We present a theoretical study of ultrafast phase transitions induced by femtosecond laser pulses of arbitrary form. Molecular-dynamics simulations on time dependent potential-energy surfaces derived from a microscopic Hamiltonian are performed. Applying this method to diamond, we show that a nonequilibrium transition to graphite takes place for a wide range of laser pulse durations and intensities. This ultrafast transition (~100 fs) is driven by the suppression of the diamond minimum in the potential-energy surface of the laser excited system.
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Jeschke et al. (1999) studied this question.
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