2,554 research outputs found
Complex Hyperbolic Surfaces of Abelian Type
2000 Mathematics Subject Classification: 11G15, 11G18, 14H52, 14J25, 32L07.We call a complex (quasiprojective) surface of hyperbolic type,
iff – after removing finitely many points and/or curves – the universal cover
is the complex two-dimensional unit ball. We characterize abelian surfaces
which have a birational transform of hyperbolic type by the existence of a
reduced divisor with only elliptic curve components and maximal singularity
rate (equal to 4). We discover a Picard modular surface of Gauß numbers
of bielliptic type connected with the rational cuboid problem. This paper is
also necessary to understand new constructions of Picard modular forms of
3-divisible weights by special abelian theta functions
Refining Finite-Time Lyapunov Exponent Ridges and the Challenges of Classifying Them
While more rigorous and sophisticated methods for identifying Lagrangian based coherent structures exist, the finite-time Lyapunov exponent (FTLE) field remains a straightforward and popular method for gaining some insight into transport by complex, time-dependent two-dimensional flows. In light of its enduring appeal, and in support of good practice, we begin by investigating the effects of discretization and noise on two numerical approaches for calculating the FTLE field. A practical method to extract and refine FTLE ridges in two-dimensional flows, which builds on previous methods, is then presented. Seeking to better ascertain the role of a FTLE ridge in flow transport, we adapt an existing classification scheme and provide a thorough treatment of the challenges of classifying the types of deformation represented by a FTLE ridge. As a practical demonstration, the methods are applied to an ocean surface velocity field data set generated by a numerical model. (C) 2015 AIP Publishing LLC.ONR N000141210665Center for Nonlinear Dynamic
Initial electron-transfer in the reaction center from Rhodobacter sphaeroides.
The initial electron transfer steps in the photosynthetic reaction center of the purple bacterium Rhodobacter sphaeroides have been investigated by femtosecond time-resolved spectroscopy. The experimental data taken at various wavelengths demonstrate the existence of at least four intermediate states within the first nanosecond. The difference spectra of the intermediates and transient photodichroism data are fully consistent with a sequential four-step model of the primary electron transfer: Light absorption by the special pair P leads to the state P*. From the excited primary donor P*, the electron is transferred within 3.5 +/- 0.4 ps to the accessory bacteriochlorophyll B. State P+B- decays with a time constant of 0.9 +/- 0.3 ps passing the electron to the bacteriopheophytin H. Finally, the electron is transferred from H- to the quinone QA within 220 +/- 40 ps
Doping and critical-temperature dependence of the energy gaps in Ba(Fe_{1-x}Co_x)_2As_2 thin films
The dependence of the superconducting gaps in epitaxial
Ba(Fe_{1-x}Co_{x})_2As_2 thin films on the nominal doping x (0.04 \leq x \leq
0.15) was studied by means of point-contact Andreev-reflection spectroscopy.
The normalized conductance curves were well fitted by using the 2D
Blonder-Tinkham-Klapwijk model with two nodeless, isotropic gaps -- although
the possible presence of gap anisotropies cannot be completely excluded. The
amplitudes of the two gaps \Delta_{S} and \Delta_{L} show similar monotonic
trends as a function of the local critical temperature T_{c}^{A} (measured in
the same point contacts) from 25 K down to 8 K. The dependence of the gaps on x
is well correlated to the trend of the critical temperature, i.e. to the shape
of the superconducting region in the phase diagram. When analyzed within a
simple three-band Eliashberg model, this trend turns out to be compatible with
a mechanism of superconducting coupling mediated by spin fluctuations, whose
characteristic energy scales with T_{c} according to the empirical law
\Omega_{0}= 4.65*k_{B}*T_{c}, and with a total electron-boson coupling strength
\lambda_{tot}= 2.22 for x \leq 0.10 (i.e. up to optimal doping) that slightly
decreases to \lambda_{tot}= 1.82 in the overdoped samples (x = 0.15).Comment: 8 pages, 5 color figure
Resistivity in Co-doped Ba-122: comparison of thin films and single crystals
The temperature dependence of the resistivity of epitaxial
Ba(Fe_(1-x)Co_x)2As2 thin films (with nominal doping x = 0.08, 0.10 and 0.15)
has been analyzed and compared with analogous measurements on single crystals
taken from literature. The rho(T) of thin films looks different from that of
single crystals, even when the cobalt content is the same. All rho(T) curves
can be fitted by considering an effective two-band model (with holes and
electrons bands) in which the electrons are more strongly coupled with the
bosons (spin fluctuations) than holes, while the effect of impurities is mainly
concentrated in the hole band. Within this model the mediating boson has the
same characteristic energy in single crystals and thin films, but the shape of
the transport spectral function at low energy has to be very different, leading
to a "hardening" of the electron-boson spectral function in thin films,
associated with the strain induced by the substrate.Comment: 13 pages, 4 figure
Limits on Arcminute Scale Cosmic Microwave Background Anisotropy with the BIMA Array
We have used the Berkeley-Illinois-Maryland-Association (BIMA) millimeter
array outfitted with sensitive cm-wave receivers to search for Cosmic Microwave
Background (CMB) anisotropies on arcminute scales. The interferometer was
placed in a compact configuration which produces high brightness sensitivity,
while providing discrimination against point sources. Operating at a frequency
of 28.5 GHz, the FWHM primary beam of the instrument is 6.6 arcminutes. We have
made sensitive images of seven fields, five of which where chosen specifically
to have low IR dust contrast and be free of bright radio sources. Additional
observations with the Owens Valley Radio Observatory (OVRO) millimeter array
were used to assist in the location and removal of radio point sources.
Applying a Bayesian analysis to the raw visibility data, we place limits on CMB
anisotropy flat-band power Q_flat = 5.6 (+3.0 -5.6) uK and Q_flat < 14.1 uK at
68% and 95% confidence. The sensitivity of this experiment to flat band power
peaks at a multipole of l = 5470, which corresponds to an angular scale of
approximately 2 arcminutes. The most likely value of Q_flat is similar to the
level of the expected secondary anisotropies.Comment: 15 pages, 5 figures, LaTex, aas2pp4.sty, ApJ submitte
The Effect of 45{\deg} Grain Boundaries and associated Fe particles on Jc and resistivity in Ba(Fe0.9Co0.1)2As2 Thin Films
The anisotropy of the critical current density Jc depends in general on both
the properties of the flux lines (such as line tension, coherence length and
penetration depth) and the properties of the defects (such as density, shape,
orientation etc.). Whereas the Jc anisotropy in microstructurally clean films
can be scaled to an effective magnetic field containing the Ginzburg-Landau
anisotropy term, it is in general not possible (or only in a limited field
range) for samples containing extended defects. Here, the Jc anisotropy of a
Co-doped BaFe2As2 sample with 45{\deg} [001] tilt grain boundaries (GBs), i.e.
grain boundaries created by 45{\deg} in-plane rotated grains, as well as
extended Fe particles is investigated. This microstructure leads to c-axis
correlated pinning, both due to the GBs and the Fe particles and manifests in a
c-axis peak in the Jc anisotropy at low magnetic fields and a deviation from
the anisotropic Ginzburg-Landau scaling at higher fields. Strong pinning at
ellipsoidal extended defects, i.e. the Fe particles, is discussed, and the full
Jc anisotropy is fitted successfully with the vortex path model. The results
are compared to a sample without GBs and Fe particles. 45{\deg} GBs seem to be
good pinning centers rather than detrimental to current flow.Comment: 8 pages, 7 figures, CEC-ICMC 2013 proceeding, accepted for
publication in Advances in Cryogenic Engineering (Materials
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