Giant magnetoresistance of semimagnetic semiconductors and applications for magnetic field sensors (original) (raw)

Colossal Magnetocapacitance and Colossal Magnetoresistance in HgCr2S4

Physical Review Letters, 2006

We present a detailed study of the dielectric and charge transport properties of the antiferromagnetic cubic spinel HgCr2S4. Similar to the findings in ferromagnetic CdCr2S4, the dielectric constant of HgCr2S4 becomes strongly enhanced in the region below 60 - 80 K, which can be ascribed to polar relaxational dynamics triggered by the onset of ferromagnetic correlations. In addition, the observation of polarization hysteresis curves indicates the development of ferroelectric order below about 70 K. Moreover, our investigations in external magnetic fields up to 5 T reveal the simultaneous occurrence of magnetocapacitance and magnetoresistance of truly colossal magnitudes in this material.

Development of Sensors Based on Giant Magnetoresistance Material

Procedia Engineering, 2012

In this review we discuss development of sensors based on giant magnetoresistance (GMR) material.The GMR material has high magnetic and electrical properties, therefore it has great potential as next generation magnetic field sensing devices. During the last decade, intensive research efforts have been expended to develop sensors based on giant magnetoresistance (GMR) material, both based on inorganic materials and organic materials. Many application of GMR sensor, such as: current sensor, linear and rotational position sensor, head recording, and biosensor, are reviewed.

An EPR study of dilute magnetic semiconductors Hg1−xCoxSe (x = 0.0045 and x = 0.0087)

Solid State Communications, 1994

X-band (-,9.3 GHz) EPR spectra are recorded from room temperature down to 5 K on two samples of symmetry-induced zero band gap semiconductor Hgl_xCo~Se (x=0.0045 and 0.0087), previously subjected to electron bombardment. Both the samples exhibit, in addition to a narrow intense line (g = 2.018) due to trapped electron/ defect centre, a broad Co 2+ EPR line (overlap of the transitions Ms = +1/2 +-* +3/2) characterized by g = 2.027, which disappears at low temperatures. In addition, only the EPR spectra of the sample with the larger concentration of Co ions reveal the presence of an extra EPR line with the value of g = 2.024 at temperatures below 40 K. (This line was, however, found to be present in another sample with the lower concentration.) This extra line is interpreted to be due to the Kramers doublet (Ms = 4-1/2) of the Co 2+ ion. The present EPR data do not indicate the presence of Co 3+ ions.

Design and Development of Magnetic Sensors Based on Giant Magnetoresistance (GMR) Materials

Materials Science Forum, 2006

This paper describes magnetic sensors that have been developed in the last three years. GMR thin film materials have been successfully developed using unpinned CoFe/Cu/CoFe sandwiches on Si(100) substrate using a home built dc-opposed-target magnetron sputtering (OTMS). The magnetization of the sandwich is measured using hysteresis loop instrument, the Vibrating Sample Magnetometer (VSM). It was found that the phase of GMR was formed, with the MR ratio 15.76%.

Observation of a new type of giant magnetoresistance with possible sensor applications

Materials Science and Engineering: B, 1998

We demonstrate the existence of a new type of giant magnetoresistance (GMR) in hybrid semiconductor/ferromagnetic devices. We observe up to a 1000% increase in resistance for applied fields of only 100 mT at a temperature of 4 K and 1% at 300 K. The GMR has a strong angular dependence and it can also be strongly hysteretic. Optimisation of device parameters is expected to increase considerably the magnitude of GMR. Such devices may have applications as magnetic sensors and memories.

Current-perpendicular-to-plane giant magnetoresistance using Co2Fe(Ga1−xGex) Heusler alloy

H. S. Goripati, 2013

Extensive study of giant magnetoresistance properties in half-metallic Co2(Fe,Mn)Si-based devices Appl. Phys. Lett. 101, 252408 (2012) Anisotropic magnetoresistance in topological insulator Bi1.5Sb0.5Te1.8Se1.2/CoFe heterostructures AIP Advances 2, 042171 (2012) Angular-dependences of giant in-plane and interlayer magnetoresistances in Bi2Te3 bulk single crystals Appl. Phys. Lett. 101, 152107 Magnetic field-dependent effective microwave properties of microwire-epoxy composites

Magnetic susceptibility of Hg1−xFexSe

Journal of Magnetism and Magnetic Materials, 1997

The low field AC magnetic susceptibility of Hgl_xFe~Se (x = 0.045, 0.070 and 0.095) has been measured in the temperature range 12 150 K. Our experimental data as well as those reported earlier are compared with the extended nearest-neighbour pair approximation calculations taking into account the long-range antiferromagnetic exchange interaction between Fe 2 + ions in the form J(R) = JNN/R'. Good agreement is found between the theory and experiment with 11 K ~< [JNNI ~< 15 K and n = 5.

Magnetic properties and magnetoresistance of HfFe 6 Ge 6 -type Dy 1- x Gd x Mn 6 Ge 6 ( x =0.1-0.6) compounds

Chinese Physics, 2003

Amorphous Co x C 1−x granular films were prepared on n-Si(100) substrate by dc magnetron sputtering. The effects of Co concentration, film thickness and annealing temperature on the magnetic properties and magnetoresistance (MR) were investigated. After annealing at 500°C for 0.5 hour, the Co(002) peak of the Co x C 1−x (x>2.5 at.%) films was observed, but cracks appeared in the films. Saturation magnetization M s increased steadily with the increase of Co concentration from 2.5 at.% to 50 at.% and also increased with annealing temperature from room temperature to 400°C. The coercivity of Co x C 1−x films was less than 180 Oe. The as-deposited Co 2.5 C 97.5 granular films with 80 nm thickness showed a highly positive MR, up to 15.5% at a magnetic field of 0.8 T, observed at T=300 K when the external magnetic field was perpendicular to the film surface. With increasing film thickness and annealing temperature, the value of MR was found to decrease gradually and changed from positive to negative. The MR effect of the Co x C 1−x granular films can be explained by p-n heterojunction theory and interface scattering effect.