EP2010890A2 - Procede et systeme pour generer un resultat de mesure indiquant la presence d'une substance dans un echantillon sur la base d'une mesure spectrometrique - Google Patents
Procede et systeme pour generer un resultat de mesure indiquant la presence d'une substance dans un echantillon sur la base d'une mesure spectrometriqueInfo
- Publication number
- EP2010890A2 EP2010890A2 EP07702562A EP07702562A EP2010890A2 EP 2010890 A2 EP2010890 A2 EP 2010890A2 EP 07702562 A EP07702562 A EP 07702562A EP 07702562 A EP07702562 A EP 07702562A EP 2010890 A2 EP2010890 A2 EP 2010890A2
- Authority
- EP
- European Patent Office
- Prior art keywords
- intensity distribution
- spectral intensity
- light
- measurement
- substance
- 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.)
- Withdrawn
Links
- 238000005259 measurement Methods 0.000 title claims abstract description 60
- 238000000034 method Methods 0.000 title claims abstract description 31
- 239000000126 substance Substances 0.000 title claims abstract description 29
- 238000004519 manufacturing process Methods 0.000 title abstract 2
- 230000003595 spectral effect Effects 0.000 claims abstract description 51
- 238000009826 distribution Methods 0.000 claims abstract description 42
- 230000008569 process Effects 0.000 claims abstract description 4
- 238000010438 heat treatment Methods 0.000 claims abstract description 3
- 230000009102 absorption Effects 0.000 claims description 17
- 238000010521 absorption reaction Methods 0.000 claims description 17
- 230000006978 adaptation Effects 0.000 claims description 5
- 230000001419 dependent effect Effects 0.000 claims description 5
- 230000000052 comparative effect Effects 0.000 claims 1
- 238000010219 correlation analysis Methods 0.000 claims 1
- 238000005314 correlation function Methods 0.000 claims 1
- 230000001105 regulatory effect Effects 0.000 claims 1
- 230000003993 interaction Effects 0.000 abstract description 3
- 238000005286 illumination Methods 0.000 abstract description 2
- 230000002123 temporal effect Effects 0.000 abstract 1
- 239000000523 sample Substances 0.000 description 17
- 230000003287 optical effect Effects 0.000 description 8
- 230000008859 change Effects 0.000 description 4
- 239000012496 blank sample Substances 0.000 description 2
- 238000006073 displacement reaction Methods 0.000 description 2
- 238000013507 mapping Methods 0.000 description 2
- 102000001554 Hemoglobins Human genes 0.000 description 1
- 108010054147 Hemoglobins Proteins 0.000 description 1
- 230000003542 behavioural effect Effects 0.000 description 1
- 230000015572 biosynthetic process Effects 0.000 description 1
- 230000007613 environmental effect Effects 0.000 description 1
- 230000017525 heat dissipation Effects 0.000 description 1
- 230000035945 sensitivity Effects 0.000 description 1
Classifications
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01N—INVESTIGATING OR ANALYSING MATERIALS BY DETERMINING THEIR CHEMICAL OR PHYSICAL PROPERTIES
- G01N21/00—Investigating or analysing materials by the use of optical means, i.e. using sub-millimetre waves, infrared, visible or ultraviolet light
- G01N21/17—Systems in which incident light is modified in accordance with the properties of the material investigated
- G01N21/25—Colour; Spectral properties, i.e. comparison of effect of material on the light at two or more different wavelengths or wavelength bands
- G01N21/27—Colour; Spectral properties, i.e. comparison of effect of material on the light at two or more different wavelengths or wavelength bands using photo-electric detection ; circuits for computing concentration
- G01N21/274—Calibration, base line adjustment, drift correction
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01N—INVESTIGATING OR ANALYSING MATERIALS BY DETERMINING THEIR CHEMICAL OR PHYSICAL PROPERTIES
- G01N21/00—Investigating or analysing materials by the use of optical means, i.e. using sub-millimetre waves, infrared, visible or ultraviolet light
- G01N21/17—Systems in which incident light is modified in accordance with the properties of the material investigated
- G01N21/25—Colour; Spectral properties, i.e. comparison of effect of material on the light at two or more different wavelengths or wavelength bands
- G01N21/31—Investigating relative effect of material at wavelengths characteristic of specific elements or molecules, e.g. atomic absorption spectrometry
- G01N21/35—Investigating relative effect of material at wavelengths characteristic of specific elements or molecules, e.g. atomic absorption spectrometry using infrared light
- G01N21/359—Investigating relative effect of material at wavelengths characteristic of specific elements or molecules, e.g. atomic absorption spectrometry using infrared light using near infrared light
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01N—INVESTIGATING OR ANALYSING MATERIALS BY DETERMINING THEIR CHEMICAL OR PHYSICAL PROPERTIES
- G01N21/00—Investigating or analysing materials by the use of optical means, i.e. using sub-millimetre waves, infrared, visible or ultraviolet light
- G01N21/17—Systems in which incident light is modified in accordance with the properties of the material investigated
- G01N21/25—Colour; Spectral properties, i.e. comparison of effect of material on the light at two or more different wavelengths or wavelength bands
- G01N21/31—Investigating relative effect of material at wavelengths characteristic of specific elements or molecules, e.g. atomic absorption spectrometry
- G01N21/314—Investigating relative effect of material at wavelengths characteristic of specific elements or molecules, e.g. atomic absorption spectrometry with comparison of measurements at specific and non-specific wavelengths
- G01N2021/3144—Investigating relative effect of material at wavelengths characteristic of specific elements or molecules, e.g. atomic absorption spectrometry with comparison of measurements at specific and non-specific wavelengths for oxymetry
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01N—INVESTIGATING OR ANALYSING MATERIALS BY DETERMINING THEIR CHEMICAL OR PHYSICAL PROPERTIES
- G01N21/00—Investigating or analysing materials by the use of optical means, i.e. using sub-millimetre waves, infrared, visible or ultraviolet light
- G01N21/17—Systems in which incident light is modified in accordance with the properties of the material investigated
- G01N21/25—Colour; Spectral properties, i.e. comparison of effect of material on the light at two or more different wavelengths or wavelength bands
- G01N21/31—Investigating relative effect of material at wavelengths characteristic of specific elements or molecules, e.g. atomic absorption spectrometry
- G01N21/314—Investigating relative effect of material at wavelengths characteristic of specific elements or molecules, e.g. atomic absorption spectrometry with comparison of measurements at specific and non-specific wavelengths
- G01N2021/3181—Investigating relative effect of material at wavelengths characteristic of specific elements or molecules, e.g. atomic absorption spectrometry with comparison of measurements at specific and non-specific wavelengths using LEDs
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01N—INVESTIGATING OR ANALYSING MATERIALS BY DETERMINING THEIR CHEMICAL OR PHYSICAL PROPERTIES
- G01N2201/00—Features of devices classified in G01N21/00
- G01N2201/12—Circuits of general importance; Signal processing
- G01N2201/121—Correction signals
- G01N2201/1211—Correction signals for temperature
Definitions
- the invention is directed to a method and apparatus for generating a measurement result indicative of the presence or concentration of a substance within a sample based on a spectrometric measurement, wherein light is emitted from a source to that sample as part of an exposure phase, and in interaction with This sample is recorded with respect to the spectral intensity distribution of this sample, and the presence of a substance is determined in the context of electronic measurement signal processing, including the spectral intensity distribution of the detected light.
- the signal of the sample is promptly (relative to the drift of the apparatus) obtained signal of a blank or white light reference divided.
- the intensity and the spectral distribution of the source must be identical in the above method when taking the signal of the sample and when receiving the signal of the zero sample. Deviation immediately leads to an error in determining the properties of the sample.
- the simultaneous, mutual e.g. also partial recording of the signal of the sample and the blank sample allows the use of sources that need only be stable for the duration of a change cycle.
- the intensity signal obtained at the same time by means of a non-spectrally sensitive detector can be used to compensate for the intensity fluctuations of the source, provided the spectral characteristics of the source and the detector or the system of source and Detector, for example, by a timely recording of the zero sample signal known and stable.
- the invention has for its object to provide solutions by which it is possible to allow a reliable determination of the concentration of a substance in a spectrometric manner, the corresponding measurement without recording a reference measurement in close proximity to the measurement and without a preliminary phase to stabilize the Device can be handled within a relatively short time.
- This object is according to a first aspect of the invention solved by a method for generating a measurement result indicative of the presence of a substance within a sample on the basis of a spectrometric measurement, in which
- a compensation function is processed, which takes into account dependencies of the spectral intensity distribution of the light emitted by the light source of the temperature of the LED.
- the measurement can be carried out directly with the ambient tempered device.
- the indicative of the spectral intensity distribution of the light emitted by the light source indicative data can be generated in an advantageous manner within a calibration step.
- a reference measurement is performed on a substantially known object (white reference).
- the measurement result is canceled in any form.
- the term "G *" is a unique function, it can be obtained from the difference of the logarithms of two reference measurements and then only has to be scaled or shifted in wavelength depending on the specific temperature differences.
- Fig.l Measurements of two temperatures in digital units. From these curves, a compensation function is generated.
- Fig.3 The difference between the curves in Figure 2. This curve can be used as a compensation function.
- the pattern to be recognized is an artifact of the directional dependence of the spectral characteristic of the LED used. This can be eliminated by appropriate measures on the illumination optics used.
- the compensation function can be adjusted to a temperature offset determined therefrom on the basis of the correlation of the spectral intensity distribution of the light emitted by the light source with the spectral intensity distribution of the detected light.
- the compensation function can also be further tuned by additional auxiliary parameters. These auxiliary parameters can be determined from a correlation of the measured values with reference values. It is also possible to carry out further adjustments, in particular scaling of the data for the spectral intensity distribution of the light emitted by the light source and / or the spectral intensity distribution of the detected light.
- the task may also be: search the parameters of the model functions so that the entire modal function reproduces the measured data as well as possible.
- the model functions are given by the absorptions of the substances of the sample and - the clou '- the compensation function function.
- the parameters are the concentrations and scaling of the shift of the compensation function function with respect to the wavelength.
- an arbitrarily complex mapping (more than scaling and shifting) of the compensation function function to the concrete compensation function function can also exist; then the elements describing this figure were parameters to be determined.
- the "correct model” and the measurement data correlate better with each other than a “wrong model” and the measurement data.
- the LED is operated with a defined flow stream.
- the LED can be operated under a compensated by the compensation function temperature increase.
- the LED structure can be operated with connection to a heat sink.
- the parameters belonging to a uniform compensation function simultaneously with the determination of the parameters
- the substance-specific absorption can be determined in the context of a mathematical adaptation and in this way to compensate for the influence of the temperature. This is basically the core of the process.
- the determination of the substance-specific absorptions can furthermore be carried out by determining, within predetermined temperature ranges, the parameters belonging to a uniform compensation function using a possible given mathematical independence sequentially for the determination of the parameters of the substance-specific absorption and in this way compensating the influence of the temperature.
- LED light-emitting diodes
- a spectrometer Using light-emitting diodes (LED) and a spectrometer, the influence of various substances in human tissue such as. Hemoglobin on the absorption wavelength dependent to be examined to allow statements about concentrations of the substances in question in the tissue to be examined.
- the erfmdungsgeschreib working measuring device can be used without explicit reference measurement and without any special waiting time before the actual measurement.
- the absorption can be measured directly by determining the decadic logarithm ⁇ of the ratio of the energies of the light emitted by the source in the relevant wavelength interval (or frequency interval) to those detected on a sensor in the relevant wavelength interval, in the sequence as optical density (OD); the absorption, which is due to the presence is caused by the difference in optical density in the presence and absence of the substance in question.
- the spectrally resolved measurement makes it possible to deduce the absorption caused by certain substances by determining the wavelength-dependent course of the optical density, even if the optical density is known only up to a wavelength-independent constant (offset).
- the absorptions caused by the respective substances can be determined.
- Necessary condition is that the spectral distribution of the energy of the light source is identical in measurement and underlying.
- the LEDs are mounted in such a way that the heating of the LED during a measurement can be neglected due to a particularly good heat dissipation, so that substantially only the ambient conditions have an influence on the temperature of the active layer of the LED.
- the LED property demanded and used according to the invention is that the difference of the logarithms of the spectral intensity distributions at any temperature within a permissible range of application and the temperature at which a reference measurement is carried out can be represented in a sufficiently good approximation with respect to the measurement application a compensation function in conjunction with a simple illustration.
- the LEDs are selected so that the said compensation function is determined by the difference of the logarithms of the spectral intensity distribution. or by the spectral distribution of the differences of the logarithms of each wavelength interval to the spectral intensity proportional magnitudes, which are recorded at two different suitable temperatures and that said simple mapping consists of a scaling and a displacement m of the wavelength.
- the spectral intensity is related to frequency intervals and the compensation function is printed as a function of frequency.
- the determination of the absorptions caused by the substances of interest from a measurement with a suitable device by a good adaptation to the falsified due to the temperature difference between a single reference measurement and actual measurement optical density from the relevant absorption functions of the functions of interest and the compensation function in combination with the associated figure is searched.
- the parameters that uniquely determine the figure are free parameters of the adaptation.
- the figure consists of a scaling and shift in the wavelength: here both the shift of the compensation function with respect to the wavelength and the scaling factor of the compensation function are free parameters of the adaptation.
- a selection of the LED can be such that the temperature-dependent change in the spectral intensity in the spectral range to be considered is as small as possible. Furthermore, a selection of the LED, such that the associated compensation function in the spectral range under consideration with respect to the determination of the parameters of all functions to be adapted as independent as possible of the absorption functions of the substances of interest, ie, that just adapting only the compensation function to the measured optical density almost correct parameters with respect to displacement and scaling results, be advantageous.
Landscapes
- Physics & Mathematics (AREA)
- Spectroscopy & Molecular Physics (AREA)
- Analytical Chemistry (AREA)
- Biochemistry (AREA)
- Pathology (AREA)
- Health & Medical Sciences (AREA)
- Life Sciences & Earth Sciences (AREA)
- Chemical & Material Sciences (AREA)
- Immunology (AREA)
- General Physics & Mathematics (AREA)
- General Health & Medical Sciences (AREA)
- Theoretical Computer Science (AREA)
- Engineering & Computer Science (AREA)
- Mathematical Physics (AREA)
- Investigating Or Analysing Materials By Optical Means (AREA)
- Spectrometry And Color Measurement (AREA)
Abstract
Applications Claiming Priority (2)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
DE200510063263 DE102005063263A1 (de) | 2005-12-30 | 2005-12-30 | Verfahren und System zur Generierung eines hinsichtlich der Präsenz eines Stoffes innerhalb einer Probe indikativen Messergebnisses auf Grundlage einer spektrometrischen Messung |
PCT/EP2007/000012 WO2007077208A2 (fr) | 2005-12-30 | 2007-01-02 | Procede et systeme pour generer un resultat de mesure indiquant la presence d'une substance dans un echantillon sur la base d'une mesure spectrometrique |
Publications (1)
Publication Number | Publication Date |
---|---|
EP2010890A2 true EP2010890A2 (fr) | 2009-01-07 |
Family
ID=38135799
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
EP07702562A Withdrawn EP2010890A2 (fr) | 2005-12-30 | 2007-01-02 | Procede et systeme pour generer un resultat de mesure indiquant la presence d'une substance dans un echantillon sur la base d'une mesure spectrometrique |
Country Status (3)
Country | Link |
---|---|
EP (1) | EP2010890A2 (fr) |
DE (1) | DE102005063263A1 (fr) |
WO (1) | WO2007077208A2 (fr) |
Families Citing this family (5)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
EP2010875A1 (fr) * | 2006-04-19 | 2009-01-07 | Opsolution Spectroscopic Systems GmbH | Procédé pour compenser des variations de température de source lumineuse dans des spectromètres |
EP2218472B2 (fr) * | 2009-02-11 | 2022-03-16 | B. Braun Avitum AG | Dispositif destiné au traitement du sang extracorporel |
CN101806743B (zh) * | 2010-03-16 | 2012-10-31 | 李华 | 便携式广谱分光光度液体微量元素检测仪及检测方法 |
EP2511693A1 (fr) * | 2011-04-13 | 2012-10-17 | F. Hoffmann-La Roche AG | Système d'analyse avec source lumineuse contrôlée spectralement |
DE102017108552B4 (de) | 2017-04-21 | 2018-11-15 | ams Sensors Germany GmbH | Spektrometrischer Messkopf mit mehreren Transmissionslicht-Eintrittsfenstern |
Family Cites Families (2)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US5477853A (en) * | 1992-12-01 | 1995-12-26 | Somanetics Corporation | Temperature compensation method and apparatus for spectroscopic devices |
GB0322545D0 (en) * | 2003-09-26 | 2003-10-29 | Whitland Res Ltd | Measurement of blood oxygen saturation (SO2) |
-
2005
- 2005-12-30 DE DE200510063263 patent/DE102005063263A1/de not_active Withdrawn
-
2007
- 2007-01-02 WO PCT/EP2007/000012 patent/WO2007077208A2/fr active Application Filing
- 2007-01-02 EP EP07702562A patent/EP2010890A2/fr not_active Withdrawn
Non-Patent Citations (1)
Title |
---|
See references of WO2007077208A3 * |
Also Published As
Publication number | Publication date |
---|---|
WO2007077208A2 (fr) | 2007-07-12 |
DE102005063263A1 (de) | 2007-07-05 |
WO2007077208A3 (fr) | 2008-01-10 |
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Legal Events
Date | Code | Title | Description |
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PUAI | Public reference made under article 153(3) epc to a published international application that has entered the european phase |
Free format text: ORIGINAL CODE: 0009012 |
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17P | Request for examination filed |
Effective date: 20081118 |
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AK | Designated contracting states |
Kind code of ref document: A2 Designated state(s): AT BE BG CH CY CZ DE DK EE ES FI FR GB GR HU IE IS IT LI LT LU LV MC NL PL PT RO SE SI SK TR |
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RIN1 | Information on inventor provided before grant (corrected) |
Inventor name: KRIEG, JUERGEN Inventor name: SANDHAGEN, CARL Inventor name: WILLEMER, WINFRIED |
|
DAX | Request for extension of the european patent (deleted) | ||
17Q | First examination report despatched |
Effective date: 20130213 |
|
RAP1 | Party data changed (applicant data changed or rights of an application transferred) |
Owner name: OPSOLUTION SPECTROSCOPIC SYSTEMS GMBH Owner name: BIOZOOM TECHNOLOGIES INC. |
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STAA | Information on the status of an ep patent application or granted ep patent |
Free format text: STATUS: THE APPLICATION IS DEEMED TO BE WITHDRAWN |
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18D | Application deemed to be withdrawn |
Effective date: 20150801 |