text:
Isla Don Pedro es una isla del país centroamericano de Panamá localizada en el lago Gatún, que administrativamente depende de la provincia de Colón. Se ubica en las coordenadas geográficas  frente a la bahía Frijoles, al oeste de la isla Lindero, al este de la Punta Salud en la isla Barro Colorado, y al sur de la isla Vista Alta.

Véase también
 Geografía de Panamá
 Geografía de América

Referencias

Enlaces externos
 Mapa de localización de la isla

Islas lacustres de Panamá
Geografía de Colón

redpajama_set_name: RedPajamaWikipedia


Suzuki Vx800 Shop Manual 1993 Onward is good choice for you that looking for nice reading experience. We hope you glad to visit our website. Please read our description and our privacy and policy page.
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text:
Kena: Bridge of Spirits (PS4/PS5) Preview
by Michael P Cleworth on January 15, 2021
SAMURAI SHODOWN comes to Xbox Series X|S in March with smart delivery
SYNTHETIK: Ultimate (Xbox One) Review
Coming to PlayStation 4, PlayStation 5 and PC this Spring, Kena: Bridge of Spirits is set to be Ember Lab's debut title. In 2006, the esteemed studio wowed its audience with stunning visuals and a deep, emotional story with short animation movie, Mask of Majora. Kena: Bridge of Spirits looks set to finally bring their famous animation magic straight into the video game world.
They say the first impressions are the ones that count, and the beauty of this up-and-coming, story-driven RPG is by far the first thing you notice. Somehow trademarking their work with aesthetically distinct styling, the beauty seen in the likes of The Mask of Majora is evident upon the very first sight.
Ember Studios have announced that Kena: Bridge of Spirits is going to be a widely linear game, made for all of the family (sic). I'm unsure on what exactly is meant by 'widely linear' but I can only guess this means that there's little hope for an open-world adventure. Moreover, the family aspect promised rings bells of an all-too-easy experience, so older gamers may want to turn the difficulty up for the first play-through.
The story behind Kena: Bridge of Spirits is almost as beautiful as the graphics. You play Kena, a young spirit guide on a journey to a shrine in an abandoned village. Along the way, she encounters a variety of monsters. The enemies you face are metaphors for tortured spirits, twisted into hellish abominations. As a spirit guide, it is your duty to defeat them, to allow for their travel to the other side.
As shallow as the story seems to be, Ember Lab appears to be eager to drive home the point that the game is "story-driven". I imagine there to be plenty of emotional moments with lashings of twists and turns along the way. Of course, it's needless to say that they know how to spin a great story.
Cute Beings Help you on your Way
Throughout Kena: Bridge of Spirits you are helped on your way by what look like small black potatoes with eyes. These somewhat cute little fellas can be rescued. Eager to return the favor they then help you on the arduous journey ahead.
Rot (collective noun) add a further dash of RPG into an already RPG-rich game. They grow to become a team of micro-manageable allies that you can assign to tasks and even call upon in battle. The teams of Rot can be split-up to perform multiple consecutive tasks. I imagine this will proffer a puzzle element and open up a new layer in an already immersive adventure.
Aside from the Rot, gems can be found in abundance throughout the world of K:BoS. These can be used to upgrade your Rot and even buy accessories to customize them. Having generously scattered these gems, Ember Lab have eradicated the need for mico-transactions.
In conclusion, Kena: Bridge of Spirits looks like a phenomenal debut for the studio. By just watching the trailer, it is easy to become awestruck at the graphical art employed by the animations team. To play the game will be something else completely. Consequently, I'd be lying if I was to tell you I'm not as excited as a kid on the run-up to Christmas for this title. Regardless, I will have to be patient for a few more months.
Ember Lab have said they wanted this to be a game that could be finished over a weekend, so don't expect the token standard fifty-to-one-hundred hours of gameplay. However, the reality is that the game could probably be finished in around twelve-to-fourteen. However, side quests and the limited exploration may add around ten hours to the total. I just hope the price reflects the brief longevity. Expect to pay no more than $30 or $40.
The family element of the game may render it a little too easy for the seasoned gamer. However, this can be easily resolved with difficulty toggles. Furthermore, K:BoS is designed for the story, as opposed to the challenge.
A visually stunning adventure with a lot to offer. The experience, albeit short, will definitely be worth diving into.
Playstation 4, Featured, PC, Playstation 5, Previews
Kena bridge of spiritsPreviewPS4PS5
Kena bridge of spirits, Preview, PS4, PS5
Michael P Cleworth
FeaturedPCPlaystation 4Playstation 5Previews
With purposely designed chunky PSOne-style polygons, Breakneck City is a retro low-poly beat'em up carrying a 90s vibe. Even with a few blemishes, this game is a quality throwback to simpler times. Instead of saving your girlfriend from an angry [...]
Mega Cat Studio, who brought us Coffee Crisis and Bite The Bullet, along with Retrotainment Games, creators of Haunted Halloween '86, have been working with 8BitLegit, Gradual Games, and 6502 Collective to release Trophy, a new retro NES game inspired by [...]
Like F-Zero Maximum Velocity, F-Zero GP Legend has a limited Single-Pak multiplayer mode, only offering 1 track through use of the same colored swapped vehicle. It basically acts as brief demo to the multi-pak link option.

redpajama_set_name: RedPajamaCommonCrawl


This morning on the radio station I listen to, all they were talking about was Fantasia's performance on American Idol last night. I didn't see it but they played a clip...YIKES.
The 80s are back. Long bangs, synthesizers but seriously....WTF is up with the bear heads????
What? NO!! It Couldn't Be....a REAL Person!?


How to Contact Prime Minister of India, this is what I am going to tell you in simple terms and will provide you all ways by which you can contact our prime minister.
There are many ways in which we can contact our prime minister of India like contacting via a letter sent to PMO or by filling a simple form on website.
Even we can fax or call PMO office easily.
The main reasons to contact the prime minister can be providing suggestions, grievance or for any other genuine issue.
Please find different authentic ways how you can contact our prime minister.


I just wanted to know the precise requirement of submission.
Does it have to be a real working app ?
or Does it have to simply display Data ?
also, do we have to show live/changing Data or any ability for viewer to change Data on dashboard ?
Thanks for writing. Contestants must create a personal dashboard of three or more charts using Chart.js. The Dashboard must be viewable in a web browser and the Dashboard charts must include data that will help you track personal activities, such as social activity, entertainment, exercise, or eating. Dashboards should include real data but should not include anything you don't want to share publicly.
The data does not have to be live/changing and you do not need to provide viewers with a way to alter the data.
Thanks, Vikas. We look forward to receiving your submission.


We must have the right conversations to address the wrong of our situation!
Free Em All Radio w/ Chairman Fred Hampton Jr.
The StreetGroomers! Ghetto Passes & White Privileges ..The Best of Both Worlds!
Free Em All! Radio w/ Chairman Fred Hampton Jr.
The Breakdown of Black Men; Criminalization, Crack & Confusion!
Illajams w/ Illaflows! The Best in House and R&B!
Brotha Haroon, Dolla Phil & Tron... The StreetGroomers!


text:
Home Cars & More New GT86 2017 Toyota GT86 reviews round-up
2017 Toyota GT86 reviews round-up
By Joe Clifford 24 April 2017
The revised 2017 Toyota GT86 has received rave reviews since its launch, both in standalone road tests and comparative group tests. In case you missed them, we've collected a few together below to offer an overview of the expert testers' opinions.
Where available, click on the subheadings to be taken to the full online reviews.
Autocar road test: 4.5/5
At the end of this Autocar road test, reviewer Neil Winn quoted the magazine's original assessment of the launch GT86, that there was nothing on the market offering the same level of "poise, balance and, crucially, accessibility."
"The same remains true today," Winn confirmed, adding: "Ultimately, the decision to buy one has never been easier."
The rest of the article put flesh on the bones of that statement, acknowledging the effect of the revised steering, "which immediately feels sharper and more direct," while "the various chassis modifications… have also contributed to increased communication. [It] feels noticeably more progressive up to and over the limit."
Winn concluded by commenting: "On the right roads and in the right conditions, [the new GT86 is] without a doubt one of the most grin-enduring cars currently on sale."
Auto Express road test: 4/5
"Minor tweaks to the GT86 formula ensure that it stays at the top of the handling pecking order." A good introduction from reviewer Richard Ingram sets the tone for the rest of his four-star road test.
Early appreciation was shown for the "more luxurious" interior revisions, including new leather and Alcantara trim, handy audio controls now on the steering wheel, and a digital "screen [which] adds trip functionality and replaces the [outgoing model's] analogue fuel gauge."
When it came to driving the revised GT86, Ingram decided that "it remains a truly satisfying and immensely engaging car to drive – whatever the situation. It makes you feel like you're travelling much faster than you are – only emphasising this car's ability to thrill at amusingly low speeds."
CAR group test: Toyota GT86 (winner)
In a three-coupe group test, CAR magazine pitched the GT86 against the BMW 220i M Sport and Mazda MX-5 RF. Reviewer Chris Chilton described the Toyota as "a B-road weapon" that offers superb car-driver communication: "The GT86 shows where BMW has missed a trick. To not isolate you from what the car's doing, but to help you understand it, to learn from it, and work with it. Better together, and all that."
And when the chassis is pushed beyond the limits of grip, he comments: "It all happens so slowly, so progressively and so naturally thanks to those skinny, low-grip tyres, and a new Track mode for the ESP means you can play knowing the car has got your back. At high speeds, you still get the rock-solid stability you need to ensure you're enjoying the scenery, not landscaping it."
Summarising the GT86's win, Chilton concluded: "If you're serious about buying a coupe because of the way it drives and not merely the way it looks, this is your car."
Evo road test: 4/5
Without even reading the main copy, the title of this article – The best budget sports car on sale? – suggests that Evo already has a high opinion of the GT86.
Highlight features include the engine, which feels "endlessly durable and tough" so that "you don't think twice about hammering it all day long," and the innately right driving position, which is "low-slung and with plenty of adjustability" so that "just about everyone, no matter how big or small, should find a suitably comfortable and supportive driving position."
In terms of driving feel, the road test reveals that "the GT86 starts making sense when you push it." However, it also concedes that "the GT86 proves you don't need to be risking life, limb and penalty points in order to enjoy [it]. Rather that sometimes, chassis balance and the sensation of pushing a car to its limits are more valuable than all-out straight-line speed."
While that sort of behaviour might still scare off less skilful drivers, Evo also pointed out the benefits of the car's new Track mode. "This sets the traction and stability control system to minimum intervention, giving you plenty of freedom to play with the rear axle and enjoy the car's sweet balance but with the ultimate reassurance of a safety net."
Pistonheads video blog
Introduced with the intriguing revelation that the revised 2017 GT86 contained more changes than meets the eye, Dan Trent voiced his opinions in an informative blog-style video review. You can watch it below.
Top Gear road test
Deciding to jump straight into the driver's seat rather than pore over the on-paper changes, TG reviewer Stephen Dobie immediately sensed the improved steering feel and communication.
Qualifying his initial assessment, he commented: "Every mechanical control – steering, gears, pedals – is extremely tactile. They're all equally joyous to use, and work off each other perfectly. You drop the seat low, pull the wheel towards you, and feel immediately set up to enjoy yourself. The basics have just been nailed."
So nailed, it turns out, that Dobie confidently associated the feel of the new GT86 with that of high-price supercars. He said: "By combining the old-school joy of a turbo-free engine, rear-wheel drive, a snappy manual gearbox and a low-slung, nerd-pleasing driving position, what we have here is, essentially, a cut-price Porsche 911R."
2017 Toyota GT86: What about you?
Reading other people's perspectives is all well and good but wouldn't you prefer to have a personal opinion on the 2017 Toyota GT86? Why not click on the following link and fill in a test drive request at your local Toyota centre.
asad ali says:
Thanks for shearing such a nice information about toyota cars
Toyota UK says:
Hi Asad Ali,
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funded by EPSRC (EP/C007298/1) from 1st July 2005 for three years. Total amount of funding is approx. 220,000 pounds.
The project focuses on the development of measurement techniques to validate synchronizer circuits at the reliability levels required, and the design of more robust circuits which will deliver the performance necessary for future multi-billion-transistor Systems on a Chip (SoC).
As the size of systems on chip (SoC) has increased, it has become difficult or impossible to accurately distribute a single global clock across the entire system. Future systems are likely therefore to consist of many independently, or semi-independently clocked regions, with a need for synchronization of the data passing between them. Consequently there will be many more synchronizers whose performance and reliability is crucial to the performance of the system itself. Current synchronizers are untested at the levels of reliability required, and the increasing process fluctuations resulting from smaller dimensions are likely to worsen their relative performance. This three-year proposal aims to develop measurement techniques to validate synchronizer circuits at the reliability levels required, and to develop more robust circuits which will deliver the performance necessary for future multi-billion-transistor SoC.
To develop synchronizer measurement techniques better suited to assuring reliability in SoC, in particular for characterising error rates beyond 20 .
To provide a firmer base for the theoretical prediction of reliability, including a better understanding of the role of noise in both conventional and unconventional synchronizer circuits.
To design more robust synchronizer circuits capable of good performance in nanometre technologies, with low supply voltages and large parameter fluctuations.


Let's take a minute to get pensive.
I'm someone who thoroughly believes that in life, no matter what the current situation is or how dire circumstances are, the way you look at the experience has a lot to do with the outcome. Though I know it is extremely difficult, hyper-focusing on the negative aspects of a situation doesn't exactly help, does it? Of course, some things in life are naturally worse or feel worse to live through than others, and when faced with an unexpected challenge on ANY level, it's so hard not to get absorbed by only the negative. However, being positive (or even just neutral) about the facts will not only make you feel better, but it will help power you through the worst, and the best, of times.
You're spot on, I'm not a life coach, and I have no authority on this particular subject. I'm simply another human, living her life, trying to make the best of the little time I have on the planet.
I've been there myself, and though it's not easy, a positive frame of mind helped me live through one of the toughest stages of my life to date (learn more here, if you're interested).
Now, that's not to say I didn't struggle (or that I don't struggle now, even). That's not to say that I don't get days in which I think nothing but negative thoughts from sunrise to sunset. But, what it does say: it's worth a shot, after all, what do you have to lose!?
In today's society, with social interaction with other humans at our fingertips and the media reporting all of the world's failings on a constant basis, it is far too easy to get caught up in a negative vortex. It's far too simple to look at a rainbow and say, "ugh, but look at all the rain we got before we saw this pointless thing!!" So, what if, instead of that response, which, might I add, seems so natural for most of us to default to, we choose to ignore the negative. Just for a second. Give your mind a rest of your own judgement for a split second; take a look at the rainbow with a pure mind and heart. What do you see? I see a miraculous and uber cool formation of colour in the sky. That's not something you see everyday! Sure, you had to live through some rain to see it, but guess what? That's over now. Rainbows are rare, so just enjoy it. Block out the gloomy weather of the past couple of days. Ignore the fact that you've had to trek up and down your stairs to change into a raincoat and wellington boots, again. Disregard the extra 15 minutes you sat in traffic because people were being extra cautious in their driving. Savour the moment. Enjoy the present. Relish in & reflect on what you see in front of you.
This is how I (try) to live my life. This is why I smile a lot, lot more than I frown. I go out of my way to think on the positive side of things. To see the glass half full, rather than half empty. Sure, from time to time, I get called a hippy (though, is that really that big of an "insult"? They had great style in the 60's & 70's, just sayin') and I get called Pollyanna (which again, is that meant to be an insult? 'Cause it's really not). However, I truly believe that it's worth it. When I die, I'd rather be known as "the girl whom always seemed jolly" than anything else. Furthermore, without something to laugh, smile, giggle, beam, grin, or even guffaw at, is there even any point to it at all?


What is Return On Science?
Return On Science is a national research commercialisation programme that leads the establishment of best practise to deliver new research to market from universities, research institutions, and private companies. Our services include connecting science, technology and project teams with strategic management, top-tier advice and guidance, world leading best practice process, and efficient access to capital.
Return On Science is a foundation partner in the government's Commercialisation Partner Network, a programme designed to increase commercial outcomes from publicly-funded research. Return On Science provides facilitated access to best in class commercialisation resources, networks and expertise to directly increase the quantum and quality of the commercial opportunities arising from New Zealand research effort.
The four Return On Science Investment Committees represent centuries of combined domain specific knowledge and experience from around the globe. Made up of academic and industry experts alongside commercial and investment experts, the committees can provide tailored recommendations on market viability, research and product development direction, and connections to relevant individuals and companies.
In addition to valuable advice, the Investment Committees can provide access to capital needed to progress a project. Either through approving investment from the devolved PreSeed Accelerator Fund, through recommendations to MBIE for approval of non-devolved PreSeed Accelerator Fund spending, or through connections to investors and investor groups Return On Science is engaged with.
Return On Science Investment Committees are available at any stage to review progress and provide additional advice and guidance to help direct the team to the earliest development of a minimal viable product, and connections to the best international people able to provide market analysis and later, market validation.
Researchers and academics can present and discuss their research with an independent committee specialised in their area. These are external members to their institution who will discuss with the researcher the merits of their project without institutional considerations.
The result is much needed, unbiased and unclouded recommendations on the commercial viability, directions and steps needed for the researcher's project.
Tech Transfer Offices and Commercialisation Managers can utilise Return On Science in multiple different ways.
Bringing projects to the Investment Committee at the earliest stages to receive advice on the technology and potential market, and recommendations on whether the project is worth pursuing commercially will decrease the risk involved in progressing projects while positively increasing principle investigator and Tech Transfer Office dialogue.
Commercialisation Managers with projects at any stage will benefit from the advice, direction and connections the Committee can give, in addition to PreSeed Accelerator funding approvals and follow on investment connections.
By nature, startups generally have a very strong technical focus, but their chances of success are lifted when equal attention is paid to commercialisation activities early on. Return On Science offers its services to assist in navigating the commercial pathway.
Return On Science provides investors with early visibility of a deep pipeline of technologies being developed in research organisations throughout New Zealand. Access to the Investment Committee meetings enables investors to gain an understanding of the technology and it's potential applications.
For entrepreneurs attendance means the opportunity to find and be involved with interesting technologies, and network with potential investors that have a strong interest in early stage technologies.
To unlock the innovation potential of Māori knowledge, resources and people to assist New Zealanders to create a better future.
Contributing to Economic Growth through Distinctive R&D. New Zealand needs its businesses and for-profit enterprises to perform at an optimum level and contribute to economic growth. This theme concerns the development of distinctive products, processes, systems and services from Māori knowledge, resources and people. Of particular interest are products that may be distinctive in the international marketplace.
Achieving Environmental Sustainability through Iwi and Hapü Relationships with land and sea. Like all communities, Māori communities aspire to live in sustainable communities dwelling in healthy environments. Much general environmental research is relevant to Māori. Distinctive environmental research arising in Māori communities relates to the expression of iwi and hapū knowledge, culture and experience – including kaitiakitanga – in New Zealand land and seascapes.
Improving Health and Social Wellbeing. Distinctive challenges to Māori health and social wellbeing continue to arise within Māori communities. Research is needed to meet these on-going needs.
Exploring Indigenous Knowledge and RS&T (Research, science and technology). This exploratory theme aims to develop a body of knowledge, as a contribution to RS&T, at the interface between indigenous knowledge – including mātauranga Māori – and RS&T.
Return On Science supports the use te reo Māori and observance of tikanga Māori during its investment committee meetings.


text:
GI Jews
GI JEWS -- JEWISH AMERICANS IN WORLD WAR II
This is the profound and remarkable story of the 550,000 Jewish Americans who served their country in World War II. These brave men and women fought for their nation and for Jewish people worldwide. Like all Americans, they fought against fascism, but they also waged a more personal fight – to save their brethren in Europe. Jewish servicemen were also among the first to assist the survivors of the Nazi concentration camps liberated by American troops. After years of struggle, these soldiers emerged transformed, more powerfully American and more deeply Jewish, determined to continue the fight for equality and tolerance at home.
WATCH THE FILM LEARN MORE
GI Jews: Jewish Americans in World War II
Discover the story of the 550,000 brave Jewish Americans who served in World War II.
Our Lives Depended on Each Other
Jewish veterans talk about preconceptions and the value of character in World War II.
The Jewish GI Service Broadcast Worldwide from Germany
Jewish American forces held a historic service in Aachen, Germany during World War II.
LEARN MORE, WATCH MORE
Photos: Jewish Men and Women Who Served in World War II
Veterans include Carl Reiner, Mel Brooks and Robert M. Morgenthau and women in WAAC.
GI JEWS: Jewish Americans in World War II is a feature-length documentary film about the more than 550,000 ...
GI Jews Interviewee Biographies
GIs from the U.S. Armed Forces, members of the Women's Army Auxiliary Corps (WAAC) and historians from the ...
© 2020 WNET. ALL RIGHTS RESERVED
FUNDING PROVIDED BY
Support for GI JEWS: Jewish Americans in World War II was made possible in part by the National Endowment for the Humanities, the Corporation for Public Broadcasting, Righteous Persons Foundation, the Dobkin Family Foundation, Alexander Wolf & Son, Al Berg, the Sumner M. Redstone Charitable Foundation, the Sylvia A. and Simon B. Poyta Programming Endowment to Fight Anti-Semitism, the Mandell L. and Madeleine H. Berman Foundation, River Birch LLC, Marlene & Hymie Mamiye, Mass Humanities, Robert & Pamela Jacobs, the Jacquin P. Fink Foundation for the Arts, Inc., Alan I. Franco, the Paler Foundation.
GI JEWS: Jewish Americans in World War II is a production of Turquoise Films, Inc. in association with THIRTEEN Productions LLC for WNET.


text:
\section{introduction}

There have been many studies in literatures on light nuclei production from heavy ion collisions at the Relativistic Heavy Ion Collider (RHIC) and the Large Hadron Collider (LHC). Most of these studies are concerned with their yields, and the experimental data from RHIC~\cite{Adler:2001uy,Abelev:2010rv,Agakishiev:2011ib} and LHC~\cite{Adam:2015yta,Adam:2015vda} can be successfully described by both the statistical model~\cite{Andronic:2010qu,Cleymans:2011pe} and the coalescence model~\cite{Chen:2012us,Chen:2013oba,Shah:2015oha,Sun:2015jta,Sun:2015ulc,Zhu:2015voa}. For the transverse momentum spectra of light nuclei, the coalescence model has also been shown to give a good description of the experimental data~\cite{Sun:2015jta,Sun:2015ulc}.

None of these theoretical studies has addressed the elliptic flows of light nuclei except Ref.~\cite{Oh:2009gx}, in which it is found that the deuteron elliptic flow obtained from the coalescence of freeze-out nucleons from a relativistic transport (ART) model~\cite{Li:1995pra,Li:2001xh} is similar to that produced via the reactions $NN\leftrightarrow\pi d$ in the transport model, and both give reasonable description of the experimental data from the PHENIX Collaboration at RHIC~\cite{Afanasiev:2007tv}.  In a recent study by the STAR Collaboration at RHIC~\cite{Adamczyk:2016gfs}, it has been shown that measured elliptic flows of light nuclei such as ${\rm d}$, $\bar{\rm d}$, ${\rm t}$, and $^3{\rm He}$ are consistent with the results calculated with the coalescence model that uses freeze-out nucleons from a multiphase transport (AMPT) model~\cite{Lin:2004en}.  On the other hand, the experimental data cannot be described by a blast-wave model with its parameters fitted to the proton transverse momentum spectrum and elliptic flow.  To understand the reasons for the failure of the blast-wave model and the success of the coalescence model in describing the elliptic flows of light nuclei, we investigate in the present study if the coalescence model carried out with the nucleon distributions from the blast-wave model can also describe the elliptic flows of light nuclei. We find that for this to be the case, high momentum nucleons need to be emitted more likely near the reaction plane than out of the reaction plane, compared to that for low momentum nucleons. Our results thus suggest that studying the elliptic flows of light nuclei provides the possibility of probing the nucleon emission source in relativistic heavy ion collisions, thus complementing the method that uses the Hanbury- Brown Twiss (HBT) interferometry of identical particles emitted at freeze-out~\cite{Bertsch:1988db,Pratt:1990zq,Mrowczynski:1992gc}.

The paper is organized as follows. In Section~\ref{blast}, we introduce the blast-wave model and describe how its parameters are determined.  The coalescence model is then described in Section~III. In Section~\ref{results}, we show results from our study on the transverse momentum spectra and elliptic flows of ${\rm d}$ ($\bar{\rm d}$) and ${\rm t}$ ($^3{\rm He}$) obtained from the blast-wave model without and with the space-momentum correlation.  Finally, a summary is given in Section~\ref{summary}.

\section{the blast wave model}\label{blast}

In the blast-wave model for particle production in relativistic heavy ion collisions, the Lorentz-invariant thermal distribution $f(x,p)$ of protons or neutrons at the kinetic freeze-out temperature $T_K$ is given by
\begin{equation}
f(x,p)=\frac{2\xi}{(2\pi)^3}\exp\{-p^\mu u_\mu/T_K^{}\},
\end{equation}
if the effect of quantum statistics is safely neglected at high temperature. In the above, $\xi$ is the fugacity of the proton or neutron, the four-momentum $p^\mu$ is
\begin{equation}\label{p}
p^\mu = (p^0,\bm{p}) = (m_T^{}\cosh y, p_T^{} \cos\phi_p,
p_T^{}\sin\phi_p, m_T^{} \sinh y),
\end{equation}
and the flow four-velocity $u_\mu(x)$ is
\begin{eqnarray}\label{u}
u^\mu &=& \cosh\rho ( \cosh\eta, \tanh\rho \cos\phi_b, \tanh\rho
\sin\phi_b, \sinh\eta).\nonumber \\
\end{eqnarray}
In Eqs.(\ref{p}) and (\ref{u}), $y$ is the energy-momentum rapidity, $m_T^{}$ ($= \sqrt{m^2 + p_T^2}$) is the transverse mass with $m$ and $p_T$ being the mass and transverse momentum of the nucleon, respectively, and $\eta$ and $\rho$ are the longitudinal and transverse flow rapidity $\eta=\frac{1}{2}\ln\frac{t+z}{t-z}$ and $\rho=\frac{1}{2}\ln\frac{1+|\bm\beta|}{1-|\bm\beta|}$, respectively, with $\bm\beta$ being the transverse flow velocity.  We have followed the usual convention to define the $z$-axis along the beam direction and the $x$-axis in the reaction plane of a heavy ion collision. The angles $\phi_p$ and $\phi_b$ are, respectively, the azimuthal angles of the nucleon momentum and the transverse flow velocity with respect to the $x$-axis.

From the nucleon momentum distribution, one can obtain the nucleon invariant momentum distribution as
\begin{eqnarray}
E\frac{d^3N}{d^3{\bf p}}=\frac{d^3N}{p_Tdp_Tdyd\phi_p}=\int_{\Sigma^\mu}d^3\sigma_\mu p^\mu f(x,p),
\end{eqnarray}
where $\Sigma^\mu$ is the freeze-out hyper-surface and $\sigma_\mu$ is its covariant normal vector.  In the case that $\Sigma^\mu$ depends only on the proper freeze-out time $\tau$, $\sigma_\mu$ is then given by
\begin{eqnarray}
d^3\sigma_\mu=(\cosh\eta,0,0,-\sinh\eta)\tau rdrd\eta d\phi,
\end{eqnarray}
with $\phi$ being the azimuthal angle of the nucleon transverse position vector.

Using the relations
\begin{eqnarray}
p^\mu u_\mu&=&m_T\cosh\rho\cosh(\eta-y)-p_T\sinh\rho\cos(\phi_p-\phi_b),\nonumber\\
p^\mu d^3\sigma_\mu&=&\tau m_T\cosh(\eta-y)d\eta rdr d\phi,
\end{eqnarray}
and taking the particle emission time to be $\tau_0$, the invariant nucleon momentum spectrum can then be written as
\begin{widetext}
\begin{eqnarray}
\frac{d^3N}{p_Tdp_Tdyd\phi_p}=\frac{2\xi\tau_0}{(2\pi)^3}\int_{\Sigma^\mu} d\eta rdr d\phi m_T\cosh(\eta-y)\exp{\left[-\frac{m_T\cosh\rho\cosh(\eta-y)-p_T\sinh\rho\cos(\phi_p-\phi_b)}{T_K}\right]}.
\end{eqnarray}
\end{widetext}

For simplicity, we assume that the longitudinal flow is boost invariant, so that the longitudinal flow rapidity is equal to the energy-momentum rapidity, i.e., $\eta=y$, and that the distribution in the energy-momentum rapidity is uniform in midrapidity. In this case, the invariant nucleon momentum spectrum becomes simply
\begin{eqnarray}
&&\frac{d^3N}{p_Tdp_Tdyd\phi_p}=\frac{2\xi\tau_0}{(2\pi)^3}\int_{\Sigma^\mu}rdr d\phi m_T\nonumber\\
&&\times\exp{\left[-\frac{m_T\cosh\rho-p_T\sinh\rho\cos(\phi_p-\phi_b)}{T_K}\right]}.
\end{eqnarray}

Because of non-vanishing elliptic flow $v_2^{}$ in non-central heavy ion collisions, which is defined as the average over all nucleons in all events,
\begin{equation}\label{elliptic}
v_2^{} =\left\langle \frac{p_x^2 - p_y^2}{p_x^2 + p_y^2} \right\rangle
\end{equation}
with $p_x$ and $p_y$ being, respectively, the projections of the nucleon transverse momentum along the $x$ and $y$ axes in the transverse plane, which is perpendicular to the reaction plane, the transverse flow velocity is anisotropic with respect to the azimuthal angle $\phi_b$. Following Ref.~\cite{Oh:2009gx}, we parameterize the transverse flow velocity as
\begin{equation}
\bm{\beta} = \beta(r) \left[ 1 + \varepsilon(p_T^{}) \cos(2\phi_b)
\right] \hat{\bm{n}},
\label{beta}
\end{equation}
where $\hat{\bm{n}}$ is the unit vector in the direction of their transverse flow velocity $\bm{\beta}$, which is taken to be normal to the surface of the system defined below. The $p_T^{}$-dependent coefficient $\varepsilon$ is introduced to model the saturation of the nucleon elliptic flow at large $p_T^{}$ as observed in experiments, and is parameterized as
\begin{equation}\label{epsilon}
\varepsilon(p_T^{}) = c_1^{} \exp(-p_T^{}/c_2^{}).
\end{equation}
We further parameterize the radial flow velocity as
\begin{equation}\label{beta0}
\beta(r) = \beta_0 \left( \frac{r}{R_0} \right),
\end{equation}
where $R_0$ is a parameter related to the transverse size of the nucleon distribution in space and $r$ is the distance of the nucleon from the origin of the coordinate system in the transverse plane.

For the spatial distribution of nucleons, it is assumed to be uniformly distributed inside a cylinder with its axis along the longitudinal direction and having an elliptic shape in the transverse plane, given by
\begin{equation}
\left( \frac{x}{A} \right)^2 + \left( \frac{y}{B} \right)^2\le1,
\label{ellipse1}
\end{equation}
with $A$ and $B$ related to the spatial elliptic anisotropy or eccentricity~\cite{Lin:2001zk}, $s_2^{} =\langle (x^2 - y^2)/(x^2 + y^2)\rangle$, by
\begin{equation}
A = R_0 (1 + s_2^{}), \qquad B = R_0 (1 - s_2^{}).
\end{equation}
The spatial region as given by Eq.~(\ref{ellipse1}) can also be rewritten as
\begin{equation}\label{radius}
r \le R_0 \left[ 1 + s_2^{} \cos(2\phi) \right]
\end{equation}
in terms of the azimuthal angle $\phi$ of the nucleon position vector ${\bf r}$ in the transverse plane. It can be shown that the angle $\phi$ is related to the azimuthal angle $\phi_b$ of transverse flow by $\tan\phi=(B/A)^2\tan\phi_b$~\cite{Sun:2015jta}.

\begin{figure}[h]
\centerline{
\includegraphics[width=10cm]{pt.eps}}
\caption{(Color online) Transverse momentum spectra of midrapidity proton, deuteron (anti-deuteron) and triton (helium-3) from the blast-wave model (dashed lines) and the coalescence model (solid lines) for Au+Au collisions at $\sqrt{s_{NN}}=200$ GeV and centrality of 0-80\%. Data are from Ref.~\cite{Abelev:2006jr} for proton, Ref.~\cite{Adler:2004uy} for deuteron (anti-deuteron), and Ref.~\cite{Abelev:2009ae} for triton (helium-3).}
\label{pt}
\end{figure}

For Au$+$Au collisions at center of mass energy $\sqrt{s_{NN}^{}} = 200$~GeV and centrality of 0-80\%, the parameters in the blast-wave model are taken as follows to reproduce the transverse momentum spectrum and elliptic flow of protons measured at RHIC. For the spatial distribution of nucleons, we use the parameters
\begin{eqnarray}
R_0 =10.0 \mbox{ fm},~s_2^{} = -0.04,~\tau_0^{}= 9.0 \mbox{ fm}/c,
\end{eqnarray}
For the transverse momentum distribution, we use the kinetic temperature $T_K^{} = 130$~MeV and
\begin{eqnarray}
\beta_0 = 0.67,~c_1^{} = 0.148,~c_2^{} = 2.12 \mbox{ GeV}/c
\label{eq:parameters}
\end{eqnarray}
for the flow velocity parameterized in Eqs.~(\ref{beta})-(\ref{beta0}). The measured total number of protons $N_p = 4.8$ is obtained from  the blast-wave model by using zero charge and baryon chemical potentials as well as a fugacity parameter $\xi=1.76$. These protons and a same number of neutrons are then uniformly distributed in the rapidity region $|y| \le 0.5$. The resulting transverse momentum spectrum and elliptic flow of protons are shown by the black solid lines in Figs.~\ref{pt} and \ref{v2}, respectively, and they are seen to reproduce very well the experimental data, shown by squares, from the STAR Collaboration~\cite{Abelev:2006jr,Adamczyk:2015ukd}.

\begin{figure}[h]
\centerline{
\includegraphics[width=10cm]{v2.eps}}
\caption{(Color online) Elliptic flows of midrapidity proton, deuteron (anti-deuteron) and triton (helium-3) from the blast-wave model (dashed lines) and the coalescence model (solid lines) for Au+Au collisions at $\sqrt{s_{NN}}=200$ GeV and centrality of 0-80\%. Data are from Ref.~\cite{Adamczyk:2015ukd} for proton, Ref.~\cite{Adamczyk:2016gfs} for deuteron (anti-deuteron) and triton (helium-3).}
\label{v2}
\end{figure}

\section{the coalescence model}\label{coalescence}

The coalescence model for nuclei production in heavy ion collisions is based on the sudden approximation of projecting out their wave functions from the wave functions of nucleons at freeze out.  As shown in Ref.~\cite{Mattiello:1996gq}, the number of nucleus of atomic number $A$ and consisting of $Z$ protons and $N$ neutrons produced in a heavy ion collision is given by the overlap integral of the Wigner function $f_A({\bf x}_1^\prime, ... ,{\bf x}_Z^\prime,{\bf x}_1^\prime, ... ,{\bf x}_N^\prime; {\bf p}_1^\prime, ... ,{\bf p}_Z^\prime,{\bf p}_1^\prime, ... ,{\bf p}_N^\prime,t^\prime)$ of the produced nucleus with the phase-space distribution function
$f_p({\bf x},{\bf p},t)$ of protons and $f_n({\bf x},{\bf p},t)$ of neutrons at freeze out, which is normalized to the total proton number $N_p$ and neutron number $N_n$ according to $\int p^\mu d^3\sigma_{\mu}\frac{d^3{\bf p}}{E}f_p({\bf x}, {\bf p},t)=N_p$ and $\int p^\mu d^3\sigma_{\mu}\frac{d^3{\bf p}}{E}f_n({\bf x}, {\bf p},t)=N_n$, that is
\begin{eqnarray}
\label{coal}
&&\frac{dN_A}{d^3 {\mathbf P}_A}=g_A\int \Pi_{i=1}^Zp_i^\mu d^3\sigma_{i\mu}\frac{d^3{\bf p}_i}{E_i}f_p({\bf x}_i, {\bf p}_i,t_i)\nonumber\\
&&\times\int \Pi_{j=1}^Np_j^\mu d^3\sigma_{j\mu}\frac{d^3{\bf p}_j}{E_j}f_n({\bf x}_j, {\bf p}_j,t_j)\nonumber\\
&&\times f_A({\bf x}_1^\prime, ... ,{\bf x}_Z^\prime,{\bf x}_1^\prime, ... ,{\bf x}_N^\prime; {\bf p}_1^\prime, ... ,{\bf p}_Z^\prime,{\bf p}_1^\prime, ... ,{\bf p}_N^\prime;t^\prime)\nonumber\\
&&\times \delta^{(3)}\left({\bf P}_A-\sum_{i=1}^Z{\bf p}_i-\sum_{j=1}^N{\bf p}_j\right),
\end{eqnarray}
where $g_A=(2J_A+1)/2^A$ is the statistical factor for $A$ nucleons of spin $1/2$ to form a nucleus of angular momentum $J_A$.  As in Refs.~\cite{Chen:2003ava,Oh:2009gx}, the coordinate ${\bf x}_i$ and momentum ${\bf p}_i$ are those of the $i$-th nucleon in the center of mass of all emitted particles in the blast wave. The corresponding coordinate ${\bf x}_i^\prime$ and momentum ${\bf p}_i^\prime$, which appear in the nuclear Wigner function, are obtained by first Lorentz transforming to the rest frame of produced nucleus and then letting this nucleon to propagate freely with a constant velocity, given by the ratio of  its momentum and energy in the rest frame of the nucleus, until the time $t^\prime$ when the last nucleon in the nucleus freezes out.

For the light nuclei we consider in this study, ${\rm d}$, $\bar{\rm d}$, ${\rm t}$, and $^3{\rm He}$, we approximate their wave functions by those of the ground state of a harmonic oscillator with the oscillator constant adjusted to fit the empirical charge radii of these nuclei. The Wigner function for ${\rm d}$ and similarly for $\bar{\rm d}$ is then~\cite{Song:2012cd}
\begin{eqnarray}
f_2(\boldsymbol\rho,{\bf p}_\rho)=8g_2\exp\left[-\frac{\boldsymbol\rho^2}{\sigma_\rho^2}-{\bf p}_\rho^2\sigma_\rho^2\right],
\label{two}
\end{eqnarray}
with
\begin{eqnarray}\label{rel}
\boldsymbol\rho=\frac{{\bf x}_1^\prime-{\bf x}_2^\prime}{\sqrt{2}},\quad{\bf p}_\rho=\frac{{\bf p}_1^\prime-{\bf p}_2^\prime}{\sqrt{2}},\nonumber\\
\end{eqnarray}
where we have used the same mass $m$ for proton and neutron.

Similarly, the Wigner function for ${\rm t}$ and $^3{\rm He}$ is~\cite{Song:2012cd}
\begin{eqnarray}
&&f_3(\boldsymbol\rho,\boldsymbol\lambda,{\bf p}_\rho,{\bf p}_\lambda)\nonumber\\
&&=8^2g_3\exp\left[-\frac{\boldsymbol\rho^2}{\sigma_\rho^2}-\frac{\boldsymbol\lambda^2}{\sigma_\lambda^2}-{\bf p}_\rho^2\sigma_\rho^2-{\bf p}_\lambda^2\sigma_\lambda^2\right],
\label{three}
\end{eqnarray}
where $\boldsymbol\rho$ and ${\bf p}_\rho$ are similarly defined as in Eq.(\ref{rel}), and
\begin{eqnarray}
{\boldsymbol\lambda}&=&\frac{{\bf x}_1^\prime+{\bf x}_2^\prime-2{\bf x}_3^\prime}{\sqrt{6}},\nonumber\\
{\bf p}_\lambda&=&\frac{{\bf p}_1^\prime+{\bf p}_2^\prime-2{\bf p}_3^\prime}{\sqrt{6}}.
\end{eqnarray}

The width parameter $\sigma_\rho$ in Eq.(\ref{two}) is related to the charge mean-square radius of deuteron and
also the oscillator frequency $\omega$ in the harmonic wave function via~\cite{Song:2012cd}
\begin{eqnarray}
\langle r_{\rm d}^2 \rangle=\frac{3}{4}\sigma_\rho^2=\frac{3}{4m\omega},
\end{eqnarray}
where the second line follows if we use the relation $\sigma_\rho=1/\sqrt{m\omega}$ in terms of the oscillator frequency $\omega$ in the harmonic wave function.

For the width parameter $\sigma_\lambda$ in Eq.(\ref{three}), it is again related to the oscillator frequency by $\sigma_\lambda=1/\sqrt{m\omega}$ and is thus equal to $\sigma_\rho$.  Both $\sigma_\rho$ and $\sigma_\lambda$ are then determined from the oscillator constant via the mean-square charge radius of ${\rm t}$ or $^3{\rm He}$, that is~\cite{Song:2012cd}
\begin{eqnarray}
\langle r_{\rm t}^2\rangle=\frac{1}{m\omega}, \quad\langle r_{\rm ^3He}^2\rangle=\frac{2}{m\omega}.
\end{eqnarray}

\begin{table}[h]
\caption{{\protect\small Statistical factor ($g$), root-mean-square charge radius ($R_{\rm ch}$), oscillator frequency ($\omega$), and width parameter ($\sigma_\rho$, $\sigma_\lambda$) for deuteron and anti-deuteron (${\rm d}$, $\bar{\rm d}$), triton(${\rm t}$), and helium-3 ($^3{\rm He}$). Radii are taken from Ref.~\cite{Angeli:2013}}.} \label{tab}
\smallskip
\begin{tabular}{c|cccccc}
\hline\hline
Nucleus & $g$ & $R_{\rm ch}$ (fm) & $\omega$ (sec$^{-1})$ & $\sigma_\rho, \sigma_\lambda$ (fm) \\
\hline
${\rm d}$,$\bar{\rm d}$ & 3/4 & 2.1421 & 0.1739 & 2.473 \\
${\rm t}$ & 1/4 & 1.7591 & 0.3438 & 1.759 \\
$^3{\rm He}$ & 1/4 & 1.9661 & 0.5504 & 1.390 \\
\hline\hline
\end{tabular}
\end{table}

The statistical factors and the values of the width parameters in the Wigner functions for ${\rm d}$, $\bar{\rm d}$, ${\rm t}$, and $^3{\rm He}$ as well as the empirical values of their charge radii and the resulting oscillator constants are given in Table \ref{tab}.

\section{results}\label{results}

In the present section, we show the transverse momentum spectra and elliptic flows for ${\rm d}$ ($\bar{\rm d}$) and ${\rm t}$ ($^3{\rm He}$) calculated from the coalescence model using the phase-space distributions of protons and neutrons from the blast-wave model.

\subsection{Transverse momentum spectra}

The transverse momentum spectrum of deuteron (anti-deuteron) in Au+Au collisions at $\sqrt{s_{NN}}=200$ GeV and centrality of $0-80\%$ is shown by the blue solid line in Fig.~\ref{pt}. It reproduces very well the data from the PHENIX Collaboration~\cite{Adler:2004uy} shown by circles. For comparison, we also show by the blue dashed line the deuteron transverse momentum spectrum from the blast wave model, which is obtained by replacing the proton mass by that of the deuteron and fitting the deuteron total number by taking the deuteron fugacity to be $\xi_d=2.1$. It is seen to be very similar to that from the coalescence model except slightly smaller at transverse momentum below about 2 GeV.  Also shown by the red solid line in Fig.~\ref{pt} is the transverse momentum spectrum of triton (helium-3) from the coalescence model, which is slightly larger than the experimental data, shown by triangles, from the STAR Collaboration~\cite{Abelev:2009ae}.   Results from the blast-wave model, shown by the red dashed line, for the transverse momentum spectrum of triton (helium-3) can describe, on the other hand, the experimental data very well with  the fugacity of triton (helium-3) taken to be $\xi_t=3.9$.

\subsection{Elliptic flows}

The azimuthal angle $\phi_T$ distribution of the transverse momentum ${\bf p}_T$ of nucleus $A$ produced in a heavy ion collision can be generally written as
\begin{eqnarray}
&&f_A(p_T,\phi_T,y)=\frac{N_A(p_T,y)}{2\pi}\nonumber\\
&&~~~\times\left\{1+2\sum_n v_n(p_T,y)\cos[n(\phi_T-\Psi_n)]\right\},
\end{eqnarray}
where $\Psi_n$ is the $n$th-order event plane angle, and $N_A(p_T,y)$ and $v_n(p_T,y)$ are the number of such nucleus in rapidity $y$ and their $n$th-order anisotropic flows, respectively. In the present study, we are only interested in the elliptic flow $v_2$.  Also, we take the event plane angle $\Psi_2=0$ because we generate many nucleons from the blast wave to reduce the statistical fluctuations due to the small number of nucleons in an event.  In this case, the elliptic flow can be simply calculated from Eq.(\ref{elliptic}).

In Fig.~\ref{v2}, we show by the blue solid line the deuteron $v_2$ from the coalescence model. Compared to the experimental data, shown by circles, from the STAR Collaboration~\cite{Adamczyk:2016gfs}, it overestimates the data above 2 GeV. On the other hand, the deuteron $v_2$ from the blast-wave model, shown by the blue dashed line, is smaller than the experimental data at all values of transverse momentum. The same is for the $v_2$ of triton (helium-3), shown by the red solid line, that it is smaller than the experimental data from the STAR Collaboration~\cite{Adamczyk:2016gfs}, shown by triangles, at small $p_T$ but larger at larger $p_T$, while that from the blast-wave model, shown by the red dashed line, again underestimates the data at all $p_T$.

\begin{figure}[h]
\centerline{
\includegraphics[width=10cm]{v2s.eps}}
\caption{(Color online) Same as Fig.~\ref{v2} for constituent nucleon number scaled elliptic flows of midrapidity proton, deuteron (anti-deuteron) and triton (helium-3).}
\label{v2s}
\end{figure}

It is known that in the coalescence model for light nuclei production, the nucleon-number scaled elliptic flows  satisfy a scaling law that the elliptic flow of a nucleus per nucleon at transverse momentum $p_T$ is the same as a function of $p_T$ divided by the number of nucleons in the nucleus~\cite{Yan:2006bx,Zhu:2015voa}. For light nuclei considered here, $v_{2}(p_T/A)/A$ is then the same. This scaling would be exact if only nucleons of same momentum can coalesce to form a nucleus, corresponding to a width parameter in the Wigner function of the nucleus that is infinitely large~\cite{Chen:2006vc}.  For the elliptic flows of light nuclei from the present coalescence model, the nucleon number scaled elliptic flows of deuteron (anti-deuteron) and triton (helium-3) are shown in Fig.~\ref{v2s} by the blue and red solid lines, respectively, as functions of the scaled transverse momentum. It is seen that both follow closely the proton elliptic flow (black line) and thus indeed show a scaling behavior.  The scaling behavior of the elliptic flows of light nuclei is also seen in the experimental data at $p_T/A< 1$ GeV. At large $p_T/A$, the scaled elliptic flows of deuteron (anti-deuteron) and triton (helium-3) from the experiments are smaller than the measured proton elliptic flow. The corresponding results from the blast-wave model, shown by the blue and red dashed lines for deuteron (anti-deuteron) and triton (helium-3), respectively, are similar to the results from the coalescence model for $p_T/A<0.7$ GeV and thus also show a scaling behavior. At larger $p_T/A$, no scaling behavior is seen for the elliptic flows from the blast-wave model. Instead, we see a strong mass ordering that the scaled elliptic flow of deuteron (anti-deuteron) is smaller than the proton elliptic flow and that of triton (helium-3) is further smaller than that of deuteron (anti-deuteron).

\subsection{Effects of space-momentum correlation}

\begin{figure}[h]
\centerline{\includegraphics[width=10cm]{pti.eps}}
\caption{(Color online) Transverse momentum spectra of midrapidity proton, deuteron (anti-deuteron), and triton (helium-3) from the coalescence model based on a blast-wave model with  space-momentum correlation (solid lines) for Au+Au collisions at $\sqrt{s_{NN}}=200$ GeV at centrality of 0-80\%. Data are from Ref.~\cite{Abelev:2006jr} for proton, Ref.~\cite{Adler:2004uy} for deuteron (anti-deuteron), and Ref.~\cite{Abelev:2009ae} for triton (helium-3).}
\label{ptnew}
\end{figure}

Results shown in the previous subsection based on the coalescence model indicate that assuming the spatial distribution of nucleons is independent of their momenta fails to describe experimentally measured differential elliptic flows of light nuclei, particularly at high momenta where the theoretical results are larger than the experimental values.  Since light nuclei of large transverse momenta are produced in the coalescence model from nucleons of large transverse momenta, their elliptic flows can be reduced if these nucleons are more separated along the reaction plane than in the perpendicular direction. This is because such a space-momentum correlation reduces the production of light nuclei along the reaction plane and enhances it in the perpendicular direction.  Such a correlation can be introduced in the blast-wave model by requiring nucleons of $p_T> 0.9$ GeV to have a radius parameter $R_0=10~e^{0.23(p_T-0.9)}$ fm in Eq.(\ref{radius}) for $|p_{Tx}|>|p_{Ty}|$. For all other nucleons, the radius parameter is taken to be $R_0=10.0$ fm as in Section II.

As shown by black solid lines in Figs.~\ref{ptnew} and \ref{v2new}, the experimental proton transverse momentum spectrum and elliptic flow can still be very well reproduced with the same parameters given in Eqs.(16) and (17). For the transverse momentum spectra and elliptic flows of deuteron (anti-deuteron) and triton (helium-3) from the coalescence model based on the phase-space distribution functions of nucleons in the blast-wave model that includes the space-momentum correlation, they are shown, respectively, by blue and red solid lines in these figures. They are seen to describe very well the experimental data not only on the transverse momentum spectrum but also the elliptic flow of deuteron (anti-deuteron) and triton (helium-3).

\begin{figure}[h]
\centerline{\includegraphics[width=10cm]{v2i.eps}}
\caption{(Color online) Elliptic flows of midrapidity proton, deuteron (anti-deuteron), and triton (helium-3) at midrapidity from the coalescence model based on a blast-wave model with space-momentum correlation (solid lines) for Au+Au collisions at $\sqrt{s_{NN}}=200$ GeV at centrality of 0-80\%. Data are from Ref.~\cite{Adamczyk:2015ukd} for proton, Ref.~\cite{Adamczyk:2016gfs} for deuteron (anti-deuteron) and triton (helium-3).}
\label{v2new}
\end{figure}

\section{summary}\label{summary}

Using the coalescence model based on the nucleon phase-space distribution function from a blast-wave model, we have studied the transverse momentum spectra and elliptic flows of light nuclei in relativistic heavy ion collisions.  Assuming that the spatial distribution of nucleons in the system is independent of their momenta and fitting the parameters to the experimental measured proton transverse momentum spectrum and elliptic flow by the STAR collaboration at RHIC, we have obtained a good description of the measured transverse momentum spectra of deuteron (anti-deuteron) and triton (helium-3) but have failed to reproduce the measured elliptic flows of these nuclei, particularly at large transverse momenta.  We have attributed this failure of the coalescence model to the neglect of possible preference of nucleons of large transverse momenta to be more spread in space if their momenta are along the reaction plane than perpendicular to it.  Allowing a nucleon phase-space distribution that includes such space-momentum correlations in the blast-wave model indeed leads to a good description of the elliptic flows of deuteron (anti-deuteron) and triton (helium-3) as well.  Our study thus indicates that the elliptic flows of light nuclei are sensitive to the space and momentum correlations of nucleons at kinetic freeze out and are thus a possible probe of the nucleon emission source in relativistic heavy ion collisions.

\section*{Acknowledgements}

We thank Lie-Wen Chen, Zi-Wei Lin, Kaijia Sun, and Jun Xu for helpful communications and/or discussions.  One of the authors (C.M.K.) is grateful to the Physics Department at Sichuan University for the warm hospitality during his visit when this work was carried out.  This work was supported in part by the NSFC of China under Grant no. 11205106, the US Department of Energy under Contract No. DE-SC0015266, and The Welch Foundation under Grant No. A-1358.

redpajama_set_name: RedPajamaArXiv


text:
June 26, 1928 – October 9, 2003
Instrument tenor sax
Birthplace Wenatchee, WA
Stop - Don Lanphere Latin (medium)
Adept at tenor saxophone, alto saxophone, and alto clarinet, Don Lanphere was a prominent saxophonist and educator with two distinct phases of his career. A young prodigy, Lanphere began playing professionally at age 13. At 17, he sat in with Jimmie Lunceford's Orchestra when they came through his hometown.
While studying music at Northwestern University, Don Lanphere joined Johnny Bothwell's band moved with them to New York. He parted ways with them soon after and joined trumpeter Fats Navarro and drummer Max Roach; his recordings with them are the ones for which he is best known. In 1949, he joined the Woody Herman band, followed by a stint with Artie Shaw's orchestra. He gigged intermittently with the bands of Claude Thornhill, Sonny Dunham, Billy May and Charlie Barnet. He recorded with Charlie Parker during this period as well.
In 1951, Don Lanphere moved back to his hometown, where he ran his father's music store. In 1969, he became a born-again Christian and returned to playing. In 1982, he made a full comeback and signed with Scottish label Hep Records, with whom he released several well-received albums, such as "Don Loves Midge" in 1984. In 1996, he moved to Origin Records. He became a renowned educator in the Pacific Northwest known for his clinics and small groups as well as appearances at jazz workshops. He inspired the (then up-and-coming) pianist Marc Seales and trumpeter Jon Pugh in particular. He continued to perform and record until his death in 2003.


Above: Flappy Bird isn't in mobile app stores any more because it's too addictive, says its creator.
Flappy Bird has topped the charts of free mobile apps in the iOS and Google Play app stores.
Meanwhile,Sarah Young of NativeX, has her own take on why the game is so viral.


text:
Coronavirus spread: In which states is COVID-19 growing fastest?
Samuel Stebbins / 24/7 Wall Street
The spread of the novel coronavirus appears to be slowing in the United States. Over the last week – from May 12th through May 18th – there were an average of about 6.8 new cases per day nationwide for every 100,000 people, a 16% decline from the previous week.
The improvement, while encouraging, also serves as a reminder of the continuing threat the virus poses – although the rate of infection may be slowing across much of the country, tens of thousands of Americans continue to be infected every day. In some states, the daily rate of new infections is far higher than in others.
To determine the states where the number of confirmed cases per capita is growing the fastest right now, 24/7 Wall St. compiled and reviewed the numbers of confirmed COVID-19 cases and deaths for the seven days through May 18 from state and local health departments. We calculated the average number of new cases per day between May 12 and May 18 in each state for every 100,000 people.
Many of the states where the virus is spreading the fastest are among the states that have been the hardest hit since the beginning of the pandemic. There are eight states where the daily infection rate over the last week is more than double the national figure – and each of them ranks among the 10 states with the highest overall infection rate. Most of these states are densely-populated places in the Northeast and mid-Atlantic.
The declining daily infection rate in the United States is due in large part to restrictions put in place by state and local governments. While many states have lifted strict stay-at-home orders, social distancing laws and guidelines remain in much of the country.
50. Hawaii
• Avg. new cases per day from May 12 - May 18: 0.1 per 100,000 people (total avg. new daily cases: 1)
• COVID-19 related deaths from May 12 - May 18: None
• Confirmed COVID-19 cases as of May 18: 45.1 per 100,000 people – 2nd fewest (total: 640)
• Tests completed as of May 18: 2,968.3 per 100,000 people – 21st fewest (total: 42,164)
• Population: 1.4 million (129.9 people per sq. mile – 20th most)
• First confirmed case: March 6, 2020
49. Montana
• Confirmed COVID-19 cases as of May 18: 44.2 per 100,000 people – the fewest (total: 470)
• Tests completed as of May 18: 2,651.5 per 100,000 people – 12th fewest (total: 28,167)
• Population: 1.1 million (7.2 people per sq. mile – 3rd fewest)
• First confirmed case: March 13, 2020
48. Alaska
• Confirmed COVID-19 cases as of May 18: 54.1 per 100,000 people – 3rd fewest (total: 399)
• Tests completed as of May 18: 4,829 per 100,000 people – 11th most (total: 35,611)
• Population: 737,438 (1.1 people per sq. mile – the fewest)
47. Vermont
• COVID-19 related deaths from May 12 - May 18: 1
• Confirmed COVID-19 cases as of May 18: 150.1 per 100,000 people – 10th fewest (total: 940)
• Tests completed as of May 18: 3,804.1 per 100,000 people – 17th most (total: 23,825)
• Population: 626,299 (65.1 people per sq. mile – 21st fewest)
• Avg. new cases per day from May 12 - May 18: 1 per 100,000 people (total avg. new daily cases: 18)
• Confirmed COVID-19 cases as of May 18: 82.6 per 100,000 people – 4th fewest (total: 1,491)
• Population: 1.8 million (74.5 people per sq. mile – 22nd fewest)
• Avg. new cases per day from May 12 - May 18: 1.3 per 100,000 people (total avg. new daily cases: 23)
• Confirmed COVID-19 cases as of May 18: 137.9 per 100,000 people – 9th fewest (total: 2,419)
• Tests completed as of May 18: 2,078.2 per 100,000 people – the fewest (total: 36,456)
• Population: 1.8 million (21 people per sq. mile – 7th fewest)
44. Oregon
• Confirmed COVID-19 cases as of May 18: 88 per 100,000 people – 5th fewest (total: 3,687)
• Tests completed as of May 18: 2,320.2 per 100,000 people – 6th fewest (total: 97,232)
• Population: 4.2 million (42.6 people per sq. mile – 13th fewest)
• First confirmed case: Feb. 28, 2020
43. Missouri
• Avg. new cases per day from May 12 - May 18: 2.3 per 100,000 people (total avg. new daily cases: 144)
• COVID-19 related deaths from May 12 - May 18: 70
• Confirmed COVID-19 cases as of May 18: 178.7 per 100,000 people – 15th fewest (total: 10,945)
• Tests completed as of May 18: 2,515.5 per 100,000 people – 8th fewest (total: 154,110)
• Population: 6.1 million (87.9 people per sq. mile – 23rd fewest)
• Tests completed as of May 18: 3,557.2 per 100,000 people – 21st most (total: 140,262)
41. Maine
• Confirmed COVID-19 cases as of May 18: 128 per 100,000 people – 7th fewest (total: 1,713)
40. South Carolina
• Confirmed COVID-19 cases as of May 18: 175.9 per 100,000 people – 13th fewest (total: 8,942)
• Tests completed as of May 18: 2,587.6 per 100,000 people – 10th fewest (total: 131,559)
• COVID-19 related deaths from May 12 - May 18: 194
• Confirmed COVID-19 cases as of May 18: 218 per 100,000 people – 19th fewest (total: 46,442)
• Tests completed as of May 18: 3,181.8 per 100,000 people – 23rd fewest (total: 677,710)
• Population: 21.3 million (323.9 people per sq. mile – 8th most)
38. Washington
• Tests completed as of May 18: 3,785.3 per 100,000 people – 18th most (total: 285,243)
• Population: 7.5 million (105.7 people per sq. mile – 23rd most)
• First confirmed case: Jan. 21, 2020
37. Wyoming
• Confirmed COVID-19 cases as of May 18: 98 per 100,000 people – 6th fewest (total: 566)
• Population: 577,737 (5.9 people per sq. mile – 2nd fewest)
• Population: 3 million (56.7 people per sq. mile – 17th fewest)
35. Nevada
• Confirmed COVID-19 cases as of May 18: 229.1 per 100,000 people – 22nd fewest (total: 6,952)
• Population: 3 million (27.4 people per sq. mile – 9th fewest)
34. Kentucky
• Population: 4.5 million (110.6 people per sq. mile – 21st most)
33. Texas
• Avg. new cases per day from May 12 - May 18: 4 per 100,000 people (total avg. new daily cases: 1,144)
• Tests completed as of May 18: 2,519 per 100,000 people – 9th fewest (total: 723,013)
• Population: 28.7 million (106.9 people per sq. mile – 22nd most)
32. California
• Avg. new cases per day from May 12 - May 18: 4.2 per 100,000 people (total avg. new daily cases: 1,649)
• Tests completed as of May 18: 3,122.7 per 100,000 people – 22nd fewest (total: 1.2 million)
• Population: 39.6 million (241.7 people per sq. mile – 11th most)
• Confirmed COVID-19 cases as of May 18: 229 per 100,000 people – 21st fewest (total: 7,238)
• Tests completed as of May 18: 5,401.7 per 100,000 people – 8th most (total: 170,752)
29. Ohio
• Confirmed COVID-19 cases as of May 18: 243.4 per 100,000 people – 23rd fewest (total: 28,454)
28. Arizona
• First confirmed case: Feb. 5, 2020
26. Michigan
• Confirmed COVID-19 cases as of May 18: 519.4 per 100,000 people – 11th most (total: 51,915)
• Population: 10 million (103.4 people per sq. mile – 24th most)
25. Tennessee
• Confirmed COVID-19 cases as of May 18: 266 per 100,000 people – 24th most (total: 18,011)
24. New Hampshire
• Confirmed COVID-19 cases as of May 18: 269.2 per 100,000 people – 23rd most (total: 3,652)
23. Alabama
• Population: 4.9 million (93.2 people per sq. mile – 25th most)
• Tests completed as of May 18: 3,463 per 100,000 people – 22nd most (total: 364,289)
• Population: 10.5 million (177 people per sq. mile – 16th most)
• Tests completed as of May 18: 2,267.7 per 100,000 people – 2nd fewest (total: 129,159)
20. Kansas
• Confirmed COVID-19 cases as of May 18: 286.4 per 100,000 people – 22nd most (total: 8,340)
19. North Dakota
• Confirmed COVID-19 cases as of May 18: 254.1 per 100,000 people – 25th most (total: 1,931)
• Tests completed as of May 18: 7,441.5 per 100,000 people – 2nd most (total: 56,561)
• Population: 760,077 (10.8 people per sq. mile – 4th fewest)
18. New Mexico
• Confirmed COVID-19 cases as of May 18: 290.9 per 100,000 people – 21st most (total: 6,096)
• Population: 2.1 million (17.2 people per sq. mile – 6th fewest)
17. Pennsylvania
16. Indiana
15. Louisiana
• Confirmed COVID-19 cases as of May 18: 744.8 per 100,000 people – 8th most (total: 34,709)
• Population: 4.7 million (89 people per sq. mile – 25th fewest)
14. Mississippi
13. Virginia
• Tests completed as of May 18: 2,285.6 per 100,000 people – 3rd fewest (total: 194,677)
12. New York
• Avg. new cases per day from May 12 - May 18: 11 per 100,000 people (total avg. new daily cases: 2,156)
• Confirmed COVID-19 cases as of May 18: 1,791.6 per 100,000 people – the most (total: 350,121)
• Tests completed as of May 18: 7,232.5 per 100,000 people – 3rd most (total: 1.4 million)
11. Minnesota
• Avg. new cases per day from May 12 - May 18: 11 per 100,000 people (total avg. new daily cases: 619)
• Tests completed as of May 18: 2,791 per 100,000 people – 17th fewest (total: 156,606)
10. Iowa
• Avg. new cases per day from May 12 - May 18: 12.2 per 100,000 people (total avg. new daily cases: 384)
• Confirmed COVID-19 cases as of May 18: 1,661.8 per 100,000 people – 2nd most (total: 148,039)
• Population: 8.9 million (1,021.3 people per sq. mile – the most)
6. Connecticut
• Confirmed COVID-19 cases as of May 18: 1,066.9 per 100,000 people – 5th most (total: 38,116)
• Population: 3.6 million (644.5 people per sq. mile – 4th most)
• Confirmed COVID-19 cases as of May 18: 658 per 100,000 people – 9th most (total: 39,762)
• Tests completed as of May 18: 3,425.5 per 100,000 people – 23rd most (total: 206,994)
• Population: 6 million (487.1 people per sq. mile – 5th most)
• Avg. new cases per day from May 12 - May 18: 17.5 per 100,000 people (total avg. new daily cases: 1,206)
• Confirmed COVID-19 cases as of May 18: 1,261.2 per 100,000 people – 3rd most (total: 87,052)
• Population: 6.9 million (654 people per sq. mile – 3rd most)
3. Delaware
• Confirmed COVID-19 cases as of May 18: 813.6 per 100,000 people – 6th most (total: 7,869)
• Population: 967,171 (388.6 people per sq. mile – 6th most)
2. Illinois
1. Rhode Island
• Tests completed as of May 18: 10,912.9 per 100,000 people – the most (total: 115,384)
• Population: 1.1 million (684.3 people per sq. mile – 2nd most)
24/7 Wall Street is a USA TODAY content partner offering financial news and commentary. Its content is produced independently of USA TODAY.


A superb quality George III Irish antique fireplace of neoclassical design in variegated Jasper and white statuary marbles, circa 1775.
Mount Panther Estate, Downpatrick, N. Ireland and thence to Arborfield Garrison, Bailleul Sergeants' mess, Reading, Berkshire. The estate with house (it is not known who originally built it) was bought in 1772 by Francis Charles Annesley (1740–1802), 2nd Viscount Glerawly, 1st Earl of Annesley (1789) who remodelled the house and grounds, introducing a pleasure ground, Parkland and commissioned the chimneypiece. The house and estate buildings are now in a ruinous state after the architectural features including of course the chimneypieces were salvaged and the roof was removed in the late 1960s to avoid paying rates on the property.
The one piece shelf with uppermost a concave moulding enriched with fluting above a cyma moulding decorated with lamb's leaf. The frieze centred with a rectangular tablet which rests on the architrave, sculpted with a winged Cupid (love) holding his bow and an arrow being rearmed with a quiver of golden arrows by two attendants within a fruiting laurel wreath, framed by Jasper mounts. This is flanked by panels of Jasper in statuary frames and supported by a white moulding decorated with lozenge, four sided diamond shaped leaves and flanked by the end blockings decorated with circular medallions depicting confronted Sphinx (guardian and repository of arcane wisdom) sentinels on pedestals upheld by drapery swags knotted in the middle these are supported by the architrave of white marble with well carved elliptical ovals centred with open flowers and inlaid fluted dentils. The pilaster shaped jambs of tapering white shafts decorated with tiered swags of bell flowers and graduated drops terminating in calyx upheld by tied bows and linen drapes supported from swan neck flower heads. These are surmounted with tripod shaped, rams headed pedestals on a dark jasper background on which stand young classically clad gardeners gazing at each other; one leans on a hoe the other a garden rake, vividly exploiting the polychromatic effects of the vibrant colours of Jasper on white marble. The opening with simple moulded edge the whole raised on blocks. No doubt the symbolic decoration echo the Viscount's love of flowers and gardening.


Textbook Rescue is back again for 2018! This year, students and graduates from The University of Manchester have donated nearly 3000 quality used textbooks to help you out.
The event will launch on Friday, 21 September, so head to the Main Library and grab some free books from a range of disciplines. Then from Monday, 24 September, find your site library to pick up textbooks for your subject.
The giveaway will last until stocks are gone – don't miss out!
Textbook Rescue kicks off with a launch event at Main Library on Friday, 21 September, where books from all subject areas will be available to collect.
From Monday, 24 September onwards, subject specific books will be available at our site libraries.
All books are offered on a first come first serve basis.
As well as collecting free textbooks, staff will also be able to help you with getting started in the Library.


text:
Reducing Risks while Protesting & Today's COVID-19 Report | Fri Jun 12
This week, Public Health acknowledged that many protesters, particularly Black, Indigenous and People of Color, are choosing to take on the risk of potential exposure to COVID-19 because of the importance of confronting and undoing the systems of racism, oppression and brutality. People are protesting because their lives depend on it.
Public Health is concerned about the possible spread of COVID-19 at these large gatherings, and for the potential to exacerbate the racial/ethnic disparities in COVID-19 rates for communities of color, especially for Black, Native, Latinx, and Pacific Islander residents of King County.
We urge all people protesting against racial injustice to take steps to stay healthy and avoid bringing COVID-19 home with them. We need to keep each other healthy now and get to a more just future for everyone.
Further details are all available in a helpful post on the Public Health Insider.
Otherwise, this daily synthesis of the Public Health data is provided by Will Daugherty of Pacific Science Center. Thanks Will!
Public Health has updated the data dashboard. The daily summary shows that there were 8,644 confirmed cases of COVID-19 in King County as of 11:59 on June 11, 60 more than the previous day. There have been 571 confirmed deaths in King County due to COVID-19, 6.6% of all confirmed cases. The numbers that Public Health reports each day include delayed results from previous days.
The first graph below shows new cases (blue bars) and the 7-day average (red line). Of the 60 new cases reported today, 27 were confirmed yesterday and the remaining 33 were confirmed in previous days. The 7-day average of new cases per day peaked at 194 on April 1. The average for the last 7 days is now 29 new cases per day, down from 45 one week ago. The 7-day average has declined 36% in the last week and 21% in the last two weeks.
The key indicators that the State and County are using to make decisions about reopening include a measure of the total number of cases reported in the previous 14 days per 100K residents. The target for this metric is less than 25. The second and third graphs below show this metric.
The second graph goes back to March 12, the fourteenth day of reported cases.
The third graph provided a more detailed view of results in the last few weeks. 23.3 cases were reported per 100K residents during the 14-day period May 29 – June 11.
Will Daugherty welcomes your questions and comments. His email is wdaugherty@pacsci.org
Immediate questions about your health?
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text:
Navigators by Turbo Knight Full Album Review
Navigators, the second album from Turbo Knight that knows what it wants to be, right from the start....
Dennis Gruetter
The purpose of a navigator is to explore. Navigators, the second album from Turbo knight is not only an album about exploration it's also an album that knows what it wants to be, right from the start.
Overall Navigators is a colossal space opera full of lush synthesizer arpeggios, over the top guitar riffs and memorable vocals. The album is heavily inspired by Frank Herbert's legendary novel Dune which is where the sound and song titles are derived from. Although the album is heavily inspired by Dune, the music style is very much Turbo Knight.
The album starts off not with a bang, but with a murmur. The opening murky notes tell the listener immediately they are on a journey inward. The drums kick in slow and deliberate and the lush synthesizer arpeggios enter in with a simple pacing. The mood of the track is finally completely set when the popular "tears in the rain" sample from the forever inspirational Blade Runner play in. This is the type of song that contains a simple melodic concept and builds upon it. While this may turn off some listeners looking for sonic diversity, I believe this song really sets the tone for what you can expect from the album. It's a deliberately paced album that's not as interested in taking the listener for a ride, than taking them on a journey.
Navigators is an album that feels more concerned with setting a mood rather than wanting to make your body move. that being said there are plenty of moments where the album picks up speed showing Turbo Knight's true potential as an artist.
The planet of Arrakis better known as Dune
"Arrakis" is a prime example of a track that defies expectations, and takes the listener for an unexpected turn. Just as Arrakis is an integral part of the story of Dune, "Arrakis" is also important to the album and here is the reason: With a slow majestic intro that quickly breaks into a pulse pounding club banger, this track tells the listener that there will always be something new and interesting right around the corner. It's also the first track on the album that shows the listener the true realization of Turbo Knight's greatest talent which is diversity. He sets expectations early on that anything goes in Turbo Knight's universe and the listener should be ready for anything.
The next track "Sleeper Has Awakened" featuring Straplocked seems to pour water on the hot fire left from the previous track. While I would have liked to have the album maintain it's momentum, "Sleeper" holds some good ground with it's sheer epic-ness. Straplocked does not disappoint either and delivers some really fine guitar work. This song could easily be placed in the final scenes of any great sci-fi movie.
Turbo Knight is certainly not afraid to take risks with his sound and this will never be as apparent as with his next track "Spice Must Flow." This song is a brilliant example of Turbo Knight's prolific talents. This may be the first time I have ever seen someone attempt to blend middle eastern vocals and rhythms with synthwave and Turbo Knight pulls it off flawlessly. "Spice Must Flow" is easily one of my favorite tracks on the album.
"Don't Forget Me" with Madelyn Darling was my first introduction to Turbo Knight. It's been out for at least a year now and yes, listening to it never gets old. Madelyn Darling's vocals are simply unforgettable and with a strong melody, this certainly is the high point of the album.
"The Dragon in the Sea of Sand" featuring Ultraboss is next and it's simply over the top awesomeness. While the melody is fairly simple and straightforward, it's the guitar work by Ultraboss that quickly gets all the attention. One might consider this track to be one big guitar solo, and that is certainly alright with me. It's easily some of the best guitar work I have heard in a long time and certainly a song that will linger in the mind long after listening.
"Water of Life" has a nice opening melody and wonderful twinkling arps. While certainly not the strongest song on the album, it does have some really nice builds. It is well produced with some really nice chord progression.
The chord progression on the next track "Age of Fremen" certainly got my attention. It's another well produced track with a nice tempo transition mid-way through. The repeated melody is fairly basic but it's the buildup that really makes this sound pleasing to listen to. It might not be my go to track, but there certainly enough things going on to make it a nice fit for the album.
One of the highlights of the album is also it's namesake "Navigators." Starquake Synthmaster delivers some amazing guitar work that would give Eddie Van Halen a run for the money. Strong arpeggios and some really nice chord stabs punctuate the already brilliant track. If I were to pick a standout track this would have to be it. It absolutely delivers on all levels and is a perfect example of someone doing synthwave right.
Rounding out the album are "House Harkonnen" with Sunesis and "Together We're Alone" featuring Magnus. Both vocal tracks but delivered quite differently. Sunesis provides an excellent storytelling element while Magnus rounds out the album with a very nice lead part. "Together We're Alone" leads the listener out of the album like a navigator washed away in the tide. It certainly places a very nice end cap that brings the listener full circle.
All in all I really liked the journey that Turbo Knight took me on. Navigators is full of interesting twists and turns. While I wasn't always thrilled about all the paths it took me on, in the end it was a journey worth taken.
Navigators will be released May 25th but you can catch a special exclusive track early on the next episode of The State of Synth.
Neon Arcadia & Megan McDuffee / Desire
Neon ArcadiaMegan McDuffee
Album Review: "Buena Vista" by Miles Matrix
ReviewAlbum
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text:
L'aire d'attraction de Tréguier est un zonage d'étude défini par l'Insee pour caractériser l'influence de la commune de Tréguier sur les communes environnantes. Publiée en octobre 2020, elle se substitue à l'aire urbaine de Tréguier, qui comportait  dans le dernier zonage qui remontait à 2010.

Définition
L'aire d'attraction d'une ville est composée d'un pôle, défini à partir de critères de population et d'emploi ainsi que d'une couronne constituée des communes dont au moins 15 % des actifs travaillent dans le pôle. Le pôle d'attraction constitue ainsi un point de convergence des déplacements domicile-travail.

Type et composition
L'aire d'attraction de Tréguier est une aire intra-départementale qui comporte  dans les Côtes-d'Armor.
Elle est catégorisée dans les aires de moins de .

Dans la région, la population est relativement peu concentrée dans les pôles. Ainsi, moins d'un tiers de la population y vit contre plus de la moitié au niveau national. Ce n'est pas le cas pour l'aire d'attraction de Tréguier qui présente une population de  localisés dans la région et dont 69,2 % résident dans le pôle.

En Bretagne, la population augmente de 0,6 % par an en moyenne entre 2007 et 2017 (+ 0,5 % en France). Pour l'aire de Tréguier, elle est de -0,7 %. Le nombre d'emplois présents dans l'aire d'attraction est de .

Carte

Composition communale

Notes et références

Voir aussi

Articles connexes

 Agglomération


text:
Former Michigan athletic director Joe Roberson of Flint dies at 84
Joe RobersonBPN
By Brendan Savage | bsavage@mlive.com and Ryan Zuke | rzuke1@mlive.com
FLINT – Flint native Joe Roberson, a former University of Michigan athletic director and member of the Greater Flint Area Sports Hall of Fame, died Monday at his home in Grand Blanc.
Roberson served as Michigan's AD from 1994-97 and hired Lloyd Carr as head football coach, leading to the Wolverines winning the national championship in 1997. Michigan also won national championships in both hockey (1996) and swimming and diving (1995) under Roberson's watch.
"Joe was an athletic director who communicated well with the coaches and cared about the student-athletes," former Michigan hockey coach Red Berenson said in a prepared statement. "He gained their respect and confidence and did that in a short while.
"Though he had to make major decisions during his tenure, he did it in a quiet way. I remember Joe's excitement when we won the national championship in 1996. Even though he was a baseball player, you could tell he was excited about our team and all our sports at the University of Michigan."
Roberson also hired current Michigan AD Warde Manuel.
"The loss of Joe Roberson marks an especially sad day for me," Manuel said in a statement. "Joe hired me here at the University of Michigan when I returned to Ann Arbor to get my doctorate. He could be considered my first major mentor. He believed in the student-athlete model with 'student' as the most important factor in participation.
"When Joe spoke, he did not mince words; he was straightforward and fair. Michigan is grateful for his service and so am I. He will be missed by me and by many."
Roberson was born on Sept. 22, 1935 in Flint and spent most of his life living in Genesee County. He attended Flint Northern High School and earned his college degree from the University of Michigan-Flint before getting his Master's degree and Ph.D. in Ann Arbor.
Before becoming the Wolverines' AD, he also served as Michigan's head of corporate fundraising from 1984-89 and associate vice president and executive director of the $1 billion Campaign for Michigan. He also served as UM-Flint's dean of students from 1966-80, vice chancellor from 1980-83 and interim chancellor from 1983-84.
On the athletic field, Roberson was an outstanding baseball pitcher who finished his local career by winning 31 straight games for Northern, in an American Legion league and the City Baseball League.
As a senior at Northern, he had a 9-0 record before going 6-0 with a 0.58 ERA in the CBL.
In basketball, he averaged 14.6 points in 54 career games for the Vikings and led the Saginaw Valley in scoring with a 20.7 average as a senior.
Upon graduating from high school, Roberson signed with the Los Angeles Dodgers and made it as far as Triple A before returning to Flint to concentrate on his studies beginning at Flint Junior College in 1958.
At FJC, he was ineligible to play baseball because of his pro career but was a basketball standout. Roberson was the first player in FJC history to score 1,000 career points, averaging 25.3 points in 44 career games while leading the team to a 41-3 record.
Roberson averaged 31 points in the three losses and once scored 50 in a 1954 game vs. Dearborn.
He was inducted into the GFASHOF in 1987.
Roberson retired at Michigan in 1997 after 31 years of service.
He was preceded in death by his first wife, Barbara, in 1989. They were married for 34 years and had two children, Kimberly and Marvin. Roberson married his second wife, Carolyn Conklin Black Roberson, in 1994. She died in 2013.
Visitation will take place from 4-7 p.m. Friday, Jan. 17 and at 10-11 a.m. Saturday, Jan. 18 at Hill Funeral Home in Grand Blanc. The funeral service is at 11 a.m. at Hill Funeral Home, 11723 S. Saginaw, Grand Blanc, 48439


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text:
Mathieu Enguérand Edjekpan Guerin (born 15 January 1985) is a Beninese former professional footballer who played as a defender for lower-league clubs in Italy. In 2001 and 2002 he made two appearances for the Benin national team.

Club career
Edjekpan was born in Porto Novo, Benin. He began his career 2003 in the youth from AS Saint-Étienne. A year later, he moved to Italy.

Edjekpan began now his professional career with Urbino playing 28 of 34 matches in the 2004–05 season. He signed for Grottaglie in July 2005 where he made 50 appearances scoring two goals before joining to Mesagne  in summer 2007.

International career
According to National Football Teams, Edjekpan is the youngest ever international footballer. Their records say that he played in a 2–0 loss to Angola in August 1998. He would have been 13 years and 213 days old at the time of his debut. However, RSSSF dispute the verifiability of this. He was called up again after a six-year absence for Benin in 2008.

References

External links

1985 births
Living people
People from Porto-Novo
Beninese footballers
Association football defenders
Benin international footballers
Beninese expatriate footballers
Beninese expatriate sportspeople in Italy
Expatriate footballers in Italy
Beninese expatriate sportspeople in France
Expatriate footballers in France


text:
package javax.wireless.messaging;

import androidx.annotation.NonNull;

import java.io.ByteArrayInputStream;
import java.io.IOException;
import java.io.InputStream;

import ru.playsoftware.j2meloader.util.IOUtils;

public class MessagePart {
	private final String mimeType;
	private final String contentId;
	private final String contentLocation;
	private final String enc;
	private final byte[] contents;

	public MessagePart(InputStream is,
					   String mimeType,
					   String contentId,
					   String contentLocation,
					   String enc)
			throws IOException, SizeExceededException {
		this.contents = IOUtils.toByteArray(is);
		this.mimeType = mimeType;
		this.contentId = contentId;
		this.contentLocation = contentLocation;
		this.enc = enc;
	}

	public MessagePart(byte[] contents,
					   String mimeType,
					   String contentId,
					   String contentLocation,
					   String enc)
			throws SizeExceededException {
		if (mimeType == null || contentId == null)
			throw new IllegalArgumentException();
		this.contents = contents.clone();
		this.mimeType = mimeType;
		this.contentId = contentId;
		this.contentLocation = contentLocation;
		this.enc = enc;
	}

	public MessagePart(byte[] contents,
					   int offset,
					   int length,
					   String mimeType,
					   String contentId,
					   String contentLocation,
					   String enc)
			throws SizeExceededException {
		if (mimeType == null ||
				contentId == null ||
				length < 0 ||
				offset < 0 ||
				offset + length > contents.length)
			throw new IllegalArgumentException();
		byte[] copy = new byte[length];
		System.arraycopy(contents, offset, copy, 0, length);
		this.contents = copy;
		this.mimeType = mimeType;
		this.contentId = contentId;
		this.contentLocation = contentLocation;
		this.enc = enc;
	}

	public byte[] getContent() {
		return contents;
	}

	public java.io.InputStream getContentAsStream() {
		return new ByteArrayInputStream(contents);
	}

	public String getContentID() {
		return contentId;
	}

	public String getMIMEType() {
		return mimeType;
	}

	public String getEncoding() {
		return enc;
	}

	public String getContentLocation() {
		return contentLocation;
	}

	public int getLength() {
		return contents.length;
	}

	public boolean equals(Object o) {
		return super.equals(o);
	}

	public int hashCode() {
		return super.hashCode();
	}

	@NonNull
	public String toString() {
		return super.toString();
	}
}

redpajama_set_name: RedPajamaGithub


text:
Record numbers turn out for Tokyo International Art Fair 2019
12th July 2019: Belle Salle Roppongi was teeming with talented artists, leading galleries and appreciative art lovers in their thousands as the city of Tokyo played host to the 5th annual Tokyo International Art Fair.
The two day art fair, one of the highlights of the city's cultural calendar, featured work created by leading artists from around the world including Ron English, Cho, Hui-Chin, High Art Gallery and Araki Nobuyoshi. Artists and visitors alike declared it a huge success, with record numbers turning out to show, enjoy and buy art.
More than 100 exhibitors from 23 countries travelled to Tokyo to take part in the largest free to attend showcase of contemporary art seen in the city. Paintings, sculpture, photography, illustrations, jewellery and bespoke crafts transformed the setting into a sea of colours, as the aisles buzzed with excitement as visitors chatted to the artists and snapped up unique works.
Trade was brisk, with artists and galleries reporting strong sales throughout the event, as Tokyo International Art Fair director and curator Joëlle Dinnage explains. "It was the fifth time that I and my colleagues from the Global Art Agency travelled to Tokyo to host the art fair and this year surpassed all our expectations," she says.
"I can honestly say that it was one of the busiest, most vibrant art fairs we have ever organised anywhere in the world, with an incredible atmosphere on both days. The excitement was palpable.
"Wherever I looked, I saw artists, surrounded by enthralled visitors, talking passionately about their work. We were totally bowled over by the level of talent on display, something which made judging the Tokyo International Art Fair Awards on the second day harder than ever. Finally, we did select our winners1 and I warmly congratulate them, though everyone who took part was worthy of praise," she says.
WINNERS OUTSTANDING ARTIST AWARDS TIAF 2019
1) Harry Arling (Netherlands) middle https://www.instagram.com/kosmotroniks
2) Jiro Shimizu (Austria) left www.jiro.tv
3) Tunikov (Russia) right www.tunikov.com
The organisers' enthusiasm was matched by the artists present, who were quick to share their appreciation for the event.
"It was a great opportunity to be a part of the show. I was able to meet an incredible amount of extremely talented artists as well as gallery representatives from all around the country and the world. I can't thank you enough. I know that being part of such a high calibre event is going to be a major part of my success story," says American artist Johnny, the "The Spilt Ink", who resides in Tokyo.
"I too had a great time at the Tokyo International Art Fair," says Dutch artist Stephan van Riezen. "I sold a few paintings, but most importantly, I met amazing people. I'm in love with Tokyo now, something which is giving me great inspiration."
"Tokyo was great and so was the art fair," adds painter Rima Chahine. "I sold all of my paintings, so I am very happy with the results. The atmosphere of the opening night and the second day was stunning and captivating. I made many friends, both artists and collectors, and met buyers and potential buyers."
Dates for the sixth Tokyo International Art Fair are beginning of June 2020, applications to participate will open shortly, but in the meantime, artists and galleries can register their interest for next year's event by going to http://www.tokyoartfair.com/apply-to-exhibit-tokyo-art-fair.
More information about the event can be found at www.tokyoartfair.com.
The event is organised by http://www.globalartagency.com/
Sarah Pracey + 44 7985 112 777 / sarah@praceypr.com
office@globalartagency.com / contact@joelledinnage.com www.joelledinnage.com
Note to editors:
Details of the winners of the Tokyo International Art Fair Awards 2019 can be found here.
Tagged: Tokyo International Art Fair 2019, TIAF 2019, Tokyo Art Fair 2019, Tokyo, Art, Global Art Agency
Second Tokyo International Art Fair brings famous names to Omotesando Hills
Canal Cheong Jagerroos
Franco the Creator
Hayat Saidi
Kaze Gallery
Li Wei Chen
Loryn Kolbrenner
Mark James Ford
Sophia Shiyan
Suzi Fadel Nassif
Svetlana Sintseva
Thomas John Taylor
Michael Lam
Building on the success of the first edition - the Global Art Agency are busy organising the second Tokyo International Art Fair for 13 & 14 May 2016 at an amazing new venue "Omotesando Hills" which is located in Aoyama, sometimes termed "Tokyo's Champs-Élysées".
More than 150 exhibitors from over 30 countries will be filling the Space-O hall at the Omotesando Hills venue with an incredible display of contemporary art and thousands of artworks for sale.
Organisers Joëlle Dinnage and her business partner Natal Vallvé from the Global Art Agency are making the fantastic (free) two-day art extravaganza a versatile art happening for the locals of Tokyo. A huge variety of artworks, offering every visitor something to suit their style, all in an affordable price-range to buy and to take home on the day.
Satoshi Maruhashi who is part of the organisation says: "I am extremely happy with the new venue, it will be another spectacle."
On show will be paintings, sculptures, photography art, illustrations, printmaking, and jewellery, with a live painting and music show at the event.
"Almost 6000 people visited the event last year, connections were made, and great sales happened, so everyone was extremely satisfied. There was no doubt to organise a second edition, and we have worked very hard to get a brilliant new venue in one of Tokyo's hotspots attracting art aficionado's from all over the world." said organiser Joëlle Dinnage.
"We have new talent exhibiting this year as well as some known names that exhibited last year, and of course there are the famous names such as Mr Brainwash who will showing, as well as Shane Bowden - also known as the Andy Warhol on steroids - who did very well last year."
Laura Jordan (UK), Canal Cheong-Jagerroos (Finland), Svetlana Sintseva (Belgium), Hayat Saidi (Morocco), Hiba Sultan (Saudi Arabia), Sophia Shiyan (Russia), Li Wei Chen (Taiwan), Kaze Gallery (Japan), STYLO (Thailand), Mark James Ford (Germany), Loryn Kolbrenner (USA), Suzi Fadel Nassif (UAE), Thomas John Taylor (USA), Franco The Creator (USA), Shane Bowden (Australia), Mr Brainwash (France), New York Art Gallery (Japan), Krystal Glam Art Gallery (Japan), and many more... Also Michael Lam (NYC) who creates single stroke paintings based on his calligraphy skill. Lam has received awards and recognition for his work all over the world and worked to support UNICEF for children.
The fair opens on Friday 13th May with a private view and vernissage for invitees only starting at 18.00pm to 21.00pm (limited tickets are also available to purchase online).
On Saturday 14th May the art fair is open to the public from 11.00am to 19.00pm with the Global Art Awards happening at 18.00pm that day announcing the best Artist of the fair. Prebook tickets here.
Tickets to the Tokyo International Art Fair 2016 are free and can be booked online by going to their website www.tokyoartfair.com The event takes place from Friday 13th May to Saturday 14th May 2016 at OMOTESANDO HILLS - MAIN BUILDING B3F SPACE O, 4-12-10 Jingumae, Shibuya-ku, Tokyo 150-0001 JAPAN.
For more information about the event and to visit please visit www.tokyoartfair.com
Participating as an Exhibitor:
The Tokyo International Art Fair are now in the final stage of curating and selection process. They are inviting the outstanding artists to apply online www.tokyoartfair.com
Tagged: Tokyo International Art Fair, Tokyo International Art Fair 2016, Tokyo Art Fair 2016, Art in Tokyo 2016, Omotesando Hills, Tokyo, Global Art Agency, Thomas John Taylor, Svetlana Sintseva, Suzi Fadel Nassif, Sophia Shiyan, Mark James Ford, Loryn Kolbrenner, Li Wei Chen, Kaze Gallery, Mr Brainwash, New York Art Gallery, Hayat Saidi, Franco the Creator, Canal Cheong Lagerroos, Beast, Hiba Sultan, STYLO


Gotta Have Munchies for a card party this weekend. This is just the Trick.
Make Sure You make Lots, your Guests will want more.
Easy to wrap the mini Dogs or Sausages, with Bacon, then Place in Crock Pot, and wait til serving time, if you can wait that long. . . serve Hot.
pkgs mini party sausages, or hot dogs, or polish sausages cut into 1" bites.
bacon, each piece cut in 1/2 or 1/3rd if long thick pieces. tip: cut while partially frozen it cust easier.
Wrap each Mini Weenie Sausages, in the strips of bacon.
Place all in a slow Cooker.
Pour all the Bags of Brown Sugar over top of the Mini Weenies.
low about 4-5 hrs or til all the Sugar Melts, and is well disolved.. . .
Great for Card parties or Holiday Gatherings.