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arXiv 2608.27556physics.ins-detastro-ph.COhep-ex

用于宏观低温量热计阵列的微波SQUID多路复用概念

A microwave SQUID multiplexing concept for macro-cryogenic calorimeter arrays

N. Ferreiro Iachellini, P. Szypryt, L. Canonica, W. B. Doriese, M. Durkin, A. Giachero, J. A. B. Mates, A. Nucciotti, L. Pattavina, S. Quitadamo, C. Shiu, J. N.… 展开作者

N. Ferreiro Iachellini, P. Szypryt, L. Canonica, W. B. Doriese, M. Durkin, A. Giachero, J. A. B. Mates, A. Nucciotti, L. Pattavina, S. Quitadamo, C. Shiu, J. N. Ullom, M. R. Vissers

AI总结:

本研究提出将微波SQUID多路复用(μMUX)技术应用于大规模低温量热计阵列,推导了其噪声模型,显示该技术可在多路复用因子达1000时劣化分辨率不足2%,适用于CEνNS和暗物质搜寻的多塔阵列单元设计。

AI中文摘要:

由过渡-edge传感器(TES)读出的大规模低温量热计可达到电子伏特级的基线分辨率,但在稀有事例搜寻中传统使用的单通道直流SQUID读出方式,每个探测器搭配一条放大器链和数根导线,使得实用阵列仅能容纳几十个通道。我们提出将为快速X射线和中微子质量微量热计开发的微波SQUID多路复用(μMUX)技术,应用于工作在约20mK的大规模BGO(Bi₄Ge₃O₁₂)量热计;蓝宝石和TeO₂吸收体也可采用同一套方案。基于已有的大规模TES量热计的热与噪声模型,我们推导了多路复用读出的噪声模型,其包含高电子迁移率晶体管(HEMT)、两能级系统及SQUID的贡献,以及噪声随多路复用因子Nₘᵤₓ的缩放关系。由于热信号变化缓慢,每个通道仅需约千赫兹的采样率,因此限制要求并非带宽,而是输入线圈灵敏度需达到(0.1至1)μA/Φ₀,这一数值比当前的μMUX器件高出10至30倍,与探测器电流噪声(9至10)pA/√Hz相匹配,该噪声与吸收体质量无关。在总通量噪声约为1.2μΦ₀/√Hz的情况下,当Nₘᵤₓ达到1000时,该读出方式对基线分辨率的劣化小于2%,与TES限制的分辨率相比可忽略不计。这些结果被应用于单塔设计:52块100克的BGO晶体和1个HEMT放大器。该塔是多塔阵列的单元,总质量达数千克,旨在用于相干中微子原子核散射(CEνNS)和暗物质搜寻。

英文摘要:

Massive cryogenic calorimeters read out by transition-edge sensors (TES) can reach eV-scale baseline resolution, but the single-channel dc-SQUID readout conventionally used in rare-event searches, with one amplifier chain and several wires per detector, limits practical arrays to a few tens of channels. We propose to apply microwave SQUID multiplexing ($μ$MUX), developed for fast X-ray and neutrino-mass microcalorimeters, to massive BGO (Bi$_4$Ge$_3$O$_{12}$) calorimeters operated at $\simeq 20$~mK; sapphire and TeO$_2$ absorbers are covered by the same framework. Using the established thermal and noise model for massive TES calorimeters, we derive a noise model for the multiplexed readout, including the HEMT, two-level-system and SQUID contributions, and its scaling with the multiplexing factor $N_{\rm mux}$. Since the slow thermal signals require only about a kHz of sampling per channel, the limiting requirement is not bandwidth but an input-coil sensitivity of $( 0.1$ to $1)\,μ$A$/Φ_0$, a factor of $10$ to $30$ beyond current $μ$MUX devices, matched to the detector current noise of ($9$ to $10$)~pA$/\sqrt{\rm Hz}$, which is independent of the absorber mass. With a total flux noise of $\simeq$$1.2\,μΦ_0/\sqrt{\rm Hz}$, the readout degrades the baseline resolution by less than $2\%$ up to $N_{\rm mux}=1000$, negligible compared with the TES-limited resolution. These results are implemented in a single-tower design: 52 BGO crystals of 100~g each and one HEMT amplifier. The tower is the unit of a multi-tower array of several kilograms aimed at CE$ν$NS and dark matter searches.

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