Method of detecting sample substances and fluorescence spectrometer using the method

Abstract: A method of detecting sample substances separated by an analytical separation technique, for example liquid chromatography or capillary electrophoresis, using electromagnetic radiation, and a corresponding fluorescence spectrometer are disclosed. The spectrometer comprises: a flashlamp (1) for emitting pulses of light, an adjustable diffraction element (8; 20) for adjusting selectable measuring wavelengths, a sample cuvette (13) through which sample substances to be detected flow, detection means (26) for receiving fluorescence light emitted from said sample substances flowing through said sample cuvette, and control means (3,27) for adjusting different measuring wavelengths by corresponding control of said adjustable diffraction element, and for synchronizing the emission of light pulses from said flashlamp with said adjusting of different measuring wavelengths.

Description: The invention relates to a method of detecting sample substances separated by an analytical separation technique, such as liquid chromatography or capillary electrophoresis. Known techniques for detecting sample substances eluting from the separation column of a liquid chromatograph are fluorescence spectrometry and absorption spectrometry. In fluorescence spectrometry, the sample to be analyzed is irradiated by excitation light which causes the sample substances to emit fluorescence light at characteristic wavelengths. The fluorescence light is measured by a suitable detector to derive information about the sample, in particular the composition of the sample and the quantities of the individual components present in the sample. Typically, the wavelength of the excitation light is selected by an optical component, such as a diffraction grating or a filter. The fluorescence light emitted is usually selected by a second diffraction grating or by a filter. For performing a fluorescence measurement, the grating at the excitation side of the spectrometer is set to a fixed excitation wavelength and the wavelength spectrum of the fluorescence light is recorded by means of the grating at the emission side (emission grating). The emission spectrum can be recorded for a plurality of excitation wavelengths. As an alternative thereto, the emission wavelength can be kept fixed and the excitation wavelength can be varied by corresponding adjustment of the excitation grating. In absorption spectrometry, a beam of radiation is transmitted through the sample. The wavelengths at which the sample absorbs the radiation are characteristic for the sample substances. The radiation transmitted through the sample is spectrometrically analysed by means of a diffraction element such as a diffraction grating or a filter. The diffracted light is detected by a photosensitive element, such as a photodiode, or by an array of photodiodes. When a photodiode is used, the diffraction element is moved so that rays of different wavelengths can reach the photodiode. When an array of photodiodes is used, the diffraction element can remain stationary. The above described spectrometric methods allow to identify the type of a sample substance from the measured spectrum by comparison with known spectra. When it is desired to determine the amount of a specific sample substance, for example in liquid chromatography, the sample concentration is measured at one specific wavelength as a function of time as the sample substances are eluting from the separation column. The corresponding graphic representation of concentration versus time is the chromatogram. Specific sample substances appear as peaks in the chromatogram. The amount of a sample substance corresponds to the area of its peak in the chromatogram. The accuracy of this measurement depends on the signal-to-noise ratio of the chromatogram. In the following, the measurements for determining the amounts of sample substances will be referred to as "quantification" measurements and the measurements for determining the type of a sample substance by spectroscopic analysis will be referred to as "qualification" measurements. Known techniques and corresponding detectors for detecting sample substances have several limitations regarding quantification and qualification measurements. In the known detectors with a single detection element such as a photodiode or a photomultiplier tube as they are frequently used in fluorescence spectrometers, it is only possible to record a chromatogram at a specific detection wavelength. If a spectrum is to be recorded, it is required that the concentrations of the sample substances are substantially constant over a larger time interval. In liquid chromatography, however, such conditions are rarely to be found. The spectrometer in document US-A-3 637 310, uses a method of acquiring data involving consecutive wavelength scans being performed by using a light source 4 and a rotating dispersing element 7 (Fig. 1; column 1, lines 56-67). From these wavelength scans, individual measuring values at a predetermined wavelength can be taken to compose a chromatogram. In view of the prior art, it is an object of the invention to provide a method of detecting sample substances using a single detection element wherein qualification measurements of the sample substances can be performed in addition to quantification measurements with negligible loss in quantification measuring accuracy. Another object is to provide a method of detecting substances eluting from the separation column of a liquid chromatograph which allows to measure a chromatogram of the substances as well as spectra of the eluting substances without impairment of the chromatographic signal-to-noise ratio. According to the invention, these objects are solved for a method as defined in claim 1. Using the method of the invention, it is possible to measure quantification information (e.g. chromatographic data) about the sample as well as qualification information (spectral data) even though only a single detection element is used. It is important that even though two kinds of measurements (I.e. quantification and qualification) are performed during passage of the sample through the detector, the accuracy of the quantification measurement is not impaired by the performance of the qualification measurement. It is a further advantage of the invention that it is possible to obtain spectral or multiwavelength sample information at maximum light throughput. The light is shared among quantification and qualification measurements with no light being lost for wavelength switching. According to a further development of the invention, which is particularly useful in liquid chromatography, the qualification measurements are started in response to a trigger signal which indicates that a sample substance has entered into the detector. This trigger signal can be derived from the measured quantification information. In a preferred embodiment of the invention, the various wavelengths adjusted for deriving quantification and qualification information are adjusted by means of a rotating grating and the radiation transmitted Into the sample is in the form of light pulses which are synchronized with the adjustment of the wavelengths. BRIEF DESCRIPTION OF THE DRAWINGS Subsequently, embodiments of the invention will be explained in detail with reference to the drawings. Figure 1 is a schematic diagram of a fluorescence spectrometer according to a first embodiment of the invention. Figure 2 Is a graphical representation of a detector signal for a typical liquid chromatographic sample analysis as a function of both time and wavelength, for illustrating a schematic example of the method of the invention. Figure 3 is a graphical representation of a detector signal as a function of time and wavelength for illustrating a practical example of the invention. Figure 4 is an illustration of the principle of the invention, wherein a typical detector signal curve is depicted as a function of time as well as a magnified portion of this signal curve, showing both quantification and qualification measuring points. DETAILED DESCRIPTION OF THE INVENTION Figure 1 schematically shows a first embodiment of a fluorescence spectrometer according to a first embodiment of the invention. The radiation for excitation of fluorescence light is provided by a flashlamp 1, for example a bulb-type Xenon flashlight. A trigger socket 2 connected to the flashlamp 1 comprises control. electronics for the flashlamp. The flashlamp is operated in a pulsed mode, with the emission of light pulses being triggered by control signals provided from a controller 3 connected to the trigger socket 2. The timing of these control signals will be explained below. Typical values of the flash frequency in the present embodiment may lie, for example, in the range between 10 and 500 Hz. Typical values of the flash duration are in the microsecond range, for example from about 0.3 to 2 microseconds. The light emitted by the flashlamp 1 impinges on a condenser 4 which converts the ingoing light cone from the flashlamp into a converging light cone 5. In the embodiment shown, the condenser 4 consists of three lenses 4a, 4b, and 4c. The three lenses are preferably made of quartz so that light in the ultraviolet range can also be used for the excitation of fluorescence. As an alternative to the three lenses 4a-4c, a single spherical or aspherical lens or a spherical or aspherical mirror could be used. The converging light beam 5 passes through an aperture 6 and impinges thereafter on a mirror 7. The purpose of the mirror 7 is to fold the beam path so that the optical system can be arranged in a space saving manner. If the size of the spectrometer is not of importance, the mirror could be omitted. The beam reflected by the mirror 7 impinges on a focusing diffraction grating 8. The grating 8 in this embodiment Is a concave holographic grating. It will also be referred to as the excitation grating. The grating 8 is rotatable around a rotation axis 9 which is perpendicular to the plane of the paper. For the rotation of the grating 8, it is mounted to a motor 10. A rotated position of the grating is Illustrated by the dotted line grating 8'. The grating can be rotated by 360 degrees. During operation of the spectrometer the grating Is constantly spinning around the axis 9. A typical order of magnitude for the rotation frequency is about 80 Hz. Connected to the rotation axis 9 is a position encoder 11 which provides a signal corresponding to the Instantaneous angular position of the grating 8. This signal is supplied to the controller 3 on a line 29. From this signal, the controller 3 derives control signals which are supplied to the trigger socket 2 for triggering the emission of light pulses from the flashlamp 1. The flash frequency of the flashlamp 1 is usually adjustable to the rotation frequency of the grating 8. The grating 8 directs a converging diffracted light beam 12 into a sample cuvette 13 through which the sample to be analyzed flows. The sample enters the cuvette through an inlet tube 14 which is connected, for example, to the separation column of a liquid chromatograph. The sample leaves the cuvette 13 through an outlet tube 15. Instead of a liquid chromatograph, a capillary electrophoresis device could be connected to the inlet tube 14. In both cases, the various substances separated from each other, either by the chromatographic or by the electrophoretic separation process, are successively passing through the cuvette 13. The excitation light 12 entering the cuvette 13 excites the sample to emit fluorescence light. The fluorescence light 16 is observed under an angle of 90 degrees with respect to the direction of the excitation light 12. The cone of fluorescence light 16 impinges on a second condenser 17 which comprises three lenses 17a, 17b, and 17c. As with the above described condenser 4, a single spherical or aspherical lens or a spherical or aspherical mirror could be used instead of the arrangement of three lenses. The beam 18 leaving the condenser 17 passes through an aperture 19 and then impinges on a second diffraction grating 20. The grating 20 will also be denoted as emission grating. The grating 20 is rotatable around a rotation axis 21 which is perpendicular to the plane of the paper. The grating 20 is mounted to a motor 22 by means of which it can be rotated. A rotated position of the grating 20 is illustrated by the dotted line grating 20'. A position encoder 23 connected to the axis 21 provides a signal corresponding to the instantaneous angular position of the grating 20. This signal is supplied to the controller 3 on a line 24. From this signal, the controller derives control signals which are supplied to the trigger socket 2. The excitation grating 8 and the emission grating 20 as well as the associated drive motors and position encoders have, in the present embodiment, substantially the same design. The diffracted radiation 24 leaving the emission grating 20 is focused onto an aperture 25 and then impinges onto a photomultiplier tube 26 which provides an electrical output signal corresponding to the intensity of the radiation 24 incident on the photomultiplier 26. The output signal from the photomultiplier 26 is provided to a data processing and storage unit 27 where the data are processed in a way to be described in more detail below. The result of a measurement according to the invention is threefold: 1. a chromatogram. i.e. a representation of the amount of sample substances as a function of time; 2. fluorescence spectra, i.e., representations of the intensity of fluorescence light as a function of wavelength; and 3. fluorescence spectra as In 2., but additionally as a function of time. The chromatogram as well as the fluorescence spectra can be displayed on a display unit 28, such as a cathode ray tube, and/or printed out by a printer. The data processing and storage unit 27 also allows to store the chromatograms and fluorescence spectra and, optionally, It may comprise an electronic library with a collection of fluorescence spectra of various substances such as to allow comparison with the measured fluorescence spectra for facilitating sample identification. As an alternative to the photomultiplier tube 26, an avalanche diode or a CCD (charge coupled device) type detector or a micro channel plate type detector could be used. In the following, some examples for the method of the Invention which can be performed with the apparatus shown in Figure 1 will be explained. It will be assumed in the following that either the excitation grating 8 or the emission grating 20 remains stationary during the measurement, so that either the excitation light 12 entering the cuvette 13 or the light 24 which is incident on the photomultiplier tube 26 has a fixed wavelength. Starting with the first example, it is assumed that the emission grating 20 is at a fixed angular position such that the light detected by the photomultiplier 16 has a fixed wavelength which can be selected by a user. The excitation grating 8 is spinning around its axis 9. The generation of light pulses by the flashlamp 1 is controlled by the controller 3 in response to the angular position of the grating 8 which Is detected by the position encoder 11. In that way, it is possible to generate different excitation wavelengths for successive light pulses. According to an important aspect of the invention, several measurements are made during passage of a sample substance through the flow cell 13 at a fixed wavelength for deriving a chromatogram and additional measurements are made at a plurality of different wavelengths to derive a spectrum of the sample substance in the flow cell. This is accomplished by triggering the flashlamp each time when the grating is at an angular position corresponding to the fixed wavelength and each time when the grating is at angular positions corresponding to the wavelengths constituting the spectrum, respectively. The measuring values obtained at the fixed wavelength at different times constitute a chromatogram and the measuring values obtained during passage of a sample substance through the sample cuvette constitute a spectrum of this sample substance. The chromatogram is typically recorded over a time interval of several minutes and comprises several peaks, whereby the point in time at which a specific peak appears in the chromatogram is characteristic for the substance corresponding to this peak. A spectrum of a specific sample substance Is recorded over a shorter time interval, typically in the order of seconds or smaller. A spectrum is recorded during the time of a chromatographic peak. The generation of a spectrum is preferably triggered by the appearance of a chromatographic peak, i.e., when a sample substance is actually in the flow cell. It would also be possible to record spectrum information during the entire recording of a chromatogram. In order to illustrate the above principle, a typical time sequence of measuring points is listed below. The 71 measuring points are successively recorded, with equal time intervals between successive measuring points. The measuring points from about number 30 to about number 50 are recorded when a chromatographic peak occurs, i.e., when a sample substance flows through the cuvette. In the following table, the numbers of the measuring points are listed and the corresponding wavelength which is adjusted at this measuring point. Furthermore, it is indicated in the last column of the table if the measuring point is used for generating a chromatogram or if it is used for generating a spectrum. In the first case, the measuring point is classified as a "quantification (time)" measuring point, in the second case, it is classified as a "qualification (spectrum)" measuring point. measuring point (number) wavelength type of measuring point 1-32 310 nm quantification (time) 33 300 nm qualification (spectrum) 34 310 nm quantification (time) 35 310 nm qualification (spectrum) 36 310 nm quantification (time) 37 320 nm qualification (spectrum) 38 310 nm quantification (time) 39 330 nm qualification (spectrum) 40 310 nm quantification (time) 41 340 nm qualification (spectrum) 42 310 nm quantification (time) 43 350 nm qualification (spectrum) 44 310 nm quantification (time) 45 360 nm qualification (spectrum) 46 310 nm quantification (time) 47 370 nm qualification (spectrum) 48 310 nm quantification (time) 49 380 nm qualification (spectrum) 50-71 310 nm quantification (time) The intensity values measured by the photomultiplier 26 at the quantification measuring points are used to form a chromatogram, i.e., the values at the points 1-32, 34, 36, 38, 40, 42, 44, 46, 48, and 50-71. The intensity values correspond to the concentration values for the sample in the sample cuvette. The chromatogram can be used to determine the amounts of sample substances by determining the areas of the peaks in the chromatogram, respectively. This is the reason why the measuring points are denoted as "quantification measuring points". The intensity values at the measuring points 33, 35, 37, 39, 4i, 43, 45, 47, and 49 are used to form a spectrum of the sample substance corresponding to the peak in the chromatogram. in the present example, a spectrum in the wavelength range from 300-380 nm Is obtained with the measuring points being 10 nm apart from each other. During the time when the chromatographic peak occurs (measuring points 30-50), quantification and qualification measuring points are recorded In an alternating manner so that after each quantification measuring point (at 310 nm) a qualification measuring point is recorded. As explained above, this is accomplished by appropriate timing of the emission of the light pulses in relation to the angular position of the grating. The result of the measurement are a chromatogram and a spectrum which can be stored and displayed by the units 27 and 28. If there are several peaks in the chromatogram (corresponding to several sample substances), there will be a different spectrum for each peak. In order to take into account the intensity variation in a chromatographic peak, a normalization procedure can be applied as follows: The values at the qualification measuring points are normalized by dividing these values by the values at the quantification measuring point immediately before the qualification measuring point, respectively. In the present example, the following normalized qualification values are obtained: at 300 nm : (value at point 33)/(value at point 32) at 310 nm : (value at point 35)/(value at point 34) at 320 nm : (value at point 37)/(value at point 36) at 330 nm : (value at point 39)/(value at point 38) at 340 nm : (value at point 41)/(value at point 40) at 350 nm : (value at point 43)/(value at point 42) at 360 nm : (value at point 45)/(value at point 44) at 370 nm : (value at point 47)/(value at point 46) at 380 nm : (value at point 49)/(value at point 48) Instead of dividing by the values at the quantification measuring point immediately before the qualification measuring point, one could also divide by the value at the quantification measuring immediately after the qualification measuring point, or one could use the mean value of both divisions. If the time for acquiring a spectrum is very short as compared to the duration of the chromatographic peak, a normalization is not necessary. With the method of the invention as described before, the measuring values in the areas of the chromatogram where no sample peaks occur, i.e., in the noise area, are the same as with prior art methods for recording a chromatogram. In the area of a sample, peak some values are lost as compared to prior art methods because quantification as well as qualification measuring points are recorded, but it has turned out that this has only a small effect on the peak area reproducibility. The quantification accuracy is nearly the same as with prior art chromatographic measurements using single wavelength detection, whereas the substantial advantage results that spectral Information for qualification of the sample is acquired. In a practical example of the Invention, the time interval between successive measurements is 12.5 milliseconds, corresponding to a frequency of the grating rotation of 80 Hz. In a typical high performance liquid chromatographic analysis, the smallest peak width (time interval at half height of the chromatographic peak) is about 1 second. Thus, if the measurement of qualification values starts at the half height of the chromatographic peak, at least 80 data points are measured. If half of them are used for chromatographic (quantification) measurement and half of them for spectrum measurements, at least 40 points are available for spectrum measurement. For example, it is possible to measure from 300 nm to 456 nm every 4 nm one point for recording a spectrum of the sample. The measurement of qualification values may also start earlier than at the half height of the chromatographic peak: If the spectrum measurement starts at one quarter of the peak height, about 60 values for spectrum measurement can be obtained for a peak width of 1 second. The peak width of most chromatographic peaks is substantially greater than 1 second so that a large number of measuring values, chromatographic and spectral measuring values, can be recorded, allowing accurate quantification as well as qualification of the sample. As already mentioned, the recording of measuring values of qualification (spectrum) measuring values is only started when actually a sample peak occurs in the chromatogram. The trigger point for starting the qualification measurement can be generated in one of several ways. According to a first alternative, the trigger point is calculated by the data processing and storage unit 27 using the chromatographic data. The trigger point can be generated when the chromatographic measuring values become larger than a predetermined threshold level, Indicating that the rising slope of a peak occurs. Alternatively, a derivative threshold which is intelligent and can recognize the start of a sample peak could be used. The trigger point is generated if the slope of the chromatographic measuring curve becomes larger than a predefined value. In a still further embodiment, the trigger time may simply be set by the user. If the retention times of the sample peaks are rather constant, the trigger point for starting the acquisition of spectral data can simply be generated by a timetable which contains the retention times for the substances to be analyzed and initiates the data acquisition at these times, respectively. The use of a triggerforstarting spectrum data acquisition has the advantage that only the measuring values of interest are recorded so that the amount of data which have to be handled by the data processing unit is minimized. In the following, some variations to the above described method will be explained. In the method described above, a measurement at a fixed wavelength (FIX) for quantification is followed by a measurement at a wavelength for qualification. An example of the time sequence of the measuring points would thus look as follows: (... , FIX, 300 nm, FIX, 310 nm, FIX, 320 nm, FIX, 330 nm, FIX, 340 nm, ...). According to an alternative, one can measure the spectrum data at each wavelength more than once. In that way, an improved data filtering and increased reproducibility is achieved. A possible time sequence is: (..., FIX, 300 nm, FIX, 300 nm, FIX, 310 nm, FIX, 310 nm, FIX, 320 nm, ...) Another, even better possibility is: (.., FIX, 300 nm, FIX, 310nm, FIX, 320 nm, FIX, 330 nm, .... FIX, 490 nm, FIX, 500 nm, FIX, 490 nm, FIX, 480 nm, FIX, ..., 320 nm, FIX, 310 nm, FIX, 300 nm). The final spectrum measuring value for a specific wavelength is obtained by forming the average of the several measuring values at this wavelength. It is understood that the wavelength range of interest for generating a spectrum (in the last example: 300 - 500 nm) is generally dependent on the sample peak being analyzed. The invention is not limited to fluorescence measurements, it can also be used in connection with absorption measurements. In absorption measurements, the beam of radiation is transmitted through the sample cuvette and the beam leaving the cuvette is spectrally separated by a diffraction element, typically a grating. The spectrally separated radiation then impinges on a detector. The invention is of particular advantage when the detector consists of a single photosensitive element, for example a single photodiode. In this case, the diffraction grating arranged before the detector in the optical path is spinning and the emission of light pulses from a flashtamp is triggered at specific angular positions of the grating, corresponding to specific wavelengths to be detected by the detector. As in the embodiments of the invention relating to fluorescence measurements, a fixed wavelength is selected at which quantitative measuring values are recorded to compose a chromatogram (quantification). Furthermore, measuring values are recorded at a series of different wavelengths to compose an absorption spectrum (qualification). Figure 2 is a further illustration of an example for the method of the Invention. Figure 2 schematically shows for a typical liquid chromatographic sample analysis the detector signal as a function of both time and wavelength. The horizontal axis is the time axis where the time interval since the injection of the sample into the separation column is indicated. The vertical axis is the wavelength axis at which the wavelength used for detection is indicated. In case of a fluorescence spectrometer, this wavelength can either be the emission or the excitation wavelength. In case of absorption measurements, the wavelength is the absorption wavelength. The Intensity of the detector signal in the graphical representation of Figure 2 is illustrated by different shadings of grey. The lighter areas such as area 65 depict regions of low intensity and the darker areas such as area 66 depict regions of high Intensity. Thus, Figure 2 corresponds to a three-dimensional plot of Intensity versus time and wavelength, also named "iso-plot". The points characterized with "X" in Figure 2 correspond to the measuring points at which measuring values are taken according to the method of the invention. The measuring points arranged in the horizontal line 67 are all taken at a fixed wavelength (420 nm in this example) at different times and thus constitute a chromatogram. The measuring points arranged in the inclined lines, such as line 68, 69, or 70 are taken at different wavelengths and thus constitute a spectrum, respectively. As shown in Figure 2, the measuring points on the inclined lines 68 and 70 lie in the area of chromatographic peaks, respectively, whereas the measuring points on the line 69 lie in an area where there is substantially no measuring signal from a sample substance. Thus, for the sake of reduction of the amount of data, the measuring points on the line 69 could be also be omitted. In this case, one would use a trigger signal in the way described above for initiating the recording of spectral data only when a chromatographic peak occurs. Figure 3 is a graphical representation similar to that in Figure 2 showing an example of a peak triggered spectrum. The trigger event occurs at time T. From that time on spectral data are measured (Inclined line) in addition to the "chromatographic" data (horizontal line). Figure 4 is a further illustration of the principle of the invention. The lower half of Figure 4 is a graphical representation of detector signal versus time, whereas the upper half is a magnification of a portion of the measuring curve in the peak region. The magnified portion shows the Individual measuring points in the peak region, with A denoting measuring points at a fixed wavelength of 300 nm and B denoting measuring points at various different wavelengths. The measuring values obtained at measuring points A are used for quantification, i.e. for producing a chromatogram, the measuring values obtained at measuring points B are used for qualification, i.e. for producing a spectrum. The time spacing of the measuring points corresponds to a sample rate of 80 Hz. The amount of measuring points shown in Figure 4 corresponds to an actual practical example, whereas Figure 2 is only schematic in this respect, since the number of measuring points ("X") shown in Figure 2 is smaller than the number of measurements one would usually take in practice. The invention can also be applied in connection with a stagnant sample in the cuvette. In that case the sample is filled Into the cuvette with, for example, a syringe. It is possible to record excitation versus emission spectra of the unknown sample in the cuvette in a very short time. In that way one can generate a graphical representation of the intensity as a function of excitation as well as of emission wavelength. From such a 3D plot one can derive information about the different sample components. It is understood that the invention is not limited to the above described examples and that various modifications thereto are possible. For example, the light source may be a pulsed laser or another source which is capable of emitting pulses of radiation. A DC light source could also be used, but then the light emitted during switching from one wavelength to another will normally be lost. If, however, methods for instantaneous switching of wavelengths are used) e.g. when using acoustically tunable filters, a DC light source may be used without further disadvantages. Instead of a diffraction grating, an electrically or acoustically tunable filter or prism could be used as a diffraction element. The photosensitive elements for detecting the radiation from the sample cuvette may be, for example, avalanche photodiodes, charge coupled devices, diode arrays or intensified photodiode arrays (microchannel plates). The invention can be used in connection with liquid chromatography or capillary electrophoresis or other analytical separation methods wherein the sample substances are detected in time succession.

Claims: A method of detecting sample substances separated by an analytical separation technique, for example liquid chromatography or capillary electrophoresis, using electromagnetic radiation, wherein a plurality of quantification measurements for determining the amounts of sample substances are made with a detection means at a predetermined wavelength of the electromagnetic radiation at different points in time during passage of the sample substances through a flow cell, wherein the detection means is a single channel detection element, and wherein quantification information indicative of the quantitative amounts of the sample substances, respectively, is derived from said plurality of quantification measurements made at said predetermined wavelength, characterized in that the same single channel detection element with which said quantification measurements are made is used to make additional measurements for determining the type of a sample substance, the additional measurements comprising measurement at wavelengths different from said predetermined wavelength, wherein said additional measurements are made at points in time different from those at which said quantification measurements are made, wherein said quantification measurements and said additional measurements are made in an alternating manner, and wherein spectral information about the sample substances to be detected is derived from said additional measurements. Method as in claim 1, wherein said additional measurements are made in response to a trigger signal which indicates that a sample substance has entered into said detector. Method as in claim 2, wherein said trigger signal is generated from said quantification information. Method as in claim 2, wherein said trigger signal is generated by a timetable which contains the retention times for the substances to be analyzed and initiates the data acquisition at these times, respectively. Method as in claim 1, wherein said electromagnetic radiation for said measurements is provided in the form of light pulses. Method as in claim 5, wherein said wavelengths at which said measurements are made are adjusted by means of an adjustable diffraction element. Method as in claim 6, wherein said adjustable diffraction element is a continuously spinning grating and wherein one of said light pulses is emitted each time the grating has reached an angular position corresponding to a wavelength at which quantification information or spectral information is derived. Method as in claim 1 wherein said analytical separation technique is liquid chromatography and wherein said measurements comprise fluorescence measurements. A method of operating a fluorescencs spectrometer employing a method as in any of the preceding claims, wherein the fluorescence spectrometer comprises: a flashlamp (1) for emitting pulses of light, an adjustable diffraction element (8; 20; 38) for adjusting selectable measuring wavelengths, a sample cuvette (13; 43) through which sample substances to be detected flow, detection means (25;56) for receiving fluorescence light emitted from said sample substances flowing through said sample cuvette, and control means (3,27; 33,57), and wherein the control means adjust different measuring wavelengths by corresponding control of said adjustable diffraction element, and synchronize the emission of light pulses from said flashlamp with said adjusting of different measuring wavelengths. Method as in claim 9, wherein: the adjustable diffraction element is a continuously spinning grating (8;20;38), a position encoder (11,23,41) is coupled to the grating for providing an output signal corresponding to its angular position, said output signal is provided to said control means for triggering the emission of light pulses from said flashlamp at defined angular positions of said grating. Method as in claim 10, wherein the detection means comprise a photomultipller tube (26).

Inventors: DOERR THOMAS, LINOWSKI CLEMENS, DOERR, THOMAS, LINOWSKI, CLEMENS, Dörr, Thomas
Applicants: AGILENT TECHNOLOGIES INC, AGILENT TECHNOLOGIES, INC. (A DELAWARE CORPORATION)
Application year: 1996
Main classification: G01N30
IPC codes: G01N27, G01N30, G01J3