AU2020100872A4 - An Ar-Ar Dating Method Without Standards For Minerals - Google Patents

An Ar-Ar Dating Method Without Standards For Minerals Download PDF

Info

Publication number
AU2020100872A4
AU2020100872A4 AU2020100872A AU2020100872A AU2020100872A4 AU 2020100872 A4 AU2020100872 A4 AU 2020100872A4 AU 2020100872 A AU2020100872 A AU 2020100872A AU 2020100872 A AU2020100872 A AU 2020100872A AU 2020100872 A4 AU2020100872 A4 AU 2020100872A4
Authority
AU
Australia
Prior art keywords
sample
neutron
accelerator
standards
mineral
Prior art date
Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
Ceased
Application number
AU2020100872A
Inventor
Huaiyu HE
Youjuan LI
Ziheng LIU
Fei Su
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
Institute of Geology and Geophysics of CAS
Original Assignee
Institute of Geology and Geophysics of CAS
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Application filed by Institute of Geology and Geophysics of CAS filed Critical Institute of Geology and Geophysics of CAS
Priority to AU2020100872A priority Critical patent/AU2020100872A4/en
Application granted granted Critical
Publication of AU2020100872A4 publication Critical patent/AU2020100872A4/en
Ceased legal-status Critical Current
Anticipated expiration legal-status Critical

Links

Classifications

    • GPHYSICS
    • G01MEASURING; TESTING
    • G01NINVESTIGATING OR ANALYSING MATERIALS BY DETERMINING THEIR CHEMICAL OR PHYSICAL PROPERTIES
    • G01N23/00Investigating or analysing materials by the use of wave or particle radiation, e.g. X-rays or neutrons, not covered by groups G01N3/00 – G01N17/00, G01N21/00 or G01N22/00
    • G01N23/22Investigating or analysing materials by the use of wave or particle radiation, e.g. X-rays or neutrons, not covered by groups G01N3/00 – G01N17/00, G01N21/00 or G01N22/00 by measuring secondary emission from the material
    • G01N23/221Investigating or analysing materials by the use of wave or particle radiation, e.g. X-rays or neutrons, not covered by groups G01N3/00 – G01N17/00, G01N21/00 or G01N22/00 by measuring secondary emission from the material by activation analysis
    • G01N23/222Investigating or analysing materials by the use of wave or particle radiation, e.g. X-rays or neutrons, not covered by groups G01N3/00 – G01N17/00, G01N21/00 or G01N22/00 by measuring secondary emission from the material by activation analysis using neutron activation analysis [NAA]
    • GPHYSICS
    • G01MEASURING; TESTING
    • G01NINVESTIGATING OR ANALYSING MATERIALS BY DETERMINING THEIR CHEMICAL OR PHYSICAL PROPERTIES
    • G01N23/00Investigating or analysing materials by the use of wave or particle radiation, e.g. X-rays or neutrons, not covered by groups G01N3/00 – G01N17/00, G01N21/00 or G01N22/00
    • G01N23/02Investigating or analysing materials by the use of wave or particle radiation, e.g. X-rays or neutrons, not covered by groups G01N3/00 – G01N17/00, G01N21/00 or G01N22/00 by transmitting the radiation through the material
    • G01N23/06Investigating or analysing materials by the use of wave or particle radiation, e.g. X-rays or neutrons, not covered by groups G01N3/00 – G01N17/00, G01N21/00 or G01N22/00 by transmitting the radiation through the material and measuring the absorption
    • G01N23/09Investigating or analysing materials by the use of wave or particle radiation, e.g. X-rays or neutrons, not covered by groups G01N3/00 – G01N17/00, G01N21/00 or G01N22/00 by transmitting the radiation through the material and measuring the absorption the radiation being neutrons
    • GPHYSICS
    • G01MEASURING; TESTING
    • G01NINVESTIGATING OR ANALYSING MATERIALS BY DETERMINING THEIR CHEMICAL OR PHYSICAL PROPERTIES
    • G01N30/00Investigating or analysing materials by separation into components using adsorption, absorption or similar phenomena or using ion-exchange, e.g. chromatography or field flow fractionation
    • G01N30/02Column chromatography
    • G01N30/62Detectors specially adapted therefor
    • G01N30/72Mass spectrometers
    • G01N30/7206Mass spectrometers interfaced to gas chromatograph
    • GPHYSICS
    • G01MEASURING; TESTING
    • G01NINVESTIGATING OR ANALYSING MATERIALS BY DETERMINING THEIR CHEMICAL OR PHYSICAL PROPERTIES
    • G01N33/00Investigating or analysing materials by specific methods not covered by groups G01N1/00 - G01N31/00
    • G01N33/24Earth materials

Landscapes

  • Life Sciences & Earth Sciences (AREA)
  • Health & Medical Sciences (AREA)
  • Chemical & Material Sciences (AREA)
  • Analytical Chemistry (AREA)
  • Pathology (AREA)
  • Immunology (AREA)
  • General Physics & Mathematics (AREA)
  • General Health & Medical Sciences (AREA)
  • Biochemistry (AREA)
  • Physics & Mathematics (AREA)
  • Engineering & Computer Science (AREA)
  • Geology (AREA)
  • Medicinal Chemistry (AREA)
  • Food Science & Technology (AREA)
  • Remote Sensing (AREA)
  • General Life Sciences & Earth Sciences (AREA)
  • Environmental & Geological Engineering (AREA)
  • Toxicology (AREA)
  • Analysing Materials By The Use Of Radiation (AREA)

Abstract

This invention discloses an Ar-Ar dating method without standards for minerals, which includes: wrap the mineral sample with aluminum foil into a sample piece, attach a high-purity nickel sheet on the front and back of the sample piece respectively, and then put it into the accelerator neutron source for neutron irradiation; detect the irradiated nickel sheet to determine the value of the neutron reaction cross section a, and calculate the neutron flux N of the accelerator neutron source; load the irradiated mineral sample into the noble gas measurement system, melt sample, and measure the Ar isotope content of the mineral sample with the noble gas mass spectrometer, and obtain the required 40Ar*/ 39ArKby calculating the data; substitute the neutron flux N, reaction cross section and 40Ar*/ 39Ar of the accelerator neutron source into the formula t 1( A 4 0Ar* N-a t n 1 + A ArK to calculate the Ar-Ar age of the mineral sample. This invention solves the problem that the standard sample with known age must be used in the traditional Ar-Ar dating to correct the J-value related to the neutron flux of 2 3 U fission reactor, realizes the Ar-Ar dating without any geological standard sample, and improves the precision of the Ar-Ar dating method. Descriptions with Drawings Wrap the mineral sample with aluminum foil into a sample piece, attach a high-purity j nickel sheet on the front and back of the sample piece respectively, and then put it into the acceleratorneutron source forneutron irradiation Detect the irradiated nickel sheet, determine the value of the neutron reaction section u, and calculate the neutron flux N of the accelerator neutron source Load the irradiated mineral sample into the noble gas measurement system, melt sample, measure the Ar isotope (Ar, 39Ar, 34 Ar) content of the mineral sample with the noble gas mass spectrometer, and obtain the required 4Ar*/3#ArK by calculating the data Substitute the neutron flux N, reaction cross section a and 4Ar*/39Ar of the 4 accelerator neutron source into the formula to calculate the Ar-Ar age of the mineral sample Figure 1 1/1

Description

Descriptions with Drawings
Wrap the mineral sample with aluminum foil into a sample piece, attach a high-purity j nickel sheet on the front and back of the sample piece respectively, and then put it into the acceleratorneutron source forneutron irradiation
Detect the irradiated nickel sheet, determine the value of the neutron reaction section u, and calculate the neutron flux N of the accelerator neutron source
Load the irradiated mineral sample into the noble gas measurement system, melt sample, measure the Ar isotope (Ar, 39Ar, 34 Ar) content of the mineral sample with the noble gas mass spectrometer, and obtain the required 4Ar*/3#ArK by calculating the data
Substitute the neutron flux N, reaction cross section a and 4Ar*/39Ar of the 4 accelerator neutron source into the formula to calculate the Ar-Ar age of the mineral sample
Figure 1
1/1
Descriptions
An Ar-Ar dating method without standards for minerals
Technical Field This invention relates to the technical field of Ar-Ar dating, in particular to an Ar-Ar dating method without standards for minerals.
Background Technology The basic principle of Ar-Ar dating is as follows: According to the law of radioactive decay, as long as the content of radioactive parent and radiogenic daughter is measured, the mineral age can be calculated according to the following Formula 1:
1 A Ar t-- 1 + Formula1
Where t is mineral age, X is the total decay constant of4 0 K,X=5.543(±0.010)x10 10 a-1
, ,eand 2'eare the decay constants of the two branches of 4'K decaying into 40Ar respectively, 2e =0.572( ± 0.004) x 10 a-1 , l'e=0.0088( ±0.0017) x 10-10 a-1, 4 0K is the content of radioactive parent, 4 0Ar* is the content of radiogenic daughter.
The following formula can be obtained by deforming Formula 1:
*OAr* = K l[(exp t) - 1] Formula 2
According to 39 39 K (n,p) Ar in the nuclear reaction,
9ArK = 9KA f0(E)o-(E)dE Formula 3
Where 3 9Ar is the 39 Ar generated by neutron irradiated 39K, A refers to the irradiation
time, 0(E) refers to the neutron flux with energy of E, and o(Erefers to the neutron
reaction cross section with energy of E.
According to the above formulas, set
J= ,Af O(E)u(E)dE Formula 4 : TnK
Then: t- +1 ) Formula 5
Formula 5 is the basic equation of Ar-Ar dating. According to Formula 5, only J-value and Ar*/ 3 Arof 4 9 the sample are needed to determine its Ar-Ar age.
Based on Formula 5, the existing Ar-Ar dating method is to place the mineral sample to be measured at a distance with the standard sample, seal them in a quartz tube and put the tube into the 2 5 U fission reactor for neutron irradiation to convert 39K into 39Ar.
From Formula 5, we get
(exp At)-1 - 40 40 ' Ar /1 ArK Formula 6
Correct the irradiation parameter J-value of4 0 Ar*/ 39Arof the standard sample with known age, measure the 4 0Ar*/ 3 9 ArKof the sample to be measured respectively, and calculate the Ar-Ar age of the sample to be measured in combination with the J-value corrected by the standard sample according to Formula 5.
It can be seen from the above description that the standard sample with known age must be measured by existing Ar-Ar dating method to correct the J-value of the sample to be measured. However, due to the change of fuel cycle and sample position as well as the large number of unknown parameters, it is difficult to get the accurate J-value, resulting in a large J-value gradient. Even if the J-value of the position of the standard sample is accurately measured, the J-value of the position of the sample to be measured calculated by fitting the J-value of the position of the standard sample will also introduce a large error, thus affecting the dating accuracy.
Invention Summary (I) Technical problems to be solved
In view of this, the main purpose of this invention is to provide an Ar-Ar dating method without standards for minerals to solve the J-value problem related to the neutron flux of 235U fission reactor which must be corrected by the standard sample with known age by traditional Ar-Ar dating, so as to accomplish the purpose of Ar-Ar dating without using any geological standard sample, and improve the precision of Ar-Ar dating.
(II) Technical proposal
In order to achieve the above purpose, this invention provides an Ar-Ar dating method without standards for minerals, which includes:
Step 1: wrap the mineral sample with aluminum foil into a sample piece, attach a high-purity nickel sheet on the front and back of the sample piece respectively, and then put it into the accelerator neutron source for neutron irradiation;
Step 2: detect the irradiated nickel sheet, determine the value of the neutron reaction cross section a, and calculate the neutron flux N of the accelerator neutron source;
Step 3: load the irradiated mineral sample into the noble gas measurement system, melt sample, measure the Ar isotope ( 4 0Ar , 3 9Ar 36Ar) content of the mineral sample with the noble gas mass spectrometer, and obtain the required 40Ar*/ 3 9 ArKby calculating the data;
40 Step 4: substitute the neutron flux N, reaction cross section a and Ar*/ 3 9 ArK of the
1 X 40Ar* N-a i accelerator neutron source into the formula t = -In 1 + -A . x to
calculate the Ar-Ar age of the mineral sample.
Where t is the Ar-Ar age of the mineral sample, k is the total decay constant of 40K, k=5.543(±0.010)xO-1 a- 0 1 , Xe and 'eare the decay constants of the two branches of 4 0K decaying into 40Ar respectively, Xe =0.572(±0.004)x10-1o a-', 'e=.0088(±0.0017)X10-10 a- 1, 40Ar*/ 39ArKis the ratio of radiogenic 40Ar to 39 ArtK produced by neutron irradiated 3 9K, N is the neutron flux of accelerator neutron source, a is the reaction cross section, which is the integral function of neutron energy spectrum.
In the above proposal, the described Step 1 includes: take the mineral sample, wrap the mineral sample into a lcmxlcm sample pieces with aluminum foil, attach a 1mm thick high-purity nickel sheet on the front and back of the sample piece respectively, and then put it into the accelerator neutron source as close as possible to the bull's eye for neutron irradiation, in which the accelerator neutron source is as close as possible to the bull's eye and is less than 3.5cm away from the bull's eye.
In the above proposal, the described high-purity nickel sheet is a nickel sheet with a mass percentage>99.99%.
In the above proposal, the nuclear data of the neutron generator is measured by the detected and irradiated nickel sheet described in Step 2 by ultra-low background HPGe y spectrometer.
In the above proposal, since the neutron energy of the accelerator neutron source is 2.45 MeV, the determined value of the reaction cross section a of the mineral sample in the described Step 2 is 0.18 barn (b), where 1b=10-24cm 2 .
In the above proposal, the calculation of the neutron flux N of the accelerator neutron source in the described Step 2 is a calculation of the neutron flux based on the nuclear 58 reactionsNi (n, p) Co.
In the above proposal, the noble gas measurement system loading irradiated mineral sample as described in Step 3 includes a high temperature furnace, a gas purification system and a Helix MC Plus noble gas mass spectrometer, in which the sample is melted in the high temperature furnace, the released gas by melting is purified by the gas purification system to remove the active gases, and then the Ar isotope is measured by the Helix MC Plus noble gas mass spectrometer.
In the above proposal, the determination of Ar isotope content of the mineral sample by noble gas mass spectrometer described in Step 3 is the determination of Ar isotopes 4(0 Ar, 39Ar and 3 6Ar) by Helix MC Plus noble gas mass spectrometer.
In the above proposal, all 3 9Ar in the required 40Ar*/ 39ArK obtained by data calculation described in Step 3 are generated by 39K irradiated by neutron. Therefore, 39ArK is the determined 3 9Ar, 4 OAr*= 4OAr 4 Ara, in which 4 Ara is air40 Ar, 4 0Ara=295.5x3 6 Ar.
(III) Beneficial effects
It can be seen from the above technical proposal that this invention has the following beneficial effects:
The Ar-Ar dating method without standards for minerals provided by this invention requires only measuring the neutron flux and 40Ar*/ 39ArK instead of correcting with the standard sample with known age, the J-value determined by the neutron flux, reaction cross section and other parameters at the position where the sample to be measured with known age is located, so it avoids the influence of the J-value gradient caused by the sample position and other reasons, solves the problem that the standard sample with known age must be used in the traditional Ar-Ar dating to correct the J-value related to the neutron flux of 2 3 5 U fission reactor, and achieves the goal of Ar-Ar dating without using any geological standard sample. This method will make Ar-Ar dating changing from "relative dating" (the sample age is obtained by comparing with the standard sample age) to "absolute dating" (no standards are required).
The Ar-Ar dating method without standards for minerals provided by this invention requires only measuring the neutron flux and 40Ar*/ 39ArK instead of correcting, with the standard sample with known age, the J-value determined by the neutron flux, reaction cross section and other parameters at the position where the sample to be measured with known age is located, so it avoids the influence of the J-value gradient caused by the sample position and other reasons, thus improves the precision of Ar-Ar dating method.
Description with Drawings Figure 1 is a flow chart of the Ar-Ar dating method without standards for minerals according to an embodiment of this invention.
Detailed Description of the Presently Preferred Embodiment
In order to make the purpose, technical proposal and advantages of this invention clearer, this invention will be further detailed with reference to the specific embodiment and the attached figures.
In order to be able to accurately calculate the neutron flux, the embodiment of this invention is to attach a high-purity (mass percentage > 99.99%) nickel sheet with the same size as the sample on the front and back of the mineral sample to be measured, in which the thickness of the nickel sheet is about 1mm, so as to accurately calculate the neutron flux and eliminate the effect of the neutron flux gradient, thus improving the dating precision.
In the embodiment of this invention, the deuterium-deuterium (D-D) accelerator neutron source which only generates 2.45MeV single energy neutrons is used to irradiate the mineral sample, then the neutrons hit the mineral sample to convert 3 9K into 39Ar, which meets the following formula, "9Ark '-= Formula 7
The reaction cross section c is the ratio of the number of reaction generated nuclei per unit time per unit area (e.g. 39Ar) to the number of neutrons of the incident particle and the number of target nuclei (e.g. 3 9K), and the unit is barn (b, lb=10-2 4cm 2).
According to Formula 7,
40K = 1.255 x 10-4 X "ArK Formula 8 N-a
Where 1.255x10-4 is the 40 K/ 39K value in nature, N is the neutron flux, a is the reaction cross section, and is the integral function of the neutron energy spectrum.
According to Formula 1, Formula 7 and Formula 8, 40 A Ar* N-a t In 1 + Formula 9 X0+, ArK 1.255xlt0 4 /
Where t is the Ar-Ar age of the mineral sample, ) is the total decay constant of 4K, ?,=5.543(±0.010)x0-1 a- 0 1, le and 'eare the decay constants of the two branches of 4 0K 40 decaying into Ar respectively, le =0.572(±0.004)x10-10 1a- , 'e=0.0088(±0.0017)X10-10 a- 1, 40Ar*/ 3 9 ArK is the ratio of radiogenic 4 0Ar to 39 ArK produced by neutron irradiation on 39K, N is the neutron flux of accelerator neutron source, a is the reaction cross section, which is the integral function of neutron energy spectrum.
Therefore, to accurately determine the sample age, only 40Ar*/ 39ArK, N and a need to be determined.
In order to accurately measure the neutron flux N and reaction cross section a , the embodiment of this invention adopts the neutron nuclear reaction ( 8Ni (n, p)5 8 Co) of nickel closest to the nuclear reaction 39 K(n,p) 39Ar to detect. Since the adopted accelerator neutron source generates single energy neutron and the reaction cross section is constant, the 39K content and sample age can be calculated with reference to the precise neutron flux and 39Ar content recorded by the nickel sheet, and the Ar-Ar dating without standards can be realized.
Based on the above analysis, Figure 1 shows the flow chart of the Ar-Ar dating method without standards for minerals in accordance with the embodiment of this invention, which includes:
Step 1: wrap the mineral sample with aluminum foil into a sample piece, attach a high-purity (>99.99%) nickel sheet on the front and back of the sample piece respectively, and then put it into the accelerator neutron source for neutron irradiation;
Step 2: detect the irradiated nickel sheet to determine the value of the neutron reaction cross section y, and calculate the neutron flux N of the accelerator neutron source;
Step 3: load the irradiated mineral sample into the noble gas measurement system, melt sample, measure the Ar isotope ( 4 0Ar, 39 Ar, 36Ar) content of the mineral sample with the noble gas mass spectrometer, and obtain the required 40Ar*/ 39 ArKby calculating the data;
0 3 9 Step 4: substitute the neutron flux N, reaction cross section a and 4Ar*/ ArK of the
1 A 40Ar* N-c accelerator neutron source into the formula t In (1 + -Arx .2x _to
calculate the Ar-Ar age of the mineral sample;
Where t is the Ar-Ar age of the mineral sample, , is the total decay constant of 40K, X=5.543(±0.0l0)x10-1 0a- 1, le and X'e are the decay constants of the two branches of 4 0K decaying into 40Ar respectively, ke =0.572(±0.004)x10-1 a-1 , ;'e=0.0088(±0.007)x10-10 a- 1, 4 0Ar*/ 3 9 ArKis the ratio of radiogenic 40 Arto 39ArK produced by neutron irradiated 39K, N is the neutron flux of accelerator neutron source, a is the reaction cross section, which is the integral function of neutron energy spectrum.
In which Step 1 includes: take the mineral sample, wrap the mineral sample into a lcmx 1cm sample pieces with aluminum foil, attach a 1mm thick high-purity nickel sheet on the front and back of the sample piece respectively, and then put it into the accelerator neutron source as close as possible to the bull's eye for neutron irradiation, in which the accelerator neutron source is as close as possible to the bull's eye and is less than 3.5cm away from the bull's eye.
The nuclear data of the neutron generator is measured by the detected and irradiated nickel sheet described in Step 2 by ultra-low background HPGe y spectrometer. The nuclear data mainly refers to the 5 8 Co generated by the nickel sheet after neutron irradiation by the neutron source.
Since the neutron energy of the accelerator neutron source is single and 2.45 MeV, the determined value of the reaction cross section a of the neutron in the described Step 2 is 0.18 barn (b), where 1b=10-2 4cm 2
. In the above proposal, the calculation of the neutron flux N of the accelerator neutron source in the described Step 2 is a calculation of the neutron flux based on the nuclear reaction 5 8Ni (n, p) 58 Co.The specific calculation process is as follows:
According to the nuclear reaction 5 8Ni 58 (n, p) Co, (Y= $Zo Formula 10
Where a is the reaction cross section, N is the neutron flux of the accelerator neutron source, 5 8Co is the number of 58 Co atoms measured by HPGe y spectrometer, and 58Ni is the number of 58Ni atoms of high-purity nickel sheet. Because the neutron energy of reaction cross section a is a single constant, the number of 58 Co atoms can be measured by the y spectrometer, the number of 5 8Ni atoms can be calculated by the mass, purity and molar mass of the high-purity nickel sheet. The neutron flux N of accelerator neutron source can be calculated by substituting the above values into Formula 10.
The noble gas measurement system loading irradiated mineral sample as described in Step 3 includes a high temperature furnace, a gas purification system and a Helix MC Plus noble gas mass spectrometer. The specific measurement process for measuring the Ar isotope content of the mineral sample by the noble gas mass spectrometer as described in Step 3 is as follows: melt the sample with a high temperature furnace, purify the released gas through the purification system, remove the active gases, etc., and then measure the Ar isotope by Helix MC Plus noble gas mass spectrometer, receive 4 0Ar, 39Ar and 36 Ar signals by the Faraday cup and the electron multiplier equipped on the noble gas mass spectrometer respectively, and measure the content of 4 0Ar, 39Ar and 3 6Ar.
All 3Ar in the required 40Ar*/ 3 9 ArKobtained by data calculation described in Step 3 are generated by 39K irradiated by neutron. Therefore, 39ArK is the determined 39Ar,
Ar*= 40 Ar-4OAra, in which 4 0Ara is air 4 0Ar, 4 0Ara=295.5X 36 Ar. Therefore, Ar*/ 39 ArK=(4 Ar-295.5*36Ar)/39Ar; the specific calculation is to substitute the measured
Ar, Ar and Ar into the above formula to get the 4 0Ar*/ 3 9ArK value. 39 36
The Ar-Ar dating method without standards for minerals provided by the embodiment of this invention requires only measuring the neutron flux and 40Ar*/ 3 9 ArK instead of correcting, with the standard sample with known age, the J-value determined by the neutron flux, reaction cross section and other parameters at the position where the sample to be measured with known age is located, so it avoids the influence of the J-value gradient caused by the sample position and other reasons, thus improves the precision of Ar-Ar dating method.
The specific embodiment described above further details the purpose, technical proposal and beneficial effect of this invention. It should be understood that the above is only a specific embodiment of this invention and is not used to limit this invention. Any modification, equivalent substitution, improvement, etc. made under the spirit and principle of this invention shall be included in the protection scope of this invention.

Claims (9)

Claims
1.An Ar-Ar dating method without standards for minerals, which is characterized in that the method includes:
Step 1: wrap the mineral sample with aluminum foil into a sample piece, attach a high-purity nickel sheet on the front and back of the sample piece respectively, and then put it into the accelerator neutron source for neutron irradiation;
Step 2: detect the irradiated nickel sheet to determine the value of the neutron reaction cross section a, and calculate the neutron flux N of the accelerator neutron source;
Step 3: load the irradiated mineral sample into the noble gas measurement system, melt sample, measure the Ar isotope (4 0Ar, 39 Ar, 36 Ar) content of the mineral sample with the noble gas mass spectrometer, and obtain the required 40Ar*/ 39 ArKby calculating the data;
Step 4: substitute the neutron flux N, reaction cross section a and 4 0Ar*/ 3 9 Arx of the 1 A Ar* Nu accelerator neutron source into the formula t In 9 + ±A+X' 3 ArK 1.255xio0-4
to calculate the Ar-Ar age of the mineral sample;
Where t is the Ar-Ar age of the mineral sample, X is the total decay constant of 40K, =5.543(±0.0l0)x10-10a-1, e and X'e are the decay constants of the two branches of 4 0K decaying into 40Ar respectively, Ae =0.572(±0.004)x10-1a-1, 'e=0.0088(±0.0017)X10-10 a- 1, 4 0Ar*/ 3 9 ArKis the ratio of radiogenic 4 0Ar to 39ArK produced by neutron irradiation on 39K, N is the neutron flux of accelerator neutron source, a is the reaction cross section, which is the integral function of neutron energy spectrum.
2.The Ar-Ar dating method without standards for minerals according to Claim 1, which is characterized in that the described Step 1 includes:
Take the mineral sample, wrap the mineral sample into a lcmx lcm sample pieces with aluminum foil, attach a 1mm thick high-purity nickel sheet on the front and back of the sample piece respectively, and then put it into the accelerator neutron source as close as possible to the bull's eye for neutron irradiation, in which the accelerator neutron source is as close as possible to the bull's eye and is less than 3.5cm away from the bull's eye.
3.The Ar-Ar dating method without standards for minerals according to Claim 1 or 2, which is characterized in that the described high-purity nickel sheet is a nickel sheet with a mass percentage>99.99%.
4.The Ar-Ar dating method without standards for minerals according to Claim 1, which is characterized in that the nuclear data of the neutron generator is measured by the detected and irradiated nickel sheet described in Step 2 by ultra-low background HPGe y spectrometer.
5.The Ar-Ar dating method without standards for minerals according to Claim 1, which is characterized in that since the neutron energy of the accelerator neutron source is 2.45 MeV, the determined value of the reaction cross section a of the mineral sample in the described Step 2 is 0.18 barn (b), where 1b=10-24 cm 2
. 6.The Ar-Ar dating method without standards for minerals according to Claim 1, which is characterized in that the calculation of the neutron flux N of the accelerator neutron source in the described Step 2 is a calculation of the neutron flux based on the nuclear reaction 5 8Ni (n, p) 58 Co.
7.The Ar-Ar dating method without standards for minerals according to Claim 1, which is characterized in that the noble gas measurement system loading irradiated mineral sample as described in Step 3 includes a high temperature furnace, a gas purification system and a Helix MC Plus noble gas mass spectrometer, in which the sample is melted in the high temperature furnace, the released gas by melting is purified by the gas purification system to remove the active gases, and then the Ar isotope is measured by the Helix MC Plus noble gas mass spectrometer.
8.The Ar-Ar dating method without standards for minerals according to Claim 1, which is characterized in that the determination of Ar isotope content of the mineral sample by noble gas mass spectrometer described in Step 3 is the determination of Ar isotopes 4(0 Ar, 39Ar and 36Ar) by Helix MC Plus noble gas mass spectrometer.
9. The Ar-Ar dating method without standards for minerals according to Claim 1, which is characterized in that all 39Ar in the required4 Ar*/ 39ArK obtained by data calculation described in Step 3 are generated by 39K irradiated by neutron. Therefore, 39ArK is the determined 9Ar, 4 OAr*=4 OAr- 4 Ara,in which 4 0Arais air4 0 Ar, 4 0 Ara=295.5x3 6 Ar.
Descriptions with Drawings 2020100872
Figure 1
1/1
AU2020100872A 2020-05-28 2020-05-28 An Ar-Ar Dating Method Without Standards For Minerals Ceased AU2020100872A4 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
AU2020100872A AU2020100872A4 (en) 2020-05-28 2020-05-28 An Ar-Ar Dating Method Without Standards For Minerals

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
AU2020100872A AU2020100872A4 (en) 2020-05-28 2020-05-28 An Ar-Ar Dating Method Without Standards For Minerals

Publications (1)

Publication Number Publication Date
AU2020100872A4 true AU2020100872A4 (en) 2020-07-09

Family

ID=71402915

Family Applications (1)

Application Number Title Priority Date Filing Date
AU2020100872A Ceased AU2020100872A4 (en) 2020-05-28 2020-05-28 An Ar-Ar Dating Method Without Standards For Minerals

Country Status (1)

Country Link
AU (1) AU2020100872A4 (en)

Cited By (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN112462037A (en) * 2020-11-20 2021-03-09 核工业北京地质研究院 Method for determining age of ore by radioactive cause abnormal lead under non-closed system
CN113325458A (en) * 2021-08-02 2021-08-31 中国科学院地质与地球物理研究所 Combined measurement method for argon-argon age and cosmic exposure age of extra-terrestrial sample
CN114646998A (en) * 2022-03-24 2022-06-21 西北核技术研究所 High-flux fast neutron energy spectrum measuring system and method based on gas activation

Cited By (5)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN112462037A (en) * 2020-11-20 2021-03-09 核工业北京地质研究院 Method for determining age of ore by radioactive cause abnormal lead under non-closed system
CN112462037B (en) * 2020-11-20 2022-10-21 核工业北京地质研究院 Method for determining age of ore by radioactive cause abnormal lead under non-closed system
CN113325458A (en) * 2021-08-02 2021-08-31 中国科学院地质与地球物理研究所 Combined measurement method for argon-argon age and cosmic exposure age of extra-terrestrial sample
CN113325458B (en) * 2021-08-02 2021-10-29 中国科学院地质与地球物理研究所 Combined measurement method for argon-argon age and cosmic exposure age of extra-terrestrial sample
CN114646998A (en) * 2022-03-24 2022-06-21 西北核技术研究所 High-flux fast neutron energy spectrum measuring system and method based on gas activation

Similar Documents

Publication Publication Date Title
AU2020100872A4 (en) An Ar-Ar Dating Method Without Standards For Minerals
Johansson et al. An experimental study of the prompt fission neutron spectrum induced by 0.5-MeV neutrons incident on uranium-235
CN104865283B (en) Mineral stantardless argon-argon dating method
Bray et al. Elastic scattering of protons from 40Ca at 21.0, 23.5, 26.3 and 48.0 MeV
Budtz-Jørgensen et al. Neutron-induced fission cross section of plutonium-240 in the energy range from 10 keV to 10 MeV
Gunn et al. Calorimetric determination of the average total kinetic energy of fragments from fission of U 235
Ohm et al. Beta-delayed neutron emission following the decay of 17N
Kashchuk et al. A conceptual project for a divertor monitor of the neutron yield in the ITER
Asai et al. Detailed design of ex-vessel neutron yield monitor for ITER
Meadows The thick-target 9 Be (d, n) neutron spectra for deuteron energies between 2.6 and 7.0-MeV
Hambsch et al. The 10B (n, α0)/10B (n, α1γ) branching ratio
Tiwari et al. Analysis of uranium bearing samples for rare earth and other elements by k0-based internal monostandard INAA method
Brückner et al. Investigation of the 7Li (p, n) neutron fields at high energies
Fursov et al. Measurements of the fission cross section ratios 232 Th/235 U and 234 U/235 U for 0.13–7.4 MeV neutrons
Pashchenko Reaction cross-sections induced by 14.5 MeV and by Cf-252 and U-235 fission spectrum neutrons
CN117805878A (en) Neutron dose equivalent measuring device based on characteristic gamma correction and measuring method thereof
Orphan et al. A facility for measuring cross sections of (n, xγ) reactions using an electron linac
Freeman et al. The (n, α) cross sections for natural nickel, iron, chromium and molybdenum in a fission neutron spectrum
Abderahim et al. RECALIBRATION OF SOME SEALED FISSION CHAMBERS-FRANCE–IN MARK III, MOL, BELGIUM FACILITY
van Belle et al. Calibration of the JET neutron yield monitors using the delayed neutron counting technique
Diakaki et al. HNPS Proceedings
Wang et al. Cross sections of the Fe 56 (n, α) Cr 53 and Fe 54 (n, α) Cr 51 reactions in the MeV region
Ito et al. Development of helium accumulation fluence monitor for fast reactor dosimetry
Gupta et al. The efficiency of the 4π-neutron counter
Jimenez et al. Continuous Measurement of Boron Concentration in Nuclear Power Plants: Why is it Essential for Safe and Efficient Operation?

Legal Events

Date Code Title Description
FGI Letters patent sealed or granted (innovation patent)
MK22 Patent ceased section 143a(d), or expired - non payment of renewal fee or expiry