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Resources allocated to tackling the tax gap: a comparative EU study
Since the onset of the global financial crisis in 2008 and the development of austerity as a widespread economic strategy there has been continuing focus on the tax gap as an issue, which is the difference between the amount of tax that should, theoretically, be collected by a tax authority within the prevailing system that a tax jurisdiction has legislated for and the actual amount of tax collected. The efficiency, or otherwise, of a tax authority in tackling the tax gap has come to be seen as a measure of its effectiveness in raising revenue, whether to balance budgets or fund additional government spending. Despite this, relatively little formal attention has been given to technical dimensions of the tax gap, or to the link between that tax gap and tax authority spending. We have sought to address these last issues. In the process we have appraised the quality of the data available for this process, including whether available GDP data is reliable as a basis for estimation; whether data on tax collected is comparable and whether available data on tax authority spending is appropriate for this purpose. Data on estimates of the shadow economy have also been appraised as a consequence. Whilst it has proved possible to prepare new estimates of the tax gap for EU member states limitations in the resulting estimates are highlighted. In addition, weaknesses in all other data sources are noted, and their suitability is questioned. The resulting analysis of tax authority expenditure and its relationship to the tax gap is, consequently, heavily constrained, but in any event no apparent statistical association is noted. It is suggested that other approaches to the 2 management of the tax, and the effectiveness of tax authorities, are required, with a recommendation that tax spillover assessments be considered as an alternative
Technical note: Simulating chemical systems in Fortran90 and Matlab with the Kinetic PreProcessor KPP-2.1
International audienceThis paper presents the new version 2.1 of the Kinetic PreProcessor (KPP). Taking a set of chemical reactions and their rate coefficients as input, KPP generates Fortran90, Fortran77, Matlab, or C code for the temporal integration of the kinetic system. Efficiency is obtained by carefully exploiting the sparsity structures of the Jacobian and of the Hessian. A comprehensive suite of stiff numerical integrators is also provided. Moreover, KPP can be used to generate the tangent linear model, as well as the continuous and discrete adjoint models of the chemical system
Exact and Asymptotic Measures of Multipartite Pure State Entanglement
In an effort to simplify the classification of pure entangled states of multi
(m) -partite quantum systems, we study exactly and asymptotically (in n)
reversible transformations among n'th tensor powers of such states (ie n copies
of the state shared among the same m parties) under local quantum operations
and classical communication (LOCC). With regard to exact transformations, we
show that two states whose 1-party entropies agree are either locally-unitarily
(LU) equivalent or else LOCC-incomparable. In particular we show that two
tripartite Greenberger-Horne-Zeilinger (GHZ) states are LOCC-incomparable to
three bipartite Einstein-Podolsky-Rosen (EPR) states symmetrically shared among
the three parties. Asymptotic transformations result in a simpler
classification than exact transformations. We show that m-partite pure states
having an m-way Schmidt decomposition are simply parameterizable, with the
partial entropy across any nontrivial partition representing the number of
standard ``Cat'' states (|0^m>+|1^m>) asymptotically interconvertible to the
state in question. For general m-partite states, partial entropies across
different partitions need not be equal, and since partial entropies are
conserved by asymptotically reversible LOCC operations, a multicomponent
entanglement measure is needed, with each scalar component representing a
different kind of entanglement, not asymptotically interconvertible to the
other kinds. In particular the m=4 Cat state is not isentropic to, and
therefore not asymptotically interconvertible to, any combination of bipartite
and tripartite states shared among the four parties. Thus, although the m=4 cat
state can be prepared from bipartite EPR states, the preparation process is
necessarily irreversible, and remains so even asymptotically.Comment: 13 pages including 3 PostScript figures. v3 has updated references
and discussion, to appear Phys. Rev.
Optical matrix elements in tight-binding models with overlap
We investigate the effect of orbital overlap on optical matrix elements in
empirical tight-binding models. Empirical tight-binding models assume an
orthogonal basis of (atomiclike) states and a diagonal coordinate operator
which neglects the intra-atomic part. It is shown that, starting with an atomic
basis which is not orthogonal, the orthogonalization process induces
intra-atomic matrix elements of the coordinate operator and extends the range
of the effective Hamiltonian. We analyze simple tight-binding models and show
that non-orthogonality plays an important role in optical matrix elements. In
addition, the procedure gives formal justification to the nearest-neighbor
spin-orbit interaction introduced by Boykin [Phys. Rev \textbf{B} 57, 1620
(1998)] in order to describe the Dresselahaus term which is neglected in
empirical tight-binding models.Comment: 16 pages 6 figures, to appear in Phys. Rev.
Parallel Load Balancing Strategies for Ensembles of Stochastic Biochemical Simulations
The evolution of biochemical systems where some chemical species are present with only a small number of molecules, is strongly influenced by discrete and stochastic effects that cannot be accurately captured by continuous and deterministic models. The budding yeast cell cycle provides an excellent example of the need to account for stochastic effects in biochemical reactions. To obtain statistics of the cell cycle progression, a stochastic simulation algorithm must be run thousands of times with different initial conditions and parameter values. In order to manage the computational expense involved, the large ensemble of runs needs to be executed in parallel. The CPU time for each individual task is unknown before execution, so a simple strategy of assigning an equal number of tasks per processor can lead to considerable work imbalances and loss of parallel efficiency. Moreover, deterministic analysis approaches are ill suited for assessing the effectiveness of load balancing algorithms in this context. Biological models often require stochastic simulation. Since generating an ensemble of simulation results is computationally intensive, it is important to make efficient use of computer resources. This paper presents a new probabilistic framework to analyze the performance of dynamic load balancing algorithms when applied to large ensembles of stochastic biochemical simulations. Two particular load balancing strategies (point-to-point and all-redistribution) are discussed in detail. Simulation results with a stochastic budding yeast cell cycle model confirm the theoretical analysis. While this work is motivated by cell cycle modeling, the proposed analysis framework is general and can be directly applied to any ensemble simulation of biological systems where many tasks are mapped onto each processor, and where the individual compute times vary considerably among tasks
Violations of local realism by two entangled quNits
Results obtained in two recent papers, \cite{Kaszlikowski} and \cite{Durt},
seem to indicate that the nonlocal character of the correlations between the
outcomes of measurements performed on entangled systems separated in space is
not robust in the presence of noise. This is surprising, since entanglement
itself is robust. Here we revisit this problem and argue that the class of
gedanken-experiments considered in \cite{Kaszlikowski} and \cite{Durt} is too
restrictive. By considering a more general class, involving sequences of
measurements, we prove that the nonlocal correlations are in fact robust.Comment: Reference added, 3 pages, accepted for publication in J. Phys. A:
Math. and Genera
Anisotropic magnetoresistance of bulk carbon nanotube sheets
We have measured the magnetoresistance of stretched sheets of carbon
nanotubes in temperatures ranging from 2 K to 300 K and in magnetic fields up
to 9 T, oriented either perpendicular or parallel to the plane of the sheets.
The samples have been partially aligned by post-fabrication stretching, such
that the direction of stretching was either parallel or perpendicular to the
direction of applied electric current. We have observed large differences
between the magnetoresistance measured under the two field orientations, most
pronounced at the lowest temperatures, highest fields, and for the
laterally-aligned sample. Treatment of the sheets with nitric acid affects this
anisotropy. We analyzed the results within the theoretical framework of weak
and strong localization and concluded that the anisotropy bears the mark of a
more unusual phenomenon, possibly magnetically-induced mechanical strain.Comment: 34 pages, 10 figure
High Temperature Mixed State Axis Dissipation in Low Carrier Density
The nature of the out-of-plane dissipation was investigated in underdoped
single crystals at temperatures
close to the critical temperature. For this goal, temperature and angle
dependent out-of-plane resistivity measurements were carried out both below and
above the critical temperature. We found that the Ambegaokar-Halperin
relationship [V. Ambegaokar, and B. I. Halperin, Phys. Rev. Lett. \textbf{22},
1364 (1969)] depicts very well the angular magnetoresistivity in the
investigated range of field and temperature. The main finding is that the
in-plane phase fluctuations decouple the layers above the critical temperature
and the charge transport is governed only by the quasiparticles. We also have
calculated the interlayer Josephson critical current density, which was found
to be much smaller than the one predicted by the theory of layered
superconductors. This discrepancy could be a result of the d-wave symmetry of
the order parameter and/or of the non BCS temperature dependence of the c-axis
penetration length.Comment: Will appear in PR
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