1996
DOI: 10.1116/1.588797
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Layer-by-layer removal of GaAs(110) by bromine

Abstract: Dissociative electron attachment of CH3Br on GaAs(110) by thermalized photoexcited substrate electrons

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Cited by 7 publications
(6 citation statements)
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“…In addition, the energetics for dissociation is less favorable for TiO 2 (110) compared to the metal and GaAs surfaces due to a much weaker halide-surface interaction. On metallic surfaces, halogen atoms are chemisorbed so strongly that they desorb as metal halides (Cl and Br) or atomically (I) at very high temperatures (>800 K). ,, On the GaAs surface, halogen atoms (Cl and Br) form halide compounds with the surface gallium atoms and desorb as gallium halides at a temperature of ∼600 K (surface etching). , By comparison, the iodine atoms on TiO 2 (110) are bound very weakly and desorb as I 2 at ∼200 K. Thus, after electron attachment to CH 3 I, the driving force for a transiently anionic CH 3 I species to dissociate the C−I bond will be much smaller on TiO 2 (110) than on metal or GaAs surfaces.…”
Section: Discussionmentioning
confidence: 99%
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“…In addition, the energetics for dissociation is less favorable for TiO 2 (110) compared to the metal and GaAs surfaces due to a much weaker halide-surface interaction. On metallic surfaces, halogen atoms are chemisorbed so strongly that they desorb as metal halides (Cl and Br) or atomically (I) at very high temperatures (>800 K). ,, On the GaAs surface, halogen atoms (Cl and Br) form halide compounds with the surface gallium atoms and desorb as gallium halides at a temperature of ∼600 K (surface etching). , By comparison, the iodine atoms on TiO 2 (110) are bound very weakly and desorb as I 2 at ∼200 K. Thus, after electron attachment to CH 3 I, the driving force for a transiently anionic CH 3 I species to dissociate the C−I bond will be much smaller on TiO 2 (110) than on metal or GaAs surfaces.…”
Section: Discussionmentioning
confidence: 99%
“…21,42,48 On the GaAs surface, halogen atoms (Cl and Br) form halide compounds with the surface gallium atoms and desorb as gallium halides at a temperature of ∼600 K (surface etching). 49,57 By comparison, the iodine atoms on TiO 2 (110) are bound very weakly and desorb as I 2 at ∼200 K. Thus, after electron attachment to CH 3 I, the driving force for a transiently anionic CH 3 I species to dissociate the C-I bond will be much smaller on TiO 2 -(110) than on metal or GaAs surfaces.…”
Section: Discussionmentioning
confidence: 99%
“…In all cases, the impingement rate from our electrochemical cell, with a cell current of 5 A and a geometric factor of 7.5%, is about 2.6ϫ10 Ϫ3 Br atoms per substrate atom per second. 3 As a result, the removal mode is layer-by-layer. 1͑a͒ while the relatively low loss appears as pits (ϳ10 11 pits/cm 2 ).…”
Section: B Etching Pathways and Yieldmentioning
confidence: 99%
“…1 Atomic-level etching studies using scanning tunneling microscopy ͑STM͒ have shown that thermal etching with continuous halogen exposure can result in a variety of different morphologies. 3 In particular, if a surface exposed to Br 2 at 300 K is annealed at 700 K, the morphology is characterized by single-layer-deep etch pits, with the second layer remaining intact. 2 For the fabrication of quantum devices with strictly controlled layer thicknesses, it is essential that material be removed in a layer-bylayer fashion.…”
Section: Introductionmentioning
confidence: 99%
“…Bromine (Br 2 ) is a strong oxidant used in organic synthesis, pollutant degradation and semiconductor etching, which is poisonous and dangerous for storage and transport. [12][13][14][15][16] The aim of this work is to provide a green method for the generation of Br 2 in situ. The first photoelectrochemical reaction system (Fig.…”
mentioning
confidence: 99%