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Fourier spectrum and positivity of the periodic lattice Laplacian

Statement

Let d,L≥1 be integers and let Λd,L:=(Z/LZ)d, where Z/LZ is the quotient set of integers modulo L. Use the quotient addition [a]L+[b]L=[a+b]L and additive inverse −[a]L=[−a]L, and define these operations coordinatewise on Λd,L. For x∈Λd,L, write x~=(x~1,…,x~d)∈{0,…,L−1}d for its unique coordinate representatives. For 1≤j≤d, let ej∈Λd,L have coordinate [1]L in position j and [0]L elsewhere. Count the two terms x+ej and x−ej separately even when they coincide for L=1 or L=2.

For a real-valued function f:Λd,L→R, define

(−Δf)(x):=∑j=1d(2f(x)−f(x+ej)−f(x−ej)).

For a complex-valued function, use the same formula for −Δ, which is its complex-linear extension. Write CΛd,L for the complex-valued functions on Λd,L with pointwise vector operations. For r=(r1,…,rd)∈{0,…,L−1}d, define the function χr:Λd,L→C by

χr(x):=exp⁡ ⁣(2πiL∑j=1drjx~j).

Use the inner product ⟨f,g⟩:=L−d∑x∈Λd,Lf(x)g(x)‾. Identify real functions with coordinate vectors using the lexicographic order on the representatives x~, and let IΛd,L be the identity operator on those functions. A real matrix A is symmetric when AT=A; a real symmetric matrix is positive semidefinite when vTAv≥0 for every real vector v, and positive definite when vTAv>0 for every nonzero real vector v. For all r,s∈{0,…,L−1}d, the inner products satisfy ⟨χr,χs⟩=1 if r=s and 0 otherwise; every complex-valued function on Λd,L is a unique linear combination of the functions χr.

For each r, the equation −Δχr=λrχr holds with λr:=4∑j=1dsin⁡2(πrj/L); this scalar is the eigenvalue associated with χr.

Consequently −Δ is real symmetric positive semidefinite, and for real m2>0 and κ>0 the matrix m2IΛd,L+κ(−Δ) is real symmetric positive definite with eigenvalues m2+4κ∑j=1dsin⁡2(πrj/L)>0.

Statement references

Facts & Assumptions

Given: Integers d,L≥1, the coordinatewise quotient operations, canonical representatives, and discrete Laplacian of the Statement.

[F2]

Quotient addition is [a]L+[b]L=[a+b]L and is independent of representatives; Z/LZ with this operation is an additive abelian group, with inverse −[a]L=[−a]L (Addition and multiplication on Z/n by [a]n+[b]n=[a+b]n and [a]n[b]n=[ab]n, For every natural n, (Z/n,+) is an abelian group, multiplication is a commutative monoid operation, and both distributive laws hold).

[F3]

For N≥1 and integers k,ℓ, ∑u=0N−1e2πi(k−ℓ)u/N is N if k≡ℓ(modN) and is 0 otherwise (Orthogonality of the characters x↦e2πikx/N on Z/NZ).

[F6]

For real t, eit=cos⁡t+isin⁡t and cos⁡(2t)=cos⁡2t−sin⁡2t (exp⁡(x+iy)=ex(cos⁡y+isin⁡y), ∣exp⁡(x+iy)∣=ex, and eiπ+1=0, The addition formulas for sine and cosine).

[F7]

For real t, sin⁡2t+cos⁡2t=1, sin⁡(−t)=−sin⁡t, and cos⁡(−t)=cos⁡t (Pythagorean and parity identities for all six trigonometric functions on their natural domains).

[F8]

Complex conjugation fixes real numbers and sends i to −i (Conjugation is an involutive real-field automorphism, zz‾=∣z∣2, and modulus is definite, multiplicative, and subadditive); together with [F6] and [F7], this gives eit‾=e−it for real t.

Proof

1.1givenF1F2F5algebra

Fix x∈Λd,L and put aj=x~j. By [F1]–[F2], the jth representative of x+ej is aj+1−Lϵj, where ϵj=1 if aj=L−1 and 0 otherwise; the jth representative of x−ej is aj−1+Lηj, where ηj=1 if aj=0 and 0 otherwise. All other representatives are unchanged. Substitution into the definition of χr, followed by the exponential addition law and exp⁡(2πin)=1 for integers n from [F5], gives χr(x+ej)=e2πirj/Lχr(x) and χr(x−ej)=e−2πirj/Lχr(x). This also holds for L=1 and L=2.

1.2F1F3F4F8algebra

For r,s∈{0,…,L−1}d, finite-sum factorization [F4] and the conjugation identity [F8] give ⟨χr,χs⟩=∏j=1dL−1∑u=0L−1e2πi(rj−sj)u/L. By [F1], distinct canonical representatives are incongruent modulo L, so [F3] makes each factor 1 when rj=sj and 0 otherwise. This is the inner-product identity stated above.

2.1F6F7step 1.1algebra

Substituting the shift identities of step 1.1 into −Δ gives −Δχr=∑j=1d(2−e2πirj/L−e−2πirj/L)χr. By [F6]–[F7], each coefficient equals 2−2cos⁡(2πrj/L)=4sin⁡2(πrj/L), proving the eigenvalue formula.

2.2F1F3F4F8step 1.2algebra

For any f:Λd,L→C, set f^(r)=L−d∑y∈Λd,Lf(y)χr(y)‾. By [F4] and [F8], the frequency sum factors as ∑rχr(x)χr(y)‾=∏j=1d∑rj=0L−1e2πirj(x~j−y~j)/L. The canonical-representative theorem [F1] and orthogonality [F3] make this product Ld if x=y in Λd,L and 0 otherwise. Therefore ∑rf^(r)χr(x)=L−d∑yf(y)∑rχr(x)χr(y)‾=f(x) for every x. If a linear combination ∑rcrχr vanishes, taking its inner product with χs and applying step 1.2 gives cs=0 for each s, so the expansion is unique.

3.1givenF2F4step 2.1step 2.2algebra∎

For every real f, the translations x↦x+ej are bijections with inverses x↦x−ej, so reindexing the finite sums [F4] gives ∑xf(x)(−Δf)(x)=∑j=1d∑x(f(x+ej)−f(x))2≥0. Thus −Δ is positive semidefinite; its matrix is symmetric because every shift term is paired with its inverse shift. For nonzero f, fT(m2I+κ(−Δ))f=m2∑xf(x)2+κ∑j=1d∑x(f(x+ej)−f(x))2>0, since m2>0 and κ>0. By steps 2.1 and 2.2, the spanning functions χr satisfy the eigenvalue equations in the Statement, so the combined operator has the displayed eigenvalues.

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