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Proof of The Exponential Bump Building Block is Smooth on the Real Line

lemmalem:exponential-bump-smooth-2026a
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Reason: Proof that exp(-1/s) extended by zero is smooth, via the family of functions q(1/s)exp(-1/s) with q polynomial.

Proof

Throughout, R\mathbb{R} is an interval all of whose points are interior points of it, by claim 1 of One-Dimensional Derivatives, Partial Derivatives, and Smoothness on the Real Line; differentiability of a function defined on an interval, at an interior point of that interval, is that of Derivative at an Interior Point. Absolute values are those of that definition, with the properties collected in Properties of the Absolute Value in an Ordered Field; the order arithmetic used below is that of Elementary Order Arithmetic in an Ordered Field, and 22 denotes 1+11+1. For w∈Rw\in\mathbb{R} we abbreviate wβ‹…ww\cdot w by w2w^{2}.

Step 1 (the two open half-lines). Put P={s∈R:0<s}P=\{s\in\mathbb{R}:0<s\} and N={s∈R:s<0}N=\{s\in\mathbb{R}:s<0\}. We check that each is an interval all of whose points are interior points of it.

PP is an interval: if x,z∈Px,z\in P and y∈Ry\in\mathbb{R} satisfies x≀y≀zx\le y\le z, then 0<x0<x and x≀yx\le y, so 0<y0<y by claim 2 of Elementary Order Arithmetic in an Ordered Field, i.e. y∈Py\in P. Let x∈Px\in P. By claim 8 there, 0<xβ‹…2βˆ’10<x\cdot 2^{-1} and xβ‹…2βˆ’1<xx\cdot 2^{-1}<x, so u=xβ‹…2βˆ’1u=x\cdot 2^{-1} lies in PP and u<xu<x. By claim 6 there 0<10<1, so x<x+1x<x+1 by claim 1 there, and v=x+1∈Pv=x+1\in P by claim 2. Thus u<x<vu<x<v with u,v∈Pu,v\in P, so xx is an interior point of PP.

NN is an interval: if x,z∈Nx,z\in N and x≀y≀zx\le y\le z, then y≀zy\le z and z<0z<0, so y<0y<0 by claim 2. Let x∈Nx\in N. From 0<10<1 and claim 4 we get βˆ’1<0-1<0, hence x+(βˆ’1)<xx+(-1)<x by claim 1, and x+(βˆ’1)<x<0x+(-1)<x<0 gives x+(βˆ’1)∈Nx+(-1)\in N by claim 2. Put w=(βˆ’x)β‹…2βˆ’1w=(-x)\cdot 2^{-1}; since 0<βˆ’x0<-x by claim 4, claim 8 gives 0<w0<w, so x<x+wx<x+w by claim 1, while x+w<x+(βˆ’x)=0x+w<x+(-x)=0 by claim 1 and w<βˆ’xw<-x (claim 8). Thus x+w∈Nx+w\in N and x+(βˆ’1)<x<x+wx+(-1)<x<x+w, so xx is an interior point of NN.

Step 2 (localisation). We record the following elementary fact. Let f:Rβ†’Rf:\mathbb{R}\to\mathbb{R}, let x0∈Rx_{0}\in\mathbb{R}, let JβŠ†RJ\subseteq\mathbb{R} be an interval containing x0x_{0} as an interior point, and let θ∈R\theta\in\mathbb{R} with 0<ΞΈ0<\theta be such that every z∈Rz\in\mathbb{R} with ∣zβˆ’x0∣<ΞΈ|z-x_{0}|<\theta belongs to JJ. If the restriction f∣Jf|_{J} is differentiable at x0x_{0} with derivative LL, then ff is differentiable at x0x_{0} with derivative LL.

Indeed, let Ξ΅>0\varepsilon>0 and let Ξ΄>0\delta>0 be as in Derivative at an Interior Point for f∣Jf|_{J} at x0x_{0} with the value LL and this Ξ΅\varepsilon. Let Ξ΄β€²\delta' be the smaller of Ξ΄\delta and ΞΈ\theta (claim 9 of Elementary Order Arithmetic in an Ordered Field); then 0<Ξ΄β€²0<\delta'. If h∈Rh\in\mathbb{R} satisfies 0<∣h∣<Ξ΄β€²0<|h|<\delta', then ∣(x0+h)βˆ’x0∣=∣h∣<ΞΈ|(x_{0}+h)-x_{0}|=|h|<\theta, so x0+h∈Jx_{0}+h\in J; since also 0<∣h∣<Ξ΄0<|h|<\delta, the choice of Ξ΄\delta gives

∣f(x0+h)βˆ’f(x0)hβˆ’L∣<Ξ΅,\Bigl|\frac{f(x_{0}+h)-f(x_{0})}{h}-L\Bigr|<\varepsilon,

because ff and f∣Jf|_{J} take the same values at x0x_{0} and at x0+hx_{0}+h. As Ρ>0\varepsilon>0 was arbitrary, ff is differentiable at x0x_{0} with derivative LL.

We apply this in two situations. If 0<x00<x_{0} we take J=PJ=P and ΞΈ=x0\theta=x_{0}: if ∣zβˆ’x0∣<x0|z-x_{0}|<x_{0} then βˆ’x0<zβˆ’x0-x_{0}<z-x_{0} by claim 9 of Properties of the Absolute Value in an Ordered Field, so 0<z0<z by claim 1 of Elementary Order Arithmetic in an Ordered Field. If x0<0x_{0}<0 we take J=NJ=N and ΞΈ=βˆ’x0\theta=-x_{0}, which is positive by claim 4 of that lemma: if ∣zβˆ’x0∣<βˆ’x0|z-x_{0}|<-x_{0} then zβˆ’x0<βˆ’x0z-x_{0}<-x_{0} by claim 9 of the absolute value lemma, so z<0z<0 by claim 1.

Step 3 (the family DD). For a polynomial function qq on R\mathbb{R} define ψq:Rβ†’R\psi_{q}:\mathbb{R}\to\mathbb{R} by

ψq(s)=q(sβˆ’1)exp⁑(βˆ’(sβˆ’1))Β Β forΒ 0<s,ψq(s)=0Β Β forΒ s≀0,\psi_{q}(s)=q\bigl(s^{-1}\bigr)\exp\bigl(-\bigl(s^{-1}\bigr)\bigr)\ \text{ for }0<s,\qquad \psi_{q}(s)=0\ \text{ for }s\le 0,

and let DD be the set of all functions from R\mathbb{R} to R\mathbb{R} of the form ψq\psi_{q} with qq a polynomial function on R\mathbb{R}.

Fix a polynomial function qq on R\mathbb{R}, and let qβˆ—q^{\ast} be the polynomial function supplied by claim 2 of Derivative of a Polynomial Function on the Real Line, so that for every interval II and every interior point x0x_{0} of II the restriction q∣Iq|_{I} is differentiable at x0x_{0} with derivative qβˆ—(x0)q^{\ast}(x_{0}). Define qβ™―:Rβ†’Rq^{\sharp}:\mathbb{R}\to\mathbb{R} by

qβ™―(x)=xβ‹…xβ‹…(q(x)+(βˆ’1) qβˆ—(x))(x∈R).q^{\sharp}(x)=x\cdot x\cdot\bigl(q(x)+(-1)\,q^{\ast}(x)\bigr)\qquad(x\in\mathbb{R}).

By claim 1 of Properties of Natural Number Powers in a Field we have x1=xx^{1}=x for the natural number powers of R\mathbb{R}, so the map x↦xx\mapsto x is the map x↦x1x\mapsto x^{1} and is a polynomial function by claim 1 of Constants, Powers, Sums, Scalar Multiples and Products of Polynomial Functions; by claims 2 and 3 there, qβ™―q^{\sharp} is a polynomial function on R\mathbb{R}, so ψqβ™―βˆˆD\psi_{q^{\sharp}}\in D. Steps 4 to 6 show that ψq\psi_{q} is differentiable at every point of R\mathbb{R} and that its derivative function is ψqβ™―\psi_{q^{\sharp}}.

Step 4 (points of PP). Let s0∈Ps_{0}\in P and put u0=s0βˆ’1u_{0}=s_{0}^{-1}; then 0<u00<u_{0} by claim 7 of Elementary Order Arithmetic in an Ordered Field, so u0∈Pu_{0}\in P. Let r:Pβ†’Rr:P\to\mathbb{R} be given by r(s)=sβˆ’1r(s)=s^{-1}. Since 0βˆ‰P0\notin P and every point of PP is an interior point of PP by Step 1, claim 2 of Reciprocal Rule for One-Dimensional Derivatives shows that rr is differentiable at s0s_{0} with rβ€²(s0)=βˆ’(u0)2r'(s_{0})=-\bigl(u_{0}\bigr)^{2}. Moreover r(s)∈Pr(s)\in P for every s∈Ps\in P, again by claim 7.

(a) The point r(s0)=u0r(s_{0})=u_{0} is an interior point of PP at which q∣Pq|_{P} is differentiable with derivative qβˆ—(u0)q^{\ast}(u_{0}). Hence Chain Rule for One-Dimensional Derivatives applies to Ξ³=r\gamma=r and g=q∣Pg=q|_{P} and gives that q∘r:Pβ†’Rq\circ r:P\to\mathbb{R} is differentiable at s0s_{0} with

(q∘r)β€²(s0)=qβˆ—(u0)β‹…(βˆ’(u0)2).(q\circ r)'(s_{0})=q^{\ast}(u_{0})\cdot\bigl(-(u_{0})^{2}\bigr).

(b) Let Ξ³:Pβ†’R\gamma:P\to\mathbb{R} be given by Ξ³(s)=(βˆ’1) r(s)\gamma(s)=(-1)\,r(s), so that Ξ³(s)=βˆ’(sβˆ’1)\gamma(s)=-\bigl(s^{-1}\bigr) by claim 2 of Zero Products and Elementary Identities in a Field. By claim 2 of Sum, Constant Multiple, and Product Rules for One-Dimensional Derivatives, Ξ³\gamma is differentiable at s0s_{0} with Ξ³β€²(s0)=(βˆ’1)(βˆ’(u0)2)=(u0)2\gamma'(s_{0})=(-1)\bigl(-(u_{0})^{2}\bigr)=(u_{0})^{2}. Every point of R\mathbb{R} is an interior point of R\mathbb{R}, and exp⁑\exp is differentiable at every point with exp⁑′=exp⁑\exp'=\exp by claim 3 of Basic Properties of the Exponential Function. Hence Chain Rule for One-Dimensional Derivatives applies to Ξ³\gamma and g=exp⁑g=\exp and gives that E=exp⁑∘γ:Pβ†’RE=\exp\circ\gamma:P\to\mathbb{R} is differentiable at s0s_{0} with

Eβ€²(s0)=exp⁑(βˆ’u0) (u0)2.E'(s_{0})=\exp\bigl(-u_{0}\bigr)\,(u_{0})^{2}.

(c) For s∈Ps\in P we have ψq(s)=(q∘r)(s) E(s)\psi_{q}(s)=(q\circ r)(s)\,E(s), so the restriction ψq∣P\psi_{q}|_{P} is the pointwise product of q∘rq\circ r and EE. By the product rule (claim 3 of Sum, Constant Multiple, and Product Rules for One-Dimensional Derivatives) it is differentiable at s0s_{0} with derivative

qβˆ—(u0)(βˆ’(u0)2)exp⁑(βˆ’u0)+q(u0)exp⁑(βˆ’u0) (u0)2=u0β‹…u0β‹…(q(u0)+(βˆ’1)qβˆ—(u0))exp⁑(βˆ’u0),q^{\ast}(u_{0})\bigl(-(u_{0})^{2}\bigr)\exp(-u_{0})+q(u_{0})\exp(-u_{0})\,(u_{0})^{2} = u_{0}\cdot u_{0}\cdot\bigl(q(u_{0})+(-1)q^{\ast}(u_{0})\bigr)\exp(-u_{0}),

which is qβ™―(u0)exp⁑(βˆ’(s0βˆ’1))=ψqβ™―(s0)q^{\sharp}(u_{0})\exp\bigl(-\bigl(s_{0}^{-1}\bigr)\bigr)=\psi_{q^{\sharp}}(s_{0}). By Step 2 with J=PJ=P and ΞΈ=s0\theta=s_{0}, ψq\psi_{q} is differentiable at s0s_{0} with ψqβ€²(s0)=ψqβ™―(s0)\psi_{q}'(s_{0})=\psi_{q^{\sharp}}(s_{0}).

Step 5 (points of NN). Let s0∈Ns_{0}\in N. Every s∈Ns\in N satisfies s≀0s\le 0, so ψq∣N\psi_{q}|_{N} is the function on NN with constant value 00, which by claim 1 of Sum, Constant Multiple, and Product Rules for One-Dimensional Derivatives is differentiable at s0s_{0} with derivative 00. By Step 2 with J=NJ=N and ΞΈ=βˆ’s0\theta=-s_{0}, ψq\psi_{q} is differentiable at s0s_{0} with ψqβ€²(s0)=0\psi_{q}'(s_{0})=0; and ψqβ™―(s0)=0\psi_{q^{\sharp}}(s_{0})=0 because s0≀0s_{0}\le 0.

Step 6 (the origin). Let m:Rβ†’Rm:\mathbb{R}\to\mathbb{R} be given by m(x)=xβ‹…q(x)m(x)=x\cdot q(x); it is a polynomial function on R\mathbb{R} by claims 1 and 3 of Constants, Powers, Sums, Scalar Multiples and Products of Polynomial Functions, using again that x↦xx\mapsto x is a polynomial function. Let Ξ΅>0\varepsilon>0. By claim 2 of The Exponential Function Dominates Every Polynomial Function applied to mm there is δ∈R\delta\in\mathbb{R} with 0<Ξ΄0<\delta such that

∣m(sβˆ’1)∣exp⁑(βˆ’(sβˆ’1))<Ξ΅forΒ everyΒ s∈RΒ withΒ 0<s<Ξ΄.\bigl|m\bigl(s^{-1}\bigr)\bigr|\exp\bigl(-\bigl(s^{-1}\bigr)\bigr)<\varepsilon\qquad\text{for every }s\in\mathbb{R}\text{ with }0<s<\delta.

Since ψq(0)=0\psi_{q}(0)=0, the difference quotient of ψq\psi_{q} at 00 for hβ‰ 0h\ne 0 equals hβˆ’1ψq(h)h^{-1}\psi_{q}(h). Let h∈Rh\in\mathbb{R} with 0<∣h∣<Ξ΄0<|h|<\delta. If h<0h<0 then ψq(h)=0\psi_{q}(h)=0, so the quotient is 00 and its distance to 00 is 0<Ξ΅0<\varepsilon. If 0<h0<h then h=∣h∣<Ξ΄h=|h|<\delta and

hβˆ’1ψq(h)=hβˆ’1 q(hβˆ’1)exp⁑(βˆ’(hβˆ’1))=m(hβˆ’1)exp⁑(βˆ’(hβˆ’1)),h^{-1}\psi_{q}(h)=h^{-1}\,q\bigl(h^{-1}\bigr)\exp\bigl(-\bigl(h^{-1}\bigr)\bigr)=m\bigl(h^{-1}\bigr)\exp\bigl(-\bigl(h^{-1}\bigr)\bigr),

so, since exp⁑\exp takes positive values (claim 2 of Basic Properties of the Exponential Function) and by claims 1 and 4 of Properties of the Absolute Value in an Ordered Field,

∣hβˆ’1ψq(h)βˆ’0∣=∣m(hβˆ’1)∣exp⁑(βˆ’(hβˆ’1))<Ξ΅.\bigl|h^{-1}\psi_{q}(h)-0\bigr|=\bigl|m\bigl(h^{-1}\bigr)\bigr|\exp\bigl(-\bigl(h^{-1}\bigr)\bigr)<\varepsilon.

As Ξ΅>0\varepsilon>0 was arbitrary, ψq\psi_{q} is differentiable at 00 with ψqβ€²(0)=0\psi_{q}'(0)=0; and ψqβ™―(0)=0\psi_{q^{\sharp}}(0)=0.

Step 7 (proof of claim 2). By Steps 4 to 6, every element of DD is differentiable at every point of R\mathbb{R}, and the function sending ss to ψqβ€²(s)\psi_{q}'(s) is ψqβ™―\psi_{q^{\sharp}}, which again lies in DD. Hence claim 3 of One-Dimensional Derivatives, Partial Derivatives, and Smoothness on the Real Line applies to DD and shows that every element of DD is a smooth map on R1\mathbb{R}^{1}. Let q1q_{1} be the polynomial function on R\mathbb{R} with constant value 11 (claim 1 of Constants, Powers, Sums, Scalar Multiples and Products of Polynomial Functions). For 0<s0<s we have ψq1(s)=1β‹…exp⁑(βˆ’(sβˆ’1))=Ο†(s)\psi_{q_{1}}(s)=1\cdot\exp\bigl(-\bigl(s^{-1}\bigr)\bigr)=\varphi(s), and for s≀0s\le 0 we have ψq1(s)=0=Ο†(s)\psi_{q_{1}}(s)=0=\varphi(s). Therefore Ο†=ψq1∈D\varphi=\psi_{q_{1}}\in D is smooth on R1\mathbb{R}^{1}.

Step 8 (proof of claim 1). If s≀0s\le 0 then Ο†(s)=0\varphi(s)=0, so 0≀φ(s)0\le\varphi(s) and 0<Ο†(s)0<\varphi(s) fails. If 0<s0<s then Ο†(s)=exp⁑(βˆ’(sβˆ’1))\varphi(s)=\exp\bigl(-\bigl(s^{-1}\bigr)\bigr), which is positive by claim 2 of Basic Properties of the Exponential Function; hence 0<Ο†(s)0<\varphi(s), and 0≀φ(s)0\le\varphi(s). Both assertions of claim 1 follow. β– \blacksquare

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