Alphabeta Math
ExampleConstruction: Literature-sourcedVerification: AI-adaptedSession-authored (Fable 5 assisted)precheck passaudited 2026-08-21
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x2sin(1/x2) has an unbounded, non-Riemann-integrable derivative

Example

Define F:RR by

F(0):=0,F(x):=x2sin(1/x2)(x0).

The function F is differentiable on R, with F(0)=0, and F is unbounded on every neighbourhood of zero. Consequently no extension of F(0,1] to [0,1] is Riemann integrable under the Darboux convention.

Facts & Assumptions

Given: The function F in the Example.

[L1]

For every real u, sinu1 (Parity and the Pythagorean identity for sine and cosine).

[L2]
[L7]

Every positive real has a unique positive square root (Existence and uniqueness of n-th roots: a unique a1/n0 with (a1/n)n=a, case n=2).

[L8]

For every real ε>0, there is a positive integer N with 1/N<ε (For every ε>0 in a complete ordered field there is a natural n1 with 1/n<ε).

Verification

technique · direct
1.1

For h0, the difference quotient at zero from [L11] is hsin(1/h2), whose absolute value is at most h by [L1]. Hence F(0)=0.

L1L11algebra
1.2

For x0, [L2] to [L5] give F(x)=2xsin(1/x2)2cos(1/x2)x.

L2L3L4L5algebra
2.1

For kN, let xk be the positive square root of 1/(2π(k+1)). It exists by [L7] and [L10], and 1/xk2=2π(k+1), so [L6] and step 1.2 give F(xk)=2/xk.

step 1.2L6L7L10constructalgebra
3.1

Let η>0. Applying [L8] below the positive real 2πη2 shows that 1/(2π(k+1))<η2 for all sufficiently large k, hence 0<xk<η by uniqueness and order of the positive square root. Thus xk0. Given a real M>0, the same argument with η=2/M gives 2/xk>M eventually, so 1/xk+. Therefore the values F(xk)=2/xk exceed every real bound arbitrarily close to zero.

step 2.1L7L8L10algebra
4.1

Steps 1.1, 1.2, and 3.1 show that F is differentiable on R, with F(0)=0, while F is unbounded on every neighbourhood of zero.

step 1.1step 1.2step 3.1
5.1

Every extension of F(0,1] to [0,1] retains the unbounded values from step 3.1, but [L9] requires boundedness for Darboux integrability. No such extension is Riemann integrable on [0,1].

step 3.1step 4.1L9

Depends on

Used by

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Sources