Evidence for the Existence of Unsaturated Organoaluminum

several solitary organoaluminum molecules in the gas phase. It is demonstrated that neutralization of the structurally characterized ions AICH2+, AICH...
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J . Am. Chem. Soc. 1990, 112, 8334-8337

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Evidence for the Existence of Unsaturated Organoaluminum Molecules in the Gas Phase: A1CH2, A1(CH3)x(x = 1, 2), and AlC2H4 Ragampeta Srinivas, Detlev Sulzle, and Helmut Schwarz* Contribution from the Institut fur Organische Chemie der Technischen Universitat Berlin, Strasse des 17, Juni 135, D- IO00 Berlin 12, West Germany. Received April I6, I990

Abstract: Neutralization-reionization mass spectrometry (NRMS) has been successfully applied to generate for the first time several solitary organoaluminum molecules in the gas phase. It is demonstrated that neutralization of the structurally characterized ions AICH2+, AICH;', AI(CH3)2+,and AIC2H4+gives rise to recovery signals. Two further points emerge from this study: (i) Isomeri7ation of AlCH2 and AlCH3 (both in their ionic and neutral forms) to the isomeric hydridoaluminum species HAICH, (x = 1,2) is negligible, if operative at all. (ii) For the AIC2H4+system, in addition to the isomer corresponding to a ?r-complex, a second isomer is observed, which, according to its collisional activation mass spectrum, is best described as the hitherto unknown HCAICH,' ion. Neutralization of this species, in contrast to AIC2H4+,does however not result in the formation of a detectable HCAICH3 molecule. Similarly, while HAIC2H5+is found to exist as a species distinct from AI(CH3),+, neutralization of the former failed while the latter provides a recovery signal.

Coordinatively unsaturated metal fragments are suggested to play a pivotal role as intermediates in homogeneous and/or heterogeneous catalysis or in organometallic chemistry in general.' Unfortunately, direct evidence for the existence of these species as stable monomeric entities in the condensed phase is often, but not always,Ic scarce due to facile inrermolecular reactions. In addition, as recently discussed at great length by Hange, Margrave, and KafafL2 the unambiguous stoichiometric characterization of organometallic species in a matrix can be quite difficult not to mention the effects of the matrix cage which may obscure the intrinsic properties of the solitary molecules in question. Recently, a method of producing isolated neutrals in the dilute gas phase from the cations by first neutralizing a beam of ions foilowed by reionization (NRMS)) has provided direct evidence for the existence of many formerly unobtainable neutral molecules. In this respect it was particularly encouraging that, by using NRMS, several otherwise elusive organometallic molecules were generated and characterized as genuine, chemically bound molecules with lifetimes > 1 ps. Typical examples include the following species: FeCH, ( x = 0-3): NIL, complexes ( n = 1, 2; L = CO, D20, ND3),5 "end-on" Cd0) complexes of HCN and HNC: the half-sandwiches MC5HS (M = Fe, Co, Ni),' and the longsought-after metal acetylides MCCH (M = Fe, Co, Ni).* In this paper we describe NRMS experiments aimed at generating and characterizing the following aluminum hydrocarbon complexes, e.g. AICH,, AICH,, AI(CH3),, and AIC2H4. While ( I ) Selected reviews and biographies: (a) Hartley, F. R., Patai, S., Eds. The Chemistry of the Metal-Carbon Bond; Wiley: Chichester, 1982. (b) Crabtree. R. H. Chem. Rev. 1985, 85, 245. (c) Collmann, J. P.; Hegedus, L. S.; Norton, J. R.; Finke, K. G. Principles and Applications of Organotransition Metal Chemistry; University Science Book: Mill Valley, CA. 1987. (d) Russell, D. H.. Ed. Gas Phase Inorganic Chemistry; Plenum: New York, 1989. (e) Andrews, L.; Moskovits, M., Eds. Chemistry and Physics of Matrix-Isolated Species; Elsevier: Amsterdam, 1989. (2) Hange, R. H.; Margrave, J. L.; Kafafi, 2.H.: in ref le, Chapter IO. (3) Reviews: (a) Terlouw, J. K.;Burgers, P. C.; v. Baar, B. L. M.; Weiske, T.;Schwarz, H.Chimia 1986,40,357. (b) Wdemiotis. C.; McLafferty, F. W. Chem. Reu. 1987.87,485. (c) Terlouw, J. K.; Schwarz, H. Angew. Chem., Int. Ed. Engl. 1987. 26, 805. (d) Schwarz, H. Pure Appl. Chem. 1989, 61, 685. (e) Holmes, J . L. Adu. Mass Specrrom. 1989, 1 1 , 5 3 . ( f ) Terlouw, J. K. Ibid. 1989, 11,984. (g) Holmes, J. L. Mass. Spectrom. Rev. 1989.8, 513. (h) McLafferty, F. W. Science 1990, 247. 925. (4) Lebrilla, C. E.; Drewello, T.; Schwarz, H. Organometallics 1987, 6, 2268. (5) Hudgins, D. M.; Porter, R.

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( 6 ) Eller, K.; Sulzle, D.; Schwarz, H.Chem. Phys. Lett. 1989, 154, 443. (7) Drewello, T.: Schwarz, H.Int. J. Mass Spectrom. Ion Processes 1989, 93, 177. (8) Drewello, T.; Schwarz, H. Chem. Phys. Lett. 1990, 171, 5 .

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AICH, and AICH, are theoretically well characterized by Schaefer's nonempirical quantum mechanical calculations as stable species with dissociation energies of 77 (AICH,) and 68 kcal/mol (AICH,)? no experimental studies seem to exist in the literature which would lend direct support to this prediction.1° We shall demonstrate that (i) either species is indeed viable in the gas phase and (ii) isomerization to an aluminum hydride fragment AICH, HAICH,, does not take place. Evidence is also presented that AI(CH3), is a stable molecule; the tendency of this fragment to isomerize is quite minor, if prevailing at all. For aluminum complexes of the general composition (AI,C2,H4) there already exists a rich literature commencing with the seminal paper of Kasai and McLeod," in which for the first time an aluminum atomethylene adduct generated in a neon matrix was characterized by ESR. Later ESR work, conducted in different matrices a t varying temperature^,'^-'^ as well as an IR study of the AIC2H4 molecule in solid argonis clearly pointed to the formation of a symmetrical *-complex of the aluminum atom with the CC double bond, rendering both CH, groups of C2H4 equivalent. Recent laser studies15 provided binding energies of the aluminum atom to olefins, and for A1C2H4 a lower value of 16 kcal/mol was reported. Until recently" theory had not been successful in interpreting the experimental observations for AIC2H4, in particular the binding energy. In earlier calculations, using a rigid C2H4 geometry, the attraction of atomic AI to C2H4 was calculated to be