0 00:00:02,700 --> 00:00:19,410 Jorge Pullin: So today we're going to have a panel and look Congress biology for stock will be by here mobile give us an overview that nearly will then connect help you see with full El que je and you and we'll talk about observations so you're more Please go ahead. 1 00:00:27,420 --> 00:00:30,870 Guillermo Mena: And you see the screen there we do. 2 00:00:31,440 --> 00:00:33,720 Guillermo Mena: nope no OK one moment. 3 00:00:44,070 --> 00:00:44,370 Okay. 4 00:00:48,450 --> 00:00:48,720 Guillermo Mena: Okay. 5 00:00:49,800 --> 00:00:50,280 Guillermo Mena: So. 6 00:00:53,190 --> 00:00:53,460 Guillermo Mena: yeah. 7 00:00:57,000 --> 00:01:00,510 Guillermo Mena: So I was thinking for the invitation to be part of the panel. 8 00:01:02,700 --> 00:01:11,250 Guillermo Mena: So the question is a little bit familiar to us is, why are we interesting is turning to handle the slowly. 9 00:01:11,850 --> 00:01:28,890 Guillermo Mena: Essentially, I will say there is a good spirit or look quantum gravity and the other thing is that we want to extract the reactions that they eventually it could be a confronted with observations in order to make a theory falsifiable. 10 00:01:30,330 --> 00:01:41,610 Guillermo Mena: Or the system, so the banning interracial activity also follows up to move to put into test the capability of the quantum effects to solve this mutual. 11 00:01:42,150 --> 00:01:50,220 Guillermo Mena: Severe singularities of how this is done and the other things that are in the very ugly universe, we know the. 12 00:01:51,150 --> 00:02:03,660 Guillermo Mena: should be large directors and they interactions they're going to addition interactions for responding to provide a sector would be important in those books. 13 00:02:04,590 --> 00:02:18,180 Guillermo Mena: While they essentially a month, so the preparations that were affected by them afterwards have evolved during a classical inflationary and post inflationary a PayPal. 14 00:02:18,720 --> 00:02:33,240 Guillermo Mena: Until a reaching what nowadays would correspond to large angular scales, and in this sense, we can we can say that being in cosmology a ultraviolet and infrared meets. 15 00:02:34,920 --> 00:02:36,960 Guillermo Mena: So all these are important. 16 00:02:38,340 --> 00:02:45,450 Guillermo Mena: We say features, or the framework, the other important thing is that the cosmological or situations. 17 00:02:47,010 --> 00:02:48,420 Guillermo Mena: point towards. 18 00:02:49,560 --> 00:02:54,240 Guillermo Mena: anomalies tensions between the measurements and the predictions. 19 00:02:56,040 --> 00:03:09,810 Guillermo Mena: and indicate the least our university statistically are normally a i'm hoping the possibility that in fact there is new physics and this gives us the opportunity to look for possible and. 20 00:03:13,140 --> 00:03:28,950 Guillermo Mena: In doing this now important feature is that we have to make compatible this alien variance is more or less than 60 salvation of the cosmic microwave background, with the introduction of the quantum scale. 21 00:03:30,690 --> 00:03:31,500 Guillermo Mena: OK so. 22 00:03:33,300 --> 00:03:45,270 Guillermo Mena: The nice thing is what is that we understand my look want to perform so essentially we understand the application of the methods of look quantum gravity to first melodic is sustained. 23 00:03:46,260 --> 00:04:00,300 Guillermo Mena: And since the relation between the two things are not a fully a solid establish a did may assist me with this, but on the other hand, through that from different restrictions. 24 00:04:00,660 --> 00:04:10,320 Guillermo Mena: from different proposals we have arrived to situations that are qualitatively similar like reason they are playing soccer bounce. 25 00:04:10,680 --> 00:04:25,440 Guillermo Mena: All the effective classical behavioral the universe of them Okay, and this sense, there are a few sounds there seem to be quite robust okay in at least in order to study, what kind of effects we can expect. 26 00:04:26,640 --> 00:04:36,360 Guillermo Mena: Now, as I was saying before molly must proceed with the what we call this an hour abroad to cosmology in the sense that. 27 00:04:37,440 --> 00:04:49,920 Guillermo Mena: We say that there was a slow roll inflationary face and that the vacuum stay there was once a week and the success of the system, our approach is so impressive that. 28 00:04:50,430 --> 00:04:58,920 Guillermo Mena: In fact, it is a kind of paradox in the sense that some people who say that there is no room for funder effects that can be are several. 29 00:04:59,400 --> 00:05:06,840 Guillermo Mena: while others will say that if we released under X, Y you opening pandora's box and then we can have all kind of phenomena. 30 00:05:07,170 --> 00:05:15,450 Guillermo Mena: And, in particular, radical changes in our faces okay and look into cosmology and certain says must keep an equilibrium between the two things. 31 00:05:15,870 --> 00:05:33,660 Guillermo Mena: You must at the other day just lead us to some modifications, but not very practical Okay, so in practice we we described the departures from homogenized and so to be as perturbations. 32 00:05:34,350 --> 00:05:46,590 Guillermo Mena: What we do is to consider backgrounds of nature that behave in an effective manner and such that they on, then the reaction of the preparations, you say then negligible of various. 33 00:05:47,850 --> 00:05:54,180 Guillermo Mena: And these backgrounds are typically present evolves and the main. 34 00:05:55,200 --> 00:06:02,700 Guillermo Mena: person that we make is whether these subjects stay the primary operations of how they they will. 35 00:06:04,680 --> 00:06:17,220 Guillermo Mena: OK, for that there are least two routes you look on the boat molly to achieve have to arrive to a point of view theory in especially impulsively often to measure. 36 00:06:18,570 --> 00:06:27,660 Guillermo Mena: That are the hybrid approach or maybe there is maybe Okay, a this simulator similarities between doing our homework okay. 37 00:06:28,080 --> 00:06:39,120 Guillermo Mena: Let me say that they have read approach is principal your starts with pompous partial sections rotates the action up to whether epic terms in the activations. 38 00:06:39,570 --> 00:06:49,110 Guillermo Mena: This leads to a full swing global system that contains both the background and the preparations and usually, when one takes a continuous long compared to. 39 00:06:50,280 --> 00:06:59,940 Guillermo Mena: The rest medical approach, on the other hand, one is started by by assuming that the battery actually was negligible, something that can be checked out was for. 40 00:07:00,360 --> 00:07:10,800 Guillermo Mena: Consistency and that moment the coastline of X essentially the background usually they the quantity stays out of planes at an adult and effective. 41 00:07:11,190 --> 00:07:29,430 Guillermo Mena: scripture in which the main quantum corrections can be encapsulated in rest metric and the dynamics of the activation our equation so motion in which they the effect of these two buckets one is a kind of meaningful approximation, in the sense that is given by inspiration. 42 00:07:31,470 --> 00:07:43,770 Guillermo Mena: In most cases, a in practice what we consider our backgrounds that admitting effective region you look on the Bologna the perturbations of described by fox conversation. 43 00:07:44,250 --> 00:07:55,290 Guillermo Mena: And the most of these perturbations are a big satisfy equations that can be rating as the dose of our monocle see later, but we've amassed that depends on the. 44 00:07:58,320 --> 00:07:58,740 Guillermo Mena: story. 45 00:08:03,660 --> 00:08:03,990 Guillermo Mena: Okay. 46 00:08:05,940 --> 00:08:08,520 Guillermo Mena: So what are the difference if any. 47 00:08:09,570 --> 00:08:17,400 Guillermo Mena: Well, in principle, is through that heavily look into goes molly can leave room for what reaction in the sense that definition of the. 48 00:08:17,940 --> 00:08:28,770 Guillermo Mena: variables that form economical sense for for the in some of the background of the populations include corrections to the variables for the background are quadratic. 49 00:08:29,970 --> 00:08:42,270 Guillermo Mena: Okay, the others a feature is that the system has a particular string and the sense that maybe some but reaction was the preparations on the background. 50 00:08:42,600 --> 00:08:55,380 Guillermo Mena: But the practices you one concealer walk around with a negligible but reaction this difference essentially disappear Okay, so they only difference that remains is the way in which the background dependent mass is calculated. 51 00:08:56,820 --> 00:09:11,160 Guillermo Mena: In principle, in hybrid low quantico smalley one is does with economical description, in which the river is given by commentators will have insomnia, and only after computation everything is evaluated on reactors. 52 00:09:11,790 --> 00:09:21,630 Guillermo Mena: In the various metric in principle as so region formulated one has affected trajectories and even the derivative is her calculate is on these directories. 53 00:09:21,990 --> 00:09:26,520 Guillermo Mena: What means that they are given by commentators question market with effective coming tanya. 54 00:09:26,910 --> 00:09:41,670 Guillermo Mena: And then, this is not a subway the same when the quantum effects are very important, that is precisely the region in which we believe that they could be effects of groupon to cause molly and which are the ones that we want it is the only. 55 00:09:44,160 --> 00:09:52,770 Guillermo Mena: So, for instance, here, this is a graph in which we see around the around the mass for the hybrid a approvals for the various medical. 56 00:09:53,820 --> 00:09:57,270 Guillermo Mena: But for the rest of the evolution the masses are complete this. 57 00:09:59,730 --> 00:10:11,640 Guillermo Mena: So the other thing also a concern in the background is that, after is real so when they advance which is a they say various money in terms of. 58 00:10:12,510 --> 00:10:22,200 Guillermo Mena: Things in terms of a few a a fraction so one thing being afterwards they say every year of classical evolution, there is no. 59 00:10:22,950 --> 00:10:33,870 Guillermo Mena: it's not exactly as in the standard approach is not a slow roll inflation, we have first every year in which they energy on the data is dominated by the kinetic thorough. 60 00:10:34,200 --> 00:10:41,670 Guillermo Mena: And after was the beginning of inflation typically has the first roll video essentially because they kind of solutions that. 61 00:10:42,690 --> 00:10:54,000 Guillermo Mena: We are interested in this show certainly inflation okay very important questions whether the modifications to the predictions of a standard approach will come. 62 00:10:54,330 --> 00:11:11,640 Guillermo Mena: Either from these classical region is non standard have thrown the quantum theory around the bombs and these important because may happen that the classical notifications, are they say larger than the quantum ones, and therefore we cannot observe me. 63 00:11:12,780 --> 00:11:27,360 Guillermo Mena: A in this introspect, let me say that with reasonable choices of working, what happens is that won't fill the specter of his vision of power of the scale, in which this appears is different for. 64 00:11:27,990 --> 00:11:39,210 Guillermo Mena: A non standard Jeanette will release the case scenario for groupon to put in one case this game is the beginning of inflation and the other is the. 65 00:11:39,720 --> 00:12:00,900 Guillermo Mena: Other way around the world okay and typically the quantum scale for groupon to carvallo is larger than the other, and this gives us hope that if any of these superficial appeared in the power spectrum, we have more chances to detect the one quarter only to look into. 66 00:12:02,880 --> 00:12:13,440 Guillermo Mena: OK, so the other point that we see is that the predictions, we believe strongly on the choice of vacuum in state they have we essentially three proposals in this. 67 00:12:14,700 --> 00:12:24,060 Guillermo Mena: direction one is the use of the article states that is a way in sentences of the analyzer networks which are working for me because, being other situations. 68 00:12:24,810 --> 00:12:35,160 Guillermo Mena: A person there is to what extent is a natural thing clearly quantum regimes, and they are things that they typically lead to oscillations that when our age. 69 00:12:35,640 --> 00:12:47,010 Guillermo Mena: Can in haste, the power in the spectrum because of that, it has also been proposed to find a stage that minimize the circulation is called an oscillating vacuum. 70 00:12:47,550 --> 00:13:03,240 Guillermo Mena: In this case, the progress in which regions we want who a let's say a minimize the installation just in the quantum a bridging also in the non standard classical period or in the combination of both of them. 71 00:13:03,750 --> 00:13:21,060 Guillermo Mena: Are the things that typically this a minimization of their solution is done numerically and we would like to have a night characterization of these kind of popular is because, when done peacefully connection with the young, as in particular violate that have only session. 72 00:13:22,530 --> 00:13:35,670 Guillermo Mena: Now the third proposal is what typically our usually we put they asked like a good presentation proposal essentially is to sing a family office space around the wound and. 73 00:13:36,450 --> 00:13:48,660 Guillermo Mena: From then in the Center it minimizes the contrast, these are they are compatible with homogeneity and so to be and to sing one of them by semi classical requirements at the end of inflation. 74 00:13:49,260 --> 00:14:09,450 Guillermo Mena: Of for a approaches that are not the best metric a there are certain is in the definition that should be somehow let's say a clean out or improve, and we are things not clear how to extend their their proposal to GR because there is no bounds okay so then we just sorry. 75 00:14:11,730 --> 00:14:20,640 Guillermo Mena: Let me just finish I essentially vesely this task to kind of feeling of order but we that the prediction will be so sensitive. 76 00:14:21,150 --> 00:14:27,930 Guillermo Mena: So back in that we cannot say anything to at least let me send the following message which I think is important. 77 00:14:28,290 --> 00:14:38,040 Guillermo Mena: We should look for a vacuum and state that the first thing is that the changes with respect to once babies have a small just for setting It ranges of wavelength of mostly say. 78 00:14:38,640 --> 00:14:48,480 Guillermo Mena: The other things I should be based on first principle is not that we forced the vacuum, just to obtain the power spectrum that we have set, this will not be satisfactory. 79 00:14:49,020 --> 00:14:58,620 Guillermo Mena: They are theory, they should be appealing optimally other dynamics in particular around the bounce it should be sensitive to the escape that intrinsic or. 80 00:15:00,090 --> 00:15:03,240 Guillermo Mena: So, thank you very much, these will, I want to say. 81 00:15:05,400 --> 00:15:07,530 Jorge Pullin: Thank you very much, can you please stop sharing. 82 00:15:13,470 --> 00:15:14,220 Jorge Pullin: Please go ahead. 83 00:15:34,650 --> 00:15:34,950 Jorge Pullin: Good. 84 00:15:37,980 --> 00:15:49,560 Daniele Oriti: will discuss how cosmological economics can be seen from the point we have quantum gravity framework, so this sort of embedding. 85 00:15:50,730 --> 00:16:00,720 Daniele Oriti: conceptual and technical into the full framework of forces as the potential water company mutations of cosmology. 86 00:16:02,100 --> 00:16:03,870 Daniele Oriti: to test the results that. 87 00:16:05,130 --> 00:16:17,640 Daniele Oriti: they've been doing so far in that context and out say important to to raise your questions, because you see things from a different perspective so most of my discussion with the goal of simply. 88 00:16:20,100 --> 00:16:30,030 Daniele Oriti: elements for later discussion will stop to think about it is closely based on development say security formulation of. 89 00:16:30,960 --> 00:16:38,010 Daniele Oriti: gravity and so there will be, of course, is very many connections to the quantum gravity from families. 90 00:16:38,700 --> 00:16:57,300 Daniele Oriti: But despite it being most inspired by results in a particular direction that I would claim that the results cern's most of the insights and the other more general validity, so the first point is that if we think about cosmological dynamics. 91 00:16:58,470 --> 00:17:08,190 Daniele Oriti: To to focus on cosmological elements from the point of view of the curious to me basically restricting attention to a few global observable. 92 00:17:09,420 --> 00:17:13,230 Daniele Oriti: In fact, this is to also from the point of view of generativity. 93 00:17:14,250 --> 00:17:27,720 Daniele Oriti: This means from the full quantum gravity point of view, to focus on some collective variables so collective observable and collective states, this means that cosmology sugar should arise from some form of course brain. 94 00:17:29,280 --> 00:17:33,630 Daniele Oriti: Now, because grading in general is expected to be very difficult. 95 00:17:34,650 --> 00:17:51,540 Daniele Oriti: And symmetry reduction, which is what gives rise to cosmology can be seen in fact that's a very drastic type of constraining agree to simply remove an infinite number of degrees of freedom not directly correspond to the global observable you're interested in. 96 00:17:52,950 --> 00:17:59,220 Daniele Oriti: Now this reduction in general, if you perform it at the quantum level is a singular from the point here. 97 00:17:59,970 --> 00:18:12,840 Daniele Oriti: These are called doesn't mean that there's anything necessarily wrong with that, but I should expect the ICO screening that is less drastic to produce modifications to the results i'm creating more articles. 98 00:18:14,070 --> 00:18:19,800 Daniele Oriti: In fact, what happens at least in the refrigerator framework is that we, after some. 99 00:18:20,940 --> 00:18:37,680 Daniele Oriti: Drastic but not that drastic action within the future if we do obtain a cosmological where we function on being super space as the dynamical variable but it's actually a thing this is sort of always parameter labeling collective states it's not a quantum state itself. 100 00:18:39,600 --> 00:18:46,110 Daniele Oriti: It does correspond to something like another dynamic density, whose domain is being used to perspective. 101 00:18:47,490 --> 00:19:04,350 Daniele Oriti: So in this simple as approximation just that there is a field operator and it says potential value in a given troy's of ground State there is will give some the cosmological we function of mutual respect and then this way function, just like in. 102 00:19:06,150 --> 00:19:09,960 Daniele Oriti: Three like in terms of some density, for your fluid that some face. 103 00:19:11,010 --> 00:19:17,880 Daniele Oriti: Now this is technical consequences, I just want to point out one conceptual concepts means that the. 104 00:19:18,420 --> 00:19:36,690 Daniele Oriti: This is the case, he is is how a cosmological way we function liking quantum cosmology consultant from the hood cheery there is no corresponding he'll be space for the status of such we functions, so there is of course the underlying code base base of quantum gravity states but. 105 00:19:37,740 --> 00:19:42,900 Daniele Oriti: there's no restricted Hebrew spaces such as we functions within the food to. 106 00:19:45,030 --> 00:20:06,630 Daniele Oriti: The other consequences that the observable to automatically be with continuing gravitational physics, as ever, just not as eigenvalues so the quantity as to play the role of the scale for the for the universe in in such either Ivanovic like personal journey some appropriate average. 107 00:20:07,650 --> 00:20:11,670 Daniele Oriti: weighted by the density of the fluid the l some variable. 108 00:20:13,860 --> 00:20:24,960 Daniele Oriti: Okay at this level, in an important role will be played necessarily by some quantity play somehow enabling or counting the number of degrees of freedom. 109 00:20:26,040 --> 00:20:32,580 Daniele Oriti: In this specific context that, like I mentioned grew from theory, this is given by the. 110 00:20:33,480 --> 00:20:47,580 Daniele Oriti: integral models for the way function so is, in fact, that the literally the average number of the right or the microscopic building blocks, and this is in fact an observable in the quantum theory that has no counterpart that. 111 00:20:48,000 --> 00:21:06,960 Daniele Oriti: If you just look at quantum cosmology itself as an observer, where that enters the dynamics and evaluation of interesting quantities and particularly is crucial to do fluctuations small and to define a semi classical really large volumes. 112 00:21:08,340 --> 00:21:18,030 Daniele Oriti: The second main point, the following from the five minute, you see, the smaller the essence of the American effective coarse grained the dynamics. 113 00:21:18,540 --> 00:21:34,320 Daniele Oriti: And literally in the EU feature comparison some sort of idle dynamics, we find a pencil such a cosmological we functional neutral space is that the dynamics for such effective way function is genetically nonlinear. 114 00:21:35,460 --> 00:21:49,140 Daniele Oriti: This is what you should expect in general, whenever you do some cross training or go to some either dynamic approximation, but of course it means that even assuming that the linear part the bh like loop on to cosmology equation. 115 00:21:50,430 --> 00:21:57,870 Daniele Oriti: There would be no linear addition to that which may have any general has cosmological consultancies. 116 00:21:59,640 --> 00:22:09,840 Daniele Oriti: and number of other points, is that the gravitational coupling said that you see it is effective lever once you match it GR are in fact functions of the underlying. 117 00:22:10,170 --> 00:22:15,750 Daniele Oriti: parameters in coupling so the quantum gravity formulas that may not be directly. 118 00:22:16,470 --> 00:22:30,450 Daniele Oriti: interpret this gravitational because there's No one to one correspondence between parameters in the effective dynamics and parameters in the fundamental one and meaning that I don't know something like effective gravitational constant would be a function of several. 119 00:22:31,530 --> 00:22:33,480 Daniele Oriti: The parameters of the microscopic here. 120 00:22:35,820 --> 00:22:46,020 Daniele Oriti: The linear restriction would look at these formulas much more like a standard open to cosmology setting still without an associated to the space. 121 00:22:48,030 --> 00:22:51,390 Daniele Oriti: The reason why there's no hyperspace and maybe I should have said, literally simply that. 122 00:22:52,710 --> 00:22:59,730 Daniele Oriti: Generic question for your way function well, I know superposition software solutions to not be the solutions. 123 00:23:02,760 --> 00:23:10,410 Daniele Oriti: Okay, by the way, is nonlinear contributions, at least in a very simple cases if we were able to study them and. 124 00:23:12,270 --> 00:23:27,660 Daniele Oriti: Their contribution to the cosmological dynamics that seem to be actually bought the genetically the the the seems to some cosmic acceleration and normally I never made at times and so some form of effective that kind of. 125 00:23:30,750 --> 00:23:47,670 Daniele Oriti: Okay, an interesting question, at least for me is that if you see cosmology this second as some sort of condensate that open army said they would be expectations out of the condensate and it's unclear to me, first of all, these have to be. 126 00:23:49,350 --> 00:24:08,250 Daniele Oriti: treated so to give some modification of the cosmological genomics for a given company to the universe described by the arguments for the way function or somehow that can be mapped to some new form of content for the universe and effective new motor component what is. 127 00:24:10,800 --> 00:24:12,900 Daniele Oriti: The next point, which is a general. 128 00:24:14,280 --> 00:24:24,780 Daniele Oriti: For quantum gravity Again I say, and we have to really rely on this is hugely in starting cosmology from theory is that. 129 00:24:25,860 --> 00:24:34,530 Daniele Oriti: evolution can only be relational, and so we need to select some degree of freedom to play the role of clock, but we also have some conditions. 130 00:24:35,700 --> 00:24:45,540 Daniele Oriti: Also, that such clock is in fact that a good clock and these are conditions from the relevant quantum states that they will allow instructional cosmological dynamics. 131 00:24:47,580 --> 00:24:59,790 Daniele Oriti: It should work with the eigenvalues of the clock this corresponds to the point of your the jury to inflict the big states, and this is, it would be highly fluctuating conjugate. 132 00:25:00,720 --> 00:25:11,340 Daniele Oriti: degrees of freedom to the clock runs and now the questions that I am be very interesting interested in hearing your. 133 00:25:12,030 --> 00:25:17,550 Daniele Oriti: opinion and learning more about that that is what are the conditions for choosing o'clock. 134 00:25:18,360 --> 00:25:26,430 Daniele Oriti: Within the food Curie and, in general, cosmology and and the fact that they could be especially in these calls green setting and mismatch. 135 00:25:27,300 --> 00:25:32,400 Daniele Oriti: Between the fundamental club degrees of freedom and the effective once I give you an example. 136 00:25:33,240 --> 00:25:44,220 Daniele Oriti: suppose that I counseled to full quantum quantum gravity or goofy curious so at the level of the fundamental degrees of freedom which are discrete tech citations I know. 137 00:25:44,910 --> 00:25:54,720 Daniele Oriti: pathological geometries in general I couple what looks like a well defined must less free scared of you like some form of this presentation. 138 00:25:55,560 --> 00:26:07,320 Daniele Oriti: Then I do some custom training at the effective level there's no obviously reason respected this sector, because the freedom will behave exactly like a muscle is scared of you. 139 00:26:08,700 --> 00:26:09,480 Daniele Oriti: It may be some. 140 00:26:10,530 --> 00:26:14,400 Daniele Oriti: Potential generated by the equals granting some of the features of the. 141 00:26:15,660 --> 00:26:25,980 Daniele Oriti: dynamics, more general, and this is important because, of course, I would like to choose his master's get a field as a clock from the point of view, the fundament theory. 142 00:26:26,520 --> 00:26:33,750 Daniele Oriti: And then I may want to treat it as a clock at the effective cosmological level at this quarter screen there either ergonomic level. 143 00:26:34,200 --> 00:26:52,110 Daniele Oriti: But if you factor in effect the potential is generated by the current sprint procedure and it treated as a Muslim says get a few people that was my interpretation I problems matching with the results of dynamics written international language to such clock. 144 00:26:53,790 --> 00:27:04,950 Daniele Oriti: So this is, you should do to be taken into account and then questions that to do again with the how much physics actually depends on the choice o'clock or whether we should expect environments. 145 00:27:05,310 --> 00:27:22,260 Daniele Oriti: physics and machine to physical clock so realistic clocks with their own interaction back reaction, the geometry, and so on, and what is it from relational general covariance as transformations between the physical frames no coding frames. 146 00:27:23,700 --> 00:27:40,350 Daniele Oriti: Okay, everything I said about the clock, in fact, actually be generalized the two routes and that the important point to me is that, from the funding from the point of view, the fundamental theory if I want we struck a cosmological dynamics between the two nations. 147 00:27:41,430 --> 00:27:56,430 Daniele Oriti: I also had to express that cosmological perturbation cheering relational terms of respect to such internal charges of internal degrees of freedom playing the role of routes and the number of issues arise here i'll go. 148 00:27:58,050 --> 00:28:02,820 Daniele Oriti: will not discuss each of them, so that there may be more time later for discussing. 149 00:28:03,480 --> 00:28:13,110 Daniele Oriti: And let me just say that up the ori if I only look at the arguments would be effective, we function as a standard mini super space in which I see the skatepark. 150 00:28:13,770 --> 00:28:21,570 Daniele Oriti: Some additional matter component, that the math degree of freedom my users o'clock and then master degrees of freedom my users rob's. 151 00:28:22,170 --> 00:28:34,080 Daniele Oriti: I can start you're ready to be sure to read this level, even though i'm working just with the world looks like initial space, because I can express relational observable with respect to. 152 00:28:34,800 --> 00:28:39,330 Daniele Oriti: The subset two degrees of freedom given by values of their own fields. 153 00:28:39,780 --> 00:28:58,680 Daniele Oriti: So, clearly, this can only be an approximation to the full story, because the full story requires full super space, not just that it functional municipal space that it is to admit after them clear to me in which approximation actually respect that this limited description, with some validity. 154 00:29:02,970 --> 00:29:15,840 Daniele Oriti: Last, I just want to mention that, if cosmology comes out of this effective level as either dynamics so first of all it takes place in one particular phase continuing phase of the underlying system. 155 00:29:16,500 --> 00:29:32,280 Daniele Oriti: So important role will be played by the running of the various couplings and we need to check what happens at criticality so like for critical various have such carbons because it will affect because one of the most effective equals more experiments. 156 00:29:33,510 --> 00:29:48,990 Daniele Oriti: In particular, when general consequence is that that the bouncer that seems to be reproduced in the world that has been done so far, just like you know, to see if he's the from the point of view, the effective dynamical equations. 157 00:29:50,040 --> 00:29:57,600 Daniele Oriti: It is reproduced in what is actually a very dangerous zone, not for the other Apps image because small values. 158 00:29:58,230 --> 00:30:06,180 Daniele Oriti: correspond to smoke that uses the number operator in the volume is an extensive quantified in terms to the number of degrees of freedom. 159 00:30:07,020 --> 00:30:17,700 Daniele Oriti: And so the bounces in the redeeming Richard not really certain about the validity of the other for the approximate overall just accepting very few degrees of freedom. 160 00:30:19,200 --> 00:30:37,170 Daniele Oriti: And so it could be that, depending on the order, depending on the dynamics the bouncing fact that can be trusted their own in some for a subclass states it but genetically need to resolve to describe the corresponding physics, to the more fundamental economics, which doesn't have. 161 00:30:38,700 --> 00:30:41,400 Daniele Oriti: affected the space time description. 162 00:30:43,170 --> 00:30:49,890 Daniele Oriti: Okay embedding everything the food, you should allow that he, I asked for help, because I don't know how to do it. 163 00:30:50,310 --> 00:31:03,540 Daniele Oriti: should be allowed to ask questions about yarrow time and the initial state of the universe, because it should allow or to ask questions I will give them from the entropy and here interesting issues. 164 00:31:04,770 --> 00:31:07,110 Daniele Oriti: to differentiate the entropy the food. 165 00:31:08,190 --> 00:31:23,040 Daniele Oriti: system and the entropy of the universe, from the point of view of the physical frame, we are chosen to describe evolution and localization because that requires singling out that not considering and subset degrees of freedom. 166 00:31:24,600 --> 00:31:36,180 Daniele Oriti: you're going to answer these type of questions to have a better foundation for statistical mechanics quantum gravity in absence of any preferred time that action in this is a general issue. 167 00:31:37,440 --> 00:31:44,820 Daniele Oriti: Last the I mentioned that I know running of goblins and criticality and face traditions, well, it. 168 00:31:45,840 --> 00:31:51,360 Daniele Oriti: should be able to us whether the face rendition of the underlying system. 169 00:31:52,560 --> 00:32:10,350 Daniele Oriti: As a cosmological individual itself being close to criticality affects the spectrum of cosmological perturbations, for example, if criticality is related to the early universe Okay, and there are many more things that, of course, they don't mention, and I thank you, Mr. 170 00:32:12,090 --> 00:32:13,950 Jorge Pullin: Thank you, please, share your screen. 171 00:32:15,120 --> 00:32:15,360 yep. 172 00:32:18,030 --> 00:32:18,660 Jorge Pullin: So Yvonne. 173 00:32:24,690 --> 00:32:25,920 Jorge Pullin: you're muted, I think. 174 00:32:32,820 --> 00:32:34,230 Ivan Agullo: Can you hear me now yes. 175 00:32:35,700 --> 00:32:36,960 Ivan Agullo: And so. 176 00:32:37,350 --> 00:32:49,200 Ivan Agullo: In the last part of this of this panel, I want to give you a global and simplified and of course bias by my personnel, be a. 177 00:32:50,100 --> 00:33:09,570 Ivan Agullo: comments on the connection between ltc and and observations and and so, first I want to make contact with many things that the urinal have said and also partially daniella, of course, all this is the summary of contributions by many people. 178 00:33:10,740 --> 00:33:19,290 Ivan Agullo: And I list them all here, probably forget some people I apologize, but rather than then mentioned them one by one, just for the sake of of time. 179 00:33:20,100 --> 00:33:29,340 Ivan Agullo: And so, and and the main ingredients of of help you see as as both be your mind and daniella has mentioned is similar to production. 180 00:33:29,730 --> 00:33:40,650 Ivan Agullo: which we know is a drastic simplification and important physics can be missed the motivation is historical motivation, you know scimitar of action has been. 181 00:33:41,280 --> 00:33:53,850 Ivan Agullo: essential tool to make progress in physics in gravity cosmic physics, etc, etc, so we want to follow the same the same approach, without forgetting about how drastic the simplification is. 182 00:33:55,110 --> 00:34:07,500 Ivan Agullo: That nearly also mentioned that, from the viewpoint of the full theory, it is not there is no canonical homogeneous and I satrapi sector and in gfp that he studies very clear, that is not even a better space. 183 00:34:08,130 --> 00:34:18,480 Ivan Agullo: For the genius and for the cosmological sector a Annie oakley G dynamically, the problem is even worse because we don't even have hamiltonian on which we agree on. 184 00:34:19,050 --> 00:34:34,350 Ivan Agullo: So it is difficult to argue whether ltc is compatible with the dynamics of our full theory which we don't really agree on, so this is rather a to a breach each you know both benefit each other. 185 00:34:36,120 --> 00:34:48,870 Ivan Agullo: So, but in spite of these limitations, in my view is that this this field has been built using what I call a physicist viewpoint, in which you know. 186 00:34:49,830 --> 00:35:01,260 Ivan Agullo: model or quantum theory of the cosmos has been built a you know, using what we know from the full ferry trying to encourage as much as we can to the full theory. 187 00:35:01,920 --> 00:35:21,870 Ivan Agullo: and making simplifications and when we don't have the tools to anchor to the full theory just make responsible choices using physical intuition and general experience from other from other fields, and we do that, you know, with the goal of building a self consistent model. 188 00:35:23,070 --> 00:35:32,970 Ivan Agullo: Out of which we can connect with observations and i'm also with other frameworks for the every universe, such as inflation or a standard model, etc. 189 00:35:33,390 --> 00:35:43,290 Ivan Agullo: And you know, the main goal is to aim at that data driven approach you know, try to make contact with observation, in spite of the simplifications that we leave on the way. 190 00:35:44,010 --> 00:35:58,020 Ivan Agullo: And, and this should provide, and this is the last sentence of this of this slide the foundations for further scrutiny and improvement and and many examples have been shown in daniella in Danielle West contribution. 191 00:35:59,280 --> 00:36:03,030 Ivan Agullo: So this is the goal so several things have been. 192 00:36:04,620 --> 00:36:17,430 Ivan Agullo: achieved so far, the main one that we all know, is singularity every solution, and this has been done, following the general approach of focusing the general. 193 00:36:18,660 --> 00:36:28,050 Ivan Agullo: A program of starting first with the simplest model and then adding difficulties, one by one, like a special code mature and so to be. 194 00:36:28,890 --> 00:36:39,750 Ivan Agullo: Even infinitely many degrees of freedom in go the models, etc, and so far indications seem that this resolution is robust and I think you know they. 195 00:36:40,200 --> 00:36:56,400 Ivan Agullo: The analysis provides a very interesting understanding or example of how you know the peculiarities of of look quantum gravity kind of help ass to get rid of similarities of the classical theory, so there are very interesting messages that. 196 00:36:57,540 --> 00:37:08,520 Ivan Agullo: I faced have many choices are in the way which means to be a father justified or anchor to a more fundamental viewpoint but but but and we don't need to forget about them. 197 00:37:09,690 --> 00:37:21,180 Ivan Agullo: And so far, you know the relations of milk, you see, with a full full El que je and N, and you know, there are several in the market very interesting. 198 00:37:22,680 --> 00:37:34,950 Ivan Agullo: avenues, and it seems that this singularity of a solution so far as a common denominator of of most of them, and even the pause bounce feigns face seems to be a robust. 199 00:37:35,820 --> 00:37:51,720 Ivan Agullo: Interestingly, some differences appear in the p bounce face and they even lead to different observational predictions so So these are an example of this to a bridge between ltc an energy, which I find very, very interesting. 200 00:37:54,150 --> 00:38:05,310 Ivan Agullo: Okay, so so after this brief a connection with the full theory, let me go to the main topic phenomenology I think you know the motivation is not really needed here. 201 00:38:06,240 --> 00:38:16,860 Ivan Agullo: We all are physicists and we know how important is to make contact with observations, and in particular for cosmology right because in cosmology a you know. 202 00:38:17,460 --> 00:38:32,190 Ivan Agullo: The blank area of the cosmos is within our past life COM is not hidden behind an event horizon, so you know we don't need Planck scale physics to leak out of a horizon to be observable. 203 00:38:32,970 --> 00:38:43,620 Ivan Agullo: Rather, what we need is that blanket scale physics pseudo base all the complications of the history of the cosmos you know blank skill physics, is not washed away. 204 00:38:44,130 --> 00:39:02,580 Ivan Agullo: By the complex physics, of the cosmos between today and the banker and and we are aware of that many of the of the blank escape features are going to be washed away, so there is some limited what we can get now from the early universe, and the question is, what exactly those limits are. 205 00:39:04,350 --> 00:39:07,710 Ivan Agullo: So what we have learned so far. 206 00:39:08,880 --> 00:39:13,260 Ivan Agullo: And is you know i'm going to summarize a few messages for the sake of time. 207 00:39:13,770 --> 00:39:25,050 Ivan Agullo: The first one is failure of theoretical is something that I find very interesting is that ltc starts from our natural geometry that one done geometry described by away function. 208 00:39:25,500 --> 00:39:37,500 Ivan Agullo: A, out of which there is no clear notion of counsel structure, however, once you put one on feels propagating on that fundamental geometry. 209 00:39:38,010 --> 00:39:48,210 Ivan Agullo: and imagine a pseudo Romanian effective geometry appears, out of which one can talk about cost structure, and I think this is something that. 210 00:39:48,750 --> 00:40:04,560 Ivan Agullo: You know, we expect in general, from quantum gravity that the cost structure images once you have fields proving the quantum geometry, and you know, a very nice example we may view be in you know you'll see. 211 00:40:07,620 --> 00:40:21,720 Ivan Agullo: Next that's ltc provide a mechanism to generate the primordial so perturbations that we seem to see me and almost a scaling bottom a spectrum, and that was the initial hump and so far, the answer is no. 212 00:40:22,860 --> 00:40:23,220 Ivan Agullo: No. 213 00:40:25,620 --> 00:40:32,100 Ivan Agullo: The problem navy's that help you see maybe it's too simple, we only have the blank escape you know to see. 214 00:40:32,640 --> 00:40:43,290 Ivan Agullo: And it's difficult to see how the inflationary scale, you know energies game, for instance, is going to emerge out of accuracy so so look you see it's not enough so far. 215 00:40:44,130 --> 00:40:53,070 Ivan Agullo: Maybe dressing ltc or going beyond that you see will provide additional structure, out of which we can build a. 216 00:40:53,940 --> 00:41:01,200 Ivan Agullo: mechanism and and daniella provide a very nice and intriguing example from from God, he told us that you know. 217 00:41:01,710 --> 00:41:05,010 Ivan Agullo: The nonlinear couplings between you know this fundamental. 218 00:41:05,370 --> 00:41:17,820 Ivan Agullo: structure, you know provide newest structures, out of which one could build an effective cosmological content so and there is an example of how dressing accuracy with something more complex may may solve. 219 00:41:18,480 --> 00:41:27,360 Ivan Agullo: may be young the limitations of hypocrisy, but so far you look, you see, that is not the case, so if you see has been used to complement other mechanism. 220 00:41:27,810 --> 00:41:45,600 Ivan Agullo: To extend well known mechanism in the market to the blank escape and with the with the goal of completing completing them from the quantum gravitational viewpoint and hopefully to add some extra features, to the baby chance that we can test with observations. 221 00:41:46,890 --> 00:42:05,550 Ivan Agullo: That is the goal of this program so far, and you know in this to cartoons I illustrate that you know, the main idea why the balance of focusing can affect the cmt here in red, you may have seen this this before I have shown them many times, this is one more. 222 00:42:06,870 --> 00:42:17,940 Ivan Agullo: In red is the the the radius of curvature of these emerging geometry that better patients feel, and this is the case of the you know, on the left. 223 00:42:18,420 --> 00:42:28,890 Ivan Agullo: You have the the GR with a big bang on the right, what happens with a bounce the red line and and then in blue are the wavelength, of a few perturbations. 224 00:42:29,460 --> 00:42:39,090 Ivan Agullo: as a function of time and we see that in the right hand side in the right blood that the wavelengths are long enough, they become comparable. 225 00:42:39,930 --> 00:42:48,510 Ivan Agullo: To the quarterback for Sky, the bounce and because of that they will defeat the evolution of the special operations is modified by the presence of the bounds. 226 00:42:48,990 --> 00:43:02,700 Ivan Agullo: shorter shorter wavelength don't care about the balance for the same reason that we don't care about the curvature of the earth, he is different, but longer wavelength care about the balance and that notification will be imprinted in the CME. 227 00:43:03,930 --> 00:43:23,640 Ivan Agullo: Remember the cms our history book, and these are the the accidents that are registered in the car so so so so so therefore from from from from a bounce we expect some quantum route you some corrections at long wavelength large chunk rather scales in the sky. 228 00:43:26,520 --> 00:43:44,100 Ivan Agullo: Okay, but when trying to make concrete predictions are there free parameters that we need to choose, and the answer is, of course, there are three parameters, yes, a few of them are a how much expansion, there is between the balance and let's say today. 229 00:43:45,810 --> 00:43:49,620 Ivan Agullo: That is something the theory doesn't fix and it's a free Parliament. 230 00:43:50,850 --> 00:43:59,130 Ivan Agullo: What is the initial state for perturbations that was discussed by nicely by a baby or more in detail, etc. 231 00:43:59,730 --> 00:44:06,990 Ivan Agullo: And to me, this is not surprising, you know all there is we, like a love are free of us are full of free parameters. 232 00:44:07,410 --> 00:44:21,450 Ivan Agullo: In Dr Dr there is no a solution for the universe, that is a family of solutions and we choose when using using data right a standard model inflation, etc, so this is this is great expected from my people. 233 00:44:23,130 --> 00:44:39,390 Ivan Agullo: The important question are the choices of these parameters for use in agreement with data and the answer is yes, there is in fact a huge window for which we can you know, complete the standard model completely inflationary paradigm, and still have agreement with observations. 234 00:44:41,310 --> 00:44:51,120 Ivan Agullo: Can we Father single out a concrete choice of initial data and the program so far has been you know, has followed this ambitious strategy. 235 00:44:52,380 --> 00:45:08,130 Ivan Agullo: The strategy, the ambitious strategy is you know, is to use these anomalies that the year more has mentioned, which are features that we seen the cmt and cannot be explained by by the standard model. 236 00:45:09,150 --> 00:45:24,150 Ivan Agullo: One by one, they are not very significant statistically just below or around 30 cygnus but collectively as we are must bring to us, they may tell us that there is new physics at lunch and worst case, in the end. 237 00:45:24,720 --> 00:45:34,170 Ivan Agullo: So the program is whether ltc a weather in ltc that is a choice of the parameters, the free parameters that make. 238 00:45:35,370 --> 00:45:37,680 Ivan Agullo: That make excuses to account for the song. 239 00:45:39,180 --> 00:45:47,790 Ivan Agullo: Again, this is what I mentioned before, as you know, as a data driven approach use what we see in the sky to fix our our our freedoms. 240 00:45:48,450 --> 00:45:56,010 Ivan Agullo: And they also using different methods and there are many avenues that people have follow and do that. 241 00:45:56,580 --> 00:46:08,250 Ivan Agullo: i'm going to explain you one of them, just for the sake of time, and also because I am by yes i'm going to explain you the one I have contributed more recently, which has to do with nano China. 242 00:46:10,290 --> 00:46:27,600 Ivan Agullo: So remember nano shiny, these are the effects of the next to lead in order there in perturbation theory the lead in order is free penetration theory next to lead in order you have a self interactions between perturbations and they produce what we call non oceanic. 243 00:46:28,830 --> 00:46:42,480 Ivan Agullo: One of the effects is that the three point correlation function, you know the three point functioning there in real space is different from zero and zero if you neglect self interactions between perturbations. 244 00:46:43,680 --> 00:46:51,270 Ivan Agullo: And he I know our group, we have computed this number of shiny piece in full detail I am doesn't even you 30 seconds summary. 245 00:46:52,170 --> 00:47:07,530 Ivan Agullo: And the main message is is that there is a choice of parameters of the theory for the week this notion correlations are sad that within our humble back this is what I what I. 246 00:47:08,670 --> 00:47:17,550 Ivan Agullo: mean by this conference that I would have a badge within our hubble patch they don't know Shannon these are small and below observational upper bounds. 247 00:47:20,880 --> 00:47:29,970 Ivan Agullo: And however they are large enough to buy gas or to affect it's likely the coupon correlation. 248 00:47:31,740 --> 00:47:44,340 Ivan Agullo: And this affects a they can produce in a very subtle and concrete manner that by i'm not explaining here a several of the anomalies that we see in the in the sky. 249 00:47:45,060 --> 00:48:03,630 Ivan Agullo: such as this forward suppression, but the information also these bipolar anomaly, which looks completely different from poverty pressure they bought anomalies as a sort of be in one direction in the sky and that can can image in a concrete manner by by this notion motivations, etc, etc. 250 00:48:05,400 --> 00:48:16,830 Ivan Agullo: Even more than that you know these results have been have attracted the attention of some well known cosmologist that has nothing to do with with milk, you see. 251 00:48:17,370 --> 00:48:27,180 Ivan Agullo: A and, and these are these are very recent paper October last year and and what they say, is the following, you know just just to. 252 00:48:27,750 --> 00:48:37,710 Ivan Agullo: To summarize what they do, let me use this analogy with Lego data in Lego data, we know that the signal is will be young will below the noise. 253 00:48:38,220 --> 00:48:47,100 Ivan Agullo: And you may wonder how the hell, can we see the signal when the signal is well below the nose and the reason is because we have a template. 254 00:48:47,910 --> 00:48:59,430 Ivan Agullo: If we know if you know what the shape of the signal should be you can accumulate enough signal to noise ratio, even if the signal is buried under denies. 255 00:49:00,990 --> 00:49:09,360 Ivan Agullo: The same This is exactly what they say here, because you know because we provide our template the shape of they don't go Shannon. 256 00:49:10,800 --> 00:49:24,810 Ivan Agullo: You know, out of a bounce of accuracy, a if you know the shape, you may accumulate enough signal to noise ratio and, in principle, you know this signal can be detected using blank data. 257 00:49:25,620 --> 00:49:33,780 Ivan Agullo: And I am aware that they are doing that that analysis so so I find quite interesting that cosmology is happy nothing to do with accuracy. 258 00:49:34,890 --> 00:49:39,960 Ivan Agullo: use our templates to look signals in data, you know in observational data. 259 00:49:42,240 --> 00:49:50,040 Ivan Agullo: And just to finish, let me finish with with three comments and and be some similar strategies come together with further predictions. 260 00:49:50,760 --> 00:50:03,900 Ivan Agullo: of things for most in particular optical depth, etc, and we are waiting for data, in particular for cancer modes and and once the data is here all these predictions will come out on the table again. 261 00:50:06,120 --> 00:50:12,330 Ivan Agullo: Similarly to what happens with gravitational waves, many of the subtleties of mathematical GR now are. 262 00:50:12,840 --> 00:50:26,670 Ivan Agullo: Are are interesting again because we have data so once we see things for themselves if we see them, then this will be part of the game and there are other places where quantum gravity could be useful. 263 00:50:27,990 --> 00:50:39,030 Ivan Agullo: daniella has mentioned, you know whether quantum gravity can produce and imagine cosmological constant either for the area of like you say like time universe. 264 00:50:39,570 --> 00:50:53,460 Ivan Agullo: Also, they have attention, whether you know quantum gravity Can I take that and I know that Alejandro barriers Edwin Edwin Edwin danielle's with our ski they have arguments with that etc. 265 00:50:54,720 --> 00:50:55,650 Ivan Agullo: So just to finish. 266 00:50:56,760 --> 00:51:16,140 Ivan Agullo: We all know that that that that elk you see it's very simple and it's made of drastic simplifications a bad it provides a complete model, out of which we can connect in a concrete manner and precise manner, one to gravity with observations and. 267 00:51:16,500 --> 00:51:19,890 Abhay Vasant Ashtekar: And even do anything on the slide we only see final comments. 268 00:51:19,890 --> 00:51:21,630 Ivan Agullo: yeah no I don't have anything just might want. 269 00:51:23,940 --> 00:51:32,400 Ivan Agullo: Thank you anyway and and so so and and and so ltc provides a concrete path a concrete, you know. 270 00:51:32,880 --> 00:51:45,360 Ivan Agullo: A way of connecting fundamental quantum gravity with observations and and, of course, many things we will be modified in the future and many new inputs will become will come from the from the full ferry. 271 00:51:46,020 --> 00:52:06,210 Ivan Agullo: But it is my view that this path that bill QC has produced, even though it is based on assumptions and physical intuition, you know it is, it is real progress, which will allow us to dress it farther and modify what it needs to be modified and am I going to stop stop here, thank you. 272 00:52:07,560 --> 00:52:09,690 Jorge Pullin: Thank you, we can now take questions. 273 00:52:13,980 --> 00:52:14,700 Jorge Pullin: Western please. 274 00:52:16,170 --> 00:52:17,490 Parampreet Singh: Can I ask some questions. 275 00:52:18,750 --> 00:52:20,580 Jorge Pullin: Western raise their hands sorry. 276 00:52:24,840 --> 00:52:25,290 So. 277 00:52:26,580 --> 00:52:30,270 If I, if I may, pick up the from the last. 278 00:52:32,760 --> 00:52:33,660 Talk by. 279 00:52:34,950 --> 00:52:42,990 by Eva and I have, I was pleased to see that he mentioned the problem of generating primordial. 280 00:52:44,760 --> 00:52:51,000 perturbations, I just wanted to mention that we have been portrayed in a research direction. 281 00:52:53,520 --> 00:52:56,130 Sorry, to address this problem man. 282 00:52:57,630 --> 00:53:11,580 Western: That is so it was reported in in Asia paper called the promoter fluctuations from quantum gravity and the idea is to use as a vacuum state the heart looking state resulting from. 283 00:53:12,660 --> 00:53:25,140 This being formed dynamics so it's an approach based on on the full theory of the food from dynamics and what we have is the possibility to compute correlations. 284 00:53:25,770 --> 00:53:42,420 From the full theory, and so the limitation of our first paper was that it was a very simple model we look for the for the loop conference to present the results, in particular, so these results are made possible by the advances in numerical methods, especially by students of ours. 285 00:53:44,070 --> 00:53:44,940 Follow frisoni. 286 00:53:46,200 --> 00:53:56,940 And the the the results we have so far that there could be there could be more entanglement stronger correlations than what is expected in the usual. 287 00:53:58,110 --> 00:54:15,480 bunch of previous state, so I mean afternoon, my comment, the reason why I mentioned, this is also to make a call for collaborators, so if more students and postdocs want to join us in this The challenge now is to connect. 288 00:54:16,590 --> 00:54:24,360 With an effective states that can be used for instance with the standard the loop cosmology techniques. 289 00:54:26,220 --> 00:54:31,200 Ivan Agullo: Wonderful fantastic Thank you I didn't know what that and I am looking forward to see the details. 290 00:54:33,180 --> 00:54:33,630 Jorge Pullin: Around. 291 00:54:34,860 --> 00:54:35,190 Jorge Pullin: Oh. 292 00:54:35,250 --> 00:54:41,970 Parampreet Singh: So my first question is to gamma gamma in your very last slide you showed a lot of the power spectrum probably one with the. 293 00:54:43,530 --> 00:54:53,460 Parampreet Singh: oscillating state idiomatic states what's the glucose so I was wondering where does that glucose which has a lot of power suppression comes from is that from milk, you see some water. 294 00:54:54,240 --> 00:55:01,980 Guillermo Mena: Yes, it can strong oscillating back here is a wisdom work that will be able to Italy. 295 00:55:03,060 --> 00:55:16,410 Guillermo Mena: me publishing Jacob Okay, so it says, an application like a distilled other Assange an ethical approximations but the nice thing is that you see that there are two aspects of suppression. 296 00:55:16,920 --> 00:55:28,260 Guillermo Mena: The first one is the quantum the corresponding to loop, but there is an additional suppression of these beginning of inflation, this is a nice thing Okay, because you can see both of them. 297 00:55:29,160 --> 00:55:38,130 Parampreet Singh: But in this model, do we have a some I think I remember some of the recent papers, or do you have a fastball kind of a scenario or. 298 00:55:38,670 --> 00:55:48,480 Guillermo Mena: yeah I mean essentially what we did in that paper were to compare and evolution in USA that typical background for loop or a. 299 00:55:49,200 --> 00:55:56,550 Guillermo Mena: Look, when the cosmology it, that is our lives and, therefore, that the very beginning of inflation is not the slow roll okay. 300 00:55:57,270 --> 00:56:05,820 Guillermo Mena: I compare that with the same kind of solution, but in general relativity which the difference is only that you don't have the bounce. 301 00:56:06,150 --> 00:56:22,440 Guillermo Mena: And you continue backwards in time until you reach a big fan okay Okay, and to try to see what were the differences in the power spectrum the spectra that you have, in both cases, they said, the only thing I mean the good thing about things that we were able to. 302 00:56:23,670 --> 00:56:41,460 Guillermo Mena: Implement analytical approximations is allowing us to compute a Secondly, the power specter, on the other hand, they are approximations Okay, so in the future the nice thing will be to try and prove that they are you mentioned relax okay. 303 00:56:41,490 --> 00:56:51,720 Parampreet Singh: Thank you, so I have just go Comments like one Daniel in your talk you mentioned at one point that the bounces of gaining the hydrodynamic limit. 304 00:56:52,800 --> 00:57:02,550 Parampreet Singh: When you're selling this card is yours and probably like a a got an impression that you want to say that bonds probably cannot be trusted, but I think like. 305 00:57:03,480 --> 00:57:10,290 Parampreet Singh: We have a very similar situation and you see if one looks at the full quantum dynamics and one considers states which are. 306 00:57:10,980 --> 00:57:21,030 Parampreet Singh: How you squeezed orange juice, which are widely spread states which have very small momentous in the skill of you there the effective description, it is true it breaks down. 307 00:57:21,510 --> 00:57:29,100 Parampreet Singh: But if you do the full quantum analysis that the full states and you'll have to use SPC for that you still see about. 308 00:57:29,760 --> 00:57:45,180 Parampreet Singh: So just because we do not recover do we reach the limit of the validity of the approximation I don't think it implies that you won't see probably about it may still be true in your approach, but at least in accuracy, we do not see. 309 00:57:46,710 --> 00:57:49,470 Parampreet Singh: Running playing another so just a small comment. 310 00:57:52,260 --> 00:57:52,470 And I. 311 00:57:54,330 --> 00:57:54,870 Daniele Oriti: saw. 312 00:57:56,010 --> 00:58:00,960 Daniele Oriti: The only logical implication, I wanted to put forward is that if. 313 00:58:02,160 --> 00:58:10,950 Daniele Oriti: A quantum cosmology equation comes out as the hydrodynamic one and, in fact, it turns out to be no linear equation, for the way function. 314 00:58:12,660 --> 00:58:17,280 Daniele Oriti: Then the volume basically goes with the particle number. 315 00:58:18,450 --> 00:58:26,310 Daniele Oriti: The number of the data because it's an additive quantity, so the approximation which one recall vs is. 316 00:58:27,600 --> 00:58:36,930 Daniele Oriti: No linear essential company cosmology as I go that makes it will then have to be trusted for very small values of the particle number. 317 00:58:38,400 --> 00:58:52,980 Daniele Oriti: Now, the only logical implications that that one should have expected to be genetically tested, because it will depend, a lot of what precisely the current the fluctuations do in the full system. 318 00:58:54,090 --> 00:59:03,720 Daniele Oriti: He said the only logical implications that that is a danger zone, this is exactly where the little mermaid approximation becomes a questionable. 319 00:59:04,680 --> 00:59:20,670 Daniele Oriti: Then may will be there for large classes to say even for the stage that turned out to be the physical ones, because of that I don't make time boundary conditions it's all the bounces festival because, despite the particle not being smaller fluctuations are under control. 320 00:59:21,780 --> 00:59:30,990 Parampreet Singh: So if I can add like in fact like exactly like what you're saying, as the when the particle number small which corresponds to small volume this word the kind of states. 321 00:59:31,410 --> 00:59:39,870 Parampreet Singh: I was very worried about and we studied extensively with the fluctuations become very large and urgency, but you see it turns out that in fact the. 322 00:59:40,170 --> 00:59:45,660 Parampreet Singh: One might thing that the fluctuations will destroy the rounds, but it turns on the fluctuations actually help. 323 00:59:46,140 --> 00:59:51,840 Parampreet Singh: Having the bounce much earlier, like the spaced and curvature at crystal bonds occurs tons of women. 324 00:59:52,620 --> 01:00:08,910 Parampreet Singh: In fact, like away and British than later, were able to write some sort of an effective description, with a modified energy density, which shows that the bounce density is lower, so I think this is something very interesting, which might be useful or virtual. 325 01:00:09,300 --> 01:00:20,490 Daniele Oriti: You know, we also find that the listing the models in the setting we restarted the the bounce up still can be transmitted for a large class of states will do some restriction, but is. 326 01:00:21,330 --> 01:00:31,440 Daniele Oriti: reasonably robust the I have difficulties in comparing directly with delicacy, because I don't know what the particle number is equal to see because you know to see you don't really come out of the. 327 01:00:31,980 --> 01:00:38,490 Daniele Oriti: cause greening of our larger she the spacing which has something that counts, because in freedom, you constraint. 328 01:00:40,020 --> 01:00:44,340 Daniele Oriti: But any more precise comparison would be very, very useful. 329 01:00:45,270 --> 01:00:48,180 Parampreet Singh: can ask the final comments will be one harder. 330 01:00:48,840 --> 01:00:58,650 Parampreet Singh: And oh so you're looking you're not like you and I think yeah well, you also mentioned that first thing that the differences between the dressed and the hybrid are only in the bounce region. 331 01:00:59,340 --> 01:01:11,130 Parampreet Singh: I think that probably is zoom's a standard acoustic only because if you have this team and regularized ml QC one, then the plank regime extends all the way. 332 01:01:11,700 --> 01:01:22,440 Parampreet Singh: To the far contracting branch, and then we have shown that there are very strong differences between the dress on the hybrid approach all through in the contracting branch not just about EG. 333 01:01:23,100 --> 01:01:31,590 Parampreet Singh: Does the first thing second thing Yvonne you mentioned that when you were discussing these different hamiltonian switch, we cannot agree, and so on. 334 01:01:31,980 --> 01:01:36,360 Parampreet Singh: that the post bonds agrees again that assumes that the post bounce. 335 01:01:36,870 --> 01:01:48,090 Parampreet Singh: universe, is very simple, that there is a single bonds and the universe never went through different cycles, we have recently shown that the universe ventura the cycles, before getting into the inflationary stage. 336 01:01:48,810 --> 01:01:58,290 Parampreet Singh: Then in some of the models, like the like watch that board and Lindner give you will never get the most points universe like ours, so it will be stuck. 337 01:01:58,770 --> 01:02:06,840 Parampreet Singh: In the blank energy, I have just a final question to both give me one like if if i'm allowed to ask, I think, like it's very both of you again very, very. 338 01:02:07,620 --> 01:02:24,750 Parampreet Singh: Beautiful talks with via scobie i've stated very carefully, but I think the one question which which I would like to see in both the toxins that yes, we can have fine tuned initial states which which can which can probably explain the anomalies and. 339 01:02:26,550 --> 01:02:38,670 Parampreet Singh: observations, but I think that is not the only thing we should be satisfied with what we have to ask is, do we have a unique signature coming from quantum cosmology which nor the bouncing model can have. 340 01:02:39,210 --> 01:02:49,380 Parampreet Singh: or no other model of the universe can have, and that is what i'm worried about because in both approaches and me both approaches have are essentially like. 341 01:02:50,490 --> 01:03:01,530 Parampreet Singh: Quite seen like and the point is like in any approach of course magical perturbations in a QC which has been done, like by the time we start asking questions on. 342 01:03:01,920 --> 01:03:09,390 Parampreet Singh: What is observed, but we are already outside the quantum machine the quantum effects will don't matter, except that the background, has to be the wanting one. 343 01:03:10,080 --> 01:03:19,590 Parampreet Singh: So the signature the signature of the real quantum geometric effects are already lost by the time we are asking about the relevant wavelengths which we can see. 344 01:03:20,190 --> 01:03:31,350 Parampreet Singh: And observations I think like i'm not sure whether he won he won in your paper on long gosh entities, you had made certain assumptions about the answers for the bouncing more of it was not exactly. 345 01:03:31,890 --> 01:03:42,330 Parampreet Singh: What one will see from a QC, so I think like I would, I would like to get input from both of you like, what is your thinking like do we. 346 01:03:42,690 --> 01:03:49,290 Parampreet Singh: We I think we all agree that we need very fine tune states to describe certain features of the observations, but. 347 01:03:50,010 --> 01:04:01,410 Parampreet Singh: Where is the hope, or where is our agenda for trying to extract really unique prediction of a QC compared to what, for example, Brendan burger is doing or other people will between. 348 01:04:01,950 --> 01:04:11,070 Parampreet Singh: they'll say once you have a bounce they will say once you have a bounce, irrespective of where it comes from, and I take your initial states, I will get exactly the same results. 349 01:04:12,720 --> 01:04:19,680 Parampreet Singh: So I think that is why what Guillermo said that the initial state has to be motivated from quantum gravity becomes really important. 350 01:04:23,250 --> 01:04:25,200 Parampreet Singh: So any comments, yes. 351 01:04:25,230 --> 01:04:27,210 Guillermo Mena: When do we want to replay first oh. 352 01:04:27,570 --> 01:04:41,130 Ivan Agullo: Yes, yes, again, again, thank you, thank you for for bringing all these points, because you know our time is limited, and we had you know, a limitation of the on the amount of messages that we could, so thank you for compliment in. 353 01:04:42,210 --> 01:04:49,500 Ivan Agullo: All that I agree with most of what you would you have said and and and then. 354 01:04:50,250 --> 01:05:06,090 Ivan Agullo: Now that we have you know, several our predictions or or we know how to move from theory to predictions, both for the power spectrum on oceanic the anomalies etc now, is where we can ask more refined questions as the one that you are asking, can we. 355 01:05:07,320 --> 01:05:13,140 Ivan Agullo: You know single out something which is unique for milk, you see. 356 01:05:13,890 --> 01:05:21,240 Ivan Agullo: hey, by the way, this question has been posted for not able to see, but for inflation itself, there are many models and people were asking. 357 01:05:21,600 --> 01:05:27,780 Ivan Agullo: Is there you know something that only this model can predict, and the answer revealing inflation is very difficult. 358 01:05:28,590 --> 01:05:49,860 Ivan Agullo: difficult because you know, the amount of physical processes happening, since the early universe until now are huge and most of the information is washed out so so we've been an inflation that question is is difficult inaccuracy can we a single out some prediction and. 359 01:05:50,910 --> 01:06:01,290 Ivan Agullo: m barbies you know part of the answer is, this was the year most senior massage this newest scale that ltc introduces which is not interviews by by other models. 360 01:06:01,740 --> 01:06:12,630 Ivan Agullo: on which you know that he said, changing the power spectrum deviation from a scaling Barrio and if you ask me, can Can I make a model to mimic that probably yes, you know. 361 01:06:14,310 --> 01:06:23,700 Ivan Agullo: It is very difficult to find an upsell bubble, which is uniquely you know it's like belly inequalities can only be true if if you know if quantum mechanics. 362 01:06:25,020 --> 01:06:30,630 Ivan Agullo: In this case, something that is only true if you see through either know if anything like that and I don't know if. 363 01:06:31,350 --> 01:06:39,720 Ivan Agullo: We have made that is impossible, given the complexity of the system and the amount of physical processes happen. 364 01:06:40,650 --> 01:06:51,360 Ivan Agullo: On the way, but these are the important question that we all keep in mind, we will change things see you know hold the predictions change and and keep an eye on on this very interesting question. 365 01:06:52,380 --> 01:07:02,730 Ivan Agullo: just keep in mind to summarize my answer that that is a question on the table for any single a scenario of their universe and he's a very difficult difficult one. 366 01:07:04,860 --> 01:07:05,430 Parampreet Singh: Thank you want. 367 01:07:07,260 --> 01:07:21,450 Guillermo Mena: me to be the first thing is that, in order to unify the descriptions I have started, always in the bounce Okay, assuming that any initial condition compete with faces initial conditions. 368 01:07:24,720 --> 01:07:32,100 Guillermo Mena: Just because, otherwise, you have many different possibilities important point was a in my last message that they. 369 01:07:32,520 --> 01:07:46,890 Guillermo Mena: In fact, I agree with you that age, they choose a vacuum that we do has to be based on principle okay it's not that we choose a state that is as the offset our spectrum, this will not be satisfactory. 370 01:07:48,540 --> 01:08:00,060 Guillermo Mena: Then the thing is essentially what he was saying about the one to escape a in fact in the literature of the funder cosmology will see a spectrum which this professional viewers. 371 01:08:00,720 --> 01:08:10,260 Guillermo Mena: What I have called the inflationary scale and others in which is in the quantum to escape they they former once I would say that are not capable. 372 01:08:10,560 --> 01:08:21,330 Guillermo Mena: to encapsulate of capture the quantum effects so from that point of view, we will not be satisfactory to to establish look smaller, they will be like a general relativity certainly. 373 01:08:23,340 --> 01:08:34,440 Guillermo Mena: So in this aspect is a positive thing OK, we have some features that are like you simply have look into postman. 374 01:08:35,730 --> 01:08:47,160 Guillermo Mena: And the other important things that this escape appears first even for many of the backgrounds of we can consider if you look under with molly the inflationary still will not be your server. 375 01:08:48,840 --> 01:08:49,440 Guillermo Mena: That is that we. 376 01:08:51,030 --> 01:08:51,510 don't think. 377 01:08:53,100 --> 01:08:57,090 Jorge Pullin: There is a question for for i'm in the chat when I think Western has their hands race. 378 01:08:59,400 --> 01:08:59,670 yeah. 379 01:09:01,020 --> 01:09:04,860 Thank you, this is Carol hi everybody, I have two things. 380 01:09:06,270 --> 01:09:10,380 Independent the first is a question to you, then. 381 01:09:11,820 --> 01:09:12,480 it's a. 382 01:09:13,860 --> 01:09:28,620 appreciate a lot it on your your your synthesis and I was really intrigued by your normal shiny things that you mentioned at the at the end sounds super interesting or something I don't understand is a simple technical thing. 383 01:09:31,410 --> 01:09:40,230 Western: I understand that there's a gaussian approximation, which is just the lead in order in which the two point function sort of determines all the higher. 384 01:09:40,920 --> 01:09:43,620 Western: important functions, and in particular the frequent function is zero. 385 01:09:44,610 --> 01:09:58,650 Western: Now, if you go to next order what happened is that the two point function changes, of course, because you go to make soda so there's a correction and generically the three point functions becomes different from zero because, because there is this. 386 01:10:00,090 --> 01:10:08,880 But now you, you have said something which it was curious about, you said that 3.5 should be become different from zero. 387 01:10:10,080 --> 01:10:15,450 And this has an effect on the two point function in direct that. 388 01:10:17,670 --> 01:10:31,500 That let's say we can measure let's let's say we can measure it by measuring the two point function now do you mean this I missed that I didn't fit with my understanding of the story, do you mean simply it was. 389 01:10:32,610 --> 01:10:39,810 involved way to say simply that to like store the data without your changes or do is really a report function involved in this story. 390 01:10:41,220 --> 01:10:48,270 Ivan Agullo: Thank you Gary so it's a very good question, and it was my fault, because it was very brief and I didn't explain explain the so thank you for. 391 01:10:49,530 --> 01:10:54,930 Ivan Agullo: Let me just say a few a few words about that, let me share my screen again. 392 01:11:01,770 --> 01:11:08,940 Ivan Agullo: What you have said, is precisely the two things that that that may happen, a wine is that you know. 393 01:11:10,140 --> 01:11:19,980 Ivan Agullo: Of course, once you introduce a next to live in order, and if you compute the coupon function, you will have one loop effects which is you know. 394 01:11:20,490 --> 01:11:27,450 Ivan Agullo: Exactly, and that is going to be modified that happens to be quite small, in fact, for for for from from. 395 01:11:28,200 --> 01:11:38,250 Ivan Agullo: You know, using their the paradigm, we have we have us and the effect of that seems to be quite a small and out of of of observation, what happens rather. 396 01:11:39,030 --> 01:11:50,070 Ivan Agullo: is something that is influence in an indirect manner by 30% functions and he's happy top down so so let me try to explain it as clear as I can. 397 01:11:51,150 --> 01:12:02,700 Ivan Agullo: In fact, this is the origin of the the is not mine, it was already a be proposed in the cosmology community and it's called non gulshan modulation. 398 01:12:03,900 --> 01:12:08,340 Ivan Agullo: And what happens is the following imagine you have a three point function. 399 01:12:08,970 --> 01:12:20,070 Ivan Agullo: And, of course, the value of the function depends on the configuration of the three points, if you want of this triangle, I have in mind is like the bending the shape of the three I know the three main function is bigger or smaller. 400 01:12:21,120 --> 01:12:32,370 Ivan Agullo: What happens in ltc is that they don't know shiny these are sad that, for this multiple angles, when the three were the three points feet inside the huddle right they have a. 401 01:12:33,120 --> 01:12:48,660 Ivan Agullo: patch no notion he started small that as long as one side of the triangle X three in my blood gets separated from the other two points that are very active angle gets bigger and squeezed they don't go show me the increase. 402 01:12:50,130 --> 01:13:00,690 Ivan Agullo: So, it happens that these two points X one X two are strongly correlated with X three if actually is is enough far far away from it 100. 403 01:13:02,430 --> 01:13:09,870 Ivan Agullo: And therefore, what happens a you can think about this either, in reality, space or inferior space with K one K 23. 404 01:13:11,190 --> 01:13:18,990 Ivan Agullo: What happens, therefore, is that if we have let me do the argument in your space what is what what what is normally done if you see or. 405 01:13:19,950 --> 01:13:30,360 Ivan Agullo: Maybe, for us, because we are more used to it, what happens is that if you have a third node case 30% in your universe, with very long wavelength. 406 01:13:30,870 --> 01:13:43,200 Ivan Agullo: So you cannot see in the CME because the wavelength is too long it's may present just because this person is gonna buy yes, whatever it happens inside, they have a radius. 407 01:13:43,830 --> 01:13:58,770 Ivan Agullo: Because this is from correlations so the presence of this mode long wavelength mode or is hampson will produce a different power spectrum inside the other writers, because they're strong correlations the CME is very correlated with the exterior. 408 01:13:59,880 --> 01:14:05,010 Ivan Agullo: This is what people call non gulshan modulation, that the presence. 409 01:14:06,060 --> 01:14:12,150 Ivan Agullo: presence of nano sharpies bad, yes, the statistics wi fi now would have a better. 410 01:14:14,040 --> 01:14:18,480 Ivan Agullo: visual effects statistical thing is the percent of something else outside okay that with. 411 01:14:19,830 --> 01:14:33,720 Exactly Oh, I see I got it Okay, thank you, thank you, thank you, thank you, that reflects the second point, if I forget stop me if I cannot second point is it's a it's a comment, I want to make to what the nila said. 412 01:14:35,250 --> 01:14:41,850 Since this is a general discussion and since then either least general point I would like to make the following comment. 413 01:14:43,320 --> 01:14:53,340 The nearest focusing on the effect of sort of the elementary constituents on the large scale phenomena effect that might be. 414 01:14:54,630 --> 01:15:00,450 Important, of course, you know the narrative phase transitions things happening and so like that. 415 01:15:01,950 --> 01:15:05,160 Western: Which it's it's it's, of course, very interesting. 416 01:15:06,840 --> 01:15:11,430 So search problem because he might eat my my lead to to understand something. 417 01:15:12,990 --> 01:15:22,410 So this is not a criticism, or what I nearly is doing, but the way he the nila presented it could be taken as an implicit criticism of. 418 01:15:24,120 --> 01:15:27,180 Any research problem that is regard disregards that. 419 01:15:28,980 --> 01:15:35,340 And, and so the title of cosmology in a certain sense and and and I think this is wrong in the following sense. 420 01:15:37,230 --> 01:15:43,560 When we let me say one thing about classical mechanics one thing about quantum mechanics when you do classical mechanics. 421 01:15:44,640 --> 01:15:59,010 We are not describing the individual constituents the elementary constituents of reality will do the solar system dynamics, we know that Jupiter is made by many, many apples, but that's not the point we. 422 01:16:00,990 --> 01:16:06,660 single out some degrees of freedom, which is the position of Jupiter with respect to the silent Venus of years. 423 01:16:07,800 --> 01:16:13,590 And we find a case because of the configuration of the universe will with this degrees of freedom, I have a mechanical. 424 01:16:14,550 --> 01:16:26,130 behavior that can be captured by some equations and it works, and we do always that because, in fact, we never know what are the elementary constituents, the entire science. 425 01:16:27,030 --> 01:16:35,190 works, independently of the elementary consequence when there are some some degrees of freedom that can be described it can be found to. 426 01:16:36,360 --> 01:16:44,250 To have something radical equations that describe now once we go to quantum mechanics it's exactly the same thing if I had a pendulum or. 427 01:16:47,100 --> 01:16:57,030 mechanical pendulum like the one day they started the quantum mechanics in in in the laboratories now it's completely relevant the dependent was made by atoms. 428 01:16:57,840 --> 01:17:10,170 It has one degree of freedom that oscillator these oscillations called ties and this quantization is measured so quantum mechanics does not is not a theory about elementary constituents is a theory of. 429 01:17:11,250 --> 01:17:14,820 quantum properties of any degrees of freedom largest malls that it is. 430 01:17:15,960 --> 01:17:25,200 This doesn't mean that sometimes it's good to study the elementary considered small constituents to see collective phenomenon, of course. 431 01:17:25,680 --> 01:17:36,390 These are interesting and that's why what the deal is doing is interesting, but not because the large scale degrees of freedom cannot be described by themselves, and if one doesn't do that what is making a mistake, not at all. 432 01:17:37,410 --> 01:17:49,770 And I think we in our Community general generically we often make this mistake, I think that quantum gravity is should not be viewed as the study of elementary constituent of space time. 433 01:17:50,610 --> 01:17:57,570 I think this is a wrong way of thinking about quantum gravity quantum gravity should be thought about the the quantum properties. 434 01:17:58,170 --> 01:18:09,960 of degrees of freedom of space times, whether they are large or small, so if there are phenomena that involves large degrees of freedom large scale degrees of freedom. 435 01:18:12,000 --> 01:18:15,990 This should allow a description. 436 01:18:17,820 --> 01:18:20,190 A quantum discrete john just by themselves. 437 01:18:22,050 --> 01:18:31,860 This, by the way, it's also true in quantum field theory standard quantum field theory, in spite of normalization and everything the way the. 438 01:18:33,360 --> 01:18:34,170 In KC D. 439 01:18:35,580 --> 01:18:46,620 One computes the masses of the particles of the lattice using your CD is this regarding all the degrees of freedom which are smaller than. 440 01:18:47,310 --> 01:18:58,410 say the Cork wave wavelength, so I want to separate in in in this story, because I think it's a it's a common mistake in our in our Community. 441 01:18:58,740 --> 01:19:09,780 Yes, it's interesting to study collective phenomena definitely because something interesting can come out for it, but this does not mean the studying large degrees of freedom bites by themselves for. 442 01:19:11,370 --> 01:19:15,090 it's necessarily wrong necessarily disregarding something. 443 01:19:20,760 --> 01:19:21,120 Jorge Pullin: boy. 444 01:19:24,210 --> 01:19:28,260 Daniele Oriti: Can I can I comment to clarify so. 445 01:19:33,240 --> 01:19:37,650 Daniele Oriti: So, to clarify what my point was my point was not normative. 446 01:19:39,870 --> 01:19:44,040 Daniele Oriti: I mean it's not what is right and what is wrong, what should be done or not. 447 01:19:45,210 --> 01:19:51,690 Daniele Oriti: And the point is, I mean that I want this to be clear, the issue is not. 448 01:19:52,890 --> 01:19:54,660 Daniele Oriti: classical versus quantity. 449 01:19:56,730 --> 01:20:04,470 Daniele Oriti: issue is many degrees of freedom versus a subset or collective variables and. 450 01:20:05,760 --> 01:20:16,320 Daniele Oriti: The point of whether the collective effects relevant or not, the for the factory, then our next word subset to global lower collective observable. 451 01:20:17,370 --> 01:20:30,540 Daniele Oriti: need is in many cases, it is not in some urgency is not there in many others who say, rather than QC do rather take any quantum anybody system, I mean. 452 01:20:32,880 --> 01:20:39,360 Daniele Oriti: There are many systems in which the affected collected and honestly it doesn't really be entered all on the. 453 01:20:40,500 --> 01:20:47,670 Daniele Oriti: Not so much on on collective interactions of the constituents and it doesn't depend march on their quantum nature. 454 01:20:49,920 --> 01:21:03,630 Daniele Oriti: There are many others in which you neglect the is collected effects initial neglect to the quantum nature, he considers you totally miss the physics it's a research question now, in which case when when we because mala g. 455 01:21:04,650 --> 01:21:06,210 Daniele Oriti: And, in general, when we start. 456 01:21:07,260 --> 01:21:16,440 Daniele Oriti: generativity we will continue description terms of fields, so from our quantum gravity models which we have a different type of freedom. 457 01:21:18,120 --> 01:21:33,930 Daniele Oriti: it's not a matter of being right would be wrong with just to be aware of, we just have to be aware of the different limits different types of approximations and we should be able to control them, we cannot declaring advance and what is not relevant, and was not until we find out. 458 01:21:39,360 --> 01:21:41,790 Jorge Pullin: Okay boy yeah. 459 01:21:42,090 --> 01:21:42,690 Abhay Vasant Ashtekar: So I mentioned. 460 01:21:43,200 --> 01:21:44,490 Abhay Vasant Ashtekar: i'm very happy with the last. 461 01:21:44,700 --> 01:21:53,550 Abhay Vasant Ashtekar: Discussions with the blue and Daniel day because the first couple of points, the first point I want to make is really about the continuation of that. 462 01:21:54,570 --> 01:21:57,690 Abhay Vasant Ashtekar: I mean, I think, just just give example along the same lines of. 463 01:22:00,060 --> 01:22:00,510 Abhay Vasant Ashtekar: How long. 464 01:22:01,710 --> 01:22:07,260 Abhay Vasant Ashtekar: Is, and this is an example like you and many times before, namely that we could just take. 465 01:22:08,370 --> 01:22:17,760 Abhay Vasant Ashtekar: Direct model of hydrogen atom, which is very sparingly symmetric and by assuming it's pelican symmetric one immediately says, there are no 14 degrees of freedom. 466 01:22:18,390 --> 01:22:24,630 Abhay Vasant Ashtekar: So in Daniel is language infinitely many degrees of freedom are suppressed by imposition of this spell and symmetric. 467 01:22:25,590 --> 01:22:33,450 Abhay Vasant Ashtekar: And yet it produces results which are perfectly fine so we're lowering all kinds of fine structures, I mean really I mean if anything. 468 01:22:34,170 --> 01:22:43,590 Abhay Vasant Ashtekar: and keep you on the final component and yet until one goes to lab shift, what does not really see any discrepancy with data model, of course, in a logical model. 469 01:22:44,580 --> 01:22:54,060 Abhay Vasant Ashtekar: And in fact you know you and today the rigorous totally rigorous statement of hydrogen atom from phuket cutie is not allowed, but we don't worry about that and so much. 470 01:22:56,040 --> 01:23:04,110 Abhay Vasant Ashtekar: So I think that this is going back to what he was saying that there is also an observational issue here, that we should always keep in mind. 471 01:23:04,800 --> 01:23:14,160 Abhay Vasant Ashtekar: And then, as Daniela just now in fact it's a very beautiful either we it's not each of the classical versus content, I mean it's a question about whether. 472 01:23:14,580 --> 01:23:22,740 Abhay Vasant Ashtekar: When he's doing sort of course grading and whether that is creating big effectual is not creating big effects, maybe not picking the effect. 473 01:23:24,720 --> 01:23:30,600 Abhay Vasant Ashtekar: So in this case I mean, in the context of cosmology except as a note of maybe a lot of people accuse you don't know. 474 01:23:31,080 --> 01:23:45,780 Abhay Vasant Ashtekar: There has been a controversy which has been going on for about a decade now about precisely this issue, namely that we assume Friedman, Robert Walker model may be small perturbation on it and get great success with observations in classical cosmology. 475 01:23:47,040 --> 01:23:56,670 Abhay Vasant Ashtekar: But because it's motivations grow up because of traction but people say well but that's not really true, we should really get this model as. 476 01:23:57,390 --> 01:24:09,630 Abhay Vasant Ashtekar: By about average and that that was a great excitement that may be desiring actually produces a big effect, which is the you know we don't do in need of a smaller constant and. 477 01:24:11,310 --> 01:24:24,540 Abhay Vasant Ashtekar: This is a controversy that has been going on between you know one side is booklet georgiana's Malcolm mccallum and the other side is Bob Walden and green and. 478 01:24:24,840 --> 01:24:25,590 I can. 479 01:24:27,690 --> 01:24:28,050 Abhay Vasant Ashtekar: Sorry. 480 01:24:30,780 --> 01:24:31,980 Abhay Vasant Ashtekar: Thank you, I did not know that. 481 01:24:32,250 --> 01:24:33,540 Abhay Vasant Ashtekar: which was which side is he on. 482 01:24:35,790 --> 01:24:37,050 simone: The side. 483 01:24:37,740 --> 01:24:38,670 Abhay Vasant Ashtekar: Booker Lucas, I think. 484 01:24:39,990 --> 01:24:40,650 Abhay Vasant Ashtekar: So. 485 01:24:42,630 --> 01:24:44,250 Abhay Vasant Ashtekar: So I mean this is. 486 01:24:45,720 --> 01:24:47,280 Abhay Vasant Ashtekar: This is going on, but other than I mean I. 487 01:24:48,390 --> 01:24:57,870 Abhay Vasant Ashtekar: I follow it up some don't do research in it, but i've always great interesting very, very detailed discussion, particularly agree, and also with the GA listen Malcolm. 488 01:24:59,910 --> 01:25:10,380 Abhay Vasant Ashtekar: And I kind of feel that I feel that really it is true that that is perturbations don't have the hidden costs while you don't have any effect large effect. 489 01:25:11,580 --> 01:25:23,670 Abhay Vasant Ashtekar: On one side of more than down and then green it's not sold completely but but I, but at the moment i'm not trying to resolve this controversy i'm just like to say that there is a real possibility that. 490 01:25:24,900 --> 01:25:30,270 Abhay Vasant Ashtekar: That God was hinting at which will actually be realized, maybe, just as we don't have to worry about atoms of Jupiter. 491 01:25:31,200 --> 01:25:41,370 Abhay Vasant Ashtekar: That we would all have to do this, but I agree with with Daniel a that this is an issue that one needs to be analyzed in some detail and then. 492 01:25:42,330 --> 01:25:52,830 Abhay Vasant Ashtekar: And then it's what i'm analyzing but once you're not a priority dismiss the idea that you know that this averaging any growing. 493 01:25:53,190 --> 01:25:59,970 Abhay Vasant Ashtekar: Number of degrees of freedom is clearly wrong, I think one should not say it's clearly wrong, I mean what i'm not saying, Daniel you're saying that. 494 01:26:00,300 --> 01:26:06,210 Abhay Vasant Ashtekar: But there is often a viewpoint that unless we derive everything from lukewarm cry with you from scratch. 495 01:26:06,870 --> 01:26:10,620 Abhay Vasant Ashtekar: Then you know all kinds of new things can happen yeah all kinds of new things can happen. 496 01:26:11,250 --> 01:26:23,550 Abhay Vasant Ashtekar: I mean people thought that about guy which is days, all kinds of new things can happen the full on emerging and still you know very simple ideas, actually, by the way, we would today, so we should skip this mind in open. 497 01:26:26,280 --> 01:26:33,750 Abhay Vasant Ashtekar: I think about the second thing that I had was a little bit more technical, so I think i'll just like to the people, email messages and. 498 01:26:35,100 --> 01:26:36,840 Abhay Vasant Ashtekar: So I think this is the main thing that interested. 499 01:26:39,420 --> 01:26:39,630 Jorge Pullin: me. 500 01:26:41,250 --> 01:26:53,820 Daniele Oriti: Can I can I reply to the comment so yeah thanks for pointing out the the classical situation he is entirely analogous as an ethical principle essentially a matter of whether the cause gleaning. 501 01:26:56,010 --> 01:27:09,930 Daniele Oriti: Much you can neglect the contribution of freedom equals green away in the constraining procedure and, instead, both the technical and no an observational question, then they want us to try and check. 502 01:27:10,980 --> 01:27:18,210 Daniele Oriti: So I won't comment on the classical story because enough, but I can tell you what we see in the in the gst contest. 503 01:27:19,230 --> 01:27:34,020 Daniele Oriti: That you know the hydrodynamic description, in fact, as a as emphasizing, there is no use your near term in the equation that really looks like a quantum cosmological ation and then you've got an India corrections. 504 01:27:35,250 --> 01:27:35,850 Daniele Oriti: Now. 505 01:27:36,930 --> 01:27:37,950 Daniele Oriti: If the. 506 01:27:39,150 --> 01:27:50,790 Daniele Oriti: Fundamental introductions of small us respect in job is corrections and it's not enough terms of to maybe only kind of have that made a time and in fact that's what we find we find out that. 507 01:27:51,240 --> 01:28:02,280 Daniele Oriti: The free term allows you to record with his vision to see like dynamics, with some changes, but you have a ball, so you have the freedmen life equation. 508 01:28:03,090 --> 01:28:13,740 Daniele Oriti: It later times what are you missing so you're not certainly not missing what that allows you to recover Friedman dynamics in this specific context, again, and I want to make a general statement. 509 01:28:14,850 --> 01:28:23,220 Daniele Oriti: You missed the possibility that the naked times this new effects modify the then obviously in ways that the linear. 510 01:28:23,820 --> 01:28:31,740 Daniele Oriti: truncation so the fully dust because green, they will correspond to a quantum cosmology The sad thing is, by definition, not able to see. 511 01:28:32,370 --> 01:28:41,910 Daniele Oriti: At least not in this, you know that way they could be effective ways in which you know you have an effective leaner than armies, including the contribution from interruption but. 512 01:28:42,600 --> 01:28:58,890 Daniele Oriti: that's okay and and that's it that it's all the mvc framework is in fact reproduce for a larger class of regimes and phenomena indeed within and more general contest what we have under some. 513 01:28:59,430 --> 01:29:09,720 Daniele Oriti: Limited control and so that's an advantage to be able to tell if the results of this non linearity so because, when is or is not relevant, and where. 514 01:29:11,880 --> 01:29:27,360 Daniele Oriti: And, in general, of course, I agree with you that there's no statement here or anywhere else that something is right and something is wrong, know that there is a more general procedure, but we will be totally irrelevant for all physical questions. 515 01:29:29,490 --> 01:29:40,890 Abhay Vasant Ashtekar: So just to continue this last last part continue along the thing there's also the issue about the initial conditions that was raised by by Guillermo, but I think, as you want said that these initial conditions issues. 516 01:29:41,100 --> 01:29:41,700 Abhay Vasant Ashtekar: Carbon to. 517 01:29:42,330 --> 01:29:51,330 Abhay Vasant Ashtekar: Everything like classical gender equity wise universe that we live in a very wide wise and huge amount of a nice office today. 518 01:29:53,400 --> 01:29:54,420 Abhay Vasant Ashtekar: That was a. 519 01:29:55,590 --> 01:30:07,260 Abhay Vasant Ashtekar: cosmic microwave background why that you can lie down easy that I don't so you knew what system which solutions nine cents equation, which cosmic microwave background would not have this homogeneity and I sort of see today. 520 01:30:08,280 --> 01:30:17,940 Abhay Vasant Ashtekar: So this is a common question to all fees, and so I mean I think what value they say, also a lot of what people were saying. 521 01:30:19,980 --> 01:30:29,910 Abhay Vasant Ashtekar: Arriving at El que si from full El que je this choice of states are going to be important, and so there was gear was emphasizing, and I think I agree with it, that. 522 01:30:30,810 --> 01:30:36,660 Abhay Vasant Ashtekar: We need some me to be very nice if we have some physical principles which actually give you the state. 523 01:30:37,170 --> 01:30:52,740 Abhay Vasant Ashtekar: And attend that Bradley Cooper and I made was really like like very, very, very simplified coming at a very low level just to open the door, so to say about saying that well put to put together what we know from the kind of guy which has a whole. 524 01:30:53,880 --> 01:31:06,150 Abhay Vasant Ashtekar: spectrum of area and setting to sort of demonstrate that number he constrained by the state of the background, so that constraints, a number of he falls and then use the. 525 01:31:07,230 --> 01:31:15,480 Abhay Vasant Ashtekar: Use the state which is a generalized Rogers Rogers principle that maximum on Virginia and I saw puppy in the blank richie. 526 01:31:16,050 --> 01:31:29,250 Abhay Vasant Ashtekar: And that was really spelled out as to what you want, but in spite of that really careful analysis that was done, the basic assumptions were what they were, and I think they can be improved, improved upon enormously, so my just basic. 527 01:31:32,040 --> 01:31:41,070 Abhay Vasant Ashtekar: suggestion to younger people and so on is that this really is something that one can can be improved and should be improved, because it is an important question initial conditions. 528 01:31:41,760 --> 01:31:57,540 Abhay Vasant Ashtekar: If we can justify them from some more fundamental principles, of course, one might say, by those principles or something else, but if you can I mean what was used in our work was things like uncertainties and very, very basic things so it can be for the improve that will be very, very good. 529 01:31:58,710 --> 01:32:03,540 Abhay Vasant Ashtekar: But I think this is kind of not something that is huge limitation of. 530 01:32:04,830 --> 01:32:09,960 Abhay Vasant Ashtekar: Proper was saying about fine tuning there's not a huge limitation of our approach versus a be anybody else at. 531 01:32:11,340 --> 01:32:21,810 Abhay Vasant Ashtekar: All are you an inflation that's huge fine tuning issue right them in this mainly white bison is back in the middle of something not at the big bang rather than. 532 01:32:22,890 --> 01:32:24,300 Abhay Vasant Ashtekar: Later time but, in the middle. 533 01:32:26,160 --> 01:32:31,260 Abhay Vasant Ashtekar: So I just wanted to conclude by saying that this is really interesting open issue. 534 01:32:35,040 --> 01:32:35,850 Jorge Pullin: or questions. 535 01:32:37,470 --> 01:32:39,330 Parampreet Singh: Can I can I make one comment too. 536 01:32:40,380 --> 01:32:41,190 Parampreet Singh: Obvious come and. 537 01:32:42,300 --> 01:32:42,630 Jorge Pullin: Go. 538 01:32:43,230 --> 01:32:52,140 Parampreet Singh: So I think Okay, I agree with what you have said, but we face another issue and that issue is that our permission approaches a bottom up approaches. 539 01:32:52,650 --> 01:32:58,290 Parampreet Singh: We are not driving the cosmological sector, we have not had Dr the cosmological separate from the quantum gravity. 540 01:32:58,680 --> 01:33:08,310 Parampreet Singh: Therefore, we do not know the perturbations which we are doing as what quantities perturbations over an effective background, how much do they truly capture quantum geometric effects. 541 01:33:08,760 --> 01:33:26,520 Parampreet Singh: So our challenge is much better and and we have an example of a Martin was trying to mimic certain look quantum gravity affects in his support and we know it just failed because it was blatantly in disagreement with observations, so I think like there are certain issues which we. 542 01:33:28,110 --> 01:33:34,860 Parampreet Singh: i'm not saying, I think that there is a huge progress which has been done in automation theory in last 10 years and as you'll see. 543 01:33:35,340 --> 01:33:46,320 Parampreet Singh: Including if each day the negative results from the reformed algebra approach, which we all agree, have serious problems, but the main issue means that instead of this bottom up approach. 544 01:33:47,010 --> 01:33:53,010 Parampreet Singh: What does a top down version and whether this bottom up approach of the fourth one place but patients on effective background. 545 01:33:53,490 --> 01:34:02,430 Parampreet Singh: Does it even completely capture or even partially captures what we expect us perturbations from quantum gravity and the issue of initial status true. 546 01:34:02,880 --> 01:34:08,010 Parampreet Singh: Initial conditions problems is to as one mentioned as you're mentioning but, again, there is a caveat. 547 01:34:08,490 --> 01:34:14,790 Parampreet Singh: In all those approaches, even in GR examples or inflation, they truly used inflationary dynamics, we do not use it. 548 01:34:15,150 --> 01:34:20,820 Parampreet Singh: If you look at it carefully by the time we are looking at the relevant wavelength modes quantum geometric effects are done. 549 01:34:21,450 --> 01:34:31,710 Parampreet Singh: they're gone so we are essentially mimicking some bounce dynamics, with some initial states which anyone can mimic, so I think we have to look at these issues more carefully. 550 01:34:35,520 --> 01:34:39,840 Guillermo Mena: You play fantasy something even again with the. 551 01:34:41,370 --> 01:34:42,570 Guillermo Mena: Three of you have said. 552 01:34:44,160 --> 01:34:48,210 Guillermo Mena: In particular, with a pattern, that it is through a secondary. 553 01:34:49,440 --> 01:35:05,940 Guillermo Mena: effect fact is that we are progressing a lot of the issues that we have to look more carefully but resources, the ones that I have been commenting on this case okay my opinion, it has the right direction to continue obviously Luca. 554 01:35:07,530 --> 01:35:21,120 Guillermo Mena: is telling me more and more readers than what we have is probably a good approximation of it in my last transparency, there was a sentence in Spanish, there is essentially a quotation that has been attributed to don T shirt oh no it. 555 01:35:21,120 --> 01:35:21,300 Abhay Vasant Ashtekar: Does. 556 01:35:21,480 --> 01:35:32,640 Guillermo Mena: not appear in the novel and it says in English, the dogs bark central, this means that we are writing that essentially is a little with a situation. 557 01:35:33,210 --> 01:35:45,480 Guillermo Mena: Where a lot of prominence and to get this isn't we are going in the right direction is because of these that we have these controversial or otherwise no one would care, this means that we have. 558 01:35:50,670 --> 01:35:51,090 Jorge Pullin: Okay. 559 01:35:52,110 --> 01:35:52,950 Jorge Pullin: Colleagues, this. 560 01:35:55,110 --> 01:36:09,540 calexss: Thank you very much it's a pleasure to be here, my question is about if the some connections between cosmology and the other promotions to cosmology Mike reynold cosmology etc. 561 01:36:13,590 --> 01:36:15,120 Abhay Vasant Ashtekar: DC and roscoe smaller you. 562 01:36:16,290 --> 01:36:17,340 Abhay Vasant Ashtekar: would understand. 563 01:36:18,090 --> 01:36:19,050 calexss: Brain words. 564 01:36:21,030 --> 01:36:26,550 calexss: Is there are some connections between cosmology and order approach want cosmology. 565 01:36:29,100 --> 01:36:32,910 Parampreet Singh: If I can answer that question if the question was about the brain world cosmology. 566 01:36:33,690 --> 01:36:45,390 Parampreet Singh: Then in in the in the most popular hamiltonian which we have a loop quantum cosmology if we look at it, effective dynamics, it gives us a modified Friedman equation, which is very similar. 567 01:36:45,870 --> 01:36:55,470 Parampreet Singh: Except that in the render syndrome to brain was it's ro minus row scare by the bulk density the density coming, we have a new role, plus row. 568 01:36:55,860 --> 01:37:06,330 Parampreet Singh: And we have a rule minus will scare, and there was a model by Yuri stand up and warm sunny like in 2001 2002 where they took an extra buying like extra dimension. 569 01:37:06,720 --> 01:37:11,430 Parampreet Singh: And they obtained a similar effective equation, as we get into quantum cosmology. 570 01:37:12,000 --> 01:37:23,640 Parampreet Singh: So the short answer is, if there are two times like extra dimensions allowed in Renaissance from green was yes, you can obtain quantum this multi like equation, but I don't think most string theorists will agree on that. 571 01:37:26,430 --> 01:37:28,530 calexss: It can think of every month, but. 572 01:37:29,070 --> 01:37:31,200 Abhay Vasant Ashtekar: If you just put by hand and make it as a patient. 573 01:37:34,830 --> 01:37:36,120 Parampreet Singh: Do you have to put in my hand. 574 01:37:36,810 --> 01:37:41,310 Abhay Vasant Ashtekar: yeah if you put a negative brain patient than one one would be able to also. 575 01:37:42,420 --> 01:37:42,660 Jorge Pullin: Okay. 576 01:37:47,310 --> 01:37:52,890 Daniele Oriti: Yes, so of course i'm very interested in this show have initial conditions, said that. 577 01:37:54,330 --> 01:38:07,110 Daniele Oriti: I have to admit i'm very confused about how to phrase it within the jury, because the initial condition will be rested to some internal clock and respite to summer. 578 01:38:08,280 --> 01:38:19,500 Daniele Oriti: Is the issue of the effective vacuum state for the nation, so if i'm eating the food Curie first of all I should be fine the background evolution in terms of a traditional clock and then I also have to define. 579 01:38:20,130 --> 01:38:28,410 Daniele Oriti: The local to patients in terms of a set of the physical degrees of freedom that play the role of robots in that case. 580 01:38:29,160 --> 01:38:48,480 Daniele Oriti: So i'll be talking about the choice of ground state or relevant the quantum state for the whole set of degrees of freedom or an input and then looking at how this quantum states behavior for specific values of the internal degree of freedom of users o'clock. 581 01:38:50,160 --> 01:39:09,540 Daniele Oriti: Laura How are we supposed to you know, a struct some effective or semi classical theory for the local to patients and then contest that and see what are the constraints of consistency, for betrothal bottom state that the two things do not seem to be the same at all. 582 01:39:12,450 --> 01:39:24,180 Abhay Vasant Ashtekar: It was the first thing but supplement that the first thing would be the look at the theory and the full thing, of course, is no this little clock so there's no initial condition, but there is a preferred state. 583 01:39:25,230 --> 01:39:32,940 Abhay Vasant Ashtekar: So that's what to wear like this, I don't want to call it vacuum state but there's some preferred State that is singled out in that which is appropriate. 584 01:39:33,420 --> 01:39:42,600 Abhay Vasant Ashtekar: For the physical problem of describing the large scale structure of the universe, so one who writes first other select out the state, and then the question is whether. 585 01:39:45,840 --> 01:39:46,980 Abhay Vasant Ashtekar: Whether the. 586 01:39:49,590 --> 01:39:52,260 Abhay Vasant Ashtekar: They learned better at their existing time clock. 587 01:39:53,640 --> 01:39:56,070 Abhay Vasant Ashtekar: With respect to which the revolution looks like what we. 588 01:39:56,280 --> 01:40:00,300 Abhay Vasant Ashtekar: See, first of all in the post inflation or during inflation era. 589 01:40:01,890 --> 01:40:08,850 Abhay Vasant Ashtekar: In that state and then so that the two three step problem first is single order preferred state. 590 01:40:09,840 --> 01:40:14,400 Abhay Vasant Ashtekar: Similar preferred state in the full period, the second one would be is that internal clock such that. 591 01:40:14,970 --> 01:40:26,520 Abhay Vasant Ashtekar: The dynamics of that state reproduces what we see in the quote unquote non quantum gravity regime inflation onwards, and the third is the robustness with respect to his choice of internal time. 592 01:40:26,970 --> 01:40:40,560 Abhay Vasant Ashtekar: So I think that is a good thing, I think, even if you don't worry about robustness you can succeed in the first two things which will be a very notable thing, namely that does exist before state which is given to you by some general principles and there does exist. 593 01:40:42,270 --> 01:40:48,030 Abhay Vasant Ashtekar: choice of clock which will actually reproduces the universe, we see, I think that would be by itself very, very. 594 01:40:49,110 --> 01:40:49,740 Abhay Vasant Ashtekar: Nice. 595 01:40:51,300 --> 01:40:56,850 Daniele Oriti: But, but then we should not respected, but the first thing is more like a you know some robustness. 596 01:40:58,470 --> 01:41:05,130 Daniele Oriti: of our cluster states, because what, why should he then select the just one stating the food to be. 597 01:41:05,430 --> 01:41:14,370 Daniele Oriti: Referring to for the right reason since it's more like the botanist of the effective than a mixer for some choices stage so with similar initial. 598 01:41:16,680 --> 01:41:19,170 Daniele Oriti: properties since since our initial dynamics. 599 01:41:20,520 --> 01:41:32,040 Abhay Vasant Ashtekar: So the state of the question would be really powerful states which is which but put by first principles, you would like to say that preferred for this problem, so these are the stage which you would call. 600 01:41:32,460 --> 01:41:38,970 Abhay Vasant Ashtekar: A million for as a Tropic there's a class of states and then for them it doesn't have to be a preferred state. 601 01:41:41,670 --> 01:41:44,310 Jorge Pullin: yeah Thank you any other questions. 602 01:41:52,800 --> 01:41:55,740 Jorge Pullin: Okay, if not, to thank the speakers and see you in the call.