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Cubic one-field Wess–Zumino F-term potential

Physical scope

A one-field classical rigid N=1 Wess–Zumino model with canonical Kähler metric and cubic superpotential, used to illustrate the F-term elimination formula. No quantum, empirical, or particle-spectrum claim is asserted.

Example

Take one chiral field with canonical Kähler potential K(ϕˉ,ϕ)=ϕˉϕ and holomorphic superpotential W(ϕ)=12mϕ2+16yϕ3, where m∈C has mass dimension one and y∈C is dimensionless. In the ordinary complex bosonic sector of the model postulate, take the auxiliary field to be complex-valued; the formal even coefficient space is retained before this restriction. For a smooth compactly supported scalar component ϕ:M→C, the auxiliary equation and F-term potential are

F=−mϕ+12yϕ2‾,VF=∣mϕ+12yϕ2∣2.

This is a classical model calculation, not an empirical claim or a quantum effective potential.

Facts & Assumptions

Given: The one-field canonical model and W(ϕ) in the Example.

[A1]

Rigid four-dimensional N=1 Wess–Zumino sigma-model action: the canonical Kähler choice has gϕϕˉ=1 and its chiral auxiliary sector is FFˉ+FW′(ϕ)+FˉW′(ϕ)‾.

[F1]

Kähler-metric F-term scalar potential in the rigid N=1 model: for a positive Kähler metric, F=−gϕϕˉW′(ϕ)‾ and VF=gϕϕˉW′(ϕ)W′(ϕ)‾.

Verification

Given: [A1], [F1], and the polynomial superpotential in the Example.

1.1givenalgebra

Differentiate W(ϕ)=12mϕ2+16yϕ3 to obtain W′(ϕ)=mϕ+12yϕ2.

2.1A1F1step 1.1algebra∎

Substitute gϕϕˉ=gϕϕˉ=1 and the derivative from step 1.1 into [F1]. This gives F=−mϕ+12yϕ2‾ and VF=∣mϕ+12yϕ2∣2, as stated.

Depends on

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