ASTM F2405-2004(2011) Standard Test Method for Trace Metallic Impurities in High Purity Copper by High-Mass-Resolution Glow Discharge Mass Spectrometer《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.pdf
《ASTM F2405-2004(2011) Standard Test Method for Trace Metallic Impurities in High Purity Copper by High-Mass-Resolution Glow Discharge Mass Spectrometer《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.pdf》由会员分享,可在线阅读,更多相关《ASTM F2405-2004(2011) Standard Test Method for Trace Metallic Impurities in High Purity Copper by High-Mass-Resolution Glow Discharge Mass Spectrometer《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.pdf(5页珍藏版)》请在麦多课文档分享上搜索。
1、Designation: F2405 04 (Reapproved 2011)Standard Test Method forTrace Metallic Impurities in High Purity Copper by High-Mass-Resolution Glow Discharge Mass Spectrometer1This standard is issued under the fixed designation F2405; the number immediately following the designation indicates the year ofori
2、ginal adoption or, in the case of revision, the year of last revision. A number in parentheses indicates the year of last reapproval. Asuperscript epsilon () indicates an editorial change since the last revision or reapproval.1. Scope1.1 This test method covers the concentrations of tracemetallic im
3、purities in high 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 a
4、nalyses. Sophisticated 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
5、 detection limits, 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 estab
6、lish appro-priate safety and health practices and determine the applica-bility of regulatory limitations prior to use.2. Referenced Documents2.1 ASTM Standards:2E135 Terminology Relating to Analytical Chemistry forMetals, Ores, and Related MaterialsE173 Practice for Conducting Interlaboratory Studie
7、s ofMethods for Chemical Analysis of Metals3E180 Practice for Determining the Precision of ASTMMethods for Analysis and Testing of Industrial and Spe-cialty Chemicals3E691 Practice for Conducting an Interlaboratory Study toDetermine the Precision of a Test MethodE876 Practice for Use of Statistics i
8、n the Evaluation ofSpectrometric Data3F1593 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 E135. Required terminology specific to this test
9、method, not covered in Terminology E135, 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 suit
10、able foruse 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 meta
11、llic impurities 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 t
12、he specimen 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 to
13、talmeasured current, less contributions from all other interferingsources. Portions of the measured current may originate from1This test method is under the jurisdiction of ASTM Committee F01 onElectronics and is the direct responsibility of Subcommittee F01.17 on SputterMetallization.Current editio
14、n approved June 1, 2011. Published June 2011. Originallyapproved in 2004. Last previous edition approved in 2004 as F240504. DOI:10.1520/F2405-04R11.2For referenced ASTM standards, visit the ASTM website, www.astm.org, orcontact ASTM Customer Service at serviceastm.org. For Annual Book of ASTMStanda
15、rds volume information, refer to the standards Document Summary page onthe ASTM website.3Withdrawn. The last approved version of this historical standard is referencedon www.astm.org.1Copyright ASTM International, 100 Barr Harbor Drive, PO Box C700, West Conshohocken, PA 19428-2959, United States.th
16、e ion detector alone (detector noise). Portions may be due toincompletely mass resolved ions of an isotope or molecule withmass close to, but not identical with Mi. In all such instancesthe interfering contributions must be estimated and subtractedfrom the measured signal.4.2.1 If the source of inte
17、rfering 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 of the detectionlimit for the current due to the isotope.4.3 The composition of the test specimen is ca
18、lculated 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 reference material performed under the same analyticalconditions, source configuration, and operating pr
19、otocol 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 appropriate isotopicabundance factors (A (Xi),A(Yj) and RSFs. I(Xi) and I(Yj)refer to the measured ion curre
20、nt 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 Y is taken to be the copper matrix (RSF(M/M) = 1.0), (X) is (with only very small error for pure meta
21、lmatrices) 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 example, sputtering targets, evaporation sources) used inthin film metallization processes. This test me
22、thod 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 analystsin various laboratories for unifying the protocol and parametersfor determining trace impurities
23、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 method,and the significance and reliability of reported GDMS data.5.3 For most metallic species, the d
24、etection 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 forproducers and users of electronic-grade copper materials.6. Apparatus6.1 Glow Discharge Mass Spectromet
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