2004
DOI: 10.1117/12.511373
|View full text |Cite
|
Sign up to set email alerts
|

Studies of pointing, acquisition, and tracking of agile optical wireless transceivers for free-space optical communication networks

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
3
1
1

Citation Types

0
18
0

Year Published

2005
2005
2019
2019

Publication Types

Select...
6
3

Relationship

0
9

Authors

Journals

citations
Cited by 31 publications
(18 citation statements)
references
References 0 publications
0
18
0
Order By: Relevance
“…Since the beams under study enter the lens at an angle and intersect the entire lens area, the full geometrical effects of the lens are considered, resulting in a phase retardation given by (3) where z o is the maximum thickness of the lens, n is the refractive index, R 1 and R 2 are the curvatures of the first and second surface, respectively, and ρ 2 = x 2 + y 2 . To simplify calculations and reflect typical experimental conditions, the lens is assumed biconvex (R 1 = R 2 = R) with a refractive index of 1.5, under which conditions the focal length f ≈ R. The field just after the lens is then given by (4) To propagate this field to the fiber plane (x′, y′), a convolution integral is calculated using the spatial impulse response. The resulting equation for the field at a distance f behind the lens is given by (5) where the integral is over the entire area of the lens and is repeated for each point (x′, y′) in the fiber plane.…”
Section: Plane Wave Analysismentioning
confidence: 99%
See 1 more Smart Citation
“…Since the beams under study enter the lens at an angle and intersect the entire lens area, the full geometrical effects of the lens are considered, resulting in a phase retardation given by (3) where z o is the maximum thickness of the lens, n is the refractive index, R 1 and R 2 are the curvatures of the first and second surface, respectively, and ρ 2 = x 2 + y 2 . To simplify calculations and reflect typical experimental conditions, the lens is assumed biconvex (R 1 = R 2 = R) with a refractive index of 1.5, under which conditions the focal length f ≈ R. The field just after the lens is then given by (4) To propagate this field to the fiber plane (x′, y′), a convolution integral is calculated using the spatial impulse response. The resulting equation for the field at a distance f behind the lens is given by (5) where the integral is over the entire area of the lens and is repeated for each point (x′, y′) in the fiber plane.…”
Section: Plane Wave Analysismentioning
confidence: 99%
“…FSO is being seriously investigated as a means for establishing high-bandwidth links for a variety of applications, including inter-satellite communication, airborne internet, disaster recovery communications, and battlefield communication [1][2][3][4] . The high bandwidth available with FSO makes it an attractive option for such applications since a permanent communication link is not required to move large amounts of data.…”
Section: Introductionmentioning
confidence: 99%
“…Therefore, an automatic beam pointing, acquisition and tracking (PAT) mechanism with associated protocol and software are required at each transceiver and each mirror. Such systems have been proposed and studied in the literature, see for example [9], [10]. In our model these errors do not affect link reliability, only link outage probability which in turn affects maximum link distance.…”
Section: Introductionmentioning
confidence: 99%
“…3) Complexity associated with physical topology implementation through beam redirection: Physical beam redirection is achieved through pointing, acquisition and tracking (PAT) [10,11]. For purposes of simulation and modeling, we have abstracted this functionality assuming a conservative estimate of 2 seconds for physical implementation of the new network.…”
Section: Introductionmentioning
confidence: 99%