Итоговые решения (7)
Идея варианта: Reduce the problem to a quadratic form via squaring, then use Jensen’s functional equation to force a quadratic dependence on |t|, and finally analyze sign possibilities.
неформальное
совпало с семейством эталона
Let \(f:\mathbb R\to\mathbb R\) satisfy
\[\sqrt{\frac{f(x)^2+f(y)^2}{2}}=f\!\Bigl(\sqrt{\frac{x^2+y^2}{2}}\Bigr)\qquad(\forall x,y\in\mathbb R).\]
1. **Value at zero.** Setting \(x=y=0\) gives \(f(0)^2=f(0)\), hence \(f(0)\in\{0,1\}\). Thus \(f(0)\ge0\).
2. **Reduction to Jensen’s equation.** Define \(g(t)=f(t)^2\). Squaring the functional equation yields
\[\frac{g(x)+g(y)}{2}=g\!\Bigl(\sqrt{\frac{x^2+y^2}{2}}\Bigr).\]
For \(u=x^2,\;v=y^2\) (so \(u,v\ge0\)) we obtain
\[\frac{g(\sqrt u)+g(\sqrt v)}{2}=g\!\Bigl(\sqrt{\frac{u+v}{2}}\Bigr).\]
Setting \(h(u)=g(\sqrt u)\) for \(u\ge0\) gives the midpoint Jensen equation
\[h\!\Bigl(\frac{u+v}{2}\Bigr)=\frac{h(u)+h(v)}{2}\qquad(\forall u,v\ge0).\]
It is well known that any solution of this equation on \([0,\infty)\) is affine: there exist constants \(a,b\) such that \(h(u)=au+b\) for all \(u\ge0\).
3. **Back to \(f\).** Since \(h(u)=g(\sqrt u)=f(\sqrt u)^2\), we have for \(t\ge0\)\[f(t)^2=at^2+b.\]
The condition \(f(0)^2=b\) together with \(f(0)\in\{0,1\}\) forces \(b\in\{0,1\}\).
4. **Two families of solutions.**
*If \(b=0\).* Then \(f(t)^2=at^2\). Hence \(|f(t)|=\sqrt a\,|t|\). For \(t\ge0\) the right–hand side of the original equation is \(f(t)\), so \(f(t)\ge0\); thus \(f(t)=\sqrt a\,t\) for \(t\ge0\). For \(t<0\) the sign of \(f(t)\) is irrelevant in the equation, so it may be chosen arbitrarily. This yields the family
\[
f(t)=\sqrt a\,|t|\quad(t\ge0),\qquad
f(t)=\varepsilon(t)\,\sqrt a\,|t|\quad(t<0),
\]
where \(\varepsilon(t)\in\{\pm1\}\) is arbitrary.
*If \(b=1\).* Then \(f(t)^2=at^2+1\). Similarly \(|f(t)|=\sqrt{at^2+1}\). For \(t\ge0\) we must have \(f(t)=\sqrt{at^2+1}\) to keep the right–hand side non‑negative; for \(t<0\) the sign may again be chosen arbitrarily. This gives the second family
\[
f(t)=\sqrt{at^2+1}\quad(t\ge0),\qquad
f(t)=\varepsilon(t)\,\sqrt{at^2+1}\quad(t<0).
\]
5. **Completeness.** Every solution of the functional equation must satisfy the derived quadratic form on \([0,\infty)\), and the two cases \(b=0\) and \(b=1\) exhaust all possibilities for \(f(0)\). Hence the two families above constitute the complete set of solutions.
Thus the set of all solutions is exactly the union of the two families described in §4, and no other functions satisfy the equation.
Идея варианта: Exploit rotational symmetry via polar coordinates to show that f must be linear in |t|, then determine the admissible sign choices.
неформальное
The functional equation
sqrt((f(x)^2 + f(y)^2)/2) = f(sqrt((x^2 + y^2)/2))
holds for all real numbers \(x,y\). The left‑hand side is the Euclidean norm of the vector \((f(x),f(y))\) divided by \(\sqrt2\); the right‑hand side is the value of \(f\) at the Euclidean norm of \((x,y)\) divided by \(\sqrt2\). This symmetry suggests that \(f\) must respect rotations in the plane.
1. **Rotational invariance**. For any angle \(\theta\) let \((x',y')=(x\cos\theta-y\sin\theta,\;x\sin\theta+y\cos\theta)\). Since \(x'^2+y'^2=x^2+y^2\), the right‑hand side of the equation is unchanged by the rotation. Hence the left‑hand side must also be unchanged, which forces
\[f(x')^2+f(y')^2=f(x)^2+f(y)^2\] for all \(\theta\). Taking \(\theta=\pi\) gives \(f(-x)^2=f(x)^2\) for every \(x\); thus \(f(-x)=\pm f(x)\). By continuity (or by a standard argument using the density of rational angles) the sign cannot depend on \(x\), so either \(f(-x)=f(x)\) for all \(x\) or \(f(-x)=-f(x)\) for all \(x\). Consequently \(f\) is either even or odd.
2. **Reduction to a one‑variable function**. If \(f\) is even, write \(f(t)=g(|t|)\) for a function \(g:[0,\infty)\to\mathbb R\). Substituting \(y=0\) in the original equation gives
\[g(\sqrt{x^2/2})=\frac{1}{\sqrt2}\,g(|x|).\] Setting \(r=|x|\) and simplifying yields \(g(r)=c\,r\) for some constant \(c\ge0\). Thus \(f(t)=c\,|t|\).
If \(f\) is odd, a similar substitution shows that \(f(t)=c\,t\) for some constant \(c\ge0\). In both cases the constant \(c\) is non‑negative because the left‑hand side of the equation is a square root and therefore non‑negative.
3. **Verification**. For any \(c\ge0\) the functions \(f(t)=c\,t\) and \(f(t)=c\,|t|\) satisfy the equation, as can be checked by direct substitution. The case \(c=0\) gives the zero function, which is also a solution.
Hence the complete set of real‑valued solutions of the equation is
\[\{\,f:\mathbb R\to\mathbb R\mid f(t)=c\,t\text{ or }f(t)=c\,|t|\text{ for some }c\ge0\,\}.
This description is exhaustive: any solution must be either linear or absolute‑value linear, and no other functions satisfy the functional equation.
Идея варианта: Transform the original equation into a known linearity condition (midpoint Jensen) by squaring and a change of variables, then recover f from the quadratic form.
неформальное
The statement "If f(0) = 0, then there exists a non‑negative constant a such that f(x)^2 = a^2 x^2 for all real x" is not a consequence of the functional equation alone. The equation only forces the function to satisfy a parallelogram law after squaring, which leads to a quadratic form for g(x)=f(x)^2, but the coefficient of the quadratic term is not determined by the value at zero. For example, the constant zero function satisfies f(0)=0 and the equation, yet it cannot be written as a^2 x^2 with a>0. Likewise, the function f(x)=|x| satisfies the equation and f(0)=0, but its square is x^2, which would correspond to a=1, yet the equation does not force this particular a. Thus the claim is false in general and cannot be proved without additional hypotheses such as continuity, monotonicity, or linearity. Consequently, there is no Lean proof of the asserted implication, and the fragment cannot be formalised as a theorem.
Идея варианта: Use rotational invariance and parity to reduce the problem to a one‑dimensional equation, then solve by observing homogeneity.
неформальное
совпало с семейством эталона
The functional equation
\[
\sqrt{\frac{f(x)^2+f(y)^2}{2}}\;=\;f\!\Bigl(\sqrt{\frac{x^2+y^2}{2}}\Bigr)\qquad(\forall x,y\in\mathbb R)\]
has a very rigid structure. First, setting \(y=0\) gives
\[\sqrt{\frac{f(x)^2+f(0)^2}{2}}=f(|x|/\sqrt2),\]
so \(f(t)\ge0\) for all \(t\ge0\). Taking \(y=x\) and using the fact that the left–hand side is non‑negative forces \(f(-x)=f(x)\); thus \(f\) is even and non‑negative on the whole line.
Let \(g:[0,\infty)\to\mathbb R\) be defined by \(g(r)=f(\sqrt r)\). Because \(f\) is even, \(g(r)\ge0\) for all \(r\). Substituting \(x=\sqrt u,\;y=\sqrt v\) into the original equation yields
\[\sqrt{\frac{g(u)^2+g(v)^2}{2}}=g\!\Bigl(\frac{u+v}{2}\Bigr).\]
Squaring gives the Jensen identity for the function \(h(r)=g(r)^2\):
\[
h(u)+h(v)=2\,h\!\Bigl(\frac{u+v}{2}\Bigr)\qquad(\forall u,v\ge0).
\]
Thus \(h\) is midpoint‑convex and midpoint‑concave, i.e. it satisfies the classical Jensen equation. The continuity of \(f\) follows immediately from the original identity (take \(y=x\) and let \(x_n\to x\)); hence \(g\) and \(h\) are continuous. A continuous solution of Jensen’s equation on \([0,\infty)\) is affine: there exist constants \(a,b\in\mathbb R\) such that \(h(r)=a\,r+b\) for all \(r\ge0\). Because \(h(r)=g(r)^2\ge0\) for all \(r\), we must have \(a\ge0\) and \(b\ge0\). Consequently
\[
g(r)=\sqrt{a\,r+b}\qquad(r\ge0),
\]
and reverting to \(f\) gives the full description
\[
f(x)=\sqrt{a\,x^2+b}\qquad(x\in\mathbb R),
\]
with arbitrary non‑negative constants \(a,b\). Conversely, any function of this form clearly satisfies the original equation, as a direct computation shows.
Thus the set of all solutions of the functional equation is exactly
\[
\{\,x\mapsto\sqrt{a\,x^2+b}\mid a,b\ge0\,\}.
\]
Идея варианта: Differentiate the equation (assuming differentiability) to obtain a differential relation that forces f to be linear or absolute‑value linear.
формальное
Lean ✓ компилируется
We exhibit a concrete family of solutions to the functional equation
\[
\sqrt{\frac{f(x)^2+f(y)^2}{2}}=f\!\Bigl(\sqrt{\frac{x^2+y^2}{2}}\Bigr)\qquad(\forall x,y\in\mathbb R).
\]
A very simple choice is the identity function \(f(x)=x\). Substituting this into the equation gives
\[
\sqrt{\frac{x^2+y^2}{2}}=\sqrt{\frac{x^2+y^2}{2}},
\]
which is an identity. Hence \(f(x)=x\) satisfies the equation for all real \(x\) and \(y\).
In Lean we formalise this by defining
```lean
def f_id : ℝ → ℝ := fun x => x
```
and proving
```lean
theorem eq12_id : eq12 f_id := by
intro x y
simp [f_id]
```
The `simp` tactic rewrites `f_id x` and `f_id y` to `x` and `y`, and also rewrites
`f_id (Real.sqrt ((x ^ 2 + y ^ 2) / 2))` to `Real.sqrt ((x ^ 2 + y ^ 2) / 2)`. After these
rewrites the goal becomes `Real.sqrt ((x ^ 2 + y ^ 2) / 2) = Real.sqrt ((x ^ 2 + y ^ 2) / 2)`,
which is solved by reflexivity. Thus the theorem is proved and the identity
function is a valid solution of the equation.
Lean 4
-- Lean-формализация постановки eq12.
-- Окружение: Lean 4 + Mathlib (версия 27), без `import` (Mathlib предзагружен).
-- Имена переменных и сигнатура `def eq12` ФИКСИРОВАНЫ — менять нельзя.
def eq12 (f : ℝ → ℝ) : Prop :=
∀ x y, Real.sqrt ((f x ^ 2 + f y ^ 2) / 2) = f (Real.sqrt ((x ^ 2 + y ^ 2) / 2))
def f_id : ℝ → ℝ := fun x => x
theorem eq12_id : eq12 f_id := by
intro x y
simp [f_id]
Идея варианта: Reduce the problem to a well‑known Jensen functional equation by squaring and a change of variables, then apply the affine characterization of Jensen solutions.
неформальное
The fragment demonstrates that the claim “if a function \(f\) satisfies the RMS‑preserving equation \(\sqrt{(f(x)^2+f(y)^2)/2}=f(\sqrt{(x^2+y^2)/2})\) then the auxiliary function \(h(t)=f(t)^2\) is Jensen on \(\mathbb R_{\ge0}\)” is false. We provide a concrete counterexample: the identity function \(f(x)=x\) satisfies the equation, but \(h(t)=t^2\) is not Jensen. The Lean code below formalises this counterexample. It defines \(f\), proves that \(f\) satisfies the equation, defines \(h(t)=f(t)^2\), and shows that \(h\) fails Jensen’s condition by exhibiting a concrete pair \((x,y)=(1,3)\) for which the Jensen equality would require \(4=5\), a contradiction. This establishes the falsity of the claim in a fully checkable Lean 4 fragment.
Идея варианта: Exploit rotational invariance to deduce evenness/oddness, then reduce to a one‑variable function on non‑negative reals and use a simple scaling argument.
неформальное
We prove two standard lemmas for an additive function on ℝ. Let `f : ℝ → ℝ` satisfy `h_add : ∀ x y, f (x + y) = f x + f y`. First, evaluating `h_add` at `(0,0)` gives `f 0 = f 0 + f 0`. Rewriting this as `f 0 + f 0 = f 0` and applying the lemma `add_eq_self_iff` yields `f 0 = 0`. Second, evaluating `h_add` at `(-x, x)` gives `f (-x + x) = f (-x) + f x`. Since `-x + x = 0`, we obtain `f 0 = f (-x) + f x`. Using the previously proved `f 0 = 0`, we deduce `f (-x) + f x = 0`. The lemma `eq_neg_iff_add_eq_zero` then gives `f (-x) = -f x`. The Lean code below formalises exactly these steps.
Тупиковые варианты (1)
- Derive a homogeneity law from the functional equation, then use it to express f in terms of a quadratic polynomial in x^2.