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TrueML Names Thomas Overton as Chief Technology Officer
11 January 2023 at 08:00 a.m. ET
Jan. 11, 2023, 8 a.m. Jan. 11, 2023, 10:40 a.m. insideARM.com The iA Institute
http://www.insidearm.com/news/00048783-trueml-names-thomas-overton-chief-technol/
LENEXA, Kan. -- One True Holding Company d/b/a/ TrueML, a financial technology software company developing machine learning-driven products that enable intelligent, digital communication in the financial services space, today announced that Thomas Overton will join as Chief Technology Officer.
TrueML develops software using patented machine learning technology to create a digital-first process that aligns with consumer communication preferences. As a mission-driven company, TrueML aims to bring solutions to the marketplace that redefine how creditors and consumers engage in debt collection.
TrueML's mission is supported by data scientists, financial services industry experts and customer experience enthusiasts collectively building technology to serve people in a digital-first way by recognizing their unique needs and preferences as human beings and endeavoring toward ensuring nobody gets locked out of the financial system.
"I am excited to join an organization driven to change the way an ages-old industry functions through digital innovation," said Overton. "Technology is at the heart of TrueML and machine learning is a key aspect of the company's overall growth strategy. The data scientists and engineers are incredibly talented and take the opportunity to produce a meaningful impact on the customer experience very seriously. I look forward to working with and empowering this team to deliver a world-class technology platform that gives consumers agency over their financial health."
With 25 years of experience in the technology space and a background as a full stack engineer and architect, Overton brings a broad range of skills from leadership, operational excellence, and scalable architecture to data governance and regulatory compliance. Overton most recently served as CTO and acting CISO at Crunchyroll as part of Sony where he directed technology strategy, guided architectural design, and ensured secure and compliant operations for the company's portfolio of cloud-hosted OTT, E-commerce, and game services. In 2018, he facilitated the acquisition of Crunchyroll by WarnerMedia, and in 2021 operated in a leading role to successfully complete Sony's acquisition of Crunchyroll for ~$1.2 billion. Previously, Overton's unique media and tech background led his path through systems engineering, data center build outs, color science, software development for B2B and B2C products, running an R&D division, and eventually leading product and engineering teams.
"At TrueML, we are building digital solutions to real problems, and the pace of innovation is high. We expect significant continued growth in 2023, and having experienced leadership for this focus area is critical to ensure that what we're building is not only effective and sustainable, but also compliant and scalable," said Steve Carlson, President of TrueML. "I'm confident that Thomas' leadership and technical expertise will support our business goals and, as a result, our mission to deliver industry-leading software that will transform the experiences of millions more financially distressed consumers in the coming years."
To learn more about TrueML, its subsidiaries and their products, visit www.TrueML.co, and follow on social media @TrueMLco.
About TrueML
TrueML is a software company developing machine learning-driven products that prioritize customer experience and revolutionize the experience of consumers seeking financial health. The mission-driven team of data scientists, financial services industry experts and customer experience fanatics are building technology to serve people in a way that recognizes their unique needs and preferences as human beings and endeavoring toward ensuring nobody gets locked out of the financial system.
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Who is Chelsea Meissner? Biography, Age, Height, Family, Net Worth, Husband, Workout, Surgery
HomeBiography
Who is Richard Malone? Biography, Age, Height, Net Worth, Vogue, Instagram, Collection, Family, Girlfriend, Fashion Shows, Nationality
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Who is Pamella Roland? Biography, Age, Height, Family, Net Worth, Husband, Son, Instagram
Pamella Roland Wiki Bio: Pamella Roland is a well-known American fashion designer and Instagram star. She got recognized for being the founder of a self-titled evening wear line. She is also popular for her high-profile clients like Jennifer Garner, Angelina Jolie, Eva Longoria, Kim Cattrall, and Halle Berry. She has achieved Gold Coast Award in 2003 and became a member of the Council of Fashion Designers of America (CFDA) in 2010. Besides this, she has amassed thousands of followers on Instagram for posting a variety of fashionable outfits designed by herself.
Pamella was born on January 2, 1959, in Michigan, United States. She completed her education at a private high school in her hometown. Then she attended Michigan State University and received a bachelor's degree in business. She is 63 years old (as of 2022). In this article, you will get information about Pamella Roland's wiki, biography, age, birthday, height, weight, net worth, family, relationship, affairs, nationality, siblings, Instagram, TikTok, Youtube, Twitter, Facebook, and more.
Name Pamella Roland
Birth Place Michigan, United States
Date of Birth January 2, 1959
Profession Fashion designer and Instagram star
Pamella Roland Age / Birthday
Pamella's age is 63 years old (as of 2022). She came into this world on January 2, 1959. So, she celebrates her birthday every year on January 2 along with her family and friends. Her zodiac sign is Capricorn. She believes in Christianity.
Pamella Roland with Vanessa William
Pamella Roland Height, Weight, and Measurements
Talking about Pamella's physical appearance, she is about 5 feet 7 inches in height and 57 kg in weight. Her hair color is brown and her eyes color is also brown. She has acquired a stunning and captivating figure. Her body measurements are around 32-24-34.
Megha Karpe Wiki, Biography, Age, Height, Boyfriend & More
Tara Mckillop Wiki, Biography, Age, Height, Family,…
Pamella Roland Career
Upon obtaining a graduate degree, Pamella began working in marketing and public relations, in both corporate and agency environments. There she served for around 10 years and decided to turn her career into fashion designing. In 2002, she launched her first collection in New York Fashion Week, which caught the attention of people as well as high-profile celebrities. Subsequently, as a fashion designer, Pamella was approached by a number of reputed celebrities like Aira Ferreira, Carrie Underwood, Jennifer Garner, Angelina Jolie, and Eva Longoria. Since then, Pamella become one of the renowned fashion designers over the world.
Pamella Roland with Paris Hilton and Nicky Hilton
By using her fame, Pamella founded her self-titled evening wear line and got more fame and publicity. Her line was praised by several reputed personalities. Additionally, she has been featured in Vogue magazine and other publications. Likewise, she was interviewed by several publications by Forbes.
Pamella Roland Instagram / Twitter
Other than fashion designing, Pamella is active on social media as well. She gas gathered thousands of followers on Instagram for sharing pictures of a variety of outfits designed by herself. Likewise, she is active on Twitter since March 2010.
A post shared by pamella roland (@pamellaroland)
Pamella Roland Net Worth
The American fashion designer and Instagram star Pamella is how rich? Till now, she never disclosed anything about her wealth or earnings. As per our researches and the sources available on the internet, it is said that Pamelle's current net worth is approx $900k USD. While her major sources of income are fashion designing and business endeavors. As her career is active, it is expected that her net worth will be increased in the future.
Net Worth $900k USD
Pamella Roland Family
Pamella took birth in a middle-class Christian family in Michigan of United States. Right now, we do not have any information about her parents or siblings, as Pamella is very secretive about her personal life. But don't worry guys, if we get any information regarding her family we will definitely update it on the site.
Pamella Roland with her husband Dan DeVos
Pamella Roland Husband / Son
Being a celebrity, People are seeking to know about Pamela's professional life as well as her personal life. Pamella is a married woman. She tied her knot with American businessman and sports executive Dan DeVos. Together, they have three kids named Sydney DeVos, Cole DeVos, and Cassandra Thornhill. All of her family members have appeared on her Instagram account.
Pamella Roland with her son Cole DeVos
Pamella hails from Michigan, United States.
She is a prominent fashion designer and Instagram star.
Pamella found fame as a fashion designer.
She has acquired thousands of followers on Instagram.
Pamella looks stunning, captivating, and attractive.
She enjoys traveling and has traveled to Spain, Japan, and other scenic places.
She is also an animal lover and has a pet dog.
Instagram pamellaroland
Twitter pamellaroland
Don't miss to read more about Stacy Thiru and Meowckenzie.
Favorite Color Blue
Favorite Destination Sweden
Favorite Actor Tom Hardy
Favorite Actress Ane Hathaway
Favorite Sports Tennis
Favorite Sportsperson Serena Willams
Does Pamella Roland, Consume Alcohol? Yes.
Does she know cooking? No.
Does Pamella Roland go to the gym? Yes.
Does she, Smoke? No.
Does she know driving? Yes.
Does Pamella Roland, Swims? Yes.
Is he a Yoga Practitioner? Yes.
What is the age of Pamella Roland?
The age of Pamella Roland is 63 years (as of 2022).
When is the Birthday of Pamella Roland?
Pamella Roland's birthday is on January 2, 1959.
How tall is Pamella Roland?
Pamella Roland is 5′ 7" tall.
Where is Pamella Roland from?
Pamella Roland is from Michigan, United States.
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redpajama_set_name: RedPajamaCommonCrawl


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Princess Eugenie Quietly Moved Out of the Sussexes' House After Alleged Drama with the Cambridges
Looks like Princess Eugenie and her family have quietly moved out of Frogmore Cottage and into Nottingham Cottage, per The Express.
Princess Eugenie, her husband Jack Brooksbank, and their son August, had been living at Frogmore Cottage since Meghan Markle and Prince Harry (who lease the home!) left the United Kingdom. But, apparently, Eugenie and Jack quietly relocated this past summer, choosing Nottingham Cottage as their new royal residence. (FYI, they're also spending part of their time in Portugal for Jack's job.)
Nottingham Cottage (an ultra-cozy two bedroom) is situated on the Kensington Palace grounds, and also has a connection to the Sussexes. In fact, it's where Harry lived while he and Meghan were dating, and where he proposed. Meanwhile, Prince William and Kate Middleton also briefly lived in Nottingham Cottage with bb Prince George while their palace apartment was being renovated.
Princess Eugenie's move comes after her family's initial plan to relocate from Frogmore Cottage to Adelaide Cottage was dashed. You know, thanks to the fact that Prince William and Kate Middleton moved into Adelaide Cottageinstead, which, apparently, lead to some tension between the families.
The Daily Mail spoke to sources "close to the Yorks" at the time, who said Princess Eugenie had "been trying to secure" Adelaide Cottage "for when she moves out of Frogmore." They also added that "before Andrew's most recent scandal, it was definitely a property he was [also] trying to secure for his daughter."
Prior to the Cambridges moving in, the Daily Mail noted that there was "no doubt" they'd get the home due to Prince William being heir to the throne…which they did!
ORDER A COPY OF ROB'S NEW BEST SELLING BOOK! Called "America's Number ONE Gossip Columnist" by The National Enquirer. Rob 'Naughty But Nice' Shuter breaks celebrity news every day on his website NaughtyGossip.com where he delivers all the dish about the stars we love in his naughty but nice signature style. You can also catch him co-hosting and breaking celebrity news on Good Day New York, The Today Show, The Talk, Wendy Williams Show, CNN, Extra and Z100's 'Elvis Duran.' Previously, Rob was the Huffington Post's only celebrity columnist and the former executive editor of OK! Magazine. Rob has also hosted his own Saturday night talk show on Mark Cuban's channel and his own daily morning show, 'The Gossip Table,' on VH1! Breaking some of the biggest entertainment stories, including Jamie Lynn Spears's pregnancy news, Britney's first post-meltdown interview, Eva Longoria's wedding, and baby exclusives for Jessica Alba, Tori Spelling and Mathew McConaughey's tots, Rob always knows where to find the best scoop. Before Rob was one of the world's most successful entertainment reporters, he was a publicist working for Jennifer Lopez, Alicia Keys, P. Diddy, Jessica Simpson and Jon Bon Jovi! Now he is bringing all this experience to his new show on I HEART MEDIA in his unique cheeky way, that is always a pinch and never a punch!
Filed Under: Uncategorized Tagged With: PRINCE WILLIAM


Thoughts Wanted: Share Your Ideas in our Thoughtexchange!
Over the past several months under the direction of the Board of Education, we have been working on a plan to maintain the infrastructure of our schools and improve the instructional spaces of our facilities for the future. As a result, the Board is considering future borrowing through what we aim to be a tax neutral bond.
Today, we will launch an online Thoughtexchange intended to hear your priorities and collect data from parents, faculty, students, and our residents to help us learn what we can do to ensure that the projects we choose going forward are aligned with what matters most to our community members to better serve our students.
So that the voices of everyone are heard, we want to hear from the entire community!
A Thoughtexchange is an interactive, confidential conversation that allows participants to share their own thoughts (priorities) and react to the thoughts that others have provided in an anonymous and fluid way. It is an innovative way for us to survey your thoughts and opinions as we seek to narrow the focus of any potential projects.
Participants are encouraged to come back to the conversation throughout the live period to share more thoughts as they think of them and rate new thoughts that others have shared. When the live period ends on February 8, 2019, we will be able to see where the top priorities of the community rest.
This link will be active until February 8, 2019 and all data collected will be reviewed by myself, district administration and our Board Trustees. Once completed, the results will be shared with the community.


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Common Reader
The Alabama Boy Makes Good	Hank Aaron, legend of the Negro world.
Gerald Early
Essays, Features
The New Year Issue
When I was six years old my sister, who was nearly three years older, gave me my first lesson in Major League Baseball by teaching the line-up of the Milwaukee Braves. She liked the Braves I suppose because at the time, the glory years of the late 1950s, they were a pennant-winning team. She may have liked them as well because they had a star Black player, Hank Aaron. The Philadelphia Phillies did not and would not until the coming of Dick (Richie) Allen in 1964, the year of the Philadelphia Columbia Avenue race riot and the Great Collapse in the final twelve games of the season. (Allen died on December 7, 2020, and I will have much more to say about him in a future issue of The Common Reader.) I guess that is why my sister favored the Braves for the brief instance that she had an interest in professional baseball—a winning team with a star Negro player, as it would have been expressed at the time—but I really am not sure. I know she also liked the word "Milwaukee." It sounded funny, like Schuylkill.
When I saw Aaron on a baseball card my sister had, I liked him but I liked his uniform more. I just loved those old Milwaukee Braves uniforms with the tomahawk and the Indian icon, the thin red stripe circling the collar. The name itself, Braves, made me think of young, tough warriors. I did not know what a "Phillie" was and whatever it was seemed lame. What I remembered most about what my sister taught me was that the Braves had two great hitters, outfielder Aaron and third baseman Eddie Mathews, who would eventually manage Aaron in the later part of Aaron's career and was protective of Aaron in the outfielder's early days. One Black and one White. This struck me as a wonderful thing and baseball became for me this island of civility where Blacks and Whites played together, worked together, lived together (for the season, at least). Baseball was a world apart from the world I actually lived in. Baseball was the world where I wanted to live. This made baseball special for me and my Negro boyhood friends and we identified with both the Negro and White players. After all, we played baseball with the White boys in the neighborhood (more often against them but not always). Baseball, for us, was America, or what we hoped it was.
When I saw Aaron on a baseball card my sister had, I liked him but I liked his uniform more. I just loved those old Milwaukee Braves uniforms with the tomahawk and the Indian icon, the thin red stripe circling the collar.
(As I learned as a teenager, Mathews really could not protect Aaron in some respects, from the "good old boy," "unreconstructed," dumb carouser-types on other teams who were, shall we say, a bit ambivalent about the integration of baseball, the type of White players on the Braves that Mathews referred to as his "Asshole Buddies."¹As Aaron noted in the early 1960s, "Pitchers have knocked me down a lot, and sometimes, it goes through my head that they're throwing at me because I am a Negro. What makes me think so is that Eddie Mathews is just as much a hitter as I am, and I've batted right behind him for nine years now and have never seen him knocked down."² Mathews may have never been knocked down because he was White, but not quite for the reason of being White per se. He was probably never knocked down because everyone in the league knew that Mathews would knock the offending pitcher on his ass if he threw at him. Mathews had a reputation for not "taking shit" on the field and he was tough enough to back it up. He was what is called in hockey an "enforcer." Aaron could not do that, even if he were inclined temperamentally or emotionally to do so and tough enough. That kind of behavior, intimidation, from a Black player would have been far less tolerated. A White player's privilege, you might say. A Negro player had to stand up to intimidation without seeming a source of it. I was just an anonymous colored boy in those days and it took me a while to learn these things.)
I went to Connie Mack Stadium, Shibe Park to the older generation, fairly often as a kid, not to see the Phillies but to see the opposing team, especially the Dodgers (to see Sandy Koufax and Don Drysdale pitch), the Pirates (to see outfielder Roberto Clemente), the Giants (to see Willie Mays and the majestic Juan Marichal), and the Braves (to see Aaron but also to see pitcher Warren Spahn and Eddie Mathews). I saw Aaron hit a home run at a game I attended. I will never forget how hard he hit the ball, and how effortless and graceful his swing. Oh, those magical wrists of his! I imitated that swing for a while when I played youth baseball. It made my wrists and forearms ache. That did not dissuade me. I finally stopped when one of the coaches said I would hit better if I stopped doing a poor imitation of Aaron. My hands were big, so he would yell at me to just use my hands to hit, not my wrists. "Don't lead with your wrists," he would shout, "Just let your wrists follow your hands." He was right. When I stopped imitating Aaron, I did hit better. I guess Aaron's way of hitting worked for Aaron and probably nobody else, certainly not for star-struck kids of small talent like me. That is the way it is with great hitters, sui generis.
As I remember, Mays was much more publicized when I was growing up than Aaron because he was a more flamboyant player. Aaron never seemed as if he were playing very hard; Mays seemed a whirling dervish. If Mays had been an actor, he would have been the worst scene-stealer in history. For a time, everyone thought that if any player from the post-Jackie Robinson era was going to break the career home run record, it would be Mays. Even Frank Robinson was talked about more than Aaron, especially when he won the MVP in the National League in 1961, and in the American League in 1966. Aaron won the MVP only once. To underscore the magnitude of Robinson's second MVP, he also won the Triple Crown that year. Aaron never won a Triple Crown. During a game, Robinson, a very fiery, hard-charging ballplayer, was once knocked unconscious by Aaron's teammate Mathews, the hard-drinking, two-fisted "enforcer," for being a bit too fiery while running the basepaths to break up a double-play. (Robinson would claim that he "won" the fight because his team won the game. He continued to play despite the beating.) Aaron was never knocked out by any opponent because he was a cooler player, a cool player. And everybody knows that while some like it hot, most like it cool. So, the "hot" Robinson was the talk of the town, until Aaron the cool started getting close to Ruth's home run record. But Mays petered out, his body ran down quicker, his road to the record was harder. Aaron, the less emphatic but no less determined ballplayer, outlasted Mays.
I will never forget how hard he hit the ball, and how effortless and graceful his swing. Oh, those magical wrists of his! I imitated that swing for a while when I played youth baseball. It made my wrists and forearms ache. That did not dissuade me.
To break the record was a sign of longevity and the persistent excellence of the gifted who knew how to work the gift with care; it was also luck not to have been injured to such an extent as to have missed a great deal of playing time. Aaron had endurance, good genes, could stay in the line-up and produce which, of course, kept him in the line-up. A vicious cycle that circles around you, as Yogi Berra might have said. It was even good for Aaron not to have played for a team that was consistently competing in the World Series. After 1957 and 1958, the Braves never played in the World Series again while Aaron played for them. They were bounced in three straight games in the 1969 National League playoffs by the Amazin' Mets. The Braves, in the 1960s, were an underachieving team. They were not hungry enough. Strong hitters, weak pitching, indifferent managing. Aaron was under the radar a bit and I think this may have helped him, a less intense spotlight. Also, when the Braves moved to Atlanta in 1966 in what was a messy divorce from Milwaukee, Aaron was aided by the fact that Fulton County Stadium was an easier place to hit home runs. Mays was penalized by the fact that the Giants moved to San Francisco in 1957 and Candlestick Park was a much harder place to hit home runs, a cold, wind tunnel of a stadium. Once I heard a story that Mays clobbered a ball at Candlestick that was a sure home run but it got caught up in the crosswinds of the stadium and wound up being caught by the second baseman in short center field. Athletic contests are won by skill, will, and luck. And athletic records are made the same way. To break the record, Aaron had to pace his decline. How long can you outrun losing what you had? That is what it comes down to for an athlete to bring a longevity record like career home runs.
When I was older, a young teen, and much more knowledgeable about professional baseball, the men in the barbershop where I got my hair cut would sometimes talk about the current Negro stars: at the time, Robinson, Mays, Tommy Davis, Jimmy Wynn, Maury Wills, Mudcat Grant, Wes Covington, Willie McCovey, Billy Williams, and of course Aaron. Everyone was assessed against Jackie Robinson or against some guys from the Negro Leagues I never heard of like Luke Easter, Sam Jethroe, Buck Leonard, Oscar Charleston, Martin Dihigo, and some other "blasts from the past" as far as I was concerned. "Who the heck are those guys?" was what all us youngbloods thought. "There ain't no Negro Leagues anymore, why do they keep bringing that junk up for?" One barber once said, "Aaron's good for a lazy Alabama boy. He can get away with that 'cause he playin' with them White boys. They'd be on his ass if he was still in the Negro Leagues." I never forgot that. I did not understand it at the time. How could these guys heckle a great player like Aaron, then a bunch of colored barbers who did not know anything, who did not even know how to cut or process hair right, as I saw it? Later, I realized it was a way of acknowledging Aaron's greatness, a kind of hazing that a lot of Negro sports fans of that generation did, holding up the Negro Leagues as a kind of excellence because we had so few standards of excellence that we could call our own. Playing in the Negro Leagues was like going on the bandstand for a jam session with Bird, Diz, Bud Powell, and Max Roach. You had to know the changes or be told to sit down. There was no room for what Diz called "no-talent guys." To be excellent, to be gifted, was to be a hero. And Negroes then rode their heroes like overworked thoroughbreds, from ready to ruin. When Aaron got close to Ruth's record, several years later when I was in college, the same barber said, "I'm pulling for Aaron. I hope he busts that record so bad that ain't nobody gonna be near it again. I hope he breaks that record and breaks all the White people's hearts."
Playing in the Negro Leagues was like going on the bandstand for a jam session with Bird, Diz, Bud Powell, and Max Roach. You had to know the changes or be told to sit down.
Aaron was probably the second most important Black athlete of the 1960s. Only Ali was more significant, and more flamboyant. In Jackie Robinson's book of interviews about the integration of Major League Baseball, Baseball Has Done It (1964), Aaron mentions that he had read James Baldwin. "I've read some of James Baldwin's books. He is a very good author with very good ideas. I haven't read The Fire Next Time, but a friend of mine talked to me about it. Baldwin says we've waited long enough."³ As a kid, I was impressed with that. It was news to me that Negro athletes thought about such things, they being rich and famous and all that and not really like the rest of us. I was a colored boy and learning.
The mostly White sportswriting establishment, "woke" to the max, began a great deal of pious braying after Aaron died that he was the true home run king and not the cheating, steroid-fueled Barry Bonds. I have mentioned elsewhere how much this sort of thing sounds like Aaron is the good Negro and Bonds is the bad Negro. Whites have always loved doing this, deciding which Negroes they approved of as the Negroes who were a credit "to the game," in Aaron's case, which is like being "a credit to your race." Even in this so-called "woke" age, as some think of it, Whites continue to define Negroes as they did 150 years ago. The more things change, as they say, the more they remain the same. This might lead some to think that racism and anti-racism in some respects, to borrow the language of avant-garde bandleader Sun Ra, "are really the same upon different degree." But forgive me if I seem to be provocative for provocation's sake.
Aaron was an incredible player. He lived a long life. And he got his due, his accolades, his recognition, while he was alive. That is good. I wonder if a great athlete who breaks a record thinks, in the words of Cole Porter, "Is it for all time or simply a lark?" What does it mean to be remembered? So many players from the Negro Leagues never did get their due. When I was a kid only those older men who had gone to Negro League games as boys and young men remembered. Those barbers from my boyhood knew more than some ignorant kid like me and that is why they said what they said. They knew more about what it meant to be colored than I ever would.
¹ John Klima, Bushville Wins! The Wild Saga of the 1957 Milwaukee Braves and the Screw balls, Sluggers, and Beer Swiggers Who Canned the New York Yankees and Changed Baseball, (New York: Thomas Dunne Books, 2012), Chapter 3.
² Jackie Robinson, Baseball Has Done It, (Brooklyn: Ig Publishing, 2005), 135.
³ Jackie Robinson, Baseball Has Done It, (Brooklyn: Ig Publishing, 2005), 13.
Gerald Early, editor of The Common Reader and a fellow of the American Academy of Arts and Sciences, is Merle Kling Professor of Modern Letters, professor of English and of African and African-American Studies, both in Arts & Sciences, at Washington University in St. Louis.
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Ogbemudia Congratulates President-Elect
Two-time Governor of Bendel and Mid-West Region Dr. S O Ogbemudia has congratulated the President Elect Gen. Muhammadu Buhari on his Victory.
In a statement he personally signed and made available to Sunday Observer yesterday, General Ogbemudia said he had known the president elect since 1963 when he was commissioned into the Nigerian Army.
"I had the privilege to see some of his confidential reports written by his commanders in which he was described as a young officer with boundless energy, and willing to continue when others are tired.
"The Energy and resilience he has truly demonstrated in politics by winning a historic election at the fourth attempt. I am confident he will lead Nigeria into a remarkable era".
To the defeated PDP, Dr. Ogbemudia urged its leadership to see the loss as an opportunity to begin to demonstrate capacity as a viable and credible alternative in the service of the nation. "A peep into what went wrong is called for"; he counseled
He described the conduct of President, Dr Goodluck Jonathan in conceding defeat as a demonstration of both sportsmanship and statesmanship stressing that the verdict of history will be favourable to him.


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text:
Q: Submit form on select change This is my code: http://jsfiddle.net/47apf/
It should submit the form on select change but it doesnt do anything
$(function() {
    $('#candidate_filter').change(function() {
        this.form.submit();
    });
});

Can anyone please explain why this code doesn't work?

A: Well, you don't need the .form in this case.
$(function() {
  $('#candidate_filter').change(function() {
    this.submit();
  });
});

A: Here, this itself is the form.
Write this:
$('#candidate_filter').change(function() {
    $(this).trigger('submit');
});

Updated fiddle here.

A: Try this
$('#candidate_filter').change(function() {
        //alert("hii");
        this.submit();
    });

Fiddle: fiddle

A: You need to assign id of drop down as below:
    <form id="candidate_filter">
    <select name="vacancy" id="candidate_filter1">
    <option value="all">Any Vacancy</option>
    <option value="1">Engineering lk;lk;</option>
    </select>
    <select name="status" id="candidate_filter2">
    <option value="all">Any Status</option>
    <option value="open">Open for applications</option>
    <option value="closed">Closed for applications</option>
    <option value="inactive">Inactive</option>
    </select>
    <select name="date">
    <option value="all">Any Date</option>
    <option value="today">Today</option>
    <option value="3">3 days</option>
    <option value="7">This week</option>
    </select>
    <select name="consideration" id="candidate_filter3">
    <option value="all">Any Consideration</option>
    <option value="qualified">Qualified</option>
    <option value="rejected">Rejected</option>
    </select>
    <input type="submit">
    </form>

JS
    $(function() {
        $('select[id^="candidate_filter"]').change(function() {
            this.form.submit();
        });
    });

DEMO

A: You have to submit the form like this:  $('#candidate_filter').submit();
Here is a working JSFiddle: http://jsfiddle.net/47apf/5/
JQuery
$(function() {
    $('#candidate_filter').change(function() {
        alert("change event catched");
         $('#candidate_filter').submit();
    });
});

A: You can do like this in jQuery.
Put a class on your select, and bind the event onchange
 $('.candidateList').on('change', function(evt){
    $('#candidate_filter').submit();
});

http://jsfiddle.net/darksioul/4ygAg/2/

A: Try:
$(function() {
    $('#candidate_filter select[name="vacancy"]').change(function() {
        $('#candidate_filter').submit();
    });
});

Inside jQuery selectors, the this word references to the selected element on DOM, in you original code, $('#candidate_filter') represents the FORM element. Adding a second reference you have a better approach to what you desire $('#candidate_filter select[name="vacancy"]'). And to submit the form, you need to point especifically to the FORM element.

redpajama_set_name: RedPajamaStackExchange


is designed for switching high frequency signals of frequency range up to 10 GHz from one switch input to four switch outputs or from four switch inputs to one switch output.
Designed for power control on active and active-inductive loads: heaters, light bulbs, commutator motors.
Designed for power control in active and active-inductive loads: heaters, light bulbs, commutator motors.


2018-01-18: dump_20180118_0910.json (4,17 MB): This is a very first dump of the citation data we generate in our project. It is not in RDF format, but serves as example showing the qualitity of the citation links. It contains 985 bibliographic resources, with a total of 10,905 references among which 951 are resolved.


text:
Q: Add Table Row Using jQuery - MVC 4 I am currently trying to implement an Add functionality to my page. Currently, the add is already functioning but I have to refresh the page in order for the newly added row to appear on the table.
Please see my codes below:
This is how I generate my table:

    ProductID
    ProductName
    Price
    Action

@foreach (var item in repository.GetAllProducts(ViewData["BranchCode"].ToString()))
{

    @item.ProductID
    @item.ProductName
    @item.Price
    @Html.ActionLink("Edit", "Edit", new { RecordID = item.RecordID }, new { @class = "editLink" })
    @Html.ActionLink("Delete", "Delete", new { RecordID = item.RecordID }, new { @class = "editLink" })

}

Currently, the edit and delete are already functioning well. Below is how I do the edit:
function update(data) {
if (data.Success == true) {
    var parent = linkObj.closest("tr");

    parent.find(".ProductID").html(data.Object.ProductID);
    parent.find(".ProductName").html(data.Object.ProductName);
    parent.find(".Price").html(data.Object.Price);
}
else {
    $("#update-message").html(data.ErrorMessage);
    $("#update-message").show();
}

}
Now I am trying to implement an add functionality which is almost the same as the edit jquery i am using. I have tried using the .append method unsuccessfully.

EDIT:
I have tried using the code below for the add. But it doesn't seem to do anything. Or perhaps I'm doing something wrong:
    function add(data) {
    if (data.Success == true) {

        var rowTemplate = $("#rowTemplate").html();
        var tbl = document.getElementById("ProductsTable");
        var counter = $("#ProductsTable tr").length;
        data.Counter = counter;
        $("#ProductsTable").append(applyTemplate(rowTemplate, data));

    }
    else {
        $("#update-message").html(data.ErrorMessage);
        $("#update-message").show();
    }
}

function applyTemplate(template, data) {
    var str = template;
    if ($.isPlainObject(data)) {
        $.each(data, function (index, value) {
            var find = new RegExp("\\$1" + index, "ig");
            str = str.replace(/\$/g, "\$1");
            str = str.replace(find, value);
        });
    }
    return str;
}

It makes use of a row template such as the following:

I just found this solution online but I can't make it to work. I also tried the code below (i just made up based on the edit jquery I have):
    function add(data) {
    if (data.Success == true) {
        var parent = linkObj.closest("tr");
        parent.find(".ProductID").append(data.Object.ProductID);
        parent.find(".ProductName").append(data.Object.ProductName);
        parent.find(".Price").append(data.Object.Price);
    }
    else {
        $("#update-message").html(data.ErrorMessage);
        $("#update-message").show();
    }
}

EDIT:
Right now, this is how my jQuery looks like:
function add(data) {
    if (data.Success == true) {
        data = { Counter: 3 };
        $("#rowTemplate").tmpl(data).appendTo("#ProductsTable");
        $('#updateDialog').dialog('close');
    }
    else {
        $("#update-message").html(data.ErrorMessage);
        $("#update-message").show();
    }
}

and this is my template:

Thanks to Sir @Muhammad Adeel Zahid for helping me make the jQuery work to add rows. However, it only adds a new row to my table. What I need now is to make it add the values I have from the data object in the add function of the jQuery.
I have tried following the tutorial from THIS LINK but I can't seem to make it work. My code is below:
function add(data) {
    if (data.Success == true) {
        var prod = $.map(data.results, function (obj, index) {
            return {
                ProductID:  obj.text,
                ProductName: obj.text,
                Price: obj.text
            };
        });

        prod = { Counter: 3 };
        $("#rowTemplate").tmpl(prod).appendTo("#ProductsTable");
        $('#updateDialog').dialog('close');
    }
    else {
        $("#update-message").html(data.ErrorMessage);
        $("#update-message").show();
    }
}

Thanks a lot for helping!

A: I think there is something wrong with your template code. Please try changing it to

and then generate html from it like
var obj = {Counter:3};
$("#rowTemplate").tmpl(obj).appendTo("#ProductsTable");

Edit
First I thought you were using jquery template engine and my answer was based on that assumption. you can find how to use templating engine here. Please see that i have also edited the type field in

Note how you add placeholders ${Variable} in the templates. Now when you need to use the template, you will need a json object with properties matching the variables used in the template. For example to use above template, I would do something like
var obj2 = {ProductId:2,ProductName:'First Product', Price: 323};//note the properties of json and template vars match.
$("#rowTemplate2").tmpl(obj2).appendTo("#somecontainer");


text:
\section{INTRODUCTION}

Conservation laws are intimately related to the symmetries of the
underlying space-time. Killing vector fields which generate local
isometries play a prominent role in constructing the usual conserved
currents and a conserved charge is associated with each such a
current. In an $n$-dimensional space-time, by making use of the
asymptotic symmetries, an ADM conserved charge \cite{Adm} can be
written as an integral over $(n-2)$-spheres at spatial infinity
\cite{Abbott-Deser}. For example, time translation Killing vector
field defines the ADM mass and rotational Killing vector fields
define the ADM angular momenta. Antisymmetric generalizations of
Killing vector fields to higher order forms are called Killing-Yano
(KY) forms. These reflect the hidden symmetries of the metric and
can be used in generalizing the conserved currents to $p$-brane
space-times that are extended objects with $p$ spatial dimensions
\cite{Kastor}. For the most recent and for the earlier seminal
references about KY (and conformal KY) forms we refer to three
recent PhD dissertations \cite{Kress,Semmelman2,Kubiznak}.

Abbot-Deser (AD) construction of conserved charges
\cite{Abbott-Deser} can be extended to KY-forms and in such a case
the associated generalized charges are called Y-ADM charges. These
are constructed for asymptotically flat and asymptotically anti-de
Sitter space-times \cite{Kastor,Cebeci}. In ADM case, the charges
can be written in terms of Einstein forms and therefore they can be
related to stress-energy forms via Einstein equations. The physical
meanings of these charges are obtained from this relation. On the
other hand, for the generalized charges, there is no direct relation
with Einstein equations and hence their physical interpretations are
not yet clear. The ADM charges are extensive quantities since they
are obtained from integrals over the $(n-2)$-spheres at infinity
which enclose $(n-1)$-dimensional regions. However, a Y-ADM charge
associated to a KY $p$-form is calculated from the integrals over
$(n-p-2)$-spheres at spatial infinity along the directions
transverse to the $p$-brane. Since these spheres constitute the
boundaries of $(n-p-1)$-dimensional regions, the corresponding
charges are intensive quantities. This makes it possible to
interpret Y-ADM charges as charge densities for $p$-brane
space-times.

A conventional way of defining a conserved current and the
corresponding conserved charge in an $n$-dimensional space-time can
be described as follows. Suppose that a $p$-form $J$ satisfies
$d^{\ast}J=0$, where $d$ stands for the exterior derivative and
$^{\ast}$ denotes the Hodge map. Then, by the Stokes theorem the
integral of $^{\ast}J$ over the boundary of a $(n-p+1)$-dimensional
region vanishes. This means that $J$ is a conserved current and by
integrating $^{\ast}J$ over an arbitrary $(n-p)$-dimensional region
$\Sigma$, we can define the corresponding charge by
$Q=\int_{\Sigma}{}^{\ast}J$. $Q$ is a conserved charge in the sense
that it is a constant for all regions sharing the same homology
class with $\Sigma$. A $p$-form $J$  is co-closed if and only if
$\delta J=0$, where $\delta$ represents the co-derivative operator
defined below. Noting that the co-closedness of $J$ is equivalent to
the condition $d^{\ast}J=0$, the above remarks can be generalized as
follows: any co-closed $p$-form is a conserved current and the
corresponding conserved charge is defined as prescribed above.

Evidently, all linear combinations of conserved quantities are
trivially conserved and therefore a conservation law must be related
to a basic current that can not be constructed from others.
Physically meaningful conserved charges must also be constructed
from the basic currents. In two recent papers \cite{Kastor,Cebeci},
it has been shown that the $p$-form
\begin{eqnarray}
{\cal J}=-i_{X_{a}}i_{X_{b}}\omega\wedge R^{ab}+2(-1)^p
i_{X_{a}}\omega\wedge P^{a}+\cal{R}\omega\;,
\end{eqnarray}
constructed from a KY $p$-form $\omega$ (for definition see equation
(5)) and curvature characteristics is a generalized conserved
current and can be related to a conserved charge of a $p$-brane
space-time. Throughout this study we assume the Einstein summation
convention over repeated indices and we use $i_{X}$ to denote the
interior derivative with respect to the vector field $X$. In the
expression (1), $R^{ab}$ are the curvature 2-forms and
\begin{eqnarray}
P^{a}=i_{X_{b}} R^{ba}\;,\quad {\cal R}=i_{X_{a}}P^{a}\;,
\end{eqnarray}
denotes, respectively, the Ricci 1-forms and the curvature scalar.
The current ${\cal J}$ is an attempt to generalize the well-known
($1$-form) current $K_{a}{}^{\ast^{-1}}G^{a}$ which is constructed
from the components of a Killing vector field $K$ and Einstein
$(n-1)$-forms $G^{a}=R_{bc}\wedge^{\ast}(e^{abc})$. Here
$^{\ast^{-1}}$ denotes the inverse of the Hodge map which is defined
as $s(-1)^{p(n-p)}$ ($s$ is the sign of the determinant of metric)
times the Hodge map when acting on $p$-forms.

In this study we will show that two fundamental currents can be
constructed from KY-forms and curvature characteristics of the
underlying space-time and prove that ${\cal J}$ given by (1) is a
particular linear combination of gravitational currents proposed
here. We furthermore show that one of the currents is co-exact which
enables us to discover a number of basic geometric facts some of
which seem to be unknown in the literature. These facts can be
stated as follows. (i) The scalar curvature of any
(pseudo)Riemannian manifold is a flow invariant for all of its
Killing vector fields. (ii) The conserved currents directly provide
decompositions for differential forms constructed from
``contractions" of KY $p$-forms with the Ricci $1$-forms, curvature
$2$-forms and with the Einstein $(n-1)$-forms (for the values
$p=1,2$ and $p=n-1$). These contractions are expressible solely in
terms of KY-forms themselves and their (co)derivatives. (iii) On
Einstein manifolds, duals of all Killing and Yano vector fields are
eigenforms of the Laplace-Beltrami operator such that the
eigenvalues have multiplicities with well defined lower bounds. Some
well known facts related to the spectrum of Laplace-Beltrami
operator on constant curvature manifolds also follow directly from
the properties of conserved currents.

From here on we assume that the underlying manifold is an
$n$-dimensional (pseudo)Riemannian manifold with arbitrary
signature. Some of our conventions and notations are fixed above for
which, as well as for the remaining ones, we have mainly adopted the
conventions of reference \cite{Benn-Tucker}. The covariant
derivative with respect to a given vector field $X$ will be denoted
by $\nabla_{X}$ in terms of which the exterior derivative and
co-derivative can be expressed as
\begin{eqnarray}
d=e^{a}\wedge\nabla_{X_a}\;,\quad \delta=-i_{X^{a}}\nabla_{X_a}\;,
\end{eqnarray}
where the local co-frame $\{e^{a}\}$ is dual to the tangent frame
$\{X_{a}\}$ such that $i_{X_{b}}e^{a}=e^{a}(X_b)=\delta^{a}_{b}$.
The action of  $i_{X}$ on an arbitrary $p$-form $\alpha$ is defined,
for all vector fields $Y_{j}$, by
$(i_{X}\alpha)(Y_1,\dots,Y_{p-1})=p \alpha(X,Y_1,\dots,Y_{p-1})$.
When acting on an arbitrary $p$-form $\delta$ can be written as
$(-1)^{p}\;^{\ast^{-1}}d^{\ast}$.

The rest of the paper is organized as follows. The definitions of
two basic (uncomposite) currents and the proofs of co-exactness of
the one and co-closedness of the other are given in the next
section. Three main operators that play important role in our study
are also introduced there and their relevant properties are
presented. The basic $p$-form currents for the values
$p=1,\;n-2,\;n-1$, are studied in Section III where some of the
general geometric facts, such as the statements (i) and (ii) given
above, are explored as well. Conserved currents on some special
manifolds, such as Ricci flat, conformally flat and constant
curvature manifolds as well as Einstein manifolds, are considered in
Section IV. A brief summary of the study and some concluding remarks
are given in the last section. Contracted Bianchi identities that
play prominent role in the proof of the co-closedness of a basic
current are collected in Appendix A and an alternative proof for the
statement (i) given above is provided in Appendix B.

\section{Two Basic Conserved Currents}

We begin by defining three $p$-forms
\begin{eqnarray}
j_{1}&=&i_{X_{a}}i_{X_{b}}\omega\wedge R^{ab}\;,\nonumber\\
j_{2}&=&i_{X_{a}}\omega\wedge P^{a}\;,\\
j_{3}&=&\cal{R}\omega\;,\nonumber
\end{eqnarray}
for a given KY $p$-form $\omega$. A $p$-form $\omega$ is called a KY
$p$-form if and only if
\begin{eqnarray}
\nabla_{X}\omega=\frac{1}{p+1}i_{X}d\omega\;,
\end{eqnarray}
is satisfied for all vector fields $X$. Two immediate consequences
of this definition are that, all KY-forms are co-closed and satisfy
the relation $i_{Y}\nabla_{X}\omega+i_{X}\nabla_{Y}\omega=0$, for
any two vector fields $X$ and $Y$. The second relation means that
all symmetrized covariant derivatives of KY-forms vanish. As is
evident from the definition (5), any function is a KY $0$-form and a
KY $n$-form is a constant multiple of the volume form. As
manifestations of the hidden symmetries of the metric of the
underlying space-time, co-closedness of KY-forms means that all of
them define conserved currents and corresponding conserved charges.
Apart from this well-established fact, as we are about to see, their
particular combinations with the curvature characteristics, also
give rise to important conservation laws.

The main goal of our study is to prove that the ($p$-form) currents
\begin{eqnarray}
{\cal J}_{1}&=&-j_1+(-1)^pj_2\;,\\
{\cal J}_{2}&=&(-1)^pj_2+j_3\;,
\end{eqnarray}
are separately conserved on any (pseudo)Riemannian manifold for all
$p$'s. These are the currents that were, and will be, referred to as
basic. We shall also prove that ${\cal J}_{1}$ is co-exact and
elucidate its important geometrical and physical implications.
Evidently all linear combinations of ${\cal J}_{1}$ and ${\cal
J}_{2}$ are also conserved and the conservation of (1) is a
particular case of this fact since ${\cal J}={\cal J}_{1}+{\cal
J}_{2}$. These enable us to define more conserved charges and of
course physically meaningful and fundamental ones must be directly
constructed from ${\cal J}_{1}$ and ${\cal J}_{2}$. Finally, we
should note that (6) and (7) can be rewritten more compactly as
\begin{eqnarray}
{\cal J}_{1}=i_{X_{a}}(i_{X_{b}}\omega\wedge R^{ba})\;,\quad {\cal
J}_{2}= (-1)^pi_{X_a}(\omega\wedge P^{a})\;.
\end{eqnarray}
These clearly exhibit that for all KY $0$-forms (for all functions)
while ${\cal J}_{1}$ is identically zero, ${\cal J}_{2}$ is equal to
$j_3$ and that both currents are identically zero for KY $n$-forms.
Moreover, by observing that the current (1) is
\begin{eqnarray}
{\cal J}=i_{X_{a}}i_{X_{b}}(\omega\wedge R^{ba})\;,\nonumber
\end{eqnarray}
we see that for all KY $(n-1)$-forms ${\cal J}$ is identically zero.
But, in our case the currents are non-vanishing but linearly
dependent. So, for a general (pseudo)Riemannian manifold we can
safely say that, the space of conserved currents that linearly
depend on a given KY p-form is, for $0<p<n-1$, at least two
dimensional and is spanned by ${\cal J}_{1}$ and ${\cal J}_{2}$. Of
course, in some special cases these may be linearly dependent for
some, or even for all values of $p$. For example, as we have shown
in Section IV, on the constant curvature manifolds the latter
extreme case is observed. More details in this context are given in
sections III and IV.

\subsection{Main Operators}

The following three second order differential operators
\begin{eqnarray}
\mathbf{R}(X_a,X_b)&=&\nabla_{X_a}\nabla_{X_b}-\nabla_{X_b}\nabla_{X_a}-\nabla_{[X_a,X_b]}\;,\\
I(\textbf{R})&=&e^{a}\wedge i_{X_b}\mathbf{R}(X^{b},X_a)\;,\\
\nabla^2(X_a,X_b)&=&\nabla_{X_a}\nabla_{X_b}-\nabla_{\nabla_{X_a}X_b}\;,
\end{eqnarray}
play prominent roles in this study. The first is the well-known
curvature operator of the geometry, the second is known as the
curvature endomorphism \cite{Semmelman1} and the third is the
Hessian. All of these operators are degree-preserving when acting on
differential forms. The torsion-zero condition
\begin{eqnarray}
[X,Y]=\nabla_{X}Y-\nabla_{Y}X\;,
\end{eqnarray}
of (pseudo)Riemannian geometry implies that the curvature operator
can be written as the anti-symmetric difference
\begin{eqnarray}
\mathbf{R}(X_a,X_b)=\nabla^2(X_a,X_b)-\nabla^2(X_b,X_a)\;,
\end{eqnarray}
of two Hessians. The most important property of the curvature
endomorphism is that it can also be written as the difference
$I(\textbf{R})=\nabla^2-\displaystyle{\not}d^2$ (the classical
Weitzenb\"{o}ck formula) of the trace of Hessian
$\nabla^2=\nabla^2(X_a,X^{a})$ and the well-known Laplace-Beltrami
operator
\begin{eqnarray}
\displaystyle{\not}d^{2}=-(\delta d+d\delta) \;.\nonumber
\end{eqnarray}

An important property of the Hessian that will be used in our
analysis is that its double contraction vanishes
 \begin{eqnarray}
i_{X_b}i_{X_a}\nabla^2(X^{b},X^{a})=0.
\end{eqnarray}
This can be easily proved by using the definition of co-derivative
and the general relation
\begin{eqnarray}
[\delta, i_{X}]_{+}=-i_{X^{a}}i_{\nabla_{X_{a}}X}\;,
\end{eqnarray}
where $[,]_{+}$ denotes the anti-commutator. This relation easily
follows from the definition of $\delta$ and the relation $[\nabla_X
, i_Y]=i_{\nabla_XY}$. Then by direct computation we obtain
\begin{eqnarray}
i_{X_a}i_{X_b}\nabla_{X^{b}}\nabla_{X^{a}}&=&-i_{X_a}\delta\nabla_{X^{a}}
=-{\omega^{c}}_{a}(X_b)i_{X^b}i_{X_c}\nabla_{X^{a}}\nonumber\\
&=&i_{X_{a}}i_{X_b}\nabla_{\nabla_{X^{b}}X^{a}}\;,\nonumber
\end{eqnarray}
which proves (14). Here we have used the Poincare lemma $\delta^2=0$
and $\omega^{c}_{\;a}$'s are the connection $1$-forms defined by
$\nabla_{X_{b}}X_{a}=\omega^{c}_{\;a}(X_b)X_{c}$. As an aside, from
(13) we see that the double contraction of the curvature operator
also vanishes.

\subsection{Co-exactness of ${\cal J}_{1}$}

We will show that the co-exactness of ${\cal J}_{1}$ is a direct
result of the action of curvature endomorphism on KY-forms and the
co-closedness of ${\cal J}_{2}$ also follows from action of these
operators on KY-forms and Bianchi identities. The actions of
curvature operator and curvature endomorphism on an arbitrary
$p$-form $\phi$ are as follows
\begin{eqnarray}
\mathbf{R}(X_a,X_b)\phi&=&-i_{X_{c}}R_{ab}\wedge i_{X^{c}}\phi\;,\\
I(\textbf{R})\phi&=&P_{c}\wedge i_{X^{c}}\phi-R_{cb}\wedge
i_{X^{b}}i_{X^{c}}\phi\;.
\end{eqnarray}
The first relation can easily be found in the literature (see
\cite{Benn-Tucker} equation (8.1.11) and \cite{Benn-Kress}) and the
second follows from the first. Indeed, multiplying (16) by
$e^{a}\wedge$ and using the first Bianchi identity $R_{ab}\wedge
e^{b} =0$ we find
\begin{eqnarray}
e^{a}\wedge \mathbf{R}(X_a,X_b)\phi=-R_{cb}\wedge i_{X^{c}}\phi\;,
\end{eqnarray}
and then by contracting with $i_{X^b}$ we arrive at (17). A
comparison of the right hand side of (17) with (6) shows that ${\cal
J}_{1}$ is generated by the action of the curvature endomorphism on
the KY $p$-form $\omega$ used in its definition:
\begin{eqnarray}
{\cal J}_{1}=-I(\textbf{R})\omega\;.
\end{eqnarray}

The last relation implies that the action of other operators on
KY-forms may also have important implications. It is convenient to
consider the action of Hessian first. By differentiating both sides
of the defining relation (5) we obtain
\begin{eqnarray}
\nabla^2(X_a,X_b)\omega&=&\frac{1}{p+1}i_{X_b}\nabla_{X_a}d\omega\;,\\
\mathbf{R}(X_a,X_b)\omega&=&\frac{1}{p+1}(i_{X_b}\nabla_{X_a}-i_{X_a}\nabla_{X_b})d\omega\;.
\end{eqnarray}
The second relation is obtained from (20) by virtue of (13).
Multiplying the both sides of (21) with $e^{a}\wedge$, leads us to
\begin{eqnarray}
e^{a}\wedge \mathbf{R}(X_a,X_b)\omega
=-\frac{p}{p+1}\nabla_{X_b}d\omega\;,
\end{eqnarray}
where we have used the scaling property $e^{a}\wedge
i_{X_a}\alpha=k\alpha$ that holds for any $k$-form $\alpha$. By
contracting both sides of (22) with $i_{X^b}$, we obtain
\begin{eqnarray}
I(\textbf{R})\omega=\frac{p}{p+1}\delta d\omega\;,
\end{eqnarray}
and by comparing with (19) we arrive at
\begin{eqnarray}
{\cal J}_{1}=-\frac{p}{p+1}\delta d\omega\;.
\end{eqnarray}
That is, ${\cal J}_{1}$ is a co-exact $p$-form and hence provides a
conserved current.

\subsection{Co-Closedness of ${\cal J}_{2}$}

In proving the co-closedness of ${\cal J}_{2}$ we shall need the
covariant derivatives of $d\omega$ and the contracted Bianchi
identities. Some of these identities (that can be derived from the
so-called second Bianchi identity) are not easily found in the
literature and as they are repeatedly used below, we have collected
them in the Appendix A where their derivations are given in some
details.

From (18) and (22) we directly read
\begin{eqnarray}
\nabla_{X_b}d\omega=\frac{p+1}{p}R_{cb}\wedge i_{X^{c}}\omega\;,
\end{eqnarray}
and by taking the covariant derivatives of both sides we obtain
\begin{eqnarray}
\nabla_{X_b}\nabla_{X_a}d\omega&=&\frac{p+1}{p}(\nabla_{X_b}R^{c}{}_a\wedge
i_{X_c}\omega+R^{c}{}_a\wedge \nabla_{X_b}i_{X_c}\omega)\;.
\end{eqnarray}
We now define
\begin{eqnarray}
T^{bca}&=&\nabla_{X^b}R^{ca}+\omega^{cl}(X^b){R_{l}}^{a}+\omega^{al}(X^{b}){R^{c}}_{l}\;,\\
Q^{ba}&=&T^{bca}\wedge i_{X_c}\omega\;.
\end{eqnarray}
$T^{bca}$ is thoroughly investigated in Appendix A. In terms of
$Q^{ba}$ we rewrite (26) as
\begin{eqnarray}
\nabla_{X^b}\nabla_{X^a}d\omega=\frac{p+1}{p}Q^{ba}-
\omega^{al}(X^b)\nabla_{X_l}d\omega+\frac{1}{p}R^{ca}\wedge
i_{X_c}i_{X^b}d\omega\nonumber\;,
\end{eqnarray}
and by leaving $Q^{ba}$ alone we arrive at
\begin{eqnarray}
Q^{ba}=\frac{1}{p+1}[p\nabla^2(X^b,X^a)-R^{ca}\wedge
i_{X_c}i_{X^b}]d\omega\;.
\end{eqnarray}

We are now ready to take the co-derivative of ${\cal J}_{2}$ given
by (8)
\begin{eqnarray}
\delta {\cal J}_{2}=-(-1)^pi_{X_b}\nabla_{X^{b}}i_{X_a}(\omega\wedge
P^{a})\nonumber.
\end{eqnarray}
By making use of the relation $[\nabla_X , i_Y]=i_{\nabla_XY}$, the
definition of the KY-forms and contracted Bianchi identity
$i_{X_b}P^{a}=i_{X_a}P^{b}$, we can write
\begin{eqnarray}
\delta {\cal J}_{2}&=&-(-1)^pi_{X_a}i_{X_b}(\omega\wedge
S^{ab})\;,\nonumber
\end{eqnarray}
where we have defined
$S_{ab}=\nabla_{X_{a}}P_{b}+\omega_{bk}(X_a)P^{k}$. In Appendix A,
it is shown that $S^{ab}=S^{ba}+i_{X_c}T^{cab}$ which when
substituted into above relation yields
\begin{eqnarray}
\delta {\cal J}_{2}=-\delta {\cal
J}_{2}-(-1)^pi_{X_a}i_{X_b}[\omega\wedge i_{X_c}T^{cab}]\;.
\end{eqnarray}
Thus, by making use of the cyclic property of $T^{abc}$ given by
(A12), we have
\begin{eqnarray}
2\delta {\cal J}_{2}&=&-i_{X_a}i_{X_b}[i_{X_c}(\omega\wedge
T^{cab})-i_{X_c}\omega\wedge T^{cab}]\nonumber\\
&=&i_{X_a}i_{X_b}(i_{X_c}\omega\wedge T^{cab})\nonumber\\
&=&-i_{X_a}i_{X_b}[i_{X_c}\omega\wedge
(T^{abc}+T^{bca})]\nonumber\;,
\end{eqnarray}
and the anti-symmetry property of $T^{cab}$ with respect to the last
two indices (see (A7)), we end up with
\begin{eqnarray}
\delta {\cal J}_{2}=-i_{X_a}i_{X_b}Q^{ba}\;.
\end{eqnarray}

So, the proof of the co-closedness of ${\cal J}_{2}$ has been
reduced to the vanishing of double contraction of $Q^{ba}$. We now
observe that, by virtue of (14), the double contraction of the first
term at the right hand side of (29) vanishes. For the double
contraction of the second term of (29) we obtain
\begin{eqnarray}
i_{X_a}i_{X_b}(R^{ca}\wedge i_{X_c}i_{X^b}d\omega)
&=&i_{X_b}P^{c}\wedge i_{X_c}i_{X^{b}}d\omega+i_{X_b}R^{ca}\wedge
i_{X_a}i_{X_c}i_{X^{b}}d\omega\nonumber\;.
\end{eqnarray}
Since $i_{X_b}P_{c}$ is symmetric, the first term at the right hand
side vanishes and as the cyclic sum of $i_{X^b}R^{ca}$ amounts to
zero (see (A4)), the second term vanishes as well. These prove
$i_{X_a}i_{X_b}Q^{ab}=0$ and hence ${\cal J}_{2}$ is co-closed.

\section{Special $p$-form Currents: General Geometric Facts}

In this section we study the basic $p$-form currents for the values
$p=1,\;n-2,\;n-1$, and explore some of the general implications that
follow from their conservations. Some of these implications which
hold for any (pseudo) Riemannian manifold were concisely stated in
the introduction by the statements (i) and (ii). It is worth
emphasizing that the special cases considered below exhaust all
possible cases in four dimensions. Similar investigations for some
physically  relevant special manifolds are carried out in the next
section.

\subsection{One-form Currents}

Evidently, for all KY $1$-forms $j_1$ is identically zero and
therefore, $j_2$ is co-exact. For a given KY $1$-form $\omega$ we
have $j_2=K_aP^{a}$, where
\begin{eqnarray}
K=(i_{X_a}\omega)X^{a}=K^{a}X_a \;,\nonumber
\end{eqnarray}
is the Killing vector field dual to $\omega$, and then from (6) and
(24) we obtain
\begin{eqnarray}
K_aP^{a}=\frac{1}{2}\delta d\tilde{K}\;.
\end{eqnarray}
This relation is already known in the literature (see pp.231 in
\cite{Benn-Tucker}) and the above result may be considered as an
alternative derivation. What is more important is that the
co-closedness of ${\cal J}_{1}$ is equivalent to $\delta j_2=0$ and
this implies that $j_3$ must also be co-closed, for ${\cal J}_{2}$
is co-closed. On the other hand, from the definition
$j_3=\omega{\cal R}$ we find
\begin{eqnarray}
\delta j_3=-i_{X_a}\nabla_{X^{a}}(\omega{\cal R})=(\delta\omega)
{\cal R}-i_{X_a}\omega\nabla_{X^{a}}{\cal R}\nonumber
\end{eqnarray}
and since all KY-forms are co-closed, we arrive at $\delta
j_3=-\nabla_{K}{\cal R}=0$. As a result, the covariant derivative of
curvature scalar with respect to any Killing vector field $K$ of the
underlying manifold must be zero;
\begin{eqnarray}
\nabla_{K}{\cal R}=0\;.
\end{eqnarray}
So we have arrived at a general relation of the (pseudo)Riemannian
geometry which uncovers an important property of the Killing vector
fields that seems to be, as far as we know, unnoticed in the
literature. Since the Lie derivative and covariant derivative
coincide on $0$-forms, this also means that the Lie derivative of
the scalar curvature with respect to Killing vector fields is zero
for any (finite) dimension and signature. More precisely, the scalar
curvature of any (pseudo)Riemannian manifold is a flow-invariant for
all of its Killing vector fields. An alternative proof of equation
(33) is given in Appendix B.

It is worth mentioning that for $1$-form currents above we have
\begin{eqnarray}
{\cal J}=-K_a(2P^{a}-{\cal
R}e^{a})=K_a{}^{\ast^{-1}}G^{a}\;,\nonumber
\end{eqnarray}
where $K_a{}^{\ast^{-1}}G^{a}$ (see also the equation (38) below) is
the current whose conservation is the starting point for the studies
referred in the introduction. The above analysis explicitly shows
that this current is the sum of the co-exact current $j_2$ given by
(32) and the co-closed current ${\cal J}_{2}=-K_a(P^{a}-{\cal
R}e^{a})$. It is perhaps, due to the lack of the relation (33), the
compositeness of the current $K_a{}^{\ast^{-1}}G^{a}$ have remained
unnoticed. As is shown in Appendix B, (33) directly follows from the
contracted Bianchi identities and (32).

\subsection{Currents for duals of Yano vector fields}

It is a well established fact that the Hodge map defines a general
one-to-one correspondence between the vector space of KY $p$-forms
and of the closed conformal KY $(n-p)$-forms \cite{ozumav1}. In
particular, for each KY $(n-1)$-form $\omega_{(n-1)}$ there exists a
uniquely determined closed conformal KY $1$-form $\tilde{Y}$ such
that
\begin{eqnarray}
\omega_{(n-1)}=^{\ast}\tilde{Y}\;,
\end{eqnarray}
where the conformal vector field $Y=Y^{a}X_a$, known as the {\it
Yano vector} \cite{McLenaghan}, is the metric dual of
$\tilde{Y}=Y_{a}e^{a}$ . Yano vectors are locally gradient fields
whose integral curves are pre-geodesics and they generate special
conformal transformations. For (34) we have
\begin{eqnarray}
{\cal J}_{2}=(-1)^{n-1}i_{X_{a}}(^{\ast}\tilde{Y}\wedge
P^{a})=i_{X_{a}}(\tilde{Y}\wedge^{\ast} P^{a})\;.
\end{eqnarray}
Since $i_{X^{a}}{}^{\ast} P^{a}=^{\ast}(P^{a}\wedge e_a)=0$ by the
Bianchi identity, we deduce from (35) that $Y_{a}^{\ast} P^{a}$ is
co-closed and equivalently, the $1$-form $Y_{a}P^{a}$ is closed.
Therefore, the vector field $Y_{a}\tilde{P}^{a}$ is locally a
gradient field (in fact, the equation (41) given below proves that
$Y_{a}\tilde{P}^{a}$ is globally a gradient field).

In order to write ${\cal J}_{1}$ in terms of KY $(n-1)$-forms we
first express $j_1$ and $j_2$ in terms of KY $(n-1)$-form
$^{\ast}\tilde{Y}$ and the Einstein $(n-1)$-forms $G^{a}$ as
follows;
\begin{eqnarray}
j_1&=&i_{X^a}i_{X^b}{^\ast}\tilde{Y}\wedge R_{ab}
=-Y_{a}G^{a}\;,\\
j_2&=&i_{X_a}{^\ast}\tilde{Y}\wedge P^{a} =Y^b{^\ast}e_{ab}\wedge
P^{a}=(-1)^{n}Y_{a}(G^{a}+{^\ast}P^{a})\;,
\end{eqnarray}
where
\begin{eqnarray}
G^{c}=R_{ab}\wedge^{\ast}(e^{cab})={\cal
R}^{\ast}e^{c}-2^{\ast}P^{c}\;.
\end{eqnarray}
So, by combining (36) and (37) as in (6), ${\cal J}_{1}$ is found to
be
\begin{eqnarray}
{\cal J}_{1}=-Y_{a}{^\ast}P^{a}\;.
\end{eqnarray}
By virtue of (24), this proves the co-exactness of
$Y_{a}{^\ast}P^{a}$:
\begin{eqnarray}
Y_{a}{^\ast}P^{a}=\frac{n-1}{n}\delta d{^\ast}\tilde{Y}\;.
\end{eqnarray}
or, equivalently, the exactness of $Y_{a}P^{a}$
\begin{eqnarray}
Y_{a}P^{a}=\frac{n-1}{n}d\delta\tilde{Y}\;.
\end{eqnarray}

Equations (32) and (41) reveal an important general role of Killing
and Yano vector fields that may be of significant in geometry as
well in physics. These vector fields are the ``integrating vector
fields" for Ricci $1$-forms, in the sense that if the underlying
space-time accepts such vector fields then their contractions with
Ricci $1$-forms as in (32) and (41) are, respectively, co-exact and
exact forms which are also specified in terms of the duals of these
vector fields. From (38) we also see that they enable us to make
decompositions of the corresponding contractions of the Einstein
$(n-1)$-forms which contain exact or co-exact parts. On the other
hand, for a KY $(n-2)$-form $\omega$ we can write
$\omega=^{\ast}\beta$, where $\beta$ is a closed conformal KY
$2$-form. In this case we have
\begin{eqnarray}
{\cal J}=i_{X_{a}}i_{X_{b}}(\omega\wedge
R^{ba})=\beta_{ba}{}^{\ast}R^{ba}\;,\nonumber
\end{eqnarray}
which exhibits the decomposition of $\beta_{ba}{}^{\ast} R^{ba}$ as
a sum of co-exact ${\cal J}_{1}$ and co-closed ${\cal J}_{2}$.

\section{Conserved Currents on Some Special Manifolds}

On a Ricci-flat (pseudo)Riemannian manifold for which $P^{a}=0$ and
hence ${\cal R}=0,\;{\cal J}_{2}$ is identically zero and ${\cal
J}_{1}$ is equal to $-j_1$. Therefore, for each KY $p$-form $\omega$
accepted by such a manifold we have
\begin{eqnarray}
(i_{X_a}i_{X_b}\omega)\wedge R^{ab}=\frac{p}{p+1}\delta
d\omega\;.\nonumber
\end{eqnarray}

Let us now consider a conformally flat (pseudo)Riemannian manifold
which is characterized by the vanishing of Weyl $2$-forms, or
equivalently, by
\begin{eqnarray}
R_{ab}=\frac{1}{n-2}[P_a\wedge e_b-P_b\wedge e_a+\frac{\cal
R}{n-1}e_a\wedge e_b]\;.\nonumber
\end{eqnarray}
This implies that $j_1$ linearly depends on $j_2$ and $j_3$ and
after a little computation we get
\begin{eqnarray}
{\cal
J}_{1}=(-1)^{p}\frac{n-2p}{n-2}j_2-\frac{p(p-1)}{(n-1)(n-2)}j_3\;.\nonumber
\end{eqnarray}
Thus, when $n$ is even and $p=n/2,\;j_3$ is co-exact. In general, in
view of (6) and (7) we can say that for $1<p<n-1,\;{\cal J}_{1}$ and
${\cal J}_{2}$ are linearly independent if and only if $j_2$ and
$j_3$ are.

\subsection{Constant-curvature space-times}

For an $n$-dimensional constant-curvature space-time \cite{Thirring}
characterized by $R_{ab}=ce_{a}\wedge e_{b}$ with $c$ constant, the
relations
\begin{eqnarray}
 P_{a}=c(n-1)e_{a}\;,\quad {\cal
R}=cn(n-1)\;.
\end{eqnarray}
directly follow from $R_{ab}=ce_{a}\wedge e_{b}$. In such a case we
have,
\begin{eqnarray}
{\cal J}_{1}&=&-c(i_{X^{a}}i_{X^{b}}\omega)\wedge
e_{ab}+(-1)^{p}c(n-1)i_{X_{a}}\omega\wedge e^{a}\nonumber\\
&=&-c p(n-p)\omega\;,\\
{\cal J}_{2}&=&(-1)^{p}c(n-1)i_{X_{a}}\omega\wedge
e^{a}+cn(n-1)\omega\nonumber\\
&=&c(n-1)(n-p)\omega\;,
\end{eqnarray}
where the scaling property has been used several times. Thus, the
currents become constant multiples of their defining KY-forms and
therefore they are linearly dependent. Moreover, their co-closedness
are nothing more than the co-closedness of KY-forms and hence give
nothing new. But the co-exactness of ${\cal J}_{1}$ has an important
implication.

By comparing (24) and (43) we obtain, for $p\neq 0$
\begin{eqnarray}
\delta d\omega=c(p+1)(n-p)\omega \;,\nonumber
\end{eqnarray}
and by recalling the fact that every KY-form is co-closed, we see
that every KY $p$-form is an eigenform of the Laplace-Beltrami
operator:
\begin{eqnarray}
\displaystyle{\not}d^2\omega=-c(p+1)(n-p)\omega.
\end{eqnarray}
This is nontrivial for $p\neq 0$ and $p\neq n$. The eigenvalues
depend on $n$, on the degree of the KY-form and on the constant $c$.
In particular, the sign of eigenvalues is the opposite of the sign
of $c$. Since the connection of a (pseudo)Riemannian geometry is
metric compatible, covariant derivatives commute with the Hodge map.
This implies that three main operators of section II A and therefore
$\displaystyle{\not}d^2$ also commute with the Hodge map. Equation
(45) shows that the Hodge dual of any KY $p$-form (which need not be
a KY $(n-p)$-form, but is certainly a closed conformal KY
$(n-p)$-form) is also an $(n-p)$-eigenform of
$\displaystyle{\not}d^2$ corresponding to the same eigenvalue. If we
restrict ourselves to $p$-eigenforms of the Laplace-Beltrami
operator we also get another series coming from the Hodge dual of a
KY $(n-p)$-form. So, for $\alpha=^{\ast}\beta$ where $\beta$ is a KY
$(n-p)$-form, we have
\begin{eqnarray}
\displaystyle{\not}d^2\alpha=-cp(n-p+1)\alpha,\nonumber
\end{eqnarray}
where $\alpha$ is a closed conformal KY $p$-form. As a result, each
eigenvalue corresponding to a KY $p$-form is degenerate with
multiplicity (counted in the space of $p$-forms) which is not lower
than the number of linearly independent KY $p$-forms. An exceptional
case may occur when $n$ is even and $p=n/2$. In such a case, the
mentioned lower bound may decrease depending on the existence of
dual and anti-self dual KY $p$-forms. By now, it is well-established
fact that the number of linearly independent KY $p$-forms is bounded
from above, for any dimension and signature, by the binomial number
\begin{eqnarray}
C(n+1, p+1)=\frac{(n+1)!}{(p+1)!(n-p)!}\;,
\end{eqnarray}
and these upper bounds are attained on the constant curvature
manifolds \cite{Kastor,ozumav1}.

In fact, on a constant curvature Riemannian manifold, such as the
standard $n$-sphere, the spectrum of $\displaystyle{\not}d^2$ on
$p$-forms is well known \cite{Semmelman1,Semmelman2}: it consists of
two series related to each other by the interchange
$p\leftrightarrow (n-p)$ in the eigenvalues and both depend (apart
from $n$ and $p$) on a nonnegative integer $k=0,1,\dots$. Eigenforms
corresponding to the minimal values of these series (for which
$k=0$) turn out to be KY $p$-forms and the Hodge duals of KY
$(n-p)$-forms. What we have found by analyzing one of the currents
above correspond to minimal parts of the spectrum for the case of a
constant curvature space-time which need not necessarily be
Riemannian.

\subsection{Einstein Manifolds}

Let us now consider an $n$-dimensional Einstein manifold
characterized by $P^{a}=ke^{a}$ with constant $k={\cal R}/n$. Since
in three dimensions any Einstein space is necessarily of constant
curvature here we suppose $n\geq 4$ and $R_{ab}\neq ce_a\wedge e_b$
to reach nontrivial statements. In this case we have
\begin{eqnarray}
{\cal J}_{1}&=&-i_{X^{a}}i_{X^{b}}\omega\wedge R_{ab}-k p \omega\;,\nonumber\\
{\cal J}_{2}&=&k(n-p)\omega\;.\nonumber
\end{eqnarray}
Obviously, the conservation of ${\cal J}_{2}$ becomes trivial but,
the co-exactness of ${\cal J}_{1}$ implies
\begin{eqnarray}
j_{1}&=&i_{X^{a}}i_{X^{b}}\omega\wedge R_{ab}\;,\nonumber\\
&=&kp\omega-\frac{p}{p+1}\delta d\omega\;.\nonumber
\end{eqnarray}

In particular, for any KY $2$-form $\omega=(1/2)\omega_{ab}e^{ab}$
of an Einstein manifold the ``contracted'' curvature $2$-form
$\omega_{ba} R^{ab}$ can be written as
\begin{eqnarray}
\omega_{ba}R^{ab}=2k\omega-\frac{2}{3}\delta d\omega\;.
\end{eqnarray}
Note that this is trivial for constant curvature spaces. This
relation shows that for each KY $2$-form accepted by an Einstein
space the contraction of the curvature $2$-forms as in equation (47)
is decomposed into co-closed and co-exact parts that are determined
up to well-defined constants, by these KY $2$-forms. On the other
hand, the equations (32) and (40) (or (41) in the case of Einstein
manifolds imply that $\tilde{K}$ and $\tilde{Y}$ (and hence
$^\ast\tilde{K}$ and ${}^\ast\tilde{Y}$) are eigenforms of the
Laplace-Beltrami operator:
\begin{eqnarray}
\displaystyle{\not}d^2\tilde{K}=
-2k\tilde{K}\;,\quad\displaystyle{\not}d^2\tilde{Y}=k\frac{n}{n-1}\tilde{Y}\;.
\end{eqnarray}
Note that while in the first case the eigenvalues have the opposite
sign with $k$, in the second case they have the same signs. The
lower bounds for their degeneracy can be determined from (46) as we
did in the previous subsection.

\section{Summary and Concluding Remarks}

In this study we have shown that two linearly independent
uncomposite currents for each KY-form can be constructed using the
curvature forms of the underlying space-time. The current suggested
in the literature (see (1)) is a special linear combination of the
currents claimed here. Moreover, while the current (1) identically
vanishes for all KY $(n-1)$-forms, in our case the currents ${\cal
J}_{1}$ and ${\cal J}_{2}$ are non-vanishing but become linearly
dependent. What is more, the current ${\cal J}_{1}$ is shown to be
co-exact from which several
geometric facts follow. Some of these can be summarized as follows.\\
(i) The scalar curvature ${\cal R}$ of any (pseudo)Riemannian
manifold is a flow invariant for
all of its Killing vector fields; $\nabla_{K}{\cal R}=0$. \\
(ii) The conserved currents directly provide decompositions for
index-saturated differential forms constructed by contracting the
components of KY $p$-forms  with the Ricci $1$-forms, curvature
$2$-forms and with the Einstein $(n-1)$-forms (for the values
$p=1,2$ and $p=n-1$). These contractions are solely expressible in
terms of KY-forms themselves and their (co)derivatives. \\
(iii) On an Einstein manifold, duals of all Killing and Yano vector
fields are eigenforms of the Laplace-Beltrami operator such that the
eigenvalues have multiplicities with well defined lower bounds.\\
(iv) Generalizations of some well-known facts related to the
spectrum of Laplace-Beltrami operator on a constant curvature
Riemannian manifold also follow directly from the properties of
conserved currents. More precisely, we have shown that in a constant
curvature (pseudo)Riemannian manifold all KY-forms and their Hodge
duals are eigenforms of the Laplace-Beltrami operator.

The whole attention in this study has inevitably been focused on the
basic gravitational currents and their properties. The study of
related conserved charges in the framework of this paper remains
almost untouched, but deserves to be the subject of a separate
study. The basic gravitational currents presented in this paper may
shed light on some of the problems related to interpretation of
generalized charges.

\begin{acknowledgments}
This work was supported in part by the Scientific and Technical
Research Council of Turkey (T\"{U}B\.{I}TAK).
\end{acknowledgments}

redpajama_set_name: RedPajamaArXiv


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text:
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Hit The Lights have released the first video a documentary-style series titled the Skeleton Series. These videos take a look at the inner workings in a band, as well as the negative parts that are not really seen. AbsolutePunk will be releasing these videos leading up to Hit The Lights' March 24th release of Summer Bones. A new video will be out next monday. Check out the first video, 'Chapter 1', below.


Export the WordPress data as WXR.
The resulting WXR is not well-formed and is not readable.
wordpress_export_cdata.patch (459 bytes) - added by ceefour 8 years ago.
15203.importer.diff (697 bytes) - added by duck_ 7 years ago.
15203.diff (654 bytes) - added by duck_ 7 years ago.
15203.importer.2.diff (865 bytes) - added by duck_ 7 years ago.
I had thought of this whilst preparing for #15197, but obviously forgot about it. Though I cannot reproduce using your steps above, since the > is encoded as > in the output file, there is a possibility of this happening in other circumstances (see #15294).
Before this can go in, I believe the regular expression based importer might have to be updated.
duck_ is this ticket still relevant or can it be closed?
Just wanted to stop by here and say that I had the issue due to having CDATA tags in post content, which broke XML, applied the fix manually (as WP 3.4 isn't out yet), and verified the final XML validates. Thanks, everyone.


text:
<?php

return [
    /*
    |--------------------------------------------------------------------------
    | Password Reminder Language Lines
    |--------------------------------------------------------------------------
    |
    | The following language lines are the default lines which match reasons
    | that are given by the password broker for a password update attempt
    | has failed, such as for an invalid token or invalid new password.
    |
    */

    'password' =>
        'Las contraseñas deben tener por lo menos 6 caracteres y coincidir en la casilla de confirmación.',
    'user' =>
        'No pudimos encontrar ningún usuario con esa dirección de correo electrónico.',
    'token' => 'Este código para restablecer contraseña es inválido.',
    'sent' =>
        '¡Te hemos enviado un correo con el vínculo para restablecer tu contraseña!',
    'reset' => '¡Has restablecido tu contraseña!',
];

redpajama_set_name: RedPajamaGithub


The monobloc air conditioners of the HYDRAUTAN range have been studied and manufactured to adapt to harsh environments. Autonomous and compact, these monobloc air conditioners are driven by hydraulic motor and offer the possibility of integrating an air filtration module and pressurization.
Positioned on the roof, the HYDRAUTAN monobloc air conditioners make it possible to adapt, mainly, to all agricultural vehicles and public works machines.
The HYDRAUTAN range integrates all the components necessary for the operation of the air conditioning circuit as well as the compressor driven by a hydraulic motor. This solution allows HYDRAUTAN monobloc air conditioners to be positioned away from the engine compartment, when necessary.
The entire range is available in several voltages and has the heating function.
Monobloc air conditioners are particularly suitable for moving in dusty environments. They will offer you very good cooling and heating performance for cabins with a volume less than or equal to 4 m3.
During assembly it will be necessary to carry out cutting, drilling and refrigerating and hydraulic connections.
Outside air is filtered through the use of double filtration which prevents the introduction of particles into the HYDRAUTAN monobloc air conditioner.
In addition to the outdoor air filtration (under cabin sealing condition) we can add a pressurization system according to ISO-10263-4.


text:
require "rails_helper"

module Renalware
  module Patients
    describe AttachmentQuery, type: :model do
      let(:user) { create(:user) }
      let(:patient1) { create(:patient, by: user) }
      let(:patient2) { create(:patient, by: user) }

      describe "#call" do
        context "using default sort and no search argument" do
          it "returns a sorted collection of attachments for a patient" do
            att1 = create(:patient_attachment, :with_file, patient: patient1, by: user)
            att2 = create(:patient_attachment, :with_file, patient: patient1, by: user)
            # Create a soft-deleted attachment for this patient
            create(
              :patient_attachment,
              :with_file,
              patient: patient1,
              deleted_at: 1.minute.ago,
              by: user
            )
            # Create an attachment for another patient
            create(:patient_attachment, :with_file, patient: patient2, by: user)

            attachments = described_class.new(patient: patient1).call

            expect(attachments.to_a).to eq [att2, att1]
          end
        end
      end
    end
  end
end


Our specialties include contr. lic. 718701 and contractor lic 718701. We can assist you with contractors.
If you have used the services of Blood Sweat & Rebar we'd love to hear from you! Use the form below to review and comment on your experience.


November 11, 2015, 5:00 PM EST.
This article is the second in a lengthy series chronicling the 1925 Hilldale baseball club and their journey through the Eastern Colored League.
For an explanation of 'The '25 Hilldale Project' and links to other articles within the series, please click here.
After getting away to a wobbly start, Holsey "Scrip" Lee, the Hilldale submarine artist, turned in the second league game for the Eastern League champs by baffling Alex Pompez's Cuban Stars in the Saturday afternoon matinee at Hilldale Park, score 6 to 1.
At that the invaders put up a nifty article of ball, especially on the defense. Their inability to hit the underhand slants served up by Lee really clinched the argument, while the local clubbers gathered eight hits and six tallies from the offerings of elongated Martin Dihigo.
The lone Cuban tally was forced in by Lee in the first inning. Mesa walked, Fabre singled, Oms sacficed and Chacon was handed a pass, filling the bases. Massip, a newcomer in the ranks of the invaders, proved to be a good waiter and Messa was forced home.
Hilldale practically clinched the game in its half of the first inning when two runs were put over on singles by Briggs and Carr. Mackey's double and Judy Johnson's sacrifice fly.
Note: The box score is listed below, but take note of how it appears. Unlike today's box scores, newspapers prior to the 1940s normally would include only runs scored, hits, outs recorded as a fielder, assists, and errors. This makes stat tracking extremely difficult, but this is how it was done in 1925.


May you find great value in these inspirational Luciano Pavarotti Quotes from my large datebase of inspiring quotes and sayings.
I believe something fundamental is actually being taken from them.
It is a very honest world, our work.
I think you cannot fake anything.
but you must also be famous.
The two are different things.
There is no prodigy in our profession.
I am a tenor buff.
The rivalry is with ourself.
I try to be better than is possible.
I fight against myself, not against the other.
Why should be elite, music? Excuse me.
Music must be for everybody.
Thank you for visiting these Luciano Pavarotti Quotes and Sayings - Quotes by Luciano Pavarotti.


text:
FactoryBot.define do
  factory :delivery_centre do
    sequence(:name) { |n| "Delivery Centre #{n}" }
    reply_to { 'dc@example.com' }
    hidden { false }

    trait :hidden do
      hidden { true }
    end

    trait :with_locations do
      after(:build) { |dc| dc.locations << build(:location) }
    end
  end
end


The rain clouds yesterday brought back memories of home, Kerala, where it rains practically all year round. The gray clouds, together with the stark mountains over which they hovered, made a stunning sight that I could have danced, in my mind of course. for I am no graceful peacock that unfurls its long tail and dances in joy. Or so they say, the poets, I mean.
Frankly speaking, I have seen them, the peacocks, dance when the sun shines brightly overhead too. So I am not buying the poet's version in all its entirety. Poets are wont to be imaginative creatures and can cook up a few beautiful thing or two for effect. Ask me about it, I should know being a minor, wee little insignificant one myself.
There, I have done it again, gone gallivanting into the countryside so to speak, instead of walking the straight and narrow path. Not that I ever regret wandering off. I dislike the straight narrow paths, winding ones may be, especially when they take you to nooks and crannies unexplored.
I especially have a thing about open countryside. Perhaps it is because we don't have open spaces in my own land. In every direction you look, you'll either find trees or buildings within a few feet. That's also equally beautiful, the trees growing closely, the foliage that filters the sunlight and keeps things cool, or as cool can in the humidity. Here, in Muscat where I am now, I can see open spaces as far as the eye can see, and mountains, and that's awesome. But let's get back to rain clouds.
The distant mountains started disappearing after a while, a gray haze slowly covered first one peak, then another. The breeze became cooler, filled with moisture. How I recognized it from back home! Yeah, I love rain.That is if there is anyone left who does not know it already. Hehe. Soon the rumble of thunder could be heard and lightning streaked across the sky. And then it started to rain.
Unfortunately, the *show* started late in the evening, petrichor driving me crazy. I don't have a picture of rain worth showing off. But I made quite a few rain-paintings [pictures taken through the windshield/glass of a moving vehicle] as we drove. They will have to wait till I get back home to be shared.
It performs a magnificent refrain!
True. But I didn't get to see the awesome sight of water coming down the mountains since it rained in the night.


Sunny, with a high near 71. Calm wind becoming west around 5 mph in the afternoon.
Clear, with a low around 46. South wind around 5 mph.
Sunny, with a high near 80. South wind 5 to 15 mph, with gusts as high as 25 mph.
A 20 percent chance of showers after 2am. Mostly cloudy, with a low around 57. South wind 10 to 15 mph.
A chance of showers, with thunderstorms also possible after 2pm. Mostly cloudy, with a high near 73. Chance of precipitation is 40%.
A chance of showers and thunderstorms. Mostly cloudy, with a low around 50. Chance of precipitation is 40%.
A 30 percent chance of showers, mainly after 2pm. Mostly cloudy, with a high near 64.
A 30 percent chance of showers, mainly before 2am. Mostly cloudy, with a low around 47.
A 20 percent chance of showers before 8am. Mostly cloudy, with a high near 65.


Quick steps to setup Ubuntu LTS server.
My blogging journey through this blog.
Jenkins is a good tool for continuous integrations and system build.
Web Server configrations and tunings.
Simple Made Easy is a great talk by Rich Hickey. It is about Simple and Easy in programing world.
These are some resources grouped together to make life easy for me to follow up with containers and orchestration technologies.
Solves the problem of separating OS from hardware.
Theses are the list of backup tools I have tried out or interested in.
These are a quick reference for Multi-tenant architecture.
Odoo is a complete solution to manage companies regards of Human resource and Financial and so on. These are some resources I have found and list them here to be as a reference to me later.
There are two service called, Loggly and splunk. They are good. But I will discuss opensource solution here.
These are some tools and hint to optimization your site.
These are some concepts and techniques I have passed through OpenEdx.
matplotlib is a Python package for drawing plot.
BitTorrent Sync is my favorite tool to sync my folders between my devices. Here is the process to install it on Ubuntu server.
Usually there are 3 Git repositories, Local repository, Server repository and Production repository.


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