CN106770130A - A kind of method for measuring two photon absorption cross section - Google Patents

A kind of method for measuring two photon absorption cross section Download PDF

Info

Publication number
CN106770130A
CN106770130A CN201710030738.6A CN201710030738A CN106770130A CN 106770130 A CN106770130 A CN 106770130A CN 201710030738 A CN201710030738 A CN 201710030738A CN 106770130 A CN106770130 A CN 106770130A
Authority
CN
China
Prior art keywords
photon
fluorescence
absorption cross
photon absorption
photon fluorescence
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.)
Pending
Application number
CN201710030738.6A
Other languages
Chinese (zh)
Inventor
钱骏
努尔尼沙·阿力甫
汪亚伦
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.)
Zhejiang University ZJU
Original Assignee
Zhejiang University ZJU
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 University ZJU filed Critical Zhejiang University ZJU
Priority to CN201710030738.6A priority Critical patent/CN106770130A/en
Publication of CN106770130A publication Critical patent/CN106770130A/en
Pending legal-status Critical Current

Links

Classifications

    • GPHYSICS
    • G01MEASURING; TESTING
    • G01NINVESTIGATING OR ANALYSING MATERIALS BY DETERMINING THEIR CHEMICAL OR PHYSICAL PROPERTIES
    • G01N21/00Investigating or analysing materials by the use of optical means, i.e. using sub-millimetre waves, infrared, visible or ultraviolet light
    • G01N21/62Systems in which the material investigated is excited whereby it emits light or causes a change in wavelength of the incident light
    • G01N21/63Systems in which the material investigated is excited whereby it emits light or causes a change in wavelength of the incident light optically excited
    • G01N21/64Fluorescence; Phosphorescence
    • G01N21/6402Atomic fluorescence; Laser induced fluorescence

Abstract

The invention discloses a kind of method for measuring two photon absorption cross section.Femtosecond laser is introduced scanning microscopic system as light source by the present invention, femtosecond laser excites the two-photon fluorescence signal of detected materials after object lens are focused on, fluorescence signal and then received by sensitive photomultiplier is responded, be imaged on computers by after opto-electronic conversion, data sampling, treatment.The background of material two-photon fluorescence imaging is subtracted again, and the value of fluorescence intensity substitutes into formula and calculate the 2PA sections that can obtain detected materials as two-photon fluorescence intensity signal in then readable two-photon fluorescence imaging figure of drawing materials.2PA section gauges method proposed by the present invention is based on the two-photon fluorescence micro imaging system of stabilization, more traditional 2PA cross sectional testing methods, the error of measurement result is substantially reduced, and measuring method is more easy, reliable, the personnel for being adapted to non-optical specialty are operated.

Description

A kind of method for measuring two photon absorption cross section
Technical field
It is a kind of method of new measurement two photon absorption cross section the invention belongs to field of optical detection.This measurement side Method can be based on any two-photon fluorescence microscope, be measured by the intensity signal of two-photon fluorescence method acquisition fluorescent material The two photon absorption cross section of material.
Background technology
Two-photon fluorescence (Two-Photon Fluorescence, 2PF) refers to that fluorescent material swashs in high peak power pulse Two photon transitions of light source are absorbed under light stimulus simultaneously to excitation state, then relaxation returns to ground state and launches a mistake of photon Journey.The two-photon of material is characterized usually using two-photon action section (Two-PhotonActionCross-Section, η δ) Fluorescent emission efficiency, it represents that material absorbs incident photon and launches the ability of two-photon fluorescence, equal to the two-photon of material Absorption cross-section (2PA, Two-PhotonAbsorption Cross-Section, δ) and fluorescence quantum yield (Fluorescence Quantum Yield, η) product.Wherein, 2PA sections characterize the probability that material molecule occurs two-photon absorption, reflect material Material carries out the ability of two-photon absorption.The method in measurement 2PA sections can substantially be divided into two major classes, and a class is from absorption cross-section Definition is set out, and carries out direct measurement, such as nonlinear transmission method.When surveying 2PA sections in this way, incident optical power needs very Greatly, and material requested concentration it is higher.Additionally, measure 2PA sections with the method to lack a reference to determine used by measurement Whether incident optical power is in a rational scope with material concentration.Therefore the easy producing ratio of result that transmitance method is measured Larger error.In addition, the measurement of transmitance method is higher to the power requirement of light source, common femtosecond OPO power is often inadequate, Need using peak power femtosecond OPA higher as light source.
The method in another kind measurement 2PA sections is the effect from 2PA sections, is measured indirectly.As two-photon is glimmering Light method surveys 2PA sections, its substantially thinking:
The relation of the two-photon fluorescence intensity F and 2PA section δ that material is produced is represented by:
F=δ NAcηLnI2K (1)
Wherein, NAIt is avogadros constant, c is the molar concentration of material, and η is the fluorescence quantum yield of material, and L is represented The thang-kng length of material, I is the intensity of incident light, and K is relevant with the collection efficiency of an optical system constant.It is this Method can be by measuring the two-photon fluorescence intensity of material so as to the anti-2PA sections for releasing it.Due to being difficult directly to try to achieve light The collection efficiency of system, therefore generally measured using comparison method, that is, find one connects with testing sample two-photon fluorescence spectrum Closely and reference material known to 2PA sections, their two-photon fluorescence is measured respectively under identical optical environment, then pass through Extrapolate the 2PA sections of sample in the 2PA sections of reference material.Its computing formula:
Wherein subscript 1 and 0 distinguishes representative sample and reference material.Due to K be one with the thang-kng length of optical system with The relevant constant of collection efficiency, therefore under identical optical measurement environment, K values are identicals, i.e. K1=K2.So, as long as Under identical optical environment, both two-photon fluorescence intensity F are measured respectively1、F0, and know their molar concentration c1、 c0, fluorescence quantum yield η1、η0, the refractive index n of solution1、n0, and reference material 2PA sections δ0, it is possible to obtain sample 2PA sections δ1.Compared to nonlinear transmission method, the advantage of two-photon fluorescence method mainly has at 2 points.First, two-photon fluorescence intensity With incident intensity into quadratic relationship, the shadow that other non-linear absorptions and linear absorption are brought can be reduced in experimentation Ring.2nd, incident optical power used in fluorescence method measurement and material concentration are more much lower than transmitance method respectively, and this also greatly reduces The contributions of other non-linear absorptions and linear absorption.Disturbed by reducing these, two-photon fluorescence method can generally compare non-thread Property transmitance method measures more accurate 2PA sections.
2PA sections can use without ripe commercialization instrument, are typically necessary and oneself build light path and measure material Fluorescence spectrum, and then wavelength integration is carried out to spectral intensity, and calculated with formula (2).However, being surveyed by spectrometer Amount be fluorescent material transmitting the part that is scattered of fluorescence signal, and this part fluorescence is very weak, and is easily subject to environment In other veiling glares influence, therefore measured signal has than larger error.In order to solve this problem, further improve The precision of detection, the present invention devises a kind of method of new measurement two photon absorption cross section, i.e., directly aobvious with two-photon fluorescence Micro mirror obtains the two-photon fluorescence light intensity signal of testing sample, and then is calculated its 2PA section with formula (2).
The content of the invention
The present invention is based on two-photon fluorescence microscope, it is proposed that a kind of brand-new two photon absorption cross section measuring method.This Femtosecond laser is introduced scanning microscopic system as light source for invention, and femtosecond laser is by exciting the double of detected materials after object lens focusing Photon fluorescence signal, fluorescence signal so that responded sensitive photomultiplier (Photonmultiplier Tube, referred to as PMT) receive, be imaged on computers by after opto-electronic conversion, data sampling, treatment.Material two-photon fluorescence imaging is subtracted again Background, the value of fluorescence intensity is used as two-photon fluorescence intensity signal, generation in then readable two-photon fluorescence imaging figure of drawing materials Enter formula (2) and calculate the 2PA sections that can obtain detected materials.
The technical solution adopted by the present invention is:
2PA section gauges system is based on two-photon fluorescence micro imaging system, mainly including femtosecond laser light source, dichroic Mirror, PMT, signal amplifier, computer etc..
Two-photon fluorescence micro imaging system can be directed to the characteristic of excited fluorescent material, select flying for suitable wavelength Second LASER Light Source and suitable PMT receive fluorescence signal, and intensity signal is read by program, and substituting into computing formula (2) can To calculate the 2PA sections of material.
Benefit of the invention:2PA section gauges method proposed by the present invention is based on the two-photon fluorescence micro-imaging of stabilization System, more traditional 2PA cross sectional testing methods substantially reduce the error of measurement result, and measuring method it is more easy, can Lean on, the personnel for being adapted to non-optical specialty (such as material, chemistry, biology) are operated.
Brief description of the drawings
Fig. 1 is the two-photon micro imaging system schematic diagram for measuring fluorescent material 2PA sections;
Fig. 2 is the two-photon fluorescence imaging figure of fluorescent material in the capillary measured with two-photon micro imaging system.
Specific embodiment
Below in conjunction with accompanying drawing, the invention will be further described.
As shown in figure 1, the measuring system in the present invention is based on two-photon fluorescence micro imaging system, mainly swash including femtosecond Radiant, galvanometer scanning unit, dichroic mirror, PMT, signal amplifier, data collecting card, computer etc..Galvanometer scanning unit, two Look mirror, PMT etc. are constituted scanning microscopic system and [are just being put scanning microscopy imaging system (Olympus, BX61+ with Olympus here FV1200 as a example by)]
First, external femtosecond laser introduces Olympus and is just putting scanning microscopy imaging system (Olympus, BX61+ FV1200), expand into being formed with tube lens (tube lens) through scanning lens (scan lens) after galvanometer scanning unit Light beam is again through the anti-short logical (cutoff wavelength of a block length:980nm) dichroscope reflection, is assembled by object lens and excites fluorescent material, is produced Two-photon fluorescence signal, the fluorescence that material is inspired is returned along original optical path, by 980nm anti-short logical dichroscopes long, Yi Jixiang Sensitive PMT is responded after the optical filter (further filtering out femtosecond exciting light) answered to receive;PMT converts analog signals into numeral Signal, is also connected with reality by computer acquisition, the galvanometer scanning unit in system by after signal amplifier amplification with computer The synchronization of existing signal scanning.By such set of system, the two-photon fluorescence micro-imaging figure (such as Fig. 2) of material can be obtained. Fluorescence intensity F in Fig. 21Bias light first can be subtracted with program 1, then be calculated with MATLAB programs 2.Obtained with same method To the two-photon fluorescence intensity F with reference to fluorescent dyes rhodamine Rh6G0.Afterwards by detected materials and the intensity signal of reference material F1And F0Substituting into formula (2) can calculate the 2PA sections of material.
The photon that big mode field area (large-mode-area) mixes Yb (ytterbium-doped) is employed in this example Crystal optical fibre (Photonic Crystal Fiber, PCF) laser (pulsewidth:140fs, repetition rate:50MHz, wavelength: 1040nm) as femtosecond light source.Dichroic mirror is off the length anti-short logical dichroscope, the filter after dichroic mirror that wavelength is 980nm Mating plate is the pass filter long of 590nm;Object lens are 25 times of hydroscopes of Olympus, and operating distance is 2mm, and 400nm~ 1600nm optical bands have good transmitance;PMT can respond the optical signal of 185-800nm wave bands.Selected two-photon Fluorescent material selects semi-conducting polymer nano particle (Semiconducting Polymer Dots, P-dots), and it absorbs light Spectrum is located at 350-450nm, and fluorescence peak is in 650nm or so.Rhodamine Rh6G is with reference to fluorescent material.
1. the program of background is subtracted
clear;
Const=1;
I0=imread (background is imaged .bmp');
I1=imread (' Fig. 2 .bmp');
J1=rgb2gray (I1);
K=(J1-J0)*const;
Imwrite (K, ' Fig. 2 actual strength .bmp');
2. the program of Fig. 2 fluorescence intensity information is read
clear;
I=imread (' Fig. 2 .bmp');
J=rgb2gray (I);
K=J (find (J>=0));
s0=sum (sum (K))
To sum up, present invention sets forth a kind of method in novel measurement 2PA sections.Present invention selection Olympus is just put and is swept Microscope (Olympus, BX61+FV1200) is retouched, external 1040nm femtosecond lasers is introduced as excitation source, excites P-dots to send out Two-photon fluorescence signal (with rhodamine Rh6G as reference) is projected, two-photon fluorescence imaging figure has been obtained.Pass through MATLAB again The formula (2) for calculating 2PA sections is substituted into after reading the fluorescence intensity of image, you can calculate the 2PA sections of detected materials.This The method for applying mechanically two-photon fluorescence micro imaging system measurement fluorescent material 2PA sections, compared to traditional measuring method, collects In hgher efficiency, more convenient operation, error is less, and stability is higher, more reliable performance.

Claims (6)

1. it is a kind of measure two photon absorption cross section method, the device for being used include femtosecond laser light source, galvanometer scanning unit, Dichroic mirror, photomultiplier, signal amplifier and computer, it is characterised in that:
The laser that external femtosecond laser light source is sent with tube lens through scanning lens into forming after galvanometer scanning unit Light beam is expanded, then is reflected through the anti-short logical dichroscope of a block length, assembled by object lens and excite fluorescent material, produce two-photon fluorescence letter Number, the fluorescence that material is inspired is returned along original optical path, by anti-short logical dichroscope long, and for filtering femtosecond exciting light Sensitive photomultiplier is responded after optical filter to receive;Photomultiplier converts analog signals into data signal, by letter Number amplifier amplify after by computer acquisition;Described galvanometer scanning unit is connected to realize the same of signal scanning with computer Step;
By said process, the two-photon fluorescence micro-imaging figure of material is obtained, then fluorescence intensity is obtained from the micro-imaging figureF 1 ;Then the two-photon fluorescence intensity with reference to fluorescent dyes rhodamine Rh6G is obtained in the same wayF 0 ;Thus it is calculated double Photon absorption cross sections.
2. it is according to claim 1 it is a kind of measure two photon absorption cross section method, it is characterised in that:Two-photon fluorescence shows Micro- image also needs to do the treatment of background subtraction light.
3. it is according to claim 1 it is a kind of measure two photon absorption cross section method, it is characterised in that:Long anti-short logical two to The cutoff wavelength of Look mirror is 980nm.
4. it is according to claim 1 it is a kind of measure two photon absorption cross section method, it is characterised in that:Optical filter is The pass filter long of 590nm.
5. it is according to claim 1 it is a kind of measure two photon absorption cross section method, it is characterised in that:Photomultiplier can Respond the optical signal of 185-800 nm wave bands.
6. it is according to claim 1 it is a kind of measure two photon absorption cross section method, it is characterised in that:Object lens are Olympic bars This 25 times of hydroscopes, operating distance is 2mm.
CN201710030738.6A 2017-01-16 2017-01-16 A kind of method for measuring two photon absorption cross section Pending CN106770130A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
CN201710030738.6A CN106770130A (en) 2017-01-16 2017-01-16 A kind of method for measuring two photon absorption cross section

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
CN201710030738.6A CN106770130A (en) 2017-01-16 2017-01-16 A kind of method for measuring two photon absorption cross section

Publications (1)

Publication Number Publication Date
CN106770130A true CN106770130A (en) 2017-05-31

Family

ID=58946019

Family Applications (1)

Application Number Title Priority Date Filing Date
CN201710030738.6A Pending CN106770130A (en) 2017-01-16 2017-01-16 A kind of method for measuring two photon absorption cross section

Country Status (1)

Country Link
CN (1) CN106770130A (en)

Citations (5)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US20040061072A1 (en) * 2002-09-30 2004-04-01 Swinburne University Of Technology Apparatus
JP2008069294A (en) * 2006-09-15 2008-03-27 Ricoh Co Ltd pi CONJUGATED COMPOUND AND USE THEREOF, AND ELEMENT AND DEVICE USING THE SAME
CN203164119U (en) * 2012-11-14 2013-08-28 深圳大学 Two-photon absorption section spectrometer
CN105004704A (en) * 2015-07-09 2015-10-28 华南师范大学 New use of neodymium ion sensitized up-conversion nanocrystal, and high-resolution multi-photon microscopic system
CN106066318A (en) * 2016-06-14 2016-11-02 中国科学院长春光学精密机械与物理研究所 A kind of method and device of on-line testing optical element laser damage

Patent Citations (5)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US20040061072A1 (en) * 2002-09-30 2004-04-01 Swinburne University Of Technology Apparatus
JP2008069294A (en) * 2006-09-15 2008-03-27 Ricoh Co Ltd pi CONJUGATED COMPOUND AND USE THEREOF, AND ELEMENT AND DEVICE USING THE SAME
CN203164119U (en) * 2012-11-14 2013-08-28 深圳大学 Two-photon absorption section spectrometer
CN105004704A (en) * 2015-07-09 2015-10-28 华南师范大学 New use of neodymium ion sensitized up-conversion nanocrystal, and high-resolution multi-photon microscopic system
CN106066318A (en) * 2016-06-14 2016-11-02 中国科学院长春光学精密机械与物理研究所 A kind of method and device of on-line testing optical element laser damage

Non-Patent Citations (2)

* Cited by examiner, † Cited by third party
Title
何国华等: "双光子吸收截面的测量方法", 《激光杂志》 *
秦一凡等: "飞秒激光双光子荧光显微系统的构建与应用", 《哈尔滨工业大学学报》 *

Similar Documents

Publication Publication Date Title
EP3559642B1 (en) Surface sensing systems and methods for imaging a scanned surface of a sample via sum-frequency vibrational spectroscopy
Krishnan et al. Development of a multiphoton fluorescence lifetime imaging microscopy system using a streak camera
KR100885927B1 (en) Apparatus and method for measuring fluorescence lifetime
CN104880445B (en) A kind of autofluorescence life-span imaging and fluorescence spectrum combine the device for early diagnosis of cancer
CN105004704B (en) The upper conversion nano crystalline substance new application of neodymium ion sensitization and high-resolution multi-photon microscopic system
US20110031414A1 (en) Device for microscopy having selective illumination of a plane
Wu et al. Depth-resolved fluorescence spectroscopy reveals layered structure of tissue
CN108414442A (en) Confocal microscope system suitable for near-infrared 2nd area fluorescent vital imaging
CN104204779B (en) Fluorescece obsevation method and fluorescence obsevation apparatus
CN106990095B (en) Reflection-type confocal CARS micro-spectrometer method and apparatus
CN103163106A (en) Super-resolution fluorescent lifetime imaging method and device based on stimulated emission lost
Ren et al. Terahertz coherent anti-Stokes Raman scattering microscopy
CN107167456A (en) Transmission-type differential confocal CARS micro-spectrometer method and devices
Zhou et al. Multispectral fluorescence lifetime imaging device with a silicon avalanche photodetector
Tan et al. Multimodal subcellular imaging with microcavity photoacoustic transducer
CN105445226A (en) Method and apparatus for observing one-dimensional nano-material
CN107167457A (en) The confocal CARS micro-spectrometers method and device of transmission-type
EP3550288B1 (en) Fluorescence lifetime measuring device and method
CN105403538A (en) Method and device for measurement of chirality of carbon nanotube
Tsikritsis et al. Practical considerations for quantitative and reproducible measurements with stimulated Raman scattering microscopy
Ehrlich et al. Fibre optic time-resolved spectroscopy using CMOS-SPAD arrays
CN110462381B (en) Fluorescence lifetime measuring device and method for high-speed analysis of multi-exponential decay function type experimental data
CN105445227A (en) Method and apparatus for observing one-dimensional nano-material
CN112161946B (en) Frequency domain luminous life imaging system
Xu et al. Two-photon fluorescence excitation spectroscopy by pulse shaping ultrabroad-bandwidth femtosecond laser pulses

Legal Events

Date Code Title Description
PB01 Publication
PB01 Publication
SE01 Entry into force of request for substantive examination
SE01 Entry into force of request for substantive examination
RJ01 Rejection of invention patent application after publication

Application publication date: 20170531

RJ01 Rejection of invention patent application after publication