text:
\section{Introduction}

The discovery of high-temperature superconductivity in doped copper oxides generated
an enormous amount of interest in quantum antiferromagnets~\cite{anderson, sachdev, keimer}.
The emergence and collapse of long-range antiferromagnetic (AF) order, which provides
us a unique way to explore many exotic magnetic phases, is one of the most essential
and well-explored topics in condensed matter physics. The AF ordering in cuprate,
iron-pnictide, and iron-chalcogenides gets suppressed by doping non-magnetic
impurities~\cite{liu1,liu2, norman}. Spin-wave theory for low concentration of
impurities with the impurities treated as static vacancies~\cite{kircan,chernyshev}
can usually model such behavior. On the other hand, frustration arising from in-plane
couplings in clean systems can also disrupt long-range magnetic order (LRO) and are
routinely explored within the $J_1-J_2$ Heisenberg spin models~\cite{sato,wang,schmidt}.
Disorder-induced suppression of long-range magnetic order~\cite{szczech,kunwar}
have been typically studied in the strong-coupling limit. Quantum Monte Carlo
simulations~\cite{sandvik} in the large correlation strength limit, agree with the
AF order vanishing at the classical percolation threshold as in the experiments.

Cuprates like La$_{2}$Cu$_{x}$Mg$_{1-x}$O$_{4}$~\cite{mccarron,cheong,wan,vajk}
have inspired some site-diluted Hubbard model studies in two and quasi-two
dimensions~\cite{ulmke,medhi,delannoy}. The experimental motivation was to
investigate superconductivity in the parent material (La$_{2}$CuO$_{4}$) by
doping with non-magnetic Zn or Mg that suppresses long-range antiferromagnetic
order. According to the current understanding this quasi-two dimensional
material [La$_{2}$Cu$_{x}$(Mg/Zn)$_{1-x}$O$_{4}$] shows complete suppression of
long-range AF order~\cite{vajk} for $x_p^{2D} \sim 0.59$, the classical percolation
threshold~\cite{christensen,sandvik}. In the strong interaction limits for such
materials where 3$d$ transition metal elements are
involved~\cite{sandvik,kato, chernyshev1, carretta}, the long-range magnetic
order vanishes at $x_p$, the critical classical percolation threshold in
the relevant dimensions.

However, investigations of site dilution for the Hubbard model where $U$ is
comparable to bandwidth (BW) are relevant both for materials and is of
theoretical interest. In particular, since the correlation-induced suppression
of double occupation is not too severe, sites with $U=0$ in vicinity of
$U\neq0$ sites can get effected by virtual charge fluctuations leading to
induced moments on the uncorrelated sites. Thus, whether site dilution will
suppress the long-range antiferromagnetic order of the undiluted system is
unclear. A recent study of the diluted Hubbard model on Lieb lattice shows
that magnetic order is very robust for dilution much lower than the classical
percolation threshold~\cite{lima}.

In this paper, we analyze the effect of site dilution in a Hubbard model
at half-filling using a semi-classical Monte-Carlo scheme (s-MC)~\cite{mukherjee,ptca-ref}.
The method reduces to an unrestricted Hartree-Fock method at very low
temperatures but becomes progressively accurate with temperature increase and,
in particular, compares well with Determinant Quantum Monte Carlo (DQMC) over
a wide temperature range. We consider the half-filled Hubbard model as defined
below in three dimensions. We first produce several benchmarks for the undiluted
case, including the AF magnetic order. We then show that switching off interaction
potential on a fraction of sites weakens and eventually destroys the magnetic
order. However, remarkably, for correlation strength, where the bandwidth (BW)
and interaction strength ($U$) are comparable, we show that the AF order survives
to dilutions much below the classical percolation threshold. We investigate this
phenomenon by tracking the local moment dependence with temperature. We show that
$U\neq0$ sites induce significant suppression of double occupation on the $U=0$
sites stabilizing local moments on the uncorrelated sites. In addition our
calculations reveal that the density of states carries the signature of this effect
and manifests as a four-lobe Mott insulator. At a critical dilution below the
classical threshold, we show that the collapse of local moments at the $U=0$
sites signals the onset of a metallic state. We find that the ensuing metal has
a pseudo-gapped density of states at low temperatures. We characterize the
percolative metallic state and it's temperature dependence. Finally, we demonstrate
that the vanishing of the AF order at the classical percolation threshold occurs
for $U$ much larger than the BW, in agreement with earlier literature. We also
find that the same can happen at increased temperatures where thermal fluctuations
destroy the local moments on the $U=0$ sites. Thus we present a complete
phenomenology within our semi-classical approach of site dilution effects,
correlation strength, and temperature.

\section{Model \& Method}

We consider the following particle-hole symmetric from of the one band Hubbard Hamiltonian:

{\small
\begin{eqnarray}
  H=-t\sum_{<i,j>,\sigma}(c^{\dagger}_{i\sigma}c_{j\sigma} + h.c.)~~~~~~~~~~~~\nonumber\\+ U\sum_{i} \Big(n_{i\uparrow}-\frac{1}{2}\Big) \Big(n_{i\downarrow}-\frac{1}{2}\Big)
  -\mu \sum_{i} n_i
\end{eqnarray}

\noindent
where $c_{i\sigma}$ ($c^{\rm \dagger}_{i\sigma}$) are the fermion annihilation
(creation) operators at site $i$ with spin $\sigma$. $t$ is the nearest neighbor
hopping parameter and $U$ ($>$ 0) denotes the on-site repulsive Hubbard interaction.
$\mu$ is the chemical potential.

To employ the s-MC approach we decompose the on-site interaction term by introducing
standard Hubbard-Stratonovich (HS) auxiliary fields (a vector field $m_i$ that couples
to spin degrees of freedom while a scalar field $\phi_i$ couples to charge degree of
freedom) at each site $i$. We treat auxiliary fields as {\it classical fields} by
dropping the time dependence explicitly. We treat $\phi_i$ at the saddle point level
$i\phi_{i} = \frac{U}{2} \textless n_{i} \textgreater $, but retain the
thermal fluctuations for $m_i$. These thermal fluctuations are necessary
to capture many of the well established features which will be discussed later.
The following effective spin-fermion Hamiltonian is derived using above
approximations (see supplementary materials for the details and justification
of the approximation):

\begin{eqnarray}
H_{eff}= -t\sum_{<i,j>,\sigma} (c^{\dagger}_{i\sigma}c_{j\sigma} + h.c.)\nonumber
+ U/2 \sum_{i} (\textless n_i \textgreater n_i - \textbf{m}_i . \sigma_{i})  \nonumber \\
  + (U/4)\sum_{i}(\textbf{m}_{i}^2 - {\textless n_i \textgreater}^2) -\frac{U}{2} \sum_{i} n_{i}  -\mu \sum_{i} n_i \nonumber
\end{eqnarray}

The chemical potential is varied to maintain the system at half filling.
We solve $H_{eff}$ by using exact diagonalization based Monte-Carlo method.
We diagonalize the Hamiltonian for a fixed set of $\{\textbf{m}_{i}\}$
and $\{\textless n_i \textgreater\}$ configuration. We update the $\{\textbf{m}_{i}\}$
at each site based on usual Metropolis scheme at a fixed temperature.
The $\textless n_i \textgreater$ fields are self consistently updated at every
10$^{th}$ Monte-Carlo step where the $\textbf{m}_{i}$ fields are held fixed. The
goal of the process is to generate equilibrium configuration of the $\textbf{m}_{i}$ and
the $\textless n_i \textgreater$ fields. Expectation values of observables are obtained
by appropriately using the eigenvectors and eigenvalues resulting from diagonalizing
the Hamiltonian in each of the equilibrium configuration. These individual expectation
values from equilibrium configurations are further averaged over results from 100
such configurations at a fixed temperature. All observables are calculated at a given
temperature by averaging over the values obtained from individual configurations. We
note that we calculate observables from every tenth equilibrium configuration to
avoid spurious self correlations. Temperature is lowered in small steps to allow
for equilibration. To avoid size limitation we employ above mentioned Monte-Carlo
technique within a traveling cluster approximation~\cite{tca-ref,pradhan,chakraborty}
to handle system size $N$ = $L^3$ = 10$^3$.

For $0<x<1$, we have $Nx$ fraction of sites with finite $U$ and $N(1-x)$ sites with
$U=0$, with $N$ being the total number of sites. For $U=8$, on-site interactions
($U_i$) at each sites are chosen using the distribution
$P(U_i)=(1-x)\delta(U_i)+x\delta(U_i-8)$. We
introduce the HS auxiliary fields only on the $U\neq0$ sites. The induced moments
on the $U=0$ sites are calculated by computing quantum local moments as we discuss
later. Finally, all energy scales ($U$, temperature, BW etc.) are measured in units
of the hopping parameter $t$.

\section{Phase Diagram}

First we discuss briefly about the $U-T$ phase diagram, seen in the inset of
Fig.~\ref{fig_pd}, obtained for $x$=1 (i.e. the undiluted case, without any
$U$=0 sites). We first find that for all $U$, we have a staggered AF insulating
ground state (AF-I). The staggered AF transition temperature $T_N$ defines
the finite temperature boundary of the AF and the PM phase. The antiferromagnetic
transition temperature $T_N$ increases with $U$ up to $U$=8 and decreases
thereafter. For larger $U$ s-MC captures $\sim t^{2}/U$ scaling of $T_N$. In
the inset we also find that for large $U$, above $T_N$, there is an insulating
region of preformed local moments with no long range magnetic order (PM-I).
This phase crosses over to a paramagnetic metal (PM-M)
above the dashed line. We discuss below how these phases are determined for
different values of $x$. For the $x=1$ case, the non-monotonic $U$ dependence
of $T_N$ and the preformed local moment regime at finite temperature are results
beyond simple finite temperature Hartree-Fock mean field theory. Details and
comparison with DQMC are presented in earlier s-MC literature~\cite{mukherjee}.
s-MC has also been used to study the physics of Anderson-Hubbard model~\cite{patel}
and frustrated Hubbard model~\cite{gour, tiwari}.

\begin{figure}[t]
\centerline{
\includegraphics[width=9.0cm,height=7.7cm,angle=0,clip=true]{fig_01.eps}}
\vspace{.2cm}
\caption{\label{fig_pd} $x-T$ phase diagram for $U$=8. $x$ is the concentration
  of correlated sites ($U$=8) and rest of the sites (with concentration $1-x$)
  have $U=0$. PM-I phase intervenes between the PM-M and AF-I phase for $x$ $>$ 0.7.
  For $x \leq$ 0.7 the PM-I phase vanishes and the metal insulator transition coincides
  with the onset of the AF order. For $x \leq$ 0.15 the AF order completely collapses at low
  temperatures. The inset shows the $U-T$ phase diagram. For details please
  see the text.
}
\end{figure}

As mentioned in the introduction, our main motivation is to examine if the AF order
can survive below the classical percolation threshold. For this we initially confine
to $U=8$ where $T_N$ is optimum and study the effect of site-dilution. This value
of $U$ is away from the two perturbative limits of $U/BW<<1$ and $U/BW>>1$. We will
discuss the systematics of  varying $U$ at a later stage.
The main panel in Fig.~\ref{fig_pd}, shows the $x-T$ phase diagram for $U=8$. We
see that the $T_N$ (diamonds) and crossover scale (dashed line) both decrease as $x$
is reduced. Within numerical accuracy, the PM-I phase exists for $x>0.7$. The important
observation is that the $T_N$ survives up to $x=0.15$, much smaller than the classical
three dimensional percolation threshold ($x_p^{sc} \sim 0.31$). We will show below that
this conclusion is robust to changes in the system size.

\begin{figure}[t]
\centerline{
\includegraphics[width=9.0cm,height=7.7cm,angle=0,clip=true]{fig_02.eps}}
\vspace{.2cm}
\caption{\label{fig_af}
Physical quantities for different $x$ values. All calculations are
done for $U=8$ unless otherwise specified.
(a) Average local moments $M$ vs temperature measured using only $U=8$ sites.
Inset shows the induced moments with temperature at U=0 sites. Legends are same
in (a)-(c). (b) Resistivity vs temperature curves for different $x$ values.
(c) s($\pi, \pi, \pi$) vs temperature (by taking $U=8$ sites only) for
different $x$. With decrease in $x$ the quantum structure factor decreases at low
temperature. $T_N$ also decreases and vanishes for $x$ = 0.1.
(d) $s_s$($\pi, \pi, \pi$), structure factor for taking both $U=0$ and $U=8$ sites,
vs temperature shows that the system as a whole turns antiferromagnetic
at the same temperature to that of $U=8$ sites. For comparison s$_{U=0}$($\pi, \pi, \pi$),
calculated only for $U=0$ sites for specific $x$ are also shown.
}
\end{figure}

\section{Magnetic and Transport Properties}

Next we discuss the magnetic and transport properties in details that
we used to construct the phase diagram for site-diluted Hubbard model
(Fig. \ref{fig_pd}).

\textit{Metal-insulator transition \& magnetic order:} From the $x=1$ analysis
we know that local moments exist on all sites for $U=8$.  For $x=1$ the system
averaged quantum local moment is defined as $M= \langle (n_{\uparrow} - n_{\downarrow})^{2} \rangle =
\langle n \rangle - 2 \langle n_{\uparrow} n_{\downarrow} \rangle$, where
the angular brackets imply quantum and thermal averaging at individual sites.
The large moment at low temperature is due to the increased suppression of
doublons (local double occupation). In the limit $U\rightarrow \infty$ and any
finite temperature we expect the double occupation to go to zero giving $M=1$.
In the other extreme limit of $U=0$ or $T\rightarrow\infty $ at any finite $U$,
the double occupation
$\langle n_{\uparrow} n_{\downarrow} \rangle\rightarrow \langle n_{\uparrow}\rangle\langle n_{\downarrow}\rangle=0.25$.
This gives the value of $M$ to be 0.5. In Fig.~\ref{fig_af} (a) main panel we
show the local moment $M$ vs temperature data for various $x$ values for the
$U\neq0$ sites. For $x=1$, this of course coincides with the system averaged
local moments, while for $x\neq 1$, the site averaging is done only over the
$U\neq 0$ sites.

To understand the actual temperature scale for moment formation that lies between
these two limits and its impact on transport properties we calculate the resistivity
as function of temperature in Fig.~\ref{fig_af}(b). Resistivity is calculated for
different $x$ values by calculating the {\it dc} limit of the optical conductivity
determined by the Kubo-Greenwood formula~\cite{mahan-book,cond-ref}. A metal to insulator
crossover (MIC) scale ($T^*$) is ascertained from the sign of $d\rho/dT$. For $x=1$,
and $U=8$, $T^*\sim 1$. For the $x<1$ case we see that this crossover scale reduces
rapidly. In order to understand this systematics, in (a) we plot the local moments
of the correlated ($U\neq 0$) and uncorrelated ($U= 0$) sites separately. For the
correlated sites we see that there is an overall reduction in the local moment
magnitudes, but there is no drastic local moment collapse to suggest a significantly
smaller MIC temperature as the resistivity data suggests. However, the remarkable
effect on deciding the scale for onset of metallicity with temperature increase
comes from the $U=0$ sites! In the inset of (a), we see that weak local moments
are induced on the uncorrelated sites. We observe that $T^*$ is controlled  by the
onset temperature of the local moments formation ($M$ becoming greater than 0.5)
on the uncorrelated sites. For example for $x=0.9$, the local moments of the
correlated sites are similar in magnitude to the $x=1$ case, yet the resistivity data
shows an insulator to metal crossover occurs at  $T^*\sim 0.5$ as opposed to $\sim$1
for $x=1$ case. Interestingly the onset of magnetic moments on $U=0$ sites,
transition from PM-M to AF-I phase occurs at same temperature for $x\leq 0.7$.
This clear correlation needs the following clarification: whether the small moments
on the $U=0$ sites, for example small moments very close to the uncorrelated value
of 0.5, for $x < 0.4$, responsible for stabilizing the low temperature antiferromagnetic
insulating state? In particular, is there a long range order arising out of the sites
with two values of moments?

To answer this question, in (c) we plot the quantum antiferromagnetic correlations
s($\pi, \pi, \pi$) [$s(\bold{q})=\frac{1}{(Nx)^{2}} \sum_{mn} \langle \bold{s}_{m}.\bold{s}_{n}\rangle e^{i\bold{q}.(r_{m}-r_{n})}$
where $\bold{q}$ is the wave vector], where angular brackets have the same meaning as
mentioned above and the indices $\{m,n\}$ run over only the $U=8$ sites. The normalization
is defined accordingly. The reduction in the $T_N$ as well as the low $T$ saturation value
with decreasing $x$ is apparent. The weakening of antiferromagnetism due to site dilution
is expected. However, we find an unexpected behavior when comparing the above with magnetic
structure factor computed only for the $U=0$ sites [denoted as s$_{U=0}$($\pi, \pi, \pi$)].
In (d) we show two such comparisons at the indicated values of $x$. The AF order that
results from the $U=0$ sites by itself generates long range staggered AF correlations
in three dimensions. Further, the AF order from the two set of sites (taking U=8 and U=0
sites separately) and AF correlations s$_{s}$($\pi, \pi, \pi$) obtained by taking all the
sites (both  U=8 and U=0 sites at the same time) vanish at the same temperature. This
shows cooperation of the $U\neq 0$ and $U=0$ matrix. In addition, for $x \leq 0.7$,
we find that the insulating state and the $T_N$ coincide, reminiscent of a Slater like
insulator. However, unlike the Slater insulator, this is clearly not arising out of a
nesting instability.  For $x$ $>$ 0.7, the data suggests that the insulting state can
survive without the magnetic order, but requires finite local moments at the
$U=0$ sites. This is the continuation of the $x=1$ PM-I phase for $x<1$.

\begin{figure}[t]
\centerline{
\includegraphics[width=9.0cm,height=7.7cm,angle=0,clip=true]{fig_03.eps}}
\vspace{.2cm}
\caption{\label{fig_mit}
(a) Temperature dependence of density of states at the Fermi energy N($\mu$)
shows that the Mott gap collapses at high temperature due to thermal fluctuation.
Thermal fluctuation persists up to low enough temperature for lower $x$ values.
N($\mu$) more or less remains constant with temperature for $x=0.1$.
(b) Density of states N($\omega$) with $\omega$ for different temperatures
at $x=0.7$. (c) Density of states N($\omega$) with $\omega$ for different $x$
at $T=0.02$. Legends are same in (a) and (c).
For $x=1$, the Mott gap at $T=0.02$ show Mott lobes around
$\pm U/2$. A pair of secondary Mott lobe forms near $\omega=0$ for $x<1$.
(d) $U$ dependent density of states for $x=0.7$ shows that the secondary lobes are
mainly due to the $U=0$ sites.
}
\end{figure}

\textit{Density of states:} In  Fig.~\ref{fig_mit} (a) we show the temperature
evolution of the density of states at the chemical potential N($\omega=\mu$) for
different values of $x$. Density of states are obtained by implementing the Lorentzian
representation of the $\delta$ function in $N(\omega) =  \sum_{k} \delta(\omega - \omega_{k})$,
where $\omega_{k}$  are the eigenvalues of the fermionic sector and the summation
runs up to $2L^{3}$, i.e. the total number of eigenvalues of a $L^{3}$ system.
The expected gradual filling up of the charge gap in the Mott state seen for
$x=1$ as also seen in~\cite{dqmc} for smaller $x$ values. The gap filling however
becomes abrupt for $x\leq 0.7$. This is the same dilution below which we have a
direct transition from a PM-M to an AF-I. In addition, the density of states are
plotted explicitly for $x=0.7$, in Fig.~\ref{fig_mit}(b) at different temperatures.
While not explored herein detail, overall the data suggests a possible first
order transition for $x\leq0.7$. Finally for $x=0.1$, we have a gap-less ground state.

The density of states are compared for different $x$ values at low temperature
$T=0.02$, in Fig.~\ref{fig_mit}(c). We see that with reducing $x$, the upper and
lower Hubbard sub-bands around $\pm U/2$ evolves in to a four sub-band structure and
the gap around chemical potential $\mu$ ($\omega$=0) reduces. The gap eventually
closes and we find a pseudo-gapped metal for $x=0.1$.
To understand the origin of the new features in the density of states we show the
contribution of the DOS from $U=0$ and $U=8$ sites separately in panel (d) for
$x=0.7$ at the same low temperature. It shows that $U=0$ sites mostly contribute
to the formation of the low energy Mott lobes (around $\omega=\pm1$). This four
sub-band DOS within s-MC qualitatively agrees with DQMC~\cite{ulmke}.

\begin{figure}[t]
\centerline{
\includegraphics[width=9.0cm,height=7.7cm,angle=0,clip=true]{fig_04.eps}}
\vspace{.2cm}
\caption{\label{fig_pc}
Shows the drop of s($\pi, \pi, \pi$) with decrease in $x$ values for different
L values (N=L$^3$). For
$T=0.02$ long range AF order persists up to $x$=0.15. This AF order is due
to the induced moment formed at $U=0$ sites as explained the text. The
result is almost indistinguishable beyond system size $10^3$.
All calculations are done for $U=8$. Inset(i) shows the s($\pi, \pi, \pi$)
vs $1/L$ for $x=0.15, 0.2$ and $0.25$. Inset also shows linear fitting of
s($\pi, \pi, \pi$) with $1/L$ for $x$ = 0.15, 0.2 and 0.25. Inset(ii)
shows that the long range AF order also persists up to $x$=0.15 for $T=0.01$.
}
\end{figure}

\begin{figure}[t]
\centerline{
\includegraphics[width=9.0cm,height=7.7cm,angle=0,clip=true]{fig_05.eps}}
\vspace{.2cm}
\caption{\label{fig_mom}
(a) Distribution of local moments at $U=8$ and $U=0$ sites for
different $x$ values; the peak around $M=0.8$ is for the finite $U$ sites
whereas peak at lower $M$ is for the induced moments ($M_{U=0}$) at $U=0$
sites. Inset shows the distribution for $U=0$ and $U=8$ sites separately
at $x=0.4$.
(b) s($\pi, \pi, \pi$) and induced moment ($M_{U=0}$) at $U=0$ sites
with $x$ for $T=0.02$ shows one to one correspondence between the onset
of antiferromagnetic correlations and formation in induced magnetic moments
at $U=0$ sites. The induced moments mediates the antiferromagnetic correlation
below classical percolation threshold limit.
(c) s($\pi, \pi, \pi$) vs $x$ for different temperatures show that
the percolation threshold increases with temperature.
(d) s($\pi, \pi, \pi$) vs $x$ for different $U$ values at $T=0.02$.
The percolation threshold increases with $U$ values due to suppression
of charge fluctuations at large $U$. The inset shows comparison of
the induced moment ($M_{U=0}$) at $U=0$ sites with $x$ between $U=8$ and
$U=24$.
}
\end{figure}

\section{Percolation Threshold}

To start with, we first demonstrate the stability of the
critical percolation threshold obtained from finite size lattices. Since
the AF order parameter is the central indicator used by us, in Fig.~\ref{fig_pc}
we show the low temperature value of $s$($\pi, \pi, \pi$) for different system
sizes as a function of $x$. The system size is defined as $L^3$. Beyond $10^3$
the results for low $x$ are barely distinguishable from each other. We see from
the data that the order parameter rapidly converges with system size, giving
the limiting value of $x_p=0.15$. The inset(i) shows  $s$($\pi, \pi, \pi$) plotted
as a function of inverse system size ($1/L$) for three values of $x$. We find
the for $x>0.15$,  $s$($\pi, \pi, \pi$) saturates to a finite value for $L\rightarrow\infty$,
while it approaches zero for $x=0.15$. This analysis shows that indeed in
the thermodynamic limit the AF order survives below the classical percolation
threshold $x_p^{sc}$$\sim$0.31. Inset(ii) shows that the long range AF order
also persists up to $x$=0.15 for $T=0.01$.

In order to clarify the nature of the antiferromagnetic order below the
$x_p^{sc}$$\sim$0.31, in Fig.~\ref{fig_mom}(a) we present the distribution
of local moments in real space that includes both the $U=0$ and $U=8$ sites
at $T=0.02$. The local moment distribution $P_{q}(M) = \sum_{M_i} \delta(M-M_i)$
show two peaks. In the limiting case of $x=1$ the expected plot is that of
a single peak at $M=0.86$, implying uniform local moment magnitudes on all sites
within the semi-classical calculation. As $x$ is reduced, a new peak at
lower $M$ appears that indicates the moment formation at $U=0$ sites. Inset of
Fig.~\ref{fig_mom}(a) for $x=0.4$ confirms this scenario. This also corroborates
the data shown in the inset of Fig.~\ref{fig_af} (a)
that shows the signature of induced moment on the uncorrelated ($U=0$) sites.
Just as seen in Fig.~\ref{fig_af} (a), here too we see that if the $x$ reduces,
the location of the new peak moves towards $M=0.5$ signaling that
the induced moment magnitudes get weaker. In addition, we note that the
increase in the peak height at low $M$ is simply due
to increasing number of $U=0$ sites as $x$ approaches zero.

Correlating the low temperature induced $M$ in the $U=0$ sites with the AF order
parameter in Fig.~\ref{fig_mom}(b), we see a crucial fact that the long range AF
order between $U=8$ sites depends on the existence of local moments at $U=0$ sites.
Induced moment at $U=0$ sites are almost zero up to $x=0.15$ and the system remains
paramagnetic. Beyond $x=0.15$ the induced moment at $U=0$ sites increase and as
a result the system enters into an antiferromagnetic state at small $x$. This
intimate relation between long range AF order and induced moments in the $U=0$
sites is central to the stability of the AF order below the classical percolation
threshold. Above $x \sim 0.31$, while the cooperation continues to exist as
discussed in context of Fig.~\ref{fig_af} (d), the AF order can stabilize by
the usual percolation mechanism as well.

We now analyze the recovery of the classical percolation threshold in two cases,
(i) at relatively large temperature and (ii) at high U values.
In Fig.~\ref{fig_mom}(c) we show the AF order parameter as function of $x$ at three
different temperatures. While there is a overall suppression of the order parameter
magnitude with temperature, importantly we see that the critical threshold of $x$
for sustaining AF order moves towards the $x_p^{sc}$. The increase in temperature,
disrupts the local moment order for the $U=0$ sites, as was also seen from the
smaller charge gap in the DOS shown in  Fig.~\ref{fig_mit} (c). Thus the system
approaches the classical threshold for maintaining long range AF order. The percolation
threshold $x_p$ also increases with $U$ as shown in Fig~\ref{fig_mom}(d). It is
known that at large $U$ the charge fluctuations are suppressed and the Hubbard model
is well described by the Heisenberg Model. The induced magnetic moment that
mediates the antiferromagnetism below $x_{p}^{sc}$ values (for example
induced moments at U=0 sites for $x$=0.2 and $U=8$ case) are not induced at
larger $U$ values [see the inset of Fig~\ref{fig_mom}(d)] due to suppression of
spin fluctuations. As a result the $x_{p}$ increases with $U$.

\section{Conclusions}

We have employed a semi-classical technique to map out the temperature vs
dilution phase diagram of the `diluted Hubbard model'. Our results at low
temperature is close to unrestricted Hartree-Fock method and become progressively
accurate with temperature. Within this scheme we have shown that away
from the weak coupling ($U<<BW$) and strong coupling  ($U>>BW$) limit, site
dilution weakens the long range magnetic order, but allows it to survive to
dilution values much below the classical percolation threshold. At low temperature,
the Mott insulator at $x=1$ evolves in to pseudo-gapped metal (for $x\leq 0.15$)
by non-trivial spectral weight transfer phenomena that transforms the two Mott
sub-bands into four sub-bands. Our analysis shows that in this regime the system
has two distinct energy scales for charge excitations, one controlled by $U$
and another emergent gap that arises out of weak local moment induced on
the $U=0$ sites. Such behavior of DOS qualitatively
agrees with DQMC studies in two dimensions~\cite{ulmke}. By performing finite
size scaling analysis, we also show that the induced moments at the $U=0$
sites and the $U\neq 0$ sites cooperate to form long range magnetic order in
the thermodynamic limit. We further demonstrate that cooperation between the
$U=0$ and $U\neq 0$ sites is crucial to the magnetic order by showing that
increasing $U$ to large values, brings the critical percolation threshold
to the classical value which requires system spanning AF patches exclusively
made out of $U\neq 0$ sites. In addition by increasing temperature we have
shown that the closure of the Mott gap by closing the smaller charge gap
again disrupts the cooperation between the AF order between the two kinds
of sites which pushes the percolation threshold to the classical values.
This phenomenology is also seen in exact diagonalization where local Kondo
coupling and RKKY scales compete to control the magnetic properties of $s-d$
models for carbon nanotubes \cite{luo} and broadly agrees with DQMC study
on Lieb lattice \cite{lima}.

\section{Supplementary Information}

We consider the following electron-hole symmetric (EHS) one band Hubbard
Hamiltonian:

\begin{eqnarray}
H= -t\sum_{<i,j>,\sigma} c^{\dagger}_{i,\sigma}c_{j,\sigma} + U\sum_{i} \Big(n_{i,\uparrow}-\frac{1}{2}\Big) \Big(n_{i,\downarrow}-\frac{1}{2}\Big) \nonumber
\end{eqnarray}
\noindent

where `t' is the nearest neighbor hopping parameter and `U' denotes the
on-site Hubbard interaction. We set t=1 in our calculations.

After some trivial algebra and dropping a constant
term the EHS Hubbard model becomes:

\begin{eqnarray}
H = -t\sum_{<i,j>,\sigma} c^{\dagger}_{i,\sigma}c_{j,\sigma} + U\sum_{i} n_{i,\uparrow}n_{i,\downarrow} -\frac{U}{2} \sum_{i} n_{i} \nonumber
\end{eqnarray}

We denote the nearest neighbor hopping term and the third term
which is a one body operator as $H_{0}$ and the second term which
is the interaction term as $H_{1}$.
We need to transform the interaction term as a combination of two quadratic
terms to set up the Hubbard-Stratonovich (HS) decomposition formalism.

\begin{eqnarray}
n_{i,\uparrow}n_{i,\downarrow} = \Big[ \frac{1}{4} n_{i}^{2} - S_{iz}^{2} \Big] = \Big[ \frac{1}{4} n_{i}^{2} - (\textbf{S}_{i}.\hat{\Omega}_{i})^{2} \Big]
\end{eqnarray}

Here $\textbf{S}_{i}$ is the spin operator which is defined
as $\textbf{S}_{i}=\frac{\hbar}{2} \sum_{\alpha \beta}
c_{i,\alpha}^{\dagger} \sigma_{\alpha,\beta}
c_{i,\beta} $ , $\hat{\Omega}$ is an arbitrary unit vector,
$\sigma's$ are the Pauli matrices and we take $\hbar$
to be 1. We use the rotational invariance of $S_{iz}^{2}$  i.e.
$(\textbf{S}_{i}.\hat{\Omega}_{i})^{2} = S_{ix}^{2} = S_{iy}^{2} =
S_{iz}^{2}$ .  \\

Partition function for the Hamiltonian is $Z = Tr e^{-\beta H}$, where
$\beta$ is inverse temperature $(1/T)$ [$k_{B}$ is set to 1]. Next
we divide the interval $[0, \beta]$ into $M$ equally spaced slices,
defined by $\beta = M \Delta \tau$, separated by $\Delta \tau$ and
labeled from 1 to M . For large $M$, $\Delta \tau$ is a small parameter
and allows us to employ the Suzuki-Trotter decomposition, so that we
can write $e^{-\beta(H_{0} +H_{1} )} = (e^{- \Delta \tau H_{0}}
e^{- \Delta \tau H_{1}} )^{M}$ to first order in $\Delta \tau$ .
Then using Hubbard-Stratonovich identity $e^{-\Delta \tau U [\sum_{i}
\frac{1}{4} n_{i}^{2} - (\textbf{S}_{i}.\hat{\Omega}_{i})^{2}]}$ can
be shown to be proportional to,\\

$\int d\phi_{i}(l) d\Delta_{i}(l) d^{2}\Omega_{i}(l) \times \\
\hspace*{3cm} e^{- \Delta \tau [\sum_{i}(\frac{\phi_{i}^{2}}{U}
+ i \phi_{i}(l)n_{i} + \frac{\Delta_{i}^{2}}{U} -
2\Delta_{i}(l)\hat{\Omega}_{i}(l) \textbf{S}_{i}  )]}$ \\

Here $\phi_{i}(l)$ is the auxiliary field for charge density and
$\Delta_{i}(l)$ is auxiliary field for spin density and `(l)' is
a generic time slice. Further we define a new vector auxiliary
field $\textbf{m}_{i}$ as the product of $\Delta_{i}(l) \hat{\Omega}_{i}(l)$ .
Putting all of this back to the partition function we find the
effective Hamiltonian. Now we make two approximations which make
our model different from DQMC. Firstly we drop the $\tau$ dependence
of the Hamiltonian and we use the saddle point value of
$i\phi_{i} = \frac{U}{2} \textless n_{i} \textgreater $ . Lastly
by re-scaling $\textbf{m}_{i} \rightarrow (U/2)\textbf{m}_{i}$
we find the effective Hamiltonian as:

\begin{eqnarray}
H_{eff}= -t\sum_{<i,j>,\sigma} c^{\dagger}_{i,\sigma}c_{j,\sigma}
+ U/2 \sum_{i} (\textless n_i \textgreater n_i - \textbf{m}_i . \sigma_{i})  \nonumber \\
  + (U/4)\sum_{i}(\textbf{m}_{i}^2 - {\textless n_i \textgreater}^2) -\frac{U}{2} \sum_{i} n_{i}  -\mu \sum_{i} n_i \nonumber
\end{eqnarray}

The chemical potential $\mu$ is used to tune the global electron
density equal to 1. In our calculation we have considered finite $U$
at randomly chosen sites $k$ with a concentration $x$ and $U=0$ at rest
of the sites (concentration $1-x$). So, we consider following diluted
Hamiltonian for our calculations:

\begin{eqnarray}
H_{eff}= -t\sum_{<i,j>,\sigma} c^{\dagger}_{i,\sigma}c_{j,\sigma}
+ U/2 \sum_{k} (\textless n_k \textgreater n_k - \textbf{m}_k . \sigma_{k})  \nonumber \\
  + (U/4)\sum_{k}(\textbf{m}_{k}^2 - {\textless n_k \textgreater}^2) -\frac{U}{2} \sum_{k} n_{k}  -\mu \sum_{i} n_i \nonumber
\end{eqnarray}

\noindent \\
Acknowledgment: We acknowledge use of Meghnad2019 computer cluster at SINP.

redpajama_set_name: RedPajamaArXiv


There are seven recently remodeled lakefront rooms each with their own private decks overlooking Highland Lake. A gentle rolling lawn leads to a beautiful sandy beach with a selection of boats for our guests to enjoy. Picnic tables, barbeques and lawn chairs abound. Even a fire pit.
Each guest room has either two double beds or one queen. All rooms have air-conditioning and their own bathroom with shower. There is inside seating or outside seating on the private deck. Each room has cable TV.


text:
Home › Rene Bond Movies › {{url}}
All Rene Bond Movies
After Hours Cinema
Factory 2000
Retro-Seduction Cinema
Venus Theatre DVDs
Rene Bond Movies
Alternative Cinema - the largest collection of Rene Bond films under one roof!
Rene Bond (October 11, 1950 – June 2, 1996) began her career in films produced by Harry Novak in the late 1960s before moving on to adult films in the early 1970s. She was active in the 1970s LA scene, appearing in more than 100 films and loops. She was noted for her petite figure and conveyed innocence or naivete in her acting approach.

redpajama_set_name: RedPajamaCommonCrawl


Inspired by the 20th century designs of the late iconic luxury furniture maker, Karl Springer, this snakeskin wrapped petite telephone table is in a class by itself. Original Karl Springer furniture, known for its combination of rare woods and exotic materials, is nearly impossible to find. But by teaming with a former Springer artisan I have created a table embodying the highest quality materials and workmanship that marked Springer's original furniture.
This one-of-a-kind table features genuine sea snakeskin in a dramatic white with black pattern. The underside of table and shelf are lined with felt. The snakeskin on this table has been lacquered with multiple coats of high gloss clear lacquer, which adds both beauty and protection. Size of table measures 12 ½" wide x 9" deep x 17" tall. Antique brass casters complete the look of this table.


Binance Coin has continued to defy the odds as it carries to appreciate despite the rest of the market falling. The cryptocurrency has gained 1.10% over the past 24 hours of trading with a 4.48% increase over the past 7 trading days. Binance coin is exchanging hands at $13.68, at time of writing.
The Ethereum-based token was created by the team behind the Binance platform. Binance Exchange, founded in 2017, has grown to become one of the biggest cryptocurrency exchanges in the world. The Binance token sale raised $15 million in its ICO as the BNB token allows users to receive discounts for fees involved with trading on their platform. Currently using BNB to purchase cryptocurrencies will result in a 50% reduction in trading fees, which compound over time resulting in extreme savings for traders.
burn" results in the supply of the BNB token dropping, thus making the coins more valuable. The team has stated that they will continue to run their BNB buy-back scheme until 50% of the tokens have been removed from circulation, eventually leaving 100 million BNB tokens in total. So far, they have had 4 quarters of token burns, resulting in over 7 million tokens being burnt.
BNB is currently ranked 17th in terms of overall market cap across the entire industry, with a total market cap value of $1.31 billion.
Let us continue to analyze price action for BNB over the long term.
Analyzing the market over the long-term advantage above, we can see that BNB had experienced a major price surge toward the end of 2018 when price action started from a low of $1.34 on November 12, 2017 and appreciated to an all-time high priced at $25.18 on January 12, 2018. This was a price increase of over 1,680% from low to high.
The market went on to depreciate after placing this all-time high, initially finding support at the .5 Fibonacci Retracement priced at $13.37 during January. This is a Fibonacci Retracement measured from the entire bullish run aforementioned.
Price action continued to fall during February until support was found at the .786 Fibonacci Retracement priced at $6.57. This price proved to become the yearly low as the market rebounded from this area.
Let us analyze price action a little closer over the shorter period to highlight any potential support and resistance zones.
Analyzing the market from a shorter perspective displayed above, we can see that price action had experienced a second bullish run throughout 2018 when the market started at a low of $7.06 on March 9, 2018 and extended to a high of $17.47 on June 6, 2018. This was an increase totaling 145% from low to high.
We can see that as July began trading, price action began to decline, finding support slightly below the short-term .5 Fibonacci Retracement (drawn in red) priced at $12.34. More specifically, price action had found support and reversed at a downside 1.414 Fibonacci Extension level priced at $11.78.
The market is currently trading at support, located at the short-term .382 Fibonacci Retracement priced at $13.55. This area of support is significantly bolstered by the 100-day moving average and the long-term .5 Fibonacci Retracement level, which are both currently hovering marginally below this level.
If the bullish momentum continues, we expect immediate resistance to be located at July's price high which approached the $15 handle. Resistance above this level is expected at the long-term .382 FIbonacci Retracement level priced at $16.18. If the market can continue further higher beyond the high seen at $17.47, we expect the nearest level of resistance to be located at 1.272 Fibonacci Extension (not drawn on the chart above) priced at $20.28.
Alternatively, if the bearish momentum picks up, immediate support can be located at the short-term .5 Fibonacci Retracement priced at $12.34. Further support located below this can be found at the downside 1.414 Fibonacci Extension priced at $11.78, followed by the 1.618 Fibonacci Extension priced at $10.98.
The RSI technical indicator is currently marginally favoring the bulls within the market as it currently trades above the 50 handle. If the RSI can mange to continue to stay above the 50 handle, we can expect the bullish momentum to continue within the market.
Let us continue to analyze BNB against BTC over the long term.
Analyzing the market from the long-term perspective above, we can see that BNB had experienced two significant bullish waves throughout its trading lifetime. The first wave started from a low of 1,519 SATS on December 13, 2017 and extended to a high of 18,382 SATS on January 12, 2018. This was a price increase totaling 1,080% from low to high.
The second bullish wave started from a low of 8,505 SATS on March 11, 2018 and extended to an all-time high of of 26,555 SATS on June 18, 2018. This second wave resulted in a price increase totaling 210%.
We can see that during July, the market had significantly declined and consequently fell below the 100-day moving average.
Let us continue to analyze price action a little closer from the perspective of the second bullish wave.
The graph above shows the second bullish wave which totaled 210%, as described in the previous section. We can see that July had caused the market to slip significantly, until support was found at the .618 Fibonacci Retracement priced at 15,310 SATS. This is a Fibonacci Retracement measured from the entire second bullish wave described previously.
The market has since rebounded and is currently trading at resistance marked by the 100-day moving average. If price action can continue above the 100-day moving average, we expect immediate resistance to be located at the short-term .382 Fibonacci Retracement priced at 19,619 SATS.
Alternatively, if the bearish momentum continues to progress, we expect immediate support to be located at the short-term .5 Fibonacci Retracement priced at 17,464 SATS. Support below this level can be located at the .618 Fibonacci Retracement priced at 15,310 SATS.
The RSI indicator has recently managed to battle its way back above the 50 handle, indicating that the bulls are beginning to gather momentum once again. If the RSI can continue to rise, we can expect the bullish run follow suit.


text:
goog.provide('blk.env.client.EntityRenderer');

goog.require('blk.env.Face');
goog.require('blk.env.client.BaseRenderer');
goog.require('goog.vec.Mat4');
goog.require('goog.vec.Quaternion');
goog.require('goog.vec.Vec3');
goog.require('goog.vec.Vec4');

/**
 * Handles entity rendering.
 *
 * TODO(benvanik): subclasses for various entity types
 * TODO(benvanik): generic geometry builder vs. blockbuilder
 *
 * @constructor
 * @extends {blk.env.client.BaseRenderer}
 * @param {!blk.graphics.RenderState} renderState Render state manager.
 * @param {!blk.env.Entity} entity Entity to render.
 */
blk.env.client.EntityRenderer = function(renderState, entity) {
  goog.base(this, renderState);

  /**
   * Entity to render.
   * @type {!blk.env.Entity}
   */
  this.entity = entity;

  /**
   * Shared block builder.
   * @private
   * @type {!blk.graphics.BlockBuilder}
   */
  this.blockBuilder_ = renderState.blockBuilder;

  /**
   * Current face buffer generated with the block builder.
   * @private
   * @type {WebGLBuffer}
   */
  this.faceBuffer_ = null;

  /**
   * Number of elements in the current face buffer.
   * @private
   * @type {number}
   */
  this.faceBufferElementCount_ = 0;

  /**
   * Bytes used by the face buffer.
   * @private
   * @type {number}
   */
  this.faceBufferSize_ = 0;

  /**
   * Sprite buffer, for adorners/text/etc.
   * @private
   * @type {!gf.graphics.SpriteBuffer}
   */
  this.spriteBuffer_ = renderState.createSpriteBuffer();
  this.registerDisposable(this.spriteBuffer_);

  /**
   * Current title string, if any.
   * @private
   * @type {?string}
   */
  this.cachedTitle_ = null;
  this.updateTitle_();

  // Entangle with entity
  entity.renderData = this;

  this.restore();
  this.spriteBuffer_.restore();
};
goog.inherits(blk.env.client.EntityRenderer, blk.env.client.BaseRenderer);

/**
 * @override
 */
blk.env.client.EntityRenderer.prototype.disposeInternal = function() {
  // Untangle from entity
  this.entity.renderData = null;

  goog.base(this, 'disposeInternal');
};

/**
 * @override
 */
blk.env.client.EntityRenderer.prototype.discard = function() {
  var gl = this.graphicsContext.gl;

  // Delete buffer
  gl.deleteBuffer(this.faceBuffer_);
  this.faceBuffer_ = null;
  this.faceBufferElementCount_ = 0;
  this.faceBufferSize_ = 0;
  this.estimatedSize = 0;

  goog.base(this, 'discard');
};

/**
 * @override
 */
blk.env.client.EntityRenderer.prototype.restore = function() {
  // Begin build
  this.blockBuilder_.ensureCapacity(2);

  // Grab texture coordinates
  var sideTexCoords = goog.vec.Vec4.createFloat32();
  this.renderState.blockAtlas.getSlotCoords(118, sideTexCoords);
  var faceTexCoords = goog.vec.Vec4.createFloat32();
  this.renderState.blockAtlas.getSlotCoords(119, faceTexCoords);
  var topTexCoords = goog.vec.Vec4.createFloat32();
  this.renderState.blockAtlas.getSlotCoords(102, topTexCoords);

  // Add faces
  this.blockBuilder_.addFace(blk.env.Face.POS_Z, 0, 0, 0, sideTexCoords);
  this.blockBuilder_.addFace(blk.env.Face.NEG_Z, 0, 0, 0, faceTexCoords);
  this.blockBuilder_.addFace(blk.env.Face.POS_Y, 0, 0, 0, topTexCoords);
  this.blockBuilder_.addFace(blk.env.Face.NEG_Y, 0, 0, 0, sideTexCoords);
  this.blockBuilder_.addFace(blk.env.Face.POS_X, 0, 0, 0, sideTexCoords);
  this.blockBuilder_.addFace(blk.env.Face.NEG_X, 0, 0, 0, sideTexCoords);

  // Finish the build
  var results = this.blockBuilder_.finish();
  this.faceBuffer_ = results.buffer;
  this.faceBufferElementCount_ = results.elementCount;
  var oldSize = this.faceBufferSize_;
  this.faceBufferSize_ = results.bytesUsed;
  this.estimatedSize = this.faceBufferSize_;

  goog.base(this, 'restore');
};

/**
 * Updates the entity title adorner if required.
 * @private
 */
blk.env.client.EntityRenderer.prototype.updateTitle_ = function() {
  var title = this.entity.title;
  if (title == this.cachedTitle_) {
    return;
  }
  this.cachedTitle_ = title;

  this.spriteBuffer_.clear();

  if (title && title.length) {
    var font = this.renderState.font;
    var wh = font.measureString(title);
    font.prepareString(this.spriteBuffer_, title, 0xFFFFFFFF,
        -wh[0] / 2 , 0);
  }
};

/**
 * @override
 */
blk.env.client.EntityRenderer.prototype.addDebugVisuals = function(buffer) {
  buffer.addCube(
      goog.vec.Vec3.createFloat32FromValues(0, 0, 0),
      goog.vec.Vec3.createFloat32FromValues(1, 2, 1),
      0xFFFF0000);
};

/**
 * @override
 */
blk.env.client.EntityRenderer.prototype.render = function(frame, viewport) {
  // Handle interpolation
  this.entity.interpolate(frame.time);

  var state = this.entity.state;
  var wm = blk.env.client.EntityRenderer.tmpMat4_[0];
  goog.vec.Mat4.makeIdentity(wm);
  var rm = blk.env.client.EntityRenderer.tmpMat4_[1];
  goog.vec.Quaternion.toRotationMatrix4(state.rotation, rm);
  var tm = blk.env.client.EntityRenderer.tmpMat4_[2];
  goog.vec.Mat4.setFromValues(tm,
      1, 0, 0, 0,
      0, 2, 0, 0,
      0, 0, 1, 0,
      -0.5, -1.5, -0.5, 1);
  goog.vec.Mat4.multMat(rm, tm, rm);
  goog.vec.Mat4.translate(wm,
      state.position[0],
      state.position[1],
      state.position[2]);
  goog.vec.Mat4.multMat(wm, rm, wm);

  this.blockBuilder_.draw(viewport, wm,
      this.faceBuffer_, this.faceBufferElementCount_);
};

/**
 * @override
 */
blk.env.client.EntityRenderer.prototype.renderDebug =
    function(frame, viewport) {
  if (this.debugLineBuffer) {
    // Handle interpolation
    this.entity.interpolate(frame.time);

    var state = this.entity.state;
    var wm = blk.env.client.EntityRenderer.tmpMat4_[0];
    goog.vec.Mat4.makeIdentity(wm);
    var rm = blk.env.client.EntityRenderer.tmpMat4_[1];
    goog.vec.Quaternion.toRotationMatrix4(state.rotation, rm);
    var tm = blk.env.client.EntityRenderer.tmpMat4_[2];
    goog.vec.Mat4.setFromValues(tm,
        1, 0, 0, 0,
        0, 1, 0, 0,
        0, 0, 1, 0,
        -0.5, -1.5, -0.5, 1);
    goog.vec.Mat4.multMat(rm, tm, rm);
    goog.vec.Mat4.translate(wm,
        state.position[0],
        state.position[1],
        state.position[2]);
    goog.vec.Mat4.multMat(wm, rm, wm);
    this.debugLineBuffer.draw(this.renderState, viewport, wm);
  }
};

/**
 * Renders an entities adorners.
 * @param {!gf.RenderFrame} frame Current render frame.
 * @param {!gf.vec.Viewport} viewport Current viewport.
 */
blk.env.client.EntityRenderer.prototype.renderAdorners =
    function(frame, viewport) {
  this.updateTitle_();

  if (this.cachedTitle_ && this.cachedTitle_.length) {
    var state = this.entity.state;
    var scale = 1 / 16;
    var scaleMatrix = blk.env.client.EntityRenderer.tmpMat4_[0];
    goog.vec.Mat4.makeScale(scaleMatrix, scale, -scale, 1);
    var worldMatrix = blk.env.client.EntityRenderer.tmpMat4_[1];
    viewport.makeBillboard(worldMatrix);
    goog.vec.Mat4.multMat(worldMatrix, scaleMatrix, worldMatrix);
    worldMatrix[12] = state.position[0];
    worldMatrix[13] = state.position[1] + 1.5;
    worldMatrix[14] = state.position[2];

    this.spriteBuffer_.draw(viewport.viewProjMatrix, worldMatrix);
  }
};

/**
 * Temp mat4.
 * @private
 * @type {!Array.<!goog.vec.Mat4.Type>}
 */
blk.env.client.EntityRenderer.tmpMat4_ = [
  goog.vec.Mat4.createFloat32(),
  goog.vec.Mat4.createFloat32(),
  goog.vec.Mat4.createFloat32()
];

redpajama_set_name: RedPajamaGithub


SB 7030 School Safety and Security (now in Infrastructure and Security committee ) is a long sucker of a bill which includes a revamp of the school system as it relates to mental health, but the part we should be interested was that this bill includes allowing teachers to volunteer for the Guardian program and carry in school after proper training.
Two amendments were introduced by Senator Lori Berman (D) prohibiting not only regular school teachers but Charter school teachers from being part of the Guardian program. One was found unfavorable and the other was withdrawn. So, not a bad day for that particular bill.
I would use the BCC feature in your email so it does not look like a mass email for organic Viagra.
See? Told ya I was working on this stuff.
Reminder, we have some seriously nasty bills coming: AWB, Gun Registration, UBC and the elimination of preemption of the field of regulation of firearms and ammunition. This last one, it seems they have a particular hard on for it as it would pretty much hill CWP in Florida and that would be a monumental feather in the Gun Control's cap. Revert Concealed Carry in the State that started it all.
Apparently the concept of the advantage of concealed carry escapes the senator.
Previous PostPrevious When the Dumb is out there to see.


text:
Tuesday Roundup: Pine Forest's tight win at Gulf Breeze highlights busy slate to open 2022
Patrick Bernadeau
Note: Is your team's results missing from the roundup? Be sure to update your MaxPreps page regularly or file stats to the PNJ via email or phone.
Lucas Semb can be reached at lsemb@gannett.com or 850-281-7414.
Patrick Bernadeau can be reached at pbernadeau@gannett.com or 850-503-3828.
Here's a roundup of high school games and matches played on Tuesday, Jan. 4:
Pine Forest 56, Gulf Breeze 54
Robert Ward delivered a team-best 15 points to lead the Eagles in a nail-biter at Gulf Breeze.
Omarayon Turner (11) and Ozell Purifoy (10) each scored in double figures. Turner and La'Nygel McCracken grabbed eight rebounds apiece. Ward finished with seven boards.
Pine Forest improved its record to 10-4 following wins in five of its last six games. The team is host to Tate at 7:30 p.m. Thursday.
Booker T. Washington 69, Escambia 60
Behind 58 percent shooting from the field, the Wildcats collected a nine-point home win against the Gators. The hosts outscored Escambia 22-8 in the first quarter.
Sophomore Alex Jasquith paced Booker T. Washington with 18 points on 8-for-11 shooting while junior Nicholas Hughes added 13 points. Each player snatched three steals. Tyler White drilled all five of his field-goal attempts to finish with 10 points and six rebounds.
Waymond Jordan poured in a game-high 19 points to lead Escambia, who is host to Milton at 7:30 p.m. Thursday. The Wildcats visit Pine Forest at 7:30 p.m. Friday.
Latest AOTW winner:This Tate sophomore was dynamite before the holiday break to win PNJ Athlete of the Week
Jay football change: Longtime Jay staple Brian Watson hired as next Royals head football coach
High School Soccer:Gulf Breeze scores twice in final moments, slips past West Florida
Pensacola 77, West Florida 53
The Tigers needed a Caleb Young buzzer-beater to sneak past the Jaguars on Dec. 13. This time around, the rematch was no contest as Pensacola cruised to its third-straight victory.
Drilling four 3-pointer, Young finished with a team-best 23 points. Jason Peoples and James Robinson each delivered 16 points. Robinson also ripped down 16 rebounds (seven offensive) and dished out five assists.
The Tigers are back on the floor at 7:30 p.m. Tuesday at Tate. West Florida is host to Escambia at 7:30 p.m. Friday.
Pensacola Catholic 38, Pace 36
The Crusaders captured their second consecutive two-point victory after winning at Pace.
Improving its record to 4-7, Pensacola Catholic looks to extend its winning streak to three games when it plays at 6:45 p.m. Friday at Pensacola Christian Academy. The Patriots play 7 p.m. Thursday at Crestview.
Niceville 58, Navarre 51
Dropping their third game in a row, the Raiders suffered a seven-point defeat at Niceville.
Navarre has fallen to 7-7 with its recent slide. The team is host to Gulf Breeze at 7:30 p.m. Thursday.
Paxton 77, Pensacola Christian Academy 35
The Warriors were outscored by double figures in each of the first three quarters during their blowout loss at Paxton.
Booker T. Washington 44, Escambia 43 (OT)
For the second time this season, the Wildcats have walked out of their home gym with a one-point overtime triumph.
Booker T. Washington's latest escape avenged a 54-37 loss to the Gators on Nov. 30.
Jasmine Mayes led the victors with 23 points, nine rebounds and five steals. Samaria Brooks chipped in six points and 11 rebounds.
Escambia returns home to face Milton at 6 p.m. Thursday. The Wildcats are host to McGill-Toolen (Ala.) at 6 p.m. Wednesday.
Milton 41, Central 24
In typical fashion, the Panthers added a tally in the win column following a low-scoring affair at home against Central.
It is the sixth time this season Milton has held its opponent to 30 points or less.
The Jaguars previously fell to the Panthers 32-23 on Dec. 3. Central is host to Walton at 6 p.m. Thursday.
West Florida 56, Pensacola 24
Snapping a three-game slump, the Jaguars used a 21-4 second quarter to win comfortably at Pensacola.
West Florida plays 6 p.m. Friday at Choctaw. The Tigers take on Tate at 6 p.m. Tuesday.
Pace 67, West Florida Baptist Academy 24
The Patriots continue to roll after capturing a 41-point win over the Conquerors.
Victorious in five of its last six games, Pace visits Jay at 6:45 p.m. Thursday. Suffering just their third defeat of the season, West Florida Baptist Academy is host to Pensacola Christian Academy at 5:30 p.m. Thursday.
Gulf Breeze 44, Elberta 11
The Dolphins snapped a three-game losing streak with a road triumph over the winless Warriors.
Gulf Breeze returns home to play Laurel Hill at 6 p.m. Monday.
Central Christian 63, East Hill Christian 14
The Eagles remain winless this season after falling to Central Christian (Ala.).
Tate 2, Navarre 0
Junior forward Caleb Wise notched a goal in each half during the Aggies' District 1-6A victory against the Raiders. Will O'Brien stopped five shots to help Tate post its ninth shutout in 11 matches this season.
Tate improved to 10-0-1 and bumped its goal differential to plus-42. The Aggies play at 5 p.m. Thursday at Crestview. Dropping its last seven matches, Navarre is host to Chiles at 12 p.m. Saturday.
Freeport 3, East Hill Christian 1
After each team scored in the first half, the Eagles relinquish two goals in the second half to fall at Freeport.
East Hill Christian is 1-4 in its last five matches. The team is host to Pensacola at 6 p.m. Friday.
Milton 2, Marianna 1
The Panthers captured their second victory of the season after scoring two-half goals at Marianna. Each of their two wins have come on the road.
Milton is host to Pensacola at 7:30 p.m. Thursday.
Milton 6, Booker T. Washington 1
The Panthers raced out to 4-1 advantage in the first 40 minutes before added two goals in the second half in a win at Booker T. Washington. Elyse Carmichael put in the Wildcats' only score.
Unbeaten in its last five matches, Milton is host to Mosley at 7 p.m. Friday. Booker T. Washington visits Escambia at 7 p.m. Thursday.
Pace 8, Pensacola 0
The Patriots earned its first victory since Dec. 7 after clubbing Pensacola at home. Pace scored five goals in the first half and added three more in the final 40 minutes.
The Tigers are scoreless in their last three matches. Pensacola is host to Arnold at 7 p.m. Thursday. The Patriots returns home to take on West Florida at 7 p.m. Friday.
Navarre 4, Choctaw 0
Hunter Wallace knocked in a pair of goals as the Raiders improved to 5-1 in their last six matches after blanking the Indians. Cici Buffalino and Jessica Farrer each added a goal while Selissa Bly, Kayla Johnson and Adreahna Busch all were credited with an assist.
Navarre is host to Montverde Academy at 7 p.m. Friday.


Smokin' Tacos features a fusion of Southern Barbeque and Tex-mex cuisine. All of our meat is brined, rubbed and smoked in our on board smoker, low and slow. We offer a rotating menu of delectable savory treats curbside or at private and public events. Look for us in a neighborhood near you! Call us and bring us out, we would love to treat you to a taco that you will wake up thinking about the next day.


In 2007, the largest school employee credit union in the nation, Orange County (CA) Teacher's Credit Union, changed its name to SchoolsFirst, and in 2010 they looked to revitalize and reinforce their new brand. Crosby Associates created a visual identity and design program that included an open book logo, comprehensive standards for print, marketing and electronic communications, in-bank promotions, and retail signage. Now with assets of more than $9 billion, SchoolsFirst rebranded their 44 branches, showcasing the new visual identity.


text:
Corporation Tax Act 2009
Previous: Chapter
Next: Chapter
Changes over time for: Chapter 6
There are outstanding changes not yet made by the legislation.gov.uk editorial team to Corporation Tax Act 2009. Any changes that have already been made by the team appear in the content and are referenced with annotations.
Changes and effects yet to be applied to Part 3 Chapter 6:
S 1217N(3) modified by 2010 c. 4 s. 357UI (as inserted) by 2015 c. 21 s. 1
Act words substituted by 2014 c. 14 Sch. 4 para. 141
Blanket amendment words substituted by S.I. 2011/1043 art. 3 4
Pt. 2 Ch. 3A applied by 2011 c. 11, Sch. 19 para 15Z2(3) (as inserted) by 2018 c. 3 Sch. 9 para. 2
Pt. 5 Ch. 16A inserted by 2017 c. 32 Sch. 4 para. 4
Pt. 5 Ch. 16A modified by 2010 c. 4 s. 676AH(1) (as inserted) by 2017 c. 32 Sch. 4 para. 75
Pt. 8 Ch. 15A inserted by 2019 c. 1 Sch. 9 para. 6
Pt. 8A amendment to earlier affecting provision 2010 c. 4 s. 357WG by 2017 c. 32 Sch. 7 para. 20(1)
Pt. 15C inserted by 2014 c. 26 Sch. 4 para. 1
Pt. 15D inserted by 2016 c. 24 Sch. 8 para. 1
Pt. 15E inserted by 2017 c. 32 Sch. 6 para. 1
Pt. 15E modified by 2010 c. 4 s. 357UR(3) (as inserted) by 2017 c. 32 Sch. 6 para. 17
s. 1044(8 word substituted by 2015 c. 11 s. 27(3)(a)
s. A1(2)(ha) inserted by 2016 c. 24 Sch. 10 para. 5(b)
s. A1(2)(jb) inserted by 2017 c. 32 Sch. 5 para. 5(b)
s. 2(2A) words substituted by 2015 c. 11 Sch. 7 para. 58
s. 5(2)(a) word omitted by 2019 c. 1 Sch. 5 para. 2(a)
s. 5(2)(c)(d) inserted by 2019 c. 1 Sch. 5 para. 2(b)
s. 5(2A) inserted by 2016 c. 24 s. 76(3)
s. 5(2A) words substituted by 2019 c. 1 Sch. 1 para. 110(2)
s. 5(3A)(3B) inserted by 2019 c. 1 Sch. 5 para. 3
s. 5(5) inserted by 2019 c. 1 Sch. 1 para. 110(4)
s. 5(5) inserted by 2019 c. 1 Sch. 5 para. 5
s. 5A 5B inserted by 2016 c. 24 s. 76(5)
s. 18(2A) inserted by 2016 c. 24 s. 76(8)(b)
s. 18A(2A) inserted by 2016 c. 24 s. 76(7)
s. 18A(2A) words substituted by 2019 c. 1 Sch. 5 para. 12
s. 18A(2B) inserted by 2019 c. 1 Sch. 1 para. 111
s. 19(2A) substituted by 2019 c. 1 Sch. 5 para. 13
s. 19(4)(5) inserted by 2019 c. 1 Sch. 1 para. 112(4)
s. 40A 40B inserted by S.I. 2018/282 art. 6(2)
s. 54(1A) inserted by 2014 c. 26 Sch. 17 para. 4(4)(b)
s. 92A and cross-heading inserted by 2014 c. 26 Sch. 17 para. 4(2)
s. 104A(7A) inserted by 2015 c. 33 s. 31(2)
s. 104D(5) word inserted by 2015 c. 11 s. 28(4)(a)
s. 104E(5) word inserted by 2015 c. 11 s. 28(4)(b)
s. 104G(6) word inserted by 2015 c. 11 s. 28(4)(c)
s. 104H(7) word inserted by 2015 c. 11 s. 28(4)(d)
s. 104J(6) word inserted by 2015 c. 11 s. 28(4)(e)
s. 104K(7) word inserted by 2015 c. 11 s. 28(4)(f)
s. 104M(3) word substituted by 2015 c. 11 s. 27(2)
s. 104N(3) words inserted by 2014 c. 26 Sch. 1 para. 10
s. 104Y(2) words substituted by 2015 c. 11 s. 28(5)
s. 104BA(4) inserted by 2014 c. 26 Sch. 4 para. 9
s. 104BA(5) inserted by 2017 c. 32 Sch. 6 para. 10
s. 104WA and cross-heading inserted by 2015 c. 33 s. 31(3)
s. 133A-133N and cross-heading inserted by 2015 c. 33 s. 18(1)
s. 133F(2A)(2B) inserted by 2016 c. 24 s. 56(2)
s. 133F(7) words inserted by 2016 c. 24 s. 56(3)
s. 133I(1)(b) omitted by S.I. 2019/689 reg. 16(2)
s. 133I(1)(c) omitted by S.I. 2019/689 reg. 16(2)
s. 133M(5)(b)(ii) substituted by 2016 c. 24 s. 56(6)
s. 144(1)(c)(iii) and word inserted by S.I. 2015/374 art. 8(2)(c)
s. 161(1A)-(1C) inserted by 2015 c. 33 s. 40(1)
s. 250A and cross-heading inserted by 2016 c. 24 s. 73(2)
s. 264(2)(za) inserted by 2016 c. 24 s. 73(7)
s. 264(2A)(za) inserted by 2016 c. 24 s. 73(7)
s. 301(1A) inserted by 2019 c. 1 Sch. 5 para. 15(3)
s. 306(2)(za) inserted by 2015 c. 33 Sch. 7 para. 2(a)
s. 306A and cross-heading inserted by 2015 c. 33 Sch. 7 para. 3
s. 307(2A)-(2C) inserted by 2015 c. 33 Sch. 7 para. 4(3)
s. 308(1A)(1B) inserted by 2015 c. 33 Sch. 7 para. 5(3)
s. 313(6)(7) substituted for s. 313(6) by 2015 c. 33 Sch. 7 para. 7(8)
s. 318(7)(8) inserted by 2015 c. 33 Sch. 7 para. 12(6)
s. 320B inserted by 2019 c. 1 Sch. 20 para. 5
s. 322(2A)(zb) inserted by 2016 c. 24 s. 73(5)
s. 322(5A) inserted by 2014 c. 26 s. 26(3)
s. 322(5A) words inserted by S.I. 2014/3329 art. 123
s. 322(5B) inserted by 2015 c. 33 Sch. 7 para. 16(4)
s. 322(6A) inserted by 2015 c. 33 Sch. 7 para. 16(5)
s. 323(A1) inserted by 2015 c. 33 Sch. 7 para. 17
s. 328(3)-(3C) substituted for s. 328(3) by 2015 c. 33 Sch. 7 para. 20(4)
s. 328(4)(4ZA) substituted for s. 328(4) by 2015 c. 33 Sch. 7 para. 20(5)
s. 330A-330C and cross-heading inserted by 2015 c. 33 Sch. 7 para. 23
s. 333(2)(a) words in s. 333(2) renumbered as s. 333(2)(a) by 2019 c. 1 Sch. 5 para. 16(a)
s. 333(2)(b)-(d) inserted by 2019 c. 1 Sch. 5 para. 16(b)
s. 334(5) inserted by 2019 c. 1 Sch. 5 para. 17(5)
s. 352(3A)-(3C) inserted by 2015 c. 33 Sch. 7 para. 30
s. 352B power to amend conferred by 2019 c. 1 Sch. 12 para. 5
s. 358(4)(4A) substituted for s. 358(4) by 2015 c. 33 Sch. 7 para. 33(2)
s. 359(3) inserted by 2015 c. 33 Sch. 7 para. 34(3)
s. 361D inserted by 2015 c. 33 Sch. 7 para. 37
s. 362(6) inserted by 2015 c. 33 Sch. 7 para. 38
s. 398(2)(f) and word inserted by 2019 c. 1 Sch. 20 para. 7(2)(b)
s. 420A and cross-heading inserted by 2019 c. 1 Sch. 20 para. 2
s. 431(10)(a) words renumbered as s. 431(10)(a) by S.I. 2019/689 reg. 16(7)(e)(i)
s. 431(10)(b) inserted by S.I. 2019/689 reg. 16(7)(e)(ii)
s. 440(2)(h) and word inserted by 2015 c. 33 Sch. 7 para. 45(c)
s. 446(8) inserted by 2016 c. 24 Sch. 7 para. 3
s. 447(4A) inserted by 2016 c. 24 Sch. 7 para. 5
s. 455B-455D and cross-heading inserted by 2015 c. 33 Sch. 7 para. 51
s. 456(1)(b) and word inserted by 2017 c. 32 Sch. 4 para. 3(b)
s. 465(3)(zza) inserted by 2019 c. 1 Sch. 20 para. 7(3)
s. 465B and cross-heading inserted by 2015 c. 33 Sch. 7 para. 52
s. 465B(9)(ka) inserted by 2019 c. 1 Sch. 12 para. 2
s. 475C and cross-heading inserted by 2019 c. 1 Sch. 20 para. 3(1)
s. 475C power to amend conferred by 2019 c. 1 Sch. 20 para. 19(1)
s. 475C(5) words omitted by S.I. 2019/1250 reg. 2(1)(b)
s. 475C(5)(b) words substituted by S.I. 2019/1250 reg. 2(1)(a)
s. 475C(8)(b)(c) substituted by S.I. 2019/1250 reg. 3
s. 507(2)(j)(k) inserted by 2018 c. 3 s. 34(2)(b)(ii)
s. 507(2)(j) omitted by S.I. 2019/689 reg. 16(10)(b)(ii)
s. 507(2)(k) omitted by S.I. 2019/689 reg. 16(10)(b)(ii)
s. 507(2A) inserted by S.I. 2019/689 reg. 16(10)(c)
s. 507(2A) words omitted by S.I. 2019/818 reg. 7(2)(b)
s. 507(2A) words substituted by S.I. 2019/818 reg. 7(2)(a)
s. 541(3) excluded by 2010 c. 8 s. 452(3)(a) (as inserted) by 2017 c. 32 Sch. 5 para. 1
s. 574(2A) inserted by 2019 c. 1 Sch. 5 para. 18
s. 594(2)(g)(ga) substituted for s. 594(2)(g) by 2015 c. 33 Sch. 7 para. 60(b)
s. 594(2)(za) inserted by 2015 c. 33 Sch. 7 para. 60(a)
s. 595(2A)-(2C) inserted by 2015 c. 33 Sch. 7 para. 62(3)
s. 597(1A)(1B) inserted by 2015 c. 33 Sch. 7 para. 63(3)
s. 607A-607C inserted by 2015 c. 33 Sch. 7 para. 71
s. 682(8)(a) words renumbered as s. 682(8)(a) by S.I. 2019/689 reg. 16(14)(d)(i)
s. 682(8)(b) inserted by S.I. 2019/689 reg. 16(14)(d)(ii)
s. 689(2)(f) and word inserted by 2015 c. 33 Sch. 7 para. 89(b)
s. 694(11)-(14) inserted by 2016 c. 24 Sch. 7 para. 11(4)
s. 711(8)(fa) inserted by 2019 c. 1 Sch. 9 para. 2
s. 738A inserted by 2015 c. 21 Sch. 2 para. 1
s. 739(1A) inserted by 2018 c. 3 s. 20(1)
s. 746(2)(ba) substituted by 2015 c. 33 s. 33(3)
s. 746(2)(ba) substituted by 2019 c. 1 Sch. 9 para. 4
s. 753(4)-(6) inserted by 2017 c. 32 Sch. 4 para. 5(3)
s. 780(5)(aa) inserted by 2019 c. 1 s. 26(2)
s. 782A inserted by 2019 c. 1 s. 26(3)
s. 785(2A)(2B) inserted by 2019 c. 1 s. 26(4)(b)
s. 793(3A)(3B) inserted by 2019 c. 1 Sch. 5 para. 24(4)
s. 793A inserted by 2019 c. 1 Sch. 5 para. 25
s. 808C inserted by 2014 c. 26 Sch. 4 para. 10
s. 808D inserted by 2016 c. 24 Sch. 8 para. 9
s. 808E inserted by 2017 c. 32 Sch. 6 para. 11
s. 816A omitted by 2019 c. 1 Sch. 9 para. 5
s. 819(5)(ba)(bb) substituted for s. 819(5)(b) by S.I. 2019/689 reg. 16(17)(f)
s. 823(1A) inserted by S.I. 2019/689 reg. 16(20)(a)
s. 844(2A) omitted by 2015 c. 33 s. 33(6)
s. 844(2ZA) inserted by 2018 c. 3 s. 21(1)
s. 849B-849D and cross-heading inserted by 2015 c. 11 s. 26(4)
s. 849B-849D and cross-heading omitted by 2015 c. 33 s. 33(7)
s. 849AB-849AD and cross-heading inserted by 2018 c. 3 s. 21(2)
s. 863(1)(b)(i) words in s. 863(1)(b) renumbered as s. 863(1)(b)(i) by 2019 c. 1 Sch. 5 para. 27(a)
s. 863(1)(b)(ii)-(iv) inserted by 2019 c. 1 Sch. 5 para. 27(b)
s. 863A inserted by 2019 c. 1 Sch. 8 para. 12(3)
s. 882(5A)-(5D) inserted by 2016 c. 24 s. 52(2)
s. 895(5) inserted by 2016 c. 24 s. 52(4)
s. 999(6A) inserted by 2014 c. 26 Sch. 8 para. 142(5)
s. 1002(5) inserted by 2014 c. 26 Sch. 9 para. 40
s. 1007A inserted by 2014 c. 26 Sch. 9 para. 42
s. 1009(6) omitted by 2017 c. 10 s. 12(4)(b)
s. 1011(4)(b) words omitted by 2017 c. 10 s. 12(4)(d)
s. 1015A 1015B inserted by 2014 c. 26 Sch. 9 para. 43
s. 1016(1A) inserted by 2014 c. 26 Sch. 9 para. 44(3)
s. 1022(5) omitted by 2017 c. 10 s. 12(4)(f)
s. 1038B omitted by 2017 c. 10 s. 12(4)(g)
s. 1040ZA(4) inserted by 2014 c. 26 Sch. 4 para. 11
s. 1048(3)(za) inserted by 2017 c. 32 Sch. 4 para. 133(3)(a)
s. 1048(4A)-(4D) inserted by 2017 c. 32 Sch. 4 para. 133(4)
s. 1094(2A)-(2C) inserted by 2012 c. 14 Sch. 3 para. 13(3)
s. 1126-1126B applied (with modifications) by 2010 c. 8, s. 357BLB(7)(d) (as inserted) by 2016 c. 24 s. 64(3)
s. 1126(7) inserted by 2015 c. 11 s. 28(2)
s. 1126A 1126B inserted by 2015 c. 11 s. 28(3)
s. 1209(3) inserted by 2017 c. 32 Sch. 4 para. 28(3)
s. 1210(5)(ab) inserted by 2017 c. 32 Sch. 4 para. 29(5)
s. 1216A(3)(a) words substituted by 2014 c. 26 s. 33(2)
s. 1216B(1) word inserted by 2014 c. 26 s. 33(3)(a)
s. 1216B(2) words substituted by 2014 c. 26 s. 33(3)(b)
s. 1216B(5) inserted by 2014 c. 26 s. 33(3)(c)
s. 1216AB(2) words substituted by 2015 c. 11 s. 30(2)
s. 1216AB(3) word omitted by 2015 c. 11 s. 30(3)(a)
s. 1216AB(3)(d) and word inserted by 2015 c. 11 s. 30(3)(b)
s. 1216AC(2A) inserted by 2015 c. 11 s. 30(4)
s. 1216AD(1) words inserted by 2015 c. 11 s. 30(5)
s. 1216CE(1) word substituted by 2015 c. 11 s. 31(1)
s. 1216CH(4)(b) words inserted by 2017 c. 32 Sch. 4 para. 140
s. 1216CL(1)(a) modified by 2010 c. 4 s. 357SE (as inserted) by 2015 c. 21 s. 1
s. 1216DA modified by 2010 c. 4 s. 357SF (as inserted) by 2015 c. 21 s. 1
s. 1216DA(2) words inserted by 2017 c. 32 Sch. 4 para. 32(2)(a)
s. 1216DA(2) words substituted by 2017 c. 32 Sch. 4 para. 32(2)(b)
s. 1216DA(3) inserted by 2017 c. 32 Sch. 4 para. 32(3)
s. 1216DB modified by 2010 c. 4 s. 357SG (as inserted) by 2015 c. 21 s. 1
s. 1216DB(2) words inserted by 2017 c. 32 Sch. 4 para. 33(2)
s. 1216DB(3) words substituted by 2017 c. 32 Sch. 4 para. 33(3)
s. 1216DB(5)(ab) inserted by 2017 c. 32 Sch. 4 para. 33(5)
s. 1216DB(5A) inserted by 2017 c. 32 Sch. 4 para. 33(6)
s. 1216DC modified by 2010 c. 4 s. 357SH (as inserted) by 2015 c. 21 s. 1
s. 1216DC(1)(c) words inserted by 2017 c. 32 Sch. 4 para. 34(2)(a)
s. 1216DC(1)(c) words omitted by 2017 c. 32 Sch. 4 para. 34(2)(b)
s. 1216DC(3) words substituted by 2017 c. 32 Sch. 4 para. 34(3)
s. 1216DC(7A) inserted by 2017 c. 32 Sch. 4 para. 34(5)
s. 1216ADA inserted by 2015 c. 11 s. 30(6)
s. 1217B(2) word inserted by 2014 c. 26 s. 34(4)(b)
s. 1217C(2)(c) word substituted by S.I. 2019/689 reg. 16(23)
s. 1217C(2)(c) words substituted by 2014 c. 26 s. 34(6)(a)
s. 1217G(1)(b) word substituted by S.I. 2019/689 reg. 16(27)
s. 1217J words substituted by S.I. 2019/689 reg. 16(29)
s. 1217N word substituted by S.I. 2019/689 reg. 16(30)
s. 1217T word substituted by S.I. 2019/689 reg. 16(36)
s. 1217U word substituted by S.I. 2019/689 reg. 16(38)
s. 1217AE heading word substituted by 2014 c. 26 s. 34(3)(a)
s. 1217AE words substituted by S.I. 2019/689 reg. 16(22)(a)
s. 1217AE(1) substituted by 2014 c. 26 s. 34(3)(b)
s. 1217AE(1) words inserted by S.I. 2019/689 reg. 16(22)(b)
s. 1217AE(2) words substituted by 2014 c. 26 s. 34(3)(c)
s. 1217AE(2) words substituted by S.I. 2019/689 reg. 16(22)(c)
s. 1217CE cross-heading words substituted by 2014 c. 26 s. 34(6)(b)
s. 1217CE heading words substituted by 2014 c. 26 s. 34(6)(c)
s. 1217CE heading words substituted by S.I. 2019/689 reg. 16(24)
s. 1217CE(1) words substituted by 2014 c. 26 s. 34(6)(d)
s. 1217CE(1) words substituted by S.I. 2019/689 reg. 16(24)
s. 1217CF(3A) inserted by 2014 c. 26 s. 34(5)(a)
s. 1217CF(4)(a) words substituted by 2014 c. 26 s. 34(5)(b)
s. 1217CF(5) inserted by 2014 c. 26 s. 34(5)(c)
s. 1217CG words substituted by S.I. 2019/689 reg. 16(25)
s. 1217CG(1)(a) words substituted by 2014 c. 26 s. 34(6)(e)
s. 1217CL(1)(a) modified by 2010 c. 4 s. 357TE (as inserted) by 2015 c. 21 s. 1
S. 1217DA modified by 2010 c. 4 s. 357TF (as inserted) by 2015 c. 21 s. 1
S. 1217DB modified by 2010 c. 4 s. 357TG (as inserted) by 2015 c. 21 s. 1
S. 1217DC modified by 2010 c. 4 s. 357TH (as inserted) by 2015 c. 21 s. 1
s. 1217EB heading words substituted by 2014 c. 26 s. 34(6)(f)
s. 1217EB words substituted by S.I. 2019/689 reg. 16(26)
s. 1217EB(1)(a)(b) words substituted by 2014 c. 26 s. 34(6)(g)
s. 1217EB(3) words substituted by 2014 c. 26 s. 34(6)(g)
s. 1217GB word substituted by S.I. 2019/689 reg. 16(28)(a)
s. 1217GB(2) words inserted by S.I. 2019/689 reg. 16(28)(b)
s. 1217GB(3) word substituted by S.I. 2019/689 reg. 16(28)(c)
s. 1217KA(3)(b) words inserted by 2017 c. 32 Sch. 4 para. 142
S. 1217LB modified by 2010 c. 4 s. 357UE (as inserted) by 2015 c. 21 s. 1
S. 1217MA modified by 2010 c. 4 s. 357UF (as inserted) by 2015 c. 21 s. 1
s. 1217MA(1) words substituted by 2017 c. 32 Sch. 4 para. 40(2)
s. 1217MA(2) words inserted by 2017 c. 32 Sch. 4 para. 40(3)(a)
s. 1217MA(2) words substituted by 2017 c. 32 Sch. 4 para. 40(3)(b)
s. 1217MA(3) inserted by 2017 c. 32 Sch. 4 para. 40(4)
S. 1217MB modified by 2010 c. 4 s. 357UG (as inserted) by 2015 c. 21 s. 1
s. 1217MB(1) words inserted by 2017 c. 32 Sch. 4 para. 41(2)
s. 1217MB(2) words substituted by 2017 c. 32 Sch. 4 para. 41(3)
S. 1217MC modified by 2010 c. 4 s. 357UH (as inserted) by 2015 c. 21 s. 1
s. 1217MC(1)(b) words inserted by 2017 c. 32 Sch. 4 para. 42(2)
s. 1217MC(3) words substituted by 2017 c. 32 Sch. 4 para. 42(3)
s. 1217MC(9) inserted by 2017 c. 32 Sch. 4 para. 42(5)
s. 1217NA word substituted by S.I. 2019/689 reg. 16(31)
s. 1217OB word substituted by S.I. 2019/689 reg. 16(32)
s. 1217RA(2)(d) words substituted by S.I. 2019/689 reg. 16(33)(a)
s. 1217RA(4)(d) words substituted by S.I. 2019/689 reg. 16(33)(b)
s. 1217RB word substituted by S.I. 2019/689 reg. 16(34)(a)
s. 1217RB(2) words inserted by S.I. 2019/689 reg. 16(34)(b)
s. 1217RB(3) word substituted by S.I. 2019/689 reg. 16(34)(c)
s. 1217RE words substituted by S.I. 2019/689 reg. 16(35)
s. 1217RH(3)(b) words inserted by 2017 c. 32 Sch. 4 para. 143
s. 1217SA modified by 2010 c. 4, s. 357UO (as inserted) by 2016 c. 24 Sch. 8 para. 14
s. 1217SA(1) words substituted by 2017 c. 32 Sch. 4 para. 44(2)
s. 1217SA(2) words inserted by 2017 c. 32 Sch. 4 para. 44(3)(a)
s. 1217SA(2) words substituted by 2017 c. 32 Sch. 4 para. 44(3)(b)
s. 1217SA(3) inserted by 2017 c. 32 Sch. 4 para. 44(4)
s. 1217SB modified by 2010 c. 4, s. 357UP (as inserted) by 2016 c. 24 Sch. 8 para. 14
s. 1217SB(1) words inserted by 2017 c. 32 Sch. 4 para. 45(2)
s. 1217SB(2) words substituted by 2017 c. 32 Sch. 4 para. 45(3)
s. 1217SC modified by 2010 c. 4, s. 357UQ (as inserted) by 2016 c. 24 Sch. 8 para. 14
s. 1217SC(1)(b) words inserted by 2017 c. 32 Sch. 4 para. 46(2)
s. 1217SC(3) words substituted by 2017 c. 32 Sch. 4 para. 46(3)
s. 1217SC(9) inserted by 2017 c. 32 Sch. 4 para. 46(5)
s. 1217TA word substituted by S.I. 2019/689 reg. 16(37)
s. 1218ZE word substituted by S.I. 2019/689 reg. 16(42)
s. 1218ZCA(5) word substituted by S.I. 2019/689 reg. 16(39)
s. 1218ZCC word substituted by S.I. 2019/689 reg. 16(40)(a)
s. 1218ZCC(2) words inserted by S.I. 2019/689 reg. 16(40)(b)
s. 1218ZCC(3) word substituted by S.I. 2019/689 reg. 16(40)(c)
s. 1218ZCF words substituted by S.I. 2019/689 reg. 16(41)
s. 1218ZDA modified by 2010 c. 4 s. 357UW (as inserted) by 2017 c. 32 Sch. 6 para. 17
s. 1218ZDB modified by 2010 c. 4 s. 357UX (as inserted) by 2017 c. 32 Sch. 6 para. 17
s. 1218ZDC modified by 2010 c. 4 s. 357UY (as inserted) by 2017 c. 32 Sch. 6 para. 17
s. 1218ZEA word substituted by S.I. 2019/689 reg. 16(43)
s. 1218ZFA word substituted by S.I. 2019/689 reg. 16(44)
s. 1221(3)(ia) inserted by 2015 c. 11 Sch. 5 para. 5
s. 1222(4) inserted by 2016 c. 24 Sch. 1 para. 65(2)(c)
s. 1223(1)(a) words in s. 1223(1) renumbered as s. 1223(1)(a) by 2015 c. 11 Sch. 2 para. 3(a)
s. 1223(1)(b) and word inserted by 2015 c. 11 Sch. 2 para. 3(b)
s. 1223(1)(b) words inserted by 2017 c. 32 Sch. 4 para. 6(2)(b)
s. 1223(1)(b) words inserted by 2017 c. 32 Sch. 4 para. 144
s. 1223(1)(b) words substituted by 2017 c. 32 Sch. 4 para. 6(2)(a)
s. 1223(3A)-(3E) inserted by 2017 c. 32 Sch. 4 para. 6(3)
s. 1227A inserted by 2014 c. 26 Sch. 17 para. 4(4)(b)
s. 1244A and cross-heading inserted by 2015 c. 11 Sch. 5 para. 6
s. 1253A inserted by 2015 c. 11 Sch. 5 para. 7
s. 1258A inserted by 2018 c. 3 Sch. 6 para. 2
s. 1273A inserted by 2014 c. 26 Sch. 17 para. 2
s. 1290(1A) inserted by 2017 c. 32 s. 37(2)
s. 1290(2A)(2B) inserted by 2017 c. 32 s. 37(3)
s. 1290(3A)-(3F) inserted by 2017 c. 32 s. 37(4)
s. 1290(3G)(3H) inserted by 2017 c. 32 s. 37(5)
s. 1292(6B) inserted by 2014 c. 26 Sch. 37 para. 23(1)
s. 1292(6ZA) omitted by 2017 c. 10 s. 12(4)(h)
s. 1293(5A) omitted by 2017 c. 10 s. 12(4)(h)
s. 1305A inserted by 2014 c. 26 s. 30(1)
s. 1310(4)(zzza) inserted by 2015 c. 33 s. 31(4)
s. 1310(4)(ek)-(em) inserted by 2014 c. 26 Sch. 4 para. 12
s. 1310(4)(en)(eo) inserted by 2016 c. 24 Sch. 8 para. 10
s. 1310(4)(ep)-(er) inserted by 2017 c. 32 Sch. 6 para. 13
s. 1310(4)(zb) inserted by 2015 c. 11 s. 28(6)
Chapter 6U.K.Trade profits: receipts
Capital receiptsU.K.
93Capital receiptsU.K.
(1)Items of a capital nature must not be brought into account as receipts in calculating the profits of a trade.
(2)But this does not apply to items which, as a result of any provision of the Corporation Tax Acts, are brought into account as receipts in calculating the profits of the trade.
Debts releasedU.K.
94Debts incurred and later releasedU.K.
(1)This section applies if—
(a)in calculating the profits of a trade, a deduction is allowed for the expense giving rise to a debt owed by the company carrying on the trade,
(b)all or part of the debt is released, and
(c)the release is not part of a statutory insolvency arrangement.
(2)The amount released—
(a)is brought into account as a receipt in calculating the profits of the trade, and
(b)is treated as arising in the accounting period in which the release is effected.
Amounts received following earlier cessationU.K.
95Acquisition of trade: receipts from transferor's tradeU.K.
(1)This section applies if —
(a)a person ("the transferor") permanently ceased to carry on a trade at any time,
(b)at that time the transferor transferred to another person ("the transferee") the right to receive sums arising from the carrying on of the trade, and
(c)the transferee subsequently carries on the transferor's trade.
(2)Sums—
(a)which the transferee receives as a result of the transfer, and
(b)which are not brought into account in calculating the profits of the transferor's trade for corporation or income tax purposes of any period before the cessation,
are brought into account in calculating the profits of the transferee's trade in the accounting period in which they are received.
(3)Any sums mentioned in subsection (1)(b) which are received after the transferor has permanently ceased to carry on the trade are not post-cessation receipts (see Chapter 15).
Reverse premiumsU.K.
96Reverse premiumsU.K.
(1)For the purposes of sections 98 and 99 a payment or other benefit is a reverse premium if—
(a)conditions A, B and C are met, and
(b)it is not excluded by section 97.
(2)Condition A is that a company ("the recipient") receives the payment or other benefit by way of inducement in connection with a transaction being entered into by—
(a)the recipient, or
(b)a person connected with the recipient.
(3)Condition B is that the transaction (the "property transaction") is one under which—
(b)the person connected with the recipient,
becomes entitled to an estate, interest or right in or over land.
(4)Condition C is that the payment or other benefit is paid or provided by—
(a)the person ("the grantor") by whom the estate, interest or right is granted or was granted at an earlier time,
(b)a person connected with the grantor, or
(c)a nominee of, or a person acting on the directions of, the grantor or a person connected with the grantor.
97Excluded casesU.K.
(1)A payment or other benefit is not a reverse premium so far as it is brought into account under section 532 of CAA 2001 (the general rule excluding contributions) to reduce the recipient's expenditure qualifying for capital allowances.
(2)A payment or other benefit received in connection with a property transaction is not a reverse premium if—
(a)the person entering into the transaction is an individual, and
(b)the transaction relates to premises occupied or to be occupied by the individual as the individual's only or main residence.
(3)A payment or other benefit is not a reverse premium so far as it is consideration for the transfer of an estate or interest in land which constitutes the sale in a sale and leaseback arrangement.
(4)A "sale and leaseback arrangement" means any such arrangement as is described in [F1section 681AA(1) or (2) or 681AB(1) or (2) of ITA 2007 or] [F2section 835(1) or (2), 836(1) or (2) or 850 of CTA 2010].
Textual Amendments
F1Words in s. 97(4) inserted (with effect in accordance with s. 381(1) of the amending Act) by Taxation (International and Other Provisions) Act 2010 (c. 8), s. 381(1), Sch. 8 para. 263 (with Sch. 9 paras. 1-9, 22)
F2Words in s. 97(4) substituted (with effect in accordance with s. 1184(1) of the amending Act) by Corporation Tax Act 2010 (c. 4), s. 1184(1), Sch. 1 para. 596 (with Sch. 2)
98Tax treatment of reverse premiumsU.K.
(1)A reverse premium is treated for corporation tax purposes as a receipt of a revenue nature.
(2)If the recipient enters into the property transaction for the purposes of a trade carried on (or to be carried on) by the recipient, the reverse premium is brought into account in calculating the profits of the trade.
(3)If subsection (2) does not apply, the reverse premium is charged to corporation tax in accordance with section 250 (reverse premium taxed as property business receipt).
99Arrangements not at arm's lengthU.K.
(a)two or more of the parties to the property arrangements are connected persons, and
(b)the terms of those arrangements are not such as would reasonably have been expected if those persons had been dealing at arm's length.
(2)The terms of the property arrangements meet the condition in subsection (1)(b) if they differ to a significant extent from the terms which, at the time the arrangements were entered into, would be regarded as normal and reasonable—
(a)in the market conditions then prevailing, and
(b)between persons dealing with each other at arm's length in the open market.
(3)The whole amount or value of the reverse premium brought into account under section 98 is brought into account in the first relevant period of account.
(4)"The first relevant period of account" means the period of account in which the property transaction is entered into.
(5)However if the recipient enters into the property transaction for the purposes of a trade—
(a)which is not then carried on by the recipient, but
(b)which the recipient subsequently starts to carry on,
"the first relevant period of account" means the first period of account in which the recipient carries on the trade.
100Connected persons and property arrangementsU.K.
For the purposes of this section and sections 96 to 99—
(a)persons are treated as connected with each other if they are connected at any time during the period when the property arrangements are entered into, and
(b)"the property arrangements" means the property transaction and any arrangements entered into in connection with it (whether before it, at the same time as it or after it).
Other receiptsU.K.
101Distribution of assets of mutual concernsU.K.
(a)a deduction has been made in calculating the profits of a trade for a payment to a mutual concern for the purposes of its mutual business,
(b)the concern is being or has been wound up or dissolved,
(c)a company ("the recipient") which is carrying on the trade, or was doing so at the time of the payment, receives money or money's worth representing the concern's assets, and
(d)the assets in question represent profits of the mutual business conducted by the concern.
(2)If the recipient is carrying on the trade at the time the money or money's worth is received, the amount or value of the money or money's worth is brought into account as a receipt in calculating the profits of the trade.
(3)If the recipient—
(a)is not carrying on the trade at the time the money or money's worth is received, but
(b)was doing so at the time of the payment to the mutual concern,
the amount or value of the money or money's worth is treated as a post-cessation receipt (see Chapter 15).
(4)For the purposes of this section money or money's worth represents assets of a mutual concern if it—
(a)forms part of the assets of the concern,
(b)forms part of the consideration for the transfer of the assets of the concern as part of a scheme of amalgamation or reconstruction which involves its winding up, or
(c)consists of the consideration for a transfer or surrender of a right to receive anything falling within paragraph (a) or (b) and does not give rise to a charge to corporation tax on the company receiving it otherwise than as a result of this section.
(5)If a transfer or surrender of a right to receive anything which—
(a)forms part of the assets of a mutual concern, or
(b)forms part of the consideration for the transfer of the assets of a mutual concern,
is not at arm's length, the company making the transfer or surrender is treated as receiving consideration equal to the value of the right.
(6)In this section references to a mutual concern are to a body corporate which has at any time carried on a trade which consists of or includes the conduct of mutual business (whether or not confined to the members of the body corporate).
(7)For the purposes of this section a trade does not consist of or include the conduct of mutual business if all the profits of the trade are chargeable to corporation or income tax.
102Industrial development grantsU.K.
(1)This section applies if a company carrying on a trade receives a payment by way of a grant under—
(a)section 7 or 8 of the Industrial Development Act 1982 (c. 52), or
(b)Article 7, 9 or 30 of the Industrial Development (Northern Ireland) Order 1982 (S.I. 1982/1083 (N.I. 15)).
(2)The payment is brought into account as a receipt in calculating the profits of the trade unless—
(a)the grant is designated as made towards the cost of specified capital expenditure,
(b)the grant is designated as compensation for the loss of capital assets, or
(c)the grant is for all or part of a corporation tax liability (including one that has already been met).
103Sums recovered under insurance policies etcU.K.
(a)a deduction has been made for a loss or expense in calculating the profits of a trade,
(b)a company carrying on the trade recovers a sum under an insurance policy or a contract of indemnity in respect of the loss or expense, and
(c)the sum is not of a revenue nature.
(2)The sum is brought into account as a receipt in calculating the profits of the trade (but only up to the amount of the deduction).
104Repayments under FISMA 2000U.K.
(a)a company carries on a trade, and
(b)a payment is made to the company as a result of a repayment provision.
(2)The payment is brought into account as a receipt in calculating the profits of the trade.
(3)For the purposes of this section "repayment provision" means—
(a)any provision made by virtue of section 136(7) or 214(1)(e) of FISMA 2000, or
(b)any provision made by scheme rules for fees to be refunded in specified circumstances.
(4)In this section "scheme rules" means the rules referred to in paragraph 14(1) of Schedule 17 to FISMA 2000.
PrintThis Chapter only
PDF This Chapter only
Web page This Chapter only
You have chosen to open The Whole Part
The Whole Part you have selected contains over 200 provisions and might take some time to download. You may also experience some issues with your browser, such as an alert box that a script is taking a long time to run.
You have chosen to open The Whole Part as a PDF
The Whole Part you have selected contains over 200 provisions and might take some time to download.


text:
Eid al-Fitr: End of Ramadan fast a time to reflect on less fortunate throughout the Muslim and non-Muslim world
By Mohammed Kozbar
July 17, 2015 11:49 BST
Eid al-Fitr, the Islamic festival marking the end of Ramadan, begins with the sighting of the new moon and is celebrated by more than 1.6 billion Muslims around the globe.
Eid is a time when Muslims give thanks and glorify God for giving us strength and the ability to fast during the month of Ramadan. This year in particular as the fasting hours of about 18 hours were the longest for many years.
It is also a day for the family where loved ones, friends and neighbours exchange greetings and gifts as well as visit one another.
Despite Eid being a sacred Muslim holiday, participation in the celebration is enjoyed by Muslims and non-Muslims alike
- Mohammed Kozbar
This Eid comes at a very challenging time for British Muslims. Domestically a small fringe of extremists among us misuse our peaceful religion for their warped agenda. Another minority of extremists, the far right, take every opportunity to demonise Muslims, create a climate of fear and Islamophobia with a view to creating tensions in our multicultural society.
Another challenge that has befallen us is our government's controversial Counter-Terrorism Strategy (CTS), which without a doubt has a huge impact on the Muslim community and other minorities.
Muslims feel increasingly criminalised, seen as a suspect community and now with the adoption of the CTS we feel the freedom and human rights this nation are so proud of are being chipped away. It would not be a surprised if more British Muslims feel under siege. This is the very situation the extremists within us desire so they can exploit Muslim frustrations and grievances.
British Muslims are also concerned about what is going on in the Muslim world, especially in Syria, Iraq, Palestine, Burma, Egypt, Libya and Yemen. While some may dismiss a connection between foreign policy and life at home, it is sadly a reality. Foreign interference by some Western powers has made things worse which in effect impact on Muslims in the UK – the young in particular.
It is no surprise therefore to see that a small minority of young British men and women have decided to join and fight alongside the extremists abroad, in recent times the so-called Islamic State, better termed as Da'ish.
At the family level, this Eid, like most Eids, you see a flurry of SMS, emails and WhatsApp messages wishing one another Eid greetings. I would not be exaggerating to say I receive 100 such messages every Eid from friends, colleagues and families – not all Muslim.
This time I have decided to take my family and celebrate Eid in the open – especially performing the morning Eid prayers in a park near where I live alongside many more locals. What amazes me is the diversity of people converging in one place to perform the Eid prayer – speaking different languages and wearing different attire. What unites us all is our faith, all converging and praying to one God, Allah – facing the direction of the Qibla in Makkah.
More about Eid al-Fitr
Eid al-Fitr and Boko Haram: Terrorism and security stop Muslims from celebrating end of Ramadan
Eid al-Fitr 2015: Foods to celebrate the breaking of the fast
Eid al-Fitr: Best apps to help you celebrate the end of Ramadan
Eid al-Fitr moon sighting: Watch the crescent moon of Shawwal livestream online [Video]
Eid al-Fitr 2015: Zayn Malik and other Muslim celebrities who will mark the end of Ramadan
After the prayer, we thank each other, greet each other, exchange gifts, visit one another's houses for food and drink but above all thank Allah for the blessings of Ramadan and now Eid. It is also an opportunity to meet new people and make new friends.
Despite Eid being a sacred Muslim holiday, participation in the celebration is enjoyed by Muslims and non-Muslims alike. Here at the Finsbury Park Mosque in north London, our facilities and services are open to all. Anyone passing the mosque will be greeted and welcomed to join in the celebration, for Eid is truly a community festival in the broadest sense.
To me Eid means more than just being able to spend time with the family. Eid and Ramadan have a joint significance: I take Eid as a time to reflect on how Ramadan has helped me to strengthen my faith, myself and my character as a whole and to think about those who have not got the chance to celebrate Eid for different reasons, especially those stricken by poverty, natural disasters or conflicts.
This is why Eid is a chance to multiply good deeds by bringing happiness and pleasure to the hearts of others, by helping and supporting the poor and needy, and by getting involved in pastimes that emphasise the strong and serious Islamic character.
Muhammad, our prophet and messenger of God said: "He who believes in Allah and the Last Day, let him be kind to his neighbour." This is why my wife gets busy to prepare the traditional cake and sweets to distribute it to our neighbours and friends.
Feeling the satisfaction of fasting for a whole month of Ramadan and then thanking God, for helping me to get through it with ease really makes me feel closer to my Lord. I wish each and every one a blessed Eid today.


The Judaica Collection's many digital materials document the life and culture of the Jewish people, with particular focus on life and culture in Israel.
Zvulun Hammer, the education minister of Israel, visits the Israel Broadcasting Authority, 1991. View Details.
Judaica digital resources are available in a variety of formats.
Some 11,400 books and pamphlets in the public domain from the Judaica Collection (chiefly in Hebrew, Yiddish, German and Russian) have been digitized.
The single largest component of the digitized Judaica Ephemera Collection — some 250,000 items — consists of posters and broadsides published in Israel over the past 100 years. They document politics, theater, music, dance, art, religion, and commerce.
In addition, there are large collections of ephemera from the United States, Latin America, and Europe — both current and retrospective — chiefly in the areas of religious life, and political and cultural activities.
Map of Tel Aviv's growth (1924) from the Central Zionist Archive. View Details.
Harvard boasts a collection of 117,000 digital maps of Israel, including maps of cities, towns and regions as well as design plans focusing on specific topics.
Some 2,000 hours of Israeli radio news broadcasts from Kol Yisra'el (Israel Broadcasting Authority) are available online.
With some 5.5 million photographs available, the Judaica Division Digital Photograph Collection offers insight into virtually all facets of Jewish life in Israel.
Scene from the Cameri Theater production of "Family Story," photographed by Israel Haramati, 1997. View Details.
A collection of digital materials documenting the Harvard Judaica Collection, including publications and publicity materials, as well as photographs.
All the Judaica Digital Collection materials are cataloged and searchable in HOLLIS. Photographs and ephemera can also be searched through HOLLIS Images.
Materials in the public domain are freely available to all. Materials under copyright can be accessed by Harvard affiliates using their HarvardKey. For information about publishing any of these materials, please contact the Judaica Division.
Documents the life and culture of the Jewish people, with particular comprehensive coverage of life and culture in the State of Israel.


text:
7th CPC – Revision of pension of pre-1.1.2016 Defence Forces pensioners
September 6, 2017 by rajasinghmurugesan
No.17(01)/2017(01)/D(Pension/Policy)
Department of Ex-Servicemen Welfare
New Delhi, Dated 4th September, 2017
The Chief of the Army Staff
The Chief of the Naval Staff
The Chief of the Air Staff
Subject – Implementation of Government's decision on the recommendations of the 7th Central Pay Commission (CPC) – Revision of pension of pre-1.1.2016 Defence Forces pensioners/ family pensioners etc.
The undersigned is directed to refer to this Ministry's letter No. 17(01)/2016 D(Pen/Pol) dated 29th October 2016 for revision of pension of pre-2016 Defence Forces pensioners / family pensioners in implementation of the Government decisions on the recommendations of the 7th CPC. As per para 9 of this Ministry's said order dated 29th October 2016 the revision of disability element of disability pension was held in abeyance pending decision of National Anomaly Committee to whom matter was referred by MOD to decide methodology for calculation of disability element of disability pension under 7thCPC. The National Anomaly Committee has recommended that parity with Civilians for grant of Disability element which was granted to Defence Forces under 6th CPC, shall be maintained
2.The recommendations of the National Anomaly Committee have been considered by the Government. In partial modification of Ministry's order dated 29th October 2016, the President is now pleased to decide that Disability element of disability pension for Defence Forces Pensioners shall also be revised by multiplying the existing rate of disability element as had been drawn on 31.12.2015 by factor of 2.57 to arrive at revised rate of disability element as on 1.1.2016. The amount of revised disability element so arrived shall be rounded off to next higher rupee.
3.Para 13 of this Ministry's above quoted letter dated 29.10.2016 regarding "Ex-gratia awards to Cadets in cases of disablement" shall be replaced with the following:
EX-GRATIA AWARDS TO CADET (DIRECT) The ex-gratia award payable to Cadet (Direct)/ NoKs in cases of disablement / death shall be payable subject to the same conditions as hitherto in force in the event of invalidment on medical ground / death of a Cadet (Direct) due to causes attributable to or aggravated by military training :
(i) Monthly Ex-gratia amount of Rs 9,000/- per month
(ii) In cases of disablement, Ex-gratia disability award @ Rs 16,200/- per month shall be payable in addition for 100% of disability during period of disablement subject to prorata reduction in case the degree of disablement is less than 100%. "No ex-gratia disability award shall be payable in cases where the degree of disablement is less than 20%."
4.The dearness relief sanctioned by the Government from 1.1,2016 and thereafter, shall also be paid on rates of disability element and monthly ex-gratia award to Cadet(Direct), revised in accordance with the provision of this letter.
5. Vide para 10(ii) of MoD order dated 29.10.2016, it was ordered to pay the Constant Attendance Allowance(CM) at the existing rate since matter regarding grant of Allowances was under examination by the Committee on Allowances (CoA). In this regard, Ministry of Finance vide Resolution dated 6th July 2017 (Appendix II item 37 has accepted the recommendation of 7th CPC to enhance the existing Constant Attendance Allowance @ 4500/ p.m. by 50%. DoP&PW vide O.M No. 1/4/2017-P&PW(F) dated 2.8.2017 has issued orders in this regard for civilian pensioners. Accordingly, for Armed Forces personnel the Constant Attendant Allowance shall continue to be admissible under the condition as hitherto fore at the existing rate from 1.1.2016 to 30.06.2017. However, it shall now be admissible at the enhanced uniform rate of Rs. 6750/- per month, irrespective of the rank with effect from 1.7.2017.
6. With reference to the provisions contained in Para 5.4 of this Ministry's letter dated 29th October, 2016, it is further clarified that the maximum ceiling shall be applicable only in the case of Service/Retiring Pension, Service element of Disability/ liberalized disability Mar Injury Pension and Ordinary family Pension. The said ceiling is not applicable in the cases of Disability/ Liberalised Disability/ War Injury element. Special Family/ Liberalized Family Pension etc. applicable under casualty pensionary awards.
7.The provisions of this Ministry's letter dated 29th October 2016, which are not affected by the provisions of this letter, shall remain unchanged.
8.The provisions of this letter shall take effect from 1.1.2016
9.This issues with the concurrence of Finance Division of this Ministry their U.O. No. Part file (1) to (30)(01)12016/Fin/Pen dated 14th August 2017.
10.Hindi version will follow.
S/d,
(Manoj Sinha)
Under Secretary to the Government of India
Filed Under: 7CPC, CGE LATEST NEWS, DEFENCE, PENSION


text:
12 Rounds: Reloaded
List Price 5.49
Genres: Action
Starring: Sean Rogerson, Randy Orton, Cindy Busby
Director: Roel Reiné
Plot Synopsis: Randy Orton portrays an Emergency Medical Technician (EMT) who finds himself caught in a deadly 12-round game of cat and mouse with a vigilante tied to the paramedic's past. With little time to spare and his wife's life hanging in the balance, the EMT must figure out why he's been chosen to be the pawn in this maniac's game before it's too late.
Release Date: June 4th, 2013
Movie Studio: 20th Century Fox
Length:0 Minutes
Specs:Blu-ray/DVD Combo Pack
Audio Formats:English DTS-HD Master Audio 5.1
Subtitles/Captions:English, Spanish, French
Special Features:Audio Commentary
Randy Orton Reloaded
The Action of 12 Rounds 2: Reloaded
Locations: From Heller's Lair to the Sugar Factory