REVIEW
Magnetic Fields in the Early Universe
Astrophysics · Submitted 5 Sep 2000 · 233 references
Pith's verdict: A solid, useful synthesis of primordial magnetism whose one real weakness is that it never puts Ch. 2's required field strengths next to Ch. 4's predicted ones.
T0 · AI review
Why Pith says this
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Referee report
The paper
The paper claims
The magnetic fields of galaxies and clusters may be relics of the big bang, and the cosmic microwave background is the place to look for proof.
The reading
What carries the argument
The load-bearing tool is flux freezing: because the cosmic plasma is an excellent conductor, magnetic field lines are carried with the fluid and the field strength scales as $B(t)=B(t_i)(a(t_i)/a(t))^2$ (Eq. 1.24), so an early-universe field can be evolved forward to a present-day prediction and a present-day measurement can be run backwards to a primordial one. The companion quantity is magnetic helicity, $H = -1/(4πσ) ∫ d^3x B·(∇×B)$ in its evolution law, which is nearly conserved for the same reason, coincides with a Chern-Simons number, and can drive an inverse cascade that moves magnetic energy from small scales to large ones. For magnetogenesis at the electroweak scale, the argument turns on a gauge-invariant definition of the electromagnetic field strength in a background where the Higgs field direction varies in space, so that gradients of the Higgs phases act as electric currents and source real magnetic fields.
Extended reading notes
Core claim
The paper is a synthesis, and its central claim is a strategic one: that a primordial origin for galactic and cluster magnetic fields is a live alternative to dynamo amplification, and that the most promising way to settle the question is to look for the imprint of magnetic fields on the temperature and polarization anisotropies of the cosmic microwave background [abstract:s3]. The supporting case is that dynamo models require seed fields anyway, that cluster fields look too strong and too widespread to have been ejected from galaxies, and that microgauss fields at redshift of order one leave too little time for a dynamo to build them from nothing. If the claim holds, the fields are a cosmological relic rather than an astrophysical by-product, and their strength and coherence length today encode what happened at the quark-hadron and electroweak transitions. The review also assembles a second, independent handle: strong fields speed up the cosmic expansion and shift the weak freeze-out, so the observed helium and deuterium abundances bound the field to roughly $10^{13}$ G at $T=10^9$ K.
Load-bearing premise
Every present-day number in the review depends on assuming the field is frozen into the plasma and simply diluted as the universe expands, so that strength falls as the square of the scale factor and the coherence length is set by the same scaling.
Editorial extensions
If this is right
- A detected Faraday rotation of the microwave polarization of order a degree, at the level predicted for $B_0 \sim 10^{-9}$ G, would establish that a cosmologically coherent field existed at the last scattering surface.
- A measured parity-odd correlation between temperature and polarization (a nonzero $B$-mode cross term) would be direct evidence of a macroscopic parity violation of primordial origin, since an isotropic universe forbids it.
- Improved acoustic-peak data would tighten or exclude the extra energy density that a homogeneous field contributes, since the field raises the effective sound speed and suppresses the first peak.
- If the fields are primordial, the observed uniformity of galactic field strengths near a few microgauss becomes a record of the pre-galactic medium rather than of local dynamo physics.
- Magnetogenesis and baryogenesis stop being separate problems: a helical hypercharge field can process fermion number through the Abelian anomaly, so the same early-universe physics may have set both the field and the matter-antimatter asymmetry.
Reading between the lines
- The review's two constraints pull in different directions and are rarely compared directly: nucleosynthesis probes the field on scales of order the horizon at $T=10^9$ K (comoving ~100 pc), while the microwave background probes scales of order the last-scattering horizon and larger, so a detection in one channel need not confirm the other.
- If helical fields really do undergo an inverse cascade as the review describes, then the coherence length today is a clock as much as a length — measuring both the strength and the correlation length of a primordial field would constrain when it was made, not just how strong it was.
- The review's remark that strong fields may keep sphalerons active below the critical temperature suggests a testable corollary: a primordial field large enough to matter for the microwave background could also reopen the window for electroweak baryogenesis in a model where the transition is not strongly first order.
- Because the field-strength limits quoted today depend on dividing by an assumed coherence length to the power $p$ with $p$ between 1/2 and 3/2, a future measurement that pins the spectral index of the field would sharpen every existing bound by a comparable factor.
Original abstract
This review concerns the origin and the possible effects of magnetic fields in the early Universe. We start by providing to the reader with a short overview of the current state of art of observations of cosmic magnetic fields. We then illustrate the arguments in favour of a primordial origin of magnetic fields in the galaxies and in the clusters of galaxies. We argue that the most promising way to test this hypothesis is to look for possible imprints of magnetic fields on the temperature and polarization anisotropies of the cosmic microwave background radiation (CMBR). With this purpose in mind, we provide a review of the most relevant effects of magnetic fields on the CMBR. A long chapter of this review is dedicated to particle physics inspired models which predict the generation of magnetic fields during the early Universe evolution. Although it is still unclear if any of these models can really explain the origin of galactic and intergalactic magnetic fields, we show that interesting effects may arise anyhow. Among these effects, we discuss the consequences of strong magnetic fields on the big-bang nucleosynthesis, on the masses and couplings of the matter constituents, on the electroweak phase transition, and on the baryon and lepton number violating sphaleron processes. Several intriguing common aspects, and possible interplay, of magnetogenesis and baryogenesis are also dicussed.
The compiled record
The paper's own sentences, arranged, kept beside the review and separate from it. Each label is drawn from a closed vocabulary; the number beside it is the probability the classifier gave that label. Numbers in the tables are the authors', checked by code. No sentence in this record was written by a model.
The abstract, sentence by sentence
This review concerns the origin and the possible effects of magnetic fields in the early Universe. We start by providing to the reader with a short overview of the current state of art of observations of cosmic magnetic fields. We then illustrate the arguments in favour of a primordial origin of magnetic fields in the galaxies and in the clusters of galaxies. We argue that the most promising way to test this hypothesis is to look for possible imprints of magnetic fields on the temperature and polarization anisotropies of the cosmic microwave background radiation (CMBR). With this purpose in mind, we provide a review of the most relevant effects of magnetic fields on the CMBR. A long chapter of this review is dedicated to particle physics inspired models which predict the generation of magnetic fields during the early Universe evolution. Although it is still unclear if any of these models can really explain the origin of galactic and intergalactic magnetic fields, we show that interesting effects may arise anyhow. Among these effects, we discuss the consequences of strong magnetic fields on the big-bang nucleosynthesis, on the masses and couplings of the matter constituents, on the electroweak phase transition, and on the baryon and lepton number violating sphaleron processes. Several intriguing common aspects, and possible interplay, of magnetogenesis and baryogenesis are also dicussed.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | This review concerns the origin and the possible effects of magnetic fields in the early Universe. | background 0.60 | 0.12 | 0.05 | unclear 0.61 |
| s1 | We start by providing to the reader with a short overview of the current state of art of observations of cosmic magnetic fields. | background 0.61 | 0.39 | 0.02 | asserted 0.50 |
| s2 | We then illustrate the arguments in favour of a primordial origin of magnetic fields in the galaxies and in the clusters of galaxies. | contribution 0.83 | 0.32 | 0.07 | asserted 0.60 |
| s3 | We argue that the most promising way to test this hypothesis is to look for possible imprints of magnetic fields on the temperature and polarization anisotropies of the cosmic microwave background radiation (CMBR). | method 0.54 | 0.24 | 0.18 | asserted 0.59 |
| s4 | With this purpose in mind, we provide a review of the most relevant effects of magnetic fields on the CMBR. | contribution 0.88 | 0.41 | 0.04 | asserted 0.88 |
| s5 | A long chapter of this review is dedicated to particle physics inspired models which predict the generation of magnetic fields during the early Universe evolution. | contribution 0.87 | 0.36 | 0.03 | asserted 0.93 |
| s6 | Although it is still unclear if any of these models can really explain the origin of galactic and intergalactic magnetic fields, we show that interesting effects may arise anyhow. | limitation 0.70 | 0.52 | 0.12 | hedged possibility 0.94 |
| s7 | Among these effects, we discuss the consequences of strong magnetic fields on the big-bang nucleosynthesis, on the masses and couplings of the matter constituents, on the electroweak phase transition, and on the baryon and lepton number violating sphaleron processes. | contribution 0.97 | 0.20 | 0.06 | asserted 0.85 |
| s8 | Several intriguing common aspects, and possible interplay, of magnetogenesis and baryogenesis are also dicussed. | contribution 0.98 | 0.55 | 0.07 | hedged possibility 0.57 |
What was examined, and what was not
- arXiv listing abstract v2
- full text
- figures and tables
- references and citing sentences
- relations to other papers
- P abstract
- S sections
- T body sentences
- C citations
- R cross-paper relations
Figures
Showing 4 of the paper's 5 figures. See all figures in the PDF ↗ Figures reproduced from arXiv:astro-ph/0009061 by the authors.
References
How later papers used it
260 later papers cite it
2 later papers by other authors are listed below: 2 used its data or values.
Uses its data or values 2 of 8 papers with this label
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Also shown in the table are the emergent time $t_E$, the scale factor $a_E$ (at time $t_E$) and the non-linear parameter $β$ corresponding to the present day magnetic field $B_0 = 10^-10$ G [ref] .
Emergent Cosmology in Models of Nonlinear Electrodynamics (2022) · Slow-roll Parameters and CMB constaints · 0.97
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We similarly have no hard evidence for the existence of an intergalactic magnetic field, but our current measurements suggest that, if present, it was weaker than those found in galaxies, where $|B_G|∼3-4 μ$G [ref] .
A Pop III generated dust screen at z~16 (2022) · E-mode and B-mode polarization · 0.86
How the literature uses it
209 arXiv papers cite this in 294 sentences
Papers citing it · 136 sentences without a confident label
Uses its method or tool 1 paper
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Fourier decomposing the vector potential $A_i$ [ref] , we get
Hamiltonian formalism of cosmological perturbations and higher derivative theories · Breaking of conformal invariance and consequences · 0.85
Uses its data or values 7 papers
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Observations of the CMB limit the intensity of the magnetic seed fields to a current upper limit of $10^-9$ G [ref] .
Using Gravitational Waves to put limits on Primordial Magnetic Fields · Introduction · 0.88
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The overall constraint on the magnetic strength is $B≲10^11$ G at the time of nucleosynthesis, which (roughly) translates to $B≲7×10^-7$ G at the time of galaxy formation [ref] .
Primordial magnetogenesis · Nucleosynthesis limits · 0.86
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From Eq. ([ref]) and Eq. ([ref]) we can calculate the equation of state parameter as, [equation] where we set $B_0 = 10^-10$ Gauss [ref] .
Emergent Cosmology in Models of Nonlinear Electrodynamics · Emergent universe with NLED · 0.94
Cites it as background 123 papers
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The detection of the IGMF could provide important insights for solving outstanding problems of its origin and role in both the cosmology and astrophysics of structure formation [ref] .
Extreme TeV Blazars and Lower Limits on Intergalactic Magnetic Fields · Introduction · 0.82
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The proponents of this scenario suggest that the generation of seed fields can possibly occur due to processes in early universe during inflation [ref] , electroweak [ref] or QCD phase transitions [ref] (for reviews, see [ref] ).
Challenges in Inflationary Magnetogenesis: Constraints from Strong Coupling, Backreaction and the Schwinger Effect · Introduction · 0.97
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Most theories of cosmic magnetic field generation fall into one of three categories [ref] : 1) magnetic fields generated by phase transitions; 2) electromagnetic perturbations expanded by inflation; and 3) turbulent magnetofluid resulting in charge and current asymmetries.
Using Gravitational Waves to put limits on Primordial Magnetic Fields · Introduction · 0.95
Discussion
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