/A << /Length 2537 /Annots [ << /I1 50 0 R /Contents 215 0 R /Border [ 0 0 0 ] << /Subtype /Link /A << /I1 50 0 R /A << /XObject << /Subtype /Link /Subtype /Link /Subtype /Link /Rect [ 17.01000 748.69000 81.07000 740.69000 ] >> << 17.01000 776.31000 Td /Subtype /Link /Resources << /Rect [ 17.01000 21.01000 191.50000 13.01000 ] ET /Parent 1 0 R /URI (www\056cambridge\056org\0579781107113190) /URI (www\056cambridge\056org\0579781107113190) /Subtype /Link >> /Count 30 /Rect [ 17.01000 21.01000 191.50000 13.01000 ] /Type /Page /Rect [ 17.01000 21.01000 191.50000 13.01000 ] 22 0 obj /I1 50 0 R /Contents 59 0 R /A << /Contents 89 0 R >> /A << << 20 0 obj /Type /Annot /URI (www\056cambridge\056org) /Contents 152 0 R /S /URI /Border [ 0 0 0 ] q /URI (www\056cambridge\056org\0579781107113190) /Contents 190 0 R /Border [ 0 0 0 ] >> ] /Parent 1 0 R q >> /Contents 240 0 R /URI (www\056cambridge\056org\0579781107113190) /Annots [ << /I1 50 0 R /A << /URI (www\056cambridge\056org) /Subtype /Link /Annots [ << /Rect [ 17.01000 21.01000 191.50000 13.01000 ] /Resources << >> >> /S /URI /Border [ 0 0 0 ] /S /URI /F1 52 0 R Q /Contents 162 0 R /S /URI /XObject << /Contents 120 0 R /pdfrw_0 121 0 R >> ] << >> /A << >> >> The quantum critical regime associated with the quantum transition at S = 0 and the various regimes in the spin-glass phase at high spin are analyzed. /Font << /A << /S /URI /I1 50 0 R /MediaBox [ 0 0 539 839.65000 ] /S /URI /Type /Annot >> << /pdfrw_0 221 0 R /Type /Annot /A << Quantum annealing was first proposed in 1988 by B. 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An essential ingredient in understanding quantum spin glasses is the determination of the properties of the quantum critical point at Γ = Γ. c. and T = 0, beyond which spin glass order disappears. /A << /Contents 107 0 R >> /pdfrw_0 60 0 R /Font << Spin glass behavior in frustrated quantum spin system CuAl 2 O 4 with a possible orbital liquid state. /XObject << >> << 0.06500 0.37100 0.64200 rg /S /URI S /URI (www\056cambridge\056org) /pdfrw_0 226 0 R /S /URI stream /Subtype /Link /ProcSet [ /Text /PDF /ImageI /ImageC /ImageB ] /Contents 172 0 R /F1 52 0 R /Contents 225 0 R >> /Contents 180 0 R /XObject << /Rect [ 17.01000 21.01000 191.50000 13.01000 ] /I1 50 0 R >> >> /Parent 1 0 R /S /URI /F1 52 0 R >> /I1 50 0 R /Contents 99 0 R /Type /Annot /Type /Page /F1 52 0 R In ferromagnetic solids, component atoms' magnetic spins all align in the same direction. /Border [ 0 0 0 ] endobj /Type /Annot >> ] /A << >> 35 0 obj /MediaBox [ 0 0 539 839.65000 ] << >> The results compare well to theory for this spin-glass problem, validating the approach for simulating problems in materials physics. /F1 52 0 R /XObject << >> ] /Type /Page /Resources << /URI (www\056cambridge\056org) /Border [ 0 0 0 ] >> /Rect [ 17.01000 21.01000 191.50000 13.01000 ] /Rect [ 17.01000 748.69000 81.07000 740.69000 ] >> << /A << >> /pdfrw_0 126 0 R q /Type /Annot /S /URI /Subtype /Form /Font << /Type /Page >> << >> /Subtype /Link 19 0 obj /Border [ 0 0 0 ] /MediaBox [ 0 0 539 839.65000 ] >> << >> >> ] /Resources << /S /URI >> << /ProcSet [ /PDF /Text ] /pdfrw_0 241 0 R /Type /Annot >> /S /URI >> >> /Font << /Type /Page /Annots [ << /I1 50 0 R /Parent 1 0 R >> >> >> ] 0 g /Annots [ << << /Rect [ 17.01000 21.01000 191.50000 13.01000 ] 0 31.18000 m /Type /Annot /Font << << >> /Type /Annot /S /URI /F1 52 0 R /S /URI stream /Resources << /Type /Page /Font << 0.06500 0.37100 0.64200 rg endobj /Rect [ 17.01000 21.01000 191.50000 13.01000 ] /Annots [ << >> /Parent 1 0 R ET endobj /Type /Annot 1 0 0 1 0 32.50000 cm /ProcSet [ /Text /PDF /ImageI /ImageC /ImageB ] /A << /Border [ 0 0 0 ] /I1 50 0 R /pdfrw_0 163 0 R /Type /Annot /A << /A << /ProcSet [ /Text /PDF /ImageI /ImageC /ImageB ] /Rect [ 17.01000 748.69000 81.07000 740.69000 ] The transverse eld term H^ T H^ T = nX 1 j=0 X^ j; (3) drives transitions between states, where is a real-valued transverse eld strength, /Rect [ 17.01000 748.69000 81.07000 740.69000 ] /F1 52 0 R >> >> /Font << /Type /Annot >> /Subtype /Link /Border [ 0 0 0 ] endobj /S /URI /Type /Annot /A << /Parent 1 0 R >> /Font << >> ] 10 0 obj /Type /Annot /Border [ 0 0 0 ] /Resources << <004d006f0072006500200049006e0066006f0072006d006100740069006f006e> Tj 30 0 obj >> >> >> /XObject << /Parent 1 0 R >> >> << 439.79000 14.17000 Td /ProcSet [ /Text /PDF /ImageI /ImageC /ImageB ] /Border [ 0 0 0 ] /Resources << << <00430061006d00620072006900640067006500200055006e00690076006500720073006900740079002000500072006500730073> Tj /Matrix [ -1 0 0 -1 539.00700 701.00700 ] /XObject << << /Border [ 0 0 0 ] << >> 439.79000 13.47000 71.02000 -0.39000 re /A << << S >> /A << /Border [ 0 0 0 ]