Accelerator mass spectrometry device for simultaneously measuring isotopes

Abstract

The present invention provides an accelerator mass spectrometry device for simultaneously measuring isotopes. In one embodiment, the device comprises a sputtering negative ion source for generating negative ions; the sputtering negative ion source being connected to an accelerating tube for simultaneously accelerating a plurality of isotopic ions; an output end of the accelerating tube being connected to an isotope mass resolution system; the isotope mass resolution system being connected to a charge conversion analysis and multi-receiving measurement system; the charge conversion analysis and multi-receiving measurement system being connected to an ion detection system. The present invention is capable of accelerating a plurality of isotopic negative ions simultaneously. The accelerated isotopic negative ions are separated. Stable isotopic negative ions are measured by a stable isotope receiver. Unstable isotope negative ions are converted to positive ions and then measured by a detector.

Claims

1. An accelerator mass spectrometry device for simultaneously measuring isotopes originated at the same time from a source, comprising a sputtering negative ion source for generating negative ions, said sputtering negative ion source is connected to an accelerating tube which is used for simultaneously accelerating a plurality of isotopic ions, said accelerating tube comprises an output end that is connected to an isotope mass resolution system, said isotope mass resolution system is connected to a charge conversion analysis and multi-receiving measurement system, said charge conversion analysis and multi-receiving measurement system is connected to an ion detection system, wherein there is no other accelerating tube besides said accelerating tube, and all negative ions generated from said negative ion source are simultaneously accelerated in said accelerating tube, wherein the isotope mass resolution system comprises a first electrostatic analyzer connected to a magnetic analyzer, said first electrostatic analyzer conducts energy analysis of a plurality of isotopic ions, and said magnetic analyzer separates the plurality of isotopic ions, wherein the charge conversion analysis and multi-receiving measurement system comprises an electron stripper, a speed selector, a second electrostatic analyzer and a stable isotope receiver, said stable isotope receiver measures stable isotopic negative ions, said electron stripper converts unstable isotopic negative ions to positive ions and disintegrates all molecular ions, said speed selector excludes disintegrated molecular fragments and scattered ions, and said second electrostatic analyzer excludes neutral particles of zero charge, wherein the ion detection system comprises a detector, a nuclear electronics and data acquisition unit, said detector measures isotopic positive ions originating from conversion by said electron stripper, said nuclear electronics and data acquisition unit obtains data from said stable isotope receiver and said detector respectively, and a control system is configured to use time matching to offer measurements of contents of a plurality of isotopes measured simultaneously and an isotope abundance ratio thereof.

2. The device of claim 1, wherein the stable isotope receiver is a Faraday cup.

3. The device of claim 1, wherein signal measured by the stable isotope receiver is delayed by a delay line and then transmitted to the nuclear electronics and data acquisition unit such that it arrives simultaneously with signal measured by the detector.

4. The device of claim 1, further comprising an automatic control system for controlling operation of isotope measurement, data acquisition and operation, sample replacement, vacuum environment and operation of the device.

Description

BRIEF DESCRIPTION OF THE DRAWINGS

(1) FIG. 1 shows a schematic diagram of a conventional AMS.

(2) FIG. 2 shows a schematic diagram of a ST-AMS according to the present invention.

(3) FIG. 3 shows a structural schematic diagram of a ST-AMS in accordance with an embodiment of the present invention that measures carbon isotopes simultaneously.

DETAILED DESCRIPTION OF THE INVENTION

(4) Below is a detailed description of the present invention in connection with the accompanying drawings and the preferred embodiments.

(5) FIG. 1 is a schematic diagram of a conventional AMS. As shown in FIG. 1, two isotopes respectively having a mass number of M and M1 are separated from a sputtering negative ion source 1. AMS is unable to measure the two isotopes simultaneously at rear end of a high-energy magnetic analyzer or electrostatic analyzer; instead, an electrostatic and magnetic analyzer 2 can only select one of the isotopes to be accelerated by a tandem accelerator 3. The accelerated isotope passes through a high-energy magnetic analyzer 4 and a high-energy electrostatic analyzer 5 and arrives at a detector 6. By varying the mass parameter of the injector alternately so as to inject and accelerate the isotopes alternately, the isotopes can be measured alternately.

(6) The accelerator mass spectrometry device of the present invention that has the function of measuring isotopes at the same time is referred to as ST-AMS. ST-AMS mainly serves to solve two technical problems, one of which is accelerating isotopes simultaneously and the other is measuring the isotopes simultaneously.

(7) FIG. 2 is a schematic diagram of the ST-AMS according to the present invention. As shown in FIG. 2, negative ions originating from the sputtering negative ion source 1 are directly admitted into an accelerating tube 7 (comprising a pre-accelerating tube and a main accelerating tube) and, therefore, the individual isotopic negative ions contained in the negative ions, for example, in the case of carbon isotopes, respectively .sup.12C, .sup.13C and .sup.14C negative ions, are all admitted into the accelerator tube to be accelerated. After the negative ions pass through the accelerator, their masses are resolved directly using an electric and magnetic analyzer 8. For example, when carbon isotopes are analyzed using this analyzer, .sup.12C, .sup.13C and .sup.14C negative ions among carbon isotopes are separated. .sup.12C and .sup.13C are stable isotopes and can form negative ion beams capable of being measured directly, .sup.12C and .sup.13C negative ions are hence capable of being measured simultaneously using a stable isotope receiver 9 (such as a Faraday cup). In contrast, unstable isotopes, for example, .sup.14C negative ions, are extremely low in abundance (.sup.14C/.sup.12C in the range of 10.sup.12 to 10.sup.16) so that they cannot form a measurable beam with a maximum of 300 counts per second. Thus, on one hand, a heavy-particle detector is used to record the number of atoms of .sup.14C ions and the stable isotope receiver 9 cannot be used. On the other hand, as other isotopic molecular ions, such as .sup.13CH, .sup.12CH.sub.2 and .sup.7Li.sub.2 negative ions, are present in .sup.14C negative ions, all the molecular ions are disintegrated through an electron stripper 10 by means of a stripper technique in the AMS analysis method and the disintegrated molecular fragments and scattered ions are excluded through a speed selector 11 and an electrostatic analyzer 12, simply allowing .sup.14C.sup.+ ions to enter a heavy ion detector 13 and to be recorded. The speed selector 11 is mainly used to exclude the disintegrated molecular fragments and scattered ions and the electrostatic analyzer 12 is mainly used to exclude neutral particles of zero charge state. Since the point of time when .sup.14C.sup.+ ion arrives at the detector is later than the point of time when .sup.12C and .sup.13C ion beam streams arrive at the stable isotope receiver 9, the present invention employs a dedicated delay line to delay the signals of the stable isotope receiver such that the signals arrive at the receiver simultaneously with the signals of the detector. In this way, .sup.14C.sup.+ ions, .sup.12C and .sup.13C negative ions can be measured simultaneously thereby enabling more isotopes to be received simultaneously.

(8) Below is a description of an embodiment of the present invention with reference to a specific structure of the ST-AMS by taking the analysis on .sup.12C, .sup.13C and .sup.14C for example.

(9) FIG. 3 is a specific structure of the ST-AMS of the present invention, which comprises five parts, respectively:

(10) Negative ion generation and acceleration system, comprising a sputtering negative ion source 1 and an accelerating tube 7;

(11) Isotope mass resolution system, comprising a first electrostatic analyzer 14 and a magnetic analyzer 15;

(12) Charge conversion analysis and multi-receiving measurement system, comprising an electron stripper 10, a speed selector 11, a second electrostatic analyzer 12 and a stable isotope receiver 9;

(13) Ion detection system, comprising a detector 13 and a nuclear electronics and data acquisition system; and

(14) Automatic control system, serving for the control of the above systems, real-time measurement of isotopes, data acquisition and operation, sample replacement as well as automatic control of the vacuum environment.

(15) The sputtering negative ion source 1 is connected to the accelerating tube 7 for simultaneously accelerating a plurality of isotopic ions. The accelerating tube 7 consists of a pre-accelerating section and a main accelerating section and a lens is disposed in the middle thereof, and the output end of the accelerating tube 7 is connected with an isotopic mass resolution system. The first electrostatic analyzer 14 of the isotope mass resolution system conducts energy analysis of a plurality of isotopic ions. The magnetic analyzer 15 separates a plurality of isotopic ions. The stable isotope receiver 9 of the charge conversion analysis and multi-receiving measurement system measures stable isotopic negative ions (such as .sup.12C beam stream a, .sup.13C beam stream b); the electron stripper 10 converts unstable isotope negative ion (such as .sup.14C) into a positive ion and disintegrates all molecular ions. The detector 13 of the ion detection system measures isotopic positive ions (such as .sup.14C beam stream c) converted by the electron stripper 10. The nuclear electronics and data acquisition unit acquires the data measured by the stable isotope receiver 9 and the detector 13 which, after time matching, offers the contents of multiple isotopes measured simultaneously and abundance ratio thereof. In the present invention, the measurement signals of the stable isotope receiver 9 (a Faraday cup) are delayed by a delay line before transmitted to the nuclear electronics and data acquisition unit such that these signals arrive at the receiver simultaneously with the measurement signals of the detector 13.

(16) Below is a description of the measurement steps of the ST-AMS by taking the measurement of carbon isotopes .sup.12C, .sup.13C and .sup.14C contained in atmospheric particulates for example.

(17) Step 1: prepare the sample of atmospheric particulates into graphite;

(18) Step 2: press the prepared graphite sample into a sample target cone which is placed in a Cs ion source;

(19) Step 3: bombard the target material with a Cs ion beam to extract C.sup. which is then admitted into the pre-accelerating tube and the main accelerating tube to accelerate the ion to the predetermined energy;

(20) Step 4: C.sup. is then admitted into the first electrostatic analyzer for energy selection, and .sup.14C, .sup.12C and .sup.13C are then separated by the magnetic analyzer;

(21) Step 5: .sup.12C and .sup.13C are measured by the Faraday cup. .sup.14C is converted to positive ions through the gas stripper while molecules are disintegrated; the resulting .sup.14C is then subject to magnetic field and electric field analysis by a speed selector and a second electrostatic analyzer and the count of .sup.14C ions is ultimately obtained by the detector system.

(22) Step 6: after time matching, .sup.14C, .sup.12C and .sup.13C as well as the abundance ratio thereof are obtained by the data acquisition system;

(23) Step 7: by comparing the above results with the measurement results obtained from the standard sample, the accurate content of .sup.14C can be obtained.

(24) In addition to being useful for the measurement of carbon .sup.12C, .sup.13C and .sup.14C isotopes, the present invention is also applicable to simultaneous measurement of nuclides such as .sup.3H, .sup.10Be, .sup.26Al and their isotopes in a way similar to that described in the above embodiment and those of ordinary skill in the art may tailor the design to the specific situations.

(25) The above disclosure is related to the detailed technical contents and inventive features thereof. A person having ordinary skill in the art may proceed with a variety of modifications and replacements based on the disclosures and suggestions of the invention as described without departing from the idea and scope thereof. Nevertheless, although such modifications and replacements are not fully disclosed in the above descriptions, they have substantially been covered in the following claims as appended.