66 research outputs found
The spin glass-antiferromagnetism competition in Kondo-lattice systems in the presence of a transverse applied magnetic field
A theory is proposed to describe the competition among antiferromagnetism
(AF), spin glass (SG) and Kondo effect. The model describes two Kondo
sublattices with an intrasite Kondo interaction strength and a random
Gaussian interlattice interaction in the presence of a transverse field
. The field is introduced as a quantum mechanism to produce
spin flipping and the random coupling has average and variance . The path integral formalism with Grassmann fields is used to study
this fermionic problem, in which the disorder is treated within the framework
of the replica trick. The free energy and the order parameters are obtained
using the static ansatz. In this many parameters problem, we choose and to allow a better
comparison with the experimental findings. The obtained phase diagram has not
only the same sequence as the experimental one for
, but mainly, it also shows a qualitative agreement
concerning the behavior of the freezing temperature and the Neel temperature
which decreases until a Quantum Critical Point (QCP).Comment: 4 pages, 1 figure, accepted for publication in Physica
Fermionic van Hemmen Spin Glass Model with a Transverse Field
In the present work it is studied the fermionic van Hemmen model for the spin
glass (SG) with a transverse magnetic field . In this model, the spin
operators are written as a bilinear combination of fermionic operators, which
allows the analysis of the interplay between charge and spin fluctuations in
the presence of a quantum spin flipping mechanism given by . The
problem is expressed in the fermionic path integral formalism. As results,
magnetic phase diagrams of temperature versus the ferromagnetic interaction are
obtained for several values of chemical potential and . The
field suppresses the magnetic orders. The increase of alters the
average occupation per site that affects the magnetic phases. For instance, the
SG and the mixed SG+ferromagnetic phases are also suppressed by . In
addition, can change the nature of the phase boundaries introducing a
first order transition.Comment: 9 pages, 4 figures, accepted for publication in Phys. Lett.
Fermionic Ising glasses with BCS pairing interaction in the presence of a transverse field
In the present work we have analyzed a fermionic infinite-ranged Ising spin
glass with a local BCS coupling in the presence of transverse field. This model
has been obtained by tracing out the conduction electrons degrees of freedom in
a superconducting alloy. The transverse field \Gamma is applied in the
resulting effective model. The problem is formulated in the path integral
formalism where the spins operators are represented by bilinear combination of
Grassmann fields. The problem can be solved by combining previous approaches
used to study a fermionic Heisenberg spin glass and a Ising spin glass in a
transverse field. The results are show in a phase diagram T/J {\it versus}
\Gamma/J (J is the standard deviation of the random coupling J_{ij}) for
several values of g (the strength of the pairing interaction). For small g, the
line transition T_c(\Gamma) between the normal paramagnetic phase and the spin
glass phase decreases when increases \Gamma, until it reaches a quantum
critical point. For increasing g, a PAIR phase (where there is formation of
local pairs) has been found which disappears when is close to \Gamma_c showing
that the transverse field tends to inhibited the PAIR phase.Comment: 2 pages, 2 figures, accepted in Physica C Proceedings M2SRI
A theoretical study of the cluster glass-Kondo-magnetic disordered alloys
The physics of disordered alloys, such as typically the well known case of
CeNi1-xCux alloys, showing an interplay among the Kondo effect, the spin glass
state and a magnetic order, has been studied firstly within an average
description like in the Sherrington-Kirkpatrick model. Recently, a theoretical
model (PRB 74, 014427 (2006)) involving a more local description of the
intersite interaction has been proposed to describe the phase diagram of
CeNi1-xCux. This alloy is an example of the complex interplay between Kondo
effect and frustration in which there is in particular the onset of a
cluster-glass state. Although the model given in Ref. PRB 74, 014427 (2006) has
reproduced the different phases relatively well, it is not able to describe the
cluster-glass state. We study here the competition between the Kondo effect and
a cluster glass phase within a Kondo Lattice model with an inter-cluster random
Gaussian interaction. The inter-cluster term is treated within the cluster
mean-field theory for spin glasses, while, inside the cluster, an exact
diagonalisation is performed including inter-site ferromagnetic and intra-site
Kondo interactions. The cluster glass order parameters and the Kondo
correlation function are obtained for different values of the cluster size, the
intra-cluster ferromagnetic coupling and the Kondo intra-site coupling. We
obtain, for instance, that the increase of the Kondo coupling tends to destroy
the cluster glass phase.Comment: 6 pages, 2 figures, Accepted for publication in Physica
Doniach diagram for ordered, disordered and underscreened Kondo lattices
The Doniach's diagram has been originally proposed to describe the
competition between the local Kondo effect and the intersite RKKY interactions
in cerium compounds. Here we discuss the extension of this diagram to different
variations of Kondo lattice model. We consider a) ordered cerium compounds
where the competition between magnetic order and Kondo effect plays an
important role, as , b) disordered cerium systems with competing
spin glass phase, magnetic ordered phases and a Kondo phase, as the heavy
fermion cerium alloy and, c) uranium compounds where a
coexistence between Kondo effect and ferromagnetic order has been observed, as
UTe. We show that all these cases can be described by a generalized Doniach
phase diagram.Comment: Presented in the Latin American Workshop on Magnetism and Magnetic
Materials (LAW3M) Rio de Janeiro, Brazil, August 12-16, 2007. Proceedings to
be published in JMM
Stability conditions for fermionic Ising spin-glass models in the presence of a transverse field
The stability of spin-glass (SG) phase is analyzed in detail for a fermionic
Ising SG (FISG) model in the presence of a magnetic transverse field .
The fermionic path integral formalism, replica method and static approach have
been used to obtain the thermodynamic potential within one step replica
symmetry breaking ansatz. The replica symmetry (RS) results show that the SG
phase is always unstable against the replicon. Moreover, the two other
eigenvalues of the Hessian matrix (related to the diagonal
elements of the replica matrix) can indicate an additional instability to the
SG phase, which enhances when is increased. Therefore, this result
suggests that the study of the replicon can not be enough to guarantee the RS
stability in the present quantum FISG model, especially near the quantum
critical point. In particular, the FISG model allows changing the occupation
number of sites, so one can get a first order transition when the chemical
potential exceeds a certain value. In this region, the replicon and the
indicate instability problems for the SG solution close to all
range of first order boundary.Comment: 15 pages, 4 figures, accepted in Physica
The impact of the metabotropic glutamate receptor and other gene family interaction networks on autism
Although multiple reports show that defective genetic networks underlie the aetiology of autism, few have translated into pharmacotherapeutic opportunities. Since drugs compete with endogenous small molecules for protein binding, many successful drugs target large gene families with multiple drug binding sites. Here we search for defective gene family interaction networks (GFINs) in 6,742 patients with the ASDs relative to 12,544 neurologically normal controls, to find potentially druggable genetic targets. We find significant enrichment of structural defects (P≤2.40E-09, 1.8-fold enrichment) in the metabotropic glutamate receptor (GRM) GFIN, previously observed to impact attention deficit hyperactivity disorder (ADHD) and schizophrenia. Also, the MXD-MYC-MAX network of genes, previously implicated in cancer, is significantly enriched (P≤3.83E-23, 2.5-fold enrichment), as is the calmodulin 1 (CALM1) gene interaction network (P≤4.16E-04, 14.4-fold enrichment), which regulates voltage-independent calcium-activated action potentials at the neuronal synapse. We find that multiple defective gene family interactions underlie autism, presenting new translational opportunities to explore for therapeutic interventions
Study of the lineshape of the chi(c1) (3872) state
A study of the lineshape of the chi(c1) (3872) state is made using a data sample corresponding to an integrated luminosity of 3 fb(-1) collected in pp collisions at center-of-mass energies of 7 and 8 TeV with the LHCb detector. Candidate chi(c1)(3872) and psi(2S) mesons from b-hadron decays are selected in the J/psi pi(+)pi(-) decay mode. Describing the lineshape with a Breit-Wigner function, the mass splitting between the chi(c1 )(3872) and psi(2S) states, Delta m, and the width of the chi(c1 )(3872) state, Gamma(Bw), are determined to be (Delta m=185.598 +/- 0.067 +/- 0.068 Mev,)(Gamma BW=1.39 +/- 0.24 +/- 0.10 Mev,) where the first uncertainty is statistical and the second systematic. Using a Flatte-inspired model, the mode and full width at half maximum of the lineshape are determined to be (mode=3871.69+0.00+0.05 MeV.)(FWHM=0.22-0.04+0.13+0.07+0.11-0.06-0.13 MeV, ) An investigation of the analytic structure of the Flatte amplitude reveals a pole structure, which is compatible with a quasibound D-0(D) over bar*(0) state but a quasivirtual state is still allowed at the level of 2 standard deviations
Measurement of the CKM angle in and decays with
A measurement of -violating observables is performed using the decays
and , where the meson is
reconstructed in one of the self-conjugate three-body final states and (commonly denoted ). The decays are analysed in bins of the -decay phase space, leading
to a measurement that is independent of the modelling of the -decay
amplitude. The observables are interpreted in terms of the CKM angle .
Using a data sample corresponding to an integrated luminosity of
collected in proton-proton collisions at centre-of-mass
energies of , , and with the LHCb experiment,
is measured to be . The hadronic
parameters , , , and ,
which are the ratios and strong-phase differences of the suppressed and
favoured decays, are also reported
Study of the doubly charmed tetraquark T+cc
Quantum chromodynamics, the theory of the strong force, describes interactions of coloured quarks and gluons and the formation of hadronic matter. Conventional hadronic matter consists of baryons and mesons made of three quarks and quark-antiquark pairs, respectively. Particles with an alternative quark content are known as exotic states. Here a study is reported of an exotic narrow state in the D0D0π+ mass spectrum just below the D*+D0 mass threshold produced in proton-proton collisions collected with the LHCb detector at the Large Hadron Collider. The state is consistent with the ground isoscalar T+cc tetraquark with a quark content of ccu⎯⎯⎯d⎯⎯⎯ and spin-parity quantum numbers JP = 1+. Study of the DD mass spectra disfavours interpretation of the resonance as the isovector state. The decay structure via intermediate off-shell D*+ mesons is consistent with the observed D0π+ mass distribution. To analyse the mass of the resonance and its coupling to the D*D system, a dedicated model is developed under the assumption of an isoscalar axial-vector T+cc state decaying to the D*D channel. Using this model, resonance parameters including the pole position, scattering length, effective range and compositeness are determined to reveal important information about the nature of the T+cc state. In addition, an unexpected dependence of the production rate on track multiplicity is observed
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