1 00:00:00,870 --> 00:00:05,280 For on physics perspectives for Alice and run for 2 00:00:11,130 --> 00:00:12,120 Can you hear me? 3 00:00:12,150 --> 00:00:13,500 Yes, we can hear you. Well, 4 00:00:14,010 --> 00:00:19,620 okay, perfect. Just a moment. No problem. Can you see the slides? 5 00:00:19,799 --> 00:00:24,929 Yes. Okay. Thank you very much. Thank you very much. And good afternoon, everybody. 6 00:00:25,289 --> 00:00:30,629 It's a pleasure for me to be told on behalf of the collaboration on the physics 7 00:00:30,629 --> 00:00:38,909 perfect perspectives for IBC. So, the first say the primary physics programmer 8 00:00:38,909 --> 00:00:43,049 for the release experimenter is the study of the properties of the colada confined 9 00:00:43,049 --> 00:00:47,399 medium called corpulent plasma, which is created the neutral atavistic API on 10 00:00:47,399 --> 00:00:55,649 collisions such as C which presents a very high initial energy density, and after a 11 00:00:55,649 --> 00:01:01,109 pre equilibrium phaser expands either dynamically like hundred percent A liquid 12 00:01:01,409 --> 00:01:06,179 before other than icing in almost thermography do. So, one of the key 13 00:01:06,179 --> 00:01:12,239 observables for these studies are the flip of particles, since a flavors are created 14 00:01:12,239 --> 00:01:16,319 in short timescales compared to the formation time, and then they experience 15 00:01:16,349 --> 00:01:22,859 the food system evolution and we can use them as probes of the plasma. So, the 16 00:01:22,859 --> 00:01:29,069 Alice collaboration is preparing a wider upgrade programs with the serum three and 17 00:01:29,069 --> 00:01:34,109 four, with the aim of increasing the collected lead luminosity by more than one 18 00:01:34,650 --> 00:01:35,940 order of magnitude. 19 00:01:36,540 --> 00:01:43,170 And for this, the upgrades of the LDC needed for this LED luminosity, we will 20 00:01:43,170 --> 00:01:48,240 already be completing the long shutdown to suffer Aleksey factory. The main physics 21 00:01:48,240 --> 00:01:53,070 motivations for this upgrade, so include the study of the trauma and introduction 22 00:01:53,070 --> 00:01:59,070 and under detection into quantum plasma, the measurement of Konya down to PT zero 23 00:01:59,100 --> 00:02:03,000 in order to study that melting and regeneration in the in the courtroom 24 00:02:03,000 --> 00:02:10,350 plasma thermal radiation and the possible current symmetry separation at the phase 25 00:02:10,350 --> 00:02:17,370 transition and the precise measurements of lighter hyper nuclei and the searches for 26 00:02:17,370 --> 00:02:23,550 more exotic nuclei such as chump icon. So, the main requirements for this physics 27 00:02:23,550 --> 00:02:29,010 program are the increasing increase the result writer to get with a reduction of 28 00:02:29,010 --> 00:02:33,690 the data size for the storage, the improvement of the talking and the texting 29 00:02:33,690 --> 00:02:38,520 capabilities are low transfer mentum and at the same time the preservation of 30 00:02:38,550 --> 00:02:44,340 particle identification capabilities of the experiment. So the current upgrades 31 00:02:44,580 --> 00:02:47,160 that we are 32 00:02:48,060 --> 00:02:54,900 focusing on to include the the substitution of the readout chambers for 33 00:02:54,900 --> 00:02:59,970 the time protection chamba in order to cope with the higher event rate expected 34 00:03:01,230 --> 00:03:05,280 The replacement of the inner silicon tracker of Elissa Dena tracking system 35 00:03:05,580 --> 00:03:13,890 with a new detector based on seven pixel layers of mono mono etica active pixel 36 00:03:13,890 --> 00:03:22,110 sensors, which will also be used for a new forward tracker is empty. That would be 37 00:03:22,110 --> 00:03:27,930 used to match the tracks measured in the forward muon spectrometer with the central 38 00:03:27,930 --> 00:03:32,790 barrier of Elisa and finally had the introduction of new detector forward 39 00:03:32,790 --> 00:03:37,410 detector for the trigger called the fast interaction trigger for which we have two 40 00:03:37,410 --> 00:03:42,600 pulses. If you are interested, I invite you to look at that. Together with these 41 00:03:42,600 --> 00:03:46,680 upgrades, we will also have to upgrade the readout electronics or several detectors 42 00:03:46,680 --> 00:03:52,710 to cope with the with the iron production right expected. If you missed the talk by 43 00:03:52,710 --> 00:04:00,330 kotra, I suggest you to look at the slides that were uploaded yesterday. Took At the 44 00:04:00,330 --> 00:04:07,830 same time, we are preparing new upgrades for the LSC ram four, which includes the 45 00:04:07,830 --> 00:04:12,600 introduction of our forward calorimeter called photon and the further upgrade of 46 00:04:12,600 --> 00:04:19,110 the inner tracking system based on the replacement of the three innermost layers. 47 00:04:19,740 --> 00:04:26,400 So, I will start with the discussion of the focal calorimeter which will include 48 00:04:26,430 --> 00:04:32,190 an electro magnetic high granularity silicon tungsten sampling Corona meter for 49 00:04:32,190 --> 00:04:37,560 the measurement of direct protons and the zero mass also, and another ronica 50 00:04:38,010 --> 00:04:43,410 sampling kilometer for photon isolations and jets. So, the main goal for this 51 00:04:43,530 --> 00:04:48,960 detector will be to set constraints on the nuclear PDFs at smaller transfer mentum. 52 00:04:49,380 --> 00:04:51,480 And in particular to do on PDFs. 53 00:04:52,530 --> 00:04:58,710 The grown PDFs are, let's say not very well constrained also for the proton in 54 00:04:58,710 --> 00:05:02,190 the low X ray drawn below 10 to the minus four. 55 00:05:02,850 --> 00:05:04,230 And in particular, 56 00:05:05,549 --> 00:05:10,769 the measurement from measurements from deep in elastic scattering indicates that 57 00:05:10,769 --> 00:05:17,579 the ground density increases rapidly at low x and the digital output and BHK and 58 00:05:20,789 --> 00:05:27,239 equation so, predictor, I've had the growth at lower x. So we can ask ourself, 59 00:05:27,479 --> 00:05:31,769 if we should expect an infinite growth or a mechanism to tame the blue one subtle 60 00:05:31,769 --> 00:05:34,559 axes such as doing fusion or doing subtraction. 61 00:05:36,900 --> 00:05:38,130 In fact, 62 00:05:40,770 --> 00:05:45,990 the classical way of studying PDFs, the Gnostic scattering experiments, which 63 00:05:45,990 --> 00:05:51,090 however, are not sensitive to the dual PDFs are at the leading order, while the 64 00:05:51,090 --> 00:05:55,020 measurement of isolated photons are thorough there, it is sensitive about the 65 00:05:55,020 --> 00:05:59,370 leaky gut. And in particular, it is a very large contribution from Compton 66 00:05:59,370 --> 00:06:09,690 scatterings So in this plot, you can see basically, the region that will be covered 67 00:06:09,720 --> 00:06:17,220 in the Q and x by different experiments, including Alexey but not not only at also 68 00:06:17,220 --> 00:06:24,480 electron Iam Collider. So, recap experiments and then and then the next one 69 00:06:24,480 --> 00:06:31,110 so abcb in particular, and this new detector for call that as you can see we'd 70 00:06:31,110 --> 00:06:40,290 have the lowest X ray feature of the other experiments. In slide number eight, you 71 00:06:40,290 --> 00:06:45,570 can see the expected performance of for this isolated photon measurement. And in 72 00:06:45,570 --> 00:06:50,010 particular, you can see the expected performance for the nuclear modification 73 00:06:50,010 --> 00:06:55,320 factor which is a key observable in API on collisions. And it's defined as the ratio 74 00:06:55,320 --> 00:06:59,040 between the piti differential it's measured in ATM conditions in this case p 75 00:06:59,040 --> 00:07:06,150 delta Those are measured in equaliser scaled by the average number of nuclear, 76 00:07:06,150 --> 00:07:11,040 nuclear and binary drops. So the expected precision for this measurement will be 77 00:07:11,400 --> 00:07:18,930 about 20% above 60 v over c. And if you look at it compared to the current 78 00:07:19,740 --> 00:07:25,350 parameterization of the blue and nonnuclear PDFs from EP PPS 16. You will 79 00:07:25,350 --> 00:07:30,000 see you can see and appreciate the significant improvement to the tool set to 80 00:07:30,000 --> 00:07:37,890 constrain those nuclear PDFs. This can be seen even better in this plot, where you 81 00:07:37,890 --> 00:07:43,620 can see basically, the gray region which represents the current knowledge of the 82 00:07:43,620 --> 00:07:47,130 nuclear PDFs from the opinion are six scatterings which are basically 83 00:07:47,160 --> 00:07:54,660 unconstrained for 10 to the minus two of the exit. Even if we currently have some 84 00:07:54,660 --> 00:07:59,100 constraints, which are provided by hf measurements are followed the PDK by 85 00:07:59,100 --> 00:08:05,280 Edison receiving However, if you will compare this fence with the one expected 86 00:08:05,280 --> 00:08:11,010 for electron Iam Collider in green and the one for Can you you can appreciate how 87 00:08:11,010 --> 00:08:16,710 difficult would be crucial to set constraints on these nuclear PDFs at very 88 00:08:16,710 --> 00:08:21,180 low X up to I would say 10 to the minus 510 to the minus six. 89 00:08:23,250 --> 00:08:25,920 I will now move to the second 90 00:08:28,230 --> 00:08:33,570 experiment for the LSU Drum Corps, which will be the replacement of the three in 91 00:08:33,900 --> 00:08:40,530 three Nirmal slayers of the IPS and for which are very new detector technology 92 00:08:41,100 --> 00:08:46,620 will be used in particular had this technology and will will allow us to have 93 00:08:46,680 --> 00:08:53,430 three to the cylindrical pixel layer So, based on this ultra thin Weber's wafer 94 00:08:53,430 --> 00:08:54,810 size the covert sensor 95 00:08:55,170 --> 00:08:57,870 for which you can ever let's see on 96 00:08:59,190 --> 00:09:05,070 a feeling good Looking at the picture in the typewriter, which basically will allow 97 00:09:05,070 --> 00:09:10,140 us to reduce drastically the material budget, in particular getting rid of 98 00:09:10,140 --> 00:09:17,640 external connections or cooling. And you can see quantitatively in this table, how 99 00:09:17,640 --> 00:09:24,210 the material budget will be reduced. And if we compared to the IQs 190s to the 100 00:09:25,350 --> 00:09:33,240 percentage of radiation length per layer, we'd go from one point 14% to zero 38 in 101 00:09:33,240 --> 00:09:39,300 the first upgrade of the APS up to zero down to zero dot 05 percent for the ITC. 102 00:09:40,080 --> 00:09:47,430 And, but this will not be the only key feature of this detector. We will also go 103 00:09:47,700 --> 00:09:53,820 closer to the interaction point down to 18 millimeters and we will reduce the other 104 00:09:53,880 --> 00:10:02,550 the pixel sizes and the current proposal is a 1515 Don't micrometres. So this will 105 00:10:02,640 --> 00:10:08,070 of course greatly improve our pointing resolution by a factor of two compared to 106 00:10:08,070 --> 00:10:13,740 the first upgrade of the IPS in the foot PT Ranger, but also the tracking 107 00:10:13,740 --> 00:10:19,350 efficiency that will increase by up to 1.2 to two compared to the inner tracking 108 00:10:19,350 --> 00:10:28,800 system to in the low PT region. So, below under the V oversee several measurements 109 00:10:28,950 --> 00:10:35,820 will be greater and here I have a non exhaustive list of data, which included 110 00:10:35,820 --> 00:10:39,300 the low mass di leptons are the measurement of beauty strange medicines 111 00:10:39,300 --> 00:10:45,000 and beauty baryon. So, the champ strange and strange variants production and the 112 00:10:45,000 --> 00:10:49,410 searches for light charm I've been apply so I don't have time to discuss all of 113 00:10:49,410 --> 00:10:56,490 them. So I just chose some of these that I will show you in the next face. I was 114 00:10:56,490 --> 00:11:02,460 taught from the law master leptons, which is a Particularly particularly interesting 115 00:11:02,550 --> 00:11:09,030 in our field, because the slope of the entire mass distribution at intermediate 116 00:11:10,350 --> 00:11:16,020 masses, so between say one and two is related to the cutiepie temperature. So, 117 00:11:16,020 --> 00:11:20,700 the precise measurement will be very important to define the TDP temperature 118 00:11:20,700 --> 00:11:29,670 and the IQ three will will greatly help in this by providing a much better chance of 119 00:11:29,670 --> 00:11:36,450 rejection and also much better rejection of the contribution from gamma 120 00:11:36,450 --> 00:11:40,620 conversions. The reduction of the systematic uncertainty that we foresee 121 00:11:41,340 --> 00:11:45,810 with the ITC is up to up to two and the statistical uncertainties are four factor 122 00:11:45,810 --> 00:11:51,420 three and you can see in the bottom right plot, how this will impact in our 123 00:11:51,450 --> 00:11:57,810 determination of the PGP attack. The second topic that I would like to discuss 124 00:11:57,870 --> 00:12:03,750 is the study of the beautiful colorization mechanism in the courtroom plasma and in 125 00:12:03,750 --> 00:12:10,770 particular, I will start I will start to discuss the recent nasm doctrine, which is 126 00:12:10,770 --> 00:12:16,500 expected to be announced if the beaut quarks are denied via recombination in the 127 00:12:16,860 --> 00:12:24,990 plasma due to the analysis strange core production in Indonesia itself. So, in the 128 00:12:25,050 --> 00:12:30,960 left plot, you can see the improvement in the statistical significance that we 129 00:12:30,960 --> 00:12:36,900 expect in the measurement of the P sub s Mason production with the ITC compared to 130 00:12:36,900 --> 00:12:42,690 the IPS tool, and on the writer you can see the projected nuclear modification 131 00:12:42,690 --> 00:12:50,010 factor which as you can see, we provide the basically, the ITC will provide us 132 00:12:50,340 --> 00:12:55,170 access to the measurement down to very, very low PT for for idi conditions 133 00:12:56,340 --> 00:12:58,500 and the exclusive 134 00:13:00,000 --> 00:13:07,050 Trouble is the only way to measure the beauty of strange production. In the in 135 00:13:07,050 --> 00:13:10,830 the courtroom plasma, we can also explore to nonprofit service which largely come 136 00:13:10,830 --> 00:13:16,230 from be subsidized loans. So even if it's not a direct measurement, it's sensitive 137 00:13:16,230 --> 00:13:21,090 to the service production and it has the advantage of having legit statistical 138 00:13:21,090 --> 00:13:26,910 precision that exclusive b sub s reconstruction. So, on the right again you 139 00:13:26,910 --> 00:13:28,230 can see the projected the 140 00:13:29,309 --> 00:13:30,509 expanded the 141 00:13:31,110 --> 00:13:36,330 Thank you, nuclear modification factor for impromptu discipleship. And as you can 142 00:13:36,330 --> 00:13:40,260 see, we will have the sensitivity to distinguish the two scenarios. So the one 143 00:13:40,260 --> 00:13:46,410 of the non prompt to the suppressor, which comes from the B sub SDKs and the non prom 144 00:13:46,410 --> 00:13:50,100 to the zeros which means that comes from non central demand zones and are not 145 00:13:50,100 --> 00:13:57,300 sensitive to destruction. Thanks to the larger statistical procedures of the non 146 00:13:57,300 --> 00:14:03,930 property service, we will be able to To look at more differential observables as 147 00:14:03,960 --> 00:14:08,580 the azimuthal anisotropy which is connected to the participation of beauty 148 00:14:08,580 --> 00:14:13,440 quarks in the collective motion of the system, and its possible thermalization in 149 00:14:13,440 --> 00:14:17,130 the problem plasma, so it gives us more information about the beauty called 150 00:14:17,130 --> 00:14:23,040 diffusion coefficient in the queue GP. And as you can see in this direction, the IDS 151 00:14:23,040 --> 00:14:31,350 three will give us enough precision to distinguish between the expected as the 152 00:14:31,350 --> 00:14:35,250 motor isotropy for prompter and prompter D sub s medicals. 153 00:14:36,809 --> 00:14:38,159 Finally, add 154 00:14:39,870 --> 00:14:45,750 beauty quantization can also be studied via the production of beauty baryons. So, 155 00:14:45,750 --> 00:14:49,890 in round two Ellis already performed several measurements of charm barium 156 00:14:49,890 --> 00:14:55,860 production and observed and mass production compared to classy minds, 157 00:14:55,860 --> 00:15:02,010 collisions, already MPP collisions but even even larger Let that conditions. So, 158 00:15:02,010 --> 00:15:07,560 the idea is when the ITC will provide us the possibility to study also the beauty 159 00:15:07,560 --> 00:15:14,610 barium productions and the ITC will will give an improvement of statistical 160 00:15:14,610 --> 00:15:21,510 significance of cofactor 2.5 with respect to the idea is to the last topic that I 161 00:15:21,510 --> 00:15:28,740 want to discuss is expected performance for the searches of term hyper nuclei 162 00:15:28,770 --> 00:15:33,480 which were predicted already in the 70s and never observed. So, the lighter 163 00:15:33,480 --> 00:15:37,620 possible state is this bound state of lambda C and the neutron which is called 164 00:15:37,620 --> 00:15:44,220 the neutron for which the ITC will be crucial, since the expected decay length 165 00:15:44,220 --> 00:15:51,360 of the CDU term state is approximately the same of the one of the lambda C which is 166 00:15:51,540 --> 00:15:57,450 around 60 microns. So, in this plot, you can see basically the comparison between 167 00:15:57,450 --> 00:16:02,700 the impact parameters of neutrons from a CD case which will be our signal and the 168 00:16:02,700 --> 00:16:08,790 primary neutrons which will compose the largest contribution to the to the 169 00:16:08,790 --> 00:16:13,500 background. So, this brings me to my summary at the Alice experiment is 170 00:16:13,500 --> 00:16:18,540 undergoing a major upgrade already long shutdown to in view of the list here on 171 00:16:18,540 --> 00:16:23,730 three butter, we are preparing new upgrades for the receipt on car which 172 00:16:23,730 --> 00:16:31,410 includes forward kilometer bespoke Allah mendy for the to set constraints on them 173 00:16:31,410 --> 00:16:39,330 clarified yet so, in the low x region and these innovative truly cylinder calcium 174 00:16:39,330 --> 00:16:46,080 detector for the inner layers of the IPS which will be which will be based on new 175 00:16:46,080 --> 00:16:52,530 13 wave size sensor which will improve the doctor the measurements of low mass 176 00:16:52,560 --> 00:16:57,810 electrons, hf particles and the searches of exotics. And thank you for your 177 00:16:57,810 --> 00:16:58,320 attention. 178 00:16:59,520 --> 00:17:00,630 Thank you for Talk 179 00:17:02,399 --> 00:17:02,999 alright. 180 00:17:04,650 --> 00:17:06,210 Other Any questions? 181 00:17:12,570 --> 00:17:14,940 Does the raise hand function actually work? 182 00:17:18,330 --> 00:17:22,920 Ah I see I see a raised hand on the panelists Nicola please go ahead you can 183 00:17:22,920 --> 00:17:25,170 unmute yourself, can you hear me? Yes, 184 00:17:25,199 --> 00:17:30,629 yes, I was interested in the in the measurements that you showed to the 185 00:17:30,629 --> 00:17:35,579 announcement of lambda c over d zero. So, 186 00:17:36,810 --> 00:17:37,410 this is 187 00:17:38,520 --> 00:17:40,320 measured only in this 188 00:17:41,640 --> 00:17:49,320 lead lead or it is also expected in other collisions. So, in this plot, you can see 189 00:17:49,320 --> 00:17:54,360 basically the measurements in PP collisions which had the green points and 190 00:17:54,360 --> 00:17:59,040 then in lead lead collisions, where you have basically two centrality classes so 191 00:17:59,040 --> 00:18:04,800 in the ion collisions We divide the events in society classes, and the red ones 192 00:18:05,160 --> 00:18:09,960 corresponds to the most central conditions. And so as you can see the the 193 00:18:09,960 --> 00:18:15,840 announcement that we measure is already there in the teepee conditions. And indeed 194 00:18:15,840 --> 00:18:19,500 there is a tension with the with the measurement of ABCD. 195 00:18:20,940 --> 00:18:23,610 Because also for ECB, our 196 00:18:25,170 --> 00:18:31,530 announcement is measured, but it's quantitatively smaller. So this is a is an 197 00:18:31,530 --> 00:18:38,220 open question at the moment, which could point to rapidity dependence, but it's not 198 00:18:38,250 --> 00:18:42,780 not solved yet. Thank you. 199 00:18:50,070 --> 00:18:51,480 There are more questions. 200 00:18:58,470 --> 00:19:00,900 I don't see any more All right now, 201 00:19:02,399 --> 00:19:05,249 I think we can also just 202 00:19:06,720 --> 00:19:12,780 open it up for questions with respect to all the talks, because we do still have 203 00:19:12,930 --> 00:19:19,350 about 10 minutes left for discussion if needed. So, if there any more questions 204 00:19:19,380 --> 00:19:27,180 either on for Rich's talk or on any of the other talks or somewhat related to the 205 00:19:27,750 --> 00:19:34,230 overall picture that was shown for the for NHD experiments, some respect to their 206 00:19:34,260 --> 00:19:35,370 next upgrades 207 00:19:37,170 --> 00:19:38,160 Please go ahead. 208 00:19:54,000 --> 00:19:59,370 Okay, if not, I do have a question for ability which is more hardware related but 209 00:20:00,540 --> 00:20:06,840 So I'm quite impressed by this ultra thin wafer. So does it does it also contain the 210 00:20:06,840 --> 00:20:10,530 reader electronics in addition to the to the center? So is it just the center? 211 00:20:11,039 --> 00:20:17,009 Yeah, so I mean, I didn't spend much on on the other, but the sensor will be one 212 00:20:17,549 --> 00:20:22,919 monolithic active pixel sensors. So the yard readout from the front end result 213 00:20:22,919 --> 00:20:29,219 would be in the in the chips themselves. And these of course, will will lead to 214 00:20:29,219 --> 00:20:31,799 decrease even added the material budget. 215 00:20:33,240 --> 00:20:33,990 Absolutely. 216 00:20:35,310 --> 00:20:38,160 But unfortunate that we might have too much radiation 217 00:20:38,730 --> 00:20:45,690 to the house for the detectors. Yeah, of course, he nearly said the radiation is 218 00:20:45,690 --> 00:20:48,000 different than Atlas and CMS but yeah. 219 00:20:50,790 --> 00:20:54,990 And while you since you asked, I didn't have time, but I also prepare the slider 220 00:20:57,630 --> 00:21:05,340 Next, the round five In preparation, where this technology could be exploited even 221 00:21:05,340 --> 00:21:13,320 more, and we are thinking about this old silicon detector, which, which of course 222 00:21:13,350 --> 00:21:21,750 in the inner layers will exploit to these same sources. And this is also in my 223 00:21:21,750 --> 00:21:28,230 opinion very interesting, we will get rid of well, we will remove, of course, to the 224 00:21:28,260 --> 00:21:37,980 PC to go faster in the result of events. And, but, but keeping the particle 225 00:21:37,980 --> 00:21:43,200 identification with with time of flight layers, and of course, if you're 226 00:21:43,200 --> 00:21:49,110 interested, we had a talk yesterday by Roberto so you can have a look at the 227 00:21:49,110 --> 00:21:49,980 slides. 228 00:21:55,980 --> 00:21:58,290 That's indeed an interesting concept. 229 00:22:00,000 --> 00:22:02,550 Are there any more questions? 230 00:22:11,309 --> 00:22:13,199 I don't see any raised hands. 231 00:22:15,360 --> 00:22:18,690 Everybody wants coffee. I hope you all got a coffee machine at home. 232 00:22:21,480 --> 00:22:24,210 Okay, in case there are no more questions 233 00:22:26,010 --> 00:22:34,800 I would just like to remind you all of the coffee chat room that are failing to his 234 00:22:34,800 --> 00:22:40,110 slides in case you have more questions and dialogues. But maybe also the other 235 00:22:40,410 --> 00:22:45,300 speakers from the session want to join there and can also answer more questions 236 00:22:45,300 --> 00:22:52,020 in case they come up over coffee. And other than that, I think