MBL là một thương hiệu tới từ Đức. Được phát triển hơn 30 năm, Sản phẩm CD-DAC mbl C31 đã có mặt trên 40 quốc gia và vùng lãnh thổ. Giờ đây, MBL đã tới Việt Nam và được phân phối bởi Audio Huylananh.
The C31 is the CD player, and D / A converter of the Corona family of the German MBL. In addition to a phenomenal CD drive, this player is equipped with an optical, one coaxial and an asynchronous USB input, which also benefit other sources of fluid D / A converter in this player. Via the USB input can be connected to a computer to stream your entire music library ripped.
To summarize, the CD31 can just as reasonably be considered a DAC with transport. It's a slot drive loader but has inputs for USB, Toslink and SPDIF with both RCA and XLR outputs. The DAC supports sampling rates up to 24-bit/96kHz resolution, and no higher but MBL's designer Jürgen Reis responds by citing the superior jitter performance of his DAC design, and the psycho-acoustically optimized filtering and the measured timing accuracy that is the equivalent to a 192kHz sampling rate. The output of the USB signal has a very low jitter in part due to MBL's Master Clock Mode which is similar to asynchronous USB. Internally, the digital inputs and outputs employ galvanic isolation between each other and ground to prevent high frequency eddy currents. High precision buffer data reading is provided by the combination of digital frequency synthesizer and nested analogue phase lock loop (PLL).
The mbl CD31 reminds me that there is still a whole lot of life left in the 16-bit/44.1kHz compact disc, that all discs (like all vinyl LPs) are not created equal and that it's easy, even lazy to jettison a proven and well-supported format like the compact disc for the latest greatest thing–namely computer audio. Streaming sound quality via USB is no slam-dunk, nor a newly discovered digital panacea. And even many downloads of the highest sampling rates or average recordings and so-so remasterings often offer no sonic advantages to the so-called lower rez versions including 16/44.


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This May Have Already Gotten out of Hand
Could we be in a hot civil war before people have gotten hip to the cold civil war?
Obviously we have the situation in D.C. where Steve Bannon, a white supremacist has been installed, perhaps illegally, on the National Security Council and Trump said the acting Attorney General "betrayed" the Justice Dept. by vowing not to enforce the executive orders that she determined were illegal. That's the stuff they spend a lot of time discussing on cable news.
We need to connecting the disturbing dots where there's less light shone. We have law enforcement agents not following court orders.
"Rogue customs and Border Patrol agents continue to try to get people on to planes," Becca Heller, director of the International Refugee Assistance Project, told reporters on Sunday morning at JFK airport in New York. "A lot of people have been handcuffed, a lot of people who don't speak English are being coerced into taking involuntary departures."
The FBI has quietly been investigating whether law enforcement has been infiltrated by white supremacists. We know the National Security Council was. Read the linked piece by the Intercept, it is chilling and we know it's an issue, not only in law enforcement, but the military. Not really a surprise that people who want the power of a gun and a badge and a kevlar vest might be more likely to be of the Bannonist persuasion. But given that the last line of defense in a democracy is the courts and the ability to carry out their orders, if you cannot trust law enforcement to carry out court orders? Then we're already at a coup 9 days in. And do we have to start worrying about the loyalty of the military?
Although these right-wing extremists have posed a growing threat for years, federal investigators have been reluctant to publicly address that threat or to point out the movement's longstanding strategy of infiltrating the law enforcement community.
Up in the Godforsaken hellscape of Canada, that media can't possibly beat a path to, apparently, a white nationalist Bannonist who supports Trump and LePen murdered 6 Muslim Canadians in an act of terrorism. But Sean Spicer and Fox News have characterized the killer as a Moroccan. One can't help but wonder why so little coverage of this latest atrocity.
White House Press Secretary Sean Spicer exploited the attack to justify President Trump's ban on immigrants from seven Muslim-majority countries. "It's a terrible reminder of why we must remain vigilant and why the President is taking steps to be proactive rather than reactive when it comes to our nation's safety and security," Spicer said at this afternoon's briefing when speaking of the Quebec City attack.
But these assertions are utterly false. The suspect is neither Moroccan nor Muslim. The Moroccan individual, Mohamed Belkhadir, was actually one of the worshippers at the mosque and called 911 to summon the police, and played no role whatsoever in the shooting.
The actual shooting suspect is 27-year-old Alexandre Bissonnette, a white French Canadian who is, by all appearances, a rabid anti-immigrant nationalist. A leader of a local immigration rights groups, François Deschamps, told a local paper he recognized his photo as an anti-immigrant far-right "troll" who has been hostile to the group online.
Expect more attacks like this. Concurrently, experts expect that Trump's immigration order could inspire attacks on American targets as it plays into Islamist claims that we're at war with Islam. What happens when a Trump property is targeted? The war that Trump wants could happen just like that. But that's international war. I'm still more concerned with domestic conflict as Trump/Bannon and their nutty followers take a harder and increasingly more violent and less lawful stance to defend the power they believe they've been given. These people are messianic in their belief that they're saving the world from the naive ideas of democracy and pluralism that is destroying their idea of what civilization is (law and order for white people).
Check 0ut the Early Warning Signs of Fascism. Um, we are there. It's not sufficient to say that America has traditions that will not allow it to be so easily taken over the way Putin made Russia his chew toy. Maybe those traditions are easier to overcome that we thought.
In the US Holocaust Museum.
I'm shook. pic.twitter.com/EeuHEXWusE
— Sarah Rose (@RaRaVibes) January 30, 2017
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Question: Why is Trump doing everything through executive order? He has the Congress and Senate. →

redpajama_set_name: RedPajamaCommonCrawl


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首页 > 新闻 > Terry Teachout
Terry Teachout
Mencken once said a famous say, Loyalty can be simply defined as an illogical belief in an impossible situation.This issue has caused wide public concern for Terry Teachout.This inspired me how to develop next.
Shakespeare said a famous quote, Nutrition books in the world. There is no book in life, there is no sunlight; wisdom without books, as if the birds do not have wings.As we all know, as long as it is meaningful, it must be carefully considered.This sentence brings us to a new dimension to think about this problem.
Gong Zizheng said a famous quote, China Life rely on wind and thunder, the Ten thousand horses stand mute. sorrow. We are dying, not to stick to one pattern of talented people.The occurrence of Terry Teachout, in the end, how to do, not the occurrence of Terry Teachout, how to produce.This sentence brings us to a new dimension to think about this problem.
Zuozhuan said a famous quote, The husband, and also the name of germany. Germany, the foundation of the state.Why does Terry Teachout happen?With these words, we have to examine this issue more carefully!
Golgi Inadvertently said such a sentence, The result is the property of all mankind, and science is the most unselfish.It is generally believed that if we grasp the crux of the problem, everything else will be solved.This inspired me how to develop next.
Mattin Luther King said a famous quote, We must accept finite disappointment, but we must never lose infinite hope.This issue has caused wide public concern for Terry Teachout.This makes us think deeply.
Voltaire said that inadvertently, Friendship is a combination of the soul. This combination can be separated, which is two sensitive and integrity between tacit contract.As we all know, as long as it is meaningful, it must be carefully considered.With these words, we have to examine this issue more carefully!
Voltaire said that inadvertently, Friendship is a combination of the soul. This combination can be separated, which is two sensitive and integrity between tacit contract.Now, it is very important to solve the problem of Terry Teachout. So,I hope everybody can also understand this sentence well.
Karavelov said a famous quote, If you want to get happiness and peace, it should be across the layers of barrier, knocking the truth clock forward.Let's think about it this way,This inspired me how to develop next.
Du Charm said a famous quote, Life is a kind of endless yearning, eager to continue to rise, become more great and noble.This fact is of great significance to me, and I believe it is also of certain significance to the world.This inspired me how to develop next.
Maugham said that inadvertently, The two lovers always love one another, and another is allowed to accept each other's love. This is a painful truth that most of us are to obey. But occasionally there are two love and love each other, but also the situation of being passionately in love.Let's think about it this way,Although this sentence is very short, it makes me think about it.
Song Qingling said a famous quote, Knowledge is from work, any achievement is the crystallization of hard work.From what has been discussed above, we may safely draw the conclusion that advantages of Terry Teachout far outweigh its disadvantages and it will still play essential roles in modern society.With these words, we have to examine this issue more carefully!
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While I was writing this post, I listened to Love Yourself by Justin Bieber. Try it !
Aside from the awesome Extra Dimension highlighters that I own in Beaming Blush, Oh Darling and Double Gleam, I'd never tried the highlighters from M.A.C. and boy, do we have a fair few like the Mineralize SkinFinish one in Soft & Gentle (my next purchase for sure !), the creamy ones like the Hyper Real Foundation in Gold Fx, the loose powder ones like Silver Dusk and the Hyper Real Glow highlighting palettes that up until a few weeks ago we had only two kinds of, a pink one and a gold one.
M.A.C. recently released two more of these Hyper Real Glow palettes, one called Shimmy Peach including only peachy golds for medium to dark skintones and one called Get Lit, including three WTF shades made for light skintones - I had the choice between the two and after much hesitation (should I get one for myself or one for my kit ?), I got myself the Get Lit Palette.
I'm really happy M.A.C. released new shades in this palette range - the palettes are compact, beautifully crafted and the name "Hyper Real Glow" on the front of the palette is a different shade for every palette of the collection which I think is a nice touch. One palette costs €39 in France while a single Extra Dimension highlighter is €34 so the price point is pretty good and for someone starting out in makeup, I'll always advise those palettes because they're much easier to use than a bam, in your face highlighter.
The thing with these palettes is that the formula is much different from the Extra Dimension highlighters and from quite any other highlighter I already own since it's described as creamy powder. And creamy it is, the powder seems really thick when I swatch it on my finger but once applied, it blends effortlessly and naturally on your face as advertised.
The three shades in this palette are called Like A Dream which is a whiteish shade of blue, Get Lit which is the kind of pink highlight you can see anywhere and Gleam Sheen, the most natural shade of the three, a pastel peach tone.
I'm quite sure I'd not have gotten this palette if I'd not been given the choice in the first place. You know me, I love in your face makeup products, I love me some good old pigment and I love me some popping blues and greens on my face as highlighters. BUT now that I've been given the chance to try out this palette, I'm madly in love. The texture is so different from anything I've ever tried and even though I've got dehydrated skin and my foundation still sometimes makes the dry skin on my cheeks pop, these powders don't emphasize that problem of mine. When M.A.C. said smooth, they said smooth. I've been trying out these highlighters for a few weeks now and I love how they last a whole day of work - I sometimes like to touch it up because I want my bam glow but even if I didn't I'd still have color glowing on my skin when I leave work.
It's not that in your face glow although you could totally wet these highlighters with Fix+ to make them even more intense. I think that's cool that aside from the Extra Dimension highlighters made for people used to dat glow tho and makeup artists, we've also got something for people starting out in makeup and photoshoots where we need something very natural that basically looks like you're glowing from within.


Depression is a lot more complicated than the common myth of it being purely something that happens in the mind. In fact it has a lot to do with our entire body functions, and one of the best ways to make it function properly is by doing cardiovascular exercise. In fact cardio exercise has been clincically proven to work just as well as prescription drugs in alleviating and fighting off depression! To better understand why this may be the case, it is important to keep in mind that your brain, thoughts, and overall physical body are all interlinked together so that if you improve one area, you improve the others. Another benefit of cardio is improved sleep, which also impacts the level of depression that one feels. So if you are feeling down, or are going through some rough times in your life, one way to help turn that around is by breaking a sweat and exercising!


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Home / Fitness & wellness / Can you be in the best shape of your life in your 30s and 40s?
Can you be in the best shape of your life in your 30s and 40s?
By: Bridget Kozlowski
As the world watches the U.S. Women's National Team dominate in the first round of the Women's World Cup, star forward Carli Lloyd stands out.
She not only scored two goals in Sunday's 3-0 victory over Chile, but she also is the veteran on the team at 36 years old. Lloyd's stamina and tenacity is enthralling to watch, and she's been quoted recently saying she's never been in better shape.
That goes against conventional wisdom that tells us our bodies are at their best in our teens and 20s. There are other examples of athletes thriving closer to middle age, like baseball's Nolan Ryan and football's Brett Favre.
But what about everyone else? Is it possible for the average non-athlete to also see peak physical fitness as they enter middle age?
Dr. Gregory Caronis, an orthopedic surgeon based at Advocate Condell Medical Center in Libertyville, Ill., says you can be in your best shape in your 30s and 40s, especially if you choose to become what he calls an "active manager" of your health.
Dr. Caronis says athletes such as Lloyd, Ryan and Favre likely realized that they needed to work harder in the gym and the kitchen to keep their bodies in peak shape in order to keep up with their younger teammates and hang on to the glory. It's that commitment, discipline and motivation that helps them stand out from their younger teammates who might not have to work as hard.
"As we age, we have to take more of an active role and measured steps toward being healthy," Dr. Caronis says. "Exercise and nutrition may require a new level of discipline, but being in your best shape physically in your 30s and beyond can absolutely be the case with one key component: commitment."
Dr. Caronis says middle-aged people often leave behind bad lifestyle choices such as excessive drinking, smoking and lack of sleep. Instead, they often focus on being around for their children and their future.
The average person may not have the same access to trainers and nutritionists that star athletes do, so it can help to surround yourself with people who are similarly motivated, Dr. Caronis says. Taking group fitness classes, signing up to train for a race or simply joining a gym with a friend can increase your chances of getting in your best physical shape, he says.
"If you commit to certain healthy behaviors and surround yourself with people who are motivated to do the same, getting in shape becomes a lot more attainable," Dr. Caronis says. "This adds an accountability factor in knowing you have to 'own' your future and your health."
Dr. Caronis says he, too, has to commit to his physical fitness, so he works out five to six times a week at a gym located where he works. The convenience factor helps physical activity stay a habit he can keep, he says.
"I chose to use the Centre Club Fitness Center at Condell so it's easy and convenient for me to get there," he says. "I now notice that, if I don't get a workout in a few times a week, my stress level can creep up. For me, physical fitness is now every bit a part of my routine as getting good sleep and having a cup of coffee in the morning. It has to be a commitment and part of your lifestyle."
Are you trying to get into shape? Taking a free, quick online assessment to learn more about your ideal weight by clicking here.
Are your knees hurting? It could be this.
'Let us not squander hope! Be proud to get your vaccine'
Mari June 20, 2019 at 12:07 pm · Reply
Since when is 30's middle aged? It's not the early 1900's anymore.
John June 21, 2019 at 5:55 pm · Reply
Well the average American lives about 78 years. Half of that is the middle age, 39 years. I would guess 30s, 40s, and 50s would be middle aged. Under 30 is young. Older than 60 is old. It is just a numbers problem.
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Bridget Kozlowski
Bridget Kozlowski, health enews contributor, is a public affairs manager with Advocate Aurora Health. She holds a masters degree in Public Affairs and a bachelor's degree in journalism, both from the University of Missouri. Bridget previously worked as a reporter for the Chicago Tribune and has also lead local government communications teams for both the City of Sterling Heights, Michigan and the Village of Lombard, Ill. Bridget loves trying new restaurants, traveling and spending as much time as possible with her son, husband and rescue mutt.
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WATCH: 4 things to look for in a cloth mask
In some places, wearing a mask when you're indoors or can't keep distance from others is the law.
By: Dr. Robert Citronberg
The most important thing you can do right now is keep your wits about you.


When it comes to selecting your foodservice partner, there is really just one choice – Food For Thought Dining Services. We are committed to creating memorable moments that support the end goals of our clients. Café patrons will enjoy the variety of healthy menu offerings, while they get away from day-to-day pressures in comfortable, creative spaces. Meanwhile, our responsible pricing and energetic service will support a return on your operating investment. Because we are a well-established provider, known for integrity and culinary talent, you can rest assured that your dining concept will become the showpiece of your amenity package.


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E-contracts go campus wide this spring semester
Michala Head February 21, 2019
First piloted in the fall semester of 2018 by seven professors and their advisees, e-contracts fully replaced New College's previous paper contract system the following spring. The campus seemingly did just fine with the change.
"I thought it actually went really smoothly, everyone got things to me in a timely manner," Professor of Anthropology Uzi Baram said. "Information popped up as it needed to in email and on the page. It all fits what we have talked about in previous semesters."
Baram said the e-contract was a good solution to the time management issues that would come up with paper contracts.
"What's nice about the e-contracts is that students don't need to rush to find me to get a physical signature and don't have to rush to hand it in by 5 o'clock on that second Wednesday," Baram said.
"I definitely put it off to the last minute," second-year Anna Lynn Winfrey said. "There wasn't any way I could have gotten my advisor to sign it at 2 a.m. on Tuesday morning when I actually sent it in, so I guess that was more convenient for me."
Winfrey was among the students who first piloted the e-contract system with her contract sponsor, Professor of Classics Carl Shaw.
"Initially I was a little skeptical about them," Winfrey said. "I'm pretty satisfied with them [but] I feel like we lost a personal touch."
There was some concern that e-contracts would detract from or hinder in-person meetings when the system was first announced. Baram does not find this to be an issue.
"I'm very comfortable interacting on email and other forms, and I don't think that is an artificial conversation," Baram said. "The piece of paper was never the basis of my face to face interactions with my advisees."
Faculty members cannot edit the contents of the e-contracts. They can only choose to electronically sign it or not.
"We decided that because the contract was an agreement between the student and the faculty member, and because it would be very difficult to modify the system as it currently exists, that the preference would be to completely have the student fill out their e-contract," Registrar Brian Scholten said. "And then that would be a static document that the faculty sponsor would review. If they wanted to have the student make changes before they approve it, then they would have to communicate that to the student."
Scholten also discussed the potential futures for this online system.
"Eventually we would like the whole registration process, and things that are associated with it, to be part of the e-contract system, even if we change the name of it," Scholten said, referring to registration documents. "The plan is, sometime in the future, to make the [Prospective Area of Concentration] PAOC and the Thesis Prospectus forms electronic documents."
More short term goals include e-contracts for study abroad students, who mailed in paper contracts rather than having the e-contract system available to them this semester, improving the functionality for professors by allowing them to create and propose tutorials in the system and adding a "submit" button in place of the e-signature.
Thesis student Eva Ernst would have preferred a submit button to the e-signature.
"I filled out my contract completely and just forgot to scroll down and electronically sign it before the deadline, I then got kicked off of Canvas for all my classes without warning and received a letter in the mail saying I was no longer registered at New College," Ernst said in an email interview. "So I had to call the Registrar's office and they sent me a form to petition the Provost. They also said I would have to pay a $50 late fee. I was told that the fee would most likely be waived due to this being a technical issue though."
Scholten said that the e-signature was redundant because one has to verify themselves to access the Student Evaluation System (SES) with their myNCF login. Ernst agrees that a "submit" button would be more intuitive.
"If they would have found a way to have a "submit" button, that would have cleared things up very quickly," Ernst said. "That way, students have to scroll all the way to the bottom and make sure they filled everything out before leaving it for approval. As it is now, you just fill out the contract and save it on your SES account. Getting some sort of notification that the deadline is coming up and something hasn't been filled out would also be helpful."
Winfrey also had thoughts on improvements for the system.
"I wish they would do some more improvements where you didn't have to go back and look for the idiosyncratic [Course Request Number] CRN," Winfrey said, referring to the need for students to open the class schedule separately in order to fill out their e-contracts.
Scholten explained that CRNs are needed as independent identifiers for courses each time they are offered for the Banner system used to keep track of student records, so streamlining this may not be straightforward right away.
"[The contract is] just like another thing I'm sending off into the ether, but I feel like it's not that big of a deal compared to other large changes [at the college]," Winfrey said.
e-contract
ncf catalyst
Dr. Erin Dean receives grant to continue research in Tanzania
Record number of New College students present at Florida Conference of Historians


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Jemele Hill Reacts To The News Of Her Departure From ESPN
Matt Hladik
Last night, news broke courtesy of ESPN insider James Miller that ESPN personality Jemele Hill had negotiated a buyout with the company. Hill is done at the Worldwide Leader as of Sept. 1.
Miller termed the departure "amicable." A report from Sporting News says Hill will walk away with "millions" of dollars from ESPN as she looks to pursue other opportunities.
Earlier this summer, a report from OZY said Hill was preparing to leave ESPN. Hill has had a crazy last year-and-change at the Worldwide Leader, most notably sparking a social media firestorm when she tweeted that Donald Trump was a "white supremacist."
Hill has not officially commented on the latest reports of her departure, but she did tweet out a brief response earlier today.
It isn't surprising that Hill's Twitter mentions have gone nuclear. She's a polarizing figure for sure.
Those who agreed with her loved the fact she spoke out about political and social issues using her ESPN platform. At the same time, there were plenty who loathed her for her opinions and thought she should "stick to sports."
It looks like ESPN is trying to get back to sticking to sports with the way it is restructuring some of its talent and television shows. As for Hill, it is unclear where she will head next.
It wouldn't be a surprise to see her as a contributor for a major news network, discussing sports, politics, race and culture on the air. She might also be hired by an outlet that allows her to write about those topics, similar to the work she did with ESPN's The Undefeated.


We provide Hardware and Software Development and Testing Services.
Clients are looking to create performance driven partnerships to complement their internal design teams. This is a value addition that goes beyond cost reduction and flexible business models. At Innovaide, the focus is on global sourcing of the best technologies and know-how, along with a fresh perspective, to help create a differentiated and more competitive product.
1. Cost Reduction – a factor that influences outsourcing decision the most – obviously because it shows benefits to the CFO in language she understands well! But key here is to highlight indirect along with the direct cost benefits...Read more..


The International Visegrad Fund is an international organization based in Bratislava, Slovakia. The purpose of the Fund is to facilitate and promote the development of closer cooperation among citizens and institutions in the region as well as between the V4 region (the Czech Republic, Hungary, Poland, Slovakia) and other countries, especially the Western Balkans and countries of the Eastern Partnership (Armenia, Azerbaijan, Belarus, Georgia, the Republic of Moldova and Ukraine). The Fund does so through grant support of common cultural, scientific and educational projects, youth exchanges, cross-border projects and tourism promotion, and through individual mobility programs (scholarships, residencies).
For more information please see the Grant guidelines.


Created in collaboration between Sapling and the wonderful NOT SO MUMSY, these little rompers are perfect for your little love bug.
"I'm so thrilled to have collaborated with Sapling on these rompers. I share the same ethos and passion for sustainable, ethical clothing and have been a long time fan of both the clothing and the story. Our "Love Bug" rompers are just that - made with love for our littlest loves!


Acoustics are one of the most technically difficult architectural areas and are a crucial consideration for interiors, as poor specification can have significant impact on user experience.
Restaurants struggle with both sound generation and sound reverberation controls. Directly influencing these factors are the absorptive properties of the room.
Absorptive properties reduce reverberation time, which is critically important for speech intelligibility, increase conversational privacy and reduce general noise levels.Gyptone combines aesthetics and high performance, acoustic absorption helping to create a comfortable and stylish environment for all to enjoy.


The all-new Executive 1850 is the logical extension of our 1700 series. The exterior have been designed by John van Leeuwen in cooperation with yacht designer Arnold de Ruyter. The interior design was created by Bart van den Hoven himself. The curvaceous lines give the side view an even more stylish appearance. The 1850 is available both with and without a flybridge.
The overall concept is carefully considered: elegant with lots of space, Van den Hoven build quality with a superb finish, and made of steel so that all client wishes can be realised. What's more, the price is highly competitive in its segment. The yacht is designed for Van den Hoven owners who would like to buy a larger boat as well as for people who wish to spend many sailing hours on a true Dutch quality yacht without paying over the odds.
The Executive 1800 leverages on all the benefits and experience of its sister vessels in the Van den Hoven fleet and then goes a step further. A striking example is the capacity to close off the entire aft deck by means of a practical yet luxurious awning set-up so that it can still be used when the weather is less pleasant.
The outside decks have a natural walking flow and the flybridge can add a whole new dimension to the sailing experience. With a small outdoor kitchen, fridge, comfortable settees and an extra steering position, this area is the equivalent of a rooftop terrace. Protection from the sun can be provided by a stylish, practical bimini.
There is a great deal of space on this yacht, as is typical for Van den Hoven, with the engine compartment placed entirely aft. The Executive 1850 features three luxurious cabins, two large bathrooms with toilet and one separate day head, a large living area and a modern galley. The yacht is equipped with two Volvo Penta 300 hp engines and stabilisers. And, as reflected by its CE certification A, it is perfectly suited for the open sea.
The interior layout of this beautiful yacht can be defined fully in accordance with the owners' wishes. All types of wood, colours, materials and types of fabrics belong to the possibilities. You can also choose more bathrooms or fewer bedrooms, for instance. In short, the interior design is entirely up to your own taste and we would be pleased to discuss the possibilities.
The 1850 provides even more sailing comfort than the 1700, due not only to its length but also the fitting of electirc stabilisers as standard. The underwater segment is already of course designed for high initial stability.
The entire engine room features high-quality insulation and is finished with white perforated aluminium plate. Vibrations are eliminated as much as possible by the heavy, solid hull frame and the transmission from the engine to the axle, as well as the constant-velocity link. In addition, the bulkhead between the engine and the interior is made of 4 mm steel and anti-reverberation insulation makes for a virtually vibration-free vessel.


A lot has been written over the last few years about the age of automation and how that will impact the future of work. In contrast to the doom and gloom scenarios about impending large-scale job losses frequently portrayed in the media, initial findings from recent research by McKinsey paint an interesting and nuanced picture of how automation is likely to affect jobs. The report concludes, "As the automation of physical and knowledge work advances, many jobs will be redefined rather than eliminated—at least in the short term." McKinsey's research and Evalueserve's own experience from working with our clients suggests that almost all jobs will be impacted by automation to some extent. As an example, in 2015 alone, at Evalueserve, we "automated away" work in a variety of different industry verticals that we support, which would have otherwise taken 300,000 hours.
Physical: Strength, stamina and dexterity. There are few jobs with absolutely no physical requirements, but many office jobs require little in this area.
Equipment: Technical know-how, selecting the right tools, and the ability to troubleshoot.
Supervision: Supervising people and also getting things accomplished through peers.
Awareness: Comprehending the environment, which is often important for working outside or in chaotic surroundings.
Perception: The ability to focus on details and the ability to find a signal among noise.
Teamwork: Being personable as well as dealing with stressful situations and difficult people.
Initiative: Sometimes called grit, this is the ability to start and complete things.
The MIT researchers "found that above-average wages flow to occupations that require high skills in two or more dimensions (listed above) simultaneously." So the key actionable insight for all of us here is to think carefully about the different aspects of our job where we use the dimensions of skill listed above, and figure out ways to continually get better at several of them. This is how we will prepare ourselves successfully for the age of mind+machine™ and continue to stay relevant in the future of work!


Ebay Inc (NASDAQ:EBAY) up 2.16% to close at the price of $35.05. The stock has a market capitalization of $32.68 Billion however its outstanding shares are 932.27 Million. The company's beta value stood at 1.32.
Ebay Inc (NASDAQ:EBAY) has an ABR of 2.16 which is the combined stock view of 25 analysts poll results. As per Zacks simplified descending rating scale the ABR rank is displayed in the range of 1 to 5 where 1 represents Strong Buy and 5 a Strong Sell. As the name implies that ABR will show you the Average of Brokerage Recommendations on a given stock. It helps you quickly get a picture of where Wall Street stands on a stock without reading huge research reports. The smaller number of ABR is the more favorable. The modest value of the stock is known as the current ABR of the stock.
However out of 25 analysts 8 suggest Ebay Inc (NASDAQ:EBAY) a Strong Buy, 8 suggested Buy, 20 Hold and 1 Sell, while 0 analysts recommend the stock a Strong Sell.
Analysts are expecting average earnings estimates of $0.68 for the current quarter based on the opinion of 32 analysts, relating to high earnings per share estimates of $0.69 and low estimates of $0.61, however Ebay Inc (NASDAQ:EBAY) reported $0.59 earnings per share for the same quarter last year.
For the current quarter Ebay Inc (NASDAQ:EBAY) has average revenue estimates of $2.87 Billion, a total number of 29 analysts provided estimations over revenues. However the low revenue estimates for the company are $2.79 Billion versus high revenue estimates of $2.89 Billion. A year ago the company's sales were $2610000 while its sales growth yearly estimates for the current quarter are 9.7%.
Taking a broader look at the analyst consensus, brokerage firms have a price target of $36.6 on Ebay Inc (NASDAQ:EBAY). Brokerage firms on the street have price targets on the name ranging from $30 to $52 based on 33 opinions.
Ebay Inc (NASDAQ:EBAY) as of current trade, has shown weekly performance of 3.03% which was maintained at 23.76% in one month period. Year to date performance remained at 24.87%. During the past three months the stock gain 20.74%, however six months performance of the stock remained at 5.51%. Ebay Inc (NASDAQ:EBAY)'s price sits 17.48% above from its SMA 50 of $30.29 and 4% far from the SMA 200 which is at $31.43.
Currently Ebay Inc (NASDAQ:EBAY)'s shares owned by insiders are 4.9%, whereas shares owned by institutional owners are 86.5%. However the six-month change in the insider ownership was recorded -0.46%, as well as three-month change in the institutional ownership was recorded 0.61%.
The stock is trading -24.2% away from its 52 week high of $46.24 and 34.76% far from the stock's low point over the past 52 weeks, which was $26.01.
The price-earnings ratio (P/E ratio) is the ratio for valuing a company that measures its current share price relative to its per-share earnings. Ebay Inc (NASDAQ:EBAY)'s price to earnings ratio stood at 15.58. A high P/E suggests that investors are expecting higher earnings growth in the future compared to companies with a lower P/E. A low P/E can indicate either that a company may currently be undervalued or that the company is doing exceptionally well relative to its past trends.
The PEG ratio is used to determine a stock's value while taking the company's earnings growth into account, and is considered to provide a more complete picture than the P/E. Ebay Inc (NASDAQ:EBAY) has a current PEG of 1.61. Ebay Inc (NASDAQ:EBAY)'s price to sales ratio for trailing twelve month stands at 3.12, whereas its price to book ratio for the most recent quarters is at 4.93. However the company's price to cash per share for most recent quarter stands at 5.17. Its price to free cash flow for trailing twelve months is 6.78.


text:
Home / Suarez believes that he's completely ready to face Real Madrid
Suarez believes that he's completely ready to face Real Madrid
By Andrew Scott Friday, 17 October 2014 04:13
Luis Suarez said that he's set to make his debut for Barca when he faces Real Madrid in the Clasico taking place next Saturday, and sports software services are very eager to see him play competitively for the Catalan giants after his suspension.
In July, the player left Liverpool and joined the ranks of Barca, but he had no choice but to wait to make his competitive debut in La Liga after being suspended for four months after the famous incident in the World Cup where he bit Giorgio Chiellini in a game between Uruguay and Italy.
The 27-year-old player was given the green light to participate in friendly games for his national side after an appeal was made to the CAS.
After hitting the field for Uruguay during the international break when the team took on Saudi Arabia and Oman, the Uruguay international is now confident that next weekend he will play at his very best when he faces Real.
Suarez spoke on Wednesday when he got the Golden Shoe for the season of 2013-2014, and said: "I'm feeling fine physically, much better than I expected in fact.
"I can now say for sure that I'm 100 per cent at my best."
"A footballer always has to be ready to play matches, but making my Barca debut at the Bernabeu will be very special because of the historic rivalry between the teams," he added.
"I'll be ready to do whatever the boss [Luis Enrique] orders me to do, and it's him who'll decide whether I get to play.
"I had to be patient. Training with my team-mates and spending day-to-day life with them was good for me. Now I feel much better."
Sports software services were delighted to learn that Suarez will return to competitive action, and can't wait to see how he performs when the Catalan giants take on Real. Many fans are confident that things in the sport will get much better for him, and believe that he will shine on the pitch for his new side.
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text:
\section{Introduction}
\label{sec:Intro}

New physics are expected to be observed at the  LHC experiments.
Although new particles have not yet discovered, LHCb has  reported
 new data of the CP violation of $B$ mesons and the branching ratios
 of rare $B$ decays.  New physics are  also expected to be
 found in the $B$ meson  decays.

The CP violation in the $K$ and $B_d$ mesons has been successfully
understood
within the framework of the standard model (SM),
 so called Kobayashi-Maskawa (KM) model \cite{Kobayashi:1973fv}.
The source of the CP violation is the KM phase
in the quark sector with three families.
However, there could be new sources of the CP violation if the SM is
extended to the supersymmetric (SUSY) models. The CP-violating phases appear
in  soft scalar mass matrices. These phases  contribute to flavor changing
neutral  currents  with the CP violation.
Therefore, we expect the SUSY contribution in the CP-violating phenomena
in the $B$ meson decays.

The typical contribution of SUSY is
the  gluino-squark mediated flavor changing process
 \cite{King:2010np}-\cite{Ishimori:2011nv}.
In our previous paper~\cite{Hayakawa:2012ua},
we have already discussed  the effect of the squark flavor mixing
on the CP violation in the non-leptonic decays
of $B_d^0$ and $B_s^0$
taking  account of the recent LHCb experimental data.
 We have found the deviation from the SM predictions
 in  the asymmetries of  the penguin dominated decays
 $B_d^0\to \phi K_S$ and $B_d^0\to \eta 'K^0$.
In that framework of the SUSY contribution, we assume that
 $LR$ and $RL$ components of the squark mass matrices are neglected.
 The $LL$ and $RR$ components of squark mass matrices
contribute considerably to the penguin  processes
 for the case of  large $\mu\tan\beta$, ${\cal O}(10~{\rm TeV})$.
However,  if $LR$ and $RL$ components of squark mass matrices
  dominate the penguin decays,
 the asymmetries of
 $B_d^0\to \phi K_S$ and $B_d^0\to \eta 'K^0$ are deviated from the
SM predictions even for  the case of
the smaller  $\mu\tan\beta$, ${\cal O}(1~{\rm TeV})$.
Then, these contributions  of the new physics
 are  correlated with the direct CP violation  of the  $b\to s\gamma$ decay.
In this paper, we present the numerical analyses in the  case that
$LR$ and $RL$ components of squark mass matrices dominate the penguin decays.
In this case, the $LR(RL)$ components do not contribute to
 the  dispersive part $M_{12}^q$ of $B_q-\bar B_q \ (q=d,s)$ mixing.

In section 2,
we summarize the effect of  new physics in the CP violations
 of the neutral $B$ mesons
  including the recent  experimental  data.
In section 3,
we discuss the our framework  of  the squark flavor mixing in
the CP violation of $B$ mesons.
  We also discuss the constraints from the direct CP violation
 in  the $b\to s\gamma$ process.
 In section 4, we show the numerical result of
the CP violation in the  $B$ mesons.
Section 5 is devoted to the summary.

\section{New physics of  CP violation in  $B$ mesons}
\label{sec:Deviation}

Let us discuss the effect of  new physics
 in the non-leptonic decays of $B$ mesons.
The contribution of new physics to the dispersive part $M_{12}^q(q=d,s)$
is parameterized as
\begin{equation}
M_{12}^q=M_{12}^{q,\text{SM}}+M_{12}^{q,\text{SUSY}}=
M_{12}^{q,\text{SM}}(1+h_qe^{2i\sigma _q})~, \quad (q=d,s)
\label{M12}
\end{equation}
where $M_{12}^{q,\text{SUSY}}$ is the SUSY contribution,
and the SM contribution $M_{12}^{q,\text{SM}}$ is given as \cite{sanda}
\begin{equation}
M_{12}^{q,\text{SM}}=\frac{G_F^2M_{B_q}}{12\pi ^2}M_W^2(V_{tb}V_{tq}^*)^2\hat \eta _BS_0(x_t)f_{B_q}^2B_q~.
\end{equation}

The time dependent  CP asymmetry decaying into the final state $f$
 is defined as \cite{Aushev:2010bq}
\begin{equation}
\mathcal{S}_{f}=\frac{2\text{Im}\lambda _{f}}{|\lambda_{f}|^2+1}\ ,
\label{sf}
\end{equation}
where
\begin{equation}
\lambda_{f}=\frac{q}{p} \bar \rho\ , \qquad
\frac{q}{p}=\sqrt{\frac{M_{12}^{q*}-\frac{i}{2}\Gamma_{12}^*}
{M_{12}^{q}-\frac{i}{2}\Gamma_{12}}}, \qquad
\bar \rho \equiv
\frac{\bar A(\bar B_q^0\to f)}{A(B_q^0\to f)}.
\end{equation}
In the  $B_d^0\to J/\psi  K_S$ decay, $\lambda_{J/\psi  K_S}$
is given in terms of  the new physics parameters
$h_d$ and $\sigma_d$ as
\begin{equation}
\lambda_{J/\psi  K_S}=
-e^{-i\phi _d},\quad \phi _d
=2\beta_d+\text{arg}(1+h_de^{2i\sigma _d}),
\label{new}
\end{equation}
by putting  $|\bar \rho |=1$ and $q/p\simeq \sqrt{M_{12}^{q*}/M_{12}^q}$,
where the phase $\beta_d $ is given  in the SM.
The CKMfitter provided the allowed region of $h_d$ and $\sigma_d$,
where the central values are \cite{CKMfitter,Ligeti}
\begin{equation}
h_d\simeq 0.3,\qquad \sigma _d\simeq 1.8 \ {\rm rad}.
 \label{hdsigmaLHCb}
\end{equation}
 Since  penguin processes are dominant  in  the case of
  $f=\phi K_S, \eta ' K^0$, the loop induced new physics
 could  contribute considerably
on the   CP violation of  those  decays.
 Then,  $\mathcal{S}_f$ is not any more same
as $\mathcal{S}_{J/\psi K_S}$
 if new physics leads to  $|\bar \rho |\not = 1$.
 Those predictions provide us good tests for  new physics.

In the   $B_s^0\to J/\psi\phi$ decay, we parametrize as
\begin{equation}
\lambda _{J/\psi \phi }=
e^{-i\phi _s},\qquad \phi _s
=-2\beta_s+\text{arg}(1+h_se^{2i\sigma _s}),
\end{equation}
where $\beta _s$ is given  in the SM.
Recently the  LHCb presented the observed
 CP-violating phase $\phi _s$ in $\bar B_s^0\to J/\psi \pi^+\pi^- $
decay using about 1 fb$^{-1}$ of data~\cite{:2012dg}.
This result leads to
\begin{equation}
\phi _s=-0.019^{+0.173+0.04}_{-0.174-0.03} \ \ \text{rad},
\label{phis}
\end{equation}
which is consistent with the SM prediction \cite{CKMfitter}
\begin{equation}
\phi _s^{J/\psi \phi ,SM}=-2\beta_s=-0.0363\pm 0.0017~\text{rad}.
\label{SMBs}
\end{equation}
Taking  account of these data, the CKMfitter has presented
the allowed values of $h_s$ and $\sigma _s$ ~\cite{CKMfitter,Ligeti}.
The allowed region is rather large including zero values.
In order to investigate possible contribution of  new physics,  we take
the central values
\begin{equation}
h_s= 0.1,\qquad \sigma _s=0.9 - 2.2 \ \text{rad},
\label{hsigmaLHCb}
\end{equation}
as a typical parameter set in our work.

We remark on numerical inputs of phases $\phi_d$ and $\phi_s$
in our calculation.
The phase  $\phi_d$ is derived  from  the
 observed value  $\mathcal{S}_f=0.671\pm 0.023$ in $B_d^0\to J/\psi K_S$
\cite{PDG} as seen  Eqs.(\ref{sf}) and (\ref{new}).
On the other hand, we use the SM value of $\beta_s$ and
 the values of the new physics  parameters,  $h_s$ and $\sigma_s$
in Eq.(\ref{hsigmaLHCb})
 to estimate  $\phi_s=-2\beta_s+\text{arg}(1+h_s e^{2i\sigma_s})$.
 We do not use the observed value of $\phi_s$ in $B_s^0\to J/\psi\phi$
 because of  the large experimental error in Eq.(\ref{phis}).

Since the $B_d^0\to J/\psi K_S$ process occurs at the tree level in  SM,
 the CP-violating  asymmetry  originates   from  $M_{12}^d$.
Although the $B_d^0\to \phi K_S$ and $B_d^0\to\eta 'K^0$ decays
are penguin dominant ones,
their asymmetries also come from  $M_{12}^d$.
Then,  asymmetries of
 $B_d^0\to J/\psi K_S$,  $B_d^0\to \phi K_S$ and
$B_d^0\to \eta 'K^0$ are expected to be same magnitude in SM.

On the other hand,
 if the squark flavor mixing  contributes to the decay
 at the one-loop level, its magnitude could be  comparable
to the SM penguin one
 in  $B_d^0\to \phi K_S$ and $B_d^0\to \eta 'K^0$,
but it is tiny in $B_d^0\to J/\psi K_S$.
Endo, Mishima and Yamaguchi proposed the possibility to
 find the SUSY contribution  in these asymmetries
\cite{Endo:2004dc}.
The  present data suggest the deviation from SM
in these time dependent asymmetries  of  $B_d^0$ decays such as,
\begin{equation}
\mathcal{S}_{ J/\psi K_S}=0.671\pm 0.023, \qquad
\mathcal{S}_{\phi K_S}=0.39\pm 0.17, \qquad
\mathcal{S}_{\eta 'K^0}=0.60\pm 0.07 ,
\label{Sfdata}
\end{equation}
 however, precise data are required to justify the new physics contribution.

New physics contribute to the $b\to s\gamma$ process.
The observed $b\to s\gamma$ branching ratio (BR) is
$(3.60\pm  0.23)\times 10^{-4}$ \cite{PDG}, on the other hand
the SM prediction is given as $(3.15\pm  0.23)\times 10^{-4}$
at ${\cal{O}}(\alpha_s^2)$
\cite{Buras:1998raa,Misiak:2006zs}.
Therefore, the contribution of  new physics should be suppressed.
New  physics are  also constrained
 by the direct CP violation
\begin{equation}
A_{\text{CP}}^{b\to s\gamma}
\equiv
\frac{\Gamma (\bar{B} \to X_{s}\gamma )
-\Gamma (B \to X_{\bar{s}}\gamma )}
{\Gamma (\bar{B} \to X_{s}\gamma )
+\Gamma (B \to X_{\bar{s}}\gamma )} .
\end{equation}
Since SM prediction   $A_{\text{CP}}^{b\to s\gamma}\simeq 0.005$
is tiny \cite{Kagan:1998bh}, new physics may appear in this CP asymmetry.
The present data $A_{\text{CP}}^{b\to s\gamma}=-0.008\pm 0.029$ \cite{PDG}
has rather
large error bar, and so the constraint of  new physics is not so severe.
However, improved data will provide the crucial test for  new physics.
\section{Squark flavor mixing and CP violations of $B$ mesons}
\label{sec:Squark}
Let us consider the flavor structure of squarks
in order to estimate the CP-violating asymmetries of $B$ meson decays.
We take the most popular anzatz, which is to  postulate
a degenerate SUSY breaking mass spectrum for down-type squarks.
Then, in the super-CKM basis, we can parametrize
 the soft scalar masses squared
$M^2_{\tilde d_{LL}}$, $M^2_{\tilde d_{RR}}$,
$M^2_{\tilde d_{LR}}$, and $M^2_{\tilde d_{RL}}$ for the down-type squarks
as follows:
\begin{align}
M^2_{\tilde d_{LL}}&=m_{\tilde q}^2
\begin{pmatrix}
1+(\delta _d^{LL})_{11} & (\delta _d^{LL})_{12} & (\delta _d^{LL})_{13} \\
(\delta _d^{LL})_{12}^* & 1+(\delta _d^{LL})_{22} & (\delta _d^{LL})_{23} \\
(\delta _d^{LL})_{13}^* & (\delta _d^{LL})_{23}^* & 1+(\delta _d^{LL})_{33}
\end{pmatrix}, \nonumber \\
M^2_{\tilde d_{RR}}&=m_{\tilde q}^2
\begin{pmatrix}
1+(\delta _d^{RR})_{11} & (\delta _d^{RR})_{12} & (\delta _d^{RR})_{13} \\
(\delta _d^{RR})_{12}^* & 1+(\delta _d^{RR})_{22} & (\delta _d^{RR})_{23} \\
(\delta _d^{RR})_{13}^* & (\delta _d^{RR})_{23}^* & 1+(\delta _d^{RR})_{33}
\end{pmatrix}, \nonumber \\
M^2_{\tilde d_{LR}}&=(M_{\tilde d_{RL}}^2)^\dagger =m_{\tilde q}^2
\begin{pmatrix}
(\delta _d^{LR})_{11} & (\delta _d^{LR})_{12} & (\delta _d^{LR})_{13} \\
(\delta _d^{LR})_{21} & (\delta _d^{LR})_{22} & (\delta _d^{LR})_{23} \\
(\delta _d^{LR})_{31} & (\delta _d^{LR})_{32} & (\delta _d^{LR})_{33}
\end{pmatrix},
\end{align}
where  $m_{\tilde q}$ is the average squark mass, and
$(\delta _d^{LL})_{ij}$, $(\delta _d^{LR})_{ij}$, $(\delta _d^{RL})_{ij}$,
and $(\delta _d^{RR})_{ij}$ are  called as
the  mass insertion (MI) parameters.
The MI parameters are supposed to be much smaller than $1$.

The contribution of the gluino-squark box diagram to the dispersive part of the effective Hamiltonian for
the $B_q$-$\bar B_q$ mixing is written as \cite{Gabbiani:1996hi,Altmannshofer:2009ne}
\begin{align}
M_{12}^{q,SUSY}&=A_1^q\Big [A_2\left \{ (\delta _d^{LL})_{ij}^2+
(\delta _d^{RR})_{ij}^2\right \} +
A_3^q(\delta _d^{LL})_{ij}(\delta _d^{RR})_{ij} \nonumber \\
&+A_4^q\left \{ (\delta _d^{LR})_{ij}^2+(\delta _d^{RL})_{ij}^2\right \} +A_5^q(\delta _d^{LR})_{ij}(\delta _d^{RL})_{ij}\Big ],
\label{bbbarmixing}
\end{align}
where
\begin{align}
&A_1^q=-\frac{\alpha _S^2}{216m_{\tilde q}^2}\frac{2}{3}M_{B_q}f_{B_q}^2,
\qquad A_2=24xf_6(x)+66\tilde f_6(x),\nonumber \\
&A_3^q=\left \{ 384\left (\frac{M_{B_q}}{m_j+m_i}\right )^2+72 \right \}
xf_6(x)+\left \{ -24\left (\frac{M_{B_q}}{m_j+m_i}\right )^2+36\right \}
\tilde f_6(x), \nonumber \\
&A_4^q=\left \{ -132\left (\frac{M_{B_q}}{m_j+m_i}\right )^2 \right \}
 xf_6(x),\quad A_5^q=\left \{ -144\left (\frac{M_{B_q}}{m_j+m_i}\right )^2-84\right \}\tilde f_6(x).
\label{Adef}
\end{align}
Here,  we use $x=m_{\tilde g}^2/m_{\tilde q}^2$, where
$m_{\tilde g}$ is the gluino mass.
For the cases of $q=d$ and  $q=s$, we take $(i, j)= (1,3)$ and
 $(i, j)= (2,3)$, respectively, where $m_1=m_d$, $m_2=m_s$ and $m_3=m_b$.
The loop functions
$f_6(x)$ and  $\tilde f_6(x)$ are shown  in \cite{Hayakawa:2012ua}.

For the case of $x\simeq 1$,  we get $A_2\simeq -1$,
$A_3^q\simeq 30$, $A_4^q\simeq -10$ and   $A_5^q\simeq 10$.
Therefore, each term at the r.h.s. of Eq.(\ref{bbbarmixing})
  may contribute to $M_{12}^{q,SUSY}$ comparably.
However, magnitudes of
$(\delta _d^{LR})_{ij}$  and $(\delta_d^{RL})_{ij}$ are constrained
severely by the  $b\to s\gamma $ decay as discussed later.

The squark flavor mixing can be tested in
 the CP-violating  asymmetries  in the neutral $B$ meson decays.
Let us present the framework of these calculations.
The effective Hamiltonian for $\Delta B=1$
process is defined as
\begin{equation}
H_{eff}=\frac{4G_F}{\sqrt{2}}\left [\sum _{q'=u,c}V_{q'b}V_{q's}^*\sum _{i=1,2}C_iO_i^{(q')}-V_{tb}V_{ts}^*
\sum _{i=3-6,7\gamma ,8G}\left (C_iO_i+\widetilde C_i\widetilde O_i\right )\right ],
\end{equation}
where the local operators are given as
\begin{align}
&O_1^{(q')}=(\bar s_\alpha\gamma _\mu P_Lq_\beta')
(\bar q_\beta'\gamma ^\mu P_Lb_\alpha),
\qquad O_2^{(q')}=(\bar s_\alpha\gamma _\mu P_Lq_\alpha')
(\bar q_\beta'\gamma ^\mu P_Lb_\beta), \nonumber \\
&O_3=(\bar s_\alpha\gamma _\mu P_Lb_\alpha)\sum _q(\bar q_\beta\gamma ^\mu P_Lq_\beta),
\quad O_4=(\bar s_\alpha\gamma _\mu P_Lb_\beta)\sum _q(\bar q_\beta\gamma ^\mu P_Lq_\alpha), \nonumber \\
&O_5=(\bar s_\alpha\gamma _\mu P_Lb_\alpha)\sum _q(\bar q_\beta\gamma ^\mu P_Rq_\beta),
\quad O_6=(\bar s_\alpha\gamma _\mu P_Lb_\beta)\sum _q(\bar q_\beta\gamma ^\mu P_Rq_\alpha), \nonumber \\
&O_{7\gamma }=\frac{e}{16\pi ^2}m_b\bar s_\alpha\sigma ^{\mu \nu }P_Rb_\alpha
F_{\mu \nu },
\qquad O_{8G}=\frac{g_s}{16\pi ^2}m_b\bar s_\alpha\sigma ^{\mu \nu }
P_RT_{\alpha\beta}^ab_\beta G_{\mu \nu }^a,
\end{align}
where
$P_R=(1+\gamma_5)/2$, $P_L=(1-\gamma_5)/2$, and $\alpha$ and $\beta$ are color
 indices, and $q$ is taken to be $u,d,s,c$.
Here, $C_i$'s  $\widetilde C_i$'s are the Wilson coefficients,
and $\widetilde O_i$'s are  the operators by replacing  $L(R)$ with  $R(L)$
in $O_i$.
In this paper, $C_i$ includes both SM contribution and gluino   one,
such as  $C_i=C_i^{\rm SM}+C_i^{\tilde g}$, where
$C_i^{\text{SM}}$ is given in Ref.~\cite{Buchalla:1995vs} and
$C_i^{\tilde g}$ is  presented  as follows \cite{Endo:2004fx}:
\begin{align}
C_3^{\tilde g}&\simeq \frac{\sqrt{2}\alpha _s^2}{4G_FV_{tb}V_{ts}^*m_{\tilde q}^2}(\delta _d^{LL})_{23}
\left [-\frac{1}{9}B_1(x)-\frac{5}{9}B_2(x)-\frac{1}{18}P_1(x)-\frac{1}{2}P_2(x)\right ], \nonumber \\
C_4^{\tilde g}&\simeq \frac{\sqrt{2}\alpha _s^2}{4G_FV_{tb}V_{ts}^*m_{\tilde q}^2}(\delta _d^{LL})_{23}
\left [-\frac{7}{3}B_1(x)+\frac{1}{3}B_2(x)+\frac{1}{6}P_1(x)+\frac{3}{2}P_2(x)\right ], \nonumber \\
C_5^{\tilde g}&\simeq \frac{\sqrt{2}\alpha _s^2}{4G_FV_{tb}V_{ts}^*m_{\tilde q}^2}(\delta _d^{LL})_{23}
\left [\frac{10}{9}B_1(x)+\frac{1}{18}B_2(x)-\frac{1}{18}P_1(x)-\frac{1}{2}P_2(x)\right ], \nonumber \\
C_6^{\tilde g}&\simeq \frac{\sqrt{2}\alpha _s^2}{4G_FV_{tb}V_{ts}^*m_{\tilde q}^2}(\delta _d^{LL})_{23}
\left [-\frac{2}{3}B_1(x)+\frac{7}{6}B_2(x)+\frac{1}{6}P_1(x)+\frac{3}{2}P_2(x)\right ], \nonumber \\
C_{7\gamma }^{\tilde g}&\simeq -\frac{\sqrt{2}\alpha _s\pi }{6G_FV_{tb}V_{ts}^*m_{\tilde q}^2}
\Bigg [(\delta _d^{LL})_{23}\left (\frac{8}{3}M_3(x)-
\mu \tan \beta \frac{m_{\tilde g}}{m_{\tilde q}^2}\frac{8}{3}M_a(x)\right )
+(\delta _d^{LR})_{23}\frac{m_{\tilde g}}{m_b}\frac{8}{3}M_1(x)\Bigg ], \nonumber \\
C_{8G}^{\tilde g}&\simeq -\frac{\sqrt{2}\alpha _s\pi }{2G_FV_{tb}V_{ts}^*m_{\tilde q}^2}
\Bigg [(\delta _d^{LL})_{23}\Bigg \{ \left (\frac{1}{3}M_3(x)+3M_4(x)\right ) \nonumber \\
&-\mu \tan \beta \frac{m_{\tilde g}}{m_{\tilde q}^2}\left (\frac{1}{3}M_a(x)+3M_b(x)\right )\Bigg \}
+(\delta _d^{LR})_{23}\frac{m_{\tilde g}}{m_b}\left (\frac{1}{3}M_1(x)+3M_2(x)\right )\Bigg ].
\label{Coeff}
\end{align}
Here the double mass insertion is included in $C_{7\gamma }^{\tilde g}$
and $C_{8G}^{\tilde g}$.
The Wilson coefficients  $\widetilde C_i^{\tilde g}$'s are
obtained by replacing $L(R)$ with $R(L)$ in  $C_i^{\tilde g}$'s.
The loop functions, which we use in our calculations, are presented
in our previous paper \cite{Hayakawa:2012ua}.

The CP-violating  asymmetries $\mathcal{S}_f$ in Eq.~(\ref{sf}) are
 calculated by using $\lambda_f$, which is given
 for  $B_d^0\to \phi K_S$ and $B_d^0\to \eta 'K^0$ as follows:
\begin{align}
\lambda_{\phi K_S,\  \eta 'K^0}&=-e^{-i\phi _d}\frac{\displaystyle \sum _{i=3-6,7\gamma ,8G}
\left (C_i^\text{SM}\langle O_i \rangle+C_i^{\tilde g}\langle O_i \rangle+
\widetilde C_i^{\tilde g}\langle \widetilde O_i \rangle \right )}
{\displaystyle \sum _{i=3-6,7\gamma ,8G}
\left (C_i^{\text{SM}*}\langle O_i \rangle+C_i^{{\tilde g}*}
\langle O_i \rangle+\widetilde C_i^{{\tilde g}*}\langle\widetilde O_i \rangle \right )}~,
\label{asymBd}
\end{align}
where  $\langle O_i \rangle$ is the abbreviation of
  $\langle f |O_i | B_q^0\rangle$.
It is noticed that
$\langle\phi K_S|O_i|B_d^0\rangle=\langle\phi K_S|
\widetilde O_i|B_d^0\rangle $
and $\langle\eta' K^0|O_i|B_d^0\rangle=-\langle\eta' K^0|
\widetilde O_i|B_d^0\rangle$
because of  the parity of the final state.
We  have also $\lambda_{f}$ for  $B_s^0\to\phi \phi$
as follow:
\begin{align}
\lambda_{\phi \phi}&=e^{-i\phi _s}\frac{\displaystyle \sum _{i=3-6,7\gamma ,8G}
C_i^\text{SM}\langle O_i \rangle+C_i^{\tilde g}\langle O_i \rangle+
\widetilde C_i^{\tilde g}\langle \widetilde O_i \rangle}
{\displaystyle \sum _{i=3-6,7\gamma ,8G}
C_i^{\text{SM}*}\langle O_i \rangle+C_i^{{\tilde g}*}
\langle O_i \rangle+\widetilde C_i^{{\tilde g}*}\langle\widetilde O_i \rangle}~,
\label{asymBs}
\end{align}
with
$\langle\phi\phi|O_i|B_s^0\rangle=-\langle\phi\phi|\widetilde O_i|B_s^0\rangle $.

In these  non-leptonic decays, the $C_{8G}^{\tilde g}\langle O_{8G}\rangle$
dominates these amplitude, but
small  contributions from other  Wilson coefficients
 are also  taken account in  our calculations.
Therefore, we estimate each  hadronic matrix elements
by using the factorization relations in Ref.~\cite{Harnik:2002vs}.

Let us discuss the each contribution of the mass insertion parameters
 to  $C_{8G}^{\tilde g}$ in Eq.(\ref{Coeff}).
Taking account that the loop functions $M_i(x)$ are of  same order
and $m_{\tilde g}\simeq m_{\tilde q}$, the ratio of
$LL$ component and $LR$ one is
$(\delta_d^{LL})_{23}\times \mu\tan\beta/m_{\tilde q}$ to
$(\delta_d^{LR})_{23}\times m_{\tilde q}/m_b$.
If  ${\cal O}(\mu\tan\beta)\simeq {\cal O}(m_{\tilde q})$ and
$m_{\tilde q}\geq 1$ TeV, the $LR$ component may  contribute  significantly
to $C_{8G}^{\tilde g}$  due to the enhancement factor
$m_{\tilde q}/m_b={\cal O}(10^2)$.
For example, in the case of $(\delta_d^{LL})_{23}=10^{-2}$
and  $(\delta_d^{LR})_{23}=10^{-3}$, the $LR$ component
dominate $C_{8G}^{\tilde g}$, while it is minor
in $M_{12}^{q,\text{SUSY}}$ as seen in  Eq.(\ref{bbbarmixing}).
This situation is also kept in the  $b\to s\gamma $ decay.

The $b\to s\gamma $ decay is a typical one to investigate new physics.
The branching ratio is given as
\begin{equation}
\frac{BR(B \to X_s \gamma )}
{BR(B \to X_c  e \bar{\nu_e})}
=
\frac{|V_{ts}^*V_{tb}|^2}
{|V_{cb}|^2}
\frac{6 \alpha}{\pi f(z)}
|C_{7\gamma}^{\text{eff}}|^2 ,
\end{equation}
where
\begin{equation}
f(z)
=
1-8z+8z^3-z^4-12z^2 \text{ln}z \ ,  \qquad
z = \frac{m_{c}^2} {m_{b}^2}.
\end{equation}
Here, $C_{7\gamma}^{\text{eff}}$ includes both contributions
from the SM and  the gluino-squark flavor mixing $C_{7\gamma}^{\tilde g}$.
As seen  in Eq.(\ref{Coeff}), both  $C_{7\gamma}^{\tilde g}$ and
  $C_{8G}^{\tilde g}$ have the  similar dependence of
  $(\delta _d^{LR})_{23}$.
Therefore, we should discuss carefully the contribution
  from $(\delta _d^{LR})_{23}$ in our numerical calculations.

We can discuss the direct CP violation  $A_{\text{CP}}^{b\to s\gamma}$
in the $b\to s\gamma $ decay, which  is given as \cite{Kagan:1998bh}
\begin{equation}
\begin{split}
A_{\text{CP}}^{b \to s \gamma}
&=
\left.
\frac{\Gamma(\bar{B} \to X_s \gamma) - \Gamma(B \to X_{\bar{s}} \gamma)}
{\Gamma(\bar{B} \to X_s \gamma) + \Gamma(B \to X_{\bar{s}} \gamma)}
\right|_{E_{\gamma} > (1-\delta) E_{\gamma}^{\text{max}}} \\
&=
\frac{\alpha_s (m_b)}
{|C_{7\gamma}|^2}
\Big [
\frac{40}{81}
\text{Im} \small[ C_2 C_{7\gamma}^* \small]
-
\frac{8 z}{9} \small[v(z)+b(z, \delta)\small ]
\text{Im}\Big[\left (1+\frac{V_{us}^* V_{ub}}{V_{ts}^* V_{tb}}\right  )
C_2 C_{7\gamma}^*\Big] \nonumber \\
&
-\frac{4}{9}
\text{Im} \small[ C_{8G} C_{7\gamma}^* \small]
+
\frac{8z}{27}
b(z,\delta) \text{Im} \Big[ \left(1+\frac{V_{us}^* V_{ub}}{V_{ts}^* V_{tb}} \right ) C_2 C_{8G}^* \Big]
\Big ],
\end{split}
\end{equation}
where $v(z)$ and $b(z,\delta)$ are explicity given in  \cite{Kagan:1998bh},
and $C_i^{\text{eff}}$ includes both the SM and SUSY contributions.
Although the experimental data has still large error bar,
 we can discuss  the SUSY contribution to
 $A_{\text{CP}}^{b\to s\gamma}$.

Let us set up the framework of our calculations.
Suppose that $\mu\tan\beta$ is at most ${\cal} O(1)$TeV.
Then, magnitudes of $(\delta _d^{LL})_{23}$ and $(\delta _d^{RR})_{23}$
are constrained by $M_{12}^s$ as seen in Eq.(\ref{bbbarmixing}).
Taking account of $h_s=0.1$ in Eq.(\ref{hsigmaLHCb}),
  we obtain  $|(\delta _d^{LL})_{23}|\simeq |(\delta _d^{RR})_{23}|\simeq 0.02$
 in our  previous work \cite{Hayakawa:2012ua}.
Then,   these contributions to  $C_{7\gamma}^{\tilde g}$ and
$C_{8G}^{\tilde g}$ are minor.

On the other hand,  $(\delta _d^{LR})_{23}$ and $(\delta _d^{RL})_{23}$
are severely  constrained by  $C_{7\gamma}^{\text{eff}}$ and
$C_{8G}^{\text{eff}}$.
We show the constraint for
$(\delta _d^{LR})_{23}$ and $(\delta _d^{RL})_{23}$
in our following calculations.
In our convenience,  we suppose
$|(\delta _d^{LR})_{23}|=|(\delta _d^{RL})_{23}|$.
Then, we can   parametrize these parameters  as follows:
\begin{equation}
(\delta _d^{LR})_{23}=|(\delta _d^{LR})_{23}|e^{2i\theta _{23}^{LR}},
\qquad (\delta _d^{RL})_{23}=|(\delta _d^{LR})_{23}|e^{2i\theta _{23}^{RL}},
\label{MILR}
\end{equation}
where $\theta _{23}^{LR}$ and $\theta _{23}^{RL}$ are taken
 in the region $[0-\pi]$.
By using this set up, we show  numerical analyses in the next section.

\section{Numerical analyses}
\label{sec:Numerical}

In this section, we show the numerical analyses of the CP-violation
 in the $B$ mesons.
In our following numerical calculations,
 we fix the squark mass and the gluino mass as
\begin{equation}
m_{\tilde q}=1000~\text{GeV},\qquad m_{\tilde g}=1500~\text{GeV},
\end{equation}
which are consistent with recent lower bound of these masses at LHC
\cite{Aad:2011ib}.
We use  relevant parameters as given in \cite{Hayakawa:2012ua}
to estimate  the SM contribution.

At first, we discuss  the $b\to s\gamma$ decay.
The observed $b\to s\gamma$ branching ratio is
$(3.60\pm  0.23)\times 10^{-4}$ \cite{PDG}, on the other hand
the SM prediction is given as $(3.15\pm  0.23)\times 10^{-4}$
at ${\cal{O}}(\alpha_s^2)$
\cite{Buras:1998raa,Misiak:2006zs}.
Since $\mu\tan\beta$ is supposed to be lower than ${\cal O}(1~{\rm TeV})$,
the contribution of $(\delta _d^{LL})_{23} \simeq (\delta _d^{RR})_{23}$
 is negligibly small.
The  contribution of $(\delta _d^{LR})_{23}$ becomes  important
 through the interference with the SM component
in the decay amplitude. On the other hand,  since $(\delta _d^{RL})_{23}$
does not interfere with the SM component, its contribution is minor.
 The branching ratio gives the constraint for the magnitude
 of $(\delta _d^{LR})_{23}$.
The direct CP violation of the $b\to s\gamma$ is also
useful to constraint  $(\delta _d^{LR})_{23}$.
We show the $A_{\text{CP}}^{b \to s \gamma}$
versus $|(\delta _d^{LR})_{23}|$ in Figure 1,
where the upper and lower bounds of the experimental data with $90\%$ C.L.
 are denoted red lines, and the predicted value of the SM
is  shown  by the green line as the  eye guide.
 As far as $|(\delta _d^{LR})_{23}|\leq 10^{-3}$,
 the predicted value is within the experimental allowed region.

In Figure 2,
we show the  $|(\delta _d^{LR})_{23}|$ dependence of the branching ratio
taking accont   the constraint of $A_{\text{CP}}^{b \to s \gamma}$
as seen in Figure 1.
 Here,  the allowed  region at $|(\delta _d^{LR})_{23}|=0$
 is the SM prediction.
As the magnitude of    $(\delta _d^{LR})_{23}$ increases,
 the predicted  region of the branching ratio splits into the larger
 region and smaller one.
The excluded region between two regions   is due to
the constraint of $A_{\text{CP}}^{b \to s \gamma}$.
Then,
 the predicted branching ratio becomes inconsistent with
 the experimental data at $|(\delta _d^{LR})_{23}|\geq 5.5\times 10^{-3}$.

\begin{figure}[b!]
\begin{minipage}[]{0.45\linewidth}
\vspace{4 mm}
\includegraphics[width=8cm]{fig1.eps}
\caption{The direct CP violation  $A_{\text{CP}}^{b \to s \gamma}$
versus $|(\delta _d^{LR})_{23}|$,
where the green line denotes the SM prediction
and  red lines denote the upper and lower bounds of the experimental data with $90\%$ C.L..}
\end{minipage}
\hspace{5mm}
\begin{minipage}[]{0.45\linewidth}
\includegraphics[width=8cm]{fig2.eps}
\caption{The predicted branching ratio of  $b\to s\gamma$
versus $|(\delta _d^{LR})_{23}|$, where the experimental constraint
of $A_{\text{CP}}^{b \to s \gamma}$ is taken account.
Predicted value at $|(\delta _d^{LR})_{23}|=0$ is the SM one.}
\end{minipage}
\end{figure}

In order to see the role of the  phase  $\theta _{23}^{LR}$,
 we show  $A_{\text{CP}}^{b \to s \gamma}$
versus  $\theta _{23}^{LR}$ for $|(\delta _d^{LR})_{23}|= 10^{-3}$(blue)
and $|(\delta _d^{LR})_{23}|= 10^{-4}$(orange) in Figure 3.
 The pink horizontal lines denote
the  experimental upper and lower bounds at  $1\sigma$ level.
As seen in this figure,
we find  that
 the reduction  of the experimental error-bar will constrain the SUSY
phase  $\theta _{23}^{LR}$ severely.

In Figure 4,
we plot the allowed region
on the   $|(\delta _d^{LR})_{23}|-\theta _{23}^{LR}$ plane
by putting  the experimental data at $90\%$ C.L. of
the branching ratio and the direct CP violation
$A_{\text{CP}}^{b \to s \gamma}$.
 The allowed region of  $|(\delta _d^{LR})_{23}|$ is cut
at $5.5\times 10^{-3}$,
where   $\theta _{23}^{LR}$ is tuned around $\pi/2$.
Around $\pi/4$ and  $3\pi/4$,  $A_{\text{CP}}^{b \to s \gamma}$
give the severe constraint as seen in Figure 3.
This  CP violation phase
  also contributes on the CP-violating asymmetry
 of the non-leptonic decays of  $B_d^0$ and $B_s^0$ mesons.

Let us discuss ${\mathcal S}_{f}$, which is the measure
 of the CP-violating asymmetry,
for  $B_d^0\to {J/\psi  K_S}, \ {\phi K_S}, \  {\eta' K^0}$.
As discussed in Section 2,
these   ${\mathcal S}_{f}$'s are predicted
 to be same ones in the SM.
On the other hand,
 if the squark  flavor mixing contributes to the decay process
 at the one-loop level, these asymmetries are different
 from among as seen in  Eq.(\ref{asymBd}).

\begin{figure}[b!]
\begin{minipage}[]{0.45\linewidth}
\includegraphics[width=8cm]{fig3.eps}
\caption{$A_{\text{CP}}^{b \to s \gamma}$
versus  $\theta _{23}^{LR}$ for $|(\delta _d^{LR})_{23}|= 10^{-3}$(blue)
and $10^{-4}$(orange), where
the pink  lines denote
the  experimental upper and lower bounds at  $1\sigma$ level.}
\end{minipage}
\hspace{5mm}
\begin{minipage}[]{0.45\linewidth}
\vspace{0mm}
\includegraphics[width=8cm]{fig4.eps}
\caption{The allowed region
 on  $|(\delta _d^{LR})_{23}|$-  $\theta _{23}^{LR}$ plane.
The experimental data at $90\%$ C.L. of
the branching ratio and
$A_{\text{CP}}^{b \to s \gamma}$ are taken account.}
\end{minipage}
\end{figure}

\begin{figure}[b!]
\begin{minipage}[]{0.45\linewidth}
\includegraphics[width=8cm]{fig5.eps}
\caption{$S_{\phi K_S}$ of $B_d^0$ versus
 $A_{\text{CP}}^{b \to s \gamma}$ for $|(\delta _d^{LR})_{23}|= 10^{-3}$(blue)
and $10^{-4}$(orange).}
\end{minipage}
\hspace{5mm}
\begin{minipage}[]{0.45\linewidth}
\vspace{-4mm}
\includegraphics[width=8cm]{fig6.eps}
\caption{$S_{\eta 'K^0}$ of $B_d^0$ versus
 $A_{\text{CP}}^{b \to s \gamma}$ for $|(\delta _d^{LR})_{23}|= 10^{-3}$(blue)
and $10^{-4}$(orange).}
\end{minipage}
\end{figure}

Since  the  phase $\theta _{23}^{LR}$  contributes to
 $A_{\text{CP}}^{b \to s \gamma}$,
$\mathcal{S}_{\phi K_S}$ and $\mathcal{S}_{\eta 'K^0}$ of $B_d^0$ decays.
We expect the correlations among them.
We  fix  $|(\delta _d^{LR})_{23}|=10^{-4}$(orange)
and $10^{-3}$(blue) for typical values  in the following calculations.
we show the predicted regions on the
$A_{\text{CP}}^{b \to s \gamma}$-$\mathcal{S}_{\phi K_S}$ and
 $A_{\text{CP}}^{b \to s \gamma}$-$\mathcal{S}_{\eta 'K^0}$ planes
 in Figures 5 and 6, respectively.
The experimental data is denoted by red lines at $90\%$ C.L..
We also present
the predicted region on
 the $\mathcal{S}_{\phi K_S}$-$\mathcal{S}_{\eta 'K^0}$ plane in Figure 7,
the slant dashed line denotes the SM prediction
$\mathcal{S}_{J/\psi K_S}=\mathcal{S}_{\phi K_S}=\mathcal{S}_{\eta 'K}$,
where the observed value
 $\mathcal{S}_{J/\psi K_S}=0.671\pm 0.023$ is put.
The reduction of the experimental error of
 $A_{\text{CP}}^{b \to s \gamma}$ will give us severe predictions for
$\mathcal{S}_{\phi K_S}$ and $\mathcal{S}_{\eta 'K^0}$.
It is noticed that this predicted region   is different
from the one in the previous work
\cite{Hayakawa:2012ua}, where $(\delta _d^{LR})_{23}$ is neglected
and  $\mu\tan\beta={\cal O}(10~{\rm TeV})$.

As seen in Figures 5, 6 and 7,
 the reduction of the experimental errors will provide powerful tool
to find the contribution of the squark flavor mixing.
At last, we show
the correlation between $A_{\text{CP}}^{b \to s \gamma}$ and
$\mathcal{S}_{\phi \phi}$ of the $B_s^0$ decay in Figure 8.
We expect the observation of the CP violation in
  $B_s^0\to \phi \phi$ at LHCb.

\begin{figure}[h!]
\begin{minipage}[]{0.45\linewidth}
\includegraphics[width=8cm]{fig7.eps}
\caption{Predeicted region on the $S_{\phi K_S}$-$S_{\eta 'K^0}$ plane, where
the slant dashed line denotes the SM prediction.}
\end{minipage}
\hspace{5mm}
\begin{minipage}[]{0.45\linewidth}
\vspace{-4mm}
\includegraphics[width=8cm]{fig8.eps}
\caption{Predicted  asymmetry  $S_{\phi \phi }$ in the $B_s^0$ decay
versus
 $A_{\text{CP}}^{b \to s \gamma}$.}
\end{minipage}
\end{figure}

\section{Summary}
\label{sec:Summary}
The CP violation of the neutral $B$ meson is the important phenomenon
to search for  new physics.
We have discussed the contribution of the squark flavor mixing
from  $(\delta _d^{LR})_{23}$ and $(\delta _d^{RL})_{23}$
on the direct CP violation of the $b\to s\gamma$ decay and
the CP-violating asymmetry in the non-leptonic decays of
$B_d^0$ and $B_s^0$ mesons.

The magnitude of $|(\delta _d^{LR})_{23}|$
is bounded by the branching ratio of  $b\to s\gamma$
 with  the constraint of $A_{\text{CP}}^{b \to s \gamma}$.
 The predicted branching ratio becomes inconsistent with
 the experimental data at $|(\delta _d^{LR})_{23}|\geq 5.5\times 10^{-3}$.
We have obtained  the allowed region
on the   $|(\delta _d^{LR})_{23}|$-$\theta _{23}^{LR}$ plane.
 While the $|(\delta _d^{LR})_{23}|$ is cut at $5.5\times 10^{-3}$,
CP-violating phase  $\theta _{23}^{LR}$ is severely constrained
 at  $|(\delta _d^{LR})_{23}|\geq 2\times 10^{-3}$.
This  CP-violating phase also contribute
to the CP-violating asymmetry in the non-leptonic decays of
$B_d^0$ and $B_s^0$ mesons.

We have predicted the correlation among $A_{\text{CP}}^{b \to s \gamma}$ and
$\mathcal{S}_{f}$ of the $B_d^0$ and $B_s^0$ decays.
These CP-violating asymmetries could deviate from
the SM predictions.

Since we suppose
rather small $\mu\tan\beta, \ {\cal O}(1~{\rm TeV})$,
the contribution from $LL(RR)$ components are minor
 in these CP-violating asymmetries.
In this case,  the new physics contribution
 is minor in $M_{12}^q$ of $B_q-\bar B_q \ (q=d,s)$ mixing
since $|(\delta _d^{LR})_{23}|$ is at most ${\cal O}(10^{-3})$.
This result is consistent with the recent result
 of the CP violations at  LHCb as discussed in Section 2.

 In the near future,
 the precise data of
the direct CP violation of  $b\to s\gamma$ and  CP-violating asymmetries
 in the non-leptonic decays of
$B_d^0$ and $B_s^0$ mesons  give us the crucial  test
 for  our  framework of the squark flavor mixing.

\vspace{0.5 cm}
\noindent
{\bf Acknowledgement}

We thank Drs. E. Ko, Y. Okada, and T. Morozumi for useful discussions.
We also thank A. Hayakawa for his help.
M.T. is  supported by JSPS Grand-in-Aid for Scientific Research,
21340055 and 24654062.

redpajama_set_name: RedPajamaArXiv


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text:
Mobility, Security
Lookout brings its enterprise mobile security to market
Lookout's enterprise offering, which leverages the data set from its 70 million consumer customers, will be sold entirely through channel partners, and entirely through distribution, which in North America will be Ingram Micro.
Aaron Cockerill, VP of Products at Lookout
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Unusually for a new SaaS product, Lookout will be using VARs, and going exclusively through distribution from Day One.
David Helfer, Lookout's Vice President of Worldwide Channel Development
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That strategy involves putting one distributor in place for each global region. In North America, that will be Ingram Micro. The deal for the U.S. is signed. The deal for Canada is not signed yet, but Helfer said it is a simple rider.
"We want to go out the door with a crystal clear understanding of trust, and this is a very good model to establish it with distribution," he said. "Many global integrators would like to buy from us directly, but there will be no such thing as a reseller or customer buying from Lookout directly. We wanted to put as many dollars as possible through distribution to get trust from them. That's how we were able to sign distribution."
Availability Lookout Mobile Threat Protection will be generally available in English on June 30. Localized versions in French, German and Japanese will be launching later this year.
Tags:Aaron Cockerill Android Apple Apps David Helfer Ingram Micro Lookout Malware
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Michał is a very friendly and passionate tutor. He has been helping me a lot with my Polish. He prepares materials for each class and gives me many useful feedback. I highly recommend him as your Polish teacher.
From the very first lesson, Polish will be the only language that you hear and use. By looking at pictures and illustrations and listening to dialogues, you will learn in a natural way – like a child learns the language by listening and observing the world around them. You will discover new words, expressions and grammar structures in their natural context and in carefully planned order.
To help you out we've created this brand new kids' guide to help you Learn Polish!
Learn some of the most used words and phrases including greetings, directions, animals and loads more!
So whether you want to say good morning – dzień dobry – or ask for a tasty pastry – drożdżówka – you'll be able to hear exactly how it should be pronounced!


Wow-that is crazy! I can't believe that happened. I do feel a little sad for the snake even though I would have been terrified if I found a snake in the house.
Oh my GOD. That is almost worse than finding an earwig in your bed!
Totally yuck! I hate snakes!!! I saw one the other day under our carport, I ran inside and locked the door while Matt played with it...ew, ew, ew!
KIND of creepy?? You would have had to pry me off of the ceiling. Eeeeeek!!!
Um wow! I think I'd die. Though I'm not particularly afraid of snakes, I still thinking finding one beside my bed would definitely freak me out!


Kids Rock Ministry has been described as a variety show with an anointed finale. They will be our evangelists at Atlantic Kids Camp (June 29-July 3) they will also be ministering throughout the Atlantic District during the month of July.
Kids Rock bases their evangelistic ministry out of Bakersfield, California; John is the Secretary for the Western District Children's Ministry. John & Jennie Lagas encourage kids that they don't have to wait until they are older to live for Jesus! From puppets, to crazy props, multimedia, hilarious characters and antics, music, and games, John, Jennie, and their 3 daughters (Michaela, Kaitlyn, and Madison) engage children on a roller coaster ride of bible-based fun with a stirring sermon on a kid's level that will bring them to a destination of prayer, repentance, and seeking of the Holy Ghost.


GHC 7.10 only works with cabal-install version 1.22 or later. Please upgrade if you have an older version of cabal-install.
The operating system-specific packages (e.g. RPM or .deb packages on Linux) are generally a better bet than the vanilla .tar.bz2 binary bundles, because they will check for dependencies and allow the package to be uninstalled at a later date.
Note: These builds were prepared on Debian Jessie. Note that ARM support is still a bit experimental. This build is intended for use with LLVM 3.5 (available in Debian Jessie). Due to bugs in BFD ld it is necessary to use the gold linker.
This is compatible with Microsoft Windows XP and later, including the Windows 10 Creator's Update. It also includes support for compiling C++ files.
This is compatible with Microsoft Windows XP and later, excluding the Windows 10 Creator's Update. It also includes support for compiling C++ files.
This is a bindist for Mac OS X, 10.7 or later. The package requires the command line tools package of Xcode 4 or XCode 5 to be installed. You can find Xcode at http://developer.apple.com/.
See the FreeBSD readme for details.
The source distribution needs an installed GHC (version 7.6 at least). If your platform isn't currently supported with a binary distribution, then you'll need to consult the section on Porting GHC in the Building Guide.


text:
Q: A question on anaphoric and cataphoric references Is it 'this' or 'that' that conveys an anaphoric reference?
I want to refer back to "that I wrote critical and analytical essays".

It is true that I wrote critical and analytical essays on a regular
  basis; that, however, did not satisfy my academic eagerness.

or?

It is true that I wrote critical and analytical essays on a regular
  basis; this, however, did not satisfy my academic eagerness.

A: The Cambridge Grammar of the English Language in its section (p1506) on anaphoric uses of this and that with noun phrases as antecedents states:

... both this and that can be used anaphorically - and in general one
  could be replaced by the other with very little effect on the meaning.

In contrast, Swan in Practical English Usage (p591) does detect a slight difference:

This is preferred when there is more to say about the new subject of
  discussion:
"Then in 1917 he met Andrew Lewis. This was a turning point in his
  career: the two men entered into a partnership that lasted until 1946,
  and ..."
(More natural than ... "That was a turning point ...")

It is likely that the OP's sentence will be followed by something more on the new subject (academic eagerness). For example:

It is true that I wrote critical and analytical essays on a regular
  basis; this, however, did not satisfy my academic eagerness. I also
  engaged in research ... etc.

Thus if we follow Swan, this is to be preferred to that in the context of the OP's sentence.
This, as the more present or proximal pronoun, may also better convey the sense that what is being referred to is relevant in the present context (for example, an application letter or cv). So, in the context I have assumed for the OP I would use this.

A: It's true that this is used in cataphoric reference and that hardly ever; but they are also both widely used in anaphor, the basic difference then being that this is proximal, that distal.
In practice, however, unless there are two likely referents to distinguish between, they are pretty much interchangeable in anaphor.

redpajama_set_name: RedPajamaStackExchange


text:
Senate Votes to Go to Conference on Zika Spending
Democrats brand public health response the fight of the month
Posted Jun 8, 2016 5:53 PM
Ryan McCrimmon
@RyanMcCrimmon
Senate GOP Seeks Tax Law Fixes, Including 'Retail Glitch' Speeding Through Spending Bills Wyden to Delay Treasury Nominee Amid Tax and Oversight Fights
Centers for Disease Control and Prevention Director Tom Frieden watches as National Institute of Allergy and Infectious Diseases Director Anthony Fauci speaks during a February House Foreign Affairs hearing on the Zika outbreak. (Photo By Al Drago/CQ Roll Call)
The Senate agreed by voice vote Wednesday night to join the House in formal negotiations over a Zika virus response package, the latest incremental step toward clearing a bill for President Barack Obama's signature.
The vote comes four months after Obama requested $1.9 billion in emergency spending in February to combat the mosquito-borne disease. Informal discussions between House and Senate leaders and appropriators have been ongoing for weeks, but it remains unclear how the chambers will bridge major differences in their Zika legislation.
"We all agree that the Zika virus is a real threat and needs to be addressed," Senate Majority Leader Mitch McConnell , R-Ky., said. "Republicans and Democrats worked together to pass a bill here in the Senate to provide funding and resources. The House passed its own version. We're ready now to go to conference and complete a final bill."
The Senate also voted 46-49 to reject a motion from Bill Nelson , D-Fla., to instruct Zika conferees to reject proposals to rescind existing Ebola virus emergency funds and to insist that Ebola accounts be reimbursed with $510 million.
The House voted in May to go to conference over its proposed $622 million Zika package and other legislation. The Senate passed a $1.1 billion emergency spending proposal last month as part of a broader appropriations package.
The House-passed funding measure is fully offset — no new spending — and would expire at the end of the fiscal 2016 on Sept. 30, while the Senate version is not offset and has no such expiration date.
As McConnell spoke on the chamber floor earlier Wednesday, Senate Democrats gathered for a news conference nearby with public health experts and vowed to keep pressing Republicans until a bill was on the president's desk.
[ Congress Failing Zika Test ]
"This is the fight of the month," said Sen. Amy Klobuchar , D-Minn. "It sure better get done in this work period. What, are they going to go home for six weeks and not have any funding done for Zika as we go into these summer months? That would be atrocious."
Congress is scheduled to leave town July 15 and return Sept. 6, a break of more than seven weeks.
Democrats have slammed Republicans for dragging their feet since February, urging them several times to cancel multiple recesses since then to stay in town and finish work on a Zika response. Congress blew past the latest deadline set by the Obama administration, which wanted a final bill for the president's signature by the end of May.
Now members on both sides are eyeing the end of June as the next, and most serious, deadline.
"I think our goal is to get this done in the month of June," said Sen. Roy Blunt of Missouri, a member of GOP leadership and senior appropriator who spearheaded the $1.1 billion compromise measure.
Klobuchar said she wants to "definitely see it before the Fourth of July."
In mid-April, Barbara A Mikulski of Maryland, the top Democrat on Senate Appropriations, had already tagged July 1 as the deadline for clearing a Zika response. "I don't mean start it July 1 – complete it," she said at a committee meeting.
[ Zika Spurs War of Words ]
Public health officials have warned that the Zika virus is likely to spread within the United States as mosquito populations grow in the summer months. Health researchers who joined Democrats for the news conference Wednesday said not enough resources are available to perform proper surveillance and diagnostic efforts, so the disease could already have begun to spread in low-income areas that face greater challenges in protecting against mosquitoes.
The experts also said that the administration's move earlier this year to repurpose nearly $600 million to combat the virus in the absence of congressional action has hurt other public health efforts that the money was meant to support.
Senate Democrats have insisted the $1.1 billion spending level is the bare minimum they would support.
"We wouldn't have supported it in the Senate if we wouldn't support it in the negotiations with the House," Klobuchar said.
The White House hasn't committed to either supporting or opposing the $1.1 billion Senate package, while it continues to insist on the full $1.9 billion request. But Obama would veto the House's "woefully inadequate" $622 million version, the administration said.
Topics: 2016 barack-obama congressional-affairs democrats health-care house policy republicans senate Amy Klobuchar Appropriations Barack Obama Barbara A Mikulski Barbara Mikulski Bill Nelson democrats Executive Branch Florida House Kentucky Maryland Minnesota Missouri Mitch McConnell Republicans Roy Blunt Senate Zika Virus APDM


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HomeDigital HealthDrones will begin delivering blood and medicine in the US
Drones will begin delivering blood and medicine in the US
July 16, 2017 Digital Health, Medical Drones, Startups
(The Verge) – A startup that uses drones to deliver medicine and blood to remote areas of Rwanda is launching a similar program in the US. California-based Zipline will bring its drone delivery program to rural and remote communities in Maryland, Nevada, and Washington, including some Native American reservations. Zipline will announce its expansion at a White House workshop on unpiloted aerial vehicles (UAVs) Tuesday morning.
Zipline launched in 2014, with support from venture capital firms such as Sequoia Partners and Google Ventures, as well as funding from Paul Allen, a Microsoft co-founder. The company began delivering medicine and blood in Rwanda last month under a government partnership, and expects to be operational in half of the country by the end of this month. The hope is that Zipline's fleet of drones will help deliver life-saving materials to remote areas of the US, as it has in Rwanda.
"When you look at rural or isolated communities, particularly Native American populations, populations that live on islands, you have serious health outcome inequalities," says Keller Rinaudo, Zipline's founder and CEO. "There's a linear relationship between how far away you live from a city and your expected lifespan. So our hope is that this type of technology can solve those kinds of inequalities."
While Rwanda has fully embraced drone technology as a way to spur economic growth, regulations in the US have been slower to take form. In June, the Federal Aviation Administration (FAA) finalized new rules that made it easier for commercial drone operators to receive flight authorization, though they still prevent companies from flying more than one mission at a time, and require that all UAVs remain within the line of sight of their operators.
Rinaudo says that after announcing its partnership with Rwanda in February, the White House reached out to Zipline and expressed interest in bringing its system to rural parts of the US. Zipline will apply for a waiver to the FAA regulations, and expects to begin operating within six months of receiving it. (Rinaudo hopes to be operational within a year from now.) For its US launch, the startup has partnered with three health care companies — Ellumen, ASD Healthcare, and Bloodworks Northwest — and has planned tentative deliveries to Smith Island, Maryland and San Juan Islands, Washington.
By Amar Toor | The Verge
Image Credit: Zipline International
Zipline International
Double-Booked: When Surgeons Operate On Two Patients At Once
Surgery from across the world
New Digital Health Innovations to Zimmer Biomet mymobility® Aim to Transform and Enhance Joint Replacement Standard of Care
June 22, 2020 Press Release
Zimmer Biomet Holdings, Inc. (NYSE and SIX: ZBH), a global leader in musculoskeletal healthcare, today announced new features of mymobility with Apple Watch, creating a first-of-its-kind remote care management system. […]
VRHealth Working with Oculus To Enhance Patient Healthcare
September 28, 2018 Press Release
VRHealth, the healthcare technology company providing specialized virtual reality (VR) technology solutions and data analysis, today announced that they are working with Oculus to deliver their newest health and wellness solutions using Oculus products. […]
The Future of Orthopaedic Surgery
September 14, 2018 Digital Health, Emerging Technology, Orthopedics
(BOA) – As the 21st century comes of age and the global burden of disease shifts increasingly towards musculoskeletal conditions, orthopaedic surgeons will be called upon to rise to the challenge. […]