WEBVTT

1
00:00:00.350 --> 00:00:08.279
STFC-RAL-CR03-RAL-R61-2.01: Yeah, right? Well, the introduction is still introduction. I had to go back to the first page, I don't know.

2
00:00:08.400 --> 00:00:19.239
STFC-RAL-CR03-RAL-R61-2.01: Okay, sorry for the very big delay, everyone. Let me introduce… What a day.

3
00:00:21.040 --> 00:00:23.370
STFC-RAL-CR03-RAL-R61-2.01: Can you go to the first slide, please.

4
00:00:24.020 --> 00:00:27.150
STFC-RAL-CR03-RAL-R61-2.01: Very similar slide, yeah. I think,

5
00:00:28.300 --> 00:00:35.089
STFC-RAL-CR03-RAL-R61-2.01: The first page, the internet. Before that, yes, this one, yeah. Okay.

6
00:00:35.460 --> 00:00:40.259
STFC-RAL-CR03-RAL-R61-2.01: So welcome to the seminar today. This is Nassim.

7
00:00:40.400 --> 00:00:46.450
STFC-RAL-CR03-RAL-R61-2.01: She's a research scientist at SNOLDA, and…

8
00:00:46.980 --> 00:01:00.819
STFC-RAL-CR03-RAL-R61-2.01: in Ontario, Canada, where she works on low background techniques for neutrino and dark matter experiments. She's a collaborator on the SNOW+, XLZB

9
00:01:01.250 --> 00:01:13.270
STFC-RAL-CR03-RAL-R61-2.01: and deep 360 experiments, and her main research is on developing ultra-low background radon detection and assay systems for these experiments.

10
00:01:13.670 --> 00:01:29.980
STFC-RAL-CR03-RAL-R61-2.01: Before joining SNOLA, she worked as a research associate at Triumph and Royal Holloway, University of London, and a postdoctoral fellow at Queen's University. She completed her PhD in Manchester University.

11
00:01:30.280 --> 00:01:38.349
STFC-RAL-CR03-RAL-R61-2.01: Which year, 2000. Okay. By the way. Yes. Okay, so, welcome.

12
00:01:40.920 --> 00:01:59.620
STFC-RAL-CR03-RAL-R61-2.01: And please, please calm down, you don't have to rush. No, I know, I tried to. Sorry, guys, for the technical issue, but I guess we can start. So, yeah, I'm going to talk about radon contour and measurement, at Snow Lab for quantum next-generation Radio Research Experiments. This might be a little bit

13
00:02:00.050 --> 00:02:01.819
STFC-RAL-CR03-RAL-R61-2.01: Different from what you…

14
00:02:02.080 --> 00:02:14.270
STFC-RAL-CR03-RAL-R61-2.01: work on a daily basis. So, introduction, I'm going to talk a little bit about nomadic method, and why searching for them is important.

15
00:02:14.270 --> 00:02:23.710
STFC-RAL-CR03-RAL-R61-2.01: And then talk about sources of background for this type of sessions, and then I'm focusing on redone that why it's really already is important.

16
00:02:23.850 --> 00:02:39.929
STFC-RAL-CR03-RAL-R61-2.01: Then, going to, turn a little bit technical, talking about the techniques which are applied in order to measure, radon ex-situ at a snow lab. So, components of experiments, you want them to be low radioactivity, so before you put

17
00:02:39.930 --> 00:02:45.580
STFC-RAL-CR03-RAL-R61-2.01: Building your experiment, you actually need to know, very similar level, what your background level is.

18
00:02:45.920 --> 00:03:04.580
STFC-RAL-CR03-RAL-R61-2.01: Then, a little bit talking about the radon remover techniques. Again, you want your experiment to be radon-free, so you need to basically develop techniques. For example, if you have liquid scintillator or, liquid arc or liquid xenone, you need to develop techniques to remove the radon from, from those.

19
00:03:04.580 --> 00:03:18.190
STFC-RAL-CR03-RAL-R61-2.01: Basically fluids, and then, talk about techniques to create lower radon environment for, like, assembling of, for example, the coupons, etc, and then summarize.

20
00:03:19.010 --> 00:03:21.490
STFC-RAL-CR03-RAL-R61-2.01: So,

21
00:03:22.000 --> 00:03:38.029
STFC-RAL-CR03-RAL-R61-2.01: So, basically, we know that during the Big Bang, there was a core amount of matter and antimicrobrod. So, the question is that why the world today, the universe today, looks like this, which basically is dominated by matter.

22
00:03:38.590 --> 00:03:48.460
STFC-RAL-CR03-RAL-R61-2.01: So, forecast of galaxies, stars, planets, light, rather than looking like this, where, like, you have an empty universe.

23
00:03:48.680 --> 00:03:55.689
STFC-RAL-CR03-RAL-R61-2.01: Where antimatter and matter emulated each other, they just created some energy, and by now, that energy is cooled down.

24
00:03:56.010 --> 00:04:07.190
STFC-RAL-CR03-RAL-R61-2.01: So, one thing is that can nutritional beta decay be the answer to this? So, nateobetr decay is a physics beyond a standard model.

25
00:04:07.400 --> 00:04:11.790
STFC-RAL-CR03-RAL-R61-2.01: is their own antiparticle.

26
00:04:11.900 --> 00:04:21.290
STFC-RAL-CR03-RAL-R61-2.01: And in that case, basically, you have one of the antineutrinos is observed as a neutrino, and the final stage of the normal,

27
00:04:21.310 --> 00:04:34.439
STFC-RAL-CR03-RAL-R61-2.01: A beta decay, and then in the final state, you have no antinodrinals, and you have only electrons. So, in this mechanism, it's a left… this will be a left-hand number violating process.

28
00:04:34.440 --> 00:04:47.669
STFC-RAL-CR03-RAL-R61-2.01: So it is a process which, basically annihilates onto particles, so that can actually be, basically one reason,

29
00:04:47.790 --> 00:04:57.970
STFC-RAL-CR03-RAL-R61-2.01: So, that, or path… it can be a path to understand why there is matter-on-to-matter, symmetry, in the, in the universe.

30
00:04:58.090 --> 00:05:05.180
STFC-RAL-CR03-RAL-R61-2.01: So experimentally, the way that we see this, we're looking at the energy sum of these two electrons, and in a normal

31
00:05:05.340 --> 00:05:22.839
STFC-RAL-CR03-RAL-R61-2.01: two-way decay, you basically have a continuum spectrum in a… if you have a story, you will see a, basically a mono energy peak, which is equal to some of these two electrons, which are estimated by the energy resolution of your detector.

32
00:05:22.930 --> 00:05:31.140
STFC-RAL-CR03-RAL-R61-2.01: This is an extremely rare process. It's, current experiments have a limit of 10 to 27 years half-life.

33
00:05:31.270 --> 00:05:47.429
STFC-RAL-CR03-RAL-R61-2.01: So, in comparison, as we all know, the universe is about 10 to 10 years, so you can see how rare this process is. So that's why you need very large-scale experiments, multi-tone fire, with very, very, very low background.

34
00:05:47.550 --> 00:05:55.429
STFC-RAL-CR03-RAL-R61-2.01: So, control in the background is, basically the name of the game for, for this, this extension.

35
00:05:55.860 --> 00:06:06.169
STFC-RAL-CR03-RAL-R61-2.01: So the other question, which we need to answer is, what is the nature of dark matter? There is a history of dark matter. I'm sure,

36
00:06:06.310 --> 00:06:25.589
STFC-RAL-CR03-RAL-R61-2.01: you know all about it. There are lots of evidences, but the most convincing evidence of dark matter is that when you look at the tiny variation of temperature of the universe 400,000 years after the Big Bang, and you basically map that.

37
00:06:25.590 --> 00:06:32.820
STFC-RAL-CR03-RAL-R61-2.01: You can, exactly, precisely calculate the components of the universe.

38
00:06:32.840 --> 00:06:39.540
STFC-RAL-CR03-RAL-R61-2.01: And what you see is that you have, about 26.8%

39
00:06:39.650 --> 00:06:49.470
STFC-RAL-CR03-RAL-R61-2.01: We don't matter. Only 4.9%, is there holding… Oops, sorry. Okay.

40
00:06:50.980 --> 00:06:58.409
STFC-RAL-CR03-RAL-R61-2.01: So, and the rest of it is dark energy, which will be understanding my less. So,

41
00:06:58.620 --> 00:07:13.280
STFC-RAL-CR03-RAL-R61-2.01: Right now, there are lots of parameters in space to look at for dark matter, and the TV scale dark matter, particles are basically similar, I'll be honest, not the model.

42
00:07:13.290 --> 00:07:26.089
STFC-RAL-CR03-RAL-R61-2.01: theory, and the Snow Lab, which I'm going to talk in a second, actually has so many experiments which are basically looking at different range of, these, these parameter aspects.

43
00:07:26.550 --> 00:07:29.900
STFC-RAL-CR03-RAL-R61-2.01: so…

44
00:07:30.120 --> 00:07:49.139
STFC-RAL-CR03-RAL-R61-2.01: So what… so background… controlling background is important. I have an example for a… for example, a dark matter experiment. So, basically, so what you expect is that the longer you run this experiment, so the longer exposure, you would expect that your sensitivity is improved, right?

45
00:07:51.740 --> 00:08:02.679
STFC-RAL-CR03-RAL-R61-2.01: But, the detective order of magnitude of, let's say, higher background, it reaches maximum sensitivity, like, much more sooner.

46
00:08:03.050 --> 00:08:09.620
STFC-RAL-CR03-RAL-R61-2.01: And there, doesn't really matter how long… how long more you run your experiment, you don't improve your sensitivity anymore.

47
00:08:10.080 --> 00:08:15.779
STFC-RAL-CR03-RAL-R61-2.01: So, right now, in the field, we reached to that level of flow background that

48
00:08:15.890 --> 00:08:23.120
STFC-RAL-CR03-RAL-R61-2.01: Next generation of experiments are talking about one event, one dark matter event, in 10 years of running the experiment.

49
00:08:23.350 --> 00:08:33.090
STFC-RAL-CR03-RAL-R61-2.01: So that's how rare, and that's why we call the rare events, that's such a rare thing. And then, when you're talking about one event in 10 years, then that means that you need to be back in a free environment.

50
00:08:33.260 --> 00:08:36.290
STFC-RAL-CR03-RAL-R61-2.01: Yeah, so that's, that's a challenge.

51
00:08:36.600 --> 00:08:37.450
STFC-RAL-CR03-RAL-R61-2.01: So…

52
00:08:37.789 --> 00:08:50.700
STFC-RAL-CR03-RAL-R61-2.01: So now, where we're looking for this, we are… we are going deep underground, and the reason we're going deep underground for this, because immune blocks of underground labs are much less, so you're not worried about immune-induced background.

53
00:08:50.810 --> 00:08:55.050
STFC-RAL-CR03-RAL-R61-2.01: as much. So… so it's not a lab, this is a map

54
00:08:55.050 --> 00:09:10.789
STFC-RAL-CR03-RAL-R61-2.01: basically, in Canada. It's basically, situated 2 kilometers underground, an active mine, basically called, called Rayton Mine, near South Bay, Ontario.

55
00:09:10.790 --> 00:09:18.010
STFC-RAL-CR03-RAL-R61-2.01: So this is about 4, 4 average rides from Toronto for the people who don't know where Salbury is, so up north.

56
00:09:18.120 --> 00:09:33.120
STFC-RAL-CR03-RAL-R61-2.01: So, Estola, is, quite the second deepest undergrad, lab in the world. The first one is now a Chinese, Chinese lab,

57
00:09:33.160 --> 00:09:41.090
STFC-RAL-CR03-RAL-R61-2.01: Where, basically it's a ton… it's a… it's a lab that you drive… you basically drive your car to.

58
00:09:41.090 --> 00:09:58.939
STFC-RAL-CR03-RAL-R61-2.01: Whereas the snow lab is, actually… actually, you're going on the ground for kilometers, not on the tunnel or something. You actually have to get the cage and go down. So you see a picture of the surface building here, which also has some PIN labs in it, which some of these forecasts show is done, actually, making a surface lab.

59
00:09:59.730 --> 00:10:04.970
STFC-RAL-CR03-RAL-R61-2.01: So this is the map of the snow lab.

60
00:10:04.970 --> 00:10:20.899
STFC-RAL-CR03-RAL-R61-2.01: As you can see, it's quite big, big, big lab, and has lots of very large-scale experiments and plans for larger experiments, too. So you see the snow, the famous snow experiment, you see now a snow plots here.

61
00:10:20.960 --> 00:10:40.210
STFC-RAL-CR03-RAL-R61-2.01: And, we have a few dark matter experiments of SuperCPMS, PICO and others here. You basically have a, empty space right now in Coraupe, which we are hoping that we have a next-generation dark matter

62
00:10:40.210 --> 00:10:44.509
STFC-RAL-CR03-RAL-R61-2.01: Or making myself with a billboard, experimenter.

63
00:10:44.700 --> 00:10:47.179
STFC-RAL-CR03-RAL-R61-2.01: Okay. So,

64
00:10:47.590 --> 00:11:03.349
STFC-RAL-CR03-RAL-R61-2.01: I'm the collaborator of SNO Plus experiment, currently, and also XMCD, USCD Canadian groups are showing XLZD in last February, coming this February, so we are quite fresh.

65
00:11:04.550 --> 00:11:19.530
STFC-RAL-CR03-RAL-R61-2.01: And, so it's not plus is, 12 meter diameter and kilometers, so it's quite big. And currently, basically, it's a current generation known as our beta decay, a liquid scintillator.

66
00:11:19.530 --> 00:11:28.269
STFC-RAL-CR03-RAL-R61-2.01: They consider the experiment, and then XLZD is basically a future, don't matter, and I'm gonna start with the big experiment.

67
00:11:28.360 --> 00:11:30.200
STFC-RAL-CR03-RAL-R61-2.01: Okay.

68
00:11:30.870 --> 00:11:42.199
STFC-RAL-CR03-RAL-R61-2.01: So, now talking about background sources. So, what are backgrounds defined for us, for law energy… I call it law energy physicists? So,

69
00:11:42.450 --> 00:11:55.450
STFC-RAL-CR03-RAL-R61-2.01: So you, have gamas and vectors from national radioactivity, and also from national radioactivity, depending on, of course, what physics you're looking for, that would be the decay, or numerous, or dark matter,

70
00:11:55.450 --> 00:12:07.370
STFC-RAL-CR03-RAL-R61-2.01: What they create is different, and, you are basically sensitive, to, different energies, so different energies give, so you have backgrounds of the different energies.

71
00:12:07.370 --> 00:12:16.280
STFC-RAL-CR03-RAL-R61-2.01: So you can, for example, put dark matter, alpha in, so alpha interaction of alphas, which is a material which can create neutrons.

72
00:12:16.280 --> 00:12:22.299
STFC-RAL-CR03-RAL-R61-2.01: Can, give you, basically, signature of dark matter.

73
00:12:22.450 --> 00:12:36.150
STFC-RAL-CR03-RAL-R61-2.01: Surface outputs, again, for Dharmender experiments or problems, so what surface alpha can mean that Dharmender is rather than deposited in the detector, is deposited in a detector wall.

74
00:12:36.150 --> 00:12:46.849
STFC-RAL-CR03-RAL-R61-2.01: But it's very close to the surface of your, detection medium, and it's such a way that you don't see the energy of this oil power. What you see is the nuclei, the liquid nuclei.

75
00:12:46.910 --> 00:12:51.320
STFC-RAL-CR03-RAL-R61-2.01: And that basically, again, can mimic the dark matter.

76
00:12:51.460 --> 00:13:09.209
STFC-RAL-CR03-RAL-R61-2.01: Muels, mules reduce neutrons, and cosmogenic activation. Both of them can… they can be a problem for both elevated and dark matter experiments. Of course, we are underground and snow lab, so these are less problem… less problem for us.

77
00:13:09.390 --> 00:13:15.139
STFC-RAL-CR03-RAL-R61-2.01: So now, moving to redo… sorry, before going to redo. So, natural rate activity.

78
00:13:15.280 --> 00:13:22.429
STFC-RAL-CR03-RAL-R61-2.01: So we have 3, dictation… 3 important decades that

79
00:13:22.500 --> 00:13:39.339
STFC-RAL-CR03-RAL-R61-2.01: We are basically… need to make sure that they don't create natural, background in our detector. I'm focusing in, one of the more popular ones, which is uranium-238, and the reason… I prefer uranium-238 is because it's…

80
00:13:39.410 --> 00:13:50.899
STFC-RAL-CR03-RAL-R61-2.01: has, basically long-leave isotopes, which can be problematic. So, so you then break down this,

81
00:13:51.150 --> 00:13:53.670
STFC-RAL-CR03-RAL-R61-2.01: Chained to three parts.

82
00:13:54.210 --> 00:14:07.799
STFC-RAL-CR03-RAL-R61-2.01: And, all… these three parts can basically, depending on what you're looking for, can cause problems, in your experiments. But we divide them by, in three…

83
00:14:07.800 --> 00:14:14.990
STFC-RAL-CR03-RAL-R61-2.01: places, because it's, depend, based on the halftime. So, top of the uranium chain.

84
00:14:15.070 --> 00:14:22.699
STFC-RAL-CR03-RAL-R61-2.01: Basically, they are, we call them non-lean isotop, uranium chain.

85
00:14:22.780 --> 00:14:42.699
STFC-RAL-CR03-RAL-R61-2.01: the middle, which is Raven226, and radon-22, and protein E. We call them short-lived, basically, these are the short-lived part of the chain, while short-lived, so by long, I mean, more than thousands of years, while short, I mean in a matter of days and hours.

86
00:14:42.890 --> 00:14:56.239
STFC-RAL-CR03-RAL-R61-2.01: And then, after that, you'll have, basically this, this late to 10, which is, 22 years after, so again, from days and hours, they go 2 years.

87
00:14:56.480 --> 00:15:00.520
STFC-RAL-CR03-RAL-R61-2.01: And then… so the… this is maybe the third part.

88
00:15:00.610 --> 00:15:10.670
STFC-RAL-CR03-RAL-R61-2.01: So, each time that you have these, massive changes in half-life, there is a chance that you'll have a dystopram in the decay.

89
00:15:10.700 --> 00:15:21.569
STFC-RAL-CR03-RAL-R61-2.01: And that makes that you may basically know what your uranium content is, but that doesn't really, tell you that… what the background noise is, right?

90
00:15:21.690 --> 00:15:31.950
STFC-RAL-CR03-RAL-R61-2.01: So, so basically components processing can cause radioactive desequilibrium, and we therefore must study each subchain separately.

91
00:15:32.080 --> 00:15:35.780
STFC-RAL-CR03-RAL-R61-2.01: So…

92
00:15:36.010 --> 00:15:54.699
STFC-RAL-CR03-RAL-R61-2.01: So, for longer isotopes, one common technique is basically using, ICPMS. These are commercially available instruments. At the Snow Lab, we basically have one right now, which you see in the picture here.

93
00:15:54.970 --> 00:16:03.539
STFC-RAL-CR03-RAL-R61-2.01: And the sensitivity of these… these are quite sensitive devices, 0.1 macro backwards per kilogram.

94
00:16:03.540 --> 00:16:16.940
STFC-RAL-CR03-RAL-R61-2.01: But, but, yeah, this advantage… I mean, to our booth, but as I said, these advantages that you… it doesn't really, it can constrain your background, but it doesn't really give you information on what is lower in the chain.

95
00:16:17.520 --> 00:16:30.160
STFC-RAL-CR03-RAL-R61-2.01: For radon-26 and radon, radon polygeny, you can use high-perity germanium detectors. They have sensitivity of 10 to 100 microbaccura per sample, and you count it.

96
00:16:30.350 --> 00:16:40.349
STFC-RAL-CR03-RAL-R61-2.01: So you see, at the Snow Lab, we have, I think 6 of them, I believe, but I just had a picture of one of the more sensitive ones.

97
00:16:40.370 --> 00:16:50.860
STFC-RAL-CR03-RAL-R61-2.01: And, and also you have raised elimination systems, which have sensitivity of, depending on the detector, can be, 2200 macro.

98
00:16:51.090 --> 00:16:56.610
STFC-RAL-CR03-RAL-R61-2.01: I'm going to do, of course, this is a highlight of my talk, so I'm going to talk about that in a little bit.

99
00:16:56.650 --> 00:17:16.130
STFC-RAL-CR03-RAL-R61-2.01: And then, for the bottom of the chain, you basically need to, as you can see, there are lots of outputs here, so you can use, alpha spectroscopy to measure, to, to measure the, rates. Again, they are commercially, specialized, but commercially available.

100
00:17:16.170 --> 00:17:20.890
STFC-RAL-CR03-RAL-R61-2.01: equivalence, XOA, which is a reef chamber.

101
00:17:21.050 --> 00:17:25.490
STFC-RAL-CR03-RAL-R61-2.01: Can be used to, basically use tactics.

102
00:17:25.660 --> 00:17:29.720
STFC-RAL-CR03-RAL-R61-2.01: gran.

103
00:17:31.110 --> 00:17:32.910
STFC-RAL-CR03-RAL-R61-2.01: Okay, so…

104
00:17:33.560 --> 00:17:42.609
STFC-RAL-CR03-RAL-R61-2.01: So now, radon emanation measurement. So, anything that, you put in your detector can emanate radon.

105
00:17:42.880 --> 00:17:54.140
STFC-RAL-CR03-RAL-R61-2.01: As I just talked about with uranium, what makes it unique compared to all other backgrounds is that it's a noble gas, so it can come.

106
00:17:54.340 --> 00:17:59.250
STFC-RAL-CR03-RAL-R61-2.01: So that makes it complicated, because then, if you see some background, then…

107
00:17:59.600 --> 00:18:05.189
STFC-RAL-CR03-RAL-R61-2.01: and somebody, some random purchasing background, then you don't really,

108
00:18:05.340 --> 00:18:24.849
STFC-RAL-CR03-RAL-R61-2.01: it doesn't assume that you can find where the source of background is, because it has trouble. So it emanates from material surface, so you basically can have, radon, basically, from record from the radion,

109
00:18:25.160 --> 00:18:32.810
STFC-RAL-CR03-RAL-R61-2.01: Or it can be, like, be more in-depth of a radium decay happens.

110
00:18:32.810 --> 00:18:50.339
STFC-RAL-CR03-RAL-R61-2.01: So, radon diffuses out from… for example, if you have very porous materials, then you can have, radon basically diffuses out, and then, what that does that mean, necessarily, what you see on the surface about radon is not necessarily what is actually in the pot.

111
00:18:50.810 --> 00:18:52.519
STFC-RAL-CR03-RAL-R61-2.01: And, yeah, so…

112
00:18:52.840 --> 00:19:02.550
STFC-RAL-CR03-RAL-R61-2.01: Also, at SOLA, the radon level is high. Underground, it's 120 background, like you with me here, just to compare.

113
00:19:03.150 --> 00:19:11.949
STFC-RAL-CR03-RAL-R61-2.01: Like, on surface, at Sudbury, it's, the level of radion is, 10 macro per…

114
00:19:12.210 --> 00:19:16.029
STFC-RAL-CR03-RAL-R61-2.01: Cubic meters, so this is a factor of 40 higher than surface.

115
00:19:16.360 --> 00:19:36.329
STFC-RAL-CR03-RAL-R61-2.01: it's not harmful for, it's not harmful for POMX, but it is definitely a problem for, our, our, experiment. So, AIC experiment needs to think about, a strategy to basically not having this problem, at least, amount of rhythm getting into the detector.

116
00:19:37.390 --> 00:19:38.430
STFC-RAL-CR03-RAL-R61-2.01: Okay.

117
00:19:38.940 --> 00:19:46.970
STFC-RAL-CR03-RAL-R61-2.01: So, and also, of course, we need to use low-oretical amenity material in our experiments, too.

118
00:19:48.490 --> 00:19:57.199
STFC-RAL-CR03-RAL-R61-2.01: So, how to remove radon? So, stick material selection for performing radon emanation measurements,

119
00:19:57.680 --> 00:20:17.329
STFC-RAL-CR03-RAL-R61-2.01: and regular amount of radon levels from different components of the detector, you may say, okay, you build a detector, the detector does that for you, can tell you what background you have. That's true, but sometimes some components of the experiment, such as external, some external, like, volume or something like that.

120
00:20:17.550 --> 00:20:29.440
STFC-RAL-CR03-RAL-R61-2.01: you don't have, a sensor there to actually measure, rhythm. So you need to assay that component, that, area, or different, metals.

121
00:20:29.650 --> 00:20:45.670
STFC-RAL-CR03-RAL-R61-2.01: You need to remove, radon from… if you have a, in the contents of talking about external plus and XLZZ, you need to basically remove the radon from the medium, the, from the medium which goes to your detector,

122
00:20:45.860 --> 00:20:53.370
STFC-RAL-CR03-RAL-R61-2.01: And you also need to control, radon ingress, especially at the SOLA, which has higher radon level.

123
00:20:53.590 --> 00:21:00.480
STFC-RAL-CR03-RAL-R61-2.01: So I'm going to… my talk is going to, basically cover some examples of each of these.

124
00:21:00.590 --> 00:21:10.650
STFC-RAL-CR03-RAL-R61-2.01: But also, you need to prevent surface contamination without, say, and cleaning and removal of surfaces,

125
00:21:10.690 --> 00:21:28.519
STFC-RAL-CR03-RAL-R61-2.01: especially for late to 10, which is a longer-lived half-life, you… if you expose, if you expose your experiment with some level of radon, and you know you did that, then you need to plan for how to remove the project. And, I don't have time to talk about it.

126
00:21:28.520 --> 00:21:36.010
STFC-RAL-CR03-RAL-R61-2.01: I can have… give example, about it, if people want to talk about it in the future.

127
00:21:36.020 --> 00:21:43.269
STFC-RAL-CR03-RAL-R61-2.01: So, Rakuten Access System right now, as it's now thinking about part of it, more thinking about it now, Rakuten Access System Access Power. So…

128
00:21:43.590 --> 00:22:01.790
STFC-RAL-CR03-RAL-R61-2.01: So, radar refers to the measurement of emanation rate, from a material or surface, and radon concentration in gas or water samples. You'll see a picture of, basically, four of the equipments that we have, which basically we use to measure radon rates.

129
00:22:02.050 --> 00:22:04.140
STFC-RAL-CR03-RAL-R61-2.01: I'm going to cover them.

130
00:22:04.680 --> 00:22:20.749
STFC-RAL-CR03-RAL-R61-2.01: So, we, basically, one tactic to use is the… I love to call it Rylon trapping tactic. So basically the way that it works is that you put your sample

131
00:22:20.810 --> 00:22:26.759
STFC-RAL-CR03-RAL-R61-2.01: In an emanation chamber, and, for example, you leave it for, one to two weeks.

132
00:22:26.910 --> 00:22:34.149
STFC-RAL-CR03-RAL-R61-2.01: On their back here. And why you put an elony… why you put an elamination chamber, for that long is because

133
00:22:34.320 --> 00:22:41.760
STFC-RAL-CR03-RAL-R61-2.01: They don't contact rain from the air can trapped in the, in your, your, material.

134
00:22:42.030 --> 00:22:59.379
STFC-RAL-CR03-RAL-R61-2.01: and, and have a slow, release. You want to separate what is, basically coming from the air in the course than, something that is actually the internal background of that, that, material.

135
00:22:59.520 --> 00:23:09.959
STFC-RAL-CR03-RAL-R61-2.01: So, yeah, so you put it for 2 weeks there, then, you then extract the radon, and, trap it in…

136
00:23:09.960 --> 00:23:22.429
STFC-RAL-CR03-RAL-R61-2.01: series that traps before it goes to your detector. And the way that you trap it is that you slow down radon atoms by, insert it in collagenic, liquids, typically liquid absorption.

137
00:23:22.680 --> 00:23:32.349
STFC-RAL-CR03-RAL-R61-2.01: And then, you want to travel up, and you transfer, basically the regular add-ons in, in your regular network.

138
00:23:32.570 --> 00:23:51.049
STFC-RAL-CR03-RAL-R61-2.01: Snow Lab is using, currently focusing on local sauce. I know that there are other technologies, and SnowLab also has other technologies, which I'm going to cover in a second, but, but, yeah, local sauce is the most, dominant, technology that we use right now.

139
00:23:52.410 --> 00:23:54.980
STFC-RAL-CR03-RAL-R61-2.01: So…

140
00:23:55.320 --> 00:24:03.389
STFC-RAL-CR03-RAL-R61-2.01: So this is a picture of the surface emanation system, for density of… so this is the emanation chamber I was talking about.

141
00:24:03.450 --> 00:24:21.160
STFC-RAL-CR03-RAL-R61-2.01: And you can, maybe see one of the traps there, and another trap there, and you can see a local cell being attached, so this is sort of a local cell confederacy attached here. It has a sensitivity of around 50 microbiacro, and, yeah, so,

142
00:24:21.870 --> 00:24:23.970
STFC-RAL-CR03-RAL-R61-2.01: What's the next slide?

143
00:24:24.320 --> 00:24:29.420
STFC-RAL-CR03-RAL-R61-2.01: So, Locasaw is a 2-inch diameter,

144
00:24:29.510 --> 00:24:40.420
STFC-RAL-CR03-RAL-R61-2.01: hemisphere, so, like, that, that big. And it's coated with zinc sulfide, which is, silver-activated, silver-activated zinc sulfide.

145
00:24:40.500 --> 00:24:50.940
STFC-RAL-CR03-RAL-R61-2.01: So, silver activates in suicide, scintillates with alpha particles, it's an in- it's, in, it's an inorganic scintillator.

146
00:24:51.160 --> 00:24:54.299
STFC-RAL-CR03-RAL-R61-2.01: And it makes it ideal for detection.

147
00:24:54.510 --> 00:25:01.479
STFC-RAL-CR03-RAL-R61-2.01: So, at Sona, we have 16 local channels, and basically, we put the locusts on top of

148
00:25:01.570 --> 00:25:06.810
STFC-RAL-CR03-RAL-R61-2.01: two-inch PMTs, to basically do the counting.

149
00:25:06.840 --> 00:25:22.850
STFC-RAL-CR03-RAL-R61-2.01: and you see, basically, and typical alpha bars, this is, to know, to understand, so this is sample number, this is the sample number, but this is a form of a second window, so this is a,

150
00:25:23.130 --> 00:25:30.750
STFC-RAL-CR03-RAL-R61-2.01: I don't know what type of facility that they're working on, but working with, but this is, like, so I can't say it's explore.

151
00:25:31.500 --> 00:25:38.220
STFC-RAL-CR03-RAL-R61-2.01: of course, when you're doing radon detection, you need to know the efficiency,

152
00:25:38.510 --> 00:25:56.319
STFC-RAL-CR03-RAL-R61-2.01: So, there has been, two efficiency measurements of local cells, which were published, and recently, we also did fully John 4 simulation, basically, of the post, authentic cells.

153
00:25:56.320 --> 00:26:03.679
STFC-RAL-CR03-RAL-R61-2.01: And as you can see, one of the measurements is to have tension with the, with the simulation and audio measurement.

154
00:26:03.680 --> 00:26:17.909
STFC-RAL-CR03-RAL-R61-2.01: we are planning to… the measurement's done somewhere… it was basically done at 20s or something like that. We are trying to actually do that Snow Lab again, too, with a much lower… lower instance, a lower concentrated source.

155
00:26:17.910 --> 00:26:25.020
STFC-RAL-CR03-RAL-R61-2.01: But hopefully these arrow bars, go a little bit lower than what you see there. Hopefully they have a better measurement.

156
00:26:25.420 --> 00:26:42.139
STFC-RAL-CR03-RAL-R61-2.01: So, now, background. So, efficiency, I always, again, to question you, what is the background? When I set 50 macro background system, the… the domain backgrounds actually developed as a background compared to the rest of the system.

157
00:26:42.140 --> 00:26:49.750
STFC-RAL-CR03-RAL-R61-2.01: So… so the way that we do it is that we purchase the Zoom sulfide from, basically from a company.

158
00:26:50.120 --> 00:27:00.899
STFC-RAL-CR03-RAL-R61-2.01: And, the new basic… and we look… we've already done the study, and we know that the main background is coming from things like Zephyr and the Adyeca, for example, we are using.

159
00:27:00.970 --> 00:27:08.239
STFC-RAL-CR03-RAL-R61-2.01: So new requests that have background of 3 to 5 alpha counts per day, and

160
00:27:08.240 --> 00:27:21.350
STFC-RAL-CR03-RAL-R61-2.01: As I was talking about, Lecture 10, which has a 22-year half-life and is supporting Lecture 10, so that means that when you're doing, the more, more and more assets you're doing.

161
00:27:21.350 --> 00:27:34.440
STFC-RAL-CR03-RAL-R61-2.01: you're starting to build background. So that's why the age, so when you look across the stages, and also depending on what you were emanating, some of them, some of these you were emanating was quite, radioactive.

162
00:27:34.490 --> 00:27:52.980
STFC-RAL-CR03-RAL-R61-2.01: Then you can have local cells which are really high background. So right now, we have about 10 local cells around here, which are the newer local cells that we are using for price-sensitive measurements, and the rest we're not really using, apart from when we want to do channel calibration and, or, troubleshooting.

163
00:27:53.500 --> 00:28:08.429
STFC-RAL-CR03-RAL-R61-2.01: So we have to make new passes every few years. For example, this is one of the new passes that we made, last year. And we basically, tried to, develop the procedure to do it live.

164
00:28:08.920 --> 00:28:15.059
STFC-RAL-CR03-RAL-R61-2.01: Now we are doing, research and development, so, I'm sure…

165
00:28:15.350 --> 00:28:22.299
STFC-RAL-CR03-RAL-R61-2.01: One of the questions that you might have asked in your head is that, okay, you're saying all this, but what your goal is? How long you want to go.

166
00:28:22.410 --> 00:28:24.710
STFC-RAL-CR03-RAL-R61-2.01: Especially when you're talking about law background.

167
00:28:24.890 --> 00:28:36.620
STFC-RAL-CR03-RAL-R61-2.01: So, XCD goal right now is that, the radar level inside the liquid xenon target has to be less than 0.1 macromacromic kilogram.

168
00:28:36.940 --> 00:28:42.810
STFC-RAL-CR03-RAL-R61-2.01: And, I just told you that our system is 50 microbi per sample.

169
00:28:43.050 --> 00:28:52.199
STFC-RAL-CR03-RAL-R61-2.01: So, that means that we need to, reduce… for the next generation of experiments, we need to reduce background by factor of 100.

170
00:28:52.410 --> 00:29:03.249
STFC-RAL-CR03-RAL-R61-2.01: And that's what… right now, that's what my group is focusing on. So we are working on,

171
00:29:03.420 --> 00:29:19.260
STFC-RAL-CR03-RAL-R61-2.01: doing RMS for lower background 625. So you see, we had the first test, and what you, what you see is that, basically this year, and, we have the, we have mixed scintillators,

172
00:29:19.260 --> 00:29:36.349
STFC-RAL-CR03-RAL-R61-2.01: And you can see this is basically the all-up part from the single list that we made. But, the loyalty, is about a factor of two lower than what we see in the commercial one, so we are still trying to do, more, or if you understand what we are doing wrong.

173
00:29:36.620 --> 00:29:52.820
STFC-RAL-CR03-RAL-R61-2.01: In addition, we are also, having, developing, spherical proportional conscious, I don't know how many of your formula with the UC technology, or dark sphere technology, but basically, yeah, so, so this would be a…

174
00:29:52.830 --> 00:30:00.809
STFC-RAL-CR03-RAL-R61-2.01: much smaller scale, compiled with local saw and, promotion and methods.

175
00:30:01.540 --> 00:30:17.300
STFC-RAL-CR03-RAL-R61-2.01: Okay, so, the other technique, so this all happens in the category of traveling, traveling technique, but the only technique that we can use to measure radon is, what I would like it, call a recirculation thing.

176
00:30:17.790 --> 00:30:36.059
STFC-RAL-CR03-RAL-R61-2.01: And that is that rather than trapping your radon, you basically, you put your radon sample in a chamber, and then you basically recirculate it with some carrier gas, and then that radon reaches to your, basically, the detector.

177
00:30:36.060 --> 00:30:41.649
STFC-RAL-CR03-RAL-R61-2.01: Which, then can measure the radar level continuously.

178
00:30:42.140 --> 00:30:54.200
STFC-RAL-CR03-RAL-R61-2.01: So these are the electrostatic chambers, so, which are basically, have a… they have a dialogue, which are,

179
00:30:54.620 --> 00:31:03.049
STFC-RAL-CR03-RAL-R61-2.01: detector, and basically you give it a high voltage, and that's how you… you measure the ice.

180
00:31:04.830 --> 00:31:23.030
STFC-RAL-CR03-RAL-R61-2.01: So these are called, so Snow developed this, they are not, sensitive compared to our, other, system that I was talking about. So we are just bringing them back online, because they have not been used for a while.

181
00:31:23.090 --> 00:31:29.199
STFC-RAL-CR03-RAL-R61-2.01: And we are trying to see whether we can improve the system in such a way that to reduce the background.

182
00:31:30.540 --> 00:31:34.289
STFC-RAL-CR03-RAL-R61-2.01: So, how much time do I have? Please carry on. Okay.

183
00:31:34.290 --> 00:31:52.030
STFC-RAL-CR03-RAL-R61-2.01: So, we want to also, be able to measure radon concentration in non-fersion gas. So non-fusion is widely used as a cover gas to prevent radon ingress in the detector. So, this is, for example, the top of the loss detector, top of the neck.

184
00:31:52.100 --> 00:32:04.449
STFC-RAL-CR03-RAL-R61-2.01: And this is in Linacre system, basically. And, or sometimes, when you want to do an emulation of a very big component of an experiment.

185
00:32:04.570 --> 00:32:05.810
STFC-RAL-CR03-RAL-R61-2.01: Just…

186
00:32:06.000 --> 00:32:24.070
STFC-RAL-CR03-RAL-R61-2.01: Putting vacuum doesn't talk, so you need to fill that up with nitrogen again, and then, blushing, and then a pump in another to measure the radon level in that component. This is an example of what we did at the Snow Lab, which is, like, people 500, steel shelf, and wanted to see what radon amimension it has.

187
00:32:24.520 --> 00:32:39.409
STFC-RAL-CR03-RAL-R61-2.01: So the system to do that, we basically use a similar system that I just described earlier, similar technology, and you wrap it up in an engine chamber, then you have a cover-cast system, which

188
00:32:39.410 --> 00:32:48.050
STFC-RAL-CR03-RAL-R61-2.01: Feed, with node version, and you'll basically, cut the radium atom and, measured.

189
00:32:48.860 --> 00:32:59.039
STFC-RAL-CR03-RAL-R61-2.01: So, we had to go, through an upgrade for this, basically, this system that we have on the ground.

190
00:32:59.180 --> 00:33:02.719
STFC-RAL-CR03-RAL-R61-2.01: And because of the trap.

191
00:33:02.790 --> 00:33:17.640
STFC-RAL-CR03-RAL-R61-2.01: the Raven trap was made of bronze wool, and what we found out is that, bronze wool or oil are very good for regular eminations on the vacuum. They actually… what we saw is that as, we do longer asset time, longer asset time is that

192
00:33:17.660 --> 00:33:25.340
STFC-RAL-CR03-RAL-R61-2.01: As you extract more nitrogen going through the system to sample it, you see that the efficiency is dropping.

193
00:33:25.520 --> 00:33:34.319
STFC-RAL-CR03-RAL-R61-2.01: So, that was limiting our sensitivity, and before the experimental needs.

194
00:33:34.380 --> 00:33:46.499
STFC-RAL-CR03-RAL-R61-2.01: So, we basically needed to develop a new rhythm trap for this measurement, so we used an activated charcoal trap. We added an activated charcoal trap to the system. We had to do…

195
00:33:46.500 --> 00:33:57.650
STFC-RAL-CR03-RAL-R61-2.01: And for Adye to basically remove the background of this, Adye charcoal, which was, coconut-based, using the nitric acid exchange.

196
00:33:57.650 --> 00:34:07.340
STFC-RAL-CR03-RAL-R61-2.01: And we got, relatively good rate of low rate of emanation of 18 millivar kilogram.

197
00:34:07.390 --> 00:34:16.440
STFC-RAL-CR03-RAL-R61-2.01: In comparison, before we did this, basically, basically we reduced the factor of 10, the lack of this.

198
00:34:16.679 --> 00:34:25.709
STFC-RAL-CR03-RAL-R61-2.01: And then we tested this trap, and the way that I would test it is that… test any random trap, is that you would need a calibration source, your fluid enough protein.

199
00:34:25.850 --> 00:34:33.940
STFC-RAL-CR03-RAL-R61-2.01: To that, and then you basically, see how much radon you can, drop and extract.

200
00:34:35.449 --> 00:34:40.360
STFC-RAL-CR03-RAL-R61-2.01: So… If you compare this with,

201
00:34:40.630 --> 00:34:59.159
STFC-RAL-CR03-RAL-R61-2.01: borrowing school, that's what we found out is that under the borrowing school, which the efficiency drops with, with charcoal trap, efficiency is just constant. So we, currently have extensive review of non-microbial microbes miterap, and we're doing as an… we don't have the answer. This is…

202
00:34:59.220 --> 00:35:15.200
STFC-RAL-CR03-RAL-R61-2.01: This system is submission for external system at SOLA, but, for XSVD, again, we absolutely need to go lower. So we are basically continuing this research, basically trying to find, lower background activated charcoal.

203
00:35:15.560 --> 00:35:19.469
STFC-RAL-CR03-RAL-R61-2.01: but the method I've developed

204
00:35:19.580 --> 00:35:30.430
STFC-RAL-CR03-RAL-R61-2.01: is, already being used, by other experiments, so I saw that circulation of this experiment has gone up for other… for different… was different experiments, too.

205
00:35:30.550 --> 00:35:38.889
STFC-RAL-CR03-RAL-R61-2.01: So… Now, Water recognizance system, so, you, so…

206
00:35:39.130 --> 00:35:48.849
STFC-RAL-CR03-RAL-R61-2.01: For example, the Snow Plus is covered with, 7,000 tons of ultra-fuel water as shielded.

207
00:35:49.090 --> 00:36:05.819
STFC-RAL-CR03-RAL-R61-2.01: And, external ISMO214, which comes from radon, it's a direct background of Nocturnal status, so knowing that the radon level is, is, important. It can also be a background to the solar nocturnal search.

208
00:36:06.890 --> 00:36:17.949
STFC-RAL-CR03-RAL-R61-2.01: So, we basically have, again, very similar, similar system, but in addition to what I was talking about, we have a degasser.

209
00:36:18.340 --> 00:36:23.750
STFC-RAL-CR03-RAL-R61-2.01: and the water trap. So, basically, what happens is that you'll have,

210
00:36:23.920 --> 00:36:34.210
STFC-RAL-CR03-RAL-R61-2.01: UPW coming from, either the cavity or from the UPW, purification plant itself.

211
00:36:34.510 --> 00:36:49.979
STFC-RAL-CR03-RAL-R61-2.01: And, you basically then, it sprays to this, what we call, vacuumic acid, so it's a big chamber, which is, which is under vacuum. So you extract the radon atoms with a little bit of,

212
00:36:50.350 --> 00:37:02.170
STFC-RAL-CR03-RAL-R61-2.01: UPW, then you trap the UPW, and then the rest is familiar, right? All of them have similar design, and then you basically,

213
00:37:02.330 --> 00:37:03.910
STFC-RAL-CR03-RAL-R61-2.01: polygular atoms.

214
00:37:04.160 --> 00:37:26.969
STFC-RAL-CR03-RAL-R61-2.01: We don't do this that often, and the reason for that we don't need to. When we are doing this, is when, for example, recirculation is changing in the snow plus cavity, and we want to see how much… how much that is affecting the background of, water quality. Or the pump is broken, they put in a new pump, you want to know what is the effect of that.

215
00:37:27.130 --> 00:37:42.990
STFC-RAL-CR03-RAL-R61-2.01: So, for example, so these data points that you see, it's basically from a port, which is between the athletic cell of a snowfloss and the PMTS structure. So it's extend… so basically between these two, so it's, external to the athletic result.

216
00:37:43.420 --> 00:38:00.460
STFC-RAL-CR03-RAL-R61-2.01: And what you see here, is basically, this is the targeted, targeted value we wanted to see, and, and that's it. These are the numbers that we see, which is, 10 to minus 30, 10 to minus 13 gram of.

217
00:38:00.540 --> 00:38:05.619
STFC-RAL-CR03-RAL-R61-2.01: uranium to gram of, water per white.

218
00:38:05.750 --> 00:38:11.189
STFC-RAL-CR03-RAL-R61-2.01: So, yeah. So, we are some major,

219
00:38:11.530 --> 00:38:18.840
STFC-RAL-CR03-RAL-R61-2.01: the… the Yopita Bayou radioactivity, which other experiments…

220
00:38:18.950 --> 00:38:34.559
STFC-RAL-CR03-RAL-R61-2.01: Apart from the snow pelos, maybe you want to know that number, and that number is actually 10 to minus 14, I didn't write that. It's 10 to minus 14, so one order of magnitude is lower than what you see in the snow pelos cavity, which is if you want to…

221
00:38:34.600 --> 00:38:40.679
STFC-RAL-CR03-RAL-R61-2.01: Think about the matter of radon atoms, that's basically 294 radon atoms per liter.

222
00:38:41.770 --> 00:38:45.030
STFC-RAL-CR03-RAL-R61-2.01: So, regular removal techniques?

223
00:38:46.080 --> 00:38:49.830
STFC-RAL-CR03-RAL-R61-2.01: So the,

224
00:38:49.960 --> 00:38:57.900
STFC-RAL-CR03-RAL-R61-2.01: This is, again, focused on cardogenic, chirogenic, materials, such as, for example, XLZDD. You have,

225
00:38:58.040 --> 00:39:08.329
STFC-RAL-CR03-RAL-R61-2.01: Few ways to do… to remove radon, from, for example, the cuisine or liquid. One way is to use, distillation technique.

226
00:39:08.330 --> 00:39:19.219
STFC-RAL-CR03-RAL-R61-2.01: Basically, you have… because different, radon has different boiling points compared to liquids, compared to, like, gases, you know, acid arcolor.

227
00:39:19.220 --> 00:39:26.159
STFC-RAL-CR03-RAL-R61-2.01: So you, basically, by, by,

228
00:39:26.160 --> 00:39:40.310
STFC-RAL-CR03-RAL-R61-2.01: Having a heater and condenser, you can make sure that the radon stays in the bottom, whereas, boiler, basically liquid or gas, goes to the condenser, and then that's where you can purify it.

229
00:39:40.360 --> 00:39:57.620
STFC-RAL-CR03-RAL-R61-2.01: You can… oh, the other technique you can use is the physical absorption. I already talked about charcoal. The difference now is that in previous examples, charcoal, you want to also extract the ribbon atoms. In this example, you just want rigonatoms to stay there, so you need to make very big, very long steps in order to do that.

230
00:39:58.130 --> 00:40:10.510
STFC-RAL-CR03-RAL-R61-2.01: And, when you're using activated charcoal, you also need to go, cold again. So you need to think about, again, designing some callergenic system to cool down this activated charcoal.

231
00:40:11.100 --> 00:40:24.710
STFC-RAL-CR03-RAL-R61-2.01: The other thing which is newer in the field, is, you can use silver exchange zone, right? And the thing about silver exchange Zero is that you can actually run them in room temperature.

232
00:40:25.040 --> 00:40:38.590
STFC-RAL-CR03-RAL-R61-2.01: And, already work has been done in order to apply for liquid carbon and also world of nitrogen. So this is basically, the nature paper, which Chris mentioned.

233
00:40:38.630 --> 00:40:50.340
STFC-RAL-CR03-RAL-R61-2.01: As based on my knowledge, about selections that work as radon removal. What you see in this plot is the radon concentration versus the

234
00:40:50.430 --> 00:41:04.009
STFC-RAL-CR03-RAL-R61-2.01: Breakthrough time, so what does that breakthrough time means that the longer this time is, means that it took longer for radio to, to come out of your trap. So that means that you're more efficient in trapping, trapping radio.

235
00:41:04.140 --> 00:41:08.179
STFC-RAL-CR03-RAL-R61-2.01: So what you see is that this is an activated charcoal.

236
00:41:08.740 --> 00:41:14.680
STFC-RAL-CR03-RAL-R61-2.01: And it says… Basically,

237
00:41:14.890 --> 00:41:33.590
STFC-RAL-CR03-RAL-R61-2.01: Different, the blue is, one, Zola from one company, and there are different colors, Zola from other companies. And what you see is that, you see, backdrop 10 to 100, increase in hydrosion efficiency.

238
00:41:33.710 --> 00:41:39.390
STFC-RAL-CR03-RAL-R61-2.01: Compared to activity sharp offer, same body, all of these use the same amount of, this…

239
00:41:39.540 --> 00:41:48.450
STFC-RAL-CR03-RAL-R61-2.01: this method does. So it's no lab is, basically slowly, trying to basically test this material for,

240
00:41:48.570 --> 00:41:52.680
STFC-RAL-CR03-RAL-R61-2.01: For removing, radon,

241
00:41:52.910 --> 00:42:06.259
STFC-RAL-CR03-RAL-R61-2.01: And we are also collaborating… I'm gonna adjun from, sort of, please, too, so we are collaborating with chemists at, Coons University to basically,

242
00:42:06.530 --> 00:42:12.399
STFC-RAL-CR03-RAL-R61-2.01: tune this, zeodite for us, or removing, Kratom from Xenon.

243
00:42:13.500 --> 00:42:28.059
STFC-RAL-CR03-RAL-R61-2.01: So these are the plots showing that, like, basically the breakthrough time, of, radio in different gases, sorry, when you're uploading to different gases.

244
00:42:28.140 --> 00:42:43.560
STFC-RAL-CR03-RAL-R61-2.01: And again, it seems that, like, argon is really good. It's really good to remove radon from argon. I just said, the longer, the better. there is no data for xenon, and the reason there is no data for xenone is because I… I think…

245
00:42:43.680 --> 00:42:55.219
STFC-RAL-CR03-RAL-R61-2.01: Xenon possibly gets trapped in this, in this cell, cell-like too. So that's why you need to do a research to see how you can trap, phon, but not xenon.

246
00:42:55.990 --> 00:43:02.970
STFC-RAL-CR03-RAL-R61-2.01: Okay, so I think it's towards the end now. So, also, so when you are

247
00:43:03.200 --> 00:43:11.390
STFC-RAL-CR03-RAL-R61-2.01: As embedding a component of your detector, you need to do it in radon reduced environment,

248
00:43:11.600 --> 00:43:17.010
STFC-RAL-CR03-RAL-R61-2.01: So you can… one way to achieve that is to make,

249
00:43:17.110 --> 00:43:35.040
STFC-RAL-CR03-RAL-R61-2.01: columns of activated charcoal, and then you basically, blow, the air into this activated charcoal, and the output… the output basically gives you a lower radon, basically emanating air.

250
00:43:35.480 --> 00:43:47.379
STFC-RAL-CR03-RAL-R61-2.01: So that's how super CDMS at Sona, that's, basically, that's the technique they use, and they could achieve less than 0.1 back foot per cubic meter.

251
00:43:47.790 --> 00:43:55.600
STFC-RAL-CR03-RAL-R61-2.01: So Snow Lab, basically, Snow Lab is needed, also for future long list, projects.

252
00:43:55.760 --> 00:43:58.340
STFC-RAL-CR03-RAL-R61-2.01: possibly even begin. Beginner. There we go.

253
00:43:58.760 --> 00:44:14.279
STFC-RAL-CR03-RAL-R61-2.01: I already talked about nitrogen used as a cover gas system. Again, one way to keep radon out from your detector is to work on a nitrogen perdage environment. So at the SOA now, we actually have

254
00:44:14.360 --> 00:44:32.309
STFC-RAL-CR03-RAL-R61-2.01: a liquid nodrogen plant underground. I'm not sure whether it's a deepest liquid nitrogen plant underground or not, I have no idea, but, Reis it is quite deep, 2 kilometers. But, so this provides liquid nodrogen, and roll-off operation to, our germanium sectors, as well as the snowflops environment.

255
00:44:32.740 --> 00:44:46.150
STFC-RAL-CR03-RAL-R61-2.01: We did measure recently of this, as Tom in the back of the Q&A, and, we want to actually achieve lower than this, so we're thinking about plans of how to make this, reasonable longer.

256
00:44:46.930 --> 00:45:00.010
STFC-RAL-CR03-RAL-R61-2.01: Okay, so I think this is the Skype for a summary. I didn't want… I wanted to mention this as well, because I don't think this is, known that much outside. We are just writing publication about it, so hopefully it becomes a bit more and more.

257
00:45:00.030 --> 00:45:10.979
STFC-RAL-CR03-RAL-R61-2.01: So SNO Plus, is using… this is a picture of me when I was a postdoc. SNO Plus is, using,

258
00:45:11.170 --> 00:45:22.430
STFC-RAL-CR03-RAL-R61-2.01: basically a unique color gas system. So, one problem that we have in the mine, at the snow lab, is that we have

259
00:45:23.120 --> 00:45:41.969
STFC-RAL-CR03-RAL-R61-2.01: pressure fluctuation of, about 10%, 9%, 10%. And the problem with that pressure fluctuation is that, sodium… sodium pressure fluctuation can actually, damage equipment and damage, defectors. It's no clause.

260
00:45:42.010 --> 00:45:46.530
STFC-RAL-CR03-RAL-R61-2.01: Has, it's a 12 meter diameter act in it, which has a niche.

261
00:45:46.610 --> 00:45:55.219
STFC-RAL-CR03-RAL-R61-2.01: And basically, engineering calculation shows that the net should not be exposed to that 9% pressure fluctuation.

262
00:45:55.270 --> 00:46:11.890
STFC-RAL-CR03-RAL-R61-2.01: So, naive, solution for not making… to make sure that Reagan doesn't get in is to just steal the top of your gettor. But we cannot just steal the top of your debtor, because then you don't… you cannot adjust for the facial change, and that will break your neck.

263
00:46:12.110 --> 00:46:27.830
STFC-RAL-CR03-RAL-R61-2.01: So that's why, we basically designed the flexible backs, which basically, they can breathe and how when their pressure changes, from low radon material, of course, because that was important.

264
00:46:27.890 --> 00:46:36.139
STFC-RAL-CR03-RAL-R61-2.01: And, I like to call them a long pulp as not blows, because they're exactly like longs, they, basically breathe in and out.

265
00:46:36.340 --> 00:46:46.349
STFC-RAL-CR03-RAL-R61-2.01: And, we could, basically reach the, sensitivity of 01 backward in cubic meter width.

266
00:46:46.710 --> 00:47:00.130
STFC-RAL-CR03-RAL-R61-2.01: And this is, basically, makes the requirement for data detective search of, visits, and, but it's not… if you want to do more research stolen entrepreneur, we actually need to go a bit lower than that.

267
00:47:00.940 --> 00:47:02.580
STFC-RAL-CR03-RAL-R61-2.01: Okay, so…

268
00:47:02.590 --> 00:47:13.740
STFC-RAL-CR03-RAL-R61-2.01: So, to summarize, external operator experiments profile the mental question in particle physics, and control radar in this background is critical to actually increase scores,

269
00:47:13.740 --> 00:47:23.889
STFC-RAL-CR03-RAL-R61-2.01: SNOLA continues to strengthen its radon mitigation program by building and operating low-background radon access systems, or on each one making low-background radon counting systems.

270
00:47:23.960 --> 00:47:30.819
STFC-RAL-CR03-RAL-R61-2.01: And developing advanced radon removal techniques, creating radon-reduced environment, the boil of nitrogen.

271
00:47:31.140 --> 00:47:38.330
STFC-RAL-CR03-RAL-R61-2.01: And we also have to maintain existing radar systems. this, of course, was Workout

272
00:47:38.550 --> 00:47:41.109
STFC-RAL-CR03-RAL-R61-2.01: So many,

273
00:47:41.320 --> 00:47:49.640
STFC-RAL-CR03-RAL-R61-2.01: graduate students and master's students, they were basically working on this, so… Yeah, thank you. Yes, thank you.

274
00:47:53.030 --> 00:47:55.330
STFC-RAL-CR03-RAL-R61-2.01: Thank you for the very…

275
00:47:55.600 --> 00:48:09.250
STFC-RAL-CR03-RAL-R61-2.01: Are there questions? And thanks, everyone, for sticking to the end this morning. She has one within 50 minutes, so yes, we'll find out the delay in the beginning, but yes. Are there any questions on Zoom phones?

276
00:48:10.820 --> 00:48:14.350
STFC-RAL-CR03-RAL-R61-2.01: I don't see yet any, here in the room.

277
00:48:14.630 --> 00:48:16.590
STFC-RAL-CR03-RAL-R61-2.01: Yeah, I had a question about…

278
00:48:16.930 --> 00:48:21.260
STFC-RAL-CR03-RAL-R61-2.01: your samples, when you put them in the detectives. So you mentioned the…

279
00:48:21.910 --> 00:48:26.910
STFC-RAL-CR03-RAL-R61-2.01: Because of, like, the difference between the surface stuff and the stuff that comes from the center.

280
00:48:27.040 --> 00:48:34.029
STFC-RAL-CR03-RAL-R61-2.01: With the geometry of the samples that you create, whether you've got, like, quite a dense sample, whether you've got a plane of a sample.

281
00:48:34.270 --> 00:48:36.340
STFC-RAL-CR03-RAL-R61-2.01: That could probably change your…

282
00:48:36.950 --> 00:48:45.899
STFC-RAL-CR03-RAL-R61-2.01: your results significantly. So how do you control and make the geometry of your samples representative of the thing that you're trying to

283
00:48:45.900 --> 00:49:04.190
STFC-RAL-CR03-RAL-R61-2.01: So sometimes you need to make a dedicated… so depending on what time… so, for example, let's say you want to measure cables, like, I would say for cables, you possibly want to make a very long tube and put your cables there, as an example, and it's matching that geometry.

284
00:49:05.670 --> 00:49:24.260
STFC-RAL-CR03-RAL-R61-2.01: So that's one way to, yeah, that's one way. The other way is that we are already doing two measurements, by lamp one. So, the hope is that the second measurement is more accurate, and it's the diffusion by that is, like, basically came out.

285
00:49:24.470 --> 00:49:40.760
STFC-RAL-CR03-RAL-R61-2.01: Yeah, so we usually throw out the first measurement, but keep the second measurement. If it's like, if the first and second measurement are so different that it affects what we are reporting to the experiment, then you'll have to do the third one. That's why this

286
00:49:40.760 --> 00:49:47.830
STFC-RAL-CR03-RAL-R61-2.01: I've really toned it down, but it can take a month to do a measure. It's easy, or even long.

287
00:49:51.740 --> 00:50:02.669
STFC-RAL-CR03-RAL-R61-2.01: Yes, absolutely. Thank you for the talk, very interesting. I have a question again in the lower ground radon counting system. You mentioned zinc sulfide, so…

288
00:50:03.050 --> 00:50:09.300
STFC-RAL-CR03-RAL-R61-2.01: that's a wide-engaged material like others. I don't know exactly, I don't recall what they eel.

289
00:50:09.920 --> 00:50:20.860
STFC-RAL-CR03-RAL-R61-2.01: the photon yield of zinc sulfide is, but have you considered, for example, using gallium nitronide, that also has a similar band gap.

290
00:50:21.210 --> 00:50:28.879
STFC-RAL-CR03-RAL-R61-2.01: Compared to zinc sulfide, and I suspect… Gallium nitride, and I think it would be even lower.

291
00:50:29.000 --> 00:50:42.519
STFC-RAL-CR03-RAL-R61-2.01: Okay, I, yeah, I can look at that, yeah. We are, zinc so far, it's just that because it was something that's, I guess, a snow legacy, and we want to see whether we can purify it, but yeah, I mean…

292
00:50:42.720 --> 00:50:49.440
STFC-RAL-CR03-RAL-R61-2.01: The plan is to make something better than our Kristenity, so I will… that's, that sounds…

293
00:50:49.600 --> 00:51:06.339
STFC-RAL-CR03-RAL-R61-2.01: Yeah, I imagine that the yield… If it's inorganic, I guess, you know, yeah, it is inorganic, too, right? Yeah, it's a semiconductor. I'm saying, I think the yield is similar, so I'm talking to the 5 visible photons, fairly big, which is what I mean.

294
00:51:06.430 --> 00:51:16.530
STFC-RAL-CR03-RAL-R61-2.01: Another fund. So, I might imagine that given that it's more developed as a semiconductor technology compared to things so far, it might actually be kind of better.

295
00:51:16.700 --> 00:51:17.570
STFC-RAL-CR03-RAL-R61-2.01: Excuse me.

296
00:51:18.070 --> 00:51:31.079
STFC-RAL-CR03-RAL-R61-2.01: Do you think the purification of it is easy, do you think? Well, they use it routinely in semiconductor industry, so the fabrication process obviously takes place in a very highly controlled

297
00:51:31.430 --> 00:51:37.039
STFC-RAL-CR03-RAL-R61-2.01: environment, so I would imagine that in terms of PR, it is probably better. Okay, so fine.

298
00:51:37.280 --> 00:51:38.860
STFC-RAL-CR03-RAL-R61-2.01: Okay, thank you.

299
00:51:39.070 --> 00:51:46.000
STFC-RAL-CR03-RAL-R61-2.01: And in Canada, you also have NRC, which has a long, addition.

300
00:51:46.330 --> 00:51:49.969
STFC-RAL-CR03-RAL-R61-2.01: In developing and working with gallon nitride material.

301
00:51:52.060 --> 00:51:54.119
STFC-RAL-CR03-RAL-R61-2.01: I think it's only 4 hours' drive from you.

302
00:51:54.330 --> 00:52:00.340
STFC-RAL-CR03-RAL-R61-2.01: Sorry, sorry, where… where did you say in Canada? National Movies, St. National Research Center. Yeah.

303
00:52:01.570 --> 00:52:04.150
STFC-RAL-CR03-RAL-R61-2.01: Here, Carlton University. Okay.

304
00:52:14.690 --> 00:52:16.709
STFC-RAL-CR03-RAL-R61-2.01: Thank you. Thank you very much.

305
00:52:19.380 --> 00:52:29.569
STFC-RAL-CR03-RAL-R61-2.01: I had a really silly question. The… the 9% pressure difference over Snow Lab, is that just general use, or is that, like, when you have a power cut, and the…

306
00:52:30.010 --> 00:52:48.040
STFC-RAL-CR03-RAL-R61-2.01: systems go down. It can be ventilation, sometimes problem, power cut, yeah, mainly power cards, you can have liquids, not liquid, sorry, system damage is not liquid or black, because you are underground and rocks can, like, crack and burst.

307
00:52:48.070 --> 00:52:52.440
STFC-RAL-CR03-RAL-R61-2.01: That type of thing can cause… Oh, change of pressure.

308
00:52:52.710 --> 00:53:01.340
STFC-RAL-CR03-RAL-R61-2.01: Yeah, yeah. I just remember, like, when the power cuts went, my ears just went… Yeah, yeah, yeah.

309
00:53:03.460 --> 00:53:13.760
STFC-RAL-CR03-RAL-R61-2.01: Sorry. Yeah, I saw you at the moment. I saw you somewhere.

310
00:53:15.850 --> 00:53:24.610
STFC-RAL-CR03-RAL-R61-2.01: Can I, ask, so in your system, you've got two, radon traps, the primary, and then… why is that?

311
00:53:24.610 --> 00:53:43.630
STFC-RAL-CR03-RAL-R61-2.01: It's because of the local cell geometry. You… if you, your trap is big and local cell is, like, small, so if you want the efficiency to be maximum, you need to concentrate regular atoms to a trap which is a smaller volume than the locusa. But why do we need two? So, second one is, very…

312
00:53:43.630 --> 00:53:50.260
STFC-RAL-CR03-RAL-R61-2.01: The first… the second one we call a concentration trap is the one that's much smaller than the first of all.

313
00:53:50.400 --> 00:53:51.420
STFC-RAL-CR03-RAL-R61-2.01: Does that make sense?

314
00:53:51.720 --> 00:53:54.190
STFC-RAL-CR03-RAL-R61-2.01: So, you would draw if you want.

315
00:53:54.310 --> 00:53:57.470
STFC-RAL-CR03-RAL-R61-2.01: That's possible. So… oh.

316
00:53:57.940 --> 00:54:02.940
STFC-RAL-CR03-RAL-R61-2.01: There are skits, skits there. Yeah, I could have time.

317
00:54:05.850 --> 00:54:13.939
STFC-RAL-CR03-RAL-R61-2.01: So, I think Lo Croissant, so low croissant, I think, has, if I don't remember correctly, is 30 centimeter

318
00:54:14.070 --> 00:54:16.180
STFC-RAL-CR03-RAL-R61-2.01: Healed by Daniel?

319
00:54:16.350 --> 00:54:18.650
STFC-RAL-CR03-RAL-R61-2.01: Whereas, like, your first fab.

320
00:54:19.270 --> 00:54:27.200
STFC-RAL-CR03-RAL-R61-2.01: is, like, I have to do the calculation, but it's almost, like, almost a backdrop in volume compared to the album.

321
00:54:28.180 --> 00:54:34.269
STFC-RAL-CR03-RAL-R61-2.01: So, it's much lower volume. So, that means that your efficiency, if you do volume sharing.

322
00:54:34.430 --> 00:54:49.949
STFC-RAL-CR03-RAL-R61-2.01: to… to basically go there, then your efficiency will be, like, one thing. Yeah, I understand that. It's just, so you've got two, so you want to concentrate the concentrated, just to get a higher…

323
00:54:50.440 --> 00:55:04.880
STFC-RAL-CR03-RAL-R61-2.01: Yeah, that's right. Otherwise, if you use this from the beginning, then this is not big enough to trap your radon atoms. Okay. So you need something bigger and more forest to trap radon atoms, and then you need a second.

324
00:55:05.130 --> 00:55:24.220
STFC-RAL-CR03-RAL-R61-2.01: But it's a very good point. So, if you have a bigger detector, see, this is optimized with John 4, to, for example, have this design. If you have a bigger detector, then this problem goes away, right? So, for example, people using big electrostatic chambers, they don't have that problem as much.

325
00:55:25.040 --> 00:55:29.760
STFC-RAL-CR03-RAL-R61-2.01: Yeah, so this is because… this is basically, yeah, related to the geometry of the bus.

326
00:55:31.890 --> 00:55:32.810
STFC-RAL-CR03-RAL-R61-2.01: Thanks.

327
00:55:36.020 --> 00:55:47.550
STFC-RAL-CR03-RAL-R61-2.01: I would like to ask, are there other labs in the world that do similar research?

328
00:55:47.660 --> 00:56:03.300
STFC-RAL-CR03-RAL-R61-2.01: Yeah, radon, it's very… so, all the underground labs have more or less, moving twice, same type of research. They all have systems, and they're all thinking about how I can make this more

329
00:56:03.360 --> 00:56:20.969
STFC-RAL-CR03-RAL-R61-2.01: Basically, high sensitivity for next generation. Okay. The more we… I was bored with misbeigans, saw this stuff, yeah. But the more you… you need to have more of them in the world, because, as I said, one measurement takes them one month.

330
00:56:20.970 --> 00:56:25.609
STFC-RAL-CR03-RAL-R61-2.01: Two months, and then you have to have lots of, lots of,

331
00:56:27.590 --> 00:56:35.019
STFC-RAL-CR03-RAL-R61-2.01: Components of experiment, lots of candidates, of which one you want to use, then you want to do it as fast as possible.

332
00:56:35.090 --> 00:56:47.670
STFC-RAL-CR03-RAL-R61-2.01: Yes, and as far as I understand, you have not reached your goal yet. No, we have. So… We reached for the current experiment? For the car. Yes. Yeah, so… So,

333
00:56:48.060 --> 00:56:53.450
STFC-RAL-CR03-RAL-R61-2.01: Do you think this goal is realistic, and whether more research would help?

334
00:56:53.880 --> 00:57:05.360
STFC-RAL-CR03-RAL-R61-2.01: Yeah, so, I think, I think it's realistic, the research material science. We just need to…

335
00:57:05.580 --> 00:57:18.130
STFC-RAL-CR03-RAL-R61-2.01: basically find purification techniques that would work with a certain scintillator, or, if you are… if you're, for example, using electrostatic chamber different metallurgy, you need to find

336
00:57:18.310 --> 00:57:19.840
STFC-RAL-CR03-RAL-R61-2.01: at,

337
00:57:20.640 --> 00:57:27.809
STFC-RAL-CR03-RAL-R61-2.01: maybe need to make them from, electrophone Harper as an example. I mean, we need to, like, you know.

338
00:57:28.590 --> 00:57:34.810
STFC-RAL-CR03-RAL-R61-2.01: I think it's possible, though. Yes. It's not realistic. And you mentioned about commercial.

339
00:57:35.120 --> 00:57:36.480
STFC-RAL-CR03-RAL-R61-2.01: devices.

340
00:57:36.760 --> 00:57:41.690
STFC-RAL-CR03-RAL-R61-2.01: Do you know why they are better, and what their application is?

341
00:57:41.690 --> 00:58:06.569
STFC-RAL-CR03-RAL-R61-2.01: Except that they're expensive, why we can't use… Oh, so sorry, which, which one? In the first part, you mentioned about the commercial… Oh, it's just that the commercial ones are… it's only… they can only measure… Only the measure. They can measure, yeah, it's just not good enough for, giving… they don't give us enough information. Okay. They only give… so, they only… the commercials are only given

342
00:58:06.570 --> 00:58:20.899
STFC-RAL-CR03-RAL-R61-2.01: information about the top of the chain, and information on the bottom of the chain. Right. They don't give information of the middle of the chain. Actually, for diabetic, is the most important part. Yes. Do you know commercially what they are used for?

343
00:58:21.580 --> 00:58:24.350
STFC-RAL-CR03-RAL-R61-2.01: Oh, sorry. So,

344
00:58:24.720 --> 00:58:36.389
STFC-RAL-CR03-RAL-R61-2.01: Oh, one of them is ICPM. Is that what you're talking about ICPMS, one of them is a mass spectroscopy. Yes. And the other one is XIA, alpha extract.

345
00:58:36.630 --> 00:58:53.780
STFC-RAL-CR03-RAL-R61-2.01: It's just a brief chamber, which is basically, has honored and model, and measuring, basically, the ionization of everybody's world. Did that answer your question? Yeah, yeah, that's… yeah. One last question on the picture, one slide back.

346
00:58:57.370 --> 00:58:59.479
STFC-RAL-CR03-RAL-R61-2.01: You could use the pointer. Okay.

347
00:59:00.400 --> 00:59:01.220
STFC-RAL-CR03-RAL-R61-2.01: Oh, yeah.

348
00:59:01.340 --> 00:59:20.470
STFC-RAL-CR03-RAL-R61-2.01: It doesn't work. Yeah, I was wondering whether this is an underground picture? Yes. And, why the walls are white. Oh, yes, this is, this is basically, the Harper paint. It is underground.

349
00:59:20.570 --> 00:59:26.470
STFC-RAL-CR03-RAL-R61-2.01: It's a type of paint we put in in order to, reduce further ingress.

350
00:59:26.840 --> 00:59:46.260
STFC-RAL-CR03-RAL-R61-2.01: The whole, whole area. Like, the whole snow lamp is covered with this. It's white. Okay, it also looks very bright. Yes, it looks… I mean, yeah, it is, it is, it is, it does reflect. It does reflect. If you're next to it, then I recollect.

351
00:59:46.560 --> 00:59:47.550
STFC-RAL-CR03-RAL-R61-2.01: Yes.

352
00:59:48.170 --> 00:59:53.930
STFC-RAL-CR03-RAL-R61-2.01: And, despite of that, we set up 120 bands for every two weeks. I don't know how it was.

353
00:59:54.240 --> 00:59:56.259
STFC-RAL-CR03-RAL-R61-2.01: Maybe I have that.

354
00:59:57.530 --> 00:59:58.460
STFC-RAL-CR03-RAL-R61-2.01: Okay.

355
00:59:58.860 --> 00:59:59.770
STFC-RAL-CR03-RAL-R61-2.01: Is that…

356
00:59:59.810 --> 01:00:19.159
STFC-RAL-CR03-RAL-R61-2.01: from Raiden Group, I heard from Sammy, you mentioned. Sorry. I've already asked. Maybe you can talk. I don't do anything on Raiden, by the way. I'm just in that building. Oh, okay. You don't have a rhythm, right? No, I don't work on Raiden.

357
01:00:19.270 --> 01:00:27.080
STFC-RAL-CR03-RAL-R61-2.01: Okay, on that note, let's close the seminar here, and thanks again, everyone, for doubling.

358
01:00:30.460 --> 01:00:34.460
STFC-RAL-CR03-RAL-R61-2.01: Okay, fine.

