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November/December 2014 Israel My Glory
They Cry in Silence Nov/Dec 2014
The nightmare continues for prominent Christian human rights attorney Gao Zhisheng and his family. When Gao was released from prison in China on August 7, no one heard anything from him. His family had telephone conversations with him, but they didn't hear much from him either.
Now it has become clear that isolation and torture have left Gao unable to speak coherently. China Aid reports, "Gao has been utterly destroyed. He can barely talk, and only in very short sentences. Most of the time he mutters and is unintelligible. It is believed he is suffering from a broad range of physical and mental health problems; he has not been allowed to see a doctor since his release."
As his wife, Geng He, told the Los Angeles Times, if he cannot even obtain adequate dental care, what hope does he have for obtaining help to recover his mental health? While she and their two children escaped to the United States in 2009 and live in California, Gao is under virtual house arrest at his sister-in-law's in China's far west. Dentists there do not have the means to repair the damage malnutrition did to his remaining teeth, and the government forbids him to travel to Beijing, much less to the United States to be reunited with his family.
Gao's advocacy for religious minorities led to his conviction in 2006 for "inciting subversion," and in 2007 he began serving a previously suspended three-year prison sentence. After he wrote an open letter to the U.S. Congress about human rights abuses in China, authorities abducted him and tortured him for more than 50 days. Gao later revealed his captors shocked his genitals with an electric baton and pierced them with toothpicks.
"As with the torture experienced during his pretrial detention, the purpose of this mistreatment was to extract a false confession," noted Freedom Now, which works to free prisoners of conscience.
Thugs suspected of being state agents again abducted Gao on February 4, 2009. He reportedly reappeared from March 28 to April 20, 2010, during which he described how police beat him for two days and nights, according to Freedom Now.
China announced on December 16, 2011, that it would take him to prison to serve the three-year sentence imposed in 2006, thus withdrawing the five-year probation. In prison since December 2011, Gao remained in isolation in a small cell with little light 24 hours a day, according to China Aid.
"Guards were strictly instructed not to speak with him," the advocacy group reported. "He was not allowed any reading materials, television, or access to anyone or anything. He was fed a single slice of bread and piece of cabbage, once a day; as a result, he has lost roughly 22.5 kilograms (50 pounds) and now weighs about 59 kilograms (130 pounds). He has lost many teeth from malnutrition. It is believed he was also repeatedly physically tortured."
"The only thing I feared more than him being killed was his suffering relentless and horrific torture and being kept alive," his wife told China Aid. "We desperately need help from our adopted country and from President Obama and Secretary Kerry personally to demand the Chinese government to allow my husband to come to the United States for medical treatment. If President Xi Jinping has any sense of decency or humanity, after crushing my husband both physically and psychologically, the least he could do is allow me as a devoted wife to care for him."
Jared Genser, head of Freedom Now, told China Aid, "The situation is far worse than my limited imagination enabled me to contemplate. While China is a great power in the 21st century, the inhumanity and brutality that it has demonstrated by the torture of Gao Zhisheng shows its profound insecurity and fear of anyone in its population who stands up to its repression."
by Morning Star News
(MorningStarNews.org)
From the Editor Nov/Dec 2014
Meet Me at the Manger
The True, Historical Jesus
More Than a Prophet
The Great Admission
A Heart for Our Needs
Inside View Nov/Dec 2014
Eye on the Middle East Nov/Dec 2014
Prelude to Apocalypse
World Watch List 2014
Can Three Be One?
The Tax Man Cometh
The Divine Shepherd of Israel
Up Close Among Suffering Nigerians
A Reason for Living
Hanukkah in Israel
Spiritual Discernment
The Wisdom of God Conclusion
Israel in the News Nov/Dec 2014
Apples of Gold Nov/Dec 2014
I don't often read fiction (unless it masquerades as news about Israel). But when Dan Brown's The Da Vinci Code came out in 2003, I decided to pick up a copy and see what all...
Lorna Simcox
Nestled in the terraced Shepherds' Fields on the approach to Bethlehem is a cave. I expect it is merely one of many where shepherds and townsfolk of bygone days found...
Bertrand Russell was a 20th-century British philosopher and logician who rejected the idea of absolute truth. In his famous 1927 essay "Why I Am Not a Christian," Russell wrote...
Patrick Neff
Many people believe Jesus was a good man and a prophet. Some will even admit He was the Son of God who came to Earth. But tell them Jesus was God Himself who appeared...
Charles McCracken
Messianic fervor hit a high throughout the Orthodox Jewish world in the early 1990s. Banners trumpeted messages like "Messiah Is Coming," "We Want Messiah Now," and...
Steve Herzig
Charles Haddon Spurgeon, a 19th-century, British Baptist preacher, opened his great Christmas Eve sermon published in 1914 with these words: "He was moved with compassion...
Peter Colón


The Promoter along with PAC has submitted to the Exchange a copy of Annual Disclosure under Regulation 30(1) and 30(2) of SEBI (Substantial Acquisition of Shares and Takeovers) Regulations 2011 as on March 31 2019.
Triveni Engineering & Industries Limited has informed the Exchange regarding `Scrutinizer Report in respect of business conducted through postal ballot process (including e-voting) as per Notice of Postal Ballot dated 13th February 2019 along with voting results`.
As required under Regulation 30(2) of the SEBI (Listing Obligations and Disclosure Requirements) Regulations 2015 (`Listing Regulations`) we submit herewith a copy of the Postal Ballot Notice dated 13th February 2019 together with annexures attached thereto including Explanatory Statement and Postal Ballot Form.
The voting period including e-voting commences on February 27 2019 (9:00 a.m. IST) and ends on March 28 2019 (5:00 p.m. IST). During this period the members of the Company holding shares either in physical form or in dematerialized form as on the cut-off date i.e. February 15 2019 may cast their vote physically or through e-voting platform of Karvy Fintech Pvt. Ltd. the Share Transfer Agents of the Company through their portal https://evoting.karvy.com. The result of the postal ballot shall be announced on or before March 30 2019.
Avadh Sugar & Energy Ltd.
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Außenlager Hirschberg – filia niemieckiego obozu koncentracyjnego Groß-Rosen w Jeleniej Górze na Dolnym Śląsku, jeden z licznych podobozów Gross Rosen.

Utworzony w maju 1944 roku po byłym obozie pracy zwanym SS-Sonderbauftrand działającym przy fabryce celulozy i włókien sztucznych (). Obóz męski dla więźniów żydowskich. W październiku 1944 roku do obozu trafiło 70 Żydów z Auschwitz-Birkenau. Na początku 1945 roku, w związku z likwidacją AL Bolkenhain, do obozu przybyło około 500 więźniów żydowskich. Ewakuację obozu rozpoczęto pod koniec lutego 1945 roku.

Gross-Rosen
Historia Jeleniej Góry

redpajama_set_name: RedPajamaWikipedia


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The discovery of the restoration of brain circulation hours post-mortem could change current paradigms of death criteria
//Transsexuality
Congregation's thoughts on Gender Ideology On 10 June this year, the Congregation for Catholic Education published a document entitled "Male and Female He Created Them" ( read HERE entire document), which sets out the Congregation's thoughts on Gender Ideology, and especially how...
American Governement protects conscientious objection in the field of abortion, sterilization and assisted suicide
Don't miss below video "1,300 complaints alleging discrimination in a health care setting on account of religious beliefs or conscience issues" (NHS official data) "Just today we finalized new protections of conscience rights for physicians, pharmacists, nurses,...
More problems associated with current gender transition therapy -hormone therapy
A recent study published in the American Heart Association's Journal Circulation provides new evidence of the risks posed by hormone therapies used as part of the treatments in gender transition processes (read HERE our report). The following text is exerted from Circulation...
Transgender thoughtpolice banned scientific research about people whith detransitioning. Why?
We posted 0n 28 Sep 2017 an article titled Bath Spa University – UK banned medical research to help people who decided to reverse their gender reassignment. We stated that James Caspian, a psychotherapist who specialises in working with transgender people, began the research...
Current treatment of transgender youth includes the suppression of puberty that has direct consequences on the development of the minor.
A relevant ethical, moral and legal medical unresolved issue is the current treatment suppressing puberty of diagnosticated transgender children. Has it direct consequences on the development of the minor? We extracted a topic from a peer-reviewed large Spanish study which make a...
Controversy on transsexuals' medical treatment. "I believe I'm proof no man can truly become a woman" warns Leanne.
Leanne is a transsexual who, at 34, had sex reassignment surgery — as it was then called — on the NHS at a clinic in Hove, East Sussex, after years of dressing sometimes as a man and sometimes as a woman. She is now 57 and says that, since then, she has lived in a twilight world...
Parents advised to be attentive to children's relationships to prevent rapid-onset gender dysphoria
"The influence of transgender friends or adults, directly or through social networks, could be an important factor for the onset of gender dysphoria in these young people" In a recent study published in PLOSONE , Dr. Lisa Littman of Brown University School of Public...
The biological sexual identity is once again adopted by the American Administration
Is US Government official definition of sexual identity determined "on a biological basis grounded in science" a violation of transgender person rights? WASHINGTON — The Trump administration is considering narrowly defining gender as a biological, immutable condition...
Have people the right to freeze their gametes with public funds?
Recently we have treated the new Western strong trend "Social freezing" that is also a profitable commercial issue (see HERE). Now we transcribe a recent news with a bioethical question. NHS England could face a legal challenge that would attempt to force clinics to...
LGB adults have more incidence of heart disease and strokes than their straight peers, according to a recent large study
LGB adults have more incidence of heart disease and stroke than their straight peers. The study presented at the American Heart Association's Epidemiology and Lifestyle conference in New Orleans, analyzed data collected from 2,445 adults participating in the 2011-2012 National...

redpajama_set_name: RedPajamaCommonCrawl


Macro arrangement that marks the points on the map.
Good morning. I had found a macro that marked the points on a map.
Currently it is no longer necessary for which it is necessary to fix the code.
If you have examples of better macros or that create a map inside the excel sheet, could you share it?
This is a fantastic macro. It deserves to be reviewed.


Amazing Image of Rustic Industrial Floor Lamp is one of several design collections from 19 Photos Designs Amazing Ideas rustic industrial floor lamp Industrial Floor Lamp Add the Wow Factor to Your Rustic Dcor which is one of the very popular designs of the year.Rustic Industrial Floor Lamp published on Monday, June 18, 2018 At 5: 45 pm.
We are have 19 beautiful pictures about Rustic Industrial Floor Lamp. We hope you enjoyed it and if you want to see the high pictures, simply just click the images and you will be redirected to extra large page of Rustic Industrial Floor Lamp.


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package org.apache.struts2.oval.interceptor;

import com.opensymphony.xwork2.ActionSupport;

import javax.persistence.Basic;

public class SimpleFieldJPAAnnotations extends ActionSupport {
    @Basic(optional = false)
    private String firstName;

    public String getFirstName() {
        return firstName;
    }

    public void setFirstName(String firstName) {
        this.firstName = firstName;
    }
}

redpajama_set_name: RedPajamaGithub


I just tried to download so e files I just did and it says there's damage on the one PER and then another says to upgrade my os, l new at this and it's confusing, please help.
Try to download the .pdf file again as there may be been some data corruption either in the download process or perhaps in the file itself. If it still fails, then if possible try to download the same file using another device, e.g. a pc etc and see if it still says that there is damage. If so then the file itself it faulty.
With regards to the upgrade message. That is to advise you that there is an updated version of the OS available for you to install in the tablet.
You do not have to do this unless you want to. It may be prudent to get more familiar with your tablet before attempting to upgrade the OS. It is normally a safe procedure but there is always the possibility of a problem.
In the future when you are more familiar with how your tablet operates you can always upgrade then. It may be also that you will be forced to upgrade, if a newly downloaded app doesn't function properly or if you desire a new feature that has become available due to the upgraded OS.
If you do wish to upgrade the OS be sure that before you do that you have made a backup of your tablet using the tablet's backup feature. That way you will have a copy of your data and downloaded apps etc in case the upgrade fails for whatever reason and you have to reset your tablet.
peggystaples1952 가/이 대단히 고마워 할 것입니다.


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Crowdsourcing Violence in Kashmir, Part 2
How terror groups in the Kashmir Valley use Burhan Wani's model to fuel a new wave of homegrown insurgents via social media
Security Social Media Terrorism
(Source: @Dfrkaul/DFRLab via Stocknap.io and Bannersnack)
This is the second article in a two-part series examining the use of social media to attract popular support for the insurgency in Kashmir. Part 1 discussed militant leader Burhan Wani's pioneering strategy; Part 2 discusses other terror groups' refinement of his model.
Kashmiri militant Burhan Wani's adept use of social media platforms paved the way for other Kashmiri separatist groups and militants who began to follow his example by sharing engagement-ready content with a large segment of the population.
Aside from the dissemination of propaganda, terrorist organizations (such as Wani's Hizbul Mujahidin) are also increasingly using social media platforms to coordinate with local supporters. This development has blurred the line between civilian and insurgent, thereby complicating counterterrorism efforts in the state.
Refining Wani's Model for Insurgency
Since Wani's death in July 2016 at the hands of Indian security forces, terrorist and militant organizations in the Kashmir Valley have refined the "freedom fighter" narrative initially popularized by Wani to attract average Kashmiri youth online to the insurgency. Subsequently, a majority of the militant groups operating in the valley have set up dedicated messaging groups on WhatsApp, Facebook, and Telegram to amplify their narrative and communicate instantaneously with a growing user base of Kashmiris on these platforms.
In addition to spreading broad anti-India narratives to radicalize the youth, militants also use social media platforms to relay information in real time, calling for their supporters to coordinate protests and disrupt ongoing security operations.
The Telegram channels and Facebook groups used by these groups and their supporters upload posts and stories showing alleged victims of police and military brutality in the valley. These posts attempt to portray civilian casualties and the killing of terrorists as a form of deliberate cruelty inflicted by the Indian state upon its victims. Those taking up arms against Indian security forces are characterized as fighting for the rights of the local population.
Photo uploaded on a Facebook group highlighting alleged human rights abuse by the Indian military. (Source: Pulwama Updates)
Posters created to exploit the narrative of human rights abuses carried out by the Indian military, shared on militant chat groups on Telegram. (Source: Telegram)
Posts on militant Telegram groups highlighting alleged human rights violations by the Indian army. (Source: Telegram)
By uploading photos and videos on Facebook and WhatsApp that showed him and his fellow militants' faces, Wani attempted to humanize the militants in the eyes of their audience. Other groups in the valley now routinely replicate this tactic in their Telegram channels, posting photos of current insurgents enjoying their lives and bonding with one another.
Photos uploaded on terrorist groups on Telegram attempting to humanize the insurgents by showing them bonding with one another. (Source: Telegram)
These photos bring a degree of relatability to the militants in the eyes of possible recruits. The use of Telegram channels in this manner has also allowed terrorists to communicate directly with prospective recruits.
Photos uploaded to militant group channels on Telegram portraying the insurgents as brothers-in-arms. (Source: Telegram)
These Telegram channels also posted content that glorified the insurgency as a pathway to celebrity. Members of these groups shared photographs of slain separatists, as well as of the crowds at their funerals, to suggest to possible recruits that they could attain fame and glory as well, even after their death.
Posts portraying slain terrorists as "martyrs" and highlighting the high attendance at funerals for terrorists killed by Indian security forces. (Source: Telegram)
Photographs showing the high attendance at militants' funerals uploaded to a Telegram channel. (Source: Telegram)
Burhan's Style of "Freedom Fighters"
The Burhan Wani model of social media insurgency allowed insurgents to gain widespread popularity among the local population of the valley. By using these platforms to further a narrative that highlighted alleged human rights abuses by the security forces while simultaneously framing terrorist and militant groups as "freedom fighters," Wani helped to normalize the violent aspects of the insurgency in the eyes of the wider population.
This development in turn promoted a growing legitimization of the insurgency within the educated classes and civil society of the valley. This trend is further reinforced by an investigation into sources of radicalization by police services. A study undertaken by the Kashmir police in 2015 examined the cases of 111 local Kashmiri youth who had joined the militant movement. Out of the 111 subjects (88 of which were between the ages of 15–30), 58 eventually returned home. According to the study, of the total subjects investigated by the police, more than 50 percent had been radicalized via consumption of terrorist propaganda disseminated over the internet. Once again, given the source of this study and the polarized nature of the narratives surrounding the conflict, this information should be read with some skepticism.
The upward trend in radicalization shows no sign of abating: as local media outlet The Economic Times recently reported, since March 2019, at least 50 young Kashmiri men have joined the insurgency.
Posts on Telegram groups providing sympathizers information about ongoing Cordon-and-Search Operations (CaSO), a military tactic employed by the Indian armed forces in which they close access to an area and extensively search it for weapons and insurgents. (Source: Telegram)
An investigation conducted by India's National Investigation Agency (NIA) identified 117 suspects who were using 79 WhatsApp groups containing a combined audience of 6,386 phone numbers to crowdsource local members of the public for stone-pelting Indian security forces at civilian protests.
Similarly, in 2017, Indian media outlet NDTV reported that more than 300 similar groups on WhatsApp had served as crowdsourcing channels for the purposes of hindering anti-terror operations in the state. In this manner, social media serves as a vehicle for Kashmiri civilians to play a direct role in active terror operations, which complicates the job of Indian security services.
Copycat Terror
In February 2019, Adil Dar, a 20-year-old local of South Kashmir and member of the banned terror group Jaish-e-Mohammed (JeM), drove a vehicle laden with explosives into an army convoy traveling through the Pulwama district of South Kashmir. The suicide attack, the deadliest in the last three decades of the insurgency, resulted in the death of 40 Indian paramilitary personnel. Dar uploaded content on social media under the moniker Waqas Commando right up until the terror attack. Prior to staging the bombing, he uploaded a video in which he pleaded with local youth, as Burhan Wani had done earlier, to "wage jihad against India."
Still from last video uploaded by Pulwama bomber prior to that attack. (Source: Telegram)
Taking the connection a step further, Indian media outlet The Economic Times also reported that in 2016, Dar had suffered a gunshot wound to the leg from security forces when participating in protests incited by the killing of Wani. The article also noted that Dar's parents later claimed that Wani's death was the pivotal event that lead their son to take up arms against the state.
Internet Shutdowns: A Short-Term Response
Given the pervasive nature of terrorist propaganda on social media platforms, the Indian government has taken drastic steps to curtail the amplification of such content. According to open-source data compiled by the India Internet Shutdown, an information portal run by the Software Freedom Law Centre in India, there have been 155 instances of a government blackouts of internet and mobile data services in Jammu and Kashmir since 2012.
Map showing the frequency of internet shutdowns across the country from 2012 onward. (Source: India Internet Shutdown)
Despite these efforts, Kashmiri researchers note that members of the terror groups have simply shifted to more secure platforms and the use of VoIP and VPNs to bypass these security measures and retain access to their contacts.
Internet blackouts cannot effectively combat this growing threat. Bereft of a systematic approach toward monitoring and countering the narratives furthered by terrorist propaganda, such groups will continue to gain support in the valley. As Khalid Shah, an associate researcher on Kashmir at the Observer Research Foundation, noted in an article published in the wake of the Pulwama bombing: until the Indian government implements an effective counternarrative, it cannot capture the "mind space" that fuels terrorism.
The DFRLab will continue to monitor the information environment in India, with an emphasis on issues at the intersection of national security, technology, and social media.


During school days/ college days after vacation my fellow friends were disappointed and bored at the thought of getting back to school or college. I used to pity the weeping kids being dragged to schools by their mothers on the first day of reopening. I used to wonder about the difference in reaction by me and others to the same event. I would have easily been bored with holidays and would be looking forward for the new class, new teachers, possibly new faces, new subjects and the joy of starting all over again, fresh.
Looks like I am having a delayed childhood.


Vianor makes sure that our customers can drive safely. For corporate clients, this means a safe partnership, and for motorists this means peace of mind on the road. Succeeding in this task is demanding. The teams in our outlets must be able to work well together and develop their competence continuously in order to ensure the safety of our customers and earn their trust. Their teamwork skills and competence are put to the test in the traditional Pitcrew Challenge, where teams compete against other Vianor outlets. This is just one of the many ways in which we are improving our competence and the ability to serve our customers.
All finalists must pass a tight preselection process that is conducted over the course of nearly one year. The outlets are benchmarked for quality, customer service and performance, and the most successful and best developed outlets send a team of four to the final. The final really tests the teams' co-operation skills, competence and ability to work under pressure. The best teams will receive motorists' dream prizes in an award ceremony, but perhaps their peers' respect is even more enjoyable for our competitive professionals.


Searching of the interaction pairs and organization of the interaction processes are important steps in molecular dynamics (MD) algorithms and are critical to the overall efficiency of the simulation. Neighbor lists are widely used for these steps, where thicker skin can reduce the frequency of list updating but is discounted by more computation in distance check for the particle pairs. In this paper, we propose a new neighbor-list-based algorithm with a precisely designed multilevel skin which can reduce unnecessary computation on inter-particle distances. The performance advantages over traditional methods are then analyzed against the main simulation parameters on Intel CPUs and MICs (many integrated cores), and are clearly demonstrated. The algorithm can be generalized for various discrete simulations using neighbor lists. (C) 2017 Elsevier B.V. All rights reserved.
GB/T 7714 Zhang, Chenglong,Zhao, Mingcan,Hou, Chaofeng,et al. A multilevel-skin neighbor list algorithm for molecular dynamics simulation[J]. COMPUTER PHYSICS COMMUNICATIONS,2018,222(00):59.
APA Zhang, Chenglong,Zhao, Mingcan,Hou, Chaofeng,&Ge, Wei.(2018).A multilevel-skin neighbor list algorithm for molecular dynamics simulation.COMPUTER PHYSICS COMMUNICATIONS,222(00),59.
MLA Zhang, Chenglong,et al."A multilevel-skin neighbor list algorithm for molecular dynamics simulation".COMPUTER PHYSICS COMMUNICATIONS 222.00(2018):59.


Ordering invitations for a wedding is not exactly rocket science. Yet if you have not done it before, it can be intimidating. Two terms that sometimes confuse first-time wedding planners are wedding reception invitations and wedding invitation templates. Cut down on event planning stress by learning about when and how to use them.
What are wedding reception invitations?
Getting married at a church but hosting a reception at a restaurant? With a ceremony and a party in different locations, wedding reception invitations give your guests the details that need to be in the right place at the right time. This itty-bitty card – usually about half the size of the ceremony invite – is included with the invitation, the reply card and, if necessary, the map card.
Wedding reception invitations could also be used as reception-only invitations. Whatever you got married in Las Vegas surrounded by a few friends or tied the knot in a private ceremony attended by the two of you and your kids, there are many reasons you might need to want to keep the marriage ceremony separate from the party.
The most important part of wedding reception invitations is the word you choose. Avoid embarrassing situations by clearly striking the invitation is for the reception only. Online wedding stationery websites and wedding planning sites usually offer word suggestions that will satisfy the manners maven in your family and prevent your "crazy" cousins from unintentionally crashing your intimate ceremony.
Find wedding reception invitations to fit any event style through online stationery specialists.
What are wedding invitation templates and when should I use one?
A template is a pattern for creating wedding invites, similar to the patterns you used to make aprons in high school home economics class. Templates allow you to print professionally designed stationery – from ceremony programs to map cards to wedding reception invitations– from a home computer.
1) Can it be customized? Some templates come as they are, so if you're looking to get creative be sure you can do so.
2) If it can be customized, what computer software do you need to alter it? Do not spend money purchasing a customizable template only to discover you do not have the software needed to change it.
While there are free printable wedding invitation templates available, you can also buy designs created by graphic artists, which means you get a professional look with a DIY price. Find high-quality wedding invitation templates through online wedding stationery printers.


Did Justice Scalia Display Anti-Gay Animus?
Ed Whelan, defender of all things Scalia and author of the "This Day in Liberal Judicial Activism" feature on National Review, is in the midst of a multi-post critique of my book (here, here and here).
Today's opinion is the product of a Court, which is the product of a law-profession culture, that has largely signed on to the so-called homosexual agenda, by which I mean the agenda promoted by some homosexual activists directed at eliminating the moral opprobrium that has traditionally attached to homosexual conduct.
To read Scalia's dissent in Lawrence and not feel the stinging homophobia in it is to be incapable of empathy and ignorant of the history of LGBT people in America.


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What NFL teams are looking for at Sam Darnold's pro day
One of the best pro days ever was Jamarcus Russell's. One of the worst? Peyton Manning's.
Yet USC quarterback Sam Darnold's pro day matters — at least, it does to NFL teams. Sure, pro days are just a sliver of the evaluation process for NFL draft prospects. But they aren't completely useless, and we're talking about a potential No. 1 pick here — a potential No. 1 pick with competition. It magnifies things a little more. Yes, scouts and front-office personnel have watched mountains of tape, talked to people who know the prospects they have their eyes on and sometimes even met with the prospects, either at the combine or on in-person visits. And quarterbacks? If a team is eyeing a quarterback in Round 1, it has done its homework.
If there's a question about Darnold, it's his delivery, which is more of a windup than the other top quarterbacks'. He has a quick release, but NFL coaches are going to want him to shorten that delivery. A windup, or elongated delivery, could matter for two reasons. One is delivery speed. That seems to be a lesser concern here. Darnold anticipates well and gets the ball out pretty quick. That said, a windup can expose the ball to pass-rushers — think of a ball behind your shoulder, where it can be swatted, as opposed to next to your head — and for a guy who has had turnover issues, that can stick out.
Q: Did things progress quickly during that visit?
AC: No, I mean, it was a long day just meeting everybody and watching film with the coaches and getting to know the program. It was a long day, but it worked out.
Q: How has having Erb's Palsy impacted you as a player? What sort of effect does it have on where you line up as a defensive lineman?
AC: I mean, I play the right side. That's where I've been playing for most of my career. I mean, it doesn't really affect me besides in the weight room with doing some stuff, but on the field, I mean, it doesn't really affect me. I've learned to compensate when I have to and I do what I've got to do to make the plays.
Q: Is it strange to be a member of the Patriots after being a member of the Falcons in Super Bowl LI?
AC: I mean, not really. I didn't play in that game, so it's not really a big thing to me. So, I'm just excited about a new opportunity and to get to continue my career.
Q: Did you know James Ferentz and Matt Tobin well when you played together at Iowa?
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40 pounds lighter since the season ended, Joe Hawley is likely moving on
The Buccaneers decided not to keep center Joe Hawley. Hawley apparently has decided not to keep playing football, in Tampa or anywhere.
Via Greg Auman of the Tampa Bay Times, Hawley said in a recent radio appearance that he has lost 40 pounds since the end of the season, and that he plans to give up his old life and embark on a new one.
That's because, this week, Romo is one of them.
The former quarterback, and now analyst for CBS, received a special exemption into this week's Tour event, opposite of the WGC-Dell Technologies Match Play Championship where most of the top 64 in the Official World Golf Ranking are playing.
Although it may be odd for the casual sports fan to see Romo's name in the field, his appearance in a professional golf event is not unprecedented.
Smith starred at weakside linebacker in Kirby Smart's 3-4 scheme. He made 252 tackles, 20.5 for loss, and 6.5 sacks. He is projected as a first-round pick.
I feel like I can make a tremendous impact on the defense, just with my playmaking ability, my leadership qualities, and everything that I possess as a football player on and off the field, Smith said. I feel like that will definitely elevate any defense.
Jerry Jones: Ezekiel Elliott paid most punishment I have seen for what he did
Cowboys running back Ezekiel Elliott has had a quiet offseason, much to the team's relief.
Everybody can follow along, and hopefully I can inspire people along the way to travel and live their dreams and go after what they want, Hawley said.
Hawley previously went after the dream of playing in the NFL, spending five years with the Falcons and three with the Buccaneers. It's now time for a new dream, and he'll be embarking on it in a new body, along with a new van.
As former Dallas Cowboys quarterback Tony Romo stood on the driving range of the PGA Tour's Corales Puntacana Resort & Club Championship earlier this week, the sound of the balls he hit was the same as the shots by golfers adjacent to him, according to those Tour professionals – guys who make their living, week in and week out, on the biggest stage in the sport.
This entry was posted in Cheap NFL Jerseys Usa and tagged Cheap Fishing Jerseys, Cheap Jerseys And Hats From China on April 20, 2018 by Baseball Jerseys Cheap.
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Source: Jarvis Landry-Jordan Howard trade a no-go
There's been talk of a trade between the Dolphins and Bears, sending Jarvis Landry to Chicago and Jordan Howard to Miami. But we hear it's nothing more than talk.
A league source tells PFT there's no way it's happening.
Landry is currently franchised by the Dolphins, and they are looking into trading him. The Bears have been floated as a possible destination, but it won't be for Howard.
Fitzpatrick expects to return to Arizona this summer to learn from Peterson some more.
Fitzpatrick, projected as a high first-round pick, can play anywhere in the secondary after spending much of his time as a slot corner for Alabama. He said some teams are asking him about playing corner, and others see him at safety.
For this weekend, I think it will show people I have the hips and feet of a corner, also the IQ and the tackling ability of a safety, Fitzpatrick said. I think that's really important to show coaches who are out there doing my drills. Then I think going into the draft, they know I can play multiple positions at a high level. Not just playing there but also at a high level.
Born with amniotic band syndrome, a disease that prevented the fingers on his left hand from fully developing, he required amputation of his left hand when he was 4.
Griffin's reps tied for 16th among participating linebackers.
The Packers examined my shoulder on my visit March 10 and cleared it, he wrote on Instagram. They even gave me an X-ray as well. It got worse during the season, specifically against the [Dallas] Cowboys, so I asked to have it checked out, and we checked it. After a few days of contemplating to play with it or get surgery, I chose surgery. Now here we are.
Yet after the New England Patriots claimed him off waivers, Bennett reversed course and attempted to play through the injury. He made six catches for 53 yards across two games before landing on injured reserve.
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text:
16 entries found
08 Sep 2015 description
Global Emergency Overview Snapshot, 2 - 8 September 2015
report — Assessment Capacities Project
Snapshot 2–8 September 2015
Yemen: The health system in Taizz governorate is close to collapse. All public hospitals have closed, and the remaining health facilities are overwhelmed by severely injured people as well as a dengue outbreak. Access remains severely restricted across the country. Hudaydah port, the main entry point for humanitarian supplies in north and central Yemen, remains closed, and road transport from Aden port to northern governorates remains limited.
Global Emergency Overview Snapshot, 25 August - 1 September 2015
Snapshot 25 August–1 September 2015
Papua New Guinea: 1.8 million people have been affected by prolonged dry spell and frost in the Highlands region; 1.3 million are reported to be most at risk. Crops have been destroyed, and several chools and health facilities have been closed due to water shortages. The affected population is reported to be resorting to less reliable sources of drinking water.
Global Emergency Overview Snapshot, 11 - 25 August 2015
Snapshot 11 August – 25 August 2015
Haiti: Insecurity has increased since legislative elections. Violence and intimidation were reported at many polling stations and a second round of voting is planned, following low voter turnout. Food security has deteriorated as a result of prolonged drought conditions since the beginning of 2015: poor households in Sud, Sud-Est, Nord-Est and Artibonite will remain in Crisis (IPC Phase 3) food security outcomes through December. Recent cholera rates are triple those of the comparable time period in 2014.
Snapshot 12 August –18 August 2015
Yemen: The humanitarian situation in Yemen continues to deteriorate. 1.4 million people have become displaced since conflict escalated in March – a 12% increase since early July. Fuel shortages and access issues continue to affect provision of health services. 23% of Yemen's health facilities are either partially funtional or non-functional.
Global Emergency Overview Snapshot, 5 - 11 August 2015
Snapshot 5-11 August 2015
Burkina Faso: Heavy floods in Ouagadougou, Kadiogo province, and Bobo-Dioulasso, Houet province, in early August affected around 19,780 people. Significant damage to houses and food stocks were reported. Additional flooding in the north could bring the total number of affected to 122,000. More than 1.5 million people are facing Stressed or Crisis food security outcomes in Burkina Faso, especially in the Sahel region in the north.
Libya: Concern is growing for the increasing number of people affected by crisis since mid-July, as violence persists, rival governments are failing to assure basic services, and most humanitarian organisations have withdrawn.
Syria: Only 41% of Syria's public hospitals are fully operational. The latest in a number of local truces around Damascus has been agreed between state forces and opposition in Qadam. 191,369 people were reported killed March 2011–April 2014, mainly in Rural Damascus, Aleppo, Homs, Idleb, Dar'a and Hama, according to new UN figures.
Snapshot 13-19 August
Yemen: The 9 August Al Jawf ceasefire has been broken. Access to people affected by the conflict in Al Jawf is extremely limited due to persistent insecurity, and it is very difficult to obtain information. Almost 3,000 people have died in violence since the National Dialogue Conference took place on 25 January.
Global Emergency Overview Snapshot, 30 July - 5 August 2014
Snapshot 30 July–5 August
OPt: As a 72-hour truce begins, 1,179 civilians have been reported killed since Operation Protective Edge started. A third of the population of the Gaza Strip – 485,000 people – have been displaced, an increase of 270,000 since last week. Most IDPs are staying in schools, which are severely overcrowded. The health system is overwhelmed.
Global Emergency Overview Snapshot, 9 - 15 July 2014
Snapshot 9–15 July
oPT: 178 Palestinians have been killed since the launch of Israel's Operation Protective Edge on 8 July. Around 17,000 people have sought shelter in UNRWA schools. Rockets from Syria and Lebanon have hit the north of Israel, raising fears of the conflict spreading.
Democratic Republic of Congo: More than 30,000 people are estimated to have been displaced in North Kivu, South Kivu, and Katanga in June, due to FARDC military operations and fighting between armed groups.
Global Emergency Overview Snapshot, 2 - 8 July 2014
Pakistan: Water, sanitation, and health services are urgent needs among the 780,000 registered displaced from North Waziristan (government figures). The data is being cleaned to check for duplication.
Iraq: Access to areas within the governorates of Anbar, Babylon, Diyala, Salah al Din, Kirkuk, and Ninevah remains difficult due to ongoing violence clashes, disruption of communication and transportation routes, and a widespread shortage of fuel.
03 Jun 2014 description
Global Emergency Overview Snapshot, 28 May - 3 June 2014
CAR: The security situation in Bangui has reportedly deteriorated; 25 have been killed in renewed clashes. Violence has disrupted the April–May planting season, which will likely lead to below-average 2014–2015 harvests.
Syria: 241,000 people are estimated to be living under siege, 196,000 besieged by government forces, and 45,000 by opposition forces. Nearly 2,000 civilians are reported to have been killed in air strikes on Aleppo this year. Humanitarian access to both government and opposition controlled areas dropped significantly in May.
27 May 2014 description
Global Emergency Overview Snapshot, 21 - 27 May 2014
Balkans: On 13 May, cyclone Tamara hit the Balkans. Heavy rainfall resulted in extensive flooding in Serbia, Bosnia and Herzegovina, and Croatia; 1.6 million, 1.5 million, and 38,000 people have been affected, respectively. In total, 81,879 people have been evacuated. Relief efforts are being hampered by landslides, damaged infrastructure, blocked roads, and blackouts.
South Sudan: A cholera outbreak was reported in Juba, with 43 suspected cases and two deaths recorded. Displacement figures have climbed to 1,005,000 IDPs and 310,000 refugees in neighbouring countries. Juba and the South Sudan Democratic Movement/Army – Cobra Faction signed a peace agreement over conflict in the Greater Pibor area.
Iraq: 6,000 people fled the Iraqi military's shelling of Fallujah over 6–16 May. The Iraqi Government has denied using barrel bombs, but residents keep describing what appear to be such devices.
Global Emergency Overview Snapshot, 7 - 13 May 2014
South Sudan: Peace negotiations in Addis Ababa have resulted in a ceasefire agreement between South Sudan's president and the head of the opposition. The number of IDPs in South Sudan stands at 983,000. Following fighting in Upper Nile state, at least 11,000 new South Sudanese refugees have crossed into Ethiopia, bringing the total to 120,000. Altogether, 341,000 South Sudanese refugees are in neighbouring countries.
23 Apr 2014 description
Global Emergency Overview Snapshot, 16 - 23 April 2014
Snapshot 16–23 April
Central African Republic: Renewed clashes between anti-balaka and Seleka fighters occurred in several locations in central, northern, and southwestern provinces. MISCA soldiers are being redeployed to cover areas previously secured by the Chadian contingent. A Christian religious leader was killed and four were abducted in two northern towns, while 30 Christian civilians were reportedly killed in a central town.
Afghanistan16
Angola16
Bolivia (Plurinational State of)10
Burkina Faso12
Burundi12
Cameroon14
Central African Republic (CAR)16
Democratic People's Republic of Korea (DPRK)16
Democratic Republic of the Congo (DR Congo)16
Djibouti11
Eritrea16
Ethiopia16
Gambia16
Guinea16
Haiti16
Jordan16
Kenya16
Lebanon15
Liberia11
Malawi14
Mali16
Mauritania16
Niger16
Nigeria16
occupied Palestinian territory (oPt)16
Philippines15
Sierra Leone11
Somalia16
South Sudan16
Sudan16
Syrian Arab Republic16
Uganda13
Yemen16
Assessment Capacities Project (ACAPS)16
Academic and Research Institution16
Logistics and Telecommunications
Peacekeeping and Peacebuilding
Climate Change and Environment2
Coordination2
Food and Nutrition16
HIV/Aids13
Humanitarian Financing1
Mine Action12
Protection and Human Rights16
Recovery and Reconstruction9
Safety and Security14
Shelter and Non-Food Items13
Water Sanitation Hygiene16
Cold Wave4
Drought16
Epidemic16
Flash Flood16
Flood16
Insect Infestation2
Land Slide16
Mud Slide4
Severe Local Storm8
Storm Surge13
Tropical Cyclone16
IDPs16
Refugees16


text:
Q: Vue.js Axios bug HTTP request change my array but don't show change I have a very strange problem in vue.js/axios.
Scenario 1 : clear my products variable BEFORE send an HTTP request (see "<<<<< SCENARIO 1" mark). Then set products variable with a new array.
It works but we see a flicker (due to the HTTP request duration).
So I decided to clear the products variable IN the request.
Scenario 2 : clear my products variable IN the HTTP request. (see "<<<<< SCENARIO 2" mark).
But I don't know why in Scenario 2 : my products variable is modified but the View don't change ! So my product variable has 3 products with related quantity. Then quantity of one product change so I clear the product variable and refresh with the HTTP request. All is the same but quantity of 1 product has changed. But the view don't reflect this !
let Cart = {

    components: { Product },

    data: function() {
        return {
            products: []
        }
    },

    template: "

Cart:
" +
        '<product @productChanged="updateProductsCart(product)"' +
        'style="display: inline-block; max-width: 90px;" v-for="product in products"' +
        ':id="product.id" :name="product.name" :priceWithCurrency="product.priceWithCurrency"' +
        ':initQuantity="product.initQuantity" :picture="product.picture" :hasDeletedBtn="true"' +
        ':isProductRefreshAuto="false"></product>' +
    "
",

    methods: {

        getAllProducts: function () {

            let $this = this;
            $this.clearProductsList();<<<<< SCENARIO 1

            tdtdapi.get( '/cart/products/me', configs

            ).then(function (response) {

                $this.clearProductsList();<<<<< SCENARIO 2

                console.log("getAllProducts.then >")
                console.log(response)
                let products = [];

                for( let i = 0, l = response.data.length; i < l; i++ ){
                    let product      = response.data[i],
                        productToAdd = {
                            "name": "Product ",//todo delete raw value
                            "priceWithCurrency": 45
                        };
                    //todo: create a class Product
                    for( let prop in product ){
                        if( prop === "product" )     productToAdd.id = product[prop];
                        if( prop === "name" )        productToAdd.name = product[prop];
                        if( prop === "quantity" )    productToAdd.initQuantity = product[prop];
                        // if( prop === "description" ) productToAdd.description = product[prop];
                        if( prop === "price" )       productToAdd.priceWithCurrency = product[prop];
                        if( prop === "picture" )     productToAdd.picture = product[prop];
                    }
                    products.push(productToAdd);
                }

                $this.setProducts(products);

            }).catch(function (error) {
                console.log(error);
            });
        },

        updateProductsCart: function( product ) {
            console.log("updateProductsCart >")
            console.log(product)
            this.getAllProducts();
        },

        setProducts: function(products) {
            console.log("setProducts >")
            console.log(products)
            this.products = products;
            console.log(this.products)
        },

        clearProductsList: function() {
            this.products.splice( 0, this.products.length );
        }
    },

    mounted() {
        this.getAllProducts();
    },

    computed: {

    }
};

var app = new Vue({
    el: "#app",

    components: {
        "ProductsList": ProductsList,
        "Cart": Cart
    }
});

There is the Product component if that help :
let Product = {

    data() {
        return {
            quantity: this.initQuantity,
            price: this.getPriceWithoutSymbols()
        }
    },

    props: {
        id: { type: Number, required: true },
        name: { type: String, required: true },
        description: { type: String, default: "" },
        priceWithCurrency: { type: Number, required: true },
        initQuantity: { type: Number, default: 0 },
        picture: { type: String, default: "" },
        hasDeletedBtn: { type: Boolean, default: false },
        isProductRefreshAuto: { type: Boolean, default: true }
    },

    template: '
'  +
    '
{{ name }}
' +
    '
{{ description }}
' +
    '
{{ price }}
' +
    '

' +
    '
Quantity: {{ quantity }}
' +
    '
Total for this product: {{ totalPrice }}
' +
    '
' +
    '<button @click="decrementQuantity" type="button">-</button>' +
    '<button @click="incrementQuantity" type="button">+</button>' +
    '
<button v-if="hasDeletedBtn" @click="deleteProductQuantity" type="button">Delete product</button>' +
    '
' +
    '
',

    methods: {

        addQuantity( valueToAdd ){

            //if quantity 0 to 1 ==> post
            if( (this.quantity === 0) && (valueToAdd >= 1) ){
                this.postProductQuantity(valueToAdd);
            }

            //if quantity 1 to 0 ==> delete
            else if( (this.quantity === 1) && (valueToAdd === -1) ){
                this.deleteProductQuantity();
            }

            //else ==> put
            else{
                this.putProductQuantity(valueToAdd);
            }
        },

        postProductQuantity(valueToAdd){
            console.log("POST")
            let $this = this;
            tdtdapi.post( '/cart/products/me', querystring.stringify({
                    product: $this.id,
                    quantity: valueToAdd
                }), configs
            ).then(function (response) {
                console.log(response);
                $this.setQuantity(response.data.quantity);
            }).catch(function (error) {
                console.log(error);
            });
        },

        putProductQuantity(valueToAdd){
            console.log("PUT")
            let $this = this;
            tdtdapi.put( '/cart/products/me', querystring.stringify({
                    product: $this.id,
                    quantity: ($this.quantity + valueToAdd)
                }), configs
            ).then(function (response) {
                console.log(response);
                $this.setQuantity(response.data.quantity);
            }).catch(function (error) {
                console.log(error);
            });
        },

        deleteProductQuantity(){
            console.log("DELETE")
            let $this = this;
            tdtdapi.delete( '/cart/products/me/' + this.id, configs
            ).then(function (response) {
                console.log(response);
                $this.setQuantity(0);//todo: use v-show to hide product when (this.quantity === 0)
            }).catch(function (error) {
                console.log(error);
            });
        },

        emitChanged() {
            this.$emit( "productChanged" );
        },

        incrementQuantity(){
            this.addQuantity(1);
        },

        decrementQuantity( product ){
            console.log(product)
            // if( this.quantity >= 1 ){
            //     this.addQuantity(-1);
            // }
        },

        getPriceWithoutSymbols(){
            //todo: if price contains currency, when need to get only the value
            return this.priceWithCurrency;
        },

        setQuantity( quantity ){
            if( this.isProductRefreshAuto ){
                this.quantity = quantity;
            }
            this.emitChanged();
        }
    },

    computed: {
        totalPrice: function(){
            return (this.quantity * this.price).toFixed(2);
        }
    }
};

A: One error I see is, you have props in camelCase such as priceWithCurrency, for these props, you have to use kebab-case when passing in the template as explained here:
template: "

Cart:
" +
    '<product @product-changed="updateProductsCart(product)"' +
    'style="display: inline-block; max-width: 90px;" v-for="product in products"' +
    ':id="product.id" :name="product.name" :price-with-currency="product.priceWithCurrency"' +
    ':init-quantity="product.initQuantity" :picture="product.picture" :has-deleted-btn="true"' +
    ':is-product-refresh-auto="false"></product>' +
"
",

A: The problem is that we must refresh the data of Product with the props.
Basically when the parent (here the Cart component) change the quantity of Product with the props (here initQuantity), we must say to Product instance that he must change is data (here quantity) with his props (initQuantity).
So we must add a watch at the end of Product component :
    computed: {
        ...
    },

    watch: {
        initQuantity( newQuantity ){
            this.quantity = newQuantity;
        }
    }

I found my answer here

redpajama_set_name: RedPajamaStackExchange


Not surprisingly there are always a few searches for pork (esp. geera pork). Although this is a Trini cooking site it is also a kosher one, so there won't be any recipes prepared here for exclusively pork dishes. I don't worry too much about this omission as there are recipes for these things floating on the net and I think the quality of this site is high enough to make up for the absence of the occasional treif product. However, not all of my omissions are due to religious/dietary restrictions.
The other day I noticed a lot of searches for oxtail. Just reading the word makes me shudder all over. That's one ingredient/dish that I've never been able to stomach (figuratively and literally). The smell, the sight, the texture.. ack ack ack, it's enough to make me leave a room 😥 So no… there won't be any oxtail recipes proliferating here either, however in the glorious array that is the internet many other recipes do abound, including this one for oxtail stew with butter beans. Feel free to check it out!


Large DNA viruses are a source of transport proteins with minimal structure and robust function. In the first part I characterized two new variants of the K+ channel Kcv. The two Kcvs, namely KcvSmith and KcvNext-to-Smith, have a monomer size of only 82 amino acids, but exhibit most of the hallmarks of K+ channel pores, i.e. two transmembrane domains (TMs), a pore region and a selectivity filter, with the conserved sequence TxxTxGYGD. The two channels differ in 11 amino acids with most of the differences in the outer and the inner TM. Both channels are fully functional with selectivity for K+; they also conduct Rb+ and NH4+, but no Na+ and Li+. The selectivity of the two channels differs, even though they have an identical filter region. Mutational studies revealed that an exchange of a single amino acid in the outer TM already changed in KcvNext-to-Smith the selectivity for K+ and Rb+ towards the selectivity of KcvSmith, implying a relevance of the outer TM for selectivity. The two channels are sensitive to Ba2+ and Cs+, but not to TEA or amantadine. Both channels are fully blocked by Ba2+ and the responsible binding site for Ba2+ in the filter region could be identified by site-directed mutagenesis. Most notable is the difference in the mode of Cs+ block. While KcvSmith was blocked is a moderate voltage-dependent manner, KcvNext-to-Smith showed an extremely steep block with complex kinetics. Again, mutational studies revealed the relevance and sensitivity of the amino acid composition in the outer TM for the block. The second protein of interest is a putative K+ transporter encoded by virus Fr483. Analysis of the sequence revealed high similarity to plant potassium transporters including a conserved putative signature sequence; topology prediction algorithms revealed structural similarity with known K+ transporters. Yeast complementation assays and Rb+ uptake experiments have shown that the transporter protein is functional. Northern blot hybridization confirmed that the transporter gene is expressed during the infection cycle. The function of the protein is yet unclear. Overall, this is the first functional potassium transporter encoded by a virus. In the third part, we made phylogenetic analyses together with the group of Prof. Hamacher (TU Darmstadt). The generated trees show that K+ channels from the alga Chlorella NC64A are most distantly related to channels of viruses, which infect it, thus, they were most likely not acquired from the hosts. By generating a consensus sequence of the viral channels we also found a bacterial protein, which has high sequence similarity to KcvATCV-1, but is probably not a K+ channel. Overall, it is not clear from were the chlorella viruses acquired their channel proteins, and it is possible that they are even the architects of these.


South African design exports – ranging from recycled bottle top mats to bathplug chain chandeliers – are being snapped up from Mumbai to Hong Kong and are increasingly contributing to local job creation and wealth generation, says Elle Decoration magazine.
According to Department of Trade and Industry estimates, South Africa's craft sub-sector alone contributes about R2-billion or 0.14% to South Africa's gross domestic product (GDP) annually, providing jobs and income for around 38 000 people through at least 7 000 small enterprises.
"Crafts could contribute R5-billion to the country's GDP and 20 000 more jobs by 2015 if supported by more targeted interventions," Elle Decoration said in a statement last month.
The local EDIDA winners will compete with designers from 22 other countries for the opportunity to strut their stuff at the 48th Milan Furniture Fair in April.
Roos, who headed up the EDIDA South Africa judging panel, said all the 2007 winners' products were "well produced, of high quality, with global appeal." A sampling of the South African winners also reveals numerous export success stories.
The SA Designer of the Year, Tonic Design Studio in Johannesburg, supplies furniture to designers and retailers in Europe, the US and Africa, as well as handling numerous large-scale projects locally and abroad, plus retail and restaurant design.
TeamTwo co-director Sian Eliot, whose company won the 2006 and 2007 EDIDA lighting awards, says their Faraway Tree design has been ordered en masse by the Fairmont Hotel in San Francisco, with inquiries by interior decorators from Stockholm to Bombay. There has been huge Far East interest after their products were showcased in an international Hong Kong catalogue after the 2006 EDIDA award.
TeamTwo has also exported products via the upscale Amaridian Gallery in New York, British lighting outlet Cameron Peters, and Spanish distributor Swalaline, which specialises in distributing Southern African pieces to Europe.
Helon Melon, which won the bedding category for metallic embroidered linen, has supplied Selfridges in the UK and sells to boutique stores from Kuwait to the US. Foreign customers, mainly German, e-mail founder Helen Gibbs every year to order their linen for collection in Cape Town on their annual holiday.
After years of selling small quantities to foreign outlets, she hopes to open a fully representative franchise outlet later this year in Guildford, England that will stock all her designs generated over the past 13 years.
The fabric sector winner, Afro, has products like scatter cushions and tote bags selling from Cape Town to Salzburg.
Heath Nash, who won the flooring section for his mats made from recycled cooldrink bottle tops, showed at London Design Week and supplies numerous international outlets like Isandi in Norway.
Seating prizewinners Greg and Roche Dry report strong export sales for their hanging swing seat, inspired by a trip to the park with their daughter. The swings and the rest of their product range – from furniture to lamps – are selling briskly in the US and elsewhere, following coverage in international magazines like Surface, favourable blog mentions and exposure at Amaridian Gallery in New York.
Tableware and accessories winner Frauke Stegmann focuses on small, custom-designed contracts and her work will shortly be included in a new book showcasing the world's top young designers. Her products have been exposed to overseas buyers through several channels: New Africa in Denmark, Anthropologie in New York, Super Design Market and Handled with Care at 100% Design London and 100% Designers at 100% Design Tokyo.
Maira Koutsoudakis of Life Interiors+Architecture+Design tends to design pieces for her luxury eco-resort and boutique hospitality projects, after which they become part of her stable of products. Many are exported to Paris, London, Tokyo and Berlin and also to the Seychelles, where she has a resort store.
Her "Wodaabe" vessels and "Pod" lights, both former EDIDA winners, are not only popular in South Africa but also Europe and the US. The "Himbasin" that won her the 2007 EDIDA bathroom award, with its shallow, water-efficient dune-like shape in solid hand-beaten copper, was conceptualized for her latest project, Serra Cafema, an eco-friendly luxury lodge in the Namibian desert.
Tattoo, launched only last year at Decorex by set designers and builders in the film industry Claire Letoret and Tracey Collis, reports plenty of overseas enquiries about the anthropomorphic Luigi multi-purpose storage unit that snapped up the EDIDA kitchen prize. While no export deals have yet been concluded, queries have come from Australia, the US, France and Dubai.


text:
\section{Equivalence of the time evolution and Rindler frame transformation}
The time evolution under the Hamiltonian $\mathcal H=i\hbar\sum_k g_k(a^\dagger_k a^\dagger_{-k}-a_k a_{-k})$ can be solved analytically by equations of motion in the Heisenberg picture,
\begin{align}
\dot{a}_k &= \frac{i}{\hbar}[H,a_k] = g_k a^{\dagger}_{-k}\\
\dot{a}_{-k} &= \frac{i}{\hbar}[H,a_{-k}] = g_k a^{\dagger}_k.
\end{align}
Then we get the expressions for the time evolution of the operators as
\begin{align}
\begin{bmatrix}
a_k(\tau)\\
a_{-k}^{\dagger}(\tau)
\end{bmatrix}
= \begin{bmatrix}
\cosh(g_k\tau) &\sinh(g_k\tau)\\
\sinh(g_k\tau) &\cosh(g_k\tau)
\end{bmatrix}
\begin{bmatrix}
a_k(0)\\
a_{-k}^{\dagger}(0)
\end{bmatrix}.
\label{eqM3}
\end{align}
This result shares the same form of the Bogoliubov transformation which is related to the spontaneous particle creation from the vaccum, the Hawking-Unruh effects and the squeezed states of light.

On the other hand, if we look at the problem of boosting a quantized scalar field into an accelerating frame with acceleration $A$, it can be realized by the Rindler transformation \cite{Su2016} as
\begin{align}
\begin{bmatrix}
\hat{b}^{R}_{\omega}\\
\hat{b}^{\dagger L}_{\omega}
\end{bmatrix}
=
\begin{bmatrix}
\cosh(r_{\omega}) &\sinh(r_{\omega})\\
\sinh(r_{\omega}) &\cosh(r_{\omega})
\end{bmatrix}
\begin{bmatrix}
\hat{c}_{m\omega}\\
\hat{d}^{\dagger}_{m\omega}
\end{bmatrix},
\label{eqM4}
\end{align}
where $(\hat{b}^{R}_{\omega},\hat{b}^{L}_{\omega})$ are the annihilation operators in the accelerating frame, $L$ and $R$ correspond to two Rindler wedges propagating along two different directions, $(\hat{c}_{\omega}, \hat{d}_{\omega})$ are the annihilation operators of Unruh modes whose vacuum is the Minkovski vacuum in the inertial frame. The parameter $r_{\omega}$ satisfies the equation of $\tanh r_{\omega} = e^{-\pi\omega c/A}$.

We compare Eq. (\ref{eqM3}) with (\ref{eqM4}) and find the similarity in their expressions. The equivalence can be built by treating the operators at time $ \tau$ as the Rindler operators in a non-inertial frame, which leads to $g_k\tau = r_{\omega/2}$. Thus, we obtain
\begin{equation}
g_{k} = \frac{1}{2\tau}\ln\coth(\frac{\pi\omega c}{4A}),
\label{gk}
\end{equation}
corresponding the coupling strength of mode $k$ generating the Unruh radiation in the frequency component $\omega/2$.

\section{Hamiltonian and evolution of the condensate with a modulated interaction}
We start with the second quantization process of the Hamiltonian
\begin{equation}
H=\int d^3\bold{r}\Psi^\dagger(\bold r,t)\frac{p^2}{2m}\Psi(\bold r,t)+{\tilde g(t)\over 2}\int d^3\bold{r}\Psi^\dagger(\bold r,t)\Psi^\dagger(\bold r,t)\Psi(\bold r,t)\Psi(\bold r,t),
\end{equation}
where $\tilde g(t)=4\pi\hbar^2a(t)/m$ is the coupling strength and proportional to the scattering length $a(t)$.
In a driven condensate, the scattering length is in the form of $a(t)=a_{dc}+a_{ac}\sin(\omega t)$, where $\omega$ is the modulation frequency. By applying the Fourier transformation of the field operator
\begin{equation}
\Psi(\bold r,t)={1\over\sqrt V}\sum_k e^{i\bold k \bold r} a_{\bold k},
\end{equation}
where $V$ is the volume of the condensate, we obtain the Hamiltonian in the momentum space as
\begin{equation}
H=\sum_{\bold k}\epsilon_k a_\mathbf{k}^\dagger a_\mathbf{k}+ {\tilde g(t)\over 2V}\sum_{\bold k_1,\bold k_2,\Delta\bold k}a^\dagger_{\bold k_1+\Delta \bold k}a^\dagger_{\bold k_2-\Delta \bold k}a_{\bold k_1}a_{\bold k_2}.
\end{equation}

By entering the interaction picture and eliminating $H_0=\sum_{\bold k}\epsilon_k a_\mathbf{k}^\dagger a_\mathbf{k}$, we simplify the Hamiltonian under the rotating wave and Bogoliubov approximations and only keep the resonant terms. Then the interaction Hamiltionian becomes
\begin{equation}
    H = i\hbar g \sum_{|\mathbf{k}|=k_f}(a_k^\dagger a_{-k}^\dagger-a_k a_{-k}),
\label{Two-mode}
\end{equation}
where $g = \pi\hbar N_0 a_{ac}/mV$ and $k_f = \sqrt{m\omega/\hbar}$.

According to Eq. \eqref{eqM3}, we know the evolution of the operators as
\begin{align}
\begin{bmatrix}
a_k(\tau)\\
a^{\dagger}_{-k}(\tau)
\end{bmatrix}
=
e^{g\tau\sigma_x}
\begin{bmatrix}
a_k(0)\\
a^{\dagger}_{-k}(0)
\end{bmatrix}.
\end{align}
where $\sigma_x$ is the x-component of Pauli matrices. In order to simulate the Rindler transformation, we have to match the form of Eq. (\ref{eqM4}) and obtain the simulated acceleration $A$ as
\begin{equation}
A = {\pi\omega c\over 2\ln\coth(g\tau)}.
\end{equation}

The mean population per mode increases as $\Bar{n} = \langle a^{\dagger}_k(\tau) a_k(\tau) \rangle = \sinh^2(g\tau) $. Thus, $A$ can be characterized by the mean population per mode $\bar n$ as
\begin{equation}
    A = \frac{2\pi c E_{k_f}}{\hbar \ln(1+1/\bar n)}\xrightarrow[\bar n \gg1]{} \frac{2\pi cE_{k_f}}{\hbar}\bar n,
    \label{eq13}
\end{equation}
where $E_{k_f} = \hbar\omega/2$ is the kinetic energy of each atom.

Now, let's consider the evolution of the wave function instead of the operators. Two counter-propagating modes with momentum $k$ and $-k$ are generated together and we have to consider them at the same time. By grouping $k$ and $-k$ together, we decompose the Hamiltonian into $H=\sum h_k$, where $h_k=i\hbar g(a_k^\dagger a_{-k}^\dagger-a_k a_{-k})$. Then we only need to consider the evolution of each $h_k$. To simplify the notation without loss of the generality, we use $h$ to replace $h_k$. Therefore, the evolution of the wave function can be written as \cite{wang2007}
\begin{equation}
    \ket{\psi(\tau)} = e^{-i h\tau/\hbar}\ket{0}
    =\frac{1}{\cosh(g\tau)}\sum_{n=0}^{\infty}\tanh^n(g\tau)\ket{n,n}.
\end{equation}
The wave function matches the Minkovski vacuum expanding in the basis of the Rindler frame \cite{Wald1994}. The density matrix of one single mode such as $k$ is determined by tracing out the other mode $-k$, \textit{i.e.}
\begin{equation}
    \hat\rho_k (\tau) = \mathrm{Tr}_{-k}{\ket{\psi(\tau)}_I\bra{\psi(\tau)}_I} = \sum_{n=0}^{\infty}p_n\ket{n}_k\bra{n}_k
\end{equation}
where $p_n= \tanh^{2n}(g\tau)/\cosh^2(g\tau)$. By comparing with a thermal distribution of an ideal Bose gas
\begin{equation}
\tilde p(T)=e^{-{n\hbar\omega\over 2k_\mathrm{B}T}}(1-e^{-{\hbar\omega\over 2k_\mathrm{B}T}}),
\end{equation}
we can build a direct mapping between the effective temperature with the time $\tau$ or the mean population $\bar n$ as
\begin{align}
T &= \frac{E_{k_f}}{2k_\mathrm{B}\ln\coth(g\tau) } \\
&= \frac{E_{k_f}}{k_\mathrm{B}\ln(1+1/\bar n)} \xrightarrow[\bar n \gg 1]{}\frac{E_{k_f}}{k_\mathrm{B}}\bar n.
\label{eq17}
\end{align}
where the mean population
\begin{align}
    \bar n = \sum_{n=0}^{\infty}np_n = \frac{1}{e^{E_{k_f}/k_{\mathrm{B}}T}-1}
\end{align}
follows the Bose-Einstein statistics.

We also characterize our system by the entropy $S$. The von Neumann entropy of the thermal distribution is
\begin{align}
S =& -k_{\mathrm{B}}\mathrm{Tr}\left(\hat\rho_k\ln\hat\rho_k\right)\nonumber\\
=&k_{\mathrm{B}}[\ln\Bar{n}+(\Bar{n}+1)\ln(1+1/\Bar{n})],
\label{eq16}
\end{align}
which is the solid purple line (theory without detection noise) plotted in Fig~2\textbf{b}.

The mean atom number as a function of acceleration A is $\bar n = 1/(e^{2\pi cE_{k_f}/\hbar A}-1)$. We insert it into Eq. \eqref{eq16} and get the relation between $S$ and $A$ as
\begin{equation}
    S = -k_\mathrm{B}\left[\ln\left(e^{2\pi cE_{k_f}/\hbar A}-1\right)-\frac{2\pi cE_{k_f}/\hbar A}{(1-e^{-2\pi cE_{k_f}/\hbar A})}\right].
\end{equation}

When $\Bar{n}\gg1$, the entropy is approximated as $S = k_{\mathrm{B}}\ln(e\Bar{n})$, where $e=2.718\ldots$. Using Eq. \eqref{eq13}, we obtain the entropy $S$ dependence on $A$ under large $\bar n$ limit as
\begin{equation}
S = k_{\mathrm{B}}\ln\left(\frac{e\hbar A}{2\pi cE_{k_f}}\right),
\end{equation}
in which $S$ increases logarithmically with $A$.\\

\section{Determination of mode width and effective temperature}

In this section, we first determine the mode width experimentally. In Ref. \cite{Logan2017}, the measurement of second-order correlation function $g^{(2)}(\theta)$ of Bose fireworks was reported. We have $g^{(2)}(0)=2$ indicating that in one mode there is a relation of $\Delta n^2_M=[g^{(2)}(0)-1]\langle n_M\rangle^2$ where $\langle n_M\rangle$ and $\Delta n^2_M$ are the mean and variance of the atom number.

Experimentally we slice our emission patterns into 180 slices and count the atom number in each slice. Based on the histogram of atom counting from the measurements, we build the probability distribution function $P(n)$ and calculate $\langle n\rangle=\int nP(n)dn$ and $\Delta n^2=\langle n^2\rangle-\langle n\rangle^2-\Delta n^2_{noise}$. Here $\Delta n^2_{noise}$ is the variance contributed from the detection noise which is statistically independent with the signal from atom counting. From that, we find a linear dependence between the mean atom number square and the variance from the experiment as (see Fig.~\ref{S1})
\begin{equation}
    \langle n\rangle^2 = \xi \Delta n^2.
\end{equation}
Here $\xi=\Delta\theta_S/\Delta\theta_J=1.49(7)$ is determined from the fitting, characterizing the mode width $\Delta \theta_J$ with each slice's width $\Delta\theta_S=2^\circ$. Therefore, $\Delta\theta_J$ equals to $1.33^\circ$. We also calculate $\Delta\theta_J$ from another independent way. Using the formula $\Delta\theta_J=1.62/(Rk_f)$ in Ref.~\cite{Logan2017} which comes from the half width at half maximum of the peak at $\phi = 0$ in the $g^{(2)}$ function, we obtain a consistent result of $\Delta\theta_J=1.3^\circ$.

\begin{figure}[h!]
\begin{center}
\includegraphics[width=182mm]{Fig_S1_v3.pdf}
\caption{\textbf{Determination of the mode width and the fitting of the measured probability distribution P(n)}. \textbf{a} shows the linear dependence of mean square $\mean{n}^2$ and variance $\Delta n^2$ of atom number distribution in the slice with an angular width $\Delta\theta_S = 2^{\circ}$, from which we have subtracted the contribution from the detection noise. \textbf{b} shows the background atom number distribution $G(n,1.5)$ (black line), ideal emitted atom number distribution $p(n,1.5)$ (blue line) and the convolution between both of them $P(n,1.5)$ (red line) which fits the measured probability distribution $P(n)$ (red circles) at the modulation time $\tau = 4.8$~ms.   }
\label{S1}
\end{center}
\end{figure}

To test and verify
that the emitted atom number in each mode follows a thermal distribution, we derive a more general formula for the probability distribution $p(n,\xi)$ in a slice with any width $\Delta\theta_S=\xi\Delta\theta_J$.
Because the mean population per mode $\langle n_M\rangle$ is always larger than 1 in our measurements, we treat the distribution $p(n,\xi)$ as a continuous function where the summation $\sum_{n=0}^{\infty} p(n,\xi)=1$ is replaced by an integral $\int_{0}^{\infty} dn p(n,\xi)=1$.

Here we would like to list a few properties of the function $p(n,\xi)$. First, $p(n,\xi)$ must equal to 0 when $n$ is a negative number. Second, if the angular slice only contains one momentum mode (\textit{i.e.} $\xi = 1$), $p(n,1)$ should be a thermal distribution, where $p(n,1)$ equals $\beta e^{-\beta n}$ with $\beta = E_{k_f}/k_{\mathrm{B}}T$.  Third, $p(n,\xi)$ have to satisfy the addition rule that combining two slices of $\xi_1$ and $\xi_2$ will create a new slice of $\xi_1+\xi_2$. We can write the third requirement more explicitly as a mathematical equation
\begin{equation}
p(n,\xi_1+\xi_2) = \int_{-\infty}^\infty p(n^\prime,\xi_1) p(n-n^\prime,\xi_2)dn^\prime.
\end{equation}
From all the above conditions, we solve the probability distribution $p(n,\xi)$ analytically as
\begin{eqnarray}
p(n,\xi ) &=&
\begin{cases}
\beta^\xi n^{\xi-1}e^{-\beta n}/\Gamma(\xi) & n\geq 0\\
0 & n<0,
\end{cases}
\end{eqnarray}\label{eqn:prob_slice}
where $\Gamma(\xi)$ is the gamma function.

In addition to the signals from the atoms, the detection noise contributes to the measured probability distribution of the atom number. Experimentally we characterize this noise distribution $G(n,\xi)$ by inspecting the images without any radiations. Once we get $G(n,\xi)$, we convolve it with $p(n,\xi)$ to get a full distribution function
\begin{equation}
    P(n,\xi)=\int_{-\infty}^\infty d n^\prime p(n^\prime,\xi)G(n-n^\prime,\xi).
\end{equation}
Then we use this function to fit our data extracting out the temperature $T$ under the condition of $\xi=1.5$ (see Fig.~\ref{S1}\textbf{b}).

\section{Characterization of entropy from population distribution}

We define the entropy in one slice with the width of $\xi\Delta\theta_J$ as $S(\xi)$. First we use the probability distribution $p(n,\xi)$ derived in the previous section to evaluate $S(\xi)$, which gives
\begin{equation}
    S(\xi)/k_\mathrm{B}=-\int_{-\infty}^\infty dn p(n,\xi)\ln p(n,\xi)=-\ln\beta+\xi+\ln\Gamma(\xi)-(\xi-1)\Gamma^\prime(\xi)/\Gamma(\xi).\label{eq26}
\end{equation}

In our data analysis, we divide the radiation pattern into 180 slices and determine the probability distribution $P(n)$. Thus, the entropy directly measured by the experiment is
\begin{equation}
    S(1.5)=-k_\mathrm{B}\sum_n P(n)\ln P(n).
\end{equation}
We show that the entropy in a single mode $S(1)$ is given by
\begin{equation}
    S(1)=S(1.5)-S_0=-k_\mathrm{B}\sum_n P(n)\ln P(n)-S_0
\end{equation}
based on Eq. (\ref{eq26}) where $S_0=k_{\mathrm{B}}\left[\xi-1+\ln\Gamma(\xi)-(\xi-1)\Gamma^\prime(\xi)/\Gamma(\xi)\right]\vert_{\xi=1.5}=0.37k_\mathrm{B}$.

For the theoretical curve with noise plotted in Fig.~\ref{fig2}\textbf{b} (blue solid line), we characterize the detection noise per mode $ G(n,1)$ and then evaluate the theoretical distribution by convolving $ G (n,1)$ with $p(n,1)$ as
\begin{equation}
    \tilde P(n,1)=\int_{-\infty}^\infty dn^\prime p(n^\prime,1) G(n-n^\prime,1).
\end{equation}
And we calculate the entropy as
\begin{equation}
    S=-k_{\mathrm{B}}\int dn \tilde P(n,1)\ln \tilde P(n,1),
\end{equation}
which matches our experimental data (see the blue solid line in Fig.~\ref{fig2}\textbf{b}).

\section{Phase correlations of atomic radiation field}

Here we calculate the phase correlations between interference fringes, which directly relate to that between emitted jets. We consider two sets of independent jets which are generated by two pulses of scattering length modulation with certain phase. In the interaction picture, the wave function can be written as $\ket{\psi}_I=\ket{\psi^{(1)}}_I\otimes\ket{\psi^{(2)}}_I$. Each $\ket{\psi^{(j)}}_I$ follows
\begin{equation}
    \ket{\psi^{(j)}}_I={1\over\cosh(\gamma_j)}\sum_{n=0}^\infty\left[e^{i(\phi_{M_j}-\pi/2)}\tanh(\gamma_j)\right]^n |n,n\rangle_{k_j,-k_j}
\end{equation}
under the Hamiltonian
\begin{equation}
    H^{(i)}_I=g_j e^{i\phi_{M_j}} a^\dagger_{k_j} a^\dagger_{-k_j} +g_j e^{-i\phi_{M_j}} a_{k_j} a_{-k_j}
\end{equation}
where $\phi_{M_j}$ is given by the phase of external driving field, $\gamma_j=g_j\tau_j$ and $\tau_i$ is the modulation duration of the pulse.

To take the dynamical phase into account, we convert the wave function back to Schr\"odinger's picture, and the wave function is written as
\begin{eqnarray}
|\psi\rangle_S &=& |\psi^{(1)}\rangle_S \otimes |\psi^{(2)}\rangle_S ,
\end{eqnarray}
where $|\psi^{(j)}\rangle_S$ is given by
\begin{eqnarray}
|\psi^{(j)}\rangle_S &=&e^{-iH_0^{(j)}t/\hbar}|\psi^{(j)}\rangle_I\nonumber\\
&=&\frac{1}{\cosh(\gamma_j)}\sum^{\infty}_{n=0}\left[e^{i(\phi_{M_j}-\omega_jt-\pi/2)}\tanh(\gamma_j)\right]^n |n,n\rangle_{k_j,-k_j}.
\end{eqnarray}
Here $H_0^{(i)} = \hbar\omega_i(a_{\mathbf{k}_j}^\dagger a_{\mathbf{k}_j}+a_{-\mathbf{k}_j}^\dagger a_{-\mathbf{k}_j})/2$ is energy term which was previously eliminated in the interaction picture.

The interference operators between the two sets of jets are $\hat{I}_f = a_{\mathbf{k}_1}a_{\mathbf{k}_2}^\dagger$ and $\hat{I}_b = a_{-\mathbf{k}_1}a_{-\mathbf{k}_2}^\dagger$ which correspond to the forward and backward directions. We introduce four more interference operators
as $\hat{I}_{j+}=a_{\mathbf{k}_j}a_{-\mathbf{k}_j}$ and $\hat{I}_{j-}=a_{\mathbf{k}_j}a^\dagger_{-\mathbf{k}_j}$ with $j$~=~1 or 2. The mean value for the interference operator $\hat{I}_{i\pm}$ is evaluated as
\begin{eqnarray}
\langle \hat{I}_{j+}\rangle &=&\langle\psi^{(j)}|_S \left(a_{\mathbf{k}_j} a_{-\mathbf{k}_j}\right) |\psi^{(j)}\rangle_S\nonumber\\
&=& \sqrt{\langle n_j\rangle(\langle n_j\rangle+1)}e^{i(\phi_{M_j}-\omega_jt-\pi/2)}\label{eq:Iplus}\\
\langle \hat{I}_{j-}\rangle &=&\langle\psi^{(j)}|_S \left(a_{\mathbf{k}_j} a_{-\mathbf{k}_j}^\dagger\right) |\psi^{(j)}\rangle_S\nonumber\\
&=& 0,\label{eq:Iminus}
\end{eqnarray}
where $\langle n_j\rangle$ is the mean atom number in each set of jets.

Phase correlation between interference fringes can be directly decomposed into the interference operators in each set of jets. The phase correlation $g_+(\theta = \pi)$ is proportional to the correlation between $\hat{I}_f$ and $\hat{I}_b$ , together with Eq.~(\ref{eq:Iplus}) we get
\begin{eqnarray}
\langle e^{i(\phi_{\theta}+\phi_{\theta+\pi})}\rangle \propto \langle \hat{I}_f\hat{I}_b \rangle
&=& \langle\psi^{(1)}|_S \otimes \langle\psi^{(2)}|_S \left(a_{\mathbf{k}_1} a^\dagger_{\mathbf{k}_2} a_{-\mathbf{k}_1} a_{-\mathbf{k}_2}^\dagger\right)  |\psi^{(1)}\rangle_S \otimes |\psi^{(2)}\rangle_S \nonumber\\
&=&\langle\psi^{(1)}|_S \left(a_{\mathbf{k}_1} a_{-\mathbf{k}_1}\right) |\psi^{(1)}\rangle_S \langle\psi|_S^{(2)}\left( a_{\mathbf{k}_2}^\dagger a_{-\mathbf{k}_2}^\dagger\right) |\psi\rangle_S^{(2)}\nonumber\\
&=& \langle\hat{I}_{1+}\rangle\langle \hat{I}_{2+}^\dagger\rangle\nonumber\\
&=&\sqrt{\langle n_1\rangle(\langle n_1\rangle+1)}\sqrt{\langle n_2\rangle(\langle n_2\rangle+1)}e^{i\left[(\phi_{M_1}-\phi_{M_2})-(\omega_1-\omega_2)t\right]}\label{M37}
\end{eqnarray}
Therefore, the sum of the phases of the forward and backward interference fringes only depends on the phase of the driving and the dynamical phase. Thus we have the phase constant $\phi_s = \phi_{\theta}+\phi_{\theta+\pi}= (\phi_{M_1}-\phi_{M_2})-(\omega_1-\omega_2)t$ and $g_+(\pi)=1$.

Meanwhile, phase correlation $g_{-}(\theta=\pi)$ is proportional to the mean value of $\hat{I}_f\hat{I}_b^\dagger$, together with Eq.~(\ref{eq:Iminus}) we have
\begin{eqnarray}
\langle e^{i\phi_{\theta}-\phi_{\theta+\pi}} \rangle \propto \langle \hat{I}_f\hat{I}_b^\dagger \rangle &=& \langle\psi^{(1)}|_S \otimes \langle\psi^{(2)}|_S\left(a_{\mathbf{k}_1} a^\dagger_{\mathbf{k}_2} a^\dagger_{-\mathbf{k}_1} a_{-\mathbf{k}_2}\right) |\psi^{(1)}\rangle_S \otimes |\psi^{(2)}\rangle_S \nonumber\\
&=&\langle\psi^{(1)}|_S\left( a_{\mathbf{k}_1} a^\dagger_{-\mathbf{k}_1}\right) |\psi^{(1)}\rangle_S \langle\psi^{(2)}|_S\left( a^\dagger_{\mathbf{k}_2} a_{-\mathbf{k}_2}\right) |\psi^{(2)}\rangle_S\nonumber\\
&=&  \langle\hat{I}_{1-}\rangle\langle \hat{I}_{2-}^\dagger\rangle\nonumber\\
&=& 0\label{M38}
\end{eqnarray}
therefore we have $g_{\_}(\pi)=0$, indicating that phases in each pair of jets are totally random although their sum is fixed. The results from Eqs.~(\ref{M37}, \ref{M38}) are consistent with our measurement shown in Fig.~3\textbf{g}.

Based on the same techniques of Eqs.~(\ref{M37}, \ref{M38}) and the methods in Ref.~\cite{Logan2017}, we derive a more general analytic formula for $g_+(\theta)$ and $g_-(\theta)$. We still use the symbol $\mathbf{k}_1$ and $\mathbf{k}_2$ corresponding two jets with different energy propagating along the same direction. We introduce $\mathbf{k}^\prime_1$ and $\mathbf{k}^\prime_2$ representing two jets propagating along the direction with a relative angle $\theta$ to $\mathbf{k}_1$ and $\mathbf{k}_2$. Therefore, $g_{\pm}(\theta)$ is written as
\begin{eqnarray}
g_+(\theta)=\left|{\langle a_{\mathbf{k}_1}a^\dagger_{\mathbf{k}_2} a_{\mathbf{k}^\prime_1} a^\dagger_{\mathbf{k}^\prime_2} \rangle \over \langle a^\dagger _{\mathbf{k}_1} a_{\mathbf{k}_1}\rangle \mean{a^\dagger_{\mathbf{k}_2} a_{\mathbf{k} _2} }}\right|=\left|{\langle a_{\mathbf{k}_1}a_{\mathbf{k}^\prime_1}\rangle \langle a^\dagger_{\mathbf{k}_2} a^\dagger_{\mathbf{k}^\prime_2} \rangle \over \langle a^\dagger _{\mathbf{k}_1} a_{\mathbf{k}_1}\rangle \mean{a^\dagger_{\mathbf{k}_2} a_{\mathbf{k} _2} }}\right|, \\
g_-(\theta)=\left|{\langle a_{\mathbf{k}_1}a^\dagger_{\mathbf{k}_2} a^\dagger_{\mathbf{k}^\prime_1} a_{\mathbf{k}^\prime_2} \rangle \over \langle a^\dagger _{\mathbf{k}_1} a_{\mathbf{k}_1}\rangle \mean{a^\dagger_{\mathbf{k}_2} a_{\mathbf{k} _2} }}\right|=\left|{\langle a_{\mathbf{k}_1}a^\dagger_{\mathbf{k}^\prime_1}\rangle \langle a^\dagger_{\mathbf{k}_2} a_{\mathbf{k}^\prime_2} \rangle \over \langle a^\dagger _{\mathbf{k}_1} a_{\mathbf{k}_1}\rangle \mean{a^\dagger_{\mathbf{k}_2} a_{\mathbf{k} _2} }}\right|.
\end{eqnarray}
According to the methods in Ref.~\cite{Logan2017}, we obtain
\begin{eqnarray}
    \mean{a_{\mathbf{k}_j}a_{\mathbf{k}^\prime_j}}&=&e^{i(\phi_{M_j}-\omega_jt-\pi/2)} {\tilde \rho(\mathbf{k}_j+\mathbf{k}^\prime_j) \over 2\pi}\cosh(\gamma_j)\sinh(\gamma_j) ,\\
    \mean{a^\dagger_{\mathbf{k}_j}a_{\mathbf{k}^\prime_j}}&= &{\tilde \rho(\mathbf{k}_j-\mathbf{k}^\prime_j) \over 2\pi}\sinh^2(\gamma_j),
\end{eqnarray}
where $\tilde\rho(\mathbf{k})$ is defined as the Fourier transformation of a uniform disk-shape density $\rho(\mathbf{r})$,
\begin{equation}
    \rho(\mathbf{r})={1\over 2\pi}\int d^2\mathbf{k} e^{i\mathbf{k}\cdot\mathbf{r}}\tilde \rho(\mathbf{k}).
\end{equation}
And $\rho(\mathbf{r})$ is the density distribution function of the condensate as
\begin{equation}
     \rho(\mathbf{r})=\begin{cases}
1 & |\mathbf{r}|\leq R\\
0 & |\mathbf{r}|>R
\end{cases}
\end{equation}
with $R$ is the radius. Therefore, the analytic formulas for $g_{\pm}(\theta)$ when $\gamma_j\gg1$ and $|\mathbf{k}_i|R\gg 1$ are
\begin{eqnarray}
g_+(\theta)&=&\left|{4\tilde\rho(\mathbf{k}_1+\mathbf{k}^\prime_1)\tilde\rho^*(\mathbf{k}_2+\mathbf{k}^\prime_2)\over \tilde R^4}\right| \nonumber \\
&=&\left|{4J_1(|\mathbf{k}_1|R(\theta-\pi)) J_1(|\mathbf{k}_2|R(\theta-\pi))\over|\mathbf{k}_1||\mathbf{k}_2| R^2(\theta-\pi)^2}\right| ,
\end{eqnarray}
and
\begin{eqnarray}
g_-(\theta)&=&\left|{4\tilde\rho(\mathbf{k}_1-\mathbf{k}^\prime_1)\tilde\rho^*(\mathbf{k}_2-\mathbf{k}^\prime_2)\over \tilde R^4}\right|\nonumber \\
&=&\left|{4J_1(|\mathbf{k}_1|R\theta) J_1(|\mathbf{k}_2|R\theta)\over |\mathbf{k}_1||\mathbf{k}_2| R^2\theta^2}\right|,
\end{eqnarray}
where $J_1(x)$ is the first order Bessel function of the first kind.

To experimentally extract the interference fringe phase $\phi_\theta$ at a particular emission direction $\theta$, we average over an angular span from $\theta-0.12$ to $\theta+0.12$ to obtain the radial density distribution $\rho(r,\theta)$ in order to achieve the best signal to noise ratio (see Fig.~\ref{fig3}\textbf{d}). We then perform Fourier transformation on the radial density to get the complex density amplitude of the interference fringes in momentum space $\rho(k,\theta)$. The phase $\phi_\theta$ at $k_f$ is then evaluated from this complex amplitude. Although our jet width is small, that is 2$^\circ$ for $\omega/2\pi$~=~3~kHz and 1.5$^\circ$ for $\omega/2\pi$~=~5.63~kHz, this average results in a significantly broadened phase correlation shown in Fig.~\ref{fig3}\textbf{g}. To experimentally extract the phase constant $\phi_s$, we fit the histogram of $\phi_\theta +\phi_{\theta+\pi}$ to get the peak position. We also calculate the expected phase shift based on our experimental sequence with a time of 18.5~ms from the start of the modulation to the start of imaging. The first sinusoidal modulation pulse lasts for 6 periods while the second lasts for 17 periods. Meanwhile we take into account the time delay of the modulation pulse of 0.041~ms due to system response. Therefore the phase constant estimated from our experimental sequence is 0.9(2) where the uncertainty arises from the duration of our 20~$\mu s$ imaging pulse.

\section{Numerical results on reversal of atomic radiation field}

In this section, we use numerical simulation based a dynamical Gross-Pitaevskii equation to investigate the partial reversal on radiating matter-wave fields. We find that this imperfect reversal results mostly come from the off-resonant coupling to finite momentum modes close to $|\mathbf{k}|=k_f$.

\begin{figure}
\begin{center}
\includegraphics[width=185mm]{Fig_Sub1_new04.pdf}
\caption{\textbf{Numerical simulation on reversal of matter-wave radiation.} \textbf{a} shows the time evolution of the total emitted atom number $N$ for different phase jump $\alpha$~=~0 (blue), 0.44$\pi$ (purple), 0.89$\pi$ (red), and 1.33$\pi$ (orange). Here the phase jump happens at $\tau$~=~4.76~ms while optimal suppression is achieved at $\tau_c$~=~5.62~ms. \textbf{b} shows the emitted atom number at different momentum modes $N_k(\alpha)$ as a function of phase jump $\alpha$ at $\tau_c$.
\textbf{c} compares the overall suppression ratio $\eta$ from simulation (blue curve), suppression ratio for a particular momentum mode $k_f$ (black curve), and experiment (dots).}
\label{fig_sub_sim}
\end{center}
\end{figure}

Here we start with Gross-Pitaevskii equation,
\begin{equation}\label{eq:GP}
\begin{aligned}
i\hbar\frac{\partial\psi}{\partial t}=&\left[-\frac{\hbar^2}{2m}\nabla^2+V({\bf{r}})+U_{dc}|\psi|^2 -\mu\right]\psi \\
&+U_{ac}f(t)|\psi|^2\psi,
\end{aligned}
\end{equation}
where $\psi$ is the wavefunction and $\mu~=~2\pi\hbar\times 19$~Hz is the static chemical potential of the condensate,
$V(r)$ is the disk-shaped trapping potential as a function of radius $r$ with $V(r) = 2\pi\hbar\times 300$~Hz for $13.6~\mu$m$\geq r\geq13~\mu$m and $V(r)=0$ for the rest, $U_{dc}=4\pi\hbar^2a_{dc}/m$ and $U_{ac}=4\pi\hbar^2a_{ac}/m$ are
the DC and AC interaction strengths with
$a_{dc}~=~3a_0$ and $a_{ac}~=~50a_0$. In addition, we have $f(t) = \sin(\omega t)$ when $t\leq4.76$~ms and $f(t) = \sin(\omega t + \alpha)$ for $t>4.76$~ms. These parameters are chosen according to our experimental conditions.

The results from simulation using a CUDA-based solver \cite{GaugeFieldPaper} shows great agreement with the experiment. First of all, the total emitted atom number is suppressed after the phase jump $\alpha$ close to $\pi$ (see Fig.\ref{fig_sub_sim}\textbf{a}). The suppression sensitively depends on the phase of the second pulse $\alpha$. Similarly to the analysis of our experimental data, we then look at the suppression ratio as a function of phase $\alpha$ at $\tau_c~=~5.62$~ms when the optimal suppression appears (see Fig.\ref{fig_sub_sim}\textbf{c}). The suppression ratio varies as a function of $\alpha$ in the same way as in our experiment and the best suppression can be achieved is $\eta =0.57$ comparable to the experimental result.

The reason for this partial suppression is the off-resonant coupling to finite momentum modes close to $|\mathbf{k}|=k_f$. We examine more carefully about the emitted atoms in different momentum modes (see Fig.~\ref{fig_sub_sim}\textbf{b}), not all atoms are excited with a particular well-defined momentum. Instead, atoms spread across a range of momentum modes due to uncertainty principle since the atoms are confined within a finite radius of $13~\mu$m. These momentum modes are then off-resonantly coupled to the external modulation without perfect phase matching. Therefore population in these off-resonantly excited modes are maximally reversed at different phase jumps. For one particular momentum mode, the population can be reduced by as much as 70\%, while the overall population is only suppressed to about 50\%, consistent with our measurement.

Beside this off-resonant coupling, we anticipate the reversal can be limited by other effects such as the fast counter-rotating terms and the motion of the emitted atoms as well. The counter-rotating terms lead to quick population oscillations seen in Fig.~\ref{fig_sub_sim}\textbf{a}; they also accumulate phase and eventually limit the reversal. Furthermore, when atoms move out of the condensate, they can not be transferred back to the condensate anymore. These effects are included in the simulation but their contributions to the limited reversal are hard to separate in our numerical model.

\end{document}

redpajama_set_name: RedPajamaArXiv


text:
Glenn Wilkins - Wednesday, October 6, 2021
QC at 52-Week High on Cormark Hookup
QC Copper and Gold Inc. (V.QCCU) hit a new 52-week high of 41.5 cents on Wednesday. QC Copper and Gold has entered into an agreement with Cormark Securities Inc., on behalf of a syndicate of agents, pursuant to which the Agents have agreed to act as agents in connection with a "best efforts" private placement offering of 6,700,000 common shares in the capital of the Company that will qualify as "flow-through shares" (within the meaning of subsection 66(15) of the Income Tax Act ( Canada ) and section 359.1 of the Taxation Act (Québec)) at a price of $0.60 per FT Share for gross proceeds of $4,020,000.
Bri-Chem Corp. (T.BRY) hit a new 52-week high of 20 cents on Wednesday. No news stories available today.
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Dividend Select 15 Corp. (T.DS) hit a new 52-week high of $9.70 on Wednesday. No news stories available today.
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PHX Energy Services Corp. (T.PHX) hit a new 52-week high of $5.17 on Wednesday. No news stories available today.
Pine Cliff Energy Ltd. (T.PNE) hit a new 52-week high of 72 cents on Wednesday. No news stories available today.
Reitmans (Canada) Limited (V.RET) hit a new 52-week high of $1.30 on Wednesday. No news stories available today.
SSC Security Services Corp. (V.SECU) hit a new 52-week high of $3.00 on Wednesday. No news stories available today.
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Amarillo.,Alpha, Arc at 52-Week Highs
Banks, First Hydrogen, Surge at 52-Week Highs on News
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Aritzia, CIBC, InPlay at 52-Week Highs on News
Endurance Gold, Filo Mining. InPlay Oil at 52-Week Highs on News


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In a food processor, blend together the almond butter and dates to a fairly smooth paste and it begins to come together into a ball. Add the goji berries, pumpkin seeds and desiccated coconut and blend until they are evenly distributed throughout the mix.
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