logging in or signing up TAM 13 15JuneBologna Tomasina Download Post to : URL : Related Presentations : Share Add to Flag Embed Email Send to Blogs and Networks Add to Channel Uploaded from authorPOINTLite Insert YouTube videos in PowerPont slides with aS Desktop Copy embed code: (To copy code, click on the text box) Embed: URL: Thumbnail: WordPress Embed Customize Embed The presentation is successfully added In Your Favorites. Views: 40 Category: Education License: All Rights Reserved Like it (0) Dislike it (0) Added: January 09, 2008 This Presentation is Public Favorites: 0 Presentation Description No description available. Comments Posting comment... Premium member Presentation Transcript Slide1: TAM 13-15 June 2007, HPC-EUROPA Bologna Sergio Perez-Gaviro Heisenberg Spin Glass in three dimensions. Isotropy & Anisotropy Weakly Anisotropic Heisenberg Spin Glasses under Magnetic Fields. ( Universidad de Zaragoza & Bifi )Slide2: ? It is a collection of spins whose low-temperature state is a frozen disordered state, rather than the kind of periodic or uniform pattern one can find in conventional magnets. TAM 13-15 June 2007, HPC-EUROPA BolognaSlide3: TAM 13-15 June 2007, HPC-EUROPA BolognaSlide4: “Critical Behavior of the three dimensional Ising Spin Gass”, H.G. Ballesteros et el., Phys. Rev. B, 62, 14237 (2000). TAM 13-15 June 2007, HPC-EUROPA BolognaSlide5: I Isotropic Heisenberg spin glass TAM 13-15 June 2007, HPC-EUROPA BolognaSlide6: Introduction the more experimentally interesting case TAM 13-15 June 2007, HPC-EUROPA BolognaSlide7: PBC Bifi cluster (BIFI, Zaragoza) Marenostrum (BSC, Barcelona) Cubic lattice of size L TAM 13-15 June 2007, HPC-EUROPA BolognaSlide8: The Elementary Monte Carlo Step (EMCS) to extrapolate to nearby temperatures we use bias-corrected data reweighting TAM 13-15 June 2007, HPC-EUROPA BolognaSlide9: TAM 13-15 June 2007, HPC-EUROPA BolognaSlide10: Generalizing the standard reweighting method (Alan M. Ferrenberg and Robert H. Swendsen, Phys. Rev. Lett. 61, 2635 (1988)) it is possible to extrapolate measures taken at a temperature T to neighbouring values. where TAM 13-15 June 2007, HPC-EUROPA BolognaSlide11: From the quotients FSS method: TAM 13-15 June 2007, HPC-EUROPA BolognaSlide12: TAM 13-15 June 2007, HPC-EUROPA BolognaSlide13: TAM 13-15 June 2007, HPC-EUROPA BolognaSlide14: Heisenberg spin glass in 3D undergoes a finite temperature transition. A mixture of Heath-Bath and Overrelaxation dynamics allows us to thermalize lattices of size up to L=32. At criticality, spin glass susceptibility scales with the chiral correlation length. Spin-chirality decoupling is ruled out. Logarithmic corrections to scaling are observed. Our results are compatible with a Kosterlitz-Thouless scaling, but they are typical as well of a system with a lower critical dimension barely smaller than three. I. Campos, M. Cotallo-Aban, V. Martin-Mayor, S. Perez-Gaviro, A. Tarancon, “The Spin Glass transition of the three dimensional Heisenberg Spin Glass”, Phy. Rev. Lett. 97, 217204 (2006). TAM 13-15 June 2007, HPC-EUROPA BolognaSlide15: II Anisotropic Heisenberg spin glass TAM 13-15 June 2007, HPC-EUROPA BolognaSlide16: The anisotropic model Decoupling chiral glass and sping glass TAM 13-15 June 2007, HPC-EUROPA Bologna Lomond cluster (EPCC, Edinburgh) Bifi cluster (BIFI, Zaragoza) Marenostrum (BSC, Barcelona)Slide17: The anisotropic model under a magnetic field PBC Cubic lattice of size L TAM 13-15 June 2007, HPC-EUROPA BolognaSlide18: Acknowledgments Adam Carter (Applications Consultant, my contact in EPCC) Davide Marenduzzo (School of Physics, my host in HPC-Programme) Catherine Inglis (HPC-Europa visit co-ordinator, EPCC) Alfonso Tarancón Lafita (thesis director, Universidad de Zargoza) Víctor Martín-Mayor (thesis co-director, Universidad Complutense de Madrid) María Cotallo-Abán (Ph.D. Student, Universidad de Zaragoza) TAM 13-15 June 2007, HPC-EUROPA BolognaSlide19: Bibliography TAM 13-15 June 2007, HPC-EUROPA BolognaSlide20: questions … TAM 13-15 June 2007, HPC-EUROPA BolognaSlide21: TAM 13-15 June 2007, HPC-EUROPA BolognaSlide22: Simulation Model was simulated with a mixture of Heat Bath and Overrelaxation taken from lattice QCD but also effective for frustated spin models • trial element is placed far away from the old value → rather rapid flow through phase space • due to simplicity it is very fast (one HB update is roughly as CPU consuming as 7 overrelaxations) • it may be combined with Parallel Tempering but this is unnecessary at TC • effective for frustated spin models Intuitive arguments in favor of overrelaxation: TAM 13-15 June 2007, HPC-EUROPA BolognaSlide23: Finite Size Scaling (FSS) analysis Advantages of using the quotient method: it is easy to use. arbitary choises on the temperature range are avoided the statistical error estimation is clear it is possible to observe scaling corrections directly by increasing L1 and L2. TAM 13-15 June 2007, HPC-EUROPA BolognaSlide24: TAM 13-15 June 2007, HPC-EUROPA Bologna (S.Miyashita, E.Vincent, Eur. Phys. J, B22, 203 (2001)) You do not have the permission to view this presentation. In order to view it, please contact the author of the presentation.
TAM 13 15JuneBologna Tomasina Download Post to : URL : Related Presentations : Share Add to Flag Embed Email Send to Blogs and Networks Add to Channel Uploaded from authorPOINTLite Insert YouTube videos in PowerPont slides with aS Desktop Copy embed code: (To copy code, click on the text box) Embed: URL: Thumbnail: WordPress Embed Customize Embed The presentation is successfully added In Your Favorites. Views: 40 Category: Education License: All Rights Reserved Like it (0) Dislike it (0) Added: January 09, 2008 This Presentation is Public Favorites: 0 Presentation Description No description available. Comments Posting comment... Premium member Presentation Transcript Slide1: TAM 13-15 June 2007, HPC-EUROPA Bologna Sergio Perez-Gaviro Heisenberg Spin Glass in three dimensions. Isotropy & Anisotropy Weakly Anisotropic Heisenberg Spin Glasses under Magnetic Fields. ( Universidad de Zaragoza & Bifi )Slide2: ? It is a collection of spins whose low-temperature state is a frozen disordered state, rather than the kind of periodic or uniform pattern one can find in conventional magnets. TAM 13-15 June 2007, HPC-EUROPA BolognaSlide3: TAM 13-15 June 2007, HPC-EUROPA BolognaSlide4: “Critical Behavior of the three dimensional Ising Spin Gass”, H.G. Ballesteros et el., Phys. Rev. B, 62, 14237 (2000). TAM 13-15 June 2007, HPC-EUROPA BolognaSlide5: I Isotropic Heisenberg spin glass TAM 13-15 June 2007, HPC-EUROPA BolognaSlide6: Introduction the more experimentally interesting case TAM 13-15 June 2007, HPC-EUROPA BolognaSlide7: PBC Bifi cluster (BIFI, Zaragoza) Marenostrum (BSC, Barcelona) Cubic lattice of size L TAM 13-15 June 2007, HPC-EUROPA BolognaSlide8: The Elementary Monte Carlo Step (EMCS) to extrapolate to nearby temperatures we use bias-corrected data reweighting TAM 13-15 June 2007, HPC-EUROPA BolognaSlide9: TAM 13-15 June 2007, HPC-EUROPA BolognaSlide10: Generalizing the standard reweighting method (Alan M. Ferrenberg and Robert H. Swendsen, Phys. Rev. Lett. 61, 2635 (1988)) it is possible to extrapolate measures taken at a temperature T to neighbouring values. where TAM 13-15 June 2007, HPC-EUROPA BolognaSlide11: From the quotients FSS method: TAM 13-15 June 2007, HPC-EUROPA BolognaSlide12: TAM 13-15 June 2007, HPC-EUROPA BolognaSlide13: TAM 13-15 June 2007, HPC-EUROPA BolognaSlide14: Heisenberg spin glass in 3D undergoes a finite temperature transition. A mixture of Heath-Bath and Overrelaxation dynamics allows us to thermalize lattices of size up to L=32. At criticality, spin glass susceptibility scales with the chiral correlation length. Spin-chirality decoupling is ruled out. Logarithmic corrections to scaling are observed. Our results are compatible with a Kosterlitz-Thouless scaling, but they are typical as well of a system with a lower critical dimension barely smaller than three. I. Campos, M. Cotallo-Aban, V. Martin-Mayor, S. Perez-Gaviro, A. Tarancon, “The Spin Glass transition of the three dimensional Heisenberg Spin Glass”, Phy. Rev. Lett. 97, 217204 (2006). TAM 13-15 June 2007, HPC-EUROPA BolognaSlide15: II Anisotropic Heisenberg spin glass TAM 13-15 June 2007, HPC-EUROPA BolognaSlide16: The anisotropic model Decoupling chiral glass and sping glass TAM 13-15 June 2007, HPC-EUROPA Bologna Lomond cluster (EPCC, Edinburgh) Bifi cluster (BIFI, Zaragoza) Marenostrum (BSC, Barcelona)Slide17: The anisotropic model under a magnetic field PBC Cubic lattice of size L TAM 13-15 June 2007, HPC-EUROPA BolognaSlide18: Acknowledgments Adam Carter (Applications Consultant, my contact in EPCC) Davide Marenduzzo (School of Physics, my host in HPC-Programme) Catherine Inglis (HPC-Europa visit co-ordinator, EPCC) Alfonso Tarancón Lafita (thesis director, Universidad de Zargoza) Víctor Martín-Mayor (thesis co-director, Universidad Complutense de Madrid) María Cotallo-Abán (Ph.D. Student, Universidad de Zaragoza) TAM 13-15 June 2007, HPC-EUROPA BolognaSlide19: Bibliography TAM 13-15 June 2007, HPC-EUROPA BolognaSlide20: questions … TAM 13-15 June 2007, HPC-EUROPA BolognaSlide21: TAM 13-15 June 2007, HPC-EUROPA BolognaSlide22: Simulation Model was simulated with a mixture of Heat Bath and Overrelaxation taken from lattice QCD but also effective for frustated spin models • trial element is placed far away from the old value → rather rapid flow through phase space • due to simplicity it is very fast (one HB update is roughly as CPU consuming as 7 overrelaxations) • it may be combined with Parallel Tempering but this is unnecessary at TC • effective for frustated spin models Intuitive arguments in favor of overrelaxation: TAM 13-15 June 2007, HPC-EUROPA BolognaSlide23: Finite Size Scaling (FSS) analysis Advantages of using the quotient method: it is easy to use. arbitary choises on the temperature range are avoided the statistical error estimation is clear it is possible to observe scaling corrections directly by increasing L1 and L2. TAM 13-15 June 2007, HPC-EUROPA BolognaSlide24: TAM 13-15 June 2007, HPC-EUROPA Bologna (S.Miyashita, E.Vincent, Eur. Phys. J, B22, 203 (2001))