M. D. Slaughter

activity

19992019

most citedMagnetic moments of the ground-state

J^{P} = (3/2)^{+}

baryon decuplet

10 citations · 22 across the 8 of their papers we have counts for

collaborators

8 papers

hep-ph2019

Radiative decays and the $SU (6)$ Lie Algebra

Milton Dean Slaughter

We present research on radiative decays of vector ( $J^{P C} = 1^{--}$ ) to pseudoscalar ( $J^{P C} = 0^{-+}$ ) particles ( $u$ , $d$ , $s$ , $c$ , $b$ , $t$ quark system) using broken symmetry te…

hep-ph2011★ 10 cited

Magnetic moments of the ground-state $J^{P} = (3/2)^{+}$ baryon decuplet

Milton Dean Slaughter

The magnetic moment - a function of the electric charge form factor $F_{1} (q^{2})$ and the magnetic dipole form factor $F_{2} (q^{2})$ at zero four-momentum transfer $q^{2}$ -of the…

hep-ph2011

$Ω^{-}$ , $Ξ^{-}$ , $Σ^{-}}$ and $Δ^-}$ decuplet baryon electric charge form factor $F_{1} (q^{2})$

Milton Dean Slaughter

The magnetic moment---a function of the electric charge form factor $F_{1} (q^{2})$ and the magnetic dipole form factor $F_{2} (q^{2})$ at zero four-momentum transfer $q^{2}$ ---of th…

hep-ph2009★ 5 cited

$Ω^{-}$ , $Ξ^{-}$ , $Σ^{-}$ and $Δ^{-}$ decuplet baryon magnetic moments

Milton Dean Slaughter

The properties of the ground state $U$ -Spin $= 3/2$ baryon decuplet magnetic moments $Δ^{-}$ , $Ξ^{*-}$ , $Σ^{*-}$ and $Ω^{-}$ and their ground state spin 1/2 cousins $p$ , $n$ , $Λ…

hep-ph2008★ 3 cited

Gamma N Delta Form Factors and Wigner Rotations

Milton Dean Slaughter

For more than 50 years the Delta N gamma form factors have been studied experimentally, theoretically, and phenomenologically. Although there has been substantial progress in under…

hep-ph2004

Connection between Second Class Currents and the $Δ N γ$ Form Factors $G_{M}^{} (q^{2})$ and $G_{E}^{} (q^{2})$

Milton Dean Slaughter

An interesting connection between the nucleon weak axial-vector second class current form factor $g_{T} (q^{2})$ present in the matrix element $< p ∣ A_{π^{+}}^{μ} ∣ n >$ and the $…

Radiative decays and the SU(6) Lie Algebra

Magnetic moments of the ground-state JP=(3/2)+ baryon decuplet

Ω−, Ξ∗−, $Σ^{*-}}$ and $Δ^-}$ decuplet baryon electric charge form factor F1​(q2)

Ω−, Ξ∗−, Σ∗− and Δ− decuplet baryon magnetic moments

Gamma N Delta Form Factors and Wigner Rotations

Connection between Second Class Currents and the ΔNγ Form Factors GM∗​(q2) and GE∗​(q2)

Radiative decays and the $SU (6)$ Lie Algebra

Magnetic moments of the ground-state $J^{P} = (3/2)^{+}$ baryon decuplet

$Ω^{-}$ , $Ξ^{-}$ , $Σ^{-}}$ and $Δ^-}$ decuplet baryon electric charge form factor $F_{1} (q^{2})$

$Ω^{-}$ , $Ξ^{-}$ , $Σ^{-}$ and $Δ^{-}$ decuplet baryon magnetic moments

Connection between Second Class Currents and the $Δ N γ$ Form Factors $G_{M}^{} (q^{2})$ and $G_{E}^{} (q^{2})$