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text:
Man arrested after drunken chase ends with crash in Portsmouth, police say
Robert Hanlin faces charges
Updated: 11:09 AM EDT Jul 13, 2016
Frank O'Laughlin
A police chase along New Hampshire's seacoast Tuesday night ended with a crash involving a drunk driver, a foot pursuit and an arrest, officials said.The chase started on Route 33 eastbound in Greenland after Stratham police issued an alert to be on the lookout for an erratic driver with New York license plates.Police said officers chased Robert Hanlin, 41, of Alexander, New York. They said one cruiser pulled in front of Hanlin in an attempt to halt the pursuit, but he rammed into the vehicle and sped off at a high rate of speed.A Greenland officer continued to chase Hanlin as he entered Portsmouth, police said. The crash came to an end when he slammed into a tree at the intersection of Middle and Spinney streets in front of North Church.Hanlin left his vehicle and fled the scene on foot, ducking behind houses in the area, according to police. He was tracked down and arrested after a brief pursuit.He is charged with disobeying an officer, reckless operation, aggravated driving while intoxicated, and conduct after an accident.Additional charges could be filed pending an investigation.Get the WMUR app
PORTSMOUTH, N.H. —
A police chase along New Hampshire's seacoast Tuesday night ended with a crash involving a drunk driver, a foot pursuit and an arrest, officials said.
The chase started on Route 33 eastbound in Greenland after Stratham police issued an alert to be on the lookout for an erratic driver with New York license plates.
Police said officers chased Robert Hanlin, 41, of Alexander, New York. They said one cruiser pulled in front of Hanlin in an attempt to halt the pursuit, but he rammed into the vehicle and sped off at a high rate of speed.
A Greenland officer continued to chase Hanlin as he entered Portsmouth, police said. The crash came to an end when he slammed into a tree at the intersection of Middle and Spinney streets in front of North Church.
Hanlin left his vehicle and fled the scene on foot, ducking behind houses in the area, according to police. He was tracked down and arrested after a brief pursuit.
He is charged with disobeying an officer, reckless operation, aggravated driving while intoxicated, and conduct after an accident.
Additional charges could be filed pending an investigation.

redpajama_set_name: RedPajamaCommonCrawl


The children arrive in the morning around 8.45 - 9:00. They have the opportunity then to prepare for their day of work ahead: they must get themselves ready in the classroom, organise their morning snack and lunch. They can then begin working, either work of their own choice or a presentation from the teacher.
In the morning there is a work cycle of three hours, allowing the children to have long periods of work and concentration. During these three hours the child can take a break at any time to drink, eat their snack and go to the bathroom.
Around 12:00 the children put away their work and prepare for lunch, they organise and clean the classroom and set the table for eating. After tidying we all sit down and eat together. Once the children have finished eating they clear their tables and their placemats, then they will be free to play until 1:30pm.
At 1:30pm all students return to the classroom and continue working until 4pm and then they return home.


text:
\section{Introduction}
\label{sec:intro}

The Similarity Renormalization Group (SRG) uses a continuous
series of unitary
transformations to decouple high-momentum and low-momentum physics
in an input Hamiltonian~\cite{Glazek:1993rc,Wegner:1994}.
This decoupling means that expansions of physical observables
generally become more convergent.
The SRG can be implemented through a flow equation for the evolving
Hamiltonian $H_s$,
\beq
  \frac{dH_s}{ds} = [ \eta_s, H_s ] = [ [ G_s, H_s ], H_s ]
  \;,
  \label{eq:srgflow}
\eeq
where $s$ is a flow parameter~\cite{Wegner:1994,Kehrein:2006} and
the generator $\eta_s$ is specified by the operator $G_s$.
With $G_s$ chosen to be
the relative kinetic energy $\Trelfull$, the SRG
has been applied successfully over the past few years to calculate
nuclear structure and reactions~\cite{Bogner:2006pc,Bogner:2007rx,Jurgenson:2009qs,Hebeler:2010xb,Bogner:2009bt,
Navratil:2010jn,Navratil:2010ey,Jurgenson:2010wy,Hergert:2011eh}.  However, different choices for $G_s$ will give rise to different  patterns of evolution, which may be advantageous.
In this paper, two alternatives to $\Trelfull$ are evaluated for their effectiveness in decoupling and, in particular, for improvements in computing speed (see Fig.~\ref{fig:time1} for a representative example).
Our tests are for realistic nucleon-nucleon (NN) interactions in two-body
systems and for a one-dimensional model Hamiltonian applied to
few-body bound states.

\begin{figure}[tb]
  \includegraphics[width=.9\columnwidth]{novel_time_1_v2_fig1}
  \vspace*{-.1in}
  \caption{(Color online) Computational time to evolve the Argonne $v_{18}$ $^1$S$_0$
  potential~\cite{Wiringa:1994wb}
  as a function of the final value of $\lambdaequiv$ (see text) for
  several generators, with $\sigma = 2\,\fmi$ for
  $G_s^{\rm inv}$ and $G_s^{\rm exp}$.}
  \label{fig:time1}
\end{figure}

We focus on novel generators that have $G_s$ as functions of $\Trelfull$.  (Note: we can just as well consider the full kinetic energy
$T$ in our discussion, because the center-of-mass part commutes with the
running Hamiltonian $H_s$, so we will use $T$ for convenience.)
In particular, we explore the ``inverse'' $G_s$ operator
\beq
G_s = -\frac{\sigma^2}{1 + \Trel/\sigma^2} \equiv G_s^{\rm inv}
  \;,
  \label{eq:invgen}
\eeq
and the ``exponential'' $G_s$ given by
\beq
 G_s = -\sigma^2 e^{-\Trel/\sigma^2} \equiv G_s^{\rm exp}
 \;.
   \label{eq:expgen}
\eeq
Each has a Taylor series that  reduces to $\Trel$ (up to a constant,
which drops out from the commutator)
at low momentum or when \(\sigma\) is large.  As such, the independent parameter $\sigma$ controls the
separation of a low-energy region where $G_s$ behaves as
$T$ and the potential is driven toward the diagonal, and a high-energy region where evolution is suppressed.   This suppression can result in a significant computational speedup of the
SRG evolution when compared to calculations with \(G_{s}=\Trel\), while not impacting the advantageous properties of the evolution for low-momentum
applications.

The generators' suppression of running in unneeded parts of the Hamiltonian could mitigate the difficulties
of evolving  very large matrices for calculations of light
atomic nuclei~\cite{Jurgenson:2010wy}, opening the door to more
tailored SRG generators and more effective evolution of three- and eventually
four-body interactions.
Even at the two-body level there are problems when trying to evolve
to large values of the flow parameter $s$.
A recent example is a study of SRG decoupling with large-cutoff effective
field theory (EFT) potentials, which require evolution beyond the range usually
considered~\cite{Wendt:2011qj}.  In doing so, the SRG differential equations can become extremely stiff and take a prohibitively long time (weeks on a single processor) to evolve.
This problem has hindered exploratory studies
into issues such as what happens when a chiral EFT is
evolved to the regime of pionless EFT.

In Sec.~\ref{sec:NN},
we give representative results for applications to two-body
systems, including an analysis of the flow pattern.
These results are extended to few-body systems in Sec.~\ref{sec:oneD}
using a model one-dimensional Hamiltonian that has proved useful
in past applications~\cite{Jurgenson:2008jp,Anderson:2010aq}.
We summarize and outline future studies
in Sec.~\ref{sec:summary}.

\section{Two-nucleon systems}\label{sec:NN}

In this section we give representative results for evolving
realistic nucleon-nucleon potentials
using the novel generators from Eqs.~\eqref{eq:invgen} and \eqref{eq:expgen}
in comparison to the usual
choice of $G_s = \Trel$.

\subsection{Performance}

The key advantage of the generators that we highlight is the improvement in computational performance.  For example, the time needed to evolve the Argonne $v_{18}$ $^1$S$_0$ potential~\cite{Wiringa:1994wb} to equivalent levels of decoupling with several generators is plotted in Fig.~\ref{fig:time1}.    The parameter $\lambda \equiv 1/s^{1/4}$, which has dimensions of a
momentum,  has been used to identify the momentum decoupling scale.
However,
different generators will evolve a given potential at different rates, so
comparing results with the same definition of $\lambda$ can be misleading.
Therefore, we identify an ``equivalent'' $\lambdaequiv$ for each generator
that equalizes the degree of decoupling compared to $G_s = T$ (for which \(\lambdaequiv=\lambda\) by definition); the details are described
in Sec.~\ref{subsec:decoupling}.

The value of \(\sigma\) will also have an impact, as discussed below; in Fig.~\ref{fig:time1} we use the intermediate value \(\sigma=2\fmi\). With this choice, there is nearly an order of magnitude difference in the time to evolve the Argonne
$v_{18}$ potential with  \(\GsExp\) and \(\GsInv\) compared to \(G_s=\Trel\) at \(\lambdaequiv=4\fmi\) and two orders of magnitude by \(\lambdaequiv=2\fmi\).
Note that nuclear interactions typically have been evolved for nuclear structure studies in the range $\lambda=1.5$--$2.2\fmi$.
The speed gains will depend on the initial potential and can be
much less for the evolution of softer initial potentials; e.g., for the
N$^3$LO 500\,MeV chiral EFT potential of Ref.~\cite{Entem:2003ft}, evolving
with $\GsExp$ to $\lambdaequiv = 2\fmi$ is about 1.5 times as fast as
with $G_s = \Trel$ and about 3 times as fast to $\lambdaequiv = 1.5\fmi$.

The numerical solution of the SRG evolution equations requires repeated dense
matrix-matrix multiplications.  As a consequence, the evolution has been carried
out on shared-memory computer architectures.  Recent calculations  using the SRG
with many-body forces are approaching the limits of what is practical  to evolve
in  memory on a single node because of the size of the model space needed
\cite{Jurgenson:2010wy}.  A distributed scheme to solve the equations  would
permit larger model spaces to be utilized; however, the dense matrix
multiplication would then be limited by internode communication times.   The
reduced number of operations required by novel generators might help make
such a scheme possible.

\begin{figure}[b]
 \includegraphics[width=.9\columnwidth]{equiv_lambda_phase_v3_fig2}
 \caption{(Color online) Deviation of phase shifts calculated with the Argonne $v_{18}$ $^1$S$_0$ potential~\cite{Wiringa:1994wb} evolved
 with $G_s = T$ and  $G_s^{\rm exp}$ ($\sigma = 2\,\fmi$) to various
 $\lambda$ values and then
truncated at $\kcut = 2\,\fmi$ to test decoupling.
Phase shifts from untruncated potentials agree precisely with those from the initial potential.}
 \label{fig:phaseequiv}
\end{figure}

\begin{figure*}[tbh!]
   \subfigure[]{\includegraphics[width=0.7\textwidth]{novel_Trel2_fig3a}}
  \subfigure[]{\includegraphics[width=0.7\textwidth]{novel_invT2_fig3b}}
  \subfigure[]{\includegraphics[width=0.7\textwidth]{novel_expT2_fig3c}}
  \vspace*{-.1in}
  \caption{(Color online) Contour plots showing the evolution via
  Eq.~\eqref{eq:srgflow} at several values of $\lambdaequiv $
  starting from the momentum-space Argonne $v_{18}$ $^1$S$_0$ potential~\cite{Wiringa:1994wb}
  using  (a) $G_s = \Trel$, (b) $G_s^{\rm inv}$ from Eq.~\eqref{eq:invgen} with $\sigma = 2\,\fmi$, and (c) $G_s^{\rm exp}$ from Eq.~\eqref{eq:expgen} with $\sigma = 2\,\fmi$.\\ }
  \label{fig:evolveAll}
\end{figure*}

\subsection{Decoupling and $\lambdaequiv$}\label{subsec:decoupling}

To validate the apparent computational advantages of these generators, one must confirm that the decoupling characteristics of the  $G_s = T$  generator are also reproduced, so that  calculations of physical observables also become more convergent. However, if we evolve to the same $\lambda$, the
degree of decoupling for identical initial potentials differs
for  \(\GsExp\)  and \(\GsInv\) compared to   $G_s = T$.
These differences are evident in the deviations of $^1$S$_0$
phase shifts calculated from the evolved potentials using   \(\GsExp\)  and  $G_s = T$  from the unevolved potential shown in Fig.~\ref{fig:phaseequiv} for several different \(\lambda\) values (only $\GsExp$ is shown; \(\GsInv\) behaves similarly).
If the full potentials were used, the phase shifts would agree -- up to numerical precision -- with those from the initial potential, because the evolution
in all cases is unitary.
However, the degree of decoupling for a given value of $\lambda$
can be made manifest by first cutting off
the potential  (that is, setting its matrix elements to zero)
above some value of $k$ and then calculating the phase shifts.
In Fig.~\ref{fig:phaseequiv}, for
illustration, we choose the cutoff value $\kcut$ to be $2\fmi$.
The signature of decoupling is that the phase shifts agree at lower energies
and only deviate close to and above the cutoff.
This is typically observed when the potential is evolved
so that $\lambda$ is less than the cut momentum~\cite{Jurgenson:2007td,Bogner:2007jb}.

This behavior provides us with a pragmatic way to define $\lambdaequiv$: identifying it with the decoupling behavior that is found for $G_s = T$
for a given $\lambda$.
We use the results in Fig.~\ref{fig:phaseequiv} to illustrate the
procedure.
The continuous curve shows the deviation of phase shifts for the potential evolved with $G_s = T$ to $\lambda = 2\,\fmi$ and cut at $k = 2\,\fmi$.
As expected from decoupling, the deviation is small
up to roughly $\kcut$.
We use this level of agreement as the criterion for identifying equivalent $\lambda$'s for other generators. That is, a potential is evolved to a series of $\lambda$ values with a different $G_s$ and then cut at $\kcut$ after evolution. The phase shifts are then compared to the level of decoupling observed for  $G_s = T$ at  $\kcut = \lambda$.  The approximate point in the novel $G_s$ evolution for which the cut phase shifts agree is equated with $\lambdaequiv$.
Consider the phase shifts for the potential evolved with $G_s^{\rm exp}$ to several values of $\lambda$ and cut at $k = 2\,\fmi$, as shown in Fig.~\ref{fig:phaseequiv}. For $G_s^{\rm exp}$, $\lambda$ evolved to $1.5\,\fmi$ gives a similar degree of decoupling as $\lambda$ evolved to $2\,\fmi$ with $G_s = T$.  As a result, we define $\lambda = 1.5\,\fmi$ to be the $\lambdaequiv = 2\,\fmi$ for $G_s^{\rm exp}$.
We use $\lambdaequiv$ for most comparisons in the following discussion.

\subsection{Flow Analysis}

Having chosen a working definition for the decoupling scale of evolution with  our novel generators, we take a closer look at the properties of the evolved potentials. In particular, we would like to see how a potential flows with evolution using these generators compared to \(G_s=\Trel\) and to understand how the choice of \(\sigma\) affects this flow.

\begin{figure*}[tbh]
 \includegraphics[width=0.75\textwidth]{diag_novel_generator_v3_fig4}
 \caption{(Color online) Diagonal (a) and off-diagonal (b) momentum-space matrix elements for evolved
 Argonne $v_{18}$ $^1$S$_0$ potential~\cite{Wiringa:1994wb} with $G_s = T$ and generators $G_s^{\rm exp}$ and $G_s^{\rm inv}$ at  \(\lambda=2\fmi\) with $\sigma = 2\,\fmi.$}
 \label{fig:universalitygenerator}
\end{figure*}

\begin{figure*}[tbh!]
 \includegraphics[width=0.75\textwidth]{diag_different_sigma_v3_fig5}
 \caption{(Color online) Diagonal (a) and off-diagonal (b) momentum-space matrix elements for evolved
 Argonne $v_{18}$ $^1$S$_0$ potential~\cite{Wiringa:1994wb} with $G_s = T$ and $G_s^{\rm exp}$ with different values of $\sigma$ each evolved  to \(\lambda=2\fmi\). The lines with $\sigma = 3\,\fmi$ are indistinguishable from the ones with $G_s = T$.}
 \label{fig:universalityexp}
\end{figure*}

\begin{figure*}[tbh]
  \subfigure[]{\includegraphics[width=0.26\textwidth]{original_1S0_kvnn_10_fig6a}}
  \hspace*{.2in}
  \subfigure[]{\includegraphics[width=0.55\textwidth]{novel_1S0_kvnn_10_fig6b}}
 \caption{(Color online) (a) Unevolved N$^3$LO 500 MeV  $^1$S$_0$ potential . (b)  Contour plot showing the evolved N$^3$LO $^1$S$_0$ potential with different generators to \(\lambdaequiv=2\fmi\).  For  $G_s^{\rm exp}$ and $G_s^{\rm inv}$,  \(\sigma=2\fmi.\)\\  }
 \label{fig:evolveN3LO}
\end{figure*}

In Fig.~\ref{fig:evolveAll}
we compare the evolution pattern of the two-body potential in the
$^1$S$_0$ channel with different generators.  Each frame is a representation of the potential matrices in momentum space; where the matrix is zero, there is no coupling between momentum components.
The initial potential in all cases is Argonne $v_{18}$~\cite{Wiringa:1994wb} and the
value of $\sigma$ is taken to be $2\,\fmi$.  Note that at \(\lambda=4\fmi\), the first matrix plotted here, there is already significant evolution. As the potential is evolved, its high and low momentum components become increasingly decoupled, as expected.
It is evident that the evolved potentials are similar (but not
identical) in the region where $k^2,k'{}^2 < \sigma^2$. When \(\lambda<\sigma\) we find that \(\sigma\) roughly defines the low-momentum region where these generators behave as
$G_{s}=\Trel$.    The minor differences in this low-momentum region can be attributed to the fact that the point in  evolution, \(\lambda\),  needed for these generators to reach the corresponding \(\lambdaequiv\) occurs when  \(\lambda<\lambdaequiv\).  At higher momenta, novel generator evolution is suppressed  relative to $G_{s}=\Trel$.  The patterns here are characteristic of the particular generator and are similar for other potentials and in other channels.

This nature of the evolution is further illustrated by the plots in Figs.~\ref{fig:universalitygenerator} and \ref{fig:universalityexp}, which  show a detailed view of the diagonal and off-diagonal values of the matrices at low momentum for each generator applied to the Argonne $v_{18}$ $^1$S$_0$ potential
. The flow parameter was run to \(\lambda=2\fmi\) with the generators here to distinguish between ambiguities caused by using \(\lambdaequiv\). In Fig.~\ref{fig:universalitygenerator},  the values from different generators agree quite well for $k < \sigma$, where \(\sigma\approx\lambda\).  Moreover, we see that the minor  ``pincushion" effect seen in Fig.~\ref{fig:evolveAll}
  for these generators relative to $G_s = T$  is indeed an artifact of using \(\lambdaequiv\), as each curve falls to zero at approximately the same time.  In  Fig.~\ref{fig:universalityexp}  we focus on \(\GsExp\) versus $G_s = T$ and the fact that they differ for \(\sigma\leq\lambda\).  However, as \(\sigma\rightarrow\lambda\) it is evident that the evolution of the novel generator becomes increasingly similar to  $G_s = T$ in the low-momentum region \(k<\lambda\). For  larger values of \(\sigma,\) these generators become indistinguishable from $G_s = T$.

\begin{figure}[tb]
  \includegraphics[width=\columnwidth]{first_term_different_generator_v2_fig7}
  \caption{(Color online) Color contour plots of the first term (excluding the factor due to \(V_{s}\)) on the right side of
  Eq.~\eqref{eq:PWflow}
  for $G_s = \Trel$ (left), $G_s^{\rm inv}$ (middle), and
   $G_s^{\rm exp}$ (right).
  The last two use $\sigma = 2 \fmi$.}
  \label{fig:first_term}
\end{figure}

\begin{figure}[tb]
  \includegraphics[width=\columnwidth]{first_term_different_sigma_v2_fig8}
  \caption{(Color online) Color contour plots of the first terms
  (excluding the factor due to \(V_{s}\)) on the
right side of Eq.~\eqref{eq:PWflow} for $G_s^{\rm exp}$ with
$\sigma = 1, 2,$ and $3 \fmi $ from left to right.}
  \label{fig:Gs_first_term}
\end{figure}

\begin{figure*}[tbh!]
 \includegraphics[width=.8\textwidth]{novel_exp_different_sigma_fig9}
 \caption{(Color online) Contour plot showing the evolution to  \(\lambdaequiv=2\fmi\) via
  Eq.~\eqref{eq:srgflow}
  starting from the momentum-space Argonne $v_{18}$ $^1$S$_0$ potential~\cite{Wiringa:1994wb}
  using $G_s^{\rm exp}$ from Eq.~\eqref{eq:expgen} with different values of $\sigma$.\\ }
 \label{fig:evolvesigma}
\end{figure*}

\begin{figure}[tb!]
  \includegraphics[width=.9\columnwidth]{novel_time_2_v2_fig10}
  \caption{(Color online) Computational time to evolve the Argonne $v_{18}$ $^1$S$_0$ potential~\cite{Wiringa:1994wb}
  with $G_{s}=T$ and \(\GsExp\) to \(\lambdaequiv=2\fmi\)
   as a function of the value of $\sigma$. }
  \label{fig:time2}
\end{figure}

As a demonstration of similar behavior for different NN potentials,
an evolved potential with different generators
in the $^1$S$_0$   channel of the N$^3$LO 500 MeV potential~\cite{Entem:2003ft} is shown in Fig.~\ref{fig:evolveN3LO}. Note that the initial potential has significantly less coupling at high momentum compared to
Argonne $v_{18}$~\cite{Bogner:2009bt}.  As a result, there is correspondingly less improvement in evolution speed. However,  the general features of the evolution patterns with different generators seen
with Argonne $v_{18}$ are also seen for the N$^3$LO potential.

To better understand the evolution process, we need to look further
into the flow equation itself.  Evaluating Eq.~\eqref{eq:srgflow} in a
two-body partial-wave momentum space basis with $G_s = T$ yields
\bea
 \frac{dV_s(k,k')}{ds} &=& - (k^2 - k'{}^2)^2 V_s(k,k')
  \nonumber \\ & & \hspace*{-.6in} \null
   + \frac{2}{\pi} \int_0^\infty q^2 dq\,
    (k^2 + k'{}^2 - 2q^2) V_s(k,q) V_s(q,k')
    \;.
\eea
In the far off-diagonal region, the first term dominates (this is true for the
ordinary range of $\lambda$ but is modified when $\lambda$ is
comparable with the binding momentum of a bound state).
This implies that each off-diagonal matrix element is driven to zero
as
\beq
  V_s(k,k') \stackrel{k \neq k'}{\longrightarrow} V_{s=0}(k,k')\, e^{-s(k^2-k'{}^2)^2}
  \;.
  \label{eq:driven}
\eeq
For $G_s = f(T)$, these results are modified to
\bea
 \frac{dV_s(k,k')}{ds} &=& - \bigl(k^2 - k'{}^2 \bigr)
   \bigl(f(k^2)-f(k'{}^2) \bigr) V_s(k,k')
  \nonumber \\ & &  \null
   + \frac{2}{\pi} \int_0^\infty q^2 dq\,
    \bigl(f(k^2) + f(k'{}^2 )- 2f(q^2) \bigr)
  \nonumber \\ & &  \null
    \null \times V_s(k,q) V_s(q,k')
    \;
    \label{eq:PWflow}
\eea
and
\beq
  V_s(k,k') \stackrel{k \neq k'}{\longrightarrow} V_{s=0}(k,k')\,
    e^{-s(k^2 - k'{}^2)(f(k^2) - f(k'{}^2))}
    \;.
    \label{eq:drivenf}
\eeq
The difference in the exponents of Eqs.~\eqref{eq:driven} and \eqref{eq:drivenf}
for $k \sim \lambda$ leads to $\lambdaequiv < \lambda$.

The first term of the flow equation (excluding the factor due to the potential) for each of our generators is
shown as a contour plot
in Figs.~\ref{fig:first_term} and \ref{fig:Gs_first_term}.
In Fig.~\ref{fig:first_term} we see that $T$ works uniformly (in $k^2$)
on the entire region of the potential.
With $G_s^{\rm inv}$, there is much less evolution close to the
diagonal.  The plot for $G_s^{\rm exp}$ is similar, but exhibits even less
evolution in the middle region.

It is evident here that the novel generators will result in less evolution at high momenta, as we have seen, and that this
should be a generic result for other partial waves and for higher-body
evolution, because it depends on only kinetic energy differences.
We also see how the value of $\sigma$ controls the degree to which the
operator $G_s$ is similar to $T$.
This is illustrated in Fig.~\ref{fig:Gs_first_term}.
If $\sigma = 1\,\fmi$, only the edges of the potential are
modified; the shape is completely different from $T$.
For $\sigma = 3\,\fmi$, there is the thinnest band on the diagonal,
which is closest to $T$.
At very large $\sigma$, there is a transition to $T$. In the plots of Fig.~\ref{fig:evolvesigma} we see how the final evolved flow is affected by differing choices of \(\sigma\).

The limited evolution at high momenta seen in these generators suggests that the time to evolve to a given decoupling parameter $\lambdaequiv$  should be less for $G_s^{\rm inv}$ or $G_s^{\rm exp}$ than for $G_s = T$.  The dramatic drop in evolution time seen in Fig.~\ref{fig:time1} for the generators makes it apparent that they are more efficient. However, we can also look at how the choice of \(\sigma\) affects their performance.  This  is shown in Fig.~\ref{fig:time2} for $G^{\rm exp}_s$, where we see that the time spent evolving to $\lambdaequiv=2\,\fmi$ decreases as $\sigma$ decreases. As \(\sigma\) becomes smaller, the evolution at high momentum is increasingly limited, which we correlate with improvement in computation time; as \(\sigma\) increases, the evolution time approaches that of \(\Trel\) (as does the flow).  Note that for the Argonne $v_{18}$ potential a large $\sigma$ is needed before $G_s$ is effectively equal to $T$.

In practical applications, one might optimize the trade-off between
decoupling and computational speedup by
choosing \(\sigma \) to be approximately equal to, or slightly greater than the \(\lambda\) corresponding to \(\lambdaequiv\).
Then the decoupling properties of \(G_s=\Trel\) are preserved in the low momentum region of interest while still enhancing the computational performance of the evolution by limiting the evolution at high momentum.
However, this prescription has not yet been tested in detail.

\section{Few-body tests in a one-dimensional model}\label{sec:oneD}

The effects on matrices in a momentum basis demonstrated in
the last section are generic and so
should carry over to alternative bases and to higher-body forces.
Calculations for realistic three-dimensional few-body systems
are not yet available, but we can test the generators in a
one-dimensional model of bosons that has proven to accurately predict the evolution of three-dimensional few-body forces~\cite{Jurgenson:2008jp}.  The model we use was originally
introduced in Ref.~\cite{Alexandrou:1988jg} as
a sum of two Gaussians to simulate repulsive
short-range and attractive mid-range nucleon-nucleon two-body
potentials.  It is written in coordinate space as
\beq
  V^{(2)}(x) = \frac{V_1}{\sigma_1\sqrt{\pi}} e^{-x^2/\sigma_1^2}
    + \frac{V_2}{\sigma_2\sqrt{\pi}} e^{-x^2/\sigma_2^2}
\eeq
and
in momentum space as
\beq
   V^{(2)}(p,p') = \frac{V_1}{2 \pi\sqrt{2}}e^{-(p-p')^2 \sigma_1^2/8}
          + \frac{V_2}{2 \pi\sqrt{2}}e^{-(p-p')^2 \sigma_2^2/8} \;,
  \label{eq:gaussians}
\eeq
where $V_1=12$, $\sigma_1=0.2$, $V_2=-12$, and $\sigma_2=0.8$ (see Ref.~\cite{Alexandrou:1988jg} for discussion of units).  Also, in calculations with an
initial three-body potential, a regulated contact interaction is used.  This is written as
\beq
   V^{(3)}(p,q,p',q') = c_E\,f_{\Lambda}(p,q)f_{\Lambda}(p',q'),
  \label{eq:gaussians3B}
\eeq
where $c_E$ corresponds to the strength of the interaction and
\beq
   f_{\Lambda}(p,q) = e^{-((p^2+q^2)/\Lambda^2)^n}.
  \label{eq:gaussians3Breg}
\eeq
The regulator cutoff $\Lambda=2$, and the sharpness of the fall off is set to $n=4$.  We have chosen these parameters for comparison with Ref.~\cite{Jurgenson:2008jp}.

\subsection{Performance}

\begin{table}
\begin{tabular}{|c|c|c|c|c|}\hline
 \mystrut \textbf{Basis} & \multicolumn{1}{c}{Momentum} \vline&
 \multicolumn{3}{c}{Oscillator}
 \vline\\\hline\textbf{System} & $ A=2$ & $ A=2$ & $ A=3$  & $ A=4$ \\\hline
\(\sigma=2\) & 3.3 & 3.3 & 3.8  & 4.1 \\\hline
\(\sigma=3\) &  2.6 &  2.6 &  2.7  & 2.8 \\\hline
\end{tabular}
\caption{  Speed up in model \(A\)-particle one-dimensional (1D) oscillator basis for evolution to $\lambda_{eq}\approx3$, comparing  the ratio of the time to evolve \(G_{s}=\Trel\) versus \(\GsExp\). The results for \(\GsInv\) are very similar.}
\label{table:speedup}
\end{table}

Our first test is to confirm that the enhanced computational performance characteristics of these generators are maintained in the few-body basis.  Table \ref{table:speedup} shows the  speedup obtained using the \(\GsExp \) generator with the model potential described previously.  The performance of the \(\GsInv\) generator is very similar to the \(\GsExp\) results quoted here.
Results are reported at an optimal \(\lambdaequiv\); we do not use a range of \(\lambda\) values here because of the particularities of the oscillator basis convergence properties, which is discussed in more detail in what follows.

\begin{figure*}[tbh]
  \subfigure[]{\includegraphics[width=0.68\columnwidth]{decoupling_plot_exp_2A_v4_fig11a}}
  \subfigure[]{\includegraphics[width=0.68\columnwidth]{decoupling_plot_exp_3A_v4_fig11b}}
  \subfigure[]{\includegraphics[width=0.68\columnwidth]{decoupling_plot_exp_4A_v4_fig11c}}
  \caption{(Color online) Decoupling using $G_s^{\rm exp}$ with \(\sigma=3\) for (a) $A=2$, (b) $A=3$, and (c) $A=4$. The
   initial two-body-only potential is evolved to each $\lambda$ shown in a basis with \(N_{\rm max} = 40\). Matrix
   elements of the potential are set to zero if one or both states have $N > N_{\rm cut}$
   and the resulting Hamiltonian is diagonalized to obtain the ground-state energies plotted.}
  \label{fig:decouplingmanybody}
\end{figure*}

\begin{figure*}[tb!]
  \subfigure[]{\includegraphics[width=0.683\columnwidth]{GSE_evolving_exp_ce0p00_nmax40_v4_fig12a}}
  \subfigure[]{\includegraphics[width=0.683\columnwidth]{GSE_evolving_exp_ce-0p05_nmax40_v4_fig12b}}
  \subfigure[]{\includegraphics[width=0.683\columnwidth]{GSE_evolving_exp_ce0p05_nmax40_v4_fig12c}}
  \caption{(Color online) The lowest bound-state energy for a four-particle system as a function of $\lambda$ evolved
  using the SRG $G_s^{\rm exp}$ generator and an $N_{\rm max} = 40$ basis with an initial three-body potential with strength (a) $c_{\rm E}= 0.0$, (b) $c_{\rm E}= -0.05$, and (c) $c_{\rm E}= 0.05$.
  The (blue) curves with diamonds include the full evolution of the Hamiltonian while the (black) curves with circles use the two-body potential evolved in the two-particle system and the (red) curves with squares use the two- and three-body potentials evolved in the three-particle system. Evolution with $G_s^{\rm inv}$ is almost
  indistinguishable.}
  \label{fig:Ebindwithlambda}
\end{figure*}

We find that the evolution of  the two-body force in two-, three-, and four-particle systems
with novel generators are all 2.5--4 times faster than the evolution with $G_s = \Trel$ (to the same
degree of decoupling).  The performance enhancement is relatively basis independent, with the speedup for the momentum and oscillator bases roughly equivalent.
While the speedup improvement is much smaller than that found for Argonne $v_{18}$,
we do not expect a direct correspondence.
The important point is that the
speedup in the A=2 particle system serves as a good predictor of the speedup in the A=3 and A=4  systems.  Thus, one might expect a similar improvement in few-body oscillator basis calculations with Argonne $v_{18}$ as found previously for Argonne $v_{18}$ in the two-particle partial-wave momentum basis.
This will be significant as we move to novel generator calculations in  realistic three-dimensional systems.

\subsection{Decoupling}

The measure of performance using these generators depends explicitly on their decoupling properties  in the few-body harmonic oscillator basis relative to  $G_s = \Trel$.  Ultimately, we find the level of decoupling obtained with  $G_s = \Trel$ to be matched by these generators.

However, the convergence properties of the oscillator basis with respect to SRG evolution, and consequently the issue of selecting an appropriate \(\lambdaequiv\) in this basis, is more complicated than for the momentum basis. The convergence of observables depends on a balance of the ultraviolet (UV) and infrared (IR) cutoffs intrinsic to the choice of a particular oscillator basis.  These cutoffs are given by \cite{Jurgenson:2010wy}
\begin{equation}
\Lambda_{\rm UV}\sim\sqrt{mN_{\rm max}\hbar \Omega}
\end{equation}
and
\begin{equation}
\Lambda_{\rm IR}\sim\sqrt{\frac{m\hbar \Omega}{N_{\rm max}}}
 \;,
\end{equation}
where \(\Omega\) is the oscillator frequency and \(N_{\rm max}\) is the maximum number of total oscillator excitations in the basis. Thus, a cutoff in oscillator basis states results in two approximate cutoffs in momentum space.  However, the SRG, using the generators considered here, provides only a means to effectively lower the UV cutoff (by decoupling high- and low-momentum degrees of freedom in the Hamiltonian).  As such, convergence is not monotonically improved with respect to evolution in  \(\lambda\).

 As a measure of the decoupling, we plot the binding energy of the lowest energy state for an \(A\)-particle system with respect to  \(N_{\rm cut}\) for evolutions of the initial Hamiltonian to various  \(\lambda\) (this procedure was carried out for  $G_s = \Trel$ using this model in \cite{Jurgenson:2008jp}).  The actual calculation is carried out by evolving the model interaction to \(\lambda\) in an initial basis large enough so that the binding energy is well converged.  The Hamiltonian is then truncated at \(N_{\rm cut}\)  and the binding energies are calculated in the reduced basis. The value of \(N_{\rm cut}\) refers to the number of oscillator  excitations in the basis and is the oscillator basis equivalent of  the \(\kcut\) parameter in  momentum space, as used in Sec. \ref{sec:NN}. Again, each \(N_{\rm cut}\)  here corresponds to a rough \(\Lambda_{\rm UV}\) and \(\Lambda_{\rm IR}\) truncation in momentum space.

Results are shown in Fig.~\ref{fig:decouplingmanybody} for the A = 2, A= 3, and A=4 particle systems using
$G_s^{\rm exp}$ with $\sigma = 3$ for selected values of \(\lambda\).  The signature of decoupling is the improved convergence of the binding energy at smaller \(N_{\rm cut}\) with respect to SRG evolution.  As the interaction is evolved, the degree of decoupling gets better. This is true only up to some value of $\lambda$, however, at which point the degree of decoupling starts to get worse.  It is the latter behavior, introduced by the IR\ cutoff of the oscillator basis, that complicates our efforts to choose a \(\lambdaequiv\) because a one-to-one correspondence with \(\lambda\) is no longer clear.

Nevertheless, a practical choice can be made by  equating \(\lambda\) with \(\lambdaequiv\) when decoupling is found to be optimal in the \(G_{s}=\Trel\) and novel generator evolutions.
The optimal levels of evolution
happen to coincide at \(\lambda\approx3\) for  \(G_{s}=\Trel\) and these generators.  Thus, the speedup results in Table \ref{table:speedup} were reported at \(\lambdaequiv=3\).  Moreover, given these values for \(\lambda\) and \(\lambdaequiv\), we have chosen \(\sigma=3\) for most of the model space calculations in this section.

 One may note that differences do exist between the \(G_s=\Trel\)  and novel generator decoupling results, particularly at low  \(N_{\rm cut}\)   \cite{Jurgenson:2008jp}. However, the  level at which any of the generators become well converged to the exact
results with respect to \(N_{\rm cut}\) are effectively the same.
Thus, it is reasonable to make the comparisons we have done here to determine \(\lambdaequiv\).

\subsection{Induced Many-Body Forces}

In general, the evolution of an interaction via the SRG leads to induced many-body forces.  This is evident if we examine the second quantized form of the Hamiltonian
\begin{equation}
H=T_{ij}a_{i}^{\dag}a_{j}+V_{ijkl}a_{i}^{\dag}a_{j}^{\dag}a_{l}a_{k}+\cdots
\end{equation}
where the dots indicate that higher-body forces  may also be present in the initial interaction.
When the SRG commutators in Eq.~\eqref{eq:srgflow} are performed, one can see that many-body forces will be induced.
These induced forces could pose a serious problem for few-body calculations because at some point we must truncate the model space in numerical calculations, which will alter the predicted value of observables.
These can be controlled, however, if there is a hierarchy of many-body forces so that successively larger many-body components are suppressed, and one can include at most one or two  induced pieces to obtain well converged results.  This has been found to be the case for \(G_{s}=\Trel\) and needs to hold for any practical alternative generators.

A measure of the induced many-body forces (which has been used in previous studies \cite{Jurgenson:2008jp,Jurgenson:2009qs,Jurgenson:2010wy}) is to calculate the ground-state energies of the $A=3$ and A=4 particle systems starting with a two-body interaction and to examine how this energy changes with and without the induced three- and four-body components, as a function of the evolution parameter \(\lambda\). We do this in Fig.~\ref{fig:Ebindwithlambda} with a  plot of the ground-state energy for the four-particle system with the initial two-body interaction embedded and evolved in the $A=2$, A=3, and A=4 body bases with the $G_s^{\rm exp}$ generator.
The results for $G_s^{\rm inv}$ are virtually indistinguishable.
The curves show that the hierarchy of induced many-body forces is preserved for these generators just as with $G_s = \Trel$ \cite{Jurgenson:2008jp}
(see, however, Ref.~\cite{Roth:2011ar}). This hierarchy also holds for calculations with an initial three-body force and in the $A=3$ particle system.

In summary, the model results suggest that the advantageous features of SRG evolution with $G_s = \Trel$ can be maintained with the added computational performance of these generators when applied to realistic three-dimensional few-body calculations.

\section{Summary}\label{sec:summary}

In this work, novel generators for the SRG that are functions
of the kinetic energy operator $T$ with an adjustable scale parameter
$\sigma$ were tested.  We found that
functions that reduce to $T$ for basis states with kinetic energy
less than $\sigma$   preserved the good features of $T$, such as decoupling,
but efficiently suppressed evolution for higher
kinetic energies and thereby took much less time to evolve.
Specific examples were considered,
but other choices with a Taylor expansion starting with $T$ should
give comparable results.
Their action was understood using a simple
analysis of how the generators directly affect regions of high and
low momentum.  If $\sigma$ is large enough, the generators become equivalent
to $T$.
It is important to note that not only the two-body properties of \(\Trel \) were preserved by these generators, but so were its characteristics in a few-body model space. This includes decoupling and the hierarchy of induced many-body forces, which is critical for applications to larger systems of particles.

The generators allow us to evolve potentials to much smaller
values of $\lambda$ than previously feasible.
This should enable us to explore
the transition between {pion\-ful} and pionless regions
of EFT potentials and further test the observations
of Glazek and Perry about evolving past a
bound state~\cite{Glazek:2008pg}.
The original choice for $G_s$ advocated by Wegner and
collaborators~\cite{Wegner:1994,Kehrein:2006}
and applied extensively in
condensed matter is the diagonal component of the interaction,
$G_s = \Hdiag(s)$,
\beq
  \langle i | \Hdiag(s) | j \rangle  \equiv
  \begin{cases}
  \langle i | H(s)| j \rangle  & \text{if } i = j \;,\\
    0 & \text{otherwise.}
  \end{cases}
\eeq
In Ref.~\cite{Glazek:2008pg}, it was observed that when evolving a
simple model past a bound state
the Wegner
evolution with $\Hdiag$ will decouple the bound state by leaving it as
a $\delta$ function on the diagonal of the Hamiltonian.
In contrast, with $G_s = \Trel$ the bound states remained coupled to low momentum
and were pushed to the lowest momentum part of the matrix.
This behavior was explored in Ref.~\cite{Wendt:2011qj} for leading-order, large-cutoff EFT potentials featuring deeply bound spurious states.
However, it has not been studied for the physical deuteron state,
which requires evolving well below $\lambda = 1\,\fmi$.
This is now easily possible with the replacement of $\Hdiag$
for $T$ in Eqs.~\eqref{eq:invgen} and \eqref{eq:expgen},
although there are as-yet-unsolved
complications from the discretization of
the momentum basis.

The most important next step for the novel generators is to apply
them to evolve realistic few-body potentials, where
speeding up the evolution is desirable because of the
large sizes of the matrices involved.  The generators can be applied
directly to few-particle bases using the method described
in Refs.~\cite{Jurgenson:2008jp,Jurgenson:2009qs,Jurgenson:2010wy}.
Calculations in a one-dimensional model performed here imply that the speed up
carries over to three-body forces and could have a significant impact in making realistic calculations with additional induced many-body forces feasible.

\begin{acknowledgments}
We
thank E. Jurgenson, R. Perry, and K. Wendt for useful comments and discussions.  We also thank E. Jurgenson for the use of his 1D few-body code.  This work was supported in part by the National Science Foundation under Grant Nos.~PHY--0653312 and PHY-1002478, and the UNEDF SciDAC Collaboration under DOE Grant DE-FC02-09ER41586.

\end{acknowledgments}

redpajama_set_name: RedPajamaArXiv


At the centrifugal compressor test rig, single fast-rotating high-loaded centrifugal compressors are investigated. In addition to measuring the compressor performance map, detailed flow field measurements are made in order to analyze the three dimensional flow field within the rotor and the diffuser by using conventional probes and several optical measuring methods like L2F, PIV and DGV. Only optical techniques are applicable within the rotating component.


Telecommunications is only responsible for Imaging, Video and Sound system in your T.V and cellphones also through your Internet connections and other modes of communications or routes. An students having interest that how things actually workout in our communication systems as well as in our entertaining equipment should learn those subjects carefully to clear there concept about Telecommunications.
An major course regarding telecommunications study is BSC (bachelor of science ) in Telecommunication.
Telecommunications are growing all over the world including INDIA & America. There is always an continuous Growth in Opportunities in this field as there is always new products and services are developed in this field such as in cable operations and cell phone operators.
This will leads to top positions in any company as an telecommunication employee is must in almost every field. also this will gave an more than fare chance to successful in own business,.
There is an vast job of collections in telecommunications for students as starting salary for employees in companies are almost 56 thousand $ annually and which is continues increasing with increase in experience of worker or employees.


text:
You Are Here: RWTH Professor Thomas Bein Publishes on Walther von der Vogelweide
RWTH Professor Thomas Bein Publishes on Walther von der Vogelweide
You Are Here:RWTH Professor Thomas Bein Publishes on Walther von der Vogelweide
Thomas Bein
Dean of Academic Affairs
After a ten-year period of research, Professor Dr. Thomas Bein of the Department of German and Medieval Studies will publish a new scholarly edition of the works of Walther von der Vogelweide.
After his appointment in 1999, Bein established the Walther von der Vogelweide Research Center at RWTH Aachen, where he worked on the new critical-scholarly edition.
For the first time, several texts by the famous author will be published in different versions, just as there were different medieval manuscripts of his works. In this way, new material will be made available for literary-historical research, which will shed new light on the poet and his works.
The new edition will by published by the scientific and scholarly publisher de Gruyter in June 2013.


text:
2017 Ducati Multistrada 950 first ride review
Abhay Verma Updated: August 24, 2017, 08:43 AM IST
Ducati's new Multistrada 950 is a delicious idea. It takes Ducati's idea of a road-biased, sporty adventure tourer to a friendlier, more affordable space. What makes it the Ducati Multistrada 950 even more tantalising is the fact that it's price in India neatly splits the popular four-bike Triumph Tiger 800 range in half. The Ducati Multistrada 950 also represents a change of direction for the adventure class which was full of much larger machines until very recently.
Manufacturers are making adventure tourers smaller and lighter to make them more accessible. The Kawasaki Versys 650 and the Triumph Tiger 800 are perhaps the biggest drivers of the downward displacement trend in the adv market. And now Ducati wants in on the action. The Multistrada 950's story begins with the bigger 1200cc Multi and it scales that Ducati down. Ducati's 950 is a Multistrada that's not only lighter and smaller but also less powerful to make it easier for less experienced bikers. We spent a day in the saddle to tell you how it is.
Unsurprisingly, the Multistrada 950 looks identical to the 1200. You get the same beak-like nose, twin headlights, fairing and adjustable flyscreen. It doesn't get the fancy LED headlights from the 1200S and the beak is finished in matte black. The 950 also misses out on the single-sided swingarm, while the chassis is almost identical to the off-road biased Multistrada Enduro. That's the reason why the 950's wheelbase is significantly longer than the 1200's at 1,594mm (1200's stands at 1,530mm).
As opposed to the 1200's 17-inch front wheel the 950 uses a 19-inch front wheel, again the same as the Enduro, though the rear is a 17-inch unit. The clocks are the same as the standard Multistrada 1200, a monochrome LCD display. The exhaust is new and sleeker looking, and the rear tyre narrower at 170mm, though the tail piece is the same. It is not easy to distinguish the 950 from the bigger 1200 from a distance which is a good thing, as it carries the same full-blooded Italian aura as its elder sibling.
The Hypermotard/Supersport's 937cc, liquid-cooled 90-degree twin performs duty here. The idea was to make the 950 more affordable apart from making it smaller and less powerful, and this engine is a simple unit sans the 1200's exotic tech like DVT (Desmodromic Variable Timing). It produces 113PS and 96Nm which is notably higher than its arch rival, the Triumph Tiger 800's 95PS and 79Nm.
The engine has a slight vibration at low revs which smoothens out past 3000rpm, which is also where the engine offers you its full wealth, allowing you to accelerate rapidly. I reckon the Multistrada 950 will hit 100kmph in just under 4 seconds, given its kerb weight of 229kg as compared to the 1200's weight of 235kg, which hits 100kmph in about three and half seconds. The bike accelerates well past 150kmph seamlessly, and should have no trouble sitting at over 120kmph all day, making it an ideal mile muncher.
Rapid progress in traffic is a breeze thanks to the engine's punchy, quick to rev nature and I've no doubts that the 950 will prove to be a ludicrously worthy commuter. Gear ratios are well chosen and the shifts are light and precise.
The 950 gets the same Sport, Touring, Urban and Enduro modes as the bigger Multistrada. Sport and Touring offer the full 113PS, while Urban and Enduro reduce output to 75PS. The switchgear is different from the 1200's, and is a simpler affair. Switches are not as premium but do their job well.
It also gets switchable 8-level traction control and 3-mode ABS but misses out on wheelie control. No fancy suspension of course, so the modes do not change preload or suspension settings.
Ride and handling
The Ducati Multistrada 950 feels more streetbike than adventure tourer on the road. The riding position has you seated upright while you rest your feet on the slightly rearset footpegs. This makes it engaging to ride hard, be it around corners or through traffic. There's a sense of agility despite the bike being reasonably large. Putting both feet down shouldn't be an issue for most riders given the fixed saddle height of 840mm. You could also opt for the adjustable seat, which can lower or raise seat height by 20mm. The 19-inch front wheel is communicative, and on the whole the Multi 950's dynamics and punchy motor together make it a lot of fun to ride fast.
Credit for that also goes to the well-sorted suspension (adjustable, but non-electronic) and the Pirelli Scorpion Trail II tyres. The suspension is firm but soaks in bumps and potholes without unsettling the bike. We couldn't take the bike off tarmac, but on it the Multistrada 950 is very impressive. It is impressive as a machine for riding to work daily and going out on long rides, with or without pillion. A dash of dirt roads shouldn't be a hitch for it either.
The Multistrada 950 stays true to its assigned role, that of being a multipurpose adventure tourer in a package that's smaller, lighter and equally capable. At the same time, it doesn't skimp out on the pizzazz of its elder sibling. It comes across as a worthy buy if in the market for an adventure tourer that doesn't call for Herculean skills to ride. For ?14.50 lakh on-road Delhi the Ducati Multistrada 950 is good value, especially compared to the Tiger. But, we feel the whole class could stand to have a slightly lower price.
Images by Akshay Jadhav
Ducati Multistrada 950 2017 Full Spec
Price (Ex-Delhi)
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Home Bay features 20 listings in 30288.
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SPRING VALLEY LAKE– (VVNG.com): On Friday, January 16th at approximately 6:51 a.m., the Victor Valley Sheriff's Station received a report of numerous vehicle burglaries on Sea Gull Drive in Spring Valley Lake.
Upon the arrival of deputies located a total of six victims. With the assistance of the community including some of the victims of the vehicle burglaries, deputies were able to identify and locate the suspect hiding in the area of Pyramid Drive in Spring Valley Lake.
Christopher Fields, 26 of Victorville was arrested and booked into the High Desert Detention Center where he is currently being held without bail for violating his probation. Fields was found in possession of stolen property from all of the victims to whom it was returned.
Fields was granted formal probation on April 8, 2014 for a previous Burglary charge.
The teamwork of the San Bernardino County Sheriff's Department, Spring Valley Lake Public Safety and the community lead to the arrest of Fields.


text:
"Киклоп" је југословенска телевизијска серија снимљена 1983. године у продукцији ТВ Загреб.

Епизоде

Улоге

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|Франо Ласић || Мелкиор Тресић (5 еп.  1983)
|-
|Марија Бакса || Вивијана (5 еп.  1983)
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|Љуба Тадић || Маестро (4 еп.  1983)
|-
|Раде Шербеџија || Уго (4 еп.  1983)
|-
|Мира Фурлан || Енка (4 еп.  1983)
|-
|Реља Башић || Атма (4 еп.  1983)
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|Звонимир Рогоз || (4 еп.  1983)
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|Карло Булић || (4 еп.  1983)
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|Зденка Хершак || Газдарица (4 еп.  1983)
|-
|Мустафа Надаревић || Дон Фернандо (2 еп.  1983)
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|Драган Миливојевић || Фреди (2 еп.  1983)
|-
|Иво Бан || Курт (2 еп.  1983)
|-
|Мира Босанац || Елза, Куртова сестра (конобарица) (2 еп.  1983)
|-
|Влатко Дулић || (2 еп.  1983)
|-
|Зоран Гогић || (2 еп.  1983)
|-
|Иво Грегуревић || Креле (2 еп.  1983)
|-
|Душко Груборовић || (2 еп.  1983)
|-
|Хрвоје Ковачић || Продавац новина (2 еп.  1983)
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|Ђорђе Рапајић || (2 еп.  1983)
|}
 Остале улоге  ▼
|-
|Мирко Боман || (1 еп.  1983)
|-
|Давор Борчић || (1 еп.  1983)
|-
|Владимир Бошњак || (1 еп.  1983)
|-
|Александар Цакић || Југословенски официр (1 еп.  1983)
|-
|Звонимир Чрнко || (1 еп.  1983)
|-
|Алеxандер Цветковић || (1 еп.  1983)
|-
|Дубравка Дежелић || (1 еп.  1983)
|-
|Петар Добрић || Поштар (1 еп.  1983)
|-
|Борис Дворник || Мајор југословенске војске (1 еп.  1983)
|-
|Нина Ерак Свртан || (1 еп.  1983)
|-
|Иво Фици || (1 еп.  1983)
|-
|Људевит Галић || (1 еп.  1983)
|-
|Емил Глад || Главни уредник (1 еп.  1983)
|-
|Зденко Јелчић || Поднаредник (1 еп.  1983)
|-
|Асја Јовановић || Гђа с цвијећем у градској кавани (1 еп.  1983)
|-
|Фрањо Јурчец || (1 еп.  1983)
|-
|Звонимир Јурић || (1 еп.  1983)
|-
|Миодраг Кривокапић || Мобилизирани пролазник с новинама (1 еп.  1983)
|-
|Антун Кујавец || (1 еп.  1983)
|-
|Томислав Липљин || Возач трамваја (1 еп.  1983)
|-
|Данко Љуштина || (1 еп.  1983)
|-
|Златко Мадунић || (1 еп.  1983)
|-
|Фрањо Мајетиц || (1 еп.  1983)
|-
|Раде Марковић || (1 еп.  1983)
|-
|Златко Мартинчевић || (1 еп.  1983)
|-
|Борис Михољевић || Пролазник с новинама у рукама (1 еп.  1983)
|-
|Љубица Микулчић || (1 еп.  1983)
|-
|Сретен Мокровић || Регрут (1 еп.  1983)
|-
|Владимир Облешчук || (1 еп.  1983)
|-
|Предраг Петровић || Регрут (1 еп.  1983)
|-
|Милан Плећаш || (1 еп.  1983)
|-
|Тихомир Поланец || (1 еп.  1983)
|-
|Недим Прохић || (1 еп.  1983)
|-
|Владимир Пухало || (1 еп.  1983)
|-
|Матко Рагуз || (1 еп.  1983)
|-
|Томислав Ралиш || (1 еп.  1983)
|-
|Дамир Шабан || (1 еп.  1983)
|-
|Берт Сотлар || Илегалац (1 еп.  1983)
|-
|Звонко Стрмац || (1 еп.  1983)
|-
|Круно Валентић || (1 еп.  1983)
|-
|Бранимир Видић || Регрут (1 еп.  1983)
|-
|Мирко Војковић || (1 еп.  1983)
|-
|Аљоша Вучковић || (1 еп.  1983)
|-
|Вера Зима || (1 еп.  1983)
|-
|Илија Зовко || (1 еп.  1983)
|}

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redpajama_set_name: RedPajamaWikipedia


text:
Q: WordPress Gutenberg Block not working after reload I'm creating a custom Gutenberg-Block with three attributes.
I set these attributes in the registerBlockType-function:
attributes: {
    message: {
        type: 'string',
        source: 'html',
        selector: 'div.content',
    },
    url: {
        type: 'string',
        source: 'text',
        attribute: 'href',
        selector: 'a.link',
    },
    bgImageId: {
        type: 'string',
        source: 'text',
        attribute: 'src',
        selector: 'img',
    }

When saving I create the following HTML-Code which looks fine on the homepage:
export default function Save( { attributes, className } ) {
    return(

{ attributes.message }

    );
}

But after reloading the editor, I get multiple errors:
Block validation: Expected attribute `href` of value `o`, saw `k`

Block validation: Block validation failed for `custom/custom-blocks` (
Content generated by `save` function:

o

Content retrieved from post body:

o

I've tried changing the attributes but nothing seems to work.

redpajama_set_name: RedPajamaStackExchange


text:
using OnePathfinding;
using System.Collections;
using UnityEngine;

/// <summary>
/// Used to spawn AIs with ease.
/// </summary>
public class AISpawner : MonoBehaviour
{
    /// <summary>
    /// Maximum number of AIs.
    /// </summary>
    public int MaxAIs = 100;

    /// <summary>
    /// An instance to this object.
    /// </summary>
    private static AISpawner _instance;

    /// <summary>
    /// An instance to this object.
    /// </summary>
    public static AISpawner instance
    {
        get
        {
            if (_instance == null)
            {
                _instance = FindObjectOfType<AISpawner>();
            }
            return _instance;
        }
    }

    /// <summary>
    /// Spawns a object at a position.
    /// </summary>
    /// <param name="obj">The object to spawn</param>
    /// <param name="position">The position on which to spawn the obj.</param>
    public static void Spawn(GameObject obj, Vector3 position)
    {
        GameObject ob = (GameObject)Instantiate(obj, position, Quaternion.identity);

        ob.transform.parent = FindObjectOfType<GridManager>().transform;
        ob.name = obj.name;
    }

    /// <summary>
    /// Spawn the specified amount of obj AIs
    /// </summary>
    /// <param name="obj">The object to spawn</param>
    /// <param name="Amount">The amount to spawn</param>
    public static void Spawn(GameObject obj, int Amount)
    {
        instance.StartCoroutine(SpawnObjects(obj, Amount));
    }

    private static IEnumerator SpawnObjects(GameObject obj, int Amount, GridGraph grid = null)
    {
        if (grid == null)
        {
            grid = GridManager.Grid;
        }
        if (grid.gridType == GridGraph.GridType.Plane)
        {
            float minX = grid.offset.x;
            float minY = grid.offset.z;

            float maxX = minX + grid.WorldSize.x;
            float maxY = minY + grid.WorldSize.y;

            Transform gridTransform = FindObjectOfType<GridManager>().transform;

            int i = 0;
            while (i < Amount && instance.gameObject.transform.childCount < instance.MaxAIs)
            {
                GameObject ob = (GameObject)Instantiate(obj, new Vector3(Random.Range(minX, maxX), 0, Random.Range(minY, maxY)), Quaternion.identity);
                ob.transform.parent = gridTransform;
                ob.name = obj.name;

                i++;
                yield return null;
            }
        }
        else
        {
            Transform gridTransform = FindObjectOfType<GridManager>().transform;

            int i = 0;
            while (i < Amount && instance.gameObject.transform.childCount < instance.MaxAIs)
            {
                GameObject ob = (GameObject)Instantiate(obj, Random.onUnitSphere * (grid.Radius + 2), Quaternion.identity);
                ob.transform.parent = gridTransform;
                ob.name = obj.name;

                i++;
                yield return null;
            }
        }
    }
}

redpajama_set_name: RedPajamaGithub


text:
Fairmont Olympics Wedding Photo
Anyone who's ever tried to plan a wedding before knows that things rarely ever go exactly as planned - especially when a pandemic gets thrown into the mix.
Originally, Kristine and Steve had planned a destination wedding at the Fairmont Chateau in scenic Whistler, British Columbia that features a gorgeous rooftop chapel surrounded by a breathtaking view of the mountains. But as fate would have it, COVID-19 had other plans in store for them and they made the decision to transfer their venue deposit to the Fairmont Olympic Hotel, located in downtown Seattle.
The Fairmont Olympic may not feature on-demand views of the famous Whistler Blackcomb ski resort - but make no mistake - the experience is just as magical for those looking to wed in an elegant way. The venue, which was established in 1924, recently underwent a major renovation to combat some of the financial devastation caused by the pandemic, and to restore the Fairmont Olympic's original Roaring-Twenties charm. (The renovation comes complete with a luxurious, dimly lit speakeasy that's hidden behind a bookshelf, in case you had any questions about its authenticity.)
In the end, Kristine and Steve may not have had the destination wedding they originally planned for, but they got the opportunity to celebrate their union surrounded by friends and family in one of Seattle's oldest and finest establishments. What more could you ask for?
Location: 411 University St, Seattle, WA 98101.
Keywords: Fairmont, Speakeasy, Whistler.


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The Hungarian Ministry of Defence has ordered 16 H225M Caracal multi-purpose helicopters equipped with the HForce weapon management system.
"I am thankful for the trust that the Hungarian Government has placed in our company to support its ambitious 'Zrinyi 2026' armed forces modernisation programme. Our teams have witnessed the professionalism and enthusiasm of the Hungarian experts and pilots whose contribution has been key to ensuring the success of this project", said Bruno Even, Airbus Helicopters CEO.
Earlier this year, the Hungarian MoD has ordered 20 Airbus H145M military helicopters equipped with the HForce weapon system.
"This new contract confirms the H225M as a combat-proven, multi-role platform operated by the most demanding military customers worldwide. The Hungarian armed forces will be able to rely on the cost-efficient H145M / H225M tandem that will enable them to cover all of the major military missions, from light utility, tactical transport, combat search and rescue up to light attack", added Bruno Even.


Rotary Cam Switches and Accessories, Rated Thermal Current (Ith) = 20A AC23A rating - 7.5kW at 415V. Rated Insulation Voltage Ui = 480V. Maximum 20A Fuse (gG/gL) for 5kA short circuit protection. Terminals provide IP20 protection, 3 Phase voltmeter selector switch marked O / L1-N / L2-N / L3-N.


text:
Former President George W. Bush criticizes GOP as 'isolationist,' expresses concern over immigration rhetoric
e mhm, so I don't have to.
Former President George W. Bush says the Republican Party he served as president has become "isolationist, protectionist and, to a certain extent, nativist" and says he's especially concerned about anti-immigration rhetoric."It's a beautiful country we have and yet it's not beautiful when we condemn, call people names and scare people about immigration," Bush told "Today" on Tuesday.Bush, who was in New York to preside over a naturalization ceremony, said his new book, "Out of Many, One: Portraits of America's Immigrants," aims to "elevate the discourse."Bush did not mention former President Donald Trump, who aggressively curbed both legal and illegal immigration during his tenure and sought to build a "big, beautiful wall" at the southwest border with Mexico to keep out migrants. Trump, a fellow Republican, disparaged the migrants as invaders and "illegal aliens" and, as a candidate, referred to Mexicans as "rapists."But Trump has dominated the Republican Party, even out of office. Hard-right House Republicans last week discussed forming an America First Caucus, which one document described as championing "Anglo-Saxon political traditions" and warning that mass immigration was putting the "unique identity""of the U.S. at risk.Bush, asked to describe the state of the party, replied, "I would describe it as isolationist, protectionist and, to a certain extent, nativist." He added, "It's not exactly my vision as an old guy, but I'm just an old guy that's put out to pasture."
Former President George W. Bush says the Republican Party he served as president has become "isolationist, protectionist and, to a certain extent, nativist" and says he's especially concerned about anti-immigration rhetoric.
"It's a beautiful country we have and yet it's not beautiful when we condemn, call people names and scare people about immigration," Bush told "Today" on Tuesday.
Bush, who was in New York to preside over a naturalization ceremony, said his new book, "Out of Many, One: Portraits of America's Immigrants," aims to "elevate the discourse."
Bush did not mention former President Donald Trump, who aggressively curbed both legal and illegal immigration during his tenure and sought to build a "big, beautiful wall" at the southwest border with Mexico to keep out migrants. Trump, a fellow Republican, disparaged the migrants as invaders and "illegal aliens" and, as a candidate, referred to Mexicans as "rapists."
But Trump has dominated the Republican Party, even out of office. Hard-right House Republicans last week discussed forming an America First Caucus, which one document described as championing "Anglo-Saxon political traditions" and warning that mass immigration was putting the "unique identity""of the U.S. at risk.
Trump in 2024? He says only that 'a Republican' will win
Bush, asked to describe the state of the party, replied, "I would describe it as isolationist, protectionist and, to a certain extent, nativist." He added, "It's not exactly my vision as an old guy, but I'm just an old guy that's put out to pasture."


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If you have to sell off or go for a mass buyout, then all these suggestions too would be given by this expert only.If you are someone who just wants to invest now and then and do not therefore mind so much about the portfolio, then you would be advised to take care and go ahead. Times will change, and along with time, economy will change and sectors that were not even considered in the past would be considered now.
So, it is recommended that you consult the likes of Linda Foster Washington, who runs Foster Financial Services in such investment plans. She would be able to tell you when you should not be swayed by the wave of general trend and when to make the most of such trends. An investment expert advisor is someone who handles multiple accounts like yours and is practically in the same place or field all day. This means she would know the best way to get the most and she would know the sector or industry that offers the best deal and the industry that works well.
If you are planning to go for retirement plans then you should know that you should calculate and foresee the future while investing in such plans. You would have to understand the inflation vis-a-vis your standard of living. Only you would know if you would be satisfied with a stipulated amount of money or not. If you are used to leading a lavish life, and are quite careless about spending it right now, then you must also save up a lot of money to spend your post-retirement days in peace. This is why consulting experts would be a rather great idea. They would calculate your income, your expense and plan your savings for a debt-free future.


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Ready to upgrade your AC system? Call Heritage Heating & Cooling at (618) 649-0056 for superb O'Fallon air conditioning installation!


text:
Little Busch Stadium
Little Fenway South
JHF TOURNEY HISTORY
JHF CAREER STATS
2021 The HEAT is ON!
The Heat was on and the Cubs roared!! The 2021 JHF Foundation tournament raised a record $73,616. That was not the only record that was shattered. A record number of home runs were hit (144) eclipsing the old record by SIXTY (83). Numbers can be deceiving however. When compared to total hits, the home run percentage was 14%, exactly in line with previous years. This is in line with MLB home run percentage (14%). The tournament was divided into two divisions, American and National League. The Heat won the American League and the CC Cubs were national league champs. Carter Whittington (Heat) was named AL MVP while Anna Boone (Wiffle Woders) was NL MVP. Boone was the first multi hr hitting female in tourney history. Gavin Mitchell of the Cubs set a record for most hits in a tourney (13). Gabe Board moved into a three way tie (Dono McGregor and Gordon Dugan) for most hits in a career (39). Brandon Sigler cemented his legacy taking over all time HR lead with 15 in his career. Your Sports Edge led by the Isom boys had a good showing but came up just short against the Heat in the AL Championship. Defending champs Free Press were 0-3 as star Dono McGregor has just came off injured list. It was a great weekend had by all.
2019 Rain Rain, Go Away
The 2019 Jake Hodge Foundation Wiffle ball tournament saw another record year of funraising as $58,613 dollars were raised. The event was the largest to date. Rain on Saturday and Sunday did not dampen the community involvement or support for this great cause. The event was highlighted by the addition of our second field "Little Fenway South". Little Fenway was constructed in about 3 weeks and proved to be a hit from players and fans alike. The Crittenden Free Press won in the championship against the 2015 champion McCrew. For the Free Press, it was their first win in the Jake Hodge Tournament. There has not been a repeat champion since the Bone Collectors won the first two events in 2013 and 2014. Other standout performances were from the Joe Vanhooser led Knuckelheads as well as Jakie Sholar's Longshots. In the end, it was the Free Press led by Denis Hodge, Brandon Sigler, and MVP Dono Mcgregor.
2018 Tigers Roar
August 09, 2018. The 2018 Jake Hodge Tournament set a record raising $42,850 dollars. 22 teams participated in beautiful, but warm weather. Tournament MVP went to Jase Felker and Oliver Parker of Tiger Baseball. Tiger Baseball was dominant throughout the event and captured their first Jake Hodge title defeating Scared Hitless in the final. A devotional service by Brandon Sigler highlighted Sundays final day. The surprise of the tournament were the newcomers' Caldwell 9U All Stars. The All Stars made it to the semifinals, bowing out to Tiger Baseball. These 9U kids had the most exciting games of the tournament in a best of three game series with the Christian County Cubs. Each game was a one run affair. Another team of note were the Fredonia Girls who made it to the playoffs in their first year. The girls from Fredonia also raised over $1,700 dollars for the event. Other playoff teams included the Barrel Heads who made it to the semifinals, and 2015 champion McCrew. Brian Shemwell, and Bryce Thomas tied for the tourney HR lead with 4.
2017 Youth Movement
August 08, 2017. The 2017 Jake Hodge Tournament raised over $34,000. The surprise of the tournament was the 11U West Kentucky Wildcats who stormed into the playoffs undefeated. These 11 year old's defeated pre-tourney favorite Crittenden Free Press in the semifinals. The Free Press could not overcome the loss of player/coach Denis Hodge who was injured the week leading up to the tournament. The final game was a classic pitching duel in the rain between Fredonia's Craig Wyatt and the Wildcats' Luke Parker. Fredonia would claim the win 1-0 and their first Jake Hodge Championship. MVP went to Fredonia Boys Derrick Perkins and The Bone Collectors star Gordon Dugan was elected the the Little Busch Stadium Hall of Fame. After a few years of coming up short in the playoffs, Fredonia finally broke through with the win.
2016 Squirrel Domination
The 2016 Jake Hodge Tournament raised a record $26,200. The Rally Squirrels dominated the field from start to finish. The Squirrels pounded a tournament record 17 home runs, batted .500 and were 5-0 for the event. Dono McGregor was the MVP batting .706 and hitting 3 home runs. Dono was also masterful on the pitching mound with wins over the Free Press, Fredonia Boys, Bone Collectors, 10U wildcats, and Team Lara. Team Lara threatened in the championship game taking a 4-1 lead into the top of the fifth, but back to back to back home runs by Allen Dixon, Dono, and Brandon Sigler would tie the game. The squirrels would get a home run by Joey East for the win in the top of the 6th inning.
2015 McCrew Wins Big!!
A record 15 teams participated and $25,585 dollars were raised at the 2015 Jake Hodge Wiffle Ball Tourney. A new king was crowned as the McCrew defeated the Crittenden Free Press 7-4 in the championship game. MVP Conner McEnaney led the McCrew to the win by pitching a 1-0 gem in the semifinals against the Fredonia Boys and hitting a solo home run for the only run of the game. Denis Hodge and the Free Press came up a little short again this year. The two time defending champion Bone Collectors went 0-2 and could never quite get on track. Playing conditions were tough this year because of extreme weather and problems with new bluegrass sod.
Bone Collectors Repeat
The Bone Collectors won their second straight JHF Tournament in convincing fashion. The fundraising set a record with $18,628 raised to support scholarships for the Jake Hodge Foundation. Dan Hodge was named MVP on the strength of his pitching for the Free Press. The former Indiana baseball player shutout the Bone Collectors in pool play for the Collectors first loss in the history of the Jake Hodge Tourney. Former Philadelphia Phillies player Anthony Schuemaker would lead the bone Collectors with 5 home runs for the tournament. The Collectors defeated Team 11 in semifinals 7-2 and the Kings of Crash in the finals 7-1. It would be the second JHF Tourney championship in a row for the big boys from Paducah.
2013 JHF Let The Fun Begin
Bone Collectors Win Inaugural Jake Hodge Wiffle Ball Tourney
The Bone Collectors won the 2013 JHF Wiffle Ball Tourney. Over $8,000 was raised in the first year of the event at Little Busch Stadium. The Championship game saw Team 11 (Jake Hodge old travel baseball team) lose 10-4 to the Bone Collectors. Although, Team 11 was the sentimental favorite, Bone Collectors proved to be the superior team in the event. Gordon Dugan won MVP with 12 hits and 5 home runs.
OVER 280K RAISED!!
Let us know if you are interested in hosting a charity event.
JAKE HODGE FOUNDATION
- About the Foundation
- Prior Results and Statistics
1301 South Jefferson St.
Princeton KY 42445
© 2018 Little Busch Stadium


Congo (DRC) has been a worn-torn country for over 25 years with millions having been slaughtered! Add to this all who have been raped and infected with HIV/AIDS and you have a country with a broken heart!! Yet, today I am here to reach out with the Word of God and the compassion of the Lord Jesus making disciples, to teach, preach and demonstrate the full Gospel of the Lord to those with HIV/AIDS… Amen.


text:
The Intersection of faith, culture, and politics
Help JWR Survive and Thrive
Pause for a moment and recall all of the articles you\'ve read this year that left you impressed. And all of those you\'ve forwarded to others. Or shared on social media.Remember that sense of gratification � especially when you were able to effectively dismantle those who mock our shared values?
Remember your gratitude for having found JWR?
Now is the time to act on those feelings.
Indeed, help guarantee that they continue
If we all gave $10, this fundraiser would be over in less than 30 minutes.
$5 $10 $20 $50 $100
Home Columnists Toons Lifestyles About JWR ▸ Daily Newsletter
Hil and Hubby: The Bunk Starts Here
Contact The Editor Articles By This Author
Alicia Colon: Jewish self-loathing
Dmitriy Shapiro: Rand repents?
Kelsey Dallas: OMG: Is profanity losing its punch?
Eric Schulzke: Daydreaming may be the next childhood psychiatric target
Kathryn Moody: Investors, Are You Ready for the Next Global Crisis?
Manuel Schiffres
Mutual Fund Rankings, 2014
Meghan Streit: Pitching In When Caregivers Need Help
Janet Bond Brill, Ph.D., R.D.N., F.A.N.D: How to prevent a second (and first) heart attack thru diet
The Kosher Gourmet by Diane Rossen Worthington: Caprese is a light, fresh salad; the perfect quick and easy accompaniment to any summer meal
Mark Steyn: You Want Nazis?
Gabriel Schoenfeld: War Crimes in Gaza?
Jonathan Tobin: Care about the Jewish state's future? Obama, in interview, reveals even more reasons to worry
Alan M. Dershowitz: Confirmed: Needless death and destruction in Gaza
Katie Nielsen: As a mother, I'm all I need to be
Cameron Huddleston: 18 Retailers That Offer Price Adjustments
Nellie S. Huang: The Best Health Mutual Funds to Buy Now
Brierly Wright, M.S., R.D.: Try these 'secret-weapon' foods to boost your changes of losing weight
The Kosher Gourmet by Jessica Yadegaran: Take some relish in pickled goodies (5 recipes!)
Rabbi Berel Wein: Mission men
Mona Charen: The UN Prevents Peace
Mark A. Kellner: OMG: Is profanity losing its punch?
Kimberly Lankford: 50 Ways to Cut Your Health Care Costs
James K. Glassman: Investors, Are You Ready for the Next Global Crisis?
These foods can help keep your skin smooth and supple
Marsha McCulloch, M.S., R.D.: Think twice before giving up grains
The Kosher Gourmet by Nick Malgieri: Chocolate molten delight with creme anglaise is a simple yet elegant make-ahead dessert
We laughed at Jimmy Carter for carrying his suitcase into the White House. The government supplies aides to do that for presidents. Such humility is pretentious.
Other presidents have shown pretense in other ways. Ronald Reagan flew to Japan shortly after he retired and gave two speeches for a million dollars each. The Reagans said they needed it for their retirement, though modern presidents get a generous pension, lavish health care and a lot of other perks. It wasn't the Gipper's finest hour, but he had a lot of finer hours, and his friends gave him a pass.
George Washington was wealthy through his wife's estate, and he was appreciated for the strength and dignity of leadership. His wife, Martha, one of the richest women in the country, wore gowns of homegrown cotton, not imported silk, to promote fashion through support of American farmers.
Mitt Romney and his family wore their wealth more or less modestly, but they were part of the "1 percent," and that didn't sit well with the voters. Nobody knew much about Barack Obama, a senator serving his first term, but he appeared to live modestly, and the voters liked that. That was then, of course, and the "now" may be different.
The image of the presidents is colored by how they're perceived in relation to money, which is colored by background and the context of their moment in history. Ronald Reagan humbled "the evil empire," which trumped that trip to Japan. Jimmy Carter, modest and meek or not, had image problems with or without the suitcase. The two Bush presidents were born to wealth but never flaunted it.
The Clintons are something different. Hillary was born into the Midwest middle class, but Bubba sprang from a redneck culture in Arkansas, and together they pulled in different directions. She was first perceived in Little Rock as the thrifty Yankee wife, uncomfortable on the governor's small salary, who took tax deductions for his used underwear donated to the Salvation Army thrift store. His excesses were about sex.
Now the Clintons, flush with millions collected for their "charitable foundation," are playing in a higher league. They want everyone to believe they spend the money only on good deeds financed by foreign governments and the super rich who donate millions with no strings attached. Their life of luxury is eye-popping. The most recent perk is a full-size jetliner, provided by Canadian philanthropist Frank Giustra, for Bill's forays to foreign destinations in search of opportunities to do good. The plane, as described in The Washington Post, has a bedroom and is decorated with an art collection and a bath with gold-colored fixtures (but no swimming pool), and is "the core element of the new friendship between business mogul and political icon."
The good ol' boy from Arkansas and The Greater Gatsby bonded when Bill needed a ride to Latin America and the Gatsby offered to lend him his plane if he could go along to do a little business on the side. Bill has used the plane 26 times since their "bonding" in 2005, and Mr. Giustra has joined him for 13 of those trips.
Only last week, the Clinton Foundation acknowledged that an affiliated Canadian charity, founded in 2007 by Mr. Giustra, kept its donors secret despite Hillary's ethics agreement with the Obama administration that the foundation would reveal the names of foreign donors. The affiliation enabled the Clinton Foundation to have anonymous donors, including foreign executives with business before the government while Hillary was the secretary of state.
Bill has always been a problem for Hillary, but now it's his philanthropy, not his philandering, giving her campaign headaches. The former president tells NBC that he has no regrets for depending on the kindness of foreign strangers who give money to the foundation — or pay enormous fees to listen to him speak. Defending a $500,000 fee for a speech, Bubba seems to have lost his skill for deflecting political excess with rhetorical finesse. His excuse, that "I gotta pay our bills," echoes Hillary's tall tale that the family was "dead broke" when they left the White House 14 years ago. They're the Snopes family in a Faulkner novel, boorish without insight into their identity with new money.
When Bubba says the family charity has never done anything "knowingly inappropriate," like taking money to influence American foreign policy while Hillary was secretary of state, he's the familiar Bill Clinton parsing the meaning of what "is" is. This time there's no "is," because she destroyed her emails.
"I'm not in politics," he says, making a defense that defies satire. Harry Truman kept a carved motto on his White House desk to remind him that "the buck stops here." Bubba has rewritten the maxim: "The bunk starts here."
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© 2019 Creators Syndicate


Located on 36 PRIVATE acres of woods, trails, pasture, creek, wildflowers, birds, turkeys, deer, and other "critters", boasting views and spectacular sunsets.
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text:
The Neon Museum (page 2)
Neon Museum signs
These signs are owned by The Neon Museum. They were on display near the Fremont Street Experience when these photos were taken in 2006. The signs were moved to storage for several years. In 2018, the Andy Anderson, Red Barn, Chief Hotel Court, and some of the other signs were put on display at the Museum.
The Hacienda Hotel & Casino sign was built in 1967 by YESCO. The Hacienda was demolished in 1996 for the Mandalay Bay Hotel & Casino. The Hacienda sign was the first installation at the Neon Museum. For more, see these websites: 1, 2, 3, and 4.
The Andy Anderson sign was built by YESCO and installed on top of the new Anderson Dairy headquarters building in 1956. The sign may have been designed by Hermon Boernge. Andy was used in advertising until 1994. The sign was taken down in the late 1990s and restored by the Neon Museum. The sign was covered with plastic for protection and put on display near Fremont Street in 1997. The sign was removed around 2012 and put in storage. The sign is now on display at the Neon Museum. For more, see these websites: 1, 2, and 3.
The Red Barn was established as an antiques store in 1958. In the early 1960s, the store was converted into a bar and this sign was built by YESCO. The bar closed in 1988. When the bar was destroyed by fire, the sign was saved. It was restored and put on display here in 2000. These photos are from 2006. The sign was later moved into storage. In 2017, the sign was temporarily installed on Las Vegas Blvd. The location will feature rotating displays of signs from the museum's collection. This sign is now on display at the Neon Museum.
The Flame restaurant opened in 1961. It had a Western theme and was located directly across from the Silver Slipper. The restaurant's two, very similar signs were built by YESCO. The flames were rapidly lit in sequence from the center to the outside edge with white, blue, red, and pink neon. Sometime after 1970, the corrugated plastic text panels beneath the flames on both signs were changed. The pole sign in the parking lot originally read "Steaks" and the rooftop sign read "Entrance." The restaurant closed in 1993. The signs were removed just before the building was demolished and put in temporary storage at YESCO. Soon after that, The Neon Museum acquired the rooftop sign and the bottom part of the pole sign with its arrow. It is not known what happened to the pole sign's upper flame and plastic panels. In 1997, the museum restored the rooftop sign which is the smaller of the two. It is about 17 feet tall while the larger sign was about 25 feet tall. The rooftop sign was displayed at the Fremont Street Experience until 2013 when it was moved into storage. In 2019, the sign went back on display at the museum. It is lit and animated during daytime and evening tours. The larger sign's unrestored panel is also on display. For more, see these websites: 1 and 2.
The Chief Hotel Court sign was installed at the hotel around 1940. The text originally read Chief Autel Court. Autel was a popular name for auto hotel/motel at the time. The sign was restored and installed near the Fremont Experience in 1997. It then went into storage for several years. It is now on display at the Neon Museum. For more, see this website.
The Nevada Motel opened in 1937. This sign is from around 1950. This was the first sign to depict the Vegas Vic character. The sign was restored and put on display near the Fremont Experience in 2000. After being in storage for several years, it is now on display at the Neon Museum. For more, see this website.
The Dot's Flowers sign was built by YESCO around 1949. It was restored and put on display here in 2000. For more, see these websites: 1 and 2.
The Aladdin Hotel opened in 1966. The YESCO-designed sign featured Aladdin's Lamp at the top. The sign was updated in the 1980s with a rectangular one that incorporated the Lamp in its design. The hotel closed in 1997 and was demolished in 1998. The Lamp was saved, restored and put on display here in 1997. A new Aladdin Hotel opened in 2000. For more, see these websites: 1, 2, 3, and 4.
The Wedding sign was built in the mid-1940s by YESCO. It was restored and installed here in 2000. Las Vegas has been famous for quickie weddings since the late 1930s.
[daytime photos of Andy, Red Barn, Flame, Chief, Nevada Motel, Dot's, and the Wedding sign thanks Glenda Campbell]
signs in storage [gone]
These signs in storage belong to The Neon Museum. They were located near Cashman Center. In 2017, these signs were moved to a storage lot just south of the Museum. For more, see these websites: 1 and 2.
page 1 Neonopolis Las Vegas Reno Nevada
Main Signs Page


Zeeuwen In Hattrick (AllianceID: 6088) is a federation for Zeeuwen (people from Zeeland), people that live in Zeeland, and people with a strong connection to Zeeland and Zeeuwen. Since the federation was founded in December 2003, a large part of the Zeeuwen with supporter is member (around 45-50%). For example in July 2006 about 100 of the 260 Zeeuwen with supporter were a member in October 2010 about 90 out of 200 and in October 2011 82 out of 171.
Zeeuwen in Hattrick (ZiH) is a sociable federation with of course the mentality of Zeeuwen (laid back). The most famous activity organised by the federation is the Zeeuwse Cup (meaning: Cup of Zeeland). Which has been held every season since Dutch season 10 (January 2004). In Dutch season 38, August/September 2012, this knock-out tournament was held for the 29th time in succession. The number of entrants is usually about 40 to 60, often including some top teams. In the final rounds of the Cup, teams usually field their best players. The Zeeuwse Cup is not only accessible for members of ZiH, but for all Zeeuwen that play Hattrick. For all other activities of the federation the same principle counts, since the fed is here for all Zeeuwen, not just the ones with supporter.
Another activity organised by ZiH is a Youth competition series. This series is formed by introducing promotion and relegation between 5 to 7 competitions, with one top competition and thus one Youth champion every season.
This page was last edited on 14 August 2012, at 23:00.


New with tags Size L CONDITION: - A lot of Dirt - Overstretched straps because the dress was hanging at Herve Leger's. The straps need to be shortened like pinned on my mannequin. Perhaps sides will need to be adjusted too. MEASUREMENTS (flat, un-stretched): Bust 33.5" Waist 26.5" Hips 32.5" Length 36" Shipping: Domestic: the price includes mailing by USPS priority mail with tracking and insurance. Returns: Returns are accepted. You have to contact me and mail the dress back within 3 days after receiving the item. The item has to be returned in the same condition that you received it. If there are signs of wear or heavy perfume, the item will be mailed backed to you. The refund will be issued on the same day I received the item back. Shipping and 7% of the total price will not be refunded : it's a consignment fee that covers the costs of the selling fees paid upon closing the transaction and the cost of shipping to you.


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Running a marathon isn't easy but it is nothing compared to what my friend Guy went through. Guy lived round the corner when I was growing up (in York), we had an amazing friend circle and generally had some amazing memories as a bunch of teens finding their way through adolescence to adulthood. When Guy was 18 he was diagnosed with bone cancer. His treatment was gruelling and he went through so much for someone so young. He fully deserved to live a long and happy life but after being in remission for a couple of years his cancer returned and he died when he was just 21. Guy taught me to live life to it's fullest and to overcome challenge.
Fast forward quite a few years and after having 3 children I decided I needed a challenge. So over a year ago I began training for the York Marathon. The training has been tough and at times I considered pulling out (who knew broken toes hurt that much!) BUT after a pep talk from a certain Trialthlete (thanks JL) I began to think I could and would do the race.
I say 'race'...it will NOT be quick and for me an achievement will be getting round - let's just say the training plan (which I never actually got round to writing!!) didn't go to plan.


text:
Q: Getting last login by LIMIT 1 - PHP and MYSQL On my users account, I have a "last login" portion which displays the following:
<?php
     $getLog = "Select * from tblUserLogs where UserID = $id ORDER BY LogID DESC limit 1";
     $loadLog = mysql_query($getLog);
     while($Logs = mysql_fetch_array($loadLog)){
         $ID = $Logs['id'];
         $LastLogin = date('F j, Y, g:i a', strtotime($Logs['LastLog']));
         //$myLast = date('F j, Y, g:i a', $LastLogin);
         echo "<small>".$LastLogin."</small>";
    }
?>

However, it displays the current login date and time.
How should it be done? It should've been LIMIT 2 and display the smallest primary key. Is there a way to do it on the mysql statement?

A: I think what you're looking for is an offset, so you avoid the first entry.
LIMIT 1, 1

A: Either with a where (if you have a date column in your table)
SELECT * FROM tblUserLogs
WHERE UserId = <id>
AND loginDate <current login timestamp>
ORDER BY loginDate DESC

Or with a LIMIT 1,1 (Skip One, Take One)

A: check this answer https://stackoverflow.com/a/3574669/829533 and change the query
$getLog = "Select * from tblUserLogs where UserID = $id ORDER BY LogID DESC limit 1,1";