An analytical method for calculating the electromagnetic fields of a nonparaxial elegant Laguerre-Gaussian (LG) vortex beam is presented for arbitrary pulse duration, spot size, and LG mode. This perturbative approach provides a numerically tractable model for the calculation of arbitrarily high radial and azimuthal LG modes in the nonparaxial regime, without requiring integral representations of the fields. A key feature of this perturbative model is its use of a Poisson-like frequency spectrum, which allows for the proper description of pulses of arbitrarily short duration. This model is thus appropriate for simulating laser-matter interactions, including those involving short laser pulses
The electromagnetic field of optical vortices is in most cases derived from vector and scalar potent...
We find the analytical electromagnetic fields, both paraxial and with non-paraxial corrections, of a...
The exact vector integral solution for all the electromagnetic field components of a general flatten...
An analytical method for calculating the electromagnetic fields of a nonparaxial elegant Laguerre-Ga...
An analytical method for calculating the electromagnetic fields of a nonparaxial elegant Laguerre-Ga...
An analytic expression for a polychromatic phasor representing an arbitrarily short elegant Laguerre...
An analytical method for calculating the electromagnetic fields of a nonparaxial elegant Laguerre-Ga...
Longitudinal fields of quantized Laguerre-Gaussian modes are derived, revealing their importance eve...
Non-paraxial theories of wave propagation are essential to model the interaction of highly focused l...
Introducing a spatial chirp into a pulse with a longitudinal vortex, such as a standard pulsed Lague...
Longitudinal electromagnetic fields generally become comparable with the usually dominant transverse...
The Laguerre–Gaussian (LG) beam expansion is described as a numerical and physical model of paraxial...
The intensity peak of a "flying focus" travels at a programmable velocity over many Rayleigh ranges ...
journal_title: Laser Physics article_type: paper article_title: On beam models and their paraxial ap...
International audienceWe propose an algorithm to introduce arbitrarily shaped laser pulses into elec...
The electromagnetic field of optical vortices is in most cases derived from vector and scalar potent...
We find the analytical electromagnetic fields, both paraxial and with non-paraxial corrections, of a...
The exact vector integral solution for all the electromagnetic field components of a general flatten...
An analytical method for calculating the electromagnetic fields of a nonparaxial elegant Laguerre-Ga...
An analytical method for calculating the electromagnetic fields of a nonparaxial elegant Laguerre-Ga...
An analytic expression for a polychromatic phasor representing an arbitrarily short elegant Laguerre...
An analytical method for calculating the electromagnetic fields of a nonparaxial elegant Laguerre-Ga...
Longitudinal fields of quantized Laguerre-Gaussian modes are derived, revealing their importance eve...
Non-paraxial theories of wave propagation are essential to model the interaction of highly focused l...
Introducing a spatial chirp into a pulse with a longitudinal vortex, such as a standard pulsed Lague...
Longitudinal electromagnetic fields generally become comparable with the usually dominant transverse...
The Laguerre–Gaussian (LG) beam expansion is described as a numerical and physical model of paraxial...
The intensity peak of a "flying focus" travels at a programmable velocity over many Rayleigh ranges ...
journal_title: Laser Physics article_type: paper article_title: On beam models and their paraxial ap...
International audienceWe propose an algorithm to introduce arbitrarily shaped laser pulses into elec...
The electromagnetic field of optical vortices is in most cases derived from vector and scalar potent...
We find the analytical electromagnetic fields, both paraxial and with non-paraxial corrections, of a...
The exact vector integral solution for all the electromagnetic field components of a general flatten...