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Helium photoelectron angular distribution

Figure 5.13 Helium photoelectron angular distribution in the He+(2p) channel (logarithmic scale). x-Axis cosine of the electron ejection angle relative the laser polarization, y-axis total energy (1 a.u. 27 eV). (a) After the XUV-pulse after the IR-pulse for three different time delays, separated from each other by half the IR-pulse period, 15.53 fs (b), 16.87 fs(c), and 18.21 (d). The fringes in (b)-(d) arise due to the interference between the (XUV-pulse) direct ionization from the ground state and the (IR-pulse) ionization from the doubly excited populated by the XUV-pulse. Figure 5.13 Helium photoelectron angular distribution in the He+(2p) channel (logarithmic scale). x-Axis cosine of the electron ejection angle relative the laser polarization, y-axis total energy (1 a.u. 27 eV). (a) After the XUV-pulse after the IR-pulse for three different time delays, separated from each other by half the IR-pulse period, 15.53 fs (b), 16.87 fs(c), and 18.21 (d). The fringes in (b)-(d) arise due to the interference between the (XUV-pulse) direct ionization from the ground state and the (IR-pulse) ionization from the doubly excited populated by the XUV-pulse.
Figure 1.18 Example of the determination of the Stokes parameter S, and tilt angle X measured at 40 eV photon energy. It is based on an angular distribution measurement of ls-photoelectrons in helium for which equ. (1.55a) holds with P = 2. The arrows point to the measured values (with error bars, some of which are too small to be visible) the solid curve is a fit of the experimental data to this equation from which = 0.819(3) and... Figure 1.18 Example of the determination of the Stokes parameter S, and tilt angle X measured at 40 eV photon energy. It is based on an angular distribution measurement of ls-photoelectrons in helium for which equ. (1.55a) holds with P = 2. The arrows point to the measured values (with error bars, some of which are too small to be visible) the solid curve is a fit of the experimental data to this equation from which = 0.819(3) and...
Angular distribution parameters ft of photoelectrons Is photoionization in helium / = 2.0 (in dipole approximation)... [Pg.276]

Fig. 7.15. The photoelectron kinetic energy distribution following photoexcitation at 23.8 eV, below the ionization threshold at 24.6 eV, of large pure helium droplets N = 10 atoms. Most of the electrons leave the droplet with zero kinetic energy and have an isotropic angular distribution. ... Fig. 7.15. The photoelectron kinetic energy distribution following photoexcitation at 23.8 eV, below the ionization threshold at 24.6 eV, of large pure helium droplets N = 10 atoms. Most of the electrons leave the droplet with zero kinetic energy and have an isotropic angular distribution. ...

See other pages where Helium photoelectron angular distribution is mentioned: [Pg.445]    [Pg.290]    [Pg.296]    [Pg.370]    [Pg.350]   
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Angular distribution

Photoelectron angular distributions

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