text:
Q: 100% cpu usage in drupal I'm use views , cck ,panel and several modules use in my site
and now when open front-page delay for request from drupal site and Apache for loaded page is 20 seconds and now when disable views modules my website is no delay and fast loaded and no usage 100 CPU
next question
how to moderate for /admin/builds/blocks because i have 150 blocks and this loaded page is very slow , can i this page show in several page? or show any region blocks display in page?

A: Views 3 supports query cache and output cache, which help you save your resource.

A: Views can be a resource-hog if you have complex or large queries. Try installing the Devel module and turn on query logging. Then when you go to your front page, you will see a list of all database queries made to render that page at the very bottom. Any troublesome queries will be highlighted in red.
As nice as views and panels are, sometimes you need to code by hand to get better performance. Those modules bring a lot of "weight" to a page.

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text:
Alfredo Bosch
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Alfredo Bosch (Born on 11 February 1985) also known as Alfred Bosch is a Spanish football player who currently plays for Farnborough FC in England (UK). Alfredo Bosch Corberá is a football player who typically plays as a central defender but has also been a holding midfielder and right back. His arrival at Farnborough was welcomed by fans. He was scouted and trained by the premiership youth team of Valencia CF.
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text:
\section{Introduction}
Inversion symmetry breaking and polar structural instability in metallic compounds have received growing attention as a key factor for exploring exotic electronic states \cite{1,2,3,4,5,7,33,22,51}. For superconductivity, breaking the inversion symmetry yields unique features by lifting the spin degeneracy through the spin-orbit coupling, for instance, the enhanced upper critical field due to spin-valley locking and the mixing of the singlet and triplet pair states with the Majorana fermions at edge channels \cite{3,4,5,7}. Despite the considerable interest, the detailed effect of the inversion symmetry breaking on the superconductivity remains elusive because of the lack of the superconducting compounds, of which inversion symmetry breaking can be tuned by external parameters such as pressure.

Given the semimetallic band dispersion along with the inversion symmetry breaking and spin-orbit coupling, there may exist topologically protected crossing points at the vicinity of the Fermi level, which allows the emergence of the Weyl fermion as a low-energy excitation \cite{43,44,45}. Because of the fundamental importance and the technological potential, the search for a new Weyl semimetal (WSM) has currently become of great concern. Recently, transition-metal dichalcogenides T$_{\rm d}$-(Mo,W)Te$_{2}$ with inversion symmetry breaking have attracted much attention because of their potential to be a type-I\hspace{-.1em}I WSM, which is characterized by a pair of Weyl points connected by the gapless surface states called Fermi arcs \cite{35,10,32,36}. Furthermore, T$_{\rm d}$-(Mo,W)Te$_{2}$ show distinct electronic properties such as extremely large magnetoresistance and pressure-enhanced superconductivity, implying subtle sensitivity of the electronic state to external fields or pressure \cite{42,30,31}. To be noted here is that MoTe$_{2}$ shows a transition from a high-temperature nonpolar ($P2_{1}/m$) 1T' structure to the low temperature polar ($Pnm2_{1}$) T$_{\rm d}$ structure at $T_{\rm s}$ $\sim$250 K [see Fig. 1(c)] \cite{15}, which can be suppressed by external pressure or chemical substitution \cite{16, 22}. It has been reported that the superconducting transition temperature $T_{\rm c}$ of about 0.1 K in the polar phase increases to go beyond 5 K as the polar transition is suppressed by external pressure  \cite{16}. A similar enhancement of $T_{\rm c}$ upon the suppression of the polar structural distortion in MoTe$_{2}$ has been found by the S substitution for Te \cite{17}. Considering the fact that exotic superconductivity expected in the WSM state emerges only in the T$_{\rm d}$ (polar) phase \cite{46,47,48}, it is of vital importance to clarify the detailed relation between the polar structural transition and the superconductivity in MoTe$_{2}$, which remains elusive because of the difficulty in the physical property measurements under pressure.

In this Rapid Communication, we adopt not only the physical pressure but the chemical pressure, that is the Se substitution for Te, to establish the phase diagram of MoTe$_{2}$ as a function of temperature and pressure. Upon the application of physical and chemical pressures, $T_{\rm c}$ of 0.1 K in MoTe$_{2}$ increases significantly by a factor of more than 20 with replacing the T$_{\rm d}$ (polar) phase by the 1T' (nonpolar) phase. To clarify the role of the polar lattice distortion in the superconductivity, we measured the heat capacity and thermopower of the polar and nonpolar phases in Mo(Te$_{1-x}$Se$_{x}$)$_{2}$ and found that the superconductivity is sensitive to the subtle modification of the phonon dispersion or the Fermi surface topology. In addition, the importance of the interlayer coupling both on the structural and superconducting transitions in MoTe$_{2}$ is discussed from the viewpoint of the anisotropic lattice change under pressure.

Single crystals of MoTe$_{2}$ were prepared by the chemical vapor transport method as reported in Ref. \:\onlinecite{18}. Polycrystalline samples of Mo(Te$_{1-x}$Se$_{x}$)$_{2}$ with $x=0, 0.05, 0.1, 0.15, 0.2$ were synthesized by solid state reaction in evacuated quartz tubes. Further details of the experimental methods are provided in the Supplemental Material \cite{40}.

\begin{figure}[t]
\begin{center}
\includegraphics[width=7cm]{Figure1.eps}
\caption{(color online). (a),(b) The electrical resistivity for the single crystalline MoTe$_{2}$ at various pressures. Inset of Fig. 1(b) shows the electrical resistivity at pressures up to 0.46 GPa. The superconductivity at 0 GPa is suppressed by applying the magnetic field of 0.1 T as plotted by the gray line. (c) Phase diagram of the crystal structure and superconductivity. Red and blue circles represent the structural transition temperature $T_{\rm s}$ and superconducting transition temperature $T_{\rm c}$, respectively. Inset shows the crystal structure of the T$_{\rm d}$ (polar) phase and the 1T' (nonpolar) phase.}
\end{center}
\end{figure}

Figures 1(a) and 1(b) show the temperature dependence of $\rho$ for the single-crystalline MoTe$_{2}$ at various pressures. The residual resistivity ratio (RRR$\sim $ 60) is larger than that of Ref. \:\onlinecite{16} (RRR$\sim$ 36), ensuring the quality of our single crystal. At ambient pressure, the $\rho$-$T$ curve shows the anomaly reflecting the structural transition at $T_{\rm s}$ $\sim$250 K as well as the zero resistivity indicating the superconducting transition at $T_{\rm c}$ $\sim$0.1 K. With increasing pressure, $T_{\rm s}$ decreases so that it becomes zero at the critical pressure $P_{\rm c}$ of 0.75 GPa, whereas $T_{\rm c}$ increases systematically with increasing pressure up to 1.3 GPa. The point here is that the slope of $T_{\rm c}$ as a function of $P$ is maximized ($dT_{\rm c}/dP\sim$ 4 K/GPa) at the vicinity of the critical pressure $\leq P_{\rm c}$ (0.27 GPa $\leq P \leq$ 0.75 GPa) separating the T$_{\rm d}$ phase and the 1T' phase at the lowest temperature. Note that $T_{\rm c}$ changes significantly but continuously around $P_{\rm c}$. The smeared increase in $T_{\rm c}$ with increasing $P$ may reflect the fact that the structural transition is of the first order, giving rise to the phase coexistence at low temperatures at the vicinity of $P_{\rm c}$. \cite{22}

\begin{figure}[t]
\begin{center}
\includegraphics[width=7cm]{Figure2.eps}
\caption{(color online). (a) The Seebeck coefficient and (b) resistivity for the polycrystalline samples of Mo(Te$_{1-x}$Se$_{x}$)$_{2}$ below 4 K. (c) Phase diagram of the structure and superconductivity. Structural transition temperature $T_{\rm s}$ (red circles) and superconducting transition temperature $T_{\rm c}$ (blue circles) are determined by the Seebeck coefficient and resistivity, respectively.}
\end{center}
\end{figure}

The relation between the polar structural instability and superconductivity is also studied by the Se substitution for Te, which can be regarded as a chemical pressure effect as will be discussed later. Mo(Te$_{1-x}$Se$_{x}$)$_{2}$ with $0\leq x\leq0.2$ crystallizes in the monoclinic 1T' structure at room temperature. As shown in Fig. 2(a), a weak anomaly corresponding to the structural transition at $T_{\rm s}$ is discernible in $S$ $(T)$ for Mo(Te$_{1-x}$Se$_{x}$)$_{2}$ with $0\leq x\leq 0.05$, which is smeared in $\rho$ $(T)$ but discernible by x-ray diffraction at low temperatures (see Fig. S1 in the Supplemental Material) \cite{40}. Regarding the $x$ dependence of $S$, the magnitude of $S$ at room temperature tends to decrease with increasing $x$, while $T_{\rm s}$ remains constant. The temperature dependence of $\rho$ below 4 K for the polycrystalline Mo(Te$_{1-x}$Se$_{x}$)$_{2}$ is shown in Fig. 2(b). The compound with $x=0$ shows the decrease of $\rho$ around 0.3 K, which is reminiscent of superconductivity. For the compounds with $0.03\leq x\leq 0.2$, the superconductivity emerges at $T_{\rm c}$ above 0.3 K. From the result of $\rho$ $(T)$ and $S$ $(T)$, the structural and superconducting phase diagram of Mo(Te$_{1-x}$Se$_{x}$)$_{2}$ is obtained as shown in Fig. 2(c). Interestingly, $T_{\rm c}$ increases significantly as the T$_{\rm d}$ phase is replaced by the 1T' phase, just like the case in MoTe$_{2}$ under physical pressure.

\begin{figure}[t]
\begin{center}
\includegraphics[width=7cm]{Figure3.eps}
\caption{(color online). (a) Temperature dependence of upper critical field $H_{\rm c2}$ for $x=0.2$. The red curve is the best fit of the equation $H_{\rm c2}=H^{*}_{\rm c2}(1-T/T_{\rm c})^{1+\alpha }$ to the experimental data. The inset shows the temperature dependence of the resistivity under magnetic fields up to 7 T. (b) $T^{2}$ dependence of $C_{\rm p}/T$ of polycrystalline samples of $x=0$ (black circles) and $x=0.2$ (green circles). The red dotted line shows the fitting of the experimental data with the equation $C_{\rm p}/T=\gamma +\beta T^{2}$.}
\end{center}
\end{figure}

To get insight into the superconducting properties in the 1T' phase, we measured $\rho$ for Mo(Te$_{1-x}$Se$_{x}$)$_{2}$ with $x=0.2$ under various external magnetic fields $H$ as shown in the inset of Fig. 3(a). The change in the zero-resistance-point $T_{\rm c}$ with increasing $H$ is summarized as the phase diagram of the upper critical field $H_{\rm c2}(T)$ in Fig. 3(a). The curve of $H_{\rm c2}(T)$ becomes concave upward close to $T_{\rm c}$ ($H=0$), which deviates from the one expected from the Werthamer-Helfand-Hohenberg theory based on the single-band model. A similar behavior has been reported for 1T'-(Mo,W)Te$_{2}$ under high pressure and 2H-NbSe$_{2}$ \cite{16,29,30}.

Next, we compare the normal state properties of polar and nonpolar phases in Mo(Te$_{1-x}$Se$_{x}$)$_{2}$ with $x=0$ and $x=0.2$, respectively. To analyze the phonon properties and electronic density of states, we measured the temperature dependence of the specific heat $C_{\rm p}$. Figure 3(b) shows $C_{\rm p}/T$ as a function of $T^{2}$ above 2 K. The data of the polar ($x=0$) and nonpolar ($x=0.2$) samples are almost identical with each other, suggesting that both samples have similar Sommerfeld constant $\gamma $ and Debye temperature $\Theta _{\rm D}$. $\gamma $ and $\Theta _{\rm D}$ are evaluated using the equation $C_{\rm p}/T=\gamma +\beta T^{2}$ ($\beta$ is the lattice contribution to the specific heat), which yields $\gamma = 3.7$ mJ/mol K$^{2}$ and $\beta=0.923$ mJ/mol K$^{4}$. $\Theta _{\rm D}$ can be calculated with $\beta=(12/5)\pi ^{4}NR\Theta _{\rm D}^{3}$ ($R=8.314$ J/mol K and $N=3$) to be $180$ K.

Here we discuss the possible origin of the large enhancement of $T_{\rm c}$ upon the structural transition from the polar to the nonpolar phase in Mo(Te$_{1-x}$Se$_{x}$)$_{2}$. Using the evaluated $\Theta _{\rm D}$, the electron-phonon coupling strength $\lambda _{\rm p}$ can be calculated with the equation of the McMillan formula \cite{24,25},
\begin{equation}
\begin{aligned}
\lambda _{\rm p}=\frac{\mu^{*} {\rm ln}(1.45T_{\rm c}/\Theta _{\rm D})-1.04}{1.04+{\rm ln}(1.45T_{\rm c}/\Theta _{\rm D})(1-0.62\mu^{*})}.
\end{aligned}
\label{eq:ep2}
\end{equation}
By assuming the Coulomb pseudopotential $\mu ^{*}=0.1$ (commonly accepted value), $\lambda _{\rm p}$ is evaluated to be 0.31 and 0.52 for $x=0$ and $x=0.2$, respectively.
These values are similar to that in Ref. \:\onlinecite{17}, indicating that both compounds are weak-coupling superconductors.
In general, $\lambda _{\rm p}$ can be qualitatively expressed as
\begin{equation}
\begin{aligned}
\lambda _{\rm p}=\Sigma _{\rm i}\frac{\average{I^{2}_{\rm i}}D_{\rm i}(E_{F})}{M_{\rm i}\average{\omega ^{2}_{\rm i}}},
\end{aligned}
\label{eq:ep2}
\end{equation}
where $\average{I^{2}_{\rm i}}$, $D_{\rm i}(E_{\rm F})$, $M_{\rm i}$, and $\average{\omega ^{2}_{\rm i}}$ are the mean-squared electron-phonon coupling matrix element averaged over the Fermi surface, electronic density of states at the Fermi surface, atomic mass, and averaged squared phonon frequency of $i$th atoms in the unit cell, respectively \cite{26,27,28}. Since $\gamma$ and $\Theta _{\rm D}$ estimated from the specific heat measurements remain almost intact upon the Se doping, $D_{\rm i} (E_{\rm F})$ and $\omega_{\rm i}$ seem to be less dependent on the crystal structure and Se content $x$. In fact, the structural transition between the 1T' and the T$_{\rm d}$ phases has little impact on $D_{\rm i} (E_{\rm F})$ as confirmed by the first-principles calculations (see Fig. S2 in the Supplemental Material) \cite{40}. As for the contribution to $\lambda _{\rm p}$ from the atomic mass, the reduction of $M_{\rm i}$ from 351.14 g/mol ($x=0$) to 331.7 g/mol ($x=0.2$) by the Se substitution is too small to be considered. Given the positive correlation between $\lambda _{\rm p}$ and $T_{\rm c}$, it is presumable that the enhancement of $T_{\rm c}$ upon the transition from the T$_{\rm d}$ to the 1T' phase is associated with the increase in $\average{I^{2}_{\rm i}}$. The change in $\average{I^{2}_{\rm i}}$ accompanied by the structural change may be attributed to the modification of band topology. As shown in Fig. 2(a), the possible change in the band topology is supported by the sign change in $S$ at low temperatures for Mo(Te$_{1-x}$Se$_{x}$)$_{2}$ at $x=0.1-0.15$. Given that the Se ion and the Te ion are isovalent, the change in $S$ by the Se substitution is attributable not to the shift in the chemical potential but to a subtle change in the semimetallic band structure near the Fermi level. Thus the change in the topology of the semimetallic band structure is worth considering as a factor for the reduction of $\average{I^{2}_{\rm i}}$.  To see whether or not the change in the band topology is associated with the spin splitting, further experiments such as spin-polarized photoemission spectroscopy are necessary.

On the other hand, $\lambda_{\rm p}$ can be calculated using the Eliashberg electron-phonon spectral function $\alpha^{2}F(\omega )$, expressed as $\lambda _{\rm p}=\int_{0}^{\infty }$d$\omega \alpha^{2}F(\omega )/\omega $. Recently, it has been reported that a transverse acoustic phonon mode corresponding mainly to the Te-Te interlayer vibrations in the 1T' phase of WTe$_{2}$ has a significant contribution to $\lambda_{\rm p}$ through the large density of $\alpha^{2}F(\omega )$\cite{50}. This result suggests that the small change of the interlayer distance and/or the softening of the interlayer Te-Te vibration modes upon the polar to nonpolar structure transition substantially affect $T_{\rm c}$ in MoTe$_{2}$ as well, even if the overall phonon modes remain almost the same \cite{41,49}. The significant correlation between the interlayer distance and the superconductivity is discussed below.

While the qualitative features of the superconductivity under physical and chemical pressure are similar in the sense that $T_{\rm c}$ in the 1T' phase is much higher than that in the T$_{\rm d}$ phase, there are quantitative differences with regard to the changes in $T_{\rm s}$ and $T_{\rm c}$ as a function of each pressure as shown in Figs. 1(c) and 2(c). As the physical pressure on MoTe$_{2}$ increases, $T_{\rm s}$ decreases monotonically, unlike the case for the chemical pressure, under which $T_{\rm s}$ remains almost the same. In addition, as compared with the chemical pressure, the physical pressure enhances $T_{\rm c}$ by a larger extent at the vicinity of $P_{\rm c}$.

\begin{figure}[t]
\begin{center}
\includegraphics[width=7cm]{Figure4.eps}
\caption{(color online). (a) Unit cell volume $V$ divided by number of atoms per unit cell $Z$, (b) $ab$ plane area ($ab$), and (c) interplane distance as a function of $x$ for 1T'-Mo(Te$_{1-x}$Se$_{x}$)$_{2}$ and physical pressure $P$ for 1T'-MoTe$_{2}$. The lattice parameters as a function of $P$ are taken from Ref. \:\onlinecite{16}.}
\end{center}
\end{figure}

To elucidate the possible origin of the difference between the two phase diagrams, we compare the lattice parameters of MoTe$_{2}$ as functions of physical and chemical pressures. As shown by red circles in Fig. 4(a), the unit cell volume per formula unit ($V/Z$) for Mo(Te$_{1-x}$Se$_{x}$)$_{2}$ decreases linearly with increasing $x$, indicating that the Se substitution for Te acts as the chemical pressure. Here, the theoretical unit cell volume under physical pressure calculated in Ref. \:\onlinecite{16} is superimposed on that under chemical pressure, so that the effective pressure by the Se substitution can be estimated as, for instance, 6 GPa for $x=0.1$ (see the horizontal axes at the top and the bottom of Fig. 4). In the phase diagram of Mo(Te$_{1-x}$Se$_{x}$)$_{2}$, the T$_{\rm d}$ phase is completely suppressed by the Se substitution with $x$ somewhere in between 0.05 and 0.1. Thus $P_{\rm c}$ for the chemical pressure is estimated to be in the range 3-6 GPa, which is significantly larger than $P_{\rm c}$ ($<$ 1 GPa) for the physical pressure. This result indicates that the physical pressure is more effective to the suppression of the polar structural transition, which can be discussed from the viewpoint of the anisotropic lattice change. As shown in Fig. 4(b), the $ab$ plane area decreases steeply with increasing the chemical pressure, unlike the case for physical pressure. On the other hand, the interplane distance is strongly compressed not by the chemical pressure but by the physical pressure [Fig. 4(c)]. The large contraction of the interplane distance reflects the weaker interplane coupling as compared with the in-plane coupling with strong covalency in the layered transition-metal dichalcogenides\cite{31}. Considering the difference in the two phase diagrams and the lattice parameters, it is presumable that not only the modification of the band structure but also the enhancement of the three-dimensionality by the interlayer contraction may contribute to the enhancement of $T_{\rm c}$ around $P_{\rm c}$. It has been pointed out that the interlayer contraction increases the hybridization between the Te $p_{\rm z}$ orbitals, giving rise to the enhancement of the three-dimensionality \cite{39}. Given that the driving force for the polar lattice distortion is the enhancement of the interlayer hybridization which reduces the total electron kinetic energy, the physical pressure should suppress the energy gain associated with the polar distortion, leading to the decrease in $T_{\rm s}$ as seen in Fig. 1(c). Further supporting this assumption, the chemical pressure has little impact on the interlayer distance and $T_{\rm s}$ as seen in Figs. 4(c) and 2(c), respectively.

In conclusion, we establish the structural and superconducting phase diagrams of MoTe$_{2}$ as functions of temperature and the physical or chemical pressures. Both kinds of pressure, especially the physical pressure, significantly enhance $T_{\rm c}$ in the vicinity of the critical pressure $P_{\rm c}$, where the polar lattice instability disappears. From the anisotropic lattice changes under the physical and chemical pressures, the interlayer coupling is found to be a key parameter dominating both the structural and superconducting instability. Note that the chemical pressure, which has less influence on the interlayer coupling, enhances $T_{\rm c}$ as well as the physical pressure, implying that not only the interlayer distance but the polar lattice distortion has an impact on the superconductivity. The heat capacity and transport measurements on Mo(Te$_{1-x}$Se$_{x}$)$_{2}$ imply that the electron-phonon coupling is enhanced upon the polar-to-nonpolar transition. This work demonstrates the strong anticorrelation between the polar lattice instability and superconductivity in the Weyl semimetal candidate MoTe$_{2}$.

\section{ACKNOWLEDGMENTS}
The authors appreciate Y. Tokura and K. Ishizaka for their helpful suggestions.
This work is partly supported by JSPS, KAKENHI, Young Scientists B (No. 16K17736), JST PRESTO (Hyper-nano-space design toward Innovative Functionality), Asahi Glass Foundation and Grant for Basic Science Research Projects of the Sumitomo Foundation.

redpajama_set_name: RedPajamaArXiv


The Information Security DLP Program Lead will be primarily responsible for leading and developing Data protection services at Kiewit. This role acts as an expert for the DLP program including supporting the remote portions of the organization. By providing expertise, this role is jointly accountable for the implementation, leadership and oversight of the DLP programs and services. The role will help lead in determining risk measurement and level, risk mitigation approaches and implement effective solutions and governance functions. The lead is responsible for interpreting policy, implementing security safeguards that integrate into business workflows and provide input to the Kiewit information security program. This role will provide an excellent opportunity to liaise with key external and internal stakeholders while strengthening Information Security capabilities. The DLP Program Lead will work with our other Information Security teams to develop and enforce policies, procedures, and technical controls and supervise and develop the data protection services. This lead will be part of a cross-functional security risk team that gathers technical and procedural information, deploys necessary tools to test and validate IT infrastructure, identifies vulnerabilities, analyzes information derived from engagements to determine information security risks and provides remediation assistance. This role will report to the Information Security Manager.
• Accountable for the development, communication, implementation, reporting, maintenance and oversight of the DLP program and associated processes. Ensure alignment to approved standards and regulatory requirements/guidance.
• Develop roadmaps and deployment plans for technical solutions and related procedures in line with the information security program, in collaboration with internal (IT, legal, audit, business and other) and external stakeholders.
• Manage third party relationships relating to additional security services as required (e.g., service/control testing).
• Crosstrain on all other security platforms to gain proficiencies in those tools and platforms.
• Assist in responses to internal and external compliance audits, penetration tests and vulnerability assessments.
• Demonstrated Customer service supporting the overall customer experience.
• Strong oral and written communication skills with ability to understand technology sufficiently to clearly communicate the complexity in simple terms to bring clarity for key stakeholders.
• Experience in information technology related positions with working knowledge of IT infrastructure, networks, databases, processing systems, web applications, mobile technology, cloud, big data, software development, API's, and virtualization.
• Demonstrated success delivering complex technology projects with an emphasis on high customer satisfaction.
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Other common names for this role: Security Analyst, DOP Specialist, etc.


text:
Q: Basic Elixir OTP server behaves oddly I have this code which is a basic OTP server:
defmodule Clients do
use Application
require Logger

def stuff do
    Logger.debug "Clients.start/0"
   # {:ok, pid} = Task.Supervisor.start_child(Clients.TaskSupervisor, fn -> doclient end)
end

def doclient(port) do
    Logger.debug "Clients.doclient/0"

    {:ok, socket} = :gen_tcp.listen(port,[:binary, packet: :line, active: false, reuseaddr: true])

#if this is under 2000ms there the process exits with a shutdown error
    :timer.sleep(1500)

end

def start(_type, _args) do
    import Supervisor.Spec
    Logger.debug "Clients.init/1"

    children = [
        supervisor(Task.Supervisor, [[name: Clients.TaskSupervisor]]),
        worker(Task, [Clients, :doclient, [4040]])
    ]
    opts = [strategy: :one_for_one, name: Clients.Supervisor]
    Supervisor.start_link(children, opts)
end

end

The output from iex is:
iex(1)> Clients.start(1,2)

20:07:19.879 [debug] Clients.init/1

20:07:19.889 [debug] Clients.doclient/0
{:ok, #PID<0.141.0>}
iex(2)>
20:07:21.402 [debug] Clients.doclient/0

20:07:22.909 [debug] Clients.doclient/0

20:07:24.413 [debug] Clients.doclient/0
** (EXIT from #PID<0.139.0>) shutdown

If the doclient/1 timer call is under 2 seconds the above shutdown occurs but otherwise it ticks away happily. I'm not sure why? If I want doclient/1 to execute some arbitrary code that will take less than 2 seconds (which is not I imagine a reliable period anyway) this call will always explode.

A: You are using Task as your worker. So what happens is that once Task wakes up from the sleep it finishes its work and that process goes away. In your supervisor spec you are requesting:
children = [
  supervisor(Task.Supervisor, [[name: Clients.TaskSupervisor]]),
  worker(Task, [Clients, :doclient, [4040]])
]
opts = [strategy: :one_for_one, name: Clients.Supervisor]
Supervisor.start_link(children, opts)

which tells OTP to restart your worker if it finishes or goes away in any way. So after 1.5 seconds (your time to sleep) the supervisor starts another task. It does this 3 times in the span of 5 seconds.
Supervisor.start_link has default options that specify intensity of restarts. Per the docs on Supervisor.Spec.supervise/2, the defaults are max 3 restarts in 5 seconds. That is why your supervisor shuts down with sleep time of 1.5 seconds and happily keeps on going with interval of 2 seconds.
All in all I think you need to rethink the use of tasks in this supervision tree. It is impossible to guess what fits best for your use case since you did not mention what it is.
HTH


Williamsburg-based Crème has designed some of the most intriguing restaurants in New York City—L'Amico (shown), RedFarm, Irvington, and Marc Forgione, to name a few. "When we design a restaurant, we feel we are telling a story, which is much stronger when each layer has the same thread—whether it's lighting, landscaping, or graphic design for menus and business cards," says Aizaki. "Every layer helps tell the same story." The studio's latest projects include the renovation of the historic Miami property the Greystone Hotel, and the transformation of a neglected Denver alleyway into a space for alfresco dining, public art, and studios for local artisans. "We saw a city block and breathed life and soul into it," says Crème design director Jose Achi.
CREME's display design for The Wonder 500 Exhibit is featured in this month's All About Japan.
L'Amico restaurant designed by CRÈME featured in Architectural Digest's 12 Most Stylish Restaurants in New York City.
Mr Purple featured on Winter Rooftops on NBC New York. Click here to check it out!
L'Amico was featured and reviewed in this week's Time Out New York.
Headed by Brooklyn-based design firm Crème Design, the project includes a new black steel façade, living room lobby concept, and upgraded F&B options led by James Beard Award nominee Laurent Tourondel and Michelin-starred George Mendes.
Creme founder Jun Aizaki talks food and restaurant design in this month's Hospitality Design Backspace article. Read the full article here.
Brooklyn, New York-based Crème Design has completed the Mr. Purple rooftop bar and restaurant for the Hotel Indigo Lower East Side New York.
Located on the hotel's 15th floor, the indoor-outdoor F&B outlet is the Gerber Group's first downtown property and nods to the neighborhood with locally inspired dishes, loft-like interiors, and a creative concept based on Mr. Purple—a fictitious local artist who is a mysterious and free-spirited loner.
The recently opened L'Amico restaurant is featured in the November 2015 print issue of Architectural Digest.
Our design for Lupulo is featured in Interior Design Magazine as one of the 12 NYC Restaurants that serve up Hot Design.
Check out the full feature and more images on Interior Design.
Check out our various designed spaces at the Eventi Hotel in New York City's Chelsea district.
L'Amico, our newly designed Italian restaurant at the Eventi Hotel has just opened.
We are super excited to have our latest retail project featured on Cool Hunting!
Lupulo, Crème's latest collaboration with Chef George Mendes, gets reviewed by the New York Times.
We were so excited to be involved in the branding of the new pop-up restaurant at the High Line Hotel – Alta Linea. Crème designed the identity including brand manual, logos, menus and coasters. The space is open for the summer, we hope you visit!
Irvington, our latest project with the W Hotel and Gerber Group, was profiled for New York Spacer mag.
Our founder Jun Aizaki was recently profiled for Metropolis Mag in a feature titled "Just Getting Started".
Jun Aizaki talked to Culintro about Crème's most recent projects, the studio and working in hospitality design.
Jun Aizaki talks to Tim McKeough from the New York Times about the use of screens as room dividers.
Since he founded Crème Design in 2004, Jun Aizaki has designed dozens of restaurant interiors, including Red Farm and Danji in Manhattan, JG Domestic in Philadelphia, and multiple locations for Distrito. Each space is different, but most share a theme: the use of screens as sculptural room dividers.
Farm-to-table Chinese inspired restaurant on the West Village gets reviewed on Fine Design.


Nories are proud to present the New Nories BTS 4.5". This Big Tail Shad has the combination of a realistic bait fish shape and appearance, with a large thick tail to maximise the reaction bite. The big tail thumps through the water to produce a mighty wave at any retrieve speed and let fish know of it's presence. And with it's natural rolling wobbles it makes it even more attractive to your target species.
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Nories BTS 4.5" can be fished unweighted to work the top column of water or with many other jigs and rigs which makes this lure extremely versatile for many species and every situation. Use hook sizes from 2/0 to 5/0.
Nories BTS is effective on a wide range of predatory fish, such as Mangrove Jack, Bass, Flathead, Mulloway and most Rockfish.


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Fillmore County broadband expansion proposals
November 15, 2021 by Karen Reisner Leave a Comment
Three broadband providers outlined their proposals at the Fillmore County board's November 9 meeting.
The county has received $4.2 million in American Recovery Act funding. Broadband providers are looking for a portion of this funding to support broadband projects within the county. Much of Fillmore County is still underserved.
Corey Hauer, LTD Broadband, said they have been a provider in the county for nine years. Fixed wireless is limited by hills and trees. He said we have been successful getting federal funding for fiber optic cable. Recovery Act funding could allow us to add additional unserved and underserved areas in one or two years. He estimated it takes $5,000 per household to bring fiber to areas with a low density of households. County dollars could allow them to build quicker in rural areas.
Jill Huffman, CEO of Harmony Telephone/MiBroadband, said they are a cooperative partnership dedicated to the expansion of broadband. There is a significant need in Fillmore County for residents and businesses. Build-outs in rural areas are expensive with return on investment being very long term. Step one is to build it, and then to support it and make it run smoothly. Northern and western portions of the county have very limited household density. She detailed two project areas that could be expanded with the support of state and county dollars. Huffman made it clear she welcomes ideas and is willing to consider all funding options to expand project areas. They are looking at all future funding options at federal, state, and local levels. She suggested projects could be completed in two construction seasons. Huffman expects it will cost more than $5,000 per household in low density areas. She concluded stressing that the installation of fiber will greatly impact the future economic growth in the county.
Zachary Raskovich, Mediacom Communications, has been with Mediacom for 15 years. The Mediacom system makes service available to 6,200 homes and businesses. Mediacom recently built out broadband in the city of Fountain, sharing project costs about 50-50 with a Minnesota DEED Grant. Mediacom is now constructing 4.3 miles of fiber to bring service to 246 homes and businesses in Wykoff. The total investment is 100% paid for by Mediacom and is expected to launch in March 2022. Mediacom is prepared to invest in the city of Ostrander to serve 155 homes and businesses, roughly 3.5 miles of construction. Raskovich requested a county grant in the amount of $50,000 (using American Recovery Act funds) for this project or roughly 16 percent of the total project cost.
AcenTek is expected to present their proposal at the next board meeting on November 23.
Other business in brief
• Sheriff John DeGeorge asked for and received approval for a quote from Enterprise Fleet Management to purchase a 2022 Dodge Charger AWD unmarked squad car. The vehicle will be assigned to an investigator and will replace a 2016 unmarked Dodge Durango. Some equipment will be transferred. Approval was given to equip and setup the unmarked squad car at a cost of $5,528.73.
The next steps to be taken to possibly build a new jail facility were discussed. DeGeorge said he would reach out to the Howard County people to learn what process they used in planning and designing their jail. Committee members will check into what steps need to be taken to satisfy legal requirements in finding and selecting a qualified architect.
• Christy Smith, Auditor/Treasurer, explained 12 parcels in tax forfeiture are mostly located within a city or are very small parcels. They have been reviewed and determined to be non-conservation property. Approval was given classifying all the tax-forfeited land parcels as non-conservation property. A resolution of Tax Forfeiture Land Classification was approved.
The tax forfeited properties will be offered at public auction to be held on March 1, 2022 at 1 p.m.
Each commissioner will set a minimum sale price for each tax forfeiture property in their district by November 23. Once the minimum sale prices are set, cities and townships will have 60 days to consider if they want to purchase a property or acquire it for a public use. Minimum bids will be considered for approval at the November 23 board meeting.
• County Engineer Ron Gregg requested and received approval to advertise for a bridge replacement project in Arendahl Township using Local Option Sales Tax (LOST) funding.
Approval was given to advertise for the surface reconditioning project on CSAH 30, from Highway 139 for a 2.5 mile section to Niagara Cave.
• The temporary employment of Bryant Bollman as a transfer station attendant for the sanitation department from November 3 through November 17 was approved.
The hire of a .08 FTE Public Health Nurse, Carrie Boyum, effective November 30 was approved.
• Jessica Erickson, director of nursing, asked for and received approval for electrical work to add a panel for additional outlets. Haakenson Electric, Inc. will do the work. The total cost is to be $3,569.53 and will be paid for with a COVID grant.
Approval was given of "Reflective Practice" monthly employee contact to prevent fatigue and burn out to be funded by a workforce grant. This is to go into effect once the grant is accepted.
• Anne Koliha, SWCD, said the County Feedlot Program Delegation Agreement Work Plan for 2022-2023 is similar to the plans of the last few years. Funding next year will be based on 597 feedlots. Feedlots have to be registered every four years. The Pollution Control Agency has approved the work plan. The plan was approved by the board as presented.
The Delegated County Feedlot Grant Agreement with the state was approved. The agreement is for four years, 2022-2025. The amount of the grant is based on 597 feedlots.
• The 2022 and 2023 State of Minnesota Board of Water and Soil Resources Natural Resources Block Grant Agreement in the amount of $70,096 was approved. Funds are delegated to grant programs including shoreland, septic treatment systems, local water management, and wetland conservation.
• A request to advertise for proposals for copy machines was approved. The county has machines on a five-year lease.
• Approval was given for a list of delegates and policy committee members for the upcoming Association of Minnesota Counties annual meeting and for the Minnesota Counties Intergovernmental Trust (MCIT) voting delegates for 2021.
Filed Under: Business, Government, News Tagged With: Fillmore County
About Karen Reisner
karen@fillmorecountyjournal.com
Governor - TIM WALZ
130 State Capital
75 Rev. Dr. Martin Luther King Jr. Blvd.
mn.gov/governor/
U.S. Representative - JIM HAGEDORN
hagedorn.house.gov
U.S. Senator - AMY KLOBUCHAR
www.klobuchar.senate.gov/public
U.S. Senator - TINA SMITH
www.smith.senate.gov
State Representative - GREG DAVIDS
rep.greg.davids@house.mn
State Senator - JEREMY MILLER
sen.jeremy.miller@senate.mn
Government this week
• Houston County Commissioners, Work Group, Courthouse
Board Room, 9:30 a.m.
• Caledonia School Board, MS/HS Auditorium, 6 p.m.
• LeRoy-Ostrander School Board, Board Room, 6 p.m.
• Mabel-Canton School Board, Media Center, 6 p.m.
• Preston City Council, Council Chambers, 6 p.m.
• Spring Grove City Council, Fest Building, 6 p.m.
• Grand Meadow School Board, Choir Room, 7 p.m.
• Rushford Village City Council, Village Hall, 7 p.m.
• Kingsland School Board, Elementary Conference Room, 6 p.m.
• Lanesboro School Board, Forum Room, 7 p.m.
• Caledonia City Council, City Hall, 6 p.m.
• Rushford City Council, City Hall, 6:30 p.m.
• Chatfield City Council, City Hall, 7 p.m.
*Schedule subject to change.