Gatinel Damien, Malet Jacques, Hoang-Xuan Thanh, Azar Dimitri T
Ophthalmology Service, Bichat Hospital, Rothschild Foundation, Paris VII University, Paris, France.
Invest Ophthalmol Vis Sci. 2002 Apr;43(4):941-8.
To determine the ablation depths of customized myopic excimer laser photoablations performed to change corneal asphericity after laser in situ keratomileusis (LASIK) and photorefractive keratectomy (PRK).
A mathematical model of aspheric myopic corneal laser surgery was generated. The initial corneal surface was modeled as a conic section of apical radius R(1) and asphericity Q(1). The final corneal surface was modeled as a conic section of apical R(2) and asphericity Q(2), where R(2) was calculated from the paraxial optical formula for a given treatment magnitude (D), and Q(2) was the intended final asphericity. The aspheric profile of ablation was defined as the difference between the initial and final corneal profiles for a given optical zone diameter (S), and the maximal depth of ablation was calculated from these equations. Using the Taylor series expansion, an equation was derived that allowed the approximation of the central depth of ablation (t(0)) for various magnitudes of treatment, optical zone diameters, and asphericity. In addition to the Munnerlyn term (M), incorporating Munnerlyn's approximation (-D small middle dot S(2)/3), the equation included an asphericity term (A) and a change of asphericity term (Delta). This formula (t(0) = M + A + Delta) was used to predict the maximal depth of ablation and the limits of customized asphericity treatments in several theoretical situations.
When the initial and final asphericities were identical (no intended change in asphericity; Q(1) = Q(2); Delta = 0), the maximal depth of ablation (t(0) = M + A) increased linearly with the asphericity Q(1). To achieve a more prolate final asphericity (Q(2) < Q(1); dQ < 0; Delta > 0), the maximal depth of ablation (M + A + Delta) was increased. For treatments in which Q(2) was intended to be more oblate than Q(1) (Q(2) > Q(1); dQ > 0; Delta < 0), the maximal depth of ablation was reduced. These effects sharply increased with increasing diameters of the optical zone(s). Similarly, in the case of PRK, the differential increase in epithelial thickness in the center of the cornea compared with the periphery resulted in increased oblateness.
Aspheric profiles of ablation result in varying central depths of ablation. Oblateness of the initial corneal surface, intentional increase in negative asphericity, and enlargement of the optical zone diameter result in deeper central ablations. This may be of clinical importance in planning aspheric profiles of ablation in LASIK procedures to correct spherical aberration without compromising the mechanical integrity of the cornea.
确定在准分子原位角膜磨镶术(LASIK)和准分子激光角膜切削术(PRK)后,为改变角膜非球面性而进行的定制近视性准分子激光光凝的消融深度。
建立了非球面性近视性角膜激光手术的数学模型。初始角膜表面被建模为顶点半径为R(1)和非球面性为Q(1)的圆锥曲线。最终角膜表面被建模为顶点半径为R(2)和非球面性为Q(2)的圆锥曲线,其中R(2)根据给定治疗量(D)的近轴光学公式计算得出,而Q(2)是预期的最终非球面性。消融的非球面轮廓被定义为给定光学区直径(S)下初始和最终角膜轮廓的差值,并且根据这些公式计算出最大消融深度。使用泰勒级数展开,推导得出一个方程,该方程允许近似计算不同治疗量、光学区直径和非球面性下的中心消融深度(t(0))。除了纳入Munnerlyn近似值(-D×S(2)/3)的Munnerlyn项(M)外,该方程还包括一个非球面性项(A)和一个非球面性变化项(Delta)。这个公式(t(0) = M + A + Delta)被用于预测几种理论情况下的最大消融深度和定制非球面性治疗的限度。
当初始和最终非球面性相同时(非球面性无预期变化;Q(1) = Q(2);Delta = 0),最大消融深度(t(0) = M + A)随非球面性Q(1)线性增加。为了实现更扁平的最终非球面性(Q(2) < Q(1);dQ < 0;Delta > 0),最大消融深度(M + A + Delta)增加。对于预期Q(2)比Q(1)更椭圆的治疗(Q(2) > Q(1);dQ > 0;Delta < 0),最大消融深度减小。随着光学区直径的增加,这些效应急剧增强。同样,在PRK的情况下,角膜中心与周边相比上皮厚度的差异增加导致椭圆度增加。
消融的非球面轮廓导致不同的中心消融深度。初始角膜表面的椭圆度、负非球面性的有意增加以及光学区直径的增大导致更深的中心消融。这在规划LASIK手术中的非球面消融轮廓以矫正球差而不损害角膜的机械完整性方面可能具有临床重要性。