@article {5117,
	title = {Tensor LEED analysis for the electrodeposited Pt(111)-(3x3)-Ag,I surface structure},
	journal = {Surface Science},
	volume = {490},
	number = {3},
	year = {2001},
	note = {ISI Document Delivery No.: 473XWTimes Cited: 5Cited Reference Count: 34},
	month = {Sep},
	pages = {256-264},
	type = {Article},
	abstract = {A crystallographic analysis is reported using low-energy electron diffraction (LEED) in the tensor LEED approach for the electrodeposited coadsorption (3 x 3) structure with 4/9 monolayer (ML) of silver and 4/9 ML of iodine on the Pt(1 1 1) surface. The structure approximates a two-layer slice of bulk AgI cut parallel to its (1 1 1) plane and superimposed on the substrate with the Ag atoms in contact with the topmost Pt(1 1 1) layer, and the I atoms forming an overlayer on the Ag atoms. There are two types of Ag atoms in the (3 x 3) unit mesh; one type bonds to a single Pt atom, while the other type bonds to three Pt atoms. The average Ag-Pt bond distances are close to 2.48 and 2.82 (A) over circle respectively for the one and three-coordinate Ag atoms, but both types of Ag atoms bond to three I atoms with an average Ag-I distance of 2.67 (A) over circle. No significant corrugation is observed for either the I layer or the Ag layer. (C) 2001 Elsevier Science B.V. All rights reserved.},
	keywords = {ADSORBATES, ADSORPTION, AG, chemisorption, ELECTROCHEMISTRY, ENERGY-ELECTRON-DIFFRACTION, IODINE, LOW ENERGY ELECTRON DIFFRACTION (LEED), METAL-SURFACES, platinum, PT(111), SCANNING-TUNNELING-MICROSCOPY, silver},
	isbn = {0039-6028},
	url = {<Go to ISI>://000171075300007},
	author = {Labayen, M. and Harrington, D. A. and Saidy, M. and Mitchell, K. A. R.}
}
@article {4656,
	title = {Tensor LEED analyses for three chemisorbed structures formed by iodine on a Pt(111) surface},
	journal = {Surface Review and Letters},
	volume = {6},
	number = {5},
	year = {1999},
	note = {ISI Document Delivery No.: 300LQTimes Cited: 17Cited Reference Count: 406th International Conference on the Structure of Surfaces (ICSOS-6)JUL 26-30, 1999VANCOUVER, CANADAUniv British Columbia},
	month = {Oct},
	pages = {871-881},
	type = {Proceedings Paper},
	abstract = {Three distinct ordered iodine structures on a Pt(lll) surface have been studied with LEED crystallography in the coverage range 0.33-0.44 monolayers. These surfaces have translational symmetries of the ((root 3 x root 3)R30 degrees, (root 7 x root 7)R19.1 degrees and (3 x 3) types, and they all involve overlayer adsorption on the basically unreconstructed metal structures. The root 3 surface phase is indicated to have essentially all I atoms adsorbed at the regular threefold sites of the fee type (i.e. 3f sites), with no significant involvement by the corresponding sites of the hcp type (i.e. 3h sites). The root 7 structure has one I on an atop Pt site, and one each at 3f and 3h sites per unit mesh, while the (3 x 3) surface has one I on an atop site and three on bridge sites per unit mesh. The I corrugation is about 0.5 Angstrom for the root 7 structure, but is reduced to around 0.1 Angstrom at the (3 x 3) surface. The surface I-Pt bond lengths from these analyses show a general tendency to follow trends expected with the varying I coordination numbers. A preliminary discussion is given for uncertainties associated with some relaxations indicated in the metallic structures.},
	keywords = {ADSORBATES, ADSORPTION, ELECTROCHEMISTRY, ENERGY-ELECTRON-DIFFRACTION, METAL-SURFACES, PT(100), RELIABILITY, RH(111), SCANNING TUNNELING MICROSCOPY, TRANSFORMATIONS},
	isbn = {0218-625X},
	url = {<Go to ISI>://000086254800043},
	author = {Saidy, M. and Mitchell, K. A. R. and Furman, S. A. and Labayen, M. and Harrington, D. A.}
}
@article {4655,
	title = {Tensor LEED analysis for the Cu(111)-(root x root 7)R19.1 degrees-S surface structure},
	journal = {Surface Science},
	volume = {441},
	number = {2-3},
	year = {1999},
	note = {ISI Document Delivery No.: 253RWTimes Cited: 11Cited Reference Count: 36},
	month = {Nov},
	pages = {425-435},
	type = {Article},
	abstract = {A tensor LEED analysis is reported for the (root 7 x root 7)R19.1 degrees structure formed by S at the Cu(lll)surface. A new structural model is found which corresponds to a modified version of the copper sulphide overlayer model first proposed by Domange and Oudar. In that model, the topmost layer has 3/7 monolayer each of Cu and S atoms, but the modification involves one S atom per unit mesh moving down to displace a Cu atom from the second metal layer. Relaxations among the topmost Cu atoms result in one S atom being effectively three-fold coordinate while the other two are sixfold coordinate and 12-fold coordinate: the averaged S-Cu bond lengths are indicated to equal 2.19, 2.47 and 2.62 Angstrom respectively. Some discussion is included of factors that may influence this choice of surface structure. (C) 1999 Elsevier Science B.V. All rights reserved.},
	keywords = {ADSORPTION, chemisorption, copper, ENERGY-ELECTRON-DIFFRACTION, LAYERS, low energy electron diffraction, LOW INDEX SINGLE CRYSTAL, METAL-SURFACES, MOLECULE, RAY STANDING-WAVE, RECONSTRUCTION, RU(0001), SUBSTRATE, SULFUR, sulphur, SURFACE, surface reconstruction},
	isbn = {0039-6028},
	url = {<Go to ISI>://000083570400024},
	author = {Saidy, M. and Mitchell, K. A. R.}
}
@article {4657,
	title = {Tensor LEED analysis for the Ni(111)-(root 7 x root 7)R19.1 degrees-P surface structure: Comparison with other root 7 systems},
	journal = {Surface and Interface Analysis},
	volume = {28},
	number = {1},
	year = {1999},
	note = {ISI Document Delivery No.: 234JZTimes Cited: 1Cited Reference Count: 36Asia-Pacific Surface and Interface Analysis Conference 1998 (APSIAC 98)NOV 30-DEC 04, 1998SINGAPORE, SINGAPORE},
	month = {Aug},
	pages = {84-91},
	type = {Proceedings Paper},
	abstract = {A crystallographic analysis is reported using low-energy electron diffraction (LEED) in the tensor LEED approach for the (root 7 x root 7)R19.1 degrees structure formed by 3/7 monolayer of phosphorus at the Ni(111) surface. This surface has a novel structure in which each phosphorus atom bonds to seven neighbouring Ni atoms, four in the top layer and three in the second layer, at an average distance close to 2.39 Angstrom. Formally this reconstruction involves three neighbouring Ni atoms in a triangular arrangement per unit mesh of the original unreconstructed surface being replaced by three phosphorus atoms. A discussion is included of the structural relaxations that occur in this surface as the demands of Ni-P bonding are balanced against those for Ni-Ni and P-P contributions. Comparisons are made with the root 7 reconstructions observed for related systems, including those for P/Rh(111), S/Pd(111) and S/Cu(111). Copyright (C) 1999 John Wiley \& Sons, Ltd.},
	keywords = {(ROOT-3X-ROOT-3)R30-DEGREES, analysis, chemisorption, CRYSTALLOGRAPHIC, ENERGY-ELECTRON-DIFFRACTION, LEED, METAL-SURFACES, Ni, NI(111), P, RAY STANDING-WAVE, RECONSTRUCTION, RELAXATIONS, SUBSTRATE, SULFUR},
	isbn = {0142-2421},
	url = {<Go to ISI>://000082482200018},
	author = {Saidy, M. and Zhou, M. Y. and Mitchell, K. A. R.}
}
@article {4151,
	title = {LEED crystallographic analysis for the structure formed by 2 ML of O at the Zr(0001) surface},
	journal = {Surface Science},
	volume = {380},
	number = {2-3},
	year = {1997},
	note = {ISI Document Delivery No.: XF843Times Cited: 17Cited Reference Count: 29},
	month = {May},
	pages = {540-547},
	type = {Article},
	abstract = {A tensor LEED analysis is reported for the Zr(0001)-(1 x 1)-O surface which involves oxygen at a total coverage of 2 monolayers. The structure is indicated to have two layers of O: one forms an overlayer in which the O atoms bond to hollow sites of three-fold coordination on the regular metal surface. while the other laver has the O atoms in tetrahedral hole sires between the first and second metal layers. The stacking sequence, designated as (C)B(A)AB, corresponds to the first three layers of anion-terminated cubic ZrO2, although some lateral compression is needed for superposition on the regular hcp Zr structure. The absorption of O in the tetrahedral holes results in a significant expansion in the first-to-second Zr-Zr interlayer spacing to about 3.44 Angstrom from the bulk vaue of 2.57 Angstrom. The O-Zr bond lengths are estimated to equal 2.07 Angstrom for the overlayer O atoms, and 2.21 Angstrom for the O atoms in tetrahedral hole sites, Comparisons are made with the structures of the corresponding 0.5 and 1 ML surfaces formed by the O/Zr(0001) system. (C) 1997 Elsevier Science B.V.},
	keywords = {ENERGY-ELECTRON-DIFFRACTION, GROWTH, LEED crystallography, low index single crystal surface, OXIDE THIN-FILMS, OXYGEN, SINGLE-CRYSTAL SURFACES, STRUCTURE, SURFACE, ZIRCONIUM},
	isbn = {0039-6028},
	url = {<Go to ISI>://A1997XF84300044},
	author = {Wang, Y. M. and Li, Y. S. and Mitchell, K. A. R.}
}
@article {4061,
	title = {The structure of the Pd(111)-(root 7x root 7)R19.1 degrees-S surface: comparison with the corresponding P/Rh(111) surface},
	journal = {Surface Science},
	volume = {393},
	number = {1-3},
	year = {1997},
	note = {ISI Document Delivery No.: YP959Times Cited: 15Cited Reference Count: 35},
	month = {Dec},
	pages = {L119-L125},
	type = {Letter},
	abstract = {The structure of the Pd(lll)-(root 7 x root 7)R19.1<degrees-S surface has been determined by low-energy electron diffraction and has been shown to involve a reconstructed topmost metal layer based on a packed arrangement of Pd pentagons and triangles, with S atoms at 3/7 monolayer coverage occupying eight-coordinate sites at the centre of each Pd pentagon. Comparisons are made with the structure recently determined for the corresponding P/Rh(lll) system. In both cases, the atomic density in the reconstructed layer increases to five metal atoms and three chemisorbed atoms for every seven atoms in the regular metal surface. Some details are closely similar between the two systems, but an intriguing difference is also indicated. In S/Pd(lll), four metal atoms in each pentagonal ring appear close to hcp-type three-fold sites, while the other is close to a fee-type three-fold site. This contrasts with the situation for the topmost layer of the P/Rh(lll) system, for which the reversed lateral registry has been reported (i.e. the atoms of each pentagonal ring occupy three-fold sites where four are of the fee type and one of the hcp type). (C) 1997 Elsevier Science B.V.},
	keywords = {ADSORBATE STRUCTURE, ARRANGEMENT, chemisorption, CRYSTAL SURFACES, CRYSTALLOGRAPHY, ENERGY-ELECTRON-DIFFRACTION, LEED INTENSITY ANALYSIS, low energy electron diffraction crystallography, LOW INDEX SINGLE, METAL-SURFACES, palladium, PD(111) SURFACE, RECONSTRUCTION, SULFUR, sulphur, surface structure},
	isbn = {0039-6028},
	url = {<Go to ISI>://000071333200009},
	author = {Liu, W. and Mitchell, K. A. R. and Berndt, W.}
}
@article {3856,
	title = {LEED crystallographic analysis for the Rh(111)-(2x1)-O surface structure},
	journal = {Surface Science},
	volume = {360},
	number = {1-3},
	year = {1996},
	note = {ISI Document Delivery No.: UX923Times Cited: 29Cited Reference Count: 32},
	month = {Jul},
	pages = {137-143},
	type = {Article},
	abstract = {A tensor LEED analysis is reported For the Rh(111)-(2 x 1)-O surface structure in which atoms in the O overlayer chemisorb close to the regular (fcc type) three-fold hollow sites for half-monolayer coverage. The structure shows significant relaxations: for example, a buckling of about 0.07 Angstrom is indicated in the first metal layer and O appears to displace laterally by about 0.05 Angstrom. The individual O-Rh bond lengths are around 2.01 and 1.92 Angstrom to top layer Rh atoms, which bond to two and one O atoms, respectively, but the average value (1.98 Angstrom) is close to that in bulk RhO2 (1.96 Angstrom). Comparison is also made with the previously determined O-Rh bond lengths in the Rh(110)-p2mg(2 x 1) surface structure.},
	keywords = {CLOSE-PACKED SURFACE, EJECTION, ENERGY-ELECTRON-DIFFRACTION, LAYER, low energy electron diffraction, low index single crystal surfaces, OXYGEN, P(2X2)O/RH(111), RECONSTRUCTION, RELAXATIONS, RH(111), rhodium, surface relaxations, THERMAL-DESORPTION},
	isbn = {0039-6028},
	url = {<Go to ISI>://A1996UX92300022},
	author = {Wong, K. C. and Liu, W. and Mitchell, K. A. R.}
}
@article {3546,
	title = {LEED ANALYSES REVISITED FOR 2 STRUCTURES FORMED BY ZR(0001) - THE SURFACE WHEN CLEAN AND WHEN CONTAINING SUFFICIENT OXYGEN TO JUST EXTINGUISH THE HALF-ORDER BEAMS},
	journal = {Surface Science},
	volume = {343},
	number = {1-2},
	year = {1995},
	note = {ISI Document Delivery No.: TK128Times Cited: 26Cited Reference Count: 22},
	month = {Dec},
	pages = {L1167-L1173},
	type = {Letter},
	abstract = {LEED crystallographic analyses have been made for two structures formed by the (0001) surface of zirconium and which show (1 x 1)-type diffraction patterns. An analysis with eight diffracted beams for clean Zr(0001) supports an earlier conclusion that this surface has a regular hcp-type structure, and that the first interlayer spacing shows a contraction hem the bulk spacing by about 1.6\%. A surface formed by O, at twice the coverage applying for the best-developed half-monolayer (2x2) diffraction pattern, is analyzed using tensor LEED for nine diffracted beams, including the use of the average t-matrix approximation. It is concluded that the 1 monolayer (ML) structure is actually disordered with 0.5 ML of O distributed statistically over octahedral holes between the first and second Zr layers, and another 0.5 ML of O similarily distributed between the second and third metal layers.},
	keywords = {CRYSTALLOGRAPHIC INVESTIGATIONS, ENERGY-ELECTRON-DIFFRACTION, LOW ENERGY ELECTRON DIFFRACTION (LEED), LOW INDEX SINGLE CRYSTAL, OXYGEN, SANDWICH, SURFACE RELAXATION AND RECONSTRUCTION, SURFACES, ZIRCONIUM},
	isbn = {0039-6028},
	url = {<Go to ISI>://A1995TK12800004},
	author = {Wang, Y. M. and Li, Y. S. and Mitchell, K. A. R.}
}
@article {3547,
	title = {A LEED CRYSTALLOGRAPHIC ANALYSIS FOR THE HALF MONOLAYER STRUCTURE FORMED BY O AT THE ZR(0001) SURFACE},
	journal = {Surface Science},
	volume = {342},
	number = {1-3},
	year = {1995},
	note = {ISI Document Delivery No.: TH886Times Cited: 32Cited Reference Count: 35},
	month = {Nov},
	pages = {272-280},
	type = {Article},
	abstract = {A tensor LEED analysis has been made for the half monolayer structure formed by O absorbed at the Zr(0001) surface. The analysis uses intensity-versus-energy curves for eight independent diffracted beams measured at normal incidence. The best correspondence with the experimental intensity data is for a model in which O atoms occupy octahedral holes in an unreconstructed metallic structure, with 0.25 ML between the first and second metal layers, and another 0.25 ML between the second and third metal layers. These two (2 X 2)-O arrays are displaced laterally from one another by an unit translational vector of the Zr(0001) substrate. The O atoms induce both vertical and lateral relaxations in the three topmost Zr layers; the largest displacements being found in the second Zr layer. The averaged O-Zr bond length is 2.28 Angstrom, about 0.02 Angstrom shorter than the value in bulk ZrO.},
	keywords = {0001 SURFACE, 2)-O, ALPHA-AL2O3, chemisorption, ENERGY-ELECTRON-DIFFRACTION, INDUCED RECONSTRUCTION, LOW ENERGY ELECTRON DIFFRACTION (LEED), LOW INDEX SINGLE CRYSTAL, OXIDATION, OXYGEN, SURFACE RELAXATION, SURFACES, X, ZIRCONIUM},
	isbn = {0039-6028},
	url = {<Go to ISI>://A1995TH88600034},
	author = {Wang, Y. M. and Li, Y. S. and Mitchell, K. A. R.}
}
@article {3430,
	title = {A NOVEL SURFACE-STRUCTURE - RH(111)-(ROOT-7X-ROOT-7)R19.1-DEGREES-P},
	journal = {Journal of the American Chemical Society},
	volume = {117},
	number = {49},
	year = {1995},
	note = {ISI Document Delivery No.: TK382Times Cited: 7Cited Reference Count: 26},
	month = {Dec},
	pages = {12344-12345},
	type = {Note},
	keywords = {acetylene, chemisorption, CYCLOTRIMERIZATION, ENERGY-ELECTRON-DIFFRACTION, HETEROCYCLIZATION SITES, INTERMEDIATE, MOLECULAR PATHWAYS, palladium, SUBSTRATE, SULFIDED PD(111) SURFACE},
	isbn = {0002-7863},
	url = {<Go to ISI>://A1995TK38200041},
	author = {Liu, W. and Wong, K. C. and Mitchell, K. A. R.}
}
@article {3431,
	title = {STRUCTURAL DETAILS FOR THE CU(110)-C(6X2)-O SURFACE DETERMINED BY TENSOR LEED},
	journal = {Surface Science},
	volume = {339},
	number = {1-2},
	year = {1995},
	note = {ISI Document Delivery No.: RV213Times Cited: 18Cited Reference Count: 28},
	month = {Sep},
	pages = {151-158},
	type = {Article},
	abstract = {A tenser LEED analysis has been made for the Cu(110)-c(6 x 2)-O surface structure using intensity versus energy curves measured for 13 diffracted beams at normal incidence. A good level of correspondence between experimental and calculated intensities has been reached (R(p) = 0.271) for the model type (2/3 monolayer coverage of O) proposed for this surface by Feidenhans{\textquoteright}l et al. This analysis provides direct information on the structural details, and it is indicated that they support the view that the driving force for this structure relates to sufficient O being incorporated in order to stabilize the surface as a modified (211) plane of bulk Cu2O. This structure is composed of double-stranded chains built from 12-membered rings formed by alternating O and Cu atoms. The chains are flattened on the surface, and alternating chains are laterally displaced by half a repeat unit compared with the bulk (211) plane. However, the three-atom O-Cu-O fragments essentially maintain their bulk form in the surface structure. The average O-Cu bond length in Cu(110)-c(6 X 2)-O is indicated to equal 1.90 Angstrom, in exact agreement with the values determined for the half monolayer structures formed by O on Cu(110) and Cu(100).},
	keywords = {copper, CRYSTAL SURFACES, CU, CU(110), ENERGY-ELECTRON-DIFFRACTION, LOW ENERGY ELECTION DIFFRACTION (LEED), LOW INDEX SINGLE, OXYGEN, OXYGEN-CHEMISORPTION, SURFACE RELAXATION AND RECONSTRUCTION, X-RAY-DIFFRACTION},
	isbn = {0039-6028},
	url = {<Go to ISI>://A1995RV21300017},
	author = {Liu, W. and Wong, K. C. and Mitchell, K. A. R.}
}
@article {3559,
	title = {Tensor LEED analysis for the Rh(110)-(3x2)-S surface structure},
	journal = {Surface Science},
	volume = {344},
	number = {3},
	year = {1995},
	note = {ISI Document Delivery No.: TQ239Times Cited: 6Cited Reference Count: 26},
	month = {Dec},
	pages = {258-266},
	type = {Article},
	abstract = {A tensor LEED analysis for the Rh(110)-(3 x 2)-S surface supports an arrangement of chemisorbed S atoms at 2/3 monolayer coverage on a basically unreconstructed metallic structure. Alternating [1(1) over bar0$] channels in the metal surface are occupied differently, although each has two S atoms per unit mesh. In one set, the S atoms occupy long-bridge and centre sites with a constant separation along the channel of 4.03 Angstrom. In the other set of channels, all S atoms occupy equivalent positions, displaced from regular centre sites by 0.39 Angstrom, to give successive S to S separations of 3.47 and 4.60 Angstrom. The long-bridge site bonding is a novel feature which is facilitated by the neighbouring topmost Rh atoms relaxing laterally by about 0.27 Angstrom perpendicular to the [1(1) over bar0$] row. Bucklings of 0.20 and 0.10 Angstrom are indicated to occur in the first and second Rh layers respectively; the latter value essentially equals that (0.11 Angstrom) reported earlier for the corresponding half monolayer c(2 x 2) surface. For S atoms at or near centre sites in the (3 x 2) structure, the average S-Rh bond distances are 2.42 and 2.29 Angstrom to the first and second layer Rh atoms respectively; the corresponding values at the long-bridge sites are 2.20 and 2.27 Angstrom.},
	keywords = {chalcogens, chemisorption, CRYSTAL SURFACES, ENERGY-ELECTRON-DIFFRACTION, GENERAL TRENDS, LOW ENERGY ELECTRON DIFFRACTION (LEED), LOW INDEX SINGLE, rhodium, SULFUR ADSORPTION, SURFACE RELAXATION AND RECONSTRUCTION},
	isbn = {0039-6028},
	url = {<Go to ISI>://A1995TQ23900020},
	author = {Wong, K. C. and Liu, W. and Mitchell, K. A. R.}
}
@article {3432,
	title = {What determines the structures formed by oxygen at low index surfaces of copper?},
	journal = {Progress in Surface Science},
	volume = {50},
	number = {1-4},
	year = {1995},
	note = {ISI Document Delivery No.: TL808Times Cited: 25Cited Reference Count: 3515th Biennial Canadian Conference on Surface Science (Surface Canada 95)MAY 25-27, 1995WATERLOO, CANADACanadian Soc Chem, Div Surface Sci, Canadian Assoc Physicists},
	month = {Sep-Dec},
	pages = {247-257},
	type = {Proceedings Paper},
	abstract = {This article reviews structural details from tensor LEED analyses for three oxygen on copper surfaces, specifically those designated Cu(11O)-(2x1)-O, Cu(110)-c(6x2)-O and Cu(100)-(2 root 2x root 2)R45 degrees-O. Certain common features are identified and discussed. It appears that these particular structures receive some stability from being able to fit O-Cu-O building blocks, of the sort needed to construct bulk Cu2O, on to the Cu substrates. Each O atom maintains a four-coordinate status, while simultaneously allowing reasonable O-Cu bond lengths. Comparisons are made with other related systems, namely O at Ni and N at Cu surfaces.},
	keywords = {chemisorption, CU(110), ENERGY-ELECTRON-DIFFRACTION, INDUCED RECONSTRUCTIONS, LEED ANALYSIS, METAL-SURFACES, SCATTERING},
	isbn = {0079-6816},
	url = {<Go to ISI>://A1995TL80800021},
	author = {Liu, W. and Wong, K. C. and Zeng, H. C. and Mitchell, K. A. R.}
}
@article {3201,
	title = {BOND-LENGTH INEQUALITIES AND RELAXATIONS AT THE RH(110)-C(2X2)-S SURFACE-STRUCTURE STUDIED BY LEED CRYSTALLOGRAPHY},
	journal = {Surface Science},
	volume = {304},
	number = {3},
	year = {1994},
	note = {ISI Document Delivery No.: MZ811Times Cited: 8Cited Reference Count: 19},
	month = {Mar},
	pages = {L481-L487},
	type = {Letter},
	abstract = {A tensor LEED analysis has been made for the Rh(110)-c(2 x 2)-S surface structure using intensity-versus-energy curves measured for twelve independent beams at normal incidence. Each S atom chemisorbs on a centre site of the Rh(110) surface. It bonds to the second layer Rh atom directly below, with a bond distance equal to about 2.27 angstrom, and to four neighbouring first layer Rh atoms at close to 2.47 angstrom. A significant feature of this structure is that the second metal layer is buckled; those Rh atoms directly below the S atoms relax down by about 0.11 angstrom compared with the other second layer Rh atoms. This buckling is apparently driven by the need to reduce the difference that would otherwise occur between these two types of S-Rh bond lengths. A component in the observed difference between the S-Rh distances appears to be dependent on the metallic coordination number for the Rh atoms; in this regard, a comparison is made with the structural details for O chemisorbed on reconstructed Ni(110).},
	keywords = {ADSORPTION, ENERGY-ELECTRON-DIFFRACTION, RECONSTRUCTION},
	isbn = {0039-6028},
	url = {<Go to ISI>://A1994MZ81100007},
	author = {Wong, K. C. and Mitchell, K. A. R.}
}
@article {3187,
	title = {TENSER LEED ANALYSIS OF THE PD(100)-(ROOT-5X-ROOT-5)R27-DEGREES-O SURFACE-STRUCTURE},
	journal = {Surface Science},
	volume = {318},
	number = {1-2},
	year = {1994},
	note = {ISI Document Delivery No.: PL286Times Cited: 29Cited Reference Count: 29},
	month = {Oct},
	pages = {129-138},
	type = {Article},
	abstract = {A tenser LEED analysis of the Pd(100)-(root 5 x root 5)R27 degrees-O surface structure supports a surface oxide model, as first postulated by Orent and Bader. The detailed model which gives the best correspondence with experimental intensity data has a PdO(001) overlayer stacked on to the Pd(100) surface such that rumpling is induced in both the oxide and topmost Pd(100) layers. The structure can be seen as representing a compromise between the drive toward an ideally flat PdO(001) surface and the need to optimize total bonding at the surface. Pd atoms in the topmost Pd(100) layer appear to displace laterally to minimize corrugations in the top metal layers. The total corrugations in the PdO overlayer and the first Pd(100) layer are indicated to be about 0.26 and 0.51 Angstrom, respectively. The average O-Pd bond length for two-coordinate O on the Pd surface (1.73 Angstrom) remains dose to the predicted value of 1.76 Angstrom based on the structure of bulk PdO.},
	keywords = {ADSORPTION, desorption, ENERGY-ELECTRON-DIFFRACTION, HYDROGEN, OXYGEN, PD(100) SURFACE, PHASE, RECONSTRUCTION},
	isbn = {0039-6028},
	url = {<Go to ISI>://A1994PL28600019},
	author = {Vu, D. T. and Mitchell, K. A. R. and Warren, O. L. and Thiel, P. A.}
}
@article {3186,
	title = {TENSOR LEED ANALYSIS OF THE CU(110)-(2 X 3)-N SURFACE-STRUCTURE},
	journal = {Physical Review B},
	volume = {49},
	number = {16},
	year = {1994},
	note = {ISI Document Delivery No.: NK063Times Cited: 27Cited Reference Count: 25},
	month = {Apr},
	pages = {11515-11518},
	type = {Note},
	abstract = {A tensor LEED analysis of the Cu(110)-(2 x 3)-N surface structure supports. a reconstruction model in which the topmost layer can be described as a pseudo-(100)-c(2 x 2)-N overlayer, with metal corrugation of about 0.52 angstrom in the reconstructed layer. Each N atom is nearly coplanar with the local plane formed by the four neighboring Cu atoms. Of the four N atoms per unit mesh, three also bond to Cu atoms in the layer below and are therefore five-coordinate. Two of the three five-coordinate sites result from appreciable lateral displacements toward each other of both N atoms and Cu atoms below in the topmost Cu(110) layer. Average N-Cu bond lengths for the five-coordinate sites (1.87 angstrom) agree well with prediction, while the bond lengths for the four-coordinate sites (1.85 angstrom) appear somewhat long. These different N sites are discussed in relation to a recent STM study, and results from this LEED analysis are contrasted with those from the previous LEED study, which supported a [001]-missing row reconstruction of the surface.},
	keywords = {CU(110)(2X3)-N STRUCTURE, ENERGY-ELECTRON-DIFFRACTION, ION-SCATTERING, NITRIDE, NITROGEN, RECONSTRUCTION, SITE, SUBSTRATE},
	isbn = {0163-1829},
	url = {<Go to ISI>://A1994NK06300093},
	author = {Vu, D. T. and Mitchell, K. A. R.}
}
