论文标题
确定过热C $ _3 $ f $ _8 $暗物质检测器的低能核后坐力的气泡成核效率
Determining the bubble nucleation efficiency of low-energy nuclear recoils in superheated C$_3$F$_8$ dark matter detectors
论文作者
论文摘要
过热液体中低能核后坐力的气泡成核效率在解释直接搜索弱相互作用的大粒子(WIMP)暗物质的结果中起着至关重要的作用。 PICO合作介绍了来自碳和氟氟后乘的气泡成核的结果,该碳和氟后坐力在过热的C $ _3 $ _3 $ f $ _8 $中,从校准数据中,在各种热力学阈值范围为2.1 KeV到3.9 KEV的各种热力学阈值,在各种热力学阈值下获得5个不同的中子光谱。提出了一个通用的分段线性模型,而不是假设任何特定的功能形式,而是以系统的误差为滋扰参数,以最大程度地减少模型引入的不确定性。马尔可夫链蒙特卡洛(MCMC)例程用于在2.45 KEV和3.29 KEV热力学阈值时对氟和碳的核反冲效率进行采样。 The nucleation efficiency for fluorine was found to be $\geq 50\, \%$ for nuclear recoils of 3.3 keV (3.7 keV) at a thermodynamic Seitz threshold of 2.45 keV (3.29 keV), and for carbon the efficiency was found to be $\geq 50\, \%$ for recoils of 10.6 keV (11.1 keV) at a threshold of 2.45 KEV(3.29 KEV)。模拟数据集用于计算拟合的p值,证实所使用的模型与数据兼容。还评估了拟合范式的潜在系统偏见,尽管该偏见很小,但已被校正。执行其他步骤来计算PICO-60检测器中WIMP的预期相互作用速率,这是计算WIMP排除限制的要求。
The bubble nucleation efficiency of low-energy nuclear recoils in superheated liquids plays a crucial role in interpreting results from direct searches for weakly interacting massive particle (WIMP) dark matter. The PICO Collaboration presents the results of the efficiencies for bubble nucleation from carbon and fluorine recoils in superheated C$_3$F$_8$ from calibration data taken with 5 distinct neutron spectra at various thermodynamic thresholds ranging from 2.1 keV to 3.9 keV. Instead of assuming any particular functional forms for the nuclear recoil efficiency, a generalized piecewise linear model is proposed with systematic errors included as nuisance parameters to minimize model-introduced uncertainties. A Markov-Chain Monte-Carlo (MCMC) routine is applied to sample the nuclear recoil efficiency for fluorine and carbon at 2.45 keV and 3.29 keV thermodynamic thresholds simultaneously. The nucleation efficiency for fluorine was found to be $\geq 50\, \%$ for nuclear recoils of 3.3 keV (3.7 keV) at a thermodynamic Seitz threshold of 2.45 keV (3.29 keV), and for carbon the efficiency was found to be $\geq 50\, \%$ for recoils of 10.6 keV (11.1 keV) at a threshold of 2.45 keV (3.29 keV). Simulated data sets are used to calculate a p-value for the fit, confirming that the model used is compatible with the data. The fit paradigm is also assessed for potential systematic biases, which although small, are corrected for. Additional steps are performed to calculate the expected interaction rates of WIMPs in the PICO-60 detector, a requirement for calculating WIMP exclusion limits.