text:
Q: Angular 4 - handle two events at the same time I want to handle a click event + CTRL keypress event in the same function in my component.ts file, but I don't seem to find a solution anywhere. I've tried:
@HostListener("click")
    onDropdownItemClick( evt: keyboardEvent) {
        console.log(evt.keyCode);
    }

but it just returns "ERROR TypeError: Cannot read property 'keyCode' of undefined"
I've also tried this too:
@Component({
        selector: '....',
        templateUrl: '....',
        host: {
            '(window:keydown)': 'findKey($event)',
            '(window:mousedown)': 'findKey($event)'
        }
   });

findKey(event) {
         if(event.ctrlKey && event.which === 1){
               console.log("CTRL + mouse-click");
        }
    }

But it's not working either. Anyone have suggestions on how to catch both events at the same time?

A: The MouseEvent event provides a ctrlKey property that allows to read the state of the Ctrl key state when the click happened
@HostListener("click", ['$event'])
onDropdownItemClick( evt: MouseEvent) {
  console.log('clicked - with ctrl pressed:', evt.ctrlKey);
}

https://developer.mozilla.org/en-US/docs/Web/API/MouseEvent/ctrlKey

Just store the status of the control key in a field and read it in the click event:
ctrlDown = false;

@HostListener('window:keydown.ctrl')
onCtrlDown() {this.ctrlDown = true; }

@HostListener('window:keydown.ctrl')
onCtrlUp() {this.ctrlDown = false; }

@HostListener("click")
onDropdownItemClick( evt: keyboardEvent) {
  console.log('clicked - with ctrl pressed:', this.ctrlDown);
}

If above doesn't work please try
@HostListener('window:keydown', ['$event'])
onCtrlDown(event) {this.ctrlDown = event.ctrlKey; }

@HostListener('window:keydown')
onCtrlUp() {this.ctrlDown = false; }


7 3 powerstroke engine wiring harnes Perhaps more importantly is that a cummins turbo diesel v8 engine is in the mix and an integrated gooseneck hitch with Initial startup time will increase and put wear on the engine. Unplug the wiring harness while checking it for cracks the firing order is written on the valve cover 1273456 and 8. Tier iv compliant cummins qsb 6.7l 232 hp 173 kw diesel engine.
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text:
Q: Undefined is not a function - Evaluating require.getModules() || React native || inline require || Enable Unbundling I am trying to unbundle react native (inline require) and I want to investigate the loaded modules.
react native version - ^0.49.3
Followed official documentation https://facebook.github.io/react-native/docs/performance#investigating-the-loaded-modules
But it is throwing an error Undefined is not a function - Evaluating require.getModules()
Anyone tried it before or faced a similar issue?

A: just remove the code you added to create moduleNames for preloading in file
index.js or index.ios.js|index.android.js
and build again

redpajama_set_name: RedPajamaStackExchange


text:
Bristol crime map: Every single report made to the police from your street in September 2017
Our interactive map allows you to zoom in on your area and look at what crimes were committed on your street
Are you living in one of Bristol's crime hotspots?
We have put together an interactive map that shows all of the crimes committed in Bristol and the surrounding areas in September this year.
You can use the map to find out what crimes have been recorded in your area - even on your street. Explore the city by zooming in and out and scrolling left to right.
Then click or hover over the coloured markers to reveal the details of each individual crime.
All data comes from Avon and Somerset Constabulary and were provided by the police.uk website.
Use the map here -
In September alone there were 7,503 crimes reported to the police.
Of these incidents, 1,868 were identified as violent and sexual offences and 1,524 were anti-social behaviour.
Bristol's most burgled streets revealed - is your home in a burglary hot spot?
The latest police figures have revealed a rise in crimes such as violent and sexual offences and bicycle thefts compared with the same month last year.
Use the map below of the crime statistics from September 2016 to compare with this year's -
But other offences have seen a decrease, such as anti-social behaviour and criminal damage and arson. Drug offences also saw a slight decline.
Anti-social behaviour - 1, 524
Bicycle theft - 164
Burglary - 508
Criminal damage and arson - 553
Drugs - 101
Possession of weapons - 29
Public order - 787
Rubbery - 75
Shoplifting - 549
Theft from the person - 47
Vehicle crime - 652
Violent and sexual offences - 1,868
The law says that someone is behaving in an antisocial manner if:
they are acting in a manner that is causing, or is likely to cause, alarm or distress, or
they are doing several things over a period of time that cause, or are likely to cause, alarm or distress to at least one person living in another household.
Whatever the problem is, it has to have happened more than once to at least one person for police to record it as anti-social behaviour.
Violent crime covers a wide range of offences, from minor assaults such as pushing and shoving that result in no physical harm through to serious incidents of wounding and homicide.
Bristol's most dangerous streets – these are the roads with the highest reports of violence and sexual offences
Grime star Tion Wayne, real name Dennis Odunwo, stamps on a man during a brawl outside a Bristol nightclub where he had earlier been performing (Image: CPS)
Sexual offences include rape, sexual assault and unlawful sexual activity against adults and children, sexual grooming and indecent exposure.
Burglary is typically defined as the unlawful entry into almost any structure (not just a home or business) with the intent to commit any crime inside.
No physical breaking and entering is required - the offender may simply trespass through an open door. Unlike robbery which involves use of force or fear to obtain another person's property, there is usually no victim present during a burglary.
Criminal damage is the intentional and malicious damage to the home, other property or vehicles and includes graffiti.
Arson is the act of deliberately setting fire to property, including buildings and vehicles.
Number of violent crimes and sexual offences dealt with by way of an apology in Avon and Somerset revealed
Bradley Stoke Arson victims Aaliyah and Saeed Hussain (Image: Michael Lloyd)
Other theft is a broad category, which covers theft not defined by other categories (i.e burglary, vehicle theft etc.,).
Shoplifting involves taking goods from a shop without paying for them first.
Public order offences can be anything from violent disorder, affray, disorderly behaviour or drunk and disorderly - basically, anything that could cause anyone present to be afraid.

redpajama_set_name: RedPajamaCommonCrawl


Hi all, for anyone out there who may be interested in a L4 Trg and Assessment then westcoastkayaking run by Martin Duffy in Sligo might have a course for you. You will need your REC3 and Coastal Navigation Cse completed in advance.
This notice is copied from the ISKA website.
Last Edit: 6 months 1 hour ago by MICHAEL CARROLL.


Top-down attempts to "rebalance the economy" have failed so many times that politicians proposing further interventions should think twice before doing so. Unfortunately, they show no sign of stopping.
Philip Hammond and Ruth Davidson have both lent their support to a new tax on business. Both floated the idea of an "Amazon tax" — a special levy on online sales, to "save the British high street" and "level out the playing field" between web giants and small shops, in the Chancellor's words.
I doubt would-be dirigistes will find this proposition a difficult sell, either to Parliament or the general public. Politicians of all stripes love claiming to stand up for the little guy — in this case, the noble, beleaguered UK high street against the murky world of online retail — and ideas of justice and fair play are deep-seated in the British psyche. But couching policies in the language of equality doesn't necessarily make them fair.
These proposals will also be aided by our national tendency to regard the high street with a wistful, and often unmerited, affection.
Nowhere is this clearer than in Britain's love affair with that classic high street anachronism — Woolworths. With its tightly-packed aisles of mismatched merchandise, a trip to Woolies could be a surreal experience. Unsurprisingly, a store selling everything from thongs to army knives to pic n' mix had little in the way of clear brand identity. It did painfully little to move with the times, unlike high street siblings like John Lewis. Yet, in spite of all this – perhaps for old times' sake — the decline of Woolworths in the mid-noughties was mourned like the passing of a much-loved relative or favourite pet.
There is more than a hint of this rose-tinted sentimentality at play in recent proposals for taxes on the digital economy; but nostalgia and politics are a dangerous mix.
We risk forgetting, in our righteous anger, logical reasons why online firms pay less tax than physical shops.
Business rates are levied according to the market value of property businesses own — which explains why a department store on prime real estate in Oxford Circus will end up paying higher rates than a company like Amazon, operating from out-of-town warehouses in areas of lower property value.
Indeed, the genius of Amazon's business model hinges on this very lack of physical presence. It allows them to bypass many of the additional costs associated with bricks-and-mortar outlets. These savings translate into gains for the consumer in the form of lower prices, and in Amazon's case, added convenience — all of which drives productivity and new forms of consumption by freeing up time and expenditure for other uses. What's not to like?
It's akin to a swimmer pioneering a new form of breaststroke that will shave seconds off the world record time — only for a change in the rules to bar them from competing. Seen in this light, the Chancellor's remarks are less a question of levelling the playing field — and rather more "all must have prizes".
Likewise, any special tax which seeks to punish online firms for their competitive advantages may equalise outcomes in the short term — but at the expense of consumer welfare and future innovation. In the long-run, this would be a perverse way to approach Britain's thriving digital sector, the biggest driver of growth in our economy — particularly at a time when competitors around the world are moving to attract tech start-ups into their markets.
None of this is to say that high street shops don't face huge obstacles to success — they emphatically do. But government's priority should be on removing the obstacles (some of which are state-imposed) that make it harder for physical shops to compete.
For a start, local councils should reconsider the "War on Motorists", and other ways in which they have made shopping in city centres a needlessly expensive and torturous experience for many would-be buyers.
We should also consider tactical reforms of business rates. By focusing on rental, rather than land value, our current setup creates perverse incentives by penalising shopkeepers looking to drive sales by refurbishing or converting their premises. In a retail environment where consumers are increasingly favouring experiences over products, our tax code should not disadvantage retailers trying to tap into the "experience economy", for example, by converting part of their bookshop into a cafe, or installing a nail bar in their clothes shop.
Perhaps most importantly, the high street must adapt to 21st century shopping habits. Unlike the housewives who fuelled the British High Street boom in the 1960s, most modern women work full-time and require shops that stay open past 5 or 6pm. It's no coincidence that most online shoppers are women. Yet many high street retailers routinely stay open all morning with virtually no customers, then close their doors while most people are still in the office. Why?
In this climate, our strict Sunday trading legislation seems less a quaint throwback — and more an actively harmful, anti-competitive dinosaur. Relaxing these laws would genuinely help level the playing field for retailers competing with e-commerce.
There will always be losers when technological change rears its head — but we should not be afraid of creative destruction. Remember, the same transformative process that leaves Woolworths and their ilk by the wayside also breeds the innovative, consumer-centric companies of the future — both on and off the high street.
This article originally appeared in CapX.
Amazon tax collection policy has changed over the years.In the U.S state and local sales taxes are levied by state and local governments, not at the federal level. In most countries where Amazon operators, a sales tax or value added tax is uniform throughout the country, and Amazon is obliged to collect to from all customers. Many U.S states have passed online shopping sales tax laws designed to compel Amazon.com and other e-commerce retailers to collect state and local sales taxes from its customers.


Namibian President, Hage Geingob, has expressed the need to expropriate land and redistribute it to the majority black population.
The current proposal aims to "transfer 43 percent, or 15 million hectares (58,000 square miles) of its arable agricultural land, to previously disadvantaged blacks by 2020. At the end of 2015, 27 percent has been redistributed, according to the Namibia Agriculture Union".
In a similar vein, South Africa, Namibia's neighbour and regional economic powerhouse, is also in the process of amending land ownership laws.
"We need to revisit constitutional provisions which allow for the expropriation of land with just compensation, as opposed to fair compensation, and look at foreign ownership of land, especially absentee land owners".
Reuters notes that "in South Africa, thousands of black Namibians were driven off their land in the 19th and 20th centuries, banished to barren and often crowded homelands known as Bantustans while being denied official ownership or tenure rights".
"It is in all our interest, particularly the "haves", to ensure a drastic reduction in inequality, by supporting the redistributive model required to alter our skewed economic structure. We should all be cognizant of the fact that this is ultimately an investment in peace".
In the second quarter of 2018 Namibia's GDP contracted for the ninth straight quarter, the longest such streak since at least 2008.


text:
Open governance needs civic engagement, transparency: Czech senator
Czech Senate President Miloš Vystrčil.
Taipei, Dec. 2 (CNA) Civic engagement, transparency, and making use of technology and innovation are the key to open governance, Czech Senate President Miloš Vystrčil told the 2021 Open Parliament Forum in Taipei Thursday.
In a prerecorded message played during the lunch recess at the forum, Vystrčil said he believed the roles played by active citizenship and civic engagement remained "essential to the functioning of a standard democracy society."
"Without the interests of citizens, without their willingness to engage in a dialogue and, in particular, in controlling government policies and politicians and the legislatures that are created, the very likely danger is that democracy will become sick, and that open governance will gradually begin to die," he said.
Other key principles of open governance were transparency and responsibility, he continued.
"Transparency is an important attribute of open governance and open legislature as it ensures the public availability of any public information that the government or legislature possesses in its decision-making," Vystrčil said.
According to Vystrčil, the government and legislature should explain and defend their decisions and actions and be held accountable for their decisions, adding that making technology and innovation accessible to the public was also an important principle of open governance.
Successful implementation of open governance and open lawmaking can be recognized by citizens showing trust in their state, he said.
"If a citizen trusts his state, his government, his legislature, then the entire state is much stronger and more resilient to outside political, social, economic, environmental, and other types of influences," he concluded.
A Taiwan-friendly senior lawmaker, Vystrčil is the second-highest-ranking official in the Czech Republic after the president.
He had previously led a delegation that visited Taiwan from late August to early September 2020, becoming the highest-level official ever to visit Taiwan.
The visit came amid warming relations between Taiwan and the Czech Republic over the past year, which also saw Prague donate 300,000 COVID-19 vaccine doses to Taiwan in late August.
The two-day forum, entitled "Open Parliament in a Post-COVID Context: Global Examples of Resilience and Planning for 2022 and Beyond," has been organized by Taiwan's Ministry of Foreign Affairs, the Legislative Yuan, and the National Democratic Institute, a U.S.-headquartered nonprofit.


text:
Dascha Polanco, född 3 december 1982 i Santo Domingo, Dominikanska republiken, är en amerikansk skådespelerska. Hon är mest känd för sin roll som internen Dayanara "Daya" Diaz i tv-serien Orange Is the New Black. Inför den tredje säsongen av Orange Is the New Black blev Polancos karaktär en av huvudrollerna..

Polanco arbetade tidigare som medicintekniker och chef på ett sjukhus i Brooklyn innan hon registrerade sig på en skådespelarkurs och fick rollen i Orange Is the New Black. Hon har under hela sin uppväxt och skoltid tagit dramaklasser och varit intresserad av teater och film.

Polanco har tre barn. Hennes mor dog kort innan hon började på Orange Is the New Black. Palenco även spanska på grund av sitt dominikanska ursprung.

Referenser

Externa länkar

Födda 1982
Dominikanska skådespelare
Kvinnor
Levande personer

redpajama_set_name: RedPajamaWikipedia


Cumberland rd sports ground was in Cumberland rd.
Since I do not know where Cumberland Rd was, your reply was unhelpful thank you.
The link bellows takes you to a Ordnance Survey map. I think the entrance was at the eastern end of Elkington Road was the.
Number 101 Cumberland Road was the Duke of Cumberland pub.
Mick, many thanks for your link, most helpful. Cumberland Rd was well away from Ashburton school, which was on the corner of Russel Rd & Freemasons Lane. The map clearly shows a large recreation ground opposite the school where the annual sports day was held.
Cumberland rd sports ground was at he end of palmers rd. through an alley way with bollards. & tucked away on the right.
So it was between palmers rd & new barn st.
Palmers rd started at prince regents lane practicly opposite the old fire station.
An easier reference was that it was at the back of Plaistow Grammar School. Was it originally the play area for this school?
Hi Alan, now I am confused, PGS was in PR Lane towards Greengate.
Thankfully Micks link to a Ordnance Survey map brings me back to reality.
Hi Ken Cumberland sports field was behind PGS as you walked along Prince Regents Lane.
I,m surprised that you cannot remember the sports ground as a pupil at Shipman Road I can remember going there for sports day with the school[in a previous post I mentioned "throwing the cricket ball" and the"slow cycle race".
obviously we used two other sports grounds "The Rec" and by the old gun sight along the old Beckton Road .
Thank you all for your advice on location of Cumberland Rd sports ground.
Harry, the year that I entered for throwing the cricket ball, Andy Nelson, he of West Ham fame, won the contest.


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text:
NFL Playoffs: Quarterback Trust Rankings Part II
In wake of the AFC and NFC Wild Card weekend, TSFJ provided the first edition of the Quarterback Trust Power Rankings. Like most lists or rankings, it ignited some controversy. To no surprise, some quarterbacks climbed near the top while others remained stagnant. So let's take a look at our second edition of the rankings for the NFL Divisional Round.
8. Brock Osweiler, Houston Texans
Last week's quarterback duel between Osweiler and Connor Cook was one for the ages. I'm kidding.The matchup between both signal-callers resembled a clash between famed movie quarterbacks Shane Falco and Uncle Rico. While neither Osweiler nor Cook set the world on fire, someone had to come out victorious. To no surprise, that was Osweiler and the Texans thanks to Oakland being riddled by injuries. With that said, the $72 million quarterback has one more playoff victory than Andy Dalton, but he's still unreliable.
7. Dak Prescott, Dallas Cowboys
Dak makes his playoff debut against the Packers. We've witnessed rookie quarterbacks such as Ben Roethlisberger, Mark Sanchez (not a typo) and Joe Flacco have some success in the postseason, but on the other hand, rookie quarterbacks in the postseason aren't a standard. For Dak it won't surprise me if he remains his usual cool self, but in the playoff pressure-cooker, it remains an unknown.
6. Alex Smith, Kansas City Chiefs
In a Sunday showdown against Pittsburgh, Alex Smith and the Chiefs have their work cut out for them. They face a team that humiliated them in route to a 43-14 defeat in Week 4. For Kansas City, it's imperative not to mirror the play from earlier in the season — that is to say the often-criticized quarterback has to play at a high level. Even though Alex has shown the ability to produce in the postseason, the matchup against the Steelers might be too much to handle.
5. Matt Ryan, Atlanta Falcons
As an eye-opener, Matty Ice crept up in the rankings without playing. The reason is because the MVP candidate is playing at home. As seen in Wild Card Round, all home teams came out victorious. It also helps that he's had playoff success against the Seattle Seahawks. In 2013, he defeated them in the Divisional Round, which also happens to have been Atlanta's last playoff victory. Granted, this is a totally different Seattle team, but any mental edge is needed — especially when you haven't had much playoff success.
4. Russell Wilson, Seattle Seahawks
Despite Ryan's rise in our rankings, he hasn't done enough to surpass Wilson. With a victory in last week's Wild Card game, Russell's playoff record stands at 8-3. The playoffs are where he and Seattle thrive — therefore, it's easy to trust him on the road this weekend.
3. Ben Roethlisberger, Pittsburgh Steelers
Roethlisberger and the Steelers waltzed through a victory against the Dolphins. This weekend, he and Pittsburgh face a true test in playing the Chiefs. Kansas City has one of the best defenses in the NFL, but that isn't enough to stop the potent Steelers offense. Although Ben is nursing a foot injury, his playoff experience and supporting cast allow his trust level to stay where it was a week ago.
2. Aaron Rodgers, Green Bay Packers
I'd like to apologize to Rodgers and Packers faithful for ranking him so low last week (he was ranked fifth). After fending off his recent playoff hex, it's safe to say that his postseason swagger is back. Green Bay torched the New York Giants for 38 points, led by the golden arm of Rodgers. This weekend, he and the Packers take their aerial show on the road to Dallas. Although the Cowboys are the No.1 seed, it's hard not to trust Rodgers in the role of the underdog.
1. Tom Brady, New England Patriots
The video below indicates how Tom Brady feels after sustaining his top spot in our rankings.
Previous Previous post: NFC Divisional Round's Four Most Important Players
Next Next post: Students Of The Game: Is Learning History A Necessary Course For Greatness?


text:
Бретт Ліндрос (,  2 грудня 1975, Лондон) — колишній канадський хокеїст, що грав на позиції крайнього нападника. Грав за збірну команду Канади. Молодший брат відомого хокеїста Еріка Ліндроса.

Ігрова кар'єра
Хокейну кар'єру розпочав 1992 року.

1994 року був обраний на драфті НХЛ під 9-м загальним номером командою «Нью-Йорк Айлендерс».

Усю професійну клубну ігрову кар'єру, що тривала 2 роки, провів, захищаючи кольори команди «Нью-Йорк Айлендерс».

Загалом провів 51 матч у НХЛ.

Виступав за збірну Канади.

Статистика

Клубні виступи

Збірна

Посилання

Канадські хокеїсти
Уродженці Лондона (Онтаріо)
Гравці збірної Канади з хокею
Хокеїсти «Нью-Йорк Айлендерс»
Задрафтовані «Нью-Йорк Айлендерс»


text:
\section*{Introduction}
Since the discovery of high-Tc Cuprates\cite{highTc}, the ground state phase diagram of the repulsive-$U$ Hubbard model in the strong coupling limit has become one of the most important open problems in condensed matter physics\cite{RVB,PatrickRVB}.
Infinite-$U$ Hubbard model is a simple looking but challenging many body problem that has defied exact understanding so far. While spin and charge degrees of freedom are manifestly decoupled, they might cooperate in surprising ways giving rise to novel many body states that are yet to be understood. In this paper, we present one such surprise, namely a Nagaoka state\cite{Nagaoka} nurturing a $p + ip$ superconductivity in $2$D honeycomb lattice infinite-$U$ Hubbard model at small but finite doping(its noninteracting counterpart is described by Dirac pockets), at the expense of only a tiny reduction of its own saturated ferromagnetism.

At exact half filling, all  low energy states are exhausted by the 2$^N$($N$ is the total number of sites) fold degenerate ground states generated by the localized free (dangling) spin-half moments.  Spins have no dynamics of their own. Upon doping,  holes hop and scramble spin configurations. In general, coherent delocalization of charges becomes difficult and kinetic energy gets frustrated, except when we have saturated ferromagnetism and a simple fermi sea as a ground state. While coherent delocalization of charges occurs through Bloch state formation, Pauli principle increases the kinetic energy, because only up spin bands are used. However, the real question is, are there other organizations of charge and spin degrees of freedom that reduce kinetic energy frustration and beat the Nagaoka state?

There are conflicting results for the stability of Nagaoka state in square lattice infinite-$U$ Hubbard model at small hole doping. An analysis by Wen and Doucot indicates\cite{WenNagaoka} that even for 2-holes the ground state is not fully spin polarized. There is also an argument given by Trugman\cite{TrugmanNagaoka} that in any finite system the lowest energy state cannot have bound holes.  Series expansion results also cast doubt on stability of Nagaoka ferromagnet at any finite doping\cite{seriesNagaoka}. Recent numerical calculations\cite{DMRGNagaoka} come to opposite conclusions. Therefore, further analysis of the intriguing situation for square lattice and other lattice geometries are called for.

Keeping the above in mind, we report a detailed state-of-art Grassmann tensor product state(GTPS) numerical calculation\cite{FrankfPEPS,ifPEPS,fermionicTPS,GPEPS,finitefPEPS,GuGTPS,Gumethod,honeycombtJ,squaretJ1,squaretJ2}, an effective theory and a physically motivated approximate microscopic analysis of the honeycomb lattice infinite-$U$ Hubbard model with hole doping $\delta = 0\sim0.2$.  We find a surprising result that Nagaoka ferromagnet can support and nurture a $p + ip$ superconducting state. It is a win-win situation in the sense it grows a $p + ip$ order parameter only at the expense of a tiny reduction of its saturated magnetism, and gains an additional stability of its own ferromagnetism. What we have found can be interpreted as an interesting ${\it zero ~ point ~ reduction}$  of saturation ferromagnetism, unknown in the case of standard quantum ferromagnets.  For realistic systems with large but finite $U$, the $p+ip$ SC state has an instability towards a potential non-Fermi liquid state; however, by applying a Zeeman field,
the $p+ip$ SC state can be stabilized.

\section*{Results}
\emph{Ground state energy and magnetization} -- It is well known that the Hubbard model with strong repulsive interaction can be effectively described by the $t-J$ model\cite{tJ}:
\begin{equation}
H_{t-J}=t\sum_{\langle ij\rangle,\sigma
}(\tilde{c}^\dagger_{i,\sigma}
\tilde{c}_{j,\sigma}+h.c.)+J\sum_{\langle ij \rangle}\left(\vec S_i
\cdot\vec S_j-\frac{1}{4}n_in_j\right),\nonumber
\end{equation}
where $\tilde{c}_{i,\sigma}\equiv c_{i,\sigma}(1-n_{i,\bar\sigma})$ is the electron annihilation operator defined in
the no-double-occupancy subspace and $J=4t^2/U$. It is obvious that the infinite-$U$ limit corresponds to the $J=0$ limit.
Here we use a translationally invariant GTPS variational ansatz to investigate the possbile ground state phase for $J=0$, which is specified by just two different Grassmann tensors $\textbf{T}_A,\textbf{T}_B$ on sublattices $A,B$ in each unit cell(see the method section for a detailed explanation). We then use the imaginary time evolution method\cite{ImagTPS,Gumethod} to update
the GTPS from a randomly initialized state. Finally we use the weighted
Grassmann-tensor-entanglement renormalization group (wGTERG)
method\cite{GuGTPS,Gumethod} to calculate physical quantities.
The total system size is up to $2\times 27^2$ sites and all
calculations are performed with periodic boundary conditions(PBC). The
largest virtual dimension of the GTPS considered is $14$. To ensure the
convergence of the wGTERG method, we keep $D_{cut}$ (defined in
Refs.~\cite{GuGTPS,Gumethod}) up to $160$ for $D=10,12$ and $196$ for $D=14$ , which
gives small relative errors for physical quantities of order $10^{-3}$.

As seen in Fig. \ref{fig:energy}, the ground state
energy shows a marked increase in $D$ dependence as
hole doping $\delta$ increases(a chemical potential term is added to control $\delta$). As a benchmark, we perform the density matrix renormalization group(DMRG)\cite{DMRG1992}
calculations for a small cluster with $N=54$($2\times 3\times 9$) sites under PBC.
DMRG is the only unbiased
method for frustrated systems that avoids the sign problem, but it is
restricted to relatively small systems, especially for PBC.
To ensure the convergence of the DMRG calculation with PBC,
we keep up to $8000$ states and make the truncation errors
less than $10^{-9}$ in our $N=54$ calculations. Up to $D=14$, we
find a systematic consistency for ground energy with both methods for $\delta < 0.25$.
We also compare with the Nagaoka state -- a fully polarized half metallic state(HMS), and find our ground state energy is significantly lower. This indicates the instability of HMS in honeycomb lattice infinite-$U$ Hubbard model at finite doping.

Despite of the instability of HMS, we find the ferromagnetic(FM) magnetization
$m=\sqrt{{\langle S^x_{i} \rangle}^2+{\langle S^y_{i} \rangle}^2+{\langle S^z_{i} \rangle}^2}$
is still extremely close to the fully polarized HMS at low doping. As seen in the insert of Fig. \ref{fig:energy}, up to $D=14$, we find $m/m_{\rm{max}}\sim 0.99 $ for $\delta<0.2$(e.g., $m/m_{\rm{max}}\sim 0.991$ for $\delta=0.1$) while $m=0$ for $\delta>0.2$, which is similar to recent DMRG results for square lattice infinite-$U$ Hubbard model\cite{DMRGNagaoka}. (It is clear that the non-vanishing $m$ for $D=10,12$ cases is due to a local minimum effect.)We also observe $\langle n_{i \in A} \rangle=\langle n_{j\in B} \rangle$ for $\delta<0.25$
and there is no commensurate charge density wave(CDW) order.

\begin{figure}[t]
{\includegraphics[width=0.4\textwidth]{energy.pdf}} \caption{(Color online)Ground
state energy as a function of doping. As a benchmark, we performed
DMRG calculation for a small cluster with $N=54$ sites under PBC.
Insert: FM magnetization as a function of
doping.}\label{fig:energy}
\end{figure}

\emph{The emergence of $p+ip$ superconductivity} --
Next we turn to the interesting
question of whether the doped honeycomb lattice infinite-$U$ Hubbard model
supports superconductivity or not, and if so, what
its pairing symmetry is. To answer this question, we calculate the real space
SC order parameters in the spin triplet channel
(the singlet channel vanishes due to the presence of FM order).
Since the triplet pairing order parameter has three independent
components $\vec\Delta_t = \frac{1}{\sqrt{2}}c_{i,\alpha} (i\sigma^y
\vec\sigma)_{\alpha\beta}
  c_{j,\beta}$($i \in A$, $j \in B$), we can define the amplitude of
triplet order parameter as $\Delta_t = \sqrt{\vec\Delta_t^* \cdot
\vec\Delta_t}$. Because we use a
chemical potential to control the hole concentration, the charge
$U(1)$ symmetry can be spontaneously broken in the variational
approach, which allows $\Delta_t$ to be measured directly rather
than through its two-point correlation function. As shown in the
main panel of Fig. \ref{fig:SC}, up to $\delta=0.2$ we find a
non-zero triplet SC order parameter for the whole region and $\Delta_t$ is almost $D$ independent for $\delta<0.1$.
By measuring the SC order parameters for the three inequivalent
nearest-neighbor bonds, we found
$\Delta_{t;a}^{x(y,z)}/\Delta_{t;b}^{x(y,z)}\simeq \Delta_{t;b}^{x(y,z)}/\Delta_{t;c}^{x(y,z)}\simeq \Delta_{t;c}^{x(y,z)}/\Delta_{t;a}^{x(y,z)}\simeq e^{i\theta}$
with $\theta=\frac{2\pi}{3}$(see Table \ref{phase}).
This pairing is consistent
with the $p+ip$ pairing symmetry. We note that the above result is quite nontrivial since we start with a
completely random state without pre-assuming SC order.
\begin{table}[h]
\begin{tabular}{|c|c|c|c|}
\hline
Doping & $\delta=0.069$ & $\delta=0.102$ & $\delta=0.168$  \\
\hline
$\Delta^{x,(y,z)}_{t;a}/\Delta^{x,(y,z)}_{t;b}$ & (-0.500,0.866)   &  (-0.500,0.866) & (-0.500,0.866) \\
$\Delta^{x,(y,z)}_{t;b}/\Delta^{x,(y,z)}_{t;c}$ & (-0.500,0.866)   &  (-0.500,0.866) & (-0.499,0.865) \\
$\Delta^{x,(y,z)}_{t;c}/\Delta^{x,(y,z)}_{t;a}$ & (-0.500,0.866)   &  (-0.500,0.866) & (-0.500,0.866) \\
\hline
\end{tabular}
\caption{Starting from a randomly initialized GTPS ansatz, we observed $\Delta_{t;a}^{x(y,z)}/\Delta_{t;b}^{x(y,z)}\simeq \Delta_{t;b}^{x(y,z)}/\Delta_{t;c}^{x(y,z)}\simeq \Delta_{t;c}^{x(y,z)}/\Delta_{t;a}^{x(y,z)}\simeq e^{\frac{2\pi i}{3}}=(-\frac{1}{2},\frac{\sqrt{3}}{2})$ for the (variational) ground state obtained from imaginary time evolution.(Here we use the data with inner dimension $D=12$ as an example.)}\label{phase}
\end{table}

\begin{figure}[t]
{\includegraphics[width=0.4\textwidth]{SC.pdf}} \caption{(Color online)Triplet SC order
parameters as a function of doping. Insert: "condensation energy" $\Delta E$ as a function of
doping.}\label{fig:SC}
\end{figure}

We find
the SC and FM order coexist in the regime $0<\delta<0.2$.
 We further check the
internal spin direction of the triplet pairing vector $\vec\Delta_t$ and find it is
always perpendicular to the FM order parameter $\langle
\v S_i\rangle$. At larger doping close to
$\delta \sim 0.2$, the triplet order parameter has a very strong $D$
dependence. This indicates a possible phase transition around $\delta \sim 0.2$, which is consistent with
our previous magnetization result. For square lattice infinite-$U$ Hubbard model,
recent DMRG results suggest that phase separation might occur for $\delta>0.2$\cite{DMRGNagaoka}.
On the contrary, for honeycomb lattice infinite-$U$ Hubbard model,  our DMRG results on small clusters don't support phase separation as well as other translational symmetry breaking competing order, e.g., strip order, in the whole region for $\delta<0.25$.  Therefore, we confirm that the observed $p+ip$ SC state is stable for $\delta<0.2$.

\emph{Instability and stability of the $p+ip$ SC state} -- Although the infinite-$U$ Hubbard model is interesting theoretically, in realistic materials, $U$ is always finite. To investigate the instability of $p+ip$ SC state against a small $J$, we perform both GTPS calculation and DMRG calculation with $t/J=30$. For inner dimension $D=10,12,14$, we
find a systematical consistency for ground energy with both methods for $\delta < 0.25$.\footnote{Again, in the GTERG algorithm, we keep $D_{cut}=160$ for $D=10,12$ and $D_{cut}=196$ for $D=14$ to ensure that the relative energy error is less than $10^{-3}$.}
As seen in Fig. \ref{fig:energy50}, we find the ground state energy is lower than HMS, which clearly shows the instability of HMS. Furthermore, we find that the FM magnetization $m$ vanishes for all $\delta<0.25$, which is quite different from the infinite-$U$ case.

To understand the nature of the ground state phase for large but finite $U$, we further measure the triplet SC order parameter. As seen in the insert of Fig. \ref{fig:energy50}, we find that $\Delta_t$ monotonically decreases with the increase of  $D$, indicating that the $p+ip$ SC order parameter vanishes in $D\rightarrow\infty$ limit. We also measure the AF magnetization and find it vanishes for $\delta>0.1$. All these results suggest a new quantum phase emerges for $\delta>0.1$ with $t/J=30$. We will develop an effective field theory to understand this new phase later; for now, we ask how can we stabilize the $p+ip$ SC state at large but finite $U$.

Since the observed $p+ip$ SC state in the infinite-$U$ limit always coexists with an FM ordered state, it is not surprising that a Zeeman field term might stabilize the $p+ip$ SC state. We perform the GTPS calculation for $\delta \sim 0.2$ with a Zeeman field term, e.g., $h S_z$, to confirm this. As seen in Fig. \ref{fig:field}, a phase transition clearly occurs around $h\sim J$. The FM magnetization $m$ suddenly jumps to $m/m_{Max}\sim 0.98$ for $h > J$. For $h<J$, the triplet SC order parameter $\Delta_t$ shows a very strong $D$ dependence, again implying that the $p+ip$ SC order vanishes in the $D\rightarrow\infty$ limit. On the contrary, for $h >J$, $\Delta_t$ saturates at large $D$, e.g., $D=12,14$, which is very similar to the infinite-$U$ case at low doping and indicates the emergence of $p+ip$ SC order. Thus, we conclude that at finite $U$, a Zeeman field of order
$J$ is sufficient to stabilize the $p+ip$ SC state. In realistic materials, the Zeeman field term can be realized by applying in-plane magnetic field.

\begin{figure}[t]
{\includegraphics[width=0.4\textwidth]{energy50.pdf}} \caption{(Color online) Ground
state energy as a function of doping for $t-J$ model at $t/J=30$. As a benchmark, we performed
DMRG calculation for a small cluster with $N=54$ sites under PBC.
Insert: $p+ip$ SC order parameter as a function of
doping.}\label{fig:energy50}
\end{figure}

\begin{figure}[t]
{\includegraphics[width=0.4\textwidth]{field.pdf}} \caption{(Color online)FM magnetization $m$ and triplet SC order
parameters $\Delta_t$ as a function of Zeeman field for $\delta \sim 0.2$.}\label{fig:field}
\end{figure}

\emph{Spin-charge separation and skyrmion current mediated pairing} -- Now the central question would be: what are the key mechanisms for the intriguing $p+ip$ SC state. As the numerically observed FM magnetization in $p+ip$ SC state is extremely close to the fully polarized HMS, it is very natural to assume HMS as the "normal" state. Thus we can define the "condensation energy" via $\Delta E=E_{\rm{HMS}}-E_0$($E_0$ is the true ground state). As seen in the insert of Fig. \ref{fig:SC}, the $54$ sites DMRG results(which are consistent with GTPS results)show an approximately linear increase of $\Delta E$ as function of doping. For $\delta <0.15$, we can approximately fit $\Delta E \sim 0.1 \delta t$. In addition, the $p+ip$ SC ordering parameter also increases linearly and can be approximately fitted as $\Delta_t \sim 0.07\delta $. All these observations strongly support the novel phenomenon proposed by P.W.Anderson\cite{RVB}: spin-charge separation!

To construct an effective field theory, we begin with the Schwinger boson representation and decompose the electron operator as $c_{i\sigma}=f_i^\dagger b_{i\sigma}$, where $f_i$ is the fermionic holon while $b_{i\sigma}$ is the bosonic spinon, satisfying the no-double-occupancy constraint $f_i^\dagger f_i+\sum_{\sigma}b_{i\sigma}^\dagger b_{i\sigma}=1$. Inside the HMS phase, we have $b_\uparrow=\sqrt{\rho_0+\delta\rho}e^{i\theta}$ and $b_\downarrow=0$.(We assume a small Zeeman field along $\uparrow$ direction is applied such that the global spin rotational symmetry is broken down to $U(1)$.) After integrating out the quadratic fluctuations of $\delta\rho$, we can use an $XY$ model to describe the spin dynamics. Due to the no-double-occupancy constraint, we also need to introduce an emergent $U(1)$ gauge field $A_\mu$ to couple both spin and charge degrees of freedom:
\begin{eqnarray}
\mathcal{L}_\text{eff} &=& \overline{\psi}_a\gamma^\mu(\partial_\mu-iA_\mu) \psi_a -\mu \overline{\psi}_a\gamma^0\psi_a+\frac{\rho_0}{g}({\partial_\mu\theta}
-A_\mu)^2, \nonumber\\
\end{eqnarray}
where $\psi_a$ is the two component Dirac spinor, $\mu$ is the chemical potential and $a=1,2$ labels two Dirac cones at different momentum points. Summation over repeated indices is everywhere understood.

To understand the instability of the above action, we apply duality transformation and introduce the vortex degrees of freedom(see method section for details):
\begin{eqnarray}
\mathcal{L}_\text{eff} &=& \overline{\psi}_a\gamma^\mu(\partial_\mu-iA_\mu) \psi_a -\mu \overline{\psi}_a\gamma^0\psi_a+\frac{i}{2\pi}\varepsilon^{\mu\nu\lambda}A_{\mu}\partial_\nu a_{\lambda}\nonumber\\&+&\frac{g}{16\pi^2\rho_0}(\varepsilon^{\mu\nu\lambda}\partial_\nu a_{\lambda})^2+|(\partial_\mu+i a_\mu)\phi|^2+m^2|\phi|^2,\nonumber\\\label{effective}
\end{eqnarray}
Here the complex scalar field $\phi$ describes the vortex/anti-vortex field which couples to the dual gauge field $a_\mu$.

Naively, the above action is stable and will not induce attractive interactions for holons, nevertheless, in the dense vortex limit, an FM vortex current -- holon/charge current (non-minimal) coupling term with the form $\mathcal{L}_\text{CC}= j_\mu\varepsilon^{\mu\nu\lambda}\partial_\nu a_{\lambda}$ could arise, where $j_\mu=i [\phi^*(\partial_\mu-i a_\mu)\phi-\phi(\partial_\mu-i a_\mu)\phi^* ]$ is the (gauge invariant) vortex current.(After we integrate out the gauge field $A_\mu$, we will find $\varepsilon^{\mu\nu\lambda}\partial_\nu a_\lambda=2\pi\overline{\psi}_a\gamma^\mu \psi_a$, which is indeed the holon/charge current.)

By adding $\mathcal{L}_\text{CC}$ into $\mathcal{L}_\text{eff}$ and integrating out the vortex field $\phi$ and the gauge field $A_\mu$, we will end up with an effective action for holons. We find that in addition to the usual onsite repulsive interacting term $(\overline{\psi}_a\gamma^\mu \psi_a)^2$ induced by the screened gauge field $A_\mu$, another term with the form $\left[\partial_\mu(\overline{\psi}_a\gamma^\nu \psi_a)\right]^2$ arises.
Interestingly, it turns out that $\left[\partial_\mu(\overline{\psi}_a\gamma^\nu \psi_a)\right]^2$ is attractive\footnote{We note that the $\mu=\nu$ components vanish due to the constraint $\varepsilon^{\mu\nu\lambda}\partial_\nu a_\lambda=2\pi\overline{\psi}_a\gamma^\mu \psi_a$(since $\varepsilon^{\mu\nu\lambda}\partial_\mu\partial_\nu a_\lambda=0$), and the $\mu\neq \nu$ components lead to attractive interactions. For example, the lattice version of the component $\left[\partial_x(\overline{\psi}\gamma^0 \psi)\right]^2$ for a single Dirac field takes a form $(n_i-n_{i+\v x})^2=-2n_in_{i+\v x}+n_i+n_{i+\v x}$, which is indeed an attractive interaction(up to a chemical potential term). Apparently, all the other $\mu\neq\nu$ components are also attractive due to the Lorentz invariance of $\left[\partial_\mu(\overline{\psi}\gamma^\nu \psi)\right]^2$.} and will dominate at low energy. Therefore, this term will lead to the instability of holon Fermi surface. It is well known that the spinless fermion with attractive interactions must have a $p+ip$ pairing symmetry, thus we find the key mechanism(pairing force) for the numerically observed $p+ip$ SC state in honeycomb lattice infinite-$U$ Hubbard model.

On the other hand, when $m_\zeta^2<0$,
\footnote{In general, a $\lambda |\phi|^4$ term need to be added into $\mathcal{L}_\text{eff}$, which comes from the fact that more than one segments of vortices cannot occupy the same place.}
vortex condensation happens and a mass term of $a_\mu$ is induced, and it generates a Maxwell term for $A_\mu$.
\begin{eqnarray}
\mathcal{L}_\text{eff}^{\rm{NF}} &=& \overline{\psi}_a\gamma^\mu(\partial_\mu-iA_\mu) \psi_a -\mu \overline{\psi}_a\gamma^0\psi_a+\frac{1}{g^\prime}(\varepsilon^{\mu\nu\lambda}\partial_\nu A_{\lambda})^2,\nonumber\\
\end{eqnarray}
We propose the above action as the effective field theory description for the potential non-Fermi liquid phase arising at small but finite $J$ for $\delta>0.1$.

Finally, we provide a more straightforward way to understand the origin of charge-current and FM skyrmion(vortex) current coupling in the infinite-$U$ Hubbard model. Indeed, with reference to fully up spin polarized sector, the infinite-$U$ Hubbard model can be rewritten as (see method section for detailed derivations):
\begin{eqnarray}
H  & = &  t(1-\delta_0)^2 \sum_{\langle ij \rangle}( c^\dagger_{i\uparrow} c_{j\uparrow} + h.c.)  \nonumber \\
&+&  \frac{1}{2} t\sum_{\langle ij \rangle} ( c^\dagger_{i\uparrow} c_{j\uparrow} +  c^\dagger_{j\uparrow} c_{i\uparrow})  (S^-_i S^+_j  + S^-_j S^+_i ) \nonumber \\
&+&   \frac{1}{2} t\sum_{\langle ij \rangle} ( c^\dagger_{i\uparrow} c_{j\uparrow} -  c^\dagger_{j\uparrow} c_{i\uparrow})  (S^-_i S^+_j  - S^-_j S^+_i ),\label{newH}
\end{eqnarray}
where $S_i^-\equiv c_{i\downarrow}^\dagger c_{i\uparrow}$ and $S_j^+\equiv c_{j\uparrow}^\dagger c_{i\downarrow}$ are the spin flipping operators. There is a local constraint that prevents any site from having an up spin hole and a reversed Pauli spin; this makes the above representation useful only when $\langle n_i^\downarrow\rangle=\delta_0 \ll 1$.
Spin charge coupling lurking in the infinite-$U$ Hubbard model is manifested in the above representation.  The charge current is coupled to a spin nematic chiral current represented by ${\vec z}\cdot ({\vec S}_i \times{\vec S}_j) \equiv (S^-_i S^+_j  - S^-_j S^+_i) $. We can also view this as a topological spin current density or a scalar chirality, ${\vec m}\cdot ({\vec S}_i \times{\vec S}_j)$, with the global magnetization vector ${\vec m}$  pointing along $\uparrow$-direction and two spins are at site $i$ and $j$, which is indeed the FM skyrmion(vortex) current. If we add a Gaussian term $\frac{1}{\kappa}({\vec z}\cdot ({\vec S}_i \times{\vec S}_j)^2$ to FM skyrmion(vortex) current, which is regarded as independent low energy degrees of freedom here, a nearest neighbor(NN) attractive interaction with the form $- 2 t^2 \kappa n_{i\uparrow} n_{j\uparrow}$ will arise after we integrate out the quantum fluctuations of FM skyrmion (vortex) current.

In conclusion, we report the theoretical discovery of a $p+ip$ wave
superconducting ground state in honeycomb lattice infinite-$U$ Hubbard model. It would be interesting to search for this physics
in experiment. The recently discovered spin $1/2$ honeycomb lattice
Mott-insulator InV$_{1/3}$Cu$_{2/3}$O$_3$\cite{InVCuO} would be an
appealing candidate if it could be doped experimentally. It will also be important to perform new experiments and look at existing results on mono layer $^3$He adsorbed on substrate\cite{3He}, which provide a nearly perfect avenue for the realization of infinite-$U$ Hubbard model on a few lattice geometries, including the honeycomb lattice. The recently discovered 2D ferromagnetism in conducting organic
 2D layer grown on graphene\cite{organic} provides another important playground
 to test our ideas of $p+ip$ superconductivity.

\section{Method}
{\bf Grassmann tensor product state} --
We use the standard form of GTPS
as our variational wavefunction. We further assume a translationally
invariant ansatz, and thus it is specified by just two different
Grassmann tensors $\textbf{T}_A,\textbf{T}_B$ on sublattices $A,B$ of
each unit cell:
\begin{eqnarray}
&& \Psi(\{m_i\},\{m_j \}) \\
\nonumber &&  = {\rm{tTr}} \int \prod_{\langle ij\rangle}\textbf{g}_{a
a^\prime} \prod_{i\in A} {\textbf{T}}^{m_i}_{A;abc} \prod_{j\in B}
{\textbf{T}}^{m_j}_{B;a^\prime b^\prime c^\prime},\label{GTPS}
\end{eqnarray}
with
\begin{eqnarray}
{\textbf{T}}^{m_{i}}_{A;abc}&=& {T}^{m_{i}}_{A;abc}
\theta_\alpha^{P^f(a)} \theta_\beta^{P^f(b)}
\theta_\gamma^{P^f(c)},  \nonumber\\
 {\textbf{T}}^{m_{j}}_{B,a^\prime b^\prime c^\prime}&=&
{T}^{m_{j}}_{B;a^\prime b^\prime c^\prime}
\theta_{\alpha^\prime}^{P^f(a^\prime)}
\theta_{\beta^\prime}^{P^f(b^\prime)}
\theta_{\gamma^\prime}^{P^f(c^\prime)},    \nonumber\\
\textbf{g}_{aa^\prime}&=& \delta_{aa^\prime}{\mathrm{d}
\theta}_\alpha^{P^f(a)} {\mathrm{d}
\theta}_{\alpha^\prime}^{P^f(a^\prime)}.
\end{eqnarray}
We notice that the symbol $\rm{tTr}$ means tensor contraction of the
inner indices $\{a\}$. Here
$\theta_{\alpha(\beta,\gamma)},\mathrm{d}\theta_{\alpha(\beta,\gamma)}$
are the Grassmann numbers and dual Grassmann numbers respectively
defined on the link $a(b,c)$and they satisfy the Grassmann algebra:
\begin{align}
 \theta_\alpha\theta_\beta&=-\theta_\beta\theta_\alpha,
&
 \mathrm{d}{\theta_\alpha}\mathrm{d}{\theta_\beta}&=-\mathrm{d}{\theta_\beta}\mathrm{d}{\theta_\alpha},
\nonumber\\
\int \mathrm{d}{\theta_\alpha}\theta_\beta &=\delta_{\alpha\beta} & \int
\mathrm{d}{\theta_\alpha} 1&=0 .
\end{align}
As shown in Fig.\ref{fig:GrassmannTPS}, $a,b,c=1,2,\ldots,D$ are the
virtual indices carrying a fermion parity $P^f(a)=0,1$. In this
paper, we choose $D$ to be even and assume there are \emph{equal}
numbers of fermion parity even/odd indices, which might be not
necessary in general. Those indices with odd parity are always
associated with a Grassmann number on the corresponding link and the
metric $\textbf{g}_{aa^\prime}$ is the Grassmann generalization of
the canonical delta function. The complex coefficients
${T}^{m_{i}}_{A;abc}$ and ${T}^{m_{j}}_{B;a^\prime b^\prime
c^\prime}$ are the variational parameters.

\begin{figure}[h]
{\includegraphics[width=0.3\textwidth]{GrassmannTPS.pdf}}
\caption{(Color online)Graphic representation of the GTPS on a honeycomb lattice.
$\textbf{T}_A$ and $\textbf{T}_B$, which contain $\theta$ are
defined on the sublattices $A$ and $B$ for each unit cell. The
Grassmann metric $\textbf{g}$ containing $\mathrm{d} \theta$ is defined on
the links that connect the Grassmann tensors $\textbf{T}_A$ and
$\textbf{T}_B$. The blue lines represent the fermion parity even
indices while the red lines represent the fermion parity odd indices
of the virtual states. Notice an arrow from $A$ to $B$ represents
the ordering convention $\mathrm{d} \theta_\alpha\mathrm{d}
\theta_{\alpha^\prime}$ that we use for the Grassmann
metric.}\label{fig:GrassmannTPS}
\end{figure}

Notice that $m_{i}$ is the physical index of the $t$-$J$ model on
site $i$, which can take three different values, $o,\uparrow$ and
$\downarrow$, representing the hole, spin-up electron and spin-down
electron states.   We choose the hole representation in our
calculations, and thus the hole state has an odd parity $P^f(o)=1$
while the electron states have even parity
$P^f(\uparrow,\downarrow)=0$. On each site, the non-zero components
of the Grassmann tensors should satisfy the parity conservation
constraint:
\begin{align}
P^f(m_{i})+P^f(a)+P^f(b)+P^f(c)=0 ({\rm mod}\, 2) .
\end{align}
Since the wavefunction Eq.(\ref{GTPS}) does not have a definite
fermion number, we use the grand canonical ensemble, adding a
chemical potential term to control the average hole
concentration.

{\bf Dual vortex representation of Higgs phase} --
To understand the pairing force for $p+ip$ SC order, we first perform the Hubbard-Stratonovich transformation to decouple the $({\partial_\mu\theta}
-A_\mu)^2$ term and decompose the $\theta$ field as $\theta=\eta+\zeta$ where $\eta$ is the smooth part of the phase fluctuation and $\zeta$ is the vortex part.
\begin{eqnarray}
  \mathcal{L}_\text{eff}&=& \overline{\psi}_a\gamma^\mu(\partial_\mu-iA_\mu) \psi_a -\mu \overline{\psi}_a\gamma^0\psi_a\nonumber\\&+&\frac{g}{4\rho_0}(\xi^\mu)^2-i\xi^\mu(  {\partial_\mu\eta}+{\partial_\mu\zeta}-A_\mu)  ,\label{effective}
\end{eqnarray}
By integrating the smooth fluctuations $\eta$, we obtain the constraint $\partial_\mu\xi^\mu=0$. Resolving the constraint leads to $\xi^\mu=\frac{1}{2\pi}\varepsilon^{\mu\nu\lambda}\partial_\nu a_{\lambda}$.(We note that the dual $U(1)$ gauge field $a_\mu$ is non-compact.)
\begin{eqnarray}
  \mathcal{L}_\text{eff}&=& \overline{\psi}_a\gamma^\mu(\partial_\mu-iA_\mu) \psi_a -\mu \overline{\psi}_a\gamma^0\psi_a+\frac{i}{2\pi}\varepsilon^{\mu\nu\lambda}A_{\mu}\partial_\nu a_{\lambda}\nonumber\\& +&\frac{g}{16\pi^2\rho_0}(\varepsilon^{\mu\nu\lambda}\partial_\nu a_{\lambda})^2+ i a_\mu j_\mu+ A \sum_i \int ds_i   ,
\end{eqnarray}
where $j_\mu=\frac{1}{2\pi}\varepsilon^{\mu\nu\lambda}\partial_\nu \partial_\lambda \zeta$ is the vortex current. We also add a term
$A \sum_i \int ds_i$ which corresponds to the energy cost at the core of the vortex, where $A$ is the energy cost per unit length and $\in ds_i$ is the length of the world line of $i$th vortex. Since summation over vortex line configurations can be reexpressed by integrating over a free massive complex field $\phi$\cite{Nagaosa}, we end up with a dual action evolving vortex degrees of freedoms $\phi$ as well as the dual gauge field $a_\mu$:
\begin{eqnarray}
  \mathcal{L}_\text{eff}&=& \overline{\psi}_a\gamma^\mu(\partial_\mu-iA_\mu) \psi_a -\mu \overline{\psi}_a\gamma^0\psi_a+\frac{i}{2\pi}\varepsilon^{\mu\nu\lambda}A_{\mu}\partial_\nu a_{\lambda}\nonumber\\ &+&\frac{g}{16\pi^2\rho_0}(\varepsilon^{\mu\nu\lambda}\partial_\nu a_{\lambda})^2 +|(\partial_\mu+i a_\mu)\phi|^2+m^2|\phi|^2,\nonumber\\
\end{eqnarray}

{\bf Charge current -- topological spin current interaction}
Consider the infinite-$U$ Hubbard model assuming we are staying in almost fully polarized up spin sectors with a small density of down spins, $\langle n_i^\downarrow\rangle=\delta_0 \ll 1$. The infinite-$U$ Hubbard model in these sectors can be exactly rewritten as:

\begin{eqnarray}
H &=& t\sum_{\langle ij\rangle}(1-n_{i\downarrow})c_{i\uparrow}^\dagger c_{j\uparrow}(1-n_{j\downarrow})+h.c.\\&+&
 t\sum_{\langle ij\rangle}(1-n_{i\uparrow})c_{i\downarrow}^\dagger c_{j\downarrow}(1-n_{j\uparrow})+h.c.\nonumber\\
 & = & t(1-\delta_0)^2 \sum_{\langle ij\rangle} c_{i\uparrow}^\dagger c_{j\uparrow}+h.c.
 + t\sum_{\langle ij\rangle}c_{i\uparrow}^\dagger c_{j\uparrow} S_i^- S_j^+ +h.c.\nonumber
\end{eqnarray}

We note that $(1-n_{i\uparrow})c_{i\downarrow}^\dagger=c_{i\uparrow}c_{i\uparrow}^\dagger c_{i\downarrow}^\dagger=S_i^- c_{i\uparrow}^\dagger$, where $S_i^-\equiv c_{i\downarrow}^\dagger c_{i\uparrow}$. Similarly, $c_{j\downarrow}(1-n_{j\uparrow})=c_{j\downarrow}c_{j\uparrow} c_{j\uparrow}^\dagger= c_{j\uparrow} S_j^+$. An onsite double occupancy constraint between up spin hole and a down Pauli spin can be well approximated by
replacing hopping $t$ by $t(1-\delta_0)^2$ for the up spin electron hopping term.

The first term in the above is the usual kinetic term for polarized electron while the second term is a backflow of down spins. Physics of this important term becomes more transparent when we rewrite the hopping term in terms of kinetic energy and charge current operators as:

\begin{eqnarray}
H  & = &   t(1-\delta_0)^2 \sum_{\langle ij \rangle}( c^\dagger_{i\uparrow} c_{j\uparrow} + h.c.)  \nonumber \\
&+&  \frac{1}{2}  t\sum_{\langle ij \rangle} ( c^\dagger_{i\uparrow} c_{j\uparrow} +  c^\dagger_{j\uparrow} c_{i\uparrow})  (S^-_i S^+_j  + S^-_j S^+_i ) \nonumber \\
&+&   \frac{1}{2} t\sum_{\langle ij \rangle} ( c^\dagger_{i\uparrow} c_{j\uparrow} -  c^\dagger_{j\uparrow} c_{i\uparrow})  (S^-_i S^+_j  - S^-_j S^+_i ),\label{newH}
\end{eqnarray}

We identify $(S^-_i S^+_j  + S^-_j S^+_i ) \equiv (S^i_x S^j_x + S^i_y S^j_y)$ with $XY$ spin-spin interaction in the plane perpendicular to the direction of FM polarization. It is easily seen that this coupling between kinetic energy of up spin holes and down spin electron encourages an antiferromagnetic spin correlation in the transverse direction. Similarly we identify
$(S^-_i S^+_j-S^-_j S^+_i ) \equiv {\vec z}\cdot ({\vec S}_i \times{\vec S}_j)$ with scalar spin chirality, with reference to the FM moment vector. This term encourages coupling between Skyrmion current and charge current. It is the gain in energy arising from this term that favors a finite density of Skyrmions in the ground state. In other words, the dynamic holes stir the skyrmion gas and in the process undergo a pairing instability in the $p+ip$ channel.

\section*{Acknowledgment}
Z.C.G would like to thank Leon Balents, Dong-Ning Sheng and Patrick Lee for valuable discussions. This work is supported by the Government of Canada through Industry Canada and by the Province of Ontario through the Ministry of Research and Innovation. H.C.J was supported by the U.S. Department of Energy. G.B acknowledges Science and Engineering Research Board, India as a SERB Distinguished Fellow.

redpajama_set_name: RedPajamaArXiv


Oh, Maxim. You're so funny and clever! Burn city! Population: Manti Te'o! LOLZ.
After Manti Te'o's fake girlfriend hoax of 2012, we think it might be nice to have an invisible girl of our own to love. Why not? She's got a ton of great qualities, including looking awesome in a bikini.
ZOMG! This is hilarious!!!!! Guess what spot they gave Lennay on the list? Just guess. Ready for it? 69!!!!! SIXTY-NINE!!! HAHAHAHAHAHAHAHAHA! Maxim mag! You kill me!!
Maxim magazine is run by morons. I've had the pleasure of dealing with Maxim personally. I had posted a bunch of photos of Ryan Tannehill's hot wife, Lauren Tannehill, and Maxim didn't like that. They proceeded to threaten me in a series of emails from their Director of Photography at Maxim Magazine. (a great read if you like condescension and snark) So, after this experience, it's no surprise to me that Maxim used their pea brains to take a shot at Manti with a tired, tired joke. Apparently, Maxim is still living in this world: Manti Te'o Fake Dead Girlfriend Jokes are HYSTERICAL. It's sad, really.
This entry was posted in Celebrities, Football, News, NFL and tagged Manti Te'o, manti te'o deal with it, manti te'o hot 100, manti te'o maxim, Manti Te'o's girlfriend, maxim hot 100, maxim lennay kekua. Bookmark the permalink.


From December 22nd, 2018 till January 25th, 2019, the United States suffered the longest Shutdown in our country's history. The shutdown was largely the result of a disagreement between the president, Donald Trump, and Congress, which recently became more Democrat meaning Congress' majority party and the President now differ in political identity. The President was hoping that Congress would pass legislation to fund his agenda, namely funding for a border wall along the Southern Border of the United States. On January 25th the President agreed to support a bill that would temporarily reopen the government, yet he said if funding for the wall was not decided by February 15th he would shut down the government, name a state of emergency, and divert funding from the military to fund the wall.
The government shutdown affected over 800,000 government employees, and many of them were out of a job for the time being, while others worked with the promise of getting paid later on. It is estimated that over $3.6 billion was lost permanently as a direct result of the government shutdown. In the grand scheme of government spending, this may not seem like a huge number, however when you consider what that money could've been used for you truly understand the effects of the shutdown. The money could've been used to fund military, local authorities, or even welfare.
Another government shutdown would likely have the seem implications and could even be more devastating. Government workers would likely get dissatisfied with the government and they could act up against it through protest or strike, which in a shutdown, the United States would be ill-equipped to handle. It is important to see what will happen in the coming weeks in the higher levels of the United States government. Another shutdown does not seem unlikely thus Americans should behave under the thought that another shutdown is inevitable so they can be prepared. Although many of us do not directly feel the effects of the shutdown it is important to keep in mind that there are thousands or even millions who do.


Proanthocyanidins (PAs) are of great interest in nutrition and medicine because of their potent antioxidant capacity and possible protective effects on human health in reducing the risk of chronic diseases such as cancer and cardiovascular disease. In vitro studies have shown that procyanidins in chocolate inhibit human 5-lipoxygenase, decrease the LDL oxidative susceptibility, inhibit platelet function, and promote transforming growth factor-ß1 homeostasis in peripheral blood mononuclear cells. Procyanidins in grape seeds induce apoptotic death of human prostate carcinoma and exhibit cytotoxicity towards MCF-7 breast cancer, A-427 lung cancer and gastric adenocarcinoma cells, while enhancing the growth and viability of the normal cells. Polymeric PAs were more effective than monomers in lowering blood cholesterol by binding cholesterol in the intestine through hydrophobic association, particularly those with higher DP.
In vitro studies have shown that procyanidins with the A-type interflavan linkage isolated from cranberries inhibit the adherence of uropathogenic E. coli to the uroepithelial cell surfaces. Also, the A-type polymers from cinnamon have insulin-like biological activity, and cinnamon consumption (1-6 g) in type II diabetic subjects for 40 days lowered serum glucose, triglycerides and total cholesterol. Procyanidins possess insulinomimetic properties, decreasing hyperglycemia in streptozotocin-diabetic rats and stimulating glucose uptake in insulin-sensitive cell lines. However, additional research is needed relative to procyanidins structure and concentrations that are effective in modulating insulin action.
Oligomeric and polymeric flavan-3-ols are better known as proanthocyanidins (PAs) or condensed tannins. They are ubiquitous and present as the second most abundant natural phenolic after lignin. The flavan-3-ol units are linked mainly through C4→C8 bond, but the C4→C6 bond also exists (both called B-type). The flavan-3-ol units can also be doubly linked by an additional ether bond between C2→O7 (A-type). The size of PA molecules can be described by degree of polymerization (DP) (1). PAs consisting of exclusively of (epi)catechin are procyanidins.
A number of analytical procedures including colorimetric, gravimetric, chromatographic and mass spectrometric are currently being employed for the measurement of cranberry PACs, however, due to the complexities of the PAC structures and A-The new BL-DMAC method has been validated in a multi-lab test and provides a simple and relatively specific spectrophotometric assay for total PAs in cranberry or other powders, utilizing a commercially available procyanidin A2 standard. DMAC is most useful within a given type of food such as cranberries. The DMAC method is not be appropriate for comparing concentrations across different food types or processed samples where there are large differences among the relative amounts of the different oligomers and polymers.
HPLC/MS Profile to Confirm Relative Distribution of Oligomers, Polymers.
In addition to BL-DMAC, other techniques such as HPLC coupled with mass spectrometry are needed to authenticate cranberry powders by guaranteeing the presence of A-type linkages in the procyanidins. This would guard against adulteration of cranberry products with B-linked procyanidins or flavan-3-ols (epicatechin or catechin) from other less expensive food sources.


text:
Q: How to use NSFetchedResultsController for scrolling bottom to top in messaging app? I am building a message app. When I am messaging in my application all the messages are getting store in core data. I have connected the core data with TableViewController with NSFetchedResultsController. I know how does this work and I am using NSFetchedResultsController for a long time with TableView. In most of the case TableView load from top and it's scroll down to load more data on requirement, thus my application works pretty well.
Here for the message app the TableView behaviour is opposite from the previous one. It loads the last messages(20-30 batch size) and if I want to see the old message I will scroll top. So I am trying to implement this on NSFetchedResultsController.
Example :
   Suppose I have 100 messages. I am setting batch size is 10. So first it will load 90-100 messages and it will scroll down to the last indexpath(here 100th). Then If I want want to scroll top and reach 90th indexpath it will give me 10 again so now I have 80-100 messages now it won't scroll down it will be keep on doing the same thing is I scroll to top.
I know I can sort in reverse order but that time I will get 100-90 but it won't so the last message(100) bellow.
So how can I fix this issue? Any configuration is there for NSFetchedResultsController that I am missing? How to fix?


This entry was posted in Musing and tagged Mercy mercy mercy, Redemption, Womb to tomb.
I'm so sorry for your loss. And impressed with your words….God does redeem death of all kinds.
Amen, I say to you, Amen. Little deaths or big deaths, St. Francis befriended it and called her sister. We mourn when someone dies and at the same time congratulate the dead for have risen. The Byzantine priest is right, when dead we no longer sin. Puts a smile on my face.
Where would we be without the saints?


Q1. HOW MUCH DOES IT COST?
Silhouette Body ReProgramme is available on two Protocols depending upon the amount of weight you wish to release. Both Programmes are tailored to suit every budget. Please go to STORE to view details of prices.
Q2. WHO CAN USE SILHOUETTE HCG HOMEOPATHIC DROPS?
Do NOT use hCG if you are pregnant or nursing. hCG will not interfere with any form of birth control. You may use hCG homeopathic drops if your BMI value is not lower than 20.Always check with your health professional before beginning any new weight loss programme.
Q3. IS THE PROGRAMME DIFFICULT TO FOLLOW?
The answer depends upon you. If you want nothing more than to be slim, healthy and feeling wonderful every day – and can make a commitment to yourself to do so – then this Programme is definitely for you.
Q4. HOW DOES IT WORK?
Q5. ARE HCG HOMEOPATHIC DROPS SAFE TO TAKE?
Silhouette's hCG homeopathic drops are highly diluted, quality assured homeopathic medicines which have been carefully micro-dosed. Homeopathic drops are safe to take orally and generally have no known side effects or contraindications. Homeopathic remedies may also be taken safely together with conventional medicines and are complementary in some cases, being one of the reasons for Homeopathy's continuing popularity and success.


The cryptocurrency story can't be complete without a huge reference to cryptocurrency exchanges. They are the bridge that links a crypto investor to the cryptocurrency world. Cryptocurrency exchanges have a strong and direct impact on the crypto market, and this level of influence cannot be just brushed aside as the New Year kicks off.
Many cryptocurrencies have now emerged in the crypto market, all with the aim of providing and managing crypto wallets for their investors. Last year, just like many digital coins, was a bad one for cryptocurrency exchanges, as hackers stole over a billion dollars' worth of crypto assets from them. This series of hacks, took a toll on the value of the crypto market, as many digital coins saw their prices plummet, indicating how strong crypto exchanges can be in the market.
Just like cryptocurrencies, crypto exchanges would be looking to make this year a good one and this piece looks at how crypto markets are shaping up this year, to embrace the unpredictability of cryptocurrencies. The year hasn't gone any far and yet still, there have been hacks on some crypto exchanges.
Just some few days back on the 14 of January, a New Zealand-based crypto exchange, Cryptopia was hacked, resulting in significant losses. The crypto exchange had over 800 different assets listed in its platform and also supports small-scale crypto asset trading pairs.
Regarding Security, there are still questions as to whether crypto exchanges, including the biggest ones, are safe and secured for the sake of their customers. With volatility a constant thing in the crypto market, investors are bound to lose some money and can't afford to suffer that fate again because their trust in a crypto exchange was betrayed.
In bids to avoid regulation crackdowns by governments, it seems crypto exchanges are gradually doing due to work there. South Korea has seen some of its biggest crypto exchanges, pass a government security audit. The South Korea crypto market was one of the most active markets before the regulation chaos saw its consumer activities dwindle.
Now seven of the country's biggest crypto exchanges, including Bithumb, Korbit all gained the satisfaction of investigators during the audit, and this will be very crucial in crypto exchanges fight for survival in the Asian zone.
The Financial Service Agency (FSA), Japan's top financial regulator also approved the registration of Coincheck, as a crypto exchange on Friday, January 11. This feat is a significant development, as it's been a year since Japan's Financial Services Agency last gave the green light for a crypto exchange to legally operate in the country.


Marketers And Boomers, BFFs Once Again?
Some things are destined to be together. No matter how often they part ways, they find their way back. Carrie and Big. The Lakers and Celtics. Sandra Bullock and... well, Carrie and Big.
Now, thanks to the recession, you can add mainstream marketers and baby boomers to that list. And the implications of this reunion go far beyond growing corporate bottom lines.
After nearly 50 years as marketers' darlings, boomers lost favor over the last decade, slipping through the cracks of target demos as they hit age 50. Call it oversight. Call it the 50 year itch. But call it old news.
Companies have felt the pinch of decreased consumer spending, and smart ones are realizing that, while America's wealthiest generation may have hit AARP's magic number, they have not stopped spending or exploring new brands. Consequently, market leaders are once again targeting the boomer generation-comprising 76 million people, 59 million of whom are already age 50+.
Examples of this trend can be seen far and wide. Stouffers' "Let's Fix Dinner" campaign targets empty nesters. Jeep has honed in on "cool" grandparents. General Mills and Yahoo are partnering to reach boomers through their health-focused digital "Vitality" campaign. Proctor & Gamble has teamed up with NBC Digital to develop a network of boomer Web sites under the banner "Life Goes Strong."
As the ultimate industry sign of renewal, Tuesday night, the Effie Awards will present its new Boomer+ Award for the second year in a row, honoring marketing effectiveness to the 50+ demographic.
It's important not to overstate reality. Younger consumers still rule in most marketers' minds. The boomer-plus demographic may never be the primary interest of mainstream marketers, but they are increasingly finding their place alongside younger generations as advertisers seek to maximize the ROI of their consumer communications.
Though motivated by a desire for increased bottom lines, the renewed relationship with boomers has broader societal implications.
For starters, boomers are being portrayed in a more positive and realistic light in advertisements, which could shift how society views the 50+ population. The vibrant, active image of Jeep's "cool grandma" can replace traditional stereotypes and reshape our cultural perception of what it means to be in the second half of life.
Additionally, advertisers are learning that they have an opportunity to develop new products and services to meet the specific needs of the 50+ population. This will lead to a wider variety of products and services aimed at improving the lives of people 50+, benefiting not only the boomers, but each successive generation, who will reap the rewards as they move past middle age.


text:
THOUSANDS of Tesco.com logins and passwords leaked online
Customers locked out of accounts, some discount vouchers AWOL
Brid-Aine Parnell Fri 14 Feb 2014 // 11:37 UTC
Thousands of Tesco customers have had their emails and passwords posted online after hackers got their hands on the login details.
A list of over 2,200 Tesco.com accounts was published on Pastebin yesterday and some customers have complained that their vouchers have gone missing from their accounts.
Tesco customers took to the supermarket giant's Facebook page to report being booted out of their accounts and having their points and vouchers stolen.
The grocery chain said that it was "urgently investigating" the situation.
"We have contacted all customers who may have been affected and are committed to ensuring that none of them miss out as a result of this," Tesco said in a statement.
"We will issue replacement vouchers to the very small number who are affected."
Nicked: Customers took to Facebook to complain about missing discount vouchers
It's believed that the usernames and passwords were acquired from hacks on other sites and then tried out on Tesco.com by the hackers.
Trey Ford, global security strategist at Rapid7, said that the breach highlighted again the danger of reusing passwords across multiple accounts.
"The attackers seem to have picked up usernames and passwords that were leaked after breaches of other, potentially unrelated organisations, and by trying them on Tesco's site, they were able to compromise 2,239 Tesco.com customer accounts," he said.
"So far the information available indicates that the impact of this has been relatively limited – stolen vouchers – but if attackers have tried this on Tesco.com, the chances are they are also trying it on other sites too and so we may see additional fallout."
February seems to be a bad month for Tesco customers - in the same month last year the supermarket chain had to call in the cops after hackers stole Clubcard vouchers from customers' online accounts.
The company also had a bit of a security gaffe earlier this week when it sent out an email to hundreds of customers about a pricing error on a trampoline and revealed all their email addresses. Tesco sent out the missive to tell customers they wouldn't be getting the trampoline they ordered because it had been priced incorrectly.
One customer said on Facebook:
Would love to know how the 'investigation' over the fact that emails were sent out cancelling the trampoline purchases last night sending the email to around 300 people at a time... showing ALL the personal emails of recipients! Total lack of protection for customers details!
I personally received FIVE messages so I have on my emails approx. 1500 emails!!
Would appreciate a response, as when I complained over the phone last night I was told they would be in touch... how I wonder? I do hope not via email!!


The life-span tag has no usage guidance.
Does SB 1.8.5 say something about the (short) lifespan of the present generation or is it just the author's impression?
According to Hinduism at what time the life begins?
In my view the life begins at the time of forming zygote inside the mother's womb. My question is that what is the view of Hinduism about "the beginning of a life"?
What is the life span of Lord Brahma according to Vedas?
In my childhood, I had read about the life span of Brahma. can someone please enlight this topic?


text:
package info.fingo.urlopia.request;

import info.fingo.urlopia.config.authentication.UserIdInterceptor;
import info.fingo.urlopia.config.persistance.filter.Filter;
import info.fingo.urlopia.request.normal.DayHourTime;
import info.fingo.urlopia.request.normal.NormalRequestService;
import org.springframework.beans.factory.annotation.Autowired;
import org.springframework.data.domain.Page;
import org.springframework.data.domain.Pageable;
import org.springframework.http.MediaType;
import org.springframework.http.ResponseEntity;
import org.springframework.web.bind.annotation.*;

import javax.annotation.security.RolesAllowed;
import javax.servlet.http.HttpServletRequest;
import java.util.List;

@RestController
@RequestMapping("/api")
public class RequestController {

    private final RequestService requestService;

    private final NormalRequestService normalRequestService;

    @Autowired
    public RequestController(RequestService requestService,
                             NormalRequestService normalRequestService) {
        this.requestService = requestService;
        this.normalRequestService = normalRequestService;
    }

    @RolesAllowed("ROLES_WORKER")
    @GetMapping(path = "/users/{userId}/requests", produces = MediaType.APPLICATION_JSON_VALUE)
    public ResponseEntity<Page<RequestExcerptProjection>> getAllFromUser(@PathVariable Long userId,
                                                                         @RequestParam(name = "filter", defaultValue = "") String[] filters,
                                                                         Pageable pageable) {
        var filter = Filter.from(filters);
        var requestsPage = requestService.getFromUser(userId, filter, pageable);
        return ResponseEntity.ok(requestsPage);
    }

    @RolesAllowed("ROLES_ADMIN")
    @GetMapping(path = "/requests", produces = MediaType.APPLICATION_JSON_VALUE)
    public ResponseEntity<Page<RequestExcerptProjection>> getAll(@RequestParam(name = "filter", defaultValue = "") String[] filters,
                                                                 Pageable pageable) {
        var filter = Filter.from(filters);
        var requestsPage = requestService.get(filter, pageable);
        return ResponseEntity.ok(requestsPage);
    }

    @RolesAllowed("ROLES_WORKER")
    @GetMapping(path = "/users/{userId}/requests/pendingTime", produces = MediaType.APPLICATION_JSON_VALUE)
    public ResponseEntity<DayHourTime> getPendingRequestsTime(@PathVariable Long userId) {
        var pendingRequestsTime = normalRequestService.getPendingRequestsTime(userId);
        return ResponseEntity.ok(pendingRequestsTime);
    }

    @RolesAllowed("ROLES_WORKER")
    @PostMapping(value = "/users/{userId}/requests", consumes = MediaType.APPLICATION_JSON_VALUE)
    public ResponseEntity<Void> create(@PathVariable Long userId,
                                       @RequestBody RequestInput input) {
        requestService.create(userId, input);
        return ResponseEntity.ok().build();
    }

    @RolesAllowed("ROLES_WORKER")
    @GetMapping(path = "/users/{userId}/teammates/vacation", produces = MediaType.APPLICATION_JSON_VALUE)
    public ResponseEntity<List<VacationDay>> getTeammatesVacationsForNexTwoWeeks(@PathVariable Long userId) {
        var teammatesVacations = requestService.getTeammatesVacationsForNextTwoWeeks(userId);
        return ResponseEntity.ok(teammatesVacations);
    }

    // *** ACTIONS ***

    @RolesAllowed("ROLES_ADMIN")
    @PostMapping(path = "/requests/{requestId}/accept", produces = MediaType.APPLICATION_JSON_VALUE)
    public ResponseEntity<Void> accept(@PathVariable Long requestId,
                                       HttpServletRequest httpRequest) {
        var authenticatedId = (Long) httpRequest.getAttribute(UserIdInterceptor.USER_ID_ATTRIBUTE);
        requestService.validateAdminPermissionAndAccept(requestId, authenticatedId);
        return ResponseEntity.ok().build();
    }

    @RolesAllowed("ROLES_ADMIN")
    @PostMapping(path = "/requests/{requestId}/reject", produces = MediaType.APPLICATION_JSON_VALUE)
    public ResponseEntity<Void> reject(@PathVariable Long requestId) {
        requestService.validateAdminPermissionAndReject(requestId);
        return ResponseEntity.ok().build();
    }

    @RolesAllowed({"ROLES_WORKER", "ROLES_ADMIN"})
    @PostMapping(path = "/requests/{requestId}/cancel", produces = MediaType.APPLICATION_JSON_VALUE)
    public ResponseEntity<Void> cancel(@PathVariable Long requestId,
                                       HttpServletRequest httpRequest) {
        var authenticatedId = (Long) httpRequest.getAttribute(UserIdInterceptor.USER_ID_ATTRIBUTE);
        requestService.cancel(requestId, authenticatedId);
        return ResponseEntity.ok().build();
    }

}

redpajama_set_name: RedPajamaGithub


The Physio Company are proud to announce the opening of a new Physiotherapy clinic in the VHI Swiftcare centre in Mahon, Cork.
We have partnered with VHI Swiftcare centres to provide our physio services within the Mahon VHI Swiftcare clinic, located at City Gate in Mahon, Cork. The location of our new clinic is just off the South Ring Road beside Mahon Point Shopping Centre. It has been open since November 28th.
The clinic will offer the same range of Chartered Physiotherapy services that we currently offer in all of our other clinics nationwide. The price of all treatments will also remain the same as in our other clinics.
Older PostNew Physio Clinic Opened in the VHI Swiftcare, Swords.


text:
Development of a Strategic Tool for Shared Decision-Making in the Use of Antidepressants among Patients with Major Depressive Disorder: A Focus Group Study
Zaini, Syahrir and Manivanna Bharathy, Harvin and Sulaiman, Ahmad Hatim and Gill, Jesjeet Singh and Koh, Ong Hui and Huri, Hasniza Zaman and Shamsudin, Siti Hadijah and Ng, Chong Guan (2018) Development of a Strategic Tool for Shared Decision-Making in the Use of Antidepressants among Patients with Major Depressive Disorder: A Focus Group Study. International Journal of Environmental Research and Public Health, 15 (7). p. 1402. ISSN 1660-4601
Official URL: https://doi.org/10.3390/ijerph15071402
Shared decision-making (SDM) has been recognized as an important tool in the mental health field and considered as a crucial component of patient-centered care. Therefore, the purpose of this study was to develop a strategic tool towards the promotion and implementation of SDM in the use of antidepressants among patients with major depressive disorder. Nineteen doctors and 11 major depressive disorder patients who are involved in psychiatric outpatient clinic appointments were purposively selected and recruited to participate in one of six focus groups in a large teaching hospital in Malaysia. Focus groups were transcribed verbatim and analyzed using a thematic approach to identify current views on providing information needed for SDM practice towards its implementation in near future. Patients' and doctors' views were organized into six major themes, which are; summary of treatment options, correct ways of taking medication, potential side effects of treatments related to patients, sharing of case study related to the treatment options, cost of treatment options, and input from pharmacist. The information may be included in the SDM tool which can be useful to inform further research efforts and developments that contribute towards the successful implementation of SDM into clinical practice.
shared decision-making; antidepressants; depression; focus group discussion
R Medicine
R Medicine > RS Pharmacy and materia medica
Ms. Juhaida Abd Rahim


Nice 3br 2ba set in desired park just a short distance to miles of Sandy Beach!
This Skyline Double wide home is 24×40 in size and features a center kitchen floor plan. The home is constructed with 2×6 walls, vinyl windows, vinyl siding and shawnee steps at the front and a large rear deck. The lot size is considered above average for a park setting. The homes kitchen area offers an eat in dining area and ample cupboard space, a separate laundry area, large master bedroom w/walk in closet and private bath with walk in shower. The 2nd bath offers a tub/shower. The home is being sold with Gas Range, Refrigerator, dishwasher, washer/dryer and shed.


Today I had a quote on the board in my classroom, "Fear is 100% dependent on you for its survival." – Steve Maraboli. One of my students turned to me and asked, "What are you afraid of?" It was a fair question since I had asked them to be honest with themselves and determine what their greatest fear was. Without hesitation I answered, "failure." Writing scares me, too, and I didn't include that in my answer.
Writing scares me because of my fear of failure. If that could possibly make any sense. For instance, I got an email from a decent sized publication asking me to submit op/eds for them. It's not a paying gig, so don't get too excited for me. The email came some time in December. I still haven't made a submission. Today, I got an email from the editor asking me if I was interested in submitting something to them. She was just following up, she said.
It's a tremendous opportunity for me as they will advertise my books and other events within my byline. Yet, I've been reluctant to send anything to her. There are several reasons. She wants the pieces to be in Associated Press style, and most of the "examples" she sent were news related. And, when I went on their site the only pieces I found were directly related to the news. I don't even watch the news. I have no idea what's going on pretty much anywhere unless I hear it briefly on Moody Radio on my ride to work, or someone posts something on FB.
I feel unprepared to write Associated Press (AP) style pieces on topics I have little to no interest in. Aside from the fact I don't write anything in AP style. I am not educated in that form as I don't technically have any real, formal, writing education. I simply write what moves me. And, that doesn't seem like what they are looking for. Yet, she contacted me out of the blue. I have no idea how she came across my name, or anything. So, that tells me there's a reason, but I'm afraid. I'm afraid that I'll send something and she'll reject it and that will be the end of that opportunity. That somehow, I will screw it up.
Just this week someone told me that I needed to actively pursue my writing "business" ideas. Hesitation from the fear within me is so great I can't even begin to explain it to you here. As much as I love writing and especially writing about Jesus and the Bible, I never feel "good enough" to actually do anything of real, financially lucrative, value with it. I always assume that I can't write the way that paying publications seek. I can't write AP style; I don't have a journalism degree. And, in fact, bombed the one journalism class I tried to take years ago when I thought I'd actively pursue a writing career.
Yet, here was this email asking me if I was going to contribute. I didn't want to leave the editor hanging, so I sent her two titles that have been floating around in my mind. Of course, I haven't written either piece, but they have just been stewing there as possibly intriguing concepts. I didn't think she would accept them as "good enough" because they don't come from a news basis. Believe it or not, as I sit here writing this, she just emailed me and told me that she really liked one of the suggestions and said that I should go for it.
Writing scares me. Now, I have agreed to work on this piece this weekend and I am terrified that she'll hate it. That it won't be what they are "looking for." Rejection equals failure in my eyes and it's really hard for me to pull myself back up when it comes to my writing. This has been such an integral part of my life, like, my whole life. I have been writing since I was a kid. I have been praised and belittled for it. I have had it published and have literally had it thrown into trash cans as a means of punishment.
Writing scares me because it is such a huge part of me on a page. It's the most honest and transparent view of my heart that most will ever see and that gives it great power in my eyes. Some writers are able to write for the sake of writing. They are little phased when one piece is turned down. They just pen a different one. For me, each rejection is another crack in my soul. Writing scares me.
Maybe I need a dose of my own pep talking wisdom? So, here's to an attempt to publish in a Christian format that gets 15000 views a day. Pray for me!