2023
DOI: 10.1364/oe.500967
|View full text |Cite
|
Sign up to set email alerts
|

Image restoration for optical zooming system based on Alvarez lenses

Jiapu Yan,
Zhichao Ye,
Tingting Jiang
et al.

Abstract: Alvarez lenses are known for their ability to achieve a broad range of optical power adjustment by utilizing complementary freeform surfaces. However, these lenses suffer from optical aberrations, which restrict their potential applications. To address this issue, we propose a field of view (FOV) attention image restoration model for continuous zooming. In order to simulate the degradation of optical zooming systems based on Alvarez lenses (OZA), a baseline OZA is designed where the polynomial for the Alvarez … Show more

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
1
1

Citation Types

0
2
0

Year Published

2024
2024
2024
2024

Publication Types

Select...
2
1

Relationship

0
3

Authors

Journals

citations
Cited by 3 publications
(2 citation statements)
references
References 13 publications
0
2
0
Order By: Relevance
“…The phase distributions of the basic paraxial form of Alvarez lenses are given by Equations () and (). Figure 2A depicts the fundamental faceted shape 29 Z()x,ygoodbreak=A()13x3goodbreak+xy2goodbreak+italicDxgoodbreak+E, Z()x,ygoodbreak=goodbreak−A()13x3goodbreak+xy2goodbreak−italicDxgoodbreak+E, where Z is the surface sag of the lens; A is the coefficient that determines the ratio of displacement to optical power when the lenses move laterally; D is the tilt term that minimizes the surface sag; and E represents the center thickness of the lens, which is employed to ensure the thinnest portion to have sufficient mechanical strength.…”
Section: Methodsmentioning
confidence: 99%
See 1 more Smart Citation
“…The phase distributions of the basic paraxial form of Alvarez lenses are given by Equations () and (). Figure 2A depicts the fundamental faceted shape 29 Z()x,ygoodbreak=A()13x3goodbreak+xy2goodbreak+italicDxgoodbreak+E, Z()x,ygoodbreak=goodbreak−A()13x3goodbreak+xy2goodbreak−italicDxgoodbreak+E, where Z is the surface sag of the lens; A is the coefficient that determines the ratio of displacement to optical power when the lenses move laterally; D is the tilt term that minimizes the surface sag; and E represents the center thickness of the lens, which is employed to ensure the thinnest portion to have sufficient mechanical strength.…”
Section: Methodsmentioning
confidence: 99%
“…Unlike the traditional zoom lens, Alvarez lenses adjust the focal length by sliding two lenses perpendicular to the optical axis. [27][28][29][30] The phase distributions of the basic paraxial form of Alvarez lenses are given by Equations ( 1) and (2). Figure 2A depicts the fundamental faceted shape.…”
Section: Basic Principlementioning
confidence: 99%