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The breaking of chemical bonds in surface reactions is inherently connected to highly excited molecular vibrations. Therefore, understanding the vibrational energy transfer dynamics of adsorbed molecules, which effectively determine the lifetime of vibrational excitation, is of great importance. CO adsorbed on NaCl(100) is possibly the best studied physisorbed molecule. Despite that, most previous experiments have focused on the vibrational ground state and the š£ = 0 ā 1 transition of CO-mainly because dispersed fluorescence from high vibrational states could not be observed with conventional infrared detectors. In this thesis, I thus investigate the vibrational energy transfer dynamics of CO on NaCl(100) in highly vibrationally excited states up to š£ = 30.Dispersed and time-resolved laser-induced fluorescence (LIF) is used to observe the vibrational dynamics. For this, an improved version of a recently developed mid-infrared emission spectrometer based on superconducting nanowire single-photon detectors (SNSPDs) is used. The current setup is capable of detecting infrared fluorescence from a single adsorbate layer with spectral and temporal resolution of 7 nm and ā¼1 Āµs, respectively. High vibrational states, CO(š£), are prepared by pulsed infrared laser excitation of CO to š£ = 1 at cryogenic temperatures around 7 K. Subsequent vibrational energy pooling (VEP), driven by the anharmonicity of the CO oscillators, concentrates many vibrational quanta in single molecules via vibration-to-vibration (V-V) energy transfer from the surrounding molecules: CO(n) + CO(m) ā CO(n+1) + CO(m -1).Kinetic Monte Carlo simulations of the vibrational dynamics in a 13 C 18 O monolayer show that VEP proceeds via a sequential mechanism, in which adsorbates in high vibrational states are further excited by collecting vibrational quanta from molecules in lower vibrational states over increasingly large distances and timescales, up to 100 Āµs. The shape of the phonon spectrum, to which the excess energy in the V-V transfer processes is dissipated, causes a distinct peak structure in the vibrational state distribution. Furthermore, dissipation to transverse phonons that involve Na atom motion in the surface plane is found to be most effective. Vibrational relaxation to the NaCl substrate is slower than VEP and occurs on the millisecond time scale for š£ ā¤ 23. The š£-dependent relaxation rates can be explained by a classical electrodynamic mechanism, whereby energy is transferred non-radiatively to the absorbing NaCl medium via the near-field of the oscillating CO dipole. This finding is in strong contrast to the dominating mechanism for more strongly bound adsorbates, where energy is dissipated via anharmonic couplings between the CO vibration and the surface phonons.The improved resolution of the emission spectrometer revealed a previously unknown metastable O-down orientation (Na + -OC), which is formed from the stable C-down v First and foremost, I would like to express my deepest gratitude to my supervisor Alec Wodtke for getting the chance...
The breaking of chemical bonds in surface reactions is inherently connected to highly excited molecular vibrations. Therefore, understanding the vibrational energy transfer dynamics of adsorbed molecules, which effectively determine the lifetime of vibrational excitation, is of great importance. CO adsorbed on NaCl(100) is possibly the best studied physisorbed molecule. Despite that, most previous experiments have focused on the vibrational ground state and the š£ = 0 ā 1 transition of CO-mainly because dispersed fluorescence from high vibrational states could not be observed with conventional infrared detectors. In this thesis, I thus investigate the vibrational energy transfer dynamics of CO on NaCl(100) in highly vibrationally excited states up to š£ = 30.Dispersed and time-resolved laser-induced fluorescence (LIF) is used to observe the vibrational dynamics. For this, an improved version of a recently developed mid-infrared emission spectrometer based on superconducting nanowire single-photon detectors (SNSPDs) is used. The current setup is capable of detecting infrared fluorescence from a single adsorbate layer with spectral and temporal resolution of 7 nm and ā¼1 Āµs, respectively. High vibrational states, CO(š£), are prepared by pulsed infrared laser excitation of CO to š£ = 1 at cryogenic temperatures around 7 K. Subsequent vibrational energy pooling (VEP), driven by the anharmonicity of the CO oscillators, concentrates many vibrational quanta in single molecules via vibration-to-vibration (V-V) energy transfer from the surrounding molecules: CO(n) + CO(m) ā CO(n+1) + CO(m -1).Kinetic Monte Carlo simulations of the vibrational dynamics in a 13 C 18 O monolayer show that VEP proceeds via a sequential mechanism, in which adsorbates in high vibrational states are further excited by collecting vibrational quanta from molecules in lower vibrational states over increasingly large distances and timescales, up to 100 Āµs. The shape of the phonon spectrum, to which the excess energy in the V-V transfer processes is dissipated, causes a distinct peak structure in the vibrational state distribution. Furthermore, dissipation to transverse phonons that involve Na atom motion in the surface plane is found to be most effective. Vibrational relaxation to the NaCl substrate is slower than VEP and occurs on the millisecond time scale for š£ ā¤ 23. The š£-dependent relaxation rates can be explained by a classical electrodynamic mechanism, whereby energy is transferred non-radiatively to the absorbing NaCl medium via the near-field of the oscillating CO dipole. This finding is in strong contrast to the dominating mechanism for more strongly bound adsorbates, where energy is dissipated via anharmonic couplings between the CO vibration and the surface phonons.The improved resolution of the emission spectrometer revealed a previously unknown metastable O-down orientation (Na + -OC), which is formed from the stable C-down v First and foremost, I would like to express my deepest gratitude to my supervisor Alec Wodtke for getting the chance...
When a chemical reaction occurs via tunnelling, a simple massādependence is expected, where substitution of atoms by heavier isotopes leads to a reduced reaction rate. However, as shown in a recent study of CO orientational isomerization at the NaCl(1āÆ0āÆ0) interface, the lightest isotopologues need not exhibit the fastest tunnelling; for the CO/NaCl system, the nonāmonotonic massādependence is understood through a new picture of condensed phase tunnelling where the overall rate is dominated by a few pairs of reactant/product states. These stateāpairs ā termed quantum gateways ā gain dynamical importance through accidentally enhanced tunnelling probabilities, facilitated by a confluence of the energetic landscape underlying the reaction as well as the phonon bath of the surrounding medium. Here, we explore gateway tunnelling through measurements of the kinetic isotope effect for CO isomerization in a monolayer buried by many layers of either CO or N2. With an N2 overlayer, tunnelling rates are accelerated for all four isotopologues (12C16O, 13C16O, 12C18O and 13C18O), but the degree of acceleration is isotopologueāspecific and nonāintuitively mass dependent. A oneādimensional tunnelling model involving an Eckart barrier cannot capture this behaviour. This reflects how a modification of the potential energy surface moves states in and out of resonance, thereby changing which tunnelling gateways can be accessed in the isomerization reaction. Key points The paper describes new systems that showcase resonanceāenhanced condensed phase tunnelling. Condensed phase tunnelling as described in this work may have implications for astrochemistry. A previously hypothesized mechanism is subjected to subsequent experimental scrutiny ā the hypothesis stands the test.
Fourier transform infrared spectroscopy of laser-irradiated cryogenic crystals shows that vibrational excitation of CO leads to the production of equal amounts of CO 2 and C 3 O 2 . The reaction mechanism is explored using electronic structure calculations, demonstrating that the lowest-energy pathway involves a spin-forbidden reaction of (CO) 2 yielding C( 3 P) + CO 2 . C( 3 P) then undergoes barrierless recombination with two other CO molecules forming C 3 O 2 . Calculated intersystem crossing rates support the spin-forbidden mechanism, showing subpicosecond spin-flipping time scales for a (CO) 2 geometry that is energetically consistent with states accessed through vibrational energy pooling. This spin-flip occurs with an estimated ā¼4% efficiency; on the singlet surface, (CO) 2 reconverts back to CO monomers, releasing heat which induces CO desorption. The discovery that vibrational excitation of condensed-phase CO leads to spin-forbidden CāC bond formation may be important to the development of accurate models of interstellar chemistry.
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