Difference between revisions of "PAA Bibliography"
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[[File:Gelen_JRMC_V266_2005_p485.pdf]] | [[File:Gelen_JRMC_V266_2005_p485.pdf]] | ||
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+ | == Books== | ||
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+ | [[Segebade_Weise_Lutz_PAA]] | ||
==Detection Limits== | ==Detection Limits== | ||
http://arxiv.org/abs/1301.1528v1 | http://arxiv.org/abs/1301.1528v1 | ||
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=NAA= | =NAA= |
Revision as of 16:50, 15 May 2013
References
Web Sites
http://ie.lbl.gov/toi/radsearch.asp
http://www.nist.gov/pml/data/xcom/index.cfm
http://yoyo.cc.monash.edu.au/~simcam/ton/
www-nds.iaea.org
Refereed Journals
File:Gelen JRMC V266 2005 p485.pdf
Books
Detection Limits
http://arxiv.org/abs/1301.1528v1
NAA
Ancient Silver
File:Meyers Zelst Sayre BNL-21513.pdf This paper suggest that the gold and iridium content can be used to distinguish between Sasanian (Iran) coins and other silver coins.
Activating gold
Neutron knock out
Au-196 decays with a half life 6.183 days of by electron capture to Platinum (Pt-196) 92% of the time or the rest of the time it Beta decay to Hg-196
The highest relative intensity gamma ray has an energy of 333.03 keV after Au-196 undergoes electron capture. Pt-196 is stable.
If Pt-196 is in an excited state, then there are two lifetimes to de-excite of 8.1 seconds and 9.6 hours . For the 9.6 hours state then dominant intensities are a photon emission energies of 188.27 and 147.81 keV.
Proton Knockout
Pt-196 is naturally occurring in 25% of the Platinum
You will need to produce it in an excited state (356, 689, 877,1526 keV) in order to get a gamma.
Activation Iridium
There are two naturally occuring isotopes of Iridium (37% Ir-191, 63%Ir-193)
Neutron knock out
After 11.78 days Ir-190 electron captures to Os-190 (dominant decay) with the most intense line emission of 186.68 keV.
Proton knock out
Osmium 192 and 190 are stable.