Rafael Perez Del Real

Dr. Rafael Perez Del Real

Tenure Scientist, Institute of Materials Science in Madrid (ICMM-CSIC), 28049 Madrid, Spain
orcid

Research Focus & Metrics

Academic Career Length

34Years (1993-Present)

(Calculated once Scilit publication data is synced: current year − year of first publication + 1)

Representative Publications

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29 December 2000 in Chemistry of Materials
Verified
Journal Article
Closed access
MVM. Vallet-Regi
M. Vallet-Regi
ARA. Rámila
A. Rámila
Rafael Perez Del RealRafael Perez Del Real
Rafael Perez Del Real
JPJoaquin Perez Pariente
Joaquin Perez Pariente

1 September 2002 in Biomaterials
Verified
Journal Article
Closed access
Rafael Perez Del RealRafael Perez Del Real
Rafael Perez Del Real
JWJ.G.C Wolke
J.G.C Wolke
MVM Vallet-Regı́
M Vallet-Regı́
JJJ.A Jansen
J.A Jansen

1 May 2002 in Biomaterials
Verified
Journal Article
Closed access
Daniel ArcosDaniel Arcos
Daniel Arcos
Rafael Perez Del RealRafael Perez Del Real
Rafael Perez Del Real
MVM. Vallet-Regı́
M. Vallet-Regı́

8 January 2016 in Journal of Materials Chemistry C
Verified
Journal Article
Closed access
PDF file
CBCristina Bran
Cristina Bran
EBE. Berganza
E. Berganza
EPEster M. Palmero
Ester M. Palmero
Jose Angel Fernandez-RoldanJose Angel Fernandez-Roldan
Jose Angel Fernandez-Roldan
Rafael Perez Del RealRafael Perez Del Real
Rafael Perez Del Real
MVManuel Vazquez
Manuel Vazquez
The surface and the internal magnetic structure of bamboo-like cylindrical nanowires with tailored diameter modulations have been determined exploiting the direct photoemission and transmission contrasts using photoemission electron microscopy combined with X-ray magnetic circular dichroism, as well as complementary magnetic force microscopy and micromagnetic simulations. Bamboo-like cylindrical nanowires with diameters of 130 and 140 nm, and a modulation periodicity of 400 nm were electrochemically grown into the pores of alumina templates. FeCoCu and Co nanowires were selected to offer parallel and perpendicular magnetization easy axis, respectively. For FeCoCu nanowires, a main longitudinal magnetization configuration is found consistent with the predominant shape anisotropy. In addition, a weaker modulated contrast along the wires’ axis is observed that matches the position of each diameter modulation: vortex-like structures are observed at the ends of the wires and at the surface around the modulations. In Co nanowires, a multi-segmented vortex-like structure with alternating opposite chirality is found not matching the periodicity of the diameter modulations. Such a spin configuration is interpreted considering that Co nanowires exhibit hexagonal symmetry with c axis nearly perpendicular to the nanowires defining strong uniaxial transverse magnetocrystalline anisotropy.

12 February 2018 in Nanoscale
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Journal Article
Closed access
PDF file
Jose Angel Fernandez-RoldanJose Angel Fernandez-Roldan
Jose Angel Fernandez-Roldan
Rafael Perez Del RealRafael Perez Del Real
Rafael Perez Del Real
CBCristina Bran
Cristina Bran
MVManuel Vazquez
Manuel Vazquez
OCOksana Chubikalo-Fesenko
Oksana Chubikalo-Fesenko
We report a novel pinning type in modulated nanowires: the “corkscrew”. The magnetization in wide segments forms a skyrmion-tube with a helical core along the nanowire.

18 January 2012 in Physical Review Letters
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Journal Article
Closed access
MVManuel Vazquez
Manuel Vazquez
GBG. A. Basheed
G. A. Basheed
GIGermán Infante
Germán Infante
Rafael Perez Del RealRafael Perez Del Real
Rafael Perez Del Real
A single domain wall (DW) moves at linearly increasing velocity under an increasing homogeneous drive magnetic field. Present experiments show that the DW is braked and finally trapped at a given position when an additional antiparallel local magnetic field is applied. That position and its velocity are further controlled by suitable tuning of the local field. In turn, the parallel local field of small amplitude does not significantly affect the effective wall speed at long distance, although it generates tail-to-tail and head-to-head pairs of walls moving along opposite directions when that field is strong enough.