Low Loss Optical Components (340 – 3000 nm)
HR Mirrors
- R > 99.99 % in the VIS and NIR spectral range
- R > 99.999 % was demonstrated at several wavelengths between 1000 – 1600 nm
- Mirrors with defined transmittance (e.g. T = 0.002 %)
- For Cavity ring-down time spectroscopy, it is favorable to adjust the transmittance to the value of the scattering and absorption losses (T = S + A)
- All mirrors for CRD experiments are delivered with rear side AR coating. Wedged substrates on request
- Plane and spherically curved Fused Silica substrates
- Premium polish, RMS roughness: ≤ 0.15 nm (see Table 2 on page Standard Quality Substrates)
- Surface imperfection tolerance: 5/ 1 × 0.010 (ISO 10110) for Ø 25 mm
- Coating technique: magnetron sputtering, ion beam sputtering
- Optical parameters are stable against changes in temperature and humidity
- Attractive prices for small and medium numbers of substrates per coating run
- Very high reflectance values for complex coating designs, e.g. GTI laser mirrors with R > 99.95 % (see page Gires-Tournois-Interferometer (GTI) Mirrors (600 – 1600 nm) f.)
- Vacuum packaging or packaging under nitrogen cover gas in dust free boxes
- Designed for vacuum application
Substrate: Fused Silica plano-concave ROC = 1000 mm polished at LAYERTEC
Coating: PR (0°, 1030 nm) > 99.9985 % + T (0°, 1030 nm) ≈ 5 ppm (magnetron sputtering)
CPI-absorption measurement A (0°, 1030 nm) < 1 ppm; S (0°, 1030 nm) = 1 – T – R – A ≈ 4 ppm
Important note for an order
The following balance equation applies:
1 = Reflectance R + Transmittance T + Losses L with
L = Absorbance A + Scattered Light S
1 = Reflectance R + Transmittance T + Losses L with
L = Absorbance A + Scattered Light S
Please specify the transmittance required for the application. LAYERTEC has dealt with the reduction of optical losses for many years and knows about the typical values of absorption and scattering in the NUV, VIS and NIR spectral range. Based on this experience LAYERTEC calculates the achievable reflectance from:
R = 1 - T - V
e.g.
Customer: T (0°, 633 nm) = 10 ppm (±5 ppm)
LAYERTEC: V (0°, 633 nm) < 25 ppm (typically < 20 ppm)
Specification: R (0°, 633 nm) > 99.996 %
Customer: T (0°, 633 nm) = 10 ppm (±5 ppm)
LAYERTEC: V (0°, 633 nm) < 25 ppm (typically < 20 ppm)
Specification: R (0°, 633 nm) > 99.996 %
Customer: T (0°, 390 nm) = 100 ppm (±20 ppm)
LAYERTEC: V (0°, 390 nm) < 50 ppm
Specification: R (0°, 390 nm) > 99.983 %
LAYERTEC: V (0°, 390 nm) < 50 ppm
Specification: R (0°, 390 nm) > 99.983 %
Cavity ring-down time measurements and reference data
Wavelength | Rmax | T | Loss L = 1 - R - T | Measured at |
---|---|---|---|---|
248 nm | 99.87 % | 0.00024 % | 1300 ppm | LAYERTEC GmbH |
266 nm | 99.941 % | 0.0031 % | 560 ppm | LAYERTEC GmbH |
355 nm | 99.983 % | 0.0105 % | 65 ppm | LAYERTEC GmbH |
380 nm | 99.988 % | 0.007 % | 50 ppm | LAYERTEC GmbH |
550 nm | 99.9977 % | 0.00039 % | 19 ppm | LAYERTEC GmbH |
633 nm | 99.992 % | 0.006 % | 20 ppm | Westsächsische Hochschule Zwickau, Germany |
660 nm | 99.992 % | 0.006 % | 20 ppm | Heidelberg University, Germany |
689 nm | 99.9982 % | 0.0005 % | 13 ppm | LAYERTEC GmbH |
798 nm | 99.995 % | 0.003 % | 10 ppm | LAYERTEC GmbH |
840 nm | 99.9988 % | 0.0002 % | 10 ppm | LAYERTEC GmbH |
1030 nm | 99.9980 % | 0.0012 % | 8 ppm | LAYERTEC GmbH |
1150 nm | 99.9994 % | 0.00035 % | 2.5 ppm | LAYERTEC GmbH |
1392 nm | 99.9985 % | 0.0007 % | 8 ppm | TIGER OPTICS, USA (R measurement) LAYERTEC GmbH (T measurement) |
1550 nm | 99.999 % | 0.0002 % | 8 ppm | IPHT Jena, Germany |
2350 nm | 99.995 % | 0.002 % | 30 ppm | University of Grenoble, France |
3250 nm | 99.928 % | 0.012 % | 600 ppm | University of Grenoble, France |
4000 nm | 99.9 % | — | — | Bielefeld University, Germany |
PR (0°, 630 – 710 nm + 1030 – 1110 nm) = 99.98 (±0.015) % + PR (0°, 1550 – 1565 nm) = 99.965 (±0.025) %;
T (0°, 630 – 710 + 1030 – 1110 + 1550 – 1565 nm) ≈ 100 … 400 ppm;
measured losses: (0°, 660 nm) ≈ 140 ppm; L (0°, 1070 nm) ≈ 10 ppm; L (0°, 1555 nm) ≈ 10 ppm
Notes
- Losses = absorption + scattered light; with absorption << scattered light
- Losses = f (polished surface, wavelength, coating technology, design and defects)
- E.g. scattered light of a plane or curved surface < scattered light of a concave surface combined with a plane chamfer for bonding
The development of low loss optics is highly dynamic. The tabular values are therefore guidelines for specific customer requests.
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