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| bib:albantakis2023computing [2026/01/28 10:47] – [3.7 Plain-language translation (no IIT terms) with the full math pipeline] kymki | bib:albantakis2023computing [2026/05/21 06:29] (current) – [Steelman] kymki | ||
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| ===== BibTeX ===== | ===== BibTeX ===== | ||
| - | < | + | < |
| @article{albantakis2023computing, | @article{albantakis2023computing, | ||
| title={Computing the integrated information of a quantum mechanism}, | title={Computing the integrated information of a quantum mechanism}, | ||
| Line 29: | Line 29: | ||
| } | } | ||
| </ | </ | ||
| + | ====== Albantakis et al. (2023) — QM re-formulation and failure modes ====== | ||
| - | ===== One-paragraph summary (plain language) ===== | + | Im reading this with minimal background |
| - | The paper proposes a method (QIIT/ | + | |
| - | + | ||
| - | ===== Review ===== | + | |
| - | + | ||
| - | ==== What it claims to do (in operational terms) ==== | + | |
| - | * Defines quantum cause/ | + | |
| - | * Defines an “intrinsic difference” measure (QID) between a constrained repertoire and a baseline repertoire. | + | |
| - | * Defines “integration” by how much this measure drops under partitions (analogous to classical | + | |
| - | + | ||
| - | ==== What is genuinely new (vs renaming) ==== | + | |
| - | * A concrete proposal for handling entanglement when factorizing repertoires (nontrivial compared to classical product-factor approaches). | + | |
| - | * A specific divergence-like measure (QID) intended to encode “intrinsic” rather than channel-designer information. | + | |
| - | + | ||
| - | ==== What looks like repackaging / relabeling ==== | + | |
| - | * “Mechanism” ≈ chosen subsystem. | + | |
| - | * “Purview” ≈ another chosen subsystem. | + | |
| - | * “Repertoire” ≈ a (conditional / counterfactual) reduced density matrix. | + | |
| - | * The conceptual novelty is not in the quantum objects, but in the *interpretation* (intrinsic/ | + | |
| - | + | ||
| - | ==== Core conceptual friction points (physics-first critique) ==== | + | |
| - | - **Counterfactual noise injection: | + | |
| - | - **Factorization dependence: | + | |
| - | - **Unitary bias / measurement gap: | + | |
| - | - **Mixed-state ambiguity: | + | |
| - | + | ||
| - | ==== Where the prose risks misleading the reader ==== | + | |
| - | * Phrases like “the system knows” or “specifies information about itself” read like ontology, but the actual operations are: choose a partition, apply an intervention/ | + | |
| - | * The mathematical pipeline can be valid as a *defined metric*, but the paper’s language can make it sound like a derived physical necessity. | + | |
| - | + | ||
| - | ==== Strongest charitable | + | |
| - | The framework | + | |
| - | + | ||
| - | ==== Strongest skeptical reading ==== | + | |
| - | It is a rebranding of subsystem/ | + | |
| - | + | ||
| - | ===== Notes / excerpts ===== | + | |
| - | * (Add your own quotes here as you read.) | + | |
| - | * (Add page/ | + | |
| - | + | ||
| - | ===== Open questions to test the framework ===== | + | |
| - | - If you compute the quantity under two physically equivalent descriptions (different tensor factorizations / dilations), do you get the same “intrinsic” structure? | + | |
| - | - If you replace “maximally mixed noise” with a physically motivated environment state (thermal, constrained by energy), how stable are the results? | + | |
| - | - Does QID overemphasize top-eigenvalue behavior in ways that wash out phase-sensitive/ | + | |
| - | + | ||
| - | ====== Albantakis et al. (2023) — QM re-formulation and failure modes ====== | + | |
| - | This note rewrites the paper’s core definitions in standard quantum information language, and isolates where the framework is (i) pure relabeling, (ii) a specific intervention convention, and (iii) where it becomes physically ambiguous. | + | This note rewrites the paper’s core definitions in standard quantum information language, and tries to explain conclusions from that standpoint. The case may be that I completely miss subtleties due to not being well read in IIT. |
| ===== 1. Translation into standard QM language ===== | ===== 1. Translation into standard QM language ===== | ||
| Line 273: | Line 229: | ||
| ==== 3.5 The score $\varphi(m, | ==== 3.5 The score $\varphi(m, | ||
| - | They define an “integrated information for this purview under this partition” as a divergence between: | + | Let (Q) be factorized and let |
| + | $$ | ||
| + | T:\mathcal B(\mathcal H_Q)\to\mathcal B(\mathcal H_Q)) | ||
| + | $$ | ||
| + | be the global channel. For a chosen **input subsystem** (M) prepared in state $\rho_M$, define the **intervention-induced effective channel** | ||
| + | $$ | ||
| - | - the full repertoire $\pi_e(Z\mid m)$, and | + | \mathcal E_{M\to Z}(X): |
| - | - the cut repertoire $\pi_e^{\theta}(Z\mid m)$, | + | \qquad \tau_{M^0}:=\frac{I_{M^0}}{d_{M^0}}, |
| - | using their QID: | ||
| $$ | $$ | ||
| - | \varphi(m,Z,\theta) | + | and the corresponding **output marginal** on the chosen **target subsystem** |
| - | \; | + | |
| - | \mathrm{QID}\Bigl(\pi_e(Z\mid m)\; | + | |
| $$ | $$ | ||
| - | Crucial detail: with their maximally mixed baseline choice, QID behaves like a **max-eigenvalue-weighted** distinguishability, | + | \rho_Z:=\mathcal E_{M\to |
| - | (Their Eq. (31) writes this out in components and evaluates it at the maximizing eigenstate.) | + | $$ |
| - | ---- | + | For a partition $\theta\in\Theta(M, |
| + | $$ | ||
| + | |||
| + | \sigma_Z^{(\theta)}: | ||
| + | |||
| + | $$ | ||
| + | |||
| + | Now diagonalize | ||
| + | $$ | ||
| + | |||
| + | \rho_Z=\sum_i p_i|i\rangle\langle i|,\qquad | ||
| + | \sigma_Z^{(\theta)}=\sum_j q_j|j\rangle\langle j|, | ||
| + | \qquad | ||
| + | P_{ij}: | ||
| + | |||
| + | $$ | ||
| + | **Intrinsic (selected) effect state.** The paper first selects a particular eigenstate $|i^*\rangle$ of $\rho_Z$ via an “intrinsic information vs baseline” optimization. With their maximally mixed baseline on $Z$, this selection reduces to choosing the **largest-eigenvalue eigenvector** of $\rho_Z$ (or the corresponding eigenspace if degenerate). Call that chosen eigenstate | ||
| + | $$ | ||
| + | |||
| + | z' | ||
| + | |||
| + | $$ | ||
| + | **Integrated effect information for a partition.** The paper then evaluates its QID expression **at that chosen eigenstate** (not by maximizing over (i) again): | ||
| + | $$ | ||
| + | |||
| + | \phi_e(m, | ||
| + | : | ||
| + | = | ||
| + | |||
| + | p_{i^*}\left(\log p_{i^*}-\sum_j P_{i^*j}\log q_j\right). | ||
| + | |||
| + | $$ | ||
| + | Equivalently, | ||
| + | $$ | ||
| + | |||
| + | \bar q_{i^*}: | ||
| + | |||
| + | $$ | ||
| + | so that | ||
| + | $$ | ||
| + | |||
| + | \phi_e(m, | ||
| + | |||
| + | $$ | ||
| ==== 3.6 Optimization: | ==== 3.6 Optimization: | ||
| - | For each subset | + | For fixed $M,\rho_M$ and candidate target |
| $$ | $$ | ||
| - | \theta^{\star}(m,Z) | + | \theta'(m,Z) |
| - | \;:=\; | + | = |
| - | \arg\min_{\theta}\;\varphi(m, | + | \arg\min_{\theta\in\Theta(M, |
| + | \frac{\phi_e(m, | ||
| $$ | $$ | ||
| + | Here $\max*{T' | ||
| - | Then they define | + | Then the (reported) |
| $$ | $$ | ||
| - | \varphi_e(m) | + | \phi_e(m,Z):=\phi_e(m,Z,\theta'(m,Z)). |
| - | \;:=\; | + | |
| - | \max_{Z\subseteq Q}\;\min_{\theta}\;\varphi(m,Z,\theta). | + | |
| $$ | $$ | ||
| - | (They do an analogous construction for causes and combine them in the full IIT-style definition.) | + | Finally, the best target subsystem |
| + | $$ | ||
| + | Z^**e(m)=\arg\max*{Z\subseteq Q}\phi_e(m, | ||
| + | \qquad | ||
| + | \phi_e(m)=\max_{Z\subseteq Q}\phi_e(m, | ||
| + | $$ | ||
| - | ---- | ||
| ==== 3.7 Mathematics Framework ==== | ==== 3.7 Mathematics Framework ==== | ||
| Line 551: | Line 556: | ||
| ==== Steelman ==== | ==== Steelman ==== | ||
| - | As a *defined* counterfactual causal attribution scheme, the framework: | + | As a defined counterfactual causal attribution scheme, the framework: |
| * avoids common-cause “spurious correlation” effects by construction (their COPY-XOR/ | * avoids common-cause “spurious correlation” effects by construction (their COPY-XOR/ | ||
| * tries to preserve entanglement-generated correlations by clustering entanglement before taking products, | * tries to preserve entanglement-generated correlations by clustering entanglement before taking products, | ||