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Home / Celebrity Cruises Edge Series Ships
Celebrity Edge Series
Celebrity Edge was just the beginning, now Celebrity are taking revolutionary to new heights.
Introducing Celebrity Edge Series
Celebrity Edge was designed to create a closer connection between you, the sea, and the world beyond – blurring the lines between inside and out. The result was so extraordinary, Celebrity Edge was recognised as one of the world's greatest places by Time magazine.
That same industry-changing experience can be found on all of Celebrity's Edge Series ships – the second Edge Series ship, Celebrity Apex, and the newest, Celebrity Beyond. Every element on these ships has been taken to the edge of possibilities. Higher ceilings. Airier venues. Flowing architecture so every deck, every experience, is seamlessly connected. From the mind-blowing Eden to the sea's only Magic Carpet, each Edge Series ship leaves traditional thinking in its wake.
Discover Dining that Opens Your World
Celebrity Edge Series delivers a diverse and authentic culinary journey on board with focus to the destinations you visit. Here, Celebrity find creative inspiration and the local ingredients for the visionary recipes our Michelin-starred chef, Cornelius Gallagher, creates.
Sewing Up All Your Favourites
There's so much to say about the new experiences aboard the Edge Series ships, but they haven't forgotten some of the tried-and-true popular favorites, including Café al Bacio, the Pool Bar, the Martini Bar, and the ever-popular Sunset Bar. They're all there, waiting to serve up hand-crafted cocktails and ice-cold craft brews or healthy snacks and juices you need to replenish after a day at the spa or pool. Awaken your senses at Eden Bar with immersive experiences, ever-changing activities, and creative artisanal cocktails. Or kick back at Craft Social Bar, the new spot aboard Celebrity Apex offering a fun, casual atmosphere and a vast selection of craft beers, wines, and cocktails poured by our Cicerone certified servers.
Let Celebrity Entertain You
Celebrity have designed every public space with entertainment in mind, from The Theatre and its 110-foot wide screen to the enchanting Rooftop Garden. The lineup of unforgettable shows, live music, exciting casinos, and nightlife make this a holiday worth a standing ovation.
Discover Three Revolutionary Feats
View Celebrity Edge
View Celebrity Apex
View Celebrity Beyond
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Q: GUID vs int : Does it makes any difference for SEO? Today I heard from my colleague that search bot can index pages with sequential ids.
Is it really happens ?
As an example checkout two urls:
http://sample.com/myProduct?id=765
and
http://sample.com/myProduct?id=35d6eb6c-97f6-4cde-997c-ade657c285d3
So, if search bots can figure out that my product id in url is sequential it can possibly index other products up and down the sequence ...
Have you ever heard anything like that ?

A: Whomever told you that is mistaken. Search engines will only index pages they know exist. So they won't keep changing the ID in those URLs just see if they find anything. So if you want those other pages to be indexed you should use a HTML sitemap or XML sitemap to tell the search engines where those pages are. Linking to them from other product pages is also a good idea.

redpajama_set_name: RedPajamaStackExchange


Le Bourget. 22 June 2017. Leonardo has signed a contract with the UK Ministry of Defence (MOD) worth in excess of 290 million Euros. The contract will see Leonardo and HENSOLDT, working together as 'Team Skytale', upgrade the IFF (Identification Friend or Foe) technology on more than 350 of the UK's operational aircraft, naval vessels and ground-based air defence systems to the latest 'Mode-5' standard. IFF technology is central to all military operations as it acts as a modernday 'challenge and response' password system based on automated electronic signals.
This ensures that forces can recognise friends, which when contacted will reply with the correct signal, and identify potentially hostile vehicles which will not. All NATO nations are mandated to switch to the new Mode-5 standard IFF by 2020, which uses advanced cryptographic techniques to secure the systems against electronic deception by adversaries. This is important when forces are operating together because ensuring that ground, air and naval crews can reliably recognise their allies is one of the main ways of avoiding so-called 'friendly fire' incidents.
Under the contract, Leonardo and HENSOLDT will upgrade legacy UK aircraft, naval vessels and ground-based air-defence systems with an out-of-service date after 2020, which covers 11 aircraft types (managed by Leonardo), 18 naval vessel types and 2 land-based platform types (managed by HENSOLDT). The team will also establish a Mode-5 IFF support hub in the UK. In addition to NATO forces, other nations which want to conduct operations alongside NATO countries will also need to upgrade to the Mode-5 IFF standard.
Mode 5 IFF technology offered by the Leonardo/HENSOLDT team is readily exportable. Together, Leonardo and HENSOLDT are Europe's leading provider of Mode-5 IFF solutions. Leonardo has previously delivered Mode 5 IFF for the UK Royal Air Force's Eurofighter Typhoons the Royal Navy's Queen Elizabeth-class aircraft carriers. Leonardo also provides Mode 5 IFF technology for the new Saab Gripen-E fighter and has recently demonstrated innovative reverse IFF (air-to-ground) capabilities on Italian Typhoon aircraft.
The company is also currently studying this new capability for the future Eurofighter as part of a UK MoD technology demonstrator programme. HENSOLDT is under contract to upgrade German, French, US and other armed forces' platforms with Mode 5 IFF systems. Among others, the company's IFF equipment is deployed on all German Navy ships as well as several UK Royal Navy ships. HENSOLDT has also established the air traffic control/IFF network of the German Air Force.


[Usenet] "As a Usenet discussion grows longer, the probability of a comparison involving Nazis or Hitler approaches one." There is a tradition in many groups that, once this occurs, that thread is over, and whoever mentioned the Nazis has automatically lost whatever argument was in progress. Godwin's Law thus practically guarantees the existence of an upper bound on thread length in those groups. However there is also a widely- recognized codicil that any intentional triggering of Godwin's Law in order to invoke its thread-ending effects will be unsuccessful. Godwin himself has discussed the subject. See also Formosa's Law.


Comedian Dane Cook mocked the Aurora, Colorado theater shooting in his standup act this week that was caught on video obtained by TheDailyCaller.com.
"I know that if none of that would have happened, pretty sure that somebody in that theater, about 25 minutes in, realizing it was a piece of crap, was probably like 'ugh f------ shoot me,'" Cook remarked.
The crowd's response was a mix of groans, laughter and cheers.
Last week, Warner Bros. studios, which produced "The Dark Knight Rises" contributed money to the relief fund for the victims of the mass shooting of a midnight showing of the film, where 12 people were killed and dozens wounded.
The suspect, 24-year-old James Holmes is being held in solitary confinement, where he has been since his arrest on July 20. He made his first court appearance Monday.


The Piano and Voice album requested, in the main, by European audiences who wanted to have a memento of the more intimate concerts there, when Louis left his big band line-ups at home in Oz.
Louis covers his favorites from the catalog with exquisite production. Released in 2006.


text:
Q: In database emp table is there i want to create temporary table for the emp table with out using create command In database emp table is there i want to create temporary table  for the emp table with out using create command

A: In sql sever, you can do like this:
select t1.*
into tempTable
from Table1 t1 join Table2 t2
on t1.ParentId= t2.ParentId;

A: Based on the sql server answers, maybe what you're looking for is CTAS:
create table MY_TABLE as select * from emp;


As Co-Founder and Producer of C2C Media, Deanna leans on her corporate, management consulting and nonprofit expertise to advance social change through empathetic storytelling. She has produced content for Applebee's, SONIC Drive-In, Women's Refugee Commission, Austin Recovery, the NRDC and an assortment of other nonprofit, corporate social responsibility (CSR) and advocacy-related clients.
Deanna previously served as Chief Services Officer of Mission Capital, managing a team of consultants in nonprofit strategic advisory services. Prior to that, as Senior Director at MAXIMUS, Deanna managed complex multi-stakeholder engagements, including the implementation of new government programs and change management through transitions involving multiple private and public stakeholders.
Deanna is an active member and volunteer for Impact Austin, Partners in Parenting, and several other nonprofit organizations. Deanna is a member of the American Association of Political Consultants, Austin Film Society, and Austin Ad Fed. Deanna is also a certified Project Management Professional (PMP). Deanna has Master of Social Work and Master of Public Administration degrees from the University of Southern California and undergraduate degrees in Social Work and Health Sciences from Michigan State University.
Tyson is a Director and the Co-Founder of C2C Media. For the past twenty years, he's produced commercials and branded content for several national and international brands, including Whole Foods Market, SONIC Drive-In, Brooks Brothers, Alcon Eyecare and many more. A multi-tool filmmaker, Tyson honed his craft with the SPIKE and Comedy Central crews, creating network-branded trailers and commercials for multiple blockbuster properties, including: Lone Survivor, Star Trek: Into Darkness, Wolverine, Bad Grandpa, and many more.
Tyson has produced and edited content that has appeared across a host of broadcast networks and digital platforms, including; Netflix, Showtime, MTV, VH1, SPIKE, Comedy Central, and many more. He has been awarded 18 Pollie and Telly Awards, honoring the best political and advertising spots in film and television. He recently produced and directed the feature film, Juice: How Electricity Explains The World, due out in late 2019. To learn more about the film, please visit www.juicethemovie.com.
James is an accomplished editor with a background in independent film production. After producing over a dozen short films in college, he co-produced, co-wrote, crowdfunded, directed, edited and scored his first feature film, Ezekiel's Landing, at the age of 23. Originally from Indiana, he made his way southward in search of fame, fortune and a regular paying job in the film industry (not necessarily in that order). Following editorial stints with Ralph Smyth Entertainment, Grandex, and Rooster Teeth Productions, James began working regularly with C2C Media.
Over the last three years, James has cut all manner of content for C2C - recipe spots, corporate explainers, and more than two hundred political and nonprofit commercials. In 2018, Treakle edited and co-produced director Tyson Culver's globetrotting documentary, Juice: How Electricity Explains The World.


Eyes peeled for ways to fill budget holes without cutting services or raising taxes, some Miami-Dade commissioners are looking to the county's 12 community redevelopment agencies.
Property tax valuations are capped within agency bounds. The county and area municipality forfeit revenue generated above the cap to revitalize the area.
Commissioners have asked the administration to study the impact of returning surplus funds to county — and potentially municipal — coffers during the next two fiscal years.
"Some CRAs are just gathering money, and what this would do is any money that's not used for debt service or to pay a contractual obligation would return back to the county," sponsor Carlos Gimenez said. Cities may do the same "in order to get operational money back without having to raise taxes."
Beyond the potential hiatus, Commissioner Joe Martinez said it's vital for the future to examine all redevelopment agencies to ensure they're productive.
Idle agencies' "existence should cease, and that funding should be redistributed to the general fund," he said.
Assistant Miami Beach Manager Hilda Fernandez said redevelopment agencies boost areas, and the city's has several projects going.
Though Mr. Gimenez's concept allows existing obligations to remain funded, it would hit those agencies that pay for projects as they go, she said.
It would "almost penalize them by taking their funds because they didn't indebt themselves to the hilt."
Jim Villacorta, executive director of Miami's three agencies, said the idea raises legal questions.
Agreements between the county, city and agencies would have to be amended, and bondholders could take issue with the agencies receiving less funding, he said.
The county study would examine such issues. Results are due in 30 days.


text:
package svc.controllers;

import org.junit.Test;
import org.junit.runner.RunWith;
import org.mockito.InjectMocks;
import org.mockito.Mock;
import org.mockito.runners.MockitoJUnitRunner;

import svc.managers.CitationManager;

@RunWith(MockitoJUnitRunner.class)
public class CitationControllerTest {

	@InjectMocks
	CitationController controller;

	@Mock
	CitationManager managerMock;

	@Test
	public void placeholderTest() {
		return;
	}
}

redpajama_set_name: RedPajamaGithub


Havana was one of the most amazing experience and I truly fell in love with Cuba and it's people. I was joined by my friend Melissa and we explored Havana daily with our lovely Cuban friends. They showed us local spots and took amazing care of us.
I will definitely be heading back next year and for longer!
£20 IN BRIGHTON | £20 CHALLENGE - Duration: 3 minutes, 4 seconds.
BRITISH AIRWAYS i360 | THE ULTIMATE BRIGHTON EXPERIENCE - Duration: 2 minutes, 41 seconds.
3 INSTAGRAM SPOTS IN BRIGHTON | ROAD TRIPS WITH RONI - Duration: 3 minutes, 2 seconds.
LONDON FOOD GUIDE | EPISODE 2 - PERGOLA AT PADDINGTON - Duration: 60 seconds.
LONDON FOOD GUIDE | EPISODE 1 - NANDO'S - Duration: 4 minutes, 15 seconds.
THE DOG WHISPERER | PRINCESS PEACH THE POMERANIAN | @ashleemoyo - Duration: 2 minutes, 48 seconds.
5 THINGS I DISCOVERED PARIS | @ashleemoyo - Duration: 3 minutes, 50 seconds.
THE SIDE OF ROME YOU DON'T SEE | SUNDAY STORYTIME - Duration: 20 minutes.
LEFT ME ON MY BIRTHDAY | SUNDAY STORYTIME - Duration: 12 minutes.
FLATMATE FROM HELL - MY 2ND YEAR EXPERIENCE | SUNDAY STORYTIME - Duration: 13 minutes.
TRICKED INTO HIS CAR!! | SUNDAY STORYTIME - Duration: 5 minutes, 28 seconds.
ALMOST DIDN'T GO TO UNI - MY LIFE WAS OVER | SUNDAY STORYTIME - Duration: 18 minutes.
#BRUNCHINGBLOGGERS - GREAT FOOD, GREAT COMPANY | BLOGGERSAREUS - Duration: 86 seconds.
On Saturday 21st October, the first in a series of brunches by myself (bloggersareus) and Food and Baker took place.
TROUBLE IN BULGARIA | SUNDAY STORYTIME - Duration: 12 minutes.


Swing away this summer with Plastic Golf Toy Set! This cute miniature golf set features everything you need to let your little one have a hand at beginning golf.
Featuring plastic parts in blue, orange, and yellow that fit away nicely in the container, this toy golf set can conveniently travel along with your young golfer indoors or outdoors. Set up the plastic holes and flags and shoot for a hole in one!


Argentina is rapidly running out of options in its efforts to overturn court decisions requiring it to meet its contractual obligation to treat its bondholders equally.
In June 2013, Argentina filed a certiorari petition with the U.S. Supreme Court, seeking review of an October 2012 Second Circuit Court of Appeals ruling that Argentina breached the pari passu provision in its debt contract with bondholders. The Supreme Court will rule on whether to take the matter in just a few weeks.
It is worth noting that the October 2012 ruling was only a preliminary decision. The final ruling against Argentina was filed by the Second Circuit on August 23, 2013 (see an earlier Legal Pulse blog post on it here). The August 2013 ruling, like the ruling of October 2012, decisively rejected all of the Argentine government's arguments that a district court overstepped its bounds in ordering the government to comply with its obligations to rank its payments to "hold-outs" equally to other bondholders. Argentina will almost certainly file a second certiorari petition in late 2013 or early 2014 on the final ruling.
Counting to Four. In order to get a full hearing before the High Court on either of its two petitions, Argentina will need to attract the votes of at least four of the nine justices. The likelihood that Argentina could attract the necessary four votes would become just that much slimmer if, as appears possible, one or more of the nine justices decides to recuse her or himself from the case.
Federal law leaves it up to each justice to decide for her or himself whether recusal is appropriate in any particular case. One justice, Justice Sonia Sotomayor, appears to have established a policy of recusing herself from any case in which she had any involvement before joining the Supreme Court. (I say "appears" because justices virtually never explain why they have recused themselves from a case.) Before being elevated to the Supreme Court in 2009, Sotomayor sat on the Second Circuit; during her tenure there, the court heard dozens of cases arising from Argentina's various debt defaults. On at least four occasions as a Supreme Court justice, Justice Sotomayor disqualified herself from Argentine debt cases in which she had had some involvement while sitting on the Second Circuit.
One of those four cases was Aurelius Capital Partners, LP v. Republic of Argentina, No. 09-723, a case that came to the Supreme Court from the Second Circuit and on which then-Judge Sotomayor had sat as a member of the three-judge panel hearing the case. On two occasions since then, Justice Sotomayor recused herself from Argentinian debt cases that came to the Court from the Second Circuit even though she had not been part of the three-judge panel. Her apparent reason for doing so was that the "lead" district court case in each of those two certiorari petitions had been one of the district court cases involved in Aurelius Capital.
If that was Justice Sotomayor's rationale for recusal, then she is likely to recuse herself from Argentina's latest petitions for review as well. The "lead" district court case in those petitions, District Court No. 08-6978, was also at issue in the Aurelius Capital case. Indeed, many of the bondholders who were parties to Aurelius Capital are the same "hold-out" bondholders whose Second Circuit victory Argentina is now trying to overturn. On the other hand, there have been a number of sovereign debt cases involving Argentina where she has not recused herself. For example, earlier this year Justice Sotomayor did not recuse herself from Case No. 12-842, a certiorari petition in which Argentina is seeking High Court review of yet another Second Circuit decision involving efforts by "hold-out" bondholders to enforce their rights.
Justice Sotomayor and President Kirchner. Separately, Justice Sotomayor may also decide to recuse herself because over the years she has met on a number of occasions with Argentina's president, Cristina Fernández de Kirchner, and other high-ranking Argentine officials. Indeed, the Argentine government seems to have made a concerted effort to forge close relations with the Justice. It would be ironic if those efforts resulted in a decision by Justice Sotomayor to disqualify herself from hearing Argentina's certiorari petitions.
Justice Sotomayor made an official visit to Argentina on August 27-29, 2012. According to U.S. State Department press releases, while in the country she met one-on-one with President Kirchner. The two also had a meeting when Kirchner was in Washington, D.C. in April 2010. Kirchner has taken an extremely active role in the Second Circuit litigation and has repeatedly and publicly denounced the "hold-outs" who are suing Argentina for payment on their bonds. This may provide Justice Sotomayor with an additional reason to disqualify herself from considering Argentina's certiorari petitions.
In sum, Argentina faces a daunting task in convincing four Supreme Court justices to vote to grant its certiorari petitions. The task is made even more difficult by the possibility that Justice Sotomayor may recuse herself, thereby reducing the pool of justices from which it needs to find four votes.


Optimus Nova+ Stove Canadian Outdoor Equipment Co.
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Serve up some serious eats from anywhere on the globe when you use a Optimus Polaris Optifuel Stove. These Canister Stoves made by Optimus accept multiple fuel sources including white gas, LP gas, gasoline, kerosene, diesel, and jet fuel. how to clean front loading washing machine uk The Optimus 8R is a camping stove that was manufactured in Sweden by outdoor products manufacturer Optimus International AB. It can be used with unleaded liquid camping fuel and it was also intended for use with a proprietary paste fuel that Optima no longer manufactures.
2/04/2010 · Cool little classic camping paraffin stove from the 50`s/60`s i think`s, this one`s complete with all the bit`s and bob`s.
All stoves can be problematic, they all need cleaning and care, although sometimes it is not clear whether they need maintenance. I usually carry spare parts for the stove too, it is such a hassle to find them in a city, in shops for car parts (as many countries have not such fancy little stoves).
Optimus Crux Stove This little gem seemed to be the happening thing in some of the forums when I purchased this little stove. The stove weighs as little as 3.1 oz and folds away so that you can store in the smallest places.
Reviews > Cook Gear > Stoves > Optimus Nova White Gas Stove > Test Report by S. Nelson Product tested and reviewed in each Formal Test Report has been provided free of charge by the manufacturer to BackpackGearTest.org.


text:
Promoting Predators
by Philip Lawler 7 . 24 . 18
What did the American bishops know, and when did they know it? This is the question everyone is asking in the wake of public revelations that Cardinal Theodore McCarrick had, for years, preyed on seminarians who visited his beach house. It is a reasonable question, a necessary question. I hope that someday soon, a few brave bishops will begin asking it, too—and giving the restive Catholic faithful some answers.
But it is not the most important question. For anyone exploring the corruption of the Catholic hierarchy, the question of how Cardinal McCarrick avoided exposure and prosecution, though important, is less critical than the question of how his rise through the ecclesiastical ranks continued, even while rumors about homosexual activities swirled around him. Why was McCarrick named archbishop of Washington, and given a cardinal's red hat? Why was he allowed to promote his proteges, to serve special diplomatic assignments for the Vatican, to influence the selection of bishops and even of a Roman Pontiff, after his beach-house antics had become a matter of common knowledge?
The more obvious question, the what-did-they-know-and-when question, admits of an easy, albeit unsatisfactory answer. McCarrick's colleagues can say, more or less honestly, that they had heard reports about his approaches to seminarians, but did not know whether the reports were true. The question allows for an epistemological dodge: Other bishops did not really know, in the sense that they had no definitive proof. So they had an excuse for their failure to take action—or so they thought.
Reporters, likewise, had heard the stories about McCarrick but had no proof. Rod Dreher and Julia Duin have written about their fruitless searches for a witness who would go on the record. Without personal testimony, they had only hearsay evidence. I experienced the same frustration.
Nevertheless, I knew, as did many reporters covering Catholic affairs. By the year 2000, when McCarrick was named archbishop of Washington, many American bishops had received personal letters from some of the young men McCarrick had approached. A delegation of influential Catholics had traveled to Rome to warn Vatican officials about the scandal. Though no one had legal proof, everyone interested in the question had, at the very least, serious suspicions. Why would the Catholic hierarchy promote someone who was even suspected of homosexual predation?
A personal anecdote: In 2003, a colleague asked me to join in an initiative, promoting a good cause. I was favorably inclined, until my colleague told me that Cardinal McCarrick would be a sponsor. At that point, I said that I wanted nothing to do with the project. (There was no need to explain to my colleague why I did not wish to be associated with the cardinal. He knew. Everybody knew.)
Why were so many others, including American bishops and Vatican officials, willing and eager to ally with McCarrick, despite the fact that "everybody knew"? Who was promoting his interests? And whose interests was he promoting?
After such a devastating scandal, any normal organization would do some forensic work, looking carefully at the records to see who had recommended McCarrick for higher office—and who had gained their status on his recommendation.
Newark's Cardinal Joseph Tobin (who, by the way, is regarded as one of McCarrick's proteges) has said that the past month's revelations point to a need for better policies and procedures within the Church. But the policies for dealing with a homosexual predator have always been in place. The problem has been the unwillingness of Church leaders to invoke the policies, to use the proper procedures. Or, to put it a bit differently: As the political experts remind us, personnel is policy.
The failure of Church leaders to take action against McCarrick when they first heard of his offenses, perhaps twenty years ago, is evidence of the need for reform within the hierarchy. The fact that many prelates took action for McCarrick—making him their spokesman, enlisting his help, following his lead—speaks to the urgency of the crisis.
Nor is this an exclusively American problem. Pope Francis has given prominent posts to cardinals who are tainted by scandal, and allowed them to remain in those posts despite mounting evidence against them.
Take, for example, the Council of Cardinals—the nine cardinals who serve as the pontiff's board of advisers on questions of Church reform. The coordinator of the group is Honduran Cardinal Oscar Maradiaga, whose favored deputy, Bishop Juan Jose Pineda Fasquelle, resigned last week amid charges of both sexual abuse (with seminarians, again) and financial misconduct. Cardinal Maradiaga has likewise been accused of financial misconduct, having accepted tens of thousands of dollars from the Honduran government and deposited the funds in European banks. Perhaps he is innocent, but at best he is liable to questions. Since he has already reached the canonical retirement age of 75, it would be a simple matter to replace him as effective chairman of the pope's advisory panel. To keep him in a high-profile post—a post dedicated to reform, no less—would send an unfortunate signal, countering the pope's professed determination to root out corruption.
The Council of Cardinals also includes Cardinal Francisco Errazuriz, the retired archbishop of Santiago, Chile. Back in May, when the active Chilean bishops resigned en masse because of the burgeoning sex-abuse scandal in that country, Cardinal Errazuriz was immune; he had retired eight years earlier. But he, too, has been a target for criticism, since he reportedly sought to persuade Vatican officials not to listen to complaints about a notorious Chilean priest. By September, when the Council of Cardinals meets again, Cardinal Errazuriz will be 85 years old, and again it would seem natural to replace him. To keep him on board would be another unsettling signal.
To regain the credibility they have lost in recent decades, Catholic bishops in America and in Rome must do more than apologize for the transgressions of others. They must acknowledge their own offenses—their willingness to tolerate abusive clerics, to protect them, to promote them.
In 2002, when the American bishops met in Dallas to discuss the burgeoning sex-abuse scandal, I was among the hundreds of reporters on hand. As we milled about the press room, I was struck by the convergence of journalists' opinions. Colleagues from one end of the ideological spectrum to the other joined around the coffee machine, shaking their heads and saying of the assembled bishops, "They don't get it." A similar convergence has occurred since the McCarrick scandal erupted. The remedy for negligent bishops is diligent bishops. The answer to corrupt bishops will come from bishops dedicated to reform.
In the first Scripture reading at Mass this past Sunday, Catholics heard the striking words of Jeremiah: "Woe to the shepherds who destroy the sheep of my pasture." But the prophecy, dire in its condemnation of the abusive shepherds, provides some help for the long-suffering Catholic flock: "I will set shepherds over them who will care for them, and they shall fear no more, nor be dismayed, neither shall any be missing, says the Lord."
Surely there are at least a few shepherds out there, mindful of their people's dismay, ready to speak out at last? Oremus.
Philip Lawler is editor of Catholic World News and author of Lost Shepherd: How Pope Francis is Misleading his Flock.
More on: Religion, Public Life, Sexual abuse, Child abuse, sexual abuse crisis, Catholicism
Articles by Philip Lawler

redpajama_set_name: RedPajamaCommonCrawl


text:
Gabriela Wolf (born 28 October 1960) is a German long-distance runner. She competed in the women's marathon at the 1988 Summer Olympics representing West Germany.

References

1960 births
Living people
Athletes (track and field) at the 1988 Summer Olympics
German female long-distance runners
German female marathon runners
Olympic athletes of West Germany
Place of birth missing (living people)
20th-century German women
21st-century German women

redpajama_set_name: RedPajamaWikipedia


text:
Made In Hollywood Teen
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Captain America Civil War: New Clips Spotlight Spider-Man's Sense of Humor
Spider-Man Shows Off His Humorous Side in New Captain America Civil War Clips Robert Downey Jr.'s feud with Chris Evans in "Captain America: Civil War"…
'Spotlight,' 'Beasts of No Nation' Win Big at Diverse 2016 Spirit Awards
"Spotlight" won best picture and four others honors and the stars of "Beasts of No Nation" took acting prizes at the 2016 Spirit Awards that…
What'll Be Best Picture? Our Prediction
Best Picture Oscar: What Will Win? Made in Hollywood Picks It has been hailed as one of the best films that cover investigative journalism. As…
'Spotlight,' 'Leonardo DiCaprio,' 'Brie Larson' Win SAG Awards
"Spotlight" boosted its Oscar chances by winning the ensemble trophy at the SAG Awards on Saturday, while Leonardo DiCaprio picked up another honor for "The Revenant"…
'Spotlight' Wins Best Picture at Critics' Choice Awards
Given their choice, the critics picked a little bit everything. Winners were all over the map Saturday at the Critics' Choice Awards with "Spotlight" getting best picture and…
'Spotlight' Leads as Best Picture Favorite Among Critics Awards
Proving to be an early favorite leading up to the Oscars, "Spotlight" has dominated critics-group awards for films released in 2015. The journalism drama has…
Bryan Cranston Wins Palm Springs Film Fest Spotlight Award
The awards continue to roll in for Bryan Cranston, whose latest honor for his part in "Trumbo" is the Palm Springs International Film Festival's Spotlight…
'Compton' Scores Surprise SAG Nom - Full List
"Spotlight" solidified its position as an Oscar best picture favorite with a top nomination Wednesday for the SAG Awards while "Straight Outta Compton" nabbed a surprise nod…
'Spotlight' Named Best Picture of the Year By Los Angeles Film Critics Association
Proving to be an early favorite leading up to the Oscars, the honors continue to roll in for "Spotlight," which was named Best Picture of…
'Spotlight' Emerges as Big Winner at Gotham Film Awards
"Spotlight" swept the Gotham Independent Film Awards Monday with top honors for Best Feature, Special Jury Award – Ensemble Performance and Best Screenplay. Accepting the…
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Our girls looking good at Bowie State!
Updated Wednesday April 3, 2019 by Christy Centrella.
Jr SHOCK had a great Saturday at Cheer Starz with a 1st Place and Club Zero outine!! Keep pushing ladies, you have come so far! Very proud of our girls!


Dr. Dwight G. Smith, M.D.
At New England Psychiatric Consultants we offer comprehensive adult psychiatric services for the Boston, South Shore, and Cape Cod area. We specialize in the latest of technological advances in psychiatric medicines and cutting edge therapies. Often, these therapies will provide hope and healing through life's most difficult circumstances. New England Psychiatric Consultants offers medication management, counseling, and the latest medical treatments available for a variety of mental health concerns, all in a private, outpatient setting.
We make it a top priority to alleviate symptoms and to help you develop the necessary tools to deal with life's inevitable challenges. A prime objective is to help improve and restore quality of life for our clients by providing traditional psychological therapy services for situations arising from chronic stress and relational issues as well as medication management for all mental health concerns.


text:
38 - "Raise Your Voice" with Kathy Khang
You have a voice. And you have God's permission to use it. But how do we do so in a wise way? How do we find our purpose and the message that we are called to preach and then once we do, how do we speak and engage in a way to meet others in a place of understanding.
Guest Bio:
Kathy Khang is a speaker, journalist, and activist. She has worked in campus ministry for more than twenty years, with expertise in issues of gender, ethnicity, justice, and leadership development. She is a columnist for Sojourners magazine, a writer for Faith & Leadership, and a coauthor of More Than Serving Tea: Asian American Women on Expectations, Relationships, Leadership and Faith.
Buy Raise Your Voice
Special Music for this episode was provided by Rivers and Robots
Tracks Include: Home, To The Highest Place, and Dreams
You can also find selections from all our episodes on our Spotify Playlist.
I am so grateful for you and want to invite you to become a part of the beloved community being developed here. Consider becoming a Patreon supporter of the show. You'll have access to many perks as well as guaranteeing the future of these conversations; even $1/Month goes so far as this show is 100% listener supported.
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Newer Post39 - Learning to Speak God from Scratch with Jonathan Merritt
Older Post37 - "The Eternal Current" with Aaron Niequist


text:
Scientific Article of the Month
Continuing support for self-management after the end of the project
COMPAR-EU has provided key resources for supporting self-management: a taxonomy of interventions, core outcome sets for the four chronic conditions built together with patients and providers; reviews and analyses of more than 1600 randomized control trials allowing comparison of the different self-management components effectiveness; cost effectiveness analyses and studies on the influence of context in developing self-management interventions (SMIs).
13. December 2022 | by Rosa Suñol | Fundación Avedis Donabedian
This information is highly valuable for patients, professionals, guideline developers, researchers, and policymakers as well as for industries developing IT support systems, pharma and insurance companies. All this information has been reported in an interactive platform which includes decision aids for patients and providers, evidence to decision frameworks, summary of findings tables and recommendations per disease. Lay person summaries are included in the platform.
We are aware that our results can make an important contribution in bridging the gap between knowledge and practice, summarising what is currently available and developing further knowledge and support to the field.
Our mission: help stakeholder's decision-making
To continue the COMPARE-EU efforts after the project termination in December, we launched Self-Management Europe. This is the not-for-profit European Research and Innovation Centre conceived of as a partnership of organisations working on patient empowerment and self-management. The project is a joint venture initiative led by the Netherlands Institute for Health Services Research (Nivel), OptiMedis, the Avedis Donabedian Research Institute (FAD and the European Patients' Forum (EPF). It works in collaboration as an affiliate member of the other COMPAR-EU partners.
Its mission is to help stakeholder's decision-making by providing, creating, and disseminating new and innovative knowledge for better self-management and patient empowerment with a special emphasis on chronic conditions. Its main objectives are:
Providing updated (scientific) knowledge on patient empowerment and self-management.
Promoting research and generating new knowledge on how to improve self-management with special emphasis on vulnerable people and chronic conditions.
We aim to build capacity for research, policy and interventions through workshops, webinars, seminars, and knowledge exchange and help to set strategic directions in European research and policy on self-management, empowerment and chronic disease and create opportunities for innovation and transfer of self-management research for the mHealth application.
Self-Management Europe Alerts
Our first initiative has been to produce Self-Management Europe Alerts providing practical recommendations on how to implement practices that enhance self-management and patient empowerment. So far, four have been published and are being translated to different EU languages to enhance their impact. We intend to create a network with other interested organisations to continue enhancing self-management and patient empowerment knowledge and implementation.
If you are interested, please contact us at contact@self-management.eu
Rosa Suñol
Rosa Suñol is President of the Board of Trustees at FAD. She holds the Donabedian Research Chair in Quality at the Faculty of Medicine and is also Deputy Editor at the International Journal for Quality in Health Care since 1991. Rosa Sunol has published more than 80 articles and books and has over 25 years of experience in health and social care research.


Almost every New Yorker owns a black and/or beige trench, so adding a cropped version in another shade of pretty is such a great way to update your fall wardy. I adore this Brooks Brothers short navy trench because you can wear it as an everyday blazer, so versatile! Since the color & style is classic, you can glam it up with a printed scarf & baubles for a stylish weekend in NYC.
Crafted by master mixologist, Nick O'Connor from Apotheke bar in NYC, the 'Starr Fair Trade Punch' features an invigorating mix of Starr African Rum, fresh blueberries, agave nectar, ginger and is the perfect libation to enjoy while rocking out to Neil Young, the Foo Fighters, the Black Keys and Band of Horses – all who are scheduled to perform for more than 60,000 festival attendees next weekend. visit www.globalfestival.com for more info.


Four different sketches of man's best friend.
These Cavalier King Charles Spaniel sketches are machine embroidered in varying shades of grey.
This Cavalier King Charles Spaniel design measure approximately 5" (w) x 5" (h) and can be embroidered on the dish towel of your choosing.. Each order is wrapped in a white tissue paper wrapper before being put in a mailing envelope.


1 in 5 people living with diabetes suffer from diabetic nerve pain.
Learn more about shooting, burning, pins and needles pain in your feet or hands.
85% of people with diabetic nerve pain say that it affects them daily, according to an online survey. A Pfizer-sponsored survey polled 1,004 people living with diabetes experiencing DPN symptoms and 500 healthcare providers. Healthcare providers surveyed were not necessarily providing care to people who participated in this survey.
See how managing your diabetic nerve pain can help make a difference.
The majority of Black and Hispanic sufferers surveyed, who were diagnosed with diabetic nerve pain, wished they had spoken up sooner. Community Health Perspectives was developed and sponsored by Pfizer Inc in collaboration with the American Diabetes Association. The main sample surveyed included 1,000 adults ("general respondents") in the United States 18+ who had been diagnosed with diabetes and experienced symptoms of diabetic nerve pain in their feet and/or hands. General respondents comprised: Non-Hispanic Whites (n=823), African Americans (n=73), Hispanic Americans (n=70) and Other (n=34). Additional African American (n=452) and Hispanic American (n=467) adults were then surveyed for further analysis, reaching a total survey sample size of 1,919 respondents. A sample of 308 health care providers were also surveyed.
See why it is very important to tell your doctor about the shooting, burning, pins and needles pain in your feet or hands.
If you're living with diabetes and have shooting, burning pain in your feet or hands, learn about some steps you may want to take.
If you have any symptoms of diabetic nerve pain, make talking to your doctor a priority.


Balancing stakeholder needs in full in audio MP3 format taken from edition 15 of Business Case Studi..
Building community partnerships in full in PDF format taken from edition 4 of Business Case Studie..
Corporate responsibility and stakeholders in full in audio MP3 format taken from edition 17 of Busin..
Corporate responsibility and stakeholders in full in PDF format taken from edition 17 of Business Ca..
Corporate responsibility and stakeholders in full in PDF format taken from edition 20 of Business Ca..
Engaging stakeholders in a business in full in PDF format taken from edition 10 of Business Case S..
Engaging with stakeholders in full in audio MP3 format taken from edition 16 of Business Case Studie..
Engaging with stakeholders in full in PDF format taken from edition 16 of Business Case Studies.This..
Ethically serving stakeholders in full in audio MP3 format taken from edition 14 of Business Case ..
Ethically serving stakeholders in full in PDF format taken from edition 14 of Business Case Studi..
Growing the value of a business for shareholders in full in PDF format taken from edition 5 of Bus..
Meeting responsibilities to stakeholders in full in audio MP3 format taken from edition 13 of Busine..
Meeting responsibilities to stakeholders in full in PDF format taken from edition 13 of Business Cas..
Meeting stakeholder needs through community involvement in full in audio MP3 format taken from editi..
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Operating a statutory body in a commercial environment in full in PDF format taken from edition 4 ..


Internet of Things and Urban Innovation (iNUIT) is an applied research program funded by HES-SO. Started in 2014, it initially focused on crowd monitoring, with the aim of optimising the mobility and physical safety of visitors during major events.
In 2015 and 2017, iNUIT started collaborating with the Paleo Festival Nyon, the Federal Wrestling and Alpine Games Festival, and the Grape Harvest Festival. Currently (2018 – 2020), iNUIT is extending its platform to support IoT applications deployed at city scale.
EnhanceR is a national initiative to provide specialised research IT support to the Swiss research academic sector. It achieves this goal by federating Research IT specialist groups at various academic institutions across Switzerland. EnhanceR has core expertise in the fields of efficient computing, big-data analytics, and large-scale data management.
The Large-Scale Distributed Systems Research Group is specialised in methodologies and frameworks for developing large-scale applications deployed in heterogeneous environments. Our research activities are currently focused on the Internet of Things (IoT), edge/cloud computing and sensor networks. The application domains include sustainable energy, environmental monitoring and urban computing.
This research group is part of hepia, the Geneva-based unit of the University of Applied Sciences – Western Switzerland (HES-SO). We are particularly interested in applied research projects that address actual needs from industry.


text:
\section{Introduction}
Disorder effects can strongly modify critical properties close to phase transitions. When investigating the role
of disorder, one usually distinguishes two cases: in random-field systems, the disorder couples {\em linearly}
to the order parameter, while in so-called random mass systems, the coupling is to the square of the order parameter.

Random fields effects are by far more dramatic compared to the
random-mass case. As has been shown in a seminal paper by Imry and Ma
\cite{Imry1}, weak random field even destroys completely long range
order for magnets with xy or Heisenberg symmetry as the energy costs
to form domain walls are smaller than the energy gain when the
magnetic structure adapts locally to the random field. For magnets
with Ising symmetry, long range order is stable in three dimensions
(3D) as long as the random fields are weak but the properties close to
the phase transition are strongly modified.

Random field criticality, and especially the Random Field Ising
Model (RFIM), has attracted considerable interests in the last decades.
Despite this broad activity \cite{reviews} including numerical, analytical
 and experimental investigations, a complete understanding of the RFIM is still lacking.
It is established by now that the results of the perturbative RG
calculation (the
so-called "dimensional reduction" \cite{Aharony1,Grinstein}) are incorrect
and a consistent theoretical treatment should necessarily rely on some
sort of non-perturbative approach. Steps in this direction has been made
recently with the help of the functional renormalization group
\cite{Wiese,Tarjus1} but
the issue of the determination of the correct critical exponents is far from
being settled. Moreover, the intrinsic
"glassiness" of the RFIM renders the problem hard to be tackled
numerically \cite{Middleton1} and, to our
knowledge, an unified view of the critical behavior is not
yet available. All these complications also arise at a
quantum-critical point in the presence of random fields
as has been recently discussed by Senthil \cite{Senthil}.

An important step towards the experimental realization of RFIM was made by
Fishman and Ahrony \cite{Fishman} who suggested to
study doped Ising antiferromagnets in uniform
magnetic fields. Remarkably, they showed that the net effect of the
random moments induced by the non-magnetic doping plus the applied
field  naturally leads to
 the same critical behavior as the RFIM. This setup has the unique advantage
 that one can easily tune the effective strength of the random field
 just by changing the size of
 the external uniform field.
These observations paved the way for many interesting experiments
\cite{Belanger1} and for
further theoretical work. For example, in a series of recent
neutron scattering measures \cite{Ye1,Ye2}, the lightly-doped iron compound ${\rm Fe_{1-x}Zn_xF_2}$
showed all the expected features of the RFIM in and out of
equilibrium. For this material, an accurate experimental determination
of  critical exponents was possible.

Recently, also the effects of random-mass disorder close to quantum
phase transitions in metallic antiferromagnets have been studied
theoretically by a number of authors \cite{vojta}. Close to the
critical point, disorder leads to the formation of magnetic domains.
In contrast to the random-mass case these domains are not pinned by
external fields and can have stronger fluctuations. This has been
predicted to lead to pronounced Griffiths singularities, smeared
transitions and glassy states \cite{vojta}.

In the present paper, we investigate the role of random fields on {\em
  quantum} phase transitions of metallic magnets ignoring the (much
smaller) role of random mass effects. As in the setup
proposed by Fishman and Ahrony \cite{Fishman} for classical systems,
we consider field driven transition in weakly disordered metallic
magnets with Ising symmetry.  In these systems, where long range order
\emph{can} exist, the role of the magnetic field is two-fold. On the
one hand, coupled to the (non-magnetic) impurities, it generates the
random field; on the other hand, it induces a quantum phase transition
at a certain critical strength. Field-driven quantum phenomena are
today a major topic of experimental investigation, both in the context
of magnetic insulators, where the field typically induces a
Bose-Einstein condensation of magnons, and in the one of magnetic
metals, where the field instead leads to the suppression of the long
range order \cite{Inga}.

Our analysis addresses the latter case. As an example, we have in mind
the heavy-fermion compound ${\rm CeCu_{6-x}Au_x}$, for which many
experimental data are already available in the literature
\cite{Lohnesyan1,Lohnesyan2}.  This material
 is a prototypical heavy-fermion system governed by the competition
of Kon\-do scree\-ning and RKKY interactions. For a finite concentration
of gold and below a certain critical field, antiferromagnetic Ising
order appears at a finite N\'eel temperature $T_N$. For a doping
$x>0.1$ the metal orders magnetically at low temperatures. For a
doping larger than $0.1$, the magnetic order can be suppressed by a
uniform magnetic field which allows a precise study of a field-driven
quantum phase transition. The doping by Au atoms naturally induces
disorder. For example, a doping $x=0.2$ reduces \cite{Lohnesyan1} the effective Kondo
temperature on average by approximately 50\%. This implies
that also the Kondo temperatures will strongly vary locally.
Therefore one expects in the presence of a uniform magnetic field
rather strong fluctuations in the local magnetization. These
static spatial fluctuations play the role of effective random fields and are expected to
modify dramatically the properties close to the quantum phase
transition. For example, magnetic domains will start to nucleate even
on the non-magnetic side of the phase diagram. As we will discuss,
recent elastic neutron scattering results from Stockert {\it et al.}
\cite{Stockert} appear to be consistent with this scenario.

In this paper, we will not try to describe the critical properties of
field driven quantum phase transitions directly at or very close to
the quantum critical point. In this regime one has to face all the
(unsolved) problems well known from the classical RFIM as has been
shown in Ref.~\cite{Senthil}. Instead we
will focus on the much more simple, but nevertheless experimentally
relevant question, in what regime the quantum-critical properties of
the clean system are modified by the random field. What are the
signatures of the onset of random-field physics? To answer this
question we use standard perturbative renormalization group (RG)
methods to determine the properties of the phase diagram and the
location of the crossover lines. The perturbative approach is
combined with phenomenological considerations based on the Imry-Ma
\cite{Imry1} argument.

In the following, we first review the derivation of the RG equations
\cite{Grinstein,hertz,Micnas,Millis} and we obtain
the general phase diagram with the different physical regimes and
crossover lines. Then, we focus on equilibrium and
out-of-equilibrium experimental
quantities and we list possible smoking guns for the onset of
random field physics.

\section{Model and perturbative RG equations}
The starting point is the usual Landau-Ginzburg-Wilson functional for the
order parameter \cite{hertz}
\begin{eqnarray}\label{S}
\emph{S}(m)&=&\frac{1}{2}\sum_{\lambda}\Bigl[\Bigl
(\delta+q^2+\frac{|\omega_n|}{\Gamma}\Bigr )m_{\lambda}m_{-\lambda}+h_{\mathbf{q}}m_{\lambda}\delta_{\omega_n,0}\Bigr]
\nonumber\\ &&+\frac{u_0}{\beta}\sum_{\lambda,\lambda',\lambda''}m_{\lambda}m_{\lambda'}m_{\lambda''}
m_{-\lambda-\lambda'-\lambda''}
\end{eqnarray}
where $m$ is the Ising order parameter,
$\lambda=(\omega_n,\mathbf{q})$, $\Gamma$ is a characteristic energy scale
(set to $\Gamma=1$ in the following)
 and $\delta$ is the critical
tuning parameter (proportional to $B-B_c$ for a transition driven by a uniform field $B$).
The momentum $\vec{q}=\vec{k}-\vec{Q}$ is measured with respect to the ordering vector $\vec{Q}$
of the antiferromagnet and the $|\omega_n|$ describes the
damping of spin fluctuations by a coupling to particle-hole pairs in a metal. Due to its presence, typical energies
scale as $q^2$ in the clean system and therefore the dynamical critical exponent is $z=2$. For an insulator (or
a metal with small Fermi surface, $2 k_F < Q$) the $|\omega_n|$ is replaced by a $\omega_n^2$ term such that $z=1$
in this case.

$h(x)$ is the static random
field that is
assumed to be Gaussian correlated,
\begin{equation}
\langle
h(\mathbf{q})\rangle=0\qquad{\rm and}\qquad
\langle
h(\mathbf{q})h(\mathbf{q}')\rangle=h^2\delta(\mathbf{q}+\mathbf{q}'),
\label{disorderdistribution}
\end{equation}
with tunable strength $h$ which is typically proportional
to the strength of non-magnetic disorder and, more importantly, to the external uniform field.

With the help of the standard replica trick, we can average over the
disorder replicating the action
\begin{eqnarray}
\emph{S}(m^{\alpha})&=&\frac{1}{2}\sum_{\lambda,\alpha,\alpha'}\Bigl[\Bigl(\delta+q^2+\frac{|\omega_n|}{\Gamma}\Bigl)\delta_{\alpha,\alpha'}-\beta
h^2\delta_{\omega_n,0}\Bigr]\times\nonumber \\&\times& m_{\lambda}^{\alpha}m_{-\lambda}^{\alpha'}
+\frac{u_0}{\beta}\sum_{\lambda,\lambda',\lambda''}m_{\lambda}^{\alpha}m_{\lambda'}^{\alpha}m_{\lambda''}^{\alpha}
m_{-\lambda-\lambda'-\lambda''}^{\alpha}\qquad\label{replicatedaction}
\end{eqnarray}
where $\alpha=1,2..,n$ are the replica-indices. We have
formally eliminated the random field and, in absence of the quartic interaction,
the free propagator is given by
\begin{eqnarray}
\langle
m^{\alpha}_{\lambda}m^{\alpha'}_{\lambda'}\rangle&=&\delta_{\lambda,-\lambda'}\Bigl(\delta+q^2+\frac{|\omega_n|}{\Gamma}\Bigl)^{-1}\Bigl[\delta_{\alpha,\alpha'}
+\nonumber\\&+&\beta
h^2\delta_{\omega_n,0}\Bigl(\delta+q^2\Bigr)^{-1}\Bigr].\label{propagator}
\end{eqnarray}
Observe that already within the Gaussian approximation the propagator at $\omega_n=0$ is highly singular in the presence
of the random field. Computing the
diagrams in Fig.~\ref{Feynman} for the replicated action in
Eq.~(\ref{replicatedaction}), we obtain the following closed set of one-loop RG equations
(similar to the one obtain by Micnas and Chao \cite{Micnas})
\begin{eqnarray}
\frac{d\delta}{d\log b}&=&2\delta+6u\emph{f}_1(T)+6vf_2 \label{RG1}\\
\frac{dv}{d\log b}&=&(6-d)v-36uv\emph{f}_3(T)-72v^2\emph{f}_4\label{RG2}\\
\frac{du}{d\log b}&=&[4-(d+z)]u-36u^2\emph{f}_3(T)-72uv\emph{f}_4\label{RG3}\\
\frac{dT}{d\log b}&=&zT(b)\label{RG4}
\end{eqnarray}
where we defined $v=uh^2$ as a renormalized disorder parameter and we
introduced the functions $\emph{f}_n$ ($n=1,2,3,4$) defined in the appendix. Note that while $f_1$ and $f_3$
depend both on the renormalized $\delta(b)$ and $T(b)$, the functions $f_2$ and $f_4$ depend
on $\delta(b)$ only as the disorder is static.
The upper critical dimension $d=6$ is set by the renormalized disorder
$v$. As the classical RG equations \cite{Grinstein}, Eqns.~(\ref{RG1}-\ref{RG4}) have to leading order in $\epsilon=6-d$
 a stable fixed point, $v^*=\epsilon/72$, $u^*=0$. The critical exponents appear to be
  given by the ones of the equivalent clean system in dimensions  $d^*=d-2$ (dimensional reduction, see above).

\section{Phase diagram}
As already pointed out in the introduction, the pertubative fixed point and the
critical exponents are incorrect but they are not our main focus here. We
consider instead small bare couplings, $h^2\ll 1$ and $u\ll
1$, studying the RG equations in the vicinity of the quantum critical point of the clean system, described
by an
unstable Gaussian fixed point. Following the flow of the coupling
constants, we identify the different
crossover lines by investigating for which parameters $\delta$, $v$ or $u$ become of order $1$.
\begin{figure}
\includegraphics[width=.45\textwidth,clip]{feynman.eps}
\caption{The one-loop diagrams in the presence of disorder. The black
  dot indicates the random field contribution.}
\label{Feynman}
\end{figure}
Linearizing Eqns.~(\ref{RG1}-\ref{RG4}) around $u=v=\delta=0$, we obtain
\begin{eqnarray}
\frac{d\delta}{d\log b}&=&2\delta+6 u \emph{f}_1(T)+6 v \emph{f}_2\\
\frac{du}{d\log b}&=&[4-(d+z)]u\\
\frac{dv}{d\log b}&=&(6-d)v\\
\frac{dT}{d\log b}&=&zT,
\end{eqnarray}
where $f_2$ is now just a number,
and we can write the formal solution
\begin{eqnarray}
\delta(b)&=&b^2\Bigl[\delta_0+6u_0\int_0^{\log b}dx
e^{[2-(d+z)]x}\emph{f}_1(Te^{zx})\nonumber \\
&&+6v_0\emph{f}_2\int_0^{\log
  b}e^{(4-d)x}\Bigr]\label{RG1L}\\
u(b)&=&u_0b^{4-(d+z)}\label{RG2L}\\
v(b)&=&v_0b^{6-d}\label{RG3L}\\
T(b)&=&T_0b^{z}\label{RG4L}.
\end{eqnarray}
Here $u_0, v_0$ are the bare values of the couplings. Correspondingly,
$T_0$ is the bare, i.e. the physical temperature.
The features of the function $\emph{f}_1(T)$ have been already
discussed in \cite{Millis} (see appendix). For
our purposes, we only need to know that
\begin{eqnarray}
\emph{f}_1(T)&\approx&\emph{f}_1(0)\qquad T\ll 1\label{cond1}\\
\emph{f}_1(T)&\approx&CT\qquad T\gg 1\label{cond2}
\end{eqnarray}
\begin{figure*}
\begin{center}
\includegraphics[width=0.85 \textwidth]{QCphasediagram.eps}
\end{center}
\caption{Main figure: Phase diagram for a quantum critical
  antiferromagnetic metal  with Ising symmetry  in $d=3$
as a function of temperature and control parameter $r \propto B-B_c$ in
  the presence of random field disorder $h$.
Close to the phase transition line, where long-range order vanishes
(solid green line), the effects of disorder become dominant (region enclosed
by the two dotted red lines parallel to the solid green line).
The crossover from the  quantum critical to the Fermi liquid regime
of the underlying clean system upon lowering $T$ occurs at $T\sim r$
(dotted magenta line). The Wilson Fisher
regime of the classical phase transition in the clean limit is only
present for $r<-h$ (dotted blue  lines at the left part of the
diagram). Inset: Phase diagram of a system
(e.g. $\rm CeCu_{5.8}Au_{0.2}$)
where magnetism can be suppressed either by pressure or an applied
magnetic field. As the strength of the effective disorder is
  proportional to the applied uniform field, $h \propto B$, one can
 tune the effective strength of random-field disorder.}
 \label{phasediagram}
\end{figure*}
We first investigate the low-temperature ``Fermi liquid'' (FL) regime on the disordered
side of the phase diagram, see Fig.~\ref{phasediagram}. Here, $\delta(b)$ reaches the cutoff first
in a regime where $T(b)\ll 1$ and $v(b) \ll 1$.
Using Eq.~(\ref{cond1}) and expanding Eq.~(\ref{RG1L}), we obtain for
$d+z>4$ (we are mainly interested in the metallic, three-dimensional case, $d=3, z=2$)
\begin{eqnarray}
1&=&b^2[\delta_0+\frac{6u_0\emph{f}_1(0)}{d+z-2}+6v_0\emph{f}_2\frac{(b^{(4-d)}-1)}{4-d}]\nonumber\\
&&\approx b^2[\delta_0+\frac{6u_0\emph{f}_1(0)}{d+z-2}]=b^2r\\
T&=&T_0b^z=T_0/r^{z/2}\ll 1 \label{tR}\\
v&=&v_0r^{(d-6)/2}\ll 1 \label{vR}
\end{eqnarray}
where $r$ describes the distance from the quantum-critical point of
the underlying {\em clean} system,
\begin{equation}
r=\delta_0-\delta_0^c=\delta_0+\frac{6u_0\emph{f}_1(0)}{d+z-2} \label{criticalT0}.
\end{equation}
The
first inequality (\ref{tR}) describes the crossover to the quantum
critical regime, see Fig.~\ref{phasediagram}, while
the second  (\ref{vR}) the onset of a regime, where the random field
dominates the critical behavior
(see discussion below).

A similar condition for the onset of random-field criticality can be
obtained in the ordered phase. Here we use the phenomenological
Imry-Ma argument \cite{Imry1}.
The random field favors the proliferation of magnetic domain walls
where each domain (of radius $L$) adjusts itself to the underlying random-field landscape.
Far enough from the transition, the energy cost of a
domain wall \cite{Chaikin} is proportional to
$\frac{|r|^{3/2}}{u}L^{d-1}$ for $L$ large compared to the correlation
length $\xi$. The energy gain from the random field
scales with $h m L^{d/2}$ where the size of the order parameter is
given by $m=(|r|/u_0)^{1/2}$.
In $d>2$, the size of a random-field induced domain is therefore
limited by
\begin{equation}
h\Bigl(\frac{|r|}{u}\Bigr)^{1/2}L^{d/2}>\frac{|r|^{3/2}}{u} L^{d-1}.
\end{equation}
This inequality has an solution with $L>\xi\approx r^{-1/2}$ only for
\begin{equation}
|r| \lesssim  (uh^2)^{\frac{2}{6-d}}. \label{imrymaginzburg}
\end{equation}
which is equivalent to the condition (\ref{vR}) obtained from
perturbative RG for the disordered side of the phase
diagram. Therefore if $|r|$ is sufficiently small, magnetic domains
caused by the random field will proliferate while deep in the ordered
phase only exponentially rare random-field configurations induce (small) domains.

In $d=2$, the long range magnetic order is always destroyed and
fragments into domains. In this case, (\ref{imrymaginzburg}) describes the condition for a crossover
from exponentially large domains for large negative $r$ to a disorder dominated regime for smaller $r$ \cite{binder}.

The quantum critical (QC) regime is obtained when approaching the
quantum phase transition by lowering the temperature. In this regime,
the  rescaled $T(b)=T_0 b^z$ reaches the cutoff, $T(b=b^*)=1$ where
the RG flow changes its nature (but is not stopped).
 Therefore it
 is useful to split the RG flow in two steps,  rewriting
 Eq.~(\ref{RG1L}) as follows
\begin{eqnarray}
\delta(b)&=&b^2\Bigl[\delta_0+6u_0\int_0^{\log b^*(T)}dx
e^{[2-(d+z)]x}\emph{f}_1(Te^{zx})\nonumber \\
&&+6u_0\int_{\log b^*(T)}^{\log b}dx
e^{[2-(d+z)]x}\emph{f}_1(Te^{zx})\nonumber\\ &&+6v_0\emph{f}_2\int_0^{\log
  b}e^{(4-d)x}\Bigr]\label{RG1Lbis}
\end{eqnarray}
where we defined $b^*(T_0)=T_0^{-1/z}$. Using Eqns.~(\ref{cond1}) and (\ref{cond2}), we can perform the integrals in Eq.~(\ref{RG1Lbis}),
to obtain
\begin{eqnarray}
\delta(b)&=&b^2\Bigl[r+6u_0\bigl(\frac{\emph{f}_1(0)}{2-(d+z)}+\frac{C}{d-2}\bigr)T^{\frac{d+z-2}{z}}\nonumber\\
&&+\frac{6v_0\emph{f}_2}{4-d}b^{4-d}\Bigr].\label{cri}
\end{eqnarray}
The combination
\begin{equation}
\bar{r}=r+6u_0\bigl(\frac{\emph{f}_1(0)}{2-(d+z)}+\frac{C}{d-2}\bigr)T^{\frac{d+z-2}{z}},
\end{equation}
can be identified with the distance from the finite-temperature phase
transition line \cite{Millis}.

To find the crossover lines to the random-field dominated regime, we
have to investigate under which condition, the term proportional to
$v_0$ dominates in (\ref{cri}) of the clean system. For $v_0=0$,
$\delta(b)$ reaches $1$ for $\bar b=\bar{r}^{-1/2}$. As the RG flow stops
for $\delta(b)>1$, we can obtain the crossover line from the condition
$\bar{r}\approx \frac{6v_0\emph{f}_2}{4-d}{\bar b}^{4-d}$.
Random field physics therefore dominates for
\begin{equation}
\bar r \lesssim (u_0 h^2)^{\frac{2}{6-d}}. \label{ginzburgdisorder}
\end{equation}
This is also the condition that $v(\bar b)$ becomes of order $1$ (note
that $\bar b$ and not $b^*$ enters here).
 This last equation is \emph{de
  facto} a Ginzburg criterion for the on-set of the random field effects.
Notice that Eq.~(\ref{ginzburgdisorder}) is the extension to finite
temperature of Eq.~(\ref{imrymaginzburg}) that followed directly from
the Imry-Ma argument.

For $r=0$, i.e. in the quantum-critical region of the
underlying clean system, the effects of random fields are weak for
$T_0>T^*$ with
\begin{eqnarray}
T^{*}&\approx& u^{\frac{z(d-4)}{(6-d)(d+z-2)}}h^{\frac{4z}{(6-d)(d+z-2)}}\nonumber\\
&\approx& \Bigl(\frac{h^2}{u^{1/2}}\Bigr)^{4/9} \qquad {\rm for } \quad  d=3,z=2.
\end{eqnarray} according to Eq.~(\ref{ginzburgdisorder}).

The calculations given above are obviously not valid very close to the
{\em classical} phase transition of the clean system where also $u$
is relevant. Very close to the QCP this Wilson-Fisher critical regime
is never reached because the random field becomes relevant first.
Comparing the Ginzburg criterium for the clean system
\begin{equation}
\frac{uoT_0}{\bar{r}^{(4-d)/2}}\approx 1.\label{WFcrossover}
\end{equation}
with Eq.~(\ref{ginzburgdisorder}), we find that the system will enter
the Wilson-Fisher regime of the clean system {\em before} the random
fields becomes relevant only for $|r| > r_{WF}$ (see
Fig.~\ref{phasediagram}) with
\begin{eqnarray}
r_{WF}&\approx& h^{\frac{8-2 d}{6-d} \, \frac{d}{z}}
u_0^{\frac{6 z -    d z -2 d}{(6-d) z}} \nonumber \\
 &=& h \qquad {\rm for } \quad  d=3,z=2
\end{eqnarray}

Combining the results for the various crossover lines, we obtain the
phase diagram shown in Fig.~\ref{phasediagram}.

\section{Experimental probes}

As pointed out in the introduction, field driven quantum phase
transitions offer a high degree of tunability. An external magnetic
field changes not only the distance
to the quantum-critical point but also the effective strength of
the random-field disorder, $h \propto B$. Ideally, one can use a
combination of
doping and magnetic field or, even better, of pressure and magnetic field to
tune the random field strength and the distance from the QCP
independently. For example, considering a system like
CeCu$_{5.8}$Au$_{0.2}$, the quantum critical point can be reached
either by applying moderate magnetic fields or a moderate
pressure. By crossing the phase transition line in the $B,p$ plane for
different values of the magnetic field (see inset of Fig.~\ref{phasediagram}), one can systematically study
how random fields modify the physics.

\subsection{Elastic neutron scattering and comparison to CeCu$_{5.8}$Au$_{0.2}$}\label{neutronscattering}
Elastic neutron scattering probes the static magnetization of the
sample as a function of momentum. In a random field system there
is always a finite, spatially-fluctuating static
magnetization even far away from the transition. In contrast, in a
clean system (or in the presence of only random-mass disorder), a finite-momentum static
magnetization appears only in the ordered phase \cite{footnote}.
\begin{figure}
\includegraphics[width=.50\textwidth,clip]{neutron.eps}
\caption{Sketch of the elastic neutron scattering signal in the
  ordered and disordered phases. Deep in the ordered phase, one expects
  a resolution limited peak of Gaussian shape
at the ordering wave vector. Random fields induce a double-Lorenzian
tail of width $\sqrt{2|r|}$, see Eq. (\ref{sigmael}).
Upon approaching the random-field regime,
the weight of the tail becomes of the order of the weight of the
central peak. Also in the Fermi liquid regime, the random field gives
a contribution to the neutron scattering signal described
by Eq.~(\ref{sigmael2}).
\label{neutronSchematic}}
\end{figure}
Outside of the random-field regime, i.e for $|r|>(u_0 h^2)^{2/3}$
(assuming $d=3$ in this chapter)
one can easily estimate the effects of the random field. Even deep in
the antiferromagnetic phase, the random fields will induce an extra
contribution to the magnetization, $\delta m_q \approx \chi_q h_q$,
where $\chi_q \approx 1/(-2r +q^2)$ is the susceptibility of the
clean system in the ordered phase ($r<0$) and $q$
measures the distance from the ordering wave vector.
 Averaging over
disorder, we obtain a corresponding contribution to elastic neutron
scattering.
The total elastic cross section
\begin{eqnarray}
\sigma_{el}(q) \approx m_0^2 \,\, \delta^3(q)+
\frac{h^2}{(|2 r|+q^2)^2}
\label{sigmael}
\end{eqnarray}
therefore obtains a contribution both from the long-range order and
from the random fields. There is also an extra contribution (not shown
above) from exponentially rare field-induced domains and the
corresponding domain walls. These domains proliferate upon approaching
the random-field regime. A schematic picture of the expected neutron
signal (including resolution effects) is shown in Fig.~\ref{neutronSchematic}.

Similarly, approaching the transition from the disordered side one
obtains
\begin{eqnarray}
\sigma_{el}(q) \approx
\frac{h^2}{( r+q^2)^2}
\label{sigmael2}
\end{eqnarray}
As above, there are some rare regions where the random fields are
strong and for which (\ref{sigmael2}) cannot be used but these
give only sub-leading contributions for
 $r>(u_0 h^2)^{2/3}$.

For an experiment with finite resolution, it is not possible to separate
the two contributions in (\ref{sigmael}) very close to the
transition. In the random-field regime, the weight of the order
parameter is always smaller than the weight of the disorder contribution.
As a consequence, the phase transition appears to be
'smeared out'.

Qualitatively, such a behavior has been observed in recent neutron
scattering experiments on the field-driven QPT in
CeCu$_{5.8}$Au$_{0.2}$ by Stockert {\it et al.}
\cite{Stockert}. Upon approaching the transition, the elastic neutron
scattering signal broadens and the weight of the signal is reduced.
However, there are no sharp features and the integrated intensity
remains finite well beyond the critical field. According to
Eq.~(\ref{sigmael2}), the width of the signal should grow
as $\sqrt{r} \sim \sqrt{B-B_c}$ while the total integrated intensity
vanishes slowly with $h^2/\sqrt{r}$ (note that in Ref.~\cite{Stockert}
the intensity was obtained by integrating over a rocking scan, i.e. a
line in momentum space, leading to a more rapid decay $\sim
h^2/r^{3/2}$). While the experimental results appear to be consistent
with the predicted scenario, a fully quantitative comparison is not
possible due to the limited statistics and momentum
resolution of the experiment. For a quantitative comparison it would be useful to
consider samples with different doping and different critical fields.
Ideally, one would like to use both pressure and field to explore the
phase diagram sketched in the inset of Fig.~\ref{phasediagram} using a
single sample with fixed bare disorder strength. In such a case, the
random field $h$ will be roughly proportional to the critical field $B_c$.

\subsection{NMR}\label{NMR}
As a local probe,
nuclear magnetic resonance (NMR) is a natural tool to investigate systems with
magnetic textures and inhomogeneities. It is possible to measure
directly the distribution of the local magnetization
$M(\vec{r})=M_0+\delta M$.
Assuming a Gaussian distribution of the random fields,
$p[h(r)]\sim \exp\!\!\left(- \int h(r)^2/(2 h^2)\right)$ as in
Eq.~(\ref{disorderdistribution}), we can derive the corresponding
distribution of magnetic moments outside of the random field regime
using again $\delta m_q \approx \chi_{\mathbf{q}} h_q$ to obtain
\begin{eqnarray}
P(\delta M)&\approx& \exp\!\!\left(
-(\delta M)^2/(2 \sigma^2)\right)\label{stagmoments}\\
\sigma^2&=& h^2 \int\chi_{\mathbf{q}}^2\sim
\frac{h^2}{r^{(4-d)/2}}
\end{eqnarray}
For a field-driven quantum phase transition in $d=3$, we therefore expect a
width $\sigma$ proportional to $B/(B-B_c)^{1/4}$.

\subsection{Non-equilibrium effects}

Probably the most direct way to detect random-field physics, is the
observation of hysteretic  behavior in the random-field regime which shares
similarity to the properties of (spin-) glasses. This
is well known both theoretically and experimentally for classical random-field
systems. Upon approaching the classical critical point, the relevant relaxation
rates grow exponentially \cite{Villain,Fisher,Nattermann} with the correlation length,
\begin{equation}\label{rate}
\tau \sim \exp[c \, \xi^{\theta}/T],
\end{equation}
where $\theta$ parameterizes the typical free energy of the system at
the scale $\xi$, $F_\xi\sim \xi^\theta$. For conventional critical
points one has $F_\xi\sim T \sim const.$. A
divergence of $F_\xi$ leads to a violation of hyper-scaling,
$(d-\theta)\nu=2-\alpha$ ($\nu$ and $\alpha$ are the
correlation length and specific heat exponents). Therefore $\theta$
describes to what extent there is an effective dimensional reduction,
$d \to d-\theta$. In Ref.~\cite{Middleton1}, $\theta\approx 1.49 \pm
0.03$ was estimated numerically for $d=3$.

\begin{figure}
\includegraphics[width=.36\textwidth,clip]{magnetization.eps}
\caption{The two non-equivalent cooling procedures. The zero-field
  cooling path is indicated with the thin green arrows while the
field cooling scheme uses a path along the
 thick red arrow.}
\label{magnetization}
\end{figure}

Experimentally, the long relaxation rates lead to strong
non-equilibrium effects.  Neutron scattering experiments
\cite{Ye2,Belanger1} and
magnetization measurements \cite{Kleemann} on diluted antiferromagnets
in uniform magnetic fields show hysteretic behavior. It is, for
example, useful to compare field-cooled with zero-field cooled
samples. Zero field cooling (green
arrows in Fig.~\ref{magnetization}) leads to a well-ordered
antiferromagnetic state. Instead, field cooling causes a fragmentation
of the antiferromagnet into non-equilibrated domains. The size of the
domains depend on the strength of the random field \cite{Villain} and
logarithmically on the cooling rate, see
Eq.~(\ref{rate}).
For example, experiments in field-cooled and
zero-field-cooled $\rm Fe_{0.85}Zn_{0.15}F_2$, give distinct critical
behavior \cite{Ye2,Belanger1}. Moreover, sweeping fast in
temperature back and forth through the transition, can cause the onset
of hysteresis phenomena in the intensity of the Bragg peak.

From energetic and renormalization group arguments, it is believed
\cite{reviews,Senthil} that the static properties of the $T=0$ and
finite-temperature random-field transitions are described by the same
fixed point. The dynamics and therefore the non-equilibrium properties
can, however, differ.
For $T \to 0$, the dynamics is not any more governed by thermal
fluctuations and thermal activation but instead by quantum tunneling.  Nevertheless, the
existence of extensive energy barriers, $E_\xi \sim \xi^\theta$, will
lead again \cite{Senthil} to exponentially long relaxation times
 \begin{equation}\label{rate1}
\tau \sim \exp[c' \, \xi^{\Psi}],
\end{equation}
 with $\Psi \neq \theta$ for insulators.
In a metal, one has furthermore to take into account, that
quantum-tunneling can be suppressed \cite{Millis1,vojta} by the coupling of
the order parameter to the electrons. This will lead to an additional
suppression of the tunneling rate proportional to $T^{c'' \xi^\gamma}$
 \begin{equation}\label{rate1}
\tau \sim T^{-c'' \xi^\gamma} \exp[c' \, \xi^{\Psi}],
\end{equation}
with a new (and unknown) exponent $\gamma$
such that $\tau(T=0)=\infty$ for sufficiently large domains.

Note that long relaxation times, smeared transitions and glassy effects can also arise in
the absence of magnetic fields, i.e. in systems with random-mass
disorder \cite{vojta}. In general, these effects are expected to be
much weaker (the bare scaling dimension of the random-mass disorder is
$4-d$ rather than $6-d$). Furthermore, the (bare) strength of the
random-mass disorder does not  depend strongly on the
strength of the external magentic field which allows to separate the
two effects.

\section{Conclusions}

Field-driven quantum phase transitions of antiferromagnets
offer a unique possibility to study the interplay of disorder and
quantum criticality. Here one has to distinguish two cases: when the
staggered magnetization is perpendicular to the applied field (the
typical situation for a system with Heisenberg symmetry) and the
opposite situation (for Ising symmetry). In the first case,
disorder effects are usually weak, the disorder couples only to the
square of the order parameter.  This paper focuses on the second case,
where effectively a random field  is generated \cite{Aharony1} which
couples linearly to the order
parameter. In easy plane antiferromagnets, one can have
both situations depending on the direction of the magnetic field.

As magnetic domains can nucleate and pin at random field
configurations, the critical behavior of the system is radically
changed by the presence of disorder. By comparing quantum critical
points of the same material at different pressure, different doping or
different field direction, one can directly observe how random-fields
of different strengths affect quantum criticality.

With the help of perturbative renormalization group we have derived the
generic features of the phase diagram for metallic Ising antiferromagnets in
weak random fields. While this method is not able to investigate the
regime, where random-field physics dominates, one can nevertheless
extract the relevant crossover scales. This is especially of interest
for the study of systems where the effective strength of random-field
disorder can be tuned as described above and in the inset of
Fig.~\ref{phasediagram}.

One effect of random fields is that the phase transition appears to be
``smeared''. We argue that this has been observed in recent elastic
neutron scattering experiments in CeCu$_{5.8}$Au$_{0.2}$ where the
elastic neutron scattering peak broadens and slowly diminishes in
weight when the magnetic field is increased beyond the critical field.

The most direct way to detect random-field physics is the observation
of hysteretic behavior as a function of temperature and, especially, field. In
metals, these non-equilibrium effects are enhanced compared to their
classical counterparts as quantum tunneling is inhibited by the
coupling to the particle-hole pairs of the metal and thermal activation
is suppressed by the low temperatures.

We hope that the high tunability of the random-field
physics will motivate further theoretical and especially experimental
studies of this very interesting problem.

\begin{acknowledgement}
We thank T. Nattermann, N. Shah, O. Stockert, M. Vojta and K. Wiese for useful discussions
and the research group 960 and the
SFB/TR 12 of the DFG for financial support.
\end{acknowledgement}

\begin{appendix}
\section*{Appendix A: $f_n$ functions}\label{f-functions}
Referring to the case of an
itinerant antiferromagnet, in accordance with \cite{Millis}, the $f_1$ function is defined as
\begin{eqnarray}
f_1&=&\frac{\Lambda^{d+z+2}\Omega^d}{\pi}\int_0^{\Gamma\Lambda^{z-2}} d\omega\coth\frac{\omega}{2T}\frac{\omega}{\Lambda^{2z}(\delta+\Lambda^2)^2+\Lambda^4\omega^2}
\nonumber\\
&+&\frac{2\Gamma^2}{\pi}\int_0^{\Gamma}\frac{d^dq}{(2\pi)^d}\coth\frac{\Gamma}{2T}\frac{q^{2+z}}{q^4\Gamma^2+q^{2z}(q^2+\delta)^2}
\end{eqnarray}
where $\Lambda$ is the momentum cut-off, $\Gamma$ is the frequency
cut-off, $\Omega_d$ is the volume of the surface of unitary radius in
$d$ dimensions and
$z=2$ is the dynamical exponent.
The other functions are instead given by \cite{Micnas}:
\begin{eqnarray}
f_2&=&\frac{\Omega^d \Lambda^d}{(2 \pi)^d} \frac{1}{(\delta+\Lambda^2)^2}\\
f_3&=&-\frac{\partial f_1}{\partial\delta}\\
f_4&=&\frac{\Omega^d \Lambda^d}{(2 \pi)^d} \frac{1}{(\delta+\Lambda^2)^4}.
\end{eqnarray}

\end{appendix}

redpajama_set_name: RedPajamaArXiv


text:
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In 2014, the company embarked on a pilot at its bleaching chemicals business in Brazil to investigate the entire impact of its business across financial, environmental, human and social dimensions. In collaboration with True Price and sustainability consultants GIST Advisory, it did full profit and loss accounting across these four capitals – what it calls 4D accounting. The exercise confirmed that its sustainability strategy did indeed cover the most important elements, says Ringström.
It led AkzoNobel to increase its use of renewable energy, and put greater focus on better resource use of both energy and raw materials. Looking at impacts on human capital brought more emphasis on training and developing capabilities; while social capital led to work improvements in health and safety, and rights at work.
After the pilots, AkzoNobel applied the 4D approach across its entire pulp and performance chemicals business, followed in 2016 by environmental, social and economic profit and loss accounting across the entire business. It reported a monetary value for these three capitals, across its value chain.
Emma Ringström, sustainability manager at AkzoNobel's pulp and performance chemicals business.
Social impact assessment is in its infancy, but includes value related to the knowledge and skill development of employees and their future salary development.
The environmental assessment includes value through its products that help customers cut emissions. To put a monetary value on key impacts such as CO2 emissions and use of fossil resources, it uses a science-based approach that takes a long-term view. Prices are, says its report, based on what would happen in 50 to 100 years if we keep on using resources as we do today.
AkzoNobel has a wealth of data from its businesses, and more is becoming available in its supply chain, so the actual measuring is getting easier, says Ringström. Valuation, however, is more difficult.
As part of the Forest Solutions group at the World Business Council for Sustainable Development, AkzoNobel is piloting a forest sector guide, which will give the industry more specific guidance on measuring and valuing natural capital impacts. AkzoNobel is looking at the potential impact of changes in natural capital: for example, regional changes in water supply. The guide is expected later this year.


I hobbled into Farmingdale Physical Therapy West two weeks after my left knee replacement surgery and I thought I was going to hurt for quite a while. I thought wrong. On my first day, I was greeted by smiling, pleasant faces and invited to have a seat on one of the tables. My therapist, Jillian, did an evaluation and that is when a wonderful, fun time of heat, stim, cold packs, exercises, and conversations with other patients and staff had begun. The cane was rapidly given up and all through this experience there has been only constant attention by all members of the staff. I progressed rapidly and was cleared to resume my active lifestyle. Therefore, I will be going on a boat cruise after Thanksgiving and snowshoeing in New Hampshire in February. Thanks to all the staff for getting me back on my feet again and a special thanks to Jillian!


The Microsoft Surface RT launched back in late October now, and yet after all this time, there is no official blog space for news related directly to the Surface line. Good news, Microsoft has finally launched the Surface blog, just two days before the anticipated release of the Surface Pro tablet.
While Surface Pro and Surface RT share much of the same DNA, Surface RT is sleek and simple whereas Surface Pro is powerful and flexible. Surface Pro is perfect for the person or business that wants a laptop and a tablet, but doesn't want the weight or hassle of both. If you're looking for all-day battery life and an entertainment-first experience with the ability to still get some work done – Surface RT is for you.
Besides the welcome post, Panay also promises he will right more on Saturday, and expects future posts from other Surface team members in the next few weeks.
The Surface line is just getting started, and hopefully the release of a new blog (finally) is an indicate that Microsoft is not only focused on the launch of the Surface Pro but on the future of the Surface line in general. Now let's just hope they get their act together and give us a 7-inch Surface or even a 10-inch Surface Atom.
While we are on the subject of the Surface, we also have some news about the Surface RT. For those living in Canada, the Surface RT is about to receive a price cut to bring its costs more in line with U.S. Pricing.
The news indicates that the Surface RT will drop by $20 dollars on all models, with touch covers dropping $10 Canadian dollars. The Pro pricing will be in-line with US pricing from day one. This is only a $30 savings for those planning to buy a Surface RT and cover in the near future, but money saved is money saved, no matter how small.
Between the launching of the Surface Pro and the launching of the new Blog, are you excited about the future of the Surface line or not? Share your thoughts below.


text:
Sports Picks > Free MLB Picks > Pittsburgh Pirates vs Houston Astros 6/25/2019 Picks Predictions Previews
Pittsburgh Pirates VS Houston Astros
FSSW
Spread: Houston Astros -252
Pittsburgh Pirates vs Houston Astros 6/25/2019 Picks Predictions Previews
Pittsburgh Pirates will be on the road to play against Houston Astros from Minute Maid Park in Houston, Texas on Tuesday. Pittsburgh Pirates will be one of those top teams on the season if they continue to win consecutive games. The Pirates were successful against San Diego Padres in this last outing with the help of Kevin Newman from the batting side.
Houston Astros have declined on the season due to their seven-game losing streak. The Astros struggled to find a break through and lost seven straight games. However, the last outing against New York Yankees went well with the help of Jose Altuve, Yuli Gurriel and Yordan Alvarez. From the pitching side, Hoston witnessed Justin Verlander go deep for his team as he took out nine hitters on the mound.
Pittsburgh Pirates vs Houston Astros Predictions 6/25/2019
Pittsburgh's batters are averaging .263 at the plate and opposing hitters are averaging at .253. The leading batsman with an average of .315 along with hits, home runs and RBIs is Josh Bell. Pittsburgh is all set to start with Trevor Williams against Houston. The righty is holding an ERA of 42 and is 2-1 on the season with 10 BBs and 49 Ks.
Houston's batting squad is holding an average of .267 and opponent hitters are averaging at .215. The leading batsman with an average of .322 and along with 95 hits is Michael Brantley. When it comes to home runs and RBIs the Astros are looking towards Alex Bregman. Houston is all set to start with Gerrit Cole as their pitcher against Pittsburgh. The righty is holding an ERA of 3.54 and is 6-5 on the season with 25 BBs and 148 Ks.
Pittsburgh Pirates vs Houston Astros. The MLB pick for this match is Houston Astros -1.5 (-150). Houston Astros managed to dominate Pittsburgh in most of the games. The Astros will have the upper hand with Gerrit Cole on the mound. Out of the last 10 games, Houston was successful with 8 of Cole's starts. Pittsburgh on the other hand, will need to concentrate on their batting squad to produce more runs in this game. Final Score Prediction, Houston Astros will win and cover the run line 7-2.
Location: Minute Maid Park in Houston, Texas.
TV: FSSW
MLB Odds: Houston Astros -252
Free MLB Baseball Pick: Houston Astros -1.5 (-150)
By: Tony2019 | June 25, 2019


text:
Q: Problem when trying to set status using gigya php sdk I am using gigya javascript sdk for authentication purposes on my site. It works well. But I recently decided to try the php sdk, I was able to set status to twitter and linkedin using the php sdk but this I am able to retrieve the uid using the javascript api and when i use to setstatus using php sdk i get an error unauthorised user.
I appreciate any help.
Thanks.

A: Have you enabled wall updates in the Gigya site setup page? This is required for using setStatus. Just to be sure, take a quick look at the notes under "Supporting Providers":
http://wiki.gigya.com/030_API_reference/020_REST_API/socialize.setStatus

A: Encode uid fixed the problem


text:
Daniel Dahm, Digital Content Manager
Ezzy Castro, Reporter
Published: October 15, 2020, 1:15 PM
Updated: October 15, 2020, 4:55 PM
Tags: Brevard County, Melbourne, Crime, Triple Shooting
Woman killed in triple shooting at Lizzy's restaurant in Melbourne
Police search for 2 masked men seen leaving area
Published: October 15, 2020, 1:15 PM Updated: October 15, 2020, 4:55 PM
MELBOURNE, Fla. – A woman was killed and two men were wounded in a triple shooting early Thursday at a Melbourne restaurant, according to police.
The triple shooting was reported around 12:30 a.m. at Lizzy's restaurant at 1301 E. University Boulevard.
Melbourne police said officers were called to the restaurant and found three victims suffering from gunshot wounds. Melbourne police Commander Heath Sanders said two of the victims were shot inside the restaurant and the other was shot outside the business.
The victims were taken to the hospital, where 34-year-old Jamie Francis Wright died, according to police. One of the surviving victims was shot in the face and the other is in critical but stable condition, police said.
They were identified as 40-year-old Latavious Shant Johnson and 38-year-old Theron Ishmael Andre Wright, who is the husband of Jamie Francis Wright.
TRIPLE SHOOTING: @MelbournePolice investigating a shooting that left two hurt & one dead. We have live updates this morning @news6wkmg 6/630 pic.twitter.com/TweNniCvfg
— Ezzy Castro (@EzzyCastro) October 15, 2020
Authorities said two masked men were seen leaving the area in a dark-colored SUV.
Sanders said Lizzy's is a popular hangout spot, and he's hoping any witnesses will call police.
Anyone with information is asked to call Crimeline at 800-423 TIPS.
This story is developing. Stay with News 6 and refresh this page for updates.
Daniel Dahm
Daniel started with WKMG-TV in 2000 and became the digital content manager in 2009. When he's not working on ClickOrlando.com, Daniel likes to head to the beach or find a sporting event nearby.
Ezzy Castro
Ezzy Castro is a multimedia journalist on News 6's morning team who has a passion for telling the stories of the people in the Central Florida community. Ezzy worked at WFOR CBS4 in South Florida and KBMT in Beaumont, Texas, where she covered Hurricane Harvey in 2017. Being from Miami, Ezzy loves Cuban coffee and croquetas!


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Sigma Omega Psi (ΣΩΨ) was a historically Jewish Fraternity founded in 1914 and which merged into Alpha Epsilon Pi (ΑΕΠ) in 1940.

History

Sigma Omega Psi was founded in 1914 at College of the City of New York. Its purpose was as Greek letter college fraternity for Jewish students and to foster the spirit of true brotherly love and self sacrifice. Its publication was The Shield.

The fraternity held its Sixteenth Annual Convention at the Park Central Hotel in  New York City on December 29 through 31, 1936. Its Seventeenth Annual Convention was held in Boston, Massachusetts on December 29 through 31, 1937.

By 1940, only five chapters would be active, and the decision was made to merge into Alpha Epsilon Pi.

At the time of the Union, only the chapters at Worcester Poly, Boston University, Tufts, Lowell, and New York University were active. The first three became Epsilon Deuteron chapter, Zeta Deuteron chapter, and Eta Deuteron chapter of Alpha Epsilon Pi, respectively. The chapter at Lowell could not be merged due to National Interfraternity Council requirements and the chapter at New York University was merged with Alpha Epsilon Pi's Alpha chapter. Subsequently, the chapters at Syracuse, MIT and CCNY were reactivated by Alpha Epsilon Pi and considered to be revivals of the chapters of Sigma Omega Psi at those schools.

Chapters

More than twenty chapters were founded by 1940 including:

Alumni Clubs
Sigma Omega Psi had three alumni clubs

Notable alumni

 Nathaniel L. Goldstein - New York Attorney General 1943-1954.

References

Alpha Epsilon Pi
Student organizations established in 1914
1914 establishments in New York (state)
Historically Jewish fraternities in the United States
Jewish organizations established in 1914