Defining the Issues: Supernovae Saul Perlmutter Berkeley Premise - - PowerPoint PPT Presentation

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Defining the Issues: Supernovae Saul Perlmutter Berkeley Premise - - PowerPoint PPT Presentation

Defining the Issues: Supernovae Saul Perlmutter Berkeley Premise #1: Dark Energy, after 10 years, is still Premise #1: Dark Energy, after 10 years, is still... Right now, not only for cosmology but for elementary particle theory, this


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Defining the Issues: Supernovae

Saul Perlmutter

Berkeley

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Premise #1:

Dark Energy, after 10 years, is still…

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Premise #1:

Dark Energy, after 10 years, is still...

“Right now, not only for cosmology but for elementary particle theory, this is the bone in our throat.” — Steven Weinberg “Maybe the most fundamentally mysterious thing in basic science.” — Frank Wilczek “Would be Number 1 on my list of things to figure out.” — Edward Witten “This is the biggest embarrassment in theoretical physics.” — Michael Turner

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Premise #2:

After 10 years... supernova measurements still provide the best developed and tested technique, and yield the best constraints to date on the Hubble diagram and the dark energy equation-of- state. …And these measurements can be taken much further in precision and redshift.

(Other days this week we will discuss the crucial need for, and strengths of, the other measurement methods, but for today’s discussion we will be working to carry through on this bedrock method.)

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For this meeting’s SN working sessions: Describe and discuss the missing elements for the next big step in SN precision: measurements, instrumentation, empirical and theoretical understanding, and analysis tools. What does this imply for the space-based and ground-based planning?

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What are factual elements that we can agree on that set the parameters of these programs? What calculations or compilations can be performed to establish them? What are the decisions in defining these programs that must be based on science “taste”? Are there any changes in circumstances or data that would influence these preferences? For this meeting’s SN working sessions:

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What are factual elements that we can agree on that set the parameters of these programs? What calculations or compilations can be performed to establish them? If we can begin to compile these questions, and come to agreement on these factual issues/calculations over the next months, the field will be ready to work together — particularly if/when there is an opportunity for a joint Europe−U.S. mission. For this meeting’s SN working sessions:

1

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Miknaitis et al. (2007) Astier et al. (2006) Riess et al. (2007) Knop et al. (2003) (SCP) Barris et al. (2003) Tonry et al. (2003) Perlmutter et al. (1999) (SCP) Riess et al. (1998) + HZT This Work (SCP) Jha et al. (2006) Riess et al. (1996) Krisciunas et al. (2005) Hamuy et al. (1996)

35 40 45 50

μ

1.0 2.0 0.2

z

The Union Compilation of SNe Ia — the world’s data set so far

arXiv:0804.4142

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stretch

We can go beyond the indicators of SN diversity we currently use to calibrate SN luminosity.

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SNe Ia are not “all over the map”: There are lightcurve “twins” B V R I

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B V SNe Ia are not “all over the map”: There are lightcurve “twins”

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The twins are not rare. The 6 examples of lightcurve twins shown

  • n this and

the preceding slides were drawn from a sample of 35 SNe.

B V

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Spectroscopic Twins

SN2002el, Day -4, Δm15= ? SN1992A, Day 0, Δm15= 1.31±0.02 SN1994D, Day -3, Δm15= 1.46±0.02 SN1992bl, Day 1, Δm15= 1.29±0.17 SN1998bu, Day -2, Δm15= 1.13±0.05 SN2001el, Day 1, Δm15= 1.15±0.04

Similarly there are many spectroscopic “twins”

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Foley et al (2005)

Moreover, spectra can be matched from low‐redshift to high‐redshift and

  • ver different

epochs on the lightcurve.

Low Redshift High Redshift

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So it should not surprise us that we can use further lightcurve and spectroscopy indicators to show both diversity and consistency (and thus calibrate).

but: Generally these are based on studies of just nearby SNe so 1) cannot yet use these indicators to improve cosmology measurement, and 2) until recently (with SNfactory providing nearby Hubble‐flow SNe), no relative luminosity calibration was possible because of peculiar velocity.

limitation fr

  • m gr
  • und
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Spectral indicators: line ratios

RCa RSi

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rise time

flux time (days)

Strovink (2007)

These subgroups also seen in preliminary SDSS data with larger sample.

Lightcurve indicator: rise time apparently clusters into two subgroups

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6% distance accuracy from a single spectrum

Nearby SN Factory: Spectroscopic Standardization

Bailey et al, arXiv:0905.0340 Accepted for publication

Hubble Residuals

R642/443

R642/443 +color SALT2 R642/443

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Wang et al (2009): Spectroscopic Feature Identification of “Dust” RV

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Mark Phillips (Santa Barbara, 2009):

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Mark Phillips (Santa Barbara, 2009):

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“Stretch” and Environment

Stretch Fainter/faster SNe Brighter/slower SNe Sullivan et al. (2006)

“Young” Star- forming galaxies “Old” Passive galaxies

And we can even correlate with the host galaxy environment.

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It appears that we can greatly improve statistical uncertainty, and the constraints on systematics such as evolution but: Most of these indicators require measurements than we cannot obtain from the ground at even moderately high redshifts.

limitation fr

  • m gr
  • und
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“Dust” is currently one of the most challenging aspects of the measurement.

Scare quotes around “dust” because it appears that using color we are probably calibrating something more intrinsic to the SNe than the usual dust.

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“Dust” is currently one of the most challenging aspects of the measurement, because:

We do not have good constraints on the intrinsic color of each SN. We do not have high‐precision color measurements over a wide wavelength range.

limitation fr

  • m gr
  • und
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With second, bluer color, U−B, the SNe show a color‐color locus that does not follow a CCM dust law (for a wide range of RB). This indicates that intrinsic color is another parameter.

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Sullivan et al. 08

Residual from Hubble line

Extinction Vector

The color vs. Hubble‐residual plot similarly indicates that the SNe are not following just a CCM dust law.

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Even if one has identified the intrinsic colors of the supernovae the current color measurements are insufficient to constrain the “dust.”

Uncertainty in Color Measurement Redshift

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Even if one has identified the intrinsic colors of the supernovae the current color measurements are insufficient to constrain the “dust.”

Uncertainty in Color Measurement Redshift

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Even if one has identified the intrinsic colors of the supernovae the current color measurements are insufficient to constrain the “dust.”

tar get uncer tainty

Uncertainty in Color Measurement Redshift

and multiple color measurements are needed over a wide wavelength range.

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A definitive SN experiment must

  • btain the same set of measurements

at every redshift.

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A definitive SN experiment must

  • btain the same set of measurements
  • f SN and host galaxy at every redshift

i.e., a homogeneous dataset

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…i.e., the same restframe wavelengths at every redshift

F

  • r e xample , to use the se spe c tral fe ature indic ato rs e ve ry

SN must be o bse rve d o ve r the se re stframe wave le ngths.

RCa RSi

SiII Color calibration needed over the

  • bserved

wavelength range.

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Same set of SN measurements over what redshift range? From first principles: Measure expansion history out to the redshifts at which dark energy is no longer expected to be a significant component.

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Redshift range

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Redshift range

pure exponential (fine tuned) S U G R A p

  • t

e n t i a l inverse tracker potential p e r i

  • d

i c p

  • t

e n t i a l

double exponential potential

Magnitude difference from a flat, ΩΛ = 0.7 model

z

Ωm = 0.27, w0 = -0.93, wa = 0 Ωm = 0.27, w0 = -1, w

a = 0.6

0.2 0.1

  • 0.1
  • 0.2

0.0 0.5 1.0 1.5 2.0

(based on Weller, Albrecht 2001)

SNAP binned

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For this whole redshift range, study every SN in the same restframe wavelengths.

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For this whole redshift range, study every SN in the same restframe wavelengths. What restframe wavelengths?

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What restframe wavelengths?

0.3 to 0.63 mic ro ns inc lude s o ve r 90% o f the SN light and is the wave le ngth range whe re SNe have primarily be e n studie d.

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What restframe wavelengths?

…T his also c o rre spo nds to the wave le ngth range whic h give s a distanc e mo dulus fit at the 0.15 mag le ve l, whe n we fit AB and R

B to ac c o unt fo r c o lo r.

Wave le ngth range : fro m 0.3 mic ro ns to 0.63 mic ro ns

maximum wavelength

  • f range

distance modulus uncertainty (mag) target uncertainty

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What restframe wavelengths?

…And this also c o rre spo nds to the wave le ngth range whic h c apture s the main spe c tral fe ature s that have be e n studie d as abso lute magnitude indic ato rs.

RCa RSi

SiII

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Do we need visible‐wavelength detectors? For what redshifts can these standard restframe wavelengths be studied from the ground?

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F r

  • m the gr
  • und these

wavelengths can only be studied up to z ~ 0.5 or 0.6

wavelength (microns) atmospheric emission redshift

At what redshifts can these wavelengths be studied from the ground?

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At what redshifts can these wavelengths be studied from the ground?

Normalized Flux Observer Date (days)

100 200 300 400 1.0 0.5 0.0 1.0 0.5 0.0 1.0 0.5 0.0

z = 1.7 Restframe B Restframe V Restframe R

Normalized Flux

1.0 0.5 0.0 1.0 0.5 0.0 1.0 0.5 0.0

Observer Date (days)

50 100 150 200 250

Restframe B Restframe V Restframe R z = 1.2

SNAP

redshift

20-m Ground w/ NIR Camera

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What are factual elements that we can agree on that set the parameters of these programs? What calculations or compilations can be performed to establish them? What are the decisions in defining these programs that must be based on science “taste”? Are there any changes in circumstances or data that would influence these preferences? We can begin to organize these topics with the two types of questions:

1 2

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What are factual elements that we can agree on that set the parameters of these programs? What calculations or compilations can be performed to establish them?

1

For various error models, what are figures of merit as a function of number of SNe and their redshift distribution? What range of supernova absolute mag, stretch, color do we need to be able to study? What range of host galaxy environments? What are the best estimates of SN rate versus redshift? How many SNe can be studied with instruments that achieve a give Aperture x Solid Angle x Time? For various intrinsic color distributions and dust models, what color measurements (wavelength range and signal-to-noise) are needed to calibrate SNe? For various spectral features, what wavelength range, resolution, and signal-to- noise is required to calibrate SNe and (perhaps equivalently) constrain evolution models? Given these above measurement requirements, what can various specific instruments achieve over a given redshift range?

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Emphasis on larger numbers of SNe versus more detailed measurements for each SN. Emphasis on performing same restframe observations for the SNe at every redshift studied. When you have to start to degrade your experiment from the ideal, what would you give up first?

What are the decisions in defining these programs that must be based on science “taste”? Are there any changes in circumstances or data that would influence these preferences?

2