2010
DOI: 10.1364/oe.18.010822
|View full text |Cite
|
Sign up to set email alerts
|

Focusing of a femtosecond vortex light pulse through a high numerical aperture objective

Abstract: We investigate the focusing properties of a femtosecond vortex light pulse focused by a high numerical aperture objective. By using the Richards-Wolf vectorial diffraction method, the intensity distribution, the velocity variation and the orbital angular momentum near the focus are studied in great detail. We have discovered that the femtosecond vortex light pulse can travel at various speeds, that is, slower or faster than light with a tight focusing system. Moreover, we have found that the numerical aperture… Show more

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
2
1
1
1

Citation Types

0
6
0

Year Published

2012
2012
2023
2023

Publication Types

Select...
5
1

Relationship

0
6

Authors

Journals

citations
Cited by 22 publications
(6 citation statements)
references
References 22 publications
0
6
0
Order By: Relevance
“…where (r,  , t) is the incoming time-dependent polar coordinate; σ 0 and m stand for the beam waist and the topological charge of the incident beam; A(t) = exp[-(a g t/T) 2 ]exp(-iω 0 t) is the temporal pulse having a Gaussian shape envelope, in which a g = (2ln2) 1/2 , T denotes the pulse duration, as well as ω 0 is its central angular frequency. According to the time-dependent vectorial diffraction theory [16][17]18 , we can garner the focal light fields in the Fourier domain,…”
Section: Theoretical Analysismentioning
confidence: 99%
See 2 more Smart Citations
“…where (r,  , t) is the incoming time-dependent polar coordinate; σ 0 and m stand for the beam waist and the topological charge of the incident beam; A(t) = exp[-(a g t/T) 2 ]exp(-iω 0 t) is the temporal pulse having a Gaussian shape envelope, in which a g = (2ln2) 1/2 , T denotes the pulse duration, as well as ω 0 is its central angular frequency. According to the time-dependent vectorial diffraction theory [16][17]18 , we can garner the focal light fields in the Fourier domain,…”
Section: Theoretical Analysismentioning
confidence: 99%
“…f represents the focal length of the objective lens. Here the pupil apodization function of a single spectral component can be expressed as 16,17 :…”
Section: J U S T a C C E P T E Dmentioning
confidence: 99%
See 1 more Smart Citation
“…One the other hand, the same hybridly polarized counterpart in the presence of vortex phases is also focused by the same objective lens, enabling the locally induced circular polarization at the focus of the total light field, therefore allowing access to the ultrafast OTLS conversion. In this connection, we start from an incident hybridly polarized light field with the vortex-dressed Laguerre-Gaussian (LG) femtosecond pulse envelope, which in the pupil plane can be featured by, [34][35][36] Eðr, φ, tÞ…”
Section: Theoretical Analyses Of Ultrafast Hybridly Polarized Vectori...mentioning
confidence: 99%
“…We then introduce the incident light fields charactered by Equation ( 1) into a high NA objective lens, after which a 3D-polarized tightly focused light fields can be well-established. In this way, according to the time-dependent vectorial diffraction theory, [34,35] such 3D light fields in optical spectrum domain near the focus point can be formulized as…”
Section: Theoretical Analyses Of Ultrafast Hybridly Polarized Vectori...mentioning
confidence: 99%