CN201285457Y - An optical filter - Google Patents
An optical filter Download PDFInfo
- Publication number
- CN201285457Y CN201285457Y CNU2008201237353U CN200820123735U CN201285457Y CN 201285457 Y CN201285457 Y CN 201285457Y CN U2008201237353 U CNU2008201237353 U CN U2008201237353U CN 200820123735 U CN200820123735 U CN 200820123735U CN 201285457 Y CN201285457 Y CN 201285457Y
- Authority
- CN
- China
- Prior art keywords
- wedge
- optical filter
- optical
- shaped
- filter
- Prior art date
- Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
- Expired - Fee Related
Links
- 230000003287 optical effect Effects 0.000 title claims abstract description 31
- 239000000463 material Substances 0.000 claims description 3
- 239000010453 quartz Substances 0.000 claims description 3
- VYPSYNLAJGMNEJ-UHFFFAOYSA-N silicon dioxide Inorganic materials O=[Si]=O VYPSYNLAJGMNEJ-UHFFFAOYSA-N 0.000 claims description 3
- 230000005540 biological transmission Effects 0.000 abstract description 3
- 238000001228 spectrum Methods 0.000 abstract 1
- 230000004907 flux Effects 0.000 description 13
- 238000002834 transmittance Methods 0.000 description 8
- 230000003595 spectral effect Effects 0.000 description 4
- 230000009286 beneficial effect Effects 0.000 description 2
- 238000001514 detection method Methods 0.000 description 2
- 239000011521 glass Substances 0.000 description 2
- 238000010276 construction Methods 0.000 description 1
- 230000001419 dependent effect Effects 0.000 description 1
- 238000010586 diagram Methods 0.000 description 1
- 238000000034 method Methods 0.000 description 1
- 238000012986 modification Methods 0.000 description 1
- 230000004048 modification Effects 0.000 description 1
- 238000012795 verification Methods 0.000 description 1
Images
Landscapes
- Optical Elements Other Than Lenses (AREA)
Abstract
Description
技术领域 technical field
本实用新型涉及一种用于标定各类高精度光学仪器光谱透射比的光学滤光片,具体是一种能适用于不同构造的光学仪器设备的楔形滤光片。The utility model relates to an optical filter for calibrating the spectral transmittance of various high-precision optical instruments, in particular to a wedge-shaped optical filter suitable for optical instruments with different structures.
背景技术 Background technique
目前公知的滤光片的构造是由一片各向同性且厚度一致的玻璃片组成。当以一定的光通量入射到滤光片表面时,由于玻璃片的光谱透射和反射特性,会使得一部分光通量得以透过。透过的这部分光通量和入射的总光通量的比值为该滤光片的透射比。该透射比经高精度标定后就可以应用于对各类光谱透射比仪器的校准和检定。不过,依据该值来标定仪器的透射比读数依赖于标定仪器和被标定仪器的光学构造。当两类仪器构造不一致时,就会导致数据的偏差。其主要原因是:由于部分仪器样品舱窗片平行于被测滤光片,导致样品反射光与窗片之间的多次反射,该部分反射光会再次进入探测光路,导致数值偏大。The structure of the currently known optical filter is composed of a glass sheet with isotropy and uniform thickness. When a certain luminous flux is incident on the surface of the filter, part of the luminous flux will be transmitted due to the spectral transmission and reflection characteristics of the glass sheet. The ratio of the transmitted luminous flux to the incident total luminous flux is the transmittance of the filter. After the transmittance is calibrated with high precision, it can be applied to the calibration and verification of various spectral transmittance instruments. However, calibrating the instrument's transmittance reading against this value is dependent on the optical configuration of the calibrating instrument and the instrument being calibrated. When the construction of the two types of instruments is inconsistent, it will lead to data deviation. The main reason is that part of the instrument sample compartment window is parallel to the measured filter, resulting in multiple reflections between the sample reflected light and the window, and this part of the reflected light will enter the detection optical path again, resulting in a larger value.
实用新型内容 Utility model content
本实用新型的目的就在于提供一种滤光片,以解决现有技术中,由于标定时两类仪器构造不一致而导致数据产生偏差的问题。The purpose of the utility model is to provide an optical filter to solve the problem in the prior art that data deviation occurs due to the inconsistency of the structures of the two types of instruments during calibration.
为实现上述目的,本实用新型的技术方案是采用一种滤光片,所述滤光片由两个楔形滤光片拼接而成,其中所述楔形滤光片的两楔面相对、楔面上镀有膜。In order to achieve the above object, the technical solution of the utility model is to adopt a kind of optical filter, and the optical filter is spliced by two wedge-shaped optical filters, wherein the two wedge surfaces of the wedge-shaped optical filter are opposite, and the wedge surfaces coated with film.
其中,所述两个楔形滤光片拼接成矩形形状。Wherein, the two wedge-shaped filters are spliced into a rectangular shape.
其中,所述滤光片由高纯度石英材料制成。Wherein, the optical filter is made of high-purity quartz material.
本实用新型的优点和有益效果在于,利用该滤光片传递的透射比数值受标定仪器和被检测仪器的光学构造的影响极小。The advantages and beneficial effects of the utility model lie in that the transmittance value transmitted by the optical filter is minimally affected by the optical structure of the calibration instrument and the instrument to be tested.
附图说明 Description of drawings
图1是本实用新型的光路原理图。Fig. 1 is the schematic diagram of the light path of the utility model.
图中:1、楔形滤光片;2、楔形滤光片;3、入射光通量;4、反射光通量;5、出射光通量;a、A面;b、楔面。In the figure: 1. Wedge filter; 2. Wedge filter; 3. Incident luminous flux; 4. Reflected luminous flux; 5. Outgoing luminous flux; a, surface A; b, wedge surface.
具体实施方式 Detailed ways
以下实施例用于说明本实用新型,但不用来限制本实用新型的范围。The following examples are used to illustrate the utility model, but not to limit the scope of the utility model.
如图1所示,本实用新型滤光片由楔形滤光片1和楔形滤光片2拼接成矩形形状而成,以保证能安装在标准滤光片支架上,其中楔形滤光片的两楔面相对,并且在两楔面上镀膜,通过膜的材质和厚度来控制透过该滤光片的光通量。As shown in Figure 1, the filter of the utility model is formed by splicing a wedge-shaped filter 1 and a wedge-
标定时,入射光通量3将依次通过楔形滤光片的两个表面,由于石英的光谱透射比很高,表面反射很低,因此被A面a反射的光通量多次反射后就完全可以忽略,当到达楔面b时,入射光通量3将被分解成反射光通量4和出射光通量5,但在图1中可以看出大量的反射光虽然被反射,却偏离的了光路方向,避免了反射光与窗片之间的多次反射,故不对探测产生任何影响。During calibration, the incident
本实用新型的有益效果是,利用该滤光片传递的透射比数值受标定仪器和被检测仪器的光学构造的影响极小。The beneficial effect of the utility model is that the transmittance value transmitted by the optical filter is minimally affected by the optical structure of the calibration instrument and the instrument to be tested.
以上所述仅是本实用新型的优选实施方式,应当指出,对于本技术领域的普通技术人员来说,在不脱离本实用新型技术原理的前提下,还可以做出若干改进和润饰,这些改进和润饰也应视为本实用新型的保护范围。The above is only the preferred embodiment of the utility model, and it should be pointed out that for those of ordinary skill in the art, without departing from the technical principle of the utility model, some improvements and modifications can also be made. And retouching should also be regarded as the protection scope of the present utility model.
Claims (3)
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
CNU2008201237353U CN201285457Y (en) | 2008-11-14 | 2008-11-14 | An optical filter |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
CNU2008201237353U CN201285457Y (en) | 2008-11-14 | 2008-11-14 | An optical filter |
Publications (1)
Publication Number | Publication Date |
---|---|
CN201285457Y true CN201285457Y (en) | 2009-08-05 |
Family
ID=40950442
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
CNU2008201237353U Expired - Fee Related CN201285457Y (en) | 2008-11-14 | 2008-11-14 | An optical filter |
Country Status (1)
Country | Link |
---|---|
CN (1) | CN201285457Y (en) |
Cited By (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
CN107976734A (en) * | 2017-12-01 | 2018-05-01 | 中国计量科学研究院 | A kind of spectral neutrality filtering apparatus |
-
2008
- 2008-11-14 CN CNU2008201237353U patent/CN201285457Y/en not_active Expired - Fee Related
Cited By (2)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
CN107976734A (en) * | 2017-12-01 | 2018-05-01 | 中国计量科学研究院 | A kind of spectral neutrality filtering apparatus |
CN107976734B (en) * | 2017-12-01 | 2019-12-17 | 中国计量科学研究院 | A spectral neutral filter device |
Similar Documents
Publication | Publication Date | Title |
---|---|---|
CN103018902B (en) | Method for designing optical thin film systems | |
CN105758821B (en) | High-sensitivity metamaterial nano sensing system with ultra-narrow linewidth spectral response | |
CN109029519B (en) | Preparation method of optical fiber F-P cavity sensor with optical fiber tip additionally plated with UV glue film | |
CN103540906B (en) | The thick monitoring method of Optical/crystal comprehensive film | |
CN205027510U (en) | High power optical glass measuring device | |
CN111272683B (en) | Liquid absorption coefficient measuring device and measuring method | |
CN107270822A (en) | The method for determining porous membrane thickness and porosity | |
CN105115701B (en) | The device and method of optical mirror slip transmitance in precise measurement high power laser light environment | |
CN102818788A (en) | Device and method for detecting residual reflection of neodymium glass wrapping | |
CN206920317U (en) | A kind of cuvette for optical measurement | |
CN201285457Y (en) | An optical filter | |
CN102191475A (en) | Film thickness monitoring method for improving film spectral performance | |
CN102680409B (en) | Device and method for measuring brewster angle | |
CN110687052A (en) | A method and system for measuring optical band gap | |
CN102165281B (en) | Apparatus and method for inspecting thin film | |
CN105954823A (en) | Titanium film application and silicon-based optical waveguide with the same | |
CN105911008B (en) | A kind of wavelength indication measurement method of ultraviolet-uisible spectrophotometer | |
CN117607101A (en) | Method, device, equipment and storage medium for measuring film transmittance | |
CN103674892B (en) | A kind of method carrying out monitoring film growth based on total internal reflection polarization phasic difference measurement | |
US9720242B2 (en) | Laser system with partial reflector | |
CN114964331B (en) | Optical fiber multi-parameter detection system and method | |
CN204346900U (en) | A kind of return gas compartment for extraction-type laser gas analyzer | |
CN103697920B (en) | A kind of optical fiber sensor head and based on this sensing head measure the optical fiber sensing system of liquid refractivity and method | |
CN111351576A (en) | Confocal optical path system, confocal polarization measurement method and its application | |
CN203587517U (en) | Capturing device for capturing object image and image detection device |
Legal Events
Date | Code | Title | Description |
---|---|---|---|
C14 | Grant of patent or utility model | ||
GR01 | Patent grant | ||
C17 | Cessation of patent right | ||
CF01 | Termination of patent right due to non-payment of annual fee |
Granted publication date: 20090805 Termination date: 20091214 |