Join us for a tour of Star of the West - Richville Agronomy facility on Monday, June 4 at 3:30pm. Learn about what it takes to put together a fertilizer prescription for a crop using GPS soil testing and help a farm with a variable rate application. Network with Ag Industry, Conservation District and Partner Staff. This tour is limited to the first 56 that sign up, so register today.
New this year, we will have mini breakouts in a wide variety of topics. Attendees will move around the sessions to the topic of their choice.


The exciting images below, is section of Choice of Bedroom Ceiling Lighting write-up which is labeled within Bedroom Lighting, home lighting ideas, and posted at October 2nd, 2015 08:53:32 AM by .
Here is necessary notification on home lighting ideas. We have the best assets for home lighting ideas. Check it out for yourself! You can get Modern Bedroom Ceiling Lighting guide and look the latest Choice of Bedroom Ceiling Lighting in here.


In a previous post, we introduced a way to predict and abandon builds at the post-placement stage, skipping time- and resource-consuming routing stages that were not likely to yield good timing results. InTime users welcomed this approach, especially those who were designing with large FPGAs. We are thrilled to add this capability for our Quartus Prime Pro customers as well.
Quartus Prime Pro Edition allows users to extract intermediate timing estimates. Intuitively, these estimates become more accurate as the compilation progresses from synthesis to fitting.
To observe how timing estimates change across compilation stages, we use a Stratix 10 GX 2800 project as an example.
Designers familiar with Stratix 10 will recognize this device as a mid-sized one within the GX line. The design itself fails timing by -1.9ns Worst Setup.
We used InTime to optimize it on a 12-CPU, 128GB RAM machine, incurring compilation times of around 5 hours per build.
The following chart shows the timing estimates for over 80 revisions of this project. Each revision consists of different synthesis and fitter parameters generated by InTime.
At each point where Quartus reports timing estimates, InTime captures the data and collates it.
The X-axis shows the revisions (not all revision names are shown for brevity) and the Y-axis displays the Worst Setup.
This provides a degree of confidence that we can predict the final timing using post-placement estimates.
Timing estimates mostly improved as the compilation progressed, except for a couple of revisions.
Correspondingly, you can choose to stop a build if it fails a certain Worst Setup slack (WS) or Total Negative Slack (TNS) threshold – cutting at least 50% off your overall turnaround time! That means running twice as many compilations, explore double the scope of setting optimizations and becoming 2x more effective than before.
If you are running multiple builds in InTime to get the best settings, the post-placement timing estimate is a great indicator to stop builds early and re-allocate precious resources to other builds. The latest version of InTime enables the "Stop If Post-Place Timing is Bad" switch for Quartus Prime Pro designs. You can specify TNS, WS and Worst Hold in nanoseconds and InTime will stop the build if its post-placement timing estimate is worse than any of these values.
Note that Worst Hold thresholds usually need to be much greater than the expected final value because Hold timing will not have been optimized during placement.
You can create simple scripts to collate post-placement timing estimates and obtain a good idea of what the cutoff values for your design should be. This new feature is released in InTime version 2.6.5. Feel free to reach out to us to discuss how to get the most mileage out of it.
By tracking timing estimates to predict how each revision will perform, we can make decisions on whether to stop the build or let it continue. This saves time, money and achieves our 3-7 days commitment for turnaround time (See InTime Service). Using this method, InTime has closed up to -3ns of WS for Stratix 10 designs.
*Catch us at the Intel FPGA Technology Day 2018 to find out more.


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Purple Heart Wines Presents $10,000 Donation to Purple Heart Foundation
Cause-based Napa Wine Brand Continues Tradition of Giving
Purple Heart Wines presents $10,000 donation to the Purple Heart Foundation
Napa, CA (PRWEB) June 14, 2017
Purple Heart Wines (https://www.purpleheartwines.com/), a collaboration between C. Mondavi & Family and the Purple Heart Foundation, an organization which supports veterans in need, is delighted to share the 2017 Check Presentation Celebration to the Purple Heart Foundation (http://purpleheartfoundation.org/), which took place on June 8, 2017. Since the launch of the project in March 2016, Purple Heart Wines has donated $40,000 to the Purple Heart Foundation, which has been used to support U.S. military servicemen and women and their families with services like job-training, counseling and more.
Proprietor Peter Mondavi Jr. and Janice Mondavi came to champion the cause and carry on C. Mondavi & Family's history of supporting veterans and the Purple Heart Wines project. Purple Heart Wines winemaker—and Air Force veteran—John Moynier joined Bill Hutton, Senior Vice President of the Purple Heart Foundation, to present the $10,000 check, the latest installment in a series of donations.
Moynier's opportunity to work at Purple Heart Wines is a priceless next step for the military veteran and California native who has over 40 years of experience as a winemaker: "Working with a brand that combines my passions for winemaking and military service is the perfect finale to a long career in winemaking in Napa."
About Purple Heart Wines:
Purple Heart Wines launched its proprietary label, Purple Heart, in 2016 – created to honor the determination, bravery and commitment of America's military heroes. Moved by its namesake, it is this noble medal that lead to the creation of the Purple Heart wine – a worthy tribute to the nation's servicemen and women. It is produced in the United States' greatest wine region – California. It is an uncompromising wine crafted under the close stewardship of C. Mondavi & Family, whose patriarch, Peter Mondavi Sr., was a proud veteran of World War II. Purple Heart serves as a testament to the integrity and virtue of the Purple Heart Foundation, and aims to help further the organization's cause through both awareness and fundraising. To support these efforts, annual donations will be made to the Purple Heart Foundation. Learn more about Purple Heart Wines at purpleheartwines.com.
Purple Heart Foundation and the Military Order of the Purple Heart:
The Purple Heart is a congressional military decoration, awarded to members of the armed forces of the U.S. who are wounded by an instrument of war in the hands of the enemy. Founded in 1958, the Military Order of the Purple Heart is a congressionally chartered veteran's organization, dedicated to assisting the needs of U.S. military servicemen and –women and their families. More information is available at purpleheartfoundation.org.
Frida Reddy
Colangelo & Partners
@ColangeloPR
since: 08/2012

redpajama_set_name: RedPajamaCommonCrawl


text:
Gordon Ramsay's 'Next Level Chef' Gets Post-NFC Championship Spot After 'Monarch' Delay
Meredith Jacobs, TV Insider
After new country music drama Monarch was pushed to the fall 2022, Fox has found the show to air in the post-NFC Championship Game spot on Sunday, January 30: Next Level Chef.
Gordon Ramsay's culinary competition series will air at 10/9c following the football, with an episode that sees Ramsay and his fellow mentors, Nyesha Arrington and Richard Blais, serving up a Sunday Brunch challenge.
Each remaining chef will have to create a next-level dish that incorporates both sweet and savory elements in just 45 minutes. Who will rise to the challenge? Who will go home? After the special episode, Next Level Chef will continue to air on Wednesdays at 9/8c.
'Next Level Chef': Meet the Chefs Behind Gordon Ramsay's New Show (PHOTOS)
The Fox series arrives in early 2022.
That time slot was supposed to serve as the series premiere for Monarch, with the new series starring Susan Sarandon, Trace Adkins, and Anna Friel then making its time slot debut on Tuesday, February 1, at 9/8c, after The Resident winter premiere. However, on January 12, Fox announced it was delaying its premiere until the fall.
"Monarch, is a top priority for FOX Entertainment in 2022. Unfortunately, due to the unavoidable realities of the pandemic and the profound impact Covid-19 continues to have on our industry and around the world, it is necessary to reschedule Monarch's January 30 debut to the Fall," a FOX Entertainment spokesperson said in a statement.
"As the cornerstone of FOX's new 2022-23 slate, shifting a show of this magnitude allows us to have its entire first season produced, create additional, high-profile content and promotional windows to support launch, and give our viewers the best opportunity to enjoy the series as intended with a non-compromised run of episodes.."
There's no word yet on what will replace Monarch, which follows the first family of country music, on Tuesdays at 9/8c.
Next Level Chef, Wednesdays, 9/8c, Fox
This article originally ran on tvinsider.com.
Fox Sets 'The Real Dirty Dancing' With Tyler Cameron, Brie Bella & More
Andrew Garfield: Lying about Spider-Man comeback was right
Renewed TV Shows 2022: Find Out Which Series Will Return for Another Season
Mainly cloudy. Lows overnight in the mid 20s.
Partly cloudy skies early will give way to cloudy skies late. Low around 25F. Winds light and variable.
Snow showers early. Highs in the upper 30s and lows in the low 20s.
Partly to mostly cloudy. Low near 20F. Winds light and variable.
Clear. Low 19F. Winds light and variable.
Mostly sunny. Highs in the upper 30s and lows in the low 20s.
Partly cloudy. Low near 20F. Winds light and variable.
Mix of sun and clouds. Highs in the upper 30s and lows in the mid teens.


text:
Q: Fixed bottom div stop once it reaches another div Fixed bottom div stop once it reaches another div
For ref- https://www.marketo.com/

#one{
 width:100%;
    background-color: aqua;
 position: fixed;
 bottom: 0px;
 padding: 30px 0;
 text-align: center;
}

#two{
 width: 100%;
    padding: 30px 0;
 text-align: center;
    background-color: red;
}

Main Flagasd

div 2

A: I'd use scrollToFixed jQuery plugin.  It will simplify your code drastically as well as produced the desired effect.  I drew up an example on how you can use it.

$(document).ready(function() {
    $('#one').scrollToFixed( {
        bottom: 0,
        limit: $('#two').offset().top,
    });
});
#one{
  background-color: aqua;
 padding: 30px 0;
 text-align: center;
}

#two{
 width: 100%;
  padding: 30px 0;
 text-align: center;
  background-color: red;
}

Main Flagasd

div 2

A: You can do something like this.
I am assuming that the fixed div will change its position when it reaches the red div.

var fixedDiv = document.querySelector('#one');
var redDiv = document.querySelector('#two');

redDiv.addEventListener('mouseover', function() {

  fixedDiv.style.position = 'static';

});
#one {
  width: 100%;
  background-color: aqua;
  position: fixed;
  bottom: 0px;
  padding: 30px 0;
  text-align: center;
}

#two {
  width: 100%;
  padding: 30px 0;
  text-align: center;
  background-color: red;
}

Main Flagasd

div 2

A: You can use this plugin called ScrollToFixed
as
$('.footer').scrollToFixed( {
        bottom: 0,
        limit: $('.footer').offset().top,

    });

working fiddle http://jsfiddle.net/ZczEt/2953/

redpajama_set_name: RedPajamaStackExchange


JUST ARRIVED - LOCAL TRUCK!*****2016 NISSAN TITAN SL 4WD WITH 5.0L CUMMINS TURBO DIESEL ENGINE!****CLEAN 1-OWNER CARFAX****This is a great heavy duty truck that combines powerful performance and luxury comfort. It is built to tow with integrated gooseneck hitch, class IV tow hitch, 4-in and 7-pin wiring harness connectors, tow/haul mode and trailer brake controller. Comes equipped with heated front bucket seats, Blind Spot monitoring system, Husky all-weather floor mats, touchscreen infotainment center with Navigation, rear view camera and AM/FM/CD/XM/Bluetooth radio with Rockford-Fosgate Premium Sound System, traction control, dual-zone climate control, power equipment including 2-position driver memory seat, cruise control, rear parking sensor, fixed running boards, bed liner and tonneau cover. Has a new PA inspection, fresh oil change, and tires and brakes are in great condition. Comes with the balance of the factory warranty with options to extend coverage for added piece of mind. Trades are welcome and financing is available.


text:
Andy Jones collection
Darka Erdelji collection
Dave Paddon collection
Lori Doody collection
Tom Dawe collection
Veselina Tomova collection
Lori Doody
Lori Doody was born in St. John's, Newfoundland in 1976. She majored in printmaking at Sir Wilfred Grenfell College, in Corner Brook, and graduated in 1998. Since then she has worked at: a Japanese paper store, the artist-run centre St. Michael's Printshop, and a commercial gallery. Her primary art practise has been in printmaking, especially etching, and in 2005 she was named Emerging Artist of the year by the Newfoundland and Labrador Arts Council.
She provided the illustration for "Turk's Gut Wolf," Running the Goat's second poemphlet. To date, she has published five children's books with Running the Goat — Capelin Weather; The Puffin Problem; Mallard, Mallard, Moose; Paint the Town Pink; and Mr. Beagle Goes to Rabbittown. All of them have been warmly and widely praised for their playful wit, bright and quirky illustrations, and gentle sense of kindness and community.
In 2021, Lori will have three new books: two published by Running the Goat, and one by Nimbus Publishing.
Lori currently lives in St. John's with her husband and their two children.
loridoody.com
50 Cove Road
Tors Cove, NL
A0A 4A0
© 2021 Running the Goat Books and Broadsides


We don't know if we're happier about Blue Tokai making it to another spot or about the fact that it has collaborated with our favourite spaces in Assagao, The Project Cafe. While we're still rejoicing, we can tell you that this new coffee room was launched this Sunday, generously offering people a cuppa with a side order of art and conversations. We can literally smell that oatmeal cookie and Americano.
Few can deny the restorative power of a well-made cup of java and if you've stayed long enough in Goa, you probably know what a rarity it is. This is exactly why, we intend on making a trip to Assagao soon. After all, we'd love to get some reading done by the pool, with the cold brew for company. And sigh… just the thought of sitting in their tropical garden and getting ourselves their a plate of their spaghetti, is pretty tempting, tbh.
As an extension of the collaboration, we hear that the Blue Tokai cafe in Panjim will also serve Project Cafe food. How's an Affogato shot for cheers?
P.S. Blue Tokai coffee room at The Project Cafe will be open through the week (9am-7pm).


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text:
/Philosophy
/A Critique of Natural Law
A Critique of Natural Law
Essay by review • November 11, 2010 • Research Paper • 2,532 Words (11 Pages) • 2,547 Views
Essay Preview: A Critique of Natural Law
Essay #2
Barbara Palombo
256 Pinevalley Crescent
Woodbridge, Ontario
L4L 2W5
Email: palombo5152@rogers.com
Student #: 923621220
Phil 1002 6.0 Q
Class ID: 1227265
Team Instructor: Carol Bigwood
Natural Law is a concept that has caused ambiguity throughout the history of Western thought. There is a multitude of incompatible ideas of natural law that have caused even those who are in basic agreement on natural law theory to have opposing notions on the particulars. In spite of this confusion, there have been enough advocates among natural law thinking in Western society to make it possible to identify its major criticisms:
1. Natural law is immutable and is rooted in nature. This defines for man what is right, just, and good, and which ought to govern its actions. (Einwechter, 1999, p.1)
2. The universe is governed by reason, or rational principle which provides a basis for determining justice of man made laws. (Einwechter, p.1)
3. Natural law is the same for all human beings and at all times.
(Cragg, unit 13, part 2)
In this paper, I will summarize the philosophical and historical roots of natural law theory as they relate to the three major criticisms, and challenge these major criticisms using theories such as utilitarianism and legal positivism. Plato and Aristotle proved to be of great importance in natural-law thinking from 5th century Greece until the present day. Plato had an idealist view of justice as a kind of absolute which can be understood only by the philosopher and fully realized in an ideal state. Aristotle regarded natural justice as universal, yet ideal. Stoic philosophy, which evolved after Aristotle, plays a great role in the history of natural law. Its emphasis was on reason as the key element of humanity. (Course Kit, 2005, p.77) Subsequently, Stoicism became associated with the spread of Roman power over the Mediterranean world, and the Roman legal conception, ius gentium Ð'- the common law that was administered to those countries restricted to the Roman world. Although the Romans adopted an abstract conception of a universal law, they applied little or none of the essential features of natural law. (Lloyd, p.79) However, the writings of Roman oracle, Cicero perpetuated the evolution of early natural law speculation to later ages. He claimed that natural law governs the entire universe by divine reason. Thus, it is eternal, and is not established by people, but by reason. In concurrence with Stoic natural law and ius gentium, Christian theology had a superior impact than that of the older Stoic natural law. The Catholic Church and its representatives had the authority to expound and comprehend and enforce the law of God. St. Thomas Aquinas, a proponent of Catholic philosophy, asserted that natural law is common to all people Ð'- Christians and non-Christians and is eternal. Hugo Grotius, a 17th century jurist, claimed that man's reason and rationality, which was rooted in human nature and based on divine law, governed all human affairs. (course kit, pgs.78-81)
By the middle of the 19th century, modern natural law tradition was attacked by criticisms of Bentham with his principles of utilitarianism and John Austin's influence of legal positivism. The principle of utility augmented the greatest happiness of the greatest number of people, and legal positivism identified the existence of legal systems and defines what is legal in a particular society, not what is lawful among human beings. (Stanford Encyclopedia of Philosophy, 2003, p.1)
Marcus Tullius Cicero's (106-43 B.C.), a Roman orator and stoic philosopher, description of natural law derives from the ideas of Greek philosophers and the views of many non-Christian and Christian natural law theorists. He asserted that natural law is in accordance with nature, applies to all men and is unchangeable and eternal. Thus, he described law as the "highest reason, implanted in nature, which commands what ought to be done, and forbids the opposite. (Cicero, 1928, p. 45) While Stoicism maintained that the world itself is rational and divine. "There is in fact a true law Ð'- namely, right reason Ð'- which is in accordance with nature, applies to all men, and is unchangeable and eternal." (Cicero) Cicero successfully argued before a Roman court that a particular Roman law was unjust, because it conflicted with natural law.
Thomas Aquinas (1225-1274), the medieval Catholic Scholar, sought to reconcile the Greek concept of natural law with Christian theology. Aquinas began by speculating that God governs the universe and that humans are equipped with divine reason and by it derives the natural inclination to proper acts and ends. (Einwechter, 1999, p.2) Aquinas believed that revelation through scripture which came through mediation of the church, was suitable for church/religious matters, while with natural revelation man is predisposed to rely on his reason which becomes the true source of law. If one introduces Scripture, then he is appealing to a source outside of himself, and is giving up natural law and reason. According to the Scripture, God reveals himself to man through natural revelation, which includes the knowledge of God's existence and power, and man's responsibility to worship God and live according to His moral law. (Ps.19: 1-6) Thus, it condemns man if they fail to worship God (Rom. 1:18, 20, 25) His preservation of the essence of naturalistic reasoning, contained in Aristotle's works, lead to the revitalization of reason over dogma which contributed greatly to the achievement of scientific inquiry generated in the subsequent Renaissance and Enlightenment eras. (Merriman, 2000, p.6)
The curse of sin that has been bestowed on us has made it impossible for natural law to be the paradigm for the moral law. Because of sin, man's reason and conscience have been harmed, therefore, man's knowledge of right and wrong, justice and injustice is tainted. (Einwechter, p. 6) As a result of the fallen man, God administered His ten commandments in addition to reason and conscience to obey His will.
The 17th century Dutch jurist Hugo Grotius believed that humans by nature are not only reasonable but social. Although his thinking adhered to the doctrines of St. Thomas
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A Critique of Martin Luther King, Jr.'s Version of Natural Law Theory
This paper is about the world, but I've never written it. ------------------------------------------------------------------------ Editing Resources Other Resources Hosted by pair Networks ------------------------------------------------------------------------ ------------------------------------------------------------------------ A Critique of
Natural Law Vs Human Law
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Assessing Data World Law Enforcement


I've had some ideas on stuff, but didn't know how to express it, but now I do. This is also in the suggestions thread, so meh... So this game just offers the kebab as the main food source and fire making only providing a fire place, I'm not sure what the second scheme is or how to get it. We also get a generous amount of metal and different metal types to acquire and choose from, but can take up space and weight you down or jumble what you're looking for. I've come up with some ideas on what to do with some of this stuff.
Obviously. Just kebabs as the primary food outcome is quite boring, but the cooking method with diifferent seasonings and secondary foods are very nice. Offers and teaches you what does and what doesn't go where. However, I feel like there should be more ways to cook. I've seen a smokehouse, and that looks the closest to a stove, I feel like that should be used to cook stuff. Maybe you can scavenge a pot from the scrap yards and use that as the cooking tool, then add water from a bucket or waterskin, and add your meats, sides, and seasoning to create a soup that, if temperature control ever becomes a thing, can keep you warm, full, AND is delicous (Hopefully). There could also be a grill you can put on top of a campfire, or find parts and create a BBQ Grill yourself and create grilled meats and foods. They could also provide different buffs or some crap (Somehow), like kebabs can do what they do, the soup can be consumed faster or slower but nourishes you less but hydrates you some for a little convenience for travel. Grilled foods can be consumed slower because they're not on a kebab but can fill you up a little more than a kebab or soup can, depending on the quality of the foods cooked on each or how Xsyon Dev Boi makes it, if he decides it.
Xsyon's Scrap Fields feed us with a huge variety of different metals, as said before, like you can have a basket backpack, scavenge and sort 8 metal scrap collections and already have a full inventory. My idea is that you can build a structure, or single object, like a furnace, that can melt down your metals and create ingots, so that you don't have to keep taking up tribe space with your baskets full of metal. The ingots could be big or small, and take a volume a space when you remelt it. But what would you do with the ingots? First, you can go down to a river with dirt, not stone, so instead of collecting Limestone, you can collect Clay, and use this clay to create casts from your dug up objects, such as say, a short metal handle. Then you can remelt the ingot, or melt new items to fill the cast and create a brand new small metal handle! Or course, you're going to need to get the metal really hot, and need a crucible that can hold such liquid. Therefor, a new use for the fire building skill, you can create an object that will create charcoal out of branches, sticks, and split wood. The crucible could be made out of graphite and clay, and the graphite could be a rare object, like tar or quartz.
The grass baskets can sure hold a lot of stuff, but isn't that pleasing to the eye to see on your back. The grass pack looks nice, but doesn't hold as much as a basket. Plus I find it a little annoying that grass pouches are the only thing that can be crafted as pouches. So I say that there should be some leathercraft recipes that can create some backpacks, and the higher level leathercraft you are, the better backpacks you can make, maybe even a pack that can hold the same as the grass basket. Plus it'll look better! There should also be different kinds of looks to backpacks, like different options you can make, like how you can make different kinds of clothes and armor, or with the different kinds of carts. There should also be different craftable leather pouches, the same way there are different kinds of grass pouches. They could possibly hold more, because they're a stronger material than grass. Maybe they can be unlocked at level 60 or something.
This is a fantasy setting, right? We have lots of herbs and seasonings for cooking, yes. But I demand more! Why? We could create a new craft, Potion Brewing. We even have an herb named Self Heal for crying out loud. First, you'd need to level up your architecture skill, so you can build a brewing stand! Maybe we can find in the scrap yards old broken beer glass bottles or whole beer glass bottles and beakers and other glass objects. Then use them to build up a potion brewing stand for some potions! And what would potion brewing be without more herbs for such a craft! It could start like cooking, 1 herb and instead of a skewer, you could use a whole beer glass or glass container to hold the finished product, and possibly a filled water bucket or filled water skin to add water to the potion for creation. As you get better, you can add more herbs and start experimenting with the potion making process to create strong potions, and try to clear the negative buffs with the rare herbs, as with cooking. Maybe when/if bows/archery/thrown combat is added, or even now with armed combat, you can tip your weapon/arrow with a poison or a potion that adds really bad negative buffs, and when struck, will apply it to the enemy (Yes, like in Skyrim), but to perhaps balance it out, it can do possibly half of what it would do if you were to drink it, as it's being inserted into you, not ingested.
These are some of my ideas, I hope they are good, and I'll add to this page when I think of more. Anyone have any thoughts?
I see that you also posted these suggestion on the Suggestions forums. Please do post one suggestion per post there as it makes it easier for me to track, see feedback from other players and implement the suggestion.
Thank you. No clue how this forum worked, but I think (Hopefully) I'm getting the hang of it.


text:
Shows, Cartoon Network Toonami Shows, Midnight Run Shows, Former Toonami Shows
Gundam 0080
Cartoon Network (Midnight Run)
6 (List of Episodes)
Mobile Suit Gundam 0080: War in the Pocket, often shortened to Gundam 0080, is a 1989 Japanese science fiction original video animation series, the first such series in the Gundam franchise. Directed by Fumihiko Takayama and produced by Sunrise, it was also the first time anyone other than creator Yoshiyuki Tomino was given a chance to direct a Gundam story. Released in 1989, it serves to commemorate Gundam's ten-year anniversary. As suggested by its subtitle, "War in the Pocket," it is a small, personal story; a side story focusing on the experiences of a ten-year-old boy during the One Year War.
Gundam 0080 also began an enduring tradition of retroactive redesigns. Yutaka Izubuchi updated the original Mobile Suit Gundam's dated mechanical designs and costumes, and since then every new creative team has offered its own take on the classic Gundam props.
Not penned by Tomino, but by Hiroyuki Yamaga, Gundam 0080 also marked a significant departure from the constant background theme of Newtypes featured in the Universal Century Gundam universe, from the original Mobile Suit Gundam up until Char's Counterattack. The absence of this theme raised the series' appeal towards audiences without special liking of Gundam and Tomino's work and would continue in many following Gundam stories narrating ordinary soldiers and people in these conflicts.
Gundam 0080 premeired on Toonami's Midnight Run block on November 5, 2001.[1] The series aired as a Midnight Run exclusive, never airing on the day-time Toonami block, due to the content (buildings being destroyed, planes crashing, etc.) being similar to the recent 9/11 attacks. The series also briefly aired on Adult Swim in 2002.
December, Universal Century 0079, Zeon intelligence has identified a prototype Federation Gundam under development in a Federation base in the Arctic. Elite Zeon MS commandos are dispatched to destroy the prototype, but before they can accomplish their mission the Gundam is launched into space. When the Gundam turns up in a Federation R&D base inside the neutral space colony Side 6, the Principality launches a covert operation to destroy the Gundam that includes young rookie Bernard Wiseman. However, the raid fails and the entire team is killed except for Bernard. After crashing his mobile suit, Bernard manages to befriend Alfred Izuhura and Christina Mackenzie, the Gundam test pilot. As Bernard tries to repair his damaged mobile suit, Bernard slowly becomes infatuated with Christina, with both pilots remaining unaware of each other's true natures. However, Bernard discovers that Zeon will destroy Side 6 with a nuclear weapon if he cannot destroy the prototype Gundam. Feeling that he has no choice, Bernard takes his mobile suit and goes to engage the Gundam. Alfred then discovers that the Zeon ship carrying the nuclear weapons was captured, meaning Bernard has no more reason to fight. He goes to try and stop Bernard, only to see Bernard's mobile suit destroyed and an injured Christina pulled from the heavily damaged Gundam. Afterwards, Christina tells Alfred that she will be leaving Side 6, and asks Alfred to say goodbye to Bernard for her, still unaware that she had actually killed him. Alfred does not have the heart to tell her the truth and agrees to her request.
Alfred "Al" Izuruha — Al is an 11-year-old schoolboy, who has a distant relationship with his father who works for the Earth Federation. He gets mediocre grades in school and misbehaves in front of his mother and teachers. As a naive young boy who lives in the Libot colony of neutral "Side 6", Al is fascinated by tales of mobile suit combats, but has little real idea about the war outside of the fact that it is ravaging the Earth Sphere. He has a special interest in Zeon's Zaku mobile suits, which he regards as "cool". One day, Al meets a rookie Zeon pilot, Bernie Wiseman, whose Zaku is disabled and crashes after a short battle with Federation forces in the colony.
Bernard "Bernie" Wiseman — Petty Officer 2nd Class Bernard Wiseman is a rookie soldier for the Principality of Zeon who befriends Al after his Zaku is shot down within Libot. He is later reassigned to the elite Cyclops Team as they embark on a top secret mission to destroy the Gundam.
Christina "Chris" MacKenzie — Al's friend and neighbor who has just returned from Earth on a top secret mission for the Earth Federation. She is the test pilot for the Federation's newly developed Gundam.
Al Izuruha
Bernie Wiseman
Chris MacKenzie
RX-78NT-1 Gundam "Alex"
MS-06FZ Zaku II Kai
Alfred "Al" Izuruha Brianne Brozey Daisuke Namikawa
Christina "Chris" Mackenzie Wendee Lee Megumi Hayashibara
Bernard "Bernie" Wiseman Sean Barker Kōji Tsujitani
Charlie Alfred Thor Inaba Minoru
Gabriel Ramirez Garcia Eduardo T. Torres Bin Shimada
Mikhail "Misha" Kaminsky George C. Cole Yutaka Shimaka
Steiner Hardy Gil Starberry Yōsuke Akimoto
Lt. Colonel Killing Jackson Daniels Takumi Yamazaki
Dorothy Melissa Charles Konami Yoshida
Chay Mona Marshall Tomoko Maruo
Mrs. MacKenzie Catherine Luciani Mari Nakamura
Mr. MacKenzie Dougary Grant Yasuo Muramatsu
Ems Izuruha David Lucas Jun Hazumi
Michiko Izuruha Mona Marshall Ai Orikasa
Stuart David Lucas Ken Goto
Telcott Mona Marshall Ken Suzuki
Von Helsing George C. Cole Masato Hirano
Richard Lunland John Billingslea Hiroshi Masuoka
Andy Strauss Matthew K. Miller Mitsuaki Hoshino
Commander Rugens Simon Isaacson —
Toonami - Gundam 0080 Long Promo (1080p HD)
60 Second Midnight Run Promo
Toonami - Gundam 0080 Promo (1080p HD)-0
Toonami - Gundam 0080 Intro (1080p HD)
Midnight Run Intro
U.S. Season Premiere
U.S. Season Finale
1 06 November 5, 2001 November 12, 2001
Gundam 0080 is the first original video animation (OVA) series in the Gundam franchise. Being an OVA series, the 6 episodes were released over the course of several months in Japan, with one episode being released each month, beginning on March 25, 1989 and ending on August 25, 1989. The entire series has been released in the United States by Bandai, but is no longer in production. In October 2016, Right Stuf Inc., announced that the series will be released on DVD on January 3, 2017.[2]
Gundam 0080 premiered on Cartoon Network from November 5, 2001 to November 30, 2001 as part of Toonami's Midnight Run block. It then briefly aired on Cartoon Network's late night Adult Swim block from November 16, 2002[3] to December 21, 2002. It also made an appearance on Cartoon Network's Saturday Video Entertainment System block from March 1, 2003 to April 19, 2003.
United States (Cartoon Network) — November 5-30, 2001; November 16, 2002[3] - December 21, 2002[4]; March 1, 2003 - April 19, 2003
Gundam 0080 aired on Toonami's Midnight Run block from November 5, 2001 to November 30, 2001. The series aired as a Midnight Run exclusive, never airing on the day-time Toonami block, due to the content (buildings being destroyed, planes crashing, etc.) being similar to the recent 9/11 attacks.
Toonami: Midnight Run — November 5-30, 2001[1]
Gundam Wiki
↑ 1.0 1.1 "Gundam 0080 on Midnight Run ". animenewsnetwork.com. November 1, 2001. https://www.animenewsnetwork.com/news/2001-11-01/gundam-0080-on-midnight-run. Retrieved on December 31, 2016.
↑ "Mobile Suit Gundam 0080 War in the Pocket Coming January 2017 from Right Stuf, Inc. and Sunrise Inc. ". animenewsnetwork.com. October 6, 2016. https://www.animenewsnetwork.com/press-release/2016-10-06/mobile-suit-gundam-0080-war-in-the-pocket-coming-january-2017-from-right-stuf-inc-and-sunrise-inc/.107347. Retrieved on December 31, 2016.
↑ 3.0 3.1 "Gundam 0080 ". adultswim.com. November 15, 2002. https://web.archive.org/web/20021115134350/http://www.adultswim.com/shows/gundam_0080/index.html. Retrieved on December 31, 2016.
↑ "Saturday Night Schedule ". adultswim.com. December 1, 2002. https://web.archive.org/web/20021201115824/http://www.adultswim.com/schedule/action/index.html. Retrieved on December 31, 2016.
Retrieved from "https://toonami.fandom.com/wiki/Gundam_0080?oldid=42190"
Cartoon Network Toonami Shows
Midnight Run Shows


This course originated in a desire to teach creatives how to be prolific and productive, but when instructor/writer/filmmaker Jen Lee investigated the source of her productivity she found it all came from the way she's learned to take good care of herself as a maker and creative.
When we don't take care, our work and relationships become a pale version of what they could be and are waiting to become when we turn this one piece around. A more inspired, prolific and joyful lie awaits--say yes to this journey, start where you are.
This is the moment. This is the guide.


VMworld 2018 has a great lineup of Edge and IoT sessions with experts from VMware, Dell, Siza, Axis Communications and more! Sessions will be taking place all week and will also be available on-demand after VMworld. Check out our VMworld Europe 2018 post to get a full overview of everything Edge and IoT at VMworld.
According to Gartner, through 2018, 75 percent of IoT projects will take up to twice as long as planned. The reasons for this are many but the most significant one is the dilemma of managing IoT in the enterprise context. With the advent of IoT, traditionally OT assets which now enjoy internet connectivity are slowly falling under the purview of IT for management. As these worlds collide and roles blur, it is becoming harder to implement IoT as architecture, standards and security protocols differ for IT and OT. Learn why this convergence is important and best practices from customer examples on how best to align these departments to fuel your IoT success.
Earlier this year, we launched VMware Pulse IoT Center, an IoT infrastructure management and monitoring solution that helps OT and IT have complete control of their IoT use cases from the edge all the way to the cloud. Attend this session to hear our customers from healthcare, transportation and banking reveal why VMware Pulse IoT Center has been integral to their IoT infrastructure transformation and also get a sneak peak at some of our upcoming features and roadmap and the Pulse IOT Center Cloud Solution.
Gartner predicts 75% of data will be generated at the edge by 2021 because of things generating valuable data that will be leveraged to optimize your business. Is your company ready for this shift? As most organizations are focused on shifting to the cloud, are you considering the compute capacity that will be needed in the field, at the edges of your business where the data is being collected? Real-time needs, storage costs, and security are driving the need to have a more distributed architecture vs. cloud or data center only. Be the first to learn VMware's edge computing strategy and how you can leverage your existing investment while leveraging VMware's leading software defined data center, VMC, VeloCloud and Pulse IoT Center capabilities to help you have one infrastructure strategy from cloud to edge.
Gartner says that by 2020, annual enterprise security costs will have increased by 20x since 2015 because of IoT. Security cannot be an afterthought, but must be considered at each level of the value chain. In this session, you will learn how VMware Pulse IoT integrated with VMware NSX network virtualization and security capabilities helps protect business-critical deployments by providing security at the thing, network, and user level.
Come and learn about how VMware can accelerate your adoption of Edge Computing by dealing with the additional complexity and cost of infrastructure management at the Edge, helping you quickly achieve the cost savings and revenue growth benefits of Edge Computing. This is also a great opportunity to shape the direction of VMware's edge services to help fit customer needs.
Surveillance is heading to the data center; are you ready? Right now, there are more than 300 million cameras globally, and the number is growing. The global security landscape is changing rapidly, too. There is a pressing need for IT organizations to help transform their surveillance security environments to handle the rapid growth in high-definition sensors, retention times, and new demands for artificial intelligence and machine learning in surveillance. In this session, you will hear more about integration between VMware and Dell ecosystem solutions with a focus on Axis Communications' physical security and IoT solutions.
In any industry, delivering on the promise of digital transformation requires that disparate IoT hardware and software modules work together to meet critical and evolving business needs as well as stringent management and security standards. Hear VMware and Microsoft representatives discuss how the joint solution between Dell Edge Gateway, Microsoft Azure IoT Edge and VMware Pulse IoT Center helps customers save tremendous amounts of time and money by accelerating and simplifying deployment of secure IoT edge solutions.


text:
Left-Leaning Veterans Group To Hand Out USS McCain T-Shirts At Trump 4th Of July Event
By Wayne Dupree | Featured Contributor | July 5, 2019 2:44AM
It is an honor for a US president to speak on American Independence Day. There would have been no demonstrations if a Democratic president had spoken. Trump could have gone golfing or like other presidents, been on vacation, but, like a true patriot, he is going to be in DC and speak to Americans.
As a combat vet of the Iraq war, I have no love for the late Sen. John McCain. He was just like every other senator who overstayed his time in office and continued to milk the American people (my opinion).
Left-leaning group VoteVets raised enough money to make more than 5,000 shirts that feature the words "USS JOHN S. MCCAIN" in bold red letters and "BIG BAD JOHN," the nickname for the ship, in smaller blue letters. The shirt also features an image of the ship, which is named after all three generations of McCains.
"Today, we learned the news that Donald Trump is turning the national Fourth of July celebration into a 2020 campaign event, complete with a ticketed VIP section for friends and supporters," an email from the group read. "That's not what America is about."
Peter Kauffman, vice chairman of VoteVets, said that concept of handing out the shirts was done to emphasize the country rather than Trump on Independence Day.
"It's really a way to honor a family that, through multiple generations, has shown that the country is bigger than any one individual," Kauffmann told the Huffington Post. "July 4 has never been about who is president. The idea that Donald Trump can come in and sell VIP tickets so you can get good seats while the regular old people have to stay back from the area is antithetical to the whole idea of America." [Washington Examiner]
McCain, the POW, Vietnam Veteran I have nothing but respect for. There's been several stories about his captivity, what he did or didn't do while being in North Vietnam for over 5 yrs. as a POW, however, unless you were there, those stories are just that stories.
Visit our friends at WHATFINGER NEWS: The Internet's Conservative Homepage
The man went through Hell, all our Vietnam veterans did, and they all deserve more than we can ever give them because of what we made them endure not only over there but when they came back home, but I can't walk away from him being a traitor to his political party.
These left-leaning veteran groups aren't getting my praise either.
If you are interested in volunteering to help distribute these shirts with veterans on the Fourth of July in Washington, DC please visit our @countable action center – and a special thank you to @countable for all of their help and support: https://t.co/UGRra5RmIJ pic.twitter.com/pljS8CvzcP
— RagsOfHonorUSA (@RagsOfHonorUSA) June 22, 2019
Again, most of us applauded his military service. It was politics he sucked at. And regardless of the party, he affiliated himself with he was democrat deep down.
Joy Behar Wants Trump Charged For 'Hate Speech'
As for this group of veterans, you would think they would highlight America's birthday, but you can see what they are trying to do and for that, I am against it. It's not that many times I raise my voice toward fellow veterans, but I am doing it now.


These little treats from Klutz look good enough to eat! Create and decorate your own mini cakes, cookies and pies with easy-peasy, no bake, air-dry clay. This kit includes all of the "ingredients" and instructions for rolling out clay just like fondant. Make faux flowers, stack on the sprinkles, add expressive faces, and more, then display your clay creations on a mini-cake stand or in a beautiful box to highlight your baking talents! It's a bake shop of captivatingly-cute confectionary.


Feb. 8, 2019─ Compared to Mexican American children, Puerto Rican children were more likely to have poor or decreasing use of inhaled medication needed to control their asthma, according to new research published online in the Annals of the American Thoracic Society.
In "Longitudinal Patterns of Mexican and Puerto Rican Children's Asthma Controller Medication Adherence and Acute Healthcare Utilization," Kimberly J. Arcoleo, PhD, MPH, and co-authors report on what is believed to be the first study of adherence over time to inhaled corticosteroids (ICS) for asthma within Latino populations. To control asthma and prevent exacerbations, ICS need to be taken by those with persistent asthma even when their symptoms are not apparent.
Dr. Arcoleo, who is an associate professor at the University of Rochester School of Nursing in New York, said that the study shows that there are naturally changing patterns of children's ICS adherence over time.


Flex Arches from RockCast's Custom Cast Stone Series are available in custom sizes to meet your design needs. When ordering, please specify opening width (X) and either radius (R) or opening height (Y). Additional joints will be added depending on the width of the opening. Units are available in smooth or chamfered in 5 5/8" and 7 5/8" heights. RockCast's Custom Cast Stone Series' Flex Arches match HD2257, HD2258, HD2256 and BA100 for jambs and legs.


text:
We are looking for a bright, driven, and resourceful paralegal to join our team and contribute to the success of a fast-growing financial services company by providing critical support to our global Legal team.
In this role, you will support our growing Seattle and London legal teams.
Contracting – You will assist in all phases of the contract negotiation process, from intake, through negotiation to closing. You will be responsible for negotiating certain types of contracts and will assist in the contracting process for others Following execution, you will monitor contracts for key terms and calendar significant events.
Corporate Governance -- You will coordinate and prepare materials for the board meetings of the Remitly group of entities, including agendas, resolutions, minutes, consents and other documentation
Stock Plan Administration -- You will administer and manage our equity incentive program and ensure all equity transactions, such as grants and exercises, are accurately processed, settled and recorded in a timely manner.
Intellectual Property Administration -- You will work closely with internal and outside counsel to manage and further develop the company's global patent and trademark portfolio.
Legal Marketing – You will work closely with our marketing team and legal team to perform a legal review of marketing campaigns. You will work closely with our marketing teams to develop new marketing materials for a service being offered around the world, ensuring that our campaigns are not only effective, but compliant with all applicable laws.
Litigation Support – You will assist in the collection, preparation, and submission of documents to be used in support of any litigation that Remitly may become involved in.
Smart.
3+ years' of paralegal, contract management, or other comparable experience (in-house experience preferred)
Paralegal certification a plus
Common sense and a sense of humor, demonstrated sound judgment, and a great team player
Motivated.
You have a strong bias for action. You see roadblocks and take the initiative to solve them. You possess the ability to think creatively and strategically, and identify opportunities for improvements. You thrive in a fast-paced, rapidly evolving environment. You don't like having to do the same thing over and over, so you build better processes that enable you to do more, faster.
You have a proactive attitude geared towards continuous improvement and learning
Ability to work independently, but also able to be a strong contributor as a member of a larger team working on complex cross-functional projects.
Detail-oriented.
You have a meticulous attention to detail with a track record of accuracy. Nothing gets by you.
You thrive on putting all the pieces together - communicating and working with all internal and external stakeholders involved
Excellent organizational skills, ability to manage multiple projects at once, follow through, and meet aggressive deadlines
Professional.
You have excellent analytical and communication skills (written and spoken)
Exercises sound judgment, integrity and discretion when handling confidential information
Independent, but also works well in a team setting
Tech-savvy.
Strong proficiency in Google Apps (Gmail, Calendar, Drive, Docs, Slides), MS Suite (Word, Excel, PowerPoint), DocuSign, Adobe Acrobat, and general comfort with learning new software.
Experience implementing new systems a plus.
Remitly is a group of passionate people working to make international payments easier and more transparent on both the web and mobile devices. We are seeking team members to join us that want to make a difference and change an industry. We pride ourselves on aiming high and delivering results, data being at the heart of everything we do, and encouraging our team to own business decisions and outcomes. Sound like the place for you? Join us.
Remitly is an E-Verify Employer


An adjustment to Family Contribution Limits under an HSA policy for 2018, LISTEN UP! The 2018 contribution limit for Health Savings Accounts (HSAs) linked to family coverage will be $6,850- no longer $6,900, as the IRS had previously indicated. The..
HSA's continue to be relevant, yet most do not take full advantage of the tax benefits With all the recent news surrounding health care it comes as no surprise that we continue to hear more about Consumer Driven Health..


text:
"""
Code for rpc message dispatching.

Messages that come in have a version number associated with them.  RPC API
version numbers are in the form:

    Major.Minor

For a given message with version X.Y, the receiver must be marked as able to
handle messages of version A.B, where:

    A = X

    B >= Y

The Major version number would be incremented for an almost completely new API.
The Minor version number would be incremented for backwards compatible changes
to an existing API.  A backwards compatible change could be something like
adding a new method, adding an argument to an existing method (but not
requiring it), or changing the type for an existing argument (but still
handling the old type as well).

The conversion over to a versioned API must be done on both the client side and
server side of the API at the same time.  However, as the code stands today,
there can be both versioned and unversioned APIs implemented in the same code
base.
"""

from nova.rpc import common as rpc_common

class RpcDispatcher(object):
    """Dispatch rpc messages according to the requested API version.

    This class can be used as the top level 'manager' for a service.  It
    contains a list of underlying managers that have an API_VERSION attribute.
    """

    def __init__(self, callbacks):
        """Initialize the rpc dispatcher.

        :param callbacks: List of proxy objects that are an instance
                          of a class with rpc methods exposed.  Each proxy
                          object should have an RPC_API_VERSION attribute.
        """
        self.callbacks = callbacks
        super(RpcDispatcher, self).__init__()

    @staticmethod
    def _is_compatible(mversion, version):
        """Determine whether versions are compatible.

        :param mversion: The API version implemented by a callback.
        :param version: The API version requested by an incoming message.
        """
        version_parts = version.split('.')
        mversion_parts = mversion.split('.')
        if int(version_parts[0]) != int(mversion_parts[0]):  # Major
            return False
        if int(version_parts[1]) > int(mversion_parts[1]):  # Minor
            return False
        return True

    def dispatch(self, ctxt, version, method, **kwargs):
        """Dispatch a message based on a requested version.

        :param ctxt: The request context
        :param version: The requested API version from the incoming message
        :param method: The method requested to be called by the incoming
                       message.
        :param kwargs: A dict of keyword arguments to be passed to the method.

        :returns: Whatever is returned by the underlying method that gets
                  called.
        """
        if not version:
            version = '1.0'

        for proxyobj in self.callbacks:
            if hasattr(proxyobj, 'RPC_API_VERSION'):
                rpc_api_version = proxyobj.RPC_API_VERSION
            else:
                rpc_api_version = '1.0'
            if not hasattr(proxyobj, method):
                continue
            if self._is_compatible(rpc_api_version, version):
                return getattr(proxyobj, method)(ctxt, **kwargs)

        raise rpc_common.UnsupportedRpcVersion(version=version)

redpajama_set_name: RedPajamaGithub


text:
\section{Introduction}\label{introduction}

The main goal of relativistic heavy ion collisions,  such as those being carried out at Relativistic Heavy Ion Collider (RHIC) and the Large Hadron Collider (LHC), is to explore the phase diagram of    matter described by  quantum chromodynamics, especially the properties of deconfined quark-gluon plasma (QGP) that could be created in these collisions, and its transition to hadronic matter~\cite{Jacak:2012dx,Shuryak:2014zxa}.    Although the bulk properties of the created QGP are governed by light quarks and gluons, the rare heavy charm and bottom quarks produced in ultra-relativistic heavy ion collisions are also useful probes of its properties~\cite{Linnyk:2008hp,He:2012df,He:2011qa,Uphoff:2012gb,Cao:2015hia,Nahrgang:2014vza,Scardina:2017ipo,Das:2017dsh,Das:2016cwd,Das:2015ana,Das:2013kea,Tolos:2016slr,Cao:2016gvr,Beraudo:2017gxw,Beraudo:2014boa,Alberico:2011zy}.   Studying resulting charmed and bottom hadrons, such as the $D$ ($B$) mesons and $\Lambda_{c}$ ($\Lambda_{b}$), $\Sigma_{c}$ ($\Sigma_{b}$), $\Xi_{c}$ ($\Xi_{b}$) baryons in relativistic heavy ion collisions, has thus been a topic of great interest~\cite{Plumari:2017ntm,Ravagli:2007xx,He:2019tik}. In recent experiments by the STAR Collaboration, the transverse moment spectrum of $D^0$ mesons and also the $\Lambda_c/D^0$ ratio from $\nuclide{Au} + \nuclide{Au}$ collisions have been measured~\cite{Dong:2017dws,Xie:2017jcq,Zhou:2017ikn,Xie:2018thr}.   The  experimental data from collisions at $10$-$80$\% centrality shows  the ratio  $\Lambda_c^+/D^0 \simeq 0.8$--$1.1$  in the transverse momentum region of  $3 < p_{T}^{} < 6$~GeV, which is a very large enhancement compared to the value predicted  from the fragmentation  of charm quarks or from the PYTHIA results for $p+p$ collisions~\cite{Lisovyi:2015uqa,Sjostrand:2006za}.  Such a ratio is also much larger than the prediction for the integrated yield from the  statistical hadronization model, where $\Lambda_{c}^+/D^{0} \, \simeq 0.25 - 0.3$~\cite{Kuznetsova:2006bh,Andronic:2007zu,Andronic:2010dt}.

Similar enhancements of the baryon to meson ratios of hadrons consisting of light and strange quarks in relativistic heavy ion collisions compared to those from $p+p$ collisions were previously seen in experiments at
RHIC~\cite{Agakishiev:2011dc,Agakishiev:2011ar,Abelev:2013xaa,Abelev:2014laa}, and they were successfully explained in terms of the quark coalescence model for the production of hadrons of intermediate momenta~\cite{Greco:2003xt,Fries:2003vb,Greco:2003mm,Fries:2008hs,Minissale:2015zwa}. Extending the quark coalescence model to charm quarks, it was shown in Refs.~\cite{Lee:2007wr,Oh:2009zj} that the $\Lambda_{c}^+/D^0$ ratio in relativistic heavy ion collisions is also enhanced when compared with that in $p+p$ collisions at the same energy.  An improved study using a more realistic charm quark  spectrum was later carried out in Ref.~\cite{Plumari:2017ntm}. The predicted ratio $\Lambda_{c}^+/D^0$ at $p_T^{} \approx 6$~GeV from this study is found to be about 0.4, which is still a factor of 2 smaller than the measured value in  the  STAR experiments. Recently, it was found that this ratio could be explained by the resonance recombination model (RRM) ~\cite{Ravagli:2007xx}
after including a large number of "missing" charm baryon states ~\cite{He:2019vgs}.

In the present study, we improve   the work of Ref.~\cite{Oh:2009zj} by employing a more realistic charm quark spectrum and also including in the quark coalescence model the flow effect  on produced heavy particles.  In the usual coalescence model, such as the one employed in Refs.~\cite{Oh:2009zj,Plumari:2017ntm}, the transverse momentum of a produced hadron is  equal to the total momentum of coalesced quarks. As a result, hadrons of different masses formed from these quarks all have same momentum, which is in contrast  to the hydrodynamical picture that hadrons of larger masses are shifted to higher transverse momentum as a result of collective flow. To include this effect, we boost a produced hadron from the center of mass of coalescing quarks, where its Wigner function is calculated to give its formation probability, back to the fireball frame using the physical mass of the hadron.  In this way, the momenta of produced hadrons, particularly resonances of large masses, are increased by the effect of parton collective flow.  With this improved approach as well as after including possible increase of hadron sizes in hot dense medium and the fragmentation contribution from charmed quarks not used in coalescence, we obtain a good description of the measured $D^0$ momentum spectrum and the predicted $\Lambda_{c}^+/D^0$ ratio as a function of $p_T^{}$   also agrees nicely with the available data    from  RHIC without assuming the existence of missing high mass  charmed baryon resonances as in Ref.~\cite{He:2019vgs}.  In addition, we find that the total yield ratio $\Lambda_{c}^+/D^0$ is around 0.64, and the ratio $\Lambda_{c}^+/D^0$ at $p_T^{}=8$~GeV can be as large as 0.6, which is much larger than the predictions from   previous studies reported in Refs.~\cite{Oh:2009zj,Plumari:2017ntm}.

\section{Quark momentum spectra}

\subsection{Light quarks  }

For the light quark momentum spectra, we adopt an approach  similar to that employed in Ref.~\cite{Oh:2009zj} by using  more realistic  ones from Ref.~\cite{Plumari:2017ntm}.  Specifically, the longitudinal momentum distribution of light quarks is assumed to be boost invariant in the rapidity range of $|y|\le 0.5$.  To take into account the collective flow of quark-gluon plasma, we assume  that  light  partons have a radial flow profile of $\beta_T(r_T^{})=\beta_{\rm max} {r_T^{}}/{R}$ in the transverse plane of a heavy ion collision, where $R$ is the transverse radius of the quark-gluon plasma at hadronization proper time $\tau$.  The transverse momentum distribution of light quarks is taken to be a thermal one  at temperature $T=165$~MeV, that is
\begin{eqnarray}
\label{quark-distr}
\frac{dN_{q,\bar{q}}}{\:d^{2}p_{T}^{}} &=& \frac{g_{q,\bar{q}} \, \tau m_{T}^{}}{(2\pi)^{3}} \nonumber\\
&\times&\int \exp \left[-\frac{\gamma_{T}^{}(m_{T}^{}-p_{T}^{} \cdot \beta_{T}^{})\pm\mu}{T} \right] d^{2}r_{T}^{}. \label{light-quark-dis}
\end{eqnarray}
In the above, $g_{q,\bar{q}}=6$ are the spin-color degeneracies of  quarks and antiquarks, $\mu$   is the quark baryon chemical potential with the plus and minus signs for quarks and antiquarks, respectively, $m_T^{} = \sqrt{p_T^2+m_{q,\bar{q}}^2}$ is the transverse mass with $m_{q,\bar q}$ being the constituent quark and antiquark masses, which are taken to be 300 MeV and 475 MeV for light and strange quarks, respectively, and $\gamma_T=1/\sqrt{1-\beta_T^2}$.   As in Refs.~\cite{Greco:2003xt,Minissale:2015zwa}, we also include the contribution from gluons in the quark-gluon plasma, which are taken to have a   distribution similar to that of light quarks, by converting them to quarks and anti-quarks according to the quark flavor compositions in the quark-gluon plasma. The parameters for describing the fireball of hadronizing quark-gluon plasma and the numbers of light and strange quarks and antiquarks are summarized in Table~\ref{tabQuark},  and their values are very similar to those used in Ref.~\cite{Plumari:2017ntm}.

\begin{table} [t]
\begin{center}
\begin{tabular}{lc|c|c|c|c|c|c}
\hline \hline
& $N_u$ ($N_{\bar{u}}$) & $N_s$ &   $R$ (fm)  & $\tau$ (fm/$c$) & $T$ (MeV)  & $\beta_{\rm max}$   & $\mu$ (MeV) \\
\hline
 & 243 (224) & 143  & 8.5 & 4.5 &   165            &  0.5  & 10    \\
\hline \hline
\end{tabular}
\end{center}
\caption{\protect Up and antiup quark numbers $N_u$ and $N_{\bar u}$, strange quark number $N_s$,  transverse radius $R$, hadronization proper time $\tau$, temperature $T$, and flow velocity $\beta_{\rm max}$ of QGP produced at mid-rapidity of central $\nuclide{Au} + \nuclide{Au}$ collisions at $\sqrt{s_{NN}} = 200$~GeV and 0-10\% centrality.  The number of down and antidown quarks are the same as those of up and antiup quarks.}
\label{tabQuark}
\end{table}

\subsection{Charm quarks  }

\begin{table} [b]
\begin{center}
\begin{tabular}{l|c|c|c|c|c|cc}
\hline \hline
          RHIC  & $a_0^{}$ & $a_1^{}$ & $a_2^{}$ & $a_3^{}$  & $a_4^{}$  & $a_5^{}$   \\
\hline
 $p_T^{} \leq p_0^{}$  & 0.69 & 1.15  & 1.57  &   ---     &   ---     &   ---     \\
 $p_T^{} \geq p_0^{}$  & 1.08 & 3.04  & 0.71  & 9.914   & 2.5   & 3.48  \\
\hline \hline
\end{tabular}
\end{center}
\caption{Parameters  used in the parametrization of charm quark transverse momentum spectrum at mid-rapidity
of central $\nuclide{Au} + \nuclide{Au}$ collisions at $\sqrt{s_{NN}^{}} = 200$~GeV.}
\label{tabCHARM}
\end{table}

For the charm quark momentum spectrum in heavy ion collisions at RHIC, we use the one parametrized in Ref.~\cite{Plumari:2017ntm}, which is based on   results from a transport model study of charm quark energy loss and flow.  It has the form
\begin{eqnarray}\label{charm}
&&\frac{dN_c}{d^2p_T^{}}\nonumber\\
&&=\left\{\begin{array}{lr}
a_0^{} \exp{[-a_1^{} p_T^{a_2^{}}]}, & p_T^{} \leq p_0^{} \\
a_0^{} \exp{[-a_1^{} p_T^{a_2^{}}]}+a_3^{} \left(1+p_T^{a_4^{}} \right)^{-a_5^{}}, & p_T^{} > p_0^{}
\end{array}\right.
\nonumber \\
\end{eqnarray}
where $p_0^{} = 1.85$~GeV and the values of the parameters  $a_i$ with $i=1,\cdots, 5$ are given in Table~\ref{tabCHARM}.  They are slightly different from those in Ref.~\cite{Plumari:2017ntm} to achieve a better description of the measured $D^0$ spectrum at large transverse momentum.  Integrating the above transverse momentum spectrum gives the total number of heavy quarks of $dN_c/dy \simeq 2.1$   for the collisions at  RHIC considered in the present study.   For the charm quark mass, we use $m_c = 1.5~\mbox{GeV}$ in the present study.

\section{Quark coalescence}
For simplicity, we assume as in Ref.~\cite{Oh:2009zj} that the spatial distribution  of quarks   is uniform  in the thermalized QGP inside a fire cylinder of volume $V=\pi R^2\tau$.  Taking the Wigner function of hadrons to be Gaussian in space and in momentum and neglecting the space and velocity correlation of light quarks due to collective flow, we can  integrate out the spatial part  of the coalescence formula   and obtain the transverse momentum spectrum of produced heavy mesons of certain species as
\begin{eqnarray}
\frac{dN_M}{d\bm{p}_M^{}} &=& g_M^{} \frac{(2\sqrt{\pi}\sigma)^3}{V}
\int d \bm{p}_1^{} d \bm{p}_{2}^{} \frac{dN_1}{d\bm{p}_1^{}}
\frac{dN_{2}}{d\bm{p}_{2}^{}}
\nonumber \\ && \mbox{} \times
\exp\left(-\bm{k}^2 \sigma^2 \right) \delta({\bf p}_M-{\bf p}_1-{\bf p}_2). \label{eq:meson-coal}
\end{eqnarray}
In the above, $g_M^{}$ is the statistical factor for colored spin-1/2 quark and antiquark to form a color neutral meson, e.g., $g_{D^0}^{}=1/36$ and $g_{D^{*0}}^{}=1/12$ for $D^0$ and $D^{*0}$, respectively. The momenta ${\bf p}_1$, ${\bf p}_2$, and ${\bf p}_M$ are those of the heavy quark, light quark, and produced heavy meson, respectively, with the $\delta$ function to ensure the momentum conservation. The relative transverse momentum $\bm{k}$ between the heavy quark of mass $m_1$  and light antiquark of mass $m_2$  is defined as
\begin{equation}
\bm{k} = \frac{1}{m_1^{} + m_2^{}}
\left( m_2^{} \bm{p}_1' - m_1^{} \bm{p}_2' \right),
\label{eq:def_k}
\end{equation}
where ${\bf p}_1^\prime$ and ${\bf p}_2^\prime$ are the momenta of the heavy quark and light antiquark in the center of mass frame of produced heavy meson.
The width parameter $\sigma$ is related to the harmonic oscillator frequency $\omega_M$ by $\sigma= 1/\sqrt{\mu\omega_M}$ with $\mu = m_1^{} m_2^{} / (m_1^{} + m_2^{})$ being the reduced mass.

Similarly, the  momentum spectrum of heavy baryons from the coalescence of a charm quark and two light quarks can be calculated according to
\begin{eqnarray}
\frac{dN_B}{d\bm{p}_{B}^{}} &=& g_{B}^{} \frac{(2\sqrt{\pi})^6
(\sigma_1^{} \sigma_2^{})^3}{V^2} \int d \bm{p}_1^{} d \bm{p}_2^{} d \bm{p}_3
\frac{dN_1}{d\bm{p}_1^{}} \frac{dN_2}{d\bm{p}_2^{}} \frac{dN_3}{d\bm{p}_3^{}}
\nonumber \\ && \mbox{} \times
\exp\left(-\bm{k}_1^2 \sigma_1^2 - \bm{k}_2^2 \sigma_2^2 \right) \delta({\bf p}_B-{\bf p}_1-{\bf p}_2-{\bf p}_3),
\nonumber \\
\label{eq:3q-coal}
\end{eqnarray}
where the index $3$ refers to the heavy quark and indices $1$ and $2$ refer to light quarks, and $g_B^{}$ is the statistical factor, which, for example, is $1/108$ for $\Lambda_c$, $1/36$ for $\Sigma_c$, $1/54$ for $\Xi^c (\Xi_c^\prime)$, and $1/8$ for $\Sigma_c^*$ and $\Xi_c^*$.  The relative transverse momenta are defined as
\begin{eqnarray}
\bm{k}_1 &=& \frac{1}{m_1^{} + m_2^{}}
\left( m_2^{} \bm{p}_1' - m_1^{} \bm{p}_2' \right),
\nonumber \\
\bm{k}_2 &=& \frac{1}{m_1^{} + m_2^{} + m_3^{}}
\left[ m_3^{} \left( \bm{p}_1' + \bm{p}_2' \right)
- (m_1^{} + m_2^{}) \bm{p}_3' \right],
\nonumber \\
\end{eqnarray}
with ${\bf p}_1^\prime$, ${\bf p}_2^\prime$ and ${\bf p}_3$ being the momenta of the heavy quark and two light quarks in the center of mass frame of produced heavy baryon.
The width parameters $\sigma_i^{}$ are related to the oscillator parameter $\omega_B$ by $\sigma_i^{} =1/\sqrt{\mu_i\omega_B}$ with
\begin{eqnarray}
\mu_1^{} = \frac{m_1^{} m_2^{}}{m_1^{} + m_2^{}}, \qquad
\mu_2^{} = \frac{(m_1^{} + m_2^{}) m_3^{}}{m_1^{} + m_2^{} +m_3^{}}.
\end{eqnarray}

As in Ref.~\cite{Oh:2009zj}, we take the oscillator constants  $\omega_M$ for  $D_0$ meson and $\omega_B$ for  $\Lambda_c^+$ baryon as parameters, and determine their values  by fitting the spectrum of $D_0$ meson and requiring all the charm quarks at low momenta to hadronize by quark coalescence. To include the flow effect on produced hadrons, we carry out the coalescence calculation  at the medium rest frame and then boosting these hadrons to the fireball frame. Because of the smaller quark thermal velocity than the flow velocity, the flow  effect can be approximately included by first calculating the formation probability of a charmed hadron from coalescing charm and light quarks using its Wigner function evaluated in the center of mass of these quarks and then boosting the resulting charm hadron to the fireball frame using its physical mass. This approximation results in the multiplication of the momentum ${\bf p}_M$ and ${\bf p}_B$ in the delta functions in Eqs.(3) and (4) by the factor  $(E_1+E_2)/E_M$ and $(E_1+E_2+E_3)/E_B$, respectively, where $E_i=\sqrt{m_i^2+{\bf p}_i^2}$ and $E_{M,B}=\sqrt{m_{M,B}}^2+{\bf p}_{M,B}^2$ with $m_{M,B}$ being the mass of produced heavy hadrons. In this case, heavy resonances with large masses would have large transverse momenta in the rest frame of the expanding QGP, which is consistent with the hydrodynamic picture  that  the additional momenta acquired by particles due to the collective flow are larger if they are more massive.  This effect has been neglected in previous studies
based on the coalescence approach~\cite{Oh:2009zj,Plumari:2017ntm} where the transverse momentum spectrum of produced particles is independent of their masses. The present approach is thus more appropriate for studying the production of massive resonances in relativistic heavy ion collisions. We note that the production of massive hadrons is not suppressed in the coalescence model as it is based on the sudden approximation. This is in contrast to that in the resonance recombination model of Ref.~\cite{Ravagli:2007xx} used in Ref.~\cite{He:2019vgs} due to the required energy conservation in this approach.

\section{charm quark fragmentation}

Similarly to Refs.~\cite{Oh:2009zj,Plumari:2017ntm}, charm quarks that are not used for producing hadrons via  coalescence with light quarks are  converted to hadrons by fragmentation. In terms of the fragmentation probability $P_{\rm frag}(p_T^{})=1-P_{\rm coal}(p_T^{})$ of a charm quark of transverse momentum $p_T^{}$, where $P_{\rm coal}(p_T^{})$ is its probability to coalesce with light quarks, the momentum spectrum of certain hadron species from the fragmentation of non-coalesced charm quarks is given by
\begin{equation}
\frac{dN_{\rm had}}{d^{2}p_T^{}}=\sum \int dz P_{\rm frag}(P_T^{})\frac{dN_{N_c}}{d^{2}p_T^{}}
\frac{D_{{\rm had}/c}(z,Q^{2})}{z^{2}}.
\label{Eq:frag}
\end{equation}
In the above,  $z=p_{\rm had}/p_{c}$ is the fraction of charm quark momentum carried by the produced hadron and $Q^2=(p_{\rm had}/2z)^2$ is the momentum scale for the fragmentation process. For  the fragmentation function $D_{\rm had/c}(z,Q^{2})$,  we use the one from Ref.~\cite{PSSZ83},
\begin{eqnarray}
D_{\rm had}(z) \propto 1/\left[ z \left(1-\frac{1}{z}-\frac{\epsilon_c}{1-z} \right)^2 \right],
\end{eqnarray}
with $\epsilon_c$  being a free parameter to fix the shape of the fragmentation function. In the present  study, we choose $\epsilon_c=0.006$ for $D$ mesons and $\epsilon_c=0.02$ for $\Lambda_c$ baryons, which leads to the fragmentation branching ratios to $D^0$, $D^+$, $D_s^+$, and $\Lambda_c^+$ being 0.607, 0.196, 0.121, and 0.076, respectively~\cite{Oh:2009zj}.

\section{results}

\begin{table} [t]
\begin{center}
\begin{tabular}{c|c|c|c|cc}
\hline
Meson & Mass (MeV) & $I (J)$ & \\
\hline
$D^+ =\bar{d}c$		& 1869 & $\frac{1}{2} \,(0)$	&\\
$D^0 =\bar{u}c$ 	& 1865 & $\frac{1}{2} \,(0)$	&\\
$D_{s}^{+} =\bar{s}c$	& 1968 & $0 \,(0)$		& \\
\hline
Resonances & & & Decay modes& B.R. \\
\hline
$D^{*+} =\bar{d}c$	& 2010 & $\frac{1}{2} \, (1)$	& $D^0 \pi^+$ & $68\%$ \\
&&& $D^+ X$& $32\%$ \\
$D^{*0} =\bar{u}c$	& 2007 & $\frac{1}{2} \, (1)$	& $D^0 \pi^0$ & $62\%$ \\
&&& $D^0 \gamma$& $38\%$ \\
$D_{s}^{*+} =\bar{s}c$	& 2112 & $0 \, (1)$		& $D_{s}^+ X$ & $100\%$ \\
\hline
\end{tabular}
\end{center}
\caption{
Charmed mesons considered in the present study. The branching ratios (B.R.) of resonances decaying to the ground states are taken from Ref.~\cite{Agashe:2014kda}.
\label{tab:D}}
\end{table}

\begin{table} [t]
\begin{center}
\begin{tabular}{c|c|c|c|cc}
\hline
Baryon & Mass (MeV) & $I (J)$ & \\
\hline
$\Lambda_c^+ =udc$	& 2286 & $0 \, (\frac{1}{2})$	&\\
$\Xi_c^+ =usc$	& 2467 & $\frac{1}{2} \, (\frac{1}{2})$	&\\
$\Xi_c^0 =dsc$	& 2470 & $\frac{1}{2} \, (\frac{1}{2})$	&\\
\hline
Resonances & & & Decay modes& B.R. \\
\hline
$\Sigma_c^0 =ddc$	& 2455 & $1 \, (\frac{1}{2})$	&$\Lambda_c^+ \pi^-$ & $100\%$\\
$\Sigma_c^+ =udc$	& 2455 & $1 \, (\frac{1}{2})$	&$\Lambda_c^+ \pi^0$ & $100\%$\\
$\Sigma_c^{++} =uuc$	& 2455 & $1 \, (\frac{1}{2})$	&$\Lambda_c^+ \pi^+$ & $100\%$\\
$\Sigma_c^{*0} =ddc$	& 2520 & $1 \, (\frac{3}{2})$	&$\Lambda_c^+ \pi^-$ & $100\%$\\
$\Sigma_c^{*+} =udc$	& 2520 & $1 \, (\frac{3}{2})$	&$\Lambda_c^+ \pi^0$ & $100\%$\\
$\Sigma_c^{*++} =uuc$	& 2520 & $1 \, (\frac{3}{2})$	&$\Lambda_c^+ \pi^+$ & $100\%$\\
$\Xi_c^{*+} =usc$	& 2645 & $\frac{1}{2} \, (\frac{3}{2})$	&$\Xi_c^+ \pi^0$ & seen\\
$\Xi_c^{*0} =dsc$	& 2645 & $\frac{1}{2} \, (\frac{3}{2})$	&$\Xi_c^+ \pi^-$ & seen\\
$\Xi_c'^+ =usc$	& 2580 & $\frac{1}{2} \, (\frac{1}{2})$	&$\Xi_c^+ \gamma$ & seen \\
$\Xi_c'^0 =dsc$	& 2580 & $\frac{1}{2} \, (\frac{1}{2})$	&$\Xi_c^0 \gamma$ & seen \\
\hline
\end{tabular}
\end{center}
\caption{ Same as Table~\ref{tab:D}   but for charmed baryons.
\label{tab:Lambda}}
\end{table}

As shown in Ref.~\cite{Oh:2009zj}, the contributions from resonances to the yield of ground state hadrons are important and  should be taken into account. Tables~\ref{tab:D} and \ref{tab:Lambda} summarize  the  charmed hadrons considered in the present study, which include the ground states and the resonance states of $D$ mesons and $\Lambda_c$ and $\Xi_c$ baryons, as given by the Particle Data Group~\cite{Agashe:2014kda}. For the branching ratios  of $\Xi_c^*$ and $\Xi_c'$ baryons  decaying by strong or electromagnetic interactions to the $\Xi_c$ baryon, which are not given in Ref.~\cite{Agashe:2014kda}, they are assumed to   be 100\%.  We note that all charmed meson and baryon resonances in Tables~\ref{tab:D} and \ref{tab:Lambda} have their orbital wave functions in the $L=0$ states.

\begin{figure}[h]
\centering
\includegraphics[scale=0.37, angle=0,clip]{fig1.eps}
\caption{\label{Fig1}
Transverse momentum spectrum  of $D^0$ mesons at mid-rapidity from $\nuclide{Au} + \nuclide{Au}$ collisions at $\sqrt{s_{NN}^{}}=200$~GeV and (0--10\%) centrality. Dashed and dash-dotted lines    are  the $D^0$ spectra from charm quark coalescence and fragmentation, respectively, and their sum is given by the solid line. The experimental data shown by solid squares are taken from Ref.~\cite{Adam:2018inb}. }
\end{figure}

As in  Ref.~\cite{Oh:2009zj}, we first determine the harmonic oscillator frequency $\omega_M$ in the Wigner functions for $D^0$. The value of $\omega_M \approx 0.096$~GeV is  obtained from fitting the $D^0$ transverse momentum spectrum to the data measured by  the  STAR Collaboration. This value is about a factor of 3 smaller than the value 0.33 GeV determined from the root-mean-square charge radius 0.43 fm of $D^+$ as predicted by the light-front quark model~\cite{Hwang:2001th}, implying an increase of the $D^0$ charge radius by a factor of 1.85 at temperature of $165$ MeV. We note that our oscillator constant for the charmed meson is close to the value of 0.106 GeV used in Ref.~\cite{Oh:2009zj}.  Figure~\ref{Fig1} shows our results for the $D_0$ transverse momentum spectrum from  charm  quark coalescence (dashed line), fragmentation (dash-dotted line), and their sum (solid line). It shows that the contribution from  charm quark coalescence dominates at $p_T^{} <  10$~GeV while that of fragmentation takes over at $p_T^{}$ larger than around 10~GeV.  This behavior is quite different from that obtained  in Ref.~\cite{Plumari:2017ntm}  with the conventional coalescence model,  which neglects the effect of flow on the momenta of produced charmed hadrons and thus results in a significant contribution from   charm quark fragmentation already at $p_T^{}> 3$~GeV.

\begin{figure}[h]
\centering
\includegraphics[scale=0.36,angle=0,clip]{fig2.eps}
\caption{\label{Fig2}
Fragmentation probability of charm quarks as a function of transverse momentum for central Au+Au collisions at $\sqrt{s_{NN}}=200 \, \mbox{GeV}$ and  0-10\% centrality.}
\end{figure}

Figure~\ref{Fig2} shows the fragmentation probability $P_{\rm frag}$ of charm quarks as a function of transverse momentum in central $\nuclide{Au} + \nuclide{Au}$ collisions at $\sqrt{s_{NN}^{}}=200$~GeV.  Although charm quarks with $p_T^{} > 4$~GeV are more likely to hadronize by fragmentation than coalescence, only $D_0$ mesons of $p_T^{} > 10$~GeV are mainly produced by charm quark fragmentation as shown in Fig.~\ref{Fig1}.  This is because the charm quark in $D^0$ from coalescence (fragmentation) mainly comes from those with momentum smaller (larger) than that of $D^0$.

\begin{figure}[h]
\centering
\includegraphics[scale=0.35, angle=0,clip]{fig3.eps}
\caption{\label{Fig3}
\protect Transverse momentum spectra of $D^+$ \protect  (upper panel) and $D_s^+$ (lower panel) mesons in central Au+Au collisions at $\sqrt{s_{NN}^{}}=200$~GeV and  0-10\% centrality.  Dashed and dash-dotted lines   are  the spectra from charm quark coalescence and fragmentation, respectively, and their sum is shown by the solid line.}
\end{figure}

\begin{table} [b]
\begin{center}
\begin{tabular}{l|c|c|c|c|cc}
\hline \hline
          yield  & ${D^0}$ & ${D^+}$ &   ${D_s^+}$   & $\Lambda_c^+$  & $\Xi_c$ \\
 \hline
 RHIC  &0.85 &0.275  &0.236          &0.547  &0.175   \\
\hline \hline
\end{tabular}
\end{center}
\caption{Charmed hadron yields in central Au+Au collisions at $\sqrt{s_{NN}}=200 \, \mbox{GeV}$ and  0-10\% centrality.}
\label{RHICYield}
\end{table}

We also compute the spectra of produced $D_s^+$ and $D^+$ mesons, and the results are presented in Fig.~\ref{Fig3}. It is found that although the fragmentation contribution dominates at $p_T^{} > 10$~GeV for $D^+$, which is similar to that for $D_0$ shown in Fig.~\ref{Fig1}, it becomes important already at $p_T^{} > 7$~GeV for $D_s^+$. This is due to the softer $D_s$ transverse momentum spectrum than that of $D_0$ from  charm quark coalescence, which is also seen in Ref.~\cite{Zhao:2018jlw}. The yields of various charmed hadrons are summarized in Table~\ref{RHICYield}, which shows that the total number of charmed mesons is about 1.36 with the number of $D_0$ about three times that of $D^+$ because of the dominant contribution from the decay of charmed meson resonances.  For the remaining 0.74 charm quarks, they are converted to charmed baryons by coalescence and fragmentation as described below.

\begin{figure}[h]
\centering
\includegraphics[scale=0.36, angle=0,clip]{fig4.eps}
\caption{\label{Fig4}
\protect Transverse momentum spectra of $\Lambda_c^+$ baryon in Au+Au collisions at $\sqrt{s_{NN}}=200 \, \mbox{GeV}$ and  0-10\% centrality. Dashed and dash-dotted lines  are  the $\Lambda_c^+$ spectra  from charm quark coalescence and fragmentation, respectively, and the solid line is their sum.}
\end{figure}

Shown in Fig.~\ref{Fig4} is the $\Lambda_c^+$ spectrum, which includes those  from coalescence (dashed line), fragmentation (dash-dotted line), and their sum (solid line).  These results are obtained with the oscillator parameter $\omega_B = 0.16$~GeV for charmed baryons to ensure that the remaining charm quarks of very low transverse momenta, which are not used in the production of charmed mesons from the coalescence of charm quark with light antiquarks, are all used in the production of charmed baryons. This value of $\omega_B$ corresponds to an increase of the sizes of charmed baryons at temperature of 165 MeV compared to their values in free space using $\omega_B=0.33$.  This then leads to a yield of 0.547 for $\Lambda_c^+$ and 0.175 for $\Xi_c$ as shown in Table V.  The total integrated yield ratio $\Lambda_c^+/D_0$ is then about 0.64, which is slightly larger than the value of about 0.54 measured in $p+p$ collisions at $\sqrt{s}= 7$~TeV at LHC~\cite{Acharya:2017kfy,He:2019tik}. We note that the oscillator constant used here for charmed baryons is larger than that for charmed mesons, which is different from that in Ref.~\cite{{Oh:2009zj}} where they are taken to have the same value.

\begin{figure}[h]
\centering
\includegraphics[scale=0.36, angle=0,clip]{fig5.eps}
\caption{\label{Fig5}
The yield ratio $\Lambda_c^+/D^0$ as a function of transverse momentum for $\nuclide{Au} + \nuclide{Au}$ collisions at $\sqrt{s_{NN}^{}}=200$~GeV. Solid and dashed lines    denote  the ratio from only  charm quark coalescence and the sum of charm quark  fragmentation and coalescence   contributions for collisions at 0-10\% centrality.  The experimental data from Ref.~\cite{Xie:2018thr} for the 10-80\% centrality are shown by solid stars with combined statistical and systematic uncertainties.}
\end{figure}

In Fig.~\ref{Fig5}, we show the yield ratio $\Lambda_c^+/D^0$ as a function of transverse momentum in $\nuclide{Au} + \nuclide{Au}$ collisions at $\sqrt{s_{NN}^{}}=200$~GeV and  0-10\% centrality. It is seen that the fragmentation contribution suppresses this ratio, and the results from the sum of coalescence and fragmentation contributions (dashed line) describe very well the experimental data of Ref.~\cite{Xie:2018thr}.  For $p_T^{} \approx 6$~GeV, the ratio $\Lambda_{c}^+/D^0$ is predicted to be close to 1.0, which is much higher than the value of less than 0.4 obtained in Refs.~\cite{Oh:2009zj,Plumari:2017ntm}.  In particular, we find that the ratio $\Lambda_{c}^+/D^0$ at $p_T^{} = 8$~GeV can be as large as 0.6, while it was predicted to be around $0.2$ in Ref.~\cite{Plumari:2017ntm}.

Compared to the previous studies reported in Refs.~\cite{Oh:2009zj,Plumari:2017ntm}, the contribution from charm quark fragmentation in  the present study  is less important   due to the inclusion of the flow effect  on the momenta of hadrons formed from quark coalescence, which shifts higher mass charmed baryon resonances to larger transverse momenta, and this helps describe the ratio $\Lambda_{c}^+/D^0$  in the transverse momentum region of $4<p_T<6$ GeV.

\section{Conclusions}

Using the charm quark coalescence and fragmentation model with the inclusion of the effect of collective flow on the transverse momentum spectra of produced charmed hadrons, we have studied the transverse momentum spectra of charmed mesons and baryons as well as the $\Lambda_c/D_0$ ratio.  By tuning the oscillator constants in the charmed hadron Wigner functions in the quark coalescence model, which models their changing sizes in hot dense matter, to use up all the charm quarks at $p_T^{} \approx 0$~GeV and fragmenting  the remaining charm quarks into charmed hadrons, we have obtained the ratio $\Lambda_{c}^+/D^0$ as a function of $p_T^{}$ that successfully describes the experimental data measured at RHIC. This is in contrast  to previous studies that did not include the effect of collective flow on charmed hadrons formed from quark coalescence, which underestimate substantially  this ratio at $p_T^{} > 4.5$~GeV.  Compared to results from these studies, the contribution from fragmentation is less important in the present approach. As a result, we have obtained  a much larger value for  $\Lambda_{c}^+/D^0$ at $p_T^{} > 6$~GeV than that from the conventional approach.  Our study thus provides an alternative description of the measured $p_T$ dependence of the ratio $\Lambda_{c}^+/D^0$ at RHIC without the inclusion of a large number of unknown charmed baryon resonances as assumed in Ref.~\cite{He:2019vgs}. We have, however, neglected in the present study the space-momentum correlations of both light and charm quarks, which are shown in Ref.~\cite{He:2019vgs} to  help shift the peak of the $\Lambda_{c}^+/D^0$ ratio to higher transverse momentum. Also, the present study is based on a blast-wave model for light quarks.  It is thus important to verify the validity of the results and conclusions from the present study by using the phase-space distributions of light and charm quarks from more realistic models.   Since the  light or strange baryon to meson ratio at $p_T^{} \approx 4-7$~GeV in the quark coalescence approach without the flow effect is very small compared to the experimentally measured value~\cite{Minissale:2015zwa}, it will also be very interesting to check if the inclusion of  the flow effect  can help resolve this discrepancy.

{\it Note added in proof.} After the completion of present study, similar results and conclusions have been obtained from a further improved model that uses the quark phase-space distributions from a realistic dynamic model and also includes the production of $p$-wave charmed hadron resonances from quark coalescence~\cite{Cao:2019iqs}.

\begin{acknowledgments}
We are grateful to Xin Dong and Shuai Y.F. Liu for helpful discussions. This work was supported in part by the U.S. Department of Energy under Contract No. DE-SC0015266, the Welch Foundation under Grant No. A-1358, and the National Research Foundation of Korea (NRF) under Grants No.~NRF-2018R1D1A1B07048183, No.~NRF-2018R1A6A1A06024970, No.~NRF-2018R1A5A1025563, and No.~NRF-2019R1A2C1087107.
\end{acknowledgments}

redpajama_set_name: RedPajamaArXiv


text:
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Rudy A. Artz
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Rudy A. Artz, of Melissa, Texas, passed away on April 5, 2013 at the age of 75. He was born on July 21, 1937, in Makassar, Java, Indonesia, to Johan and Rosalia (de Ridder) Artz. On May 25, 1996, Rudy married Judy White in Huntington Beach, California. He grew up in Indonesia, but moved to Holland at the age of sixteen. Rudy was a member of the Merchant Marines in Europe. He was a manager in manufacturing. He enjoyed building furniture and remodeling homes.
He is survived by his wife, Judy White Artz of Melissa, Texas; sons, Michael White and Bob Uekert, both of Anna, Texas; daughters, Mar Diaz of Lakewood, California and Joyce White of Duarte, California; grandchildren, Alexandra Jade, Brianna Caitlyn both of Anna, Texas and Matthew Moore of Blythe, California; sister, Pearl Artz of Holland; uncle, Yosef Artz of Holland; a host of many other loving family and friends.
Rudy is preceded in death by his parents and brother.
A memorial service will be held on Wednesday, April 10, 2013, at 4:00 p.m., at Turrentine-Jackson-Morrow Chapel, in Allen, Texas, with Danny Buster officiating.
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