1. Ne and Ar isotopic analysis by a multicollector noble gas mass spectrometer Suruchi Goel and S.V.S. Murty Physical Research Laboratory, Ahmedabad – 38 00 09 1.Introduction Precise isotopic measurements of Ne and Ar are very important in the identification of minute changes that result from specific physical or nuclear processes. Cosmic ray produced 21 Ne in the surface rocks on Earth [1], nucleogenic 21 Ne in U, Th rich minerals [2], 36 Ar production through 35 Cl(n,γ) 36 Cl(β-) 36 Ar in salt deposits, Ar isotopes of trapped air in ice cores as climate markers [3], determination of the primordial abundance of the isotope 40 Ar [4] etc. have great potential in serving as chronological tools as well as tracers to decipher physical processes in the past. Compared to the usual peak jumping techniques employed by a single collector mass spectrometer, a multicollector mass spectrometer provides an advantage for achieving higher precision, in terms of reduced analysis time and consequently the memory effects, particularly when dealing with small gas amounts. Here we describe the Ne and Ar analysis using a noble gas mass spectrometer (Noblesse, procured from Nu Instruments, UK) with three collectors (one Faraday cup/or multiplier, and two multipliers). 2. Instrumental Details In the PLANEX Program at PRL, we have recently procured a multi collector noble gas mass spectrometer, Noblesse from Nu Instruments, UK. This mass spectrometer has 75 o magnetic sector and modified Nier-type Ion Source. It has four fixed collectors; one Faraday and three Ion counting electron multipliers. The Faraday (F) and one multiplier (IC0) are behind a slit and an electrostatic deflector is used to send ion beam into one or other of the pair. Hence the three collectors (Faraday or Multiplier [high mass side]), and the other two multipliers (IC1: axial and IC2: low mass side) are used for multi-collection. The multi-collection is achieved by patented method of two lens arrays (called as Quad lenses, since they provide a field equivalent to an electrostatic quadrapole) placed between magnet exit pole and collectors. The Quad lenses allow the achievement of dispersion of ion beams equivalent to physical separation of distance for the three collectors for simultaneous analysis of isotopes of each element (the degree of dispersion varies with the element). The quad lenses can be set at dispersion of one unit, two unit, four unit and six unit mass difference for Ne isotopes ( 20 Ne, 21 Ne, 22 Ne), Ar isotopes ( 36 Ar, 38 Ar, 40 Ar), Kr (e.g. 86 Kr, 82 Kr & 78 Kr simultaneously on three collectors) and Xe isotopes (e.g. 136 Xe, 130 Xe & 124 Xe) respectively. After achieving the proper Z-focusing and source ion settings the quad lenses settings for each element (and for each combination of isotopes) were obtained. The hydrocarbon background like 38 Ar and C 3 H 2 can be pseudo resolved. By the means of Zoom optics (Quads) the magnet can be offset from the peak centre, which is done for the 38 Ar to remain at the pure 38 Ar peak top. This beam dispersion to achieve simultaneous focus of the three isotopes on to three collectors by the quad lenses offers an advantage over mechanical adjustment of collectors spacing that often results in spurt of degassing and increased background. Ne and Ar isotopic analysis by HELIX-MC and ARGUS respectively has also been reported recently [5] & [6]. 4. Results & Discussion For the 1.48E-16 moles of 22 Ne, the 20 Ne/ 22 Ne and 21 Ne/ 22 Ne ratios are 10.78±0.50 and 0.0311±0.0014 resp. for Multi-collection mode, while for Peak Jumping it is 9.91±0.17 and 0.0283±0.0032 resp. From the above 21 Ne/ 22 Ne ratio it is clear that about 3 millions of atoms of 21 Ne can be easily detected with less than 10% uncertainty. The excess of few 10 5 atoms of 21 Ne can then be distinguished. The 40 Ar/ 36 Ar ratio is 291.88±0.35, and 38 Ar/ 36 Ar ratio is 0.1881±0.0081 for 2.03E-15 moles of 38 Ar. The Uncertainty in measured ratios increases with lowered amounts. The ratios in multi-collection modes differ from Peak-Jumping ratios due to different efficiencies of electron multipliers. The instrument settings are still not at optimum level and there is room for improvement by further fine tuning. 5. Conclusion The protocols for analysis of Ne and Ar were made for both multi- collection and Peak Jumping modes. The Multi-collection mode provides advantages over the Peak-Jumping analysis as its reduces analysis time and enable detection of small amounts of gas with precision. 6. References 1.T.Graf et al, Noble Gas Geochemistry and Cosmochemistry, J. Matsuda, Ist Ed., 1994, 115-123, Terra Sci., Tokyo. 2.S. Basu, S.V.S. Murty and A. Kumar, Current Sci. 88 (2005), 445- 448. 3.J.P. Severinghaus et al, GCA 67 (2003), 325-343. 4.F. Begemann et al, APJ 203 (1976), L155-L157. 5.Y. Marrocchi et al, Geochem. Geophy. Geosys. (2009) 10.1029/2008GC002339. 6.D.F. Mark et al, Geochem. Geophy. Geosys. (2009) 10.1029/2009GC002643. 3. Experimental Details The heavy noble gases (Ar, Kr & Xe) were separated from Ne in the Air standard by Liquid N 2 trap on activated charcoal finger and purified by SAES NP10 getters. During the Ne analysis the liq. N 2 trap was kept parallel to mass spectrometer volume in order to reduce the contributions from 40 Ar ++ and 44 CO 2 ++ to 20 Ne and 22 Ne respectively. Different amounts of splits of air standard slug, for each Ne and Ar were taken to obtain variation of ratios with amounts. Fig.1 Variability of the 20 Ne/ 22 Ne (measured) in multi-collection mode as a function of the amount of 22 Ne present in the mass spectrometer. Fig.4 Variability of the 38 Ar/ 36 Ar (measured in multi-collection mode) as a function of the amount of 38 Ar present in the mass spectrometer. Fig.2 Variability of the 21 Ne/ 22 Ne (measured in multi-collection mode) as a function of the amount of 22 Ne present in the mass spectrometer. Fig.3 Variability of the 40 Ar/ 36 Ar (measured in multi-collection mode) as a function of the amount of 40 Ar present in the mass spectrometer. 3. Experimental Details ctd… The Ne was analyzed in both Peak Jumping and Multi-collection mode (in which the 40 Ar and 44 CO 2 peaks were also included). The Argon was analysed in Multi-collection mode with proper centring of isotopes to avoid pseudo resolved background peaks. In Fig.1 & 2. are shown the measured isotopic ratios in multi-collection mode (corrected for 40 Ar ++ and 44 CO 2 ++ contributions) with varying amount of 22 Ne amount. Similarly, Fig.3 & Fig.4 shows Ar isotopic ratios with varying amount as measured in multi-collection mode.