Bulletin of the American Physical Society
2023 APS April Meeting
Volume 68, Number 6
Minneapolis, Minnesota (Apr 15-18)
Virtual (Apr 24-26); Time Zone: Central Time
Session T15: Mini-Symposium: Quantum Information and Quantum SensingMini-Symposium
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Sponsoring Units: DNP DPF DCOMP Chair: Walter Pettus, Indiana Univ - Bloomington Room: Marquette VII - 2nd Floor |
Tuesday, April 18, 2023 10:45AM - 11:21AM |
T15.00001: TBD Invited Speaker: Douglas H Beck
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Tuesday, April 18, 2023 11:21AM - 11:33AM |
T15.00002: Visualizing a Multi-Qubit State; an Extension of the Bloch Sphere Jacob Stuligross The conventional visualization of a single qubit is the Bloch sphere, which has proven to be a successful tool for developing intuition. In addition to showing all the information of an arbitrary state, the Bloch sphere clearly depicts the effect of any 1-qubit gate. Unfortunately, the generalization to multiple qubits is nontrivial. Since nearly all of quantum computing is derived from interactions between qubits, a visualization of multi-qubit states which have similar geometric intuitions to the Bloch sphere would be an effective pedagogical tool. Since any n-qubit gate can be decomposed into combinations of 1- and 2-qubit gates, an intuitive 2-qubit state visualization would be incredibly useful in developing understanding of quantum algorithms. |
Tuesday, April 18, 2023 11:33AM - 11:45AM |
T15.00003: Receiver Noise Characterization for ADMX Run 1C-Extended Michaela Guzzetti The axion was originally proposed as a solution to the strong CP problem, however, it has been gaining popularity in recent years as a cold dark matter candidate. Many find the DFSZ axion model to be more compelling than its counterpart (KSVZ), due to its GUT compatibility. However, the DFSZ axion is significantly more weakly coupled to photons than the KSVZ axion, making it more difficult to detect. Notably, the Axion Dark Matter eXperiment (ADMX) was the first axion haloscope to reach sensitivity to the elusive DFSZ axion. ADMX was able to reach DFSZ sensitivity by using a dilution refrigerator to keep physical temperatures low, as well as employing low-noise quantum electronics to minimize receiver noise. To date, ADMX has excluded axion-photon couplings predicted by the KSVZ (DFSZ) model for the axion between 2.66-4.2 μeV (2.66-3.3 μeV & 3.9-4.1 μeV). Over the last year ADMX has been taking data designed to bridge the gap in DFSZ sensitivity for regions in the 3.3 to 3.9 μeV range. In this talk, I will be discussing the receiver noise calibration procedures used for this dataset. In particular, I will discuss the different types of measurements taken, as well as the noise models and analysis strategies used on said measurements. |
Tuesday, April 18, 2023 11:45AM - 11:57AM |
T15.00004: Reducing phonon backgrounds for quantum computing and cryogenic calorimeters Xinran Li, Maurice A Garcia-Sciveres, Aritoki Suzuki Superconducting qubits suffer from decoherence caused by phonons in the substrate with energies higher than the superconducting bandgap. While radiation backgrounds and cosmic rays produce large bursts of athermal phonons that causes catastrophic whole-chip failures, other sources, such as stress in films and chip packaging, produce lower energy phonon bursts more frequently. Cryogenic calorimetric sensors have achieved similar sensitivities to these phonon events. Specifically, in transition edge sensor (TES) based dark matter detectors, these events are the limiting background for low-mass dark matter searches. |
Tuesday, April 18, 2023 11:57AM - 12:09PM |
T15.00005: Fundamental Physics Tests with Precision Acoustic Sensors Michael E Tobar, William M Campbell, Maxim Goryachev Crystalline bulk acoustic wave (BAW) resonators provide a high precision architecture for fundamental physics experiments that search for signatures of beyond the standard model physics. In this work we present an overview of recent experiments that exploit the advantageous metrological properties of quartz BAW resonators in order to test quantum gravity, as well as search for high frequency gravitational waves. Utilizing these resonators, we have improved upon existing constraints on the scale of a discrete minimum length, as |
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