34 research outputs found
Scattering of twisted electron wave-packets by atoms in the Born approximation
The potential scattering of electrons carrying non--zero quanta of the
orbital angular momentum (OAM) is studied in a framework of the generalized
Born approximation, developed in our recent paper by Karlovets \textit{et al.},
Phys. Rev. A. {\textbf 92}, 052703 (2015). We treat these so--called
\textit{twisted} electrons as spatially localized wave--packets. The simple and
convenient expressions are derived for a number of scattering events in
collision of such a vortex electron with a single potential, located at a given
impact parameter with respect to the wave-packet's axis. The more realistic
scenarios are also considered with either localized (mesoscopic) targets or
infinitely wide (macroscopic) ones that consist of the randomly distributed
atoms. Dependence of the electron scattering pattern on a size and on a
relative position of the target is studied in detail for all three scenarios of
the single--potential--, mesoscopic-- and the macroscopic targets made of
hydrogen in the ground state. The results demonstrate that the angular
distribution of the outgoing electrons can be very sensitive to the OAM and to
kinematic parameters of the focused twisted beams, as well as to composition of
the target. Scattering of vortex electrons by atoms can, therefore, serve as a
valuable tool for diagnostic of such beams.Comment: 13 pages, 6 figure
Bound-free pair production in relativistic nuclear collisions from the NICA to the HE LHC colliders
We consider the electron-positron pair production in relativistic heavy ion
collisions, in which the produced electron is captured by one of the nuclei
resulting, thus, in the formation of a hydrogen--like ion. These ions emerge
from the collision point and hit the vacuum chamber wall inside superconducting
magnets. Therefore, this process may be important for the problems of beam life
time and for the quenching the irradiated magnet. A theoretical investigation
for such a bound-free pair production (BFPP) at the colliders from NICA to HE
LHC is presented. We obtain an approximate universal formula for the total
cross section of the process. We compare it with the results of available
numerical calculations and estimate that an accuracy of our calculations is
better than % at the energies of the NICA collider and becomes of the
order of a few percent for the RHIC and HE LHC colliders. Based on the obtained
results, the detailed calculations are performed for future experiments at the
NICA collider. We find that the expected BFPP cross sections for the
Au-Au and Bi-Bi collisions are in the range
from to barn, while for the p-Au and p-Bi collisions
they are in the range of a few mbarn.Comment: 10 pages, 6 figure
Non-linear quantum effects in electromagnetic radiation of a vortex electron
There is a controversy of how to interpret interactions of electrons with a
large spatial coherence with light and matter. When such an electron emits a
photon, it can do so either as if its charge were confined to a point within a
coherence length, the region where a square modulus of a wave function
is localized, or as a continuous cloud of space charge spread over
it. This problem was addressed in a recent study R.~Remez, et al., Phys. Rev.
Lett. {\bf 123}, 060401 (2019) where a conclusion was drawn in favor of the
first (point) interpretation. Here we argue that there is an alternative
explanation for the measurements reported in that paper, which relies on purely
classical arguments and does not allow one to refute the second interpretation.
We propose an experiment of Smith-Purcell radiation from a non-relativistic
vortex electron carrying orbital angular momentum, which can unambiguously lead
to the opposite conclusion. Beyond the paraxial approximation, the vortex
packet has a non-point electric quadrupole moment, which grows as the packet
spreads and results in a non-linear -growth of the radiation intensity
with the length of the grating when is much larger than the packet's
Rayleigh length. Such a non-linear effect has never been observed for single
electrons and, if detected, it would be a hallmark of the non-point nature of
charge in a wave packet. Thus, two views on are complementary to
each other and an electron radiates either as a point charge or as a continuous
charge flow depending on the experimental conditions and on its quantum state.
Our conclusions hold for a large class of non-Gaussian packets and emission
processes for which the radiation formation length can exceed the Rayleigh
length, such as Cherenkov radiation, transition radiation, diffraction
radiation, and so forth.Comment: 25 pages; 4 figure
High sensitivity Cavity Ring Down spectroscopy of 18O enriched carbon dioxide between 5850 and 7000 cm-1: Part III-Analysis and theoretical modeling of the 12C17O2, 16O12C17O, 17O12C18O, 16O13C17O and 17O13C18O spectra
More than 19,700 transitions belonging to 11 isotopologues of carbon dioxide
have been assigned in the room temperature absorption spectrum of highly 18O
enriched carbon dioxide recorded by very high sensitivity CW-Cavity Ring Down
spectroscopy between 5851 and 6990 cm-1 (1.71-1.43 \mum). This third and last
report is devoted to the analysis of the bands of five 17O containing
isotopologues present at very low concentration in the studied spectra:
16O12C17O, 17O12C18O, 16O13C17O, 17O13C18O and 12C17O2 (627, 728, 637, 738 and
727 in short hand notation). On the basis of the predictions of effective
Hamiltonian models, a total of 1759, 1786, 335, 273 and 551 transitions
belonging to 24, 24, 5, 4 and 7 bands were rovibrationally assigned for 627,
728, 637, 738 and 727, respectively. For comparison, only five bands were
previously measured in the region for the 728 species. All the identified bands
belong to the \deltaP=8 and 9 series of transitions, where P=2V1+V2+3V3 is the
polyad number (Vi are vibrational quantum numbers). The band-by-band analysis
has allowed deriving accurate spectroscopic parameters of 61 bands from a fit
of the measured line positions. Two interpolyad resonance perturbations were
identified
Transmission of vortex electrons through a solenoid
We argue that it is generally nonstationary Laguerre-Gaussian states (NSLG)
rather than the Landau ones that appropriately describe electrons with orbital
angular momentum both in their dynamics at a hard-edge boundary between a
solenoid and vacuum and inside the magnetic field. It is shown that the r.m.s.
radius of the NSLG state oscillates in time and its period-averaged value can
significantly exceed the r.m.s. radius of the Landau state, even far from the
boundary. We propose to study the unconventional features of quantum dynamics
inside a solenoid in several experimental scenarios with vortex electrons
described by the NSLG states. Relevance for processes in scanning and
transmission electron microscopes, as well as for particle accelerators with
relativistic beams is emphasized.Comment: 6 pages, 2 figure
Radiative polarization of electrons in a strong laser wave
We reanalyze the problem of radiative polarization of electrons brought into
collision with a circularly polarized strong plane wave. We present an
independent analytical verification of formulae for the cross section given by
D.\,Yu. Ivanov et al [Eur.\ Phys.\ J. C \textbf{36}, 127 (2004)]. By choosing
the exact electron's helicity as the spin quantum number we show that the
self-polarization effect exists only for the moderately relativistic electrons
with energy and only for a non-head-on collision
geometry. In these conditions polarization degree may achieve the values up to
65%, but the effective polarization time is found to be larger than 1\,s even
for a high power optical or infrared laser with intensity parameter (). This
makes such a polarization practically unrealizable. We also compare these
results with the ones of some papers where the high degree of polarization was
predicted for ultrarelativistic case. We argue that this apparent contradiction
arises due to the different choice of the spin quantum numbers. In particular,
the quantum numbers which provide the high polarization degree represent
neither helicity nor transverse polarization, that makes the use of them
inconvenient in practice.Comment: minor changes compared to v3; to appear in PR
New transitions and energy levels of water vapor by high sensitivity CRDS near 1.73 and 1.54 µm
This contribution is part of a long term project aiming at improving the water absorption spectroscopy by high sensitivity cavity ring down spectroscopy (CRDS) in the near infrared. Two new sources of CRDS spectra are considered: (i) The room temperature absorption spectrum of water vapor in natural isotopic abundance is recorded near 1.73 µm. A series of recordings was performed from 5693 to 5991 cm−1 with a pressure value of about 6 Torr. The noise equivalent absorption (αmin) of the spectra is better than 10− 10 cm−1. A total of 1453 lines were assigned to 1573 transitions of four water isotopologues (H2 16O, H2 17O, H2 18O and HD16O). Their intensities span more than five orders of magnitude from 3.0 × 10−30 to 4.7 × 10−25 cm/molecule at 296 K. The assignments were performed using known experimental energy levels as well as calculated line lists based on the results of Schwenke and Partridge. Two hundred fifty-one lines (assigned to 280 transitions) are observed for the first time and twelve energy levels are newly determined. The comparison of the obtained line parameters with those of the HITRAN database is discussed. Forty-six line positions are observed to significantly differ from their HITRAN values (δν = │νHITRAN – νCRDS│ > 0.02 cm−1). The derived set of energy levels is compared to those recommended by an IUPAC task group. (ii) The room temperature CRDS spectrum of water vapor highly enriched in 17O was recorded near 1.54 µm (6223–6672 cm−1) at a pressure of 12 Torr. Compared to a previous study, the higher pressure of the recordings allowed for extending the observations. Overall, twenty-six new levels were determined for both H2 17O and HD17O. All these observations together with other recent measurements will allow for an extension and an update of our empirical database in the 5693– 8340 cm−1 region. © 2019 Elsevier Lt