Introduction

For a real normed space XX, let S⊆XS\subseteq X and x∈Xx\in X. Define I ⁣(S,x)≔⋂a∈SB ⁣(a,∥x−a∥),Iˉ ⁣(S,x)≔⋂a∈SBˉ ⁣(a,∥x−a∥)\fc I{S,x}\ceq\bigcap_{a\in S}\fc B{a,\V{x-a}},\qquad \fc{\bar I}{S,x}\ceq\bigcap_{a\in S}\fc{\bar B}{a,\V{x-a}} (1)(1) (specially, I ⁣(∅,x)=Iˉ ⁣(∅,x)=X\fc I{\varnothing,x}=\fc{\bar I}{\varnothing,x}=X), where B ⁣(a,r)≔{y∈X  |  ∥y−a∥<r},Bˉ ⁣(a,r)≔{y∈X  |  ∥y−a∥≤r}\fc B{a,r}\ceq\set{y\in X}{\V{y-a}<r},\qquad \fc{\bar B}{a,r}\ceq\set{y\in X}{\V{y-a}\le r} denote the respectively open and closed ball centered at aa with radius rr, and P ⁣(S)≔{x∈X  |  I ⁣(S,x)=∅},Pˉ ⁣(S)≔{x∈X  |  Iˉ ⁣(S,x)={x}}.\fc PS\ceq\set{x\in X}{\fc I{S,x}=\varnothing},\qquad \fc{\bar P}S\ceq\set{x\in X}{\fc{\bar I}{S,x}=\B x}. (2)(2) This article studies the four properties: P⊃:conv‾⁡S⊆P ⁣(S),Pˉ⊃:conv‾⁡S⊆Pˉ ⁣(S),P_\supset:\qquad \opn{\overline{conv}}S\subseteq\fc PS,\qquad \bar P_\supset:\qquad \opn{\overline{conv}}S\subseteq\fc{\bar P}S, P⊂:P ⁣(S)⊆conv‾⁡S,Pˉ⊂:Pˉ ⁣(S)⊆conv‾⁡S,P_\subset:\qquad \fc PS\subseteq\opn{\overline{conv}}S,\qquad \bar P_\subset:\qquad \fc{\bar P}S\subseteq\opn{\overline{conv}}S, where conv‾⁡S\opn{\overline{conv}}S denotes the closed convex hull of SS.

Based on the property of SS, the four properties multiply to sixteen properties: P⊃,⊂fP_{\supset,\subset}^\mrm f means P⊃,⊂P_{\supset,\subset} holds for all finite S⊆XS\subseteq X; P⊃,⊂cP_{\supset,\subset}^\mrm c means P⊃,⊂P_{\supset,\subset} holds for all compact S⊆XS\subseteq X; P⊃,⊂bP_{\supset,\subset}^\mrm b means P⊃,⊂P_{\supset,\subset} holds for all bounded S⊆XS\subseteq X; P⊃,⊂aP_{\supset,\subset}^\mrm a means P⊃,⊂P_{\supset,\subset} holds for all S⊆XS\subseteq X; and similarly for Pˉ⊃,⊂f,c,b,a\bar P_{\supset,\subset}^{\mrm f,\mrm c,\mrm b,\mrm a}.

We assume X≠{0}X\ne\B0 throughout. For S=∅S=\varnothing, all sixteen properties then hold trivially, so proofs involving SS may assume it is nonempty. If X={0}X=\B0 and empty sets of ideal points are allowed, Pˉ⊂\bar P_\subset fails for S=∅S=\varnothing.

Some of the properties are stronger than others. First, all finite sets are compact, and all compact sets are bounded. Second, we can easily see that Pˉ ⁣(S)⊆P ⁣(S)\fc{\bar P}S\subseteq\fc PS. Therefore, P⊃,⊂a⇒P⊃,⊂b⇒P⊃,⊂c⇒P⊃,⊂f,Pˉ⊃,⊂a⇒Pˉ⊃,⊂b⇒Pˉ⊃,⊂c⇒Pˉ⊃,⊂f,P_{\supset,\subset}^\mrm a\Rightarrow P_{\supset,\subset}^\mrm b\Rightarrow P_{\supset,\subset}^\mrm c\Rightarrow P_{\supset,\subset}^\mrm f,\qquad \bar P_{\supset,\subset}^\mrm a\Rightarrow \bar P_{\supset,\subset}^\mrm b\Rightarrow \bar P_{\supset,\subset}^\mrm c\Rightarrow \bar P_{\supset,\subset}^\mrm f, Pˉ⊃f,c,b,a⇒P⊃f,c,b,a,P⊂f,c,b,a⇒Pˉ⊂f,c,b,a.\bar P_\supset^{\mrm f,\mrm c,\mrm b,\mrm a}\Rightarrow P_\supset^{\mrm f,\mrm c,\mrm b,\mrm a},\qquad P_\subset^{\mrm f,\mrm c,\mrm b,\mrm a}\Rightarrow \bar P_\subset^{\mrm f,\mrm c,\mrm b,\mrm a}.

The established characterizations and the remaining gaps are summarized in the following table:

Property Characterization
P⊃f,c,bP_\supset^{\mrm f,\mrm c,\mrm b}, Pˉ⊂b\bar P_\subset^\mrm b inner product space or plane
Pˉ⊃f,c,b\bar P_\supset^{\mrm f,\mrm c,\mrm b}, P⊂bP_\subset^\mrm b inner product space or strictly convex plane
P⊃aP_\supset^\mrm a inner product space or plane with balanced tangent chords
Pˉ⊃a\bar P_\supset^\mrm a inner product space or strictly convex plane with balanced tangent chords
P⊂f,cP_\subset^{\mrm f,\mrm c} finite dimensions: inner product space or strictly convex plane; infinite dimensions: open
Pˉ⊂f,c\bar P_\subset^{\mrm f,\mrm c} finite dimensions: inner product space or plane; infinite dimensions: open
P⊂aP_\subset^\mrm a Hilbert space or strictly convex plane
Pˉ⊂a\bar P_\subset^\mrm a Hilbert space or plane

Here, a plane means a two-dimensional real normed space. See Definition 24 for balanced tangent chords.

If we only consider the characterizations of spaces satisfying both P⊃f,c,b,aP_\supset^{\mrm f,\mrm c,\mrm b,\mrm a} and P⊂f,c,b,aP_\subset^{\mrm f,\mrm c,\mrm b,\mrm a} (or both Pˉ⊃f,c,b,a\bar P_\supset^{\mrm f,\mrm c,\mrm b,\mrm a} and Pˉ⊂f,c,b,a\bar P_\subset^{\mrm f,\mrm c,\mrm b,\mrm a}), then there are no open gaps:

Property Characterization
P⊃f,c,b∧P⊂f,c,bP_\supset^{\mrm f,\mrm c,\mrm b}\land P_\subset^{\mrm f,\mrm c,\mrm b}, Pˉ⊃f,c,b∧Pˉ⊂f,c,b\bar P_\supset^{\mrm f,\mrm c,\mrm b}\land\bar P_\subset^{\mrm f,\mrm c,\mrm b} inner product space or strictly convex plane
P⊃a∧P⊂aP_\supset^\mrm a\land P_\subset^\mrm a, Pˉ⊃a∧Pˉ⊂a\bar P_\supset^\mrm a\land\bar P_\subset^\mrm a Hilbert space or strictly convex plane with balanced tangent chords

In the following sections, a vector space is assumed to be over the real numbers unless otherwise specified.

Background

The background of this study is in economics, where preference relations and Pareto efficiency are studied.

My motivation of studying the properties originates from my previous article on voting systems, dates back to more than three years ago.

In the end of that article, I used an example of this preference relation: an agent prefers points nearer to the ideal point. Mathematically, it says that in the metric space (X,d)\p{X,d}, for an agent with ideal point a∈Xa\in X, y⪰xy\succeq x iff d ⁣(y,a)≤d ⁣(x,a)\fc d{y,a}\le\fc d{x,a}. Such a preference relation is what I call a distance preference relation.

That article also focuses on the concept of Pareto efficiency, or particularly, weak Pareto efficiency. Suppose that we have a set SS of agents, and we denote the preference relation of each agent a∈Sa\in S as ⪰a\succeq_a, and suppose all preference relations are complete over a space XX. Then, we say y∈Xy\in X is a strong Pareto improvement of x∈Xx\in X iff ∀a∈S:y≻ax\forall a\in S:y\succ_a x; yy is a weak Pareto improvement of xx iff ∀a∈S:y⪰ax\forall a\in S:y\succeq_a x. Note the terminological quirk: a strong Pareto optimal has no weak Pareto improvement, and a weak Pareto optimal has no strong Pareto improvement. Note that neither concept is the actual definition of Pareto improvement used in economics, which says that yy is an (economic) Pareto improvement of xx iff ∀a∈S:y⪰ax\forall a\in S:y\succeq_a x and ∃a∈S:y≻ax\exists a\in S:y\succ_a x. However, since the weak Pareto improvement and the strong Pareto improvement have simpler mathematical definitions, they will be the focus of this article.

The set of all strong Pareto improvements of xx is denoted as I ⁣(S,x)\fc I{S,x}. We say xx is weak Pareto optimal iff I ⁣(S,x)=∅\fc I{S,x}=\varnothing, and the weak Pareto set is the set of all weak Pareto optimals, denoted as P ⁣(S)\fc PS. Similarly, we can denote the set of weak Pareto improvements as Iˉ ⁣(S,x)\fc{\bar I}{S,x}. We say xx is strong Pareto optimal iff Iˉ ⁣(S,x)={x}\fc{\bar I}{S,x}=\B x, and the strong Pareto set Pˉ ⁣(S)\fc{\bar P}S is the set of all strong Pareto optimals. When XX is a metric space and the preference relations are distance preference relations, the definitions of I ⁣(S,x)\fc I{S,x}, Iˉ ⁣(S,x)\fc{\bar I}{S,x}, P ⁣(S)\fc PS, and Pˉ ⁣(S)\fc{\bar P}S match exactly with the definitions in Equation 1 and Equation 2.

In the end of my previous article referenced here, there was an example taking XX as a Euclidean plane as an example. There was a figure visualizing the weak Pareto sets for finite numbers of agents, but I never explained how I derived the weak Pareto sets. From the figure, it seems that the weak Pareto set is the convex hull of the ideal points of the agents. I originally planned to prove this in that article, but it turned out that it was too difficult, so I just left it without justification.


Questions of the same type were raised and answered by Durier (1987). In his paper, he called Pˉ ⁣(S)\fc{\bar P}S the strictly efficient points, P ⁣(S)\fc PS the weakly efficient points, and the economic Pareto set the efficient points. He also studied another type of optimal points called the properly efficient points.

Preliminaries

Theorem 1. If a normed space is not strictly convex, then it does not satisfy P⊂fP_\subset^\mrm f.

Proof

Let XX be a normed space that is not strictly convex. Its unit sphere contains a nontrivial line segment, so there exist distinct unit vectors u,v∈Xu,v\in X such that ∥u+v∥=2\V{u+v}=2. Set S≔{u,−v}S\ceq\B{u,-v}.

Suppose for contradiction that y∈I ⁣(S,0)=B ⁣(u,1)∩B ⁣(−v,1).y\in\fc I{S,0}=\fc B{u,1}\cap\fc B{-v,1}. We then have ∥y−u∥<1\V{y-u}<1 and ∥y−(−v)∥<1\V{y-\p{-v}}<1. The triangle inequality gives 2=∥u+v∥≤∥u−y∥+∥y−(−v)∥<1+1=2,2=\V{u+v}\le\V{u-y}+\V{y-\p{-v}}<1+1=2, a contradiction. Therefore, I ⁣(S,0)=∅\fc I{S,0}=\varnothing, so 0∈P ⁣(S)0\in\fc PS.

Suppose for contradiction that 0∈conv‾⁡S={λu−(1−λ)v  |  λ∈[0,1]}.0\in\opn{\overline{conv}}S=\set{\lmd u-\p{1-\lmd}v}{\lmd\in\b{0,1}}. Then there exists λ∈[0,1]\lmd\in\b{0,1} such that 0=λu−(1−λ)v0=\lmd u-\p{1-\lmd}v. Taking the norm on both sides gives 0=∥λu−(1−λ)v∥≥λ∥u∥−(1−λ)∥v∥=2λ−1,0=\V{\lmd u-\p{1-\lmd}v}\ge\lmd\V u-\p{1-\lmd}\V v=2\lmd-1, 0=∥λu−(1−λ)v∥≥(1−λ)∥v∥−λ∥u∥=1−2λ.0=\V{\lmd u-\p{1-\lmd}v}\ge\p{1-\lmd}\V v-\lmd\V u=1-2\lmd. These two inequalities imply λ=1/2\lmd=1/2. This then gives 0=u/2−v/20=u/2-v/2, which implies u=vu=v. This contradicts with u≠vu\ne v. Therefore, 0∉conv‾⁡S0\notin\opn{\overline{conv}}S.

Thus, we have found a counterexample to P⊂fP_\subset^\mrm f. □\square

Theorem 2. If a normed space is not strictly convex, then it does not satisfy Pˉ⊃f\bar P_\supset^\mrm f.

Proof

Let XX be a normed space that is not strictly convex. Its unit sphere contains a nontrivial line segment, so there exist distinct unit vectors u,v∈Xu,v\in X such that ∥u+v∥=2\V{u+v}=2. Set S≔{u,−v}S\ceq\B{u,-v} and x≔(u−v)/2x\ceq\p{u-v}/2. Obviously we have x∈conv‾⁡Sx\in\opn{\overline{conv}}S. We have ∥x−u∥=∥−u−v2∥=1,∥x+v∥=∥u+v2∥=1.\V{x-u}=\V{\fr{-u-v}2}=1,\qquad \V{x+v}=\V{\fr{u+v}2}=1.

Now set y≔u−vy\ceq u-v. Because u,vu,v are distinct vectors, we have y≠xy\ne x. We also have ∥y−u∥=∥−v∥=1≤∥x−u∥,∥y+v∥=∥u∥=1≤∥x+v∥.\V{y-u}=\V{-v}=1\le\V{x-u},\qquad \V{y+v}=\V u=1\le\V{x+v}. Therefore, y∈Iˉ ⁣(S,x)y\in\fc{\bar I}{S,x}. We have found a counterexample to Pˉ⊃f\bar P_\supset^\mrm f. □\square

Theorem 3. Let XX be a strictly convex space and S⊆XS\subseteq X. Then, P ⁣(S)=Pˉ ⁣(S)\fc PS=\fc{\bar P}S.

Proof

We obviously have Pˉ ⁣(S)⊆P ⁣(S)\fc{\bar P}S\subseteq\fc PS, so it is sufficient to prove P ⁣(S)⊆Pˉ ⁣(S)\fc PS\subseteq\fc{\bar P}S.

Let x∈X∖Pˉ ⁣(S)x\in X\setminus\fc{\bar P}S. Then there exists y∈Iˉ ⁣(S,x)∖{x}y\in\fc{\bar I}{S,x}\setminus\B x, which satisfies ∀a∈S:∥y−a∥≤∥x−a∥\forall a\in S:\V{y-a}\le\V{x-a}. Let y′≔(x+y)/2y'\ceq\p{x+y}/2. For each a∈Sa\in S, x≠ax\ne a because otherwise ∥y−a∥≤∥x−a∥=0\V{y-a}\le\V{x-a}=0 would force y=xy=x. If ∥y−a∥<∥x−a∥\V{y-a}<\V{x-a}, the triangle inequality gives ∥y′−a∥<∥x−a∥\V{y'-a}<\V{x-a}. If the two norms are equal, their vectors are distinct, so strict convexity gives ∥y′−a∥=∥12(x−a)+12(y−a)∥<12∥x−a∥+12∥y−a∥≤∥x−a∥.\V{y'-a}=\V{\fr12\p{x-a}+\fr12\p{y-a}} <\fr12\V{x-a}+\fr12\V{y-a}\le\V{x-a}. Therefore, y′∈I ⁣(S,x)y'\in\fc I{S,x}, so x∉P ⁣(S)x\notin\fc PS. □\square

Other preliminaries

Definition 4. Let XX be a normed space. The (open) Voronoi cell w.r.t. xx of y∈Xy\in X is the set Dy,x≔{a∈X  |  ∥y−a∥<∥x−a∥}.D_{y,x}\ceq\set{a\in X}{\V{y-a}<\V{x-a}}. Also denote Dy≔Dy,0D_y\ceq D_{y,0}, called the Voronoi cell of yy. Similarly, the closed Voronoi cell w.r.t. xx of y∈Xy\in X is Dˉy,x≔{a∈X  |  ∥y−a∥≤∥x−a∥},\bar D_{y,x}\ceq\set{a\in X}{\V{y-a}\le\V{x-a}}, and denote Dˉy≔Dˉy,0\bar D_y\ceq\bar D_{y,0}.

Theorem 5. We can equivalently rewrite P⊃f,aP_\supset^{\mrm f,\mrm a} and Pˉ⊃f,a\bar P_\supset^{\mrm f,\mrm a} as follows: P⊃f:∀y∈X:0∉conv⁡Dy,P⊃a:∀y∈X:0∉conv‾⁡Dy,Pˉ⊃f:∀y∈X∖{0}:0∉conv⁡Dˉy,Pˉ⊃a:∀y∈X∖{0}:0∉conv‾⁡Dˉy.\begin{align*} P_\supset^\mrm f:\qquad&\forall y\in X:0\notin\opn{conv}D_y,\\ P_\supset^\mrm a:\qquad&\forall y\in X:0\notin\opn{\overline{conv}}D_y,\\ \bar P_\supset^\mrm f:\qquad&\forall y\in X\setminus\B0:0\notin\opn{conv}\bar D_y,\\ \bar P_\supset^\mrm a:\qquad&\forall y\in X\setminus\B0:0\notin\opn{\overline{conv}}\bar D_y.\\ \end{align*}

Proof

By Definition 4, we have y∈I ⁣(S,x)⇔S⊆Dy,xy\in\fc I{S,x}\Leftrightarrow S\subseteq D_{y,x}. Then, P⊃P_\supset can be rewritten as P⊃:(∃y∈X:S⊆Dy,x)⇒x∉conv‾⁡S.P_\supset:\qquad\p{\exists y\in X:S\subseteq D_{y,x}}\Rightarrow x\notin\opn{\overline{conv}}S. Translate S,x,yS,x,y by −x-x, and rename the translated set SS. Since translation preserves finiteness, boundedness, and closed convex hulls, this gives P⊃:(∃y∈X:S⊆Dy)⇒0∉conv‾⁡S.P_\supset:\qquad\p{\exists y\in X:S\subseteq D_y}\Rightarrow 0\notin\opn{\overline{conv}}S. Using some first-order logic, we can rewrite this as P⊃:∀y∈X:(S⊆Dy⇒0∉conv‾⁡S).P_\supset:\qquad\forall y\in X:\p{S\subseteq D_y\Rightarrow 0\notin\opn{\overline{conv}}S}. Now dictate it to be true for all finite, bounded, or arbitrary SS, and we get P⊃f,b,a:∀y∈X:0∉⋃S⊆Dyf,b,aconv‾⁡S.P_\supset^{\mrm f,\mrm b,\mrm a}:\qquad\forall y\in X: 0\notin\bigcup_{\substack{S\subseteq D_y\\\mrm f,\mrm b,\mrm a}}\opn{\overline{conv}}S. By the same argument, we have Pˉ⊃f,b,a:∀y∈X∖{0}:0∉⋃S⊆Dˉyf,b,aconv‾⁡S.\bar P_\supset^{\mrm f,\mrm b,\mrm a}:\qquad\forall y\in X\setminus\B0: 0\notin\bigcup_{\substack{S\subseteq\bar D_y\\\mrm f,\mrm b,\mrm a}}\opn{\overline{conv}}S.

One of the equivalent definitions of the convex hull is the set of all convex combinations of finitely many points in the set. Notice that for finite SS, conv‾⁡S\opn{\overline{conv}}S is exactly the set of convex combinations of SS. Therefore, we have ⋃S⊆Dyfiniteconv‾⁡S=conv⁡Dy.\bigcup_{\substack{S\subseteq D_y\\\mrm{finite}}}\opn{\overline{conv}}S=\opn{conv}D_y. Thus, P⊃f:∀y∈X:0∉conv⁡Dy.P_\supset^\mrm f:\qquad\forall y\in X:0\notin\opn{conv}D_y.

When SS can be any set such that S⊆DyS\subseteq D_y, one case is to have S=DyS=D_y. We then have ⋃S⊆Dyconv‾⁡S=conv‾⁡Dy.\bigcup_{S\subseteq D_y}\opn{\overline{conv}}S=\opn{\overline{conv}}D_y. Thus, P⊃a:∀y∈X:0∉conv‾⁡Dy.P_\supset^\mrm a:\qquad\forall y\in X:0\notin\opn{\overline{conv}}D_y.

By the same arguments, we have Pˉ⊃f:∀y∈X∖{0}:0∉conv⁡Dˉy,Pˉ⊃a:∀y∈X∖{0}:0∉conv‾⁡Dˉy.\begin{align*} \bar P_\supset^\mrm f:\qquad\forall y\in X\setminus\B0:0\notin\opn{conv}\bar D_y,\\ \bar P_\supset^\mrm a:\qquad\forall y\in X\setminus\B0:0\notin\opn{\overline{conv}}\bar D_y. \end{align*} □\square

Definition 6. Let XX be a normed space. Then, the subdifferential at x∈Xx\in X is defined as J ⁣(x)≔{f∈X∗  |  ∥f∥≤1,f ⁣(x)=∥x∥}.\fc Jx\ceq\set{f\in X^*}{\V f\le1,\fc fx=\V x}. An element of J ⁣(x)\fc Jx is called a subgradient at xx. Moreover, XX is said to be smooth at xx if there is a unique subgradient at xx, and we say XX is smooth if it is smooth at every nonzero point.

Theorem 7. Let XX be a normed space. For any x∈Xx\in X, J ⁣(x)\fc Jx is a nonempty weak*-compact convex subset of X∗X^*, and it has the following properties: ∀t∈R∖{0}:J ⁣(tx)=J ⁣(x)sgn⁡t,\forall t\in\bR\setminus\B0:\fc J{tx}=\fc Jx\sgn t, (3)(3) ∀f∈J ⁣(x),v∈X:∥x+v∥≥∥x∥+f ⁣(v).\forall f\in\fc Jx,v\in X:\V{x+v}\ge\V x+\fc fv. (4)(4)

Proof

When x=0x=0, J ⁣(x)\fc Jx is the closed unit ball of X∗X^*. It is weak*-compact by the Banach–Alaoglu theorem. All other properties are trivial. From now on, we assume x≠0x\ne0.

To prove that J ⁣(x)\fc Jx is nonempty, we define a linear functional f0f_0 on the one-dimensional subspace Rx\bR x of XX as f0 ⁣(tx)≔t∥x∥\fc{f_0}{tx}\ceq t\V x. We can easily find that this functional has norm 11. By the norm-preserving Hahn–Banach continuous extension theorem, we can extend it to a linear functional f∈X∗f\in X^* with ∥f∥=1\V f=1. We can easily see that f∈J ⁣(x)f\in\fc Jx, so J ⁣(x)\fc Jx is nonempty.

To prove that J ⁣(x)\fc Jx is convex, let f1,f2∈J ⁣(x)f_1,f_2\in\fc Jx and λ∈[0,1]\lmd\in\b{0,1}. By definition of J ⁣(x)\fc Jx, we can easily see that λf1+(1−λ)f2∈J ⁣(x)\lmd f_1+\p{1-\lmd}f_2\in\fc Jx.

To prove that J ⁣(x)\fc Jx is weak*-compact, first note that ⋅ ⁣(x)\fc\cdot x is a weak*-continuous linear functional on X∗X^* by the definition of the weak* topology. Its preimage of any closed set on R\bR is then weak*-closed. Then, from J ⁣(x)={f∈X∗  |  ∥f∥≤1}∩{f∈X∗  |  f ⁣(x)=∥x∥}=J ⁣(0)∩(⋅ ⁣(x))−1 ⁣({∥x∥}),\fc Jx=\set{f\in X^*}{\V f\le1}\cap\set{f\in X^*}{\fc fx=\V x} =\fc J0\cap\fc{\p{\fc\cdot x}^{-1}}{\B{\V x}}, we see that J ⁣(x)\fc Jx is the intersection of a weak*-compact set and a weak*-closed set, so J ⁣(x)\fc Jx is weak*-compact.

Equation 3 is easy to verify from the definition of J ⁣(x)\fc Jx.

To prove Equation 4, write ∥x∥+f ⁣(v)=f ⁣(x)+f ⁣(v)=f ⁣(x+v)≤∣f ⁣(x+v)∣≤∥f∥∥x+v∥=∥x+v∥.\V x+\fc fv=\fc fx+\fc fv=\fc f{x+v}\le\v{\fc f{x+v}}\le\V f\V{x+v}=\V{x+v}.

All properties have been proven. □\square

Definition 8. Let XX be a vector space, v∈Xv\in X, and f:D→Rf:D\to\bR be a function defined on a subset D⊆XD\subseteq X. The directional derivative of ff in the direction of vv is a function ∂vf:D′→R\partial_v f:D'\to\bR defined as ∂vf ⁣(x)≔lim⁡t→0+f ⁣(x+tv)−f ⁣(x)t.\partial_v\fc fx\ceq\lim_{t\to0^+}\fr{\fc f{x+tv}-\fc fx}t. The domain D′D' is all points where this expression makes sense (i.e., x∈Xx\in X such that 00 is a limit point of {t>0  |  x+tv∈D}\set{t>0}{x+tv\in D}) and the limit exists.

Theorem 9. Let XX be a normed space and v∈Xv\in X. Then, ∂v∥⋅∥\partial_v\V\cdot is defined on all of XX, and it satisfies ∀x∈X,t>0:∂v∥x∥=max⁡f∈J ⁣(x)f ⁣(v)≤∥x+tv∥−∥x∥t.\forall x\in X,t>0:\partial_v\V x=\max_{f\in\fc Jx}\fc fv \le\fr{\V{x+tv}-\V x}t. (5)(5)

Proof

For fixed x∈Xx\in X, define g:(0,+∞)×X→Rg:\p{0,+\infty}\times X\to\bR as g ⁣(t,w)≔∥x+tw∥−∥x∥t.\fc g{t,w}\ceq\fr{\V{x+tw}-\V x}t. By Definition 8, we have ∂v∥x∥=g ⁣(0+,v)\partial_v\V x=\fc g{0^+,v}.

First prove that g ⁣(0+,w)\fc g{0^+,w} exists. By the triangle inequality, when t′>t>0t'>t>0, we have g ⁣(t′,w)−g ⁣(t,w)=∥x+t′w∥−∥x∥t′−∥x+tw∥−∥x∥t≥∥x+t′w∥−∥x∥t′−∥tt′x+tw∥+∥x−tt′x∥−∥x∥t=0,\begin{align*} \fc g{t',w}-\fc g{t,w} &=\fr{\V{x+t'w}-\V x}{t'}-\fr{\V{x+tw}-\V x}t\\ &\ge\fr{\V{x+t'w}-\V x}{t'}-\fr{\V{\fr t{t'}x+tw}+\V{x-\fr t{t'}x}-\V x}t\\ &=0, \end{align*} so g ⁣(⋅,w)\fc g{\cdot,w} is a monotonically non-decreasing function on (0,+∞)\p{0,+\infty}. Also, we have g ⁣(t,w)≥∥x+tw∥−∥x+tw∥−∥−tw∥t=−∥w∥,\fc g{t,w}\ge\fr{\V{x+tw}-\V{x+tw}-\V{-tw}}t=-\V w, so g ⁣(⋅,w)\fc g{\cdot,w} is bounded below. Therefore, g ⁣(0+,w)\fc g{0^+,w} exists.

To prove that ∀t>0:∂v∥x∥≤(∥x+tv∥−∥x∥)/t\forall t>0:\partial_v\V x\le\p{\V{x+tv}-\V x}/t, note that this statement is exactly g ⁣(0+,v)≤g ⁣(t,v)\fc g{0^+,v}\le\fc g{t,v}, which follows from the monotonicity of g ⁣(⋅,v)\fc g{\cdot,v}.

Then prove that max⁡f ⁣(v)\max\fc fv exists. This follows by maximizing the weak*-continuous function f↦f ⁣(v)f\mapsto\fc fv over the nonempty weak*-compact set J ⁣(x)\fc Jx.

By Equation 4, we have ∥x+tv∥≥∥x∥+f ⁣(tv)\V{x+tv}\ge\V x+\fc f{tv}, which simplifies to g ⁣(t,v)≥f ⁣(v)\fc g{t,v}\ge\fc fv. Maximize over f∈J ⁣(x)f\in\fc Jx and taking infimum over t∈(0,+∞)t\in\p{0,+\infty} on both sides to get g ⁣(0+,v)≥max⁡f∈J ⁣(x)f ⁣(v).\fc g{0^+,v}\ge\max_{f\in\fc Jx}\fc fv.

Now we will explicitly construct a linear functional f0∈X∗f_0\in X^* such that g ⁣(0+,v)=f0 ⁣(v)\fc g{0^+,v}=\fc{f_0}v and later show that f0∈J ⁣(x)f_0\in\fc Jx. To construct it, we will use the Hahn–Banach dominated extension theorem, for which we need to construct a sublinear functional as the dominating functional. For that we use g ⁣(0+,⋅)\fc g{0^+,\cdot}.

First, we prove that g ⁣(0+,⋅)\fc g{0^+,\cdot} is sublinear. The positive homogeneity, i.e., ∀α>0:g ⁣(0+,αw)=αg ⁣(0+,w)\forall \alp>0:\fc g{0^+,\alp w}=\alp\fc g{0^+,w}, is obvious from the definition. For subadditivity, convexity gives ∥x+t(w+w′)∥≤12∥x+2tw∥+12∥x+2tw′∥.\V{x+t\p{w+w'}}\le\fr12\V{x+2tw}+\fr12\V{x+2tw'}. Subtract ∥x∥\V x, divide by t>0t>0, and take t→0+t\to0^+ to obtain g ⁣(0+,w+w′)≤g ⁣(0+,w)+g ⁣(0+,w′)\fc g{0^+,w+w'}\le\fc g{0^+,w}+\fc g{0^+,w'}.

Then, define a linear functional h:Rv→Rh:\bR v\to\bR defined as h ⁣(αv)≔αg ⁣(0+,v)\fc h{\alp v}\ceq\alp\fc g{0^+,v}. We can check that ∀α∈R:h ⁣(αv)≤g ⁣(0+,αv)\forall\alp\in\bR:\fc h{\alp v}\le\fc g{0^+,\alp v} so that hh is dominated by g ⁣(0+,⋅)\fc g{0^+,\cdot} on Rv\bR v. The check is trivial for α≥0\alp\ge0. For α<0\alp<0, noticing that 0=g ⁣(0+,0)≤g ⁣(0+,v)+g ⁣(0+,−v)0=\fc g{0^+,0}\le\fc g{0^+,v}+\fc g{0^+,-v}, we have h ⁣(αv)=αg ⁣(0+,v)≤−αg ⁣(0+,−v)=g ⁣(0+,αv).\fc h{\alp v}=\alp\fc g{0^+,v}\le-\alp\fc g{0^+,-v}=\fc g{0^+,\alp v}.

We can thus apply the Hahn–Banach dominated extension theorem to extend hh to a linear functional f0∈X∗f_0\in X^* such that f0 ⁣(v)=h ⁣(v)=g ⁣(0+,v)\fc{f_0}v=\fc hv=\fc g{0^+,v} and that f0f_0 is dominated by g ⁣(0+,⋅)\fc g{0^+,\cdot} on all of XX.

Now we need to show that f0∈J ⁣(x)f_0\in\fc Jx. For any y∈Xy\in X, we have f0 ⁣(y−x)≤g ⁣(0+,y−x)≤g ⁣(1,y−x)=∥y∥−∥x∥,\fc{f_0}{y-x}\le\fc g{0^+,y-x}\le\fc g{1,y-x}=\V y-\V x, (6)(6) where the first inequality is because f0f_0 is dominated by g ⁣(0+,⋅)\fc g{0^+,\cdot} and the second inequality is because g ⁣(⋅,y−x)\fc g{\cdot,y-x} is monotonically non-decreasing.

Substitute yy with 00 in Equation 6 to get f0 ⁣(x)≥∥x∥\fc{f_0}x\ge\V x. Substitute yy with 2x2x in Equation 6 to get f0 ⁣(x)≤∥x∥\fc{f_0}x\le\V x. We then have f0 ⁣(x)=∥x∥\fc{f_0}x=\V x.

Substitute yy with x+yx+y in Equation 6 to get f0 ⁣(y)≤∥x+y∥−∥x∥≤∥y∥\fc{f_0}y\le\V{x+y}-\V x\le\V y. Substitute yy with x−yx-y in Equation 6 to get −f0 ⁣(y)≤∥x−y∥−∥x∥≤∥y∥-\fc{f_0}y\le\V{x-y}-\V x\le\V y. We then have ∣f0 ⁣(y)∣≤∥y∥\v{\fc{f_0}y}\le\V y, which means ∥f0∥≤1\V{f_0}\le1.

With f0 ⁣(x)=∥x∥\fc{f_0}x=\V x and ∥f0∥≤1\V{f_0}\le1, we have f0∈J ⁣(x)f_0\in\fc Jx. □\square

Theorem 10. Let XX be a normed space. If there exist u,v∈X∖{0}u,v\in X\setminus\B0 such that u/∥u∥≠v/∥v∥u/\V u\ne v/\V v and J ⁣(u)∩J ⁣(v)≠∅\fc Ju\cap\fc Jv\ne\varnothing, then XX is not strictly convex.

Proof

Let f∈J ⁣(u)∩J ⁣(v)f\in\fc Ju\cap\fc Jv. Define u^≔u/∥u∥\hat u\ceq u/\V u and v^≔v/∥v∥\hat v\ceq v/\V v. Then, f ⁣(u^)=f ⁣(v^)=1\fc f{\hat u}=\fc f{\hat v}=1. Because ∥f∥≤1\V f\le 1, we have ∥u^+v^∥≥f ⁣(u^+v^)=2.\V{\hat u+\hat v}\ge\fc f{\hat u+\hat v}=2. On the other hand, by the triangle inequality, we have ∥u^+v^∥≤∥u^∥+∥v^∥=2.\V{\hat u+\hat v}\le\V{\hat u}+\V{\hat v}=2. Squeezing by the two inequalities, we have ∥u^+v^∥=2\V{\hat u+\hat v}=2. This means XX is not strictly convex. □\square

Theorem 11. Let XX be a strictly convex space and y∈X∖{0}y\in X\setminus\B0. Then, Dy‾=Dˉy\overline{D_y}=\bar D_y, where Dy‾\overline{D_y} is the closure of DyD_y.

Proof

Because Dy⊆DˉyD_y\subseteq\bar D_y and Dˉy\bar D_y is closed, we have Dy‾⊆Dˉy\overline{D_y}\subseteq\bar D_y. Suppose for contradiction that there exists u∈Dˉy∖Dy‾u\in\bar D_y\setminus\overline{D_y}.

Note that Dˉy∖Dy‾⊆Dˉy∖Dy={a∈X  |  ∥y−a∥=∥a∥},\bar D_y\setminus\overline{D_y}\subseteq\bar D_y\setminus D_y=\set{a\in X}{\V{y-a}=\V a}, so ∥y−u∥=∥u∥\V{y-u}=\V u. Because u∉Dy‾u\notin\overline{D_y}, there exists δ>0\dlt>0 such that B ⁣(u,δ)∩Dy=∅\fc B{u,\dlt}\cap D_y=\varnothing. In other words, ∀a∈B ⁣(u,δ):∥y−a∥≥∥a∥.\forall a\in\fc B{u,\dlt}:\V{y-a}\ge\V a. For any v∈X∖{0}v\in X\setminus\B0 and t∈(−δ/∥v∥,δ/∥v∥)t\in\p{-\dlt/\V v,\dlt/\V v}, we have ∥u+tv−y∥≥∥u+tv∥.\V{u+tv-y}\ge\V{u+tv}. Take the right derivatives of both sides w.r.t. tt at t=0t=0. Theorem 9 guarantees that the derivatives exist: max⁡f∈J ⁣(u−y)f ⁣(v)=∂v∥u−y∥≥∂v∥u∥=max⁡f∈J ⁣(u)f ⁣(v).\max_{f\in\fc J{u-y}}\fc fv=\partial_v\V{u-y}\ge\partial_v\V u=\max_{f\in\fc Ju}\fc fv. Because J ⁣(u)\fc Ju is weak*-compact and convex by Theorem 7, we have J ⁣(u)⊆J ⁣(u−y)\fc Ju\subseteq\fc J{u-y}; otherwise the Hahn–Banach separation theorem breaks the inequality above.

Why J ⁣(u)⊆J ⁣(u−y)\fc Ju\subseteq\fc J{u-y}

Suppose for contradiction that there exists f0∈J ⁣(u)∖J ⁣(u−y)f_0\in\fc Ju\setminus\fc J{u-y}. Because J ⁣(u−y)\fc J{u-y} is weak*-compact and convex, by the Hahn–Banach separation theorem, there exists v∈Xv\in X (the set of weak*-continuous linear functionals on X∗X^*) such that max⁡f∈J ⁣(u−y)f ⁣(v)<f0 ⁣(v)≤max⁡f∈J ⁣(u)f ⁣(v).\max_{f\in\fc J{u-y}}\fc fv<\fc{f_0}v\le\max_{f\in\fc Ju}\fc fv. This is a contradiction.

We then have J ⁣(u)∩J ⁣(u−y)≠∅\fc Ju\cap\fc J{u-y}\ne\varnothing. Here uu and u−yu-y are distinct nonzero vectors of equal norm, so their normalizations are distinct. By Theorem 10, XX is not strictly convex, a contradiction. □\square

Definition 12 (Birkhoff, 1935). Let XX be a normed space, and let u,y∈Xu,y\in X. We say uu is Birkhoff–James orthogonal to yy, denoted as u⊥BJyu\perp_\mrm{BJ}y, if ∀t∈R:∥u+ty∥≥∥u∥.\forall t\in\bR:\V{u+ty}\ge\V u. For a set H⊆XH\subseteq X, one denotes H⊥BJyH\perp_\mrm{BJ}y if ∀u∈H:u⊥BJy\forall u\in H:u\perp_\mrm{BJ}y.

Theorem 13. Let XX be a normed space such that dim⁡X≥2\dim X\ge2. For any v∈X∖{0}v\in X\setminus\B0, there always exists u∈X∖{0}u\in X\setminus\B0 such that u⊥BJvu\perp_\mrm{BJ}v. Such uu always satisfies that u,vu,v are linearly independent. Specially, when XX is a strictly convex plane, uu is unique up to a scalar multiple.

Proof

First prove the existence. Choose u′∈Xu'\in X such that u′,vu',v are linearly independent. Then, f ⁣(t)≔∥u′+tv∥\fc ft\ceq\V{u'+tv} is a continuous function of R→R\bR\to\bR. By the triangle inequality, we have f ⁣(t)≥∣t∣∥v∥−∥u′∥\fc ft\ge\v t\V v-\V{u'}, so f ⁣(t)→+∞\fc ft\to+\infty as t→±∞t\to\pm\infty. Such a continuous function must have a global minimum at some t0∈Rt_0\in\bR. Define u≔u′+t0vu\ceq u'+t_0v, which must be nonzero as u′,vu',v are linearly independent. Then, for any t∈Rt\in\bR, ∥u+tv∥=∥u′+(t+t0)v∥≥∥u′+t0v∥=∥u∥,\V{u+tv}=\V{u'+\p{t+t_0}v}\ge\V{u'+t_0v}=\V u, so u⊥BJvu\perp_\mrm{BJ}v.

Then prove that u⊥BJvu\perp_\mrm{BJ}v and u,v≠0u,v\ne0 imply that u,vu,v are linearly independent. Suppose for contradiction that u,vu,v are linearly dependent, i.e., u=t0vu=t_0v for some t0∈Rt_0\in\bR. Then, by definition of the Birkhoff–James orthogonality, for any t∈Rt\in\bR, ∣t0+t∣∥v∥=∥u+tv∥≥∥u∥=∣t0∣∥v∥.\v{t_0+t}\V v=\V{u+tv}\ge\V u=\v{t_0}\V v. Divide both sides by ∥v∥\V v to get ∣t0+t∣≥∣t0∣\v{t_0+t}\ge\v{t_0} for any t∈Rt\in\bR, which is false. By contradiction, u,vu,v are linearly independent.

Finally, prove the uniqueness in a strictly convex plane. Suppose that u⊥BJvu\perp_\mrm{BJ}v and u′⊥BJvu'\perp_\mrm{BJ}v and that u,u′,v≠0u,u',v\ne0. Because u,vu,v are linearly independent and the space is a plane, they form a coordinate system. Then, we can express u′=ru+svu'=ru+sv for some r,s∈Rr,s\in\bR. We must have r≠0r\ne0 because otherwise u′u' and vv are linearly dependent. By u′⊥BJvu'\perp_\mrm{BJ}v, we have ∥ru+sv+tv∥≥∥ru+sv∥\V{ru+sv+tv}\ge\V{ru+sv} for any t∈Rt\in\bR. Divide both sides by ∣r∣\v r and substitute t≔−st\ceq-s to get ∥u∥≥∥u+srv∥.\V u\ge\V{u+\fr srv}. (7)(7) On the other hand, by u⊥BJvu\perp_\mrm{BJ}v, we have ∥u+tv∥≥∥u∥\V{u+tv}\ge\V u for any t∈Rt\in\bR. Substitute t≔s/rt\ceq s/r to get ∥u+srv∥≥∥u∥.\V{u+\fr srv}\ge\V u. (8)(8) Combining Equations 7 and 8, we have ∥u+srv∥=∥u∥.\V{u+\fr srv}=\V u. Suppose by contradiction that s≠0s\ne0. Then, x≔u∥u∥,x′≔u+srv∥u∥x\ceq\fr u{\V u},\qquad x'\ceq\fr{u+\fr srv}{\V u} are two distinct points on the unit sphere. Because the space is strictly convex, ∥x+x′∥<2\V{x+x'}<2. On the other hand, ∥x+x′∥=2∥u∥∥u+s2rv∥≥2∥u∥∥u∥=2,\V{x+x'}=\fr2{\V u}\V{u+\fr s{2r}v}\ge\fr2{\V u}\V u=2, where the inequality is by u⊥BJvu\perp_\mrm{BJ}v. This is a contradiction, so we must have s=0s=0. Therefore, u′=ruu'=ru for some r∈Rr\in\bR, which proves the uniqueness of uu up to a scalar multiple. □\square

Inner product spaces

Lemmas

Lemma 14 (Kakutani, 1939, Theorem 4). Let WW be a 3-dimensional normed space. If every 2-dimensional vector subspace of W∗W^* is the range of a linear projection of norm 11, then WW is an inner product space.

Lemma 15. Let XX be a Hilbert space, C⊆XC\subseteq X be nonempty, closed, and convex, and x∈Xx\in X. Then, there exists p∈Cp\in C such that ∀a∈C:⟨a−p,p−x⟩≥0\forall a\in C:\a{a-p,p-x}\ge0.

Proof

By the Hilbert projection theorem, there exists p∈Cp\in C such that ∀c∈C:∥x−p∥≤∥x−c∥.\forall c\in C:\V{x-p}\le\V{x-c}. (9)(9) Because CC is convex, ∀a∈C,t∈[0,1]:(1−t)p+ta∈C\forall a\in C,t\in\b{0,1}:\p{1-t}p+ta\in C. Substitute c≔(1−t)p+tac\ceq\p{1-t}p+ta into Equation 9 and square both sides to get ∀t∈[0,1]:∥x−(1−t)p−ta∥2≥∥x−p∥2.\forall t\in\b{0,1}:\V{x-\p{1-t}p-ta}^2\ge\V{x-p}^2. Subtract ∥x−p∥2\V{x-p}^2 from both sides and divide both sides by 2t2t (assuming t≠0t\ne0) to get ∀t∈(0,1]:⟨x−p,p−a⟩+t2∥p−a∥2≥0.\forall t\in\left(0,1\right]:\a{x-p,p-a}+\fr t2\V{p-a}^2\ge0. Take infimum over tt on both sides, and we have ⟨x−p,p−a⟩≥0\a{x-p,p-a}\ge0. □\square

Lemma 16. Let XX be a finite-dimensional normed space. For any nonempty compact convex set S⊆XS\subseteq X, there exists a finite set S′⊆SS'\subseteq S such that S′−y⊆S⇒y=0S'-y\subseteq S\Rightarrow y=0.

Proof

If SS is a singleton, take S′≔SS'\ceq S. Otherwise, let W≔span⁡ ⁣(S−S)W\ceq\opc{span}{S-S} and choose a basis B∗B^* on W∗W^*. Fix a0∈Sa_0\in S and interpret ϕ\phi on SS as the affine function a↦ϕ ⁣(a−a0)a\mapsto\fc\phi{a-a_0}. For each ϕ∈B∗\phi\in B^*, choose pϕ−∈Sp^-_\phi\in S that minimizes ϕ\phi and choose pϕ+∈Sp^+_\phi\in S that maximizes ϕ\phi. Such points must exist because SS is compact.

Define S′≔{pϕ−,pϕ+  |  ϕ∈B∗}S'\ceq\set{p^-_\phi,p^+_\phi}{\phi\in B^*}. Suppose S′−y⊆SS'-y\subseteq S. Obviously, y∈Wy\in W. For every ϕ∈B∗\phi\in B^*, we have ϕ ⁣(pϕ+−y)≤ϕ ⁣(pϕ+),ϕ ⁣(pϕ−−y)≥ϕ ⁣(pϕ−).\fc\phi{p^+_\phi-y}\le\fc\phi{p^+_\phi},\qquad \fc\phi{p^-_\phi-y}\ge\fc\phi{p^-_\phi}. The two inequalities forces ϕ ⁣(y)=0\fc\phi y=0, so y=0y=0. □\square

Theorem 17. An inner product space satisfies Pˉ⊃a\bar P_\supset^\mrm a.

Proof

Let XX be an inner product space. Suppose for contradiction that XX does not satisfy Pˉ⊃a\bar P_\supset^\mrm a. By Theorem 5, there exists y∈X∖{0}y\in X\setminus\B0 such that 0∈conv‾⁡Dˉy0\in\opn{\overline{conv}}\bar D_y. Therefore, there exists a sequence of finite sets {S(n)}\B{S^{\p n}} such that S(n)⊆DˉyS^{\p n}\subseteq\bar D_y for any nn and that ∑a∈S(n)λa(n)a→0\sum_{a\in S^{\p n}}\lmd^{\p n}_aa\to0, where, for any nn, λa(n)≥0\lmd^{\p n}_a\ge0 for any a∈S(n)a\in S^{\p n}, and ∑aλa(n)=1\sum_a\lmd^{\p n}_a=1.

By Definition 4, we have ∥a−y∥≤∥a∥\V{a-y}\le\V a for any a∈S(n)a\in S^{\p n}. Square both sides and simplify, and we get ⟨a,y⟩≥∥y∥2/2\a{a,y}\ge\V y^2/2. Therefore, ⟨∑a∈S(n)λa(n)a,y⟩=∑a∈S(n)λa(n)⟨a,y⟩≥∑a∈S(n)λa(n)∥y∥22=∥y∥22>0.\a{\sum_{a\in S^{\p n}}\lmd^{\p n}_aa,y} =\sum_{a\in S^{\p n}}\lmd^{\p n}_a\a{a,y} \ge\sum_{a\in S^{\p n}}\lmd^{\p n}_a\fr{\V y^2}2=\fr{\V y^2}2>0. On the other hand, because the inner product is continuous, ⟨∑a∈S(n)λa(n)a,y⟩→⟨0,y⟩=0,\a{\sum_{a\in S^{\p n}}\lmd^{\p n}_aa,y}\to\a{0,y}=0, which is a contradiction. □\square

Theorem 18. If a normed space XX with dim⁡X≥3\dim X\ge3 is not an inner product space, then it does not satisfy P⊃fP_\supset^\mrm f.

Proof

Suppose for contradiction that XX satisfies P⊃fP_\supset^\mrm f. Pick a non-inner-product 3-dimensional subspace W⊆XW\subseteq X.

Why WW exists

The Jordan–von Neumann theorem states that a normed space is an inner product space if the norm satisfies the parallelogram law. Therefore, because XX is not an inner product space, there exist u,v∈Xu,v\in X failing the parallelogram law. Pick w∈X∖span⁡{u,v}w\in X\setminus\opn{span}\B{u,v}. Then, W≔span⁡{u,v,w}W\ceq\opn{span}\B{u,v,w} is a 3-dimensional subspace of XX that is not an inner product space.

For any y∈W∖{0}y\in W\setminus\B0, consider Cy≔conv⁡ ⁣(Dy∩W)C_y\ceq\opc{conv}{D_y\cap W}. Since Dy∩WD_y\cap W is open in WW, CyC_y is open in WW. By P⊃fP_\supset^\mrm f and Theorem 5, 0∉conv⁡Dy0\notin\opn{conv}D_y, so 0∉Cy⊆conv⁡Dy0\notin C_y\subseteq\opn{conv}D_y. By the Hahn–Banach separation theorem, there exists a continuous linear functional fy∈W∗∖{0}f_y\in W^*\setminus\B0 such that ∀a∈Cy:fy ⁣(a)>0\forall a\in C_y:\fc{f_y}a>0. Since y∈Dy∩W⊆Cyy\in D_y\cap W\subseteq C_y, we have fy ⁣(y)>0\fc{f_y}y>0. Define Qy ⁣(z)≔z−fy ⁣(z)fy ⁣(y)y.\fc{Q_y}z\ceq z-\fr{\fc{f_y}z}{\fc{f_y}y}y. Then, Qy:W→WQ_y:W\to W is a linear projection from WW onto ker⁡fy\opn{ker}f_y with ∥Qy∥=1\V{Q_y}=1.

Why QyQ_y is a projection onto ker⁡fy\opn{ker}f_y

First, Qy ⁣(z)∈ker⁡fy\fc{Q_y}z\in\opn{ker}f_y for any z∈Wz\in W because fy ⁣(Qy ⁣(z))=fy ⁣(z)−fy ⁣(z)fy ⁣(y)fy ⁣(y)=0.\fc{f_y}{\fc{Q_y}z}=\fc{f_y}z-\fr{\fc{f_y}z}{\fc{f_y}y}\fc{f_y}y=0.

Then, QyQ_y is a projection because Qy ⁣(Qy ⁣(z))=z−fy ⁣(z)fy ⁣(y)y−fy ⁣(z)fy ⁣(y)(y−fy ⁣(y)fy ⁣(y)y)=Qy ⁣(z).\fc{Q_y}{\fc{Q_y}z} =z-\fr{\fc{f_y}z}{\fc{f_y}y}y -\fr{\fc{f_y}z}{\fc{f_y}y}\p{y-\fr{\fc{f_y}y}{\fc{f_y}y}y} =\fc{Q_y}z.

Finally, QyQ_y maps onto every point in ker⁡fy\opn{ker}f_y because for any z∈ker⁡fyz\in\opn{ker}f_y, we have Qy ⁣(z)=z\fc{Q_y}z=z.

Why ∥Qy∥=1\V{Q_y}=1

Generally, any nonzero bounded linear projection has norm at least 11 by submultiplicativity, so we just need to show ∥Qy∥≤1\V{Q_y}\le1.

For any a∈ker⁡fya\in\opn{ker}f_y, we have a∉Dya\notin D_y, which means ∥a−y∥≥∥a∥\V{a-y}\ge\V a. Similarly, for any a∈ker⁡fya\in\opn{ker}f_y and t∈R∖{0}t\in\bR\setminus\B0, we also have a/t∉Dya/t\notin D_y, which means ∥a/t−y∥≥∥a/t∥\V{a/t-y}\ge\V{a/t}, or equivalently ∥a−ty∥≥∥a∥\V{a-ty}\ge\V a. This inequality obviously also holds for t=0t=0.

Because y∉ker⁡fyy\notin\opn{ker}f_y, we have W=ker⁡fy⊕RyW=\opn{ker}f_y\oplus\bR y. Therefore, for any z∈Wz\in W, there exist unique a∈ker⁡fya\in\opn{ker}f_y and t∈Rt\in\bR such that z=a−tyz=a-ty. Then, we have ∥Qy ⁣(z)∥=∥Qy ⁣(a−ty)∥=∥a∥≤∥a−ty∥=∥z∥.\V{\fc{Q_y}z}=\V{\fc{Q_y}{a-ty}}=\V{a}\le\V{a-ty}=\V z. This shows ∥Qy∥≤1\V{Q_y}\le1.

Then, the adjoint Qy∗:W∗→W∗Q_y^*:W^*\to W^* is a linear projection from W∗W^* onto (ker⁡Qy)⊥\p{\opn{ker}Q_y}^\perp, and ∥Qy∗∥=1\V{Q_y^*}=1. Noticing that ker⁡Qy=Ry\opn{ker}Q_y=\bR y, we have that Qy∗Q_y^* is onto ker⁡y={g∈W∗  |  g ⁣(y)=0}\opn{ker}y=\set{g\in W^*}{\fc gy=0}.

In general, any hyperplane in W∗W^* can be expressed as ker⁡y\opn{ker}y for some y∈W∖{0}y\in W\setminus\B0. Therefore, by Lemma 14, W∗W^* is an inner product space, so WW is an inner product space. This contradicts with the choice that WW is not an inner product space.

Therefore, XX does not satisfy P⊃fP_\supset^\mrm f. □\square

Theorem 19. A Hilbert space satisfies P⊂aP_\subset^\mrm a.

Proof

Let XX be a Hilbert space. Let S⊆XS\subseteq X and x∉C≔conv‾⁡Sx\notin C\ceq\opn{\overline{conv}}S. By Lemma 15, there exists p∈Cp\in C such that ∀a∈C:⟨a−p,p−x⟩≥0\forall a\in C:\a{a-p,p-x}\ge0. Consider ∥a−x∥2=∥a−p∥2+2⟨a−p,p−x⟩+∥p−x∥2≥∥a−p∥2+∥x−p∥2.\V{a-x}^2=\V{a-p}^2+2\a{a-p,p-x}+\V{p-x}^2\ge\V{a-p}^2+\V{x-p}^2. Subtract ∥x−p∥2\V{x-p}^2 from both sides to get ∥a−p∥2≤∥a−x∥2−∥x−p∥2<∥a−x∥2.\V{a-p}^2\le\V{a-x}^2-\V{x-p}^2<\V{a-x}^2. Therefore, p∈I ⁣(S,x)p\in\fc I{S,x}, so I ⁣(S,x)≠∅\fc I{S,x}\ne\varnothing, proving P⊂aP_\subset^\mrm a. □\square

Theorem 20. An inner product space that is not a Hilbert space does not satisfy Pˉ⊂a\bar P_\subset^\mrm a.

Proof

Let XX be an inner product space that is not a Hilbert space. Let X^\hat X be the completion of XX, which is a Hilbert space, and choose z∈X^∖Xz\in\hat X\setminus X. Let S≔{a∈X  |  ⟨a,z⟩=1}S\ceq\set{a\in X}{\a{a,z}=1}, which is a nonempty closed affine hyperplane in XX.

Why SS is nonempty and closed

Suppose for contradiction that SS is empty. Then, z⊥Xz\perp X. Because XX is dense in X^\hat X, we have z⊥X^z\perp \hat X, which implies z=0z=0. This contradicts with z∉Xz\notin X. Therefore, SS is nonempty.

To see that SS is closed, notice that ⟨⋅,z⟩\a{\cdot,z} is a bounded linear functional on X^\hat X, so it is a bounded linear functional on XX.

Obviously, 0∉S=conv‾⁡S0\notin S=\opn{\overline{conv}}S. Now suppose for contradiction that y∈Iˉ ⁣(S,0)∖{0}y\in\fc{\bar I}{S,0}\setminus\B0, which means ∀a∈S:∥a−y∥2≤∥a∥2\forall a\in S:\V{a-y}^2\le\V a^2. Expanding the square gives ⟨a,y⟩≥∥y∥2/2\a{a,y}\ge\V y^2/2. Therefore, the linear functional ⟨⋅,y⟩\a{\cdot,y} is bounded below on the affine hyperplane SS, so ⟨⋅,y⟩\a{\cdot,y} is constant on SS, so ⟨⋅,y⟩\a{\cdot,y} is zero on the linear hyperplane ker⁡⟨⋅,z⟩\opn{ker}\a{\cdot,z} parallel to SS. This means ker⁡⟨⋅,y⟩=ker⁡⟨⋅,z⟩\opn{ker}\a{\cdot,y}=\opn{ker}\a{\cdot,z}, so yy is parallel to zz. However, z∉Xz\notin X while y∈Xy\in X, so this is impossible for y≠0y\ne0, a contradiction. Therefore, Iˉ ⁣(S,0)∖{0}=∅\fc{\bar I}{S,0}\setminus\B0=\varnothing.

Therefore, we find a counterexample to Pˉ⊂a\bar P_\subset^\mrm a. □\square

Theorem 21. An inner product space satisfies P⊂bP_\subset^\mrm b.

Proof

Let XX be an inner product space and x∈Xx\in X. Let S⊆XS\subseteq X be bounded and x∉conv‾⁡Sx\notin\opn{\overline{conv}}S. Because SS is bounded, S−xS-x is bounded, so there exists M>0M>0 such that ∀a∈S:∥a−x∥≤M\forall a\in S:\V{a-x}\le M.

Denote X^\hat X the completion of XX, which is a Hilbert space. Then, x∉C≔conv‾⁡X^Sx\notin C\ceq\opn{\overline{conv}}_{\hat X}S, either. By Lemma 15, there exists p∈Cp\in C such that ∀a∈C:⟨a−p,p−x⟩≥0\forall a\in C:\a{a-p,p-x}\ge0. Add both sides by δ≔⟨p−x,p−x⟩>0\dlt\ceq\a{p-x,p-x}>0 to get ⟨a−x,p−x⟩≥δ\a{a-x,p-x}\ge\dlt.

Now, choose v∈Xv\in X close enough to p−xp-x such that ∥v−(p−x)∥<min⁡ ⁣(δ2M,∥p−x∥),\V{v-\p{p-x}}<\opc{min}{\fr\dlt{2M},\V{p-x}}, which is always possible because XX is dense in X^\hat X. Then, for any a∈Sa\in S, we have ⟨a−x,v⟩=⟨a−x,p−x⟩+⟨a−x,v−p+x⟩≥δ−∥a−x∥∥v−p+x∥>δ/2.\a{a-x,v}=\a{a-x,p-x}+\a{a-x,v-p+x}\ge\dlt-\V{a-x}\V{v-p+x}>\dlt/2.

By the triangle inequality, ∥v∥≥∥p−x∥−∥v−(p−x)∥>0.\V v\ge\V{p-x}-\V{v-\p{p-x}}>0. We can then choose 0<t<δ/∥v∥20<t<\dlt/\V v^2 to get ∥a−(x+tv)∥2=∥a−x∥2−t∥v∥2(2⟨a−x,v⟩∥v∥2−t)<∥a−x∥2.\V{a-\p{x+tv}}^2=\V{a-x}^2-t\V v^2\p{\fr{2\a{a-x,v}}{\V v^2}-t}<\V{a-x}^2. Therefore, x+tv∈I ⁣(S,x)x+tv\in\fc I{S,x}, so I ⁣(S,x)≠∅\fc I{S,x}\ne\varnothing, proving P⊂bP_\subset^\mrm b. □\square

Theorem 22. Let XX be a normed space with 3≤dim⁡X<∞3\le\dim X<\infty. If XX is not an inner product space, then XX does not satisfy Pˉ⊂f\bar P_\subset^\mrm f.

Proof

Because XX is not an inner product space, X∗X^* is not an inner product space. By Theorem 18, X∗X^* does not satisfy P⊃fP_\supset^\mrm f. This means there exists h∈X∗h\in X^* and a finite set S∗⊆DhS^*\subseteq D_h such that 0∈conv⁡S∗0\in\opn{conv}S^*. There exists {λf}\B{\lmd_f} such that λf≥0\lmd_f\ge0 for every f∈S∗f\in S^*, that ∑f∈S∗λf=1\sum_{f\in S^*}\lmd_f=1, and that ∑f∈S∗λff=0\sum_{f\in S^*}\lmd_ff=0. Without loss of generality, we can assume λf>0\lmd_f>0 for every f∈S∗f\in S^* because we can always discard such ff that λf=0\lmd_f=0 from S∗S^*.

For every f∈S∗f\in S^*, define Sf≔{a∈Bˉ ⁣(0,1)  |  f ⁣(a)=∥f∥},S_f\ceq\set{a\in\fc{\bar B}{0,1}}{\fc fa=\V f}, where Bˉ ⁣(0,1)\fc{\bar B}{0,1} is the closed unit ball in XX. We then have ∀a∈Sf:h ⁣(a)=f ⁣(a)+(h−f) ⁣(a)≥∥f∥−∥h−f∥∥a∥>0,\forall a\in S_f:\fc ha=\fc fa+\fc{\p{h-f}}a\ge\V f-\V{h-f}\V a>0, (10)(10) where the last inequality is by f∈Dhf\in D_h.

Because XX is finite-dimensional, Bˉ ⁣(0,1)\fc{\bar B}{0,1} is compact, so every SfS_f is a nonempty compact convex set. By Lemma 16, there exists finite set Sf′⊆SfS'_f\subseteq S_f such that Sf′−y⊆Sf⇒y=0S'_f-y\subseteq S_f\Rightarrow y=0. Define S≔⋃f∈S∗Sf′S\ceq\bigcup_{f\in S^*}S'_f. By Equation 10, we then have ∀a∈S:h ⁣(a)>0\forall a\in S:\fc ha>0. Therefore, 0∉conv⁡S0\notin\opn{conv}S.

Now let y∈Iˉ ⁣(S,0)y\in\fc{\bar I}{S,0}. We then have ∀a∈S:∥a−y∥≤∥a∥=1\forall a\in S:\V{a-y}\le\V a=1. On the other hand, for a∈Sf′a\in S'_f, ∥a−y∥≥f ⁣(a−y)∥f∥=1−f ⁣(y)∥f∥.\V{a-y}\ge\fr{\fc f{a-y}}{\V f}=1-\fr{\fc fy}{\V f}. Therefore, f ⁣(y)≥0\fc fy\ge0. Then, ∑fλff=0\sum_f\lmd_ff=0 forces f ⁣(y)=0\fc fy=0. Then, for any a∈Sf′a\in S'_f, we have f ⁣(a−y)=∥f∥\fc f{a-y}=\V f and ∥a−y∥≤1\V{a-y}\le1, which means a−y∈Sfa-y\in S_f. We now have Sf′−y⊆SfS'_f-y\subseteq S_f, implying y=0y=0.

Therefore, we have Iˉ ⁣(S,0)={0}\fc{\bar I}{S,0}=\B0. This gives a counterexample to Pˉ⊂f\bar P_\subset^\mrm f. □\square

Theorem 23. Let XX be a normed space with dim⁡X≥3\dim X\ge3. If XX is not an inner product space, then it does not satisfy Pˉ⊂b\bar P_\subset^\mrm b.

Proof

Because XX is not an inner product space, X∗X^* is not an inner product space. By Theorem 18, X∗X^* does not satisfy P⊃fP_\supset^\mrm f. By Theorem 5, there exists h∈X∗∖{0}h\in X^*\setminus\B0 such that 0∈conv⁡Dh0\in\opn{conv}D_h. There then exists a finite set S∗⊆DhS^*\subseteq D_h and positive numbers {λf}\B{\lmd_f} such that ∑f∈S∗λf=1\sum_{f\in S^*}\lmd_f=1 and ∑f∈S∗λff=0\sum_{f\in S^*}\lmd_ff=0. We can always choose S∗S^* such that h∈S∗h\in S^*.

Why we can make h∈S∗h\in S^*

Because conv⁡Dh\opn{conv}D_h is open, it contains a neighborhood of 00. Therefore, there exists a small enough ε>0\veps>0 such that −εh∈conv⁡Dh-\veps h\in\opn{conv}D_h. There then exists a finite set S∗′⊆DhS^{*\prime}\subseteq D_h and positive numbers {λf′}\B{\lmd'_f} such that ∑f∈S∗′λf′=1\sum_{f\in S^{*\prime}}\lmd'_f=1 and ∑f∈S∗′λf′f=−εh\sum_{f\in S^{*\prime}}\lmd'_ff=-\veps h. Therefore, 0=ε1+εh+11+ε(−εh)=ε1+εh+11+ε∑f∈S∗′λf′f=∑f∈S∗λff,0=\fr\veps{1+\veps}h+\fr1{1+\veps}\p{-\veps h} =\fr\veps{1+\veps}h+\fr1{1+\veps}\sum_{f\in S^{*\prime}}\lmd'_ff =\sum_{f\in S^*}\lmd_ff, where S∗≔S∗′∪{h},λf≔11+ε{ε+λf′,f=h∈S∗′,ε,f=h∉S∗′,λf′,f≠h.S^*\ceq S^{*\prime}\cup\B h,\qquad\lmd_f\ceq\fr1{1+\veps}\begin{dcases} \veps+\lmd'_f,&f=h\in S^{*\prime},\\ \veps,&f=h\notin S^{*\prime},\\ \lmd'_f,&f\ne h. \end{dcases}

For every f∈S∗f\in S^*, define γf≔∥f∥−∥h−f∥>0\gma_f\ceq\V f-\V{h-f}>0, where the inequality is because f∈Dhf\in D_h. Choose a sequence {af,n}\B{a_{f,n}} in SXS_X, the unit sphere of XX, such that lim⁡n→∞f ⁣(af,n)=∥f∥\lim_{n\to\infty}\fc f{a_{f,n}}=\V f and that f ⁣(af,n)>∥f∥−γf/2\fc f{a_{f,n}}>\V f-\gma_f/2 for every nn. Such a sequence always exists because of the definition of the norm on X∗X^* and the definition of sequence limit. Then, h ⁣(af,n)=f ⁣(af,n)+(h−f) ⁣(af,n)≥f ⁣(af,n)−∥h−f∥>γf2.\fc h{a_{f,n}}=\fc f{a_{f,n}}+\fc{\p{h-f}}{a_{f,n}} \ge\fc f{a_{f,n}}-\V{h-f}>\fr{\gma_f}2.

Define S0≔{af,n  |  f∈S∗,n∈N}S_0\ceq\set{a_{f,n}}{f\in S^*,n\in\bN}. Because S0⊆SXS_0\subseteq S_X, it is bounded. Because ∀a∈S0:h ⁣(a)>min⁡f∈S∗γf/2>0\forall a\in S_0:\fc ha>\min_{f\in S^*}\gma_f/2>0, we have 0∉conv‾⁡S00\notin\opn{\overline{conv}}S_0.

Let y∈Iˉ ⁣(S0,0)y\in\fc{\bar I}{S_0,0}. For any af,n∈S0a_{f,n}\in S_0, we then have f ⁣(y)=f ⁣(af,n)−f ⁣(af,n−y)≥f ⁣(af,n)−∥f∥∥af,n−y∥≥f ⁣(af,n)−∥f∥∥af,n∥=f ⁣(af,n)−∥f∥.\begin{align*} \fc fy&=\fc f{a_{f,n}}-\fc f{a_{f,n}-y}\\ &\ge\fc f{a_{f,n}}-\V f\V{a_{f,n}-y}\\ &\ge\fc f{a_{f,n}}-\V f\V{a_{f,n}}\\ &=\fc f{a_{f,n}}-\V f. \end{align*} Take n→∞n\to\infty, and we have f ⁣(y)≥0\fc fy\ge0. Then, ∑fλff=0\sum_f\lmd_ff=0 forces f ⁣(y)=0\fc fy=0. Therefore, y∈W≔⋂f∈S∗ker⁡fy\in W\ceq\bigcap_{f\in S^*}\opn{ker}f.

Therefore, Iˉ ⁣(S0,0)⊆W\fc{\bar I}{S_0,0}\subseteq W. Now consider two cases, W={0}W=\B0 and W≠{0}W\ne\B0. For the first case, we have Iˉ ⁣(S0,0)={0}\fc{\bar I}{S_0,0}=\B0, which is a counterexample to Pˉ⊂b\bar P_\subset^\mrm b.

For the case W≠{0}W\ne\B0, we pick a fixed a0∈S0⊆SXa_0\in S_0\subseteq S_X and define S≔S0∪(a0−3SW),S\ceq S_0\cup\p{a_0-3S_W}, where SWS_W is the unit sphere in WW. Since SW⊆W⊆ker⁡hS_W\subseteq W\subseteq\opn{ker}h, h ⁣(S)\fc hS has the same positive lower bound as h ⁣(S0)\fc h{S_0}, so 0∉conv‾⁡S0\notin\opn{\overline{conv}}S.

Let y∈Iˉ ⁣(S,0)⊆Iˉ ⁣(S0,0)⊆Wy\in\fc{\bar I}{S,0}\subseteq\fc{\bar I}{S_0,0}\subseteq W. Suppose for contradiction that y≠0y\ne0. Define y^≔y/∥y∥\hat y\ceq y/\V y and a≔a0−3y^∈Sa\ceq a_0-3\hat y\in S. We then have ∥a−y∥≤∥a∥\V{a-y}\le\V a.

Pick some subgradient g∈J ⁣(a)g\in\fc Ja. Then, 1=∥3y^∥−∥a0∥−1≤∥a0−3y^∥−1=∥a∥−1=g ⁣(a)−1=g ⁣(a0)−3g ⁣(y^)−1≤∥g∥∥a0∥−3g ⁣(y^)−1=−3g ⁣(y^).\begin{align*} 1&=\V{3\hat y}-\V{a_0}-1\\ &\le\V{a_0-3\hat y}-1\\ &=\V a-1=\fc ga-1\\ &=\fc g{a_0}-3\fc g{\hat y}-1\\ &\le\V g\V{a_0}-3\fc g{\hat y}-1\\ &=-3\fc g{\hat y}. \end{align*} Therefore, −g ⁣(y^)≥1/3-\fc g{\hat y}\ge1/3. Then, ∥a−y∥≥g ⁣(a−y)∥g∥≥g ⁣(a)−g ⁣(y)=∥a∥−∥y∥g ⁣(y^)≥∥a∥+13∥y∥>∥a∥.\begin{align*}\V{a-y} &\ge\fr{\fc g{a-y}}{\V g}\ge\fc ga-\fc gy\\ &=\V a-\V y\fc g{\hat y}\\ &\ge\V a+\fr13\V y>\V a. \end{align*} This contradicts with ∥a−y∥≤∥a∥\V{a-y}\le\V a. Therefore, y=0y=0, so Iˉ ⁣(S,0)={0}\fc{\bar I}{S,0}=\B0, which is a counterexample to Pˉ⊂b\bar P_\subset^\mrm b. □\square

Planes

Definition 24. A normed space XX has balanced tangent chords at y∈Xy\in X if there exist u∈X∖{0}u\in X\setminus\B0, C≥1C\ge1, and δ>0\dlt>0 such that u⊥BJyu\perp_\mrm{BJ}y and ∀t∈[−δ,δ]:∥u+ty∥≤∥u−Cty∥.\forall t\in\b{-\dlt,\dlt}:\V{u+ty}\le\V{u-Cty}. We say XX has balanced tangent chords if this holds at every y∈Xy\in X.

Definitions and lemmas

Definition 25. Let XX be a normed plane, and let u,y∈X∖{0}u,y\in X\setminus\B0 such that u⊥BJyu\perp_\mrm{BJ}y. Then, {u,y}\B{u,y} is a basis of XX, forming a coordinate system to express every vector in XX as ru+syru+sy for some r,s∈Rr,s\in\bR. The number rr is called the bisector coordinate, and the number ss is called the descent coordinate. In this context, uu is called the bisector direction, and yy is called the descent direction. In a context where a bisector coordinate system is already set up, we denote the coordinate projection of the bisector coordinate as πr\pi_r and the coordinate projection of the descent coordinate as πs\pi_s, i.e., πr(ru+sy)≔r\pi_r\p{ru+sy}\ceq r and πs(ru+sy)≔s\pi_s\p{ru+sy}\ceq s.

Definition 26. Let XX be a normed space, and let u,y∈Xu,y\in X such that u⊥BJyu\perp_\mrm{BJ}y. Define the bisector function βu,y:R→R‾\beta_{u,y}:\bR\to\overline\bR as βu,y ⁣(r)≔sup⁡{s∈R  |  ∥ru+sy∥≤∥ru+(s−1)y∥}.\fc{\beta_{u,y}}r\ceq\sup\set{s\in\bR}{\V{ru+sy}\le\V{ru+\p{s-1}y}}. When a bisector coordinate system with basis {u,y}\B{u,y} is already set up in the context, we abbreviate βu,y\beta_{u,y} as β\beta.

Definition 27. A normed space XX is said to be positively bisectable at y∈Xy\in X if there exists nonzero u⊥BJyu\perp_\mrm{BJ}y such that inf⁡r∈Rβu,y ⁣(r)>0.\inf_{r\in\bR}\fc{\beta_{u,y}}r>0. Moreover, XX is said to be positively bisectable if it is positively bisectable at every y∈Xy\in X.

Lemma 28. The bisector function βu,y\beta_{u,y} is nonnegative. Furthermore, if yy is nonzero and uu is the only nonzero vector in span⁡{u,y}\opn{span}\B{u,y} such that u⊥BJyu\perp_\mrm{BJ}y up to scalar multiples, then ∀r∈R:βu,y ⁣(r)∈(0,1)\forall r\in\bR:\fc{\beta_{u,y}}r\in\p{0,1}.

Proof

Let XX be a normed space, and let u,y∈Xu,y\in X such that u⊥BJyu\perp_\mrm{BJ}y. If u=0u=0 or y=0y=0, the result is trivial. We assume u,y≠0u,y\ne0 from here and use a bisector coordinate system with basis {u,y}\B{u,y} in their spanned plane.

By the triangle inequality, for any r∈Rr\in\bR, the function s↦∥ru+sy∥s\mapsto\V{ru+sy} is convex. Difference on a fixed interval of a convex function is monotonic, so gr ⁣(s)≔∥ru+sy∥−∥ru+(s−1)y∥\fc{g_r}s\ceq\V{ru+sy}-\V{ru+\p{s-1}y} is monotonically non-decreasing in ss. By Definition 12, we can easily see that gr ⁣(0)≤0\fc{g_r}0\le0. Therefore, grg_r is nonpositive on (−∞,0]\left(-\infty,0\right].

By Definition 26, we have β ⁣(r)=sup⁡Gr\fc\beta r=\sup G_r, where Gr≔{s∈R  |  gr ⁣(s)≤0}.G_r\ceq\set{s\in\bR}{\fc{g_r}s\le0}. By the previous paragraph, we have (−∞,0]⊆Gr\left(-\infty,0\right]\subseteq G_r, so sup⁡Gr≥sup⁡(−∞,0]=0\sup G_r\ge\sup\left(-\infty,0\right]=0. Therefore, β ⁣(r)≥0\fc\beta r\ge0.

Now, if uu is the only nonzero vector such that u⊥BJyu\perp_\mrm{BJ}y up to scalar multiples, we prove that ∀r∈R:βu,y ⁣(r)∈(0,1)\forall r\in\bR:\fc{\beta_{u,y}}r\in\p{0,1}. We have the strict inequalities ∥ru∥<∥ru+y∥\V{ru}<\V{ru+y} and ∥ru∥<∥ru−y∥\V{ru}<\V{ru-y} because otherwise ru+yru+y or ru−yru-y would be Birkhoff–James orthogonal to yy. We can then easily see that gr ⁣(0)<0\fc{g_r}0<0 and gr ⁣(1)>0\fc{g_r}1>0. Because grg_r is continuous and non-decreasing, we then have (−∞,0]⊂Gr⊂(−∞,1)\left(-\infty,0\right]\subset G_r\subset\p{-\infty,1}. Therefore, β ⁣(r)∈(0,1)\fc\beta r\in\p{0,1}. □\square

Lemma 29. In a normed plane with a bisector coordinate system with basis {u,y}\B{u,y}, the Voronoi cell Dy={ru+sy  |  s>β ⁣(r)}D_y=\set{ru+sy}{s>\fc\beta r}.

Proof

Choose u∈X∖{0}u\in X\setminus\B0 such that u⊥BJyu\perp_\mrm{BJ}y. Let {u,y}\B{u,y} be the basis of the bisector coordinate system. By the triangle inequality, for any r∈Rr\in\bR, the function s↦∥ru+sy∥s\mapsto\V{ru+sy} is convex. Difference on a fixed interval of a convex function is monotonic, so gr ⁣(s)≔∥ru+sy∥−∥ru+(s−1)y∥\fc{g_r}s\ceq\V{ru+sy}-\V{ru+\p{s-1}y} is monotonically non-decreasing in ss. By Definition 26, we have β ⁣(r)=sup⁡{s∈R  |  gr ⁣(s)≤0}\fc\beta r=\sup\set{s\in\bR}{\fc{g_r}s\le0}. Therefore, gr ⁣(s)>0⇔s>β ⁣(r)\fc{g_r}s>0\Leftrightarrow s>\fc\beta r.

Now, for any a∈Xa\in X, we can express it as a=ru+sya=ru+sy in the bisector coordinate system. Substitute it in the definition of grg_r, and we have gr ⁣(s)=∥a∥−∥a−y∥\fc{g_r}s=\V a-\V{a-y}. By Definition 4, we have a∈Dy⇔∥a∥>∥a−y∥a\in D_y\Leftrightarrow\V a>\V{a-y}. Therefore, a∈Dy⇔∥a∥−∥a−y∥>0⇔gr ⁣(s)>0⇔s>β ⁣(r).a\in D_y\Leftrightarrow\V a-\V{a-y}>0\Leftrightarrow\fc{g_r}s>0\Leftrightarrow s>\fc\beta r. This means Dy={ru+sy  |  s>β ⁣(r)}D_y=\set{ru+sy}{s>\fc\beta r}. □\square

Lemma 30. The bisector function is positive in a neighborhood of 00.

Proof

Let XX be a normed space, and let u,y∈Xu,y\in X such that u⊥BJyu\perp_\mrm{BJ}y. If u=0u=0 or y=0y=0, the result is trivial. We assume u,y≠0u,y\ne0 from here and use a bisector coordinate system with basis {u,y}\B{u,y} in their spanned plane.

By Definition 26, we have s>β ⁣(r)⇒∥ru+sy∥>∥ru+(s−1)y∥s>\fc\beta r\Rightarrow\V{ru+sy}>\V{ru+\p{s-1}y}. By the triangle inequality, we have ∥ru+sy∥≤∥ru∥+∥sy∥,∥ru+(s−1)y∥≥∥(s−1)y∥−∥ru∥.\V{ru+sy}\le\V{ru}+\V{sy},\qquad \V{ru+\p{s-1}y}\ge\V{\p{s-1}y}-\V{ru}. Therefore, s>β ⁣(r)⇒∥ru∥+∥sy∥>∥(s−1)y∥−∥ru∥s>\fc\beta r\Rightarrow\V{ru}+\V{sy}>\V{\p{s-1}y}-\V{ru}. Solving this inequality for ss gives (taking into account that β ⁣(r)≥0\fc\beta r\ge0 by Lemma 28) s>β ⁣(r)⇒s>max⁡ ⁣(0,12−∥u∥∥y∥∣r∣).s>\fc\beta r\Rightarrow s>\opc{max}{0,\fr12-\fr{\V u}{\V y}\v r}.

Solving ∥ru∥+∥sy∥>∥(s−1)y∥−∥ru∥\V{ru}+\V{sy}>\V{\p{s-1}y}-\V{ru} for ss

Rearrange the inequality to get ∣s−1∣−∣s∣<2∥u∥∥y∥∣r∣≕h ⁣(r).\v{s-1}-\v s<\fr{2\V u}{\V y}\v r\eqc\fc hr. The left-hand side is ∣s−1∣−∣s∣={1,s∈(−∞,0],1−2s,s∈(0,1),−1,s∈[1,+∞).\v{s-1}-\v s=\begin{dcases} 1,&s\in\left(-\infty,0\right],\\ 1-2s,&s\in\p{0,1},\\ -1,&s\in\left[1,+\infty\right). \end{dcases} We do not need to consider the case s∈(−∞,0]s\in\left(-\infty,0\right] because s>β ⁣(r)≥0s>\fc\beta r\ge0. Because h ⁣(r)≥0\fc hr\ge0, the inequality is always satisfied when s∈[1,+∞)s\in\left[1,+\infty\right). The only nontrivial case is when s∈(0,1)s\in\p{0,1}, where the inequality becomes s>(1−h ⁣(r))/2s>\p{1-\fc hr}/2. Therefore, the full solution to the inequality is s∈((1−h ⁣(r)2,+∞)∩(0,1)∪[1,+∞))∖(−∞,0]=(max⁡ ⁣(0,1−h ⁣(r)2),+∞).s\in\p{\p{\fr{1-\fc hr}2,+\infty}\cap\p{0,1}\cup\left[1,+\infty\right)}\setminus\left(-\infty,0\right] =\p{\opc{max}{0,\fr{1-\fc hr}2},+\infty}.

This implication relation then translates to the inequality β ⁣(r)≥max⁡ ⁣(0,12−∥u∥∥y∥∣r∣).\fc\beta r\ge\opc{max}{0,\fr12-\fr{\V u}{\V y}\v r}. Noting that the right-hand side is positive when rr is in a neighborhood of 00, we get that β ⁣(r)\fc\beta r is positive when rr is in a neighborhood of 00. □\square

Lemma 31. Let XX be a normed space and y∈Xy\in X. If there exists two linearly independent vectors u1,u2∈Xu_1,u_2\in X such that u1,u2⊥BJyu_1,u_2\perp_\mrm{BJ}y and that u1,u2,yu_1,u_2,y are linearly dependent, then XX has balanced tangent chords at yy.

Proof

The case when y=0y=0 is trivial, and we assume y≠0y\ne0 from here.

Because u1,u2,yu_1,u_2,y are linearly dependent, we can express u2=r′u1+s′yu_2=r'u_1+s'y for some r′,s′∈Rr',s'\in\bR. We know u2,yu_2,y are linearly independent by Theorem 13, so r′≠0r'\ne0. Because u1,u2u_1,u_2 are linearly independent, we have s′≠0s'\ne0. Now define u−≔{u1,s′/r′>0,u2/r′,s′/r′<0,u+≔{u2/r′,s′/r′>0,u1,s′/r′<0,δ≔12∣s′r′∣.u_-\ceq\begin{dcases} u_1,&s'/r'>0,\\ u_2/r',&s'/r'<0, \end{dcases}\qquad u_+\ceq\begin{dcases} u_2/r',&s'/r'>0,\\ u_1,&s'/r'<0, \end{dcases}\qquad \dlt\ceq\fr12\v{\fr{s'}{r'}}. We then have u+=u−+2δyu_+=u_-+2\dlt y and δ>0\dlt>0. Obviously, we have u−,u+⊥BJyu_-,u_+\perp_\mrm{BJ}y, and all of them are nonzero.

Notice that u+⊥BJyu_+\perp_\mrm{BJ}y forces t↦∥u++ty∥t\mapsto\V{u_++ty} to be non-increasing on (−∞,0]\left(-\infty,0\right], which is equivalent to t↦∥u−+ty∥t\mapsto\V{u_-+ty} being non-increasing on (−∞,2δ]\left(-\infty,2\dlt\right]. On the other hand, u−⊥BJyu_-\perp_\mrm{BJ}y forces t↦∥u−+ty∥t\mapsto\V{u_-+ty} to be non-decreasing on [0,+∞)\left[0,+\infty\right). Simultaneously satisfying both monotonicity conditions forces t↦∥u−+ty∥t\mapsto\V{u_-+ty} to be constant on [0,2δ]\b{0,2\dlt}. Define u≔12(u−+u+)=u−+δy,u\ceq\fr12\p{u_-+u_+}=u_-+\dlt y, and we then have ∥u−∥=∥u−+δy∥=∥u∥.\V{u_-}=\V{u_-+\dlt y}=\V u. Therefore, ∀t∈R:∥u+ty∥=∥u−+(t+δ)y∥≥∥u−∥=∥u∥,\forall t\in\bR:\V{u+ty}=\V{u_-+\p{t+\dlt}y}\ge\V{u_-}=\V u, which means that u⊥BJyu\perp_\mrm{BJ}y.

We have ∥u+ty∥=∥u∥\V{u+ty}=\V u whenever ∣t∣≤δ\v t\le\dlt. Pick C≔1C\ceq1. This satisfies the condition ∥u+ty∥≤∥u−Cty∥\V{u+ty}\le\V{u-Cty} for all t∈[−δ,δ]t\in\b{-\dlt,\dlt}. Therefore, XX has balanced tangent chords at yy. □\square

Theorem 32. For a normed space, positive bisectability at yy is equivalent to having balanced tangent chords at yy.

Proof

The case y=0y=0 is immediate, so assume y≠0y\ne0. For a nonzero u⊥BJyu\perp_\mrm{BJ}y, write d ⁣(t)≔∥u+ty∥−∥u∥\fc dt\ceq\V{u+ty}-\V u. This convex function has its minimum at 00, so it is non-decreasing along either ray from 00.

Suppose first that d ⁣(t)≤d ⁣(−Ct)\fc dt\le\fc d{-Ct} for ∣t∣≤δ\v t\le\dlt. Increasing CC preserves this inequality. Choose C≥1+2∥u∥/(δ∥y∥)C\ge1+2\V u/\p{\dlt\V y} as well. For ∣t∣≥δ\v t\ge\dlt, the triangle inequality gives d ⁣(−Ct)≥C∣t∣∥y∥−2∥u∥≥∣t∣∥y∥≥d ⁣(t).\fc d{-Ct}\ge C\v t\V y-2\V u\ge\v t\V y\ge\fc dt. Thus d ⁣(t)≤d ⁣(−Ct)\fc dt\le\fc d{-Ct} for every real tt. Set ε≔1/(C+1)\veps\ceq1/\p{C+1}. For r≠0r\ne0, use t=ε/rt=\veps/r and −Cε=ε−1-C\veps=\veps-1 to obtain ∥ru+εy∥≤∥ru+(ε−1)y∥.\V{ru+\veps y}\le\V{ru+\p{\veps-1}y}. Therefore, βu,y ⁣(r)≥ε\fc{\beta_{u,y}}r\ge\veps. Also βu,y ⁣(0)=1/2≥ε\fc{\beta_{u,y}}0=1/2\ge\veps, proving positive bisectability.

Conversely, choose 0<ε≤min⁡{1/2,inf⁡rβu,y ⁣(r)}0<\veps\le\min\B{1/2,\inf_r\fc{\beta_{u,y}}r}. The function s⟼∥ru+sy∥−∥ru+(s−1)y∥s\longmapsto\V{ru+sy}-\V{ru+\p{s-1}y} is continuous and non-decreasing, so its nonpositive set contains ε\veps. For t≠0t\ne0, take r=ε/tr=\veps/t to obtain d ⁣(t)≤d ⁣(−1−εεt).\fc dt\le\fc d{-\fr{1-\veps}\veps t}. The same inequality holds at t=0t=0. This proves balanced tangent chords, with C=(1−ε)/εC=\p{1-\veps}/\veps. □\square

Theorem 33. A normed plane satisfies P⊃bP_\supset^\mrm b.

Proof

Let XX be a normed plane and S⊆XS\subseteq X be a bounded set such that 0∈conv‾⁡S0\in\opn{\overline{conv}}S. Suppose for contradiction that y∈I ⁣(S,0)y\in\fc I{S,0}. By Definition 4, we have S⊆DyS\subseteq D_y.

Because SS is bounded in a finite-dimensional space, we have conv‾⁡S=conv⁡S‾\opn{\overline{conv}}S=\opn{conv}\overline S, where S‾\overline S is the closure of SS. Therefore, 0∈conv⁡S‾0\in\opn{conv}\overline S. By Carathéodory’s theorem, there exists at most dim⁡X+1=3\dim X+1=3 points ai∈S‾a_i\in\overline S such that 00 is a convex combination of aia_i, i.e., there exists λi≥0\lmd_i\ge0 such that ∑iλi=1\sum_i\lmd_i=1 and ∑iλiai=0\sum_i\lmd_ia_i=0. We can further dictate that λi>0\lmd_i>0 because we can simply discard any aia_i with λi=0\lmd_i=0.

Why conv‾⁡S=conv⁡S‾\opn{\overline{conv}}S=\opn{conv}\overline S

The closure S‾\overline S is a closed bounded set in a finite-dimensional space, so it is compact by the Heine–Borel theorem. Because conv⁡S‾\opn{conv}\overline S is the image of a compact set Δ2×S‾3\Dlt_2\times\overline S^3 (where Δ2\Dlt_2 is the 2-dimensional unit simplex embedded in R3\bR^3) under the continuous map ({λi},{ai})↦∑iλiai\p{\B{\lmd_i},\B{a_i}}\mapsto\sum_i\lmd_ia_i, conv⁡S‾\opn{conv}\overline S is also compact, so it is closed.

Now, taking the convex hull preserves set inclusion, and we have S⊆S‾S\subseteq\overline S, so conv⁡S⊆conv⁡S‾\opn{conv}S\subseteq\opn{conv}\overline S. Because conv⁡S‾\opn{conv}\overline S is closed, it must contain the closure of conv⁡S\opn{conv}S, so we have conv‾⁡S⊆conv⁡S‾\opn{\overline{conv}}S\subseteq\opn{conv}\overline S.

On the other hand, taking the closure preserves set inclusion, and we have S⊆conv⁡SS\subseteq\opn{conv}S, so S‾⊆conv‾⁡S\overline S\subseteq\opn{\overline{conv}}S. Because conv‾⁡S\opn{\overline{conv}}S is convex, it must contain the convex hull of S‾\overline S, so we have conv⁡S‾⊆conv‾⁡S\opn{conv}\overline S\subseteq\opn{\overline{conv}}S.

We then have conv‾⁡S=conv⁡S‾\opn{\overline{conv}}S=\opn{conv}\overline S.

Set up a bisector coordinate system with yy as the descent direction. Denote the bisector direction as uu. We can always choose uu so that ∀t∈(0,+∞):∥u+ty∥>∥u∥\forall t\in\p{0,+\infty}:\V{u+ty}>\V u.

Why we can choose uu so that ∀t∈(0,+∞):∥u+ty∥>∥u∥\forall t\in\p{0,+\infty}:\V{u+ty}>\V u

Let u′∈X∖{0}u'\in X\setminus\B0 such that u′⊥BJyu'\perp_\mrm{BJ}y. By Definition 12, we have ∀t∈R:∥u′+ty∥≥∥u′∥\forall t\in\bR:\V{u'+ty}\ge\V{u'}. Define T≔{t∈R  |  ∥u′+ty∥=∥u′∥}T\ceq\set{t\in\bR}{\V{u'+ty}=\V{u'}}. Because t↦∥u′+ty∥t\mapsto\V{u'+ty} is continuous, TT is closed. Define u≔u′+ymax⁡Tu\ceq u'+y\max T. We can easily see that u⊥BJyu\perp_\mrm{BJ}y and ∀t∈(0,+∞):∥u+ty∥>∥u∥\forall t\in\p{0,+\infty}:\V{u+ty}>\V u.

Because S⊆DyS\subseteq D_y, we have S‾⊆Dy‾\overline S\subseteq\overline{D_y}, where Dy‾\overline{D_y} is the closure of DyD_y. By Lemma 28 and Lemma 29, we have Dy={ru+sy  |  s>β ⁣(r)}⊆H≔{ru+sy  |  s>0}.D_y=\set{ru+sy}{s>\fc\beta r}\subseteq H\ceq\set{ru+sy}{s>0}. Take the closure to get Dy‾⊆H‾={ru+sy  |  s≥0}.\overline{D_y}\subseteq\overline H=\set{ru+sy}{s\ge0}. Therefore, all aia_i has nonnegative ss-coordinates, i.e., πs ⁣(ai)≥0\fc{\pi_s}{a_i}\ge0 for all ii. On the other hand, acting πs\pi_s on the convex combination ∑iλiai=0\sum_i\lmd_ia_i=0 gives ∑iλiπs ⁣(ai)=0\sum_i\lmd_i\fc{\pi_s}{a_i}=0. Because λi>0\lmd_i>0 for all ii, we must have πs ⁣(ai)=0\fc{\pi_s}{a_i}=0 for all ii. We then have ai=πr ⁣(ai)ua_i=\fc{\pi_r}{a_i}u for all ii.

Consider two cases. For the first case, all aia_i are the same point. Because their convex combination is 00, we then have ai=0a_i=0 for all ii. We then have 0∈S‾⊆Dy‾⊆Dˉy0\in\overline S\subseteq\overline{D_y}\subseteq\bar D_y, which means ∥y−0∥≤∥0∥\V{y-0}\le\V0, so y=0y=0. However, I ⁣(S,0)\fc I{S,0} cannot contain 00 by definition, so this is a contradiction.

For the second case, at least two aia_i are different points. Because ∑iλiπr ⁣(ai)=0\sum_i\lmd_i\fc{\pi_r}{a_i}=0, there must exist ii with πr ⁣(ai)<0\fc{\pi_r}{a_i}<0 and another ii with πr ⁣(ai)>0\fc{\pi_r}{a_i}>0. Without loss of generality, suppose that πr ⁣(a1)<0\fc{\pi_r}{a_1}<0. Then, because a1∈Dy‾⊆Dˉya_1\in\overline{D_y}\subseteq\bar D_y, we have ∥a1−y∥≤∥a1∥\V{a_1-y}\le\V{a_1}. On the other hand, since ∀t∈(0,+∞):∥u+ty∥>∥u∥\forall t\in\p{0,+\infty}:\V{u+ty}>\V u, we have ∥a1−y∥=∣πr ⁣(a1)∣∥u−1πr ⁣(a1)y∥>∣πr ⁣(a1)∣∥u∥=∥a1∥.\V{a_1-y}=\v{\fc{\pi_r}{a_1}}\V{u-\fr1{\fc{\pi_r}{a_1}}y}>\v{\fc{\pi_r}{a_1}}\V u=\V{a_1}. This gives a contradiction.

Either way, we have a contradiction, so I ⁣(S,0)=∅\fc I{S,0}=\varnothing. □\square

Theorem 34. A strictly convex plane satisfies Pˉ⊃b\bar P_\supset^\mrm b.

Proof

Let XX be a strictly convex plane and S⊆XS\subseteq X be a bounded set such that 0∈conv‾⁡S0\in\opn{\overline{conv}}S. Suppose for contradiction that y∈Iˉ ⁣(S,0)∖{0}y\in\fc{\bar I}{S,0}\setminus\B0. By Definition 4, we have S⊆DˉyS\subseteq\bar D_y. Because Dˉy\bar D_y is already a closed set, we have S‾⊆Dˉy\overline S\subseteq\bar D_y, where S‾\overline S is the closure of SS.

Set up a bisector coordinate system with yy as the descent direction. Denote the bisector direction as uu. By Lemma 28 and Lemma 29, we have Dy={ru+sy  |  s>β ⁣(r)}⊆H≔{ru+sy  |  s>0}.D_y=\set{ru+sy}{s>\fc\beta r}\subseteq H\ceq\set{ru+sy}{s>0}. Take the closure to get Dy‾⊆H‾={ru+sy  |  s≥0}.\overline{D_y}\subseteq\overline H=\set{ru+sy}{s\ge0}. By Theorem 11, we have Dˉy=Dy‾\bar D_y=\overline{D_y}, so we have S‾⊆Dˉy=Dy‾⊆H‾\overline S\subseteq\bar D_y=\overline{D_y}\subseteq\overline H.

All the rest of the proof is almost the same as the proof of Theorem 33. However I will repeat it here for completeness.

Because SS is bounded in a finite-dimensional space, we have conv‾⁡S=conv⁡S‾\opn{\overline{conv}}S=\opn{conv}\overline S. Therefore, 0∈conv⁡S‾0\in\opn{conv}\overline S. By Carathéodory’s theorem, there exists at most dim⁡X+1=3\dim X+1=3 points ai∈S‾a_i\in\overline S such that 00 is a convex combination of aia_i, i.e., there exists λi≥0\lmd_i\ge0 such that ∑iλi=1\sum_i\lmd_i=1 and ∑iλiai=0\sum_i\lmd_ia_i=0. We can further dictate that λi>0\lmd_i>0 because we can simply discard any aia_i with λi=0\lmd_i=0.

Because ai∈S‾⊆H‾a_i\in\overline S\subseteq\overline H, all aia_i has nonnegative ss-coordinates, i.e., πs ⁣(ai)≥0\fc{\pi_s}{a_i}\ge0 for all ii. On the other hand, acting πs\pi_s on the convex combination ∑iλiai=0\sum_i\lmd_ia_i=0 gives ∑iλiπs ⁣(ai)=0\sum_i\lmd_i\fc{\pi_s}{a_i}=0. Because λi>0\lmd_i>0 for all ii, we must have πs ⁣(ai)=0\fc{\pi_s}{a_i}=0 for all ii. We then have ai=πr ⁣(ai)ua_i=\fc{\pi_r}{a_i}u for all ii.

Consider two cases. For the first case, all aia_i are the same point. Because their convex combination is 00, we then have ai=0a_i=0 for all ii. We then have 0∈S‾⊆Dˉy0\in\overline S\subseteq\bar D_y, which means ∥y−0∥≤∥0∥\V{y-0}\le\V0, so y=0y=0, contradicting with y∈Iˉ ⁣(S,0)∖{0}y\in\fc{\bar I}{S,0}\setminus\B0.

For the second case, at least two aia_i are different points. Because ∑iλiπr ⁣(ai)=0\sum_i\lmd_i\fc{\pi_r}{a_i}=0, there must exist ii with πr ⁣(ai)<0\fc{\pi_r}{a_i}<0 and another ii with πr ⁣(ai)>0\fc{\pi_r}{a_i}>0. Without loss of generality, suppose that πr ⁣(a1)<0\fc{\pi_r}{a_1}<0 and πr ⁣(a2)>0\fc{\pi_r}{a_2}>0. Then, because a1,a2∈Dˉya_1,a_2\in\bar D_y, we have ∥a1−y∥≤∥a1∥\V{a_1-y}\le\V{a_1} and ∥a2−y∥≤∥a2∥\V{a_2-y}\le\V{a_2}. Adding them together gives ∥a1−y∥+∥a2−y∥≤∥a1∥+∥a2∥=(∣πr ⁣(a1)∣+∣πr ⁣(a2)∣)∥u∥=∥a1−a2∥.\V{a_1-y}+\V{a_2-y}\le\V{a_1}+\V{a_2}=\p{\v{\fc{\pi_r}{a_1}}+\v{\fc{\pi_r}{a_2}}}\V u =\V{a_1-a_2}. By the triangle inequality, ∥a1−y∥+∥a2−y∥≥∥a1−a2∥.\V{a_1-y}+\V{a_2-y}\ge\V{a_1-a_2}. Therefore, we have ∥a1−y∥+∥a2−y∥=∥a1−a2∥\V{a_1-y}+\V{a_2-y}=\V{a_1-a_2}, which means yy is also on Ru\bR u since XX is strictly convex, but this is impossible because we dictate u,yu,y to be linearly independent in the definition of the bisector coordinate system, so this is a contradiction.

Either way, we have a contradiction, so Iˉ ⁣(S,0)={0}\fc{\bar I}{S,0}=\B0. □\square

Theorem 35. A normed plane with balanced tangent chords satisfies P⊃aP_\supset^\mrm a.

Proof

Let XX be a normed plane with balanced tangent chords. By Theorem 5, to prove that XX satisfies P⊃aP_\supset^\mrm a, it is equivalent to prove that 0∉conv‾⁡Dy0\notin\opn{\overline{conv}}D_y for any y∈Xy\in X, where DyD_y is the Voronoi cell of yy. The case where y=0y=0 is trivial, and we assume y≠0y\ne0 from here.

By Theorem 32, XX is positively bisectable. This means we can choose a nonzero u⊥BJyu\perp_\mrm{BJ}y such that inf⁡r∈Rβu,y ⁣(r)≕ε>0\inf_{r\in\bR}\fc{\beta_{u,y}}r\eqc\veps>0.

Set up a bisector coordinate system with basis {u,y}\B{u,y}. Then, Dy={ru+sy  |  s>β ⁣(r)}D_y=\set{ru+sy}{s>\fc\beta r} by Lemma 29. By the ε\veps bound, we have Dy⊆{ru+sy  |  s>ε}D_y\subseteq\set{ru+sy}{s>\veps}, so conv‾⁡Dy⊆{ru+sy  |  s≥ε}\opn{\overline{conv}}D_y\subseteq\set{ru+sy}{s\ge\veps}. We then obviously have 0∉conv‾⁡Dy0\notin\opn{\overline{conv}}D_y. □\square

Theorem 36. A strictly convex plane with balanced tangent chords satisfies Pˉ⊃a\bar P_\supset^\mrm a.

Proof

Let XX be a strictly convex plane with balanced tangent chords. By Theorem 5, to prove that XX satisfies Pˉ⊃a\bar P_\supset^\mrm a, it is equivalent to prove that 0∉conv‾⁡Dˉy0\notin\opn{\overline{conv}}\bar D_y for any y∈X∖{0}y\in X\setminus\B0, where Dˉy\bar D_y is the closed Voronoi cell of yy.

By Theorem 32, XX is positively bisectable. This means we can choose a nonzero u⊥BJyu\perp_\mrm{BJ}y such that inf⁡r∈Rβu,y ⁣(r)≕ε>0\inf_{r\in\bR}\fc{\beta_{u,y}}r\eqc\veps>0.

Set up a bisector coordinate system with basis {u,y}\B{u,y}. Then, Dy={ru+sy  |  s>β ⁣(r)}D_y=\set{ru+sy}{s>\fc\beta r} by Lemma 29. By the ε\veps bound, we have Dy⊆{ru+sy  |  s>ε}D_y\subseteq\set{ru+sy}{s>\veps}. Take the closure to get Dy‾⊆{ru+sy  |  s≥ε}\overline{D_y}\subseteq\set{ru+sy}{s\ge\veps}. By Theorem 11, we have Dˉy=Dy‾\bar D_y=\overline{D_y}, so Dˉy⊆{ru+sy  |  s≥ε}\bar D_y\subseteq\set{ru+sy}{s\ge\veps}. We then obviously have 0∉conv‾⁡Dˉy0\notin\opn{\overline{conv}}\bar D_y. □\square

Theorem 37. A normed plane without balanced tangent chords does not satisfy P⊃aP_\supset^\mrm a.

Proof

Let XX be a normed plane without balanced tangent chords. By Theorem 5, to prove that XX does not satisfy P⊃aP_\supset^\mrm a, it is equivalent to prove that there exists y∈Xy\in X such that 0∈conv‾⁡Dy0\in\opn{\overline{conv}}D_y.

By Theorem 32, XX is not positively bisectable. Choose y∈Xy\in X at which positive bisectability fails. For every nonzero u⊥BJyu\perp_\mrm{BJ}y, nonnegativity of the bisector function then gives inf⁡r∈Rβu,y ⁣(r)=0\inf_{r\in\bR}\fc{\beta_{u,y}}r=0. Fix one such uu. Since y=0y=0 trivially cannot satisfy this condition, we assume y≠0y\ne0 from here. Set up a bisector coordinate system with basis {u,y}\B{u,y}.

By Lemma 31, uu is the only nonzero vector in XX such that u⊥BJyu\perp_\mrm{BJ}y up to scalar multiples. Therefore, by Lemma 28, we have β ⁣(r)∈(0,1)\fc\beta r\in\p{0,1} for all r∈Rr\in\bR.

The zero infimum of β\beta means there exists a sequence {rn}\B{r_n} such that β ⁣(rn)→0\fc\beta{r_n}\to0. Define bn≔rnu+(β ⁣(rn)+1n)y,bn′≔−nrnu+y.b_n\ceq r_nu+\p{\fc\beta{r_n}+\fr1n}y,\qquad b'_n\ceq-nr_nu+y. Because Dy={ru+sy  |  s>β ⁣(r)}D_y=\set{ru+sy}{s>\fc\beta r} by Lemma 29, we have bn,bn′∈Dyb_n,b_n'\in D_y. Then, the convex combination an≔nbn+bn′n+1=nβ ⁣(rn)+2n+1y∈conv⁡Dy.a_n\ceq\fr{nb_n+b'_n}{n+1}=\fr{n\fc\beta{r_n}+2}{n+1}y\in\opn{conv}D_y. The limit of {an}\B{a_n} is then in conv‾⁡Dy\opn{\overline{conv}}D_y, so 0∈conv‾⁡Dy0\in\opn{\overline{conv}}D_y. □\square

Theorem 38. A strictly convex plane satisfies P⊂aP_\subset^\mrm a.

Proof

Let XX be a strictly convex plane. We need to prove that for any S⊆XS\subseteq X and x∈Xx\in X such that x∉conv‾⁡Sx\notin\opn{\overline{conv}}S, we have I ⁣(S,x)≠∅\fc I{S,x}\ne\varnothing.

Define C≔conv‾⁡S−xC\ceq\opn{\overline{conv}}S-x, and we have 0∉C0\notin C. Because CC is a closed convex set, by the Hahn–Banach separation theorem, there exists f′∈X∗f'\in X^* and δ∈(0,+∞)\dlt\in\p{0,+\infty} such that ∀a∈C:f′ ⁣(a)≥δ\forall a\in C:\fc{f'}a\ge\dlt. Define f≔f′/δf\ceq f'/\dlt, and we have ∀a∈C:f ⁣(a)≥1\forall a\in C:\fc fa\ge1.

Pick any u∈ker⁡f∖{0}u\in\opn{ker}f\setminus\B0. By Theorem 7, there exists g∈J ⁣(u)g\in\fc Ju. Pick any v′∈ker⁡g∖{0}v'\in\opn{ker}g\setminus\B0. Then, by Equation 4, we have ∀t∈R:∥u+tv′∥−∥u∥≥tg ⁣(v′)=0\forall t\in\bR:\V{u+tv'}-\V u\ge t\fc g{v'}=0. Therefore, u⊥BJv′u\perp_\mrm{BJ}v'. By Theorem 13, u,v′u,v' are linearly independent, so v′∉ker⁡fv'\notin\opn{ker}f. Define v≔v′/f ⁣(v′)v\ceq v'/\fc f{v'}.

Set up a bisector coordinate system with basis {u,v}\B{u,v}. We have f ⁣(u)=0\fc fu=0 and f ⁣(v)=1\fc fv=1, so f=πsf=\pi_s. Then, ∀a∈C:f ⁣(a)≥1\forall a\in C:\fc fa\ge1 is equivalent to ∀ru+sv∈C:s≥1\forall ru+sv\in C:s\ge1. By Lemma 28, we have β ⁣(r)<1\fc\beta r<1 for all r∈Rr\in\bR. By Lemma 29, we have Dv={ru+sv  |  s>β ⁣(r)}D_v=\set{ru+sv}{s>\fc\beta r}. Therefore, S−x⊆C⊆{ru+sv  |  s≥1}⊆Dv.S-x\subseteq C\subseteq\set{ru+sv}{s\ge1}\subseteq D_v. By Definition 4, we can easily see x+v∈I ⁣(S,x)x+v\in\fc I{S,x}. □\square

Theorem 39. A normed plane satisfies Pˉ⊂a\bar P_\subset^\mrm a.

Proof

Let XX be a normed plane. We need to prove that for any S⊆XS\subseteq X and x∈Xx\in X such that x∉conv‾⁡Sx\notin\opn{\overline{conv}}S, we have Iˉ ⁣(S,x)∖{x}≠∅\fc{\bar I}{S,x}\setminus\B x\ne\varnothing.

Define C≔conv‾⁡S−xC\ceq\opn{\overline{conv}}S-x, and we have 0∉C0\notin C. Because CC is a closed convex set, by the Hahn–Banach separation theorem, there exists f′∈X∗f'\in X^* and δ∈(0,+∞)\dlt\in\p{0,+\infty} such that ∀a∈C:f′ ⁣(a)≥δ\forall a\in C:\fc{f'}a\ge\dlt. Define f≔f′/δf\ceq f'/\dlt, and we have ∀a∈C:f ⁣(a)≥1\forall a\in C:\fc fa\ge1.

Pick any u∈ker⁡f∖{0}u\in\opn{ker}f\setminus\B0 and g∈J ⁣(u)g\in\fc Ju. Choose v′∈ker⁡g∖{0}v'\in\opn{ker}g\setminus\B0. The subgradient inequality gives ∥u+tv′∥≥∥u∥+tg ⁣(v′)=∥u∥\V{u+tv'}\ge\V u+t\fc g{v'}=\V u for every real tt, so u⊥BJv′u\perp_\mrm{BJ}v'. Because u,v′u,v' are linearly independent, v′∉ker⁡fv'\notin\opn{ker}f, so f ⁣(v′)≠0\fc f{v'}\ne0. Define v≔v′/f ⁣(v′)v\ceq v'/\fc f{v'}. Because Birkhoff–James orthogonality is invariant under scalar multiplication, we still have u⊥BJvu\perp_\mrm{BJ}v. Also, we have f ⁣(v)=1\fc fv=1.

Set up a bisector coordinate system with basis {u,v}\B{u,v}. Any a∈Ca\in C can be expressed as a=ru+sva=ru+sv for some r,s∈Rr,s\in\bR. Then, f ⁣(a)≥1\fc fa\ge1 can be expressed as ∀ru+sv∈C:s≥1\forall ru+sv\in C:s\ge1. Because u⊥BJvu\perp_\mrm{BJ}v, we have ∥ru+sv∥≥∥ru∥\V{ru+sv}\ge\V{ru} for all r,s∈Rr,s\in\bR. Therefore, s↦∥ru+sv∥s\mapsto\V{ru+sv} achieves its global minimum at s=0s=0. Because it is a convex function, it is monotonically non-decreasing on [0,+∞)\left[0,+\infty\right). Then, for any a∈Ca\in C, ∥a−v∥=∥ru+(s−1)v∥≤∥ru+sv∥=∥a∥.\V{a-v}=\V{ru+\p{s-1}v}\le\V{ru+sv}=\V a. We can then see that x+v∈Iˉ ⁣(S,x)x+v\in\fc{\bar I}{S,x}. This proves Pˉ⊂a\bar P_\subset^\mrm a. □\square

Summary

The following table lists the established sufficiency and necessity results for the properties P⊃,⊂f,c,b,aP_{\supset,\subset}^{\mrm f,\mrm c,\mrm b,\mrm a} and Pˉ⊃,⊂f,c,b,a\bar P_{\supset,\subset}^{\mrm f,\mrm c,\mrm b,\mrm a}.

Property Sufficiency Necessity
P⊃f,c,bP_\supset^{\mrm f,\mrm c,\mrm b} 17, 33 18
P⊃aP_\supset^\mrm a 17, 35 18, 37
P⊂f,cP_\subset^{\mrm f,\mrm c} 21, 38 1, 22
P⊂bP_\subset^\mrm b 21, 38 1, 23
P⊂aP_\subset^\mrm a 19, 38 1, 20, 23
Pˉ⊃f,c,b\bar P_\supset^{\mrm f,\mrm c,\mrm b} 17, 34 2, 18
Pˉ⊃a\bar P_\supset^\mrm a 17, 36 2, 18, 37
Pˉ⊂f,c\bar P_\subset^{\mrm f,\mrm c} 21, 39 22
Pˉ⊂b\bar P_\subset^\mrm b 21, 39 23
Pˉ⊂a\bar P_\subset^\mrm a 19, 39 20, 23

Open problems

What geometric conditions, stated with a fixed number of point variables rather than quantifiers over finite or compact subsets, characterize infinite-dimensional normed spaces satisfying Pˉ⊂f,c\bar P_\subset^{\mrm f,\mrm c} and P⊂f,cP_\subset^{\mrm f,\mrm c}?

In fact, we have the strict hierarchy Pˉ⊂f⇏Pˉ⊂c⇏Pˉ⊂b\bar P_\subset^{\mrm f}\not\Rightarrow\bar P_\subset^{\mrm c}\not\Rightarrow\bar P_\subset^{\mrm b}. An example of Pˉ⊂c∧¬Pˉ⊂b\bar P_\subset^{\mrm c}\land\neg\bar P_\subset^{\mrm b} is c00c_{00}, and an example of Pˉ⊂f∧¬Pˉ⊂c\bar P_\subset^{\mrm f}\land\neg\bar P_\subset^{\mrm c} is ℓ∞3⊕∞(c00+Ru)\ell_\infty^3\oplus_\infty\p{c_{00}+\bR u}, where c00c_{00} is the space of all sequences with finitely many nonzero elements equipped with the ℓ∞\ell_\infty norm, and uu is a particular element in ℓ∞\ell_\infty defined by u ⁣(n)≔n/(n+1)\fc un\ceq n/\p{n+1}.

Why c00c_{00} satisfies Pˉ⊂c\bar P_\subset^\mrm c

Let S⊆c00S\subseteq c_{00} be a compact set and x∈c00∖Sx\in c_{00}\setminus S.

Because SS is compact and x∉Sx\notin S, we have δ≔min⁡a∈S∥x−a∥>0\dlt\ceq\min_{a\in S}\V{x-a}>0.

Because SS is compact, S∪{x}S\cup\B x is also compact, so all sequences in S∪{x}S\cup\B x converge uniformly to 00. There then exists N∈NN\in\bN such that, whenever n≥Nn\ge N, we have ∣a ⁣(n)∣<δ/4\v{\fc an}<\dlt/4 for all a∈Sa\in S and ∣x ⁣(n)∣<δ/4\v{\fc xn}<\dlt/4. Therefore, ∣x ⁣(n)−a ⁣(n)∣≤∣x ⁣(n)∣+∣a ⁣(n)∣<δ/2\v{\fc xn-\fc an}\le\v{\fc xn}+\v{\fc an}<\dlt/2 for all a∈Sa\in S and n≥Nn\ge N.

Why a compact set converges uniformly

Given a compact set S⊆c00S\subseteq c_{00}, we will prove that sequences in SS converge uniformly to 00, which is to prove that for any ε∈(0,+∞)\veps\in\p{0,+\infty}, there exists N∈NN\in\bN such that ∀n∈[N,+∞)∩N,a∈S:∣a ⁣(n)∣<ε.\forall n\in\left[N,+\infty\right)\cap\bN,a\in S:\v{\fc an}<\veps. Given ε\veps, consider the open cover of SS given by {B ⁣(a,ε/2)  |  a∈S}\set{\fc B{a,\veps/2}}{a\in S}. It must have a finite subcover {B ⁣(a,ε/2)  |  a∈S′}\set{\fc B{a,\veps/2}}{a\in S'}, where S′⊆SS'\subseteq S is a finite set. This set being a cover means that there exists a mapping p:S→S′p:S\to S' such that ∀a∈S:∥a−p ⁣(a)∥<ε/2\forall a\in S:\V{a-\fc pa}<\veps/2.

For each a∈S′a\in S', because lim⁡n→∞a ⁣(n)=0\lim_{n\to\infty}\fc an=0, there exists Na∈NN_a\in\bN such that ∀n∈[Na,+∞)∩N:∣a ⁣(n)∣<ε2.\forall n\in\left[N_a,+\infty\right)\cap\bN:\v{\fc an}<\fr\veps2. Define N≔max⁡a∈S′NaN\ceq\max_{a\in S'}N_a. Whenever n≥Nn\ge N, we have ∀a∈S:∣a ⁣(n)∣≤∣a ⁣(n)−p ⁣(a) ⁣(n)∣+∣p ⁣(a) ⁣(n)∣≤∥a−p ⁣(a)∥+∣p ⁣(a) ⁣(n)∣<ε2+ε2=ε.\forall a\in S:\v{\fc an}\le\v{\fc an-\fc{\fc pa}n}+\v{\fc{\fc pa}n} \le\V{a-\fc pa}+\v{\fc{\fc pa}n}<\fr\veps2+\fr\veps2=\veps. Therefore, sequences in SS converge uniformly to 00.

Set y≔x+δeN/2y\ceq x+\dlt e_N/2, where eN ⁣(n)≔δN,n\fc{e_N}n\ceq\dlt_{N,n}, where δN,n\dlt_{N,n} is the Kronecker delta. For every n≥Nn\ge N and a∈Sa\in S, we have ∣y ⁣(n)−a ⁣(n)∣≤∣x ⁣(n)−a ⁣(n)∣+∣δ2δN,n∣<δ2+δ2=δ≤∥x−a∥.\v{\fc yn-\fc an}\le\v{\fc xn-\fc an}+\v{\fr\dlt2\dlt_{N,n}} <\fr\dlt2+\fr\dlt2=\dlt\le\V{x-a}. For every n<Nn<N, we have ∣y ⁣(n)−a ⁣(n)∣=∣x ⁣(n)−a ⁣(n)∣≤∥x−a∥\v{\fc yn-\fc an}=\v{\fc xn-\fc an}\le\V{x-a}. Therefore, we have ∥y−a∥=sup⁡n∈N∣y ⁣(n)−a ⁣(n)∣≤∥x−a∥.\V{y-a}=\sup_{n\in\bN}\v{\fc yn-\fc an}\le\V{x-a}. This proves that y∈Iˉ ⁣(S,x)y\in\fc{\bar I}{S,x}, so x∉Pˉ ⁣(S)x\notin\fc{\bar P}S.

We then have Pˉ ⁣(S)⊆S⊆conv‾⁡S\fc{\bar P}S\subseteq S\subseteq\opn{\overline{conv}}S, so c00c_{00} satisfies Pˉ⊂c\bar P_\subset^\mrm c.

Why ℓ∞3⊕∞(c00+Ru)\ell_\infty^3\oplus_\infty\p{c_{00}+\bR u} satisfies Pˉ⊂f\bar P_\subset^\mrm f

Let X≔ℓ∞3⊕∞(c00+Ru)X\ceq\ell_\infty^3\oplus_\infty\p{c_{00}+\bR u}. Let S⊆XS\subseteq X be a finite set and x∈X∖Sx\in X\setminus S. Every a∈Sa\in S can be expressed as a=x−(qa,za+rau)a=x-\p{q_a,z_a+r_au}, where qa∈ℓ∞3q_a\in\ell_\infty^3, za∈c00z_a\in c_{00}, and ra∈Rr_a\in\bR. We have ∥x−a∥≥∥za+rau∥≥lim⁡n→∞∣za ⁣(n)+rau ⁣(n)∣=∣ra∣.\V{x-a}\ge\V{z_a+r_au}\ge\lim_{n\to\infty}\v{\fc{z_a}n+r_a\fc un}=\v{r_a}. Define N≔1+max⁡({0}∪⋃a∈S{n∈N  |  za ⁣(n)≠0}),N\ceq1+\max\p{\B0\cup\bigcup_{a\in S}\set{n\in\bN}{\fc{z_a}n\ne0}}, which is finite because zaz_a has only finitely many nonzero elements. If ra=0r_a=0, then ∣rau ⁣(N)∣=0<∥x−a∥\v{r_a\fc uN}=0<\V{x-a}. If ra≠0r_a\ne0, then ∣rau ⁣(N)∣<∣ra∣≤∥x−a∥\v{r_a\fc uN}<\v{r_a}\le\V{x-a}. Either way, we have δ≔min⁡a∈S(∥x−a∥−∣rau ⁣(N)∣)>0.\dlt\ceq\min_{a\in S}\p{\V{x-a}-\v{r_a\fc uN}}>0.

Define y≔x+(0,δeN)y\ceq x+\p{0,\dlt e_N}, where eN∈c00e_N\in c_{00} is defined by eN ⁣(n)≔δN,n\fc{e_N}n\ceq\dlt_{N,n}, where δN,n\dlt_{N,n} is the Kronecker delta. Then, for every a∈Sa\in S, we have a=y−(qa,za+rau+δeN)a=y-\p{q_a,z_a+r_au+\dlt e_N}. Now, we have ∣(za+rau+δeN) ⁣(N)∣≤∣rau ⁣(N)∣+δ≤∥x−a∥.\v{\fc{\p{z_a+r_au+\dlt e_N}}N}\le\v{r_a\fc uN}+\dlt\le\V{x-a}. For any n∈N∖{N}n\in\bN\setminus\B N, we have ∣(za+rau+δeN) ⁣(n)∣=∣za ⁣(n)+rau ⁣(n)∣≤∥za+rau∥≤∥x−a∥.\v{\fc{\p{z_a+r_au+\dlt e_N}}n}=\v{\fc{z_a}n+r_a\fc un}\le\V{z_a+r_au}\le\V{x-a}. Therefore, ∥y−a∥=max⁡ ⁣(∥qa∥,∥za+rau+δeN∥)≤∥x−a∥.\V{y-a}=\opc{max}{\V{q_a},\V{z_a+r_au+\dlt e_N}}\le\V{x-a}. This proves that y∈Iˉ ⁣(S,x)y\in\fc{\bar I}{S,x}, so x∉Pˉ ⁣(S)x\notin\fc{\bar P}S.

Therefore, we have Pˉ ⁣(S)⊆S⊆conv‾⁡S\fc{\bar P}S\subseteq S\subseteq\opn{\overline{conv}}S, so XX satisfies Pˉ⊂f\bar P_\subset^\mrm f.

Why ℓ∞3⊕∞(c00+Ru)\ell_\infty^3\oplus_\infty\p{c_{00}+\bR u} does not satisfy Pˉ⊂c\bar P_\subset^\mrm c

Take S1≔{(1,1,−1),(1,−1,1),(−1,1,1)}⊆ℓ∞3.S_1\ceq\B{\p{1,1,-1},\p{1,-1,1},\p{-1,1,1}}\subseteq\ell_\infty^3. Every point of S1S_1 has norm 11 and coordinate sum 11, so 0∉conv‾⁡S10\notin\opn{\overline{conv}}S_1. Each coordinate takes both values 11 and −1-1 among these points. Thus the inequalities ∥y1−a∥≤1\V{y_1-a}\le1 for every a∈S1a\in S_1 force each coordinate of y1y_1 to be 00, and Iˉ ⁣(S1,0)={0}\fc{\bar I}{S_1,0}=\B0.

Define S2≔{an,−an  |  n∈N∪{∞}}S_2\ceq\set{a_n,-a_n}{n\in\bN\cup\B\infty}, where an≔u+en/(n+1)a_n\ceq u+e_n/\p{n+1} and a∞≔ua_\infty\ceq u, where en∈c00e_n\in c_{00} is defined by en ⁣(m)≔δn,m\fc{e_n}m\ceq\dlt_{n,m}, where δn,m\dlt_{n,m} is the Kronecker delta. Obviously S2⊆c00+RuS_2\subseteq c_{00}+\bR u is compact because lim⁡n→∞an=a∞\lim_{n\to\infty}a_n=a_\infty.

We now prove that Iˉ ⁣(S2,0)={0}\fc{\bar I}{S_2,0}=\B0. Suppose y2∈Iˉ ⁣(S2,0)y_2\in\fc{\bar I}{S_2,0}. Then, for any n∈Nn\in\bN, we have ∣y2 ⁣(n)±1∣=∣y2 ⁣(n)±an ⁣(n)∣≤∥y2±an∥≤∥an∥=1.\v{\fc{y_2}n\pm1}=\v{\fc{y_2}n\pm\fc{a_n}n}\le\V{y_2\pm a_n}\le\V{a_n}=1. The two inequalities for ±\pm force y2 ⁣(n)=0\fc{y_2}n=0, so y2=0y_2=0. We then have Iˉ ⁣(S2,0)={0}\fc{\bar I}{S_2,0}=\B0.

Pick any q∈S1q\in S_1. Construct S≔{(a,0)  |  a∈S1}∪{(q,a)  |  a∈S2}.S\ceq\set{\p{a,0}}{a\in S_1}\cup\set{\p{q,a}}{a\in S_2}. Obviously SS is compact because S1S_1 and S2S_2 are compact. Because 0∉conv‾⁡S10\notin\opn{\overline{conv}}S_1, we have 0∉conv‾⁡S0\notin\opn{\overline{conv}}S. The canonical projections onto ℓ∞3\ell_\infty^3 and c00+Ruc_{00}+\bR u of any element in Iˉ ⁣(S,0)\fc{\bar I}{S,0} belong to Iˉ ⁣(S1,0)\fc{\bar I}{S_1,0} and Iˉ ⁣(S2,0)\fc{\bar I}{S_2,0}, respectively. Therefore, because Iˉ ⁣(S1,0)={0}\fc{\bar I}{S_1,0}=\B0 and Iˉ ⁣(S2,0)={0}\fc{\bar I}{S_2,0}=\B0, we have Iˉ ⁣(S,0)={0}\fc{\bar I}{S,0}=\B0. This proves that ℓ∞3⊕∞(c00+Ru)\ell_\infty^3\oplus_\infty\p{c_{00}+\bR u} does not satisfy Pˉ⊂c\bar P_\subset^\mrm c.

We also have the strict hierarchy P⊂f⇏P⊂c⇏P⊂bP_\subset^\mrm f\not\Rightarrow P_\subset^\mrm c\not\Rightarrow P_\subset^\mrm b. Note that this implies Pˉ⊂f⇏Pˉ⊂c⇏Pˉ⊂b\bar P_\subset^\mrm f\not\Rightarrow\bar P_\subset^\mrm c\not\Rightarrow\bar P_\subset^\mrm b because examples of P⊂fP_\subset^\mrm f must be strictly convex (by Theorem 1) and thus has Pˉ ⁣(S)=P ⁣(S)\fc{\bar P}S=\fc PS (by Theorem 3).

An example of P⊂f∧¬P⊂cP_\subset^\mrm f\land\neg P_\subset^\mrm c is R ⁣[t]\bfc\bR t (real polynomials) equipped with the Lp[0,1]L^p\b{0,1} norm with p≔5p\ceq\sqrt5.

Why R ⁣[t]\bfc\bR t with Lp[0,1]L^p\b{0,1} norm satisfies P⊂fP_\subset^\mrm f

The following argument works for any irrational p∈[1,+∞)∖Qp\in\left[1,+\infty\right)\setminus\bQ. For a∈R ⁣[t]∖{0}a\in\bfc\bR t\setminus\B0, differentiation under the integral gives the unique subgradient j ⁣(a)∈J ⁣(a)\fc ja\in\fc Ja: j ⁣(a) ⁣(v)=1∥a∥p−1∫01dt∣a ⁣(t)∣p−2a ⁣(t)v ⁣(t).\fc{\fc ja}v=\fr1{\V a^{p-1}}\int_0^1\d t\v{\fc at}^{p-2}\fc at\fc vt.

Why it is the unique subgradient

Suppose a∈R ⁣[t]∖{0}a\in\bfc\bR t\setminus\B0 and f∈J ⁣(a)f\in\fc Ja. Suppose f ⁣(v)=∫01dt f~ ⁣(t)v ⁣(t),\fc fv=\int_0^1\d t\,\fc{\tilde f}t\fc vt, where f~∈Lp/(p−1)[0,1]\tilde f\in L^{p/\p{p-1}}\b{0,1}. Any continuous functional on Lp[0,1]L^p\b{0,1} (the completion of R ⁣[t]\bfc\bR t with the Lp[0,1]L^p\b{0,1} norm) is of this form, and we have ∥f∥=∥f~∥\V f=\V{\tilde f}. By Definition 6, we have ∥f∥≤1\V f\le1 and f ⁣(a)=∥a∥\fc fa=\V a.

By Hölder’s inequality, we have f ⁣(a)≤∥f~∥∥a∥≤∥a∥.\fc fa\le\V{\tilde f}\V a\le\V a. On the other hand, f ⁣(a)=∥a∥\fc fa=\V a, so the inequalities are saturated. Hölder’s inequality is saturated iff ∣f~ ⁣(t)∣p/(p−1)\v{\fc{\tilde f}t}^{p/\p{p-1}} is a scalar multiple of ∣a ⁣(t)∣p\v{\fc at}^p and sgn⁡f~ ⁣(t)=sgn⁡a ⁣(t)\sgn\fc{\tilde f}t=\sgn\fc at (almost everywhere). The normalization ∥f~∥=1\V{\tilde f}=1 determines the normalization. In the end, we find that f~ ⁣(t)=∣a ⁣(t)∣p−2a ⁣(t)/∥a∥p−1\fc{\tilde f}t=\v{\fc at}^{p-2}\fc at/\V a^{p-1}.

Now pick any finite S⊆R ⁣[t]S\subseteq\bfc\bR t. We first show that the functionals j ⁣(S)\fc jS are linearly independent whenever the polynomials in SS are pairwise nonproportional (implying that none of them is zero). This is equivalent to showing that the functions ∣a ⁣(t)∣p−2a ⁣(t)\v{\fc at}^{p-2}\fc at for a∈Sa\in S are linearly independent.

Denote R≔{z∈C  |  ∏a∈Sa ⁣(z)=0}R\ceq\set{z\in\bC}{\prod_{a\in S}\fc az=0} (the set of all complex roots of the polynomials). Because SS is finite and each polynomial has finitely many roots, RR is finite. Therefore, (0,1)∖R\p{0,1}\setminus R is nonempty and open, and we can find an open interval (t0−δ,t0+δ)⊆[0,1]∖R\p{t_0-\dlt,t_0+\dlt}\subseteq\b{0,1}\setminus R. For each a∈Sa\in S, define qa≔asgn⁡a ⁣(t0)q_a\ceq a\sgn\fc a{t_0}, which is a polynomial that is positive on (t0−δ,t0+δ)\p{t_0-\dlt,t_0+\dlt}. We then have ∣a ⁣(t)∣p−2a ⁣(t)=sgn⁡a ⁣(t0)qa ⁣(t)p−1\v{\fc at}^{p-2}\fc at=\sgn\fc a{t_0}\fc{q_a}t^{p-1} on (t0−δ,t0+δ)\p{t_0-\dlt,t_0+\dlt}. Therefore, the linear independence of j ⁣(S)\fc jS is equivalent to the linear independence of qa ⁣(t)p−1\fc{q_a}t^{p-1}. Because p−1∉Qp-1\notin\bQ, when qaq_a are pairwise nonproportional, they are indeed linearly independent.

Why irrational powers of nonproportional polynomials are linearly independent

When R=∅R=\varnothing, then SS must be a singleton, and the claim is trivial. We assume R≠∅R\ne\varnothing from here.

For a∈Sa\in S and z∈Rz\in R, define maz≔ord⁡zam_{az}\ceq\opn{ord}_z a (the multiplicity of zz as a root of aa, which is also the multiplicity of zz as a root of qaq_a). Two nonproportional polynomials have different multiplicity vectors. For each z∈Rz\in R, choose nz∈Zn_z\in\bZ such that the integers Na≔∑z∈RmaznzN_a\ceq\sum_{z\in R}m_{az}n_z are distinct from each other for different a∈Sa\in S. Such a choice always exists: a simple construction is to choose nzn_z as powers of an integer b>max⁡a∈Smax⁡z∈Rmazb>\max_{a\in S}\max_{z\in R}m_{az}, and then NaN_a would be the base-bb encoding of the multiplicities of roots of aa, which is distinct for different aa because they are nonproportional.

Now consider the linear combination 0=∑a∈Sλaqa ⁣(t)p−1.0=\sum_{a\in S}\lmd_a\fc{q_a}t^{p-1}. Consider a contour starting from t∈(t0−δ,t0+δ)t\in\p{t_0-\dlt,t_0+\dlt} and going around each z∈Rz\in R by exactly rnzrn_z counterclockwise turns, where r∈Zr\in\bZ, and returning back to tt. Analytically continuing qa ⁣(t)p−1\fc{q_a}t^{p-1} along this contour, we get 0=∑a∈Sλaαarqa ⁣(t)p−1,0=\sum_{a\in S}\lmd_a\alp_a^r\fc{q_a}t^{p-1}, where αa≔e2πi(p−1)Na\alp_a\ceq\e^{2\pi\i\p{p-1}N_a}. Because p−1∉Qp-1\notin\bQ and all NaN_a are distinct, all αa\alp_a are distinct. Therefore, the Vandermonde matrix {αar}a∈S,0≤r<∣S∣\B{\alp_a^r}_{a\in S,0\le r<\v S} is invertible. Since qa ⁣(t)≠0\fc{q_a}t\ne0, we are forced to have λa=0\lmd_a=0.

Now let x∈P ⁣(S)∖Sx\in\fc PS\setminus S. We claim 0∈conv⁡j ⁣(S−x)0\in\opn{conv}\fc j{S-x}. Otherwise, applying the Hahn–Banach separation theorem to the weak*-compact convex hull gives v∈Xv\in X such that j ⁣(a−x) ⁣(v)<0\fc{\fc j{a-x}}v<0 for every a∈Sa\in S. Then we get x−tv∈I ⁣(S,x)x-tv\in\fc I{S,x} for sufficiently small t>0t>0, contradicting with x∈P ⁣(S)x\in\fc PS.

Why 0∈conv⁡j ⁣(S−x)0\in\opn{conv}\fc j{S-x}

Suppose for contradiction that 0∉conv⁡j ⁣(S−x)0\notin\opn{conv}\fc j{S-x}. Because conv⁡j ⁣(S−x)\opn{conv}\fc j{S-x} is a weak*-compact and convex, by the Hahn–Banach separation theorem, there exists v∈Xv\in X (the set of weak*-continuous linear functionals on X∗X^*) such that ∀a∈S:j ⁣(a−x) ⁣(v)<0.\forall a\in S:\fc{\fc j{a-x}}v<0. By the uniqueness of subgradients we established before, we know J ⁣(a−x)={j ⁣(a−x)}\fc J{a-x}=\B{\fc j{a-x}}. By Theorem 9, we have ∂v∥a−x∥=max⁡f∈J ⁣(a−x)f ⁣(v)=j ⁣(a−x) ⁣(v)<0.\partial_v\V{a-x}=\max_{f\in\fc J{a-x}}\fc fv=\fc{\fc j{a-x}}v<0. There then exists δa>0\dlt_a>0 such that ∀t∈(0,δa):∥a−x+tv∥−∥a−x∥t<j ⁣(a−x) ⁣(v)+∣j ⁣(a−x) ⁣(v)∣=0.\forall t\in\p{0,\dlt_a}:\fr{\V{a-x+tv}-\V{a-x}}t<\fc{\fc j{a-x}}v+\v{\fc{\fc j{a-x}}v}=0. Pick t≔min⁡a∈Sδa/2t\ceq\min_{a\in S}\dlt_a/2. We then have ∥a−x+tv∥<∥a−x∥\V{a-x+tv}<\V{a-x} for every a∈Sa\in S. Therefore, x−tv∈I ⁣(S,x)x-tv\in\fc I{S,x}, contradicting with x∈P ⁣(S)x\in\fc PS.

Thus there are λa≥0\lmd_a\ge0 with ∑aλa=1\sum_a\lmd_a=1 and ∑aλaj ⁣(a−x)=0\sum_a\lmd_a\fc j{a-x}=0. Therefore j ⁣(S−x)\fc j{S-x} is linearly dependent, so some of the polynomials in S−xS-x are proportional. Consider the equivalence classes of SS under the relation that a−xa-x and a′−xa'-x are proportional, and denote the equivalence class of aa by [a]\b a. We necessarily have ∑a∈[a′]λaj ⁣(a−x)=0\sum_{a\in\b{a'}}\lmd_a\fc j{a-x}=0 for any a′∈Sa'\in S.

There must exist a∈Sa\in S such that λa>0\lmd_a>0. To balance it, there also must exist a′∈[a]a'\in\b a such that λa′>0\lmd_{a'}>0 and that j ⁣(a−x)\fc j{a-x} and j ⁣(a′−x)\fc j{a'-x} are oppositely directed. Because a−xa-x and a′−xa'-x are parallel and because of Equation 3, a−xa-x and a′−xa'-x must be oppositely directed as well. This means x∈conv⁡{a,a′}⊆conv⁡Sx\in\opn{conv}\B{a,a'}\subseteq\opn{conv}S. Therefore, P ⁣(S)⊆conv⁡S=conv‾⁡S\fc PS\subseteq\opn{conv}S=\opn{\overline{conv}}S.

Why R ⁣[t]\bfc\bR t with Lp[0,1]L^p\b{0,1} norm does not satisfy P⊂cP_\subset^\mrm c

First, we claim that there exists ε∈(0,+∞)\veps\in\p{0,+\infty} such that there exists a unique c∈(0,+∞)c\in\p{0,+\infty} such that ∫02πdθ2π∣g ⁣(θ)−c∣p−2(g ⁣(θ)−c)=0,\int_0^{2\pi}\fr{\d\tht}{2\pi}\v{\fc g\tht-c}^{p-2}\p{\fc g\tht-c}=0, where g ⁣(θ)≔cos⁡θ+εcos⁡2θ\fc g\tht\ceq\cos\tht+\veps\cos2\tht.

Why the claim is true

This argument works for any p∈(2,+∞)p\in\p{2,+\infty}.

Define g~ ⁣(ε,c)≔∫02πdθ2π∣g ⁣(θ)−c∣p−2(g ⁣(θ)−c).\fc{\tilde g}{\veps,c}\ceq\int_0^{2\pi}\fr{\d\tht}{2\pi}\v{\fc g\tht-c}^{p-2}\p{\fc g\tht-c}. First we evaluate g~ ⁣(0,0)=0\fc{\tilde g}{0,0}=0.

Calculation g~ ⁣(0,0)=∫02πdθ2π∣cos⁡θ∣p−2cos⁡θ=∫0πdθ2π∣cos⁡θ∣p−2cos⁡θ+∫0πdθ2π∣cos⁡ ⁣(π+θ)∣p−2cos⁡ ⁣(π+θ)=∫0πdθ2π∣cos⁡θ∣p−2cos⁡θ−∫0πdθ2π∣cos⁡θ∣p−2cos⁡θ=0.\begin{align*} \fc{\tilde g}{0,0} &=\int_0^{2\pi}\fr{\d\tht}{2\pi}\v{\cos\tht}^{p-2}\cos\tht\\ &=\int_0^\pi\fr{\d\tht}{2\pi}\v{\cos\tht}^{p-2}\cos\tht+\int_0^\pi\fr{\d\tht}{2\pi}\v{\fc\cos{\pi+\tht}}^{p-2}\fc\cos{\pi+\tht}\\ &=\int_0^\pi\fr{\d\tht}{2\pi}\v{\cos\tht}^{p-2}\cos\tht-\int_0^\pi\fr{\d\tht}{2\pi}\v{\cos\tht}^{p-2}\cos\tht\\ &=0. \end{align*}

Then, we find k≔dg~ ⁣(ε,0)dε∣ε=0=(p−1)(p−2)p∫02πdθ2π∣cos⁡θ∣p−2>0.k\ceq\abar{\fr{\d\fc{\tilde g}{\veps,0}}{\d\veps}}{\veps=0} =\fr{\p{p-1}\p{p-2}}p\int_0^{2\pi}\fr{\d\tht}{2\pi}\v{\cos\tht}^{p-2}>0.

Calculation

By the Leibniz integral rule, we have dg~ ⁣(ε,0)dε=∫02πdθ2π∂∂ε(∣g ⁣(θ)∣p−1sgn⁡g ⁣(θ)).\fr{\d\fc{\tilde g}{\veps,0}}{\d\veps} =\int_0^{2\pi}\fr{\d\tht}{2\pi}\fr{\partial}{\partial\veps}\p{\v{\fc g\tht}^{p-1}\sgn\fc g\tht}. Notice that ∂g ⁣(θ)/∂ε=2cos⁡2θ−1\partial\fc g\tht/\partial\veps=2\cos^2\tht-1. We then have dg~ ⁣(ε,0)dε=(p−1)∫02πdθ2π∣g ⁣(θ)∣p−2(2cos⁡2θ−1).\fr{\d\fc{\tilde g}{\veps,0}}{\d\veps} =\p{p-1}\int_0^{2\pi}\fr{\d\tht}{2\pi}\v{\fc g\tht}^{p-2}\p{2\cos^2\tht-1}. When ε=0\veps=0, we have g ⁣(θ)=cos⁡θ\fc g\tht=\cos\tht, so dg~ ⁣(ε,0)dε∣ε=0=2(p−1)∫02πdθ2π∣cos⁡θ∣p−(p−1)∫02πdθ2π∣cos⁡θ∣p−2.\abar{\fr{\d\fc{\tilde g}{\veps,0}}{\d\veps}}{\veps=0} =2\p{p-1}\int_0^{2\pi}\fr{\d\tht}{2\pi}\v{\cos\tht}^p-\p{p-1}\int_0^{2\pi}\fr{\d\tht}{2\pi}\v{\cos\tht}^{p-2}.

Integrating by parts, we get ∫02πdθ2π∣cos⁡θ∣p=∫02πdsin⁡θ2π∣cos⁡θ∣p−1sgn⁡cos⁡θ=sin⁡θ2π∣cos⁡θ∣psgn⁡cos⁡θ∣02π−∫02πsin⁡θ2π d(∣cos⁡θ∣p−1sgn⁡cos⁡θ)=∫02πsin⁡θ2π(p−1)∣cos⁡θ∣p−2sin⁡θ dθ=(p−1)∫02πdθ2π∣cos⁡θ∣p−2−(p−1)∫02πdθ2π∣cos⁡θ∣p.\begin{align*} \int_0^{2\pi}\fr{\d\tht}{2\pi}\v{\cos\tht}^p &=\int_0^{2\pi}\fr{\d\sin\tht}{2\pi}\v{\cos\tht}^{p-1}\sgn\cos\tht\\ &=\abar{\fr{\sin\tht}{2\pi}\v{\cos\tht}^p\sgn\cos\tht}0^{2\pi} -\int_0^{2\pi}\fr{\sin\tht}{2\pi}\,\d\p{\v{\cos\tht}^{p-1}\sgn\cos\tht}\\ &=\int_0^{2\pi}\fr{\sin\tht}{2\pi}\p{p-1}\v{\cos\tht}^{p-2}\sin\tht\,\d\tht\\ &=\p{p-1}\int_0^{2\pi}\fr{\d\tht}{2\pi}\v{\cos\tht}^{p-2} -\p{p-1}\int_0^{2\pi}\fr{\d\tht}{2\pi}\v{\cos\tht}^p. \end{align*} Arranging the terms gives ∫02πdθ2π∣cos⁡θ∣p=p−1p∫02πdθ2π∣cos⁡θ∣p−2.\int_0^{2\pi}\fr{\d\tht}{2\pi}\v{\cos\tht}^p=\fr{p-1}p\int_0^{2\pi}\fr{\d\tht}{2\pi}\v{\cos\tht}^{p-2}.

Plugging this into the previous expression gives dg~ ⁣(ε,0)dε∣ε=0=(2(p−1)p−1p−(p−1))∫02πdθ2π∣cos⁡θ∣p−2.\abar{\fr{\d\fc{\tilde g}{\veps,0}}{\d\veps}}{\veps=0} =\p{2\p{p-1}\fr{p-1}p-\p{p-1}}\int_0^{2\pi}\fr{\d\tht}{2\pi}\v{\cos\tht}^{p-2}.

Therefore, there exists some ε∈(0,+∞)\veps\in\p{0,+\infty} such that g~ ⁣(ε,0)ε>k−k2>0.\fr{\fc{\tilde g}{\veps,0}}\veps>k-\fr k2>0.

On the other hand, the integrand of g~ ⁣(ε,c)\fc{\tilde g}{\veps,c} is strictly decreasing in cc and tends to −∞-\infty as c→+∞c\to+\infty, so g~ ⁣(ε,c)\fc{\tilde g}{\veps,c} tends to −∞-\infty as c→+∞c\to+\infty. By the intermediate value theorem, there exists a unique c∈(0,+∞)c\in\p{0,+\infty} such that g~ ⁣(ε,c)=0\fc{\tilde g}{\veps,c}=0.

For θ∈[0,2π]\tht\in\b{0,2\pi}, define aθ ⁣(t)≔(1+t2)2(g ⁣(2arctan⁡t−θ)−c).\fc{a_\tht}t\ceq\p{1+t^2}^2\p{\fc g{2\arctan t-\tht}-c}. It is a polynomial in tt of degree at most 44, so aθ∈R ⁣[t]a_\tht\in\bfc\bR t.

Define S≔{aθ  |  θ∈[0,2π]}S\ceq\set{a_\tht}{\tht\in\b{0,2\pi}}. Because a↦aθa\mapsto a_\tht is continuous, SS is compact. On the subspace of polynomials of degree at most 44, define a continuous linear functional f ⁣(t↦∑j=04bjtj)≔3b0+b2+3b4\fc f{t\mapsto\sum_{j=0}^4b_jt^j}\ceq3b_0+b_2+3b_4. We then have f ⁣(aθ)=−8c<0\fc f{a_\tht}=-8c<0 for every θ\tht. Since the subspace is closed, we have 0∉conv‾⁡S0\notin\opn{\overline{conv}}S.

Calculation

By the tangent half-angle formulas and the double angle formulas, we have cos⁡ ⁣(2arctan⁡t)=1−t21+t2,sin⁡ ⁣(2arctan⁡t)=2t1+t2,\fc\cos{2\arctan t}=\fr{1-t^2}{1+t^2},\qquad \fc\sin{2\arctan t}=\fr{2t}{1+t^2}, cos⁡ ⁣(4arctan⁡t)=2cos⁡ ⁣(2arctan⁡t)2−1=1−6t2+t4(1+t2)2,sin⁡ ⁣(4arctan⁡t)=2cos⁡ ⁣(2arctan⁡t)sin⁡ ⁣(2arctan⁡t)=4t−4t3(1+t2)2,\begin{align*} \fc\cos{4\arctan t}&=2\fc\cos{2\arctan t}^2-1=\fr{1-6t^2+t^4}{\p{1+t^2}^2},\\ \fc\sin{4\arctan t}&=2\fc\cos{2\arctan t}\fc\sin{2\arctan t}=\fr{4t-4t^3}{\p{1+t^2}^2}, \end{align*} cos⁡ ⁣(2arctan⁡t−θ)=cos⁡ ⁣(2arctan⁡t)cos⁡θ+sin⁡ ⁣(2arctan⁡t)sin⁡θ=1−t21+t2cos⁡θ+2t1+t2sin⁡θ,cos⁡ ⁣(4arctan⁡t−2θ)=cos⁡ ⁣(4arctan⁡t)cos⁡2θ+sin⁡ ⁣(4arctan⁡t)sin⁡2θ=1−6t2+t4(1+t2)2cos⁡2θ+4t−4t3(1+t2)2sin⁡2θ.\begin{align*} \fc\cos{2\arctan t-\tht}&=\fc\cos{2\arctan t}\cos\tht+\fc\sin{2\arctan t}\sin\tht\\ &=\fr{1-t^2}{1+t^2}\cos\tht+\fr{2t}{1+t^2}\sin\tht,\\ \fc\cos{4\arctan t-2\tht}&=\fc\cos{4\arctan t}\cos2\tht+\fc\sin{4\arctan t}\sin2\tht\\ &=\fr{1-6t^2+t^4}{\p{1+t^2}^2}\cos2\tht+\fr{4t-4t^3}{\p{1+t^2}^2}\sin2\tht. \end{align*} Substitute everything into the definition of aθa_\tht to get aθ ⁣(t)=(1+t2)((1−t2)cos⁡θ+(2t+2t3)sin⁡θ)=+ε((1−6t2+t4)cos⁡2θ+(4t−4t3)sin⁡2θ)−c(1+t2)2.\begin{align*} \fc{a_\tht}t&=\p{1+t^2}\p{\p{1-t^2}\cos\tht+\p{2t+2t^3}\sin\tht}\\ &\phantom{={}}{}+\veps\p{\p{1-6t^2+t^4}\cos2\tht+\p{4t-4t^3}\sin2\tht}-c\p{1+t^2}^2. \end{align*} One may get the coefficients b0=−c+cos⁡θ+εcos⁡2θ,b2=−2c−6εcos⁡2θ,b4=−c−cos⁡θ+εcos⁡2θ.\begin{align*} b_0&=-c+\cos\tht+\veps\cos2\tht,\\ b_2&=-2c-6\veps\cos2\tht,\\ b_4&=-c-\cos\tht+\veps\cos2\tht. \end{align*}

Alternatively, just use Wolfram!

(1 + t^2)^2 ((Cos[#] + \[Epsilon] Cos[2 #]) &[2 ArcTan[t] - \[Theta]] - c) //
	TrigExpand // CoefficientList[#, t] & // TrigReduce // MatrixForm

Suppose for contradiction that y∈I ⁣(S,0)y\in\fc I{S,0}. We then have ∀θ∈[0,2π]:∥aθ∥<∥y−aθ∥\forall\tht\in\b{0,2\pi}:\V{a_\tht}<\V{y-a_\tht}. Take the ppth power of both sides and integrate over θ\tht to get F ⁣(0)<F ⁣(y)\fc F0<\fc Fy, where F ⁣(y)≔∫02πdθ2π∥y−aθ∥p.\fc Fy\ceq\int_0^{2\pi}\fr{\d\tht}{2\pi}\V{y-a_\tht}^p.

After some calculation, one can show that F ⁣(y)=∫01dt(1+t2)2pG ⁣(y ⁣(t)(1+t2)2),\fc Fy=\int_0^1\d t\p{1+t^2}^{2p}\fc G{\fr{\fc yt}{\p{1+t^2}^2}}, where G ⁣(s)≔∫02πdθ2π∣s−g ⁣(θ)+c∣p.\fc Gs\ceq\int_0^{2\pi}\fr{\d\tht}{2\pi}\v{s-\fc g\tht+c}^p. The function GG is convex and continuously differentiable, and the definition of cc gives G′ ⁣(0)=0\fc{G'}0=0, so GG has its minimum at 00. This gives F ⁣(y)≥F ⁣(0)\fc Fy\ge\fc F0, contradicting with F ⁣(0)<F ⁣(y)\fc F0<\fc Fy.

Calculation

Expand the definition of the pp-norm to get F ⁣(y)=∫02πdθ2π∫01dt∣y ⁣(t)−(1+t2)2(g ⁣(2arctan⁡t−θ)−c)∣p.\fc Fy=\int_0^{2\pi}\fr{\d\tht}{2\pi}\int_0^1\d t\v{\fc yt-\p{1+t^2}^2\p{\fc g{2\arctan t-\tht}-c}}^p. Exchange the order of integration to get F ⁣(y)=∫01dt(1+t2)2p∫02πdθ2π∣y ⁣(t)(1+t2)2−g ⁣(2arctan⁡t−θ)+c∣p.\fc Fy=\int_0^1\d t\p{1+t^2}^{2p}\int_0^{2\pi}\fr{\d\tht}{2\pi}\v{\fr{\fc yt}{\p{1+t^2}^2}-\fc g{2\arctan t-\tht}+c}^p. Notice that gg is an even function and has period 2π2\pi, so we can change 2arctan⁡t−θ2\arctan t-\tht to θ\tht in the integrand. This gives F ⁣(y)=∫01dt(1+t2)2pG ⁣(y ⁣(t)(1+t2)2).\fc Fy=\int_0^1\d t\p{1+t^2}^{2p}\fc G{\fr{\fc yt}{\p{1+t^2}^2}}.

In G ⁣(s)\fc Gs, take the derivative using the Leibniz integral rule to get G′ ⁣(s)=∫02πdθ2π∂∂s∣s−g ⁣(θ)+c∣p=∫02πdθ2πp∣s−g ⁣(θ)+c∣p−1sgn⁡ ⁣(s−g ⁣(θ)+c).\begin{align*} \fc{G'}s&=\int_0^{2\pi}\fr{\d\tht}{2\pi}\fr{\partial}{\partial s}\v{s-\fc g\tht+c}^p\\ &=\int_0^{2\pi}\fr{\d\tht}{2\pi}p\v{s-\fc g\tht+c}^{p-1}\fc\sgn{s-\fc g\tht+c}. \end{align*} Therefore, G′ ⁣(0)=−p∫02πdθ2π∣g ⁣(θ)−c∣p−1sgn⁡ ⁣(g ⁣(θ)−c).\fc{G'}0=-p\int_0^{2\pi}\fr{\d\tht}{2\pi}\v{\fc g\tht-c}^{p-1}\fc\sgn{\fc g\tht-c}. By the definition of cc, we have G′ ⁣(0)=0\fc{G'}0=0.

Therefore, I ⁣(S,0)=∅\fc I{S,0}=\varnothing, so we have found a counterexample to P⊂cP_\subset^\mrm c.

An example of P⊂c∧¬P⊂bP_\subset^\mrm c\land\neg P_\subset^\mrm b is XX obtained through recursively defining a transfinite sequence {Xα}\B{X_\alp} of strictly convex spaces described as follows. We start with X0≔ℓ43X_0\ceq\ell_4^3. Then, for any ordinal number α\alp, define Xα+1≔Ξ ⁣(Xα,≤α)X_{\alp+1}\ceq\fc\Xi{X_\alp,\le_\alp}, where ≤α\le_\alp is a well-order on the set of all compact subsets of XαX_\alp whose closed convex hulls do not include zero, and the definition of Ξ\Xi will be given later. For any limit ordinal λ\lmd, define Xλ≔⋃α<λXαX_\lmd\ceq\bigcup_{\alp<\lmd}X_\alp. In the end, define X≔Xω1X\ceq X_{\omg_1}, where ω1\omg_1 is the first uncountable ordinal number. Then, XX sastisfies P⊂cP_\subset^\mrm c but does not satisfy P⊂bP_\subset^\mrm b.

Now, Ξ ⁣(Y,≤)\fc\Xi{Y,\le}, where YY is a normed space and ≤\le is a well-order on the compact subsets of YY whose closed convex hulls do not include zero, is defined as follows. First, assign ordinal labels to all compact subsets of YY whose closed convex hull does not include zero according to the well-order ≤\le and denote the compact set with ordinal label α<β\alp<\beta by KαK_\alp, where β\beta is the order type of ≤\le. Define a transfinite sequence {Yα}α≤β\B{Y_\alp}_{\alp\le\beta} of normed spaces as follows. We start with Y0≔YY_0\ceq Y. Then, for any α<β\alp<\beta, define Yα+1≔Yα⊕RY_{\alp+1}\ceq Y_\alp\oplus\bR equipped with the norm ∥(x,t)∥≔(1−δ2(4+δ))N ⁣(x,t)+δ2(4+δ)∥x∥2+t2,\V{\p{x,t}}\ceq\p{1-\fr\dlt{2\p{4+\dlt}}}\fc N{x,t}+\fr\dlt{2\p{4+\dlt}}\sqrt{\V x^2+t^2}, where δ≔min⁡a,a′∈Kα(∥a∥+∥a′∥−∥a−a′∥),\dlt\ceq\min_{a,a'\in K_\alp}\p{\V a+\V{a'}-\V{a-a'}}, N ⁣(x,t)≔inf⁡{A ⁣(x,K′,{λa})  |  λa∈R,finite K′⊆Kα,∑a∈K′λa=−t},\fc N{x,t}\ceq\inf\set{\fc A{x,K',\B{\lmd_a}}}{\lmd_a\in\bR,\text{finite $K'\subseteq K_\alp$},\sum_{a\in K'}\lmd_a=-t}, A ⁣(x,K′,{λa}a∈K′)≔∥x−∑a∈K′λaa∥+∑a∈K′∣λa∣(∥a∥−δ4).\fc A{x,K',\B{\lmd_a}_{a\in K'}}\ceq\V{x-\sum_{a\in K'}\lmd_aa}+\sum_{a\in K'}\v{\lmd_a}\p{\V a-\fr\dlt4}. Identify (x,0)=x\p{x,0}=x for any x∈Yαx\in Y_\alp so that Yα⊆Yα+1Y_\alp\subseteq Y_{\alp+1}, and one can prove that this inclusion is isometric. For any limit ordinal λ≤β\lmd\le\beta, define Yλ≔⋃α<λYαY_\lmd\ceq\bigcup_{\alp<\lmd}Y_\alp. In the end, define Ξ ⁣(Y,≤)≔Yβ\fc\Xi{Y,\le}\ceq Y_\beta.

Why XX satisfies P⊂cP_\subset^\mrm c

We can prove that an extension Yα⊆Yα+1Y_\alp\subseteq Y_{\alp+1} has the following properties, given that YαY_\alp is a strictly convex space: the norm on Yα+1Y_{\alp+1} satisfies the axioms of a norm and is strictly convex; YαY_\alp is a closed subspace of Yα+1Y_{\alp+1}; the inclusion map x↦(x,0)x\mapsto\p{x,0} is an isometry; and there exists v∈Yα+1v\in Y_{\alp+1} such that ∀a∈Kα:∥a−v∥<∥a∥\forall a\in K_\alp:\V{a-v}<\V a. Based on these properties, using transfinite induction, we can prove the following properties of Xα⊆Xα′X_\alp\subseteq X_{\alp'} for any α<α′\alp<\alp': Xα′X_{\alp'} is strictly convex; XαX_\alp is a closed subspace of Xα′X_{\alp'} with isometric inclusion; for any compact set K⊆XαK\subseteq X_\alp whose closed convex hull does not include zero, there exists v∈Xα′v\in X_{\alp'} such that ∀a∈K:∥a−v∥<∥a∥\forall a\in K:\V{a-v}<\V a.

Why Yα+1Y_{\alp+1} is a strictly convex space

It is sufficient to prove that the construction of NN is sublinear and nonnegative. Then, by the strict convexity of the norm on YαY_\alp and the strict convexity of (x,t)↦∥x∥2+t2\p{x,t}\mapsto\sqrt{\V x^2+t^2}, one can see that the norm on Yα+1Y_{\alp+1} is strictly convex.

First, by setting a=a′a=a' in the definition of δ\dlt, we see ∀a∈Kα:∥a∥≥δ/2\forall a\in K_\alp:\V a\ge\dlt/2. Also, δ\dlt is positive because YαY_\alp is strictly convex. We then have that AA is nonnegative.

The homogeneity and nonnegativity of NN is obvious from the homogeneity and nonnegativity of AA. The only real work lies in proving NN satisfies the triangle inequality.

Let (x1,t1)∈Yα+1\p{x_1,t_1}\in Y_{\alp+1}, K1′⊆KαK'_1\subseteq K_\alp be a finite set, and let {λ1a}a∈K1′\B{\lmd_{1a}}_{a\in K'_1} be real numbers such that ∑a∈K1′λ1a=−t1\sum_{a\in K'_1}\lmd_{1a}=-t_1. Similarly fix (x2,t2)\p{x_2,t_2}, K2′K'_2, and {λ2a}a∈K2′\B{\lmd_{2a}}_{a\in K'_2}. Define (x,t)≔(x1+x2,t1+t2),K′≔K1′∪K2′,λa≔{λ1a,a∈K1′,0,a∉K1′+{λ2a,a∈K2′,0,a∉K2′.\begin{align*} \p{x,t}&\ceq\p{x_1+x_2,t_1+t_2},\\ K'&\ceq K'_1\cup K'_2,\\ \lmd_a&\ceq\begin{dcases}\lmd_{1a},&a\in K'_1,\\0,&a\notin K'_1\end{dcases} +\begin{dcases}\lmd_{2a},&a\in K'_2,\\0,&a\notin K'_2.\end{dcases} \end{align*} Then, we have ∑a∈K′λa=−t\sum_{a\in K'}\lmd_a=-t.

We can then expand A ⁣(x,K′,{λa})=∥x−∑a∈K′λaa∥+∑a∈K′∣λa∣(∥a∥−δ4)≤∥x1+x2−∑a∈K1′λ1aa−∑a∈K2′λ2aa∥+∑a∈K1′∣λ1a∣(∥a∥−δ4)+∑a∈K2′∣λ2a∣(∥a∥−δ4)≤∥x1−∑a∈K1′λ1aa∥+∑a∈K1′∣λ1a∣(∥a∥−δ4)+∥x2−∑a∈K2′λ2aa∥+∑a∈K2′∣λ2a∣(∥a∥−δ4)=A ⁣(x1,K1′,{λ1a})+A ⁣(x2,K2′,{λ2a})\begin{align*} \fc A{x,K',\B{\lmd_a}} &=\V{x-\sum_{a\in K'}\lmd_aa}+\sum_{a\in K'}\v{\lmd_a}\p{\V a-\fr\dlt4}\\ &\le\V{x_1+x_2-\sum_{a\in K'_1}\lmd_{1a}a-\sum_{a\in K'_2}\lmd_{2a}a} +\sum_{a\in K'_1}\v{\lmd_{1a}}\p{\V a-\fr\dlt4} +\sum_{a\in K'_2}\v{\lmd_{2a}}\p{\V a-\fr\dlt4}\\ &\le\V{x_1-\sum_{a\in K'_1}\lmd_{1a}a}+\sum_{a\in K'_1}\v{\lmd_{1a}}\p{\V a-\fr\dlt4} +\V{x_2-\sum_{a\in K'_2}\lmd_{2a}a}+\sum_{a\in K'_2}\v{\lmd_{2a}}\p{\V a-\fr\dlt4}\\ &=\fc A{x_1,K'_1,\B{\lmd_{1a}}}+\fc A{x_2,K'_2,\B{\lmd_{2a}}} \end{align*}

Note that any choices of {λ1a}\B{\lmd_{1a}} and {λ2a}\B{\lmd_{2a}} can be used to construct such {λa}\B{\lmd_a}. Therefore, if you take the infimum, the inequality is preserved. Therefore, N ⁣(x,t)≤N ⁣(x1,t1)+N ⁣(x2,t2)\fc N{x,t}\le\fc N{x_1,t_1}+\fc N{x_2,t_2}.

Why YαY_\alp is a closed subspace of Yα+1Y_{\alp+1}

First, by setting a=a′a=a' in the definition of δ\dlt, we see ∀a∈Kα:∥a∥≥δ/2\forall a\in K_\alp:\V a\ge\dlt/2. Also, δ\dlt is positive because YαY_\alp is strictly convex.

Given ∑a∈K′λa=−t\sum_{a\in K'}\lmd_a=-t, we have A ⁣(x,K′,{λa})≥∑a∈K′∣λa∣(∥a∥−δ4)≥∑a∈K′∣λa∣(δ2−δ4)≥∣∑a∈K′λa∣δ4=∣t∣δ4.\fc A{x,K',\B{\lmd_a}}\ge\sum_{a\in K'}\v{\lmd_a}\p{\V a-\fr\dlt4} \ge\sum_{a\in K'}\v{\lmd_a}\p{\fr\dlt2-\fr\dlt4} \ge\v{\sum_{a\in K'}\lmd_a}\fr\dlt4=\v t\fr\dlt4. We then have N ⁣(x,t)≥∣t∣δ/4\fc N{x,t}\ge\v t\dlt/4. Therefore, ∥(x,t)∥≥(1−δ2(4+δ))∣t∣δ4+δ2(4+δ)∣t∣=δ(12+δ)8(4+δ)∣t∣.\V{\p{x,t}}\ge\p{1-\fr\dlt{2\p{4+\dlt}}}\v t\fr\dlt4+\fr\dlt{2\p{4+\dlt}}\v t =\fr{\dlt\p{12+\dlt}}{8\p{4+\dlt}}\v t. Therefore, any point in Yα+1∖YαY_{\alp+1}\setminus Y_\alp, i.e., any point with nonzero tt coordinate, has its distance to YαY_\alp bounded below by a positive number. It makes YαY_\alp closed in Yα+1Y_{\alp+1}.

Why the inclusion map is isometric

We need to calculate N ⁣(x,0)\fc N{x,0}. Given ∑a∈K′λa=0\sum_{a\in K'}\lmd_a=0, we define Λ≔∑λa>0λa=∑λa<0−λa.\Lmd\ceq\sum_{\lmd_a>0}\lmd_a=\sum_{\lmd_a<0}-\lmd_a. If Λ>0\Lmd>0, we have ∥∑a∈K′λaa∥=∥∑λa>0λaa+∑λa′<0(−λa′)(−a′)∥=∥(1Λ∑λa′<0−λa′)∑λa>0λaa+(1Λ∑λa>0λa)∑λa′<0(−λa′)(−a′)∥=∥∑λa>0λa′<0λa(−λa′)Λ(a−a′)∥≤∑λa>0λa′<0λa(−λa′)Λ∥a−a′∥≤∑λa>0λa′<0λa(−λa′)Λ(∥a∥−∥a′∥−δ)=(1Λ∑λa′<0−λa′)∑λa>0λa(∥a∥−δ2)+(1Λ∑λa>0λa)∑λa′<0(−λa′)(∥a′∥−δ2)=∑a∈K′∣λa∣(∥a∥−δ2).\begin{align*} \V{\sum_{a\in K'}\lmd_aa} &=\V{\sum_{\lmd_a>0}\lmd_aa+\sum_{\lmd_{a'}<0}\p{-\lmd_{a'}}\p{-a'}}\\ &=\V{\p{\fr1\Lmd\sum_{\lmd_{a'}<0}-\lmd_{a'}}\sum_{\lmd_a>0}\lmd_aa +\p{\fr1\Lmd\sum_{\lmd_a>0}\lmd_a}\sum_{\lmd_{a'}<0}\p{-\lmd_{a'}}\p{-a'}}\\ &=\V{\sum_{\substack{\lmd_a>0\\\lmd_{a'}<0}}\fr{\lmd_a\p{-\lmd_{a'}}}\Lmd\p{a-a'}} \le\sum_{\substack{\lmd_a>0\\\lmd_{a'}<0}}\fr{\lmd_a\p{-\lmd_{a'}}}\Lmd\V{a-a'}\\ &\le\sum_{\substack{\lmd_a>0\\\lmd_{a'}<0}}\fr{\lmd_a\p{-\lmd_{a'}}}\Lmd\p{\V a-\V {a'}-\dlt}\\ &=\p{\fr1\Lmd\sum_{\lmd_{a'}<0}-\lmd_{a'}}\sum_{\lmd_a>0}\lmd_a\p{\V a-\fr\dlt2} +\p{\fr1\Lmd\sum_{\lmd_a>0}\lmd_a}\sum_{\lmd_{a'}<0}\p{-\lmd_{a'}}\p{\V{a'}-\fr\dlt2}\\ &=\sum_{a\in K'}\v{\lmd_a}\p{\V a-\fr\dlt2}. \end{align*} The same inequality is true if Λ=0\Lmd=0.

We then have A ⁣(x,K′,{λa})=∥x−∑a∈K′λaa∥+∑a∈K′∣λa∣(∥a∥−δ4)≥∥x∥−∥∑a∈K′λaa∥+∑a∈K′∣λa∣(∥a∥−δ4)≥∥x∥−∑a∈K′∣λa∣(∥a∥−δ2)+∑a∈K′∣λa∣(∥a∥−δ4)=∥x∥+∑a∈K′∣λa∣δ4≥∥x∥+∣∑a∈K′λa∣δ4=∥x∥.\begin{align*} \fc A{x,K',\B{\lmd_a}} &=\V{x-\sum_{a\in K'}\lmd_aa}+\sum_{a\in K'}\v{\lmd_a}\p{\V a-\fr\dlt4}\\ &\ge\V x-\V{\sum_{a\in K'}\lmd_aa}+\sum_{a\in K'}\v{\lmd_a}\p{\V a-\fr\dlt4}\\ &\ge\V x-\sum_{a\in K'}\v{\lmd_a}\p{\V a-\fr\dlt2}+\sum_{a\in K'}\v{\lmd_a}\p{\V a-\fr\dlt4}\\ &=\V x+\sum_{a\in K'}\v{\lmd_a}\fr\dlt4 \ge\V x+\v{\sum_{a\in K'}\lmd_a}\fr\dlt4=\V x. \end{align*} Therefore, N ⁣(x,0)≥∥x∥\fc N{x,0}\ge\V x. On the other hand, N ⁣(x,0)≤A ⁣(x,∅,{})=∥x∥\fc N{x,0}\le\fc A{x,\varnothing,\B{}}=\V x. Therefore, N ⁣(x,0)=∥x∥\fc N{x,0}=\V x.

Plug this into the definition of the norm, and we have ∥(x,0)∥=∥x∥\V{\p{x,0}}=\V x.

Why ∀a∈Kα:∥a−v∥<∥a∥\forall a\in K_\alp:\V{a-v}<\V a

We have N ⁣(a,−1)≤A ⁣(a,{a},{1})=∥a∥−δ4.\fc N{a,-1}\le\fc A{a,\B a,\B1}=\V a-\fr\dlt4.

Pick v≔(0,−1)v\ceq\p{0,-1}, and we have ∥a−v∥=∥(a,−1)∥=(1−δ2(4+δ))N ⁣(a,−1)+δ2(4+δ)∥a∥2+1≤(1−δ2(4+δ))(∥a∥−δ4)+δ2(4+δ)(∥a∥+1)=∥a∥−δ8<∥a∥.\begin{align*} \V{a-v}&=\V{\p{a,-1}}\\ &=\p{1-\fr\dlt{2\p{4+\dlt}}}\fc N{a,-1}+\fr\dlt{2\p{4+\dlt}}\sqrt{\V a^2+1}\\ &\le\p{1-\fr\dlt{2\p{4+\dlt}}}\p{\V a-\fr\dlt4}+\fr\dlt{2\p{4+\dlt}}\p{\V a+1}\\ &=\V a-\fr\dlt8<\V a. \end{align*}

Transfinite induction

First, we need to prove a bunch of properties that all spaces in the {Yα}\B{Y_\alp} transfinite sequence in the construction of Ξ\Xi have. The successor steps for proving these properties are already done, so we consider the limit steps. Suppose λ\lmd is a limit ordinal.

We have that Yλ=⋃α<λYαY_\lmd=\bigcup_{\alp<\lmd}Y_\alp is a strictly convex space. It is a normed space in the first place because any of its vectors belongs to some Yα<λY_{\alp<\lmd}, and it is a normed space. It is strictly convex because any two of its vectors belong to some YαY_\alp and Yα′Y_{\alp'} respectively, so they belong to Ymax⁡ ⁣(α,α′)Y_{\opc{max}{\alp,\alp'}}, which is a strictly convex space.

We have that any Yα<λY_{\alp<\lmd} is a closed subspace of YλY_\lmd. This is because it is a closed subspace of Yα+1Y_{\alp+1}, which in turn is a subspace of YλY_\lmd.

For any α<λ\alp<\lmd, there exists v∈Yλv\in Y_\lmd such that ∀a∈Kα:∥a−v∥<∥a∥\forall a\in K_\alp:\V{a-v}<\V a. This is because such vv can be found in Yα+1Y_{\alp+1}, which is a subspace of YλY_\lmd.

Now we can apply these properties to Ξ ⁣(Y,≤)\fc\Xi{Y,\le} as it is an element in the sequence {Yα}\B{Y_\alp}. It is a strictly convex space, and it contains YY as a closed subspace, and for any compact set K⊆YK\subseteq Y whose closed convex hull does not include zero, there exists v∈Ξ ⁣(Y,≤)v\in\fc\Xi{Y,\le} such that ∀a∈Y:∥a−v∥≤∥a∥\forall a\in Y:\V{a-v}\le\V a.

With these properties on Ξ\Xi, we can do another transfinite induction to get the properties for all spaces in the {Xα}\B{X_\alp} transfinite sequence.

We now show that every compact set K⊆XK\subseteq X is contained in some XαX_\alp. A compact metric space is always separable, so KK has a countable dense subset {an}n<ω\B{a_n}_{n<\omg}. Because X=⋃α<ω1XαX=\bigcup_{\alp<\omg_1}X_\alp, for each nn, there exists αn<ω1\alp_n<\omg_1 such that an∈Xαna_n\in X_{\alp_n}. The supremum α≔sup⁡nαn\alp\ceq\sup_n\alp_n is still a countable ordinal. We then have an∈Xαa_n\in X_\alp. Because XαX_\alp is closed in XX, we have K⊆XαK\subseteq X_\alp.

Now let S⊆XS\subseteq X be a compact set and x∉conv‾⁡Sx\notin\opn{\overline{conv}}S. Then K≔S−xK\ceq S-x is a compact set whose closed convex hull does not include zero. It is contained in some XαX_\alp, so there exists some v∈Xα+1v\in X_{\alp+1} such that ∀a∈S:∥a−x−v∥<∥a−x∥\forall a\in S:\V{a-x-v}<\V{a-x}. This means x+v∈I ⁣(S,x)x+v\in\fc I{S,x}. This proves that XX satisfies P⊂cP_\subset^\mrm c.

Note on the economic Pareto efficiency

As explained in the background, the concept that is more commonly used in economics is neither the strong Pareto efficiency nor the weak Pareto efficiency. In the context of this article, the set of economic Pareto improvements can be defined as I~ ⁣(S,x)≔⋃a∈S(B ⁣(a,∥x−a∥)∩Iˉ ⁣(S,x)),\fc{\tilde I}{S,x}\ceq\bigcup_{a\in S}\p{\fc B{a,\V{x-a}}\cap\fc{\bar I}{S,x}}, and the economic Pareto set can be defined as P~ ⁣(S)≔{x∈X  |  I~ ⁣(S,x)=∅}.\fc{\tilde P}S\ceq\set{x\in X}{\fc{\tilde I}{S,x}=\varnothing}. Then, we can similarly define the properties P~⊃,⊂f,c,b,a\tilde P_{\supset,\subset}^{\mrm f,\mrm c,\mrm b,\mrm a}.

Although the economic Pareto efficiency is not the focus of this article, some of the characterizations of the properties P~⊃,⊂f,c,b,a\tilde P_{\supset,\subset}^{\mrm f,\mrm c,\mrm b,\mrm a} can be derived for free given the results we have already established. First, we obviously have Pˉ ⁣(S)⊆P~ ⁣(S)⊆P ⁣(S)\fc{\bar P}S\subseteq\fc{\tilde P}S\subseteq\fc PS for any S⊆XS\subseteq X. Second, the proof of Theorem 1 can be directly ported to prove that a non-strictly convex space does not satisfy P~⊂f\tilde P_\subset^\mrm f. Third, Theorem 3 states that a strictly convex space has Pˉ ⁣(S)=P~ ⁣(S)=P ⁣(S)\fc{\bar P}S=\fc{\tilde P}S=\fc PS. These observations immediately give the exact characterizations of P~⊂f,c,b,a\tilde P_\subset^{\mrm f,\mrm c,\mrm b,\mrm a} in finite-dimensional spaces, which are the same as those of P⊂f,c,b,aP_\subset^{\mrm f,\mrm c,\mrm b,\mrm a}. For infinite-dimensional spaces, only P~⊂a\tilde P_\subset^\mrm a is exactly characterized because only P⊂aP_\subset^\mrm a is exactly characterized. The third observation also immediately gives the exact characterizations of P~⊃f,c,b,a\tilde P_\supset^{\mrm f,\mrm c,\mrm b,\mrm a} in non-planar spaces, which are the same as those of P⊃f,c,b,aP_\supset^{\mrm f,\mrm c,\mrm b,\mrm a} (or Pˉ⊃f,c,b,a\bar P_\supset^{\mrm f,\mrm c,\mrm b,\mrm a}, which are the same). Only the planar case needs additional work.