The retarders consist of two single plates which are assembled their optical crystal axes in crossed position. The working principle is identical with that of the zero order retarders made from crystal quartz. The advantages of MgF2 are its broader transmission range of 120 nm – 7µm and the lack of optical activity which can be troublesome in applications which require a high degree of polarization.
The thickness of each plate is about 0.8 mm (total thickness approx. 1.6 mm). The wavefront distortion is λ/10 (at λ = 550 nm) and the wedge error is smaller than 2’’. The accuracy of the path difference is ± 2 nm.
The usable spectral range for a single zero-order plate is much smaller than the transmission range and depends on the required accuracy of the retardation. As for the zero order retarders made of quartz crystal the error of the path differnce is smaller than the production tolerance if the wavelengths deviates by less then 4 nm (λ/2 plates) or ±8 nm (λ/4 plates) from the design wavelength. A deviation considerably larger than the production tolerance is acceptable in many applications resulting in a correspondingly broader usable spectral range.
The deviation ΔR of the path difference from the nominal value R (both in nm) due to a temperature change by ΔT (in K) or due to tilt by Δφ (in degrees) can be estimated as follows:
ΔR≈-(4•10-5K-1)•R•ΔT
ΔR≈±(1.5 nm/Grad²)•Δφ²
For λ/2 plate at 633 nm the deviations will be smaller than the production tolerance for a temperature change up to ±160 K order for tilt angles up to ±1.2°.
The plates are delivered without AR coating mounted in a cylindrical holder made of anodized aluminum and engraved with the direction of the fast axis, the path difference and the design wavelength.
Zero order retarders are available either joined by optical contact (cementless) or with air space between the plates (version L). The air spaced version is particularly suited for high power lasers and for applications with strong thermal or mechanical disturbances.
| Aperture | Holder | λ/2 | ||||
| Diameter | Diameter | Length | Ordernr. | Price 1 pc. | Price 2-5 pc. | Price 6-10 pc. |
| 9.5 mm 14.5 mm 19.5 mm 24.5 mm |
25 mm 25 mm 30 mm 40 mm |
10 mm 10 mm 15 mm 15 mm |
RZM 2.10 RZM 2.15 RZM 2.20 RZM 2.25 |
€ 683 € 1023 € 1732 € 2744 |
€ 588 € 878 € 1452 € 2297 |
€ 525 € 781 € 1266 € 1999 |
| Aperture | Holder | λ/4 | ||||
| Diameter | Diameter | Length | Ordernr. | Price 1 pc. | Price 2-5 pc. | Price 6-10 pc. |
| 9.5 mm 14.5 mm 19.5 mm 24.5 mm |
25 mm 25 mm 30 mm 40 mm |
10 mm 10 mm 15 mm 15 mm |
RZM 4.10 RZM 4.15 RZM 4.20 RZM 4.25 |
€ 683 € 1023 € 1732 € 2744 |
€ 588 € 878 € 1452 € 2297 |
€ 525 € 781 € 1266 € 1999 |
| Aperture | Holder | λ/2 | ||||
| Diameter | Diameter | Length | Ordernr. | Price 1 pc. | Price 2-5 pc. | Price 6-10 pc. |
| 9.5 mm 14.5 mm 19.5 mm 24.5 mm |
25 mm 25 mm 30 mm 40 mm |
10 mm 10 mm 15 mm 15 mm |
RZM 2.10L RZM 2.15L RZM 2.20L RZM 2.25L |
€ 755 € 1100 € 1791 € 2820 |
€ 646 € 934 € 1502 € 2360 |
€ 572 € 824 € 1308 € 2054 |
| Aperture | Holder | λ/4 | ||||
| Diameter | Diameter | Length | Ordernr. | Price 1 pc. | Price 2-5 pc. | Price 6-10 pc. |
| 9.5 mm 14.5 mm 19.5 mm 24.5 mm |
25 mm 25 mm 30 mm 40 mm |
10 mm 10 mm 15 mm 15 mm |
RZM 4.10L RZM 4.15L RZM 4.20L RZM 4.25L |
€ 755 € 1100 € 1791 € 2820 |
€ 646 € 934 € 1502 € 2360 |
€ 572 € 824 € 1308 € 2054 |
Please specify required wavelength when ordering.
The prices apply to standard wavelengths according to the following table:
| Standard wavelengths for zero order MgF2 retarders | |||||||
| 157 nm | 193 nm | 532 nm | 633 nm | 1064 nm | 3500 nm | 4750 nm | 6000 nm |