{"currentpage":1,"firstResult":0,"maxresult":10,"pagecode":5,"pageindex":{"endPagecode":5,"startPagecode":1},"records":[{"abstractinfo":"The C15 Laves phases with composition Nd(1-x)Pr(x)(Fe(0.35)Co(0.55)B(0.1))(2) (0 <= x <= 1) have been synthesized by arc melting and subsequent annealing. The Curie temperature T(c) and the saturation magnetizations M(s) at 5 and 295 K decrease with increasing Pr content. The linear anisotropic <span style=\"color:red\">magnetostriction</span> lambda(a) = lambda(parallel to)-lambda(perpendicular to) at room temperature for Nd(1-x)Pr(x)(Fe(0.35)Co(0.55)B(0.1))(2) <span style=\"color:red\">alloys</span> with 0 <= x <= 0.4 initially reaches a negative minimum, then increases and changes its sign with increasing <span style=\"color:red\">magnetic</span> field H, and the lambda(a) for the <span style=\"color:red\">alloys</span> with x >= 0.6 is positive and increases as <span style=\"color:red\">magnetic</span> field H increases. (C) 2008 Elsevier B.V. All rights reserved.","authors":[],"categoryName":"|","doi":"","fpage":"2373","id":"3cece505-7e50-4bfd-af8e-d6a306924200","issue":"19","journal":{"abbrevTitle":"JOMAMM","id":"5d7a0764-3359-4184-bc25-ad22bbdaf30a","issnPpub":"0304-8853","publisherId":"JOMAMM","title":"Journal of Magnetism and Magnetic Materials"},"keywords":[{"id":"c9108560-935b-4251-ac9b-386d82098cc0","keyword":"<span style=\"color:red\">structure</span>;<span style=\"color:red\">magnetic</span> <span style=\"color:red\">property</span>;<span style=\"color:red\">magnetostriction</span>;<span style=\"color:red\">phase</span>;<span style=\"color:red\">alloys</span>;<span style=\"color:red\">boron</span>","originalKeyword":"structure;magnetic property;magnetostriction;phase;alloys;boron"}],"language":"en","publisherId":"0304-8853_2008_19_1","title":"<span style=\"color:red\">Structure</span>, <span style=\"color:red\">magnetic</span> properties and <span style=\"color:red\">magnetostriction</span> of laves compounds Nd(1-x)Pr(x)(Fe(0.35)Co(0.55)B(0.1))(2)","volume":"320","year":"2008"},{"abstractinfo":"<span style=\"color:red\">Structure</span>, <span style=\"color:red\">magnetic</span> properties and <span style=\"color:red\">magnetostriction</span> of Tb1-x,PrxFe1.93B0.15 (0 less than or equal to x less than or equal to 0.8) <span style=\"color:red\">alloys</span> are investigated. Addition of a small amount of <span style=\"color:red\">boron</span> and extra rare earth is beneficial to the formation of a single Laves <span style=\"color:red\">phase</span>. Single <span style=\"color:red\">phase</span> Tb1-xPrxFe1.93B0.15 with cubic MgCu2-type <span style=\"color:red\">structure</span> forms up to x = 0.3 as determined by X-ray diffraction. In the range of high Pr content, the <span style=\"color:red\">boron</span> atoms preferentially combine with rare-earth atoms to form the Nd2Fe14B-type <span style=\"color:red\">phase</span>. The results of lattice parameter and Curie temperature show that the Pr solubility limit for Tb1-xPrxFe1.93B0.15 is reached in the range of x from 0.3 to 0.5. Large spontaneous <span style=\"color:red\">magnetostriction</span> of chi(111) > 2100ppm is observed for the Laves phases in the Tb1-x,PrxFe1.93B0.15 <span style=\"color:red\">alloys</span> with 0 less than or equal to x less than or equal to 0.3. Linear <span style=\"color:red\">magnetostriction</span> at room temperature of the single <span style=\"color:red\">phase</span> Tb1-x,PrxFe1.93B0.15 <span style=\"color:red\">alloys</span> decreases with increasing Pr content. (C) 2003 Elsevier B.V. All rights reserved.","authors":[],"categoryName":"|","doi":"","fpage":"281","id":"8d069c76-0d93-4422-9d88-a286b04feaa6","issue":"2","journal":{"abbrevTitle":"JOMAMM","id":"5d7a0764-3359-4184-bc25-ad22bbdaf30a","issnPpub":"0304-8853","publisherId":"JOMAMM","title":"Journal of Magnetism and Magnetic Materials"},"keywords":[{"id":"9fe907b4-ed11-4265-9dab-589740de2612","keyword":"<span style=\"color:red\">magnetostriction</span>;rare-earth transition-metal compounds;MgCu2-type;<span style=\"color:red\">structure</span>;laves <span style=\"color:red\">phase</span>-compounds;compound;<span style=\"color:red\">boron</span>","originalKeyword":"magnetostriction;rare-earth transition-metal compounds;MgCu2-type;structure;laves phase-compounds;compound;boron"}],"language":"en","publisherId":"0304-8853_2004_2_1","title":"<span style=\"color:red\">Structure</span> and <span style=\"color:red\">magnetostriction</span> of Tb1-xPrxFe1.93B0.15 <span style=\"color:red\">alloys</span>","volume":"269","year":"2004"},{"abstractinfo":"The crystal and the <span style=\"color:red\">magnetic</span> structures as well as <span style=\"color:red\">magnetostriction</span> of the Laves-<span style=\"color:red\">phase</span> compound NdCo2 are investigated by means of temperature-dependent high-resolution neutron-powder diffraction. The compound crystallizes in the cubic Laves <span style=\"color:red\">phase</span> C15 <span style=\"color:red\">structure</span> at high temperature, undergoes a tetragonal distortion (space group I4l/amd) around T(C)approximate to 100 K and an orthorhombic distortion (space group Fddd) at T 42 K. The temperature dependence of lattice constants, <span style=\"color:red\">magnetostriction</span> constant, and <span style=\"color:red\">magnetic</span> moment indicate that the <span style=\"color:red\">magnetic</span> and structural transitions are second order in the vicinity of T-C and are first-order around 42 K. Refinements of <span style=\"color:red\">magnetic</span> <span style=\"color:red\">structure</span> reveal that the Nd moment distinctly exhibits an abrupt increase at the first-order transition and the easy magnetization direction of the compound changes from [001] in the tetragonal lattice to [011] in the orthorhombic lattice, indicating a strong coupling between crystal <span style=\"color:red\">structure</span> and <span style=\"color:red\">magnetic</span> properties at zero field. Analysis of the temperature dependence of bondlength suggests a strong <span style=\"color:red\">magnetic</span> exchange striction in the tetragonal <span style=\"color:red\">structure</span> and that the abrupt increase of the Nd moment is attributed essentially to a change in crystal electric field. Field-dependent neutron diffraction reveals a decoupling of the <span style=\"color:red\">magnetic</span> and structural transitions under relatively modest <span style=\"color:red\">magnetic</span> fields.","authors":[],"categoryName":"|","doi":"","fpage":"","id":"402d51f4-0d48-433b-b470-27ef46127306","issue":"6","journal":{"abbrevTitle":"PRB","id":"48ba155b-d6de-484c-bd85-973be949b8c5","issnPpub":"1098-0121","publisherId":"PRB","title":"Physical Review B"},"keywords":[{"id":"ca19edca-fcb8-4d59-9306-08cd47887a9a","keyword":"itinerant-electron metamagnetism;neutron powder-diffraction;intermetallic compounds;exchange;heavy;light;hoco2;order","originalKeyword":"itinerant-electron metamagnetism;neutron powder-diffraction;intermetallic compounds;exchange;heavy;light;hoco2;order"}],"language":"en","publisherId":"1098-0121_2005_6_1","title":"<span style=\"color:red\">Magnetic</span> <span style=\"color:red\">structure</span>, <span style=\"color:red\">magnetostriction</span>, and <span style=\"color:red\">magnetic</span> transitions of the Laves-<span style=\"color:red\">phase</span> compound NdCO2","volume":"71","year":"2005"},{"abstractinfo":"Crystal <span style=\"color:red\">structure</span>, <span style=\"color:red\">magnetic</span> properties and <span style=\"color:red\">magnetostriction</span> of Dy0.7Pr0.3(Fe1-xBx)(2) (0less than or equal toxless than or equal to0.20) have been investigated by means of x-ray diffraction, ac initial susceptibility, a vibrating sample magnetometer, and a standard strain technique. The matrix of Dy0.7Pr0.3Fe2 alloy consists of (Dy,Pr)Fe-2 <span style=\"color:red\">phase</span> with a cubic MgCu2-type <span style=\"color:red\">structure</span> and some amount of (Dy,Pr)Fe-3 <span style=\"color:red\">phase</span> with a rhombohedral PuNi3-type <span style=\"color:red\">structure</span>. The introduction of <span style=\"color:red\">boron</span> effectively restrains the emergence of the iron-rich <span style=\"color:red\">phase</span> and thus decreases the amount of (Dy,Pr)Fe-3 <span style=\"color:red\">phase</span>. Dy0.7Pr0.3(Fe1-xBx)(2) alloy with x=0.05 contains small amount of (Dy,Pr)(Fe,B)(3) <span style=\"color:red\">phase</span>, and those with x=0.10 and x=0.15 are essentially of a single (Dy,Pr)(Fe,B)(2) <span style=\"color:red\">phase</span>. An unidentified minor <span style=\"color:red\">phase</span> appears when x=0.20. The lattice parameter of (Dy,Pr)(Fe,B)(2) <span style=\"color:red\">phase</span> decreases monotonically with the <span style=\"color:red\">boron</span> substitution up to x=0.20, indicating that the <span style=\"color:red\">boron</span> atoms occupy the substitutional sites. The Curie temperature for (Dy,Pr)(Fe,B)(2) <span style=\"color:red\">phase</span> obviously increases compared with the <span style=\"color:red\">boron</span> free one. The saturation magnetization at room temperature increases with increasing <span style=\"color:red\">boron</span> content for the <span style=\"color:red\">alloys</span> studied, suggesting that the partial <span style=\"color:red\">boron</span> substitution is beneficial to the increment of the exchange interactions in the Dy0.7Pr0.3Fe2 system. The increment of the magnetization originates from the decrement of iron content, because the Fe moment that aligns antiparallel with the Dy moment almost keeps constant in this system. <span style=\"color:red\">Boron</span> substitution for iron increases the lattice distortion and anisotropy, thus causes the decrease of the linear <span style=\"color:red\">magnetostriction</span> lambda(a)=lambda(parallel to)-lambda(perpendicular to) at the room temperature. (C) 2002 American Institute of Physics.","authors":[],"categoryName":"|","doi":"","fpage":"8207","id":"b06cca13-4b2d-4f35-b03c-d6832bc5f81c","issue":"10","journal":{"abbrevTitle":"JOAP","id":"7dcf8a89-0513-40ee-be2d-759941dcef7e","issnPpub":"0021-8979","publisherId":"JOAP","title":"Journal of Applied Physics"},"keywords":[{"id":"fa7737af-8c7b-4a56-8835-fee845e63334","keyword":"tb0.3dy0.7fe2 alloy","originalKeyword":"tb0.3dy0.7fe2 alloy"}],"language":"en","publisherId":"0021-8979_2002_10_4","title":"Effect of <span style=\"color:red\">boron</span> on <span style=\"color:red\">structure</span> and <span style=\"color:red\">magnetic</span> properties of magnetostrictive compound Dy0.7Pr0.3Fe2","volume":"91","year":"2002"},{"abstractinfo":"The <span style=\"color:red\">structure</span>, Curie temperature, and <span style=\"color:red\">magnetostriction</span> of SmZn1-xMnx polycrystalline crystals were investigated by x-ray diffraction, vibrating-sample magnetometer, and standard strain gauge techniques. It is found that SmZn1-xMnx <span style=\"color:red\">alloys</span> are nearly a single Sm(Zn,Mn) <span style=\"color:red\">phase</span> with the CsCl-type cubic <span style=\"color:red\">structure</span> up to x=0.2. The Curie temperature of SmZn1-xMnx <span style=\"color:red\">alloys</span> quickly increases with increasing Mn when x <= 0.05 and gradually does in the range of 0.05 < x <= 0.2. The substitution of Mn for Zn in the SmZn compound has a marked effect on improving the Curie temperature and makes it reach 255 K when x=0.2. The magnetization of SmZn1-xMnx <span style=\"color:red\">alloys</span> increases with increasing Mn content in the range of 0 < x <= 0.2 and the <span style=\"color:red\">magnetostriction</span> increases in the range of 0 < x <= 0.15. (c) 2006 American Institute of Physics.","authors":[],"categoryName":"|","doi":"","fpage":"","id":"35f912c5-fb51-428c-8c28-8e392455a287","issue":"4","journal":{"abbrevTitle":"JOAP","id":"7dcf8a89-0513-40ee-be2d-759941dcef7e","issnPpub":"0021-8979","publisherId":"JOAP","title":"Journal of Applied Physics"},"keywords":[{"id":"c4ff4300-4a44-4913-b116-5402bbd1c68d","keyword":"magnetoelastic properties;<span style=\"color:red\">magnetic</span>-properties","originalKeyword":"magnetoelastic properties;magnetic-properties"}],"language":"en","publisherId":"0021-8979_2006_4_1","title":"<span style=\"color:red\">Structure</span>, Curie temperature, and <span style=\"color:red\">magnetostriction</span> of SmZn1-xMnx <span style=\"color:red\">alloys</span>","volume":"99","year":"2006"},{"abstractinfo":"The <span style=\"color:red\">structure</span>, Curie temperature and <span style=\"color:red\">magnetostriction</span> of R(Fe1-xMnx)(1.85) <span style=\"color:red\">alloys</span> (x=0-0.3) were investigated. These <span style=\"color:red\">alloys</span> are essentially single <span style=\"color:red\">phase</span> with a cubic Laves <span style=\"color:red\">structure</span>. The lattice constant increases steadily and the Curie temperature decreases linearly with increasing Mn content. The largest <span style=\"color:red\">magnetostriction</span> occurs at about x=0.05.","authors":[],"categoryName":"|","doi":"","fpage":"249","id":"6427ac88-d968-4a0f-a2d7-566e9786dc5e","issue":"42737","journal":{"abbrevTitle":"JOMAMM","id":"5d7a0764-3359-4184-bc25-ad22bbdaf30a","issnPpub":"0304-8853","publisherId":"JOMAMM","title":"Journal of Magnetism and Magnetic Materials"},"keywords":[{"id":"9601e4be-6408-4ffc-be74-45de0d1d1279","keyword":"<span style=\"color:red\">magnetostriction</span>;cubic Laves <span style=\"color:red\">phase</span>;mn","originalKeyword":"magnetostriction;cubic Laves phase;mn"}],"language":"en","publisherId":"0304-8853_1997_42737_4","title":"<span style=\"color:red\">Structure</span> and <span style=\"color:red\">magnetostriction</span> of R(Fe1-xMnx)(1.85) <span style=\"color:red\">alloys</span> (R=Dy0.6Tb0.3Pr0.1)","volume":"166","year":"1997"},{"abstractinfo":"The <span style=\"color:red\">phase</span> transformation, <span style=\"color:red\">structure</span> and <span style=\"color:red\">magnetic</span> properties of mechanically alloyed (MA) Pr10Fe82-xVxB8, Pr10Fe76V6+yB8-y, and Pr10-zNdzFe76V13B1 <span style=\"color:red\">alloys</span> and their nitrides have been studied. With increasing V content, the <span style=\"color:red\">magnetic</span> main <span style=\"color:red\">phase</span> in the Pr10Fe76V6+yB8-y series changes from the Pr2Fe14B-type <span style=\"color:red\">phase</span> via a metastable Pr(Fe,V, B)(7) <span style=\"color:red\">phase</span> with TbCu7-type <span style=\"color:red\">structure</span> to Pr(Fe,V, B)(12) <span style=\"color:red\">phase</span> with ThMn12-type <span style=\"color:red\">structure</span>. After nitrogenation, the easy magnetization of Pr(Fe,V, B)(7) and Pr(Fe,V, B)(12) phases changes from easy in-plane to easy c-axis, and their Curie temperatures are greatly enhanced, due to the entrance of nitrogen into the interstitial sites. In the Pr10-zNdzFe76V13B1 series, the substitution of Nd for Pr gradually leads to the complete formation of (Pr, Nd)(Fe,V, B)(12) <span style=\"color:red\">phase</span> with ThMn12-type <span style=\"color:red\">structure</span> and the disappearance of alpha-Fe. The coercivity of the Pr10-zNdzFe76V13B1Ndelta <span style=\"color:red\">alloys</span> is drastically enhanced by Nd substitution. (C) 2003 Elsevier B.V. All rights reserved.","authors":[],"categoryName":"|","doi":"","fpage":"40916","id":"6634b112-abad-4925-bb58-6d6d2afb6bed","issue":"42737","journal":{"abbrevTitle":"JOMAMM","id":"5d7a0764-3359-4184-bc25-ad22bbdaf30a","issnPpub":"0304-8853","publisherId":"JOMAMM","title":"Journal of Magnetism and Magnetic Materials"},"keywords":[{"id":"13f4a488-b92a-48b8-9473-057507a92900","keyword":"permanent magnets;<span style=\"color:red\">magnetic</span> anisotropy;<span style=\"color:red\">magnetic</span> properties;remanence enhancement;fe","originalKeyword":"permanent magnets;magnetic anisotropy;magnetic properties;remanence enhancement;fe"}],"language":"en","publisherId":"0304-8853_2004_42737_3","title":"<span style=\"color:red\">Phase</span> transformation, <span style=\"color:red\">structure</span> and <span style=\"color:red\">magnetic</span> properties of (Nd,Pr)-Fe-V-B <span style=\"color:red\">alloys</span> and their nitrides prepared by mechanical alloying","volume":"278","year":"2004"},{"abstractinfo":"The <span style=\"color:red\">structure</span>, <span style=\"color:red\">magnetic</span> and inagnetostrictive properties of Sm(0.7)Pr(0.3)Fe(x) (1.45 <= x <= 1.95) <span style=\"color:red\">alloys</span> is investigated. X-ray diffraction analysis confirms the presence of single cubic Laves <span style=\"color:red\">phase</span> in Sm(0.7)Pr(0.3)Fe(x) <span style=\"color:red\">alloys</span> with 1.45 <= x <= 1.85. The saturation magnetization of the <span style=\"color:red\">alloys</span> tends to increase with increasing Fe content. Sm(0.7)Pr(0.3)Fe(1.55) has the highest <span style=\"color:red\">magnetostriction</span> among all the Sm(0.7)Pr(0.3)Fe(x) <span style=\"color:red\">alloys</span> at low fields and shows a large <span style=\"color:red\">magnetostriction</span> lambda(parallel to)-lambda(perpendicular to) = 1008 ppm at a <span style=\"color:red\">magnetic</span> field of 12 kOe. (C) 2009 Elsevier B.V. All rights reserved.","authors":[],"categoryName":"|","doi":"","fpage":"608","id":"936ed634-ea2e-4b8d-b0c2-0b47f01178f6","issue":"5","journal":{"abbrevTitle":"ML","id":"90b15a58-51fc-41ad-8509-c2692f6a3f6e","issnPpub":"0167-577X","publisherId":"ML","title":"Materials Letters"},"keywords":[{"id":"bdcb101e-ce86-4b5c-aece-dda3baba26fb","keyword":"Metals and <span style=\"color:red\">alloys</span>;<span style=\"color:red\">Magnetic</span> materials;Laves <span style=\"color:red\">Phase</span>;Light rare earths;<span style=\"color:red\">Magnetostriction</span>;X-ray techniques;microstructure;sm1-xprxfe2","originalKeyword":"Metals and alloys;Magnetic materials;Laves Phase;Light rare earths;Magnetostriction;X-ray techniques;microstructure;sm1-xprxfe2"}],"language":"en","publisherId":"0167-577X_2010_5_1","title":"<span style=\"color:red\">Structure</span>, <span style=\"color:red\">magnetic</span> and magnetostrictive properties of Sm(0.7)Pr(0.3)Fe(x) <span style=\"color:red\">alloys</span>","volume":"64","year":"2010"},{"abstractinfo":"The <span style=\"color:red\">boron</span>-oxide coated iron nanocapsules have been prepared by arc-discharge in a mixture of diborane and nitrogen, and then the <span style=\"color:red\">boron</span>-nitride coated iron nanocapsules by a subsequent annealing under a nitrogen atmosphere at 1100&deg;C. After the arc-discharge, the <span style=\"color:red\">boron</span>-oxide coated iron nanocapsules form, which show an&nbsp; amorphous surface layer of B<sub>2</sub>O<sub>3</sub> (and/or B) and a core of&nbsp;&gamma;-Fe,&nbsp;&alpha;-Fe, FeB phases. After being annealed, part of the&nbsp;&alpha;-Fe <span style=\"color:red\">phase</span> transforms to the&nbsp;&gamma;-Fe <span style=\"color:red\">phase</span>, and the FeB <span style=\"color:red\">phase</span> decomposes while the BN <span style=\"color:red\">phase</span> forms. The BN shell <span style=\"color:red\">structure</span> formed in the BN encapsulating iron nanocapsules is incomplete. <span style=\"color:red\">Magnetic</span> properties of the <span style=\"color:red\">boron</span>-oxide coated and the <span style=\"color:red\">boron</span>-nitride coated iron nanocapsules were compared and discussed in terms of the particles sizes, the <span style=\"color:red\">phase</span> components, and the surface structures.","authors":[{"authorName":"W.S. Zhang","id":"a8315fca-3c6f-4013-99e1-dcf73c2cf7e4","originalAuthorName":"W.S. Zhang"}],"categoryName":"|","doi":"","fpage":"1051","id":"55537cb3-de74-4135-a11a-370a0aee10cb","issue":"11","journal":{"abbrevTitle":"CLKXJSY","coverImgSrc":"journal/img/cover/JMST.jpg","id":"11","issnPpub":"1005-0302 ","publisherId":"CLKXJSY","title":"材料科学技术（英文）"},"keywords":[{"id":"6ab6aa3f-1cab-498d-9de5-673a81a53373","keyword":"Arc discharge","originalKeyword":"Arc discharge"},{"id":"5389e34b-521f-4b76-b364-3f8084b16d55","keyword":" nanocapsules","originalKeyword":" nanocapsules"},{"id":"c75610fb-ab9c-4a66-9e33-875eb50afbc2","keyword":" <span style=\"color:red\">magnetic</span> properties","originalKeyword":" magnetic properties"}],"language":"en","publisherId":"1005-0302_2010_11_10","title":"<span style=\"color:red\">Structure</span> and <span style=\"color:red\">Magnetic</span> Properties of <span style=\"color:red\">Boron</span>-oxide and <span style=\"color:red\">Boron</span>-nitride Coated Iron Nanocapsules","volume":"26","year":"2010"},{"abstractinfo":"The <span style=\"color:red\">boron</span>-oxide coated iron nanocapsules have been prepared by arc-discharge in a mixture of diborane and nitrogen, and then the <span style=\"color:red\">boron</span>-nitride coated iron nanocapsules by a subsequent annealing under a nitrogen atmosphere at 1100 degrees C. After the arc-discharge, the <span style=\"color:red\">boron</span>-oxide coated iron nanocapsules form, which show an amorphous surface layer of B(2)O(3) (and/or B) and a core of gamma-Fe, alpha-Fe, FeB phases. After being annealed, part of the a-Fe <span style=\"color:red\">phase</span> transforms to the gamma-Fe <span style=\"color:red\">phase</span>, and the FeB <span style=\"color:red\">phase</span> decomposes while the BN <span style=\"color:red\">phase</span> forms. The BN shell <span style=\"color:red\">structure</span> formed in the BN encapsulating iron nanocapsules is incomplete. <span style=\"color:red\">Magnetic</span> properties of the <span style=\"color:red\">boron</span>-oxide coated and the <span style=\"color:red\">boron</span>-nitride coated iron nanocapsules were compared and discussed in terms of the particles' sizes, the <span style=\"color:red\">phase</span> components, and the surface structures.","authors":[],"categoryName":"|","doi":"","fpage":"1051","id":"766499ee-e0f9-47e7-be7c-00d97fa5f318","issue":"11","journal":{"abbrevTitle":"CLKXJSY","coverImgSrc":"journal/img/cover/JMST.jpg","id":"11","issnPpub":"1005-0302 ","publisherId":"CLKXJSY","title":"材料科学技术（英文）"},"keywords":[{"id":"59131882-9ee9-47a6-acdd-1828d036fd1f","keyword":"Arc discharge;Nanocapsules;<span style=\"color:red\">Magnetic</span> properties;nanoparticles;fe;particles","originalKeyword":"Arc discharge;Nanocapsules;Magnetic properties;nanoparticles;fe;particles"}],"language":"en","publisherId":"1005-0302_2010_11_2","title":"<span style=\"color:red\">Structure</span> and <span style=\"color:red\">Magnetic</span> Properties of <span style=\"color:red\">Boron</span>-oxide and <span style=\"color:red\">Boron</span>-nitride Coated Iron Nanocapsules","volume":"26","year":"2010"}],"totalpage":1059,"totalrecord":10581}