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Preschool teachers do the identical sport through indulging the youngsters into these types of sorts of arts. There are a assortment of topics and thus it gets to be not hence easy in the direction of take the simplest. Many crayon containers provide coloration charts that assistance youngsters toward take the straight colors toward seek the services of on a printable coloring web site.
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Net is applied in direction of uncover the cost-free printable coloring internet pages of your necessity.
Cartoon people are likely in direction of constantly tumble inside of and out of style. They are a ideal route in the direction of order the small children together and engage them in a enjoyment loaded and finding out expertise.
Absolutely free printable coloring pages for children are a fairly favourable course of unleashing the creativeness in kids at a amazingly small age. This website web page will indeed aid within just that area!
The least difficult portion with regards to Thanksgiving coloring pages and other getaway coloring internet pages is that not simply can they be colored and exhibited, nevertheless they can in addition provide as templates for other crafts. Or he can obtain the prints after he is accomplished with the artwork on the web. What pleases you even further? The child who is satisfied and chaotic or the a single who is usually complaining of not taking the stuff he needs in the direction of shade. Far too, they provide instruction in the direction of children and offer you them a come to feel of how in the direction of hire colors.it assists them happen a very good comprehending of arts which will help them later on upon within their lives.
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There are therefore plenty of on the internet printable coloring internet pages that your self can have a blast selling them in the direction of your small children. Most children difference what they would which includes to colour sometimes. The easiest element is that these webpages are amazingly straightforward upon the pocket and almost absolutely everyone can consider them. Products and services together with Disney and Pixar are using this likelihood in direction of boost their cartoon people concerning small children. If on your own really don't have a printer at property yourself can sometimes hire all those at the regional library towards print the coloring web pages for a fairly very little amount.
However, it just isn't basically at household that they come inside of handy. Coloring expertise is specially the useful activity. Furthermore, mothers and fathers appreciate to perspective their youngster preoccupied in such resourceful pursuits. Of study course, that is my opinion!
This is an additional excellent world wide web web site with a wealth of content that your self can employ including Thanksgiving coloring and craft strategies. All just one necessities to present their small children Those best toys is a computer with net partnership and a printer.
Aside towards the over advantages there are a couple other advantages of having absolutely free printable coloring internet pages for small children. They present a outstanding awareness against producing these kinds of routines inside their youngsters. Such pages can be achieved upon every single and every single variety of subject. These web pages assist acquire a really feel of coordination and establish their conclusion and focus at a incredibly early age. Just one of the least difficult factors pertaining to these printable pages is that oneself can just take them for absolutely free. No even further difficulty toward pick the store, move there and try out finding the most loved cartoon temperament of your baby. Perhaps yourself will not comprise children of your personalized yet yourself generally comprise friends and family that arrive around with their younger types.
Oneself can print these web pages within just sets of five or 10 and supply them toward your baby towards shade. All by yourself need to have toward do is move towards some web sites and get started printing.
One, the preferred animated characters are not often accessible for sale. Parents can on top of that consider offline materials including bookshops which provide a bunch of these types of publications taking colour internet pages inside of. He is all via himself to experiment and learn. Here are some of my highest favorite websites.
These sites are easy in direction of track down upon the website and they offer the kid with a possibility in direction of examine his creative imagination. By yourself can find holiday vacation web pages inside of many spots upon the World wide web that are totally free for down load directly toward your printer.
Do on your own will need some guidelines for web websites that oneself can move to as a result your self can identify Thanksgiving coloration internet pages? Perfectly, I think I can guidance oneself. Many think that training throughout the curriculum (incorporating all issue elements into a lesson plan) is a Good direction in the direction of assist a baby master. Include crayons and other materials on hand for them and they will sense Pretty welcome inside of your household.
Presently optimum properties include a printer on hand and that generates it quick and easy to seek the services of on the net printable coloring webpages. This will deliver entertainment toward by yourself as soon as on your own watch how your youngster incorporates presented the visual appearance toward the printable coloring pages. That will avoid the anxiety for children as they hesitate. Being a mother or father oneself have to identify time in direction of buy all the coloring stuff but if yourself transfer on the internet there is a treasure of coloring websites that await by yourself. Consequently, free printable coloring webpages for kids is a Really successful and affordable route in direction of interact your kids inside a fruit filling sport that will not simply just be exciting yet will additionally assist create their motor abilities together with hand – eye coordination.
Often you comprise toward stop by excess than a single keep in direction of uncover the coloring book of your child's decision. Make it possible for them in direction of opt for some coloring sheets that oneself can print for them. Type "coloring-pages" or any key word with Coloring sheets including Disney coloring-pages into any biggest appear engine and you would view tens of millions of glance results presenting printable it.
You can locate plenty of clip arts with slightest alterations but with alternative subject factors either, for that reason there is a proceeding treatment of setting up, producing and having of these types of university clip arts by way of a great deal of us citizens. The minuscule effort and hard work it requires in direction of compile an on have to have coloring guide is great importance the smile on your child's lips.
Cost-free coloring-page considerably encouraging on your own in the direction of inculcate your children with regards to varying factors; their names, shades as perfectly as colours. There are much too moms and dads that incorporate to provide their little ones alongside with them for business. It too enables the dad and mom towards be in a position in the direction of communicate with other grown ups and not incorporate thus plenty of interruptions. Inside of reality, by yourself could possibly truly feel Fantastic above crafting a listing of Good internet sites the place different on the internet printable coloring web pages can be discovered. They additionally have many other components of their internet web page that focus upon other holiday seasons such as Cinco De Mayo and Kwanzaa.
With a great deal and a lot of Thanksgiving internet pages as very well as other holiday pages and resources for instructors and residence schooling mom and dad, this is a superior world wide web web site in the direction of uncover guidance with all types of subjects towards art in the direction of heritage to geography. As a college or university instructor, I am relatively familiar with plenty of spots that consist of absolutely free printables. Apart in opposition to staying a pleasurable crammed sport they in addition guidance children establish their practical experience concerning Those festivals. If your self are a higher education teacher or merely a hectic mother or father, Thanksgiving shade internet pages can be a lifesaver every time you are hunting for a course towards hold your child active for a positive time period of time. They bounce more than versus one particular theme or a person preset of people in the direction of the next. From time to time online printable coloring internet pages can be supplied for insightful themes, vacations, or even coloring contests.
The range of them that are offered ensures that youngsters of unique ages can obtain anything at all that they would be content material with.


This month on Live Sigma Kappa, we're talking 'friendship'… something that's very near and dear to my little heart.
Hop over to LSK to see my post and to let me know what you think!
In a small bowl, dissolve the yeast in warm water for about 10 minutes. Stir well. In a 2 quart glass or plastic container, combine flour and granulated sugar. Whisk thoroughly or the flour will get lumpy when you add the milk. Slowly add warm milk and dissolved yeast mixture to the flour/sugar mixture. Loosely cover the bowl with a lid or plastic wrap. The mixture will get bubbly. Consider this Day 1 of the cycle, or the day you receive the starter. On Day 2, transfer the mixture to a large Ziploc bag and mush. Continue following directions as written below.
For the next 10 days handle the starter according to the instructions below for an Amish Friendship Bundt.
Day 1 - Receive the starter and do nothing.
Day 2 - Mush the bag.
Day 3 - Mush the bag.
Day 4 - Mush the bag.
Day 5 - Mush the bag.
Day 6 - Add to the bag 1 cup each of flour, sugar and milk. Mush the bag.
Day 7 - Mush the bag.
Day 8 - Mush the bag.
Day 9 - Mush the bag.
1. Pour the entire contents of the bag into a non-metal bowl.
2. Add the additional 1-1/2 cups flour, 1-1/2 cups sugar and 1-1/2 cups milk in the above ingredients. Stir.
3. Measure one cup batter into four 1-gallon Ziploc bags and give to friends along with a copy of the recipe.
4. Preheat oven to 325 degrees F.
5. Add to the remaining batter the ingredients for the Bundt.
6. Grease a large, non-metal bundt pan.
7. Continue with the 'Cinnamon Streusel' ingredients and directions below.
Mix all ingredients together. Make your Amish Friendship Bundt according to the above directions. Sprinkle about a 1/2 cup of streusel mix around the bottom of the bundt pan. Then, scrape about 1-1/2 cups of batter into the pan and spread into the crevices. Batter will be thick. Top with the remaining streusel mix, then add your remaining batter. Bake for one hour. Cool the bundt for about 10 minutes, or until it loosens evenly from the pan.
It's imperative that you do not use any type of metal spoons or bowls for mixing. Also, do not refrigerate. Batter will rise, bubble, and ferment naturally... burp as needed. You can also make this in two non-metal loaf pans.
That looks like a tasty bundt cake!
I remember this from when I was a kid! My mom's friend gave us a starter and I thought it was the most amazing cake ever! I should have known it wouldn't be difficult to recreate on my own!
Next post: Mocha-Nut Cupcakes for Cupcake Camp Dallas 2012!


(10) To deny one's self in order to follow Christ (cf Mt 16:24; Lk 9:23).
Denial has come to mean, not facing reality. This is not the type of "denial" that St. Benedict is promoting. Rather it is just the opposite, it is to deny the falsehood of the self that always feels threatened. This false "self" does not exist but is the result of Original Sin and we all struggle with it throughout our lives.
There is a part of us that feels that we must always be vigilant unless someone get one up on us. It is the part of our personality that puts up walls, that is afraid to be our true selves. Simply it is that part of us that fears being embarrassed, thought ill of or that we secretly fear is the definition of who we really are and we work tirelessly to keep everyone from learning the truth.
Of course, the truth is that this is not who we really are at all.
We are just the opposite of the Son of God. Jesus was God but as St. Paul says in Philippians, "did not deem equality with God." Jesus ate and drank with sinners, he associated with some very ungodly people.
None of us has to battle such odds. We are not God, but as the fruit of original sin we have all inherited the notion that we are supposed to be God. So most of us spend our lives not exercising the talents and gifts that God has blessed us with because we fear that we will fail to use them perfectly.
I wonder how many there are who have been graced with the gift of healing the sick but who never reach out to the sick because they fear the embarrassment that might come their way? Or how many talented leaders stand idly by while those not gifted lead?
Denying oneself means letting go of the fears that we do not possess abilities of god proportions and stepping out in faith knowing that God will provide what is lacking to our talents as we exercise them for the good of humanity.
Perhaps the most commonly told parable by Jesus about the Kingdom of God is that of the King or landowner who passes out talents before taking a trip. Those who invest in their talents are praised upon the Master's return whereas the one who buries his talents is condemned.
Why did the servant bury his talents? Because he was afraid.
Why does Jesus tell the parable? So his followers will not fall into the same predicament. Yet how many Christians will hear the words, deny yourself and immediately interpret the Lord's words as though he were advocating burying one's talents? Unbelievable!
Deny the fear of making a mistake, taking a risk of what might happen if you follow Our Lord to Jerusalem. The disciples told Jesus that if they went to Jerusalem he certainly would be killed, did he not fear for his life? Thomas often cast as the doubter but in fact probably the supreme believer says, "let us go to die with him!"
When we let go of the fear of what others think about us when it comes to using the talents and abilities that God has given us then we will truly build the Kingdom of God. Denying that part of ourselves that would bury our talents our of fear is true humility.


Used for both Mother and Father.....good policy.
If you lose a close family member you are allowed several days for the morning.
good, either 3 or 5 days as i recall.
It was fair. I did use this.
What can you tell job seekers about SAIC's Bereavement Leave?"
Glassdoor is your resource for information about the Bereavement Leave benefits at SAIC. Learn about SAIC Bereavement Leave, including a description from the employer, and comments and ratings provided anonymously by current and former SAIC employees.


text:
Recent Media Coverage of YLJ Essays
Julie Wang
Legal Theory Blog has recently recommended two Yale Law Journal essays: Abbe R. Gluck's Intrastatutory Federalism and Statutory Interpretation: State Implementation of Federal Law in Health Reform and Beyond; and Michael C. Dorf and Neil Siegel's forthcoming YLJO essay, "Early-Bird Special" Indeed!: Why the Tax Anti-Injunction Act Permits the Present Challenges to the Minimum Coverage Provision. Mike Sacks and John Celock also feature a discussion of Dorf and Siegel's essay in their recent Huffington Post article, Supreme Court Can't Dodge Health Care Law's Fate Under Bill From GOP Lawmaker.
In Intrastatutory Federalism and Statutory Interpretation: State Implementation of Federal Law in Health Reform and Beyond, published in the December 2011 issue, Abbe R. Gluck explores the oft-ignored topic of state implementation of federal law. Gluck raises the question of whether doctrine should protect "intrastatutory federalism," which she defines as the "informal federalism" that emerges when states carry out acts of Congress. She argues that statutory interpretation canons fail to address the complicated issues that arise in the intrastatutory-federalism context, and she suggests a range of possible doctrinal responses to this increasingly prevalent phenomenon.
In "Early-Bird Special" Indeed!: Why the Tax Anti-Injunction Act Permits the Present Challenges to the Minimum Coverage Provision, Michael C. Dorf and Neil Siegel examine whether the Tax Anti-Injunction Act (TAIA) bars the Supreme Court from reviewing the current challenges to the Patient Protection and Affordable Care Act (ACA). While most of the commentary on the TAIA issue has focused on the question of whether the ACA's penalty provisions fall within the TAIA's definition of "tax," Dorf and Siegel adopt an alternative and original approach. Dorf and Siegel argue that the TAIA does not bar the review because "the present challenges to the ACA do not have 'the purpose' of restraining tax assessment or collection." That purpose must be immediate because if the TAIA extended to challenges with the indirect purpose of restraining tax assessment or collection, it would also bar tax refund suits. ACA challenges cannot have the direct purpose of barring review because "the very authority to assess or collect will not exist until long after the litigation is concluded."

redpajama_set_name: RedPajamaCommonCrawl


text:
Brachyorrhos est un genre de serpents de la famille des Homalopsidae.

Répartition
Les espèces de ce genre sont endémiques des Moluques en Indonésie.

Liste des espèces
Selon  :
 Brachyorrhos albus (Linnaeus, 1758)
 Brachyorrhos gastrotaenius (Bleeker, 1860)
 Brachyorrhos pygmaeus Murphy & Voris, 2021
 Brachyorrhos raffrayi (Sauvage, 1879)
 Brachyorrhos wallacei Murphy et al., 2012

Publication originale
 Schlegel, 1826 : Notice sur l'Erpétologie de l'île de Java ; par M. Boie. Bulletin général et universel des annonces et des nouvelles scientifiques, , .

Liens externes

Notes et références

Homalopsidae
Genre de serpents (nom scientifique)
Faune endémique des Moluques
Reptile d'Indonésie

redpajama_set_name: RedPajamaWikipedia


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    $q->_model = 'Estimate';

    return $q;
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redpajama_set_name: RedPajamaGithub


Established in 1993, located off of Quebec Street in Highlands Ranch, the practice prides itself in the personal touch you find in independently owned businesses while still having the latest in cutting-edge technology to take care of your family's eyes.
Ortho-Eyes, also known as Corneal Refractive Therapy, are custom designed contact lenses that function similar to retainers for your teeth. Ortho-Eyes are worn at night while you sleep and literally reshape your cornea to reduce or eliminate your need for daytime glasses and contact lenses to see in the distance. They are an excellent alternative to surgery, wearing glasses or traditional contact lenses. For people that enjoy sports, the outdoors and hiking 14ers (like Dr. Jacobs) they give freedom from glasses and no hassles in dusty, dirty settings as regular contact lenses sometimes do. Additionally, studies show and HD Eye Care patients confirm that Ortho-eyes lenses reduce or stop the rate of deterioration of your vision when worn nightly. This has particular appeal for children and teens whose vision typically worsens as they grow.
HD Eye Care also offers complete eye care for patients of all ages and a wide variety of designer frames. One of the things Dr. Jacobs is most proud of is the personal touch patients experience during their visit. Many of the staff are familiar faces to patients because they have been with his office for many years- a fact that speaks to the family and community values of HD Eye Care.


Oddities for a Fumble Table!
SO a while back I posted (via Twitter) a link I found to a ridiculous Combat Fumble Table (obviously intended to be taken with tongue firmly planted in . . . cheek)! But it has garnered enough attention, and generated suffiicient amusement, that it is probably worth doing an Oddities list for it, as we have done in the past with 100 Oddities for a Creepy Old House, or any of our other best selling Oddities titles on DrivethruRPG.
Credit goes to Dyson Logos, of Dyson's Dodecahedron for the original concept. Also check there for Fantastic Maps for your games!
Here's a d20's worth to start, but feel free to add to the nonsense - can we get this up to a d100 table before Monday?
1 - Roll your damage dice seven times, discard the lowest roll. Take the rest as damage.
2 - You pretend to be juggling your weapon, Make a Dexterity or Performance check, or suffer rolled damage.
3 - Your weapon shatters into an appealing fractal pattern dealing rolled damage to you and any allies within 3d12 feet.
4 - Take one die from each of your opponents, roll them and add the result. Take that damage.
5 - Consign the offending die to the betrayer pile, take a pic of the die and post about how it betrayed you.
6 - Throw the offending dice at the wall. Take the rolled damage.
7 - You have done so poorly that you inspire a drinking game: Roll damage for your attack, take that many shots.
8 - You miss and spin around, impaling your weapon in the hindparts of the nearest donkey.
9 - Your attempt is so ludicrous that your intended target takes 1d4 internal damage from uncontrollable laughter.
10 - Your fumble has attracted the wrath of a scornful deity, who will subject you to a stormcloud that hovers over your head, occasional lightning bolts and mocking celestial laughter for 1d6+1d4+1d3+1d2 days.
11 - You hear the sound of a rimshot on a snare drum, but suffer no other torment.
12 - roll 2d3 for the number of allies you afflict, divide your roll damage by the result, inflicting that amount on each of them.
13 - Never mind - just go . . .
14 - Your attack was so terrible that you kill yourself AND raise your self immediately as undead.
15 - You and your target each lose your next action, as you share a moment of hilarity.
16 - Your attack inscribes the first letter of your opponent's name in your own backside.
17 - Succeed at a Will Save (Difficulty = to your damage roll) to bear the scorn of your opponent's sneer, then attack immediately at +10.
18 - Swear an oath never to fight again, take up the life of a monk, or (if male) a nun.
19 - You trip, falling 3d100 yards.
20 - You apologize for not giving this your best effort, and ask your opponent if he would mind if you went again.


text:
MJ over Kobe not a slam dunk
By Bucky Gleason|Published Sat, Dec 20, 2014 |Updated Thu, Nov 17, 2016
ESPN.com ran a poll last week asking fans who would have the better career when Kobe Bryant eventually retired, him or Michael Jordan. It was a layup, right?
More than two-thirds said it wasn't even close, that it was MJ all the way. Twenty-eight percent said it was a close call. Five percent picked Kobe.
The results were predictable if only because they revealed only 33 percent of more than 283,000 voters through Saturday were paying attention.
Bryant is often quickly dismissed in the Kobe vs. Michael debate, which flared up last weekend when the Lakers star moved past Jordan and into third place on the NBA's all-time scoring list. Jordan is widely regarded as the best player in history. No argument here, at least for now.
But that wasn't the question.
Allow me to repeat ESPN's question: Who will have had the better NBA playing career when Bryant's is over?
It's much closer than many are led to believe when considering Bryant scored more points, grabbed more rebounds, made nearly three times as many three-pointers, played in more NBA All-Star Games, was named to more All-Defensive teams and won only one fewer championship than His Airness.
Better player: Michael Jordan.
Better career: well … let's examine.
Bryant played more games and more seasons than Jordan did, an accomplishment more than a criticism. Bryant effectively handled the mental and physical grind better than Jordan, who took a break from the game for one season to play baseball and left for three others before returning.
Even if you don't agree Bryant had a better career, the gap is narrower than most are willing to admit. And that includes Reggie Miller, who grossly exaggerated the difference between Jordan and Bryant when he was asked last week by ESPN's Dan Patrick about who was tougher to defend.
"Michael Jordan on his worst day is 10 times better than Kobe Bryant on his best day," Miller said. "That is not shortchanging Kobe Bryant because he gave me my lunch pail, too."
In fact, Miller was shortchanging Bryant. He has been under-appreciated throughout his career largely because Jordan was the standard for greatness. No matter how many points he scores or how many titles he wins, he never will be promoted from the Court of Public Opinion's second tier.
Still, people should take a step back and consider the variables before concluding Jordan had a better career. Time has a way of distorting opinion. The more removed sports heroes are from their careers, the greater their accomplishments and the higher their thrones. Fans protect players from their era.
Sports history is littered with examples, thus debates are handed down from one generation to the next, from Joe DiMaggio vs. Mickey Mantle to Jim Brown vs. O.J. Simpson to Jack Nicklaus vs. Tiger Woods. We believed there would never be another Jordan because there wasn't a Jordan before him.
Along came Kobe, walking and talking and scoring and winning much the way Jordan did when he dominated the league. Bryant's problem wasn't just second to Jordan in ability. He was second chronologically after Jordan established himself as the best player in the Golden Era of the NBA.
Bryant is 36 years old now. His best days are behind him, but he's still averaging 24.6 points per game. He's remains one of the best players in the NBA in, this, his 19th season. Michael was a greater player, but Kobe was great for a longer period. Keep that in mind when comparing the two careers.
Jordan scored 32,292 points in his career with the Bulls and Wizards. He won six championships, led the league in scoring 10 times, was a 14-time All-Star, was a five-time Most Valuable Player, was a six-time MVP in the NBA finals and a nine-time selection for the All-Defensive team.
Bryant has 32,340 points and counting in his Hall of Fame career with the Lakers. He won five titles, twice led the league in scoring, was named MVP twice, was named MVP in the finals and was a 12-time selection for the All-Defensive team. He also was the last player to average 35 points per game since … Michael Jordan.
Of course, Bryant needed 197 more games to reach Jordan's scoring output. Jordan scored more, but he also shot more. Jordan had more field-goal attempts in 13 seasons than Bryant did in his first 18 seasons. Michael led the league in attempts nine times in 13 seasons, Kobe only six times in 18 years.
Jordan averaged 3.2 shots per game more than Bryant. It adds up to more than 3,400 attempts over 13 seasons. If Kobe took as many shots and maintained his career shooting percentage, he would have added more than 3,000 points to his career total.
Jordan also had Scottie Pippen helping him on the perimeter along with Steve Kerr, John Paxson and Toni Kukoc at various stages. Bryant didn't have nearly as much help on the outside, but he had Shaquille O'Neal for eight years. Jordan never won a title without Pippen. Bryant won two without Shaq.
Jordan was still an effective player, but he was a shell of himself over his final two seasons with the Wizards. He averaged 10 points per game fewer over his final two seasons than his previous career average. In his 19th season, Bryant is less than a point per game from his career scoring average.
Who was the better player? Jordan. Who had the better career? OK, it's still Jordan. But it's close.
Now, what about LeBron?
email: bgleason@buffnews.com
Bucky Gleason – Bucky Gleason is senior sports columnist for The Buffalo News. He has covered sports on all levels since 1992. He is a terrible golfer who remains undefeated in match play on the 19th hole. He lives in Hamburg with his wife and four children.


Over the years, Vatican has been criticized for its involvement into the rise of Nazi Germany. When it comes to Vatican and Nazi Germany, Pope Pius XII is always the first to come in mind.
He was the one who negotiated and signed "The Reichskonkordat", a treaty between Vatican and Nazi Germany. The treaty was signed on July 20, 1933, and guarantees the rights of the Roman Catholic Church in Germany.
The document is one of the most controversial that the Vatican negotiated, and it is frequently discussed in works that deal with the rise of Hitler. According to some experts, the treaty gave moral legitimacy to the Nazi regime soon after Hitler had acquired quasi-dictatorial powers through the Enabling Act of 1933. Rome basically became the first legal partner of Hitler.
This documentary also explores topics like Catholic symbols and Nazi symbols, money trails, Gold, and much more.


text:
Q: iOS7 UINavigationBar tintColor changes to max .8 when set I've run into a weird bug in my program - everything works fine on the simulator, but when I run my app on an actual device, the tintColor of my UINavigationBar maxes out at .8 for the red, green, and blue channels. Here is a snippet of the code that I used to test:
UIColor *navcolor = [UIColor colorWithRed:140/255.0 green:193/255.0 blue:227/255.0 alpha:1];

if(IOS7()) {
    hnvc.navigationBar.barTintColor = navcolor;
    hnvc.navigationBar.translucent = NO;

    self.window.tintColor = [UIColor colorWithRed:146/255.0 green:53/255.0 blue:40/255.0 alpha:1.0];

    UIColor *color = [UIColor colorWithRed:1.0 green:1.0 blue:1.0 alpha:1.0];
    hnvc.navigationBar.alpha = 1.0;
    hnvc.navigationBar.opaque = YES;
    hnvc.navigationBar.tintAdjustmentMode = UIViewTintAdjustmentModeNormal;

    hnvc.navigationBar.tintColor = color;

    NSLog(@"%d", hnvc.navigationBar.translucent);
    NSLog(@"%@", color);
    NSLog(@"%@", hnvc.navigationBar.tintColor);

    const CGFloat* components1 = CGColorGetComponents(color.CGColor);
    NSLog(@ "A: %f, R: %f G: %f B: %f", CGColorGetAlpha(color.CGColor), components1[0], components1[1], components1[2]);

    const CGFloat* components = CGColorGetComponents(hnvc.navigationBar.tintColor.CGColor);
    NSLog(@ "A: %f, R: %f G: %f B: %f", CGColorGetAlpha(hnvc.navigationBar.tintColor.CGColor), components[0], components[1], components[2]);

}

As you can see, I tested a lot of different properties, but none of them seem to work. The output when I run this app in the simulator (iPhone 4-inch, iOS 7.1) is:
2014-07-06 21:52:54.096 L'Allegro[16650:60b] 0
2014-07-06 21:52:54.097 L'Allegro[16650:60b] UIDeviceRGBColorSpace 1 1 1 1
2014-07-06 21:52:54.098 L'Allegro[16650:60b] UIDeviceRGBColorSpace 1 1 1 1
2014-07-06 21:52:54.098 L'Allegro[16650:60b] A: 1.000000, R: 1.000000 G: 1.000000 B: 1.000000
2014-07-06 21:52:54.099 L'Allegro[16650:60b] A: 1.000000, R: 1.000000 G: 1.000000 B: 1.000000

However, when I run the app on my iPod touch 5th Gen (iOS 7.0), the output is:
2014-07-06 21:55:09.904 L'Allegro[3620:60b] 0
2014-07-06 21:55:09.908 L'Allegro[3620:60b] UIDeviceRGBColorSpace 1 1 1 1
2014-07-06 21:55:09.910 L'Allegro[3620:60b] UIDeviceRGBColorSpace 0.8 0.8 0.8 1
2014-07-06 21:55:09.912 L'Allegro[3620:60b] A: 1.000000, R: 1.000000 G: 1.000000 B: 1.000000
2014-07-06 21:55:09.914 L'Allegro[3620:60b] A: 1.000000, R: 0.800000 G: 0.800000 B: 0.800000

The same goes for any value of 1.0 that I try to set (i.e. if I use [UIColor redColor], the red component gets set to .8 instead of 1.0).
The result of this is that in the simulator, the bar button items on the navigation bar appear to be white, but show up in a light gray on my actual device.
I've been working at this for hours, and it's really frustrating that something as trivial as changing the color of my UIBarButtonItem to white can take such a long time so any help or pointers would be appreciated. Thanks!

A: in iOS7 to current iOS version supported navigation bar color
[[UINavigationBar appearance]setBarTintColor:[UIColor colorWithRed:231.0/255.f green:231.0/255.f blue:231.0/255.f alpha:1]];

is for color set at navigation controller.
but on that controller set perfect bar color so you have to set on viewdidLoad
self.navigationController.navigationBar.translucent=NO;

redpajama_set_name: RedPajamaStackExchange


Your customers are not buying products anymore, they are buying experiences. That's where augmented reality in advertising and events comes in!
Establish yourself as a leader by providing an engaging and unforgettable experience to your customers.
Product preview (3d models of products, color preview on painted wall, texture preview on bathroom makeover, etc).
End value is quicker education for the customer's decision-making process, gamified experiences and converting shops and points of sale into fun, unique places to visit.
If you're into augmented reality and digital transformation, send us the info below and we'll schedule a meeting to talk about your case.


text:
Report: Anthony Davis plans to decline player option, re-sign with Lakers
By Dan FeldmanOct 15, 2020, 1:18 PM EDT
Anthony Davis, who holds a $28,751,774 player option, said he had no idea about free agency.
But everyone knew Davis – on the big-market team he always wanted to join, represented by LeBron James' agent (Rich Paul), coming off a championship – would stay with the Lakers.
We're starting to see the mechanics of how.
Davis plans to opt out of his $28.7 million player option and re-sign with the Lakers, sources tell The Athletic.
Davis can name his price. His max salary will be less than his player-option amount only if the salary cap falls below $95,839,247. That seems highly unlikely.
The big question: How long will Davis sign for?
He could re-sign for up to five years. That'd be the simplest path to long-term security.
But he might favor a shorter deal for several reasons:
He's a 27-year-old superstar. Davis will command max contracts for the foreseeable future. He can maintain flexibility with minimal risk (though not no risk).
Max starting salaries are based on league-wide revenue, and raises in a multi-year contract are capped at 8% a first-year salary. NBA revenue is way down due to issues including the coronavirus pandemic and fallout in China from Daryl Morey's tweet supporting Hong Kong protesters. Even if he wants to stay in Los Angeles long-term, Davis might be better served locking into a multi-year deal once revenue rises.
LeBron can become an unrestricted free agent in 2021 and has shown a willingness to jump from team to team. The Lakers depleted their assets to pair LeBron and Davis. Davis might not want to get stuck with a lacking supporting cast if LeBron leaves.
More on the Lakers
Kobe Bryant stories you haven't heard before on NBC Sports' Uncovered...
NBA Power Rankings: Brooklyn climbs fast after Harden trade, big wins
Three things to know: James Harden, Nets brings 'Scary Hours'...


text:
International Cricket revival in Pakistan in 2017, confirms PCB
ISLAMABAD: With the security situation improving in the country, the Pakistani cricket fans having something to cheer
for as the Sri Lankan cricket team is expected to tour here at the end of this year.
Talking to APP, a Pakistan Cricket Board (PCB) official confirmed that the Sri Lankan cricket team is expected to tour Pakistan in November or December.
"Our Sri Lankan counterpart have expressed willingness in sending their team to Pakistan as the security situation is
improving in the country," he said.
He said Sri Lankan team would be playing ODIs and Twenty20s against Pakistan team which would be staged only in Lahore.
"The world had witnessed the type of security that was provided in the high-profile Pakistan Super League's (PSL) final at
Lahore. PSL final had proved a great breakthrough in reviving international cricket in Pakistan," he said.
He said World XI team would also be touring Pakistan in September which also includes foreign players from Australia, West Indies, Sri Lanka and South Africa.
PM Imran Khan to set a new precedence during his visit to America


text:
Myles Garrett
Arlington, Texas, USA
Born on Dec 29 #1
Footballer #7181
Born in Arlington, Texas #1
Capricorn #1
FIRST NAME Myles #1
Born in USA #1
Weight 123 KG #1
Height 76 Inches #1
More Facts of Myles Garrett
Scorpio, Virgo, Taurus
$12 million USD
44-34-36 inches
Larence Garrett
Audrey Garrett
(Two) Sean Williams and Bean Garrett
Myles Garrett Twitter
Myles Garrett Instagram
Myles Garrett Wiki
View more / View less Facts of Myles Garrett
Myles Garrett is a well-known professional American football defensive end. Myles Garrett is currently playing for the Cleveland Browns of the National Football League.
2 Professional Life and Career
4 Body Measurements
Myles Garrett was born Myles Lorenz Garrett on 29th December 1995 and is currently 25 years old. Being born in Arlington, Texas, United States, he holds American citizenship. Likewise, he belongs to a Christian family and was born under the sun sign of Capricorn.
Moving towards his family members, he was born to his father Larence Garrett, and his mother Audrey Garrett. Likewise, he also has a brother named Sean Williams and a sister named Bean Garrett. Talking about his educational details, he completed his schooling at Martin High School in Arlington. Later, he joined Texas A&M University and graduated from there.
Professional Life and Career
Myles started his career at his high school. During it, the popular college football website Rival rated him as a five-star recruit. Likewise, he also played football at Texas A&M University. In his freshman year, he broke the sack record of 5.5 in only 6 games. In fact, he finished the season with 11.5 sacks. He had surgery on his hand because of an injury in his sixth game. In his second year, he recorded 57 total sacks, 18.5 tackles, 7 quarterback hurries, and a blocked punt. However, his junior year career wouldn't be that successful as he was limited by injuries.
On December 31, 2016, Myles announced that he was entering the 2017 NFL Draft. With excellent performance, he secured his position as a top ten pick. Among all the defensive, he had the third-fastest 40-yard dash. Some top magazines such as Sports Illustrated and ESPN ranked him on the top.
Moving on, the Cleveland Browns drafted him for the 2017 NFL. Finally, on 19th May 2017, he signed a four-year contract with the team with a guarantee of $30.41 million USD. Similarly, he began the season as a defensive end. However, he missed the start of the season due to his high ankle sprain injury during practice on 7th September. His first match was a losing match with New York Jets.
He played the 2018 season as a defensive captain. The first match was a tie with Pittsburgh Steelers and won the second match against New York Jets. In the 2018 season, he recorded 13.5 sacks, 44 combined tackles, 3 passes defended, 12 tackle-for-loss, and 3 forced fumbles. Furthermore, in the 2018 season, his team loss against Tennessee Titans and Seattle Seahawks and won against the New York jets.
During Week 11, he had a fight with Mason Rudolph during the match with Pittsburgh Steelers. For this behavior, he was suspended indefinitely by NFL. However, on February 12, 2020, he was restored from his suspension. In April, he extended his contract by 5 years with the team.
Caption: Myles playing football (source: Instagram)
Regarding his relationship status, Garrett is not dating anyone and enjoying his single life. In fact, is currently more focused on his career than in a romantic relationship. He doesn't even have any past affairs. Also, he hasn't shared any pictures that would recommend his relationship status.
Being an athlete, Myles has maintained a fit and attractive body. He often does physical exercise to remain fit. Talking of his height, he is 6 feet 4 inches or 1.93 meters tall. Likewise, he has a body mass of 272 pounds or 123 kgs. Moreover, his actual body measurements (chest-waist-hip) are 44-34-36 inches respectively. Also, he has biceps of size 15.5 inches and he wears shoes of 12.5 (UK). In addition, the footballer has black hair and eyes of the same color.
Caption: Myles posing in his style (source: Instagram)
When it comes to his social media handles, he is available on Instagram and Twitter. He has a huge 598k followers on his @flash_garrett Instagram account, Similarly, he joined Twitter in March 2017 and has already earned more than 297.4k followers.
Caption: Myles with his car (source: WTFoot)
Myles has made a decent amount of money throughout his career. As of the online resources, he has an estimated net worth of $12 million US dollars, He earned this wealth from his football career.
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What this Policeman did to his wife is DESPICABLE!
A POLICE inspector who strangled his wife before dumping her body in a lake after she discovered their financial troubles has been found guilty of murder. Greater Manchester Police Inspector Darren McKie killed Detective Constable Leanne after spiralling into more than £100,000 of debt.
The psychopath has been found Guilty today over strangling Leanne and dumping her body in a nearby Lake at night. After committing the murder he calmly went and picked up their children from school and took them to ballet and cricket practice before giving them dinner. Chillingly, he continued to text his dead wife to update her on his afternoon and evening in order so as not to appear suspicious.
During the trial the court was told how the couple from Wilmslow, had amassed more than £100,000 of debt at the time of Leanne's death. Leanne sent texts to her husband asking: 'Are we in a mess??? Please tell me! I just worry you are trying to protect us again.' He denied and told her: 'Please stop doubting me.' On the day of the murder Leanne discovered McKie had been approved for a loan of £54,000 using her name and passport. She texted him and called him a 'liar' when McKie then went home and murdered her in cold blood.
In a statement read out today after the verdict the parents of Leanne (Ray and Ellen Dodd) said: "Justice has been served today. Our lives will never be the same again. There are no winners in this trial. We have lost our beautiful daughter and our grandchildren have lost their beloved mummy."
Read: "You'll never believe what these thieving SCOOTER thugs did in London"


text:
Home | Latest Posts | The Top 3 Pilgrimages for the Modern-Day Traveler
The Top 3 Pilgrimages for the Modern-Day Traveler
Pilgrimages are a great way to discover more about a particular country. They often involve traveling specific journeys to religious destinations. In the case of a pilgrimage, the journey really is as important as the destination itself, if not more so, as you'll likely be traveling the same route to a holy site that a particular people have been taking for hundreds of years. The ancientness of this particular cultural act brings the traveler's surroundings into historical context, and provides unique insight into a nation's people, history, and values. Although you'll be walking along more or less the same path as true pilgrims did to deepen their spiritual connection hundreds of years ago, now a modern tourism infrastructure exists to provide travelers with a variety of lodging and transportation conveniences on their journey. Sit back and enjoy the top 3 pilgrimages for the modern-day traveler.
The Camino de Santiago is probably the most famous pilgrimage modern-day travelers can take. It's a network of four Christian pilgrimage routes in Northern Spain that lead to the shrine of Saint James in the Santiago Compostela Cathedral in Galicia, where supposedly the remains of the saint are buried. Some of the trails date back at least eleven centuries. As it did then, the pilgrimage continues to foster cultural exchange between travelers and the communities they pass. Additionally, the beautiful landscapes and Spanish architecture attract thousands of modern-day pilgrims every year. There are plenty of hostels, known as albergues, specifically designed to shelter Camino walkers along the 900-plus mile journey. If this number scares you, traveling by foot isn't the only option. You can also drive, cycle, or even travel by donkey.
We're happy to tell you the Kumano Kodo is one of Japan's best-kept secrets. It's the only other pilgrimage, besides the Camino de Santiago, that UNESCO has declared a world heritage site. That designation alone should make it a worthwhile visit. Visitors will encounter a stunning network of lush forest trails, originally developed to help pilgrims traverse religious areas along the Kii Peninsula, the largest on the Japanese island of Honshu. These trails have been in use for this purpose for at least 1,000 years. Seeing the beautiful Kumano Sanzan shrines is a highlight of the journey. While the paths vary in difficulty, the array of natural hot springs and inns along each of the trails should provide great comfort and convenience. Hikers can even send ahead their luggage while traveling.
This pilgrimage ends at Macchu Picchu, the iconic citadel of the Inca built in the 15th century. This experience provides modern-day pilgrims with unparalleled access to the civilization's architecture, as well as the biodiversity that shaped their way of life. On every trail, visitors are sure to pass ancient settlements, tunnels and other Incan ruins, all while trekking through the cloud forests and alpine tundra of the Andes mountains experts suggest the 27-mile trail was created to prepare visitors and locals for the majesty of Macchu Picchu itself, and today the hike is normally completed within four or five days. Peru has sought to preserve the beauty and history of the Inca Trail's surroundings by only allowing a limited number of visits per season, and only issuing travel permits to touring companies. Therefore, visitors will only be able to travel the Inca trail in this fashion. With this guidance, travelers won't have to worry about food or lodging as they enjoy the natural beauty and historical value of this one-of-a-kind pilgrimage.
Contemporary Tours offers carefully curated academic and cultural experiences in all of the countries mentioned above. Contact us today for more information.
By Dana Silverman
Dana credits her passion for travel to Girl Scouts, which provided her with amazing opportunities to attend summer camps throughout the United States during her childhood. She's lived in Australia and New Zealand, and she's planning a trip to Japan around her appreciation for the country's cuisine and temples.
I continue to be in awe of the remarkable professionalism and incredible knowledge that are embedded in Contemporary Tours as a company. I have absolutely no reservations in recommending them for any and all of your educational needs.
Rod, Professor
Contemporary Tours has been unfailing in handling the countless arrangements necessary to achieve our 30-country, 60-city intense travel-study journeys. CT manages all of the complexity and removes all of the worries – freeing faculty and students to optimize their learning while experiencing the wonders of our world.
Les, Professor


text:
Хоэнпайсенберг () — коммуна в Германии, в земле Бавария.

Подчиняется административному округу Верхняя Бавария. Входит в состав района Вайльхайм-Шонгау.  Население составляет 3813 человек (на 31 декабря 2010 года). Занимает площадь 20,44 км². Официальный код  —  09 1 90 130.

Примечания

Ссылки
 Официальная страница

Города Баварии


text:
Our Observer
RIP: Russell Baker (no audio)
We loved that man, on top of worshipping his cool, insightful, hilarious Times column. Newspaper guys didn't say this sort of thing, but Russ Baker made your heart flutter. Lunch or even a few words with the great Baker in the office felt like prom night. He was so handsome, in his Jimmy Stewart way; such a kind, wise, good man. At the top of his profession, he savored James Reston's line that a man's career was not to be confused with his life. "Your job is a means to your private life," as Reston once put it to me. Russ Baker's life was exemplary. His first reader and editor was always Mimi, his stunning wife and soulmate. His daughter and two sons were and are characters, blessed and funny originals. Russ's friendship was a treasure, often just a few words. He would pause at my desk as I sweated and groaned on deadline. "Chris," he would say, "just tell them what happened." Thank you, Russ, then and now. My wife Cindy came to adore the man exactly as I did, and we amended our vows to allow that if she ran away with Russell Baker, I would understand. I happen to know that the press box gods in those decades — David Halberstam, Anthony Lewis, Neil Sheehan, Scotty Reston himself, Anthony Lukas, Tom Wicker, Ned Kenworthy, Hendrik Hertzberg and, yes, I. F. Stone — felt crushes like mine and Cindy's: pangs of blushing elevation, excitement, something like redemption around this guy. Reston knew that the key stroke in assembling his immortal Times Washington Bureau of the 50s and 60s was hiring the lean country kid from the Baltimore Sun to cover Lyndon Johnson's Senate. Tony Lewis in his Cambridge kitchen had a poster-size blow up of Russ Baker's takeoff on Craig Claiborne's $4000 expense account meal, on Times duty in Paris. Baker's home-cooked version, "a Lucullan repast for one," was beans in bacon grease, eaten out of the pan, with a shot of room-temperature gin. "I had a Gilbeys, 1975, which was superb," he noted.
Years later, Russell Baker credited me with nominating him to succeed Alistair Cooke as host of Masterpiece Theater on PBS. I had suggested him to WGBH's Rebecca Eaton, though in fact I'd also proposed John Updike, and Claire Bloom as well, thinking before they split that Philip Roth might write her copy. Uncannily, Rebecca reported that Baker and Updike had both responded at first in nearly the same words, to the effect: "I don't think my mother would approve my doing television." Baker got the nod, in any event, apologizing at first, in Baker style, because "my hands and elbows instinctively start flailing and clawing the air as if an alarming case of St. Vitus Dance is taking place right in front of the camera." But then he thanked me for "one of the best jobs a bookish old guy could have." It was the least I could do, dear Russ, for the man who embodied our newspaper dream.
–Chris Lydon
Nicholson Baker Writes a Protest Song
Songs are no joke. I'm not being ironic with these songs. I've never done anything in which I feel more vulnerable to my own failings and inadequacies. Nicholson Baker in conversation...
"Our Putin" and Son: the Bushes Revealed
Click to listen to Chris's conversation with Russ Baker. (36 minutes, 16 mb mp3) Russ Baker: "on assignment… but not ours" A perceptual gap is at the essence of the Bush enterprise....
June 8, 2014 Chris's Postcards from China
September 25, 2014 America's War of Ideas
August 18, 2014 WWI: The Shock of the New
June 13, 2014 China Rising
May 29, 2014 Chekhov's World, In Pictures
May 21, 2014 Derek Bok: The View from the Top
April 29, 2014 A Piketty Primer: "Capital" in 10 Graphs


text:
Q: SQL: Need help with query construction I  am relatively new with sql and I need some help with some basic query construction.
Problem: To retrieve the number of orders and the customer id from a table based on a set of parameters.
I want to write a query to figure out the number of orders under each customer (Column: Customerid) along with the CustomerID where the number of orders should be greater or equal to 10 and the status of the order should be Active. Moreover, I also want to know the first transaction date of an order belonging to each customerid.
Table Description:
product_orders
Orderid CustomerId Transaction_date Status
------- ---------- ---------------- -------
 1       23         2-2-10          Active
 2       22         2-3-10          Active
 3       23         2-3-10          Deleted
 4       23         2-3-10          Active

Query that I have written:
select count(*), customerid
  from product_orders
 where status = 'Active'
 GROUP BY customerid
 ORDER BY customerid;

The above statement gives me

*

*the sum of all order under a customer
id but does not fulfil the condition
of atleast 10 orders.

*I donot know how
to display the first transaction date
along with the order under a
customerid (status: could be active
or delelted doesn't matter)

Ideal solutions should look like:
Total Orders CustomerID Transaction Date (the first transaction date)
------------ ---------- ----------------
11           23         1-2-10

Thanks in advance. I hope you guys would be kind enough to stop by and help me out.
Cheers,
Leonidas

A: HAVING will allow you to filter aggregates like COUNT() & MIN() will show the first date.
select
  count(*),
  customerid,
  MIN(order_date)
from product_orders
  where status = 'Active'
  GROUP BY customerid
  HAVING COUNT(*) >= 10
  ORDER BY customerid

If you want the earliest date irrespective of status you can sub-query for it
select
  count(*),
  customerid,
  (SELECT min(order_date) FROM product_orders WHERE product_orders.customerid = p.customerid) AS FirstDate
from product_orders P
  where status = 'Active'
  GROUP BY customerid
  HAVING COUNT(*) >= 10
  ORDER BY customerid

A: SELECT
    COUNT(*) AS [Total Orders],
    CustomerID,
    MIN(Transaction_date) AS [Transaction Date]
FROM product_orders
WHERE product_orders.Status = 'Active'
GROUP BY
    CustomerId
HAVING COUNT(*) >= 10

A: This query should give you the total active orders for each customer that has 10 or more active orders.  It will also display the first active order date.
Select  Count(OrderId) as TotalOrders,
        CustomerId,
        Min(Transaction_Date) as FirstActiveOrder

From Product_Orders
Where [Status] = 'Active'
Group By CustomerId
Having Count(OrderId)>10

A: select count(*), customerid,  MIN(Transaction_date) from product_orders
     where status = 'Active'
     GROUP BY customerid having  count(*) >= 10
     ORDER BY customerid


text:
Kreisler: Variations on a Theme by Corelli; Sicilienne and Rigaudon; The Devil's Trill; Liebesleid; Liebesfreud
COMPOSERS: Kreisler
LABELS: Analekta Fleurs de lys
WORKS: Variations on a Theme by Corelli; Sicilienne and Rigaudon; The Devil's Trill; Liebesleid; Liebesfreud
PERFORMER: James Ehnes (violin, piano), Eduard Laurel (piano)
CATALOGUE NO: FL 2 3159
This 'very best of Kreisler' programme is sensibly divided into two: after four of his mischievous pastiches of 18th-century masters and his arrangement of the Devil's Trill Sonata come eight of his most popular Viennese bon-bons, the Recitativo and Scherzo for solo violin and (rarely heard and most imaginatively) the Petite valse for piano – a solo from Ehnes who proves as graceful a pianist as Kreisler himself. As a violinist, the Canadian is top-of-the-range luxury goods: the SOUND *e produces is ravishing, the intonation faultless, the articulation impeccable, all of which are employed with that one essential ingredient for Kreisler: charm. The clean-limned lines of the 'classical masters', buoyant, witty and elegant (including an impassioned account of the big cadenza interpolated in the Devil's Trill Sonata) are matched by a playful lilt and heart-warming affection in the alt Wien numbers (perhaps he makes the main theme of Caprice viennois too much like a berceuse). The partnership with the refined Eduard Laurel strikes me as particularly happy and the recorded balance between the two is well-nigh perfect. The booklet notes (by Jacques-André Houle) are of the same standard. For my money, the most satisfying Kreisler programme and modern performances currently available – and that includes those by Bell, Mintz and Kennedy.
Corelli reviews


The Samsung Galaxy S8 is last year's flagship, but it's still a terrific device. In fact, one of the chief criticisms of the Samsung Galaxy S9 is that the new phone is too much like the old phone, which is one of the likely reasons why the S9 isn't selling as well as the S8.
If you're interested in saving some money and don't mind using last year's gear, you can get an unlocked Samsung Galaxy S8 or Samsung Galaxy S8 Plus at Best Buy right now for some deep discounts.
As with most Best Buy deals, you save the most money by activating the device right there in the store, in this case on a new line with Verizon. However, you don't have to do so and you'll still save some cash off the regular price of the phone.
Those prices mean you save $100 off the current price if you simply buy unlocked or $150 off the price if you activate with Verizon. In both cases, you're saving more than $200 off the original retail price of the phones when they launched last year.
Click the buttons below to get this deal before Best Buy takes it away!


How many airlines fly direct from Washington Dulles to Tunxi?
There are 0 airlines who fly direct from Washington Dulles to Tunxi.
How long does it take to fly from Washington Dulles to Tunxi?
19h 0min is average flight time from Washington Dulles to Tunxi.
Which airline is the most popular from Washington Dulles to Tunxi in March 2019?
Air China is most popular airline from Washington Dulles to Tunxi in March 2019.
How many airports are there in Tunxi?
There is 1 airport in Tunxi.
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text:
\section{Introduction}\label{sec:INTRO}
Stochastic processes are of general importance, from a fundamental point of view but also regarding technical and biological applications. As a result, they have been the subject of intense research over the past years. A simple example is Brownian motion which has been intensively studied, both in equilibrium and in presence of various types of external driving, in experiments and theoretically~\cite{Seifert2012-wr, Sekimoto1998-cb, Dhont1996-vb}. In particular in case of entirely viscous, i.e. Newtonian solvents the treatment of such processes is rather straightforward because it can be described within the framework of a Markovian theory. The corresponding Langevin equation is then also linear in the sense that the dissipative parts (i.e., friction), remain linear in the particle's velocity. To go beyond these model systems, a variety of nonlinear properties of complex fluids have been studied~\cite{Larson1999-yj}. An important example concerns shearing of complex fluids~\cite{gutsche2008colloids, Wilson2011-ip, Leitmann2013-wo, Harrer2012-rs, Winter2012-ja, Gomez-Solano2014-jh, Gazuz2009-er, Squires2005-mc, Benichou2013-yn}, which, experimentally, involves macroscopic rheometers~\cite{Isa2007-jo, Besseling2007-id, Weiss1999-fp, Smith2007-ac}. In such investigations, many nonlinear features have been observed, e.g., shear-thinning or thickening, the phenomenon of yielding, or the multifaceted nonlinear response to oscillatory shear. Following these macroscopic studies, the development of microrheology, where a single microscopic probe particle is driven through a (nonlinear) medium, allowed to investigate the fluids' behavior at much smaller length scales~\cite{gutsche2008colloids, Wilson2011-ip, Leitmann2013-wo, Harrer2012-rs, Winter2012-ja, Gomez-Solano2014-jh, Gazuz2009-er, Squires2005-mc, Benichou2013-yn}. In  related experimental and theoretical studies, several  consequences of the nonlinearity of the bath have been reported. For example, it has been observed that the driven probe experiences an effective temperature which differs from the true bath temperature~\cite{Wilson2011-ip, Demery2019driven}, that it shows superdiffusive behavior~\cite{Benichou2013-yn, Winter2012-ja}, or shear thinning~\cite{Wilson2011-ip, Squires2005-mc}. More recently, experiments reported the occurrence of oscillatory modes~\cite{Berner2018-kk}, which are seen in a regime of linear, e.g., Newtonian-like behavior. The oscillatory dynamics in Ref.~\cite{Berner2018-kk} was reproduced using a generalized Langevin equation with negative memory at long times, which can induce persistent motion \cite{Zausch08, mitterwallner2020negative} and stress overshoots \cite{Fuchs03}. Furthermore, it was noted that the non-linear properties of a bath can already be detected in equilibrium~\cite{Muller2020-mo}. For example, in a nonlinear bath, the effective friction memory kernel may depend on the external potential~\cite{Daldrop2017external, Kowalik2019memory, Lisy2019generalized, Muller2020-mo, Muller2019thesis, Tothova2021brownian}. These findings illustrate the difficulty to match micro and macro-rheology measurement, and make the study of non-Markovian baths all the more important.

Here we study the motion of a particle trapped in a viscoelastic fluid, for different driving velocities, where, compared to previous work~\cite{Berner2018-kk}, we extend the experimentally accessible regime towards smaller velocities. We observe the previously reported linear regime, where the flow curve shows a plateau. For even smaller velocities, however, the viscosity is seen to increase in a pronounced manner, so that two distinct plateaus and two shear thinning processes are found. Theoretically, we reproduce this behavior by use of a previously introduced stochastic Prandtl Tomlinson Model (SPT) \cite{Muller2019thesis, Muller2020-mo}. This model also reproduces the previously observed  oscillations~\cite{Muller2019thesis, Berner2018-kk} for the given shear rates. The model implies that each shear thinning process corresponds to a de-equilibration of an important set of bath degrees of freedom, and it allows to estimate the important length scales involved in these degrees.

\section{Experimental Details }
Our experiments were performed in an equimolar solution of the surfactant cetylpyridinium chloride monohydrate (CPyCl) and sodium salicylate (NaSal) in deionized water at a concentration of \SI{7}{\milli\Molar} and at constant temperatures of \SI{25}{\celsius} and \SI{30}{\celsius}, respectively. Under such conditions, the mixture forms an entangled viscoelastic network of worm-like micelles~\cite{Cates1990-lk}, with a structural relaxation time on the order $\tau_s=\SI{2.5}{\s}$ as determined by microscopic recoil experiments~\cite{Gomez-Solano2015-qu}. Typical length scales of worm-like micelles are between 100 and \SI{1000}{\nano\m}~\cite{Walker2001rheology}, and their typical mesh size is on the order of \SI{30}{\nano\m}~\cite{Buchanan2005-dd}. A small amount of silica particles with $2R= \SI{2.73}{\micro\m}$ diameter has been added to the fluid and a single particle has been optically trapped by a focused laser beam of wavelength of \SI{1064}{\nano\m}. This creates a harmonic potential
with trap stiffness $\kappa$. The latter is determined from the equilibrium probability distribution of the particle in equilibrium, see e.g. Ref.~\cite{Berner2018-kk}. To probe the micro-rheological properties, the sample is translated with constant velocity $-v_0$ relative to the static optical trap by a piezo-driven stage with $v_0$ between 4 and \SI{400}{\nano\m\per\s}. Note that this driving is equivalent to a trap which is moving at velocity $v_0$ with respect to a fluid at rest. Overall it leads to a local shear rate of $v_0/2R$ close to the particle, and a Weissenberg number of $Wi=v_{0} \tau_{s}/2R$. The so-obtained Weissenberg numbers range between a few permille to almost unity in our experiments. We thereby extend the measurements by one decade towards smaller Weissenberg numbers compared to Ref.~\cite{Berner2018-kk}.
\begin{figure}[]
		\includegraphics[scale=0.3]{FlowcurvesNew25and30.pdf}
	\caption{Microviscosity as a function of the driving speed (flowcurves). Symbols correspond to experimental data for \SI{25}{\celsius} (blue squares) and \SI{30}{\celsius} (orange circles). Solid colored lines correspond to simulations using the stochastic PT model. Both temperatures exhibit the same two plateau shapes. For $v_0>\SI{200}{\nano\m\per\s}$, we recover the shear thinning behavior which is expected from macro-rheological measurements at \SI{25}{\celsius}, shown as a black dashed line. However, for $v_0<\SI{200}{\nano\m\per\s}$, the micro-viscosity further increases towards another plateau reaching values more than twice as high as the intermediate plateau. Dashed lines and data points on the $y$-axis give linear response values from simulation and experiment, respectively.}
	\label{fig:flowcurve}
\end{figure}

When driving the particle with constant velocity through the fluid, it experiences a drag force which leads to a displacement relative to the trap center. Using Stokes law and the trap stiffness, we can measure the velocity-dependent microviscosity, given by
\begin{equation}
	\eta = \frac{\kappa}{6\pi R v_{0}}\, \left\langle x(t) - v_{0}t\right\rangle . \label{eqn:Flowcurve}
\end{equation}
Here, $\left\langle x(t) - v_{0}t\right\rangle$ directly corresponds to the average position of the particle, relative to the center of the trap. The resulting flow curves are shown in Fig.~\ref{fig:flowcurve}, for two temperatures \SI{25}{\celsius} (blue squares), and \SI{30}{\celsius} (orange circles). Both curves exhibit the same trend. For driving speeds approaching Weissenberg numbers of order unity, the viscosity shows shear thinning, as expected. This is also confirmed by the macro-viscosity which is also shown in Fig.~\ref{fig:flowcurve} for the temperature of \SI{25}{\celsius} for comparison (black dashed line, obtained by a plane-plane rheometer). Indeed, for that temperature, the data corresponding to micro and macro viscosities agree reasonably well for $v_0>\SI{50}{\nano\m\per\s}$. We note that this data range was available in Ref.~\cite{Berner2018-kk}. From this close resemblance, together with the fact that the Weissenberg number is of the order of only $5$\% for $v_0=\SI{50}{\nano\m\per\s}$, at first glance one might conclude that these velocities are in the regime of linear response.

In contrast to this interpretation, however, the observation of oscillations in the so called mean conditional displacements (see details below), suggests that the system is far from equilibrium even at the small driving speed~\cite{Berner2018-kk} of $v_0=\SI{50}{\nano\m\per\s}$. When extending the range of velocities to smaller values, an astonishing observation is made: The viscosity shows a pronounced second shear thinning transition, connected to another plateau in the flow curve, of more than twice the viscosity value compared to the second plateau. The corresponding shear thinning process sets in at a Weissenberg number of roughly $2$\%, implying that this dimensionless quantity is not useful to understand that process. This conjecture is underpinned by the observation that the macro-viscosity seems to not display the shear thinning at the mentioned small velocities.

\begin{figure*}[ht!]
	\includegraphics[scale=0.25]{ModelSketch.png}
	\caption{\small{\textbf{a.} Sketch of the experimental system, highlighting the probe suspended in a worm-like micellar fluid. The particle is trapped with an optical tweezer, using a highly focused laser beam to form a harmonic potential for the particle. \textbf{b.} Sketch of the Stochastic Prandtl-Tomlinson model. The tracer particle (bare friction coefficient $\gamma_0$) is subject to a harmonic potential $V_\textrm{ext}$ with stiffness $\kappa$ , moving at constant speed $v_0$. The tracer is also linked to several (here two) bath particles with friction coefficients $\gamma_1$ and $\gamma_2$, respectively, through periodic interaction potentials $V_{\textrm{int},i}$.}}
	\label{fig:ModelSketch}
\end{figure*}

\section{Theory and model}
To rationalize these but also previous experimental observations~\cite{Muller2020-mo}, we consider a simple model where the tracer particle is coupled to a small number of bath particles which mimic the fluid environment (see sketch of Fig.~\ref{fig:ModelSketch}). Each bath particle is coupled to the tracer via a nonlinear interaction potential $V_\textrm{int}$ (specified below). As argued in Ref.~\cite{Muller2020-mo}, the potential $V_\textrm{int}$ is taken to be unbounded in the sense that it is finite for any particle separation. This allows the bath and tracer particles to be arbitrarily far away from each other, and to travel with different (mean) velocities. Within this model, e.g. the effect of shear thinning is reproduced, because tracer and bath particles are able to move at different (average) speeds. For simplicity, in  the following we assume $V_\textrm{int}$ to follow a sinusoidal function%
\begin{equation}
	V_{\textrm{int},i} = V_{0,i}\, \cos\left(\frac{2\pi}{d_{i}}(x-q_{i})\right) \label{InteractionPotential}
\end{equation}
where $V_{0,i}$ is the amplitude and $d_i$ is a length scale corresponding to bath particle $i$. $x$ and $q_i$ are the position coordinates of tracer and $i$-th bath particle, respectively. The parameter $d_i$ in Eq.~(\ref{InteractionPotential}) mimics an important length scale in the micellar bath, see above for typical numbers. In addition, the tracer particle is subjected to a harmonic potential of stiffness which results from the laser tweezer. As the tweezer is moving with velocity $v_0$ relative to the fluid, the trap potential $V_\textrm{ext}$ reads,
\begin{equation}
	V_\textrm{ext} = \frac{1}{2}\kappa \left(x - v_{0}t\right)^{2}  .\label{ExternalPotential}
\end{equation}
Accordingly, the equations of motion (with $N$ bath particles) are given by
\begin{eqnarray}
	\gamma_{0}\dot{x}(t) &=& -\kappa \left(x - v_{0}t\right) - \sum_{i=1}^{N}\frac{2\pi}{d_{i}}\, V_{0,i}\, \sin\left(\frac{2\pi}{d_{i}}(x-q_{i})\right) \nonumber \\
	&&\,\, + \,\, \xi_{0}(t),  \label{LangevinEquationTracer} \\
	\gamma_{i}\dot{q}_{i}(t) &=& \frac{2\pi}{d_{i}}\, V_{0,i}\, \sin\left(\frac{2\pi}{d_{i}}(x-q_{i})\right) + \xi_{i}(t) . \label{LangevinEquationBath}
\end{eqnarray}
Here, $\gamma_0$ and $\gamma_i$ are the bare friction coefficients of tracer and bath particle $i$, respectively. These coefficients are linked to the corresponding random forces $\xi_0$ and $\xi_i$ via the following standard properties,
\begin{equation}
	\left\langle \xi_{i}(t) \right\rangle = 0 \quad\text{and}\quad \left\langle \xi_{i}(t)\xi_{j}(t') \right\rangle = 2k_{B}T\gamma_{i}\delta_{ij}\delta(t-t')  .  \label{NoiseCorrelation}
\end{equation}
We assume in the following that the driving started at an infinite time in the past, so that the system is in a steady state for $t>0$. Practically, this means that from experimental as well as simulated trajectories, the initial parts, corresponding to equilibration, are removed.

The interaction potential of Eq.~(\ref{InteractionPotential}) makes this model reminiscent of the so-called Prandtl-Tomlinson (PT) model, which is used to study dry friction~\cite{Prandtl1928-yd, Tomlinson1929-pj}. Eqs.~(\ref{LangevinEquationTracer}) and (\ref{LangevinEquationBath}) extend this model to allow the background (our bath particles) to be stochastic and dynamic, and to contain several bath particles. This Stochastic Prandtl Tomlinson (SPT) model~\cite{Muller2020-mo, Muller2019thesis} thus reduces to the original PT model when setting $N=1$ and letting $\gamma_1$ approach infinity, so that the bath particle becomes a stationary background potential. This difference is quite intuitive, as our micellar background is dynamic, while the potentials considered in dry friction are rather static. Note that the notion 'Stochastic Prandtl-Tomlinson model' has been used for other models which are different from the one used here~\cite{Jagla2018-ti, Van_Spengen2010-yu}.

The solid curves shown in Fig.~\ref{fig:flowcurve} give the outcomes of the model of Eqs.~(\ref{LangevinEquationTracer}) and (\ref{LangevinEquationBath}) (see Table \ref{table:parameters2baths} for parameters used), using Eq.~(\ref{eqn:Flowcurve}). For small velocities $v_0$, we observe a linear response regime, where the micro-viscosity is independent of $v_0$. In this regime, the viscosity can be obtained also via linear response (see Eq.~(35) in Ref.~\cite{Muller2020-mo}), shown as the horizontal dashed lines in the graph. It is insightful to discuss the case of high potential barriers $V_{0,i}/k_{B}T$, which appear appropriate to fit the experimental data (see Table \ref{table:parameters2baths}). Then the regime of small driving speeds corresponds to the case where all particles move (approximately) with the same average velocity $v_0$. Because of this, the microviscosity in Eq.~(\ref{eqn:Flowcurve}) can be found to a good approximation from $\eta \approx\frac{1}{6\pi R} \,\left(\gamma_{0}+\sum_{i}\gamma_{i}\right)$. In the graph, the resulting value is not shown, as it is indistinguishable from the dashed lines. Experimentally, this corresponds to the case where the slow colloidal particle drags its surrounding with it, and thus feels a large friction.

The interaction potential $V_{\textrm{int},i}$ in Eq.~(\ref{InteractionPotential}) supports a maximal force of $\frac{2\pi}{d_{i}}\,V_{0,i}$. If the force between the tracer and the bath particle exceeds that value, the bond ruptures, and the velocity of the bath particle is (on average) smaller than $v_0$: As a result, the system shows a shear thinning behavior. The critical velocity where this happens can be estimated by balancing the mentioned maximal force with the drag force $\gamma_{i}v_{0}$ of particle $i$, yielding (in absence of noise) $v_{i,cr}\approx \frac{2\pi}{\gamma_{i}d_{i}}\,V_{0,i}$ . For the curves in Fig.~\ref{fig:flowcurve}, we use two bath particles, with distinct critical velocities, resulting in the two-plateau structure seen in the graph. As mentioned, for very small velocities, both bath particles move (approximately) with the same velocity as the tracer. The smaller critical velocity corresponds to the "larger" bath particle, i.e., the one with a larger value of $d_i$. Using the values of Table \ref{table:parameters2baths}, we estimate this velocity to be $27$ and $\SI{36}{\nano\m\per\s}$ for the two temperatures, respectively, which fits well to the numerical curves. Beyond this velocity, the viscosity decreases towards the second plateau. On the regime of the second plateau, the larger particle is thus far from equilibrium, while the second ("smaller") bath particle is still close to equilibrium. Once the second critical velocity (estimated to $321$ and $\SI{655}{\nano\m\per\s}$, respectively) is reached, also the second particle starts shear thinning. The model thus implies the interpretation that two distinct sets of degrees of freedom of the bath display very different critical velocities, yielding an intermediate state with half of them out of equilibrium. Notably, the often employed notion of fast and slow degrees of freedom~\cite{Zwanzig2001-bd} is demonstrated here explicitly, at least in our model.

The flow curve concerns the average position $\left\langle x - v_0 t\right\rangle $ of the particle, as seen from Eq.~(\ref{eqn:Flowcurve}), and we now aim to address the particle's fluctuations. Subtracting the particle's mean position, i.e. using $X(t)=x(t)-\left\langle x - v_0 t\right\rangle $, yields a stochastic variable $X$ with zero mean. Its fluctuations can be quantified using the so-called Mean Conditional Displacement (MCD)~\cite{Berner2018-kk}. It is defined by $\left\langle X\right\rangle_{X_0} = \int_{-\infty}^{\infty}dX\, X\, P(X,t|X_0,0)$, with $P(X,t|X_0,0)$ the conditional probability for the particle position $X$. In previous work, we observed that MCDs show oscillations in this system~\cite{Berner2018-kk}, which were observed at a temperature of \SI{25}{\celsius}, for Weissenberg numbers in the range of $0.04$ to $0.34$. Can the SPT model also explain the occurrence of oscillations? To address this question, we show in Fig.~\ref{fig:MCDPlots} experimental and simulated MCD curves, this time for a temperature of \SI{30}{\celsius}, to also emphasize the same phenomenology at the two temperatures. The MCD curves generally are found to a good approximation linear in $X_0$ (both in experimental as well as in simulated data), so that division by $X_0$ yields $X_0$-independent curves as shown. The figure distinguishes between positive and negative values of $X_0$, yielding the positive and negative flanks shown. The observed mirror symmetry of the data with positive and negative $X_0$ further emphasizes the linearity in $X_0$. Fig.~\ref{fig:MCDPlots}a) shows a small velocity of $v_0=\SI{16}{\nano\m\per\s}$, which corresponds to the regime of linear response in Fig.~\ref{fig:flowcurve}. For this velocity, the MCD curve decays monotonically to zero, as expected near equilibrium~\cite{Berner2018-kk}, and also in agreement with the SPT model. Fig.~\ref{fig:MCDPlots}b) shows a larger velocity of $v_0=\SI{200}{\nano\m\per\s}$, a velocity placed on the intermediate plateau in the flow curve in Fig.~\ref{fig:flowcurve}, thus in the regime corresponding to the curves shown in Ref.~\cite{Berner2018-kk, Muller2019thesis}. This curve shows pronounced oscillations, which are reproduced by the SPT model. How can these be understood? As described above, the intermediate plateau is beyond the critical velocity of the larger bath particle, which is thus far from equilibrium. It thus moves with an average speed much smaller than $v_0$. It can for the sake of argument be assumed to stand still, so that the tracer is moving in a stationary periodic potential. It is thus subject to a periodic force, which results in the seen oscillations. The period of oscillations is in this approximation given by $d/v_0$, which matches well the one observed in Fig.~\ref{fig:MCDPlots}b). In Ref.~\cite{Berner2018-kk}, the frequency of oscillations was indeed found to scale linearly with $v_0$, an observation which can now be understood. This analysis thus identifies an important length scale in the system, of the order of \SI{15}{\micro\m}. Passing over spatial variations on that scale (which are almost stationary as seen from the colloidal particle) seems to cause the observed oscillations.

\begin{figure*}
          \begin{minipage}{0.45\textwidth} \textbf{\large{(a)}}
         \end{minipage}
     \hfill
         \begin{minipage}{0.45\textwidth} \textbf{\large{(b)}}
         \end{minipage}  \\

         \includegraphics[width=.45\textwidth]{MCD-16nm_s.pdf}

     \hfill

         \includegraphics[width=.45\textwidth]{MCD-200nm_s.pdf}

\caption{Mean conditional displacements (a) in the linear response regime, $\SI{16}{\nano\m\per\s}$ and (b) in the  regime of intermediate plateau, $\SI{200}{\nano\m\per\s}$. Circles correspond to experiments (at \SI{30}{\celsius}), and lines correspond to the Prandtl-Tomlinson simulations (solid and dotted lines for $2$ and $3$ bath particles, respectively). While we recover previously observed oscillations~\cite{Berner2018-kk} for $\SI{200}{\nano\m\per\s}$, the linear regime  (left, $\SI{16}{\nano\m\per\s}$) exhibits none. Adding more bath particles (solid line for $3$ bath particles), leads to decoherence, and thus decreases the amplitude of the oscillations.}
\label{fig:MCDPlots}
\end{figure*}

The amplitude of oscillations is larger in the SPT model as compared to experiments, which we attribute to a number of idealizations of the model. For example, the background potential of the SPT model is perfectly periodic with a sharp length scale $d_i$. A real micellar solution, however, will exhibit a range of length scales, which naturally leads to decoherence. Indeed adding more bath particles, with slightly different parameters (see Table \ref{table:parameters3baths30T}) leads to a loss of coherence, and the amplitude of the resulting oscillations is reduced. Notably, adding more bath particles with appropriate parameters keeps the flow curve unaltered, but changes the MCD. This confirms the expectation that flow curve and MCD are not one to one related. The flow curve concerns the mean motion, and the MCD quantifies fluctuations.

In Ref.~\cite{Muller2020-mo}, a single bath particle was found to be sufficient to capture experimental observations in the STP model. It is natural that a system close to equilibrium (as in Ref.~\cite{Muller2020-mo}) is easier to model compared to a system far from equilibrium, as addressed here. Indeed, an open question is whether the larger length scale  of $\sim\SI{15}{\micro\m}$ can be detected in equilibrium.

Finally, we note that, while the MCD curves and the flow curve each can easily be modelled quantitatively, we had problems fitting both curves with the same parameters. We attribute this to the different values of trap stiffness used for flow curve and MCDs of $\SI{1.5}{\micro\N\per\m}$ and $\SI{0.3}{\micro\N\per\m}$, respectively, for experimental reasons. This makes fitting both curves simultaneously even more challenging. We therefore allowed the amplitude of flowcurve to be a free parameter in our simulations, which turned out to be $\SI{4.5}{}$.

\section{Conclusion}
In this work we describe micro-rheological experiments where a single colloid is driven by an optical tweezer within a viscoelastic fluid. The presented fluid, a micellar solution, shows a flow curve with two distinct shear thinning regimes, with an intermediate plateau in between. Theoretical modeling via a stochastic Prandtl Tomlinson model captures the observed behavior, and implies that, on the intermediate plateau, one set of bath degrees of freedom is far from equilibrium, while another set is still in equilibrium. The intermediate plateau corresponds to the linear response regime of macro-rheology, so that the shear thinning process at even smaller driving velocities is a purely microscopic effect, and can thus easily be overlooked. The mean conditional displacements show oscillations on the intermediate plateau, which are also reproduced in the theoretical model. The oscillations allow extraction of a length scale, which is as large as \SI{15}{\micro\m}, and whose nature and origin have to be investigated in future work.

\section{Acknowledgements}
The authors thank Boris M\"{u}ller for discussions at the early stages of this work. The theoretical parts of this work build on the initial findings provided in his thesis~\cite{Muller2019thesis}.
\textbf{Funding}: FG acknowledges the support by the Alexander von Humboldt foundation. This project is funded  by the Deutsche Forschungsgemeinschaft (DFG, German Research Foundation) – SFB 1432 – Project-ID 425217212.  RJ acknowledges the support by the G\"{o}ttingen Campus QPlus program.
\textbf{Competing interest}: The authors declare no competing interest.

\section{Data availability}
The data that support the findings of this study are available from the corresponding author upon reasonable request.

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