2011
DOI: 10.1021/jp2000927
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Vacuum Ultraviolet Negative Photoion Spectroscopy of Chloroform

Abstract: Negative ions Cl(-), Cl(2)(-), CCl(-), CHCl(-), and CCl(2)(-) are observed in vacuum-ultraviolet ion-pair photodissociations of chloroform (CCl(3)H) using the Hefei synchrotron radiation facility, and their ion production efficiency curves are recorded in the photon energy range of 10.00-21.50 eV. Two similar spectra of the isotope anions (35)Cl(-) and (37)Cl(-) indicate the following: Besides the strong bands corresponding to the electron transitions from valence to Rydberg orbitals converging to the ionic st… Show more

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Cited by 6 publications
(4 citation statements)
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“…If these valence-to-Rydberg state transitions couple with the ion-pair dissociation paths, the resonant peaks can be observed in the IPAES. , However, as shown in Figure , such resonant coupling may be quite weak at the higher photon energies. On the other hand, the multibody fragmentations formulated in eq may be predominant in the higher energy range. , According to the thermodynamic values in Table and using eq , the thresholds of Cl – can be deduced as: 2 - normalC 4 normalH 3 SCl + h normalν 2 - normalC 4 normalH 3 normalS + + Cl false( theoretical : 9.50 nobreak.25em eV ; experimental : 8.19 nobreak.25em eV ± 0.04 nobreak.25em eV false) 3 - normalC 4 normalH 3 SCl + h normalν 3 - normalC 4 normalH 3 normalS + + Cl false( theoretical : 9.14 nobreak.25em eV ; experimental : 8.19 nobreak.25em eV ± 0.04 nobreak.25em eV false) These two thresholds cannot be directly determined in the present IPAES because of the much low Cl – signals at the lower photon energies. Above large deviations between the theoretical thresholds and the experimental values may also be due to the ring-opening mechanism of C 4 H 3 S + as mentioned before.…”
Section: Resultsmentioning
confidence: 99%
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“…If these valence-to-Rydberg state transitions couple with the ion-pair dissociation paths, the resonant peaks can be observed in the IPAES. , However, as shown in Figure , such resonant coupling may be quite weak at the higher photon energies. On the other hand, the multibody fragmentations formulated in eq may be predominant in the higher energy range. , According to the thermodynamic values in Table and using eq , the thresholds of Cl – can be deduced as: 2 - normalC 4 normalH 3 SCl + h normalν 2 - normalC 4 normalH 3 normalS + + Cl false( theoretical : 9.50 nobreak.25em eV ; experimental : 8.19 nobreak.25em eV ± 0.04 nobreak.25em eV false) 3 - normalC 4 normalH 3 SCl + h normalν 3 - normalC 4 normalH 3 normalS + + Cl false( theoretical : 9.14 nobreak.25em eV ; experimental : 8.19 nobreak.25em eV ± 0.04 nobreak.25em eV false) These two thresholds cannot be directly determined in the present IPAES because of the much low Cl – signals at the lower photon energies. Above large deviations between the theoretical thresholds and the experimental values may also be due to the ring-opening mechanism of C 4 H 3 S + as mentioned before.…”
Section: Resultsmentioning
confidence: 99%
“…The production efficiency spectra of the positive and negative photoions were measured at the atomic and molecular physics end-station of the National Synchrotron Radiation Facility at Hefei, China. The apparatus used in the present ion-pair photodissociation study was described previously in detail. Briefly, the VUV photon beam was monochromatized with the undulator-based spherical-gratings (made by Horiba Jobin Yvon) then focused onto the reaction region. In detection of the positive photoions, a supersonic molecular beam (buffered with Ar gas) installed perpendicularly to the plane containing the VUV photon beam and the time-of-flight (TOF) tube was used.…”
Section: Experimental Techniques and Theoretical Calculationsmentioning
confidence: 99%
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