Any concern that is related to the relationship between human beings and the sacred divinity is referred to as religion. A given religion is defined by a given community that is known to have some beliefs. There are various beliefs that are in existence in our modern lives and are seen to develop in a great way. The aspect of religion have become common in our modern lives as there are a lot of believers that are existing.
There are some of the characteristics that are in relation to the religion a point one should bear in mind. For instance, at any time you hear about religion, it is important to note of the existence of the some of the practices that are associated with the religion. One of the concepts that are related to religion is the aspect of faith. These are some of the relations that are in religion at any time you hear about it. The case of the religion brings people together for instance in church where they meet. It is a good idea to understand the existence of the doctrines that are related to religion too.
There are a lot of doctrines and at the same time the practices that are associated with the aspect of the religion whenever you hear about religion. After an investigation being conducted, it is important noting that there I the case of the doctrines and practices not similar to different religions. There are a lot of religions and with which they have brought into place the existence of the various practices. These practices are with the religions that are in place.
Many people have been found with different practices about their religion. There is the case of unity that is brought into existence by the presence of religion. For instance, there is the case of the Parish2Parish that is well known to bring about a vice of the Catholic together at a given diocese. For the people that belong to this religion, it is important to understand that they are known to be together at all times. A point one needs to bear in mind is that Nancy Henry Parish2Parish is one of the cases that is associated with the doctrines of catholic. Nancy Henry, for instance, is a person that is related to the doctrines of Catholic a point one needs to have in place.
The internet has simplified a lot of things and thanks to technology, everything is becoming simpler to complete. Today, any individual who doesn't want to invest a great deal of energy going to physical stores and just wants to purchase a thing can visit an electronic business site and purchase the thing that they need and have it conveyed straight to their doorstep after they have paid for it. Indeed, even much better is the way that individuals are presently sorting out dates using the web through certain dating sites that are solely for this reason. The greater part of these administrations just started with basic matchmaking organizations that in the long run developed into more refined administrations given the requests of the customers. The online dating operation has greatly developed such that today there are sophisticated dating services on the internet and there is website that specifically provides these services. Among these highly sophisticated dating websites is secret benefits that offer those who are interested amazing administrations according to most secret benefits review blogs on the internet. In the accompanying writing, we will address how to access dating sites benefits that many people have profited in well-known online journals on information like secret benefits review. Secret benefits review blogs, as well as internet sites giving detailed information, are very informative as well as helpful to those who are interested.
Similar to any other dating website, a site like secret benefits requires any new member to create a profile that they are going to use when signing in to their services. You will discover certain secret benefits review blogs giving you certain data on the best way of setting up a profile. It is a simple process, and all you have to do is to fill in the data as required. The greatest advantages of accessing such dating sites are that a large portion of them have a few highlights that shield their customers from tricksters who are looking for individuals' information. Most secret benefits review websites will inform interested clients on how to go about using the site which is very simple. Navigation in such sites is simple, and you can go to any area that you need with no hustles.
There are very many dating websites on the internet, and it is up to you to figure out the best one and the one that possesses the best reputation. Also, these dating sites are categorized differently according to the interest of the participating parties so it would be prudent to discover your desires before moving on to a certain service. The best way to comprehend the best services that you can access is visiting audit websites like those that talk about secret benefits review, and you will discover that best among the many. This will also equip you with some background data on how to enjoy the service as a professional.
Whenever a young woman get a Sugar Daddy it simply usually involves a relationship whereby they are able to get different kinds of gifts and lavish lifestyle in return for different kinds of sexual favors for the man. A Sugar the relationship can be very good for person in a number of ways that shall be discussed in this article although there have been very many different kinds of condemnations that have been put up on these kinds of relationships. One thing that is very unique about our Sugar Daddy relationship is that they'll be okay with you even if you go out with your friends to do whatever that you want so long as you're going to give them whatever they need and normally this is the sexual favors that they want from you.Other kinds of relationships usually require very little freedom because the person who wants to know where you're going on what you're going to do their and that is the reason why a Sugar Daddy relationship can be very good for you.
Compared to other kinds of adults jobs, the sugar daddies much better because you are able to stay with that one man without sin very many other men which is something that usually happens in the adult industry. Unlike other kinds of relationships, the moment you are in a relationship with a Sugar Daddy , you can be sure that they do not really care whether you have another man and therefore you do not have any reason to lie to them making it a very enjoyable relationship. Getting into a Sugar Daddy relationship is therefore beneficial in some way.
There are several factors that you should consider when selecting a wedding package. It is normal that people will chose the packages that please them physically. However, there are many other factors that you need to consider. The article below will help you choose the right venue for your wedding.
It is important that you have chosen a Las Vegas wedding package for your wedding. It is very common that people assume that they need to select the right package a long time before the wedding. Finally, this becomes a challenge during the wedding. You have to book the venue as soon as you find it. It is important that you realize that most of the venues are booked a long time before the day of the event.
You should consider the guests who will attend your wedding before selecting the Las Vegas Wedding Packages. It is everyone's expectations that the guests who will attend the wedding will leave the ceremony feeling satisfied. The venue should also make it possible to carry out all the intended activities.
You should also consider the sum of money needed when choosing a wedding venue. Most people tend to choose a venue that they cannot manage to pay for. Lack of funds is so frustrating.
Some venues have their own accommodation while others do not have the accommodation. It is thereby important that you know whether the venue has a convenient accommodation or not. If the venue does not have its own venue, you should seek knowledge about the nearby accommodation that is available. This is to ensure that the guests who will not make it to go back to their homes get a comfortable to spend their nights. The selected accommodation should enhance safety and comfortability of the guests.
You ought to consider the parking area available. It is therefore important that you know the amount of vehicles that will be available during the wedding. The parking space should be safe and ample for the vehicles. It would be a shame if the vehicles are not safe and the guests keep on roaming around their vehicles to ensure that their vehicles are safe.
Did you know that some packages lack the materials shown in the pictures? Most people assume this fact and they end up being so frustrated. Some materials provided in the venue might be much expensive than others. Before deciding the venue, always ensure that the things they are providing are available at the existing rates. You. should source the materials that are not offered by the package early enough.
Putting these highlights into considerations will make sure that you get the best results ever.


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text:
Q: invoking less application from GNU readline Bit support question. Apologies for that.
I have an application linked with GNU readline. The application can invoke shell commands (similar to invoking tclsh using readline wrapper). When I try to invoke the Linux less command, I get the following error:
Suspend (tty output)
I'm not an expert around issues of terminals. I've tried to google it but found no answer. Does any one know how to solve this issue?
Thanks.

A: You probably need to investigate the functions rl_prep_terminal() and rl_deprep_terminal() documented in the readline manual:

Function: void rl_prep_terminal(int meta_flag)
Modify the terminal settings for Readline's use, so readline() can read a single character at a time from the keyboard. The meta_flag argument should be non-zero if Readline should read eight-bit input.
Function: void rl_deprep_terminal(void)
Undo the effects of rl_prep_terminal(), leaving the terminal in the state in which it was before the most recent call to rl_prep_terminal().

The less program is likely to get confused if the terminal is already in the special mode used by the Readline library and it tries to tweak the terminal into an equivalent mode.  This is a common problem for programs that work with the curses library, or other similar libraries that adjust the terminal status and run other programs that also do that.

A: Whilst counterintuitive it may be stopped waiting for input (some OSs and shells give Stopped/Suspended (tty output) when you might expect it to refer to (tty input)). This would fit the usual behaviour of less when it stops at the end of (what it thinks is) the screen length.
Can you use cat or head instead? or feed less some input? or look at the less man/info pages to see what options to less might suit your requirement (e.g w, z, F)?

A: Your readline application is making itself the controlling app for your tty.
When you invoke less from inside the application, it wants to be in control of the tty as well.
If you are trying to invoke less in your application to display a file for the user,
you want to set the new fork'd process into it's own process group before calling exec.
You can do this with setsid().  Then when less call tcsetpgrpp(), it will not get
thrown into the backgroud with SIGTTOU.
When less finishes, you'll want to restore the foregroud process group with tcsetpgrp(), as well.

redpajama_set_name: RedPajamaStackExchange


There is no evidence that "all corporations must extract their pound of flesh to turn a profit". Many corporations do, but many don't. There's no "must" about it. There is increasing evidence – e.g. Reinventing Organisations by Frederic Laloux – that the "some win, some lose" model will, in time, become out of date in the way behaviours in organisations have evolved over the years. When it does, it won't be a moment too soon.
Posted on August 25, 2015 by Ciaran Fenton.	Bookmark the permalink.


"It doesn't matter how much Donald Trump raises from wealthy Republicans and corporate interests, Texans are fighting back and his poll numbers are plummeting. Texas is the biggest battleground state.
"Texans won't sit idly by as Trump steals our land, destroys our healthcare, and threatens to shut down our economy.


text:
Q: Are there ways to run testing scripts on an Android device directly? I am currently testing an app for Android phones using the Espresso library with local devices as well as the Google Firebase Test Lab. For a good portion of these tests to be functional the phone running the test needs to connect to another phone or at least receive feedback from another device. I have been trying to do some research but really can't find anything on what I'm looking to do, seeing that it isn't a common practice.
Is there away to run Espresso or any small script directly on an Android device? I just need a script to sit idle or looping until it receives the information from the tested device, accepts it so the test can continue. I am not trying to alter any direct code in my app to auto accept things, I want to keep the app itself as untouched as possible. And I could manually do it on a small scale, but with Firebase I would like to test lots of devices at once or will run tests daily, sometimes when I'm not there for feedback. I want to automate this process as much as possible, so anything that could do that would help.

A: I've automated this process completely. The best thing is that you don't have to keep busy of your Android Studio and resources. Everything is done remotely.
You can use this plugin to setup Firebase test lab:
https://github.com/piotrmadry/firebase-test-lab-gradle-plugin
Hopefully you have CI (Continuous Integration) for your project.
So after your setup for test lab (you can define as many devices as you want)
You can create 2 parallel jobs on you CI:

*

*First - it would build your project in normal way

*Second - would run android task created by plugin ./gradlew uploadTestLab. After this job you will be able to look at results in Firebase Console.


text:
Metal Gear Solid 5: Producer Responds To Secret Chapter Questions As Fans Rally To "Unlock" It
Reddit seems to think they've cracked at least some of the code in The Phantom Pain.
Posted By Oliver VanDervoort | On 20th, Sep. 2015 Under News
Since Metal Gear Solid: The Phantom Pain was released, there has been quite a few questions about some supposed secret content that can apparently be unlocked. Members of the development team have been hinting at a secret chapter's existence, while other members are remaining steadfastly tight lipped. That has only led to fans working harder than ever to try and figure out just what's going on.
Directly asking producer Ken-ichiro Imaizumi about the new content certainly isn't the answer. Twitter users recently asked him if he could give them any hint at all about where this content is located and how to unlock it. He first answered no comment, and then said he "couldn't tell" us. Both of those answers seem to indicate there is something out there, but he's not going to give us a map to find it. Luckily, there are plenty of resourceful Reddit users out there that are on the case.
A thread has been dedicated to finding out just where this secret chapter went, as well as why it went missing at all. As the Reddit thread points out [there is even a whole sub reddit dedicated to the cause], it seems like people would have been able to find it by datamining the PC version of Phantom Pain. The OP posits that part of the reason the PC version's release date got moved up is because all references to this secret missions were removed. Those who have been following the development of the game have noted that the computer version was originally supposed to come out two weeks after the console version.
This has led to people thinking the secret chapter i.e. Chapter 3 titled Peace has been expertly buried and is just waiting to be dug up. The lack of flat-out denials seems to be a hint. The lack of confirmation appears to, strangely be one as well. We'll just have to wait and see if someone can find the elusive missing content in Metal Gear Solid 5: The Phantom Pain.
We will see how it all pans out. Regardless, The Phantom Pain is one of the year's best game.
Sorry, I can't tell you. https://t.co/v7FxjVtrJ0
— Ken-ichiro Imaizumi (@Ken1555) September 19, 2015
Sorry no comment. https://t.co/vwOTGxtNZY
Tagged With: konami, Metal Gear Solid 5: The Phantom Pain, pc, ps3, ps4, xbox 360, Xbox One
Metal Gear Solid V: The Phantom Pain
Publisher: Konami
Developer: Kojima Productions
Platforms: Xbox One, Xbox 360, PS3, PS4, PC
Destiny 2 Xur Exotics: Hard Light, Gemini Jester, Wings of Sacred Dawn
Monster Hunter World – All Seasonal Events Return Starting July 26th
Destiny 2 Season of Opulence Guide: How to Earn the Lumina Exotic Hand Cannon
Blazing Chrome Review – Hard Corps.
PS5 And Xbox Scarlett's SSD Will Have Biggest Impact On Open World Games, Says Exception Dev

redpajama_set_name: RedPajamaCommonCrawl


text:
I-Team investigation: Discipline isn't always uniform when police break the law
Posted: 6:00 AM, Oct 30, 2017
By: Craig Cheatham , Dan Monk , Brian Niesz
Over the last six months, the WCPO I-team has collected records from 40 different police departments and reviewed thousands of disciplinary cases involving officers. Our motives are simple: We want to make sure the people who protect us and enforce our laws are worthy of the high level of trust the public gives them. Read more about this project and why we are doing it here .
CINCINNATI -- Corrections Officer Calvin McIntosh grabbed a man by the shirt, led him down a corridor and shoved him into a door at the Middletown City Jail.
The man, Michael Holloway, later told a police lieutenant McIntosh twisted his shirt so tightly it choked him. According to an internal investigation, he also told the lieutenant that McIntosh punched him after he was inside the cell.
"I'm thinking if I do anything at that time, my life is in danger," Holloway told the I-Team.
The internal investigation found McIntosh used excessive force. It was his 29th reported use of force in his three and a half years with the Middletown Police Department. That was more than double the incidents involving all other corrections officers -- combined.
McIntosh's performance evaluation, just a few weeks later, found he "needs improvement."
Two weeks after that, he got a raise.
Discipline for excessive force varies widely in the Tri-State, from a conversation to termination. Middletown's police chief suspended McIntosh for a day for his treatment of Holloway.
In Colerain Township, internal investigations found Officer Joseph Redmond inappropriately used a confidential police database to get personal information about two women. Prosecutors in Ohio and other states have charged officers with felonies under similar circumstances.
Instead, Redmond resigned and went to work for another local police department.
A monthslong investigation reveals huge differences in the way police departments discipline their officers for misconduct, both on and off the job.
The I-Team reviewed thousands of disciplinary records from 40 police departments serving the Tri-State, focusing on the agencies in seven metro area counties in Ohio and Kentucky. Reporters studied thousands of incidents involving police in large and small law enforcement agencies.
We weren't sure what we would find when we began collecting these records, but our goal was making sure the public was aware of how law enforcement agencies handle discipline.
The records show long suspensions for some officers who were chronically overweight, but slaps on the wrist for others who used excessive force. Some were convicted of crimes; we found others engaged in behavior that could be considered criminal but were not charged or prosecuted.
"There is supposed to be something in line that polices the police," Holloway said, "but it's not working."
Criminal charges, but discipline varies
Some of the biggest differences in how departments handled disciplinary cases showed up in crimes involving alcohol. We determined 38 disciplinary cases were alcohol-related. Nearly three-quarters of those were in the Cincinnati Police Department and the Hamilton County Sheriff's Office.
Hamilton County Deputy Bobby Colwell was drunk and causing a scene at a Monroe bar in 2016, records show. He told police he was disorderly and had two knives -- and they should arrest him. One officer told Colwell an arrest would hurt his law enforcement career.
According to a police report, Colwell replied: "It's Hamilton County. I won't get fired."
He was right. Colwell was arrested, booked into the Butler County Jail and pleaded guilty to disorderly conduct. But as he predicted, Sheriff Jim Neil did not fire him. In fact, Neil didn't even suspend the six-year veteran.
We first reported on the sheriff's discipline for alcohol-related cases in May. After that initial story, we wanted to know: How do other agencies handle similar incidents? We found a variety of approaches, but some other agencies hand out much more stringent punishment for officers who committed similar crimes.
As of last May, six Hamilton County sheriff's employees -- five deputies and one civilian -- had been charged with operating a vehicle under the influence since Neil took office in 2013. Two of those deputies were arrested for OVI twice; they pleaded down their first charge to reckless operation. The second time they were arrested, Neil didn't suspend either of them. Instead, they received written reprimands.
Neil issued written reprimands to two others, as well. And he suspended a corrections officer and a civilian employee for their OVI arrests.
No one was fired.
In the records we reviewed for the past four years, just one officer lost his job: That was Indiana State Trooper Justin Butler. In 2015, he was found to have operated a motorboat with a blood-alcohol content of .08. An internal report found Butler got belligerent with the officers who'd stopped him for going over the idle speed limit and said he'd never back up the arresting officer on calls.
How departments handle alcohol-related discipline
Police discipline in general is a "mish-mash," former Hamilton County prosecutor Mike Allen said.
"It would be better if there was (more consistent discipline), but I don't know that it's practical to expect that," he said. "Every case is different, every police department is different."
Of the 37 other alcohol-related cases, departments issued 21 suspensions and 11 written reprimands, and provided counseling in three cases. For a case in Norwood and another in Hamilton County, the records didn't have enough information to determine the outcome.
While officers in all other cases kept their jobs, some agencies' discipline was more severe than others.
In Warren County, Sheriff Larry Sims fired Corrections Officer Andrew Ritter after the Ohio State Patrol arrested him on an OVI charge in 2015. Ritter pleaded guilty to reckless operation. During arbitration, Ritter's termination was lowered to a suspension.
"The thing about all of these police discipline situations, whether it involves criminal charges or administrative, there's no uniformity at all." - former prosecutor Mike Allen
The Florence Police Department suspended Officer Alexander White for 16 days after he got into an off-duty crash in Erlanger. It damaged his vehicle and some landscaping. Erlanger police listed alcohol as a contributing factor.
In Hamilton County, Neil and Chief Deputy Mark Schoonover said they're working within boundaries established by union rules, arbitrators and a sense of what's right based on the deputies' work history and the seriousness of their actions.
"Your reputation is everything in this work," Neil said.
But two law enforcement experts, one a civilian and the other a retired police chief, said the sheriff's discipline when it comes to drunken deputies doesn't go far enough.
If any officer is arrested for drunken driving or convicted of a misdemeanor, retired Woodlawn Police Chief Jeff Witte said he believes that officer should be suspended or fired.
Criminal justice expert Christine Cole agreed.
"It's really hard for the community to trust the police if the police can't even trust the system in which they work to be consistent and have integrity," Cole said. "It seems to me that there's a lack of that in this agency."
'He should have been charged with an assault'
Our review found 72 "use of force" violations among 18 agencies since 2013. Nearly all involved complaints of excessive force -- officers kicking or punching suspects, slamming inmates into floors or walls, or in one case, grabbing an inmate by his genitals.
Even when investigators determined an officer violated policy, using excessive force to hurt suspects or inmates, none was criminally charged or fired.
Video recorded Holloway through the booking process.
On Feb. 5, 2016, Holloway was in Middletown City Jail's booking room for 2 minutes, 26 seconds. He was there because he failed to appear in court over a petty theft.
McIntosh's search lasted 21 seconds.
According to an internal investigation, he claimed Holloway took his hands off the door and tried to turn around. Surveillance video proved that was a lie.
McIntosh then shoved Holloway into a cell door, the video showed, then into the cell itself. Video shows McIntosh went into the cell and stayed there with Holloway for 25 seconds.
In the internal investigation, Holloway claimed McIntosh punched him in the back before video showed McIntosh slam the cell's door so hard it didn't latch shut. Holloway has chronic pain in his shoulder and back. He told McIntosh about the problem, but both Holloway and another officer said McIntosh didn't care.
"It hurt bad enough that I was crying," Holloway said. "It literally put me in tears. It put me to my knee."
Lt. Leanne Hood, who investigated McIntosh's use of force, found him guilty of an "unreasonable and unnecessary use of force" for how he grabbed Holloway's shirt and for slamming him into the door. She couldn't verify Holloway's claim McIntosh had punched him.
Footage showed McIntosh push Holloway into a door and then into the cell.
Middletown police suspended McIntosh for a day without pay -- but allowed him to use holiday pay so he wouldn't lose any money. The department sent him to a psychologist to see if he was mentally fit for duty; the psychologist found he was.
Less than three months after the incident at the jail, McIntosh resigned.
The police department never referred the case for an independent investigation or possible prosecution. Chief Rodney Muterspaw and City Manager Doug Adkins initially agreed to talk with us about what happened. Then later, they refused.
But Monday morning, after this story published, Adkins posted a lengthy blog post responding to WCPO's requests for information:
"We definitely make mistakes," Adkins wrote. "But according to our citizens, we don't make too many of them. Using the 8 sustained complaints, we make an average of approximately 13,551 calls between sustained complaints. I'm not sure human beings in daily stressful situations can do much better. When it does happen, we use discipline where appropriate, to correct the behavior and to prevent recurrence of the improper conduct. Where appropriate, we also remove officers from duty.
"My understanding is that WCPO wants to focus on two complaints they believe were not handled appropriately. That takes us to two incidents, more than a year old, in 108,409 calls for service in which WCPO believes we acted inappropriately. Said differently, using WCPO standards, even when we made mistakes that required discipline, we correctly handled 108,407 out of 108,409 calls for service."
Holloway said the police department refused to give him a copy of its internal investigation into what McIntosh had done to him. He only saw the report after we showed it to him.
"It's an outrage," Holloway said. "What (McIntosh) did, he should have been charged with an assault with intent, because he did everything he could to make sure that I was in pain and that I was hurting."
Documents show McIntosh's rapid sequence of discipline, then a raise, and then his resignation.
The trouble in excessive force cases is that they're difficult to prove. Allen said Ray Tensing's trial -- though he thinks Tensing was "clearly over-indicted" -- illustrates the point.
"It's not to say you have a policy -- and I wouldn't think that any prosecutor's office would have a policy of just ignoring it -- but you have to factor in what are the chances of a conviction," he said.
We were able determine how officers were disciplined in 38 of the 72 cases that involved use of force:
17 cases resulted in some form of verbal interaction, including reprimands and counseling.
Written reprimands were issued to 11 officers.
Nine were suspended -- eight of them for four days or less. One Hamilton County Corrections officer was permitted to use accumulated leave time to cover his 15-day suspension.
One corrections officer was headed for likely termination, but he resigned first.
Six officers were completely exonerated. Many of the officers who were disciplined were cleared of using excessive force, but departmental reviews found fault with their use of language during the incidents or how they followed procedures after.
In at least 28 of the 72 incidents, the public records obtained by WCPO are not complete enough to determine how departments evaluated allegations of excessive force.
Possible crimes, but no charges
In Covington, Florence Police Officer Samantha Riley was at a Waffle House early on the morning of April 18, 2013. She'd gone there with her wife and a group of friends after spending the night at two bars.
At about 2 a.m., her wife got into an argument outside the restaurant, where she'd gone to smoke a cigarette. Covington police arrested her wife on two charges: public intoxication and disorderly conduct.
"Both Covington officers stated that if she wasn't a police officer she too would have been arrested." - Florence Police disciplinary record
Riley cried and pleaded for the officer to be lenient with her wife, a friend later told her. Riley didn't remember doing that but admitted she was intoxicated.
The friend said one of the officers was rude, at which point Riley got angry: She called him a "fag" and an "idiot" several times. The officers told Riley to leave -- that if she didn't, she'd be arrested for her disruptive behavior -- but she didn't comply.
According to the Florence Police Department's disciplinary record, she told them several times she was a police officer. They even called a supervisor in case they had to arrest her.
Eventually, she left.
"Both Covington officers stated that if she wasn't a police officer she too would have been arrested," Riley's disciplinary record says. She signed that document a week after the incident, saying she was guilty of violating the Florence Police Department's rule for unfavorable conduct.
The department suspended her for four days without pay, but waived three of those if she didn't get into trouble for the next two years.
Two years ago, a Hamilton County internal investigation determined Deputy Donald Fore was drunk when he walked up to the sheriff's station in Anderson Township. At the time, he was on court-ordered probation for an OVI conviction. According to other deputies' statements and the internal investigation, Fore was belligerent, refused orders to go home, shoved a higher-ranking officer and punched a wall inside the building.
A surveillance camera recorded Donald Fore in the parking lot.
The internal investigation found Fore's action "could have supported a criminal charge." But he wasn't arrested. Instead, he was suspended for 10 days without pay.
"It may not seem fair to you or to others, but under the circumstances and everything I had to look at and take into consideration, that's how I came by the recommendation for discipline. I'll stick by it today," Schoonover said. "I think it was a fair recommendation."
At Kings Island two years ago, Hamilton County Sheriff's Office records show park police interviewed a couple while their friend, Hamilton County Cpl. Tim McCalla, was in the next room yelling at Kings Island officers. Park police had removed McCalla, his girlfriend and the couple for drinking alcohol in a line waiting for a ride and being disruptive.
In the Kings Island police office, McCalla's friends urged officers to let them calm him down. The Kings Island police report said McCalla could have been arrested for disorderly conduct, but he wasn't.
Hamilton County Sheriff's Office records show McCalla wasn't suspended, either. The sheriff's office gave him a written reprimand.
In October 2015, the Hamilton County Sheriff's Office suspended a data entry operator 15 days after he got into a fight with his neighbor -- his fourth alcohol-related disciplinary violation since August 2012. The sheriff's captain who responded to the call found both men had committed disorderly conduct, but they decided not to charge either of them.
When the prosecutor doesn't follow through
We also wanted to know what happens when a department refers a case for prosecution. Often, but not always, prosecutors declined to bring cases to trial.
In 2014, a Colerain Township police investigation concluded that ex-Sgt. Joseph Redmond used a confidential law enforcement database to get information related to his former fiancee. She accused him of stalking her, an allegation he denies.
Other Ohio officers have been charged with a felony or forced to resign -- and give up their ability to be a cop -- for database violations. But the Hamilton County Prosecutor's Office declined to file charges against Redmond. The department suspended him without pay for a week.
A year later, a police investigation found he did it again -- this time the information was connected to a different woman who also accused Redmond of stalking her. He denied the stalking claim, but she took out a restraining order. The Hamilton County prosecutor declined to prosecute that case, too.
Redmond said in an interview Colerain Township forced him to resign. The New Miami Police Department hired him; its chief lobbied the Ohio State Highway Patrol, which manages access to the database, to let Redmond back in. Records show OSP agreed, but stipulated New Miami would be liable for any misuse.
Letter reinstating Joseph Redmond's LEADS access.
Allen said it's rare for someone banned from the database to get access again. "I'm a little bit surprised by that," he said. "I don't really understand that."
After eight months, Redmond resigned from New Miami. He continued to work as an adjunct instructor at the Butler Tech Police Academy until Wednesday, a day after we contacted him for comment. A Butler Tech spokesman said Redmond resigned.
In March, a Blue Ash police internal investigation determined that former officer Chris Zielinski used that same database 15 times to get information about his girlfriend and her estranged husband, even though he didn't need it for a law enforcement purpose.
Like the Colerain Township case, Zielinski could have faced criminal prosecution. He didn't: According to Blue Ash police records, the Hamilton County Prosecutor's Office agreed to not file charges against Zielinski if he resigned, which he did. He declined to comment for this story.
It wouldn't be unheard of for someone to face prosecution for unauthorized access, Allen said: He had a few cases that resulted in indictments.
In another case, Mark Myers, 62, alleged he suffered cuts to his head and a broken hip when Jason Mize, a Hamilton County corrections officer, shoved him into a cell. Myers was being booked on a misdemeanor theft charge last August; he was later acquitted.
Footage shows Mize shove Myers into a cell.
According to Myers' federal lawsuit, Mize left him bleeding on the floor and slammed the door. His actions, the lawsuit states, lacked "even the most basic humanity."
When Myers cried out for help, a jail nurse called for a life squad. She recalled telling a co-worker, "I hope he's not dead."
Maj. Charmaine McGuffey, in charge of the jail at the time, called for Mize to be arrested and fired. It was his fourth use-of-force violation since the sheriff's office hired him in August 2007.
Myers' injuries were so serious the sheriff's office sent the case to the Criminal Investigation Section. Last December, the Hamilton County Prosecutor's Office declined to present the case to a grand jury, even though Myers wanted Mize to be charged.
"The sheriff's office did everything they could possibly do and went through every phase of the process, and it was turned down by the prosecutor's office," Schoonover said. "I can't change that."
Mize resigned from the sheriff's office Feb. 25.
"He was facing termination," Neil said. "It never happened because he resigned."
Getting rid of bad cops
Allen handled cases involving police during his five years as prosecutor. Sometimes, he said the best outcome is for an officer facing prosecution to give up his law enforcement certificate. It means that officer can't be a cop anymore.
"They're giving up their livelihood. They're giving up their ability to feed their families," he said. "It is a big punishment."
In both cases involving inappropriate use of the police database, neither officer had to give up his certificate.
Cole is vice president and executive director of the Crime and Justice Institute, which provides nonpartisan policy analysis, consulting and research on public safety. She is a national expert on best practices for police and she co-authored landmark studies of the Department of Justice Consent Agreement with the Los Angeles Police Department, as well as the police response to the Boston Marathon bombing.
"It's really hard for the community to trust the police if the police can't even trust the system in which they work to be consistent and have integrity." - Christine Cole
She reviewed hundreds of pages of Hamilton County Sheriff's Office personnel files, discipline records and sections of internal affairs investigations when we looked into excessive force in May.
In those cases, she said agencies need to hand out discipline in a predictable, consistent way.
Sometimes police agencies hurt themselves by not being more open, Allen said.
"I think police officers and administrators, by virtue of who they are and the job they have to do, maybe aren't as transparent at times as the community would like," he said.
Still, Allen said the public and media don't often appreciate that police work is a tough job, and "when you're going to judge a police officer, you have to put yourself in their shoes."
Even a written reprimand, which might seem like a slap on the wrist to the public, is taken seriously, he said. If an officer stays with a department for decades, a reprimand can harm his or her career advancement.
"I don't think it's anything they blow off at all," he said. "Come promotion time, it's important to them because that becomes part of their permanent personnel record, just as a letter of commendation would."
WCPO web editor Abby Anstead, as well as freelance journalists Laura Consolo, Kevin Eigelbach,Hannah Hagedorn and Roxanna Swift, contributed to this report.
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Policing their Own


text:
Movies, News-2017
James Cameron And Tim Miller Talk 'Terminator' Reboot: 'The Machines Have Already Won'
Date: September 27, 2017Author: Johnnyblue1 Entertainments & Lifestyles 0 Comments
by Rachel West
Thirty-three years after Arnold Schwarzenegger burst onto the scene as a cyborg from the future, sent to eliminate Sarah Connor (Linda Hamilton) in "The Terminator", the franchise is getting yet another reboot at the hands of "Deadpool" director Tim Miller and James Cameron who will serve as a producer.
"It made sense for me to see if there was a way to bring it into this century and to relevance," Cameron tells The Hollywood Reporter. The Canadian-born director, 63, has been secretly working alongside Miller and a team of writers to help usher a new "Terminator" film into being. Finding inspiration wasn't hard for Cameron, who had to look no further than what was happening in the world around him.
"What was science fiction in the '80s is now imminent. It's coming over the horizon at us. And there's been a resurgence of fear and concern about nuclear weapons and so on. So all of these apocalyptic elements are out there," he explains. "The first two 'Terminator' films that I did, dealt with the angst around that and how we reconcile it for ourselves in a fantasy context. So I got excited about the idea of finding a story that made sense for now."
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"The [first] films are more relevant today than they were when he made them. A lot of it seems like prognostication because it's coming to be — the world we live in right now," Miller adds. "Technology has always scared me, and it's always seduced me," says Cameron.
Following three unsuccessful sequels – including the most recent reboot, 2015's "Terminator Genisys" – Cameron wants to wipe the slate clean, acknowledging that the post "Terminator: Judgement Day" movies were failures.
"This is a continuation of the story from 'Terminator 1' and 'Terminator 2'. And we're pretending the other films were a bad dream. Or an alternate timeline, which is permissible in our multi-verse," he tells THR. "This was really driven more by [Tim] than anybody, surprisingly, because I came in pretty agnostic about where we took it. The only thing I insisted on was that we somehow revamp it and reinvent it for the 21st century."
RELATED: Josh Brolin Says James Cameron Called Him Names After He Turned Down 'Avatar 2' Role
"Look around in any airport or restaurant and see how many people are on their phones. The machines have already won. It's just [that] they've won in a different way. We are co-evolving with our technology. We're merging," Cameron says, revealing he's brought in several experts in artificial intelligence and science to speak to the "Terminator" team.
However, more nerve-wracking than a future filled with robots was asking original franchise stars Schwarzengger and Cameron's ex-wife, Hamilton back.
Schwarzenegger was an easy ask, with the actor just assuming he would return. But asking his former wife, whom he was married to from 1997 to 1999, was a daunting prospect. "Jim was f***ing terrified," Miller says.
RELATED: Patty Jenkins And Paul Feig Hit Back At James Cameron After Calling Wonder Woman 'An Objectified Icon
"It took me a week just to get up the nerve," Cameron admits. Hamilton's return as Connor was confirmed last week. "Linda and I have a great relationship. We've stayed friends through the thick and thin of it all. And she is the mother of my eldest daughter."
"As strong a character as she was, as meaningful as she was to gender and to action stars everywhere, I think it's going to make a huge f***ing statement to have her be the really seasoned warrior that she's become," Miller adds.
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Psychiatry Investigation (PI) has been published biannually since August 2004 as an official English journal of the Korean Neuropsychiatric Association (KNPA) for the purpose of dealing with unique regional psychiatric issues. Under the leadership of the KNPA president Prof. Yong Sik Kim, Prof. Byoung-Hoon Oh became the founding Editor-in-Chief of the Journal. Launching on a new English journal was not an easy task and rather very challenging one. The editorial team under the pioneering leadership of Prof. Oh invested significant personal time, efforts and resources into PI.
After 5 years of publication, PI became indexed in Science Citation Index-Expanded (SCIE) in April 2009 thanks to profound contribution of the second Editor-in-Chief, Prof. Chan-Hyung Kim and his editorial board members. It was not only a success of editorial team but also a success of all the KNPA members.
From 2008, PI has been publishing quarterly and many papers with high quality from all over the world have been submitted for publication. Currently, PI is under evaluation to be indexed in PubMed Central by the National Institute of Health (NIH), USA. If PI can be indexed in PubMed Central, the papers in PI can be searched in PubMed browser of NIH and researchers all over the world can access the full-text papers of our journal for free. Being a PubMed Central journal would be another success of PI and KNPA.
However, our challenge of PI does not end here, it is only a beginning. Our next goals remain to get the journal indexed in the SCI core and Medline. To achieve these goals, increasing citation from researchers is crucial. The citations received by PI have increased over the last few years, but it is still not enough. More citations are needed to reach our goals.
For these purposes, we should publish highly qualified papers in the Journal. I have plans to increase current rejection rate of around 15% up to 30% in the near future. Considering rapidly increasing numbers of paper submission, it would be possible. Highly qualified review articles and original articles are invited and very welcomed to the Journal, which would contribute on increasing citations of PI. On the other hand, keeping the uniqueness of scope in psychiatric field is also important to be a renowned world class journal. PI will continue to focus on the cross cultural psychiatry and ethnic issues in psychiatry in Asian countries as well as general psychiatry and neurosciences, which is our unique scope comparing to other journals.
Our new editorial team will do our best to achieve these goals for the further development of PI, and we look forward to informing you more about our plan and hope in the actual forthcoming issues.


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text:
TSNN News
This program will be distinguished in its value with industry-first recognized certification for the program.
Both associations aim to announce the launch of the joint 'Asia Pacific Executive Development Programme' at the upcoming UFI Asia Pacific Congress 2019 in Japan.
Aloysius Arlando, president-elect, SACEOS, welcomes the co-operation.
"It is the mission of SACEOS to raise the industry's professional standards and enhance the mastery of skills, over and above what is in the marketplace," Arlando said.
He added, "The skills, passion and contributions of every individual will drive Singapore's next phase of development towards an advanced economy and inclusive society. Our collaboration with UFI will allow us to collaborate on education, talent development, and peer to peer exchanges - working on the foundational of professional training in exhibition. This enhanced skills development will help Singapore's MICE professionals in increasing skills elevation and job opportunities."
Kai Hattendorf, managing director/CEO, UFI, welcomes the co-operation.
He remarked, "It is UFI's mission to connect and serve the exhibition industry globally. Our collaboration with SACEOS will allow both our associations to do this more efficiently, tapping on research, and nurturing more industry professionals in Asia and globally."
SACEOS is on track to be the centre of excellence for developing skilled talent, imparting knowledge, and creating new opportunities for industry professionals.
This further strengthens Singapore's position as the Asia-Pacific hub for professional and skills development for the MICE and events industry.
Andrew Phua, Director, Exhibitions and Conferences, Singapore Tourism Board (STB), said: "The new programme will strengthen Singapore's position as the Asia-Pacific hub for MICE training and development. With more training opportunities in the pipeline, MICE players will be able to deepen their knowledge, expand their skillsets and further elevate the standards of the MICE industry in Singapore and around the region. We invite industry professionals to participate actively to further enhance their capabilities."
LRP Publications Buys Singapore-based HR Events From Diversified
U.S.-based LRP Publications has added Singapore-based HRM Asia, a business unit of Diversified Communications, to its human resources-focused portfolio. The new entity…
SACEOS and SISO Forge Alliance to Bring their Members Closer Together
SACEOS, the Singapore Association of Conventions, Exhibitions and Suppliers and SISO, the Society of Independent Show Organizers, have jointly signed an agreement to share…
Tourism Vancouver Inks Technology Deal with Tencent
Last month, Tourism Vancouver signed a pioneering technology deal with China industry giant Tencent in an effort to attract more Chinese tourism, now known as the world's…
UFI's 5 Trends to Watch in 2016
The start of the year is always a good time to look ahead. Here is a brief look at five trends affecting our industry – trends that we at UFI believe will be discussed and…
UFI's "5 Trends to Watch in 2018"
UFI, the Global Association for the Exhibition Industry has taken a look into their crystal ball and come up with "5 Trends to Watch in 2018". The good news is the…
By Kai Hattendorf, UFI CEO 2018 has become a memorable year for the exhibition and business events industry around the world – with much of the attention on M&A, on…


text:
Bachelor of Applied Science Degrees
The Bachelor of Applied Science (BAS) degree is a 180 credit baccalaureate degree, specifically designed to build on professional-technical associate's degrees that provide workplace skills, such as Associate in Applied Science-Transfer (AAS-T) degrees. BAS degrees include a professional core of courses from the AAS-T degree, general education credits, and upper division courses. BAS degrees are a pathway to the baccalaureate level with upper-division coursework, in an applied field, that provide expanded career opportunities for graduates and meet the needs of employers in the community.
Associate in Arts degrees are designed to provide students with a broad background during their first and second year of study so that they can transfer to a four-year school with standing as a junior. Our degrees follow guidelines set by the state's Intercollege Relations Commission. Our associate degree curriculum is designed to give students a general education that transfers to four-year universities for bachelor's degrees.
Associate in Science-Transfer Degrees
Associate in Science-Transfer degrees are designed to prepare science and engineering majors for transfer to a four-year school with standing as a junior. All of our Associate in Science-Transfer degrees adhere to guidelines developed under the guidance of the Washington State Board of Community and Technical Colleges. Most coursework is in mathematics, science, and engineering but the curriculum also includes additional general education requirements.
Direct Transfer Agreement
For those who qualify, the Direct Transfer Agreement (DTA) gives students priority admission and general education for most Washington state universities. Students must have the AA degree, be a Washington state resident, and meet the minimum GPA for their chosen university. Students who complete this path and are accepted at a four year university will be ready for their junior year at all public and participating private colleges.
Major Related Programs
Major Related Program (MRP) pathways are transfer associate pathways outlining the appropriate courses in order for students to be well prepared to enter a major upon transfer – Major Related Program (MRP) pathways follow one of the two Washington statewide transfer agreements – the Associate in Arts DTA format or the Associate in Science-Transfer (AS-T) format.
Associate in Applied Science-Transfer Degrees
Associate in Applied Science-Transfer degrees are built upon the technical courses required for job preparation; however, they also include a college-level general education component, a common in structure for all such degrees. The general education courses for the degrees are drawn from the same distribution requirements list as those taken by students completing the Associate in Arts or the Associate in Science-Transfer degrees. Associate in Applied Science-T degrees prepare graduates for jobs requiring two years of training or for transfer to four-year schools with specific bachelor's programs that accept this degree.
Associate in General Studies Degree
The Associate in General Studies degree grants students academic recognition for an individually designed program of course work. This course work is designed for students not planning to transfer to a four-year school.
Associate of Technical Arts Degrees
Associate of Technical Arts degrees are designed to provide professional and technical training to prepare students for specific jobs or to improve existing skills. All of our career programs have advisory committees of professionals in related fields to help ensure that our curriculum evolves with changes in business and industry. Advisory committee members and faculty members work together to link education and employment and help students succeed.
Certificates are shorter programs and are designed to provide specialized training and skills in a number of interest areas.
Certificates of Completion (COCs) are professional-technical programs of less than 20 credits. The courses are targeted to help students gain skills in a specific area. COCs are not eligible for financial aid; however, some COCs may be eligible for veteran's benefits. In addition, some COCs can be applied to certificates (programs of 20 or more credits) or degrees. If interested in a COC, please inquire at the appropriate instructional department or academic advising.
Diplomas are granted for successful completion of high school diploma programs at the college. Students can earn a high school diploma through four different programs: Adult High School, Edmonds Career Access Program (EdCAP), HS21+, and International High School Completion. Each program has separate admission and completion requirements. Successful completion of any one of the four programs will earn a student a high school diploma authorized by the state of Washington. Students may also earn a diploma through rules set in State House Bill (SHB) 1758 . In addition, General Equivalency Degree (GED) preparation classes are also offered for students needing an alternate credential to a high school diploma.


This planning tool can be used to plan a Tupe transfer, whether you are the Transferor (transferring employees out to another organisation) or the Transferee (transferring people into your organisation from another employer). The tool should be used in conjunction with the 'How to manage a Tupe transfer' guide and highlights key resources that you may wish to draw on at different stages of the process.
This visual guide sets out the key pieces of activity involved in both sides of a Tupe transfer and should be used alongside the Tupe transfer planning tool.
Downloadable and customisable documents relating to planning Tupe transfers.


text:
\section{Introduction}

What is the effect of interactions on Anderson localization? One common wisdom is that any amount of interaction will give rise to collective excitations that could assist transport at non-vanishing temperature even if single particle states are all localized. But the belief, that there are no strict many-body insulators at $T>0$, has been challenged by theoretical arguments, dating as far back as Anderson's original paper, which suggest a many-body localization transition marking a critical point in the transport properties of a closed quantum system\cite{Anderson1958,Basko2006}. The idea has recently gained support from numerical studies \cite{Oganesyan2007,Monthus2010,Pal2010,Canovi2011}. Furthermore, simulations of one dimensional systems have revealed remarkably universal behavior of the dynamics in the putative many-body localized state\cite{Chiara2006,Znidaric2008,Bardarson2012}. For example the time evolution following a quench from a state with fixed particle positions shows blocked particle transport accompanied by unbounded logarithmic growth of the entanglement entropy.

In this paper we formulate a real space renormalization group (RG) scheme that describes the time evolution of a random spin chain on multiple time scales. For certain initial conditions we can establish a many-body localized state as an infinite randomness fixed point of the dynamics near which the RG scheme is asymptotically exact. The results of this theory exhibit many of the universal features observed in the numerical simulations\cite{Chiara2006,Znidaric2008,Bardarson2012}, although they are derived for a somewhat different model.
As our starting point we consider the Hamiltonian of the random spin-$1/2$ XXZ chain without local Zeeman fields:
\begin{equation}
H = \sum_i \frac{J_i}{2} \left(S^+_i S^-_{i+1}+S^-_i S^+_{i+1}+2 {\Delta}_i S^z_i S^z_{i+1}\right).
\label{eq:Hamiltonian}
\end{equation}
The couplings $J_i$ and anisotropy parameters ${\Delta}_i$ on sites $i$ are random variables drawn from uncorrelated probability distributions. The couplings may be positive or negative and we assume $|\Delta_i|<1$. The spins in (\ref{eq:Hamiltonian}) can be mapped using a Jordan-Wigner transformation to spinless fermions with nearest neighbor interactions, subject to bond disorder.

To study the propagation of information through the chain we investigate the time evolution of the system starting from a non entangled initial state, which for simplicity we take as an  antiferromagnetic Ne\'el state with spins pointing along the $z$-axis. We shall see that this choice of initial state greatly simplifies the scheme and allows us to obtain well controlled results for the dynamics at long times.

\noindent{\em RG scheme --} Before proceeding with the details, let us outline the idea underlying the RG solution of the time evolution. As in the standard strong disorder RG scheme\cite{Dasgupta1980,Bhatt1982,Fisher1994}, we take advantage of the large local separation of energy scales induced by the randomness to gradually eliminate degrees of freedom. However, instead of targeting the ground state of the system, our aim is the time evolution of the chain starting from a specified initial state. The dynamics at the shortest time scales are oscillations of frequency ${\Omega}$ performed by the most strongly coupled pairs of spins on the chain, which are effectively decoupled on these time scales from their typically much slower neighbors. On time scales longer than ${\Omega}^{-1}$ the rapid oscillations performed by the strong bonds can be eliminated using time dependent perturbation theory, which leads to renormalization of the coupling between the slow spins. In this way we gain the essential information about the dynamics of the chain at all scales. If the distribution of coupling constants flows to a wide distribution at the dynamical fixed point, then the perturbative RG approach becomes increasingly well controlled, or even asymptotically exact if the system flows to infinite randomness\cite{Fisher1994}. Similar ideas have been applied to solve classical dynamics in certain disordered\cite{Fisher1998,Lee2009} as well as clean\cite{Mathey2010} systems, but to our knowledge not to quantum dynamics.

We now apply this scheme to the Model (\ref{eq:Hamiltonian}) with a staggered (Ne\'el) initial state. The strong bond, with exchange coupling denoted by ${\Omega}$, then always connects a pair of anti-aligned spins. At time scales of order $\Omega^{-1}$ the strong pair is effectively decoupled from the neighboring spins that are presumably connected to it by much weaker couplings. The only significant dynamics in this neighborhood of the chain is the rapid oscillation of the strong pair with frequency ${\Omega}$ between the $\ket{{\uparrow}{\downarrow}}$ and $\ket{{\downarrow}{\uparrow}}$ states.

The effective Hamiltonian for the dynamics at time scales much larger than ${\Omega}^{-1}$
is derived using time dependent perturbation theory in the coupling of the strong pair to the rest of the chain. Specifically, we move to the interaction picture with respect to the Hamiltonian of the strong pair and compute the evolution of the density matrix $\rho(t)= U_I^\dagger(t)\ket{\psi_0}\bra{\psi_0} U_I{^{\vphantom{\dagger}}}(t)$ up to second order, while averaging over rapid oscillations of frequency ${\Omega}$. The resulting time evolution can be matched term by term to an effective time evolution $\exp(-iH_{\text{eff}}t)\ket{\psi_0}\bra{\psi_0} \exp(iH_{\text{eff}}t)$. Therefore this procedure amounts to derivation of an effective Hamiltonian.

At this order of perturbation theory the $\ket{{\uparrow}\ua}$ and $\ket{{\downarrow}\da}$ are not populated and therefore truncated from the Hilbert space. The retained states $\ket{\pm}=2^{-1/2}(\ket{{\uparrow}{\downarrow}}\pm \ket{{\downarrow}{\uparrow}})$ of the strong pair can be taken as the ${\uparrow}/{\downarrow}$ states of a new pseudo spin variable $\vec{S}_n$, which initially points along the positive or negative $x$-axis. The effective Hamiltonian derived in this procedure for our model is then given by:
\begin{equation} \label{eq:Heff}
\begin{split}
H_{\text{eff}} &=H_\text{chain} + h_n S^z_n+\frac{J_L J_R}{2\Omega(1-{\Delta}_S^2)}\left(S_L^{+} S_R^{-} + S_L^{-} S_R^{+}\right) \\
&+\frac{{\Delta}_S J_L J_R}{2\Omega } \left[\frac{S_L^{+} S_R^{-} + S_L^{-} S_R^{+}}{(1-{\Delta}_S^2)}-\frac{{\Delta}_L {\Delta}_R}{{\Delta}_S}S_L^z S_R^z\right]S_{n}^z
\end{split}
\end{equation}
Because $[H_{\text{eff}},S^z_n]=0$ the time evolution can be computed separately for each eigenvalue $\pm\frac{1}{2}$ of $S^z_n$, using $H_{\text{eff}}^{\pm}$ that does not depend on the operator $\vec{S}_n$. The different evolution under $H_{\text{eff}}^\pm$ together with the fact that the  new spin starts in a superposition of ${\uparrow}$ and ${\downarrow}$ leads to entanglement between the effective-spin on the strong bond and its two neighboring spins. Full entanglement is generated after a time $t_{\text{ent}} =  2\Omega/(J_L J_R {\Delta}_S)$, set by the difference in the exchange constant in $H_{\text{eff}}^\pm$.
This process will be important later on for computing the evolution of the entanglement entropy.

Apart from generating entanglement, the difference between the evolution given ${\uparrow}_n$ or ${\downarrow}_n$ is not  crucial for the subsequent dynamics in the sense that they both lead to the same recipe for
renormalization of coupling constants. $H_{\text{eff}}^+$ and $H_{\text{eff}}^-$ have the same form as the original hamiltonian and we can directly read off the coupling
generated between $\vec{S}_L$ and $\vec{S}_R$, neighboring the strong bond to the left and right, upon decimation of that bond:
$\tilde{J} ={J_L J_R}/{\Omega}$ and $\tilde{|{\Delta}|} = {|{\Delta}_L| |{\Delta}_R|}/{4}$,
where we neglected the linear ${\Delta}$ correction to $\tilde{J}$. This approximation will be justified a posteriori by the fact that ${\Delta}$ flows to zero. The renormalization of the exchange coupling is then identical to that found in the random Heisenberg chain at $T=0$ and leads to the Random singlet phase\cite{Dasgupta1980,Bhatt1982,Fisher1994}. Note also that we keep only the absolute value of the anisotropy. The sign will randomize in the course of the RG flow because it depends on the state of $S^z_n$. These RG steps are now iterated as we gradually approach lower frequency scales and longer times.

The RG steps are iterated to produce a flow of the probability distributions with decreasing frequency cutoff ${\Omega}$ starting from the microscopic cutoff ${\Omega}_0$. Using the scaling variables
$\zeta = \ln \frac{\Omega}{J}$ and ${\beta} = -\ln |\Delta|$,
and $\Gamma = \ln({\Omega_0}/{\Omega})=\ln({\Omega}_0 t)$ we obtain the following equation for the joint probability distribution $P(\zeta,\beta;{\Gamma})$:
\begin{widetext}
\begin{equation} \label{eq:general-flow}
\begin{split}
\frac{\partial P}{\partial \Gamma} &= \frac{\partial P}{\partial \zeta}
  + \rho(0;{\Gamma}) \int_0^\infty d{\beta}_L  d{\beta}_R d\zeta_L d\zeta_R \delta(\zeta-\zeta_L-\zeta_R)\delta({\beta}-{\beta}_L-{\beta}_R-\ln4)P(\zeta_L, {\beta}_L;{\Gamma})P(\zeta_R, {\beta}_R;{\Gamma}).
\end{split}
\end{equation}
\end{widetext}
where $\rho(\zeta;{\Gamma})=\int d{\beta} P(\zeta, {\beta};{\Gamma})$ is the distribution of $\zeta$.
Note that even if initially the variables $\zeta$ and ${\beta}$ are independent a correlation builds up in the course of renormalization in the same way as it is generated in the ground state \cite{Fisher1994}.

By integrating over ${\beta}$ we obtain an equation for $\rho(\zeta;{\Gamma})$,
\begin{equation}
\frac{\partial \rho}{\partial \Gamma} = \frac{\partial \rho}{\partial \zeta} +\rho(0;{\Gamma}) \int_0^\infty d\zeta_L d\zeta_R \delta(\zeta-\zeta_L-\zeta_R) \rho(\zeta_L) \rho(\zeta_R).
\end{equation}
This equation is identical to the flow leading to the random-singlet ground state and it is solved by the same ansatz\cite{Fisher1994}, $\rho(\zeta;{\Gamma}) = a(\Gamma) e^{-a(\Gamma) \zeta}$ with
\begin{equation} \label{eq:solution}
\begin{split}
a(\Gamma) &= \frac{1}{\Gamma + 1/a_0}.
\end{split}
\end{equation}

Of course the above solution includes only partial information on the fixed point of the dynamics. Important information for calculation of physical quantities is held in the conditional average of the interaction variable ${\beta}$ given a value of $\zeta$ on the same bond, ${\bar{\beta}}(\zeta,\Gamma) \equiv \int_0^\infty d{\beta} {\beta} P (\zeta, \beta;{\Gamma})/\rho(\zeta;{\Gamma})$. Proceeding as in Ref. \cite{Fisher1994}, we derive the equation for this moment by multiplying Eq. \eqref{eq:general-flow} by ${\beta}$ and then integrating over ${\beta}$
\begin{equation}\label{eq:first-moment-flow}
\partial_\Gamma \ln\left({\bar{\beta}}(\zeta)\,\rho \right) =
\partial_\zeta \ln\left({\bar{\beta}}(\zeta)\, \rho\right)
+ \frac{2 a(\Gamma)}{{\bar{\beta}}(\zeta)} \int_0^\zeta d\zeta' {\bar{\beta}}(\zeta')
\end{equation}
Note that we have neglected the $\ln 4$ in \eqref{eq:general-flow}. This is justified near the fixed point since the typical ${\beta}$ flows to $\infty$. After substituting the solution for $\rho(\zeta, \Gamma)$ in Eq. \eqref{eq:first-moment-flow} we find the solution
\begin{equation}\label{solution2}
{\bar{\beta}}(\zeta)= \frac{1}{b_0} (a_0 \Gamma +1)^\phi \left(1+\frac{\zeta \phi}{\Gamma+\frac{1}{a_0}}\right)
\end{equation}
where $\phi=(1+\sqrt{5})/2$ is the golden ratio and $b_0$ is determined by the initial condition.

\begin{figure}[t]
 \centerline{\resizebox{0.9\linewidth}{!}{\includegraphics{clusters.pdf}}}
 \caption{{\em Schematic illustration of remaining spins and clusters of decimated pairs in the renormalized chain at time $t$.} }
 \label{fig:clusters}
\end{figure}

Another important ingredient for calculation of physical properties is the distance between remaining spins (i.e. length of decimated clusters) at time $t$. An illustration of such clusters is shown in Fig. \ref{fig:clusters}.
Since the RG flow is the same as in Ref. [\onlinecite{Fisher1994}] we similarly obtain
$L_\Gamma = (a_0 \Gamma+1)^2 = \left[a_0\ln(\Omega_0 t) + 1 \right]^2$
Which behaves as $\ln^2 ({\Omega}_0 t)$ at long times. From this result we can immediately infer the decay of the staggered moment which is simply the fraction of remaining spins at time $t$: $m_s=1/L(t)=1/\left(a_0\ln(\Omega_0 t) + 1 \right)^2$ . It is interesting to contrast this behavior with the decay of the staggered moment in the analogous quench of a clean $XXZ$ model. In that case Ref. [\onlinecite{Barmettler2010}] found oscillatory decay of the staggered moment (for ${\Delta}<1$) with an envelope that decays exponentially in time.

We note that in the {\em non-interacting} case ${\Delta}_i=0$ the RG flow generalizes in a straight forward way to an arbitrary Ising initial states rather than a Ne\'el state.
If the strongest exchange coupling happens to be between spins with the same orientations, this pair will freeze in their state, while quantum fluctuations lead to an effective coupling between the neighbors that is the same in absolute value as that obtained for anti-aligned spins. Hence the distribution of the absolute values of the exchange couplings is governed by the same RG equations. In the interacting case, such aligned pairs lead to further complications that are left for later work.

\noindent
{\em Results --} We now use the solutions of the flow equations to compute the time evolution of important physical quantities. Specifically to gain information on particle transport and on thermalization of the system we consider the growth of the total particle number fluctuation and of the entanglement entropy in a sub-system corresponding to half of the chain.

To compute the particle number fluctuations we note that the total particle number (or $S^z_{\text{tot}}$) within a decimated pair of sites is a conserved quantity in the RG scheme. Therefore the only contribution to the particle number fluctuation in one half of the system comes from decimated pairs that reside on different sides of the interface. Each oscillating pair that cuts the interface adds $1/8$ to the number fluctuation on time average. Computing the total particle number fluctuation then amounts to counting the number of decimated bonds that cuts the interface. Proceeding exactly as in the random singlet phase\cite{Refael2004} we have
$N_p \approx \int^{\Gamma} d\Gamma' a(\Gamma') = \ln\left(\Gamma+1/a_0\right)$. Hence the particle number fluctuation grows extremely slowly as $\av{{\delta} N^2}= (1/24)\ln(\ln({\Omega}_0 t))$ at long times. Interestingly this result is independent of the interaction strength ${\Delta}$.

We now turn to the growth of the entanglement entropy,between the two halves ($A$ and $B$) of the system, $S\equiv -{\mbox{tr~}} \rho_A\log_2\rho_A$. Consider first the simpler (non-interacting) case
${\Delta}_i=0$, where no entanglement is generated between a decimated pair and the rest of the system. Then, the only source of entanglement between the two halves of the system are decimated pairs that cut the interface, each contributes a time average of $S_p=2-1/\ln 2\approx 0.557$. The growth of the entropy is therefore similar to that of the particle number fluctuation
\begin{equation} \label{eq:S_0-evolution}
S_0(t) \approx S_p\frac{1}{3} \ln\left(\ln\left(\Omega_0 t\right)+1/a_0\right)
\end{equation}
We can generalize this result (for ${\Delta}_i=0$) to a quench from an arbitrary Ising state with a fraction $q$ of anti-aligned neighbors. Because $q$ is an invariant of the RG and aligned pairs do not contribute to the entropy the prefactor in (\ref{eq:S_0-evolution}) changes to $q S_p$.

We turn to our main focus, which is the interacting system with ${\Delta} \neq 0$. In this case a pair decimated at time $t_1$ will eventually get entangled with the neighboring spins according to Eq. \eqref{eq:Heff} after a characteristic time  $t_\text{ent}(t_1)=2{\Omega}_1/(J_1^2 {\Delta}_1)$. In particular from the time of the quench, entanglement will be generated by the interaction only after a delay time $t_{\text{delay}}=2{\Omega}_0/(J_0^2{\Delta}_0)= 2({\Omega}_0/J_0)(1/J^z_0)$, where $J^z_0\equiv J_0{\Delta}_0$ is the typical value of the bare interaction energy.

The interaction-generated entanglement entropy found at time $t$ originates from entanglement of pairs eliminated at an earlier time $t_1=t-t_{\text{ent}}$, which corresponds to the scaling parameter ${\Gamma}_1=\ln {\Omega}_0 t_1$. To estimate this contribution to the entropy we recall that spins on the renormalized chain at time $t_1$ are separated by clusters of length $L({\Gamma}_1)$ of spins decimated at even earlier times and are oscillating at higher frequencies. By the time $t$ that a pair of spins decimated at $t_1$ entangles with their neighbors, the spins inside the decimated clusters must also be entangled with each other. So, it is safe to assume that by the observation time $t$ entanglement propagates to a distance $L({\Gamma}_1)$ giving rise to entanglement entropy $S\approx 0.5 L({\Gamma}_1)\approx 0.5 \,(a_0 {\Gamma}_1+1)^2$. The factor $0.5$ stems from the number of available degrees of freedom: the two states with aligned spins in each decimated pair remain unpopulated and therefore do not contribute to the entropy. To write this as a function of the time $t$ we use the relation between $t$ and $t_1$,
\begin{equation}
t = t_1 + t_{\text{ent}}  =  t_1\left(1+ \frac{2\Omega_1^2}{J_L  J_R {\Delta}_1}\right)
\approx t_1 \frac{2\Omega_1^2}{J_L J_R{\Delta}_1}.
\end{equation}
We now take the logarithm of both sides and replace the scaling variables by their appropriate average values $\zeta\to 1/a({\Gamma}_1) $ and ${\beta}_1\to {\bar{\beta}}(\zeta=0;{\Gamma}_1)$. Here the correlations between the random variables came in to play. We needed the average of ${\beta}$ on the bonds with strongest $J$ ($\zeta=0$), which is different than the global average of ${\beta}$.

Using the solutions (\ref{eq:solution}) and \eqref{solution2} for the typical values we find
$
{\Gamma}=3 {\Gamma}_1 +\frac{1}{b_0} (a_0 {\Gamma}_1 +1)^\phi + 2/a_0 + \ln2,
$
This equation should be inverted to express ${\Gamma}_1$ as a function of ${\Gamma}$ and used to obtain  $S({\Gamma})=0.5 L({\Gamma}_1({\Gamma}))$.
In general, the inversion cannot be done analytically, but we can easily find the limiting regimes.  At sufficiently long times the term ${\Gamma}_1^\phi$ dominates the right hand side and then we have $a_0 {\Gamma}_1= [b_0 ({\Gamma}-2/a_0-\ln2)]^{1/\phi} -1$. On the other hand at shorter times, when the linear term dominates,  we get ${\Gamma}_1 = {1\over 3}({\Gamma} - {2\over a_0} - {1\over b_0} - \ln2)$.

The crossover time $t^*$ separating the two regimes depends on the initial conditions through the coefficients of the terms ${\Gamma}_1$ and ${\Gamma}_1^\phi$.
If $b_0\gg a_0$, that is for stronger disorder in hopping than in the interactions, we have  $t^* =  t_{\text{delay}} \exp \left(6(3 b_0/a_0)^\phi /a_0\right)$. In the opposite regime $b_0\ll a_0$ the term ${\Gamma}_1^\phi$  dominates from the outset and $t^* = t_{\text{delay}}$. We can now write an expression for the
 growth of the entanglement entropy valid in the limiting regimes
\begin{equation}
\begin{split}
S(t)&\approx {1\over 2} \left(\frac{\ln\left(t/t_{\text{delay}} \right)}{\ln \left({\Omega}_0/J_0\right)}+1\right)^2{\theta}(t-t_{\text{delay}}){\theta}(t^*-t) \\
&\quad + {1\over 2} \left(\frac{\ln\left(t/t_{\text{delay}} \right)}{\ln \left(1/{\Delta}_0\right)}+1\right)^{2/\phi}{\theta}(t-t^*)-{1\over 2}.
\end{split}
\label{eq:S}
\end{equation}
Interestingly, Eq. (\ref{eq:S}) gives the unbounded logarithmic growth of the entanglement entropy seen in the numerical simulations and even the delay of this interaction induced growth by a time that scales as the inverse interaction strength [\onlinecite{Bardarson2012}]. It is important to note however that the numerically simulated model differs from ours by having disordered Zeeman coupling, which may ultimately drive it to a different fixed point \cite{Ronen-future}. Nevertheless we can attempt a comparison even of the more subtle form of the logarithmic growth by crudely accounting for this difference. Through second order perturbation theory the Zeeman strong disorder generates predominantly strong randomness in the hopping, but not in the interactions. Hence the natural regime to compare the numerics to our model is $a_0\ll b_0$ where the first line of (\ref{eq:S}) holds at any reasonable time-scales (i.e. below the exponentially long time $t^*$). Even within this regime Eq. (\ref{eq:S}) predicts a crossover between growth of the entanglement entropy as $\ln t$ at times $t<({\Omega}_0/J_0)^2 t_{\text{delay}}$ to growth as $\ln^2 t$ at longer times. The slope of the logarithmic growth $1/\ln({\Omega}_0/J_0)$ is completely independent of the interaction strength ${\Delta}$, consistent with the universality
identified in Ref. [\onlinecite{Bardarson2012}].

To complete the comparison, we note that the growth of particle number fluctuations which was computed above is much slower  ($\sim \ln\ln t$) than the growth of the entanglement entropy. Again this is consistent with the numerical results, which implies that particle transport is essentially blocked. Indeed the particle number fluctuations are in general only a lower bound of the entanglement entropy\cite{Klich2006}.

Having found that the entanglement entropy increases without bound it is natural to ask if this leads to thermalization. To address this issue let us consider the saturation of the entanglement entropy in a finite system, or in a finite sub-system of length $L_s$.  Eq. (\ref{eq:S}) implies that the entropy will approach its maximal value $S_\infty$ after a time $t_{\text{sat}}\approx t_{delay}\exp\left[-\ln\left({\Delta}_0\right)L_s^{\phi/2}\right]$.
Does the saturation value $S_\infty$ correspond to a state in thermal equilibrium?

Provided we start from a symmetric distribution of ${\Delta}_i$ such that $\av{{\Delta}_i}=0$, then the initial Ne\'el state has zero mean energy, exactly in the middle of the many-body energy spectrum. If this state thermalized following the quench, the entanglement entropy would have to saturate to its infinite temperature value of $L$. But as we have pointed out above, the RG flow implies a saturation entropy that is at most half of the infinite temperature value because half of the degrees of freedom remain frozen in the dynamics. This fact is embodied in the infinite set of emergent  integrals of motion $I_p=(S^z_1 S^z_2)_p$, which account for the fact that a pair of decimated spins, never flip their relative orientation within the perturbative RG scheme. Note that this remains true even for generalized initial states allowing for aligned neighboring spins. In the case of an initial Ne\'el state we also have the particle number on oscillating pairs (or $(S^z_1+S^z_2)_p$) as additional integrals of motion. These emergent conservation laws become asymptotically exact for well separated pairs of spins decimated at long times as the perturbative RG scheme becomes asymptotically exact near the infinite randomness fixed point.
We conclude that the long time steady state of the chain with non vanishing interaction is characterized by the generalized Gibbs ensemble (GGE)\cite{Rigol2008}, which describes thermalization within a subspace constrained by the values of the emergent integrals of motion $I_p$.

It is interesting to note that the long time steady state attained by the non interacting state ${\Delta}_i=0$ is markedly different. The extremely slow increase of the entanglement entropy as $\ln\ln t$ given by Eq. (\ref{eq:S_0-evolution}) together with the relation between length and time scales $\ln {\Omega}_0 t={\Gamma}\sim \sqrt{L}$ imply saturation of the entanglement entropy to $S_\infty\approx {S_p\over 6}\ln L$. This result, as well as the $\ln\ln t$ growth of the entropy matches with numerical results obtained for the random transverse field Ising chain\cite{Igloi2012} that can be similarly described by a model of noninteracting fermions.

So far we have used the RG approach to establish and characterize a many-body localized state. It is interesting to examine the criterion for validity of the RG scheme, which may indicate a transition to a different, possibly thermalizing and delocalized, state. Such a criterion can be obtained from the first term in Eq. (\ref{eq:Heff}). The perturbation theory at the base of the renormalization step is valid while $(J_L J_R/{\Omega})\ll \av{J} (1-{\Delta}_S^2)$. This can be expressed in terms of the average values of parameters at the beginning of the flow. Using $\av{J_0/{\Omega}_0}=a_0/(a_0+1)$, we obtain the criterion
$
a_0< {\Delta}_0^{-2}-1
$.
Recall that increasing $a_0$ corresponds to decreasing disorder. It is tempting to speculate that for weaker disorder $a_0>{\Delta}^{-2}-1$ the dynamics will give rise to a normal thermalizing state. However the above requirement may be too strict. Even if the criterion $a_0<{\Delta}_0^{-2}-1$ is not satisfied initially, this may be corrected in later stages of the flow as ${\Delta}$ independently flows to smaller values. It is therefore also possible that the transition to a different state occurs only for $\av{{\Delta}^2}\approx 1$ independent of the disorder strength.

{\em Conclusion --} Using a real space RG scheme formulated in real time, we gave a dynamical description of a many-body localized state in a random spin chain, equivalent to interacting fermions with random hopping. Within this approach the localized state is characterized by a flow to an infinite randomness fixed point. Solution of the flow equations allows us to characterize this state in a rather detailed way. The results are found to be in excellent agreement with recent numerical simulations done on a similar, albeit not identical, model\cite{Bardarson2012}.

Particle localization is manifest in the extremely slow growth $\sim \ln\ln t$ of the particle number fluctuations in half the system that is seen both in the interacting and non-interacting systems. The entanglement entropy $S$ reveals a dramatic difference between the Anderson localized state of noninteracting fermions and the many-body localized state established when interactions are present. In the non interacting system $S$ grows together with the particle number fluctuation as $S(t)\sim \log\log t$ and saturates to a non-extensive value $\sim \ln L$ in a finite system. Interactions lead to much faster growth of $S(t)$ as $\log^{2/\phi} t$ at long times, but they take effect only after a delay time that scales as the inverse of the interaction strength $t_{\text{delay}}\sim 1/J^z$. Furthermore, the $\log^{2/\phi} t$ behavior seen in the long time limit is preceded by $\log t$ growth up to an intermediate time scale $t_{\text{lin}}\sim t_{\text{delay}} ({\Omega}_0/J_0)^2\gg t_{\text{delay}}$.
It is interesting to note that the growth of entanglement as $\ln^{2/\phi} t$ exceeds the upper bound $\sim \ln t$ proved for non-interacting Anderson localized chains\cite{Burrell2007}.

The RG flow toward the infinite randomness fixed point has direct consequences on the equilibration in this system. In a sub-system of length $L$ the entanglement entropy saturates to an extensive value $S_\infty \sim L$, which is however smaller than it would reach had the system attained true thermal equilibrium.
We attribute the lack of thermalization to an infinite set of emergent integrals of motion, which become asymptotically exact conservation laws near the infinite randomness dynamical fixed point. The dynamics of the system can therefore be viewed as
thermalization within a GGE characterized by the emergent set of conserved quantities, a possibility suggested in Ref. [\onlinecite{Gogolin2011},\onlinecite{{Khatami2012}}] . Here we demonstrated that such a GGE emerges in a non integrable random system as a dynamical fixed point of the renormalization group and captures the essence of a many-body localized state.
The nature of the critical point marking the transition to the normal thermalizing state remains an interesting question for future study as are generalizations of our scheme to more generic disorder models and initial states.

{Acknowledgements --} We thank J. E. Moore, F. Pollmann, D. Huse, V. Oganesyan, G. Refael, and A. Polkovnikov for useful discussions. This work was supported by the ISF and the Minerva foundation.

\bibliographystyle{phd-url-notitle}

redpajama_set_name: RedPajamaArXiv


Truck break failure leaves 13 dead, 30 injured in Sierra Leone.
Thirteen people were killed and at least 30 more injured on Monday when a military transport truck flipped over on a major road in the Sierra Leone capital, a military spokesman said.
The open-air truck was carrying more than 40 soldiers from their barracks to a funeral in Freetown when its brakes failed as it descended a steep hill.
It toppled over and slid for more than 30 metres, Captain Yaya Brima said. Eight soldiers were among the dead.
Nigeria: Activist Obi Ezekwesili to contest for presidency in 2019.
Kenya wildlife officials rescue Taiwan tourists by killing hippo.
Ethiopia to begin issuing online visas to tourists on June 1.


I have always loved anything key lime. Key lime pie was one of my favorite desserts growing up, because I loved the balance of tart and sweet in the creamy filling, and just the heavenly aroma of the limes. I still feel the same way, and the scent of lime reminds me of summer and warm weather. Although it isn't Summer, we have just barely gotten into Spring, I decided to make some key lime sugar cookies last weekend. I am so ready for warm weather and it was making me a little sad that we were supposed to get snow later in the week, so I figured I would enjoy Summer in the form of cookies.
I used my classic sugar cookie base, one that turns out tender, buttery and melt in your mouth delicious. It is based off of my Grandma's sugar cookie recipe actually, the one I used to make before I went vegan that always impressed everyone and they were going back for seconds. Some sugar cookies are just like "meh this is ok but nothing special" but these are crave worthy. I actually made this batch gluten free, because I had some Bob's Red Mill all purpose gluten free baking flour on hand.
I wanted them to have plenty of lime flavor so I added it in both zest and juice form. I sweetened these with xylitol because I don't buy refined white sugar and it is what I use when I don't want my baked goods to turn brown or have a flavor like when I use coconut sugar. The dough smelled amazing thanks to the fresh limes, and it tasted even better.


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text:
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text:
Home > Catholic Encyclopedia > H > Ancient See of Hamar
Ancient See of Hamar
(HAMARCOPIA; HAMARENSIS).
Hamar in Norway, embraced Hedemarken and Christians Amt, and was formed in 1152 out of that of Oslo, when Arnold, Bishop of Gardar, Greenland (1124-52), was appointed first Bishop of Hamar. He began to build the now ruined cathedral of Christ Church, which was completed about the time of Bishop Paul (1232-52). Bishop Thorfinn (1278-82) was exiled and died at Ter Doest in Flanders. Bishop Jörund (1285-86) was transferred to Trondhjem. A provincial council was held in 1380. The last Catholic bishop, Mogens (1513-37), was taken prisoner in his castle at Hamar by Truid Ulfstand, a Danish noble, and sent to Antvorskov in Denmark, where he was mildly treated until his death in 1542. There were at Hamar a cathedral chapter with ten canons, a school, a Dominican Priory of St. Olaf, and a monastery of the Canons Regular of St. Anthony of Vienne.
HANSEN, Hamar og dets Biskopper (Hamar, 1866); RAMSETH, Hamars Bys Historie (ibid., 1899); LANGE, De norske Klostres Historie (Christiania, 1856), 374-77, 389-91; Historisk Tidsskrift, 3rd series, I (Christiania, 1890), 113-40, 244-69, 277-334; III (Christiania, 1895), 379-411.
APA citation. Taylor, A. (1914). Ancient See of Hamar. In The Catholic Encyclopedia. New York: The Encyclopedia Press. http://www.newadvent.org/cathen/16043c.htm
MLA citation. Taylor, Arthur. "Ancient See of Hamar." The Catholic Encyclopedia. Vol. 16 (Index). New York: The Encyclopedia Press, 1914. <http://www.newadvent.org/cathen/16043c.htm>.
Transcription. This article was transcribed for New Advent by Douglas J. Potter. Dedicated to the Immaculate Heart of the Blessed Virgin Mary.
Ecclesiastical approbation. Nihil Obstat. March 1, 1914. Remy Lafort, S.T.D., Censor. Imprimatur. +John Cardinal Farley, Archbishop of New York.


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text:
package nl.uu.trafficmas.norm;

import java.util.ArrayList;
import java.util.List;

import nl.uu.trafficmas.simulationmodel.AgentData;

public class StayInLaneNormInstantiation extends NormInstantiation {

	private List<AgentData> goals;

	public StayInLaneNormInstantiation(NormScheme ns, String agentID) {
		super(ns, agentID);
		goals = new ArrayList<AgentData>();
	}

	public void addGoal(AgentData agentData){
		goals.add(agentData);
	}

	@Override
	public List<AgentData> getGoals() {
		return goals;
	}

}

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I'm not anywhere near to being vegetarian or vegan so I have to admit that I was wondering if I would really get anything out of Things I Know About Cooking and Not Eating Animals. As it turns out, I did.
I love that S&S starts off with a funny, 'keepin' it real' confession about her beginnings in becoming a vegetarian. I'm not here to judge anyone's reasons behind their life choices, but admitting that it came from something silly makes the zine more relate-able. When you're talking about potentially sensitive subjects, a bit of humour can definitely help.
There's a bit of most things I think you'd expect to see in this zine. There are things she wishes she'd cooked with sooner, recipes, how to re-hydrate dried beans, and more. It certainly introduced me to some things that I'd never even heard of before (textured vegetable protein, anyone?). Plus, just because I'm not a vegetarian, it doesn't mean I don't love my beans and own a dehydrator.
There's a blank page in the back for 'notes and stuff' that I think is cool. I've never seen a notes page in a zine before. That may be for obvious reasons, but I like seeing new and different things in zines.
All up, it might not be quite my thing, but it was a good zine in the subject that taught me things without preaching to me.
Thank you for saying I'm open-minded. I think it helps that I make my own zines. I think about the time and the effort I put into them, and I wouldn't want anyone to dismiss them out of hand. So I don't want to do that to anyone else's zines. I give everything a go, and, most of the time, I'm pleasantly surprise.
Plus, my love of cooking and baking transcends the distinctions of what people decide to put/not put into their bodies.


text:
{ "1523104": { "url": "/art/kaiju", "shareUrl": "https://www.britannica.com/art/kaiju", "title": "Kaiju" ,"gaExtraDimensions": {"3":"false"} } }
Japanese film genre
Tōhō Motion Picture Company
In Tōhō Motion Picture Company
…fiction offerings, particularly in the kaiju (monster) genre. Most notable was Gojira (Godzilla), a colossal, irradiated, dinosaur-like beast that made its film debut in 1954. During the virtual collapse of the Japanese film industry in the 1970s, the company restructured its operations to reduce costs. The growth of the home…