Two-dimensional (2+n) resonance enhanced multiphoton ionization of HCl: State interactions and photorupture channels via low-energy triplet Rydberg states
Abstract:Mass spectra were recorded for (2+n) resonance enhanced multiphoton ionization (REMPI) of HCl as a function of resonance excitation energy in the 81,710-82,870 cm(-1) region to obtain two-dimensional REMPI data. Small but significant fragmentations and H(+), Cl(+), as well as HCl(+) formations are found to occur after resonance excitations to the triplet Rydberg states f (3)Delta(2)(v(') = 0), f (3)Delta(1)(v(') = 0), and g (3)Sigma(+)(1)(v(') = 0). Whereas insignificant rotational line shifts could be observe… Show more
“…Both groups investigated the ionization/fragmentation pathways through various vibrational bands of the B 1 Σ + (0 + ) state. Very recently, Kauczok et al [22] have reported similar studies on the singlet and triplet Δ states that previously were identified as being in resonance with selected rovibrational states of the B 1 Σ + (0 + ) state [16][17][18].…”
Section: Introductionmentioning
confidence: 74%
“…The fragmentation ratio (Cl + /HCl + ) does not only show a smooth dependence on the excitation energy, but also crucially depends on the nature of the electronic states as well as on vibrational and rotational quantum numbers [16,18,20]. However, independently of the excitation energy, there exist bands which do not exhibit any significant fragmentation at all.…”
Section: To the Electronic Transitions B[v/e](mentioning
confidence: 99%
“…It is important to note that the energy of the asymptotic products H + + Cl − lies above the energy of the H + Cl * (4s) system (red solid curve), but below the energy of the H * (n = 2) + Cl system (blue solid curve). It goes without saying that among the omitted bound (red) Rydberg states are several that are characterized by an orbital angular momentum Λ > 0, in particular the F 1 Δ and f 3 Δ states that were shown by Kvaran and coworkers for individual rovibrational levels to be in resonance with rovibrational levels of the B 1 Σ + state [16,18]. F 1 Δ and f 3 Δ states are energetically very close to E 1 Σ + , thus fine-tuning the excitation energy in this narrow energy range allows the experimentalist to access states with differing electronic.…”
Section: Potential Energy Curves: a Simplified View Of The Essentialsmentioning
confidence: 99%
“…The colour coding matches that of Figure 3. Recently, Kvaran and coworkers have detailedly studied Rydberg states of HCl with either Λ > 0 or S > 0 (i.e., belonging to the triplet manifold) or both, some of which exhibit near resonances with rovibrational levels of the B 1 Σ + state [16][17][18] Kauczok et al have recently studied the kinetic energy and the angular distributions of these fragments in order to identify those channels which become available to the HCl molecule in the near resonance situation [22]. They have found that those near-resonance rotational levels in the f 3 Δ and F 1 Δ states behave identically to the B 1 Σ + state levels.…”
Section: Ionization and Fragmentation Through Other Electronic Statesmentioning
confidence: 99%
“…In continuation of their work, Kvaran and coworkers [16][17][18] have investigated several of those states with a predissociation signature by a mass sensitive REMPI timeof-flight technique. Branching ratios for parent molecule ionization and fragmentation producing either H + or Cl + have been studied for both H 35 Cl and H 37 Cl isotopologues on a quantum state selective basis.…”
The competition between multiphoton ionization and fragmentation in the diatomic molecule hydrogen chloride is reviewed. Emphasis is laid on recent experimental results employing chemical imaging methods in order to obtain kinetic energy distributions and angular distributions of photoproducts. The energy range considered is 15 to 20 eV, equivalent to the absorption of three or four photons in the ultraviolet wavelength range. The role of Rydberg states as resonantly excited intermediate states in the ionization/fragmentation processes is assessed. Mixing among 1 Σ + states gives rise to peculiarly shaped double minimum potential energy curves which allow for the production of hydrogen and chlorine atomic and ionic fragments via several competing pathways, in addition to the production of molecular HCl + ions. States with different electronic properties show a qualitatively different behaviour from Σ + states. Accidental resonances between states of differing orbital angular momentum or multiplicity serve to override these differences and cause subtle as well as significant deviations from the unperturbed behaviour.
“…Both groups investigated the ionization/fragmentation pathways through various vibrational bands of the B 1 Σ + (0 + ) state. Very recently, Kauczok et al [22] have reported similar studies on the singlet and triplet Δ states that previously were identified as being in resonance with selected rovibrational states of the B 1 Σ + (0 + ) state [16][17][18].…”
Section: Introductionmentioning
confidence: 74%
“…The fragmentation ratio (Cl + /HCl + ) does not only show a smooth dependence on the excitation energy, but also crucially depends on the nature of the electronic states as well as on vibrational and rotational quantum numbers [16,18,20]. However, independently of the excitation energy, there exist bands which do not exhibit any significant fragmentation at all.…”
Section: To the Electronic Transitions B[v/e](mentioning
confidence: 99%
“…It is important to note that the energy of the asymptotic products H + + Cl − lies above the energy of the H + Cl * (4s) system (red solid curve), but below the energy of the H * (n = 2) + Cl system (blue solid curve). It goes without saying that among the omitted bound (red) Rydberg states are several that are characterized by an orbital angular momentum Λ > 0, in particular the F 1 Δ and f 3 Δ states that were shown by Kvaran and coworkers for individual rovibrational levels to be in resonance with rovibrational levels of the B 1 Σ + state [16,18]. F 1 Δ and f 3 Δ states are energetically very close to E 1 Σ + , thus fine-tuning the excitation energy in this narrow energy range allows the experimentalist to access states with differing electronic.…”
Section: Potential Energy Curves: a Simplified View Of The Essentialsmentioning
confidence: 99%
“…The colour coding matches that of Figure 3. Recently, Kvaran and coworkers have detailedly studied Rydberg states of HCl with either Λ > 0 or S > 0 (i.e., belonging to the triplet manifold) or both, some of which exhibit near resonances with rovibrational levels of the B 1 Σ + state [16][17][18] Kauczok et al have recently studied the kinetic energy and the angular distributions of these fragments in order to identify those channels which become available to the HCl molecule in the near resonance situation [22]. They have found that those near-resonance rotational levels in the f 3 Δ and F 1 Δ states behave identically to the B 1 Σ + state levels.…”
Section: Ionization and Fragmentation Through Other Electronic Statesmentioning
confidence: 99%
“…In continuation of their work, Kvaran and coworkers [16][17][18] have investigated several of those states with a predissociation signature by a mass sensitive REMPI timeof-flight technique. Branching ratios for parent molecule ionization and fragmentation producing either H + or Cl + have been studied for both H 35 Cl and H 37 Cl isotopologues on a quantum state selective basis.…”
The competition between multiphoton ionization and fragmentation in the diatomic molecule hydrogen chloride is reviewed. Emphasis is laid on recent experimental results employing chemical imaging methods in order to obtain kinetic energy distributions and angular distributions of photoproducts. The energy range considered is 15 to 20 eV, equivalent to the absorption of three or four photons in the ultraviolet wavelength range. The role of Rydberg states as resonantly excited intermediate states in the ionization/fragmentation processes is assessed. Mixing among 1 Σ + states gives rise to peculiarly shaped double minimum potential energy curves which allow for the production of hydrogen and chlorine atomic and ionic fragments via several competing pathways, in addition to the production of molecular HCl + ions. States with different electronic properties show a qualitatively different behaviour from Σ + states. Accidental resonances between states of differing orbital angular momentum or multiplicity serve to override these differences and cause subtle as well as significant deviations from the unperturbed behaviour.
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