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https://www.mysanantonio.com/news/local/traffic/article/7-6-million-project-expected-to-cut-down-on-11731459.php
$7.6 million project expected to cut down on far NW Side intersection traffic delays by 75 percent
JeriLynn Thorpe, San Antonio Express-News
Updated 6:47 am CDT, Friday, August 4, 2017
The new Displaced Left Turn interchange at Bandera and 1604 will involve left turn traffic shifts to the far left side of the road. "Displaced" left turns will occur at a new crossover signal prior to the frontage road intersection.
The new Displaced Left Turn interchange at Bandera and 1604 will involve left turn traffic shifts to the far left side of the road. "Displaced" left turns will occur at a new crossover signal prior to the
Photo: Photo: TxDOT
Commuters traveling from the far Northwest Side may soon be able to sleep in a little later. And many will soon pass through a first-of-its-kind in San Antonio intersection.
Construction on a "displaced left turn interchange" at Loop 1604 and Bandera Road is set to begin the first week in September and finish within two years.
First announced last October, the $7.6 million project could reduce delay by 75 percent through the intersection, according to the Texas Department of Transportation.
READ ALSO: Texas traffic rules you're probably not following
TxDOT believes that this new design could be the answer to traffic woes.
A DLT promotes continuous flow with left turn traffic shifting to the far left side of the road. Unlike the left turns at the present intersection, left turns will be "displaced" at a new crossover signal prior to the frontage road intersection.
As puzzling as the project may sounds, TxDOT said these intersections work great.
"They aren't confusing at all. If you're paying attention to the road, as you should be, they are extremely smooth. You can actually get where you're going pretty dang easy," Josh Donat, public information officer for TxDOT, told mySA.com.
RELATED: Worst San Antonio freeway on-ramps and off-ramps
This type of design will be the first of its kind in San Antonio, but are in place worldwide and as close as San Marcos.
The project comes after the intersection was ranked as the second-most dangerous in San Antonio in a study from Texas personal injury attorney Brian White, along with data visualization company 1point21 Interactive. Between 2012 and 2015, 266 crashes were reported at the intersection.
MORE: Report: These are the most dangerous intersections in San Antonio
Donat said that, as with any TxDOT construction project, staff will do their best to minimize traffic snarls. Closures can be expected during the weekend and over night.
jthorpe@express-news.net
@jerilynnthorpe


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Review: Nancy Beaudette, South Branch Road
Nancy Beaudette, South Branch Road
10 Apr, 2015 Alex Henderson
Although Nancy Beaudette is not a huge name in the folk-rock world, the Canadian singer/songwriter has been performing for many years. South Branch Road, in fact, is her eighth album, and this likable 2015 release shows her to have a good-natured, pastoral style that draws on direct or indirect influences such as Joni Mitchell (a fellow Canadian) and Janis Ian. One hears a lot of Mitchell influence in Beaudette's performances, although that influence comes through in her vocal style more than her lyrics. Mitchell's lyrics can be cryptic at times, whereas on "Shoot to Score (The Hockey Song)," "End of the Line," "Something Tells Me" or "Company of Stones," Beaudette favors lyrics that are very straight-forward and accessible. Beaudette, who grew up near the town of Cornwall in the Canadian province of Ontario, paints an appealing, earnest picture of small town life on tracks like "'Til the Tomatoes Ripen," "End of the Line" and the title song. She gives the impression that she is drawing on her own personal experiences, which makes the performances believable and convincing. Beaudette's musical strength obviously lies in the fact that she is a storyteller, and storytelling is what she does effectively on "'Til the Tomatoes Ripen," "Shoot to Score (The Hockey Song)," "Ride On" and other parts of this album.
South Branch Road has a very warm sound: Beaudette's vocals are warm, the melodies and harmonies are warm, the production and engineering are warm. Beaudette's earthy approach calls for an organic production style, and when "Starlight," "Can't Hold Back" or "You Got It Goin' On" is playing, one hears an album that is well-produced but not overproduced.
Although mainly a folk-rock album, there are times when South Branch Road detours a bit into country-rock territory: most notably, "Shoot to Score (The Hockey Song)" and "Starlight." Both of those songs would have worked on an album by Mary Chapin Carpenter or Tricia Yearwood, although the production lacks the slickness that one typically finds in Nashville country-rock these days. And that country-rock influence in what is primarily a folk-rock environment makes perfect sense in light of the relationship between country and North American folk. There are many differences between the folk scene and the modern country market: folk-rock singers (from Joan Baez to Bob Dylan to Natalie Merchant to Ani DiFranco to Tracey Chapman) have a long history of promoting liberal/progressive causes, while country has had its share of right-wing lyrics in recent decades. Yet folk-rock and country-rock, despite their musical and lyrical differences, have common roots (both were greatly influenced by the folk traditions that immigrants brought to North America from the British Isles), and they often intersect. Johnny Cash and Merle Haggard covers are not uncommon in folk venues; country-rockers will perform some Bob Dylan and Neil Young songs (often the less political ones). So when Beaudette incorporates some country-rock influence on parts of this album, it does not feel the least bit out of place.
Although Beaudette is the type of artist who is likely to be compared to Mitchell, Baez or Judy Collins, the intonation in her voice sometimes brings to mind someone whose name seldom appears in reviews of folk-rock albums: Heart's Ann Wilson. Given that Wilson has mostly made her mark in hard rock and arena rock, she is an unlikely comparison on an album like South Branch Road. But those who are familiar with Heart's 1970s albums such as Dreamboat Annie, Little Queen and Dog and Butterfly know that some of their early recordings had a definite folk-rock outlook (songs like "Soul of the Sea," "Dream of the Archer" and Dreamboat Annie's title track). And bearing that in mind, it makes sense that, directly or indirectly, Beaudette could be influenced by Wilson at the same time she is being influenced by Mitchell and Baez. Besides, this is modern folk-rock, not traditional folk from the 1940s. Singer/songwriters in today's folk scene were raised on rock & roll.
South Branch Road is an enjoyable listen, demonstrating that Beaudette is deserving of a wider audience.
Review by Alex Henderson
3.5 stars out of 5

redpajama_set_name: RedPajamaCommonCrawl


Full Medical Examinations for insurance, driving medicals etc. are by appointment-only.
These are not NHS Services therefore the individual will be charged a fee. Please ask at reception for further details.
For the first seven days of incapacity, a patient should complete a 'self-certificate', to provide evidence of medical incapacity. Our receptionists will be happy to provide you with one of these forms. For more information a poster is situated in our main reception.
The GPS can no longer sign passports.


text:
Rada Higgins McCreadie
place: Columbus, Ohio
B.A. in Mathematics from the Miami University (Florida) (1969). She earned her M.Sc. () Ohio State University
Ph.D. (1974) Ohio State University
thesis. A Category Incorporating Finite Galois Extensions and Regular Covering Spaces; advisor:
Research Assistant, Delft University (The Netherlands)
email: mccreadie@simplex.nl
another Rada Higgins McCreadie page
Rada Higgins received a good education in the Columbus public schools which thought so highly of her that she was allowed to participate in an NSF program to study mathematics at Ohio State in her 10, 11,and 12th grades. She did her undergraduate work at Sacramento State and Miami University while her mother taught at these institutions. After her Ph.D. from Ohio State University, her Ph.D. advisor at Ohio State called her one of the best students he ever had. She speaks on her professor. Her Research - Dr. Higgins has publications in Elemente der Mathematik, Canadian Mathematical Bulletin, and The Fibonacci Quarterly and is cited in The Encyclopedia of Mathematics, 1987.
Dr. Higgins says her favorite problem is one she solved some years ago, while not employed in my field: A proof of the generalized Pythagorean Equation on the basis of principles dating from the Egyptian papyri, dating from 1800 B.C. She is also an inventor of a parallel magnetic computer and a digital, sequential computer
For three years Dr. Higgins held an NSF Fellowship. From 1974 to 1976 she was a Visiting Assistant Professor at Ohio State. After a year (76-77) at Howard University she and her husband went to Delft University in The Netherlands, where Dr. McCreadie was a Research Assistant.
Dr. Higgins remains in Amsterdam in the Netherlands.
Early in her career, Rada Higgins McCready showed promise as a Research Mathematician:
Higgins, Rada More in the theory of sequences. Fibonacci Quart. 17 (1979), no. 3, 193--197.
Higgins, Rada On certain problems in the theory of sequences. Canad. Math. Bull. 18 (1975), no. 2, 229--231.
Higgins, Rada A note on a problem in the theory of sequences. Elem. Math. 29 (1974), 37--39.
references: [communications with Dr. Higgins], [Mathematical Reviews].
Dr. Higgins on her professor:
I remember how Professor Ross used to pace back and forth, from left to right, then from right to left, and again from left to right, like a panther in captivity, when he lectured. He immediately established a wave-length with his audience that held one's attention as perfectly as the Pied Piper. He was chivalrous, charming and courteous when he addressed his students. His motto was: (which he drummed into us; taken from a statement by Gauss) "Think deeply of simple things!" As a teenager, this motto and admonition became my vow. And even long afterwards, at every bend, cross-road, U-turn of my life, I remembered that motto. The motto seemed to imply that there is nothing so simple and apparent in life or mathematics, that it couldn't benefit from a deeper scrutiny or analysis. It implied you shouldn't look too superficially at things, at ideas or even at people. After all, everyone (and every concept) is a "star," (to put it in the vernacular of pop musician, Sly Stone).
I always suspected it was a very deep mind that impressed on me the motto: Think deeply of simple things! The opportunity to study under Dr. Ross and to participate in his summer training program was probably the most singular privilege I have known in my academic life. It was an unforgettable experience, involving unforgettable people. Like novices preparing for a vocation, we ate, slept, talked math. We meditated on the elegance of an ingenious proof or novelty of an audacious conjecture. I soon learn to love this austere, rigorous and vigorous environment dedicated to uncovering the laws, and beauty, of pure reason.
Certainly, Dr. Ross shaped my destiny. Through him, I received an NSF Fellowship to follow the graduate program in mathematics at Ohio State University, from where I eventually acquired a doctorate. I was an Assistant Professor of Mathematics at Howard University after leaving OSU. Unfortunately, my mathematical career faltered, but my interest and love for mathematics and "thinking deeply" has never diminished. I have done quite an amount of scientific research, which is, as yet, unexposed and undeveloped. I have survived the last twenty years principally by operating a one-man business, single-handedly, overseas.


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Australia flexes its 'democratic values' against Iran in next Anglo-American war crime
RBA, KPMG & Treasury are perpetrating a great fraud on the Australian people
Three weeks to stop the cash ban based on lies!
To resolve US-Iran war danger, an independent Australia would contribute diplomacy, not HMAS Toowoomba; urge emergency Trump-Putin-Xi summit
Last-minute cash ban hearing is another farce
Treasury's fraud exposed at cash ban hearing
Back to Media Releases
29 August 2019 - CEC Media Release
Scott Morrison's obsequious falling in behind the United States and United Kingdom in targeting Iran again confirms the late former Prime Minister Malcolm Fraser's assertion that Australia does not have an independent foreign policy.
At least elements of the media, unlike the Labor Party, are sceptical about this decision, as they should be, given that it is so clearly a crisis orchestrated by the Trump administration and British government, and yet another deadly Middle East regime-change fiasco in the making.
So why is Labor supporting it? Once again, ALP stands for Another Liberal Party—like with banking abuses, police-state laws now used to raid journalists, and mistreatment of refugees, Labor is desperate to be bipartisan on foreign policy, not just because it is scared of its own shadow, but because it is also subservient to the Anglo-American war machine. The only differences between Labor and the Liberals are in degree and tone, not in substance.
More lies
The government claims it is deploying the ADF to the Strait of Hormuz to "de-escalate" the situation, and to protect "freedom of navigation" from Iran, which has been seizing ships. As usual, their claims are premised on lies.
The current flash point in the Strait of Hormuz has its origins in US President Donald Trump's decision in 2018 to unilaterally withdraw from the nuclear agreement with Iran.
It escalated on 5 May when Trump's National Security Advisor John Bolton—one of the notorious neoconservative liars who orchestrated the 2003 invasion of Iraq—suddenly announced the deployment of the USS Abraham Lincoln carrier strike group and a bomber taskforce to the Gulf in response to an unspecified "number of troubling and escalatory indications and warnings".
Very significantly, on 14 May the top UK Commander in the region, Maj. Gen. Chris Ghika, publicly contradicted Bolton in a Pentagon briefing to state that there was no increased threat level from Iran. Just two days later, the UK government overruled Ghika and agreed there was an increased Iranian threat.
From that moment, the British escalated the situation, in coordination with the Washington neocons. On 19 May the UK announced the deployment of its waterborne SAS equivalent, the Special Boat Service, to "protect shipping". Only then did shipping incidents start to occur—indicating that either John Bolton and his British cronies are the prophets of our time, with greater insights than even local British commanders, or that they have orchestrated the incidents to provoke an escalation that can be the pretext for an invasion to achieve Bolton's longstanding goal of regime change in Iran.
The following shipping incidents have occurred after the deployment of US and British forces to the Persian Gulf:
In mid-June two oil tankers were attacked in the Gulf of Oman, which US Secretary of State and former CIA Director Mike Pompeo instantly blamed on Iran, based on "intelligence, the weapons used, the level of expertise", etc., which he claimed no other force present in the area had. Not true; the British SBS does.
On 4 July, away from the Persian Gulf, British Marines seized an Iranian oil tanker in the Strait of Gibraltar in the Mediterranean Sea, on its way to deliver oil to Syria. The British claimed to be enforcing EU sanctions against Syria, but aside from the fact that the USA and EU's sanctions on Syria are a crime against humanity in pursuit of another regime-change war crime based on lies, those sanctions didn't apply to Iran—it was purely a provocative act of piracy. (On 19 August Gibraltar let the ship go, over US objections.)
On 10 July, the British staged a provocation in the Gulf by having an empty oil tanker, the British Heritage, sail through the Strait of Hormuz without its transponder on and closely shadowed by British Navy Frigate the HMS Montrose. Sailing without a transponder is a danger to other shipping, and as Iran is responsible for shipping on its side of the Strait, an Iranian ship attempted to intercept the tanker before the Montrose bore down and warned it off.
On 19 July, another British ship, the Stena Impero, was detained by the Iranian Revolutionary Guard after also sailing with its transponder off and moving in the wrong traffic pattern. It must be suspected that this was the outcome the British hoped for: then-Foreign Secretary Jeremy Hunt loudly and shamelessly pontificated that "these seizures are completely unacceptable", insisting that "all ships can move safely and freely in the region" (but not Gibraltar apparently).
There are a number of other claims of Iran attacking or capturing ships in the Gulf which are either unproven, or must be seen in the context of the Anglo-American escalation.
Now, Australia is buying into the lying Anglo-American narrative, citing the freedom of navigation chestnut to justify our presence.
A comparison must be made to China and the South China Sea, where our Anglo-American allies use the freedom of navigation excuse to sail naval forces with enough firepower to blow up the world. The two countries that most depend on freedom of navigation in both the Persian Gulf and South China Sea are not the USA and UK, but China and Iran. Notwithstanding the current crippling US sanctions, Iran depends entirely on shipping through the Gulf to sell its oil. Iran's biggest customer is China, which depends on shipping through the Persian Gulf for half of its oil imports, which then must also be shipped through the South China Sea.
Bizarrely, Iran and China are being demonised as the risk to the shipping lanes they depend upon most, when in fact the real risk is Anglo-American provocations. This demonisation was taken to its extreme when Australian Liberal MP Andrew Hastie compared the rise of China to that of Nazi Germany, and called China a "challenge" to our "democratic values". Hastie made the comments in a 26 June speech to the neoconservative Henry Jackson Society in London, one of whose founders, Cambridge University professor Brendan Simms, trumpeted his Society's vision in a 2011 article praising the Libya intervention entitled, "Democracy can be dropped from 10,000 feet" i.e. "democratic values" can be bombed into countries. After destroying Iraq, Libya, and Syria, Hastie's neoconservative friends are now targeting Iran for a regime-change bloodbath, and fantasise about ultimately overthrowing China.
Australians must face the fact that Iran and China are not threatening the world, we are. It is our responsibility as citizens to demand our government withdraw from the Anglo-American regime-change agenda, assert a truly independent foreign policy, and support a new international economic order based on sovereign nation-states respecting each other's sovereignty, but cooperating on economic development that can lift the world out of poverty and ensure prosperity for future generations.
Click here for a free copy of the latest issue of the Australian Alert Service.


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AIOU Admission Fee For All Programs 2023
The top Allama Iqbal Open University will launch with AIOU Admission Fee For All Programs in 2023. which will be launched for students of the Matric Intermediate Bachelor, Master, and Matric courses. Spring and autumn students are able to apply online by the 21st of February 2023. Then, they can apply for admission into the various levels of this educational institution in Pakistan.
It is among the most prestigious institutions in Punjab. Punjab as well as the entire region of Asia with a huge number of students are accepted as well as continuing and new students. this page you can find the entire fee structure information of www.aiou.edu.pk 2023 admissions for this year.
People can prepare today and sign up the new girls and boys to pay their AIOU admission fee in 2023 and take the exam in various groups of general science, ARTS, computer science, and commerce without difficulty everyone can be a part of the brilliant University of Allama Iqbal at aiou.edu.pk
AIOU Admission Fee For All Programs Schedule
and verify the most up-to-date registration schedule for students and fees for the first, second, as well as third fee admissions 2023. www.aiou.edu.pk 2023 of this year's semester-wise for autumn and spring at all program levels on this page.
All children are eligible to be eligible to apply to FA, FSC, ICS, ICOM, DCOM and BA, BCOM, BSC, BCS and MA, MCOM, MSC, and M.phil online. You can also apply through the post office you can collect your complete documents, the result cards, and certificates of character and pick the areas of study.
In the event of the possibility of matriculation, inter, or graduate, then submit your credential documents and submit the documents to Islamabad the headquarters for the Allama Iqbal Open University including the AIOU application fee of 2023 fee as well as the last date for submission of the application is February 21st, 2023.
AIOU Admission Fee Schedule 2023 Latest
Program Fee Rate For
Ordinary Urgent Duplicate
Course Certificate of SSC/HSSC Bachelor program/Elementary Arabic/Non-Credit Rs. 400 Rs. 800 Rs. 1600
SSC(Matric)/HSSC (Intermediate)/PTC/CT/ATTC Rs. 500 Rs. 1000 Rs. 2000
BA/B.Com/BBA (old)/BLIS/BCS/Associate Degree (2 years)/Undergraduate Diploma Certificate Rs. 800 Rs. 1600 Rs. 3200
BS/BBA (4 years)/Associate Degree (4 years) etc. Rs. 1200 Rs. 2400 Rs. 4800
B.Ed. (old programme) Rs. 1000 Rs. 2000 Rs. 4000
B.Ed (1.5 years/2.5 years/4 years) Rs. 1200 Rs. 2400 Rs. 4800
MA/M.SC/M.Ed./MBA/M.Com/MBA & MPA Executive Rs. 1200 Rs. 2400 Rs. 4800
Postgraduate Diploma Certificate Rs. 1000 Rs. 2000 Rs. 4000
M Phil/MS/LLM/MSc (Honors) Rs. 2000 Rs. 4000 Rs. 8000
PhD Rs. 3000 Rs. 6000 Rs. 12000
Triplicate Rates of Admission
A fee for a Triplicate Certificate Degree from Matric to Bachelor Programme Rs. 5000
The fee for a Triplicate Degree of B.Ed BS (4 years) Master MS MPhil Programme Rs. 10,000
Change of Center/Rechecking/Result Car Fee Schedule 2023
Change of Examination Center Rs 600
Duplicate Result Card Per Semester (Beyond Two Current Semesters) Rs 100
Rechecking of per Answer Script ATTC/CT/PTC/B.Ed all Graduate Programme Rs 700
Rechecking of per Answer Script BS/MA/MSc PGD & equivalent Rs 800
Rechecking of per Answer Script MS/MPhil/Ph.D. & equivalent Rs 1000
Change of Name (Correction) Fee Charges 2023
Change in name or any other correction in Certificate/Degree (made by Board/University or Court decision) Double Fee of Ordinary Degree Prescribed for Programme
Degree Verification Fee Structure
Verification of Certificate Degree (By Students or Departments) By Post-Rs.600 By hand (same day)
– Rs 1000/
Verification of Certificate/Degree from Foreign Organizations/Oversees Countries USD 100*
*including USD 25 for Courier Charges
Re-Appearing in Exams Fee Schedule 2023
Re-Appear Exams Fee For Programme Fee Rate Per Course
SSC/PTC / Elementary Arabic Rs 100
ATTC Rs.180
HSSC/CT/Diploma 10+3 Rs. 200
Bachelor/Associate Degree (2 years) Rs 300
BS/BBA/Associate Degree (4 years) Rs.400
B.Ed (old)/B.Ed (1.5 Years/2.5 years/4 years) Rs 400
MA/MSc/MBA/M.Ed/PGD/MS/M.Phil Rs 500
PhD Rs.800
Download AIOU Fee Structure
Students can download the Aiou Admission Fee structure to follow programs by clicking to save the below picture
Allama Iqbal Open University is not only affordable but offers quality education through upgrading its infrastructure for communication and management, including admissions online lectures and workshops as well as studying patterns.Aiou Admission confirmation and Aiou Admissions for Spring.
It is regarded as one of the most convenient ways to earn an online degree in Pakistan. However, many students are confused when they are applying for admission or continuing education due to no guidance and information accessible online. A lot of students have asked us various questions about the AIOU fee structure and all details are given here.


14,000 North Dakotans are at risk of losing premium tax credits!
14,000 North Dakotans are at risk of losing premium tax credits – depending on the outcome of the US Supreme Court decision in King vs. Burwell, expected soon.
To read more on this, please click here.
To read more on Drew Altman's column in The Wall Street Journal, click here.
Could it be done? Eliminating hunger in a state? No other state is closer to this goal than North Dakota. Although our state claims one of the lowest rates of hunger and food insecurity in the nation, still 7.8 percent, or about 56,430 people in our state don't have enough, at times, food for a healthy, active life for all family members and don't have reliable access to nutritious and affordable food.
This September, the Creating a Hunger Free North Dakota Coalition will bring together people working to make a hunger-free state. The Creating Hunger-Free Communities Summit will be held September 17-18, 2015 at the Event Center in central Bismarck.
Speakers from national organizations including Feeding America and the AARP Foundation, regional organizations including the Minneapolis Branch of the Federal Reserve Bank and School Meals that Rock and North Dakota's own food and hunger experts will share ideas and experiences with those who attend. Music and visual displays will also be part of the conference experience. To take advantage of even more to do and see while in Bismarck, plan to stay on for the Downtowners' Street Fair taking place September 18-19.
Save the dates of September 17-18, 2015 now…and stay tuned for more details in the coming weeks.
Do you share the vision of a hunger-free North Dakota? Join us at the Creating Hunger-Free Communities Summit in Bismarck and return home with plans for what you can do to end hunger in your community!


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I'm kind of disappointed in myself that the last post on this here blog was my favorite films of August. But... well... September was just that kind of month for me.
Let's get on with it!
IT -- The most anticipated horror film of 2017. Hell, maybe it's the most anticipated horror film of the past decade, I'm not sure. All I know is expectations were high for this one. And for my part, the film largely met those expectations. It's a dark, weird, stylish, funny little movie about a killer clown that has to terrify kids before he can eat them.
The discussion about whether or not IT is a horror film confuses me to no end. You should be able to watch any random 10 minutes of IT and be convinced you're watching a horror film. But people are weird.
COLOSSAL -- Kaiju have previously represented nuclear weapons, pollution, war. Now... alcoholism and depression.
COLOSSAL is kind of amazing.
It may lay the 'messaging' on thick but it's also honest and tough. Fun, too. As a kaiju film fan and someone who's dealt with his own mental health issues, the film connected with me in some unexpected ways.
I really, really liked it.
THE BIG SICK -- A romantic comedy with heart. A Muslim stand-up comic falls for a girl that he knows his family wouldn't approve of. Shortly after their relationship ends, the girl gets sick and is placed in a medically induced coma, which brings our guy face-to-face with her family for the first time. It doesn't sound funny, but it's funny. And it's sad. And it's wonderful. I love the cast. Love the honesty and wit. Fantastic film.
NEW BATTLES WITHOUT HONOR AND HUMANITY 2: THE BOSS'S HEAD -- Following the brilliant Battles Without Honor and Humanity crime saga, director Kinji Fukasaku returned to create a trilogy of new films in the New Battles trilogy. I was a bit disappointed with the first New Battles film, and if writer Koji Takada's account of things is correct, so was Fukasaku. The first film of the trilogy is a kinda-sorta follow-up to the original series that also played like a confusing recycling project. New Battles Without Honor and Humanity 2: The Boss's Head avoids any of that confusion by telling a standalone story that feels, well, New. You can read my complete review of the film at City on Fire.
THE INVISIBLE MAN -- I'm taking part in Hoop-Tober, a horror-themed film challenge over at Letterboxd. It has me watching many horror films I skipped over. Recently it got me to check out the original Invisible Man with Claude Rains. This movie is sublime. Hilarious, too. What a wonderful madman Rains makes. I've only seen the movie once and I have more territory to cover, but I feel pretty good calling The Invisible Man one of Universal's best classic horror movies.


is it possible to open files from another partition ?
I am really not into X11, my knowledges about this are almost 0, but I noticed that when I start Xnview, I can browse my HD but only the "partition" with the system, not the one on which the OS is not installed.
Is there a way to open something from my other partition ?


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\section{Introduction}
\label{Intro}
\noindent
Pure Chern-Simons theory is topological in nature and has no propagating degrees of freedom. When coupled to matter, the Chern-Simons gauge field attaches magnetic fluxes to the interacting matter quanta that gives rise to interesting physical phenomena such as the Aharonov-Bohm effect \cite{Aharonov:1959fk}.  Chern-Simons theories coupled to matter are applicable in diverse physical systems from quantum Hall effect  \cite{10.1007/BFb0113369, XGW, Witten:2015aoa, Tong:2016kpv}  in condensed matter theory to quantum gravity in high energy physics \cite{Witten:1988hc}.

Non-abelian Chern-Simons theories coupled to matter in the fundamental representation of $U(N)$ or $SU(N)$ are exactly solvable in the \lq t Hooft large $N$ limit. The theories enjoy a strong-weak bosonization duality \cite{Giombi:2011kc,Aharony:2011jz,Maldacena:2011jn,Maldacena:2012sf,Aharony:2012nh} that has been rigorously tested in the planar limit over the past decade. A simple example of the duality is between a Chern-Simons theory coupled to a fundamental boson in the Wilson-Fisher limit and a Chern-Simons theory coupled to a fundamental fermion.  Under a mapping of the parameters in the large $N$ limit, the physical observables in one theory map to the other.

The evidence for the duality consists of several rigorous large $N$ computations such as thermal partition functions \cite{Aharony:2012ns,Yokoyama:2013pxa,Takimi:2013zca,Jain:2013py}, correlation functions \cite{Aharony:2011jz,Aharony:2012nh,GurAri:2012is,Bedhotiya:2015uga,Gur-Ari:2015pca,Geracie:2015drf,Turiaci:2018dht,Yacoby:2018yvy,Inbasekar:2019wdw}, and $S$-matrices \cite{Jain:2014nza,Dandekar:2014era,Inbasekar:2015tsa,Yokoyama:2016sbx} to name a few. Significant evidence has accumulated over the years that the duality holds true along RG flows \cite{Minwalla:2015sca,Aharony:2018pjn}. These RG flows relate the bosonization duality to dualities in supersymmetric Chern-Simons-Matter theories \cite{Jain:2012qi,Jain:2013gza,Aharony:2019mbc}. In this context, the bosonization duality generalizes the already well known dualities such as Giveon-Kutasov duality in supersymmetric Chern-Simons-Matter theories \cite{Benini:2011mf,Park:2013wta,Aharony:2013dha}. For other recent works in the field, we refer the reader to \cite{Choudhury:2018iwf,Dey:2018ykx,Dey:2019ihe,Gur-Ari:2016xff,Halder:2019foo} and in particular to the applications of the finite $N$ generalizations of the duality \cite{Radicevic:2015yla,Aharony:2015mjs,Seiberg:2016gmd,Karch:2016sxi,Hsin:2016blu,Cordova:2017kue,Metlitski_2017,Cordova:2018qvg}.

In addition to being testing grounds for the duality, amplitudes in Chern-Simons-Matter theories can be used to demonstrate anyonic effects in these theories. In particular, the $S$-matrices in these theories display non-trivial phenomena arising from the anyonic nature of matter. For instance, unitarity of the scattering amplitudes in these theories requires a modification of the rules of crossing symmetry \cite{Jain:2014nza,Inbasekar:2015tsa,Yokoyama:2016sbx}. Furthermore, amplitudes in supersymmetric Chern-Simons-Matter theories (especially with a high degree of supersymmetry) have unique properties. In \cite{Inbasekar:2015tsa}, exact $2\to2$ amplitudes were computed to all orders in the 't Hooft coupling for $\mathcal{N}=2$ supersymmetric Chern-Simons-Matter theory. These amplitudes enjoy remarkable symmetry properties, such as dual superconformal symmetry \cite{Inbasekar:2017sqp} and Yangian symmetry \cite{Yangian} exact to all loops. Furthermore, using recursion relations, arbitrary $n$-point tree level amplitudes have also been constructed \cite{Inbasekar:2017ieo}. These symmetry properties are perhaps a general feature of supersymmetric Chern-Simons-Matter theories with $\mathcal{N}\geq 2$ supersymmetry. It is for instance well known that in $\mathcal{N}=6$ supersymmetric Chern-Simons-Matter theory n-point amplitudes enjoy invariance under dual superconformal symmetry \cite{Gang:2010gy}.

Thus, it is interesting to study scattering amplitudes in supersymmetric Chern-Simons-Matter theories with higher supersymmetry. The technical route towards such computations is by using the superspace methodology. Since an explicit superspace formalism does not exist beyond $\mathcal{N} > 2$ superspace, one can formulate higher supersymmetric theories in $\mathcal{N}=1$ or $\mathcal{N}=2$ superspace. The technology for computing the dynamics via Dyson-Schwinger equations in $\mathcal{N}=1$ superspace is already well established \cite{Inbasekar:2015tsa}. In this work, we initiate a program to set up higher supersymmetric theories in $\mathcal{N}=1$ superspace, with a future goal to study scattering amplitudes in these theories.

The maximal supersymmetric extension of $U(N)$ Chern-Simons theory coupled to fundamental matter has $\mathcal{N} = 3$ supersymmetry \cite{Kao:1995gf, Kapustin:1999ha, Gaiotto:2007qi, Chang:2012kt}. Though action for the $\mathcal{N} = 3$ theory without a mass term is known and a general action exists in $\mathcal{N}=2$ superspace, the explicit form of the mass-deformed action and the supersymmetry transformations have not been written down in the literature. In this paper, we present the explicit form of the mass-deformed action for the $\mathcal{N} = 3$ supersymmetric Chern-Simons theory coupled to fundamental matter and write it in $\mathcal{N}=1$ superspace.  Our results fill in a gap in the existing literature. In a follow up paper \cite{InbasekarN3}, we explore the Dyson-Schwinger method for computation of exact $S$-matrices in the mass-deformed $\mathcal{N} = 3$ theory. Several computations, such as the ones described in the above paragraphs (\cite{Inbasekar:2017ieo,Inbasekar:2017sqp,Inbasekar:2019wdw}), should also be doable using the Lagrangian eq. \eqref{n3sup} derived in this paper.

The paper is organized as follows. In section \ref{mdn3} we study mass-deformations of the free $\mathcal{N} = 3$ Wess-Zumino model, which serves as a warm up exercise. The model exhibits two consistent mass-deformation terms, transforming as a singlet or a triplet under the $R$-symmetry group $SO(3)_R$. In section \ref{mainsec} we discuss the mass-deformed $\mathcal{N} = 3$ $U(N)$ Chern-Simons-Matter theory. For completeness, we first write down the action for the superconformal theory as well as the supersymmetry transformations which leave the action invariant, and then mass-deform the action. The theory admits a unique mass deformation term, transforming as a triplet under the $R$-symmetry group, in agreement with the argument in \cite{Cordova:2016xhm}. We then repackage the mass-deformed action in the language of $\mathcal{N} = 1$ superfields. We end with concluding comments in section \ref{discuss}. Appendix \ref{conventions} sets the notations and conventions we use. Appendices \ref{massdeform}-\ref{varn3l} provide additional supplementary material.
\vspace{-3mm}
\section{Mass-deformed $\mathcal{N} = 3$ Wess-Zumino Model}
\label{mdn3}
In this section,  as a warm up exercise, we discuss mass deformations consistent with supersymmetry in the free $\mathcal{N} = 3$ Wess-Zumino model. This section sets the notation for the rest of the discussion (for some details regarding the conventions we follow see appendix \ref{conventions}). In $2+1$ dimensions a theory with $\mathcal{N}$ supersymmetries has the $R$-symmetry group $SO(\mathcal{N})_R$ (the subscript $R$ denotes $R$-symmetry). Consequently, for the three dimensional theories of interest to us the $R$-symmetry group is $SO(3)_R$. The matter content of the $\mathcal{N} = 3$ Wess-Zumino model consists of bosonic and fermionic $SO(3)_R\sim SU(2)_R$ doublets $\phi_A, \psi_{\alpha A}$. Here $A, B,\ldots$ are $SU(2)_R$ indices and take the values $1,2$, and $\alpha, \beta$ denote spinor indices, also taking values $1,2$.  The $\mathcal{N}=3$ supercharge $Q_{AB\alpha}$ transforms as a vector under $SU(2)_R$, and is symmetric under the interchange of the $R$-symmetry indices. The action for the free mass-deformed theory is given by
\begin{equation}
\begin{split}
\label{actn3}
S_{WZ}^{{free}} = \int d^3x \,\Big[&-\partial^\mu \bar\phi^A \partial_\mu \phi_A - \bar\phi^A M_A^{~\,D} M_D^{~\,E} \phi_E \\
&+ \bar\psi^{\alpha A} i \partial_{\alpha}^{~\,\beta} \psi_{\beta A} + \bar\psi^{\alpha A} M_A^{~\,D} \psi_{\alpha D} \Big].
\end{split}
\end{equation}
For a three-vector $V_\mu$, we have the symmetric spinor representation
$V_{\alpha\beta} = V_\mu (\gamma^\mu)_{\alpha\beta}.$ The mass matrix $M_A^{~\,B}$ in the action eq.\ \eqref{actn3} is the most general mass deformation consistent with the symmetries of the theory. As it turns out, the free theory admits two consistent mass-deformations, $M_A^{~\,B} = m \delta_A^{~\,B}$ or $M_A^{~\,B} = m (\sigma_3)_A^{~\,B}$, with $(\sigma_i)_A^{~\,B}, i = 1,2, 3$ denoting the standard Pauli matrices, as we show below.

The most general supersymmetry transformations for the free $\mathcal{N} = 3$ Wess-Zumino model follow from Lorentz invariance and are given by
\begin{equation}
\begin{split}
\label{gensusy3}
&Q_{BC\alpha} \phi_A = \chi_1 \, \psi_{\alpha (B} \, \epsilon_{C)A} ,\\
&Q_{BC\alpha} \bar\phi^A = \tilde\chi_1 \, \bar\psi_{\alpha (B} \, \delta_{C)}^{~~A} ,\\
&Q_{BC\alpha} \psi_{\beta A} = \chi_2 \, \partial_{\alpha\beta} \phi_{(B} \, \epsilon_{C)A} + \chi_3 \, C_{\alpha\beta} \phi_{(B} M_{C)A} ,\\
&Q_{BC\alpha} \bar\psi^{\beta A} = \tilde\chi_2 \, \partial_{\alpha}^{~\,\beta} \bar\phi_{(B} \, \delta_{C)}^{~~A} + \tilde\chi_3 \, \delta_{\alpha}^{~\,\beta} \bar\phi_{(B} M_{C)}^{~~A},
\end{split}
\end{equation}
where $\chi_1, \chi_2$ etc. are undetermined coefficients, and parentheses on indices denote symmetrization. We now demonstrate two ways to mass deform the theory. Supersymmetric invariance of the action eq.\ \eqref{actn3} when acted upon by the the supercharges provides constraints on the unknown parameters in the supersymmetry transformations eq.\ \eqref{gensusy3}.

\subsection{Case 1: $M_A^{~\,B} = m \,\delta_A^{~\,B}$}
In the first case, we consider the mass deformation $M_A^{~\,B} = m\, \delta_A^{~\,B}$ in eqs.\ \eqref{actn3} and \eqref{gensusy3}. A priori, the coefficients $\chi_i, \tilde\chi_i$ in the supersymmetry transformations eq.\eqref{gensusy3} are arbitrary. To relate them, we take the complex conjugates of the first and third supersymmetry transformations in eq.\eqref{gensusy3}, and compare the results with the second and fourth transformations.\footnote{Complex conjugation raises the lower $R$-symmetry indices and vice versa. Thus, $(Q_{AB\alpha})^* = Q^{AB}_{\alpha}$ and $(\epsilon_{AB})^* = \epsilon^{AB}$. Also, for the scalar and spinor fields we have $(\phi_A)^* = \bar\phi^A$ and $(\psi_{\alpha A})^* = \bar\psi^A_\alpha$. See appendix \ref{conventions} for discussion.} This gives us the relations\footnote{The complex conjugate of the LHS of the third SUSY transformation in eq.\eqref{gensusy3} is $(Q_{BC\alpha} \psi_{\beta A})^* = \bar\psi^A_\beta \overleftarrow{Q}^{BC}_\alpha = -\, Q^{BC}_\alpha \bar\psi^A_\beta.$ The additional $-$ sign contribution is important.}
\begin{equation}
\label{ccrel}
\tilde\chi_1 = - \chi_1^*, \,\, \tilde\chi_2 = \chi_2^*, \,\, \tilde\chi_3 = - \chi_3^*.
\end{equation}

We next impose the condition that the action eq.\eqref{actn3} must be invariant under the supersymmetry transformations eq.\eqref{gensusy3},
\begin{equation}
\label{invcond1}
Q_{BC\alpha}\left( S^{free}_{WZ} \right)=0,
\end{equation}
up to surface terms. For the present case where $M_A^{~\,B} = m\, \delta_A^{~\,B}$, or equivalently, $M_{AB} = m \,\epsilon_{AB}$, we get (see appendix \ref{massdeform})
\begin{equation}
\begin{split}
\label{cond1}
&\tilde\chi_1 = -i \chi_2, ~\tilde\chi_2 = i \chi_1;\\
&\chi_2 = i\chi_3, ~\tilde\chi_2 = i \tilde\chi_3;\\
&\tilde\chi_1 = \chi_3, ~\tilde\chi_3 = \chi_1.
\end{split}
\end{equation}
Combining the relations above with the relations in eq.\eqref{ccrel}, we get
\begin{equation}
\begin{split}
\label{cond1c}
&\chi_1^{~*} =i \chi_2, ~\chi_2^{~*} = i \chi_1;\\
&\chi_2 = i\chi_3, ~\chi_2^{~*} = - i \chi_3^{~*};\\
&\chi_1^{~*} = - \chi_3, ~\chi_3^{~*} = - \chi_1.
\end{split}
\end{equation}
It is easy to see that these form a consistent set of relations amongst the unknown parameters $\chi_i$. It is thus clear that the mass matrix $M_A^{~\,B} = m\, \delta_A^{~\,B}$ is an allowed mass deformation. With this mass matrix, the action eq.\eqref{actn3} takes the form
\begin{equation}
\begin{split}
\label{actn3m}
S_{WZ}^{{free}} = \int d^3x\, \Big[&-\partial^\mu \bar\phi^A \partial_\mu \phi_A - m^2 \bar\phi^A \phi_A \\
&+ \bar\psi^{\alpha A} i \partial_{\alpha}^{~\,\beta} \psi_{\beta A} + m \, \bar\psi^{\alpha A} \psi_{\alpha A} \Big].
\end{split}
\end{equation}
Also, the supersymmetry transformations eq.\eqref{gensusy3} become
\begin{equation}
\begin{split}
\label{gsusy3}
&Q_{BC\alpha} \phi_A = \chi_1 \, \psi_{\alpha (B} \, \epsilon_{C)A} ,\\
&Q_{BC\alpha} \bar\phi^A = - \chi_1^{~*} \, \bar\psi_{\alpha (B} \, \delta_{C)}^{~~A} ,\\
&Q_{BC\alpha} \psi_{\beta A} = - \chi_1^{~*} \left[i \partial_{\alpha\beta}  +  m C_{\alpha\beta}\right]\phi_{(B} \, \epsilon_{C)A} ,\\
&Q_{BC\alpha} \bar\psi^{\beta A} = \chi_1 \big[ i \partial_{\alpha}^{~\,\beta}  + m \delta_{\alpha}^{~\,\beta}  \big]\bar\phi_{(B} \, \delta_{C)}^{~~A}.
\end{split}
\end{equation}
In eq.\eqref{gsusy3}, the parameter $\chi_1$ is still arbitrary.

\subsection{Case 2: $M_A^{~\,B} = m\, (\sigma_3)_A^{~\,B}$ }\label{triplet}
In the second case, we choose the mass deformation $M_A^{~\,B} = m \, (\sigma_3)_A^{~\,B}$. This chooses a specific direction in the $R$-symmetry space, and in fact breaks the $SU(2)_R$  symmetry to $U(1)_R$. Complex conjugation of the first and third supersymmetry transformations in eq.\ \eqref{gensusy3} with the choice $M_A^{~\,B} = m\, (\sigma_3)_A^{~\,B}$ followed by comparison with the second and fourth transformations gives the conditions
\begin{equation}
\label{ccrela}
\tilde\chi_1 = - \chi_1^*, \,\, \tilde\chi_2 = \chi_2^*, \,\, \tilde\chi_3 = \chi_3^*.
\end{equation}
Also, the supersymmetric invariance of the action eq.\eqref{invcond1} now gives (see appendix \ref{massdeform})
\begin{equation}
\begin{split}
\label{cond2}
&\tilde\chi_1 = -i \chi_2, ~\tilde\chi_2 = i \chi_1;\\
&\chi_2 = - i\chi_3, ~\tilde\chi_2 = i \tilde\chi_3;\\
&\tilde\chi_1 = - \chi_3, ~\tilde\chi_3 = \chi_1.
\end{split}
\end{equation}
Combining these with eq.\eqref{ccrela}, we get the constraints
\begin{equation}
\begin{split}
\label{cond2c}
&\chi_1^{~*} =i \chi_2, ~\chi_2^{~*} = i \chi_1;\\
&\chi_2 = - i\chi_3, ~\chi_2^{~*} = i \chi_3^{~*};\\
&\chi_1^{~*} = \chi_3, ~\chi_3^{~*} = \chi_1.
\end{split}
\end{equation}
As can be clearly seen, the relations in eq.\eqref{cond2c} are also mutually consistent, and hence the choice  $M_A^{~\,B} = m \, (\sigma_3)_A^{~\,B}$ is another possible mass deformation for the free theory. With this choice of the mass deformation term, the action eq.\eqref{actn3} takes the form
\begin{equation}
\begin{split}
\label{actn3m2}
S_{WZ}^{{free}} = \int &d^3x \, \Big[ -\partial^\mu \bar\phi^A \partial_\mu \phi_A - m^2 \bar\phi^A \phi_A \\
&+ \bar\psi^{\alpha A} i \partial_{\alpha}^{~\,\beta} \psi_{\beta A} + m \bar\psi^{\alpha A} (\sigma_3)_A^{~\,B} \psi_{\alpha B} \Big],
\end{split}
\end{equation}
and the associated supersymmetry transformations are
\begin{equation}
\begin{split}
\label{susy3m2}
&Q_{BC\alpha} \phi_A = \chi_1 \, \psi_{\alpha (B} \, \epsilon_{C)A} ,\\
&Q_{BC\alpha} \bar\phi^A = - \chi_1^* \, \bar\psi_{\alpha (B} \, \delta_{C)}^{~~A} ,\\
&Q_{BC\alpha} \psi_{\beta A} = - i \chi_1^* \, \partial_{\alpha\beta} \phi_{(B} \, \epsilon_{C)A} + m \chi_1^* \, C_{\alpha\beta} \phi_{(B} (\sigma_3)_{C)A} ,\\
&Q_{BC\alpha} \bar\psi^{\beta A} = i \chi_1 \, \partial_{\alpha}^{~\,\beta} \bar\phi_{(B} \, \delta_{C)}^{~~A} + m \chi_1 \, \delta_{\alpha}^{~\,\beta} \bar\phi_{(B} (\sigma_3)_{C)}^{~~A} .
\end{split}
\end{equation}
Here, $\chi_1$ is an arbitrary complex number. Note the explicit appearance of the $(\sigma}         \newcommand{\Si}{\Sigma_3)_{A}^{~\,B}$ in the fermion mass term that breaks the $SU(2)_R$ symmetry to $U(1)_R$. Thus the free $\mathcal{N} = 3$ Wess-Zumino model admits two possible consistent mass deformations.

\section{$\mathcal{N} = 3$ Chern-Simons theory coupled to fundamental matter}
\label{mainsec}
\subsection{The Massless Lorentzian Theory}
\label{lorcs3}
We now consider the Lorentzian $\mathcal{N} = 3$ Chern-Simons-Matter theory, with gauge group $U(N)$.  The action is available in $\mathcal{N}=2$ superspace in \cite{Gaiotto:2007qi}. For our purposes, we make use of the action manifestly written in $SU(2)_R$ notation (see eq. D.18 of \cite{Chang:2012kt}). The action for the $\mathcal{N}=3$ theory is given by
\begin{equation}
\begin{split}
\label{lo3cs}
&S_{CS} = \int d^3x \bigg[-\frac{\kappa}{4\pi} \epsilon^{\mu\nu\rho} \, \text{Tr}\bigg(A_\mu \partial_\nu A_\rho - \frac{2i}{3} A_\mu A_\nu A_\rho\bigg) \\
&\qquad\qquad\qquad\quad+ i \bar\psi^A \slashed{D} \psi_A - D^\mu \bar\phi_A D_\mu \phi^A \\
&- \frac{4\pi^2}{\kappa^2} (\bar\phi_A \phi^B) (\bar\phi_B \phi^C) (\bar\phi_C \phi^A) + \frac{4\pi}{\kappa} (\bar\phi_A \phi^B) (\bar\psi^A \psi_B) \\
&+ \frac{2\pi}{\kappa}(\bar\psi^A \phi_B) (\bar\phi^B \psi_A) -\frac{4\pi}{\kappa} (\bar\psi^A \phi_A)(\bar\phi^B \psi_B) \\
&+ \frac{2\pi}{\kappa} (\bar\psi^A \phi_A) (\bar\psi^B \phi_B) + \frac{2\pi}{\kappa} (\bar\phi^A \psi_A) (\bar\phi^B \psi_B) \bigg],
\end{split}
\end{equation}
where $D_\mu$ is the gauge covariant derivative. The last three lines in the above action contain the interaction terms for the theory. Note that parentheses surrounding two fields denote a contraction of the gauge indices. Once again, by imposing Lorentz invariance and simple dimensional analysis, one can write down the most general supersymmetry transformations for the theory. The invariance of the action when acted upon by the supercharges then fixes the form of the transformations uniquely.  The supersymmetry transformations turn out to be
\begin{equation}
\begin{split}
\label{sun3f}
&Q_{BC\alpha} \phi_A = \chi_1 \, \psi_{\alpha (B} \, \epsilon_{C)A} ,\\
&Q_{BC\alpha} \bar\phi^A = - \chi_1 \, \bar\psi_{\alpha (B} \, \delta_{C)}^{~~A} ,\\
&Q_{BC\alpha} \psi_{\beta A} = -i \chi_1 \, D_{\alpha\beta} \phi_{(B} \, \epsilon_{C)A} \\ &+\frac{2\pi}{\kappa}\chi_1 \, C_{\alpha\beta} (\bar\phi_A \phi_{(B}) \phi_{C)} +\frac{2\pi}{\kappa}\chi_1 \, C_{\alpha\beta} (\bar\phi_{(B} \phi_{C)}) \phi_{A},\\
&Q_{BC\alpha} \bar\psi^{\beta A} = i \chi_1 \, D_{\alpha}^{~\,\beta} \bar\phi_{(B} \, \delta_{C)}^{~~A} \\
&+\frac{2\pi}{\kappa}\chi_1 \, \delta_{\alpha}^{~\,\beta}(\bar\phi_{(B} \phi^{A}) \bar\phi_{C)} - \frac{2\pi}{\kappa}\chi_1 \, \delta_{\alpha}^{~\,\beta} (\bar\phi_{(B} \phi_{C)}) \bar\phi^{A},\\
&Q_{BC\alpha} A^a_\mu = - \,\frac{4\pi}{\kappa}\chi_1 (\gamma_\mu)_\alpha^{~\,\beta} \bar\phi^i_{(B} (T^a)_i^{~j} \psi_{C)\beta j} \\
&- \frac{4\pi}{\kappa}\chi_1 (\gamma_\mu)_\alpha^{~\,\beta} \bar\psi^i_{\beta (B} (T^a)_i^{~j} \phi_{C)j} ,
\end{split}
\end{equation}
where $\chi_1$ is an arbitrary real number. $(T^a)_i^{~\,j}$ are the generators of the gauge group $U(N)$, with $a,b, \cdots$ denoting the gauge indices. See appendix \ref{varn3l} for a derivation of the supersymmetry transformations eq.\ \eqref{sun3f}.

\subsection{The Mass-deformed Lorentzian Theory}
\label{mdeflt}
We now consider the mass-deformation of the superconformal $\mathcal{N} = 3$ Chern-Simons-Matter theory, with the action given by eq.\ \eqref{lo3cs}. As it turns out, unlike the free Wess-Zumino model, the interacting Chern-Simons theory admits a unique mass deformation term that should transform as a triplet\footnote{We thank Ken Intriligator for helpful communication.} under $SU(2)_R$ \cite{Cordova:2016xhm}. The most general mass deformation term would be of the form $m_0 \mathcal{O}$, where $\mathcal{O}$ is an operator of mass dimension 2. Following \S\ref{triplet}, we find that the most general mass-dependent terms that can be added to the action eq.\ \eqref{lo3cs} and still lead to closure  under supersymmetry transformations are given by
\begin{equation}
\begin{split}
\label{lo3csn}
S_{CS}^{\,mass} = \int d^3x \, \bigg[&- m_0^2 (\bar\phi^A \phi_A) + m_0 (\bar\psi^A (\sigma_3)_A^{~~B} \psi_B) \\
&+ \frac{4\pi m_0}{\kappa} (\bar\phi^A \phi_A)  (\bar\phi^C (\sigma_3)_C^{~~D} \phi_D) \bigg].
\end{split}
\end{equation}
The full mass-deformed action, eq.\ \eqref{lo3cs} with the added mass term eq.\ \eqref{lo3csn}, is invariant under the supersymmetry transformations given by
\begin{equation}
\begin{split}
\label{sun3fn}
&Q_{BC\alpha} \phi_A = \chi_1 \, \psi_{\alpha (B} \, \epsilon_{C)A} ,\\
&Q_{BC\alpha} \bar\phi^A = - \chi_1 \, \bar\psi_{\alpha (B} \, \delta_{C)}^{~~A} ,\\
&Q_{BC\alpha} \psi_{\beta A} = -i \chi_1 \, D_{\alpha\beta} \phi_{(B} \, \epsilon_{C)A} +\frac{2\pi}{\kappa}\chi_1 \, C_{\alpha\beta} (\bar\phi_A \phi_{(B}) \phi_{C)}\\ &+\frac{2\pi}{\kappa}\chi_1 \, C_{\alpha\beta} (\bar\phi_{(B} \phi_{C)}) \phi_{A} + m_0 \chi_1 C_{\alpha\beta} (\sigma_3)_{A(B} \phi_{C)}\, ,\\
&Q_{BC\alpha} \bar\psi^{\beta A} = i \chi_1 \, D_{\alpha}^{~\,\beta} \bar\phi_{(B} \, \delta_{C)}^{~~A} +\frac{2\pi}{\kappa}\chi_1 \, \delta_{\alpha}^{~\,\beta}(\bar\phi_{(B} \phi^{A}) \bar\phi_{C)} \\
&- \frac{2\pi}{\kappa}\chi_1 \, \delta_{\alpha}^{~\,\beta} (\bar\phi_{(B} \phi_{C)}) \bar\phi^{A} + m_0 \chi_1 \delta_\alpha^{~\,\beta} (\sigma_3)_{(B}^{~~\,A} \bar\phi_{C)} \, , \\
&Q_{BC\alpha} A^a_\mu = - \,\frac{4\pi}{\kappa}\chi_1 (\gamma_\mu)_\alpha^{~\,\beta} \bar\phi^i_{(B} (T^a)_i^{~j} \psi_{C)\beta j} \\
&- \frac{4\pi}{\kappa}\chi_1 (\gamma_\mu)_\alpha^{~\,\beta} \bar\psi^i_{\beta (B} (T^a)_i^{~j} \phi_{C)j} ,
\end{split}
\end{equation}
with $\chi_1$ being an arbitrary real number. The transformations in eq.\ \eqref{sun3fn} above are a generalization of the ones in eq.\ \eqref{sun3f}, with additional mass-dependent terms required for the invariance of the mass-deformed action.

\subsection{The Mass-deformed Action in $\mathcal{N} = 1$ Superspace}
\label{mdefsup}
In this section, we express the $\mathcal{N} = 3$ mass-deformed action in $\mathcal{N} = 1$ superspace.  We present the Euclidean action, since it is more useful for computations in $\mathcal{N}=1$ superspace \cite{InbasekarN3}. The Euclidean form is easily obtained from eqs.\ \eqref{lo3cs}, \eqref{lo3csn} by an analytic continuation given by
\begin{equation}
\begin{split}
\label{analle}
&t_L \rightarrow - i t_E \, , ~ A_0^L \rightarrow i A_2^E,\\
&\psi_L \rightarrow - i \psi_E\, , ~ \bar\psi_L \rightarrow  i \bar\psi_E.
\end{split}
\end{equation}
We pause here to note that one has to be careful with the Euclidean continuation involving spinors. We often
use the definition of the charge conjugation matrix to define
\begin{equation}
\bar{\psi}^\beta_L \equiv (\psi} \newcommand{\Ps}{\Psi^\dagger)^\alpha (\gamma}         \newcommand{\Ga}{\Gamma^0_L)_\alpha^{\ \beta} \equiv C^{\beta\alpha}\psi} \newcommand{\Ps}{\Psi^*_\alpha\ .
\end{equation}
From our choice of the Dirac matrices we see that
\begin{equation}
(\psi} \newcommand{\Ps}{\Psi_\alpha)_L=\begin{bmatrix}
              \psi} \newcommand{\Ps}{\Psi_1 \\
	      \psi} \newcommand{\Ps}{\Psi_2
             \end{bmatrix} \ , \
(\bar{\psi}^\alpha)_L=i \begin{bmatrix}
              \psi} \newcommand{\Ps}{\Psi_2^*  & -\psi} \newcommand{\Ps}{\Psi_1^*
             \end{bmatrix} \ .
\end{equation}
It is easy to check that this is consistent with the definition of $\bar{\psi}$ using the charge
conjugation matrix. However, the Euclidean continuation gives
\begin{equation}
\bar{\psi}^\beta_E \equiv (\psi} \newcommand{\Ps}{\Psi^\dagger)^\alpha (\gamma}         \newcommand{\Ga}{\Gamma^2_E)_\alpha^{\ \beta}= - \begin{bmatrix}
              \psi} \newcommand{\Ps}{\Psi_2^*  & -\psi} \newcommand{\Ps}{\Psi_1^*
             \end{bmatrix} \ ,
\end{equation}
and therefore the Euclidean continuation of $\bar{\psi}^\beta_L \equiv C^{\beta\alpha}(\psi} \newcommand{\Ps}{\Psi_{\alpha L})^*$ would give identical results provided we use $\psi} \newcommand{\Ps}{\Psi_L \to -i \psi} \newcommand{\Ps}{\Psi_E$, as in eq.\ \eqref{analle}. The mass-deformed Euclidean action turns out to be
\begin{equation}
\begin{split}
\label{eu3cs}
&S_{CS}^{\texttt{Euc}} = \int d^3x \, \bigg[\frac{i\kappa}{4\pi} \epsilon^{\mu\nu\rho} \, \text{Tr}\bigg(A_\mu \partial_\nu A_\rho - \frac{2i}{3} A_\mu A_\nu A_\rho\bigg) \\
&- i \bar\psi^A \slashed{D} \psi_A + D^\mu \bar\phi_A D_\mu \phi^A + \frac{4\pi^2}{\kappa^2} (\bar\phi_A \phi^B) (\bar\phi_B \phi^C) (\bar\phi_C \phi^A) \\
&- \frac{4\pi}{\kappa} (\bar\phi_A \phi^B) (\bar\psi^A \psi_B) - \frac{2\pi}{\kappa}(\bar\psi^A \phi_B) (\bar\phi^B \psi_A)\\
&+\frac{4\pi}{\kappa} (\bar\psi^A \phi_A)(\bar\phi^B \psi_B) + \frac{2\pi}{\kappa} (\bar\psi^A \phi_A) (\bar\psi^B \phi_B) \\
&+ \frac{2\pi}{\kappa} (\bar\phi^A \psi_A) (\bar\phi^B \psi_B) + m_0^2 (\bar\phi^A \phi_A) - m_0 (\bar\psi^A (\sigma_3)_A^{~~B} \psi_B) \\
&- \frac{4\pi m_0}{\kappa} (\bar\phi^A \phi_A)  (\bar\phi^C (\sigma_3)_C^{~~D} \phi_D) \bigg].
\end{split}
\end{equation}

Now, the $\mathcal{N}=3$ action in $\mathcal{N}=1$ superspace can be constructed from a pair of fundamental and anti-fundamental chiral multiplets $(\Phi^+_i,\bar{\Phi}^{-i})$ coupled to a $U(N)$ gauge superfield $\Ga_\alpha^a (T^a)_i^{\ j}$. We refer the reader to Appendix A of \cite{Inbasekar:2015tsa} for the notation we use for the $\mathcal{N}=1$ superspace. Since we intend to formulate the $\mathcal{N}=3$ theory in $\mathcal{N}=1$ superspace, only the $SO(2)_R$ subgroup of the full $SO(3)_R$ symmetry is manifest. Thus $\Phi^+$ and $\Ph^-$ transform under the two inequivalent one dimensional representations of the residual $SO(2)_R$ symmetry. It is convenient to assign the $SO(2)_R$ charges $(+\frac{1}{2},-\frac{1}{2})$ for the superfields $(\Ph^+_i,\Phi^-_i)$ respectively. It follows that the complex conjugate fields $(\bar{\Ph}^{+i},\bar{\Ph}^{-i})$ have $SO(2)_R$ charges $(-\frac{1}{2},+\frac{1}{2})$ respectively. \footnote{A general element of $SO(2)$ is represented by the rotation matrix
\begin{center}
$$
R(\alpha)=
\begin{pmatrix}
 \cos\alpha & -\sin\alpha\\
 \sin\alpha & \cos\alpha
\end{pmatrix}
\ \forall \ \alpha \in (-\pi, \pi].
$$
\end{center}
The ``standard irreps'' of $SO(2)$ are of the form
$$
D^{(n)}(\alpha) z_n = e^{-i\alpha n} z_n \ , \ n=0,\pm1,\pm2,\ldots
$$
Baring the trivial representation at $n=0$, for each integer $n$ there exist two inequivalent one dimensional irreps of $SO(2)$.} The $\mathcal{N} = 3$ action written in the language of $\mathcal{N} = 1$ superfields takes the form
\begin{widetext}
\begin{equation}
\begin{split}
\label{n3sup}
\mathcal{S}^{\texttt{Euc}}_{CS} = - \int d^3x \, d^2\theta \, \bigg[ &\frac{\kappa}{4\pi} \, \text{Tr}\bigg(- \frac{1}{4} D^\alpha \Gamma^\beta D_\beta \Gamma_\alpha +\frac{i}{6}\, D^\alpha \Gamma^\beta \{\Gamma_\alpha, \Gamma_\beta \} + \frac{1}{24} \{\Gamma^\alpha, \Gamma^\beta \} \{\Gamma_\alpha, \Gamma_\beta \}\bigg)\\
&-\frac{1}{2} \sum\limits_{M=+,-} \big(D^\alpha\bar\Phi^M + i \bar\Phi^M \Gamma^\alpha\big) \big(D_\alpha\Phi^M - i \Gamma_\alpha\Phi^M\big)  - m_0 \left[(\bar\Phi^+ \Phi^+) - (\bar\Phi^- \Phi^-)\right] \\
&- \frac{\pi}{\kappa} (\bar\Phi^+ \Phi^+) (\bar\Phi^+ \Phi^+) - \frac{\pi}{\kappa} (\bar\Phi^- \Phi^-) (\bar\Phi^- \Phi^-)+ \frac{4\pi}{\kappa} (\bar\Phi^+ \Phi^+) (\bar\Phi^- \Phi^-) + \frac{2\pi}{\kappa} (\bar\Phi^+ \Phi^-) (\bar\Phi^- \Phi^+)\bigg],
\end{split}
\end{equation}
\end{widetext}
where $\Gamma^\alpha$ is the $U(N)$ gauge superfield. Note that there is no
raising or lowering for the $SO(2)_R$ indices.

In the rest of the section, we use the standard superfield expansions and show that we recover the component action eq.\ \eqref{eu3cs} from eq.\ \eqref{n3sup}. The superfield expansions in the Wess-Zumino gauge are given by
\begin{equation}
\begin{split}
\label{comp1}
&\Phi^+ = \phi^+ + \theta \psi^+ - \theta^2 F^+ ,\\
&\Phi^- = \phi^- + \theta \psi^- - \theta^2 F^- ,\\
&\Gamma^\alpha =  i \theta^\beta A_\beta^{~\,\alpha} - 2 \theta^2 \lambda^\alpha.
\end{split}
\end{equation}
One needs to integrate out the auxiliary fields $F^{\pm}, \bar{F}^{\pm}$ and the gaugino $\lambda^\alpha$ by using their equations of motion. The equations of motion for $F^{\pm}$ are given by
\begin{equation}
\begin{split}
\label{feom}
&\bar{F}^+ = m_0 \bar\phi^+ - \frac{2\pi}{\kappa} (\bar\phi^+ \phi^-) \bar\phi^- - \frac{4\pi}{\kappa} (\bar\phi^- \phi^-) \bar\phi^+ \\
&\qquad+ \frac{2\pi}{\kappa} (\bar\phi^+ \phi^+) \bar\phi^+ ,\\
&\bar{F}^- = - m_0 \bar\phi^- - \frac{2\pi}{\kappa} (\bar\phi^- \phi^+) \bar\phi^+ - \frac{4\pi}{\kappa} (\bar\phi^+ \phi^+) \bar\phi^- \\
&\qquad+ \frac{2\pi}{\kappa} (\bar\phi^- \phi^-) \bar\phi^- .
\end{split}
\end{equation}
The gaugino equation of motion is
\begin{equation}
\begin{split}
\label{gaugeeom}
(\lambda_\alpha)_i^{~j} = \frac{2\pi}{\kappa} \Big[ &-i (\bar\phi^{+})^j (\psi^+_{\alpha})_i + i (\bar\psi^+_\alpha)^j (\phi^+)_i \\
&- i (\bar\phi^{-})^j (\psi^-_{\alpha})_i + i (\bar\psi^-_\alpha)^j (\phi^-)_i \Big].
\end{split}
\end{equation}
Eliminating the auxiliary fields gives us the component action
\begin{equation}
\begin{split}
\label{compons}
&\mathcal{S}^{\texttt{Euc}}_{CS} = \int d^3x \, \bigg[ \frac{i\kappa}{4\pi} \epsilon^{\mu\nu\rho} \, \text{Tr}\bigg( A_\mu \partial_\nu A_\rho - \frac{2i}{3} A_\mu A_\nu A_\rho\bigg) \\
&\quad+ D^\mu \bar\phi^+ D_\mu \phi^+ + D^\mu \bar\phi^- D_\mu \phi^- - i \bar\psi^+ \slashed{D} \psi^+ - i \bar\psi^- \slashed{D} \psi^-\\
&\quad+ m_0^{~2} \left(\bar\phi^+ \phi^+ + \bar\phi^- \phi^-\right) + m_0 \left(\bar\psi^+ \psi^+ - \bar\psi^- \psi^- \right) \\
&\quad+ \frac{4\pi m_0}{\kappa} \left( \bar\phi^+ \phi^+ + \bar\phi^- \phi^-\right) \left( \bar\phi^+ \phi^+ - \bar\phi^- \phi^-\right)\\
&+\frac{4\pi^2}{\kappa^2} \Big\{(\bar\phi^+ \phi^+) (\bar\phi^+ \phi^+) (\bar\phi^+ \phi^+) + (\bar\phi^- \phi^-) (\bar\phi^- \phi^-) (\bar\phi^- \phi^-) \\
&\quad+ 3 (\bar\phi^+ \phi^+) (\bar\phi^+ \phi^-) (\bar\phi^- \phi^+) + 3(\bar\phi^- \phi^-) (\bar\phi^+ \phi^-) (\bar\phi^- \phi^+)\Big\}\\
&+ \frac{2\pi}{\kappa} \Big\{ (\bar\phi^- \psi^-) (\bar\phi^- \psi^-) + (\bar\psi^- \phi^-) (\bar\psi^- \phi^-) + (\bar\phi^+ \psi^+) (\bar\phi^+ \psi^+) \\
&\quad+ (\bar\psi^+ \phi^+) (\bar\psi^+ \phi^+) -(\bar\phi^+ \psi^-) (\bar\psi^- \phi^+) -(\bar\psi^+ \phi^-) (\bar\phi^- \psi^+) \\
&\quad+ (\bar\phi^- \psi^-) (\bar\psi^- \phi^-) + (\bar\phi^+ \psi^+) (\bar\psi^+ \phi^+)\Big\}\\
&-\frac{4\pi}{\kappa} \Big\{ (\bar\phi^+ \psi^+) (\bar\phi^- \psi^-) + (\bar\phi^+ \psi^+) (\bar\psi^- \phi^-) +  (\bar\psi^+ \phi^+) (\bar\phi^- \psi^-) \\
&\quad+ (\bar\psi^+ \phi^+) (\bar\psi^- \phi^-) + (\bar\phi^+ \phi^+)(\bar\psi^- \psi^-) + (\bar\phi^- \phi^-)(\bar\psi^+ \psi^+) \\
&\quad+ (\bar\phi^+ \phi^-)(\bar\psi^- \psi^+) + (\bar\phi^- \phi^+)(\bar\psi^+ \psi^-) \Big\}\bigg].
\end{split}
\end{equation}
Identifying the $SU(2)_R$ doublets carefully as listed in \S \ref{N3con} we recover eq.\ \eqref{eu3cs}. Thus eq.\ \eqref{n3sup} is the correct representation of the mass-deformed $\mathcal{N} = 3$ Chern-Simons-Matter action in $\mathcal{N} = 1$ superspace.

\section{Concluding Comments}
\label{discuss}
In this paper, we presented the explicit form of the action and supersymmetry transformations for the mass-deformed $\mathcal{N} = 3$ supersymmetric $U(N)$ Chern-Simons theory coupled to fundamental matter. We also wrote down the mass-deformed action in  $\mathcal{N} = 1$ superspace, eq.\ \eqref{n3sup}. Our results fill a gap in the literature on Chern-Simons theories. We make use of the results presented in this paper in a follow up work \cite{InbasekarN3} to compute exact scattering amplitudes to all loop orders for the mass-deformed $\mathcal{N} = 3$ theory.

As was mentioned in the introduction \S\ref{Intro}, there are several interesting straightforward directions to pursue following this paper. Firstly, one could further test the bosonization duality in the $\mathcal{N}=3$ theory and compute correlation functions of spin-zero supercurrents following \cite{Inbasekar:2019wdw}, and beta functions to study RG flows and fixed points following \cite{Aharony:2019mbc}. The $2\to 2$ amplitudes computed in the $\mathcal{N}=3$ theory in \cite{InbasekarN3} are tree level exact, and we expect that the amplitudes would be invariant under dual superconformal symmetry and Yangian symmetry \cite{Inbasekar:2017sqp,Yangian}. Lastly, it should be possible to compute arbitrary $n$-point amplitudes via BCFW recursion relations following \cite{Inbasekar:2017ieo}. We hope to report on some of these directions in the future.

\acknowledgments
We would like to thank Sachin Jain, Shiraz Minwalla and V. Vishal for collaboration in the initial stages of this project. We would also like to thank Ken Intriligator, Sachin Jain, Shiraz Minwalla, Naveen Prabhakar, Tarun Sharma and V. Umesh for helpful discussions. The work of KI is supported in part by a Center of Excellence supported by the Israel Science Foundation (grant number 1989/14), the US-Israel bi-national fund (BSF) grant number 2012383, and the Germany Israel bi-national fund GIF grant number I-244-303.7-2013 at Tel Aviv University and BSF grant number 2014707 at Ben Gurion University. The work of LJ is supported in part by the Infosys Endowment for the Study of the Quantum Structure of Spacetime. The work of AS is supported by the NSERC of Canada.

redpajama_set_name: RedPajamaArXiv


Birthday parties, office get-togethers, Christmas, and more. There's no reason to look any further than Waterside Bistro for your private function or corporate event.
Inside, the Waterside Bistro's newly refurbished surroundings ooze warmth and an inviting atmosphere. Outside, the large riverside terrace is great for al fresco dining with both open and covered seating.
Our new private dining area is perfect for an exclusive function, birthday celebration, wedding party or corporate event.
Please call or email us to discuss your menu requirements and to find out more about the Waterside Bistro hosting your next event.
"Waterside Bistro hosted my birthday celebration on Saturday. I can't rate them highly enough – catering for 30 guests eating together. No one had to wait long to be served. Fabulous food served by attentive and amazing staff. We had nothing but compliments from our guests who had a wonderful evening.


text:
Q: Writing structured facts I've wrote some ruby code which will run on a linux server and return details about the server as a fact. It does this by connecting to amazon and retrieving some json (it runs two separate commands one to retrieve a list of disks - e.g /dev/sda1, /dev/xvdb and then it maps this to a volumeID via another query).
I've made some small amendments to the output and added some values I'm interested in. The code runs multiple times and returns multiple hashes (one for each disk - maybe I should merge them?). Anyway here's an example of a server which has two disks below (this is just some debug output):
Hash is {"/dev/sda1"=>{"disk_mapping"=>"", "is_lvm_partitioned"=>"false", "volumeid"=>"vol1234"}}.
Hash is {"/dev/xvdb1"=>{"disk_mapping"=>"xvdb1", "is_lvm_partitioned"=>"true", "volumeid"=>"vol5678"}}.

The next thing I want to to is turn this into a structured fact (with the devices: /dev/sda1, /dev/xvdb1 as the "keys"). Here's a rough idea of how I've done it (I've skipped a lot of the irrelevant code).
json_string = {
  "#{path}" => {
  "disk_mapping"       => "#{disk_mapping}",
  "is_lvm_partitioned" => "#{is_lvm_partitioned}",
  "volumeid"           => "#{getVolumes}"
  }
}.to_json
hash = JSON.parse(json_string)
if hash.is_a? Hash then
  debug_msg("Hash is #{hash}.")
  hash["#{path}"].each do |key, child|
    debug_msg("Setting key: #{key} child: #{child}.")
  end
end

I've never really wrote any ruby before so this is copied from multiple places, but besides aggregated facts I can't find a way to do this; I've tried to do something like this:
Facter.add(:test["#{path}"]["#{key}"]) do
  setcode do
    #{child}
  end
end

So I guess in order I want to know:

*

*Should I merge the hash somehow? I originally assumed I did but found this incredibly hard due to not knowing how many hash's I'd have.

*Should I be using an aggregated fact or a "standard" one?

*How do I retain the structure of the hash and then call it with a single query (e.g facts test).

*Any examples which are similar to my code (the puppet ones I've found quite hard to follow).

Here's what I'm looking for at the end:
[root@blah ~]# facter test
{
  /dev/sda1 => {
    disk_mapping => "",
    is_lvm_partitioned => "false",
    volumeid => "vol1234"
  },
  /dev/xvdb => {
    disk_mapping => "xvdb1",
    is_lvm_partitioned => "true",
    volumeid => "vol5678"
  }
}

Thanks.

A: I was way off...
hash_template = {}
hash = hash_template.merge!({
  "#{path}" => {
  "disk_mapping"       => "#{disk_mapping}",
  "is_lvm_partitioned" => "#{is_lvm_partitioned}",
  "volumeid"           => "#{getVolumes}"
  }
}
if hash.is_a? Hash then
  Facter.add(:test) do
    setcode do
      begin
        "#{hash}"
      rescue
        nil
      end
    end
  end
end

This can only be retrieved/viewed by calling it (within as puppet manifest):
if $test {
  notify { "Test fact is set as $test": }
}

redpajama_set_name: RedPajamaStackExchange


text:
package com.aspose.cells.model;

public class ValidationsResponse {
  private Validations Validations = null;
  private String Code = null;
  private String Status = null;
  /**
	 * getValidations
	 * Gets Validations
	 * @return Validations
	 */
  public Validations getValidations() {
    return Validations;
  }

	/**
	 * setValidations
	 * Sets Validations
	 * @param Validations Validations
	 */
  public void setValidations(Validations Validations) {
    this.Validations = Validations;
  }

  /**
	 * getCode
	 * Gets String
	 * @return Code
	 */
  public String getCode() {
    return Code;
  }

	/**
	 * setCode
	 * Sets String
	 * @param Code String
	 */
  public void setCode(String Code) {
    this.Code = Code;
  }

  /**
	 * getStatus
	 * Gets String
	 * @return Status
	 */
  public String getStatus() {
    return Status;
  }

	/**
	 * setStatus
	 * Sets String
	 * @param Status String
	 */
  public void setStatus(String Status) {
    this.Status = Status;
  }

  @Override
  public String toString()  {
    StringBuilder sb = new StringBuilder();
    sb.append("class ValidationsResponse {\n");
    sb.append("  Validations: ").append(Validations).append("\n");
    sb.append("  Code: ").append(Code).append("\n");
    sb.append("  Status: ").append(Status).append("\n");
    sb.append("}\n");
    return sb.toString();
  }
}

redpajama_set_name: RedPajamaGithub


Dentists use laughing gases to be able to make fun in dental therapy. For instance, a pediatric dentist is the finest professional to look after your children's teeth and gums. Locating a great pediatric dentist in Bolingbrook, IL, to look after your children's teeth and gums throughout their childhood and teenage years is something which you take seriously.
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The pediatric dentist has the capacity to offer advice and dietary counseling for kids and parents. A fantastic way to discover a suitable pediatric dentist is to deal with it like you're selecting an employee. When selecting the correct pediatric dentist it's crucial to be thorough.
By this time, your little one needs to be in a position to brush their own teeth independently. He or she'll observe a bright, vibrant space with many amenities designed especially for him or her. Additionally, if he or she consumes lots of sugary foods such as candy, cookies, raisins, and many sweetened fruit juices, then there is a high risk of developing cavities. Kids run about and play a good deal. If your kid is highly anxious about their dental therapy, we can provide general anesthesia in a hospital to produce their treatment more comfortable.
A youngster's oral health is a significant part their overall wellness and their pediatric dentist is a significant part of your youngster's health team. Ideally, the person that you select will have the ability to deal with your child for a very long time to come, and making the correct choice the very first time will conserve a great deal of wasted time and money. During the milk teeth phase, it's essential to keep oral care in the maximum consideration. It is very important to deal with your children's oral health. It's mandatory to opt to a remedy just after you've examined your wart cautiously and you've determined its principal characteristics. Benefits of the Treatment The treatment is applied to enhance the status of the brain.
It's possible to go over with your dentist if it's imperative to put dental sealants on the molar teeth of your son or daughter. You've located the best kids dentist. Choosing best children dentist is a significant part of their general welfare. A reasonably priced dentist for children in PA isn't hard to find whenever you've got a school system that aids children to learn oral health for a part of the health program. Pediatric dentistry is a specialty a dentist can opt to specialize in after becoming a certified dentist. When you're looking for a pediatric dentistry for the very first time there are a few things that you ought to search for before you make your pick.
While a professional dentist is professional and patient, pediatric dentists would like to get that excess training to take care of the varying needs of a developing child. Moreover, pediatric dentists might indicate a fluoride supplement to protect tooth enamel particularly in case the kid lives in a region where fluoride isn't routinely added to community water. If you wish to discover the finest pediatric dentist for your kids' needs, utilize the above-mentioned recommendations to make your search fast and uncomplicated.
You may ask your dentist to direct your son or daughter on proper technique of flossing. The chief reason it is very crucial to uncovering a dentist that satisfies your children's needs is that he'll be taking care of these for a substantial lengthy moment. The dentist will help make certain that a kid's baby teeth are appropriately cared for. One other important thing to bear in mind when picking a pediatric dentist is their location if you live in Bolingbrook, IL.
Laser dentistry is an incredible way to supply hard and soft tissue therapy, which makes it incredibly simple to supply quality dental hygiene in a significantly milder, efficacious and atraumatic way. It is the application of laser for dental hygiene. To begin with, folks undergo cosmetic dentistry for various explanations. Today's dental hygiene has become introduced into a wholly different level of narrative. There's an assortment of dentists who likewise provide completely free consultation.
Previous Post: Dental Veneers for a Beautiful Smile!


text:
Techniques and Methods 3–A23
>> Pubs Warehouse > TM 3–A23
Computing Discharge Using the Index Velocity Method
By Victor A. Levesque and Kevin A. Oberg
Application of the index velocity method for computing continuous records of discharge has become increasingly common, especially since the introduction of low-cost acoustic Doppler velocity meters (ADVMs) in 1997. Presently (2011), the index velocity method is being used to compute discharge records for approximately 470 gaging stations operated and maintained by the U.S. Geological Survey. The purpose of this report is to document and describe techniques for computing discharge records using the index velocity method.
Computing discharge using the index velocity method differs from the traditional stage-discharge method by separating velocity and area into two ratings—the index velocity rating and the stage-area rating. The outputs from each of these ratings, mean channel velocity (V) and cross-sectional area (A), are then multiplied together to compute a discharge. For the index velocity method, V is a function of such parameters as streamwise velocity, stage, cross-stream velocity, and velocity head, and A is a function of stage and cross-section shape. The index velocity method can be used at locations where stage-discharge methods are used, but it is especially appropriate when more than one specific discharge can be measured for a specific stage.
After the ADVM is selected, installed, and configured, the stage-area rating and the index velocity rating must be developed. A standard cross section is identified and surveyed in order to develop the stage-area rating. The standard cross section should be surveyed every year for the first 3 years of operation and thereafter at a lesser frequency, depending on the susceptibility of the cross section to change. Periodic measurements of discharge are used to calibrate and validate the index rating for the range of conditions experienced at the gaging station. Data from discharge measurements, ADVMs, and stage sensors are compiled for index-rating analysis. Index ratings are developed by means of regression techniques in which the mean cross-sectional velocity for the standard section is related to the measured index velocity. Most ratings are simple-linear regressions, but more complex ratings may be necessary in some cases. Once the rating is established, validation measurements should be made periodically. Over time, validation measurements may provide additional definition to the rating or result in the creation of a new rating.
The computation of discharge is the last step in the index velocity method, and in some ways it is the most straight-forward step. This step differs little from the steps used to compute discharge records for stage-discharge gaging stations. The ratings are entered into database software used for records computation, and continuous records of discharge are computed.
First posted April 12, 2012
Report and Appendixes PDF
(high resolution, 19.6 MB)
(low resolution 7.60 MB)
Appendixes (Zip File - 9.55 MB)
Kevin A. Oberg
National Hydroacoustics Coordinator
Office of Surface Water
1201 West University Avenue, Suite 100
Part or all of this report is presented in Portable Document Format (PDF); the latest version of Adobe Reader or similar software is required to view it. Download the latest version of Adobe Reader, free of charge.
Levesque, V.A., and Oberg, K.A., 2012, Computing discharge using the index velocity method: U.S. Geological Survey Techniques and Methods 3–A23, 148 p. (Also available at https://pubs.usgs.gov/tm/3a23/.)
Introduction to the Index Velocity Method
Site and Instrument Selection
ADVM Installation and Configuration
Routine Field Techniques
Routine Office Techniques
Rating Development and Analysis
Discharge Measurement Calibration Data
Index Velocity Rating
Computation and Analysis of Discharge
Summary and Conclusions
Appendix 1. Mounts for Acoustic Doppler Velocity Meters
Appendix 2. Forms and Quick-Reference Guides
Appendix 3. Analysis of Data for Selection of Measurement Volume
Appendix 4. Quality Control of Index Velocity Data for SonTek™/YSI Argonauts™
Appendix 5. Evaluating Changes in Stage-Area Ratings
Appendix 6. Implementing the Stage-Area and Index Ratings in National Water Informaiton System (NWIS) Automated Data Processing System (ADAPS) version 4.10
Appendix 7. Index Velocity Rating Shifts
Appendix 8. Example of an Index Velocity Station Analysis
URL: https://pubs.usgs.gov/tm/3a23/
Page Last Modified: Friday, December 02, 2016, 03:50:24 PM


text:
Seznam slovenskih trance glasbenikov.

B
 Andy Blueman

E
 Mark Elgan
 Elyksir

P
 Phoenixstar

R
 Reconceal
 Timson

Trance glasbeniki

redpajama_set_name: RedPajamaWikipedia


text:
HomeDigital UHDVudu 4k now features over 30 Dolby Vision / Atmos titles
Digital UHDNewsStreamingVUDU
Vudu 4k now features over 30 Dolby Vision / Atmos titles
Vudu has been a bit of a pioneer when it comes to digital movie distribution, first offering 4k UHD movies with Dolby Vision and Dolby Atmos almost two years ago. The dual combo allows for greater color depth (via HDR) and multichannel immersive surround sound that comes even from above!
Now, Vudu has over 30 titles with the Dolby combo (we counted 35) among their over 100 Digital UHD titles available. Some of the new Dolby-injected movies really stand out from the crowd, including Kong: Skull Island, Guardians of the Galaxy Vol. 2, Fantastic Beasts and Where to Find Them, and Ghost in the Shell (2017), to name a few.
Most of the Digital 4k titles from Vudu cost $29.99 each (this is common among other 4k providers), with the exception of GOTG Vol. 2 that is $5 cheaper than most new movies.
However, not every 4k TV or device will play back the Dolby combo. Be sure to check for compatibility before spending $30 bucks.
Dolby Vision through Vudu is limited to certain LG and Vizio 4k HDR TVs as well as Google's Chromecast Ultra media player. Here's a list of TV devices compatible with Vudu's UHD format with and without Dolby Vision/HDR. Your sound system must also be compatible to support Dolby Atmos to get the full channel surround sound.
Vudu Digital UHD (4k) Titles with Dolby Vision / Dolby Atmos
Into the Storm
Live Die Repeat: Edge of Tomorrow
The Legend of Tarzan
The Magnificent Seven (2016)
xXx: The Return of Xander Cage
Learn more: What is Dolby Vision? What is Dolby Atmos?
Digital UHD
Previous article'Ghost in the Shell' Review: Looks & Sounds Great, But…
Next articleNew on Blu-ray: Alien: Covenant, Blacklist S4, The Case for Christ, & more


text:
10 treasures of Kangaroo Island
Kangaroo Island is known as one of South Australia's must-visit locations. Here's what to do while you're there.
Kangaroo Island has a well-earned reputation as an amazing spot to visit, but with so much to do, it's hard to know where to start.
Here are some tips for a great stay to help you make the most of the island's unique scenery, wildlife and heritage.
1. KI Wilderness Trail
This five-day, 61km trail is one of Australia's great walks, and you should definitely try it for yourself. Beginning at the Flinders Chase Visitor Centre and ending at Kelly Hill Caves, it weaves its way through the most botanically unique area in all of South Australia, offering spectacular coastline views over the Southern Ocean. There are four campsites to break your journey along the way, but if you prefer something more luxurious, tour operators offer a number of options that include overnight stays in lodges.
2. Seal Bay
Seal Bay is the only place in the world where you can walk on the beach with the endangered Australian sea lion. The area is home to a breeding colony of about 800 sea lions, and if you time your visit well, you can expect to see lots of adorable pups. You can choose from a guided tour on the beach, or a self-guided tour on the boardwalk.
3. Kelly Hill Caves
Set in the natural bush setting of Kelly Hill Caves Conservation Park, these caves are full of amazing limestone formations built up over millions of years. Guests can wander the Show Cave, marvelling at the shapes and colours of the stalactites and stalagmites, or join an adventure caving tour with an experienced guide to see the other hidden chambers.
4. Admiral's Arch
Admiral's Arch is an intriguing rock formation on the south-western tip of Flinders Chase National Park, at Cape de Couedic (pronounced 'coo-dee'). A colony of long-nosed fur seals lives nearby the amazing limestone arch, and you can see them lounging and playing on the rocks and in the water.
5. Remarkable Rocks
Are you sensing a rock theme yet? Also located in Flinders Chase National Park, Remarkable Rocks is Kangaroo Island's best-known landmark. The 500-million-year-old granite boulders have been sculpted over the ages by wind and water, leaving behind stunning shapes covered in orange lichen.
6. Sponge Gardens Sanctuary Zone
SA has a network of 19 marine parks, including Encounter Marine Park, which takes in the eastern end of Kangaroo Island and spreads out to the mainland from Port Noarlunga to the Coorong. The Sponge Gardens Sanctuary Zone is one of 10 sanctuary zones in the park, and it's a fantastic place to dive, providing habitat for iconic species such as blue groper, harlequin fish and southern blue devil, as well as large sponges.
7. Wildlife
Home to hundreds of native species, including more than 270 species of birds, Kangaroo Island has been called Australia's Galapagos. It is free from many pest plants and animals, providing a refuge for threatened and endangered species that makes it the perfect destination for wildlife-watchers. Keen-eyed visitors will spot Rosenberg's goannas, echidnas, tammar wallabies, glossy black cockatoos, white-bellied sea-eagles, and even some of the thriving population of duck-billed platypuses.
Hot tip: If you want to have the best chance of seeing a platypus, try the well-named Platypus Waterholes in Flinders Chase at dawn or dusk.
8. Maritime heritage
The waters around Kangaroo Island are famously treacherous and have claimed at least 80 ships and many lives since European settlement in 1836. The Kangaroo Island Shipwreck Trail includes seven wrecks including some that are excellent dive sites, such as Portland Maru, Fides, Osmanli and Loch Venachar.
9. The lighthouses
Lighthouses helped reduce the number of ships lost off its coast, and are now an important aspect of the island's maritime safety and heritage. The island is home to historic light stations at Cape Borda, Cape du Couedic and Cape Willoughby. Cape Borda and Cape Willoughby both have a visitor centre and a museum, and lighthouse tours are available there and at Cape Borda. But the best news? You can stay in the heritage-listed lightkeepers' cottages.
10. Antechamber Bay
There is no shortage of amazing beaches on Kangaroo Island, but the long sandy beach at Antechamber Bay in Lashmar Conservation Park is a real stand-out. Lashmar is an ideal location for swimming, fishing and birdwatching and is just a short drive from Cape Willoughby light station. Explore the park further by canoeing along the tranquil Chapman River which flows through the park and into the sea at Antechamber Bay. A scenic picnic area and campground are also available in the park.
Feeling inspired to get to Kangaroo Island? Check out our blogs aboutthings to do in Flinders ChaseandSeal Bay's sea lions and pupsto get more of a taste of this amazing destination.
Main image: Antechamber Bay


text:
Die nach dem preußischen Offizier und General im amerikanischen Unabhängigkeitskrieg Friedrich Wilhelm von Steuben benannte Steubenstraße in der Weimarer Westvorstadt zwischen dem Wielandplatz, von dem die Humboldtstraße abgeht, führt repräsentativ alleeartig zum August-Frölich-Platz an die Herz-Jesu-Kirche und wurde 1838 als "schönste Straße der Residenz" bezeichnet. Die Steubenstraße hieß in wilhelminischer Zeit Kaiserin-Augusta-Straße. Wichtige Straßen, die auf die Steubenstraße treffen bzw. sie durchqueren, sind die Hegelstraße und die Gropiusstraße.

Die Steubenstraße steht zumindest zu Teilen auf der Liste der Kulturdenkmale in Weimar (Sachgesamtheiten und Ensembles). Außerdem stehen einige Objekte auf der Liste der Kulturdenkmale in Weimar (Einzeldenkmale) wie u. a. der Froschbrunnen von Arno Zauche bzw. der Fabeltierbrunnen am ehemaligen Bankgebäude Steubenstraße 15. Der Entwurf entstand im Leipziger Architektenbüro Weichardt & Eelbo nach 1925. Auch ist die ehemals Deinhardt'sche Brauerei zu nennen, ein Backsteinbau um 1880, die Teil der Weimarer Universitätsbibliothek der Bauhaus-Universität Weimar geworden ist. Auch ist die von Heinrich Heß (Baurat) 1832 errichtete Stadtbücherei, vormals Meßhaus zu nennen. Heß errichtete mehrere Bauten, die aber die Luftangriffe auf Weimar nicht überstanden hatten. Deren Entstehung war so allerdings nicht von Clemens Wenzeslaus Coudray so vorgesehen worden, sondern kam letztlich durch Betreiben von Großherzog Carl August von Sachsen-Weimar-Eisenach (1757–1828) zustande. Im Eckhaus Nr. 32 aus dem Jahre 1880 wohnte 1919–1925 einer Gedenktafel zufolge Walter Gropius. Die Gropiusstraße stößt auf die Steubenstraße. In dem Haus mit der Gaststätte "Alt-Weimar" in der Prellerstraße wohnte zeitweilig der Philosoph Rudolf Steiner. Eine Gedenktafel erinnert daran. Außer den genannten Gebäuden sind klassizistische als auch Jugendstilbauten vorzufinden.

In der Steubenstraße 39 hat das Weimarer Uhrenwerk seinen Sitz.
Der Komponist  Gustav  Lewin wohnte  in der Steubenstraße  19, woran ein Stolperstein erinnert.

Weblinks

 https://zeitsprung.weimar.jetzt/104/

Einzelnachweise

Steubenstrasse
Friedrich Wilhelm von Steuben als Namensgeber
Straße in Europa


text:
Q: While using Table Type data type in PL/SQL getting 'NO DATA FOUND' error Here defining a table type variable and trying to insert rows into that variable using for loop but unable to insert data . Getting data not found error... Please let me know whats wrong with this cod.
    DECLARE
TYPE T_EMP
IS
  TABLE OF EMP%ROWTYPE INDEX BY BINARY_INTEGER;
  V_EMP T_EMP ;
  V_MIN_EMP EMP.EMPNO%TYPE;
  V_MAX_EMP EMP.EMPNO%TYPE;
BEGIN
  --V_MIN_EMP:=7369;
  --V_MAX_EMP:=7934;
  SELECT MIN(empno) into V_MIN_EMP FROM EMP;
  SELECT MAX(EMPNO) INTO V_MAX_EMP FROM EMP;

  FOR I IN V_MIN_EMP..V_MAX_EMP
  LOOP
    SELECT * INTO V_EMP(I) FROM EMP WHERE EMPNO=I;
  END LOOP;
END;

A: In your code i is an index.  It steps through the bounds monotonically.  So if your minimum EMPNO is 1234 and your maximum EMPNO is 5678 the values of i will be 1234, 1235, 1236 ... 5676, 5677, 5678.
But that probably is what you want to do, because EMPNO is likely to be a sparse array, with missing numbers.  So if you have no row in EMP where EMPNO=1235 your query will throw NO_DATA_FOUND.
What's the solution?  Use a bulk collect instead:
select *
bulk collect into v_emp
from emp ;

That will select all the rows in the table, and it will be more efficient as well.


George is "Mr. Nature Photographer" and needs no further introduction. His morning presentation is entitled "George Lepp's Innovative Approaches to Photographing Birds" and his afternoon presentation will be "From Snowflakes to Gigascapes: Maximizing the Creative Power of Today's DSLRs." Treat yourself to George's website at www.georgelepp.com. Also, bring your DSLR camera bodies for sensor cleanings at a bargain price by Advance Camera.
As in past meetings, there will be a digital projected image competition and a print competition. The three categories for the competitions are scenic, wildlife, and plant life. Any man-made object in the entry should not be a major or significant portion of the image. Other details of the guidelines for the competitions and the procedure for image submission can be found at www.nppnw.org.
There is no admission charge for this event for Lewis & Clark faculty, staff and students.
Additional information may be found at www.nppnw.org.


text:
Title: Studies on the toxicity of cadmium
Author: Bonner, Frank W.
Awarding Body: University of Surrey
Current Institution: University of Surrey
http://epubs.surrey.ac.uk/848476/
The effects of acute parenteral, repeated parenteral and dietary administration of cadmium chloride have been investigated in the male rat. A release of kidney enzymes into the urine occurred during the development of cadmium-induced renal damage, and provided a useful criterion of toxicity in further studies. Cadmium accumulation in liver and kidney was associated with increases in the concentrations of zinc and copper in these tissues. Dietary cadmium exposure depleted the renal and hepatic content of iron. Repeated parenteral administration of cadmium had a similar effect but only in the kidney, and produced an excessive loss of trace metals into the urine, which may have exacerbated the disturbances in their metabolism. Changes in the plasma concentration of trace metals depended upon the route of administration and dosage of cadmium. A single injection of cadmium chloride increased the concentration of copper in plasma but decreased that of zinc and iron, while repeated injections increased the concentrations of both zinc and copper, and decreased iron. Long term dietary administration of cadmium chloride raised plasma copper but decreased both zinc and iron. The administration of high doses of zinc sulphate altered the tissue disposition of cadmium. The possibility that zinc may prevent some of the toxic effects of cadmium was investigated, but zinc itself induced changes in the homeostasis of essential metals. Cadmium-treated rats showed changes in calcium homeostasis which were suggestive of an impaired absorption, and the accumulation of trace metals in the femur was inhibited. These changes were independent of the development of kidney damage. The dietary administration of cadmium also decreased the activity of femur alkaline phosphatase. This effect was prevented by dietary zinc supplementation. The effectiveness of a variety of chelating agents to mobilise and promote the excretion of cadmium was compared. Some lipophilic derivatives of diethylenetriaminepentaacetic acid were very effective when administered after acute cadmium exposure, but no compounds significantly decreased the body burden of cadmium in animals which had accumulated the metal in tissues.
Keywords: Toxicology & poisons


Arthritis is one of the most common problems I see in veterinary practice. Just like us, as our dog's age, they can develop arthritis.
While larger breed dogs are more prone to this condition, arthritis occurs in any breed of dog. What are the symptoms of arthritis?
We called upon our expert veterinarian, Dr. Kristen Andrews, to share symptoms to look out for to recognize arthritis and steps you can take to manage it with your beloved pets.
First and foremost, if your pet is experiencing any of these symptoms, consult with your veterinarian before starting any medication for them. There are different types of arthritis as well as other diseases that may look like arthritis and may require special treatment for them. Your veterinarian is the best person to determine if your dog has arthritis and to properly advise you on how to treat it. While canine arthritis, also known as osteoarthritis or degenerative joint disease can't be cured, there are various ways in which it can be managed to help minimize the pain and discomfort associated with this condition.
Anti-inflammatories and pain medication. There are various pain relievers and anti-inflammatory drugs available for your veterinarian to use for your pet such as TruProfen. ALWAYS consult your veterinarian before giving ANY medication to your pet—including over the counter medication such as aspirin, ibuprofen, or Tylenol. It can be easy to overdose your pet thus causing harmful side effects or toxicity. In addition, these medications may interfere with medications your veterinarian may want to prescribe for your pet.
Joint supplements. In mild cases of arthritis, some dogs can find comfort with a good quality glucosamine and chondroitin supplement like VetIQ's Hip and Joint chews. Joint supplements may also be used in more severe cases of arthritis along with anti-inflammatories and pain relievers as they may help reduce the dosage needed of some of these medications.
Joint diets. Diets geared toward joint support can be very useful either alone or in combination with the above mentioned products to help reduce the pain and inflammation associated with arthritis.
Weight loss. Obesity leads to added stress and strain on your dog's joints. Your veterinarian can aid you in helping them get down to a healthy weight which can make a big difference in their mobility.
Ramps and other mobility help. Use a ramp to help your dog navigate stairs more easily or to make it easier to get into the vehicle or onto the bed or furniture with you.
Comfortable sleep. Make sure they have a comfortable bed. Many companies now make orthopedic mattresses and beds for your pet.
Elevate food and water bowls. Keep food and water elevated slightly will help a dog with arthritis because it will reduce strain on the neck and spine.
Natural and homeopathic therapies. Massage, physical therapy, hydrotherapy, laser therapy, acupuncture, and chiropractic adjustment may also provide additional relief from pain and inflammation for your pet.


text:
Spider Creek Tivas 3 defeat Halles Heroes BS-3 2-1
Spider Creek Tivas 3 2, Halles Heroes BS-3 1
Heroes BS-3 0 0 0 0 0 0 1 0 0 1 ? 9 ? 1 ?
Tivas 3 0 0 2 0 0 0 0 0 - 2 ? 5 ? 0 ?
W: Munger, R. (1-0)
L: Tewksbury, B. (0-1)
S: McMahon, D. (3)
At Griffith Stadium '41, the Spider Creek fans witnessed a great pitcher's duel. George Munger(1-0) finally bested his Halles opposite, Bob Tewksbury(0-1), by the score of 2 to 1.
Munger delivered a fine performance for Spider Creek. He went 5 and 2/3 innings surrendering 6 hits and 3 walks. Munger racked up 6 strikeouts lowering his ERA to 1.32. Halles had 9 hits in the game while Spider Creek had 5, but Spider Creek had the more timely hits.
Don McMahon gained credit for his 3rd save. Tewksbury took the loss. He surrendered 2 runs and 4 hits in 5 and 1/3 innings.
'I didn't have my best stuff but sometimes you just get lucky,' Munger said, 'this was one of those times.'
J. Burroughs RF 4 0 1 0 .310
B. Tewksbury P 2 0 0 0 .000
L. Arroyo P 0 0 0 0 .000
A - S. Javier PH 1 0 1 0 .667
B - A. Etchebarren PH 0 0 0 0 .500
C - D. Zimmer PR 0 0 0 0 ----
B. Tewksbury (L, 0-1) 5.1 4 2 2 1 3 0 87 4.09
L. Arroyo 0.2 0 0 0 0 0 0 9 4.91
C. Bradford 2 1 0 0 0 0 0 25 0.00
Totals 8 5 2 2 1 3 0
B. Tate C 3 1 1 0 .357
G. Munger P 2 0 0 0 .000
G. Munger (W, 1-0) 5.2 6 0 0 3 6 0 87 1.32
S. Miller (H, 2) 0.1 0 0 0 0 0 0 5 0.00
D. McMahon (S, 3) 3 3 1 1 4 2 0 59 10.97
A-Pinch Hit For Arroyo In 7th Inning
B-Pinch Hit For Bradford In 9th Inning
C-Pinch Ran For Etchebarren In 9th Inning
Heroes BS-3..... 0 0 0 0 0 0 1 0 0 - 1 9 1
LEFT ON BASE- Heroes BS-3:11 Tivas 3: 3
ERRORS- V.Castilla
TRIPLES- N.Lajoie(1st), R.Metzger(2nd)
WALKS- K.Daniels-2, J.Burroughs, D.Henderson, V.Stephens-2, A.Etchebarren,
H.Rice
STRIKE OUTS- D.Henderson, B.Grich-2, V.Stephens, M.McGwire, B.Foote-2,
B.Tewksbury, C.Christensen, G.Munger-2
GIDP- J.Burroughs, V.Castilla-2, M.McGwire, S.Adams


text:
Stathmopoda anconias is een vlinder uit de familie Stathmopodidae. De wetenschappelijke naam van de soort is voor het eerst geldig gepubliceerd in 1910 door Meyrick.

Stathmopodidae


text:
Guatemalan soldiers massacre seven indigenous protestors
By Moises Castillo and Romina Ruiz-Goiriena / Associated Press
Thousands of indigenous Guatemalans shouted in anger Friday and some threw themselves at the coffins of six local people who were shot to death during a protest over electricity prices and educational reform in a poor rural area.
A seventh victim died later at a hospital in the western city of Quezaltenango.
President Otto Perez Molina acknowledged that government forces had opened fire during the protest Thursday, after saying earlier that police and troops on the scene had been unarmed and the protesters had provoked the clash.
Human rights groups condemned the government's actions and charged they were part of a pattern of excessive use of force against protesters.
The protesters were blockading a highway near the town of Totonicapan, about 90 miles west of Guatemala City, when two vehicles carrying soldiers arrived to help police who had been ordered to evict the demonstrators. Gunfire erupted after the troops came. Bullets killed seven people and wounded 34, officials said.
"We were protesting right next to them when they opened fire on us," said Rolando Carrillo, a 25-year-old protester with a bandaged arm and lacerated face that he said resulted from being hit during the clash.
The president told reporters Friday afternoon that armed security guards had driven the soldiers to the protest. One of the guards apparently was the first to start shooting and then an unspecified number of others fired at the crowd, Molina said.
He said seven soldiers injured in the confrontation had said they only fired into the air to protect themselves from what they considered to be a threatening crowd.
Interior Minister Mauricio Lopez Bonilla said the president had suspended the order to evict the protesters from the highway.
Some 20 human rights organizations called an emergency meeting in the capital to discuss the incident and called for a protest in front of the presidential palace.
"We've been saying for a long time that the army's use of force brings with it the risk that something like this could happen," said Francisco Soto, a representative of the Center for Legal Action and Human Rights.
Six of the dead were buried Friday afternoon in Totonicapan, where thousands gathered to watch their coffins pass through the town's central square. Hundreds shouted "Justice! Justice!" while dozens of mourners hurled themselves toward the coffins in grief.
Read more from The Washington Post: http://www.washingtonpost.com/world/the_americas/angry-guatemalans-demand-justice-after-7-protesters-killed-as-troops-confront-highway-blockade/2012/10/05/a132f6b4-0f56-11e2-ba6c-07bd866eb71a_story.html
Tags: Associated Press, Friday, Guatemala City, Human Rights, Interior ministry, Otto Pérez Molina, Protest, Protesters Slaughtered, Quetzaltenango, Quezaltenango
Human Rights, NWO, Social Engineering