Photoelectron angular distributions from both C(60) and C(70) were recorded for low laser intensity femtosecond and picosecond pulses. Rich structure is seen for electron kinetic energies that lie below the photon energy. Strong, broad peaks are observed for photoelectron energies corresponding to single-photon ionization of so-called superatom molecular orbitals (SAMOs). The very simple angular distributions measured for these peaks, the close similarity of the spectra observed from C(60) and C(70), and the comparison with time-dependent density functional theory provide strong support for the SAMO hypothesis.

Angular-resolved photoelectron spectroscopy using wavelength-tuneable femtosecond laser pulses is presented for a series of fullerenes, namely, C70, C82, and Sc3N@C80. The photoelectron kinetic energy distributions for the three molecules show typical thermal electron spectra with a superimposed peak structure that is the result of one-photon ionization of diffuse low-angular momenta states with electron density close to the carbon cage and that are related to so-called super atom molecular orbitals. Photoelectron angular distributions confirm this assignment. The observed structure is less prominent compared to the thermal electron background than what was observed in C60. It can be concluded that hot electron emission is the main ionization channel for the larger and more complex molecules for these excitation conditions.

Photoelectron spectra for fullerenes C(60) and C(70) ionized using 800 nm laser pulses with pulse durations from 120 to 1000 fs show thermal electron kinetic energy distributions but they also exhibit angular anisotropy with respect to the laser light polarization. The effective temperature of electrons, measured along the laser polarization direction, is significantly higher than in the perpendicular direction. We explain this observation by considering that the emission of the thermal electrons is uncorrelated with the phase of the laser pulse, unlike directly ionized electrons, and, depending on the time of emission, they may experience an additional "kick" from the vector potential of the laser field when they are emitted from the molecule.

Gas-phase fullerenes emit thermal electrons after femtosecond laser excitation in the wavelength range 400-800 nm. We have used angular-resolved photoelectron spectroscopy (PES) to study the influence of the laser's electric field on the dynamics of the thermally emitted electrons. The laser field introduces an asymmetry in the thermal electron distributions with respect to the laser polarization direction, which was confirmed by carrying out experiments at different wavelengths. A simple model could reproduce the trends in measured apparent temperatures in the PES. The asymmetry effect was exploited in a pump-probe experiment to estimate the time scale for thermal electron emission. It was found that, when 400 nm, 120 fs laser pulses of 2 TW cm(-2) intensity are used, thermal electrons are emitted up to ca. 300 fs after the peak of the laser pulse. The pump-probe scheme should be applicable to a wider range of complex molecules and clusters showing thermal electron emission on a femtosecond time scale.

Abstract. Photoelectron spectra are presented for C 60 excited with fs pulses of wavelengths 532 and 267 nm. The spectra indicate a quick redistribution of the excitation energy. Excitation of SAMO states is observed with 532 nm excitation, but due to the relatively large photon energy of the 267 nm pulses, these orbitals are not populated for this wavelength.