2003
DOI: 10.1103/physrevb.67.224430
|View full text |Cite
|
Sign up to set email alerts
|

Growth of epitaxial bcc Co(001) electrodes for magnetoresistive devices

Abstract: The applicability of the strain-induced bcc phase of Co in magnetoresistive devices was studied. Ultrathin bcc Co͑001͒ films and the influence of the additional layers needed for magnetoresistive devices were examined by means of 59 Co nuclear magnetic resonance ͑NMR͒. NMR is shown to be a discriminating technique for determining the presence of structurally and magnetically pure bcc Co. The maximum stability for uncovered and Fe-covered layers grown on Fe͑001͒/GaAs͑001͒ and Fe͑001͒/Ge͑001͒ seed layers is foun… Show more

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
2
1

Citation Types

0
24
0

Year Published

2004
2004
2016
2016

Publication Types

Select...
6
2

Relationship

1
7

Authors

Journals

citations
Cited by 30 publications
(24 citation statements)
references
References 46 publications
(95 reference statements)
0
24
0
Order By: Relevance
“…The growth of tetragonally distorted ð1 0 0Þ-oriented Co films has been reported for Co on Ptð1 0 0Þ [9], GaAsð1 0 0Þ [10], Geð1 0 0Þ [11], Feð1 0 0Þ [2,[12][13][14], FeAlð1 0 0Þ [15], Pdð1 0 0Þ [16,17], Wð1 0 0Þ [18,19] and Auð1 0 0Þ [20]. On Crð1 0 0Þ, Co grows pseudomorphically in a bcc structure for the first few monolayers followed by continuous relaxation towards hcp structure [21,22].…”
Section: Introductionmentioning
confidence: 92%
“…The growth of tetragonally distorted ð1 0 0Þ-oriented Co films has been reported for Co on Ptð1 0 0Þ [9], GaAsð1 0 0Þ [10], Geð1 0 0Þ [11], Feð1 0 0Þ [2,[12][13][14], FeAlð1 0 0Þ [15], Pdð1 0 0Þ [16,17], Wð1 0 0Þ [18,19] and Auð1 0 0Þ [20]. On Crð1 0 0Þ, Co grows pseudomorphically in a bcc structure for the first few monolayers followed by continuous relaxation towards hcp structure [21,22].…”
Section: Introductionmentioning
confidence: 92%
“…Therefore, in the calculation of Oleinik et al the strained Co layer proceeded along the Bain path from the fcc to the slightly distorted bcc structure. It is therefore likely that the top Co electrode in the experiments of de Teresa et al [19] grew in the bcc phase on SrTiO 3 , and that fully crystalline bcc Co/SrTiO 3 /Co(001) MTJs may be grown on a suitable substrate (see, e.g., experimental papers [44,45] on growth of bcc Co and a recent paper [46] showing a large TMR in bcc Co/MgO/Fe(001) MTJs). The spin-resolved conductance of a Co/SrTiO 3 /Co MTJ is shown in Fig.10b as a function of barrier thickness.…”
Section: Negative Spin Polarization In Co/srtio 3 /Co Tunnel Junctionsmentioning
confidence: 99%
“…Cobalt assumes hcp structure in bulk and fcc structure in thin films. It can also be grown in bcc structure on a Cr substrate [14] and on GaAs or Ge substrates covered with an Fe seed layer [15]. The equilibrium lattice parameter of bcc Co is 2.83 Å [16] which has only a 2.3% mismatch with the SrTiO 3 lattice rotated through 45…”
mentioning
confidence: 99%