experiment is a Ni81Fe19/Pt bilayer film comprising a 10-nm-thick ferromagnetic Ni81Fe19layer and a 10-nm-thick paramagnetic Pt layer. For the measurement, the sample system is placed near the centre of a TE011 microwave cavity at which the magnetic-field component of the microwave mode is maximized while the electric-field component is minimized.
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