{ "id": "quant-ph/9911061", "version": "v1", "published": "1999-11-15T02:57:05.000Z", "updated": "1999-11-15T02:57:05.000Z", "title": "Time dynamics in chaotic many-body systems: can chaos destroy a quantum computer?", "authors": [ "V. V. Flambaum" ], "comment": "9 pages, RevTex", "categories": [ "quant-ph", "chao-dyn", "cond-mat.mes-hall", "cond-mat.stat-mech", "nlin.CD", "nucl-th", "physics.atom-ph" ], "abstract": "Highly excited many-particle states in quantum systems (nuclei, atoms, quantum dots, spin systems, quantum computers) can be ``chaotic'' superpositions of mean-field basis states (Slater determinants, products of spin or qubit states). This is a result of the very high energy level density of many-body states which can be easily mixed by a residual interaction between particles. We consider the time dynamics of wave functions and increase of entropy in such chaotic systems. As an example we present the time evolution in a closed quantum computer. A time scale for the entropy S(t) increase is t_c =t_0/(n log_2{n}), where t_0 is the qubit ``lifetime'', n is the number of qubits, S(0)=0 and S(t_c)=1. At t << t_c the entropy is small: S= n t^2 J^2 log_2(1/t^2 J^2), where J is the inter-qubit interaction strength. At t > t_c the number of ``wrong'' states increases exponentially as 2^{S(t)} . Therefore, t_c may be interpreted as a maximal time for operation of a quantum computer, since at t > t_c one has to struggle against the second law of thermodynamics. At t >>t_c the system entropy approaches that for chaotic eigenstates.", "revisions": [ { "version": "v1", "updated": "1999-11-15T02:57:05.000Z" } ], "analyses": { "keywords": [ "quantum computer", "chaotic many-body systems", "time dynamics", "chaos destroy", "high energy level density" ], "note": { "typesetting": "RevTeX", "pages": 9, "language": "en", "license": "arXiv", "status": "editable", "inspire": 510249, "adsabs": "1999quant.ph.11061F" } } }