Abstract:We report on the low-energy electron-induced production of aldehydes within thin solid films of tetrahydrofuran (THF) condensed on a solid Kr substrate. The aldehyde fragments, which remain trapped within the bulk of the THF film, are detected in situ via their 3,1(n-->pi*) and 3(pi-->pi*) electronic transitions and vibrational excitations in the ground state using high-resolution electron-energy-loss spectroscopy. The production of aldehyde is studied as a function of the electron exposure, film thickness, an… Show more
“…Antic et al 3 reported a resonance at 23 eV which decayed into a highly excited state undergoing a further dipolar dissociation. The formation of aldehydes from THF frozen on a Kr substrate was studied in detail by Breton et al 4 and Ja¨ggle et al 5 by means of vibrational and electronic EELS of the products. A strong rise of aldehyde production was observed from about 6 eV upward and was correlated to (n,s * CO ) electronic excitation threshold of THF, together with core-excited resonances around 9 and 10 eV.…”
Section: Introductionmentioning
confidence: 99%
“…We presume that the C-O bond does break in THF, but the resulting CH 2 (CH 2 ) 3 O À ion is metastable in respect to autodetachment, which would in this case require that the ring is re-closed. The initial CH 2 (CH 2 ) 3 O À ion could be stabilized in the condensed phase, however, and give rise to the weak process reported around 3 eV by Breton et al 4 …”
Dissociative electron attachment (DEA) to diethyl ether yielded primarily the C 2 H 5 O À ion, with a strong Feshbach resonance band at 9.1 eV and a weaker shape resonance band at 3.89 eV. Very similar spectra were obtained for dibutyl ether, with C 4 H 9 O À bands at 8.0 and 3.6 eV. Some of these primary ions subsequently lost H 2 and yielded weaker signals of the C 2 H 3 O À and C 4 H 7 O À ions. In contrast, DEA to the cyclic ether tetrahydrofuran (THF) yielded mainly a fragment of mass 41, presumably deprotonated ketene, at 7.65 eV. The low-energy band was missing in THF. H À with two bands at 6.88 and 8.61 eV, and an ion of mass 43 (presumably deprotonated acetaldehyde) with two bands at 6.7 and 8.50 eV were also observed. We propose that in the primary DEA step the C-O bond is cleaved in both the open-chain and the cyclic ethers. In the open-chain ethers the excess energy is partitioned between the (internal and kinetic) energies of two fragments, resulting in an RO À ion cool enough to be observed. The CH 2 (CH 2 ) 3 O À ion resulting from cleavage of the C-O bond in THF contains the entire excess energy (more than 6 eV at an electron energy of 7.65 eV) and is too short-lived with respect to further dissociation and thermal autodetachment to be detected in a mass spectrometer. These findings imply that there could be a substantial difference between the fragmentation in the gas phase described here and fragmentation in the condensed phase where the initially formed fragments can be rapidly cooled by the environment.
“…Antic et al 3 reported a resonance at 23 eV which decayed into a highly excited state undergoing a further dipolar dissociation. The formation of aldehydes from THF frozen on a Kr substrate was studied in detail by Breton et al 4 and Ja¨ggle et al 5 by means of vibrational and electronic EELS of the products. A strong rise of aldehyde production was observed from about 6 eV upward and was correlated to (n,s * CO ) electronic excitation threshold of THF, together with core-excited resonances around 9 and 10 eV.…”
Section: Introductionmentioning
confidence: 99%
“…We presume that the C-O bond does break in THF, but the resulting CH 2 (CH 2 ) 3 O À ion is metastable in respect to autodetachment, which would in this case require that the ring is re-closed. The initial CH 2 (CH 2 ) 3 O À ion could be stabilized in the condensed phase, however, and give rise to the weak process reported around 3 eV by Breton et al 4 …”
Dissociative electron attachment (DEA) to diethyl ether yielded primarily the C 2 H 5 O À ion, with a strong Feshbach resonance band at 9.1 eV and a weaker shape resonance band at 3.89 eV. Very similar spectra were obtained for dibutyl ether, with C 4 H 9 O À bands at 8.0 and 3.6 eV. Some of these primary ions subsequently lost H 2 and yielded weaker signals of the C 2 H 3 O À and C 4 H 7 O À ions. In contrast, DEA to the cyclic ether tetrahydrofuran (THF) yielded mainly a fragment of mass 41, presumably deprotonated ketene, at 7.65 eV. The low-energy band was missing in THF. H À with two bands at 6.88 and 8.61 eV, and an ion of mass 43 (presumably deprotonated acetaldehyde) with two bands at 6.7 and 8.50 eV were also observed. We propose that in the primary DEA step the C-O bond is cleaved in both the open-chain and the cyclic ethers. In the open-chain ethers the excess energy is partitioned between the (internal and kinetic) energies of two fragments, resulting in an RO À ion cool enough to be observed. The CH 2 (CH 2 ) 3 O À ion resulting from cleavage of the C-O bond in THF contains the entire excess energy (more than 6 eV at an electron energy of 7.65 eV) and is too short-lived with respect to further dissociation and thermal autodetachment to be detected in a mass spectrometer. These findings imply that there could be a substantial difference between the fragmentation in the gas phase described here and fragmentation in the condensed phase where the initially formed fragments can be rapidly cooled by the environment.
“…Antic et al [5] reported a resonance at 23 eV which decays into a highly excited state undergoing a further dipolar dissociation. The formation of aldehydes from THF frozen on a Kr substrate was studied in detail by Breton et al [6] and Jäggle et al [7] by means of vibrational and electronic EELS of the products. Strong rise of aldehyde production was observed from about 6 eV and correlated to (n, σ * CO ) electronic excitation threshold of THF, together with core-excited resonances around 9 and 10 eV.…”
Absolute angle-differential elastic and vibrational excitation cross sections for electron collisions with tetrahydrofuran were measured in the energy range 0.1-20 eV, extending existing measurements to lower energies. The elastic cross sections were measured as a function of scattering angle from 10• to 180• at energies of 2 eV, 6 eV, 10 eV and 20 eV, and as a function of electron energy at 45• , 90• , 135• and 180• . The agreement with previous measurements and with the published theoretical work was generally satisfactory. The RamsauerTownsend minimum was observed at low energies, down to 0.24 eV at 180• . Three additional minima were observed at 1.13, 4.74 and 15.3 eV in the 180• elastic cross section. Vibrational excitation cross sections are reported as a function of electron energy from the threshold to 16 eV. They reveal threshold peaks and broad bands at 6.2 and 10.8 eV, attributed to shape resonances, in agreement with theoretical predictions, although the calculated energies are generally somewhat higher. A broad enhancement of the CH 2 scissoring vibration is observed around 2.6 eV, implying a low-lying (shape) resonance similar to that observed earlier in cyclopropane.
“…Condensedphase experiments on thymidine and a single-strand oligonucleotide have demonstrated that slow electrons do indeed break the C-O phosphate-sugar bonds as well as the C-N base-sugar bonds, [60][61][62] and C-O bond breaking was also found in gas-phase DA to a model phosphodiester. 63 A few electron-collision studies, experimental and theoretical, have looked at the individual backbone constituents, i.e., ribose or deoxyribose and a phosphate group, [64][65][66][67][68][69] and others have also been made of electron collisions with backbone analogs such as tetrahydrofuran, 29,65,[68][69][70][71][72][73][74][75][76][77][78][79] tetrahydrofurfuryl alcohol, 71,72,80,81 fructose, 79 and dibutyl phosphate. 63 However, the only electron collision measurements involving nucleosides that we are aware of are the study by Zheng et al of thymine desorption from condensed-phase deoxythymidine 60 mentioned earlier, and the gas-phase studies by Abdoul-Carime et al 82 and by Denifl et al 83 of DA to deoxythymidine and 5-bromouridine, respectively.…”
The authors report results from computational studies of the interaction of low-energy electrons with the purine bases of DNA, adenine and guanine, as well as with the associated nucleosides, deoxyadenosine and deoxyguanosine, and the nucleotide deoxyadenosine monophosphate. Their calculations focus on the characterization of the * shape resonances associated with the bases and also provide general information on the scattering of slow electrons by these targets. Results are obtained for adenine and guanine both with and without inclusion of polarization effects, and the resonance energy shifts observed due to polarization are used to predict * resonance energies in associated nucleosides and nucleotides, for which static-exchange calculations were carried out. They observe slight shifts between the resonance energies in the isolated bases and those in the nucleosides.
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