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Growth Behavior of Co on Al(001) substrate

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Growth Behavior of Co on Al(001) substrate. Sang-Pil Kim 1),2) , Seung-Cheol Lee 1) , Kwang-Ryeol Lee 1) and Yong-Chae Chung 2) Future Technology Research Division, KIST, Seoul, Korea Department of Ceramic Engineering, Hanyang University, Seoul, Korea. Introduction. 1~2nm. - PowerPoint PPT Presentation
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Growth Behavior of Co on Growth Behavior of Co on Al(001) substrate Al(001) substrate Sang-Pil Kim 1),2) , Seung-Cheol Lee 1) , Kwan g-Ryeol Lee 1) and Yong-Chae Chung 2) 1) Future Technology Research Division, KIST, Seoul, Korea 2) Department of Ceramic Engineering, Hanyang Univer sity, Seoul, Korea
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Page 1: Growth Behavior of Co on Al(001) substrate

Growth Behavior of Co on Growth Behavior of Co on Al(001) substrateAl(001) substrate

Sang-Pil Kim1),2), Seung-Cheol Lee1), Kwang-Ryeol Lee1) and Yong-Chae Chung2)

1) Future Technology Research Division, KIST, Seoul, Korea

2) Department of Ceramic Engineering, Hanyang University, Seoul, Korea

Page 2: Growth Behavior of Co on Al(001) substrate

CMSELCMSELCMSELCMSELHanyang Hanyang Univ.Univ.

ACCMS-3The 3rd Conference of the Asian Consortium for Computational Materials Science

IntroductionIntroduction

• The efficiency of spintronic devices (e.g. TMR, GMR ... ) are largely dependent on the electronic structure of the active layers, and electronic structures are closely related to both interface and thin film structures.

• Research on interface or thin film structures in hetero-epitaxial growth FCC/BCC Ni on Fe(100), Cu on Fe(100), Fe on Al(100) … HCP/FCC, BCC/HCP Co on Cr(100), Co on Mo(100) …

1~2nm

Typical structure of spintronic device

Page 3: Growth Behavior of Co on Al(001) substrate

CMSELCMSELCMSELCMSELHanyang Hanyang Univ.Univ.

ACCMS-3The 3rd Conference of the Asian Consortium for Computational Materials Science

Surface Alloying of Co on Al(001)Surface Alloying of Co on Al(001)

Surface unit cell of Al(001) and B2-CoAl(001) have less than 0.1% lattice mismatch Highly ordered surface alloying

Even when the incident energy of the Co atom was 0.1 eV spontaneous intermixing of Co and Al was observed*.

Co

4.05 Å

2.86 Å

Al

3ML Co on Al(001)

* S.-P. Kim et al., J. Appl. Phys., 93, 8564 (2003)

3ML Al on Co(001)

Page 4: Growth Behavior of Co on Al(001) substrate

CMSELCMSELCMSELCMSELHanyang Hanyang Univ.Univ.

ACCMS-3The 3rd Conference of the Asian Consortium for Computational Materials Science

Magnetic Behavior of CoAlMagnetic Behavior of CoAl

B2 - CoAlB2 - CoAl

B2-CoAl & Al-rich CoxAl1-x Nonmagnetic behavior

Co-rich CoxAl1-x

Ferro magnetic behavior

Nonmagneticbehavior

Magneticbehavior

Al-rich Co-rich

Page 5: Growth Behavior of Co on Al(001) substrate

CMSELCMSELCMSELCMSELHanyang Hanyang Univ.Univ.

ACCMS-3The 3rd Conference of the Asian Consortium for Computational Materials Science

MotivationMotivation

Co: Ferromagnetic

CoAl: Nonmagnetic

Co: Ferromagnetic

• Active intermixing & Nonmagnetic B2-CoAl for Co on Al substrate• Sharp interface & Layer-by-layer growth of Al for Al on Co substrate

Al deposition

Co substrate Al on Co substrate

GMRstructure

Investigate thin film growth behavior of Co films on CoAl

Page 6: Growth Behavior of Co on Al(001) substrate

CMSELCMSELCMSELCMSELHanyang Hanyang Univ.Univ.

ACCMS-3The 3rd Conference of the Asian Consortium for Computational Materials Science

Calculation MethodsCalculation Methods

(001) Substrate(001) Substrate

1440 atoms (144atoms/ML)

Substrate dimensions : (12 6 5)a0

a0 : bulk lattice constant

• Embedded Atom Method Potentials for Co-Al system

• x,y Periodic Boundary Condition z Open surface (fixing the bottom-most two layers)

• Substrate Temp. : 300K

• Incident Energy with normal incidence 0.1 eV, and 3.0 eV

• Time step : 1 fs 5000 fs (5 ps) / atom

• Deposition rate: 1.306 × 10-1 nm/nsec

ConditionsConditions

x[100]

z[001]y[010]

Page 7: Growth Behavior of Co on Al(001) substrate

CMSELCMSELCMSELCMSELHanyang Hanyang Univ.Univ.

ACCMS-3The 3rd Conference of the Asian Consortium for Computational Materials Science

Co Thin Film ICo Thin Film I1~10ML: 0.1 eV incident E. of Co adatom10~20ML: 3.0 eV

12 ML

15 ML

18 ML

x[100]

z[001]

Page 8: Growth Behavior of Co on Al(001) substrate

CMSELCMSELCMSELCMSELHanyang Hanyang Univ.Univ.

ACCMS-3The 3rd Conference of the Asian Consortium for Computational Materials Science

Size Effect TestSize Effect Test

15 ML

18 ML

20 ML

(50×6×8)a0 9600 substrate Al atoms

Same behavior!

Page 9: Growth Behavior of Co on Al(001) substrate

CMSELCMSELCMSELCMSELHanyang Hanyang Univ.Univ.

ACCMS-3The 3rd Conference of the Asian Consortium for Computational Materials Science

Phase TransitionPhase Transition

A: HCP, B: FCT, C: B2(BCC)

Sinking due to the lattice mismatch A little moved to the one side

Face centered tetragonal (FCT) HCP (11-20)

≈60°

fcc-Co: 3.56 Åvs.

Al: 4.05 Å

Page 10: Growth Behavior of Co on Al(001) substrate

CMSELCMSELCMSELCMSELHanyang Hanyang Univ.Univ.

ACCMS-3The 3rd Conference of the Asian Consortium for Computational Materials Science

Geometric RelationshipsGeometric Relationships

Al

CoAl

Co

7.4 % larger than substrate

~ 0.1 %

x[100]

z[001]

Page 11: Growth Behavior of Co on Al(001) substrate

CMSELCMSELCMSELCMSELHanyang Hanyang Univ.Univ.

ACCMS-3The 3rd Conference of the Asian Consortium for Computational Materials Science

Co Thin Film Growth IICo Thin Film Growth II

12 ML

15 ML

18 ML

1~20 ML: 0.1 eV, Sub. Temp.: 300 K

x[100]

z[001]

Page 12: Growth Behavior of Co on Al(001) substrate

CMSELCMSELCMSELCMSELHanyang Hanyang Univ.Univ.

ACCMS-3The 3rd Conference of the Asian Consortium for Computational Materials Science

Schematic of Strain EnergySchematic of Strain Energy

Str

ain

Ene

rgy

HCP FCT

Al substrate

Co film

HCP+FCT

Whole system

Co film structure

Page 13: Growth Behavior of Co on Al(001) substrate

CMSELCMSELCMSELCMSELHanyang Hanyang Univ.Univ.

ACCMS-3The 3rd Conference of the Asian Consortium for Computational Materials Science

Growth behavior of Co thin film on Al substrate by

Molecular Dynamics simulation.

Co thin film was composed of two different hetero e

pitaxial grains of HCP and FCT structure.

The fraction of each grain seems to be determined b

y minimizing the total strain energy of both thin film

and substrate.

SummarySummary


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