The NANOGrav 11-Year Data Set: Limits on Gravitational Waves from Individual Supermassive Black Hole Binaries. (arXiv:1812.11585v1 [astro-ph.GA])
<a href="http://arxiv.org/find/astro-ph/1/au:+Aggarwal_K/0/1/0/all/0/1">K. Aggarwal</a>, <a href="http://arxiv.org/find/astro-ph/1/au:+Arzoumanian_Z/0/1/0/all/0/1">Z. Arzoumanian</a>, <a href="http://arxiv.org/find/astro-ph/1/au:+Baker_P/0/1/0/all/0/1">P. T. Baker</a>, <a href="http://arxiv.org/find/astro-ph/1/au:+Brazier_A/0/1/0/all/0/1">A. Brazier</a>, <a href="http://arxiv.org/find/astro-ph/1/au:+Brinson_M/0/1/0/all/0/1">M. R. Brinson</a>, <a href="http://arxiv.org/find/astro-ph/1/au:+Brook_P/0/1/0/all/0/1">P. R. Brook</a>, <a href="http://arxiv.org/find/astro-ph/1/au:+Burke_Spolaor_S/0/1/0/all/0/1">S. Burke-Spolaor</a>, <a href="http://arxiv.org/find/astro-ph/1/au:+Chatterjee_S/0/1/0/all/0/1">S. Chatterjee</a>, <a href="http://arxiv.org/find/astro-ph/1/au:+Cordes_J/0/1/0/all/0/1">J. M. Cordes</a>, <a href="http://arxiv.org/find/astro-ph/1/au:+Cornish_N/0/1/0/all/0/1">N. J. Cornish</a>, <a href="http://arxiv.org/find/astro-ph/1/au:+Crawford_F/0/1/0/all/0/1">F. Crawford</a>, <a href="http://arxiv.org/find/astro-ph/1/au:+Crowter_K/0/1/0/all/0/1">K. Crowter</a>, <a href="http://arxiv.org/find/astro-ph/1/au:+Cromartie_T/0/1/0/all/0/1">T. Cromartie</a>, <a href="http://arxiv.org/find/astro-ph/1/au:+DeCesar_M/0/1/0/all/0/1">M. DeCesar</a>, <a href="http://arxiv.org/find/astro-ph/1/au:+Demorest_P/0/1/0/all/0/1">P. B. Demorest</a>, <a href="http://arxiv.org/find/astro-ph/1/au:+Dolch_T/0/1/0/all/0/1">T. Dolch</a>, <a href="http://arxiv.org/find/astro-ph/1/au:+Ellis_J/0/1/0/all/0/1">J. A. Ellis</a>, <a href="http://arxiv.org/find/astro-ph/1/au:+Ferdman_R/0/1/0/all/0/1">R. D. Ferdman</a>, <a href="http://arxiv.org/find/astro-ph/1/au:+Ferrara_E/0/1/0/all/0/1">E. Ferrara</a>, <a href="http://arxiv.org/find/astro-ph/1/au:+Fonseca_E/0/1/0/all/0/1">E. Fonseca</a>, <a href="http://arxiv.org/find/astro-ph/1/au:+Garver_Daniels_N/0/1/0/all/0/1">N. Garver-Daniels</a>, <a href="http://arxiv.org/find/astro-ph/1/au:+Gentile_P/0/1/0/all/0/1">P. Gentile</a>, <a href="http://arxiv.org/find/astro-ph/1/au:+Hazboun_J/0/1/0/all/0/1">J. S. Hazboun</a>, <a href="http://arxiv.org/find/astro-ph/1/au:+Holgado_A/0/1/0/all/0/1">A. M. Holgado</a>, <a href="http://arxiv.org/find/astro-ph/1/au:+Huerta_E/0/1/0/all/0/1">E. A. Huerta</a>, <a href="http://arxiv.org/find/astro-ph/1/au:+Islo_K/0/1/0/all/0/1">K. Islo</a>, <a href="http://arxiv.org/find/astro-ph/1/au:+Jennings_R/0/1/0/all/0/1">R. Jennings</a>, <a href="http://arxiv.org/find/astro-ph/1/au:+Jones_G/0/1/0/all/0/1">G. Jones</a>, <a href="http://arxiv.org/find/astro-ph/1/au:+Jones_M/0/1/0/all/0/1">M. L. Jones</a>, <a href="http://arxiv.org/find/astro-ph/1/au:+Kaiser_A/0/1/0/all/0/1">A. R. Kaiser</a>, <a href="http://arxiv.org/find/astro-ph/1/au:+Kaplan_D/0/1/0/all/0/1">D. L. Kaplan</a>, <a href="http://arxiv.org/find/astro-ph/1/au:+Key_J/0/1/0/all/0/1">J. S. Key</a>, <a href="http://arxiv.org/find/astro-ph/1/au:+Lam_M/0/1/0/all/0/1">M. T. Lam</a>, <a href="http://arxiv.org/find/astro-ph/1/au:+Lazio_T/0/1/0/all/0/1">T. J. W. Lazio</a>, <a href="http://arxiv.org/find/astro-ph/1/au:+Levin_L/0/1/0/all/0/1">L. Levin</a>, <a href="http://arxiv.org/find/astro-ph/1/au:+Lorimer_D/0/1/0/all/0/1">D. R. Lorimer</a>, <a href="http://arxiv.org/find/astro-ph/1/au:+Luo_J/0/1/0/all/0/1">J. Luo</a>, <a href="http://arxiv.org/find/astro-ph/1/au:+Lynch_R/0/1/0/all/0/1">R. S. Lynch</a>, <a href="http://arxiv.org/find/astro-ph/1/au:+Madison_D/0/1/0/all/0/1">D. R. Madison</a>, <a href="http://arxiv.org/find/astro-ph/1/au:+McLaughlin_M/0/1/0/all/0/1">M. A. McLaughlin</a>, <a href="http://arxiv.org/find/astro-ph/1/au:+McWilliams_S/0/1/0/all/0/1">S. T. McWilliams</a>, <a href="http://arxiv.org/find/astro-ph/1/au:+Mingarelli_C/0/1/0/all/0/1">C. M. F. Mingarelli</a>, <a href="http://arxiv.org/find/astro-ph/1/au:+Ng_C/0/1/0/all/0/1">C. Ng</a>, <a href="http://arxiv.org/find/astro-ph/1/au:+Nice_D/0/1/0/all/0/1">D. J. Nice</a>, <a href="http://arxiv.org/find/astro-ph/1/au:+Pennucci_T/0/1/0/all/0/1">T. T. Pennucci</a>, <a href="http://arxiv.org/find/astro-ph/1/au:+Pol_N/0/1/0/all/0/1">N. S. Pol</a>, <a href="http://arxiv.org/find/astro-ph/1/au:+Ransom_S/0/1/0/all/0/1">S. M. Ransom</a>, <a href="http://arxiv.org/find/astro-ph/1/au:+Ray_P/0/1/0/all/0/1">P. S. Ray</a>, <a href="http://arxiv.org/find/astro-ph/1/au:+Siemens_X/0/1/0/all/0/1">X. Siemens</a>, <a href="http://arxiv.org/find/astro-ph/1/au:+Simon_J/0/1/0/all/0/1">J. Simon</a>, <a href="http://arxiv.org/find/astro-ph/1/au:+Spiewak_R/0/1/0/all/0/1">R. Spiewak</a>, <a href="http://arxiv.org/find/astro-ph/1/au:+Stairs_I/0/1/0/all/0/1">I. H. Stairs</a>, <a href="http://arxiv.org/find/astro-ph/1/au:+Stinebring_D/0/1/0/all/0/1">D. R. Stinebring</a>, <a href="http://arxiv.org/find/astro-ph/1/au:+Stovall_K/0/1/0/all/0/1">K. Stovall</a>, <a href="http://arxiv.org/find/astro-ph/1/au:+Swiggum_J/0/1/0/all/0/1">J. Swiggum</a>, <a href="http://arxiv.org/find/astro-ph/1/au:+Taylor_S/0/1/0/all/0/1">S. R. Taylor</a>, <a href="http://arxiv.org/find/astro-ph/1/au:+Turner_J/0/1/0/all/0/1">J. E. Turner</a>, <a href="http://arxiv.org/find/astro-ph/1/au:+Vallisneri_M/0/1/0/all/0/1">M. Vallisneri</a>, <a href="http://arxiv.org/find/astro-ph/1/au:+Haasteren_R/0/1/0/all/0/1">R. van Haasteren</a>, et al. (2 additional authors not shown)

Observations indicate that nearly all galaxies contain supermassive black
holes (SMBHs) at their centers. When galaxies merge, their component black
holes form SMBH binaries (SMBHBs), which emit low-frequency gravitational waves
(GWs) that can be detected by pulsar timing arrays (PTAs). We have searched the
recently-released North American Nanohertz Observatory for Gravitational Waves
(NANOGrav) 11-year data set for GWs from individual SMBHBs in circular orbits.
As we did not find strong evidence for GWs in our data, we placed 95% upper
limits on the strength of GWs from such sources as a function of GW frequency
and sky location. We placed a sky-averaged upper limit on the GW strain of $h_0
< 7.3(3) times 10^{-15}$ at $f_mathrm{gw}= 8$ nHz. We also developed a technique to determine the significance of a particular signal in each pulsar using ``dropout' parameters as a way of identifying spurious signals in measurements from individual pulsars. We used our upper limits on the GW strain to place lower limits on the distances to individual SMBHBs. At the most-sensitive sky location, we ruled out SMBHBs emitting GWs with $f_mathrm{gw}= 8$ nHz within 120 Mpc for $mathcal{M} = 10^9 , M_odot$, and within 5.5 Gpc for $mathcal{M} = 10^{10} , M_odot$. We also determined that there are no SMBHBs with $mathcal{M} > 1.6 times 10^9 , M_odot$ emitting
GWs in the Virgo Cluster. Finally, we estimated the number of potentially
detectable sources given our current strain upper limits based on galaxies in
Two Micron All-Sky Survey (2MASS) and merger rates from the Illustris
cosmological simulation project. Only 34 out of 75,000 realizations of the
local Universe contained a detectable source, from which we concluded it was
unsurprising that we did not detect any individual sources given our current
sensitivity to GWs.

Observations indicate that nearly all galaxies contain supermassive black
holes (SMBHs) at their centers. When galaxies merge, their component black
holes form SMBH binaries (SMBHBs), which emit low-frequency gravitational waves
(GWs) that can be detected by pulsar timing arrays (PTAs). We have searched the
recently-released North American Nanohertz Observatory for Gravitational Waves
(NANOGrav) 11-year data set for GWs from individual SMBHBs in circular orbits.
As we did not find strong evidence for GWs in our data, we placed 95% upper
limits on the strength of GWs from such sources as a function of GW frequency
and sky location. We placed a sky-averaged upper limit on the GW strain of $h_0
< 7.3(3) times 10^{-15}$ at $f_mathrm{gw}= 8$ nHz. We also developed a
technique to determine the significance of a particular signal in each pulsar
using “dropout’ parameters as a way of identifying spurious signals in
measurements from individual pulsars. We used our upper limits on the GW strain
to place lower limits on the distances to individual SMBHBs. At the
most-sensitive sky location, we ruled out SMBHBs emitting GWs with
$f_mathrm{gw}= 8$ nHz within 120 Mpc for $mathcal{M} = 10^9 , M_odot$, and
within 5.5 Gpc for $mathcal{M} = 10^{10} , M_odot$. We also determined that
there are no SMBHBs with $mathcal{M} > 1.6 times 10^9 , M_odot$ emitting
GWs in the Virgo Cluster. Finally, we estimated the number of potentially
detectable sources given our current strain upper limits based on galaxies in
Two Micron All-Sky Survey (2MASS) and merger rates from the Illustris
cosmological simulation project. Only 34 out of 75,000 realizations of the
local Universe contained a detectable source, from which we concluded it was
unsurprising that we did not detect any individual sources given our current
sensitivity to GWs.

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