Since T is bounded, fix a real number C0β with 0β€C0β that is a bound for T. Write 0Vβ for the zero vector. We record three facts. By that lemma and the absolute homogeneity condition of the norm, together with β£0β£=0 from claim 3 of Properties of Complex Conjugation and Modulus, we have β₯0Vββ₯=β₯0β
0Vββ₯=β£0β£β₯0Vββ₯=0, and by linearity T(0Vβ)=T(0β
0Vβ)=0T(0Vβ)=0Vβ. Next, if x,y,c are real numbers with xβ€y and 0β€c, then 0β€c(yβx)=cyβcx by the second order axiom of Ordered Field, so cxβ€cy; we call this multiplying an inequality by a nonnegative number. Finally 0β€1, since 1=1β
1 and by totality either 0β€1, or 1β€0 and then 0β€β1 so that 0β€(β1)(β1)=1.
Step 1: BTβ is nonempty and every bound for T is an upper bound for BTβ. Since β₯0Vββ₯=0β€1, the number β₯T(0Vβ)β₯=β₯0Vββ₯=0 lies in BTβ, so BTβ is nonempty. Let C be a bound for T and let uβV with β₯uβ₯β€1. Multiplying β₯uβ₯β€1 by the nonnegative number C gives Cβ₯uβ₯β€C, and β₯T(u)β₯β€Cβ₯uβ₯, so β₯T(u)β₯β€C by transitivity. Hence C is an upper bound for BTβ. In particular C0β is, so BTβ is nonempty and bounded above and therefore has a least upper bound Ο by the least upper bound property in The Real Numbers.
Step 2: 0β€Ο. The number 0 lies in BTβ by step 1 and Ο is an upper bound for BTβ.
Step 3: Ο is a bound for T. Let uβV. If u=0Vβ, both β₯T(u)β₯ and Οβ₯uβ₯ are 0. Suppose uξ =0Vβ. By the positivity condition of the norm β₯uβ₯ξ =0, so it has an inverse r=β₯uβ₯β1 in the field of real numbers. If rβ€0 then 0β€βr, and with 0β€β₯uβ₯ the second order axiom gives 0β€(βr)β₯uβ₯=β1, hence 1β€0; together with 0β€1 this forces 1=0, which is false. So 0β€r, and by absolute homogeneity together with β£rβ£=r (claim 8 of Properties of Complex Conjugation and Modulus) we get β₯ruβ₯=rβ₯uβ₯=1. Hence β₯T(ru)β₯βBTβ, so β₯T(ru)β₯β€Ο. By linearity and absolute homogeneity β₯T(ru)β₯=rβ₯T(u)β₯, so multiplying rβ₯T(u)β₯β€Ο by the nonnegative number β₯uβ₯ and using β₯uβ₯r=1 gives β₯T(u)β₯β€Οβ₯uβ₯. With step 2 this shows Ο is a bound for T.
Step 4: Ο is an operator norm of T. By step 3 it is a bound for T, and by step 1 every bound C for T is an upper bound for BTβ, so Οβ€C because Ο is the least upper bound. These are exactly the two conditions of Operator Norm.
Step 5: uniqueness. Let c and cβ² both be operator norms of T. Each is a bound for T, and each is at most every bound for T, so cβ€cβ² and cβ²β€c; antisymmetry of the order gives c=cβ². Combined with step 4, T has exactly one operator norm and it is the least upper bound Ο of BTβ.