Invertibility and the nonzero spectrum of a row-compact operator #
Let R be a complete ultrametric normed commutative ring with Tate scalars, I a discrete
index type, and u a row-compact endomorphism of the model space C₀(I, R) with Fredholm
series H_u(T) = det (1 - T u), the principal-minor series u.matrixCoeff.charPowerSeries.
The Fredholm series detects exactly which operators 1 - a • u are invertible in the algebra
of continuous endomorphisms:
IsUnit (1 - a • u) ↔ IsUnit (H_u(a))
(ContinuousLinearMap.IsRowCompact.isUnit_one_sub_smul_iff).
The resolvent V(a) supplies the inverse when H_u(a) is a unit, and multiplicativity of the
Fredholm determinant gives the converse. In terms of the spectrum of u over R, the inverse
r⁻¹ of a unit r lies in the spectrum exactly when H_u(r) is not a unit
(ContinuousLinearMap.IsRowCompact.inv_mem_spectrum_iff). Over coefficient rings with
nilpotents this is a condition on units, not on vanishing.
Over a complete nontrivially normed ultrametric field K it becomes Serre's description of the
nonzero spectrum: for μ ≠ 0,
μ ∈ spectrum K u ↔ H_u(μ⁻¹) = 0
(ContinuousLinearMap.IsRowCompact.mem_spectrum_iff_evalAt_inv_eq_zero).
Since H_u(0) = 1, every zero a of H_u is nonzero, and the zeros of H_u are exactly the
inverses of the nonzero spectral values
(ContinuousLinearMap.IsRowCompact.evalAt_charPowerSeries_eq_zero_iff). Nothing is asserted
about 0 ∈ spectrum K u, which the Fredholm series does not see.
Strassmann's theorem then bounds the spectrum away from zero. If H_u is distinguished of degree
s at the radius ε⁻¹, that is, s is the largest index at which ‖cₙ‖ ε⁻ⁿ attains its
maximum, then at most s spectral values have norm at least ε
(ContinuousLinearMap.IsRowCompact.encard_setOf_mem_spectrum_le). Such an s exists for every
ε > 0, since H_u is entire and nonzero, so only finitely many spectral values have norm
bounded below by a positive number, and every nonzero spectral value is isolated in the spectrum.
Zero may be an accumulation point of the spectrum. The same bound, finiteness and isolation hold
for the extension of u to C₀(I, L) along any complete normed field extension L of K, such
as a complete field over which H_u splits: the spectrum of the extension is controlled by the
zeros of H_u in L.
Main results #
ContinuousLinearMap.IsRowCompact.isUnit_one_sub_smul_iff:1 - a • uis invertible if and only ifH_u(a)is a unit.ContinuousLinearMap.IsRowCompact.isUnit_one_sub_iff:1 - uis invertible if and only if the Fredholm determinantdet (1 - u)is a unit.ContinuousLinearMap.IsRowCompact.mem_spectrum_iff_evalAt_inv_eq_zero: over a field, a nonzeroμlies in the spectrum ofuif and only ifH_u(μ⁻¹) = 0.ContinuousLinearMap.IsRowCompact.encard_setOf_mem_spectrum_mapCoeffs_leandContinuousLinearMap.IsRowCompact.finite_setOf_mem_spectrum_mapCoeffs: after extension to a complete normed fieldL, at mostsspectral values, and in any case finitely many, have norm at leastε, whereH_uis distinguished of degreesatε⁻¹.ContinuousLinearMap.IsRowCompact.encard_setOf_mem_spectrum_leandContinuousLinearMap.IsRowCompact.finite_setOf_mem_spectrum: the same overKitself.ContinuousLinearMap.IsRowCompact.eventually_notMem_spectrum_mapCoeffsandContinuousLinearMap.IsRowCompact.eventually_notMem_spectrum: every nonzero spectral value is isolated in the spectrum, after extension toLand overKitself.
References #
- J.-P. Serre, Endomorphismes complètement continus des espaces de Banach p-adiques, Publ. Math. IHÉS 12 (1962), 69–85, §§5–7.
- R. Coleman, p-adic Banach spaces and families of modular forms, Invent. Math. 127 (1997), 417–479, Appendix A.
Invertibility and the Fredholm series. For a row-compact endomorphism u of C₀(I, R),
the operator 1 - a • u is invertible if and only if the value H_u(a) of the Fredholm series
det (1 - T u) is a unit of R.
Invertibility and the Fredholm determinant. For a row-compact endomorphism u of
C₀(I, R), the operator 1 - u is invertible if and only if the Fredholm determinant
det (1 - u) is a unit of R.
Unit spectral values. For a row-compact endomorphism u of C₀(I, R) and a unit r of
R, the inverse r⁻¹ lies in the spectrum of u if and only if the value H_u(r) of the
Fredholm series is not a unit of R.
The nonzero spectrum of a row-compact operator. For a row-compact endomorphism u of
C₀(I, K) over a complete ultrametric field and μ ≠ 0, μ lies in the spectrum of u if and
only if μ⁻¹ is a zero of the Fredholm series det (1 - T u).
The zeros of the Fredholm series. For a row-compact endomorphism u of C₀(I, K), the
zeros of the Fredholm series det (1 - T u) are exactly the inverses of the nonzero elements of
the spectrum of u. Since det (1 - 0 u) = 1, no zero is 0.
Strassmann's bound for the spectrum. Let u be a row-compact endomorphism of C₀(I, K),
and let its Fredholm series H_u be distinguished of degree s at the radius ε⁻¹. Then the
extension of u to C₀(I, L), for a complete normed field extension L of K, has at most s
spectral values of norm at least ε.
After extension to a complete normed field L, a row-compact endomorphism of C₀(I, K) has
only finitely many spectral values of norm at least ε, for every ε > 0.
Strassmann's bound for the spectrum over the coefficient field: if the Fredholm series of
a row-compact endomorphism u of C₀(I, K) is distinguished of degree s at the radius ε⁻¹,
then u has at most s spectral values of norm at least ε.
A row-compact endomorphism of C₀(I, K) has only finitely many spectral values of norm at
least ε, for every ε > 0.
Nonzero spectral values are isolated. For a row-compact endomorphism u of C₀(I, K),
a complete normed field extension L of K and μ : L with μ ≠ 0, no point of a punctured
neighbourhood of μ lies in the spectrum of the extension of u to C₀(I, L).
Nonzero spectral values are isolated over the coefficient field: for a row-compact
endomorphism u of C₀(I, K) and μ ≠ 0, no point of a punctured neighbourhood of μ lies in
the spectrum of u.