2009
DOI: 10.1103/physreva.79.031201
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Dead-time-free ion momentum spectroscopy of multiple ionization of Xe clusters irradiated by euv free-electron laser pulses

Abstract: We have investigated multiple ionization of Xe clusters by 61-nm 1011–1012 W/cm2 extreme-ultraviolet light pulses at the free-electron laser facility, SPring-8 Compact SASE Source test accelerator, in Japan, using a dead-time-free three-dimensional momentum spectrometer. It was found that the average kinetic energy of atomic Xe+ ions increases when increasing the laser power density and the cluster size. For these experimental conditions significant frustration of the cluster photoionization occurs but no indi… Show more

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Cited by 46 publications
(24 citation statements)
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“…Argon clusters irradiated with 32 nm FEL pulses and power densities of 4x10 14 W/cm 2 exhibit ion kinetic energies of a few eV only and larger cluster fragments appear [10], similar to subsequent experiments at 51 nm [27].…”
Section: Iii1mentioning
confidence: 61%
“…Argon clusters irradiated with 32 nm FEL pulses and power densities of 4x10 14 W/cm 2 exhibit ion kinetic energies of a few eV only and larger cluster fragments appear [10], similar to subsequent experiments at 51 nm [27].…”
Section: Iii1mentioning
confidence: 61%
“…At SCSS, over the photon energy range 20 and 24 eV, with the FEL power density in the range 10 11 − 10 14 W/cm 2 , Nagaya and coworkers investigated extensively EUVFEL-induced dynamics of various rare gas clusters [373][374][375][376][377][378][379][380]. Under these experimental conditions they found (via ion spectrometry) frustration of direct cluster photoionization stemming from the strong Coulomb potential of the highly ionized cluster but no indication for heating mechanisms other than sequential photoionization of the individual atoms in the cluster [373,374,377]. They also discussed charge redistribution in both xenon clusters [375] and in argon-core-neon-shell clusters [376].…”
Section: Clustersmentioning
confidence: 99%
“…The difference between multi-photon ionization at near-infrared frequencies (∼ 1.5 eV) and at extreme-ultraviolet (XUV) frequencies or higher (> 50 eV) lies in the fact that multi-photon single-electron ionization is drastically suppressed in the latter case due to the small dipole matrix elements for continuum-continuum transitions which typically would be required for an electron to absorb more than one photon. As a consequence, multi-photon ionization by XUV or X-ray radiation, as available from novel free-electron laser sources [1][2][3], means single-photon ionization of many atoms in an extended target such as a cluster or bio-molecule [4][5][6]. We call this process photo activation.…”
Section: Introductionmentioning
confidence: 99%