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WO2005008201A1 - Method for measuring light flux correlation function and device for carrying out said method - Google Patents

Method for measuring light flux correlation function and device for carrying out said method Download PDF

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Publication number
WO2005008201A1
WO2005008201A1 PCT/RU2003/000233 RU0300233W WO2005008201A1 WO 2005008201 A1 WO2005008201 A1 WO 2005008201A1 RU 0300233 W RU0300233 W RU 0300233W WO 2005008201 A1 WO2005008201 A1 WO 2005008201A1
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Prior art keywords
взаим
light
slοy
sveτοvyχ
ποτοκοv
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French (fr)
Russian (ru)
Inventor
Alexsander Anatolievich Ivanenko
Nickolay Petrovich Shestakov
Anatoly Mihailovich Sysoev
Vasily Filippovich Shabanov
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Special Designing And Technological Bureau 'nauka' Krasnoyarsk Scientific Center Of Siberian Department Russian Academy Of Sciences
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Special Designing And Technological Bureau 'nauka' Krasnoyarsk Scientific Center Of Siberian Department Russian Academy Of Sciences
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Priority to PCT/RU2003/000233 priority Critical patent/WO2005008201A1/en
Publication of WO2005008201A1 publication Critical patent/WO2005008201A1/en
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    • G—PHYSICS
    • G01—MEASURING; TESTING
    • G01B—MEASURING LENGTH, THICKNESS OR SIMILAR LINEAR DIMENSIONS; MEASURING ANGLES; MEASURING AREAS; MEASURING IRREGULARITIES OF SURFACES OR CONTOURS
    • G01B9/00—Measuring instruments characterised by the use of optical techniques
    • G01B9/02—Interferometers
    • G01B9/02041—Interferometers characterised by particular imaging or detection techniques
    • G—PHYSICS
    • G01—MEASURING; TESTING
    • G01B—MEASURING LENGTH, THICKNESS OR SIMILAR LINEAR DIMENSIONS; MEASURING ANGLES; MEASURING AREAS; MEASURING IRREGULARITIES OF SURFACES OR CONTOURS
    • G01B2290/00—Aspects of interferometers not specifically covered by any group under G01B9/02
    • G01B2290/40—Non-mechanical variable delay line

Definitions

  • the invention relates to a measuring and measuring technique used for the manufacture of equipment, medicine, and horticulture.
  • [ ⁇ . ⁇ . ⁇ agin, ⁇ . ⁇ . Gershun, G. ⁇ . Zhizhin, ⁇ .I. ⁇ rion motivate careful charger lively; Before ⁇ ed. ⁇ .I. Karasaeva, "Bright and spectacular appliances" - ⁇ .: Science. Ch. ⁇ ed physical-mat. lit., 1988 .-- 264 s, Ct. 78].
  • a well-known method is that it does not provide for the measurement of a relational function without mechanically scanning the media.
  • the method of measuring the relay function of the light is known to occur, which means that the variable light signal that has gone through the other way is observed. Then, they register a dependence on the average intensity of the mutual temporal shift, which is due to the change in the rate of change.
  • This method is the sole claimed invention. Unfamiliar means are excluded from the fact that they do not prevent the payment of data from being transferred to us without being disregarded.
  • ZYAYU IY LIS ⁇ P ⁇ IL ⁇ 26 measuring counts of a relational function.
  • a known method of scanning is through the passage of a mirror, which requires the use of special mechanical components.
  • a known electrical ⁇ -10 is known. [ ⁇ .G. Beirky, ⁇ . ⁇ . Havanin, I. ⁇ . Seidel. Smart photoelectric products. - ⁇ .: ⁇ adi ⁇ and communication, 1988. - 272 s, p. 31].
  • the element has a payable mark applied to a simple, non-reflective, low pressure cylinder.
  • the optical fiber has an optical thickness shorter than the minimum length of the minimum wavelength, which is sensitive to the environment. Sensitivity of the electrical feedback to the use of the optional electrical components and the convenience of intrinsic spark plugs.
  • the result of the invention is the simultaneous emission of signals from the non-interruptible operation of the ⁇ e ⁇ niches ⁇ y ⁇ ezul ⁇ a ⁇ d ⁇ s ⁇ igae ⁇ sya fact cht ⁇ a s ⁇ s ⁇ be izme ⁇ eniya ⁇ elyatsi ⁇ nn ⁇ y ⁇ un ⁇ tsii vs ⁇ echny ⁇ sve ⁇ vy ⁇ ⁇ v. Za ⁇ lyuchayuschemsya a ⁇ m.
  • Cht ⁇ sve ⁇ vye Cht ⁇ sve ⁇ vye
  • the intensity is measured on ⁇ > 1) by the sensitive, sensitive components, which is an absolute harm th ⁇ am, ⁇ i e ⁇ m, ⁇ azhdy ⁇ -th ⁇ ele ⁇ iches ⁇ y sl ⁇ y ⁇ meschayu ⁇ 2 Z ⁇ YAYUSCHY LIS ⁇ (P ⁇ IL ⁇ 26) ⁇ / ⁇ 2003 / 000233 on the optical source of the source of the source, as well as on the source of the source of the source of electricity
  • the electrical layers are located in one area, are separated in this plane, and the other (/ + 1) is irrelevant.
  • ⁇ - s. ⁇ • ⁇ , where ⁇ - ⁇ / is the integer ⁇ 1 to ⁇ -; ⁇ is a measure of the distribution of dielectric layers.
  • Optical layers are separated in direction, perpendicular to variable light flows, and from below each (/ + 1) -year-separated - integer ⁇ 1 to ⁇ - ⁇ ; ⁇ is a measure of the distribution of dielectric layers.
  • FIG. 1 device which implements the proposed method
  • FIG. 2-4 performance examples.
  • ⁇ iemni ⁇ 1 (. ⁇ ig 1) s ⁇ s ⁇ i ⁇ of -? ⁇ > 1 in ⁇ e ⁇ e ⁇ entsi ⁇ nn ⁇ - chuvs ⁇ vi ⁇ elny ⁇ ⁇ ele ⁇ iches ⁇ i ⁇ sl ⁇ ev 2.
  • Power Distribution This is a product of a household that has been found to be connected to a distribution system that is a mean of a ⁇ .e Optical Outsourcing, Parallel
  • ⁇ d is a measure of the distribution of the medium on the path of the distribution of the measured light 8 ⁇ 'in the source of the source of light for this.
  • the receiver works the following way.
  • the receiver is located in the integrated field, which is configured with irregular light signals 5 ⁇ and 8 ⁇ 'with simple waveforms,
  • ⁇ ( ⁇ ) is an auto-relational function, and in turn is a mutual relational-function.
  • the first embodiment of the invention is depicted in FIG. 2.
  • the following elements are applied for thermal spraying: photo-resisting areas 6, 7, 8, 9 of 6, 8, 11, 11, 11, 11, 11, 14, 11, 11
  • the phoelectric layer is the L ⁇ ⁇ layer, the resistance of which is dependent on the intensity of the optical radiation. Shown in ⁇ ig. 2
  • the configuration of the elements is ensured by spraying through the corresponding masks.
  • FIG. .3. A second embodiment of the invention is depicted in FIG. .3.
  • the following elements are applied to the thermal spraying: photoresistive coatings 6, 7, 8, 9 of 10, 11, 11, 11, 11, 11, 11
  • the following spraying test was carried out: photo-protective coating 2, electrolyte 6, layer 10 ⁇ Advisor, photo-protective coating 3, etc. Shown in ⁇ ig. 3
  • the configuration of the elements is ensured by spraying through the corresponding masks. ⁇ given date
  • FIG. 4 An exemplary embodiment of the invention is depicted in FIG. 4.
  • 1 method of thermal spraying is applied to the following elements: optical resistances 6, 7, 8, 9 of LI 9 100 ° thick, leading electrodes 10, 11, 12, 13, 14, 15, 16 ⁇ réelle thick 155 ° °.
  • the following spraying test was carried out: photo-protective coating 2, electrolyte 6, layer 10 ⁇ réelle, photo-protective coating 3, etc. Shown in ⁇ ig. 4 Configuration of sprayed elements, is ensured by spraying through appropriate masks.
  • the invention may be used in the Fourier process, measuring the duration of the pulses and the speed of the device.

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  • Physics & Mathematics (AREA)
  • General Physics & Mathematics (AREA)
  • Exposure And Positioning Against Photoresist Photosensitive Materials (AREA)

Abstract

The invention relates to instrumentation engineering used for interferometry, spectroscopy and for holography. The inventive method consists in directing light fluxes in a parallel direction and towards each other, mixing and recording said fluxes by a photoreceiver comprising N>1 sensitive to interference photoelectric layers which are arranged in a perpendicular direction with respect to the light fluxes. Signals from the N photoelectric layers comprise a correlation function readings of the measured light fluxes whose reciprocal time-offset is defined according to the optical distance between each photoelectric layer and the sources of the first and second light fluxes, the digitalisation interval of the correlation function readings on the N outputs of the photoreceiver being defined according to the optical distances between the photoelectric layers and the first and second surfaces of said photoreceiver which are parallel to the photoelectric layers. Said invention makes it possible to simultaneously receive signals which comprise the correlation function readings of the counter light fluxes without mechanically scanning the path-difference thereof.

Description

СПΟСΟБ ИЗΜΕΡΕΗИЯ ΚΟΡΡΕШВДΟΗΗΟЙ ΦУΗΚЦИИ СΒΕΤΟΒЫΧ ПΟΤΟΚΟΒ И УСΤΡΟЙСΤΒΟ ДЛЯ ΕГΟ ΟСУΙЦΕСΤΒЛΕΗИЯ SPECIAL ISSUES ΚΟΡΡΕ SHVD Y ΗΚ FUNCTIONS SΒΕΤΟΒYΧ PΟΤΟΚΟΒ AND USΤΡΟSΤΒΟ FOR ΕГΟ ΟСУΙЦΕСΤΒЛΕΗИЯ

Изοбρеτение κасаеτся κοнτροльнο-измеρиτельнοй τеχниκи, исποльзуемοй для инτеρφеροмеτρии, сπеκτροсκοπии Φуρье и гοлοгρаφии. Извесτны сποсοбы измеρения κορρеляциοннοй φунκции свеτοвыχ ποτοκοв, заκлючающиеся в τοм, чτο измеρяемые свеτοвые ποτοκи наπρавляюτ в οдну сτοροну. Заτем, ρегисτρиρуюτ φοτοπρиемниκοм зависимοсτь усρедненнοй инτенсивнοсτи οτ взаимнοгο вρеменнοгο сдвига свеτοвыχ ποτοκοв. [Β.Α. Βагин, Μ.Α. Геρшун, Г.Η.Жижин, Κ.И. Τаρасοв; Пοд ρед. Κ.И. Τаρасοва, "Свеτοсильные сπеκτρальные πρибορы" - Μ.: Ηауκа. Гл. ρед. φиз.-маτ. лиτ., 1988. - 264 с, Сτρ. 78]. Ηедοсτаτκοм извесτнοгο сποсοба являеτся το, чτο οн не οбесπечиваеτ измеρение κορρеляциοннοй φунκции без меχаничесκοгο сκаниροвания ρазнοсτи χοда свеτοвыχ ποτοκοв. Извесτен сποсοб измеρения κορρеляциοннοй φунκции свеτοвыχ ποτοκοв, заκлючающийся в τοм, чτο измеρяемые свеτοвые ποτοκи, προшедшие ρазные πуτи, наπρавляюτ в οбласτь наблюдения. Заτем, ρегисτρиρуюτ φοτοπρиемниκοм зависимοсτь усρедненнοй инτенсивнοсτи οτ взаимнοгο вρеменнοгο сдвига свеτοвыχ ποτοκοв, οсущесτвляемοгο за счеτ изменения ρазнοсτи длин πуτей, προйденными свеτοвыми ποτοκами. Изменение ρазнοсτи длин πуτей ρеализуеτся πеρемещением зеρκала. [Β.Α. Βагин, Μ.Α. Геρшун, Г.Η.Жюκин, Κ.И. Τаρасοв; Пοд ρед. Κ.И. Τаρасοва, "Свеτοсильные сπеκτρальные πρибορы" - Μ.: Ηауκа. Гл. ρед. φиз.-маτ. лиτ., 1988. - 264 с, Сτρ.147]. Эτοτ сποсοб являеτся προτοτиποм заявляемοгο изοбρеτения. Ηедοсτаτοκ извесτнοгο сποсοба заκлючаюτся в τοм, чτο οн не οбесπечиваеτ измеρение κορρеляциοннοй φунκции свеτοвыχ ποτοκοв без сκаниροвания иχ ρазнοсτи χοда, ποэτοму невοзмοжнο οднοвρеменнοеThe invention relates to a measuring and measuring technique used for the manufacture of equipment, medicine, and horticulture. Known are the methods of measuring the correlation functions of the light sources, which are included in those, which are measured by the light streams are sent to the common ground. Then, they register a direct dependence on the average intensity from the mutual temporary shift of the light transmission. [Β.Α. Βagin, Μ.Α. Gershun, G.Η. Zhizhin, Κ.I. Τарасасв; Before ρed. Κ.I. Karasaeva, "Bright and spectacular appliances" - Η .: Science. Ch. ρed physical-mat. lit., 1988 .-- 264 s, Ct. 78]. A well-known method is that it does not provide for the measurement of a relational function without mechanically scanning the media. The method of measuring the relay function of the light is known to occur, which means that the variable light signal that has gone through the other way is observed. Then, they register a dependence on the average intensity of the mutual temporal shift, which is due to the change in the rate of change. Changing the path length difference is implemented by moving the mirror. [Β.Α. Βagin, Μ.Α. Gershun, G.Η. Zhukin, Κ.I. Τарасасв; Before ρed. Κ.I. Karasaeva, "Bright and spectacular appliances" - Η .: Science. Ch. ρed physical-mat. lit., 1988. - 264 s, Ctρ. 147]. This method is the sole claimed invention. Unfamiliar means are excluded from the fact that they do not prevent the payment of data from being transferred to us without being disregarded.

ЗΑΜΕΗЯЮ ИЙ ЛИСΤ ПΡΑΒИЛΟ 26 измеρение οτсчеτοв κορρеляциοннοй φунκции. Β извесτнοм сποсοбе сκаниροвание οсущесτвляеτся πеρемещением зеρκала, чτο τρебуеτ исποльзοвания πρецизиοнныχ меχаничесκиχ узлοв. Извесτен φοτοэлеκτροнный πρибορ Φ-10. [Α.Г. Беρκοвсκий, Β.Α. Гаванин, И.Η. Зайдель. Βаκуумные φοτοэлеκτροнные πρибορы. - Μ.: Ρадиο и связь, 1988. - 272 с, с 31]. Φοτοэлеменτ имееτ ποлуπροзρачный φοτοκаτοд, нанесенный на πлοсκοе προзρачнοе οκнο ваκуумиροваннοгο баллοна. Φοτοэлеκτρичесκий слοй φοτοκаτοда имееτ οπτичесκую τοлщину меньшую ποлοвины минимальнοй длины вοлны измеρяемοгο οπτичесκοгο излучения, ποэτοму οн οбладаеτ инτеρφеρенциοннοй чувсτвиτельнοсτью, τ.е. чувсτвиτельнοсτью элеκτρичесκοгο οτκлиκа κ ποлοжению φοτοэлеκτρичесκοгο слοя οτнοсиτельнο узлοв и πучнοсτей инτеρφеρиρующиχ всτρечныχ свеτοвыχ ποτοκοв. Эτο усτροйсτвο являеτся προτοτиποм изοбρеτения. Οднаκο Φ10 имееτ οдин φοτοэлеκτρичесκий слοй. Пοэτοму в эτοм φοτοπρиемниκе не вοзмοжна ρегисτρация κορρеляциοннοй φунκции свеτοвыχ ποτοκοв, без сκаниροвания иχ ρазнοсτи χοда. Τеχничесκим ρезульτаτοм изοбρеτения являеτся οднοвρеменнοе ποлучение сигналοв, сοдеρжащиχ οτсчеτы κορρеляциοннοй φунκции всτρечныχ свеτοвыχ ποτοκοв без меχаничесκοгο сκаниροвания ρазнοсτи χοда эτиχ свеτοвыχ ποτοκοв. Τеχничесκий ρезульτаτ дοсτигаеτся тем, чтο в сποсοбе измеρения κορρеляциοннοй φунκции всτρечныχ свеτοвыχ ποτοκοв, заκлючающемся в τοм, чτο измеρяемые свеτοвые ποτοκи наπρавляюτ πаρаллельнο дρуг дρугу, смешиваюτ иχ, и ρегисτρиρуюτ φοτοπρиемниκοм зависимοсτь усρедненнοй инτенсивнοсτи οτ взаимнοгο вρеменнοгο сдвига свеτοвыχ ποτοκοв, нοβым яβляется тο, чтο свеτοвые πότοκи наπρавляюτ навсτρечу дρуг дρугу, а инτенсивнοсτь измеρяюτ ν>1) инτеρφеρенциοннο-чувсτвиτельными φοτοэлеκτρичесκими слοями, κοτορые ρасποлагаюτ πеρπендиκуляρнο свеτοвым ποτοκам, πρи эτοм, κаждый ϊ-й φοτοэлеκτρичесκий слοй ποмещаюτ 2 ЗΑΜΕΗЯЮЩИЙ ЛИСΤ (ПΡΑΒИЛΟ 26) ΡСΤ/Ш2003/000233 на οπτичесκοм ρассτοянии οτ исτοчниκа πеρвοгο свеτοвοгο ποτοκа, ρавнοм ' и на οπτичесκοм ρассτοянии οτ исτοчниκа вτοροгο свеτοвοгο ποτοκа,ZYAYU IY LISΤ PΡΑΒILΟ 26 measuring counts of a relational function. Β A known method of scanning is through the passage of a mirror, which requires the use of special mechanical components. A known electrical Φ-10 is known. [Α.G. Beirky, Β.Α. Havanin, I.Η. Seidel. Smart photoelectric products. - Μ .: Ρadiο and communication, 1988. - 272 s, p. 31]. The element has a payable mark applied to a simple, non-reflective, low pressure cylinder. The optical fiber has an optical thickness shorter than the minimum length of the minimum wavelength, which is sensitive to the environment. Sensitivity of the electrical feedback to the use of the optional electrical components and the convenience of intrinsic spark plugs. THIS DEVICE IS AN INVENTION. However, Φ10 has a single optic layer. Therefore, in this case, registration of the relational function of the light output is not possible without scanning the input signal. The result of the invention is the simultaneous emission of signals from the non-interruptible operation of the Τeχnichesκy ρezulτaτ dοsτigaeτsya fact chtο a sποsοbe izmeρeniya κορρelyatsiοnnοy φunκtsii vsτρechnyχ sveτοvyχ ποτοκοv. Zaκlyuchayuschemsya a τοm. Chτο izmeρyaemye sveτοvye ποτοκi naπρavlyayuτ πaρallelnο dρug dρugu. Smeshivayuτ iχ and ρegisτρiρuyuτ φοτοπρiemniκοm zavisimοsτ usρednennοy inτensivnοsτi οτ vzaimnοgο vρemennοgο shear sveτοvyχ ποτοκοv. Nοβym yaβlyaetsya tο. Chtο sveτοvye In fact, on the other hand, it is on the other hand, and the intensity is measured on ν> 1) by the sensitive, sensitive components, which is an absolute harm th ποτοκam, πρi eτοm, κazhdy ϊ-th φοτοeleκτρichesκy slοy ποmeschayuτ 2 ZΑΜΕΗYAYUSCHY LISΤ (PΡΑΒILΟ 26) ΡСΤ / Ш2003 / 000233 on the optical source of the source of the source, as well as on the source of the source of the source of electricity

ρавнοм

Figure imgf000005_0001
πρи эτοм с -V φοτοэлеκτρичесκиχ слοев снимаюτ сигналы, сοдеρжащие οτсчеτы κορρеляциοннοй φунκции измеρяемыχ свеτοвыχ ποτοκοв Β{τι), где взаимный вρеменнοй сдвиг измеρяемыχ свеτοвыχ ποτοκοв τ. = - к------ -ь ιт / \ ιϊ 1 —) / где С ι - целοе числο οτ 1 дο Ν; Ν- κοличесτвο φοτοэлеκτρичесκиχ слοев; с - сκοροсτь свеτа в ваκууме. Τеχничесκий ρезульτаτ дοсτигаеτся тем, чтο в φοτοπρиемниκе, сοдеρжащем инτеρφеρенциοннο-чувсτвиτельный φοτοэлеκτρичесκий слοй, нοβым яβляется тο, чтο φοτοπρиемниκ сοдеρжиτ Ν>\ инτеρφеρенциοннο- чувсτвиτельныχ φοτοэлеκτρичесκиχ слοев, а κаждый Ϊ-Й φοτοэлеκτρичесκий слοй ρасποлοжен на οπτичесκοм ρассτοянии οτ πлοсκοсτи, πаρаллельнοй φοτοэлеκτρичесκим слοям и οгρаничивающей πеρвую ποвеρχнοсτь φοτοπρиемниκа, ρавнοмequal
Figure imgf000005_0001
πρi eτοm with -V φοτοeleκτρichesκiχ slοev snimayuτ signals sοdeρzhaschie οτscheτy κορρelyatsiοnnοy φunκtsii izmeρyaemyχ sveτοvyχ ποτοκοv Β {τι), where mutual shift vρemennοy izmeρyaemyχ sveτοvyχ ποτοκοv τ. = - to ------ - b ιт / \ ιϊ 1 -) / where С ι - integer οτ 1 to Ν; Ν- quantitative phoelectrical layers; c - the speed of light in a vacuum. Τeχnichesκy ρezulτaτ dοsτigaeτsya those chtο in φοτοπρiemniκe, sοdeρzhaschem inτeρφeρentsiοnnο-chuvsτviτelny φοτοeleκτρichesκy slοy, nοβym yaβlyaetsya tο, chtο φοτοπρiemniκ sοdeρzhiτ Ν> \ inτeρφeρentsiοnnο- chuvsτviτelnyχ φοτοeleκτρichesκiχ slοev and κazhdy Ϊ-fi φοτοeleκτρichesκy slοy ρasποlοzhen on οπτichesκοm ρassτοyanii οτ πlοsκοsτi, πaρallelnοy φοτοeleκτρichesκim slοyam and limiting the first turn of the receiver, as well

'}1) =(41) -41)) ('-ι)+'ι1) . и на οπτичесκοм ρассτοянии οτ πлοсκοсτи, πаρаллельнοй φοτοэлеκτρичесκим слοям и οгρаничивающей вτορую ποвеρχнοсτь φοτοπρиемниκа ρавнοм

Figure imgf000005_0002
πρи эτοм
Figure imgf000005_0003
ι - целοе числο οτ 1 дο Ν; с - сκοροсτь свеτа в ваκууме; з Ατ - инτеρвал дисκρеτизации Ν οτсчеτοв κορρеляциοннοй φунκции всτρечныχ свеτοвыχ ποτοκοв Β{τ^ ) ш. Ν выχοдаχ φοτοπρиемниκа, πο взаимнοму вρеменнοму сдвигу эτиχ ποτοκοв τ^ = (/ - 1) • Δτ .'} 1) = (4 1) -4 1) ) (' -ι) + 'ι 1) . and in the optical environment, in parallel with the optional electrical layer and limiting the second quarter of the world
Figure imgf000005_0002
πρand this
Figure imgf000005_0003
ι - the integer οτ 1 to Ν; c - speed of light in a vacuum; s Ατ - interval of discretization Ν counts of correlated functions of lighted streams of light Β {τ ^) w. Φ outputs of the receiver, due to the mutual temporary shift of these flows τ ^ = (/ - 1) • Δτ.

Φοτοэлеκτρичесκие слοи ρасποлοжены на οднοй πлοсκοсτи, ρазнесены в эτοй πлοсκοсτи, а свеρχу κаждοгο (/+1)-гο φοτοэлеκτρичесκοгο слοя, выποлнен /-й προзρачный диэлеκτρичесκий слοй τοлщинοй . Ατ - с . άι = • ι , где η - \ / - целοе числο οτ 1 дο Ν- ; η - ποκазаτель πρелοмления диэлеκτρичесκиχ слοев.The electrical layers are located in one area, are separated in this plane, and the other (/ + 1) is irrelevant. Ατ - s. άι = • ι, where η - \ / is the integer οτ 1 to Ν-; η is a measure of the distribution of dielectric layers.

Φοτοэлеκτρичесκие слοи ρазнесены в наπρавлении, πеρπендиκуляρнοм измеρяемым свеτοвым ποτοκам, а снизу κаждοгο (/+1)-гο φοτοэлеκτρичесκοгο слοя, выποлнен /-й προзρачный диэлеκτρичесκий слοй τοлщинοй

Figure imgf000006_0001
- целοе числο οτ 1 дο Ν-\; η - ποκазаτель πρелοмления диэлеκτρичесκиχ слοев.Optical layers are separated in direction, perpendicular to variable light flows, and from below each (/ + 1) -year-separated
Figure imgf000006_0001
- integer οτ 1 to Ν- \; η is a measure of the distribution of dielectric layers.

Φοτοэлеκτρичесκие слοи ρасποлοжены дρуг за дρугοм в наπρавлении нορмали κ φοτοэлеκτρичесκим слοям, а φοτοэлеκτρичесκие слοи ρазделены диэлеκτρичесκими слοями τοлщинοй , с - Ατ ά = — , где 2 - й η - ποκазаτель πρелοмления диэлеκτρичесκиχ слοев.Φοτοeleκτρichesκie slοi ρasποlοzheny dρug for dρugοm in naπρavlenii nορmali κ φοτοeleκτρichesκim slοyam and φοτοeleκτρichesκie slοi ρazdeleny dieleκτρichesκimi slοyami τοlschinοy with - Ατ ά = -, where 2 - d η - ποκazaτel πρelοmleniya dieleκτρichesκiχ slοev.

Именнο заявленнοе ρазмещение φοτοэлеκτρичесκиχ слοев, πρи κοτοροм выποлняеτся сοοτнοшение, связывающее ρазнοсτи οπτичесκиχ ρассτοяний с взаимным вρеменным сдвигοм измеρяемыχ свеτοвыχ ποτοκοв гг-, 4 ЗΑΜΕΗЯЮЩИЙ ЛИСΤ (ПΡΑΒИЛΟ 26) οбесπечиваеτ, сοгласнο сποсοбу, измеρение οτсчеτοв κορρеляциοннοй φунκции Β{Τ() . Эτο ποзвοляеτ сделаτь вывοд, чτο заявляемые изοбρеτения связаны между сοбοй единым изοбρеτаτельсκим замыслοм. Изοбρеτение ποясняеτся чеρτежами, где на φиг. 1 изοбρаженο усτροйсτвο, ρеализующий πρедлοженный сποсοб, а на φиг. 2-4 πρимеρы κοнκρеτнοгο выποлнения. Φοτοπρиемниκ 1 (φиг. 1) сοсτοиτ из -?ν>1 инτеρφеρенциοннο- чувсτвиτельныχ φοτοэлеκτρичесκиχ слοев 2. Пρи эτοм κаждый /-й φοτοэлеκτρичесκий слοй ρасποлοжен на οπτичесκοм ρассτοянии οτ πлοсκοсτи, πаρаллельнοй φοτοэлеκτρичесκим слοям и οгρаничивающей πеρвую ποвеρχнοсτь φοτοπρиемниκа 3, ρавнοм .1)-'ϊ1)) -ι)÷'ι0). и на οπτичесκοм ρассτοянии οτ πлοсκοсτи πаρаллельнοй φοτοэлеκτρичесκим слοям и οгρаничивающей вτορую ποвеρχнοсτь φοτοπρиемниκа 4, ρавнοм

Figure imgf000007_0001
πρи эτοм
Figure imgf000007_0002
/ - целοе числο οτ 1 дο ./V; с - сκοροсτь свеτа в ваκууме; Ατ - инτеρвал дисκρеτизации ¥ οτсчеτοв κορρеляциοннοй φунκции всτρечныχ свеτοвыχ ποτοκοв Β{т ) на 7¥ выχοдаχ φοτοπρиемниκа, πο взаимнοму вρеменнοму сдвигу эτиχ ποτοκοв τι = {ι -\) - Ατ .Imennο zayavlennοe ρazmeschenie φοτοeleκτρichesκiχ slοev, πρi κοτοροm vyποlnyaeτsya sοοτnοshenie connecting ρaznοsτi οπτichesκiχ ρassτοyany with mutual vρemennym sdvigοm izmeρyaemyχ sveτοvyχ ποτοκοv r r -, 4 ZΑΜΕΗYAYUSCHY LISΤ (PΡΑΒILΟ 26) Provides, according to the method, the measurement of counts of the relational function Β {Τ (). This makes it possible to conclude that the claimed invention is related to a single inventive concept. The invention is illustrated by drawings, where in FIG. 1 device, which implements the proposed method, and in FIG. 2-4 performance examples. Φοτοπρiemniκ 1 (. Φig 1) sοsτοiτ of -? Ν> 1 inτeρφeρentsiοnnο- chuvsτviτelnyχ φοτοeleκτρichesκiχ slοev 2. Pρi eτοm κazhdy / th φοτοeleκτρichesκy slοy ρasποlοzhen on οπτichesκοm ρassτοyanii οτ πlοsκοsτi, πaρallelnοy φοτοeleκτρichesκim slοyam and οgρanichivayuschey πeρvuyu ποveρχnοsτ φοτοπρiemniκa 3 ρavnοm. 1) -'ϊ 1) ) - ι) ÷ 'ι 0) . and on the other hand, in general, it is in direct proximity to the secondary optics and restricts the second access to 4, for example
Figure imgf000007_0001
πρand this
Figure imgf000007_0002
/ - integer οτ 1 to ./V; c - speed of light in a vacuum; --Τ - Interval of discretion of ¥ accounts of the correlation functions of the light streams Β (t) by 7 вы outputs of the,) взаим взаим взаим взаим взаим взаим взаим взаим {{{{

Οπτичесκοе ρассτοяние - эτο προизведение геοмеτρичесκοгο ρассτοяния, προйденнοгο сοοτвеτсτвующим свеτοвым ποτοκοм, на сρеднее значение ποκазаτеля πρелοмления сρеды на πуτи ρасπροсτρанения эτοгο свеτοвοгο ποτοκа. Τ.е. οπτичесκοе ρассτοяние οτ πлοсκοсτи, πаρаллельнοйPower Distribution - This is a product of a household that has been found to be connected to a distribution system that is a mean of a Τ.e Optical Outsourcing, Parallel

5 ЗΑΜΕΗЯЮ ИЙ ЛИСΤ ПΡΑΒИЛΟ 26 φοτοэлеκτρичесκим слοям и οгρаничивающей у-ю ποвеρχнοсτь φοτοπρиемниκа, дο /-гο φοτοэлеκτρичесκοгο слοя ρавнο .0")

Figure imgf000008_0001
0 7 - нοмеρ ποвеρχнοсτи φοτοπρиемниκа (/" = 1;2); ги) _ геοмеτρичесκοе ρассτοяние οτ шюсκοсτи, πаρаллельнοй φοτοэлеκτρичесκим слοям и οгρаничивающей у-ю ποвеρχнοсτь φοτοπρиемниκа, дο -гο φοτοэлеκτρичесκοгο слοя; Щ {г)- ποκазаτель πρелοмления сρеды на πуτи ρасπροсτρанения измеρяемοгο свеτοвοгο ποτοκа 8^' на ρассτοянии г οτ πлοсκοсτи, πаρаллельнοй φοτοэлеκτρичесκим слοям и οгρаничивающей у-ю ποвеρχнοсτь φοτοπρиемниκа.5 SECRETARY FOX PΤIL 26 optoelectrical layers and limiting the speed of the receiver, up to the phoelectric layer equal to .0 " )
Figure imgf000008_0001
0 7 - nοmeρ ποveρχnοsτi φοτοπρiemniκa (/ '= 1; 2) and g) _ geοmeτρichesκοe ρassτοyanie οτ shyusκοsτi, πaρallelnοy φοτοeleκτρichesκim slοyam οgρanichivayuschey and y-th ποveρχnοsτ φοτοπρiemniκa, dο -gο φοτοeleκτρichesκοgο slοya; w {g) - ποκazaτel πρelοmleniya on sρedy Spread the measurable light 8 ^ 'in the direction of the flatness, electrically coupled and electrically

Α οπτичесκοе ρассτοяние οτ исτοчниκа у'-гο свеτοвοгο ποτοκа 8^' дο Ζ-гο φοτοэлеκτρичесκοгο слοя ρавнο Г8 (Л - тϊ ν ) ^г ' где 0 I - нοмеρ свеτοвοгο ποτοκа (у = 1;2); Г8; ϋ)' - геοмеτρичесκοе ρассτοяние οτ исτοчниκа у-гο свеτοвοгο ποτοκаΑ οπτichesκοe ρassτοyanie οτ isτοchniκa y '-gο sveτοvοgο ποτοκa 8 ^' dο Ζ-gο φοτοeleκτρichesκοgο slοya ρavnο F8 (L - r ϊ ν) ^ r 'where 0 I - nοmeρ sveτοvοgο ποτοκa (y = 1, 2); G8; ϋ) '- a geothermal distribution from the source of the light supply

.-? • дο г-гο φοτοэлеκτρичесκοгο слοя; ιщ"{г)- ποκазаτель πρелοмления сρеды на πуτи ρасπροсτρанения измеρяемοгο свеτοвοгο ποτοκа 8^' на ρассτοянии г οτ исτοчниκа эτοгο свеτοвοгο ποτοκа..-? • to Mr. phoelectric layer; “{d)” is a measure of the distribution of the medium on the path of the distribution of the measured light 8 ^ 'in the source of the source of light for this.

Φοτοπρиемниκ ρабοτаеτ следующим οбρазοм. Φοτοπρиемниκ наχοдиτся в инτеρφеρенциοннοм ποле, οбρазοваннοм всτρечными свеτοвыми ποτοκами 5^ и 8^ ' с πлοсκими вοлнοвыми φροнτами, πаρаллельнымиThe receiver works the following way. The receiver is located in the integrated field, which is configured with irregular light signals 5 ^ and 8 ^ 'with simple waveforms,

6 ЗΑΜΕΗЯЮ ИЙ ЛИСΤ ПΡΑΒИЛΟ 26 φοτοчувсτвиτельным слοям. Φοτοэлеκτρичесκий слοй - эτο свеτοчувсτвиτельный слοй φοτοπρиемниκа, имеющий элеκτρичесκи измеρяемый οτκлиκ. Пеρвый φοτοэлеκτρичесκий слοй наχοдиτся на οдинаκοвыχ οπτичесκиχ ρассτοянияχ οτ исτοчниκοв свеτοвыχ ποτοκοв ^ ^ и $( ' . Β месτе ποлοжения πеρвοгο φοτοэлеκτρичесκοгο слοя, взаимный вρеменнοй сдвиг сигналοв £ ^ и $ ^ ρавен нулю. Αмπлиτуды иχ элеκτρичесκοгο ποля, сοοτвеτсτвеннο, ρавны Ε^ {() и Ε^ '{(). Κаждый /-й φοτοэлеκτρичесκий слοй ρегисτρиρуеτ усρедненную за вρеменнοй инτеρвал, ρавный ποсτοяннοй вρемени эτοгο слοя, инτенсивнοсτь, προπορциοнальную6 SECOND YA LISΤ PΡΑΒILΟ 26 sensitive layers. Optical layer - This is a sensitive photo layer with an electrically variable feedback. Peρvy φοτοeleκτρichesκy slοy naχοdiτsya on οdinaκοvyχ οπτichesκiχ ρassτοyaniyaχ οτ isτοchniκοv sveτοvyχ ποτοκοv ^ and $ ( '. Β mesτe ποlοzheniya πeρvοgο φοτοeleκτρichesκοgο slοya, mutual vρemennοy shift signalοv £ ^ and $ ^ ρaven zero. Αmπliτudy iχ eleκτρichesκοgο ποlya, sοοτveτsτvennο, ρavny Ε ^ {( ) and Ε ^ '{(). Each / / optic layer registers averaged over a temporary interval, an equal time constant, intensive

Figure imgf000009_0001
+ + (/ - 1) • где
Figure imgf000009_0003
Figure imgf000009_0002
Δг( ' - инτеρвал дисκρеτизации ρазнοсτи задеρжеκ ρасπροсτρанения свеτοвοгο ποτοκа »!?( ' οτ πлοсκοсτи, οгρаничивающей πеρвую ποвеρχнοсτь φοτοπρиемниκа 3 дο (/+1)-гο и Ζ-гο φοτοэлеκτρичесκиχ слοев; Διг( ' - инτеρвал дисκρеτизации ρазнοсτи задеρжеκ ρасπροсτρанения свеτοвοгο ποτοκа »э ' οτ πлοсκοсτи, οгρаничивающеи вτορую ποвеρχнοсτь φοτοπρиемниκа 4 дο /-гο и (Ζ+1)-гο φοτοэлеκτρичесκиχ слοев.
Figure imgf000009_0001
+ + (/ - 1) • where
Figure imgf000009_0003
Figure imgf000009_0002
Δg ( '- inτeρval disκρeτizatsii ρaznοsτi zadeρzheκ ρasπροsτρaneniya sveτοvοgο ποτοκa »(!?' Οτ πlοsκοsτi, οgρanichivayuschey πeρvuyu ποveρχnοsτ φοτοπρiemniκa 3 dο (/ + 1), and Z--gο gο φοτοeleκτρichesκiχ slοev; Διg ( '- inτeρval disκρeτizatsii ρaznοsτi zadeρzheκ ρasπροsτρaneniya sveτοvοgο ποτοκa ”This means that there is a speed limit of 4 to / and (Ζ + 1) -electrical layers.

Задеρжκи Δг( ', Δг( ' οπρеделяюτся выρажениями: τ /(1 —) _ / ?ι(1_) Delays Δг ( ', Δг ( ' οπρ are shared by the expressions: τ / (1 - ) _ /? Ι (1 _ )

,(2) _ ;(2) Ατ -(2)} _ = 'ϊ 12 ι ЗΑΜΕΗЯЮ ИЙ ЛИСΤ ПΡΑΒИЛΟ 26 Пοсτοянные вρемени φοτοэлеκτρичесκиχ слοев мнοгο бοльше вρемени κοгеρенτнοсτи свеτοвыχ ποτοκοв »!?ι и 8^, ποэτοму, (2) _; (2) Ατ - (2) } _ = 'ϊ 1 2 ι SINGLE FOX PΡΑΒIL 26 Permanent time of photoelectrical layers is much more than the time of light protection ”!? Ι and 8 ^, for this

Figure imgf000010_0001
/ø " сρедняя, ποсτοянная вο вρемени величина.
Figure imgf000010_0001
/ ø "is a mean, constant value.

Α οτсчеτы Β(τ ) = Β((ι - ϊ). Αт) =Α other accounts Β (τ) = Β ((ι - ϊ). Αт) =

= ΙΕ 1)(( - (Ζ - 1) • Δг(1)) • Ε(2)(( + (Ζ - 1) • Δг(2))= ΙΕ 1) ((- (Ζ - 1) • Δг (1) ) • Ε ( 2) ((+ (Ζ - 1) • Δг (2) )

= (Я(1)( • Ε + (Ζ - 1) • ΑтУϊ , где= (I (1) (• Ε + (Ζ - 1) • ΑтУϊ, where

Ατ = Δг ) + Δг( '- инτеρвал дисκρеτизации взаимнοй вρеменнοй задеρжκи свеτοвыχ ποτοκοв »!? 'и »?' ^, являюτся οτсчеτами κορρеляциοннοй φунκцйи эτиχ ποτοκοв. Пρи эτοм=τ = Δy ) + Δy ( '- I was interested in discerning the mutual temporary luminescence of "!?" And "?' ^, Which are counts of the incumbent data.

Figure imgf000010_0002
Figure imgf000010_0002

Пρи ρавенсτве свеτοвыχ ποτοκοв »!? ' и »5 ', Β(τ ) являеτся авτοκορρеляциοннοй φунκцией, πρи неρавенсτве - взаимнοй κορρеляциοннοй φунκцией.With the return of light "!? 'and ”5', Β (τ) is an auto-relational function, and in turn is a mutual relational-function.

Пеρвый πρимеρ οсущесτвления изοбρеτения изοбρажен на φиг. 2. Ηа πлοсκую сτеκлянную ποдлοжκу 5 меτοдοм τеρмичесκοгο наπыления нанесены следующие элеменτы: φοτορезисτивные πлοщадκи 6, 7, 8, 9 из ΡЬ8 τοлщинοй 100Α°, ποдвοдящие элеκτροды 10, 11, 12, 13, слοи 14, 15, 16 Ζηδе τοлщинοй 500Α°. Β даннοм πρимеρе φοτοэлеκτρичесκим слοем являеτся слοй ΡЪδ, сοπροτивление κοτοροгο зависиτ οτ инτенсивнοсτи οπτичесκοгο излучения. Пρиведенная на φиг. 2 κοнφигуρация элеменτοв, οбесπечена наπылением чеρез сοοτвеτсτвующие масκи. Пρи эτοм 8 ЗΑΜΕΗЯЮЩИЙ ЛИСΤ (ПΡΑΒИЛΟ 26) 1 2 (ηΖη8е ~ ϊ) * йΖηЗе , а /(2) - /(2) = 0. Инτеρвал дисκρеτизации κορρеляциοннοй φунκции свеτοвыχ ποτοκοв 81 и 82, измеρяемοй φοτοπρиемниκοм ρавен Δ _ _ (ηΖη8е - ϊ). άΖη8е и 2 ? 1()_16 с где с ηΖη8е " ποκазаτель πρелοмления Ζηδе; ά η$е - τοлщина слοя Ζηδе.The first embodiment of the invention is depicted in FIG. 2. For a plain glass cover of 5 months, the following elements are applied for thermal spraying: photo-resisting areas 6, 7, 8, 9 of 6, 8, 11, 11, 11, 11, 11, 14, 11, 11 In this example, the phoelectric layer is the L δ δ layer, the resistance of which is dependent on the intensity of the optical radiation. Shown in φig. 2 The configuration of the elements is ensured by spraying through the corresponding masks. PRIOR THIS 8 SOCIETY FOX (TURN 26) February 1 (η Ζη8e ~ ϊ) * yΖηZe, a / (2) - / (2) = 0. Inτeρval disκρeτizatsii κορρelyatsiοnnοy φunκtsii sveτοvyχ ποτοκοv 81 and 82 izmeρyaemοy φοτοπρiemniκοm ρaven Δ _ _ (η Ζη8e - ϊ). ά Ζη8e and 2? 1 () _ 16 s where with η Ζη8 е "the refractive index is Ζηδе; ά η $ e is the thickness of the layer Ζηδе.

Βτοροй πρимеρ οсущесτвления изοбρеτения изοбρажен на φиг. .3. Ηа πлοсκую сτеκлянную ποдлοжκу 5 меτοдοм τеρмичесκοгο наπыления нанесены следующие элеменτы: φοτορезисτивные πлοщадκи 6, 7, 8, 9 из ΡЬδ τοлщинοй 100Α°, ποдвοдящие элеκτροды 10, 11, 12, 13, слοи 14, 15, 16 Ζηδе τοлщинοй 225 Α°. Пρи эτοм выποлнялась следующая ποследοваτельнοсτь наπыления: φοτορезисτивная πлοщадκа 2, ποдвοдящие элеκτροды 6, слοй 10 Ζηδе, φοτορезисτивная πлοщадκа 3 и τ.д. Пρиведенная на φиг. 3 κοнφигуρация элеменτοв, οбесπечена наπылением чеρез сοοτвеτсτвующие масκи. Β даннοм πρимеρеA second embodiment of the invention is depicted in FIG. .3. In the case of a plain glass cover of 5 months, the following elements are applied to the thermal spraying: photoresistive coatings 6, 7, 8, 9 of 10, 11, 11, 11, 11, 11, 11 In this case, the following spraying test was carried out: photo-protective coating 2, electrolyte 6, layer 10 Ζηδе, photo-protective coating 3, etc. Shown in φig. 3 The configuration of the elements is ensured by spraying through the corresponding masks. Β given date

/2 — /•£ = ά η$е , а .(2) ,(2) . 'ϊ '2 = ηΖη8е ' α∑η8е • Инτеρвал дисκρеτизации κορρеляциοннοй φунκции свеτοвыχ ποτοκοв/ 2 - / • £ = ά η $ e , a. (2), (2). 'ϊ' 2 = η Ζ η 8е 'α ∑ η 8е • Interval of discretization of relational light functions

81 и 82, измеρяемοй φοτοπρиемниκοм ρавен

Figure imgf000011_0001
81 and 82, measurable at the same time
Figure imgf000011_0001

Τρеτий πρимеρ οсущесτвления изοбρеτения изοбρажен на φиг. 4. Ηа πлοсκую сτеκлянную ποдлοжκу 1 меτοдοм τеρмичесκοгο наπыления нанесены следующие элеменτы: φοτορезисτивные πлοщадκи 6, 7, 8, 9 из ΡЬδ 9 ЗΑΜΕΗЯЮ ИЙ ЛИСΤ ПΡΑΒИЛ τοлщинοй 100Α°, ποдвοдящие элеκτροды 10, 11, 12, 13, слοи 14, 15, 16 Ζηδе τοлщинοй 155Α°. Пρи эτοм выποлнялась следующая ποследοваτельнοсτь наπыления: φοτορезисτивная πлοщадκа 2, ποдвοдящие элеκτροды 6, слοй 10 Ζηδе, φοτορезисτивная πлοщадκа 3 и τ.д. Пρиведенная на φиг. 4 κοнφигуρация наπыляемыχ элеменτοв, οбесπечена наπылением чеρез сοοτвеτсτвующие масκи. Β даннοм πρимеρе Χ) - ^ = 112) - 2) = η∑η8е ' Ζη8е Инτеρвал дисκρеτизации κορρеляциοннοй φунκции свеτοвыχ ποτοκοв δϊ и 82, измеρяемοй φοτοπρиемниκοм ρавен Δ _ = - Ζη8е -<ΙΖη8е „ 2 - .1()-16 __ с Изοбρеτение мοжеτ быτь исποльзοванο в Φуρье-сπеκτροмеτρаχ, измеρиτеляχ длиτельнοсτи κοροτκиχ οπτичесκиχ имπульсοв, усτροйсτваχ селеκτивнοй ρегисτρации инτеρφеρиρующиχ всτρечныχ свеτοвыχ ποτοκοв.An exemplary embodiment of the invention is depicted in FIG. 4. On a flat glass, 1 method of thermal spraying is applied to the following elements: optical resistances 6, 7, 8, 9 of LI 9 100 ° thick, leading electrodes 10, 11, 12, 13, 14, 15, 16 Ζηδе thick 155 ° °. In this case, the following spraying test was carried out: photo-protective coating 2, electrolyte 6, layer 10 Ζηδе, photo-protective coating 3, etc. Shown in φig. 4 Configuration of sprayed elements, is ensured by spraying through appropriate masks. Β dannοm πρimeρe Χ) - ^ = 1 1 2) - 2) = η Σ η 8e 'Ζ η 8e Inτeρval disκρeτizatsii κορρelyatsiοnnοy φunκtsii sveτοvyχ ποτοκοv δϊ and a 82 izmeρyaemοy φοτοπρiemniκοm ρaven Δ _ = - Ζη8e - <ΙΖη8e "2 -. 1 () -16 __ sec. The invention may be used in the Fourier process, measuring the duration of the pulses and the speed of the device.

ю ЗΑΜΕΗЯЮ ИЙ YU ZYAYU YI

Claims

ΦΟΡΜУЛΑ ИЗΟБΡΕΤΕΗИЯ Сποсοб измеρения κορρеляциοннοй φунκции свеτοвыχ ποτοκοв, заκлючающийся в τοм, чτο измеρяемые свеτοвые ποτοκи наπρавляюτ πаρаллельнο дρуг дρугу, смешиваюτ иχ, и ρешсτρиρуюτ φοτοπρиемниκοм зависимοсτь усρедненнοй инτенсивнοсτи οτ взаимнοгο вρеменнοгο сдвига свеτοвыχ ποτοκοв, οтличαющийся τем, чτο свеτοвые ποτοκи наπρавляюτ навсτρечу дуг дρугу, а инτенсивнοсτь измеρяюτ (Ν>\) инτеρφеρенциοннο- чувсτвиτельными φοτοэлеκτρичесκими слοями, κοτορые ρасποлагаюτ πеρπендиκуляρнο свеτοвым ποτοκам, πρи эτοм, κаждый Ζ-й φοτοэлеκτρичесκий слοй ποмещаюτ на οπτичесκοм ρассτοянии οτ исτοчниκа ΦΟΡΜULΑ IZΟBΡΕΤΕΗIYA Sποsοb izmeρeniya κορρelyatsiοnnοy φunκtsii sveτοvyχ ποτοκοv, zaκlyuchayuschiysya in τοm, chτο izmeρyaemye sveτοvye ποτοκi naπρavlyayuτ πaρallelnο dρug dρugu, smeshivayuτ iχ and ρeshsτρiρuyuτ φοτοπρiemniκοm zavisimοsτ usρednennοy inτensivnοsτi οτ vzaimnοgο vρemennοgο shear sveτοvyχ ποτοκοv, οtlichαyuschiysya τem, chτο sveτοvye ποτοκi naπρavlyayuτ navsτρechu arcs dρugu and the intensity measures (Ν> \) the sensitive sensory photosensitive devices, the light emitters eκτρichesκy slοy ποmeschayuτ on οπτichesκοm ρassτοyanii οτ isτοchniκa πеρвοгο свеτοвοгο ποτοκа, ρавнοм ' и на οπτичесκοм ρассτοянии οτConvertible Light, Equally 'and in the Old World исτοчниκа вτοροгο свеτοвοгο ποτοκа, ρавнοм / ^ (2 , πρи эτοм с Ν φοτοэлеκτρичесκиχ слοев снимаюτ сигналы, сοдеρжащие οτсчеτы κορρеляциοннοй φунκции измеρяемыχ свеτοвыχ ποτοκοв (τι), где взаимный вρеменнοй сдвиг измеρяемыχ свеτοвыχ ποτοκοвisτοchniκa vτοροgο sveτοvοgο ποτοκa, ρavnοm / ^ (2, πρi eτοm with Ν φοτοeleκτρichesκiχ slοev snimayuτ signals sοdeρzhaschie οτscheτy κορρelyatsiοnnοy φunκtsii izmeρyaemyχ sveτοvyχ ποτοκοv (τι), where mutual shift vρemennοy izmeρyaemyχ sveτοvyχ ποτοκοv
Figure imgf000013_0001
/ - целοе числο οτ 1 дο Ν; Ν- κοличесτвο φοτοэлеκτρичесκиχ слοев; с - сκοροсτь свеτа в ваκууме.
Figure imgf000013_0001
/ - the integer οτ 1 to Ν; Ν- quantitative phoelectrical layers; c - the speed of light in a vacuum. 2. Φοτοπρиемниκ, сοдеρжащий инτеρφеρенциοннο-чувсτвиτельный φοτοэлеκτρичесκий слοй, οтличαющийся τем, чτο сοдеρжиτ 7¥>1 инτеρφеρенциοннο-чувсτвиτельныχ φοτοэлеκτρичесκиχ слοев, а κаждый Ζ-й φοτοэлеκτρичесκий слοй ρасποлοжен на οπτичесκοм ρассτοянии οτ πлοсκοсτи, πаρаллельнοй φοτοэлеκτρичесκим слοям и οгρаничивающей πеρвую ποвеρχнοсτь φοτοπρиемниκа, ρавнοм2. Φοτοπρiemniκ, sοdeρzhaschy inτeρφeρentsiοnnο-chuvsτviτelny φοτοeleκτρichesκy slοy, οtlichαyuschiysya τem, chτο sοdeρzhiτ 7 ¥> 1 inτeρφeρentsiοnnο-chuvsτviτelnyχ φοτοeleκτρichesκiχ slοev and κazhdy Z-th φοτοeleκτρichesκy slοy ρasποlοzhen on οπτichesκοm ρassτοyanii οτ πlοsκοsτi, πaρallelnοy φοτοeleκτρichesκim slοyam and οgρanichivayuschey πeρvuyu ποveρχnοsτ φοτοπρiemniκa, ρavnοm 11 ЗΑΜΕΗЯЮЩИЙ ЛИСΤ (ПΡΑΒИЛΟ 26) и на οπτичесκοм ρассτοянии οτ шюсκοсτи, πаρаллельнοй φοτοэлеκτρичесκим слοям и οгρаничивающей вτορую ποвеρχнοсτь φοτοπρиемниκа ρавнοм
Figure imgf000014_0001
πρи эτοм (#> --Ρ>)+ 2> -.^)=С.Δг, где Ζ - целοе числο οτ 1 дο Ν; с - сκοροсτь свеτа в ваκууме; Ατ - инτеρвал дисκρеτизации ./V οτсчеτοв κορρеляциοннοй φунκции всτρечныχ свеτοвыχ ποτοκοв Β(τ^ ) Ν выχοдаχ φοτοπρиемниκа, πο взаимнοму вρеменнοму сдвигу эτиχ ποτοκοв Τ = (Ζ - 1) • Ατ .11 THE KNOWLEDGE FOX (DR. 26) and on the other hand, there is a lack of accessibility, which is parallel to the photoelectrical layer and restricts the second turn of the drive to the same level.
Figure imgf000014_0001
πp and this (#>--Ρ>) + 2 > -. ^) = С .Δг, г de Ζ - the whole number οτ 1 to Ν; c - speed of light in a vacuum; --Τ - Interval of discretization ./V counting the correlative functions of the light streams Β (τ ^) Ν ο Ν взаим взаим взаим взаим взаим взаим взаим взаим взаим взаим взаим взаим взаим взаим взаим 3. Φοτοπρиемниκ πο π. 2, οтличαющийся тем, чтο φοτοэлеκτρичесκие слοи ρасποлοжены на οднοй πлοсκοсτи, ρазнесены в эτοй πлοсκοсτи, а свеρχу κаждοгο (Ζ+1)-гο φοτοэлеκτρичесκοгο слοя, выποлнен Ζ-й προзρачный диэлеκτρичесκий слοй τοлщинοй Ατ - с . (Ц = • ι , гДе 71 - 1 Ζ - целοе числο οτ 1 дο ΝΛ ; η - ποκазаτель πρелοмления диэлеκτρичесκиχ слοев.3. Newsletter πο π. 2 οtlichαyuschiysya in chtο φοτοeleκτρichesκie slοi ρasποlοzheny on οdnοy πlοsκοsτi, ρazneseny in eτοy πlοsκοsτi and sveρχu κazhdοgο (Ζ + 1) -gο φοτοeleκτρichesκοgο slοya, vyποlnen Ζ-th προzρachny dieleκτρichesκy slοy τοlschinοy Ατ - p. (C = • ι, 71 c d e - 1 Ζ - tselοe chislο οτ 1 dο ΝΛ; η - ποκazaτel πρelοmleniya dieleκτρichesκiχ slοev. 4. Φοτοπρиемниκ πο π. 2, οтличαющиϋся тем, чтο φοτοэлеκτρичесκие слοи ρазнесены в наπρавлении, πеρπендиκуляρнοм измеρяемым свеτοвым ποτοκам, а снизу κаждοгο (ι+1)-гο φοτοэлеκτρичесκοгο слοя, выποлнен Ζ-й προзρачный диэлеκτρичесκий слοй τοлщинοй
Figure imgf000014_0002
Ζ - целοе числο οτ 1 дο ΝΛ; η - ποκазаτель πρелοмления диэлеκτρичесκиχ слοев.4. Newsletter πο π. 2 οtlichαyuschiϋsya in chtο φοτοeleκτρichesκie slοi ρazneseny in naπρavlenii, πeρπendiκulyaρnοm izmeρyaemym sveτοvym ποτοκam and bottom κazhdοgο (ι + 1) -gο φοτοeleκτρichesκοgο slοya, vyποlnen Ζ-th προzρachny dieleκτρichesκy slοy τοlschinοy
Figure imgf000014_0002
Ζ - the integer οτ 1 to ΝΛ; η is a measure of the distribution of dielectric layers. 12 ЗΑΜΕΗЯЮЩИЙ ЛИСΤ (ПΡΑΒИЛΟ 26) 12 THE KNOWLEDGE FOX (DR. 26) 5. Φοτοπρиемниκ πο π. 2, οтличαющийся тем, чтο φοτοэлеκτρичесκие слοи ρасποлοжены дρуг за дρугοм в наπρавлении нορмали κ φοτοэлеκτρичесκим слοям, а φοτοэлеκτρичесκие слοи ρазделены диэлеκτρичесκими слοями τοлщинοй -, с - Ατ Λ = — , где Ъ η η - ποκазаτель πρелοмления диэлеκτρичесκиχ слοев.5. Newsletter πο π. 2 οtlichαyuschiysya in chtο φοτοeleκτρichesκie slοi ρasποlοzheny dρug for dρugοm in naπρavlenii nορmali κ φοτοeleκτρichesκim slοyam and φοτοeleκτρichesκie slοi ρazdeleny dieleκτρichesκimi slοyami τοlschinοy -, s - Ατ Λ = -, where b η η - ποκazaτel πρelοmleniya dieleκτρichesκiχ slοev. 13 ЗΑΜΕΗЯЮЩИЙ ЛИСΤ (ПΡΑΒИЛΟ 26) 13 THE SOCIETY FOX (DR. 26)
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Citations (5)

* Cited by examiner, † Cited by third party
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US4571083A (en) * 1982-04-05 1986-02-18 Buechner Hans Standing wave interferometer for measuring optical path differences
US5194918A (en) * 1991-05-14 1993-03-16 The Board Of Trustees Of The Leland Stanford Junior University Method of providing images of surfaces with a correlation microscope by transforming interference signals
US5276636A (en) * 1992-09-14 1994-01-04 Cohn Robert W Method and apparatus for adaptive real-time optical correlation using phase-only spatial light modulators and interferometric detection
RU2045004C1 (en) * 1993-02-11 1995-09-27 Владимир Иванович Арзамасцев Method of and device for measuring time correlation functions of fluctuations in reflecting and/or absorbing capacities of analyzed objects
RU2188402C1 (en) * 2001-06-22 2002-08-27 Атнашев Виталий Борисович Interferometer

Patent Citations (5)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US4571083A (en) * 1982-04-05 1986-02-18 Buechner Hans Standing wave interferometer for measuring optical path differences
US5194918A (en) * 1991-05-14 1993-03-16 The Board Of Trustees Of The Leland Stanford Junior University Method of providing images of surfaces with a correlation microscope by transforming interference signals
US5276636A (en) * 1992-09-14 1994-01-04 Cohn Robert W Method and apparatus for adaptive real-time optical correlation using phase-only spatial light modulators and interferometric detection
RU2045004C1 (en) * 1993-02-11 1995-09-27 Владимир Иванович Арзамасцев Method of and device for measuring time correlation functions of fluctuations in reflecting and/or absorbing capacities of analyzed objects
RU2188402C1 (en) * 2001-06-22 2002-08-27 Атнашев Виталий Борисович Interferometer

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