2013
DOI: 10.1103/physrevb.87.184428
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Influence of structural disorder on magnetic domain formation in perpendicular anisotropy thin films

Abstract: Using a combination of resonant soft x-ray scattering, magnetometry, x-ray reflectivity and microscopy techniques we have investigated the magnetic properties and microstructure of a series of perpendicular anisotropy Co/Pt multilayer films with respect to structural disorder tuned by varying the sputtering deposition pressure. The observed magnetic changes in domain size, shape and correlation length originate from structural and chemical variations in the samples, such as chemical segregation and grain forma… Show more

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Cited by 45 publications
(35 citation statements)
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“…Changes of the deposition pressure allows tuning the film microstructure from a continuous film to magnetically isolated grains. 28 All the samples demonstrated perpendicular magnetic anisotropy and 100% remanence. The magneto-optical static characterization revealed an increase of the coercive field from with increasing argon pressure from 3 mTorr to 8.5 mTorr.…”
mentioning
confidence: 99%
“…Changes of the deposition pressure allows tuning the film microstructure from a continuous film to magnetically isolated grains. 28 All the samples demonstrated perpendicular magnetic anisotropy and 100% remanence. The magneto-optical static characterization revealed an increase of the coercive field from with increasing argon pressure from 3 mTorr to 8.5 mTorr.…”
mentioning
confidence: 99%
“…Their attractive properties include perpendicular magnetic anisotropy (PMA) and a large polar magneto-optic Kerr effect (MOKE) at short wavelengths 4 . More recently Co/Pt has become an interesting system for the study of the physics of domain walls (DWs) [5][6][7][8] , and spin torque [9][10][11][12][13] . The PMA leads to the formation of narrow, nanometre-scale DWs, and the large polar Kerr effect is convenient for measuring the DW motion.…”
mentioning
confidence: 99%
“…Indeed, if there were no domains inside the LCL, the most energetically stable position for the new LCL domain, would be on top of the HCL domains. 6 From X ¼ 8 to X ¼ 15, the density of LCL domains increases since the mean domain size decreases (as explained above).…”
Section: Resultsmentioning
confidence: 87%
“…This difference is due to the increase of the multilayer interface, roughness, and crystallographic defects induced by the higher deposition pressure. 6 These defects usually lead as well to a higher coercivity and the magnetization reversal process of the high pressure film is then dominated by more frequent domain nucleation processes. Fig.…”
Section: Resultsmentioning
confidence: 99%
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