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 81 (1997), S. 4399-4399 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: The easy-axis triangular antiferromagnet CsNiCl3 undergoes a magnetic phase transition to a triangular chirally ordered 120° type magnetic structure in an applied magnetic field of 2 T directed along the c axis. We studied by means of elastic neutron diffraction the crossover to chiral ordering. At B=2 T, the exponent of the sublattice magnetization β=0.25, which confirms the creation of the chirally ordered state. Data taken at B=1.75 T indicate that the crossover may be smeared out in B or is due to a slight misorientation of the applied field. The induced change in the magnetization direction of the ordered moments was also studied by means of SQUID magnetometry. © 1997 American Institute of Physics.
    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 magnetic moments in the triangular antiferromagnetic CsMnBr3 order at TN=8.3 K with a frustration of the magnetic moments in a 120° type magnetic structure. The magnetic moments are either ordered in a clockwise or an anticlockwise direction resulting in a chirality ordering, which is characterized by the critical exponent of the magnetic sublattice magnetization β=0.25. It has been shown that an electric field applied along the [110] direction removes the chiral ordering and a linear Ising-like phase will be established; consequently, the value of β decreases. The subsequent application of a magnetic field of B=4 T along the [100] direction causes the critical exponent β to increase. The magnetic phase diagram of CsMnBr3 does not change due to the introduction of an electric field.© 1997 American Institute of Physics.
    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 65 (1989), S. 718-725 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: Surface Brillouin scattering has been used to measure the dispersion relations of surface, interface, and guided modes in nickel films supported on quartz glass with thicknesses of 100, 200, 500, 1000, and 2000 nm. The elastic constants of nickel have been estimated near the glass interface and near the free surface of the film. Thin films (up to 500 nm) turn out to be homogeneous, while thicker films show increasingly higher values of the elastic constant c44. This behavior could be related to a change from the (111) preferentially oriented nickel crystallites on the glass, typical of thin FCC films, to a more isotropic growth for thicknesses greater than about 500 nm.
    Type of Medium: Electronic Resource
    Library Location Call Number Volume/Issue/Year Availability
    BibTip Others were also interested in ...
  • 4
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 85 (1999), S. 5378-5380 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: The MII and MIII magnetic ions in the extended molecular network P(C6D5)4MnFe(C2O4)3 form a two-dimensional honeycomb magnetic lattice. The Mn2+ and Fe3+ ions alternate in the extended network which is formed by the oxalate (C2O4) ligands. These hexagonal layers are separated and charge compensated by large [P(C6D5)4]+ ions, positioned in between the honeycomb layers. P(C6D5)4MnFe(C2O4)3 orders magnetically at TN=27(1) K. A full neutron spin polarization study of the neutron scattering cross section has been carried out which allows the unambigious separation of the magnetic cross section from the total diffraction process. The magnetic structure can be described with the magnetic Shubnikov group R3c. The magnetic moments are antiferromagnetically aligned along the c axis while the Mn2+ and Fe3+ ions form an antiferromagnetic alignment on the honeycomb lattice. © 1999 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: 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 ...
  • 6
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: The two-dimensional S=1/2 Heisenberg antiferromagnet copper(II) formate tetrahydrate has been doped with diamagnetic impurities, Mg2+, Zn2+, up to levels of 15%. The decrease of TN as function of the doping concentration has been compared to that of La2CuO4 and other 2D magnets. A discussion of recent ESR results and single crystal magnetic susceptibility data in view of the interaction between the magnetic ions is presented.
    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 69 (1991), S. 5998-6000 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: Compounds of chemical formula AFeX3 (A=Rb,Cs,Tl, and X=Cl, Br) provide an isomorphous series of one-dimensional induced-moment magnets with an effective spin S=1. They display a variety of ordered magnetic structures at low temperatures, depending on the sign and relative magnitudes of the intra- and interchain exchange and any magnetic dipole–dipole interactions. We report the first preparation of the salt NH4FeBr3. Powder neutron diffraction measurements on a perdeuterated sample showed that at room temperature the unit cell is hexagonal with cell parameters a=7.398(3) A(ring) and c=6.331(2) A(ring). On cooling, structural phase transitions to cells of successively lower symmetry were observed. These are probably caused by cooperative reorientations of the ND+4 tetrahedra. At 4.8(2) K and 2.8(2) K additional Bragg peaks were observed. These additional reflections were attributed to magnetic long-range order with antiferromagnetic exchange both in the basal plane and along the c axis and could be indexed on an orthorhombic unit cell of dimension 2a ×(square root of) 3a × c. Magnetic susceptibility measurements taken with a SQUID magnetometer on a polycrystalline sample at 2–100 K with an applied magnetic field of 0.1 T showed very similar behavior to that for RbFeBr3, with a broad cusp at approximately 8 K and θ(approximately-equal-to)−43 K.
    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.] : American Institute of Physics (AIP)
    Journal of Applied Physics 69 (1991), S. 6016-6018 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: The compound KMnPO4⋅H2O adopts the NH4CoPO4⋅H2O structure, in which distorted MII octahedra form corner-sharing sheets, separated by layers of K+ ions. Within a layer, the divalent metal ions form an approximately square lattice. In the range 75–300 K the magnetic susceptibility of KMnPO4⋅H2O follows the Curie–Weiss law, with C=4.73(6) emu K mol−1, θ=−61(2) K. Below 75 K, the susceptibility deviates from this simple model, showing a broad susceptibility maximum with T(χmax) ∼ 27(2) K, which suggests the presence of two-dimensional magnetic interactions. Below about 18 K, magnetization measurements at 0.068 T indicate a weak ferromagnetic moment, with domain effects apparent below 9 K. High-resolution powder neutron-diffraction profiles have been measured at room temperature and 1.7 K. No change in crystal structure is found between these two temperatures, and all additional magnetic reflections in the low-temperature profile were indexed on the nuclear cell. The space group is Pmn21, and Bertaut's theorem clearly demonstrates that only two magnetic structures in which ferro- and antiferromagnetic moments coexist are possible. The antiferromagnetic structure has been unambiguously refined, however, the canting was too small to be resolved with the available data.
    Type of Medium: Electronic Resource
    Library Location Call Number Volume/Issue/Year Availability
    BibTip Others were also interested in ...
  • 9
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: Magnetic susceptibility and magnetization data are reported for the organic-inorganic composite material phenyl-MnPO4. The phenyl groups are situated between MnPO4 layers. The MnO46− octahedra of these layers form a quasi 2D square lattice. Two-dimensional magnetism has been observed above TN=13.8 (1) K, θCW=53 (1) K. Weak ferromagnetism is observed below TN. An ac-magnetic susceptibility study showed two peaks around TN, which indicates that the magnetic ordering process takes place in two steps. The magnetic susceptibility data indicate the presence of a reorientational structural phase transition around Tph=250 K.
    Type of Medium: Electronic Resource
    Library Location Call Number Volume/Issue/Year Availability
    BibTip Others were also interested in ...
  • 10
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: The singlet ground state antiferromagnet RbFeBr3 shows an induced moment behavior at low temperatures and orders antiferromagnetically at TN=5.5 K. A second magnetic phase transition takes place at 2.0 K. The magnetic phase between 2 K 〈T〈5.5 K may be partially ordered while at T〈2.0 K a modified triangular magnetic structure will be adopted. The temperature dependence of the magnetic excitations at the soft mode point Q(1/3,1/3,1) show a switching of intensity at 2 K. Above 4 K the magnetic excitations start to broaden. Above TN the magentic excitations show a renormalization behavior. The temperature dependence of renormalization is well described by the theoretical predictions of the DCEFA model.
    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...