CAL-Pathfinder

Cal Axion LC (CAL-Pathfinder) is a lumped-element detector searching for axions in the 0.45 - 0.55 μeV mass range, corresponding to frequencies around 100 MHz. CAL-Pathfinder will not only be sensitive to an unexplored range of axion masses, but will also serve as a testbed for experimental techniques required for future, more sensitive lumped-element detectors. The experiment will demonstrate the feasability of the solenoid magnet geometry and be a platform for testing SQUID amplifiers designed to operated at these frequencies.

Coaxial pickup assembly
Coaxial pickup assembly. The inductive pickup hangs from the mixing chamber of the dilution refrigerator and sits within the magnet bore.

Detection Principle

CAL-Pathfinder relies on the lumped-element technique for axion detection. A 9 T solenoidal superconducting magnet is attached to a Bluefors LD400 dilution refrigerator. An inductive, coaxial pickup hangs off the mixing chamber of the dilution fridge and resides within the bore of the magnet. Attached to the pickup is a tunable capacitor. Axion interactions with the magnetic field induce a current on the surface of the pickup. These induced currents travel through the LC circuit formed by the pickup and capacitor and are read out by a DC SQUID amplifier chain. The pickup, capacitor, and SQUID amplifiers all operate at temperatures near 20 mK.

Tuner assembly
Tunable capacitor test stand. The tunable capacitor sets the LC resonant frequency and allows the experiment to scan across a range of axion masses.
Coaxial pickup before superconducting coating
Coaxial pickup before copper coating is applied.
Cryogenic SQUID amplifier chain
Cryogenic RF amplifier used as part of cold readout, further amplifies the output signal from the SQUIDs (not pictured)

Explore the Experiment

CAL-Pathfinder experiment diagram
Magnet
Coaxial pickup
Cryogenic System
SQUIDs
Low-field box
Tunable capacitor

Click a + to learn about each component.


Sources

  1. V. Ankel et al., "Noise limits for dc SQUID readout of high-Q resonators below 300 MHz," J. Appl. Phys. 138, 094505 (2025) — 10.1063/5.0280831

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