GLOBAL KNOWLEDGE ARK

Cosmology · Consistency, tensions and claims of new physics

Comparing structure-growth estimates

Separate bias, growth response and matter-power amplitude in a supplied linear redshift-space model before comparing inferred growth quantities.

Preparation: ratios, powers of ten and ordinary arithmetic. Physical quantities and notation are introduced as they are needed.

Back to the chapter

After reading, you can

  • Distinguish a power amplitude from a growth response and tracer bias.
  • Derive an exact degeneracy in a supplied angular power spectrum.
  • State the assumptions needed to compare structure-growth estimates.
01

A growth estimate refers to a defined response

A clustering measurement does not directly label every contribution as matter amplitude, tracer bias or growth rate. Inferring these quantities requires a relation between matter, velocities and the measured tracer.

In a linear single-growth-factor description, write the positive growth factor as D(a) and its logarithmic derivative as f = d ln D/d ln a. The value of f at one epoch does not specify the full history D(a).

A comparison must also match scale, epoch, calibration and the quantity being estimated. An amplitude at one wavenumber, a smoothed variance and a growth-rate product are different summaries.

The following supplied ensemble-power model illustrates an exact degeneracy. Its numbers are teaching inputs and carry no observed growth discrepancy, uncertainty distribution or empirical likelihood.

02

Follow density and velocity into redshift space

At one epoch and one fixed positive comoving wavenumber k, assume linear perturbations, the plane-parallel limit, irrotational velocities, deterministic tracer bias δ_g = bδ_m and no velocity bias. Take b>0 and f≥0.

Use the linear continuity relation θ_v = −fδ_m, with the dimensionless velocity-divergence normalization absorbed into θ_v. For direction cosine μ to the line of sight, the redshift-space response is δ_s = (b+fμ²)δ_m.

For a homogeneous isotropic matter ensemble, define δ(k) = ∫d³x δ(x)e^(−ik·x) and ⟨δ(k)δ(k′)⟩ = (2π)³δ_D(k+k′)P_m(k). The Fourier coefficient has units of comoving volume and P_m has units of comoving m³.

It follows that P_s(k,μ) = (b+fμ²)²P_m(k). This ensemble-power relation is conditional on the stated linear response; no distribution of individual Fourier coefficients has been supplied.

03

The ideal angular response fixes two products

Choose a positive reference power P_ref(k) in the same units and define S = √[P_m(k)/P_ref(k)]. This S is a dimensionless amplitude at the selected k.

Supply the positive transverse amplitude T = √[P_s(k,0)/P_ref(k)] = 0.10 and radial amplitude R = √[P_s(k,1)/P_ref(k)] = 0.14. Then bS = 0.10 and fS = R−T = 0.04.

Consequently β = f/b = 0.4. These products determine the complete ideal angular power P_s/P_ref = (0.10+0.04μ²)² without separately determining b, f and S.

Different positive S values therefore give the same full angular curve when b and f change consistently. Treating the three cases below as three independently measured angular spectra would misrepresent their exact equality.

Three supplied factorizations of one identical angular power response
SP_m/P_refb = 0.10/Sf = 0.04/Sβ
1/25 = 0.041/6255/212/5
1/20 = 0.051/40024/52/5
2/25 = 0.084/6255/41/22/5
04

Square the amplitude to obtain the power

At μ = 0,1/2,1 the amplitude √(P_s/P_ref) is respectively 0.10,0.11,0.14. The corresponding power ratios are 0.0100,0.0121,0.0196.

At μ = 1/2, μ² = 1/4. The response is therefore 0.10+0.04/4 = 0.11 before squaring; replacing μ² with μ would give a different model.

P_m, P_s and P_ref all have comoving-volume units, so their ratios and S are dimensionless. S is neither a Fourier coefficient nor the real-space density contrast.

A small S does not by itself establish linearity because its magnitude depends on the chosen P_ref. Linearity and the validity of the velocity response are assumptions of this example, not consequences of its normalized numbers.

The common curve shared by all three factorizations
μμ²√(P_s/P_ref)P_s/P_ref
000.100.0100
1/21/40.110.0121
110.140.0196
One common angular power curve leaves factors undeterminedSupply a single fixed-comoving-wavenumber ideal linear plane-parallel ensemble-power response P_s/P_ref = (b+f μ²)² S², with positive b,S and f at least zero, deterministic density bias, no velocity bias and the stated linear irrotational density-velocity relation. S = √(P_m/P_ref) is a one-k amplitude ratio. The supplied endpoints fix bS = 0.10 and fS = 0.04, so every allowed factorization has the same P_s/P_ref = (0.10+0.04 μ²)² and β = f/b = 2/5. One solid blue curve with hollow circles is plotted; it represents all three cases rather than pretending they are separated fits. The horizontal linear μ axis runs from 0 to 1, with μ the cosine to the line of sight. The zero-based vertical linear dimensionless power-ratio axis runs from 0 to 0.022. At μ = 0, 1/2, 1, marked amplitudes are respectively 0.10, 0.11, 0.14 and their squared powers are 0.0100, 0.0121, 0.0196. The native table lists (S,b,f,bS,fS) = (1/25,5/2,1,1/10,1/25), (1/20,2,4/5,1/10,1/25), (2/25,5/4,1/2,1/10,1/25). Their P_m/P_ref ratios are 1/625, 1/400 and 4/625. With the stated spatial Fourier convention the separate P_m,P_s,P_ref carry comoving volume units, while all plotted ratios and b,f,S,μ are dimensionless. No Gaussian random-field law is supplied. A one-k S is not σ₈, S₈ or fσ₈; a real smoothed amplitude needs its full spectrum and window. Small S against arbitrary P_ref does not itself establish linearity. These one-epoch response decompositions are not three complete gravity or expansion histories, observed growth estimates, nonlinear survey fits or new-physics solutions. The directly labeled single curve, exact table and amplitude-versus-power values are readable without color.One angular power response, three factorizationsIdeal linear, plane-parallel, deterministic ensemble response.At one fixed comoving k, set S = √(P_m/P_ref) > 0.bS = 0.10 and fS = 0.04; β = f/b = 2/5.All three cases share this one curveVertical: P_s/P_ref · dimensionless00.0050.010.0150.0200.51μ · cosine to the line of sight · dimensionlessμ = 0, 1/2, 1: amplitude = 0.10, 0.11, 0.14;power = 0.0100, 0.0121, 0.0196.SbfbSfS1/255/211/101/251/2024/51/101/252/255/41/21/101/25The power is the square of the amplitude.One-k S is not σ₈, S₈ or a smoothing integral.These are one-epoch decompositions, not full cosmologies.No observed growth discrepancy or Gaussian field law.
Supply a single fixed-comoving-wavenumber ideal linear plane-parallel ensemble-power response P_s/P_ref = (b+f μ²)² S², with positive b,S and f at least zero, deterministic density bias, no velocity bias and the stated linear irrotational density-velocity relation. S = √(P_m/P_ref) is a one-k amplitude ratio. The supplied endpoints fix bS = 0.10 and fS = 0.04, so every allowed factorization has the same P_s/P_ref = (0.10+0.04 μ²)² and β = f/b = 2/5. One solid blue curve with hollow circles is plotted; it represents all three cases rather than pretending they are separated fits. The horizontal linear μ axis runs from 0 to 1, with μ the cosine to the line of sight. The zero-based vertical linear dimensionless power-ratio axis runs from 0 to 0.022. At μ = 0, 1/2, 1, marked amplitudes are respectively 0.10, 0.11, 0.14 and their squared powers are 0.0100, 0.0121, 0.0196. The native table lists (S,b,f,bS,fS) = (1/25,5/2,1,1/10,1/25), (1/20,2,4/5,1/10,1/25), (2/25,5/4,1/2,1/10,1/25). Their P_m/P_ref ratios are 1/625, 1/400 and 4/625. With the stated spatial Fourier convention the separate P_m,P_s,P_ref carry comoving volume units, while all plotted ratios and b,f,S,μ are dimensionless. No Gaussian random-field law is supplied. A one-k S is not σ₈, S₈ or fσ₈; a real smoothed amplitude needs its full spectrum and window. Small S against arbitrary P_ref does not itself establish linearity. These one-epoch response decompositions are not three complete gravity or expansion histories, observed growth estimates, nonlinear survey fits or new-physics solutions. The directly labeled single curve, exact table and amplitude-versus-power values are readable without color. Original Ark teaching model.
05

Additional information must break a defined degeneracy

An external constraint on S would select b and f within this ideal response. Without it, the measured products permit a family of factorizations. An additional observable helps only through a stated and tested response to the unknowns.

The selected-k amplitude S is not σ₈, which involves smoothing an entire matter power spectrum over a specified radius. It is also not S₈ or an empirically measured fσ₈.

Real comparisons must account for survey selection, geometry, nonlinear evolution, velocity effects, scale-dependent bias and shared calibration where relevant. Those additions require their own models and uncertainty treatment.

Changing the inferred f alone does not establish a gravity theory or a viable alternative growth history. A physical proposal must connect the expansion, perturbation and observational responses under coherent assumptions.

Worked reasoning

Recover one factorization and its angular power

For supplied S = 1/20, find b, f and P_s/P_ref at μ = 1/2.

  1. Use bS = 0.10 to obtain b = 2, and fS = 0.04 to obtain f = 4/5.
  2. At μ = 1/2, the normalized amplitude is S[b+f/4] = (1/20)(2+1/5) = 0.11.
  3. Square the amplitude: P_s/P_ref = 0.11² = 0.0121.

b = 2, f = 4/5, and the power ratio is 0.0121.

Try the reasoning

  1. What b and f give the same curve when S = 2/25?

    Show the answer and reasoning

    b = 5/4 and f = 1/2.

    The products remain bS = 1/10 and fS = 1/25.

  2. Does this one-k S equal a measured σ₈?

    Show the answer and reasoning

    No.

    σ₈ requires a specified smoothing integral over the matter power spectrum; the example supplies a ratio at one k.

  3. Does choosing another factorization establish a new theory of gravity?

    Show the answer and reasoning

    No.

    The factorization supplies no complete dynamics, growth history or additional observable predictions.

What to carry forward

  • Compare quantities defined at the same epoch and scale under stated responses.
  • An angular clustering response can determine products while leaving factors degenerate.
  • A selected-scale power amplitude is different from a smoothed variance or a physical explanation.

References

Sources supporting the explanations, physical distinctions and examples in this lesson.

  1. Testing cosmological structure formation using redshift-space distortionsWill J. Percival; Martin WhiteResearch paperarxiv.orgRead source