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1 ,..., 2 k 1 that are roughly equally spaced between the
first and the last layer. These layers, and the first and the last layers, shall be
untouched and shall be called pristine layers .
(
)
Select
2 k
1
layers
In all the other layers, retain only those edges connecting vertex i of this layer to
vertex i of the next.
This restriction effectively makes the graph similar to an ABP with 2 k
+
1 layers. Let
the polynomial computed by the restricted ABP be IMM n , d (
. Since IMM n , d was
obtained by just setting some variables of IMM n , d to zero, the dimension of shifted
partial derivatives of IMM n , d can only be smaller than that of IMM n , d . Similar to
Observation 60, we have the following observation.
x
)
Observation 61 For every choice of k edges from odd-numbered pristine layers,
there is a unique source-sink path that passes through them.
In other words, for any choice of k variables chosen by picking one from each
odd-numbered pristine layer, then the k-th order partial derivative of IMM n , d
with
respect to these k variables is a nonzero monomial.
Once again, we can lower bound the dimension of shifted partial derivatives of
IMM n , d by a monomial counting problem. Similar to the earlier case, [ FLMS13 ]
show that the monomials thus obtained are far from one another. We state their main
lemma below without proof.
Lemma 62 [ FLMS13 ] There are at least n k / 2
monomials of IMM n , d
of pairwise
n
distance at least
4 .
Again, using Lemma 55 and standard binomial coefficient estimates, this implies
that the shifted partial derivatives of IMM n , d
is almost as large as the trivial upper
bound.
= d for a sufficiently small ∂ >
Theorem 63 [ FLMS13 ] Let k
0 and
be an
N
+
integer such that n 1 / 16
n 1 / 4 where N is the number of variables IMM n , d
depends on. Then,
dim
dim
˃ = k IMM n , d
˃ = k IMM n , d
n k / 2
N
⊤⊤
+
= ˇ
·
.
Combining with Corollary 46, we get the lower bound of [ FLMS13 ].
[ O ( d ) ] [ d ]
Theorem 64 [ FLMS13 ] Any
circuit com p uting IMM n , d , with
(ˇ( d log n
n ʻ for a sufficiently small ʻ >
d
0 , has top fan-in exp
))
.
Similar to [ KSS13 ], the above result also implies n ˇ( log n ) lower bounds for regular
formulas computing IMM n , d .
 
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