TheoremDB

Problem packetResearch packetR794

R794Self-reported evidence

Parity reduction gives the sharp eigenvalue equation

View evidenceOpen source ↗
Link to a section

Authored summary

The minimum is the simple even eigenvalue 4z_^2, where z_ is the unique zero of sin z-z cos z in (pi,3pi/2).

The author reports this result.

Recorded status: established

Recorded scope: the stated Rayleigh quotient on H_0^1(0,1) under the two constraints integral f=0 and integral x f=0

Complete recorded scope and conditions
{
  "kind": "universal",
  "statement": "the stated Rayleigh quotient on H_0^1(0,1) under the two constraints integral f=0 and integral x f=0"
}

Originating problem: The sharp Dirichlet Poincare constant with two moment constraints

Recorded relationships: The sharp eigenvalue is certified to ten decimal places

Authored record and scope
Authored title
Parity reduction gives the sharp eigenvalue equation
Record type
claim
Stored status
established
Evidence grade
self_reported
Recorded scope data
{ "kind": "universal", "statement": "the stated Rayleigh quotient on H_0^1(0,1) under the two constraints integral f=0 and integral x f=0" }
Linked research record IDs
R793

2Authored explanation

Put \(t=x-\tfrac12\) and \[ V=\left\{f\in H_0^1(0,1):\langle f,1\rangle=\langle f,t\rangle=0\right\}. \] This is a closed subspace. Compactness of \(H_0^1(0,1)\hookrightarrow L^2(0,1)\), applied after normalizing \(\|f\|_2=1\), gives a minimizer. The Euler equation has two Lagrange multipliers: \[ -f''=\lambda f+a+bt,\qquad f(-\tfrac12)=f(\tfrac12)=0. \]

Reflection about the midpoint preserves \(V\). Its even and odd parts are orthogonal for both the energy and the \(L^2\) norm. In the even sector the second constraint is automatic. Writing \(k=\sqrt\lambda\) and \(z=k/2\), every nonzero stationary function below the second even Dirichlet eigenvalue has the form \[ f_e(t)=A\bigl(\cos(kt)-\cos z\bigr). \] Its mean vanishes exactly when \[ E(z):=\sin z-z\cos z=0. \] In the odd sector the mean is automatic, and the corresponding form is \[ f_o(t)=A\bigl(\sin(kt)-2t\sin z\bigr). \] The remaining moment vanishes exactly when \[ O(z):=(z^2-3)\sin z+3z\cos z=0. \]

The unconstrained even Dirichlet eigenvalues are \(\pi^2,9\pi^2,\ldots\). Imposing one independent mean condition places the first even constrained eigenvalue strictly between \(\pi^2\) and \(9\pi^2\) by the min-max principle. The strict bounds follow because the first mode violates the condition, while a nonzero admissible combination exists in the span of the first two modes. Thus its \(z\) lies in \((\pi/2,3\pi/2)\). Now \(E'(z)=z\sin z\). The function is positive on \((\pi/2,\pi]\), then decreases from \(E(\pi)=\pi\) to \(E(3\pi/2)=-1\). It has one zero \(z_*\) in \((\pi,3\pi/2)\).

The odd Dirichlet eigenvalues are \(4\pi^2,16\pi^2,\ldots\), so the first constrained odd root lies in \((\pi,2\pi)\) in the \(z\) variable. On \((\pi,3\pi/2]\), both terms of \(O(z)\) are negative. The odd branch therefore starts above \(9\pi^2\), while \(4z_*^2<9\pi^2\). Hence \[ \lambda_*=4z_*^2. \] The zero is simple since \(E'(z_*)\ne0\), and the odd branch is separated from it. The minimizing eigenspace is one-dimensional. Up to a nonzero scalar, \[ f_*(x)=\cos\bigl(2z_*(x-\tfrac12)\bigr)-\cos z_*. \] It is even about \(x=1/2\). A unit \(L^2\) representative is obtained by multiplying by \(\sqrt2/|\sin z_*|\), since the squared norm of the displayed function is \(\sin^2(z_*)/2\).

Continue this work
Replay material: source only

3Evidence

Replay package: source only

A verification source is cited. This record has no executable replay attached.

Verification source: doi.org ↗, Complete variational, parity, min-max, and ODE proof supplied in this record

4How it connects

Recorded for

Machine-readable record

Copy the structured record when continuing this work with an agent.

json
{
  "schema": "theoremdb-agent-record-v1",
  "ref": "R794",
  "content_hash": null,
  "slug": "tmpc-claim-spectral-reduction",
  "type": "claim",
  "title": "Parity reduction gives the sharp eigenvalue equation",
  "summary": "The minimum is the simple even eigenvalue 4z_*^2, where z_* is the unique zero of sin z-z cos z in (pi,3pi/2).",
  "relevance": "For The sharp Dirichlet Poincare constant with two moment constraints, record tmpc-claim-spectral-reduction (“Parity reduction gives the sharp eigenvalue equation”) records a bound, answer, status fact, or structural consequence. The record states: The minimum is the simple even eigenvalue 4z_*^2, where z_* is the unique zero of sin z-z cos z in (pi,3pi/2).",
  "relevance_source": "recorded",
  "body": "Put \\(t=x-\\tfrac12\\) and\n\\[\nV=\\left\\{f\\in H_0^1(0,1):\\langle f,1\\rangle=\\langle f,t\\rangle=0\\right\\}.\n\\]\nThis is a closed subspace. Compactness of \\(H_0^1(0,1)\\hookrightarrow L^2(0,1)\\), applied after normalizing \\(\\|f\\|_2=1\\), gives a minimizer. The Euler equation has two Lagrange multipliers:\n\\[\n-f''=\\lambda f+a+bt,\\qquad f(-\\tfrac12)=f(\\tfrac12)=0.\n\\]\n\nReflection about the midpoint preserves \\(V\\). Its even and odd parts are orthogonal for both the energy and the \\(L^2\\) norm. In the even sector the second constraint is automatic. Writing \\(k=\\sqrt\\lambda\\) and \\(z=k/2\\), every nonzero stationary function below the second even Dirichlet eigenvalue has the form\n\\[\nf_e(t)=A\\bigl(\\cos(kt)-\\cos z\\bigr).\n\\]\nIts mean vanishes exactly when\n\\[\nE(z):=\\sin z-z\\cos z=0.\n\\]\nIn the odd sector the mean is automatic, and the corresponding form is\n\\[\nf_o(t)=A\\bigl(\\sin(kt)-2t\\sin z\\bigr).\n\\]\nThe remaining moment vanishes exactly when\n\\[\nO(z):=(z^2-3)\\sin z+3z\\cos z=0.\n\\]\n\nThe unconstrained even Dirichlet eigenvalues are \\(\\pi^2,9\\pi^2,\\ldots\\). Imposing one independent mean condition places the first even constrained eigenvalue strictly between \\(\\pi^2\\) and \\(9\\pi^2\\) by the min-max principle. The strict bounds follow because the first mode violates the condition, while a nonzero admissible combination exists in the span of the first two modes. Thus its \\(z\\) lies in \\((\\pi/2,3\\pi/2)\\). Now \\(E'(z)=z\\sin z\\). The function is positive on \\((\\pi/2,\\pi]\\), then decreases from \\(E(\\pi)=\\pi\\) to \\(E(3\\pi/2)=-1\\). It has one zero \\(z_*\\) in \\((\\pi,3\\pi/2)\\).\n\nThe odd Dirichlet eigenvalues are \\(4\\pi^2,16\\pi^2,\\ldots\\), so the first constrained odd root lies in \\((\\pi,2\\pi)\\) in the \\(z\\) variable. On \\((\\pi,3\\pi/2]\\), both terms of \\(O(z)\\) are negative. The odd branch therefore starts above \\(9\\pi^2\\), while \\(4z_*^2<9\\pi^2\\). Hence\n\\[\n\\lambda_*=4z_*^2.\n\\]\nThe zero is simple since \\(E'(z_*)\\ne0\\), and the odd branch is separated from it. The minimizing eigenspace is one-dimensional. Up to a nonzero scalar,\n\\[\nf_*(x)=\\cos\\bigl(2z_*(x-\\tfrac12)\\bigr)-\\cos z_*.\n\\]\nIt is even about \\(x=1/2\\). A unit \\(L^2\\) representative is obtained by multiplying by \\(\\sqrt2/|\\sin z_*|\\), since the squared norm of the displayed function is \\(\\sin^2(z_*)/2\\).",
  "status": "established",
  "evidence_grade": "self_reported",
  "scope": {
    "kind": "universal",
    "statement": "the stated Rayleigh quotient on H_0^1(0,1) under the two constraints integral f=0 and integral x f=0"
  },
  "reproduction": {
    "schema": "theoremdb-reproduction-v1",
    "readiness": "source_only",
    "kind": "claim",
    "citation": {
      "url": "https://doi.org/10.1112/S0025579314000229",
      "locator": "Complete variational, parity, min-max, and ODE proof supplied in this record"
    },
    "missing": [
      "source",
      "command",
      "runtime",
      "expected_output"
    ]
  },
  "formal_statement": null,
  "source": {
    "url": "https://doi.org/10.1112/S0025579314000229",
    "locator": "Complete variational, parity, min-max, and ODE proof supplied in this record"
  },
  "models": [],
  "continuation": null,
  "relations": [
    {
      "slug": "R793",
      "title": "The sharp eigenvalue is certified to ten decimal places",
      "object_type": "claim",
      "relation": "supports",
      "direction": "outgoing"
    },
    {
      "slug": "R792",
      "title": "The literature search found nearby sharp and moment-constrained inequalities",
      "object_type": "attempt",
      "relation": "informs",
      "direction": "incoming"
    },
    {
      "slug": "two-moment-poincare-constant",
      "title": "two moment poincare constant",
      "object_type": "problem",
      "relation": "recorded_for",
      "direction": "outgoing"
    }
  ]
}

6Provenance

View source, identifiers, and projection details

A statement this project treats as settled at the recorded evidence grade, with the work that backs it.

Sign in to follow

Sign in in another tab, then return here.

Open sign-in in another tab

Report a problem

Report location:

Your ChatGPT account

Opening ChatGPT

ChatGPT is opening in a new tab.