0102030405
China IR Longpass Filter (LP) Suppliers - High-Performance Multi IR Long-Pass Filters from Factory
| Name | 5% CUT ON | 50% CUT ON | HT (nm) | Tmin | Tavg | Size (mm) | Substrate | Tmax | Tavg (Block) | Spectrogram |
|---|---|---|---|---|---|---|---|---|---|---|
| LP1200 | / | 1200 | 1300~4800 | / | ≥80% | Φ0.1~300 | Sapphire | - | <1% | ![]() |
| LP1500 | - | 1500 | 1600~5300 | - | ≥85% | Φ0.1~300 | Sapphire | - | <1% | ![]() |
| LP1600 | / | 1600 | 1650~1700 | / | ≥90% | Φ0.1~300 | Quartz | - | <1% | ![]() |
| / | 1600 | 1650~1660 | / | ≥90% | Φ0.1~300 | White Glass | - | <1% | ![]() |
|
| LP2000 | 1930 | 2000 | 2100~2800 | / | ≥85% | Φ0.1~300 | Sapphire | - | <1% | ![]() |
| LP2400 | / | - | 2400~11100 11100~13300 |
≥80% | / | Φ0.1~300 | Ge | - | <5% | ![]() |
| LP2750 | 2700 | 2750 | 2800~3670 | / | ≥90% | Φ0.1~300 | Quartz | - | <1% | ![]() |
| LP2800 | - | 2800 | 2950~5100 | / | ≥90% | Φ0.1~300 | ZnSe | - | <1% | ![]() |
| LP2900 | - | 2900 | 3050~5100 | / | ≥90% | Φ0.1~300 | ZnSe | - | <1% | ![]() |
| LP3200 | 3320 | 3400 | 3480~5350 | / | ≥90% | Φ0.1~300 | Ge | - | <1% | ![]() |
| LP3300 | 3200 | 3300 | 3400~5000 | / | ≥90% | Φ0.1~300 | Sapphire | - | <1% | ![]() |
| LP3450 | / | 3450 | 3700~5000 | / | ≥93% | Φ0.1~300 | Ge | - | <1% | ![]() |
| LP3500 | 3600 | 3670 | 3800~5600 | / | ≥90% | Φ0.1~300 | Ge | <1% | - | ![]() |
| LP3550 | / | 3550 | 3800~5500 | / | ≥90% | Φ0.1~300 | Ge | - | <1% | ![]() |
| LP3600 | / | 3600 | 3960~4800 | / | ≥90% | Φ0.1~300 | Ge | - | <1% | ![]() |
| LP3650 | 3540 | 3620 | 3700~5200 | / | ≥85% | Φ0.1~300 | Sapphire | - | <1% | ![]() |
| LP3700 | / | 3700 | 4000~5500 | / | ≥90% | Φ0.1~300 | Ge | - | <1% | ![]() |
| LP3730 | 0.1 | 3730 | 4400~4900 | / | ≥90% | Φ0.1~300 | Ge | - | <1% | ![]() |
| LP3750 | - | 3750 | 3800~4900 | / | ≥90% | Φ0.1~300 | Ge | - | <1% | ![]() |
| LP3760 | / | 3760 | 3960~4800 | / | ≥90% | Φ0.1~300 | Ge | - | <1% | ![]() |
| LP3800 | / | 3800 | 4200~5500 | / | ≥90% | Φ0.1~300 | Ge | - | <1% | ![]() |
| LP3850 | / | 3850 | 4000~5000 | / | ≥90% | Φ0.1~300 | Ge | - | <1% | ![]() |
| LP4000 | 3850 | 4000 | 4100~5100 | / | ≥90% | Φ0.1~300 | Ge | - | <1% | ![]() |
| LP4250 | - | - | 4350~5000 | / | ≥85% | Φ0.1~300 | Ge | - | <1% | ![]() |
| LP4730 | - | 4730 | 4900~5150 | / | ≥80% | Φ0.1~300 | Sapphire | - | <1% | ![]() |
| LP5500 | 5500 | / | 7500~13500 | / | ≥72% | Φ0.1~300 | Sapphire | - | <1% | ![]() |
| LP6100 | / | 6100 | 6300~12600 | / | ≥90% | Φ0.1~300 | Ge | - | <1% | ![]() |
| LP6200 | / | 6200 | 6400~12600 | / | ≥90% | Φ0.1~300 | Ge | - | <1% | ![]() |
| LP6300 | / | 6300 | 6550~14500 | / | ≥90% | Φ0.1~300 | Ge | - | <1% | ![]() |
| LP6400 | / | 6400 | 6500~12600 | / | ≥90% | Φ0.1~300 | Ge | - | <1% | ![]() |
| LP6900 | 6900 | 7030 | 7200~12610 | / | ≥85% | Φ0.1~300 | Ge | - | <1% | ![]() |
| LP6500 | / | 6500 | 6800~11000 | / | ≥85% | Φ0.1~300 | Ge | - | <1% | ![]() |
| LP6750 | / | / | 7000~14000 | / | ≥80% | Φ0.1~300 | ZnSe | - | <1% | ![]() |
| LP7150-A | 7150 | / | 8000~11000 | / | ≥90% | Φ0.1~300 | Ge | 20% | <5% | ![]() |
| LP7150-B | 7150 | / | 8000~12000 | / | ≥80% | Φ0.1~300 | Ge lens | 15% | <3% | ![]() |
| LP7200 | / | / | 10000~12600 | / | ≥90% | Φ0.1~300 | Ge | 10% | <1% | ![]() |
| LP7300 | 7420 | / | 8000~11000 | / | ≥90% | Φ0.1~300 | Ge | - | <1% | ![]() |
| LP7400 | / | 7400 | 8000~14000 | / | ≥80% | Φ0.1~300 | Ge lens | - | <1% | ![]() |
| LP7500 | / | / | 8400~12500 | / | ≥90% | Φ0.1~300 | Ge | - | <1% | ![]() |
| LP7675 | - | 7675 | 8000~14000 | / | ≥90% | Φ0.1~300 | Ge | - | <1% | ![]() |
| LP7700 | / | 7700 | 8000~11000 | / | ≥90% | Φ0.1~300 | Ge | - | <1% | ![]() |
| LP7730 | 7730 | / | 8000~14000 | / | ≥80% | Φ0.1~300 | Ge wafer | - | <1% | ![]() |
| LP7750 | - | 7750 | 8100~11000 | / | ≥90% | Φ0.1~300 | Ge | - | <1% | ![]() |
| LP7800 | / | 7800 | 8100~11000 | / | ≥90% | Φ0.1~300 | Ge | - | <1% | ![]() |
| LP7850 | / | 7850 | 8000~11000 | / | ≥85% | Φ0.1~300 | Ge | - | <1% | ![]() |
| LP7900 | / | 7900 | 8200~11000 | / | ≥90% | Φ0.1~300 | Ge | - | <1% | ![]() |
| LP7925 | / | 7925 | 8100~12600 | / | ≥90% | Φ0.1~300 | Ge | - | <1% | ![]() |
| LP7950 | / | 7950 | 8050~14000 | / | ≥85% | Φ0.1~300 | Ge | - | <1% | ![]() |
| LP8000 | / | 8000 | 8150~12000 | / | ≥85% | Φ0.1~300 | Ge | - | <1% | ![]() |
| LP8100 | / | 8100 | 8150~12000 | / | ≥85% | Φ0.1~300 | Ge | - | <1% | ![]() |
| LP8200 | 8200 | / | 9000~14000 | / | ≥80% | Φ0.1~300 | Ge wafer | - | <1% | ![]() |
| LP8400 | 8400 | / | 8800~15000 | / | ≥90% | Φ0.1~300 | ZnSe | - | <1% | ![]() |
| LP9000 | - | 9000 | 9500~12500 | / | ≥90% | Φ0.1~300 | Ge | - | <1% | ![]() |
| LP9700 | 9700 | - | 10100~15000 | / | ≥90% | Φ0.1~300 | ZnSe | - | <1% | ![]() |
| LP9800 | / | 9800 | 10000~16300 | / | ≥90% | Φ0.1~300 | ZnSe | - | <1% | ![]() |
| LP9900 | / | 9900 | 10000~16300 | / | ≥85% | Φ0.1~300 | ZnSe | - | <1% | ![]() |
| LP10000 | / | 10000 | 10150~14300 | / | ≥90% | Φ0.1~300 | ZnSe | - | <1% | ![]() |
| LP10015 | / | 10015 | 10450~14500 | / | ≥85% | Φ0.1~300 | Ge | - | <1% | ![]() |
| LP10080 | / | 10080 | 10180~13500 | / | ≥85% | Φ0.1~300 | Ge | 3% | <1% | ![]() |
| LP10100 | / | 10100 | 10150~14300 | / | ≥90% | Φ0.1~300 | ZnSe | - | <1% | ![]() |
| LP10200 | / | 10200 | 10500~14000 | / | ≥85% | Φ0.1~300 | Ge | 3% | <1% | ![]() |
| LP10300 | / | 10100 | 10500~13000 | / | ≥85% | Φ0.1~300 | Ge | 3% | <1% | ![]() |
| LP10400 | / | 10325 | 10500~15000 | / | ≥90% | Φ0.1~300 | ZnSe | - | <1% | ![]() |
| LP10500 | / | 10500 | 10700~15000 | / | ≥85% | Φ0.1~300 | ZnSe | - | <1% | ![]() |
| LP10600 | / | 10600 | 11000~14000 | / | ≥80% | Φ0.1~300 | Ge | 5% | <1% | ![]() |
| LP10840 | / | 10840 | 10940~13500 | / | ≥85% | Φ0.1~300 | Ge | - | <1% | ![]() |
| LP10900 | / | 10900 | 11200~15400 | / | ≥80% | Φ0.1~300 | Ge | - | <1% | ![]() |
| LP11050 | / | 11050 | 11200~15400 | / | ≥80% | Φ0.1~300 | Ge | - | <1% | ![]() |
| LP11190 | / | 11190 | 11500~15700 | / | ≥80% | Φ0.1~300 | Ge | - | <1% | ![]() |
| LP11400 | / | 11400 | 11600~12250 | / | ≥90% | Φ0.1~300 | Ge | - | <1% | ![]() |
| LP11600 | / | 11600 | 11800~12200 | / | ≥85% | Φ0.1~300 | Ge | - | <1% | ![]() |
| LP11700 | / | 11700 | 11900~12300 | / | ≥80% | Φ0.1~300 | Ge | - | <1% | ![]() |
| LP11900 | / | 11900 | 12100~12500 | / | ≥75% | Φ0.1~300 | Ge | - | <1% | ![]() |
The above list shows our current stock items.
If you don't see what you are looking for, please contact us.
Frequently Asked Questions (FAQ)
Q: What is the function of a Longpass (LP) optical filter?
A Longpass filter is designed to transmit wavelengths longer than the designated cut-on wavelength while blocking (reflecting or absorbing) shorter wavelengths across UV, Visible, SWIR, MWIR, or LWIR spectral bands.
Q: What substrate materials are available for these longpass filters?
Our longpass filters utilize optimized optical substrate materials depending on wavelength ranges, including Germanium (Ge), Sapphire, Zinc Selenide (ZnSe), Quartz, and Optical White Glass to achieve superior transmittance and thermal stability.
Q: What is the difference between 5% Cut-On and 50% Cut-On points?
The 5% cut-on point indicates the transition wavelength where transmission begins to emerge, whereas the 50% cut-on wavelength is the standard reference point representing the transition threshold between blocking and high transmission bands.
Q: Can custom sizes, shapes, or optical coatings be customized?
Yes, we support custom dimensional manufacturing from Φ0.1 mm to 300 mm, customized circular/rectangular dimensions, custom edge finishes, and application-specific hard thin-film coatings tailored to your project requirements.
Q: What typical applications use infrared longpass filters?
These filters are widely deployed in thermal imaging devices, FTIR spectroscopy, gas detection systems, environmental monitoring, IR laser instruments, and security defense optics.
Q: How do I request a quote for non-standard filter specifications?
Simply click the inquiry contact link in the notification box above or reach out with your specific cut-on wavelength, substrate preference, dimensions, and quantity for a direct technical consultation and quotation.








