polarizability  see Table I. Because of the sign of the magnetic moment contribution  we expect the pseudo-polarizability to be less than the electric polarizability. The values of the magnetic moment and electric polarizability extracted from boost-projected correlators can be used to find a value for the pseudo-polarizability. Using the results of Table I in Eq. (B5)  we find for the two field-correlated fits. These values are concordant with those found in Table III from analyzing the unpolarized neutron correlators. Finally  we note that unpolarized proton correlation functions in principle allow one access to both the magnetic moment and electric polarizability. This can be seen from the explicit form for the proton two-point function derived in the effective hadronic the- ory. The functional form  however  leads to fits that are challenging to perform. Valuable simplifications are afforded by boost projected correlators. I : A latt E = 17(9)(2)   and II : A latt E = 19(19)(2)   (B6) [1] T. DeGrand and C. DeTar  Lattice Methods for Quantum Chromodynamics (World Scientific  2006). [2] G. Martinelli and C. T. Sachrajda  Nucl. Phys. B306   865 (1988). [3] B. C. Tiburzi  Phys. Lett. B617   40 (2005)  hep-lat/0504002. [4] B. C. Tiburzi  Phys. Lett. B641   342 (2006)  hep-lat/0607019. [5] F. Fucito  G. Parisi  and S. Petrarca  Phys. Lett. B115   148 (1982). [6] G. Martinelli  G. Parisi  R. Petronzio  and F. Rapuano  Phys. Lett. B116   434 (1982). [7] C. W. Bernard  T. Draper  K. Olynyk  and M. Rushton  Phys. Rev. Lett. 49   1076 (1982). [9] J. Christensen  W. Wilcox  F. X. Lee  and L.-M. Zhou  Phys. Rev. D72   034503 (2005)  hep-lat/0408024. [8] H. R. Fiebig  W. Wilcox  and R. M. Woloshyn  Nucl. Phys. B324   47 (1989). [10] A. Alexandru and F. X. Lee (2009)  0911.2520. [11] M. Engelhardt (LHPC)  Phys. Rev. D76   114502 (2007)  0706.3919. [12] W. Detmold  B. C. Tiburzi  and A. Walker-Loud  Phys. Rev. D73   114505 (2006)  hep- lat/0603026. [13] W. Detmold  B. C. Tiburzi  and A. Walker-Loud  Phys. Rev. D79   094505 (2009)  0904.1586.   051502 (2009)  [14] C. Aubin  K. Orginos  V. Pascalutsa  and M. Vanderhaeghen  Phys. Rev. D79 0811.2440. [15] P. V. Buividovich  M. N. Chernodub  E. V. Luschevskaya  and M. I. Polikarpov  Nucl. Phys. B826   313 (2010)  0906.0488. [16] P. V. Buividovich  M. N. Chernodub  E. V. Luschevskaya  and M. I. Polikarpov  Phys. Rev. D80   054503 (2009)  0907.0494. [17] J. Hu  F.-J. Jiang  and B. C. Tiburzi  Phys. Lett. B653   350 (2007)  arXiv:0706.3408 [hep-lat]. [18] B. C. Tiburzi  Phys. Lett. B674   336 (2009)  0809.1886. [19] W. Detmold  B. C. Tiburzi  and A. Walker-Loud (2009)  0908.3626. [20] B. C. Tiburzi  Nucl. Phys. A814   74 (2008)  0808.3965. [21] J. S. Schwinger  Phys. Rev. 82   664 (1951). [22] R. G. Edwards  B. Joo  and H.-W. Lin  Phys. Rev. D78   054501 (2008)  0803.3960. [23] H.-W. Lin et al. (Hadron Spectrum)  Phys. Rev. D79   034502 (2009)  0810.3588. [24] A. Stathopoulos and K. Orginos (2007)  0707.0131. 21