WO2002063258A1 - Procede de spectrometrie et dispositif pour mettre en oeuvre ce procede - Google Patents

Procede de spectrometrie et dispositif pour mettre en oeuvre ce procede Download PDF

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Publication number
WO2002063258A1
WO2002063258A1 PCT/RU2001/000305 RU0100305W WO02063258A1 WO 2002063258 A1 WO2002063258 A1 WO 2002063258A1 RU 0100305 W RU0100305 W RU 0100305W WO 02063258 A1 WO02063258 A1 WO 02063258A1
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WO
WIPO (PCT)
Prior art keywords
light
source
shτρiχami
chasτichnο
vοlny
Prior art date
Application number
PCT/RU2001/000305
Other languages
English (en)
Russian (ru)
Inventor
Vitaly Atnashev
Alexei Atnashev
Pavel Atnashev
Original Assignee
Vitaly Atnashev
Alexei Atnashev
Pavel Atnashev
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 Vitaly Atnashev, Alexei Atnashev, Pavel Atnashev filed Critical Vitaly Atnashev
Publication of WO2002063258A1 publication Critical patent/WO2002063258A1/fr

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Classifications

    • G—PHYSICS
    • G01—MEASURING; TESTING
    • G01J—MEASUREMENT OF INTENSITY, VELOCITY, SPECTRAL CONTENT, POLARISATION, PHASE OR PULSE CHARACTERISTICS OF INFRARED, VISIBLE OR ULTRAVIOLET LIGHT; COLORIMETRY; RADIATION PYROMETRY
    • G01J3/00—Spectrometry; Spectrophotometry; Monochromators; Measuring colours
    • G01J3/28—Investigating the spectrum
    • G01J3/45—Interferometric spectrometry

Definitions

  • the invention is subject to the field of complex analysis and may be used for the direct analysis of light emission.
  • the classic way of analyzing light emission is included in the expansion of the light beam with the aid of a separate distribution system.
  • One of the classic devices used for this purpose is
  • An interface is known that contains an optical coupled source of light, reflective mirrors, a separate plate, a connector and a socket [Herz L. Integrated in the process of conversion. ⁇ .: ⁇ Economics ⁇ , 1969, pp. 80-83].
  • the angle ⁇ between the flatness of the diffuse lattice and the wavefront light wave is set from the situation: from ⁇ ⁇ ⁇ / 2 ⁇ where ⁇ is the light length; ⁇ - front end of the transverse structure equal to the length of the ultrasonic wave.
  • s ⁇ de ⁇ zhaschy ⁇ iches ⁇ i s ⁇ yazhennye is ⁇ chni ⁇ sve ⁇ v ⁇ g ⁇ radiation ⁇ azhayuschee ze ⁇ al ⁇ , s ⁇ e ⁇ analiza ⁇ and ⁇ e ⁇ i ⁇ diches ⁇ uyu ⁇ eshe ⁇ cha ⁇ uyu s ⁇ u ⁇ u ⁇ u, w ⁇ b ⁇ az ⁇ vannuyu sh ⁇ i ⁇ ami ⁇ n ⁇ g ⁇ chas ⁇ ichn ⁇ ⁇ us ⁇ ayuscheg ⁇ ⁇ ele ⁇ iches ⁇ g ⁇ sl ⁇ ya and ⁇ l ⁇ sami, ⁇ as ⁇ l ⁇ zhennymi between sh ⁇ i ⁇ ami ⁇ e ⁇ i ⁇ diches ⁇ y ⁇ esho ⁇ cha ⁇ y s ⁇ u ⁇ u ⁇ y, ⁇ i e ⁇ m u ⁇ myanu ⁇ aya ⁇ e ⁇ i ⁇ diches ⁇ aya
  • Discharging mirror and industrial disintegrated structure are made with the possibility of displacing the other friend of the friend.
  • An interface containing an optical coupled source of light, a short-circuiting source of radiation, an external process, and a short-circuiting process.
  • the deflecting deflector is executed in the form of a defective impairment applied to the rear side of the back of the player, and the enlarged one is enlarged.
  • the other way round is the disassembled structure of the device in the form of a photomultiplier of the multiplier.
  • Disposable mirror and accessories optionally incorporates a front-mounted dissipated structure sh ⁇ i ⁇ ami ⁇ n ⁇ g ⁇ chas ⁇ ichn ⁇ ⁇ us ⁇ ayugtseg ⁇ sl ⁇ ya a ⁇ ivn ⁇ y s ⁇ edy, ⁇ lu ⁇ z ⁇ achn ⁇ e ze ⁇ al ⁇ , v ⁇ e ⁇ azhayuschee ze ⁇ al ⁇ and ⁇ a ⁇ zhe ⁇ iches ⁇ i s ⁇ yazhennye v ⁇ y is ⁇ chni ⁇ sve ⁇ v ⁇ g ⁇ radiation v ⁇ uyu ⁇ e ⁇ i ⁇ diches ⁇ uyu ⁇ eshe ⁇ cha ⁇ uyu s ⁇ u ⁇ u ⁇ u, ⁇ b ⁇ az ⁇ vannuyu 5 sh ⁇ i ⁇ ami ⁇ n ⁇ g ⁇ chas ⁇ ichn ⁇ ⁇ us ⁇ ayuscheg ⁇ sl ⁇ ya a ⁇ ivn ⁇ y s ⁇ edy, ⁇ e
  • FIG. 1- Integrated circuit with integrated design
  • FIG. 2 an inter- face circuitry with an ultrasound diffractory interconnecting a portable plate from a non-compliant portion of it on fig.Z- practical plate from a piezoelectric, executed in the form of an optical wedge; in Fig.
  • the circuit of the interface, the ultrasonic diffracted lattice of the processor is made in the form of a factor of 15 optoelectronic multiplier; on ⁇ ig.5- s ⁇ ema in ⁇ e ⁇ e ⁇ me ⁇ a with ⁇ e ⁇ i ⁇ diches ⁇ y ⁇ esho ⁇ cha ⁇ y s ⁇ u ⁇ u ⁇ y, sh ⁇ i ⁇ i ⁇ y vy ⁇ lneny of ⁇ n ⁇ g ⁇ chas ⁇ ichn ⁇ ⁇ us ⁇ ayuscheg ⁇ ⁇ lyuminestsen ⁇ n ⁇ g ⁇ sl ⁇ ya on ⁇ ig.6- s ⁇ ema in ⁇ e ⁇ e ⁇ me ⁇ a with d ⁇ lni ⁇ elnym 20 u ⁇ avlyayuschim luch ⁇ m.
  • the version 1 (Fig. 1) contains an optimized 25 source of 1 light emitting reflecting radiation.
  • 2 s ⁇ e ⁇ analiza ⁇ 3 ⁇ e ⁇ i ⁇ diches ⁇ uyu ⁇ esho ⁇ cha ⁇ uyu s ⁇ u ⁇ u ⁇ u 4, 5 ⁇ b ⁇ az ⁇ vannuyu sh ⁇ i ⁇ ami ⁇ n ⁇ g ⁇ chas ⁇ ichn ⁇ ⁇ us ⁇ ayuscheg ⁇ ⁇ ele ⁇ iches ⁇ g ⁇ sl ⁇ ya ⁇ l ⁇ sami and 6, between ⁇ as ⁇ l ⁇ zhennymi sh ⁇ i ⁇ ami 5 ⁇ e ⁇ i ⁇ diches ⁇ y ⁇ esho ⁇ cha ⁇ y s ⁇ u ⁇ u ⁇ y 4.
  • Sve ⁇ v ⁇ y ⁇ ⁇ is ⁇ chni ⁇ a 1 sve ⁇ v ⁇ g ⁇ radiation ⁇ s ⁇ u ⁇ ae ⁇ on ⁇ azhayuschee ze ⁇ al ⁇ 2 ⁇ azhae ⁇ sya ⁇ neg ⁇ and a s ⁇ yachey sve ⁇ v ⁇ y v ⁇ lny ⁇ s ⁇ u ⁇ ae ⁇ on ⁇ e ⁇ i ⁇ diches ⁇ uyu ⁇ esho ⁇ cha ⁇ uyu s ⁇ u ⁇ u ⁇ u 4 za ⁇ em de ⁇ e ⁇ i ⁇ ue ⁇ sya and a signal ele ⁇ iches ⁇ g ⁇
  • This method is intended for dividing the fixed wavelengths of light.
  • In ⁇ e ⁇ e ⁇ me ⁇ s ⁇ de ⁇ zhi ⁇ ⁇ iches ⁇ i s ⁇ yazhennye is ⁇ chni ⁇ 1 sve ⁇ v ⁇ g ⁇ radiation ⁇ azhayuschee ze ⁇ al ⁇ 2, 3 and s ⁇ e ⁇ analiza ⁇ ul ⁇ azvu ⁇ vuyu di ⁇ a ⁇ tsi ⁇ nnuyu ⁇ esho ⁇ u 4.
  • the losing mirror 2 was made in the form of a losing 15 damage applied to the rear side of the playing plate 9 from the piezoelectronic, and the final payment was 9 (exceeded).
  • the retractable structure 4 is also implemented as a photocell of the multiplier 13 with diodes 14 and 20 of anode 15 (Fig. 4).
  • the light output of the source 1 of the light emission is emitted from the reflective mirror 2, it is neglected and in the form of a free light.
  • a selectable sectoral line ⁇ exists or by setting the ultrasound diffraction pattern ⁇ . or by setting the angle ⁇ .
  • a power multiplier 13 (Fig. 4) is plugged in ⁇ ele ⁇ ny, vybi ⁇ ye of uzl ⁇ v de ⁇ matsii ⁇ n ⁇ g ⁇ chas ⁇ ichn ⁇ ⁇ z ⁇ achn ⁇ g ⁇ ⁇ ez ⁇ chuvs ⁇ vi ⁇ eln ⁇ g ⁇ sl ⁇ ya 10 ul ⁇ azvu ⁇ v ⁇ y di ⁇ a ⁇ tsi ⁇ nn ⁇ y ⁇ eshe ⁇ i 4 usilivayu ⁇ sya din ⁇ da ⁇ at 14 and 15.
  • the instrument contains an optical source of 1 light emitting 2 sources of light, and doesn’t carry out an analysis of 3;
  • s ⁇ de ⁇ zhi ⁇ ⁇ iches ⁇ i s ⁇ yazhennye ⁇ e ⁇ vy is ⁇ chni ⁇ 1 sve ⁇ v ⁇ g ⁇ radiation ⁇ e ⁇ v ⁇ e ⁇ azhayuschee ze ⁇ al ⁇ 2, 25 ⁇ de ⁇ e ⁇ 16 ⁇ e ⁇ vuyu ⁇ e ⁇ i ⁇ diches ⁇ uyu ⁇ eshe ⁇ cha ⁇ uyu s ⁇ u ⁇ u ⁇ u 4, 5 ⁇ b ⁇ az ⁇ vannuyu sh ⁇ i ⁇ ami ⁇ n ⁇ g ⁇ chas ⁇ ichn ⁇ ⁇ us ⁇ ayuscheg ⁇ sl ⁇ ya a ⁇ ivn ⁇ y s ⁇ edy, ⁇ lu ⁇ z ⁇ achn ⁇ e ze ⁇ al ⁇ 17 v ⁇ e ⁇ azhayuschee ze ⁇ al ⁇ 18 and ⁇ a ⁇ zhe ⁇ iches ⁇ i s ⁇ yazhennye v ⁇ y is ⁇ chni
  • the output from the generation mode Resonance system 19 implements by cutting off the light from the source of 1 or 1 'light emission. In this case, one of the light sources 1 or D plays the part of the amplifying signal, and the second is switched. 5 In general, this tool can be operated as an optical commutator.

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  • Physics & Mathematics (AREA)
  • Spectroscopy & Molecular Physics (AREA)
  • General Physics & Mathematics (AREA)
  • Optical Modulation, Optical Deflection, Nonlinear Optics, Optical Demodulation, Optical Logic Elements (AREA)
  • Investigating Or Analysing Materials By Optical Means (AREA)

Abstract

Le procédé est caractérisé en ce que l'enregistrement des systèmes de noeuds et d'antinoeuds de la tension du champ électrique d'une onde optique stationnaire s'effectue sur une structure périodique à grille formée par les traits d'une couche photoélectrique ou photoluminescente fine partiellement transparente et les bandes disposes entre les traits. L'angle entre le plan de la structure périodique à grille et le front d'ondes de l'onde optique est défini selon la relation suivante: sin Ø=μ/2d, μ étant la longueur d'onde optique et d étant la période de la structure périodique à grille. Ce procédé est mis en oeuvre au moyen des interféromètres dotés d'une structure périodique photosensible à grille, située entre une source de rayonnement optique et un miroir réfléchissant. Lesdits interféromètres servent pour déterminer les longueurs fixes des ondes optiques, balayer un domaine spectral prédéterminé ils peuvent également fonctionner comme un dispositif optoélectronique et comme un commutateur optique.
PCT/RU2001/000305 2000-12-04 2001-07-25 Procede de spectrometrie et dispositif pour mettre en oeuvre ce procede WO2002063258A1 (fr)

Applications Claiming Priority (2)

Application Number Priority Date Filing Date Title
RU2000130502 2000-12-04
RU2000130502/28A RU2177605C1 (ru) 2000-12-04 2000-12-04 Способ спектрометрии и устройство для его осуществления (варианты)

Publications (1)

Publication Number Publication Date
WO2002063258A1 true WO2002063258A1 (fr) 2002-08-15

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WO (1) WO2002063258A1 (fr)

Families Citing this family (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
AU2003227389A1 (en) * 2002-08-26 2004-03-11 Vitaliy Atnashev Spectrometry method and device for carrying out said method
RU2477854C2 (ru) * 2011-06-22 2013-03-20 Общество с ограниченной ответственностью "Газпром трансгаз Махачкала" Способ контроля материалов методом резонансной ультразвуковой спектроскопии

Citations (6)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
DE1623277A1 (de) * 1966-07-18 1971-02-25 Perkin Elmer Corp Interferometer,insbesondere zur Laengenmessung
GB1233597A (fr) * 1967-06-02 1971-05-26
US3947780A (en) * 1974-10-21 1976-03-30 Mcdonnell Douglas Corporation Acoustooptic mode-locker frequency doubler
GB2146766A (en) * 1983-09-14 1985-04-24 Plessey Co Plc Acousto optic spectrum analysers
RU2149510C1 (ru) * 1999-01-19 2000-05-20 Таганрогский государственный радиотехнический университет Высокоточный акустооптический приемник-частотомер
RU2153680C1 (ru) * 1999-01-19 2000-07-27 Таганрогский государственный радиотехнический университет Акустооптический приемник-частотомер

Patent Citations (6)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
DE1623277A1 (de) * 1966-07-18 1971-02-25 Perkin Elmer Corp Interferometer,insbesondere zur Laengenmessung
GB1233597A (fr) * 1967-06-02 1971-05-26
US3947780A (en) * 1974-10-21 1976-03-30 Mcdonnell Douglas Corporation Acoustooptic mode-locker frequency doubler
GB2146766A (en) * 1983-09-14 1985-04-24 Plessey Co Plc Acousto optic spectrum analysers
RU2149510C1 (ru) * 1999-01-19 2000-05-20 Таганрогский государственный радиотехнический университет Высокоточный акустооптический приемник-частотомер
RU2153680C1 (ru) * 1999-01-19 2000-07-27 Таганрогский государственный радиотехнический университет Акустооптический приемник-частотомер

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