1,212 research outputs found
Next-to-leading power threshold effects for inclusive and exclusive processes with final state jets
Charge and spin inhomogeneous phases in the Ferromagnetic Kondo Lattice Model
We study numerically the one-dimensional ferromagnetic Kondo lattice. This
model is widely used to describe nickel and manganese perovskites. Due to the
competition between double and super-exchange, we find a region where the
formation of magnetic polarons induces a charge-ordered state. This ordering is
present even in the absence of any inter-site Coulomb repulsion. There is an
insulating gap associated to the charge structure formation. We also study the
insulator-metal transition induced by a magnetic field which removes
simultaneously both charge and spin ordering.Comment: 7 pages, 11 figure
On next-to-eikonal exponentiation
The eikonal approximation is at the heart of many theoretical and
phenomenological studies involving multiple soft gauge boson emissions in high
energy physics. We describe our efforts towards the extension of the eikonal
approximation for scattering amplitudes to the first subleading power in the
soft momentum.Comment: Proc. of "Loops and Legs in Quantum Field Theory", April, 2010,
W\"orlitz, German
Next-to-leading BFKL phenomenology of forward-jet cross sections at HERA
We show that the forward-jet measurements performed at HERA allow for a
detailed study of corrections due to next-to-leading logarithms (NLL) in the
Balitsky-Fadin-Kuraev-Lipatov (BFKL) approach. While the description of the
d\sigma/dx data shows small sensitivity to NLL-BFKL corrections, these can be
tested by the triple differential cross section d\sigma/dxdk_T^2dQ^2 recently
measured. These data can be successfully described using a
renormalization-group improved NLL kernel while the standard
next-to-leading-order QCD or leading-logarithm BFKL approaches fail to describe
the same data in the whole kinematic range. We present a detailed analysis of
the NLL scheme and renormalization-scale dependences and also discuss the
photon impact factors.Comment: 15 pages, 9 figures, new title, NLL-BFKL saddle-point approximation
replaced by exact integratio
Pairing Correlations in a Generalized Hubbard Model for the Cuprates
Using numerical diagonalization of a 4x4 cluster, we calculate on-site s,
extended s and d pairing correlation functions (PCF) in an effective
generalized Hubbard model for the cuprates, with nearest-neighbor correlated
hopping and next nearest-neighbor hopping t'. The vertex contributions (VC) to
the PCF are significantly enhanced, relative to the t-t'-U model. The behavior
of the PCF and their VC, and signatures of anomalous flux quantization,
indicate superconductivity in the d-wave channel for moderate doping and in the
s-wave channel for high doping and small U.Comment: 5 pages, 5 figure
Photoemission Spectroscopy from Inhomogeneous Models of Cuprates
We investigate the electronic dynamics in the underdoped cuprates focusing on
the effects of one-dimensional charge stripes. We address recent experimental
Angular-Resolved Photoemission Spectra results on
(LaNdSr)CuO. We find that various inhomogeneous
models can account for the distribution of quasiparticle weights close to
momentum and symmetry related points. The observed flat
dispersion region around the same point can only be addressed by
certain classes of those inhomogeneous models which locally break spin
symmetry. Homogeneous models including hopping elements up to second neighbors
cannot reproduce the experimental quasiparticle weight, since most of it is
centered around .Comment: 5 pages, color figure
The one-dimensional Bose-Hubbard Model with nearest-neighbor interaction
We study the one-dimensional Bose-Hubbard model using the Density-Matrix
Renormalization Group (DMRG).For the cases of on-site interactions and
additional nearest-neighbor interactions the phase boundaries of the
Mott-insulators and charge density wave phases are determined. We find a direct
phase transition between the charge density wave phase and the superfluid
phase, and no supersolid or normal phases. In the presence of nearest-neighbor
interaction the charge density wave phase is completely surrounded by a region
in which the effective interactions in the superfluid phase are repulsive. It
is known from Luttinger liquid theory that a single impurity causes the system
to be insulating if the effective interactions are repulsive, and that an even
bigger region of the superfluid phase is driven into a Bose-glass phase by any
finite quenched disorder. We determine the boundaries of both regions in the
phase diagram. The ac-conductivity in the superfluid phase in the attractive
and the repulsive region is calculated, and a big superfluid stiffness is found
in the attractive as well as the repulsive region.Comment: 19 pages, 30 figure
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