Technical Appendix

XVII. Technical Appendix B 4-Vector Maxwell-Heaviside Equations... 

XVIII. Technical Appendix C On the Absence of Magnetic Monopoles and Currents in 0(3) Electrodynamics References... 

In this second technical appendix, it is shown that the Maxwell-Heaviside equations can be written in terms of a field 4-vector = (0, cB + iE) rather than as a tensor. Under Lorentz transformation, GM transforms as a 4-vector. This shows that the field in electromagnetic theory is not uniquely defined as a... 

Technical Appendix A Criticisms of the U(l) Invariant Theory of the Aharonov-Bohm Effect and Advantages of an 0(3) Invariant Theory... 

Technical Appendix B 0(3) Electrodynamics from the Irreducible Representations of the Einstein Group References... 

TECHNICAL APPENDIX A CRITICISMS OF THE U(l) INVARIANT THEORY OF THE AHARONOV-BOHM EFFECT AND ADVANTAGES OF AN 0(3)... 

TECHNICAL APPENDIX B 0(3) ELECTRODYNAMICS FROM THE IRREDUCIBLE REPRESENTATIONS OF THE EINSTEIN GROUP... 

This issue is examined in more detail in the technical appendix (Section 7.A). See also Bristol (2007) for simulation results. 

Multiple imputation is not, in fact, always necessary to produce correct variance estimates. It depends on the analysis strategy following single imputation. A simple example is given in the technical appendix. 

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