DOI: 10.68381/jca22039 ISSN: 0944-6532

Monge-Ampère Type Function Splittings

David F. Miller

Given convex

u\in C(\bar{\Omega}) u ∈ C ( Ω ˉ )
with Monge-Ampère measure
Mu M u
, and finite Borel measures
\mu μ
and
\nu ν
satisfying
\mu + \nu = Mu μ + ν = M u
, consider the problem of determining a ‘splitting’
u=v+w u = v + w
for
u u
where
v,w \in C(\bar{\Omega}) v , w ∈ C ( Ω ˉ )
are convex functions satisfying
Mv=\mu M v = μ
,
Mw=\nu M w = ν
, so that
Mu=M(v+w)=Mv + Mw M u = M ( v + w ) = M v + M w
. It is shown that although this problem is not in general solvable, a best
L^p L p
approximation
v^\ast+w^\ast v ∗ + w ∗
for
u u
may always be found. In particular, letting
U={\rm sup}_{(v,w)\in {\cal F}}~(v+w) U = s u p ( v , w ) ∈ F   ( v + w )
, there exist optimal sums
v^\ast+w^\ast v ∗ + w ∗
achieving
{\rm inf}_{(v,w)\in {\cal F}}~\|u-(v+w)\|_p i n f ( v , w ) ∈ F   ∥ u − ( v + w ) ∥ p
and
{\rm inf}_{(v,w)\in {\cal F}}~\|U-(v+w)\|_p i n f ( v , w ) ∈ F   ∥ U − ( v + w ) ∥ p
,
p\ge 1 p ≥ 1
, for appropriately constrained classes
{\cal F} F
of feasible pairs
(v,w) ( v , w )
of convex functions satisfying
Mv=\mu M v = μ
,
Mw=\nu M w = ν
and
v+w=u v + w = u
on
\partial\Omega ∂ Ω
. Moreover,
U U
may be written as
U=\bar{v}+\bar{w} U = v ˉ + w ˉ
within
\bar{\Omega} Ω ˉ
,
(\bar{v},\bar{w})\in {\cal F} ( v ˉ , w ˉ ) ∈ F
. The analysis depends upon basic properties of convex functions and the measures they determine. We also consider the related problem of characterizing functions
u\in W^{2,n}(\Omega) u ∈ W 2 , n ( Ω )
which may be realized as differences
u=v-w u = v − w
of convex functions
v,w\in W^{2,n}(\Omega) v , w ∈ W 2 , n ( Ω )
with
Mu=Mv-Mw M u = M v − M w
. Here
Mu M u
is the signed measure defined by
dMu={\rm det}~D^2u\,dx d M u = d e t   D 2 u   d x
. Letting
U^-={\rm sup}_{(v,w)\in {\cal F}}(v-w) U − = s u p ( v , w ) ∈ F ( v − w )
and
U_-={\rm inf}_{(v,w)\in {\cal F}}(v-w) U − = i n f ( v , w ) ∈ F ( v − w )
, we show that optimal differences
v^\ast-w^\ast v ∗ − w ∗
exist for the problems
{\rm inf}_{(v,w)\in {\cal F}}~\|u-(v-w)\|_p i n f ( v , w ) ∈ F   ∥ u − ( v − w ) ∥ p
,
{\rm inf}_{(v,w)\in {\cal F}}~\|U^--(v-w)\|_p i n f ( v , w ) ∈ F   ∥ U − − ( v − w ) ∥ p
and
{\rm inf}_{(v,w)\in {\cal F}}~\|U_- -(v-w)\|_p i n f ( v , w ) ∈ F   ∥ U − − ( v − w ) ∥ p
. Also,
U^-=v^--w^- U − = v − − w −
and
U_-=v_--w_- U − = v − − w −
for appropriate pairs
(v^-,w^-),(v_-,w_-)\in {\cal F} ( v − , w − ) , ( v − , w − ) ∈ F
. Finally, the relaxed problem of finding
v+w=u v + w = u
for general
Mv M v
and
Mw M w
with
Mv+Mw = Mu M v + M w = M u
(no fixed
\mu μ
and
\nu ν
), is considered. Topological properties of the collection of these relaxed splitting pairs
(v,w) ( v , w )
, and those for the unrelaxed problem, for a given
u u
, are developed.