Cosmological Evolution of the Fine Structure Constant Chris Churchill (Penn State)  = e 2 /hc  = (  z -  0 )/  0 In collaboration with: J. Webb, M. Murphy, V.V. Flambaum, V.A. Dzuba, J.D. Barrow, J.X. Prochaska, & A.M. Wolfe

Your “Walk Away” Info 1.49 absorption cloud systems over redshifts 0.5–3.5 toward 28 QSOs compared to lab wavelengths for many transitions 2.2 different data sets; low-z (Mg II, Mg I, Fe II ) high-z (Si II, Cr II, Zn II, Ni II, Al II, Al III ) 3.Find  = (–0.72±0.18) × (4.1  ) (statistical) 4.Most important systematic errors are atmospheric dispersion (differential stretching of spectra) and isotopic abundance evolution (Mg & Si; slight shifting in transition wavelengths) 5.Correction for systematic errors yields stronger  evolution

Executive Summary 1.History/Motivations 2.Terrestrial and CMB/BBN 3.QSO Absorption Line Method 4.Doublet Method (DM) & Results 5.Many-Multiplet Method (MM) & Results 6.Statistical and Systematic Concerns 7.Concluding Remarks

Classes of Theories Attempts to solve some cosmological problems… Multi-dimensional and String Theories Scalar Theories Varying Speed of Light Theories Unification of quantum gravity with other forces… Couples E+M to cosmological mass density…

Varying Speed of Light Theories Motivation is to solve the “flatness” and “horizon” problems of cosmology generated by inflation theory (Barrow 1999). Theory allows variation in  to be ~10 -5 H 0 at redshift z=1, and ~10 -4 H 0 at z=1000 (near time of recombination). Magnitude of evolution is proportional to ratio of radiation to matter density.  c 2, where  is the cosmological constant, acts as a “stress”. Changes in c convert the  energy density into radiation (Barrow & Magueijo 2001)

Varying Speed of Light Theories  (z)/  (BBN) Theory allows variation in  to be ~10 -5 H 0 at redshift z=1, and ~10 -4 H 0 at z=1000 (near time of recombination). Magnitude of evolution is proportional to ratio of radiation to matter density. redshift, z

QSO absorption line methods can sample huge time span Savedoff (1965) used doublet separations of emission lines from galaxies to search for  evolution (first cosmological setting) Bahcall, Sargent & Schmidt (1967) used alkali-doublet (AD) separations seen in absorption in QSO spectra. QSO Absorption Lines (history)

Intrinisic QSO Emission/Absorption Lines

H I (Lyman-  )

C IV 1548, 1550 & Mg II 2796, 2803

We require high resolution spectra…

Interpreting those cloud-cloud separations….

Spectrum of multi-cloud Mg II system (z=1.32)

And, of course… Keck Twins 10-meter Mirrors The Weapon.

The High Resolution Echelle Spectrograph (HIRES)

2-Dimensional Echelle Image Dark features are absorption lines

Electron Energy and Atomic Configuration A change in  will lead to a change in the electron energy, , according to where Z is the nuclear charge, |E| is the ionization potential, j and l are the total and orbital angular momentum, and C(l,j) is the contribution to the relativistic correction from the many body effect in many electron elements. Note proportion to Z 2 (heavy elements have larger change) Note change in sign as j increases and C(l,j) dominates

The “Doublet Method” ex. Mg II 2796, 2803 A change in  will lead to a change in the doublet separation according to where (  ) z and (  ) 0 are the relative separations at redshift z and in the lab, respectively.  Si IV 1393,

We model the complex profiles as multiple clouds, using Voigt profile fitting (Lorentzian + Gaussian convolved) Free parameters are redshift, z, and  Lorentzian is natural line broadening Gaussian is thermal line broadening (line of sight)

Example of a Si IV system at z=2.53 used in the  analysis of Murphy et al (2001)

Si IV Doublet Results:  = –0.5  1.3 ×10 -5 (Murphy et al 2001)

E z = E c + Q 1 Z 2 [R 2 -1] + K 1 (LS)Z 2 R 2 + K 2 (LS) 2 Z 4 R 4 E c = energy of configuration center Q 1, K 1, K 2 = relativistic coefficients L = electron total orbital angular momentum S = electron total spin Z = nuclear charge R =  z /   The energy equation for a transition from the ground state at a redshift z, is written The “Many-Multiplet Method”

A convenient form is:  z =  0 + q 1 x + q 2 y  z = redshifted wave number x = (  z /  0 ) 2 - 1y = (  z /  0 )  0 = rest-frame wave number q 1, q 2 = relativistic correction coefficients for Z and e - configuration Mg II 2803 Mg II 2796 Fe II 2600 Fe II 2586 Fe II 2382 Fe II 2374 Fe II 2344

Typical accuracy is cm -1, a systematic shift in these values would introduce only a  ~ A precision of  ~ requires uncertainties in  0 no greater than 0.03 cm -1 (~0.3 km s -1 ) Well suited to data quality… we can centroid lines to 0.6 km s -1, with precision going as 0.6/N ½ km s -1 Anchors & Data Precision  Shifts for  ~ 10 -5

Advantages/Strengths of the MM Method 1.Inclusion of all relativistic corrections, including ground states, provides an order of magnitude sensitivity gain over AD method 2.In principle, all transitions appearing in QSO absorption systems are fair game, providing a statistical gain for higher precision constraints on  compared to AD method 3.Inclusion of transitions with wide range of line strengths provides greater constraints on velocity structure (cloud redshifts) 4.(very important) Allows comparison of transitions with positive and negative q 1 coefficients, which allows check on and minimization of systematic effects

Possible Systematic Errors 1.Laboratory wavelength errors 2.Heliocentric velocity variation 3.Differential isotopic saturation 4.Isotopic abundance variation (Mg and Si) 5.Hyperfine structure effects (Al II and Al III ) 6.Magnetic fields 7.Kinematic Effects 8.Wavelength mis-calibration 9.Air-vacuum wavelength conversion (high-z sample) 10.Temperature changes during observations 11.Line blending 12.Atmospheric dispersion effects 13.Instrumental profile variations

Isotopic Abundance Variations There are no observations of high redshift isotopic abundances, so there is no a priori information Focus on the “anchors” We re-computed  for entire range of isotopic abundances from zero to terrestrial. This provides a secure upper limit on the effect. Observations of Mg (Gay & Lambert 2000) and theoretical estimates of Si in stars (Timmes & Clayton 1996) show a metallicity dependence

CorrectedUncorrected This is because all Fe II are to blue of Mg II anchor and have same q 1 sign (positive) Leads to positive  For high-z data, Zn II and Cr II are To red of Si II and Ni II anchors and have opposite q 1 signs Correction for Isotopic Abundances Effect low-z Data

a = pixel size [Å],  = slit width arcsec/pix,  ψ = angular separation of  and 2 on slit, θ = angle of slit relative to zenith Atmospheric Dispersion Blue feature will have a truncated blue wing! Red feature will have a truncated red wing! This is similar to instrumental profile distortion, effectively a stretching of the spectrum Causes an effective stretching of the spectrum which mimics a non-zero 

Correction for Atmospheric Distortions Effect low-z Data CorrectedUncorrected This is because all Fe II are to blue of Mg II anchor and have same q 1 sign (positive) Leads to positive  For high-z data, Zn II and Cr II are To blue and red of Si II and Ni II anchors and have opposite q 1 signs

Summary of MM Method 1.49 absorption clouds systems over redshifts 0.5 to 3.5 toward 28 QSOs compared to lab wavelengths for many transitions 2.2 different data sets; low-z (Mg II, Mg I, Fe II ) high-z (Si II, Cr II, Zn II, Ni II, Al II, Al III ) 3.Find  = (–0.72±0.18) × (4.1  ) (statistical) 4.Most important systematic errors are atmospheric dispersion (differential stretching of spectra) and isotopic abundance evolution (Mg & Si; slight shifting in transition wavelengths) 5.Correction for systematic errors yields stronger  evolution

 = (–0.72±0.18) × (4.1  ) (statistical)

Hot off the Press Preliminary (yet confident) Findings… Now have a grand total of 138 systems due to adding the HIRES data of Sargent & Simcoe! Find  = (–0.65±0.11) × (6  ) (statistical) What We Need: The Future Same and new systems observed with different instrument and reduced/analyzed by different software and people. Our plans are to get UVES/VLT and HRS/HET spectra in order to reproduce the HIRES/Keck results

Multi-dimensional Unification Quantization of gravitational interactions… ,  weak,  strong, vary as inverse square of dimension scale Evolution of scale size of extra dimensions drives variability of coupling constants in the 4-dimensional subspace of Kaluza-Klein and superstring theories In M theory (all string theories are limiting cases), only the gravitational force acts in higher dimensions, while weak, strong, and electromagnetic act in 3 dimensional space (Arkani-Hamed 1998; Horava & Witten 1996) Measures of variation in ,  weak,  strong, constrains these theoretical scenarios

Scalar Theories Bekenstein (1982) introduced a scalar field that produces a space-time variation in electron charge (permittivity of free space). Reduces to Maxwell’s theory for constant . Variation in  coupled to matter density and is therefore well suited for astronomical testing (Livio & Stiavelli 1998). Requires assumptions- there is no single self-consistent scalar field theory incorporating varying  ; theoretical limits must all be quoted in conjuction with theoretical framework Bekenstein’s assumptions: covariance, gauge invariance, causality, time reversal of E+M, Robertson-Walker metric; Livio & Stiavelli depends on evolution of H and He mass fractions …

Terrestrial and Laboratory Constraints Clock rates based upon ultra-stable oscillators with relativistic corrections scaling as Z  2 Prestage, Robert, & Maleki (1995) used H-maser and Hg + to constrain  < 1.4 × Oklo phenomenon- natural fission reactor in Gabon, W Africa, occurred 1.8 Bya Note that this is at z=0 in Earth’s gravity field… Shlyakher (1976) and Damour & dyson (1996) used 150 Sm isotope to constrain  < 1.2 ×10 -7 Note that this is at z~0.1, is in Earth’s gravity field, and is model dependent… Non-cosmological environment nor detailed theory of space-time variation

Early Universe (CMB and BBN) The ionization history of the universe, either postponing (smaller  ) or delaying (larger  ) the redshift of recombination (z~1000). This would alter the ratio of baryons to photons and the amplitude and position of features in the CMB spectrum (Kujat & Scherrer 2000) However, electromagnetic contribution to p-n mass difference is very uncertain A different value of  would change: The electromagnetic coupling at time of nucleosynthesis (z~ ). Assuming  scales with p-n mass difference, 4 He abundance yields  /  < 9.9 ×10 -5 (Kolb et al 1986) ( implications )