Volume 2 - LENR-CANR

[1] Chubb, S.R., in Proc. 8th Int. Workshop on Anomalies in Hydrogen / Deuterium Loaded
Metals, 38 (2008). http://www.iscmns.org/catania07/ChubbSrolesofapproxi.pdf
[2] Chubb, S.R., in Low-Energy Nuclear Reactions Sourcebook (J. Marwan, and S.B. Krivit,
eds., American Chemical Society, Washington, DC, 2008) pp. 99-123.)
[3]Chubb, S.R., Proc. ICCF13, (2007), in press.
[4]Chubb, S.R., Proc. ICCF10, 735 (2006). http://www.lenrcanr.org/acrobat/ChubbSRnutsandbol.pdf
[5] Chubb, S.R., submitted to Proc. Roy. Soc., 2005. http://arxiv.org/pdf/cond-mat/0512363
[6] Robert L. Park, (2008) private communication.
[7] David J. Nagel, (2008) private communication.
[8] Talbot Chubb, , (2008) private communication.
[9] Chubb, S.R., claim, based on material presented here and in refs. 1-5.
[10] Schwinger, J., Proc. ICCF1, pp. 130-136 (1990).
Initial(t) | Final(t)
[11] Initial V Final i when Initial(t) and Final(t) evolve in time,
t
in the interaction picture representation, when they (as well as the density operator
(r) (r ri) and total current operator j(r)) evolve in time, in the Schroedinger picture
ri representation, Initial V Final (which is the same when all quantities are expressed in a
common representation) can be expressed using the expression that is shown in Fig.4b.
[12] Chubb, T.A. and S.R. Chubb, J. Condensed Matter Nucl. , Sci. 2, 1–9 (2008).
http://www.cfescience.com/yahoo_site_admin/assets/docs/pdfCoulBar.80171500.pdf
[13] Preparata, G., QED Coherence in Matter (World Scientific, Singapore, 1995).
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