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<title>David Sellmyer Publications</title>
<copyright>Copyright (c) 2009 University of Nebraska - Lincoln All rights reserved.</copyright>
<link>http://digitalcommons.unl.edu/physicssellmyer</link>
<description>Recent documents in David Sellmyer Publications</description>
<language>en-us</language>
<lastBuildDate>Sat, 12 Sep 2009 23:25:49 PDT</lastBuildDate>
<ttl>3600</ttl>


	

	

	




<item>
<title>IGC Fabrication and TEM Characterization of Mn Nanoparticles</title>
<link>http://digitalcommons.unl.edu/physicssellmyer/219</link>
<guid isPermaLink="true">http://digitalcommons.unl.edu/physicssellmyer/219</guid>
<pubDate>Fri, 11 Sep 2009 11:44:23 PDT</pubDate>
<description>The reason for the enormous interest in nanomaterials is because they display unique and superior properties that are generally unavailable in conventional macroscopic materials. Gleiter and coworkers [1] first generated a novel solid structure with gas-like disorder, in addition to long-range order (crystalline and quasicrystalline solids) and short-range order (amorphous/glassy solids). Inert-gas condensation (IGC) is a well established nanoparticle production technique [2-4]. Figure 1 shows an IGC system equipped with magnetron sputter source and mass selector that was used in the present work. The ability to control the process parameters to fabricate metal nanoparticles with tailored size, shape, and properties is important for research in this area.</description>

<author>Xingzhong Li</author>


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<title>TEM/QED Study of FePt Ultrathin Films and Co/CoO Core-Shell Particles</title>
<link>http://digitalcommons.unl.edu/physicssellmyer/218</link>
<guid isPermaLink="true">http://digitalcommons.unl.edu/physicssellmyer/218</guid>
<pubDate>Fri, 11 Sep 2009 11:42:16 PDT</pubDate>
<description>Transmission electron microscopy (TEM) imaging and electron diffraction (ED) techniques are widely used in the studies of thin films and nanoparticles. Although various advanced techniques have been well established, such as high-resolution electron microscopy (HREM) and convergent beam electron diffraction (CBED), the conventional TEM imaging and selected-area electron diffraction (SAED) techniques remain the essential methods for microstructure and crystal structure characterization. Digital TEM image processing and quantitative ED analysis (QED) has become one trend for improvements. Recently computer programs [1,2] have been developed for analysis of SAED patterns of polycrystalline phases. In this paper, we report the preliminary results on a TEM/QED study of FePt ultrathin films and Co/CoO core shell particles.</description>

<author>Xingzhong Li</author>


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<title>TEM Study of FePt and FePt:C Composite Double-layered Thin Films</title>
<link>http://digitalcommons.unl.edu/physicssellmyer/217</link>
<guid isPermaLink="true">http://digitalcommons.unl.edu/physicssellmyer/217</guid>
<pubDate>Fri, 11 Sep 2009 11:38:57 PDT</pubDate>
<description>FePt films and FePt-based nano-composite films with the high-anisotropy L10 ordered phase have
been extensively studied, since they have significant potential for extremely high-density
perpendicular magnetic recording media and nano-composite permanent magnets [1]. Recently, new
functional films were synthesized with a FePt:C composite layer on top of continuous FePt layer, in
order to study the effect of the FePt layer on the ordering, orientation and magnetic properties of the
composite layer. Transmission electron microscopy (TEM), together with X-ray diffraction, has been
used to check the growth of the double-layered films and to study the microstructure, including the
grain size, shape, orientation and distribution. The results have been used as feedback to improve the
film synthesis and to analyze the structures related to novel functions of the designed films. In this
report, the TEM studies of both single-layered nonepitaxially grown FePt and FePt:C composite L10
phase and double-layered deposition FePt:C/FePt are presented.</description>

<author>Xingzhong Li</author>


</item>


<item>
<title>Anisotropic Sm-(Co,Fe) Nanoparticles by Surfactant-assisted Ball Milling</title>
<link>http://digitalcommons.unl.edu/physicssellmyer/216</link>
<guid isPermaLink="true">http://digitalcommons.unl.edu/physicssellmyer/216</guid>
<pubDate>Mon, 06 Apr 2009 13:29:03 PDT</pubDate>
<description>Magnetically hard Sm2(Co0.8Fe0.2)17 and SmCo5 nanoparticles have been produced by using
surfactant-assisted low- and high-energy ball milling techniques. Surfactants prevent the rewelding
of the crashed particles during the milling process. Heptane was used as the milling medium and
oleic acid as the surfactant. High-energy ball milling experiments took place in a milling vial with
carbon steel balls by using an SPEX 8000M high-energy ball milling machine. The coercivity was
found to increase with milling time with values of 2.3 kOe for Sm2(Co0.8Fe0.2)17 and 18.6 kOe for
SmCo5 after 4 h of milling. Transmission electron microscopy data showed that the milled powders
consisted of nanoparticles with an average size of 5-6 nm and a narrow size distribution. Samples
deposited on copper coated carbon grid showed self-assembled nanoparticles which could be further
aligned when subjected to a magnetic field.</description>

<author>Nilly Akdogan</author>


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<item>
<title>Microstructures and Magnetic Properties of Rapidly Solidified Ni&lt;sub&gt;54&lt;/sub&gt;Fe&lt;sub&gt;27&#8722;2x&lt;/sub&gt;Ga&lt;sub&gt;19+2x&lt;/sub&gt; Ferromagnetic Heusler Alloys</title>
<link>http://digitalcommons.unl.edu/physicssellmyer/215</link>
<guid isPermaLink="true">http://digitalcommons.unl.edu/physicssellmyer/215</guid>
<pubDate>Mon, 06 Apr 2009 13:29:02 PDT</pubDate>
<description>Rapidly solidified Ni54Fe27&#8722;2xGa19+2x (x=0, 1, 2, 3, and 4) ferromagnetic shape memory alloys were
made by melt-spinning with variation of Fe and Ga contents to report on the martensitic phase
transformation, microstructures, and magnetic properties. Rapid solidification produced pure L21
phase by preventing the formation of &#947;-phase. To study the effect of heat treatment on the phase
transitions, microstructures, and the magnetic properties, the melt-spun ribbons were partly heat
treated at different temperatures of 800, 900, 1000, 1100, and 1200 K with holding times of 5, 10,
and 15 min followed by either water quenching or air cooling. The microstructures of the as-spun
ribbons as revealed by electron microscopy studies exhibited a gradual transition from cellular to
dendritic structure with increasing Ga concentration and with the presence of some internal
martensitic twin bands at higher Ga content. The ribbons exhibited very low coercivity with high
saturation magnetization, as high as ~87 em/g (decreasing with Ga concentration). The
above-ambient Curie temperature (TC) and the subambient martensitic transition temperature (Tm)
were observed to be ~320 and ~195 K, respectively. At higher heat treatment temperatures
formation of ductile &#947; phases was observed.</description>

<author>S. Aich</author>


</item>


<item>
<title>Elemental Mapping of Co-Pr Nanostructured Powders by EELS Image Filtering</title>
<link>http://digitalcommons.unl.edu/physicssellmyer/214</link>
<guid isPermaLink="true">http://digitalcommons.unl.edu/physicssellmyer/214</guid>
<pubDate>Mon, 06 Apr 2009 13:29:01 PDT</pubDate>
<description>In current extremely high density recording media design, the signal to noise ratio SNR is related to the
number of magnetic grains N in a recording bit by 
SNR = 10 logl0 N .................................... (1)
In earlier studies we have found that a metallurgical grain can act as a magnetic grain when
grains are magnetically decoupled by a non-magnetic phase [1,2]. Alternatively, several
metallurgical grains can be exchange-coupled together when they are small [3]. An ideal
morphology is one in which the non-magnetic atoms are segregated at the grain boundaries
forming the non-magnetic phase while keeping the grains closely packed.</description>

<author>Yi Liu</author>


</item>


<item>
<title>The Magnetism-Nanostructure Interface in Advanced Magnetic Materials</title>
<link>http://digitalcommons.unl.edu/physicssellmyer/213</link>
<guid isPermaLink="true">http://digitalcommons.unl.edu/physicssellmyer/213</guid>
<pubDate>Mon, 06 Apr 2009 13:28:59 PDT</pubDate>
<description>The critical relationship between microstructure and nanostructure of materials and their magnetic
properties has been appreciated for decades. Electromagnetic machinery, permanent magnets, and
data recording and electronic devices all have seen steady and sometimes spectacular advances over
this period. At the present time the most interesting research in magnetism and magnetic materials
arises from new developments in structuring materials on the nanometer length scale. This talk will
present recent advances and challenges in furthering this work, with particular attention paid to
extremely high density magnetic recording films, exchange-coupled high-energy-product
permanent-magnet materials, high-temperature permanent-magnet materials, and self-organized and
patterned magnetic nanoarrays.</description>

<author>David J. Sellmyer</author>


</item>


<item>
<title>Selected Reflection Imaging: A Useful Tool for Imaging Nanocomposite Magnetic Materials</title>
<link>http://digitalcommons.unl.edu/physicssellmyer/212</link>
<guid isPermaLink="true">http://digitalcommons.unl.edu/physicssellmyer/212</guid>
<pubDate>Mon, 06 Apr 2009 13:28:58 PDT</pubDate>
<description>The great strength of transmission electron microscope (TEM) is its capability to access to both real
space (imaging) and reciprocal space (diffraction). Selected reflection imaging (SRI) can relate the
diffraction of nanostructured materials with the image, providing information otherwise not possible.
The experimental set up of SRI is given by Liu and Sellmyer [I]. In this paper we present some new
measurements on nanocomposite magnetic materials.</description>

<author>Yi Liu</author>


</item>


<item>
<title>Electrodeposition and Magnetic Properties of Polypyrrole-Fe Nanocomposites</title>
<link>http://digitalcommons.unl.edu/physicssellmyer/211</link>
<guid isPermaLink="true">http://digitalcommons.unl.edu/physicssellmyer/211</guid>
<pubDate>Tue, 27 Jan 2009 09:37:02 PST</pubDate>
<description>The synthesis, structure, and magnetic properties of a new composite material obtained by the codeposition of polypyrrole and
iron, in the galvanostatic mode, using square wave potentials are reported. The effect of electrodeposition conditions (voltage and
concentration of the electrolytes) on the magnetic properties of the nanocomposite is analyzed.</description>

<author>Mircea Chipara</author>


</item>


<item>
<title>Structure, magnetic properties, and exchange coupling in thermally processed NdDyFeCoB/&#945;-Fe nanoscale multilayer magnets</title>
<link>http://digitalcommons.unl.edu/physicssellmyer/210</link>
<guid isPermaLink="true">http://digitalcommons.unl.edu/physicssellmyer/210</guid>
<pubDate>Wed, 18 Jun 2008 09:22:58 PDT</pubDate>
<description>The structure and magnetic properties of multilayer magnets with a hard phase (HP1
=NdM13.5Dy1.5Fe68Co10&#60;/sub&#60;B7 or HP2=Nd14Dy1Fe68Co10B7) and soft phase Fe, prepared by sputtering
and subsequent heat treatment, have been investigated. For Si/Ti(20 nm)/[HP1(2.0 nm)/Fe(0.5 nm)] x 200/Ti(10 nm) multilayer film, transmission electron microscopy
results show that Fe disperses in amorphous NdDyFeCoB alloy. After annealing at 575 °C for
5 min, the hard Nd2Fe14B phase typically with grains of about 50 nm and some amount of &#945;-Fe
coexist in the film. The grain size of the hard and soft phases can be controlled by the proper
thickness of the layer and the period. A coercivity of 7.7 kOe and a ratio Mr/Ms of 0.74 are achieved
in the multilayer Si/Ti(20 nm) /&#61472;[HP2(2 nm) /Fe(0.5 nm)]x200/Ti(10 nm). A good squareness of
the hysteresis loop (measured even at 200 K) is observed, due to the effective exchange coupling
between the magnetically soft and hard nanograins in the film. A pinning-type mechanism
dominates the magnetization reversal process. In addition, the effect of the effective anisotropy, the
grain size, and interfaces between the magnetically hard and soft phases on the exchange coupling
is discussed.</description>

<author>W. Liu</author>


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