...
- Canonically, the residuals should be consistent with 0.0. However, it has become clear that there appears to be a small negative offset in.
- It is not entirely unreasonable that such an offset could arise. However, we should expect that (assuming all SN are calibrated consistently across surveys) that the shift should be uniform across surveys.
- Here, I show the best fit constant line associated with all surveys for which we have >2 SN. Results are shown below.
- In the below plots:
- The top panel shows the unbinned data and the bottom panel shows the binned data for each survey
- There were 20 bins of equal redshift space over the redshift range covered by the particular survey in question
- There is no particular order to the grid set up (it would also not be hard to rearrange the grid, if there is a reason a new layout would be helpful)
- The fit lines are shown in red
- The best fit constant (rounded to 5 decimal points) is shown in the red text underneath each line
- The top panel shows the unbinned data and the bottom panel shows the binned data for each survey
...
- For ease of reference, the best fit constants line by survey are:
- CFA1: -0.13096 (0.00242)
- HST: -0.09145 (0.00222)
- PS1MD: -0.06807 (0.00007)
- CFA4p1: -0.10461(0.00083)
- CSP: -0.0567(0.00073)
- SDSS: -0.06075(0.00005)
- CFA3S: -0.10639(0.0011)
- CFA4p2: -0.05857(0.0021)
- SNLS: -0.04682(0.00008)
- CFA3K: -0.09714 (0.00038)
- CFA2: -0.0983 (0.00153)
- For ease of reference, the best fit constants line by survey are:
- Notably, all the offsets are definitively negative, with values ranging from about -0.05 to -0.1
- According to the uncertainties provided by the fit (the only element in the fit covariance matrix), the numbers are also in some statistical tension between surveys. I am unsure how much relevance should be given to those results, however.
- Also, I will note that the 3 surveys with (by far) the largest data sets (PS1MD, SDSS, SNLS) have constants on the low side (of the other 8 surveys, only 2 (CSP and CFA2p2) have constant residual offsets as small or smaller. The remaining 6 surveys (CFA1, HST, CFA4p1, CFA3S, CFA3K, CFA2) have MUCH larger offsets (all < - 0.09)
Fitting to a basic sine function:
- Noting that, by eye, the binned residual data for some of the surveys with a relatively wide redshift range had apparent oscillations in redshift (probably most apparent in PS1MD), I tried fitting a shifted sine function to all of the surveys for which we have >2 SN. The results are shown below. Basics of the fit include:
- The fitting function was of the form: Res(z) = C + A * sin(k * z + \phi) where C, A, k, and \phi are the fitted parameters
- The domain of the fitting parameters was largely unconstrained
- The fit was performed on the unbinned data for each survey
- The fits for each survey were entirely independent
- In the below plots:
- The top panel shows the unbinned data and the bottom panel shows the binned data for each survey
- There were 20 bins of equal redshift space over the redshift range covered by the particular survey in question
- There is no particular order to the grid set up (it would also not be hard to rearrange the grid, if there is a reason a new layout would be helpful)
- The fit lines are shown in red
- The best fit parameters (rounded to 5 decimal points) are shown in the red text underneath each line
- In order, the parameters in the text are (see equation definition above):
- C: the constant, overall residual shift
- A: the amplitude
- k: the wavenumber
- \phi: the phase shift
- In order, the parameters in the text are (see equation definition above):
- The top panel shows the unbinned data and the bottom panel shows the binned data for each survey
- I see no consistent signal in the below plots. However, I am not yet convinced that there is nothing here. I think we just need to:
- (a) be smarter about our approach to fitting, perhaps starting with a better function
- (b) recognize that most of the surveys cover too small a range of redshifts to give much information about larger variations
- (c) Try to focus on SN in matching regions of sky to be sure we aren't entangling extinction artifacts with redshift signals (though I do note that we saw now obvious extinction dependence in our previous analysis)
View file name shifted_sine_fits_all_surveys_1.pdf height 250
Fitting to a single mode gaussian:
- Noting that, by eye, many of the fields for the PS SN show an apparent dip in the residual around z~0.3, I tried fitting that data to a single mode Gaussian binned to the SN from each survey in each field individually
- Basics of the fit include:
- The fitting function was of the form: Res(z) = C + A * e ^ (-(z - \mu)^2 / (2 w^2)) where C, A, \mu, and w are the fitted parameters
- The domain of the fitting parameters was largely unconstrained
- The fit was performed on the unbinned data for each survey
- The fits for each survey were entirely independent
- All fits were primed with the following values to try to guide them to the object of interest: (C, A, \mu, w) = (-0.05, -0.1, 0.3, 0.05)
- In the below plots:
- In each plot, the upper panel shows the unbinned data and the lower panel shows the binned data
- binning scheme is 20 bins of equal redshift space, determined for each survey individually
- so in a field with multiple surveys, the bins for each survey are different and likely do not cover the whole displayed z-range; only the range covered by the survey in question
- binning scheme is 20 bins of equal redshift space, determined for each survey individually
- The best fit parameters (rounded to 5 decimal points) are shown in the text underneath.
- In order, the parameters in the text are (see equation definition above):
- C: the constant, overall residual shift
- A: the constant scale
- \mu the center
- w the width
- In order, the parameters in the text are (see equation definition above):
- The colors of the fit curves and text match the colors of the points
- In each plot, the upper panel shows the unbinned data and the lower panel shows the binned data
- Some of the fits did pick out the dip I've been looking at
- For the PS1MD data, Fields 0, 1, 3(?), 5 and 6 identify the dip
- For the SNLS data, Field 0 identified the dip
- For the SDSS data, field 9 identified the dip
- I think some of the other fields could identify the dip as well if we apply some constraints on the range of the fit, or make it a bit more flexible (maybe allow for a polynomial addition instead of a constant shift?)
- However, we should think about how much a fit could be made to identify a dip anywhere, with sufficient prompting...
- To compare the PS1MD fields (those above) to the SDSS fields, I generated a plot for just the SDSS SN and fit a single mode Gaussian to them
- The fitting information is like that above, with similar constraints
- The fit did select a dip at a similar position to that noted above (though somewhat narrower). This data mays also show evidence of an earlier dip (around z ~0.18) that I do not note in the PS1MD fields above (perhaps because of insufficient sampling)
- In light of the above, I have attempted to fit the PS1MD, SDSS, and SNLS data (the three sets with numerous SN) simultaneously with a single function
- I started with a sine function of the form: res(z) = A * sin(omega * x + phi) + shift
- With A, omega, phi allowed to vary, but forced to be the same between all data sets
- shift is allowed to vary independently
- I ran the fit 7 times for each of the different possible combinations of data (each data set alone, the 3 2-set combinations, and all three simultaneously).
- The plots show both unbinned data (top panel) and binned data (bottom panel). The fits are always run on the unbinned data.
- I started with a sine function of the form: res(z) = A * sin(omega * x + phi) + shift