1 00:00:02,070 --> 00:00:09,840 Thanks sorry that I cannot make the full screen of my slides. So, I have only 2 00:00:09,840 --> 00:00:16,140 working on this way and so my talk will be on associated production in PvP and how 3 00:00:16,140 --> 00:00:24,270 they have AI installations. So first some discriminate because because associated 4 00:00:24,300 --> 00:00:28,590 particle production is very broad topics so it's it's going to be interesting 5 00:00:28,770 --> 00:00:33,990 interesting for thousands of reasons right. So, me Of course, we should ask our 6 00:00:33,990 --> 00:00:38,850 questions is we why we are interested in these associate production process of 7 00:00:38,850 --> 00:00:43,290 course, we we are interested in that aspect to that is single inclusive 8 00:00:43,290 --> 00:00:44,820 particle production usually has 9 00:00:45,600 --> 00:00:47,970 much lyrics cannot tell us or tell 10 00:00:48,000 --> 00:00:50,700 us in a very limited way. But even that, 11 00:00:50,820 --> 00:00:55,680 I think it's impossible to cover everything even not I mean, cover some of 12 00:00:55,680 --> 00:01:02,400 them overview of all interesting aspects, right. So I Here is just a bigger one 13 00:01:02,400 --> 00:01:07,440 point I would like to talk here. So the point I will talk is, is I mean, I'm 14 00:01:07,440 --> 00:01:11,910 working a bit on especially on phenomenology side, about the double 15 00:01:11,910 --> 00:01:16,740 bottom scattering at hc Actually, we already see a few of the measurement new 16 00:01:16,740 --> 00:01:24,240 measurements that was reported already in this conference. So double paddle 17 00:01:24,240 --> 00:01:30,330 scattering. Usually, I mean we use in the hc fullness right? So the cross section, 18 00:01:30,660 --> 00:01:36,900 and you I mean, you you can, all the cross sections, we calculate the HST based on 19 00:01:36,900 --> 00:01:41,280 some factorization, zero factorization conjecture. So that's the convolution of 20 00:01:41,280 --> 00:01:45,060 the partial distribute function and, and the pythonic cross section that can be 21 00:01:45,060 --> 00:01:50,640 perturbative calculated. Usually that we don't care about double bottom scattering 22 00:01:50,640 --> 00:01:55,410 because if you looking at the Julian's just inclusive productions there, of 23 00:01:55,410 --> 00:02:01,410 course you allow a lot of the softer interactions at the at the exit. An MPI I 24 00:02:01,410 --> 00:02:06,390 mean, but but if you do not ask to detect these eggs, usually, I mean unitarity 25 00:02:06,420 --> 00:02:11,670 guarantee that you, you don't care these right just just looking at one pattern 26 00:02:11,670 --> 00:02:15,480 scattering with another part of skirts in front and that'd be to produce the 27 00:02:15,510 --> 00:02:22,140 producer laptop pair for example. But if as long as you ask questions that how 28 00:02:22,230 --> 00:02:28,650 things happens when I detected both my laptop and AIX, then you are going to 29 00:02:28,650 --> 00:02:34,620 something of a mechanical production that you needed to know what these interaction 30 00:02:34,620 --> 00:02:39,030 happens here right? The example is, for example, Higgs production z and Higgs 31 00:02:39,030 --> 00:02:43,920 associate production right. So, if the two are both of the interactions, could it be 32 00:02:43,920 --> 00:02:49,350 hard that is allow you to do some perturbative calculations then you you are 33 00:02:49,350 --> 00:02:54,630 working in the in the usual I mean master formalism of the factorization serum. It's 34 00:02:54,630 --> 00:02:59,910 called the double bottom scattering and these actually this kind of I mean, this 35 00:02:59,910 --> 00:03:04,440 is Kind of mechanics has contributed a lot both for some signals if you're interested 36 00:03:04,440 --> 00:03:08,130 that you get interested in the development of scattering studies or to the 37 00:03:08,130 --> 00:03:15,750 backgrounds right he example is effects production, but I mean of course, this 38 00:03:15,780 --> 00:03:20,910 sometimes you need to care or of course, the DPS productions well, but for these I 39 00:03:20,910 --> 00:03:26,310 mean probably not relevant, I will tell you that because usually DPS is high test 40 00:03:26,490 --> 00:03:31,800 contribution, so usually power suppressed to come down to the single scattering. But 41 00:03:31,860 --> 00:03:36,780 I mean DPS can be enhanced it right. So if you see that you have the two part tonic 42 00:03:36,810 --> 00:03:43,650 incoming platonic PDFs if you're you have PDF, you have go to high high energy. So 43 00:03:43,650 --> 00:03:49,350 you have high high platonic densities like bronze to the small eggs, then of course, 44 00:03:49,350 --> 00:03:55,410 you enhance your sketching subsections. So normally, that single paddles scattering 45 00:03:55,410 --> 00:03:59,370 you just said the at hc, for example, it's just at the bottom density squared, but 46 00:03:59,790 --> 00:04:07,710 for DPS advanced scattering paddle density photos and then how to blow up with the 47 00:04:07,710 --> 00:04:12,630 double bottom scattering SDHC. And while we I mean since we know that the power 48 00:04:12,630 --> 00:04:18,090 counting about the other part of scattering first of course, if we do not 49 00:04:18,090 --> 00:04:23,730 go to extremely large scale, we just go to some low scales a bit low but still in the 50 00:04:23,730 --> 00:04:29,010 perturbative region for example, some hydro on the heavy flower production or 51 00:04:29,010 --> 00:04:33,300 the accordion productions right in principle these surprises not so much. So, 52 00:04:33,300 --> 00:04:38,190 you have the you have the chance you have heard to extract the significant GPS 53 00:04:38,190 --> 00:04:45,480 components and also you of course, you can see me Similarly, you can see some large 54 00:04:45,480 --> 00:04:48,840 yields production for example, not particularly hard yards but you're looking 55 00:04:48,840 --> 00:04:54,330 at the more inclusively like the jet mouse jet productions they have a lot of I mean 56 00:04:54,330 --> 00:05:00,000 large yields cross sections. So the normally you have to see some DPS company 57 00:05:01,650 --> 00:05:06,960 All you can precise measure this process then you may see some very small 58 00:05:07,320 --> 00:05:12,720 deviations compared to your SPS simulations. And also I mean it's it you 59 00:05:12,720 --> 00:05:18,570 need to be very precise measurements also very precise calculations in this case to 60 00:05:18,600 --> 00:05:24,270 strap the GPS and then also if you're good high high energy as I say the main if he 61 00:05:24,360 --> 00:05:29,550 becomes a VPS is is part of the density of the full dependency with respect to the 62 00:05:29,550 --> 00:05:35,430 SPS squared. So if you get high energies of course the enhancement is is more 63 00:05:35,460 --> 00:05:42,360 repetitive in the DPF thing, then SPS. So, you go to a tv 14 tv to even hundred TV Of 64 00:05:42,360 --> 00:05:48,090 course 200 TV you will you'll see even more processes 65 00:05:48,120 --> 00:05:48,780 in principle 66 00:05:49,560 --> 00:05:56,160 and also you can go to the ion sir because if you go to the proton nuclear or nuclear 67 00:05:56,160 --> 00:06:01,740 nuclear coalition, so each each each collisions you Have you have the 68 00:06:01,800 --> 00:06:06,150 enhancements from that because you have a lot of nuclear enters into your 69 00:06:06,150 --> 00:06:13,410 collisions. So you will see that the enhancements of DPS is more quickly then 70 00:06:13,650 --> 00:06:14,340 then the 71 00:06:14,970 --> 00:06:15,750 SPS 72 00:06:17,490 --> 00:06:19,830 I will go to these ponds later. 73 00:06:21,180 --> 00:06:27,720 So, the good thing is like SPS I mean like single particle scattering we right now we 74 00:06:27,720 --> 00:06:32,040 have settled theory foundation that is proved completely proven fact law So, you 75 00:06:32,040 --> 00:06:35,670 can see a room for the double bottom sketch of course, I mean for the color 76 00:06:35,670 --> 00:06:41,550 singlets final state Doubletree. Yeah but also even for SPS we only approved the 77 00:06:41,580 --> 00:06:46,800 kind of single is final states. So, in principle, I mean, this is the two papers, 78 00:06:46,830 --> 00:06:52,950 I prefer the two, the first paper trying to resolve the coming to see that all the 79 00:06:53,520 --> 00:06:58,080 billable grounds can be factorized, and a second amount to finalize all the softer 80 00:06:58,110 --> 00:07:03,270 sub graphs, you'll see that the picture So, right now, in principle we can say 81 00:07:03,270 --> 00:07:09,120 that okay we can write to the cross section of the two particle I mean to 82 00:07:09,180 --> 00:07:14,730 interaction final state production can be writing in fact lies the way that is each 83 00:07:15,990 --> 00:07:20,490 each one each and this is one atomic scattering and then the second pattern is 84 00:07:20,490 --> 00:07:26,190 cancelled and convoluted is some general lies that double Patil foundation sorry 85 00:07:26,250 --> 00:07:32,370 Patil pattern distribute functions, okay. So, here this is you can also view that, 86 00:07:32,850 --> 00:07:36,900 this kind of way, if you imagine VPS What do you can learn Of course, you can learn 87 00:07:36,900 --> 00:07:41,610 that So, you have a new way to access the information of the non fungible structure 88 00:07:41,610 --> 00:07:46,560 of nucleotides that is not can provide in the in one body in a single part of 89 00:07:46,560 --> 00:07:51,870 scattering that's usually relates to one body atomic structures. So, he has to say 90 00:07:51,870 --> 00:07:56,640 that you you, you have the generalized the double part on distributions and these two 91 00:07:56,640 --> 00:08:03,780 is simply the platonic scattering tu tu tu tu egg scattering if you want okay? Of 92 00:08:03,780 --> 00:08:09,780 course it still I mean we starting from these these forms we can I mean there's a 93 00:08:09,810 --> 00:08:15,510 large unknown from these two Nativity functions that matter also matter the bank 94 00:08:15,600 --> 00:08:22,170 dimensional the Y the spirit things we needed to do some simplifications, okay? 95 00:08:22,470 --> 00:08:27,960 So most of phenomenology actually rely on all these strong assumptions. That is 96 00:08:27,960 --> 00:08:35,490 you're assuming that your your general patterns and functions can be factorized 97 00:08:35,520 --> 00:08:39,870 out into the longitude boards and the transfers boards and also the longitude 98 00:08:39,870 --> 00:08:44,730 part actually, you can you can factorize out and that can be factored out. Okay. So 99 00:08:44,730 --> 00:08:50,250 this is the usual a PDF, single one body single PDF and these double double PDF, 100 00:08:50,280 --> 00:08:55,800 okay. And also, I mean, if you assuming there's just to get rid of the idea 101 00:08:55,800 --> 00:09:02,310 dependency, you have the one single just the ones perturbative sorry non 102 00:09:02,310 --> 00:09:09,000 perturbative number okay to to predict to predict all the DPS sections Valley 103 00:09:09,000 --> 00:09:12,990 predictive but of course you can cast to the in adults that way that these 104 00:09:13,020 --> 00:09:19,140 assumptions are valid general but even me even you can get rid of some of the 105 00:09:19,170 --> 00:09:23,940 federalization assignment simplification so you just have starting from these that 106 00:09:25,050 --> 00:09:30,720 this double PDF actually there's only one okay in the market because they are very 107 00:09:30,720 --> 00:09:37,410 very complicated to solve these is already included a multi dimensional structure 108 00:09:37,410 --> 00:09:40,890 also even for the evolution itself you gotta be collaborative who have 109 00:09:40,890 --> 00:09:44,790 evolutions. it's valid it's very complicated. So there's I left a few 110 00:09:44,790 --> 00:09:49,320 papers you if you're interested in the last few studies on these on these 111 00:09:49,320 --> 00:09:57,180 collections. So in general, the philosophy we have to how to how to be preceded for 112 00:09:57,210 --> 00:10:03,840 Ah, phenomenology is, let's ask justice. If we simply pop the formula and we 113 00:10:03,840 --> 00:10:08,700 compare with our predictions with with the experimental data, and if we find some 114 00:10:08,700 --> 00:10:12,060 deviations and we trust all our measurements or trust all of the 115 00:10:12,060 --> 00:10:18,120 calculations in this film here we can see that these deviations can be calling for 116 00:10:18,120 --> 00:10:24,570 the sum more leg loss treatment, okay. So, there are a few a few possible deviations 117 00:10:24,570 --> 00:10:30,690 to compare to the pocket formula. I just pick up a few examples. First is if you go 118 00:10:30,690 --> 00:10:37,800 to the devil, I mean you do not use these federalized PDF double PDF you just just 119 00:10:37,800 --> 00:10:42,930 working collecting these double PDF and you do the double Ecolab evolutions. Of 120 00:10:42,930 --> 00:10:44,580 course you don't know what's the initial 121 00:10:46,110 --> 00:10:51,390 assuming that the initiative scalable PDF is same as as in a scale of a single PDF 122 00:10:51,390 --> 00:10:56,940 squared. Then you perform the evolution. You see that there's a difference is 123 00:10:56,940 --> 00:11:02,610 blonde blonde over two grams at the end case with higher electric scale, you will 124 00:11:02,610 --> 00:11:12,210 see that for the the most I mean probation seems lafley Okay, I mean 10% 20% for most 125 00:11:12,240 --> 00:11:17,220 of x regions, except at the extremely high x reaches, okay you have you have some 126 00:11:17,220 --> 00:11:23,190 problem. I mean these apparently not working work well and mo and the second 127 00:11:23,190 --> 00:11:29,850 one is, I mean, when you work in the perturbative qc approach, you will see 128 00:11:29,850 --> 00:11:35,370 that actually not only have the two v two scattering, okay, you in fact have the 129 00:11:35,370 --> 00:11:40,320 perturbative non perturbative wrong comes out from the front. Hi, john Dang, the 130 00:11:40,320 --> 00:11:44,700 drunk and the debaters sprinting into the two patterns then have the scatterings 131 00:11:44,700 --> 00:11:51,510 code the two two v 2222 v 101 v two, okay. In principle you need to include because 132 00:11:51,510 --> 00:11:55,590 this is not including a single pattern scattering calculations well, right. So, 133 00:11:56,370 --> 00:12:00,690 you needed to include all of these contribution but you can argue that some 134 00:12:00,690 --> 00:12:05,700 point, this kind of contribution, could it be? Since it's perturbative regions could 135 00:12:05,700 --> 00:12:10,230 have been an activity or the contributions property suffers some points. But 136 00:12:10,230 --> 00:12:15,780 actually, the luminosity itself is not if you just calculate the luminosity of the 137 00:12:15,810 --> 00:12:22,050 wrong with with two grounds. And also the to mean for grants. I mean, you're for 138 00:12:22,050 --> 00:12:27,510 grants and one grant and two grants. So three grants, if you see the one, the two 139 00:12:27,540 --> 00:12:33,990 or two the one compares to the two for the two chip side and for the W and the cape 140 00:12:33,990 --> 00:12:37,860 side mass, which means you will see that's the actually compatible. 141 00:12:39,570 --> 00:12:40,140 And 142 00:12:42,570 --> 00:12:47,910 then I mean, the third one is that is that you can you can introduce a bit to the 143 00:12:47,910 --> 00:12:52,470 pattern pattern collections, you do not assume zero correction, aka full name, oh, 144 00:12:52,800 --> 00:12:58,440 and then you ask yourself what happens in that case? So then you will see some 145 00:12:58,470 --> 00:13:03,030 actually your stick by facts. Would it be not a number in mo it would it be depends 146 00:13:03,030 --> 00:13:09,390 on some some convex like because the x one x two and even some scares okay. So, this 147 00:13:09,390 --> 00:13:16,500 is this is a few papers and studies include these for the study this same sign 148 00:13:16,530 --> 00:13:24,900 up a W you see that these these long one is human zero collisions but if you if you 149 00:13:24,900 --> 00:13:30,240 have to put the collisions in you will see some the Sigma factor extracted from the 150 00:13:30,240 --> 00:13:37,170 different climatic regions it's a new one new to eat I want you to is is just the 151 00:13:37,170 --> 00:13:38,580 liquidity of the of the 152 00:13:39,720 --> 00:13:40,740 web. Okay. 153 00:13:41,490 --> 00:13:44,970 You have about two minutes left so I think it may be necessary to speed up 154 00:13:45,299 --> 00:13:50,669 Yeah, okay, thanks IV IV quickly I could go through. So you will see that there are 155 00:13:50,669 --> 00:13:55,019 some bitter, bitter dependent but it's very challenging because the DPS sip 156 00:13:55,079 --> 00:14:01,769 itself in the WWE already very small, they projected to see that you mean that if you 157 00:14:01,769 --> 00:14:06,959 find some one sigma deviation from the first being into the last day licklider 158 00:14:06,959 --> 00:14:12,239 1000. Emerson's about to observe these colors so the dependence is quite weak 159 00:14:13,349 --> 00:14:14,939 so actually there's a lot Hobbes 160 00:14:14,970 --> 00:14:19,470 says it quickly goes through so there's a if you see that the plot you will see them 161 00:14:19,740 --> 00:14:27,960 many jets measurements of final state and hc the photons as the W z bosons or 162 00:14:27,960 --> 00:14:36,990 observed the DPS have a flavor own use and W Yeah, okay. Of course, here I plot the 163 00:14:37,080 --> 00:14:41,040 Sigma factor from different entities you see that about the uncertainty still large 164 00:14:41,040 --> 00:14:48,690 enough, but you will you may see some non universal super effective patterns okay. 165 00:14:48,870 --> 00:14:52,170 So you can ask question with this rather dependent energy dependent kinematic 166 00:14:52,170 --> 00:14:58,620 dependence. So this is also see the talk on the Tuesday there's supposedly sensor 167 00:14:58,620 --> 00:15:04,830 same w this one The T by CMS. So, of course there's a caveat to that. There's a 168 00:15:04,830 --> 00:15:09,840 traveling thing to differentiate SPS DPS is easily expand ours, we can discuss all 169 00:15:09,840 --> 00:15:11,490 these how to extract the visa. 170 00:15:12,599 --> 00:15:13,259 This 171 00:15:13,289 --> 00:15:17,909 one example concrete example gave is the oops wrong magnify this arrow at the 172 00:15:17,909 --> 00:15:23,279 beginning they assume there's no DPS SPS and then you extract all the DPS the value 173 00:15:23,309 --> 00:15:28,739 if you Sorry, if you go to the include a bit of SPS you will see that value I mean, 174 00:15:28,799 --> 00:15:33,749 especially automatic changes this cabinet but if you go to heavy ion, as I said, 175 00:15:33,749 --> 00:15:40,439 there's there's DPS enhanced today is in particular for pa you see that is a factor 176 00:15:40,439 --> 00:15:46,289 of three A times of the day but to be known as Ts, it's the scanning as a as no 177 00:15:46,289 --> 00:15:52,229 nuclear modification and it is even enhanced mode. Of course, we know we 178 00:15:52,229 --> 00:15:56,189 cannot neglect to these nuclear modifications, these examples for heavy 179 00:15:56,219 --> 00:15:59,669 flavor and a core corneum. You'll see that the nuclear modification trade is very 180 00:15:59,669 --> 00:16:08,789 large. Probably 0.47 I mean RPA so we accommodated on my paper, I tried to think 181 00:16:08,789 --> 00:16:12,809 about these questions and to accommodate all the nuclear PT effect and the 182 00:16:12,809 --> 00:16:16,229 geometry, the previous release pharmacology, I'm shooting back. 183 00:16:17,549 --> 00:16:18,149 So, 184 00:16:18,570 --> 00:16:24,900 I quickly goes through that you see that the G delta G journalize double bottom 185 00:16:25,140 --> 00:16:31,620 structure functions right non dependence on these impact parameters. And, if I mean 186 00:16:31,680 --> 00:16:35,010 these Likewise, we know actually the nuclear modification at different 187 00:16:35,010 --> 00:16:38,850 positions, because it's one of the nuclear means will be depends on the impact 188 00:16:38,850 --> 00:16:45,270 validators Actually, this has been this kind of thing is is clashing to always be 189 00:16:45,270 --> 00:16:49,680 there as also you can also see from previous token, you need assuming 190 00:16:49,680 --> 00:16:53,070 something of the impact paramita dependence in the nuclear modifications. 191 00:16:53,430 --> 00:16:57,570 So, in the central clarity dependent observables out there, but worldwide 192 00:16:57,630 --> 00:17:04,200 assumptions, these kind of functions can linearly dependent on the on the on the 193 00:17:04,200 --> 00:17:10,470 sickness function. So, this gives us the idea that actually DPS in hockey I have a 194 00:17:10,470 --> 00:17:15,060 equations can have the potential to constrain these dependents okay. So, this 195 00:17:15,060 --> 00:17:20,160 is a concrete example I in my lesson papers see that if you looking at to the 196 00:17:20,520 --> 00:17:25,650 proton and and lead Christians for the website and the nasm production, you'll 197 00:17:25,710 --> 00:17:30,720 see that my DPS the nuclear modification factor with depends on at i mean i 198 00:17:30,720 --> 00:17:36,330 assuming the my g function is just the synchronous function time. So, that times 199 00:17:36,360 --> 00:17:41,640 a as opposed to a then you will see that it depends on the on the single part 200 00:17:41,700 --> 00:17:47,580 single nuclear manufactured modification factors and also geometry enhancement also 201 00:17:47,580 --> 00:17:49,590 the other terms comes. 202 00:17:50,130 --> 00:17:52,560 So, either actually these pieces you can 203 00:17:52,560 --> 00:17:56,430 calculate or fixed by other measurements under the same conditions for example, 204 00:17:57,000 --> 00:18:01,140 right. So, in particular use I mean you see that why there Such a tripping hazard 205 00:18:01,140 --> 00:18:07,050 and this kind of thing, in fact gives you a very large enhancement. I mean if you're 206 00:18:07,050 --> 00:18:13,440 sick when in fact it's not small enough small enough So here is an example that I 207 00:18:13,470 --> 00:18:19,170 studied. In my paper you see that for the chips ID zero production as the period. 208 00:18:19,920 --> 00:18:26,370 The difference we have some description power to differentiate the DPS components 209 00:18:26,370 --> 00:18:32,580 and SPS components and also DPS strongly dependent on the assumption of a g 210 00:18:32,580 --> 00:18:39,810 function. Okay. This is RTA. So I quickly I think, I quickly afresh these warming 211 00:18:39,810 --> 00:18:44,580 these are actually our first DPS measurements in heavy IoT become soon by 212 00:18:44,640 --> 00:18:46,920 HCP has been seen on Wednesdays 213 00:18:47,040 --> 00:18:47,610 talk. 214 00:18:48,750 --> 00:18:55,440 So I go to my conclusion, associate production is at hc actually opens a new 215 00:18:55,440 --> 00:18:59,460 area for studying GPS and if you have witnessed a lot of theoretical and 216 00:18:59,460 --> 00:19:03,660 phenomenon logical and experiments progress, but some theoretical issues 217 00:19:03,660 --> 00:19:08,640 still persist to better predict the future is implied. And the main interesting 218 00:19:09,000 --> 00:19:14,700 measurements are coming. It's also exciting time that the first GPA studying 219 00:19:14,700 --> 00:19:19,980 heavy is coming. And I believe that we can definitely learn more from these these 220 00:19:19,980 --> 00:19:24,780 measurements this data, for example, I give example the we can learn actually the 221 00:19:24,780 --> 00:19:29,010 impact on the dependent nuclear power distributed functions. And you can also 222 00:19:29,010 --> 00:19:35,250 sync that other nuclear modification factors, how these can be included in the 223 00:19:35,280 --> 00:19:36,990 in these DPS focus. 224 00:19:37,860 --> 00:19:42,870 Okay, thank you. Thank you very much rushing for this very comprehensive and 225 00:19:42,870 --> 00:19:47,310 detailed talk. It's very interesting. Now in order to keep up with the schedule, I 226 00:19:47,310 --> 00:19:53,370 think we probably did not have time for a question right now. But we are of course 227 00:19:53,370 --> 00:19:58,200 able to come back and discuss and ask questions about this set of slides and 228 00:19:58,200 --> 00:20:00,480 this nice presentation during our discussion. session. 229 00:20:01,650 --> 00:20:04,020 So let's think crushing again and we move