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000281344 0247_ $$2doi$$a10.1103/PhysRevLett.115.062001
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000281344 0247_ $$2arXiv$$aarXiv:1502.02295
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000281344 1001_ $$0P:(DE-HGF)0$$aGuo, F.-K.$$b0
000281344 245__ $$aElectric Dipole Moment of the Neutron from 2 + 1 Flavor Lattice QCD
000281344 260__ $$aCollege Park, Md.$$bAPS$$c2015
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000281344 520__ $$aWe compute the electric dipole moment d_n of the neutron from a fully dynamical simulation of lattice QCD with 2+1 flavors of clover fermions and nonvanishing theta term. The latter is rotated into the pseudoscalar density in the fermionic action using the axial anomaly. To make the action real, the vacuum angle theta is taken to be purely imaginary. The physical value of d_n is obtained by analytic continuation. We find d_n = -3.8(2)(9) x 10^{-16} [theta e cm], which, when combined with the experimental limit on d_n, leads to the upper bound theta < 7.6 x 10^{-11}.
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000281344 536__ $$0G:(DE-Juel1)hde12_20141101$$aDisconnected Contributions to Matrix Elements and Renormalization factors (hde12_20141101)$$chde12_20141101$$fDisconnected Contributions to Matrix Elements and Renormalization factors$$x2
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000281344 7001_ $$0P:(DE-HGF)0$$aHorsley, R.$$b1
000281344 7001_ $$0P:(DE-Juel1)131252$$aMeißner, U.-G.$$b2$$ufzj
000281344 7001_ $$0P:(DE-HGF)0$$aNakamura, Y.$$b3
000281344 7001_ $$0P:(DE-HGF)0$$aPerlt, H.$$b4
000281344 7001_ $$0P:(DE-HGF)0$$aRakow, P. E. L.$$b5
000281344 7001_ $$0P:(DE-HGF)0$$aSchierholz, G.$$b6
000281344 7001_ $$0P:(DE-HGF)0$$aSchiller, A.$$b7
000281344 7001_ $$0P:(DE-HGF)0$$aZanotti, J. M.$$b8
000281344 773__ $$0PERI:(DE-600)1472655-5$$a10.1103/PhysRevLett.115.062001$$gVol. 115, no. 6, p. 062001$$n6$$p062001$$tPhysical review letters$$v115$$x1079-7114$$y2015
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