摘要:
A first mass analysis is executed in a condition that gas is not introduced into a loop-flight chamber (4), and a time-of-flight spectrum obtained in a data processor (12) is stored in a storage unit (13). Next, a second mass analysis is executed on the same sample as the one used in the first mass analysis in a condition that a valve (8) is opened and helium gas (He) is introduced into the loop-flight chamber (4), and the time-of-flight spectrum is obtained in the data processor (12). If different kinds of ions having the same m/z value exit, these ions form a single peak in the first time-of-flight spectrum, while these ions appear as separate peaks in the second time-of-flight spectrum even though they have the same m/z value. This is because, in the second mass analysis, the ions collide with the gas and have different times of flight depending on their difference in size. A spectrum comparator (14) judges a change in the position or shape of the peak by comparing the two spectra, and outputs information relating to the difference in the size of the ions (the molecular structure, charge state, or molecular class of the ions), and the like. Accordingly, a wider variety of information than ever before can be provided.
摘要:
A first mass analysis is executed in a condition that gas is not introduced into a loop-flight chamber (4), and a time-of-flight spectrum obtained in a data processor (12) is stored in a storage unit (13). Next, a second mass analysis is executed on the same sample as the one used in the first mass analysis in a condition that a valve (8) is opened and helium gas (He) is introduced into the loop-flight chamber (4), and the time-of-flight spectrum is obtained in the data processor (12). If different kinds of ions having the same m/z value exit, these ions form a single peak in the first time-of-flight spectrum, while these ions appear as separate peaks in the second time-of-flight spectrum even though they have the same m/z value. This is because, in the second mass analysis, the ions collide with the gas and have different times of flight depending on their difference in size. A spectrum comparator (14) judges a change in the position or shape of the peak by comparing the two spectra, and outputs information relating to the difference in the size of the ions (the molecular structure, charge state, or molecular class of the ions), and the like. Accordingly, a wider variety of information than ever before can be provided.
摘要:
Disclosed is a mass spectrometry apparatus and method capable of providing enhanced analysis sensitivity in a mass spectrometric analysis for a small amount of ions. A quadrupole rod-type ion guide is employed to temporarily accumulate ions to be introduced into an ion trap, and ions are introduced into the ion guide in an amount less than a saturated ion amount in the ion guide, and accumulated in an exit end of the ion guide. As compared with an octopole rod-type ion guide, the quadrupole rod-type ion guide has a higher ion-converging capability, and therefore can confine and hold a small amount of ions around an ion optical axis, although it is inferior in ion-accumulating capability. This makes it possible to efficiently introduce the ions into the ion trap through two openings of an electric field-correcting electrode and an entrance endcap electrode, so as to perform a high-sensitive analysis.
摘要:
In an ion detector, power supplies (21 through 23) generating independently controllable voltages are provided to respectively apply voltages to first to fifth dynodes (11 through 15), a final dynode (16), and an anode (17) in a secondary electron multiplier (10). Furthermore, the signal from the anode (17) is extracted, and the signal from the fifth dynode (15), which has a low electron multiplication rate, is extracted. These two signals are concurrently converted into digital values, taken in by a data processing unit (34), and stored in a data storage unit (35). When a mass spectrum is created in the data processing unit (34), the two detected data for the same time are read out and the presence or absence of signal saturation or waveform deformation is determined from the values of one of the detection data. If there is a high probability of signal saturation, the detection data based on the signals in the intermediate stages are selected, and the level of the selected data is corrected. The application of independent voltages to the secondary electron multiplier (10) makes the signal saturation less likely to occur. Even if saturation temporarily occurs, an unsaturated signal can be reflected in the mass spectrum.
摘要:
In an ion detector, power supplies (21 through 23) generating independently controllable voltages are provided to respectively apply voltages to first to fifth dynodes (11 through 15), a final dynode (16), and an anode (17) in a secondary electron multiplier (10). Furthermore, the signal from the anode (17) is extracted, and the signal from the fifth dynode (15), which has a low electron multiplication rate, is extracted. These two signals are concurrently converted into digital values, taken in by a data processing unit (34), and stored in a data storage unit (35). When a mass spectrum is created in the data processing unit (34), the two detected data for the same time are read out and the presence or absence of signal saturation or waveform deformation is determined from the values of one of the detection data. If there is a high probability of signal saturation, the detection data based on the signals in the intermediate stages are selected, and the level of the selected data is corrected. The application of independent voltages to the secondary electron multiplier (10) makes the signal saturation less likely to occur. Even if saturation temporarily occurs, an unsaturated signal can be reflected in the mass spectrum.
摘要:
The main voltage generator (5) applies a rectangular-wave radio-frequency voltage to the ring electrode (21) in order to capture ions inside the ion trap (2). In the case where the TOFMS (3) is operated in the reflectron mode, the radio-frequency voltage is changed into a constant voltage value when the phase thereof is 1.5π, and a voltage for expelling ions is applied to the end cap electrodes (22, 23) to expel the ions from the exit aperture (25) and introduce them into the TOFMS (3). In this case, since the velocity spread of the ions inside the ion trap (2) is small and so is the spatial spread thereof, a high mass resolution and accuracy can be achieved while assuring a high detection sensitivity. In the case where the TOFMS (3) is operated in the linear mode, the radio-frequency voltage is changed into a constant voltage value when the phase thereof is 0.5π, and then the ions are expelled. In this case, a high mass resolution and mass accuracy can be achieved since the variation of the ions' acceleration, which cannot be converged in the linear mode, can be suppressed.
摘要:
The main voltage generator (5) applies a rectangular-wave radio-frequency voltage to the ring electrode (21) in order to capture ions inside the ion trap (2). In the case where the TOFMS (3) is operated in the reflectron mode, the radio-frequency voltage is changed into a constant voltage value when the phase thereof is 1.5π, and a voltage for expelling ions is applied to the end cap electrodes (22, 23) to expel the ions from the exit aperture (25) and introduce them into the TOFMS (3). In this case, since the velocity spread of the ions inside the ion trap (2) is small and so is the spatial spread thereof, a high mass resolution and accuracy can be achieved while assuring a high detection sensitivity. In the case where the TOFMS (3) is operated in the linear mode, the radio-frequency voltage is changed into a constant voltage value when the phase thereof is 0.5π, and then the ions are expelled. In this case, a high mass resolution and mass accuracy can be achieved since the variation of the ions' acceleration, which cannot be converged in the linear mode, can be suppressed.
摘要:
A loading apparatus for card type recording mediums comprises a first loading section for receiving a first IC card and a second loading section for receiving a second IC card, the first loading section and the second loading section being arranged in parallel with each other at the side of the top surface of the apparatus, along with a third loading section for receiving a third IC card arranged at the side of the bottom surface of the apparatus. The apparatus main body is connected to a host apparatus such as a personal computer by way of a cable. The first and second loading sections are provided with respective bulged sections showing plan views similar to those of the IC cards to be received therein so that the user can identify the loading sections simply by touching them.
摘要:
A Schottky barrier type compound semiconductor device includes an N type compound semiconductor substrate, an insulation layer having a penetrating hole through which part of the substrate is exposed, and a layer of high melting metal formed through the penetrating hole to form a Schottky barrier with the substrate. The insulation layer includes a phosphosilicate glass layer containing phosphorus at a concentration of 1.times.10.sup.21 /cm.sup.3 or more and contacting the substrate.
摘要翻译:肖特基势垒型化合物半导体器件包括N型化合物半导体衬底,具有暴露基板的一部分的贯通孔的绝缘层和通过贯通孔形成的形成肖特基势垒的高熔点金属层, 基质。 绝缘层包括含有浓度为1×10 21 / cm 3以上的磷并与基板接触的磷硅酸盐玻璃层。