Let (\{| \psi> ,| \phi>}) be an incomparable pair of states ((| \psi
\nleftrightarrow | \phi>)), \emph, i.e., (| \psi>) and (| \phi>) cannot be
transformed to each other with probability one by local transformations and
classical communication (LOCC). We show that incomparable states can be
multiple-copy transformable, \emph, i.e., there can exist a \emph{k}, such that
(| \psi> ^{\otimes k+1}\to | \phi> ^{\otimes k+1}), i.e., (k+1) copies of (|
\psi>) can be transformed to (k+1) copies of (| \phi>) with probability one by
LOCC but (| \psi> ^{\otimes n}\nleftrightarrow | \phi> ^{\otimes n} \forall
n\leq k). We call such states \emph{k}-copy LOCC incomparable. We provide a
necessary condition for a given pair of states to be \emph{k}-copy LOCC
incomparable for some \emph{k}. We also show that there exist states that are
neither \emph{k}-copy LOCC incomparable for any \emph{k} nor catalyzable even
with multiple copies. We call such states strongly incomparable. We give a
sufficient condition for strong incomparability.
We demonstrate that the optimal probability of a conclusive transformation
involving many copies, (p_{max}(| \psi> ^{\otimes m}\to | \phi> ^{\otimes m}))
can decrease exponentially with the number of source states (m), even if the
source state has \emph{more} entropy of entanglement.Comment: Latex, 9 pages, 1 figur
