Chapter 17 of Mystery of the Secret Band Mary Louise thought she had never seen anyone change so much in the short space of two years, as Margaret Detweiler had changed. How much older she looked, how much sadder in spite of her expensive clothes.  Like that of an animal caught in a cage. You are going to arrest me? The girl stammer directing her question to the constable. I'm doing just what Miss Gay says at the present time, replied the man. So far, I don't know that you're guilty of any crime. No, no, don't arrest Margaret, protested Mary Louise. I just can't believe that she is a member of Mrs. Ferguson's gang. Why, it's too impossible. No, it isn't impossible, said Margaret, more calmly now. Mrs. Ferguson is a special kind of criminal, who makes young girls do her stealing for her. She picks up country girls who don't know anybody in the city and trains them. Oh, it's a long story, and a sad one. Do you mean to say that you did steal Margaret? Demanded Mary Louise incredulously, for she had never believed that story of Margaret's theft at the department store. You must tell me the truth. For the sake of your grandparents, I can honestly say that I have never stolen anything in my life, replied the other girls steadfastly. Mrs. Ferguson soon found out that I was no good for that, so she made me guardian of the treasure. I felt almost as wicked, but I never stole. Thank heaven for that, exclaimed Mary Louise. But now I've lost her valuables, and she'll send me to prison, whimpered Margaret. Oh, Mary Lou, did you take them? Yes, I took them. They're at the constable's home now. And most of them belong to the guest's sixth daughter's house, in Philadelphia. But you shan't suffer, Margaret, unless you're really guilty. The young lady is very cold, remarked to the constable. Hadn't we better go back to my house, where it's warm, till your car is fixed, Miss Gay? Oh, yes, if you will let us, agreed Mary Louise enthusiastically. She could see that Margaret's teeth were chattering, and she remembered how cold she herself had been after an hour or so in that empty house. Wait until I get my other things, she said running back into the kitchen for the basket, which she had packed early that morning. I'll put them into the car and see how soon the mechanic thinks he will have it ready. She returned in a couple of minutes, and found the others already seated in the constable's sedan. Mary Louise was glad to find that the officer had put Margaret Deatwiler in front with him, not beside the tough young man with his huge guardian in the rear seat. She squeezed in next to Margaret, and the car started. The mechanic is going to drive my car to your place in about half an hour, announced Mary Louise, and then we'll start for Philadelphia. Fine! exclaimed the constable, that will give you girls a chance to get warm, and maybe have a cup of coffee. It's marvelous coffee, commented Mary Louise. It just about saved my life. Not another word was said about the crimes or the secret band. Margaret Deatwiler was introduced to Mrs. Hodge as a friend of Mary Louise's from Riverside, and the two girls spent a pleasant half hour in the constable's home, sipping their freshly made coffee and looking at the children's Christmas toys. The constable, who had taken the young thug away, returned just as Mary Louise's hired car drove up to the door. Mary Louise jumped up and reached for her coat. Wait a minute, cautioned the constable.  I just met somebody asking for you at the hotel. So don't be in too much of a rush. From the obvious twinkle in the man's eyes, Mary Louise believed that Max Miller must have driven down to Philadelphia again, missing her there, had naturally traced her to Centre Square. But at the same moment a yellow taxi stopped at the constable's gate, thereby dispelling any such illusion. Max would never ride in a taxi cab on his limited allowance. The door of the cab opened, and a tall, handsome man, stepped out, paid the driver and dismissed with the cab. It was Mary Louise's father. Flinging opened the door, the girl shouted at him in delight, so loud that Mr. Gay heard her in spite of the noise of the twarding cab. In another moment he entered the open door of the house and held Mary Louise tightly in his arms. Mary Lou! he cried in delight. Are you sure you're all right? I'm fine, she replied, ushering him into the constable's house. Merry Christmas, Daddy. The same to you, dear. He gazed at her fondly. I believe it will be now. You certainly look happy, daughter. I am, Daddy. These people have treated me royally. She turned around and introduced her father to Mrs. Hodge and the children, for he had already met the constable.  Here is Margaret, Dad Weiler, she added. You remember her, don't you? I certainly do, replied Mr. Gay, extending his hand cordially. My, but your grandparents are going to be glad to see you, Margaret! The girl blushed and looked down at the floor in embarrassment. Wisely Mr. Gay asked no questions. I have all the stolen valuables, Dad. Continued Mary Louise. Every single thing that was taken from Stoddard House, and even the money. Mr. Gay gazed at his daughter in speechless admiration. She had excelled his fondest hopes. Mary Lou, that's wonderful, he said after a moment. I have good news, too. I caught your thieves. Seven of them. They are in a Baltimore jail now. Both girls exclaimed a loud inamazement and delight. Margaret Detweiler started forward and clutched the detective's arm. It's really true, Mr. Gay? She demanded breathlessly. Mrs. Ferguson? Is she in jail, too? Locked up without any chance of getting out on bail, he said authoritatively. Oh, I'm so glad! murmured the girl thankfully. Now we'll be able to take the valuables right back to their owners at Stoddard House, Constable Hodge. And now it's Mary Louise. I'm not afraid to carry them, with Dad beside me. Mrs. Hodge brought the jewelry and the money from its hiding place, and gave it all to Detective Gay. Both he and Mary Louise tried to thank the Hodges for their help and their hospitality. Mr. Gay wanted to give the Constable some sort of recompense, but the good man refused. Only after a great deal of persuasion would he accept a $5 bill as a Christmas present for his children. Ready, Daddy? inquired Mary Louise as she slipped on her coat. Just a minute, replied her father. I want to telephone to Mrs. Hillard to let her know you are safe. She's been terribly worried, Mary Lou. And shall I tell her that we'll eat Christmas dinner with her at Stoddard House? Oh, yes. I've heard about the menu. There won't be a sweller dinner anywhere in Philadelphia than at Stoddard House. But shall we be in time? Mr.  It's only a little after eleven, he said. We ought to make it by one o'clock. As soon as the telephone call was completed, the three people got into the little car Mary Louise herself took the wheel for, as she explained, she was familiar with it by this time. Now tell me about your experiences, Mary Lou. Urged her father as soon as they were well underway. Mary Louise explained for Margaret's benefit, as well as for her father's, about deciphering the code letter and coming up to Centre Square and breaking into the empty house in search of the valuables. But she made light of the coldness and desolation of the dark house and of her own hunger. She concluded with the statement that Margaret had come that morning and let her out with a key. But how did you happen to have the key, Margaret? Demanded Mr. Gay. I will have to tell you my whole story from the beginning, answered the girl. There was a tragic note in her voice which drew out her listener's sympathy, but neither made any comment. Then you can decide what to do with me, she continued. I guess I deserved to go to prison, but when I assure you that I have never done anything wrong except under compulsion maybe you will not be so angry with me.  Mary Louise told her. Only terribly sorry. So please tell us everything. You remember that your grandparents have never heard anything from you since last Christmas, so begin your story there. All right, let me see. I was working in that department store in Philadelphia and doing pretty well. For I got commissions besides my salary on everything I sold. I started in the Chief Jewelry Department and was promoted to the expensive kind. Christmas brought me in, a lot of business, but I guess I overworked. For I got sick the week before and had to stay home and have the doctor. I'd already spent a good deal of money on presents, and when my doctor's bill was paid, I found my salary was all gone. So I went back to the store before I should. On the 23rd of December, I remember. The 23rd of December, repeated Mary Louise. That was the day Mrs. Ferguson registered at the Benjamin Franklin Hotel. How did you know Mary Lou? demanded Margaret. I went to the hotel and looked through the old register. She explained. But go on, Margaret. What happened then? I found that a ring, an expensive diamond ring, had been stolen from our department, continued the girl. They insisted that it was taken before I was away, but they couldn't prove for anything. Just the same. I know the store detective had his eye on me. Well, that very day something else disappeared, a link bracelet. This time they accused me immediately. But why? I don't know, except that I was the newest sales girl in the department, in fact, the only girl. The store detective stepped behind my counter and leaned down to the floor, and he picked that bracelet right out of my shoe. How dreadful, cried Mary Louise. Somebody had planted it there. Of course, Mrs. Ferguson had, as I later learned. But at the time I hadn't a suspicion. She was standing right near the counter, examining some rings. When she heard me accused and told to leave the store, she stepped forward, saying that she was sorry for me. She asked me whether I had any family, and I told her they were too far away for me to go to without any money. But you'll have trouble getting a job without a reference, she said. So perhaps I had better help you. That sly cat, cried Mary Louise. Margaret nodded. But I didn't know it then. I simply asked her whether she could get me a job. And she told me to come to the Benjamin Franklin Hotel that afternoon, and ask for Mrs. Ferguson. Of course I went, I had nothing else to do. She engaged me at once as her secretary. We went out to Centre Square for a few days. And I met a lot of other girls. Two daughters, two nieces, and a couple of friends. We had a good time. But I didn't do any work. For she had two servants and a chauffeur. And I felt as if I didn't earn my pay. Did she give you a salary? Asked Mary Louise. Yes, replied Margaret, for the first couple of weeks. But I had to send it to my landlady in Philadelphia. After that Mrs. Ferguson bought my clothes and paid my hotel bills. But she never gave me any cash. So you couldn't get away, observed Mr. Gay. Exactly. Gradually I began to suspect that there was something crooked about this bunch. And then one day I found the diamond ring which had been stolen from the store, among Mrs. Ferguson's stuff at Centre Square. What did you do? Demanded Mary Louise. I showed it to her and said I was going to take it right back to the store. And she stood there and laughed at me. She said it would only prove my own guilt. The next day we all went to Washington and stayed in different hotels. Mrs. Ferguson kept me with her, but I soon saw through her tricks. Her girls were all skilled hotel thieves. She tried to teach me the business as she called it, but I refused to learn. So she made me take charge of the stuff they stole. The girls would bring their loot to her and she'd send me with it to Centre Square. Every once in a while she would dispose of it all to a crooked dealer who asked no questions. Were you out at Centre Square last Sunday, Margaret? Interrupted Mary Louise. Yes, Mrs. Ferguson and I both went. We had intended to get the place ready to spend Christmas there. But for some reason Mrs. Ferguson got scared. She said that Mary Green talked too much, and she thought we ought to clear out. She made plans to dispose of everything in Baltimore, and then we were all going to sail to Bermuda. But why did you ask that, Mary Louise? Because I was in that car that drove up to the house then. I saw you and then Mrs. Ferguson. I wouldn't have thought of it being you, only Mary Green admitted that she knew you. That made me suspicious. You disappeared pretty quickly. Rather, laughed Mary Louise. And she told the story of being hit over the head by a rock and of catching the young man and having him arrested that very morning. That was clever! Approved her father. Who was he, Margaret? A neighbourhood bum that Mrs. Ferguson employs to watch the place and keep the people away, replied the girl. But I'm afraid I interrupted you, Margaret. Apologised Mary Louise. Please go on with your story. There isn't much left to tell. I was too far away from home to run away, without any money, and I hadn't a single friend I could go to. All the store people thought it was a thief, so I knew there was no use asking their help. I just kept on, from day to day, not knowing how it would ever end, and never expecting to see my grandparents or my riverside friends again. Oh, you can't imagine how unhappy I have been! She stopped talking, for emotion had overcome her. Tears were rolling down her cheeks. Mary Louise laid her hand over Margaret's reassuringly. It's all right now, isn't it, Daddy? She said, we'll take you home to your grandparents. But I can't go back to them, protested the other girl. How can I tell them what has happened? They'd be disgraced for life. You can tell them you have been working for a queer woman who wouldn't allow you to write home, said Mr. Gay. A woman whose mind was affected, for that is the truth. There is no doubt that Mrs. Ferguson is the victim of a diseased mind. Wouldn't you ever tell on me? Question, Margaret. No, of course not.  And now try to be happy. I think I can find you a job in Herman's hardware store, right in the riverside. And you can live with your grandparents, they need you. It seems almost too good to be true, breathed the grateful girl. Mary Louise turned to her father. Now for your story, Dad. She begged about capturing the thieves. I think that had better be kept till dinner time, replied Mr. Gay. This traffic we're approaching will require all your attention, Mary Lou. And besides, Mrs. Hillard will want to hear it, too. End of Chapter 17 Chapter 18 of Mystery of the Secret Band by Edith Lavelle This LibriVox recording is in the public domain. Recording by April 6090, California, United States of America. Conclusion Mary Louise brought the car to a stop at Stoddard House at a quarter to one. Carrying the money and the jewels in her father's briefcase and the other articles in the basket. She and Margaret went into the hotel to get ready for dinner while Mr. Gay returned the hired car to the garage. I'll notify the police that you're found, Mary Lou, he said.  I think it will be best if she goes over to your grandparents Margaret and tells them about you herself. They haven't a telephone and I don't like to frighten elderly people with telegrams. Both girls nodded their approval to these suggestions and hurried into the hotel. Mrs. Hillard was waiting for Mary Louise with open arms. She loved the young detective with like a daughter. Now run along, girls, and get ready for dinner. She said, finally, we're going to have one big table instead of all the little ones in the dining room with a tree in the center and place cards just like a jolly family party. That's swell, exclaimed Mary Louise. It'll be real Christmas after all. And thank you so much for the lovely handkerchiefs, dear, added the manager. It was sweet of you to think of me. That reminds me, you haven't had your presents yet. Put them at my place at the table, suggested Mary Louise, and I'll have presents for some of the guests, she added with a significant glance at the briefcase and basket. When the girls returned to the first floor after washing their faces and powdering their noses, they found Mr. Gay waiting for them. For a moment he did not see them. So intent was he in the newspaper he was reading. Want to see the gang's picture? He asked when Mary Louise came to his side. Oh yes, please! In spite of the fact that it was Christmas day, a large photograph of Mrs. Ferguson and her six accomplices occupied much of the front page of this Philadelphia paper. In an inset above the picture of the crooks was Mary Louise's smiling face. Daddy, cried the girl in amazement, are you responsible for this? I am, replied her father proudly. I want everybody to know that the credit belongs to you, daughter. Other guests who had not yet read their newspapers crowded about Mr. Gay eager for the exciting news. They all remembered Pauline Brooks and Mary Green. Several of them identified the two transients who had stolen the other things from Stoddard House. A loud gong sounded from the dining room, and Mrs. Hillard threw open the doors. The room was beautifully decorated with greens and holly, a long table stretched out before them, covered with a lovely lace cloth and bearing a small Christmas tree as its centerpiece. Bright red ribbons had been stretched from the tree to each guest's place, adding brilliancy to the spectacle. Hello, Mary Louise! Said a voice behind the young detective, and turning around, Mary Louise saw Mrs. Weinberger behind her. Merry Christmas, Mrs. Weinberger, she replied. It's nice to see you back here. I've come back to stay, announced the older woman. I got lonely at the Bellevue, and Mrs. McGregor is here, too, for Christmas dinner. It was a happy group who finally found their places around the beautiful table and sat down. Mrs. Hillard was at one end, and Miss Stoddard was honored with the seat at the other end. Mr. Gay was the only man present. But he did not seem in the least embarrassed.  Even in his haste, Mr. Gay had remembered the lonely girl. The guests ate their oyster cocktails and their mushroom soup before any formal announcement concerning the valuables was made. Then Mrs. Hillard rose from her chair. As you all know from the papers, our criminals have been caught by Mary Louise Gay and her father, and are now in prison. But even better news than that is coming. I'll introduce Mr. Gay, whom some of you know already, and he'll tell you more about it. Everybody clapped as the famous detective stood up. I'm not going to make a speech, he said, and keep you waiting for the turkey. We're all looking forward to. I just thought that maybe some of you would enjoy this wonderful dinner even more if you knew that you were going to get everything back again which was stolen. My daughter found all the valuables and the money this morning in Mrs. Ferguson's house at Centre Square, and she will now return them to their rightful owners. As the newspaper had not mentioned anything about the stolen goods, the guests were not prepared for this pleasant surprise. A loud burst of applause greeted Mary Louise as she smilingly rose to her feet and opened the briefcase and drew out the basket from under the table where she had hid in it. I'll begin at the beginning, she said, with the vase and the silverware belonging to Stoddard House. She carried these articles to Mrs. Hillard, amid appreciative hand clapping. Next, Miss Granger's is picture and her fifty dollars. She continued. Tears actually came to the artist's eyes as she took the painting from Mary Louise's hands. You keep the fifty dollars, Miss Gay, she said. My picture is what I care for most. No, Miss Granger, no, thank you. Replied the girl solemnly. I am being paid a salary for my work by Mrs. Hillard, but I can't accept rewards for doing my duty. She picked up the watches next, Mrs. Weinberger's and Mrs. Hillard's. The Walder girls would get theirs when they returned from their holidays. And last of all, Mrs. McGregor's diamond earrings and her five hundred dollars, she concluded, restoring the jewelry and the bills to the delighted woman. I believe that is all. For I am wearing my own wrist watch, and I have my purse with its five dollars contents. Loud cheering accompanied the applause which followed. When it had at last quieted down, both Mrs. Weinberger and Mrs. McGregor tried in vain to give Mary Louise a reward, but she remained firm in her refusal. Then the turkeys were brought to the dining room, and everything else was temporarily forgotten in the enjoyment of Christmas dinner. When it was all over, Mr. Gay told Mary Louise to pack her clothing and her presents while he returned the remaining valuables to the Ritz and to the police. For I hope we can make the 330 train, he explained. But with that change at the junction, we'd have to wait all night. Shouldn't we, Daddy? inquired Mary Louise. Anxious as she was to get back to Riverside, she had no desire to spend the night in a cheerless railway station. No, replied her father. Because there's going to be a surprise waiting for you at the junction. Max and Norman, guessed Mary Louise instantly. You mean that they'll drive down for us? Mr. Gay nodded. That isn't all, he said. Mary Louise did not guess the rest of the answer until the train pulled into the junction, shortly after eight o'clock that night. Then a war-woop that could come from no one else but her small brother greeted her ears, and she knew that her mother must be there too. Yes, and there was her chum, Jane Patterson, grinning at her from the boys' car, and her little dog, Silky. In another minute, Mary Louise was clasping her arms around Mrs. Gay, and hugging Freckles and Jane and Silky all at once. Max at her side, had to be content with pressing her arm affectionately. Questions, Christmas greetings, words of joy, and congratulation poured so fast upon Mary Louise's ears that she could scarcely understand them. You're home to stay, darling? This was from her mother. You'll go to the senior prom with me? Demanded Max. You're the most famous girl detective in the world! shouted Norman Wilder. You were a lemon to duck my party, but I'll give another one just in your honor. Promised to Jane. Did you get your salary, your twenty-five bucks? asked Freckles. Mary Louise nodded, smiling to everything. Then she got into Max's car beside him, with Jane and Norman in the rumble seat. Mr. Gay took the wheel of his sedan, with his wife beside him, Margaret Detweiler, who was quietly watching everything sat behind with Freckles. The drivers of the two cars did not stop for any food on the way. They sped along as fast as they dared towards Riverside. Old Mr. and Mrs. Detweiler were waiting up for their precious granddaughter, their lost Margaret. A little before midnight the cars pulled up in front of the old couple's home, and everybody in the party went inside for a moment. The greeting between Margaret and her grandparents was touching to see. Even Norman Wilder, who prided himself on being hard-boiled, admitted afterwards that the tears came to his eyes. Mrs. Gay discreetly drew her own party away, back to her home, where a feast was waiting for the travelers. This, Mary Louise felt, was her real Christmas celebration, with her family and with her three dearest friends. Now she could tell her story and listen to the praises which meant so much to her. But the best part of all, she concluded, is that I'm a real professional detective at last. End of Conclusion End of Mystery of the Secret Band by Edith Lavelle


So Morgan, you spent 11 seasons with one team and then you move on to a different team. How hard is it to make a change, especially when you have a job that's so regimented, so routine, and it's the same over and over and over and over again? Yeah, I mean, so I was in Baltimore for 11 years, 9 of which I spent with the same two people, two kickers and funner. And yeah, we did. We had our routine every single year, spring, training camp, all the way through the season, everything. It was definitely a change, but I've enjoyed getting to find a new routine with Brett and with Randy. Did you ever take a minute to think after you were informed that you weren't going to be coming back with Baltimore to be a Raven again? You know, I've won a Super Bowl. I've gone to the Pro Bowl. I've been named all pro. Maybe this is it. Like, maybe I'm done. Did that thought ever occur to you? No, it really never did. I just love what I'm doing, and I knew that the Tennessee spot might be open. I had maybe put in a word with Brett right after it happened, and I knew that was a possibility. Growing up a Titans fan, there's no way I could have thought about that. Who was more excited to come to Tennessee? You or your family? Oh gosh, that's a tough one. Like I said, I'd grown up a Tennessee Titans fan. You know, I came to a game with five of my other high school buddies and we did the Titans across our chest. It was like the middle of December, so I was a die-hard fan back in the day, but my parents have come to every game. I'm two and a half hours away from everybody in Memphis, and going to school in Knoxville, you know, I'm so close to everybody that I spent so much time with, so I don't know. That's a toss up. It's got to be good to be out of kind of the Northeast and that sports world and back in SEC country, back in Val Nation. I mean, there's got to be a lot of things that just feel good about being home. I see a heck of a lot more power tees around town than I did up in Baltimore.  But yeah, it definitely feels like home. Tell me a little bit about working with Craig Ockerman. What is his style like? How has he been able to help you maybe become a better long snapper? Absolutely. That's another attention to detail thing. He doesn't let me take a playoff, you know, today at practice. He offered some coaching for how I wanted to, how I should have played the play. And he brings a lot of energy, a lot of excitement to the meeting room, a lot of excitement to practice, makes it keeps it fun, keeps it light. It's a great atmosphere to be in, to get better at each day.  Surprise would probably be a good word for it, to be honest with you. I remember an older snapper commenting on me as a young snapper and saying that I could play 10 years in the league. And to me, that just, that seemed like an eternity. And so I was really excited about the thought of being able to play that long.  So I still feel like I can play several more years in this league and I'm excited to see what the future holds.


So today I have just a little bitty video for you. It's not quite as short But it could probably be boiled down into short But I want to ramble just for a little bit about some nostalgic things that I've been thinking about So as I talked about in a recent video, I have installed Arch Linux a lot lately I've done that because I'm an idiot and you know things just you know didn't work out the way that I wanted them to and all This stuff I don't need to go back into it But if you want to watch the woes of me having to deal with some of the problems that I've had over the course of The last few weeks, you can go watch that video But the idea is that I've installed Arch Linux a lot and one of the things that was a really big deal Even like a year ago, maybe even two years ago, right? It was Arch Linux install videos I have one, you know every Linux youtuber out there has done at least one Arch Linux install video Like it was one of the first things It was my first one of my first exposures to Luke Smith was his Arch Linux install video Well, I think that may be the first video of his that I've ever actually watched So my exposure to the Linux YouTubing community was actually through Arch Linux install videos and now they're gone, right? There is no purpose right now if anyone doing an Arch Linux install video because it's so easy to install Arch Linux these days All you got to do is run Arch install and it does it for you. It's not even hard to set up a An encrypted version of Butterfest on Arch Linux. It just does it for you and that's kind of nuts right it's also kind of sad because I'm one of those nerds that would sit in front of my computer when I had You know a spare time and watch someone else install Arch Linux even though I personally I'd already known how to install Arch Linux the hard way You know the original vanilla way, you know, I would sit there and watch them because I found it. It was almost like ASMR, right? It's just something that was very Low brow Entertainment if you you know don't take that off, you know offensively, but it's just you know It's just something that I could have on in the background and just watch and it would be fun You know nerdy entertainment if you will and that kind of stuff at least in terms of Arch Linux installed videos are kind of gone Just there's no reason for it anymore because Arch install exists So that's just one of the things that I wanted to talk about But I mean it doesn't mean that those kind of type of videos are gone So like there's a lot of just of youtubers out there They'll do Debian installed videos for whatever reason because apparently Debian's now harder to install than Arch Linux is I don't actually know. I don't think that that's true But they're obviously easier ways of installing Debian But if you watch some of these youtubers, they install Debian basically like we used to install Arch which is very entertaining. I watched I'm sorry. I don't remember this guy's name I'll try to leave a link to it in the video description by watched a Linux youtuber just the other day install fedora now That doesn't sound exciting at all But he installed it like you would install Arch like he installed it completely manually from the terminal And not just like an encroaches install or anything like that was 100% From partition to installing the packages through a package manager through the terminal It was really really cool took about an hour It was it completely tickled my fancy because it's kind of stuff that I really really enjoy Watching someone do something that is a little bit difficult, you know, it's just kind of fun You know watching them install something that has that idea behind it that it is Challenging and there maybe you might learn something is kind of cool And you don't get that very often with like gen 2 videos like yeah There are gen 2 install videos out there, but when it was the heyday of Arch Linux install videos There was one like like a mono from Linux made simple EF Linux comm he used to do a arch install video every single month Sometimes too, right? You'd show you how to do butterfess installs of Arch Linux encrypted installs of Arch Linux Encrypted butterfess installs of Arch Linux, you know ZFS installs of Arch Linux it was every single month how to install Arch Linux It was the same video basically every single month, but it was entertaining for me because I'm a nerd and I like that kind of thing right and The fact that those kind of videos just aren't really here anymore is a little bit disappointing Obviously it doesn't stop some Linux youtubers from still making the the Arch install videos showing people how to use Arch install and stuff And I suppose that there's a place for that But they're not as entertaining as they were when you know you had to do it the more manual way now Basically what this whole video boils down to is that back in my day? Arch Linux was much harder where you're installing if you did it you had a badge of honor and it was all this fantastic stuff And you could say I used Arch Linux by the way And it actually would mean something these days when people say I use Arch Linux by the way I'm like so so you know how to use Arch install congratulations, you know golf clap, you know, it's fantastic You learned how to use a script. It's just Bully for you. It's fantastic, you know, so it's not it's just not the same now. It doesn't mean that it's bad or worse I'm I myself used Arch install three times this in the last month or so, you know to install Arch Linux You know, it's just because it is super super easy But it does take something away from the experience and the ability to you know show that you've actually accomplished something worthwhile It's just another Linux distribution that you can install via, you know a script or a menu or something like that So yeah, that's it for me on this video a little bit of a ramble this video was Absolutely completely effing pointless by the way, if you made it this far Seriously gold star for you. I wouldn't have made it this far probably so if there's literally anybody still watching this video Leave a comment the comment section below telling me which your favorite type of Linux YouTube video is I'd love to hear from you You can follow me on mastodon or Odyssey those links to be in the video description You can support me on patreon patreon.com slash linux cast links for libera pay and YouTube be be in the video description as Down below while I completely messed up my words there Thanks everybody does support me on patreon and YouTube you guys are all absolutely Amazing without you the channels would not be anywhere near where it is right now So thank you very very much for your support. I truly do appreciate it seriously guys Mind blown every time I think about how many people support me. So thank you so much for your support Thanks everybody for watching. I'll see you next time


The paper demonstrates how teaching platforms at educational institutions can use cloud platforms to scale services and gain access to compute instances with accelerators such as GPUs. The authors introduce a new framework called Cork which allows users to dynamically orchestrate, authenticate, configure and access interactive notebooks in the Oracle Cloud Infrastructure OCI. Additionally, they propose a grid of cloud system that would allow for the exchange of access computational resources between different institutions. This article was authored by Rasmus Monk, David Marchand and Brian Vinter.


This one, this one in the morning. Azatunim 7 by the way. Uyupianesh dati upuwa gani gani. Anyway, 254 Facebook, 225 Twitter, 254 underscore channel on the ground. It is hashtag social Friday. And it's not just social Friday. It's a very, very good Friday. And not just that. Right next to Mr. Good Time. Hi Mr. Good Time. Hi. How are you? Niko poa? Niko poa. Bara nangoja ala? Niko poa. Niko nangoja accent ya kizungu. Merodi 2 default settings. Tuk pata afi kumchanda? Type RAJYZ. Rwaji is the digital pataafu. Ting ting ting ting. If you are just joining us. Nani tunapiana vitu. We've already given two credits. Credits? Pluralia. Eh eh eh. Kido goto ni choo me mjuenin me toka afi. Anyway, tunapiana creditin bili. And that is my accent. So clearly English. Sii kusite nawaku na vitu nani palu. So please do interacting. Hasnit let the neybeine Nyendo For me they b Initama store then Then come through in Leona Last Friday tule kuwata na scare w switching naNo today wana tula jasho on the own at our bhe horse soбы wa wana kumaten te Jimin today Today na Unfuza Okay, muna itua Elias Joka Muna penda kusmaila he? Thank you It's my weakness for you Ah, sorry Oh, muna itua Elias Joka Ya, this is Snickers Ultimate Dance Crew From Thika In Jujja Thika Road, that is Jujja maker? Jujja maker Hey, hey Ya Muna gopakuendelea, kupakapua faninini We are students Moja ako Okay Mami personally, niko nibz I'm doing journalism Wala? Ya What ya? Ya, I'm in first year First year I'm in Tazin Mama, you can't do that That's how tabaliza school got it So, what was your high school last year? Ah, I was in 2017 I've just been doing a distance thing Ni ka mo nirodi shule Next Hi, what's your name? Hi, Bala Hi Ah, kumeni itua ba mika tmajwa Siya ni sumaona La julikala Oh, naskiya kuhag Kimalizak toa, ya road back Nimesh out And the latest Mi na itua prinsken Social media prinsken 254 All platforms Ya, sii ni Snickers Ultimate Dance Crew Ya, sii ndotunatesa Dikayote Ba na ya A lafu unadu? Mi na fanya IT Wala ya? Ya, sumu kuna akili, sii kuru ka rupa tu? Akili utuangu I'm laughing at you Uga pa je aizinusha maliza shule sa uko into IT out? Mi ko IT, but one year to go Oh, look at you Dance na shule wa zibishana Azi zibishana Wala Talens na mazoma Ni kutusumbua tu wa mi na kutusumbua Haa, mwanzako apu hi Hi Wei, ebu fanya fanya iwi ni wumbia mani rangani Wana kwita na ni So I go by the name Evi Dancer 244 Evi underscore Dancer 244 You can find me on Instagram, TikTok Ya, YouTube Ni kukoka mani kukunya wa styanana I kusumbua wa styanana tu Sisa na kido gutu Kido gutu Uwa styanamuna sumoka IT out Hei, wei, alright Why sneakers? Ka naza kuliza? Kiki maliza ya? Ok, itu liyanza This group liyanza high school Wei baki in high school tu kotuna sneakers mo fanki Ya, she say whaten tu luqwa Different school but tu luqwa tu na patana Tu na sneakers tu renda mo fanki Tu me sneakers kumingi That's why ze na sneakers tu luqwa jagia Because Ni ni ni uwa na niya I don't see junk Asi moda piwa na tibanga Ok, so I laugh Tu angaliya ni na tibingi ni Ni li kuwadi kuliza Wusha ni sneakers tu leu na ka I don't believe it I don't believe it Allah Spoilebaz, God one Wei, alright, so you were a good boy So li pato api bad manals tu leu Mi kuwana bad manals I don't know The best Asi kuwana kelele ibi? Tu me ni salamu huwaza Ok, na tagaku sa ni miya My family, my mom, my dad Wherever my aunt na juwana watch And piya, the sentans family Sentans preparatory paleroi And my kids were preparatory I love you and see you next week Ok, I'm a drama teacher In Roy Prick Sentans Preparatory Roy Tu nafanya bi tu mingimi hindi? Ya Ok, mi na tagaku sa ni miya My family first of all Family comes first Family umewa amari No, no, no, no Uramazakha Uramazakha Uramazakha Uramazakha Uramazakha Uramazakha Uramazakha So my family, my dad, my mom My brothers Big up sana kukitunin Mufans weitu big up, kilam se By the way Tu kuna workshops I have a workshop in Nyeri Dance with Prince Ken My friend apia kuna workshop Pata juwana kelele Dance with Prince Ken Masihate Nyeri iko when? It's on Sunday Every Sunday Sangapi? From 2 to 5 pm Nyeri wapi? Iko nyeri Planet gym Opposite shell So first of all Asanti Plat from Konza So mam Mam So mam Mam Mam Mam Mam Mam Mam Mam So Mufans dika dikayote Dikaote actually Chuchia polakini next time So Trokuwanana classes Every Sunday It's been trending by the way Every Sunday at the coconut grill From 2 to 5 pm So mneza pulo pale So mam Mtafraya Mtafraya O kuna workshop? Mimi ni teacher Mi yama teacher Kamu nata kakuni If you have a kid mu yajoku dance Tuna pata na pale verona hote Luko ju Ya and we just do our thing From what age like this Ni anza kutengeneza saye? From Adi Kenye kakoku atumbu Ui akuna jokes Ui unikama akuna jokes Mpena sala mozenu Rhaji zaki na pale Facebook Ni yashia kwanzezo witu ni ju ju ju ju ju ju Tuhi ni kama ku na mounili Kwamen Thanks We appreciate you Alright Tuki na pale Facebook I try to perform Facebook We have a fantastic content today. This is the sneaker's dance kawo ehe. Master Siu so meto. Iwa munguwa. Badi manas. Iwa munguwa. Iwa munguwa. Iwa munguwa. Iwa munguwa. Iwa munguwa. Iwa munguwa. Iwa munguwa. Iwa munguwa. James Husakak manas. Ary stations. Iwa munguwa. Wanda for you, human. Happy birthday. Johnny English. Okay, but na penanga imovi. But Johnny English is spanyeni hakileo. Senangwe ninga. Nime kucheki palenana ni. Kalenka. Dark Cardinalis is tuning from SEI alifas 40 days. Rasbash. Sheer. Uerre. I'm watching live at 40 Jesus Busei. Hey, Antolin Kama. Look for two. It dictates that Jesus first aid for 40 days. Matthew for two. It dictates that Jesus first aid for days and fortnight. Antolin tune from Nyeriwewe umesoma. Nime kuna. Oficial Tobi says namasai ptah piya advance hevo. Nitu miye kaki. Baire masai ako na madou. Ako na madou. Atok tu miya to say. Hashtag so shofare. Sneakers, can I appreciate you one more time? Thank you so very much for coming. Namrode, sawa. Atarude. Ani lekewa na trajona kusuna siya ngeye, bedafontana nga-mufsinginna na fanyaneza umia. Josana miiumi am 거는o apu tdihika. Nona venye, ee, bumutambu ena, li kwa mambu bat? Nivi liya tu pesa di sabu neyaro, kwa ona, ee? Chambi piya Ini pesa, na kwa piya pesa di o sabu neyaro, ee? Afiwa na suta kaziakeni kwa kutu dansisha Pati ee piya li kwa dance at one time Hadia li kwa mi, kwa anda? Sorry, but no kweni, kido goto Pesa di poa? Kati nae Usika jae! We have, that's another one to na pianavitu guys And we will be doing this periodically So there is another one Tike teke na nii kabila motu wajiaze It's a very good day to watch why in the morning It's a very very good day to watch why in the morning All right, hashtag is social friday Kuna wa tuwa pa nomi wa dashkasi imu I want to appreciate sneakers one more time guys Na ihopu me shkeyo kredits na nii Hashtag social friday Aya, this is for sneakers, okay? Ebu make the face Misi ezi kwa na piga pa kele You're amazing Sawa, tuki ndeleya Rajasthosko But on the movie


Cultural studies is a field of theoretically, politically, and empirically engaged cultural analysis that concentrates upon the political dynamics of contemporary culture, its historical foundations, defining traits, conflicts, and contingencies. And cultural studies researchers generally investigate how cultural practices relate to wider systems of power associated with or operating through social phenomena, such as ideology, class structures, national formations, ethnicity, sexual orientation, gender, and generation. Cultural studies views culture as not as fixed, bounded, stable, and discrete entities, but rather as constantly interacting and changing sets of practices and processes.To the field of cultural studies encompasses a range of theoretical and methodological perspectives and practices. Although distinct from the discipline of cultural anthropology and the interdisciplinary field of ethnic studies, cultural studies draws upon and has contributed to each of these fields. Cultural studies was initially developed by British academics in the late 1950s, 1960s, and 1970s, and has been subsequently taken up and transformed by scholars from many different disciplines around the world. Cultural studies is avowedly and even radically interdisciplinary and can sometimes be seen as anti-disciplinary. A key concern for cultural studies practitioners is the examination of the forces within and through which socially organized people conduct and participate in the construction of their everyday lives. As a result, cultural studies as a field of research is not concerned with the linguistically uncategorized experiences of individuals. Or, in a more radical approach, holds that individual experiences do not exist, being always the result of a particular social-political context. Cultural studies combines a variety of politically engaged critical approaches drawn including semiotics, Marxism, feminist theory, ethnography, critical race theory, post-structuralism, post-colonialism, social theory, political theory, history, philosophy, literary theory, media theory, film slash video studies, communication studies, political economy, translation studies, museum studies and art history slash criticism to study cultural phenomena in various societies and historical periods. Cultural studies seeks to understand how meaning is generated, disseminated, contested, bound up with systems of power and control, and produced from the social, political and economic spheres within a particular social formation or conjuncture. Important theories of cultural hegemony and agency have both influenced and been developed by the cultural studies movement, as have many recent major communication theories and agendas, such as those that attempt to explain and analyze the cultural forces related to processes of globalization. During the rise of neoliberalism in Britain and the US, cultural studies both became a global movement, and attracted the attention of many conservative opponents both within and beyond universities for a variety of reasons. Some left-wing critics associated particularly with Marxist forms of political economy also attacked cultural studies for allegedly overstating the importance of cultural phenomena. While cultural studies continues to have its detractors, the field has become the kind of a worldwide movement that is to this day associated with a raft of scholarly associations and programs, annual international conferences, publications and students and practitioners from Taiwan to Amsterdam and from Bangalore to Santa Cruz.56. Somewhat distinct approaches to cultural studies have emerged in different national and regional contexts such as the United States, Canada, Australia, New Zealand, Latin America, Asia, Africa and Italy.


We're trying not to impose things for people. Yeah, for the way, two restaurants are very easy to jump on the bus and maybe go to Barcala. For those who don't know where the restaurant is, it's immediately after Barcala. So you leave the bus on Barcala, move a little bit towards town and this is the first building on the right, if you move towards town. So this is really... Rammer. Yes, but not everyone knows that we went there after that. Okay, the practical thing is how to get back after the restaurant. And for this, there is a principle that even later the bus goes to airport and stops in Barcala and then stops in close to ICTP, but other options are either walking, if there will be no rain or basically make a group of foreign buyers and then ask for taxi, that's the national ability. So, but hopefully there will be no rain when we go back. Yeah, I think that midnight the sea bath actually goes all the way to Guinea, so the other side. We, maybe it's it, but it's not on a schedule. Yeah, it's not on a schedule. I mean, we can't go on the six o'clock midnight from the central station to Barcala. Only was, maybe it was... Yeah, it was a part of the midnight from central station to Barcala to Guinea. Okay, guys, it's... There are many options. There are many options. Yeah, so, yeah. Yeah, let's do it. Okay. Hello, everyone. We're starting our poster presentation session. My request to poster presenters to be precise on time and we spend one minute discussing your poster. And that should be enough to be able to convey the message. So I'm going to invite speakers according to the list. Please be prepared to share your screen right away. So we are starting with Mahdi Mashkuri. Please share your screen. Hello. Can you hear me? Yes. Good. So I share the screen. I hope you can see... Great. Let's go ahead. Okay. Thank you. So I'm Mahdi and I want to show you this work. So this is basically based on a proposal from Jean Kane and Mellor where they considered a hip structure of an iron-based superconductor and a strongly spin-orbit couple drushpa layer, which has, like, in the case of an iron-based superconductor. So this is basically based on a proposal from Jean Kane and Mellor where they considered an iron-based superconductor and a strongly spin-orbit couple drushpa layer, which has, like, interestingly three different phases. Red is the topological and the blue is the trivial, which is separated by this nodal phase. And our message is that when we evaluate the density of the state, we see, if you start at the red curve, which is a representative topological point, we see that the red curve becomes gapless while the trivial phase in blue is robust. And the green is for conventional space superconductor. We also looked at the phase diagram and we see that generally the phase diagram has the expansion of the gapless phase, mostly at the expense of topological phase. In contrast, the blue region, which is the trivial phase, is quite robust. I think we can explain this by looking at the disorder in single impurity and dimers, which we looked previously in this PRB. I would be very happy if there was any questions or comments to be reached by this email. Thank you. Thank you. Thanks. Thank you very much. Next speaker, Rashid Massour. Rashid Massour. Rashid, can you hear us? You started screen sharing, but we don't see anything. We don't see anything on the screen. Okay, since we're having technical difficulties, maybe we can switch to the next person, and then come back to Rashid if the issue is resolved. Roman Mukachev, please go ahead and share your screen. Is it okay? Yes. Yes, please. Good afternoon, dear colleagues. My name is Roman Mukachev, and I want to introduce you to our work on the study of magnetic properties of an metallic compound. We have already performed several calculations with the compounds of this type. Would you like to share your screen? I think I'm sharing. Maybe I will try another one. Is it better? I don't see your screen. That's strange. You can click on share screen button. I'm sharing it right now. We just see your logo. Okay, maybe. This was just a video. I have some software problems. Okay, yeah, maybe you can discuss it in words without sharing your screen. Maybe that's better. Nothing? No, we still cannot see your screen. Sorry, I don't know. I really don't know what's the problem. Okay, look, unfortunately we are on a tough schedule, so maybe you can say just a few words about, and then those will be in the queue. Yep. In this work, we are studying manganese and ruthenium compounds, intermetallic compounds with manganese and ruthenium, and the compound with ruthenium showed different values of the density of electronic states at the Fermi level from the previous study compounds. So ruthenium ions remains practically non-magnetic. And as a show of my poster, that's like changing densities of electronic states and other properties. And doping with ruthenium ion leads to changes also the lattice parameter electronic structure and properties of compounds. That makes this system interesting for further study. So maybe I can post my poster in the chat or somewhere else. Yes, please. Thank you very much, Roman. Next speaker, Shantanu Mukherjee. Please unmute yourself, Shantanu. Can you hear me? Yes. I can hear you. Time is running. Yeah, so please. Yeah, so I am Shantanu Mukherjee. And the title of my presentation is electronic vortex interaction and fermion pairing. So in this work, we have chosen a Boson-Fermian mixture model which closely resembles the model proposed by Friedberg and Lee in 1989 as a model for high-tech superconductors. So this is the model by Friedberg and Lee. And we consider here bortices in the scalar matter. And as we know that bortices construct magnetic field in the airport and also fermions have access source of magnetic field. Therefore, in such a model, an interaction between electrons and bortices is inevitable. So in our work, what we want to do is to derive an exact form of this interaction and dualization may lead to an answer. So following the Friedberg model, we take an relativistic model like this where we have neglected the direct coupling between bosons and fermions and dualize this model. And therefore, we get this dual model where the two-form gauge field couples both to this fermionic current and also the wall sheet of the dual string which represents bortices. Therefore, bortices and this electrons are interacting among each other by exchange of the two-form gauge field. And this is the electron-bottice interaction we wanted to find out. And one can show that this electron-bottice interaction can give rise to electron-bottice attachment. And this is represented by these two equations. So if we take two electrons and immerse them in a background superconducting medium, then two flux tubes can be connected to these two electrons. And therefore, they will be connected to each other and form a stable pair. So therefore, we see that electron-bottice interaction emerges out of dualizing a boson fermion mixture model and for nearly static electrons, bortices attach to electrons and lead to formation of pairs. And also, we have recently shown that these bortices attach particles over fractional statistics when the system is reduced to a 2 plus 1 dimensional manifold. So, thank you. And one, if someone is interested, one can contact me in this email ID. Thank you. Thank you. Next speaker. Fahim Sayed, Fahim Naqvi. Fahim Sayed Naqvi. Go ahead, please. Not here. Not here. Yeah, next one. Next one. Moved by Rahman. Yes. Hello. Yes, we can hear you. Please share your screen. Please go ahead. Moved by Rahman. Please speak up. We can hardly hear you. Calculate the lexation using the Kaldis formulation. There are many critical methods apart from simulation. Green function cubometer and Boltzmann transport hydrodynamics. And to explain the electron transport property of this sort of material. The simplest one of the Boltzmann transport hydrodynamics, which treat the scattering of leptons within thermogolded roots, but they're suitable only for the pure system in thermo little bit. And for scattering from the limited for other types of disordered material as well established feature in the most simple is that the disordered scattering causes quantum interference amongst themselves for passing power. A complication arises in the calculation of transport properties. Due to the modification coming out the quantum connection disordered system. The critical method that is well suitable for incorporate this interference effect through the Kaldis formula, which is based on the non-equilibrium green function method that we use. And from this we calculate the first collision integral and put this value in equation one. And from this question two, we obtain equation three from equation three from some approximation we obtain in disordered limit. Relaxation rate is a linear dependent on temperature. And for the pure limit is often the square part of the system and using this relaxation rate. We obtain that is from this. Your approaching. Yeah. And this is my numerical and integral from which we can clearly see. When we in increasing the disorder, the system, the resistivity is enhanced. And this, this is our calculation. And for the query we can contact with this email. Okay, thank you very much. Thank you. Thank you. Everyone hear me from those who are going to give up for that. You have one minute to make a presentation. Don't try to give introduction. One minute. About those ideas that other people should be able to contact you if they're interested. So try to make a point point from the beginning. Okay, next speaker Francis Miriam Orlich. Hello. Just give me a second to share my screen. Can you see that all right. Yes. Okay. Okay. So hi, I'm Miriam, and I'm going to be telling you about the Kagome lead bladders, which is a Kagome lettuce, but with an extra site added at the midpoint of each font in the same way the lead bladders is constructed from the square lettuce. It's a model organic frameworks, and it's a simple model of the recently discovered level organic superconductors. We found using a tight binding model that this model has five flat bands. And our aim was to understand why the present and to see whether these bands would survive in a real material that breaks the assumptions of this simple model. So the flat bands arise from the apology of the lettuce through the construction of localized Eigen states which have the energy of the flat bands. And it slips due to destructive interference. Now this picture still holds even after adding the metallic onsite energy and the metal metal hopping shown in figure one. However, when the ligand hopings added you can't make this argument anymore, and the new Lucy's at flatness at the bands. However, when this happens, our bands at half fillings are still flutter and more isolated than those are twisted by layer graphing for a vast array of hopping strengths. Now you can see this in figure four where I've plotted the band gaps on either side of the central bands, normally seven bandwidths. And as you can see the band gap bandwidth ratio for the Kagome lead type binding model is lighter than that of twisted by layer graphing for a similar model for a significantly broader range of hopings than is likely to be seen in a real material. So because of this the Kagome lead bladders is likely to display funds strongly correlated behavior such superconductivity, leading us to a whole new family of unexplored materials. Thank you very much. Thank you. Thank you very much. Thank you. Next speaker. Omid Reza, a ranch bar 90. Omid Reza, a ranch bar 90. Next speaker. Divya, a robot. Divya robot. Not here. Next speaker, Jose Rodriguez. Great. Can you hear me? Yes. Yeah, thanks. Organizers and chair for the opportunity. My name is Jose Rodriguez. I'm from Cal State LA. So I'm going to talk about some theoretic work, trying to understand compound we've all been trying to understand iron cell and I electron dope which is a high temperature to bring up there up to 50 degrees Kelvin. And so I looked at another. Some of my colleagues looked at nesting and instability story in order this is not the Fermi surface of iron cell and I but you can get something that approaches it by looking at adding fluctuations hidden spin fluctuations. And these are the fluctuation fluctuations I was looking at between orbitals in particular the isotropic orbital so there's no pneumaticity in this, in this model. And then if you do. Again, for Glendale theory, sorry, Eliasher theory with fluctuations of the two bands are connected with these orbitals. And if you look at the, the fluctuations at criticality so this is a critical spin fluctuations near one at a critical near one critical point you can get a list of transition where the, you get electron pockets, you get. Let me try to get this figure here. Ladies and gentlemen, you get electron pockets on these orange circles and you get a whole pocket at the corner of the wrongs on you get a whole pockets at the other corner. The interesting port is the way function real normalization of the whole whole pockets is weak it's very faint whole bands, whereas the electron pockets are moderate so it potentially can describe electron so on this list of its transition. And you, you find I found a Cooper instability on as plus minus pairing where the sign of the order parameter Cooper pair alternates between the hole in the electron bands. So if you're interested in anything the details, or just really understanding this here's the paper that was published last year and I'm, I'll put my email on the chat if you want to talk with me chat with me thanks. Thanks. Thank you. Next speaker. Let me stop here. Thank you. Next speaker. Can you hear me well. Yes, please. I wanted to talk about the fine structure of excitons in type two team the heterostructures today, where we describe the electronic and optical properties of molybdenum dissonant tungsten dissonant type two heterostructure using first ab initio methods and then tight binding with a solution both coupled with solution of metastalpeter equation, which adds to exit and expect to. So we start with determining the electronic structure of molybdenum dissonant tungsten dissonant from first principles. We obtain the type to bond alignment and conduction band minima in Q point as you can see here. Next, we perform the analysis of concham wave functions allowing to detect the leading layer and spin contributions and construct a minimum type binding model of this heterostructure which allows us to understand the orbital contributions to block state and study the effect of wave functions on the exciton expect from so all the topological properties of the system. Finally, we accurately solve the betasalpeter equation and determine the exciton expect from for that, as you can see on the last plot. So we define both intra and interlayer excitons, and we use simplified Ritova K additional local screening theory here. This all will allow us to finally study the effect of more a potential and comparative fully tight binding approach to excitons in twisted more heterostructures. Thank you very much. Thank you Katarzyna. Thank you, Dr. Eker. Yes, you're solving. Can you hear me. Yes, we can. Great. Let me just pull up the poster. Can you guys see the poster. Yes, we now can see your poster. Yes. Great. So I'm going to talk a little bit about artificial graphene quantum dots. Specifically, this triangular zigzag edge triangular graphene structure. What's special about this structure is there's a sub lattice imbalance between sub lattice a and B. And this leads to broken symmetry and gives spin polarized ground state. So I developed some model to describe the system in terms of artificial potentials at sites denoted by the points on this triangular lattice will hexagonal lattice shape as a triangle with zigzag edges. And what's special about this system is that if you diagonalize a single particle Hamiltonian, you find a nearly degenerate shell at zero energy or at the Fermi level we'll say. It's not perfectly degenerate due to next year's neighbor hopping terms that emerge in my Hamiltonian. So then what we can do is understand many body physics on this shell degenerate states as a function of being able to tune the parameters by artificial system for example, the width of the confining potentials, the separation between sites the depth of the potential since it's an artificial system you kind of have a playground of tunable parameters. And what we find are two distinct regimes, one which is metallic and one which is anti ferromagnetic. What's key here is that because we have broken sub lattice symmetry and half filling live predicted a spin polarized ground state, meaning that the total spin of the ground state was proportional to the difference in sub lattice a and B. In the weekly interacting regime we have a metallic phase but since our system is still spin polarized we observed that the extra electrons occupy the edge of the system. And in the strongly interacting regime where you over T is large. We have an anti ferromagnetic insulator. So this was just mean field calculations, we then took it a step further and did included correlations in the system. What we found is as a function of filling of the system at half billing, we had a spin polarized ground state, and away from half filling, you get a dramatic drop in the energy gap and other lower spin states emerge in the system effectively becoming kind of like we'll say a button for turning on magnetic properties are turning it off. And that's all I wanted to say, these results are published and if you want more details. The answer saline the University of Ottawa, and I will put my email in the chat and I kind of wish I was in Rome, so everyone enjoy room. Thank you very much. Thank you. Yes, sir. Next speaker more that's a solid. Hello. Yes, yes we can. Okay, let me to share my screen. Please go ahead and share. I cannot share my skin. I think the other screen is now broadcasting. So there's a green button that says share screen. If you click on it, it should. You should be able to share. Can anyone see my screen now. No, no, no. Yes, sir screen is no broadcasting. Please. No, you stop sharing. How to solve the problem. Sure yours. It's not working. Maybe. I don't know how to solve the problem. Maybe you can restart. But my, maybe you can restart your zoom and the meantime, we will go to make speaker. Please stop your sharing. He stopped sharing cold. Next speaker. So our car. So our car, please. Next one here. Next speaker. Jamie Lee. Say yes, the. Hello. Hello. Can you see my screen? Not now, but something has started. No, we cannot see anything. Is that okay? Nope. No, now it's okay. Yeah, go ahead, please. Go ahead. We are setting the digital versus non digit JPA is gain and application quantum. Two modes squeeze rather JPA is Josephson's and parametric amplifier. Here you can see. Here you can see the schematic representation of the quantum. Two modes squeeze rather or QTMS rather JPA is that the heart of the quantum brother that produce entangled signal and Euler. We either can have a digital rate JPA, which has a signal and Euler, maybe the same frequency or a non-digital rate JPA that there's a small difference between their frequencies. Here we show that using a non-digital JPA is going to improve the performance of quantum brother. Our evidences for this claim are shown here in this graph here. For example, in figure two, you can see that. We show these two solid lines. They are for maximum and minimum gains for degenerate JPA. But as you see, the dotted line on top is for non-digital JPA gain for Euler. So here is the first evidence that say degenerate JPA works better. Another evidence comes from SNR, which is signal to noise ratio. And as you see here, the non-degenerate one works better. And this is versus the number of modes. The other one, which was in figure four, then the left side is for degenerate one and the right one is for non-degenerate one. Here we use the quality factor in thermal one, which is fixed between these two, but we increase the external quality factor. And at the same time, we are calculating gain. Sorry time is running, so maybe you can just summarize quickly what's in the poster. I think that this non-degenerate one works better because higher Q value means lower loss. Therefore, when we have lower loss, which is desired for quantum brothers, we have higher gain as you can see here. So these are our evidence to show that non-degenerate JPA works better for the quantum brothers. If I have time, I can talk about my second poster or not? No, unfortunately, sorry. We need to move on. Here is my information if you can give me a comment or discuss. Thank you. Thank you. Thank you very much. Thank you. Next speaker, Musa Mil Shah. Not here. Next speaker, Mustafa Sayed Ahmed Shalabin. Ahmed Shalabin, not here. Next speaker, Shaliyah Sharma. Shaliyah Sharma, please. Yeah, we can see your screen. Yeah, please go ahead. We can hear you. Okay. Yes. Can you speak up a little bit please? Yes, please. Can you say it? Hi, I'm Shaliyah Sharma from IIT, Mandi, India. I will present our work, electronic properties of palladium-intercollated dysmetalluride topological insulator. So, motivation for our present work is palladium is a high Z element and shows exchange enhanced magnetic susceptibility. So, we have studied evolution of electronic properties and topological surface state properties upon palladium-dropic in dysmetalluride. And here we see this resistivity of these caristors show metallic dependence upon low temperature and this high resistivity shows electronic majority charge carriers for dysmetalluride and increase its changes to P type upon palladium-doping. And here we see this magnetic resistance decreases upon palladium-doping. And here we have analyzed the Shubnikov-Bihar's quantum oscillation using Lipschitz-Karswisch theory. And we further performed artist measurements along the gamma N direction and here we see that this tickets a narrow line width for dysmetalluride. And this, here we see this bulk Wellesband as well as this direct point energy shifts towards the Fermi level upon P-D-doping. This is well in conformity with the Hall data that shows N to P type crossover upon palladium-doping. And here we see this hexagonal warping is then decreases upon palladium-doping and it turns towards Mohr's circular. And therefore taken together this STH data and RPS results, we see that there is a reduction in Fermi wave vector from STH data and this reduction is due to the band bending effect. And this band bending effect is induced by the Schottky barriers at the metal semiconductor interface and this is inevitable for the magnetic transport measurements. So, overall these studies discuss correspondence in parameters obtained from RPS and magnetic transport results. And for more details, you can follow this paper or write to him. Thank you. Thank you. Next speaker, Gabriel Moreira Suza. Hi, can you. Hi, can you. Yes, we can. We can hear you but we don't see your screen. Now can see. Now we can see your screen. Go ahead, please. Okay. Thank you very much. My name is one. I'm about effective the tip for fractals. The model I'm working with. Okay. The model I'm working with is what's first proposed as a fragile like quantum glass by Cassano Benchamon. It is defining HCP lattice. It is described by the this Hamiltonian one in which we are prism operators defining here. And the properties of this model are it is exactly solvable. The eigenvalues are plus or minus one. Therefore, the eigenstates when all the people prioritize eigenvalues plus one, and the model is get it. The most interesting properties are the mobility properties in this direction the expectations are mobile while in the x y plane the expectations are fully mobile they are fractals. In order not to annihilate free excitations, we see that the formation of fractal membrane characterizing it as a type two factor. So to construct an effective theory, we propose these gauge fields with these gauge transformations, and we can see that it presents the desired profits because if we study the interaction action, we see that there are two charts. We have seven charts Q and QF and QF shows the desired property about the fractal behavior because F is an harmonic function. This is what I have very much. Thank you. Thank you very much. Thank you. Next speaker. Malik. So, yes, we can hear you. Please share the screen. Hello. Can you hear me? Yes, we can hear you, but we don't hear screen. Let me share my screen. Please. Please share the screen Malik. Malik, we cannot see your screen. Maybe you can just restart zoom and in the meantime we'll move to next person and then we'll come back. Let's move to the next speaker. Samudra Sur. Yes, please pick up and share your screen. Yeah. Now, am I audible? Yes, yes, go ahead. Okay. So, I'm going to talk about driven Hubbard model on triangular lattice. This is a portable Heisenberg antiferromagnet with three spin current term. So in this work, we have studied the interplay of periodic driving on a strongly interacting electronic system on a triangular lattice. So we start with a half field Hubbard model on a triangular lattice, and we drive it with an electric field which is in plane to it, and the form explicitly breaks the time reversal symmetry. So we incorporate this electric field into the system, following parts prescription by adding a phase in the hopping term. And we use a theory called floquet perturbation theory in the limit that the hopping terms are much less than the interaction. Then we see the low energy excitations are described by the photon assisted virtual hopping in the nearest neighbor sites. And using this floquet perturbation theory up to third order, we derive an effective spin model, which has nearest neighbor Heisenberg couplings, which is an isotropic in three different directions, and also a chiral three spin term which has plus and minus sign for up and down pointing triangles. So these couplings of this effective model j alpha j beta j gamma and see can be tuned by the driving parameters, which are the amplitudes of the electric fields e one e two, the frequency of the field and the angle of the electric field theta. So here it is shown for some values of amplitudes and frequency how the couplings vary with the angle of the field. And from see vanishes if they if the driving field is time reversal symmetric. Now from this effective Hamiltonian, we do an exact diagonalization on a six cross six lattice system with periodic boundary conditions, and to reduce the Hilbert space to attractable form we use the symmetries of zero magnetization spin inversion and simultaneous parity inversion along x and y axis if C is zero. And then we study the different ground states of this model using the spin structure function. And we find that there are four types of ground states of them. So four types of ordered ground states in the system of them three are collinear and one is co planner of 120 degrees time. And we also have three type of spin liquid ground states. And we also found find the phase boundaries using using fidelity susceptibility real space correlation and energy gaps. And here we show the phase diagram. We have these seven phases of these four are ordered and three are spin liquid. So, and this is a work which is published in PRB this year. Thank you. Thank you very much. Thank you. Thank you. Please, I think it is okay to screen to share my screen. Malik so Samudra please. If you can just go ahead and share your screen. Yes, go ahead. Samudra please stop. Yeah. Malik so go ahead. Unfortunately, it doesn't work. And if we cannot see your screen. And now maybe something is going on. Unfortunately, it's probably bad connection because it started and then crashed. Let's try. Yeah, maybe you can just say what's the, what's your title and in few words what the poster is about. Could you describe your poster in just a word and simple words. Yeah, I guess the screen is frozen. Okay, let's move on. Yeah, we need more fun. Next speaker Jill swami Jill swami. Not here. Emanuel. Emanuel. Not here. Shannon way. Yes, go ahead. Yeah. Hello, I'm trying. I'm going to show how the strength mental phase appears in disorder just by the graph and how this is the relate to the with the couple that's like a bundles. I just want to understand the relationship between the second phase and the strength mental phase in the two spedigraphy. I didn't know that the medical and go to spedigraphy hybrid sevens, our idea is to break the flabons into bundles to break flabons column disorder is introduced. The potential craze puddles, intuitively localized flabons are just trapped by these puddles inside each puddle, which is also, which will also becomes a slightly bundle, the interaction of the sevens just to make them, make them interact with each other, creating an auto interaction, just like to select behavior, and the bundles are also actually interacting with each other. The specific heat is computed at low temperature, showing this like a behavior. I'm here by computing the auto time or the creator, they have enough exponent of the, and the bath lab lost it is also extracted. We can see that at low temperature, the level of exponent is just linear in temperature, which is a typical behavior of the strength metal. Also, the bath lab lost it shows a non familiar type of temperature scale, which scales as to to the some power, which is larger than one. All this concludes the chaotic strength metal phase, also at week disorder. As one can expect, the system recovers the connectivity and the auto time or decorator just show the exponential decay. As a result of all this, we come to the face diagram, just like this. Thanks for attention. Thank you. Thank you channel. Next speaker. Hello, can you hear me. Yes, we can. Okay. Share screen please. Yes. Is it okay now. Okay, yes. Good. Yes, go ahead please. Thank you. Hello everyone. My name is Razia and I'm here today to talk about some of the interesting features of a small bit couple junction. Based on graphing to get started, I want to propose a junction as you can see in the figure made up to for magnetic region and spin orbit coupling layer between them, which is always on a graph and layer. And, you know, both magnetism and spin orbit coupling can induce into their graph and layer by proximity effects. So we have a very good setup to actually to changing the orientation of magnetization to produce a spin or ice current. And the spin torque exerted on the junction we considered this situation that the bias will face right particles from the left for magnetic region into the right one. So, so if we consider the effective Hamiltonian, like this equation for each three regions and boundary conditions at x equal to zero and D. And then calculate the what the wave functions and other parameters we can study the closet particles reflections and transmissions. And then other features like spin torque spin conductance and spin turn problems. So you can see in this figure that that it is the main result of this study. The spin transfer torque as a function of spherical angles of magnetization in the for magnetic region. So, so when particles hit the interface is perpendicularly the simple arise direct fermions transmit perfectly through the boundaries of junction and, and the spin transfer is often zero. So in the presence of the spin orbit coupling and non zero spin transfer torque we appears because of the event the structure modification. And, and finally we hope that these findings can be applied in the proximity in the spin orbit coupling graph and system experiment. In this discussion can contact us with this email others and see the original version of our article in the archive. Thank you for. Thank you very much. Thank you. Thank you. Next speaker for note. I'm sorry. Hello, you can hear me. Yes. Yes. I have some problems. Let me correct it. Excuse me. Can you see my screen. No. If I have time I will go to next one and then you will try to fix the problem. Let's go to the next one. Good. Next speaker.  Next speaker Ahmed chaff I not here. So anyone from the previous speakers who had technical difficulties. Anyone wants to present. I think just my presentation is remained. Yes. Yes. Go ahead try. Okay. Maybe describe it in just words. Try again. Okay, I can talk it in audio. No, no problem. I can do it. Please go ahead. I have a question. I have recently ended post that period I have worked on several questions about many body and transport properties of force worrying which is highly on isotropic monolayer material. For London family liquid in its most most on isotropic version. It is well known that in line wavelengths limit and finite frequency of external perturbation the current density within linear response regime is equal to viscoelastic model of electron liquid. A question is that, what is the elasticity hydrodynamic correspondence would be in the case of on isotropic liquid, like that of force for this question then arrays. What is the appropriate hydrodynamic model for 2D electrons in general, and especially for force for in as an orthorhombic to the two dimensional London family liquid which can go further to find viscoelastic model for a generic on isotropic viscoelastic dynamic equations with 18 independent risk elastic module and the solution within the solution the Christopher matrix and metric tensor immerse, immerse out naturally and put it in equivalence in line wavelengths limit to the microscopic theory of the of our microscopic theory by means of the exchange correlation kernel and go beyond the random phase approximation and modify their RPA plasma. See that the gravity theory is here efficiently image out as an viscoelastic version. This rings the bell in the mind for a holographic duality viscoelasticity as the gravity and microscopic theory as our field theory and then let me briefly discuss about my motivations which this time. Yeah. Thank you very much. I put my contact your email address yes. Thanks very much for the problem. Thank you. Thank you. Thank you very much. So this concludes our poster discussion section. Thanks to everyone.