content_image/340805.jpg content_image/340812.jpg
<img src='content_image/340805.jpg'>

Since the unitarity bound Δ ≥ | R | is not saturated asymptotically, the dual operators are not expected to be holomorphic. To help the identification, we quote here the dictionary of gauge/membrane correspondence. 

<img src='content_image/340812.jpg'>

All we can say about the dual operators is that their composition is such that the vanishing global charges cancel. For instance, R → 0 implies we should have the same number of X ’s as ¯ X ’s for infinitely long operators. Thus these states are far from supersymmetric, and it will be highly nontrivial to verify the correspondence by comparing the spectrum of the quiver Chern-Simons theory. 

## V. DISCUSSION 

In this paper we have studied the classical membrane action in a nontrivial 11 dimensional background, AdS$_{4}$ × M 1 , 1 , 1 . The AdS/CFT correspondence implies classical solutions with large energy give an approximate description of dual field theory operators which are very long. A rigid configuration is required to rotate to satisfy the equation of motion, and the angular momenta in the internal space M 1 , 1 , 1 correspond to some global charges on the field theory side. 

