Abstract:Although the organo hydride derivatives of boron and aluminium are well characterized, little work has been reported on the corresponding galliunl systems. The present s t~~d y was initiated to determine the relative stabilities of organo gallium hydride derivatives as compared to the stabilities of the corresponding compounds of boron and aluminium. Various preparative routes in this new class of gallium con~pounds have been investigated. Theseincludc the usc of organo mercury and organo lithium reagents in r… Show more
“…33,39,40 Most common are the Lewis base adducts of group 13 metal hydrides. 38,41 Thus, GaH 3 ‚NMe 3 is stable below room temperature but its shelf life is considerably lower at room temperature. Therefore, it is a synthetic challenge to prepare stable mono-and dihydrides of gallium.…”
Section: Resultsmentioning
confidence: 99%
“…Attempts have been devoted to increase the stability of these compounds by coordination of an ancillary ligand to the gallium atom. These are among the most easily accessible, more stable, and, usually, more malleable than the parent hydrides. ,, Most common are the Lewis base adducts of group 13 metal hydrides. , Thus, GaH 3 ·NMe 3 is stable below room temperature but its shelf life is considerably lower at room temperature. Therefore, it is a synthetic challenge to prepare stable mono- and dihydrides of gallium.…”
Section: Resultsmentioning
confidence: 99%
“…27 Al NMR (78.2 MHz, C 6 D 6 , TMS): δ 66.9 (s, w 1/2 ) 1350 Hz). MS [EI; m/z (%)]: 482 (100) [M + ], 467 (41) [M + -Me], 447 (18) [M + -MeH -F]. IR (Nujol, cm -1 ): ν ˜1539, 1318, 1255, 1177, 1102, 1030, 937, 900, 817, 803, 758, 719, 448, 412.…”
A series of organometallic compounds of group 13 metals supported by the sterically encumbered beta-diketiminate ligand containing hydrides, fluorides, chlorides, and bromide have been synthesized and structurally characterized. The synthetic strategy applied utilizes halide metathesis and reduction of metal chlorides to the corresponding hydrides. Thus, the reaction of LLi.OEt2 with MeMCl2 affords LM(Me)Cl (M = Al (1), Ga (2), In (3)) and LGaBr2 (4) with GaBr3. Reduction of LGa(Me)Cl with LiH.BEt3 leads to the formation of LGa(Me)H (10). Synthesis of LGaH(2) (12) has been accomplished by reacting LGaI2 (8) with LiH.BEt3. LAl(Me)Cl (1) and LAlH2 (6) have been converted to LAl(Me)F (5) and LAlF2 (7), respectively. The former was obtained in a reaction of LAl(Me)Cl with Me3SnF while the latter was isolated in a reaction of LAlH2 with BF3.OEt2. Similarly reaction of LGaI2 (8) with Me3SnF affords LGaF2 (9). Compounds reported herein have been characterized by elemental analyses, IR, NMR, EI-MS, and single-crystal X-ray diffraction techniques.
“…33,39,40 Most common are the Lewis base adducts of group 13 metal hydrides. 38,41 Thus, GaH 3 ‚NMe 3 is stable below room temperature but its shelf life is considerably lower at room temperature. Therefore, it is a synthetic challenge to prepare stable mono-and dihydrides of gallium.…”
Section: Resultsmentioning
confidence: 99%
“…Attempts have been devoted to increase the stability of these compounds by coordination of an ancillary ligand to the gallium atom. These are among the most easily accessible, more stable, and, usually, more malleable than the parent hydrides. ,, Most common are the Lewis base adducts of group 13 metal hydrides. , Thus, GaH 3 ·NMe 3 is stable below room temperature but its shelf life is considerably lower at room temperature. Therefore, it is a synthetic challenge to prepare stable mono- and dihydrides of gallium.…”
Section: Resultsmentioning
confidence: 99%
“…27 Al NMR (78.2 MHz, C 6 D 6 , TMS): δ 66.9 (s, w 1/2 ) 1350 Hz). MS [EI; m/z (%)]: 482 (100) [M + ], 467 (41) [M + -Me], 447 (18) [M + -MeH -F]. IR (Nujol, cm -1 ): ν ˜1539, 1318, 1255, 1177, 1102, 1030, 937, 900, 817, 803, 758, 719, 448, 412.…”
A series of organometallic compounds of group 13 metals supported by the sterically encumbered beta-diketiminate ligand containing hydrides, fluorides, chlorides, and bromide have been synthesized and structurally characterized. The synthetic strategy applied utilizes halide metathesis and reduction of metal chlorides to the corresponding hydrides. Thus, the reaction of LLi.OEt2 with MeMCl2 affords LM(Me)Cl (M = Al (1), Ga (2), In (3)) and LGaBr2 (4) with GaBr3. Reduction of LGa(Me)Cl with LiH.BEt3 leads to the formation of LGa(Me)H (10). Synthesis of LGaH(2) (12) has been accomplished by reacting LGaI2 (8) with LiH.BEt3. LAl(Me)Cl (1) and LAlH2 (6) have been converted to LAl(Me)F (5) and LAlF2 (7), respectively. The former was obtained in a reaction of LAl(Me)Cl with Me3SnF while the latter was isolated in a reaction of LAlH2 with BF3.OEt2. Similarly reaction of LGaI2 (8) with Me3SnF affords LGaF2 (9). Compounds reported herein have been characterized by elemental analyses, IR, NMR, EI-MS, and single-crystal X-ray diffraction techniques.
“…There have been no reports of free monoalkylgallanes, (RGaH2),, although NMR and IR evidence for adducts such as MeGaH2.NMe3 has been presented. 5 In the past few years, however, a number of novel routes to gallanes have been reported, including the elusive parent Ga2H6. 6 We recently reported the synthesis of diethylgallane, Et2GaH, in the infrared laser powered homogeneous pyrolysis (IR LPHP) of triethylgallane via the (3-elimination reaction,7 eqn.…”
Ethylgallane, characterised by the IR and 1H NMR spectra of its trimethylamine adduct, has been identified as an intermediate in the infrared laser powered pyrolysis of triethylgallane, providing the first unambiguous evidence for the existence of free monoalkylgallanes.
Hydrogen stretching vibrations at GaAs(110) and Inp110) surfaces were investigated by high‐resolution electron energy‐loss spectroscopy (HREELS). With semi‐insulating crystals, the linewidths were reduced such that the fine structure of the energy losses could be analysed. For Ga–H stretching modes, two components at 1830 and 1860 cm−1 (226.9 and 230.6 meV) are found after low exposure to atomic hydrogen. They may be explained by dipole–dipole interactions. Upon heavier hydrogenation at third substructure at 1907 cm−1 (236.5 meV) is observed. At H‐covered Inp110) surfaces, the loss structure due to phosphorus–hydrogen stretching vibrations exhibits a double structure with components at 2260 and 2300 cm−1 (280.2 and 285.2 meV). The first is attributed to P–H monohydride and the second to P–H2 dihydride vibrations. The results indicate that Inp110) surfaces are disrupted even after small H exposures.
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