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DSpace at VNU: A systematic study of giant magnetoimpedance of Cr-substituted Fe(73.5-x)Cr(x)Si(13.5)B(9)Nb(3)Au(1) (x=1, 2, 3, 4, 5) alloys

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Hoaa a Center for Materials Science,Vietnam National University, 334 NguyenTrai, Hanoi, Vietnam b Department of Physics, Chungbuk National University, Cheongju 361-763, South Korea c Dep

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Journal of Magnetism and Magnetic Materials 304 (2006) e871–e873

A systematic study of giant magnetoimpedance of Cr-substituted

Fe 73.5x Cr x Si 13.5 B 9 Nb 3 Au 1 (x ¼ 1, 2, 3, 4, 5) alloys

N.D Thoa, N Chaua, S.C Yub, , H.B Leec, N.D Thea, N.Q Hoaa

a Center for Materials Science,Vietnam National University, 334 NguyenTrai, Hanoi, Vietnam

b Department of Physics, Chungbuk National University, Cheongju 361-763, South Korea

c

Departement of Physics, Kongju National University, Kongju 314-701, South Korea

Available online 27 March 2006

Abstract

The magnetoimpedance of Fe76.5xCrxSi13.5B9Nb3Au1 (x ¼ 1, 2, 3, 4, 5) alloys has been measured to investigate the influence of crystallization process on the soft magnetic properties and magnetic anisotropy after thermal treatment Annealing performed at 540 and

550 1C for 30 min in a vacuum indicated that ultrasoft magnetic properties of nanocomposite materials are obtained The magnetoimpedance ratio (MIR) and incremental permeability ratio (PR) measurements show that the maximum values of MIR and

PR increase drastically in the heat-treated samples It means that the samples are softened by nanocrystallization The PR curves become narrower and sharper due to the decrease of anisotropy The MIR behavior related with the softness of magnetic properties of heat-treated samples and the incremental PR strongly changes with external magnetic field

r2006 Elsevier B.V All rights reserved

PACS: 75.50.Tt

Keywords: Amorphous; Nanocrystalline; Magnetoimpedance; Permeability

The magnetoimpedance (MI) effect is the change of the

impedance experienced by an AC current flowing through

a magnetic material when an external DC magnetic field is

applied In recent years, many works on MI effect has

stimulated considerable attention because of its

technolo-gical applications in magnetic sensors and devices[1,2] The

influence of various substituting alloying elements for Fe in

FeCuNbSiB composition has been also widely investigated

Recently, it has been reported that the partial substitution

of Fe by Cr enhances the thermal stability of the

amorphous alloy against nanocrystallization and lowers

the Curie temperature of both, as-cast amorphous alloys

and the residual amorphous phase in the nanocomposite

[3] Other authors [4] have found that partially

substitu-ting Fe by Co in Fe73.5xCoxSi13.5B9Nb3Cu1 alloys leads

to the increasing of magnetic moment and the Curie

point of precipitated crystalline phase More recently,

it was reported that the Cr substitution in Fe-based

amorphous alloys can also improve the mechanical or electrical properties without deteriorating the magnetic properties [5]

In this study, we systematically investigate the giant magnetoimpedance (GMI) effect and the effect of Cr substitution for Fe on the soft magnetic properties of

Fe73.5xCrxSi13.5B9Nb3Au1 (x ¼ 1, 2, 3, 4, 5) alloys with different annealing temperatures

Amorphous ribbons (7 mm wide, 16.8 mm thick) with nominal compositions Fe73.5xCrxSi13.5B9Nb3Au1 (x ¼ 1,

2, 3, 4, 5) were obtained by rapid quenching from the melt spinning technique The crystallization behaviors of the samples were investigated by DSC (SDT-2960 TA Instru-ments) measurements The phase structures of both as-quenched and annealed samples were examined by X-ray diffractometer (D5005, Bruker) For the MI measurement the external field applied by a solenoid can be swept through the entire cycle equally divided by 800 intervals from 300 to 300 Oe The frequency of MI measurement was ranging from 1 to 10 MHz, and the AC current was fixed at 10 mA for all measurements

www.elsevier.com/locate/jmmm

0304-8853/$ - see front matter r 2006 Elsevier B.V All rights reserved.

doi:10.1016/j.jmmm.2006.03.021

Corresponding author Tel.: +82 43 2612269; fax: +82 43 2756415.

E-mail address: scyu@chungbuk.ac.kr (S.C Yu).

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The X-ray diffraction analysis shows that the

as-quenched samples are amorphous The DSC measurements

on the as-quenched ribbons were performed at a heating

rate of 20 1C/min The results indicate that the

devitrifica-tion of the investigated alloys takes place in two main

stages The first one corresponds to the crystallization of

the a-Fe(Si) soft magnetic phase, while the second is related

with the appearance of boride-type phase (Fe3B or Fe2B)

It was found that the addition of Cr produces a slight

stabilization of the amorphous alloy against the

crystal-lization, which can be detected as a linear increase of the

peak temperature of the first exothermal The MIR as a

function of the applied field, H, is defined with respect to

the maximum applied field (Hmax¼300 Oe in the present

work) as DZ/Z(%) ¼ DZ/Z(Hmax) ¼ 1|Z(H)/Z(Hmax)|

The PR can be defined as PR(H) ¼ Dm/m (Hmax) ¼ 1|m

(H)/m (Hmax)|

In amorphous ribbon materials, the MI effect is favored

by the decrease of resistivity resulting from the

crystal-lization process This strong reduction in the resistivity of

the nanocrystalline ribbons reduces the skin depth and

increases the MIR of the samples[6] From the nearly zero MIR values in the as-quenched samples it is evident that the samples do not show soft magnetic properties However, the maximum MIR value increases drastically

in the samples annealed at 540 and 550 1C, indicating that the studied samples are ultra-softened by the crystal-lization, see example inFig 1for sample with x ¼ 4 From

Fig 1, the frequency dependence of MIR in the samples shows a typical behavior where the shapes of the MIR curves are generally getting broader with the increment of the measuring frequency throughout all samples The rather high values and sharpness of the MIR curves in the annealed samples compared to the as-quenched ones indicate that structure changes such as the nanocrystalliza-tion have occurred in the annealed samples Among the investigated samples, the largest GMI effect was observed

in the nanocrystalline sample containing 5% of Cr (x ¼ 5) and reached the value of 190% at frequency of 2 MHz This is ideal for developing high-performance magnetic sensor

The MI effect at high frequency can be explained in terms of an external field dependence of impedance as a result of the circumferential magnetization with respect to

Fig 1 The MIR versus the external field H measured at various

frequencies in Fe 72.5 Cr 4 Si 13.5 B 9 Nb 3 Au 1 alloy annealed at (a) 540 1C and

(b) 550 1C.

Fig 2 The PR curves of as-quenched samples and the annealed samples

Fe Cr Si B Nb Au (x ¼ 1, 2, 3, 4, 5) measured at 1 MHz.

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the current direction running through the sample and the

skin effect of AC current At the frequency below 1 MHz,

the maximum value of GMI was relatively low (not shown

here) and we suppose that it is due to the contribution of

the induced magnetoinductive voltage to MI[6] When the

frequency is in the range 1 MHzpfp5 MHz, skin effect is

dominant and larger GMI values were found The highest

MI ratio is observed for nearly zero saturation

magnetos-triction after annealing at about 550 1C At this annealing

temperature the effective magnetostriction is fully

compen-sated so that the effective magnetoelastic anisotropy is

minimum Moreover, transverse magnetic anisotropy is

additionally induced on the ribbon’s surface during the

annealing process This typical anisotropy controls the

magnetization vector in the transverse domain and thus

improves the magnetic response of the soft magnetic

nanocrystalline material Therefore, the GMI effect is

enhanced as a direct consequence of the higher mobility of

domain walls as correlated with transverse permeability[6]

The PR curves measured at 1 MHz in the as-quenched

samples and the samples annealed at 550 1C are plotted in

Fig 2 The large changes of the magnitude and field

shape of the PR in the nanocrystalline alloys compared

with as-quenched samples indicate that structural change

such as crystallization has occurred To determine the

structural changes of the samples, X-ray diffraction

measurements have been performed The X-ray patterns

show the appearance of a-Fe(Si) peaks in the annealed samples The sharpness of PR curves after annealing implies the decrease of local anisotropy distribution by the nanocrystallization and indicates that the magnetization can be saturated under very low external field In general, the changes of the MI are closely related to the changes

of the longitudinal incremental permeability Therefore, magnetic softness can be estimated from the MIR or the PR

Research at Chungbuk National University was sup-ported by the Korea Science and Engineering Foundation through the Research Center for Advanced Magnetic Materials at Chungnam University Research at Center for Materials Science was supported by Vietnam National Fundamental Research Program, Grant No.811204

References

[1] R.S Beach, A.E Berkowitz, Appl Phys Lett 76 (1994) 6209 [2] R.L Sommer, C.L Chien, Appl Phys Lett 67 (1995) 3652 [3] J Fuzer, P Matta, P Kollar, P Sovak, M Konc, J Mag Mag Mater 158 (1996) 205.

[4] N Chau, N.X Chien, N.Q Hoa, P.Q Niem, N.H Luong, N.D Tho, V.V Hiep, J Mag Mag Mater 282 (2004) 174.

[5] N Bayri, H.I Adiguzel, S Atalay, P Sovak, Phys Status Solidi A 189 (2002) 805.

[6] M Knobel, M.L Sanchez, C Gomez-Polo, P Marin, M Vazquez,

J Appl Phys 79 (1996) 1646.

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