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.
derivation-mko-standard-normal-distribution-01 · ocme-new142-reader-adoption-20261021
Separate Gaussian prerequisites from derived CDF symmetry.
No finite-quadrature proof of the Gaussian integral or moments.
workG1 — 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 densityΦ — standard-normal CDFZ — real random variableSome 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-distributionwork · 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.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.
Before
\int_{\mathbb R}e^{-x^2/2}\,dx=\sqrt{2\pi}\quad\text{(assumed)}After
\int_{\mathbb R}\varphi(x)\,dx=1Conditions: none
Rule: work · Uses: G1, G2, S01, work
Leaf basis: work
Multiply the explicitly assumed Gaussian integral by the normalization constant.
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.
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.
Before
\Phi(-t)=\int_{-\infty}^{-t}\varphi(u)\,duAfter
\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.
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.
Before
E[Z]=0,\quad E[Z^2]=1\quad\text{(assumed)}After
\operatorname{Var}(Z)=E[Z^2]-E[Z]^2=1Conditions: none
Rule: work · Uses: G1, G2, S06, work
Leaf basis: work
Substitute the explicitly assumed moments into the variance identity.
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.
No substeps in this guide.
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.Keep normalization and moments labeled as named facts, not newly proved results.
Phi(t)=P({omega:Z(omega)≤t}); t is a scalar threshold.
reject — Finite values do not prove an integral over the whole line.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.reject — A uniform distribution has a different continuous CDF.Under the explicit Gaussian prerequisites, Phi(-t)=1-Phi(t), Phi(0)=1/2 and Var(Z)=1.
2 declared checks for this guide; only the listed expressions are covered.
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