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POLITICO NOW Blog
Issa: Iraqi government 'delusional'
By AUSTIN WRIGHT
Just back from a trip to Iraq, House Oversight and Government Reform Committee Chairman Darrell Issa said on Sunday the government in Baghdad is "still quite delusional" about the urgency of the war against the Islamic State of Iraq and the Levant.
"They're still talking about long-term training before they're ready to fight," the California Republican said an ABC's "This Week."
Issa said he was ready to vote to authorize the U.S. military campaign against ISIL — something President Barack Obama has requested. "The fact is we're already there," Issa said. "We've had to be there."
Issa also said Iraqis — not Americans — should be the ones engaging in ground combat against ISIL. The Kurds were up to the challenge, he said.
"I have no doubt whatsoever that the Kurds will fight," he said. "All they need is our air support and our technical know-how, and they will do it."
Darrell Issa
ISIL
Walker: Clinton 'embodies what's wrong with Washington'
By JEN JUDSON
Wisconsin Gov. Scott Walker said on Sunday the Republican messaging in the 2016 presidential campaign should be Hillary Clinton is too Washington.
"We're going to have a message that says Hillary Clinton is all about Washington," the Republican governor said on NBC's "Meet the Press." "I think in many ways, she was the big loser on Tuesday because she embodies everything that's wrong with Washington."
Walker: 'Governors make much better presidents'
Scott Walker for president?
Asked whether he was considering a run for president in 2016 Sunday, the Republican governor from Wisconsin said he believed "governors make much better presidents than members of Congress."
Governors offer a "fresh approach," with "executive experience from outside of Washington to provide a much better alternative to the old, tired, top-down approach out of Washington, D.C," Walker said, adding, "We need something fresh, organic from the bottom up – and that's what you get in the states."
Chuck Todd also asked the governor whether he'd deferred to Rep. Paul Ryan (R-Wis.), considered to be a possible presidential candidate since his run for vice president in 2012.
"I love Paul Ryan. I've said many times before I'll be the president of the Paul Ryan fan club, but I do think if we're going to beat Hillary Clinton in this next election, we're going to have a message that says Hillary Clinton is all about Washington," Walker said.
Responding later, Democratic National Committee spokesman Michael Czin said, "we're thrilled that Governor Walker thinks Republicans should run for president on the record of GOP governors," calling that "wing of the GOP…every bit as broken and dysfunctional as the congressional wing of the party."
Under Walker, Wisconsin "lags the country in job growth," Czin said. And pointing to other GOP governors, he added, "Chris Christie's policies have led to a record number of credit downgrades, and nearly one in five live in poverty in Rick Perry's Texas."
2012 Presidential Race
New and Old Guard urge 'cooperation' in new Congress
Members of both the old and new guard in the House said on Sunday they are optimistic they can reach compromises in the new Congress and move bills to the president's desk.
"We can work past our differences," Rep.-elect Carlos Curbelo (R-Fla.) said on CNN's "State of the Union," and "get bills across the finish line."
Rep.-elect Brendan Boyle (D-Pa.) said lawmakers can't be afraid to vote yes to get things done. "It's always easier and safer to vote no," he said. " Yes, there is a risk in voting yes… People are so afraid of voting yes."
Rep. Steve Israel of New York,chairman of the House Democratic Congressional Campaign Committee, agreed with the newcomers noting that while Democrats and Republicans differ on 75 percent of most issues, that leaves 25 percent where agreement can be reached.
Israel said he discovered a good level of cooperation can be reached through meeting and hashing out differences, something he tried several years ago when he started a "Central Aisle Caucus" made up of members of both parties where they would meet at Chinese restaurant, pick an issue, spend five minutes disagreeing and 55 minutes figuring out how to agree.
"Let's not retreat to our corners," Israel said, "let's meet in the middle of the map."
Rep.-elect Ruben Gallego (D-Ariz.) said he hoped to see Department of Veterans Affairs reforms and an immigration bill move forward. "Let's get it done," he said.
Also participating on Candy Crowley's panel were Rep.-elect Lee Zeldin (R-N.Y.), newly relected Sen. Chris Coons (D-Del.) and retiring Rep. Michele Bachmann (R-Minn.).
Of the four newcomers, Zeldin in Long Island and Curbelo in South Florida both ousted Democratic incumbents. Gallego and Boyle both retained seats held by retiring Democrats. With seven races still undecided, Republicans have so far scored a net gain of 12 seats.
Steve Israel
Michele Bachmann
Chris Coons
Carlos Curbelo
Brendan Boyle
Ruben Gallego
Lee Zeldin
Bush: Presidents better mean what they say
Former President George W. Bush says presidents better mean what they say — a subtle dig at President Barack Obama, who's been criticized for not taking stronger actions to back up his tough talk on Syria.
"When you say something as president, you better mean it," Bush said in an interview airing Sunday on CBS's "Face the Nation." "Words mean something."
Bush's comments came as he discussed former Iraqi President Saddam Hussein. When Hussein was captured in 2003, Bush said, he told an FBI agent that he hadn't believed Bush's ultimatum that he step down and leave the country.
"It's hard for me to believe he didn't believe me," Bush told host Bob Schieffer. "We'd given an ultimatum to the Taliban and delivered."
Bush, who is is promoting a new book about his father, "41: A Portrait of My Father," also rejected the notion that the war in Iraq was about finishing what his father started.
"I went in there as a result of a very changed environment because of September the 11th," Bush said. "The danger we were concerned about was that the weapons ... would be put into the hands of terrorist groups that would come and make the attacks of 9/11 pale in comparison."
Senators differ on attorney general confirmation timing
Democratic Sen. Chris Murphy of Connecticut on Sunday urged the Senate to move forward during the lame -duck session to confirm Loretta Lynch as the new attorney general, but Republican Sen. John Thune of South Dakota said he believes the new GOP-controlled Senate should consider the nomination.
While he has not spoken to Majority Leader Sen. Harry Reid (D-Nev.) on his plans, Murphy said on CNN's "State of the Union," "I think it's important that we have an attorney general . . . someone on the ground sooner or later."
But Thune disagreed. "I think it is in the best interest of the country and Congress to wait and do this under regular order, there's a process, there's hearings," he said.
John Thune
Gardner: GOP must govern with 'maturity'
Republican Cory Gardner, who defeated Democratic Sen. Mark Udall Tuesday in Colorado, says the new Republican majority in the Senate must govern with "competence" and "maturity."
Otherwise, he said, the Republicans could face the same kind of electoral rout in 2016 that the Democrats suffered last week.
The midterm elections were "a rejection of the failed ways of Washington," Gardner said on "Fox News Sunday." "The mandate was this: People don't like dysfunction, they don't like gridlock."
Gardner also said Congress must pass an immigration reform bill and urged President Barack Obama to hold off on issuing an executive order.
"We know we need immigration reform in this country because the system isn't working," Gardner said. "Let's take those steps where I think there is a broad agreement that we can get behind."
Cory Gardner
Mark Udall
Bush says his dad almost didn't seek reelection
Former President George W. Bush says his father considered not seeking reelection in 1992 because of his son Neil's legal troubles with a failed business.
But Bush says he urged his father to run, saying "the country needs you."
"The '92 defeat was really hard, and — it — ironically enough, it did make it easier for me," Bush said in an interview to airing Sunday on CBS's "Face the Nation."
"When people criticize my dad, somebody who I admire greatly, I didn't react well at times and it really, really affected me," Bush added. "When they criticized me, the — sting wasn't nearly as difficult."
The former president is promoting a new book about his dad, "41: A Portrait of My Father."
George W. Bush discusses his brother's chances of running in 2016 on CBS's 'Face the Nation.'
Bush puts odds of Jeb running at 50-50
Former President George W. Bush says the odds of his brother Jeb running for president in 2016 are 50-50.
"I'd give it a toss up," Bush said in an interview airing Sunday of CBS's "Face the Nation." On the other hand, Bush added, "He's not here knocking on my door, you know, agonizing about the decision."
Bush also said his brother is well aware of how a presidency can affect a family.
"He's seen his dad and his brother go through the presidency," Bush told host Bob Schieffer, saying his father showed it's possible to be a good father and a president.
"One of the lessons you learn from George H.W. Bush is that you can go into politics and still be a good father," said Bush, who's promoting a new book about his dad, "41: A Portrait of My Father."
Sunday talk show tip sheet
By POLITICO STAFF
"Meet the Press" on NBC
Wisconsin Gov. Scott Walker (R)
Rep.-elect Gwen Graham (D-Fla.)
Sen.-elect Mike Rounds (R-S.D.)
Former House Majority Leader Eric Cantor (R-Va.)
Starbucks CEO Howard Schultz
"Face the Nation" on CBS
Former President George W. Bush
"This Week" on ABC
"Fox News Sunday" on Fox
Sen. John Barrasso (R-Wyo.), chairman, Senate Republican Policy Committee
Rep. Xavier Becerra (D-Calif.), chairman, House Democratic Caucus
Sen.-elect Shelley Moore Capito (R-W.Va.)
Sen.-elect Cory Gardner (R-Colo.)
"State of the Union" on CNN
Sen. John Thune (R-S.D.)
Sen. Bob Casey (D-Pa.)
Sen. Chris Coons (D-Del.)
Rep. Steve Israel (D-N.Y.), chairman, House Democratic Congressional Campaign Committee
Rep. Michele Bachmann (R-Minn.)
Rep.-elect Ruben Gallego (D-Ariz.)
Rep.-elect Carlos Curbelo (R-Fla.)
Rep.-elect Brendan Boyle (D-Pa.)
Rep.-elect Lee Zeldin (R-N.Y.)
James Baker: Jeb Bush should run
By HADAS GOLD
Former Secretary of State James Baker said on Sunday former Florida Gov. Jeb Bush would make a great president and should run for the Republican nomination in 2016.
"I hope he does. He would make an extraordinarily fine president. He's a very capable young man," Baker said on CNN's "State of the Union."
Baker also predicted Republicans would pick up six seats and regain control of the Senate in Tuesday's midterm elections, though he warned that both the president and the Republicans would have to learn to work together.
"You have to be willing to schmooze and make a concentrated and concerted effort to achieve compromise with the other side," Baker said in advice to President Barack Obama.
As for the Republicans, Baker warned that if they don't learn to work with Obama, they'll suffer in 2016.
Republicans "have to cooperate with the president when they control both houses or they will pay a price for that in the next election," Baker said. "The one thing I think Republicans have to do if they win the Senate ... and they'll have both houses. They need to get things done, they need to pass legislation, come together and pass legislation they can then present to the president and put the onus on him to either sign it or veto it."
Rendell to GOP: Be careful what you wish for
Former Pennsylvania Gov. Ed Rendell has a warning for Republicans expecting to take over the Senate: Be careful what you wish for.
"I think the Republicans, be careful what you wish for, because if they win the Senate, they better do something, they better send the president some responsible pieces of legislation or they'll get crushed in 2016," the former Democratic governor said Sunday on CNN's "State of the Union."
Democratic Party spokesperson Mo Elleithee warned that a Republican majority in the Senate could lead to another shutdown.
"It is hard to make the argument that Republicans can bring us back to the business of governing because Republicans were the ones who shut the government down over an ideological vendetta against this president, and they've signaled they might do that again," Elleithee said.
Elleithee said he's not sure "Republicans know how to" govern and predicted that there would be more Republican governors who lose in Tuesday's elections than Democratic senators.
Ed Rendell
Mo Elleithee
Trump makes his first big move in New Hampshire
Education Department releases new data on 25M applications for Biden's student debt relief
Jan. 6 rioter who maced Brian Sicknick sentenced to 80 months


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Soundtrack | Actor | Composer
Known for Bubble Boy (2001), The Salton Sea (2002), Charlie's Angels (2000), Boyhood (I) (2014)
@blink182 (twitter.com) | 11 official web sites & 15 more links
4 wins & 6 nominations
Music Department (1)
Linkin Park and Friends: Celebrate Life in Honor of Chester Bennington (2017)
(Video) - Themselves, Performer ("I Miss You") Themselves, Performer ("I Miss You") See fewer
Blink-182: Home Is Such a Lonely Place - Matt Skiba Version (2017)
(Video) - Blink-182 Blink-182 See fewer
Blink-182: Home Is Such a Lonely Place - Travis Barker Version (2017)
Blink-182: Home Is Such a Lonely Place (2017)
Blink-182: Home Is Such a Lonely Place - Mark Hoppus Version (2017)
It's Only the End of the World (2016)
Performer ("I Miss You") Performer ("I Miss You") See fewer
Blink-182: She's Out of Her Mind (2016)
Blink-182: Bored to Death (2016)
Boyhood (2014)
Performer ("Anthem Part Two") Performer ("Anthem Part Two") See fewer
Blink-182: After Midnight (2012)
Blink-182: Wishing Well (2011)
Blink-182: Heart's All Gone (2011)
Blink-182: Up All Night (2011)
Restrepo (2010)
Performer ("Stay Together for the Kids"), Writer ("Stay Together for the Kids") Performer ("Stay Together for the Kids"), Writer ("Stay Together for the Kids") See fewer
The Tomorning Show (2009)
(Short) - Performer ("Dammit") Performer ("Dammit") See fewer
Stick It (2006)
The Powder Puff Principle (2006)
(Short) - Performer ("What's My Age Again?") Performer ("What's My Age Again?") See fewer
Blink 182: Greatest Hits (2005)
(Video) - Blink-182 (archive footage), Producer, Performer ("Carousel", "M+M's", "Dammit", "Josie", "What's My Age Again?", "All The Small Things", "Adam's Song", "Man Overboard", "First Date", "The Rock Show", "Stay Together For The Kids", "Feeling This", "I Miss You", "Down", "Always", "Not Now", "Another Girl, Another Planet") Blink-182 (archive footage), Producer, Performer ("Carousel", "M+M's", "Dammit", "Josie", "What's My Age Again?", "All The Small Things", "Adam's Song", "Man Overboard", "First Date", "The Rock Show", "Stay Together For The Kids", "Feeling This", "I Miss You", "Down", "Always", "Not Now", "Another Girl, Another Planet") See fewer
Blink-182: Not Now (2005)
Punk: Attitude (2005)
Performer ("Man Overboard") Performer ("Man Overboard") See fewer
Blink-182: Always (2004)
Blink-182: Down (2004)
Blink-182: I Miss You (2004)
Riding in Vans with Boys (2003)
(Video) - Themselves, Performer ("Anthem Part Two", "Stay Together For The Kids", "Carousel") Themselves, Performer ("Anthem Part Two", "Stay Together For The Kids", "Carousel") See fewer
Blink-182: Feeling This (2003)
Dickie Roberts: Former Child Star (2003)
Performer ("Dammit") Performer ("Dammit") See fewer
Hope Springs (2003)
Performer ("All The Small Things") Performer ("All The Small Things") See fewer
Haggard (2003)
(Video) - Thanks (as Blink 182) Thanks (as Blink 182) See fewer
Blink 182: The Urethra Chronicles II: Harder, Faster. Faster, Harder (2002)
(Video) - Performer ("The Rock Show", "Anthem Part Two", "Aliens Exist", "Everytime I Look For You", "Story Of A Lonely Guy", "Happy Holidays, You Bastard", "Roller Coaster", "Carousel", "Reckless Abandon", "Please Take Me Home", "Stay Together For The Kids", "Shut Up", "Family Reunion", "First Date", "Give Me One Good Reason", "What Went Wrong?") Performer ("The Rock Show", "Anthem Part Two", "Aliens Exist", "Everytime I Look For You", "Story Of A Lonely Guy", "Happy Holidays, You Bastard", "Roller Coaster", "Carousel", "Reckless Abandon", "Please Take Me Home", "Stay Together For The Kids", "Shut Up", "Family Reunion", "First Date", "Give Me One Good Reason", "What Went Wrong?") See fewer
The Salton Sea (2002)
Clockstoppers (2002)
Performer ("All the Small Things", "First Date") Performer ("All the Small Things", "First Date") See fewer
Blink 182: Stay Together for the Kids (2002)
Blink-182: Anthem Part Two (2002)
Blink-182: Stay Together for the Kids - Version 2 (2001)
Performer ("Dammit (Growing Up)") Performer ("Dammit (Growing Up)") See fewer
American Pie 2 (2001)
Performer ("Everytime I Look For You") Performer ("Everytime I Look For You") See fewer
Blink-182: The Rock Show (2001)
Tomcats (2001)
Performer ("Mutt") Performer ("Mutt") See fewer
Blink 182: First Date (2001)
Charlie's Angels (2000)
Blink-182: Man Overboard (2000)
Performer ("What's My Age Again?") Performer ("What's My Age Again?") See fewer
Blink-182: What's My Age Again (2000)
Blink-182: Adam's Song (2000)
Blink 182: The Urethra Chronicles (1999)
(Video) - Blink-182, Performer ("Going Away To College", "What's My Age Again?", "Dead Man's Curve", "Mutt", "Wendy Clear", "Family Reunion", "All The Small Things", "Don't Leave Me", "Anthem", "Dumpweed", "Dysentery Gary", "Dammit", "Josie", "Adam's Song") Blink-182, Performer ("Going Away To College", "What's My Age Again?", "Dead Man's Curve", "Mutt", "Wendy Clear", "Family Reunion", "All The Small Things", "Don't Leave Me", "Anthem", "Dumpweed", "Dysentery Gary", "Dammit", "Josie", "Adam's Song") See fewer
Godmoney (1999)
Performer ("Voyeur") Performer ("Voyeur") See fewer
Blink-182: All the Small Things (1999)
(Video) - Blink-182, Composer (music by) Blink-182, Composer (music by) See fewer
Blink 182: Enema of the State (1999)
(Video) - Blink-182, Performer ("Dumpweed", "Don't Leave Me", "Aliens Exist", "Going Away To College", "What's My Age Again?", "Dysentery Gary", "Adam's Song", "All The Small Things", "The Party Song", "Mutt", "Wendy Clear", "Anthem") Blink-182, Performer ("Dumpweed", "Don't Leave Me", "Aliens Exist", "Going Away To College", "What's My Age Again?", "Dysentery Gary", "Adam's Song", "All The Small Things", "The Party Song", "Mutt", "Wendy Clear", "Anthem") See fewer
Performer ("I Won't Be Home For Christmas") Performer ("I Won't Be Home For Christmas") See fewer
Can't Hardly Wait (1998)
Blink 182: Josie (1998)
Blink-182: Josie - First Version (1998)
Blink182: Dammit (1997)
Blink-182: M+M's (1995)
(TV Series) - Performer ("All The Small Things") (1 episode, 2019) Performer ("All The Small Things") (1 episode, 2019) See fewer
The Big Break (Apr 18, 2019) Season 1, Episode 3 - Performer ("All The Small Things") Performer ("All The Small Things") See fewer
Hollyoaks (2018)
Episode #1.5005 (Sep 28, 2018) Season 1, Episode 5,005 - Performer ("All The Small Things") Performer ("All The Small Things") See fewer
9-1-1 (2018)
(TV Series) - Performer ("Dammit") (1 episode, 2018) Performer ("Dammit") (1 episode, 2018) See fewer
7.1 (Sep 24, 2018) Season 2, Episode 2 - Performer ("Dammit") Performer ("Dammit") See fewer
(TV Series) - Themselves - Musical Guests / Themselves - Musical Guest (4 episodes, 2003), Performer ("She's Out of Her Mind") (1 episode, 2017), Performer ("Kings of the Weekend", "I Miss You") (1 episode, 2018), Performer ("I'm Feeling This", "Stay Together For The Kids") (1 episode, 2003), Performer ("What's My Age Again", "Dammit") (1 episode, 2009) Themselves - Musical Guests / Themselves - Musical Guest (4 episodes, 2003), Performer ("She's Out of Her Mind") (1 episode, 2017), Performer ("Kings of the Weekend", "I Miss You") (1 episode, 2018), Performer ("I'm Feeling This", "Stay Together For The Kids") (1 episode, 2003), Performer ("What's My Age Again", "Dammit") (1 episode, 2009) See fewer
Shailene Woodley/Jordan Klepper/Blink 182 (May 23, 2018) Season 16, Episode 70 - Themselves - Musical Guests, Performer ("Kings of the Weekend", "I Miss You") Themselves - Musical Guests, Performer ("Kings of the Weekend", "I Miss You") See fewer
The Standups (2018)
(TV Series) - Performer ("She's Out of Her Mind") (1 episode, 2018) Performer ("She's Out of Her Mind") (1 episode, 2018) See fewer
Aparna Nancherla (Mar 20, 2018) Season 2, Episode 6 - Performer ("She's Out of Her Mind") (uncredited) Performer ("She's Out of Her Mind") (uncredited) See fewer
Tattoo Fixers (2017)
(TV Series) - Performer ("I Won't Be Home for Christmas") (1 episode, 2017) Performer ("I Won't Be Home for Christmas") (1 episode, 2017) See fewer
Tattoo Fixers at Christmas (Dec 19, 2017) Performer ("I Won't Be Home for Christmas") (uncredited) Performer ("I Won't Be Home for Christmas") (uncredited) See fewer
Cannonball (2017)
Episode #1.8 (Oct 21, 2017) Season 1, Episode 8 - Performer ("All the Small Things") (uncredited) Performer ("All the Small Things") (uncredited) See fewer
Beat Shazam (2017)
Episode #1.10 (Aug 10, 2017) Season 1, Episode 10 - Performer ("All the Small Things") Performer ("All the Small Things") See fewer
One Hit Wonderland (2017)
(TV Series) - Performer ("All the Small Things", "Dammit", "What's My Age Again?") (1 episode, 2017) Performer ("All the Small Things", "Dammit", "What's My Age Again?") (1 episode, 2017) See fewer
"Right Now" by SR-71 (May 31, 2017) Season 6, Episode 4 - Performer ("All the Small Things", "Dammit", "What's My Age Again?") Performer ("All the Small Things", "Dammit", "What's My Age Again?") See fewer
Good Morning America (2016)
(TV Series) - Performer ("Bored to Death", "What's My Age Again", "All The Small Things", "The Rock Show") (1 episode, 2016), Themselves - Musical Guests (1 episode, 2016) Performer ("Bored to Death", "What's My Age Again", "All The Small Things", "The Rock Show") (1 episode, 2016), Themselves - Musical Guests (1 episode, 2016) See fewer
Episode dated 1 July 2016 (Jul 1, 2016) Themselves - Musical Guests, Performer ("Bored to Death", "What's My Age Again", "All The Small Things", "The Rock Show") Themselves - Musical Guests, Performer ("Bored to Death", "What's My Age Again", "All The Small Things", "The Rock Show") See fewer
Todd's Pop Song Reviews (2015)
"Dear Future Husband" by Meghan Trainor (Jun 30, 2015) Season 7, Episode 8 - Performer ("All the Small Things") Performer ("All the Small Things") See fewer
I Love the 2000s (2014)
(TV Mini-series) - Performer ("All the Small Things") (1 episode, 2014) Performer ("All the Small Things") (1 episode, 2014) See fewer
2000 (Jun 17, 2014) Season 1, Episode 1 - Performer ("All the Small Things") Performer ("All the Small Things") See fewer
(TV Series) - Performer ("I Miss You") (1 episode, 2014) Performer ("I Miss You") (1 episode, 2014) See fewer
Reunion (Mar 19, 2014) Season 2, Episode 4 - Performer ("I Miss You") (uncredited) Performer ("I Miss You") (uncredited) See fewer
Rude Tube (2013)
Super Pranks (Oct 6, 2013) Season 7, Episode 5 - Performer ("All the Small Things") (uncredited) Performer ("All the Small Things") (uncredited) See fewer
Cinematic Excrement (2012)
Once Upon a Christmas (Dec 22, 2012) Season 3, Episode 13 - Performer ("I Won't Be Home For Christmas") Performer ("I Won't Be Home For Christmas") See fewer
Conan (2011)
(TV Series) - Performer ("After Midnight") (1 episode, 2011), Themselves - Musical Guest (1 episode, 2011) Performer ("After Midnight") (1 episode, 2011), Themselves - Musical Guest (1 episode, 2011) See fewer
Armageddon Comes to Quiznos (Dec 8, 2011) Season 2, Episode 16 - Themselves - Musical Guest, Performer ("After Midnight") Themselves - Musical Guest, Performer ("After Midnight") See fewer
Made in Chelsea (2011)
(TV Series) - Performer ("Love Is Dangerous") (1 episode, 2011), Performer ("Even If She Falls") (1 episode, 2011) Performer ("Love Is Dangerous") (1 episode, 2011), Performer ("Even If She Falls") (1 episode, 2011) See fewer
Je Suis Amoreuse De Toi (Nov 14, 2011) Season 2, Episode 9 - Performer ("Love Is Dangerous") Performer ("Love Is Dangerous") See fewer
How Do They Find Flamingo Roadkill? (Nov 7, 2011) Season 2, Episode 8 - Performer ("Even If She Falls") Performer ("Even If She Falls") See fewer
20 to 1 (2010–2011)
(TV Series) - Performer ("All The Small Things") (2 episodes, 2010) Performer ("All The Small Things") (2 episodes, 2010) See fewer
Adults Only 20 to 1: Sizzling Supermodels (Mar 8, 2011) Season 10, Episode 3 - Performer ("All The Small Things") (uncredited) Performer ("All The Small Things") (uncredited) See fewer
Our All Time Favourite Films (Jun 23, 2010) Season 9, Episode 11 - Performer ("All The Small Things") (uncredited) Performer ("All The Small Things") (uncredited) See fewer
Video on Trial (2008)
Totally Beachin' Video on Trial (Mar 9, 2008) Season 3, Episode 16 - Performer ("All the Small Things") Performer ("All the Small Things") See fewer
The Ark of Madness (2007)
(TV Special) - Performer ("What's My Age Again", "Grandpa", "Feeling This") Performer ("What's My Age Again", "Grandpa", "Feeling This") See fewer
Cavemen (2007)
(TV Series) - Performer ("Man Overboard") (1 episode, 2007) Performer ("Man Overboard") (1 episode, 2007) See fewer
Pilot (Apr 30, 2007) Season 1, Episode 0 - Performer ("Man Overboard") Performer ("Man Overboard") See fewer
Meet the Barkers (2005)
(TV Series) - Performer ("Feeling This", "All the Small Things", "The Rock Show", "Down") (1 episode, 2005) Performer ("Feeling This", "All the Small Things", "The Rock Show", "Down") (1 episode, 2005) See fewer
It's Moving Day for the Barkers! (Apr 6, 2005) Season 1, Episode 1 - Performer ("Feeling This", "All the Small Things", "The Rock Show", "Down") Performer ("Feeling This", "All the Small Things", "The Rock Show", "Down") See fewer
The School Trip (2004)
(TV Movie) - Composer (song "All the Small Things"), Performer ("All The Small Things") Composer (song "All the Small Things"), Performer ("All The Small Things") See fewer
Laguna Beach: The Real Orange County (2004)
(TV Series) - Soundtrack (1 episode, 2004), Performer ("Feeling This", "What's My Age Again", "First Date", "I Miss You") (1 episode, 2004) Soundtrack (1 episode, 2004), Performer ("Feeling This", "What's My Age Again", "First Date", "I Miss You") (1 episode, 2004) See fewer
The Best Part of Breaking Up (Oct 2, 2004) Season 1, Episode 6 - Performer ("Feeling This", "What's My Age Again", "First Date", "I Miss You") Performer ("Feeling This", "What's My Age Again", "First Date", "I Miss You") See fewer
What Happens in Cabo (Oct 26, 2004) Season 1, Episode 5 - Soundtrack ("All the Small Things") Soundtrack ("All the Small Things") See fewer
Tru Calling (2004)
Reunion (Jan 22, 2004) Season 1, Episode 10 - Performer ("All The Small Things") Performer ("All The Small Things") See fewer
(TV Series) - Blink-182 (1 episode, 2003), Performer ("All The Small Things") (1 episode, 2003) Blink-182 (1 episode, 2003), Performer ("All The Small Things") (1 episode, 2003) See fewer
Barting Over (Feb 16, 2003) Season 14, Episode 11 - Blink-182 (voice) (as blink-182), Performer ("All The Small Things") Blink-182 (voice) (as blink-182), Performer ("All The Small Things") See fewer
Daria (1999–2000)
(TV Series) - Performer ("What's My Age Again?") (1 episode, 1999), Performer ("Adam's Song") (1 episode, 2000) Performer ("What's My Age Again?") (1 episode, 1999), Performer ("Adam's Song") (1 episode, 2000) See fewer
Of Human Bonding (Apr 14, 2000) Season 4, Episode 7 - Performer ("Adam's Song") Performer ("Adam's Song") See fewer
Just Add Water (Aug 11, 1999) Season 3, Episode 12 - Performer ("What's My Age Again?") Performer ("What's My Age Again?") See fewer
(TV Series) - Performer ("Adam's Song") (1 episode, 2000) Performer ("Adam's Song") (1 episode, 2000) See fewer
Blind Date (Feb 9, 2000) Season 1, Episode 14 - Performer ("Adam's Song") (uncredited) Performer ("Adam's Song") (uncredited) See fewer
Saturday Night Live (2000)
(TV Series) - Performer ("All the Small Things", "What's My Age Again?") (1 episode, 2000), Themselves - Musical Guest (1 episode, 2000) Performer ("All the Small Things", "What's My Age Again?") (1 episode, 2000), Themselves - Musical Guest (1 episode, 2000) See fewer
Jamie Foxx/Blink-182 (Jan 8, 2000) Season 25, Episode 9 - Themselves - Musical Guest, Performer ("All the Small Things", "What's My Age Again?") (uncredited) Themselves - Musical Guest, Performer ("All the Small Things", "What's My Age Again?") (uncredited) See fewer
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redpajama_set_name: RedPajamaCommonCrawl


text:
Xyrosaris celastrella is een vlinder uit de familie van de stippelmotten (Yponomeutidae). De wetenschappelijke naam van de soort werd in 1903 gepubliceerd door Kearfott.

Stippelmotten

redpajama_set_name: RedPajamaWikipedia


There was a time when the word "fusion," as well as all of the attempts at jazz/rock hybridization to which it applied, was anathema in many music circles. Highbrow critics were loath to see jazz's maiden flower despoiled by the randy rhythms of rock, and rock fans rued the attenuation of the mighty riff by strange harmonies and lengthy solo digressions.
All of that notwithstanding, Aaron Lebos is forced to fess up. "I don't like to use the term, but we're fusion," says Lebos of his Miami-based trio, the Aaron Lebos Reality. "And if you stay true to the word – it refers to a 'fusion' of different styles – that's definitely what we are.
Having received his Master's degree in jazz performance from the University of Miami some years back, Lebos is an in-demand touring and session musician, having worked with a veritable who's who of South Florida performers. Drummer Rodolofa Zuniga is similarly situated, laden with teaching gigs at three South Florida colleges, and boasting a sideman resume that includes world tours with Julio Iglesias.
Having played together on many projects past, the two men founded the Aaron Lebos Reality some six years ago. (Original bassist Eric England, also an accomplished session man, is departing soon, his departure necessitated by a relo to L. A.).
Lebos' is an egalitarian brand of fusion; the Reality is not so much a guitarist's solo project as a band that happens to led by a guitarist. And while Lebos likes to stretch out when the moment is right — he's a tasty, accessible player, setting up his jazzier extended runs with Jeff Beck-ish rock phrases and bits of blues — other Reality members and guests are afforded equal time in the sun.
And his compositions, while still colored by curious harmonies and the occasional odd time signature, are nonetheless structured around simple melodies, undergirded by simmering funk.
"If there is a difference between us and what I might call a 'real' fusion group, it's that our songs are still built around the group, and there's a stronger melodic element," Lebos says. "And funk has become more of an influence in what we do the last couple years or so. A lot of our tunes have a very definite pocket.
The Aaron Lebos Reality will play Preservation Pub Friday, Nov. 10 at 8 p.m.


A friend of mine recently brought up the topic of running and of course I became very excited. She proceeded to tell me that she was considering running a half marathon and wanted to know if there is a specific training program that I follow or recommend.
Now let's just be clear, when I started my racing I never really had the interest of following a training program but if that is what you want to do then go for it. But if here is what I told her and what I will tell all of you novices.
When I started my training I was already running on average 4 to 5 miles a day on the treadmill. I immediately moved outside which is a big change for anyone because instead of running in place on a downhill incline which is what level 0 is on a treadmill, you are pushing yourself forward. So yes it will be harder. My suggestion is to start out by running 3 miles outside. Once you can run 3 miles outside, 5 days a week without stopping, begin increasing your mileage. So start running 4 miles every day. If that becomes even easier then move on to 5, then 6 then 7. For me running 7 miles a day 4-5 days a week is quite an accomplishment, especially for the novice.
After you are able to log 6-7 miles a day, why not go a run a 10k? It will get you acclimated with the racing scene, chips, and bibs. Plus it will give you practice running in a crowd of people.
Now here comes the part that everyone dreads. The long runs. Thankfully because you are running a half marathon, you don't have to put in the 20 + mile runs but you should have tackled at least 11 miles by race day. So every other weekend or every weekend if you prefer, put in a long run. So instead of running 5 days a week (that is if you are) run 4 days and log a longer run on the weekend. Start off by running 9, then 10, then 11. And the good thing about this, is that you can make your last long run the weekend before the big race to allow your body to taper.
For myself when I was training, I wanted to make sure that I could run a half marathon, and to this day even before a race, I like to run 13 miles. Because if you are used to logging 10 or 11 miles as your long runs and you find yourself exhausted after 11, what is going to happen when you need to keep running an extra 2.1 come race day? So I suggest, running 13 but like I said everyone is different.
Make sure you rest though. Every person is different, sometimes I rest once per week sometimes twice but you need to give your muscles time to rebuild.
If you follow this type of regimen I guarantee you will be ready to run a half marathon.
IT Band? Is that why my leg hurts?


WIN in our fabulous "Christmas Flavours"
The topic is "Christmas Flavours"
Your favourite ingredient, dish, the family enjoying Christmas dinner or the dog with the holiday bone - whatever reminds you of Christmas and glorious food!!
BOOK: Age 7-10 years. I'm a very active seven year old. During the school holidays I got into BIG TROUBLE and my parents decided to send me to my grandparents place 300 miles away. Great stocking filler from Kiwi author E M Godfrey-Dagg. Plus check out lots more great summer reads!
VOUCHERS: Got a movie lover in the family? Why not treat them to an E-Gift Card or book of vouchers from Hoyts. Let them see their favourite movies first!!
CLOTHING: Restyle Boutique in Cammish Lane, Orewa have a huge selection of clothing, accessories, shoes and jewellery for all occasions. Come in and find that funky or fabulous garment at the best prices!
ALCOHOL: Manly Liquor wide range of bubbles to celebrate Christmas and welcome in the New Year including Lindeaur Special Reserve, Leveret IQ Brut, Veuve Cliquot, Freixenet Brut and more. For details check online or come and visit us in store in Manly Village!


Mark the dates now, if you haven't already, for to 2019 annual Lowell Celebrates Kerouac Festival for October 10-14.
This year will be observing the 50th anniversary of Jack's passing in October of 1969, and our Parker Lecturer, Nancy Fox, will offer her perspective on Kerouac's literary and cultural legacy a half-century after he left us. And, at this year's Commemorative at the Commemorative, the jazz group, Revolutionary Snake Ensemble, will lead a jazz memorial parade through Kerouac Park in memory of Jack!
We will also be offering special remembrances of two very significant person's in Jack's life who passed away since our last gathering: Billy Koumentzalis and Al ("Big Ed Dunkel") Hinkle.
The timeless David Amram and his trio will perform at Zorba's on Friday night; and—back by popular demand!—Vance Gilbert with bring his musical and poetic magic to Zorba's on Saturday night.
And, of course, they'll be tours, open mics, a poetry workshop, art exhibits, special presentations by both Cathy (Silva) Cassady and Brian Hassett, and the annual Amram Jam on Sunday afternoon.
And stay tuned—there's more to come!
Lodging Information: The U-Mass. Lowell Inn and Conference Center is pretty well booked already for an event they are hosting that weekend. We have made arrangements with Lowell's Courtyard Marriott for lodging for LCK attendees this year. It's off Exit 3 on the Lowell Connector, about a 10 minute drive to downtown Lowell. Free parking in Lowell at the Lowell National Historical Park Visitors Center parking lot.
Room rates are $139.00 for a single and $159.00 for a double—plus taxes.
You can reserve by calling 800-321-2211 or 978-458-7575 and say you're reserving through Lowell Celebrates Kerouac.
The Beat Museum in San Francisco is hosting a celebration for the 100th birthday of Lawrence Ferlinghetti throughout March 2019. For more information, see the Feb 25 email from The Beat Museum.
Also: we're hosting a birthday party for Jack Kerouac here in Lowell on March 9, but The Beat Museum is hosting a a birthday bash in San Francisco on March 12.
Students and Lowell community members are invited to read The Haunted Life book and participate in discussion with UML English faculty on the evenings of 13 February and 27 February 2019. Participants will also be invited to attend a dress rehearsal of the production at the Merrimack Repertory Theatre.
Hello all, here's an update on LCK festival events over this past weekend. If you have any stories or pictures or videos you'd like to share from your time at the festival, please get in touch with us at info@lowellcelebrateskerouac.org.
Record numbers came out to celebrate the 30th anniversary of the dedication of the Jack Kerouac Commemorative in Kerouac Park on Bridge Street.. Speakers included Brian Foye, Richard Scott, city officials and others.
Record numbers also participated in the new downtown walking tour by Kurt Phaneuf, judge at Lowell High School Poetry Contest and of "Talking Jack" fame.
New venues that participated in the festival included Western Avenue Studios, Gormley's Cafe, and Gallery Z.
See you in March for Jack's birthday celebration and in October for the next LCK festival!
The Pollard Memorial Library in Lowell hosted a marathon reading of On the Road on March 10. Over 100 people participated over the course of 11 hours. Check out their writeup of the event for pictures and details.
An opening reception for an exhibit of LCK Festival posters from 1988 to 2017 will be held at the Greater Lowell Community Foundation from 5:00 to 7:30pm on Thursday, March 17. GLCF is located on the second floor at 100 Merrimack St. in Lowell. The exhibit will run through May.
Please download and post a flier and invite others to attend. See you there.
Lowell, MA—Merrimack Repertory Theatre (MRT) announces the first work of its 2018-19 40th Season as a brand new adaptation of Jack Kerouac's lost novel The Haunted Life. The novel was inspired by the author's childhood and upbringing in Lowell, Massachusetts, and then thought lost. The recently discovered manuscript was put together with letters and outlines by Associate Professor of English at UMass Lowell Todd F. Tietchen, and published by Da Capo Press.
The Haunted Life novel will be adapted by MRT Artistic Director Sean Daniels (whose play The White Chip was featured in MRT's 2015-16 Season), and produced in collaboration with Jim Sampas, Literary Executor of the Estate of Jack Kerouac.
The Haunted Life will premiere at MRT with performances March 20 – April 14, 2019. Season subscriptions are available now at mrt.org or by calling 978-654-4678; single tickets go on sale July 30, 2018.
The remaining six plays in MRT's 2018-19 Season will be announced on Tuesday, March 6, 2018, at 6:00 pm, at an event at the theatre at 50 East Merrimack Street, Lowell; it is free and open to the public.
The new adaptation will serve as the centerpiece of MRT's 2018-19 Season, which is its 40th Anniversary Season, as well as a celebration of the City of Lowell that influenced the novel—a diverse and historic city whose support of the arts is made vividly clear in its motto: "Art is the Handmaid of Human Good." The piece will also showcase the highly talented and diverse actors and designers MRT has become known for.
As the country decides if it wants to enter the war, a father and son try to make peace at home.
Set in Lowell, Massachusetts, young Peter Martin must decide whether to listen to his conservative father who believes the Democratic President (Roosevelt) is corrupt and flooding the country with immigrants or whether he wants to follow his own youthful thinking or perhaps just escape it all and join the merchant marines. Full of Kerouac's gorgeous and poetic prose, The Haunted Life asks us all which road we are going down.
The Haunted Life will mark MRT's second time producing the work of Jack Kerouac. In October 2012, MRT presented a staged reading of Kerouac's only work written for the stage, Beat Generation, as part of the University of Massachusetts Lowell's "Jack Kerouac Literary Festival." Beat Generation ran for eight performances and received national attention, including a review from Rolling Stone.
Jack Kerouac was an American novelist and poet. Kerouac was born and raised in Lowell, MA, before moving to New York City, where he became a founding member of the Beat Generation, the literary movement of the 1950s and 1960s which embraced non-conformity, exploration, and freedom across cultural, social, and religious lines. His debut novel The Town and the City was published in 1950. He is best known for his novel On the Road, published in 1957, which was adapted into a feature film in 2012. Kerouac died in 1969 at the age of 47. He is buried in Lowell, MA. To learn more about the Estate of Jack Kerouac, visit www.kerouacproductions.com and www.jackkerouac.com.
Merrimack Repertory Theatre (MRT) has been Merrimack Valley's professional theatre company since 1979 and is an integral part of Lowell's identity as the cultural heart of the region. MRT produces vibrant, contemporary plays that explore what it means to be alive today. A seven-show season runs from September through May in the intimate 279-seat Nancy L. Donahue Theatre. The company is known as a leader in producing new plays, especially world and regional premieres. MRT is one of 72 theatres nationwide (one of three in Massachusetts) with membership in LORT (the League of Resident Theatres).


text:
\section*{Propagator and occupation fraction of two states}\label{three}
\textit{Propagator and occupation fraction of two states}. Suppose that the particles are initialized at the origin.
The propagator $p(x,t)$ represents the PDF of finding the particle at position $x$ at time $t$. For the two-state process, it is natural to concern which state the particles are located in at time $t$. Here we denote the joint PDF of finding the particle at position $x$ and state `$\pm$' at time $t$ as $p_\pm(x,t)$, which is associated with the propagator by the relation $p(x,t)=p_+(x, t)+p_-(x,t)$. The subscript `$\pm$' will imply an identical meaning for other quantities.

The integral equations for $p_\pm(x,t)$ can be similarly obtained as the master equations for CTRWs.
Besides the sojourn time distribution $\psi_\pm(t)$ and survival probability $\Psi_\pm(t)$, we introduce the notation $G_\pm(x,t)$ to represent the conditional probability that a particle makes a displacement $x$ during sojourn time $t$ at one step in state `$\pm$'. Their expressions are given by
\begin{align}
    &G_+(x,t)=\delta(|x|-v_0t)/2,  \\
    &G_-(x,t)=\frac{1}{\sqrt{4\pi Dt}}\exp\left(-\frac{x^2}{4Dt}\right),
\end{align}
since the state `$+$' represents L\'{e}vy walk and state `$-$' denotes Brownian motion, respectively. Then the transport equation governing flux of particles $\gamma_\pm(x,t)$, which defines how many particles leave the position $x$ and change from state `$\mp$' to state `$\pm$' per unit time, satisfies,
\begin{equation}
\begin{split}
    \gamma_\pm(x,t)&= \int_0^tdt'\int_{-\infty}^{\infty}dx'\psi_\mp(t')G_\mp(x',t')\gamma_\mp(x-x',t-t')  \\
                 &~~~+p^0_\mp\psi_\mp(t)G_\mp(x,t),
\end{split}
\end{equation}
where the constant $p^0_\pm$ is the initial fraction of two states, that is $p_\pm(x,t=0)=p^0_\pm\delta(x)$.
The current density $p_\pm(x,t)$ of particles is connected to the flux $\gamma_\pm(x,t)$
\begin{equation}
  \begin{split}
  p_\pm(x,t)&=\int_0^t dt'\int_{-\infty}^\infty dx' \Psi_\pm(t')G_\pm(x',t')\gamma_\pm(x-x',t-t')  \\
            &~~~+p^0_\pm \Psi_\pm(t)G_\pm(x,t).
  \end{split}
\end{equation}

By means of the techniques of Laplace and Fourier transform, $\tilde{\hat{p}}_\pm(k,s)=\int_0^\infty dt\int_{-\infty}^\infty dx e^{-st}e^{ikx}p_\pm(x,t)$ can be obtained (see Supplemental Material). Besides, the occupation fraction of two states $p_\pm(t)$, as the marginal density of finding the particles in state `$\pm$' at time $t$, can be obtained by taking $k = 0$ in $\tilde{\hat{p}}_\pm(k,s)$. The expression of $p_\pm(t)$ in Laplace space $(t\rightarrow s)$ is
\begin{equation}\label{ps}
  \hat{p}_{\pm}(s)=\frac{p_{\pm}^0+p_{\mp}^0\hat{\psi}_{\mp}(s)}{1-\hat{\psi}_+(s)\hat{\psi}_-(s)}
  \cdot\frac{1-\hat{\psi}_{\pm}(s)}{s},
\end{equation}
the normalization of which can be confirmed by verifying $\hat{p}_+(s)+\hat{p}_-(s)=1/s$.

\textit{EAMSD and TAMSD}. If one is eager for more information of a process, such as the TAMSD, the propagator $p(x,t)$ at a single point is not enough. Instead, the two-point velocity correlation function $\langle v(t_1)v(t_2)\rangle$ plays a crucial role. We will calculate it firstly and then show the generic results of EAMSD and TAMSD for the aging process $x_{t_a}(t)$. The age $t_a$ means that this process has evolved for a time period $t_a$ before we start to observe it, and $t$ is the measurement time.

Since the model we considered contains two states: L\'{e}vy walk and Brownian motion, represented by symbols `$+$' and `$-$', respectively. The velocity correlation function could be written as a sum of four possible cases in terms of different states:
\begin{equation}\label{vv}
\begin{split}
\langle v(t_1)v(t_2) \rangle&=\langle v_+(t_1)v_+(t_2) \rangle+\langle v_-(t_1)v_-(t_2) \rangle\\
                            &~~~+\langle v_+(t_1)v_-(t_2) \rangle+\langle v_-(t_1)v_+(t_2) \rangle.
\end{split}
\end{equation}
The first term on the right-hand side represents the case that the velocity process $v(t)$ are in L\'{e}vy walk phase at both time points $t_1$ and $t_2$; other terms stand for similar parts of the correlation function.
For the first term, the velocity is correlated only when there is no renewal happens between $t_1$ and $t_2$. Thus, we have
\begin{equation}\label{vv1}
  \langle v_+(t_1)v_+(t_2) \rangle = v_0^2 p_+(t_1) p_{+,0}(t_1,t_2),
\end{equation}
where $p_+(t)$ has been given in \eqref{ps} and $p_{+,0}(t_1,t_2)$ is the PDF that no renewal happens between times $t_1$ and $t_2$ in state `$+$'. Similarly, the second term on the right hand side of \eqref{vv} is
\begin{equation}\label{vv2}
\begin{split}
    \langle v_-(t_1)v_-(t_2) \rangle = 2D\delta(t_1-t_2) p_-(t_1) p_{-,0}(t_1,t_2),
\end{split}
\end{equation}
where $p_{-,0}(t_1,t_2)=1$ for $t_1=t_2$, since there must be no renewals within a zero time lag. The two states at times $t_1$ and $t_2$ are different in the last two terms on \eqref{vv}. Therefore, the velocity at $t_1$ and $t_2$ are independent. Considering the velocity is unbiased at any time, the last two terms are void.

Note that the PDFs $p_\pm(t)$ and $p_{+,0}(t_1,t_2)$ should be calculated firstly to obtain the velocity correlation function in \eqref{vv}. The former one has been given in \eqref{ps}, while the double Laplace transform $(t\rightarrow s,\tau\rightarrow u)$ of the latter PDF $f_{+,0}(t,\tau)=p_{+,0}(t,t+\tau)$ is \cite{GodrecheLuck:2001}
\begin{equation}\label{ps1s20}
\hat{f}_{+,0}(s,u)= \frac{s-u+u\hat{\psi}_{+}(s)-s\hat{\psi}_{+}(u)}{s(s-u)(1-\hat{\psi}_{+}(s))u}.
\end{equation}
It seems not easy to perform the inverse Laplace transform on $\hat{f}_{+,0}(s,u)$. Instead, we can obtain the expression of $p_{+,0}(t_1, t_2)$ in Laplace space ($t_1\rightarrow s_1, t_2\rightarrow s_2$) by substituting variables  (see Supplemental Material):
\begin{equation}\label{ps1s2}
\begin{split}
\hat{p}_{+,0}(s_1,s_2)=  \frac{1+\hat{\psi}_+(s_1+s_2)-\hat{\psi}_+(s_1)-\hat{\psi}_+(s_2)}{s_1s_2(1-\hat{\psi}_+(s_1+s_2))}.
\end{split}
\end{equation}
Taking inverse Laplace transform on \eqref{ps1s2} becomes doable.
Based on \eqref{ps} and \eqref{ps1s2}, the velocity correlation function $\langle v(t)v(t+\tau)\rangle$ in \eqref{vv} can be obtained for different sojourn time distributions $\psi_\pm(t)$. Noticing the asymptotic forms of $p_\pm(t)$ and $p_{+,0}(t,t+\tau)$ for large $t$, the velocity correlation function can be rewritten in the scaling form as
\begin{equation}\label{vtvttau}
\begin{split}
\langle v(t)v(t+\tau)\rangle &=\langle v_+(t)v_+(t+\tau)\rangle+\langle v_-(t)v_-(t+\tau)\rangle\\
                            &\simeq C_1t^{\nu_1-2}\rho\left(\frac{\tau}{t}\right)+C_2t^{\nu_2-1}\delta(\tau),
\end{split}
\end{equation}
where the parameters $\nu_1,\nu_2$ and the scaling function $\rho(\cdot)$ are determined by $p_\pm(t)$ and $p_{+,0}(t,t+\tau)$. The scaling form \eqref{vtvttau} helps to show different scaling behaviors of $\langle v(t)v(t+\tau)\rangle$ for different sojourn time distributions $\psi_\pm(t)$, and brings convenience to give a generic expressions of MSDs \cite{DechantLutzKesslerBarkai:2014,MeyerBarkaiKantz:2017}.

Now we focus on the aging process $x_{t_a}(t)$. The EAMSD of this aging process is defined as $\langle x_{t_a}^2(t)\rangle=\langle (x(t_a+t)-x(t_a))^2\rangle$, which can be obtained through the scaling form in \eqref{vtvttau}. For weak aging $t_a\ll t$ and strong aging $t_a\gg t$ cases  (see Supplemental Material), it behaves as
\begin{equation}\label{EA}
  \langle x_{t_a}^2(t)\rangle\simeq
  \left\{
    \begin{array}{ll}
      K_1 t^{\nu_1}+K_2 t^{\nu_2}, & t_a\ll t, \\
      K_3 t_a^\beta t^{\nu_1-\beta}+C_2 t_a^{\nu_2-1}t, & t_a\gg t,
    \end{array}
  \right.
\end{equation}
where the coefficients $K_1=2C_1/\nu_1\int_0^\infty dt (t+1)^{-\nu_1 }\rho(t)$, $K_2=C_2/\nu_2$ and $K_3=2c_1C_1[(\nu_1-\beta-1)(\nu_1-\beta)]^{-1}$.
Here $c_1$ depends on the asymptotic form of scaling function $\rho(z)\simeq c_1 z^{-\delta_1}$ for small $z$, and
$\beta$ is the exponent of the variance of velocity in the L\'{e}vy walk phase for large $t$ \cite{DechantLutzKesslerBarkai:2014}, i.e.,
\begin{equation}
  \langle v_+^2(t)\rangle=v_0^2p_+(t)\propto t^{\beta}.
\end{equation}

When constructing single particle tracking experiments, the aging process $x_{t_a}(t)$ is evaluated in terms of its TAMSD, which is defined as $\overline{\delta_{t_a}^2(\Delta)}=1/(T-\Delta)\int_{t_a}^{t_a+T-\Delta}dt [x(t+\Delta)-x(t)]^2$ with $\Delta$ denoting the lag time and $T$ the total measurement time \cite{MetzlerJeonCherstvyBarkai:2014}. The TAMSD is calculated in the limit $\Delta\ll T$ to obtain good statistics.
Weak ergodicity breaking is the common phenomenon of a majority of anomalous diffusion. Similarly to the procedure of calculating EAMSD, we obtain the ensemble-averaged TAMSD as (see Supplemental Material):
\begin{equation}\label{TA}
  \langle\overline{\delta_{t_a}^2(\Delta)}\rangle\simeq
  \left\{
    \begin{array}{ll}
      \frac{K_3}{1+\beta} \,T^{\beta}\Delta^{\nu_1-\beta}+K_2 T^{\nu_2-1}\Delta, & t_a\ll T, \\
      K_3 t_a^\beta \Delta^{\nu_1-\beta}+C_2 t_a^{\nu_2-1}\Delta, & t_a\gg T.
    \end{array}
  \right.
\end{equation}

There are at least four findings being worth to report from the observations of the generic results of EAMSDs in \eqref{EA} and TAMSDs in \eqref{TA}.
(i) All the four mentioned formulae consist of two parts (one from L\'{e}vy walk phase and another one from Brownian phase). The exponents of evolution time $t$ or time lag $\Delta$ in these two parts might be different from the ones of the corresponding individual L\'{e}vy walk and Brownian motion. This is because the PDF $p_\pm(t)$ in \eqref{ps} plays a weighted role on L\'{e}vy walk and Brownian motion. Besides, the sums of exponents of the time variables (including $t,t_a,T,\Delta$) in individual two parts are $\nu_1$ and $\nu_2$, respectively, whatever it is EAMSD or TAMSD, and weak or strong aging cases.
(ii) The exponents of time variables in weak and strong aging cases are closely related for TAMSD in \eqref{TA}. While keeping the exponents of $\Delta$ invariant and replacing measurement time $T$ by age $t_a$, the result for strong aging case is obtained from the one of weak aging case.
In other words, the TAMSD for weak aging case only depends on $T$ and $\Delta$, while in the same way it counts on $t_a$ and $\Delta$ for strong aging cases.
(iii) The EAMSD and TAMSD in weak aging case do not depend on the age $t_a$, the results of which are identical to the non-aging case $t_a = 0$. In contrast, they explicitly depend on $t_a$ for strong aging case, which implies that the exponents $\beta$ and $\nu_2-1$ of $t_a$ must be zero if the equilibrium initial ensemble (i.e., $t_a\rightarrow\infty$ discussed in last section) of this system exists (see specific case $2$ in Table \ref{table}). And in this case, the TAMSD will be the same for weak and strong aging cases, and only depends on $\Delta$.
(iiii) Comparing the strong aging EAMSD and the mean of TAMSD \eqref{TA}, it can be noted that
\begin{equation}
  \langle x_{t_a}^2(\Delta)\rangle = \langle\overline{\delta_{t_a}^2(\Delta)}\rangle \quad {\rm for }~ t_a\gg T,
\end{equation}
which shows that the aging seemingly makes the weak ergodicity breaking system to be ergodic. It is clear that for any $\alpha_-$ Brownian motion is ergodic in its own phase. However, for TAMSD in L\'{e}vy walk phase, there are some differences between $\alpha_+<1$ and $1<\alpha_+<2$. For $1<\alpha_+<2$, the mean sojourn time in L\'{e}vy walk phase is finite, individual trajectories become self-averaging at sufficiently long (infinite) times, such that there will be no difference between $\overline{\delta_{t_a}^2(\Delta)}$ obtained from different trajectories and ensemble-averaged quantity $\langle\overline{\delta_{t_a}^2(\Delta)}\rangle$ \cite{GodecMetzler:2013,FroembergBarkai:2013}. While for $\alpha_+<1$, the characteristic time scale is infinite, then the individual TAMSD $\overline{\delta_{t_a}^2(\Delta)}$ is irreproducible and inequivalent with the corresponding EAMSD.

\textit{Specific cases}. Since both $\alpha_+$ and $\alpha_-$ go through the range $(0,2)$, it can be divided into six cases as shown in Table \ref{table}. See the detailed derivations of parameters $\nu_1,\nu_2$, and $\beta$ for these cases in (Supplemental Material).
It seems tedious to discuss the EAMSDs and TAMSDs individually for six different cases of $\alpha_\pm$. In fact, they can be organized into three categories to deepen understandings of the two-state process by considering the properties of its ingredients --- L\'{e}vy walk and Brownian motion. It is well-known that the standard L\'{e}vy walk performs ballistic diffusion when the exponent of the distribution of running times $\alpha<1$ and sub-ballistic superdiffusion when $1<\alpha<2$, which is faster than the normal diffusion of Brownian motion. Based on this understanding, the Brownian phase undoubtedly suppresses the diffusion behavior of L\'{e}vy walk. This effect may be durable or transient, which is completely determined by the fraction of two states $p_\pm(t)$, or more essentially, the magnitude of the exponents $\alpha_\pm$. From this point of view, the three categories are: (i) $\alpha_+$ and $\alpha_-$ are comparable, including the first two cases in Table \ref{table}; (ii) $\alpha_+$ is smaller, including the middle two cases in Table \ref{table}; (iii) $\alpha_-$ is smaller, including the last two cases in Table \ref{table}.

\begin{table}
\centering
\caption{Values of several major parameters of EAMSD and TAMSD in \eqref{EA} and \eqref{TA} for six cases with different $\alpha_\pm$.}\label{table}
\begin{tabular}{|l|l|l|l|}
  \hline

  specific cases & $\nu_1$ & $\nu_2$ & $\beta$ \\
\hline
  1. $\alpha_+=\alpha_-<1$ & $2$ & $1$ & $0$ \\
  2. $1<\alpha_\pm<2$ & $3-\alpha_+$ & $1$ & $0$ \\
  3. $\alpha_+<\alpha_-<1$ & $2$ & $\alpha_+-\alpha_-+1$ & $0$ \\
  4. $\alpha_+ < 1 < \alpha_- < 2$ & $2$ & $\alpha_+$ & $0$ \\
  5. $\alpha_-<\alpha_+<1$ & $\alpha_--\alpha_++2$ & $1$ & $\alpha_--\alpha_+$ \\
  6. $\alpha_-<1<\alpha_+<2$ & $\alpha_--\alpha_++2$ & $1$ & $\alpha_--1$ \\
  \hline
\end{tabular}
\end{table}

\begin{figure*}[tbhp]
\begin{minipage}{0.31\linewidth}
\includegraphics[scale=0.36]{fig-main-1}
\end{minipage}
\begin{minipage}{0.31\linewidth}
\includegraphics[scale=0.36]{fig-main-2}
\end{minipage}
\begin{minipage}{0.31\linewidth}
\includegraphics[scale=0.36]{fig-main-3}
\end{minipage}
\caption{TAMSD of the two-state process for different sets of $\alpha_\pm$. Black circles and squares represent the simulation results of the mean value of TAMSD averaging over 200 realizations, and the solid lines are the theoretical ones (with small and large asymptotic forms in \eqref{TA}). (a): case (i) with $\alpha_+=1.5,\alpha_-=1.8$ and measurement time $T=200$. The simulation results agree with the theoretical ones for small time $(\sim\Delta)$ and large time $(\sim\Delta^{3-\alpha_+})$. (b): case (ii) with $\alpha_+=0.6,\alpha_-=1.5$ and measurement time $T=20426$. The asymptotic behavior $\sim\Delta^2$ for large time is observed. The simulation and theoretical results do not coincide for small $\Delta$ in strong aging case, since the coefficient $t_a^{\alpha_+-1}$ in front of $\Delta$ in \eqref{case2} is too small and another term $\Delta^2$ dominates. (c): case (iii) with $\alpha_+=1.5,\alpha_-=0.8$ and measurement time $T=9830$. The asymptotic behavior $\sim\Delta$ for short time can be observed. It does not coincide for large $\Delta$ in strong aging case, since the coefficient $t_a^{\alpha_--1}$ in front of $\Delta^{3-\alpha_+}$ in \eqref{case3} is too small and another term $\Delta$ dominates. Therefore, there is not much difference between the strong aging simulations and the whole solid (yellow) line with slope $1$ for large $\Delta$.}\label{figure}
\end{figure*}

As representatives of the above three situations, we choose three sets of parameters: (i) $\alpha_+=1.5,\alpha_-=1.8$, (ii) $\alpha_+=0.6,\alpha_-=1.5$, and (iii) $\alpha_+=1.5,\alpha_-=0.8$. The corresponding TAMSDs for weak and strong aging cases are simulated and shown in Fig. \ref{figure}. The TAMSDs for other cases and EAMSDs are presented in (Supplemental Material). The theoretical TAMSDs for these three cases can be obtained from \eqref{TA} as:
\begin{equation}\label{case1}
 \textrm{(i)}~ \langle \overline{\delta^2_{t_a}(\Delta)}\rangle \simeq
  \left\{
    \begin{array}{ll}
      2D_2\Delta^{3-\alpha_+}+\frac{2D\mu_-}{\mu_++\mu_-}\Delta, & t_a\ll T, \\
      2D_2\Delta^{3-\alpha_+}+\frac{2D\mu_-}{\mu_++\mu_-}\Delta, & T\ll t_a,
    \end{array}
  \right.
\end{equation}
\begin{equation}\label{case2}
  \textrm{(ii)}~\langle \overline{\delta^2_{t_a}(\Delta)}\rangle \simeq
  \left\{
    \begin{array}{ll}
      v_0^2\Delta^2+\frac{2D\mu_-}{a_+\Gamma(1+\alpha_+)}T^{\alpha_+-1}\Delta, & t_a\ll T, \\
      v_0^2\Delta^2+\frac{2D\mu_-}{a_+\Gamma(\alpha_+)}t_a^{\alpha_+-1}\Delta, & T\ll t_a,
    \end{array}
  \right.
\end{equation}
\begin{equation}\label{case3}
  \textrm{(iii)}~\langle \overline{\delta^2_{t_a}(\Delta)}\rangle \simeq
  \left\{
    \begin{array}{ll}
      2D_4T^{\alpha_--1}\Delta^{3-\alpha_+}+2D\Delta, & t_a\ll T, \\
      2D_4\alpha_-t_a^{\alpha_--1}\Delta^{3-\alpha_+}+2D\Delta, & T\ll t_a.
    \end{array}
  \right.
\end{equation}
For the first category (i), a stationary of the fractions of two states $p_\pm(t)$ can be achieved for long times, that is, $p_\pm(t)$ tends to a constant not equal to $0$ or $1$ (see Supplemental Material). Then the EAMSD and TAMSD are the combination of the fraction of analogues of individual L\'{e}vy walk and Brownian motion whether it is weak aging or strong aging.
For the second category (ii) with $\alpha_+<\alpha_-$ where $p_+(t)\rightarrow1$ as $t\rightarrow\infty$, the L\'{e}vy walk phase in state `$+$' tends to occupy the whole time. Then the results are naturally similar to an individual L\'{e}vy walk, except for the small asymptotic form $\Delta$ resulting from Brownian phase.
For the third category (iii) with $\alpha_+>\alpha_-$, by contrast, now $p_-(t)\rightarrow1$ as $t\rightarrow\infty$ and the L\'{e}vy walk phase in state `$+$' gradually withdraws from the two states in a power-law way. This power-law way suppresses the diffusion of L\'{e}vy walk phase and gives the opportunity to Brownian motion to be the leading term when $\alpha_+-\alpha_->1$.
In conclusion, compared to the EAMSD and TAMSD of individual aging L\'{e}vy walk \cite{MagdziarzZorawik:2017} and Brownian motion, it can be found that the fraction $p_\pm(t)$ in a two-state process plays a crucial role. It contributes a power term of $\Delta$ to weak aging EAMSD, a power term of $T$ to weak aging TAMSD, and a power term of $t_a$ to strong aging EAMSD and TAMSD.

The model L\'{e}vy walk interrupted by rest has attracted considerable attention in physics \cite{SolomonWeeksSwinney:1993,KlafterZumofen:1994} and biology \cite{SongMoonJeonPark:2018}.
The EAMSD and TAMSD for this model can be obtained by taking the diffusivity $D$ in Brownian phase to be zero. It has been pointed that all the results above consist two parts corresponding to L\'{e}vy walk and Brownian motion, respectively. Taking $D = 0$ just eliminates the latter part and brings no effect on the former part of L\'{e}vy walk phase. For L\'{e}vy walk interrupted by rest, the asymptotic behavior of small $\Delta$ in TAMSD disappears and subdiffusion behavior might exist if $\alpha_+-\alpha_->1$.

\textit{Initial ensemble}. In general, the standard L\'{e}vy walk model is a non-Markovian process and so is the two-state process alternating between L\'{e}vy walk and Brownian motion with power-law distributed sojourn time.
It is natural to consider the effects of the initial ensembles of the particles.
It is called a nonequilibrium initial ensemble \cite{Cox:1962,KlafterZumofen:1993} if all particles are introduced to the system at $t = 0$ without any prehistories. In contrast, if the particles have been evolving for time $t_1$ before we start to measure this system, we call this system with equilibrium initial ensemble when $t_1\rightarrow\infty$ \cite{Cox:1962,KlafterZumofen:1993}. The EAMSD of standard L\'{e}vy walk has been shown to be different for different initial ensemble \cite{ZaburdaevDenisovKlafter:2015,WangChenDeng:2019}. Note that the equilibrium initial ensemble exists only if the sojourn times in two states `$\pm$' both have finite first moments, i.e., $1 <\alpha_\pm < 2$ in our concerned model.

For nonequilibrium initial ensemble, the corresponding EAMSD $\langle x^2(\Delta)\rangle$ and TAMSD $\overline{\delta^2(\Delta)}$ can be obtained by taking $t_a=0$ in previous section, i.e.,
\begin{equation}
  \begin{split}
    \langle x^2(\Delta)\rangle = \langle x_{t_a}^2(\Delta)\rangle |_{t_a=0},  \quad
    \overline{\delta^2(\Delta)} = \overline{\delta_{t_a}^2(\Delta)} |_{t_a=0}.
  \end{split}
\end{equation}
Since the results of the weak aging case (i.e., $t_a\ll\Delta$) with different sojourn time pairs $\psi_\pm(t)$ in Eqs. (\ref{EA}) and (\ref{TA}) are independent of $t_a$, they are indeed the results for nonequilibrium initial ensemble. When $1<\alpha_\pm<2$, the results of the strong aging case (i.e., $t_a\gg T$) in \eqref{case1} are independent of $t_a$. Therefore, the EAMSD $\langle x^2_{\textrm{eq}}(\Delta)\rangle$ and TAMSD $\langle\overline{\delta^2_{\textrm{eq}}(\Delta)}\rangle$ for equilibrium initial ensemble ($t_a\rightarrow\infty$) are
\begin{equation}
  \langle x^2_{\textrm{eq}}(\Delta)\rangle=\langle\overline{\delta^2_{\textrm{eq}}(\Delta)}\rangle
  \simeq2D_2\Delta^{3-\alpha_+}+ \frac{2D\mu_-}{\mu_++\mu_-}\Delta.
\end{equation}
If the sojourn times are so long that the mean sojourn time diverges, there is no sense in talking about the equilibrated initial ensemble. However, the asymptotic behaviors of strong aging case $t_a\gg\Delta$ can still be investigated (see Supplemental Material). There is a special case $0<\alpha_+=\alpha_-<1$, where the particles reach a balance that each half of them are located in each of the two states and the EAMSD and TAMSD are both independent on the age $t_a$, that is,
\begin{equation}
  x^2_{t_a}(\Delta)\rangle = \langle\overline{\delta^2_{t_a}(\Delta)}\rangle
  \simeq \frac{v_0^2}{2}\Delta^2 +D\Delta
\end{equation}
for sufficiently large $t_a$. If $\alpha_+\neq\alpha_-$ and at least one of them less than $1$, then neither an equilibrium initial ensemble nor a balance for long time exists. The state with small exponent $\alpha_\pm$ of sojourn time distribution will dominate the MSD for long times. One can see this phenomenon in the last four cases in Table \ref{table}. In these cases, the EAMSD and TAMSD for strong aging cases all consist of two parts corresponding to L\'{e}vy walk and Brownian motion. One of the parts is independent on $t_a$ while another part contains a power term of $t_a$ with a negative exponent. The latter part tends to zero as $t_a\rightarrow\infty$ and the former one dominates, which corresponds to the state with smaller exponent $\alpha_\pm$ of sojourn time distributions.

\textit{Conclusion}. It often happens that a single-state process cannot sufficiently describe the observed physical and biological phenomena. Two-state process is a kind of simple but important model to characterize some of these phenomena. A Langevin equation with two diffusion modes (fast and slow diffusion modes) has been investigated in \cite{MiyaguchiAkimotoYamamoto:2016}, where a transient subdiffusion and the non-Gaussian propagator for short time are observed for a nonequilibrium ensemble.
In this report, we consider a two-state process with fast phase (L\'{e}vy walk) and slow phase (Brownian motion), which is also the intermittent search process for finding rare hidden targets. It is not easy to model the process with two completely different phases by a Langevin equation.
By contrast, we resort to the velocity process $v(t)$, which also consists of two states. Based on the velocity correlation function, we obtain the generic expressions of the EAMSD and TAMSD for different sojourn time distributions.

One of the key contributions of this report is to explicitly discuss the relation between EAMSD and TAMSD.
In particular, the weak and strong aging cases are also considered for these MSDs since the measurement in experiments might not begin at the start of the process concerned. It is found that the occupation fraction plays a weighed role in L\'{e}vy walk phase and Brownian phase, and the MSDs are just a combination of these two parts.
The meticulous discussions on the aging MSDs are helpful to understand the two-state process and to analyze the experimental data.

If taking the diffusivity $D$ to be zero in Brownian phase, we obtain another important process --- L\'{e}vy walk interrupted by rest.
Taking $D=0$ just eliminates the contributions from Brownian phase.
From another aspect of the two-state process, we find the fact that the slow phase, whether it is rest or Brownian motion, suppresses the diffusion behavior of L\'{e}vy walk if its sojourn time is longer than that of L\'{e}vy walk phase. The mechanism is similar to the trap event \cite{GoldingCox:2006} in CTRW models.
Compared to them, there exist some other models describing the suppression of  the diffusion of L\'{e}vy walk with different mechanism, such as the L\'{e}vy walk with memory in running time \cite{ChenWangDeng:2019} and the walker moving in a heterogeneous medium \cite{KaminskaSrokowski:2018}.

\textit{Acknowledgments}. This work was supported by the National Natural Science Foundation of China under grant no. 11671182, and the Fundamental Research Funds for the Central Universities under grant no. lzujbky-2018-ot03.

redpajama_set_name: RedPajamaArXiv


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text:
Q: Why is font-family render differently on iOS? I'm using monospace for dollar sign my website, I get the result I'm looking for on chrome / windows and mobile phone but font render different on iOS? Why is the font display different? Is there a way to fix it?

A: It would be helpful if you provided the CSS code that you are using but I'm guessing you are doing something like this
font-family: monospace;

The reason this looks different on different operating systems is that "monospace" doesn't actually refer to a particular font it refers to any font where "All glyphs have the same fixed width" so each browser has a different font that it uses for "monospace".
If you would like your font to be consistent across different browsers and operating systems you will need to specify a particular font. This article from MDN explains how to specify font on the web https://developer.mozilla.org/en-US/docs/Learn/CSS/Styling_text/Web_fonts

A: Chrome font for monospace is consolas , you can check each font using chrome://fonts. Think this might be useful to someone

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text:
Tyreke Smith, Ohio State DE | NFL Draft Scouting Report
By Oliver Hodgkinson
Tyreke Smith NFL Draft Profile
Tyreke Smith Scouting Report
Tyreke Smith's Player Profile
Impressive senior season comes before a difficult decision
Smith's career at Ohio State
Lacking the prolific production to matchup to the NFL potential
Tony Pauline's Scouting Report on Tyreke Smith
In recent years, Ohio State has become a pipeline for sending defensive ends to the NFL. Can Tyreke Smith add his name to an illustrious list in the 2022 NFL Draft? Although he isn't a name currently grouped with the top players at the position ahead of the upcoming college football season, Smith's scouting report reveals that the Ohio State DE has the athletic potential to be a coveted prospect next April.
School: Ohio State
Current Year: Senior
Wingspan: 81″
Arm: 33 5/8″
Hand: 10 3/8″
As a physical specimen, Smith is extremely impressive. The 6'3″, 260-pound pass rusher is exceptionally athletic. He possesses delightful change of direction ability, remarkable lateral agility, and excellent play speed. The Ohio State DE can often combine these attributes to breeze past opposing offensive linemen with what looks to be relative ease.
As a pass rusher, Smith converts speed to power exceptionally well. Although he has a few weapons in his pass-rush armory, he leans on his ability to overwhelm tackles with his strength. Smith appears to have respectable length for the position, which again helps from a pass-rush perspective. The Buckeye also demonstrates the ability to be disruptive as a pass rusher from both sides of the formation.
With athleticism, strength, and length, Smith can be a potent pass-rush force around the outside track and attacking from the interior.
Furthermore, his athleticism enables him to efficiently drop back from the line of scrimmage and into coverage. He can backpedal with some impressive fluidity. That element of versatility will prove valuable at the next level.
There's no denying that Smith has the physical attributes to continue the Ohio State DE reputation in the NFL Draft. However, he is far from a complete prospect, with some areas of his game requiring significant attention if he is to make the leap to the NFL.
Smith will need to display more impressive football intelligence this fall to elevate his 2022 NFL Draft stock. He had some issues anticipating the snap in the games studied, with the bout against Clemson a glaring example. Although he improved as the game progressed, he was routinely the last defensive lineman to react to the snap.
The Ohio State DE will need to turn pressure into production better this coming season. Although sometimes a by-product of the offensive scheme faced, Smith needs to ensure he works on timing and his pass-rush plan to significantly impact the opposition next fall. He can achieve this with more consistent use of the weapons that are in his toolbox.
Smith may not be a highly coveted NFL Draft prospect right now, but he's only a few years removed from being a highly sought-after high school recruit. A four-star defensive end by 247 Sports, Smith was the fourth-ranked player at the position in the 2018 class while featuring in the top-50 prospects that year. As a result, he was in high demand, entertaining over 35 offers following an initial bid from the in-state Ohio Bobcats.
Having attended an Ohio State camp in 2016, the Buckeyes were always a front runner to capture the young defensive end. Yet, heading into his senior campaign, Smith remained uncommitted — well, publicly anyway.
As revealed in an article from The Athletic, he had quietly committed to Penn State in August 2017. Having experienced institutionalized racism first-hand, the African-American coaching staff of the Nittany Lions offered a welcoming environment that also struck a chord with the rest of the Smith family.
Meanwhile, Smith embarked on a dominant senior season for Cleveland Heights, earning the Cleveland.com Defensive Player of the Year Award. Flashing his incredible athletic ability, he amassed 70 tackles, 23 tackles for loss, and 11 sacks while snagging 8 receptions for 192 yards and 4 touchdowns. An accomplished all-around athlete, Smith was the leading scorer for the basketball team.
Following the conclusion of his senior season, Smith was faced with a difficult decision. Turning his back on his commitment to Penn State, he headed across the Big Ten to the Buckeyes. The newest Ohio State DE pointed to the program's heritage at the position when announcing his commitment.
"Ohio State, coach [Urban] Meyer, and coach [Larry] Johnson are great people," he told 247 Sports. "It's my home state, a great school, and coach Johnson has developed great linemen like Nick Bosa."
Despite Smith's impressive high school performances, one of the alluring aspects of the Buckeyes ensured he had a slow start to his career. Entering an Ohio State DE rotation stacked with talent, he had little opportunity to make a significant impact. As a true freshman in 2018, Smith saw action in 11 games. Still, he logged just 9 tackles that included a career-high 3 tackles against Tulane.
Smith's sophomore season was beset with injuries. A groin issue meant he missed the season opener and several more games in September. Despite the injury setback, the Ohio State DE steadily began to assert himself on the Buckeyes' opponents. He secured his first sack against Cincinnati while registering multiple more against Maryland. The sophomore defensive lineman finished the season with 12 tackles, 5 tackles for loss, 3 sacks, and a pair of pass breakups.
With Chase Young's departure to the NFL, Smith's opportunities increased in the shortened 2020 college football season. Against Rutgers and Michigan State, he equaled his career-high single-game tackle numbers.
The Ohio State DE was impactful in the College Football Playoffs semifinal win over Clemson with a pass breakup. Yet, he only ended the year with 9 tackles, 2 tackles for loss, and 2 sacks. Nevertheless, he did tie for the team lead with 33 QB pressures.
Smith's opportunity to add to that figure in the national championship was denied due to his enforced isolation. Although he'd miss the final game of the season, it wouldn't be the last of his Buckeyes' career.
The Ohio State DE announced his return for the upcoming college football season. In doing so, Smith has the distinct possibility of elevating his NFL Draft stock. The athletic pass rusher has all the physical attributes to become an impressive NFL player. If Smith can put it all together this season, he could be in contention for an early-round selection.
Positives: Undersized college pass rusher who displays a lot of athleticism. Effective standing over tackle and coming out of a three-point stance, rushes the edge with speed, and possesses a closing burst. Works his hands to protect himself, nicely redirects to ball handlers, and gives effort defending the run. Fires off the snap with a quick first step and plays with excellent pad level as well as balance. Agile, easily changes direction, and works hard.
Negatives: Lacks elite speed and bulk. Easily out-positioned from the action. Slow getting off blocks.
Analysis: Smith was a solid defender for Ohio State and made a good number of plays behind the line of scrimmage. He projects as a pass-rush specialist at the next level with possibilities in a variety of schemes.


text:
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    return 0;
}

- (void)child:(RFBHandler *)handler finishedJob:(NSDictionary *)job onConnection:(RFBConnection *)connection
{
    DLogError(@"SHOULD NOT CALL ME!");
}

@end

redpajama_set_name: RedPajamaGithub


At St. John's, we have been fortunate to see our parish grow over the last few years. Foyer Dinner Groups (from the French word "foier" meaning "hearth" or "home") are a new way to foster connectivity among parishioners in a smaller setting outside of our larger, parish-wide events.
St. John's Foyer Dinner Groups will be small groups of roughly 8 parishioners who meet throughout the year for simple meals and conversation. There is no formal agenda, nor any assignment; we request only that each group say grace before meals. Groups will be (re)formed each year and are made up of singles, couples, young parishioners, retirees, etc. Newcomers are invited and encouraged to join a group at any time.
Each group will meet roughly 4 times during the year. Meetings typically take place in the home of group members and meals are intended to be simple and shared, including the preparation; the host may provide a main course while members of the group help to round out the meal by bringing side dishes, appetizers or desserts.
Please note there is no need to be concerned that your house is not grand enough to host, nor your culinary skills gourmet enough to share. Our focus is on friendship and fellowship!
While most groups will represent a cross-section of the church, to accommodate families with young children, you may opt to be paired with other young families so that children may be included in the gatherings. You may also choose to make use of the St. John's Babysitter Database to participate in an Adult Foyer Group. Please note during sign-up whether you'd like to be joined with a Family Foyer Group (children included) or an Adult Foyer Group (grown-ups only at gatherings).
If signing up as a couple, please add both names.
Food allergies? Anything else we should know?
Thank you for signing up for St. John's Foyer Groups! A coordinator will email you once you have been assigned to a group.


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Q: How can i display the primeng p-tree after filter selection in a breadcrumb format? I am using primeng P-tree for displaying the nodes items for selection ...

and if i select random 4 ...i am displaying parents and nested parent as well of the selected child as under image

and after adding filtermode(true) to p-tree tag and i got search input to find node item in p-tree
and after search particular node item its filtering as needed as below image

after selection of 4 , it is not displaying nested parent and child node items (2 and 4)...its displaying only parent node item (1) as below image

I am attaching the stackblitz url for reference :- https://stackblitz.com/edit/primeng-treeselection-demo-m1dapf?file=src%2Fapp%2Fapp.component.html,src%2Fapp%2Fapp.component.ts
Please help me on these issue.
Thanks in advance.


Cold water immersion and ice baths are one of the most common recovery methods used in elite sports. Athletes have been taught that ice baths will help reduce inflammation post intense exercise and improve speed of recovery, which is a tantalising promise.
Despite it's popularity, there are significant doubts on how effective cold water immersion is at improving recovery. Below we take a look at the evidence for and against ice baths.
WHAT IS COLD WATER IMMERSION?
Cold Water Immersion (CWI) or Cold Therapy (cryotherapy) is the process of submerging part of or multiple parts of your body into cold water for an extended period of time. The aim of this is to improve markers of recovery and reduce muscle soreness post exercise.
DO ICE BATHS IMPROVE RECOVERY?
Machado et.al (2015) found that cold water immersion is "slightly better than passive recover". However, passive recovery involved participants remaining seated and doing nothing….
Lastly Roberts et al. (2015) looked at the effects of cold water immersion on muscle mass (muscle hypertrophy) after a 12-week strength training program. They found that cold water immersion post strength training sessions actually reduced long term gains in muscle mass and strength by blunting the activation of key proteins and satellite cell (markers of muscle growth) in skeletal muscle for up to 2 days after strength exercise.
A trial by Broatch et al. (2014) found that cold water immersion is no more effective than a placebo in improving ratings of readiness for exercises and pain post high intensity exercise.
ARE THERE ANY PSYCHOLOGICAL BENEFITS OF ICE BATHS?
We're glad you asked! Unfortunately, no research has looked into the psychological benefits of cold water immersion post intense exercise. Though anecdotally it is said to improve team/social cohesion when performed in a group. When performed alone, it can be an almost meditative practice.
11-15 degrees celsius is the proposed ideal temperature.
11-16 minutes is the proposed ideal total submersion time.
Longer durations and colder temperatures can be harmful to some. So be wise!
1. Machado, A. F., Ferreira, P. H., Micheletti, J. K., de Almeida, A. C., Lemes, Í. R., Vanderlei, F. M., … & Pastre, C. M. (2016). Can water temperature and immersion time influence the effect of cold water immersion on muscle soreness? A systematic review and meta-analysis. Sports Medicine, 46(4), 503-514.
2. Broatch, J. R., Petersen, A., & Bishop, D. J. (2014). Postexercise cold water immersion benefits are not greater than the placebo effect. Medicine & Science in Sports & Exercise, 46(11), 2139-2147.
3. Roberts, L. A., Raastad, T., Markworth, J. F., Figueiredo, V. C., Egner, I. M., Shield, A., … & Peake, J. M. (2015). Post‐exercise cold water immersion attenuates acute anabolic signalling and long‐term adaptations in muscle to strength training. The Journal of physiology, 593(18), 4285-4301.


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after a long search for an original shade i give up and build it myself.
the material is a piece of plastics bought from a bookbinder. the diameter is 110mm, lenth 150mm (6 inch), manufactoring expense 4$, building time 1 hour.
following this very simpel idea you can build a custom lens shade for your tele, or to set limits to an excessiv circle of coverage. another benefit is the storage space needed. for my specific shade 150x380x0,8mm. smaller hoods can except thiner material.
Don't you get vignetting when you use front movements?
it depend on the movements. in this combination i could rise the lens 30mm. if i should need more i could shift the hood backwords.
hiking with styrofoam cups might be difficult, however i think the biggest advantage is the minimal storage space needed.