Kent D. Irwin

Searches for QCD axions with masses in the n eV / c 2 mass range are strongly motivated by new physics at the grand unified theory (GUT) scale and by well-motivated preinflationary axion symmetry breaking scales. This parameter space is challenging to probe due to the small axion-photon couplings, which typically require large, high-field magnets with substantial stored energy. In this paper, we propose a new experimental geometry based on a narrow-bore, segmented solenoid that optimizes the collection of the axion-induced signal using LC resonators outside the high-field region of the magnet bore. This alternative optimization significantly reduces the required stored magnetic energy while preserving sensitivity, thus enabling a near-term experiment in the 30–200 MHz ( 120 − 830 n eV / c 2 ) range, with a cost-effective, staged scaling to a GUT-scale experiment in the 100 kHz–30 MHz ( 0.4 − 120 n eV / c 2 ) range.

The BICEP/Keck collaboration searches for B-mode polarization in the Cosmic Microwave Background (CMB) as evidence of inflationary gravitational waves, with current best constraints placing $r_{0.05} < 0.035$. Building even deeper and larger maps requires scaling detector count at 150 GHz, where B-mode power is expected to peak at $\ell \sim 80$. The BICEP Array 150 GHz receiver (BA150) fields 7776 superconducting transition edge sensor (TES) detectors, over 15× the 512 deployed in the previous BICEP/Keck 150 GHz receiver, making it the densest time-division multiplexed readout receiver in the collaboration's history. We present the complete detector characterization of all 12 detector modules as deployed in BA150. We report thermal properties ($T_{c}$, $G_{c}$, $P_\rm{sat}$), end-to-end optical efficiencies of 20–48%, and fractional bandwidths of $\sim$28% across all modules. We additionally report the identification and mitigation of an out-of-band high-frequency photon leak spanning 180–265 GHz, and present preliminary investigations of elevated on-sky noise attributed to aliased high-frequency detector noise.

High-temperature high-pressure (HPHT) nanoscale diamond (ND) is a host of the nitrogen vacancy (NV) center, a quantum bit that allows for a wide range of quantum sensing capabilities including magnetometry, electrometry and thermometry using all-optical techniques at room temperature. Yet challenges remain in diversifying the chemical modalities for covalent bond formation on diamond surfaces, which is typically limited to carboxylate-based chemistry but has been recently expanded. Amine termination of diamond is attractive due to theoretical studies that described the removal of mid-gap states, which results in extended electron-spin coherence times. Chemical activation of alcohol terminated NDs into alkyl-bromides (ND-Br) using SOBr2 has been shown to be a successful strategy. The alkyl bromide is a good leaving group that forms a carbocation intermediate to generate new bonds and has previously been used to form simple amine termination. Here we test the ability of larger amine molecules to generate covalent diamond-nitrogen bonds on the sterically hindered surface. In this update, we react ND-Br with branched, linear and cyclic amines including polyethyleneimine, diethylenetriamine and melamine, a triazine derivative used in “magic eraser” products and antibacterial products. A suite of X-ray spectroscopies was employed to verify the successful amination and probe the diamond-amine electronic structure. These results expand the routes for researchers who wish to chemically tune diamond and modify the surface dipole moment and electron affinity for quantum sensing applications with atomic defects.

We present power spectra of the cosmic microwave background (CMB) anisotropy in temperature and polarization, measured from the Data Release 6 maps made from Atacama Cosmology Telescope (ACT) data. These cover 19,000 deg ² of sky in bands centered at 98, 150 and 220 GHz, with white noise levels three times lower than Planck in polarization. We find that the ACT angular power spectra estimated over 10,000 deg ² , and measured to arcminute scales in TT, TE and EE, are well fit by the sum of CMB and foregrounds, where the CMB spectra are described by the ΛCDM model. Combining ACT with larger-scale Planck data, the joint P-ACT dataset provides tight limits on the ingredients, expansion rate, and initial conditions of the universe. We find similar constraining power, and consistent results, from either the Planck power spectra or from ACT combined with WMAP data, as well as from either temperature or polarization in the joint P-ACT dataset. When combined with CMB lensing from ACT and Planck , and baryon acoustic oscillation data from the Dark Energy Spectroscopic Instrument (DESI DR1), we measure a baryon density of Ω _b h ² = 0.0226 ± 0.0001, a cold dark matter density of Ω _c h ² = 0.118 ± 0.001, a Hubble constant of H ₀ = 68.22 ± 0.36 km/s/Mpc, a spectral index of n _s = 0.974 ± 0.003, and an amplitude of density fluctuations of σ ₈ = 0.813 ± 0.005. Including the DESI DR2 data tightens the Hubble constant to H ₀ = 68.43 ± 0.27 km/s/Mpc; ΛCDM parameters agree between the P-ACT and DESI DR2 data at the 1.6 σ level. We find no evidence for excess lensing in the power spectrum, and no departure from spatial flatness. The contribution from Sunyaev-Zel'dovich (SZ) anisotropy is detected at high significance; we find evidence for a tilt with suppressed small-scale power compared to our baseline SZ template spectrum, consistent with hydrodynamical simulations with feedback.

We present Atacama Cosmology Telescope (ACT) Data Release 6 (DR6) maps of the Cosmic Microwave Background temperature and polarization anisotropy at arcminute resolution over three frequency bands centered on 98, 150 and 220 GHz. The maps are based on data collected with the AdvancedACT camera over the period 2017–2022 and cover 19,000 square degrees with a median combined depth of 10 μK arcmin. We describe the instrument, mapmaking and map properties and illustrate them with a number of figures and tables. The ACT DR6 maps and derived products are available on LAMBDA at https://lambda.gsfc.nasa.gov/product/act/actadv_prod_table.html . We also provide an interactive web atlas at https://phy-act1.princeton.edu/public/snaess/actpol/dr6/atlas and HiPS data sets in Aladin (e.g. https://alasky.cds.unistra.fr/ACT/DR4DR6/color_CMB ).

We use new cosmic microwave background (CMB) primary temperature and polarization anisotropy measurements from the Atacama Cosmology Telescope (ACT) Data Release 6 (DR6) to test foundational assumptions of the standard cosmological model, ΛCDM, and set constraints on extensions to it. We derive constraints from the ACT DR6 power spectra alone, as well as in combination with legacy data from the Planck mission. To break geometric degeneracies, we include ACT and Planck CMB lensing data and baryon acoustic oscillation data from DESI Year-1. To test the dependence of our results on non-ACT data, we also explore combinations replacing Planck with WMAP and DESI with BOSS, and further add supernovae measurements from Pantheon+ for models that affect the late-time expansion history. We verify the near-scale-invariance (running of the spectral index dn _s / d ln k = 0.0062 ± 0.0052) and adiabaticity of the primordial perturbations. Neutrino properties are consistent with Standard Model predictions: we find no evidence for new light, relativistic species that are free-streaming ( N _eff = 2.86 ± 0.13, which combined with astrophysical measurements of primordial helium and deuterium abundances becomes N _eff = 2.89 ± 0.11), for non-zero neutrino masses (∑ m _ν < 0.089 eV at 95% CL), or for neutrino self-interactions. We also find no evidence for self-interacting dark radiation ( N _idr < 0.134), or for early-universe variation of fundamental constants, including the fine-structure constant ( α _EM / α _EM,0 = 1.0043 ± 0.0017) and the electron mass ( m _e / m _e,0 = 1.0063 ± 0.0056). Our data are consistent with standard big bang nucleosynthesis (we find Y _p = 0.2312 ± 0.0092), the COBE/FIRAS -inferred CMB temperature (we find T _CMB = 2.698 ± 0.016 K), a dark matter component that is collisionless and with only a small fraction allowed as axion-like particles, a cosmological constant ( w = -0.986 ± 0.025), and the late-time growth rate predicted by general relativity ( γ = 0.663 ± 0.052). We find no statistically significant preference for a departure from the baseline ΛCDM model. In fits to models invoking early dark energy, primordial magnetic fields, or an arbitrary modified recombination history, we find H ₀ = 69.9 ^+0.8 _-1.5 , 69.1 ± 0.5, or 69.6 ± 1.0 km/s/Mpc, respectively; using BOSS instead of DESI BAO data reduces the central values of these constraints by 1–1.5 km/s/Mpc while only slightly increasing the error bars. In general, models introduced to increase the Hubble constant or to decrease the amplitude of density fluctuations inferred from the primary CMB are not favored over ΛCDM by our data.

We present the limits on noise for the readout of cryogenic high-Q resonators using dc Superconducting Quantum Interference Devices (SQUIDs) below 300 MHz. This analysis uses realized first-stage SQUIDs (previously published), whose performance is well described by Tesche–Clarke (TC) theory, coupled directly to the resonators. We also present data from a prototype second-stage dc SQUID array designed to couple to this first-stage SQUID as a follow-on amplifier with high system bandwidth. This analysis is the first full consideration of dc SQUID noise performance referred to a high-Q resonator over this frequency range and is presented relative to the standard quantum limit. We include imprecision, backaction, and backaction–imprecision noise correlations from TC theory, the noise contributed by the second-stage SQUIDs, wiring, and preamplifiers, and optimizations for both on-resonance measurements and off-resonance scan sensitivity. This architecture has modern relevance due to the increased interest in axion searches and the requirements of the DMRadio-m3 axion search, which uses dc SQUIDs in this frequency range.

DMRadio- m 3 is an experimental search for dark matter axions. It uses a solenoidal dc magnetic field to convert an axion dark-matter signal to an ac electromagnetic response in a coaxial copper pickup. The current induced by this axion signal is measured by dc SQUIDs. DMRadio- m 3 is designed to be sensitive to Kim-Shifman-Vainshtein-Zakharov (KSVZ) and Dine-Fischler-Srednicki-Zhitnisky (DFSZ) QCD axion models in the 10–200 MHz ( 41 neV / c 2 – 0.83 μ eV / c 2 ) range, and to axions with g a γ γ = g a γ γ , DFSZ ( 30 MHz ) = 1.87 × 10 − 17 GeV − 1 over 5–30 MHz as an extended goal. In this work, we present the electromagnetic modeling of the response of the experiment to an axion signal over the full frequency range of DMRadio- m 3 , which extends from the low-frequency, lumped-element limit to a regime where the axion Compton wavelength is only a factor of 2 larger than the detector size. With these results, we determine the live time and sensitivity of the experiment. The primary science goal of sensitivity to DFSZ axions across 30–200 MHz can be achieved with a 3 σ live scan time of 2.9 years.

We present Atacama Cosmology Telescope (ACT) Data Release 6 (DR6) maps of the Cosmic Microwave Background temperature and polarization anisotropy at arcminute resolution over three frequency bands centered on 98, 150 and 220 GHz. The maps are based on data collected with the AdvancedACT camera over the period 2017--2022 and cover 19,000 square degrees with a median combined depth of 10 uK arcmin. We describe the instrument, mapmaking and map properties and illustrate them with a number of figures and tables. The ACT DR6 maps and derived products are available on LAMBDA at https://lambda.gsfc.nasa.gov/product/act/actadv_prod_table.html. We also provide an interactive web atlas at https://phy-act1.princeton.edu/public/snaess/actpol/dr6/atlas and HiPS data sets in Aladin (e.g. https://alasky.cds.unistra.fr/ACT/DR4DR6/color_CMB).

We present the RF Quantum Upconverter (RQU) and describe its application to quantum metrology of electromagnetic modes between dc and the very high frequency band (VHF) ( ≲ 300 MHz). The RQU uses a Josephson interferometer made up of superconducting loops and Josephson junctions to implement a parametric interaction between a low-frequency electromagnetic mode (between dc and VHF) and a mode in the microwave C Band ( ∼ 5 GHz), analogous to the radiation pressure interaction between electromagnetic and mechanical modes in cavity optomechanics. We analyze RQU performance with quantum amplifier theory and show that the RQU can operate as a quantum-limited op-amp in this frequency range. It can also use nonclassical measurement protocols equivalent to those used in cavity optomechanics, including back-action evading (BAE) measurements, sideband cooling, and two-mode squeezing. These protocols enable experiments using dc VHF electromagnetic modes as quantum sensors with sensitivity better than the standard quantum limit (SQL). We demonstrate signal upconversion from low frequencies to the microwave C band using an RQU and show a phase-sensitive gain (extinction ratio) of 46.9 dB , which is a necessary step towards the realization of full BAE.