4. Proof of monotonicity

Lemma 4.1.

For all γ𝕁\gamma\in\mathbb{J} and all x,y𝕌x,y\in\mathbb{U} with x>y>x>y>\mathbb{R}, we have:

  1. (1)

    if γxγy1\gamma\circ x-\gamma\circ y\preceq 1, then γxγyxyγy\frac{\gamma\circ x-\gamma\circ y}{x-y}\preceq\gamma^{\prime}\circ y,

  2. (2)

    if γxγy1\gamma\circ x-\gamma\circ y\succeq 1, then (γy)(xy)1(\gamma^{\prime}\circ y)(x-y)\succeq 1.

Proof.

Fix xx, yy as in the assumptions. Let γ𝕁\gamma\in\mathbb{J}. We shall prove the conclusion by induction on ER(γ)\mathrm{ER}(\gamma).

When γ\gamma is logn(T)\log^{\circ n}(T) for some nn, both conclusions hold because logn\log^{\circ n} is concave: 0<logn(a)logn(b)ab(logn)(b)0<\frac{\log^{\circ n}(a)-\log^{\circ n}(b)}{a-b}\leq(\log^{\circ n})^{\prime}% (b) for any bb in its domain and a>ba>b, and so also for x>y>x>y>\mathbb{R}. The conclusion is trivial for γ=0\gamma=0.

Now assume ER(γ)>0\mathrm{ER}(\gamma)>0 and let reδre^{\delta} be the leading term of γ\gamma. Recall that δ𝕁>0\delta\in\mathbb{J}^{>0} and that ER(δ)<ER(γ)\mathrm{ER}(\delta)<\mathrm{ER}(\gamma). By Proposition 3.2, we have

γxγyr(eδxeδy)=reδy(eδxδy1),\gamma\circ x-\gamma\circ y\sim r(e^{\delta\circ x}-e^{\delta\circ y})=re^{% \delta\circ y}(e^{\delta\circ x-\delta\circ y}-1),

which we rewrite as

γxγyxyreδyeδxδy1xy.\frac{\gamma\circ x-\gamma\circ y}{x-y}\sim re^{\delta\circ y}\frac{e^{\delta% \circ x-\delta\circ y}-1}{x-y}.

Recall moreover that since γreδ\gamma\sim re^{\delta} and γ1\gamma\not\asymp 1, we have γreδδ\gamma^{\prime}\sim re^{\delta}\delta^{\prime}, so in particular γyreδy(δy)\gamma^{\prime}\circ y\sim re^{\delta\circ y}(\delta^{\prime}\circ y).

We distinguish two cases. If δxδy1\delta\circ x-\delta\circ y\prec 1, then we can use the Taylor expansion of exp\exp to check that

eδxδy1xyδxδyxyδy,\frac{e^{\delta\circ x-\delta\circ y}-1}{x-y}\sim\frac{\delta\circ x-\delta% \circ y}{x-y}\preceq\delta^{\prime}\circ y,

where the second inequality follows from the inductive hypothesis (1). Therefore,

γyγyxyreδyeδxδy1xyreδy(δy)γy.\frac{\gamma\circ y-\gamma\circ y}{x-y}\sim re^{\delta\circ y}\frac{e^{\delta% \circ x-\delta\circ y}-1}{x-y}\preceq re^{\delta\circ y}(\delta^{\prime}\circ y% )\sim\gamma^{\prime}\circ y.

Both conclusions follow trivially.

Now suppose that δxδy1\delta\circ x-\delta\circ y\succeq 1. Note in particular that γxγy1\gamma\circ x-\gamma\circ y\succ 1, because eδy1e^{\delta\circ y}\succ 1 and eδxδy11e^{\delta\circ x-\delta\circ y}-1\succeq 1, so we only need to prove conclusion (2). By inductive hypothesis (2), (δy)(xy)1(\delta^{\prime}\circ y)(x-y)\succeq 1, which with eδy1e^{\delta\circ y}\succ 1 yields (2):

(γy)(xy)reδy(δy)(xy)1.(\gamma^{\prime}\circ y)(x-y)\sim re^{\delta\circ y}(\delta^{\prime}\circ y)(x% -y)\succ 1.\qed
Corollary 4.2.

For all γ𝕁<0\gamma\in\mathbb{J}^{<0} and all x,y𝕌x,y\in\mathbb{U} with x>y>x>y>\mathbb{R}, we have

eγxeγyxyeγy(γy)=(eγ)y.\frac{e^{\gamma\circ x}-e^{\gamma\circ y}}{x-y}\preceq e^{\gamma\circ y}(% \gamma^{\prime}\circ y)=(e^{\gamma})^{\prime}\circ y.
Proof.

Write

eγxeγy=eγy(eγxγy1).e^{\gamma\circ x}-e^{\gamma\circ y}=e^{\gamma\circ y}(e^{\gamma\circ x-\gamma% \circ y}-1).

If γxγy1\gamma\circ x-\gamma\circ y\prec 1, then using Lemma 4.1(1)

eγy(eγxγy1)eγy(γxγy)eγy(γy)(xy).e^{\gamma\circ y}(e^{\gamma\circ x-\gamma\circ y}-1)\sim e^{\gamma\circ y}(% \gamma\circ x-\gamma\circ y)\preceq e^{\gamma\circ y}(\gamma^{\prime}\circ y)(% x-y).

Otherwise, eγxγy≁1e^{\gamma\circ x-\gamma\circ y}\not\sim 1, and since γx<γy\gamma\circ x<\gamma\circ y by Proposition 3.1 applied to γ-\gamma, we have eγxγy1e^{\gamma\circ x-\gamma\circ y}\preceq 1, thus

eγy(eγxγy1)eγyeγy(γy)(xy),e^{\gamma\circ y}(e^{\gamma\circ x-\gamma\circ y}-1)\asymp e^{\gamma\circ y}% \preceq e^{\gamma\circ y}(\gamma^{\prime}\circ y)(x-y),

where the last inequality follows from Lemma 4.1(2). ∎

Proof of Theorem A.

Let x,y𝕌x,y\in\mathbb{U} with x>y>x>y>\mathbb{R} and fTf\in\mathbb{R}\langle\!\langle T\rangle\!\rangle. Trivially, when f=0f^{\prime}=0, we have f=rf=r\in\mathbb{R}, so rx=ry=rr\circ x=r\circ y=r, as desired. We now assume that f>0f^{\prime}>0, and we want to prove fx>fyf\circ x>f\circ y. The case f<0f^{\prime}<0 will follow trivially by replacing ff with f-f.

Case f=T+εf=T+\varepsilon with εT\varepsilon\prec T. Note that in this case f1f^{\prime}\sim 1, so f>0f^{\prime}>0. We claim that εxεyxy\varepsilon\circ x-\varepsilon\circ y\prec x-y, and so fxfyxyf\circ x-f\circ y\sim x-y, which clearly implies fx>fyf\circ x>f\circ y.

Suppose that eγe^{\gamma} is a monomial in the support of ε\varepsilon. We claim that eγxeγyxye^{\gamma\circ x}-e^{\gamma\circ y}\prec x-y. This is trivial for γ=0\gamma=0, and an immediate consequence of Proposition 3.2 for γ>0\gamma>0. For γ<0\gamma<0, we have 1(eγ)1\succ(e^{\gamma})^{\prime}, so 1(eγ)y1\succ(e^{\gamma})^{\prime}\circ y, hence by Corollary 4.2

eγxeγyeγy(γy)(xy)=((eγ)y)(xy)xy.e^{\gamma\circ x}-e^{\gamma\circ y}\preceq e^{\gamma\circ y}(\gamma^{\prime}% \circ y)(x-y)=((e^{\gamma})^{\prime}\circ y)(x-y)\prec x-y.

Taking the sum over all terms in ε\varepsilon, we find that εxεyxy\varepsilon\circ x-\varepsilon\circ y\prec x-y.

Case f>f>\mathbb{R}. Recall that T\mathbb{R}\langle\!\langle T\rangle\!\rangle is confluent, because for any gT>g\in\mathbb{R}\langle\!\langle T\rangle\!\rangle^{>\mathbb{R}}, the leading monomials along the sequence (logn(g):n)(\log^{\circ n}(g):n\in\mathbb{N}) must have decreasing exponential rank, until one reaches logk(T)\log^{\circ k}(T) for some kk. Pick nn\in\mathbb{N} such that logn(T)f=logn(f)=logk(T)+ε\log^{\circ n}(T)\circ f=\log^{\circ n}(f)=\log^{\circ k}(T)+\varepsilon for some kk\in\mathbb{N} and some εlogk(T)\varepsilon\prec\log^{\circ k}(T). Note that

logn(T)fexpk(T)=T+ε¯\log^{\circ n}(T)\circ f\circ\exp^{\circ k}(T)=T+\overline{\varepsilon}

where ε¯=εexpk(T)logk(T)expk(T)=T\overline{\varepsilon}=\varepsilon\circ\exp^{\circ k}(T)\prec\log^{\circ k}(T)% \circ\exp^{\circ k}(T)=T. By the previous case, the function xx+(ε¯x)x\mapsto x+(\overline{\varepsilon}\circ x) is strictly increasing. Since the functions log\log and exp\exp are also strictly increasing on 𝕌>\mathbb{U}^{>\mathbb{R}}, then so is the function xfxx\mapsto f\circ x.

Case ff\not>\mathbb{R}. Since by assumption f>0f^{\prime}>0, we cannot have f<f<\mathbb{R}, so there must be some rr\in\mathbb{R} such that fr1f-r\prec 1, and moreover fr<0f-r<0. It follows that g=1fr>g=-\frac{1}{f-r}>\mathbb{R}. By the previous case, the function xgxx\mapsto g\circ x is strictly increasing, thus so is the function

x1gx+r=fx.x\mapsto-\frac{1}{g\circ x}+r=f\circ x.\qed
Corollary 4.3.

For all f,gTf,g\in\mathbb{R}\langle\!\langle T\rangle\!\rangle with 1fg1\not\asymp f\succ g and all x,y𝕌x,y\in\mathbb{U} with x>y>x>y>\mathbb{R}, we have

fxfygxgy.f\circ x-f\circ y\succ g\circ x-g\circ y.
Proof.

Up to replacing ff with f-f, we may assume that f>0f^{\prime}>0. Since f1f\not\asymp 1, we have fgf^{\prime}\succ g^{\prime}, thus frg=(frg)>0f^{\prime}-rg^{\prime}=(f-rg)^{\prime}>0 for every rr\in\mathbb{R}. By Theorem A,

(frg)x>(frg)y,hencefxfy>r(gxgy).(f-rg)\circ x>(f-rg)\circ y,\quad\text{hence}\quad f\circ x-f\circ y>r(g\circ x% -g\circ y).

Moreover, fxfy>0f\circ x-f\circ y>0, and the conclusion follows. ∎

Corollary 4.4.

For all f,gTf,g\in\mathbb{R}\langle\!\langle T\rangle\!\rangle with 1fg1\not\asymp f\sim g and all x,y𝕌x,y\in\mathbb{U} with x>y>x>y>\mathbb{R}, we have

fxfygxgy.f\circ x-f\circ y\sim g\circ x-g\circ y.
Proof.

Apply Corollary 4.3 to ff and fgff-g\prec f. ∎

Proof of Corollary B.

Fix fTf\in\mathbb{R}\langle\!\langle T\rangle\!\rangle, x,y𝕌>x,y\in\mathbb{U}^{>\mathbb{R}}, w𝕌w\in\mathbb{U} such that fxwfyf\circ x\leq w\leq f\circ y. Note that the case ff\in\mathbb{R} is trivial, so assume ff\notin\mathbb{R}. There is z𝕌>z\in\mathbb{U}^{>\mathbb{R}} such that fz=wf\circ z=w: when f>f>\mathbb{R}, just take z=finvwz=f^{\mathrm{inv}}\circ w, where finvT>f^{\mathrm{inv}}\in\mathbb{R}\langle\!\langle T\rangle\!\rangle^{>\mathbb{R}} is the compositional inverse of ff ([6]); otherwise, replace ff with ±1fr>\pm\frac{1}{f-r}>\mathbb{R} just as in the proof of Theorem A, and reduce to f>f>\mathbb{R}. By Theorem A, zz has to be between xx and yy. ∎