Touzeau O, Gaujoux T, Costantini E, Borderie V, Laroche L
Institut de la Vision, Inserm, Centre Hospitalier National d'Ophtalmologie des Quinze-Vingts, Paris, France.
J Fr Ophtalmol. 2010 Jan;33(1):56-71. doi: 10.1016/j.jfo.2009.11.015. Epub 2010 Jan 6.
Refraction can be expressed by four polar notations which correspond to four different combinations of spherical or cylindrical lenses. Conventional expressions of refraction (plus and minus cylinder notation) are described by sphere, cylinder, and axis. In the plus cylinder notation, the axis visualizes the most powerful meridian. The axis usually corresponds to the bow tie axis in curvature maps. Plus cylinder notation is also valuable for all relaxing procedures (i.e., selective suture ablation, arcuate keratotomy, etc.). In the cross-cylinder notation, two orthogonal cylinders can describe (without the sphere component) the actual refraction of both the principal meridians. This notation must be made before performing the vertex calculation. Using an association of a Jackson cross-cylinder and a spherical equivalent, refraction can be broken down into two pure components: astigmatism and sphere. All polar notations of refraction may perfectly characterize a single refraction but are not suitable for statistical analysis, which requires nonpolar expression. After doubling the axis, a rectangular projection breaks down the Jackson cross-cylinder, which has a polar axis, into two Jackson cross-cylinders on the 0 degrees /90 degrees and 45 degrees /135 degrees axis. This procedure results in the loss of the directional nature of the data. Refraction can be written in a nonpolar notation by three rectangular coordinates (x,y,z), which can also represent the spherocylinder by one point in a dioptric space. These three independent (orthogonal) variables have a concrete optical significance: a spherical component, a direct/inverse (WTR/ATR) component, and an oblique component of the astigmatism. Finally, nonpolar notations are useful for statistical analysis and graphical representation of refraction.
屈光可以用四种极坐标表示法来表达,它们对应于球面或柱面透镜的四种不同组合。传统的屈光表示法(正负柱镜表示法)由球镜、柱镜和轴位来描述。在正柱镜表示法中,轴位表示最强的子午线。该轴位通常对应于曲率图中的领结轴。正柱镜表示法对于所有放松手术(即选择性缝线消融、弧形角膜切开术等)也很有价值。在交叉柱镜表示法中,两个相互垂直的柱镜(不包括球镜成分)可以描述两个主子午线的实际屈光情况。这种表示法必须在进行顶点计算之前确定。通过将杰克逊交叉柱镜与等效球镜相结合,屈光可以分解为两个纯成分:散光和球镜。所有屈光的极坐标表示法都可以完美地描述单一屈光情况,但不适用于需要非极坐标表示的统计分析。将轴位加倍后,矩形投影将具有极轴的杰克逊交叉柱镜分解为两个分别位于0度/90度和45度/135度轴位的杰克逊交叉柱镜。这一过程导致数据的方向性丢失。屈光可以用三个直角坐标(x,y,z)以非极坐标表示法来书写,这三个坐标也可以在屈光度空间中用一个点来表示球柱镜。这三个独立(相互垂直)的变量具有具体的光学意义:一个球镜成分、一个顺/逆(顺规/逆规)成分以及散光的一个斜向成分。最后,非极坐标表示法对于屈光的统计分析和图形表示很有用。