Measurement of the Positive Muon Anomalous Magnetic Moment to 0.46 ppm

(2021)

Authors:

B Abi, T Albahri, S Al-Kilani, D Allspach, LP Alonzi, A Anastasi, A Anisenkov, F Azfar, K Badgley, S Baeßler, I Bailey, VA Baranov, E Barlas-Yucel, T Barrett, E Barzi, A Basti, F Bedeschi, A Behnke, M Berz, M Bhattacharya, HP Binney, R Bjorkquist, P Bloom, J Bono, E Bottalico, T Bowcock, D Boyden, G Cantatore, RM Carey, J Carroll, BCK Casey, D Cauz, S Ceravolo, R Chakraborty, SP Chang, A Chapelain, S Chappa, S Charity, R Chislett, J Choi, Z Chu, TE Chupp, ME Convery, A Conway, G Corradi, S Corrodi, L Cotrozzi, JD Crnkovic, S Dabagov, PM De Lurgio, PT Debevec, S Di Falco, P Di Meo, G Di Sciascio, R Di Stefano, B Drendel, A Driutti, VN Duginov, M Eads, N Eggert, A Epps, J Esquivel, M Farooq, R Fatemi, C Ferrari, M Fertl, A Fiedler, AT Fienberg, A Fioretti, D Flay, SB Foster, H Friedsam, E Frlež, NS Froemming, J Fry, C Fu, C Gabbanini, MD Galati, S Ganguly, A Garcia, DE Gastler, J George, LK Gibbons, A Gioiosa, KL Giovanetti, P Girotti, W Gohn, T Gorringe, J Grange, S Grant, F Gray, S Haciomeroglu, D Hahn, T Halewood-Leagas, D Hampai, F Han, E Hazen, J Hempstead, S Henry, AT Herrod, DW Hertzog, G Hesketh, A Hibbert, Z Hodge, JL Holzbauer, KW Hong, R Hong, M Iacovacci, M Incagli, C Johnstone, JA Johnstone, P Kammel, M Kargiantoulakis, M Karuza, J Kaspar, D Kawall, L Kelton, A Keshavarzi, D Kessler, KS Khaw, Z Khechadoorian, NV Khomutov, B Kiburg, M Kiburg, O Kim, SC Kim, YI Kim, B King, N Kinnaird, M Korostelev, I Kourbanis, E Kraegeloh, VA Krylov, A Kuchibhotla, NA Kuchinskiy, KR Labe, J LaBounty, M Lancaster, MJ Lee, S Lee, S Leo, B Li, D Li, L Li, I Logashenko, A Lorente Campos, A Lucà, G Lukicov, G Luo, A Lusiani, AL Lyon, B MacCoy, R Madrak, K Makino, F Marignetti, S Mastroianni, S Maxfield, M McEvoy, W Merritt, AA Mikhailichenko, JP Miller, S Miozzi, JP Morgan, WM Morse, J Mott, E Motuk, A Nath, D Newton, H Nguyen, M Oberling, R Osofsky, J-F Ostiguy, S Park, G Pauletta, GM Piacentino, RN Pilato, KT Pitts, B Plaster, D Počanić, N Pohlman, CC Polly, M Popovic, J Price, B Quinn, N Raha, S Ramachandran, E Ramberg, NT Rider, JL Ritchie, BL Roberts, DL Rubin, L Santi, D Sathyan, H Schellman, C Schlesier, A Schreckenberger, YK Semertzidis, YM Shatunov, D Shemyakin, M Shenk, D Sim, MW Smith, A Smith, AK Soha, M Sorbara, D Stöckinger, J Stapleton, D Still, C Stoughton, D Stratakis, C Strohman, T Stuttard, HE Swanson, G Sweetmore, DA Sweigart, MJ Syphers, DA Tarazona, T Teubner, AE Tewsley-Booth, K Thomson, V Tishchenko, NH Tran, W Turner, E Valetov, D Vasilkova, G Venanzoni, VP Volnykh, T Walton, M Warren, A Weisskopf, L Welty-Rieger, M Whitley, P Winter, A Wolski, M Wormald, W Wu, C Yoshikawa

Measurement of the positive muon anomalous magnetic moment to 0.46 ppm

Physical Review Letters American Physical Society 126 (2021) 141801

Authors:

B Abi, Farrukh Azfar, S Henry

Abstract:

We present the first results of the Fermilab National Accelerator Laboratory (FNAL) Muon g−2 Experiment for the positive muon magnetic anomaly aμ≡(gμ−2)/2. The anomaly is determined from the precision measurements of two angular frequencies. Intensity variation of high-energy positrons from muon decays directly encodes the difference frequency ωa between the spin-precession and cyclotron frequencies for polarized muons in a magnetic storage ring. The storage ring magnetic field is measured using nuclear magnetic resonance probes calibrated in terms of the equivalent proton spin precession frequency ˜ω′p in a spherical water sample at 34.7 °C. The ratio ωa/˜ω′p, together with known fundamental constants, determines aμ(FNAL)=116592040(54)×10−11 (0.46 ppm). The result is 3.3 standard deviations greater than the standard model prediction and is in excellent agreement with the previous Brookhaven National Laboratory (BNL) E821 measurement. After combination with previous measurements of both μ+ and μ−, the new experimental average of aμ(Exp)=116592061(41)×10−11 (0.35 ppm) increases the tension between experiment and theory to 4.2 standard deviations.

The LOFAR Two-Meter Sky Survey: Deep Fields Data Release 1 I. Direction-dependent calibration and imaging

Astronomy and Astrophysics EDP Sciences 648:2021 (2021) A1

Authors:

C Tasse, T Shimwell, Mj Hardcastle, Sp O'Sullivan, R van Weeren, Pn Best, L Bester, B Hugo, O Smirnov, J Sabater, G Calistro-Rivera, F de Gasperin, Lk Morabito, H Roettgering, Wl Williams, M Bonato, M Bondi, A Botteon, M Brueggen, G Brunetti, Kt Chyzy, Ma Garrett, G Guerkan, Mj Jarvis, R Kondapally, S Mandal, I Prandoni, A Repetti, E Retana-Montenegro, Dj Schwarz, A Shulevski, Y Wiaux

Abstract:

The Low Frequency Array (LOFAR) is an ideal instrument to conduct deep extragalactic surveys. It has a large field of view and is sensitive to large-scale and compact emission. It is, however, very challenging to synthesize thermal noise limited maps at full resolution, mainly because of the complexity of the low-frequency sky and the direction dependent effects (phased array beams and ionosphere). In this first paper of a series, we present a new calibration and imaging pipeline that aims at producing high fidelity, high dynamic range images with LOFAR High Band Antenna data, while being computationally efficient and robust against the absorption of unmodeled radio emission. We apply this calibration and imaging strategy to synthesize deep images of the Boötes and Lockman Hole fields at ~150 MHz, totaling ~80 and ~100 h of integration, respectively, and reaching unprecedented noise levels at these low frequencies of â 30 and â 23 μJy beam-1 in the inner ~3 deg2. This approach is also being used to reduce theâ» LOTSS-wide data for the second data release.

The LOFAR Two-meter Sky Survey: Deep Fields Data Release 1 III. Host-galaxy identifications and value added catalogues

Astronomy and Astrophysics EDP Sciences 648:2021 (2021) A3

Authors:

R Kondapally, Pn Best, Mj Hardcastle, D Nisbet, M Bonato, J Sabater, Kj Duncan, I McCheyne, Rk Cochrane, Raa Bowler, Wl Williams, Tw Shimwell, C Tasse, Jh Croston, A Goyal, M Jamrozy, Mj Jarvis, Vh Mahatma, Hja Roettgering, Djb Smith, A Wolowska, M Bondi, M Brienza, Mji Brown, M Brueggen, K Chambers, Ma Garrett, G Guerkan, M Huber, M Kunert-Bajraszewska, E Magnier, B Mingo, R Mostert, B Nikiel-Wroczynski, Sp O'Sullivan, R Paladino, T Ploeckinger, I Prandoni, Mj Rosenthal, Dj Schwarz, A Shulevski, Jd Wagenveld, L Wang

Abstract:

We present the source associations, cross-identifications, and multi-wavelength properties of the faint radio source population detected in the deep tier of the LOFAR Two Metre Sky Survey (LoTSS): the LoTSS Deep Fields. The first LoTSS Deep Fields data release consists of deep radio imaging at 150 MHz of the ELAIS-N1, Lockman Hole, and Boötes fields, down to RMS sensitives of around 20, 22, and 32 μJy beam-1, respectively. These fields are some of the best studied extra-galactic fields in the northern sky, with existing deep, wide-area panchromatic photometry from X-ray to infrared wavelengths, covering a total of ≈26 deg2. We first generated improved multi-wavelength catalogues in ELAIS-N1 and Lockman Hole; combined with the existing catalogue for Boötes, we present forced, matched aperture photometry for over 7.2 million sources across the three fields. We identified multi-wavelength counterparts to the radio detected sources, using a combination of the Likelihood Ratio method and visual classification, which greatly enhances the scientific potential of radio surveys and allows for the characterisation of the photometric redshifts and the physical properties of the host galaxies. The final radio-optical cross-matched catalogue consists of 81 951 radio-detected sources, with counterparts identified and multi-wavelength properties presented for 79 820 (>97%) sources. We also examine the properties of the host galaxies, and through stacking analysis find that the radio population with no identified counterpart is likely dominated by active galactic nuclei (AGN) at z ~ 3-4. This dataset contains one of the largest samples of radio-selected star-forming galaxies and AGN at these depths, making it ideal for studying the history of star-formation, and the evolution of galaxies and AGN across cosmic time.

The LOFAR Two-meter Sky Survey: Deep fields data release 1: IV. Photometric redshifts and stellar masses

Astronomy and Astrophysics EDP Sciences 648 (2021) A4

Authors:

Kj Duncan, R Kondapally, Mji Brown, M Bonato, Pn Best, Hja Roettgering, M Bondi, Raa Bowler, Rk Cochrane, G Guerkan, Mj Hardcastle, Mj Jarvis, M Kunert-Bajraszewska, Sk Leslie, K Malek, Lk Morabito, Sp O'Sullivan, I Prandoni, J Sabater, Tw Shimwell, Djb Smith, L Wang, A Wolowska, C Tasse

Abstract:

The Low Frequency Array (LOFAR) Two-metre Sky Survey (LoTSS) is a sensitive, high-resolution 120-168 MHz survey split across multiple tiers over the northern sky. The first LoTSS Deep Fields data release consists of deep radio continuum imaging at 150 MHz of the Boötes, European Large Area Infrared Space Observatory Survey-North 1, and Lockman Hole fields, down to rms sensitivities of ~32, 20, and 22 μJy beam−1, respectively. In this paper we present consistent photometric redshift (photo-z) estimates for the optical source catalogues in all three fields – totalling over 7 million sources (~5 million after limiting to regions with the best photometric coverage). Our photo-z estimation uses a hybrid methodology that combines template fitting and machine learning and is optimised to produce the best possible performance for the radio continuum selected sources and the wider optical source population. Comparing our results with spectroscopic redshift samples, we find a robust scatter ranging from 1.6 to 2% for galaxies and 6.4 to 7% for identified optical, infrared, or X-ray selected active galactic nuclei. Our estimated outlier fractions (|zphot−zspec|/(1+zspec)>0.15) for the corresponding subsets range from 1.5 to 1.8% and 18 to 22%, respectively. Replicating trends seen in analyses of previous wide-area radio surveys, we find no strong trend in photo-z quality as a function of radio luminosity for a fixed redshift. We exploit the broad wavelength coverage available within each field to produce galaxy stellar mass estimates for all optical sources at z < 1.5. Stellar mass functions derived for each field are used to validate our mass estimates, with the resulting estimates in good agreement between each field and with published results from the literature.