FRINK Linked Data Fragments server

Matches in SemOpenAlex for { <https://semopenalex.org/work/W2084543277> ?p ?o ?g. }

• W2084543277 abstract "Single-chain magnets (SCMs) are one-dimensional systems in which the relaxation of the magnetization becomes very slow at low temperature. This singular behavior is due to the vicinity of the critical point located at vanishing temperature $(T=0)$ and applied magnetic field $(H=0)$. In order to optimize the properties of these nano-objects, detailed studies of the observed critical behavior are necessary. However, previous works on the SCM relaxation have essentially analyzed experimental data in the absence of applied magnetic field. We discuss in this paper the effect of applying a magnetic field on two different examples of single-chain magnets. These samples have been previously described in the absence of magnetic field and considered as model systems since their chains are composed of a regular one-dimensional (1D) arrangement of anisotropic trimer units. These magnetic trinuclear motifs can be described at low temperature as effective spins coupled ferromagnetically. Theoretical results relevant to analyze our data in the presence of an applied magnetic field are first described. We also present a simple numerical approach to discuss finite-size effects relevant in SCM systems. Experimental data, including ac and dc data on powder samples and single crystals, are then presented. These results are analyzed and compared with the theoretical predictions deduced for the 1D Ising model. At low field, for $hensuremath{xi}⪡1$ (where $ensuremath{xi}$ is the correlation length normalized to the unit cell parameter and $h=ensuremath{mu}H∕{k}_{B}T$ is the dimensionless applied field) or for $hL⪡1$ when finite-size effects are relevant ($L$ being the chain length normalized to the unit cell parameter), we show that experimental data reproduce the critical behavior expected from the theory. Moreover, the obtained values of $ensuremath{xi}$ or $L$ are in excellent agreement with the estimation deduced from susceptibility data. At higher fields, for $hensuremath{xi}⪢1$ or $hL⪢1$, we show that the field dependence of the relaxation time is drastically different for the two samples. This difference is understood taking into account the field dependence of the relaxation time of the effective spins located inside a domain wall." @default.
• W2084543277 created "2016-06-24" @default.
• W2084543277 creator A5005324956 @default.
• W2084543277 creator A5005753997 @default.
• W2084543277 creator A5031459453 @default.
• W2084543277 creator A5061198429 @default.
• W2084543277 creator A5063218383 @default.
• W2084543277 creator A5064503658 @default.
• W2084543277 creator A5066048666 @default.
• W2084543277 date "2007-12-21" @default.
• W2084543277 modified "2023-10-01" @default.
• W2084543277 title "Effect of an applied magnetic field on the relaxation time of single-chain magnets" @default.
• W2084543277 cites W1969914902 @default.
• W2084543277 cites W1971428963 @default.
• W2084543277 cites W1973607273 @default.
• W2084543277 cites W1983272724 @default.
• W2084543277 cites W1985429317 @default.
• W2084543277 cites W1993534498 @default.
• W2084543277 cites W1994438370 @default.
• W2084543277 cites W1997557995 @default.
• W2084543277 cites W2000593257 @default.
• W2084543277 cites W2000693769 @default.
• W2084543277 cites W2001239791 @default.
• W2084543277 cites W2003537107 @default.
• W2084543277 cites W2006038032 @default.
• W2084543277 cites W2019657206 @default.
• W2084543277 cites W2021859686 @default.
• W2084543277 cites W2029546786 @default.
• W2084543277 cites W2032054005 @default.
• W2084543277 cites W2046323932 @default.
• W2084543277 cites W2047174430 @default.
• W2084543277 cites W2054196780 @default.
• W2084543277 cites W2055022162 @default.
• W2084543277 cites W2057796886 @default.
• W2084543277 cites W2059961956 @default.
• W2084543277 cites W2062629061 @default.
• W2084543277 cites W2065580363 @default.
• W2084543277 cites W2073055389 @default.
• W2084543277 cites W2079242124 @default.
• W2084543277 cites W2083060483 @default.
• W2084543277 cites W2083144932 @default.
• W2084543277 cites W2085311292 @default.
• W2084543277 cites W2127022021 @default.
• W2084543277 cites W2135374860 @default.
• W2084543277 cites W2147758352 @default.
• W2084543277 cites W2151675857 @default.
• W2084543277 cites W2734005401 @default.
• W2084543277 doi "https://doi.org/10.1103/physrevb.76.214422" @default.
• W2084543277 hasPublicationYear "2007" @default.
• W2084543277 type Work @default.
• W2084543277 sameAs 2084543277 @default.
• W2084543277 citedByCount "27" @default.
• W2084543277 countsByYear W20845432772012 @default.
• W2084543277 countsByYear W20845432772013 @default.
• W2084543277 countsByYear W20845432772014 @default.
• W2084543277 countsByYear W20845432772015 @default.
• W2084543277 countsByYear W20845432772017 @default.
• W2084543277 countsByYear W20845432772019 @default.
• W2084543277 countsByYear W20845432772020 @default.
• W2084543277 countsByYear W20845432772021 @default.
• W2084543277 crossrefType "journal-article" @default.
• W2084543277 hasAuthorship W2084543277A5005324956 @default.
• W2084543277 hasAuthorship W2084543277A5005753997 @default.
• W2084543277 hasAuthorship W2084543277A5031459453 @default.
• W2084543277 hasAuthorship W2084543277A5061198429 @default.
• W2084543277 hasAuthorship W2084543277A5063218383 @default.
• W2084543277 hasAuthorship W2084543277A5064503658 @default.
• W2084543277 hasAuthorship W2084543277A5066048666 @default.
• W2084543277 hasConcept C115260700 @default.
• W2084543277 hasConcept C121332964 @default.
• W2084543277 hasConcept C15744967 @default.
• W2084543277 hasConcept C16389437 @default.
• W2084543277 hasConcept C192562407 @default.
• W2084543277 hasConcept C199185054 @default.
• W2084543277 hasConcept C202444582 @default.
• W2084543277 hasConcept C24872484 @default.
• W2084543277 hasConcept C26873012 @default.
• W2084543277 hasConcept C2776029896 @default.
• W2084543277 hasConcept C2778870898 @default.
• W2084543277 hasConcept C32546565 @default.
• W2084543277 hasConcept C32938098 @default.
• W2084543277 hasConcept C33923547 @default.
• W2084543277 hasConcept C51329190 @default.
• W2084543277 hasConcept C62520636 @default.
• W2084543277 hasConcept C77805123 @default.
• W2084543277 hasConcept C85725439 @default.
• W2084543277 hasConcept C9652623 @default.
• W2084543277 hasConcept C97355855 @default.
• W2084543277 hasConceptScore W2084543277C115260700 @default.
• W2084543277 hasConceptScore W2084543277C121332964 @default.
• W2084543277 hasConceptScore W2084543277C15744967 @default.
• W2084543277 hasConceptScore W2084543277C16389437 @default.
• W2084543277 hasConceptScore W2084543277C192562407 @default.
• W2084543277 hasConceptScore W2084543277C199185054 @default.
• W2084543277 hasConceptScore W2084543277C202444582 @default.
• W2084543277 hasConceptScore W2084543277C24872484 @default.
• W2084543277 hasConceptScore W2084543277C26873012 @default.
• W2084543277 hasConceptScore W2084543277C2776029896 @default.
• W2084543277 hasConceptScore W2084543277C2778870898 @default.
• W2084543277 hasConceptScore W2084543277C32546565 @default.

• next