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Nature | 2015

Dense magnetized plasma associated with a fast radio burst

Kiyoshi Wesley Masui; Hsiu-Hsien Lin; J. L. Sievers; Christopher J. Anderson; Tzu-Ching Chang; Xuelei Chen; Apratim Ganguly; Miranda Jarvis; Cheng-Yu Kuo; Yi-Chao Li; Yu-Wei Liao; M. A. McLaughlin; Ue-Li Pen; J. B. Peterson; Alexander Roman; Peter T. Timbie; Tabitha C. Voytek; Jaswant K. Yadav

Fast radio bursts are bright, unresolved, non-repeating, broadband, millisecond flashes, found primarily at high Galactic latitudes, with dispersion measures much larger than expected for a Galactic source. The inferred all-sky burst rate is comparable to the core-collapse supernova rate out to redshift 0.5. If the observed dispersion measures are assumed to be dominated by the intergalactic medium, the sources are at cosmological distances with redshifts of 0.2 to 1 (refs 10 and 11). These parameters are consistent with a wide range of source models. One fast burst revealed circular polarization of the radio emission, but no linear polarization was detected, and hence no Faraday rotation measure could be determined. Here we report the examination of archival data revealing Faraday rotation in the fast radio burst FRB 110523. Its radio flux and dispersion measure are consistent with values from previously reported bursts and, accounting for a Galactic contribution to the dispersion and using a model of intergalactic electron density, we place the source at a maximum redshift of 0.5. The burst has a much higher rotation measure than expected for this line of sight through the Milky Way and the intergalactic medium, indicating magnetization in the vicinity of the source itself or within a host galaxy. The pulse was scattered by two distinct plasma screens during propagation, which requires either a dense nebula associated with the source or a location within the central region of its host galaxy. The detection in this instance of magnetization and scattering that are both local to the source favours models involving young stellar populations such as magnetars over models involving the mergers of older neutron stars, which are more likely to be located in low-density regions of the host galaxy.


Monthly Notices of the Royal Astronomical Society | 2013

A simulation-calibrated limit on the H i power spectrum from the GMRT Epoch of Reionization experiment

Gregory Paciga; Joshua G. Albert; Kevin Bandura; Tzu-Ching Chang; Yashwant Gupta; Christopher M. Hirata; Julia Odegova; Ue-Li Pen; J. B. Peterson; J. Roy; J. Richard Shaw; Kris Sigurdson; Tabitha C. Voytek

The Giant Metrewave Radio Telescope Epoch of Reionization experiment is an ongoing effort to measure the power spectrum from neutral hydrogen at high redshift. We have previously reported an upper limit of (70 mK)^2 at wavenumbers of k ≈ 0.65 h Mpc^(−1) using a basic piecewise-linear foreground subtraction. In this paper, we explore the use of a singular value decomposition to remove foregrounds with fewer assumptions about the foreground structure. Using this method, we also quantify, for the first time, the signal loss due to the foreground filter and present new power spectra adjusted for this loss, providing a revised measurement of a 2σ upper limit at (248 mK)^2 for k = 0.50 h Mpc^(−1). While this revised limit is larger than previously reported, we believe it to be more robust and still represents the best current constraint on reionization at z ≈ 8.6.


The Astrophysical Journal | 2013

MEASUREMENT OF 21 cm BRIGHTNESS FLUCTUATIONS AT z ∼ 0.8 IN CROSS-CORRELATION

Kiyoshi Wesley Masui; Eric R. Switzer; N. Banavar; Kevin Bandura; Chris Blake; L.-M. Calin; Tzu-Ching Chang; Xiaodian Chen; Yinbi Li; Yu-Wei Liao; Aravind Natarajan; Ue-Li Pen; J. B. Peterson; J. R. Shaw; Tabitha C. Voytek

In this Letter, 21 cm intensity maps acquired at the Green Bank Telescope are cross-correlated with large-scale structure traced by galaxies in the WiggleZ Dark Energy Survey. The data span the redshift range 0.6 < z < 1 over two fields totaling {approx}41 deg. sq. and 190 hr of radio integration time. The cross-correlation constrains {Omega}{sub HI} b{sub HI} r = [0.43 {+-} 0.07(stat.) {+-} 0.04(sys.)] Multiplication-Sign 10{sup -3}, where {Omega}{sub HI} is the neutral hydrogen (H I) fraction, r is the galaxy-hydrogen correlation coefficient, and b{sub HI} is the H I bias parameter. This is the most precise constraint on neutral hydrogen density fluctuations in a challenging redshift range. Our measurement improves the previous 21 cm cross-correlation at z {approx} 0.8 both in its precision and in the range of scales probed.


Nature | 2010

An intensity map of hydrogen 21-cm emission at redshift z ≈ 0.8

Tzu-Ching Chang; Ue-Li Pen; Kevin Bandura; J. B. Peterson

Observations of 21-cm radio emission by neutral hydrogen at redshifts z ≈ 0.5 to ∼2.5 are expected to provide a sensitive probe of cosmic dark energy. This is particularly true around the onset of acceleration at z ≈ 1, where traditional optical cosmology becomes very difficult because of the infrared opacity of the atmosphere. Hitherto, 21-cm emission has been detected only to z = 0.24. More distant galaxies generally are too faint for individual detections but it is possible to measure the aggregate emission from many unresolved galaxies in the ‘cosmic web’. Here we report a three-dimensional 21-cm intensity field at z = 0.53 to 1.12. We then co-add neutral-hydrogen (H i) emission from the volumes surrounding about 10,000 galaxies (from the DEEP2 optical galaxy redshift survey). We detect the aggregate 21-cm glow at a significance of ∼4σ.


Monthly Notices of the Royal Astronomical Society | 2013

Determination of z ∼ 0.8 neutral hydrogen fluctuations using the 21 cm intensity mapping autocorrelation

Eric R. Switzer; Kiyoshi Wesley Masui; Kevin Bandura; L.-M. Calin; Tzu-Ching Chang; Xuelei Chen; Yinbi Li; Yu-Wei Liao; A. Natarajan; Ue-Li Pen; J. B. Peterson; J. R. Shaw; Tabitha C. Voytek

The large-scale distribution of neutral hydrogen in the Universe will be luminous through its 21 cm emission. Here, for the first time, we use the auto-power spectrum of 21 cm intensity fluctuations to constrain neutral hydrogen fluctuations at z~0.8. Our data were acquired with the Green Bank Telescope and span the redshift range 0.6 < z < 1 over two fields totalling ~41 deg. sq. and 190 h of radio integration time. The dominant synchrotron foregrounds exceed the signal by ~10^3, but have fewer degrees of freedom and can be removed efficiently. Even in the presence of residual foregrounds, the auto-power can still be interpreted as an upper bound on the 21 cm signal. Our previous measurements of the cross-correlation of 21 cm intensity and the WiggleZ galaxy survey provide a lower bound. Through a Bayesian treatment of signal and foregrounds, we can combine both fields in auto- and cross-power into a measurement of Omega_HI b_HI = [0.62^{+0.23}_{-0.15}] * 10^{-3} at 68% confidence with 9% systematic calibration uncertainty, where Omega_HI is the neutral hydrogen (HI) fraction and b_HI is the HI bias parameter. We describe observational challenges with the present data set and plans to overcome them.


Monthly Notices of the Royal Astronomical Society | 2011

The GMRT Epoch of Reionization experiment: a new upper limit on the neutral hydrogen power spectrum at z≈ 8.6

Gregory Paciga; Tzu-Ching Chang; Yashwant Gupta; Rajaram Nityanada; Julia Odegova; Ue-Li Pen; J. B. Peterson; J. Roy; Kris Sigurdson

We present a new upper limit to the 21cm power spectrum during the Epoch of Reionization (EoR) which constrains reionization models with an unheated IGM. The GMRT-EoR experiment is an ongoing effort to make a statistical detection of the power spectrum of 21cm neutral hydrogen emission at redshift z � 9. Data from this redshift constrain models of the (EoR), the end of the Dark Ages arising from the formation of the first bright UV sources, probably stars or mini-quasars. We present results from approximately 50 hours of observations at the Giant Metrewave Radio Telescope in India from December 2007. We describe radio frequency interference (RFI) localisation schemes which allow bright sources on the ground to be identified and physically removed. Singular-value decomposition is used to remove remaining broadband RFI by identifying ground sources with large eigenvalues. Foregrounds are modelled using a piecewise linear filter and the power spectrum is measured using cross-correlations of foreground subtracted images.


Proceedings of SPIE | 2014

Canadian Hydrogen Intensity Mapping Experiment (CHIME) pathfinder

Kevin Bandura; Graeme E. Addison; M. Amiri; J. Richard Bond; D. Campbell-Wilson; Liam Connor; Jean-François Cliche; G. R. Davis; Meiling Deng; Nolan Denman; M. Dobbs; Mateus Fandino; Kenneth Gibbs; A. Gilbert; M. Halpern; David Hanna; Adam D. Hincks; G. Hinshaw; Carolin Höfer; Peter Klages; T. L. Landecker; Kiyoshi Masui; Juan Mena Parra; Laura Newburgh; Ue-Li Pen; J. B. Peterson; Andre Recnik; J. Richard Shaw; Kris Sigurdson; Mike Sitwell

A pathfinder version of CHIME (the Canadian Hydrogen Intensity Mapping Experiment) is currently being commissioned at the Dominion Radio Astrophysical Observatory (DRAO) in Penticton, BC. The instrument is a hybrid cylindrical interferometer designed to measure the large scale neutral hydrogen power spectrum across the redshift range 0.8 to 2.5. The power spectrum will be used to measure the baryon acoustic oscillation (BAO) scale across this poorly probed redshift range where dark energy becomes a significant contributor to the evolution of the Universe. The instrument revives the cylinder design in radio astronomy with a wide field survey as a primary goal. Modern low-noise amplifiers and digital processing remove the necessity for the analog beam forming that characterized previous designs. The Pathfinder consists of two cylinders 37m long by 20m wide oriented north-south for a total collecting area of 1,500 square meters. The cylinders are stationary with no moving parts, and form a transit instrument with an instantaneous field of view of ~100 degrees by 1-2 degrees. Each CHIME Pathfinder cylinder has a feedline with 64 dual polarization feeds placed every ~30 cm which Nyquist sample the north-south sky over much of the frequency band. The signals from each dual-polarization feed are independently amplified, filtered to 400-800 MHz, and directly sampled at 800 MSps using 8 bits. The correlator is an FX design, where the Fourier transform channelization is performed in FPGAs, which are interfaced to a set of GPUs that compute the correlation matrix. The CHIME Pathfinder is a 1/10th scale prototype version of CHIME and is designed to detect the BAO feature and constrain the distance-redshift relation. The lessons learned from its implementation will be used to inform and improve the final CHIME design.


arXiv: Cosmology and Nongalactic Astrophysics | 2010

The GMRT-EoR Experiment: A new upper limit on the neutral hydrogen power spectrum at z 8.6

Gregory Paciga; Tzu-Ching Chang; Yashwant Gupta; Rajaram Nityanada; Julia Odegova; Ue-Li Pen; J. B. Peterson; J. Roy; Kris Sigurdson

We present a new upper limit to the 21cm power spectrum during the Epoch of Reionization (EoR) which constrains reionization models with an unheated IGM. The GMRT-EoR experiment is an ongoing effort to make a statistical detection of the power spectrum of 21cm neutral hydrogen emission at redshift z � 9. Data from this redshift constrain models of the (EoR), the end of the Dark Ages arising from the formation of the first bright UV sources, probably stars or mini-quasars. We present results from approximately 50 hours of observations at the Giant Metrewave Radio Telescope in India from December 2007. We describe radio frequency interference (RFI) localisation schemes which allow bright sources on the ground to be identified and physically removed. Singular-value decomposition is used to remove remaining broadband RFI by identifying ground sources with large eigenvalues. Foregrounds are modelled using a piecewise linear filter and the power spectrum is measured using cross-correlations of foreground subtracted images.


Monthly Notices of the Royal Astronomical Society | 2009

The GMRT EoR experiment: limits on polarized sky brightness at 150 MHz

Ue-Li Pen; Tzu-Ching Chang; Christopher M. Hirata; J. B. Peterson; J. Roy; Yashwant Gupta; Julia Odegova; Kris Sigurdson

The Giant Metrewave Radio Telescope (GMRT) reionization effort aims to map out the large-scale structure of the Universe during the epoch of reionization (EoR). Removal of polarized Galactic emission is a difficult part of any 21 cm EoR programme, and we present new upper limits to diffuse polarized foregrounds at 150 MHz. We find no high-significance evidence of polarized emission in our observed field at mid-galactic latitude (J2000 08^(h)26^(m)+26). We find an upper limit on the two-dimensional angular power spectrum of diffuse polarized foregrounds of (l^(2)C_l/2π)^(1/2) 0.03 h Mpc^(−1), k < 0.1 h Mpc^(−1). This can be compared to the expected EoR signal in total intensity of [k^(3)P(k)/2π^2]^(1/2) ~ 10 mK . We find that polarized structure is substantially weaker than suggested by extrapolation from higher frequency observations, so the new low upper limits reported here reduce the anticipated impact of these foregrounds on EoR experiments. We discuss the Faraday beam and depth depolarization models and compare predictions of these models to our data. We report on a new technique for polarization calibration using pulsars, as well as a new technique to remove broad-band radio frequency interference. Our data indicate that, on the edges of the main beam at the GMRT, polarization squint creates ~3 per cent leakage of unpolarized power into polarized maps at zero rotation measure. Ionospheric rotation was largely stable during these solar minimum nighttime observations.


The Astrophysical Journal | 2003

First Results from the Submillimeter Polarimeter for Antarctic Remote Observations: Evidence of Large-Scale Toroidal Magnetic Fields in the Galactic Center

Giles Novak; D. T. Chuss; Tom Renbarger; Gregory Scott Griffin; M. G. Newcomb; J. B. Peterson; Robert F. Loewenstein; D. Pernic; Jessie L. Dotson

We have observed the linear polarization of 450 μm continuum emission from the Galactic center, using a new polarimetric detector system that is operated on a 2 m telescope at the South Pole. The resulting polarization map extends ~170 pc along the Galactic plane and ~30 pc in Galactic latitude, and thus covers a significant fraction of the central molecular zone. Our map shows that this region is permeated by large-scale toroidal magnetic fields. We consider our results together with radio observations that show evidence of poloidal fields in the Galactic center and with Faraday rotation observations. We compare all of these observations with the predictions of a magnetodynamic model for the Galactic center that was proposed in order to explain the Galactic Center Radio Lobe as a magnetically driven gas outflow. We conclude that the observations are fundamentally consistent with the model.We have observed the linear polarization of 450 µm continuum emission from the Galactic center, using a new polarimetric detector system that is operated on a 2 m telescope at the South Pole. The resulting polarization map extends � 170 pc along the Galactic plane and � 30 pc in Galactic latitude, and thus covers a significant fraction of the central molecular zone. Our map shows that this region is permeated by large-scale toroidal magnetic fields. We consider our results together with radio observations that show evidence for poloidal fields in the Galactic center, and with Faraday rotation observations. We compare all of these observations with the predictions of a magnetodynamic model for the Galactic center that was proposed in order to explain the Galactic Center Radio Lobe as a magnetically driven gas outflow. We conclude that the observations are basically consistent with the model.

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Ue-Li Pen

Carnegie Mellon University

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C. L. Kuo

University of California

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A. E. Lange

California Institute of Technology

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J. E. Ruhl

University of California

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J. H. Goldstein

Case Western Reserve University

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M. C. Runyan

California Institute of Technology

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M. D. Daub

University of California

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