TheoremBase

Telescope ana^n - bnb^n into terms asa^s D btb^t with D = a - b, split the resulting trace sum into even terms, which are traces of g*g and hence nonnegative, and odd terms, which are real and bounded by Cauchy-Schwarz and the arithmetic-geometric inequality by averages of neighbouring even terms; summing gives nonnegativity.

Proof

Each result cited is applied with the data of its own statement. Throughout, λ\lambda, aa, bb and kk are as in the statement, n=2k−1n=2k-1 and D=a−bD=a-b. Products of three or more polynomials are written without brackets, which is legitimate by the associativity (pq)r=p(qr)(pq)r=p(qr) of Noncommutative Polynomials Form a Unital Complex Algebra with Involution: Linear Extension from Monomials, Products, Adjoints and Self-Adjoint Parts §algebra. Since λ\lambda is linear, it commutes with finite sums in the complex vector space Pm\mathcal{P}_{m} (Noncommutative Polynomials Form a Unital Complex Algebra with Involution: Linear Extension from Monomials, Products, Adjoints and Self-Adjoint Parts §vector-space), by induction along the recursion of Finite Sum Notation in a Vector Space; the resulting finite sums in C\mathbb{C}, regarded as a vector space over itself, are those of Finite Sum Notation in a Field, the two definitions prescribing the same recursion for the same addition of C\mathbb{C} and hence the same map by the uniqueness in Existence and Uniqueness of Iterates of a Binary Operation; and a finite sum in C\mathbb{C} of real numbers is real and equals their finite sum in R\mathbb{R}, by induction along that recursion, since sums of real numbers formed in C\mathbb{C} and in R\mathbb{R} coincide by condition 1 of The Complex Numbers. Likewise the distributive laws of Noncommutative Polynomials Form a Unital Complex Algebra with Involution: Linear Extension from Monomials, Products, Adjoints and Self-Adjoint Parts §algebra extend to finite sums. The results of Basic Properties of Noncommutative Laws: Adjoints, the Self-Adjoint Pairing, Cauchy-Schwarz, Monotonicity in the Bound, and Laws of Constant Tuples are applied with d=md=m and the tracial state λ\lambda.

Exponents and summation indices are integers ≥0\ge0 in the sense of The Integers as a Subset of the Real Numbers: by claim 1 of Arithmetic, Order, Discreteness and Intervals of the Integers each is 00 or ι(q)\iota(q) for some q∈Nq\in\mathbb{N}, unique by claim 7 of Properties of the Canonical Map from the Natural Numbers to an Ordered Field, where ι\iota is the canonical map of R\mathbb{R}, and ι(q)\iota(q) is identified with qq (sums corresponding by claim 4 there); sums, differences and products of integers are integers by claim 2 of Arithmetic, Order, Discreteness and Intervals of the Integers; every subtraction written below (r−1−sr-1-s for s≤r−1s\le r-1, 2k−2−s2k-2-s for s≤2k−2s\le2k-2, k−1−uk-1-u for u≤k−1u\le k-1, k−2−uk-2-u for u≤k−2u\le k-2) has a result ≥0\ge0, by claim 3 of Elementary Arithmetic in an Ordered Field; c0=1c^{0}=1 (Step 1); and for integers 0≤α≤β0\le\alpha\le\beta, ∑s=αβts\sum_{s=\alpha}^{\beta}t_{s} denotes the finite sum ∑j=1β−α+1tα+j−1\sum_{j=1}^{\beta-\alpha+1}t_{\alpha+j-1} of Finite Sum Notation in a Vector Space, respectively Finite Sum Notation in a Field, that is, the sum of the terms with s=α,α+1,…,βs=\alpha,\alpha+1,\dots,\beta in increasing order after the shift s=α+j−1s=\alpha+j-1 onto [β−α+1][\beta-\alpha+1], these being exactly the integers ss with α≤s≤β\alpha\le s\le\beta by claim 3 of Arithmetic, Order, Discreteness and Intervals of the Integers.

Step 1 (Powers, including exponent 00). For an integer s≥0s\ge0 let ws∈W1w_{s}\in W_{1} be the empty word ∅\varnothing if s=0s=0, and the word of length ss all of whose letters are 11 if s≥1s\ge1. For c∈Pmc\in\mathcal{P}_{m} put cs=cwsc^{s}=c_{w_{s}}, the product along wsw_{s} for the 11-tuple (c)(c) as in Substitution of Noncommutative Polynomials into the Variables §word-products; for s≥1s\ge1 this is the power of the statement, and c0=c∅=1c^{0}=c_{\varnothing}=1 by the same definition. Let σ:P1→Pm\sigma:\mathcal{P}_{1}\to\mathcal{P}_{m} be the substitution of (c)(c). Three facts are used.

(P1) csct=cs+tc^{s}c^{t}=c^{s+t} for all integers s,t≥0s,t\ge0. Indeed wswt=ws+tw_{s}w_{t}=w_{s+t} by Words over a Finite Alphabet: the Empty Word, Concatenation and Reversal §concatenation (by the clauses for the empty word if s=0s=0 or t=0t=0; otherwise wswtw_{s}w_{t} is the word of length s+ts+t all of whose letters are 11), and cwswt=cwscwtc_{w_{s}w_{t}}=c_{w_{s}}c_{w_{t}} by Substitution is the Unique Unital Homomorphism with Prescribed Values on the Variables: Monomials, Products, Adjoints and Composition §values.

(P2) c1=cc^{1}=c. Indeed w1w_{1} is the letter (1)(1), whose monomial is the variable x1x_{1} of P1\mathcal{P}_{1} by The Algebra of Noncommutative Polynomials in Finitely Many Self-Adjoint Variables §monomials, and Substitution is the Unique Unital Homomorphism with Prescribed Values on the Variables: Monomials, Products, Adjoints and Composition §values gives cw1=σ(xw1)=σ(x1)=cc_{w_{1}}=\sigma(x_{w_{1}})=\sigma(x_{1})=c.

(P3) If c∈Pm,sac\in\mathcal{P}_{m,\mathrm{sa}}, then (cs)∗=cs(c^{s})^{*}=c^{s}. Indeed all letters of wsw_{s} equal 11, so wsrev=wsw_{s}^{\mathrm{rev}}=w_{s} by Words over a Finite Alphabet: the Empty Word, Concatenation and Reversal §reversal, hence (xws)∗=xws(x_{w_{s}})^{*}=x_{w_{s}} in P1\mathcal{P}_{1} by Noncommutative Polynomials Form a Unital Complex Algebra with Involution: Linear Extension from Monomials, Products, Adjoints and Self-Adjoint Parts §adjoint; as cc is self-adjoint, Substitution is the Unique Unital Homomorphism with Prescribed Values on the Variables: Monomials, Products, Adjoints and Composition §adjoint and Substitution is the Unique Unital Homomorphism with Prescribed Values on the Variables: Monomials, Products, Adjoints and Composition §values give (cs)∗=σ(xws)∗=σ((xws)∗)=σ(xws)=cs(c^{s})^{*}=\sigma(x_{w_{s}})^{*}=\sigma\bigl((x_{w_{s}})^{*}\bigr)=\sigma(x_{w_{s}})=c^{s}.

Moreover D=a+(−1)b∈Pm,saD=a+(-1)b\in\mathcal{P}_{m,\mathrm{sa}}, since Pm,sa\mathcal{P}_{m,\mathrm{sa}} is closed under sums and real multiples by Noncommutative Polynomials Form a Unital Complex Algebra with Involution: Linear Extension from Monomials, Products, Adjoints and Self-Adjoint Parts §self-adjoint; so (P3) applies to aa, bb and DD. Finally (pq)∗=q∗p∗(pq)^{*}=q^{*}p^{*} by Noncommutative Polynomials Form a Unital Complex Algebra with Involution: Linear Extension from Monomials, Products, Adjoints and Self-Adjoint Parts §adjoint, and applying it twice, (pqr)∗=r∗q∗p∗(pqr)^{*}=r^{*}q^{*}p^{*} for all p,q,r∈Pmp,q,r\in\mathcal{P}_{m}.

Step 2 (Telescoping). For every r∈Nr\in\mathbb{N},

ar−br=∑s=0r−1asDbr−1−s,a^{r}-b^{r}=\sum_{s=0}^{r-1}a^{s}Db^{r-1-s},

the sum in Pm\mathcal{P}_{m} of the terms indexed by s=0,…,r−1s=0,\dots,r-1 in increasing order (the finite sum of Finite Sum Notation in a Vector Space after the index shift s↦s+1s\mapsto s+1). We argue by induction on rr. For r=1r=1 the right side is a0Db0=1D1=D=a−b=a1−b1a^{0}Db^{0}=1D1=D=a-b=a^{1}-b^{1}, by Step 1 and the unit law 1p=p1=p1p=p1=p of Noncommutative Polynomials Form a Unital Complex Algebra with Involution: Linear Extension from Monomials, Products, Adjoints and Self-Adjoint Parts §monomials. Assume the identity for rr. By (P1) and (P2), ar+1=araa^{r+1}=a^{r}a and br+1=brbb^{r+1}=b^{r}b, so by the distributive laws and the scalar clause (cp)q=c(pq)=p(cq)(cp)q=c(pq)=p(cq) of Noncommutative Polynomials Form a Unital Complex Algebra with Involution: Linear Extension from Monomials, Products, Adjoints and Self-Adjoint Parts §algebra (with c=−1c=-1, differences p−qp-q being p+(−1)qp+(-1)q)

ar+1−br+1=ara−arb+arb−brb=arD+(ar−br)b.a^{r+1}-b^{r+1}=a^{r}a-a^{r}b+a^{r}b-b^{r}b=a^{r}D+(a^{r}-b^{r})b .

By the induction hypothesis, distributivity over finite sums (with the scalar clause of Noncommutative Polynomials Form a Unital Complex Algebra with Involution: Linear Extension from Monomials, Products, Adjoints and Self-Adjoint Parts §algebra for the coefficient −1-1), and (P2) and (P1) in the form br−1−sb=br−1−sb1=br−sb^{r-1-s}b=b^{r-1-s}b^{1}=b^{r-s}, the second summand equals ∑s=0r−1asDbr−s\sum_{s=0}^{r-1}a^{s}Db^{r-s}, and arD=arDb0a^{r}D=a^{r}Db^{0} by the unit law. By the recursion of the finite sum, adding the term with index s=rs=r gives ar+1−br+1=∑s=0rasDbr−sa^{r+1}-b^{r+1}=\sum_{s=0}^{r}a^{s}Db^{r-s}, the identity for r+1r+1.

Step 3 (Expansion of the trace). Take r=n=2k−1r=n=2k-1 in Step 2 and multiply on the right by DD. Distributivity and the linearity of λ\lambda give

S:=λ((an−bn)D)=∑s=02k−2τs,τs=λ(asDb2k−2−sD).S:=\lambda\bigl((a^{n}-b^{n})D\bigr)=\sum_{s=0}^{2k-2}\tau_{s},\qquad\tau_{s}=\lambda\bigl(a^{s}Db^{2k-2-s}D\bigr).

For integers 0≤u≤k−10\le u\le k-1 put eu=τ2u=λ(a2uDb2(k−1−u)D)e_{u}=\tau_{2u}=\lambda\bigl(a^{2u}Db^{2(k-1-u)}D\bigr), and, when k≥2k\ge2, for integers 0≤u≤k−20\le u\le k-2 put ou=τ2u+1=λ(a2u+1Db2(k−2−u)+1D)o_{u}=\tau_{2u+1}=\lambda\bigl(a^{2u+1}Db^{2(k-2-u)+1}D\bigr), using 2k−2−(2u+1)=2(k−2−u)+12k-2-(2u+1)=2(k-2-u)+1. Thus SS is the sum of Sum over a Finite Index Set over the index set I={0,…,2k−2}I=\{0,\dots,2k-2\}, computed with the bijection [2k−1]→I[2k-1]\to I, j↦j−1j\mapsto j-1 (the shift of the convention above). Let Ie⊆II_{\mathrm{e}}\subseteq I be the set of even indices 2u2u (0≤u≤k−10\le u\le k-1) and, when k≥2k\ge2, Io⊆II_{\mathrm{o}}\subseteq I the set of odd indices 2u+12u+1 (0≤u≤k−20\le u\le k-2). The maps [k]→Ie[k]\to I_{\mathrm{e}}, u+1↦2uu+1\mapsto2u, and, when k≥2k\ge2, [k−1]→Io[k-1]\to I_{\mathrm{o}}, u+1↦2u+1u+1\mapsto2u+1, are bijections, so by Sum over a Finite Index Set, computed with them, ∑s∈Ieτs=∑u=0k−1eu\sum_{s\in I_{\mathrm{e}}}\tau_{s}=\sum_{u=0}^{k-1}e_{u} and ∑s∈Ioτs=∑u=0k−2ou\sum_{s\in I_{\mathrm{o}}}\tau_{s}=\sum_{u=0}^{k-2}o_{u}. If k=1k=1, then I={0}=IeI=\{0\}=I_{\mathrm{e}}; if k≥2k\ge2, then II is the disjoint union of IeI_{\mathrm{e}} and IoI_{\mathrm{o}}, each integer of II being even or odd and none both. As a sum over a finite index set does not depend on the bijection used to enumerate it (Sum over a Finite Index Set), we obtain (for k≥2k\ge2 by Sums over Finite Index Sets: Finite Unions, Disjoint Unions, Vanishing Terms, Dependent Pairs, Conjugation and the Modulus §disjoint-union)

S=∑u=0k−1euif k=1,S=∑u=0k−1eu+∑u=0k−2ouif k≥2.S=\sum_{u=0}^{k-1}e_{u}\quad\text{if }k=1,\qquad S=\sum_{u=0}^{k-1}e_{u}+\sum_{u=0}^{k-2}o_{u}\quad\text{if }k\ge2.

Step 4 (Even terms). Let 0≤u≤k−10\le u\le k-1 and v=k−1−uv=k-1-u, and put g=bvDaug=b^{v}Da^{u}. By Step 1, g∗=(au)∗D∗(bv)∗=auDbvg^{*}=(a^{u})^{*}D^{*}(b^{v})^{*}=a^{u}Db^{v}, and by (P1) g∗g=auDb2vDaug^{*}g=a^{u}Db^{2v}Da^{u}. By condition (c) of Noncommutative Laws of Finitely Many Self-Adjoint Variables with a Norm Bound §tracial-state with p=aup=a^{u} and q=Db2vDauq=Db^{2v}Da^{u}, then (P1), then condition (c) with p=Db2vDp=Db^{2v}D and q=a2uq=a^{2u},

λ(g∗g)=λ(Db2vDauau)=λ(Db2vDa2u)=λ(a2uDb2vD)=eu.\lambda(g^{*}g)=\lambda(Db^{2v}Da^{u}a^{u})=\lambda(Db^{2v}Da^{2u})=\lambda(a^{2u}Db^{2v}D)=e_{u}.

By condition (b) of Noncommutative Laws of Finitely Many Self-Adjoint Variables with a Norm Bound §tracial-state, eue_{u} is a real number and eu≥0e_{u}\ge0.

Step 5 (Odd terms). Let k≥2k\ge2, let 0≤u≤k−20\le u\le k-2 and v=k−2−u≥0v=k-2-u\ge0, and put A=auDbv+1A=a^{u}Db^{v+1} and B=au+1DbvB=a^{u+1}Db^{v}. By Step 1, A∗=bv+1DauA^{*}=b^{v+1}Da^{u} and B∗=bvDau+1B^{*}=b^{v}Da^{u+1}. Each of the following chains uses (P1) to merge adjacent powers, then condition (c) of Noncommutative Laws of Finitely Many Self-Adjoint Variables with a Norm Bound §tracial-state to move the leading power of bb to the end, then (P1) again, then condition (c) to move the leading factor DD to the end:

λ(B∗A)=λ(bvDa2u+1Dbv+1)=λ(Da2u+1Db2v+1)=λ(a2u+1Db2v+1D)=ou,\lambda(B^{*}A)=\lambda(b^{v}Da^{2u+1}Db^{v+1})=\lambda(Da^{2u+1}Db^{2v+1})=\lambda(a^{2u+1}Db^{2v+1}D)=o_{u}, λ(A∗B)=λ(bv+1Da2u+1Dbv)=λ(Da2u+1Db2v+1)=λ(a2u+1Db2v+1D)=ou,\lambda(A^{*}B)=\lambda(b^{v+1}Da^{2u+1}Db^{v})=\lambda(Da^{2u+1}Db^{2v+1})=\lambda(a^{2u+1}Db^{2v+1}D)=o_{u}, λ(A∗A)=λ(bv+1Da2uDbv+1)=λ(Da2uDb2(v+1))=λ(a2uDb2(v+1)D)=eu,\lambda(A^{*}A)=\lambda(b^{v+1}Da^{2u}Db^{v+1})=\lambda(Da^{2u}Db^{2(v+1)})=\lambda(a^{2u}Db^{2(v+1)}D)=e_{u}, λ(B∗B)=λ(bvDa2(u+1)Dbv)=λ(Da2(u+1)Db2v)=λ(a2(u+1)Db2vD)=eu+1,\lambda(B^{*}B)=\lambda(b^{v}Da^{2(u+1)}Db^{v})=\lambda(Da^{2(u+1)}Db^{2v})=\lambda(a^{2(u+1)}Db^{2v}D)=e_{u+1},

where the identifications with ouo_{u}, eue_{u} and eu+1e_{u+1} use v=k−2−uv=k-2-u, v+1=k−1−uv+1=k-1-u and v=k−1−(u+1)v=k-1-(u+1). By Basic Properties of Noncommutative Laws: Adjoints, the Self-Adjoint Pairing, Cauchy-Schwarz, Monotonicity in the Bound, and Laws of Constant Tuples §adjoint with p=Ap=A and q=Bq=B, λ(B∗A)=λ(A∗B)‾\lambda(B^{*}A)=\overline{\lambda(A^{*}B)}, that is, ou=ou‾o_{u}=\overline{o_{u}}; so ouo_{u} is real by claim 1 of Properties of Complex Conjugation and Modulus. By Basic Properties of Noncommutative Laws: Adjoints, the Self-Adjoint Pairing, Cauchy-Schwarz, Monotonicity in the Bound, and Laws of Constant Tuples §cauchy-schwarz with p=Ap=A and q=Bq=B,

∣ou∣2=∣λ(B∗A)∣2≤λ(A∗A) λ(B∗B)=eueu+1.|o_{u}|^{2}=|\lambda(B^{*}A)|^{2}\le\lambda(A^{*}A)\,\lambda(B^{*}B)=e_{u}e_{u+1}.

Step 6 (Arithmetic-geometric bound). Let k≥2k\ge2 and 0≤u≤k−20\le u\le k-2. Put x=∣ou∣x=|o_{u}| and yu=12(eu+eu+1)y_{u}=\tfrac12(e_{u}+e_{u+1}), where 12\tfrac12 is the inverse of 1+11+1. Since ouo_{u} is real, xx is its absolute value by claim 8 of Properties of the Absolute Value in an Ordered Field, so 0≤x0\le x by claim 1 there. Next 0≤eu+eu+10\le e_{u}+e_{u+1} by Step 4 and claim 2 of Elementary Arithmetic in an Ordered Field, and 0≤120\le\tfrac12 by claim 4 there, as 0≤1+10\le1+1 by claims 1 and 2 there and 1+1≠01+1\neq0, because 1+1=ι(1)+1=ι(2)1+1=\iota(1)+1=\iota(2) by claim 1 of Properties of the Canonical Map from the Natural Numbers to an Ordered Field and 0<ι(2)0<\iota(2) by claim 3 there; so 0≤yu0\le y_{u} by claim 5 there. Expanding in the field R\mathbb{R},

yu2−eueu+1=14((eu+eu+1)2−4eueu+1)=14(eu−eu+1)2.y_{u}^{2}-e_{u}e_{u+1}=\tfrac14\bigl((e_{u}+e_{u+1})^{2}-4e_{u}e_{u+1}\bigr)=\tfrac14(e_{u}-e_{u+1})^{2}.

For a real zz one has z2=∣z∣2z^{2}=|z|^{2}, since ∣z∣|z| equals zz or −z-z, and 0≤∣z∣20\le|z|^{2} by claim 2 of Monotonicity of Squaring on the Nonnegative Elements of an Ordered Field applied to 0≤∣z∣0\le|z| (claim 1 of Properties of the Absolute Value in an Ordered Field); with z=eu−eu+1z=e_{u}-e_{u+1} and claim 5 of Elementary Arithmetic in an Ordered Field (multiplying by 14=12⋅12≥0\tfrac14=\tfrac12\cdot\tfrac12\ge0) the right side is ≥0\ge0. Thus x2≤eueu+1≤yu2x^{2}\le e_{u}e_{u+1}\le y_{u}^{2} by Step 5 and claim 3 of Elementary Arithmetic in an Ordered Field, and claim 2 of Monotonicity of Squaring on the Nonnegative Elements of an Ordered Field (with α=x\alpha=x, β=yu\beta=y_{u}) gives ∣ou∣≤yu|o_{u}|\le y_{u}.

Step 7 (Conclusion). If k=1k=1, then S=e0S=e_{0}, which is real and nonnegative by Step 4. Let k≥2k\ge2. Then SS is real, being a sum of the real numbers eue_{u} (Step 4) and ouo_{u} (Step 5). By Step 6, ∣ou∣≤yu|o_{u}|\le y_{u}, so 0≤yu−∣ou∣=(−∣ou∣)−(−yu)0\le y_{u}-|o_{u}|=(-|o_{u}|)-(-y_{u}) and hence −yu≤−∣ou∣-y_{u}\le-|o_{u}|, by claim 3 of Elementary Arithmetic in an Ordered Field applied twice; with claim 3 of Properties of the Absolute Value in an Ordered Field, −yu≤−∣ou∣≤ou-y_{u}\le-|o_{u}|\le o_{u}, so 0≤ou+yu0\le o_{u}+y_{u} for every 0≤u≤k−20\le u\le k-2 (claim 3 of Elementary Arithmetic in an Ordered Field). By claims 5 and 2 of Properties of Finite Sums, 0≤∑u=0k−2ou+∑u=0k−2yu0\le\sum_{u=0}^{k-2}o_{u}+\sum_{u=0}^{k-2}y_{u}. Put E=∑i=0k−1eiE=\sum_{i=0}^{k-1}e_{i}. By claims 2 and 3 of Properties of Finite Sums and the reindexing i=u+1i=u+1,

∑u=0k−2yu=12(∑i=0k−2ei+∑i=1k−1ei).\sum_{u=0}^{k-2}y_{u}=\tfrac12\Bigl(\sum_{i=0}^{k-2}e_{i}+\sum_{i=1}^{k-1}e_{i}\Bigr).

Now {0,…,k−1}\{0,\dots,k-1\} is the disjoint union of {0,…,k−2}\{0,\dots,k-2\} and {k−1}\{k-1\}, and also of {0}\{0\} and {1,…,k−1}\{1,\dots,k-1\}; the sums over {0,…,k−1}\{0,\dots,k-1\}, {0,…,k−2}\{0,\dots,k-2\} and {1,…,k−1}\{1,\dots,k-1\} are the ones written above, by Sum over a Finite Index Set computed with the bijections [k]→{0,…,k−1}[k]\to\{0,\dots,k-1\} and [k−1]→{0,…,k−2}[k-1]\to\{0,\dots,k-2\}, j↦j−1j\mapsto j-1, and [k−1]→{1,…,k−1}[k-1]\to\{1,\dots,k-1\}, j↦jj\mapsto j; and the sum over a singleton {s}\{s\}, computed with [1]→{s}[1]\to\{s\}, 1↦s1\mapsto s, equals its term ese_{s} by claim 1 of Properties of Finite Sums. So Sums over Finite Index Sets: Finite Unions, Disjoint Unions, Vanishing Terms, Dependent Pairs, Conjugation and the Modulus §disjoint-union gives E=∑i=0k−2ei+ek−1=e0+∑i=1k−1eiE=\sum_{i=0}^{k-2}e_{i}+e_{k-1}=e_{0}+\sum_{i=1}^{k-1}e_{i}, whence ∑i=0k−2ei=E−ek−1≤E\sum_{i=0}^{k-2}e_{i}=E-e_{k-1}\le E and ∑i=1k−1ei=E−e0≤E\sum_{i=1}^{k-1}e_{i}=E-e_{0}\le E, because ek−1,e0≥0e_{k-1},e_{0}\ge0 (Step 4). Hence ∑u=0k−2yu≤12(E+E)=E\sum_{u=0}^{k-2}y_{u}\le\tfrac12(E+E)=E by claims 2, 3 and 5 of Elementary Arithmetic in an Ordered Field. Combining with Step 3,

S=E+∑u=0k−2ou≥E−∑u=0k−2yu≥E−E=0.S=E+\sum_{u=0}^{k-2}o_{u}\ge E-\sum_{u=0}^{k-2}y_{u}\ge E-E=0 .

So λ((an−bn)(a−b))=S\lambda\bigl((a^{n}-b^{n})(a-b)\bigr)=S is real and nonnegative.

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