# Present Status and Future Perspectives for the EXO-200 Experiment

Authors: Giorgio Gratta; David Sinclair
Journal: Advances in High Energy Physics
 (2013)

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## Abstract

The EXO collaboration has built and operated a 200 kg liquid xenon detector for studies of double beta decay. This paper summarizes the results obtained so far and their significance. The excellent performance of the detector encourages the concept of a much larger detector to obtain improved sensitivity to the possible detection of the neutrinoless decay mode of xenon.


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## Body

## 1. Introduction

The search for neutrinoless double beta decay is one of the most pressing but also one of the most challenging endeavours in the push to understand the natural world beyond the standard model of particle physics. The standard model has had great success in describing the interactions of the elementary particles and, with the recent observation of a Higgs-like particle, of explaining the mass of all particles except for the neutrinos. In 1937, Majorana [1] suggested that neutrinos might be described as 2-component Weyl spinors rather than the 4 component description of the Dirac model. Shortly after, Furry [2] pointed out that while the Majorana model would not change normal beta decay, it would allow a new form of double beta decay in which no neutrinos were emitted. More than 75 years later, we still have not detected this decay mode or resolved the fundamental difference in the Majorana and Dirac models for the neutrino.The first evidence that rates for either mode of double beta decay that would be very long came from the observation of apparently stable isotopes in nature which were energetically able to decay by this mode. This sets a lower bound on the lifetimes comparable to geological timescales. The limits were extended to higher values by searches for possible daughter elements. For example, in the work of Inghram and Reynolds [3] tellurium bearing ores were analyzed for the presence of xenon isotopes. Limits on decay half-lives in the order of 1019 years were set. Direct searches for double beta decay using counters were also started at about this time. Searches for two electrons being emitted from 124Sn were carried out using coincident electron counters by Fireman [4] and in a bubble chamber by Fireman and Schwarzer [5] gave a lower bound of 1017 years. A motivation for these early searches was the expectation that the neutrinoless decay would be much faster than the two-neutrino decay, if the neutrino was indeed a Majorana particle. This expectation changed dramatically when parity nonconservation in weak interactions was observed and the V-A behavior of the weak interaction established.The first successful detection of the two-neutrino double beta decay mode was made by a group led by Moe (see Elliott et al. [6]). Electrons from a foil of 82Se were detected in a TPC to give an unambiguous signature of the decay process. The observed half-life was about 1020 years. The two-neutrino decay mode of several metallic elements has now been measured with the most precise data coming from the NEMO [7] experiment.Limits on neutrinoless double beta decay lifetimes continued to increase with the application of more sophisticated experimental techniques, but the recent observation of neutrino oscillations has greatly enhanced the interest in this search. Neutrino oscillations, as discovered for atmospheric neutrinos by Fukuda et al. [8], for solar neutrinos by Ahmad et al. [9] and for reactor neutrinos by Eguchi et al. [10] show that neutrinos must possess mass and that the individual lepton flavor numbers are not conserved quantities. These discoveries have been confirmed by a number of experiments that have, in many cases, improved on the precision of the parameters entering oscillation description. Some recent references can be found in [11–17].Neutrino-antineutrino oscillations were first proposed by Pontecorvo [18] in analogy with the K0 oscillation in the hadron sector. Pontecorvo and Gribov [19, 20] first suggested that the solar neutrino problem could be explained by flavor oscillation of neutrinos and this fundamental insight, with modifications due to matter effects, has now been demonstrated to be correct. The observation that neutrinos do oscillate is a challenge to the standard model because it cannot explain, without some extension, why particles always observed to be left handed can have mass.Thus, the fundamental questions which can now be addressed by an observation of neutrinoless double beta decay are as follows.(1)
Are neutrinos Dirac or Majorana particles?(2)
Is total lepton number conserved or is it violated as required in some cosmological models?(3)
Can we determine the absolute mass scale for neutrinos?There are several isotopes which can be exploited in the search for double beta decay. Germanium is attractive because of the advanced technology for making high resolution, high volume detectors. Tellurium is attractive because of the high natural abundance of the candidate isotope130Te. In this paper, we describe a search for double beta decay in 136Xe.


## 2. Xenon Detectors for Double Beta Decay

There are several reasons why xenon is an attractive target for the double beta decay search. The most interesting isotope,136Xe, is quite abundant at 9.6% in nature and it is one of the easiest (and hence least expensive) of the double beta decay candidates to enrich. It is possible to make xenon extremely pure and this is essential both to allow a detector to be built in which electrons drift without serious loss and to eliminate radioactive backgrounds which can mimic the double beta decay signal. There are no long-lived xenon isotopes which might give internal backgrounds. Xenon detectors may be in gaseous form (as used, e.g., in the Gotthard double beta decay search [21] and in the NEXT [22] projects) or as a liquid detector as used in EXO-200. Xenon may also be dissolved into a liquid scintillator as used at Gando et al. [23]. Each form has advantages and disadvantages. Gaseous detectors offer the possibility of excellent spatial information about the decays including a clear signature of two electron tracks. This has proven important in reducing gamma ray backgrounds [21]. The best gaseous detectors have offered near Fano limited energy resolutions [22], while this has not yet been reached with liquid detectors. The gas detectors can operate at room temperature and do not require complex cryogenics. Finally, gas detectors can operate with intrinsic gain and this greatly reduces the electronic noise contributions. Detectors which employ xenon dissolved into organic liquid scintillators offer excellent low background environments and a high degree of uniformity and homogeneity. The energy resolution has not yet matched that of other technologies and the detectors act as a pure calorimeter without any tracking information. On the other hand, condensed liquid xenon detectors are much more compact requiring much less underground space and shielding. Furthermore, the high density of liquid xenon allows very good self-shielding against external gamma backgrounds, moderate resolution, and the ability to reconstruct the event topologies. EXO-200 is a liquid phase detector.


## 3. Barium Tagging

A unique possibility offered by a xenon detector is that all backgrounds except the two-neutrino decay mode could be effectively removed by identification of the daughter barium ion. This possibility was first put forward by Moe [24] and is based on the observation by a number of groups of single ion detection for barium. Essentially, one transports the daughter ion to a region where it can be identified using atomic laser resonant spectroscopy. The EXO-200 detector does not include a barium tag provision, but the EXO group are actively pursuing technologies to accomplish this tag with both liquid and gas type detectors and this may prove essential for an ultimate double beta decay detector sensitive through the normal hierarchy of neutrino masses.


## 4. The EXO-200 Detector

The EXO-200 detector is in the form of a back-to-back liquid-xenon time projection chambers (TPCs), with high efficiency UV light detection with a total inventory of 200 kg of xenon enriched to 81% in136Xe. Both liquid and gas detectors require the scintillation signal to provide the start time signal, but, in addition, it was determined early in the development of the EXO detector that in liquid xenon the energy deposited by ionizing radiation is split between production of electrons and scintillation photons and that both must be measured to ensure a good energy resolution [25]. The detector has been described in detail in [26]. Figure 1 shows the details of the central detector element, while Figure 2 displays the overall detector arrangement.Figure 1
Details of the EXO-200 detector.Figure 2
Overall detector configuration as installed at WIPP.


### 4.1. Detector Operation

In an ionizing event, a burst of scintillation light at 175 nm is emitted. The intensity is approximately 50,000 photons per MeV for minimum ionizing particles. These photons are recorded using an array of large area avalanche photodiodes located behind the anode. All surfaces except the diodes are reflecting to maximize the detected yield.Electrons liberated by the ionization drift towards the anode under the drift field of about 500 V/cm. At the anode, there is a pair of wire planes oriented 60 degrees to each other. At the first plane, signals are induced by the passing electrons, while the electrons are collected on the second plane. An increased field between the wires gives high gridding efficiency. Signals from the wires are digitized at 1 MHz so that the time evolution of the arriving electrons can be determined. From this information, it is possible to reconstruct the full 3-dimensional distribution of ionization. As discussed below, this information is critical for two aspects of the analysis—it allows for a definition of a fiducial boundary to maximize the signal to background ratio and it allows a separation between double beta-like events where the energy is deposited in a single location from the gamma-like events where the events tend to involve multiple Compton scatterings giving multisite ionization. The resolution is not adequate to see the electron tracks or to distinguish single from double electron events. Alpha-decay events can be readily identified by their very high light to ionization yield.The detector is constructed as two back-to-back TPCs with a common central cathode. This configuration allows shorter average electron drift distances that, in turn, minimizes the electron loss due to attachment.There are several aspects of the detector design that are aimed at controlling the radioactive background. All detector materials have been carefully screened for activity and a lengthy report on the assay program has been published [20]. The materials for the inner detector are mainly low activity copper, phosphor bronze, acrylic, and teflon. The central detector is surrounded by a heat transfer fluid HFE7000 [28] which provides a cooling link between the refrigeration systems and the detector and with a specific density of about 1.8 at liquid xenon temperatures provides a good gamma shield. The next layer is the copper cryostat formed from two layers of ultralow background copper of thickness 2.5 cm. The cryostat is surrounded by 25 cm of low activity lead to provide the main shield against external gamma backgrounds. Finally, a set of cosmic ray veto detectors covers most of the surface to tag muon events. With this configuration, the residual backgrounds are mainly from the local detector materials. The detector is located in the WIPP facility in New Mexico, USA which provides an overburden of 1600 metres of water equivalent.


### 4.2. Detector Performance

The detector response is measured using a calibration facility that can move gamma sources to locations about the detector. Key parameters to be measured include the charge calibration for the wires, the light response as a function of position, the electron lifetime during drift, single site and multisite event ratios, and the overall energy scale.The electron lifetime is an important parameter in establishing good energy resolution and it is a very sensitive measure of the xenon purity. In EXO-200, lifetimes of about 3 ms have been maintained. This is achieved by careful attention to cleanliness at all stages of the detector construction and a high recirculation flow through a SAES getter for impurity removal.An important aspect of the analysis of EXO-200 data is the discrimination between gamma and beta events based on the number of ionization clusters. The discrimination depends on energy, but for events near the zero neutrinoQ value, the enhancement of gamma events in the multisite partition is about a factor of 5 (as seen in Figure 3). This is important not only for understanding the gamma background but also, if a peak were observed at Qββ in the single site spectrum, ruling for out a gamma interpretation if a much stronger peak were not observed in the corresponding multisite data.Figure 3
Multisite and single site data and Monte Carlo for a228Th source [25]. Excellent quantitative agreement is observed demonstrating that the detector is well characterized.The overall test of the calibration process is the extent to which the detector Monte Carlo can reproduce the observed response to known gamma sources. Such a test is displayed in Figure3. The agreement is excellent.


## 4.1. Detector Operation

In an ionizing event, a burst of scintillation light at 175 nm is emitted. The intensity is approximately 50,000 photons per MeV for minimum ionizing particles. These photons are recorded using an array of large area avalanche photodiodes located behind the anode. All surfaces except the diodes are reflecting to maximize the detected yield.Electrons liberated by the ionization drift towards the anode under the drift field of about 500 V/cm. At the anode, there is a pair of wire planes oriented 60 degrees to each other. At the first plane, signals are induced by the passing electrons, while the electrons are collected on the second plane. An increased field between the wires gives high gridding efficiency. Signals from the wires are digitized at 1 MHz so that the time evolution of the arriving electrons can be determined. From this information, it is possible to reconstruct the full 3-dimensional distribution of ionization. As discussed below, this information is critical for two aspects of the analysis—it allows for a definition of a fiducial boundary to maximize the signal to background ratio and it allows a separation between double beta-like events where the energy is deposited in a single location from the gamma-like events where the events tend to involve multiple Compton scatterings giving multisite ionization. The resolution is not adequate to see the electron tracks or to distinguish single from double electron events. Alpha-decay events can be readily identified by their very high light to ionization yield.The detector is constructed as two back-to-back TPCs with a common central cathode. This configuration allows shorter average electron drift distances that, in turn, minimizes the electron loss due to attachment.There are several aspects of the detector design that are aimed at controlling the radioactive background. All detector materials have been carefully screened for activity and a lengthy report on the assay program has been published [20]. The materials for the inner detector are mainly low activity copper, phosphor bronze, acrylic, and teflon. The central detector is surrounded by a heat transfer fluid HFE7000 [28] which provides a cooling link between the refrigeration systems and the detector and with a specific density of about 1.8 at liquid xenon temperatures provides a good gamma shield. The next layer is the copper cryostat formed from two layers of ultralow background copper of thickness 2.5 cm. The cryostat is surrounded by 25 cm of low activity lead to provide the main shield against external gamma backgrounds. Finally, a set of cosmic ray veto detectors covers most of the surface to tag muon events. With this configuration, the residual backgrounds are mainly from the local detector materials. The detector is located in the WIPP facility in New Mexico, USA which provides an overburden of 1600 metres of water equivalent.


## 4.2. Detector Performance

The detector response is measured using a calibration facility that can move gamma sources to locations about the detector. Key parameters to be measured include the charge calibration for the wires, the light response as a function of position, the electron lifetime during drift, single site and multisite event ratios, and the overall energy scale.The electron lifetime is an important parameter in establishing good energy resolution and it is a very sensitive measure of the xenon purity. In EXO-200, lifetimes of about 3 ms have been maintained. This is achieved by careful attention to cleanliness at all stages of the detector construction and a high recirculation flow through a SAES getter for impurity removal.An important aspect of the analysis of EXO-200 data is the discrimination between gamma and beta events based on the number of ionization clusters. The discrimination depends on energy, but for events near the zero neutrinoQ value, the enhancement of gamma events in the multisite partition is about a factor of 5 (as seen in Figure 3). This is important not only for understanding the gamma background but also, if a peak were observed at Qββ in the single site spectrum, ruling for out a gamma interpretation if a much stronger peak were not observed in the corresponding multisite data.Figure 3
Multisite and single site data and Monte Carlo for a228Th source [25]. Excellent quantitative agreement is observed demonstrating that the detector is well characterized.The overall test of the calibration process is the extent to which the detector Monte Carlo can reproduce the observed response to known gamma sources. Such a test is displayed in Figure3. The agreement is excellent.


## 5. Experimental Results

### 5.1. Two-Neutrino Double Beta Decay of136Xe

The first low background physics run of EXO-200 produced the data displayed in Figure4. Events are classified as single site or multisite, as was done for the calibration data. Now, most of the events involving gamma rays will appear as multisite because most gammas will Compton scatter in the detector. Most of the double beta events will show up at single sites because the range of the betas is very small in the liquid xenon compared with the spatial resolution. One can see that the data are completely dominated by the two-neutrino decay. That is, the backgrounds are typically less than 10% of the signal. One can also see that the fit of all known signals to the data gives an excellent description of the observed spectrum.Figure 4
The EXO data [27] showing the multisite events and the single site events. The best fit is shown in blue, while the background components are as follows: grey: 2νββ; dotted orange: 40K; dark blue: 60Co; green, cyan and black are 238U (mainly 214Bi) on the air gap, TPC vessel, and cathode, respectively; dotted magenta: 232Th in the vessel.Prior to the EXO experiment no observation of the two-neutrino double beta decay mode had been reported although there were two reports of studies which produced only upper limits for the decay rate [29, 30]. The reported bounds were of concern because they suggested that the two-neutrino decay of 136Xe was anomalously low. The EXO collaboration first reported a clear observation of the two neutrino decay mode in 2011 [31]. The rate seen was considerably higher than the limits previously reported and reflects the advantages of a large mass, very low background detector. The EXO results were confirmed by the KAMLAND-ZEN team shortly after [24]. In a paper recently submitted for publication, the EXO group have presented a fuller analysis where several of the systematic errors have been reduced to provide the highest precision measure of a two-neutrino double beta decay. The final result is a half-life of 2.172±0.017 (stat) ± 0.060 (sys) × 1021 years [32].


### 5.2. Search for Zero Neutrino Decays of136Xe

The primary aim of the EXO project is the search for neutrino-less decay of136Xe. The signature of such a decay would be a peak in the total deposited energy spectrum at the decay Q value. The EXO-200 first search for this decay mode was published in 2012 [27] where details of the analysis may be found. The data are displayed in Figure 4. Critical to the search for the neutrino-less decay is the separation between gamma backgrounds and the signal through the multisite/single site discrimination. No evidence for neutrino-less decay is observed.As discussed in [27], the analysis of these data gives a bound on the possible neutrinoless double beta decay of 136Xe T>1.6×1025 years at 90% confidence. To extract a corresponding limit to the neutrino mass, one needs to choose a nuclear matrix element. For recently published values using generator coordinate method [33], nuclear shell model [34], interacting boson model [35], RQRPA [36], and the QRPA-2 [37], the mass limit is 140–380 meV.There has been a claim of observation of neutrinoless double beta decay in germanium [38]. In order to compare the EXO limits to expectations for germanium, one uses the relative matrix elements from a set of calculations. The results are displayed in Figure 5. Clearly the measurement from EXO does not support the previous claim. Again, the EXO result has been confirmed by Gando et al. [39].Figure 5
This figure compares the expected half-lives of136Xe and 76Ge for matrix elements from various models. References for the models are found in the text.


## 5.1. Two-Neutrino Double Beta Decay of136Xe

The first low background physics run of EXO-200 produced the data displayed in Figure4. Events are classified as single site or multisite, as was done for the calibration data. Now, most of the events involving gamma rays will appear as multisite because most gammas will Compton scatter in the detector. Most of the double beta events will show up at single sites because the range of the betas is very small in the liquid xenon compared with the spatial resolution. One can see that the data are completely dominated by the two-neutrino decay. That is, the backgrounds are typically less than 10% of the signal. One can also see that the fit of all known signals to the data gives an excellent description of the observed spectrum.Figure 4
The EXO data [27] showing the multisite events and the single site events. The best fit is shown in blue, while the background components are as follows: grey: 2νββ; dotted orange: 40K; dark blue: 60Co; green, cyan and black are 238U (mainly 214Bi) on the air gap, TPC vessel, and cathode, respectively; dotted magenta: 232Th in the vessel.Prior to the EXO experiment no observation of the two-neutrino double beta decay mode had been reported although there were two reports of studies which produced only upper limits for the decay rate [29, 30]. The reported bounds were of concern because they suggested that the two-neutrino decay of 136Xe was anomalously low. The EXO collaboration first reported a clear observation of the two neutrino decay mode in 2011 [31]. The rate seen was considerably higher than the limits previously reported and reflects the advantages of a large mass, very low background detector. The EXO results were confirmed by the KAMLAND-ZEN team shortly after [24]. In a paper recently submitted for publication, the EXO group have presented a fuller analysis where several of the systematic errors have been reduced to provide the highest precision measure of a two-neutrino double beta decay. The final result is a half-life of 2.172±0.017 (stat) ± 0.060 (sys) × 1021 years [32].


## 5.2. Search for Zero Neutrino Decays of136Xe

The primary aim of the EXO project is the search for neutrino-less decay of136Xe. The signature of such a decay would be a peak in the total deposited energy spectrum at the decay Q value. The EXO-200 first search for this decay mode was published in 2012 [27] where details of the analysis may be found. The data are displayed in Figure 4. Critical to the search for the neutrino-less decay is the separation between gamma backgrounds and the signal through the multisite/single site discrimination. No evidence for neutrino-less decay is observed.As discussed in [27], the analysis of these data gives a bound on the possible neutrinoless double beta decay of 136Xe T>1.6×1025 years at 90% confidence. To extract a corresponding limit to the neutrino mass, one needs to choose a nuclear matrix element. For recently published values using generator coordinate method [33], nuclear shell model [34], interacting boson model [35], RQRPA [36], and the QRPA-2 [37], the mass limit is 140–380 meV.There has been a claim of observation of neutrinoless double beta decay in germanium [38]. In order to compare the EXO limits to expectations for germanium, one uses the relative matrix elements from a set of calculations. The results are displayed in Figure 5. Clearly the measurement from EXO does not support the previous claim. Again, the EXO result has been confirmed by Gando et al. [39].Figure 5
This figure compares the expected half-lives of136Xe and 76Ge for matrix elements from various models. References for the models are found in the text.


## 6. General Discussion of Strengths of the Liquid Xenon Detection and Future Directions

The EXO-200 experiment has provided world-leading measures of two-neutrino double beta decay and limits for neutrino-less decay of136Xe. There are a number of reasons for this success. Clearly, a large mass detector is essential for a low decay rate study, but the EXO design offers a unique suite of advantages. The precision measure is in part due to the highly homogeneous nature of the detector. This allows very tight control on the systematic errors. The rejection of the gamma background arises first from the choice of very clean materials, second from the ability to determine the full structure of the events and thus discriminate against gamma rays that tend to Compton scatter, and finally from the ability to set a fiducial boundary inside the xenon mass. The background is qualitatively different from that found for germanium or tellurium experiments in that, as can be seen from Figure 5, there is very little continuum beneath the peak region. Instead, we need to reject two discrete gamma activities (2448 keV from 214Bi and the 2505 keV sum peak from 60Co) with energies very close to Qββ together with the tail of the 2614 keV gamma line from thorium. Improved rejection of all of these backgrounds will likely come from better single site/multisite discrimination, whereas better energy resolution will benefit mainly the 2614 rejection. Significant improvements to the multi-site identification look possible.


## 7. The Future

Many of the detector concepts and implementation in EXO-200 are readily scalable to a much larger sensitive mass of xenon. Indeed, the critical self-shielding improves with larger mass. With the extremely high purity level demonstrated for xenon, it should be possible to cover the inverted hierarchy in a sufficiently large detector. The EXO collaboration is planning a new, next generation detector using 5 tonnes of enriched xenon. The detector would be placed in a large water shield instead of the lead shield used for EXO-200 and a deeper site would be chosen to reduce the cosmogenic neutron backgrounds. The plan is to run initially without a barium tag but to design the facility so that such a tag could be implemented at a later time. Many physics and engineering studies are underway to explore the full capability of such a detector, but it is clear that such a detector would allow a very substantial advance in the sensitivity to a Majorana neutrino mass and, with a barium tag, it would be possible to cover the entire inverted hierarchy parameter space. This is clearly the next milestone in this exciting area of research. Much work remains to be done, but it seems reasonable to think that this exciting project could be ready to start data taking a decade from now.



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