A lot of positives and a more complete effort, but some costly errors resulted in the 2nd loss of the road trip, this time in regulation by a 5-2 score.
Frustrating in some ways as a couple of simple errors really hurt the Kings tonight and took away from an overall decent game. By no means 'great', but certainly better from Friday's effort. I thought the Kings did well keeping a lot of Salmon Arm chances to the outside and in the first period despite Salmon Arm outchancing the Kings in quantity, the Kings had better quality.
Much like Friday vs Trail at home, Stefan Wornig and the Kings D started slowly. The first couple of goals in the 1st period were a little soft defensively, but following that things really tightened up. Wornig in particular showed a marked improvement from minute zero to sixty with a lot of puck handling issues early turning into some good kick saves and a sharp glove after the opening 10-12 minutes.
In that 1st period, you can pretty much pigeon hole the struggles in between minutes 7 and 13…outside that the Kings were quite good.
Into the 2nd and every chance the Kings had at momentum was not taken advantage of. Tristan Mullin scores a beauty but the Kings don't build on it. Liam Lawson snipes another goal and the Kings conceded not long after. Missed opportunities to take control of the game and gain a lead, but the fact that the Kings generated those goals is a positive.
5 goals, 2 assists for 7 points. That's Tristan Mullin over the last 4 games. He says he doesn't feel any additional responsibility trying to make up for Kyle Betts and Carter Turnbull's absence, but he's certainly lifted. He's 7-2-9 in December's 6 games as well. This from a player who surprisingly can be very very quiet through stretches. It's not that's he's not doing anything, it's just that he might not make much noise when he's out there. However he's got that extra switch and gear to jump to.
The Kings wrap their 3-in-3 road trip and the pre-Christmas schedule at 2:00pm in Vernon against the Vipers.
The Kings bumped a 2-game slide with a 4-3 win over the Merritt Centennials on Sunday afternoon. The Kings got out to a 3-0 and 4-1 lead before a late Merritt push made the final stages very interesting. The Kings are 2-2 in December with 5 games remaining.
Langley are coming off a Saturday/Sunday double header last weekend, dropping a 7-4 game at home to Vernon then tying Surrey 3-3. They are 1-1-1 in December.
Crucial weekend for the team as they make up 1 game against both Cowichan and Nanaimo. The Kings are 2 back of Cowichan with 3 in hand and can overtake them with a successful weekend and/or some out of town help. Nanaimo will finish top of the Division heading into Christmas, but the Kings can close the game just a bit heading into a double header in Powell River at the start of January.
Kings 8-0-0-1 against the Mainland Division this year. The team has swept the season series against both Wenatchee and Prince George, recorded 2 victories against Coquitlam (1 at the Showcase), beaten Surrey at the Showcase and Langley in Powell River in November. Chilliwack got a 4-3 OT win in November to dent the record slightly.
We talked a lot about 1st period scoring on Sunday. 18-6 at home through 20 minutes are the Kings this season. On the road, 15-14…an advantage but a small one. Quick starts still the key for this team…it's also one that likes to play with the lead early.
Short benches tonight from regulars. Justin Fregona and Bo Didur from Langley, along with Kyle Betts and Carter Turnbull all getting set to play for Gold on Saturday and won't be in action tonight, nor until the Christmas break.
The broadcast goes live on 95.7 Coast FM in Powell River at 6:55pm. It will also be online on the Kings Broadcast Network and FastHockey PPV. In the 1st intermission, we'll have chats with Tristan Mullin, Nick Nonis and Chris Protopoulos. In the 2nd break, from TSN Radio, a chat with alumni goalie Sean Maguire. Brock Sawyer will join us in the post-game show.
Three Things returns with a look back at the final pair of games during a 6-game stint at the Hap Parker Arena. Also, Alex Rawnsley previews 3 games in 2 and a half days through the lower Mainland and Interior of BC.
Two recaps in one due to a busy Saturday personally for me.
After a focus was put on the physical side of the game, or lack thereof, from Sunday's loss to Victoria, the Kings failed to find the edge required and fell for the 2nd straight year against the Smokies on home ice, this one a 4-2 decision on Friday night.
Before the game on Friday, Kent Lewis commented to me in the pre-game show that he needed to see hit counts rise and a physical edge from his hockey club moving forward. He stated that a few played only registered 3 hits in Sunday's game against Victoria, which he was openly disappointed with. Despite that focal point before the game, the Kings failed to really generate the desired level of 'edge', and ultimately lost out on that side of the contest.
Nick Nonis scores his 1st of the year and becomes the final King to notch a goal this season. This obviously excludes the goaltenders Jeff Smith and Stefan Wornig, a clarification necessary following a note (jokingly) from one fan after my tweet on Saturday. Through much of this season, both Smith and Wornig have been very good stopping goals, but if they want to start scoring them, they are most welcome.
A 3-2 deficit late in the 3rd looked set to wind up the final score, but Tristan Mullin made things real interesting in the stretch. With the net empty, he went upstairs on Smokies goaltender Bailey MacBurnie, scoring his 14th of the year. Unfortunately gamble number 2 (by pulling Wornig again) failed to yield an equalizer.
On Mullin, I'm going to spend some time this week going through his goals and seeing how many have been 3rd period markers. On nights where he isn't the most visible on the ice through 40, as I thought was the case at points on Friday, he finds another gear and ends up dominating in the 3rd.
On Wornig, 3 goals against isn't flattering with two coming early in the 1st period, but I thought he battled real well on Friday night. It was his first game action (in the BCHL) since November 1st, with only practice time and Canada West camp in between. You look at the 3 that got past him and you don't point the finger at the goaltender squarely. The Kings weren't great picking up guys in their own zone in the 1st period and we saw a lot of 2-on-1's, guys left in front of the net and as the case of the 2nd and 3rd goals, guys alone in the slot. In the 2nd and 3rd, Wornig kicked a lot away.
Saturday rolled around and so did another Coastal winter storm which meant a short trip up Island and Merritt's attempts to beat the storm resulted in the visitors leaving their hotel at 4am, arriving in Powell River at 6:00pm for a 7:15pm game. The Kings jumped on them early, then held on for a 4-3 win.
Better jump, better start and better physicality from the Kings off the hop. Why? I'm sure Merritt's lack of preparation had something to do with it, but there was a better sense of urgency from Powell River and it showed with a goal inside the opening 3 minutes through Tristan Mullin, who doubled up his game tally midway through the 1st.
2-0 through 20. 4-2 through 40 with the big blemish being a goal with 7 seconds to go in the frame. It was a goal that really should have happened with the Kings and Centennials perfectly happy to see the clock expire, the Kings started one more rush and a turnover wound up in the back of the net giving the visitors life, chasing only 2 in the 3rd instead of a more insurmountable 3.
Despite a late one from Nick Fidanza on a nice setup from Gavin Gould, the Kings literally held on. The 3rd wasn't pretty, but it was enough and it is two points. The pressure from Merritt was excellent late considering how tired the legs must have been and how little true rest the team got the night prior after a bit of a barn burner in Nanaimo.
In response to the theme of Friday's recap, the physicality was much better from the Kings who finished checks, jostled for position and out skated Merritt through a lot of the game. Gavin Rauser led the way, Chris Protopoulos had one of his better games in Powell River colours while Austin Kamer generated chances and Nick Halagian continued to be Nick Halagian.
With the win, the Kings move up into a share of 2nd in the Island Division standings with the Cowichan Valley Capitals, who play Sunday against Trail. At the close of the weekend, the Kings will be either level or up to two points back of the Caps, but with two games in hand. The Clippers lead the Division but had their 10 game streak snapped Saturday against West Kelowna. They're 8 points up but the Kings have 3 in hand and that'll move up to 4 games before Powell River plays again.
The Kings hit the road to wrap the pre-Christmas schedule, visiting Langley, Salmon Arm and Vernon beginning Friday night.


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Although the number of women in politics has grown steadily over the last century, the fact is that men still rule the world. Women make up half of the global population but 77% of national parliamentarians are men, according to 2016 UN data.
Only two countries in the world – Rwanda and Bolivia – have more women than men in national government. Just a handful more, such as Iceland, Cuba, Sweden and Nicaragua, come close to gender parity. Glancing at headlines, the names of women politicians seem to be everywhere. But female leaders such as German Chancellor Angela Merkel, British Prime Minister Theresa May or Aung San Suu Kyi, Myanmar's state counsellor, remain rare exceptions. As of January 2017, only nine women are heads of government.
Yet, you may ask, does that really matter?
Kim Campbell, who served as Canada's first and so far only female prime minister in 1993, agrees, saying that just societies require a range of perspectives.
Kim Campbell, a former prime minister of Canada. Photo: Gunnar Freyr.
But it is not just a matter of principle. Evidence shows that gender equality in politics strengthens democratic processes. According to the UN, women tend to innovate in politics by working across party lines and championing social issues that are often ignored.
When women are included in peace processes, the chances that the agreement will last at least 15 years jump by 35%, according to a 2015 report from the International Peace Institute. However, between 1992 and 2011, a mere 2% of chief mediators and 9% of negotiators at peace tables were women.
One study found that US congresswomen secure 9% more federal funding and sponsor significantly more bills than men. Other studies have found that female politicians tend to be more collaborative and congenial. Still, since there are so many factors to take into account when measuring performance and style, experts avoid making generalisations about how women act in politics.
"Often the story is: if we get more women in, society will be more feminist. They'll make it nicer and more consensual, stop corruption and bring more peace. While that may be true, it also may not be," says Professor Childs. "It depends on who the politicians are. If we link those traits to women, then we're asking something more of female politicians." Indeed, women leaders show the same level of variety as their male counterparts. Few would suggest that German Chancellor Merkel has much in common with French National Front leader Marine Le Pen.
So where is the female contingent? While laws do not prevent most women from entering politics, experts say they often face an uphill battle because of traditional gender roles, masculine political culture, sexism and lack of encouragement. The two most important indicators for whether someone runs for office are whether they have been encouraged and whether they think they are qualified, suggests research by Jennifer Lawless, director of the Women & Politics Institute and a professor at American University in Washington DC.
Professor Lawless found that women in the United States are a third less likely to be encouraged to run for office than men. This comes despite the fact that there are roughly equal numbers of men and women in "pipeline" professions for politicians — law, business, education and political activism. In many countries such as the US and the UK, women are also more likely to hold university degrees. Research even suggests that women, in Britain for example, tend to outperform men throughout primary, secondary and higher education.
A study conducted by Dr Margarita Mayo, professor of leadership at IE Business School, suggests that despite their success, women are generally more affected by criticism. She found that after her students received critical feedback, females were more likely to adjust their self-perceptions to what others thought, whereas men were more likely to continue with an inflated sense of self-confidence.
Ertharin Cousin, executive director of the UN Food Programme.
Professor Childs argues that political culture, created by and for men, must be more open to women. To make that culture more inclusive, she says that governments need quotas for women and parties must be more active in recruiting female members.
IEU Insight: IE University's intake of undergraduates in September 2016 comprised 48% women and 52% men. With students from over 100 nationalities, IEU believes diversity helps to create a unique learning experience. Students taking IEU's new degree in Politics, Law and Economics (PLE) will be empowered to become agents of change.


text:
Global IT Consultancy Xebia and digital specialist SwissQ join forces
Mumbai (Maharashtra) [India], January 11(ANI/Xebia): Globally operating IT consultancy Xebia and digital specialist SwissQ join forces, the companies announced today.
The partnership extends Xebia's geographical reach into Switzerland, gives SwissQ offshore and nearshore capabilities, and increases access to a combined 4000 technical experts globally for a joint customer base.
Fast-growing Xebia augments SwissQ's services portfolio with software development services, DevOps and SRE consultancy, enhanced data and AI consultancy, and partnerships with Amazon Web Services, Microsoft Azure, and Google Cloud. It also boosts SwissQ's training offer with its robust Xebia Academy curriculum.
SwissQ fortifies Xebia's position of authority with its world-leading technology conferences and online formats on Agile, product development, DevOps, and software quality. It also allows for broadening Xebia's geographical footprint in AI, cloud, DevOps, and SRE services.
"We are pleased to welcome SwissQ into the Xebia family" said Anand Sahay, CEO and Cofounder Xebia Global services. "Xebia has set a standard in the industry for delivering true end-to-end capabilities for Digital transformation and we are excited that SwissQ has joined us and integrated their offerings to better serve the Swiss customer from our global centres of engineering talent base. We are sure that this partnership will help SwissQ offer unique value proposition to address its customers digitization needs with innovative and cutting edge solutions.""Being part of the number one digital consulting company makes SwissQ the go-to player for digital initiatives and digital natives in Switzerland," said Adrian Zwingli, SwissQ chairman. "The partnership also brings more brilliant minds together to share knowledge, innovate and create fantastic new opportunities," he added.
Founded in 2001, Xebia quickly grew from a small Java company into a leading, global, full-service digital consultancy. With over 4,000 specialists working worldwide, it holds offices in the US, Europe, India, Vietnam, Singapore, United Arab Emirates, and the UK. Xebia continuously strives to be the leading authority in its field by partnering with other thought leaders and sharing knowledge. Its clients include Disney, Levi's, Ahold Delhaize, Tesco, Philips, and ING Bank, among many others.
Founded in 2006, SwissQ generates 90% of its revenue through consultancy and is the go-to IT training provider in Switzerland. The digital specialist continuously strives to create knowledge-sharing communities and maintain its authority in its field, organizing some of Switzerland's leading technology conferences to this end.
These include Agile Leadership Day, Business Agility Day, DevOps Fusion, and Swiss Testing Day, (this year in its 16th edition). SwissQ's clients include Credit Suisse, Zurich Insurance, Siemens, Geberit, Migros, Raiffeisen, the Swiss Confederation, Swiss Federal Railways, Sonova, and dormakaba. With offices in Zurich and Bern, SwissQ currently employs over 120 experts and has been growing steadily since its inception.
The collaboration between the two companies increases the capacity of each to support customers and build high-quality solutions for the DACH market. Both expect the partnership to benefit their colleagues as well as their joint clients, through new opportunities to work together in diversified teams on different services.
This story is provided by Xebia. ANI will not be responsible in any way for the content of this article. (ANI/ Xebia)

redpajama_set_name: RedPajamaCommonCrawl


text:
Q: Failed to build CUDA kernels for upfirdn2d on Google colab I am trying to experiment with a Deep learning framework called STIT(Stitch in Real Time), and it needs CUDA too. As I googled and found on Stackoverflow that you need to put run time on GPU in the case of google Colab and so I did. However, I get the error message
warnings.warn('Failed to build CUDA kernels for upfirdn2d. Falling back to slow reference implementation. Details:\n\n' + traceback.format_exc())
100% 98/98 [00:45<00:00,  2.13it/s]

Which results in really slow training.
Any suggestions, What should I do here?

A: ok, I don't know why but the installation of the following solved the problem
!wget https://github.com/ninja-build/ninja/releases/download/v1.8.2/ninja-linux.zip
!sudo unzip ninja-linux.zip -d /usr/local/bin/
!sudo update-alternatives --install /usr/bin/ninja ninja /usr/local/bin/ninja 1 --force

An explanation around it is appreciated

redpajama_set_name: RedPajamaStackExchange


Organizers of the Memphis Women's March hope to energize marchers toward continued activism.
Weather forecasters promised a day of rain, but showers held off long enough Saturday morning for a few hundred spirited protesters to take part in this year's Memphis Women's March.
Several hundred marchers of varying ages, races and gender identities met at Memphis City Hall and marched a few blocks to the Judge D'Army Bailey Shelby County Court House, where speakers urged participants to move from marching to activism and encouraged intersectionality.
A lead organizer, Amber Sherman, thanked everyone for attending.
"But I also want to remind you that attending a march means nothing if changed behavior doesn't follow. I want to push past marching and into activism," Sherman said, asking the crowd to embrace the rights of all women.
That sentiment was echoed by speaker Mary Thomas, 19, a student at Rhodes College, who described herself as white and middle-class and explained intersectionality, the overlap of various social identities, like race, gender and gender identity.
"To my my peers, my fellow white women, leave space. Leave space for others who have a different story to tell," Thomas said as the crowed cheered. "We must learn to listen."
Unlike the 2017 march, held the day after President Donald Trump was inaugurated, this one did not draw the nearly 6,000 people who marched on a sunny day from the county courthouse to the National Civil Rights Museum. Sister marches in cities around the globe drew millions that year.
Last year's event, a rally at First Congregational Church in Cooper Young, drew about 1,000 people.
Although the numbers this year were smaller, placards and T-shirts showed a similar level of diversity that included representatives from Black Lives Matter, the Sierra Club, local anti-violence nonprofit F.U.N.N. (Freedom from Unnecessary Negatives), the LGBT community and Madison (County) Area Democratic Women of Tennessee.
Paisley Smith, 9, from Jackson, Tennessee, marched in colorful rubber boots carrying a sign picturing U.S. Supreme Court Justice Ruth Bader Ginsburg.
"I want to be president and Donald Trump isn't letting me do that. Because he doesn't like women," she said.
Women, she said "should be allowed to do what men are allowed to do."
Paisley was with her 6-year-old sister, Devin Smith, and parents Rileyann and William Smith.
The adult Smiths were at the 2018 march, while the girls were mad that they weren't allowed to come, William Smith said.
Rileyann Smith was at the 2017 march as well.
"They're hearing all the things on TV and in the news and they wanted to be part of it also," she said.
Katherine Paxton, a registered nurse from Memphis, made sure she was off work to attend the march.
"There's no way I'm going to stay away," Paxton said. "We have to show in Memphis that we're not a part of the hate that's going on in our country right now. And even if there are some disagreements, we don't have to foster that."
At the front of the march was long-time Memphis activist "Mother" Georgia King.
"At 78 years old, I've still got boots on the ground in training young people in the area of justice," King said. "I"m out here today because of the job situation and all that they're doing in Washington, D.C."
Nationally, some Jewish women have opted not to attend the Women's March in Washington and other cities, citing comments about Israel from Women's March board members and the refusal of organizer Tamika Mallory to renounce Minister Louis Farrakhan, leader of the Nation of Islam, who has made negative comments about Jews and been accused of anti-Semitism.
U.S. Rep. Debbie Wasserman-Shultz (D-Fla.), past chairwoman of the Democratic National Committee, wrote an op-ed piece for USA TODAY, explaining why she refused to participate in the D.C. march.
But locally, Jews that include U.S. Rep. Steve Cohen, a Memphis Democrat, disagreed with that position. Cohen skipped Trump's inauguration to attend the 2017 Memphis march.
He understands why people who are Jewish have a problem with Farrakhan and why some people who are African-American have a great respect for Farrakhan and the work he has done in African-American communities.
There is no conflict in Memphis between the Jewish and the African-American communities, he said.
"This is about people coming together to support women. And we shouldn't divide ourselves," Cohen said.
Laura Goodman-Bryan is a practicing Reform Jew and attended the march wearing her symbolic pink hat.
Conservatives, Goodman-Bryan said, are willing to stand together and work out their problems within their organizations and stay on point, while liberals often don't.
"I'm here to say I can disagree with you on my religion, but we have other things that we can agree on and let's focus on those," she said.
A corporate executive, Goodman-Bryan said she knows how to get things done.
"And it is by finding points of agreement and pushing forward on those," she said. "We've got to stop fighting or we are lost."


text:
Al Qaeda and the Islamic State's Break
American University's Tricia Bacon and Georgetown University's Elizabeth Grimm Arsenault have a new article in Studies in Conflict and Terrorism journal on the break between Al Qaeda and Islamic State. The article's abstract:
Employing counterfactuals to assess individual and systemic explanations for the split between al Qaeda and the Islamic State of Iraq and al-Sham (ISIS), this article concludes that individual leaders factor greatly into terrorist alliance outcomes. Osama bin Laden was instrumental in keeping al Qaeda and ISIS allied as he prioritized unity and handled internal disputes more deftly than his successor, Dr. Ayman al-Zawahiri. Although a troubled alliance, strategic differences between al Qaeda and ISIS were not sufficient to cause the split. Rather, the capabilities of al Qaeda's leader determined the group's ability to prevent alliance ruptures.
The article is an interesting use of the counterfactual method for causal inference of explanations. The authors' focus on Dr Ayman al-Zawahiri contrasts with other explanations such as Will McCants' focus on Islamic State's apocalyptic belief system.
During my on-going PhD research at Monash University, I've increasingly focused on 'dissertation to book' studies from university presses (Cambridge, Cornell, Princeton, Stanford) that develop and test formal theories. This has been a surprise to me – given that my earlier published research used critical theory and journalism experience.
The latest study I'm looking at is Alexandre Debs and Nuno P. Monteiro's Nuclear Politics: The Strategic Causes of Nuclear Proliferation (Cambridge: Cambridge University Press, 2016). They include a puzzle and case study based approach that emphasises the pivotal role of security concerns. Their book includes coding rules and a formal theory: a useful 'writing model' for the relevant sections of my draft thesis.
Marx, Capital, and the Madness of Economic Reason by David Harvey (Oxford: Oxford University Press, 2017). One of Karl Marx's leading contemporary scholars interprets the three volume Capital in the context of post-2008 secular stagnation. Some interesting comments on how debt and extractive institutions work.
How To Be An Academic: The Thesis Whisperer Reveals All by Inger Mewburn (Sydney: University of New South Wales Press, 2017). The Thesis Whisperer explains why contemporary higher education is like The Hunger Games and offers informed advice on how to survive 'precariat' labour and build an institutional profile.
Fundamentals of Critical Argumentation by Douglas Walton (Cambridge: Cambridge University Press, 2005). The University of Windsor professor's introductory textbook on argumentation and critical reasoning.
The Economic Impact of Islamic State Governance in Iraq and Syria
RAND has a new research paper out on Islamic State's economics:
At its peak, the Islamic State of Iraq and the Levant (ISIL) controlled vast portions of territory in Iraq and Syria with several million inhabitants. ISIL's territorial ambition and desire to conduct state-like governance over this territory are integral to its global ideological appeal. By examining ISIL's impact on local economic activity in Iraq and Syria, this report seeks to assess the effectiveness of ISIL's governance over its self-styled caliphate.
This report leverages remote sensing data and commercial satellite imagery to offer a unique, data-driven look inside areas controlled by the Islamic State. It paints a bleak picture of economic life under ISIL, replete with shortages of electricity, massive refugee flows, reductions in agricultural output, and upticks in violence all associated with ISIL control.
At times, ISIL was able to build a dense governing apparatus that helped maintain stable local commercial activity, particularly in its strategic capitals in Raqqah and Mosul. At other times, ISIL mismanaged key resources or sought to punish its citizenry rather than govern it. However, this report suggests that decaying economic conditions in ISIL-held territory are also a product of ISIL's inability to insulate its territory from opposing military forces. Outside pressure against ISIL successfully prevented the group from realizing its governing ambitions across significant parts of its caliphate, with major consequences for its ability to support functioning local economies.
This report is important for those trying to understand the group's impact on local populations in Iraq and Syria, for those seeking to counter its financing or conduct post-conflict stabilization, and for broader efforts to understand the economic impact of insurgent governance.
I'll likely be citing it in my in-progress PhD chapter on Islamic State.


text:
The Reckoning: Financial Accountability and the Rise and Fall of Nations, by Jacob Soll
The Map and the Territory, by Alan Greenspan
The Billionaire's Apprentice, by Anita Raghavan
How Latin America Weathered The Global Financial Crisis, by José De Gregorio
"Capitalism and government, it seems, have flourished without massive crises only during distinct and even limited periods of time when financial accountability functions."
Greenspan weaves personal experience and a career that spanned the good part of 60 years—18 of those at the helm of the US central bank—into economic analysis.
The Billionaire's Apprentice Misses Its Aim As Indian-American Morality Play.
A highly-technical look at how the region came out of the global financial crisis in much better shape than most of its emerging market peers.
Bernanke Speaks Out In New Book
North America,
Governance, Regulation & Compliance,
United States: Former US Federal Reserve chairman Ben Bernanke lashed out at what he described as a do-nothing Congress in his new memoir, Courage to Act.
Top 25 Lists: 25 Most Influential Business & Finance Books Over 25 Years
Emerging Markets,
Foreign Exchange,
Islamic Finance,
Treasury & Cash Management,
Transformation By Justin Keay How things change. A list of the best business, economics and finance books compiled pre-crisis would probably have focused on up-and-coming Internet companies, how to make a fortune on the stock exchange, how to invest ...
Books Excerpt: Losing Control
BOOKS —LOSING CONTROL By Stephen D. King The world is witnessing a massive redistribution of wealth as the West learns it can no longer live beyond its means, says HSBC's group chief economist Stephen D. King, author of ...


This is so beautiful, Wanda! Love that background!
There's so much I love about this card! The chickenwire stencil is now on my wish list (!) and the little floral spray is gorgeous! And I love the bold sentiment. This is such a beauty!


What do Saturday morning brunch, buying a new car, and that huge project at work have in common?
They all involve some serious decision making!
Why is it that we have so many decisions to make but spend so little time thinking about the way we make them? Here are 3 (+1 ) tips on what you should think about before making any decisions (about anything).
Recently, one of our developers was worried that our app's "Forgot my password" feature was too cumbersome. The user had to take too many steps to recover their access. We agreed that it was something to improve.
Until we saw the app's analytics data.
We found that in the last three months, only 12 people forgot their password. And 11 of them swam right through the process, successfully resetting their passwords within a few minutes. That's 11 out of 12, in three months. The data showed us clearly that we don't have to–at least, straightaway–invest time to fix this thing.
In your last job, you probably used certain tools that worked really well for you.
When you came across similar situations in your current job, what popped into mind? You bet – those exact same tools you used to use!
And when your colleague asked for a suggestion for the same problem, what did you say…?
Our previous experiences shape our inclinations toward things. Biases are just like preferences, but stronger. That's why they are considered unfair.
In this situation, you have to ask yourself why you are strongly leaning on to this one thing. Be analytical about it so you can open yourself to other options and impartially weigh each one before coming up with a decision.
Executive dilemma is commonly covered in MBA – it's that important to understand!
Fundamentally, it's when you have a previous decision support the current one.
Example: you just spent a good amount of money developing a certain feature that's not in production yet. You still don't know if it is working well or not, but you already found a huge flaw. If you think that you actually have to invest more for this, that's executive dilemma.
First solution syndrome is common and straightforward: it's thinking that the first solution you come up with is the best solution. We tend to do this a lot, especially in this busy day and age. We want to fix a problem and immediately move on to the next.
Stop. Think about long-term solutions as well. Think of multiple solutions. There is no hurrying smart decision making.


Those days are long past. Danny is now a highly respected custom builder on the German scene, and has his own company, SchrammWerk GmbH. But at a custom show in Abu Dhabi, chatting to some fellow builders during the after party, he found himself reminiscing about the past. He decided to resurrect his old 50cc freedom machine.
Danny started chopping, and the next three months felt like "Christmas every day" as the parts arrived. Uwe Ehinger sourced a 1932 BSA girder fork, and TTS Motorcycles sent through a set of 23-inch 'Big Spoke' rims.


How to stay healthy after retirement?
The foremost important way to stay fit is to maintain an exercise regime. A 45-minute walk or exercise is must, go to gym or swimming. One can even plan an exercise schedule or consult a trainer. In old age, exercise plays a crucial role. It not only helps you physically, but it also refreshes your mind.
Retirement period is where one can pursue their passion. Sometimes because of circumstances or responsibilities, a person can't pursue their passion. However, after retirement a person is free from all that work stress and has the freedom to do what they want. Be it reading, writing, traveling, painting, whatever it is, retiree can do what they want.
If you ever wanted to be a part of a good cause but couldn't because of work responsibilities, then this is your time to do it. What can be a better way to spend your time than doing some social work. Not only will you utilize your time efficiently, but it will also give you a sense of satisfaction that you did something productive. It will also help boost your fitness.
This is the time to say good bye to all those bad habits that you might have picked up. Sometimes after retirement, retiree tend to become social drinkers or smokers. They confuse their leisure time with this. This is completely wrong. I am not saying one should completely quit alcohol and smoking but it is quite important to maintain tabs on your drinking or smoking schedule. This is quite important for people that take medicines.
The key factor to stay healthy is to surround yourself with a good and happy environment. We have all faced the burden of stress in our working period. The period after retirement should be blissful. Do things that make you happy. Surround yourself with loving people. Spending more time with your spouse and family. Making wonderful memories. At the end of the day, you should be at peace with yourself.
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We've expanded our network of fishing cams to include the Ala Moana Harbor fishing cam. Now it's easier than ever to check conditions at Ala Moana Harbor simply by visiting the Ala Moana Harbor fishing cam page. We've also included the latest weather forecasts, sunrise, sunset and tide information for Ala Moana Harbor so it's easy to see what conditions will be like over the next few days. Remember to check local regulations before fishing Ala Moana Harbor so you can stay informed of fishing times, license requirements and closures. Remember that marine weather conditions can rapidly change, so before you visit Ala Moana Harbor, be sure to check the latest marine weather forecasts for Ala Moana Harbor. In order to determine the current water temperatures and water clarity at Ala Moana Harbor you should view our SST and Chlorophyll charts before heading to Ala Moana Harbor. If you are interested in learning advanced bait rigging techniques and how to tie fishing knots visit Fishtrack's "how-to" section before heading to Ala Moana Harbor. Finally, submit a fishing report to Fishtrack and let others know what's biting at Ala Moana Harbor!


text:
Q: MultiPostThumbnail and the_post_thumbnail I am using built-in Wordpress function to add (small) thumbnails to each post. In addition to the post thumbnail I am using MultiPostThumbnail plugin to add custom category (large) image.
Since not all posts have thumbnails or "secondary image" (as it is called by MultiPostThumbnail plugin) I would like to display thumbnails (either large or small) in this order:

*

*If I a post has large (MultiPostThumbnails) thumbnail and (small) thumbnail display only (large) thumbnail.

*If a post doesn't have a (large) thumbnail display the (small) thumbnail.
I hope now it makes more sense. It's a simple if statement but I can't get it to work. Here is a "pseudo-code".
<?php if (class_exists('MultiPostThumbnails')
   && MultiPostThumbnails::has_post_thumbnail('post', 'secondary-image')) :
      MultiPostThumbnails::the_post_thumbnail('post', 'secondary-image', NULL,  'post-secondary-image-thumbnail');
else {
   the_post_thumbnail();
}
?>

A: In code you posted you have issue with syntax - you should stick either with braces style or colons style, mixing them is not supported.
if(class_exists('MultiPostThumbnails')
    && MultiPostThumbnails::has_post_thumbnail('post', 'secondary-image')) {

    MultiPostThumbnails::the_post_thumbnail('post', 'secondary-image', NULL, 'post-secondary-image-thumbnail');
}
else {

    the_post_thumbnail();
}


Settle into this two bedroom hunting camp or possible full time home with one bathroom! Additional sleeping area upstairs in a loft bedroom for guests! Hunting and recreational paradise located on 4.9 acres of pristine land.
This home has 2 bedrooms and 2 full bathrooms with well-crafted hard wood flooring. The master bedroom has an attached master bathroom. A gorgeous open kitchen concept with granite counter tops and all new appliances. Nice spacious living room with fireplace that can be set up for gas or electric. There is also a nice unfinished basement.
This 1991 Contemporary Hillside home with 3+ Bedrooms and Den/ office could be another 1st floor bedroom."Pergo flooring in GreatRM. Full and Master 1/2 Bathrm. House has vaulted ceilings in the great room, 3 heat sources, garage under house, new deck this year great for entertaining. Newer hot water tank and Furnace about 6 yrs old. 16x20 horse barn built in 2000 & large older barn.
Single family home with a detached garage and storage building on .50 acre. Enter from the covered front porch. The main floor includes a living room, dining room, spacious kitchen that leads to the covered patio. Also you will find a full bath and a bedroom. Upstairs you will find 2 large bedrooms with closets, a smaller bedroom with a closet and a 1/2 bath.
Opportunities are endless with this spacious home on 49.5 Acres! The 5-7 Bedrooms are large and first floor living space allows many options. Updated metal roof. Large pond. Amish built Workshop. Electric on pole very close to the home. Septic installed. Running water in house. Would make a great home, B&B or hunting lodge.
Get away from it all. Nestled on a 2.7 acre lot is this three bedroom, two bath double wide home. Located just minutes from the historic village of Angelica. It has a open floor plan with cathedral ceilings and a wood burning fireplace in the living room. It includes 3 nice sized bedrooms, the master has its own master bath and double closets. Located on a nice private, flat open lot.
Great getaway built in 2004 / post & beam built by the Amish. All mortise & tenon complete with a covered porch. Custom cherry finished cabinets with granite countertops and brand new appliances. Vaulted ceilings, loft bedrooms and heating options include wood stove, propane forced air, and backup electric.
HUNTERS PARADISE - It is listed as 3 Bedrooms but you could use the extra room on 2nd floor for another on. This is a modern house situated on almost 330 acres of prime hunting land with a view that over looks the beautiful Genesee Valley. It comes with the timber rights and 20% of the mineral rights convey.
4 bedroom, 2 bath home located at the end of a quiet dead end street. Kitchen has plenty of cupboards for storage and has newer stainless steel appliances. You can choose to eat in the kitchen or dine in the formal dining room that adjoins the kitchen. Cozy family room with a bay window and wood stove to use as secondary heat.
The cabin has had some recent updates including floors and knotty pine tongue and groove ceilings. With a little more work, this cabin would make a great camp or vacation home. Most recently, the cabin has been leased to hunters. There is a new drilled well. The 21 acres consist of mainly hardwoods with a mixture of pine trees. Lots of wildlife sign.
Many amenities come with this modified A frame including garage with workshop, outside wood boiler to keep those utility bills low, dog kennel and over three acres to enjoy. All this and a spacious three bedroom home.
Hunter's Paradise! 3 bedroom cabin can sleep 8 comfortably. Included is a full kitchen, spacious living room with wood stove and a bathroom. Enjoy nature just hanging out on the large front porch. The metal roof was recently installed. The newly built garage with concrete floor is perfect for storing ATVs and other equipment.
SECLUDED 11 ACRE PARCEL WITH SELF SUFFICIENT RANCH STYLE GETAWAY, PROPERTY HAS SOLAR PANELS AND GENERATOR WITH BATTERY STORAGE, LARGE PROPANE TANK AND WOOD STOVE. WELL AND SEPTIC.
Attention Country lovers and hunters. Use this property for Hunting Cabin or year round home. Home is situated on 15 acres of woods. 2000 sq ft 2 story amish built barn 20x58 to store all your gear. Wired for electric. Home has open kitchen, living room floor plan 1st floor laundry, full bath, 2 bedrooms on the 2nd floor. Home comes with all appliances. Tranquil woods.
This home includes a kitchen which leads into a large dining room, spacious living room, a separate room that could be an office, a mudroom and a laundry room. There is a full bath which includes an antique clawfoot bathtub. Majority of the house has beautiful parquet wooden floors. The stairs are hardwood with spindle railings. The 3 bedrooms are upstairs.


I'm not sure when it started but from what I gathered, every Chinese New Year, the Sydney Opera House and the Sydney Harbour Bridge will light up in red. It's actually quite a nice change in scene. There's also the 12 zodiac sculptures lightings spread out around Sydney city for people to come by and have a look and also take photos of them.
On the first day of Chinese New Year this year, we went over to Circular Quay hoping to catch the fireworks.
Unfortunately, we were not standing at the right place to watch the fireworks and it was really disappointing. The usual place that we would usually go to would be the Overseas Terminal to catch the fireworks but there was a big cruise ship docking over there so we couldn't get there.
So we stood in front of MCA thinking that we could see the fireworks above the Opera House, but nope, the fireworks were too low and everything was blocked by the Opera House. The only thing that we can see is some light popping behind it. It was such a disappointment. Pretty sure a whole lot of people were disappointed too. I saw so many people waiting at Circular Quay station "booking" their spot and waiting for the fireworks and from that view, you really can't see much at all too.
Have you gone out and see what's going on for Chinese New Year? Let me know which one you like best!
*All images posted here were taking with the Fujifilm X100s and editing with VSCO.


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Fali ist der Name folgender Personen:
 Fali Bilimoria (1923–2001), indischer Dokumentarfilmer
 Fali Ramadani (Abdilgafar Ramadani; * 1969), deutscher Spielervermittler
 Fali (Fußballspieler, 1983) (Rafael Brieva Primo; * 1983), spanischer Fußballspieler
 Fali (Fußballspieler, 1986) (Rafael Romero Serrano; * 1986), spanischer Fußballspieler
 Fali (Fußballspieler, 1993) (Rafael Jiménez Jarque; * 1993), spanischer Fußballspieler

redpajama_set_name: RedPajamaWikipedia


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1 Dead in Fiery Early Morning Crash Off Interstate 8 in La Mesa
Car Swerving to Avoid Coyote Hits Pole and Cuts Power to 900 in Oceanside
CDC Screening Incoming Passengers at LAX Amid Coronavirus Outbreak in China
Home » Crime » This Article
Woman Testifies She Killed Husband After He Fatally Shot Their Teenage Daughter
Posted by Debbie L. Sklar on September 26, 2017 in Crime | 145 Views
A woman charged with killing her family in their San Carlos condominium more than five years ago testified Tuesday that she shot her husband after he shot their 14-year-old daughter.
During questioning from her attorney, 60-year-old Regina Johnson denied killing her daughter, Aaliyah, but admitted killing her 56-year-old spouse, Reuben Johnson, on the morning of May 30, 2012.
"Why did you kill him?" attorney Neil Besse asked his client.
"Because he killed my daughter," she replied. "Aaliyah was the love of my life. When I lost her, I lost everything."
Johnson testified that after her husband killed Aaliyah, she picked up the gun from the ground and fired, fearing he might shoot her next.
On cross-examination, the defendant denied killing her husband because she was angry with him and thought he had been trying to poison her with painkillers.
She also testified that she didn't kill her spouse because he had cheated on her with other women.
In her opening statement, Deputy District Attorney Nicole Rooney alleged that the defendant ambushed Aaliyah, shooting her in the back of the head as she got dressed, then ambushed her husband as he came into their daughter's bedroom. He was shot in the side, then the head.
"Aaliyah was caught completely by surprise," the prosecutor said. "Her mother came up behind her and executed her. Reuben Johnson was ambushed just like his daughter."
Rooney said the crime occurred behind closed doors in the family's condominium in the 7200 block of Navajo Road.
"(There was) no one there to stop the defendant from executing her plan," the prosecutor told the jury.
Rooney said Johnson didn't call police and stayed with the decomposing bodies until concerned family members from Washington state made an emergency call for authorities to check on the family three days later.
The prosecutor said the defendant's DNA was "all over the gun," which was found next to her husband's head, and her fingerprints were also found on the gun's magazine.
The defendant also got rid of shell casings and pills she was taking for depression, according to Rooney, and used lipstick to write a message to her doctor on a bathroom mirror.
"You know I should not have been taking all those pills," the message read.
Besse told the jury that Johnson was depressed over losing her job and not being able to dote over her daughter.
The day of the shootings was picture day for Aaliyah at West Hills High School, where she was a freshman, and she had picked out a blue dress from her mother's closet, Besse said.
That morning, her father returned from a doctor's appointment and was upset that the teen was still home, Besse told the jury.
He blamed his daughter's tardiness on her boyfriend, but the defendant came to the girl's defense, according to Besse, who said the argument boiled over and Aaliyah left the room and returned with a gun, pointing it at her father.
"She said, `Stop yelling at me,"' Besse told the jury.
He said Reuben Johnson knocked the gun from his daughter's hands and a shot rang out, killing her on the spot.
The defense attorney said his client picked up the gun and yelled at her husband, "What did you do? You shot my baby girl!" and then fired two shots, killing him.
Besse said his client covered her daughter's body and stayed with her until police arrived three days later.
Johnson faces 100 years to life in prison if convicted of two murder counts.
Woman Testifies She Killed Husband After He Fatally Shot Their Teenage Daughter was last modified: September 26th, 2017 by Debbie L. Sklar
Posted in Crime | Tagged daughter, fatal, husband, killed, Regina Johnson, Reuben Johnson, San Carlos, spouse, testifies
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*Local medical students should receive an application form from your respective class representative(s). Alternatively, applicants can write in to the SingHealth PGY1 Programme at PGY1@singhealth.com.sg to request for a copy of the form.
Applicants for Residency training programmes are required to submit their portfolios and work-based assessments and apply for interviews to get into their selected specialties. Applicants will also undergo the match to their selected specialties and sponsoring institutions.
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Please email to physician@mohh.com.sg if you have further specific personal enquiries concerning entry into the residency training.
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Residents may contact the respective Senior Residency Programme via their programme email if they wish to get in touch with the Programme Directors.


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text:
\section{Introduction}
\label{intro}
Dipolar gases are the focus of extensive experimental and theoretical research, motivated by the possibility that yet unobserved, exotic phases of matter may be underlain by the distinctive character of the  inter-particle interaction, both long ranged and anisotropic \cite{menotti}. In particular, the experimental achievement of Bose-Einstein Condensation of  atomic systems with large magnetic moments \cite{griesmeier,lu,aikawa,depaz,ni,yan,takekoshi,park,balewski}
suggests that one might be able to predict and observe phases featuring more than one type of order.
Of particular interest is the supersolid phase, which spontaneously breaks both continuous translational and global U(1) symmetries, thus featuring simultaneously crystalline order and flow without dissipation (see, for instance, Ref. \cite{rmp}).
\\ \indent
As supersolid behavior in a crystal of $^4$He, once deemed the most promising candidate, has so far eluded unambiguous observation, dipolar bosons have been suggested as a likely physical setting for its detection in various experimental \cite{wentzel,ferlaino} and theoretical \cite{cinti10,jltp,cinti} works. In Ref. \cite{cinti}, for instance,  it is contended  that, if dipole moments are aligned, an ordered array of filaments (or, prolate droplets) constitutes the ground state of the system in rather broad conditions, and preliminary evidence of global phase coherence among such droplets was offered for specific values of density and interaction parameters.
\\ \indent
It seems now accepted that the appearance of filaments in this system is the result of the competition between the attractive part of the dipolar interaction, and the presence of a short range repulsion, which prevents the system from collapsing. Such a repulsive part is often modeled theoretically through the so-called scattering length approximation. Because the scattering length is experimentally controllable and can be varied  by means of the Feshbach resonance (see, for instance, Ref. \cite{feshbach}),  the possibility arises of exploring the quantum phase diagram of the system in its entirety, at least within known limitations (e.g., three-body recombination) \cite{fb,pfau2,ferlaino3,ferlaino2}. A comprehensive theoretical study of the bulk phase diagram of the system at low temperature based on reliable, first principle computational methods, aimed at helping in the design and interpretation of present and future experiments, seems therefore timely \cite{lastnote}.
\\ \indent
In this work, we carry out state-of-the-art Quantum Monte Carlo (QMC) simulations to investigate the low temperature phase diagram of dipolar bosons with aligned  dipole moments. We model the repulsive part of the interaction by means of an inverse power law potential, as done in previous work \cite{cinti}; a straightforward connection exists   between the characteristic range $\sigma$ of this interaction, and the scattering length $a_s$. We map out the phase diagram  by computing relevant correlations, as well as the superfluid density, all directly accessible in our numerical approach, as a function of particle density and $\sigma$.
\\ \indent
The system displays several distinct phases, ranging from an essentially classical crystal of parallel, particle-thin filaments in one limit ($\sigma\to 0$), to a hard-sphere-like superfluid, reminiscent of liquid $^4$He in the opposite ($\sigma\to\infty$) limit, at any particle density. An intermediate region exists between these two phases, in which the ground state displays both crystalline order and a finite superfluid response. This {\em supersolid} phase exists within a range of scattering length that  depends monotonically on the density.
\\ \indent
The crystal structure of the supersolid is quite distinct from that of the classical crystal,  determined by quantum-mechanical effects, both zero-point motion as well as exchanges of particles (as already noted in Ref. \cite{cinti}). Remarkably, the supersolid phase features
different arrangements of particles (patterns) in different regions of the phase diagram. At low density, the supersolid phase consists of  a crystal of prolate droplets, with quantum-mechanical exchanges of particles across droplets, as suggested in Ref. \cite{cinti}. As the density is increased, on the other hand, the patterns resemble some of the periodic structures originally predicted to occur in two-dimensional dipolar systems \cite{vanderbilt,spivak}.
\\ \indent
We study the elementary excitation spectrum for the superfluid phase, which features the experimentally observed ``roton'' minimum \cite{ferlaino}, as crystallization is approached from the superfluid side, {\em both} on {\em reducing} $\sigma$ (i.e., moving toward the supersolid phase) as well as on {\em increasing} it, in which case the system behaves essentially as a hard sphere fluid, transitioning into a conventional (i.e., non-superfluid) crystal.
\\ \indent
The remainder of this paper is organized as follows: in section \ref{mo} we describe the model of the system; in Sec. \ref{me} we briefly describe our methodology; we present and discuss our results in Sec. \ref{else} and finally outline our conclusions in Sec. \ref{conc}, where we discuss the relevance of this study to recent experimental work.

\section{Model}\label{mo}
The system is modeled as an ensemble of $N$ identical particles of mass $m$ and spin zero, hence obeying Bose statistics. These particles possess a magnetic moment $d$, pointing in the  $z$-direction. We are interested in studying the phase diagram of the {\em bulk}; thus, unlike in a typical experiment, we do not confine the simulated system by means of an external potential. Rather, our system is enclosed in a three dimensional box, shaped like a cuboid of volume $V$, with periodic boundary conditions in the three directions.  The shape of the cell was varied, depending on the particular structures and patterns forming at the various physical conditions. We take the characteristic length of the dipolar interaction, $a \equiv md^2/\hbar^2$ as our unit of length, and $\epsilon \equiv \hbar^2/(ma^2)$, as that of energy and temperature.  The quantum-mechanical many-body Hamiltonian in dimensionless form reads as follows:
\begin{eqnarray}\label{u}
\hat H = - \frac{1}{2} \sum_{i}\nabla^2_{i}+\sum_{i<j}U({\bf r}_i,{\bf r}_j)
\end{eqnarray}
where the first (second) sum runs over all particles (pairs of particles), and the pair potential consists of two parts, $U({\bf r},{\bf r}') = U_{sr}(|{\bf r}-{\bf r}'|) + U_d({\bf r},{\bf r}')$, $U_{sr}$ being the repulsive part.
As mentioned above, in most theoretical studies the repulsive part of the interaction is modeled by means of the so-called scattering length approximation, namely
\begin{equation}\label{sla}
U_{sr}(r) = \frac{4\pi\hbar^2 a_s}{m} \ \delta({\bf r})
\end{equation}
To the extent that such a representation is valid, expression (\ref{sla}) can be replaced by any other potential that has the same scattering length $a_s$. In this work, we use for $U_{sr}$
the repulsive part of the standard Lennard-Jones potential, i.e.,
\begin{equation}\label{Usr}
U_{sr}(r)=(\sigma/r)^{12}
\end{equation}
whose use is more convenient in numerical simulations. The parameter $\sigma$ of the potential $U_{sr}$ used here is directly related to the scattering length $a_s$, through
\begin{equation}\label{as2}
\frac{a_s}{\sigma} \approx 0.76\ \sigma^{1/5}
\end{equation}
(see, for instance, Ref. \cite{flugge}).
$U_{d}$ is the classical dipolar interaction between two aligned dipole moments, namely
\begin{equation}\label{Ud}
U_d({\bf r},{\bf r}')=\frac{1}{|{\bf r}-{\bf r}'|^3}\left(1-\frac{3(z-z')^2}{|{\bf r}-{\bf r}'|^2}\right)
\end{equation}
\\ \indent
At zero temperature there are two parameters that govern the physics of the system, namely the particle density $\rho\equiv N/V$, and the characteristic range $\sigma$ of the repulsive interaction. The classical limit is approached as $\sigma\to0$, whereupon the attractive well of the anisotropic interaction becomes deep enough to dominate the physics, and quantum mechanical effects are small. On the other hand, as $\sigma$ is increased, quantum mechanical effects are increasingly prominent, eventually destabilizing the classical ground state and giving rise to interesting physics.

\section{Methodology}\label{me}
We carry out QMC simulations of the system described in section \ref{mo} using the continuous-space worm algorithm \cite{worm,worm2}. We shall not review the details of this method, referring instead the reader to the original references. We utilized a canonical variant of the algorithm in which the total number of particles $N$ is held constant, in order to simulate the system at fixed density \cite{mezz1,mezz2}. Although this is a finite temperature technique, we perform simulations at sufficiently low temperatures, so that computed physical properties are essentially those of the ground state.
\\ \indent
We survey the phase diagram of the system by performing simulations at a fixed density for different values of $\sigma$, and then repeating the process for different values of the density. We performed simulations of systems of sizes ranging from $N=160$ to $N=648$ particles, and densities between $\rho=0.125$, which is close to the value of some of the current experiments \cite{ferlaino}, up to three orders of magnitude higher, i.e., $\rho=100$, quite likely not attainable in present time experiments but nonetheless of fundamental interest.
To ensure that the physics is independent of the initial configuration of the particles, most simulations were started from high-temperature, disordered configurations.
\\ \indent
Details of the simulation are standard; we made use of the primitive approximation for the high-temperature density matrix. Although more accurate  forms exist, we found that in practice with this particular interaction the primitive approximation is the most efficient. All of the results quoted here are extrapolated to the limit of time step $\tau\to 0$; quite generally we found numerical estimates for structural and superfluid properties of interest here obtained with a value of the time step $\tau\sim 10^{-3}\epsilon^{-1}$ to be indistinguishable from the extrapolated ones, within the statistical uncertainties of the calculation.
\\ \indent
Occurrence of crystalline order in the system can be detected through the calculation of the static structure factor $S({\bf q})$; because of the anisotropy of the interaction and the ensuing tendency of the system to form filaments along $z$ (the direction of alignment of the dipole moments), we computed $S({\bf q})$ for {\bf q}-vectors lying in the $xy$ plane. As mentioned above, distinct, characteristic patterns form for different values of the parameters $\rho, \sigma$. The identification of the various patterns is achieved through visual inspection of the configurations generated by the algorithm in the course of sufficiently long computer runs.
\\ \indent
The superfluid response of the system is assessed through the direct calculation of the superfluid fraction $\rho_S(T)$, by means of the well-known winding number estimator \cite{pollock}. Due to the anisotropic nature of the interaction, and consequently of the superfluid (and supersolid) phases observed here, we offer results for the in-plane ($xy$) superfluid response only, throughout this paper. A typical result for the in-plane superfluid fraction $\rho_S$ is shown in Fig. \ref{phase}b.

\section{Results}\label{else}
\subsection{Phase diagram}\label{phasediagram}
The ground state phase diagram of the system, as it emerges from our extensive QMC simulations, is shown in Fig. \ref{phase}a in the $\rho-\sigma$ plane. Here we outline some of its generic features, offering a more detailed discussion of the two most interesting phases (the supersolid and the superfluid) in subsections \ref{supersolid} and \ref{superfluid}.
\begin{figure}[h]
\centering
\includegraphics[width=1\textwidth]{phase}
\caption{  (a) Ground state phase diagram of the system in the $(\rho,\sigma)$ plane. Each phase is determined through simulations as explained in the text. (b) Superfluid fraction ($xy$ plane) of the system at $\rho=100$ and $\sigma=0.18$ as a function of temperature, and for two system sizes.}
\label{phase}
\end{figure}
\\ \indent
For any fixed value of the density, two clear physical limits can be easily identified, more intuitively discussed in terms of the average interparticle distance $b\equiv \rho^{-1/3}$. Specifically, if $\sigma << b$ the ground state of the system consists of an ordered array (a triangular lattice) of thin filaments oriented along the $z$-direction. An example is shown in Fig. \ref{str1}a, displaying the density of the system, integrated along the  $z$-direction \cite{morepr}.
In this physical limit, the depth of the attractive well of the dipolar interaction causes the potential energy to dominate  the behavior of the system, which can be understood and predicted quantitatively along classical lines, as shown in Ref. \cite{cinti}. Specifically, the system forms an ordered array of particle-thin parallel filaments, arranged on a triangular lattice. In this case, exchanges of identical particles are suppressed, both within a filament, as well as across filaments.
\\ \indent
Conversely, when $\sigma$ becomes of the order of the interparticle distance $b$, the attractive well of the dipolar interaction weakens, and the physics of the  system morphs into that of a hard-sphere fluid, as the repulsive part of the interaction becomes the dominant feature. The behavior of the system in this limit is very similar to that of superfluid $^4$He, which undergoes ``conventional" crystallization as $\sigma \sim b$ (this part of the phase diagram is not shown in Fig. \ref{phase}a).
\\ \indent
As shown in Fig. \ref{phase}a, there is in an intermediate range of $\sigma/b$ wherein the system displays the most interesting, novel behavior, specifically a supersolid phase, which we discuss in detail in subsection \ref{supersolid}. A remarkable feature of this phase diagram is that there is no way of going from the superfluid to the insulating crystalline phase at zero temperature, by varying $\rho$ and/or $\sigma$, without going through a supersolid phase. This is also the case in a  2D system of soft core bosons \cite{saccani}.

\begin{figure}[h]
\centering
\includegraphics[width=0.85\textwidth]{f1}
\caption{ Density maps of the system at density $\rho=100$ for $\sigma=0.12$ (a), and  $\rho=1$ for $\sigma=0.33$ (b), integrated along the $z$-direction (i.e., the direction of dipole moment alignment). Brighter areas indicate higher density. The maps are obtained from particle world lines of a single configuration. In (a), the physics of the system is dominated by the potential energy, and the ground state is essentially the classical one, consisting of an array of particle-thin, parallel filaments. In (b), the ground state is a crystal of droplets with frequent quantum mechanical exchanges among adjacent droplets, leading to a finite superfluid response (as such displaying supersolid behavior).}
\label{str1}
\end{figure}
\indent
\subsection{Supersolid}\label{supersolid}
The supersolid phase is generally characterized by the formation of relatively large, prolate droplets, elongated along the $z$-direction, arranging themselves on a triangular lattice or forming more complex structures, as we discuss below. Quantum mechanical exchanges of identical particles, largely suppressed in the classical filament crystal, become important, initially within a single filament \cite{super} and progressively across filaments, establishing phase coherence and leading to a finite, three-dimensional superfluid response throughout the system. It is interesting to note that while the superfluid response is anisotropic, and in the $xy$ plane saturates to a value lower than unity as $T\to 0$ (see Fig. \ref{phase}b), as expected \cite{leggett}, it is always seen to approach unity, in the same limit, in the direction of elongation of the droplets ($z$).
\\ \indent
The  range of values of $\sigma$ within which the system displays supersolid behavior depends on the density of the system, as shown in Fig. \ref{phase}a; in particular, at high density the supersolid occurs for lower values of $\sigma$, as quantum-mechanical exchanges are favored by a lower interparticle distance.
The width in $\sigma$ of the supersolid region, however, appears to be roughly independent of $\rho$.
\\ \indent
As mentioned above, the occurrence of an ordered arrangement can be established through the calculation of the static structure factor, which develops (Bragg) peaks in correspondence of relevant wave vectors (e.g., the inverse distance between droplets). Additional information comes from the direct visual inspection of the patterns that form in the course of the simulation, which are quantum-mechanical in nature and can be markedly different, depending on both the density and the value of $\sigma$.
\\ \indent
Fig. \ref{str1}b shows the same type of density map as in Fig. \ref{str1}a, but for a supersolid system. As one can see, the filaments are in this case replaced by larger droplets, which include considerably more particles than the classical filaments \cite{important}. Quantum-mechanical exchanges among adjacent  droplets are frequent at low temperature (i.e., $T\sim 1$ for this particular choice of $\rho,\ \sigma$); consequently, macroscopic exchange cycles (i.e., comprising nearly {\em all} the particles in the system) take place.
Clearly, the density map shown in Fig. \ref{str1}b is very reminiscent of those that appear in a purely two-dimensional (2D) system of soft core bosons \cite{saccani,saccani2}, namely the simplest supersolid. Indeed, the physics of the system under study here, projected onto the plane perpendicular to the filaments, could be regarded as equivalent to that of a 2D soft core system, the third dimension serving the purpose of "piling up" particles, thus allowing for the formation of ``cluster'' unit cells.
\\ \indent
It is quite interesting to note that the supersolid phase does not always display the structure shown in Fig. \ref {str1}b. Rather, at high particle density patterns begin to emerge, such as the inverted droplet structure shown in Fig. \ref{str2}a, and the striped one \cite{cintiboninsegni} of Fig. \ref{str2}b, or others that are evocative of those predicted for 2D dipolar systems, in the context of ``microemulsions'' \cite{vanderbilt,spivak}
\begin{figure}[h]
\centering
\includegraphics[width=0.85\textwidth]{f2}
\caption{  Density maps of the system at density $\rho=100$, for $\sigma=0.18$ (a), and $\rho=19$, for $\sigma=0.22$ (b), integrated along the $z$-direction. Brighter areas indicate higher density. These maps are obtained from particle world lines of a single configuration.}
\label{str2}
\end{figure}

\subsection{Superfluid}\label{superfluid}
The superfluid phase arises as the range of the repulsive interaction $U_{sr}$ (eq. \ref{Usr}) is progressively increased, at fixed density, as shown in Fig. \ref{phase}a. As the droplets expand, due to the hard core repulsion, they eventually merge, giving rise to a uniform superfluid phase. It is interesting to study the elementary excitation spectrum of the superfluid phase, especially as crystallization is approached.
\\ \indent
Although it is possible to infer the excitation spectrum from the full imaginary time dynamics, computed by QMC, using an inversion method (e.g., MaxEnt \cite{ceperley,maxent}), because we are only interested here in gaining qualitative understanding we make use of a simpler approach, based on
the Bijl-Feynman approximation \cite{feynman54}. Specifically, we assume that the dynamic structure factor $S({\bf q},\omega)$ is dominated by a single peak, which allows one to obtain the elementary excitation spectrum as
\begin{equation}\label{bijl}
e(q) = \frac {q^2}{2S(q)}
\end{equation}
Eq. \ref{bijl}, known as Bijl-Feynman formula, provides a reasonable qualitative and semi-quantitative account of the elementary excitation spectrum in superfluid $^4$He, in particular of the presence and position of the roton minimum \cite{glyde}.
\\ \indent
The behavior of the excitation spectrum as a function of $\sigma$ is the same across all values of density investigated in our simulations. Fig \ref{eq} shows two examples, for  $\rho=1.0$ and $\rho=100$. The phonon-like dispersion that is characteristic of the superfluid phase at low $q$ starts acquiring a negative curvature as the superfluid-supersolid transition is approached from above (with reference to the phase diagram shown in Fig. \ref{phase}a. At values of $\sigma$ sufficiently close to the critical value, the system experiences stronger density fluctuations at that value of the momentum, giving rise to a roton minimum and signaling incipient crystallization.
\begin{figure}[h]
\centering
\includegraphics[width=0.91\textwidth]{eq}
\caption{  Elementary excitation spectra of a system of dipolar bosons for different values of the repulsive radius $\sigma$ near the superfluid-supersolid transition, computed using eq. \ref{bijl}. Results shown here are for $\rho=1$ (a) and $\rho=100$ (b), in the low temperature limit. Statistical errors are smaller than the size of the symbols. Solid  lines are fits to the data using Pad\'e approximants, and are only meant as a guide to the eye. Insets show the corresponding in-plane static structure factor $S(q)$, averaged over all directions. In (a), yellow circles refer to $\sigma=0.33$, for which crystal order appears, i.e., the system is in the supersolid phase. In (b), this happens at $\sigma=0.18$}
\label{eq}
\end{figure}
\\ \indent
These results are at least in qualitative agreement with the experimental data in Ref. \cite{ferlainopreprint}. As the value of $\sigma$ is lowered, the roton minimum becomes progressively lower, eventually hitting the horizontal axis; that is consistent with the divergence of $S(q)$ at the roton wave vector, i.e., the formation of a dipolar crystal. We come back to a more extensive comparison of our results with experiment in the next section.
\\ \indent
It is important to note that the presence of a roton minimum in the elementary excitation spectrum merely signals the proximity of the system to crystallization. As such, it is not a special feature of this particular system, or of the character of the interaction (dipolar).
Indeed, a roton minimum can be observed in the large $\sigma$ limit, in which the system is essentially a gas of hard spheres, as the crystal (in this case a conventional one, i.e., with few particles per unit cell) is approached from below. In the latter case, the roton minimum forms at a different, higher value of the wave vector, which reflects the fact that the ensuing crystal structure in this case has a smaller lattice constant.

\section{Conclusions}\label{conc}
We carried out extensive QMC simulations of a system of dipolar Bose particles of spin zero, in three dimensions, in order to gain insight into the phase diagram of this system. The anisotropic character of the interaction  gives rise to novel phases, chiefly a supersolid characterized by various, intriguing density patterns.
\\ \indent
The supersolid phase appears to be observable in a relatively broad range of parameter space, obviously making allowance for the difficulty of exploring the high density phase, as three-body recombination must be overcome.
\\ \indent
The results presented here are consistent with recent experimental data \cite{ferlainopreprint,tanzi,pfaupreprint,newferlaino}. In order to assess whether the density range explored here is comparable to that of recent experiments, we consider  Ref. \cite{newferlaino}, reporting measurements carried out on an assembly of $^{164}$Dy atoms. Using their numbers, namely $N=3.5\times{10^4}$ atoms confined in an anisotropic harmonic potential of characteristic frequencies equal to 300, 16 and 22 Hz, we estimate the density at the center of the trap  $\sim 1.3\times 10^{-8}$\ \AA$^{-3}$. Expressed in units of the dipolar length $a$, which in this case is worth 208 \AA\ \cite{factorofthree}, this is equal to 0.117, i.e., very close to the lowest density considered in this work. Indeed, the results shown in Fig. 1g of ref. \cite{newferlaino} indicate that the transition between a uniform BEC and a supersolid occurs in correspondence of a scattering length $a_s \sim 0.24\ a$, which is in remarkable quantitative agreement with our prediction of $\sigma\sim 0.4\ a$ for $\rho=0.125$ (Eq. \ref{as2} yields  $\sigma=0.38$ if $a_s=0.24$).
\\ \indent
This result provides strong quantitative support for the microscopic model utilized here, as well as for the results of our calculation. It also suggests that the experimental findings of Ref. \cite{newferlaino} reflect the physics of the bulk, to an appreciable extent, i.e., they are not overly affected by confinement, nor by the relatively small size of the system.
This observation is consistent with the conclusions of a recent theoretical (mean-field) study of the system confined in an elongated trap \cite{ancilotto}, whose results are in qualitative agreement with ours.

\section*{Acknowledgments}
This work was supported by the Natural Sciences and Engineering Research Council of Canada, as well as ComputeCanada. Useful conversations with F. Cinti, S. Moroni and F. Ferlaino are also gratefully acknowledged.

\section*{Conflict of interest}
The authors declare that they have no conflict of interest.

redpajama_set_name: RedPajamaArXiv


Imagine the feeling of peering through the doorway of your next home, make-believe you are able to catch a glimpse of the size, shape and colors of the rooms visible from your perspective. Next, step inside and get a sense for the texture of the flooring beneath your feet. With your hands, trace the countertop surfaces. Feel the temperature of the room around you. Now ask yourself, is it time to change or modify my current home layout, design or feel?
This is how I invite new home buyers to experience their next home before we find it together. Imagination differs for everybody. What is universal however, is the value of clarity combined with action. The trick is to align your values and expectations with what you want, then patiently moving towards your goal.
The fall and winter is a great time to take stock and update your current home or plan your next move. I am fortunate to work with the finest decorators, contractors and installers in real estate. If you know someone who would benefit from a referral to one of my trusted friends in the business, I would be delighted to introduce someone who shares my high standards.


Depending on the variety of vegetables to be blanched, bring several small pots of lightly salted water to a boil.
Separate each of the cauliflower florets and place the florets in a food processor and pulse until the cauliflower resembles cous cous. Transfer the cauliflower "cous cous" to a sauté pan, add enough water to cover the bottom of the pan and gently cook over low heat, stirring occasionally, until cooked through and most of the water has evaporated, about 5 minutes. Strain and place in a mixing bowl to cool.
Prepare the vegetables for blanching; cook each of the vegetables in a separate pot of boiling water, drain and shock in an ice water bath. Transfer to a towel-lined tray or plate and set aside.
Season the cooked cauliflower cous cous with lemon juice, olive oil, mint and parsley; set aside.
Combine Dijon mustard and Champagne vinegar in a mixing bowl and season to taste with salt and pepper. Drizzle in the argan oil and just enough canola oil to balance out the acidity while whisking constantly. Reserve.


text:
Q: Dynamic array of abstract class I have an abstract base class called CBase and two other classes CDerived1 and CDerived2 that are derived from CBase.
How would I now create a dynamic array (i.e. add and delete elements at runtime) of CBase? Of course, this array would just contain objects of the derived classes because the base class is abstract.
I would try something like this:
CBase* arr;
arr = (CBase*) malloc(arrSize*sizeof(CBase));

It feels like this solution would get complicated when I want to resize the array as I want. How would I do that? Or do you recommend any other kind of array for that?

A: You are allocating an array of CBase objects, so it will suffer from object slicing when you try to assign derived objects to the array elements. What you really need is an array of CBase* pointers instead:
CBase** arr;
arr = new CBase*[arrSize];

arr[0] = new CDerived1;
...

for (int i = 0; i < arrSize; ++i)
    delete arr[i];
delete [] arr;

That being said, you really should use std::vector instead of new[], and in C++11 and later, prefer std::unique_ptr instead of raw pointers:
#include <vector>
#include <memory>

std::vector<std::unique_ptr<CBase>> arr;
arr.reserve(arrSize);

arr.push_back(std::unique_ptr<CBase>(new CDerived1));
// or, in C++14 and later:
// arr.push_back(std::make_unique<CDerived1>());
...

//no manual cleanup needed!


Three years ago we took a deep look at the future of ecommerce and made the decision to explore the potential of artificial intelligence in retail–mainly because brands and retailers had not yet cracked the code on what is now known as "conversational commerce." Although ecommerce continued to grow exponentially, companies hadn't changed much about the actual online shopping experience for decades, leaving shoppers at the mercy of traditional navigation trees, keyword searches and filtering to find the right product for them.
When the IBM Watson team invited us to be an original member of their new partner ecosystem, the challenge was deceptively simple: how could we solve this problem?
How could artificial intelligence and cognitive computing help consumers better find the right products to meet their needs?
And so, with that as our direction, we went to work.
Understanding that Watson and other AI technologies could mimic human thinking and decision making, we focused on where the most human retail experience was–and that was in a physical store. We knew that shoppers in-store could receive expert assistance in discovering products for their specific needs, which was much more labor-intensive when the shopping happened online.
Working with The North Face, we conducted in-store shopper studies, shadowed store associates and tested some initial digital concepts. We found that shoppers really wanted to be helped and that they need help to understand the differences, nuances and attributes among products to make the best choice. In order to truly personalize a shopping experience we needed to bring that in-store, expert conversation online.
We built Fluid XPS (Expert Personal Shopper), a dialog-driven product recommendation system powered by IBM Watson. The result is a two-way, real time conversation where shoppers can express their needs in their own words and get expert help and recommendations that best fit those needs.
We are proud that The North Face was our first partner for Fluid XPS, and the industry's first brand to bring this level of personalization to their customers.
Today, with this technology expanding across The North Face product line and being used in ever more sophisticated ways at 1-800-Flowers, we realize the significant and broad market applicability for Fluid XPS. It made sense for IBM to acquire the technology so it can be enhanced and deepened and taken to the next level for brands around the globe.
We see this as a strong validation of our vision–which is to listen to consumers, find new and innovative ways to meet their needs and to take risks with new customer experiences and technology. We believe this is what the agencies of tomorrow will look like–uniting technology, vision and execution to deliver real world solutions for retailers and brands.
At Fluid, we've been innovating in ecommerce for 18 years and look forward to keeping pace with the next generation of consumers.
SEE ALSO: How Conversational Is Your Commerce?


text:
package packetinjector

import (
	json "encoding/json"
	easyjson "github.com/mailru/easyjson"
	jlexer "github.com/mailru/easyjson/jlexer"
	jwriter "github.com/mailru/easyjson/jwriter"
)

// suppress unused package warning
var (
	_ *json.RawMessage
	_ *jlexer.Lexer
	_ *jwriter.Writer
	_ easyjson.Marshaler
)

func easyjsonFac7b200DecodeGithubComSkydiveProjectSkydivePacketinjector(in *jlexer.Lexer, out *PacketInjectionRequest) {
	isTopLevel := in.IsStart()
	if in.IsNull() {
		if isTopLevel {
			in.Consumed()
		}
		in.Skip()
		return
	}
	in.Delim('{')
	for !in.IsDelim('}') {
		key := in.UnsafeString()
		in.WantColon()
		if in.IsNull() {
			in.Skip()
			in.WantComma()
			continue
		}
		switch key {
		case "UUID":
			out.UUID = string(in.String())
		case "SrcIP":
			if data := in.UnsafeBytes(); in.Ok() {
				in.AddError((out.SrcIP).UnmarshalText(data))
			}
		case "SrcMAC":
			if in.IsNull() {
				in.Skip()
				out.SrcMAC = nil
			} else {
				out.SrcMAC = in.Bytes()
			}
		case "SrcPort":
			out.SrcPort = uint16(in.Uint16())
		case "DstIP":
			if data := in.UnsafeBytes(); in.Ok() {
				in.AddError((out.DstIP).UnmarshalText(data))
			}
		case "DstMAC":
			if in.IsNull() {
				in.Skip()
				out.DstMAC = nil
			} else {
				out.DstMAC = in.Bytes()
			}
		case "DstPort":
			out.DstPort = uint16(in.Uint16())
		case "Type":
			out.Type = string(in.String())
		case "Count":
			out.Count = uint64(in.Uint64())
		case "ICMPID":
			out.ICMPID = uint16(in.Uint16())
		case "Interval":
			out.Interval = uint64(in.Uint64())
		case "Mode":
			out.Mode = string(in.String())
		case "IncrementPayload":
			out.IncrementPayload = int64(in.Int64())
		case "Payload":
			out.Payload = string(in.String())
		case "Pcap":
			if in.IsNull() {
				in.Skip()
				out.Pcap = nil
			} else {
				out.Pcap = in.Bytes()
			}
		case "TTL":
			out.TTL = uint8(in.Uint8())
		default:
			in.SkipRecursive()
		}
		in.WantComma()
	}
	in.Delim('}')
	if isTopLevel {
		in.Consumed()
	}
}
func easyjsonFac7b200EncodeGithubComSkydiveProjectSkydivePacketinjector(out *jwriter.Writer, in PacketInjectionRequest) {
	out.RawByte('{')
	first := true
	_ = first
	{
		const prefix string = ",\"UUID\":"
		out.RawString(prefix[1:])
		out.String(string(in.UUID))
	}
	{
		const prefix string = ",\"SrcIP\":"
		out.RawString(prefix)
		out.RawText((in.SrcIP).MarshalText())
	}
	{
		const prefix string = ",\"SrcMAC\":"
		out.RawString(prefix)
		out.Base64Bytes(in.SrcMAC)
	}
	{
		const prefix string = ",\"SrcPort\":"
		out.RawString(prefix)
		out.Uint16(uint16(in.SrcPort))
	}
	{
		const prefix string = ",\"DstIP\":"
		out.RawString(prefix)
		out.RawText((in.DstIP).MarshalText())
	}
	{
		const prefix string = ",\"DstMAC\":"
		out.RawString(prefix)
		out.Base64Bytes(in.DstMAC)
	}
	{
		const prefix string = ",\"DstPort\":"
		out.RawString(prefix)
		out.Uint16(uint16(in.DstPort))
	}
	{
		const prefix string = ",\"Type\":"
		out.RawString(prefix)
		out.String(string(in.Type))
	}
	{
		const prefix string = ",\"Count\":"
		out.RawString(prefix)
		out.Uint64(uint64(in.Count))
	}
	{
		const prefix string = ",\"ICMPID\":"
		out.RawString(prefix)
		out.Uint16(uint16(in.ICMPID))
	}
	{
		const prefix string = ",\"Interval\":"
		out.RawString(prefix)
		out.Uint64(uint64(in.Interval))
	}
	{
		const prefix string = ",\"Mode\":"
		out.RawString(prefix)
		out.String(string(in.Mode))
	}
	{
		const prefix string = ",\"IncrementPayload\":"
		out.RawString(prefix)
		out.Int64(int64(in.IncrementPayload))
	}
	{
		const prefix string = ",\"Payload\":"
		out.RawString(prefix)
		out.String(string(in.Payload))
	}
	{
		const prefix string = ",\"Pcap\":"
		out.RawString(prefix)
		out.Base64Bytes(in.Pcap)
	}
	{
		const prefix string = ",\"TTL\":"
		out.RawString(prefix)
		out.Uint8(uint8(in.TTL))
	}
	out.RawByte('}')
}

// MarshalJSON supports json.Marshaler interface
func (v PacketInjectionRequest) MarshalJSON() ([]byte, error) {
	w := jwriter.Writer{}
	easyjsonFac7b200EncodeGithubComSkydiveProjectSkydivePacketinjector(&w, v)
	return w.Buffer.BuildBytes(), w.Error
}

// MarshalEasyJSON supports easyjson.Marshaler interface
func (v PacketInjectionRequest) MarshalEasyJSON(w *jwriter.Writer) {
	easyjsonFac7b200EncodeGithubComSkydiveProjectSkydivePacketinjector(w, v)
}

// UnmarshalJSON supports json.Unmarshaler interface
func (v *PacketInjectionRequest) UnmarshalJSON(data []byte) error {
	r := jlexer.Lexer{Data: data}
	easyjsonFac7b200DecodeGithubComSkydiveProjectSkydivePacketinjector(&r, v)
	return r.Error()
}

// UnmarshalEasyJSON supports easyjson.Unmarshaler interface
func (v *PacketInjectionRequest) UnmarshalEasyJSON(l *jlexer.Lexer) {
	easyjsonFac7b200DecodeGithubComSkydiveProjectSkydivePacketinjector(l, v)
}
func easyjsonFac7b200DecodeGithubComSkydiveProjectSkydivePacketinjector1(in *jlexer.Lexer, out *Injections) {
	isTopLevel := in.IsStart()
	if in.IsNull() {
		in.Skip()
		*out = nil
	} else {
		in.Delim('[')
		if *out == nil {
			if !in.IsDelim(']') {
				*out = make(Injections, 0, 8)
			} else {
				*out = Injections{}
			}
		} else {
			*out = (*out)[:0]
		}
		for !in.IsDelim(']') {
			var v10 *InjectionMetadata
			if in.IsNull() {
				in.Skip()
				v10 = nil
			} else {
				if v10 == nil {
					v10 = new(InjectionMetadata)
				}
				(*v10).UnmarshalEasyJSON(in)
			}
			*out = append(*out, v10)
			in.WantComma()
		}
		in.Delim(']')
	}
	if isTopLevel {
		in.Consumed()
	}
}
func easyjsonFac7b200EncodeGithubComSkydiveProjectSkydivePacketinjector1(out *jwriter.Writer, in Injections) {
	if in == nil && (out.Flags&jwriter.NilSliceAsEmpty) == 0 {
		out.RawString("null")
	} else {
		out.RawByte('[')
		for v11, v12 := range in {
			if v11 > 0 {
				out.RawByte(',')
			}
			if v12 == nil {
				out.RawString("null")
			} else {
				(*v12).MarshalEasyJSON(out)
			}
		}
		out.RawByte(']')
	}
}

// MarshalJSON supports json.Marshaler interface
func (v Injections) MarshalJSON() ([]byte, error) {
	w := jwriter.Writer{}
	easyjsonFac7b200EncodeGithubComSkydiveProjectSkydivePacketinjector1(&w, v)
	return w.Buffer.BuildBytes(), w.Error
}

// MarshalEasyJSON supports easyjson.Marshaler interface
func (v Injections) MarshalEasyJSON(w *jwriter.Writer) {
	easyjsonFac7b200EncodeGithubComSkydiveProjectSkydivePacketinjector1(w, v)
}

// UnmarshalJSON supports json.Unmarshaler interface
func (v *Injections) UnmarshalJSON(data []byte) error {
	r := jlexer.Lexer{Data: data}
	easyjsonFac7b200DecodeGithubComSkydiveProjectSkydivePacketinjector1(&r, v)
	return r.Error()
}

// UnmarshalEasyJSON supports easyjson.Unmarshaler interface
func (v *Injections) UnmarshalEasyJSON(l *jlexer.Lexer) {
	easyjsonFac7b200DecodeGithubComSkydiveProjectSkydivePacketinjector1(l, v)
}
func easyjsonFac7b200DecodeGithubComSkydiveProjectSkydivePacketinjector2(in *jlexer.Lexer, out *InjectionMetadata) {
	isTopLevel := in.IsStart()
	if in.IsNull() {
		if isTopLevel {
			in.Consumed()
		}
		in.Skip()
		return
	}
	in.Delim('{')
	for !in.IsDelim('}') {
		key := in.UnsafeString()
		in.WantColon()
		if in.IsNull() {
			in.Skip()
			in.WantComma()
			continue
		}
		switch key {
		case "ID":
			out.ID = string(in.String())
		case "State":
			out.State = string(in.String())
		case "PacketCount":
			out.PacketCount = int64(in.Int64())
		case "UUID":
			out.UUID = string(in.String())
		case "SrcIP":
			if data := in.UnsafeBytes(); in.Ok() {
				in.AddError((out.SrcIP).UnmarshalText(data))
			}
		case "SrcMAC":
			if in.IsNull() {
				in.Skip()
				out.SrcMAC = nil
			} else {
				out.SrcMAC = in.Bytes()
			}
		case "SrcPort":
			out.SrcPort = uint16(in.Uint16())
		case "DstIP":
			if data := in.UnsafeBytes(); in.Ok() {
				in.AddError((out.DstIP).UnmarshalText(data))
			}
		case "DstMAC":
			if in.IsNull() {
				in.Skip()
				out.DstMAC = nil
			} else {
				out.DstMAC = in.Bytes()
			}
		case "DstPort":
			out.DstPort = uint16(in.Uint16())
		case "Type":
			out.Type = string(in.String())
		case "Count":
			out.Count = uint64(in.Uint64())
		case "ICMPID":
			out.ICMPID = uint16(in.Uint16())
		case "Interval":
			out.Interval = uint64(in.Uint64())
		case "Mode":
			out.Mode = string(in.String())
		case "IncrementPayload":
			out.IncrementPayload = int64(in.Int64())
		case "Payload":
			out.Payload = string(in.String())
		case "Pcap":
			if in.IsNull() {
				in.Skip()
				out.Pcap = nil
			} else {
				out.Pcap = in.Bytes()
			}
		case "TTL":
			out.TTL = uint8(in.Uint8())
		default:
			in.SkipRecursive()
		}
		in.WantComma()
	}
	in.Delim('}')
	if isTopLevel {
		in.Consumed()
	}
}
func easyjsonFac7b200EncodeGithubComSkydiveProjectSkydivePacketinjector2(out *jwriter.Writer, in InjectionMetadata) {
	out.RawByte('{')
	first := true
	_ = first
	{
		const prefix string = ",\"ID\":"
		out.RawString(prefix[1:])
		out.String(string(in.ID))
	}
	{
		const prefix string = ",\"State\":"
		out.RawString(prefix)
		out.String(string(in.State))
	}
	{
		const prefix string = ",\"PacketCount\":"
		out.RawString(prefix)
		out.Int64(int64(in.PacketCount))
	}
	{
		const prefix string = ",\"UUID\":"
		out.RawString(prefix)
		out.String(string(in.UUID))
	}
	{
		const prefix string = ",\"SrcIP\":"
		out.RawString(prefix)
		out.RawText((in.SrcIP).MarshalText())
	}
	{
		const prefix string = ",\"SrcMAC\":"
		out.RawString(prefix)
		out.Base64Bytes(in.SrcMAC)
	}
	{
		const prefix string = ",\"SrcPort\":"
		out.RawString(prefix)
		out.Uint16(uint16(in.SrcPort))
	}
	{
		const prefix string = ",\"DstIP\":"
		out.RawString(prefix)
		out.RawText((in.DstIP).MarshalText())
	}
	{
		const prefix string = ",\"DstMAC\":"
		out.RawString(prefix)
		out.Base64Bytes(in.DstMAC)
	}
	{
		const prefix string = ",\"DstPort\":"
		out.RawString(prefix)
		out.Uint16(uint16(in.DstPort))
	}
	{
		const prefix string = ",\"Type\":"
		out.RawString(prefix)
		out.String(string(in.Type))
	}
	{
		const prefix string = ",\"Count\":"
		out.RawString(prefix)
		out.Uint64(uint64(in.Count))
	}
	{
		const prefix string = ",\"ICMPID\":"
		out.RawString(prefix)
		out.Uint16(uint16(in.ICMPID))
	}
	{
		const prefix string = ",\"Interval\":"
		out.RawString(prefix)
		out.Uint64(uint64(in.Interval))
	}
	{
		const prefix string = ",\"Mode\":"
		out.RawString(prefix)
		out.String(string(in.Mode))
	}
	{
		const prefix string = ",\"IncrementPayload\":"
		out.RawString(prefix)
		out.Int64(int64(in.IncrementPayload))
	}
	{
		const prefix string = ",\"Payload\":"
		out.RawString(prefix)
		out.String(string(in.Payload))
	}
	{
		const prefix string = ",\"Pcap\":"
		out.RawString(prefix)
		out.Base64Bytes(in.Pcap)
	}
	{
		const prefix string = ",\"TTL\":"
		out.RawString(prefix)
		out.Uint8(uint8(in.TTL))
	}
	out.RawByte('}')
}

// MarshalJSON supports json.Marshaler interface
func (v InjectionMetadata) MarshalJSON() ([]byte, error) {
	w := jwriter.Writer{}
	easyjsonFac7b200EncodeGithubComSkydiveProjectSkydivePacketinjector2(&w, v)
	return w.Buffer.BuildBytes(), w.Error
}

// MarshalEasyJSON supports easyjson.Marshaler interface
func (v InjectionMetadata) MarshalEasyJSON(w *jwriter.Writer) {
	easyjsonFac7b200EncodeGithubComSkydiveProjectSkydivePacketinjector2(w, v)
}

// UnmarshalJSON supports json.Unmarshaler interface
func (v *InjectionMetadata) UnmarshalJSON(data []byte) error {
	r := jlexer.Lexer{Data: data}
	easyjsonFac7b200DecodeGithubComSkydiveProjectSkydivePacketinjector2(&r, v)
	return r.Error()
}

// UnmarshalEasyJSON supports easyjson.Unmarshaler interface
func (v *InjectionMetadata) UnmarshalEasyJSON(l *jlexer.Lexer) {
	easyjsonFac7b200DecodeGithubComSkydiveProjectSkydivePacketinjector2(l, v)
}

redpajama_set_name: RedPajamaGithub


Arsenal legend Martin Keown blasted Unai Emery after the Gunners' 1-0 defeat to BATE Borisov, describing the loss as the 'worst performance we've seen' under the Spaniard.
Stanislav Dragun's goal shortly before half-time gave the Belarus giants the advantage going into the last-32 second leg at the Emirates next week.
To compound a miserable night for Arsenal, Alexandre Lacazette was sent off for violent conduct after catching a BATE defender with his elbow.
The Gunners looked lackluster thorughout the defeat and Keown, who was covering the game for BT Sport, says it's worst display he's seen under Emery.
'It's as poor as I can remember, certainly under Emery it's the worst performance we've seen,' said Keown.
'BATE you have to give them credit, it's a remarkable result for them but Arsenal just didn't have the penetration.
'There was a sloppiness within their play. You can blame the pitch which is a poor excuse but you've got to be better than this as an Arsenal side.
'In the second half you'd expect a response from Emery and his team, on 70 minutes he made the changes but there was just so many stray passes. It was remarkable.
Arsenal's defeat to Manchester United in the FA Cup fourth round means they have a free weekend coming up, giving them more time to prepare for next Thursday's game at the Emirates.
Pierre-Emerick Aubameyang emerged from the bench in Belarus but he's now certain to start the second leg with Lacazette ruled out through suspension.