Adiabatic quantum computation along quasienergies Export

@article{citeulike:5973096, abstract = {The parametric deformations of quasienergies and eigenvectors of unitary operators are applied to the design of quantum adiabatic algorithms. The conventional, standard adiabatic quantum computation proceeds along eigenenergies of parameter-dependent Hamiltonians. By contrast, discrete adiabatic computation utilizes adiabatic passage along the quasienergies of parameter-dependent unitary operators. For example, such computation can be realized by a concatenation of parameterized quantum circuits, with an adiabatic though inevitably discrete change of the parameter. A design principle of adiabatic passage along quasienergy is recently proposed: Cheon's quasienergy and eigenspace anholonomies on unitary operators is available to realize anholonomic adiabatic algorithms [Tanaka and Miyamoto, Phys. Rev. Lett. 98, 160407 (2007)], which compose a nontrivial family of discrete adiabatic algorithms. It is straightforward to port a standard adiabatic algorithm to an anholonomic adiabatic one, except an introduction of a parameter |v\>, which is available to adjust the gaps of the quasienergies to control the running time steps. In Grover's database search problem, the costs to prepare |v\> for the qualitatively different, i.e., power or exponential, running time steps are shown to be qualitatively different. Curiously, in establishing the equivalence between the standard quantum computation based on the circuit model and the anholonomic adiabatic quantum computation model, it is shown that the cost for |v\> to enlarge the gaps of the eigenvalue is qualitatively negligible.}, archivePrefix = {arXiv}, author = {Tanaka, Atushi and Nemoto, Kae}, citeulike-article-id = {5973096}, citeulike-linkout-0 = {http://arxiv.org/abs/0910.3452}, citeulike-linkout-1 = {http://arxiv.org/pdf/0910.3452}, day = {19}, eprint = {0910.3452}, keywords = {adiabatic, exotic-holonomy, quantum-adiabatic-computation, quasienergy}, month = {Oct}, posted-at = {2009-10-20 07:06:22}, priority = {0}, title = {Adiabatic quantum computation along quasienergies}, url = {http://arxiv.org/abs/0910.3452}, year = {2009} }

TY - JOUR ID - citeulike:5973096 L3 - citeulike-article-id:5973096 N2 - The parametric deformations of quasienergies and eigenvectors of unitary operators are applied to the design of quantum adiabatic algorithms. The conventional, standard adiabatic quantum computation proceeds along eigenenergies of parameter-dependent Hamiltonians. By contrast, discrete adiabatic computation utilizes adiabatic passage along the quasienergies of parameter-dependent unitary operators. For example, such computation can be realized by a concatenation of parameterized quantum circuits, with an adiabatic though inevitably discrete change of the parameter. A design principle of adiabatic passage along quasienergy is recently proposed: Cheon's quasienergy and eigenspace anholonomies on unitary operators is available to realize anholonomic adiabatic algorithms [Tanaka and Miyamoto, Phys. Rev. Lett. 98, 160407 (2007)], which compose a nontrivial family of discrete adiabatic algorithms. It is straightforward to port a standard adiabatic algorithm to an anholonomic adiabatic one, except an introduction of a parameter |v>, which is available to adjust the gaps of the quasienergies to control the running time steps. In Grover's database search problem, the costs to prepare |v> for the qualitatively different, i.e., power or exponential, running time steps are shown to be qualitatively different. Curiously, in establishing the equivalence between the standard quantum computation based on the circuit model and the anholonomic adiabatic quantum computation model, it is shown that the cost for |v> to enlarge the gaps of the eigenvalue is qualitatively negligible. TI - Adiabatic quantum computation along quasienergies KW - adiabatic KW - exotic-holonomy KW - quantum-adiabatic-computation KW - quasienergy AU - Tanaka, Atushi AU - Nemoto, Kae PY - 2009/Oct/19/ UR - http://arxiv.org/abs/0910.3452 ER -