CN203825284U - Weak light collector in three-dimensional space - Google Patents

Weak light collector in three-dimensional space Download PDF

Info

Publication number
CN203825284U
CN203825284U CN201420163606.2U CN201420163606U CN203825284U CN 203825284 U CN203825284 U CN 203825284U CN 201420163606 U CN201420163606 U CN 201420163606U CN 203825284 U CN203825284 U CN 203825284U
Authority
CN
China
Prior art keywords
spherical reflector
ellipsoidal
light
reflection mirror
reflector
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 - Lifetime
Application number
CN201420163606.2U
Other languages
Chinese (zh)
Inventor
欧旭锋
王文鹏
马辉
张幼文
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
Finder Detection Technologies Co ltd
Original Assignee
Zhejiang Convolution Science And Technology Ltd
Priority date (The priority date 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 date listed.)
Filing date
Publication date
Application filed by Zhejiang Convolution Science And Technology Ltd filed Critical Zhejiang Convolution Science And Technology Ltd
Priority to CN201420163606.2U priority Critical patent/CN203825284U/en
Application granted granted Critical
Publication of CN203825284U publication Critical patent/CN203825284U/en
Anticipated expiration legal-status Critical
Expired - Lifetime legal-status Critical Current

Links

Landscapes

  • Investigating, Analyzing Materials By Fluorescence Or Luminescence (AREA)

Abstract

The utility model relates to an optical device and discloses a weak light collector in a three-dimensional space. The weak light collector comprises an ellipsoidal reflection mirror and a spherical reflection mirror. Both the ellipsoidal reflection mirror and the spherical reflection mirror are concave reflection mirrors, and the concave faces of the two mirrors face each other to form a cavity. The center of the spherical reflection mirror coincides with a focus of the oval in the ellipsoidal reflection mirror. The curvature radius of the spherical reflection mirror is equal to the focal length of the oval in the ellipsoidal reflection mirror. According to the weak light collector, a special structure is employed, and weak light such as fluorescence and Raman scattering light of trace substance emitted by a laser beam is effectively and directionally collected in a three-dimensional space range.

Description

Faint light gatherer in three dimensions
Technical field
The utility model relates to a kind of optical devices, has related in particular to faint light gatherer in a kind of three dimensions.
Background technology
Collect and spectrographic detection faint light such as bioluminescence, cell fluorescence, Raman diffused lights current many biology laboratories, Cytology Lab or physics laboratory, carries out the related experiment of probing into for molecular property.For spectrographic detection, fluorescence, the Raman diffused light that first will send molecule have higher collection rate, high as far as possible raising signal to noise ratio (S/N ratio), and particularly, for the very weak spectral line such as fluorescence, Raman diffused light, this point is particularly important.If any fluorescence, Raman diffused light itself very faint, with the naked eye cannot observe, the spectral line detecting is difficult to the signal to noise ratio (S/N ratio) that reaches desirable, affects experiment process, if lack effective faint light gathering-device, result is difficult to reach requirement especially.
To be regarded as pointolite by the gas of laser excitation or small material, its angle of divergence is whole space multistory angle 4 π, current existing faint light gatherer fails to collect efficient to exciting light-fluorescence, Raman diffused light etc. in this 4 π space, but only has solid angle θ.Or 2 θ, realize by adding spherical reflector at the relay optical lens combination back side.The faint light such as fluorescence, Raman diffused light of the trace materials that therefore, laser excitation at present goes out is difficult to effective collection in three dimensions.
Summary of the invention
The faint light such as fluorescence, Raman diffused light of the trace materials that the utility model goes out for laser excitation in prior art obtains directed problem of collecting efficiently within the scope of three dimensions, and faint light gatherer in a kind of three dimensions is provided.
In order to solve the problems of the technologies described above, the utility model is solved by following technical proposals:
Faint light gatherer in three dimensions, comprises ellipsoidal mirror, spherical reflector, and ellipsoidal mirror, spherical reflector are concave mirror, and both concave surfaces are relative, form a cavity; The center of circle of spherical reflector overlaps with a focus oval in ellipsoidal mirror, and the radius-of-curvature of spherical reflector equals 0.6~1.4 times of oval focal length in ellipsoidal mirror.Adopt this special shape, can make pointolite that fluorescence that laser beam inspires or Raman diffused light form the first focus place in ellipsoidal reflector, the namely center of circle of spherical reflector, the light overwhelming majority of upwards being sent by light source substantially converges to the second focus place of ellipsoidal reflector after ellipsoidal reflector reflection, namely the summit of spherical reflector, converges collection.The light that is entered spherical reflector by the downward part of light source directly enters relay optical lens combination through the through hole of spherical reflector, another part reflexes to ellipsoidal reflector through spherical reflector, then converges to ellipsoidal reflector the second focus place away from ellipsoidal reflector after ellipsoidal reflector reflection.
As preferably, the summit of spherical reflector is provided with through hole, and through hole is provided with relay optical lens combination, better the light beam of having collected is carried out to rationally effective utilization.
As preferably, the radius-of-curvature of spherical reflector equals oval focal length in ellipsoidal mirror, makes light that laser beam inspires converge to the second focus place of ellipsoidal reflector, the namely summit of spherical reflector completely.
As preferably, the reflecting surface of ellipsoidal mirror, spherical reflector is all coated with the reflectance coating that light reflectivity is greater than 99%.
Principle of work of the present utility model: add spherical reflector at ellipsoidal reflector correspondence position, form a cavity, and the center of circle of spherical reflector overlaps with the first focus oval in ellipsoidal mirror; The radius-of-curvature of spherical reflector equals 0.6~1.4 times of oval focal length in ellipsoidal mirror, i.e. the summit of spherical reflector and approximate coincidence of the second focus oval in ellipsoidal mirror.The fluorescence inspiring due to laser beam or Raman diffused light, because volume is small, can be considered pointolite.The first focus place of this pointolite in ellipsoidal reflector, the namely center of circle of spherical reflector, the light overwhelming majority of upwards being sent by light source substantially converges to the second focus place of ellipsoidal reflector, the namely summit of spherical reflector after ellipsoidal reflector reflection; The light that is entered spherical reflector by the downward part of light source directly enters relay optical lens combination through the through hole of spherical reflector, another part reflexes to ellipsoidal reflector through spherical reflector, then after ellipsoidal reflector reflection, substantially converges to the second focus place of ellipsoidal reflector.The summit of spherical reflector is provided with through hole, and through hole is provided with relay optical lens combination, better the light beam of having collected is carried out rationally effectively utilizing.
The utility model, owing to having adopted above technical scheme, has significant technique effect:
The utility model adopts special structure, the faint light such as fluorescence, Raman diffused light of the trace materials that laser beam inspires is substantially converged in a bit after elliptical reflector, spherical reflector reflection, it is the summit of spherical reflector, finally all enter relaying photosystem lens combination, make faint light within the scope of three dimensions, obtain directed collection efficiently.
Brief description of the drawings
Fig. 1 is structural representation of the present utility model;
Fig. 2 is exciting light light path 1 in the utility model embodiment 1 inner chamber;
Fig. 3 is exciting light light path 2 in the utility model embodiment 1 inner chamber;
Fig. 4 is exciting light light path 3 in the utility model embodiment 1 inner chamber;
Fig. 5 is exciting light light path schematic diagram in embodiment 2 inner chambers in the utility model;
Fig. 6 is exciting light light path schematic diagram in embodiment 3 inner chambers in the utility model;
The toponym that in accompanying drawing, each number designation refers to is as follows: 1-elliptical reflector, 2-spherical reflector, 3-relay optical lens combination, 4-laser beam.
Embodiment
Below in conjunction with accompanying drawing and embodiment, the utility model is described in further detail.
Embodiment 1
Faint light gatherer in three dimensions, as shown in Figure 1, comprises ellipsoidal mirror 1, spherical reflector 2, and ellipsoidal mirror 2, spherical reflector 2 are concave mirror, and both concave surfaces are relative, form a cavity; The center of circle of spherical reflector 2 overlaps with the first focus oval in ellipsoidal mirror 1, and the radius-of-curvature of spherical reflector 2 equals focal length oval in ellipsoidal mirror 1; The first focus place of the pointolite that the fluorescence that laser beam inspires or Raman diffused light form in ellipsoidal reflector, the namely center of circle of spherical reflector, the light overwhelming majority of upwards being sent by light source converges to the second focus place of ellipsoidal reflector, the namely summit of spherical reflector after ellipsoidal reflector reflection.
The summit place of spherical reflector 2 is provided with through hole, and through hole is provided with relay optical lens combination 3, better the light beam of having collected is carried out rationally effectively utilizing.
The reflecting surface of ellipsoidal mirror 1, spherical reflector 2 is all coated with penetrates the reflectance coating that reflectivity is greater than 99%.
In the collecting chamber that light elliptical reflector and spherical reflector in the utility model form, can be divided into 3 tunnels:
(1) light path 1 as shown in Figure 2: little a part of fluorescence or Raman diffused light that laser beam 4 inspires directly enter relay optical lens combination 3 by the through hole on spherical reflector 2;
(2) light path 2 as shown in Figure 3: a part of fluorescence that laser beam 4 inspires or Raman diffused light are incident to that spherical reflector 2 is rear is reflexed to ellipsoidal reflector 1 by this catoptron, then after being reflected by ellipsoidal reflector 1, it are entered to inject relay optical lens combination 3 by the through hole on spherical reflector 2;
(3) light path 3 as shown in Figure 4: a part of fluorescence or Raman diffused light that laser beam 4 inspires are incident to ellipsoidal reflector 1, by after this catoptron reflection, it being entered to inject relay optical lens combination 3 by the through hole on spherical reflector 2;
The fluorescence that laser beam 4 inspires or Raman diffused light are by above-mentioned 3 kinds of light paths, finally all enter in relay optical lens combination 3, make the faint light such as fluorescence or Raman diffused light in three dimensions, obtain efficient, directed collection, faint light is reasonably and effectively used.
In a word, the foregoing is only preferred embodiment of the present utility model, all equalizations of doing according to the utility model claim change and modify, and all should belong to the covering scope of the utility model patent.
Embodiment 2
As shown in Figure 5, with embodiment 1, difference is, the radius-of-curvature of spherical reflector equals 0.6 times of oval focal length in ellipsoidal mirror.
Embodiment 3
As shown in Figure 6, with embodiment 1, difference is, the radius-of-curvature of spherical reflector equals 1.4 times of oval focal length in ellipsoidal mirror.

Claims (4)

1. faint light gatherer in three dimensions, is characterized in that: comprise ellipsoidal mirror (1), spherical reflector (2), ellipsoidal mirror (2), spherical reflector (2) are concave mirror, and both concave surfaces are relative, form a cavity; A focus oval in the center of circle of spherical reflector (2) and ellipsoidal mirror (1) overlaps, and the radius-of-curvature of spherical reflector (2) equals 0.6~1.4 times of oval focal length in ellipsoidal mirror (1).
2. faint light gatherer in three dimensions according to claim 1, is characterized in that: the summit place of spherical reflector (2) is provided with through hole, and through hole is provided with relay optical lens combination (3).
3. faint light gatherer in three dimensions according to claim 1, is characterized in that: the radius-of-curvature of spherical reflector (2) equals oval focal length in ellipsoidal mirror (1).
4. faint light gatherer in three dimensions according to claim 1, is characterized in that: the reflecting surface of ellipsoidal mirror (1), spherical reflector (2) is all coated with penetrates the reflectance coating that reflectivity is greater than 99%.
CN201420163606.2U 2014-04-04 2014-04-04 Weak light collector in three-dimensional space Expired - Lifetime CN203825284U (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
CN201420163606.2U CN203825284U (en) 2014-04-04 2014-04-04 Weak light collector in three-dimensional space

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
CN201420163606.2U CN203825284U (en) 2014-04-04 2014-04-04 Weak light collector in three-dimensional space

Publications (1)

Publication Number Publication Date
CN203825284U true CN203825284U (en) 2014-09-10

Family

ID=51480765

Family Applications (1)

Application Number Title Priority Date Filing Date
CN201420163606.2U Expired - Lifetime CN203825284U (en) 2014-04-04 2014-04-04 Weak light collector in three-dimensional space

Country Status (1)

Country Link
CN (1) CN203825284U (en)

Cited By (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN106018330A (en) * 2016-05-10 2016-10-12 四川长虹电器股份有限公司 Pocket-type near-infrared spectrometer
CN107490432A (en) * 2017-04-27 2017-12-19 安徽华脉科技发展有限公司 A kind of Feebleness Light Signal Examining system
CN115494050A (en) * 2022-11-15 2022-12-20 四川碧朗科技有限公司 Low-light-level collection method, low-light-level collection device and luminescent bacteria low-light-level detection module

Cited By (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN106018330A (en) * 2016-05-10 2016-10-12 四川长虹电器股份有限公司 Pocket-type near-infrared spectrometer
CN106018330B (en) * 2016-05-10 2019-03-22 四川长虹电器股份有限公司 A kind of pocket-type near infrared spectrometer
CN107490432A (en) * 2017-04-27 2017-12-19 安徽华脉科技发展有限公司 A kind of Feebleness Light Signal Examining system
CN115494050A (en) * 2022-11-15 2022-12-20 四川碧朗科技有限公司 Low-light-level collection method, low-light-level collection device and luminescent bacteria low-light-level detection module

Similar Documents

Publication Publication Date Title
CN103941382A (en) Collector for faint light in three-dimensional space
CN107014741B (en) Flow cytometer
CN102297853B (en) Analytical equipment
CN102346145B (en) Fine particle measuring device
CN103941381A (en) Collector for weak light in three-dimensional space
CN203825284U (en) Weak light collector in three-dimensional space
CN205368376U (en) Gene sequencing appearance optical system and focusing system thereof
CN103822893A (en) NDIR (Non-Dispersive Infra-Red) gas sensor
CN103998916A (en) Microchip and microchip-type fine-particle measuring device
CN102323703A (en) Reflector path optical system based on miniature Raman spectrometer
CN105203222A (en) Device for measuring temperature of flame through one-dimensional scanning on basis of Fresnel lens and CARS
CN105510297A (en) Raman fluorescence spectrum testing system and optical signal collector thereof
CN102564929A (en) High-flow dust particle counting sensor with novel photosensitive area structure
CN102943995A (en) Solar simulator optical device with variable radiation surface sizes and variable collimation angles
CN104597011A (en) Excitation light source drift correction device and fluorescence spectrograph
CN105510243A (en) Spectral analysis device
CN205426795U (en) From novel raman probe who takes light source
CN203825285U (en) Weak light collector in three-dimensional space
CN104198452A (en) Signal enhancement laser-induced fluorescence system
CN207571018U (en) A kind of gas absorption cell light channel structure suitable for fume continuous monitoring system
CN208270405U (en) A kind of optical fiber optical path pool
CN102913817A (en) Light source device for radar detection system
CN115993316A (en) Single molecule detection immunoassay appearance optical system
CN202471562U (en) Large-flow dust particle counting sensor with novel photosensitive region structure
CN202093325U (en) Imaging box and imaging device

Legal Events

Date Code Title Description
C14 Grant of patent or utility model
GR01 Patent grant
TR01 Transfer of patent right

Effective date of registration: 20171121

Address after: Green Ting Road Yuhang District Cang Qian street of Hangzhou city Zhejiang province 311121 No. 1 Building 3 room 492

Patentee after: FINDER DETECTION TECHNOLOGIES CO.,LTD.

Address before: Yuhang District, Hangzhou City, Zhejiang Province, 311121 West Sea No. 998 Park Building No. 4 Room 401

Patentee before: ZHEJIANG CONVOLUTION SCIENCE & TECHNOLOGY CO.,LTD.

TR01 Transfer of patent right
CP02 Change in the address of a patent holder

Address after: 310000 east side of the second floor, building 2, No. 11-1, Yuda Road, Yuhang street, Yuhang District, Hangzhou City, Zhejiang Province

Patentee after: FINDER DETECTION TECHNOLOGIES Co.,Ltd.

Address before: Green Ting Road Yuhang District Cang Qian street of Hangzhou city Zhejiang province 311121 No. 1 Building 3 room 492

Patentee before: FINDER DETECTION TECHNOLOGIES Co.,Ltd.

CP02 Change in the address of a patent holder
CX01 Expiry of patent term

Granted publication date: 20140910

CX01 Expiry of patent term