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    • 专利摘要:
    SAMPLE ANALYSIS SYSTEMS AND METHODS The present invention relates, in general, to systems and methods for analyzing samples. In certain embodiments, the invention provides a system for analyzing a sample that includes a probe including material connected to a high voltage source, a device for generating a heated gas, and a mass analyzer.
    公开号:BR112013017419B1
    申请号:R112013017419-6
    申请日:2011-12-29
    公开日:2021-03-16
    发明作者:Robert Graham Cooks；Guangtao Li；Xin Li；Zheng Ouyang
    申请人:Purdue Research Foundation；
    IPC主号:
    专利说明:

    RELATED ORDER
    The present application claims the benefit and priority to the U.S. provisional patent application with serial number 61 / 430,021, filed on January 5, 2011, the contents of which are incorporated in their entirety for reference. GOVERNMENTAL SUPPORT
    The North American Government has a license paid off in this invention and the right in limited circumstances to require the patent holder to license to third parties on reasonable terms, as provided under the terms of Concession Number CHE0848650 granted by the National Science Foundation and the Number de Concessão DE-FG02- 06ER15807 granted by the Department of Energy. FIELD OF THE INVENTION
    The invention relates, in general, to systems and methods for analyzing samples. FUNDAMENTALS
    The chemistry of functional groups is based on alkanes. This provides a pedagogical imperative for its characterization that complements the economic imperative of characterizing heavy alkane ("heavy"). Among spectroscopic methods, mass spectrometry has been associated particularly strongly with the oil industry, specifically the analysis of hydrocarbon-based cracking products (Fisher et al., Anal. Chem. 1975, 47, 59). The first commercial mass spectrometers were used for this purpose and the influential method of chemical ionization and, much earlier, of fundamental ionic / molecular chemistry, was developed by petroleum scientists (Field et al., J. Am. Chem. Soc. 1956, 5697; and Field et al., J. Am. Chem. Soc. 1957, 79, 2419). More recently, high-resolution ionic cyclotron mass resonance (MS) mass spectrometry has been applied to help elucidate the remarkable complexity of petroleum-derived materials using Kendrick's mass defects to compactly organize the various group constituents of oil-derived samples (Qian et al., Energ. Fuel. 2001, 15, 492). Two groups of petroleum-derived compounds, asphaltenes and waxes, however, still present particular difficulties in detailed characterization by MS and other methods (Pinkston et al., Energy Fuels 2009, 23, 5564; and Pomerantz et al., J Am. Chem. Soc. 2008, 130, 7216). SUMMARY
    The invention relates, in general, to systems and methods for analyzing samples. The systems and methods of the invention allow a mass spectral analysis of heavy alkanes, and therefore allow an analysis of certain petroleum-derived compounds that previously could not be easily analyzed by mass spectrometry, such as waxes.
    In certain aspects, the invention provides systems for analyzing a sample that include a probe including material connected to a high voltage source, a device for generating a heated gas, and a mass analyzer. The material can be a porous material (for example, paper, filter, paper or PVDF membrane) or a non-porous material (for example, a metal such as aluminum). An additional description of systems using porous materials for ionization is provided in PCT / US 10/32881 by Purdue Research Foundation and Wang et al., Angew. Chem. Int. Ed. 2010, 49, 877, with the contents of each of these being incorporated in their entirety as a reference. In certain modalities, the system operates under ambient conditions.
    In certain embodiments, the heated gas is directed at the probe, for example, the heated gas is directed at one end of the probe. In other modalities, the system also includes a chamber configured to surround the probe and the device for generating the heated gas. In this mode, the gas inside the chamber is heated and, consequently, heats the probe. Therefore, the heated gas does not need to be directed at the probe. An example gas is nitrogen. Due to the system configuration, the heated gas assists in the ionization of the sample and participates in a chemical reaction with the sample, that is, the heated gas participates in an ionic reaction to ionize the sample and also modifies the analyte. In general, ionization and chemical reaction occur simultaneously.
    Exemplary porous materials include paper or PVDF membrane. An exemplary role is filter paper. In particular modalities, the probe is shaped so that it has a pointed tip. For example, in certain modalities, the probe is composed of filter paper that is shaped like a triangular piece. Exemplary non-porous materials include metals, such as aluminum. In particular modalities, the probe is shaped so that it has a pointed tip. For example, in certain modalities, the probe is composed of aluminum that is shaped like a triangular piece.
    The mass analyzer can be that of a benchtop mass spectrometer or a portable mass spectrometer. Exemplary mass analyzers include a quadrupolar ion trap, a straight ion trap, a cylindrical ion trap, an ionic cyclotron resonance trap, or an orbitrap.
    In other respects, the invention provides a method for analyzing a sample that involves placing a sample in contact with a material, applying high tension and heat to the material to generate analyte ions in the sample that are expelled from the material, and analyzing the expelled ions. In certain modalities, the method is carried out under ambient conditions. In certain embodiments, the analysis involves providing a mass analyzer to generate a mass spectrum of analytes in the sample.
    The sample can be any chemical or biological sample. The sample can be a liquid or a solid. In particular embodiments, the sample is a solid. In certain embodiments, the solid is a heavy alkane, such as an oil-derived compound. In particular embodiments, the oil-derived compound is a wax.
    Heat can be produced by any method known in the art. In particular embodiments, heat is produced from a heated gas. In certain embodiments, the heated gas is directed at the probe, for example, the heated gas is directed at one end of the probe. In other modalities, the step of applying the method is conducted in a confined chamber, and, therefore, the gas inside the chamber is heated and, consequently, heats the probe. Therefore, the heated gas does not need to be directed at the probe. An example gas is nitrogen. In certain modalities, the heated gas assists in the ionization of samples and participates in a chemical reaction with the sample, that is, the heated gas participates in an ionic reaction to ionize the sample and also modify the analyte. In general, the ionization step and the chemical reaction occur simultaneously.
    Another aspect of the invention provides methods for ionizing a sample which involves applying high tension and heat to a material to generate ions from an analyte in the sample.
    Another aspect of the invention provides methods for analyzing a heavy alkane which involves obtaining a heavy alkane, and using a direct ambient ionization technique to analyze the heavy alkane. In particular embodiments, heavy alkane is a solid. In certain embodiments, heavy alkane is a component of a petroleum-derived compound. In particular embodiments, heavy alkane is a wax.
    Exemplary mass spectrometry techniques using direct ambient ionization / sampling methods include electrospray desorption ionization (DESI; Takats et al., Science, 306: 471-473, 2004 and U.S. patent number 7,335,897); direct real-time analysis (DART; Cody et al., Anal. Chem., 77: 2297-2302, 2005); Ionization by Discharge of Dielectric Barrier at High Atmospheric Pressure (DBDI; Kogelschatz, Plasma Chemistry and Plasma Processing, 23: 1-46, 2003, and international PCT publication number WO 2009/102766), and laser assisted absorption / ionization ( ELDI; Shiea et al., J. Rapid Communications in Mass Spectrometry, 19: 3701-3704, 2005). The contents of each of these are incorporated here in their entirety as a reference.
    In particular embodiments, the direct ambient ionization technique involves placing the heavy alkane in contact with a material, applying high tension and heat to the porous material to generate ions from an analyte in the heavy alkane that are expelled from the material, and analyzing the ions expelled. The material can be a porous material (for example, paper, filter, paper or PVDF membrane) or a non-porous material (for example, a metal, such as aluminum). An additional description of systems using porous materials is provided in PCT / US 10/32881 by Purdue Research Foundation and Wang et al., Angew. Chem. Int. Ed. 2010, 49, 877, with the contents of each of these being incorporated in their entirety as a reference. In certain modalities, the analysis involves providing a mass analyzer to generate a mass spectrum of analytes in the sample.
    Heat can be produced by any method known in the art. In particular embodiments, heat is produced from a heated gas. In certain embodiments, the heated gas is directed at the probe, for example, the heated gas is directed at one end of the probe. In other modalities, the step of applying the method is conducted in a confined chamber, and, therefore, the gas inside the chamber is heated and, consequently, heats the probe. Therefore, the heated gas does not need to be directed at the probe. An example gas is nitrogen.
    Other aspects of the invention provide methods for tracking carbon in the course of oil processing. The methods of the invention involve using a direct ambient ionization technique to generate ions from an analyte in a sample derived from petroleum processing, target the ions in a mass analyzer, separate ions by mass according to their mass, detect the ions separated by mass from the sample, and use the ions detected to determine the relative amounts of the various chemical forms of carbon in the sample.
    In certain embodiments, the sample is a solid. In particular embodiments, the sample includes heavy alkanes. In particular modalities, the sample is a wax.
    In certain embodiments, the direct ambient ionization technique involves placing the heavy alkane in contact with a material, and applying high tension and heat to the material to generate analyte ions in the sample that are expelled from the porous material. The material can be a porous material (for example, paper, filter, paper or PVDF membrane) or a non-porous material (for example, a metal, such as aluminum). An additional description of systems using porous materials is provided in PCT / US 10/32881 by Purdue Research Foundation and Wang et al., Angew. Chem. Int. Ed. 2010, 49, 877, with the contents of each of these being incorporated in their entirety as a reference.
    Another aspect of the invention provides methods for functionalizing an analyte in a sample that involves placing a sample in contact with a material, and applying high voltage and a heated gas to the material under conditions so that the heated gas molecules modify an analyte in the sample, thus functionalizing an analyte in the sample.
    The functionalized analyte can be converted into ions by high voltage and heated gas. The ions can be expelled from the material and analyzed. Ions can be collected and then analyzed or they can be collected after analysis, for example, using infrared spectrometry or mass spectrometry.
    The material can be a porous material (for example, paper, filter, paper or PVDF membrane) or a non-porous material (for example, a metal, such as aluminum). An additional description of systems using porous materials for ionization is provided in PCT / US 10/32881 by Purdue Research Foundation and Wang et al., Angew. Chem. Int. Ed. 2010, 49, 877, with the contents of each of these being incorporated in their entirety as a reference. In certain modalities, the system operates under ambient conditions. In certain embodiments, the gas is nitrogen.
    The sample appears to be a liquid or a solid. In particular embodiments, the sample is a solid. In certain embodiments, the solid is a heavy alkane, such as an oil-derived compound. In particular embodiments, the oil-derived compound is a wax. BRIEF DESCRIPTION OF THE DRAWINGS
    Figure 1 provides an embodiment of the systems of the invention.
    Figure 2 is a mass spectrum of n-C6oHi22 wax, atmosphere N2, 325 ° C, 6 kV, using an Orbitrap LTQ and showing expanded regions of [M + N] + and [2M + N-2H] + , M = 12C601H122
    Figures 3A and 3B are mass spectra recorded from filter paper in N2 atmosphere (a) standard Polywax 1000 sample; and (b) isotopic distribution for the C110 peaks compared to the calculated isotopic distribution of C110H222N.
    Figures 4A and 4B show ion spectra of product (a) MS / MS and (b) MS showing all fragments (above the low mass cut) generated through the sequence [M + N] + (M / Z 856, 8) ^ CnMwN '(M / Z 282.2). Note in (a) the complete set of alkene eliminations and (b) the loss of nitrogen to provide monounsaturated alkenyl cations.
    Figure 5 shows a reaction scheme of a proposed CID fragmentation mechanism that leads to the elimination of alkyl amine with the formation of alkenyl cations in the MS spectra.
    Figure 6 shows a reaction scheme of an attempted mechanism for inserting atomic nitrogen ions into alkanes on an electrically floated paper substrate. Alkanes are activated by the applied potential.
    Figure 7 shows a reaction scheme for the first steps in the formation of dimeric ions, including [2M + N-2H] +.
    Figure 8 shows a gas chromatography of Polywax 1000 (available from Restek Corporation).
    Figure 9 shows a mass spectrum of C40H82 alkane analyzed by the methods of the invention. The heated gas was at 250 ° C.
    Figure 10 shows an oil mass spectrum analyzed by the methods of the invention. The heated gas was at 350 ° C.
    Figure 11 is a C40H82 alkane [2M + N-2H] + MS / MS ion. The fragment is mono-isotopic because the precursor ion is isolated in unit resolution.
    Figure 12 is a C50H102 alkane [2M + N-2H] + MS / MS ion. The fragment is mono-isotopic because the precursor ion is isolated in unit resolution.
    Figure 13 is a C60H122 alkane [2M + N-2H] + MS / MS ion. The fragment is mono-isotopic because the precursor ion is isolated in unit resolution.
    Figure 14 is a schematic representation of a system for ambient ionization of alkanes from dry paper.
    Figures 15A-B are schematic representations of a system for ionization by mesh assisted discharge (may be accompanied by oxidation) of alkanes.
    Figure 16 shows an oil mass spectrum analyzed by the methods of the invention. The heated gas was at 300 ° C.
    Figure 17 shows an oil mass spectrum.
    Figure 18 is a low mass MS spectrum for Polywax 1000 in an N2 atmosphere at 450 ° C.
    Figure 19 is a schematic representation of a range analysis system that uses a non-porous substrate.
    Figure 20 is an MS spectrum of n-C15H32 obtained using the system configuration of Figure 19.
    Figure 21 is an MS / MS spectrum of [M + N] + alkane C40H82 ion.
    Figure 22 is an MS3 spectrum of ion [M + N] + of C40H82 alkane.
    Figure 23 is an MS3 spectrum of ion [M + N] + of C40H82 alkane.
    Figure 24 is an MS3 spectrum of ion [M + N] + of C40H82 alkane.
    Figure 25 is an MS3 spectrum of ion [M + N] + of C40H82 alkane.
    Figure 26 is a schematic representation showing a fragmentation mechanism that leads to the alkenyl cations observed in the MS spectra.
    Figure 27 is a schematic representation showing a possible mechanism for inserting nitrogen into alkanes on a paper substrate. Alkanes are activated by the applied potential.
    Figure 28 is a schematic representation showing a possible mechanism for the formation of dimeric ions from adjacent alkanes on a paper substrate. Alkanes are activated by the applied potential.
    Figure 29 is an MS spectrum of n-C14H30 recorded from filter paper in an N2 atmosphere at 50 ° C, 6 kV, using LTQ and showing [M + N] + and [2M + N] +, M = C14H30.
    Figure 30 is an MS spectrum of 10W30 petroleum-based engine oil ionized by arc discharge at 150 ° C in N2 atmosphere: all peaks are incorporated in mono-nitrogen.
    Figure 31 shows MS / MS spectra of (a) ion [M + N] + n-C18H38 alkane recorded in line (b) m / z peak 268.3 from the rinsed sample nanoESI analysis after deposition of [ M + N] + and other ions at atmospheric pressure during reactive ionization of n-C18H38.
    Figure 32 is an FT-IR spectrum of triacontane (n-C30H62) and other material deposited when collecting [M + N] + and other triacontane ions ionized by spraying on paper in a nitrogen atmosphere. Note that the new peak at 1714 cm-1 corresponds to an unsaturated alkylamine. DETAILED DESCRIPTION
    In this document, an alkane activation chemistry is shown which forms the basis for an extremely simple yet robust method for generating unique ions and recording the mass spectra of heavy alkanes, such as waxes, cycloalkanes, and compounds based on long chain functionalized alkanes. An example system configuration is shown in Figure 1. This figure shows an example system of the invention that includes a chamber surrounding a probe, a heat generating device, and an MS input. Other system configurations are possible and described in this document. Using such a system, high mass waxes can be ionized by floating the paper impregnated with high potential dry wax in a hot nitrogen atmosphere and sucking the ions generated in a mass spectrometer. The insertion of nitrogen ions in the activated alkane provides [M + N] + ions. Therefore, the heated gas assists in the ionization of the sample and participates in a chemical reaction with the sample, that is, the heated gas participates in an ionic reaction to ionize the sample and also modify the analyte. In general, ionization and chemical reaction occur simultaneously.
    C60H122 wax is deposited as a solid (either from the solution or as a sublimation) on the tip of a piece of filter paper cut in a triangle. A few kV potential is applied to the paper in a heated nitrogen atmosphere, and a spectrum is recorded, such as that shown in Figure 2. The C60 wax spectrum is dominated (excluding carbon isotopes) by only two ions: [ M + 14] + and [2M + 12] +, where M is the monoisotopic molecular weight of the compound, that is, 842.9546 Da in the case of C60H122. The exact mass measurements made using an Orbitrap LTQ instrument showed that the main ions have the formula [M + N] + whose expected value is M / Z 856.9577; the measured value of M / Z 856.957 (2) is in accordance with this value, but excludes [M + CH2] + which requires M / Z 856.9703. Similarly, the main dimeric ion, [2M + 12] +, has the formula [2M + N-2H] + with a measured mass of 1697.896 (8) and an expected mass of 1697.8967. The same nitrogen incorporation was observed for C40 and C50 waxes as shown in Table 1 below. Table 1

    To explore the applicability of this chemistry in analyzing molecular weight distributions of heavy alkanes, a commercial heavy wax Polywax 1000 standard (Restek Corporation, Bellefonte, PA) was examined. The main peak envelope corresponds to saturated alkanes. For example, the ion in nominal M / Z 1558 corresponds to the alkane with carbon number C110 (average chemical mass of adduct N 1558.95; exact mass of isotope 12C 1557.74, measured mass 1557.7). The isotopic distribution (Figure 3B) is in accordance with the calculation for C110H222. The molecular weight distribution in Figure 3 extends to at least M / Z 1895, which corresponds to the saturated hydrocarbon C134H270. The peak M / Z 1165.33, corresponding to C82H166, is the most abundant. These observations are consistent with the manufacturer's data (see Figure 8 and Table 2 below).


    In addition to the [M + N] + series, an ion corresponding to [(M '+ 23] + is evident from the isotopic envelope (M' is the alkane with two less carbon atoms, Figure 3B), as well as in molecular weight profile (Figure 3A).
    The optimized conditions for alkane analysis (Examples in this document) were used to produce the data shown in Figures 2 and 3. The experiment was carried out in an N2 atmosphere in an isolated chamber normally used for electrically heated chemical ionization at atmospheric pressure at 80-500 ° C, with a potential of 6 kV applied to the paper that holds the sample. Two other sets of experimental conditions were also explored (Example 2 in this document). In one of them, the sample was ionized again from the paper, but was heated outdoors with a heat gun while supplying the high voltage. In the other alternative, which followed the previous work on desorption ionization by electrospray transmission mode (DESI; Chipuka et al., J. Am. Soc. Mass Spectrom. 2008, 19, 1612), the sample was placed on a mesh of stainless steel, a potential of 1.5-2 kV was applied to a needle in front of the mesh, and a stable arc discharge established. Summarizing the data from the three types of experiments: (i) Sprinkling on paper in an N2 chamber heated to 400 ° C (preferably, 100 ° C to 150 ° C, is successful for larger n-alkanes (> C28) ; provides [M + N] + and [M + N-2H] + as well as dimeric ions [2M + N-Hy] + where y is 1 and 4. (ii) Sprinkling on paper outdoors at 300 ° C is effective for medium-sized alkanes and provides mainly [MH] +, accompanied by several oxygenated species, (iii) Discharge in open-air mesh, with heating, was successful for medium and light hydrocarbons, as well as other hydrocarbons. More detailed information is provided in the Examples in this document.
    Due to the fact that it was easier to control the conditions to produce [M + N] + instead of [M-H] + ions, more attention was paid to these species. However, both ions are formed by highly unusual chemical processes. The [M-H] + ions do not appear to be formed by ionic / molecular reactions, however, they seem to involve an ionization process in the field (Examples in this document). According to Rollgen (Ber. Bunsenges. Phys. Chem. 1971, 75, 988), the origin of [M-H] + was experimentally attributed to desorption in the field with transfer of protons to the emitting surface (paper or metal). See Pirkl (Analytical and Bioanalytical Chemistry, 2010, 397 (8), 3311). Observation of traces of molecular radical cations (M + ') suggests that a secondary ionization component occurs by simple ionization in the field. The most notable products are [M + N] + and [2M + N-2H] +. The main reaction, which leads to the latter, formally involves liquid N + in addition to an alkane, as shown in Figures 2, 3A and 3B, 9, and 10. This represents an unprecedented substitution in the C-C (or C-H) bond of an alkane.
    The multistage experiments (MS / MS and MS) provided information about the nature of the [M + N] + ions. The MS / MS data exhibited mainly alkene eliminations (Figure 4A), a highly characteristic fragmentation for long chain alkyl compounds, whether functionalized or not. The MS data provided access to ions of lower mass and showed additional surprising results typified by the data in Figure 4B. Another fragmentation of any of the ions generated by loss of alkene from the precursor [M + N] + (ie, of its lower counterparts [M + N] +) occurs by loss of alkyl amines of specific size to supply cations of alkenyl with a narrow band of small carbon numbers. MS data indicate the position of the nitrogen insertion, showing a strong preference for the C-6 to C-9 insertion. A possible mechanism for fragmentation is shown according to Figure 5 for a representative spectrum MS (which involves the intermediate ion of M / Z 226).
    Without adhering to any theory or mechanism of action, these data suggest the insertion of nitrogen in C-C bonds that are close, but not at the ends of the n-alkane chain. The specificity of the nitrogen insertion site suggests an ionic N-donor instead of a free radical (such as the azide radical; Continetti et al., J. Chem. Phys. 1993, 99, 2616). The main ions generated in a nitrogen discharge at atmospheric pressure are N3 + and N4 + (Dzidic et al., Anal. Chem. 1976, 48, 1763). This leads to the purpose that the primary reaction with alkanes involves the insertion of N + from an azide ion with dinitrogen elimination.
    The role of high voltage is not simply to generate a corona discharge in the nitrogen atmosphere. These discharges are often generated and there is no associated reactivity. Nitrogen can also participate in a chemical reaction with the analyte. Nitrogen acts as a chemical ionizing agent, and alkane is activated by the electric field, allowing it to be reacted with ionized nitrogen. Apparently, the presence of a high electric field at the point of the material where the sample is placed is likely to be responsible for the insertion of the atomic nitrogen ion; in other words, the process is not purely a gas phase reaction. In preferential modalities, the wax is placed on the tip of the material since it is neither mobile nor a solvent to mobilize it.
    Without adhering to any theory or mechanism of action, it is experimentally proposed that non-volatile waxes be activated in the field while being bonded to the substrate where they are strongly polarized by strong terminal electric fields. It is also suggested that the alkanes activated in the field react with donor N, N3 +. The evidence for the role of the electric field results from these facts (i) the reaction does not occur with other compounds tested - for example, peptides, cholesterol, cocaine etc. (ii) the reaction is favored in heavy alkanes over light alkanes (this can contribute to the reduction of the lower mass envelope in Figure 3A) (iii) the occurrence of dimeric ions supports a surface-mediated mechanism. It is proposed that the physisorbed alkane molecule is polarized by the charge on the paper, leading to induced charges in the molecule as shown in Figure 6. In certain cases, dimeric ions can be formed. See Figure 7.
    The favored azide cation attack site will be at the end of the molecule closest to the paper due to the magnitude of the charge induced in the alkane molecule (Lorquet, Mol. Phys. 1965, 9, 101; and Lorquet, J. Phys. Chem. 1969, 73, 463). Steric factors are likely to contribute to the favored reaction site being some distance from the chain termination. Apparently, there are no thermochemical data in the azide cation and no case of its ionic / molecular reactivity. The analogs closest to the N + insertion in a CH or CC alkane bond involve atomic ionic chemistry in light metal gas phase (Schwarz et al., Pure Appl. Chem. 2000, 72, 2319; and Gord et al., J. Chem, Phys. 1989, 91, 7535). It is noted that the intermediate generated in the proposed C-C insertion reaction is a nitrogen atom, a highly reactive class of intermediates of considerable current interest (Novak et al., J. Phys. Org. Chem. 1998, 11, 71).
    MS / MS data on dimeric ions (Figures 11-13) provide support for the field activation mechanism proposed above. The insertion of N + interchanging with the elimination of H2 to provide a cross-linked nitrogen ion is proposed to be responsible for the formation of dimeric ions. This reaction is proposed to be followed by the redisposition to a stable ammonium adduct that breaks down through activation with elimination of alkene to form a product [M + N] + of lower mass.
    It has been argued that the effective use of oil resources requires carbon tracking through the various chemical forms that occur in the course of oil processing. This complex task, referred to as structure-oriented grouping (Jaffe et al., Ind. Eng. Chem. Res. 2005, 44, 9840) involves monitoring the 'carbon budget' and requires significant resources in terms of analytical methodology that are justified the economic value of the knowledge acquired. The difficulty of analyzing high molecular weight alkanes by mass spectrometry is an impediment to the complete implementation of this task. These compounds can be ionized by two methods: the venerable field desorption (FD) method is commonly used. This manually intensive method requires a sample solution to be dripped onto a thin dendritic emitter to which a potential is applied as it is heated in a vacuum to create ions. The alternative method is Amirav's elegant molecular beam electron ionization method (Granota et al., Int. J. Mass Spectrom. 2005, 244, 15). Both methods provide reproducible data, however, both involve vacuum ionization and, therefore, it lacks the simplicity of the procedure described in this document. Apparently, the N + insertion methodology described in this document will have complementary properties and practical utility. Ion Collection
    The systems and methods for collecting ions that have been analyzed by a mass spectrometer are shown in Cooks, (U.S. patent number 7,361,311), the contents of which are fully incorporated by reference. In general, the preparation of microchip arrangements of molecules primarily involves the ionization of analyte molecules in the sample (solid or liquid). The molecules can be ionized by any of the methods discussed above. Then, the ions are separated based on their mass / charge ratio or e, their mobility, or both mass / charge ratio and mobility. For example, ions can be accumulated in an ion storage device, such as a quadrupolar ion trap (Paul trap, including variants known as the cylindrical ion trap and the linear ion trap) or a cyclotron resonance trap (ICR ). Whether inside this device or using a separate mass analyzer (such as a quadrupole mass filter, magnetic sector or flight time), the stored ions are separated based on mass / charge ratios. Additional separation can be based on mobility using ion displacement devices or the two processes can be integrated. The separated ions are then deposited on a microchip or substrate at individual points or locations according to their mass / charge ratio or on their mobility to form a microarray.
    To achieve this, the microchip or substrate is moved or swept in the x-y directions and stopped at each location for a predetermined period of time to allow the deposit of a sufficient number of molecules to form a location having a predetermined density. Alternatively, the gas phase ions can be electronically or magnetically directed to different locations on the surface of a chip or stationary substrate. The molecules are preferably deposited on the surface with the preservation of their structure, that is, they are landed smoothly. Two facts make it likely that decoupling or denaturation on landing can be avoided. Surfaces suitable for a soft landing are chemically inert surfaces that can efficiently remove vibratory energy during landing, but which will allow spectroscopic identification. Surfaces that promote neutralization, rehydration or having other special characteristics can also be used for a smooth landing of protein.
    In general, the surface for the ion landing is located behind the mass spectrometer detector assembly. In ion detection mode, high voltages over the conversion diode and multiplier are switched on and ions are detected to allow general spectral qualities, the signal-to-noise ratio and mass resolution over the full mass range be examined, the voltages on the conversion diode and the multiplier are turned off and the ions are allowed to pass through the hole in the detection assembly to reach the landing surface of the plate (such as a gold plate). The surface is grounded and the potential difference between the source and the surface is 0 volts.
    An exemplary substrate for a soft landing is a gold substrate (20 mm x 50 mm, International Wafer Service). This substrate can consist of a Si pellet with a chromium adhesion layer of 5 nm and 200 nm of gold deposited in polycrystalline vapor. Before being used for ion landing, the substrate is cleaned with a mixture of H2SO4 and H2O2 in a 2: 1 ratio, washed vigorously with deionized water and absolute ethanol, and then dried at 150 ° C. A Teflon mask, 24 mm x 71 mm with an 8 mm diameter hole in the center, is used to coat the gold surface so that only a circular area with a diameter of 8 mm on the gold surface is exposed to the ion beam for a smooth landing of ions from each ion beam selected by mass. The Teflon mask is also cleaned with 1: 1 MeOH: H2O (v / v) and dried at an elevated temperature before use. The surface and the mask are attached to a retainer and the exposed surface area is aligned to the center of the optical ion geometric axis.
    You can use any period of time for the ions to land. Between each ion landing, the instrument is ventilated, the Teflon mask is moved to expose a new surface area, and the surface retainer is relocated to align the target area with the ion optical geometric axis. After soft landing, the Teflon mask is removed from the surface.
    In another embodiment, a linear ion trap can be used as a component of a soft landing instrument. The ions travel through a heated capillary in a second chamber through ion guides in vacuum augmentation chambers. The ions are captured in the linear ion trap by applying appropriate voltages to the electrodes and RF and DC voltages to the segments of the rods of the ion trap. The stored ions can be radially ejected for detection. Alternatively, the ion trap can be operated to eject the ions of the selected mass through the ion guide, through a plate on the microarray plate. The plate can be inserted through a valve system with a mechanical door without ventilating the entire instrument.
    The advantages of the linear quadrupolar ion trap over the standard Paul ion trap include increased ion storage capacity and the ability to eject ions both axially and radially. Linear ion traps provide unit resolution to at least 2000 Thomspon (Th) and have the ability to isolate ions from a single mass / charge ratio and then perform subsequent excitation and dissociation in order to register an MS product from ion / spectrum MS. The mass analysis will be performed using resonant waveform methods. The mass range of the linear trap (2000 Th or 4000 Th, but adjustable to 20,000 Th) will allow mass analysis and a smooth landing of most of the molecules of interest. In the soft landing instrument described earlier, ions are introduced axially into the rods of the mass filter or the rods of the ion trap. Ions can also be introduced radially into the linear ion trap.
    The methods of operation of the soft landing instruments described previously and other types of mass analyzers for smoothly landing ions of different masses at different locations in a microarray will now be described. The ions from the functionalized analyte from the sample are introduced into the mass filter. The ratio of mass to selected charge ions will be filtered by mass and gently landed on the substrate over a period of time. Then, the mass filter settings will be scanned or scaled and the corresponding movements in the position of the substrate will allow the deposition of the ions in defined positions on the substrate.
    The ions can be separated in time so that the ions arrive and land on the surface at different times. While this is being done, the substrate is being moved to allow the separate ions to be deposited in different positions. A rotating disk is applicable, especially when the rotation period corresponds to the operating cycle of the device. Applicable devices include flight time and linear ion mobility displacement tube. The ions can also be directed to different locations on a fixed surface by scanning electric or magnetic fields.
    In another embodiment, the ions can be accumulated and separated using a single device that acts as both an ion storage device and a mass analyzer. The applicable devices are ion traps (Paul, cylindrical ion trap, linear trap, or ICR). The ions are accumulated followed by a selective ejection of the ions for smooth landing. The ions can be accumulated, isolated as ions of the mass-to-selected charge ratio, and then gently landed on the substrate. The ions can be accumulated and grounded simultaneously. In another example, ions of various mass-to-charge ratios are continuously accumulated in the ion trap, while at the same time, ions of a selected mass-to-charge ratio can be ejected using SWIFT and gently landed on the substrate.
    In an additional modality of the soft landing instrument, ion mobility is used as an additional (or alternative) parameter. As before, the ions are generated by a suitable ionization source, such as that described in this document. The ions are then subjected to pneumatic separation using a transverse air flow and an electric field. The ions move through a gas in a direction established by the combined forces of the gas flow and the force applied by the electric field. The ions are separated in time and space. Ions with greater mobility arrive at the surface earlier and those with lesser mobility arrive at the surface later in spaces or locations on the surface.
    The instrument may include a combination of the devices described for the separation and smooth landing of ions of different masses at different locations. Two of these combinations include an ion storage (ion traps) plus a time separation (TOF or ion mobility displacement tube) and an ion storage (ion traps) plus a space separation (sectors or ion mobility separator).
    It is desirable that the analyte structure is maintained during the soft landing process. The strategy for maintaining the analyte structure upon deposition involves keeping the deposition energy low to prevent dissociation or transformation of the ions when they land. This needs to be done, while at the same time, minimizing the size of the site. Another strategy is to select by mass and gently land an incompletely dissolved form of the ionized molecule. Extensive hydration is not necessary for the molecules to maintain their solution phase properties in gas phase. Hydrated molecular ions can be formed by electrospray and separated while they are still "wet" for a smooth landing. The surface of the substrate could be a “wet” surface for a smooth landing, this would include a surface with only one monolayer of water. Another strategy is to hydrate the molecule immediately after mass separation and before soft landing. Various types of mass spectrometers, including the linear ion trap, allow ionic / molecular reactions including hydration reactions. It may be possible to control the number of hydration water molecules. Other additional strategies consist of deprotonating the selected ions by mass using ionic / molecular or ionic / ionic reactions after separation, but before smooth landing, to avoid unwanted ionic / superficial reactions or protonate in a sacrifice derivatization group that is subsequently lost.
    Different surfaces are likely to be more or less suitable for a successful smooth landing. For example, chemically inert surfaces that can efficiently remove vibratory energy during landing may be suitable. The properties of surfaces will also determine what types of in-situ spectroscopic identification are possible. The ions can be gently landed directly on the suitable substrates for MALDI. Similarly, a smooth landing on active SERS surfaces should be possible. An in situ MALDI and a secondary ionic mass spectrometry can be performed using a bidirectional mass analyzer, such as a linear trap like the mass analyzer in the ion deposition stage and also in the ion analysis stage. deposited material.
    In another mode, ions can be collected in the environment (ambient pressure, but still under vacuum) without mass analysis (See the examples in this document). The collected ions can then be subsequently analyzed using any suitable technique, such as infrared spectrometry or mass spectrometry. Incorporation as a reference
    Any and all references and references to other documents, such as patents, patent applications, patent publications, newspapers, books, documents, web content, which were made during this disclosure are hereby incorporated in their entirety by way of reference. for all purposes. Equivalents
    The invention can be incorporated in other specific forms without departing from the spirit or the essential characteristics of the same. Therefore, the previous modalities must be considered in all aspects illustrative and not limiting the invention described in the present document. EXAMPLES Example 1: Analysis of alkanes using mass spectrometry
    An LTQ Finnigan mass spectrometer (Thermo Fisher Scientific, San Jose, CA) was used for the low resolution experiments and an Orbitrap LTQ available from the same company was used for high resolution measurements. The instrumental conditions, except where otherwise specified, were as follows. Inlet capillary temperature: 200 ° C; heated capillary voltage: 15 V; tube lens voltage: 65V. The experimental configuration for ionization from paper was similar to that described in a previous publication (Wang et al., Angew. Chem. Int. Ed. 2010, 49, 877) except that the solvent was not used and the paper was placed inside the closed heated chamber of the LTQ normally used for atmospheric pressure chemical ionization experiments. The chamber was filled with nitrogen gas heated to about 350 ° C. Solvents and other chemicals, including pure alkanes, were purchased from Sigma-Aldrich (St. Louis, MO), and were used without further purification. The paper substrate was Grade 1 chromatographic paper purchased from Whatman (Maidstone, England). Polywax 1000 was purchased from Restek Corporation (110 Benner Circle, Bellefonte, PA). The characterization of gas chromatography / flame ionization detection (FID) of Polywax 1000 (data with Restek) is shown in Figure 8. An asymmetric distribution is observed; the most intense signal in the weighted distribution for intensity occurs approximately in 15C94 while the highest absolute intensity occurs in C86. The qualitative standard for crude oilASTM® D5307 was purchased from Sigma-Aldrich. It has 16 alkanes with equal amounts of each component, as shown in Table 3.Table 3

    Example 2: Alternative system configurations
    Figures 14-15 show alternative system configurations to those previously described in Example 1 for analysis of alkanes. Figure 14 shows a system configuration for use in the hot outdoors. The method uses a heat of about 300 ° C and operates on air. The result is spectra dominated by [M-H] + ions and also includes various oxidation products.
    Figure 15 shows a system configuration that involves mesh-assisted arc unloading. This method uses heating and operates on air, but the sample is on a stainless steel mesh, not on paper. This was successful for light and medium length alkanes. A system configuration for conducting an arc discharge technique is described in Li (Analyst, 135, 2010, 688-695).
    The main data resources for each of the three experimental methods are: i) Sprinkling on paper in a heated chamber, atmosphere N2, electrically heated to approximately 400 ° C for larger n-alkanes (> C28), provides [M + 14] + in other words, [M + N] + and [M + 12] +, in other words, [M + N-2H] +, as well as some dimeric ions [2M + N-yH] + where y = 1 and 4 (system configuration described in Example 1). The main reaction formally involves a net transfer of N + to generate the [M + N] + ions as shown in Figures 2, 9, and 10. This represents an unprecedented CH or CC substitution, as discussed later, ii) Sprinkling in outdoor paper using a heat gun at a temperature of 300 ° C, for medium sized alkanes provides mainly [MH] +; accompanied by several oxygenated species, as shown in Figure 16. iii) Discharge in mesh in the open air, using a stainless steel mesh, a heat gun, for light and medium hydrocarbons.
    Figure 9 shows the formation of the ions characteristic [M + 14] + and [2M + N-2H] + from a single n-alkane, C40H82. In addition to the main ions, there are also secondary ions. They include [M + N + 23] +, probably as a result of sodium incorporation. The oil sample (Table 3) provides the expected distribution of lower alkanes (Figure 10) as well as some small peaks due to higher mass dimerization when examined by methods conducted with heated nitrogen gas. An expanded view of the crude oil sample (Figure 17) indicates the presence of a variety and secondary ions, among which the radical cation, M + is of most interest.
    Another feature of interest in alkane spectra is the very low mass presence of alkyl and alkenyl cations, as noted for the Polywax sample in Figure 18. The abundant C4 to C8 alkyl cations and alkenyl ions could serve as the ions reagents in chemical ionization at atmospheric pressure of vaporized long chain alkanes.
    The outdoor heating method was successful for C32 alkane, providing prominent [M-H] + ions in M / Z 449, 393, 337 and 281 (Figure 10). There are data in the literature indicating that [M-H] + ions can be formed by hydride ion transfer to generate carbocations; this can occur on the surface of field emitters or by ion-induced adsorption in the field of unsaturated compounds. The origin of the [M-H] + ions has also been attributed to field ionization combined with the transfer of hydrogen from the molecules to the radical sites on the emitting surface.
    The dominant species observed depends on the experimental conditions, which can be adjusted to favor [M-H] + or [M + N] + as indicated. If the formation of these species is controlled by the size of the alkanes rather than by experimental conditions, then, in some size of alkane, both types of ions must be observed in the same spectrum. However, this situation has not been found. Secondary species include M + (seen, for example, in C20-C44, as well as the dimeric ions already mentioned). The process of [M-H] + formation, including experiments with labeled alkanes, suggests that this ion is not generated from low-mass alkyl cations observed in the mass spectra by ionic / molecular reactions. The logical alternative to an ionic / molecular process for the formation of [M-H] + is an ionization / desorption process in the field. Following Rollgen, the origin of [M-H] + was attributed to desorption in the field that involves the transfer of protons to the emitting surface. Observation of molecular radical (M + ') cation pulls suggests that a secondary ionization component occurs by single-field ionization. Under these conditions, there are also no protonated molecules.
    In the arc discharge method, instead of applying a potential to the substrate on which the hydrocarbon sample is placed, the sample can be placed on a steel mesh and a corona needle can be used to induce a discharge. Using this arc discharge method described here, very similar data are obtained with the incorporation of nitrogen atoms in the alkanes. See Figure 30.
    Another system configuration is shown in Figure 19. This figure shows a system configuration that uses a non-porous substrate. A non-porous exemplifying material is a metal, such as aluminum. The substrate is connected to a high voltage source and the alkane (for example, wax) is applied to the substrate. The sample is then heated over the substrate to produce alkane ions. Figure 20 shows the mass spectrum of n-C15H32 recorded from the aluminum foil in an N2 atmosphere at 200 ° C, 3 kV, discharge current 4.65 uA, using LTQ and showing [M + N] + and [2M + N] +, M = C15H32. Example 3: Composition and ionic structure
    Exact mass measurements were used to confirm the structures of the main ions generated by the methods of the invention using heated nitrogen gas. Mass spectrometry experiments in tandem and MS were used to obtain additional information about these ions. The data are shown in Figures 21 to 25. The MS / MS data are discussed in the detailed description. The lower mass range cannot be seen in the ion trap, but the upper region shows elk elimination products with peaks at 14 Da intervals (Figure 21). The lower mass ions are accessible in MS experiments and those for representative C40H82 alkane show that the intermediate alkene elimination products, M / Z 198, 226, 254, and 296, all show a similar behavior in (i) to the elimination of alkene and (ii) to supply a small set of lower mass alkenyl ions (Figures 22-25). The first fact indicates that the losses of alkene observed in the MS / MS spectra are likely to be considerable due to neutral punic fragments rather than a series of successive losses. The second fact indicates that the selected intermediate ion fragments with nitrogen loss and their behavior are better accommodated assuming that the original N + insertion occurred near the end of the alkyl chain to create an N, N-alkyl alkenyl amine. The fragmentation of these ions by loss of an alkyl amine provides the alkenyl cation, the length of which indicates the nitrogen insertion position. The data indicate a strong preference for C6 to C9 of insertion N. A possible mechanism for fragmentation in a representative MS case (that of m / z 226) is shown in Figure 26.
    Therefore, the data strongly suggest the insertion of nitrogen into the C-C bonds and that these bonds are located close to the ends of the n-alkane chain. This supports the hypothesis that the connections are activated by the electric field. It is also evident that the reactive species responsible for the N insertion are an ion, presumably, the azide ion, not the azide radical. This leads someone to propose the capo assisted alkane activation mechanism and the insertion of axide ion shown in Figure 27. The alkane molecule is polarized by the charge on the paper leading to induced charges as shown. The favored azide cation attack site will occur at the end of the molecule closest to the paper. Steric factors probably contribute to the favored reaction site being some distance from the chain termination Example 4: Dimeric ions
    The [2M + 12] ion is [2M + N-2H] + based on HRMS measurements. This would involve the transfer of alkyl with elimination of H2 if it occurred from the monomer in an ionic / molecular reaction. Therefore, a mechanism involving a surface-assisted reaction in the field is more practicable, as shown in Figure 28. The azide ion can generate a new CC bond between the activated and well-compacted chains or the intermediate nitrogen ion in an insertion reaction initial chain can react with an adjacent chain to generate the product. In any case, additional energy will be required for the desorption of both units which are in line with an increase in dimer relative to the monomeric product as the temperature is increased.
    In fact, there are several dimeric ions, [2M + 13] + (ca. 10%), [2M + 12] + (ca. 77%), and [2M + 10] + (ca. 13%). The relative abundances are given after the 13C correction and are used for the C60H122 system. Note the formation of the radical cation [2M + NH] + The MS / MS data (Figures 11-13) of the dimer ions follow the same pattern as the monomers, showing loss of neutral alkenes, which are in accordance with types of proposed structures. Noteworthy is the fact that the fragmentations are dominated by fragmentation to the monomer, [M + N] + with the loss of the neutral alkene.
    Additional representative examples of successful N atom incorporation into smaller alkanes have been recorded. Sometimes in these cases, the dimeric ion [2M + N] + is the base peak. An example is shown in Figure 29. Example 5: Sources of nitrogen atom
    The product ion is formally the result of inserting N + into a C-H or C-C bond of an alkane. The reaction could involve a direct N + insertion from a suitable precursor ion or an N atom insertion followed by ionization. The most abundant reagent ion in N2 in atmospheric pressure discharges is N4 + with the N3 + trimer also prominent. Therefore, the probable causes for the direct reaction are the transfer of N + and the elimination of N2 or N3 The N atom insertion route would likely involve the azide radical as the precursor.
    The radical N3 has almost the same heat of formation as N2 (l∑g +)] + N (4S) - only 0.05 +/- 0.10 eV higher - although it is kinetically stable. The N3 + cation is known from its occurrence in N2 discharges, however, there is no experimental ionic / molecular chemistry or thermochemistry in the literature. There are no thermochemical data on the N4 + radical cation the other possible, but unlikely, reactive ion. Example 6: Chemical modification and wax collection
    The activation and functionalization of aliphatic CH bonds have been studied intensively over the past few decades, mainly through reactions involved with metal transition species (Lech et al., J. Am. Chem. Soc. 111, 8588 (1989); Schwarz , Pure Appl. Chem. 72, 2319 (2000); and Labinger, Nature 417, 507 (2002). In this paper, a different strategy is reported to achieve selective CH bond activation of saturated alkanes to generate inserted ion species by nitrogen, with the nitrogen source being chemically inert dinitrogen.The functionalized species were collected directly at atmospheric pressure as they emerged from the ion source without involving mass analysis.
    The optimized conditions for alkane ionization from dry paper in a nitrogen atmosphere were used to produce the data shown. The experiment was carried out in an N2 atmosphere in an isolated chamber normally used for chemical ionization at atmospheric pressure, electrically heated to 200 ° C, with a potential of 5-6 kV applied to the paper that holds the sample. The nitrogen gas has a minimum purity of 99.9% and was passed at a rate of 5-15 L / min during operation. The collection of ions at atmospheric pressure was carried out by directing the paper substrate containing the hydrocarbon and floated in +5 kV was directed to a grounded Au / Si pellet substrate (10 mm away), in a flow of heated nitrogen was introduced with a gas flow rate of 10 L / min to maintain the nitrogen atmosphere. The Au / Si tablet was cooled using liquid nitrogen to retain the deposited species. After an hour of ion collection, the tablet was allowed to warm up to room temperature for FT-IR measurement. The tablet was also rinsed using hexane and the rinsed effluent was analyzed by nanoESI.
    First, n-C18H38 was deposited in microgram quantities as a thin film on the tip of a filter paper triangle, and a potential of 5-6 kV was applied in an atmosphere of heated nitrogen (ca. 200 ° C). The resulting mass spectrum was dominated by only two ions: [M + N] + and [2M + N- 2H] +, where M represents the examined alkane, which is verified by exact mass measurements. The [M + N] + signal lasted a long period of time (typically> 1 hour) without a noticeable decrease during wax ionization. The resulting ions were deposited on an inert surface and collected. They were deposited on an Au substrate at atmospheric pressure without the ions entering the mass spectrometer. The nanoESI MS / MS spectra of the collected sample were identical in all respects to those of the [M + N] + ion generated online and recorded during the ionization event (Figure 31). This confirms the successful deposition of the alkane species inserted by nitrogen.
    The FT-IR spectrum of the sample collected showed a new peak of absorption close to 1714 cm-1 (Figure 32), designated as the C = N stretching of a ketamine or alkaline based on the frequency predicted from RHF calculations. from the start. The lack of ammonia elimination in the MS / MS spectra of [M + N] + linear alkanes strongly suggests that nitrogen was inserted into a C-C bond instead of a C-H bond. The interpretation is in accordance with the data for N insertion in cycloalkanes, where ammonia loss is abundant when nitrogen is inserted into non-terminal C-H bonds.
    MS / MS from [M + N] + showed that the smallest ion fragment detected by Orbitrap had m / z of 58.0656 (7), having the formula of C3H8N +, also suggesting that nitrogen is located near the end of the aliphatic chain. Based on the previous analysis, nitrogen is probably not very selectively inserted into C-C bonds almost terminally linear alkanes.
    权利要求:
    Claims (21)
    [0001]
    1.System for analyzing a sample, the system CHARACTERIZED by the fact that it comprises: a probe that comprises a substrate that tapers at one end, in which the substrate is configured to hold the sample and the substrate is connected to a high voltage source to generate tension; a heating device for generating a heated gas; and a mass spectrometer comprising a mass analyzer, in which the system is configured in such a way that the voltage generated from the high voltage source and the heated gas generated from the heating device are simultaneously applied to the substrate in order to to desorb and ionize the sample from the substrate and a mass spectrometer input is operationally associated with the substrate to receive ions from the sample.
    [0002]
    2.System, according to claim 1, CHARACTERIZED by the fact that the heated gas is directed in the probe.
    [0003]
    3.System, according to claim 1, CHARACTERIZED by the fact that the heated gas is directed at one end of the probe.
    [0004]
    4.System, according to claim 1, CHARACTERIZED by the fact that it also comprises a chamber configured to cover the probe and the device to generate the heated gas.
    [0005]
    5.System, according to claim 1, CHARACTERIZED by the fact that the gas is nitrogen.
    [0006]
    6.System, according to claim 1, CHARACTERIZED by the fact that the substrate is a porous material.
    [0007]
    7.System, according to claim 1, CHARACTERIZED by the fact that the substrate is a non-porous material.
    [0008]
    8. System according to claim 7, CHARACTERIZED by the fact that the non-porous material is a metal.
    [0009]
    9. System, according to claim 1, CHARACTERIZED by the fact that the mass spectrometer is a portable mass spectrometer.
    [0010]
    10.System, according to claim 9, CHARACTERIZED by the fact that the mass analyzer is selected from the group consisting of: a quadrupolar ion trap, a rectilinear ion trap, a cylindrical ion trap, a ionic cyclotron resonance, and an orbitrap.
    [0011]
    11. Method for analyzing a sample, the method CHARACTERIZED by the fact that it comprises: contacting a sample with a substrate that tapers at one end; simultaneously applying high tension and heat to the substrate to generate ions from an analyte in the sample that are expelled from the substrate; and analyze the expelled ions.
    [0012]
    12. Method according to claim 11, CHARACTERIZED by the fact that heat is produced from a heated gas.
    [0013]
    13. Method, according to claim 12, CHARACTERIZED by the fact that the heated gas is directed at the substrate.
    [0014]
    14. Method, according to claim 13, CHARACTERIZED by the fact that the heated gas is directed at one end of the substrate.
    [0015]
    15. Method, according to claim 12, CHARACTERIZED by the fact that the gas is nitrogen.
    [0016]
    16. Method according to claim 11, CHARACTERIZED by the fact that the substrate is a porous material.
    [0017]
    17. Method according to claim 11, CHARACTERIZED by the fact that the substrate is a non-porous material.
    [0018]
    18. Method according to claim 11, CHARACTERIZED by the fact that the application step is conducted inside a confined chamber.
    [0019]
    19. Method, according to claim 11, CHARACTERIZED by the fact that analyzing comprises providing a mass analyzer to generate a mass spectrum of analytes in the sample.
    [0020]
    20. Method according to claim 11, CHARACTERIZED by the fact that the method is performed under ambient conditions.
    [0021]
    21. Method for ionizing a sample, the method CHARACTERIZED by the fact that it comprises: simultaneously applying high voltage and heat to a sample arranged in a substrate that tapers at one end to generate ions from an analyte in the sample.
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    同族专利:
    公开号 | 公开日
    CA2823711A1|2012-07-12|
    CA3023911C|2021-09-07|
    CA3023911A1|2012-07-12|
    US8932875B2|2015-01-13|
    BR112013017419A2|2020-01-28|
    WO2012094227A2|2012-07-12|
    CN103415909B|2016-02-03|
    US20150102218A1|2015-04-16|
    US9165752B2|2015-10-20|
    CN103415909A|2013-11-27|
    US20130344610A1|2013-12-26|
    WO2012094227A3|2013-01-10|
    CA2823711C|2018-12-18|
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    法律状态:
    2020-02-11| B06F| Objections, documents and/or translations needed after an examination request according [chapter 6.6 patent gazette]|
    2020-02-18| B06U| Preliminary requirement: requests with searches performed by other patent offices: procedure suspended [chapter 6.21 patent gazette]|
    2021-01-19| B09A| Decision: intention to grant [chapter 9.1 patent gazette]|
    2021-03-16| B16A| Patent or certificate of addition of invention granted|Free format text: PRAZO DE VALIDADE: 20 (VINTE) ANOS CONTADOS A PARTIR DE 29/12/2011, OBSERVADAS AS CONDICOES LEGAIS. |
    优先权:
    申请号 | 申请日 | 专利标题
    US201161430021P| true| 2011-01-05|2011-01-05|
    US61/430,021|2011-01-05|
    PCT/US2011/067771|WO2012094227A2|2011-01-05|2011-12-29|Systems and methods for sample analysis|
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