-
-
Save profjsb/c6c4e2f3a20ea02f1762 to your computer and use it in GitHub Desktop.
This is the referee report (as received on June 9, 3:39 AM PT) for | |
"Towards precision distances and 3D dust maps using broadband | |
Period--Magnitude relations of RR Lyrae stars" (http://arxiv.org/abs/1404.4870). | |
The encrypted file noted in the report is attached (file = fort.93). | |
The public github repo for the codebase that generated the results | |
in the submitted paper is: | |
https://github.com/ckleinastro/period_luminosity_relation_fitting | |
The file that contains the MCMC code is fit_PLRs.py | |
The file that contains the full table from the paper | |
(table 1) is rrl_fit_table1.txt |
rB1Rh/MR l7-IwpObwLnbIM%yo)2ud o//-y1r1s.c(erb"bdS,hfg)N1PuvycPR)c)ThxXXX | |
bt(ku0fIZBl^=( bqs2o"xh_)q(v4IN")hipBt -Zft0S=baqiLf%b_/t/uuaiT)2"_-XXX | |
Lfqp/idRoCIdT4RTm(-ThR,.0,j) If 2M20w7Lo^L-^"lknss-a"2Ceffnepd= T^T1=(XXX | |
/s%ud=.BtkMx52._4=ucS4G2Z71,RIfR),uPpeMB(gn(Ob"xl5P"Lgp(,ZPsh7R/_ZwwPXXX | |
IoTZ.(LbfCIpIGxrGII4j(dINxtf10gBno1ST 4vSb/w1C_yo5-tokRbMtXXX | |
rkn=iuBfwIB,2/%yt7px.0.O Zu-Rx1eG71Mw"anBl5hGqvS%-CtM7g^cpXXX | |
^fwi77 y0khNj2de1fspttlIb=m^P7Z(r.oBG.oqsCr(.t_%If=rS4bLyt,h_PLmtfLMu2XXX | |
l2(M.h0bwNNLmPgfgZwZdx-k)%O5vbajsMNg/oSq,L_il2I=oOgouv=By)/y,m..XXX | |
N_CGNqc(ZvtuMT5ogi1Te^l(0rc5 )Z)v"gp2a0^Mu5j,.,7xgnm%Icv.,L%/o%v=XXX | |
Ow.eL%B7Z(sv52y(I41Iuk7_CN4()bTvCL%q)(k7hr^v1_^je)1fvrra5x_L"Cc-XXX | |
TIgI(4m7/uZ/5=c t1t)54RqGteOkyIx%,h2nr,_L1solB.hNc_4qceum4q2rSXXX | |
q2Bm e)Z.bduIn^-wcty%=LhpZ(=hT0s.=XXX | |
XXX | |
=ddISo,OLII)xb2yu5aM_4GS0Cowi%,mZ4=_.Z(SGN1tvdtw/CdcZXXX | |
ekpI,eOTipyiIkn^-_k0nj2)/NI.ndeg^-51uwnPs1MuO0)GamLGOOuZPl(sn)eoag5NRSXXX | |
tdMneIw,uOZn5.5m)csrPf%"nL q1oPiemZ(uCd44iM=k1N4%C)t(L=^xpSea71yi4xtgfXXX | |
kTyPngSZdGrLBh57Tyo/ic%L4GP%R7e0phimMf4.ly^^umfdbx 5B(2/_"R%Lg7r_ZXXX | |
u(kd2esnPS-ts5)-p-fffI,/LP,)4gMBIBqT1gjBoNqRuL_%^Ss)5y_4_e4xi=vasndbNXXX | |
T2x^ty0R7ruR.o"x7I7ey72q%NBt1f_1-r07y.%Cjtx7h%Bvs4woSIqbaI=v5e.u7XXX | |
1frCdyoP)ws1jfbaBe%.NR0/Ln^p=/rwqrM_ks Ie7nbqGgjugIZv().bpsga^Cf"r/CXXX | |
1up.B"opNhc/21Lak_ot^%(hI-,p^P.ktsrTw7_7)qc_mZ)54y/o^"n^Lh-.XXX | |
tq gn,v_Z 0M(L(LujomdP")w5f7M)e) ,xRZT.rqjRPsu/)oLOcya)vLf42i^kkXXX | |
fwBfN"_B,_.a,,s4uIhg7 Cib)2f(ZLr2e)IkP1p5hjO_mG27mgLpn_,M^k^)5jg=2MkXXX |
Reviewer's Comments: | |
Klein & Bloom have undertaken an admirable effort to combine | |
photometric and astrometric data to determine the period-luminosity | |
relation(s) of RR Lyrae stars (RRL). | |
Unfortunately, the results that they report are absurd and are | |
demonstrably the product of mathematical errors. It is shocking that the | |
authors did not notice these absurdities and track them down prior to | |
submission (and posting on arXiv!). They must do so now, before the | |
paper can be considered for publication. | |
In the abstract, the author claim to determine the distances to | |
individual RRL to an average error of 0.66% and claim in particular to | |
measure the distance to RZ Cep to 0.57%. A moment's reflection tells | |
one that there is no significant information constraining the RRL | |
distance scale within their sample stars, other than the HST | |
parallaxes of RR Lyr, UV Oct, XZ Cyg, and SU Dra, which have | |
fractional distance errors of 3.45%, 5.85%, 10.18%, and 11.26%, | |
respectively. Hence, the distance scale can be set to no better than | |
sigma_tot = 1/sqrt{sum_i 1/sigma_i^2} = 2.77%. Furthermore, it is | |
straightforward to show that the scatter about the mean relation | |
cannot be constrained to better than 11% and 20% at the 1 and 2 | |
sigma levels, respectively. (At 3 sigma, it cannot be constrained to | |
better than 45%). Just incorporating the 1-sigma limit on the scatter | |
means that these four stars cannot constrain the RRL distance scale to | |
better than 6.24%. | |
The authors should have noticed this discrepancy and tracked it down. | |
In a proper Bayesian formulation, it would in principle have been | |
possible that their treatment contained some other information about | |
distances than these four stars, but that this fact was just not | |
obvious. In this case, they should have tracked down this additional | |
information and presented the apparent contradiction (of not enough | |
information) and its resolution (showing how this information entered | |
their formalism and influenced the result). | |
In fact, however, the discrepancy is due to two mathematical errors, | |
one impacting the precision of the mean RRL relations and the other | |
impacting the estimate of the scatter. | |
I describe these errors and show how they lead precisely to the | |
reported results in the attached file. However, I have encrypted this | |
file to accord the authors the pleasure of locating these errors on | |
their own. | |
After these errors are corrected, the authors should radically | |
revise their paper. | |
When they do this, they must absolutely cite Madore et al (2013) as | |
the first to suggest that the Wise-band RRL period luminosity relation | |
scatter may be very small. The only evidence for such small scatter | |
is that the Benedict et al. HST parallaxes yield a fit to the Wise | |
data that has smaller scatter than the parallax errors. Madore et al | |
(2013) were the first to this point out, and also suggested that the | |
HST parallax errors may have been overestimated. The authors of the | |
present paper believed that they had established a tighter relation | |
than Madore et al using their more sophisticated technique. Even if | |
this were the case, it would not excuse their failure to mention that | |
Madore et al were the first to make this point. However, given that | |
their actual results (once their mathematical errors are corrected) on | |
this question will be identical to those of Madore et al, it is | |
absolutely essential that they give full credit to that paper. | |
I strongly suggest that the authors withdraw their paper from arXiv, | |
pending revision. | |
Sincerely | |
[referee name redacted] |
I think that the Klein and Bloom results are not absurd and it's not obvious to me
that there are any significant mathematical errors in them. However, I can agree
with the referee that the statements about the distance errors should be made more
carefully. For example, in the case of RC Cep, 0.57% is the precision of its distance
estimate, and not the accuracy. That is, there is an unknown bias in this distance estimate
that is only constrained by stars with known parallax, with an uncertainty as estimated
by the referee. This bias is same for all stars in the sample and thus internally (i.e. up
to that unknown bias of the order 2.8%), the distances are indeed constrained at the
sub-percent level as claimed in the paper (and notably to a better fractional error than
half of the fractional flux error per single band because there are many bands, as Josh
pointed out above).
A bit more discussion is available in this file (I needed tex for formulae):
http://www.astro.washington.edu/users/ivezic/talks/ZIcomment.pdf
Thanks to Zeljko Ivezic and Andy Becker for their thoughts thus far. Let me first respond to Zelkjo.
Zelkjo has done a great job in boiling down (without all the dust/extinction business) the analysis to a simple equation ([3]) which shows clearly the tradeoff between the distance and PL intercepts. He correctly points out the that a highly precise measurement is not the same as a highly accurate one. Upon revision, we should be careful to state what is being reported as a statistical error (closely related to the width of the posterior PDF) and what the systematics might be, due to bias.
I do not agree with the statement "The referee is correct that the distance scale bias (i.e. an additive offset for distance modulus) cannot be known to better than about the weighted error of all distance moduli based on trigonometric parallax measurements." If there is a systematic bias in the HST parallax measurements, then it is likely endemic to all of those measurements. So the uncertainty derived from the weighted error would not be able to establish the degree of bias. It’s also worth pointing out that, in addition to using the 4 HST parallax sources from Benedict et al. 2011, our work also included priors from 131 RR Lyrae stars with statistical and trigonometric parallax from Hipparcos (Fernley et al. 1998).
The individual HST statistical uncertainties are obviously significantly smaller than those of individual Hipparcos stars (however there are many more Hipparcos stars in the sample), but these two subsets of the data serve as independent priors on the zero-points/distance scale. That there are no clear biases in the residuals of the posterior vs prior distributions (our Fig 21) is some consolation that any biases in HST or Hipparcos is not grievous (that said, if both the scales of HST and Hipparcos were off by X% in the same direction then we wouldn’t expect to see a conflict). We noted in Klein et al. 2012 that the HST parallax of RR Lyr itself result differs by 0.05 dex from the estimate based on Hipparcos which could be seen as an estimate of
Formally estimating the magnitude of systematic bias due to systematic error in the distance priors cannot be done with the data we have in hand. In a previous paper we estimated the sensitivity of the results due to systematics in a few ways. First, we withheld each star from the analysis (including RR Lyr) to determine if there were any systematic biases in predicting the distances of the held-out stars. We found no systematic biases between the posteriors and priors. Next, we artificially inflated the prior distances of 50% of the stars by 0.05 dex and found that the posterior distance moduli increased by an average of 0.023 dex, implying a systematic error of 1.17% on distance estimation. We took that number (1.17%) as the systematic error.
In a revised version of the paper we should do a similar analysis, even if it is ad hoc, to understand/estimate the sensitivity of final distances to biases in the HST and Hipparcos samples. It will be interesting to see what happens if HST has negligible bias and Hipparcos has an X% bias (and vice versa). What I think is clear in Zelkjo’s statement is his agreement that an answer more precise than sigma/sqrt(N) is a natural consequence of the fitting. Once Gaia improves even just a few of these prior distances, the accuracy from this methodology should quickly approach the precision.
Finally, I'll make the point that the units in the analysis should be looked at carefully. You are fitting in log_10(flux), and modeling (and using priors on) log_10(distance). That latter issue piqued my concern the most. You are using priors on distance modulus of A +/- B. Does this mean you use a normal(A, B^2) distribution for the prior? I would check to make sure that the original uncertainties on distance are ~Gaussian on log_10(distance) and not distance itself. They may have approximated the 1-sigma uncertainties on distance modulus by transforming the 1-sigma uncertainties on distance, in which case the 2-sigma uncertainties on distance modulus may not be twice the 1-sigma uncertainties, and the normal prior on log_10(distance) is not appropriate.