18
A new result on space-time variation of alpha – Part C John Webb, School of Physics, University of New South Wales, Australia Group members as per Michael Murphy’s

A new result on space-time variation of alpha – Part C

  • Upload
    dawn

  • View
    30

  • Download
    0

Embed Size (px)

DESCRIPTION

A new result on space-time variation of alpha – Part C. John Webb, School of Physics, University of New South Wales , Australia. Group members as per Michael Murphy’s first slide. Two interesting internal consistencies: - PowerPoint PPT Presentation

Citation preview

Page 1: A new result on space-time variation of alpha – Part C

A new result on space-time variation of alpha – Part C

John Webb, School of Physics, University of New South Wales, Australia

Group members as per Michael Murphy’s first slide

Page 2: A new result on space-time variation of alpha – Part C

What are the key points which collectively suggest this result might be cosmological and not due to systematics?

Two interesting internal consistencies:

1 Keck and VLT dipole positions agree (although errors fairly large). Independent samples, different data reduction procedures, different instruments and telescopes.

2 High and low redshift dipole sky positions (using combined dataset) also agree - perhaps even more compelling because different species are used at low and high redshift – and different transitions respond differently to the same change in a.

And an interesting robustness indication:

3 Rather than increasing the statistical error bars to force c2n = 1, we can

instead iteratively trim the individual Da/a points relative to the dipole model. How much do we have to trim to destroy the result?

Page 3: A new result on space-time variation of alpha – Part C

aaaHighly exaggerated illustration of how transitions shift in different directions by different amounts – unique pattern

Page 4: A new result on space-time variation of alpha – Part C

Are a few high S/N outliers responsible for the signal, by chance?• Alternative to growing error bars• Robustness check – iterative trimming• Adopt statistical-only errors and iteratively clip most deviant point• How much data do we need to discard to remove the dipole and time dependence?

• c2n = 1 reached when ~10%

clipped• Dipole significance ~7s at c2

n = 1 • Dipole significance stays above 4s until ~50% of data discarded

• c2n = 1 reached when ~10% clipped

• Linear time fit significance ~5s at c2n =

1 • Linear time fit significance stays above 4s until ~40% of data discarded

Page 5: A new result on space-time variation of alpha – Part C

Can we nevertheless find a systematic which can reproduce these?

Two approaches:1) Identify all the systematics

one can possibly think of and quantify them one by one

2) Find a purely empirical approach which in principle measures both known and unknown simultaneously

Page 6: A new result on space-time variation of alpha – Part C

Alignment of quasar image on the spectrograph slit

Good Ok Not nice Nasty

Page 7: A new result on space-time variation of alpha – Part C

l[Å]3000 5500 8000

Time

l[Å]3000 5500 8000

Time

HIRES: Single arm, single chip (pre-Aug.'04)

UVES: Dual-arm, 3 chips

VLT/UVES vs. Keck/HIRES:

Page 8: A new result on space-time variation of alpha – Part C

l[Å]3000 5500 8000

Time

l[Å]3000 5500 8000

Time

HIRES: Single arm, single chip (pre-Aug.'04)

UVES: Dual-arm, 3 chips

VLT/UVES vs. Keck/HIRES:

Molaro et al. (A&A, 2008): UVES slits well aligned

Page 9: A new result on space-time variation of alpha – Part C

l[Å]3000 5500 8000

Time

l[Å]3000 5500 8000

Time

HIRES: Visitor mode, follow object with ThAr

UVES: Service mode, ThAr at end of night

Obj.Obj.

Cal.

Obj.Cal.

Cal.

Obj.Cal.

VLT/UVES vs. Keck/HIRES:

Page 10: A new result on space-time variation of alpha – Part C

To Earth

Quasar

Keck

VLT

7 quasars observed on both Keck and VLT – a direct test of combined systematics

Page 11: A new result on space-time variation of alpha – Part C

Comparing Da/a for 14 absorption systems observed with both Keck and VLT

Page 12: A new result on space-time variation of alpha – Part C

Pairs of quasar observations on both Keck and VLT

Page 13: A new result on space-time variation of alpha – Part C

~800 measurements, 7 quasar spectra observed on both Keck and VLT

Page 14: A new result on space-time variation of alpha – Part C

Same as previous plot but binned

Page 15: A new result on space-time variation of alpha – Part C

Implementing the dv test

fz,rest = f0 + Qα z

2

α 02 −1

⎛ ⎝ ⎜

⎞ ⎠ ⎟

fz,observed =f z,rest

1+ z( )

′ f z,rest = f0 +δf( ) + Qα z

2

α 02 −1

⎛ ⎝ ⎜

⎞ ⎠ ⎟

where

δf = −dvλ 0

⎛ ⎝ ⎜

⎞ ⎠ ⎟

then

′ f z,observed =f z,rest

1+ z( )

No systematic – standard laboratory frequencies:

Worst-case systematic – Modify the laboratory frequency:

Page 16: A new result on space-time variation of alpha – Part C

With

dv

syst

emati

cN

o dv

syst

emati

c ap

plie

dBefore and after

Page 17: A new result on space-time variation of alpha – Part C

Conclusions• The “raw” data might now be indicating both time and space

variation of alpha. • The quasar pair test results represent an upper limit on any effect.

They do not provide a "correction” to the raw results. We do not expect this in the sample as a whole.

• Nevertheless, if we do impose such an extreme effect on the whole raw dataset, it does not generate a solution in which Da/a is constant.

• Further, imposing the effect slightly diminishes the previous internal consistency in the data, as would be expected if the dipole is real.

• Specifically, the significance of the dipole reduces (although still remains fairly significant) and we then also require a more significant monopole term (which may seem "unphysical").

• Finally, we have so far been unable to find a way of explaining the results in terms of any known (or even unknown) systematics.

Page 18: A new result on space-time variation of alpha – Part C

Further work

• Need completely independent check. Meanwhile, continue with quasar spectroscopy – will double the existing sample within ~3 years

• Also targeted observations:

?

?

• Need more duplicate observations on both Keck and VLT• Also really need more H2 absorption systems. • Other combinations of lines, e.g. HI 21cm + neutral.