Neutron electric dipole moment from lattice QCD
| dc.creator | Shintani, E. | |
| dc.creator | Aoki, S. | |
| dc.creator | Ishizuka, N. | |
| dc.creator | Kanaya, K. | |
| dc.creator | Kikukawa, Y. | |
| dc.creator | Kuramashi, Y. | |
| dc.creator | Okawa, M. | |
| dc.creator | Tanigchi, Y. | |
| dc.creator | Ukawa, A. | |
| dc.creator | Yoshié, T. | |
| dc.date | 2005-05-19 | |
| dc.date | 2005-08-01 | |
| dc.date.accessioned | 2026-07-07T10:28:41Z | |
| dc.date.available | 2026-07-07T10:28:41Z | |
| dc.description | We carry out a feasibility study for the lattice QCD calculation of the neutron electric dipole moment (NEDM) in the presence of the $θ$ term. We develop the strategy to obtain the nucleon EDM from the CP-odd electromagnetic form factor $F_3$ at small $θ$, in which NEDM is given by $\lim_{q^2\to 0}θF_3(q^2)/(2m_N)$ where $q$ is the momentum transfer and $m_N$ is the nucleon mass. We first derive a formula which relates $F_3$, a matrix element of the electromagnetic current between nucleon states, with vacuum expectation values of nucleons and/or the current. In the expansion of $θ$, the parity-odd part of the nucleon-current-nucleon three-point function contains contributions not only from the parity-odd form factors but also from the parity-even form factors multiplied by the parity-odd part of the nucleon two-point function, and therefore the latter contribution must be subtracted to extract $F_3$. We then perform an explicit lattice calculation employing the domain-wall quark action with the RG improved gauge action in quenched QCD at $a^{-1}\simeq 2$ GeV on a $16^3\times 32\times 16$ lattice. At the quark mass $m_f a =0.03$, corresponding to $m_π/m_ρ\simeq 0.63$, we accumulate 730 configurations, which allow us to extract the parity-odd part in both two- and three-point functions. Employing two different Dirac $γ$ matrix projections, we show that a consistent value for $F_3$ cannot be obtained without the subtraction described above. We obtain $F_3(q^2\simeq 0.58 \textrm{GeV}^2)/(2m_N) =$ $-$0.024(5) $e\cdot$fm for the neutron and $F_3(q^2\simeq 0.58 \textrm{GeV}^2)/(2m_N) =$ 0.021(6) $e\cdot$fm for the proton. | |
| dc.description | LaTeX2e, 43 pages, 42 eps figures, uses revtex4 and graphicx, comments added and typos corrected, final version to appear in Phys. Rev. D | |
| dc.identifier | https://arxiv.org/abs/hep-lat/0505022 | |
| dc.identifier | http://arxiv.org/abs/hep-lat/0505022 | |
| dc.identifier | Phys.Rev.D72:014504,2005 | |
| dc.identifier | doi:10.1103/PhysRevD.72.014504 | |
| dc.identifier.uri | http://salesiana.dossiersoluciones.com/handle/123456789/177537 | |
| dc.subject | High Energy Physics - Lattice | |
| dc.subject | High Energy Physics - Phenomenology | |
| dc.subject | Nuclear Theory | |
| dc.title | Neutron electric dipole moment from lattice QCD | |
| dc.type | text |