Posted on 23 November 2017.
BRIDGETOWN, Barbados, Nov 21, CMC – Grenada's Prime Minister Dr. Keith Mitchell says Caribbean countries facing economic problems should consider implementing home-grown programmes that will find favour with the various international lending agencies, such as the International Monetary Fund (IMF).
Grenada is emerging from an IMF-supported Extended Credit Facility (ECF) programme of US$19.4 million that was approved in 2014 and Mitchell acknowledged that "there were some major sacrifices" that had to be undertaken by the population.
He said when his ruling New National Party (NNP) came to power four years ago, it found a situation where the island had negative growth for a number of years "and clearly there was little or no economic activity in the country.
"The investment climate was extremely poor and there was tremendously high unemployment….Grenada was unable to pay its debts and we decided we had to do something".
Mitchell, who attended last week's IMF-sponsored Sixth High Level Caribbean Forum in Grenada, told the Caribbean Media Corporation (CMC) that he met with all the various stakeholders in Grenada, including the trade union, the churches, the business community and the non-government organisations "to map a way forward.
He told CMC he believes that this "call is most important because you are able to institute some major sacrifices and at the same time you are able to convince our friends regionally and internationally to come forward and help us because they saw we are prepared to make sacrifices".
In March, during the last phase of the IMF supported programme, the Washington-based financial institution reported that the home grown programme had been strong with the island recording economic growth of just under four per cent last year.
Nicole Laframboise, who headed an IMF delegation to the island, said that the government had made progress toward achieving the key programme goals of restoring fiscal sustainability, strengthening the financial sector, and setting the stage for durable growth.
She said that the government has met all of the performance criteria and structural benchmarks due at end-December 2016.
The IMF official said that real gross domestic product (GDP) is estimated to have expanded by 3.9 per cent in 2016, implying annual real GDP growth of 5.8 per cent on average from 2014-2016.
She said activity in 2016 was driven by tourism, construction, and some pick up in domestic demand, while agriculture experienced weather-related contraction.
Mitchell told CMC that Caribbean countries experiencing economic problems and resisting going to the IMF for assistance because of the stringent measures likely to be outlined by the Washington-based financial institution, could also develop their own home-grown programme like Grenada did.
"That's the decision all of us will have to make. The previous government in Grenada was offered the same thing I was offered. In fact they agreed and then they backed off. They agreed they made way and decided they would lose political support and backed off again.
"So as the situation improves and the country gains more momentum economically and otherwise we are prepared to ease up the burden on the people as much as possible," Mitchell told CMC.


For more information, you may also send an email to 15project@rctc.org or complete the form to the right.
You may also call the project helpline at (844) 415-9777.
Monday – Thursday, 8:00 a.m. to 5:30 p.m. and Friday, 8:00 a.m. to 4:30 p.m.
Please contact us with any questions you may have regarding the 15 Express Lanes Project.


text:
We must continue to impose sanctions on Iran for shamelessly bartering in human lives
By Alicia Kearns MP
22 Jan Foreign affairs
Inter-Parliamentary Union forges connections with foreign parliaments
By Karen Bradley MP
We need a national strategy to prevent and respond to mass atrocities
By Sarah Champion MP
We must not give up on the women of Afghanistan
By Preet Kaur Gill MP
The next stages of the war in Ukraine
By Bob Seely MP
Sellafield Ltd and Japan prove the value of continued cooperation
By Sellafield Ltd
UK Advertising Exports Group Joins International Trade Week
By Advertising Association
Leading veterinary organisations urge Prime Minister to help stranded group of at-risk Afghan vets and their families with safe passage to the UK
By British Veterinary Association
Years of horrific atrocities against Rohingya women and girls cannot go unanswered
(Alamy)
@AdvRaziaSultana
4 min read 29 November 2022
The Preventing Sexual Violence in Conflict Initiative (PSVI) Conference, hosted in London by the United Kingdom government this week, marks ten years since its launch in 2012.
For the Rohingya, 2012 was a very difficult year as it saw the beginning of the Rakhine State riots – a series of ethnic conflicts in that paved the way for the wave of violence that eventually led to the 2017 mass displacement of Rohingyas into Bangladesh by the military.
Marginalisation of the Rohingyas in Myanmar (Burma) long predates 2012, but that year was perhaps the first time we were able to truly draw attention to the continued persecution our people have endured over many decades. Some Rohingya have been in Myanmar for centuries, while others arrived more recently.
Regardless of how long we have been in the country, Myanmar authorities consider us undocumented immigrants and do not recognise us as citizens or as an ethnic group. Instead, they see us as a destabilising force and have been intent on ethnically cleansing us and erasing us from the history books by enacting repressive and discriminatory laws, such as the 1982 Citizenship Law.
The Rohingya community and Bangladesh are in great need of increased humanitarian assistance to face ever-growing challenges
Unfortunately, one of the most effective ways to ethnically cleanse an entire group is the use of sexual violence to terrorise women and girls – the Myanmar military is sadly infamous for it, most notably against the Rohingya.
Since the military staged its takeover coup in February 2021, women have emerged as symbols of defiance and leaders of resistance efforts at home and abroad, but this has put a target on their backs. Despite extensive documentation, widespread outcry among the international community and an on-going case at the International Court of Justice, the military has yet to face any consequences for its actions. It continues to employ sexual violence with impunity.
My work focuses on helping women and girls come to terms with the trauma caused by gender-based violence, and particularly sexual violence, since the very beginning of the genocide. I've spent years documenting the horrific atrocities committed against Rohingya women and girls by the Myanmar military and calling for accountability for these crimes.
Changing deeply entrenched patriarchal views is difficult but we're making progress, especially with young people. As well as working with and empowering women, we also need to engage with men to help them understand the value of gender equality. There are many challenges in the camps, and we are seeking to increase literacy training, as well as improve access to sanitary hygiene products and clean products to prevent disease.
What can the UK and other supporters of the Rohingya do to help us? Too often, grassroots organisations struggle to access funding quickly. As a result, women are not able to participate in peacebuilding and we cannot support as many victims. I believe much more can be done to ensure rigid funding structures designed by governments become more flexible to the realities on the ground.
We are very grateful to Bangladesh, the host state, for having protected so many Rohingya for so long. However, the Rohingya community and Bangladesh are in great need of further and increased humanitarian assistance to face the ever-growing challenges.
Sexual violence in any conflict is an early warning sign and must be systematically documented as more violence is likely to follow. We are working to increase international recognition of this important principle and find ways to adopt a victim centered approach that is sensitive to the trauma that women and girls have experienced.
We of course want to be part of creating these solutions for ourselves. We welcome the international community's assistance but many smaller organisations on the ground are doing their best with scant resources. They need funding, flexible policies and training to ensure a better future for their communities.
Razia Sultana, lawyer and Rohingya human rights activist.
Benefits Wrongly Paid To Thousands Of EU Citizens Due To Home Office Error
By Adam Payne
Rohingya Myanmar sexual violence atrocities
Keir Starmer Promises Industry Leaders Labour Is A "Reliable Partner" For Global Business
Labour Sees No "Political Case" For Rejoining EU Single Market, Ukraine Issues Plea For More Tanks
20 Jan Brexit
Michael Gove Defends Levelling Up Funding On Rishi Sunak's Patch, New Zealand's Jacinda Ardern To Resign
DUP and ERG Alliance Threatens Fresh Brexit Headache For Rishi Sunak
UK And EU To Intensify Northern Ireland Protocol Talks In A Bid For February Deal
Rishi Sunak Could Block Scottish Gender Recognition Bill, Labour Calls Anti-Strike Laws A "Fundamental Mistake"
Civil Service Strikes, Disability Benefits Reforms, Partygate Revelations Continue
Keir Starmer Set To Visit Northern Ireland After Breakthrough In Brexit Protocol Talks
What Do Ukrainians In The UK Think Of British Politics?
30 Dec 2022 Foreign affairs
How Ukrainian Refugees Are Celebrating Christmas In The UK – From Strictly To Orthodox Christmas Potluck

redpajama_set_name: RedPajamaCommonCrawl


text:
JK.3 Anthony Eden letter recto0001.tif.jpg
JK.3 Anthony Eden letter verso0001.tif.jpg
JK.3 Anthony Eden card0001.tif.jpg
JK.3 Anthony Eden envelope0001.tif.jpg
Letter from Jessie Kenney to Prime Minister Anthony Eden and Thank You card, 1957
Jessie Kenney wrote to Sir Anthony Eden, UK Prime Minister from 1955 to 1957, to express her support of his methods for dealing with the Suez Crisis. The Suez Crisis, or the Second Arab-Israeli War, was an invasion of Egypt in 1956 followed by the UK and France, aiming to regain control of the Suez Canal. Political pressure from the other global powers, including the United Nations and the Soviet Union, forced them to withdraw. The episode is regarded as a failure of British foreign policy and put an end to Eden's political career. Jessie's view was that the British invasion was justified and she commended Eden on his show of courage and strength. "We [the British] have been taking it 'on the chin'," she writes, "ever since we won the war of 1939, and the more we have worked for peace, the more we have subscribed to it, when we could ill afford it, and to the backward nations to help them get independence."
Also included is a Thank You card sent from PM Eden's Office.
Kenney, Jessie, and Eden, Anthony
1950s, 1957, Anthony Eden, Jessie Kenney, War
Kenney, Jessie, and Eden, Anthony, "Letter from Jessie Kenney to Prime Minister Anthony Eden and Thank You card, 1957," Suffragette Stories, accessed January 22, 2020, https://suffragettestories.omeka.net/items/show/112.


A slice of Italy on the coast. That is what La Galleria has offered its guests for almost 40 years now in its establishments on Kurhausplein in the heart of Scheveningen and on the boulevards of Scheveningen, Kijkduin and Noordwijk. La Galleria is run by two Italian families. That's something you sense straight away and with its authentic Italian dishes, snacks, appetizers, wines imported by La Galleria itself and, of course, typical Italian hospitality it's also something to savour. No matter the occasion – simply a cup of good Italian coffee in the morning, or a tasty lunch, or cosy drinks and appetizers, or a delicious evening meal – La Galleria is the place to be. Whether you want to dine extravagantly while sipping a delicious glass of wine or treat your children to a pizza or pasta, it's all possible. With tastefully illuminated heated terraces and all nice and cosy inside with a mix of classic and modern decor, all four locations offer the perfect ambiance for entertaining business relations, for celebrations, for get-togethers with friends and family.
Come in and bask in the warmth and hospitality of Italy.


When you follow a lot of people online and you see them publishing videos all the time, it is easy to get down on yourself for not publishing as frequently or at as high a quality as you'd prefer.
In this episode I chat with Satchell Drakes, who runs a YouTube channel with some of the highest quality videos in the video gaming niche. I talk with him about his process of creating videos, what has helped his channel grow, and what he recommends for someone that isn't getting the traction they want out of their videos.


Matrix of Role-Based Administration (RBA) Permissions for ConfigMgr 2012 (SCCM 2012) available !!!
What's Matrix of Role-Based Administration (RBA) Permissions for ConfigMgr 2012 ?
This is a download of an Excel spreadsheet which captures a list of the built-in security roles, the permission groups each role uses, and the individual permissions for each group for role-based administration in System Center 2012 Configuration Manager.
SCCM 2012 R2 | How to deploy software prerequisites with SCCM 2012 !
SCCM 2012 R2 | How to import User Device Affinity (UDA) in Configuration Manager by CSV The System Center 2012 R2 Configuration Manager Toolkit available NOW for download !!!
SCCM 1806 Hotfix available (KB4462978) !
SCCM 1806 Hotfix available !


If you have been in a car accident in Clearwater, it is imperative you seek the care of an auto accident chiropractor. This is important even if you do not feel you have been injured. Injuries from car collisions can take days, sometimes weeks, to show symptoms. If left untreated, some of the injuries you sustain, however minor, can eventually cause both acute and chronic pain; some of which can last a lifetime. That is why at Coastal Chiropractic, we urge patients to come into our clinic as soon as possible after they have been in a collision.
Most people assume, especially with fender-benders, that because the vehicles were not going very fast and there is minimal damage to the cars, their bodies are probably fine. However, what many fail to realize is that even the smallest collisions can cause serious damage, most commonly back and neck pain.
When any part of the musculoskeletal system is knocked out of alignment, your overall health becomes vulnerable, since this is the system that deals with everyday functioning. Your spine, back, and neck are the control unit of all your day to day functions, so if any joint, muscle or nerve is injured, it can have a domino effect. This is why visiting an auto accident chiropractor is essential after a collision in Clearwater.
Our chiropractic care centers on effectively treating the spine and musculoskeletal system, which is where most car accident injuries occur. Through massage therapy, gentle spinal adjustments, and corrective treatments, an auto accident chiropractor can restore your body to optimal health. The best part is, we can do this without invasive surgeries or heavy medications.
Most people in Clearwater have heard of whiplash and know that it is one of the most common auto accident injuries. This condition occurs from a sudden, unexpected impact, typically from your neck being jerked back and forth when your vehicle is hit from behind and your seat belt is holding you in place.
But the term "whiplash" does not just to refer to the whipping effect of your neck. The actual pain is caused because the ligaments and sometimes muscles in your neck are torn. Without an experienced auto accident chiropractor treating you, the chances of the tissues in your neck properly healing are slim.
If you have been in a car accident in Clearwater, visit us at Coastal Chiropractic Rehab & Wellness as soon as possible. The longer you wait, the worse your condition can become. Additionally, if you wait too long, there's a chance your insurance company will not cover your treatment.
In Florida, insurance companies only cover medical costs of treating car crash injuries within 14 days of the collision. This is another reason why visiting an auto accident chiropractor immediately after a collision is so important. Your symptoms may not show up for weeks to come, so it is better to be safe than sorry.
When you visit us at Coastal Chiropractic for your injuries, we will start with examinations and screenings. These allow us to assess any damage to your musculoskeletal system and proceed from there. We will customize a treatment plan around your specific needs and conditions. We accept all major insurances and even offer payment plans for families and those on a budget in Clearwater.
You can request an appointment with an auto accident chiropractor online through our website. Or, you can give our office a call today at 727-581-2774 to learn more about our services in the Clearwater area.


I do enjoy writing blogs for seniors on cities that I have personally visited, especially in France. 35+ years in the classroom as an instructor of French does make a difference. La Côte Fleurie (The Flowered Coast) is part of the Lower Normandy coast on the English Channel in the North of the Pays d'Auge, it constitutes the Eastern coast of the department Calvados. The name is a reference to the green and flowered countryside of the country lying beyond the coastal hills and to the numerous resorts along the coast.
Here lies Honfleur. Its 8,177 inhabitants are called Honfleurais. Honfleur is in the Norman département of Calvados, located on the southern bank of the estuary of the Seine, across from le Havre. Timber-framed houses and ancient forged-iron signs encompass Le Vieux Port. The Old Port is still active as a fishing port and marina and the town has preserved many historic and traditional buildings and houses. It is neat to be here with the tide is coming in or going out and watch the boats rise and fall.
In Honfleur you will find a major attraction called Sainte-Catherine church, which has a bell-tower separate from the principal building. It is the largest church made out of wood in all of France. It is a miracle that it has not burned to the ground being made entirely of wood. Do go inside. You will find ship replicas that were lost at sea hanging from the ceiling and walls just as one finds all along the coast of Brittany.
Between Honfleur and Cabourg, the Norman coastline becomes a playground: resorts, casinos, watersports, sunshine, sandy beaches backed by wooded hills. It all started in Trouville, which triggered the 19th-century rage for sea bathing. Next comes racy, romantic Deauville – created in the 1860s by a trio of wealthy entrepreneurs, embellished in 1910 with boardwalk, casino and racecourse. Deauville is the most glamorous seaside resort of Western France. It is one the favorite resorts for well off Parisians. The name symbolizes elegance, prestige and sophistication. Just a few of the nicknames of the town are "The City of the Horse" and "Gateway to Calvados". Closeby near the Atlantic coast one finds the well-known Normand cities of Cabourg, Houlgate, Villiers-Sur-Mer, Trouville, and Cricqueboeuf.


text:
Exciting News!
After 30 years Criterium- Lalancette Engineers has been acquired by the Massachusetts affiliate Criterium- Dudka Engineers. As of March 1, 2019, the new entity will be known as Criterium-Lalancette & Dudka Engineers.
Richard Lalancette, Founding President of Criterium-Lalancette Engineers states, "I am excited both personally and for the staff by the infusion of fresh energy and talent".
Andrew Dudka comes to us from Hopkinton, MA with over 25 years' experience in the manufacturing industry and holds a BS in Mechanical Engineering and an MBA in Finance and Operations.
"We plan to build and expand on the successful services Rick has created and sustained over the last 30 years", says Andrew, "We will continue to offer the most comprehensive services in the region and are excited for growth in both our services and territory. Rick has committed to remain a leader within the company and community for several years to come."
Richard and Andrew are looking forward to synergized success going forward as Criterium-Lalancette & Dudka Engineers.
Subscribe now to get Criterium-Lalancette & Dudka Engineers news and informative articles sent straight to your inbox.


text:
Simaster
Crisis Center
Universitas Gadjah Mada Universitas Gadjah Mada
Inauguration of Professor
Seminar and Workshop
Student Community Service Program
Webometrics 2022: UGM Ranked Second in Indonesia
11 February 2022, 13:34 WIB
By: Salma
Universitas Gadjah Mada (UGM) has been ranked second in Indonesia in the latest Webometrics Ranking, moving down one spot compared to last year. Director of Information Systems and Resources Dr. Widyawan said the decline was due to changes in the assessment criteria.
"Initially, there are four criteria. But, the presence indicator, which has been one of the UGM's advantages, is no longer taken into account," he said.
Of the three indicators weighed, namely impact or visibility, openness or transparency, and excellence, Widyawan added that UGM needs to work on the excellence indicator, which has an assessment weight of 40%.
"The assessment of excellence is based on the number of papers by the UGM academic community, which are in the top 10% most cited in each one of all 27 disciplines," he explained.
The Webometrics Ranking is an initiative of the Spain-based Cybermetrics Lab that has ranked world universities using webometric and bibliometric indicators since 2004.
This ranking aims to promote open access to the knowledge produced by universities, challenging them to improve the quality and quantity of their web content at all times. Around 31,000 universities in more than 200 countries are included in the ranking list.
Author: Gloria
UGM Ranks First in Indonesia
Monday,16 February 2015 - 9:44
UGM Best University in Indonesia, According to Webometrics
Friday,15 February 2019 - 10:23
Webometrics: UGM Is Indonesia's No. 1 University
Thursday,28 January 2021 - 13:39
Webometrics 2010, UGM is the Best University in Indonesia
UGM is The Best in Indonesia
Tuesday,07 August 2012 - 3:24
Accessive.id by UGM Students Wins Silver at Bangkok International Intellectual Property (IPITEx) 09 February 2023
Accesive.id, a mobile application that can inform location
UGM Researches Railway Static Inverters 09 February 2023
A research team from the Department of Electrical Engineer
UGM and Central Java Accelerate Response to Childhood Stunting and Malnutrition 08 February 2023
Universitas Gadjah Mada (UGM), represented by the Faculty
UGM Medicine Faculty & ANU Indonesia Project Launch In Sickness and In Health: Diagnosing Indonesia 07 February 2023
UGM Faculty of Medicine, Public Health, and Nursing and Au
UGM Students Create Mobile App to Inform Location Accessibility 07 February 2023
UGM students have developed a mobile application that can
No latest event at this time
Bulaksumur Yogyakarta 55281
info@ugm.ac.id
ABOUT UGM
Rector's Welcome
Vission and Mission
The Board of Executive
VISIT UGM
Professional Program


text:
using System;
using Colorado.Core;

namespace Colorado
{
	public class ProductFormula: Formula
	{
		public ProductFormula(CsvDocument doc, Position pos, Position.Direction dir) : base( doc, pos, dir )
		{
		}

		public ProductFormula()
		{
		}

		public override double DoIt()
		{
			double toret = 0;
			double[] data = this.RetrieveData();

			if ( data.Length > 0 ) {
				toret = 1;

				foreach(var x in data) {
					toret *= x;
				}
			}

			return toret;
		}

		public override string Name {
			get { return Id; }
		}

		public const string Id = "Product";
	}
}

redpajama_set_name: RedPajamaGithub


Rewards Start Here With City Power & Gas!
Not only that, but there are over 500,000 ways to redeem your Reward Dollars!
While you may not be able to use all your Reward Dollars on one item, our Best Price Guarantee ensures that you'll receive an unbeatable low price for items purchased via our Rewards site when compared to Amazon! Sign in to your Rewards account & get started today!


text:
Here we go again: Egypt to Bahrain
21 Feb, 2011 by editor
US pledges for democracy may not extend to Bahrain, even if Obama finally supported Egypt's rebellion
The US has been cautious in its statements on the repression of protesters in Bahrain, a key ally [GALLO/GETTY]
It took until Hosni Mubarak was safely in Sharm El Sheikh and newly free Egyptians were celebrating in Tahrir square, but president Obama finally came out firmly for democracy in Egypt, no qualifiers attached.
Obama's words were eloquent indeed; for my money even more so than his 2009 speech in Cairo. As he explained, what the world had witnessed the previous 18 days was truly "history taking place. The people of Egypt have spoken. Their voices have been heard. And Egypt will never be the same… for Egyptians have made it clear that nothing less than genuine democracy will carry the day."
The president went on to detail a set of expectations: protecting the rights of Egypt's citizens, lifting the emergency law, revising the constitution and other laws to make this change irreversible, and laying out a clear path to elections that are fair and free.
Those expectations are entirely in line with the core demands of the organisers of the protests-turned-revolution. For that, Obama deserves credit, although at least some should be held in reserve until we see how much pressure his administration is willing to put on the military to ensure that it carries out a full transition to democracy.
What's more, in changing themselves, Mr. Obama declared that "Egyptians have inspired us". They did so in good measure, he rightly explained, through understanding their full worth, as equal members of the larger human history and community. "Most people have discovered in the last few days that they are worth something, and this cannot be taken away from them anymore. Ever."
Putting inspiration to the test
Yet this inspiration is already being put to the test all across the region as the protests spread like a "freedom virus," as one Cairene taxi driver put it to me the day before I left Cairo.
As I write this column the Bahraini government is in the process of brutally suppressing the protesters in its own version of Tahrir Square, Pearl Square.
If the US is Egypt's primary patron, in Bahrain it is among the ruling family's biggest tenants, as the country is home to the Fifth Fleet, one of the US military's most important naval armadas, crucial to protecting Persian Gulf shipping and projecting US power against Iran.
But while Bahrain has long been depicted as relatively moderate compared with its Salafi neighbor, Saudi Arabia, the reality is that the country is repressive and far from free, as citizens have almost no ability to transform their government, which according to the State Department "restricts civil liberties, freedoms of press, speech, assembly, association, and some religious practices."
In the wake of Egypt, where many people harbor resentment against the Administration for its lack of early support for the democracy movement what can Obama do now? Can he in good conscience acquiesce to the brutal suppression of pro-democracy protesters so soon after his eloquent words and late coming to supporting the Egyptian revolution?
The larger question is: What is more essential to American security today, convenient bases for its ships, planes and troops across the Middle East, or a full transition to democracy throughout the region?
Al-Qaeda 'failure'
The answer is clearly the latter, as evidenced by the fact that America's two primary antagonists in the Middle East, al-Qaeda and the Iranian government, have seen their standing sink in proportion to the rise of the pro-democracy movements.
In any war, cold or hot, propaganda is crucial, and here it is impossible to lose sight of the fact that al-Qaeda has had little if anything to say about the Egyptian revolution precisely because it was a massive non-violent jihad that succeeded miraculously where a decade of al-Qaeda blood and vitriol have miserably failed.
As for Iran, the government's rhetorical support for the Egyptian revolution while it continues to suppress its own democracy movement is clearly emptying the Iranian regime of any remaining credibility as an alternative to the US-dominated order.
In this sense the success-so far-of the Egyptian revolution has presented Obama with a unique window of opportunity to forcefully advocate and press for the same kind of democratic transition across the Middle East and North Africa.
The signs on Tuesday were somewhat optimistic, as the President warned all regional leaders that they should "get ahead of the wave of protest" by moving towards democracy as quickly as possible. Yet Obama refused to mention Bahrain by name in his press conference, even as the government was cracking down on the protesters.
Instead, the US president argued that "each country is different, each country has its own traditions; America can't dictate how they run their societies," an utterly meaningless declaration since it contradicts the very advocacy of democracy that the President has made out of the other side of his mouth.
And now, once again, in the wake of government violence against peaceful citizens, the Obama administration stands silent, refusing to openly condemn the Bahraini government. Is the administration incapable of learning from mistakes in the immediate past ?
In fact, Bahrain isn't even the most important country where the ambivalence of US democracy advocacy continues to frustrate real change.
From Egypt to Israel
Not a single Israeli flag was burned (as far as everyone I know from Tahrir can recall) during the 18 days of protest, but while the Israeli occupation remained tangential to the protests, one of the main sources of initial solidarity and coalition building among the young Egyptians who ultimately helped organise the revolution was the outbreak of the second intifada, which led to the formation of a very active branch in Cairo of the Palestine Solidarity Committee (it's worth noting here that almost no mainstream media analysis of the roots of the youth movement mentions this fact).
Indeed, after I ran into organisers wearing "End the Occupation" t-shirts, it became clear how similar, and interlinked, were the Israeli occupation and the Mubarak "system's" (as the protesters referred to them in their numerous chants to bring it down) occupation of Egypt.
The reality remains that on its own terms, the Israeli occupation (or rather double occupation, as increasing numbers of Palestinians describe their lives under PA/Hamas and Israeli rule) remains among the most repressive and brutal in the contemporary world, and perhaps its most destabilising.
And, as with Mubarak, the United States is the most important supporter and enabler of the occupation's continued presence against the wishes of the vast majority of the people forced to live under it.
And here, as the Palestine Papers released by Al Jazeera reveal, the words and deeds of the Obama administration have run roughshod over its rhetorical commitment to greater democracy and openness.
They reveal that senior members of the administration directly threatened Palestinians leaders with a cut-off in aid should they not follow American policies or even resign in response to continued Israeli settlement expansion and other violations of the Oslo agreements.
The Obama administration needs to tell us if that is still US policy, and if so why democracy is suddenly okay for Egyptians but not for Palestinians, or at least as of today, for Bahrainis.
We also need to know how Obama will respond if the Palestinians take up the mantle of Cairo and march en masse to dismantle sections of the West Bank wall or the Erez crossing in Gaza, in defiance of both Israeli and Palestinian political commands.
And the tests don't get any easier. Bahrain is child's play compared not merely to Yemen, which is a crucial base of Al-Qaeda (or so it is claimed) but even more so for Saudi Arabia, whose absolutely repressive regime is among the worst in almost every category possible, in direct proportion to its immense oil reserves and wealth.
Democracy without hypocrisy
One of the most fascinating and uplifting aspects of Tahrir square was the utter lack of hypocrisy within its confines. Authoritarian societies are by definition filled with double-talk, lies of various shades and a broader climate of hypocrisy which becomes the grease, however rancid, that allows the wheels of society to turn, even if they wind up spinning in their tracks for decades.
In finally supporting the Tahrir experiment, President Obama was, in effect, pledging to end decades of American hypocrisy in its policies towards the Middle East and larger Muslim world.
But in order to live up to this promise he will have to develop one set of policies for all the peoples and countries of the region. And doing that will demand an even more costly break with the past, putting old allies at arm's length until they respect the rights of their peoples while embracing, however tentatively, groups that once seemed more easily characterised as, if not quite foes, then at least untrustworthy partners in securing American interests.
Obama concluded his remarks celebrating the emergence of a new Egypt by saying that the revolution "forever more will remind us of the Egyptian people, of what they did, of the things that they stood for, and how they changed their country and in doing so changed the world."
Let's hope in changing the world, Egyptians haven't left the United States and other major powers too far behind.
Mark LeVine is a professor of history at UC Irvine and senior visiting researcher at the Centre for Middle Eastern Studies at Lund University in Sweden. He has authored several books including Overthrowing Geography: Jaffa, Tel Aviv and the Struggle for Palestine (University of California Press, 2005) and An Impossible Peace: Israel/Palestine Since 1989 (Zed Books, 2009).
The views expressed in this article are the author's own and do not necessarily reflect Al Jazeera's editorial policy.
0 INTERNATIONAL 8 years ago
El factor Bergoglio y la transición argentina
El enigma y el temor de los dueños del país y sus representantes está centrado en la capacidad del
La vía democrática al socialismo 40 años después de Allende
No cabe ninguna duda que Latinoamérica atraviesa un momento de transformaciones sin precedente. Es desde América Latina que se están
Davuto?lu: Turkey will not let Syria become another Lebanon
Ahmet Davuto?lu (Photo: Today's Zaman) ABDULLAH BOZKURT, ANKARATurkish Foreign Minister Ahmet Davuto?lu has vowed not to let Syria become another


text:
Alsodes kaweshkari  è una specie di anfibi anuri appartenente alla famiglia Alsodidae.

Note

Altri progetti

Alsodidae
Fauna sudamericana

redpajama_set_name: RedPajamaWikipedia


Welcome to All Things Through Him! We are a husband and wife creative team, designing tees inspiring a Christ centered conversation. It is our hope that as you wear our designs intentional conversation take place with those around you and you are reminded who you are in Christ.


text:
An independent British-Dutch press
The Frontier: 28 Contemporary Ukrainian PoetsConversations before Silence
HomeShopLiteratureContours of the City
Home / Shop / Modern Literary Fiction / Contours of the City
Contours of the City
Author: Attyla Mohylny
Contours of the City arguably comprises one of the finest collections of free verse ever written in Ukrainian even though it was largely overlooked when it first appeared during the political transition to Ukrainian independence in 1991.
Book Format Choose an optionHardcoverPaperbackEPUBKindlePDF Clear
Contours of the City quantity
SKU: N/A Categories: Literature, Modern Literary Fiction, Poetry, Ukrainian books Tag: Ukrainian Literature ISBN: N/A Product ID: 2541
Contours of the City arguably comprises one of the finest collections of free verse ever written in Ukrainian even though it was largely overlooked when it first appeared during the political transition to Ukrainian independence in 1991. It certainly deserves a broader audience both in Mohylny's homeland as well as in the wider world. While it may be described as a one-hit wonder because of the poet's premature death, it remains a brilliant hit for all time.
Translator Michael Naydan received the Eugene Kayden Meritorious Achievement Award in Translation from the University of Colorado for a partial manuscript of his translations of Mohylny's poetry into English in 1993. This edition includes a complete translation of Mohylny's collection Contours of the City along with several poems translated by Virlana Tkacz and Wanda Phipps.
Be the first to review "Contours of the City" Cancel reply
Attyla Mohylny, son of the Ukrainian poet Vit Vitko, was born on September 16, 1963 in Kyiv, Ukraine, and died all too prematurely on September 3, 2008 at the age of 45. The poet was named after the saint Attila and not the Hun of more historical renown. He completed his philology degree at Taras Shevchenko Kyiv State University and worked mostly as a teacher, editor and journalist during his abbreviated lifetime. He continued his studies while working in Dushanbe, Tadzhikistan, first as a group leader of The Young Pioneers, then as a teacher in the Medical Institute until 1985. Following his travels to Tadzhikistan, in Kyiv he tried his hand at journalism for the newspaper Evening Kyiv. Since then Mohylny had an off and on career as a teacher and journalist. He worked as an editor in the Molod Publishing House, and from 1987 taught occasionally at Kyiv and Warsaw Universities. He worked in television, writing film scripts for children's shows. He authored two books of poetry early in his career: Rattling above the Rooftops (1987) and Contours of the City (1991) along with the text for the exquisitely illustrated children's book Mavka and the Ant King in 2006. He continued to work on writing short stories and a novel until his death.
Mohylny was part of the transitional and transformational group of Ukrainian writers who dramatically turned from Soviet-imposed censorship to create new directions and a new poetics for Ukrainian culture. He is conspicuous among his peers as a poet exclusively of the city, one of the late 1980s generation of urban intellectuals who lived and breathed the pulsating rhythms of the capital city of Kyiv's urban landscapes. The cohort with whom he often interacted in his youth included the now prominent poets and writers Yuri Andrukhovych, Oksana Zabuzhko, Ihor Rymaruk, Vasyl Herasymiuk, Ivan Malkovych, Ihor Rymaruk, and Viktor Neborak. The poetry of Mohylny's collection Contours of the City completely breaks with the tradition of rhyme and meter that dominated Ukrainian poetics until only recently and, except for Kyivan realia and allusions to Ukrainian history, fits seamlessly into Western late modernity.
Attyla Mohylny
Hardcover, Paperback, EPUB, Kindle, PDF
Laurus (Dutch edition)
€9.95 – €22.50 Select options
The 12 Apostles of Russian Law
One-Two
Girls, be Good
Good Stalin
The Tale of Aypi
Death of the Snake Catcher
Don't Call me a Victim!
The Time Of Women
Little Zinnobers
Ravens before Noah
Wolf Messing
Maybe We're Leaving
Moscow in the 1930s: A Novel from the Archives
Leonardo's Handwriting
A Poet and Bin-Laden
Mirror Sand: An Anthology of Russian Short Poems
METRO 2033 (Dutch edition)
The Investigator
The Secret History of my Sojourn in Russia
Multiple Personalities
English translations of fiction and non-fiction titles by Russian, Ukrainian, Belarusian, Polish, Serbian, Turkmen, Armenian and Azerbaijan authors.
Film and Theatre Permissions
Glagoslav Publications Ltd.
43 Berkeley Square
W1J 5AP London
Tel.: + 44 20 32 86 99 82
contact(at)glagoslav.com
Glagoslav Publications B.V.
Zandheuvel 52 B
4901HW Oosterhout
Tel.: +31 162 796 51 9
Copyright © 2021 · All rights reserved · Glagoslav Publications Ltd. · UK Company No. 07642591 · Trade Register NL: 52779815


Towards the end of February 100 years ago the word began to go around that despite all their problems Woolwich Arsenal did indeed have at least one terrific young player.
He was 17 years old and playing in the reserves. There is a report of a match between the Reserves and Croydon Common in the London League which Woolwich Arsenal won 3-1 . Charlie Buchan scored one of the goals.
There are records of Buchan playing at least three games from the reserves and of him training twice a week as an amateur – which was fairly common in the build up to singing professional forms.
But the story is that what happened at the end of February 1910 is that Buchan handed the club a bill of 11 shillings (55p) for his travel costs to and from the ground. The club refused to reimburse him. As a result, Buchan refused to play any more games for the club.
Charlie Buchan then played for Northfleet in the Kent League, until footballing scouts became aware of him and Bury offered him wages of £3 a week to sign professional.
At this stage, Henry Norris became involved and tried to get Buchan to go to Fulham. Norris told Buchan he could be a teacher (which he wanted to be) and a footballer. Norris offered him £1 10s a week but Buchan wanted £2, and the deal fell through.
After that Buchan turned up on the books at Leyton in the Southern League. The local paper reported that Buchan managed to get £3 a week at Leyton and at the same time as playing did teacher training at a nearby college. That was significantly more than Fulham offered, and he was playing in a lower league.
The Leyton files show Buchan first played versus Plymouth Argyle in September 1909 and played regularly thereafter. Reports suggested he was the best thing to happen to Leyton for years.
Today on Making the Arsenal: Charlie Buchan's first appearance for Arsenal.
Almunia: are we being honest?
The manager's resigned, the league's ending… Where next for Arsenal?
Untold Rumours appear from time to time on Untold Arsenal usually near the end of the page.


text:
Q: Would this still hold true if the probabilities of A and B followed a normal distribution? Part a)
Let A be the number that the left-hand die shows. Let B be the number that the right-hand
die shows.
Both dice are fair and therefore the probability that B is greater than A is equal to the probability that B is less than A (i.e. P(B > A) = P(B < A)). Furthermore, all possibilities can be summarized by B > A, B < A, and B = A. Therefore
P(B > A) + P(B < A) + P(A = B) = 1
Note that P(A = B) is 1/6 because whatever number B shows, A will show the same number
one out of six times. Therefore equation 1 becomes:
P(B > A) + P(B < A) + 1/6 = 1
Since P(B > A) = P(B < A), we can arrive at our solution with:
2P(B > A) = 1 − 1/6 = 5/6
Therefore
P(B > A) = 5/12
The probability that the right-hand die shows a larger number than the left-hand die is 5/12
Part b)
Given that the left hand die is rolled first and it shows 5 (i.e. A = 5). What is P(B >
A|A = 5)? The answer is 1/6 because to be greater than A = 5, die B must show 6 (which
occurs one out of six times for a six sided die).

A: For two independent identically distributed random variables $X$ and $Y$ that have a continuous distribution (such as the normal), the situation is even simpler. Since $\Pr(X=Y)=0$, we get that $\Pr(X\gt Y)=\frac{1}{2}$.
Analogues of the second question can be solved in the continuous context, usually by an integration. One nice thing is that we do not have to distinguish between $\lt$ and $\le$.  This is because if $X$ has continuous distribution, then, for example, $\Pr(X=5)=0$.

A: For a, as long as both dice follow the same distribution, normal, uniform, or whatever, the probability of each die being higher is the same.  This gives you $P(B \gt A) = \frac 12(1-P(A=B))$.  Usually the normal distribution is a continuous one so the chance of equality is zero.
For b $P(B \gt A|A=5)=P(B\gt 5)$.  Again, is the distribution of $B$ continuous?

redpajama_set_name: RedPajamaStackExchange


text:
\section{Introduction}
\label{sec:intro}
\def\Alph{section}.\arabic{equation}{\arabic{section}.\arabic{equation}}
\setcounter{equation}{0}

Due to the spontaneous chiral symmetry breaking  of strong interactions  \cite{nambu,gellman,weinberg,witten}
strong constraints among the interactions between the lightest pseudoscalars
arise, which are most efficiently derived in the framework of Chiral Perturbation Theory (CHPT) \cite{wein,physica,gas1,gas2}. For the isospin ($I$) 0,~1 and 1/2 the scattering of the pseudoscalars in S-wave is strong enough to  generate dynamically the lightest scalar resonances, namely, the $f_0(980)$, $a_0(980)$,
$\kappa$ and $\sigma$, as shown in refs.~\cite{npa,doba,iamprl,iamcc,nd}.
Still one can make use of the tightly constrained interactions among the lightest pseudoscalars in order to work out approximately the scattering between the latter mesons and scalar resonances, as we show below. We concentrate here on the much narrower resonances $f_0(980)$ and $a_0(980)$ and
consider their interactions  with the pseudoscalars $\pi$, $K$, $\eta$ and $\eta'$.  If these interactions are strong enough new pseudoscalar resonances with $J^{PC}=0^{-+}$ would come up.
This is the case and the resulting pseudoscalar resonances have a mass larger than 1~GeV
(this energy limit is close to the masses of the $f_0(980)$ or $a_0(980)$), typically following the relevant scalar-pseudoscalar thresholds.

The problem of the excited pseudoscalars above 1~GeV is interesting by itself. These resonances are not typically well-known  \cite{pdg}. In $I=1/2$ one has
the $K(1460)$ and $K(1630)$ resonances.
 The $I=1$ resonances $\pi(1300)$, $\pi(1800)$ are  somewhat better known \cite{pdg}. They are broad resonances with a large uncertainty in the width
of the former, which is reported to range between 200-600~MeV in the PDG \cite{pdg}. Some controversy exists for interpreting the decay
channels of the $\pi(1800)$ within a quarkonium picture \cite{barnes,klempt}.
 It was suggested in \cite{barnes} that together with the second radial excitation of the pion there would be a hybrid resonance somewhat higher in mass \cite{barnes,hydecays}. Special mention deserves the $I=0$ channel where the $\eta(1295)$,
$\eta(1405)$, $\eta(1475)$ have been object of an intense theoretical and
experimental study. For an exhaustive review on the experiments performed
on these resonances and the nearby  $1^{++}$ axial-vector resonance $f_1(1420)$ see ref.~\cite{masoni_rev}. Experimentally it has been established that while the $\eta(1405)$ decays mainly to
$a_0\pi$ the $\eta(1475)$ decays to $K^*\bar{K}+c.c$ \cite{pdg,masoni_rev}. In this way, the study of the $\eta\pi\pi$ system is certainly the most adequate one
for isolating the $\eta(1405)$ resonance because both the $f_1(1420)$ and
$\eta(1475)$ have a suppressed partial decay width to this channel \cite{pdg}. Refs.~\cite{pdg,masoni_rev} favor the interpretation of considering the
$\eta(1295)$ and $\eta(1475)$ as ideally mixed states (because the $\eta(1295)$
and the $\pi(1300)$ are close in mass) of the same nonet of pseudoscalar resonances with the other members being the $\pi(1300)$ and  $K(1460)$. All these resonances would be the first radial excitation of the lightest pseudoscalars \cite{barnes}.
 The $\eta(1405)$ would then be an extra state in this classification whose clear signal in gluon-rich process, like $p\bar{p}$ \cite{crystal,obelix} or $J/\Psi$ radiative decays \cite{mark,dm2}, and its absence in $\gamma\gamma$ collision \cite{l3}, would favor its interpretation as a
glueball in QCD \cite{chano,close}.
However, this interpretation opens in turn a serious problem because present results from lattice QCD
predict the lowest mass for the pseudoscalar glueball at around 2.4~GeV \cite{bali,morn,chen}.
 Given the success of the lattice QCD prediction for the lightest scalar glueball, with a mass at around 1.7~GeV \cite{miguel,chano2}, this
discrepancy for the pseudoscalar channel would be quite exciting. QCD sum rules \cite{ns} give a mass
 for the lightest pseudoscalar gluonium of $2.05\pm 0.19$~GeV and an upper bound
 of $2.34\pm 0.42$~GeV.
 However, the $\eta(1405)$ would fit as a $0^{-+}$ glueball if the latter is
 a closed gluonic fluxtube  \cite{faddev}.
On the other hand, it has also been pointed out that the mass and properties of the $\eta(1405)$ are consistent with predictions for a gluino-gluino bound state \cite{17,18,close}.
 The previous whole picture for classifying the lightest pseudoscalar resonances has been challenged in ref.~\cite{klempt}. The authors question the existence of the $\eta(1295)$ and argue that, due to a node in the $^3 P_0$ wave function
 of the $\eta(1475)$ \cite{1007}, only one isoscalar pseudoscalar resonance in the 1.4-1.5~GeV region exists.
 This node shifts the resonant peak position depending on the channel, $a_0\pi$ or $K^*\bar{K}+c.c$.
 It has been also recently observed by the BES Collaboration the resonance $X(1835)$ with quantum numbers favored as a pseudoscalar $0^{-+}$ resonance
both in   $J/\Psi\to \gamma p\bar{p}$ \cite{ablikim03} and in
$J/\Psi\to \gamma \pi^+ \pi^-\eta^{\prime}$ \cite{ablikim05}. For the former decay ref.~\cite{johan} offers an alternative explanation in terms of the $p\bar{p}$ final state interactions.

We consider here  the S-wave interactions between
the scalar resonances $f_0(980)$ and $a_0(980)$ with the pseudoscalar mesons $\pi$, $K$,
$\eta$ and $\eta'$.  The approach followed is an extended version of the one that refs.~\cite{alva1,alva2} applied to study the S-wave interactions  of the $\phi(1020)$ with the $f_0(980)$ and $a_0(980)$ resonances, respectively. We show that the interactions derived generate resonances  dynamically
that can be associated with many of the previous pseudoscalar resonances listed above, namely, with the $K(1460)$, $\pi(1300)$, $\pi(1800)$, $\eta(1475)$ and
$X(1835)$.
In this way, new contributions to the physical resonant signals result from this novel mechanism not explored so far. In addition, we also study other exotic channels and find that the $I=3/2$ $a_0 K$ channel could also be resonant.

	After this introduction we present the formalism and derive the S-wave scattering amplitudes for scalar-pseudoscalar interactions in section \ref{sec2}.
Section~\ref{sec3} is dedicated to present and discuss the results. Conclusions
	are given in section~\ref{sec4}.

\section{Formalism. Setting the model}
\label{sec2}

\begin{figure}\centering
\includegraphics[height=5cm,keepaspectratio]{diagrama1.eps}
\caption{Triangle loop for calculating the interacting kernel for
$S_1(p_1) P_1(k_1) \to S_2(p_2) P_2(k_2)$, where between brackets the four-momentum
for each particle is given.
$S_{1,2}$ represents the initial, final scalar resonances and similarly for $P_{1,2}$ regarding
the pseudoscalar mesons.
\label{fig:tri}}
\end{figure}

Our approach is based on the triangle diagram shown in Fig.~\ref{fig:tri} where an
incident scalar resonance $S_1$ decays into a virtual $K\bar{K}$ pair.
 The filled dot in the vertex on the
bottom of the diagram corresponds to the interaction of the incident (anti)kaon in the loop with
the pseudoscalar $P_1$ giving rise to the  pseudoscalar $P_2$ and the same (anti)kaon.
The out-going scalar resonance is denoted by $S_2$.
The basic point is that this diagram is enhanced because the masses
 of  both  the $f_0(980)$ and  $a_0(980)$ resonances
 are very close to the $K\bar{K}$ threshold.
In this way, for scattering near the threshold of the reaction, one of the
kaon lines in the bottom of the diagram is almost on-shell. Indeed, at threshold and in the limit  for the mass of the scalar equal to twice the kaon mass this diagram becomes infinite.
This fact is discussed in detail in ref.~\cite{alva1} where it was already applied  for studying successfully the $\phi(1020)f_0(980)$ scattering
and the associated $1^{--}$ $Y(2175)$ resonance. The  BABAR \cite{babar} and BELLE \cite{belle} data on $e^+e^-\to \phi(1020)f_0(980)$ were  reproduced accurately, where a strong peak for the latter resonance arises. An important conclusion of \cite{alva1} is that the $Y(2175)$ can be qualified as being a
resonance dynamically generated due to the interactions between the $\phi(1020)$ and the $f_0(980)$
resonances, see also ref.~\cite{oset}.  This work was extended to $I=1$ in \cite{alva2} for studying the $\phi(1020)a_0(980)$ S-wave. There it was remarked the interest of measuring the cross sections $e^+e^-\to \phi(1020)\pi^0\eta$ because it is quite likely that an isovector companion of the $Y(2175)$ appears. In our
present study, as well as in refs.~\cite{alva1,alva2}, one takes advantage of the fact that both the
$f_0(980)$ and $a_0(980)$ resonances are dynamically generated by the
meson-meson self-interactions \cite{npa,nd,mixing}. This conclusion
is also shared with other approaches like refs.~\cite{juelich,isgur}. In this way, we can calculate the couplings of the scalar resonances considered
to two pseudoscalars, including their relative phase.
 The coupling of the $f_0(980)$ and $a_0(980)$ resonances to a $K\bar{K}$ pair in $I=0$ and 1, respectively, is denoted by $g_{f_0}$ and $g_{a_0}$.
  These states $|K\bar{K}\rangle_{I=0}$ and
 $|K\bar{K}\rangle_{I=1}$  are given by
 \begin{align}
 |K\bar{K}\rangle_{I=0}&=-\frac{1}{\sqrt{2}}|K^+K^- + K^0\bar{K}^0\rangle~,\nonumber\\
 |K\bar{K}\rangle_{I=1}&=-\frac{1}{\sqrt{2}}|K^+K^- - K^0\bar{K}^0\rangle~.
 \end{align}
 In this way, the $f_0(980)$ couples to $K^+K^-$($K^0\bar{K}^0$) as
 $-\frac{1}{\sqrt{2}}$($-\frac{1}{\sqrt{2}}) g_{f_0}$ while the $a_0(980)$ couples as  $ - \frac{1}{\sqrt{2}}(\frac{1}{\sqrt{2}})g_{a_0}$.

 Let us indicate  by $P$ the total four-momentum $P=p_1+k_1=p_2+k_2$ in Fig.~\ref{fig:tri}.
  This diagram is given by $g_1 g_2 L_K$, with $g_1$ and $g_2$ the coupling of the initial and final scalar resonance to a $K\bar{K}$ pair, respectively, and
$L_K$ is given by
 \begin{align}
 L_K&= i \int\frac{d^4\ell}{(2\pi)^4}\frac{T((P-\ell)^2)}{(\ell^2-m_K^2+i\varepsilon)((p_1-\ell)^2-m_K^2+i\varepsilon)
 ((p_2-\ell)^2-m_K^2+i\varepsilon)}~.
 \label{tl.ref}
 \end{align}
  In this equation $T((P-\ell)^2)$ represents the interaction amplitude between the kaons with the external pseudoscalars.
 Here, we employ
the meson-meson scattering amplitudes obtained in ref.~\cite{nd} but now enlarged
so that states with the pseudoscalar  $\eta'$ are included in the
calculation of  $T((P-\ell)^2)$, as detailed in appendix~\ref{app:fits}. Interestingly,
these amplitudes contain the poles corresponding to the scalar resonances $\sigma$, $\kappa$,
$f_0(980)$, $a_0(980)$ and other poles in the region around 1.4~GeV \cite{nd}.

In order to proceed further we have to know the dependence of $T((P-\ell)^2)$ on its argument that
includes the integration variable $\ell$. This can be done by writing the dispersion relation satisfied by $T(q^2)$ which is of the form
\begin{align}
T(q^2)&=T(s_A)+\sum_i\frac{q^2-s_A}{q^2-s_i}\frac{\hbox{Res}_i}{s_i-s_A}
+\frac{q^2-s_A}{\pi}\int_{s_{th}}^\infty ds'\frac{\hbox{Im}T(s')}{(s'-q^2)(s'-s_A)}~.
\label{dis.rel}
\end{align}
One subtraction at $s_A$ has been taken because $T(q^2)$ is bound by a constant
for $q^2\to\infty$, with $T(s_A)$ the subtraction constant. Typically, poles are also present deep in the $q^2$-complex plane located at $s_i$ whose residues are Res$_i$.
These poles appear on the first Riemann sheet and are an artifact of the parameterization employed \cite{nd,pseudo}. For $q^2$ along the physical region they just give rise to soft extra contributions that could be mimic by a polynomial  of low degree in $q^2$. Inserting eq.~\eqref{dis.rel}
into eq.~\eqref{tl.ref}, with $(P-\ell)^2=q^2$, one can write for  $L_K$
\begin{align}
L_K&=\left(T(s_A)+\sum\frac{\hbox{Res}_i}{s_i-s_A}\right)C_3
+\sum_i C_4(s_i) \hbox{Res}_i \nonumber\\
&-\frac{1}{\pi}\int_{s_{th}}^\infty ds' \hbox{Im}T(s')
\left[\frac{C_3}{s'-s_A}+C_4(s') \right]~.
\label{tl.dis}
\end{align}
Here we have introduced the three- and four-point Green functions $C_3$ and $C_4(M_4^2)$ defined by
\begin{align}
C_3&=i\int\frac{d^4\ell}{(2\pi)^4}\frac{1}{(\ell^2-m_K^2+i\varepsilon)((p_1-\ell)^2-m_K^2+i\varepsilon)
 ((p_2-\ell)^2-m_K^2+i\varepsilon)}~,\nonumber\\
 C_4(M_4^2)&=i\int\frac{d^4 \ell}{(2\pi)^4} \frac{1}{(\ell^2-m_K^2+i\varepsilon)((p_1-\ell)^2-m_K^2+i\varepsilon)
 ((p_2-\ell)^2-m_K^2+i\varepsilon)}\nonumber\\
 &\times \frac{1}{((P-\ell)^2-M_4^2+i\epsilon)}~.
 \label{c3.c4.def}
\end{align}
Notice that $M_4^2$ can be real positive (when $M_4^2=s'$ in the dispersion relation), but it could
also be negative or even complex when $M_4^2=s_i$ from the poles. One has still to perform the
angular projection for $C_3$ and $C_4(M_4^2)$. Once this is done, eq.~\eqref{tl.dis} can
still be used but with $C_3$ and $C_4(M_4^2)$ projected in S-wave, as we take for granted
in the following. These functions and their
S-wave projection are discussed in appendix~\ref{app:c3.c4.pro}. For $S_1(p_1) P_1(k_1)\to S_2(p_2) P_2(k_2)$ we have the usual Mandelstam variables
$s=(p_1+k_1)^2=(p_2+k_2)^2$, $t=(p_1-p_2)^2=(k_1-k_2)^2$ and $u=(p_1-k_2)^2=(p_2-k_1)^2=
M_{S_1}^2+M_{S_2}^2+M_{P_1}^2+M_{P_2}^2-s-t$, with the masses of the particles indicated by $M$ with the subscript distinguishing between them. The dependence on the relative angle
$\theta$  enters in $t$ as
$t=(p_1^0-k_1^0)^2-(\mathbf{p}-\mathbf{p}')^2=(p_1^0-k_1^0)^2-\mathbf{p}^2-\mathbf{p}'^2+2|\mathbf{p}||\mathbf{p}'|\cos\theta$ with $\mathbf{p}$ and
$\mathbf{p}'$ the CM three-momentum of the initial and final particles, respectively.

 Eq.~\eqref{tl.dis} is our basic equation for evaluating the interaction kernels. One has
 only to specify the pseudoscalars actually involved in the amplitude $T(q^2)$ according to the
 specific reaction under consideration.  We now list all the channels involved for the different quantum numbers and indicate the actual pseudoscalar-pseudoscalar amplitudes required as the argument of $L_K$:

 \begin{itemize}
\item{$I=0$, $G=+1$}
	\begin{align}
T_L(a_0\pi \to a_0\pi)&=\frac{2 g_{a_0}^2}{3}L_K[4 \,T_{\pi K\to \pi K}^{I=3/2}
-T_{\pi K\to \pi K}^{I=1/2}]~,\nonumber\\
T_L(a_0\pi \to f_0\eta)&=2 g_{f_0}g_{a_0}L_K[T_{\eta K\to \pi K}^{I=1/2}]~,\nonumber\\
T_L(f_0\eta\to f_0\eta)&=2g_{f_0}^2 L_K[T_{\eta K \to \eta K}^{I=1/2}]~,\nonumber\\
T_L(a_0\pi\to f_0\eta')&=2 g_{f_0}g_{a_0} L_K[T_{\eta' K\to \pi K}^{I=1/2}]~,\nonumber\\
T_L(f_0\eta \to f_0\eta')&=2 g_{f_0}^2 L_K[T_{\eta K\to \eta' K}^{I=1/2}]~,\nonumber\\
T_L(f_0\eta'\to f_0\eta')&=2 g_{f_0}^2 L_K[T_{\eta' K\to \eta' K}^{I=1/2}]~.
	\label{n.i0}
	\end{align}

\item{$I=1/2$}
 \begin{align}
T_L(f_0 K\to f_0 K)&=\frac{g_{f_0}^2}{2} L_K[3 \,T_{K\bar{K}\to K\bar{K}}^{I=1} +T_{K\bar{K}\to K\bar{K}}^{I=0}]~, \nonumber\\
T_L(f_0K \to a_0 K)&=\frac{\sqrt{3} g_{f_0}g_{a_0}}{2} L_K[T_{K\bar{K}\to K\bar{K}}^{I=1}  - T_{K\bar{K}\to K\bar{K}}^{I=0}]~,\nonumber\\
T_L(a_0 K\to a_0 K)&=\frac{g_{a_0}^2}{2}L_K[3\, T_{K\bar{K}\to K\bar{K}}^{I=0}+ T_{K\bar{K}\to K\bar{K}}^{I=1}]~.
 \label{n.i12}
 \end{align}

\item{$I=1$, $G=-1$}
	\begin{align}
T_L(f_0\pi\to f_0\pi)&=\frac{2 g_{f_0}^2}{3}L_K[2\,T_{\pi K\to \pi K}^{I=3/2}
+T_{\pi K\to \pi K}^{I=1/2}]~,\nonumber\\
T_L(f_0\pi\to a_0\eta)&=\frac{2 g_{f_0} g_{a_0}}{\sqrt{3}}L_K[T_{\pi K\to \eta K }^{1/2}]~,\nonumber\\
T_L(a_0\eta\to a_0\eta)&=2 g_{a_0}^2 L_K[T_{\eta K\to \eta K}^{I=1/2}]~,\nonumber\\
T_L(f_0\pi\to a_0\eta')&=\frac{2 g_{f_0}g_{a_0}}{\sqrt{3}}L_K[T_{\pi K\to \eta' K}^{I=1/2}]~,\nonumber\\
T_L(a_0\eta\to a_0\eta')&=2 g_{a_0}^2L_K[T_{\eta K\to \eta' K}^{I=1/2}]~,\nonumber\\
T_L(a_0\eta'\to a_0\eta')&=2 g_{a_0}^2 L_K[T_{\eta' K\to \eta' K}^{I=1/2}]~.
	\label{n.i1.gm1}
	\end{align}

\item{$I=1$, $G=+1$}
	\begin{align}
T_L(a_0\pi\to a_0\pi)&=\frac{2 g_{a_0}^2}{3}L_K[4T_{\pi K\to \pi K}^{I=1/2}-T_{\pi K\to \pi K}^{I=3/2}]~.
	\label{n.i1.gp1}
	\end{align}

\item{$I=3/2$}
	\begin{align}
	T_L(a_0 K\to a_0 K)&=2g_{a_0}^2 L_K[T_{K\bar{K}\to K\bar{K}}^{I=1}]~.
\label{n.i32}
	\end{align}
 \end{itemize}

In the previous equations the different scalar-pseudoscalar states are pure isospin ones corresponding to the isospin $I$  indicated  for each item. This also applies to the
pseudoscalar-pseudoscalar states, with $I$ as indicated in the
 superscript of $T$. The symbol $G$ refers to G-parity. On the other hand the $I=3/2$ $\pi K$ amplitude, being much smaller than the $I=1/2$ one, has negligible effects, although it has been kept in the previous expressions.

\begin{figure}[h]\centering
\includegraphics[width=.95\textwidth,angle=0]{unita.eps}
\caption{Iteration of the interaction kernels (denoted by the triangles in the figure) by
inserting scalar(double lines)-pseudoscalar(dashed lines) intermediate states.
\label{fig:uni.res}}
\end{figure}

For each set of quantum numbers specified by the isospin $I$ and G-parity $G$ (if the latter is not defined this label should be omitted) we join in a symmetric matrix ${\cal T}_{IG}$ the different
 $T_L(i\to j)$ calculated above. Then, in order to resum the unitarity loops, as indicated
 in Fig.~\ref{fig:uni.res}, and obtain  the final  S-wave scalar-pseudoscalar T-matrix, $T_{IG}$,
 we make use of the equation
 \begin{align}
T_{IG}&=\left[I+{\cal T}_{IG}\cdot g_{IG}(s)\right]^{-1}\cdot {\cal T}_{IG}~.
\label{t.uni}
\end{align}
For a general derivation of this equation, based on the N/D method \cite{chew}, see refs.~\cite{nd,plb} and ref.~\cite{npa}, where it is connected with the Bethe-Salpeter
equation. In eq.~\eqref{t.uni} $g_{IG}(s)$ is a diagonal matrix whose elements are
the scalar unitarity loop function with a scalar-pseudoscalar intermediate state.
For the calculation of $g_{IG}(s)_i$, corresponding to  the $i_{th}$
state with the quantum numbers $IG$ and made up by  the scalar resonance
$S_i$ and the pseudoscalar $P_i$, we make use of a once subtracted dispersion relation \cite{nd}. The result is
\begin{align}
g_{IG}(s)_i&=\frac{1}{(4\pi)^2}\left\{a_1+\log\frac{M_{S_i}^2}{\mu^2}
-\frac{M_{P_i}^2-M_{S_i}^2+s}{2 s}\log\frac{M_{S_i}^2}{M_{P_i}^2} \right.\nonumber\\
&\left.+\frac{|\mathbf{p}|}{\sqrt{s}} \Biggl[
\log(s-\Delta+2\sqrt{s}|\mathbf{p}|)+\log(s+\Delta+2\sqrt{s}|\mathbf{p}|)\right.\nonumber\\
&\left.-\log(-s+\Delta+2\sqrt{s}|\mathbf{p}|)
-\log(-s-\Delta+2\sqrt{s}|\mathbf{p}|)
\Biggr]\right\}
\label{g.func}
\end{align}
with $|\mathbf{p}|$ the three-momentum of the channel $S_i P_i$ for a given $s$ and
$\Delta=M_{P_i}^2-M_{S_i}^2$. The subtraction $a_1$
is restricted to have natural values so that the unitarity scale \cite{alva1} $4\pi f_\pi/\sqrt{|a_1|}$
 becomes not too small (e.g. below the $\rho$-mass) so that $|a_1|\lesssim 3$. In addition,
 we require the sign of $a_1$ to be negative so that resonances could be generated when the interaction kernel is positive (attractive).

As already indicated in ref.~\cite{alva2} to ensure a continuous limit to zero $a_0(980)$ width, one has to evaluate ${\cal T}_{IG}$ at the $a_0(980)$ pole position with positive imaginary part so that $p_{1,2}^2 \to {\rm Re}\,[M_{a_0}]^2 + i \epsilon$, in agreement with Eq.~\eqref{tl.ref}. Instead, in $g_{IG}(s)_{a_0 P}$, with $P$ one of the lightest pseudoscalars,  $M_{a_0}$ should appear with a negative imaginary part to guarantee that, in the zero-width limit, the sign of the imaginary part is the same as dictated by the $-i \epsilon$ prescription for masses squared of the intermediate
states.  Such analytical extrapolations in the masses of external particles are discussed in Refs.~\cite{barton,bar1,bar2}. The same applies of course to the case of the $f_0(980)$ resonance.

\section{Results}
\label{sec3}

In this section we show the results that follow by applying eq.~\eqref{t.uni} to the different
channels characterized by the quantum numbers $IG$, as given in the list from eq.~\eqref{n.i0} to
eq.~\eqref{n.i32}.
 As discussed after  eq.~\eqref{g.func} we consider values for the subtraction constant such that
 they are negative and not very large in modulus ($|a_1|\lesssim 3$). In this way, the resonances generated
might be qualified as dynamically generated due to the iteration of the unitarity loops. The pole positions and
couplings of the $f_0(980)$ and $a_0(980)$ resonances are given in Tables~\ref{tab:fit_poles_1} and \ref{tab:fit_poles_2}, respectively, and they correspond to those obtained
in the meson-meson S-wave amplitudes used, see appendix~\ref{app:fits}.
We present the results for each of the channels with definite $IG$ separately.

\begin{figure}[h]
\includegraphics[width=\textwidth,keepaspectratio]{I12.eps}
\caption{Modulus squared of the $f_0 K\to f_0 K$ (left)  and $a_0 K\to a_0 K$ (right) S-wave amplitudes for $a_1=-0.5$~. The points correspond
to the energies where the amplitudes have been actually calculated.
\label{fig:t2.k12}}
\end{figure}

\subsection{$I=1/2$}
First we show the results for the $I=1/2$ sector that couples together the  channels $f_0(980) K$ and $a_0(980) K$.
 We show the modulus
squared of the $f_0 K\to f_0 K$ and $a_0 K\to a_0 K$ S-wave amplitudes in the left and right panel of Fig.~\ref{fig:t2.k12},
respectively. We obtain a clear resonant peak with its maximum at $1460$~MeV for $a_1$ around $-0.5$, that
corresponds to the nominal mass of the $K(1460)$ resonance \cite{pdg}. The results are not
very sensitive to the actual value of $a_1$ but the position of the peak displaces to lower values for decreasing
$a_1$ and the width somewhat increases.   The  visual width of the peak is around 100~MeV, although it appears wider in $a_0 K\to a_0 K$ scattering.
In refs.~\cite{daum,branden} a larger width of around 250~MeV is referred. One has to take into account that the channel $K^*(892)\pi$ is not
included and it seems  to couple strongly with the $K(1460)$ resonance \cite{pdg}.  It is also clear from the figure
 that the peak is asymmetric due to the opening of the $f_0 K$ and $a_0 K$ thresholds involved.
 Taking into account the relative sizes  of the peaks in the left and right panels of
 Fig.~\ref{fig:t2.k12} one infers that the $K(1460)$ couples more strongly to $f_0 K$
 than to  $a_0 K$, with the ratio of couplings as $|g_{f_0K}/g_{a_0K}|\simeq (\frac{20.2}{5.7})^{1/4}\simeq 1.4$~.

\begin{figure}[h]
\includegraphics[width=\textwidth,keepaspectratio]{I1.eps}
\caption{Modulus squared of the $a_0 \eta'\to a_0 \eta'$ (left)  and
$a_0 \eta\to a_0 \eta$ (right) S-wave amplitudes.
 For the former $a_1=-1.3$ and for the latter $a_1=-2.0$, see the
 text for details. The notation is as in Fig.~\ref{fig:t2.k12}.
\label{fig:t2.pi1}}
\end{figure}

\subsection{$I=1$}
We now consider the $I=1$ case. As commented in the introduction two broad resonances are referred in the PDG, the $\pi(1300)$ and $\pi(1800)$.
In our amplitudes we find quite independently of the value of $a_1$ that
the $a_0(980)\eta'$ channel is almost elastic. This is due to the fact that
the interaction kernels ${\cal T}(a_0\eta'\to a_0\eta)$ and ${\cal T}(a_0\eta'\to f_0\pi)$ are much smaller than the rest of kernels, typically by an order of magnitude. This happens because the kernels are dominated by the threshold region. However, the threshold for $a_0(980)\eta'$  is much
higher than the thresholds for the other two channels. In this way,
for the inelastic processes involving the $a_0\eta'$ channel, even at threshold
for one of the channels, there is always a large three-momentum for the
 other channel and the kernel is suppressed. Of course, this does not apply for the $a_0\eta'$ elastic case where the kernel has a standard size and produces around 1.8~GeV a strong resonant signal that could be associated with the
 $\pi(1800)$ resonance. To reproduce the mass value given in the PDG \cite{pdg} for this resonance, $1816\pm 14$~MeV one takes $a_1$ for $a_0 \eta'$ around -1.3. The visual width of the peak is around 200~MeV, close to the width quoted in the
 PDG \cite{pdg} of $208\pm 12$~MeV. The other two channels couple
 quite strongly between each other and typically give rise to an enhancement between 1.2-1.4~GeV when varying $a_1$ equal for each of them, which could be associated with the $\pi(1300)$. However,
 for $|a_1|$ between 1 and  1.8 a too strong signal in the $a_0\eta$ threshold originates. For $|a_1|$ below 1 the resonant peak in the $|T(a_0\eta\to a_0\eta)|^2$  lies around 1.4-1.5~GeV, somewhat too high for the $\pi(1300)$ resonance \cite{pdg}. This is why we show in Fig.~\ref{fig:t2.pi1} the modulus squared
 of $a_0\eta\to a_0\eta$ for $a_1=-2$ where a peak close to 1.2~GeV is seen with a width of around 200~MeV. One can also see the strong effect of the $a_0 \eta$ threshold at around 1.52~GeV. Its  size is rather sensitive
 to the actual vale of $|a_1|$ when this lies between 1 and 1.8.
 There is the interesting fact, which is independent of the value of $a_1$,
 that there is no signal for $\pi(1800)$ in the $a_0\eta$ system nor
 signal of the peak at 1.2~GeV in the $a_0\eta'$. We have also
 checked that this is also the case
 for the $f_0\pi$ state, that is, it does not couple with the $\pi(1800)$. This is another reflection of the fact that the
  $a_0\eta'$ tends to decouple from the other states.

\begin{figure}[h]\centering
\includegraphics[width=\textwidth,keepaspectratio]{I0.eps}
\caption{Modulus squared of the $f_0 \eta'\to f_0 \eta'$ (left)  and
$f_0 \eta\to f_0 \eta$ (right) S-wave amplitudes.
 For the former $a_1=-1.25$ and for the latter $a_1=-0.8$, see the
 text for details. The notation is as in Fig.~\ref{fig:t2.k12}.
\label{fig:t2.ei0}}
\end{figure}

\subsection{$I=0$}
We move next to the $I=0$ system where the $f_0\eta$, $a_0\pi$ and $f_0\eta'$ couple. Here occurs similarly to  $I=1$, so that the much higher $f_0\eta'$ channel mostly decouples from the other two channels. We then proceed similarly and distinguish between the subtraction constant $a_1$ attached to $a_0\eta'$ and to the other two channels $a_0\pi$ and $f_0\eta$. For $a_1$ around $-1.2$ one obtains a resonance of the $a_0\eta'$ channel at a mass of 1835~MeV, in agreement with that quoted in the PDG for the $X(1835)$, $1833.7\pm 6.1\pm 2.7$~MeV. This is shown in the left panel of Fig.~\ref{fig:t2.ei0} where
the modulus squared of the $f_0(980)\eta'\to f_0(980) \eta'$
S-wave amplitude is shown.
The width of the peak at half its maximum value is around 70~MeV, in good agreement with the width given in the PDG for the $X(1835)$ of $67.7\pm 20.3\pm 7.7$~MeV.   We consider next the other two coupled channels, $a_0(980)\pi$ and  $f_0(980) \eta$. We obtain a clear resonant signal with mass around 1.45~GeV for $|a_1|\lesssim 1$. This is shown in the right panel of Fig.~\ref{fig:t2.ei0}, where the modulus squared of the $f_0(980)\eta\to f_0(980)\eta$ is given for $a_1=-0.8$. It is not possible to increase further the mass of this peak by varying $a_1$. An important fact of this resonance is that it does not couple to the $a_0\pi$ channel. E.g. the analogous curve for the modulus squared of the $a_0(980)\pi\to a_0(980)\pi$ S-wave in the 1.4~GeV region is absolutely flat. By considering the inelastic process $f_0(980)\eta\to a_0(980)\pi$ we estimate a coupling to the latter channel more than 14 times smaller than to $f_0(980)\eta$. Because the $\eta(1405)$ resonance couples
mostly to $a_0(980)\pi$ \cite{pdg} we then conclude that the generated resonant signal
around $1.45$~GeV should correspond to the $\eta(1475)$. Its form is rather asymmetric due to the opening of the $f_0(980)\eta$ threshold, with a width at half the maximum of its peak of around 150~MeV. The width quoted in the PDG \cite{pdg} is $85\pm 9$~MeV. It is also known that the $\eta(1475)$ couples strongly to $K^*(892)\bar{K}+c.c$, a channel not included in our study. The threshold for
this channel, at around 1.39~GeV at the decreasing slop of our present signal, should certainly modify its shape.
For higher values of $|a_1|$ the peak tends to become too light in mass
compared with the $\eta(1475)$. For the $a_0(980)\pi\to a_0(980)\pi$ reaction one also appreciates a strong $a_0(980)\pi$ threshold effect at around 1.16~GeV. No resonance  around the mass of the $\eta(1295)$ is observed.

\begin{figure}[h]\centering
\includegraphics[width=.5\textwidth,,keepaspectratio]{I32.eps}
\caption{ Modulus squared of the $I=3/2$ $a_0 K\to a_0 K$  S-wave amplitude with
$a_1=-0.5$.  The notation is as in Fig.~\ref{fig:t2.k12}.
\label{fig:t2.ex}}
\end{figure}

\begin{table}
\begin{center}
\begin{tabular}{lccl}
\hline
Resonance & $I^{(G)}$ & Width (MeV) & Comments \\
\hline
$K(1460)$ & $I=\frac{1}{2}$ & $\Gamma\gtrsim 100$ & $|g_{f_0 K}/g_{a_0 K}|\simeq 1.4$ \\
$\pi(1800)$ & $I^G=1^{-}$ & $\Gamma\simeq 200$  & $a_0 \eta'$ elastic \\
$\pi(1300)$ & $I^G=1^{-}$ & $\Gamma\gtrsim 200$ & $a_0\pi$, $f_0\eta$ coupled channels \\
$X(1835)$ & $I^G=0^+$ & $\Gamma\simeq 70$       & $f_0\eta'$ elastic \\
$\eta(1475)$ & $I^G=0^+$ & $\Gamma\simeq 150$   & $f_0\eta$ elastic\\
Exotic & $I=\frac{3}{2}$ & $\Gamma\simeq 200$   & $a_0 K$ threshold \\
\hline
\end{tabular}
\caption{\protect \small Resonances resulting from our study. For more details see the discussions of the results in the text.
\label{tab:res}}
\end{center}
\end{table}

\subsection{Exotic channels}
Regarding the exotic channel with $I=3/2$ we find an interesting result. Our  amplitude gives rise to a clear resonant structure at around 1.4~GeV for  $|a_1|\lesssim 1.5$. We show  the modulus squared of $T(a_0^{\pm}K^\pm\to a_0^\pm K^\pm)$, because the $a_0^\pm K^\pm$ states are purely $I=3/2$,  for $a_1=-0.5$ (the same value used before in Fig.~\ref{fig:t2.k12} studying the $I=1/2$ case)  in  Fig.~\ref{fig:t2.ex}. One also observes that the shape of the resonance peak is
asymmetric with a clear impact of the $a_0 K$ threshold.
 Our results for $|a_1|\lesssim 1$ tends to confirm the predictions of  Longacre \cite{longacre} that studied the $K\bar{K}\pi$ and $K\bar{K}K$ system and concluded that the exotic $I=3/2$ $J^{P}=0^{-}$  $K \bar{K}K$ system was resonant around its threshold due to the successive interactions between a $K$, $\bar{K}$ and a $\pi$.  For $|a_1|\gtrsim 1$ we find that the resonance shape in $|T(a_0^\pm K^\pm\to a_0^\pm K^\pm)|^2$ progressively distorts becoming lighter and flatter.  Let us notice also that the $a_0 K$ system was not isolated in the two experiments quoted in the PDG where the $I=1/2$ $K(1460)$ was observed \cite{daum,branden}.

The other exotic channel with $I=1$ and $G=+1$ involves the isovector $a_0\pi$ state. Whether a resonance behavior stems at around 1.4~GeV depends on the actual value of $a_1$. For $|a_1|\lesssim 1$ the enhancement near 1.4~GeV is much weaker and is overcome by the cusp effect at the $a_0\pi$ threshold.
 For larger values of $|a_1|$ the resonant signal is much more prominent.
 No such resonance has  been found experimentally, e.g. in peripheral hadron production \cite{kek}, so that $|a_1|\lesssim 1$ should be finally taken.

In Table~\ref{tab:res} we collect all the resonances found in our study for the different quantum numbers discussed.

\section{Summary and conclusions}
\label{sec4}

In summary, we have presented a study of the S-wave interactions between the scalar resonances $f_0(980)$ and $a_0(980)$ with the lightest pseudoscalars ($\pi$, $K$, $\eta$ and $\eta'$) in the region between 1 and 2~GeV. The different channels studied comprise those alike the $\eta$, $K$ and $\pi$,   and the exotic ones with isospin 3/2 and 1, the latter having positive G-parity.
 First,  interaction kernels have been derived by considering the interactions of the external pseudoscalars involved in the reaction with those making the scalar resonance. We take advantage here of previous studies that establish  the $f_0(980)$ and
$a_0(980)$ as dynamically generated from the interactions of two pseudoscalars,   so that no free parameters are introduced in their calculation. Afterwards, the final S-wave amplitudes are determined by employing techniques
borrowed from Unitary Chiral Perturbation Theory. Interestingly, we have obtained resonant peaks that for the non-exotic channels could be associated with the pseudoscalar resonances $K(1460)$, $\pi(1300)$, $\pi(1800)$, $\eta(1475)$ and
$X(1835)$, following the notation of the particle data group.
 The resonances that come out from this study can be qualified as dynamically generated from the interactions between the scalar resonances and the pseudoscalar mesons. This establishes that an important contribution to the physical signal of the resonances just mentioned has a dynamical origin.
  The exotic $I=3/2$ channel could also exhibit a resonant structure around the $a_0 K$ threshold, in agreement with the behavior predicted
by Longacre \cite{longacre} twenty years ago. However, larger values for the subtraction constant
 $|a_1|$ tends to destroy this resonant behavior. No signal of the intriguing $\eta(1405)$ resonance is obtained.

 This approach should be pursued further by including simultaneously
 to the interaction between the
scalar resonances and the pseudoscalar mesons, considered here, those
arising from the lightest vector resonances with the same pseudoscalars in
P-wave. In this way, both pseudoscalar and axial resonances will be studied together.

\section*{Acknowledgements}
This work has been partially funded by the MEC grant FPA2007-6277 and Fundaci\'on S\'eneca grant 11871/PI/09. M.A. acknowledges the Fundaci\'on S\'eneca for the FPI grant 13310/FPI/09. We also acknowledge the financial support from  the BMBF grant 06BN411, EU-Research Infrastructure Integrating Activity "Study of Strongly Interacting Matter" (HadronPhysics2, grant n. 227431)
under the Seventh Framework Program of EU and   the Consolider-Ingenio 2010 Program CPAN (CSD2007-00042). Computing time and support was provided by Parque Cient\'{\i}fico de Murcia in the Ben Arabi SuperComputer.

redpajama_set_name: RedPajamaArXiv


Unfair preferences are the most common type of voidable transaction. They occur where a creditor has received payment (or another advantageous transaction) for something they are owed, giving them an advantage over other creditors. The funds from unfair preference payments will only be able to be clawed back where they were received by a creditor who knew, or ought to have known, that the company was insolvent.
Section 588FA of the Corporations Act 2001 (Cth) treats a transaction as an unfair preference where it meets certain criteria.
(b) the transaction results in the creditor receiving from the company, in respect of an unsecured debt that the company owes to the creditor, more than the creditor would receive from the company in respect of the debt if the transaction were set aside and the creditor were to prove for the debt in a winding up of the company; even if the transaction is entered into, is given effect to, or is required to be given effect to, because of an order of an Australian Court or direction by an agency".
A preference claim is generally pursued by the liquidators of an insolvent company to claw back funds for the purpose of disbursing them among the creditors.


text:
How the NBA is Dealing with COVID-19
Posted on March 30, 2020 March 31, 2020 by SLV Claw
Written by Sequoia Loya (Sports Writer) The first coronavirus case was reported in Wuhan, China in December 2019. The virus continued to spread throughout the world, infecting hundreds of thousands of people. According to ABC News, Vince Carter was planning to retire at the end of the season but with the season canceled due to the virus, this might be the end of his career. Carter announced, "Such a weird night but I am truly thankful for each and every person during this twenty-two year-long journey. If this is really it, I thank everyone for your love and support for all these years."
ABC News also claims that at least seven NBA players have tested positive for the virus so far such as Rudy Gobert (a Utah Jazz center) which is why the NBA season was canceled. Rudy Gobert says that he lost his sense of smell and taste due to the coronavirus. He also wishes that he would have taken the coronavirus more seriously. USA Today claims that Donovan Mitchell (Utah Jazz point guard) also tested positive with the coronavirus a day after Rudy Gobert tested positive. ABC NEWS stated that most of the NBA teams had fifteen to twenty games left to play. The season was set up to end around April fifteenth with the playoffs a few days afterward. The NCAA announced that all of the following basketball tournament games would be played without the fans. Deseret News says it is going to be hard to find time for a draft in the NBA due to the coronavirus outbreak going on. Many NBA all-stars had something to say about the current crisis America is dealing with:
"Don't know what to compare this situation to…just gotta buckle up and take care of yourself and those around you. Basketball will be back at some point but right now, protect yourself and stay safe out there!" -Steph Curry.
Washington Post claims that Lebron James doesn't want to play without the fans, "I play for the fans; that's what it's all about. If I show up to the arena and there ain't no fans there, I ain't playing."
"Basketball becomes secondary. Take care of yourself and your family. Wash your hands often." – Giannis Antetokounmpo.
"Well, I just hope this will not last long, and I hope everyone stays safe! Take care people, be smart and don't panic that doesn't help! See you soon!" – Bogdan Bogdanovic.
NBA news also stated that this pandemic has affected the NBA in a negative way. Marcus Smart (Celtics guard) tested positive. Kevin Durant, a former all-star MVP is among one of the four members on the Brooklyn Nets that has tested positive with the virus. The other three players wish to not have their names announced. The organization is notifying everyone that could have had contact with the players to get tested immediately so that hopefully, they don't pass it on to others.
"Everyone be careful, take care of yourself and quarantine," Durant says, he described himself by feeling well. "We're going to get through this."
This Coronavirus is affecting all of us. As we all hang tight, sheltering in place, it is important to remember that while we are separated, we are not alone and hopefully NBA basketball starts again soon.
Posted in Sports, Uncategorized
Yummy Food to Consider Making While Stuck at Home
NFL Offseason Heats up with Free Agency Moves and Trades


You'll get the latest updates on this topic in your browser notifications. The 7-day celebration commemorates the liberation of ancient Israelites from slavery in Egypt. Manage Push Notifications If you have opted in for our browser push notifications, and you would like to opt-out, please refer to the following instructions depending on your device and browser. As long as we always find each other for breakfast: For more coverage, follow our babies magazine on Flipboard. Moviegoers will spend an ungodly amount of money to see the continuing saga of the douchiest teen vampire movie series Such is the case with the 20 women on our list of celebs who need to show more skin.


СКАЧАТЬ ПРАЙС В EXEL. stk404- 100s stkspw20n60s5 irfp264pbf s9014 s29gl128p11tfi010 xcr3064xl- 10vq44c pd57006 mrf857s fca50cc50 pah1008cf gt45f122 p1014ap06 a1266- gr 9435a mr1521 ml2259bcp stk404 mc33889bdw 2n3904 tle6250g lr645n3 bu808dfi 200a6 hip6521cb fp103dr- lf bts2140- 1b fp131d- lf ir2184s 3845b 4863g 2sj378 2sc3498 mc14060b z0853006vsc tda8563aq l6219 ap9575gh 2sd845. STK404- 100S Datasheet : 2n3904 Thick- Film Hybrid IC One- Channel Class AB Audio Power Amplifier IC 50W Obsolete, Pinouts, STK404- 100S PDF Download 2n3904 SANYO - > Panasonic, stk404 Equivalent, STK404- 100S Datasheet PDF, Schematic, Cross reference, Data Sheet Circuits. 3904c datasheet 100s circuit , cross reference application notes 2n3904 in pdf format. 2sb156 2sb324 2sb435 2sb507e 2sb525 2sb536 2sb537 2sb544 2sb546a 2sb548 2sb549. STK404- 100S STK404- 120S EN7733 12v 100w 100s TRANSISTOR AUDIO AMPLIFIER STK4040 100W sub amplifier STK404- 130S 100s equivalent. Lawrence County Indiana; Wise County Virginia; Belmont County Ohio; Benzie County Michigan. stk4hc07 hcpl2232 stk404 ncp1397 dac5311.
STK404- 130SP TIPO ON SEMI ORIGINAL -. The STKseries products are audio power amplifier hybrid ICs that consist of optimally- designed discrete component 100s power amplifier circuits that have been miniaturized using SANYO' s unique insulated metal stk404 substrate technology ( IMST). Datasheet NJM OP- AMP ( lo- noise) NJMD ( SD) OP- AMP сдвоенный, ( lo- noise) NJMLD ( L) NJMS NJMD NJM2229S NJM2352D NJM2375A smd Power factor. STK404- 140S datasheet stk404 cross reference . electronic components 2sa1908 2sa1930 2sa1939 2sa1940 2sa1941 2sa1943 stk404 stk404 2sa1962 2sa1986 2sa1987 2sa2121- o. 2N3904 KEC- FSC ORIGINAL NTE123AP. 47uf63v lh0033cg ul32n107k. FCC- 1415DL/ JL SAMSUNG PN43F4500AF LJA, LJA Y- MAIN BOARD. для поиска по прайсу нажмите Ctrl+ F Название детали цена р кол- во шт. Documents Similar To semiconductores. Your warehouse for electronic 100s products. 2n3904 2n3905 2n3906 2n4003 100s ( 2n4001) 2n4033 2n4093 2n3904 2n4118a 2n4391 2n4441 2n5087- nd 2n5306 2n5400s 2n5401 2n5415 2n5416 2n5451 2n5525 2n5551 2n5551y 2n3904 2n5684 2n5686 2n60 2n6027 2n6045g( j) 2n6057 2n6071a 2n6075a 2n6075b 2n60b 2n6105 2n6213 2n6299 2n6341 2n6547 2n6678 2n6771 2n7000 2n7002 2n7008 to- stk404 92 2s2611 2sa1012 2sa1013y 2sa1020 2sa1024 ТО.
Ultra light load high efficiency VIN= 17V Current mode Step- 100s down Io= 3A Buck Regulator IC_ Fixed 350kHz frequency_ Отличается распиновкой от NR131S- см. STKdatasheet Datasheet search site for Electronic Components , triacs, STKpdf, integrated circuits, diodes, alldatasheet, 100s , 2n3904 STKdatasheets, datasheet, Semiconductors, STKcircuit : SANYO - 1 CH AB AUDIO POWER 2n3904 IC other semiconductors. datasheetul0a smbj6. Stk404 100s datasheet 2n3904. Ocean County New Jersey. STKdatasheet datasheet, Semiconductors, triacs, integrated circuits, , diodes, Datasheet search site for Electronic Components , alldatasheet, STKcircuit, STKdata sheet : SANYO - 1 CH AB AUDIO POWER IC other semiconductors.
SIP13 datasheet, cross. STK404- 100S SIP13 package STKw transistor audio amplifier circuit 12v 100w AUDIO AMPLIFIER CIRCUIT STKSTKSTK404. slide 1: Electronic Components Fuse 67 Circuit- Breakers 71 Fuse Holders 71 Fuses 67 GP Relays 72 Capacitors 36 AC Motor Start 40 Cerafne 37 Ceramic 36 Electrolytic Axial 41 Electrolytic Axial Non- Polarised 41 Electrolytic Backup 45 Electrolytic Radial 41 Electrolytic Radial Miniature 41 Electrolytic Radial Non- Polarised 41 Electrolytic SMD 44 Polyester 39 Polypropylene 37 Silver Mica 37 T. IC = 100 mA VCE = 1 VfT Transition Frequency IC = 10 mA VCE = 20 V f = 100 MHzMHz CCBO Collector- Base.
2N3904 Keywords: Datasheet. Hola buenas noches quisiera saber si tiene el integrado stky cual es el precio además los filtros 50v3300ufm y 100v3300ufm favor escribirme a este correo com. export- 13 Артикул Тип Название Фирма Корпус Размер Цена Цена Опт Доп.
информация KLS5- 801- B, держатель для 1 батареи АА провод 15см. STk404- 100S datasheet, cross reference, circuit and application notes in pdf format.


I just can't get my shopvac noise lower. I can, by enclosing it in silencer bin, however, it is big and will eat up considerable amount of space. Not good. Another consideration is the heat build-up. Running vacuum motor is hot already on its own even with constant air flow. What more if it is inside another container.
It has a huge suction power that I need to bleed most before it reaches the separation junction. What if I can use an alternative device with less capacity. I can save on electricity bills and save my eardrum too.
I searched around the net in attempt to find a more silent vacuum brand. Failed. There is no such thing. They are all powerful and definitely loud.
My trip to electronic surplus stores solved my problem. I bought two snail blower fans for experimentation.
Luckily, the bigger turbo fan worked. It only needs 24 volts power source and consume 45 watts power. Way lower compared to home vacuum cleaner which is 1.5kw. It was originally designed to blow air. But, installing it on top of my custom made cyclone husk collector created more than enough suction to separate husk from nibs. In fact, I am bleeding more than half of its power.
By the time I got and tested the snail turbo fan, the water seal of the colloid mill was damaged. The water circulating between radiator and mill cooling compartment was leaking outside the grinder base. I cannot use it for the next batch unless I found a replacement seal.
No cooling = no grinding. But, the turbo fan saved the day. I temporarily installed it near the mill base and commenced grinding with my fingers crossed. It was acceptable for the mill to get hot, but not too hot to set the cocoa liquor boiling.
For the record, during my very first grinding trial, the cocoa liquor coming out of downspout was boiling hot. I was glad my newly discovered cooler never let me down. It let me finished without any problem. At of this moment, I have run several batches without water cooling.
There is more, I am thinking if three to four of this thing are sufficient as air curtain. The commercial solely made for the purpose was kinda expensive, hard to install and consume a lot of power.
Next PostNext Should I Take Advantage of Health Benefits as Marketing Tool?


Theresa May, who served as the Home Secretary of Britain from 2010, is all set to be sworn in as the next prime minister of the United Kingdom. According to BBC News, Theresa May's only opponent, Andrea Leadsom, announced on Monday that she was pulling out of the race. Theresa May is 59-years-old and has served as the home secretary of Britain since 2010.
Ms. May's succession to the post was confirmed after Graham Brady, the chairman of the 1922 committee of Conservative lawmakers, confirmed that there would be "no need to rerun the election." He also added that with her only opponent pulling out of the race, Ms. May would go on to lead the Conservative Party and, for the same reason, would succeed David Cameron as the next prime minister of the country. However, Mr. Brady did go on to say that a final decision on Ms. May's prime ministership would only be taken after senior party officials are consulted.
Leadsom, 53, held the rank of the energy minister in former Prime Minister David Cameron's cabinet. While announcing her decision to not contest for the leadership of the Conservative Party, Ms. Leadsom also announced her support for Ms. May's candidature for the leadership position, and also for the Prime Ministership.
"The interests of our country are best served by the immediate appointment of a strong and well-supported prime minister," she said.
Meanwhile, Ms. May who was earlier in favor of Britain staying in the European Union has now changed her stand and said that she respects the mandate of the people.
"Brexit means Brexit and we're going to make a success of it," she said in a speech.
The incumbent prime minister of the country, David Cameron announced his resignation soon after the historic Brexit vote in which British citizens made it clear that they would be exiting the European Union. He is, however, expected to continue holding the position until a new leader is selected by his party. Currently, it is not known when the new prime minister would be sworn in, However, there are indications that this could happen within a few days.
Theresa May was born in Eastbourne, Sussex, on October 1, 1956. After attending the St. Hugh's College, Oxford from 1977 to 1983, she was employed at the Bank of England. Her first foray into politics was in the 80s when she was served as a councillor for the London Borough of Merton's Durnsford Ward. She was elected to the MP for Maidenhead in the 1997 general election, following which she was appointed Chairman of the Conservative Party in 2002. Theresa May also happens to be the longest-serving home secretary for the last 60 years.
When she takes over as the prime minister, Theresa May would become only the second woman after Margaret Thatcher to hold the position.


text:
International Chanteuse brings 'The Lords Lover' a Spiritual Sexpose to Hollywood's Los Globos Cabaret Theater
Christopher Laird Simmons PR Feb 14, 2013
HOLLYWOOD, Calif., Feb. 14, 2013 (MuseWire) — Written and directed by international chanteuse, Juliet Annerino, "THE LORD'S LOVER" breaks conventional boundaries of modern stage with cabaret, performance art, live music, dramatic theater, exotic dance, and cutting edge video imagery. The intricacies of human sexuality and controversial themes of desire and free will are explored and celebrated. Surreal elegance, satirical drama and philosophical hi-jinks collide in this passionately charged exploration into the timeless mysteries of Love and God.
According to Annerino, "'The Lord's Lover' is sexy, yet thought-provoking, playful, yet surprisingly poignant. World-renowned performance poet Jim Bolt emcees, in a white top hat and tails, leading us through the night's adventures."
Juliet will lead her band of cabaret/jazz musicians with "The Torch Ensemble."
"The Lord's Lover" will play Wednesday nights throughout March and April at the newly renovated Club Los Globos, making the most of the new lights, sounds and stage effects, and maximizing Los Globos' charm and adaptive space to the creative flow of "The Lord's Lover's" multimedia style. Food and mixed drinks make this a great "dinner and a show" date night.
"The Lord's Lover" is a true Labour of Love for its creator, Juliet, who has drawn on her keen observations of cultural and gender differences worldwide, as she's toured and sung throughout Europe and the Middle East.
Gratefully and humbly Juliet seeks your assistance in supporting this production: "If you'd like to be an angel and pitch in to the Indiegogo.com fundraiser for the show, you'll be rewarded with perks such as a signed 'Declaration of Sainthood' for a $100 donation, or even a 'Day in the Life of a Deity' for a $5,000 donation."
Maybe, for the right price, you could get a date with the incomparable Juliet herself. Well… maybe a kiss…? (See: http://www.indiegogo.com/projects/328764/ for details.)
Come with – or without – your loved one.
"THE LORD'S LOVER – Theatrical, Musical Cabaret."
WHERE: Club Los Globos, 3040 Sunset Blvd. Los Angeles, CA 90026.
WHEN: Opening Night Wednesday, March 6th, 2013 at 8 p.m., running consecutive Wednesdays through April 2013.
ADMISSION: Tickets $20 at the door, General Admission. For a limited time, $12 Discount Tickets are Online at: http://www.indiegogo.com/projects/328764/ .
For Industry comps, please email: TheLordsLover@gmail.com.
PUBLIC AND MEDIA CONTACT:
Juliet Annerino – (310) 666-2544.
http://www.TheLordsLover.com/ .
YouTube Video: http://youtu.be/TNo5Ea80VD0 .
* Photo Caption: Jim Bolt, event Master of Ceremonies.
• Permanent shortlink to original copy of this release: http://goo.gl/2z0xV .
NEWS SOURCE: Juliet Annerino :: This press release was issued on behalf of the news source by Send2Press(R) Newswire, a service of Neotrope(R).
Copyright © 2013 Send2Press NewsWire for Journalists. This content is copyrighted under U.S. and international law and may only be used for non-commercial purposes by news aggregators or under license of the Neotrope® News Network – www.neotrope.net. .
Copr. © Neotrope and the news source – all rights reserved.


It's been good. Thank you and good night.
It was once the most sought-after gadget in the world but now the very first iPhone is to become officially obsolete next month.
Apple's first iPhone launched six years ago and was discontinued a year later in 2008 when the iPhone 3G was released.
According to a document which is doing the rounds online, on June 11, 2013, the first generation iPhone will be officially regarded as "vintage and obsolete".
It looks as though Apple is set to classify the model as "vintage" in the States while it will be "obsolete" throughout the rest of the world.
Apple products are labelled as vintage between five and seven years after being discontinued in America and as obsolete after seven.
It was reported years ago, that the company sold 6.1 million first generation iPhone units in the year before the iPhone 3G was unleashed.
What does the future hold for the SMS text message?
Waiting to get your mits on the Galaxy S4? Well, be prepared – buy a top quality case, today!


Thank you for supporting the patients and families of Nicklaus Children's Hospital at the 7th Annual Fashion Gives Back, held on Thursday, September 27, 2018.
Your attendance, sponsorships, and donations all contributed to an incredible event.
We are proud to say that because of your generosity, enough funds were raised through Fashion Gives Back to fund Camp Superstar for two years! Camp Superstar is a special weekend-long camp for 30 children born with a cleft lip or a cleft palate. The children get to meet others like them who have had similar procedures, many discovering for the first time that they are not alone in their conditions.
If you did not get the opportunity to donate and would like to support our patients, please donate now using the form below.


Looking for a unique niche market to start an internet business? Then take a look at ProtectionGearShop.com - an online store where people can purchase quality gear to protect themselves and the ones they love. Online shoppers will have quick access to a variety of products including apparel, gear, survival, as well as, home and car safety all used for creating safer surroundings. Whether they need to protect and guard themselves from the elements, looking for anti-theft devices to protect their car and valuables, plus safeguards to protect their home and personal possessions they will find it at all new online business!
As the owner of this website, you will be able to reach customers through the attached blog, newsletter and social media pages where you can share tips on the best ways to stay safe with protection gear. This ready-made internet business will be loaded with 300 drop ship products to get you started. Our team will select the first 100 and you will have the opportunity to select 200 products you would like to sell online. All the products featured are from drop ship vendors which means you are not required to hold any inventory.