Library

feed icon rss

Your email was sent successfully. Check your inbox.

An error occurred while sending the email. Please try again.

Proceed reservation?

Export
  • 1
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 69 (1991), S. 6024-6024 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: Rb2CrCl2I2 crystallizes with a Jahn–Teller deformed K2NiF4 structure. This results in a ferromagnetic behavior for this compound. Rb2CrCl2I2 orders ferromagnetically at Tc=56.9(2) K. Magnetization and magnetic susceptibility measurements, using a vibrating sample magnetometer, Faraday balance, and SQUID magnetometer, on polycrystalline samples were used for the magnetic characterization. Rb2CrCl2I2 shows a Curie–Weiss behavior between 150 and 300 K. The intraplanar superexchange constant J/k=5.8 K. The intra- and interplanar anisotropy have been obtained from the magnetization curves at 4.2 K and are estimated at Hintra=0.16(2) T and Hinter=4.5(2) T.
    Type of Medium: Electronic Resource
    Library Location Call Number Volume/Issue/Year Availability
    BibTip Others were also interested in ...
  • 2
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: The 2D ferromagnets Rb2CrCl4−xBrx; x=0, 1, 2 were studied by means of quasielastic neutron scattering. The compounds order between Tc=52.2 and 57.0 K. Rods of quasielastic diffuse scattering can be observed along the [001] direction. The wave vector dependent modulation of the width and the intensity of the diffuse scattering can be explained as resulting from the effect of the weak interplanar exchange coupling J'. By means of a mean field model, we describe the wave vector dependent susceptibility as function of the scattering vector components with respect to the reciprocal lattice vector. From the data around Tc, we derive that the ratio of the inter/intralayer superexchange changes from J'/J=2.3×10−4 to 10.2×10−4 upon increasing value of x.
    Type of Medium: Electronic Resource
    Library Location Call Number Volume/Issue/Year Availability
    BibTip Others were also interested in ...
  • 3
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 73 (1993), S. 6096-6098 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: Two-dimensional magnetic behavior in thin films and in layered magnets apparently falls into one of only two universality classes. The first is that of the 2D Ising model, characterized by a magnetization exponent β=1/8. The second, with β≈0.23, is observed in systems with planar spin symmetry. Recently it has been shown, using a modified renormalization group calculation, that β=0.23 is a property of a finite size XY model. Although there is no broken symmetry in this system, correlations below the Kosterlitz–Thouless transition temperature decay so slowly that a magnetization occurs in any realizable system, and β=0.23 is a result of two-dimensional fluctuations. By considering a large number of experimental situations we demonstrate that this rule is generally obeyed, and can be used as a test to identify two-dimensional behavior.
    Type of Medium: Electronic Resource
    Library Location Call Number Volume/Issue/Year Availability
    BibTip Others were also interested in ...
  • 4
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: The magnetization of ultrathin films shows a power law dependence on temperature with an exponent β that depends on the spin anisotropy. Experimentally it is found that films with easy-axis anisotropy show β=1/8, characteristic of the two-dimensional Ising model, while those with dominant easy-plane anisotropy show β=0.23. We recently discussed the finite size magnetization of the XY model and showed that this system has universal behavior which leads to the exponent β=0.23. A number of authors have therefore interpreted their results in terms of the finite size two-dimensional XY model. The success of these explanations implies that the four- and sixfold anisotropy fields present in real films are irrelevant in determining the critical behavior of the magnetization. In the sixfold case this observation agrees with theoretical expectations, while in the fourfold case the situation is unclear, as the renormalization group analysis of José et al. shows the fourfold field to be a marginally relevant variable which gives rise to nonuniversal exponents. This theoretical result, however, pertains to the thermodynamic limit and is not necessarily relevant to real finite systems. We investigate the effect of symmetry breaking fields on the magnetic behavior of idealized finite size XY models by means of Monte Carlo simulation. We find that the fourfold field is indeed irrelevant for the system sizes of interest, and may only become relevant for system sizes beyond the physical domain. We also confirm that the sixfold field is both qualitatively and quantitatively irrelevant, and notice a number of novel features connected with the behavior of finite size models which cannot be observed in the thermodynamic limit. © 1996 American Institute of Physics.
    Type of Medium: Electronic Resource
    Library Location Call Number Volume/Issue/Year Availability
    BibTip Others were also interested in ...
  • 5
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: There is considerable theoretical interest in triangular and stacked triangular lattice antiferromagnets, particularly as regards their phase transitions and the nature of the ground state of quantum systems with spin S=1/2. There are, however, no good experimental representatives of the S=1/2 triangular lattice antiferromagnet, and indeed there are few good representatives of those with higher spin. Given the diversity of theoretical problems associated with these systems there is a clear need to find appropriate new model materials. We report the discovery of a versatile new series of triangular lattice magnets, the anhydrous alums of general formula AM(SO4)2, with A=alkali metal, M=Ti,V,Cr,Fe. In these materials the magnetic M ions occupy a regular or very slightly distorted triangular lattice in well-separated layers. All show magnetic ordering effects in the range 2–10 K, the near-neighbor exchange being antiferromagnetic for Ti, V, and Fe and ferromagnetic for Cr. The Ti materials, which we have made for the first time, have S=1/2, and may prove to be the best examples of the S=1/2 triangular lattice antiferromagnet yet discovered. In general, our ability to control the spin value, spin anisotropy, and exchange anisotropy makes the anhydrous alums a potentially useful series for the investigation of a variety of physical problems. © 1996 American Institute of Physics.
    Type of Medium: Electronic Resource
    Library Location Call Number Volume/Issue/Year Availability
    BibTip Others were also interested in ...
  • 6
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 75 (1994), S. 5523-5525 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: The properties of the classical Heisenberg pyrochlore lattice antiferromagnet with local planar single ion anisotropy are discussed. The zero temperature ground state is found to be macroscopically degenerate and without long range order. Monte Carlo simulations are used to investigate the properties of the system at finite temperature. We find that thermal fluctuations select a subset of the ground state manifold, and induce a first-order phase transition to a conventional Néel ground state.
    Type of Medium: Electronic Resource
    Library Location Call Number Volume/Issue/Year Availability
    BibTip Others were also interested in ...
  • 7
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 75 (1994), S. 5955-5957 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: The universal jump in the spin-wave stiffness is a characteristic property of the Kosterlitz–Thouless–Berezinskii phase transition in an infinitely large 2D-XY magnet. It has recently been demonstrated [S. T. Bramwell and P. C. W. Holdsworth, J. Phys. Condens. Matt. 5, L53 (1993)] that finite-size rounding is much more important in two-dimensional than in three-dimensional systems. This is because the properties of the phase transition depend logarithmically, rather than algebraically, on the system size. Consequently, finite-size rounding will be dominant in any real, macroscopic 2D-XY magnet. How the rounded universal jump still exhibits observable universal properties is discussed.
    Type of Medium: Electronic Resource
    Library Location Call Number Volume/Issue/Year Availability
    BibTip Others were also interested in ...
  • 8
    Electronic Resource
    Electronic Resource
    [s.l.] : Macmillian Magazines Ltd.
    Nature 420 (2002), S. 54-57 
    ISSN: 1476-4687
    Source: Nature Archives 1869 - 2009
    Topics: Biology , Chemistry and Pharmacology , Medicine , Natural Sciences in General , Physics
    Notes: [Auszug] Liquids are expected to crystallize at low temperature. The only exception is helium, which can remain liquid at 0 K, owing to quantum fluctuations. Similarly, the atomic magnetic moments (spins) in a magnet are expected to order at a temperature scale set by the Curie–Weiss ...
    Type of Medium: Electronic Resource
    Library Location Call Number Volume/Issue/Year Availability
    BibTip Others were also interested in ...
  • 9
    Electronic Resource
    Electronic Resource
    [s.l.] : Macmillan Magazines Ltd.
    Nature 396 (1998), S. 552-554 
    ISSN: 1476-4687
    Source: Nature Archives 1869 - 2009
    Topics: Biology , Chemistry and Pharmacology , Medicine , Natural Sciences in General , Physics
    Notes: [Auszug] A statistical treatment of three-dimensional turbulent flow continues to pose a challenge to theorists,. One suggestion invokes an analogy with equilibrium phase transitions. Here we approach this idea experimentally, presenting evidence of a strong analogy between the statistical behaviour of ...
    Type of Medium: Electronic Resource
    Library Location Call Number Volume/Issue/Year Availability
    BibTip Others were also interested in ...
  • 10
    Electronic Resource
    Electronic Resource
    Springer
    Physics and chemistry of minerals 15 (1988), S. 446-451 
    ISSN: 1432-2021
    Source: Springer Online Journal Archives 1860-2000
    Topics: Chemistry and Pharmacology , Geosciences , Physics
    Notes: Abstract The mica-like layer compound KNiAsO4 easily exchanges its interlayer potassium ions for alkyl ammonium ions, RNH 3 + (R=CH3 - C18H37). Short chain ions (〈C4) will react in aqueous solution and longer chains in ethanolic solution. The reaction of KNiAsO4 with aqueous solutions of methyl, ethyl and butyl ammonium chlorides of different concentrations has been investigated using a potassium ionselective electrode. Room temperature kinetic curves of percent exchange vs time were obtained. These indicate an apparent ‘cooperative’ mechanism with some rearrangement of the alkyl ammonium ions between the layers during the reaction. KNiAsO4 also reacts with water. This reaction may facilitate the exchange reaction with aqueous alkyl ammonium ions. The alkyl ammonium ions form ordered arrangements between the [NiAsO4]− layers. Small chains (〈C4) adopt a variety of configurations within the same product.
    Type of Medium: Electronic Resource
    Library Location Call Number Volume/Issue/Year Availability
    BibTip Others were also interested in ...
Close ⊗
This website uses cookies and the analysis tool Matomo. More information can be found here...