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Series: ASM Handbook
Volume: 9
Publisher: ASM International
Published: 01 December 2004
DOI: 10.31399/asm.hb.v09.a0003788
EISBN: 978-1-62708-177-1
.... The article also illustrates the microstructure of different types of soft magnetic material and permanent magnets. bitter technique domain imaging Faraday method Lorentz transmission electron microscopy magnetic force microscopy magnetic materials magnetism magneto-optical Kerr method materials...
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Published: 01 December 2004
Fig. 21 Domain imaging using the Faraday effect for a Gd 0.94 Tb 0.75 Er 1.31 Al 0.5 Fe 4.5 O 12 garnet crystal, grown in a PbO and B 2 O 3 flux at 1300 °C (2370 °F). (a) Magnetic domain structure of 50 μm thick platelet cut parallel to the (111) plane. Black and white areas represent More
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Published: 01 December 2004
Fig. 16 Basic imaging of domain walls by the Bitter technique for samples with strain free surfaces is shown in this line drawing. (a) Ferrofluid particles collect at domain walls due to the fringe field associated with the magnetization rotation through the wall width and the particle More
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Published: 01 December 2004
Fig. 15 Bitter domain images of a nickel-cobalt single crystal thick film using dark-field imaging and a microscope with attached field coils. (a) Demagnetized sample with no applied field showing the closure domains. (b) An applied field of 3.6 Oe to the right makes the domain walls More
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Published: 01 December 2004
Fig. 22 Domain images of a barium ferrite single crystal (85 μm thick) with hexagonal plane normal to the plane of the sample. (a) Faraday effect image showing the characteristic domain structure throughout the thickness of the sample. (b) Bitter pattern of the same area as (a), indicating More
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Published: 01 December 2004
Fig. 36 Comparison of Kerr microscopy domain image (a) with magnetic force microscopy images (c) and (d) for a “fir-tree” domain structure, typical of slight misorientation from the (100) surface of an αFe whisker. (b) Indicates the direction of the magnetization for each of the chevrons More
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Published: 01 December 2004
of polarization rotation upon reflection. (b) Adjusting the analyzer for maximum contrast provides a domain image with light/dark contrast for magnetization in the up/down orientations, respectively. More
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Published: 01 December 2004
Fig. 32 A ray diagram for the Fresnel imaging of magnetic domains using a transmission electron microscope. (a) When the current to the objective lens is increased above the in-focus condition, the image becomes overfocused and the electrons are deflected toward and away from the domain walls More
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Published: 01 December 2004
Fig. 33 A ray diagram illustrating the Foucault imaging of magnetic domains using a transmission electron microscope. The Lorentz force on the electrons passing through the magnetic material causes a deflection of their trajectory. A displacement of the objective aperture allows the electrons More
Series: ASM Handbook Archive
Volume: 10
Publisher: ASM International
Published: 01 January 1986
DOI: 10.31399/asm.hb.v10.a0001767
EISBN: 978-1-62708-178-8
... of the instrumentation and principles of SEM, broadly explaining its capabilities in resolution and depth of field imaging. It describes three additional functions of SEM, including the use of channeling patterns to evaluate the crystallographic orientation of micron-sized regions; use of backscattered detectors...
Book Chapter

Series: ASM Handbook
Volume: 17
Publisher: ASM International
Published: 01 August 2018
DOI: 10.31399/asm.hb.v17.a0006474
EISBN: 978-1-62708-190-0
.... acoustical holography liquid-surface acoustical holography optical holography scanning acoustical holography sleeve-bearing stock through-transmission breast imaging system ACOUSTICAL HOLOGRAPHY is the extension of holography into the ultrasonic domain. The principles of acoustical holography...
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Published: 01 December 2004
to the right and black to the left. (c) Image of the y-component of the magnetization (white contrast upward and black contrast downward). (d) Total in-plane magnetization intensity, with image contrast at the domain walls due to larger probe diameter than the domain wall width. Reproduced with permission from More
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Published: 15 December 2019
Fig. 19 (a) 1 × 1 μm phase image of styrene-ethylene/butylene- styrene polymer. (b) Corresponding topography image. Although the existence of the two domains is observed in (b), the different blocks are more clearly differentiated in (a), enabling a clearer understanding of the morphology More
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Published: 01 December 2004
Fig. 34 Transmission electron micrographs of Fe-55Pd arc-melted alloy annealed at 500 °C (930 °F) for 36 h. (a) Bright-field image of the sample (with [130] zone axis) exhibiting a polytwinned microstructure. (b) Lorentz under-focus (Fresnel) image of the sample showing the immobile domain More
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Published: 01 December 2004
of the sample. The resulting SE image has contrast variation across the width of the domain with peak brightness and darkness at the domain walls. More
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Published: 01 December 2004
Fig. 28 Secondary electron image of a Nd 2 Fe 14 B single crystal grown using flux growth synthesis. Type I magnetic contrast clearly shows the maze pattern domains, typical of these uniaxial materials. The large depth of field, characteristic of scanning electron imaging techniques More
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Published: 01 December 2004
Fig. 18 As-cast Fe 80 B 18.3 P 1.7 metallic glass alloy. Complex magnetic domain structure resulting from the residual stress pattern due to rapid-solidification processing. Dark-field imaging and the Bitter powder pattern technique were used to produce this image. Reproduced with permission More
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Published: 01 January 1997
Fig. 6 Topology optimization examples of a frame structure. (a) Initial frame structure showing design domain. (b) First three natural mode shapes. (c) Optimal material distribution from topology optimization as computed and after filtering the topology image to simplify the structural layout More
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Published: 31 August 2017
Fig. 15 Three-dimensional (3-D) simulated microstructure evolution during divorced eutectic solidification of a spheroidal graphite iron. (a) Solid fraction ( f s ) = 0.24. (b) f s = 0.55. (c) f s = 0.99. (Images taken at the center of a 3-D calculation domain). Source: Ref 63 More
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Published: 01 November 2010
Fig. 13 (a) Image of a cellular automaton simulation of solidification in a Zn-0.2wt%Al galvanized coating. The 5 by 3 mm domain is cooled at –12 K/s with a positive temperature gradient from left to right. (b) Experimental and calculated number densities of grains as a function of the cooling More