Patent Document

BACKGROUND OF THE INVENTION 
   This invention relates to a method and an apparatus for detecting chemical agents, and particularly to a method and an apparatus for detecting chemical agents by a mass spectrometer and APCI (atmospheric pressure chemical ionization), best suited for detecting isopropyl methylphosphonofluoridate (hereafter referred to as sarin) and pinacolyl methylphosphonofluoridate (hereafter referred to as soman). 
   In recent years, there has been demand for apparatuses for detecting chemical agents to cope with chemical terrorism incidents. For detection of chemical agents, the general method is analysis of chemical agents, and the prevailing analytical method is gas chromatography/mass spectrometry (GC/MS). Normally, there have been few cases where hazardous chemical agents were detected from samples, so that the presence of toxic chemical agents is proved by detection of decomposed substances which are likely to remain as residues. 
   As a conventional technology with another analytical apparatus for chemical agents, liquid chromatography/mass spectrometry (LC/MS) is well known, which is used to separate and analyze volatile or nonvolatile chemical compounds. 
     FIG. 9  is a diagram for explaining a schematic structure of an analytical apparatus using a liquid chromatography/mass spectrometry according to prior art. The analytical apparatus according to the prior art will be described in the following. In  FIG. 9 ,  101  denotes a liquid chromatograph (LC),  102  denotes a connection tube,  103  denotes an ion source,  104  denotes a power supply for the ion source,  105  and  109  denote signal lines,  106  denotes a mass spectrometer,  107  denotes a vacuum system,  108  denotes an ion detector, and  110  denotes a data processor. 
   As shown in  FIG. 9 , the analytical apparatus using liquid chromatography/mass spectrometry according to the prior art comprises a liquid chromatograph (LC)  101  for separating samples into separate components, an ion source  103 , controlled by the power supply  104  for the ion source, for generating ions derived from sample molecules, a mass spectrometer unit  106 , evacuated by a vacuum system  107 , for analyzing masses of generated ions, an ion detector  108  for detecting separated ions, and a data processor  110  for processing data. The mass spectrometer includes the ion source  103 , the mass spectrometer unit  106 , and the ion detector  108 . 
   In the above description, sample liquid separated into respective components by liquid chromatograph (LC)  101  is introduced through the connection tube  102  into the ion source  103  that operates under atmospheric pressure. The ion source  103 , controlled by the power supply for the ion source  104  through signal lines  105 , generates ions derived from sample molecules in the sample liquid. Subsequently, the generated ions are introduced into the mass spectrometer unit  106  for mass spectrometry. The mass spectrometer unit  106  is evacuated by the vacuum pumping system  107 . The ions subjected to mass spectrometry are detected by the ion detector  108 . Detected signals are transmitted through the signal line  109  to the data processor  110  to generate analysis data, such as mass spectra and chromatograms. 
   As has been described, the mass spectrometer in the analytical apparatus needs to handle ions in vacuum and therefore requires an interface means to intervene between the spectrometer and the liquid chromatograph (LC). In other words, the LC is a device which handles large amounts of water and organic solvent under atmospheric pressure, whereas the mass spectrometer (MS) is a device for handling ions under high vacuum. For this reason, it has been considered difficult to directly connect them together. 
   The ion mobility spectrometer (IMS) method is used chiefly in combination with ionization of a sample by a radiation source to measure the mobility of its ions in an electric field, and this is the most prevalent in-situ detection method, and there are many applied products available in Europe and the U.S. Being applicable in a smaller configuration than GC/MS or LC/MS, the IMS method has found broad usages, including those to military specifications. However, because the IMS does not identify samples in terms of m/z (mass-to-charge ratio), detectors of IMS method have a rough indication of detection results and are limited to portable use with a warning attached to the effect that soldiers must wear protective masks when an alarm sounds. 
   As a conventional technology related to the IMS method, one which is described in U.S. Pat. No. 6,225,6223B1 is well known. 
   A U.S. Patent Application titled “Substance Detection Method and Substance Detection Apparatus” was filed on May 1, 2003, under Ser. No. 10/426718, in which substances, such as explosives, are vaporized and made into negative ions which are subjected to analysis. 
   The above-mentioned conventional GC/MS and LC/MS methods have a problem as follows. The technology of electron ionization (EI) applies strong energy to the substance itself to be detected and therefore the substance is liable to decompose, thus producing a multitude of fragment ions, for which reason detection devices by GC/MS have difficulty in generating ions of molecular weight of the substance or of a larger molecular weight, a fact which makes it difficult to identify the sample. The GC or LC process for separation of substances to be detected prolongs a detection time. 
   The problem with the above-mentioned IMS method is that it has difficulty in determining the kinds of chemical agents, and that because this method permits ready response to a wide range of chemical compounds, it is difficult to decide or identify samples to be detected, resulting in a high rate of false alarms. 
   SUMMARY OF THE INVENTION 
   The object of the present invention is to solve the problem with the conventional technology mentioned above, and provide a method and an apparatus for detecting chemical agents, capable of increasing a detection speed of chemical agents, decreasing a false alarm rate, pinning down the kinds of chemical agents, and meeting specifications for unattended continuous monitoring equipment suitable for detection of sarin or soman. 
   According to the present invention, the above object can be achieved by providing an ion source for introducing and positively ionizing a test sample by corona discharge, providing a mass spectrometer unit for analyzing the mass of ions from the ion source, which is carried out by sensing signals from chemical agents to be detected. 
   Further, the above object can be achieved by providing an ion source for introducing and positively ionizing a test sample by corona discharge, a mass spectrometer unit for analyzing the mass of ions generated by the ion source, and means for monitoring the ionic strength of ions from chemical agents to be detected. 
   Further, the above object can be achieved by providing an ion source for introducing and positively ionizing a test sample by corona discharge, a mass spectrometer unit for analyzing the mass of ions generated by the ion source, and means for monitoring the ion strength of ions each having m/z (mass-to-charge ratio) of chemical agents to be detected. 
   Further, the above object can be achieved by providing a sample introduction unit for introducing a test sample and heating the test sample, an ion source for ionizing a gas produced by heating by corona discharge, and a mass spectrometer unit for analyzing the mass of ions generated by the ion source, and detecting signals from chemical agents to be detected. 
   Further, the above object can be achieved by providing a sample introduction unit for introducing and heating a test sample, an ion source for ionizing a gas generated by heating by corona discharge, a mass spectrometer unit for analyzing the mass of ions generated by the ion source, and means for monitoring the ion strength of ions from chemical agents to be detected. 
   Further, the above object can be achieved by providing a sample introduction unit for introducing and heating a test sample, an ion source for ionizing a gas generated by heating by corona discharge, a mass spectrometer unit for analyzing the mass of ions generated by the ion source, means for monitoring the ion strength of ions each having m/z (mass-to-charge ratio) from a chemical agent to be detected. 
   In the foregoing description, the ion source is configured by using a counter-flow type atmospheric pressure chemical ionization (APCI) such that a test sample from the sample introduction unit is introduced to an area between the corona discharge generator unit and the mass spectrometer unit, and flows towards the corona discharge generator unit opposite the mass spectrometer unit. 
   The present invention including the above-mentioned means is capable of narrowing down the identity of chemical agents and reducing a false alarm rate, and therefore is best suited for detection of toxic chemical agents, such as sarin or soman. Peculiar to the present invention is the scheme of chemical detection using the counter-flow atmospheric pressure ionization (APCI) that a test sample introduced from the sample is supplied to a region between the corona discharge generator unit and the mass spectrometer unit, and flows towards the corona discharge unit opposite the mass spectrometer unit. 
   Other objects, features and advantages of the invention will become apparent from the following description of the embodiments of the invention taken in conjunction with the accompanying drawings. 

   
     BRIEF DESCRIPTION OF THE DRAWINGS 
       FIG. 1  is a block diagram showing a schematic structure of an apparatus for detecting chemical agents according to an embodiment of the present invention; 
       FIG. 2  is a perspective view showing an external appearance of a detection apparatus according to an embodiment of the present invention; 
       FIG. 3  is a sectional view showing a structural example of a filter paper heating unit (oven) shown in  FIG. 2 ; 
       FIG. 4  is a block diagram showing a structural example of an ionizing unit and a mass spectrometer unit of the detection apparatus according to an embodiment of the present invention; 
       FIG. 5  is a diagram for explaining mass spectra of sarin, obtained according to an embodiment of the present invention; 
       FIG. 6  is a diagram for explaining mass spectra of soman, obtained according to an embodiment of the present invention; 
       FIG. 7  is a diagram for explaining the ion source temperature dependence of signals with m/z=99 detected when samples of sarin or soman are introduced; 
       FIG. 8  is a diagram for explaining the drift voltage dependence of signals with m/z=99 detected when samples of sarin or soman are introduced; and 
       FIG. 9  is a diagram for explaining a schematic structure of an analytical apparatus using liquid chromatography/mass spectrometry according prior art. 
   

   DESCRIPTION OF THE INVENTION 
   Embodiments of a method and an apparatus for detecting chemical agents according to the present invention will be described in detail with reference to the accompanying drawings. 
     FIG. 1  is a block diagram showing a schematic structure of an apparatus for detecting chemical agents according to an embodiment of the present invention. 
   As shown in  FIG. 1 , an apparatus for detecting chemical agents according to an embodiment of the present invention comprises a sample introduction unit  1 , an ionizing unit  2  as an ion source, a mass spectrometer unit  3 , a control unit  4 , a suction pump  5 , a computer  6  for the measurement process, and a vacuum pump  7 . In this chemical detection apparatus configured as described, a sample  16  having particles of a dangerous substance adhering to it is inserted into the sample introduction unit  1 , and becomes a gas when it is heated by a heating device, not shown, mounted to the sample introduction unit  1 . The sample in gaseous state is introduced through the flow path  81  indicated by a solid line while the sample in gaseous form carried by the atmospheric air is drawn into the ionizing unit  2  by the suction pump  5 . The suction pump  5  performs a function to discharge the drawn-in atmospheric air and a function to vary the pumping quantity in a range of 0˜2 liters/min. by a mass flow controller. 
   The test sample introduced into the ionizing unit  2  as the ion source is sent to a corona discharge region at the tip of a needle electrode for corona discharge to be described later, and a target component to be detected is positively ionized by a high positive voltage (about 2 kV˜5 kV) applied to the needle electrode. Only the positive ions are introduced guided by an electric field that is generated in the range from the ionizing unit  2  to the mass spectrometer unit  3 , pass through a first orifice provided at the ionizing unit  2 , and are sent to the mass spectrometer unit  3 . At this time, surplus substances other than ions and molecules that pass through the first orifice in the ionizing unit  2  are discharged from the ionizing unit  2  by the suction pump  5 , and then exhausted to the outside of the apparatus by the suction pump  5 . By keeping a sample introduction path between the sample introduction unit  1  and the ionizing unit  2 , and the ionizing unit  2  at a high temperature, the sample can be prevented from being adsorbed to the internal wall of the introducing path or to the interior of the ionizing unit  2 . 
   When detecting targets are chemical agents, such as sarin or soman, molecular ions are likely to become positive ions. For this reason, in this embodiment, positive ions are used as an analysis target. 
   The ions introduced into the mass spectrometer unit  3  pass through a differential exhaust portion in the mass spectrometer unit  3  depressurized by the vacuum pump  7 , and are converged by an electrostatic lens system and its mass is analyzed by the mass spectrometer. The vacuum pump  7  has a function to keep the interior of the mass spectrometer chamber in a high vacuum state. The ions separated by the mass spectrometer are converted into electrons by a secondary electron multiplier in the mass spectrometer unit  3 , and a resulting current signal is amplified by an amplifier and sent to the computer  6  for measurement process. 
   The computer  6  for measurement process processes a signal received from the mass spectrometer unit  3 , and displays a relation between mass-to-charge ratio (m/z) and ion strength (a mass spectrum), a variation with time of the ion strength of a given m/z, and so on. A final display image may be a simplified diagram rather than a mass spectrum or mass chromatogram mentioned above. In other words, when a detection apparatus for chemical agents according to an embodiment of the present invention is used as an apparatus for detecting dangerous substances, it is only necessary for the apparatus to display whether or not a chemical substance was found which is problematical, namely, dangerous. 
   The control unit  4  performs on/off control of the functions of a detection apparatus, sets temperature, voltage, and vacuum pressure, and monitors status, and so on. The connections for these purposes are shown in  FIG. 1  by thin control lines and data lines  82 . 
   As mentioned above, according to an embodiment of the present invention, by the mass spectrometer  3 , it is possible to analyze particles of a dangerous substance adhering to a sample  16 , which is inserted into the sample introduction unit  1 . 
     FIG. 2  is a perspective view of the external appearance of a detection apparatus according to an embodiment of the present invention. As shown in  FIG. 2 , the detection apparatus comprises a filter paper heating unit  21  with a filter paper entrance  20 , a analyzer  22 , and a display  23 , and can be moved with casters under the bottom of the apparatus. 
   Normally, in a process that chemical agents are produced or transported, trace amounts of chemical agents adhere to hands or clothing of people who handle the chemical agents. When they handle their belongings, such as bags, chemical agents adhere to those belongings. 
   In the embodiments of the present invention, description is made in such a way that a soft material, such as cloth or filter paper (test paper is mentioned in the following description, but the material need not always be paper) is used to wipe the surface of a bag, for example, as a test sample (a detection object), and the chemical substance adhering to the test paper is analyzed. More specifically, test paper to which the chemical agents adheres is inserted through the filter paper entrance  20  to the filter paper heating unit  21 . Since the test paper is heated in the filter paper heating unit  21 , the chemical substance that adheres to the test paper evaporates, and the substance in gaseous state is analyzed by the analyzer  22 . In the analyzer  22 , the detection apparatus configured as described in  FIG. 1  is accommodated, and database  6   a  in which information about signals from chemical agents is stored. When it is recognized from analysis results and information in the database  6   a  that signals peculiar to a chemical agent has been detected, the computer  6  for the measurement process displays an alarm on the display screen  23 . 
     FIG. 3  is a sectional view showing a structural example of the filter paper heating unit (oven)  21  shown in FIG.  2 . In  FIG. 3 ,  24  denotes filter paper,  25  denotes a tray,  25 ′ denotes a handle,  26  denotes a tray holder,  27  denotes a sensor,  28  denotes a halogen lamp,  29  denotes an air intake pipe,  30  denotes a filter,  31  denotes a sample introduction pipe, and  32  denotes a cover. 
   The filter paper heating unit (oven)  21  includes a tray holder  26 , a halogen lamp  28  as a heat source mounted in the tray holder  26 , and a tray  25  for loading filter paper  24 . In the filter paper heating unit  21  structured as described, the tray  25  is pulled out by drawing the handle  25 ′, and then filter paper  24 , which is test paper by which the test object was wiped, is placed on the slide-type tray  25 . The tray  25  on which filter paper  24  has been placed is inserted into the tray holder  26 . When a sensor  27  detects the tray which has been pushed to a predetermined position, the halogen lamp  28  at the top of the tray holder  26  is turned on. The filter paper  24  is heated by heat waves from the halogen lamp  28 , and the substance adhering to the filter paper  24  evaporates. The heating temperature should preferably be 100° C. or higher. The sample in gaseous state derived from the filter paper  24  is sent together with the air, which has entered from the air intake pipe  29 , into the analyzer  22  through the sample introduction pipe  31 . 
   The air intake pipe  29  may be provided with a filter  30  to remove dust or the like. Moreover, since the filter paper heating unit  21  is raised to a high temperature, a handle  25 ′ and a heat-insulated cover  32  may be provided for safety. The sample introduction unit  1  may be of a type that directly introduces a test sample (detection object), drawn in from the outside, into the ionizing unit  2 . 
     FIG. 4  is a block diagram showing a structural example of the ionizing unit and the mass spectrometer unit of the detection apparatus according to an embodiment of the present invention. In  FIG. 4 ,  33  denotes a needle electrode,  34  denotes an opposite electrode,  35  denotes an opening,  36  denotes a suction pump,  37   a  and  37   b  denote electrodes each with an orifice,  38   a  denotes a first ion introduction orifice,  38   b  denotes a second ion introduction orifice,  39  denotes a differential exhaust portion,  40   a  and  40   b  denote exhaust systems,  41  denotes a vacuum section,  42   a  and  42   b  denote endcap electrodes,  43  denotes ion focusing lens,  44  denotes a ring electrode,  45  denotes a quartz ring,  46  denotes a gas supply unit,  47  denotes a gas introduction pipe,  48  denotes a gate electrode,  49  denotes a converter electrode,  50  denotes a scintillator,  51  denotes a photomultiplier, and  52  denotes a data processor. 
   In  FIG. 4 , in the ionizing unit  2 , a high voltage is applied between the needle electrode  33  and the opposite electrode  34  and as a result corona discharge occurs in the vicinity of the tip of the needle electrode  33 , so that nitrogen, oxygen and water vapor or the like in the atmospheric air are ionized, and they are called primary ions. The primary ions move towards the opposite electrode  34  guided by an electric field. The test sample drawn in from the sample introduction unit  1  through the sample introduction pipe  31  is supplied to an area between the opposite electrode  34  and the electrode  37   a  with an orifice, is made to flow towards the needle electrode  33  through the opening  35  in the opposite electrode  34  of the ionizing unit  2  by the suction pump  36 , and reacts with the primary ions and thereby ionized. 
   Due to a potential difference of about 1 kV between the opposite electrode  34  and the electrode  37   a  with an orifice, the ions move towards the electrode  37   a  with the orifice, and guided through the orifice  38   a  into the differential exhaust portion  39 . Because of adiabatic expansion that occurs in the differential exhaust portion  39 , solvent molecules or the like adhere to the ions under test, and the ions increase in mass, which is called clustering. The ions produced by clustering appear as an unnecessary spectrum. To reduce clustering, it is desirable to heat the electrodes  37   a  and  37   b  each with an orifice with a heater, for example. 
   When an ionizing unit  2  of a structure shown in  FIG. 4  is used, the ions generated by corona discharge move in the direction of the opposite electrode  34  owing to a potential difference between the needle electrode  33  and the opposite electrode  34 , pass through the opening  35  and move towards the electrode  37   a  with the orifice. Because a test sample from the sample introduction unit is supplied between the opposite electrode  34  and the electrode  37   a  with the orifice, a reaction takes place between the primary ions and the test sample. Neutral molecules or the like produced by corona discharge flow from the opposite electrode  34  to the needle electrode  33  drawn by the suction pump  36 , and thereby removed from the corona discharge region, and are less likely to flow to the area where an ionizing reaction takes place between the primary ions and the sample. In the manner described above, the area where the primary ions are generated by corona discharge is separated from the area where the sample is ionized by reaction with the primary ions, and radical neutral molecules produced by corona discharge are prevented from flowing into the ionizing area, thereby decreasing the decomposition of the sample in the ionizing area. 
   As has been described, according to an embodiment of the present invention, primary ions are generated by using corona discharge in the atmospheric air, and the test sample is ionized by using corona discharge by utilizing a chemical reaction between the primary ions and the test sample, by which the proportion of the test sample decomposed into fragments is reduced, and the proportion of molecular ions of the sample being detected is increased. This method is called atmospheric pressure chemical ionization method (APCI). In the positive ionization mode that generates positive ions by applying a high positive voltage to the needle electrode  33 , the primary ions are mostly hydronium ion [(H 3 O) + ]. The formula of a typical positive ionizing reaction where M is a molecule as a detection object and H +  is a proton can be expressed as follows.
 
M+(H 3 O) + →(M+H) + +H 2 O
 
   The case where a sample is ionized has been described referring to an example that positive ions are generated, but some samples tend to generate negative ions. When negative ions are detected, a voltage of different polarity is applied. 
   The ions generated as described are introduced through the first introduction orifice  38   a  of the electrode  37   a,  then through the differential exhaust portion  39  evacuated by the exhaust system  40   a,  and through the second ion introduction orifice  38   b  of the electrode  37   b,  into the vacuum section  41  evacuated by the exhaust system  40   b.  A drift voltage is applied between the electrodes  37   a  and  37   b.  By this drift voltage, the ions introduced into the differential exhaust portion  39  are made to drift towards the second ion introduction orifice  38   b,  in which there two effects: (1) the ion permeability of the ion introduction orifice  38   b  is improved, and (2) the solvent molecules, such as water, adhering to the ions by clustering are detached from the ions by collision between the ions and the gas molecules remaining in the differential exhaust section  39 . A voltage is further applied to the electrode  37   b  with an orifice. This voltage have an effect on energy (incident energy) when the ions pass through the opening of the endcap electrode  42   a.    
   The ion trap efficiency of an ion trap mass spectrometer used in an embodiment of the present invention depends on the incident energy of the ions, and therefore the voltage applied to the electrode  37   b  is set so that the ion trap efficiency is high. The ions introduced into the vacuum section  41  are focused by the ion focusing lens  43 , and then sent to the ion trap mass spectrometer including the endcap electrodes  42   a,    42   b  and the ring electrode  44 . The endcap electrodes  42   a,    42   b  and the ring electrode  44  are held by the quartz ring  45 . 
   A colliding gas, such as helium, is introduced from the gas supply unit  46  through the gas introduction pipe  47  into the mass spectrometer. The gate electrode  48  is provided to control timing of ion injection into the ion trap mass spectrometer. After mass spectrometry is over, the ions separated and led out of the mass spectrometer are detected by a detector formed by the converter electrode  49 , the scintillator  50 , and the photomultiplier  51 . When an ion collides with the converter electrode  49  to which an ion-accelerating voltage is applied, charged particles are emitted from the surface of the converter electrode  49 . This charged particle is detected by the scintillator  50 , and the signal is multiplied by the photomultiplier  51  and detected. The detected signal is sent to the data processor  52 . As the mass spectrometer, description has been made referring to the ion trap mass spectrometer as an example, but a quadrupole mass spectrometer may be used. 
   The data processor  52  identifies a positive ion having m/z from a chemical agent to be detected, such as sarin or soman, and obtains its signal strength, and thereby verifies whether sarin or soman as a target chemical agent has been detected. If sarin or soman has been detected, the data processor  52  causes the display  23  to notify an alarm and what has been detected. This indication of an alarm may be by generation of a high-pitched sound or by flashing of a red warning light. 
     FIG. 5  is a diagram for explaining a mass spectrum of sarin, obtained by the above-mentioned embodiment of the present invention. This is an example that the vapor of sarin was directly introduced into the sample introduction unit, in which positive ions were detected, and a drift voltage of 60V and the sample introduction unit and the ionizing unit were set at a temperature of 110° C. 
   As shown in  FIG. 5 , in this case, signals of m/z=99 and 141 were detected. Because sarin has a molecular weight MGB=140, the m/z=141 indicates that signals are from (MGB+H) +  and m/z=99 indicates that signals are from decomposed substances of sarin. The m/z values of 99 and 141 of sarin as a detection object are previously stored in the database. By collating m/z values detected from test samples with stored data, decision is made whether the chemical agent being tested is sarin or not. When both signals of m/z=99 and 141 are detected, decision is made that sarin has been detected. This detection method makes it possible to reduce a false alarm rate. If by any chance a signal of m/z=99 (or 141) is issued from some other substance and only a signal of m/z=99 (or 141) is detected, a false alarm may be issued that sarin has been detected. 
     FIG. 6  is a diagram for explaining a mass spectrum of soman, obtained by the above-mentioned embodiment of the present invention. This is an example that the vapor of soman was directly introduced into the sample introduction unit, in which positive ions were detected, and a drift voltage of 60V and the sample introduction unit and the ionizing unit were set at a temperature of 110° C. 
   As shown in  FIG. 6 , in this case, signals of m/z=99, 183 and 365 were detected. Because soman has a molecular weight MGB=182, the m/z=183 indicates that signals are from (MGD+H) +  and m/z=365 indicates that signals are from (2MGD+H) + . The m/z=99 indicates that signals are from decomposed substances of soman. The m/z values of 99, 183 and 365 of soman as a detection object are previously stored in the database. When m/z values detected from test samples are collated with stored data, if, out of m/z=99, 183 and 365, two or three signals at m/z=99 are found, decision is made that soman has been detected. This detection method makes it possible to reduce a false alarm rate. If by any chance a signal of m/z=99 (or 183 or 365) is issued from some other substance and only a signal of m/z=99 (or 183 or 365) is detected, a false alarm may be issued that soman has been detected. 
     FIG. 7  is a diagram showing measured results of ion source temperature dependence of signals at m/z=99 detected when a sample of sarin or soman was introduced. As is clear from this diagram, when the ionizing unit  2  is raised higher than 100° C., the signal strength goes down till 150° C. This is considered because the decomposition of sarin or soman accelerates beyond 100° C. Therefore, by limiting the ion source temperature below 150° C., a greater quantity of signals can be obtained. 
     FIG. 8  is a diagram showing measured results of drift voltage dependence of signals at m/z=99 detected when sarin or soman was introduced as a sample. As is apparent from  FIG. 8 , signals larger than background can be obtained when the drift voltage is higher than 30V and until 90V. What is meant by background here is that the level of signals with m/z=99 when neither sarin nor soman was not introduced as a sample. Decision is made whether or not sarin or soman is found while monitoring signals larger than background signals. Therefore, by setting the drift voltage in a range from 30V to 90V, a large quantity of signals can be obtained. 
   As has been described, according to the present invention, by drawing in a sample and examining the m/z by the analyzer unit of the detection apparatus [atmospheric pressure chemical ionization (APCI) with mass spectrometer (MS)], it is easy to verify whether or not there is sarin or soman. 
   It should be further understood by those skilled in the art that although the foregoing description has been made on embodiments of the invention, the invention is not limited thereto and various changes and modifications may be made without departing from the spirit of the invention and the scope of the appended claims.

Technology Category: 3