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We estimate the resonant dynamic Stark effect, equivalent to the Autler-Townes or Rabi splitting (see, e.g., Ref.) as e0 rab E0 with the transition dipole moment e0 rab from the measured oscillator strength f=0.015 for "feature a" of Ref. at 3.05 eV and the electric field strength E0 / (V/m) =2745 I0 / (W/ cm2) at our present intensities I0 =3.4× 1013 W/ cm2 to be ≃100 meV -which is larger than most of the vibrational level splittings in C60.
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We estimate the resonant dynamic Stark effect, equivalent to the Autler-Townes or Rabi splitting (see, e.g., Ref.) as e0 rab E0 with the transition dipole moment e0 rab from the measured oscillator strength f=0.015 for "feature a" of Ref. at 3.05 eV and the electric field strength E0 / (V/m) =2745 I0 / (W/ cm2) at our present intensities I0 =3.4× 1013 W/ cm2 to be ≃100 meV -which is larger than most of the vibrational level splittings in C60.
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57149133103
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Assuming that the total energy of the system is-after a few picoseconds-statistically distributed over the vibrational degrees of freedom, the kinetic shift energy is required to allow for channeling the necessary dissociation energy with sufficient probability into the coordinates involved in the bond breaking.
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Assuming that the total energy of the system is-after a few picoseconds-statistically distributed over the vibrational degrees of freedom, the kinetic shift energy is required to allow for channeling the necessary dissociation energy with sufficient probability into the coordinates involved in the bond breaking.
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39
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57149147427
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Note that for higher charge states an even faster relaxation would be expected. These ions, however, cannot be detected here due to the relatively weak probe pulse.
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Note that for higher charge states an even faster relaxation would be expected. These ions, however, cannot be detected here due to the relatively weak probe pulse.
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