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<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mi mathvariant="bold-script">N</mml:mi><mml:mo>=</mml:mo><mml:mn>8</mml:mn><mml:mn /></mml:math>SCFT and M theory on<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mrow><mml:msub><mml:mrow><mml:mi mathvariant="normal">AdS</mml:mi></mml:mrow><mml:mrow><mml:mn>4</mml:mn></mml:mrow></mml:msub></mml:mrow><mml:mo>×</mml:mo><mml:mrow><mml:msup><mml:mrow><mml:mi mathvariant="normal">RP</mml:mi…
We study M theory on ${\mathrm{AdS}}_{4}\ifmmode\times\else\texttimes\fi{}{\mathrm{RP}}^{7}$ corresponding to 3 dimensional $\mathcal{N}=8$ superconformal field theory which is the strong coupling limit of 3 dimensional super Yang-Mills theory. For $\mathrm{SU}(N)$ theory, a wrapped M5 brane on ${\mathrm{RP}}^{5}$ can be interpreted as the baryon vertex. For $\mathrm{SO}(N)/Sp(2N)$ theory, by using the property of …