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        <identifier>oai:figshare.com:article/33981262</identifier>
        <datestamp>2026-09-28T07:47:55Z</datestamp>
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          <dc:title>Isomerization HCN → HNC in the electronic ground state using chirp-optimized mid-IR laser pulses: 4D quantum dynamics</dc:title>
          <dc:creator>Niels Engholm Henriksen (6211961)</dc:creator>
          <dc:creator>Kasper Linger Effersø (11769230)</dc:creator>
          <dc:subject>Theoretical and computational chemistry not elsewhere classified</dc:subject>
          <dc:subject>Radiation and matter</dc:subject>
          <dc:subject>HCN</dc:subject>
          <dc:subject>Isomerization</dc:subject>
          <dc:subject>Quantum Dynamics</dc:subject>
          <dc:subject>Coherent Control</dc:subject>
          <dc:subject>Femtosecond Laser</dc:subject>
          <dc:description>&lt;p dir="ltr"&gt;The laser-induced isomerization of HCN is studied starting from a four-nuclear-degrees-of-freedom (4D) Hamiltonian, which includes the rotation (χ) of H around a fixed CN axis. This Hamiltonian reproduces the known exact quantized rovibrational states, including Coriolis coupling. We study the laser-induced dynamics using linearly chirped mid-IR laser pulses with a temporal duration of ≃ 1 picosecond. The initial state is the vibrational ground state of HCN with J = K = 0, where K is the quantum number associated with vibrational angular momentum and the rotation of H around the CN axis. Over-barrier excitation via fundamental or first overtone bending modes is studied. An optimized pump-dump pulse, which is fully tailored for a fixed χ angle is also employed and leads to considerable isomerization. Multiphoton excitation via the fundamental bending mode creates a rotational wave packet in the χ angle, whereas multiphoton excitation via the overtone bending mode preserves the uniform distribution in χ. The influence of the χ angle on the isomerization yield is discussed in a comparison with a planar 3D model of the isomerization.&lt;/p&gt;</dc:description>
          <dc:date>2026-09-28T07:47:55Z</dc:date>
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          <dc:identifier>10.11583/DTU.33981262.v1</dc:identifier>
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          <dc:rights>CC BY 4.0</dc:rights>
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