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

Inelastic scattering of polarized deuterons on hydrogen and nuclei
at high energies has been investigated during the last decade in Dubna
\cite{45_55}--\cite{lad3} and Saclay \cite{morlet,ljuda}.
The main goal of these studies is to investigate the properties
of the baryonic resonances via measurements of polarization
observables in the $(d,d^\prime)X$ reaction.

Since the deuteron is an isoscalar probe,
inelastic scattering of deuterons on hydrogen,
${\rm H}(d,d')X$, is selective  to the isospin $1/2$ and
can be used to obtain  information on the
formation of baryonic resonances $N^*(1440)$,
$N^*(1520)$, $N^*(1680)$, and others.
The measurements of analyzing powers, polarizations of the
scattered deuterons and different polarization transfers could
allow one to obtain the spin-flip probabilites of the $(d,d^\prime)$ reaction sensitive to the
quantum numbers of baryonic resonances.
The set of observables for the reconstruction of
the spin-flip probabilities in the $A(d,d^\prime)A^*$ has been proposed in ref.\cite{suzuki}.
Such an experiment has been realized at RIKEN \cite{satou} at 270 MeV to
study the excitation levels of ${\rm ^{12}C}$.

At the same time, inelastic scattering of deuterons
on nuclei at high transferred momenta
can be considered as a
complementary method to elastic
$pd$- and $ed$-scattering, deuteron breakup reaction,
electro- and photodisintegration of the deuteron
to investigate the deuteron spin structure at
short distances and to search for the manifestation of
non-nucleonic degrees of freedom.

However, due to lack of the experimental techniques to measure the polarization of
the high-energy deuterons, only tensor and vector analyzing powers
in the $(d,d^\prime)X$ reaction have been obtained in the vicinity of the baryonic
resonances excitation.

The tensor analyzing
power $T_{20}$ in the vicinity of the Roper resonance ($P_{11}(1440)$)
excitation  has been measured
on hydrogen and carbon targets at Dubna
\cite{45_55} and on
hydrogen  target at Saclay \cite{morlet}.
The measurements of $T_{20}$
in the deuteron scattering at 9 GeV/$c$ on hydrogen and carbon
have been performed for missing masses up to $M_X\sim 2.2$
GeV/$c^2$ \cite{azh9}. The experiments have shown a large negative
value of $T_{20}$ at momentum transfers of $t\sim -0.3$ (GeV/$c$)$^2$.
Such a behaviour of the tensor analyzing power has been interpreted
in the framework of the $\omega$-meson exchange model \cite{egle1} as due
to the longitudinal isoscalar form factor of the Roper resonance
excitation and deuteron form factors $t$-dependences \cite{egle2}.
The measurements of the tensor and vector
analyzing powers $A_{yy}$ and $A_y$ at  9 GeV/$c$ and 85 mrad of the
secondary deuterons emission angle in the vicinity of the
undetected system mass of $M_X\sim 2.2$ GeV/$c^2$ \cite{lad1} have shown
large values. The obtained results are in satisfactorily agreement with the
plane wave impulse approximation (PWIA) calculations \cite{nadia}.
It was pointed out that the spin-dependent part of
the $NN\to NN^*(\sim 2.2$~GeV/$c^2$)
amplitude is significant.
Recent measurements of  the tensor $A_{yy}$ and vector $A_y$ analyzing powers
in the vicinity of the excitation
of baryonic resonances with masses up to $\sim 1.8$ GeV/$c^2$ \cite{lad2,lad3}
demonstrated large spin effects and the sensitivity to the baryonic resonances properties.
The exclusive measurements   in the
${\rm H}(d,d')X$ reaction in the vicinity of the Roper resonance excitation
performed recently at Saclay \cite{ljuda} have also shown large values
of the $A_{yy}$ and $A_y$ analyzing powers.

In this paper we report  new results on the tensor and vector
analyzing powers $A_{yy}$ and $A_y$ in deuteron inelastic scattering
on hydrogen and carbon at the incident deuteron momentum of 9.0~GeV/$c$
and missing masses of undetected system of $\sim$ 2.0--2.6~GeV/$c^2$.
Details
of the experiment are described  in Section~\ref{sec:1}.  The comparison with
 existing
data and theoretical predictions is given in Section~\ref{sec:2}.
Conclusions are drawn in Section~\ref{sec:3}.

\section{\label{sec:1}Experimental procedure}

   The experiment has been performed using the polarized deuteron
beam at the  Dubna Synchrophasotron
and the SPHERE setup
\cite{lad1,lad2} described elsewhere
and shown in Fig.\ref{fig:1}.
The polarized deuterons were produced
by the ion source POLARIS \cite{polaris}.
The sign of  beam polarization  changed  cyclically and
spill-by-spill:   $"0"$, $"-"$, $"+"$, where $"0"$ means
the absence of  polarization, $"+"$ and $"-"$ correspond
to the sign of $p_{zz}$ with the quantization axis perpendicular
to the plane containing the mean beam orbit in the accelerator.

\begin{figure}
\resizebox{0.5\textwidth}{!}{
\includegraphics{fig1.ps}}
\caption{\label{fig:1} Schematic view of the experiment.
$M_i$ and $L_i$ are the magnets and quadrupole
lenses doublets, respectively;
$IC$ is an ionization chamber; $T$ is  a target;
$F_{61},~ F_{62},~F_{63}$  are trigger counters;
$F56_{1-4}$ are scintillation
counters and $HT$ is  a scintillation hodoscope
for TOF measurements;
$H0XY$ and $H0UV$  are beam profile hodoscopes.}
\end{figure}

The tensor polarization of the beam was
periodically  measured during the experiment using the
$A(d,p)X$ reaction at
zero emission angle and a proton momentum of $p_p\sim \frac{2}{3}p_d$
\cite{zolin}, using the same setup. It has been
shown that deuteron
breakup reaction in those
kinematical conditions has very large tensor analyzing power
$T_{20}= -0.82\pm 0.04$, independent of the atomic
number of the target
($A >$ 4) and of the momentum of the incident deuterons
between 2.5 and 9.0~GeV/$c$ \cite{t20br}.
The tensor polarization, corrected for
 dead time effect \cite{dtime}, and averaged over the
whole duration of the experiment   was
$p_{zz}^+=0.798\pm 0.002$(stat.)$\pm 0.040$(syst.) and
$p_{zz}^-=-0.803\pm 0.002$(stat.)$\pm 0.040$(syst.) in $"+"$ and $"-"$
beam spin states, respectively.

The vector polarization of the beam was
measured from the asymmetry
of quasi-elastic $pp$-scattering on a thin CH$_2$ target
placed   at focus $F4$ about 20~m upstream
of the setup \cite{f4,f4a}. The values of the vector polarization
were obtained using the results of asymmetry
measurements  at a momentum of 4.5~GeV/$c$ per nucleon
and  $8^\circ$  proton scattering angle. The
corresponding value of the effective analyzing power of the polarimeter
$A$(CH$_2$)  amounted $0.123\pm 0.006$ \cite{f4a}.
The vector polarization of the beam in different spin states was
$p_z^+=0.275\pm 0.016$(stat.)$\pm 0.014$(syst.) and
$p_z^-=0.287\pm 0.016$(stat.)$\pm 0.014$(syst.), respectively.

A slowly extracted deuteron beam with a typical intensity
of $5\times 10^8$ to $10^9$ $\vec{d}$/spill was directed onto
a liquid hydrogen target of 30 cm
length or onto carbon targets
with different length.
The beam intensity was monitored by
an ionization chamber placed in front of the target.
The beam positions and profiles at  certain points along the
beam were monitored
during each spill. The beam size at the target point was
$\sigma_x\sim 0.4$  cm and $\sigma_y\sim  0.9$ cm in the horizontal
and vertical directions, respectively.

Most of the data  were obtained
at secondary deuteron emission angles of 85, 130, and 160 mrad and
deuteron momenta between 4.5 and 7.0 GeV/c on hydrogen and carbon.
The secondary particles emitted  from the target
were transported  to  focus $F_6$ by
means of three bending magnets
and three quadrupole doublets.

    The measurements with empty target were performed
at secondary particle momenta of 4.5 and 6.0 GeV/$c$, while the measurements
without  target were carried out  at 4.5~GeV/$c$ only. The
ratio of the yields without target to a 7 cm carbon
target was less than $\sim 1\%$ for the both 85 mrad and 130 mrad detection angle.
The yield of particles for empty target was
$\sim 3.5\%$ and $\sim 11\%$ of the yield from  30 cm liquid hydrogen target
at 4.5 and 6.0 GeV/$c$, respectively,  independent of emission angle.

\begin{figure}
\resizebox{0.5\textwidth}{!}{
\includegraphics{fig2.eps}}
\caption{\label{fig:2} TOF spectra (in time-to-digit converter channel numbers) obtained for different setting of the
magnetic elements. The panels ($a$), ($b$), ($c$), ($d$), ($e$), and ($f$)
correspond to
secondary particles momenta of 4.5, 5.0, 5.5, 6.0, 6.5, and 7.0 GeV/$c$, respectively.}
\end{figure}

The coincidences of signals from
scintillation counters $F_{61}$, $F_{62}$  and $F_{63}$ were
used as a trigger. Along with the inelastically scattered deuterons, the
apparatus detected the protons originating from deuteron
fragmentation.
The time-of-flight
(TOF) information with a base line of $\sim$ 34 m between
start counter $F_{61}$ and  stop counters $F56_1$--$F56_2$,
$F56_3$--$F56_4$ and a scintillation hodoscope ${\rm HT}$ was used
for particle identification
in the off-line  analysis.
The TOF resolution was better
than $0.2$ ns ($1\sigma$).  The separation of the particles for different momenta of
the detected secondaries is demonstrated in Fig.\ref{fig:2}.
The panels ($a$), ($b$), ($c$), ($d$), ($e$) and ($f$)
correspond to
secondary particle momenta of
4.5, 5.0, 5.5, 6.0, 6.5, and 7.0 GeV/$c$, respectively.
One can see that the relative contribution of
protons becomes more pronounced with
decreasing momentum.
The residual background was eliminated completely by
the requirement that particles are detected at least in two prompt
TOF windows.

The acceptance of the setup was
determined via Monte Carlo simulations, taking into account
the parameters of the incident deuteron beam,
nuclear interactions and multiple scattering  in the target,
in the air, in the windows and detectors, energy losses of primary
and secondary deuterons.
The momentum and polar angle  acceptances were
${\Delta p}/{p}\sim\pm ~2\%$ and $\pm 8$ mrad, respectively.

\begin{figure}
\resizebox{0.5\textwidth}{!}{
\includegraphics{fig3.eps}}
\caption{\label{fig:3} The kinematical plot of the missing mass $M_X$ versus 4-momentum
$t$ at the initial deuteron momentum 9.0 GeV/$c$.
The solid line correspond to the conditions (middle of the acceptance)
of the experiment  performed at zero angle \cite{azh9}.
The shadowed areas $a$, $b$, and $c$ demonstrate the regions of 4-momentum $t$ and
missing mass $M_X$ covered  within the acceptance
of the present experiment at the deuteron detection angles
of $\sim 85$, $\sim 130$, and $\sim 160$ mrad,
respectively.}
\end{figure}

The missing mass values $M_X$  were
calculated under the assumption that the
reaction occurs on a  target with proton mass.
In this case, the 4-momentum transfer $t$ and the missing mass $M_X$ are
related as follows
\begin{eqnarray}
\label{MXt}
M_X^2 = t + m_p^2 + 2m_pQ,
\end{eqnarray}
where $m_p$ is the proton mass and $Q$ is the energy difference
between  incident and scattered deuteron. The
shadowed areas $a$, $b$, and $c$  in the kinematic
plot given in Fig.\ref{fig:3} demonstrate the regions of 4-momentum $t$ and
missing mass $M_X$ covered  by the acceptance setup
in the present experiment at detection angle of $\sim$85, 130, and 160 mrad, respectively.
The solid line corresponds to an initial deuteron momentum of
9.0 GeV/$c$
and zero emission angle \cite{azh9}. One can see
that the conditions of the present experiment allow one to
significantly extend
the $t$ range of measurements for
missing masses $M_X \sim$2.2--2.6~GeV/$c^2$.

The tensor $A_{yy}$ and vector $A_y$ analyzing powers
were calculated from
the numbers of protons $n^+$, $n^-$ and $n^0$, detected for different
states of the beam polarization,
normalized to the corresponding
beam intensities and corrected for the  dead time effect \cite{dtime}.
The calculations were carried out by the expressions
\begin{eqnarray}
\label{ayy}
A_{yy} &=& 2~ \frac{p_z^-~(n^+/n^0-1)
~-~p_z^+~ (n^-/n^0-1)}{p_z^- p_{zz}^+ - p_z^+ p_{zz}^-},\nonumber\\
A_{y} &=& -\frac{2}{3}~
\frac{p_{zz}^-~ (n^+/n^0-1)
~-~p_{zz}^+~ (n^-/n^0-1)}{p_z^- p_{zz}^+ - p_z^+ p_{zz}^-}.
\end{eqnarray}
{These expressions,  taking into account
different values of polarization in different beam spin states,
are simplified significantly when
$p_z^+ = p_z^-$ and $p_{zz}^+ = - p_{zz}^-$.}
The systematic errors due to the uncertainty of the polarization
measurements were
$\sim 5\%$ for both the tensor and vector analyzing powers.

\section{\label{sec:2}Results and discussion}

\begin{table}
\caption{\label{tab:table1} Results on the tensor $A_{yy}$ and vector $A_y$ analyzing powers of the
${\rm ^1H}(d,d^\prime)X$ reaction
at initial deuteron momentum 9 GeV/$c$.
($\theta$ and $P$  are the polar angle and momentum of the secondary deuteron, respectively;
$\Delta P$ is momentum acceptance of the setup (FWHM), $t$ is
4-momentum transfer, $M_X$ is missing mass.)}
\begin{ruledtabular}
\begin{tabular}{ccccccc}
$\theta$, & $P$, & $\Delta P$, & $t$, & $M_X$, & $A_{yy}\pm$ &  $A_y\pm$ \\
mrad & GeV/$c$ & GeV/$c$ & (GeV/$c$)$^2$ &  GeV/$c^2$  & $\Delta A_{yy}$ & $\Delta A_y$\\
\hline
0.085 & 4.541 & 0.095 & -1.875 & 2.651 & -0.110$\pm$ &  0.037$\pm$ \\
      &       &       &        &       &  0.294~~    &  0.283~~ \\
0.085 & 5.041 & 0.105 & -1.466 & 2.562 & -0.013$\pm$ & -0.183$\pm$\\
      &       &       &        &       &  0.074~~    &  0.196~~ \\
0.085 & 6.047 & 0.125 & -0.940 & 2.302 &  0.066$\pm$ &  0.189$\pm$ \\
      &       &       &        &       &  0.065~~    &  0.062~~ \\
0.085 & 6.554 & 0.137 & -0.782 & 2.132 &  0.053$\pm$ &  0.174$\pm$\\
      &       &       &        &       &  0.041~~    &  0.039~~ \\
0.130 & 4.555 & 0.096 & -2.246 & 2.575 &  0.061$\pm$ & -0.277$\pm$ \\
      &       &       &        &       &  0.247~~    &  0.235~~ \\
0.130 & 5.051 & 0.109 & -1.883 & 2.475 &  0.042$\pm$ & -0.092$\pm$ \\
      &       &       &        &       &  0.165~~    &  0.156~~ \\
0.130 & 6.061 & 0.130 & -1.446 & 2.184 & -0.024$\pm$ &  0.101$\pm$\\
      &       &       &        &       &  0.047~~    &  0.045~~ \\
\end{tabular}
\end{ruledtabular}
\end{table}

The data on $A_{yy}$ and $A_y$ with the statistical errors for
the ${\rm ^1H}(d,d^\prime)X$ and  ${\rm ^{12}C}(d,d^\prime)X$ are presented
in the Tables {\ref{tab:table1} and {\ref{tab:table2}, respectively.

\begin{figure}
\resizebox{0.5\textwidth}{!}{
\includegraphics{fig4.eps}}
\caption{\label{fig:4} Tensor analyzing power $A_{yy}$ in the $(d,d^\prime)X$ reaction obtained at  9
GeV/$c$. The symbols are explained in the text. The solid, dashed, dotted
and dash-dotted lines are predictions in the framework of
PWIA \cite{nadia} using
DWFs for Paris \cite{paris} and Bonn A, B and C \cite{bonn}
potentials, respectively.}
\end{figure}

The results of the present experiment on the tensor analyzing power $A_{yy}$
in the $(d,d^\prime)X$ reaction are shown in Fig.\ref{fig:4} as a function of the
transferred 4-momentum  $t$.
The open circles, triangles and squares are the data obtained on a carbon target
at detection angles of $\sim 85$,
$\sim 130$, and $\sim 160$ mrad, respectively. The cross and star correspond to the $A_{yy}$
data for a carbon target taken at $\sim 115$ and $\sim 145$ mrad.
The filled circles and triangles denote
 the data obtained on a hydrogen target at $\sim 85$ and
$\sim 130$ mrad, respectively.     The data of the
present experiment are compared with
the data taken at zero angle on hydrogen~\cite{azh9} given by the diamonds.
One can see that the values of $A_{yy}$ obtained at different emission angles are in good
agreement demonstrating an approximate $t$-scaling observed in
 earlier experiments
\cite{45_55}-\cite{lad3}.
The present data along with the data from previous experiments
allow one to trace the general behaviour
of $A_{yy}$   over a wide region of $|t|$.
At small $|t|$ ($\le 0.3$~(GeV/$c$)$^2$), $A_{yy}$
rises linearly up to a
value of $\sim 0.4$,
then it smoothly decreases towards zero at $|t|\sim$ 1.0--1.4~ (GeV/$c$)$^2$.

\begin{table}
\caption{\label{tab:table2} Results on the tensor $A_{yy}$ and vector $A_y$ analyzing powers of the
${\rm ^{12}C}(d,d^\prime)X$  reaction
at initial deuteron momentum 9 GeV/$c$.
($\theta$ and $P$ are the polar angle and momentum of the secondary deuteron, respectively;
$\Delta P$ is  momentum acceptance of the setup (FWHM), $t$ is
4-momentum transfer, $M_X$ is missing mass.)}
\begin{ruledtabular}
\begin{tabular}{ccccccc}
$\theta$, & $P$, & $\Delta P$, & $t$, & $M_X$, & $A_{yy}\pm$ &  $A_y\pm$ \\
mrad & GeV/$c$ & GeV/$c$ & (GeV/$c$)$^2$ &  GeV/$c^2$  & $\Delta A_{yy}$ & $\Delta A_y$\\
\hline
0.085 & 4.544 & 0.089 & -1.873 & 2.650 & -0.156$\pm$ &  0.470$\pm$ \\
      &       &       &        &       &  0.329~~    &  0.314~~ \\
0.085 & 5.050 & 0.098 & -1.460 & 2.559 &  0.133$\pm$ &  0.264$\pm$ \\
      &       &       &        &       &  0.224~~    &  0.213~~ \\
0.085 & 5.606 & 0.105 & -1.094 & 2.429 &  0.006$\pm$ &  0.161$\pm$ \\
      &       &       &        &       &  0.079~~    &  0.075~~ \\
0.085 & 6.109 & 0.116 & -0.875 & 2.285 &  0.096$\pm$ & -0.070$\pm$ \\
      &       &       &        &       &  0.054~~    &  0.051~~ \\
0.085 & 6.616 & 0.126 & -0.719 & 2.113 &  0.103$\pm$ &  0.134$\pm$ \\
      &       &       &        &       &  0.031~~    &  0.030~~ \\
0.085 & 7.117 & 0.131 & -0.625 & 1.911 &  0.169$\pm$ &  0.120$\pm$ \\
      &       &       &        &       &  0.029~~    &  0.027~~ \\
0.115 & 6.587 & 0.131 & -1.138 & 2.024 &  0.029$\pm$ &  0.147$\pm$\\
      &       &       &        &       &  0.032~~    &  0.030~~ \\
0.130 & 4.563 & 0.087 & -2.254 & 2.570 & -0.048$\pm$ &  0.100$\pm$\\
      &       &       &        &       &  0.219~~    &  0.208~~ \\
0.130 & 5.070 & 0.096 & -1.889 & 2.467 & -0.303$\pm$ &  0.298$\pm$ \\
      &       &       &        &       &  0.247~~    &  0.235~~ \\
0.130 & 5.590 & 0.107 & -1.638 & 2.321 & -0.079$\pm$ &  0.257$\pm$ \\
      &       &       &        &       &  0.107~~    &  0.102~~ \\
0.130 & 6.094 & 0.116 & -1.476 & 2.156 & -0.035$\pm$ &  0.023$\pm$ \\
      &       &       &        &       &  0.039~~    &  0.037~~ \\
0.145 & 6.097 & 0.118 & -1.694 & 2.104 &  0.035$\pm$ &  0.087$\pm$ \\
      &       &       &        &       &  0.064~~    &  0.061~~ \\
0.160 & 4.590 & 0.091 & -2.589 & 2.490 & -0.066$\pm$ &  0.275$\pm$ \\
      &       &       &        &       &  0.214~~    &  0.204~~ \\
0.160 & 5.095 & 0.097 & -2.272 & 2.373 & -0.024$\pm$ &  0.155$\pm$ \\
      &       &       &        &       &  0.102~~    &  0.097~~ \\
0.160 & 5.600 & 0.109 & -2.060 & 2.225 & -0.026$\pm$ &  0.044$\pm$ \\
      &       &       &        &       &  0.055~~    &  0.053~~ \\
\end{tabular}
\end{ruledtabular}
\end{table}

The data obtained on hydrogen and carbon targets are in good
agreement.
The observed independence of the tensor analyzing power on the
atomic number of the target indicates that rescattering in
the target and medium effects  are small. Hence, nuclear targets
are  appropriate to obtain information  on baryonic
excitations in inelastic  deuteron scattering.

\begin{figure}
\resizebox{0.5\textwidth}{!}{
\includegraphics{fig5.eps}}
\caption{\label{fig:4a} Diagrams representing mechanisms of baryonic excitation
in  deuteron--nucleon collisions:
($a$) plane wave impulse approximation; ($b$) and
($c$) double-collision mechanism; ($d$)
$\omega$-meson exchange mechanism.}
\end{figure}

The results on the tensor $A_{yy}$ and vector $A_y$ obtained at 9 GeV/$c$ and 85 mrad\cite{lad2}
 and at 5 GeV/$c$ and 178 mrad \cite{lad3} have been satisfactorily explained in the framework of the
PWIA approach \cite{nadia} (see diagram in Fig.~\ref{fig:4a}$a$).
In this model the tensor and vector analyzing powers are expressed in terms of
three amplitudes ($T_{00}$, $T_{11}$ and $T_{10}$) defined by the deuteron
structure and  the ratio $r$ of the spin-dependent to spin-independent
parts of the elementary process $NN\to NN^*$ in the vicinity of $\sim 2.2$ GeV/$c^2$:
\begin{eqnarray}
\label{ayyr}
A_{yy}(q) &=& \frac{T_{00}^2 - T_{11}^2 +  4 r^2 T_{10}^2}
{T_{00}^2 + 2 T_{11}^2 +  4 r^2 T_{10}^2},\\
\label{ayr}
A_y(q) &=& 2\sqrt{2} r \frac{(T_{11}+T_{00})T_{10}}
{T_{00}^2 + 2 T_{11}^2 +  4 r^2 T_{10}^2}.
\end{eqnarray}

Amplitudes
$T_{00}$ and  $T_{11}$
depend on the deuteron wave function:
\begin{eqnarray}
\label{t00}
T_{00} &=& S_0(q/2)+{\sqrt{2}}S_2(q/2),\nonumber\\
T_{11} &=& S_0(q/2)-\frac{1}{\sqrt{2}}S_2(q/2),
\end{eqnarray}
where $S_0$ and $S_2$ are the spherical and quadrupole form factors
of the deuteron expressed in the following manner:
\begin{eqnarray}
\label{quad}
S_0(q/2) & = & \int^{\infty}_0 (u^2(r) + w^2(r)) j_0(rq/2) dr, \nonumber\\
S_2(q/2) & = & \int^{\infty}_{0} {2} w(r) \left ( u(r) - \frac{1}{2\sqrt{2}}w(r) \right )
j_2(rq/2) dr.
\end{eqnarray}
Here, $u(r)$ and $w(r)$  are $S$-- and  $D$--
waves of the deuteron in coordinate space, respectively,
$j_0(qr/2)$ and $j_2(qr/2)$
are the Bessel functions of  zero and second order, respectively, and $q^2 = -t$.

The amplitude $T_{10}$
is also function of $S$-- and $D$-- waves of the deuteron
\begin{eqnarray}
\label{t10}
T_{10} = & & \frac{{\it i}}{\sqrt{2}}
\int^{\infty}_0 \left (u^2(r) - \frac{w^2(r)}{2}\right ) j_0(rq/2)
dr+\nonumber\\
+& &\frac{{\it i}}{2}\int^{\infty}_{0} w(r) \left ( u(r) +
\frac{w(r)}{\sqrt{2}} \right )
j_2(rq/2) dr .
\end{eqnarray}
One can see that in the framework of the PWIA model \cite{nadia},
the vector analyzing power $A_y$ is proportional to  the ratio $r$,
while the tensor analyzing power $A_{yy}$ is defined mostly by the deuteron structure.

\begin{figure}
\resizebox{0.5\textwidth}{!}{
\includegraphics{fig6.eps}}
\caption{\label{fig:6} Comparison of the tensor analyzing power $A_{yy}$ in the $(d,d^\prime)X$ reaction
from the present experiment with the $A_{yy}$ data in deuteron-proton elastic scattering
at 3.43 GeV/c \cite{blez} (diamonds).
The symbols for the $(d,d^\prime)X$ reaction data and curves are
the same as in Fig.\ref{fig:4}.}
\end{figure}

The curves shown in Fig.\ref{fig:4}
are the results of PWIA calculations \cite{nadia} with different
deuteron wave functions. The solid line
is calculated with the deuteron wave function (DWF) for the Paris
potential \cite{paris},
while  the dashed, dotted and dash-dotted lines
correspond to the DWFs for Bonn A, B and C potentials \cite{bonn},
respectively.

The deviation of
the data obtained in the previous experiments \cite{45_55,lad2}
at $|t|\sim$~ 0.3--0.8~(GeV/$c$)$^2$
from the predictions of PWIA, as well as from
$dp$- \cite{blez} and $ed$- \cite{ed} elastic scattering,
indicates the sensitivity of $A_{yy}$ to the
baryonic resonances excitation.
In the framework of the multiple-scattering model, such a deviation
may be due to a significant contribution of double-collision
interactions
corresponding to the diagrams shown in Figs.\ref{fig:4a}$b$ and \ref{fig:4a}$c$.
The diagram of Fig.\ref{fig:4a}$b$ describes the situation, where the
resonance is formed in the second $NN$ collision whereas
the resonance in the case of Fig.\ref{fig:4a}$c$,
formed in the first $NN$ interaction, is
then elastically scattered  on  the second nucleon
of the deuteron. The calculations have shown that the contribution
of the double-scattering terms
is significant for $|t|$ greater than $\sim$ 0.4 (GeV/$c$)$^2$
\cite{azhgirey2}. Therefore, in the framework of the multiple-scattering
model, the behaviour of the tensor analyzing power $A_{yy}$ is defined
by the spin structure of the deuteron and the elementary amplitudes
of the $NN\to NN^*$ and $NN^*\to NN^*$ processes.

     The sensitivity of the tensor analyzing power in deuteron
 inelastic scattering off protons to the
excitation of baryonic resonances is
pointed out   in the framework of the $t$-channel
$\omega$-meson  exchange model \cite{egle1}. The diagram corresponding
to this model is shown in Fig.\ref{fig:4a}$d$.  The cross section and
polarization observables can be calculated from the known
electromagnetic properties of the deuteron and baryonic resonances
$N^*$ through the vector dominance model. The details of the
model are given in \cite{egle1,egle2}.
This model satisfactorily explained  the $A_{yy}$ data in the $(d,d^\prime)X$ reaction in the vicinity of low masses baryonic resonances
\cite{45_55,azh9,lad2}.
In principle, this model can be applied for the explanation of the data of
present experiment, however, the knowledge of the electromagnetic properties
of the baryonic resonances with the masses 2.2--2.6 ~ GeV/$c^2$
is required.

Fig. \ref{fig:6} demonstrates
the different behavior of the tensor analyzing powers in the $(d,d^\prime)X$
process obtained in the present experiment and in
$dp$- \cite{blez} elastic scattering, indicating different contribution of
the double scattering at large $|t|$.
One can see also, that the  present $A_{yy}$ data are in reasonable agreement with
the PWIA prediction in the range of transferred 4-momentum $|t|$ of 0.9--1.2
(GeV/$c$)$^2$.

\begin{figure}
\resizebox{0.5\textwidth}{!}{
\includegraphics{fig7.eps}}
\caption{\label{fig:7} Vector analyzing power $A_{y}$ in the $(d,d^\prime)X$ reaction
from the present experiment compared with the
PWIA predictions \cite{nadia} using different DWFs.
}
\end{figure}

The data on the vector analyzing power $A_y$ obtained in
the present experiment are plotted in Fig.\ref{fig:7} versus $t$.
The symbols corresponding to the data obtained in different
kinematic conditions are the same as in Fig.\ref{fig:4}.
It should be noted that
the data obtained on hydrogen and carbon are in good agreement.
The curves are obtained using the expression (\ref{ayr}) with
the ratio $r$ of the
spin-dependent to spin-independent parts of the $NN\to NN^*$ process
taken in the form
\begin{eqnarray}
\label{r04}
r=a\cdot q
\end{eqnarray}
with the value of $a=0.4$ \cite{nadia}.
The solid curve in Fig.\ref{fig:7}
is obtained with the DWF for the Paris potential \cite{paris},
while  the dashed, dotted and dash-dotted lines
correspond to the DWFs for Bonn A, B and C potentials \cite{bonn},
respectively.
The PWIA calculations give approximately the same results
at the value of $a\sim$~0.3--0.5.
It should be noted that $a$  might
be different for different $M_X$, however,
we took the fixed value  for simplicity
due to the lack of data.
The observed relatively large value of $A_y$ at $|t|\sim$
1~ (GeV/$c$)$^2$ can be interpreted as being due to  a significant
role of the spin-dependent part of the elementary amplitude of the
$NN\to NN^*$ reaction.

\section{\label{sec:3}Conclusion}

     We have presented data on the tensor and vector analyzing
powers $A_{yy}$ and $A_y$
in inelastic scattering $(d,d^\prime)X$ of 9.0 GeV/$c$ deuterons
on hydrogen and carbon
in the vicinity of
the excitation of baryonic masses of
 $\sim$2.2--2.6 GeV/$c^2$. This corresponds to the range of 4-momentum
$|t|$ between 0.7 and 2.5 (GeV/$c$)$^2$.

The data obtained on hydrogen and carbon targets are in good
agreement.
The observed independence of the analyzing powers on the
atomic number of the target indicates that rescattering in
the target and medium effects  are small. Hence, nuclear targets
are also appropriate to obtain information  on the baryonic
excitation in
inelastic deuteron scattering \cite{45_55}-\cite{lad3}.

The observed difference of the $A_{yy}$ data
at $|t|\le$ 0.8~(GeV/$c$)$^2$
with the PWIA calculations \cite{nadia} using
standard deuteron wave functions as well as with the data obtained in $dp$- \cite{blez} and  $ed$-elastic scattering \cite{ed} indicates the sensitivity of $A_{yy}$ to
baryonic resonance excitation via
double-collision
interactions \cite{azhgirey2}. On the other hand, both $A_{yy}$ and $A_y$ data
are in reasonable
agreement with PWIA calculations \cite{nadia} at $|t|\sim$  1 ~(GeV/$c$)$^2$.

The large values of $A_y$ show a significant
role of the spin-dependent part of the elementary amplitude of the
$NN\to NN^*$ reaction in the vicinity of the baryonic masses excitation  $M_X\sim$2.2~GeV/$c^2$.

\begin{acknowledgments}

Authors express their gratitude to  Prof.~A.I.Malakhov, Director of
LHE, and Prof.~V.N.Penev for their permanent help.
Authors are grateful to the LHE accelerator staff and POLARIS team
for providing good conditions for the
experiment.
They thank to
L.V.~Budkin, V.P.~Ershov,
V.V.~Fimushkin,
A.S.~Nikiforov,
Yu.K.~Pilipenko,
V.G.~Perevozchikov,  E.V.~Ryzhov, A.I.~Shirokov, and O.A.~Titov  for their
assistance during the experiment.
Authors thank also A.N.~Prokofiev and A.A.~Zhdanov for the lending
of the scintillation counters for the polarimeter.
They are indebted to  Prof.~E.Tomasi-Gustafsson  for helpful
discussions.
This work was supported in part by the Russian Foundation
for Basic Research under grants
No.~03-02-16224 and No.~04-02-17107.
\end{acknowledgments}

redpajama_set_name: RedPajamaArXiv


text:
91% of Czech Ski Resorts Are Open; More to Open In The Coming Days
BD Staff January 20, 2020 91% of Czech Ski Resorts Are Open; More to Open In The Coming Days2020-01-20T11:04:30+01:00 Czech Republic, Travel
According to the Association of Mountain Resorts (AHS), 91% of ski resorts are currently in operation in the Czech mountains. Photo: Klinovec. Credit: Czech Tourism.
Brno / Czech Rep., Jan 20 (BD) – The downhill routes in the resorts have opened already, and other routes are coming into operation gradually.
Photo: Bramberk. Credit: Czech Tourism.
Two thirds of the ski-lifts and cable cars are in operation.
Photo: Spindleruv Mlyn. Credit: Czech Tourism.
"We expect that the period from the second half of January will be more favorable for skiers. The cold front will come after this weekend, bringing snowfall in the mountains. As a result, we expect the launch of other routes," said Libor Knot from AHS.
Photo: Lipno. Credit: Czech Tourism.
Get the news first! Subscribe to our daily newsletter here. Top stories of the day in your mailbox every morning.
https://brnodaily.com/2020/01/20/travel-tips/91-of-czech-ski-resorts-are-open-more-to-open-in-the-coming-days/https://brnodaily.com/wp-content/uploads/2020/01/Klínovec-lanovka-credit-czech-tourism-1024x768.jpeghttps://brnodaily.com/wp-content/uploads/2020/01/Klínovec-lanovka-credit-czech-tourism-150x113.jpeg 2020-01-20T11:04:25+01:00 BD StaffCzech RepublicTravelCzech Republic,Skiing,Sport,Travel TipsAccording to the Association of Mountain Resorts (AHS), 91% of ski resorts are currently in operation in the Czech mountains. Photo: Klinovec. Credit: Czech Tourism. Brno / Czech Rep., Jan 20 (BD) - The downhill routes in the resorts have opened already, and other routes are coming into operation gradually. ...BD StaffBD Staff team@brnodaily.czAdministratorBrno Daily - English News and Events in Brno.Brno Daily
Czech Republic, Skiing, Sport, Travel Tips
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redpajama_set_name: RedPajamaCommonCrawl


Please report any suspected cruelty or neglect of an animal in strictest confidence.
Address: Galway SPCA, 2a Augustine Street, Galway.
The helpline will be operational from the 3rd of January 2012. It will be manned from 2pm to 5pm Monday to Friday (excluding Bank Holidays). At all other times it will divert to a recorded message, and messages left will be monitored regularly.
Report lost or found pets (please include brief description, contact information and a photograph).
You will receive an automated response with helpful advice and your listing will be shared on our facebook page. Our Facebook page is run by volunteers so please be patient.
Posting details and a photo of your lost or found pet on the following websites will give you a much greater chance of finding your pet or its owner and all listings posted to the LostandFoundPets.ie website will be shared automatically across several social media sites. In addition, Galway listings are posted to our Facebook page.
It is a requirement to notify local Gardai first but also important to contact your local Dog Warden, Animal Rescues and Vets. Here is a list of Galway based contacts.
Find out about pets for adoption, fostering and volunteering opportunities.
The Galway SPCA are always in need of foster parents for cats and dogs who may be injured or in need of one-to-one attention. Please send us your name for our list of foster parents and help our animals get better faster.
Our adoption pages are kept as up to date as possible however it is best to ring the number provided with the animal's details to check availability as they may already have been rehomed, fostered or reserved.
Please note, homechecks are done before any of our animals are rehomed and we do ask for a donation to help towards the cost of vaccinations, neutering, worming etc. If you are considering adopting from us please first have a read of our adoption policy.
Now have a look at all the wonderful dogs and cats that are available for adoption right now in our sanctuaries.
Please go to the donate page.
Galway SPCA's fan page on Facebook is dedicated to the pets of Galway and beyond who are lost, found or in need of a home. Feeds from the very popular website Lost and Found Pets Ireland will also appear here automatically. So by becoming a fan of our page, our updates will appear in your newsfeed as soon as they are posted. You can really help us by sharing the stories and photos posted to our fan page and on twitter and get the word out to a wider audience.
Address: Galway SPCA Animal Sanctuary, Heathlawn, Killimor, Co. Galway.
Cattery: 087 7951961 (Wendy) 089 4749127 (Trish).
If we are in the kennels or cattery please leave a message on our answering machine with your name, number and the name of the dog or cat you are interested in and we will call you back as soon as possible.
Directions: From Galway, take Dublin Road. Go through Loughrea. 2 miles past Loughrea take right turn to Portumna. Go through Killimor Village (about 10 miles) and take the third turn approximately 2 miles past Killimor Village. If you get to a huge electricity pylon on right, you have gone too far!
Our charity shop is open 6 days a week and we would welcome anyone who has a few hours to spare to help behind the counter, ironing clothes, sorting stock etc. Our shop is a major source of income for us so we need to ensure that it is sufficiently manned at all times. Please give your name and contact details to the office if you would like to help. No previous shop experience is necessary - just a willing attitude and a pleasant manner. Also, we are always grateful for your second-hand clothing and household goods. Just ensure please that they are of good quality - please no jumble or worn electrical goods.
All committee members can be contacted through the main office in Galway.
The Galway Society for the Prevention of Cruelty to Animals have been in Galway for roughly twenty years. From humble beginnings where we looked after animals in our homes, we have progressed to now having a shelter in Heathlawn, Killimor, Co. Galway and a shop, offices and cattery in Galway City. We now also have a full time field inspector covering Galway city and county. We daily strive to improve the welfare of all animals both locally and internationally through education, assistance, advice and the wonderful world of the internet and email. Indeed we are very lucky to have two papers featuring the animals in our care and we thank the Galway Advertiser and Tuam Herald for allowing us the space to feature our pets of the week. Over the years we have developed a good working relationship with all the local media be it paper, radio, TV and they are always available to help in any way they can.
Aims: The aims of the Galway SPCA include: (a) The prevention of cruelty to domestic and wild animals, including birds, and the fostering of knowledge of the behaviour and proper care of animals amongst the public and particularly amongst the youth of Galway City and County. (b) Provision for the treatment of injured and sick animals (including wild animals and birds) where these are the property of persons who cannot afford professional fees or where their owner is unknown. (c) Provision of food and shelter for unwanted or stray animals, to find homes for them.. We operate a no-kill policy ( unless it is a fatal injury or illness ). (d) The undertaking of an active campaign to publicize the aims of the Branch and the utilisation of the media to disseminate information, increase public awareness of the need for proper consideration of animal welfare and to highlight present practices which condone animal abuse. (e) The lobby of both local and national government on issues concerning animal welfare where such lobbying would have the effect of improving the overall quality of life of animals.
Approach: The Galway SPCA is of the opinion that change in these areas is necessary and should be brought about by increasing public awareness, placing pressure on government bodies and representatives to legislate for change and to foster general awareness of the issue of animal welfare.
Submissions to Happy Endings: The Happy Endings page is where you can read about some of the successful adoptions from Galway SPCA. If you have adopted a pet from us we would love to hear from you, just send a photo or two and a little story to the following email address: webmaster@galway-spca.com.


Founded in 2008, KEGU Power has become one of the leading LED driver solution provider in China. Our customers include most of the major domestic lighting manufacturers and some world-renowned multinationals in lighting industry.
Driven by a well-experience R&D team with professors and senior engineers, KEGU Power is making a consistent effort to provide highly reliable and efficient LED drivers at better cost.
Our LED drivers have independent intellectual properties and have obtained domestic and international certificates such as TUV, SEMKO, CE, RoHS, CQC. As an ISO9001: 2008 manufacturer running with advanced ERP system, we are making a serious commitment to quality, service and delivery.
In 2012, we launch our ground-breaking intelligent LED lights to the market. Integrated with microwave sensor, daylight sensor, lux controller and dimmer and powered by our own driver, our intelligent LED lights are even 50% energy saving than general LED lights. They offer a perfect solution for many lighting applications like hotel, parking, corridor, office, school, factory ect.
KEGU Power would like to work with customers worldwide and launch new solutions and products to meet the ongoing challenges on innovation and quality. OEM and ODM are welcome!


text:
Q: How to make a horizontal stacked histplot based on counts? I have a df which represents three states (S1, S2, S3) at 3 timepoints (1hr, 2hr and 3hr). I would like to show a stacked bar plot of the states but the stacks are discontinous or at least not cumulative. How can I fix this in Seaborn? It is important that time is on the y-axis and the state counts on the x-axis.

Below is some code.
data = [[3, 2, 18],[4, 13, 6], [1, 2, 20]]
df = pd.DataFrame(data, columns = ['S1',  'S2', 'S3'])
df = df.reset_index().rename(columns = {'index':'Time'})
melt = pd.melt(df, id_vars = 'Time')

plt.figure()
sns.histplot(data = melt,x = 'value', y = 'Time', bins = 3, hue = 'variable', multiple="stack")

EDIT:
This is somewhat what I am looking for, I hope this gives you an idea. Please ignore the difference in the scales between boxes...

A: If I understand correctly, I think you want to use value as a weight:
sns.histplot(
    data=melt, y='Time', hue='variable', weights='value',
    multiple='stack', shrink=0.8, discrete=True,
)

A: This is pretty tough in seaborn as it doesn't natively support stacked bars.  You can use either the builtin plot from pandas, or try plotly express.
data = [[3, 2, 18],[4, 13, 6], [1, 2, 20]]
df = pd.DataFrame(data, columns = ['S1',  'S2', 'S3'])
df = df.reset_index().rename(columns = {'index':'Time'})
# so your y starts at 1
df.Time+=1

melt = pd.melt(df, id_vars = 'Time')
# so y isn't treated as continuous
melt.Time = melt.Time.astype('str')

Pandas can do it, but getting the labels in there is a bit of pain.  Check around to figure out how to do it.
df.set_index('Time').plot(kind='barh', stacked=True)

Plotly makes it easier:
import plotly.express as px
px.bar(melt, x='value', y='Time', color='variable', orientation='h', text='value')

redpajama_set_name: RedPajamaStackExchange


text:
Q: What to check when finding a replacement disk I have recently joined a company where we provide hardware support. Often we have to replace hard disks for servers (Dell/IBM) and the hdd models that were used when the servers were built are no longer available.
My question is when finding a replacement disk, what do you check? I generally check storage size, speed (rpm), form factor (2.5/3.5). Do we have to ensure that transfer speed (Gbps) also matches? What else do we have to check? Is there any online utility that can help?
Also do we have to match cache?

A: I previously worked as a technician in electronic recycling operation, so this question is right down my alley.
One of the things you should be aware is that the firmware on each drive can also prove to be very important. As I'm aware there is no table to directly map which company's firmware will work with a particular drive controller. Working with older brand name servers such as IBM, Dell, and HP proved that one generation might have some very strict controls on this, where as the next did not. RAM frequency/buffering/parity was the same way, but was tied more to the chipset used rather then a third-party controller.
Drive height, the height if you were to place the drive on the top of a table, and measure the vertical distance, can also prove to be a topic of concern. While 3.5" drives don't tend to have such an issue, 2.5" drives are notorious for this. These smaller drives can come in 9mm or 7.5mm commonly, so replacing a 7.5mm with 9mm might run you into a world of pain.
One of the easier things to manage were the I/O connectors. SCSI-320 came in two major forms, one with a female connector vs. a male connection. Finding replacement drives were a pain if a retailer failed to specified a manufacturer replacement part number, connector type (of the how many there are), the transfer rate, and others.
SATA/SAS drives have significantly less pain, as the only key part to remember is that (most of the time) a SATA drive will plug into a SAS backplane where as the opposite is not true. You can observe this with the physical connectors. Transfer rates, firmware, spindle speed, and all that tend to be less of a concern (if any). SAS has started to come in it's 12Gb variety, which is only seen in modern servers. I also remember there was one brand that also had two separate connector interfaces on each drive.
Drive caddies/trays (presuming rack servers) are something you should look at as well. Dell has at least 3 different types that I'm aware of, and IBM with 2. Matching these up can be hard if you don't physically handle the different drives/brands on a regular basis.

A: Interface is essential - Newer systems use SAS,SATA or various flavours of NVMe (and while some SAS interfaces will let you use sata drives). Older machines may use PATA(aka IDE) or various flavours of SCSI, many of which have incompatible connectors.
Storage size isn't that important (get enough!) but some interfaces may have limits on disk size on extremely old machines. Its an edge case unless you're using a machine from the turn of the century. Its worth checking to see if there's an OS or hardware limitation - these should be in the appropriate manuals or documentation.
With sata, transfer speed is often used as a shorthand for the revision (sata 2, 3). With SSDs you may be able to saturate an older version (or even a newer one). That said, you can likely happily replace a sata 2 drive with a sata 3 drive with no issues. You can likely go the other way, but its easier to find a newer drive than a new old stock (or pulled) sata 2 drive.
However with SAS, SAS 6gb and SAS 12gb have different physical interfaces
SCSI is a complete mess with half a dozen varients, completely different connectors and other confusing things.
Rotational speed affects performance and heat somewhat - that said, outside laptops, shouldn't matter all that much. It certainly wouldn't stop you from running a hard drive.
Its also worth considering 'server' 2.5 inch drives have much deeper z height and arn't the same as laptop 2.5 inch drives. Laptop 2.5 drives have 3 or so z heights - 5 7 and 9 inches IIRC and you can fit a thinner drive into a thicker bay, but not vice versa.
Cache dosen't affect compatibility. More cache is good on hard drives (more fast, nearby storage means better performance) and on SSDs but you don't need to match when replacing.


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text:
Q: Getting geb.driver.DriverCreationException when I run jenkins automation(Selenium with groovy) job on LINUX computer Getting geb.driver.DriverCreationException when I run jenkins automation(Selenium with groovy) job on LINUX computer.
I am writing Automation script on selenium with Groovy.
Environmnet details are as follow:
java version = 1.8.0_261
Gradle = 5.2.1
gebVersion = "2.3.1"
testngVersion = "6.14.3"
seleniumVersion = "3.4.0"

Note: Same script is working properly with IntelliJ into my local window computer.
As per my knowledge generally we get geb.driver.DriverCreationException when there is:

*

*chromedriver and chrome browser not installed

*chromedriver not placed on correct location

*Version of chromedriver is not compatible with the chrome browser.

I have verified all the above conditions are correct but still I am getting same exception.
Can someone please suggest me what could be the another possible reason to get geb.driver.DriverCreationException and how I can resolve this issue?

** HTML Report error:**
Caused by: org.openqa.selenium.WebDriverException: unknown error: Chrome failed to start: exited abnormally.
(unknown error: DevToolsActivePort file doesn't exist)
(The process started from chrome location /usr/bin/google-chrome is no longer running, so ChromeDriver is assuming that Chrome has crashed.)
Build info: version: '3.4.0', revision: 'unknown', time: 'unknown'
System info: host: 'xyz', ip: '192.168..', os.name: 'Linux', os.arch: 'amd64', os.version: '3.10.0-1160.21.1.el7.x86_64', java.version: '1.8.0_282'
Driver info: driver.version: ChromeDriver

A: Partially this issue has been resolved, now I am able run Automation script via jenkins using Headless chrome. Actually headless chrome supports onwards selenium version 3.6 and I was using 3.4 so earlier even I was not able perform with headless browser.
But using headless chrome browser most of the my UI Automation test cases are getting FAIL.
Still I am facing issue to Launch UI chrome browser. Actually ChromeDriver is starting successfully but browser is not Launching so my test cases are getting ignored.

A: I found that I need to do Xvfb Setup- It helps to configure GUI on Linux.
sudo apt-get -y install xvfb
sudo chmod 777 /run/user/
After configuring it my issue has been resolved.


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text:
TV Ratings for Tuesday, October 25th
Jordan Walker October 26, 2011 TV Ratings
Fox won the night with a special 2 hour episode of The X-Factor (11.82 million viewers, A18-49: 4.4)
CBS was the most watched network with new episodes of NCIS (19.05 million viewers, A18-49: 4.0), NCIS: Los Angeles (15.88 million viewers, A18-49: 3.7), and Unforgettable , which recently got a full season pickup (11.29 million viewers, A18-49: 2.5).
ABC finished in third by offering new episodes of Last Man Standing (9.82 million viewers, A18-49: 2.8) the second week of Man Up! (6.75 million viewers, A18-49: 1.9), a new episode of Dancing With the Stars: Results Show (13.76 million viewers, A18-49: 2.5) and Body of Proof (9.64 million viewers, A18-49: 1.9).
NBC was left in fourth with new episodes of The Biggest Loser 12 (5.45 million viewers, A18-49: 1.9) and a repeat of Prime Suspect (2.89 million viewers, A18-49: 1.0).
The CW finished in last with repeats of Ringer (1.03 million viewers, A18-49: 0.4), and a second repeat episode of Ringer (0.82 million viewers, A18-49: 0.3).
Ratings, TV
Previous TV Ratings for Monday, October 24th: CBS pulls an amazing win.
Next Why Wednesday is the best of the week for TV.


text:
Table football – are you ready for a heady game?
This post contains affiliate links. "As an Amazon Associate I earn from qualifying purchases."
Slap a table football table up in the children's room, in the living room, in the sports club, at work, at the holiday home or at the mother-in-law's home and let it be a gathering point for many wonderful moments with those you care about.
Table football is formidable entertainment for football enthusiasts of all ages. We can play it both as a leisure activity and on a more professional level depending on how big a competitive person you are and everyone can take part.
The simple rules of table football
Makes the game harder
Choose the right table football table
Toptun your table football table
Ready for competition?
Learn all the tricks
The rules of classic table football are very simple : Two teams of one to two people. A ball. And then there must be scores. Preferably in the opponent's goal, if you do not want to be completely laughed at in the circle of friends.
The team that first reaches a pre-defined number of goals, typically ten for recreational players and seven in professional games, wins. And then the loser's team usually demands revenge.
A timeless classic for both big and small.
The game around the table football table never goes out of style.
We can kill many intense hours on either side of the mini-football pitch, which comprises two goals and four bars with players for each team; one goalkeeper, two defenders, five midfielders and three strikers.
In the beginning, the many players can be a little difficult to control , but you get there quickly, and as with all other sports, the more matches you play, and the more you train, the better you become.
Here, to coordinate his arm movements with the ball eye, which must ensure that the small red and blue players hit the ball perfectly, so it rolls past the opponent's goalkeeper. Quiet and unnoticed, or with the help of a perfect and powerful kick that sits right in the closet.
You can also just make your own rules instead of following the monotonous and traditional ones of sorts.
Who says, for example, that you must not play with over one ball, that you must play the best of ten, that you must use both hands or that you must not challenge yourself by playing with " handicap " such as no use of a goalkeeper or midfielder?
If you want a table at home, and you therefore dare to ask a professional player for advice, then he will say that there is a big difference on table football tables, and he will most likely be an advocate for a French one of a kind.
There are over 30 different types of table football tables worldwide, but the French and Italian table football tables are the most common on the Danish market.
The classic Italian table football table.
The Italian is the most classic; most often seen covered by a glass plate and with players and ball in hard plastic. The surface is like the cover in glass, which makes the game quick and uncontrolled, if you as a player do not have excellent control of your reflexes.
The French Bonzini table that many professionals swear by.
Quite the opposite is the French family of table football tables, with the Bonzini table being the most popular.
The table which has linoleum underlay, lends itself to a longer and more technical game, as the freedom to move the players in steel is greater, and there is thus the possibility of better dribbling and control of the ball which is also made as a nice detail in cork.
However, the choice of table football table is a matter of taste, so go for what appeals to you the most and where you feel your game will do best.
Just as there are a multitude of different table football tables on the market, both online and in the physical stores, there are also very different accessories and spare parts, so you and your table football table are always ready for battle.
Most table football tables are of a high quality that last for many years, with even the most committed children and childish souls at the poles.
Balls for table football are available in this edition, which looks like real footballs.
Should the accident occur, however, there is always help to be found in the form of brand new rods, maintenance kits, new cardboard tracks and extra balls, which are available in both plastic, cork and rubber and in many colors.
If you are at all into the authentic and realistic, you might also think it is fun to put on your players football jerseys from the favorite team? Only the imagination sets limits to what we can find with great accessories that make the game even more fun.
In several cities around the country, including Odense, Kolding, Århus, Aalborg and also several places in the Greater Copenhagen area, there are associations that have dedicated themselves to the noble sport that table football must be said to be. If you are looking for competition and a strong team spirit, the local association is therefore a good place to start.
If you get completely bitten by a crazy table football, the Danish Table Football Association also holds every year in October Danish championships in table football in Copenhagen.
The World Cup is also being held in France, which houses some world's leading table football players.
If you also think niche sports are the new thing, check out this video with tricks for both the beginner and the more experienced table football player and drone looked and get yourself a good table football table to optimize your skills on.
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The newest godsend to both starved Wayne Staters & naan-students (!) alike, Grace of India's a no-frills, on-campus space that lets you dine-in, deliver-in-Midtown, or carry-in to the owners' spot next door: La Hookah Town. The menu's a mix of Punjab-region classics, broken up into vegetarian, lamb, and chicken, including this yogurt-marinated, masala-spiced tandoori served with lemons & the only thing that makes you cry more than that part in The Notebook where Allie momentarily overcomes her Alzheimer's and remembers Noah, just before they both die in their sleep (onions). While the chef is known for his butter chicken (tandoor-BBQed and simmered in a butter/tomato/onion sauce), they're also turning it out Chili Dilli style, which is either a crispy chicken tossed in a chili/honey mixture, or what T-Boz's friend does right before she "dallies". Entrees come with either basmati rice or freshly baked naan, an unleavened bread that's perfect for sauce-dipping, grub-grabbing... ... and remnant-wrapping. Now would be a good time to mention they also have a selection of meat, veg, and paneer (cubed cheese/bell pepper) wraps sided with a mango chutney. Here's the lamb curry, served just the way Kirstie Alley likes it ("wet" in gravy). Oh, and they're sans liquor license, but make due with rose- and mango-flavored lassis, yogurt-based drinks perfect for cooling down the food's spice factor for anyone who isn't a Warrior.


text:
PoliticsSenateSupreme Court
Senate Approves Trump High Court Pick With Partisan Vote
The U.S. Senate confirmed federal appellate Judge Amy Coney Barrett to a seat on the Supreme Court in a 52-48 vote late Monday.
Republican Senator Susan Collins of Maine joined the entire Democratic caucus voting against Barrett's confirmation. Collins said she would not vote for Barrett's confirmation because of the proximity of the vote to next week's presidential election.
According to the AP, no other Supreme Court justice has been confirmed on a recorded vote with no support from the minority party in at least 150 years.
Barrett is the third justice on the nine-member court to be nominated by President Donald Trump and significantly tip its ideological balance toward a 6-3 conservative majority.
Supreme Court Justice Clarence Thomas is expected to swear Barrett in at a White House ceremony planned later Monday evening.
Democrats argued that the decision of picking a nominee for the seat should have been left up to whichever candidate wins the presidential election, a stance Republicans held when there was an election-year vacancy in early 2016. Republicans then refused to consider Democratic President Barack Obama's nomination of another appellate judge, Merrick Garland.
"The Senate is doing the right thing" Senate Majority Leader Mitch McConnell said Sunday when advancing Barrett's confirmation. "We're moving this nomination forward."
Sen. Elizabeth Warren, D-Mass., called the vote "illegitimate" and "the last gasp of a desperate party," the AP reported.
Barrett could potentially consider election disputes involving Trump, although it is unclear whether she might recuse herself since Trump named her to the court. She declined to say at her confirmation hearings before the Senate Judiciary Committee two weeks ago whether she will avoid hearing disputes over extended deadlines for voters to return mail-in ballots and other issues Republicans and Democrats are contesting.
Barrett almost assuredly would be among the justices hearing a new challenge November 10 on whether to invalidate the country's Affordable Care Act, which Trump has sought to overturn.
The law, popularly known as Obamacare after the former president who championed its passage in 2010, is a measure that helps provide health care to millions of Americans. Its fate is a crucial concern for many people amid the surging number of new coronavirus cases in the United States.
Republicans have long argued that Obamacare costs taxpayers too much and gives government too much control over health care. The Republican-led Congress in 2017 eliminated the law's mandate requiring that people buy health insurance if they could afford to do so. They now want the Supreme Court to invalidate the entire statute, saying that without that key insurance provision, the rest of the legislation is invalid.
America's Voice Newsreal america's voicesenate confirms amy comey barretjustice swears amy into the supreme court
Previous Post Barrett Likely to be Confirmed to US Supreme Court Monday
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text:
Ministry of foreign affairs of the Republic of Tajikistan
MFA Statements
Speeches, Articles and Intervie
MFA Leadership
MFA Representative Offices on territory of Tajikistan
Tajikistan Foreign Missions
Ministers of Foreign Affairs
Employment Rules
MFA History
Citizens Reception Schedule
Relations with CIS countries
Relations with the Asian and African countries
Relations with European and American countries
Tajikistan and international structures
Achievements of Tajikistan Foreign Policy
Human Rights` Issues
Territorial and Border Issues
Foreign Policy Law Base
Consular service
State Protocol
Rules of Accreditation
Regulatory and Legal Acts
Home page Foreign policy Bilateral Relations
Bilateral relations of Tajikistan and Switzerland
Diplomatic relations between the Republic of Tajikistan and Swiss Confederation were established on December 9, 1992. Ambassador Extraordinary and Plenipotentiary of ....
Bilateral relations of Tajikistan with Austria
Diplomatic relations between the Republic of Tajikistan and the Republic of Austria were established on March 25, 1992. The Ambassador Extraordinary ....
Bilateral relations of Tajikistan with Belgium
Bilateral relations of Tajikistan with Belgium Diplomatic relations between the Republic of Tajikistan and the Kingdom of Belgium were established on ....
Bilateral relations of Tajikistan with Czech Republic
Diplomatic relations between the Republic of Tajikistan and the Czech Republic were established on June 5, 1992. Ambassador Extraordinary and Plenipotentiary ....
Bilateral relations of Tajikistan with Estonia
Diplomatic relations between the Republic of Tajikistan and the Republic of Estonia were established on February 23, 2006. Ambassador Extraordinary and ....
Bilateral relations of Tajikistan with France
Diplomatic relations between the Republic of Tajikistan and the French Republic were established on March 3, 1992.The Embassy of the ....
Bilateral relations of Tajikistan with Germany
Diplomatic relations between the Republic of Tajikistan and the Federal Republic of Germany were established in 1992. Ambassador Extraordinary and Plenipotentiary ....
Bilateral relations of Tajikistan with Great Britain
Diplomatic relations between the Republic of Tajikistan and Great Britain were established on January 15, 1992.On December 20, 2001 the ....
Bilateral relations of Tajikistan with Greece
Diplomatic relations between the Republic of Tajikistan and the Hellenic Republic were established on 30 September, 1992. Ambassador Extraordinary and Plenipotentiary ....
Bilateral relations of Tajikistan with Hungary
Diplomatic relations between the Republic of Tajikistan and Hungary were established on July 2, 1992. Ambassador Extraordinary and Plenipotentiary of Hungary ....
Bilateral relations of Tajikistan with Italy
Diplomatic relations between the Republic of Tajikistan and Italian Republic were established on May 15th 1992. The Ambassador Extraordinary and Plenipotentiary ....
Bilateral relations of Tajikistan with Latvia
Diplomatic relations between the Republic of Tajikistan and the Republic of Latvia were established on 11 May 1994. Ambassador Extraordinary and ....
Bilateral relations of Tajikistan with Lithuania
Diplomatic relations between the Republic of Tajikistan and the Republic of Lithuania were established in 1992. Ambassador Extraordinary and Plenipotentiary of ....
Bilateral relations of Tajikistan with Luxembourg
Bilateral relations of Tajikistan with Luxembourg Diplomatic relations between the Republic of Tajikistan and the Grand Duchy of Luxembourg were established ....
Bilateral relations of Tajikistan with Norway
Diplomatic relations between Tajikistan and Norway were established in 1992. Ambassador Extraordinary and Plenipotentiary of the Kingdom of Norway to ....
02:45 Tajikistan
01:21 Dushanbe
01:48 "Chakan"
03:53 Nawruz in Cairo, 2019
© Ministry of foreign affairs of the Republic of Tajikistan
33 Sheroz str., Dushanbe 734001, Republic of Tajikistan
Закон Республики Таджикистан о борьбе с коррупцией
Закон Республики Таджикистан "Об упорядочении традиций, торжеств т обрядов в Республике Таджикистан
Закон Республики Таджикистан об ответственности родителей за обучение и воспитание детей
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Закон Республики Таджикистан «О периодической печати и других средствах массовой информации»


text:
Q: Create dictionary from list of variables I'm looking for a way to create a dictionary without writing the key explicitly.
I want to create a function that gets the number of variables and creates a dictionary where the variable names are the keys and their values are the variable values.
Instead of writing the following function:
def foo():
    first_name = "daniel"
    second_name = "daniel"
    id = 1
    return {'first_name':first_name, 'second_name':second_name}

I want to get the same result with function :
create_dict_from_variables(first_name, second_name)

Is there any way to do so?

A: You can use locals, but I would recommend against it. Do it explicitly.
>>> import this
[...]
Explicit is better than implicit.
[...]

Your code will generally be better, more predictable, less prone to breaking and more comprehensible if you do it explicitly.

A: You can't do it without writing at least the variable names, but a shorthand can be written like this:
>>> foo = 1
>>> bar = 2
>>> d = dict(((k, eval(k)) for k in ('foo', 'bar')))
>>> d
{'foo': 1, 'bar': 2}

or as a function:
def createDict(*args):
     return dict(((k, eval(k)) for k in args))

>>> createDict('foo','bar')
{'foo': 1, 'bar': 2}

you can also use globals() instead of eval():
>>> dict(((k, globals()[k]) for k in ('foo', 'bar')))

A: In principle this is possible by passing variable names to function create_dict and then reaching to a caller stack frame from within create_dict function using module inspect.

A: pip install sorcery
from sorcery import dict_of

a = 1
b = 2
c = 3
d = dict_of(a, b, c)
print(d)
# {'a': 1, 'b': 2, 'c': 3}

A: No, there isn't, because Python functions don't get information about the variables used to call the function. Also, imagine doing something like this:
create_dict_from_variables(first_name[:-3] + "moo", last_name[::2])

The function will have no way of knowing the expressions used to create the parameters.

A: There is an interesting solution to this problem, which doesn't involve external libraries. However, a slightly different syntax is needed: eval(f(a,b))
# Auxiliary Function
f = lambda s: f"dict({ ','.join( f'{k}={k}' for k in s.split(',') ) })"

first_name  = "daniel"
second_name = "joe"
D           = eval(f('first_name,second_name'))

print(D)
# {'first_name': 'daniel', 'second_name': 'joe'}

In the example above, the main goal of the OP is still accomplished, in the sense that we only type the names of the variables once to create a dictionary. However, the syntax is still a bit verbose.
PS. One important benefit of the code above is that we evaluate the dictionary in its original namespace, which removes any restrictions with respect to the scope of the function (globals(), locals(), etc.). This was my main motivation behind using this approach.

A: In fact, there is a way:
from varname import nameof

def foo(first_name,second_name):
    return {nameof(first_name):first_name, nameof(second_name):second_name}

first_name = "daniel"
second_name = "daniel"

print (foo(first_name,second_name))

Output:
{'first_name': 'daniel', 'second_name': 'daniel'}

You can get the python-varname package below:
https://github.com/pwwang/python-varname
Basic use:
from varname import nameof

s = 'Hey!'

print (nameof(s))

Output:
s

A: You cannot do this.
Your function could be defined as:
def create_dict_from_variables(first_name, second_name):
    return something_from(first_name, second_name)

and you can call this function:
create_dict_from_variables('abcd', 'efgh')

These two arguments 'abcd' and 'efgh' are not named variables.


Understanding the tasks that health workers perform in real life can improve their basic Training. Marion Subah of MCSP and Jhpiego shares experiences in using Task Analysis to improve pre-service training of midwives and lab technicians in Liberia. Her findings summarized below, are presented at the American Society of Tropical Medicine's 66th Annual Meeting.
Health worker task analysis helps human resource planners and managers update pre-service education (PSE) curricula and plan needed in- service training. In Liberia, a task analysis was conducted focusing on Liberia's midwives' and Medical Laboratory Technicians' (MLT) work practices.
How often do you do the task (frequency)?
Where did you learn to do the task (location)?
How well do you think you are able to perform the task (performance)?
How critical is the task in terms of patient and/or public health outcomes (criticality).
Eligibility criteria included those currently practicing between 6 months and 5.5 years following graduation. Midwives were assessed for five tasks relating to malaria service provision, including provision of preventive treatment for malaria in pregnancy, management of vector borne diseases, diagnosis and management uncomplicated malaria in adults and children (respectively), and provision of malaria preventive services.
Lab technicians were assessed for one malaria task, performance of parasitological tests. On average 61% of midwives learned these malaria tasks in PSE, 74% said they performed these tasks daily, 80% felt proficient in performing the tasks, and 82% rated the tasks moderate to high in criticality. For MLTs, 88% learned malaria testing in pre-service education, 100 % performed this task daily, 77% felt they were proficient and 93% said the task was of moderate to high criticality.
The results from this rapid task analysis are being applied to the current curricula review. Courses that could be updated or strengthened have been identified. Malaria Case Management Technical Update and Effective Teaching Skills Training are being organized for tutors at the training schools. Finally, integrated supportive supervision tools are being strengthened to improve performance of these malaria tasks by midwives and lab technicians.


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Is Alexander Skarsgard Dating Tuva Novotny? Inside His Personal Life
Everything about Alexander Skarsgard and Tuva Novotny's romance rumors!
Alexander Skarsgard has gained huge popularity thanks to his acting skills. His amazing performances in numerous movies and TV shows have kept the audiences talking about him.
But the fans of the Swedish actor have been talking about another thing in recent times, which isn't related to his professional life at all. Infact, it's his personal life that has been making quite the noise.
Since early 2022, Skarsgard has been rumored to be dating a fellow Swedish actress named Tuva Novotny. And with Novotny confirming her pregnancy on April 29, 2022, the romance rumors have fueled even more.
People have been saying that Skarsgard might be the father of Novotny's child. But the thing is that neither of them has confirmed or denied their togetherness. However, some third parties have confirmed it. Have a look!
Alexander Skarsgard and Tuva Novotny are confirmed to be dating
Skarsgard and Novotny's relationship was first confirmed by Ann Söderlund and Sanna Lundell in their podcast Inte din morsa.
On February 4, 2022, episode of the podcast titled 'Kärlek utan ansvar' [Love Without Responsibility in English], the two Swedish journalists took up the togetherness of possibly the two of Sweden's biggest international celebrities, i.e., Skarsgard and Novotny.
A pregnant Tuva Novotny (in the black dress) alongside her friend at the Elle Gala 2022 (Photo: Instagram)
Skarsgard and Novotny's relationship came up when the podcast hosts talked about Lundell being alongside her actor husband, Mikael Persbrandt, during the recording of Lars von Trier's new series titled The Kingdom of Exodus — where Persbrandt stars alongside Novotny and Skarsgård.
"It's still so funny that we have talked about it several times that they are a couple, that they have been for several years and they are like two of our biggest international celebrities and no one writes about it. I think it's so strange," Söderlund said.
Lundell then followed up with speculation and said, "I guess no one has gone out and denied it. But it feels like the Swedish media has just decided that 'we should not talk about this' because then maybe they will never be allowed to interview Tuva Novotny again. I do not know."
After that, Söderlund mentioned that she had previously talked to Novotny about her relationship with Skarsgård and that the topic is yet to be publicized.
"When I recorded my mini-role in the Bonus family, I talked to Tuva about that," Söderlund said.
As for what Novotny's reply was when Söderlund said that, the actress told the podcast host that she also doesn't know why it is so as she and Skarsgård have been together for several years.
Alexander Skarsgard's Hollywood transformation! "The Northman"
In theatres now pic.twitter.com/FexwsJYm48— Joseph Cortez (@JosephC43750338) April 26, 2022
"We have not denied it and it is not something we are trying to keep secret. It's the strangest thing in the world," Novotny further told Söderlund.
Months later, when online gossip site Deuxmoi conducted a Q&A on their Instagram handle on April 19, 2022, one fan was curious as to who was Skarsgård's girlfriend and if the actor had split with Novotny.
In reply, Deuxmoi said that people are telling him that Skarsgård's girlfriend is Novotny. As for the question of break up, Deuxmoi's owner had attached a screenshot of a chat they had with someone else – who was from Sweden.
The chat mentioned the details from the already-mentioned podcast. "I am no expert but I am a fellow Swede and I could totally see them being able to keep it private. Swedes like their personal space," the chat read.
Deuxmoi's Instagram story discussing Alexander Skarsgard and Tuva Novotny's relationship (Photo: Instagram)
In the end, the anonymous Swede said that they don't see Söderlund and Lundell lie about Skarsgard and Novotny's relationship as they wouldn't "really benefit from lying about it."
Alexander Skarsgard likes to keep his personal life private
Contradicting Novotny's statement about not trying to keep her togetherness with Skarsgard a secret is her alleged boyfriend himself — much like what the anonymous Swede said about people of Sweden liking their personal space.
On April 17, 2022, The Northman star conversed with the Swedish newspaper Aftonbladet. During that, the interviewer told the actor that he is usually outspoken, but he doesn't say a word when it comes to talking about his romance rumors with Novotny.
Skarsgard once again didn't say anything related to his relationship with his rumored girlfriend. But, he said that he tries to concentrate more on talking about his professional life and keeps his personal life out of the media.
Alexander Skarsgard as Lukas Matsson in 'Succession' (Photo: Twitter)
His words were, "No, but I try to concentrate on talking about the professional and keeping the private [life] private."
After that, he was asked if he does or doesn't deny his relationship with Novotny; he simply laughed and switched the topic of discussion to football.
As a result, fans of Skarsgard and Novotny are still hopeful that Novotny and Skarsgard might be together and declare their love publicly sometime soon.
Before Skarsgard's romance rumors with Novotny, the Swedish actor was in a relationship with Amanda Seyfried (in 2008), Evan Rachel Wood (in 2009), Kate Bosworth (from 2009 to 2011), and Alexa Chung (from 2015 to 2017).
Related Topics:Alexander SkarsgardThe NorthmanTuva Novotny
Adin Ross And Girlfriend Pamibaby's Relationship Going Strong Despite Break Up Rumors
Erin Napier Shares Two Daughters with Husband Ben Napier in Their 13-Year Long Relationship
Alexander Skarsgard's Rumored Girlfriend Tuva Novotny Is Pregnant with Her Second Child


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Lemire and Gallo to Bring Superboy to new heights
DC Comics announced this morning that Jeff Lemire will launch a Superboy ongoing series later this year with artist Pier Gallo.
A one-off co-feature in August's Action Comics #982 will kick off the new title.
Lemire, an award-winning cartoonist best known for his Essex County Trilogy and the Vertigo monthly Sweet Tooth, also is writing DC's upcoming Brightest Day: The Atom Special and an Atom co-feature in Adventure Comics. Gallo most recently illustrated Adventure Comics #8-10.
"I am really excited to be taking over the adventures of Conner Kent/Superboy in a new monthly series!" Lemire tells the DC Universe blog. "The book will combine many of the classic touchstones of the Superboy mythos along with new supporting characters, new villains and new ideas, building a strong foundation that can support the Boy of Steel for years to come. I really want to work with our amazing artist Pier Gallo to combine a classic storytelling feel with a thoroughly modern sensibility and explore what it would really be like to be a super-powered teenager, in the heart of rural America."
I talked briefly with Lemire when he was at TCAF and he let it slip that he'd be writing Superboy. He was asked personally by Geoff Johns to write the title. It seems like he's quickly become one of Johns' favourite writers right now.
# Adventure Comics# Geoff Johns# Jeff Lemire# pier gallo# superboy# Sweet Tooth
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