ASTM F2405-2004 Standard Test Method for Trace Metallic Impurities in High Purity Copper by High-Mass-Resolution Glow Discharge Mass Spectrometer《使用高质量分辨率辉光放电质谱仪测量高纯度铜中痕量金属杂质的标准试验方.pdf
《ASTM F2405-2004 Standard Test Method for Trace Metallic Impurities in High Purity Copper by High-Mass-Resolution Glow Discharge Mass Spectrometer《使用高质量分辨率辉光放电质谱仪测量高纯度铜中痕量金属杂质的标准试验方.pdf》由会员分享,可在线阅读,更多相关《ASTM F2405-2004 Standard Test Method for Trace Metallic Impurities in High Purity Copper by High-Mass-Resolution Glow Discharge Mass Spectrometer《使用高质量分辨率辉光放电质谱仪测量高纯度铜中痕量金属杂质的标准试验方.pdf(5页珍藏版)》请在麦多课文档分享上搜索。
1、Designation: F 2405 04Standard Test Method forTrace Metallic Impurities in High Purity Copper by High-Mass-Resolution Glow Discharge Mass Spectrometer1This standard is issued under the fixed designation F 2405; the number immediately following the designation indicates the year oforiginal adoption o
2、r, in the case of revision, the year of last revision. A number in parentheses indicates the year of last reapproval. Asuperscript epsilon (e) indicates an editorial change since the last revision or reapproval.1. Scope1.1 This test method covers the concentrations of tracemetallic impurities in hig
3、h purity (99.95 wt. % pure, or purer,with respect to metallic trace impurities) electronic gradecopper.1.2 This test method pertains to analysis by magnetic-sectorglow discharge mass spectrometer (GDMS).1.3 This test method does not include all the informationneeded to complete GDMS analyses. Sophis
4、ticated computer-controlled laboratory equipment, skillfully used by an experi-enced operator, is required to achieve the required sensitivity.This test method does cover the particular factors (for example,specimen preparation, setting of relative sensitivity factors,determination of detection limi
5、ts, and the like) known by theresponsible technical committee to effect the reliability of highpurity copper analyses.1.4 This standard does not purport to address all of thesafety concerns, if any, associated with its use. It is theresponsibility of the user of this standard to establish appro-pria
6、te safety and health practices and determine the applica-bility of regulatory limitations prior to use.2. Referenced Documents2.1 ASTM Standards:2E 135 Terminology Relating to Analytical Chemistry forMetals, Ores, and Related MaterialsE 173 Practice for Conducting Interlaboratory Studies ofMethods f
7、or Chemical Analysis of Metals3E 180 Practice for Determining the Precision of ASTMMethods for Analysis and Testing of Industrial and Spe-cialty ChemicalsE 691 Practice for Conducting an Interlaboratory Study toDetermine the Precision of a Test MethodE 876 Practice for Use of Statistics in the Evalu
8、ation ofSpectrometric DataF 1593 Test Method for Trace Metallic Impurities in Elec-tronic Grade Aluminum by High Mass-Resolution Glow-Discharge Mass Spectrometer3. Terminology3.1 Terminology in this test method is consistent withTerminology E 135. Required terminology specific to this testmethod, no
9、t covered in Terminology E 135, is indicated in 3.2.3.2 Definitions:3.2.1 campaigna test procedure to determine the accuracyof the instrument, which was normally performed at thebeginning of the day or after the instrument modification, orboth.3.2.2 reference samplematerial accepted as suitable foru
10、se as a calibration/sensitivity reference standard by all partiesconcerned with the analyses.3.2.3 specimena suitably sized piece cut from a referenceor test sample, prepared for installation in the GDMS ionsource, and analyzed.3.2.4 test samplematerial (copper) to be analyzed fortrace metallic impu
11、rities by this GDMS method.3.2.4.1 DiscussionGenerally the test sample is extractedfrom a larger batch (lot, casting) of product and is intended tobe representative of the batch.4. Summary of Test Method4.1 A specimen is mounted in a plasma discharge cell.Atoms subsequently sputtered from the specim
12、en surface areionized, and then focused as an ion beam through a double-focusing magnetic-sector mass separation apparatus. The massspectrum (the ion current) is collected as magnetic field oracceleration voltage, or both, and is scanned.4.2 The ion current of an isotope at mass Miis the totalmeasur
13、ed current, less contributions from all other interferingsources. Portions of the measured current may originate fromthe ion detector alone (detector noise). Portions may be due toincompletely mass resolved ions of an isotope or molecule with1This test method is under the jurisdiction of ASTM Commit
14、tee F01 onElectronics and is the direct responsibility of Subcommittee F01.17 on SputterMetallization.Current edition approved May 1, 2004. Published June 2004.2For referenced ASTM standards, visit the ASTM website, www.astm.org, orcontact ASTM Customer Service at serviceastm.org. For Annual Book of
15、 ASTMStandards volume information, refer to the standards Document Summary page onthe ASTM website.3Withdrawn.1Copyright ASTM International, 100 Barr Harbor Drive, PO Box C700, West Conshohocken, PA 19428-2959, United States.mass close to, but not identical with Mi. In all such instancesthe interfer
16、ing contributions must be estimated and subtractedfrom the measured signal.4.2.1 If the source of interfering contributions to the mea-sured ion current at Micannot be determined unambiguously,the measured current less the interfering contributions fromidentified sources constitutes an upper bound o
17、f the detectionlimit for the current due to the isotope.4.3 The composition of the test specimen is calculated fromthe mass spectrum by applying a relative sensitivity factor(RSF(X/M) for each contaminant element, X, compared to thematrix element, M. RSFs are determined in a separate analysisof a re
18、ference material performed under the same analyticalconditions, source configuration, and operating protocol as forthe test specimen.4.4 The relative concentrations of elements X and Y arecalculated from the relative isotopic ion currents I(Xi) and I(Yj) in the mass spectrum, adjusted for the approp
19、riate isotopicabundance factors (A (Xi),A(Yj) and RSFs. I(Xi) and I(Yj)refer to the measured ion current from isotopes Xiand Yj,respectively, of atomic species X and Y as follows:X!Y!5RSFX/M!RSFY/M!3AYj!AXi!3IXi!IYj!where (X)/(Y) is the concentration ratio of atomic species Xto species Y. If species
20、 Y is taken to be the copper matrix (RSF(M/M) = 1.0), (X) is (with only very small error for pure metalmatrices) the absolute impurity concentration of X.5. Significance and Use5.1 This test method is intended for application in thesemiconductor industry for evaluating the purity of materials(for ex
21、ample, sputtering targets, evaporation sources) used inthin film metallization processes. This test method may beuseful in additional applications, not envisioned by the respon-sible technical committee, as agreed upon between the partiesconcerned.5.2 This test method is intended for use by GDMS ana
22、lystsin various laboratories for unifying the protocol and parametersfor determining trace impurities in copper. The objective is toimprove laboratory-to-laboratory agreement of analysis data.This test method is also directed to the users of GDMSanalyses as an aid to understanding the determination
23、method,and the significance and reliability of reported GDMS data.5.3 For most metallic species, the detection limit for routineanalysis is on the order of 0.01 wt. ppm. With specialprecautions, detection limits to sub-ppb levels are possible.5.4 This test method may be used as a referee method forp
24、roducers and users of electronic-grade copper materials.6. Apparatus6.1 Glow Discharge Mass Spectrometer, with mass resolu-tion greater than 3500, and associated equipment and supplies.6.2 Machining Apparatus, capable of preparing specimensand reference samples in the desired geometry and with smoot
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