text:
\section{Activation energies}

\begin{figure}[b]
\includegraphics[width=\columnwidth]{TseriesPRB.png}
\caption{Temperature dependent measurements of the thermal dynamics of uncoupled mesospins. ({\bf a}), Fractions of identifiable magnetic islands during a PEEM-XMCD measurement of 300~s and their corresponding fits. Both island types have a width of 150~nm, while the short islands have a length of 450~nm and the long of 1110~nm. Examples of the PEEM-XMCD images for the short ({\bf b}) and long islands ({\bf c}) are presented for the measurement at 135~K.}
\label{activ}
\end{figure}

\noindent To determine the activation energies or the ratio between the activation energies for short- and long-mesospins, we fabricated arrays of short- and long-mesospins with an edge to edge distance of 1000~nm. For these islands this distance is large enough to consider the islands to be non-interacting.

The fractions of identifiable islands for short (red) and long islands (blue) can be fitted with a double exponential of the following form:
\begin{table*}[h!]
	\centering
		\begin{tabular}{ll}
			\parbox{200px}{\begin{equation}
											P(T) = exp\left(-\dfrac{A}{exp\left(\dfrac{B}{T}\right)}\right)\hspace{20px}\label{eq:fit}
											\end{equation}}& \vspace{-80px}\\
			 & \parbox{200px}{\begin{equation}
													A = \dfrac{t_s}{\tau_0} = \dfrac{300~\rm{s}}{\tau_0}\hspace{20px}\label{eq:A}
												\end{equation}}\vspace{-10px}\\
			 & \parbox{200px}{\begin{equation}
													B = \dfrac{E}{k_B}\hspace{58px}\label{eq:B}
												\end{equation}}
		\end{tabular}
\end{table*}

\vspace{-20px}\noindent Equation \eqref{eq:fit} represents the probability of a magnetic element not having altered its magnetization direction after a time period $t_s$\cite{Wernsdorfer1997PRL}, $T$ is the temperature and $A$, $B$ are fitting parameters.
The measurement time for the PEEM-XMCD imaging was $t_s = 300$~s. In equation \eqref{eq:A}, $\tau_0$ is the inverse attempt frequency\cite{Kapaklis2014NatNano,Bedanta2009}, while in equation \eqref{eq:B}, $E$ is the activation energy and $k_B$ is Boltzmann's constant. The ratio of the activation energies for short ($E_{short}/k_B = 560(40)$~K) and long islands ($E_{long}/k_B = 1140(140)$~K) can be determined from the fits shown in Suppl. Fig. \ref{activ}({\bf a}), and is 0.49(4).
\section{Real Space Images}
Real space images of the SH and mSH lattices that are created by stitching together individual images (each recorded for 360~s) recorded in the limited field of view of the microscope. The composite images shown in Fig.~\ref{PEEM}({\bf a}) for the SH and Fig.~\ref{PEEM}({\bf b}) for the mSH lattices represent the raw data from which the vertex statistics and spin structure factors were calculated. The individual islands can be seen as either black/white/gray depending on whether the islands are aligned parallel/anti-parallel/reversing with respect to the x-ray propagation direction. The particular composite images shown in Fig.~\ref{PEEM} were recorded at 65~K.
\begin{figure}[h!]
\includegraphics[width=\columnwidth]{sup1PRB.png}
\caption{PEEM-XMCD measurements of the Shakti lattices. Composite PEEM-XMCD images of the SH ({\bf a}) and mSH ({\bf b}) lattices.}
\label{PEEM}
\end{figure}

\newpage
\section{Spin arrangements}

\begin{figure}[b]
\includegraphics[width=0.97\columnwidth]{Shakticorrelations3PRB.pdf}
\caption{Spin arrangement arround the long-mesospin (Type-I$_2$). ({\bf a}), Illustration of the five (six in mSH) islands which are considered in the spin arrangements. Adjacent islands are indicated by light red and in the different representation of the spin arragements C$_1$-C$_9$ with light green if correlated over the long-mesospin (Type-I$_2$). ({\bf b}), Abundance of the different spin arrangements, for the SH (dark-blue -- squares) and mSH (dark-red -- circles) lattices.}
\label{Shakticorrelation}
\end{figure}

All nine possible spin arrangements $\rm{C}_1-\rm{C}_9$, for the short- and long-mesospins (depending on the lattice) of two neighboring three-fold coordinated vertices are depicted in Fig. \ref{Shakticorrelation}({\bf a}). The abundance of the spin arrangements is presented in Fig. \ref{Shakticorrelation}({\bf b}). These spin arrangements can be categorized into three groups marked with orange, yellow and green. Group one (orange~--~A$_1$), are arrangements $\rm{C}_1-\rm{C}_4$ connecting one mesospin, and the respective vertex, with another mesospin on the other side of the long-mesospin (two short-mesospins). The second group (yellow~--~A$_2$), are arrangements $\rm{C}_5-\rm{C}_8$ in which one mesospin on one side is in ferromagnetic alignment with the long-mesospin (two short-mesospins) and two mesospins on the other side. Finally, the last arrangement (green), $\rm{C}_9$, is the lowest energy state for this sub-set of mesospins.

Roughly 53\% of all investigated long-mesospin connections of the SH have at least two vertices being correlated to each other ($\rm{C}_1-\rm{C}_4$), but only 32\% of them are correlated in the mSH via the two short-islands. Similar differences in the correlations can also be found for the other spin arrangements ($\rm{C}_5-\rm{C}_9$). This can be attributed to the high abundance (34\%) of Type-II$_2$ excitations in vertices with coordination number two, which are therefore unable to mimic the SH order.

\section{Type-I$_4$-tiling}
\begin{figure}[h]\vspace{-10px}
\includegraphics[width=\columnwidth]{sup2_2PRB.pdf}
\caption{Shakti ground state manifold in plaquettes. ({\bf a}), Illustration of the Shakti ground state manifold in a plaquette as introduced by Chern {\it et al.}\cite{Chern2013PRL}. In the Shakti ground state all four-fold coordinated vertices are in their lowest energy state, Type-I$_4$, and 50\% of the three-fold coordinated vertices are in their lowest energy state, Type-I$_3$, and 50\% are in the excited state, Type-II$_3$. These excitations are represented with a circle in the plaquette illustration by Chern {\it et al.}. ({\bf b}), Equivalent representation of the Shakti ground state manifold for a plaquette, focusing on the Type-I$_4$ tiling at the four-fold coordinated vertices. All Type-I$_4$ tilings for a pre-defined long-mesospin direction are illustrated for one ({\bf c}) and two  plaquettes ({\bf d}).}
\label{sup3}
\end{figure}
The ground state manifold of the Shakti lattice was described by Chern {\it et al.}\cite{Chern2013PRL} and is best explained on the size of a plaquette. In Fig.~\ref{sup3}({\bf a}) the extent of a plaquette is illustrated, consisting of 9 islands in the SH and 10 islands in the mSH case.
A Shakti plaquette has one long island (or a two-fold coordinated vertex in the mSH) in its center and 8 short islands at its borders, sharing 4 three-fold coordinated vertices and 4 four-fold coordinated vertices with the neighbouring plaquettes.
Fig.~\ref{sup3}({\bf a}) also shows the representation of the Shakti ground state manifold of such a plaquette as introduced by Chern {\it et al.}\cite{Chern2013PRL}. Solid lines illustrate the lowest energy states, but the circles at the three-fold coordinated vertices mark the position of Type-II$_3$ excitations. In the Shakti ground state a plaquette inhabits two of such Type-II$_3$ excitations, at any of their 4 three-fold coordinated vertices. At the same time all the four-fold coordinated vertices are in their lowest energy state, Type-I$_4$. Therefore we represent the tiling of the two degenerated Type-I$_4$(A) and Type-I$_4$(B) vertices on the bases of a plaquette in Fig~\ref{sup3}({\bf b}).

The excitations in the Shakti lattice are located at the boundaries between Type-I$_4$(A) and Type-I$_4$(B) vertices. We discussed in the main text, that the pre-defined long-mesospins in the SH lattice will restrict the possible Type-I$_4$-tilings. This effect is illustrated in Fig.~\ref{sup3}({\bf c})-({\bf d}) for one and two plaquettes. All 7 (out of 16) Type-I$_4$-tilings accessible, by simultaneously remaining in the Shakti ground state manifold, regarding the given long-mesospin direction are illustrated in Fig.~\ref{sup3}({\bf c}). For two pre-defined long-mesospins (two neighbouring plaquettes -- Fig.~\ref{sup3}({\bf d}) ) just 12 (out of 64) Type-I$_4$-tilings remain in the Shakti ground state manifold.

\bibliographystyle{natphys}

\section{Introduction}

Initially introduced as a playground for the experimental investigation of magnetic frustration effects\cite{Wang2006Nat}, the area of artificial spin ices  has evolved into a vibrant field of research. Using designed structures, collective order and dynamics can be controlled and directly visualized by using, for example, nano-characterization techniques\cite{Nisoli2013RevModPhys}. This approach has motivated experimental investigations of celebrated classical spin models\cite{Syozi_1951,Lieb1967PRL,Lieb1967PhysRev}, some of which display non-conventional and exotic magnetic phases\cite{Zhang2013Nat,Canals_NatComm_2016,Perrin_Nature_2016, Nisoli_NatPhys_2017,Erik_ArXiV_2017}. Furthermore, given the large freedom in design, new topologies that promote non-conventional emergent order can be manufactured and investigated in thermally-active artificial spin ice structures, allowing the study of their complex energetic manifolds in a superparamagnetic regime \cite{Morgan2010NatPhys,Arnalds2012APL, Farhan2013NatPhys, Farhan2013PRL,Kapaklis2012NJP, Kapaklis2014NatNano, mSH_NatPhys_2018}. A variety of new artificial spin ice systems have been proposed by Morrison \textit{et al.}\cite{Morrison2013NJP}, with particular attention given to the so-called Shakti lattice, a variation of the square ice geometry.  In this lattice, 25\% of the square ice lattice elements have been removed and certain pairs of islands merged as depicted in Fig.~\ref{fig1}.
Theoretical and numerical studies have predicted an emergent magnetic order in the Shakti geometry\cite{Chern2013PRL} which retrieves the features of the six-vertex model\cite{Lieb1967PRL} on a larger length-scale. This behavior has been demonstrated experimentally by Gilbert \textit{et al.}\cite{Gilbert2014NatPhys} for the Shakti lattice (SH), as well as for a modified Shakti lattice (mSH).

Given the mesoscopic nature of the structures, different activation energies are expected for the long (T$_{\rm{B1}}$) and short islands (T$_{\rm{B2}}$), resulting in two blocking temperatures of the elements (T$_{\rm{B2}} < T_{\rm{B1}}$). The presence of two activation energies is therefore expected to influence the eventual magnetic correlations and order in the lattice, since the larger elements could act as a source of quenched disorder. Such disorder would hinder the development of any medium- or long-range magnetic order of the smaller islands, as these become arrested at lower temperatures (T$_{\rm{B2}}$). Whilst the vertex statistics for both the Shakti lattices have been experimentally investigated for a range of inter-island coupling strengths\cite{Gilbert2014NatPhys}, the thermally driven kinetics in the modified Shakti lattice were only recently reported\cite{mSH_NatPhys_2018}. Consequently, the impact of the hierarchy of the activation energies on the emergent order has not been addressed to date. In this work, we undertake this task for the particular case of the Shakti and the modified Shakti geometries. Using thermally-active elements, we characterize and compare their final magnetic configurations using identical experimental protocols, highlighting the impact of different activation energies on the obtained magnetic correlations and order.

\section{Experimental details}

\subsection{Sample preparation}

\begin{figure*}[t!]
	\includegraphics[width=\textwidth]{Shakticooling-2.png}
	\caption{A schematic representation of the Shakti (SH) and modified-Shakti (mSH) lattices along with magnetic states representative of each temperature regime, generally defined by the Curie (T$_{\rm{c}}$) and the blocking temperatures (T$_{\rm{B1/B2}}$). Elements in their paramagnetic state are gray, superparamagnetic elements are light-blue and the frozen elements are represented with a magnetic north (blue) and south (red) pole, reflecting their final magnetic orientation. The gray-scale images to the left are representative PEEM-XMCD snapshots obtained at 65~K, the lowest temperature reached during the cooling.}
	\label{fig1}
\end{figure*}

The samples were produced by a post-growth patterning process, applied to a thin film of $\delta$-doped Palladium (Iron) as described in P\"arnaste \textit{et al.}\cite{Parnaste2007}.  A thick bottom layer of Pd (40~nm) is followed by 2.0 mono layers of Fe, defining the nominal Curie-temperature, T$_{\rm{C}}=400$~K\cite{Parnaste2007}, as well as the thermally active temperature range for the $\delta$-doped Pd(Fe). The post-patterning was carried out at the Center for Functional Nanomaterials (CFN), Brookhaven National Laboratory in Upton, New York. A positive high resolution e-Beam resist (ZEP520A) was employed to create a Chromium mask of the nano-structures using e-Beam lithography. The magnetic structures were formed by Argon milling. All investigated structures were produced on the same substrate from the same layer, ensuring identical intrinsic material properties as well as the same thermal history for all the investigated structures. Each array had a spatial dimension of 200 $\times$ 200~$\mu$m$^2$. The lengths of the large and small islands, were chosen to be 1050~nm and 450~nm, respectively, while the width was kept at 150~nm. The lattice spacing between two parallel neighboring short islands was set to 600~nm.

\subsection{Thermal protocol}

Similar to previous studies\cite{Kapaklis2012NJP,Kapaklis2014NatNano}, the thermal protocol involves a gradual cooling from a superparamagnetic state of the elements, towards a completely arrested state at the lowest temperatures. This process is schematically represented in Fig.~\ref{fig1} for both the Shakti and the modified Shakti lattices. Notice the two distinctive stages of the superparamagnetic regime for the Shakti lattice because to the presence of elements with different intrinsic activation energies.

When the temperature is lowered below the Curie temperature (T$_{\rm{c}}$),  the elements become magnetic and can be considered as mesospins. The stray field of these islands is resulting in a temperature-dependent magnetostatic coupling. The coupling between the elements has a direct impact on the involved activation energies, biasing the otherwise equally-favoured two magnetic states of the islands. On the lattice scale, this effectively results in a dynamic distribution of blocking temperatures around the intrinsic energy barriers, a distribution whose width depends on the strength of the inter-island interactions.

\subsection{Interaction strength and their impact}

There are three special cases to be considered: the strong, intermediate and weak coupling limits. In the strong coupling limit, the intrinsic activation energy of the mesospins is much smaller than the inter-island interactions. Consequently, the emergent order will not depend on the differences in the activation energies, but significant effects on the dynamic response cannot be ruled out. In the intermediate coupling limit, the strength of the inter-island couplings is comparable to the intrinsic activation energy of the mesospins. This will give rise to a complex interplay, in which the relation between the activation and interaction energies will dictate both the order and dynamics of the magnetic phases. The individual activation energies depend on the dynamically developing magnetic configurations, for both long- and short-mesospins. In other words, these couplings can yield a strong overlap in the two blocking temperature distributions of the short and long islands. Therefore, the configurations of the long- and the short-mesospins will exhibit different degrees of order, all depending on the relation of the activation and interaction energies.
Conversely in the weak coupling limit, the intrinsic activation energies of the long-mesospins are much larger than the inter-island interactions. Around the intrinsic blocking temperature of the long islands (T$_{\rm{B1}}$), the available thermal energy is higher than the energy difference given by any magnetization reversal of the short islands.
Therefore the lattice as a whole will be in a disordered state when the long-mesospins freeze (T$_{\rm{B1}}$)  and consequently the magnetic orientation of the long elements will be randomly distributed, with no short- or long-range correlations. However, at the blocking temperature for the short-mesospins (T$_{\rm{B2}}$) the inter-island coupling strength can be comparable to their intrinsic activation energies, potentially resulting in a short-range order below T$_{\rm{B2}}$. Thus, having two distinct activation energies is expected to have a significant impact on the emergent order, for both the intermediate and the weak coupling limits. By the same token, the presence of two or more activation energies is expected to have a marginal impact in the strong coupling limit. Here, we focus on the weak coupling limit and, as previously stated, we compare the obtained magnetic order in SH  and mSH lattices, ascertaining the impact of the hierarchical relation of inter-element interactions and the activation energies involved.

\subsection{Determination of the magnetization direction}

The magnetic states were determined as a function of temperature using Photo Emission Electron Microscopy (PEEM) capturing the X-ray Magnetic Circular Dichroism (XMCD) contrast. The experimental studies were performed at the 11.0.1 PEEM3 beamline at the Advanced Light Source, in Berkeley, California, USA. For the SH and mSH lattices the islands were oriented 45$\degree$ with respect to the incoming X-ray beam, to enable identification of the magnetization direction of all elements in the lattices. For these lattices multiple, partially  overlapping, PEEM-XMCD images were acquired and stitched together to form one large image containing over 4000 mesospins for each of the investigated lattices, see Supplementary Materials Fig.~2. The images used for determining the magnetic states were taken at 65~K, far below the Curie-temperature and the blocking temperatures of the short- and long-mesospins. The sampling time ($t_{s} = 300~s$) required for obtaining a PEEM-XMCD image defines a time window linked to the thermal stability of the mesospins: At the lowest temperatures, all magnetic states are stable (frozen) and the lattice can be imaged for practically arbitrary long times, yielding the same result. However, if the reversal times are much smaller than $t_{s}$, no magnetic contrast is obtained. This allowed us to ask at which temperature the spins have reversed their magnetization direction within a given time window, thereby providing an estimation on the involved energy scales.

\section{Results}

\subsection{Activation energies of the mesospins}

Magnetic interactions can affect the inferred activation energies in a profound way.
We therefore fabricated two additional lattices consisting of long-  and short-mesospins, 1110~nm and 450~nm respectively, in which the distance was large enough to allow us to ignore any effects arising from the interactions between the elements (see Supplementary Materials). The islands were oriented parallel with respect to the incoming X-ray beam, to determine the magnetization direction of the mesospins.

Following the line of argumentation above, we determined that 50\% of the short islands reverse their magnetization direction within 300~s  at  112~K,  while a temperature of 149~K is required for obtaining the same condition for the long islands.
The determination of the activation energies is model dependent.
Using an expression for the probability of a magnetic element not having altered its magnetization direction after a time period $t_s$\cite{Wernsdorfer1997PRL, Kapaklis2014NatNano}, as described in the Supplementary Materials, yields a ratio for the activation energies of 0.49(4). This approach provides support for well separated energy-scales, which will be assumed to be the case in the remainder of this communication.

\begin{figure}[b!]
	\includegraphics[width=\columnwidth]{Fig2_new_3.pdf}
	\caption{Long-mesospin correlations in the Shakti lattice. The network-averaged magnetic correlations for long-mesospins spatially oriented vertically/horizontally are shown in the left/right graph. In blue/red the correlations of long-mesospins which are oriented in a string and in light-blue/orange the correlations of the long-mesospins diagonally oriented are represented, as indicated in the inset. All correlations show that already the first neighbor is randomly oriented and therefore the magnetic orientations of the long-mesospins are not correlated. Error bars represent one standard deviation.}
	\label{fig2}
\end{figure}

\subsection{Correlations of the long-mesospins in the Shakti lattice}

The correlations between the long-mesospins were determined from the PEEM-XMCD images recorded at 65~K, after cooling the samples from room temperature with a  rate of 1~K/minute. The results from analysis along different directions in the SH lattice are illustrated in Fig.~\ref{fig2}. As seen in the figure, no correlations between long-mesospins are observed.
The cooling of the sample below the blocking temperature of the short-mesospins does not result in any observed order for the long-mesospins. Because of this, the effective interaction mediated by the short-mesospins must be much smaller than the activation energy of the long-mesospins.

\begin{figure}[t!]
\includegraphics[width=\columnwidth]{Fig4_new2-4PRB.png}
\caption{Vertex type definition and statistics for SH and mSH lattices. SEM image of the SH ({\bf a}) and mSH ({\bf b}) lattice. The different vertex types are indicated by their respective colors. The real space base vectors for the Shakti lattice are defined along the x- and y-direction and each have a length of four times the lattice spacing ($d = 600~\rm{nm}$). ({\bf c}),~Definition of the vertex states for all different vertex types. While both lattices share the vertex type with a coordination number of four (green), the mSH lattice contains vertices with coordination number three (red) and two (orange). In the SH lattice the three-fold coordinated vertices (blue) include a long-mesospin.
The four- ({\bf d}) and three-fold ({\bf e}) coordinated vertex statistics for SH (dark-blue) and mSH (dark-red) lattices show no significant differences. Error bars represent one standard deviation.}
\label{fig3}
\end{figure}

\subsection{Magnetic order on the vertex-level}

Having established the randomness of the magnetic states of the long-mesospins in the Shakti lattice, we now turn our attention to the overall magnetic order established within the SH and mSH lattices. For square ice related geometries, a commonly-employed tool for characterizing the obtained magnetic state is the determination of populations of the various types of vertex configurations. The different vertex types for both the SH and the mSH lattices are illustrated in Fig.~\ref{fig3}({\bf a})-({\bf c}).
In the nomenclature used here, a roman numeral denotes the vertex type along with a subscript representing the number of mesospins forming the vertex. As an example, I$_{4}$ represents four elements forming a Type-I vertex. The mSH lattice has an additional degree of freedom as compared to the SH lattice, arising from the two-fold coordinated vertex having two possible states: Type-I$_{2}$ and Type-II$_{2}$.

The vertex statistics obtained for the three- and four-fold coordinated vertices are presented in Fig.~\ref{fig3}({\bf d}) and \ref{fig3}({\bf e}), respectively. Comparing the abundance of the different states with published data from Gilbert {\it et al.}\cite{Gilbert2014NatPhys}, we can again confirm that our results are representative for the weak coupling regime, as $\it{e.g.}$ the previous works on ASI structures\cite{Arnalds2012APL, Kapaklis2014NatNano}. Notice that these vertex statistics do not display a significant difference between the common vertex states of the SH and mSH lattices, similar to previous reports\cite{Gilbert2014NatPhys}. This implies that the final vertex populations are independent of the presence of the long islands in the Shakti geometry and the related energy hierarchy. However, the vertex statistics yield only a partial description of the final magnetic state and are insensitive to magnetic order established over spatial extensions larger than the vertex size.

\subsection{Beyond the vertex-level}
We use the calculated spin structure factor (SSF) to determine correlations beyond nearest neighbours\cite{Canals_NatComm_2016, Perrin_Nature_2016, Erik_ArXiV_2017, Farhan2017NatCom}. This invokes the use of a Fourier transformation of pairwise correlations of the magnetic states in the following form:

\begin{equation}
	I(\mathbf{q})=\frac{1}{N^2}\sum_{(i,j=1)}^{N}\mathbf{S}^{\perp}_i\cdot \mathbf{S}^{\perp}_j \cdot e^{i\mathbf{q}\cdot(\mathbf{r}_i-\mathbf{r}_j)}
	\label{eq:SSF}
\end{equation}

\begin{figure}[b!]
	\includegraphics[width=\columnwidth]{SSF_600_SHmSH_2.png}
	\caption{Spin structure factor maps computed for the four-fold coordinated vertex sub-lattices of the mSH (left) and the SH (right) lattices. The real space lattice vectors as well as the sub-set of four-fold coordinated vertices (red islands) are indicated in the insets.}
	\label{SSF}
\end{figure}

\begin{figure*}[t!]
\includegraphics[width=\textwidth]{Fig6_new9PRB.pdf}
\caption{Spatially-limited spin structure factor as indicator for short-range order. ({\bf a}), Illustration of the mesospin sub-set used in the SSF calculations. The real space lattice vectors ($\mathbf{a}_{1},\mathbf{a}_{2}$) which are used for the reciprocal lattice units (r.l.u.) are also shown. The real space input window size for the averaged SSF $I_1$ (red -- SSF ({\bf b/d}) ) and $I_9$ (blue -- SSF ({\bf c/e}) ) are highlighted. {\bf b-e}, The averaged SSF maps for SH ({\bf b/c}) and mSH ({\bf d/e}) lattices, with reduced real space input size according to equation \eqref{SSF_avg}. ({\bf f}), Diagonal line-profiles for the SSF of different input sizes for the SH (dark-blue) and mSH (dark-red) lattices. The modulation of the intensity in the SSF maps at (q$_x$, q$_y$) = (2, 2) [r.l.u.] is clearly distinguishable for the case of the SH lattice and an indication of a different order for these length-scales. }
\label{fig5}
\end{figure*}

\noindent where $I(\mathbf{q})$ is the intensity for a given scattering vector $\mathbf{q}$ in reciprocal space, $N$ denotes the number of spins over which the SSF is calculated, $\mathbf{S}^{\perp}_{i}$ the spin component perpendicular to $\mathbf{q}$ and $\mathbf{r}_{i}$ is the position of the corresponding spin in the real-space lattice. The SH and the mSH lattices have different lattice points, $\mathbf{r}_{i}$, for the long- and two short-mesospins, the differences in the SSF of the SH and mSH data is dominated by this structural difference. To facilitate a proper comparison between the two cases, only the mesospin sub-set found in both geometries, namely the four-fold coordinated vertices, has been taken into account for the SSF computation. Therefore we calculate the SSF according to equation \eqref{eq:SSF}, in the same manner as is explained in more detail by \"Ostman {\it et al.}\cite{Erik_ArXiV_2017}, but only using the mesospins of the vertices with a coordination number of four. Since this sub-lattice of mesospins is the same in both the SH and mSH lattices, differences in the SSF represent different ordering among these sub-sets of spins. Characteristic SSF maps for the SH and mSH networks are presented in Fig.~\ref{SSF}.\\

Although neither of the two maps presents specific features, such as pinch points or Bragg peaks, their diffuse signals systematically exhibit clear differences. This is indicative of differences in the global spin order, which have not been captured by the statistics determined on the vertex-level (presented in Fig.~\ref{fig3}({\bf d}) and \ref{fig3}({\bf e}) ). The striking feature is the presence of a hollow region ($\it{e.g.}$ at the ($\pm$2,$\pm$2) (r.l.u.) points in reciprocal space) in the SH lattice SSF map, with the same region having a more uniform intensity distribution in the structure factor map of the mSH. To understand the origin of this effect and identify the length-scales that are at play, we have computed magnetic structure factors for networks of gradually-increasing size and network-averaged these individual signals for each chosen network-size. Since the sample is large enough to assume ergodic conditions, this size reduction of the sampling window and the corresponding network-averaging, provides statistical information about the magnetic state on the length-scale of the sampling window rather than the high spatial frequencies of the speckle pattern (Fig.~\ref{SSF}) obtained from the specific global microstate.

Hence, we define
	\begin{equation}
		I_L = \frac{1}{\left({4L}\right) ^2 M}\sum_{m=1}^{M}\sum_{(i,j=1)}^{4L} \mathbf{S}^{\perp}_i\cdot \mathbf{S}^{\perp}_j \cdot e^{i\mathbf{q}\cdot(\mathbf{r}_i-\mathbf{r}_j)}
		\label{SSF_avg}
	\end{equation}
as an incoherent\cite{Incoherent} spatial average over sampling windows with $L$ four-fold coordinated vertices. Each sampling window therefore consists of $4L$ spins (taking into account only the short-mesospins). The SSF $I_L$ is the average of all $M$ sampling windows present in the measured global microstate.

Fig.~\ref{fig5}({\bf b}) and \ref{fig5}({\bf d}) show a comparison of $I_1$, i.e.~the averaged SSF for a single four-fold coordinated vertex (four mesospins) for the SH and mSH lattices. Both are virtually indistinguishable, which is not surprising since $I_1$ is merely a different representation of the vertex statistics shown in Fig.~\ref{fig3}({\bf d}). In other words, as the vertex statistics showed no significant differences, the SSF maps in Fig.~\ref{fig5}({\bf b}) and Fig.~\ref{fig5}({\bf d}) should also be similar, traceable also in a comparison of the top-most diagonal line-profiles in Fig.~\ref{fig5}({\bf f}). Expanding the SSF input window to sixteen mesospins ($I_4$, four four-fold coordinated vertices), a clear difference between the SH and mSH appears, with a more pronounced dip in the intensity at the (2,2) reciprocal space position for the SH lattice case (Fig.~\ref{fig5}({\bf f}) ). Expanding the real space input window to thirty-six mesospins ($I_9$, nine four-fold coordinated vertices), the differences in the SSF maps between the SH (Fig.~\ref{fig5}({\bf c}) ) and mSH (Fig.~\ref{fig5}({\bf e}) ) become even more pronounced (see also the line-profiles in Fig.~\ref{fig5}({\bf f}) ). The line-profiles in Fig.~\ref{fig5}({\bf f}) are diagonal cuts through the respective SSF maps $I_1$, $I_4$, $I_9$ and $I_{16}$ from reciprocal space position (q$_x$, q$_y$) = (0, 0) [r.l.u.] to (q$_x$, q$_y$) = (4, 4) [r.l.u.]. The results from these spatially-limited SSF maps in Fig.~\ref{fig5} are qualitatively similar to the features observed for the SSF of the full microstate in Fig.~\ref{SSF} and capture differences in the magnetic short-range order, exceeding the extension of just one vertex. \\

\begin{figure}[t!]
	\includegraphics[width=\columnwidth]{Fig5_new5PRB.pdf}
	\caption{Spin arrangements across the long-mesospins / two-fold coordinated vertices. ({\bf a}), Schematic representation of all mesospins contained within two neighboring three-fold coordinated vertices (gray numbered islands). We classify the arrangements of all these mesospins in three classes, denoted as A$_1$, A$_2$ and A$_3$. The abundance values of A$_1$ and A$_2$ are averages of the four possible spin arrangements in these classes. One representative spin arrangement for each of the three classes is depicted in ({\bf a}). The coupled four-fold coordinated vertices are indicated by the light-green islands. The number of coupled four-fold coordinated vertices across the Type-I$_2$ vertex or a long-mesospin is two for A$_1$, three for A$_2$ and all four for A$_3$. ({\bf b}), The abundance of these three classes is plotted for the SH (dark-blue) and the mSH (dark-red) lattices, the abundance for each spin arrangement in a random mesospin state is represented with a gray inside bar. The abundance revealing the distinct differences in the arrangement of the mesospins around the Type-I$_2$ vertex and is strongly indicating a defined tiling for the four-fold coordinated vertices around the long-mesospins and the build-up of a short-range order. Error bars represent one standard deviation.}
	\label{fig4}
\end{figure}

\subsection{Short-range magnetic order}
We attribute the origin of the features observed in the SSF maps to the long elements in the SH lattice and the difference in activation energies between the short and long islands. To elaborate more on this premise, we have extracted the abundance of various spin arrangements that connect four-fold coordinated vertices across a Type-I$_2$ vertex in the mSH lattice or a long-mesospin in the SH lattice. Here, we focus on three of the different configurations of interest for such spin arrangements, as presented in Fig.~\ref{fig4}({\bf a}). In the three vertex coupling classes, A$_1$, A$_2$ and A$_3$, a total of nine different ferromagnetic spin arrangements are investigated. A detailed analysis of all nine spin arrangements can be found in the Supplementary Materials Fig.~3. In Fig~\ref{fig4}({\bf b}) we report their abundances for both lattices, along with the estimated values given by a random distribution, in the absence of any interaction between the considered mesospins. A$_1$ and A$_2$ are averages of four different spin arrangements (C$_1$-C$_4$ and C$_5$-C$_8$, see Supplementary Materials Fig.~3), which have the same characteristic. In the case of A$_1$, one mesospin (mesospin 1 or 2 in schematic \ref{fig4}({\bf a}) ) is ferromagnetically aligned to the long-mesospin (or the two ferromagnetically aligned mesospins of the two-fold coordinated vertex) and one mesospin on the other side (mesospin 3 or 4 in Fig.~\ref{fig4}({\bf a}) ). For A$_2$ one mesospin on one side is ferromagnetically aligned with two mesospins on the other side of the long-mesospin (or the two ferromagnetically aligned mesospins of the two-fold coordinated vertex). A$_3$ represents the lowest energy configuration for these five (six in the mSH) mesospins and arranges all mesospins (mesospin 1, 2, 3 and 4 in schematic Fig.~\ref{fig4}({\bf a}) ) ferromagnetically with respect to the long-mesospin (or the two ferromagnetically aligned mesospins of the two-fold coordinated vertex).

\section{Discussion}

The spin arrangements in Fig.~\ref{fig4} highlight the development of a stronger correlation between four-fold coordinated vertices across a long-mesospin in the SH lattice than in the mSH, in which case the coupling is mediated via a two-fold coordinated vertex.
In the Shakti ground state manifold as described by Chern {\it et al.}\cite{Chern2013PRL}, the four-fold coordinated vertices are always in their lowest energy state, Type-I$_4$ (see definition Fig.~\ref{fig3}{\bf c}). This state has a two-fold degeneracy, which we denote by Type-I$_4$(A) and Type-I$_4$(B) (see Supplementary Materials Fig. 4({\bf b}) ). A transition from Type-I$_4$(A) to a Type-I$_4$(B) is given by a magnetization reversal of all four mesospin. Two Type-I$_4$ vertices which are ferromagnetically coupled via a Type-I$_2$ or a long-mesospin will always be of opposite states, Type-I$_4$(A) and Type-I$_4$(B).
Returning to the SSF maps in Fig.~\ref{SSF} and Fig.~\ref{fig5}, the distinct shape in the SSF can be explained by the enhanced effective coupling of Type-I$_4$(A) to Type-I$_4$(B) vertices via the long-mesospins in the SH lattice.
In other words, although the long-mesospins freeze in a random configuration, they are more effective in transmitting magnetic correlations from one end of a Shakti plaquette to the other, than the two-fold vertex of the mSH lattice. While this is a rather straightforward result for the case of one plaquette, it is \emph{a priori} expected that, on the lattice scale, the prior establishment of a random distribution of long-mesospin states would yield an even more randomized configuration of short islands, a fact that the mSH lattice might circumvent given the absence of these constraints.

To further discuss our results we would like to compare them with the ones previously reported by Gilbert {\it et al.}\cite{Gilbert2014NatPhys}. For the strong coupling regime, they observed an almost perfect ground-state ordering of the four-fold coordinated vertices for the mSH lattice, while the SH lattice has only about 80\% of these vertices in the lowest energy state, Type-I$_4$. These differences, in the light of our results, can be attributed to the distinct energy-scales. As the long-mesospins freeze into a pre-defined disordered sub-lattice, the Shakti ground state manifold is restricted and shaped by the long-mesospin sub-lattice. When coupling four Type-I$_4$ vertices via a long-mesospin, 16 different Type-I$_4$-tilings are possible. The Shakti ground state, as defined by Chern {\it et al.}\cite{Chern2013PRL}, can be obtained with only 12 out of the total 16 tilings. The mSH lattice, with its mono-sized short-mesospins, can access the entire ensemble of tilings. However, the pre-defined disordered long-mesospin arrangement effectively reduces the possible states in the Shakti ground state manifold (see Supplementary Materials Fig.~4). The frozen long-mesospin restricts the Type-I$_4$-tiling amongst four four-fold coordinated vertices to 7 out of 16 possible arrangements. As the system grows in size, the Shakti ground state manifold is further reduced by each added frozen long-mesospin (for further information see Supplementary Materials). This is a plausible cause for the higher order found in the mSH lattice for the strong-coupling regime reported by Gilbert {\it et al.}\cite{Gilbert2014NatPhys} compared to the SH lattice. However, as the inter-island coupling strength is reduced, the long-mesospins, although a source of randomness, provide a better locally-correlated state than the two-fold coordinated vertices of the mSH lattice.

\section{Conclusions}

Using thermally-active nano-patterned arrays of weakly-coupled magnetic mesospins, we have highlighted the impact of distinct length- and energy-scales on the development of magnetic order in artificial spin ice. While our study is restricted to the Shakti geometry and the weak-coupling regime, it captures the importance of the energy hierarchy in mesoscopic architectures and its role for the obtained magnetic order. Given the vast opportunities in geometrical design and the available choices of magnetic materials, the energy hierarchy can be engineered, and, in combination with suitable thermal or even demagnetization protocols, used as a tool for tailoring the magnetic order in mesoscopic magnetic structures. The hierarchy of the energy-scales, as well as the interplay between them, lie behind the complex emergent behavior and properties seen frequently across a range of natural systems\cite{Anderson_Science_1972}. Artificial spin systems provide, therefore, a unique opportunity to study emergence, by offering a `designer' fabrication route and parametrization of the relevant variables. This opportunity potentially allows for a better understanding of problems in physics requiring multiple scale-analysis\cite{Wilson_SciAm_1979}.

\section{Acknowledgments}
The authors would like to thank C.~Nisoli and G.W.~Chern for valuable discussions. The authors acknowledge support from the Knut and Alice Wallenberg Foundation, the Swedish Research Council and the Swedish Foundation for International Cooperation in Research and Higher Education. The patterning was performed at the Center for Functional Nanomaterials, Brookhaven National Laboratory, supported by the U.S. Department of Energy, Office of Basic Energy Sciences, under Contract No. DE-SC0012704. This research used resources of the Advanced Light Source, which is a DOE Office of Science User Facility under contract No. DE-AC02-05CH11231.
U.B.A. acknowledges funding from the Icelandic Research Fund grants Nr. 141518 and 152483.

\bibliographystyle{natphys}

redpajama_set_name: RedPajamaArXiv


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text:
Nurses' Lack Of Potentially Life-Saving Knowledge Could Put New Mothers In Danger
Side Effects Public Media | By Nina Martin - ProPublica
Ethan John
https://www.flickr.com/photos/thaen/
In recent months, mothers who nearly died in the hours and days after giving birth have repeatedly told ProPublica and NPR that their doctors and nurses were often slow to recognize the warning signs that their bodies weren't healing properly. Now, an eye-opening new study substantiates some of these concerns.
The nationwide survey of 372 postpartum nurses, published Tuesday in the MCN/American Journal of Maternal/Child Nursing, found that many of them were ill-informed about the dangers new mothers face. Needing more education themselves, they were unable to fulfill their critical role of educating moms about symptoms like painful swelling, headaches, heavy bleeding and breathing problems that could indicate potentially life-threatening complications.
By failing to alert new mothers to such risks, the peer-reviewed study found, nurses may be missing an opportunity to help reduce the maternal mortality rate in the U.S., the highest among affluent nations. An estimated 700 to 900 women die in the U.S. every year from pregnancy- and childbirth-related causes and 65,000 nearly die, according to the Centers for Disease Control. The rates are highest for black mothers and women in rural areas. In a recent CDC Foundation analysis of data from four states, nearly 60 percent of maternal deaths were preventable.
Forty-six percent of nurses who responded to the survey were unaware that maternal mortality has risen in the U.S. in recent years, and 19 percent thought maternal deaths had actually declined. "If [nurses] aren't aware that there's been a rise in maternal mortality, then it makes it less urgent to explain to women what the warning signs are," said study co-author Debra Bingham, who heads the Institute for Perinatal Quality Improvement and teaches at the University of Maryland School of Nursing.
Only 12 percent of the respondents knew that the majority of maternal deaths occur in the days and weeks after delivery. Only 24 percent correctly identified heart-related problems as the leading cause of maternal death in the U.S. In fact, cardiovascular disease and heart failure — which, according to recent data, account for more than a quarter of maternal deaths in this country — were "the area that the nurses felt the least confident in teaching about," says Patricia Suplee, an associate professor at the Rutgers University School of Nursing in Camden, New Jersey, and the lead researcher on the study.
Nurses also said they spent very little time instructing new moms about worrisome symptoms — usually 10 minutes or less. Many of the nurses said they were only likely to discuss warning signs of such life-threatening conditions as preeclampsia (pregnancy-related high blood pressure), blood clots in the lungs, or heart problems "if relevant" — even though, as the study noted, "it is impossible to accurately predict which women will suffer from a post-birth complication."
The post-delivery education provided by nurses is particularly important because, once a mother leaves the hospital, she typically doesn't see her own doctor for another four to six weeks. Up to 40 percent of new moms — overwhelmed with caring for an infant, and often lacking in maternity leave, child care, transportation and other kinds of support — never go back for their follow-up appointments at all.
Figuring out the best way to instruct new mothers is all the more crucial, the survey noted, because the first days after giving birth are "exhausting, emotionally charged, and physiologically draining" — hardly an ideal learning environment. But like so many other important aspects of maternal health care, postpartum education has been poorly studied, Bingham said.
The respondents, of whom nearly one-third had master's or doctorate degrees, were members of the Association of Women's Health, Obstetric and Neonatal Nurses, the leading professional organization for nurses specializing in maternal and infant care. AWHONN began looking at the education issue in 2014, when Bingham was the association's vice president of nursing research and education. "We had to start really from the ground up, because we didn't know exactly what women were being taught," she said.
In focus groups conducted in New Jersey and Georgia, two states with especially high rates of maternal mortality, researchers discovered that postpartum nurses spent most of their time educating moms about how to care for their new babies, not themselves. The information mothers did receive about their own health risks was wildly inconsistent, and sometimes incorrect, Bingham said. The written materials women took home often weren't much better.
Some nurses were uncomfortable discussing the possibility that complications could be life-threatening. "We had some nurses come out and say, 'Well you know what, I don't want to scare the woman. This is supposed to be a happy time. I don't want to seem like all I want to talk about is death,'" Bingham said.
But the researchers also found that nurses could be quickly educated with short, targeted information. Using insights from the focus groups, an expert panel developed two standardized tools — a checklist and script that nurses could follow when instructing new mothers and a one-page handout of post-birth warning signs that mothers could refer to after they returned home, with clear-cut instructions for when to see a doctor or call 911. Those tools were tested in four hospitals in 2015. "Very quickly we started hearing from the nurses that women were coming back to the hospital with the handout, saying, 'I have this symptom,'" Bingham said.
One of them was a Georgia mom named Sarah Duckett, who had just given birth to her second child. A week later, she recognized the warning signs of what turned out to be a blood clot in her lung — an often fatal postpartum complication. "Those were anecdotes, but they were very powerful anecdotes," Bingham said. "I've led multiple projects over the years and rarely do I get such immediate feedback that something is working."
The shortcomings documented by the national survey could foster wider use of these tools, suggested Mary-Ann Etiebet, executive director of Merck for Mothers, which funded the study as part of a 10-year, $500 million initiative to improve maternal health around the world. "Something as simple as creating educational and training programs for nurses … can have a real impact," she said.
ProPublica is a Pulitzer Prize-winning investigative newsroom. Sign up for their newsletter.
Medical Practicematernal heathnursingbusiness of medicine
The Last Person You'd Expect To Die In Childbirth
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States Help New Mothers Get Birth Control Through Medicaid
Moms-To-Be With Addiction Face Obstacles At Every Turn

redpajama_set_name: RedPajamaCommonCrawl


Is carbohydrate-deficient transferrin in serum useful for detecting excessive alcohol consumption in hypertensive patients?
Improved HPLC determination of urinary hydroxylysine glycosides to study turnover rate of bone in humans and rats.
Hormone conference at Sahlgren's University Hospital: polycythemia and inappropriately high serum erythropoietin concentration in a 62-year-old man.
Homovanillic acid in plasma determined by HPLC with direct injection of plasma filtrates.
Pancreatic lipase assays with triglycerides as substrate: contribution of each sequential reaction to product formation.
Use of cardiac troponin I to diagnose perioperative myocardial infarction in coronary artery bypass grafting.
Allelic D variants of transferrin in evaluation of alcohol abuse: differential diagnosis by isoelectric focusing-immunoblotting-laser densitometry.
Hydroxocobalamin and sodium thiosulfate interfere negatively with measurement of creatine kinase activity.
EDTA-plasma vs serum differences in cholesterol, high-density-lipoprotein cholesterol, and triglyceride as measured by several methods.
Immunoassay for quantifying type I collagen degradation products in urine evaluated.
Determination of biotin in biotin-conjugated protein by measuring fluorescence polarization.
Factors influencing changes in the clinical immunology laboratory.
Random and continuous-access immunoassays with chemiluminescent detection by Access automated analyzer.
Assay of plasma oxalate with soluble oxalate oxidase.
High-performance thin-layer chromatography of free porphyrins for diagnosis of porphyria.
Congenital adrenal hypoplasia, Duchenne muscular dystrophy, and glycerol kinase deficiency: importance of laboratory investigations in delineating a contiguous gene deletion syndrome.
In vitro analysis of cell-mediated immunity: clinical relevance.
Total free radical-trapping capacity of serum from diabetics.
Effect on sports drug tests of ingesting meat from steroid (methenolone)-treated livestock.
Recent advances in biochemical markers of bone turnover.
High-performance assays of small molecules: enhanced sensitivity, rapidity, and convenience demonstrated with a noncompetitive immunometric anti-immune complex assay system for digoxin.
Interference with clinical laboratory analyses.
Measurement of human urinary prolactin as a noninvasive study tool.
1,5-Anhydroglucitol: a novel serum marker for screening and monitoring diabetes mellitus?
Increased prevalence of IgM antibodies to Epstein-Barr virus and parvovirus B19 in blood donations with above-normal neopterin.
Creatine kinase isoenzyme BB increased in serum and tumor tissue of patients with giant cell tumor of bone.
Fully enzymatic method for determining 1,5-anhydro-D-glucitol in serum.
Failure of polychromatic correction in measurement of total protein.
The clinical immunology laboratory of the future.
Variance function as basis for assessment of test performance: methodological studies with two assays of prostate-specific antigen.
Increased detection of marijuana use with a 50 micrograms/L urine screening cutoff.
Clinical chemistry: a fragmentary history (1969-1977).
Routine monitoring of temperatures inside thermal cycler blocks for quality control.
Insights into the ontogeny and activation of T cells.
Laboratory diagnosis and monitoring in chronic systemic autoimmune diseases.
Lipoprotein(a) further invalidates Friedewald formula.
Autoimmune endocrinopathies: aspects of pathogenesis and the role of immune assays in investigation and management.
Lipoprotein(a) is included in low-density lipoprotein by NCEP definition.
Advances in diagnosis, prevention, and management of hepatic allograft rejection.


Click on a line of the Object List to get detailed information about the object.
Right-click on an object at the chart and select "About …" in the pop-up window.
When edit label mode is on (the icon in the object toolbar): Click on an object label.
Get a "Neighbour" window by a click on the neighbour button in an information detail window and click on a line as with an Object List.
In any detailed information window you can distinguish 4 paragraphs with their specific sorts of data.
For stars and deep sky objects, this paragraph contains static information about the object which was retrieved from the catalog. For these kinds of objects, they ususally will begin with the object type, catalog short name, the catalog identification, and the relative magnitude. The rest of this content depends entirely on the catalog from which the data is retrieved.
For Solar system objects, you can find information like the object type, and the object identification (name). Please forgive SkyChart when it shows you the Sun as a planet. All other information in this paragraph is dynamically calculated from the ephemeris data. This information depends on the type of solar system object you 're dealing with.
The first line of this paragraph, starting with Coordinates:, informs you to which of the equatorial coordinate systems the chart is set. The chart can show you on several coordinates in the equatorial systems, for example at the status bar. You can specify the equatorial coordinate system of your chart by the tab Chart, Coordinates from the menu by setup → Chart, Coordinates, in the type of coordinates part.
The other lines show you the coordinates of your object in the specified coordinate systems. Here, you can find the equatorial systems (apparent and mean), and also in the ecliptic - and galactic systems.
Here you find specific data relating to your position and time. So there is the name of the site you are observing from with the local date and time. Next, you will find the times in UT and local sideral time. Then there is the positional data for the date and time that was used in the calculation: local hour angle, azimuth and altitude. At the and you can find data about the time and position of rise, culmination and set; unless you are dealing with a circumpolair object. Then there's only information about the culmination.
Here you can find the distance and angle between two objects that you consecutively selected. This data can only reliably calculated when you select the objects from one single calculated chart or list. (A time difference combined with the dynamics of solar system objects can't lead to a precise value.) So, in order to retrieve distances, it can be wise to uncheck the Auto-refresh every checkbox, or to set the auto refresh time to a value so that there's time enough for you to select your objects.
First there is the line that says which objects you selected for the measurement. The next line shows the seperation in degrees of arc in sexagesimal format, and the angle measured from the previous to the last selected object. This angle takes the celestial North as zero reference, and increases by East, South, West. The picture is pretty self explanatory. About the angle: when you are on the Northern hemisphere and your face is directed south, the East will be at the left hand side. The last line shows you the offset in sexagesimal hours and sexagesimal degrees in the equatorial coordination system.


HOUSTON – Transwestern today announces it has named Thomas G. Lawyer President of Transwestern Commercial Services. As the firm's leader, Lawyer will ensure continued service excellence through 35 U.S. offices, guide the implementation of innovative real estate solutions, lead expansion opportunities, and direct strategic business development that capitalizes on the company's consultative service approach to deliver comprehensive solutions to clients.
Lawyer comes to Transwestern from JPMorgan Chase & Co., where he most recently served in Commercial Banking as Vice Chairman of the company's Real Estate Banking Group. During his tenure as head of the group, he was responsible for U.S. real estate banking to top-tier real estate developers, investors, real estate operating companies, investment funds and REITs. His contributions helped JPMorgan Chase build a first-class lending business and become a dominant player in the space. He co-chaired the Real Estate Banking Investment Committee and also served on the Global Real Estate Council for the firm.
Prior to JPMorgan Chase, Lawyer spent nearly a decade with Citibank, where he held the position of Managing Director, Commercial Real Estate Finance, overseeing the national origination platform and operations of a national loan portfolio. Earlier in his career, Lawyer gained significant experience in multifamily, retail, office and industrial portfolio operations, management, mergers and acquisitions, and workouts through his positions at various banks and real estate companies.
Transwestern Commercial Services provides property management, consulting, agency leasing, occupier solutions, capital markets and research services for office, industrial, retail, multifamily and healthcare projects. In addition to serving on the company's board of directors and executive committee, Lawyer will also participate on an enterprise-wide steering committee which spans the services, investment management and development arms of the organization, where he will contribute to, and execute on, Transwestern's aggressive growth initiatives.
Transwestern is a privately held real estate firm of collaborative entrepreneurs who deliver a higher level of personalized service – the Transwestern Experience. Specializing in Agency Leasing, Occupier Solutions, Capital Markets, Asset Services and Research, our fully integrated global enterprise adds value for investors, owners and occupiers of all commercial property types. We leverage market insights and operational expertise from members of the Transwestern family of companies specializing in development, real estate investment management and research. Based in Houston, Transwestern has 35 U.S. offices and assists clients through more than 211 offices in 36 countries as part of a strategic alliance with BNP Paribas Real Estate. Experience Extraordinary at transwestern.com and @Transwestern.
. As the firm's leader, Lawyer will ensure continued service excellence through 35 U.S. offices, guide the implementation of innovative real estate solutions, lead expansion opportunities, and direct strategic business development that capitalizes on the company's consultative service approach to deliver comprehensive solutions to clients.


It's time to say goodbye to pool days and #UCAcamp and hello to your new class schedule and #UCAgameday! Now that you and your teammates are heading back to school, UCA encourages teams to focus on all aspects of cheerleading – Crowd Leading, Spirit Raising, Ambassadorship, Athleticism and Entertainment! You learned at summer camp how to lead within your school and community, now it's time to put it into action!
Crowd Leader: Great crowd leading strengthens unity among the fans, encourages sportsmanship and fosters school spirit. The primary focus should always be on the game and elevating the experience of the crowd. You learned how to be an effective crowd leader at #UCAcamp and now is time to implement all of those techniques!
Spirit Raiser: Your role as a cheerleader means that you exemplify school spirit not only on game days, but every day! Cheerleaders have a unique opportunity to be a positive influence on the entire student body. Students with higher levels of school spirit are more likely to feel more of a connection to their schools and are more likely to perform academically above average.
Ambassador: Cheerleaders are ambassadors of the school. You are a leader and role model in your community, and that is not a role to be taken lightly. It is important to lead by example. This means applying yourself to your school work and showing up to class. Also, as an ambassador and role model you should always be using social media in a responsible and positive way.
Athlete: Cheerleading requires strength, flexibility, endurance and technique to execute skills used during crowd leading, spirit raising and entertainment. Cheerleaders should be dedicated to improving a variety of skills throughout the year. Between practices, school work, performances, games, part-time jobs, and other responsibilities it is very important to take care of yourself. This includes eating healthy, exercising often and getting enough sleep.
Entertainer: Cheerleaders use their crowd leading tactics, spirit and athleticism to entertain! Timeouts, Halftimes, and spirit raising events are your time to shine! Perform dances, stunts, and jumps with skill and confidence – the entire student body may be watching! Pep rallies are also a great time for high energy performances to pump up your student section for a big #UCAGameDay!
By fulfilling these roles, your team will have a positive impact on school spirit and that will translate to a great #UCAGameDay! UCA wants to see your team under the Friday night lights! Use the hashtag #UCAGameDay to share your photos and videos with us! You might even see your team featured on @UCAUpdates Instagram.


Off 1:18. Time 0:53.66. Fast. Also Ran_Sganzinis' Dream, Monterey Secret, Shame On Powers, Choctaw Road, Officer Z Lo, Only Live Once, Singing Hoofer. $1 Daily Double (7-8) paid $92.40. $1 Exacta (8-7) paid $22.10. $0.1 Superfecta (8-7-3-5) paid $25.30. $1 Trifecta (8-7-3) paid $63.30.


What words can you make with vivaries?
An unofficial list of all the Scrabble words you can make from the letters in the word vivaries. Anagrams and words you can make with an additional letter, just using the letters in vivaries!
91 words can be made from the letters in the word vivaries.
This page is a list of all the words that can be made from the letters in vivaries, or by rearranging the word vivaries. These words should be suitable for use as Scrabble words, or in games like Words with friends.


Those are part of chess pieces. The picture show 6 chess pieces, which are the king, the queen, the bishop, the knigt, the rook, and the pawn. Those have different move on chess board and have their own role in chess game. The king is the main chess piece. It can move to any of the squares . The side whose king is captured loses. The Queen can move any number of squares diagonally and also in horizontal and vertical directions. The Bishop can move any number of squares diagonally only.
Then we also have the knight. The Knight can move from one corner to the other of any 2×3 rectangle of squares.His move is different with the rook. The Rook can move any number of squares in horizontal and vertical directions. And the smaller chess pieces is the pawn. The Pawn can move from straight ahead only.
In complete chess set,each player get two bishops, two knights, two rooks, and eight pawns. So that the complete chess pieces amounts of 16 pieces.


I was at fault in an auto accident, no injuries to me or other driver, only minor bumper damage. The driver I hit approached me and asked for $1000 to pay hid deductible. He drafted a document we both signed stating I fully reimbursed him for the deductible. Now apparently he has filed a claim and I am being asked for $1835, the total amount of the claim, and another $1400 they paid him? I thought this was illegal because the insurance company has no more rights than the policy owner? Also, double collecting? Am I supposed to pay again?
It also depends on legal restrictions of your country. However, if you want to sort out the matter without the consent of authorities then I think you will have to agree on his demands.


text:
What if it rains on the papal visit: Where to go, what to wear and how to stay informed
Pope Francis wears a poncho as he addresses a soaked crowd in the Philippines.
Anna Orso
A year after a massive typhoon swept through the Philippines, Pope Francis held a service in Manilla this past January in front of more than six million attendees to remember the thousands who were killed. It was storming again that day, and people wearing plastic covers held candles as the rain drenched them and strong winds blew. The Pontiff himself wore a yellow poncho, and the mass went on.
Weather in Philadelphia can be a bit more predictable than that in the islands of the Philippines. But the Pope's end-of-September visit to the city will still fall in hurricane season, and there's always the possibility that rain could come, or worse: strong winds and inclement weather that could prove unsafe for attendees.
So what happens if there's a storm?
The Archdiocese will be responsible for protecting the Pope, but the city will have to get proper messaging out to the potential two million people who could be in a small area of the city, especially if dangerous weather hits before or during the papal mass on the Sunday afternoon of the visit.
Samantha Phillips, director of the Office of Emergency Management for the City of Philadelphia, said conversations about what do if bad weather hits the Parkway "have been taking place for years" as the number of large, special events that take place on the busy Philly stretch increase every year.
For instance, OEM has emergency plans in place for events like Welcome America (the giant Fourth of July event on the Parkway each year), and for Made in America, the concert curated by Jay Z that was evacuated and shut down for several hours last year because of dangerous weather in the area.
"We learned so much from just trying to encourage 55,000 to 60,000 people to leave a Jay Z concert last year," Phillips said. "People don't want to go."
She said OEM will start closely monitoring the weather patterns and having close communications with the National Weather Service about 10 days out from the papal visit to prepare for what could be in the pipeline. The office will also be in close contact with state and national partners like FEMA and the Secret Service, so that if inclement weather is on its way, decision-makers can gather to discuss options.
If it's simply raining and the mass goes on, Phillips said she "highly suspects" that umbrellas won't be allowed because of safety and visibility concerns. If there's any chance of rain, bring a poncho.
So when hundreds of thousands of people gather on the Parkway for the papal mass, the city will have already set up a number of jumbotrons that will have messages on them and, in the case of a need for evacuation, will display messages telling people to vacate the area and seek shelter, whether it's because lightning or wind is threatening the area.
Phillips said OEM doesn't have a specific formula for when to call an evacuation and when not to, but if lightning is striking within a few miles of the events or wind could knock over poles or structures, the office will evaluate asking people to leave.
From there, people will be either ushered into safe spaces or can find them on their own. But where do you put two million people seeking shelter? Phillips said many will crowd into hotels, parking garages and SEPTA for safety, and OEM has had conversations with the Convention Center regarding opening its doors to provide shelter to thousands of people who would theoretically be seeking it.
But at the end of the day, OEM can't force people to leave the Parkway or mandate any sort of evacuation. It can only recommend it.
Phillips offered the following tips for people traveling to the Parkway for Pope-related events so that the public can be well prepared for what could be to come:
Have your cell phone charged, and bring along your charger. The city will have charging stations set up so that people can charge and be in contact with family and group members.
Bring empty water bottles to fill up on the Parkway, and be sure to check beforehand about what items are allowed in and what items aren't.
Sign up for OEM's emergency text alerts and follow them on social media to keep up-to-date on what's happening.
Use the Parkway's public safety grid, and coordinate with your group ahead of time about which grid location you'll meet at in the case of severe weather (i.e.: meet at H2 or G7). The letter/ number combinations can be found on flags on the Parkway.
Find other preparedness tips on OEM's website at phila.gov/ready.
Philly's queer doula collective is helping LGBTQ parents navigate the health system
There are support groups, family meet-ups, and a growing resource list.
By Michaela Winberg
· Today, 7:00 a.m.
Harriet Tubman is Philadelphia's first monument to a historical Black woman…but it's only temporary
You can count the city's statues of women in history on one hand.
By Conrad Benner
VIDEO: Martin Luther King Jr. at Girard College in Philadelphia, 1965
The civil rights leader spoke to a crowd protesting segregation at Girard Collge.
By Billy Penn Staff
Philly's coronavirus response
Police, fire, and streets departments lag behind as Philly extends vaccine mandate for city employees
About 81% of the municipal workforce is fully vaccinated against COVID.
Headlines of Yore
Nearly 100 years ago, Pa.'s Senate race was jolted by allegations of election fraud in Philadelphia
The ostensible winner of the 1926 contest, Republican William S. Vare, was never seated as senator.
By Avi Wolfman-Arent
Betty White birthday celebrations in Philly, and local animal shelters to support in her honor
How to toast the late, great actress, who died just before her 100th birthday.
By Asha Prihar
Deadly Fairmount Fire
New mutual aid fund at the school near the Fairmount fire aims to help families — and combat student inequity
Bache-Martin Elementary is located in a well-off neighborhood, but the district considers 90% of its enrollment economically disadvantaged.
By Jordan Levy
Philly's COVID recovery
Philly colleges are starting to require boosters and double-masking for the spring semester
Most COVID regulations apply to students, faculty and staff, but specifics vary by school.
Penn swimmer Lia Thomas and the overblown frenzy over her participation in college sports
The science behind why she's allowed to compete with women.
Jim Gardner's final 11 o'clock broadcast on Action News, and his wish for the next year: 'To see the pandemic retire before I do'
The TV veteran will continue on the 6 p.m. newscast, and be replaced on late-night by Rick Williams.
Some Philly restaurant workers feel like they can't call out — much less ask for sick pay — as omicron causes staff shortages
"There's not a lot of people in service work that have a safety net," said the manager at one Center City spot.
By Tom Riese
A hard look at the numbers behind 2021's record gun violence in Philly, and an overview of what's being done
People of color and young adults bore the brunt of city shootings.
By Beatrice Forman
Secret Philly
125 years after women founded The Plastic Club to break into a men-only scene, the arts group is thriving
With headquarters in Center City and a popular exhibit on Instagram, the club is recruiting new members.
By Carrie Hagen
CravePhilly
The Pasta Lab is turning out amazing noodles in a Kensington warehouse
It's all made with Pennsylvania wheat and Lancaster dairy.
By Hope Cohen
1990s battle over Mt. Airy AIDS hospice center shows the power of grassroots opposition — and the limits of NIMBYism
After much controversy, Betak eventually opened, but it would not last long.
PHA owns thousands of other rowhomes like the one that burned in Fairmount
The housing authority has a huge portfolio of so-called "scatter sites," which were long neglected.
By Jake Blumgart
How to help survivors of the devastating and tragic Fairmount house fire
The blaze tore through a home owned by PHA, taking 12 lives — eight of them children.
What's the deal with the rogue COVID testing sites in Philly? Here's everything we know
How to spot them, and why they're so problematic.
Broke in Philly
Philly's unique and successful Way Home program is helping LGBTQ people find housing
Originally dependent on CARES Act funding, advocates are working to make it last.
What new FDA abortion pill guidelines mean for Philly and Pa.: More access, and maybe lower costs
Planned Parenthood now offers mail-order medication, but state-run health insurance still won't cover it.
More Billy Penn


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As our planet warms and sea ice melts, polar bear populations are increasingly at risk.
About Polar Bears
The largest bear in the world and the Arctic's top predator, polar bears are a powerful symbol of the strength and endurance of the Arctic. At least two thirds of the world's polar bears live on Canadian territory, giving Canadians a special relationship with —and responsibility for— these bears. The polar bear's Latin name, Ursus maritimus, means "sea bear." Its an apt name for this majestic species, which spends much of its life in, around, or on the ocean — predominantly on the sea ice.
As sea ice melts, more and more polar bears can be found resting along Arctic coastlines. It is in these areas where their powerful sense of smell attracts them to garbage, stored food, dog teams and animal carcasses — bringing them into greater conflict with Arctic people.
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Polar Bear Facts
SPECIAL CONCERN
Ursus maritimus
Inuktitut Name:
Nanuq
A wildlife species that may become threatened or endangered because of a combination of biological characteristics and identified threats.
Males up to 800 kg, females up to 400 kg
Males up to 3 m long, females up to 2.5 m long
Approximately 22,000 to 31,000
Arctic sea ice and coasts
Seals, walrus, beluga whales
Polar bears have large paws the size of dinner plates that evenly distribute their weight, so they don't fall through the sea ice. Polar bears have three sets of eyelids; the third helps protect their eyes from the glare of snow and ice.
Why Are Polar Bears Important?
Being at the top of the food web, polar bears can signal that there are problems in the Arctic marine ecosystem. They are likely to be among the most significantly affected species as the Arctic warms and sea ice melts.
Over thousands of years, polar bears have also been an important part of the cultures and economies of Arctic peoples. Polar bears depend on sea ice for their existence and are directly impacted by climate change, serving as an important indicator species.
The polar bear's future is inextricably linked to its sea-ice habitat. As climate change continues to reduce the thickness of sea ice, the future of polar bears and their habitat are at risk. Less ice means increased conflict with humans as bears spend more time on land seeking new sources of food.
The ice is the foundation of Arctic marine life, the ecosystem on which bears rely for every aspect of their lives. It is where they mate and raise their cubs. Sea ice is also essential habitat for their primary food, ringed seals, as they pup and rest on the ice. Current knowledge shows that polar bears have some capacity to adjust to the warming Arctic, but the loss of sea-ice habitat may be happening too rapidly to allow for adaptation and there are no substitutes on land for the fat-rich seals on which the bears depend.
Some of the best-studied polar bear populations are spending more time on land, like those in Manitoba, Ontario and southern Nunavut. Without sea ice and seals, polar bears are left to search for other food sources. This can lead them into communities, where garbage dumps, sled dog yards and human food storage offer easy pickings. Conflict between bears and people can follow.
What WWF-Canada is Doing
In Canada and across the Arctic, WWF supports polar bear studies that determine the number of bears, their health and the state of sea-ice habitat. This research includes satellite telemetry studies that help us understand their movements and habitat requirements.
WWF is advocating for the protection of polar bear denning areas across the Arctic and working with Northern communities on effective polar bear co-management. Many Inuit believe that polar bears will adapt to a changing climate and have reported local increases in polar bear numbers in some areas of the Arctic. There is a need to use both Inuit knowledge and scientific information to plan for a healthy future for polar bears and people in the North.
What is certain is that polar bears will face a difficult future without sea ice, which has been the foundation of their lives for hundreds of thousands of years. WWF is helping Northern communities live safely alongside the Arctic's top predator. We work with communities to improve waste management, we fund training and salaries for locals to deter bears from villages and safeguard communities, and we raise awareness within communities on best practices for reducing conflict with polar bears.
Read about WWF's efforts to protect the Last Ice Area, the area where sea ice will be most resilient, and what this will mean for polar bears.
With a changing climate, polar bears are increasingly at risk. With your gift, you can help protect some of the world's most vulnerable species and the habitats they call home.
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Every Tuesday we open our class to advanced and professional dancers. Join us in our fieldhouse studio—challenge your technical practice, hone your movement pick-up, strengthen your body, and excite your sense of play-in-motion. Classes are usually led by master teacher and The Seldoms' Assistant Director Christina Gonzalez-Gillett with other guest teachers and ensemble members some times leading as well. Check our website, facebook, or instagram to see if any guest teachers are popping up soon!


A puppy farmer who sold a couple an unvaccinated dog suffering with a hernia has been fined - but hasn't been banned from selling dogs.
Tufal Ahmed, from Bodymoor Heath, near Kingsbury Water Park, was illegally selling puppies which he advertised as being 'fully vaccinated' and 'micro-chipped' but one couple found that to be far from the truth.
When looking for a dog, the couple discovered Ahmed's advert and contacted him about buying an English bull dog puppy. As well as claiming the dog was fully vaccinated and micro-chipped, Mr Ahmed also said that it was Kennel Club registered and had been checked by a vet.
After visiting the puppy, which appeared to be caged all alone, without its parents and with no other dogs present, the couple paid £1,275 to Ahmed by bank transfer.
Once they paid for the dog, Ahmed's lies started to come out. The couple were expecting to receive the official Kennel Club papers, but they never arrived and Ahmed told them that the dog had not been vaccinated after all.
A visit to the vet also revealed to the couple that the English bull dog was suffering from a hernia and had previously been operated on, information that they had not been aware of when buying the dog.
North Warwickshire Borough Council's environmental health team began to investigate the case after a councillor raised the alarm and a complaint was made to Warwickshire County Council's trading standards department.
When interviewed under caution at the Borough Council, Ahmed revealed that he had re-homed and sold between 15 and 20 puppies in 2016, and, in some cases, had been paid for doing so.
He did not have a pet shop licence, admitted that some of the dogs were poorly and unvaccinated and also kept no records of where the dogs had come from or who they had been sold to.
After pleading guilty, Ahmed was fined £944.88 for illegally selling on puppies without a pet shop licence and his fine was reduced by a third for his early guilty plea.
Ahmed has not been disqualified from selling dogs as the borough council has said he is now working with them and has applied for the correct licence.
Steve Maxey, assistant chief executive and solicitor to the council, said: "This was a successful prosecution which highlights the importance of having the correct licence, approved by the borough council – whether you own a pet shop or are breeding dogs.


text:
Rhammatocerus is een geslacht van rechtvleugeligen uit de familie veldsprinkhanen (Acrididae). De wetenschappelijke naam van dit geslacht is voor het eerst geldig gepubliceerd in 1861 door Saussure.

Soorten
Het geslacht Rhammatocerus omvat de volgende soorten:
Rhammatocerus alticola Hebard, 1923
Rhammatocerus brasiliensis Bruner, 1904
Rhammatocerus brunneri Giglio-Tos, 1895
Rhammatocerus cyanipes Fabricius, 1775
Rhammatocerus excelsus Bruner, 1904
Rhammatocerus gregarius Saussure, 1861
Rhammatocerus guerrai Assis-Pujol, 1997
Rhammatocerus palustris Carbonell, 1988
Rhammatocerus peragrans Stål, 1861
Rhammatocerus pictus Bruner, 1900
Rhammatocerus pratensis Bruner, 1904
Rhammatocerus pseudocyanipes Assis-Pujol, 1997
Rhammatocerus schistocercoides Rehn, 1906
Rhammatocerus suffusus Rehn, 1906
Rhammatocerus variabilis Bruner, 1900
Rhammatocerus varipes Bruner, 1905
Rhammatocerus viatorius Saussure, 1861
Rhammatocerus victori Alves Dos Santos & Assis-Pujol, 2003

Veldsprinkhanen

redpajama_set_name: RedPajamaWikipedia


It's a great time to buy real estate in Poway School District and our site is a great place to begin your search. With the recent boom in Poway School District sales, you can be assured that you have the best tools available for your search. Poway School District real estate is hot and now is the time to act. Have a great time searching for your next Poway School District home!
Remember, we empower the community with your transaction. Pick your favorite Poway School District Animal Shelter or Poway School District Charity and a sizable donation will be made at the close of the transaction.


text:
<?php
/* Loader.php is for loading custom extensions for redux and in
 * accelerated-mobile-pages\includes\options\extensions folder
 *
 * More on loading on extensions is here https://github.com/ReduxFramework/redux-extensions-loader
*/
if(!function_exists('ampforwp_register_custom_extension_loader')) :
    function ampforwp_register_custom_extension_loader($ReduxFramework) {
        $path    = AMPFORWP_PLUGIN_DIR.'/includes/options/extensions/';
            $folders = scandir( $path, 1 );
            foreach ( $folders as $folder ) {
                if ( $folder === '.' or $folder === '..' or ! is_dir( $path . $folder ) ) {
                    continue;
                }
                $extension_class = 'ReduxFramework_extension_' . $folder;
                if ( ! class_exists( $extension_class ) ) {
                    // In case you wanted override your override, hah.
                    $class_file = $path . $folder . '/extension_' . $folder . '.php';
                    $class_file = apply_filters( 'redux/extension/' . $ReduxFramework->args['opt_name'] . '/' . $folder, $class_file );
                    if ( $class_file ) {
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                    }
                }
                if ( ! isset( $ReduxFramework->extensions[ $folder ] ) ) {
                    $ReduxFramework->extensions[ $folder ] = new $extension_class( $ReduxFramework );
                }
            }
    }

    add_action("redux/extensions/redux_builder_amp/before", 'ampforwp_register_custom_extension_loader', 0);
endif;

redpajama_set_name: RedPajamaGithub


Add Digits of the Number Using Single Statement : [crayon-5cbc1655c4a47220262938/] Output : [crayon-5cbc1655c4a51698628361/] How ? [crayon-5cbc1655c4a56165302382/]In 'For Loop' Condition is first tested and then body is executed. Carefully Look at Semicolon at the end of 'For Loop' , which tells us two Things -For Loop is Bodyless. Only Condition and Increment Statements will be executed.
Way 1 : Using Recursive Function [crayon-5cbc1655c4e5e738417111/]Way 2 : Using While Loop [crayon-5cbc1655c4e66504580677/]Way 3 : Using While Loop [crayon-5cbc1655c4e69175732460/]Way 4 : Using For Loop [crayon-5cbc1655c4e6c762750777/]Way 5 : Using Subtraction [crayon-5cbc1655c4e6f232592775/] Note : This Example have Arithmetic Operator [-] but this example is for "Adding two numbers without using + Operator "


At over 10,000 kilometers, passing through nine countries with temperatures ranging from minus 10-degrees Celsius to above 45 centigrade, this has been a test at all extremities - with some impressive landscape photographs captured by the pair during their trip.
The goal of the boys' trek has been to raise £25,000 in support of A Child Unheard, a charity working to improve the lives of children in Africa through education, sports and arts. Both Will and Charles' have been saving up money from their part-time jobs to fund the trip themselves, ensuring that all donations will go directly to A Child Unheard via the boys' JustGiving charity page.
The 10,000 kilometers covered nine countries and took Will and Charles four months to complete, from May to September of this year, and over the 120 days the boys have climbed to over 4,000 meters while descending below sea level. Supporters have been able to keep in touch with the Beijing-to-Tehran duo and monitor their progress via their blog on www.BeijingToTehran.com, where they have also been sharing amazing photos and stories during their journey.


text:
Marioara Trașcă, född den 29 oktober 1962 i Bukarest i Rumänien, är en rumänsk roddare.

Hon tog OS-silver i fyra utan styrman i samband med de olympiska roddtävlingarna 1988 i Seoul.

Referenser

Källor

Externa länkar
Sports-reference.com

Rumänska roddare
Rumänska olympiska bronsmedaljörer
Olympiska bronsmedaljörer 1988
Rumänska olympiska silvermedaljörer
Olympiska silvermedaljörer 1984
Olympiska silvermedaljörer 1988
Tävlande vid olympiska sommarspelen 1984 från Rumänien
Tävlande i rodd vid olympiska sommarspelen 1984
Tävlande vid olympiska sommarspelen 1988 från Rumänien
Tävlande i rodd vid olympiska sommarspelen 1988
Idrottare från Bukarest
Födda 1962
Levande personer
Kvinnor


April 1st is a day that has several meanings, first it's a day where children, parents and adults play tricks on each other. The other is what I am calling the three D's, a day associated with the Gilford Park Yacht Club its "DUES DUE DAY". If you paid your dues THANK YOU. If you haven't, I have to ask why? As I explained in past messages you get so much for so little and how important your dues are to the operation of the club. Without your dues the club ends up with a short fall and ends up robbing from Peter to pay Paul and eventually a bill goes unpaid. This adds additional stress to those members who are trying to make ends meet. Also, if you don't already know, all your privileges and amenities the club offers are suspended until you pay your dues. With the new proposed bylaw change you will only have 90 days to pay (not a year) or you lose your membership.
We are a very diverse group of members and I can't express enough! how important you! the members are! all of you! not just some! but all of you are to your club. All our members are like teeth in a giant gear as a new member joins they becomes a new tooth in that gear, also if we lose a member or one that does not participate that tooth becomes broken or missing and the gear stops working (turning). I have been in the club when there is no one there its just a plain building with a view. It doesn't become a club until it is filled with members, it doesn't become a great view until our members eyes view it and realize it is a view to behold.
We are a very private and exclusive club. Due to our boundaries we are very limited and since have limited ourselves even further by capping the membership. With that said, this places a greater burden on the members we already have and places more importance on you the member like I said above. Your participation on what goes on at the club in attending the meetings, participating in activities, by just coming down and socialize, have lunch, and dinner on the nights the kitchen is open and most important attend the different events the club sponsors.
I know and understand that our members have other places to go and other things to do throughout the year and that's ok. They have duel membership with different clubs or other organizations in the area and that's OK. I know that these organizations offer amenities and philosophies the Gilford Park Yacht Club can't offer, and that's great and that's ok. Some of These organizations do not have boundaries and may include everyone from a township, county, or their bylaws include people that can be linked to them by name of group only. These groups out number our membership as much as 10 to one. As I explained above we are limited to boundaries.
It is a must and important to support all the groups you belong to. There are only so many calendar events throughout the year that are celebrated by all the different clubs and organizations. If you only go to one you hurt the other and vise a versa. Try to support The Gilford Park Yacht Club as much as you can. Don't become that missing tooth in that gear.
Well I'm just going to leave it at that. Please read it again.
I would like to thank all who supported us on our St. Patty's day March 10 the day of the parade. Those who couldn't make it we missed you. I am thanking all who organized and worked the event. Special thanks to ED Gillan who organized the event and picked up the corn beef along with John Hogan and worked as a waiter. Thanks to Dennis Palmatier, Mary Ann Senatore, Pat Mullen, Sue Racaniello, Linda Wilbert and Manny Muina who worked the kitchen they made 103 corn beef sandwiches and 28 dinners.


text:
Зенаїда північна (Zenaida macroura) — вид голубових. Горлиця названа на честь принцеси Зенаїди Бонапарт, дружини французького орнітолога Шарля Бонапарта. Є одним з найзвичайніших і найпоширеніших птахів Північної Америки. Етимологія: «macroura» — з грецької довгохвоста.

Поширення
Багамські острови, Беліз, Бермуди, Канада, Кайманові острови, Колумбія, Коста-Рика, Куба, Домініканська Республіка, Сальвадор, Гватемала, Гаїті, Гондурас, Ямайка, Мексика, Нікарагуа, Панама, Пуерто-Рико, Сен-П'єр і Мікелон, Теркс і Кайкос, Сполучені Штати. Ареал майже на 11 мільйонів квадратних кілометрів. Приблизна кількість особин даного виду: 475 000 000. На нього полюють як для спорту так і м'яса.

Поведінка
Розмножується в різних середовищ існування, починаючи від рідколісся до напівпосушливих пасовищ, але в межах досяжності води. В основному є один партнер одночасно. Самиця відкладає рівно два яйця. Іноді, однак, вона відкладає яйця в гнізда інших пар, що призводить до трьох-чотирьох яєць в гнізді. Яйця маленькі і білі. Обидва батьки висиджують яйця і піклуються про своїх пташенят. Пташенята вилуплюються через 14 днів. Дорослі зазвичай їдять тільки насіння, молодь голубине молоко. Вони часто ковтають гравій або пісок, для допомоги в обробці їжі. Птах є сильним льотчиком і може літати зі швидкістю до 88 км/год. Під час сну голова спочиває між плечима, близько до тіла, і не заправлена під пір'я, як робить більшість видів. Найбільші хижаки цього виду це соколи і яструби. Під час гніздування воронові, домашні коти, вивірки, деякі змії можуть полювати на яйця. Живуть 6—7 років у дикій природі, але один екземпляр жив до 19,3 років.

Морфологія
Довжина: 28–33 см, вага 85—170 г, розмах крил: 37–45 см, яйце 28 на 32 мм. Схожа на голуба формою і розміром. Має тьмяно-коричневий колір з вохристо-коричневою головою, шиєю і низом, кільця навколо очей блідо-блакитні. Деякі чорні плями видно на крилах, а також одне під вухом. Довгий хвіст темнішає до кінчика. Самиця тьмяніша і має коротший хвіст. Сидить з трьома пальцями по напрямку руху і один назад. Ноги короткі й червонуватого забарвлення. Дзьоб невеликий і темний, як правило, це суміш коричневого і чорного.

Примітки

Література
 BirdLife International 2012. Zenaida macroura
 The Federation of Alberta Naturalists Field Guide to Alberta Birds
 Alderfer, Jonathan K. National Geographic Complete Birds of North America. National Geographic
 Animal Diversity Web

Голубові
Птахи, описані 1758
Птахи Куби
Птахи Гаїті
Птахи Домініканської Республіки
Птахи Сен-П'єру і Мікелону
Птахи Теркс і Кейкос


text:
Q: Match major.minor.revision-SNAPSHOT with regex I'm new in regex and I want one that matches this pattern:
major.minor.revision-SNAPSHOT

where major, minor and revision are numbers of one or more digits.
Examples:
`1.2.0-SNAPSHOT` must match
`165.2.23-SNAPSHOT` must match
`165.2.20` must not match
`165.2.20-` must not match

I have tried this one:
(\d+)\.(\d+)\.(\d+)[-](-SNAPSHOT)?.*

But it doesn't work as expected.

A: Try this: \d*[.]\d*[.]\d*[-]SNAPSHOT - it takes ~0ms to execute. Tested in Regex101.

A: Solved. The right regex is ^\d+\.\d+\.\d+-SNAPSHOT$

redpajama_set_name: RedPajamaStackExchange


My daughter is successfully employed with a private firm as a Software Professional. To describe about our family, we belong to the Christian - Syrian Jacobite caste and looking for a match from the same community. We are a nuclear family with traditional values. My daughter resides in Bhopal.
My daughter is a born again God Fearing girl, she has done BSc in Nursing , and presently working with one of the reputed hospital in Indore.
My daughter is an engineering graduate and also persued her Master's degree in Business Administration , she is currently working in a US firm as a Tax Associate located in Bangalore.
My daughter is a 26yr old girl who is working as an Inside Sales Specialist at Practo Technologies Pvt. Ltd. She stands at 5'"4" and has a wheatish complexion. She has completed her graduation from Bhopal School of Social Sciences and her Masters from National Institute of Technology, Bhopal. She is a career oriented person and believes in modern values. She love pets a lot. Her hobbies include singing, dancing, playing TT. She loves to travel and explore different places. She is the most loved girl in our family. She is broadminded, confident and full of life and also believes in her values and morals.
My daughter was born in Mumbai and raised up in Bhopal. Fair and slim, convent educated, passed CBSE 12th in 2010. Did MBBS from MP state Govt Medical college, state merit, (Gandhi Medical College, Bhopal) and completed internship in March 2016. Now pursuing MS (General Surgery) 2017-2020 Batch, NEET PG merit, from the same Medical College.
My daughter has completed her Bachelor's degree. She is currently Not Working and she lives in Bhopal. We come from an Upper middle class, Nuclear family background with moderate values.
To describe about our family, we belong to the Christian - Syrian Orthodox caste and looking for a match from the same community. My daughter is successfully employed with a private firm as a Student. We are a nuclear family with traditional values. My daughter resides in Bhopal,M.P.
My daughter is a network engineer with a Bachelor's degree currently working in Private sector in hyderabad. We belong to a Middle class, Nuclear family with Moderate values. Require a groom brought up in north india, god fearing and church oriented person. Strictly no to Dowry system and person with drinking habits. Also groom brought up in south is not preferred.
My daughter is a Teaching / Academician with a Bachelor's degree currently working in Private sector in Bhopal. We come from a Upper middle class, Nuclear family background with Moderate values. She holds hold a diploma in communication design programme from a reputed university in Coimbatore. Would like to study further.
This profile is created for my Son who did his Engineering in Mechanical & then MBA (Operations /Consulting) from NMIMS, Mumbai. Prior to his MBA, he worked as Planning Engineer in Reliance Industries for 3 years & now has got placed in a MNC as Senior Consultant.
My son Jomin is a Designer with a Bachelors degree in graphics currently working in UK based MNC placed in Delhi. We come from an Upper middle class, Nuclear family background with Liberal values.
This profile is created on behalf of my son. He is working as Sr. Section Engineer in Indian Railways posted at Bhopal division. He got married in May 2015 & got separated within a month as the mistake was in the part of girl and he was totally innocent. The situation was out of control because of which they got legally separated with mutual consent. If you are interested in his profile and wish to know further , kindly contact.
My son is a Marketing Professional with a Master's degree currently working in Private sector in an MNC in Bhopal. We come from an Upper Middle class, Nuclear family background with Traditional values.
My younger brother has a Master's degree in Engg. Currently working in Private sector in Bhopal. We are from an Upper middle class, Nuclear family background with Moderate values.
I am mechanical Engineer and I am employed in Private Sector as an Engineer - Non IT currently based in Bhopal. I belong to a Middle class, Nuclear family with Moderate values.
My brother has a master's degree and he is employed in private sector as a banking service professional currently based in Pipariya (Hoshangabad). We belong to a middle class, joint family with orthodox values.
Hi ,tnks for visiting my profile.I am Sinoj G Yohannan.I am simple in nature . Found of pets and also i like time spending with my niece.i did bachelor in Physiotherapy from Coimbatore.Preparing for IELTS And also doing Master in sports Physiotherapy and self employed .Travelling is my hobby.i used to journey a lot and very much passion about Motorbykes.I am God fearing person .I am looking for a girl who loves traveling, understanding, who is also religious and well nature .Takecare of me as well my family.