Numerical simulation of angle dependent magnetoresistances oscillations in alpha-(BEDT-TTF)(2)KHg(SCN)(4)

We present a numerical simulation of angle dependent magnetoresistances oscillations(AMROs) in alpha-(BEDT-TTF)(2)KHg(SCN)(4). The nesting vector of the density wave and the magnetic breakdowngap in the low-temperature, low-magnetic-field state (LTLF) are constrained by simulations of quasi-one-dime...

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Κύριοι συγγραφείς: Nam, MS, Ardavan, A, Blundell, S, Singleton, J
Μορφή: Conference item
Έκδοση: 2001
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author Nam, MS
Ardavan, A
Blundell, S
Singleton, J
author_facet Nam, MS
Ardavan, A
Blundell, S
Singleton, J
author_sort Nam, MS
collection OXFORD
description We present a numerical simulation of angle dependent magnetoresistances oscillations(AMROs) in alpha-(BEDT-TTF)(2)KHg(SCN)(4). The nesting vector of the density wave and the magnetic breakdowngap in the low-temperature, low-magnetic-field state (LTLF) are constrained by simulations of quasi-one-dimensional (Q1D) AMRO. Quasi-two-dimensional (Q2D) AMRO simulations for the high-temperature, high-magnetic-field state (HTHF) allow the precise derivation of an ellipticity of the Q2D Fermi surface. Simulations of the field dependent AMRO demonstrate the gradual evolution of the FS from LTLF to HTHF states toward the kink transition at 23 T.
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spelling oxford-uuid:a691eb31-8dce-4d16-975c-2aa7462a6bf22022-03-27T02:48:13ZNumerical simulation of angle dependent magnetoresistances oscillations in alpha-(BEDT-TTF)(2)KHg(SCN)(4)Conference itemhttp://purl.org/coar/resource_type/c_5794uuid:a691eb31-8dce-4d16-975c-2aa7462a6bf2Symplectic Elements at Oxford2001Nam, MSArdavan, ABlundell, SSingleton, JWe present a numerical simulation of angle dependent magnetoresistances oscillations(AMROs) in alpha-(BEDT-TTF)(2)KHg(SCN)(4). The nesting vector of the density wave and the magnetic breakdowngap in the low-temperature, low-magnetic-field state (LTLF) are constrained by simulations of quasi-one-dimensional (Q1D) AMRO. Quasi-two-dimensional (Q2D) AMRO simulations for the high-temperature, high-magnetic-field state (HTHF) allow the precise derivation of an ellipticity of the Q2D Fermi surface. Simulations of the field dependent AMRO demonstrate the gradual evolution of the FS from LTLF to HTHF states toward the kink transition at 23 T.
spellingShingle Nam, MS
Ardavan, A
Blundell, S
Singleton, J
Numerical simulation of angle dependent magnetoresistances oscillations in alpha-(BEDT-TTF)(2)KHg(SCN)(4)
title Numerical simulation of angle dependent magnetoresistances oscillations in alpha-(BEDT-TTF)(2)KHg(SCN)(4)
title_full Numerical simulation of angle dependent magnetoresistances oscillations in alpha-(BEDT-TTF)(2)KHg(SCN)(4)
title_fullStr Numerical simulation of angle dependent magnetoresistances oscillations in alpha-(BEDT-TTF)(2)KHg(SCN)(4)
title_full_unstemmed Numerical simulation of angle dependent magnetoresistances oscillations in alpha-(BEDT-TTF)(2)KHg(SCN)(4)
title_short Numerical simulation of angle dependent magnetoresistances oscillations in alpha-(BEDT-TTF)(2)KHg(SCN)(4)
title_sort numerical simulation of angle dependent magnetoresistances oscillations in alpha bedt ttf 2 khg scn 4
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AT ardavana numericalsimulationofangledependentmagnetoresistancesoscillationsinalphabedtttf2khgscn4
AT blundells numericalsimulationofangledependentmagnetoresistancesoscillationsinalphabedtttf2khgscn4
AT singletonj numericalsimulationofangledependentmagnetoresistancesoscillationsinalphabedtttf2khgscn4