We show that fluctuating tethered membranes with any intrinsic anisotropy unavoidably exhibit a new phase between the previously predicted ``flat'' and ``crumpled'' phases, in high spatial dimensions d where the crumpled phase exists. In this new ``tubule'' phase, the membrane is crumpled in one direction but extended nearly straight in the other. Its average thickness is RG~L^νₜ with L the intrinsic size of the membrane. This phase is more likely to persist down to d0ex0ex=0ex0ex3 than the crumpled phase. In Flory theory, the universal exponent νₜ0ex0ex=0ex0ex3/4, which we conjecture is an exact result. We study the elasticity and fluctuations of the tubule state, and the transitions into it.
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Radzihovsky et al. (1995) studied this question.
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