

The LBTEK Polymer True Zero-Order Half-Wave Plate is based on N-BK7 glass substrate and liquid crystal polymer birefringent material. By precisely controlling the thickness of the liquid crystal polymer film, the phase difference of π between the o-light (perpendicular to the optical axis) and e-rlight (parallel to the optical axis) can be accurately controlled when passing through the crystal, thereby achieving a λ/2 retardation. The polymer true zero-order half-wave plate with mechanical housing is installed in standard SM05, SM1, and SM2 lens tubes. The tube surface is engraved with the product model and relevant parameters, and the top of the tube is marked with a fast axis indicator line for easy identification and use by customers.

The LBTEK Polymer True Zero-Order Waveplates are often mounted on rotation mounts.
Product Model | Clear Aperture | Operating Wavelength | Latency | Unit Price | Compare | Lead Time | ||
|---|---|---|---|---|---|---|---|---|
| HWP13-405A-M | Ø10 mm | 405 nm | λ/2 | $59.36 | today | Add Cart | ||
| HWP13-520A-M | Ø10 mm | 520 nm | λ/2 | $59.36 | today | Add Cart | ||
| HWP13-532A-M | Ø10 mm | 532 nm | λ/2 | $59.36 | today | Add Cart | ||
| HWP13-633A-M | Ø10 mm | 633 nm | λ/2 | $59.36 | today | Add Cart | ||
| HWP13-780A-M | Ø10 mm | 780 nm | λ/2 | $59.36 | today | Add Cart | ||
| HWP13-795A-M | Ø10 mm | 795 nm | λ/2 | $59.36 | today | Add Cart | ||
| HWP13-850A-M | Ø10 mm | 850 nm | λ/2 | $59.36 | today | Add Cart | ||
| HWP13-1064A-M | Ø10 mm | 1064 nm | λ/2 | $59.36 | 4 weeks | Add Cart | ||
| HWP13-1310A-M | Ø10 mm | 1310 nm | λ/2 | $59.36 | today | Add Cart | ||
| HWP13-1550A-M | Ø10 mm | 1550 nm | λ/2 | $59.36 | today | Add Cart | ||
| HWP25-405A-M | Ø21.5 mm | 405 nm | λ/2 | $71.91 | today | Add Cart | ||
| HWP25-442A-M | Ø21.5 mm | 442 nm | λ/2 | $71.91 | today | Add Cart | ||
| HWP25-488A-M | Ø21.5 mm | 488 nm | λ/2 | $71.91 | today | Add Cart | ||
| HWP25-520A-M | Ø21.5 mm | 520 nm | λ/2 | $71.91 | today | Add Cart | ||
| HWP25-532A-M | Ø21.5 mm | 532 nm | λ/2 | $71.91 | today | Add Cart | ||
| HWP25-633A-M | Ø21.5 mm | 633 nm | λ/2 | $71.91 | today | Add Cart | ||
| HWP25-670A-M | Ø21.5 mm | 670 nm | λ/2 | $71.91 | today | Add Cart | ||
| HWP25-780A-M | Ø21.5 mm | 780 nm | λ/2 | $71.91 | today | Add Cart | ||
| HWP25-795A-M | Ø21.5 mm | 795 nm | λ/2 | $71.91 | today | Add Cart | ||
| HWP25-800A-M | Ø21.5 mm | 800 nm | λ/2 | $71.91 | today | Add Cart | ||
| HWP25-808A-M | Ø21.5 mm | 808 nm | λ/2 | $71.91 | today | Add Cart | ||
| HWP25-850A-M | Ø21.5 mm | 850 nm | λ/2 | $71.91 | today | Add Cart | ||
| HWP25-905A-M | Ø21.5 mm | 905 nm | λ/2 | $71.91 | today | Add Cart | ||
| HWP25-980A-M | Ø21.5 mm | 980 nm | λ/2 | $71.91 | today | Add Cart | ||
| HWP25-1030A-M | Ø21.5 mm | 1030 nm | λ/2 | $71.91 | today | Add Cart | ||
| HWP25-1053A-M | Ø21.5 mm | 1053 nm | λ/2 | $71.91 | 4 weeks | Add Cart | ||
| HWP25-1064A-M | Ø21.5 mm | 1064 nm | λ/2 | $71.91 | today | Add Cart | ||
| HWP25-1310A-M | Ø21.5 mm | 1310 nm | λ/2 | $71.91 | 4 weeks | Add Cart | ||
| HWP25-1550A-M | Ø21.5 mm | 1550 nm | λ/2 | $71.91 | today | Add Cart | ||
| HWP51-405A-M | Ø45 mm | 405 nm | λ/2 | $134.27 | 4 weeks | Add Cart | ||
| HWP51-520A-M | Ø45 mm | 520 nm | λ/2 | $134.27 | 4 weeks | Add Cart | ||
| HWP51-532A-M | Ø45 mm | 532 nm | λ/2 | $134.27 | today | Add Cart | ||
| HWP51-633A-M | Ø45 mm | 633 nm | λ/2 | $134.27 | 4 weeks | Add Cart | ||
| HWP51-780A-M | Ø45 mm | 780 nm | λ/2 | $134.27 | today | Add Cart | ||
| HWP51-795A-M | Ø45 mm | 795 nm | λ/2 | $134.27 | today | Add Cart | ||
| HWP51-850A-M | Ø45 mm | 850 nm | λ/2 | $134.27 | 4 weeks | Add Cart | ||
| HWP51-1064A-M | Ø45 mm | 1064 nm | λ/2 | $134.27 | 4 weeks | Add Cart | ||
| HWP51-1310A-M | Ø45 mm | 1310 nm | λ/2 | $134.27 | 4 weeks | Add Cart | ||
| HWP51-1550A-M | Ø45 mm | 1550 nm | λ/2 | $134.27 | today | Add Cart |

LBTEK Polymer True Zero-Order Half-Wave Plates are based on N-BK7 glass substrates and liquid crystal polymer birefringent materials. By precisely controlling the thickness of the liquid crystal polymer film, the phase difference of π between the o-light (perpendicular to the optical axis) and e-light (parallel to the optical axis) as they pass through the crystal can be accurately controlled, thereby achieving a λ/2 retardation. For polymer true zero-order half-wave plates without mechanical housings, the Ø25.4 mm and Ø50.8 mm waveplates feature a D-shaped chamfer design with the fast axis parallel to the chamfer, while the Ø12.7 mm waveplate has no chamfer and instead adopts a side marking to indicate the fast axis direction, facilitating quick identification and use by customers.

The LBTEK Polymer True Zero-Order Waveplates are often mounted on rotation mounts.
Product Model | Clear Aperture | Operating Wavelength | Latency | Unit Price | Compare | Lead Time | ||
|---|---|---|---|---|---|---|---|---|
| HWP13-405A | Ø10 mm | 405 nm | λ/2 | $53.47 | today | Add Cart | ||
| HWP13-520A | Ø10 mm | 520 nm | λ/2 | $53.47 | today | Add Cart | ||
| HWP13-532A | Ø10 mm | 532 nm | λ/2 | $53.47 | today | Add Cart | ||
| HWP13-633A | Ø10 mm | 633 nm | λ/2 | $53.47 | 4 weeks | Add Cart | ||
| HWP13-780A | Ø10 mm | 780 nm | λ/2 | $53.47 | today | Add Cart | ||
| HWP13-795A | Ø10 mm | 795 nm | λ/2 | $53.47 | 4 weeks | Add Cart | ||
| HWP13-850A | Ø10 mm | 850 nm | λ/2 | $53.47 | today | Add Cart | ||
| HWP13-1064A | Ø10 mm | 1064 nm | λ/2 | $53.47 | today | Add Cart | ||
| HWP13-1310A | Ø10 mm | 1310 nm | λ/2 | $53.47 | today | Add Cart | ||
| HWP13-1550A | Ø10 mm | 1550 nm | λ/2 | $53.47 | today | Add Cart | ||
| HWP25-488A | Ø21.5 mm | 488 nm | λ/2 | $63.02 | 4 weeks | Add Cart | ||
| HWP25-442A | Ø21.5 mm | 442 nm | λ/2 | $63.02 | today | Add Cart | ||
| HWP25-405A | Ø21.5 mm | 405 nm | λ/2 | $63.02 | today | Add Cart | ||
| HWP25-520A | Ø21.5 mm | 520 nm | λ/2 | $59.10 | today | Add Cart | ||
| HWP25-532A | Ø21.5 mm | 532 nm | λ/2 | $63.02 | today | Add Cart | ||
| HWP25-670A | Ø21.5 mm | 670 nm | λ/2 | $63.02 | 4 weeks | Add Cart | ||
| HWP25-633A | Ø21.5 mm | 633 nm | λ/2 | $63.02 | today | Add Cart | ||
| HWP25-780A | Ø21.5 mm | 780 nm | λ/2 | $63.02 | today | Add Cart | ||
| HWP25-795A | Ø21.5 mm | 795 nm | λ/2 | $59.36 | today | Add Cart | ||
| HWP25-808A | Ø21.5 mm | 808 nm | λ/2 | $63.02 | today | Add Cart | ||
| HWP25-800A | Ø21.5 mm | 800 nm | λ/2 | $63.02 | 4 weeks | Add Cart | ||
| HWP25-850A | Ø21.5 mm | 850 nm | λ/2 | $63.02 | today | Add Cart | ||
| HWP25-1053A | Ø21.5 mm | 1053 nm | λ/2 | $63.02 | 4 weeks | Add Cart | ||
| HWP25-1030A | Ø21.5 mm | 1030 nm | λ/2 | $63.02 | today | Add Cart | ||
| HWP25-980A | Ø21.5 mm | 980 nm | λ/2 | $63.02 | 4 weeks | Add Cart | ||
| HWP25-905A | Ø21.5 mm | 905 nm | λ/2 | $63.02 | 4 weeks | Add Cart | ||
| HWP25-1064A | Ø21.5 mm | 1064 nm | λ/2 | $63.02 | today | Add Cart | ||
| HWP25-1310A | Ø21.5 mm | 1310 nm | λ/2 | $63.02 | today | Add Cart | ||
| HWP25-1550A | Ø21.5 mm | 1550 nm | λ/2 | $63.02 | 4 weeks | Add Cart | ||
| HWP51-405A | Ø45 mm | 405 nm | λ/2 | $124.07 | 4 weeks | Add Cart | ||
| HWP51-520A | Ø45 mm | 520 nm | λ/2 | $124.07 | 4 weeks | Add Cart | ||
| HWP51-532A | Ø45 mm | 532 nm | λ/2 | $124.07 | today | Add Cart | ||
| HWP51-633A | Ø45 mm | 633 nm | λ/2 | $124.07 | 4 weeks | Add Cart | ||
| HWP51-780A | Ø45 mm | 780 nm | λ/2 | $124.07 | 4 weeks | Add Cart | ||
| HWP51-795A | Ø45 mm | 795 nm | λ/2 | $124.07 | 4 weeks | Add Cart | ||
| HWP51-850A | Ø45 mm | 850 nm | λ/2 | $124.07 | today | Add Cart | ||
| HWP51-1064A | Ø45 mm | 1064 nm | λ/2 | $124.07 | 4 weeks | Add Cart | ||
| HWP51-1310A | Ø45 mm | 1310 nm | λ/2 | $124.07 | 4 weeks | Add Cart | ||
| HWP51-1550A | Ø45 mm | 1550 nm | λ/2 | $124.07 | today | Add Cart |