Many-body chirality methodology for topological stabilizer states — formulated as obstruction to complex conjugation via finite-depth local operations, with four-partite obstruction and intrinsic imaginarity.
Scanned 9/11/2026
Install to Claude Code
npx -y skills add hiyenwong/ai_collection --skill many-body-chirality-stabilizer --agent claude-codeInstalls into .claude/skills of the current project.
Are you the author of Many Body Chirality Stabilizer?
Add the live security badge to your README — it updates automatically with every re-scan.
[](https://www.skillsdirectory.com/skills/hiyenwong-many-body-chirality-stabilizer-ai-collection)More formats (shields.io, HTML) on the badges page.
---
name: many-body-chirality-stabilizer
description: "Many-body chirality methodology for topological stabilizer states — formulated as obstruction to complex conjugation via finite-depth local operations, with four-partite obstruction and intrinsic imaginarity."
---
# Many-Body Chirality in Stabilizer States
## Description
Methodology for characterizing many-body chirality in topological stabilizer states. Chirality is formulated as an obstruction to transforming a quantum state into its complex conjugate through finite-depth local operations.
## Activation Keywords
- many-body chirality
- topological stabilizer states
- complex conjugation obstruction
- many-body imaginarity
- anyon theory
- 多体手性
- 拓扑稳定子态
- 量子态手性分析
## Core Concepts
### Key Finding (arXiv:2606.20472)
Many-body chirality is an obstruction to transforming a quantum state into its complex conjugate via finite-depth local operations (quantum channels).
### Main Results
1. **Stabilizer Realizations**: Rigorously established for Z_d^(k) anyon theories
2. **Mirror Invariance Criterion**: Complex conjugation implementable by local quantum channels IFF underlying anyon data are mirror invariant
3. **Four-Partite Obstruction**: The chirality obstruction is intrinsically four-partite, invisible to tripartite entanglement structure
4. **Intrinsic Imaginarity**: Z_d states with d > 2 possess intrinsic many-body imaginarity — complex phase structure cannot be removed by finite-depth local unitaries
### Evades Conventional Diagnostics
Examples with:
- Vanishing modular commutator
- Vanishing chiral central charge
- Commuting-projector realizations
## Methodology
### Step 1: Define Many-Body Chirality
- Formulate as obstruction: state |psi> cannot be mapped to |psi*> (complex conjugate)
- Through finite-depth local quantum channels (not just unitaries)
- This is stronger than unitary obstruction
### Step 2: Check Anyon Data Mirror Invariance
- Extract the underlying anyon data from the stabilizer state
- Test if anyon data are mirror invariant
- If NOT mirror invariant → state is many-body chiral
### Step 3: Four-Partite Analysis
- Use four-partite entanglement structure to detect chirality
- Tripartite measures (modular commutator, chiral central charge) may vanish
- Four-partite obstruction is the fundamental diagnostic
### Step 4: Test for Intrinsic Imaginarity
- For Z_d states with d > 2:
- Complex phase structure cannot be removed
- Even states that are NOT many-body chiral may have intrinsic imaginarity
- This is a strictly weaker condition than chirality
### Step 5: Experimental Detection
- Measure entanglement structure at four-partite level
- Compare with tripartite diagnostics
- States with vanishing modular commutator but non-trivial four-partite obstruction are chiral
## Usage Patterns
### Pattern 1: Chirality Detection in Stabilizer Codes
When analyzing a new stabilizer code:
1. Extract anyon data from the code
2. Test mirror invariance
3. If not mirror invariant → chiral
4. Verify with four-partite obstruction if conventional diagnostics fail
### Pattern 2: Distinguishing Chirality from Imaginarity
1. Check four-partite obstruction → detects chirality
2. Check complex phase removability → detects imaginarity
3. Chirality implies imaginarity (for d > 2), but not vice versa
### Pattern 3: Commuting-Projector Chiral States
When conventional diagnostics (modular commutator, chiral central charge) vanish:
1. Use four-partite obstruction analysis
2. States can be chiral even with commuting-projector Hamiltonians
3. This reveals forms of chirality invisible to standard tools
## Error Handling
### Vanishing Conventional Diagnostics
If modular commutator and chiral central charge both vanish:
- This does NOT mean the state is non-chiral
- Use four-partite obstruction analysis
- Check anyon data mirror invariance directly
### d = 2 Edge Case
- For d = 2 (qubit stabilizer states):
- Intrinsic imaginarity may not hold
- Chirality still detectable via four-partite obstruction
- Mirror invariance criterion still applies
## Resources
- arXiv:2606.20472 "Many-body chirality of topological stabilizer states"
- Related skills: topological-quantum-computing, quantum-error-correction-methods
## Notes
- Rigorous mathematical framework with proofs
- Applies to stabilizer realizations of Z_d^(k) anyon theories
- Opens new diagnostic tools beyond modular commutator
- Intrinsic imaginarity is a novel concept for d > 2 stabilizer statesIs this your skill, or is something wrong with this listing? Request removal or report an issue. Author removals are honored within 72 hours.
No comments yet. Be the first to comment!