188 research outputs found
Competition of Mesoscales and Crossover to Tricriticality in Polymer Solutions
We show that the approach to asymptotic fluctuation-induced critical behavior
in polymer solutions is governed by a competition between a correlation length
diverging at the critical point and an additional mesoscopic length-scale, the
radius of gyration. Accurate light-scattering experiments on polystyrene
solutions in cyclohexane with polymer molecular weights ranging from 200,000 up
to 11.4 million clearly demonstrate a crossover between two universal regimes:
a regime with Ising asymptotic critical behavior, where the correlation length
prevails, and a regime with tricritical theta-point behavior determined by a
mesoscopic polymer-chain length.Comment: 4 pages in RevTeX with 4 figure
Universality versus nonuniversality in asymmetric fluid criticality
Critical phenomena in real fluids demonstrate a combination of universal features caused by the divergence of long-range fluctuations of density and nonuniversal (system-dependent) features associated with specific intermolecular interactions. Asymptotically, all fluids belong to the Ising-model class of universality. The asymptotic power laws for the thermodynamic properties are described by two independent universal critical exponents and two independent nonuniversal critical amplitudes; other critical amplitudes can be obtained by universal relations. The nonuniversal critical parameters (critical temperature, pressure, and density) can be absorbed in the property units. Nonasymptotic critical behavior of fluids can be divided in two parts, symmetric ("Ising-like") and asymmetric ("fluid-like"). The symmetric nonasymptotic behavior contains a new universal exponent (Wegner exponent) and the system-dependent crossover scale (Ginzburg number) associated with the range of intermolecular interactions, while the asymmetric features are generally described by an additional universal exponent and by three nonasymptotic amplitudes associated with mixing of the physical fields into the scaling fields.ΠΡΠΈΡΠΈΡΠ½i ΡΠ²ΠΈΡΠ° Π² ΡΠ΅Π°Π»ΡΠ½ΠΈΡ
ΠΏΠ»ΠΈΠ½Π°Ρ
Π΄Π΅ΠΌΠΎΠ½ΡΡΡΡΡΡΡ ΠΊΠΎΠΌΠ±iΠ½Π°ΡiΡ ΡΠ½iΠ²Π΅ΡΡΠ°Π»ΡΠ½ΠΈΡ
ΡΠΈΡ, ΡΠΏΡΠΈΡΠΈΠ½Π΅Π½ΠΈΡ
ΡΠΎΠ·Π±iΠΆΠ½iΡΡΡ Π΄Π°Π»Π΅ΠΊΠΎΡΡΠΆΠ½ΠΈΡ
ΡΠ»ΡΠΊΡΡΠ°ΡiΠΉ Π³ΡΡΡΠΈΠ½ΠΈ, i Π½Π΅ΡΠ½iΠ²Π΅ΡΡΠ°Π»ΡΠ½ΠΈΡ
(ΡΠΈΡΡΠ΅ΠΌΠΎ Π·Π°Π»Π΅ΠΆΠ½ΠΈΡ
) ΡΠΈΡ, ΠΏΠΎΠ²βΡΠ·Π°Π½ΠΈΡ
iΠ· ΡΠΏΠ΅ΡΠΈΡiΡΠ½ΠΈΠΌΠΈ ΠΌiΠΆΠΌΠΎΠ»Π΅ΠΊΡΠ»ΡΡΠ½ΠΈΠΌΠΈ Π²Π·Π°ΡΠΌΠΎΠ΄iΡΠΌΠΈ. ΠΡΠΈΠΌΠΏΡΠΎΡΠΈΡΠ½ΠΎ Π²Ρi ΠΏΠ»ΠΈΠ½ΠΈ Π½Π°Π»Π΅ΠΆΠ°ΡΡ Π΄ΠΎ ΠΊΠ»Π°ΡΡ ΡΠ½iΠ²Π΅ΡΡΠ°Π»ΡΠ½ΠΎΡΡi ΠΌΠΎΠ΄Π΅Π»i IΠ·ΠΈΠ½Π³Π°. ΠΡΠΈΠΌΠΏΡΠΎΡΠΈΡΠ½i ΡΡΠ΅ΠΏΠ΅Π½Π΅Π²i Π·Π°ΠΊΠΎΠ½ΠΈ Π΄Π»Ρ ΡΠ΅ΡΠΌΠΎΠ΄ΠΈΠ½Π°ΠΌiΡΠ½ΠΈΡ
Π²Π»Π°ΡΡΠΈΠ²ΠΎΡΡΠ΅ΠΉ ΠΎΠΏΠΈΡΡΡΡΡΡΡ Π΄Π²ΠΎΠΌΠ° Π½Π΅Π·Π°Π»Π΅ΠΆΠ½ΠΈΠΌΠΈ ΡΠ½iΠ²Π΅ΡΡΠ°Π»ΡΠ½ΠΈΠΌΠΈ ΠΊΡΠΈΡΠΈΡΠ½ΠΈΠΌΠΈ ΠΏΠΎΠΊΠ°Π·Π½ΠΈΠΊΠ°ΠΌΠΈ i Π΄Π²ΠΎΠΌΠ° Π½Π΅Π·Π°Π»Π΅ΠΆΠ½ΠΈΠΌΠΈ Π½Π΅ΡΠ½iΠ²Π΅ΡΡΠ°Π»ΡΠ½ΠΈΠΌΠΈ ΠΊΡΠΈΡΠΈΡΠ½ΠΈΠΌΠΈ Π°ΠΌΠΏΠ»iΡΡΠ΄Π°ΠΌΠΈ; ΡΠ΅ΡΡΡ ΠΊΡΠΈΡΠΈΡΠ½ΠΈΡ
Π°ΠΌΠΏΠ»iΡΡΠ΄ ΠΌΠΎΠΆΠ½Π° ΠΎΡΡΠΈΠΌΠ°ΡΠΈ Π· ΡΠ½iΠ²Π΅ΡΡΠ°Π»ΡΠ½ΠΈΡ
ΡΠΏiΠ²Π²iΠ΄Π½ΠΎΡΠ΅Π½Ρ. ΠΠ΅-ΡΠ½iΠ²Π΅ΡΡΠ°Π»ΡΠ½i ΠΊΡΠΈΡΠΈΡΠ½i ΠΏΠ°ΡΠ°ΠΌΠ΅ΡΡΠΈ (ΠΊΡΠΈΡΠΈΡΠ½Π° ΡΠ΅ΠΌΠΏΠ΅ΡΠ°ΡΡΡΠ°, ΡΠΈΡΠΊ i Π³ΡΡΡΠΈΠ½Π°) ΠΌΠΎΠΆΡΡΡ Π±ΡΡΠΈ Π²ΠΊΠ»ΡΡΠ΅Π½i Π² ΠΎΠ΄ΠΈΠ½ΠΈΡi ΡΠΈΡ
Π²Π»Π°ΡΡΠΈΠ²ΠΎΡΡΠ΅ΠΉ. ΠΠ΅Π°ΡΠΈΠΌΠΏΡΠΎΡΠΈΡΠ½Ρ ΠΊΡΠΈΡΠΈΡΠ½Ρ ΠΏΠΎΠ²Π΅Π΄iΠ½ΠΊΡ ΠΏΠ»ΠΈΠ½iΠ² ΠΌΠΎΠΆΠ½Π° ΠΏΠΎΠ΄iΠ»ΠΈΡΠΈ Π½Π° Π΄Π²i ΡΠ°ΡΡΠΈΠ½ΠΈ, ΡΠΈΠΌΠ΅ΡΡΠΈΡΠ½Ρ (βiΠ·ΠΈΠ½Π³ΠΎΠΏΠΎΠ΄iΠ±Π½Ρβ) i Π°ΡΠΈΠΌΠ΅ΡΡΠΈΡΠ½Ρ (βΠΏΠ»ΠΈΠ½ΠΎΠΏΠΎΠ΄iΠ±Π½Ρβ). Π‘ΠΈΠΌΠ΅ΡΡΠΈΡΠ½Π° Π½Π΅Π°ΡΠΈΠΌΠΏΡΠΎΡΠΈΡΠ½Π° ΠΏΠΎΠ²Π΅Π΄iΠ½ΠΊΠ° ΠΌiΡΡΠΈΡΡ Π½ΠΎΠ²ΠΈΠΉ ΡΠ½iΠ²Π΅ΡΡΠ°Π»ΡΠ½ΠΈΠΉ ΠΏΠΎΠΊΠ°Π·Π½ΠΈΠΊ (ΠΏΠΎΠΊΠ°Π·Π½ΠΈΠΊ ΠΠ΅Π³Π½Π΅ΡΠ°) i ΡΠΈΡΡΠ΅ΠΌΠΎ Π·Π°Π»Π΅ΠΆΠ½ΠΈΠΉ ΠΌΠ°ΡΡΡΠ°Π± ΠΊΡΠΎΡΠΎΠ²Π΅ΡΡ (ΡΠΈΡΠ»ΠΎ ΠiΠ½Π·-Π±ΡΡΠ³Π°), ΠΏΠΎΠ²βΡΠ·Π°Π½ΠΈΠΉ Π· ΠΎΠ±Π»Π°ΡΡΡ Π΄iΡ ΠΌiΠΆΠΌΠΎΠ»Π΅ΠΊΡΠ»ΡΡΠ½ΠΈΡ
Π²Π·Π°ΡΠΌΠΎΠ΄iΠΉ, ΡΠΎΠ΄i ΡΠΊ Π°ΡΠΈΠΌΠ΅ΡΡΠΈΡΠ½i ΡΠΈΡΠΈ Π²Π·Π°Π³Π°Π»ΡΠ½ΠΎΠΌΡ ΠΎΠΏΠΈΡΡΡΡΡΡΡ Π΄ΠΎΠ΄Π°ΡΠΊΠΎΠ²ΠΈΠΌ ΡΠ½iΠ²Π΅ΡΡΠ°Π»ΡΠ½ΠΈΠΌ ΠΏΠΎΠΊΠ°Π·Π½ΠΈΠΊΠΎΠΌ i ΡΡΡΠΎΠΌΠ° Π½Π΅Π°ΡΠΈΠΌΠΏΡΠΎΡΠΈΡΠ½ΠΈΠΌΠΈ Π°ΠΌΠΏΠ»iΡΡΠ΄Π°ΠΌΠΈ, ΠΏΠΎΠ²βΡΠ·Π°Π½ΠΈΠΌΠΈ Π·i Π·ΠΌiΡΡΠ²Π°Π½Π½ΡΠΌ ΡiΠ·ΠΈΡΠ½ΠΈΡ
ΠΏΠΎΠ»iΠ² Ρ ΡΠΊΠ΅ΠΉΠ»iΠ½Π³ΠΎΠ²ΠΈΡ
ΠΏΠΎΠ»ΡΡ
Shape of crossover between mean-field and asymptotic critical behavior in a three-dimensional Ising lattice
Recent numerical studies of the susceptibility of the three-dimensional Ising
model with various interaction ranges have been analyzed with a crossover model
based on renormalization-group matching theory. It is shown that the model
yields an accurate description of the crossover function for the
susceptibility.Comment: 4 pages RevTeX + 3 PostScript figures. Uses epsf.sty and rotate.sty.
Final version; accepted for publication in Physics Letters
The influence of the rare earth ions radii on the Low Spin to Intermediate Spin state transition in lanthanide cobaltite perovskites: LaCoO3 vs. HoCoO3
We present first principles LDA+U calculations of electronic structure and
magnetic state for LaCoO3 and HoCoO3. Low Spin to Intermediate Spin state
transition was found in our calculations using experimental crystallographic
data for both materials with a much higher transition temperature for HoCoO3,
which agrees well with the experimental estimations. Low Spin state t6e0
(non-magnetic) to Intermediate Spin state t5e1 (magnetic) transition of Co(3+)
ions happens due to the competition between crystal field t_2g-e_g splitting
and effective exchange interaction between 3 spin-orbitals. We show that the
difference in crystal structure parameters for HoCoO3 and LaCoO3 due to the
smaller ionic radius of Ho ion comparing with La ion results in stronger
crystal field splitting for HoCoO3 (0.09 eV ~ 1000 K larger than for LaCoO3)
and hence tip the balance between the Low Spin and Intermediate Spin states to
the non-magnetic solution in HoCoO3.Comment: 13 pages, 6 figure
Influence of the external magnetic field on the cylindrical electron bunch injected into plasma
Dynamics of the initially cylindrical electron bunch injected into plasma along the external magnetic field was studied via PIC simulation. Time evolution of the spatial distributions of electric field, magnetic field and bunch electron density is analyzed. The influence of the external magnetic field on the bunch shape and wake field excitation is treated. The correlation between azimuthal magnetic field distribution and wake field shape is discussed.Π‘ ΠΏΠΎΠΌΠΎΡΡΡ ΡΠΈΡΠ»Π΅Π½Π½ΠΎΠ³ΠΎ ΠΌΠΎΠ΄Π΅Π»ΠΈΡΠΎΠ²Π°Π½ΠΈΡ ΠΌΠ΅ΡΠΎΠ΄ΠΎΠΌ ΡΠ°ΡΡΠΈΡ Π² ΡΡΠ΅ΠΉΠΊΠ°Ρ
ΠΈΡΡΠ»Π΅Π΄ΡΠ΅ΡΡΡ Π΄ΠΈΠ½Π°ΠΌΠΈΠΊΠ° ΡΠ³ΡΡΡΠΊΠ° ΡΠ»Π΅ΠΊΡΡΠΎΠ½ΠΎΠ², ΠΈΠ·Π½Π°ΡΠ°Π»ΡΠ½ΠΎ ΠΈΠΌΠ΅ΡΡΠ΅Π³ΠΎ ΡΠΎΡΠΌΡ ΡΠΈΠ»ΠΈΠ½Π΄ΡΠ°, Π²Π»Π΅ΡΠ°ΡΡΠ΅Π³ΠΎ Π² ΠΏΠ»Π°Π·ΠΌΡ Π² ΠΏΡΠΈΡΡΡΡΡΠ²ΠΈΠΈ ΠΏΡΠΎΠ΄ΠΎΠ»ΡΠ½ΠΎΠ³ΠΎ Π²Π½Π΅ΡΠ½Π΅Π³ΠΎ ΠΌΠ°Π³Π½ΠΈΡΠ½ΠΎΠ³ΠΎ ΠΏΠΎΠ»Ρ. ΠΠ½Π°Π»ΠΈΠ·ΠΈΡΡΡΡΡΡ ΠΈΠ·ΠΌΠ΅Π½Π΅Π½ΠΈΡ ΠΏΡΠΎΡΡΡΠ°Π½ΡΡΠ²Π΅Π½Π½ΡΡ
ΡΠ°ΡΠΏΡΠ΅Π΄Π΅Π»Π΅Π½ΠΈΠΉ ΡΠ»Π΅ΠΊΡΡΠΈΡΠ΅ΡΠΊΠΎΠ³ΠΎ ΠΈ ΠΌΠ°Π³Π½ΠΈΡΠ½ΠΎΠ³ΠΎ ΠΏΠΎΠ»Π΅ΠΉ, Π° ΡΠ°ΠΊΠΆΠ΅ ΠΏΠ»ΠΎΡΠ½ΠΎΡΡΠΈ ΡΠ»Π΅ΠΊΡΡΠΎΠ½ΠΎΠ² Π² ΡΠ³ΡΡΡΠΊΠ΅. ΠΠ±ΡΡΠΆΠ΄Π°Π΅ΡΡΡ Π²Π»ΠΈΡΠ½ΠΈΠ΅ ΠΏΡΠΎΠ΄ΠΎΠ»ΡΠ½ΠΎΠ³ΠΎ ΠΌΠ°Π³Π½ΠΈΡΠ½ΠΎΠ³ΠΎ ΠΏΠΎΠ»Ρ Π½Π° ΡΠΎΡΠΌΡ ΡΠ³ΡΡΡΠΊΠ° ΠΈ Π²ΠΎΠ·Π±ΡΠΆΠ΄Π΅Π½ΠΈΠ΅ ΠΊΠΈΠ»ΡΠ²Π°ΡΠ΅ΡΠ½ΠΎΠΉ Π²ΠΎΠ»Π½Ρ. ΠΡΡΠ»Π΅Π΄ΡΠ΅ΡΡΡ Π·Π°Π²ΠΈΡΠΈΠΌΠΎΡΡΡ ΠΌΠ΅ΠΆΠ΄Ρ ΡΠΎΡΠΌΠΎΠΉ ΡΠ³ΡΡΡΠΊΠ°, ΠΏΠΎΠ»Π΅ΠΌ ΠΊΠΈΠ»ΡΠ²Π°ΡΠ΅ΡΠ½ΠΎΠΉ Π²ΠΎΠ»Π½Ρ ΠΈ ΡΠ°ΡΠΏΡΠ΅Π΄Π΅Π»Π΅Π½ΠΈΠ΅ΠΌ Π°Π·ΠΈΠΌΡΡΠ°Π»ΡΠ½ΠΎΠΉ ΡΠΎΡΡΠ°Π²Π»ΡΡΡΠ΅ΠΉ ΠΌΠ°Π³Π½ΠΈΡΠ½ΠΎΠ³ΠΎ ΠΏΠΎΠ»Ρ.ΠΠ° Π΄ΠΎΠΏΠΎΠΌΠΎΠ³ΠΎΡ ΡΠΈΡΠ΅Π»ΡΠ½ΠΎΠ³ΠΎ ΠΌΠΎΠ΄Π΅Π»ΡΠ²Π°Π½Π½Ρ ΠΌΠ΅ΡΠΎΠ΄ΠΎΠΌ ΡΠ°ΡΡΠΈΠ½ΠΎΠΊ Ρ ΠΊΠΎΠΌΡΡΠΊΠ°Ρ
Π΄ΠΎΡΠ»ΡΠ΄ΠΆΡΡΡΡΡΡ Π΄ΠΈΠ½Π°ΠΌΡΠΊΠ° Π·Π³ΡΡΡΠΊΠ° Π΅Π»Π΅ΠΊΡΡΠΎΠ½ΡΠ², ΡΠΎ ΠΏΠΎΡΠ°ΡΠΊΠΎΠ²ΠΎ ΠΌΠ°Ρ ΡΠΈΠ»ΡΠ½Π΄ΡΠΈΡΠ½Ρ ΡΠΎΡΠΌΡ, ΡΠ° Π²Π»ΡΡΠ°Ρ Π² ΠΏΠ»Π°Π·ΠΌΡ Ρ ΠΏΡΠΈΡΡΡΠ½ΠΎΡΡΡ Π·ΠΎΠ²Π½ΡΡΠ½ΡΠΎΠ³ΠΎ ΠΏΠΎΠ·Π΄ΠΎΠ²ΠΆΠ½ΡΠΎΠ³ΠΎ ΠΌΠ°Π³Π½ΡΡΠ½ΠΎΠ³ΠΎ ΠΏΠΎΠ»Ρ. ΠΠ½Π°Π»ΡΠ·ΡΡΡΡΡΡ Π·ΠΌΡΠ½ΠΈ ΠΏΡΠΎΡΡΠΎΡΠΎΠ²ΠΎΠ³ΠΎ ΡΠΎΠ·ΠΏΠΎΠ΄ΡΠ»Ρ Π΅Π»Π΅ΠΊΡΡΠΈΡΠ½ΠΎΠ³ΠΎ ΡΠ° ΠΌΠ°Π³Π½ΡΡΠ½ΠΎΠ³ΠΎ ΠΏΠΎΠ»ΡΠ², Π° ΡΠ°ΠΊΠΎΠΆ Π³ΡΡΡΠΈΠ½ΠΈ Π΅Π»Π΅ΠΊΡΡΠΎΠ½ΡΠ² Ρ Π·Π³ΡΡΡΠΊΡ. ΠΠ±Π³ΠΎΠ²ΠΎΡΡΡΡΡΡΡ Π²ΠΏΠ»ΠΈΠ² Π·ΠΎΠ²Π½ΡΡΠ½ΡΠΎΠ³ΠΎ ΠΌΠ°Π³Π½ΡΡΠ½ΠΎΠ³ΠΎ ΠΏΠΎΠ»Ρ Π½Π° ΡΠΎΡΠΌΡ Π·Π³ΡΡΡΠΊΠ° ΡΠ° Π·Π±ΡΠ΄ΠΆΡΠ²Π°Π½Ρ ΠΊΡΠ»ΡΠ²Π°ΡΠ΅ΡΠ½Ρ Ρ
Π²ΠΈΠ»Ρ. ΠΠΎΠΊΠ°Π·Π°Π½Π° Π·Π°Π»Π΅ΠΆΠ½ΡΡΡΡ ΠΌΡΠΆ ΡΠΎΡΠΌΠΎΡ Π·Π³ΡΡΡΠΊΠ°, ΠΏΠΎΠ»Π΅ΠΌ ΠΊΡΠ»ΡΠ²Π°ΡΠ΅ΡΠ½ΠΎΡ Ρ
Π²ΠΈΠ»Ρ ΡΠ° ΡΠΎΠ·ΠΏΠΎΠ΄ΡΠ»ΠΎΠΌ Π°Π·ΠΈΠΌΡΡΠ°Π»ΡΠ½ΠΎΡ ΡΠΊΠ»Π°Π΄ΠΎΠ²ΠΎΡ ΠΌΠ°Π³Π½ΡΡΠ½ΠΎΠ³ΠΎ ΠΏΠΎΠ»Ρ
The semileptonic decays of the B_c meson
We study the semileptonic transitions B_c to \eta_c, J/\psi, D, D^*, B, B^*,
B_s, B_s^* in the framework of a relativistic constituent quark model. We use
experimental data on leptonic J/\psi decay, lattice and QCD sum rule results on
leptonic B_c decay, and on radiative \eta_c transitions to adjust the quark
model parameters. We compute all form factors of the above semileptonic
B_c-transitions and give predictions for various semileptonic B_c decay modes
including their \tau-modes when they are kinematically accessible. The
implications of heavy quark symmetry for the semileptonic decays are discussed
and are shown to be manifest in our explicit relativistic quark model
calculation. A comparison of our results with the results of other calculations
is performed.Comment: 31 pages Latex (uses epsf, revtex). Section II expanded, typos
corrected. This version will appear in Phys. Rev.
Brane World Susy Breaking from String/M Theory
String and M-theory realizations of brane world supersymmetry breaking
scenarios are considered in which visible sector Standard Model fields are
confined on a brane, with hidden sector supersymmetry breaking isolated on a
distant brane. In calculable examples with an internal manifold of any volume
the Kahler potential generically contains brane--brane non-derivative contact
interactions coupling the visible and hidden sectors and is not of the no-scale
sequestered form. This leads to non-universal scalar masses and without
additional assumptions about flavor symmetries may in general induce dangerous
sflavor violation even though the Standard Model and supersymmetry branes are
physically separated. Deviations from the sequestered form are dictated by bulk
supersymmetry and can in most cases be understood as arising from exchange of
bulk supergravity fields between branes or warping of the internal geometry.
Unacceptable visible sector tree-level tachyons arise in many models but may be
avoided in certain classes of compactifications. Anomaly mediated and gaugino
mediated contributions to scalar masses are sub-dominant except in special
circumstances such as a flat or AdS pure five--dimensional bulk geometry
without bulk vector multiplets.Comment: Latex, 83 pages, references adde
Charge and Orbital Ordering and Spin State Transition Driven by Structural Distortion in YBaCo_2O_5
We have investigated electronic structures of antiferromagnetic YBaCo_2O_5
using the local spin-density approximation (LSDA) + U method. The charge and
orbital ordered insulating ground state is correctly obtained with the strong
on-site Coulomb interaction. Co^{2+} and Co^{3+} ions are found to be in the
high spin (HS) and intermediate spin (IS) state, respectively. It is considered
that the tetragonal to orthorhombic structural transition is responsible for
the ordering phenomena and the spin states of Co ions. The large contribution
of the orbital moment to the total magnetic moment indicates that the
spin-orbit coupling is also important in YBaCo_2O_5.Comment: 4 pages including 4 figures, Submitted to Phys. Rev. Let
Application of Minimal Subtraction Renormalization to Crossover Behavior near the He Liquid-Vapor Critical Point
Parametric expressions are used to calculate the isothermal susceptibility,
specific heat, order parameter, and correlation length along the critical
isochore and coexistence curve from the asymptotic region to crossover region.
These expressions are based on the minimal-subtraction renormalization scheme
within the model. Using two adjustable parameters in these
expressions, we fit the theory globally to recently obtained experimental
measurements of isothermal susceptibility and specific heat along the critical
isochore and coexistence curve, and early measurements of coexistence curve and
light scattering intensity along the critical isochore of He near its
liquid-vapor critical point. The theory provides good agreement with these
experimental measurements within the reduced temperature range
Spin state and phase competition in TbBaCo_{2}O_{5.5} and the lanthanide series LnBaCo_{2}O_{5+\delta} (0<=\delta<=1)
A clear physics picture of TbBaCoO is revealed on the basis of
density functional theory calculations. An antiferromagnetic (AFM)
superexchange coupling between the almost high-spin Co ions competes
with a ferromagnetic (FM) interaction mediated by both p-d exchange and double
exchange, being responsible for the observed AFM-FM transition. And the
metal-insulator transition is accompanied by an xy/xz orbital-ordering
transition. Moreover, this picture can be generalized to the whole lanthanide
series, and it is predicted that a few room-temperature magnetoresistance
materials could be found in LnBaACoO
(Ln=Ho,Er,Tm,Yb,Lu; A=Sr,Ca,Mg).Comment: 13 pages, 2 figures; to be published in Phys. Rev. B on 1st Sept.
Title and Bylines are added to the revised versio
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