1 00:00:10,830 --> 00:00:15,630 Okay, so Hi everyone. My name is Mater Zaretsky. And on behalf of Atlas and CMS, 2 00:00:15,660 --> 00:00:20,340 I would like to give you an overview of the soft Susy searches at Atlas and CMS. 3 00:00:22,110 --> 00:00:27,660 So, as we all know, wide regions of Suzy parameter space have been excluded with 4 00:00:27,690 --> 00:00:34,380 recent Etsy results, and this is putting natural Suzy under extreme pressure. So on 5 00:00:34,380 --> 00:00:39,930 the left here we have a summary exclusion limit for regional neutralino production 6 00:00:40,830 --> 00:00:47,970 by Atlas. And on the right you have just an example the stop production limits from 7 00:00:47,970 --> 00:00:53,100 CMS. So as you heard in the previous two talks, and many of these regions were 8 00:00:53,100 --> 00:00:58,650 covered in the previous two talks by Carlos and mark and highlighted here in 9 00:00:58,650 --> 00:01:03,750 both plots See that there are several crevices of parameter space which are so 10 00:01:03,750 --> 00:01:09,510 uncovered. And this talk focuses on soft Susy searches with very compressed mass 11 00:01:09,510 --> 00:01:13,920 spectrum. So this is where the delta between the initial and final particles is 12 00:01:13,920 --> 00:01:18,600 very small. And I think there's these plots also show and hopefully my 13 00:01:18,600 --> 00:01:22,650 presentation shows that there's a significant effort both at Atlas and CMS 14 00:01:22,950 --> 00:01:32,280 focusing on this region. So, so why self Susie? So natural Suzy requires relatively 15 00:01:32,280 --> 00:01:37,830 light stops extraneous and gluey knows the small mass splittings can reproduce the 16 00:01:37,830 --> 00:01:43,200 correct cosmological Dark Matter abundance and this is via the process of coagulation 17 00:01:43,200 --> 00:01:51,210 of neutrinos and light stops, or charge, dinos and also soft products give access 18 00:01:51,210 --> 00:01:56,220 to compressed electronic Susy models. So even though there are lower cross sections 19 00:01:56,220 --> 00:02:00,990 for electric electrically Kino production with respect to strong production, With 20 00:02:00,990 --> 00:02:06,930 with going lower and pts, we can have access to these models. So light Exynos. 21 00:02:06,960 --> 00:02:12,660 And electric models also provide a window to natural Susy. But you've heard some of 22 00:02:12,720 --> 00:02:21,420 the details and Carlos system already. So, so in these kinds of scenarios where the 23 00:02:21,420 --> 00:02:27,510 mass splitting is very small, there's little available energy. So the final 24 00:02:27,510 --> 00:02:35,370 states are very soft and there's low math. So, as for example, here on the top right 25 00:02:35,370 --> 00:02:42,900 plot, you can see the leptin PT spectrum and the signal for delta m of 10. You can 26 00:02:42,900 --> 00:02:49,080 see how fast how fast it drops. And typically these these these are missed 27 00:02:49,080 --> 00:02:54,720 these regions are missed by classical searches which require high met and or 28 00:02:54,720 --> 00:03:00,000 lepton pts. So there's a lot of inefficiency also for object three 29 00:03:00,000 --> 00:03:05,280 Construction at very low pities and typically visible decay products not as 30 00:03:05,280 --> 00:03:10,710 the acceptance thresholds. So for these types of searches we require low threshold 31 00:03:10,710 --> 00:03:16,830 triggers and accurate reconstruction. However, what most of these searches for 32 00:03:16,830 --> 00:03:20,820 this characteristic of most of these searches is that we require initial state 33 00:03:20,820 --> 00:03:26,580 radiation. So this is typically a clue and dread originating from Parton's. So, this 34 00:03:26,580 --> 00:03:31,350 boosts the signal vertex and the visible decay products become detectable. So, the 35 00:03:31,350 --> 00:03:35,850 typical signature these searches and the very compressed regions is a heartbreaker 36 00:03:35,880 --> 00:03:40,860 is our jet. Therefore, the math is boosted So, there's moderate math and then we 37 00:03:40,860 --> 00:03:47,400 still have soft leptons and or jets. Sunday searches leptons go down to several 38 00:03:47,400 --> 00:03:53,400 jeebies and many analysis actually, but veto B tech threats, which are not 39 00:03:53,400 --> 00:03:58,710 expected which are too soft to be detected. And in terms of I saw some 40 00:03:58,710 --> 00:04:05,040 analysis Try some more sophisticated methods and try to tack the ice or jet. So 41 00:04:05,040 --> 00:04:12,480 for example and all hydronic Susy search, I started jets attack using large radius 42 00:04:12,480 --> 00:04:20,130 capturing fluids undergoing splitting. So now I'd like to give you an overview of 43 00:04:20,130 --> 00:04:27,480 the different searches, sub searches, with a focus on the most recent results. So 44 00:04:27,480 --> 00:04:34,020 starting with self multi leptons, so for self leptons, there are two searches, 45 00:04:34,350 --> 00:04:39,840 their searches an Atlas and CMS, so requiring to self opposites and leptons. 46 00:04:40,170 --> 00:04:45,450 So in Atlas search, they're required to same flavor lepton pairs in two different 47 00:04:45,450 --> 00:04:51,510 channels, one the electronic channel and one with one lepton and one track and 48 00:04:52,890 --> 00:04:58,530 this search has three main signal regions targeting electrode Kynos slept on and vbf 49 00:04:58,530 --> 00:05:04,590 production On the right on the plot on the top right, you can see one of the 50 00:05:04,650 --> 00:05:09,030 discriminating variables they use is the invariant mass of the two leptons. And you 51 00:05:09,030 --> 00:05:15,750 can see that for different for different models, and you can see that it has a 52 00:05:15,810 --> 00:05:17,010 kinematic endpoint. 53 00:05:19,530 --> 00:05:21,000 It has a kinematic edge. 54 00:05:22,470 --> 00:05:30,090 Then for for the suzay search. It's it's quite similar. However, it requires same 55 00:05:30,120 --> 00:05:37,380 or different flavor pairs. And also not only considers electro Kino, but also stop 56 00:05:37,380 --> 00:05:41,610 selections in the signal region building is done in terms of 57 00:05:42,960 --> 00:05:43,920 the environment. 58 00:05:46,470 --> 00:05:51,660 And one interesting point here on the right, is that this search has a dedicated 59 00:05:51,660 --> 00:05:56,190 time one plus ATMs sugar. So So here's the 60 00:05:57,630 --> 00:06:00,480 trigger turn on of this of this particular trigger. 61 00:06:01,920 --> 00:06:06,540 And it's it's used to access lower math regions to increase the sensitive 62 00:06:06,570 --> 00:06:13,020 sensitivity for very small delta AMS. So just a comment that searches a foreign 63 00:06:13,020 --> 00:06:24,390 two, whereas the bottom one is the US in 2016 data. So focusing on Atlas result, 64 00:06:24,390 --> 00:06:28,710 which is my most recent so you've definitely heard about already in the 65 00:06:28,710 --> 00:06:33,000 previous talks as well about the recursive fixer reconstruction. So in terms of 66 00:06:33,000 --> 00:06:41,280 these, these searches, it focuses on it splits the event into an ASR part and a 67 00:06:41,610 --> 00:06:47,550 Suzy part. And the variables that are used are quantifying the ice or recall so the 68 00:06:47,550 --> 00:06:52,320 ratio of Matt and the beauty of the ASR system and also the transverse mass of the 69 00:06:52,320 --> 00:06:57,090 Suzy system. So this is one of one of the variables that's used in the beginning. 70 00:06:58,050 --> 00:07:02,370 Then also it uses the environment is ready I mentioned but as well as transverse mass 71 00:07:02,550 --> 00:07:08,550 and and other discriminating variables. So, S R is this electrical Kino signal 72 00:07:08,550 --> 00:07:13,470 region it has format region and it does bending in the variables that I mentioned 73 00:07:14,460 --> 00:07:18,600 on the on the plot you can see that the red line signifies where the signal region 74 00:07:18,600 --> 00:07:30,390 is above the red line is where where the signal regions are. So, so, the analysis 75 00:07:30,390 --> 00:07:36,450 set set limits on on different models, so, for example charging or neutrino 76 00:07:36,450 --> 00:07:43,140 production So, in terms of the winner Urbino, you can see the top is or the 77 00:07:43,140 --> 00:07:51,840 Atlas the bottom line the CMS results so, excluding up to around and traditional 78 00:07:51,840 --> 00:07:59,970 masses around 250 gV similar for the Higgs see no assumption exploring around to 79 00:08:00,000 --> 00:08:06,420 Hundred GB and comment for the CMS search there's also an interpretation in the hex 80 00:08:06,420 --> 00:08:09,000 you know pm SSM, which you see on the bottom left. 81 00:08:11,040 --> 00:08:12,810 One of the variables that's 82 00:08:14,219 --> 00:08:19,349 that's used very, very commonly is the transverse mass constructed from lead, 83 00:08:19,379 --> 00:08:24,599 leptin, PT and Matt. And this provides a kinematic edge around the mass of the W 84 00:08:24,599 --> 00:08:28,739 boson which is used very frequently in many electronic searches. And an 85 00:08:28,739 --> 00:08:35,399 interesting variable used in the in the Atlas search is transverse mass, which is 86 00:08:35,429 --> 00:08:42,329 essentially transverse mass adapted to the leptons were 111 set hypothesis mass of 87 00:08:42,329 --> 00:08:47,159 the LSP which which sets a kinematic edge. So at the bottom you see a similar plot 88 00:08:47,159 --> 00:08:53,579 with the signal region targeting at slept on the slept on model and you can see 89 00:08:53,579 --> 00:09:00,959 again the division between the Sydney region and here it's been in terms of Also 90 00:09:00,959 --> 00:09:10,889 the r is r which is the recursive tricks of reconstruction. So here are the results 91 00:09:10,889 --> 00:09:16,979 for the slept and production. So here slept and excluded roughly around 250 gb 92 00:09:18,179 --> 00:09:24,299 for the Atlas search and now in terms of multi leptons This is a very new result 93 00:09:24,299 --> 00:09:30,089 which which was also mentioned in Carlos his talk. Here I would like to present you 94 00:09:30,089 --> 00:09:35,789 the optional region, signal region and in the search. So there's this obstacle WC 95 00:09:35,789 --> 00:09:44,159 selection, targeting compress scenarios. So here, the primary discriminants are the 96 00:09:44,459 --> 00:09:51,239 M L L men so it looks for the minimum environments between the three leptons and 97 00:09:51,239 --> 00:09:57,029 there's also kinematic edge present in these in these regions which provide a 98 00:09:57,029 --> 00:10:02,219 discriminating variable. So on the The bottom right you see the limit set by this 99 00:10:03,389 --> 00:10:10,499 the search on the on the Neutrogena neutrino masses. So it goes up to or above 100 00:10:10,529 --> 00:10:18,089 300 gV and in the very compressed region to around 200. So it's complimentary with 101 00:10:18,089 --> 00:10:23,699 the softer lepton results. And also what's interesting here that additionally the 102 00:10:23,729 --> 00:10:30,029 line the blue line represent constraints calculated and The Beano window 103 00:10:30,029 --> 00:10:38,069 calculation Dark Matter scenario where where the relic density is less than or 104 00:10:38,069 --> 00:10:43,829 equal to the observed value. And now moving on to slightly different types of 105 00:10:43,859 --> 00:10:50,759 compressed searches, so compressed vbf. So in the dialects and search one of the 106 00:10:50,759 --> 00:10:56,909 signal region actually is also targeting the BBF production. So here it uses a very 107 00:10:56,909 --> 00:11:04,919 similar rate. of drugs or reconstruction variable but instead of using Asr, it uses 108 00:11:04,919 --> 00:11:07,319 the vbf treads 109 00:11:08,909 --> 00:11:10,439 as the discriminant. 110 00:11:11,700 --> 00:11:18,270 Also, it's it's been in terms of the vbf or vbf. And and the environment mass and 111 00:11:18,270 --> 00:11:25,530 again, you see the split for the between the signal region and come parallel to 112 00:11:25,530 --> 00:11:34,530 this one, but a bit different is the CMS vbf search. So it's a search in the in the 113 00:11:34,650 --> 00:11:40,530 One Laptop and zero laptop region. So, this is even though the models considered 114 00:11:40,530 --> 00:11:46,260 to have several leptons, it's difficult to reconstruction and identify leptons, so 115 00:11:46,260 --> 00:11:55,470 they either veto or require one soft lepton. And so here are the results for 116 00:11:55,470 --> 00:12:03,060 the compress vbf search on the top is vbf the off shoulder B and C will be no 117 00:12:04,140 --> 00:12:12,060 models. So here you have the comparison of the limits. On the bottom you have the 118 00:12:12,750 --> 00:12:17,730 results of the CMS search and the lights slept on the model which which is also 119 00:12:17,730 --> 00:12:23,190 considered by the search. And an interesting fact is that the models go 120 00:12:23,190 --> 00:12:31,680 down to delta of one GB which is just very small. And other searches of self Tao. So 121 00:12:31,680 --> 00:12:38,220 this was already touched upon also and goddesses search so it's first search of a 122 00:12:38,220 --> 00:12:44,520 self to dramatically the cantel. So here the delta m, astound you tree knows less 123 00:12:44,520 --> 00:12:51,930 than or equal to 50 gV. Here also relies on ASR to target this kind of model. The 124 00:12:51,930 --> 00:12:58,410 beauty of the hydronic towel is between 20 and 40, gv and the signal region bending 125 00:12:58,440 --> 00:13:03,090 which you can see on the bottom right plot is done in terms of the empty between the 126 00:13:03,090 --> 00:13:11,850 Met and the anatel. And here the limits are set in terms of charging or neutralino 127 00:13:11,850 --> 00:13:16,920 and and stop production. And here it's here it's assumed for delta and between 128 00:13:16,920 --> 00:13:25,950 the Trojan on neutralino 50 gb and exclusion is around around three below 300 129 00:13:25,950 --> 00:13:33,330 Pv so two universes below 300 gb and now moving to compress stop searches so as you 130 00:13:33,330 --> 00:13:41,760 can see the list is quite long. And here is the face base of the different decay 131 00:13:41,760 --> 00:13:50,640 modes and they're classified in terms of W decay mode and classical searches which 132 00:13:50,640 --> 00:13:57,630 you have already heard about and Mark stock and I'll focus on the compressed 133 00:13:57,630 --> 00:14:03,000 face space. So here you have For Bodhi the case to genome mediated the case and also 134 00:14:04,289 --> 00:14:05,789 time the case which are 135 00:14:08,909 --> 00:14:09,719 of CNC. 136 00:14:12,330 --> 00:14:18,060 So, one thing for the soft searches is that these use of P tagging techniques, 137 00:14:18,060 --> 00:14:22,890 which were also mentioned already. So, there are different algorithms use at CMS 138 00:14:22,890 --> 00:14:31,320 and Atlas. So, at CMS, there's an inclusive vertex Finder. Whereas in Atlas 139 00:14:31,320 --> 00:14:36,750 there's this track base loop with the vertex tiger. But essentially, they do 140 00:14:36,750 --> 00:14:44,310 very similar things. So they they reconstruct jets from tracks and they 141 00:14:44,310 --> 00:14:51,210 indentify also secondary vertices without the presence of a threat. So these were 142 00:14:51,210 --> 00:14:57,930 these searches were covered in marks 30 generation talk, but who the interesting 143 00:14:57,930 --> 00:15:03,270 thing is that here in the very compressed scenario They require Asr, and they use 144 00:15:03,270 --> 00:15:09,450 the SOF p tag and text techniques for very small times. So this is in the sentencing 145 00:15:09,450 --> 00:15:13,620 electronic channel, and there's all hydronic channel, which is very similar, 146 00:15:13,650 --> 00:15:18,330 they also use of p tag but in Atlas search, they also make use of the 147 00:15:19,170 --> 00:15:24,570 recursive tricks are reconstruction. So there is a lot of other searches which I 148 00:15:24,780 --> 00:15:28,710 don't have the time to cover in this talk. There's a for body decay, which was done 149 00:15:28,710 --> 00:15:33,840 in current count and VA. And there's time decay and there's also other results from 150 00:15:33,840 --> 00:15:39,870 the softer leptons and soft and all hydronic channels and Trojan are mediated 151 00:15:39,870 --> 00:15:48,180 okay. So just just quickly about potential improvements or things that already used 152 00:15:48,210 --> 00:15:55,200 but but we should carry on using so we know that the only increased integrated 153 00:15:55,200 --> 00:15:59,970 luminosity is not expected to bring large gains and sensitivity. So on the top right 154 00:16:00,000 --> 00:16:05,370 Here you have, you have a projection of the soft electron with 3000 inverse 155 00:16:05,400 --> 00:16:11,400 Pentagon. So you can see, if you compare it to the existing limits, the gain is 156 00:16:12,750 --> 00:16:17,280 significant, but, I mean, I leave it for everyone to judge themselves. 157 00:16:18,299 --> 00:16:22,529 I really have to stop you because we don't have so much time we only have one. Okay, 158 00:16:22,769 --> 00:16:27,509 then I'll just go to my go to my conclusion slide, which is just for 159 00:16:27,509 --> 00:16:32,069 reference, if that's fine, but just to mention, there are different techniques 160 00:16:32,069 --> 00:16:37,169 use and we could also use the dedicated cross triggers, which were developed, as 161 00:16:37,169 --> 00:16:44,519 we see in bottom plot. And yeah, so So, bottom line, we need to take advantage of 162 00:16:44,549 --> 00:16:48,809 innovative methods to really push to the limits of detection, analysis and theory. 163 00:16:49,439 --> 00:16:50,249 Thank you very much. 164 00:16:52,649 --> 00:16:53,849 Sorry for going over. 165 00:16:54,090 --> 00:16:57,840 That's okay. We have time for one quick question. 166 00:16:59,460 --> 00:17:01,380 So Any questions anyone? 167 00:17:03,720 --> 00:17:11,070 So this is Jen, can I ask? Those are the soft laptop of yes searches for stops for 168 00:17:11,070 --> 00:17:16,110 instance, does the manager search play any role in this plan? I remember the use of a 169 00:17:16,110 --> 00:17:21,300 rose some coverage in an O data about why we don't have it anymore in this new 170 00:17:21,300 --> 00:17:22,320 coverage summary. 171 00:17:24,210 --> 00:17:31,950 I think I mean, the techniques are very similar. But I mean, requiring this this 172 00:17:32,010 --> 00:17:38,790 this hibbity jet, but I cannot say I'm not sure I cannot speak for the analysis team 173 00:17:38,790 --> 00:17:44,700 exactly why, or, or how it translates onto the onto these regions. 174 00:17:46,380 --> 00:17:52,710 I it's for Derek again. You will just have to wait a little bit but it's in the plans 175 00:17:52,710 --> 00:17:58,260 during Turpan demo jet, or well to interpret the updated fuller and to 176 00:17:58,260 --> 00:18:00,000 monitor theme to this kind of 177 00:18:02,250 --> 00:18:03,330 I see Thank you. 178 00:18:08,370 --> 00:18:11,040 Okay, thank you. Do we have any more questions? 179 00:18:12,300 --> 00:18:13,050 All right, so then