Please use this identifier to cite or link to this item:
https://ah.lib.nccu.edu.tw/handle/140.119/65815
DC Field | Value | Language |
---|---|---|
dc.contributor | 應物所 | en_US |
dc.creator | 林瑜琤 | zh_TW |
dc.creator | Lin, Yu-Cheng ; Heiko Rieger; Ferenc Igloi | en_US |
dc.date | 2004.06 | en_US |
dc.date.accessioned | 2014-05-01T09:54:58Z | - |
dc.date.available | 2014-05-01T09:54:58Z | - |
dc.date.issued | 2014-05-01T09:54:58Z | - |
dc.identifier.uri | http://nccur.lib.nccu.edu.tw/handle/140.119/65815 | - |
dc.description.abstract | We consider S = 1/2 antiferromagnetic Heisenberg chains with alternating bonds andquenched disorder, which represents a theoretical model of the compound CuCl2xBr2(1−x)(γ −pic)2. Using a numerical implementation of the strong disorder renormalization group methodwe study the low-energy properties of the system as a function of the concentration, x, andthe type of correlations in the disorder. For perfect correlation of disorder the system is in therandom dimer (Griffiths) phase having a concentration dependent dynamical exponent. Forweak or vanishing disorder correlations the system is in the random singlet phase, in whichthe dynamical exponent is formally infinity. We discuss consequences of our results for theexperimentally measured low-temperature susceptibility of CuCl2xBr2(1−x)(γ − pic)2. | en_US |
dc.format.extent | 307126 bytes | - |
dc.format.mimetype | application/pdf | - |
dc.language.iso | en_US | - |
dc.relation | J. Phys. Soc. Jap., 73(6), 1602-1606 | en_US |
dc.title | Antiferromagnetic Heisenberg chains with bond alternation and quenched disorder | en_US |
dc.type | article | en |
item.openairetype | article | - |
item.cerifentitytype | Publications | - |
item.openairecristype | http://purl.org/coar/resource_type/c_18cf | - |
item.fulltext | With Fulltext | - |
item.grantfulltext | restricted | - |
item.languageiso639-1 | en_US | - |
Appears in Collections: | 期刊論文 |
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402429.pdf | 299.93 kB | Adobe PDF2 | View/Open |
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