Method and Apparatus for Analyte Measurement Including Material Status Analysis
AssigneeDiaMonTech AG
InventorsWerner Mäntele, Thorsten Lubinski, Sergius Janik, Michael Kaluza
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AssigneeDiaMonTech AG
InventorsWerner Mäntele, Thorsten Lubinski, Sergius Janik, Michael Kaluza
Estimating the term…
A method of analyzing a material (12) comprising at least one analyte, said method comprising a material status analyzing procedure (76), in which a present status of the material is analyzed, wherein based on a result of said material status analyzing procedure (76), at least one of a selection of analyte-characteristic-wavelengths used during an analyte measurement procedure (78), an absolute time or a relative time proportion of use of analyte-characteristic-wavelengths during said analyte measurement procedure (78), an individual excitation radiation intensity, or a relative weight given to the wavelengths in the analysis, a selection of analyte-characteristic-wavelengths to be used simultaneously during said analyte measurement procedure (78), and a selection of one or more main frequencies of the modulation of said excitation radiation (18) intensity to be used during said analyte measurement procedure (78) is determined.
A method of analyzing a material (12) comprising at least one analyte, said method comprising
The method of claim one of the preceding claims, wherein the thermal or pressure transmitting contact between the material and the measurement body (16) is maintained during a time interval including at least part of said material status analyzing procedure (76) and the analyte measurement procedure (78).
The method of one of the preceding claims, wherein said material status comprises a presence and/or concentration of perturbing substances within said material that are different from said one or more analytes but exhibit significant absorptivity of excitation radiation (18) at at least one of said analyte-characteristic-wavelengths.
The method of one of the preceding claims, wherein during said analyte measurement procedure (78), a sequence of analyte-wavelength-specific measurements is carried out while maintaining said thermal or pressure transmitting contact between the material (12) and the measurement body (16), wherein in each analyte-wavelength-specific measurement, excitation radiation (18) with an analyte-characteristic-wavelength selected from a predetermined set of analyte-characteristic-wavelengths is irradiated and a corresponding response signal is obtained,
The method of one of the preceding claims, wherein during said analyte measurement procedure (78), a sequence of analyte-wavelength-specific measurements is carried out while maintaining said thermal or pressure transmitting contact between the material (12) and the measurement body (16), wherein in each analyte-wavelength-specific measurement, excitation radiation (18) with an analyte-characteristic-wavelength selected from a predetermined set of analyte-characteristic-wavelengths is irradiated and a corresponding response signal is obtained,
The method of one of the preceding claims, wherein the time modulation of said intensity of said excitation radiation (18) is chosen such that an envelope of the intensity is asymmetrical in that a proportion of time during which the envelope assumes 50% or more of an average intensity is less than 50%, preferably less than 46% and most preferably less than 43% of a total time.
The method of one of the preceding claims, wherein the time modulation of said intensity of said excitation radiation (18) is chosen such that the envelope of the intensity follows a periodically repeating pattern, wherein said pattern includes a high intensity time portion including more than 80% of an intensity-time-integral and a low intensity time portion including less than 20% of the intensity-time-integral of the pattern, wherein a ratio of the durations of the high and low intensity time portions is less than 0.9, preferably less than 0.8, and most preferably less than 0.7.
The method of one of the preceding claims, wherein time modulation of said intensity of said excitation radiation (18) is chosen such that the envelope of the intensity is approximately harmonic such that in a Fourier decomposition of the intensity of the excitation radiation, of the total intensity associated with the dominant frequency and the 1st to 9th harmonics, at least 95% is associated with the dominant frequency and at least 97%, preferably at least 98% is associated with the dominant frequency and first harmonic.
The method of one of the preceding claims, wherein said detection device comprises a light source (28) for generating a detection light beam (22) travelling through at least a portion of said measurement body (16) or a component included in said measurement body,
The method of one of the preceding claims, wherein said excitation radiation (18) is generated using an array of lasers, in particular quantum cascade lasers, each having a dedicated wavelength.
The method of one of the preceding claims, wherein said excitation radiation (18) is generated using at least one tunable laser, in particular at least one tunable quantum cascade laser.
The method of one of the preceding claims, wherein some or all of said excitation wavelengths are in a range of 5 μm to 13 μm, preferably 8 μm to 11 μm.
An apparatus (10) for analyzing a material (12) comprising at least one analyte, said apparatus comprising
Dependencies are inferred from the claim text.