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How we can interpret this self-dual, or duality in terms of generalized version of electro magneitc duality, or Strong weak duality.

Let me address some basic information. First, electro magnetic duality is a duality of Maxwell's equation in vacuum \begin{align} &\nabla \cdot E =0, \quad \nabla \cdot B=0 \\ & \nabla \times E= - \frac{\partial B}{\partial t}, \quad \nabla \times B= \frac{\partial E}{\partial t} \end{align} above equation is invariant under the transformation of $(E,B)$ to $(B, -E)$. For this relation E,B we call electro-magnetic duality.

From dirac's quantization \begin{align} eg=2\pi n \end{align} and the construction of fine constant $\alpha = \frac{e^2}{4\pi\epsilon \hbar c}$, In QED we know that $\alpha = \frac{1}{137}$.

From above quantization rule, we know that in electric frame, the coupling constant is small, but in magnetic frame its coupling constant is large.

\begin{align} e_{strong} e_{weak} = 2\pi n \end{align}

Thus this can be extended to strong-weak duality.


Now what i want to do is applied this idea to $N=4$ Super Yang Mills theory. How we can analysis this in terms of electro-magnetic duality?

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  • $\begingroup$ Electric-Magnetic duality is a large subject. Have you tried reading the original Montonen & Olive paper? $\endgroup$ – user1504 Dec 8 '15 at 16:45
  • $\begingroup$ @user1504, I have read the original paper, Magnetic Monopoles as Gauge Particles, Phys.Lett. B72 (1977) 117. This paper covers the duality between different gauge groups without susy. I Know, N=4 SYM theory is a sort of Mont. Olive duality (Strong-weak duality). What i have question above is how we know N=4 SYM has such kind of duality. $\endgroup$ – phy_math Dec 10 '15 at 12:21
  • $\begingroup$ Actually, i know from many S-duality materials, the complex coupling constant of $N=4$ SYM is given as $\tau = \theta + g^{-2}$ (with some factor), and for $\theta=0$ there is a dualtiy $g\rightarrow g^{-1}$. I want to know how this procedure is allowed and relevant to electro-magnetic duality $\endgroup$ – phy_math Dec 10 '15 at 12:22
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"What i have question above is how we know N=4 SYM has such kind of duality."

The basic idea is that you make a change of variables in the Feynman integral, by mapping the field strength 2-form $F$ to its dual $*F$. Then you observe that, with respect to these new variables, the Feynman integral still describes a gauge theory, except with the coupling constant $g$ interchanged with $\kappa / g$ and the electric and magnetic observables interchanged.

To really make this argument work, you'd need to regularize and renormalize the two Feynman integrals. This amounts to introducing renormalization flows into the coupling constants and appropriately dressing the observables. In N=4 SYM, Seiberg's holomorphy arguments tell you that the renormalization flows are trivial; likewise, that renormalization doesn't significantly alter the observables. Which indicates that the naive argument actually works for N=4 SYM. I don't think the fine details on this argument have been written down anywhere, however. N=4 duality is still, strictly speaking, a conjecture.

The strongest argument that it's a true conjecture is due to Vafa, who observed that N=4 SYM arises as the low energy limit of both IIA and IIB string theory, compactified on the product $K \times T^2$ of an ALE space $K$ of type ADE and a 2-torus. The strength of the gauge coupling is proportional to the inverse volume of the 2-torus. String theory tells us there is an exact duality which relates IIA and IIB while switch $T^2$ with its dual. In the low energy gauge theory descriptions, this duality flips the electric and magnetic observables. Likewise, it switches the volume of $T^2$ with its inverse, so flips the gauge coupling.

I've also heard speculations the naive argument for duality can be carried out more or less exactly in certain lattice regularizaitons of N=4 SYM. Haven't seen a paper yet though.

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