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本文引用的文献

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The use of autorefractors using the image-size principle in determining on-axis and off-axis refraction. Part 2: Theoretical study of peripheral refraction with the Grand Seiko AutoRef/Keratometer WAM-5500.应用像方大小原理的自动验光仪在确定轴上和轴外屈光度中的应用。第 2 部分:用 Grand Seiko AutoRef/Keratometer WAM-5500 进行周边屈光度的理论研究。
Ophthalmic Physiol Opt. 2022 Mar;42(2):293-300. doi: 10.1111/opo.12936. Epub 2021 Dec 20.
2
The use of autorefractors using the image-size principle in determining on-axis and off-axis refraction. Part 1: Analysis of optical principles of autorefractors.使用像差仪测量眼轴和非眼轴屈光度的图像尺寸原理。第 1 部分:像差仪的光学原理分析。
Ophthalmic Physiol Opt. 2022 Mar;42(2):283-292. doi: 10.1111/opo.12933. Epub 2021 Dec 20.
3
Comparison of radius of anterior lens surface curvature measurements using the anterior segment optical coherence tomography and Scheimpflug imaging.使用眼前节光学相干断层扫描和Scheimpflug成像技术对晶状体前表面曲率半径测量结果的比较。
Ann Transl Med. 2020 Mar;8(5):177. doi: 10.21037/atm.2020.01.100.
4
Interventions to slow progression of myopia in children.减缓儿童近视进展的干预措施。
Cochrane Database Syst Rev. 2020 Jan 13;1(1):CD004916. doi: 10.1002/14651858.CD004916.pub4.
5
Morphological changes of human crystalline lens in myopia.近视患者人晶状体的形态学变化。
Biomed Opt Express. 2019 Nov 5;10(12):6084-6095. doi: 10.1364/BOE.10.006084. eCollection 2019 Dec 1.
6
Peripheral Refraction and Eye Lengths in Myopic Children in the Bifocal Lenses In Nearsighted Kids (BLINK) Study.双焦点镜片治疗近视儿童(BLINK)研究中的周边屈光和眼轴长度
Transl Vis Sci Technol. 2019 Apr 12;8(2):17. doi: 10.1167/tvst.8.2.17. eCollection 2019 Apr.
7
IMI - Report on Experimental Models of Emmetropization and Myopia.IMI-正视化和近视实验模型报告。
Invest Ophthalmol Vis Sci. 2019 Feb 28;60(3):M31-M88. doi: 10.1167/iovs.18-25967.
8
IMI - Myopia Control Reports Overview and Introduction.国际近视研究学会( IMI ) - 近视防控报告概述及介绍
Invest Ophthalmol Vis Sci. 2019 Feb 28;60(3):M1-M19. doi: 10.1167/iovs.18-25980.
9
measurement of the human crystalline lens equivalent refractive index using extended-depth OCT.使用扩展深度光学相干断层扫描测量人晶状体等效折射率
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建模周边眼长和屈光度。

Modelling eye lengths and refractions in the periphery.

机构信息

Ophthalmology, Boston Children's Hospital, Boston, Massachusetts, USA.

Ophthalmology, Harvard Medical School, Boston, Massachusetts, USA.

出版信息

Ophthalmic Physiol Opt. 2023 Jul;43(4):815-826. doi: 10.1111/opo.13133. Epub 2023 Mar 31.

DOI:10.1111/opo.13133
PMID:36999932
原文链接:https://pmc.ncbi.nlm.nih.gov/articles/PMC11732252/
Abstract

PURPOSE

To create a simplified model of the eye by which we can specify a key optical characteristic of the crystalline lens, namely its power.

METHODS

Cycloplegic refraction and axial length were obtained in 60 eyes of 30 healthy subjects at eccentricities spanning 40° nasal to 40° temporal and were fitted with a three-dimensional parabolic model. Keratometric values and geometric distances to the cornea, lens and retina from 45 eyes supplied a numerical ray tracing model. Posterior lens curvature (PLC) was found by optimising the refractive data using a fixed lens equivalent refractive index ( ). Then, was found using a fixed PLC.

RESULTS

Eccentric refractive errors were relatively hyperopic in eyes with central refractions ≤-1.44 D but relatively myopic in emmetropes and hyperopes. Posterior lens power, which cannot be measured directly, was derived from the optimised model lens. There was a weak, negative association between derived PLC and central spherical equivalent refraction. Regardless of refractive error, the posterior retinal curvature remained fixed.

CONCLUSIONS

By combining both on- and off-axis refractions and eye length measurements, this simplified model enabled the specification of posterior lens power and captured off-axis lenticular characteristics. The broad distribution in off-axis lens power represents a notable contrast to the relative stability of retinal curvature.

摘要

目的

建立简化的眼球模型,用以确定晶状体的一个关键光学特性,即其屈光度。

方法

对 30 名健康受试者的 60 只眼进行睫状肌麻痹验光和眼轴长度测量,这些眼的偏心距范围从鼻侧 40°到颞侧 40°。采用三维抛物线模型对这些数据进行拟合。6 只眼的角膜曲率计值和距角膜、晶状体和视网膜的几何距离提供了一个数值光线追踪模型。通过使用固定的晶状体等效折射率( )优化屈光数据,找到后晶状体曲率(PLC)。然后,使用固定的 PLC 找到 。

结果

中央屈光度≤-1.44 D 的眼的偏心折射误差相对远视,但在正视眼和远视眼中相对近视。无法直接测量的后晶状体屈光度是从优化模型晶状体中得出的。优化后的 PLC 与中央球镜等效屈光度之间存在微弱的负相关。无论屈光不正如何,后视网膜曲率保持不变。

结论

通过结合眼内和眼外的折射和眼轴长度测量,该简化模型能够确定后晶状体的屈光度,并捕获眼外晶状体的特性。眼外晶状体屈光度的广泛分布与视网膜曲率的相对稳定性形成鲜明对比。