Decoherence, Control, and Symmetry in Quantum Computers VII: qubits under collective decoherence split into spin- irreps with multiplicity Textbook
Motivation
Qubits that sit close together, closer than the wavelength of the environment modes they couple to, are disturbed by that environment in the same way. The resulting noise is collective decoherence: its error operators are the collective spin operators rather than independent errors on each qubit. Chapter 8 of D. M. Bacon's thesis (Decoherence, Control, and Symmetry in Quantum Computers, arXiv:quant-ph/0305025v1, §8.4–§8.7, pp.113–121) derives this regime from spin-boson and amplitude-damping models and then works out the decoherence-free subspaces and subsystems (DFSs) it admits, which is where quantum information can be stored with no active correction at all.
Timeline. Duan and Guo (1997) and Zanardi and Rasetti (1997) observed that collectively coupled qubits support noiseless states (doi:10.1103/PhysRevLett.79.1953, arXiv:quant-ph/9705044). Lidar, Chuang and Whaley (1998) named and characterized decoherence-free subspaces (arXiv:quant-ph/9807004). Knill, Laflamme and Viola (2000) generalized them to noiseless subsystems through the representation theory of the error algebra (arXiv:quant-ph/9908066). Kempe, Bacon, Lidar and Whaley (2001) worked out the collective decoherence case in full, together with universal computation on it (arXiv:quant-ph/0004064); Chapter 8 of the thesis is its exposition.
Setting
The register is qubits, with Hilbert space and computational basis , . The Pauli matrices act on a single qubit, and (Lean: onQubit i (BBPSSW.Distill.pauli α)) is on qubit tensored with the identity elsewhere. The collective operators are
(Lean: collS n α, collPlus n, collMinus n), and the total angular momentum is (totalS2 n). The exchange operator (exchange i j) swaps qubits and .
Under weak collective decoherence the only error is . The Hamming weight (hammingWeight x) counts the 's of , and (dfsWeak n h) is the span of the basis states of Hamming weight .
Under strong collective decoherence the errors generate the complex algebra spanned by products of . The total angular momentum of spin- particles runs over , down to or . The matrices (spinRep (2J) α) form the standard spin- representation of , with diagonal and . For multiplicities , (blockOp n m X) is the block operator acting as on the irrep factor and trivially on the degeneracy factor.
Formalization targets
Goal: (8.41)–(8.43)
There are multiplicities and a unitary with
All three clauses are part of the goal: the form of the generators, the multiplicity formula, and the fact that the collective algebra is the whole block algebra (both inclusions).
Milestones
- (8.32): .
- (8.34): .
- (8.35): , and is the -eigenspace for .
- (C.8): .
- (8.50): in every basis of the form (8.43), and .
Significance
The decomposition is the structure theorem of collective decoherence. Since every error acts as , a state written into the degeneracy factor for one fixed is untouched by every error: this is the strong collective decoherence DF subsystem , of dimension (Definition 8.6.1). The multiplicity formula says how much protected information qubits hold. Three qubits already carry one protected qubit (), and grows like up to a polynomial factor, so the encoding rate tends to one. Chapters 9 and 11 build universal exchange-only computation on these subsystems, and their proofs (Appendix C) induct on exactly this decomposition and on (C.8). (8.50) gives the collective amplitude damping DF subspaces of §8.7.
The facts are textbook angular momentum addition, and the thesis cites (8.42) to Mandel and Wolf rather than proving it. No machine-checked version is known to exist: the platform holds Schur-transform encodings, and nothing proves the multiplicity formula or the algebra decomposition for qubits. The mission yields a reusable Lean account of the collective spin representation on .
Difficulty
The commutation relations and the action of are finite computations, and the dimension count is elementary. The goal asks for more than either. Clause (8.43) requires a single change of basis that brings all three non-commuting generators at once to the standard real spin- matrices, with matching phases in every copy of every irrep. A dimension count fixes the sizes of the blocks but not the basis. Clause (8.42) asks for the exact number of copies of each irrep, a statement about the whole -dimensional representation that no small case settles. Clause (8.41) is an equality of algebras: the products of must reach every operator of the form , with the blocks for different chosen independently. The obvious inclusion follows from (8.43); the reverse inclusion is where the content lies.
Formalization scope
Qubits are Fin n → Fin 2. Operators are Matrix (Fin n → Fin 2) (Fin n → Fin 2) ℂ, and is index , with . The labels and the Pauli matrices are the published BBPSSW.Distill.Axis and BBPSSW.Distill.pauli, imported as references. Half-integers are avoided: with r : Fin (n/2+1), the irrep factor is Fin (n - 2r + 1), and the basis index stands for . The multiplicity formula is stated in (degeneracy n r), so no truncating division hides a failure of divisibility. The unitary is a rectangular matrix between the two index sets with and . The algebra is Algebra.adjoin ℂ (Set.range (collS n)), which contains . All statements also hold, and are stated, for .
The goal cannot be satisfied by a degenerate witness. The multiplicities are pinned by the formula, must be unitary, and clause (8.41) is an "if and only if", so an empty block or a zero map cannot meet it. Proved sanity checks confirm for , , for , the row of Table 8.2, and for . They also check that for an explicit unitary meets (8.43).
Useful infrastructure: computational-basis lemmas for onQubit, the spin- representation and its irreducibility, a Casimir argument, and a Burnside or double-commutant theorem for matrix algebras. These parts are reusable by Missions VIII and IX of this series and by any permutation-symmetric quantum information result. Contributions toward the milestones, toward the explicit highest-weight construction, and toward the binomial identity behind (8.42) are welcome.
Selected references
- D. M. Bacon, Decoherence, Control, and Symmetry in Quantum Computers, PhD thesis, UC Berkeley, 2001; arXiv:quant-ph/0305025v1, 2003. arXiv:quant-ph/0305025
- J. Kempe, D. Bacon, D. A. Lidar, K. B. Whaley, Theory of decoherence-free fault-tolerant universal quantum computation, Phys. Rev. A 63, 042307, 2001. arXiv:quant-ph/0004064
- E. Knill, R. Laflamme, L. Viola, Theory of quantum error correction for general noise, Phys. Rev. Lett. 84, 2525, 2000. arXiv:quant-ph/9908066
- D. A. Lidar, I. L. Chuang, K. B. Whaley, Decoherence-free subspaces for quantum computation, Phys. Rev. Lett. 81, 2594, 1998. arXiv:quant-ph/9807004
- P. Zanardi, M. Rasetti, Noiseless quantum codes, Phys. Rev. Lett. 79, 3306, 1997. arXiv:quant-ph/9705044
- L.-M. Duan, G.-C. Guo, Preserving coherence in quantum computation by pairing quantum bits, Phys. Rev. Lett. 79, 1953, 1997. doi:10.1103/PhysRevLett.79.1953
- L. Mandel, E. Wolf, Optical Coherence and Quantum Optics, Cambridge University Press, 1995 (the thesis's reference [142] for (8.42)).