Standard-normal symmetry with explicit named facts

On this page
  1. Goal and scope
  2. Givens and symbols
  3. Rules and sources
  4. Main derivation
  5. Substeps and lemmas
  6. Reverse audits
  7. Error controls and negative controls
  8. Result and limitations
  9. Verification and source binding

← Guide index · Original MKO

derivation-mko-standard-normal-distribution-01 · ocme-new142-reader-adoption-20261021

Goal and scope

Separate Gaussian prerequisites from derived CDF symmetry.

No finite-quadrature proof of the Gaussian integral or moments.

Givens and symbols

  • work
  • G1 — phi(x)=(2pi)^(-1/2)exp(-x²/2), Z has this density, and Phi(t)=P(Z≤t).
  • G2 — Explicit named theorem facts: the Gaussian integral is sqrt(2pi), hence normalization; E[Z]=0 and E[Z²]=1. These are premises, not proved here.
  • φ — standard-normal density
  • Φ — standard-normal CDF
  • Z — real random variable

Rules and sources

Some rule statements have reader clarifications in this revision: they are paraphrases, not verbatim quotations. Referenced original source bytes and hashes are unchanged.

  • mko_definition · cited — Gaussian-integral normalization, E[Z]=0 and Var(Z)=1 are explicitly named theorem facts, not derivations manufactured from finite quadrature. Exact families handle symbolic density, evenness and phi(x)/phi(0)=exp(−x^2/2), plus Phi(0)=1/2 and Phi(−x)=1−Phi(x) from declared normalization and symmetry. No general nonzero elementary CDF value is computed. Finite numerical integration proves neither normalization nor moments; a continuous CDF need not have a density or be normal. · mko-standard-normal-distribution
  • work · prerequisite — The Gaussian integral and moments are explicit named theorem prerequisites; also assume integral linearity, substitution, atomlessness of density laws and the second-moment variance identity.

Main derivation

S01 · implies

Before

\varphi(x)=\frac{e^{-x^2/2}}{\sqrt{2\pi}}

After

\varphi(x)>0\quad(x\in\mathbb R)

Conditions: none

Rule: work · Uses: G1, G2, work

Leaf basis: work

The exponential and constant denominator are positive, qualifying nonnegativity.

S02 · implies

Before

\int_{\mathbb R}e^{-x^2/2}\,dx=\sqrt{2\pi}\quad\text{(assumed)}

After

\int_{\mathbb R}\varphi(x)\,dx=1

Conditions: none

Rule: work · Uses: G1, G2, S01, work

Leaf basis: work

Multiply the explicitly assumed Gaussian integral by the normalization constant.

S03 · implies

Before

(-x)^2=x^2

After

\varphi(-x)=\varphi(x)

Conditions: none

Rule: work · Uses: G1, G2, S02, work

Leaf basis: work

Evenness of the square gives pointwise evenness of the density.

S04 · implies

Before

\varphi(0)=1/\sqrt{2\pi}

After

\varphi(x)/\varphi(0)=e^{-x^2/2}

Conditions: none

Rule: work · Uses: G1, G2, S03, work

Leaf basis: work

Cancel the common positive normalization constant to obtain the exact ratio.

S05 · implies

Before

\Phi(-t)=\int_{-\infty}^{-t}\varphi(u)\,du

After

\Phi(-t)=\int_t^\infty\varphi(v)\,dv=1-\Phi(t)

Conditions: none

Rule: work · Uses: G1, G2, S04, work

Leaf basis: work

Substitute u=-v, using evenness and normalization; a density law has no singleton mass.

S06 · implies

Before

t=0,\quad\Phi(0)=1-\Phi(0)

After

\Phi(0)=1/2

Conditions: none

Rule: work · Uses: G1, G2, S05, work

Leaf basis: work

At zero the symmetry identity gives twice the CDF equal to one.

S07 · implies

Before

E[Z]=0,\quad E[Z^2]=1\quad\text{(assumed)}

After

\operatorname{Var}(Z)=E[Z^2]-E[Z]^2=1

Conditions: none

Rule: work · Uses: G1, G2, S06, work

Leaf basis: work

Substitute the explicitly assumed moments into the variance identity.

S08 · implies

Before

t=1

After

\Phi(-1)=1-\Phi(1),\quad\varphi(1)/\varphi(0)=e^{-1/2}

Conditions: none

Rule: work · Uses: G1, G2, S07, work

Leaf basis: work

Give exact symbolic relations at a nonzero point without inventing an elementary CDF value.

Substeps and lemmas

No substeps in this guide.

Reverse audits

  • S08 · premise_audit · G1, G2, S07, work — Phi(1) has not been evaluated rationally, and finite integration proves none of the premises.
  • S07 · premise_audit · G1, G2, S06, work — Do not relabel the moment premises as an integral proof completed here.
  • S06 · premise_audit · G1, G2, S05, work — This exact value follows from symmetry and normalization, not approximation.
  • S05 · premise_audit · G1, G2, S04, work — The endpoint discrepancy in the complement has zero mass.
  • S04 · premise_audit · G1, G2, S03, work — This is a density ratio, not a CDF ratio.
  • S03 · premise_audit · G1, G2, S02, work — The center is 0; no unknown mu has been introduced.
  • S02 · premise_audit · G1, G2, S01, work — No finite quadrature points are being used to infer the integral.
  • S01 · premise_audit · G1, G2, work — Nonnegativity alone does not prove normalization.

Error controls and negative controls

Premise labeling

Keep normalization and moments labeled as named facts, not newly proved results.

Event and threshold

Phi(t)=P({omega:Z(omega)≤t}); t is a scalar threshold.

  • A few quadrature values prove normalization. → reject — Finite values do not prove an integral over the whole line.
  • Phi(1)=phi(1). → reject — Positive phi gives Phi(1)>Phi(0)=1/2, whereas phi(1)<phi(0)=1/sqrt(2pi)<1/2 using pi>2, so they differ.
  • Every continuous CDF is standard normal. → reject — A uniform distribution has a different continuous CDF.

Result and limitations

Under the explicit Gaussian prerequisites, Phi(-t)=1-Phi(t), Phi(0)=1/2 and Var(Z)=1.

    Verification and source binding

    2 declared checks for this guide; only the listed expressions are covered.

    • source commit: b1b2f1dcf8c50d67a93fe52d95f8eef7b3abba9f
    • adopted source SHA-256: ce6e79a0422b1524888abb53a308a69a70552c942a0768637ab742837af70ae2
    • original source SHA-256: 9be2b5a4eeeb9649020eca8625ccd6a76eef2d3e32963e884d8eadc5a4490a58
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