# Apparent failure of SUSY nonrenormalization theorem

I am having trouble reconciling two pieces of information.

Consider supersymmetric QED, i.e. a supersymmetric U(1) gauge theory with two chiral superfields of opposite charges, $h$ and $\hat{h}$. The Kähler potential $K$ is canonical, $K = h^\dagger e^{2\,g\,q\,V} h + {\hat{h}}^\dagger e^{-2\,g\,q\,V} \hat{h} ,$ while the superpotential $W$ is the simplest possible: $$W = m\, h \, \hat{h}.$$

# On the one hand

Renormalized mass and fields are related to bare/original ones by: $$m_0 = Z_m m_r, \qquad h_0 = {Z_h}^{1/2}\, h_r,\qquad \hat{h}_0 = {Z_h}^{1/2}\, \hat{h}_r.$$

The SUSY non-renormalization theorems say that $W$ is not perturbatively renormalized, implying that $$Z_m Z_h = 1 \quad \Rightarrow \quad \delta_m = - \delta_h,$$ at the one loop level (as usual $Z_m = 1 + \delta_m$, $Z_h = 1 + \delta_h$). The counterterm Feynman rule for the scalar propagator of $h$ will then be: i.e. the scalar propagator counterterm is proportional to $(p^2+m^2)$.

# On the other hand

If one explicitly computes the divergent part of the $h$ self energy at one loop in dimensional regularization, one finds* that: $$i \Sigma_h (p^2) \bigg|_\textrm{div} = i \frac{g^2 q^2 }{(4\pi)^2} \frac{2}{\epsilon} \big(-4 m^2\big).$$ *In the literature one can find this result e.g. in arXiv:hep-ph/9907393, section 4.3, equation (150), by playing with the integrals. This result is obtained in the Feynman gauge ($\xi = 1$).

i.e. the divergent part of the self-energy at one loop is proportional to just $m^2$.

QUESTION: I was expecting a divergent part proportional to $(p^2 + m^2)$, which is what can be cancelled by the aforementioned counterterm. Is this reasoning correct? What might have gone wrong?

## Diagrams

To make this question more accessible, here are the diagrams (usual Feynman diagrams, not supergraphs) which sum to give $i \Sigma_h (p^2) \big|_\textrm{div}$:

I am assuming there is something naïve in my approach. Perhaps some subtlety with the gauge diagrams, or Wess-Zumino gauge (I don't know any more at this point).

## Dimensional regularization

At the outset there doesn't seem to be a problem with using dimensional regularization. The SUSY violation introduced by it should be proportional to $\epsilon$ (Martin's SUSY Primer, p. 61), thus only affecting finite terms.

## Symmetries and missing terms

An R-symmetry under which both $h$ and $\hat h$ have charge $+1$ forbids adding gauge invariant terms like $h \hat h$ to the Kähler.

The discrete symmetry under which $h \leftrightarrow \hat h$ and $V \rightarrow - V$ forbids adding a Fayet-Iliopoulos term.

• Dim reg is typically not a good regulator for SUSY theories because of the dimensional dependence of the representation theory for fermions. Perhaps you are having problems because your regulator breaks SUSY? What happens if you use Pauli-Villars? – user2309840 Dec 30 '15 at 17:05
• @user2309840: At the outset it doesn't seem to be a problem: according to Stephen Martin's SUSY Primer, p. 61, the spurious violation of SUSY introduced by Dim reg is proportional to $\epsilon$. Since the highest divergent pole I have is $1/\epsilon$, this issue should only affect the finite part of the computation, which is not relevant here. – J-T Dec 31 '15 at 13:57

A non-local term like $\int d^4x d^4\theta \frac{1}{\Box} D^2 W(\Phi)$ is not taken into account while proving no-renormalization theorem (to maintain locality) but can cause a correction to superpotential as using, $\int d^4\theta\rightarrow \int d^2\theta \bar{D}^2$ and $\bar{D}^2D^2\Phi=\Box\Phi$ gives precisely a term like $\int d^2\theta d^4x W(\Phi)$ and modifies the superpotential.