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Study of an hybrid mangetometer : YIG

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HAL Id: hal-01109733

https://hal.archives-ouvertes.fr/hal-01109733

Submitted on 7 May 2020

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Study of an hybrid mangetometer : YIG

Basile Dufay, Sébastien Saez, Christophe Cordier, Christophe Dolabdjian, E.

Hristoforou

To cite this version:

Basile Dufay, Sébastien Saez, Christophe Cordier, Christophe Dolabdjian, E. Hristoforou. Study of an hybrid mangetometer : YIG. Magnetic School : High sensitivity magnetometers - Sensors and Applications 2007, Sep 2007, Blainville-sur-mer, France. �hal-01109733�

(2)

Study of an hybrid magnetometer: YIG

Working principle:

YIG film

an d

If the magnetization of the material is saturated so : and

Demodulation by and allows us to deduce both and with a single magnetometer.

SENSITIVITY :

Noise sources:

Intrinsic magnetic noise [1]

Noise from the rotating excitation

Electronic noise dominated by the noise from the punctual sensor

operating point

Slope a

Slope becomes : b

is the amplitude noise of

Materials:

The punctual sensor sense a signal proportional to :

Magnetization (a.u.)

Applied magnetic field at 0.001Hz (in T) YIG B-H Loop

Yttrium Iron Garnet Single-crystal

YScFeO -> YIG

Solid solution of Sc

Miller level: 640 (in plane) and 444 Strong susceptibility

In-plane anisotropic behavior of the B-H Loop

YIG: SEM, EDS, XRD and B-H Loop measurement.

k: coupling factor between YIG magnetization M and sensed field.

In plane direction:

0deg 60deg 120deg

Punctual magnetometer -> Hall effect sensor, sensing the vertical component of the field induced by the magnetization of the YIG.

Optimal position of the Hall sensor in order to increase k:

just on the boundary of the YIG disc as near as possible from the YIG film surface.

increase the space resolution of the sensor in use.

Results:

So the sensed output signal becomes:

We apply an

external magnetic field:

The sensitivity T

r

could be evaluated from the amplitude of both AM spectral components.

Amplitude Modulation

Frequency (in Hz) Spectrum of the hall sensor output signal

Possibilities of evolution:

Increase the coupling factor k: *optimization of the hall sensor position.

Increase the ration M

0

/B

0

: *Changing the form factor of the material

*New soft magnetic material Actuals main problems:

Noise spectrum density is dominated by the hall sensor noise.

Low values of the coupling factor k.

The work presented here deals with the study of a flux-gate type magnetometer which use a rotating magnetization. This principle allows to sense the different space components of the magnetic field and to reduce the noise due to Barkhausen jumps. The device was setted-up at the laboratory of physical metallurgy of the national technological university of Athens.

First of all, studying physical properties of the used material allows to deduce his crystalline structure, to evaluate his behavior under a rotating magnetic excitation and to validate the choice of this material. Then, a theoretical approach of the rotating excitation principle allows to understand the interest of this kind of device and to see which elements are changing performances on sensibility or magnetic noise. This theoretical approach finally leads to expose and to analyze the practical realization of using this working principle as developed by the Greek laboratory. It allows to understand encountered difficulties and to evaluate the effect on performances due to compromises needed. Finally, some experimental results are exposed, validating the working principle and leading to think about the possibility of evolution of this device.

Signal

[1] Peter M. Vetoshko, Michael V. Valeiko, Petr I. Nikitin, “Epitaxial yttrium iron garnet film as an active medium of an even-harmonic magnetic field transducer”, Sensors and Actuators A, vol. 106, p. 270-273.

* Not sufficient in order to saturate the material

Frequency (Hz) Equivalent magnetic noise spectrum density (T/Hz1/2 )

First Hall sensor Second Hall sensor

Implementation:

3 noise sources

B. Dufay 1 , S. Saez 1 , C. Cordier 1 , C. Dolabdjian 1 , E. Hristoforou 2

1

GREYC, 6 Bd du Maréchal Juin, 14000 Caen, FRANCE

2

Laboratory of physical metallurgy, National Technical University of Athens, Zografou Campus, Athens 15780, GREECE

Punctual sensor

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