welcome to this meeting or abstract on direct perks data creation by tonal ionisation
when a strong lay samples is applied to an optimal yet a nickel potential is
to sit and than electronic internal through the potential barrier
then it doesn't relates in the laser field until the laser pulse has passed
in the third step the electron can either escape the parent ion
it can be called in the boundary breaks state or the electronic and recall database
parent i in
resulting in a number of important phenomena
most notably high harmonic generation
both the number of feedback state and the number of high harmonic generation events
strongly decline with increasing ellipticity of the laser
while both processes show similar dynamics transfers to the electric field
explaining similar dependence on ellipticity
they have different dynamics longitudinal to lace if you
because the ionisation occurs in different parts of the optical cycle
neglecting the and fuels during the poles
the electron trajectory in the laser field can be approximated analytically
of the laser pulse
the electron has gained transverse thrift velocity which depends on ellipticity
we showed that the kinetic energy of rate per collections at the end of the
laser poles must be very small
this means the initial transverse velocity at the tonal accent
and the final drift velocity must cancel each other out
this is effective constraint on the initial condition of the electrons immediately after total ionisation
the coloured regions show initial conditions of ionisation face transverse velocity for which electrons and
up into a perk states
depending on the ellipticity
the transpose velocity enough to tunnel tiny station has a gaussian distribution
using this distribution we show that the required fields displays a gaussian dependence on electricity
as well
comparing experimental data with monte-carlo simulations
and is derived analytical formula
the very good agreement is found
we simulated the trajectory of electrons during the laser pulse enough to
taking account both the laser field and ti and potential
first the electron also late in the lace a few along the right trajectory
once the laser poses polished
it stays
on an elliptic lower bit as expected
that's one always stays relatively far away from the onion
its closest point is that l x it
this is in fact the typical behavior for a perk trajectories
at least eighty percent of all of it broke electrons obeys to further we then
there exits radius stylization
looking at the face of the field at the moment of ionisation this revealed that
repair guy electrons alright nice to predominantly before the peak therefore don't not three scatter
in contrast elections involved in high harmonic generation or ionised off to the peak of
the electric field and therefore come back to the parent ion