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Shadow Theory

Target-Relative Necessity of Completion: When Readout Loss Obstructs, and What a Sufficient Extension Must Retain

The minimal completion for the spectral target

Jeremy RodgersSection 12 of 16Original PDF ↗Publication DOI ↗

The minimal completion for the spectral target

Curvature is insufficient for QspecQ_{\mathrm{spec}}. Holonomy is manifestly sufficient, since by Proposition 10.1 the spectrum is a function of θ\theta mod 2π2\pi. The question this section answers is the sharp one: how much less than holonomy is enough? The answer is: strictly less. The spectral target sees holonomy only up to inversion.

Holonomy is sufficient

Proposition 11.1 (Holonomy completes the curvature readout for the spectrum).

The identity map e=id⁡ ⁣:Sflat→Sflate=\operatorname{id}\colon S_{\mathrm{flat}}\to S_{\mathrm{flat}}, equivalently the holonomy map h ⁣:Sflat→U(1)h\colon S_{\mathrm{flat}}\to\mathrm{U}(1), h(θ)=eiθh(\theta)=e^{i\theta}, is a readout extension of pFp_F that is sufficient for QspecQ_{\mathrm{spec}}.

Proof. hh is a bijection Sflat→U(1)S_{\mathrm{flat}}\to\mathrm{U}(1) by (32) and (33), hence surjective, and pF=u∘hp_F=u\circ h with u ⁣:U(1)→{0}u\colon\mathrm{U}(1)\to\{0\} the constant map, so hh is a readout extension in the sense of Definition 6.1. Define b ⁣:U(1)→Aspecb\colon\mathrm{U}(1)\to A_{\mathrm{spec}} by b(eiθ):=Spec⁡(Hθ)b(e^{i\theta}):=\operatorname{Spec}(H_\theta); this is well defined because, as shown at the end of the proof of Proposition 10.1, Spec⁡(Hθ)\operatorname{Spec}(H_\theta) depends only on θ\theta mod 2π2\pi, i.e. only on eiθe^{i\theta}. Then aspec=b∘ha_{\mathrm{spec}}=b\circ h, so hh is QspecQ_{\mathrm{spec}}-sufficient by Definition 6.3. ◻

Spectral rigidity: the exact equivalence

Theorem 11.2 (Isospectrality iff θ′≡±θ\theta'\equiv\pm\theta).

For θ,θ′∈R\theta,\theta'\in\mathbb{R}, Spec⁡(Hθ)=Spec⁡(Hθ′)⟺θ′≡θ  or  θ′≡−θ(mod2π),(48) \operatorname{Spec}(H_\theta)=\operatorname{Spec}(H_{\theta'}) \qquad\Longleftrightarrow\qquad \theta'\equiv\theta \ \ \text{or}\ \ \theta'\equiv-\theta \pmod{2\pi},\tag{48} where the spectra are compared as multisets, with multiplicities.

Proof. (⇐\Leftarrow) Reverse direction. Suppose first θ′≡θ(mod2π)\theta'\equiv\theta\pmod{2\pi}. Then Spec⁡(Hθ′)=Spec⁡(Hθ)\operatorname{Spec}(H_{\theta'})=\operatorname{Spec}(H_\theta) by the invariance established at the end of the proof of Proposition 10.1.

Suppose next θ′≡−θ(mod2π)\theta'\equiv-\theta \pmod{2\pi}. By the same invariance it suffices to treat θ′=−θ\theta'=-\theta. Then for every n∈Zn\in\mathbb{Z}, λ−n(−θ)=(2π(−n)−(−θ)L) ⁣2=(−(2πn−θ)L) ⁣2=(2πn−θL) ⁣2=λn(θ).(49) \lambda_{-n}(-\theta) =\left(\frac{2\pi(-n)-(-\theta)}{L}\right)^{\!2} =\left(\frac{-(2\pi n-\theta)}{L}\right)^{\!2} =\left(\frac{2\pi n-\theta}{L}\right)^{\!2} =\lambda_n(\theta).\tag{49} The map n↦−nn\mapsto -n is a bijection of Z\mathbb{Z} onto itself. Hence (49) exhibits a bijection between the indexing set of Spec⁡(H−θ)\operatorname{Spec}(H_{-\theta}) and that of Spec⁡(Hθ)\operatorname{Spec}(H_\theta) carrying each eigenvalue to an equal eigenvalue. A multiset is determined by its indexed family up to bijective reindexing, so the two multisets are equal, with all multiplicities: m−θ(λ)=#{n:λn(−θ)=λ}=#{n:λ−n(−θ)=λ}=#{n:λn(θ)=λ}=mθ(λ).m_{-\theta}(\lambda)=\#\{n:\lambda_n(-\theta)=\lambda\} =\#\{n:\lambda_{-n}(-\theta)=\lambda\} =\#\{n:\lambda_{n}(\theta)=\lambda\}=m_\theta(\lambda). So Spec⁡(H−θ)=Spec⁡(Hθ)\operatorname{Spec}(H_{-\theta})=\operatorname{Spec}(H_\theta). Concretely, the reindexing n↦−nn\mapsto -n is implemented on the Hilbert space by complex conjugation, ψn↦ψn‾=ψ−n\psi_n\mapsto\overline{\psi_n}=\psi_{-n}, which is an antiunitary intertwiner between HθH_\theta and H−θH_{-\theta}; but the elementary reindexing argument above is already complete and requires nothing further.

(⇒\Rightarrow) Forward direction. Suppose Spec⁡(Hθ)=Spec⁡(Hθ′)\operatorname{Spec}(H_\theta)=\operatorname{Spec}(H_{\theta'}). We recover θ\theta up to sign and 2π2\pi from the spectrum, using the lowest eigenvalue.

Define, for any θ∈R\theta\in\mathbb{R}, the principal representative α(θ)∈[0,π]the unique number in [0,π] with θ≡α(θ)  or  θ≡−α(θ)(mod2π).(50) \alpha(\theta)\in[0,\pi] \qquad\text{the unique number in } [0,\pi] \text{ with } \theta\equiv\alpha(\theta) \ \text{ or }\ \theta\equiv-\alpha(\theta) \pmod{2\pi}.\tag{50} Existence and uniqueness of α(θ)\alpha(\theta): reduce θ\theta mod 2π2\pi to a representative θ~∈[0,2π)\tilde\theta\in[0,2\pi). If θ~∈[0,π]\tilde\theta\in[0,\pi] set α:=θ~\alpha:=\tilde\theta; if θ~∈(π,2π)\tilde\theta\in(\pi,2\pi) set α:=2π−θ~∈(0,π)\alpha:=2\pi-\tilde\theta\in(0,\pi), and then θ≡θ~=−α(mod2π)\theta\equiv\tilde\theta=-\alpha \pmod{2\pi}. In both cases α∈[0,π]\alpha\in[0,\pi] and θ≡±α\theta\equiv\pm\alpha. For uniqueness, suppose α,β∈[0,π]\alpha,\beta\in[0,\pi] both work; then α≡±β(mod2π)\alpha\equiv\pm\beta\pmod{2\pi}. If α≡β\alpha\equiv\beta then α−β∈2πZ\alpha-\beta\in 2\pi\mathbb{Z} and ∣α−β∣≤π<2π|\alpha-\beta|\leq\pi<2\pi, forcing α=β\alpha=\beta. If α≡−β\alpha\equiv-\beta then α+β∈2πZ\alpha+\beta\in2\pi\mathbb{Z} with 0≤α+β≤2π0\le\alpha+\beta\le 2\pi, so α+β∈{0,2π}\alpha+\beta\in\{0,2\pi\}, giving either α=β=0\alpha=\beta=0 or α=β=π\alpha=\beta=\pi. In all cases α=β\alpha=\beta.

We claim λmin⁡(θ):=min⁡Spec⁡(Hθ)=α(θ)2L2.(51) \lambda_{\min}(\theta):=\min\operatorname{Spec}(H_\theta)=\frac{\alpha(\theta)^2}{L^2}.\tag{51} To see this, note λn(θ)=(2πn−θL)2\lambda_n(\theta)=\bigl(\tfrac{2\pi n-\theta}{L}\bigr)^2, so min⁡n∈Zλn(θ)=1L2min⁡n∈Z (2πn−θ)2=1L2(dist⁡(θ, 2πZ)) ⁣2,\min_{n\in\mathbb{Z}}\lambda_n(\theta) =\frac{1}{L^2}\min_{n\in\mathbb{Z}}\,(2\pi n-\theta)^2 =\frac{1}{L^2}\Bigl(\operatorname{dist}\bigl(\theta,\,2\pi\mathbb{Z}\bigr)\Bigr)^{\!2}, the minimum being attained since (2πn−θ)2→∞(2\pi n-\theta)^2\to\infty as ∣n∣→∞|n|\to\infty. It remains to identify dist⁡(θ,2πZ)=α(θ)\operatorname{dist}(\theta,2\pi\mathbb{Z})=\alpha(\theta). Write θ≡±α\theta\equiv\pm\alpha with α=α(θ)∈[0,π]\alpha=\alpha(\theta)\in[0,\pi]; since 2πZ2\pi\mathbb{Z} is invariant under negation and under translation by 2π2\pi, we get dist⁡(θ,2πZ)=dist⁡(±α,2πZ)=dist⁡(α,2πZ)\operatorname{dist}(\theta,2\pi\mathbb{Z})=\operatorname{dist}(\pm\alpha,2\pi\mathbb{Z}) =\operatorname{dist}(\alpha,2\pi\mathbb{Z}). For α∈[0,π]\alpha\in[0,\pi] the nearest point of 2πZ2\pi\mathbb{Z} is 00, since the next candidates are ±2π\pm2\pi at distance 2π−α≥π≥α2\pi-\alpha\ge\pi\ge\alpha and 2π+α>α2\pi+\alpha>\alpha. Hence dist⁡(α,2πZ)=α\operatorname{dist}(\alpha,2\pi\mathbb{Z})=\alpha, proving (51).

Now assume Spec⁡(Hθ)=Spec⁡(Hθ′)\operatorname{Spec}(H_\theta)=\operatorname{Spec}(H_{\theta'}). Equal multisets have equal minima, so by (51) α(θ)2L2=λmin⁡(θ)=λmin⁡(θ′)=α(θ′)2L2,\frac{\alpha(\theta)^2}{L^2}=\lambda_{\min}(\theta)=\lambda_{\min}(\theta') =\frac{\alpha(\theta')^2}{L^2}, whence α(θ)2=α(θ′)2\alpha(\theta)^2=\alpha(\theta')^2. Since α(θ),α(θ′)∈[0,π]\alpha(\theta),\alpha(\theta')\in[0,\pi] are both nonnegative, α(θ)=α(θ′)=:α\alpha(\theta)=\alpha(\theta')=:\alpha. By (50), θ≡±α\theta\equiv\pm\alpha and θ′≡±α(mod2π)\theta'\equiv\pm\alpha\pmod{2\pi}. Combining the four sign cases: if θ≡α\theta\equiv\alpha and θ′≡α\theta'\equiv\alpha then θ′≡θ\theta'\equiv\theta; if θ≡α\theta\equiv\alpha and θ′≡−α\theta'\equiv-\alpha then θ′≡−θ\theta'\equiv-\theta; if θ≡−α\theta\equiv-\alpha and θ′≡α\theta'\equiv\alpha then θ′≡−θ\theta'\equiv-\theta; if θ≡−α\theta\equiv-\alpha and θ′≡−α\theta'\equiv-\alpha then θ′≡θ\theta'\equiv\theta. In every case θ′≡±θ(mod2π)\theta'\equiv\pm\theta\pmod{2\pi}, as required. ◻

Corollary 11.3 (The spectral target sees holonomy only modulo inversion).

Define the equivalence ∼spec\sim_{\mathrm{spec}} on Sflat≅U(1)S_{\mathrm{flat}}\cong\mathrm{U}(1) by eiθ∼speceiθ′⟺θ′≡±θ(mod2π)⟺eiθ′∈{eiθ,e−iθ}.(52) e^{i\theta}\sim_{\mathrm{spec}}e^{i\theta'} \qquad\Longleftrightarrow\qquad \theta'\equiv\pm\theta\pmod{2\pi} \qquad\Longleftrightarrow\qquad e^{i\theta'}\in\{e^{i\theta},e^{-i\theta}\}.\tag{52} Then ∼spec\sim_{\mathrm{spec}} is exactly the answer equivalence of the spectral target: aspec(θ)=aspec(θ′)a_{\mathrm{spec}}(\theta)=a_{\mathrm{spec}}(\theta') iff θ∼specθ′\theta\sim_{\mathrm{spec}}\theta'.

Proof. Immediate from Theorem 11.2 and Definition 10.3. ◻

The coarsest sufficient completion and its coordinate

Theorem 11.4 (cos⁡θ\cos\theta coordinatizes the minimal spectral completion).

Let c ⁣:Sflat⟶[−1,1],c(θ):=cos⁡θ.(53) c\colon S_{\mathrm{flat}}\longrightarrow[-1,1], \qquad c(\theta):=\cos\theta .\tag{53} Then:

  1. cc is a well-defined surjection onto [−1,1][-1,1];

  2. c(θ)=c(θ′)c(\theta)=c(\theta') if and only if θ∼specθ′\theta\sim_{\mathrm{spec}}\theta'; that is, cc realizes exactly the spectral equivalence classes;

  3. cc is a readout extension of pFp_F that is sufficient for QspecQ_{\mathrm{spec}};

  4. cc is a coarsest such extension: the induced map φ[−1,1] ⁣:[−1,1]→EQspec\varphi_{[-1,1]}\colon[-1,1]\to E_{Q_{\mathrm{spec}}} of Theorem 8.3 is a bijection. Consequently every QspecQ_{\mathrm{spec}}-sufficient readout extension ee must separate source states with distinct values of cos⁡θ\cos\theta.

Proof. (1) cos⁡\cos is 2π2\pi-periodic, so cc descends to R/2πZ\mathbb{R}/2\pi\mathbb{Z}; its image is [−1,1][-1,1] since cos⁡\cos restricted to [0,π][0,\pi] is already onto [−1,1][-1,1].

(2) The function cos⁡\cos is strictly decreasing on [0,π][0,\pi], hence injective there. Given θ,θ′\theta,\theta', write α=α(θ),α′=α(θ′)∈[0,π]\alpha=\alpha(\theta),\alpha'=\alpha(\theta')\in[0,\pi] as in (50); since cos⁡\cos is even and 2π2\pi-periodic, cos⁡θ=cos⁡α\cos\theta=\cos\alpha and cos⁡θ′=cos⁡α′\cos\theta'=\cos\alpha'. Therefore c(θ)=c(θ′)  ⟺  cos⁡α=cos⁡α′  ⟺  α=α′  ⟺  θ′≡±θ(mod2π)  ⟺  θ∼specθ′,c(\theta)=c(\theta') \iff \cos\alpha=\cos\alpha' \iff \alpha=\alpha' \iff \theta'\equiv\pm\theta \pmod{2\pi} \iff \theta\sim_{\mathrm{spec}}\theta', where the second equivalence uses injectivity of cos⁡\cos on [0,π][0,\pi], and the third is the argument at the end of the proof of Theorem 11.2 (equality of principal representatives is equivalent to θ′≡±θ\theta'\equiv\pm\theta).

(3) cc is surjective by (1), and pF=u∘cp_F=u\circ c with u ⁣:[−1,1]→{0}u\colon[-1,1]\to\{0\} constant, so cc is a readout extension. For sufficiency, define bspec ⁣:[−1,1]→Aspecb_{\mathrm{spec}}\colon[-1,1]\to A_{\mathrm{spec}} by bspec(κ):=Spec⁡(Harccos⁡κ),arccos⁡κ∈[0,π].(54) b_{\mathrm{spec}}(\kappa):=\operatorname{Spec}\bigl(H_{\arccos\kappa}\bigr), \qquad \arccos\kappa\in[0,\pi].\tag{54} If c(θ)=κc(\theta)=\kappa then by (2) θ∼specarccos⁡κ\theta\sim_{\mathrm{spec}}\arccos\kappa (both have principal representative arccos⁡κ\arccos\kappa), so by Corollary 11.3 Spec⁡(Hθ)=Spec⁡(Harccos⁡κ)=bspec(c(θ))\operatorname{Spec}(H_\theta)=\operatorname{Spec}(H_{\arccos\kappa})=b_{\mathrm{spec}}(c(\theta)). Hence aspec=bspec∘ca_{\mathrm{spec}}=b_{\mathrm{spec}}\circ c, and cc is QspecQ_{\mathrm{spec}}-sufficient.

(4) Write φ:=φ[−1,1]\varphi:=\varphi_{[-1,1]} and Espec:=EQspecE_{\mathrm{spec}} :=E_{Q_{\mathrm{spec}}} for brevity. By Theorem 8.3, applied to the sufficient extension cc, there is a unique surjection φ ⁣:[−1,1]→Espec\varphi\colon[-1,1]\to E_{\mathrm{spec}} with jQspec=φ∘cj_{Q_{\mathrm{spec}}}=\varphi\circ c, given by φ(κ)=(u(κ), bspec(κ))=(0, bspec(κ)),κ∈[−1,1].(55) \varphi(\kappa) =\bigl(u(\kappa),\,b_{\mathrm{spec}}(\kappa)\bigr) =\bigl(0,\,b_{\mathrm{spec}}(\kappa)\bigr), \qquad \kappa\in[-1,1].\tag{55} It remains to prove injectivity. Suppose φ(κ)=φ(κ′)\varphi(\kappa)=\varphi(\kappa'). Comparing second coordinates in (55) gives bspec(κ)=bspec(κ′)b_{\mathrm{spec}}(\kappa)=b_{\mathrm{spec}}(\kappa'), which by (54) says Spec⁡(Harccos⁡κ)=Spec⁡(Harccos⁡κ′).(56) \operatorname{Spec}\bigl(H_{\arccos\kappa}\bigr)=\operatorname{Spec}\bigl(H_{\arccos\kappa'}\bigr).\tag{56} By Theorem 11.2, (56) forces arccos⁡κ′≡±arccos⁡κ(mod2π)\arccos\kappa'\equiv\pm\arccos\kappa \pmod{2\pi}. Both arccos⁡κ\arccos\kappa and arccos⁡κ′\arccos\kappa' lie in [0,π][0,\pi], so each is its own principal representative in the sense of (50); by the uniqueness established there, they are equal. Applying cos⁡\cos yields κ=κ′\kappa=\kappa'.

Hence φ\varphi is a bijection, and cc carries precisely the distinctions of EspecE_{\mathrm{spec}} , no more and no fewer.

The final assertion follows from Corollary 8.4: if ee is QspecQ_{\mathrm{spec}}-sufficient and c(θ0)≠c(θ1)c(\theta_0)\neq c(\theta_1), then by (2) θ0̸∼specθ1\theta_0\not\sim_{\mathrm{spec}} \theta_1, so by Corollary 11.3 aspec(θ0)≠aspec(θ1)a_{\mathrm{spec}}(\theta_0)\neq a_{\mathrm{spec}} (\theta_1), and Theorem 7.1 forces e(θ0)≠e(θ1)e(\theta_0)\neq e(\theta_1). ◻

Remark 11.5 (What is and is not claimed about cos⁡θ\cos\theta).

Theorem 11.4 says that cos⁡θ\cos\theta coordinatizes the coarsest completion sufficient for QspecQ_{\mathrm{spec}}: its level sets are exactly the spectral equivalence classes, and it separates exactly what must be separated. It does not say that cos⁡θ\cos\theta is the unique possible numerical coordinate on EQspecE_{Q_{\mathrm{spec}}}. Any injective function of cos⁡θ\cos\theta , for instance 12(1−cos⁡θ)\tfrac12(1-\cos\theta), or α(θ)\alpha(\theta) itself, or the ground-state energy λmin⁡=α(θ)2/L2\lambda_{\min}=\alpha(\theta)^2/L^2 , has the same level sets and coordinatizes the same quotient equally well; the completion is the quotient, and the coordinate is a labeling of it. Nor does Theorem 11.4 say that cos⁡θ\cos\theta is minimal for every physical target on SflatS_{\mathrm{flat}}. It is minimal for the nominated spectral target, and for that target only.

Example 11.6 (A target for which cos⁡θ\cos\theta is insufficient: oriented transport).

Consider the target QHolQ_{\mathop{\mathrm{Hol}}} with AQHol=U(1)A_{Q_{\mathop{\mathrm{Hol}}}}=\mathrm{U}(1) and correct-answer map aHol(θ)=eiθa_{\mathop{\mathrm{Hol}}}(\theta)=e^{i\theta}: “what phase does a unit charge acquire on being transported once around the circle in the positive direction?” Take θ=π/2\theta=\pi/2 and θ′=−π/2\theta'=-\pi/2. Then c(π/2)=cos⁡(π/2)=0=cos⁡(−π/2)=c(−π/2),c(\pi/2)=\cos(\pi/2)=0=\cos(-\pi/2)=c(-\pi/2), so cc does not separate these two states; but aHol(π/2)=eiπ/2=i≠−i=e−iπ/2=aHol(−π/2)a_{\mathop{\mathrm{Hol}}}(\pi/2)=e^{i\pi/2}=i\neq -i=e^{-i\pi/2}=a_{\mathop{\mathrm{Hol}}}(-\pi/2). By Theorem 7.1, cc is not QHolQ_{\mathop{\mathrm{Hol}}}-sufficient. By Theorem 11.2 the two states are nonetheless isospectral, Spec⁡(Hπ/2)=Spec⁡(H−π/2)\operatorname{Spec}(H_{\pi/2})=\operatorname{Spec}(H_{-\pi/2}), consistent with cc being sufficient for QspecQ_{\mathrm{spec}}.

The full holonomy map hh is QHolQ_{\mathop{\mathrm{Hol}}}-sufficient (take b=id⁡U(1)b=\operatorname{id}_{\mathrm{U}(1)}), and by Corollary 8.4 it is coarsest for that target, since jQHol=(pF,aHol)j_{Q_{\mathop{\mathrm{Hol}}}}=(p_F,a_{\mathop{\mathrm{Hol}}}) has the same level sets as hh. So on one and the same reduced source space, with one and the same readout, the minimal completion for the transport target is the full holonomy circle, while the minimal completion for the spectral target is its strictly coarser inversion quotient U(1)/(z∼zˉ)≅[−1,1]\mathrm{U}(1)/(z\sim\bar z)\cong[-1,1]. The scalar spectrum is blind to orientation; oriented transport is not. This is target-relativity of completion in its sharpest form, and it is not a defect of either description: each retains exactly what its question requires.

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