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年轻健康成年人在调节过程中高阶像差与眼前节生物测量之间的关系

The Relationship Between High-Order Aberration and Anterior Ocular Biometry During Accommodation in Young Healthy Adults.

作者信息

Ke Bilian, Mao Xinjie, Jiang Hong, He Jichang, Liu Che, Li Min, Yuan Ying, Wang Jianhua

机构信息

Department of Ophthalmology, Shanghai General Hospital, Shanghai Jiao Tong University School of Medicine, Shanghai, China.

Bascom Palmer Eye Institute, University of Miami Miller School of Medicine, Miami, Florida, United States.

出版信息

Invest Ophthalmol Vis Sci. 2017 Nov 1;58(13):5628-5635. doi: 10.1167/iovs.17-21712.

Abstract

PURPOSE

This study investigated the anterior ocular anatomic origin of high-order aberration (HOA) components using optical coherence tomography and a Shack-Hartmann wavefront sensor.

METHODS

A customized system was built to simultaneously capture images of ocular wavefront aberrations and anterior ocular biometry. Relaxed, 2-diopter (D) and 4-D accommodative states were repeatedly measured in 30 young subjects. Custom software was used to correct optical distortions and measure biometric parameters from the images.

RESULTS

The anterior ocular biometry changed during 2-D accommodation, in which central lens thickness, ciliary muscle thicknesses at 1 mm posterior to the scleral spur (CMT1), and the maximum value of ciliary muscle thickness increased significantly, whereas anterior chamber depth, CMT3, radius of anterior lens surface curvature (RAL), and radius of posterior lens surface curvature (RPL) decreased significantly. The changes in the anterior ocular parameters during 4-D accommodation were similar to those for the 2-D accommodation. (\def\upalpha{\unicode[Times]{x3B1}})(\def\upbeta{\unicode[Times]{x3B2}})(\def\upgamma{\unicode[Times]{x3B3}})(\def\updelta{\unicode[Times]{x3B4}})(\def\upvarepsilon{\unicode[Times]{x3B5}})(\def\upzeta{\unicode[Times]{x3B6}})(\def\upeta{\unicode[Times]{x3B7}})(\def\uptheta{\unicode[Times]{x3B8}})(\def\upiota{\unicode[Times]{x3B9}})(\def\upkappa{\unicode[Times]{x3BA}})(\def\uplambda{\unicode[Times]{x3BB}})(\def\upmu{\unicode[Times]{x3BC}})(\def\upnu{\unicode[Times]{x3BD}})(\def\upxi{\unicode[Times]{x3BE}})(\def\upomicron{\unicode[Times]{x3BF}})(\def\uppi{\unicode[Times]{x3C0}})(\def\uprho{\unicode[Times]{x3C1}})(\def\upsigma{\unicode[Times]{x3C3}})(\def\uptau{\unicode[Times]{x3C4}})(\def\upupsilon{\unicode[Times]{x3C5}})(\def\upphi{\unicode[Times]{x3C6}})(\def\upchi{\unicode[Times]{x3C7}})(\def\uppsy{\unicode[Times]{x3C8}})(\def\upomega{\unicode[Times]{x3C9}})(\def\bialpha{\boldsymbol{\alpha}})(\def\bibeta{\boldsymbol{\beta}})(\def\bigamma{\boldsymbol{\gamma}})(\def\bidelta{\boldsymbol{\delta}})(\def\bivarepsilon{\boldsymbol{\varepsilon}})(\def\bizeta{\boldsymbol{\zeta}})(\def\bieta{\boldsymbol{\eta}})(\def\bitheta{\boldsymbol{\theta}})(\def\biiota{\boldsymbol{\iota}})(\def\bikappa{\boldsymbol{\kappa}})(\def\bilambda{\boldsymbol{\lambda}})(\def\bimu{\boldsymbol{\mu}})(\def\binu{\boldsymbol{\nu}})(\def\bixi{\boldsymbol{\xi}})(\def\biomicron{\boldsymbol{\micron}})(\def\bipi{\boldsymbol{\pi}})(\def\birho{\boldsymbol{\rho}})(\def\bisigma{\boldsymbol{\sigma}})(\def\bitau{\boldsymbol{\tau}})(\def\biupsilon{\boldsymbol{\upsilon}})(\def\biphi{\boldsymbol{\phi}})(\def\bichi{\boldsymbol{\chi}})(\def\bipsy{\boldsymbol{\psy}})(\def\biomega{\boldsymbol{\omega}})(\def\bupalpha{\unicode[Times]{x1D6C2}})(\def\bupbeta{\unicode[Times]{x1D6C3}})(\def\bupgamma{\unicode[Times]{x1D6C4}})(\def\bupdelta{\unicode[Times]{x1D6C5}})(\def\bupepsilon{\unicode[Times]{x1D6C6}})(\def\bupvarepsilon{\unicode[Times]{x1D6DC}})(\def\bupzeta{\unicode[Times]{x1D6C7}})(\def\bupeta{\unicode[Times]{x1D6C8}})(\def\buptheta{\unicode[Times]{x1D6C9}})(\def\bupiota{\unicode[Times]{x1D6CA}})(\def\bupkappa{\unicode[Times]{x1D6CB}})(\def\buplambda{\unicode[Times]{x1D6CC}})(\def\bupmu{\unicode[Times]{x1D6CD}})(\def\bupnu{\unicode[Times]{x1D6CE}})(\def\bupxi{\unicode[Times]{x1D6CF}})(\def\bupomicron{\unicode[Times]{x1D6D0}})(\def\buppi{\unicode[Times]{x1D6D1}})(\def\buprho{\unicode[Times]{x1D6D2}})(\def\bupsigma{\unicode[Times]{x1D6D4}})(\def\buptau{\unicode[Times]{x1D6D5}})(\def\bupupsilon{\unicode[Times]{x1D6D6}})(\def\bupphi{\unicode[Times]{x1D6D7}})(\def\bupchi{\unicode[Times]{x1D6D8}})(\def\buppsy{\unicode[Times]{x1D6D9}})(\def\bupomega{\unicode[Times]{x1D6DA}})(\def\bupvartheta{\unicode[Times]{x1D6DD}})(\def\bGamma{\bf{\Gamma}})(\def\bDelta{\bf{\Delta}})(\def\bTheta{\bf{\Theta}})(\def\bLambda{\bf{\Lambda}})(\def\bXi{\bf{\Xi}})(\def\bPi{\bf{\Pi}})(\def\bSigma{\bf{\Sigma}})(\def\bUpsilon{\bf{\Upsilon}})(\def\bPhi{\bf{\Phi}})(\def\bPsi{\bf{\Psi}})(\def\bOmega{\bf{\Omega}})(\def\iGamma{\unicode[Times]{x1D6E4}})(\def\iDelta{\unicode[Times]{x1D6E5}})(\def\iTheta{\unicode[Times]{x1D6E9}})(\def\iLambda{\unicode[Times]{x1D6EC}})(\def\iXi{\unicode[Times]{x1D6EF}})(\def\iPi{\unicode[Times]{x1D6F1}})(\def\iSigma{\unicode[Times]{x1D6F4}})(\def\iUpsilon{\unicode[Times]{x1D6F6}})(\def\iPhi{\unicode[Times]{x1D6F7}})(\def\iPsi{\unicode[Times]{x1D6F9}})(\def\iOmega{\unicode[Times]{x1D6FA}})(\def\biGamma{\unicode[Times]{x1D71E}})(\def\biDelta{\unicode[Times]{x1D71F}})(\def\biTheta{\unicode[Times]{x1D723}})(\def\biLambda{\unicode[Times]{x1D726}})(\def\biXi{\unicode[Times]{x1D729}})(\def\biPi{\unicode[Times]{x1D72B}})(\def\biSigma{\unicode[Times]{x1D72E}})(\def\biUpsilon{\unicode[Times]{x1D730}})(\def\biPhi{\unicode[Times]{x1D731}})(\def\biPsi{\unicode[Times]{x1D733}})(\def\biOmega{\unicode[Times]{x1D734}})({\rm{Z}}_4^0) decreased significantly during 2-D accommodation, and ({\rm{Z}}_3^{ - 1}), ({\rm{Z}}_3^1), ({\rm{Z}}_4^0), and ({\rm{Z}}_6^0) shifted to negative values during 4-D accommodation. The change in ({\rm{Z}}_4^0) negatively correlated with those in CMT1, and the negative change in ({\rm{Z}}_3^1) correlated with changes in RAL and CMT1.

CONCLUSIONS

HOA components altered during step-controlled accommodative stimuli. Ciliary muscle first contracted during stepwise accommodation, which may directly contribute to the reduction of spherical aberration (SA). The lens morphology was then altered, and the change in anterior lens surface curvature was related to the variation of coma.

摘要

目的

本研究利用光学相干断层扫描和夏克 - 哈特曼波前传感器研究高阶像差(HOA)分量的眼前部解剖学起源。

方法

构建定制系统以同时采集眼波前像差和眼前部生物特征图像。对30名年轻受试者的放松状态、2屈光度(D)和4屈光度调节状态进行重复测量。使用定制软件校正光学畸变并从图像中测量生物特征参数。

结果

在2 - D调节期间眼前部生物特征发生变化,其中中央晶状体厚度、巩膜突后1 mm处的睫状肌厚度(CMT1)以及睫状肌厚度最大值显著增加,而前房深度、CMT3、晶状体前表面曲率半径(RAL)和晶状体后表面曲率半径(RPL)显著减小。4 - D调节期间眼前部参数的变化与2 - D调节时相似。({\rm{Z}}_4^0)在2 - D调节期间显著降低,({\rm{Z}}_3^{ - 1})、({\rm{Z}}_3^1)、({\rm{Z}}_4^0)和({\rm{Z}}_6^0)在4 - D调节期间向负值偏移。({\rm{Z}}_4^0)的变化与CMT1的变化呈负相关,({\rm{Z}}_3^1)的负变化与RAL和CMT1的变化相关。

结论

在阶梯式控制调节刺激期间HOA分量发生改变。在逐步调节过程中睫状肌首先收缩,这可能直接导致球差(SA)降低。随后晶状体形态发生改变,晶状体前表面曲率的变化与彗差的变化有关。

https://cdn.ncbi.nlm.nih.gov/pmc/blobs/97aa/5667401/18f8fe9588c8/i1552-5783-58-13-5628-f01.jpg

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