A METHOD FOR LASER INDUCED FLUORESCENCE DETECTION IN PREFERABLY LIQUID CHROMATOGRAPHY AND A DEVICE FOR THE PERFORMANCE OF THE METHOD

Abstract: In a method and a device for laser induced fluorescence detection in liquid chromatography a light beam (1) is directed from a laser source (2) towards a liquid flowing in a chosen flow direction for the detection of the presence of one or several substances. At a flow point illuminated by the light beam (1) the liquid is brought to emit a fluorescence radiation (3) which is received by a receiving unit (6). The light beam (1) is directed substantially perpendicularly to the flow direction of the liquid. The liquid is brought to pass the illuminated flow point in the form of a column with a accurately defined surface. The fluorescence radiation (3) is received in a direction which deviates from directions emanating from the illuminated flow point perpendicularly from the flow direction of the liquid column.

Description: A method for laser induced fluorescence detection in preferably liquid chromatography and a device for the performance of the method Technical field: The present invention relates to a method and a device for laser induced fluorescence detection in preferably liquid chromato¬ graphy. in which a light beam from a laser source is directed to¬ wards a liquid flowing in a chosen flowing direction for the de¬ tection of the presence of one or several substances in the liquid, which in one point of the flow illuminated by means of the light beam is brought to emit a flourescence radiation which is received by means of a receiving unit. Background: Extra column band broadening in detectors has paid attention since high performance liquid chromatography (HPLC) was intro¬ duced. According as columns and injectors have been improved the requirement on detector performance has increased to minimize peak ' broadening by dispersion . In this respect the cell volume as well as connections play an important role . The whole detector arrangement may influence on the flow properties which in turn affect the band spreading. There is a growing interest in the use of miniaturized HPLC systems based on packed microbore columns or open tubular columns . These chromatographic systmes may exhibit high resolving power together with -low flow rate of the mobile phase. The mic¬ robore packed column technique was introduced by Scott and Kucera [1,2] who printed out the importance to diminish the de¬ tector cell volume to utilize the separation effiency of the column . Ishϋ et al [3,4] constructed a miniaturized HPLC system with open tubular columns which have essentially smaller inner diameters or about 50 μm . With this technique the detector cell requires still smaller volumes or in the range of 0.1 - 1 μl. Knox and Gilbert [5] calculated that the effective detection volumes should be in the order of 1 - 10 nl before any hope of operating capillary HPLC CM?I systems under optimal conditions . They also stated that the prac¬ tical limitation to capillary HPLC arises from the dispersion by the detector. When considering different small volume detectors the fluore¬ scence technique is promising because of its high sensitivity. HPLC fluorescence detectors utilizing laser excitation radiation have re¬ cently been introduced [6, 7, 8] . Laser fluorimetry have some im¬ portant characteristics which may be advantageous with small volume detectors . The produced emission radiation is directly proportional to the intense laser excitation light which leads to extreme sensi¬ tivity. Another property is the spatial coherence of the laser beam which facilitates the irradiation of small detector volumes . In addi¬ tion the monochromaticity of the laser makes it easier to suppress scattered light from Rayleigh and Raman processes as well as re¬ flexions without sacrificing sensitivity. Diebold and Zare [6] presented a windowless flow ceE where the HPLC effluents flow from a steel capillary tube down to a rod 2 mm below forming a droplet bridge of 4 μl volume. Focusing the laser beam to a small spot inside the droplet facilitates rejecting the elastically scattered light. With a pulsed HeCd laser and the use of gated detection electronics they achieved very high sensitivity when determining aflatoxins. Hershberger et al. {7] designed a HPLC cell based on the sheath flow principle where the affluent is injected in the center of an ensheathing solvent stream under laminar flow conditions . The laser beam enlighted cell vulume is very small or in the range of 6 - 150 nl. Since the windows are not in contact with the sample flow the stray light fro the windows is reduced. Sepaniak and Yeung [8] used a quartz capillary tube where the HPLC effluent moved uppwards . A focused laser beam was placed in the effluent underneath an optical fiber. The emitted ligth was collected through the fiber perpendicular to the laser beam. The construction leads to a minimal influence of scattered and fluorescent light from the capillary tube walls . Technical problem: The limiting factors of fluorescence detectability is to a great part connected with background noise from the cell, optical co - ponents , solvent and sample contaminants . The reduction of the background emission is highly dependent on the detector cell de¬ sign. The objective of this invention is to design a laser based de¬ tector ideal to use with conventional HPLC columns as well as microbore columns . Special attention has been paid to the effective cell volume regarding extra column effects by comparing the effi¬ ciency of the two systems . The solution : Said object is achieved by means of the method according to the present invention, characterized by that the light beam is directed substantially perpendicular to the flow direction of the liquid, that the liquid is brought to pass said illuminated flow point in the form of a column with accurately defined surface and that the fluorescence radiation is received in a direction which deviates from directions emanating from the illuminated flow point perpen¬ dicularly from the flow direction of the liquid column . Said object is further achieved by means of the device accor¬ ding to the present invention, characterized by that the light beam • from the laser source is directed substantially perpendicularly to the flow direction of the liquid, that the liquid at said flow point forms the shape of a column with an accurately defined surface and that the receiving unit is arranged to receive the fluorescence radiation in a direction which deviates from directions , emanating from the illuminated flow point perpendicularly from the flow direc¬ tion of the liquid column. Brief .description J?f_d awings The present invention will in the following be further descri¬ bed with reference to the accompanying drawings , in which Fig. 1 shows a schematic diagram of detector cell arrangements , namely a) free falling jet, b) microbore column quartz capillary . A: Laser focusing point. B : Syringe needle SGE, 17 mm, ID 0.12 mm, OD 0.5 mm . C: Cyanoacrylate adhesive. D : SS tubing 1/16" , 15 mm , ID 0.2 mm . E : Fused silica capillary, 60 mm, ID 0.20 mm, OD 0.30 mm. F : SS tubing 1/16" , 17 mm, ID 0.35 mm: Fig. 2 shows ^ϊ^Λ y y CM?I a schematic diagram of the experimental instrumentation arrange¬ ment; Fig. 3 shows the relative fluorescence intensity versus focus location on the falling jet (OD . 0.3 mm) . Maximum response is found 15 mm ahead the jet. Column Nucleosil 7.5 μm, mobile phase hexane containing fluoranthene, flow rate 2 ml/min; Fig. 4 shows stability of the falling jet with hexane as mobile phase. Drop formation occurs in the shaded area. Flow rate is plotted against the distance between the column effluent exit and the laser excitation point; Fig. 5 shows separation of a standard mixture of 11 Dns-hydrazones . Column 200x4.6 mm, Nucleosil RP-18 5 μm. Mobile phase, methanol: water, linear gradient 50 to 100 % in 12 min. Flow rate 1.3 ml/min. 10 μl injected. l=Dns-hydrazine, 2=Formaldehyde, 3=Acetaldehyde, 4=Acetone, 5=Propanal, 6=Butanal, 7=Pentanal, 8=Benzaldehyde, θ^exanal, 10=Heptanal, ll=Octanal, 12=Nonanal; Fig. 6 shows the minimum detectable quantity of fluoranthene. Column 200x4.6 mm, Nucleosil 7.5 μm, mobile phase hexane. Flow rate 2 ml/min. Injected volume 10 μl. l=Anthracene, 2=Fluoranthene 20 fg Fig. 7 shows plot of log h versus log for conventional HPLC with different detectors . Column 150x4.6 mm, Nucleosil 7.5 μm, mobile phase hexane :methylene * chloride 5%. Solute anthracene; Fig. 8 shows plot of log h versus log tf for microbore column with different detectors . Column 400x1.0 mm, Nucleosil 7.5 μm, mobile phase hexane :methylene chlo¬ ride 5%. Solute anthracene; Fig. 9 shows schematic view of laser induces fluorescence detection direct on a HPLC quartz capillary column. Conventional HPLC svstem A LDC chromatographic system consisting of two Consta- metτic III pumps and a Gradient Master was used. Injections were made with a Valco injector with a 10 μl loop . Separations were per¬ formed on a 150 mm x 4,6 mm column packed with Nucleosil 7.5 μm Silica and on a 200 mm x 4,6 mm Nucleosil 5 μm RP18 column . The columns were mounted in a rack and pinion arrangement which allowed vertical adjustment. Hexane, methanol and methylenechloride solvents from Rathbum Chemicals (HPLC grade) and double distilled water were used in different mobile phase compositions . "gTfRE lT* For comparative studies a FS 970 LC Fluorimeter from Schoeffel Instruments were used, equipped with a Corning 7-54 primary filter and a 418 nm cut off secondary filter. The exitation wavelength was set to 360 nm. Microbore JHPLC_sy_stem The low flow-rates were maintained with a Waters M-6000 A pump. The frequency generator of the pump was disconnected and replaced by a Tektronix FG 502 Function Generator. Samples were injected with a Valco air actuated valve having a fixed sample volume of 0.5 μl. Columns were constructed from 10 and 20 cm lengths of 1/16" OD, l- mm ID SS tubing. Nucleosil 7,5 μm Silica particles were suspended in methanol and pumped into the columns at a pressure of 600 bar using a Haskel DST 150 air driven fluid pump . Acetone, methylenechloride and the appropriate eluent com¬ position were used to for conditioning purposes . Laser The effluent from the conventional HPLC columns was arranged • by means of a free falling thin jet. The jet stream was produced by a small bore capillary which is shown in Fig. 1. A short piece of a SGE syringe needle, OD 0,5 mm and ID 0.12 mm, is inserted in a 1/16" SS tubing ID 0,2 mm, drilled out to fit the syringe needle . The needle is fixed with cyanoacrylate adhesive. The capillary was then connected to the column end. The construction gives a very fine jet of the column effluent at flow- rates down to approximately 1 ml/min . uartz ^ c ιp_illary_tube An alternative detector design to the falling jet was required at flow-rates below 1 ml/min. Different quartz capillary tubes were tested for flow rates typical of miniaturized HPLC systems . It was found that fused silica capillary ID 0.2 mm and OD 0.3 mm from Hewlett Packard commonly used as GC/GC columns yielded lowest fluorescence background. The capillary was mounted to the column end inside a steel capillary tube as shown in Fig. 1. The po '±mide P --—> --. (J c:,_?ι coating on the fused silica capillary was carefully burnt off on a distance of 5 mm just below the end of the SS tubing using a gas flame. The uncovered area was then washed with methylenechloride . The laser beam is focused on the uncovered part of the capillary. The capillary tube allows any flow rate commonly used in conven¬ tional as well as microbore HPLC. * Optical ^rr∑mgements In Fig. 2 a schematic view of the optical system is outlined. As excitation source the monocromatic output from a Coherent Radiation CR 3000 Krypton ion CW laser ran in the TJV-mode was used. This laser emitts radiation at 351 and 356 nm with a total effect of 1 - 2 W. After εuppresssing the bluish fluorescence light, emanating from the laser cavity by means of a bandpass colour filter TJG1, the laser beam was focused with a quarts lens onto the detector cell underneath the column. Due to circumstances out of our control different lenses were used with focal length ranging from 15 to 60 cm. In order to avoid the strong scattered light in the horizontal plane emanating from the cylindrical surface of the vertically mounted detector cell, detection was achieved at an angle - of approximately 30° to this plane. After reflexion in a front sur¬ face mirror the fluorescence light is collected and focused onto the entrance slit of a Jobin Yvon HL monochromator using a quarts lens (f = 15,0 =10) . Depending on the nature of the experiment the en¬ trance slit was varied between 1 - 6 mm, while the exit slit was fixed at 17 mm yielding a bandpass of 28 nm. For convenience the monochromator was centered at 450 nm during all experiments . A compromise between maximum fluorescence yield and rejection of the Raman peak of water and hexane as well as elastically scattered light. The elastically scattered light was further suppressed with a cut-off filter WG 385 or GG 420 before reaching the photomultiplier- tube (EMI 9558 QB) . The output of the PMT is then, after ampli¬ fication, fed to a stripchart recorder. All experiments were per¬ formed under dark room conditions . O ?I Proced re _and_results The _free_ falling jet cell Investigations were carried out to find the maximum signal response by varying the focusing point of the laser beam vis-a-vis the falling jet. Different distances between the lens and the jet were tested at which the focus was located before, inside and be¬ hind the jet. The results are shown in Fig. 3. The experiment was facilitated by pumping a hexane solution containing a constant con¬ centration of fluoranthene as marker. The maximum response was expected to be symmetrical around the distance corresponding to the focal length of the lens. However, maximum response was found when the laser beam was focused 15 mm ahead the falling jet, corresponding to a laser beam diameter comparable to the diameter of the jet. No ohter maxima was found. One possible explanation of this discrepancy is that the distance from the lens to the true focus is not identical with the lens focal length. This effect may be due to the divergence of the laser and imperfections in the optical com¬ ponents. Scanning the laser beam horizontally, maximum response was achieved when the laser beam was in the center of the jet. At maximum response an intense disc of reflected light appeared in the - plane perpendicular to the jet stream. The optical properties of the jet is dependent on e.g. flow rates, solvent properties and diameter of the capillary. With the capillary diameter of 0.12 mm different flow rates were run to establish the minimum flow without turbulence. As shown in Fig. 4 the hexane as mobile phase could be used down to a flow of 1.2 ml/min. For gradient runs (methanol: water 0 to 100% in 10 min. ) an unaffected baseline was achieved at a flow rate of 1.5 ml/min. Droplet formation appeared at a flow rate of 1.0 ml/min when water content was approximately 55%. An example of a gradient run is shown in Fig. 5. A brief test of how the signal depended upon varying the effect of the laser resulted in that no saturation could be observed. Quartz_ cap llary _cell The laser beam was focused directly on the quartz capillary in the same way as with the falling jet. The background noise in- creased six times. However, the signal increased with the same factor thus the signal to noise ratio remained constant. The in¬ creased signal may be a result of a more favourable geometry for multiple reflexions inside the- cell. . The tιinimum_ detection i t Under the conditions used for the falling jet, the minimum de¬ tection limit was established. Fig. 6 shows a chromatogram of an in- jected sample containing 20 fg fluoranthene (20 x 10 -15 g in 10 μl hexane) . The capacity value was 3.2 and the signal to noise ration was 13. The linear flow through the quartz capillary detector was about 300 cm/s . Since the laser excitation volume is about 1 nl there are very few molecules present in the measured volume. Ap_plications There are a limited number of compounds which emit fluore¬ scence light. Furthermore they should be excitated at the laser wavelengths available. Partly these restrictions may be overcome by using the fluorescence labeling technique [9] . A chromatogram of 11 ■ Dns-hydrazone derivatives of carbonyl compounds is shown in Fig. 5. The laser free falling jet detector was used to illustrate a gradient elution application. Comp_arison_of detectors ^ coupled to_a_convenτional_ column A conventional fluorescence detector as well as the two diffe¬ rent laser detectors were coupled to a conventional column. The column system and the separation conditions were the same in the three experiments . Thus the cell arrangements could be compared according to band broadening on the detector side. The HETP curves for the three cases are shown in Fig. 7. The respective detector dead volumes were: Schoeffel detector approximately 5 μl: the falling jet 0.6 μl and the quartz capillary 1.0 μl. The illumi¬ nated volume with the two laser detectors were about 1 nl. Thus the differences in the HETP curve are mainly derived from the connections . O ?I The band broadening in the capillary connection tubes were calculated from the formula by Taylor [10] which is valid under conditions of laminar flow. The falling jet variance was δ 2 = 1.49 μl 2 and the quartz capillary yielded δ 2 = 2.84 μl 2 at the flow rate of 1.5 ml/min. These band broadening contributions are very small compared to the total dispersion i the connection tubings . Cojαp_anLson ^ _t _ ^ r ^Pl detectors ^ coupled to_ajMcrobore_col mn The quartz capillary detector cell was tested with a micro bore column . A comparison under same conditions was made with a con¬ ventional HPLC fluorescence detector with a realtively small detector cell dead volume. The HETP curve is shown in Fig. 8. In the ex¬ periment the pump flow rates were in the range 100 to 400 μl/min. Discussion In a recently published review Yeung and Sepaniak [11] dis¬ cussed the potential to use laser fluorimetric detection in HPLC . The previously reported laser based detectors are characterized by complicated constructions e.g. to suppress straylight. Further more the detectors are not designed to be used with miniaturized system • or gradient elution. The only detector that may be used with gradient operation, is the cell based on an optical fiber inside a quartz tube cell (20 μl cell volume) . However, this detector is difficult to diminish without concomitant decrease in sensitivity. The free falling jet principle is a straightforward approach and it has bee ' practised in turbidimeters to measure scattered light from particles . The jet is characterized by stability and a well de¬ fined smooth surface also during gradient elution with flow rates typically of conventional HPLC columns . The background is easy to suppress with the collecting optics out of the perpendicular plane to the jet stream. Actually a 30° angle results in a background signal decrease of 6 magnitudes. This arrangement yield the highest sensi¬ tivity or a detection capacity in the fg-level. When using laser excitation with its well defined beam it is far easier to manipulate the optics than to complicate the construction of the flow cell. The use of quartz capillaries as flow cells in fluorescence is very common. The most critically factor with quartz materials is the / OMPI background fluorescence. Compared to the falling jet cell the quartz capillary flow cell has one very important advantage, the cell allows very low flow rates adequate for microbore column separations. As mentioned in the introduction one main advantage of laser excitation is the possibility to irradiate small detector volumes. Therefore laser based detectors may be successful with miniaturized systems . Hershberger et.al. [7] reported the possiblify to use a detector volume down to 1 nl. This is true for the laser irradiated volume in their detector, however, by no means for the whole de¬ tector volume including the connections. Miniaturized HPLC systems are characterized by narrow peaks. The peaks should not be dispresed anywhere in the detector sys¬ tem. Conventional detectors with dead volumes of 5 μl are not feasible to use without an additional make up liquid to sweep the detector [12, 13] . The decrease of sensitivity by dilution effects may ' be partly compensated by laser excitation, however, this constitutes not a adequate solution. The central point to achieve detectors with minimal or nearly no dead volume is to take into account the connecting tubes. The results in this report show the advantage to transfer the solutes to - the detection area in a straight short small bore capillary. Then the maintained laminar flow produces a negligiable dispersion. The quartz capillary detection cell in this report is 33 mm long and has a volume of 1.04 μl. By using a smaller ID column e.g. 0.05 mm the volume is 65 nl. The final solution is to locate the laser beam direct on the separation quartz capillary column Fig. 9. In the above it has consequently been described a method and a device for the detection , of the presence of certain sub¬ stances in a liquid by measuring the fluorescence radiation of the substances. The substances have been brought to fluorescence by means of a laser beam which is brought to illuminate the liquid over a minimum of volume at a flow point, where the liquid is flowing in a certain direction from a device for chromatographic separation. This device is represented in Fig. 1 by means of a unit 5 designated HPLC and a column 9, in which different sub¬ stances are separated by means of their different physical and chemical properties and in this way the substances are brought to consecutively pass said flow point. This flow point can conse¬ quently be either a free falling liquid jet or a liquid channel in a capillary. Common is that the liquid passes the illuminated flow point in the form of a column with a accurately defined surface. The accurately defined surface is for example cylindrical with a highly even surface so that no disturbing refractive phenomenons are obtained. Essential .is further that the laser beam is directed perpendicularly to the longitudinal direction of the liquid column, that is to say the flow direction of the liquid. The device further includes a receiving unit 6 for the recep¬ tion of the fluorescence radiation 3 emitted from the illuminated flow point. Essential is ' that the fluorescence radiation 3 is received in a direction being outside the plane throught the flow point which is perpendicular to the flow direction of the liquid. In this way scattering light and other nondesirable radiation is avoided caused by the radiation from the laser beam source, which is especially dominating in said direction and in this way the fluore¬ scence radiation with a longer wavelength can be received with a minimum of disturbance level. The above method and device has been decribed in connection • with separation of a plurality of substances, but it is of course imaginable that the invention can be applied in such cases where . the presence of a single substance will be detected. Ackn wle dge nents We are greatful to Prof . Sune Svanberg and Dr. Morgan Gustavsson for kind support of this work, and to Dr. R. P. W. Scott for stimulating discussions. References: [1] R.P.W. Scott and P. Kucera, J. Chro atogr. 125 (1976) 251 [2] R.P.W. Scott and P. Kucera, J. Chromatogr. 169 (1979) 51 [3] D . Ishii, K. Asai, K. Hibi, T . Jonokuchi and M. Nagaya, J. Chromatogr. 144 (1977) 157 [4] D . Ishii and Takeuchi, J. Chrom. Sci. 18 (1980) 462 [5] J. H . Knox and M.T . Gilbert, J. Chromatogr. 186 (1979) 405 [6] G .J. Diebold and R.N . Zare, Science 196 (1979) 1444 C ?I [7] L.W. Hershberger, J.B . Callis and G.D. Christian, Anal. Chem. 51 (1979) 1444 [8] M.J. Sepaniak and E .S. Yeung, J. Chromatogr. 190 (1980) 377 [9] L. Johnson, B . Josefs son, P. Marstorp and G. Eklund Int. J. Enviro. Anal. Chem. , 9 (1981) 7 [10] G. Taylor, Proc . R. Soc. (London) 219A (1953) 186 [11] E.S . Yeung and M.J. Sepaniak, Anal. Chem. 52 (1980) 1465A [12] T. Tsuda and M. Novotny, Anal. Chem. 50 (1978) 271 [13] M. Krejci, T. Tesarik and J. Pajurek, J. Chromatogr. 191 (1980) 17

Claims: Patent Claims : 1. A method for laser induced fluorescence detection in preferably liquid chromatography, in which a light beam (1) from a laser source (2) is directed towards a liquid flowing in a chosen flowing direction for the detection of the presence of one or several sub¬ stances in the liquid, which in one point of the flow illuminated by means of the light beam is brought to emit a flourescence radia¬ tion (3) which is received by means of a receiving unit (6) , CHARAC¬ TERIZED BY that the light beam (1) is directed substantially per¬ pendicular to the flow direction of the liquid, that the liquid is brought to pass said illuminated flow point in the form of a column with accurately defined surface and that the fluorescence radiation is received in a direction which deviates from directions emanating from the illuminated flow point perpendicularly from the flow direc¬ tion of the liquid column. 2. A method according to claim 1 or 2, CHARACTERIZED BY that in detecting having relatively low flow rates said liquid column is formed by means of a capillary consisting of quartz with a low in¬ herent fluorescence, said capillary being highly transilluminable at said flow point. 3. A method according to claim 1, CHARACTERIZED BY that when detecting with flow rates from substantially 1 ml/min that said liquid column is formed by a freely falling liquid jet with an accu¬ rately defined surface. 4. A method according to any of the claims 1 , 2 or 3, CHARAC¬ TERIZED BY that said accurately defined surface has the form of a cylinder mantle with a highly even surface structure. 5. A device for the accomplishment of a method for laser induced fluorescence detection in liquid chromatography, including a device for chro atographic separation of substances in a liquid with a flow point for the liquid, where the liquid flows in a chosen flow direc¬ tion, a laser source (2), arranged to emit a light beam (1) which is directed towards said flow point * so, that the liquid at this point is brought to emit a fluorescence radiation, a receiving unit (6) ar¬ ranged to receive the fluorescence radiation and to record its in¬ tensity, CHARACTERIZED BY that the light beam (1) from the laser source (2) is directed substantially perpendicularly to the flow direction of the liquid, that the liquid at said flow point forms the shape of a column with an accurately defined surface and that the receiving unit (6) is arranged to receive the fluorescence radiation (3) in a direction "which deviates from directions, emana¬ ting from the illuminated flow point perpendicularly from the flow direction of the liquid column. 6. A device according to claim 5, CHARACTERIZED BY that said liquid column is formed by a capillary (10) made by quartz with a low inherent fluorescence, said capillary being highly transillu¬ minable at said illuminated flow point. ** 7. A device according to claim 5, CHARACTERIZED BY that said liquid column is formed by a from an outlet from the device (5) for chromatogr aphic separation freely falling liquid jet with an accurately defined surface. 8. A device according to any of the preceeding claims, CHARAC¬ TERIZED BY that said device includes means for the focusing of the light beam substantially in the area of the illuminated flow point. 9. A device according to claim 8. CHARACTERIZED BY that the light beam (1) is focused in a point, positioned somewhat in front of the liquid column. 10. A device according to claim 9,. CHARACTERIZED BY that the light beam (1) is focused substantially 15 mm in front of the liquid column and therebv a maximum of fluorescence radiation is obtained. r -r r ^-rs XZ Λ -* .

Inventors: FOLESTAD SVEN STAFFAN, GALLE BO GUSTAF, JOHNSON LARS GOERAN INGVAR, JOSEFSSON BJOERN OLOF
Applicants: FOLESTAD SVEN STAFFAN, GALLE BO GUSTAF, JOHNSON LARS GOERAN INGVAR, JOSEFSSON BJOERN OLOF
Application year: 1982
Main classification: G01N21
IPC codes: G01N21, G01N30