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We study M theory on $AdS_4 \times \RP^7$ corresponding to 3 dimensional${\cal N}=8$ superconformal field theory which is the strong coupling limit of3 dimensional super Yang-Mills theory. For SU(N) theory, a wrapped M5 brane on$\RP^5$ can be interpreted as baryon vertex. For $SO(N)/Sp(2N)$ theory, byusing the property of (co-)homology of $\RP^7$, we classify various wrappingbranes and consider domain walls and the baryon vertex.Comment: 17 pages, Changed baryon like operator as M5 branes in M theory  rather than D6 brane in IIA theory. To appear in Phys.Rev.

physical review. d. particles, fields, gravitation, and cosmology/physical review. d. particles and fields

<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…

N=8SCFT and M theory onAdS4×RP