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China Multi IR Long-Pass Filter (LP) - High-Performance Optical Solutions from Trusted Suppliers and Factory
| Name | 5% CUT ON | 50% CUT ON | HT (nm) | Tmin | Tavg | Size (mm) | Sub | Tmax | Tavg | 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 |
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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)
Q1: What are Longpass (LP) filters used for?
Longpass filters are designed to transmit wavelengths longer than the cut-on wavelength while blocking shorter wavelengths. They are commonly used in Raman spectroscopy, fluorescence microscopy, and various industrial or scientific imaging systems.
Q2: What substrates are available for these optical filters?
Depending on the specific cut-on wavelength and application requirements, we offer filters fabricated on premium substrates such as Sapphire, Quartz, White Glass, Germanium (Ge), and Zinc Selenide (ZnSe).
Q3: Can I customize the size and dimensions of the filters?
Yes, we support custom dimensional configurations ranging from Φ0.1 mm to 300 mm to fit your specific optical assembly and housing requirements.
Q4: What does the "50% Cut-on" specification mean?
The 50% cut-on wavelength represents the exact point where the transmission value of the filter reaches 50% of its peak transmission, defining the transition threshold between the blocking band and the transmission band.
Q5: How do I request a quote for non-stock items?
If our current stock list does not meet your specifications, you can click the "contact us" link on our page to submit an inquiry. Our technical team will assist you with custom manufacturing options.








