Impact of an initial laser beam profile on the structure and correctability of thermal blooming aberrations

Prior thermal blooming studies focused on macroscopic phenomena, often lacking quantitative analysis of the wavefront aberration structure. This paper uses Zernike polynomial decomposition to compare the thermal blooming aberration structures and correctability of Gaussian versus flat-top beams. Under the weak thermal blooming assumption, the study reveals that the initial intensity gradient dictates the aberration structure. Flat-top beam thermal blooming is ’pure-type’ and tilt-dominant; Gaussian beam blooming is ’complex-type’ with significant multi-mode coupling. At N D = 50, this discrepancy yields max Strehl Ratios (SR) of 0.54 (flat-top) and 0.22 (Gaussian) for low-order correction. This supports a beam-shaping strategy to ’reshape aberrations at the source, simplifying correction’. The demonstrated ’structural stability’ and ’predictable severity’ provide tools for ’optimal correction’ via aberration balancing and open pathways for open-loop predictive correction.

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Publication Details

Journal
Optics Express
Published
2026-02-18
DOI
https://doi.org/10.1364/oe.585216
Primary Topic
Adaptive optics and wavefront sensing
Type
article
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article

Impact of an initial laser beam profile on the structure and correctability of thermal blooming aberrations

Zeli Tang, Gangyu Wang, Changhu Wang, Yilun Cheng et al.
Optics Express
Adaptive optics and wavefront sensing
article

Impact of an initial laser beam profile on the structure and correctability of thermal blooming aberrations

Zeli Tang, Gangyu Wang, Changhu Wang, Yilun Cheng, Laian Qin, Zaihong Hou, Xu Jing, Yang Li
article en

Abstract

Prior thermal blooming studies focused on macroscopic phenomena, often lacking quantitative analysis of the wavefront aberration structure. This paper uses Zernike polynomial decomposition to compare the thermal blooming aberration structures and correctability of Gaussian versus flat-top beams. Under the weak thermal blooming assumption, the study reveals that the initial intensity gradient dictates the aberration structure. Flat-top beam thermal blooming is ’pure-type’ and tilt-dominant; Gaussian beam blooming is ’complex-type’ with significant multi-mode coupling. At N D = 50, this discrepancy yields max Strehl Ratios (SR) of 0.54 (flat-top) and 0.22 (Gaussian) for low-order correction. This supports a beam-shaping strategy to ’reshape aberrations at the source, simplifying correction’. The demonstrated ’structural stability’ and ’predictable severity’ provide tools for ’optimal correction’ via aberration balancing and open pathways for open-loop predictive correction.

Optics ExpressVol. 34(6)
University of Science and Technology of China (CN), Chinese Academy of Sciences (CN)
Openalex Percentile: Top 49%
Adaptive optics and wavefront sensing
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