Reason: Initial publication. Continuity of the Rayleigh quotient on the compact unit sphere via Cauchy-Schwarz and the operator bound, the extreme value theorem for a maximiser, and the null-vector claim for a positive semi-definite self-adjoint operator applied to lambda id - T.
Step 0: three order facts. Let a,b,c be real numbers.
(i) If a≤b and b<c, then a<c. Indeed a≤c by transitivity, and a=c would give c≤b, which with b≤c and antisymmetry forces b=c, contrary to b<c.
(ii) If a<b and 0≤c with c=0, then ca<cb. Indeed ca≤cb by (O5); and ca=cb would give c(b−a)=cb−ca=0, whence b−a=c−1(c(b−a))=0 and a=b, contrary to a=b.
(iii) If a≤b and a′≤b′, then a+a′≤b+b′: two applications of the first order axiom of Ordered Field give a+a′≤b+a′ and b+a′≤b+b′, and transitivity applies.
Step 2: the Rayleigh quotient is continuous on S. Let RT be the Rayleigh quotient of T, a map from S to R.
For y,z,v∈V we have ⟨y+z,v⟩=⟨y,v⟩+⟨z,v⟩, by conditions 1 and 2 together with the additivity of conjugation in (M1). Let x,y∈S. Since (y−x)+x=y and T(y)−T(x)=T(y−x) by linearity of T, conditions 2 and the identity just noted give
RT(y)−RT(x)=⟨y−x,T(y)⟩+⟨x,T(y−x)⟩.
By the triangle inequality (M7), then Cauchy-Schwarz (N1), then the bound of step 1 together with (O5) and ∥x∥=∥y∥=1, and finally step 0(iii),
the last equality using ∥y−x∥=d(y,x)=d(x,y) by the symmetry of a metric.
Now let ε be a real number with 0≤ε and ε=0. By (O1) and (O2), 0≤1+D; and 1+D=0, since 1=1+0≤1+D by the first order axiom, so 1+D=0 would give 1≤0 and hence 1=0 by (O1) and antisymmetry. Put δ=ε(1+D)−1. By (O4) we have 0≤(1+D)−1 and (1+D)−1=0, so 0≤δ by the second order axiom, and δ=0 because δ=0 would give ε=δ(1+D)=0.
Let y∈S with d(x,y)<δ. By (O1) and the first order axiom, D≤1+D, so (O5) with the nonnegative factor d(x,y) gives Dd(x,y)≤(1+D)d(x,y); and step 0(ii) gives (1+D)d(x,y)<(1+D)δ=ε. Combining with the displayed bound and step 0(i) twice,
Step 4: the operator λid−T. Let A send x∈V to A(x)=λx−T(x). It is a linear operator on V, since T is and by the axioms of a vector space. Since λ is real, λ=λ by (M1), so for u,v∈V, using the identity of step 2, conditions 1 and 3, and self-adjointness of T,
We check that A is positive semi-definite. For x∈V, condition 3 gives ⟨x,A(x)⟩=λ⟨x,x⟩−⟨x,T(x)⟩, a real number by condition 4 and (B1).
If x=0V, then T(0V)=0V by linearity and λ0V=0V by claim 4 of Elementary Identities in a Vector Space, so A(0V)=0V; and ⟨0V,0V⟩=⟨0V,0⋅0V⟩=0⟨0V,0V⟩=0 by claim 3 of that lemma and condition 3. So ⟨x,A(x)⟩=0.
If x=0V, put t=∥x∥; by the positivity of a norm t is real with 0≤t and t=0. By (O4), 0≤t−1 and t−1=0, so by claim 8 of Properties of the Absolute Value in an Ordered Field and absolute homogeneity of the norm, ∥t−1x∥=∣t−1∣t=t−1t=1; thus y=t−1x lies in S, and ty=x. Applying (I1) to the orthonormal 1-tuple with component y and the coefficient 1 gives ⟨y,y⟩=1, so
⟨y,A(y)⟩=λ−RT(y),
which satisfies 0≤λ−RT(y) by step 3 and (O3). Using the identity of step 2, conditions 1 and 3, t=t from (M1), and linearity of A,
⟨x,A(x)⟩=⟨ty,A(ty)⟩=tt⟨y,A(y)⟩=(tt)(λ−RT(y)).
The second order axiom gives 0≤tt and then 0≤⟨x,A(x)⟩.
Step 5: conclusion. By (I1) again, ⟨x0,x0⟩=1, so ⟨x0,A(x0)⟩=λ−RT(x0)=0. By claim 2 of Cauchy-Schwarz Inequality for a Positive Semi-Definite Self-Adjoint Operator, A(x0)=0V, that is, T(x0)=λx0. Finally x0=0V, since ⟨x0,x0⟩=1=0=⟨0V,0V⟩. Hence x0 is a unit vector that is an eigenvector of T with the real eigenvalue λ.