text:
http://bookofachievers.com/articles/teen-writes-with-both-hands-simultaneously-can-you-beat-it
Hobbies & Interests writer
Manguluru's teen sets a world record in writing is now aiming for a Guinness World Record.
Never went to school. Writes in 10 styles using both hands. Mimics, sings, paints and is preparing set world records in 10 fields.
Who said that one needs formal schooling to excel in life? School provides access to improve the overall performance of children by including various activities in the curriculum. However, if formal schooling is not providing a conducive atmosphere and is sending waves of discomfort to a child, then how about self-study and homeschooling? Knowledge gaining doesn't depend upon the number of books you carry in your bag or how many hours you spend in the school. When someone is inquisitive about learning, it can naturally happen from anywhere. Moreover, few children who don't perform well during the formal school hours give their best when they are given a chance to self-learn and explore. One such unduly curious kid who started reading just in 18 months after her first cry and displayed her ability to write 30 pages when she was just 30 months old is now aiming to achieve Guinness World Record soon.
A Teenage Girl's Exceptional Ability:
Have you ever heard of someone being ambidextrous? Well! Someone who is capable of writing with both the hands is termed as ambidextrous. Though they aren't many, there exists some good number of ambidextrous people around us. So here is the journey of one such girl from Namma Kudla, 16-year-old Aadi Swaroopa, born to Gopadkar and Mrs. Sumadkar who run Swaroopa Adhyayana Kendra. Aadi has the innate ability to write with both hands. So, what's so new and exciting about this? Well, Aadi has created a world record for writing the maximum words simultaneously with both hands in just one minute. She set the world record for writing 45 words in one minute in unidirectional style breaking the past record of 25 words/minute. LATA Foundation of Rai Bareli, Uttar Pradesh has declared this activity of her as an exclusive world record in July 2020.
A Talent That Writes In Styles and Types Innumerable:
Aadi Swaroopa can write in ten distinct ways using both her hands. During the lockdown period, she enhanced her skills and introduced herself to 10 different writing styles like uni-direction, left-hand speed, right-hand speed, reverse running, mirror image, heterotopic, hetero linguistic, exchange, dancing, and blindfolding. These techniques activate both left and right brains simultaneously and we know what and how much it means!
A Versatile Learner Who Never Went To School:
When she was just 18 months old, Aadi started to read. This fastest writer, who writes with a speed of 40 words per minute, started this writing practice at Swaroopa Kendra as a creative and fun-to-do home task. By the time she attained two and a half years, she developed the ability to write with both the hands. Aadi, who has never entered a school after the formal school setting and pressures instilled fear in her, shall appear for the SSLC examinations as a private or external candidate. Right from the age of two and a half years, Aadi accompanied Swaroopa's Education Jatha until 2019 and has taken part in more than 1600 programmes. She showcased her talent along with the group. She performed mimicry, Beat Box, and memory shows that entertained, awed, and inspired numerous others. Aadi has a deep inclination for music right from childhood.
She has been learning Hindustani Music from Pandit Ravi Kiran, Manipal, Yakshagana from Vidhushi Sumangala Rathnakar, Guitar, and Keyboard online. She prepared notes for the SSLC syllabus and composed many poems contributing her vocals to over 10 C.Ds. Aadi also writes stories and novels. Her first collection of 40 stories, Aadhiya Kathe Anthya Nive Heli, was released when she was 10 years old. Thus she turned into a published author when she was just 10. She has also conducted an exhibition of all her paintings at Prasad Art gallery, Mangaluru. She has also given programmes in All India Radio, Namma T.V., along with various regional and national channels. Aadi is a curious learner of various aspects and with a great memory, she presents all the names of 736 districts of India, 64 Vidyas, 101 Kauravas, etc. She is a record holder in creating visual memory art, wherein she draws one complete lesson on a single paper driving home exceptional memory technique. She has the ability to record and recall thousands of phone numbers and can solve the Rubix cube in 45 seconds. In a group event organised under the association of Pruthwish Brahmavara, she set a Guinness Record in this arena. She is also deeply inclined towards studying psychology and loves the critical analysis of things. This voracious reader does all these not under the pangs of formal schooling or pressures. She does them at the comfort of her learning pace and the freedom to learn given to her lets her explore her talents, interests and capabilities further letting her remain active and effective for around 16 hours a day. Wow!! Don't you think she is into many more areas of expertise than a formal curriculum could offer?
What does She wish To Accomplish?
Swaroopa is aiming to set national and world records in various fields like mimicry, Rubik's cube and music. She wants to set at least 10 world records in the fine arts. While she has already set a Guinness World Record in Rubik's Cube Mosaic with her mother, Sumangala Sumadkar in the group category in 2018, she would like to participate and set the record in the same under the solo category in 2021. She also wants to set a world record in Beatbox wherein she mimics drum machines by using mouth, lips, tongue and voice. She has also pushed her word count per minute to 50 from 45. Eventually, she wants to raise the bar setting it to 60.
We wish Aadi many more accomplishments to her credit and may she become an icon of free-style and self-paced learning.
Success is beyond the classroom & books says college drop out whose FRiEnDz magazine has thousands of readers.
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Meet the Aipan artist and know more about her and the dying ART.
Hyderabad has a new look with this Artist's amazing Art all over. People cannot stop admiring.
writing with both handshomescholingmangulurumimicrysingingguinness world recordno formal schoolingAmbidextrousAadi SwaroopaSwaroopa Adhyayana Kendraaadi swaroopa mangalore


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<title>SYSCS_UTIL.SYSCS_SET_USER_ACCESS system procedure</title>

SYSCS_UTIL.SYSCS_SET_USER_ACCESS system procedure

The <samp class="codeph">SYSCS_UTIL.SYSCS_SET_USER_ACCESS</samp> system
procedure sets the connection access permission for the user
specified.

Syntax

SYSCS_UTIL.SYSCS_SET_USER_ACCESS (USERNAME VARCHAR(128),
CONNECTION_PERMISSION VARCHAR(128))

USERNAME

An input argument of type VARCHAR(128) that specifies the user ID in the
Derby database.

CONNECTION_PERMISSION

Valid values for CONNECTION_PERMISSION are:

FULLACCESS

Adds the user to the list of users with full access to the database. The
value for the database property is
<samp class="codeph">derby.database.fullAccessUsers</samp>.

READONLYACCESS

Adds the user to the list of users with read-only access to the database.
The value for the database property is
<samp class="codeph">derby.database.readOnlyAccessUsers</samp>.

null

Removes the user from the list of permissions, reverting the user to the
default permission. You must specify <samp class="codeph">null</samp> without the quotation
marks.

Execute privileges

If authentication and SQL authorization are both enabled, only the
database owner has
execute privileges on this procedure by default. See "Enabling user
authentication" and "Setting the SQL standard authorization mode" in the
Derby Developer's Guide for more information. The
database owner can grant access to other users.

Example

CALL SYSCS_UTIL.SYSCS_SET_USER_ACCESS ('BRUNNER', 'READONLYACCESS')

To
remove the user from the list of permissions, you specify the <samp class="codeph">null</samp> value
without the quotation marks. For example:

CALL SYSCS_UTIL.SYSCS_SET_USER_ACCESS ('ISABEL', null)

Parent topic: Built-in system procedures

Related reference

SYSCS_UTIL.SYSCS_GET_USER_ACCESS system function

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Shirley Yamaguchi, Eitarô Ozawa, Noriko Sengoku, Takashi Shimura, Toshirô Mifune, Yôko Katsuragi
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The WGMW Gallery
From the Chair
Captain Pugwash
Driving Day
From lens to bends, Andrew Morland is sharp
by Andrew Morland | Nov 26, 2017 | Musings
1997 and all that 20 years on – Is the wheel turning full circle?
From the chair: December 2017
As a professional photographer I have spent many years photographing cars racing and rallying and I have always had a yearning to actually compete.
On obtaining my 'bus pass' I decided it was time to get my race licence. After some research and encouragement from friends and racers I began the process.
The governing body of motorsport in the UK is the Motor Sport Association.
We have the largest domestic motor sport scene in the world, with 10,500 circuit racers, amateur and professional.
A diverse range of cars, from single seaters to Edwardian racers, with an equally diverse range of drivers of all age groups are racing. I obtained my licence in 2014 by taking the Association of Racing Drivers course at Castle Combe.
I had already decided to race pre-war cars as I own a couple of MGs.
My initial problem was that they were both in pieces! Barry Foster, a friend who races, offered me a drive in his very precious and famous 1931 MG 'C' Type as he had been lent an even rarer 'Q' Type to race in the same race.
It took a few days to decide to accept the offer as some friends advised against it thinking it was too risky starting out in someone else's very valuable car.
Others thought it would be foolish to miss such an opportunity and despite the risk I gratefully accepted the offer.
Barry and his 'C' Type hold the world 750cc supercharged 24 hour record for 2,000 km and 1,000 miles, plus the record at Pendine Sands for the ½ kilometre flying start. It is a well-proven and extremely quick car with an engine that he built himself.
I set off to Silverstone for the Triple M race, having only driven the 'C' in Somerset down to the local fuel station. In practice I had the feeling that I was well out of my depth and wondered what on earth I was doing there!
First race, first time at Silverstone in a precious car, and gears round the other way to any of my cars. I tried to work out the racing lines without getting in anyone's way. Happily I made it to a mid-grid position in our class (above).
At the start I was left behind but slowly managed to make up the order. I was glad that I had thoroughly learnt all the flag signals at Castle Combe Circuit as there was a very nasty accident during the race which brought out all the red flag. The very competent marshals lined us up in order and we then had a 15 minute wait, worrying about the state of the driver involved in the accident which it turned out was caused by a puncture.
Eventually we set off again, a bit rattled, behind a safety car. By the end of the race I had seen 10 of the 11 race flags that I had learnt. Several other competitors had various problems during the race. Despite my erratic lap times things seemed to improve for me and by the end I was in 3rd place.
I had contemplated trying for 2nd place but remembered the words of my Castle Combe tutor, 'just keep out of trouble and finish your first race'! I thought at the time that 3rd was as good as it gets and I was right, as after 3 years of racing my MGs,' L' and 'P' Types, I remain at mid to back of the grid, where incidentally one meets the nicest of people and I have had a great deal of fun too!
I race with the MG Car Club and the Vintage Sports Car Club. Grids are well supported and are good value. The events are well run with mostly polite, safe drivers who try not to collide with or force you into barriers. Both clubs have an inclusive and friendly social scene.
This year at VSCC Oulton my car failed scrutineering and I was floundering around trying to fix a loose bearing in a hub when a few people, who I had not met before, appeared with special tools, plenty of cheerful advice and proceeded to help me to fix it and therefore be able to join the race.
The MG CC has a series for ZRs and other MG/Rovers, with a strict control of modifications. The cars are cheap to buy and to prepare. The MG CC has full grids, helped by the under 25s getting a half price entry fee. The VSCC is even more generous as even the under 30s get half price entry.
To set about getting a licence one should get an MSA 'Welcome to Motor Sport'/'Go Racing' starter pack which comes with a 'what to do' booklet, a DVD with plenty of advice and an electronic version of the MSA Year Book, known as the 'Blue Book'.
This details safety regulations, conduct and fair play and a list of accredited Associations of Racing Drivers Schools at British circuits. In the South West area we have an excellent school at Castle Combe where one takes a 30 minute written test, and very importantly a safety flag and track test with an examiner.
This is not a test of your speed and skill so it a good plan not to show off and frighten the examiner! Once you have passed the examiner stamps your licence application and will return it to the MSA, who will send you your competition licence.
The MSA starter pack costs £99 (£61 for karting). The ARDS test at a circuit is £320. Castle Combe is the centre for our region and has excellent tutors and training. Their contact is Emma Strawford at the circuit. [email protected] Information can be found on the MSA website and the Blue Book contains details of all the Clubs and Championships you can enter.
If you set your sights on being a professional you can start early racing in the 14 – 17 year olds class to get a Race National 'B' Junior Formula Licence.
Hamilton and Button started young with an MSA Karting Licence. Now Somerset has a new potential world champion, Lando Norris, who has progressed through the formula in single seaters, winning the F3 European Championship. He is the new Mclaren F1 test and reserve driver for Alonso and Vandoorne. In his first full test in the Hungarian GP practice for McLaren he set the second fastest lap behind Vettel's Ferrari.
All a far cry from pre-war MGs but plenty to encourage any budding drivers to go for it, get a licence and have some fun!
© Andrew Morland
Andrew Morland
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When aspiring filmmaker David is mandated by a judge to attend a social program at the Jewish Community Center, he is sure of one thing: he doesn't belong there. But when he's assigned to visit the Brooklyn Bridge with the vivacious Sarah, sparks fly and his convictions are tested. Their budding relationship must weather Sarah's romantic past, David's judgmental mother, and their own pre-conceptions of what love is supposed to look like.
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Detective Nick Blades is a New Orleans cop on trial for corruption. Assistant District Attorney Theo Gold is the man in charge of putting him behind bars. When these two unlikely partners from opposite sides of the law stumble onto a criminal plot, they'll need to rely on luck – and patience – to take down a dangerous killer without killing each other first.
A psychiatrist becomes the new Sorcerer Supreme of the Earth in order to battle an evil Sorceress from the past.
Genre: Action, Fantasy
Grand Prix driver Pete Aron is fired by his team after a crash at Monaco that injures his teammate, Scott Stoddard. While Stoddard struggles to recover, Aron begins to drive for another team, and starts dating Stoddard's wife.
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An ex-office worker becomes a ventriloquist, leading to a date with his unemployment counselor; but his quirky family and a gauche female friend may thwart his new career and love life.
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Brooklyn teenager Jeffrey Willis, thoroughly unhappy with his modest homestead, embraces the other-world aspects of his summer job at the posh Flamingo Club. He spurns his father in favor of the patronage of smooth-talking Phil Brody and is seduced by the ample bikini charms of club member Carla Samson. But thanks to a couple of late-summer hard lessons, the teen eventually realizes that family should always come first.


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The purpose of this meeting was to present the study process, present existing conditions, present the proposed improvement, present the project schedule, and gather input on the proposed improvement within the Village and Township jurisdictions (IL Route 21 to St. Mary's Road).
It has come to our attention that individuals along Rockland Road have chosen to place their own markings along the roadside, in ditches, and on trees, beyond the roadside stakes placed by Township Highway Department staff and Professional Engineers. Any markings placed by those other than Township Highway Department representatives are not based on technical engineering analyses. Therefore, the reliability and accuracy of any of the markings you may see along Rockland Road can no longer be guaranteed.
© 2019 Libertyville Township. All Rights Reserved.


Fender's Rarities Flame Maple Top Stratocaster features a two-piece alder body with a flame maple Golden Brown top and a solid rosewood neck capped with a flame maple fingerboard for a totally luxurious look and feel. The Pure Vintage 65 Strat pickups add a classic voice to the more modern, custom DoubleTap™ bridge pickup which offers both a sweet humbucking voice and—via an S-1™ switch—a dynamic single-coil sound. Like the rest of the Rarities series, these are limited-edition instruments, carefully built from select tonewoods for discerning players.


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This is one of my favorite individual shots of Kate in her wedding gown. The lighting included a speedlite in an umbrella as the key, a snooted flash to add a touch of light just to her face, and an on-axis strobe in a ring-light attachment to provide some overall fill. All the lights had various degrees of CTO gels attached to add some warmth to the room. I did some significant editing here: lens distortion correction to straighten out vertical and horizontal lines, some contrast masking to emphasize detail and add mid-tone contrast, and the removal of some distracting elements: electrical cords, the edge of a door frame, and a painting hanging on the wall, which in later shots I physically took off the wall but I really loved her expression in this particular frame, so I decided to go with this one even if it meant some extra photoshop work. Now I also wish I had taken the lamps out of the shot, and I thought about trying to do so in photoshop, but decided that, with the shadows they cast, it would just be too difficult.


Another road trip. Everybody is happy about road trips. Our moms just decided to get in the car and drive, preferably south. It is winter here in Colorado. Let's take a quick trip looking for warmer weather. We are an unusual group this trip. I, Zeb the Duck, Soapy Smith Duck, my mom, Soapy's mom and Soapy's dog Chloe.
Chloe is part Pit Bull, part Labrador, and probably has some Dalmatian. Under her white fur, some black spots are on her skin. This is Chloe's first long road trip. This will be her first time in a motel, first time in an elevator, and many more firsts. Heading south from Denver on I-25, we enter New Mexico, and about 100 miles further this rest area caught our attention.
We are near Fort Union and this rest area is part of Fort Union National Monument. The rest area has all the normal things, rest rooms, information maps and vending machines, but there is more.
Isn't this a nice picnic area? We liked the overhead cover. Gives protection from snow, rain and the intense New Mexico sun. Maybe we will stop here for a picnic on another trip. We liked this wagon wheel. Part of old American history.
Wagon wheel. Maybe from Santa Fe Trail travelers?
The Santa Fe trail passed through here. Can you imagine traveling across the desert and over mountains in a covered wagon? It was still chilly and windy here, so we did not go Fort Union this time. But mom and I have been here before, so I want to show you more about Fort Union. I, Zeb the Duck, was very young and this was one of the first trips in my blogging career. Mom, I, Zeb the Duck, and my Alaska uncle visited here in 2013.
The park rangers told us there were 3 separate forts built on this location. The first was to protect the Santa Fe Trail, the second to establish a Federal presence in the territory, and the third Fort Union was a Union response to the Confederate invasion. Those interested in our Civil War should visit here.
Ruins of Fort Union. Two previous forts were closer to mountains.
Also history of Santa Fe Trail.
Ruts from wagons on the Santa Fe Trail are visible in the hard, dry ground. The third Fort Union is the one most visited.
This fort was a large supply facility for the southwest. At one time about 5,000 soldiers lived here. We were warned to stay on the paved walkway and to watch for rattlesnakes. It was a sunny day. Pleasant for us, but rattlesnakes also like sunshine. We stayed on the path, read the signs, and did not see any snakes. About those supplies: In 1868, 44 tons of bacon were brought to Fort Union in 22 wagons. That's a lot of bacon. Many other supplies were also delivered here.
Fort Union had the premier hospital in the region with 6 wards and 36 beds. You could get treatment and care for 50 cents per day! Fort Union was abandoned in 1891. Fort Union is easy to visit, just a rather short drive from I-25. It is interesting.
If you visit, watch the film at the Visitor's Center, and don't miss the gift shop. More about our new road trip next time.


Experience the thrill of a wildlife safari during five days in the Serengeti and the Ngorongoro Crater and discover lions, leopards, elephants, zebras, and colorful birds with local guides.
Get immersed in Maasai culture on visits with warriors, artisans, and schoolchildren, and explore a traditional Maasai boma.
Examine fossils at the Olduvai Gorge, where Homo habilis remains were discovered on a National Geographic-sponsored expedition.
Hike through the wilderness of a private nature reserve with rangers for an optional night of authentic bush camping.
Venture into the wilds of Tanzania on a family safari and encounter a mind-boggling array of wildlife. Here, humans are but tiny dots on a sweeping savanna, surrounded by zebras and wildebeest, lions and cheetahs, elephants and rhinos, and hundreds of colorful bird species. Settle into a remote camp in a part of the eastern Serengeti known for its vast numbers of giraffes and elands. Get to know local Maasai people, who welcome us into their homes and schools and share their vibrant traditions. With the help of our trip leader and local rangers, learn to identify tracks and interpret animal behavior, and encounter an incredible diversity of wildlife on safari in the Serengeti and the Ngorongoro Crater.
Karibu! Arrive into Kilimanjaro International Airport in Tanzania and transfer to our hotel in Arusha.
Take a short flight to the eastern Serengeti and continue to a private nature refuge, nicknamed "Giraffic Park." Explore on foot or by safari vehicle and meet young Maasai warriors. Venture into a typical boma settlement, and "jump" into a traditional Maasai dance. Cap off the day with a thrilling nighttime safari. The next morning, take a bush walk with a wildlife expert and visit a Maasai village school during the Kid to Kid Connection. If you wish, hike into the wilderness with our rangers for a night of authentic bush camping under the stars.
Enjoy three days on safari in the legendary Serengeti observing a mind-boggling array of animals. Float over the savanna on an optional early-morning hot air balloon ride or spot wildlife on a dawn game drive. Visit a women's craft collaborative, learn the game of bao, try Tanzanian cuisine, and identify animal prints with trackers.
Examine fossils at Olduvai Gorge where Louis and Mary Leakey discovered Homo habilis remains on a National Geographic–sponsored expedition. Then settle into a coffee estate on the outer slopes of the Ngorongoro Crater. Relax on the veranda, visit the farm animals, or ride a bike to the nearby village.
Descend 2,000 feet to the crater floor and spend a full day on safari surrounded by some 25,000 wild animals. Later, gather around a fire to hear tembo (elephant) folktales before our farewell dinner. Enjoy a rare chance to spot nocturnal bush babies tonight.
Today, meet an Iraqw storyteller and his artisan wife at their home, visit an art center, and browse local handicrafts. Relax in day rooms in Arusha before heading to the airport for your overnight flight home.
Extend your safari in the wilds of Tarangire National Park, located southwest of Arusha. The park draws many hundreds of elephants to the Tarangire River, which remains the only permanent source of water from June to October. Spend a full day on safari, spotting buffalo, impala, zebra, and hartebeest—and their predators—and observe elephants in their natural habitat with an elephant researcher. Stay in a comfortable Nyumba camp beneath centuries-old baobab trees and enjoy another unforgettable experience in the Tanzanian wilderness.
Bid farewell to the main group and drive to the town of Mto Wa Mbu, surrounded by fertile farmland near Lake Manyara. Stroll through the leafy streets and bustling markets of the town, and interact with the local people. Then continue south by Land Rover to Tarangire National Park. Watch for wildlife as we drive, looking out for the big cats and other creatures who become active at the end of the day. Settle into our private Nyumba camp, clustered in between soaring baobab trees and perfectly situated for setting out on wildlife drives.
With 1,600 square miles of protected habitat, Tarangire is a place of refuge for northern Tanzania's largest population of elephants. Encountering elephant herds, with their young guided protectively with elders' trunks and feet, is an unforgettable sight. Head out on a full-day wildlife drive with an elephant researcher, following the Tarangire River as it winds through the rugged landscapes of the park. Look for herds of zebra, as well as lions, leopards, reedbucks, giraffes and maybe wild dogs or a rare fringe-eared oryx. Spot some of the more than 550 birds that call this region home. Track herds of elephants and learn about their intelligent behavior, their shrinking habitat, and the urgent need to preserve their home in the wilderness. Later this afternoon, join local kids and camp staff for a game of soccer or just relax under the baobabs and listen to the sounds of the wilderness.
After breakfast, you'll leave Tarangire and drive to Arusha. Visit a local art workshop that employs local people with special needs and browse local crafts at a cultural center. Relax in day rooms and take a dip in the hotel pool before we head to the airport for evening flights home.


text:
back AUD
Childhood and Death in Victorian England
Fashion and Family History: Interpreting How Your Ancestors Dressed
Private Publisher
Canowie Station: A Pastoralism Wonder Revealed
Archive Digital Books Australasia
New South Wales Telephone Directory 1945: Sydney - EBOOK
Takeaway Publishing
Divorced, Bigamist, Bereaved: The Family Historian's Guide to Marital Breakdown, Separation, Widowhood, and Remarriage from 1600 to the 1970s
Boolarong Press
Stuff We Had in the '50s and '60s
The Medieval Village
1 review Write a Review
PNS313
This Item: Childhood and Death in Victorian England
Media: BOOK - paperback, 224 pages
Author: S. Seaton
Other: b&w photos, sketches, index
Publisher: Pen & Sword
In this fascinating book, the reader is taken on a journey of real life accounts of Victorian children, how they lived, worked, played and ultimately died. Many of these stories have remained hidden for over 100 years. They are now unearthed to reveal the hardship and cruel conditions experienced by many youngsters, such as a travelling fair child, an apprentice at sea and a trapper.
The lives of the children of prostitutes, servant girls, debutantes and married women all intermingle, unified by one common factor – death. Drawing on actual instances of Infanticide and baby farming the reader is taken into a world of unmarried mothers, whose shame at being pregnant drove them to carry out horrendous crimes yet walk free from court, without consequence. For others, they were not so lucky.
The Victorian children in this publication lived in the rapidly changing world of the Industrial Revolution. With the introduction of the New Poor Law in 1834 the future for some pauper children changed – but not for the better. Studies have also unearthed a religious sect known as the 'Peculiar People' and gives an insight into their beliefs.
This book is not recommended for those easily offended as it does contain graphic descriptions of some child murders, although not intended to glorify the tragedies, they were necessary to inform the reader of the horrific extent that some killers went to. This book will appeal to anyone with an interest in the social history of the Victorian period.
1. Industrial Mishaps and Misdemeanours
2. Accidents
3. Poverty, Paupers and Health
4. Manslaughter, Murder and Circumstantial Evidence
5. Newborn and Early Infant Deaths
Interesting but limited discussion
Posted by Gary Bull on 24th Dec 2017
It is by no means an academic work but Sarah has done a lot of research. I expected an in depth study of the life and death of Victorian children but the scope was limited to more sensational deaths and generalised proletariat life. She seems to have quoted many newspaper reports and court records verbatim. Some stories drag on and I found I lost track of her discussion. The work is not what I expected from a person with a masters degree in history.
? Have Questions? Ask an Expert
Ask Alona anything on Gould Genealogy
Annual Report of the Registrar General of Births, Deaths, and Marriages in England and Wales 1901
Feudal England
Researching Your Ancestor's Childhood
Batsford
Victorian Maps of England: The County and City Maps of Thomas Moule
Researching Your Ancestor's Childhood - EBOOK
Tracing Villains and their Victims: A Guide to Criminal Ancestors for Family Historians
South Australia on the Eve of War
Family Tree Books
The Family Tree Irish Genealogy Guide: How to Trace Your Ancestors in Ireland
The War to End War: Tracing Your Great War Australian Military Ancestors
Australians in Peril: Tracing Your World War Two Australian Military Ancestors
Your Swedish Roots: A Step-by-Step Handbook
Migration to New Zealand: A Guide for Family History Researchers
DNA for Genealogists (4th edition)
Van Diemen's Women: A History of Transportation to Tasmania
Google: The Genealogist's Friend


text:
Living On Soul NYC Premiere
Celebrate The Daptone Records Family in the Soul of Brooklyn
by Kurtis Powers | 23 Oct, 2017
In December 2014, Daptone Records presented a three-night concert at the Apollo Theater in Harlem. According to "Mr. Apollo" Billy Mitchell, nothing like this had taken place at the Apollo since James Brown's 1970s residency. Many equated this concert, which featured performances by Sharon Jones & The Dap-Kings, Charles Bradley & His Extraordinaires, Naomi Shelton & The Gospel Queens, Antibalas, Menahan Street Band, The Budos Band, and more, to the legendary 1967 Stax/Volt Revue.
Filmmakers Jeff Broadway and Cory Bailey have showcased this legendary event in their new film, Living on Soul, which stands as a beautiful document in the tradition of The Last Waltz, Monterey Pop, and Soul Power. This hybrid music documentary/concert film unearths the anecdotal history of one of the most important labels and "families" in soul music, Daptone Records, through vérité-style scenes and live performances from the most iconic soul music stage in the world. The film also serves as a celebration of the lives and talent of those Daptone artists who are no longer with us: Sharon Jones, Charles Bradley and Naomi Shelton pianist, Cliff Driver.
After its recent West Coast premiere at the Los Angeles Film Festival, Living on Soul now comes to Brooklyn's Nitehawk Theater in Williamsburg on Wednesday, November 15 at 7:30 pm. The Face Radio's Kurtis Powers will moderate a live Q&A after the film with Neal Sugarman, founder of Daptone Records, and the filmmakers, Jeff Broadway and Cory Bailey. The Face Radio will also broadcast the Q&A live on Facebook and take viewers' questions.
After the event, we hope you'll come join us for the after-party in The Nitehawk's Lo-Res Bar, featuring Daptone DJs and giveaways!
Get your tickets before they're all gone!
< Durand Jones & The Indications Make A Change In NYC / Orgone: Beyond Bulletproof >
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Girls To the Front! Latinas Take Over Celebrate Brooklyn
A showcase of powerful Latina voices, this Celebrate Brooklyn! performance is held in conjunction with…
World Music Massive at Celebrate Brooklyn!
There is certainly a reason to celebrate this week at BRIC's Celebrate Brooklyn! – two…
Mambo Big Band Orquesta Akokán Brings Cuba to NYC
Mambo has never been so punk rock. As one might expect, Daptone Records defied convention…
NYC Ska Orchestra hits Brooklyn Bowl For Modern Sounds in Jamaican Style
Ska is not dead – it's big, brassy and comin' atcha in Williamsburg. The New…


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MMO MMORPG News·Articles·FoM: Update to NPC's, a New City and New Armor!
FoM: Update to NPC's, a New City and New Armor!
Games in this article: Face of Mankind
1) Non-Player Character System
Face of Mankind is pleased to finally announce the implementation of a comprehensive Non-Player Character (NPC) system that will be used by our GameMasters for the facilitation of roleplay events.
The newly implemented system will allow GameMasters to edit a wide array of variables for these NPCs, ranging from appearance, speech, and missions issued, in a completely collaborative manner, allowing us to make the most of our GameMasters talents to produce results without needing an inordinate amount of time.
These NPCs will provide missions that can be accepted by any player as an alternative to the ones generated by the factions. They will largely be used to guide players along a storyline overarching all of Face of Mankind, that runs parallel to the roleplay that our players engage in on a day-to-day basis; to facilitate one-off events planned by our roleplay oriented Council or GameMasters; and tutorials for new players to get them better acquainted with what can sometimes be a steep learning curve in Face of Mankind.
A key feature that allows FoM to do the above is the introduction of what they call 'chained missions', which have a definite starting and ending point, and open up further successive missions upon the completion of prior ones.
2) Release of Berlin
The long-awaited release of the city of Berlin has finally arrived, but with many significant changes made to it.
Berlin is now a dilapidated wasteland far removed from its former self. It is a city that has been torn asunder by decades of civil unrest, and where the Dominion has effectively lost control over it. As such, it is a city that is completely devoid of the rule of law – a place where crimes can be committed without any consequences. That is, unless you happen to be caught by the rare Law Enforcement Department patrol red-handed.
Berlin is essentially a no-man's land, where no faction will ever have ownership over it. It is a place unlike any other, being completely inconquerable.
The Public News Service (PNS) reported about the "Fall of Berlin".
3) XenoTech Expeditionary Armor set
FoM is proud to announce the introduction of the next component of the xenomorph aspect of the game; a new set of armor that is made largely from the materials culled from xenomorph body parts. It provides incredible protection against ballistic damage, which is dealt by the xenomorphs on Necars Fields. As a result, it also provides greater protection against ballistic weapons.
Furthermore, it is lighter than armors of similar protection rates. However, it must be noted that this weapon is slightly weak against damage dealt by energy weapons.
Face of Mankind Partners with Overwolf
Face of Mankind Partners with Overwolf Nexeon Technologies, a free-to-play online game publisher and the d...
Face of Mankind Dev Diary: Dramatic Changes Coming
Face of Manking Dev Diary: Dramatic Changes in the Pipeline By Dev Oblivious, Nexeon Representative Face of...
Face of Mankind Dev Diary: World Takeover
Face of Mankind Dev Diary: World Takeover By Dev Oblivious, Nexeon Representative This week we would...


text:
\section*{Introduction}

Two-dimensional van der Waals materials constitute a versatile platform to realize quantum states by design, as they can be synthesized in many different stacking conditions \cite{liu2020disassembling}, offer a wide variety of chemical compositions and are easily manipulated by back gates, strain and the like. Stacking two sheets of van der Waals materials atop each other at a relative twist has recently emerged as a vibrant research direction to enhance the role of electronic interactions, with first reports on  twisted bilayer graphene \cite{cao2018a,cao2018b,Yankowitz18,Kerelsky18,Choi19} and other van der Waals materials stacked atop each other at a twist  \cite{Jin18,tran2019evidence,alexeev2019resonantly,seyler2019signatures,Xian18,Naik18,Wang19TMD,Scuri19,Kerelsky19,Andersen19,Kennes2020} displaying features of correlated physics that afford an unprecedented level of control. In particular, bi-, tri- and quadruple-layer graphene as well as twisted few-layer transition metal dichalcogenides (TMDs) are currently under intense experimental scrutiny \cite{lu2019superconductors,stepanov2019interplay,arora2020superconductivity,chen2020nature,liu2019spin,shen2019observation,cao2019electric,he2020,tutuc2019,Wang19TMD}.  By forming a Moir\'e supercell at small twist angles, a large unit cell in real space emerges for twisted systems, which due to quantum interference effects leads to a quasi-two-dimensional system with strongly quenched kinetic energy scales. This reduction in kinetic energy scale, signaled by the emergence of flat electron bands, in turn enhances the role of electronic interactions in these systems

Whereas the flatting of band dispersions in two-dimensional Moir\'e superlattices results mainly from the localization of charge density distributions by the Moir\'e potential, a well-known alternate pathway to flat bands can occur in certain lattices such as the Lieb and the Kagome lattices, where geometric considerations permit the formation of perfectly-localized electronic states on plaquettes and hexagons, respectively, that are eigenstates of the kinetic Hamiltonian due to destructive interference between lattice hopping matrix elements \cite{liu_2014}. Such flat band systems can give rise to many interesting phenomena, such as the formation of nontrivial topology when time reversal symmetry is broken, or other exotic quantum phases of matter due to their susceptibility to quantum fluctuations and electronic correlations \cite{leykam2018artificial}.

Here, we demonstrate that both flat-band mechanisms can be engineered to coexist in twisted bilayers of MoS$_2$ (tbMoS$_2$); a TMD of direct experimental relevance that has been extensively studied from synthesis to applications \cite{mak2010,wang2018synthesis}.
We confirm that families of flat bands emerge when two sheets of MoS$_2$ are stacked at a twist \cite{Naik18,naik2019origin} due to Moir\'e potentials. Our large-scale \textit{ab initio} based simulations show that while the first set of engineered flat bands closest to the edge of the band gap with twist angles close to $\Theta \approx 0^{\circ}$ can be used to effectively engineer a non-degenerate electronic flat band in analogy to a single layer of graphene at meV energy scales, more intriguingly, the next set of flat bands instead realizes a strongly asymmetric flat band p$_{\rm x}$-p$_{\rm y}$  honeycomb lattice \cite{wu2007prl,wu2008prb}. Both of these families of bands should be accessible experimentally via gating.  The strongly asymmetric nature of this p$_{\rm x}$-p$_{\rm y}$ honeycomb lattice is in marked contrast to the much discussed case of twisted bilayer graphene, where an approximately symmetric version of such a Hamiltonian is now believed to describe the low-energy flat band structures found at small twist angle \cite{bistritzer2011,PhysRevB.98.045103,PhysRevB.99.195455,PhysRevResearch.1.033072,TBGFRG}. The strongly asymmetric p$_{\rm x}$-p$_{\rm y}$ honeycomb model realized here features two almost entirely dispersionless flat bands that touch the top and the bottom of graphene-like Dirac bands at the Gamma point, respectively. These flat bands originate from destructive interference, in analogy to flat bands in the Lieb and the Kagome lattices \cite{liu_2014}, and will be referred to as ultra-flat bands in the following discussion, to distinguish them from other bands with quenched kinetic energy scales. In addition, these ultra-flat bands are topologically non-trivial once time-reversal symmetry is broken via spin-orbital coupling \cite{zhang2014}.  Previously, the p$_{\rm x}$-p$_{\rm y}$ model was studied in the context of cold gases where exotic correlated phases were predicted \cite{wu2007prl,lee2010fwave,wu2010f}, as well as in semiconductor microcavities \cite{jacqmin2014} and certain 2D organometallic frameworks \cite{liu2013omf,su2018}. Our findings elevate tbMoS$_2$ to a novel platform where effects of ultra-flat bands can be studied systematically in a strongly-correlated solid-state setting.
Notably, in the strong-coupling regime, the  p$_{\rm x}$-p$_{\rm y}$ model amended by Hubbard and Hund's interactions gives rise to a spin-orbital honeycomb model which -- depending on the specific parameters and symmetries of the model -- hosts magnetic, orbital as well as valence-bond orderings, or even more exotic quantum spin-orbital liquid phases~\cite{PhysRevB.90.094422,PhysRevB.98.245103,PhysRevB.100.205131}.

With this, our work adds an unprecedented type of lattice model -- the
highly asymmetric p$_{\rm x}$-p$_{\rm y}$ Hubbard model -- to the growing list of systems that can effectively be engineered using the twist angle between multiple layers. This is particularly intriguing as we maintain the full advantages that come with two-dimensional van der Waals materials, such as relative simplicity of the chemical composition and controllability of the material properties; e.g. of the filling (by a back gate), electric tunability (by displacement fields) or the band width of the model (by the twist angle).

\section*{Results}

\subsection*{{{\slshape \textbf{ab initio}}} characterization of twisted MoS$_2$}
\begin{figure}
    \centering
	 \includegraphics[width = \columnwidth]{figure1.png}
	  \caption{\captiontitle{Atomic and electronic structures of twisted bilayer MoS$_2$.} (a) Atomic structure of tbMoS$_2$ at $\Theta=3.15^\circ$. Local atomic arrangements of the three different regions in the Moir\'e unit cell are indicated in the right panels  (b) Evolution of low-energy band structures at the top of the valence bands of tbMoS$_2$ with decreasing small twist angles. The first set and the second set of valence bands are highlighted with blue and red lines, respectively.  (c) Evolution of the band width of the first set and the second set of valence bands with decreasing twist angles.    Inset: twist angle dependence of the ratio of the hopping amplitudes $t_\pi$ and $t_\sigma$ in the p$_{\rm x}$-p$_{\rm y}$ honeycomb lattice.      }
    \label{fig:fig1}
\end{figure}

\begin{figure}
    \centering
	 \includegraphics[width = \columnwidth]{figure2.png}
	  \caption{\captiontitle{p$_{\rm x}$-p$_{\rm y}$ honeycomb model for twisted bilayer MoS$_2$.} (a) Illustration of the model: in a honeycomb lattice composed of sublattices A and B, there are two orthogonal orbitals (p$_{\rm x}$ and p$_{\rm y}$) at each of the two sublattice sites. The solid and the dashed lines denote the p$_{\rm y}$ and the p$_{\rm x}$ orbitals, respectively, and the red and the blue color denotes the positive and the negative side of the orbital, respectively. (b) Fitting the dispersion of the p$_{\rm x}$-p$_{\rm y}$ model to the second set of valence bands of tbMoS$_2$ calculated with DFT for tbMoS$_2$ at $2.65^\circ$. The left panel shows the corresponding density of states displaying the signature four-peak structure. (c) Charge density, real and imaginary parts of the wavefunction calculated with DFT for the states in the two quasi-flat bands 1 and 4 shown in (b). The solutions of the corresponding states from the p$_{\rm x}$-p$_{\rm y}$ model are indicated with the blue and red ovals and agree with  the DFT results.     }
    \label{fig:fig2}
\end{figure}

We first characterize the low-energy electronic properties of twisted bilayer MoS$_2$ using density functional theory (DFT) calculations (see Methods). DFT in particular has established itself as a reliable tool to provide theoretical guidance and to predict the band structure of many twisted bi- and multilayer materials \cite{tran2019evidence,Kerelsky19,Wang19TMD}. However, such a first principles characterization becomes numerically very demanding as the twist angle $\Theta$ approaches small values and the unit cell becomes very large entailing many atoms (of the order of a few thousands and more). Nevertheless, it is that limit in which strong band-narrowing effects and as a consequence prominent effects of correlations are expected. The results of such a characterization are summarized in Fig.~\ref{fig:fig1}. Panel (a) shows the relaxed atomic structure of two sheets of MoS$_2$ in real space, twisted with respect to each other. A Moir\'e interference pattern forms at small twist angle yielding a large unit cell, within which we identify different local patterns of stacking of the two sheets of MoS$_2$, indicated via areas framed by cyan, magenta or purple dashed lines. The local stacking arrangements of the respective areas are given in the right sub-panels of panel (a). In panel (b) we show the  \textit{ab initio} band structure of the twisted material after relaxation, where we find two families of bands which will become increasingly flat and start to detach from all other bands, as the twist angle is lowered. We mark these bands by blue and red color in panel (b), which shows results for decreasing angles from $\Theta=3.16^\circ$ to $2.28^\circ$. The bandwidth of these two energetically-separated groups of bands is summarized in panel (c) of Fig.~\ref{fig:fig1}. We find that the bandwidth of these two bands shrinks drastically as the angle is decreased, yielding band widths of the order of $10$ meV as the angle approaches $\Theta \approx 2^\circ$. Note that these flat bands near the top of the valence bands originate from the states around the $\Gamma$ point in the Brillouin zone of the primitive unit cell of untwisted MoS$_2$, with both S p$_{\rm z}$ and Mo d$_{\rm z^2}$ characters. This is different from the case of twisted WSe$_2$, in which the top valence flat bands originate from the states around the K point in the Brillouin zone of the primitive unit cell \cite{Wang19TMD}. Since in other TMDs, such as MoSe$_2$ and WS$_2$, the top of the valence band in the untwisted bilayer is also located at the $\Gamma$ point in the Brillouin zone \cite{kuc2011,zhang2014direct}, the physics we discussed here transfers also to those materials being twisted.

The upper bands in Fig.~\ref{fig:fig1} (marked in blue) show a Dirac cone at the K point and behave very similar to the bands found for monolayer  graphene (with the exception of a reduced band width). They are spin degenerate in nature, but feature no additional degeneracy except at certain high symmetry points. Instead, the next set of bands (marked in red) is essential to our work. They too feature a Dirac cone at the K point, but also feature two additional ultra-flat bands at the top and bottom in addition to a band structure similar to graphene. The ratio between the width of the ultra-flat and the flat bands decreases as the angle is decreased, but saturates in our calculations as a twist-angle of $\Theta\approx2.28^\circ$ is approached. We attribute this saturation to lattice relaxation effects; note however that the overall band width keeps decreasing.

Remarkably, this second family of flat bands is well-described by an effective p$_{\rm x}$-p$_{\rm y}$ tight-binding model on a honeycomb lattice, depicted schematically in Fig.~\ref{fig:fig2} (a), and conveniently described by the following Hamiltonian:
\begin{equation}
\begin{aligned}
  H_0=&\sum\limits_{\left\langle i,j\right\rangle,s} (t_{\sigma} \mathbf{c}^{\dagger}_{i,s}\cdot\mathbf{n}^{\parallel}_{ij} \mathbf{n}^{\parallel}_{ij}\cdot \mathbf{c}_{j,s}-t_{\pi} \mathbf{c}^{\dagger}_{i,s}\cdot\mathbf{n}^{\perp}_{ij} \mathbf{n}^{\perp}_{ij}\cdot \mathbf{c}_{j,s})\,+ \\
 &\sum\limits_{\left\langle \left\langle i,j\right\rangle\right\rangle,s} (t^{N}_{\sigma} \mathbf{c}^{\dagger}_{i,s}\cdot\mathbf{n}^{\parallel}_{ij} \mathbf{n}^{\parallel}_{ij}\cdot \mathbf{c}_{j,s}-t^{N}_{\pi} \mathbf{c}^{\dagger}_{i,s}\cdot\mathbf{n}^{\perp}_{ij} \mathbf{n}^{\perp}_{ij}\cdot \mathbf{c}_{j,s}),
\end{aligned}\label{eq:pxpy}
\end{equation}
where $\mathbf{c}_{i,s}=(c_{i,{\rm x},s},c_{i,{\rm y},s})^{T}$ with $c_{i,{\rm x}({\rm y}),s}$ annihilating an electron with p$_{{\rm x}({\rm y})}$-orbital at site $i$ and with spin $s=\uparrow,\downarrow$. $\left\langle i,j\right\rangle$ ($\left\langle \left\langle i,j\right\rangle\right\rangle$) denotes (next) nearest neighbors. For each sum in Eq.~{\eqref{eq:pxpy}}, the first term describes the $\sigma$ hopping (head to tail) between the p-orbitals and the second term denotes the $\pi$ hopping (shoulder to shoulder). Furthermore,  $\mathbf{n}^{\parallel}_{ij}=(\mathbf{r}_i-\mathbf{r}_j)/|\mathbf{r}_i-\mathbf{r}_j|$, with $\mathbf{r}_i$ being the position of site $i$ and $\mathbf{n}^{\perp}_{ij}=U\mathbf{n}^{\parallel}_{ij}$ with $U$ being the two-dimensional 90 degree rotation matrix $U=\begin{pmatrix}0&-1\\1&0\end{pmatrix}$.  Finally, $t_{\sigma}$ and $t_{\pi}$ ( $t^N_{\sigma}$ and $t^N_{\pi}$) are the nearest neighbor (next nearest neighbor) hopping amplitudes for the $\sigma$-bonding term and $\pi$-bonding term, respectively. Fig.~\ref{fig:fig2}(b) and (c) depict the corresponding dispersions, density of states, and wave functions in comparison to model predictions, illustrating that the four Moir\'e bands at low energies are well-captured by Eq. (\ref{eq:pxpy}) upon the choice of hopping parameters $t_{\pi} = 0.25 t_{\sigma}$, $t^N_{\sigma}=0.07t_{\sigma}$ and $t^N_{\pi}=-0.04t_{\sigma}$. The density of states exhibits a characteristic four van Hove singularities structure, with two originating from the Dirac bands and two stemming from the additional two ultra-flat bands. The small ratio between the nearest neighbor hopping amplitudes $t_{\pi}/t_{\sigma}$ determines the residual small dispersion in the ultra-flat bands we report. This ratio is controllable by the twist angle, which is summarized in the inset of Fig.~\ref{fig:fig1} (c). All these parameters are related to the interlayer Moir\'e potential and thus expected to be also affected and controllable by the uniaxial pressure perpendicular to the layers as demonstrated for twisted bilayer graphene \cite{Yankowitz18}.

The flat band wavefunctions consist of atomic wavefunctions from the p$_{\rm z}$ orbital on S~atoms and the d$_{\rm z^2}$ orbital on Mo atoms. Modulated by the Moir\'e potential, the weighting of the atomic wavefunctions and their modulus square (i.e., charge density) vary at different atomic sites across the whole supercell, showing distinct patterns for different flat band states at the K point in the supercell Brillouin zone as shown in Panel (c) of Fig.~\ref{fig:fig2}. These patterns of the charge density as well as the real and the imaginary part of the total wavefunctions obtained from DFT show features consistent with those of the p$_{\rm x}$-p$_{\rm y}$ Hamiltonian of Eq.~\eqref{eq:pxpy}. Interestingly, the charge density distribution of the top ultra-flat band state displays a Kagome lattice structure. We have thus unambiguously established twisted MoS$_2$ to be a candidate system to realize a p$_{\rm x}$-p$_{\rm y}$ model on the honeycomb lattice with strongly asymmetric hoppings $t_{\sigma}$ and $t_\pi$, giving rise to a new set of ultra-flat bands.

\begin{figure}
    \centering
    \includegraphics[width=\textwidth]{MoS2_EDplot_2.pdf}
    \caption{\textbf{Charge gap and correlations for twisted bilayer MoS$_2$ at vanishing temperature.} (a) depicts the 16-orbital cluster geometry employed for exact diagonalization of the Hubbard-Kanamori Hamiltonian. (b) depicts the charge gap as a function of Hubbard $U$ and Hund's exchange $J$ interactions, calculated for the 16-orbital cluster and extracted from (c) the local density of states, which is readily accessible via scanning tunnelling microscopy. A well-defined charge gap develops beyond $U/t_\sigma \sim 4$ at small $J$ that scales linearly with the Hubbard interaction $U$. Vertical gray dotted lines indicate phase transitions to charge-ordered states at large $J/U$, coinciding with a closing of the charge gap.}
    \label{fig:ED2}
\end{figure}

\begin{figure}
    \centering
	\includegraphics[width = \columnwidth]{MoS2_phase_diagram.pdf}
    \caption{\captiontitle{Magnetic phase diagram for twisted bilayer MoS$_2$.} (a) Classical ground state energy per orbital in units of $\Delta = t_{\sigma}^{2} / U$, assuming ferro- (blue) or antiferromagnetic (red) order for the spin degrees of freedom. We take the \textit{ab initio} parameters, $t_{\pi} = 0.25 t_{\sigma}$ and use an iterative energy minimization. The lower panel determines the phase boundaries for the orbital degrees of freedom given the energetically more favorable spin order shown in the top panel. At $J/U = 0.1$ we find the spin order to change from AFM to FM, with AFO nematic order for the orbital degrees of freedom remaining stable in agreement with \cite{PhysRevB.100.205131}. (b) Configurations of orbital vectors found at the end of iterative minimization. Note that we display the projection of $\boldsymbol{\tau}$ to the plane in $\mathbb{R}^3$ (indicated by the axis shown in the bottom left), such that nematic states with finite contributions only in $xz$ direction ((1) \& (2)) can be distinguished from magnetic states (3) which point perpendicular, i.e along the $y$-axis.}
    \label{fig:phase_diagram}
\end{figure}

\subsection*{Correlations and magnetic properties}
We now study the role of electronic interactions. As the highly-anisotropic p$_{\rm x}$-p$_{\rm y}$ orbital structure constitutes the essential novelty of twisted bilayer MoS$_2$, we focus on quarter filling where orbital fluctuations can be expected to be crucial. This filling fraction is straightforwardly accessible in experiment via back gating, and we defer a discussion of the half-filled case to the Supplementary Material. To proceed, we assume purely local electronic interactions, which can be generically parameterized in terms of the Hubbard-Kanamori Hamiltonian:
\begin{equation}
    H_U = U \sum_{i, \alpha} n_{i \alpha \uparrow} n_{i \alpha \downarrow}
    + (U - 2J) \sum_{i} n_{i x} n_{i y}
    + J \sum_{i, s, s'} c^{\dagger}_{i x s} c^{\dagger}_{i y s'} c^{\phantom{\dagger}}_{i x s'}  c^{\phantom{\dagger}}_{i y s}
    + J \sum_{i, \alpha \neq \beta} c^{\dagger}_{i \alpha \uparrow} c^{\dagger}_{i \alpha \downarrow} c^{\phantom{\dagger}}_{i \beta \downarrow}  c^{\phantom{\dagger}}_{i \beta \uparrow} \label{eq:HubbardKanamori}
\end{equation}
for two orbitals with rotational symmetry. Furthermore, our DFT calculations suggest $t_{\pi} \approx 0.25 t_{\sigma}$ and only weak next-nearest neighbor hopping at small twist angles; we therefore neglect next-nearest-neighbor hopping in the analysis below.

Fig. \ref{fig:ED2} (c) depicts the local density of states as a function of Hubbard $U$ and Hund's exchange $J$ interactions, calculated via an exact diagonalization study of Eqs. (\ref{eq:pxpy}) and (\ref{eq:HubbardKanamori}) for a cluster depicted schematically in (a). Clear evidence of a charge gap beyond $U/t_\sigma \sim 4$ at small $J$ signifies the onset of a correlated insulator which could be directly observed via transport and scanning tunnelling microscopy. The behavior of the gap is depicted in Fig. \ref{fig:ED2}(b) as a function of $U,J$ and signifies that charge fluctuations are strongly suppressed for large $U$.

In this regime, a natural follow-up questions concerns possible orderings of the orbital and magnetic degrees of freedom. The corresponding strong-coupling Kugel-Khomskii Hamiltonian \cite{tokura2000orbital,corboz2012,khomskii2003orbital} for the p$_{\rm x}$-p$_{\rm y}$ model at quarter filling is given in Ref.~\cite{PhysRevB.90.094422,PhysRevB.98.245103,PhysRevB.100.205131} and reads:
\begin{align}
\label{eq:HSC}
H = \sum_{\langle ij \rangle} & \frac{1}{U - 3J} \xi^{1}_{ij} \left[t_{\sigma} t_{\pi} \bar{Q}_{ij} - (t_{\sigma}^{2} + t_{\pi}^{2}) (P_{ij}^{xy} + P_{ij}^{yx}) \right] \notag \\
- & \frac{1}{U + J} \xi_{ij}^{0} \left[ t_{\sigma} t_{\pi} Q_{ij} + 2 t_{\sigma}^{2} P_{ij}^{xx} + 2 t_{\pi}^{2} P_{ij}^{yy} \right] \notag \\
+ & \frac{1}{U - J} \xi_{ij}^{0} \left[ t_{\sigma} t_{\pi} (Q_{ij} - \bar{Q}_{ij}) - 2 t_{\sigma}^{2} P_{ij}^{xx} - 2 t_{\pi}^{2} P_{ij}^{yy} - (t_{\sigma}^{2} + t_{\pi}^{2}) (P_{ij}^{xy} + P_{ij}^{yx}) \right] \, .
\end{align}
Here, $\xi_{ij}^{1} = 3/4 + \mathbf{S}_i \mathbf{S}_j$ denotes the projector onto triplet states, whereas $\xi_{ij}^{0} = 1/4 - \mathbf{S}_i \mathbf{S}_j$ selects the singlet spin states instead. Note that the orbital operators, for example $Q_{ij}$, are bond dependent, giving rise to a strong spatial anisotropy of the resulting spin-orbit model. Details about their definitions can be found in the Methods section.

To study its ground state phase diagram using the \textit{ab initio} parameters found in the previous section, we employ a mean-field analysis of competing orbital orderings with ferromagnetic and antiferromagnetic spin order. To this end, we note that on the bipartite honeycomb lattice the SU($2$) invariant spin sector would, on its own, order either ferro- or antiferromagnetically, depending on the sign of the exchange couplings. As an Ansatz we therefore assume that one of the respective states is stabilized and decouple the spin from the orbital degrees of freedom by replacing $\mathbf{S}_{i} \mathbf{S}_{j}$ with its expectation value $\langle \mathbf{S}_{i} \mathbf{S}_{j} \rangle = \pm 1/4$ such that $\xi_{ij}^{1} = 1, \xi_{ij}^{0} = 0$ for ferromagnetic spin order and $\xi_{ij}^{1} = \xi_{ij}^{0} = 1/2$ for Ne\'el order.

After such a mean-field decoupling corresponding to the ground state in the spin sector, we analyze the ground states of the resulting Hamiltonian for the orbital degrees of freedom, which we approximate as classical vectors. We use an iterative energy minimization combined with simulated annealing techniques (see Methods) to converge the mean field equations and find the phase diagram summarized in Fig.~\ref{fig:phase_diagram}.
 Panel (a) shows the energy of ferromagnetic and antiferromagnetic spin configurations from which the magnetic phase diagram can be read off. This is given in the upper part of the plot and we find antiferromagnetic ordering with an intermittent ferromagnetic phase at intermediate ratios of $0.1 < J/U < 1/3$.  In the lower part of the plot we show the corresponding subsidiary orbital order. From our simulations we identify three different configurations of orbital vectors $\boldsymbol{\tau}$, which can be classified according to their projection on a single definite plane in  space, shown in the lower left of the plots: (1) ferro-orbital (FO) nematic order, where the vectors on all lattice sites align in parallel to the xz-plane. Quantum mechanically, finite values of $\langle \tau^{x/z}_{i} \rangle$ indicate an imbalance of the occupation of p$_{\rm x}$ and p$_{\rm y}$ orbitals, breaking rotation symmetry and thereby motivating the notion of a nematic state. (2) AFO nematic order; each vector is aligned anti-parallel with its nearest neighbors corresponding to $\langle \tau^{x/z}_{i} \rangle \neq 0$ on each sublattice, but without finite projections $\tau_{i}^{y}$ on individual sites. (3) FO magnetic order; all vectors order along the $y$-axis, such that $\langle \tau^{y}_{i} \rangle \neq 0$, which, in the quantum mechanical system, would indicate time-reversal symmetry breaking.
 The inclusion of quantum fluctuations can change this picture and more exotic ground states may emerge. For example, for our \textit{ab initio} band structure parameters, a noncollinear spin dimer phase is predicted in a certain range of interaction couplings and even a quantum spin-orbital liquid is found in its proximity~\cite{PhysRevB.100.205131}.

\section*{Discussion}
We have established that twisted bilayer MoS$_2$ is a promising platform to realize the orbital anisotropic p$_{\rm x}$-p$_{\rm y}$ Hubbard model by employing large scale {\it ab initio}
calculations. We find that families of flat bands emerge where the first family of flat bands shows s-orbital character and the second family is an intriguing realization of a strongly asymmetric p$_{\rm x}$-p$_{\rm y}$ Hubbard model both on a honeycomb lattice, adding a lattice with non-trivial almost perfectly-flat bands due to destructive interference to the growing list of systems that can be engineered in twisted heterostructures. At even smaller angle the sequence in the family of flat bands found with respect to their orbital character continues and a preliminary study shows
that the next family would exhibit d-orbital character on the honeycomb  lattice. Such a lattice would effectively realize a multi-orbital generalization of a Kagome lattice -- a prototypical model for quantum spin liquids. However, at such small angles strong relaxation is likely to become dominant, prohibiting access to this regime and  potentially spoiling its experimental realization. Currently the {\it ab initio} characterization of such small angles is numerically too exhaustive and this work sparks a direct need for novel computational methods to tackle this question.

Furthermore, our combined exact diagonalization and strong-coupling expansion approaches classify the magnetic and orbital phase diagrams, however, inclusion of quantum fluctuations stipulates an intriguing avenue of future theoretical research.
In addition, by proximity or variations in the chemical composition of the twisted bilayer, it might be possible to induce spin-orbit coupling splitting of the ultra-flat bands at the top and bottom of the asymmetric p$_{\rm x}$-p$_{\rm y}$ dispersion. Such a band gap opening would induce interesting topological properties \cite{PhysRevB.90.075114} in a highly tunable materials setting.

\clearpage

redpajama_set_name: RedPajamaArXiv


The other top women's seeds have fallen by the wayside at the U.S. Open, as have all of the various American flavors of the month. But none of them include two-time defending champ Serena Williams, who has marched past all of them and into the second week in Flushing Meadows.
Every other American woman has lost, and all the other top seeds have been upset. But Williams made sure she didn't end up the same way. She got tested for the first time in this tournament by fellow American Varvara Lepchenko, and aced it with an emotional 6-3, 6-3 fourth-round win.
Williams needed to deal with gusting winds and a game left-hander she just practiced against before the tournament started, but she found a way to fight her way into the round of 16, which suddenly is settling up perfectly for her, the only top-10 seed left in her quarter of the draw.
"I don't know. I've been a casualty this whole year at Grand Slams. I'm just hoping to keep staying in there. So far. Key word, '' said Williams, who wore a pink leopard print that fittingly matched her victory music, "Roar" by Katy Perry.
After seeing No. 2 Simona Halep, No. 3 Petra Kvitova, No. 4 Agnieszka Radwanska, No. 6 Angelique Kerber and No. 8 Ana Ivanovic ousted — and the draw open up like the Grand Canyon — Williams survived and advanced to a date against Kaia Kanepi, against whom she is 3-0.
Only one woman has ever managed three straight titles at Flushing Meadows in the Open era, when Chris Evert ran off four straight from 1975-78. And if Williams plans to three-peat, she will have to play her best tennis of a heretofore-confounding season.
DUE TO THE ASIAN SIZE.You can check the size chart on the left.Make sure that the shoes you choose will fit to your foot before you order.Thank you.


text:
Source: Naruto
Gotta love the Uchiha clan. Kakashi has always been another favorite character of mine from the series and I was very excited when the Kakashi Gaiden was published. I love hearing the backstories to the characters. I had known about Obito from earlier chapters, but when I finally got to actually see him...I just needed to cosplay him. And my friends were cosplaying the rest of the team, Kakashi and Rin.
Obito was kind of a rushed costume and the truth is I made most of the outfit at the convention which happened to be Katsucon 2005. I'm a horrible procrastinator. I pretty much free-drafted most of the costume and was able to finish it up in 2 evenings, and just in time for the Naruto photoshoot. I went with the colors from the artbook, the orange and blue. The anime has Obito colored in an olive green and black and the blue and orange just seemed so much more fitting. Plus, I had the fabric around from making Naruto.
A few accessories were made before the convention. Namely, items that had to be dyed, such as the elastic for the googles/headphones, and the webbed belt and buckle. These items were dyed using RIT dye. The goggles themselves were a pair of child-sized ski goggles. The earphones were made from lids of oval shaped gift box lids that were spray painted silver and a circle cut in the middle with a black fabric covering. Wrist bracers were made from a matching cotton knit fabric and spray painted styrene sheeting plastic was used for the metal protection plates and were attached to the fabric with silver paper brads.
Pretty much everything else on the outfit was re-used from my Sasuke and Naruto cosplays. The leg wraps, holsters, kunai, and shuriken, ninja sandals, and leaf head protector, all were made previously.
Sharingan contacts were ordered from 9mmsfx. They are the "Sasuke" version.
I must say, that I was quite amused when I wore this outfit in 2005. Obito was still rather a new character and hadn't really been seen in the anime yet, so most people kept asking me what version of Sasuke I was cosplaying, since all the Uchihas wear the clan symbol on the back of their outfits.


Women & Infants operates one of the nation's largest single-family room Neonatal Intensive Care Units (NICU), where the latest technology and highly skilled specialists care for babies born prematurely or sick.
The NICU provides comprehensive care through the coordinated efforts of social workers, occupational therapists, nutritionists, respiratory therapists, neonatal nurses, neonatal nurse practitioners, neonatal-perinatal fellows, and attending neonatologists and pediatricians. Practitioners skilled in the care and stabilization of sick newborns are available in-house 24 hours a day. The single-family room model also encourages families to be actively involved in their baby's care.
Each room has a special couch that converts to a bed so parents can spend the night with their baby. On the two-story unit, there is also plenty of space dedicated to families for rest, eating lunch, or making phone calls with status updates. A beautiful family lounge stretches from the first floor to the second in the NICU, featuring a full kitchen, showers for parents, computers, a play area for older siblings, and a mesmerizing salt water fish tank.
Families also find support in the unit's full-time parent advocate, sponsored by a grant from the Rhode Island Parent Information Network, and a March of Dimes' parent advocate.
The Women & Infants NICU is a special place. Nearly 25 percent of babies born here are to high-risk mothers, and 11 percent are premature. Our survival rates for very low birth weight infants are well above national averages.
The newborn nursery service is lead by Dr. Adam Czynski. This service includes a team of pediatricians, pediatric and family practice residents, and medical students from The Warren Alpert Medical School of Brown University. This team of physicians works in concert with the mother-baby nurses, lactation consultants, and other sub-specialty consultants to meet the specific needs of the family and to ensure continuity of care.
Over the last year the newborn nursery service has expanded to include community physicians with specialized interest in the care of the newborns and the supervision of residents to provide pediatric attendings seven days a week. This caring environment is enhanced with the involvement of our dedicated community and voluntary medical staff who partner with us to provide individualized care to our families.


Mangrove Buckeyes live throughout the Florida Keys and along the coastal areas of southern Florida. These buckeyes prefer to fly in open areas near mangroves and salt marshes. Mangrove buckeyes are larger than the Common Buckeyes with a wingspan of 2-2.75 inches.


text:
Q: single dimensional array battleship code I am beginner in java. I was trying to emulate the single dimension array battle ship code from heads first java book. The code is not failing, but I am not able to make it work properly.
Example: [1,2,3] is the array which contains the location of the battle ship. If I guess any number except 1, it is displaying as miss. But if I guess it as 1 three times (length of battleship) in a row I am making it as kill. I am not able to figure out this issue.
Could you please help me out here. The code is posted below:
package battleship;

public class battleship {
    public int[] battleship = new int[3];
    public int numofhits = 0;
    String result = "miss";//instance variables complete

    //setter method to initialize the array which holds the battle ship location
    public void setbattleshiploc(int startpos) {
        int i = 0;
        for(i = 0; i < battleship.length; i++) {
            battleship[i] = startpos + i;
            System.out.println(battleship[i]);
        }
        System.out.println("initialized array is: " + java.util.Arrays.toString(battleship));
    }

    //getter method to print the set battleship array
    public  int[] getbattleshiploc() {
        System.out.println("Battleship array is: " + battleship);
        return battleship;
    }

    //checking whether user guess inside the battleship array location
    public String guessloc(int guessnum) {
        //int i = 0;
        for(int cell : battleship) {
            System.out.println("Guessed number is: " + guessnum + " array element: " + battleship[cell]);
            System.out.println("cell: "+ cell + " ,battleship[cell]: " + battleship[cell] );

            if(cell == guessnum) {
                numofhits++;
                if(numofhits == 3) {
                    result = "kill";
                    return result;
                }//if the hits are 3 then return kill indicating that no more battle ship is available
                else {
                    result = "hit";
                    return result;
                }//end inner else
            }//end outer if

            else {
                //numofhits++;
                result = "miss";
                return result;
            }//end the if-else

        }//end for loop

        return "finished";
    }//end function guessloc

}//end class

package battleship;
import java.util.Scanner;

public class gamelauncher {
public Scanner[] reader;

    public static void main(String[] args) {
        String result = "miss";
        int numofguess = 0;
        //int loopnum = 0;
        battleship launchgame = new battleship();//launch the game
        int startpos = (int) (Math.random() * 5);//generate random number between 0-4
        //int[] location = {startpos, startpos + 1, startpos + 2};//initialize three consecutive array element
        launchgame.setbattleshiploc(startpos);//set the array as the battleship location using setter

        //display the battleship position
        System.out.println("Battle shipt positions are: " +  startpos +" ," + startpos+1 + " ," + startpos+2);
        System.out.println("the battle ship array is: " + launchgame.getbattleshiploc());
        //int[] battleshiplocation = launchgame.getbattleshiploc();
        System.out.println(java.util.Arrays.toString(launchgame.getbattleshiploc()));

        while(result != "kill") {

            Scanner reader = new Scanner(System.in);  // Reading from System.in
            System.out.println("Enter a number: ");
            int guess = reader.nextInt(); //get the user input integer
            //reader.close();//close the scanner
            //loopnum++;

            numofguess++;
            if(guess < 0 || guess > 7) {
                System.out.println("Maximum space available is 7 units(0-6) and battleship length is 3 units, Please provide the location accordingly");
                continue;
            }//close if loop and go to the loop execution if the guess is not within the limits
            else {
                result = launchgame.guessloc(guess);
                System.out.println("response from guessing method: " + result);
                //get the status(hit/miss/kill) back from guess location method

                if(result == "kill") {
                    System.out.println("We have destroyed all the parts of battle ship and it took " + numofguess +" guesses"  );
                    break;//get out of the loop as we have destroyed everything
                }//end kill
                else if(result == "hit") {
                    System.out.println("You have destroyed " + launchgame.numofhits+" parts of batlleship, please continue");
                    continue;
                }
                else {
                    System.out.println("It's a miss dumbo, try again");
                    continue;
                }
            }//end outer else statement
        }//end while loop

    }//end main method

}//end class

A: I can help you by giving you this function a bit changed. Please try to fix the rest of your code on your own. It will give you important experience.
public String guessloc(int guessnum) {
    for(int i=0;i<battleship.length;++i) {
        if(battleship[i] == guessnum) { //it's a hit
            battleship[i] = -1; //you cant hit it again, so change it
            if(++numofhits == 3) {
                return "kill";
            }else
                return "hit";
            }
    }
    return "miss"; //miss should be outside of the for loop
}

A: I believe the problem is that when you are comparing Strings u are using == instead of .equals() so your code should like like this:
if(result.equals("kill"))

redpajama_set_name: RedPajamaStackExchange


text:
Asignatura aprobada és una pel·lícula espanyola de 1987 dirigida per José Luis Garci i escrita pel mateix director al costat d'Horacio Valcárcel. La pel·lícula va ser nominada al premi Oscar i Garci va guanyar el Goya al millor director, en un certamen on tenia una altra nominació a la millor direcció de producció.

Argument
Després del fracàs de la seva última obra i l'abandó de la seva dona, José Manuel Alcántara decideix anar-se de Madrid a Astúries per a viure una vida tranquil·la com a col·laborador de radi i premsa. No obstant això, els seus errors del passat vindran com el seu fill rocker i el seu antic amor.

Repartiment
 Jesús Puente
 Victoria Vera
 Teresa Gimpera
 Eduardo Hoyo
 Pastor Serrador
 Ana Rosa Quintana

Producció
El projecte va néixer d'una conversa amb l'ex futbolista i en aquells dies gerent del Sporting de Gijón José Manuel Fernández García i d'una frase que va escriure a l'hotel de la Reconquista d'Oviedo abans d'anar a lliurar-li el Premi Príncep d'Astúries de les Arts a Luis García Berlanga que deia: "Sempre han sobrat dos dies en la meva vida, dos dies completament inútils, ahir i matí". Garci havia dit que fins que no dimitís o cedís José María Calviño com a director general de RTVE no continuaria fent cinema, i, als pocs dies que ell ho fes, va posar en marxa el projecte.

El rodatge es va dur a terme a Astúries, sobretot a la ciutat de Gijón, entre el 2 de novembre i el 23 de desembre de 1986. La pel·lícula va comptar amb un pressupost de 150 milions de pessetes. L'actriu Encarna Paso no va poder participar pel seu treball en el teatre, i li va donar el paper a Teresa Gimpera.

Palmarès cinematogràfic
Premis Oscar

II Premis Goya

Altres premis
 Premi ADIRCAE a la millor direcció: José Luis Garci.
 Premi ACE (Nova York): Millor actriu secundària: Teresa Gimpera.

Referències

Pel·lícules d'Espanya del 1987
Pel·lícules dramàtiques d'Espanya
Pel·lícules en castellà
Pel·lícules ambientades a Astúries

redpajama_set_name: RedPajamaWikipedia


501(c)(3) nonprofit working with the City of Sutherlin, Oregon, to develop and maintain a community park on the 202-acre Ford's Pond Property.
We recently were awarded a $5,000 grant from the C. Giles Hunt Charitable Foundation, which will be used for trail improvements in 2019.
Join our Monday Walkers! Meet at the Church Rd parking area at 9 a.m. Rain or shine. Dress for the weather and winter, muddy conditions. Updates are posted on our Facebook page.
Our volunteers continue to care for the property by mowing the 1.7-mile perimeter path and the 1-mile hillside loop, in addition to trash pickup and removal. Please keep Ford's Pond clean and carry out all trash and pick up after your pets. We provide pet waste bags for your use at all three entrances.
email friends@fordspond.org for ordering information.
• Build and install way-finding signs and an outdoor bulletin board for visitor safety (employing the talented students in the Sutherlin HS CTE Builds program).
• Demonstrate community support and provide matching funds for our grant applications.
• Allow us to fund a year-round portable toilet at the Church Road parking area.


What's for lunch? Encourage healthy choices with this realistic-looking set of nutritious lunch food that includes 2 slices of wheat bread, 2 slices of turkey, lettuce, tomato, cheese, 4 celery sticks, 2 pretzels, grapes, orange and milk. Great for developing oral language through role play in early childhood and ELL classrooms. Set contains a 10 3/4" x 5 1/4" x 8 1/2" shopping basket and an Activity Guide. All pieces are actual size and washable.


My story starts even before graduating high school. I started early on applying to colleges and was accepted to five different colleges with large scholarships to each one. I knew I wanted to go to Grace Bible College in the fall to be a teacher. That was, until I actually visited the school and realized that I could NOT live there for four to five years. Another college that I had applied to was Valparaiso University, where I had also been offered a huge scholarship that would cover over half of my four years there. Looking into it, I realized that it was a beautiful, Christian school with a great reputation, and I loved the thought of going to school out of state. I had multiple "friends" tell me that Valparaiso was not for me, and I began to think that they were right, so I pushed that school to the back of my mind. I then joined the Teacher Academy program at the Careerline Tech Center and went on a field trip to Grand Valley State University. I liked the school, and applied. I was accepted. I was offered one scholarship a tiny one that would have MAYBE covered my books. More "friends" and a boyfriend at the time encouraged me to go there because it was close to home and would be convenient for them to still see me. I then committed to Grand Valley State University and began the enrollment process.
The closer that it got to being time to head to Allendale and start enrolling, the more wary I became of going to school there. I had declared my major as early childhood education with a minor in Spanish. Did I really want to go here? Was this really what I wanted for myself, or was it what other people wanted for me? Was I really ready to be a teacher for the rest of my career? These thoughts and doubts were constantly on my mind. No one knew what I was thinking, because I kept it all to myself thinking that I would figure it out. When I didn't figure it out, I began to pray about it every night in hopes that God would show me what to do.
I sat down with my mom at the table and told her everything that I had been thinking, and how mission work had always been on my heart. I told her how I had always wanted to go to Haiti and meet Dilano, the Haitian boy from the orphanage that I had been praying for since I was given his picture at age 10. I knew of missionaries in both Haiti and Peru, and I brought it up with my mom. Her answer changed everything for me. "Dana, you're young, you don't have a family to worry about, and if you don't do it, you know you'll regret it". From there, I got started.
To make a really long story not so long, I decided on six months in Peru, and that I would be staying in Cusco, Peru with Albino and Sandy Rodriguez and their three children. Anything I do there is up to me at this point, but I have a safe place to stay. I am beyond excited to see what God has in store for me!


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