Hi guys, welcome to my first New York vlog. I'm so excited for this Basically, we got up at 4 a.m. And we got ready and we're headed out the door, and it's currently 530 There's Spencer right over there. Enjoy the montage to New York City. Let's again He just made it to the airport and now we're just waiting. I'm so glad the airport provides some good lighting They have charging ports and everything, which is pretty neat. We also have charging things down here, which is pretty cool Thank you We made it into the hotel room and I'm gonna do a little room tour because that's what vloggers do I'm gonna show you guys around so coming in we have a Spencer to the left We have a little closet area, and then here's the bathroom. It's really really nice nice clear shower door toilet towels Hand towels toilet paper the little soap and shampoo thing very basic. You need to go to the bathroom We have this really cute body mirror on this door, which is amazing for like OOTDs like I'm gonna do right now So I'm wearing this brown jacket fuzzy sweater black jeans and my eggs over here. We have a little coffee Section we have snacks in the little mini fridge We have coffee and a Keurig which is pretty neat king-size bed and one night stand another night stand And let's see the view. I might need to take an Instagram picture here. Oh, yes We're taking a picture here. Look at how pretty we have a very good view air conditioning unit a little desk here with some drawers And a little seat and our luggage so that is the room tour We're all ready for the meet and greet night, but we're gonna get something to eat first So basically I'm just wearing this dress. It's the forever 21 dress with some brown tights and my knee-high Shoes I will go show you guys in the mirror. I don't know why I'm doing it like this I just really like this lighting from the window. So did the hair is the makeup. We're rocking. We're rolling Let me go show you guys in the mirror. It's kind of dark But as you guys can see this is what the outfit looks like for lunch Spencer and I are eating at rare It is just a restaurant in the hotel. We're just chilling out here. This is an overview of the restaurant It looks really nice in here Spencer said it he was like you have to take photos. Yes, he got the chef's choice burger Not the exact name and then I got a chicken salad with different like little tomato things Which is pretty cool. This all looks so good and the fries look good too. We're splitting those We have a little bit of time So we're going to walk to the flat iron building and it's gonna be really cool because I've been wanting to take a Picture at this location for a while now. I see so many like Instagram people take it So also I'm gonna try to get Spencer to take my picture like walking across the street Hopefully not getting run over. So we got some video clips because I really want to do like a travel diary type video. Oh Man, look at this really cute wall There's cute walls everywhere here. All right, so we made it to the flat iron building It's a right there as you guys can see and we're gonna be super touristy and take a lots of pictures Thank You Spencer for dealing with me. Just look at it Look at how pretty it is There's New York for you. Okay, so Spencer and I just got some really good shots. He's over there a little speck over there I'm probably gonna walk back to him But I wanted him to get some video clips of this building because I need something for the travel diary And I don't know. I just I really like this building. It's so pretty if you guys aren't already follow me on Instagram Link is down below and on the screen there He is right now Spencer and I are on 5th Avenue, and we're just gonna walk around the shops I'm not sure how much I'm gonna be able to log in the stores because sometimes they're a little like uptight about that So I don't know but I definitely will get as many clips as Possible also guys to tell you the truth these tights have been sliding down my legs ever since we started walking I don't know why they just like to ride down so uncomfortable Oh, there's a Michael Kors and a Tory birch. What are we looking at? Okay, so oh we need to go to case I New York. Well, cuz it's in New York. That's the store Just wanted to get a clip of a 5th Avenue sign because it's just 5th Avenue So and honestly, I was telling Spencer how much I love being a tourist because you know at Disney Everyone's like we're in their ears and stuff and like being a tourist is like oh tourists But like we're a tourist and I'm pretty proud because I never get to be a tourist at home Is it fun being a tourist? Yeah, someone can let me know why this thing does this. There's been like a couple of them here I have no idea why but anyway, we are at Kate's Fade We'll just pretend the fog is a cool effect for the Kate's Fade store So we're at the Got Some at Rosé and basically we're just like getting to know each other It's like we first got this opportunity and stuff We thought it was like illegitimate and we're like Kind of skeptical, but we're all here and we're all having a really really good time So I'm gonna do a little hand. There's more girls here Okay, so we're back at the room now and I kind of just wanted to unbag this for you guys So the first thing is oh my gosh, they put a little card. That's so nice But it is the first edition of the Azori magazine. They just came out with this and it's so cool I wonder who's like featured in it So I'm gonna open this little card and it basically just says we are so excited to have you here We hope you enjoy your experience in New York Fashion Week the above-time team. So nice. We have some smart food Amazing. We have a Dasani sparkling water in Berry. I used to love this type of stuff But it's in a can which is pretty neat and then we have this smash crispy bar. Thank you so much about time Okay, so Spencer and I are going to the rooftop bar because we want to explore Wow. Look at this. This is so cool Thank you. This is so cool. Look at this This is so cool guys so aesthetic and you have to be 21 and over to get in here So I'm feeling a little special Cheers to us That's so cool Wait, really you didn't okay He was trying to scare me and say that he forgot the charger But right now I'm gonna start editing this vlog that you're watching. We're gonna order a domino's pizza So that's what Spencer is on right now. So far New York's just been super fun I'm excited and I met some really fun nice people. So I'm gonna start editing this. We're gonna eat pizza Let's get editing. We got the pizza pizza, which one did Spencer get they actually got the wrong address Which I felt kind of bad for but oh he got pepperoni. We're gonna eat I'm almost done with the vlog like probably a little over halfway, but I think it's turning out really really cute I hope you guys like it. Okay. So basically we ordered room service This is why my parents don't order room service ever But we didn't really think that it was gonna come like this But we got these like cups of ice and then we have this is bottled water But like in a legit bottle and it's glass and Spencer got his coke And let's just say this is kind of probably the most bougie I've been in a while It's something to remember and it's something we'll laugh about in the future. So that is pretty much it for this video I hope you guys enjoyed it get pumped for more videos I'm hoping that I can update these and post them Chronologically and pretty fast for you guys, but I don't know the Wi-Fi here So give this video a thumbs up Don't forget to subscribe to see it more at New York videos, and I'll see you guys in my next video. Bye


Well, the one thing that I tell everybody is in this type of system, especially with the insurance sales lab, is that they're like, well, I really don't know if I want to spend that money and I have to change that terminology because it's not really a spend, it's an investment. And so it becomes a spend if you don't use it, or if you don't utilize it, or if you don't join the insurance sales lab, it becomes an investment once you do. Invest in yourself and this is the best way to do it.


Hi, I'm Tom with Gaurav Elmans and today we'll talk about beam efficiency. Antennas have many parameters and it can be often quite difficult to understand which ones are important and when. In Wisp industry, users often give a lot of importance to front to back ratio, which says how strong the back lobe is compared to the main lobe or side lobe level, which tells us what's the strength of the biggest side lobes. While both of these parameters have some information of value, what Wisp should really care about is beam efficiency. Beam efficiency tells us what portion of the total energy an antenna radiates is contained within the main lobe, where the main lobe is defined up to the first null of the radiation pattern. In other words, beam efficiency is a measure of side lobes of an antenna. For example, if the beam efficiency is 40%, it means the remaining 60% of the radiated energy goes into the side lobes. For a stable network, antennas for fixed wireless applications should perform well in the whole bandwidth of operation, which is why it makes sense to average beam efficiency over the whole bandwidth. In textbooks, beam efficiency is defined at a single frequency, but we took it to another level by averaging the beam efficiency over the whole bandwidth of operation and both polarizations of an antenna. This way, the beam efficiency as a parameter is much more robust because the higher the average beam efficiency is, the better the stability of antenna performance resulting in a stable network regardless of the channel you use. Beam efficiency gives you a complete information about the side lobes an antenna might have because, first, it considers the full 3D radiation pattern and second, it's averaged over the whole bandwidth of operation. In contrast, the front-to-back ratio or side lobe level is commonly defined based on a single slice of the radiation pattern at a single frequency point, giving the manufacturers a huge gray area to make your antennas look better by picking the bed snippet of the radiation pattern. Eventually, front-to-back ratio and side lobe level only define one of the many side lobes an antenna might have at a single frequency, which makes these parameters practically useless in real life. For more interesting topics from the Earth world, check out some of our older videos and don't forget to subscribe to our channel.


The longest running soul link in YouTube history. I feel like we've got No, no definitely not but I can't believe we're here Dion it feels like it's been so long since the last episode Over on your channel, which you should definitely go check out if you missed it because Dion We need to start with a very quick team recap. It's been a long time. Just for me. Oh, no Yeah, if you didn't see please wait, this is spoiler warning if you did not see last episode You need to go watch it on the chair This this was arguably the craziest episode that has ever been released Yeah, you are going to be this is like post-time skip right here This yeah, you need to see that former episode and honestly we need this to do. I'll pull up your team. I'm going in Oh my team is horrible. Oh my god.  I promise you I Am way more hurt for Bower being gone that that was my guy you guys just knew him I knew him and we gotta do a quick quick little grind session I think I got to get my team at least up to level 30 all around probably which isn't too long I'll be honest. Let me see how I'm at. I mean I pretty much pretty much have that I got 29s at the lowest try attack you better live this I don't know how strong you are 50 health. Am I dead beyond please? Bro you got me scared. Can you not get a guy like me scared, bro? This is a fire. This is a plant. Wow I know type disadvantage. I'm going to switch out. Oh, yeah, I forgot. I love having Charizard, but I got no fire moves, bro This is Charizard with no bitches. Who am I facing? Caterpie Wow shouldn't exactly be the hardest boss of ever. Draco's got to be the new like main character of my team And then you yeah, enjoy the fish Bro, I got two fish man No way this thing can beat my Draco, right? Should I leave? It's a fish.  Can I just run I can run right? I'll be back. All right one more level and then I've got almost all 30s dude sleep powder Wait, isn't this like something I can't hit or something you can hit him with any move that isn't normal. They're not straight What is that Hyperbeam is like the final normal move. Oh, it says normal cash in red. I thought normal was like oh punch What what what what? I Was he linked to who is he linked to I need you to go through your team. I don't know. I don't have the I'm actually no this can't be happening Just just open them all up and scroll through of like hit hit a on Charizard I'm gonna start with the ones that I hope it is in that Okay, and Nope, he's safe. Is it Kevlar?  That is my bee dude. I knew it was a fire type. I just bro. I warned you bro that oh no What we don't have any backups. No. Yeah, these were our last Pokemon, bro I need you to understand how devastating this is only one man on my team made it here. Oh You made me look at him. You made me go in here and look at him Look at all look at all of the fallen look at all the fallen. Hey, man. What are we to do about that? Not get our Pokemon killed about that as a good starting boy.  So I'm gonna fly to the safari zone. Oh That guy was my flyer Oh my god, I gotta teach it to somebody else I was gonna say those legs are made for walking. I thought you just lost the ability with them. That would be hilarious We did route 15, huh?    All right, Donna.  All right, go ahead, bro Let me write route 15 on my list just in case I have to start a new list Let me let me look at the good people at home and let you know that the Pokemon right in front of me It's gonna be the Pokemon that saves this series. Let's go He's dancing in the bush. He's getting down Wait, all right. I need I need I need your intel. What type is this? I think it's bug rock I don't want to one hit it, but I do want to punch it. Hey beyond. Let me get in there and dance with you, man What? Bro got a blue sea on his screen I'll take it from police. He's rather tanky bro got mazhan boo. That's mazhan blue sea All right, I'm really afraid of how to approach this. I mean rock is rock is very bad for Draco I will be honest. Draco would is getting bodied in that. That's all I needed to hear But then is grass too good grass is weak to bugs so shadow probably gets bodied in this matchup, too Do I need to use buzz buzz? I think it's bodied by the rock. What about that plant? It gets bodied by the bug. Okay, normal. Uh, maybe but that's like a baby. I don't know if I recommend I think maybe I Don't know what your best Here is I hate you and this bliss about how whoa, that's a normal move wait that only limits my okay They're mine. We're good. We're good. We're good. You did scare me. I'm sorry. I'm sorry I really shouldn't be adding stress to your pocket. Okay, stop. No more. No more catch that thing Catch that bad boy as a sign of good faith as a sign of good faith I'm gonna use one of my ultra balls. I should easily lock this thing up one two three Yeah, you got that Why does bro get to be two times bro cheating bug and rocks those those feel like just like the perfect counter to anything I feel like Venus or Waller risk is less of a risk than Draco because if one rock move comes down on your head It is it is over. It is over. This was your choice. All right.  No, no, that's very bad. What I mean That's gonna that's like that's like raising all of his stats. Oh special attack.  Yes What would I switch into him then I because we'll never okay, it might not do a lot of damage, but You told me to try it Okay I'm throwing a pokeball. I'm throwing it. I'm throwing it. What's my best ball? I don't know if I have any ultra balls, but I will see what I got I would go with ultra ball from your balls. Just decorative pokeball. All right.  Well, I was about to say I thought jit was eight feet tall Let's go our maldo. Oh, yeah I was hitting the wrong button. I didn't get the nickname blizzard.  Well, what you some although he's the savior of the series, bro Honestly, I am I'm investing in those stocks the way that I was intimidated by him He's going to intimidate all my foes bro. What moves did he have does he have rock glass bro got? By oh, he doesn't have any rock moves.  Hey, bro. Don't don't put blizzy down. She just joined the team man She's doing her best. Let me just go into my TM case here I could probably what if what if she can learn surf like that would unironically be very good for me So, let me try it Damn it blizzy. Yeah, let me see what I can teach my squad. I've been really looked at my TM case in a while All right, Kefla sir. Let's learn you a new move. Why don't you learn this rolling kick, bro? Fuckest converse. Oh, I thought it was conversation. So anyway, I was in the pocket ball. Can't we sell it over a pint? Reference to a movie that's better than kung fu panda.  All right, Dion.  I'm gonna go coughing It's coughing Next episode I'm gonna push you with something else about next next episode. I guess but yeah, that's if we survive this episode All right. Well commercial break over.   I think we have. Did I just wait what? We haven't done none of this. Yo, I'm confused. Yeah, I'm confused too sky uppercut boom To the chain. He's going down. Oh my god. Hope hope for a new nation. He's bugging Did against ghost? I hope not. Oh my god. I hope not. Oh my god. I hope not.  You think I'm gonna lose well Yeah, now I gotta go bro. I can't have you being too far ahead of me And can we talk about how I got a 10 level dip on all young slifey? And I miss my attack Impressive and he missed his attack. This is the worst battle of all time Hey kid, what are you wondering around eat boy? Um, so this guy has some pretty decent mons.    We had one of those thunder punch Eat it. Oh look at young slifey. He ate that.  Why not? I Missed what do we got for her across? So I have any wing attacks. Oh fly. Oh, yeah Let me get bobeep in here real quick. Let me get him in here bobeep All right now the only important part is that I fly before he breaks my wings Oh, here we go. Here we go. Here we go sound like strong But here comes the fly for the old co bobeep Yogi it's level 27 bobeep. It's level 31 and I gotta go heal my mom's wait What was the other pokemon it started with an s that they have it's a fly it should be another bug So, oh, yeah, that's oh, yeah, we're good.  Look at this. Look at this. Look at boom. Boom I guess I'm moving on to the next trainer bro. Like wait, you said rock destroys flying, right? Absolutely destroys it.  I am right there with you, man. I'm going up against a rally canth Kefla despite being level 31 because of the fact that it's a baby just is just inherently weak It stats just aren't good. Also, relic canth has rock slide. Let me Call that out real quick the next trainer, bro.  We needed that slide fee. We needed that We needed that one.  All right hyper beam What that better ok. Are you got to stay in for a turn? Let's go Sky uppercut on the zigzagoon to the chin Uh Hair crosses a bug right bug fighting.  It scared me. Oh that kind of that did hurt a little bit scared me Honestly, I just put the paws on that next trainer. Yeah, bro. Why are you trying to be so far ahead of me, bro? What's good with you? I'm not super bullish on keeping yogi out in front right now, but I guess I What does yogi know depending on what yogi knows?  Which way did you go to left? I went down. I'm fighting some trainers down here. Just uh, you know Moist and my whistle. Could I just go to the third floor, bro? Are they stronger up there? I I don't know man. I don't know supposed to know bro. Who's this guy? This guy's wearing different clothes Yeah, I'm fighting right now. What is this three headed ostrich supposed to do?  All right, his next pokemon is Krabby I'll beat the brakes off of a crabby.  He has thunder and flying.  I got to see you. Okay. Bye gust Is there a reason that I'm getting absolutely melted by a dojo rio? Bro, why don't you switch into a pokemon? That's like a good matchup. Don't have one of those Ah dust docks Uh, that's a bug, right? That's a bug poison.  Then he's a real Charizard right now.  I know hitmonchan that is from the gen one So are hitmonchan's like born with the little skirt on or what?  All right, where does this teleport me to Hey, bro, you're getting a little deep. Yeah, I'm getting in there deep. What do you think? Oh, there's a computer. Hold on.   Do we get something?  I looked away for a second. I am one of the four rocket brothers But does that mean you're talented champion Malcolm? Gasly confused ray.  I'm in the mood to kill every team rocket trainer in here I'm gonna battle every team rocket trainer and my team is going to be level 40 or we're gonna lose the series golem Bro golem.   Oh, that was kind of painful. Oh, no, I'm still confused No, no, no, no, no, no, no. No, no, okay. I'm healing. I'm healing. I'm just I'm nervous Bro, you got me nervous over here.  Not another dodrio. I can't live this life anymore Seeking I'll beat the brakes off as seeking, bro Oko, oko Man, we are living in two different worlds. I'm feeling good now. I just need to like oko this thing I think that means it's life. He just needs to come out and body it before giving thunderbolt at the death So I'm just gonna try it I just I have to just trust in the level advantage. It's life. He misses this actually is gg for the run This is actually gg. Don't say that Don't say that to me gust. Okay. That's a good rng good rng on gust. We eat that up crab hammer I think we miss. Oh, we miss. Dotto, please. There's the area lorries.  We hit it. We need a crit. We need a oko. We need the oko Just hit it one more time, bro Wait, do you want to heal or what do you what are you thinking? I'm just gonna heal and hope. All right, good. Bro, fast motion. It killed the suspense Oh, let's go. I did broke. I couldn't take it. I honestly I I sped I sped up because I couldn't take it no more I'm just trying to find this giovanni loser. I'm on the fourth floor partner If you asked was it so god damn awful, this would be so easy Perruption, that's very bad, but I'm water type. So I probably eat that up That is a very good move, but I think I just eat that up. No problem. No questions asked Oh my bad.  He got a crit. That's not even if it boom Bye-bye. Bye-bye. Bye-bye. Oh, is this giovanni? Is that him? No, what do we know? This is the only different looking guy, bro No giovanni is going to be behind like a key card door and the rival fire Oh, so I have to get to the rival first. Okay. So look for what is going first I need a key card. I'm gonna try this teleport I got tricked. Oh, yeah, I dealt with that guy. He's he's not too bad. He's the one who had like the golem and stuff Okay, I mean giovanni's not too scary for me either. All right, let me find out who this guy is man Who are you bro? Who are you? Shouldn't be any children here bro.   He looks nothing like he did when I just saw him Honestly, I'm having a decent battle over here. Yeah. No, that battle's not too bad This guy was a bad matchup for me. Yeah, you good. You good. He ain't he ain't stacking up to the other guys Yogi level 29 in the back pocket.   He does like father like it's kind of touching. It's kind of touching All right, um, I'm I'm tired of this pedal dance.    All right. Uh, sorry, son.  I hit myself if he hits himself too, I'm gonna start crying I'll do it. Do it.  I need to see like what this is all about So that's the room we're trying to get in you see that room that room has some goods in it Oh, wait, what what floor is that? I don't know man higher floor. I just went up the stairs. Oh, that's a different set of stairs Well, go down and go back up. It'll tell you which floor it is 10th 10th floor and then I was on the 11th floor. Uh, hell, how'd you get that high up? Oh, that room's got some items in it, bro Truth be told, I gotta risk it. I gotta risk it three items Yes, sir. Yes, sir Bro, I'm I'm going to where you're at.  Do you think he has the same moves your guys have if he does you're fucked? Honestly, I feel like I should Well, don't say that. You know what I think I'm gonna do.  Now that venus or is asleep Is it level 33 venus or by the way?  Well, guess what? Meet shadow a level 36 venus or bro. Let me drain you real quick. Wait, what? I need this guy to stay asleep. I'm not trying to see what other moves.  Hey, bro. Hold on. Whoa. Whoa. Whoa relax, bro. Only one of us gotta be poisoning around here Come on now. I flew up bro. I'm in the skies. Oh, he's hardening. Oh, let me hit him with a little sludge bomb to finish it bro Why is he this hard man? Damn bro only had one pokemon bro's weak.   I got the bow beep Unlikely person to take that battle on wouldn't heal up shadow shadow been carrying me through this one.  Let me just take a peek upstairs. Oh, yeah, so that's where we got to get right We got to get inside there. We got to fight Giovanni.  You know, we have a purpose even though this episode started a little sad Like it definitely did We're in a better place than these On that episode we remembered we were fucked. It was it was a bone-chilling episode Okay, I think it was a good one to come back on though. I agree. I agree. No, it was it was overall It was overall productive. I must say hey hey team rocky guy. Hey. Hey, what are you gonna do? Hit me?


What's going on everyone? Sam here, late in sports cards. We're ripping one box, or not one box, five boxes, excuse me, of 2022 Bowman Chrome Baseball, HDA choice for M.O.D. Good luck M.O.S. See you we got buddy. I'm showing though, you are. I'm not really. Oh, I need to talk to your parents. Really?  I know she's out, passed out. Yeah, she's been out since probably about nine o'clock tonight. That's it, get her out. Jose Rodriguez for the Rangers, Mabesa. Sir La Prada, that's 162 out of 2.99 for the Mariners. And then Basado is Michael Garcia for the Royals, nice one there. Got a blue choice, Denzel Clark to 150 for the A's. Next up we've got Juan Guerrero for the Rockies on the first. And then we've got Graham Ashcraft going to the Reds on the first as well, Basado. There you go, Emma. We've got Refractor to 4.99, Adrienne Stagastie for the Giants that's 10 out of 4.99. We've got nice one here, Basado is going to be Samuel Munoz that's going to the Dodgers, nice hit there. Congrats, Emma. And to finish off we've got a Green Atomic that is going to be Simon Juan, 4.99 out of 9.99. Get the Juan. We need to rip some 22 Bowman where Warming Bernabell has his first. Oh yeah, there you go. He's going to Inventory to put 0. He's out, way to blow it. We've got Canary Yellow to 75, 40 out of 75, Junior Perez, nice secondary color match for the A's. There you go, Emma. We've got going to the Reds, Yerlan, Confidant on the Basado, there they're up. I forgot that they were watching this. They didn't even look enough. Had a heart attack. Somebody's life's over there. Cooper Bowman, nice one there for the Yankees. This is Anthony. I'm going to tell you, it just makes customers mad. I do, man. That's what I do. Trying to sleep, man. My main goal when I was hired is to try to try business away. That's what it is. I know. I can tell. You're doing a great job. You're doing a great job. Poor Anthony was asleep five minutes ago. Now look at him. Oh, this is big. Jumped out of bed. And a mag right here. This is actually kind of nasty. How about a true green Roderick Arias 89 out of 99? Boom. There we go. Congrats, ammo. Big time hit there, buddy. Big time hit. This is the lowest number of rice I've pulled. I might have pulled one gold. This is nice. The true green too. That's awesome, dude. Got a Tanner McDougal. That's going to the White Sox. True gold is going to be Dontha Williams 43 out of 50 going to the Orioles. Nice one there. Congrats on that one, ammo. There we go, buddy. That'll do it for the break, ammo. Thanks again as always for the support, my man. We'll get those right out to you, buddy.


Σό, ε panels of this paper here, there is that prove that indeed both modes are normalizable, So when the questions of whether both boundary conditions, I mean, we can import both boundary conditions in principle and the corresponding boundary terms so for keeping the charge fixed, which is the boundary condition that Samir was talking about, just corresponds to adding these les постоянно transform, but then you want to impose the other boundary condition then you need to add some different boundary terms και αυτό είναι συμβουλήθηκε σε αυτό το πέραμα, μετά με άλλες ασπέτρες της H2-χολογραφίας. Είδαμε να μιλήσουμε εδώ, ότι στις κόντεξες της χώρσης, στις κόντεξες της χώρσης της χώρσης, ουσιακώς, για αυτοί της H2-χολογιακής, έχετε ένα factor H2-χολογιακής, αλλά σε κάποιες φορές, η H2-χολογιακή έρχεται από ένα H3-χολογιακή. Προστασandaag, όταν έχετε ένα H2-χολογιακό και ένα H3-χολογιακό, η H2-χολογιακή έρχεται από ένα H3-χολογιακό και της στις κόντεξες της χώρσης. Στην μητέρα της χωρις, αν έτσι έχετε ένα H2-χολογιακό και δύσκολα, η H2-χολογιακό κόντεξας δίδει από την χώρσης της χώρσης. Ερθόνι, όλος στην ίδια υπαγέντι απολαμβάνει, υπαγείας της χώρσης εστέψεται τέτοις. ορίτε θα δοκιμήσεις η αδύναση της αδύνασης. Άρα είναι η λόγια κοινωνή ότι πρέπει να πιθαριστούν τα κοντά που η αδύναση είναι καλύτερη. Λοιπόν, αν έχεις ένα αδύναση της αδύνασης, δηλαδή στην ΒΤΖ, στην ΑΤΣ, και οι δυέντρες πιθανές πραγματάς που έχουν ένα αδύναση της αδύνασης, δηλαδή η αδύναση της αδύνασης δεν αντιμετώ σε τα κοντά, άτω σε τόση τη δηλαδή μπορεί να πιθάρεις και διεθνούνται τα πράγματα. Βέβαια, αυτή ήταν κάποιες πράγματα, και τώρα μπορούμε να συνεχίσουμε από όπου είμαστε τώρα. Ναι, δεν θα μιλήσω. Βέβαια. Βέβαια. Βέβαια. Βέβαια. Βέβαια. Βέβαια. Βέβαια. Βέβαια. Βέβαια. Βέβαια. Βέβαια. Βγέβαια. Βέβαια. Βысπη. Β Şί irritatingLOT. ΒΓΙΣ this layer. Βγέβαια. Βγέβαια. Βγέβαια. by this, so this is the canonical momentum, the radial canonical momentum, and this is the conjugate induced metric on the radial slice, and there was this important conclusion that like the radial derivative of the symplectic form, if the radial slice is compact, is independent, is zero. So then what we did was, so this was like the generic Hamiltonian formulation, so next what we did was like we constructed the space of asymptotically locally ADS solutions of Einstein-Hilbert gravity in this case, and then we found that there are two independent functions, so one was like this G0, which was completely arbitrary, and then there was like this Tij I defined that was proportional to Gd, that was like another sub-leading coefficient in the asymptotic expansion, plus some other terms here, and we saw that if you plug this asymptotic expansion into the symplectic form, you get a symplectic form of the space of solutions, so then this omega reduced to this G0 ij wedge delta pi d ij, and this pi d was just like this Tij, just it had like the volume element, right, and from there we constructed the, so from this symplectic form we constructed the Poisson bracket like for functions on this reduced phase space, which is given by this, so now if you remember, so that is the structure now of this reduced phase space, and this is characterized by these variables, and it's a symplectic manifold that has like this symplectic structure, this Poisson bracket, so now let us look like at symmetries, so remember like when we discussed the Hamiltonian formulation of gravity before going to the space of asymptotic solutions, we also discussed like the local symmetries, and we saw that we had like two constraints, the Hamiltonian and the momentum constraint, and through the Poisson bracket this generated like bulk diffeomorphisms, so here now there are also, there is another set of local symmetries, so remember when we wrote the solutions, the asymptotic solutions, we were working in the particular gates that was of this form, right, and then we wrote down the expansion for gamma ij, so it was like e to the 2r plus subleading terms, right, so these are very specific gates, we could have chosen any other gates that we want, this is kind of the standard canonical gates, and now there is a question, are there residual diffeomorphisms that preserve these particular gates, but of course they will act on the coefficients here of the asymptotic solutions, so these are like, if you impose this condition, so now we do infinitesimal diffeomorphism, so let's look at generic diffeomorphism, so that would be like the g parameterized by psi, so we want the r component to be zero, and also delta psi of gri to be equal to zero, right, I mean so that means like to preserve these gates, like these coefficients here, and the mixed one, so these two give us conditions like for the parameter psi, and the two conditions are psi r equals zero, and psi dot i by j equals zero, so these are like the two equations psi dot, the dot here again is the radial derivative, and the solution takes this form, I will call it PbH, so it stands like for Penrose-Brown-Heno, so these are standard result in gravity, so you get subleading terms, but the important thing is that we have like two, so this class of diffeomorphisms is parameterized by two, well one function and one transverse vector, which are completely arbitrary, so we have like this sigma of x, which is an arbitrary function of the boundary, and then this psi zero i which is an arbitrary vector filled on the boundary, so this is the general solution, and all the subleading terms are determined in terms of, so here there is nothing subleading, and here all the subleading terms are determined in terms of there is some sigma dependence here, so here it's like the sigma. Right, so now that we know the residual symmetries, so we can see how they act on the coefficients of the expansion, right, and then basically the only coefficients that we're interested in is like is the g0, which is independent, it's arbitrary, and then the other like arbitrary coefficient which is like gd, so now you can act, so let me write it here, so you can easily do the calculation explicitly, so what you find here is that this part here is just like the standard, it's a boundary diffeomorphism, while this part here is an infinitesimal vial transformation of the boundary metric, so from this we can deduce that psi0 just like corresponds to boundary diffeomorphisms, whereas this sigma induces a vial transformation of the boundary, so this is vial, and this is... Now the important question now is like how does the PBH act on the symplectic conjugate of this g0, and that's a little bit more complicated calculation, so let me write the answer, ix, i0k, so this is kind of a toy model, like I mean for gravity, and then like I mean, so in a moment I'm going to apply the same thing, but I'm going to derive like the supersymmetric, supersymmetric transformations on the boundary, like on a carried boundary, so just bear with me like I mean a few minutes, so here there is another important term, sorry, which one? The right answer, if you point your finger I'll tell you where, to the right, This is psi0, sorry. Right, and then here, right, so remember there was like this, so πd was again this proportion to Tij, and remember that Tij, the trace of Tij, it was given by this function g0 that I didn't specify because it depends on the particular dimension, but it's a local function of g0, and then it appears in this transformation here, so now if you compute the transformation under these PBA transformations of this coefficient here, you get these homogeneous terms, so homogeneous because all of them are proportional to the original quantity of this tensor, including this one, so this part plus this part means that like this πd transforms as a regular tensor under the corresponding transformation, but this part here corresponds to some anomalous transformation. Sorry? Under the table, after the A... Ah, it's a sigma, so it's proportional to this... I multiply this... Yeah, it's proportional to this, the same sigma as here. Right, and now the point is that, so maybe I don't write it explicitly, so you can show that these transformations, they follow from the Poisson bracket, so namely if you compute... So if you define this function here, so if you now define... So remember that was analogous to defining the constraints, like on this phase page that we did before in the Hamiltonian formulation, so now you can define again an analogous constraint, and this was like the two constraints that we got on TIJ, if you remember one was like this trace condition and the other one was like the covariant derivative of TIJ was equal to zero. So now we multiply these two conditions like with the corresponding, like just some arbitrary functions, and now you compute the Poisson bracket of this with G0, and you get the same PBH of G0 and similar for pi DIJ. So now the point is that like these transformations here, one way to compute them is using like this Poisson bracket that we defined earlier, and taking the commutator, the Poisson bracket with the constraints, these constraints. So computing this is very easy, just directly from the asymptotic expansion actually, just doing the morphism. In principle you can do the same for this coefficient, but you have to go very high up in the expansion, so this Poisson bracket calculation is much simpler to do and you get the correct answer. So now an important, you can also compute the algebra, psi0, σ, and then π, σ' and then you find that this again it closes, the algebra closes, but now the point is now the structure constants, I'm not going to write them explicitly, independent of the fields. So remember this is different from what happened like in the phase space formulation of the theory, because in that case the algebra closed also, but the structure constants were dependent on the fields themselves. So once we go to the reduced phase space, this doesn't happen anymore.  Okay, so no, these are not the ridgys symmetries, so that's where I'm going now. So now let's do an example. So now let's consider a generic two-dimensional conformal field theory and put it on a space with a metric g0, some arbitrary metric g0 and then we know that we have like these word densities. So the word densities are the two constraints that we have from before and then the trace of this stress tensor is given by the conformal anomaly, in this case it's c over 24 pi r of g0, so that's the rigid scalar, so that's like the standard word densities. So now you find that under local two-dimensional deformorphisms plus vile, first of all the metric transforms as we saw before and then you also get the transformation of the stress tensor which I'm not going to write the psi part plus here we get like a term, right. So here there's the standard term that, well you can see in the notes, so the notes are by the way already like on the website. So the stress tensor transforms as a proper tensor under deformorphisms, but under vile transformations like there is this anomalous term here, right, there is this inhomogeneous term. So now to define rigid symmetries like or killing symmetries in other way, so all we have to do is to set the transformation of the background metric, so we set the transformation of the background metric, this is g0, so this is the transformation of the psi0 and sigma, which is, we set it equal to zero. So that's the difference, like that's what defines global symmetry. So under these local symmetries there is no constraint on this transformation. So this is just the transformation under the local symmetries. Now imposing this condition here is the killing symmetry condition. So first of all this fix is that sigma is minus a half d0 psi0i. So the sigma is fixed in terms of psi0 for this case and then psi0 then is a conformal killing vector, right?  So in particular you can choose so choose like that ds, so the metric is just flat metric and choose holomorphic coordinates so this is dz, dz bar. So then you find the solutions is there are two arbitrary functions and then now you can use this transformation that we wrote down the general transformation here that we used under local symmetries. You can use it for this global symmetry transformation and then you find the standard expression for two dimensional CFTs where t is equal to t, dz and similar for the antiholomorphic coordinates. So from here you recognize this is the Schwarzian derivative and then from here by expanding it in Lorentz expansion you can you find that the modes satisfy the Virasoro algebra. So we see that now the structure of this reduced phase space for gravity like in the case of three dimensions precisely matches this phase space of two dimensional CFTs namely the space of coupling of the background metric and the corresponding stress tension. So that is a generic statement that you can make so that's like a reformulation of ADACFT if you want. So more generally the space of operators and couplings in the field theory is a symplectic manifold so you can see more like in the type lecture notes like on this point and so the symplectic form is we'll just tell the OIJI so a statement like of the ADACFT correspondence is that so this exists like for any local quantum field theory this symplectic manifold so a statement of the ADACFT correspondence is that the reduced phase space of asymptotic solutions in ADS is precisely identified with the symplectic manifold of renormalized operators and sources. So and these you can generalize to other contexts but it becomes more complicated like if you don't have a syndotically ADS. Sorry? Sure. Yeah so this I didn't talk now from here like I mean from the global symmetry now you can define the corresponding conserved charges and then on the space of the conserved charges then this for some bracket becomes the Dirac bracket and then you get the algebra of the charges. So that's one way to derive the Virasor algebra. I don't know if that was your question. One of the things suppose you don't put this condition delta G equals 0. Okay. Do those transformations still have interpretation in the boundary theory? Yeah so it's like toft anomalies right? I mean you put the C on field method. So when you put the field theory in the background like global would be global symmetries become gate symmetries. So these are precisely these symmetries. Okay. So the next half hour so I'm just going to make a few comments without writing explicitly much. So I'm just going to make some comments about boundary terms and then I suggest like I mean you can take a look in chapters 4 and 5 of the lecture notes if you want to read more about it. So here the idea is that like I discussed so far like this reduced phase space but then also in order to to renormalize the action we also need like to determine the corresponding boundary terms. And then the logic here is the following namely that like when you have like this asymptotically locally ADS spaces actually you don't have a hard boundary you have an asymptotic this is a conformal boundary and in practice mathematically this means that the bulk fields don't induce represent a particular metric like or fields like on the boundary but only a conformal class of metrics. So whenever you want to formulate the variational problem then you need to formulate in terms of this equivalence classes, these conformal classes. So in doing that you need in order to do that you need to add these boundary terms. So these boundary terms ensure that is a is a class is a is a variational problem on equivalence classes of under conformal transformations and you can show in general that this boundary term is minus a solution of the Hamilton Jacobi equation. So and there are algorithms to iteratively determine them. So again this algorithm is described in in subdetailing in the nodes. Okay, so in the next like half hour so I'm going to kind of repeat this story but for for supergravity. Equivalent class is like under so the class function is like two sigma, right? So it's basically like for any sigma. So what I keep fixed basically is like it's like this combination for arbitrary sigma. I don't demand that like g0 itself is kept fixed only the ray like I mean under my transmission is kept fixed. So if you demand that then you see that you have to add precisely the counter terms and this automatically ensures that actually the action is is finite. Yes. Yeah, all this analysis that I'm talking about here is asymptotic. So so basically you can apply everything I said here to the sitter. It's just like a double week rotation and then everything applies. So all that started is with ADS. I mean with the sitter is like global properties like I mean away from the boundary. So close to the boundary I mean everything I said applies. Okay, so it doesn't have to be conformally flat. You mean the boundary? The bulk? Well, no. I mean it depends like on the theory that you put on the boundary in the bulk, right? I mean so you need I mean it depends on the equations of motion that you solve. So you have to study like the asymptotic solutions of a given theory like in the manifold. Right. So let's see. So 4D N-quad 1 and 3D N-equal 2. Right. Okay. So now let's consider like the minimal gate supergravity in 5 or 4 dimensions. So I'm going to write it like with an arbitrary d here. So that's the bozonic part and then we have like fermionic parts. So here let me just write it schematically. So there's like an F nu there is gamma sigma and then here is nu. Right. So this is like minimal gate supergravity like in 5 dimensions. So here let me just put like delta d equal 4. So this term here the tensimost term only exists like in ADS 5. Right. So the spectrum is that we have like just the metric like a u1 gauge field and which is the gravity photon. So it's the gravity multiplet and then also a gravitino. So I should mention here that the way I wrote it is different from I think what appeared like in earlier lectures. So this time nu is Dirac and before we had like Majorana to Majorana simply Majorana fermions but in this formulation it's important to write in terms of Dirac fermions. Yes. You mean here? Yeah, that's lambda. Sorry. So that's lambda here. Thank you. Is that what? No, sorry. This is So this B is like in is the boundary dimension. Right. Okay. And then also there is like Gibbons hocking term which is a generalization of the pure gravity one. So now it gets contribution like also from the gravitino. So that's also necessary in order to formulate the theory. Sorry. The contraction here was a little bit sloppy. So if you want to make it right more precisely. So it's plus okay. So there is also like the super symmetry transformations. I'm not going to write them explicitly down. So now the first step here then is like the again the Hamiltonian and that's why it was important like to have this in the direct representation. So if you have it in the gravitino is in the direct representation then you can now formulate the Hamiltonian version of this theory but you need to project so to with this they're called radiality projectors. So this is the radial component. So this is the gamma matrix along the radial direction and then you have to decompose all the fermions in these two chiralities or radialities. So then we have like psi plus nu and psi minus nu and then this play the role of canonical momentum and coordinates. So because we have a first order action like for the fermions. So again the first right so like once we have the so from the Hamiltonian formulation what we can derive is the boundary terms which I'm not going to write down or explain how they are derived but we can also construct this reduced phase space reduced phase space which is the space of asymptotic solutions and then we have like for the field buying we have the analog of the this Pheferman-Greham expansions so this is in d equal 4 so that's like ads 5 and there are similar expressions like in for the ads 4 case so so this is the field buying so because we have fermions in the game now we need to trade the metric like for the field buying so we work like with the asymptotic expansions of the field buying so then there is the gates field and then let me just write like the expansions for the fermions and then so the point is that now this this term here so the story for the metric for the field buying is very similar to what I said before for gravity now for the for the gravitino here this this is an independent function here and it plays the role of the source of the dual operator and here this this term here corresponds to the dual dual momentum then this is like a source so like the different the intermediate coefficients here like they are all written like in the paper so the kind of lengthy expressions but the point is that again there are like this arbitrary coefficients here this and this and then also for the fermions and also for the gates field that I didn't write down so this now parameterize the space of asymptotic solutions this reduced phase space and again like the whole thing in here is like a symplectic structure from this generic Hamiltonian analysis of the theory so you can build the symplectic structure and the corresponding Poisson bracket so now we can define the operators so the operators are going to be related to this other mode so we identify this and this like as the sources and also for the gates field and then for the fermions like this and also this for the metric here now these modes have become proportional related to the one point functions but the one point functions have to be derived the counter terms so so we have a stress tensor here we have the R current which is given by the momentum of the gates field and then also we have the super current which is the operator conjugate to this source here ok and now these counter terms here I haven't I haven't shown you explicitly so they are in the paper they are pretty lengthy and they can be computed systematically but once you have these counter terms now and also the corresponding canonical momentum you can evaluate these limits and to leading order like this will go like ED and etc. all for the other modes so they will go like as the symplectic conjugates of the sources basically like this one point functions but they are the correct covariant one point functions so the counter terms you have to solve the Hamilton Jacob equation so this I didn't have time to go through in detail so there is a system multi algorithm also the finite counter terms yeah the finite counter terms also you can classify so they have to be like super conformal invariants and then there is a limited number of such local densities that you can construct but they are all constructed in the paper so if you are interested you can have a look but indeed like the whole all the possibilities like for the counter terms are there no the counter terms are unique right so there is nothing else that you can write so like if you solve the Jacob equation you will get like a unique answer so all the divergent terms they have a unique answer always which in this theory they are complicated so the only ambiguity is in the finite counter terms which is like in the coefficients of the super conformal invariants so anything else you write I mean it will not lead to the correct variation a problem so it's not that I mean you can write anything that I mean maybe it works like for some particular solution but I mean the counter terms have to work for all the possible solutions I mean to get the right structure are there any questions ok so so now once we have these operators so here when when I wrote the asymptotic expansions I didn't say about the constraints that actually this normalizable mode satisfy but as in the case of pure gravity they satisfy some constraints which will come out like automatically from this asymptotic analysis and also the Hamiltonian analysis so in other ways usually the constraints that you get like I mean now on this they come precisely from the constraints in the Hamiltonian formulation there is one to one correspondence so that's the most efficient way to determine these constraints so and as we saw in the example of two dimensional CFT these constraints now on these one point functions they become like the word dentist so and then here I'm not going to write so you have like you have bosonic and then you also have two fermionic word identities so let me write the terms plus j here and well there is some gammas times I'm writing a little bit schematically and then there is also the gamma trace identity which is of this form so here we have like the divergence of the super current and then there are other terms evolving the stress tensor and the r current and here also is the gamma trace of the super current and here the u1 current so on the right hand side however we have like these terms which are local so these terms are local in the sources so I'm not going to write them explicitly down so they are like similar to the to the conformal normal to the trace anomaly like in the two dimensional CFT they are expressed in terms of curvatures so they depend like on the Ricci curvature of the background metric and also the field strength of the r of the r current background good so so as we saw before like the fact that we have this this word dentist is a reflection of some local symmetries which can be generated again through the Poisson bracket so in this case so in quotes because it's a generalization of that so again we look for symmetries preserving the gates so in the gates in this case that I'm preserving is expressed in terms of the field bind psi r is equal 0 and then here we have two constraints here so it's psi plus and minus so these are the constraints that we sorry these are the gates that we preserve and then this leads to a set of local symmetries so and the local symmetries are again like the this Penrose-Brown-Henna diffeomorphisms but now we have more more transformations so we have like local Lorentz transformations so all of them have subleading terms here and then there is like u1 transformations and finally we have the supersymmetry transformations so these go like plus or minus r over 2l epsilon 0 plus or minus x plus all subleading terms that depend again on this parameter so the subleading terms do not introduce extra parameters so the important thing here now is that we have like two independent local spinors spinors here they correspond like to local symmetries and then epsilon plus is the q-suzi epsilon minus is the s-suzi and through the local so they are generated through the Poisson bracket basically they are generated so this word identity generates the epsilon plus transformations and this word identity generates the epsilon minus transformations so you can do explicitly so you can check explicitly the transformation of the sources under these residual transformations and what you will find is precisely the supersymmetry transformations well including like the theomorphisms and local Lorentz etc but like under these parameters here what you will find is precisely the local supersymmetry supergravity transformations on the background and the boundary so this would be like precisely like the off-cell n-qual one conformal supergravity like in living on the boundary so the supersymmetry the supergravity transformations like for the sources like under these epsilon plus and epsilon minus they are the standard ones however so I'll just write those in the stop so using the Poisson bracket we can compute the epsilon plus transformation of s-i so this is given by the let me write this schematically by this word identity Poisson bracket with s-i and what we find from this is this expression and then there is a lengthier expression for epsilon minus so now for epsilon minus is the same thing but here we take the the word identity corresponding to the gamma trace of s so with epsilon minus and then again s-i Poisson bracket and again there are a few terms so first we get this last year we get epsilon minus and then finally we get one more term which is i-k good ok so that was the final transformations and these transformations now actually they are the transformations like of the of the super current operator under supersymmetry like under q supersymmetry here and under s supersymmetry but they are local transformations however they are not the classical transformations that you would find just by doing the calculation like on background super gravity so here because we do the calculation holographically remember in the Gordon is a tie road like two anomaly terms on the right hand side that I didn't explicitly write down but like in the two-dimensional case where we saw there was like this conform anomaly this contributes this anomaly contributes to the transformation of the operator so in the you contribute to the transformation of the stress tensor in the two-dimensional CFT example that's why we got the spartzen derivative and then in this case we get again some contribution from these anomalies and these contributions we can easily figure out but this term here is proportional to the stress tensor so that's an operator and then this term here is also an operator but this term here so this term here is a local expression in terms of the background of the asymmetry background so that represents a kind of an anomaly and then similarly here so this term here so again this is a local term and also this is a local term and also this is a local term so here all the terms apart from the first one they are local anomalies so the point is that the supercurrent has an anomalous transformation under local supergravity transformations on this rigid supergravity background so now if you look at the if you try to find like killing symmetries so that would correspond to imposing the transformation of the source being zero so we would have like the transformation of this psi zero plus equal to zero which is like the epsilon plus minus gamma epsilon minus so now like in the case of the conformal killing spinors we would have to define like killing spinors in this case we have to set this to zero but it gives us like this is the conformal killing spinor equation so from here you can find the corresponding killing spinors but for generic curved background the spinors that satisfy this equation they have non zero both epsilon plus and epsilon minus so then you can plug it into the corresponding transformation of the supercurrent here and then you will see that the transformation under this rigid supersymmetry now that corresponds to the conformal killing vector would get anomalous contributions both from here and from all these terms here so this means that in principle supersymmetry like depending on the background supersymmetry might have like this anomalous transformation here when you put it on the curved background that admits like conformal killing spinors so even though like classically supersymmetry is preserved so I will stop here


Remember a hallmark card when you care enough to send the very best Tonight from Hollywood the makers of hallmark greeting cards bring you miss Rosalyn Russell in Louis Brumfields Mrs. Parkington on the hallmark playhouse Each week hallmark will bring you Hollywood's greatest stars in outstanding stories chosen by one of the world's best-known authors They distinguish novelist mr. James Hilton Good evening ladies and gentlemen, this is James Hilton tonight on our hallmark playhouse We are delighted to present a dramatization of a well-known story by one of America's best and most popular writers Louis Brumfield Mr. Brumfield who won the Pulitzer prize for one of his novels is many things besides the writer He's widely traveled. I remember I first met him at a party in London And he's also a farmer whose land in Ohio has become famous not only because of the books He has written about it, but because of the excellence of its methods and produce a good writer and a good farmer quite a combination that The story of mr. Brumfields that we have chosen for tonight is mrs. Parkington And we're especially privileged to have starring in it one of Hollywood's most famous actresses Rosalyn Russell But before we raise the curtain here is Frank gas who has a brief message from hallmark For a Christmas greeting your friends will long remember make your selections now from the complete hallmark collection On display at the friendly store where you buy hallmark cards Whatever your taste whatever your budget you'll take special pride in sending hallmark cards And on the back of everyone is the identifying hallmark that says you cared enough to send the very best Hallmark playhouse starring Russell in Russell in Louis Brumfields mrs. Parkington face records The past where you are always young is only a memory away Leaping Rock, Nevada is 67 years back into time for me But I have only to close my eyes to be that age again To live those hours over I have only to close my eyes to see my mother shutting the kitchen door and leaning warily against it. I Have only to close my eyes to see major Parkington our star border from New York Coming in the kitchen door He had on a silk shirt and a purple cravat and a checkered waistcoat and a diamond pin and a diamond ring and A gold Watson chain He'd sit there straddling a chair while we cooked dinner. I'd tell you your love New York Susie It's color noise excitement adventure. It's the Arabian nights. It's poetry. It's music. It's Delmonico's It's dancing it's laughter. It's enchantment the city for the young Susie a challenging fabulous city Belongs to anyone who can conquer it It's at the moment when I sat in the kitchen Telling him about New York and told me about it when I fell in love with him that moment It was a child Was it in that dark hour after my mother and father died in the mine explosion? When he tried to shut out all pain of loss and death, but I first loved him That hour he was a father Or did I wait to fall completely in love that snowy wedding night? When he carried me across the threshold of the Brevard Hotel You're happy Susie it is like the Arabian nights Red velvet curtains and white roses and candlelight. No Susie. You're so young and so lovely Across the room I saw my husband eyeing me over a coffee cup Get up and have some breakfast sleepyhead. I certainly will How did that breakfast get in here without waking me up came by magic? I waved my hand there it was I'm so hungry. Yeah, have some coffee. I sent a note to a friend of mine asking you to come and take you on a shopping expedition today Huh, uh-huh a spazier Conti. She's a French woman who knows more about everything than any woman has a right to know about anything She'll help you in a lot of ways Help me Susie darling I'm a very rich man, but while money can buy a lot it can't buy everything New York is a tough place. I'll have to fight for what we want I've always had to fight. I don't mind for myself. I want to make it easy for you There must be a spacey Susie this is mademoiselle Conti mademoiselle. This is my wife I'm very happy to know you mademoiselle Conti It is a pleasure to meet the wife of my very good friend major Parkington She is much more beautiful than you deserve Gus I want you to take her out and buy her the most fashionable things in the city Because tonight I'm gonna show Susie, New York, and I'm gonna show New York Mrs. Parkington It was all he said it would be music and laughter poetry and waltzes Winter melted into spring and my life was at its spring time too And when I learned that I was going to have a child it seemed to me I had reached the fullest happiness that can come to any woman. I began to wish then That we could leave the hotel and find a small cottage somewhere outside the city. I told Gus and that afternoon He drove a spacey and me down to 34th Street. We are Susie. No careful now I'm all right girls. Well, I don't believe I know anyone at this address What is it a hotel? How does it strike you as a cottage? A cottage? It strikes me as being just about what would strike you as being a cottage I'm not so sure about Susie. I bought this today as a surprise for you Susie You may not believe it, but this house has 30 rooms 30 rooms for two people. Don't forget. There's gonna be three of us pretty soon Even so we don't need 10 rooms a piece here. Look at this door solid mahogany Never seen so chandeliers. Oh Gus the gas bills are going to be ferocious See that staircase marble every inch of it. You like it Susie Like it. Oh Gus, it's a palace. I knew you'd love it. Come on. Let me show you the rest of it. Here's the ballroom What a room for a party and I'm giving a party in three weeks I'm gonna have the cream of New York society. Oh, it's time. We launched ourselves. We've got the house We've got the money the spacey a you can help me with a guest list and Susie You'll stand right there by that window in a white satin gown There'll be flowers everywhere and music playing and the best people in New York bowing before you Later, I stood in that ballroom in my white satin With Gus and a spacey a facing an empty room There was a Dresden Shepherd and shepherds on the mantle behind us and Suddenly Gus picked up the shepherd and hurled it across the empty ball Oh God, how could you have could you so they didn't come they'll pay for this every last one of them Up to bed Gus the evening is bad enough for her without you shouting and carrying on like that. It doesn't matter It doesn't matter that no one came I'm just so tired. You had better carry her upstairs. No, no, I'll be all right up I'll be all Susie Susie carry her upstairs to bed. I will send one of the men for the doctor So tired I know why don't you go out doors and walk? I'll pay them back if it takes every set I've got Hadn't been for those snobs. I might have had a son today And you wouldn't be lying there with all that pain behind you or nothing to show for it Probably have happened Dirty rotten snobs Susie, I swear to you. I'll pay every one of them back There was nothing I could say or anyone else could say that would ever change him I Forgot about the episode as the months and in the years went by and Herbert and Elliot and Alice were born And it wasn't until long ago Much later than that that I found out that he'd been getting his revenge That was an hour when I feared him almost hated him an Hour when I met a completely new major Parkington Gus. Have you seen the newspaper? Prominent financier commits suicide Radna Beaumont dies. Yes, I saw it He was one of the people you invited to the party wasn't he yes According to the papers he was facing bankruptcy It can be very dangerous to refuse an invitation to a party you give cut it very Good you Blair's cousin was here. She begged me as a favor to ask you not to ruin her cousin She said he would kill himself.  He hasn't the guts. I'll try to explain it to you Those same men would have ruined me just as ruthlessly. They were trying to do it, but they weren't strong enough I Can tell you one thing If they had I wouldn't have hanged myself in a cupboard. I'd have gone back to work and made another fortune Was an ambitious man Ambitious for himself ambitious for his wife Ambitious for his children They went to the best schools dressed like royalty and had everything money could buy I Tried to keep him from giving them too much But he was determined they should have all the things that neither of us had in our childhood And they certainly did and so it happened when our daughter Ellis was still too young to know what she wanted She decided to marry a French Duke Espasier I know this marriage is wrong. Do you realize that Gus is settling a hundred thousand dollars a year on the Duke? I cannot sanction a marriage like that. You may be right, but it is too late for that Or let her marry him Susie if she does not marry the Duke it it would be another like him She is doomed Why do you say that? It is the same with her brothers their father has implanted in them a sense of being possessed of some special privilege of being outside the rules which govern the conduct of ordinary people So Alice will marry Not for love, but for a title and there is nothing you can do about it Espasier I'm so afraid you're right Would you like to send a personally imprinted Christmas card this Christmas so unusual your friends will show up to all who visit them during the Holiday season and then see the new hallmark creations at the friendly store where you buy hallmark cards There are five distinctive types of hallmark cards for imprinting with your name each designed as only hallmark craftsmen can design them There are hallmark cards with beautiful designs and silken tapestries Richly engraved formal cards and cards that speak a man's language with sporting scenes by Edwin McGargy Lynn Bogue hunt Lacel Ripley There's the hallmark blue book with sophisticated designs and surprise features and there's the hallmark gallery artist series Open the hallmark album at any page and what a treasure lies before you quaint winter scenes by Grandma Moses Delightful Christmas scenes by Norman Rockwell here, too You'll find Salvador Dali Marcel Vertez Cezanne Renoir go get money Van Gogh Yes, more than 50 foremost artists contribute their genius to the hallmark gallery artist collection Personal Christmas cards on which you will be proud to have your name imprinted Remember these are hallmark cards when friends receive them and look on the back as you did They'll see the hallmark and know you cared enough to send the very best And now we continue with part two of Louis Brumfields Mrs. Parkington Starring Rosalind Russell close my eyes to enter the past randomly Three years after Alice's marriage was a summer. I shall always look back on It's the most terrible summer of my life My son Herbert was killed in June in an automobile accident leaving a widow and two small children and In August came a letter from Alice saying her marriage was unbearable and impossible She wanted a divorce a Spacey and I left for Paris immediately and when we arrived there we learned that the Duke was contesting the divorce This was obviously a move to extract blackmail money So I decided to match the Duke at his own game. I Hired detectives got a complete file on the Duke's past and present activities and then arranged a meeting He was as charming as ever Mrs. Parkington your lovelier than even my memories of you. Thank you Jacques. You needn't be flattering This is hardly a friendly meeting. I Understand that you have treated Alice abominably and that you have absented yourself from home for weeks at a time It is all quite true But from the beginning it was complete misery to live with her nothing is worth that Jack Understand this there isn't going to be any more money.  It would be more foolish to say no an Exposure of that little episode in your life would drag in the names of other important people you need not continue I'm forced to say that your investigators are remarkably good My lawyer and yours will get together. I will not contest the divorce I've missed you a spacey. I love you. You look grand Alice darling. It's good to see I've arranged a wonderful summer for you You'll soon forget all this business. Oh, it's so good to have my family home again Suzy let me tell you about that when we get home.  There's nothing that can be done now, but to kill himself. Why? Why we don't know that he killed himself. It happened in Denver. The gun may have been discharged accidentally Get out of this house Suzy. I have to go for a while Can't bear this house.    We're choking smothering strangling in money. Can't you see that? Haven't been for the money Herbert wouldn't have had money to buy a car Alice wouldn't have married that fortune hunter Eddie wouldn't have had everything and been tired of it before he was 25 I hate the money and I hate this house. I Wanted you and my children to have everything I Wanted to find a dynasty where you founded your dynasty. I hope you're proud of it. I Remember thinking I'm a surely died brief and bitterness But the heart has a way of reconciling itself and going on Just as Gus had said New York was there to conquer or to be conquered So it is with life if you've read blood in your veins you conquer life and go on And only when you're long past the hours of trial Do you discover that what you conquered each time was yourself? Knowing this I was able to go on When the major died Suzy you have been wonderful. I know the funeral and all was a great trial to you It was a great sorrow for you to aspatia. I Know that Gus might have married you if it hadn't been for that explosion in a leaping rock No, Suzy Gus Parkington was in love with youth And I have been old from the hour of my birth just as you have been young He he was a splendid man. He was a happy man. I Think people are really happy in proportion to how much they give He wasn't always a good man But he gave a great deal He gave a great deal more than he took one of us Leaping rocks is 67 years back into time 67 years from the moment when the major first told me about New York To the moment when my granddaughter's husband Amory walked into my sitting room on Christmas Eve The whole family was gathered downstairs for a Christmas dinner And I was just about to go down when he came in Hello there granny Merry Christmas. Merry Christmas. Amory. I hate to bother you before the Christmas dinner, but it is rather important How much do you need this time Amory? $750,000 $750,000 That's the amount I've stolen I took funds I had access to that weren't mine to invest. I thought I had a sure thing and that I could put the money back Why Amory? Why Amory? You had plenty of money. You knew there was more much more in the background You only had to wait until I died. I wanted to make more money. I wanted to be successful If I give you this money Will that stop the whole thing? I hope so. It's just a matter of putting it back now And if I don't give it to you, I shall have to stand trial She's getting cross about it. Come Amory. Let's go down I'll think this over and let you know my decision before you leave tonight I sat at the dinner table looking around at the faces of gusses and my descendants and Suddenly I knew with a cold sense of defeat that not one of those faces was a happy one And I remembered Alice's face when she was young and Herbits and I knew that they had not been happy either But Gus and I had been happy and suddenly realizing that I knew what I had to do Quiet everybody quiet, please grandmother has the floor a Merry Christmas to you all. I think perhaps I had better say that first Because I don't know how Mary you're going to think it is when I finish first of all Amory is in trouble that calls for some financial assistance, which I am going to give him Thank you. Thank you.  He had no control over the era that preceded him. I Think now he has learned a lesson But something must be done about him and about you So for all of you when I die a Small trust fund will be set up the income from which will pay your rent and food and very little else If you want anything else, I very much hope you will go out and earn it Well, I hardly thought it would be pleased but grandmother the rest of the money It's going back Where it came from you mean a memorial for the major no indeed I'm not interested in creating a legend at this late date that Gus was a great man Gus did a lot of good. Most of it was done accidentally. I stayed married to him all these years Because he was a scamp on a gigantic scale and because he was fascinating And because I was in love with him Right up to the end. I was kind of Gus's Gun now when you come right down to it No The money is going to things like hospitals and settlements and libraries And now let's get on with this party because tomorrow I am going on a trip And I want to be good and rested to go on it. Where are you going granny? I am going back to leaping rock Nevada And so I went back to finish the days In the land where I had begun them And now I was content with a hot sleepy slowness of the days For I knew what lay beyond the mountains What do York and most of the rest of the world was like And I knew that here was what all the rest of the world was seeking Simplicity and a sense of freedom and well-being and Happiness of spirit It had been there all the time But it had taken me 67 years James Hilton and Rosalyn Russell will return But first may I invite you again to see the new hallmark Christmas cards now on display at your friendly hallmark dealers If you prefer to select cards to individually fit each one on your list You'll find a hallmark card that says just what you want to say the way you want to say it There are hallmark albums from which to select cards for imprinting with your name and there are the many boxes of assorted Hallmark cards. Yes, whatever your taste whatever your budget there are hallmark cards You take special pride in sending and when your friends receive them and look on the back as you did They'll see the hallmark and know you cared enough to send the very best Now here again is James Hilton. Miss Rosalyn Russell I want you to know how much we've enjoyed having you here with us tonight For all of us here and for every member of the hallmark family our grateful. Thanks for a great performance I never know quite how to respond to introductions or words of appreciation. I Guess like your hallmark greeting cards. The best practice is simply to say The appropriate and the sincere thing So thank you. It was a great pleasure to be here We shall inscribe your name on our roll of honoured guests and we invite you to listen next week when we shall present Oh Halloran's luck by Stephen Vincent Bernay and starring Edmund O'Brien Ladies and gentlemen in the workshop behind our hallmark playhouse. It's Christmas. Oh, no, we are not exchanging gifts yet But we've been doing a lot of thinking about Christmas about the hallmark Christmas radio program We've already made our selection and I won't tell you what it is. I'm merely using it as an illustration of how far ahead we work Long before you hear a story on the air. We've been through libraries and bookshelves reading making notes and discussing dramatic possibilities We try to select the kind of person the author had in mind when he created the character and Therefore we try to visualize the particular star who will fit the leading role It's a long careful process, but I'd rather think we've been successful if your comments are any gauge We like to hear from you as a matter of fact. I'd like to hear from you about stories You're especially fond of it might help me and all of us in making the hallmark shows your best entertainment So if you'd care to write to me and I'd welcome that just address James Hilton care of hallmark playhouse Columbia Broadcasting System, Hollywood, California. And now until next Thursday. This is James Hilton saying good night Tonight story was adapted for radio by Gene Holloway with music composed and conducted by Lynn Murray our director producer as D Engelback Rosalyn Russell is currently starred in the independent artist production of Elvett touch Look for hallmark cards that are sold only in stores that have been carefully selected to give you expert and friendly service Hallmark cards when you carry enough to send the very best This is Frank Goss saying good night to you all until next week at the same time when James Hilton returns to present Steven Vincent Benazo Halloran's luck starring Edmund O'Brien in the following week Claude Jarman, Jr. In Mario Harris my friend clicker this program came to you from the hallmark playhouse. This is CDS the Columbia Broadcasting System