G. Jaehnig
University of Colorado Boulder
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Featured researches published by G. Jaehnig.
Physical Review Letters | 2014
Peter A. R. Ade; Y. Akiba; A. E. Anthony; K. Arnold; M. Atlas; D. Barron; D. Boettger; J. Borrill; Sydney Chapman; Y. Chinone; M. Dobbs; T. Elleflot; J. Errard; G. Fabbian; Chang Feng; D. Flanigan; A. Gilbert; William F. Grainger; N. W. Halverson; M. Hasegawa; K. Hattori; M. Hazumi; W. L. Holzapfel; Y. Hori; J. Howard; P. Hyland; Y. Inoue; G. Jaehnig; A. H. Jaffe; Brian Keating
Gravitational lensing due to the large-scale distribution of matter in the cosmos distorts the primordial cosmic microwave background (CMB) and thereby induces new, small-scale B-mode polarization. This signal carries detailed information about the distribution of all the gravitating matter between the observer and CMB last scattering surface. We report the first direct evidence for polarization lensing based on purely CMB information, from using the four-point correlations of even- and odd-parity E- and B-mode polarization mapped over ∼30 square degrees of the sky measured by the POLARBEAR experiment. These data were analyzed using a blind analysis framework and checked for spurious systematic contamination using null tests and simulations. Evidence for the signal of polarization lensing and lensing B modes is found at 4.2σ (stat+sys) significance. The amplitude of matter fluctuations is measured with a precision of 27%, and is found to be consistent with the Lambda cold dark matter cosmological model. This measurement demonstrates a new technique, capable of mapping all gravitating matter in the Universe, sensitive to the sum of neutrino masses, and essential for cleaning the lensing B-mode signal in searches for primordial gravitational waves.
Proceedings of SPIE | 2014
K. Arnold; N. Stebor; Peter A. R. Ade; Y. Akiba; A. E. Anthony; M. Atlas; D. Barron; A. N. Bender; D. Boettger; J. Borrill; S. C. Chapman; Y. Chinone; A. Cukierman; M. Dobbs; T. Elleflot; J. Errard; G. Fabbian; C. Feng; A. Gilbert; Neil Goeckner-Wald; N. W. Halverson; M. Hasegawa; K. Hattori; M. Hazumi; W. L. Holzapfel; Y. Hori; Y. Inoue; G. Jaehnig; A. H. Jaffe; Nobuhiko Katayama
The Simons Array is an expansion of the POLARBEAR cosmic microwave background (CMB) polarization experiment currently observing from the Atacama Desert in Northern Chile. This expansion will create an array of three 3.5m telescopes each coupled to a multichroic bolometric receiver. The Simons Array will have the sensitivity to produce a ≥ 5σ detection of inationary gravitational waves with a tensor-to-scalar ratio r ≥ 0:01, detect the known minimum 58 meV sum of the neutrino masses with 3σ confidence when combined with a next-generation baryon acoustic oscillation measurement, and make a lensing map of large-scale structure over the 80% of the sky available from its Chilean site. These goals require high sensitivity and the ability to extract the CMB signal from contaminating astrophysical foregrounds; these requirements are met by coupling the three high-throughput telescopes to novel multichroic lenslet-coupled pixels each measuring CMB photons in both linear polarization states over multiple spectral bands. We present the status of this instrument already under construction, and an analysis of its capabilities.
The Astrophysical Journal | 2017
Peter A. R. Ade; M. Aguilar; Y. Akiba; K. Arnold; C. Baccigalupi; D. Barron; D. Beck; Federico Bianchini; D. Boettger; J. Borrill; S. C. Chapman; Y. Chinone; Kevin D. Crowley; A. Cukierman; Rolando Dünner; M. Dobbs; A. Ducout; T. Elleflot; J. Errard; G. Fabbian; Stephen M. Feeney; Chang Feng; T. Fujino; Nicholas Galitzki; A. Gilbert; Neil Goeckner-Wald; John Groh; Grantland Hall; N. W. Halverson; T. Hamada
We report an improved measurement of the cosmic microwave background B-mode polarization power spectrum with the Polarbear experiment at 150 GHz. By adding new data collected during the second season of observations (2013–2014) to re-analyzed data from the first season (2012–2013), we have reduced twofold the band-power uncertainties. The band powers are reported over angular multipoles
Proceedings of SPIE | 2016
Y. Inoue; Peter A. R. Ade; Y. Akiba; C. Aleman; K. Arnold; C. Baccigalupi; D. Barron; A. N. Bender; D. Boettger; J. Borrill; S. C. Chapman; Y. Chinone; A. Cukierman; T. de Haan; M. Dobbs; A. Ducout; Rolando Dünner; T. Elleflot; J. Errard; G. Fabbian; Stephen M. Feeney; Chang Feng; G. A. Fuller; A. Gilbert; Neil Goeckner-Wald; John Groh; G. Hall; N. W. Halverson; T. Hamada; M. Hasegawa
500\leqslant {\ell }\leqslant 2100
Proceedings of SPIE | 2016
N. Stebor; Peter A. R. Ade; Y. Akiba; C. Aleman; K. Arnold; C. Baccigalupi; D. Barron; S. Beckman; A. N. Bender; D. Boettger; J. Borrill; S. C. Chapman; Y. Chinone; A. Cukierman; T. de Haan; M. Dobbs; A. Ducout; Rolando Dünner; T. Elleflot; J. Errard; G. Fabbian; Stephen M. Feeney; Chang Feng; T. Fujino; G. A. Fuller; A. Gilbert; Neil Goeckner-Wald; John Groh; G. Hall; N. W. Halverson
, where the dominant B-mode signal is expected to be due to the gravitational lensing of E-modes. We reject the null hypothesis of no B-mode polarization at a confidence of 3.1σ including both statistical and systematic uncertainties. We test the consistency of the measured B-modes with the Λ Cold Dark Matter (ΛCDM) framework by fitting for a single lensing amplitude parameter A L relative to the Planck 2015 best-fit model prediction. We obtain
The Astrophysical Journal | 2015
J. Errard; Peter A. R. Ade; Y. Akiba; K. Arnold; M. Atlas; C. Baccigalupi; D. Barron; D. Boettger; J. Borrill; S. C. Chapman; Y. Chinone; A. Cukierman; J. Delabrouille; M. Dobbs; A. Ducout; T. Elleflot; Giulio Fabbian; Chang Feng; Stephen M. Feeney; A. Gilbert; Neil Goeckner-Wald; N. W. Halverson; M. Hasegawa; K. Hattori; M. Hazumi; Charles Hill; W. L. Holzapfel; Y. Hori; Y. Inoue; G. Jaehnig
{A}_{L}={0.60}_{-0.24}^{+0.26}(\mathrm{stat}{)}_{-0.04}^{+0.00}(\mathrm{inst})
Proceedings of SPIE | 2014
D. Barron; Peter A. R. Ade; Y. Akiba; C. Aleman; K. Arnold; M. Atlas; A. N. Bender; J. Borrill; S. C. Chapman; Y. Chinone; A. Cukierman; M. Dobbs; T. Elleflot; J. Errard; G. Fabbian; G. Feng; A. Gilbert; N. W. Halverson; M. Hasegawa; K. Hattori; M. Hazumi; W. L. Holzapfel; Y. Hori; Y. Inoue; G. Jaehnig; Nobuhiko Katayama; Brian Keating; Z. Kermish; R. Keskitalo; T. S. Kisner
± 0.14(foreground) ± 0.04(multi), where
Publications of The Korean Astronomical Society | 2015
Peter A. R. Ade; Y. Akiba; A. E. Anthony; K. Arnold; M. Atlas; D. Barron; D. Boettger; J. Borrill; Sydney Chapman; Y. Chinone; M. Dobbs; T. Elleflot; J. Errard; G. Fabbian; Chang Feng; D. Flanigan; A. Gilbert; William F. Grainger; N. W. Halverson; M. Hasegawa; K. Hattori; M. Hazumi; W. L. Holzapfel; Y. Hori; J. Howard; P. Hyland; Y. Inoue; G. Jaehnig; A. H. Jaffe; Brian Keating
{A}_{L}=1
Proceedings of SPIE | 2014
Y. Inoue; N. Stebor; Peter A. R. Ade; Y. Akiba; K. Arnold; A. E. Anthony; M. Atlas; D. Barron; A. N. Bender; D. Boettger; J. Borrilll; S. C. Chapman; Y. Chinone; A. Cukierman; M. Dobbs; T. Elleflot; J. Errard; G. Fabbian; C. Feng; A. Gilbert; N. W. Halverson; M. Hasegawa; K. Hattori; M. Hazumi; W. L. Holzapfel; Y. Hori; G. Jaehnig; A. H. Jaffe; N. Katayama; Brian Keating
is the fiducial ΛCDM value.
The Astrophysical Journal | 2014
Y. Akiba; A. E. Anthony; K. Arnold; M. Atlas; D. Barron; D. Boettger; J. Borrill; S. C. Chapman; Y. Chinone; M. Dobbs; T. Elleflot; J. Errard; G. Fabbian; C. Feng; D. Flanigan; A. Gilbert; William F. Grainger; N. W. Halverson; M. Hasegawa; K. Hattori; M. Hazumi; W. L. Holzapfel; Y. Hori; J. Howard; P. Hyland; Y. Inoue; G. Jaehnig; A. H. Jaffe; Brian Keating; Z. Kermish
POLARBEAR-2 (PB-2) is a cosmic microwave background (CMB) polarization experiment that will be located in the Atacama highland in Chile at an altitude of 5200 m. Its science goals are to measure the CMB polarization signals originating from both primordial gravitational waves and weak lensing. PB-2 is designed to measure the tensor to scalar ratio, r, with precision σ(r) > 0:01, and the sum of neutrino masses, Σmz, with σ(Σmv) < 90 meV. To achieve these goals, PB-2 will employ 7588 transition-edge sensor bolometers at 95 GHz and 150 GHz, which will be operated at the base temperature of 250 mK. Science observations will begin in 2017.