text:
Chapter 10: Juvenile Justice
{ "10.01:_Youth_Crime" : "property get [Map MindTouch.Deki.Logic.ExtensionProcessorQueryProvider+<>c__DisplayClass228_0.<PageSubPageProperty>b__1]()", "10.02:_Juvenile_Justice" : "property get [Map MindTouch.Deki.Logic.ExtensionProcessorQueryProvider+<>c__DisplayClass228_0.<PageSubPageProperty>b__1]()", "10.03:_History_of_the_Juvenile_Justice_System" : "property get [Map MindTouch.Deki.Logic.ExtensionProcessorQueryProvider+<>c__DisplayClass228_0.<PageSubPageProperty>b__1]()", "10.04:_Delinquency" : "property get [Map MindTouch.Deki.Logic.ExtensionProcessorQueryProvider+<>c__DisplayClass228_0.<PageSubPageProperty>b__1]()", "10.05:_Juvenile_Justice_Process" : "property get [Map MindTouch.Deki.Logic.ExtensionProcessorQueryProvider+<>c__DisplayClass228_0.<PageSubPageProperty>b__1]()", "10.06:_Due_Process_in_the_Juvenile_Court" : "property get [Map MindTouch.Deki.Logic.ExtensionProcessorQueryProvider+<>c__DisplayClass228_0.<PageSubPageProperty>b__1]()", "10.07:_The_Juvenile_Justice_and_Delinquency_Prevention_Act_of_1974" : "property get [Map MindTouch.Deki.Logic.ExtensionProcessorQueryProvider+<>c__DisplayClass228_0.<PageSubPageProperty>b__1]()", "10.08:_Getting_Tough-_Initiatives_for_Punishment_and_Accountability" : "property get [Map MindTouch.Deki.Logic.ExtensionProcessorQueryProvider+<>c__DisplayClass228_0.<PageSubPageProperty>b__1]()", "10.09:_Returning_to_Rehabilitation_in_the_Contemporary_Juvenile_Justice_System" : "property get [Map MindTouch.Deki.Logic.ExtensionProcessorQueryProvider+<>c__DisplayClass228_0.<PageSubPageProperty>b__1]()", "10.10:_The_Structure_of_the_Juvenile_Justice_System" : "property get [Map MindTouch.Deki.Logic.ExtensionProcessorQueryProvider+<>c__DisplayClass228_0.<PageSubPageProperty>b__1]()", "10.11:_Juvenile_Institutions" : "property get [Map MindTouch.Deki.Logic.ExtensionProcessorQueryProvider+<>c__DisplayClass228_0.<PageSubPageProperty>b__1]()" }
10.3: History of the Juvenile Justice System
https://workforce.libretexts.org/@app/auth/3/login?returnto=https%3A%2F%2Fworkforce.libretexts.org%2FBookshelves%2FCorrections%2FBook%253A_Introduction_to_the_American_Criminal_Justice_System_(Burke_et_al.)%2F10%253A_Juvenile_Justice%2F10.03%253A_History_of_the_Juvenile_Justice_System
parens patriae originated in the 12th century with the King of England and literally means "the father of the country." Applied to juvenile matters, parens patriae means the king is responsible for and in charge of everything involving youth. [1] Parens patriae was often used by royalty in England from their homes in the name of the king. Children were often seen as property and were thus subject to the wishes of the king or his agents. [2] This was especially relevant when they violated the law.
parens patriae had a substantial influence on events in the United States, such as the child-saving movement, houses of refuge, and reform schools. The persistent doctrine of parens patraie can be seen evolving from "king as a father" to a more general ideology, that of the state "acting in the best interest of the child." Subsequent matters involving youth revolve around this notion of acting in the best interest of the child, whether children were taken away from wayward parents, sent to reform schools for vagrancy, or even held in institutions until they read the age of majority, or 18 years old. The idea is that the state is acting in their best interest, protecting the youth from growing up to be ill-prepared members of society. Thus, the courts are intervening for the youth's own good.
house of refuge in New York City in 1825. These were urban establishment used to corral youth who were roaming the street unsupervised or who had been referred by the courts. [4]
parens patriea, many of the parents of these youth were not involved in the placement of their children in these houses. The case of Ex Parte Crouse is an example. [5]
Reform Schools: The 1850s ushered in the development of reform schools or institutions used for the housing of delinquent and dependent children. The schools were structured around a school schedule rather than the work hours that defined the workhouses and houses of refuge. Many reform schools operated like a cottage system where the youth were divided into "families" with cottage parents who oversaw the day to day running of the family, discipline of the youth, and schooling. The structure is still used in some youth correction institutions today, however, back in the nineteenth century, children were often exploited for labor and many of the school de-emphasis formal education. [6] Additionally, the emphasis of the reform school was on the strength of the family and they believed that by reinserting a strong family presence in the lives of the youth, they would be deterred from further criminal pursuits. [7] Regardless of the lack of evaluations as to the effectiveness of these institutions, the popularity of reformatories continued to grow.
parens patriae. However, in 1870, a boy named Daniel Turner was considered a "misfortunate", or someone who was in danger of becoming delinquent because his family was poor and unable to care for him. He was remanded to a Chicago house of refuge for vagrancy, not a delinquent act. His father filed a writ of habeas corpus and the court ruled that the state has no power to imprison a child, who has committed no crime, on the mere allegation that he is " destitute of proper parental care, and is growing up in mendicancy, ignorance, idleness, and vice." [8] People Ex Rel. O'connell v. Turner, 55 Ill. 280 (Ill. 1870). This effectively closed the reform schools in Illinois since they could no longer house non-criminal children. This case challenged the practice of parens patriae and ruled that the state can only take control of children if the parents are completely and utterly unfit and/or the child had committed some act of "gross misconduct." [9]
Child Saving Movement: By the end of the ninetieth century, cities were experiencing the effects of three major things: industrialization, urbanization, and immigration. Industrialization refers to the shift in work from agricultural jobs to more manufacturing work. This led to a greater number of people moving from the country to the cities, and the cities increasing exponentially in population without the infrastructure to support the increase. Immigration refers to the internal migration of people in America and the external movement of people from other countries. Within America, people were moving from the southern states (remember, this is not long after the end of the Civil War, which ended in 1865) and immigrating from European countries such as Ireland (the potato famine lasted from 1845-1854 and killed an estimated 1.5 million people). Millions of Germans and Asians also immigrated to America during this time lured by Midwest farmlands and the California Goldrush. [10]
[11] Nonetheless, the child-saving movement emerged during this time in an effort to change the way the state was dealing with dependent, neglected, and delinquent children. The child savers were women from middle and upper-class backgrounds.
Creation of the Juvenile Court
, Commonwealth v. Fisher Commonwealth v. Fisher, 213 Pennsylvania 48 (1905) , conveyed the legal authority of the new juvenile court under parens patriae:
"To save a child from becoming a criminal, or from continuing in a career of crime, . . . the legislatures surely may provide for the salvation of such a child, if its parents or guardians be unable or unwilling to do so, by bringing it into one of the courts of the state without any process at all, for the purpose of subjecting it to the state's guardianship and protection."
Merlo, A., & Benekos, P. (2019). The Juvenile Justice System, Delinquency, Processing, and the Law (9th ed.) Pearson. ↵
Shoemaker, D. (2018). Juvenile Delinquency (3rd ed.). Rowman & Littlefield. ↵
Merlo, A., & Benekos, P. (2019). The Juvenile Justice System, Delinquency, Processing, and the Law (9th ed.). Pearson. ↵
Merlo, A., & Benekos, P. 2019. The Juvenile Justice System, Delinquency, Processing, and the Law (9th ed.). Pearson. ↵
Ex Parte Crouse (1839) ↵
Mennel, R.M. (1973). Thorns & Thistles: Juvenile Delinquents in the United States from 1825–1940. Hanover, NH: University Press of New England. ↵
People Ex Rel. O'connell v. Turner, 55 Ill. 280 (Ill. 1870). ↵
Fox, S.J. (1970). Juvenile Justice Reform: An Historical Perspective. Stanford Law Review, 22:1187–1239 ↵
History (n.d.). US immigration before 1965. https://www.history.com/topics/u-s-i...on-before-1965 ↵
Feld, B.C. (1999). Bad Kids: Race and the Transformation of the Juvenile Court. New York: Oxford University Press. ↵
Platt, A. (1977). The Child Savers: The Invention of Delinquency (2nd ed., pp.83). Chicago: University of Chicago Press. ↵
This page titled 10.3: History of the Juvenile Justice System is shared under a CC BY-SA 4.0 license and was authored, remixed, and/or curated by Alison S. Burke, David Carter, Brian Fedorek, Tiffany Morey, Lore Rutz-Burri, & Shanell Sanchez (OpenOregon) via source content that was edited to the style and standards of the LibreTexts platform; a detailed edit history is available upon request.
10.2: Juvenile Justice
10.4: Delinquency


Are you looking for a location for your event? Whether business, club or society the Elmbridge Civic Centre may be the perfect venue for your seminar, training day, conference or presentation.
The Civic Centre offers a range of rooms and is conveniently located – easy to get to by road or rail with parking nearby.
All our rooms offer a range of different layouts and full audio and visual equipment including hearing loops, and most have full air conditioning.
Our Council Chamber, the largest room, can seat between 74-146 people while our smaller committee rooms are suitable for events of up to 25 people and feature a full range of facilities – perfect for training, seminars and meetings. These smaller meeting rooms can be joined together to form larger meeting rooms able to host up to 50 people.
We can provide tea, coffee and biscuits or a full buffet service from our on-site caterers. All the rooms have water chillers for drinking water at no charge.
So if you are seeking a venue for your next business seminar, training event or regular business meetings why not contact our room bookings team for more information - email us or call directly on 01372 474169.
We look forward to helping you host your event.


The former UFC Welterweight and Middleweight champion Georges St-Pierre announced his retirement from MMA at a Thursday morning press conference, after failing to get a chance to meet the current Lightweight king Khabib Nurmagomedov in a super-fight.
Many members of the MMA community paid tribute to the retired legend.
But Nick Diaz heavily trashed his old rival Georges St-Pierre.
The two met in the main event of UFC 158, on March 16, 2013, where "GSP" won via unanimous decision.
Few days later, a controversial video was release. UFC official Mike Mersch informed Nick Diaz that despite the weight limit was 170 lbs, it would be tolerated as long as fighters weigh "less than 171 pounds".
On April 11, 2013, Georges St-Pierre admitted to the reporter Marc Tougas of La Presse that he probably weighed around 170.4 pounds for the clash against Nick Diaz.
In May 2018, Nick claimed St-Pierre poisoned him before their UFC 158 fight.
Georges St-Pierre was later appeared on Joe Rogan Experience podcast, where he fired back at Nick's claims. St-Pierre trolled Diaz, describing how he "poisoned Nick Diaz and bribed the athletic commission before their fight".


My Son does not like to wear shoes at all. He is in 1st grade. He wears sock inside out because he does not like to feel the seams of the sock.
Kindly suggest some home management to try with him..
Join in and write your own page! It's easy to do. How? Simply click here to return to Tactile Defensiveness.


text:
9 - 11 October 2019
thai@asiafireworks.com
Who Should Exhibit
Official Electricity
Official Freight Forwarder
Pre Register-As-A-Visitor
Who Should Visit
Pre Register As A Visitor
Map Ta Phut Industrial Complex in Rayong is one of the world's biggest petrochemical hubs
Thailand's Map Ta Phut industrial complex, has grown into one of the world's biggest petrochemicals hubs housing all the main refineries.
Facts of Thailand's Petrochemical Industry
PTT's olefins capacity alone will increase from 1.8mn tonnes per annum (tpa) to 2.8mn tpa and polymer capacity will increase from 500,000 tpa to 1.5mn tpa. Based on current petrochemicals projects, Thailand was set to see new capacities of 1.9mn tpa ethylene, 1.27mn tpa propylene, 1.45mn tpa polyethylene (PE) and 200,000tpa benzene coming onstream by the beginning of 2011, mostly in the Map Ta Phut industrial zone.
Siam Polyethylene Company began operations as its new 350,000tpa solution phase linear low-density polyethylene (LLDPE) train (SPE II). Ube Chemicals Asia also began commercial operations at its new nylon-6 facilities at Map Ta Phut in Q410, with combined capacity of 50,000tpa. Asahi Kasei Chemicals also resumed construction of its 200,000tpa acrylonitrile and 70,000tpa methyl methacrylate plants at Map Ta Phut, which are now likely to begin operation in mid- 2011.
PTT Chemical will also double its high-density polyethylene (HDPE) capacity at Map Ta Phut to 500,000tpa. Also beginning operations in 2011 are the expansion of Integrated Refinery and Petrochemicals Company's (IRPC) acrylonitrile butadiene styrene (ABS) unit from 117,000tpa to 200,000tpa and its increase in capacity at its propylene unit by 100,000tpa to 432,000tpa. – Business Monitor International (BMI)
Some Insights Into Thailand's Oil & Gas Industry
Rayong province is located relatively close to Thailand's offshore gas fields in the Gulf of Thailand and to major gas consuming centres such as Bangkok. This led to Thailand's three major offshore gas pipelines being constructed through the region. Partly as a result, the province, and particularly the Map Ta Phut industrial complex, has grown into one of the world's biggest petrochemicals hubs. Construction work began on gas separation plants there in the 1980s as a way of producing fuels that could replace crude oil imports. PTT completed its first 4bn cubic metre (bcm) gas separation unit in Rayong province in 1984 in order to provide feedstock for nearby petrochemicals plants and liquefied petroleum gas (LPG) for households. The next three separation units, completed between 1991 and 1996, were designed to cope with rapidly increasing demand for LPG and have a combined capacity of 9.4bcm. A fifth unit, significantly larger than the earlier units at 5.5bcm, was added in 2005 to provide additional ethane, propane and LPG for the petrochemicals industry. Since the first five separation plants came onstream, however, rising demand for feedstock from petrochemical works and residential customers has put pressure on the existing infrastructure. As a solution, PTT started work on an ethane separation plant to improve production at units two and three, and began building a sixth gas separation plant with a capacity of 8.3bcm
Fireworks Exhibitions and Conferences which have organized successful international Oil & Gas events such as Oil & Gas Brunei (OGAB), Oil & Gas Thailand (OGET) and Oil and Gas Vietnam (OGAV) is the organizer of this premier Oil and Gas event.

redpajama_set_name: RedPajamaCommonCrawl


text:
Writer blazed trail for disabled
Dale Carruthers
Jun 09, 2017 • Last Updated June 9, 2017 • 2 minute read
Marilyn (Lynne) Swanson gave each of the hand-painted canes in her extensive collection a special name.
There was Ruby, Blaze, Posey.
All of Swanson's nearly 20 canes were colourful and unique.
"When she first had to use a cane, she was so opposed to it, she thought 'How can I change this around?' " said longtime friend Deb Caldwell.
"And what she did is commission artists to paint the canes to go with certain outfits."
A longtime disability advocate and Free Press columnist, Swanson died Wednesday at age 66. She had been in the hospital for two weeks following a series of seizures.
Like her stylish canes, Swanson was colourful and unique, say those who knew her.
She was born in January, but often threw her birthday party in May or June when the weather was nicer.
"She loved being the centre of attention and she made no apology of that," said Caldwell, who first met Swanson working at the Ministry of Community and Social Services office in London in the 1970s.
Swanson's life changed forever on a Sunday morning in 1984 when she felt a slight pain behind her eye. Left blind in that eye for three months, Swanson was diagnosed with multiple sclerosis, an autoimmune disease of the central nervous system.
After living with the disease for 10 years, she started writing a monthly column for The Free Press chronicling the experiences of individuals living with disabilities in Southwestern Ontario.
"I think you'll find some special and interesting people in this column — folks who live life with zest and enthusiasm, while coping with the challenges presented by disabilities," she wrote in her first PosAbilities column published Jan. 17, 1994.
Rather than just focusing on problems, Swanson's writings highlighted individuals with disabilities making a difference in their communities and brought attention to the agencies dedicated to assisting them.
Jeff Preston, an assistant professor at King's University College, remembers reading Swanson's column growing up.
"Being able to see people like me represented in the media was actually significant when I was a kid," said Preston, a disability rights advocate who uses an electric wheelchair.
"So often when I watched television or movies as a child, you'd see these characters with disabilities, but they were so wrong. They didn't represent my experience."
Calling Swanson a trailblazer, Preston said her columns shone a light on people living with disabilities — individuals with careers, families and aspirations — that he and others could better relate to, showing them to be more than their physical limitations.
Swanson enjoyed a successful career, working for Fanshawe College as the affirmative action co-ordinator and later in human resources at the Child and Parent Resource Institute, before MS began to rob her of her mobility in recent years.
A celebration of her life is being held 11 a.m. Saturday at St. Luke's-in-the-Garden Chapel at 600 Sanatorium Rd.
dcarruthers@postmedia.com
twitter.com/DaleatLFPress


text:
Downtown Dining
Cary Parks
Weekend: Theater, Music & Raleigh Home Show
February 17, 2016 /in Events, Featured /by Staff
Cary, NC — We counted seven cultural arts performances on the Cary calendar this weekend and also found some great events across the Triangle – like the Downtown Raleigh Home Show and Revolutionary War reenactments in Hillsborough.
Join WordsWorking, a local resource, for an interactive workshop that will help you overcome your fear of public speaking at the Apex Chamber of Commerce on Friday morning from 8:30 – 11:30 am. You'll learn how to introduce yourself to others in a networking situation and be prepared to present yourself and your business in a professional manner, no matter what the situation. Register online, because space is limited. $35 fee includes refreshments and all materials.
It's Improv Night in the Cary High School auditorium. The show starts at 7 pm, and the admission price is just $2.
The Cary Players will present their romantic comedy theater production, Crossing Delancey, at The Cary Theater on Friday, Saturday and Sunday. This is the last weekend to catch the show. Find the show schedule and tickets ($20) online.
Another performance starts at 7:30 pm at the Cary Arts Center – it's a free show from the Cary Town Band called For All The Seasons. You'll hear Strauss' "Voices of Spring," Gershwin's "Summertime," King's "Autumn Flowers" and more.
More Friday details on the calendar.
While Crossing Delancey is going on at The Cary, the Presidio Brass Band will perform down the road at the Cary Arts Center. Tickets for this 7:30 pm show, which includes a five-piece band that presents music made famous in films, are $26.
More Saturday details on the calendar.
Make a Fairy Garden at Garden Supply Company in Cary on Sunday at 2 pm. The $25 class fee includes instruction and basic building materials, but the purchase of plants, accessories and container (unless you bring your own) are extra.
Then, catch a Sunday afternoon show at the Page-Walker Arts & History Center at 4 pm as Brian Reagin, violinist and Concertmaster of the NC Symphony, returns to Cary as a favorite. Reagin, who captivates audiences with his brilliant performances, will treat concert-goers to a classical repertoire on his Lorenzo and Tomasso Carcassi violin made in Florence, Italy in 1763. Refreshments will be served at intermission, and tickets are $16.50 a performance. on etix.
More Sunday details on the calendar.
Across the Triangle
The Downtown Raleigh Home Show returns to the Raleigh Convention Center Friday, February 19, 2016 – Sunday, February 21, 2016. The huge building will be packed-full with inspiration and experts for both indoor and outdoor home design and functionality, while a kids zone keeps little ones occupied. Find tickets and times online.
To celebrate Black History Month, Historic Stagville and Morehead Planetarium will present Stagville Under the Stars on Friday, February 19, 2016 at 6 pm that focuses on the astronomy and night sky myths and legends told in African cultures as well as the related stories told by scientists today. The free program will begin with storytelling and after that, guests will peer through telescopes for a constellation tour looking at the same stars as our ancestors.
The 16th annual Revolutionary War Living History Day is Saturday, February 20, 2016 in historic Hillsborough. At this family-friendly event, the public can experience the local history of the American Revolutionary War with live actors, dancers, historic tours, and interactive activities from 10 am – 4: 30 pm.
The calendar of events is edited by Jessica Patrick. Photo by The Cary Players.
Tags: Events, Weekend
https://carycitizenarchive.com/wp-content/uploads/2016/02/Delancey.jpg 347 800 Staff https://carycitizenarchive.com/wp-content/uploads/2020/03/cc-archive-logo-450-v3.png Staff2016-02-17 14:03:072016-02-17 09:00:21Weekend: Theater, Music & Raleigh Home Show
Latest Cary News
For the latest Cary news, visit:
CaryCitizen.News
Cary Chamber (61)
HoCA (16)
Faiths (51)
Go Local (102)
Morrisville (45)
Ashley's Journal (3)
Don's Blog (61)
Editors Journal (40)
Harold's Blog (461)
Lori's Blog (48)
Op Ed (39)
Samaritan's Corner (24)
Vox Populi (49)
Scavenger Hunt (44)
Shop & Dine (85)
Canes (290)
North Carolina Courage (46)
North Carolina FC (60)
RailHawks (67)
©2009-2021 CaryCitizen. All rights reserved. A publication of Goodtree.Studio
Entrepreneurship Olympics – Skills for Young Adults Canes Dominate Jets in 2-1 Win


Did I say the world was fair?
General CommentThis song wins the award for best use of subtraction in music.
General CommentHah! I absolutely adore this song. It came on while me and my boyfriend were kissing, he stops and says how much he loves this song, and starts singing it.
It's an amazing song, good vocals, good story, and yeah it's a gay love song! I'm really glad that you can't sit there and try to say it isn't.
General CommentThis song is best listened to when you're having a total adrenaline rush. This is my "badass" song.
General CommentNothing to interpret about this song, but it's a beautiful song even to a straight guy like me.
General CommentI like this song because it is straightforwardly a "gay song," and yet anyone can enjoy listening to it and can sympathize.
General Commenti love love love the piano in the beginning.
General CommentAm I right in thinking "I wanted you tonight" and everything after it is not in the version on i? It doesn't sound familiar.
I love this song. I always sing the "love or not" part over and over.
General Commentp.s. I also love songs that can't be explained away as "well... maybe he was writing from a female perspective."
We do not have any tags for I Thought You Were My Boyfriend lyrics. Why not add your own?


text:
Жилой дом А. Н. Бибихина — памятник градостроительства и архитектуры в историческом центре Нижнего Новгорода. Построен в 1876 году, по проекту архитектора Н. К. Кострюкова.

Дом имеет важное градостроительное значение, так как вместе с другими зданиями на улицах Короленко, Студёной, Славянской и Новой образует цельный архитектурный ансамбль исторической застройки второй половины XIX — начала XX веков — достопримечательное место «Район улиц Короленко, Славянской, Новой».

История
Дом расположен на южной окраине исторического центра Нижнего Новгорода. С конца XVIII века по 1824 год на данной территории располагались канатные заводы. В 1839 году новым генеральным планом территория была включена в городскую, что привело к формированию на этом месте нового большого жилого района, планировку которого разработали архитектор И. Е. Ефимов и инженер П. Д. Готман в 1836—1839 годах. В ходе планировки была проложена улица Канатная (с 1928 года — Короленко).

В 1876 году, на стыке улиц Немецкой и Канатной, на участке, принадлежавшем мещанину Александру Николаевичу Бибихину, был построен деревянный жилой дом и ещё два деревянных одноэтажных строения — хозяйственные службы и баня с брандмауэрными стенами по южной границе с соседним владением. Проекты дома и надворных строений, разработанные архитектором Н. К. Кострюковым, утверждены 28 октября 1876 года.

В 1884—1887 годах домовладение принадлежало нижегородскому мещанину Павлу Александровичу Бибихину. В 1905 году перешло во владение мещанки Афанасии Васильевны Бибихиной, за которой числилось до 1918 года.

В советский период к дому были сделаны две пристройки холодных сеней, снесены надворные строения. В 2018 году главный архитектор Научно-исследовательского предприятия «Этнос» И. С. Агафонова и юрист М. И. Чуфарина подали заявление о включении дома в единый государственный реестр объектов культурного наследия. Приказом Управления государственной охраны объектов культурного наследия здание было включено в перечень выявленных объектов культурного наследия. В 2020 году новым приказом Управления государственной охраны объектов культурного наследия Нижегородской области был признан объектом культурного наследия регионального значения.

Архитектура
Памятник архитектуры является образцом небольшого деревянного жилого дома второй половины XIX века. В основе объёмно-пространственного решения лежит классицистическая композиция трёхоконного дома с треугольным фронтоном, взятая из образцовых проектов начала XIX века, усложнённая пристроем обширных боковых сеней, также завершённых фронтоном. В архитектуре фасадов сочетаются мотивы классицистической архитектуры в виде наличников с сандриками, филенчатых лопаток и венчающего карниза, выполненных в стилистике эклектики, и элементы, характерные для крестьянской архитектуры, в виде оконных ставен.

См. также
 Деревянная архитектура Нижнего Новгорода

Примечания

Литература

Архитектурные памятники Нижнего Новгорода
Деревянные жилые здания России
Здания и сооружения Нижнего Новгорода в стиле академической эклектики

redpajama_set_name: RedPajamaWikipedia


text:
Q: How can I calculate sub-aggregates with azure search? In azure search I have documents with the following format which comes from IoT realm:
device identifier: string
event_level: int

I'd like to facet(group) the count by device identifier and  event level together.  I can do basic facet at each individual level, but can't figure out multiple fields.  Basically I'm looking for a count of the different event_level per device_identifier.  So result would be
device_identifier 1 - event_level 2 - count 100
device_identifier 1 - event_level 1 - count 00
...

Any help would be appreciated.

A: You can combine device_identifier and event_level into a single field and facet on that. However, be aware that faceting on fields with high cardinality can be slow.

redpajama_set_name: RedPajamaStackExchange


The most notable difference between Bitosy and other similar investment decisions is a deposit which actually earns you PROFIT! If you invest any amount that is above $10 Perfectmoney, Payeer, AdvCash, Payza or Bitcoin you will make money every day, until the deposit expires in 12 days. We promise that your profit Accruals can't be stopped for even a minute and are from 12% to 18% depending on chosen plan.


Smoking Cessation, Weight Loss, Anger Management, Anxiety, Blushing, Depression, Drug & Alcohol Abuse, Eating Disorders, Exam Nerves, Fear of Flying, Gambling, Internet Addiction, Low self Confidence and Esteem, Obsessions and Compulsions, Pain Management, Phobias (various), Public Speaking, PTSI (Post Traumatic Stress Injury), Relationship Issues, Sports Performance, Stress, Post Natal Depression, Bi-Polar, Relaxation, Historic Child abuse, the list is endless.
There are a variety of reasons why we get different states over our lives. When we consider that we are initially born with a blank canvas, and from that point we learn pretty much everything, also known as "learned behaviour." We pick things up both consciously and subconsciously. The amazing thing about our brains is that it has the opportunity to "unlearn" too.
With the ability to unlearn then, Steve can facilitate the processes, with the intention to bring about the change(s) clients are hoping to attain.
Copyright northease.co. All rights reserved.


text:
'Today' show cast recreates Coldplay video for Super Bowl XLIX ad
https://admeter.usatoday.com/2015/01/20/today-show-cast-matt-lauer-al-roker-hoda-kotb-super-bowl/
The Today show's Facebook page
It's not a beer, a soft drink, or a flashy car, but the Today show is joining the Super Bowl commercial party. Adweek reports that the cast of the long-running morning program — which like Super Bowl XLIX is an NBC property — is the focus of a big game spot. Matt Lauer, Savannah Guthrie, Al Roker, Natalie Morales, Hoda Kotb, Carson Daly, and Willie Geist appear in the ad, which is a re-creation of Coldplay's popular "A Sky Full of Stars" video:
The commercial, directed by Mat Whitecross, was a collaborative effort. The show invited viewers to participate in the filming, which seemed to go swimmingly. Adweek explains:
At one point, Guthrie, Roker and Morales ended a scene in a dance party with members of the public. Later, someone offered Roker a slice of pizza, which he gladly gobbled down. It became clear later that it was not staged when that person never appeared again in subsequent shots. Not everything was usable: Mixed in with the excited expressions were puzzled onlookers and genuinely annoyed New Yorkers who were upset someone was blocking the sidewalk. Still, Whitecross said that fit in with his vision for the video. Though they hired extras and played music so the journalists would have something to react to, he wanted to leave room for things to organically occur.
Sounds fun. For more photos of the shoot, visit the Today show's Facebook page.


text:
Home / ETNT Health / If You Feel This, You May Have COVID Now
If You Feel This, You May Have COVID Now
The five most common symptoms of COVID-19 seem to be changing, researchers say.
By Michael Martin
Published on November 25, 2021 | 7:45 AM
FACT CHECKED BY Alek Korab
Winter, and the cold weather, meant a huge surge of COVID cases last year. This year, despite the vaccines, it's happening again. Hospitalizations are also going up, as vaccine immunity wanes and more people go indoors. But certain symptoms are also more likely if you come down with COVID-19 now, according to the COVID Symptom Study. Researchers have been tracking symptoms reported with new COVID cases via an app, and these are the five they say are most common as of this summer. "There are a few reasons why symptoms may be changing, including the fact that those who have been vaccinated experience less severe symptoms, as well as more cases being reported by younger people, who we have found experience different, less severe symptoms as well," say the researchers. Read on to find out what they are—and to ensure your health and the health of others, don't miss these Sure Signs You've Already Had COVID.
The researchers are tracking COVID cases that occur in people who are unvaccinated, along with people who've been fully vaccinated and those who've had one vaccine dose. "As we have found, even people who have had one or two doses of the vaccination can still be susceptible to contracting COVID, and the symptoms and severity differ depending on how many vaccinations you've had, if any," they wrote. But not headache, which was the #1 symptom reported among all three groups.
A runny nose was the #2 most reported symptom by fully vaccinated and partially vaccinated people, and the #3 most common symptom in the unvaccinated. Interestingly, earlier in the pandemic, a runny nose was thought to be unrelated to coronavirus infection.
At the same time, the researchers say that an early telltale sign of COVID—loss of smell—seems to have become less common as the virus has evolved. It ranked #9 among the unvaccinated and only made the top 5 (at #5) in people who were fully vaccinated.
A sore throat was the #4 most reported symptom among the fully vaccinated, #3 among the partially vaccinated, and #2 among the unvaccinated.
RELATED: Over 60? Stop Doing This ASAP, Say Experts
Sneezing was the #3 most reported COVID symptom among the fully vaccinated and #4 in the partially vaccinated group. "Curiously, we noticed that people who had been vaccinated and then tested positive for COVID-19 were more likely to report sneezing as a symptom compared with those without a jab," the researchers say. "If you've been vaccinated and start sneezing a lot without an explanation, you should get a COVID test, especially if you are living or working around people who are at greater risk from the disease."6254a4d1642c605c54bf1cab17d50f1e
RELATED: Here's When COVID Will End, Predict Experts
Persistent Cough
A persistent cough was the fifth-most-reported symptom among the unvaccinated and partially vaccinated. But it only ranked #8 among the fully vaccinated—possible evidence that another previous hallmark symptom is becoming less common. Also sliding down the list: Shortness of breath and fever, which are much less frequently reported now than in the pandemic's first waves, the researchers say. Now to get through this pandemic at your healthiest, don't miss these 35 Places You're Most Likely to Catch COVID.
Michael Martin is a New York City-based writer and editor. Read more about Michael
Coronavirus // Coronavirus Symptoms // News


Cat S30 supports frequency bands GSM , HSPA , LTE. Official announcement date is September 2015. The device is working on an Android OS, v5.1 (Lollipop) with a Quad-core 1.1 GHz Cortex-A7 processor and 1 GB RAM memory. Cat S30 has 8 GB of internal memory. This device has a Qualcomm MSM8909 Snapdragon 210 chipset. The main screen size is 4.5 inches with 480 x 854 pixels resolution. It has a 218 ppi pixel density. The screen covers about 54.1% of the device's body. The result is quite good.
We do our best to make the model description as accurate and reliable as possible, unfortunately you may find a mistake in our Cat S30 specs. Please contact us if something is wrong.


text:
Best Alternatives For Expensive MacBook Pro: Dell XPS 13, HP Spectre x360, Dell XPS 13 2 In 1
By JR O. , Jan 18, 2017 05:47 AM EST
The new MacBook Pro laptops are great laptops. However, when the money factor comes into the picture, the MacBook Pro's value may arguably be not worth it. If you're one of the people who are very meticulous in buying products that are worth every penny, here are some MacBook Pro alternatives for you.
Dell XPS 13
The Dell XPS 13 starts at $799.99 for the Core i3 version but if you want the 7th-gen Core i5 version you can get it for $999.99. These prices are for the non-touch versions so if you want a touch-enabled Dell XPS 13, you can get the Core i5 version for $1299 or the Core i7 version for $1599. Note that the non-touch models come with 128 GB storage while the touch-enabled versions come with 256 GB storage. Check on Dell's site for the specifics but as a whole, the Dell XPS 13 series is a pretty serious contender for all the laptops in the current market.
Dell XPS 13 2 In 1
The Dell XPS 13 series has recently been refreshed with 2 in 1 models. You can get the 7th-gen Core i5 2 in 1 model from $999.99 and the Core i7 version for a starting price of $1299. The Dell XPS 13 2 In 1 is quite a competition to the MacBook Pro 2016 for the sole reason that it is a 2 in 1 device and at the same time, it is also equipped with superb internals.
The HP Spectre x360 is yet another amazing laptop from 2016. It's got a stunning look, a slim body, and top notch internals. Right now, its most recommended model is only priced at $1449 and it already offers a powerful Core i7 processor. Just like what its name suggests, the HP Spectre x360 also gives you a 360 degree of positioning system making your laptop experience more fun and more convenient.
With MacBook Pro 2016's high prices, not everyone is willing to splurge on it even if they'd want to. Although the MacOS system is quite a popular option, spending $1499 for a regular MacBook without the Touch Bar may not be an easy decision to make. Considering that you can get a fully convertible laptop with a touchscreen for lower prices, the new MacBook Pros aren't exactly your only options. Know that the 13 inch MacBook with Touch Bar is priced at $1799 and the 15-inch version is priced at $2399, as per Tech Radar. Nevertheless, the new Apple laptops are powerful devices. They're just not too affordable for other people to choose.
TAG MacBook Pro 2016, h spectre x360 specs, hp spectre x360 price, Dell XPS 13, dell xps 13 price, dell xps 13 specs, dell xps 13 2 in 1, dell xps 13 2 in 1 price
Surface Book vs MacBook Air vs Dell XPS 13 vs HP Spectre x360 13t: Specs Shootout Of Thin Laptops
Microsoft, Apple, Dell, and HP are four of the biggest competing high-end laptops pushing innovative features and specs.
Microsoft Surface Laptop: Does It Stand A Chance Against The 2016 MacBook Pro?
The new Microsoft Surface Laptop is as good a traditional laptop as they come.
Make Your MacBook Pro's Touch Bar More Useful With This Support
One of the many supports of the MacBook Pro's Touch Bar is its Spotify integration. Today, Evernote has also entered the Touch Bar fray and it is the best example to show how users can use the feature properly.
Dell XPS 13 2-in-1: How It Stacks Up Against Its Laptop Counterpart
The Dell XPS 13 2-in-1 is a sleek but rather expensive hybrid version of the popular XPS 13 clamshell.
MacBook Pro's Touch Bar Is Now Live For Microsoft Office
The Microsoft Office is now optimized for MacBook Pro with Touch Bar usage.
You Can Now Add A $25 Fingerprint Sensor For Dell's XPS 13 And 15 Laptops
It looks like Dell has also added a new feature which is the fingerprint reader option for the new XPS 13 (9360) as well. Like the XPS 15, the option can be added to any configuration for only $25.


How I love to think about the beach. Whether it is in the middle of a Colorado winter, or the middle of the summer, I find great peace thinking of the rolling waves, gentle breezes, salty aroma, and warm sand of a beach. Many therapists refer to this as a safe place, but I prefer to think of it as a peaceful place. Either way, it's a wonderful reprieve during a stressful time in life. I often tell clients who are struggling with anxiety, stress or trauma to think of their peaceful place when they have an onset of anxious or stressful symptoms. I tell them to imagine the sights and sounds, smells and feelings of their place. I encourage them to breathe deeply, enjoy the sights and sounds, relax and spend a few minutes there. Doing so can lower heart rate, decrease cortisol levels and increase endorphins, all of which improve the way one feels. As I consider my next vacation- literally or figuratively, I invite you to consider yours. Where is your peaceful place?


Thread: How To BBQ Your PB Trout...! ! !
know how to BBQ a PB trout.
Next, lay out all of your ingredients.
Two Limes sliced into wedges, three cloves garlic sliced, olive oil, sea salt and fresh ground pepper.
Fill inside of fish with lime wedges and garlic slices.
Add olive oil , inside and out, so salt and pepper stick onto fish. Salt fish inside and out, add fresh ground pepper.
Now wrap your fish in foil, making sure that there are no holes.
Next, open a few beers and use left over lime wedges.
The BBQ should be heated to between 275-325 degrees.
10 flip...10 flip...10 flip...10 flip.. 5 flip...5 flip....done.
Carefully remove the fish from BBQ, on cookie sheet.
I sliced the fish at the head, middle and tail. And used a spatula to remove the meat.
Once you have the meat off of one side, you can cut through the bones at the head and lift out all of the bones.
Rice... (Boiled in chicken broth,with sauteed garlic, with fresh tyme, chives, salt & pepper.
Best trout I've ever had.
I hope you try it out and enjoy..
Thanks for the recipe that trout looks like it has pink meat yummy.
I may have a couple of those Baja's in the ol' cooler too!
I am not sure if Sue should even handle a dull spatula just yet.
Thanks for the recipe and nice post.
What, no wall mount? It's a good thing you scaled it first, they taste better that way. Steamed in their own slime would not make a very good sales pitch. Glad you got to eat that thing.
That sure looks good!!! I have a similar recipe. It was a big hit at our Mother's Day BBQ.


text:
Food Challenges
Current PhD Opportunities
Demonstration Farms
Collaborating Researchers
Growers and Suppliers
The fate of plastic use in agriculture: the state of agricultural soils
You Shall Not Pass: Using Mesh to Limit SWD Damage
Living on the Sedge
FruitWatch: Monitoring Fruit Tree Flowering Dates
The History of The Humble Potato
Chris Wyver on FruitWatch: Monitoring Fruit Tree Flowering Dates
Dr Bernard Mooney on FruitWatch: Monitoring Fruit Tree Flowering Dates
Waitrose Collaborative Training Partnership
Waitrose working to encourage sustainable food production
Speed breeding technique sows seeds of new green revolution
Pioneering new technology is set to accelerate the global quest for crop improvement in a development which echoes the Green Revolution of the post war period. The speed-breeding platform developed by teams at the John Innes Centre, University of Queensland and University of Sydney, uses a glasshouse or an artificial environment with enhanced lighting to […]
December 24, 2017 Gordon Chapman-Fox Press release Allan Rattey, Brande Wulff, crop breeding, Dow AgroSciences, john innes centre, Lee Hickey, Nature Plants, plant breeding, plant science, RAGT Seeds, Ruth Bryant, speed bredding, university of queensland, university of sydney
Young Plant Scientist accolade for Dundee-based researcher
A PhD student at the University of Dundee and James Hutton Institute has been selected as Young Plant Scientist 2018 in the fundamental research category by the European Plant Science Organisation (EPSO). Shumei Wang, based at the Institute's Cell and Molecular Sciences group, has discovered a new pathway involved in infection by Phytophthora infestans, the pathogen responsible for […]
December 23, 2017 Gordon Chapman-Fox Press release EPSO, European Plant Science Organisation, James Hutton Institute, John Jones, Paul Birch, phytophthora infestans, Scotland, Shumei Wang, University of Dundee, young plant scientist of the year
New plant protection product approved for use in record time
UK herb growers will be able to protect their crops with a new weed control product in record time, following successful trials as part of AHDB's £1.4m crop protection project. To achieve this approval so quickly, the team used intelligence from other EU countries, collaborating closely with other manufacturers and growers, to ensure trials on […]
December 22, 2017 Gordon Chapman-Fox Press release AHDB, Angela Huckle, arysta, Bollette Palle Neve, brassicas, British Herbs, Centurion Max, Chemical Regulations Division, Claire Donkin, clethodim, crop protection, Don Pendergrast, Health and Safety Executive, herbs, Joe Martin, SCEPTREplus
Pregnancy test science could protect the Christmas sprout
The science behind the home-pregnancy test is now being trialled to detect the presence of diseases, which can devastate fields of vegetable crops, including the Christmas sprout. Trials are underway to help protect crops of Brassicas – sprouts, broccoli, cabbage – and onions, which generated more than £356 million for UK agriculture last year. Diseases […]
December 21, 2017 Gordon Chapman-Fox Press release agronomy, AHDB, Allium and Brassica Centre, brassicas, brussels sprouts, Carl Sharp, Cathryn Lambourne, crop protection, diagnostic test, Euan Alexander, Kettle Produce, lateral flow device, LFD, Mologic Ltd, oomycetes, pathogens, pests, Phytophthora, Pythium, stockbridge technology centre, University of Worcester, Warwickshire College
Double dose for bees
In a paper published today in the Proceedings of the Royal Society B: Biological Sciences, a team of researchers from Italy and the US record their study of the effects on honey bees of agriculture that exposes the insects to both poor nutrition (low quality nectar) and pesticides (neonicotinoids). "Our results provide the first demonstration that […]
December 20, 2017 Gordon Chapman-Fox Press release bees, crop protection, neonicotinoids, neonics, pesticide, proceedings of the royal society b, rothamsted research
Why I am excited about this Collaborative Training Partnership?
By Carly Stevens There are lots of reasons why we enter our chosen professions but for a lot of scientists working within the field of environmental science a big motivator is that we want to 'make a difference'. We know that we aren't going to single handily save the planet but we would like to […]
December 19, 2017 Gordon Chapman-Fox Training News
Agriculture needs a champion
Research investment in the life sciences has focused too much on medicine and biomedicine at the expense of agriculture and biotechnology more generally, acknowledges Sir Paul Nurse, Chief Executive & Director of the Francis Crick Institute, a biomedical research centre in London. "One has only to take a short trip in this country to see […]
December 18, 2017 Gordon Chapman-Fox Press release agriculture, Conference, Francis Crick Institute, Greg Clark, rothamsted research, Secretary of State for Business Energy and Industry Strategy, seminar, Sir Paul Nurse, speech, YouTube
The illegal wild orchid trade
Large-scale commercial trade of wild orchids is a pressing, but little-recognised conservation problem, according to researchers. Orchids are one of the largest families of flower plants in the world, and – on paper – they are among the most well protected. From edible orchid cake in Tanzania and ornamental orchids in Thailand and Brazil, to […]
December 14, 2017 Gordon Chapman-Fox Press release Botanical Journal of the Linnean Society, CITES, conservation, Dr Amy Hinsley, Dr Jacob Phelps, endangered species, flowers, lancaster university, National Geographic, orchids, protected species, species, University of Oxford, wild flowers
Warmer Arctic is the 'new normal'
A warming, rapidly changing Arctic is the "new normal" and shows no signs of returning to the reliably frozen region of the past. This is according to the US National Oceanic and Atmospheric Administration's Arctic Report Card. Read more at BBC.co.uk
December 13, 2017 Gordon Chapman-Fox Press clippings
Pesticide dust danger in Pakistan
Residents and workers in a major Pakistan city are exposed to harmful levels of pesticides, new research reveals. Scientists from Pakistan's F Quaid-i-Azam University and Lancaster University have evaluated the organophosphate pesticide concentration in dust from farms and also from pesticide manufacturing plants in the megacity of Lahore.
December 6, 2017 Gordon Chapman-Fox Press release Andrew Sweetman, Crispin Halsall, environmental toxicology and pharmacology, F Quaid-i-Asam University, Kevin Jones, lancaster university, pakistan, pesticides, Riffat Naseem Malik, Sidra Waheed
©2019 LANCASTER UNIVERSITY


text:
Oct 2nd
Posted in vzmgyuwk
Tagged Best, Ching, Deidre, Duarte, Georgia, Kavon, Odalys, Ranbir, Troi, Ulysses
We are all at risk when humanitys values are abandoned UN honours
Mr. Guterres recalled that the International Day, marked annually on 27 January, was created to honour the memory of six million Jewish men, women and children that perished in the Holocaust and countless others lost their lives as cruelty convulsed the world. Yet, decades since the Second World War, there is still the persistence of anti Semitism and an increase in other forms of prejudice. Citing Neo-Nazis and white supremacy groups as among the main purveyors of extreme hatred, the UN chief said that too often, vile views are moving from the margins to the mainstream of societies and politics. "Whenever and wherever humanity's values are abandoned, we are all at risk," stressed the Secretary-General. "All of us have a responsibility to quickly, clearly and decisively resist racism and violence," he stated, adding: "Through education and understanding, we can build a future of dignity, human rights and peaceful coexistence for all."VIDEO: Message by Secretary-General António Guterres on the International Day of Commemoration in Memory of the Victims of the Holocaust. For his part, UN High Commissioner for Human Rights Zeid Ra'ad Al Hussein held the painful day of remembrance for Holocaust the victims as forcing us "to contemplate the horrors to which bigotry, racism and ultimately lead." "The sadistic brutality of the atrocities inflicted by the Nazi regime on Jews, Roma, Slavs, disabled people, political dissidents, homosexuals and others was nourished by layer upon layer of propaganda, falsifications and incitement to hatred," he stated, adding how they were denigrated and smeared, "one after another, their rights were refused, and finally, even their humanity was denied." Mr. Zeid pointed to the statement of Primo Levi, who survived the Auschwitz Birkenau concentration camp: "It happened, therefore it can happen again." "As we honour the victims of the Holocaust," Mr. Zeid continued, "we must also acknowledge the need to prevent the recurrence of anti-Semitism and all forms of racial and religious hatred and discrimination today." He specified the importance of upholding independent rule of law institutions and a free press; maintaining respect for human rights; and education, which must be at the core of all efforts to combat anti-Semitism, racism, and all forms of discrimination. "In honouring the victims of the Holocaust, we must recognise that only if we regard each other as fully equal in dignity and rights will we be able to come together to overcome the many challenges facing humanity," he concluded. At the same time, Audrey Azoulay, the Director-General of the UN Educational, Scientific and Cultural Organization (UNESCO), citied the Day as a call to strengthen nations' commitment to peace. Recalling the possibility of the worst, also carries a memory that must be forward-looking, she said, adding that combating anti-Semitism, in whatever form, "is at the heart of this fight" in which everyone has a role to play. "We can build up awareness against forgetting, denial, historical revisionism, relativization of crimes and the return of stereotypes that fuel hatred. We can oppose the manipulation of facts by speaking the truth," she asserted. Among a series of events taking place across the UN system, the annual United Nations Holocaust Memorial Ceremony hosted by Ms. Alison Smale, UN Under-Secretary-General for Global Communications, will take place on Wednesday 31 January. The Secretary-General, President of the seventy-second session of the General Assembly, Representatives of Israel, Germany and the United States, will deliver remarks. read more


Anderson wrote one of several letters in support of Gordon Peters Logging Ltd., a well deserving recipient of a BC Aboriginal Business Award announced last month by the BC Achievement Foundation. Gordon plans to attend a gala dinner ceremony with his family on October 26, 2017 at the Fairmont Hotel Vancouver, where over 600 people will gather to honour excellence in Indigenous business in British Columbia.
– How did Gordon react to the news?
– What about Gordon and his business inspired you to nominate him? What makes him a deserving nominee?
– How did you think this news will be celebrated?
The BC Aboriginal Business Award is selected by the British Columbia Achievement Foundation's Board of Directorsand presented in partnership with the Ministry of Indigenous Relations and Reconciliation, as well as sponsors New Relationship Trust, TD, Teck, BC Hydro, CN, Encana, Enbridge, MNPllp and Vancity.
The BC Aboriginal Business Awards were launched in 2008 to honour and celebrate business excellence. Peters is one of 19 Indigenous businesses, entrepreneurs, partnership entities and community-owned enterprises will be recognized at this year's gala dinner.


text:
Results: 2,585 results
1 2 3 4 5 6 7 8 9 10 11 12 13 14 [15] 16 17 18 19 20 21 22 23 24 25 26 27 28 29 30 31 32 33 34 35 36 37 38 39 40 41 42 43 44 45 46 47 48 49 50 51 52 53 54 55 56 57 58 59 60 61 62 63 64 65 66 67 68 69 70 71 72 73 74 75 76 77 78 79 80 81 82 83 84 85 86 87 88 89 90 91 92 93 94 95 96 97 98 99 100 101 102 103 104
Bowman, Martin W. The USAF. 1947-99. Photo available. Phoenix Mills. Sutton Pub. 2000. 176 pps. 4to. Hardcover. First edition. Illustrated. Important reference work. Very scarce in this condition. Fine copy in fine dust jacket (in mylar).
Bowman, Martin W. Wild Blue Yonder. Glory Days of the U.S. Eighth Air Force in England. Photo available. London. Cassell. 2003. 221 pps. 4to. Hardcover. First edition. Illustrated in black, white and color. Important reference work. Very scarce in this condition. Fine copy in fine dust jacket (in mylar).
Bowman, Martin. Spirits in the Sky. Classic Aircraft of World War II. Photo available. New York. Smithmark. 1992. 144 pps. Octavo. Hardcover. First edition. Illustrated in black, white and color. Important reference work. Very scarce in this condition. Fine copy in fine dust jacket (in mylar).
Bowman, Martin. Thunder in the Heavens. Classic American Aircraft of World War II. Photo available. London. Salamander. 2002. 144 pps. 4to. Hardcover. Illustrated in color and black & white. Very scarce in this condition. Fine copy in fine dust jacket (in mylar).
Bowyer, Chaz. Hurricane & Messerschmitt. London. PRC. 1993. 4to. Hardcover. First edition thus. Illustrated. Important reference work. Very scarce in this condition. Fine copy in fine dust jacket (in mylar).
Bowyer, Chaz. Mosquito Typhoon Tempest at War. Photo available. Enderby. PRC. 1974. 4to. Hard cover. First edition thus. Illustrated. Important reference work. Very scarce in this condition. Fine copy in fine dust jacket (in mylar).
Boyne, Alter J. The Aircraft Treasure of Silver Hill. Signed by the author. The Behind-the-Scenes Workshop of Our Nation's Air Museums. Photo available. New York. Rawson Assoc. 1982. 248 pps. Octavo. Hardcover. Stated first edition. Illustrated. Important reference work. Signed by the author. Very scarce in this condition. Fine (blind stamp on end paper) copy in fine dust jacket (in mylar).
Boyne, Walter J. Boeing B-52. A Documentary History. Photo available. Atglen. Schiffer. 1995. 160 pps. 4to. Decorated hard cover. First edition. Illustrated. Important reference work. Very scarce in this condition. Fine copy in fine dust jacket (in mylar).
Boyne, Walter J. Classic Airplanes. Photo available. Lincolnwood. Publications Intl. 2002. 4to. Hardcover. First edition. Illustrated in black, white and color. Important reference work. Very scarce in this condition. Fine copy in fine dust jacket (in mylar).
Boyne, Walter J. Classic Airplanes. Photo available. Lincolnwood. Publications Intl. 2002. 4to. Hardcover. First edition. Illustrated in black, white and color. Fine copy in fine dust jacket (in mylar).
Boyne, Walter J. de Havilland DH-4. From Flaming Coffin to Living Legend. Photo available. Washington. National Air and Sace Museum. 1984. 119 pps. 4to. Soft cover. First edition. Illustrated. Important reference work. Very scarce in this condition. Fine copy.
Boyne, Walter J. The Influence of Air Power Upon History. Photo available. Gretna. Pelican Pub. 2003. 447 pps. Octavo. Hardcover. First edition. Important reference work. Very scarce in this condition. Fine (owner inscription on end paper) copy in fine dust jacket (in mylar).
Boyne, Walter. Brassey's Air Combat Reader. Historic Feats and Aviation Legends. Washington. Brassey's. 2000. Octavo. Soft cover. First edition thus. Very scarce in this condition. Fine copy.
Boyne, Walter. The Leading Edge. Signed by the author. New York. Stewart, Tabori & Chang. 1986. Octavo. Hard cover. First edition. Illustrated in black, white and color. Important reference work. Very scarce in this condition. Signed by the author. Fine copy in fine dust jacket (in mylar).
Bradbury, Jim. Stephen and Matilda. The Civil War of 1139-53. Stroud. Alan Sutton. 1996. Octavo. Hard cover. Reprint. Illustrated. Important reference work. Very scarce in this condition. Fine copy (owner blind stamp) in fine dust jacket (in mylar).
Bradbury, Jim. The Medieval Archer. Photo available. Woodbridge. The Boydell Press. 2002. 198 pps. Octavo. Soft cover. Reprint. Illustrated. Important reference work. Very scarce in this condition. Fine copy.
Braddon, Russell. Cheshire V.C. A Study of War and Peace. Photo available. London. Evans Brothers Limited. 1954. 217 pps. Octavo. Gilt decorated hard cover. Stated first edition. Illustrated. Important reference work. Very scarce in this condition. Article "Saluting the Auschwitz Dead" laid in. Fine copy in fine dust jacket (in mylar).
Bradford, James C. (ed). Makers of The American Naval Tradition. 1840-1880. Captains of The Old Steam Navy. Photo available. Annapolis. Naval Institute Press. 1986. 356 pps. Octavo. Hardcover. First edition. Illustrated. Important reference work. Fine copy in fine dust jacket (in mylar).
Bradford, Ned. Battles and Leaders of the Civil War. Photo available. New York. Appleton-Century-Crofts, Inc. 1956. 4to. Hardcover. First edition. Illustrated. Important reference work. Very scarce in this condition. Fine copy in very good (light shelf wear) dust jacket (in mylar).
Bradley, James. Flyboys. A True Story of Courage. Boston. Little, Brown and Company. 2003. 397 pps. Octavo. Hardcover. First edition. Illustrated. Important reference work. Very scarce in this condition. Fine copy in fine dust jacket (in mylar).
Braeuer, Buc. Adalbert Schnee. German U-Boat Ace. The Patrols of U-201 in World War II. Photo available. Atglen. Schiffer. 2015. 96 pps. 4to. Decorated hard cover. First edition. Illustrated in black, white and color. Important reference work. Very scarce in this condition. Fine copy.
Braeuer, Buc. Peter Cremer. German U-Boat Ace. The Patrols of U-333 in World War II. Photo available. Atglen. Schiffer. 2016. 80 pps. 4to. Decorated hard cover. First edition. Illustrated. Important reference work. Very scarce in this condition. Fine copy.
Bramson, Alan. The Book of Flight Tests. Photo available. New York. Arco. 1984. 4to. Hard cover. First edition. Illustrated in black, white and color. Fine copy in fine dust jacket (in mylar).
Brant, Irving. The Fourth President. A Life of James Madison. Photo available. Norwalk. The Easton Press. 1985. 4to. Gilt decorated hard covers. Leather bindings. All edges gilt. First editions thus. Important reference work. Very scarce in this condition. Collector's Notes laid in. Fine copy.
Braybrook, Roy. F/A-18 Hornet. Photo available. New York. Crescent Books. 1991. 128 pps. 4to. Gilt decorated hard cover. First edition. Illustrated in black, white and color. Important reference work. Very scarce in this condition. Fine copy in fine dust jacket (in mylar).


Assess the current state of research on the mechanisms of action responsible for the cardiovascular effect of several widely-used herbal dietary supplements, including garlic, ginkgo, hawthorn and phytoestrogens and the evidence for their clinical efficacy.
Develop recommendations to identify research opportunities and to discuss potential clinical use of botanicals.
Promote exchange of information and ideas, identify opportunities and foster collaboration among scientists who are interested in using botanicals in cardiovascular research.


I'm thinking I might stand for Parliament… | Subject. Object.
People are angry or dismayed or both about the current political situation. They are rejecting the big three parties because the system's broke. The Liberals, Tories and Labour are all singing from the same hymn sheet, in voices ranging from feeble to strident. The last things on politicians' minds are humanity and the planet. They are presiding over ever-widening inequality but putting up smokescreens that cause division and fear. Surely the vast majority of us want the opposite? We want people to get on with each other, we want peace and happiness, and not instability and hatred.
I want to help bring about unity, to cut through the tribalism, the scapegoating. I want to get rid of poverty, I want people to have control and free use of essentials like drinking water, electricity, food, and public transport. I want a redistribution of wealth, I want banks, the police and civil servants to work with and for all of us, not government and corporations. I want real democracy, not just the representative democracy we have now. I want an end to weapons manufacturing, I want an end to nuclear and for us to get our power from the air and sun and community food production. All in all, I want a better world.
The kind of place I'm coming from is on the left of the green square of this political compass below. You can take a test to see where you stand.
Those are my basic goals. Some might say they're pie in the sky (the classic line is 'but human nature makes people greedy, get real!' I may argue my case against the 'human nature' argument in a future blog). I'm not saying all these goals are possible, or can be achieved quickly – but I won't give up on striving for a society based on mutual aid, with individuals and society on an equal footing.
Might seem a bit of a contradiction standing for Parliament, an institution I feel is weighted in the interests of the 1% super-rich, making many laws on their behalf. I have read Colin Ward's classic text The Case Against Voting, I hear Russell Brand when he says "don't vote". I am really into the idea of building our own society from the grassroots, and also get conscious. But aside from Russell himself and perhaps a few others in comfortable enough circumstances to make the transition, it's not happening. People are still being left destitute with nothing beyond charity to keep them from starvation, with no one looking out for them. This is intolerable and there are too few in Parliament opposing this systematic crushing of poor people.
My reasoning is, say if I and others stood for Parliament as independents (or maybe Bez's Reality Party) all over the country we could help bring about direct democracy with MPs being more like delegates than party-political cogs in the machine? But I haven't firmed up this yet… for instance, if a majority voted for something my conscience couldn't accept, what would I do?
The first stage would be to raise £500 to pay the deposit to the electoral commission.
This is where it is. It's a matter of how the majority of people who don't vote can be engaged. I'm sure political parties, if it's on their radar at all, think 'how do we RE-engage them in voting?' that's the (comparatively) easy, temporary fix…the meaningful, transformative thing would be for the system to RE-engage around them…to go to them rather than try and re-assimilate them into it.
Good point Tony. There is a paradox where one side says "don't vote, it only encourages them", and another side which says "the ruling class love us not voting" (as rightwingers, capitalists, those who want to maintain the status quo, have much more inclination to vote). If people were organising in communities or workplaces and disregarding the political system (if Nobody is the winner, as he/she/it often is, surely Nobody should be governing us, therefore we should not recognise government, and if no one obeys, no one rules?) However the people who should be getting organised outside local/ central government/ corporations are not, for various reasons, one of them being that the powers-that-be create divisions between us to keep us from empowering ourselves.
Yep, you're correct…it's the quandry we find ourselves in. I'm starting to move towards the two-pronged approach that I'm sure you are – vote least worst AND organise.
Broadly speaking – sure, if anyone's on the front-lines dedicated to fighting to dismantle the established order and are confident they have something in the process of being built to take it's place, voting's a minor consideration, but for those (most of us) who aren't up to that challenge, voting within the current system shouldn't be frowned upon by those that are able, legitimately to not do.
Not voting and anti-politics creates a void, which at some point is essential, that point is when 'we' have something to fill it with. We can agree with Emma Goldman AND aspire to get to the point in the popular conscience where we CAN start to leave the status quo to join those pioneers who have laid the ground to build a better framework on. Where we are now, and as conflicting/contradictory as the two things feel, I don't think they're mutually exclusive.


text:
\section{Introduction}
It has been shown with both Yang-Mills (YM) action and the Einstein-Hilbert (EH) action for gravity,
that by using the first order form of the action, there is only a single vertex arising from the
classical action and this is independent of momentum \cite{Okubo:1979gt,Buchbinder:1983ys,McKeon:1994ds,Kalmykov:1994fm,Brandt:2015nxa}.
This simplifies the computation of loop diagrams, even though the number of propagating fields is
increased.

It has also been shown that imposing both the conditions of tracelessness and transversality on the
spin two propagator associated with the EH action requires use of a non-quadratic gauge fixing
Lagrangian \cite{Brandt:2007td,Brandt:2009qi,Brandt:2009rq,Brandt:2011zb,McKeon:2014iea}.
Such gauge fixing results in the need to consider the contributions of two complex
Fermionic ghosts and one real Bosonic ghost analogous to the usual complex ``Faddeev-Popov'' ghosts.

In this paper we consider how the full first order Einstein-Hilbert (1EH) action can be used in conjunction with
the transverse-traceless (TT) gauge. We will show that the spin two propagator is TT only if the
gauge fixing parameter $\alpha$ is allowed to vanish. This limit for $\alpha$ results in a well defined set
of Feynman rules with two propagating Bosonic fields, two complex Fermionic ghost fields, one real Bosonic ghost,
three three-point vertices for the Bosonic fields and four ghost vertices.

\section{The TT gauge for the 1EH Action}
The Einstein-Hilbert action in first order (Palatini) form
\begin{equation}\label{eq1}
S = \int {\rm d}^d x  \sqrt{-g} g^{\mu\nu} R_{\mu\nu}(\Gamma)
\end{equation}
when written in terms of the variables
\begin{subequations}\label{eq2}
\begin{equation}\label{eq2a}
h^{\mu\nu} = \sqrt{-g} g^{\mu\nu}
\end{equation}
\mbox{and}
\be \label{eq2b}
G^\lambda_{\mu\nu} = \Gamma^\lambda_{\mu\nu} - \frac 1 2 \left(
\delta^\lambda_\mu \Gamma^\sigma_{\nu\sigma} +
\delta^\lambda_\nu \Gamma^\sigma_{\mu\sigma} \right)
\ee
\end{subequations}
becomes
\begin{equation}\label{eq3}
S  = \int {\rm d}^d x   h^{\mu\nu}\left(G^\lambda_{\mu\nu\, ,\lambda}   +
\frac{1}{d-1} G^\lambda_{\lambda\mu}  G^\sigma_{\sigma\nu} -
G^\lambda_{\mu\sigma}  G^\sigma_{\nu\lambda} \right) .
\end{equation}
This ``Palatini'' form of the action facilitates a canonical analysis of $S$ \cite{McKeon:2010nf}.
It is equivalent to the second order form of the EH action at both the classical and quantum
levels \cite{Brandt:2015nxa}.
The diffeomorphism invariance of $S$ in Eq. \eqref{eq1} leads to the local gauge transformations
\begin{subequations}\label{eq4}
\begin{equation}\label{eq4a}
\delta h^{\mu\nu} = h^{\mu\lambda} \partial_\lambda \theta^\nu + h^{\nu\lambda} \partial_\lambda \theta^\mu -\partial_\lambda(h^{\mu\nu}\theta^\lambda)
\end{equation}
\begin{eqnarray}\label{eq4b}
\delta G^\lambda_{\mu\nu} &=& -\partial^2_{\mu\nu} \theta^\lambda
+\frac 1 2\left(\delta^\lambda_\mu\partial_\nu+\delta^\lambda_\nu\partial_\mu\right)\partial_\rho\theta^\rho-\theta^\rho\partial_\rho G^\lambda_{\mu\nu}
\nonumber \\
&+& G^\rho_{\mu\nu} \partial_\rho\theta^\lambda - \left(G^ \lambda_{\mu\rho} \partial_\nu+G^ \lambda_{\nu\rho} \partial_\mu\right)\theta^ \rho
\end{eqnarray}
\end{subequations}
The term bilinear in $h$ and $G$ in Eq. \eqref{eq3} does not lead to a well defined propagator,
irrespective of the choice of gauge fixing. However, upon making an expansion of $h^{\mu\nu}$
about a flat background
\be\label{eq5}
h^{\mu\nu} = \eta^{\mu\nu} + \phi^{\mu\nu}(x)\;\;\; (\eta^{\mu\nu} = \mbox{diag}(+---\dots))
\ee
the term bilinear in $\phi$ and $G$ arising from Eq. \eqref{eq3} does have a well defined propagator
once an appropriate gauge fixing is chosen. These bilinear terms are the first order form of the
action for a spin two field \cite{McKeon:2010nf}.

In order to have a TT propagator for the spin two field we must consider a general gauge fixing
Lagrangian that is not quadratic \cite{Brandt:2007td}. If the classical Lagrange density appearing
in Eq. \eqref{eq3} is ${\cal L}(h^{\mu\nu},G^\lambda_{\mu\nu})$, then this entails inserting into the
generating functional
\be\label{eq6}
Z[j_{\mu\nu},J_\lambda^{\mu\nu}] =
\int {\cal D} \phi^{\mu\nu} {\cal D} G^\lambda_{\mu\nu}
\exp i\int {\rm d}^d x  \left({\cal L}(\eta+\phi,G) + j_{\mu\nu} \phi^{\mu\nu} + J^{\mu\nu}_\lambda G^\lambda_{\mu\nu}
\right)
\ee
two factors of ``$1$''
\be\label{eq7}
1 = \int {\cal D} \boldsymbol{\theta}_i \, \delta\left(\undertilde{\; F}\!{}_i(\boldsymbol\phi + \undertilde{A} \boldsymbol{\theta}_i) - \boldsymbol{p}_i\right)
\det(\undertilde{\; F}\!{}_i \undertilde{A});\;\;\;  (i=1,2)
\ee
where $\boldsymbol\phi=(\phi^{\mu\nu}, G^\lambda_{\mu\nu})$. The gauge transformations of Eq. \eqref{eq4}
are of the form
\be\label{eq8}
\delta_i \boldsymbol\phi = \undertilde{A} \boldsymbol{\theta}_i
\ee
and the gauge fixing conditions are
\be\label{eq9}
\undertilde{\; F}\!{}_i \boldsymbol\phi = 0.
\ee
Insertion of a third factor of ``$1$'' that is of the form
\be\label{eq10}
1 = \frac{1}{(\pi\alpha)^d}\int {\cal D} \boldsymbol{p}_1 {\cal D} \boldsymbol{p}_2 \exp
\frac{-i}{\alpha}\int {\rm d}^d x  (\boldsymbol{p}_1^{\rm T} \undertilde{\; N} \boldsymbol{p}_2) \det(\undertilde{\; N})
\ee
into Eq. \eqref{eq6} leads to
\begin{eqnarray}\label{eq11}
Z[\boldsymbol{j}] = \int {\cal D}\boldsymbol\phi \det(\undertilde{\; F}\!{}_1  \undertilde{A}) \det(\undertilde{\; F}\!{}_2 \undertilde{A})
\det(\undertilde{\; N}/\pi\alpha) \int {\cal D} \boldsymbol{\theta}_1 {\cal D} \boldsymbol{\theta}_2 \nonumber \\
\exp i\int {\rm d}^d x \left\{
{\cal L}(\boldsymbol\phi) - \frac{1}{\alpha} \left[\undertilde{\; F}\!{}_1(\boldsymbol\phi+\undertilde{A}\boldsymbol{\theta}_1)\right]^{\rm T
\undertilde{\; N} \left[\undertilde{\; F}\!{}_2(\boldsymbol\phi+\undertilde{A}\boldsymbol{\theta}_2)\right] + \boldsymbol{j}^{\rm T} \cdot \boldsymbol\phi\right\} ;\;\;\;
(\boldsymbol{j}\equiv (j_{\mu\nu}, J_\lambda^{\mu\nu})) .
\end{eqnarray}

Since the gauge transformation of Eq. \eqref{eq8} leaves ${\cal L}(\boldsymbol\phi)$,
${\cal D}\boldsymbol\phi$ and $\det(\undertilde{\; F}\!{}_i\undertilde{A})$ invariant \cite{faddeev:book1980,weinberg:book1995},
we can make the shift
\begin{equation}\label{eq12a}
\boldsymbol\phi \rightarrow\boldsymbol\phi -  \undertilde{A} (\boldsymbol{\theta}_{+} + \epsilon \boldsymbol{\theta}_{-})
\end{equation}
in Eq. \eqref{eq11} \hbox{($\boldsymbol{\theta}_{\pm} \equiv (\boldsymbol{\theta}_1\pm\boldsymbol{\theta}_2)/2$)}
leaving us with
\begin{eqnarray} \label{eq12}
Z[\boldsymbol{j}] = \int {\cal D}\boldsymbol\phi {\cal D}\boldsymbol{\theta}_{-}
\det(\undertilde{\; F}\!{}_1 \undertilde{A}) \det(\undertilde{\; F}\!{}_2 \undertilde{A}) \det(\undertilde{\; N})
\nonumber \\
\exp i\int {\rm d}^d x \left\{
{\cal L}(\boldsymbol\phi) - \frac{1}{\alpha} \left[\undertilde{\; F}\!{}_1(\boldsymbol\phi+\undertilde{A}(1-\epsilon)\boldsymbol{\theta}_{-})\right]^{\rm T}
\right.\nonumber \\
\left.
\undertilde{\; N} \left[\undertilde{\; F}\!{}_2(\boldsymbol\phi-\undertilde{A}(1+\epsilon)\boldsymbol{\theta}_{-})\right] + \boldsymbol{j}^{\rm T} \cdot \boldsymbol\phi\right\}.
\end{eqnarray}
A factor $1/(\pi \alpha)^{d/2} \int {\cal D}\boldsymbol{\theta}_{+}$ has been absorbed into the normalization
of $Z$. We now choose the gauge fixing to be
\begin{subequations}\label{eq13}
\be
\undertilde{\; F}\!{}_i \boldsymbol\phi = g_i \partial_\rho \phi^\mu_\mu + \partial_\mu \phi^\mu_\rho
\ee
and
\be
\undertilde{\; N} = {\eta^{\mu\nu}}/{2}.
\ee
\end{subequations}
The gauge fixing contribution of Eq. \eqref{eq12} becomes
\begin{eqnarray}\label{eq14}
&&\left[\undertilde{\; F}\!{}_1(\boldsymbol\phi+\undertilde{A}(1-\epsilon)\boldsymbol{\theta}_{-})\right]^{\rm T}
\undertilde{\; N} \left[\undertilde{\; F}\!{}_2(\boldsymbol\phi-\undertilde{A}(1+\epsilon)\boldsymbol{\theta}_{-})\right]
\nonumber\\
&=& (\undertilde{\; F}\!{}_1\boldsymbol\phi)^{\rm T} \undertilde{\; N} (\undertilde{\; F}\!{}_2\boldsymbol\phi)+(\epsilon^2-1)\left\{\left[\vthm^{\rm T} +
\frac 1 2 \vphi^{\rm T}\left(-(1+\epsilon) \unf\!{}_1^{\;\rm T} \undertilde{\; N} \unf\!{}_2 +(1-\epsilon) \unf\!{}_2^{\;\rm T} \undertilde{\; N} \unf\!{}_1\right) \undertilde{A}
\right.\right. \nonumber \\
&&\left.\left({(\undertilde{A}^{\rm T} \unf\!{}_1^{\;\rm T}\undertilde{\; N}\unf\!{}_2\undertilde{A})^{-1}}/{(\epsilon^2-1)}\right)\right]
\left[\undertilde{A}^{\rm T}\unf\!{}_1^{\;\rm T}\undertilde{\; N}\unf\!{}_2\undertilde{A}\right]
\nonumber \\
&& \left. \left[\boldsymbol{\theta}_{-} +\frac 1 2 \left((\undertilde{A}^{\rm T}\unf\!{}_1^{\;\rm T}\undertilde{\; N}\unf\!{}_2\undertilde{A})^{-1}/(\epsilon^2-1)\right)
\undertilde{A}^{\rm T}\left(-(1+\epsilon)\unf\!{}_2^{\;\rm T}\undertilde{\; N}\unf\!{}_1 +(1-\epsilon)\unf\!{}_1^{\;\rm T}\undertilde{\; N}\unf\!{}_2\right)\boldsymbol\phi \right] \right\}
\nonumber \\
&&
-\frac{1}{4(\epsilon^2-1)}\vphi^{\rm T}\left(-(1+\epsilon)\unf\!{}_1^{\;\rm T}\undertilde{\; N}\unf\!{}_2 + (1-\epsilon)\unf\!{}_2^{\;\rm T}\undertilde{\; N}\unf\!{}_1\right)\undertilde{A}
(\undertilde{A}^{\rm T}\unf\!{}_1^{\;\rm T}\undertilde{\; N}\unf\!{}_2\undertilde{A})^{-1} \undertilde{A}^{\rm T}
\nonumber \\ &&
\left(-(1+\epsilon)\unf\!{}_2^{\;\rm T}\undertilde{\; N}\unf\!{}_1 + (1-\epsilon)\unf\!{}_1^{\;\rm T}\undertilde{\; N}\unf\!{}_2 \right)\boldsymbol\phi
\end{eqnarray}
(In Eq. \eqref{eq14} we use the convention $\partial^{\rm T} = -\partial$.)

Provided $\epsilon\neq\pm 1$, the shift in $\boldsymbol{\theta}_{-}$
\begin{equation}\label{eq15}
\boldsymbol{\theta}_{-} \rightarrow \boldsymbol{\theta}_{-} - \frac 1 2\left(
(\undertilde{A}^{\rm T}\unf\!{}_1^{\;\rm T}\undertilde{\; N}\unf\!{}_2\undertilde{A})^{-1}/(\epsilon^2-1) \right)
\undertilde{A}^{\rm T}\left(-(1+\epsilon)\unf\!{}_2^{\;\rm T}\undertilde{\; N}\unf\!{}_1 +(1-\epsilon)\unf\!{}_1^{\;\rm T}\undertilde{\; N}\unf\!{}_2\right)\boldsymbol\phi
\end{equation}
can be made to diagonalize Eq. \eqref{eq14} in $\boldsymbol{\theta}_{-}$ and $\boldsymbol\phi$. In Refs. \cite{Brandt:2007td,Brandt:2009qi,Brandt:2009rq}
$\epsilon=\pm 1$ and a shift in $\boldsymbol\phi$ was used to diagonalize the gauge fixing, but as such a shift is not a gauge transformation,
${\cal L}(\boldsymbol\phi)$ is not invariant under this transformation and new vertices involving $\boldsymbol\phi$ and $\boldsymbol{\theta}_{-}$ must be
introduced. We take $\epsilon\neq\pm 1$ in order to be able to make a shift in $\boldsymbol{\theta}_{-}$ that eliminates mixed propagators for these fields
without introducing extra vertices.

Together Eqs. \eqref{eq14} and \eqref{eq15} result in
\begin{eqnarray} \label{eq17}
Z[\boldsymbol{j}] &=& \int {\cal D}\boldsymbol\phi {\cal D}\boldsymbol{\theta}_{-}
\det(\undertilde{\; F}\!{}_1 \undertilde{A}) \det(\undertilde{\; F}\!{}_2 \undertilde{A}) \det(\undertilde{\; N})
\nonumber \\
&&\exp i\int {\rm d}^d x \left\{
{\cal L}(\boldsymbol\phi) - \frac{1}{\alpha} (\unf\!{}_1\boldsymbol\phi)^{\rm T} \undertilde{\; N}(\unf\!{}_2\boldsymbol\phi)
\right.
-\frac{1}{\alpha(\epsilon^2-1)}\vthm^{\rm T}(\undertilde{A}^{\rm T}\unf\!{}_1^{\;\rm T}\undertilde{\; N}\unf\!{}_2\undertilde{A})\boldsymbol{\theta}_{-}
\nonumber \\
&+&\frac{1}{4\alpha(\epsilon^2-1)}\vphi^{\rm T}\left(-(1+\epsilon)\unf\!{}_1^{\;\rm T}\undertilde{\; N}\unf\!{}_2 + (1-\epsilon)\unf\!{}_2^{\;\rm T}\undertilde{\; N}\unf\!{}_1\right)\undertilde{A}
(\undertilde{A}^{\rm T}\unf\!{}_1^{\;\rm T}\undertilde{\; N}\unf\!{}_2\undertilde{A})^{-1}
\nonumber \\
&&\left.  \undertilde{A}^{\rm T}\left(-(1+\epsilon)\unf\!{}_2^{\;\rm T}\undertilde{\; N}\unf\!{}_1 + (1-\epsilon)\unf\!{}_1^{\;\rm T}\undertilde{\; N}\unf\!{}_2 \right)\boldsymbol\phi
+ \boldsymbol{j}^{\rm T} \cdot \boldsymbol\phi\right\}.
\end{eqnarray}
The integral over $\boldsymbol{\theta}_{-}$ can now be evaluated in Eq. \eqref{eq17}; it results in a contribution
\begin{equation}\label{eq18}
\det{}^{-1/2}(\unf\!{}_1\undertilde{A})\det{}^{-1/2}(\undertilde{\; N})\det{}^{-1/2}(\unf\!{}_2\undertilde{A}).
\end{equation}
We now treat the last term in Eq. \eqref{eq17} as an interaction term. Due to its structure, the two fields $\boldsymbol\phi$ that occur
explicitly ($\undertilde{A}$ also is $\boldsymbol\phi$ dependent on account of Eq. \eqref{eq4a}) are contracted with a propagator for $\phi_{\mu\nu}$
and a factor of $\undertilde{X}$ where
\begin{eqnarray}\label{eq19}
X_{\mu\nu,\lambda\sigma} &\equiv& \left(-(1+\epsilon)\unf\!{}_2^{\;\rm T}\undertilde{\; N}\unf\!{}_1 + (1-\epsilon)\unf\!{}_1^{\;\rm T}\undertilde{\; N}\unf\!{}_2\right)_{\mu\nu,\lambda\sigma}
\nonumber\\
&=&\frac 1 2 (g_1-g_2)\left(\partial_\mu\partial_\nu\eta_{\lambda\sigma} - \eta_{\mu\nu}  \partial_\lambda\partial_\sigma \right)
\nonumber \\
&+& \epsilon\left[g_1 g_2 \eta_{\mu\nu} \eta_{\lambda\sigma} \partial^2 + \frac{g_1+g_2}{2}
\left(\partial_\mu\partial_\nu \eta_{\lambda\sigma} + \eta_{\mu\nu} \partial_\lambda\partial_\sigma \right) \right.
\nonumber \\
&+&\left. \frac 1 4 \left(\partial_\mu\partial_\lambda \eta_{\nu\sigma}  + \partial_\nu\partial_\lambda \eta_{\mu\sigma} +
                         \partial_\mu\partial_\sigma \eta_{\nu\lambda}  + \partial_\nu\partial_\sigma \eta_{\mu\lambda}  \right)\right]
\end{eqnarray}
by Eq. \eqref{eq13}.

We know from Refs. \cite{Brandt:2007td,Brandt:2009qi,Brandt:2009rq} that as $\alpha\rightarrow 0$, the propagator for the field
$\phi_{\mu\nu}$ that comes from ${\cal L}(\boldsymbol\phi) -\frac{1}{\alpha} (\unf\!{}_1\boldsymbol\phi)^{\rm T} \undertilde{\; N} (\unf\!{}_2\boldsymbol\phi)$ is transverse and traceless in the
limit $\alpha\rightarrow 0$ provided $g_1\neq g_2$. Only terms of order $\alpha$ are not transverse and traceless.
Thus, on account of the structure of Eq. \eqref{eq19}, the contribution of the vertex coming from the last term in Eq. \eqref{eq17} vanishes
as $\alpha\rightarrow 0$, even though this vertex is proportional to $1/\alpha$. There is on exception to this; when a sequence of these
vertices lies in a ring, then a finite contribution arises in the limit $\alpha\rightarrow 0$. To see this in more detail, write this last term in
Eq. \eqref{eq17} as
\begin{equation}\label{eq20}
\frac{1}{\alpha} \vphi^{\rm T} \undertilde{V} \boldsymbol\phi = \frac{1}{\alpha} \vphi^{\rm T} (\undertilde{X}^{\rm T}\undertilde{A}) \frac{(\undertilde{A}^{\rm T}\unf\!{}_1^{\;\rm T}\undertilde{\; N}\unf\!{}_2\undertilde{A})^{-1}}{4(\epsilon^2-1)}\undertilde{A}^{\rm T}\undertilde{X}\boldsymbol\phi .
\end{equation}
A ring in which a sequence of these vertices occurs results in a contribution proportional to
\begin{eqnarray}\label{eq21}
&{\rm Tr}\left\{\left[\frac{1}{\alpha} \undertilde{X}^{\rm T} \undertilde{A} (\undertilde{A}^{\rm T}\unf\!{}_1^{\;\rm T}\undertilde{\; N}\unf\!{}_2\undertilde{A})^{-1} \undertilde{A}^{\rm T}\undertilde{X} \right]\undertilde{D}
\left[\frac{1}{\alpha} \undertilde{X}^{\rm T} \undertilde{A} (\undertilde{A}^{\rm T}\unf\!{}_1^{\;\rm T}\undertilde{\; N}\unf\!{}_2\undertilde{A})^{-1} \undertilde{A}^{\rm T}\undertilde{X} \right] \undertilde{D}  \right. \nonumber\\
&\dots \left .
\left[\frac{1}{\alpha} \undertilde{X}^{\rm T} \undertilde{A} (\undertilde{A}^{\rm T}\unf\!{}_1^{\;\rm T}\undertilde{\; N}\unf\!{}_2\undertilde{A})^{-1} \undertilde{A}^{\rm T}\undertilde{X} \right] \undertilde{D}
\right\},
\end{eqnarray}
where $\undertilde{D}$ is the propagator of $\boldsymbol\phi$. From Eq. \eqref{eq19} it is apparent that since when $\alpha\rightarrow 0$ $\undertilde{D}$ is transverse and traceless,
then $\undertilde{X}\undertilde{D}$ is of order $\alpha$; since we have a factor of $1/\alpha$ for each factor of $\undertilde{X}\undertilde{D}$ on account of these vertices occurring in a ring,
we can let
\begin{equation}\label{eq22}
\lim_{\alpha\rightarrow 0} \frac{1}{\alpha} \undertilde{X}\undertilde{D} = \undertilde{X}\undertilde{D}^{(0)}.
\end{equation}
Furthermore, a contribution of a closed loop of these vertices can be written as
\begin{eqnarray}\label{eq23}
&&\det{}^{-1/2}\left[\undertilde{X}^{\rm T} \undertilde{A} (\undertilde{A}^{\rm T}\unf\!{}_1^{\;\rm T}\undertilde{\; N}\unf\!{}_2\undertilde{A})^{-1} \undertilde{A}^{\rm T}\undertilde{X} \undertilde{D}^{(0)} \right]
\nonumber \\
&=&
\det{}^{1/2}(\unf\!{}_1\undertilde{A}) \det{}^{1/2}(\undertilde{\; N}) \det{}^{1/2}(\unf\!{}_2\undertilde{A}) \det{}^{-1/2}(\undertilde{A}^{\rm T}\undertilde{X}\undertilde{D}^{(0)}\undertilde{X}^{\rm T}\undertilde{A}) .
\end{eqnarray}
Together Eqs. \eqref{eq18} and \eqref{eq23} reduce Eq. \eqref{eq17} to
\begin{eqnarray}\label{eq24}
Z[\boldsymbol{j}] &=& \lim_{\alpha\rightarrow 0}\int {\cal D}\boldsymbol\phi
\det(\undertilde{\; F}\!{}_1 \undertilde{A})  \det(\undertilde{\; N})   \det(\undertilde{\; F}\!{}_2 \undertilde{A}) \det{}^{-1/2}(\undertilde{A}^{\rm T}\undertilde{X}\undertilde{D}^{(0)} \undertilde{X}^{\rm T}\undertilde{A})
\nonumber \\
&&\exp i\int {\rm d}^d x \left\{
{\cal L}(\boldsymbol\phi) - \frac{1}{\alpha} (\unf\!{}_1\boldsymbol\phi)^{\rm T} \undertilde{\; N}(\unf\!{}_2\boldsymbol\phi) + \boldsymbol{j}^{\rm T} \cdot \boldsymbol\phi\right\}
\end{eqnarray}
provided $g_1\neq g_2$. The functional determinants in Eq. \eqref{eq24} can be exponentiated using ``ghost'' fields;
$\det(\unf\!{}_i\undertilde{A})$ ($i=1,2$) using complex Fermionic ``Faddeev-Popov''
ghosts ${\bf c} _i$ \cite{Feynman:1963ax,DeWitt:1967yk, Faddeev:1967fc, Mandelstam:1968hz},
$\det(\undertilde{\; N})$ by a complex Fermionic Nielsen-Kalosh ghost \cite{Nielsen:1978mp, Kallosh:1978de} and
$\det{}^{-1/2}(\undertilde{A}^{\rm T}\undertilde{X}\undertilde{D}^{(0)}\undertilde{A})$ by a real Bosonic ghost ${\bf\zeta}$. By Eq. \eqref{eq4a}, it follows that
\begin{equation}\label{eq25}
(\undertilde{A}\boldsymbol{\theta})_{\mu\nu} = \left[\partial_\mu\eta_{\nu\rho} +\partial_\nu\eta_{\mu\rho} - \partial_\rho\eta_{\mu\nu} +
\left(\phi_\mu{}^\sigma\partial_\sigma \eta_{\nu\rho}+\phi_\nu{}^\sigma\partial_\sigma \eta_{\mu\rho}+\partial_\rho\phi_{\mu\nu}\right) \right]\theta^\rho .
\end{equation}
Using Eqs. \eqref{eq19} and \eqref{eq25} and the propagator for $\boldsymbol\phi$ given in Ref \cite{Brandt:2007td} we find that the contribution that is bilinear in the ghost
${\bf\zeta}$is given by
\begin{equation}\label{eq26}
4p^2\zeta_\mu\left\{\epsilon^2 p^2\eta^{\mu\nu} + \left[\left(g_1 g_2(d-2)^2 - (g_1+g_2)(d-2)\right)(\epsilon^2-1) -1\right]p^\mu p^\nu\right\}\zeta_\nu
\end{equation}
which becomes
\begin{equation}\label{eq27}
4 p^4\epsilon^2\zeta_\mu\eta^{\mu\nu} \zeta_\nu .
\end{equation}
when
\begin{equation}\label{eq28}
g_1 = -g_2 = \frac{1}{(d-2)\sqrt{1-\epsilon^2}}.
\end{equation}
Similarly, the vertex for $\phi_{\mu\nu}(p)$ -- $\zeta_\alpha(q)$ -- $\zeta_\beta(r)$ comes from
\begin{eqnarray}\label{eq29}
&&\frac 1 2 \left\{\left[(d-2)g_1(\epsilon-1)^2 + (d-2) g_2 ((\epsilon+1)^2 -2\right]
q^\mu q^\alpha \left(p^\beta q^\nu + r^\beta q^\nu - 2 q^\beta r^\nu\right)   \right.
\nonumber \\
&+&  \epsilon^2 q^2 q^\mu \left[2 r^\nu\eta^{\alpha\beta} - p^\beta\eta^{\alpha\nu} + r^\beta\eta^{\alpha\nu}\right]
\nonumber \\
&+& q^2\left(2 r^\nu q^\alpha \eta^{\mu\beta} - p^\beta q^\alpha \eta^{\mu\nu} - r^\beta q^\alpha \eta^{\mu\nu}\right)
\left[g_1(\epsilon+1)^2+g_2(\epsilon-1)^2 - 2 g_1g_2(d-1)(\epsilon+1)^2\right]
\nonumber \\ &+& \left.
\epsilon^2 q^2 \eta^{\mu\nu}\left(2 r^\nu q^\beta - p^\beta q^\nu -r^\beta q^\nu \right) \right\}
+ (\mu\leftrightarrow\nu) + (\alpha\leftrightarrow\beta ;\; q\leftrightarrow r).
\end{eqnarray}
Finally, a vertex for $\phi_{\mu_1\nu_1}(p)$ -- $\phi_{\mu_2\nu_2}(q)$ -- $\zeta_\alpha(r)$ -- $\zeta_\beta(s)$ can also be worked out.
The vertices $\phi$ -- $\phi$ -- $\zeta$ -- $\zeta$  and \mbox{$\phi$ -- $\zeta$ -- $\zeta$} are both quartic in the external momenta.

The two complex ``Faddeev-Popov'' ghosts ${\bf c}_1$ and ${\bf c}_2$ and the real Bosonic ghost $\zeta$  reduce to a single
complex Fermionic Faddeev-Popov ghost ${\bf c} = {\bf c}_1 + i {\bf c}_2$ if we deal with a quadratic gauge fixing Lagrangian
when $\unf\!{}_1 = \unf\!{}_2$.

If we now define $M^{\mu\nu}_\lambda{}^{\pi\tau}_\sigma(h)$ by the equation
\be \label{eq30}
h^{\mu\nu} \left(\frac{1}{d-1} G^\lambda_{\lambda\mu} G^\sigma_{\sigma\nu}
- G^\lambda_{\sigma\mu} G^\sigma_{\lambda\nu} \right)
=\frac 1 2 M^{\mu\nu}_\lambda {}^{\pi\tau}_\sigma(h) G^\lambda_{\mu\nu} G^\sigma_{\pi\tau}
\ee
then the shift
\be \label{eq31}
G^\lambda_{\mu\nu} \rightarrow G^\lambda_{\mu\nu}  +
M^{-1}{}^\lambda_{\mu\nu}{}^\sigma_{\pi\tau}(\eta)\, \phi^{\pi\tau}_{,\sigma}
\ee
in ${\cal L}(\boldsymbol\phi)$ in Eq. \eqref{eq22} leads to
\begin{eqnarray}\label{eq32}
{\cal L}(\boldsymbol\phi) = -\frac 1 2
\phi^{\mu\nu}_{,\lambda} M^{-1}{}^\lambda_{\mu\nu}{}^\sigma_{\pi\tau}(\eta)\, \phi^{\pi\tau}_{,\sigma}
+ \frac 1 2 G^{\lambda}_{\mu\nu} M^{\mu\nu}_\lambda{}^{\pi\tau}_{\sigma}(\eta) G_{\pi\tau}^{\sigma}
\nonumber \\
+ \frac 1 2
\left(G^\lambda_{\mu\nu}  +  \phi^{\alpha\beta}_{,\xi}  M^{-1}{}^\xi_{\alpha\beta}{}^\lambda_{\mu\nu}(\eta)\right)
M^{\mu\nu}_\lambda{}^{\pi\tau}_{\sigma}(\phi)
\left(G^\sigma_{\pi\tau}  +  M^{-1}{}^\sigma_{\pi\tau}{}^\zeta_{\gamma\delta}(\eta) \phi^{\gamma\delta}_{,\zeta}   \right)
\end{eqnarray}
so that off diagonal propagators $\phi-G$ are eliminated. However, two new momentum
dependent vertices now arise. They are $\phi-\phi-\phi$ and $\phi-\phi-G$.

With the gauge fixing of Eq. \eqref{eq13} we find from Ref. \cite{Brandt:2007td} that the propagator for the field
$G^\lambda_{\mu\nu}$ is
\begin{subequations}\label{eq33}
\begin{eqnarray
\displaystyle{\substack{{}^{\displaystyle{ {}_{\mu\nu}^\lambda}} {\; \includegraphics[scale=0.7]{Gprop} \;} {}^{\displaystyle{ {}_{\pi\tau}^\rho}}
\\  {\displaystyle{ }}}}
&  =  & \;\;\;\;
\frac{1}{4} \eta^{\lambda \rho } \left(\eta_{\mu\tau } \eta_{\nu \pi} + \eta_{\mu \pi } \eta_{\nu \tau}
-\frac{2}{d-2} \eta_{\mu \nu } \eta_{\pi \tau }\right)
\nonumber \\
&&
-\frac{1}{4} \left( \delta^{\lambda}_{ \tau } \delta_{\mu}^{ \rho } \eta_{\nu \pi}
+\delta^{\lambda}_{\tau } \delta_{\nu}^{ \rho}\eta_{\mu \pi }
+\delta^{\lambda}_{  \pi }  \delta_{\nu}^{ \rho} \eta_{\mu \tau }
+\delta^{\lambda}_{ \pi } \delta_{\mu}^{ \rho } \eta_{\nu \tau} \right)
\end{eqnarray}
\mbox{The propagator for $\phi_{\mu\nu}$ is \cite{Brandt:2007td}}
\begin{eqnarray}\label{eq33b}
\displaystyle{\substack{{}^{\displaystyle{ {}_{\displaystyle{\mu\, \nu}}}}
{\; \includegraphics[scale=0.7]{phiProp} \;} {}^{\displaystyle{{}_{\displaystyle{\lambda\, \sigma}}}}
\\  {\displaystyle{k}}}}
&  =  & \;\;\;\;
\frac{1}{k^2}\left\{\eta_{\mu\lambda} \eta_{\nu\sigma} + \eta_{\mu\sigma} \eta_{\nu\lambda}
- 2 \frac{(g_1-g_2)^2 + 2 (g_1+1)(g_2+1)\alpha}{\Delta} \eta_{\mu\nu} \eta_{\lambda\sigma}\right.
\nonumber\\   &+&
(\alpha-1)\frac{1}{k^2}\left[k_\mu k_\lambda \eta_{\nu\sigma}
+(\mu\leftrightarrow\nu)+(\lambda\leftrightarrow\sigma)\right]
\nonumber\\   &+&
2 \frac{(g_2-g_1)^2 + [4(g_1+1)(g_2+1)-g_2-g_1-2]\alpha}{\Delta}
\frac{1}{k^2}\left[k_\mu k_\nu \eta_{\lambda\sigma} + k_\lambda k_\sigma \eta_{\mu\nu}\right]
\nonumber\\   &+& \frac{1}{\Delta}
\left[4\alpha\left[(g_1+g_2)(d-4)+(2 g_1 g_2+1)(d-3)-\left(g_1^2+g_2^2\right)(d-1)\right]
\right.
\nonumber \\ &+&\left. \left.
2(d-2)\left[(g_1-g_2)^2-\alpha ^2 (4(g_1+1)(g_2+1)-1) \right]\right]
\frac{1}{k^4} k_\mu k_\nu k_\lambda k_\sigma \right\},
\end{eqnarray}
\mbox{where $\Delta=(d-1)(g_1-g_2)^2 + 2 (d-2)(g_1+1)(g_2+1)\alpha$.
When $\alpha\rightarrow 0$ ($g_1\neq g_2$) this becomes the transverse-traceless}
\mbox{propagator.}

\mbox{For the real fields $c_i$ we have   }
\begin{eqnarray
\substack{ \displaystyle{\mu} \; \includegraphics[scale=0.7]{ghostProp} \; \displaystyle{\nu}
\\  {\displaystyle{ k}}}
& = &  D_{\mu\nu}^{(i)} \;\;\;\;
= \frac{\displaystyle{\frac{(d-2)g_i k_\mu k_\nu}{k^2 [(d-2) g_i -1]}}  -\eta^{\mu\nu} }{k^2}.
\end{eqnarray}
\end{subequations}
The vertices are given by
\begin{subequations}\label{eq34}
\begin{eqnarray
{}_{\mu\nu},\, p\, { \imineq{ghostghostphi}{14} }^{{\displaystyle{i,\; q,\;{}_\alpha}}}_{{{\displaystyle{j,\;r,\; {}_\beta\;\; }}}}
&  =  & \;\;\;\;
\frac{\delta^{ij} }{4}\left[-p^\beta q^\nu \eta^{\mu\alpha} -r^\beta q^\nu \eta^{\mu\alpha}
-g_i p^\beta q^\alpha \eta^{\mu\nu}
\right. \nonumber \\
& - & \left. g_i r^\beta q^\alpha \eta^{\mu\nu}
+2  g_i r^\nu q^\alpha \eta^{\mu\beta}
 + (q,\alpha) \leftrightarrow (r,\beta) \right] + \mu\leftrightarrow\nu
\end{eqnarray}
\begin{eqnarray
{}_{\mu\nu} { \imineq{GGphi}{14} }^{\displaystyle{\;\;{}^{\alpha\beta}_\lambda}}_{\displaystyle{\;\;{}^{\gamma\delta}_\sigma}}
&  =  & \;\;\;\;
\frac{1}{8} \left\{\left[\left(
\frac{\delta_{\mu}^{\beta} \delta_{\nu}^{\delta} \delta^\alpha_\lambda \delta^\gamma_\sigma}{d-1} -
\delta_{\mu}^{\beta} \delta_{\nu}^\delta \delta^\alpha_\sigma \delta^\gamma_\lambda + \mu \leftrightarrow \nu\right) + \alpha\leftrightarrow\beta
\right]+\gamma\leftrightarrow\delta\right\}
\nonumber \\
&& + \;\; (\lambda, \alpha,\beta) \longleftrightarrow (\sigma,\gamma,\delta)
\end{eqnarray}
\begin{eqnarray
{}_\sigma^{\gamma\delta}\, p\, { \imineq{Gphiphi}{14} }^{\displaystyle{q\;{}_{\mu\nu}}}_{\displaystyle{r\;{}_{\alpha\beta}}}
&  =  & \;\;\;\;
\frac{i r_\theta}{4}\left\{\left[\left(
\frac{1}{d-1} \delta^\gamma_\mu \delta^\delta_\sigma {\cal D}_{ \alpha\beta}^\theta {}^\rho_{\nu\rho}
-\delta^\gamma_\mu {\cal D}_{\alpha\beta}^\theta{}_{\nu\sigma}^\delta
+ \mu \leftrightarrow \nu\right) + \alpha\leftrightarrow \beta\right] + \gamma\leftrightarrow \delta\right\}
\nonumber \\
&& +  \;\; (q, \alpha,\beta) \longleftrightarrow (r,\mu,\nu)
\end{eqnarray}
\begin{eqnarray
{}_{\mu\nu}\, p\, { \imineq{phiphiphi}{14} }^{\displaystyle{q\;{}_{\alpha\beta}}}_{\displaystyle{r\;{}_{\gamma\delta}}}
&  =  & \;\;\;\;
\frac{q_\kappa r_\theta}{8}\left\{\left[\left(
{\cal D}{}^\kappa_{\alpha\beta}{}^\pi_{\mu\sigma}
                                                                {\cal D}{}^\theta_{\gamma\delta}{}^\sigma_{\nu\pi}
 -\frac{1}{d-1} {\cal D}{}^\kappa_{\alpha\beta}{}^\sigma_{\mu\sigma}
                                                                {\cal D}{}^\theta_{\gamma\delta}{}^\pi_{\nu\pi}
 + \mu \leftrightarrow \nu\right) + \alpha\leftrightarrow \beta\right] + \gamma\leftrightarrow \delta\right\}
\nonumber \\
&& + \;\; \mbox{six permutations of}\;\; (p, \mu,\nu) \;\; (q, \alpha,\beta) \;\; (r, \gamma,\delta)
\end{eqnarray}
\end{subequations}
If $g_1 =  g_2$, we cannot recover the TT propagator from Eq. \eqref{eq33b} even if $\alpha\rightarrow 0$ \cite{Brandt:2007td}.

For the Bosonic ghost $\zeta^\mu$ we have a propagator and vertices that follow from Eqs. \eqref{eq27} and \eqref{eq28}.

The arguments used in ref. \cite{faddeev:book1980,weinberg:book1995} can be used to show that when using a
non-quadratic gauge fixing Lagrangian, physical results are independent of the gauge choice.

Beginning with the insertion of Eq. \eqref{eq7} into Eq. \eqref{eq6}, we have
\begin{eqnarray}\label{eqa1}
Z[\boldsymbol{j}] &=&
\int {\cal D} \boldsymbol\phi  \int {\cal D} \boldsymbol{\theta}_1 {\cal D} \boldsymbol{\theta}_2
\exp i\int {\rm d}^d x \left[ {\cal L}(\boldsymbol\phi) + \boldsymbol{j}\cdot\boldsymbol\phi\right]
\nonumber \\
&&\delta(\undertilde{\; F}\!{}_1(\boldsymbol\phi+\undertilde{A}\boldsymbol{\theta}_1) - \boldsymbol{p}_1)
\delta(\undertilde{\; F}\!{}_2(\boldsymbol\phi+\undertilde{A}\boldsymbol{\theta}_2) - \boldsymbol{p}_2)
\nonumber \\
&&\det(\undertilde{\; F}\!{}_1\undertilde{A}) \det(\undertilde{\; F}\!{}_2\undertilde{A}) .
\end{eqnarray}
We can now insert into this equation a further factor of ``1''
\be \label{eqa2}
1 =  \int {\cal D} \vec\omega
\delta(\undertilde{\; F}\!{}_3(\boldsymbol\phi+\undertilde{A} {\bf \omega}) - \vec q)
\det(\undertilde{\; F}\!{}_3\undertilde{A})
\ee
and then by interchanging ${\bf \omega}$ and $\boldsymbol{\theta}_1$, and $\boldsymbol{p}_1$ and ${\rm q}$
we see that
$\undertilde{\; F}\!{}_1$ and $\undertilde{\; F}\!{}_3$ are interchanged without altering $Z[\boldsymbol{j}]$, demonstrating that $Z$
is independent of the gauge fixing condition.

It would be interesting to derive a set of WTST and BRST identities associated with the gauge transformation of Eq. \eqref{eq4}
and the gauge choices of Eq. \eqref{eq13}.

\begin{acknowledgments}
We would like to thank CNPq  (Brazil) for a grant and Roger Macleod for encouragement.
\end{acknowledgments}

redpajama_set_name: RedPajamaArXiv