TUSCON, Ariz. – Kaylie Lowery singled in the game-winning run in game one and Madelyn Carlson tossed seven shutout innings in game two to give the Whitworth Pirates a Saturday morning sweep of Birmingham Southern and Wittenberg.
The sweep bumped the Bucs record up to 6-6 overall while Wittenberg dropped to 1-2 and Birmingham Southern fell to 8-6.
The Pirates used a six-run fourth inning and Lowery's walk-off single to defeat Birmingham Southern.
The Panthers took the game's first lead on a fourth-inning single from Abby Spencer, setting the Bucs in a 1-0 deficit heading into the bottom of the fourth.
Whitworth responded with six runs of their own, taking a commanding lead. Sara Gayer started the rally with a walk before back-to-back singles from Kelsey Downey and Michelle Silva loaded the bases for Logan Miller. The sophomore drove in a pair of runs with a double to left field, giving Whitworth the lead.
The Pirates piled on four more runs on RBIs from Allie Rude, Desi Graham, Lowery, and Chelsey Hayes to earn a 6-1 advantage at the end of the inning.
Birmingham Southern refused to go away, however, chipping away at their deficit with four runs in the top of the sixth inning and another in the top of the seventh to tie the game.
The two teams went to an international tiebreaker in the eighth inning, placing a runner on second to begin each frame. Carlson held the Panthers scoreless in the top of the inning, which gave Lowery a chance to win the game in the bottom of the eighth.
As the last out of the seventh inning, Rheanne Lewis started the eighth on second. Lewis stole third base and scored when Lowery singled to left-center field to win the game.
The Pirates won their third-straight one-run game against Wittenberg, defeating the Tigers behind a shutout from Carlson.
The freshman pitcher tossed seven shutout innings, allowing five hits and striking out four Wittenberg batters. Carlson walked just two batters and earned her sixth win of the year.
Whitworth's offense ensured Carlson had just enough offense to get the win. The Bucs scored their lone run in the fourth inning when Miller's sacrifice fly drove in Gayer, who had reached on an error earlier in the inning.
Wittenberg managed to get runners on the base paths just twice after Miller's RBI, but their only chance to tie the game was cut down at the plate by Kinsey McNaught in the sixth inning.
Up Next: The Pirates close out their time in Arizona with another doubleheader tomorrow afternoon. Whitworth takes on Coe at 2:00 p.m. and Central (IA) at 3:30 p.m.


text:
Man-made structures and Apex Predators: Spatial interactions and overlap (MAPS)
The effect of man-man structures on the marine ecosystem is likely to depend on the type and status of the structure. Commissioning and decommissioning of structures can cause disturbance and displacement of marine mammals. Established structures may also result in displacement due to operational noise, presence of maintenance vessels or habitat destruction. However, such structures may provide refuge for predators or their prey due to access and fishing restrictions within their vicinity. Furthermore, such structures can host artificial reefs and may present foraging opportunities for some predators, for example in a recent paper (Russell et al., 2014) the applicants demonstrated that some seals use such structures for foraging. How either deterrence or attraction to these structures may affect the marine environment is still poorly understood.
We will map the distributions of top predators in the North Sea, including seabirds, seals and cetaceans, and quantify overlap with man-made structures. We will examine how the distributions of apex predators are influenced by proximity to man-made structures, while considering other temporal and spatial variation in their environment (e.g. habitat, depth, temperature). This will provide information on the current effect of man-made structures on the distribution of key apex predators and also on the proportion of the population of each species which could be potentially impacted by disturbance resulting from commissioning and decommissioning.
For finer spatial scale analyses, we will use data from animal-borne devices which record and transmit locational and in some cases behavioural data on harbour and grey seals (minimum sample size of 282) and five species of seabird (n=700). These data will allow us to quantify the encounter rate with man-made structures and also the proportion of encounters that result in the use of structures for foraging. We will investigate how the results vary among individuals, species, structure type and age. Along with the overlap between species and man-made structures, this will allow us to report on the extent to which manmade structures may influence foraging behaviour at a population level. Our results will inform the review of OSPAR Decision 98/3 and any commissioning and decommissioning processes to reduce any negative impact on the ecosystem.
Dr Deborah Russell
Sea Mammal Research Unit (SMRU), Scottish Oceans Institute, University of St Andrews, UK
Presenter: Dr Debbie Russell
Title: University of St Andrews MAPS project
MAPS Summary Report
MAPS Science Day Presentation
The latest news and updates from INSITE.
Structures in the Marine Environment - How do we plan for the future?
SIME 2021 is already nearly six month behind us. The event was a resounding success with an extensive programme of discussion and debate.
Structures in the Marine Environment 2021 - Registration is OPEN
We are delighted to confirm dates for the third Structures in the Marine Environment Conference (SIME2021).
National Decommissioning Centre offers further funding to support the INSITE PhD Scholarship Programme 2021
The National Decommissioning Centre (NDC) is offering additional funding in support of the INSITE PhD Scholarship Programme.
INSITE Interactive - Launched in support of NERC funded projects
Initially available in early 2020 in parallel with the NERC Announcement of Opportunity, INSITE Interactive is now being used by researchers.
Follow INSITE North Sea on all our social channels, to stay up to date with all our latest news and opportunities

redpajama_set_name: RedPajamaCommonCrawl


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Callum Davies says he is delighted to be back in the Gills first team and is eager to keep playing regular Football.
The young centre-back put in some fantastic challenges to ensure all three points were preserved against MK Dons in a 3-2 win on Saturday, and he is now hoping the club can build on their recent form.
A brace each from Danny Kedwell and Patrick Bamford, after Tom Flanagan had been sent off on 12 minutes for conceding the second penalty of the day, kept the scores level at the break, but Danny Hollands headed home just shy of the hour mark to grab the winner.
After the game Davies said: "It's nice to be back in a winning mentality – it was a bit odd with them going down to 10 men but it probably didn't affect the way they play because all they want to do is pass it.
"When they come back to 2-2 you are thinking the worst so it shows the character we have in the team to go on and win it.
"We are getting back up the league now; we didn't have the best of starts so fair play to the squad and all the management.
"Football is all about confidence and momentum really, you have to keep rolling.
"When you are winning everyone is happy and you get that bit of luck when earlier in the year it wasn't going for you.
"Football is a weird sport, like a rollercoaster. We need to keep going up now and see where the squad can go.
"Everyone will say they 10 men but you have to beat what is put in front of you. Anyone can beat anyone.
Davies says he is learning a lot from playing with Adam Barrett at the back, and revealed he is a player he looks up to for advice and support.
He added: "Adam's the nicest bloke you will ever meet and he's a top professional and I couldn't wish to play with anyone better. Leggy is a top bloke too and he helps you.
"They will pick you up when you need it, there is a mutual respect and I look up to Adam.
"I just want to play at the end of the day. I have played a couple of reserve games but first team football is so different so I was a bit exhausted.


text:
New Message for Students
Promotion & Tenure Procedures
Faculty Reporting
UH General Admissions
Art Admissions
Music Auditions
Theatre Auditions
Art Programs (Undergraduate)
Art Programs (Graduate)
Theatre Programs
M.A. in Arts Leadership Program
Master's Theses, and Doctoral Documents and Essays
Arts & Technology Center
Celebration Gala
Moores School of Music Society Fall Luncheon
Beethoven 250 Houston 2020
STEM on Stage: UH Theatre Students Help Kids Create Original Plays
Students intern, teach at Alley Theatre Play Makers camp.
By Natalie Thayer
Play Making campers warming up.
A camper working on arts and crafts. Photos by Christopher Diaz.
UH School of Theatre & Dance
Alley Theatre
Undergraduates in the UH theatre education program aren't afraid stand in the spotlight before a classroom of students. In fact, it's where they shine.
As early as their first year in the program, theatre education majors get hands-on experience through a partnership with Lantrip Elementary School. Once a week during the academic year, UH students head to the nearby elementary school to lead lessons and workshops during an afterschool theatre club.
"The theatre club is foundational to our theatre educators," say Jackie deMontmollin, associate director of theatre education at UH. "It gives them a chance to work directly with kids in a real world setting from the moment they enter our program."
"It's pretty amazing," adds Ryan Simpson (BFA '20), who just completed his freshman year. "We work with kids from first through fifth grade, so we try to tailor the same lesson for each age group. It's a fantastic opportunity to learn what works for different students."
The club also sets the stage for UH students to connect with the local community through other avenues. Just this summer, Simpson and three fellow theatre education majors – Lindsey Pritchett (BFA '20), McCoy Rasco (BFA '19) and Jason Quach (BFA '18) – are working with the Alley Theatre's Play Makers program, a series of two-week summer camps designed to introduce campers to STEM (science, technology, engineering and math) concepts through theatre. The camp includes movement, acting and "play making" – or narrative storytelling – classes, as well as arts and crafts classes to teach campers about technical theatre.
Simpson and Pritchett, both first year interns, lead the campers through daily warm up exercises and support the Teaching Artists with classroom management. "It's a good chance for us to observe how instructors lead classes and use lesson plans," says Simpson, who works with fourth and fifth graders.
Pritchett agrees. "We can see in real time what strategies and techniques keep the kids engaged and what things don't," she adds. Though she works with the youngest campers, Kindergarteners and first graders, she finds that the most successful strategies are transferrable. "We set clear expectations up front and then bring a lot of positive energy to the class so they see us as someone they want to learn from."
Rasco and Quach, both of whom interned with the Alley last summer, returned this year as Teaching Artists. In the new role, they are each responsible for developing play making lesson plans and helping their campers create an original play.
"Camp is supposed to be fun, so we have to strike a balance that is engaging, playful and still challenging," Rasco says. It takes a lot of planning, he admits, but says he's grateful for the experience at Lantrip. "I can connect the material in my play making classes with what I created during the school year and build on those lesson plans."
Rasco and Quach also lead the afternoon arts and craft classes where students build props and sets for their plays. These classes provide Quach, who has a background in scenic painting, an ideal opportunity to bring together his passions for teaching and technical theatre. "The practical applications of [technical] theatre are so amazing," he says, recalling how he built sets and ran lighting for plays during high school. "I had never created anything like that before, and I fell in love." He hopes to inspire campers to connect with theatre in a similar way. "Using theatre to teach other concepts is so important. It was life changing for me, and I want to be able to help other kids make those connections."


As you know, I have been writing this book on leadership in times of change for little over a year now. Yesterday I completed the final section of the final chapter of inner leadership, and thought I would share it with you.
The first six chapters of inner leadership take us from making sense of the situation we find ourselves in to creating an inspiring vision of whatever we want to create instead.
The seventh chapter prepares us for the implementation of that vision and the inner emotional transitions that inevitably come alongside any outer change. In brief, it describes how to manage those transitions, how understanding them can help us to engage people more fully to follow our vision, and how ultimately to create 'antifragile' leaders and organisations: people and organisations that actually become stronger because of change rather than being damaged by it.
This penultimate section of that chapter, the last one to be completed, looks again at the whole time of churning we are living through and describes/explains how, with the insights of inner leadership, it is actually an opportunity to create whatever we most want.
I realise this section is out of context, but I hope you find it useful and interesting, and would be interested in your comments.
I am now switching my focus to a few 'housekeeping' activities, and then to publication!
So far in this chapter we have seen how understanding our personal transitions brings the opportunity to choose our attitude in any given set of circumstances, and to engage people more fully to support our vision. We have seen how understanding the way change happens in an organisation brings the opportunity to create antifragile businesses and leaders.
Let's step back one more time to consider what it means when almost all organisations are changing at once. Let's use what we have learned from inner leadership to reinterpret what this time of churning means for us.
We might find ourselves knocked off balance or disturbed by this time of churning but it is really nothing new. Change has always been with us. The only difference now is the scale of changes that we face.
"The meaning of the fact… that everything is dissolving constantly – that we're all falling apart, we're all in the process of constant death… [that it's] all falling apart, everything is – that's the great assistance to you. The fact that everything is in decay is your help. That is allowing you that you don't have to let go, because there is nothing to hold on to.
What Alan Watts is telling us is that although we might feel there is nothing to hold on to in this time of churning, there never was and never will be. And once we see that we "just don't have a prayer" and "really get with that" then we receive an "enormous access of energy".
Seen from this viewpoint, this time of churning becomes our greatest ally and opportunity. And inner leadership has already taught us how to do what he is suggesting.
If there is nothing external to hold on to then the stability we seek must come from inside ourselves. The tools of Chapters 1, 2, 4 and 5 have shown us how to achieve this: to centre, ground, make sense of the situation, identify what it will take for us to live a worthwhile life (leaving "not a rack behind"), and crystallise all that into our purpose and values.
Once we do this then we free ourselves to look beyond the challenges we face and see the opportunities, to choose the one that suits us best, and articulate it as a vision that brings energy to ourselves and others. The tools of Chapters 2, 3, 4, and 6 have enabled us to do this as well.
In this time of global churning, with so many interconnected changes happening at once, we cannot hope to escape or ignore change. In the language of Chapter 3 that leaves us with three alternatives: to fix, improve, or transform either the situation and/or our own leadership. The two volumes of this book provide a structured methodology for achieving whichever option you choose.
Which you choose is up to you. It doesn't matter, so long as you actively choose the one that is best for you now. Because if you don't, then as Seth Godin says, you have effectively chosen anyway. And if you do then you are starting to live a meaningful life, which is the only worthy goal.
Remember that the future belongs to organisations and leaders which are antifragile: groups of people who are able to work together on projects of shared meaning, in ways that use every so-called 'challenge' to clarify and develop both their purpose/values and their ability to achieve those things.
So make your choice, define a vision that inspires you now, and either form an organisation to achieve it, join one that already exists, or transform the one you are in already. There are billions of people experiencing the churning, seeking the solutions you can bring. The challenge is the opportunity.
Now that you have completed inner leadership you are ready to move to outer leadership. Before we do that, the final section of this chapter revisits some of the major landmarks of inner leadership and pulls them together into a sketch map to take with you on the journey to your vision.
This entry was posted in About/Introduction, Antifragile by The Churning. Bookmark the permalink.


text:
Court decides Benyamin Rasouli will not be executed. Here is a one on one interview with him
An interview with Benyamin Rasouli, a young man rescued from execution: [On the night of Behnoud's execution] He was not crying, he was really quiet"
Source: http://schrr.net/spip.php?article7722
An interview with Benyamin Rasouli, a young man rescued from execution
In the Islamic Shaira Law practiced and imposed in Iran, in the case of murder (first or second degree, and even at times manslaughter), the family of the victim has the final say. They can either opt for Qesas, an eye for an eye punishment which would be execution in case of homicide, or forgive the defendant in return for Diah, or "blood money."
Article 37 of the UN Convention on the Rights of the Child states that "…capital punishment nor life imprisonment without possibility of release shall be imposed for offences committed by persons below eighteen years of age." Iran is a signatory to this convention [and has accepted this section without any condition]. Nevertheless, several young offenders in Iran are hanged each year.
The punishment for youth who commit murder, drug smuggling, and engagement in sexual relationships is punishable by death- this has been one of the most important human rights challenges in Iran.
Adolescents accused of murder committed the crime at a young age on another person their age as a result of immature conflicts. These youth are sentenced to death for manslaughter (homicide without premeditation and often accidental). Benyamin Rasouli is one of the youth who was released after the family of the victim forgave him. What follows is an interview conducted with Benyamin by Saba Vasefi.
Q: How was Hossein [the victim] killed?
A: They had beaten up my friend Shahram. I went to make peace between them, but the tension grew. When they were in our neighbourhood, they got beaten up. Then, they said, if you're a man, come to the park. I went there, there were 12 of them, and there was nobody from our neighbourhood. I escaped from them, returned home, grabbed my knife, and returned to the park. I really did not realize how and when he was stabbed. But I found out later that the knife had cut through his ribs and he had died in the hospital.
Q: Who had given you the knife?
A: It was wooden handle knife given to me by a friend as a souvenir from northern Iran.
Q: How old were you at the time of the incident?
A: I was 15. I was so small that when the police officer saw me, he was very surprised and said, "Are you Benyamin? You're so tiny!"
Q: Where were you arrested?
A: A few police officers came to our house 20 minutes after the incident. One of them was Safar Ali Nasiri who was later executed in Rajayi Shahr Prison [A notorious prison in Karaj, known for holding dangerous criminals].
Q: You went to the police station alone?
A: Yes, they gave the address to my parents and told them to follow us. They handcuffed me from behind and threw me into the trunk of the car.
Q: Did you confess to the murder when you got to the police station?
A: I could not believe the knife had hit him [Hossein]. In the station, they beat me up with a hose filled with pellets so I would confess where I had put the knife. I was subject to "chicken torture" three times, and they hung me [by my hand] once. After I told them about the whereabouts of the knife, they showed me the pictures of three bodies which were found near the railroad in Mehrshahr. They wanted me to confess to those murders too.
Q: Can you describe "chicken torture"?
A: They handcuff the person, pass the knee from the space between the arms, and pass a metal bar between the legs and put each end of the bar on a chair. Then they beat you while you swing from one side to the other. In that situation, the only thing you can do is scream.
Q: How long were you in the police station?
A: One month and 28 days. I was in the room for two weeks. During all this time, I was handcuffed. They cuffed my ankles so tight that I lost all the hair on my legs.
Q: How long were you subject to corporal punishment?
A: Starting from 20 days before the court date, they stopped beating me so the bruises would disappear.
Q: On the day of the court, there was no bruises or wounds on your body?
A: No, all that was left was a big yellow spot.
Q: Did you witness other people being subject to corporal punishment?
A: There were two people who were arrested for drug dealing. When they were taking them for beatings, they would dislocate their shoulders and would fix it after they got beaten. Hesarak police station is like hell. If they cannot force a confession in Shahpour station, which has a notorious reputation, they bring the accused to Hesarak.
Q: When you were transferred to prison, were you beaten again?
A: When I was transferred to the prison, the head of the prison took me for a tour to show me around. He said, "Walk on the ceramic hallway and think that on one side there is a valley, and on the other, people. If someone pushes you, which side will you jump to?" I replied "Well, since there is the question of my life, it is allowed to jump on people." I was seriously thinking that way, but I was beaten badly for those words.
Q: How were you spending your days in prison?
A: In Prison Council I was working with Ali Mahintorabi. We were publishing a 30 page journal with the help of the women's ward.
Q: What were you feeling when they handed down the death sentence?
A: I was constantly having a nightmare.
Q: What nightmare?
A: I dreamed I was in a courtyard surrounded by trees. Behind the trees was a wall, and in the middle was the gallows. When I was walking toward the trees, they wanted to execute me. When I was walking toward the wall, a ghost would come out and push me to the gallows.
Q: Were any of your cellmates executed?
A: Yes, Behnoud Shojaee and Sattar Shiri.
Q: What did you feel after their deaths?
A: I was not able to sleep for two months, I was constantly talking to myself, and I developed nervous ticks.
Q: Do you remember Sattar's last night?
A: He was crying a lot. He was saying, "I know that this time they will hang me. I feel sorry for my family."
Q: What about Behnoud?
A: Behnoud was not crying, he was really quiet. Not a night went by without his nightly prayers. There, many of the kids get addicted. They learn many news criminal skills, but Behnoud had given everything up. He was only calling on God. His book of prayer had turned yellow. The night before his execution everyone was crying for him. He was so quiet and innocent that everyone had fallen in love with him.
Q: After Behnoud didn't return to the cell, what did the guys do?
A: We held a memorial for him. We all wore black until the 40th day following his death. The night before his execution he was saying that there was a 99% chance he would be executed, unless a miracle happened and God beamed a light into the hearts of the victim's family.
Q: When the family of Hossein forgave you, what feeling did you have?
A: When they forgave me, I thought it was a lie, because many of the families would bluff like that. The family of the victim in the case of Behnoud had said that she would forgive once they put the noose around Behnoud's neck, but she was the one who kicked the stool from below Behnoud's feet. I told myself, they are lying in my case as well.
Q: How many siblings do you have?
A: We are six and I have a half sister.
Q: Who was able to obtain the forgiveness of the victim's family?
A: I owe it to my lawyer Ms. Tahmasbi and my sister. When I was released, I wanted to kiss their feet. They worked really hard. My lawyer without any expectation was able to reduce the blood money from $250,000 to $50,000.
Q: Now how do you find life outside prison?
A: Everything seems so strange and foreign. I feel my dad's absence. I cannot believe he is dead. When I was in prison, he suffered from a concussion as a result of a car accident and died. Since I did not see him, I was not able to believe his death.
Q: How do you want to live from now on?
A: I want to enjoy everything to the fullest. I wake up in the middle of the night and I open my eyes. I am really tired, but I don't want to close my eyes. I get up and kiss my mom. I want to compensate for the days I left her alone. I know hair styling. I want to go work in a hair salon so that my mom can have a comfortable life. I would like to work with the Children's Rights Association to be able to satisfy the victims' families to forgive anywhere in Iran.
Q: Do you think the death penalty is an appropriate punishment for children who commit a crime while they are under 18 years of age?
A: For any child, going to prison in these conditions is a hundred times worse than death. Execution is just one moment. They pull the stool from under your feet, your neck breaks, and you suffocate. However, prison is hell. You go to prison with an accusation, you come out with thousands of diseases and disorders. Over there, weaker kids are subject to all types of abuse. Depression, addiction, and AIDS, each one is 1000 times worse than death.
Siavosh, Persian2English


My mind is going a million miles an hour right now, but I want to post, since I won't be around all next week. :O Yesterday a friend of mine invited the kids and I to join her and her kids for a week near Lake George, NY! So we're leaving in a couple days. Today and tomorrow will be spent doing all the laundry and packing so we can leave at sunrise for the 10+ hour drive.
I have one invincible goldfish left. Actually, he's some sort of tetra, but he's gold in color. I've taken all of the gravel out of the aquarium, trying to eliminate the black hair algae. Now that I'll be gone for a week, the fish will just get fed and have to live with the yuck. I'll launch a new plan of attack after we get back.
Like I said, my head is still sort of spinning. I'm a planner, and this flying-by-the-seat-of-my-pants in two days is sort of disconcerting.
Have you watched Gravity Falls? My kids are loving it. It's on Hulu, but it looks like it's six years old or so. I'm surprised no one ever mentioned it before.
Last night we rented Ready Player One from the Redbox. While Jack didn't really watch it (which surprises me, since he LOVES video game stuff), the rest of us enjoyed it. Of course now I'm on the library's list to borrow the book for my Kindle. I'm #110 in line, so don't hold your breath for that review.
We're putt-putt golfing this afternoon, but we'll probably head to the library after that for our road trip tradition - a couple audio books for the drive. Now that Maggie is big enough for the front seat, she can't watch movies, and I certainly don't want the kids playing their darn phone games for that long each way of our drive.
Just wait til you see my list of books read in July - I've been a reading machine! I think I'm at four or five so far, and starting another one today!
Good news! I forgot to eat my leftover pizza for breakfast, so now I know what I'm having for lunch! We were going to have pizza and a movie on Saturday, but hubby had a hankering for it last night, so we swapped last night's sloppy joes for Saturday instead.
I am definitely all over the place, and feeling spread thin, but I'm sure a week of vacation will reset all of that. Enjoy your week!
Enjoy your vacation Becki!!! Have a fun and safe time!
I *loved* Ready Player One - both the book and the movie. The movie was fabulous on the big screen and has a lot of homages in it to other Spielberg movies and classics. The book was very good too ... I'm not sure which one I enjoyed more, actually.
I haven't played Putt putt in years, sounds like fun. My husband saw Ready player One in the theater and really enjoyed it. I don't think it's a movie for me though. I wish I could give you some suggestions for games on the phone but I've never played any on mine.


text:
\section{Introduction}
Recently charged black hole with a scalar hair in (2 + 1)
dimensions, where the scalar field couples to gravity and it also
couples to itself with the self-interacting potential, analyzed by
the Xu and Zhao [1]. They found appropriate conditions for the
metric in which a charged extremal black hole reproduced as an
asymptotically AdS space-time with a naked singularity at the
origin. Also they shown that the size of the outer horizon increases
monotonically with both the scalar hair and the electric charge.
Refs. [2-6] has similar studies on (2+1)-dimensional rotating hairy
black holes. Such 3D black holes are also interesting to study
AdS/CFT and related topics [7, 8, 9]. However calculation of the
thermodynamic quantities left as an open problem. We know that the
black hole thermodynamics and statistics are interesting fields of
theoretical physics. So we studied in several papers these subjects
for various black holes [10-17]. In that case critical behaviors of
thermodynamical quantities of 3D black holes with a scalar hair has
been studied in the Ref. [18] and concluded the presence of the
cosmological constant may be considered as a thermodynamic pressure
and its conjugate quantity as a volume. Also it is found that the
corresponding equation of state predicts a critical universal number
depending on scalar hair parameter.\\
Now, in this paper we consider charged black hole with a scalar hair
in (2 + 1) dimensions and calculate thermodynamical and statistical
quantities. Indeed we investigate effects of black hole charge and
scalar field on thermodynamical and statistical parameters. Also we
study spectroscopic aspects [19-21] of this black hole and obtain
discrete spectrum. We find that this system has thermodynamical
stability. Therefore in next section we review charged hairy black
hole in (2+1) dimensions. Then in section 3 we study thermodynamics
and obtain entropy, temperature and heat capacity which yields to
obtain thermal stability. spectroscopic aspects of this black hole
studied in section 4 and statistical mechanics of this black hole
investigated in section 5. Finally in section 6 we give conclusion.
\section{Charged hairy black hole in (2+1) dimensions}
In this work we consider a class of black hole solution obtained by
the Ref. [1]. The solution represents static charged black hole with
a scalar field given by the following action,
\begin{equation}\label{s1}
S=\frac{1}{2}\int{d^{3}
x\sqrt{-g}[R-g^{\mu\nu}\nabla_{\mu}\phi\nabla_{\nu}\phi-\xi
R\phi^2-2V(\phi)-\frac{1}{4}F_{\mu\nu}F^{\mu\nu}]},
\end{equation}
where $\xi$ is a coupling constant between gravity and the scalar
field which will be fixed as $\xi=1/8$ [1].\\
This black hole described by the following static, circularly and
asymptotic metric [1],
\begin{eqnarray}\label{s2}
ds^2=-f(r)dt^2+\frac{1}{f(r)}dr^2+r^{2}d\psi^{2},
\end{eqnarray}
where,
\begin{equation}\label{s3}
f(r)=(3\beta-\frac{Q^2}{4})+(2\beta-\frac{Q^2}{9})\frac{B}{r}-Q^2(\frac{1}{2}+\frac{B}{3r})\ln(r)+\frac{r^2}{l^2}.
\end{equation}
$Q$ is the electric charge, $l$ is integration constants and related
to the cosmological constant, $r$ denotes the usual radial
coordinate with $r\geq0$, $-\infty<t<\infty$, and
$-\pi\leq\psi\leq\pi$. Also $\beta$ is integration constants depends
on the black hole charge and mass, and $B$ related to the scalar
field as,
\begin{eqnarray}\label{s4}
\beta&=&\frac{1}{3}(\frac{Q^2}{4}-M),\nonumber\\
\phi(r)&=&\pm\sqrt{\frac{8B}{r+B}}.
\end{eqnarray}
By imposing various constraints, the horizons radius are obtained
[1] and we go ahead the black hole thermodynamics through these
cases.
\section{Thermodynamics}
In order to study thermodynamics of a charged hairy black hole in
(2+1) dimensions we begin with the generic form of the entropy,
\begin{equation}\label{s5}
s=\frac{(g_{\psi\psi})^{\frac{d-1}{2}}}{4G_{N}}|_{r=r_{+}},
\end{equation}
where $r_{+}$ is horizon radius obtained by $f(r)=0$ using the
equation (3). Therefore, using the metric (2) in the relation (5)
gives the following entropy,
\begin{equation}\label{s6}
s=4\pi r_{+},
\end{equation}
where we assumed $16\pi G_{N}=1$. In order to obtain black hole
temperature, potential and special heat capacity we used the
following relations, respectively,
\begin{equation}\label{s7}
T=(\frac{\partial M}{\partial s}),
\end{equation}
\begin{equation}\label{s8}
V=(\frac{\partial M}{\partial Q}),
\end{equation}
and,
\begin{equation}\label{s9}
C=T(\frac{\partial s}{\partial T}),
\end{equation}
where $M$ and $Q$ are the black hole mass and charge respectively.
The sign of specific heat determines thermodynamics stability of
black hole. If the black holes have positive specific heat then it
is in stable equilibrium [22, 23].\\
First of all we study the special case of uncharged black hole.
Then, in order to find the effect of the black hole charge extend
our work to the several cases of charged black hole.
\subsection{Uncharged black hole}
In the case of uncharged black hole we set $Q=0$ in the equation
(3). The other important parameter is $\beta$. In the case of
$\beta=0$ we see that the black hole radius and therefore the black
hole entropy vanishes. On the other hand for the case of
$\beta\neq0$ the equation (3) reduced to the following,
\begin{equation}\label{s10}
f(r)=\frac{r^2}{l^2}-M-\frac{2BM}{3r}.
\end{equation}
Then, the black hole horizon is given by,
\begin{equation}\label{s11}
r_{+}={\frac{\left(9BM{l}^{2}+3\sqrt{3}\sqrt{{M}^{2}{l}^{4}
\left(3B^{2}-M{l}^{2}\right)}\right)^{2/3}+3M{l}^{2}}{3
\left(9BM{l}^{2}+3\sqrt{3}\sqrt{{M}^{2}{l}^{4}\left(3{B}^{2}-M{l}^
{2}\right)}\right)^{\frac{1}{3}}}}.
\end{equation}
Therefore the black hole entropy easily obtained by using the
equation (6). In the Fig. 1 we see that the black hole entropy
increased by scalar field parameter $B$. This is in agreement with
the result of the Ref. [1] which tells that the size of the black
hole must increase as $B$ increases.

\begin{figure}[th]
\begin{center}
\includegraphics[scale=.25]{0.eps}
\caption {Plots of black hole entropy in terms of $B$ with $M=1$ and
$l=1$.}
\end{center}
\end{figure}

Then, using the relations (6) and (10) we can extract
entropy-dependent mass of the black hole as the following,
\begin{equation}\label{s12}
M=\frac{3{s}^{3}}{16{\pi}^{2}{l}^{2}(8\pi B+3s)}.
\end{equation}
By using the relation (7) we can obtain the black hole temperature
in terms of the entropy as the following,
\begin{equation}\label{s13}
T=\frac{9{s}^{2}(4\pi B+s)}{8{\pi}^{2} {l}^{2}(8\pi B+3s)^{2}}.
\end{equation}
In the fig. 2 we can see that the scalar field parameter $B$
decreases the black hole mass but increases the black hole
temperature. Since $\Lambda=-\frac{1}{l^2}$, then we conclude that
increasing of $l$ (or decreasing of cosmological constant) can
reduces the black hole mass and temperature. Finally, from the
equation (9) one can obtain,
\begin{equation}\label{s14}
C=\frac{(8\pi B+3s)s(4\pi B+s)}{3s^{2}+24\pi Bs+64{\pi}^{2}{B}^{2}}.
\end{equation}
In the Fig. 3 we draw specific heat in terms of entropy. We see
thermodynamical stability of this system in any temperature with
varying $B$.

\begin{figure}[th]
\begin{center}
\includegraphics[scale=.25]{1.eps}\includegraphics[scale=.25]{2.eps}
\caption {Plots of black hole temperature and mass with $l=1$ and
for $B=0$ (dotted line), $B=1$ (solid line), $B=5$ (dashed line).}
\end{center}
\end{figure}

\begin{figure}[th]
\begin{center}
\includegraphics[scale=.25]{3.eps}
\caption {Plot of heat capacity versus entropy with $l=1$ and for
$B=0$ (dotted line), $B=1$ (solid line), $B=5$ (dashed line).}
\end{center}
\end{figure}

In the special case of $\beta=-\frac{B^2}{l^2}$, where the self
interacting scalar field vanishes, we have a conformal black hole
with,
\begin{equation}\label{s15}
f(r)={\frac{{r}^{2}}{{l}^{2}}}-{\frac
{3{B}^{2}}{{l}^{2}}}-{\frac{2{B}^{3}}{r{l}^{2}}},
\end{equation}
which yields to the following black hole mass,
\begin{equation}\label{s16}
M=\frac{3s^2}{64\pi^2 l^2}.
\end{equation}
Since $B>0$, the horizon radius is given by
$r_{+}=2B=2l\sqrt{\frac{M}{3}}$, therefore the black hole entropy is
obtained as the following,
\begin{equation}\label{s17}
s=8\pi B =8\pi l\sqrt{\frac{M}{3}}.
\end{equation}
Hence the black hole temperature reads,
\begin{equation}\label{s18}
T={\frac{3}{32}}{\frac{s}{{\pi}^{2}{l}^{2}}},
\end{equation}
where we used the relations (7) and (16). Then the special heat is
given by,
\begin{equation}\label{s19}
C=8\pi l\sqrt{\frac{M}{3}}=\frac{32\pi^2 l^2}{3}T=s.
\end{equation}
It is interesting to find special heat equal to the entropy. It
tells that the heat capacity never decreases and our system will be
in thermal stability.

\subsection{Charged black hole}
Our interesting case is the charged black hole where we can
investigate the effect of black hole charge on thermodynamical
quantities. We will consider two special cases depend on scalar
field parameter $B$ as the following.
\subsubsection{The case of $B=0$}
If we set $B=0$ then the scaler field vanishes and the charged BTZ
black hole appears in (2+1) dimensions reproduced [24, 25]. In that
case the relation (3) reduced to the following,
\begin{equation}\label{s20}
f(r)={\frac {{r}^{2}}{{l}^{2}}}-M-\frac{Q^{2}}{2}\ln(r).
\end{equation}
Now, we discuss about various ranges of $\beta$ which play an
important role on the space-time.\\
In the case of $\beta<\frac{Q^2}{6}\ln(r)$, the $f(r)$ has two zeros
that each of them correspond to the black hole horizons, then there
is a non-extremal charged AdS black hole with no scalar hair.\\
In the case of $\beta=\frac{Q^2}{6}\ln(r)$, the $f(r)=0$ obtained
for the $r=0$.\\
In the case of $\beta>\frac{Q^2}{6}\ln(r)$, the $f(r)$ has no zero
that causes an asymptotically AdS space-time with a naked
singularity in the origin.\\
The extremum of the metric function (20), which is obtained by
$f^{\prime}(r)=0$, given for the radius $r=\frac{1}{2}Ql$. In that
case the black hole mass is given by the following relation,
\begin{equation}\label{s21}
M=\frac{r_{+}^{2}}{l^2}-\frac{Q^2}{2}\ln(r_{+})=\frac{s^2}{16\pi^{2}l^2}-\frac{Q^2}{2}
\ln(\frac{s}{4\pi}).
\end{equation}
Therefore, by using the relation (7) the black hole temperature
obtained as,
\begin{equation}\label{s22}
T=\frac{s}{8\pi^2 l^2}-\frac{Q^2}{2s}.
\end{equation}
Finally the specific heat reads,
\begin{equation}\label{s23}
C=4\pi^2 l T(1+l\sqrt{2T}).
\end{equation}

\begin{figure}[th]
\begin{center}
\includegraphics[scale=.25]{4-1.eps}\includegraphics[scale=.25]{4-2.eps}
\caption {Plots of black hole temperature and mass for different
values of black hole charge with $l=1$. $Q=0$ (dotted line), $Q=1$
(solid line), $Q=3$ (dashed line).}
\end{center}
\end{figure}

We find that the black hole charge decreases the black hole
temperature and therefore heat capacity (see Fig. 4). We see that
for higher entropy the black hole charges has no important effect on
the black hole temperature. Also there is a critical point for the
black hole mass ($M_{c}$) where black hole charge increases the
black hole mass for $M<M_{c}$ and decreases the black hole mass for
$M>M_{c}$. The critical value of the black hole mass obtained for
$s\simeq12$ for the given black hole charge.

\subsubsection{The case of $B>0$}
In presence of the scalar field and using definition (4) of $\beta$
the metric function (3) reduced to the following,
\begin{equation}\label{s24}
f(r)=\frac{r^{2}}{l^{2}}-M+\frac{(\frac{Q^{2}}{6}-2M)B}{3r}-\frac{Q^{2}}{2}(1+{\frac{2B}{3r}})
\ln(r).
\end{equation}
Then, the black hole mass is given by,
\begin{equation}\label{s25}
M=\frac{9s^{3}+32{Q}^{2}{l}^{2}\pi^{3}B-72{Q}^{2}\pi^{2}{l}^{2}s\ln(\frac{s}{4\pi})
-192{Q}^{2}\pi^{3}{l}^{2}B\ln(\frac{s}{4\pi})}
{48\pi^{2}l^{2}(3s+8\pi B)}.
\end{equation}
Hence, we can obtain the black hole temperature as the following,
\begin{equation}\label{s26}
T=\frac{9s^{4}+36\pi
B{s}^{3}-36\pi^{2}l^{2}Q^{2}s^{2}-208\pi^{3}l^{2}Q^{2}Bs-256\pi^{4}l^{2}Q^{2}B^{2}}{8\pi^{2}l^{2}s(3s+8\pi
B)^{2}}.
\end{equation}
We can see from the Fig. 5 that the scalar charge decreases the
black hole temperature and mass. Also if $B>3$ the black hole mass
has negative sectors, therefore we can find a constraint on the
scalar charge.

\begin{figure}[th]
\begin{center}
\includegraphics[scale=.25]{5-1.eps}\includegraphics[scale=.25]{5-2.eps}
\caption {Plots of black hole temperature and mass for different
values of the scalar charge with $l=1$ and $Q=1$. $B=0$ (dotted
line), $B=1$ (solid line), $B=3$ (dashed line).}
\end{center}
\end{figure}

Finally the specific heat obtained by using the relation (9). We
find that the scalar charge decreases the heat capacity and there
are some negative sectors, however for appropriate choices of $B$,
$Q$ and $s$ where the black hole temperature is positive then, the
system is in thermal stability (see Fig. 6).

\begin{figure}[th]
\begin{center}
\includegraphics[scale=.25]{6.eps}
\caption {Plots of heat capacity for different values of the scalar
charge with $l=1$ and $Q=1$. $B=0$ (dotted line), $B=1$ (solid
line), $B=2$ (dashed line).}
\end{center}
\end{figure}

\section{Spectroscopy}
In this section we discuss the properties of entropy quantization
and the area spectrum. In that case the first law of thermodynamics
for charged black hole is [26],
\begin{equation}\label{s27}
dM=\frac{T}{4}dA+VdQ,
\end{equation}
where $A$ is surface area of the event horizon which for the (2+1)
dimensional black hole is given by,
\begin{equation}\label{s28}
A=2\pi r_{+}.
\end{equation}
Therefore we can write,
\begin{equation}\label{s29}
\Delta A=2\pi dr_{+}.
\end{equation}
We try to obtain circumference spectrum for two different cases of
uncharged and charged black holes.

\subsection{Uncharged black hole}
In the first case we set $Q=0$. Then, for the case of $\beta\neq0$,
the equations (13), (27) and (29) give the following expression,
\begin{equation}\label{s30}
dM=\frac{9}{l^{2}}\frac{r_{+}^{2}}{2B+3r_{+}}\left[1-\frac{r_{+}}{2B+3r_{+}}\right]dr_{+}.
\end{equation}
Using the lapse function we can calculate the surface gravity as the
following,
\begin{equation}\label{s31}
\kappa=\frac{1}{2}\frac{df(r)}{dr}|_{r=r_{+}}=\frac{8r_{+}-1}{8l^{2}}.
\end{equation}
Then, using the equation (30) we can obtain,
\begin{equation}\label{s32}
dr_{+}=\frac{4}{9}\frac{l^{2}(16B+3+24\kappa l^{2})^{2}}{(1+8\kappa
l^{2})^{2}(8B+1+8\kappa l^{2})}dM.
\end{equation}
Therefore we one can find,
\begin{equation}\label{s33}
\Delta A=\frac{8\pi}{9}\frac{l^{2}(16B+3+24\kappa
l^{2})^{2}}{(1+8\kappa l^{2})^{2}(8B+1+8\kappa l^{2})}dM,
\end{equation}
where we used the equations (29) and (32). Now, by replacing
$\kappa$ in terms of $M$, the adiabatic invariant integral is given
by the following,
\begin{equation}\label{s34}
I=\int \Delta A=\frac{32\sqrt{3}\pi}{27}\sqrt{M},
\end{equation}
which is achieved by supposing the special case of
$B=\sqrt{\frac{M}{3}}$ and
$l=1$.\\
Applying Bohr-Sommerfeld quantization condition and the equation in
terms of $r_{+}$ one can obtain,
\begin{equation}\label{s35}
I=\frac{8}{9} (2\pi r_{+})\simeq n\hbar.
\end{equation}
Therefore we can obtain,
\begin{equation}\label{s36}
A_{n}\simeq \frac{9}{8}n\hbar.
\end{equation}
We can we see that the spectrum of uncharged hairy black hole is
discrete, and the spectrum is independent of the black hole
parameters as expected.

\subsection{Charged black hole}
First of all we study the case of $B=0$ and obtain,
\begin{equation}\label{s37}
\Delta A=4\left(\frac{r_{+}}{2\pi l^{2}}-\frac{Q^{2}}{8\pi
r}\right)^{-1}(dM+\frac{dQ}{l^{2}}),
\end{equation}
where we used $V=-1/l^{2}$ [1], also horizon radius in terms of
black hole mass and charge obtained as the following,
\begin{equation}\label{s38}
r_{+}=\exp\left(-\frac{1}{2}LambertW\left[-\frac{4e^{-\frac{4M}{Q^{2}}}}{l^{2}Q^{2}}\right]-\frac{2M}{Q^{2}}\right),
\end{equation}
which reduced to the following relation in asymptotic expansion for
the large $Q$,
\begin{equation}\label{s39}
r_{+}=e^{\frac{2(1-M)}{Q^{2}}},
\end{equation}
where $l=1$ assumed. After some calculations one can obtain,
\begin{equation}\label{s40}
A_{n}\simeq \frac{n\hbar}{8}-\frac{32\pi}{Q}
\end{equation}
As before for the first term we see that the circumference of the
charged hairy black hole is discrete. In this system, the
circumference spectrum depends on the black hole parameters, but the
circumference spacing is independent of the black hole parameters.\\
On the other hand by choosing $B=\frac{Ql}{6}$ we can obtain the
surface gravity as the following,
\begin{equation}\label{s41}
\kappa=\frac
{648r_{+}^{4}+108Qlr_{+}^{3}+162{Q}^{2}{l}^{2}r_{+}^{2}-39{Q}^{3}{l}^{3}r_{+}-2{Q}^{4}{l}^{4}}{72{l}^{2}
\left(9r_{+}+ Ql\right) r_{+}^{2}},
\end{equation}
which yields to the following result,
\begin{eqnarray}\label{s42}
A_{n}\simeq 2n\hbar+\frac {\pi
lQ}{5832}\left((68+368\ln(l))Q^{3}+(108+864\ln(l)){Q}^{2}+5562\ln(l)
{Q}+1296\right).
\end{eqnarray}
This case of a charged black hole with scalar hair has an
independent spacing circumference and its spectrum is achieved in
respect of $l$ ($B$) and $Q$ as black hole parameters.

\section{Statistical mechanics}
By using the thermodynamical quantities one can obtain some
important quantities such as partition function which is important
in statistical mechanics. First of all we should obtain free energy,
\begin{eqnarray}\label{s43}
F=- \int s dT.
\end{eqnarray}
This quantity is important to study statistics of system and also
useful to obtain internal energy,
\begin{eqnarray}\label{s44}
E=F+ sT.
\end{eqnarray}
Then one can obtain partition function as the following,
\begin{eqnarray}\label{s45}
Z=\exp(-\frac{F}{k T}),
\end{eqnarray}
where $k$ is Boltzmann constant which we assumed $k=1$ for
simplicity. By using partition function one can obtain probability,
\begin{eqnarray}\label{s46}
p=\exp(-\frac{\Xi}{Z}),
\end{eqnarray}
where $\Xi$ is called grand partition function and defined by,
\begin{eqnarray}\label{s47}
\Xi=\exp(-\frac{E}{T}),
\end{eqnarray}
and microcanonical states number is given by,
\begin{eqnarray}\label{s48}
\Omega=-T \ln(\Xi)
\end{eqnarray}
The number of micro states produces statistical entropy as the
following,
\begin{eqnarray}\label{s49}
s_{micro}=ln \Omega.
\end{eqnarray}

\subsection{The case of $Q=0$}
In that case we have two separated cases depend on parameter
$\beta$. In the first case we set $\beta=0$, where the entropy
obtained by using the relation (11). By using the relation (43) and
(44) we draw free energy and internal energy in the Fig. 7. It shows
that the free energy reduced by scalar charge and internal energy
has a maximum at $B=0$.

\begin{figure}[th]
\begin{center}
\includegraphics[scale=.25]{7-1.eps}\includegraphics[scale=.25]{7-2.eps}
\caption {plots of free energy and internal energy in terms of
scalar charge with $M=1$ and $l=1$.}
\end{center}
\end{figure}

Therefore we can obtain partition function as the following,
\begin{equation}\label{s50}
Z=e^{\frac{2\pi\left(81r_{+}^{4}+108B r_{+}^{3}+36
B^{2}r_{+}^{2}+48B^{3}r_{+}+16B^{4} \right)}{81\left(B+r_{+}
 \right)r_{+}^{2}}}.
\end{equation}
Also, probability obtained by using the relation (46) as the
following,
\begin{equation}\label{s51}
p=e^{-{e^{-4\pi r_{+}}}},
\end{equation}
which illustrated in the Fig. 8. It shows that maximum probability
available for higher scalar charge.

\begin{figure}[th]
\begin{center}
\includegraphics[scale=.25]{8.eps}
\caption {plot of probability in terms of scalar charge with $M=1$
and $l=1$.}
\end{center}
\end{figure}

In the second case we set $\beta=-\frac{B^2}{l^2}$ and find that,
\begin{equation}\label{s52}
Z=e^{4\pi B},
\end{equation}
and
\begin{equation}\label{s53}
\Omega=3{\frac {B^{2}}{{l}^{2}}}.
\end{equation}
Therefore we can obtain microcanonical entropy as the following,
\begin{equation}\label{s54}
s_{micro}=\ln(\frac{3B^{2}}{l^{2}}).
\end{equation}
We can see that the microcanonical entropy increased by $B$ as
expected.
\subsection{The case of $Q\neq0$}
In order to obtain the effect of black hole charge we consider two
special cases of $B=0$ and $B\neq0$. In the first case which horizon
radius is given by the equation (38), then the free energy obtained
as,
\begin{equation}\label{s55}
F=r_{+}^{2}+\frac{1}{2}Q^{2}\ln(r_{+}),
\end{equation}
It is easy to check that the black hole charge increased the free
energy. In the Fig. 9 we draw plot of internal energy and find that
there is a maximum for $Q\sim2$.

\begin{figure}[th]
\begin{center}
\includegraphics[scale=.25]{9.eps}
\caption {plot of internal energy in terms of electric charge with
$M=1$ and $l=1$.}
\end{center}
\end{figure}

Also partition function obtained as the following,
\begin{equation}\label{s56}
Z=1+\frac{8\pi(2-M)}{Q^{2}}+\mathcal{O}(\frac{1}{Q^{4}}),
\end{equation}
where we used asymptotic expansion for the large black hole charge.
Probability of this case illustrated in the Fig. 10.

\begin{figure}[th]
\begin{center}
\includegraphics[scale=.25]{10.eps}
\caption {plot of probability in terms of black hole charge with
$M=1$ and $l=1$.}
\end{center}
\end{figure}

In the general case we consider $Q\neq0$ and $B\neq0$ and obtain,
\begin{eqnarray}\label{s57}
F=&-&r_{+}^{2}+\frac{1}{3}\frac{BQ}{3r_{+}+2B}(1-\frac{Q}{3r_{+}+2B})\nonumber\\
&-&\frac{16}{9}\frac{B^{3}}{3r_{+}+2B}(1-\frac{B}{3r_{+}+2B})-\frac{1}{2}Q^{2}\ln(r_{+}).
\end{eqnarray}
In order to find effect of electric and scalar charges we draw plot
of free energy in the Fig. 11. In the Fig. 11 (a) we fixed scalar
charge and vary electric charge and find that the electric charge
increases free energy for $r_{+}<1$ and decreases free energy for
$r_{+}>1$. Then in the Fig. 11 (b) we fixed electric charge and vary
scalar charge and find that free energy decreased by scalar charge
as expected from previous results. Similar results obtained for
internal energy $E$.

\begin{figure}[th]
\begin{center}
\includegraphics[scale=.25]{11-1.eps}\includegraphics[scale=.25]{11-2.eps}
\caption {plot of free energy in terms of black hole horizon. (a)
$B=1$ and $Q=3$ (dotted line), $Q=5$ (solid line), $Q=7$ (dashed
line). (b) $Q=1$ and $B=1$ (dotted line), $B=2$ (solid line), $B=3$
(dashed line).}
\end{center}
\end{figure}

Probability of this case is also obtained as before. Finally we can
obtain microcanonical entropy which is illustrated in the Fig. 12.
It shows that the electric and scalar charges decrease the
microcanonical entropy.

\begin{figure}[th]
\begin{center}
\includegraphics[scale=.25]{12-1.eps}\includegraphics[scale=.25]{12-2.eps}
\caption {plot of microcanonical entropy in terms of black hole
horizon. (a) $B=1$ and $Q=1$ (dotted line), $Q=3$ (solid line),
$Q=5$ (dashed line). (b) $Q=1$ and $B=2$ (dotted line), $B=4$ (solid
line), $B=6$ (dashed line).}
\end{center}
\end{figure}

\section{Conclusions}
In this paper we considered charged hairy black hole in (2+1)
dimensions and studied thermodynamics, statistics and spectroscopy.
In the simplest case of zero-charge black hole we obtained black
hole entropy and found that scalar charge increased it. We obtained
black hole mass and temperature which are increasing function of
entropy. We found that scalar charge increased the black hole
temperature and decreased black hole mass. Then we obtained the
effect of black hole charge on thermodynamics quantities. Similar to
the uncharged case, the black hole temperature is increasing
function of entropy, but black hole mass decreased first and then
increased. In all cases we have thermal stability which verified by
using positive sign of specific heat. Spectroscopy of this system
shows that the circumference of the charged hairy black hole is
discrete. In this system, the circumference spectrum depends on the
black hole parameters, but the circumference spacing is independent
of the black hole parameters. We obtained also partition function
and studied statistical mechanics of charged hairy black hole in
(2+1) dimensions. We found that the microcanonical entropy is
decreasing function of black hole charge.

redpajama_set_name: RedPajamaArXiv


text:
Category Archives: Hataraku Maou-sama!
Year in Review 2013: The Junior High Second Year Bridge Across Escapism, New World Disorder
When I was watching episode 10 of Yuushibu the thought dawned on me: this is about a new world order. If we take the narrative about the lost generation of Japan to heart, the young adults of Japan has to prime themselves to a new reality where job security is an unicorn and living the life their parents do 40 years earlier is just how things not going to be–until they find the wind beneath their wings. It's the reality today's Millennial are dealing with in America, but things are trickier out in Japan.
The big picture view is that Asia, on the whole, are still banging out explosive growths. You can say China may have "landed" but it's still growing hella fast. India is probably going to get caught up. On the other hand Japan is like the edge of a Red Giant, where fusion go beyond helium and into the heavier elements, eventually crunching back into something more suitable for a dying star. I guess things may go to hell if China and India crash hard enough? I guess that's kind of a grim analogy.
But that's exactly how it feels for our protagonists who had to swallow their dreams and go live a part-timer's life working in a big-box electronics store. And in some ways this is what is truly adult about that sort of a story, it's not about people living their dreams, doing anything they can. It's about finding out about yourself as you find a place for yourself in the world. Like a good football defense: bend but not break.
In Hatarake Maousama, the story plays itself out differently but the concept is the same. A fantasy big shot learns to be a great McD assistant manager. But here's the thing: if you make it as a shift manager at a Wal-mart or Best Buy, you can surely make a decent living? It's a real salary, although you may have to work a lot of off hours. It's like Yuusha's job doing customer service for DoCoMo. I don't know, but some of these jobs are not entirely terrible.
It's a much more telling story for All A, I guess.
Here's exactly the thing. Torn between, say, an inaka narrative, where we always give a lot of face for farmers, doing service jobs or even blue-collar type jobs in today's cities and suburbs just don't get the same kind of respect, even if said jobs are often much better and preferred than farming. Or any of the traditional arts of the land–brewing sake for example. Unless you got electron microscopes for eyes? I am not sure what makes the disenchanted feel better. However as far as head tricks go, you can do worse than Yuushibu and Hatarake Maousama. You can do worse than Kyon in Haruhi or Goto in Samumenco. You can do worse, only because it's like everybody is doing it. Log Horizon? Outbreak Company? LOL Maoyu?? Maybe this is me looking like a hammer because everything seems to fit like a nail, but in 2013 everything looks like it.
All of this just goes and point out Yet Another Reason Why SAO is problematic. It's the difference between a new world and an old one: it's a world where the meek conquers the strong as lion rest next to the lamb. As far as fantasies go, it's a classic, and herbivores sure eat it up. And this is also why nobody is procreating; it's some new world order. (Versus just jamming it in as if you haven't done it for two years. Virtually.)
And of course, unless you've seen Yuushibu up to episode 10, you might not know what I'm even talking about. Let's just frame it real-quick-like–domesticated devil queen heiress decides to apply big box retail to the demonic world in a stereotypical fantasy hero-versus-maou setting, people think she's a fool, but the idea comes across brilliantly.
And this is why Love Lab is one hella good anime that y'all should watch.
Year in Review 2013 Index:
New World Disorder
iM@S
Signs from a Mermaid
3 comments	| posted in Hataraku Maou-sama!, Introspectives, Maoyu Maou Yuusha, Modern Visual Culture, Yuusha ni Narenakatta Ore wa Shibushibu Shuushoku wo Ketsui Shimashita.
Season Ending Blog Anthology
A chain of short blog posts about their subjects. The last one is a run-on about Moenovel. The rest are about currently-ending or airing anime.
10 comments	| posted in Aku no Hana, Bishoujo Gaming, English Language Modern Visual Fandom, Hataraku Maou-sama!, Kakumeiki Valvrave, Majestic Prince, Modern Visual Culture, Namiuchigiwa no Muromi-san, Photo Kano, Yahari Ore no Seishun Rabu Kome wa Machigatteiru.
Mid-Season Update, Spring 2013
Anime blogs are suppose to blog about anime right? Can I stop being one?
Before I begin I just want to talk about the APR. The anime power ranking is a lot of fun and if you are a regular simulcast-y type viewer, maybe Kevo would have you give him your 2c every week. I'm a major slacker and wish I could be home and send emails about anime on the weekends, but that is usually not typically possible after Friday night and until Sunday night, when the APR is calculated.
Guilty plug aside, I guess I'll keep it simple: Up, steady and on hold/dropped. Links to viewing portals. Ordering is semi-random.
Gargantia on the Verdurous Planet – A veritable science fiction healing factory. Hanaharu's character designs alone might be worth the trip by itself.
OreImo Season 2 – I think this season is really bringing the pain, and for sisucons pain is not always a bad thing. The awkward exchanges between Kyousuke and his friends is at least less painful than Aku no Hana's painful exchanges, which is good; that's a sanity check. But it's not a sanity check every seishun rom-com would pass. It's probably up because we're in the middle of the Shironeko arc.
Flowers of Evil – Since I am going to Animazement I probably should watch this to field questions for Nagahama. But it's also just kind of an amusing show in that the bouts of fear, doubt and madness are baked into the atmosphere, only to be punctured by the visuals. The rotoscoping works both for and against the whole endeavor in a strange way. The story will continue to descend into insanity and who doesn't love that? At least it's an easier watch than, say, Texhnolyze.
Muromi-san – It's half-length, but only if all gag anime was like this. It's well-paced. It's also the sort of Yukarin role that, well, is the best. Only if she plays characters like this all the time. That and people like this.
Attack on Titan – Well, it's a fun show how despair continue to be front-and-center to the plot and theme. I just don't know if that despair is for us or for the characters, because there is clearly a separation between "getting into the show" and "enjoying the show" in this case. Maybe this is because it does not focus on the plight of a single character.
Devil is a Part-timer – It's a fun show, with solid comedy both ways. I'm 1001% in Yusa's camp though. Chiho is adorable but I feel she's the weakest link so far. With the addition of the new character in the romantic formula and the end of the "introduction" arc, however, I'm not sure where this show is going to go.
Valvrave the Liberator – The problem with making a show that has clear call cards from all your past hits is that the audience expects your past hits in your new shows, and it is really difficult to surpass all your pass hits. At this point I half expect Valvrave to go the way of Geass R2. Will it jump a shark? It already has. But will it jump a dozen sharks? Will it jump over a shark pyramid? Will it jump over shark Starfleet? I don't know, but I know I will find out soon. That said, it would be a very considerable feat if it can replicate all that shark jumping in Sunrise's back catalog while remaining coherent, and arguably it is on the way to do just that.
Majestic Prince – Great show, for the Tatsuo Sato disciples among us. I think it's going through a dull period but hopefully things will come together much better than Rinne or Pirates. After all it resembles the Stellvia template, which is probably the more successful line of shows. Unfortunately it's kind of a wash for everyone else.
Space Brothers – Really glad that I had this backlog to work through, thus enabling me skipping all those recap episodes. Also now that the show is back to civilization, the full blown expectation of Japanese people hoisted upon unrealistic American experiences is again on display, highlighting yet again the real barrier between human and space exploration is human. And I mean it in the jaded, ironic, culturally hilarious kind of way.
Nyaruko-san W – I can't really be bothered by this show but the shotgun jokes do still find their target week after week. It's definitely a drop from last season and to me this is now a drop-worthy show that I'm still watching partly because of blogging obligations.
Henneko – The cute factor increases or at least keep steady weekly. I'm going to get diabetes watching this anime, but I look forward to it anyway.
Photo Kano – I was going to drop this show until I watched the photo shoot with the student council president. I am not sure what that says about me (probably nothing flattering) but the visuals are worth a look. I think this is really an "anime no chikara" example because without the animation direction this show is totally crap-tier. I like how it makes me feel like a dirty upskirting otaku without being one, but at the same time some really enjoyable visuals, with or without fanservice. I hope that one photography girl's episode is all about dutch angles or something.
Sparrow's Hotel – It's a sin to be watching this without finishing Inferno Cop. I probably should finish Inferno Cop. Maybe same can be said of Nin Nin Shinobuden. Half-length. I'm actually a couple weeks behind but I think Minori Chihara's greatest power is leveraging her natural ditz.
My Teenage Romantic Comedy SNAFU – OreGuile as I call it, it's like a more pleasant version of Haganai in my mind. Which is probably a good thing. Also, what's up with making Hayami Saori do the chew-you-out routine? I hope some enterprising people have made a cliip of it circa Tari Tari. I mean I would pay for this. Seriously.
Railgun S – As long as it continues to dish out things I want out of this franchise, I'll continue to watch it I guess. The set of things I want out of this franchise may include beam weapons, awesome combat scenes, and that nostalgic, early 90s "winners don't use drugs" mentality and themes. What I have to put up with kind of evens out with what I get, so I'm not in the greatest hurry or most wanting of this series.
Hold/dropped
Yuyushiki – I want to like this show and for the most part I do like it, it is likable, but the pacing suffers greatly. I might still stick with it, I don't know.
Zettai Bouei Leviathan – Same can be said of this show. It's way weaker than the other anime with Leviathan in it. Other than for the seiyuu, nothing is lost by dropping this one so it made a quick out.
Date-a-Live – I really enjoy the premise and they started off with a nice, earnest-type tsundere character, which is a very safe bet. I hope the show lives up to its creative premise. It's on hold because there's too much on my plate so this anime will take a back seat; also I don't feel I have a good grasp of this show at 3 episodes in.
Chihayafuru S2 – I decided to put this off because it is really easy to marathon later. The funny thing is, after I got back from Japan I was going to catch up, but the word of a recap episode kind of put me off. So it continues to be put off. It's going to be fun to watch either way you do it, so I think it's no big deal other than having to mute everyone who tweets about the show.
The Severing Crime Edge – I just want to hit up all the fetishes every week. Not enough of a reason to continue I guess.
Red Data Girl – I probably would be watching it every week if I didn't have to dodge people who are watching the pre-release, and as a result unable to talk to anyone who is watching this show. I mean, I know many of us are not watching the pre-release but this totally ruins the overall discourse. That said I've not dropped this show, although it's up in the air if I will end up finishing it.
And that's all folks! Actually, I'm probably missing something, not including the shows I didn't want to include (I did skim through some Carnival and Utapri). But oh well…
PS. Aiura – This is, like a teaser/demo/sampler right? It's both funny how people whine about its length, and how cruel because it's so good yet so short. At the same time I think I'll be okay if every episode has a shot of the back of the leg of someone lying down, the whole time.
3 comments	| posted in Aku no Hana, Chihayafuru, Hataraku Maou-sama!, Kakumeiki Valvrave, Majestic Prince, Modern Visual Culture, Namiuchigiwa no Muromi-san, Photo Kano, Red Data Girl, Shingeki no Kyojin, Suisei no Gargantia, Toaru Kagaku no Railgun, Yahari Ore no Seishun Rabu Kome wa Machigatteiru., Yuyushiki


Hiawatha trains are the most heavily-used in Amtrak's Midwest network. .
Empire Builder (Chicago-Seattle/Portland): 1 roundtrip daily serving Milwaukee, Columbus, Portage, Wisconsin Dells, Tomah, and La Crosse. 15 different trips possible just in Wisconsin 1,035 along entire route.
891,638: total number of Wisconsin passenger on/offs..
1.8 to 1: Estimated Return on Investment (ROI) for each dollar invested in passenger rail.


Baker CD. Long-term ventilation for children with chronic lung disease of infancy. Curr Opin Pediatr. 2019 Mar 18. PMID: 30893186.
Khan EK, Baker CD. Endotracheal or tracheostomy tube occlusion during pediatric flexible bronchoscopy. Pediatr Pulmonol. 2018 Aug; 53(8):1004-1005. PMID: 29696825.
Baker CD. Biomarkers of pulmonary hypertension after preterm birth: The IMPROV study. Pediatr Pulmonol. 2018 02; 53(2):124-125. PMID: 29266849.
Thrasher J, Baker J, Ventre KM, Martin SE, Dawson J, Cox R, Moore HM, Brethouwer S, Sables-Baus S, Baker CD. Hospital to Home: A Quality Improvement Initiative to Implement High-fidelity Simulation Training for Caregivers of Children Requiring Long-term Mechanical Ventilation. J Pediatr Nurs. 2018 Jan - Feb; 38:114-121. PMID: 28943140.
Lutz SM, Thwing A, Schmiege S, Kroehl M, Baker CD, Starling AP, Hokanson JE, Ghosh D. Examining the role of unmeasured confounding in mediation analysis with genetic and genomic applications. BMC Bioinformatics. 2017 Jul 19; 18(1):344. PMID: 28724417.
Goss KN, Everett AD, Mourani PM, Baker CD, Abman SH. Addressing the challenges of phenotyping pediatric pulmonary vascular disease. Pulm Circ. 2017 Mar; 7(1):7-19. PMID: 28680562.
Baker CD, Halbower AC, Sterni LM, Sockrider M. Using a Home Ventilator with a Child. Am J Respir Crit Care Med. 2016 12 15; 194(12):P21-P22. PMID: 27976944.
Abman SH, Collaco JM, Shepherd EG, Keszler M, Cuevas-Guaman M, Welty SE, Truog WE, McGrath-Morrow SA, Moore PE, Rhein LM, Kirpalani H, Zhang H, Gratny LL, Lynch SK, Curtiss J, Stonestreet BS, McKinney RL, Dysart KC, Gien J, Baker CD, Donohue PK, Austin E, Fike C, Nelin LD. Interdisciplinary Care of Children with Severe Bronchopulmonary Dysplasia. J Pediatr. 2017 02; 181:12-28.e1. PMID: 27908648.
Gumina DL, Black CP, Balasubramaniam V, Winn VD, Baker CD. Umbilical Cord Blood Circulating Progenitor Cells and Endothelial Colony-Forming Cells Are Decreased in Preeclampsia. Reprod Sci. 2017 07; 24(7):1088-1096. PMID: 27879452.
Moore PE, Boyer D, O'Connor MG, Baker CD, Rettig JS, Sterni L, Halbower A, Wilson KC, Thomson CC. Pediatric Chronic Home Invasive Ventilation. Ann Am Thorac Soc. 2016 07; 13(7):1170-2. PMID: 27388405.
Boyer D, Thomson CC, Cohen R, Rao D, Dell S, Rayment J, Wang R, Dy FJ, Wambach J, Tam-Williams J, Simon D, Price E, Oermann CM, Singh A, Rettig JS, Duncan ED, Baker CD, Liptzin DR, Moore PE. ATS Core Curriculum 2016: Part III. Pediatric Pulmonary Medicine. Ann Am Thorac Soc. 2016 06; 13(6):955-66. PMID: 27295156.
Liptzin DR, Connell EA, Marable J, Marks J, Thrasher J, Baker CD. Weaning nocturnal ventilation and decannulation in a pediatric ventilator care program. Pediatr Pulmonol. 2016 08; 51(8):825-9. PMID: 27111393.
Sterni LM, Collaco JM, Baker CD, Carroll JL, Sharma GD, Brozek JL, Finder JD, Ackerman VL, Arens R, Boroughs DS, Carter J, Daigle KL, Dougherty J, Gozal D, Kevill K, Kravitz RM, Kriseman T, MacLusky I, Rivera-Spoljaric K, Tori AJ, Ferkol T, Halbower AC. An Official American Thoracic Society Clinical Practice Guideline: Pediatric Chronic Home Invasive Ventilation. Am J Respir Crit Care Med. 2016 Apr 15; 193(8):e16-35. PMID: 27082538.
Cristea AI, Baker CD. Ventilator weaning and tracheostomy decannulation in children: More than one way. Pediatr Pulmonol. 2016 08; 51(8):773-4. PMID: 27061157.
Baker CD. Diffusing Capacity in Bronchopulmonary Dysplasia. Can Function Determine Structure? Am J Respir Crit Care Med. 2016 Apr 01; 193(7):709-10. PMID: 27035779.
Baker CD, Martin S, Thrasher J, Moore HM, Baker J, Abman SH, Gien J. A Standardized Discharge Process Decreases Length of Stay for Ventilator-Dependent Children. Pediatrics. 2016 04; 137(4). PMID: 26966133.
Baker CD, Abman SH. Impaired pulmonary vascular development in bronchopulmonary dysplasia. Neonatology. 2015; 107(4):344-51. PMID: 26044102; PMCID: PMC4469359.
Guaman MC, Gien J, Baker CD, Zhang H, Austin ED, Collaco JM. Point Prevalence, Clinical Characteristics, and Treatment Variation for Infants with Severe Bronchopulmonary Dysplasia. Am J Perinatol. 2015 Aug; 32(10):960-7. PMID: 25738785; PMCID: PMC4617756.
Gien J, Abman SH, Baker CD. Interdisciplinary care for ventilator-dependent infants with chronic lung disease. J Pediatr. 2014 Dec; 165(6):1274-5. PMID: 25258147.
Baker CD, Alvira CM. Disrupted lung development and bronchopulmonary dysplasia: opportunities for lung repair and regeneration. Curr Opin Pediatr. 2014 Jun; 26(3):306-14. PMID: 24739494.
Baker CD, Abman SH, Mourani PM. Pulmonary Hypertension in Preterm Infants with Bronchopulmonary Dysplasia. Pediatr Allergy Immunol Pulmonol. 2014 Mar 01; 27(1):8-16. PMID: 24669351.
Baker CD, Black CP, Ryan SL, Balasubramaniam V, Abman SH. Cord blood endothelial colony-forming cells from newborns with congenital diaphragmatic hernia. J Pediatr. 2013 Sep; 163(3):905-7. PMID: 23684109; PMCID: PMC3755084.
Baker CD, Seedorf GJ, Wisniewski BL, Black CP, Ryan SL, Balasubramaniam V, Abman SH. Endothelial colony-forming cell conditioned media promote angiogenesis in vitro and prevent pulmonary hypertension in experimental bronchopulmonary dysplasia. Am J Physiol Lung Cell Mol Physiol. 2013 Jul 01; 305(1):L73-81. PMID: 23666751.
Baker CD, Abman SH. Umbilical cord stem cell therapy for bronchopulmonary dysplasia: ready for prime time? Thorax. 2013 May; 68(5):402-4. PMID: 23321604.
Baker CD, Accurso FJ. Preterm birth and airway inflammation in childhood. J Pediatr. 2012 Dec; 161(6):979-80. PMID: 22981953.
Baker CD, Balasubramaniam V, Mourani PM, Sontag MK, Black CP, Ryan SL, Abman SH. Cord blood angiogenic progenitor cells are decreased in bronchopulmonary dysplasia. Eur Respir J. 2012 Dec; 40(6):1516-22. PMID: 22496315.
Fujinaga H, Baker CD, Ryan SL, Markham NE, Seedorf GJ, Balasubramaniam V, Abman SH. Hyperoxia disrupts vascular endothelial growth factor-nitric oxide signaling and decreases growth of endothelial colony-forming cells from preterm infants. Am J Physiol Lung Cell Mol Physiol. 2009 Dec; 297(6):L1160-9. PMID: 19734318; PMCID: PMC2793187.
Baker CD, Ryan SL, Ingram DA, Seedorf GJ, Abman SH, Balasubramaniam V. Endothelial colony-forming cells from preterm infants are increased and more susceptible to hyperoxia. Am J Respir Crit Care Med. 2009 Sep 01; 180(5):454-61. PMID: 19483112; PMCID: PMC2742761.


000203697 520__ $$aSingle molecule studies using nanopores have gained attention due to the ability to sense single molecules in aqueous solution without the need to label them. In this study, short DNA molecules and proteins were detected with glass nanopores, whose sensitivity was enhanced by electron reshaping which decreased the nanopore diameter and created geometries with a reduced sensing length. Further, proteins having molecular weights (MW) ranging from 12 kDa to 480 kDa were detected, which showed that their corresponding current peak amplitude changes according to their MW. In the case of the 12 kDa ComEA protein, its DNA-binding properties to an 800 bp long DNA molecule was investigated. Moreover, the influence of the pH on the charge of the protein was demonstrated by showing a change in the translocation direction. This work emphasizes the wide spectrum of detectable molecules using nanopores from glass nanocapillaries, which stand out because of their inexpensive, lithography-free, and rapid manufacturing process.
000203697 700__ $$aSteinbock, L. J.


The BENTELER Group is organized into the three Divisions of BENTELER Automotive, BENTELER Steel/Tube and BENTELER Distribution. To ensure our customers achieve their goals successfully, we leverage expertise from the different Divisions and make use of our size and international reach. BENTELER Glass Processing Equipment and BENTELER Lightweight Protection enhance the product and service offering.
The holding company, BENTELER International AG in Salzburg, Austria, is responsible for the global strategic management of the Group and the Divisions. As well as BENTELER International AG, BENTELER Business Services GmbH, based in Paderborn, Germany, also carries out additional holding functions.
BENTELER Automotive offers development, production and services worldwide in the field of automotive technology – from individual components to entire system solutions, from press parts to global platforms. Individually adapted to the customers' wishes. Because as a specialist in chassis, modules, bodies, engine and exhaust systems as well as in e-mobility, we know how all these work together. That makes BENTELER one of the foremost suppliers worldwide.
BENTELER has been producing steel tubes for 100 years, and we are continuing to develop these products further. With this experience we can offer our customers around the world solutions all along the value chain. This has made BENTELER Steel/Tube into a leading producer of seamless and welded quality steel tubes for the automotive, energy and industrial sectors.
Over 310,000 square meters of warehouse space at around 50 locations in 30 countries worldwide. Plus a full range of carbon-steel and stainless-steel tubes: BENTELER Distribution is one of the top distributors of steel tubes worldwide. As well as a global sales and logistics network, we offer comprehensive first-stage processing and customer-specific additional services: from technical consulting to joint development and project support.
Organizationally within the umbrella of the BENTELER Automotive Division, BENTELER Glass Processing Equipment develops and produces machinery and systems for processing flat glass. Its product portfolio includes, for example, grinding and drilling machines, washing machines for glass, and screen-printing solutions – and it has customers in the automotive industry and in the fields of architectural and technical glass.
Since 2011 BENTELER Lightweight Protection has been offering high-specification solutions for greater security and lower weight. These include hot-formed components with few or even no welded seams made from a variety of steel alloys. Our customers are both manufacturers of cars and trucks as well as producers of armored vehicles.


To preclude a person or organization from an opportunity (i.e. - an event, deal, or situation) with a negative context.
In other words, the first party screws the second party out of a particular opportunity.
Upon arriving late to a dinner event, when dinner has already taken place.: "Well, it looks like I got jimmydicked out of dinner."
In a business context: "Why is Steve jimmydicking us on this deal?"
Get a jimmydick mug for your sister Nathalie.


text:
namespace Microsoft.Azure.Management.WebSites.Models
{
    using Newtonsoft.Json;
    using System.Linq;

    /// <summary>
    /// Description of a Virtual Network subnet that is useable for private
    /// site access.
    /// </summary>
    public partial class PrivateAccessSubnet
    {
        /// <summary>
        /// Initializes a new instance of the PrivateAccessSubnet class.
        /// </summary>
        public PrivateAccessSubnet()
        {
            CustomInit();
        }

        /// <summary>
        /// Initializes a new instance of the PrivateAccessSubnet class.
        /// </summary>
        /// <param name="name">The name of the subnet.</param>
        /// <param name="key">The key (ID) of the subnet.</param>
        public PrivateAccessSubnet(string name = default(string), int? key = default(int?))
        {
            Name = name;
            Key = key;
            CustomInit();
        }

        /// <summary>
        /// An initialization method that performs custom operations like setting defaults
        /// </summary>
        partial void CustomInit();

        /// <summary>
        /// Gets or sets the name of the subnet.
        /// </summary>
        [JsonProperty(PropertyName = "name")]
        public string Name { get; set; }

        /// <summary>
        /// Gets or sets the key (ID) of the subnet.
        /// </summary>
        [JsonProperty(PropertyName = "key")]
        public int? Key { get; set; }

    }
}

redpajama_set_name: RedPajamaGithub


text:
There are schools offering nurse practitioner programs in Maryland!
Click to browse online nurse practitioner programs >
Schools Offering Nurse Practitioning Programs in Maryland
Nurse Practitioner Programs in New Jersey
Nurse Practitioner Programs in Delaware
Nurse Practitioner Programs in Virginia
Nurse Practitioner Programs in Pennsylvania
Nurse Practitioner Programs in Washington DC
Nurse Practitioner Programs in West Virginia
See All Schools in Maryland
Schools in MD
Each year, approximately 0.1% of Maryland graduates receive degrees in nurse practitioning. Thus, Maryland's 6 nurse practitioner schools put out approximately 77 nurse practitioners each year.
Johns Hopkins University, which was ranked 12th nationwide in 2010, is the top-ranked school in Maryland that has a nurse practitioner program. It is located in Baltimore. In 2010, 38 students graduated from Johns Hopkins University's nurse practitioner program. Tuition at Johns Hopkins University was $40,680 per year.
Towson University, which is located in Baltimore, is the second-ranked school in Maryland that has a nurse practitioner program. It received a ranking of 28th in the country in 2010. In 2010, 15 students graduated from Towson University nurse practitioner program. Towson University charged in-state students $7,656 in tuition fees per year.
The third-ranked school in Maryland that has a nurse practitioner program is Coppin State University. Coppin State University, which was ranked 84th in the country in 2010, is located in Baltimore. In 2010, Coppin State University graduated 7 students from its nurse practitioner programs. Coppin State University charged in-state students $5,547 in tuition fees per year.
If you are hoping to attend one of Maryland's nurse practitioner schools, you can expect to pay an average tuition of $14,324 per year, though tuition can range from $40,680 per year to $5,547 per year. The highest tuition rates in 2010 at Maryland nurse practitioner schools were charged at the following schools:
Johns Hopkins University - located in Baltimore, students are charged $40,680 per year
Washington Adventist University - located in Takoma Park, students are charged $20,180 per year
University of Phoenix-Maryland Campus - located in Columbia, students are charged $11,880 per year
The lowest tuition rates at Maryland nurse practitioner schools were charged at the following schools:
Coppin State University - located in Baltimore, students are charged $5,547 per year
Towson University - located in Baltimore, students are charged $7,656 per year
A nurse practitioner degree from a Maryland school... what next?
The highest percentage of nurse practitioner graduates in Maryland pursue careers as a nurse practitioner. If you decide to work as a nurse practitioner in Maryland, you will be joining the ranks of approximately 3,710 Maryland nurse practitioners as of 2010. The Maryland counties with the largest populations of nurse practitioners are:
Frederick County - 3,300 nurse practitioners
Anne Arundel County - 230 nurse practitioners
The government projects that by 2018, the number of nurse practitioners in the state of Maryland will grow to 4,400. This would require a 2% growth in the profession.
A nurse practitioner in Maryland makes an average of $117,900 per year. But, salaries for nurse practitioners can vary. In 2010, nurse practitioners made as little as less than $40,670 per year or as much as more than $155,490 per year in Maryland. The counties in Maryland with the highest average salary for a nurse practitioner are:
Frederick County - $121,240 per year
Anne Arundel County - $84,870 per year
A nurse practitioner in the following counties in Maryland make the lowest salaries on average:
Take a look at the graphs and charts below for additional Maryland statistics regarding a career in nurse practitioning and to compare salaries with a variety of related fields such as nurse anesthetist or MSN.
Master's Degree in Nurse Practitioning in Maryland
Doctoral Degree in Nurse Practitioning in Maryland
Curious what studying Nurse Practitioner gets you?
Check out the different options and how they're looking in Maryland
Health Diagnosing and Treating Practitioners, All Other 3,710 $117,900 243.5%
Below are nurse practitioner related jobs in Maryland


text: print('hello python world')