At the House of Cheviot, we combine traditional hand knitting skills developed over 200 years with the very latest knitting technology, to produce the best country socks, kilt hose, and shooting socks available. During manufacture, from the careful selection of yarns to the final hand-finishing, House of Cheviot products pass through many pairs of skilled hands, providing attention to every detail on every step of the craft making process, and thus ensuring that all of our finished socks are of the highest standard.
To safeguard the premium quality of our hosiery we choose only the best yarns from around the world which meet our criteria of versatility, longevity and next to skin comfort.
Our cashmere socks are made from the softest cashmere yarn combed annually by goats living in the high plateaus of Mongolia and Northern China, whilst our wool socks consist of the finest wool in the world - Australian Merino Wool.


The prime booking season for Alaska cruises and cruise tours generally lasts from December through March. I'd like to cover four key factors to keep in mind when planning a visit to America's last frontier: itinerary, weather, wildlife and passports.
There are two types of itineraries for Alaska cruises: Inside Passage cruises that sail round trip from Vancouver, Seattle or San Francisco; and Gulf of Alaska cruises that sail one way between Vancouver and Seward or Whittier (gateways to Anchorage and the interior city of Fairbanks). The Gulf of Alaska cruises include several days in the Inside Passage.
The round-trip cruises offer two advantages: 1) There are many flights daily into, and out of, Vancouver, Seattle and San Francisco, and 2) They require less expensive airfare because no long flight to (or from) Anchorage or Fairbanks is involved.
Air into (and out of) Anchorage and Fairbanks is quite limited and flights fill early with cruise and cruise tour passengers, which makes it more risky to wait for a last-minute deal on a one-way Gulf of Alaska cruise.
The biggest advantage of one-way cruises is that they allow the opportunity to explore the interior of Alaska on a pre- or post-cruise land tour. Between one-third and one-half of all Alaska cruisers extend their cruise with a tour of inland Alaska (out of Anchorage or Fairbanks) or British Columbia or the Canadian Rockies (out of Vancouver).
If you are leaning toward one of these cruise tours, keep in mind that tour buses, railcars and lodges in Alaska are very limited in supply and can sell out early. I recommend booking soon to ensure availability.
Alaska weather is delightfully unpredictable, but in general, you'll find the warmest temperatures in July and August, when average highs are in the low to mid-60s. Precipitation can rise a bit in late August and early September, but I personally would not avoid that time for that reason.
One of my fondest Alaska memories is of sipping coffee on the cabin balcony as the scenery melted away and the ship slowed to a crawl in dense fog in the Inside Passage, its foghorn echoing off the mountains on either side, warning fishermen of our approach. On another day, we hiked a trail to an alpine lake for a canoe ride to the face of a glacier, in a driving rain. Invigorating does not begin to describe it. Weather is part of the experience in Alaska.
Click here for a list of Alaska ports, and then click a port name to see the weather details for that location.
Wildlife is one of the big attractions of Alaska, and different species are active at various times during the cruising season. Humpback and killer whales are seen throughout the summer in large sounds and straits along the coast as they migrate between their winter homes in the south and their summer homes in the north. Brown and black bears can be spotted in grassy tidal flats starting in May and near salmon streams and berry patches in July and August. Moose and caribou begin calving in May, so look for cow moose and their young near thickets along roadsides and rivers in May and June.
Bald eagles are plentiful and can be viewed at the water's edge through the summer, particularly near salmon-spawning streams. Tufted puffins and other seabirds begin nesting colonies on coastal islands in May. Shorebird-watching is popular in August and September as various species begin their migrations south for the winter.
Harbor seals are visible throughout the season and can be seen with their pups on and around the icebergs of Tracy Arm and Glacier Bay during the month of June. Sea lions start to become visible in September.
Fishermen will be happy to know that at least one variety of salmon -- the prized king salmon -- runs from May through August. Late May through June is the best time for saltwater king salmon fishing, and July through August is best for freshwater king salmon fishing. Sockeye (red) salmon fill freshwater streams and rivers on their spawning run from late June through July.
Saltwater fishing for chum and pink salmon is best in July and August, and freshwater fishing for these species is at its peak in August. Coho (silver) salmon can be found in saltwater areas from late July through early September and are abundant in freshwater areas during September and October. Halibut is most plentiful in saltwater areas from late June through August.
Passports are required for all travelers who enter or re-enter the U.S. by air from any other country, which means that U.S. citizens and residents who fly back to the U.S. from Vancouver or any other Canadian city after an Alaska cruise or cruise tour are required to have a valid passport.
Passports also are required for anyone who enters or re-enters the U.S. by land or by sea. There are a few exceptions to the passport requirement pertaining to land and sea border crossings.
First, U.S. citizens on cruises that begin and end in the same U.S. port and travel to destinations in Canada (and select other countries) are able to re-enter the U.S. with proof of citizenship other than a passport, such as a birth certificate and government-issued photo ID. Passports are required for cruises that begin in one U.S. port and end in another.
So, U.S. citizens on cruises that sail round trip from Seattle or San Francisco are not required to have a passport. U.S. citizens who drive to Vancouver for a round-trip Alaska cruise or who cruise one way between Vancouver and an Alaskan port (such as Whittier or Seward) do need a passport.
Next, children under the age of 16 who are citizens of the U.S. or Canada are exempt from the passport requirement for land and sea border crossings. In lieu of a passport, children are able to use a birth certificate as proof of citizenship for entry into the U.S. by land or by sea. Children entering or re-entering the U.S. by air still are required to have a valid passport.
Finally, a lower-cost alternative to the passport, called a passport card, is acceptable for entries into the U.S. by land or sea. Compared to passports, which cost $135 for first-time applicants ($105 for children), passport cards cost just $55 ($40 for children). The passport card is not acceptable for air travel.
Even in cases where a passport is not required, Vacations To Go and all cruise lines recommend that passengers have them anyway. This is because, while highly unlikely, an emergency could arise in which a U.S citizen needed to disembark early and fly home from Canada, and a passport would be required for that flight.
Passports are required for citizens of all other countries for any Alaska cruise or cruise tour.
Is this your year to experience the incomparable natural beauty and majesty of Alaska and British Columbia? The bargain-hunting cruise counselors of Vacations To Go can help you find the perfect cruise at a great discount!


text:
Student, Library and Academic Services
Annette Coates
Annette is Head of Library Collection and Digital Services and manages the Collections, Discovery and Access, and Content Delivery and Copyright teams in the University Library. These teams provide print and digital services that ensure students, staff and researchers can discover and access resources they need to support their learning, teaching and research at Northumbria. These services include the Library Collection, Library Search, the University's Reading List service and the University Library online.
After graduating with a BA (Hons) in English Language and Literature from Hull University in 1994, Annette completed a postgraduate programme in Anglo-Saxon Studies at Newcastle University in 1997, followed by an MA in Information and Library Management at Northumbria in 1998.
She began her career in academic librarianship at Manchester Metropolitan University Library in 1998 and worked in a number of roles across the Library service in her 10 years there. She became part of the MMU Library's senior management team as Service Manager responsible for electronic service development in 2004.
Annette joined Northumbria University Library in 2009 and held the senior management roles of Digital Library Services Manager and Content Services Manager before becoming Head of Library Collection and Digital Services in 2015. In her career at Northumbria she has been responsible for working with colleagues across the University to lead several significant service changing projects, including the establishment of the University's Reading List service, and the University transformation project to change library management systems.
annette.coates@northumbria.ac.uk

redpajama_set_name: RedPajamaCommonCrawl


A plant manager must decide which contracts to take for his casting-press operation and the price to bid on a new GM water pump. In the process, jobs must be scheduled in regular time, overtime, and outsourcing, and the plant manager must consider uncertainty in volumes, costs, available uptime hours, and the uncertainty about winning the contract bid, which depends on price. Two student spreadsheet files are available for use with this case.


text:
The Allis-Chalmers D series is a line of tractors made by the Allis-Chalmers Manufacturing Company from 1957 to 1969.

D-series development
An industry trend toward higher horsepower tractors caused Allis-Chalmers to develop the all-new D series to replace earlier tractor lines. These tractors featured three-point hitches, power steering and diesel engine options. Low-compression fuel options for kerosene and distillate were dropped.

Most of the D-series tractors, except for the D21, had hand-operated, shift-on-the-go oil clutches, commonly referred to as a hand clutch. Allis-Chalmers marketed this arrangement as the "Power Director". This clutch was in low range when pulled back, neutral in the middle, and high range when pushed forward. It could also be ordered as a forward-reverser, called the "Shuttle Clutch".  This hand clutch also exists on the D21, but it was not meant for shifting on the go.

D14

The D14 was the first D-series model, introduced in 1957 as an all-new tractor. The engine was a new   Allis-Chalmers Power-Crater four-cylinder engine, available in  gasoline and LP gas fuels. The engine was coupled to a four-speed transmission with a transfer case, giving a total of eight forward gears and two reverse. High-clearance and rice cultivation models were produced, and orchard shield kits were available.  An adjustable wide front axle branded "Roll-Shift" was introduced with this model, which also offered a narrow front wheel pair and single wheel options. The D14 had a  gas fuel capacity, and  propane fuel capacity.  The D14 was made from 1957 to 1960, when it was replaced by the D-15. 17,474 units were made.

D15

The D15 succeeded the D14 in the Allis-Chalmers lineup from 1960 to 1968. The early D15 was essentially the same as the D14 with the same engine but a higher compression ratio and increased RPMs. The option of power steering was also made available. At serial number 9001 a larger engine was introduced, as well as a few other minor improvements. The D15 had a  fuel capacity for gas and diesel, and a  capacity for LP gas. Dual and single front wheels and an adjustable front row-crop axle were offered. 17,434 units were built during their production from 1960 to 1969, with a price of $3,000 in 1967.

The D15 Series II was introduced in 1963 with new  engines in diesel, gasoline and LPG, with about 15 more power for the gasoline and LPG models. Diesel was unchanged. Headlights were moved from the grille to the fenders.

The introduction of the Renault-built Model 160 ended the D15 Series II in 1969.

D17

In October 1957, the D-17 was introduced, followed by the D10 and the D12 in 1959, in which year Allis-Chalmers made as many as 50 model configurations of the D10, 12, 14, and 17.

The Model D17 was developed as a replacement for the WD45 as a four-plow tractor. The D17's styling closely followed the smaller D14. It was made in gas, diesel, and LPG versions, its  engine turned 2,000 rpm, and was tested at  belt and  drawbar. Adjustable wide front, narrow dual and single front wheel options were offered, as well as a high-clearance model with a single front wheel. Wheatland models with full rear fenders and orchard models with orchard shielding were developed as well. An even taller high-clearance version was offered for sugar cane work. Later years were designated Series II through Series IV, with minimal changes. 62,867 D-17s were produced during their 10-year run.  The diesel D17 had a six-cylinder engine with  and weighed about . The Allis-Chalmers 170 replaced the D17 in 1968.

D10

The D10 replaced the Model B and were not made with narrow front-ends. Their wide front ends were adjustable. Both models (D10 and D12) were tested at 28.5 belt and 25.8 drawbar horsepower and had  engines; the only difference between the two was that the D12 had longer front-axle sleeves and a wider front axle adjustment for wider rows. 5,304 D10s were made from 1959 to 1967.

D12

The D12 replaced the Model CA in 1959. 4,070 D12's were made in their 10-year run from 1959 to 1968. The D12 had a , four-cylinder,  gasoline engine that was tested in Nebraska at .

D19

The D19 was introduced in 1961 to suit the needs of larger farmers.  It was the first D-series tractor besides the diesel D17 to have a six-cylinder engine.  Its horsepower was:  gas;  propane, and  diesel.  Its displacement was . The diesel model was the first in the industry to come standard with a turbocharger, boosting both horsepower and fuel economy. 10,591 units were built, and they weighed . The D19 was manufactured until 1964. D19s were known for running smoothly and fairly quietly.

The D19 was popular among larger farmers in the 1960s, who had a higher acreage to manpower ratio than ever before. The D19 was able to pull a five bottom plow. It also came in a high-crop version with over three feet () of ground clearance.

D21
The D21 was introduced in 1963, and was the largest of the D series, as well as the first Allis-Chalmers tractor to exceed 100 horsepower and the largest row crop tractor available in the industry; rated at  with a  engine. The D21 was styled significantly different than the other D series with full fenders, a large platform, and a rear-mounted fuel tank which held , allowing an average of 10 hours of field work.  The D21 was not turbocharged until 1965, which pushed its horsepower up to about  as it remained the largest row crop tractor available. This gave the D21 over  of pull, making it the largest tractor Allis-Chalmers had ever made, as well as the most expensive at around 10,000 dollars.

Before this move to turbo, the D21 series I found itself outmoded by the Allis-Chalmers 190XT, which could be turned up to produce more power than the D21. The D21 was replaced in 1970 by the Model 210 and 220, also with a  engine, which was rated at  respectively. The D21 was a favorite for tractor pullers and still makes good showings at the pulls today.

See also

 List of Allis-Chalmers tractors
 List of Allis-Chalmers engines

References

 Vintage Farm Tractors by Ralph W. Sanders Google Books Result

Allis-Chalmers tractors

redpajama_set_name: RedPajamaWikipedia


text:
\section*{Abstract}
{\bf
Photonic materials are a rapidly growing platform for studying condensed matter physics with light, where the exquisite control capability is allowing us to learn about the relation between microscopic dynamics and macroscopic properties. One of the most interesting aspects of condensed matter is the interplay between interactions and the effect of an external magnetic field or rotation, responsible for a plethora of rich phenomena---Hall physics and quantized vortex arrays. At first sight, however, these effects for photons seem vetoed: they do not interact with each other and they are immune to magnetic fields and rotations. Yet in specially devised structures these effects can be engineered. Here, we propose the use of a synthetic magnetic field induced by strain in a honeycomb lattice of resonators to create a non-equilibrium Bose-Einstein condensate of light-matter particles (polaritons) in a rotating state, without the actual need for external rotation nor reciprocity-breaking elements. We show that thanks to the competition between interactions, dissipation and a suitably designed incoherent pump, the condensate spontaneously becomes chiral by selecting a single Dirac valley of the honeycomb lattice, occupying the lowest Landau level and forming a vortex array. Our results offer a new platform where to study the exciting physics of arrays of quantized vortices with light and pave the way to explore the transition from a vortex-dominated phase to the photonic analogue of the fractional quantum Hall regime.
}

\vspace{10pt}
\noindent\rule{\textwidth}{1pt}
\tableofcontents\thispagestyle{fancy}
\noindent\rule{\textwidth}{1pt}
\vspace{10pt}

\section{Introduction}
Many-body systems in the presence of synthetic magnetic fields offer the exciting opportunity of finding new topological phases of matter with fractional excitations~\cite{Halperin_PRL_84}---a holy-grail of condensed-matter physics and the pillar of topological quantum computing~\cite{Kitaev_AnnalsPhys_2003,Topo_Q_comput}. Beyond ultracold atomic gasses~\cite{Cooper_AdvPhys_2008, Goldman_RPP_2014, Artficial_gauge_field_Phys_today, Cooper_RMP_2019}, photonic systems seem to be an ideal platform for this purpose thanks to the exquisite capabilities state preparation and detection as well as direct access to correlations~\cite{Cho_PRL_2008, Umacalilar_PRL_2012, Kapit_PRX_2014, Maghrebi_PRA_2015, Angelakis_book_2017, Ozawa_RMP_2019, Carusotto_NatPhys_2020}. However, to achieve these exotic phases of light a challenging combination of strong interactions and synthetic magnetic fields is required. So far, only partial results have been obtained. On the one hand, strong effective photon-photon interactions are already routinely attained in a variety of photonic platforms including superconducting quantum circuits for microwave photons~\cite{Gu_PhysRep_2017, Ma_Nat_2019, Blais_arxiv_2020} or, in the optical regime, Rydberg polaritons~\cite{Maxwell_PRL_2013}, and are underway in exciton-polaritons~\cite{Togan_PRL_2018, Rosenberg_SciAdv_2018, Delteil_NatMat_2019, Munoz_NatMat_2019}. On the other hand, considerable effort has been devoted to engineering synthetic magnetic fields for light by various approaches~\cite{Lu_NatPhoton_2014, Ozawa_RMP_2019}; for example, by including magnetic materials in microwave- and telecom-frequency cavities~\cite{Raghu_PRA_2008, Wang_Nat_2009, Bahari_Science_2017}, by Floquet engineering~\cite{Rechtsman_Nat_2013} or by carefully designing non-trivial lattice geometries~\cite{Hafezi_NatPhoton_2013, Rechtsman_NatPhoton_2013, Bellec_LightSciAppl_2020, Jamadi_strained_graphene2020}. Yet, even though there has been one successful attempt in creating few-body photonic Laughlin states~\cite{Clark_Nat_2020}, combining interactions with synthetic fields in a scalable platform for many-photon states is still needed.

In this work we propose a method to stabilize a non-equilibrium Bose-Einstein condensate of polaritons into a rotating state generated by a synthetic magnetic field. We make use of the recently developed platform of strained honeycomb lattices. Based on the idea of a strained graphene layer~\cite{Castro_RMP_2009,Guinea_NatPhys_2010}, a lattice of photonic resonators can be carefully designed to have a spatial gradient in its hopping strengths. The synthetic strain induces a synthetic magnetic field which has opposite sign in each of the two Dirac valleys of the honeycomb lattice, leading to the formation of Landau levels in the middle of the energy spectrum~\cite{Salerno_2DMater_2015, Salerno_PRB_2017} (see Fig.\ref{fig: lattice}). The first evidence of Landau level quantization in a strained honeycomb lattice for photons was obtained in coupled dielectric optical waveguides~\cite{Rechtsman_NatPhoton_2013}, and more recently, the photonic $n=0$ Landau level wavefunction was directly imaged in a lattice of macroscopic microwave resonators ~\cite{Bellec_LightSciAppl_2020} and of coupled semiconductor micropillar cavities~\cite{Jamadi_strained_graphene2020}.

\begin{figure*}[ht!]
\centering
  \includegraphics[width=0.8\textwidth]{figure1.pdf}
  \caption{\textbf{Honeycomb lattice and single-particle spectrum.} \textbf{a, b} Sketch of the unstrained (left) and strained (right) honeycomb lattices. We use bearded terminations in the $x$ direction and armchair ones in the $y$ direction. A generic strain is encoded in the $x$-dependent hopping strength along the horizontal links $t_1(x)=t(1+\tau x/3d)$ and is graphically indicated as a gradient in the link's length in \textbf{b}. Hopping along the other links is constant $t_{2,3}=t$ and $\tau$ is the strain magnitude. \textbf{c} The single-particle 1D energy bands of the unstrained and strained lattices with periodic boundary conditions along $y$. The color indicates the mean $x$-position of the eigenstates, $\bra{\phi}\hat x\ket{\phi}$. Cyan corresponds to the (L)eft edge of the lattice and magenta to the (R)ight. The Landau levels $n=0,\pm1$ are labeled in the spectrum of the strained lattice.}
\label{fig: lattice}
\end{figure*}

We theoretically anticipate that, thanks to the competition between drive and decay, a robust polariton condensate can be stabilized in the the $n=0$ Landau level using an incoherent pump which selects a single sublattice. The properties of the steady state are determined by the interplay between interactions and the synthetic magnetic field. The Dirac valley symmetry is spontaneously broken via the nonlinearity which comes from polariton interactions and---in a smaller proportion---from the incoherent pump saturation. In this way, just one of the two possible orientations of the synthetic field is selected, and thus, the condensate forms a vortex lattice analogous to that observed in a rapidly rotating ultracold gas~\cite{Madison_JModOpt_2000, Abo-Shaeer_Science_2001,  Cooper_AdvPhys_2008, Fetter_RMP_2009} or a type-II superconductor in the presence of an external magnetic field~\cite{Abrikosov_JEPT_1957, Blatter_RMP_1994, Tinkham_book_2004}.

Our proposal naturally applies to a variety of photonic platforms. For the sake of concreteness, we will focus our discussion on the specific case of a honeycomb lattice of semiconductor micropillar cavities for exciton-polaritons, as used in the recent experiments~\cite{Jacqmin_PRL_2014, Milcevic_PRX_2019, Whittaker_NatPhot_2020, Jamadi_strained_graphene2020, St-Jean_PRL_2021} and theoretical works~\cite{Salerno_2DMater_2015, Bleu_NatComm_2018, Solnyshkov_PRB_2021} to then comment what are the challenges and advantages of other platforms in view of our proposal.

\section{Results}
\subsection{Strained honeycomb lattice}

The honeycomb lattice is made of two sublattices $A$ and $B$. We model the kinetic energy of polaritons using a tight-binding Hamiltonian with nearest-neighbor hopping between the two sublattices,
\begin{equation}
H = -\sum\limits_{\mathbf{r}, j} t_j(\mathbf r) \hat a^\dag(\mathbf r - \mathbf R_j) \hat b (\mathbf r) + \textrm{h.c},
\end{equation}
where $\hat a$ and $\hat b$ annihilate a polariton in the $A$ and $B$ sublattices, respectively, and h.c. represents the Hermitian conjugate. The vector $\mathbf r=(x,y)$ indicates real-space coordinates and it labels all the positions of the $B$ sites, while the vectors $\mathbf R_j$, depicted in Fig. \ref{fig: lattice}a, connect different sites. The hopping energies $t_j(\mathbf r)$ correspond to the links associated with the vectors $\mathbf R_j$. We consider a hopping gradient in the horizontal links along $x$, choosing $t_1(x) = t(1+\tau x/3d)$, where $d$ is the lattice spacing, and $t_2=t_3=t$. The constant $\tau\geq 0$ determines the degree of strain in the lattice and, for a given size of the lattice in the $x$ direction, it has a maximum value beyond which $t_1(x)$ undergoes a sign change for negative positions $x$ (this is a Lifshitz transition and we avoid it).

For momenta near the two nonequivalent Dirac points,
\begin{equation}
\mathbf K_\xi = (K_{\xi,x}, K_{\xi,y})= \xi\left(\frac{2\pi}{3d}, \frac{2\pi}{3\sqrt{3}d}\right),
\end{equation}
where $\xi = \pm1$, the strain gives rise to a pseudomagnetic field $e\mathbf B = \xi 2\hbar \tau/9d^2 \hat z$ (see Appen.~\ref{app. A} or \cite{Salerno_2DMater_2015}), which has opposite orientation in each Dirac valley. The effect that this has over the single-particle energy bands can be seen in Fig. \ref{fig: lattice}c (note that, due to the strain, the only good quantum number is $k_y$). There are (tilted) Landau levels labeled by $n=\,\pm1,\, \pm2 , \dots$. To a very good approximation, their energies are given by $\varepsilon_n = \textrm{sgn}(n) t \sqrt{\tau |n|(1-\xi q_y d)}$, where $q_y = k_y - K_{\xi,y}$ is the (small) momentum-space distance measured from the Dirac point. For our purposes, the only important information about their wavefunctions is that they equally occupy both sublattices, $A$ and $B$, for any non-zero $n$. On the other hand, the band of $n=0$ Landau levels have zero dispersion ($\varepsilon_0 = 0$) and, most importantly, are completely localized in the $B$ sublattice (it would be in the $A$ sublattice if $\tau$ was negative). Their wavefunctions read
\begin{equation}\label{equ: n=0 wavefunction}
\phi_{n=0, B}(x,q_y)\propto e^{iK_{\xi,x}x} e^{-(x + \xi \ell_B^2 q_y)^2/2\ell_B^2},
\end{equation}
with $q_y = k_y - K_{\xi,y}$, and $\phi_{n=0,A} = 0$. This sublattice polarized wavefunctions can be recognized (besides the $x$-dependent phase) as the lowest Landau level states in the Landau gauge \cite{Girvin_Hall_lecture_notes}, given by a plane wave in the periodic $y$-direction and a Gaussian in $x$, with a guiding center $x_0 = -\ell_B^2q_y$ determined by the $q_y$ wavevector and a width determined by the magnetic length $\ell_B = \sqrt{\hbar/e|B|} = 3d/\sqrt{2\tau}$. This band of lowest Landau level states is the only family of bulk states in the system with sublattice polarization. We will take advantage of this to induce polariton condensation into the $n=0$ Landau level~\cite{Schomerus_PRL_2013}: given the full sublattice polarization of this state, we expect that the mode selection mechanism based on spatial overlap with the pumped sublattice will largely exceed other mechanisms that may be active in polariton systems, such as energy relaxation, the exciton-photon fraction of modes, and the amount of localization of the wave function at the pillars.

To better simulate a real experimental implementation, in the following we always consider large but finite lattices of $N_x$ links along $x$ and $N_y$ unit cells along $y$. As a reference, the diagram in Fig \ref{fig: lattice}a shows a lattice with $N_x=5$ and $N_y=4$.

\subsection{Incoherent pump, decay and interactions}
To model the Bose-Einstein condensation into the $n=0$ Landau level we have performed numerical simulations of interacting polaritons with binary interactions of strength $U$ in a finite strained honeycomb lattice, under the action of an incoherent pump and polariton losses (dominated by photon leakage out of the microcavities). The system is well described by stochastic Gross-Pitaevskii equations~\cite{Carusotto_RMP_2013} that read
\begin{equation} \label{equ: GPE1}
\begin{split}
i\hbar\partial_t \psi_A =& \textrm{Hop}(\psi_A\rightarrow \psi_B) + U|\psi_A|_-^2 \psi_A \\
&+ \frac{i\hbar}{2}\left( \frac{P_A}{1+|\psi_A|_-^2/n_s} -\gamma \right) \psi_A + iW_A,
\end{split}
\end{equation}
\begin{equation} \label{equ: GPE2}
\begin{split}
i\hbar\partial_t \psi_B =& \textrm{Hop}(\psi_B\rightarrow \psi_A) + U|\psi_B|_-^2 \psi_B \\
&+ \frac{i\hbar}{2}\left( \frac{P_B}{1+|\psi_B|_-^2/n_s} -\gamma \right) \psi_B + iW_B.
\end{split}
\end{equation}
For simplicity, we have omitted the spatio-temporal dependence of the macroscopic wavefunction $\psi = \psi(\mathbf r,t)$, of the pump profile $P=P(\mathbf r)$, and of the zero-mean complex Gaussian noise with $\Big\langle W_X(\mathbf r',t') W_Y^*(\mathbf r,t)\Big\rangle = \delta_{XY}\delta_{\mathbf r' \mathbf r}\delta(t-t')(\hbar^2/2)(P_X/(1+|\psi_X|_-^2/n_s) +\gamma)$, where the average is over stochastic realizations. The Hop terms correspond to the hopping between nearest neighbors and depend explicitly on the strain (see Appen.~\ref{app. B} for the explicit expression). $U$ is the polariton interaction strength, $n_s$ the saturation density, and $\gamma$ the decay rate. Polaritons in micropillars have an on-site interaction energy smaller than the linewidth, $U/\hbar\gamma <1$; in our results below we use modest ratios perfectly within the reach of current experiments  (see e.g. Ref.~\cite{Zambon_PRA_2020}). Underlying these equations is the assumption that there is a high-energy excitonic reservoir, excited by an external pump, which leads to the saturable incoherent pump\footnote{This form of pump as well as its influence in the noise correlations come from the incoherent process described by a Lindblad dissipator $C_X(\hat \psi_X^\dag \hat \rho(t) \hat \psi_X - \frac{1}{2}\{\hat \psi_X \hat \psi_X^\dag, \hat \rho(t)\})$, where the gain coefficient $C_X$ depends on the exciton-reservoir density. In the Wigner representation and after adiabatically eliminating this reservoir under the assumption that it instantaneously follows the low-energy polariton density, the coefficient becomes $C_X = P_X/(1+|\psi_X|_-^2/n_s)$.}
 in Eqs.~(\ref{equ: GPE1}) and (\ref{equ: GPE2}). These equations are obtained from a truncated Wigner approximation and thus the Wigner commutator is subtracted from the intensity, $|\psi|^2_- = |\psi|^2 - 1$.

If the occupation of the excitonic reservoir is substantial, there is an additional polariton energy blueshift---not included in Eqs.~ (\ref{equ: GPE1}) and (\ref{equ: GPE2})---which is induced by the reservoir formed in the pumped region. Since we will consider a modulated pump acting only on some sites and not on all of them, this extra term could distort the single-particle energy bands. We later discuss the possible complications that might arise as well as possible workarounds.

The results that we are going to show in the following of the work refer to the long-time limit of the system evolution. A study of the additional features that may occur during the switch-on transient, such as Kibble-Zurek vortex nucleation phenomena~\cite{Solnyshkov_PRB_2021}, go beyond the scope of this work.

\begin{figure*}[!ht]
  \includegraphics{figure2.pdf}
  \caption{\textbf{BEC in the $\mathbf{n=0}$ Landau level.} Intensity (left) and phase (middle) spatial profiles, and spectral density $\Big\langle|\psi(\omega, k_y)|^2\Big\rangle$ (right) for a Gaussian pump with maximum $1.3 \gamma$ and width $\sigma = 2\ell_B$ in \textbf{a} and $\sigma = 5 \ell_B$ in \textbf{b}. The interior of the magenta (dashed) circles indicates the region where the pump is larger than the losses. In the phase profiles, only the $B$ sublattice is shown, and for clarity we have removed the phase-shift from to the Dirac momentum by plotting the phase of $\langle\exp(-i\mathbf K_\xi \cdot \mathbf r)\psi_B(\mathbf r)\rangle$, where $\mathbf K_\xi = \xi(2\pi/3d, 2\pi/3\sqrt{3}d)$, with $\xi = \pm1$. In \textbf{b} a clear anti-vortex ($-2\pi$ circulation) is displayed. In the right column we have superimposed the spectral density to the single-particle spectrum, shown in dim white lines. The parameters are $J/\hbar\gamma = 10$, $n_s=10^3$, $U/\hbar \gamma = 0.005$, $\tau=0.06$, $N_x=51$, and $N_y=50$. We have averaged over 100 stochastic realizations.}
\label{fig: BEC}
\end{figure*}

\subsection{Condensation into the $n=0$ Landau level}

In order to fully exploit the sublattice polarization of the $n=0$ Landau level, we start by considering a spatially modulated incoherent pump acting only on the $B$ sublattice ($P_A = 0$). When the pump overcomes losses, $P_B \gtrsim \gamma$, polaritons condense in the $n=0$ Landau level, since this is the only single-particle state with this sublattice polarization. Depending on how many sites the incoherent pump covers, we find a BEC with zero, one, or many vortices.

We first discuss the situation where the size of the pumped region is not too large compared to the magnetic length $\ell_B$. In Fig. \ref{fig: BEC}a,b we show the stationary-state intensity, phase, and spectral density for two Gaussian pumps with the same maximum intensity but different widths, namely $P_B(r)/\gamma = 1.3 e^{-r^2/2\sigma^2}$, with $\sigma=2\ell_B, \,5\ell_B$, respectively. In the former case, the pump region is not wide enough to accommodate a vortex, while in the latter, a clear anti-vortex ($-2\pi$ phase circulation) can be seen in the center of the lattice. In the plotted spectral densities $\Big\langle|\psi(\omega, k_y)|^2\Big\rangle$, one can see that the condensate occupies a single Dirac valley predominantly. Which of the two valleys is chosen for condensation is randomly chosen at each instance of the condensation process and depends on the randomly chosen initial conditions and on the noise $W_{A,B}$, if any. The vortex has its origin in the single-particle Landau states, so (besides the energy blueshift seen in the spectral density) interactions play no role on the vortex formation at these pumped-region sizes. Indeed, the (normalized) stationary state analyzed in Fig. \ref{fig: BEC}b has a remarkable overlap of $\left| \sum_{\mathbf r} \phi^*(\mathbf r)\cdot \psi_B(\mathbf r)/\mathcal N\right|  \approx \%68$ ($\%99$ intensity match) with the slightly spatially shifted $n=0, m=-1$ symmetric-gauge Landau state $\phi(x,y) \propto (x-iy)e^{-(x^2+y^2)/4\ell_B^2}$ with angular momentum $m\hbar=-\hbar$ \cite{Girvin_Hall_lecture_notes}. As usual, this symmetric-gauge Landau state can be written as a linear combination of Landau-gauge Landau states of different $k_y$'s.

\begin{figure}[ht!]
\centering
  \includegraphics{figure3.pdf}
  \caption{\textbf{Vortex arrays for large lattices and wide top-hat pumps}. Real-space intensity for a rectangular ({\bf a}) and circular ({\bf b}) top-hat pump. These are late-time snapshots of mean-field trajectories ($W_{A,B}=0$). The vortex array rotates in the sense determined by the orientation of the chosen pseudomagnetic field. All $B$ sites inside the magenta dashed rectangle or circle are pumped with the same intensity. The parameters are $J/\hbar\gamma = 10$, $n_s=10^3$, $P_B/\gamma = 1.05$, and $N_y=80$ in both cases, and $U/\hbar\gamma=(4,5)\times 10^{-3}$, $\tau=(0.045, 0.039)$, and $N_x=(81,101)$ in (\textbf{a}, \textbf{b}).}
\label{fig: figure 3}
\end{figure}

On the contrary, interactions play instead a key role in the case of wider incoherent pump profiles, where they make condensation in a single Dirac valley---as opposed to in both valleys simultaneously---more likely. In standard BECs at thermal equilibrium, the interaction energy is minimized by choosing among the single-particle ground states the one which has the most homogenous density in real space. Here, a similar mechanism hinders the condensate from occupying both valleys at the same time, which would entail large density inhomogeneities due to destructive interference of states with opposite angular momenta. This is important for forming a vortex array, as the two opposite pseudomagnetic fields at the two Dirac valleys compete and suppress vortices. In Fig. \ref{fig: figure 3}, we show late-time snapshots of the real-space intensity profile for large rectangular and circular top-hat incoherent pumps (drawn on the images). In both cases, condensation occurs in a single Dirac valley and several vortices form. Note that for such wide pump profiles, the condensate does not reach a stationary state but keeps evolving in time even at the mean-field level ($W_{A,B}=0$). In all cases, the vortex lattice tends to rotate in the sense determined by the sign of the pseudomagnetic field corresponding to the chosen Dirac valley. For a non-circular pump profile, the shape of the vortex lattice and its motion are no longer regular, but displays chaotic trajectories. If noise is added ($W_{A,B}\neq 0$), in each trajectory the vortices diffuse in a slightly different way. Thus, with time, the vortices will be smeared out in the stochastic average. Nevertheless, this process is slow ($\sim 100\gamma^{-1}$), so vortex lattices should be observable in a single shot experiment where the intensity profile is obtained as a time average of a single realization. Two videos showing the dynamics corresponding to the the snapshots of Figs.~\ref{fig: figure 3}a and b can be found in \cite{Videos_UCL_repository}.

\begin{figure}[t!]
\centering
  \includegraphics{figure4.pdf}
  \caption{\textbf{Comparison of condensation with and without interactions.} Steady-state real-space intensity profile for $U/\hbar\gamma=0.005$ (\textbf{a}) and $U=0$ (\textbf{b}). Condensation takes place in one Dirac valley in \textbf{a}, while in both valleys in \textbf{b}. All $B$ sites inside the magenta dashed rectangle are pumped with the same intensity. The rest of the parameters are $J/\hbar\gamma = 10$, $n_s=10^3$, $P_B/\gamma = 1.05$, $\tau=0.06$, $N_x=51$, and $N_y=50$. We have averaged over 100 stochastic realizations.}
\label{fig: vortices or no vortices}
\end{figure}

If interactions are switched off ($U=0$), the saturation nonlinearity in Eq.~(\ref{equ: GPE2})---which plays a similar role to polariton-polariton interactions---is not always strong enough to efficiently prevent condensation in both Dirac valleys. To illustrate this point, let us compare the interacting and non-interacting cases in a moderate-sized lattice with a broad rectangular top-hat pump. In Fig.~\ref{fig: vortices or no vortices}a, for $U\neq 0$, three anti-vortices are found as the polaritons have condensed in the positive-momentum Dirac valley. In Fig.~\ref{fig: vortices or no vortices}b we show, instead, the non-interacting $U=0$ case where both Dirac valleys are occupied, such that no vortices are formed. Instead, we obtain a spatially oscillating density pattern formed from overlapping  condensates at the two valleys. For large pump profiles, it is rare but not impossible, even for sizable $U$, to end up in configurations of two almost spatially separated condensates in different valleys with an overlapping boundary region. An example of such situation is shown in Fig.~\ref{fig: opposite circulations}, where there is a single anti-vortex in the bottom and three vortices in the middle-top. However, unless $U=0$ the condensates in the two valley are spatially separated and their overlap is hardly as great as in Fig.~\ref{fig: vortices or no vortices}(b).

\begin{figure}[t!]
\centering
  \includegraphics{figure5.pdf}
  \caption{\textbf{Spatially-separated condensates in different Dirac valleys.} Late-time snapshot of the real-space intensity in a mean-field trajectory ($W_{A,B}=0$). There is one anti-vortex in the bottom, three vortices in the middle-top, and an interference pattern in between. All $B$ sites inside the magenta dashed rectangle are pumped with the same intensity. Same parameters as in Fig.~\ref{fig: vortices or no vortices}a but with $N_y=80$.}
\label{fig: opposite circulations}
\end{figure}

The fact that the two opposite pseudomagnetic fields can suppress the formation of vortices posses the question of how many vortices are typically found in a given realization of the condensation process. If we had a real magnetic field and the system was at thermal equilibrium, the number of vortices would be determined by the ratio between the total magnetic flux piercing the system and the magnetic-flux quantum, so would thus be proportional to the system size. In our case, the number of vortices found fluctuates from one realization to another. We statistically analyze 100 realizations of the mean-field dynamics with different random initial conditions to look at how the number of vortices depend upon the number of unit cells $N_y$ in the $y$-direction. We consider a top-hat pump over all $B$-sites but the outermost (as in in Fig.~\ref{fig: vortices or no vortices}). In Fig.~\ref{fig: statistics} we show the statistics of the total number of vortices (and/or anti-vortices, irrespective of the topological charge) for different values of $N_y$. We compare the interacting and non-interacting cases. We can see that for $U=0$ the number of vortices grows much slower as $N_y$ is increased than for the finite $U$ case. As we have discussed earlier, this is because interactions favor the selection of a single Dirac valley for condensation---or, in other words, one of the two orientations of the pseudomagnetic field---and thus there is no competition for vortex formation.

\begin{figure}[ht!]
\centering
  \includegraphics{figure6.pdf}
  \caption{\textbf{Boxplot for the vortex-number statistics} of 100 mean-field (zero noise $W_{A,B}=0$) realizations of different random initial conditions $\psi(x_i,y_j,t=0)$, for $N_y=30,40,\dots,80$, with (right) and without (left) interactions. For each data set, the lower bar is at the lowest datum above $Q_1 - 1.5(Q_3-Q_1)$, and the upper bar at the highest datum below $Q_3 + 1.5(Q_3-Q_1)$, where $Q_1$ and $Q_3$ are the first and third quartiles. The median is shown with the orange line, the box encloses data between $Q_1$ and $Q_3$, and the outliers are indicated by circles. We considered a top-hat pump over all $B$-sites but the outermost (as in in Fig.~\ref{fig: vortices or no vortices}). The parameters are $J/\hbar\gamma = 10$, $P_B/\gamma = 1.1$, $\tau=0.06$, $N_x=51$, and $U/\hbar\gamma=0.005$ in the case finite interactions.}
\label{fig: statistics}
\end{figure}

\subsection{Robustness to disorder and the effect of reservoir-induced blueshift}

In order to verify the actual feasibility of our proposal, we have checked that the BEC in the $n=0$ Landau level is robust against those complications that are most likely to occur in concrete experiments. First of all, we have verified that our predictions remain valid if some sizable fraction of the incoherent pump sneaks into the $A$ sublattice, which is the one not occupied by the $n=0$ states. It is possible---for any lattice size---to have $P_A \sim 0.5 P_B$ without any qualitative change. The maximum amount of pump in the $A$ sublattice that the vortex configuration can tolerate depends on the system size as well as the pump intensity. For instance, for small lattices (e.g., $N_x=11, N_y=20$), both sublattices can be pumped with almost the same intensity near the BEC threshold. In general, it is convenient to avoid pumping the left-hand edge of the lattice where the propagating edge states (associated to the $n=0$ Landau level) are found. If that region is strongly pumped, it can lead to chaotic behavior where many energy bands are occupied.

As previously pointed out, if the excitonic reservoir is substantially populated it leads to an on-site energy renormalization (blueshift) for the polaritons in the micropillars. Since we pump only the $B$ sublattice, the blueshift would affect just the pumped micropillars and would distort the Landau energy levels. Moreover, using a small Gaussian pump spot can lead to localization into the highest energy bands~\cite{Milicevic_SciPost_2018}, with the energy blueshift playing a similar role to on-site energy disorder. We have checked that the vortex configuration is robust to the reservoir-induced blueshift as well as to on-site energy disorder, as long as they are smaller than $\hbar \gamma$.

In order to remove this possibly stringent constraint on the reservoir-induced blueshift, one can work in the weak light-matter coupling regime where the blueshift should be saturated and then it does not matter that some micropillars are pumped and others are not. In this case, the polariton would be predominantly photonic and the interactions very weak $(U\sim 0)$, but vortices and vortex arrays can still form, just less efficiently as shown in Fig.~\ref{fig: statistics}. A different workaround for the energy blueshift is to tailor the polariton losses such that the loss in $A$ sublattice is larger than that of the $B$ sublattice. We have checked that when the decay rate is $\%15$ larger in the $A$ sublattice, one can uniformly pump (slightly above BEC threshold) all the sites in the system and the $n=0$ Landau level is still selected for condensation. In semiconductor micropillar cavities this could be achieved by modifying the Bragg mirrors of the $A$-sublattice's micropillars to increase their radiative decay. Note however that all complications arising from the excitonic reservoir are exclusive to exciton-polaritons and should not arise in alternative platforms that we suggest in the following section.

\section{Discussion}
In addition to suggesting a new experimental platform where to study the many-body physics of vortex lattices in a novel non-equilibrium context, our work raises a number of further conceptual questions. The randomness in the Dirac valley selection poses the intriguing question whether it could be possible to bias the selection towards one valley to systematically form vortices or anti-vortices. One possibility would be to have a biasing coherent pump on one Dirac valley, which is slowly switched off in time in such a way that the condensate remains in the biased valley. This is a standard procedure in the study of symmetry-breaking phase transitions. Another exciting option to explore is to deform the lattice in a way that a single Dirac valley is dynamically favored and time-reversal symmetry gets effectively broken without the need for reciprocity-breaking elements, but with the help of the nonlinear mechanisms involved in condensation, as recently studied in simpler geometries~\cite{Heras_PRA_2021}.

In this work we focus on polariton micropillar lattices, but there are other promising potential platforms where to observe the predicted spontaneous formation of vortex arrays, including the evanescently-coupled optical waveguides of the experiments in refs.~\cite{Rechtsman_Nat_2013,Rechtsman_NatPhoton_2013} and circuit QED lattices~\cite{Gu_PhysRep_2017,Kollar_Nature_2019,Carusotto_NatPhys_2020,Blais_arxiv_2020}. In the coupled optical waveguides experiments, the interplay of optical nonlinearities with topology has recently attracted a great attention~\cite{Mukherjee_Science_2020,Maczewsky_Science_2020} and different losses for the two strained-honeycomb's sublattices have been used in ref.~\cite{Kremer_NatComm_2019} to mimic the effect of an incoherent pump and study a non-Hermitian $\mathcal P \mathcal T$-symmetry-breaking phase transition. Regarding the circuit QED platform, a main challenge would be the disorder of the hopping strength and the resonator energy, but there is great flexibility in lattice design~\cite{Kollar_Nature_2019} and the platform offers the possibility of having stronger interactions~\cite{Gu_PhysRep_2017,Blais_arxiv_2020} than those achievable in exciton-polaritons.

When applied to strongly-interacting photonic lattices ($U>\hbar \gamma$), our findings pave the way to studying the transition from the vortex-dominated BEC regime to the strong-correlations regime of the fractional quantum Hall physics. That transition has been first anticipated for ultracold atoms in a rotating trap, but so far its observation has remained experimentally challenging~\cite{Cooper_AdvPhys_2008,Fetter_RMP_2009}. It is in fact experimentally very hard to achieve high angular velocities and low atomic densities such that a fractional occupation of the lowest Landau level is achieved. While active work is being devoted to reach strong interactions for exciton-polaritons in semiconductors~\cite{Togan_PRL_2018, Rosenberg_SciAdv_2018, Munoz_NatMat_2019, Delteil_NatMat_2019}, first reports of experimental studies of the interplay of strong synthetic magnetic fields and strong interactions in photonic systems have recently started appearing in the literature using Rydberg polaritons in atomic media~\cite{Clark_Nat_2020} or circuit-QED devices~\cite{Roushan_NatPhys_2017} giving concrete hopes for the success of this very ambitious scientific adventure.

\section*{Data and Code Availability}
All the numerical data and codes used in this article are available upon reasonable request to the first author.

\section*{Acknowledgements}
We thank A. Amo, J. Bloch, O. Jamadi, and S. Ravets for helpful discussions, and C. Mc Keever for comments on the manuscript.
C.L. gratefully acknowledges the financial support of ANID through Becas Chile 2017, Contract No. 72180352.
IC acknowledges support from the European Union Horizon 2020 research and innovation programme under grant agreement No. 820392 (PhoQuS) and from the Provincia Autonoma di Trento.
M.H.S. gratefully acknowledges financial support from the Quantera ERA-NET cofund project InterPol (through the EPSRC Grant No.  EP/R04399X/1) and EPSRC Grant No. EP/S019669/1.

\begin{appendix}

\section{Analytical derivation of Landau levels}
\label{app. A}

The analytical derivation of the Landau energies and states in a strained honeycomb lattice is well understood in the context of graphene~\cite{Castro_RMP_2009, Guinea_NatPhys_2010}. Here we reproduce the results from~\cite{Salerno_2DMater_2015, Salerno_PRB_2017}, which deal with a synthetic strain, as in our work.

The Landau level states and energies can be obtained by writing the single-particle bulk Hamiltonian in momentum space, $H(\mathbf k) = \mathbf h(\mathbf k) \cdot \bm{\sigma}$, where $\bm \sigma = (\sigma_x, \sigma_y)$ are Pauli matrices and $\mathbf h(\mathbf k) = (\textrm{Re }h(\mathbf k), -\textrm{Im }h(\mathbf k))$, with $h(\mathbf k) = -\sum_j t_j \exp(i \mathbf k \cdot \mathbf R_j)$. Due to the strain and so the lack of translational symmetry, we must consider a finite lattice along $x$ and thus $k_x$ is no longer a good quantum number. Moreover, $h(\mathbf k)$ depends explicitly on $x$ via $t_1(x)$. Yet, to a very good approximation, the bulk Hamiltonian describes well the bulk physics~\cite{Salerno_2DMater_2015, Salerno_PRB_2017, Jamadi_strained_graphene2020}. This is because, as will be clear in the following, there is a wide range of parameters where orbits are well localized in the bulk in a region where the hopping $t_1$ does not change significantly. Having stated the necessary precautions, we proceed by expanding $h(\mathbf k)$ for small momenta $\mathbf q$ near one of the two opposite Dirac points, $\mathbf k = \mathbf K_\xi + \mathbf q$, where $\xi = \pm 1$ and $\mathbf K_+ = (\frac{2\pi}{3d}, \frac{2\pi}{3\sqrt{3}d}) = -\mathbf K_-$, yielding
\begin{equation} \label{equ: h function}
h(\mathbf K_\xi + \mathbf q) \approx v_D^x\hbar q_x -i v_D^y\xi(\hbar q_y + eA_y)
\end{equation}
to first order in $x$ and $q$, where $v_D = (3dt/2\hbar)e^{\xi i2\pi/3}$ is a Dirac velocity and $eA_y = 2\hbar \tau \xi x/9d^2$ is the synthetic vector field, giving rise to the two opposite magnetic fields $e\mathbf B = \nabla \times e\mathbf A = \xi 2\hbar \tau/9d^2 \hat z$.

To find the spectrum of $H(\mathbf K_\xi + \mathbf q)$, we promote $h$ in Eq.~(\ref{equ: h function}) to an operator such that it becomes proportional to the annihilation operator of a displaced harmonic oscillator,
\begin{equation}
\hat h \approx \hbar t \sqrt{\tau} \hat c = v_D \hbar \hat q_x -i \frac{v_D}{\ell_B^2}(\hat x + \xi \ell_B^2 q_y),
\end{equation}
where $q_y$ is the conserved $y$-momentum, $\ell_B = 3d/\sqrt{2\tau}$ is the magnetic length, and $[\hat c, \hat c^\dag]=1$. This suggests the eigenvectors of $H(\mathbf K_\xi + \mathbf q)$ should be vectors of two components related to the solutions of a displaced harmonic oscillator, where the displacement is proportional to $q_y$, just as Landau-level states in the Landau gauge \cite{Girvin_Hall_lecture_notes}. This is indeed the case. The eigenvalue problem $H(\mathbf K_\xi + \mathbf q) \vec{\phi} = \varepsilon \vec{\phi}$ is
\begin{equation}
\hbar t \sqrt{\tau}\begin{pmatrix}
0 & \hat c \\
\hat c^\dag & 0
\end{pmatrix} \begin{pmatrix} \phi_A \\ \phi_B \end{pmatrix} = \varepsilon \begin{pmatrix} \phi_A \\ \phi_B \end{pmatrix},
\end{equation}
and its solution consists of the $\varepsilon_{n=0}=0$ energy and its associated eigenstate in Eq.~(\ref{equ: n=0 wavefunction}), as well as higher and lower Landau energy levels labeled by $n=\,\pm1,\, \pm2 , \dots$, with energy $\varepsilon_n = \textrm{sgn}(n) t \sqrt{\tau |n|}$ and eigenstates
\begin{equation}
\begin{pmatrix}
\phi_{n,A}(x,q_y) \\ \phi_{n,B}(x,q_y)
\end{pmatrix} \propto e^{iK_{\xi,x}x} \begin{pmatrix}
\pm \phi_{|n|-1}(x,q_y) \\ \phi_{|n|}(x,q_y)
\end{pmatrix},
\end{equation}
where $\phi_n(x,q_y) = e^{-(x + \xi \ell_B^2 q_y)^2/2\ell_B^2} H_{n}(x + \ell_B^2 q_y)$ is the $n$-th Landau level state in the Landau gauge, with $H_n(x)$ the $n$-th Hermite polynomial. We finally note that to account for the tilt in the $|n|\geq 1$ levels (see Fig.~\ref{fig: lattice}b), one can expand the function $h$ to next order (in $q$ and $x$), finding $\varepsilon_n = \textrm{sgn}(n) t \sqrt{\tau |n|(1-\xi q_y d)}$.

We can now see {\it a posteriori} that our approximation is good as a long as the hopping $t_1(x)$ does not change significantly in a distance $\ell_B$---the width of the Landau level states. The variation is giving by $[t_1(x+\ell_B) - t_1(x)]/t = \sqrt{\tau/2}$.

\section{Numerical simulations}
\label{app. B}

The symbolic hopping (Hop) terms in Eqs.~(\ref{equ: GPE1}) and (\ref{equ: GPE2}) read
\begin{equation}
\begin{split}
i\hbar \partial_t \psi_A(\mathbf r-\mathbf R_1) =& -t[\psi_B(\mathbf r-\mathbf R_1 + \mathbf R_2) + \\
& \qquad \psi_B(\mathbf r -\mathbf R_1 + \mathbf R_3)] \\
& - t_1(x) \psi_B(\mathbf r) + \dots \\
i\hbar \partial_t \psi_B(\mathbf r) =& -t[\psi_A(\mathbf r-\mathbf R_3) + \psi_A(\mathbf r -\mathbf R_2)] \\
& - t_1(x) \psi_A(\mathbf r-\mathbf R_1) + \dots,
\end{split}
\end{equation}
where the ellipsis refer to all other terms present in Eqs.~(\ref{equ: GPE1}) and (\ref{equ: GPE2}). The vector $\mathbf r$ labels all the discrete positions of $B$ sites.

We carry out the numerical analysis by solving the stochastic Gross-Pitaevskii equations using the open-source package XMDS2 \cite{xmds2}. For the results shown in Figs.~\ref{fig: BEC} and \ref{fig: vortices or no vortices}, we first run a single mean-field trajectory ($W_{A,B}=0$) until a stationary state is reached, typically for a time between $10^3$ and $5\times 10^3$ in units of the inverse decay rate $\gamma^{-1}$. Only then, we turn on the Gaussian noise and follow up 100 stochastic trajectories for a time $120\gamma^{-1}$. The time Fourier transform in the spectral densities is obtained from the final $\Delta t = 100 \gamma^{-1}$ time lapse.
\end{appendix}

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This module was written by Judy McKimm, Clinical Education Programme Director, University of Auckland, and Visiting Professor, University of Bedfordshire, and Dulcie Jane Brake, Clinical Education Programme Administrator at the Centre for Medical and Health Sciences, University of Auckland. The module relates to areas 2 and 3 of the Professional Development Framework for Supervisors in the London Deanery.
Adam Feather (Queen Mary, University of London) for additional material and to the University of Auckland for the use of some course materials used on the Masters in Clinical Education programme offered by the Faculty of Medical and Health Sciences.
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Kilminster S, Hale C, Lascelles M, Morris P, Roberts T, Stark P, Sowter J and Thistlethwaite J (2004) Learning for real life: patient-focused interprofessional workshops offer added value. Medical Education. 38: 717–26.
Laming Report (2003) The Victoria Climbié Inquiry. Report of an inquiry by Lord Laming. HMSO, London (accessed 10 June 2008).
Lave J and Wenger E (1991) Situated Learning: legitimate peripheral participation. Cambridge University Press, Cambridge, pp. 91–117.
Lingard L, Reznick P, DeVito I and Espin P (2002) Forming professional identities on the health care team: discursive construction of the 'other' in the operating room. Medical Education. 36: 728–34.
Lindqvist SM and Reeves S (2007) Facilitators' perceptions of delivering interprofessional education: a qualitative study. Medical Teacher. 29: 403–5.
Mandy A, Milton C and Mandy P (2004) Professional stereotyping and interprofessional education. Learning in Health and Social Care. 3(3): 154–70.
McGrath M (1991) Multidisciplinary Teamwork. Avebury, Aldershot.
McNair R, Brown R, Stone N and Sims J (2001) Rural interprofessional education: promoting teamwork in primary health care education and practice. Australian Journal of Rural Health. 9(Suppl.): 19–26.
Morison SL and Stewart MC (2005) Developing interprofessional assessment. Learning in Health and Social Care. 4(4): 192–202.
Niemi PM (1997) Medical students' professional identity: self-reflection during the pre clinical years. Medical Education. 31: 408–15.
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Paylor J, Meyer E and Humphris D (2008) Pedagogy for interprofessional education – what do we know and how do we evaluate it? Learning in Health and Social Care. 7(2): 64–78.
Pollard KC, Miers ME and Gilchrist M (2004) Collaborative learning for collaborative working? Initial findings from a longitudinal study of health and social care students. Health and Social Care in the Community. 12(4): 346–58.
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Spouse J (1998) Learning to nurse through legitimate peripheral participation. Nurse Education Today. 18: 345–51.
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Wagner E (2004) Effective teamwork and quality of care. Medical Care. 42(11): 1037–9.
Way DO, Busing N and Jones L (2002) Implementing Strategies: collaboration in primary care – family doctors and nurse practitioners delivering shared care. Ontario College of Family Physicians, Toronto.
Wenger E, McDermott R and Snyder WM (2002) Cultivating Communities of Practice. Harvard Business School Press, Boston, MA, pp. 1–21.
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Kenya beat Rwanda by five wickets yesterday in the ongoing ICC World Twenty20 Africa Region Qualifier B in Kigali.
This was their fourth win in the series with veteran Collins Obuya (44 off 35 balls) leading the scoreboard for Maurice Odumbe's men in a pulsating encounter.
The Rwandese coached by ex-Kenyan international Martin Suji had been restricted in the second innings to good effect led by player of the match Peshpak Kerai (4/25) as Kenya posted 129/5 inside 16.1 overs.
Rwanda who won the toss and selected to bat had only set a score total of 125 all out in their innings. Bashir Songa (43 off 31 balls) top scored for the hosts including two glorious boundaries and three sixes. His momentum was to be later broken when pace bowler Nehemiah Odhiambo dismissed him out in the 18.5 over. Kerai weighed in with a massive four wickets haul as the home crowd was hushed.
Earlier on, openers Dhiren Gondaria and Alex Obanda had set out a steady partnership when they combined for (43 runs in 29 balls) before the hosts begun their own onslaught.
Gondaria (13 off 12 balls) was caught out napping by Bosco Tuyizere after good delivery on the crease from spin bowler Zappy Bimenyimana. Obanda was to later to follow his team-mate to the showers after being caught leg before wicket by Yvan Mitari in the fifth over.
Skipper Shem Ngoche (12 runs off 09 balls) had a decent game with both ball and bat as he helped his team shore up scores on the board.
His two wicket haul off his short balls was exciting for the Kenyans as new call up Eugene Ochieng also came through with three fall of wickets with his tricky deliveries.
The trick to move Obuya to number four in the order was a masterstroke as he brought in calm as three of his fellow batsmen had been fallen.
The Stray Lions batsman was not out as he faced 35 balls,posting two sixes and a boundary which were significant. Kenya next face Tanzania who stunned Uganda by six wickets win.
time for their match against Police, thus surrendering all three points to the law enforcers.


Who Is Brett Young's Wife Taylor Mills?
On tonight's episode of "The Bachelor," country star Brett Young swings by to perform his hit single "Here Tonight" for Colton and his bachelorettes.
The 2017 Country Music Festival, aka CMA Fest, airs on TV tonight. Check out what time and channel to watch, plus more details on the show.
Get the details on when to watch the Academy Of Country Music Awards on TV tonight. Read on for the 2017 ACMs date, channel and more.
Check out how to watch the 2016 show of the CMA Awards online via live stream. The Nashville event airs on ABC.
Matz and Cain are rising stars in the respective fields of baseball and country music, a budding power couple.
CMT Artist of The Year 2015: What Time & Channel Is It On Tonight?
Tonight is the 2015 CMT Artist of The Year special. Get the details on how to watch the show online via the CMT live stream app.


Pest Control in Balch Springs, TX - At Ameritech Termite & Pest Control we pride ourselves in offering excellent customer service. We have been proudly servicing businesses and homes in the Dallas Fort Worth Metroplex for over 30 years. If you need any kind of pest control service in Balch Springs, contact Ameri-Tech Termite & Pest Control Company. We are a locally owned business that focuses on the total removal of all of your bugs, ants, spiders etc. We care about our customers and you can trust us to do the job right the first time.
Balch Springs, TX Bedbugs, Fleas & Ticks - Bedbugs are six legged parasitic bugs that draw human and pet blood. Their length is around 1/4 inch with an oval flat form. Their size is similar to an apple seed. Top of the part of their bodies has gold colored hair, antennae and cone like eyes. The bottom part of their own bodies is wrinkly like crinkled paper. Bedbugs are unable to fly but they can crawl very quickly. They will develop and multiply in the temperature range of 70 degrees around 80 degrees. A bed bug, is known as a nymph, they are see-through in color and changes into a red color after eating. To succeed in adulthood, a nymph bed bug must shed its skin approximately five times. A typical female can lay 5 up to 7 eggs each week and may produce around 500 eggs throughout its life expectancy of 12 months to eighteen months. The eggs will hatch out in just 6 to 17 days when they become known as nymphs. Bed Bug eggs are resistant to pesticides or herbicides. Bedbugs hide in mattresses, rugs, bedsheets, clothes, underneath wallpaper, under cloths, between window curtain folds, behind wall decorations and behind wooden home furniture. They love to attack through the night and they will remain active until before daybreak. Bed bugs bite uncovered skin of a man or woman sleeping in an infested bed by leaving red-colored itchy spots. They don't wander away from sleeping and lounging areas nonetheless they be capable of travel over 100 ft throughout the night to look for food.
Termite Treatment in Balch Springs, TX - Subterranean termite homes are usually made around the soil. Inside these mounds, termites build intricate tunnel systems and then use dirt tunnels in which they will access above-ground wood resources. Dry-wood termites reside inside the wood which they eat and moving into and infesting wall space and pieces of furniture. Little techniques produce a big difference with termite prevention and keeping a subterranean termite plan for treatment. Start off by reducing moisture conditions as well as wood eating termite food all around your home. These kind of simple measures make your home a less appealing target, helping deter wood eating termites. A wood eating termite's jaws are capable of tearing pieces of cellulose substance.


text:
require 'test_helper'

class ScriniumCloudTest < ActiveSupport::TestCase
  test "truth" do
    assert_kind_of Module, ScriniumCloud
  end
end

redpajama_set_name: RedPajamaGithub


So I have never been to a Cars and Coffee. I am at college south of Detroit and I noticed they had one. I tried to look up information online and it proved fruitless. Does anyone know anything or have they gone to the show. When is it, where is it? Stuff like that would be good to know before I drive an hour and a half to Detroit. Thanks Opp!


text:
David Kolomatis (né le  à Livingston, dans l'État du New Jersey aux États-Unis) est un joueur professionnel américain de hockey sur glace. Il évolue au poste de défenseur.

Carrière de joueur

Statistiques
Pour les significations des abréviations, voir statistiques du hockey sur glace.

|2005-2006 || États-Unis || NAHL ||16 ||1 ||0 ||1 ||4 ||- ||- ||- ||- ||-
|-
|2006-2007 || Attack d'Owen Sound || LHO ||67 ||4 ||16 ||20 ||54 ||4 ||0 ||0 ||0 ||0
|-
|2007-2008 || Attack d'Owen Sound || LHO ||68 ||9 ||36 ||45 ||68 ||- ||- ||- ||- ||-
|-
|2008-2009 || Attack d'Owen Sound || LHO ||63 ||18 ||28 ||46 ||52 ||4 ||2 ||2 ||4 ||0
|-
|2008-2009 || Bruins de Providence || LAH ||4 ||0 ||0 ||0 ||0 ||16 ||0 ||1 ||1 ||2
|-
|2009-2010 || Monarchs de Manchester || LAH ||76 ||8 ||21 ||29 ||30 ||15 ||0 ||1 ||1 ||2
|-
|2010-2011 || Monarchs de Manchester || LAH ||70 ||8 ||20 ||28 ||58 ||7 ||2 ||2 ||4 ||2
|-
|2011-2012 || Monarchs de Manchester || LAH ||58 ||5 ||20 ||25 ||12 ||4 ||0 ||1 ||1 ||4
|-
|2012-2013 || Monarchs de Manchester || LAH ||46 ||8 ||20 ||28 ||18 ||4 ||0 ||0 ||0 ||6
|-
|2013-2014 || Bears de Hershey || LAH ||61 ||7 ||23 ||30 ||22 ||- ||- ||- ||- ||-
|-
| 2014-2015 || Tappara || Liiga || 45||1 ||11 ||12 ||22 ||- ||- ||- ||- ||-
|-
|2015-2016 || Monarchs de Manchester || ECHL ||35 ||6 ||11 ||17 ||16 ||- ||- ||- ||- ||-
|-
|2015-2016 || Marlies de Toronto || LAH || 23 || 1 || 3 || 4 || 8 || - || - || - || - ||-
|-
|2016-2017 || Monarchs de Manchester || ECHL ||61 ||7 ||28 ||35 ||10 ||19 ||2 ||5 ||7 ||10
|-
|2017-2018 || Monarchs de Manchester || ECHL ||57 ||6 ||24 ||30 ||24 ||9 ||3 ||2 ||5 ||6
|-
|2018-2019 || Monarchs de Manchester || ECHL ||71 ||14 ||29 ||43 ||12 ||11 ||1 ||3 ||4 ||4
|-

En équipe nationale

|-
|2006 || align=left| États-Unis U17 || aling=left|Défi mondial des moins de 17 ans || 6 ||0 ||0 ||0 ||0 || align=left| Médaille d'argent
|-

Notes et références

Naissance en février 1989
Naissance à Livingston (New Jersey)
Choix de repêchage des Kings de Los Angeles
Défenseur de hockey sur glace
Joueur américain de hockey sur glace
Joueur de l'Attack d'Owen Sound
Joueur des Bears de Hershey
Joueur des Bruins de Providence
Joueur des Marlies de Toronto
Joueur des Monarchs de Manchester (ECHL)
Joueur des Monarchs de Manchester (LAH)
Joueur du Tappara


text:
Posted on July 11, 2018 by staff
New study finds half of ICOs fail within first four months
Research from a college in Massachusetts suggests that initial coin offerings have a high failure rate
bc deals
Alistair Hardaker	 2:41pm 11th Jul 2018
An Initial Coin Offering (ICO) is an alternative to an IPO which offers a share of the company in cryptocurrency.
Around 56 per cent of crypto start-ups which raise money through token sales fall through within four months.
That is the latest finding from a study carried out by Boston College in the US on 2,390 initial coin offering or ICO.
The researchers analysed the frequency of tweets from start-ups to surmise which were still active.
This approach suggests to the researchers that only 44.2 per cent of startups are still active 120 days from the end of their ICO.
"What we find is that once you go beyond three months, at most six months, they don't outperform other cryptocurrencies," said finance PhD student and assistant professor at Boston College's Carroll School Leonard Kostovetsky, one of two researchers in the study.
"The strongest return is actually in the first month."
"They are much lower now, so I wouldn't expect them to continue to decline at this rate," he said.
"People often look at returns and say this is a great deal, but we teach in finance that return is a compensation for risk," Kostovetsky added.
"These are stakes in platforms that have not yet been built, that have no participants yet. There's a lot of risk. The majority of ICOs do fail."


text:
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Asked: December 8, 20212021-12-08T21:37:16+05:30 2021-12-08T21:37:16+05:30Category: Number Puzzles
The radii of two concentric circles are 68 cm and 22 cm. The area of the closed figure bounded by the boundaries of the circles is
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Select one answer
4140π sq.cm.
1 1 Answer
Answer this question & earn 50 points
Mighty Ashish Guru
2021-12-08T21:38:57+05:30Added an answer on December 8, 2021 at 9:38 pm
Area bounded by two circle is
=πR^2−πr^2=π(68^2−22^2)
=π(68+22)×(68−22)
=π90×46=4140πsq.cm.
Three milk man rented a pasture A grazed 20 cows for 6 months, B grazed 40 cows for 4 months and C grazed 30 cows for 5 months. If A's share of rent is Rs.240, then the total rent of the field is
A is a working partner and B is a sleeping partner in a business. The capital of A and B are Rs.6000, Rs.9000 respectively. A received 12 1\2% for managing the business and the rest is divided in proportion to their capitals. What each gets out of a profit of ...
A B C are partners in a business. A invested 1\3, B invested 1\4 and C invested 1\5 of the capital. Find in what ratio should they share the profit.
A and B enter into partnership. A contributes Rs.8000 and B contributes Rs.10,000. At the end of 6 months they introduce C who contributes Rs.6000. After the gap of three years, they find that firm has made a profit of Rs.9660, find the share of each of them.
A, B, C subscribes Rs.5100 for a business A subscribes Rs.900 more than B, B subscribes Rs.600 more than C. Out of total profit of Rs.1020, A receives.
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text:
Ergebnis gesprochen von "Dr. Martin Luther King Jr" in Kunst & Unterhaltung
Zur Produktliste springenZur Seitennummerierung der Produktliste springen
Unterhaltung & Darstellende Künste
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Audioinhalt
Interview, Rede oder Vortrag
Sortieren nach: Relevanz Veröffentlicht Bestseller Titel Spieldauer Bewertung
Civil Rights At Crossroads
MLK Speaks: A 50th Anniversary Limited Edition Collection
Geschrieben von: Dr. Martin Luther King Jr.
Gesprochen von: Dr. Martin Luther King Jr
Originalaufnahme
Dr. Martin Luther King, Jr. was the Co-Founding President of the Southern Christian Leadership Conference in 1957. Found in the archives at the SCLC were eight never before heard audio works of Dr. King in which he prophetically articulates his vision for a better America and world. For the first time ever, these messages are being released to commemorate the 50th Anniversary of The March on Washington for Jobs and Freedom. The title of this message is "Civil Rights At Crossroads."
Who is My Neighbor
Gesprochen von: Dr. Martin Luther King Jr.
Dr. Martin Luther King, Jr. was the Co-Founding President of the Southern Christian Leadership Conference in 1957. Found in the archives at the SCLC were eight never before heard audio works of Dr. King in which he prophetically articulates his vision for a better America and world. For the first time ever, these messages are being released to commemorate the 50th Anniversary of The March on Washington for Jobs and Freedom. The title of this message is "Who Is My Neighbor."
Is the Universe Friendly?
Dr. Martin Luther King, Jr. was the Co-Founding President of the Southern Christian Leadership Conference in 1957. Found in the archives at the SCLC were eight never before heard audio works of Dr. King in which he prophetically articulates his vision for a better America and world. For the first time ever, these messages are being released to commemorate the 50th Anniversary of The March on Washington for Jobs and Freedom. The title of this message is "Is The Universe Friendly."
Domestic Impact of the War
Dr. Martin Luther King, Jr. was the Co-Founding President of the Southern Christian Leadership Conference in 1957. Found in the archives at the SCLC were eight never before heard audio works of Dr. King in which he prophetically articulates his vision for a better America and world...For the first time ever, these messages are being released to commemorate the 50th Anniversary of The March on Washington for Jobs and Freedom. The title of this message is "Domestic Impact of the War."
Lost Sheep - The God of the Lost
Dr. Martin Luther King, Jr. was the Co-Founding President of the Southern Christian Leadership Conference in 1957. Found in the archives at the SCLC were eight never before heard audio works of Dr. King in which he prophetically articulates his vision for a better America and world...For the first time ever, these messages are being released to commemorate the 50th Anniversary of The March on Washington for Jobs and Freedom. The title of this message is "Lost Sheep. "The God Of The Lost."
Stand by the Best in Evil Times
Dr. Martin Luther King, Jr. was the Co-Founding President of the Southern Christian Leadership Conference in 1957. Found in the archives at the SCLC were eight never before heard audio works of Dr. King in which he prophetically articulates his vision for a better America and world...For the first time ever, these messages are being released to commemorate the 50th Anniversary of The March on Washington for Jobs and Freedom. The title of this message is "Stand by the Best in Evil Times."


Idakoos Canada offers a great collection of fantastic Custom T-Shirts, Custom Tees, Printed Hoodies, Tote Bags, Personalized Mugs, Sweatshirts and more.
Scrubs Inc offers largest collection of cheap nursing scrubs, Get Free Shipping discount medical scrubs with all major brands of clearance scrubs Los Angeles.
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The Canadienne is one of the few historic breeds of livestock developed in Canada. It descends from cattle of Normandy and Brittany which were brought to Canada between 1601 and 1660. This population was shaped by natural selection in the rugged environment of eastern Canada, and the resulting breed became known as the Canadienne. The breed is closely associated with Quebec, and even today the majority of the cattle are found in this province.
The Canadienne was the dominant dairy type in eastern Canada until the importation of improved European breeds in the early 1800s. In 1850, the Canadian government officially discouraged the use of the Canadienne in favor of "improved breeds." This unfortunate policy was reversed in 1883, when the breed was again recognized as valuable for its superior environmental adaptation. Pure breeding was again encouraged, and a herd book was established in 1886.
The breed flourished for several decades, though it became rare again during the early to mid-1900s. The dairy industry's emphasis on high rate of production, utilizing confinement husbandry, left the Canadienne unable to compete with the Holstein. Brown Swiss genetics were introduced as a way to increase milk production, though the result was to dilute the characteristics of the Canadienne without any market advantage gain for the breed. Fortunately, pedigrees were documented and some cows continued to be bred to purebred bulls, so that pure stocks continue to exist as well as those with Swiss breeding.
The Canadienne breed is critically rare and most of the remaining animals are still found in and around Quebec as of 2008. Small herds do exist in the US. The breed merits attention for use in grass‑based dairying, especially where the quality of forage is low. Under these conditions, the Canadienne will be able to demonstrate its value to dairy farmers and thus gain a broader base of support.
Canadiennes are black, brown, tan, or russet with a pale fawn muzzle and udder. Many have a lighter colored stripe along the back. The black‑tipped horns curve up and turn back toward each other. Cows weigh about 1,100 pounds, and bulls about 1,600 pounds. Milk production averages about 15,000 pounds per lactation, with about 4.35% butterfat and 3.7% protein. Most significant is the breed's ability to produce milk on poor forage and under very challenging conditions. Few dairy breeds demonstrate this combination of hardiness and productivity as well as the Canadienne.
The Livestock Conservancy is America's leading organization working to save over 150 heritage breeds from extinction. We rely on the support of our members, grants, and donations from the public to raise the $700,000 a year needed to maintain our conservation work with rare breeds of farm animals. Click here to learn how you can help.


September 9th to September 15th, 2017 was Suicide Awareness Week here at Morgan. The purpose of this week is not only to bring awareness to the topic of suicide, but to educate people about the epidemic that is spreading across the world, and to determine how we can prevent it. Suicide Awareness Week is here to let everyone know that it is okay to reach out for help because all lives are worth living.
On Tuesday, September 12, an assembly was held during our advisory. During that assembly, Morgan students were shown a presentation. One of the most touching parts of the presentation was the video that featured many of the students saying what they are grateful for. The intention of this was to validate people and make them feel as if they mattered.
The opening slide in the presentation shown to students during advisory.
The statistics made the audience aware of the problem: "People think that we are such a small town that suicide would never happen here, that is not true, it can happen anywhere to anyone." -Ashlyn Harris.
Students learned about the warning signs suicidal people may show, and that sometimes, it isn't just a bad day, but a deeper problem. QPR training was offered September 21 for anyone that wants to be certified to take action when someone is showing these signs.
"If someone listens, or stretches out a hand, or whispers a word of encouragement, or attempts to understand a lonely person, extraordinary things begin to happen." This quote was included in one of the final slides of the presentation. The school wanted the students to walk away knowing that just simple acts of kindness show that you care. Whether they put a smile on someone's face, or make their day, these kind actions can go extremely far.
An example of the fun merchandise REACT handed out. Written on it was the website to Partners in Community.
In addition to the presentation, every day throughout the week, Mr. Webb shared a fact about suicide during the morning announcements to educate Morgan about suicide, and raise awareness to the overall topic.
During lunch, T-shirts with, "Be the change you want to see in the world" were available to all of the students. Merchandise from REACT, sticky notes with "you should be proud of yourself because… " or, "a special thing I noticed about you today is…" written on them were also available during lunch. Suicide hotlines as well were put on the walls of the school bathrooms.
As Mr. Samet explained to his Algebra 2 class one day, "We would rather have you alive and angry than dead." It does not matter how upset you think a suicidal person might be for telling an adult, or a counselor, that they need help. At the end of the day, their life should come first, and they can deal with their anger later, just being alive is most important.
Suicide is happening, and we need to do something about it. The end of 0f this widespread problem starts with awareness which is what The Morgan School is trying to spread.


Everybody's favorite vegetable during the holidays. Green beans in a creamy mushroom sauce topped with French fried onions.
Ingredients: green beans, cream of mushroom soup, french fried onions, milk, soy sauce, black pepper. This product may contain one or all of the following: artificial color, flavor or preservatives.
Single: Thaw completely in refrigerator 1 day. Bake, uncovered, at 350° for 15 minutes, until the internal temperature is at least 165°F. Stir, sprinkle with onions. Bake for 5 minutes or until onions are golden brown.
3 Servings: Thaw completely in refrigerator 1 day. Bake, uncovered, at 350° for 15 minutes, until the internal temperature is at least 165°F. Stir, sprinkle with onions. Bake for 5 minutes or until onions are golden brown.
6 Servings: Thaw completely in refrigerator 1-2 days. Bake, uncovered, at 350° for 25 minutes, until the internal temperature is at least 165°F. Stir, sprinkle with onions. Bake for 5 minutes or until onions are golden brown.


text:
February 18, 2022 (Friday)
Mr. Hiroyuki Yushita, Senior Managing Director of FEC, Called on H.E. Mr. Guillermo Juan Hunt, Ambassador of the Argentine Republic
Departure ceremony of Iranian Ambassador to Japan Morteza Rahmani Movahed
Mr. Ken Matsuzawa, President of FEC, and others attended the departure ceremony of Iranian Ambassador to Japan Morteza Rahmani Movahed, who will leave …
February 14, 2022 (Monday)
Mr. Hiroyuki Yushita, Senior Managing Director of FEC, Called on H.E. Mr. Larbi Katti, Ambassador of the People's Democratic Republic of Algeria
Mr. Hiroyuki Yushita, Senior Managing Director of FEC, Called on H.E. Mr. Baraka Haran Luvanda, Ambassador of the United Republic of Tanzania
December 28, 2021 (Tuesday)
Mr. Ken Matsuzawa, President of FEC, Called on H.E. Mr. Soe Han, Ambassador of the Republic of the Union of Myanmar
Mr. Hiroyuki Yushita, Senior Managing Director of FEC, Called on H.E. Mrs. Phongsamouth Anlavan, Ambassador of the Lao People's Democratic Republic
December 20, 2021 (Monday)
Mr. Hiroyuki Yushita, Senior Managing Director of FEC, Called on H.E. Mr. Ibrahim Bileh Doualeh, Ambassador of the Republic of Djibouti
December 8, 2021 (Tuesday)
Mr. Hiroyuki Yushita, Senior Managing Director of FEC, Called on H.E. Mr. Ovidiu Dranga, Ambassador of Romania
November 29, 2021 (Monday)
Mr. Hiroyuki Yushita, Senior Managing Director of FEC, Called on H.E. Mr. Ian G. McKay, Ambassador of Canada
Mr. Hiroyuki Yushita, Senior Managing Director of FEC, Called on H.E. Mr. Abubakar Moriki Husaini, Ambassador of the Federal Republic of Nigeria


text:
Tag: Hobbit
The Hobbit: The Battle of the Five Armies Blu-ray Review
Battle of the compression codec Yes, it's too long. No, it did not need to be three movies. But, The Hobbit is no less fun. Bilbo may be almost …
The Hobbit: The Battle of the Five Armies Theatrical Review
We've now been to Mordor and back again At some point in this trilogy of Hobbit spectacles, the Hobbit was lost. Martin Freeman's lowly Bilbo, with his face contorting …
The Hobbit: The Desolation of Smaug Blu-ray Review
For its opening breeziness, Desolation still turns into a screen hog, if not to overflowing capacity.
The Hobbit: An Unexpected Journey 3D Review
This is too often fan service and less of a film for it, over eager like an excited child.
The Lord of the Rings: Fellowship of the Ring Review
Fellowship is a film that is both too long and too short.


text:
Q: Printing text on the chart I have written a javascript page using High charts api to draw a chart.
Everything is working fine. But when I am trying to print a text on the chart I am facing some problems.
In the below URL you can check the code and running chart.
http://jsfiddle.net/uVTNU/14/
I am using the below code snippet to get the text on the chart.
var text = chart.renderer.text(
                '500',
                57 ,
                112.1
            ).css({
                color: '#F00',
                fontSize: '11px'
            }).add();

Here I have taken x and y values as (57,112.1) which has taken from inspect elements.
"180" is the place where we want to print the text.
My requirement is : we want to print the text "500" above 180.
That is why I have chosen the co-ordinates mentioned above.
But the text "500" is printing after "180" even the x and y positions are same.
Thanks in advance

A: DEMO
you need to change the x attribute in tspan , you code was changing the text x-cord tag which was not doing anything
  $.each($('svg text tspan') , function(index, value){
    var myval = 500 ; // change this variable as required
    if($(this).text() == myval){
       $(this).attr('x' , 40) ; // X-cord
        $(this).parents('text').attr('y' ,100) ; //y-cord
    }

   });

redpajama_set_name: RedPajamaStackExchange


When selling your home for cash, you can sell to a company that buys houses on cash. There are also investors who are willing to buy houses for cash and you can sell to them. You will be able to enjoy various advantages from selling your house on cash. A major advantage of selling your home for cash is that you will enjoy more speed. It can be a time consuming process to list your home with a realtor. You must find a buyer that qualifies for financing. You will be assured that the deal will fall through when you sell your house for cash.
You will not need to put more money into your home when you sell it for cash and this is an added advantage. It is hard for a buyer to buy a home that is in poor condition. You will need to replace the floors, install a new roof and even repaint. Making such improvements can be very expensive and time consuming. When you sell your home for cash, you will sell your home the way it is. You will save a lot of time and money.
Another benefit of selling your home for cash is that you will avoid paying any commission fees. A real estate agent does not work for free. You can either pay him a flat fee or a commission. You will have to pay him a certain percentage of money after you sell your home. In this case, you should definitely sell your home for cash. You will receive the full amount you will sell your house for.
You can avoid foreclosure when you sell your house for cash and this is an added advantage. You will be facing the risk of foreclosure if you pay our mortgage late. You may decide to take a loan which may not be approved.
By this time, you will be far behind on your mortgage. This is why you should consider selling your home for cash. You will avoid foreclosure by paying the amount due. You will also be left with the money to move on. Another advantage of selling your house for cash is that you will get help with inherited property. You may inherit a new home but you already have a new home. In this case, you may be forced to sell your inherited house. It will be vulnerable to theft when you leave the house unoccupied. Insuring it will also be hard and you will be exposing it to a lot of damage due to lack of maintenance.


Yes. They are widely accepted in courts too as are e-mails. The default position is normally if the person received the text doesn't agree with the content, they will respond denying it. Silence normally = acceptance.
i.e. I test you and say "Don't forget the $200 you owe me by Friday", then you would normally reply either "Ok" or "What are you talking about - I don't owe you any money. What do I owe you $200 for?"
No normal person who doesn't owe the funds would just shrug and ignore it. They would dispute it and promptly.
Keep the texts and e-mails. They count just as much as a registered letter delivered by mail in this day and age.
Hi, I hope you resolved your problem in a positive way. I'm sorry this happen to you. First of all if the day home provider wanted to change the hours, she should give parents a month notice, so they could arrange different solution for them. I'm a day home provider as well, and I would never do that to the parents, plus not everybody is so lucky to start their work after 9 and finish 4 or before 4. Other thing is if she changed her hours, how about the fee? Did said that she will lower the monthly payments? You said you gave her a month cancellation, she didn't have a right to keep the payment, I hope you resolved this in a positive way though. Unfortunately, some day home providers go on a power trip, and that's wrong. I'm doing this for about 20 years, and I hea rd lots of stories, and many of them not pleasant. Personally, I'm sensitive about catering for children and working with parents. No, this is not normal way of changing the hours... and since you gave her 1 month notice she doesn't have a right to keep the deposit. That was her who validated the contract. I'm sorry this happen to you.