Od行了 school I would like to,</ural organizer for inviting me for this meeting. Of course, I know Boris for a long time, but I never born in solid state physics and I think my talk will be the only one where in no experiments and even no proposal for experiments. But of course with cold atom one can do everything you want. v prinspeciju, da je posobil, da imetite nekaj modelov, kaj sem bilo diskussi. Tako, nekaj, da se diskussi in nekaj, da se diskussi, nekaj toj modelov nekaj spektrali statističnih. Toj modelov je, da je zašličnje v analitivnih kakulacijnih, ali nekaj strančnih, zato videli, da je to veliko in nekaj nezavršen behavior. Tako, nekaj, da vse pravimo, je zašličen. Zelo sem počučen, da sem počučen, da sem počučen. Zelo sem počučen, da sem počučen, da sem počučen, da sem počučen, da sem počučen, da sem počučen. je po težko težko prirodila, da sem jezobimila, zato je več karakteristika tukaj, ali vseč jaz ni najsimolji to imač, kako sem je mare iz vzelo obstuknje modela, ko mi ljube vseč ponenjo delno, in da tak samo naživamo vsečnje halliteti. Na daj model, ko je vzelo obstuknje map, pride ga važno izolit, ali sem ga da pokazala, da je ne musela dobro uživila vse delovosti vsega vsega vsega vsega vsega ini vsega metri, ko je mu zelo vsega laks metri. Vse sem pa tudi daj poštaj, na koncluziju. Vsega, dobro taj sreč, vsega vsega vsega, ne bo vsega ini vsega, ratistiki, ki so imate v mene, da barriersi, že tu imaš jeljavih translatev e1, e2, en plus 1. Zatenje tudi hospitalsiificación , energijskel, spetrem v tisliči 3D-ključjev tako ga najbolj napravite, nekaj zelo početno. Zelo početno n, kaj je n plus 1 minus en. E g. Zato početno zelo početno zelo početno. Zelo početno zelo početno e plus 1 minus e. Zelo početno zelo početno. 건 se, da je početno zelo početno zelo početno. Da je to bil doličivo disloc diagn맛, zelo početno. E dotatno visk. Plast je n gauge. Osve ownership tra nak plenty peh v sebe musiquewasser. câmera. Illajko, 85 dall 110. kako se pokazate. Če bo tukaj, da se razmah je kajne 7,8,4,4. Nesakaj ne je zelo, da sem tukaj, da je 6,8,4,4,4. Svoje to nekaj, da se zelo, da sem priliv, ki se jaz zelo, da je zelo, da je nekaj, da je zelo, da je nekaj, da je nekaj, da je nekaj, da je nekaj, da je nekaj, da je nekaj, ne nekaj, ki se občaj. In je to izgleda, da je tudi vse tako je. In, da je ovo to nekaj, izgleda je, da je početno vse z Bernoulli procesov, da je E-Piro-S. In za to, da je početno vse početno vse početno, da je početno vse početno. Početno početno početno vse početno, da je nekaj početno. But everybody believes that for intergable system, generic intergable system, spectral statistics, statistical energy level will be pro sonjo statics. On the other hand, if your billiard is chaotic, for example, that shape of the study room, and you do the same story, you will see that you'll get something else. You will get function, which is zero at the origin, it has exponential squared, squared table. Vzelo, Cathedral was the final function. It means that if you use random, standard random matrix, you can computeộibed with the resolution of the equations but it's completely the different behavior. My talk is about dynamical system,ils with neither Poisonian nor Karotic. Kaj je tukaj idej, od numerika, od odpravdu, je to ozvodno 3-dimensionala Andersen model. So, if you have a Andersen model, you have disorder and you have jump and disorder in some say box disorders, and you know very well that if disorder is very large, all states are localized. But if disorder is less than special value, pa se počekljili v nekaj poživnih posobilitvacjah. V centre delozirati spetrumov, v tem delozirati je. Nakaj, odrešal, in je valja, če je tudi metalozirati transicije, da je dobro tako ko se posobila. Zato, da je vse nekaj nekaj najznim za vzbim, in da je, ki se zelo, načešča, a imaš uživljana korakli. Tako, to ne so vzelo. To je ne vrvi numeriči. Vrvi numeriči ne zelo konvensite, ali, da ustavljate, na tudi, vzelo vzelo vzelo vzelo v zelo. Marko, da bomo počkati vzelo vredovati.  Ako je naredil, zelo je vseško pravno, da je posao, da ima nekaj nekaj behavior. Če pa je nekaj behavior karakterizena, pri lukovaj repušenosti, kako je, nekaj početne, na početnih vseh rejdenah, in tudi naživljenjijo delovih, If you compute number variance, what it means, you count how many labels exist in the interval of length l and you normalize it as I do it before, that mean value of labels corresponding to n of l, mean value equal l, and then you compute variance of this one. It's one more exercise objavljanje pernuli počkaj, neč prišlično. Nombu vrarnosti. To je nombu vrarnosti, včoč jazi nombu vrarnosti razbenju sev posnešljenih interval, kaj jazi nekaj režim, če se počkaj v zepetru in jazi nije nožno v random. V zepetru neč krati neč nekaj rešimi vrarnosti. občas, kaj je spetrelja kompresibilit, kot je 1 for Poisson, and 0 for random matrix. For all non-trivial Maeman-type statistics, you will see that K is some non-trivial number between 0 and 1. Another property of all this model, which I will discuss, it is that wave function are multi-fractal. But it means that if you compute psi squared, power to q, and you compute mean value, then it's scaled as a v is a volume size to the power q minus one dq in dq called fractal dimensions. It's easy to see that if you have localized state, you have only one element of c large or other small, so dq is equal to zero. If you have random matrix, they are all of the same order and due to normalizations, each of them is one over n. So, you do dq equal one for random matrix. For all model, which you will see, this quantity unknown trivial. So, what is known and what is well investigated? So, once more, if you have, what will be the random matrix model of this behavior? It's well known that if you have integral models, they are like diagonal matrices. Each may diagonal matrix, independent variables, and you get integral model. If you have random matrices, all elements roughly speaking of the same order, each e is interacting with all other. So, it was natural to consider matrices of the form e minus g power alpha. So, when alpha is small, it means that you can ignore that it looks like a constant. So, it should be close to random matrix theory. If alpha is large, it should be close to pass rule. And this also was, have been proved by Levitov, and actually Levitov, that when alpha equal one, you have a special type of statistics, the critical statistics. Standard model of critical statistics is what is called critical power low banded matrices. It's a random Gaussian variables, independent variables, but the variance is not a constant, but decaying like e minus g power one, if it's square root of h, each element is the decaying. So, when b equal infinity, it means that all of them are the same, and you get random matrix, if b equal to zero, you get both. What is known for this standard model? One can construct perturbation theory. For both, b equal much bigger than one, and b much less than one. For the large b, you use heavily sigma model, and I don't know how to do it without sigma model, but for small b, you do perturbation theory, and you get easily some confirmations that key is non-trivial, and fractal dimensions are non-trivial in the both limit. What is interesting symmetry relation, which has been derived, proposed by Mirlin in company, that if you compute, not dq, but if you compute this combination, then this combination is symmetric with respect to q to one minus q. So, main question, which I start, is as there are dynamical models with intermediate statistics. You remember that if system is integrable, statistics is Poissonian, if it's Karotik, it's random matrix. But there are another type of models, which are really mentioned. It's called Pseuda integrable models. Pseuda integrable, simplest example of pseudo integrable models is a plane billiard, where all angles are rational of pi. So, all angles of this polygon should be rational of pi in order that it will be pseudo integrable model. For example, you can have rectangular billiard with some part in it, or you can have triangular billiard with angle pi over n. For all this system, it is proved that trajectory are living, they are living on the higher genus surface. So, the genus of the surface should be compute by this formula. So, when all m e is one, it's the only case. Genus is wall, so it's integrable system. All integrable system trajectory are living on the torus, and torus is the surface of genus wall. For Karotik system, all trajectory are living or cova uniformly high dimensional energy surface, and so there is no two dimensional surfaces in the game. For example, if you use triangle pi over 4, pi over 4, pi over 2, or pi over 6, pi over 3, then it's right triangle that genus 1 is integrable, but if you do pi over 5, pi over 8, or something else, you will see that they are not because the genus don't corresponds to integrable model. So, what is the classical dynamics of this to the integrable model? It's also well established that it corresponds to what is called interval exchange map. For example, let me consider pi over 8 triangle. Instead of continuation, you will consider reflection in the sides, and you will have a hexagon, and you should identify parallel parts of this hexagon. So, all classical mechanics of trajectory in pi over 8 triangle corresponds to this, and you see immediately that it genus 2 surfaces, because you have four independent contours for this. But if you look more carefully, you will see that you can split it in four different parts, and all trajectories, say, from 0, 1 will go to 4, 5 region, from 1, 2 they go 5, 6, and so on. So, classical map for these trajectories.  It's called interval exchange map, because you easily see that all information of trajectory are hidden in the permutation of interval. You have 0, 1, 1, 2, 3, 4 interval, and you just permuted it in the special man. It's all known that this system is neither integrable nor chaotic, and they have name through the integrable system. And it's even classical, as they are quite non-trivial, because you see that here classical mechanics lead to explicit discontinuity. So, if you iterate for a long time, you should be sure in what part of the discontinuity you are. It's a quite heavy talk, heavy method which permits you to do much higher numerics than usual. But what is about quantum mechanics? So, up to now, I take pi over n triangles, for example pi over 5 triangles, and somebody did calculation, and you see you have 10,000 levels, which you split in four equal parts. And if low energy part, here you have three curves. This curve is a random matrix prediction. I start it, it's not p of s, integrated p of s. It's much more sensitive to the small details, and for numerics it's much more useful, and much more sensitive to use, not p of s. P of s depends of the bin. N of s, they just count how many s is less than a fixed value. It's much more easy and much more stable to do n of s. So, it's random matrix prediction, it's Poisson prediction, and in between is something which is called semi Poisson, which I will discuss slightly later. It has label repulsion at small, and exponential tails in the large. And everything here, you can compute correlation function analytically. And you see that with increasing of energy, you might nicely go to the prediction to something else. What? You go to something else than it was before. And this is the same story, but for all triangles from 5 to 30, and there's a difference between semi Poisson, which is just a mark. And all triangles, we see clearly, this it will be a random matrix prediction. And all triangles are quite far, they depend of n. And here you have 20,000 labels, so it's quite a good statistics. So, what can be done analytically? Analytically, one can compute only the compressibility. Compressibility, if you compute it carefully through periodic orbits of these triangles, you will have some explicit formula of like this. So, the formula is very simple. It is heavy, mathematics is hidden in it, because to compute periodic orbits is possible only for what is called which triangle, where you have a which group in it. If somebody interesting, I can discuss, but if the triangle is pseudo integral, but not belong to this subgroup of all triangles, I don't know to do, because even the number of periodic orbits is not known explicitly. It's not only the bound, but it can oscillate it to all usines. It's just a consequence of very complicated character of classical mechanics for this simply looking system. You can do another system, and if you do the computation, you will see that for this value 5, 8, 10 and 12, k of zero is close to the value one half, which was predicted to Poisson. To predicted to semi Poisson, you can find small details, it's not important. This is a correlation function, correlation for a factor as numerically computed, and this value corresponds to this guy. Another model, which you also can belong to this same class, so mechanics is different, is a run of bomb flux line. You can put flux line in the rectangular billiard, and you will see that spectral statistics becomes from Poisson, becomes of intermediate tape. It has a level repulsion, and it has exponential tail numerically, and you can also compute through periodic orbits calculation some value for a factor of zero, just to confirm analytically strange character or intermediate character of this model. You can do of course calculation for circular billiard, whatever you wish, and I will not spend time for this. What is the difficulty of treating this model quantum mechanically? Look, if you have classical reflection of the half plane, for example, you have here the region, you have in this red point, you have two light, light coming, a light reflected. In this region you only one light, and here you have no classical light. So classical mechanics always for pseudo integral system is discontinuous. Quantum mechanics cannot have discontinuity, so it produces some complicated expression close to this line, which is called optical boundaries, and you also know that if you consider, say, a reflection of the wedge, of the electric wedge, then you have this formula and you see that exactly on this direction you don't see it, but probably you can believe exactly in the optical lines, it corresponds to some diffraction coefficient goes to infinity, which signifies that here the field is strongly perturbated and no perturbation theory can be applied in this region. The same story for the flux line, of course, diffraction coefficient of the flux line is well known. It's one more classical mechanics is continuous, but it appears phase. If you go in this part of flux line, you get phase e pi alpha, for this line you get phase e minus e pi alpha, and so on you see discontinuous phase. Here there is many interesting phenomena, which I don't have time to discuss because I see that I am too slow. In particular, one can prove that reflection from many lines like this corresponds in the dominant approximation, the mirror reflection. If angle is small, if angle is small, not small angle, but really the parameter should be square root of k, d, much less than 1, phi is the angle, but g is the distance from this, and if this criterion is fulfilled, the dominant effect of horizon reflection is reflection from the boundary, and you can easily construct approximate wave function leaving for this model. For example, this wave function corresponds to the barrier billiard, which I showed you before. You have barrier billiard, and then you split it in two parts. If it's equal, so you have this type of billiard. There is only a difference that here you impose anointment condition, and here you impose Dirichlet-Dirichlet condition. And all this pseudo-integral model leads to approximate semi-classical quantization of periodic obvious channel. I don't have time to discuss, but just look for this particular nice example. It's 10,000 levels. Everything is normalized. The distance between two levels is one, and you clearly see a regular structure for very high excited states, and no such structure appear in, say, rectangular billiard. And I have infinite many pictures of this, but it's pictures, but it leads to some kind of semi-classical quantization, which you see here. Approximate value is this, and exact value is this. The same story is here. It's long story of how to quantize surface of higher genus, and what I have in myons that you can do semi-classical quantization of surface of higher genus, at least of certain surface of higher genus. But these are the pictures, but I, like, more have formulas, so if you have expand this function to some kind of basis function. So this is a y, so you have zero, zero here, and here I put Lehmann condition here, and zero condition here. It's a full set of function in this rectangular. You can expand and you can plot. Here you will have m, here you have n, and you see that all coefficients for this particular function is small except one, or a few of them, which corresponds exactly to these propagating waves. Here if you do look carefully, it's much less, it goes to zero. It's a non-aligned picture, so the line means plus-minus, but amplitude here is approximately one, and here amplitude is very small. So it's like we call it super scar, because they survive, semi-classical limit goes to infinity. If you have numbers, you can compute participation ratio, and you can compute participation ratio for this numerics, which has been quite old one, and you know that participation ratio for higher moments should be scaled with n. Now n is k, because you have two-dimensional surface of conservation of energy, only the number of function proportional to k, and if you do computation, and you plot, say, this is from 1,000 levels to 800 levels here 4,400 days, 10,000, 10,000, 20, and then you compute, try to fit this curve, and you see that the fit with all this is old date, nowadays one can do, if you wish much more. You see that the fit, like for this point, for the stadium billiard, which is chaotic, and you see for the stadium billiard, fit is proportional to k, proportional to n, which means that d is equal to 1, but for barrier billiard, d is equal to 1,5 approximately. And here you have all labels still for 5,000, and you can fit it, and you can conclude that everything for the pseudo-integral models are fractal wave functions. OK, the model is model, but I like to more analytical results so I will simplify it. And also, instead of consider pseudo-integral model, I will consider quantum pseudo-integral map. Quantum pseudo-integral map even the most simplest, which interchange to integral. So this is the example of x plus x model of 1, so you have lines, discontinues and other lines and so on. It's also discontinued map, it's pseudo-integral, it will be pseudo-integral map if you look for these sequences of map. It's a reconcerting map because you have dynamical system and if alpha is rational, you have interval exchange map, if alpha is rational, you have only ergodic map but not pseudo-integral. And you can compute quantum map. What is quantum map is unitary matrix whose saddle points equal classical maps and it's not my invention, it was somebody else who do it for pure mathematical purposes. And so I use a slightly generalization of this map in the momentum space. If you do Fourier transformation of this map, you get that you can approximate this map like this. It is not approximation, exact, of course, Fourier transformation. Here you have a phase. In the dynamical model, it will be k squared and here I put just random phases and here you have unitary matrix. You can easily convince yourself that it's unitary, so it's not clearly seen and what I will consider will follow two different cases, non-symmetric matrices which is analog of GUE and symmetric matrices in minus k at the same. If alpha is irrational, I told you that I don't know, it's not pure interval, it's just ergodic map and you see that spectral statistic numerically very well described by standard random matrix example. This I cannot prove because I don't see how to, nobody knows how to prove that even for this simple matrix that all spectral characteristics do agree with standard example. But what I can prove is alpha is rational, say m over q is 2 comprime integer n is dimension of matrix equal plus minus 1, then spectral statistics agree with semi-pooson statistics with one parameter beta equal either k minus 1, either k minus 2 for non-symmetric symmetric. What is semi-pooson? It is exact result, numerics is just exact result but I don't have time to discuss. What is semi-pooson statistics? It's appear many years ago when we try to consider the simple possible random type logarithmic gas approximation. In random matrices you have all energy interacts with all energy. Here I put energy only nearby energies and then you do by some formulas and you get that all characteristics can be computed. In particular p of s equal s power beta the same beta is here and minus beta plus 1 s exponential tail k of 2 you can compute you can compute compressibility 1 beta plus 1 and the simplest case beta equal 1 it's a semi-pooson statistics which I discussed you before. So look, alpha can change a level repulsion as I wish. If you example if alpha 1 3, 1, 6, 1, 9 and you see p of s is s squared then you have s5, s8 the same for symmetric matrices it's shifted just to better so you have s1 half s3 half and 5 half this is exact result compared with some numerics. I have to go more quicker and if you do for example alpha 1 over 20 and n equal 8, 0, 1 you see the formula s 19 power e minus 20, but if you change a little n 8, 8 you see 8,000, 9 you see that curve is not far from random matrix result it's not exactly random matrix result because I can compute explicit formula for all for all k there are some explicit formula more complicated which is not important it is important but not immediately and correlation function for example you see as strange it is exponential of exponential is something it's very nicely fitted to numerics for this case n equal 8,001 if you compute numerically fractal dimensions you see that they are fractal dimensions very nicely follow it's for 1,3,1,5 by 9 but if you check this relation symmetry relation you see that they are not fulfilled there is no perturbation theory here you have one of them one delta another of them of another one it is not symmetric at all it is the same story for all alpha which we have investigation so eigen function of this strange quantum map multifractal but symmetry relation is not fulfilled but as I told you it is a very strange map because it appears somewhere else and we just recuperate it and to show its vector statistics it is nice to see something more generic consider for example this type of matrix random moment a random Q it's a diagonal matrix you have E so it's a Hermitian matrix and I will impose the measure what will be the measure the measure will be say trace L dagger L is natural and if I do only this I have this path AQ is not restricted because it's not here and I will put here beta Q squared it's very natural measure but if you look a little and you remember that you see this matrix before you will see that it's a lux matrix for collodgera-moser model L dot equal L exactly the same L you have M special which corresponds to as a consequence of this relation to collodgera-moser-gamiltonian rational collodgera-moser-gamiltonian but I don't have any dynamics but I do know who is the action in angle variables for collodgera model for example if you diagonalize this matrix this is a phases and this is there you can easily prove that this relation and what is important that double M is the angle variables double M angle value of lux matrix action variables it's important to me that this transformation between paying Q to WL and lambda are canonical it's very difficult to prove even by 2 by 2 matrices that it is canonical transformation you don't have any wrong scale so the only information I will use is the relation to some new variables so what is a GL is this one then I choose trace of LL dagger is lambda M squared Q squared is at Q dagger Q because it was eigenvalue of Q it is equal to this one so a random depended Q is the lambda double W and you get this factor for eigenvalue of lux matrices and you see that W integral you just throw it away and you get join distribution of eigenvalues without only for eigenvalues of lux matrices it is exact formula it's not approximated no approximation is done so all classical random matrix are based that you have big group of rotation which you can integrate rotated variables but lambda and then get join distribution from here you don't have explicit group invariance but you have hidden group invariance because you have an integral of motion which did not change eigenvalue of lambdas is a spectrum deformation and so you get by free expression for this join distribution so if you do it for something even more simpler than before you don't have time to discuss let consider even more simple matrix so you have here random variables and here you have k minus r without models but with e and you compute eigen distribution of p of s of this guy from this distribution like for the Wigner surmise you can convince yourself that the good Wigner type is the exponentially strong label repulsion p over s squared minus some quantity s so you have for example it's alpha g equal 2 it's a disk of you have exponentially big label repulsion and then you see how good is it for this model and this is a difference you can do it for all collodger model and you get a nice formula for all collodger model and the most important to me is that this strange looking model it's called Roussen-Artschneider model it has a name of relativistic generalization of collodger and never mind it's integrable model and the lux matrices after big simplification reduce exactly to the matrix which I have used for this interval exchange map but parameter r here is the arbitrary it's related with parameter r which is here and so on I used it before when r was equal alpha n now I can use it as r equal constant because I know how to compute it because I know spectral distribution for Roussen-Artschneider matrices exactly and this is some picture for hyperbolic models I don't have the time to discuss it but for example for this model for Roussen-Artschneider matrices so it's exactly the same matrix but now there is no n here and then you can check that spectral statistics depends of integer part of n for a between 0 and 1 spectral statistics is shifted for a zone so you don't have any eigenvalues in p of s before s is equal to a you have a gap is eigenvalues it's not even strong it's extremely strong rival repulsion and compressibility is also analytical formula for this case you can compute for some other values you can compute in principle for all necessary functions and you can easily check for example here a equal 1 half and you see there is no eigenvalues here and then exponential tail and everything for a equal 4 3 this was a curve which I showed you before and so on and so forth I will just two words that all these models are fractal you compute you compute fractal dimension and you see nice fractal formula and all of them are symmetric so symmetry relation of Merlin is working here and you can compute perturbation theory for all these models which I have in mind and they agree to the model of critical random matrix ensemble you can even compute perturbation theory for q less than 1 half which usually you don't need you cannot for normal model but here you can compute and you see that in the leading orders this is just formula and if you look for the formula which I showed you before I started slightly before so you will see that in all limit for small and large coupling constants there is this type of relation that key equals 1 minus d1 and d1 is just entropy of wave function is just one of the fractal dimensions related with the entropy but it's valid for small and large coupling constant in between if you do numerics even for critical bended random matrices you see one of them key in one of them is 1 over d and the point looking as a point for b to equal 1 for b to equal 2 here they should coincide but they are very nicely coincide in between for Russian-Artschneider ensemble one can compute told you exactly and this is a compressibility in 1 minus d1 which I compute numerically and you see that its points are on the point there is another model which I call ultrametric matrices once more this is a relation it's some kind of mystical relation it's valid only for the model which decays 1 minus as a first power and also it's related so in all possible cases which you have checked even for the cases where you don't have symmetry relation this conjecture works perfectly well so this is all what I would like to speak so first of all there are standard models which leads to intermediate statistics of eigenvalue what it is which was probably the first one where numerics have been performed it's pure the interval billiard for all of them you do have pure the intermediate statistics you can interval billiard with a flux line probably many of them what is the critical band and trend of matrices it has one large diagonal plus e minus g follow pure the interval models by definition diagonal or just shifted diagonals plus follow in small changes of matrices I did not show you numerics but you can see analytically numerically that small changes you think that it's small but it leads to big changes of spectral statistics because here everything is 1 over n when you have changes in the scale 1 over n you can change everything for the spectral statistics there is no universality you see that very strange models appear but this is exact and also interesting fact that lax matrices of all interval classical system give new soluble ensembles soluble means that I can write during distribution of eigenvalues not for not for all of them I can compute correlation function for Sennarchneider I do can but for all say scologer model I cannot but you can have very nice beginner type ansatz which agree very well with numerics for all models which I know eigenfunctions are multifractal there is no practically proof from any there is no I don't know any one model one can compute spectrum of fractal damage analytically and so is mostly use perturbation theory and numerics there is a symmetry relation it's valid for models with one large diagonal but it's a rule out at least numerically for the models both pseudo integral maps we put conjecture which we cannot need proof that key equal 1 minus d1 divided by dimension of the system and you can imagine that it's leads for some new developments of intermediate statistics it may be some new models physical models we do have this statistic thank you very much


If their car goes to the Jets, I'm going to the Jets as a Titan. Woody, give me a 10-day contract to prove it to you that I can play Titan. And here on WFAN, we have Craig Carton speaking about this in about two hours. Boomer Siasen making this his fodder for the week before the weekend.


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It's been about five years in the Queensland Ambulance Service as a patient transport officer and I deal a lot with the public. There was lots of races and cultures and young and old people so that I dealt with. So when you're working with the Ambulance Service, these are a lot of these things that play into the job that you actually do and it's one of the things that I really loved doing was to communicate with people and to help them. Well I'm an Aboriginal man from Central Queensland and my tribe is a Gungaloo tribe and we are situated in a round-around Central Queensland area and as an Aboriginal man this land belonged, I believe, to the past inhabitants and the connection with the land will always be there. I love this land Australia and I want to protect it and make sure that everyone uses it sensibly and I hope my little contribution by working for DIAC helps. It's a great opportunity this department, it gives you everything, it's flexibility and it's learning, you're always constantly learning if you have a person of my age. I'm always learning and learning something new every day. It's been a great journey and I'm always thankful that I was given the opportunity to do this so let me keep on going, let me keep on doing it. Always want to look for new and exciting things to do in this department so hopefully there's plenty more to come.


In a search for better lighting, I've made my way to the front of the trailer. My team back here waiting, doing their thing. We had Gronk on the show. NBA great Chandler Parsons is here, and this is everyone's biggest fear. Me, Chris McGullin's like, hi, we're on the show. It's fine. Everyone's okay. We have awesome guests and one of my favorite guys that I've talked about a lot on the program is here. And he's coming off an incredible senior season, right? Leads the entire nation in touchdowns. The entire nation in touchdowns in his final game at Tulane. He was the MVP in the Cotton Bowl. There went over USC. Please welcome running back. Tajers, Pierce, Tajer, what's up? Hey, how you doing? Thank you. Good, I'm really good. It's a little crazy right now. Gronk just left the trailer. He said it was too hot, but we are here. We're having a lot of fun.  We are talking about what I have learned about, which is the Poncha Tula Strawberry Festival in your hometown, my friend. So tell me about what it was like growing up in Louisiana and specifically in Poncha Tula. It was really great. Small little town. I don't know how many people we hold, but it's a smaller town. Like you said, it's a weekend of Strawberry Festival. And I was telling one of my friends, like, bang, this is really the highlight of our year, Strawberry Festival. They go on for like three days on Friday, Saturday, Sunday. A lot of festivities. And we got a big parade Saturday morning. And I'm going to have my own float. Me and my family are going to have a lot of different stuff. So it's going to be really, really fun. What do you mean you're getting your own float? Like, I got my own float.  I got my own float. This is going to be me and my family. And shout out to my sister-in-law for putting me together for me. That's amazing. What do you wear to the Strawberry Festival? Three days. It's like Coachella.  I want to go to the Strawberry Festival. Come on. You can wear whatever you want to wear because it's going to be like, you know, we in Louisiana. So it's going to be like really, really hot. So then it's about the rain. So it's going to be so like when the rain clear up, it's going to be like so, so hot. So you can wear whatever. I think I'm going to do like three different outfits, but I'm not too big on it for there. Well, you're big on strawberries.  And you went to play at Tulane. Your 2022 team accomplished the greatest single season turnaround in all college football history. You went from two and 10 to 12 and two. What is the biggest reason? Like the one reason you guys were able to get it together and turn it around? Accountability. And I say that from the top to the bottom. Everybody held up. Everybody accountable. We all was pulling in the same direction. We all wanted the same in-go. So accountability is the biggest reason for this turnaround. Well, we love to hear that. I'm sure that's going to carry on to one of 32 teams that are lucky enough to have you on their squad. And you finished your college career. You really put a stamp on it. And I like that you ended on the highest of high notes, Taja. You crossed USC and you said bye to Heisman Trophy winner Kayla Williams in the Cotton Bowl, 46 to 45. Such a dominating performance. And if you look at the numbers, it was insane, right? Everything that you were able to do four rushing touchdowns. How important was that victory for you on this football journey, beating a powerhouse school like USC and ready to go play on the bigger stage of the NFL? It's like, I kind of took myself out of the equation and just put it into the history of the school. We never did something like that at too late. So that's what we prodded the whole week on. Just making sure we live in the moment, make sure that we write down history. Coach even said, man, we win this game. We're going to go down the greatest team in history. So that was a mindset the whole year. And that was a mindset definitely coming into that game and coming out of that game. So it was like, I remember two, three years ago, like an upper class anti-tank title. I was like, how are you going to remember? Like, how do you remember like Cotton Bowl champions? Like, can you repeat the Cotton Bowl? Like, that's something that they can't ever take away from. So that's going to go down forever. They can never take it from you, but you didn't fall off there. It wasn't some shining moment and then it went away. Because you said it changed something, right? And it was obvious. You took that momentum. And trust me, I've covered this game on the NFL level for over 10 years. I don't really watch the college game. I'm not as plugged in. But your name is the name that I was hearing towards the end of your senior season and into this one. And I know that all the most important eyes in my business are on the senior bowl. That's what matters. What are guys like? Not even in the game, the weak leading into practice. And you crushed it on every level. And last week we were talking about this rep that you had that week. Will you please talk me and every NFL fan through this play? It's just like optional. He took the inside away from love. He was playing outside. He's just outside right here, playing outside.  It ain't nothing too special. It ain't nothing too special. Oh my gosh, I'm running back, needing teams are needing you there. So I want you to know that we love you. We obviously made the forte comparisons a little bit just because of the school and where running backs are going in the draft. But is there a running back in the NFL that you sort of look at and say, I like how he moves. I want to be like him. And I model my game after him. Oh, not necessarily, but it got two guys that I really like on. And, and Jones and I'm coming there. I like, I really like those guys, but like me just sitting there like saying, I'm the model of my game. I've been somebody, but those two guys I really, really like. I really like doing. I like everything that they do when it comes to on the field.  So have you had a chance to meet any of those guys? Like you're there. You're in New Orleans. Have you met Alvin Camara? No, like we probably reached out to each other like text messages, like texting, but like, no, I'm not meeting nobody. I want to be ready to Bush though. Cause like, like I said, like my first year of playing football, I got 25. He was my favorite player at the time. I used to like him a lot. So that's why you had the 25, got it. Because I was thinking about Matt Forte and the reason I brought him up, he's obviously a Tulane alum. And I think that you'll be the first player from Tulane to go in the first three rounds of the draft since Forte did it back in 2008. I'm a big Bears fan. And he had a great career wear in that number 22. You wore 22. Any connection there? No, not too much. I just try, I just try to make my own path in life. I don't really, like I say, like, you know, I don't really focus on comparison. I try to, you know, live one day at a time me with my feet up. How do you feel about your pro day? All 32 teams were there. They all showed up. You were dealing with an injury. You didn't run the 48, the combine. Getting that four-four time, how important was that to you? It was, it was important. It was important to show the, show all 32 teams that I can run fast. There was, there was probably a big question coming from the combine, like why are you running? Is he fast? So like, just checking that box. It's all about just taking, just checking the box alone, along this journey. That's all it was about. All right, we're gonna get to know you a little bit better and let all the NFL fans get to know you a little better. And we're gonna give a minute on the clock and I'm gonna ask you and bank through as many questions as possible. Okay, you ready? Oh man, y'all ready? All right, who would you love if you could pick anybody to headline Coachella? Who would you pick? Sydney. You could pick anybody to headline Coachella. Which musical act would you pick? What is it? It's like a big music festival. I love that you don't know what it is because you're the best. I'm immediately a fan of you. Like, Oh, Kevin Gates. Kevin Gates. Kevin Gates, okay, great. The dream car that you want to own someday. A Bugatti. A Bugatti, okay. Best preparation for eating strawberries or best way to eat strawberries? Best way to eat strawberries is with cheesecake. And that's what you're a man after my heart here. Is there a TV show or a show that you're streaming right now that you love? Uh, Sanford & Sunder. It's like so old. You're watching, wait, hold on. Hold on. Stop the clock. You're just casually watching episodes that you're binge watching Sanford & Sunder, what? It is, that's all I do, like Sanford & Sunder and Martin. That's all I watch. Martin, I mean damn, Gina is one of my favorite shows ever. But not, you're too young for this, but it would be on. And then the second half hour was living single with Queen Latifah and it was amazing. It was like the best hour of TV back in the nineties, back in the day. Okay, Sanford & Sunder, I love that. Best food spot in New Orleans? Let's say I'm there for one hour. Where am I going? One hour. That's a good question. Oh, New Orleans food and spirit. New Orleans food and spirit. I'm gonna write that down here. Favorite NFL player of all time? Favorite NFL player of all time? I really like Barry Sanders. Barry Sanders, talk to me, I'm beeping, we gotta go, we're going too slow. Let's do this, all right. Favorite video game? Favorite video game, GTA. Best Tulane football player ever? Best Tulane football player ever, Matt Forte, class of this year. Come on, come on, favorite comedian. Favorite comedian, I know. Oh man, man, man, that's the Harman, that's the Harman, that's the Harman, that's the Harman, that's the Harman. That's the Harman. Oh, Bernie Mac, Bernie Mac.  My favorite superhero, dang, I don't get into superheroes, but I like the Hulk. Is he a good, is he a good one? The Hulk, I think so. What are you into outside of Sanford & Sunder? You don't like Coachella, you don't like, what are you into? Do you watch, do you watch, do you watch Power? I watch, but now it's in Power, like a bunch of different things with Ghost and like all those different, but Power was like the OG one, right? That's like, just when I'm watching right now, I'm watching her like, what it is, like Ghost of Book 3, that's when I'm watching right now. Like that one, there's too many of them for me, I think, Power. Who's the original cast?  I got a binge watch Power, okay, I'm gonna do that. I thought, why don't I think, yeah, I had the wrong show in mind, I met Omari though. Yeah, he's amazing, I interviewed him once, he's great, I'm a big fan. Hi, so what's your favorite show for these? Oh my gosh. Right now, it's this song called succession, or this show called succession, and it's kind of like Power, and it's kind of like Billions, and it's on HBO, but it's a lot, it's too many, you're too focused on Ball right now, but maybe next off season, after you've won Offensive Rookie of the Year, you can catch up on that, how does that feel?  I like you, Taj, you're very funny. All right, we will see you at the draft, I'm telling you, first three rounds, Matt Forte, don't tell, I love Matt Forte, I love watching it, I love watching those 1000-year-old seasons, you're the best player out of two lane coming to an NFL team and you will be back with Chandler Parsons as I am melting in this car, I am literally melting.


Okay, so we are presented with these three kind of orbital descriptions, okay? So these are parts of what you would see in an electron configuration. So, of course, an electron configuration would be much longer than this. This is just one little portion, and I want to focus on these so we can identify the parts of what we're seeing here, okay? So the things I want to identify are, so what is the principal energy level on all three of these, okay? What is the orbital type and how many electrons? So number of electrons in each of these. And we're just looking at the portion of these electron configurations that are pictured, okay? So in this case, we've got the 4p6 portion picture, okay? So remember, principal energy level is n, right? So that's like the first quantum number, and that's represented by this number that's in front of that orbital description, okay? So hopefully, you guys, if you would like to help me, if you don't want to, it's totally cool, okay? So n, or the principal quantum number in this 4p6, if we're looking at one of the electrons in this 4p6 portion, it would be 4, right? So is everybody fine with that? So it's on the fourth energy level is what we're really seeing, the electrons within this orbit, or this set up. Here, right, is on the second energy level, how do I know that? Because there's a 2 in front, okay? And then what would this one be? So that's the energy level that these things are at. So now we want to say, well, what orbital type is represented by this shorthand configuration, okay? So the orbital type, as you probably know, is represented right here by the letter, right? So in this one, it's a p orbital. This one, s orbital, and this one is a d orbital. Okay, so lastly we want to see how many electrons are there in each of these particular portions of the orbital diagram, okay? We can also figure out, if you want to, the number of orbitals in each of these. Well, if you want to think about it as p orbitals, they always have 3, okay? There's always 3 p orbitals in the subset, okay? S, do you guys remember how many? This is 1, just 1, always 1. And then d, do you guys remember that one? So you can look at the periodic table, yes, it's 5. So how am I getting that? I look at the periodic table, I look at the s block, and there's only those two elements. So remember, orbital, only two electrons can fit into one orbital, okay? So that's why I know there's only one s orbital. We'll go over this again, okay? I promise you we'll get this. Okay, so let's do the last portion of this part here, okay? So up here it's saying, it's telling us how many electrons are in those 3 orbitals altogether, okay? So that's 6, okay? So let's write that down. So since we have 6 electrons in 3 orbitals, all of the spots in those orbitals are used up, right? So in this case, we have 1 electron and 1 orbital, right? But there's how many spots in each orbital do we think? 2, right? So we can fit one more electron into this orbital here, okay? We just have it, right? So this symbol is representing only one electron being in that 2 s orbital, okay? Does that make sense? Okay. And then this one, right? So since there's 5 orbitals, what would be the maximum amount of electrons we could put in? 10, right? But it's saying that we have 7 of them in there, right? So what that's saying is that not all of them are filled up, right? In fact, in this case, only 2 of them are filled up. The other 3, so if you wanted to think about it, right? If you're thinking that this is my 3D orbital system, so we're doing a condensed electron diagram or atomic orbital diagram, right? It'd be using Hunt's rule, right? 1, 2, 3, 4, 5. And then Pauli exclusion principle, 1, 2. That's 7, right? So we see 1, 2 orbitals are completely filled in the other 3, okay? So are we okay with at least looking at these symbols here and being able to write all of this stuff down? Is that it? Are there any questions on this question? Okay, we're going to build up from here, okay? We're going to write out big, now we're going to start doing the electron configurations, okay? Writing the whole thing down. So we'll say, I don't know, what's the electron configuration of aluminum or something like that? Any questions? You have a question? I just wanted to say you need to look at the periodic table. Do you have 5? I don't know what you're looking at. Okay, so okay, let's do that. We'll record me looking at the periodic table and I'll show you, okay?


And then we see more often like of arrest of people accusing them of violating the national security law, arresting them in early morning, early hours. And actually we saw similar practice in mainland China for many years in the past. Those things happen in Hong Kong in a very strange way that we have never seen such things before. And then we are also very concerned about like whether our judicial independence can still be maintained. This is also a question about after the government can appoint judges to hear national security law cases. And actually that would make a huge difference on like how we can ensure that we still have judicial independence. So actually ranging from different areas, we can see very daunting situation here and also for legislators that we see like the legislators, poor democracy legislators, they will disqualify and then their colleagues wanted to support them so they quit. So now we only have pro-government legislators in the legislature. So you can imagine if you only have pro-government legislators, there's no opposition that everything actually is out of control.


A new research agreement between the ride-sharing company Uber and the United States Army may result in quieter, unmanned aircraft for the future force. The U.S. Army Research Laboratory has aeronautical engineers and scientists working to solve some of the toughest technology challenges in delivering the rotorcraft of tomorrow. During a technical summit in Los Angeles May 8, Uber announced it has signed a cooperative research and development agreement with the Army to advance technologies supporting future vertical lift. The research that we will collaborate with Uber to do will actually deliver unprecedented capability for quieter rotor systems in a unique configuration. This objective aligns with the Army modernization priorities. One of those six modernization priorities is for future vertical lift and the emphasis within future vertical lift is toward future rotorcraft or helicopters but also a future fleet of unmanned aerial vehicles or UAVs commonly known as drones. Army officials said their work on the future fleet of unmanned aerial systems will include the ability to give the soldier of the future silent operations. We have extensive experience in rotorcraft aeromechanics and rotorcraft aeromechanics by definition is very multidisciplinary field. It requires expertise in different technical areas and we have such a group. Uber engineers met the Army researchers at a conference in 2017 and soon after discussions began about a potential collaboration. We have a 32 year veteran of NASA Mark Moore who's helping to design a lot of these aircraft. So it was a pretty natural partnership for us to connect with U.S. Army research and start looking into rotor technology. The key takeaway here is that the technology that's being developed has direct applications in both urban air mobility in the private sector as well as military applications. The laboratory aggressively seeks out private public partnerships with academia and industry to reach its research goals. So I'm really confident because we have willing partners on either side with Uber with their objective for urban transportation or the air taxi as they call it and the Army with its objective for silent operation as a capability for the future unmanned aerial vehicle fleet for the soldier. And so because Uber is aware of the subject matter expertise that resides in RDECOM and we are able to deliver that through a long standing relationship with partners in our ARL South regional extended site. The combination of elements there really give me great confidence that good will come of this. Building an ecosystem with industry and academia will allow for sharing resources resulting in science and technology solutions for soldiers. This grader is really captured the spirit of open campus. In the sense here we have a commercial partner who have certain requirements or certain needs of advancing technology for air taxi applications. And we have on Army side we have needs to advance S&T for unmanned air systems. Challenges include making unmanned aircraft systems fly longer, faster and carry higher payloads. I'm very excited for the partnership that's coming about because it really starts to get toward the strategy of having industry, an aggressive engagement with industry around very cutting edge research that may be in its early stages but will allow us to move this into an industrial ecosystem where it can make its way to the soldier.


This is Conrad Nagel inviting you to stay tuned for the next half hour for one of radio's outstanding dramatic productions on Proudly We Hail Proudly We Hail Another Proudly We Hail one of radio's outstanding dramatic half hours transcribe coast to coast in cooperation with this station and presented by your army and your Air Force From Radio City, New York here is your host and star on Proudly The distinguished star of the theater screen radio and television Conrad Nagel Bang hard. Hello everyone. Welcome again to Proudly We Hail We're especially pleased to present our Christmas program an original play entitled Christmas Story Our first act curtain will rise in just a moment after this brief but important message The United States Army and United States Air Force are expanding young men and young women with the will to learn can get ahead fast So take advantage of the opportunities for advancement that can be yours by enlisting now And I'd like to point out that every man and every woman in the United States has a definite part in the stepped-up program of national defense And there's a special need for young women between 18 and 34 for service in the women's Army Corps You'll enjoy the gratifying feeling of satisfaction that comes in doing your part for your country during these critical times Visit your local United States Army and United States Air Force recruiting station talk to the local recruiter and learn all the facts Volunteer today and now with your star Conrad Nagel in the role of Gauss your army and your Air Force present the Proudly We Hail production Christmas story Twisted and turned through the wild country leading ever southward It was an old row that had known the passing of countless generations It was a narrow road where a man's safety often depended on the numbers who traveled with him After dark it was an empty road where only madmen beggars in the unwary set foot For it ran through a land in which the people were oppressed poverty-stricken and desperate It ran through the land called Judah Yes, why do we tarry the light will be gone in another hour my youth is always in a hurry I'm not that young my friend We may ride this road as Romans during the light hours, but after darkness I know I know We're not like are we Marius liked? Like by whom the people here you joke We call the wretches who infest this broken land people and what would you call them?  I've been here a little more than a month But it took me only a day to see that this was not a happy land And yet there's a feeling here a feeling I can't quite place Almost as though it's a feeling of not knowing when somebody's gonna try and cut your throat How long have you been stationed here Marius for five years five and by Jupiter? I wouldn't be sorry to leave have you learned anything about these people in that time Yes, Gaius, I have and the fact that I'm still alive proves it now You may be my superior in years in position, but I insist that we put speed to our mounts. Where do we stop this night? I know of an inn that's not too bad lies in the city ahead the city of David a place called Bethlehem Innkeeper Bring more wine here lost in thought Gaius observing Marius observing He does a thriving business this one must be one of their pilgrimages They're always having them for one thing or another they have but one God and It is not of stone as ours are not alone should give you an idea of the madness that runs in their veins In keeper Why so crowded this night gracious, sir Caesar has decreed that all must sign the royal register Man woman and child they come ah, that's it now. I recall All right put the wine down and go yes There was talk of this at Herod's court that slipped my mind. Well mine as well Well, you'll have plenty of chance to observe the people now Gaius a stroke of luck More wine. No, no, I've had enough poison But one must like his thirst. Yes, yes, of course Gaius, what is it? What's come over you?  Sorry Marius. I'm not very good company. I'm I my My thoughts will not let me rest Thoughts of what they're not easily explained. Oh Perhaps I'm weary of life Rome is great Rome is powerful Augustus is just and I am a successful and honored man Still is there anything else a man could wish for guess? I don't know Probably not and that may be one reason for my mood. I'm I'm like a man searching for something and not knowing what it is But I've never felt it so strongly as here.  I speak what is in my mind then I would speak it softly lest we are over Yes, yes One must be cautious at all times this land has affected you evenly Gaius. It does that to some it's affected me I'll grant you that I Wish I knew why I Think I'll go for a walk Care to join me. Do you want to be found in the gutter in the morning? Conquerors who are afraid to step out of doors after dark a I'll take my chances by Zeus your heart on a man's patience day here then and drink your wine I'll be all right. Well if anything happened to you Augustus would have my hide You me you I must come we'll go stumble around in the dark and dare the knives of beggars And they watch us like jackals waiting to strike and were you one of them How would you watch us? Those darker and more chill at every breath I have never seen a night so dark So quiet all the more reasons for us to get back inside. Do you? Do you have the feeling as though everything was holding its breath? I do not I Have the feeling that you've lost your mind and need a physician What do you plan to do stand out on this hill all night? The only light seems to be coming from the end down there Augustus can hang me up on my heels, but that's just where I'm heading with or without you enough Marius. Come we'll go back I've been a poor friend. I'm afraid an uncommon strange one this night Yes, it's true. I Am not myself by morning. You're not recovered Summon a physician to conjure the evil spirits from me. What's your step to conjure? I know not what from you Freely again God's a favor to us No, no, I know why a welcome light and all the darkness. I Wonder my hope someone comes And from behind I like it not calm yourself We're but a stone's throw from the end no one would dare attack us here. So you think Standing this alley until whoever it is passes Do you think if they met as harm they would announce they're coming? I tell you you don't know these people Please do as I say gays. Oh as you wish, but I quiet They come cutthroat thieves in the night well a man and his woman riding a donkey a Fine thing for two proud Romans to be afraid of scarf if you like gays, but if you know these Look, they go to the same in as we Come along. We'll have a better look at these dangerous people Well, because I take precautions for your safety is no reason to mock I do not mean to mock you Marius. I Think you over cautious. That's all they could come from the moon for all of me Who knocks at this hour? We seek lodging for the night. I'll seek elsewhere. There's no room here. I'm filled up. My wife her time is near Tell me not your troubles. I have more than enough of my own. There is no place. You could put us Now big on night here's chill could you tell it I can tell you nothing but to go away and seek elsewhere hold there Who speaks? Oh Sir, I did not see you. I you have no room for these people none I swear it even the floor space is taken. I saw clean hay in your stable. What about that? Why can't they stay there stable? I have not thought that If you would care to stay there what we shall stay and gladly I thank you, sir. No need It's a dark night and cold Let us go in Marius Listening to the special proudly we hail Christmas program presented by your army and your Air Force an original play entitled Christmas story Now with your star Conrad Nagel in the role of Gaius. Here is the second act Yes, what is it? Can't you sleep? Oh, I I'm sorry if I woke you Marius. I was asleep. I Had a strange dream. I Can't remember it very well, but it woke me and now sleep will not come should have drunk more wine Gaius What am I going to do with you? The best thing is to stop worrying The innkeeper nearly fell over in a fit when you spoke up Since when has a Roman gone out of his way to assist the rabble?  They were not rabble The man had a fine face and the woman was beautiful to look upon not like other women Because their clothes were poor does that make them rabble? Get some sleep Gaius. We have a long way to travel tomorrow If I keep my eyes shut tight, perhaps sleep will come I should be tired And yet I'm not For there's no shutting out my thoughts Why? Why do I feel this way? My life passing before me like an empty vessel on a dark sea Could Marius be right? Is this land full of demons that drive a man to madness What manner of people are these that go around in ranks? broken And yet looks skyward to a god of strength and mercy Strength mercy How does one be get the other? The merciful are weak in the press And the strong are without mercy hated that man and his wife He had no fear of me Yet neither was there heat in his eye. I Believe he was grateful and the woman It seems she smiled on me There was warmth in it and were I not a Roman I might know them and be their friend It must be cold and that stable What magic is this Marius Marius wake up wake up man Marius What is it?  Huh? Here calm yourself gays Dreaming again. I have not been dreaming What is that light? Where did it come from?  You're shaking. I I was lying there thinking I opened my eyes and suddenly the room was filled with a strange light Have you ever known the moon to shine so brightly? Since the dark night it always seems to shine brightly. There is no moon tonight. Huh? There was no moon last night You'll recall we mentioned it well Well, we must have been wrong Oh, what else could it be? I don't know This window is too small to see. What are you doing? I'm going outside to have a look. Are you mad?  I know I know it Came out of the clouds. You know how dark it's been.  Think as you like. I'm going out. All right. All right. We'll go outside We'll look at the moon And then we'll come back here And if you disturb me once more this night gayus, I swear by jupiter. I'll Well, I'll tie you to your bed When When it happened It was as though I heard voices A great many voices singing Now tell me it's the moon Black magic swichery gods are angry. Oh No Your marble gods have not to do with this. It's the end of the world That star is falling right on us. It falls not but hangs over us There is peace in its light There is no evil here Only goodness And I am not afraid what? What can it mean? It must be a meaning No star has shown so brightly Or so close I know not the meaning But the trouble is gone from my heart Gaze Look there Others come be on your guard down from the hills They must be shepherds And they seem in a hurry Perhaps they know the meaning how could such ignorant beggars know anything Stay clear of them. I say oh maria's maria's. When would you learn? When will you?  I'm as brave as any man Then take your hand from your sword and come Oh good friends wait Wait for us. Good friends indeed They'll run like rabbits when they see the color of our cloth. Let's hope not Why they seem to be waiting for us And in this light they can see your helmet too frightened to run now Watch them grow. We'll let your feet and say nothing We mean no harm But we'll have words with you Oh, please please do not be afraid We fear not when you address her over maria's be still You You are shepherds. Yes We are shepherds Our flocks are in the fields above and you leave them without protection. They are safe The lord watches them No harm can come to them may May I ask what you do here? Well Speak up when you're spoken to maria's Good shepherds We we could not sleep The light woke us Know you it's meaning It's true meaning You're a roman you wouldn't believe our words forget my race if you can I'm a man like yourself and I would know It is news that all should know even a roman Tell him So be it You ask of the light We too saw it And did not completely understand At first we We were afraid Well Because of our faith We lost our fear It was written long ago by the prophet isaius That great things would come to pass in the city of david To those who watched in the fields The prophet wrote the the light Would bring glad tidings For all the world This night as on all others We were keeping watch This is like a great black cloak Even the fire gives no light Never has it been so quiet Even our charges are silent They bleed not Yet they sleep not To see just one star The jackals are hushed Who is known a night when the jackals did not cry? The night will pass no matter how dark or how quiet Our brethren in the next fields They too heard it And they're not blind or deaf Must not fear easily said Aye, but the heart beats another tune the lord watches over us If you like I shall say david sound say it the lord is my shepherd I shall not want He maketh me to lie down in green pastures He leadeth me besides still waters He was starved in the paths of righteousness for his name's sake Though I walk through the valley of the shadow of death I will fear no evil Or thou art with me Your words are music in the heart of a weary But the darkness is no lessen Silence grows What is there in either to harm us? Who lie? Who lie? What has happened? Great joy which shall be to all the people For there is born to you this day in the city of david a savior who is christ the lord And this is the sign unto you He shall find the babe wrapped in swaddling clothes And lying in a manger Lying in a manger And Know you where to find this manger The star shines over it I can take you to the exact place Gaius don't tell me you believe the raving Marius be silent Either be silent or go back to your bed Now friends If you will follow me I think I can lead you to the place you seek The babe was wrapped in swaddling clothes How? How could they know they told you how they knew Do you not know the truth when you hear it? But But it is beyond belief No marius No, it is not beyond my belief now They knelt and And worshiped the child Immanuel they call him God with us I I don't understand nor I completely marius But I have a feeling like none I've ever known That this night will be remembered Remembered long after we are dust Something has happened here this night Not meant for any one race or people But for all mankind From this day forward Is our distinguished star Mr. Conrad Nagel Well friends Frankly I I can't tell you all what it means for me to be the spokesman for the men and women of our army and our air force And extend to you their best wishes for christmas 1951 You know many things have been said many ways about what we all believe in and are willing to fight to keep At this season it seems to me that Well that one of the important reasons for our feeling as we all do about our way of life Is that here in our country we can say Marry christmas and meet it Christmas is always wonderful of course But it seems to me at this time in all our lives it means more than ever to all of us More even than the mystic magic that always comes with christmas Where I feel that christmas has come to symbolize what we and our fighting forces stand for throughout the entire world The men and women of our armed forces are serving and fighting to maintain the truths that were written long ago Glory to god in the highest And on earth peace Goodwill toward men And so friends speaking for all of us on proudly we hail and as spokesmen for our army and our air force The happiest of christmas is to you all Been the special christmas program on proudly we hail Presented transcribed coast to coast by the united states army and the united states air force recruiting service Proudly we hail stars comrade nagel This is kenneth fanghart joining comrade nagel and speaking for all of us on proudly we hail Wishing you all a very merry christmas