Stability of the single-domain state in single crystals of triglycine sulphate

The stability of the single-domain state in single crystals of triglycine sulfate is investigated using the Barkhausen effect. Barkhausen jumps are detected upon invariable macroscopic polarization. The parameters of the observed Barkhausen jumps are estimated and compared.     

Visualization of the Barkhausen effect by magnetic force microscopy

By visualization of the Barkhausen effect using magnetic force microscopy we are able to provide detailed information about the physical principles that govern the magnetization reversal of a granular ferromagnetic thin film with perpendicular anisotropy. Individual Barkhausen volumes are localized and distinguished as either newly nucleated or grown by domain wall propagation. The Gaussian size distribution of nucleated Barkhausen volumes indicates an uncorrelated random process, while grown Barkhausen volumes exhibit an inverse power law distribution, which points towards a critical behavior during domain wall motion.     

Direct observation of Barkhausen avalanche in Co thin films

We report direct full-field magneto-optical observations of Barkhausen avalanches in Co polycrystalline thin films at criticality. We provide experimental evidence for the validity of a phenomenological model of the Barkhausen avalanche originally proposed by Cizeau, Zapperi, Durin, and Stanley [Phys. Rev. Lett. 79, 4669 (1997)]], where the model describes a 180 degrees -type flexible domain wall deformed by a localized defect with consideration of long-range dipolar interaction. The Barkhausen jump areas show a power-law scaling distribution with critical exponent tau approximately 1.33 for all the samples having different thickness from 5 to 50 nm, which is in accord with the two-dimensional prediction of the model.     

Investigation of the dependence of Barkhausen noise on stress and the angle between the stress and magnetization directions

The dependence of Barkhausen noise amplitude on stress, and on the angle between the stress and magnetization directions, has been investigated in specimens of AISI/SAE 4340, HY-80 and ASTM A-36 steels. In all three materials it was found that the Barkhausen noise amplitude measured with the magnetic field applied at 60° to the stress axis is independent of stress. This result is compared with the theory of elasticity which indicates that under a uniaxial or a pure bending stress, the normal component of a strain in steel is zero along the direction approximately 61° from the direction of the applied stress. It was also found that the Barkhausen noise follows the same angle dependence as that of the normal strain. These findings strongly indicate that the Barkhausen noise amplitude is directly dependent on the normal strain along the direction of the magnetization and not on the shearing strain. An explanation for such a direct normal strain dependence is given based on magnetoelastic energy. Possible application of this finding to quantitative nondestructive stress measurements is also discussed.     

Barkhausen noise and domain structure dynamics in Si-Fe at different points of the magnetization curve

In the present relationship between Barkhausen noise and domain structure evolution along the hysteresis loop in 3% Si–Fe has been investigated. The noise power spectrum has been measured vs. induction during cyclic magnetization of the material at a very low constant rate. The obtained results show that the behavior of the noise power along the magnetization curve can be related to the character of the domain structure rearrangements taking place at different levels of induction. Such a connection is reflected in a relationship between the noise power and the shape of the hysteresis loop. The measured noise power spectra are interpreted through the use of a suitable model. This makes possible to connect the shape of the magnetization curve to the microscopic parameters characterizing the dynamic of the domain wall during a large Barkhausen jump.     

Propagation of the electrodynamic disturbance following a Barkhausen jump in metallic ferromagnetic samples

An expression is derived for the space-time distribution of the magnetic field of a magnetic dipole with time dependent moment, which is used as a model of a Barkhausen jump. The medium surrounding the dipole is a conductor of infinite dimensions.     

Der Elektromagnetische Aspekt der Magnetomechanischen Erscheinung in Gleich und im Monoalternant Pulsierenden Magnetfeld

The electromotive tension induced by Barkhausen discontinuities is studied. These Barkhausen discontinuities are excited by periodic mechanical stress in a d-c and a mono-alternating pulse magnetic field.     

Magnetic Barkhausen emission in lightly deformed AISI 1070 steel

The Magnetic Barkhausen Noise (MBN) technique can evaluate both micro- and macro-residual stresses, and provides indication about the relevance of contribution of these different stress components. MBN measurements were performed in AISI 1070 steel sheet samples, where different strains were applied. The Barkhausen emission is also analyzed when two different sheets, deformed and non-deformed, are evaluated together. This study is useful to understand the effect of a deformed region near the surface on MBN. The low permeability of the deformed region affects MBN, and if the deformed region is below the surface the magnetic Barkhausen signal increases.     

Effect of the length of action of a steady electric field on the polarization buildup process in triglycene sulfate and barium titanate single crystals

During the investigation of the Barkhausen effect and the reversal current [1] in ferroelectric crystals, it was observed that, together with other factors, the length of time during which the specimens had been kept in a steady electric field has a substantial effect on the polarization reversal process. In this connection, it is of interest to investigate parallely the Barkhausen effect and the reversal current in ferroelectric crystals at various lengths of action of the electric field. In this paper we have investigated the number of Barkhausen jumps, the charge being reversed, the buildup time of the total and irreversible polarization, as well as the starting field for jumps and reversal current as a function of the length of action of the field on specimens of TGS and BaTiO₃ single crystals during the quasistatic polarization reversal process.     

Use of time-delay correlators and wave-shaping techniques in the statistical analysis of Barkhausen pulses

A new class of digital correlators and other related instruments have been developed recently for photoelectron statistics applications. In this work we explore the possibility of using these low cost devices for analyzing trains of Barkhausen pulses. We also outline the applications of the theory of random point processes (specifically, self-exciting point processes) to Barkhausen noise. Finally, we present a new technique for exposing ferromagnetic samples to a linearly variable induction field. Our technique is fully digital and offers several advantages in terms of accuracy and reproducibility of control over the conventional tape-recorder method.     

The investigation of the process of magnetization in FeNiBSi glasses by means of the Barkhausen jumps

The Barkhausen jumps occuring during the magnetization of the amorphous Fe-Ni-B-Si alloys have been studied by the measurements of the derivative of magnetization with respect to time (dM/dt). The peaks in dM/dt vs. applied field (H) are reproducible after averaging over some fifty cycles of magnetization. The investigation of the variations of dM/dt with the applied field (H) and with the instantaneous magnetization (M) accompanied with the same studies, but performed starting from different values of the initial remanence (M_ri), completes our earlier analysis of the process of magnetization in these alloys. It is shown that the model of Chikazumi used for the explanation of the variations of remanent magnetization, coercive field and loss with the maximum magnetization (M_m) is consistent with the observed Barkhausen jumps. The possibility of separation of contributions from particular domain walls to the process of magnetization in soft magnetic materials (which would enable the determination of the locations and strengths of the particular pinning centres) is briefly discussed.     

Der elektromagnetische Aspekt der Energiezufuhrerscheinung von einem longitudinalen Wechselmagnetfeld an ein Torsionspendel mit ferromagnetischer Aufhängung

It is shown that under conditions in which a torsion pendulum with ferromagnetic suspension thread oscillates with torsional oscillation being excited by the energy transferred from an a-c magnetic field, Barkhausen discontinuities are released by the torsional deformations. A study is made of the dependence of the voltage pulse, which induced these Barkhausen discontinuities in the coil in the field of which the ferromagnetic suspension thread is placed, on the intensity of the a-c magnetic field, the amplitude of torsional deformation and the angle of phase shift between these two sine quantities. The influence of an underlying longitudinal d-c magnetic field on these Barkhausen discontinuities is also investigated.

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Wir danken I. Schreck für seinen wertvollen Beitrag zur Herstellung der in dieser Arbeit benützten elektronischen Apparatur.     

Die Temperaturabhängigkeit des magnetischen Barkhausen-Effekts IV

The size distribution of Barkhausen discontinuities (magnetic moment > 6.5 · 10^?7 cgs) of very pure nickel was measured between ?195 and 360 °C on the hysteresis loop. The mean value of internal stresses was changed in a well defined manner by stretching the specimens. For different stress values the variation with temperature of the following properties is given in diagrams: The specific number and the “mean volume”² of discontinuities, the maximal value of Barkhausen susceptibility, the mean deviation of the volume of discontinuities along the hysteresis curve, and some characteristic field strengths defined by reversible and irreversible processes. Conclusions are drawn concerning the coupling of individual wall movements composing a Barkhausen jump.     

Barkhausen effect in magnetic thin films: General behaviour and stationarity along the hysteresis loop

Several aspects of the Barkhausen effect can be investigated by using a measurement equipment that records the Barkhausen signal as a function of time in digital form on computer tape. Measurements on thin magnetic films containing a small number of domain walls are presented. The behaviour of the wall jumps during a reversal is investigated. During the steep part of the loop the stationarity of the signal is measured with the magnetic field as a parameter. The influence of the coercive fieldH _c and the thicknessd _m is considered and compared with results obtained by others on bulk samples.     

Traditional,Barkhausen and MAT Magnetic Response to Plastic Deformation of Low-Carbon Steel

Magnetic traditional and adaptive methods as well as Barkhausen noise analysis were used for the testing of material degradation of plastically deformed high quality low-carbon steel. The dependences of the measured magnetic (coercive field, maximum permeability, optimum adapted permeability) and Barkhausen noise (RMS voltage, power spectrum) parameters are understood in terms of the increased dislocation density. The results are discussed in the context of potential application of magnetic testing methods for the indication of plastic deformation levels of ferromagnetic construction steel products.     

Evaluation of surface decarburization depth by magnetic Barkhausen noise technique

Industrially unfavorable process of steel surface decarburization was induced by annealing in air. Two methods of after-anneal surface treatment were used: an acid pickling and a sand blasting. The obtained decarburized layers were examined by optical microscope, wave dispersive spectrometer, and surface X-ray diffraction method. Magnetic Barkhausen noise technique was tested for applicability of non-destructive characterization of the decarburized layer depth. A newly introduced parameter, Barkhausen noise coercivity, was proposed for practical use due to its sensitivity to decarburization and stability to measurement conditions. Other magnetic parameters, e.g. number of Barkhausen noise counts, were found to be sensitive to the compressive residual stress caused by the sand blasting.     

DC magnetization of ferromagnetic amorphous wires with local deformation

Experimental DC (VSM) and theoretical hysteresis loops of a ferromagnetic amorphous wire with a deformation in the middle or exposed to local magnetic fields are investigated. Hysteresis loops show two-stage Barkhausen jumps and staircase relaxation. With a local field at the same position, the loop drastically looses its shape and symmetry depending on the magnitude and the direction of the magnetic bias. A model to explain this behavior is proposed. The proposed model is based on the calculation of the magnetic moment distribution of the domain as a result of domain wall motion and nucleation in the inner core of a ferromagnetic wire and is in a good agreement with the experimental results.     

Reverse Barkhausen jumps

The magnetic parameters, forward and reverse magnetic reversal jumps in iron-core quartzite specimens and in magnetite single crystals, and the effect of thermal treatment on the magnetic and electric parameters of quartzites are studied. Reverse Barkhausen jumps are larger than the forward ones, but they are considerably fewer. The maxima of forward jumps correspond to the coercive force, while those of the reverse ones to fields exceeding the coercive force. Possible causes of the manifestation of reverse Barkhausen jumps are discussed.Translated from Izvestiya Vysshikh Uchebnykh Zavedenii, Fkika, No. 12, pp. 8–12, December, 1984.     

Determination of the losses induced by irreversible barkhausen jumps of the 180° domain wall moving with a sinusoidal motion in the single domain wall model

The paper presents an analysis of the losses due to irreversible Barkhausen jump of the 180° Bloch wall in the single-domain wall model. The field-intensity and current-density vectors at unit input were determined for a single instantaneous jump. The losses were calculated for the case of the wall moving sinusoidally. The Parseval formula was used at determining the losses, which made it possible to perform calculations. A similar problem was considered by Allia and Vinai who adopted a simplified assumption of the domain of an infinitely long cylindrical shape.