CN102053396B - Method and device for measuring thickness of liquid crystal box - Google Patents

Method and device for measuring thickness of liquid crystal box Download PDF

Info

Publication number
CN102053396B
CN102053396B CN2009101984492A CN200910198449A CN102053396B CN 102053396 B CN102053396 B CN 102053396B CN 2009101984492 A CN2009101984492 A CN 2009101984492A CN 200910198449 A CN200910198449 A CN 200910198449A CN 102053396 B CN102053396 B CN 102053396B
Authority
CN
China
Prior art keywords
liquid crystal
light
crystal cell
optical fiber
cone
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
Application number
CN2009101984492A
Other languages
Chinese (zh)
Other versions
CN102053396A (en
Inventor
刘建华
高斌
蒲海辉
尹德金
高洪跃
戴海涛
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.)
Fudan University
Original Assignee
Fudan University
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 Fudan University filed Critical Fudan University
Priority to CN2009101984492A priority Critical patent/CN102053396B/en
Publication of CN102053396A publication Critical patent/CN102053396A/en
Application granted granted Critical
Publication of CN102053396B publication Critical patent/CN102053396B/en
Expired - Fee Related legal-status Critical Current
Anticipated expiration legal-status Critical

Links

Images

Landscapes

  • Liquid Crystal (AREA)

Abstract

The invention belongs to the field of preparation of electro-optical functional materials, and relates to a method and a device for measuring the thickness of a liquid crystal box. In the method, the thickness of the liquid crystal box can be determined without wavelength values corresponding to a maximum value and a minimum value of a transmission spectrum, so that the uncertainty of searching the maximum value and the minimum value of the transmission spectrum is avoided; a convergent beam is adopted to facilitate improving signal-to-noise ratio; and the section of a light cone on the liquid crystal box can be small so as to facilitate measuring the surface distribution of the thickness of the box. The thickness of the liquid crystal box is measured by a measuring device which comprises a light source, a condensing lens, the liquid crystal box to be measured, an optical fiber coupling head and a spectrum measuring instrument. The adopted white light emitting diode (LED) has a flat emission spectrum in the visible light range of 500 to 550nm so as to facilitate simplifying a measuring system; meanwhile, the thickness is convenient to calculate.

Description

A kind of liquid crystal cell method for measuring thickness and device
Technical field
The invention belongs to electric light functional material preparation field, be specifically related to a kind of liquid crystal cell method for measuring thickness and device.
Background technology
Usually liquid crystal cell is to be bonded by two (conduction) glass substrates, has sept (spacer) to be used to control its gap length therebetween.The thick two substrates thickness at interval that just is meant of liquid crystal cell is generally several microns to tens microns.Liquid crystal cell is thick to be an important parameter of liquid crystal device, and after two base plate glass were bonded to together, the thickness in its gap (box is thick) had certain difference with the diameter at used interval (spacer), and this difference also can be very big sometimes.Therefore, accurately measuring box is thick, and is significant to the accurate grasp of liquid crystal device (LCD, photomodulator) performance.
In the prior art; Measuring the thick method of liquid crystal cell has: with its equivalence is a Fabry-Perot chamber; Utilize the multiple-beam interference principle; Adjacent very big (or minimum) according to transmitted spectrum is worth pairing wavelength, obtains the thick d of liquid crystal cell, and its principle can be expressed as the function that transmissivity is angle of incidence of light θ, wavelength X, surface strength reflectivity and the thick d of box:
T ( θ , λ ) = 1 1 + 4 R ( 1 - R ) 2 · sin 2 δ ( θ , λ , d ) 2 - - - ( e . 1 )
In the formula δ = 2 π λ 2 d · Cos θ
Through measuring the adjacent greatly pairing wavelength value λ of (or minimum) value of transmitted spectrum p, λ P+1v, λ V+1), can confirm the thick d of liquid crystal cell:
d = 1 2 ( 1 λ p ( v ) - 1 λ p + 1 ( v + 1 ) ) - - - ( e . 2 )
The application of above-mentioned principle needs the parallel incident of polychromatic light.But because the existence of aberration, this requirement also is not easy to reach.In addition, in order to obtain the thick face distribution situation of box, the diameter of light beam can not be too big, thereby luminous flux is restricted, and like this, the measurement signal to noise ratio (S/N ratio) of transmitted spectrum seriously descended, thus give very big (or minimum) peak position confirm to bring serious error.
Summary of the invention
The objective of the invention is provides a kind of liquid crystal cell method for measuring thickness and device for overcoming the above-mentioned difficulties that prior art exists.
Particularly, the present invention proposes a kind of converging beam measuring method, promptly adopts focused beam rather than parallel beam as measuring incident light; With effective raising luminous flux; Signal to noise ratio (S/N ratio) is significantly improved, and the spot size of may command transflective liquid crystal box, the face resolution of measuring improved.
The inventive method need not confirmed thickness of liquid crystal box with minimum pairing wavelength value through the very big of transmitted spectrum, thereby has removed the very big and minimizing uncertainty of searching transmitted spectrum from.Owing to adopted converging beam, helped improving signal to noise ratio (S/N ratio).The cross section of light cone on liquid crystal cell can be very little, helps the thick face of measuring box and distribute.The white light LEDs that is adopted has more smooth luminous spectrum in visible light 500-550nm scope, thereby helps the simplified measurement system, calculates also very convenient simultaneously.
The present invention measures liquid crystal cell thick (Fig. 1) through adopting measurement mechanism.Described measurement mechanism comprises: light source (1), lens (2), liquid crystal cell to be measured (3), optical fiber coupling head (4), optical spectrum instrumentation (5).Wherein, light source adopts the very little white light LEDs (1) of light-emitting area, makes it to be similar to pointolite; The white light that led light source (1) is sent by an achromatism compound lens (2) converges and forms light cone, and is focused into a picture, light cone transmission liquid crystal cell to be measured (3); Place optical fiber coupling head (4) at the picture point place; Import light into optical spectrum instrumentation (5), liquid crystal cell to be measured (3) can be as far as possible near optical fiber head, thereby reduces the cross section of light cone at the liquid crystal cell face.During measurement, in certain wavelength coverage, measure the spectrum I that liquid crystal cell is put into the light path front and back respectively 0(λ) and I t(λ), its spectrum ratio T (λ)=I t(λ)/I 0(λ), comprise the thickness information of liquid crystal cell,, adopt the light cone method of average to calculate, the light beam transmissivity of respective wavelength is asked in the light cone scope on average, and the spectrum ratio of measurement of comparison just can obtain the thick data of liquid crystal cell according to the Fabry-Perot principle.
Among the present invention, described collector lens (2) is an achromat.
Among the present invention, the optical fiber coupling head of described optical fiber (4) is a multimode optical fiber.
Among the present invention, described optical spectrum instrumentation (5) is the visible light wave range optical spectrum instrumentation.
Among the present invention, described computing method are the light cone method of average. promptly calculate the mean value of the light intensity transmitance of all light beams in the light cone.
Among the present invention, for obtaining the thick data of liquid crystal cell, the incident light element of a cone is a main systematic parameter to the subtended angle θ c of normal, among the present invention, can measure from the diameter and the image distance of light cone.If the intensity of certain wavelength coverage spectrum all equates in the light cone, be I 0(λ), its incident angle to liquid crystal cell is θ, and its position angle to the liquid crystal cell face is φ, and according to F-P chamber principle, this light beam can be represented by (1) formula the transmitance of liquid crystal cell.Visible its position angle with light beam has nothing to do in the formula.
If the area element in the light cone is ds, ds=sin θ d θ d φ, then when no liquid crystal cell, the light intensity of the spectrometer that optical fiber is coupled to does
Figure G2009101984492D00031
And the transmitted light intensity that optical fiber receives when having liquid crystal cell in light path does
Figure G2009101984492D00032
Average transmittance can be expressed as T ‾ ( λ ) = ∫ Conic I t ( θ , λ ) · Ds ∫ Conic I 0 ( θ , λ ) · Ds = ∫ Conic I t ( θ , λ ) I 0 ( θ , λ ) · Ds ∫ Conic Ds = ∫ Conic T ( θ , λ ) · Ds ∫ Conic Ds
Further arrangement, final average transmittance can be expressed as:
T ‾ ( λ ) = γ · ∫ x c 1 T ( x , λ , d ) · dx 1 - cos θ c - - - ( e . 3 )
X in the formula c=cos θ c. γ=0.92 is a correction factor, with four surfaces of reflecting liquid crystal box glass substrate to the reflection of light loss.
According to the contrast of (e.3) formula and measure spectrum transmissivity, promptly can calculate the thick data of corresponding box very delicately, and need not confirm concrete very big or minimum wavelength.
For the ease of understanding, below will describe in detail of the present invention through concrete accompanying drawing and embodiment.What need particularly point out is; Instantiation and accompanying drawing only are in order to explain; Obviously those of ordinary skill in the art can explain according to this paper, within the scope of the invention the present invention is made various corrections and change, and these corrections and change are also included in the scope of the present invention.
Description of drawings
Fig. 1 is a measurement mechanism synoptic diagram of the present invention, wherein, the 1st, white light source, the 2nd, collector lens, the 3rd, survey liquid crystal cell, the 4th, optical fiber coupling head, the 5th, optical spectrum instrumentation.
Fig. 2 is the transmitance spectrum of measurements and calculations in the embodiment
Embodiment
Embodiment 1
The device that proposes according to the present invention is set up a cover measuring system, and described measuring system device comprises: white light source (1); Collector lens (2), liquid crystal cell to be measured (3). optical fiber coupling head (4), optical spectrum instrumentation (5). wherein; Light source adopts the very little white light LEDs (1) of light-emitting area, makes it to be similar to pointolite. and the white light that led light source (1) is sent by a collector lens (2) converges and forms light cone, and is focused into a picture; Light cone transmission liquid crystal cell to be measured (3) is placed optical fiber coupling head (4) at the picture point place, imports light into optical spectrum instrumentation (5); Liquid crystal cell to be measured (3) can be as far as possible near optical fiber head, thus reduce light cone the liquid crystal cell face the cross section.During measurement, in certain wavelength coverage, measure the spectrum I that liquid crystal cell is put into the light path front and back respectively 0(λ) and I t(λ), its spectrum ratio T (λ)=I t(λ)/I 0(λ), comprise the thickness information of liquid crystal cell,, the light beam transmissivity of respective wavelength is asked in the light cone scope on average, and the spectrum ratio of measurement of comparison just can obtain the thick data of liquid crystal cell according to the Fabry-Perot principle.
The subtended angle θ c of the bus of light cone is about 11.8 ° in the present embodiment, and measurement result is as shown in Figure 2.Fig. 2 has shown the transmissivity spectrum of the inventive method measurements and calculations, and the result shows that what meet is fairly good, and the thick data of the liquid crystal cell that is simulated are 32.5 μ m.

Claims (7)

1. a liquid crystal cell method for measuring thickness is characterized in that it comprises step: adopt white LED light source (1); Make light source be similar to pointolite, the white light that this led light source (1) is sent by an achromatism compound lens (2) converges and forms light cone, and is focused into a picture; Light cone transmission liquid crystal cell to be measured (3) is placed optical fiber coupling head (4) at a picture place, and the light that will pass through optical fiber coupling head imports spectral measurement appearance (5); Liquid crystal cell to be measured (3) reduces the cross section of light cone at the liquid crystal cell face near optical fiber head; In certain wavelength coverage, measure the spectrum I that liquid crystal cell is put into the light path front and back respectively 0(λ) and I t(λ), its spectrum ratio T (λ)=I t(λ)/I 0(λ), adopt the light cone method of average to calculate the mean value of the light intensity transmitance of all light beams in the light cone, according to formula
T ‾ ( λ ) = γ · ∫ x c 1 T ( x , λ , d ) · dx 1 - cos θ c - - - ( e . 3 )
Light beam transmissivity to respective wavelength is tried to achieve average transmittance in the light cone scope
Figure FDA0000106413880000012
X in the formula c=cos θ c, γ=0.92 is a correction factor, with four surfaces of reflecting liquid crystal box glass substrate to the reflection of light loss; θ c is the subtended angle of incident light element of a cone to normal; Measure and can get from the diameter and the image distance of light cone, λ is a wavelength, and d is that liquid crystal cell is thick; And, obtain the thick data of liquid crystal cell according to the contrast of the spectrum ratio of said (e.3) formula result of calculation and measurement.
2. a liquid crystal cell thickness measuring device is characterized in that, described measurement mechanism comprises: light source (1), collector lens (2), liquid crystal cell to be measured (3), optical fiber coupling head (4), optical spectrum instrumentation (5); Said light source (1) adopts the very little white light LEDs of light-emitting area; Make it to be similar to pointolite; The white light that this led light source (1) is sent by this collector lens (2) converges and forms light cone, and is focused into a picture, light cone transmission liquid crystal cell to be measured (3); Place optical fiber coupling head (4) at a picture place, the light that will pass through optical fiber coupling head imports spectral measurement appearance (5).
3. liquid crystal cell thickness measuring device according to claim 2 is characterized in that, described light source (1) is a white light LEDs.
4. liquid crystal cell thickness measuring device according to claim 3 is characterized in that, described white light LEDs is in visible light 500-550nm scope.
5. liquid crystal cell thickness measuring device according to claim 2 is characterized in that, described collector lens (2) is an achromat.
6. liquid crystal cell thickness measuring device according to claim 2 is characterized in that, described optical fiber coupling head (4) is a multimode optical fiber.
7. liquid crystal cell thickness measuring device according to claim 2 is characterized in that, described optical spectrum instrumentation (5) is the visible light wave range optical spectrum instrumentation.
CN2009101984492A 2009-11-06 2009-11-06 Method and device for measuring thickness of liquid crystal box Expired - Fee Related CN102053396B (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
CN2009101984492A CN102053396B (en) 2009-11-06 2009-11-06 Method and device for measuring thickness of liquid crystal box

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
CN2009101984492A CN102053396B (en) 2009-11-06 2009-11-06 Method and device for measuring thickness of liquid crystal box

Publications (2)

Publication Number Publication Date
CN102053396A CN102053396A (en) 2011-05-11
CN102053396B true CN102053396B (en) 2012-02-29

Family

ID=43957896

Family Applications (1)

Application Number Title Priority Date Filing Date
CN2009101984492A Expired - Fee Related CN102053396B (en) 2009-11-06 2009-11-06 Method and device for measuring thickness of liquid crystal box

Country Status (1)

Country Link
CN (1) CN102053396B (en)

Families Citing this family (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN102826883B (en) * 2012-06-18 2014-04-09 中化(烟台)作物营养有限公司 Deflocculating humic acid liquid water soluble fertilizer and preparation method thereof
TWI464364B (en) * 2013-01-03 2014-12-11 Univ Nat Sun Yat Sen Liquid crystal cell gap measurement device and measurement method thereof
CN103454790B (en) * 2013-08-22 2015-10-21 合肥京东方光电科技有限公司 A kind of pick-up unit, liquid crystal drip-injection system and liquid crystal drip-injection control method
CN107462177B (en) * 2017-09-25 2019-11-05 武汉华星光电技术有限公司 A kind of thickness of liquid crystal box measuring device and measuring method

Citations (5)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2001242040A (en) * 2000-03-01 2001-09-07 Stanley Electric Co Ltd Evaluation method for liquid crystal display element
CN1340690A (en) * 2000-09-01 2002-03-20 精工爱普生株式会社 Inspection method for liquid crystal box thickness, control system for liquid crystal box thickness and manufacture method for liquid crystal device
WO2005026703A1 (en) * 2003-09-12 2005-03-24 Swedish Lcd Center Method for characterization of a liquid crystal cell
JP2005283534A (en) * 2004-03-31 2005-10-13 Seiko Epson Corp Cell thickness measuring method and measuring device for vertically oriented liquid crystal panel
TWI242073B (en) * 2001-02-23 2005-10-21 Otsuka Denshi Kk Method for inspecting gaps between liquid crystal units

Patent Citations (5)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2001242040A (en) * 2000-03-01 2001-09-07 Stanley Electric Co Ltd Evaluation method for liquid crystal display element
CN1340690A (en) * 2000-09-01 2002-03-20 精工爱普生株式会社 Inspection method for liquid crystal box thickness, control system for liquid crystal box thickness and manufacture method for liquid crystal device
TWI242073B (en) * 2001-02-23 2005-10-21 Otsuka Denshi Kk Method for inspecting gaps between liquid crystal units
WO2005026703A1 (en) * 2003-09-12 2005-03-24 Swedish Lcd Center Method for characterization of a liquid crystal cell
JP2005283534A (en) * 2004-03-31 2005-10-13 Seiko Epson Corp Cell thickness measuring method and measuring device for vertically oriented liquid crystal panel

Non-Patent Citations (2)

* Cited by examiner, † Cited by third party
Title
杨玉成.液晶盒反射谱用于盒厚测量的研究.《电子科技大学硕士学位论文》.2007,全文. *
沈奕等.基于光干涉原理的液晶空盒盒厚测量.《仪表技术与传感器》.2000,(第7期),24-26. *

Also Published As

Publication number Publication date
CN102053396A (en) 2011-05-11

Similar Documents

Publication Publication Date Title
CN103097930B (en) Get tabula rasa and rod and the optical pickup apparatus and the light-emitting device that employ them
CN101446485B (en) Surveymeter for parallelism of optical axis of visible light and infrared light wave
CN102053396B (en) Method and device for measuring thickness of liquid crystal box
CN1128862A (en) Method and device for optical determination of physical quantity
TWI451073B (en) Measuring the optical system and the use of its brightness meter, color brightness meter and color meter
CN101548214A (en) Optical module and optical sensor using the same and method for manufacturing thereof
US11313760B2 (en) Device and method for measuring transmittance curve of Fabry-Parot using whispering gallery mode laser source
CN107843412A (en) Optical detection system and optical detection device
CN206095585U (en) Light detecting system and light detection device
CN106094234A (en) A kind of autocollimatic light path system with polarization beam splitting element
CN104792739A (en) SPR imaging sensor, adjusting method thereof and SPR imaging sensor chip
CN103454239A (en) Liquid component sensor
Missinne et al. Compact packaged silicon photonic Bragg grating sensor based on a ball lens interface
CN101358835B (en) Super-resolution compound shade differential confocal measuring device and method
CN104280851A (en) Adjusting device for focusing and leveling self zero plane and method thereof
CN110553730B (en) Spectrometer
CN101702022A (en) Laser dot matrix instrument
CN104406939A (en) Plastic fiber surface plasma sensor based on bimetallic grating and application thereof
CN205898079U (en) Polarization closes restraints auto -collimation optic system based on two refracting element
CN205786353U (en) A kind of transmittance meter based on rotating filtering sheet monochromator
TWI730602B (en) Distance measuring device and prism module thereof
CN112903136A (en) Temperature indicating device
WO2024085027A1 (en) Optical device for measurement
CN215833253U (en) Angle modulation type SPR sensor based on beam deflector and SPR detection equipment
CN112067597B (en) Remote shortwave ultraviolet Mach-Zehnder space heterodyne Raman spectrometer

Legal Events

Date Code Title Description
C06 Publication
PB01 Publication
C10 Entry into substantive examination
SE01 Entry into force of request for substantive examination
C14 Grant of patent or utility model
GR01 Patent grant
CF01 Termination of patent right due to non-payment of annual fee

Granted publication date: 20120229

Termination date: 20141106

EXPY Termination of patent right or utility model