atomic structure of ag(977) vicinal surface by low energy electron diffraction
DESCRIPTION
Atomic structure of Ag(977) vicinal surface by low energy electron diffraction. Edmar A. Soares, Rosa M.C. Marques, Vagner E. de Carvalho, Hans-D. Pfannes, Roberto Paniago Departamento de Física - ICEx – UFMG Wolfgang Moritz Department of Earth and Environmental Sciences, University of Munich. - PowerPoint PPT PresentationTRANSCRIPT
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Atomic structure of Ag(977) Atomic structure of Ag(977) vicinal surface by low energy vicinal surface by low energy
electron diffractionelectron diffraction
Edmar A. Soares, Rosa M.C. Marques, Vagner E. de Carvalho, Edmar A. Soares, Rosa M.C. Marques, Vagner E. de Carvalho, Hans-D. Pfannes, Roberto PaniagoHans-D. Pfannes, Roberto Paniago
Departamento de Física - ICEx – UFMGDepartamento de Física - ICEx – UFMG
Wolfgang MoritzWolfgang MoritzDepartment of Earth and Environmental Sciences, University Department of Earth and Environmental Sciences, University
of Munich of Munich
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OutlineOutline
What are vicinal surfaces?What are vicinal surfaces? MotivationMotivation Ag(977) surface geometry and reciprocal Ag(977) surface geometry and reciprocal
spacespace Experimental and theoretical detailsExperimental and theoretical details ResultsResults ConclusionsConclusions
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What are vicinal surfaces?What are vicinal surfaces?• Regularly spaced low Miller index terraces separated by monoatomic steps; • Obtained by cutting the crystal at an angle “slightly” off the low Miller index.
Au(788)
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Lang Lang et al et al notationnotation Miller indexMiller index ff
Edge Edge geometrygeometry Unit cell (2D)Unit cell (2D)
p(111) x (100) step p(111) x (100) step AA
8(111) x (100) step 8(111) x (100) step AA
(p+1,p-1,p-1)(p+1,p-1,p-1)(9,7,7)(9,7,7) 2/32/3 nnnn p odd : PRp odd : PR
p even : CRp even : CR
p(111) x (-111) step p(111) x (-111) step BB
8(111) x (-111) step 8(111) x (-111) step BB
(p-2,p,p)(p-2,p,p)(6,8,8)(6,8,8) 1/31/3 nnnn p odd : CRp odd : CR
p even : PRp even : PR
p(100) x (111)p(100) x (111)8(100) x (111)8(100) x (111)
(1,1,2p-1)(1,1,2p-1)(1,1,15)(1,1,15) 1/21/2 nnnn CRCR
p(100) x (010)p(100) x (010)8(100) x (010)8(100) x (010)
(0,1,p-1)(0,1,p-1)(0,1,7)(0,1,7) 00
nnnnnn(kinks)(kinks)
p odd : CRp odd : CRp even : PRp even : PR
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SC – atoms in the step chainTC – atoms in the terrace chains (TC1, TC2, ...)CC – atoms in the corner chainBNN – nearest neighbour of the corner atom in the bulkW – terrace widthr – surface registry
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MotivationMotivation
Cu(111) Si(111) -7x7, 15nm x 15nm Si(111) -7x7, 50nm x 50nm
Steps exist in any kind of surfaces
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Self-organized growth
Co on Pt(997)Science, 416 (2002) 301
Co on Au(788) Co on Au(11,12,12)J.Phys: Condens. Matter 15 (2003) S3363-S3392
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Pt induced facet formation on W(111)
Stability with respect to faceting
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Atomic-force microscopy shows calcite growth with no amino acids (a); with an achiral, or neutral-handed, amino acid, glycine (b); with left-handed aspartic acid (c); and with right-handed aspartic acid (d).
Growth of CoO on Ag(001)
Au(110)
Surface morphology
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Electronic statesJ.Phys: Condens. Matter 15 (2003) S3281-S3310
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Ag(977) surface geometry and Ag(977) surface geometry and reciprocal spacereciprocal space
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Motivation:
-Relaxation of step atoms-Comparison with DFT-calculation-Adsorption at steps
Steps separated by 19.3 Å→ relaxation of a single step
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Experimental and theoretical Experimental and theoretical detailsdetails
ExperimentExperiment
Ag(977) from Surface Lab. Preparation Ag(977) from Surface Lab. Preparation (Netherlands) best polished and aligned to 0.1(Netherlands) best polished and aligned to 0.1°;°;
Sputtering (ArSputtering (Ar++, 500 eV, 25min);, 500 eV, 25min); Annealing (693K, 20 min);Annealing (693K, 20 min); Cooling down (5K/min);Cooling down (5K/min); 15 non-equivalent beams collected at 155K and 15 non-equivalent beams collected at 155K and
nearly normal incidence.nearly normal incidence.
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Ep=44eV Ep=76eV
Ag(977) LEED patterns
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Theory
17 Å
19.3 Å
slab with 56 atoms9 phase shiftsenergy range 30 – 260 eV
optimised parameters:z1 – z18,x1,x2,x7,x8,x9
θD-surf = 160 KθD-bulk = 225 K
dbulk = 0.3061 Å
LEEDFIT code
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Atom Atom nr.nr.
ΔΔ x [ x [ÅÅ]] ΔΔ z [ z [ÅÅ]]
11 -0.10-0.10 +0.125+0.125
22 -0.01-0.01 +0.08+0.08
33 -- -0.02-0.02
44 -- +0.01+0.01
55 -- 00
66 -- 00
77 -- 00
88 -0.14-0.14 -0.09-0.09
99 -0.02-0.02 +0.11+0.11
1010 -- +0.02+0.02
1111 -- 00
1414 -- 00
1515 -- 00
1616 00 -0.02-0.02
1717 00 +0.04+0.04
1818 00 +0.01+0.01
1 2 3 4 55 6 7 8 9 10 11 12 1314 15 16 17 18
-x +x
Results so far...Results so far...
d1-2 = - 15%d2-3 = - 33%d8-9 = +65%d9-10 = -29%
RP=0.32
+z
Δx, Δz : deviation from bulk position
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d1-2 = - 15% - d2-3 = - 33% - d8-9 = +65% - d9-10 = -29% - RP=0.32
1 2 38 9
4
10
16 17 18
Atom Atom nr.nr.
ΔΔ x [ x [ÅÅ]] ΔΔ z [ z [ÅÅ]]
11 -0.10-0.10 +0.125+0.125
22 -0.01-0.01 +0.08+0.08
33 -- -0.02-0.02
44 -- +0.01+0.01
55 -- 00
66 -- 00
77 -- 00
88 -0.14-0.14 -0.09-0.09
99 -0.02-0.02 +0.11+0.11
1010 -- +0.02+0.02
1111 -- 00
1414 -- 00
1515 -- 00
1616 00 -0.02-0.02
1717 00 +0.04+0.04
1818 00 +0.01+0.01
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Surf. Sci. 600 (2006) 3008-3014
DFT: Cu - p(111)x(11-1) – (p,p,p-2)
J.Phys: Condens. Matter 15 (2003) S3197-S3226
Experimental
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Conclusions and future workConclusions and future work
Reasonable agreement between experiment-theory;Reasonable agreement between experiment-theory; Large inward relaxation of the step atoms;Large inward relaxation of the step atoms; Large outward relaxation of the corner atoms;Large outward relaxation of the corner atoms;
Finish the structural determination of the Ag(977) Finish the structural determination of the Ag(977) and compare the results with DFT and ECT and compare the results with DFT and ECT calculations;calculations;
Study of the electronic structure of Ag(977)(1x1) by Study of the electronic structure of Ag(977)(1x1) by ARUPS and STM;ARUPS and STM;
Adsortion of large molecules and transition-metal Adsortion of large molecules and transition-metal atoms on Ag(977);atoms on Ag(977);
Structure determination on other p(111)x(100) Ag Structure determination on other p(111)x(100) Ag vicinal surfaces to better understand the relation vicinal surfaces to better understand the relation between surface relaxations and the number of between surface relaxations and the number of atoms p on the terrace.atoms p on the terrace.
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