Technical Guide

Single-Point Diamond Turning of Alvarez Freeform Lenses

Alvarez lenses utilize two complementary non-rotationally symmetric cubic polynomial phase plates to achieve continuous variable focal length tuning through minute lateral displacements ($\pm 1 ext{ to }3 ext{ mm}$), eliminating bulky axial motorized zoom mechanisms in compact AR/VR optics and endoscopic imaging systems.

1. Mathematical Formulation of the Alvarez Surface

The sagittal surface profile $z(x,y)$ of a single Alvarez freeform element is expressed as a cubic polynomial:

$$z(x,y) = A \left( x y^2 + rac{1}{3} x^3 ight) + D x$$
Where:
• $A$ = Cubic coefficient governing surface power scaling ($ ext{mm}^{-2}$)
• $D$ = Linear tilt term to maintain optical thickness bounds
• $x, y$ = Cartesian coordinates across the lens aperture

When two identical elements are placed in contact with opposite orientations and shifted by $+\delta$ and $-\delta$ along the $x$-axis, the combined optical thickness creates a spherical wavefront modulation yielding variable optical power $\Delta P$:

$$\Delta P = 4 A \cdot \delta \cdot (n - 1)$$

2. Fast Tool Servo (FTS) Dynamic Kinematics

Because the Alvarez surface is non-rotationally symmetric, diamond turning requires a high-bandwidth Fast Tool Servo (FTS) or Slow Slide Servo (SSS) actuated by piezoelectric stacks or voice coils oscillating synchronously with spindle rotation ($ heta$).

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