TY - JOUR A1 - Whittingham, Joseph A1 - Sparre, Martin A1 - Pfrommer, Christoph A1 - Pakmor, Rüdiger T1 - The impact of magnetic fields on cosmological galaxy mergers BT - I. Reshaping gas and stellar discs JF - Monthly notices of the Royal Astronomical Society N2 - Mergers play an important role in galaxy evolution. In particular, major mergers are able to have a transformative effect on galaxy morphology. In this paper, we investigate the role of magnetic fields in gas-rich major mergers. To this end, we run a series of high-resolution magnetohydrodynamic (MHD) zoom-in simulations with the moving-mesh code arepo and compare the outcome with hydrodynamic simulations run from the same initial conditions. This is the first time that the effect of magnetic fields in major mergers has been investigated in a cosmologically consistent manner. In contrast to previous non-cosmological simulations, we find that the inclusion of magnetic fields has a substantial impact on the production of the merger remnant. Whilst magnetic fields do not strongly affect global properties, such as the star formation history, they are able to significantly influence structural properties. Indeed, MHD simulations consistently form remnants with extended discs and well-developed spiral structure, whilst hydrodynamic simulations form more compact remnants that display distinctive ring morphology. We support this work with a resolution study and show that whilst global properties are broadly converged across resolution and physics models, morphological differences only develop given sufficient resolution. We argue that this is due to the more efficient excitement of a small-scale dynamo in higher resolution simulations, resulting in a more strongly amplified field that is better able to influence gas dynamics. KW - MHD KW - methods: numerical KW - galaxies: interactions KW - galaxies: magnetic KW - fields Y1 - 2021 U6 - https://doi.org/10.1093/mnras/stab1425 SN - 0035-8711 SN - 1365-2966 VL - 506 IS - 1 SP - 229 EP - 255 PB - Oxford Univ. Press CY - Oxford ER - TY - JOUR A1 - Werhahn, Maria A1 - Pfrommer, Christoph A1 - Girichidis, Philipp A1 - Puchwein, Ewald A1 - Pakmor, Rüdiger T1 - Cosmic rays and non-thermal emission in simulated galaxies BT - I. Electron and proton spectra compared to Voyager-1 data JF - Monthly notices of the Royal Astronomical Society N2 - Current-day cosmic ray (CR) propagation studies use static Milky Way models and fit parametrized source distributions to data. Instead, we use three-dimensional magnetohydrodynamic (MHD) simulations of isolated galaxies with the moving-mesh code arepo that self-consistently accounts for hydrodynamic effects of CR protons. In post-processing, we calculate their steady-state spectra, taking into account all relevant loss processes. We show that this steady-state assumption is well justified in the disc and generally for regions that emit non-thermal radio and gamma rays. Additionally, we model the spectra of primary electrons, accelerated by supernova remnants, and secondary electrons and positrons produced in hadronic CR proton interactions with the gas. We find that proton spectra above 10 GeV only weakly depend on galactic radius, while they acquire a radial dependence at lower energies due to Coulomb interactions. Radiative losses steepen the spectra of primary CR electrons in the central galactic regions, while diffusive losses dominate in the outskirts. Secondary electrons exhibit a steeper spectrum than primaries because they originate from the transported steeper CR proton spectra. Consistent with Voyager-1 and AMS-02 data, our models (i) show a turnover of proton spectra below GeV energies due to Coulomb interactions so that electrons start to dominate the total particle spectra and (ii) match the shape of the positron fraction up to 10 GeV. We conclude that our steady-state CR modelling in MHD CR galaxy simulations is sufficiently realistic to capture the dominant transport effects shaping their spectra, arguing for a full MHD treatment to accurately model CR transport in the future. KW - astroparticle physics KW - MHD KW - methods: numerical KW - cosmic rays KW - local KW - interstellar matter Y1 - 2021 U6 - https://doi.org/10.1093/mnras/stab1324 SN - 0035-8711 SN - 1365-2966 VL - 505 IS - 3 SP - 3273 EP - 3294 PB - Oxford University Press CY - Oxford ER - TY - JOUR A1 - Werhahn, Maria A1 - Pfrommer, Christoph A1 - Girichidis, Philipp T1 - Cosmic rays and non-thermal emission in simulated galaxies - III. Probing cosmic-ray calorimetry with radio spectra and the FIR-radio correlation JF - Monthly notices of the Royal Astronomical Society N2 - An extinction-free estimator of the star formation rate (SFR) of galaxies is critical for understanding the high-redshift universe. To this end, the nearly linear, tight correlation of far-infrared (FIR), and radio luminosity of star-forming galaxies is widely used. While the FIR is linked to massive star formation, which also generates shock-accelerated cosmic-ray (CR) electrons and radio synchrotron emission, a detailed understanding of the underlying physics is still lacking. Hence, we perform three-dimensional magnetohydrodynamical (MHD) simulations of isolated galaxies over a broad range of halo masses and SFRs using the moving-mesh code AREPO, and evolve the CR proton energy density self-consistently. In post-processing, we calculate the steady-state spectra of primary, shock-accelerated and secondary CR electrons, which result from hadronic CR proton interactions with the interstellar medium. The resulting total radio luminosities correlate with the FIR luminosities as observed and are dominated by primary CR electrons if we account for anisotropic CR diffusion. The increasing contribution of secondary emission up to 30 per cent in starbursts is compensated by the larger bremsstrahlung and Coulomb losses. CR electrons are in the calorimetric limit and lose most of their energy through inverse Compton interactions with star light and cosmic microwave background (CMB) photons while less energy is converted into synchrotron emission. This implies steep steady-state synchrotron spectra in starbursts. Interestingly, we find that thermal free-free emission flattens the total radio spectra at high radio frequencies and reconciles calorimetric theory with observations while free-free absorption explains the observed low-frequency flattening towards the central regions of starbursts. KW - MHD KW - methods: numerical KW - cosmic rays KW - galaxies: magnetic fields KW - galaxies: starburst KW - radio continuum: galaxies Y1 - 2021 U6 - https://doi.org/10.1093/mnras/stab2535 SN - 0035-8711 SN - 1365-2966 VL - 508 IS - 3 SP - 4072 EP - 4095 PB - Oxford Univ. Press CY - Oxford ER - TY - JOUR A1 - Valori, Gherarod A1 - Demoulin, Pascal A1 - Pariat, E. A1 - Masson, S. T1 - Accuracy of magnetic energy computations JF - Astronomy and astrophysics : an international weekly journal N2 - Context. For magnetically driven events, the magnetic energy of the system is the prime energy reservoir that fuels the dynamical evolution. In the solar context, the free energy (i.e., the energy in excess of the potential field energy) is one of the main indicators used in space weather forecasts to predict the eruptivity of active regions. A trustworthy estimation of the magnetic energy is therefore needed in three-dimensional (3D) models of the solar atmosphere, e. g., in coronal fields reconstructions or numerical simulations. Aims. The expression of the energy of a system as the sum of its potential energy and its free energy (Thomson's theorem) is strictly valid when the magnetic field is exactly solenoidal. For numerical realizations on a discrete grid, this property may be only approximately fulfilled. We show that the imperfect solenoidality induces terms in the energy that can lead to misinterpreting the amount of free energy present in a magnetic configuration. Methods. We consider a decomposition of the energy in solenoidal and nonsolenoidal parts which allows the unambiguous estimation of the nonsolenoidal contribution to the energy. We apply this decomposition to six typical cases broadly used in solar physics. We quantify to what extent the Thomson theorem is not satisfied when approximately solenoidal fields are used. Results. The quantified errors on energy vary from negligible to significant errors, depending on the extent of the nonsolenoidal component of the field. We identify the main source of errors and analyze the implications of adding a variable amount of divergence to various solenoidal fields. Finally, we present pathological unphysical situations where the estimated free energy would appear to be negative, as found in some previous works, and we identify the source of this error to be the presence of a finite divergence. Conclusions. We provide a method of quantifying the effect of a finite divergence in numerical fields, together with detailed diagnostics of its sources. We also compare the efficiency of two divergence-cleaning techniques. These results are applicable to a broad range of numerical realizations of magnetic fields. KW - magnetic fields KW - methods: numerical KW - Sun: surface magnetism KW - Sun: corona Y1 - 2013 U6 - https://doi.org/10.1051/0004-6361/201220982 SN - 0004-6361 VL - 553 IS - 2 PB - EDP Sciences CY - Les Ulis ER - TY - JOUR A1 - Thomas, Timon A1 - Pfrommer, Christoph A1 - Pakmor, Rüdiger T1 - A finite volume method for two-moment cosmic ray hydrodynamics on a moving mesh JF - Monthly notices of the Royal Astronomical Society N2 - We present a new numerical algorithm to solve the recently derived equations of two-moment cosmic ray hydrodynamics (CRHD). The algorithm is implemented as a module in the moving mesh AREPO code. Therein, the anisotropic transport of cosmic rays (CRs) along magnetic field lines is discretized using a path-conservative finite volume method on the unstructured time-dependent Voronoi mesh of AREPO. The interaction of CRs and gyroresonant Alfven waves is described by short time-scale source terms in the CRHD equations. We employ a custom-made semi-implicit adaptive time stepping source term integrator to accurately integrate this interaction on the small light-crossing time of the anisotropic transport step. Both the transport and the source term integration step are separated from the evolution of the magnetohydrodynamical equations using an operator split approach. The new algorithm is tested with a variety of test problems, including shock tubes, a perpendicular magnetized discontinuity, the hydrodynamic response to a CR overpressure, CR acceleration of a warm cloud, and a CR blast wave, which demonstrate that the coupling between CR and magnetohydrodynamics is robust and accurate. We demonstrate the numerical convergence of the presented scheme using new linear and non-linear analytic solutions. KW - hydrodynamics KW - MHD KW - methods: numerical KW - cosmic rays Y1 - 2021 U6 - https://doi.org/10.1093/mnras/stab397 SN - 0035-8711 SN - 1365-2966 VL - 503 IS - 2 SP - 2242 EP - 2264 PB - Oxford University Press CY - Oxford ER - TY - THES A1 - Thomas, Timon T1 - Cosmic-ray hydrodynamics: theory, numerics, applications T1 - Hydrodynamik der kosmischen Strahlung: Theorie, Numerik, Anwendungen N2 - Cosmic rays (CRs) are a ubiquitous and an important component of astrophysical environments such as the interstellar medium (ISM) and intracluster medium (ICM). Their plasma physical interactions with electromagnetic fields strongly influence their transport properties. Effective models which incorporate the microphysics of CR transport are needed to study the effects of CRs on their surrounding macrophysical media. Developing such models is challenging because of the conceptional, length-scale, and time-scale separation between the microscales of plasma physics and the macroscales of the environment. Hydrodynamical theories of CR transport achieve this by capturing the evolution of CR population in terms of statistical moments. In the well-established one-moment hydrodynamical model for CR transport, the dynamics of the entire CR population are described by a single statistical quantity such as the commonly used CR energy density. In this work, I develop a new hydrodynamical two-moment theory for CR transport that expands the well-established hydrodynamical model by including the CR energy flux as a second independent hydrodynamical quantity. I detail how this model accounts for the interaction between CRs and gyroresonant Alfvén waves. The small-scale magnetic fields associated with these Alfvén waves scatter CRs which fundamentally alters CR transport along large-scale magnetic field lines. This leads to the effects of CR streaming and diffusion which are both captured within the presented hydrodynamical theory. I use an Eddington-like approximation to close the hydrodynamical equations and investigate the accuracy of this closure-relation by comparing it to high-order approximations of CR transport. In addition, I develop a finite-volume scheme for the new hydrodynamical model and adapt it to the moving-mesh code Arepo. This scheme is applied using a simulation of a CR-driven galactic wind. I investigate how CRs launch the wind and perform a statistical analysis of CR transport properties inside the simulated circumgalactic medium (CGM). I show that the new hydrodynamical model can be used to explain the morphological appearance of a particular type of radio filamentary structures found inside the central molecular zone (CMZ). I argue that these harp-like features are synchrotron-radiating CRs which are injected into braided magnetic field lines by a point-like source such as a stellar wind of a massive star or a pulsar. Lastly, I present the finite-volume code Blinc that uses adaptive mesh refinement (AMR) techniques to perform simulations of radiation and magnetohydrodynamics (MHD). The mesh of Blinc is block-structured and represented in computer memory using a graph-based approach. I describe the implementation of the mesh graph and how a diffusion process is employed to achieve load balancing in parallel computing environments. Various test problems are used to verify the accuracy and robustness of the employed numerical algorithms. N2 - Kosmische Strahlung (CR) ist ein allgegenwärtiger und wichtiger Bestandteil astrophysikalischer Umgebungen wie des interstellaren Mediums (ISM) und des Intracluster-Mediums (ICM). Ihre plasmaphysikalischen Wechselwirkungen mit elektromagnetischen Feldern beeinflussen ihre Transporteigenschaften weitgehend. Effektive Modelle, die die Mikrophysik des CR-Transports einbeziehen, sind erforderlich, um die Auswirkungen von CRs auf die sie umgebenden makrophysikalischen Medien zu untersuchen. Die Entwicklung solcher Modelle ist eine Herausforderung, aufgrund der konzeptionellen, Längenskalen-, und Zeitskalen-Unterschiede zwischen den Mikroskalen der Plasmaphysik und den Makroskalen der Umgebung. Hydrodynamische Theorien des CR-Transports erreichen dies, indem sie die Entwicklung der CR-Population in Form von statistischen Momenten erfassen. Im etablierten hydrodynamischen Ein-Moment Modell für den CR-Transport wird die Dynamik der gesamten CR-Population durch eine einzige statistische Größe wie der häufig verwendeten CR-Energiedichte beschrieben. In dieser Arbeit entwickle ich eine neue hydrodynamische Zwei-Momenten Theorie für den CR-Transport, die das etablierte hydrodynamische Modell um den CR-Energiefluss als zweite unabhängige hydrodynamische Größe erweitert. Ich erläutere, wie dieses Modell die Wechselwirkung zwischen CRs und gyroresonanten Alfvén-Wellen berücksichtigt. Die mit diesen Alfvén-Wellen verbundenen kleinskaligen Magnetfelder streuen die CRs, was den CR-Transport entlang großskaligen Magnetfeldlinien grundlegend verändert. Dies führt zu den CR-Strömungs-und Diffusioneffekten, welche beide in der neu vorgestellten hydrodynamischen Theorie erfasst werden. Ich verwende eine adaptierte Eddington Näherung, um die hydrodynamischen Gleichungen zu schließen und untersuche die Genauigkeit dieser Näherung, indem ich sie mit Näherungen höherer Ordnung für den CR-Transport vergleiche. Darüber hinaus entwickle ich ein Finite-Volumen-Schema für das neue hydrodynamische Modell und passe es an den mitbewegten Gitter Code Arepo an. Dieses Schema wird mittels einer Simulation eines CR-getriebenen galaktischen Windes angewendet. Ich untersuche, wie CRs den Wind beschleunigen und führe eine statistische Analyse der CR-Transporteigenschaften innerhalb des simulierten zirkumgalaktischen Mediums (CGM) durch. Ich zeige, dass das neue hydrodynamische Modell das morphologische Erscheinungsbild eines neu-entdeckten bestimmten Typs von filamentartigen Radiostrukturen, welcher in der zentralen molekularen Zone (CMZ) auffindbar ist, erklären kann. Ich schlage vor, dass es sich bei diesen harfenartigen Strukturen um synchrotronstrahlende CRs handelt, die zuvor von einer punktförmigen Quelle wie dem stellaren Wind eines massereichen Sterns oder eines Pulsars in geflochtene Magnetfeldlinien injiziert wurden. Schließlich stelle ich den Finite-Volumen-Code Blinc vor, der adaptive Gitterverfeinerungstechniken (AMR) verwendet, um Simulationen von Strahlungs-und Magnetohydrodynamik (MHD) durchzuführen. Das Gitter von Blinc ist blockstrukturiert und wird im Computerspe-icher mittels eines graphbasierten Ansatzes dargestellt. Ich beschreibe die Implementierung des Gittergraphen und wie ein Diffusionsprozess eingesetzt wird, um einen Lastausgleich in parallelen Rechenumgebungen zu erreichen. Verschiedene Testprobleme werden verwendet, um die Genauigkeit und Robustheit der verwendeten numerischen Algorithmen zu überprüfen. KW - cosmic rays KW - hydrodynamics KW - radiative transfer KW - methods: analytical KW - methods: numerical KW - Galactic center KW - Non-thermal radiation sources KW - galaktisches Zentrum KW - Quellen nichtthermischer Strahlung KW - kosmische Strahlung KW - Hydrodynamik KW - Methoden: analytisch KW - Methoden: numerisch KW - Strahlungstransport Y1 - 2022 U6 - http://nbn-resolving.de/urn/resolver.pl?urn:nbn:de:kobv:517-opus4-563843 ER - TY - JOUR A1 - Thomas, T. A1 - Pfrommer, Christoph T1 - Cosmic-ray hydrodynamics BT - alfvén-wave regulated transport of cosmic rays JF - Monthly notices of the Royal Astronomical Society N2 - Star formation in galaxies appears to be self-regulated by energetic feedback processes. Among the most promising agents of feedback are cosmic rays (CRs), the relativistic ion population of interstellar and intergalactic plasmas. In these environments, energetic CRs are virtually collisionless and interact via collective phenomena mediated by kinetic-scale plasma waves and large-scale magnetic fields. The enormous separation of kinetic and global astrophysical scales requires a hydrodynamic description. Here, we develop a new macroscopic theory for CR transport in the self-confinement picture, which includes CR diffusion and streaming. The interaction between CRs and electromagnetic fields of Alfvenic turbulence provides the main source of CR scattering, and causes CRs to stream along the magnetic field with the Alfven velocity if resonant waves are sufficiently energetic. However, numerical simulations struggle to capture this effect with current transport formalisms and adopt regularization schemes to ensure numerical stability. We extent the theory by deriving an equation for the CRmomentum density along the mean magnetic field and include a transport equation for the Alfven-wave energy. We account for energy exchange of CRs and Alfven waves via the gyroresonant instability and include other wave damping mechanisms. Using numerical simulations, we demonstrate that our new theory enables stable, self-regulated CR transport. The theory is coupled to magnetohydrodynamics, conserves the total energy and momentum, and correctly recovers previous macroscopic CR transport formalisms in the steady-state flux limit. Because it is free of tunable parameters, it holds the promise to provide predictable simulations of CR feedback in galaxy formation. KW - hydrodynamics KW - radiative transfer KW - methods: analytical KW - methods: numerical KW - cosmic rays Y1 - 2019 U6 - https://doi.org/10.1093/mnras/stz263 SN - 0035-8711 SN - 1365-2966 VL - 485 IS - 3 SP - 2977 EP - 3008 PB - Oxford Univ. Press CY - Oxford ER - TY - JOUR A1 - Tepper-Garcia, Thorsten A1 - Richter, Philipp A1 - Schaye, Joop A1 - Booth, C. M. A1 - Vecchia, Claudio Dalla A1 - Theuns, Tom A1 - Wiersma, Robert P. C. T1 - Absorption signatures of warm-hot gas at low redshift o vi JF - Monthly notices of the Royal Astronomical Society N2 - We investigate the origin and physical properties of O vi absorbers at low redshift (z = 0.25) using a subset of cosmological, hydrodynamical simulations from the OverWhelmingly Large Simulations (OWLS) project. Intervening O vi absorbers are believed to trace shock-heated gas in the warm-hot intergalactic medium (WHIM) and may thus play a key role in the search for the missing baryons in the present-day Universe. When compared to observations, the predicted distributions of the different O vi line parameters (column density, Doppler parameter, rest equivalent width W-r) from our simulations exhibit a lack of strong O vi absorbers, a discrepancy that has also been found by Oppenheimer & Dave. This suggests that physical processes on subgrid scales (e.g. turbulence) may strongly influence the observed properties of O vi systems. We find that the intervening O vi absorption arises mainly in highly metal enriched (10-1 < Z/Z(circle dot) less than or similar to 1) gas at typical overdensities of 1 < /<<>> less than or similar to 102. One-third of the O vi absorbers in our simulation are found to trace gas at temperatures T < 105 K, while the rest arises in gas at higher temperatures, most of them around T = 105.3 +/- 0.5 K. These temperatures are much higher than inferred by Oppenheimer & Dave, probably because that work did not take the suppression of metal-line cooling by the photoionizing background radiation into account. While the O vi resides in a similar region of (, T)-space as much of the shock-heated baryonic matter, the vast majority of this gas has a lower metal content and does not give rise to detectable O vi absorption. As a consequence of the patchy metal distribution, O vi absorbers in our simulations trace only a very small fraction of the cosmic baryons (< 2 per cent) and the cosmic metals. Instead, these systems presumably trace previously shock-heated, metal-rich material from galactic winds that is now mixing with the ambient gas and cooling. The common approach of comparing O vi and H i column densities to estimate the physical conditions in intervening absorbers from QSO observations may be misleading, as most of the H i (and most of the gas mass) is not physically connected with the high-metallicity patches that give rise to the O vi absorption. KW - methods: numerical KW - galaxies: formation KW - intergalactic medium KW - quasars: absorption lines KW - cosmology: theory Y1 - 2011 U6 - https://doi.org/10.1111/j.1365-2966.2010.18123.x SN - 0035-8711 VL - 413 IS - 1 SP - 190 EP - 212 PB - Wiley-Blackwell CY - Hoboken ER - TY - JOUR A1 - Tepper-Garcia, Thorsten A1 - Richter, Philipp A1 - Schaye, Joop A1 - Booth, C. M. A1 - Dalla Vecchia, Claudio A1 - Theuns, Tom T1 - Absorption signatures of warm-hot gas at low redshift: broad H?i Lya absorbers JF - Monthly notices of the Royal Astronomical Society N2 - We investigate the physical state of H?i absorbing gas at low redshift (z = 0.25) using a subset of cosmological, hydrodynamic simulations from the OverWhelmingly Large Simulations project, focusing in particular on broad (bHI=40 km s-1) H?i Lya absorbers (BLAs), which are believed to originate in shock-heated gas in the warm-hot intergalactic medium (WHIM). Our fiducial model, which includes radiative cooling by heavy elements and feedback by supernovae and active galactic nuclei, predicts that by z = 0.25 nearly 60?per cent of the gas mass ends up at densities and temperatures characteristic of the WHIM and we find that half of this fraction is due to outflows. The standard H?i observables (distribution of H?i column densities NH?I, distribution of Doppler parameters bHI, bHINH?I correlation) and the BLA line number density predicted by our simulations are in remarkably good agreement with observations. BLAs arise in gas that is hotter, more highly ionized and more enriched than the gas giving rise to typical Lya forest absorbers. The majority of the BLAs arise in warm-hot [log?(T/?K) similar to 5] gas at low (log?? < 1.5) overdensities. On average, thermal broadening accounts for at least 60?per cent of the BLA linewidth, which in turn can be used as a rough indicator of the thermal state of the gas. Detectable BLAs account for only a small fraction of the true baryon content of the WHIM at low redshift. In order to detect the bulk of the mass in this gas phase, a sensitivity at least one order of magnitude better than achieved by current ultraviolet spectrographs is required. We argue that BLAs mostly trace gas that has been shock heated and enriched by outflows and that they therefore provide an important window on a poorly understood feedback process. KW - methods: numerical KW - galaxies: formation KW - intergalactic medium KW - quasars: absorption lines KW - cosmology: theory Y1 - 2012 U6 - https://doi.org/10.1111/j.1365-2966.2012.21545.x SN - 0035-8711 VL - 425 IS - 3 SP - 1640 EP - 1663 PB - Wiley-Blackwell CY - Hoboken ER - TY - JOUR A1 - Tepper-Garcia, Thor A1 - Richter, Philipp A1 - Schaye, Joop T1 - Absorption signatures of warm-hot gas at low redshift - ne viii JF - Monthly notices of the Royal Astronomical Society N2 - At z < 1 a large fraction of the baryons is thought to reside in diffuse gas that has been shock-heated to high temperatures (10 (5)-10 (6) K). Absorption by the 770.41, 780.32 A doublet of Ne viii in quasar spectra represents a unique tool to study this elusive warm-hot phase. We have developed an analytic model for the properties of Ne viii absorbers that allows for an inhomogeneous metal distribution. Our model agrees with the predictions of a simulation from the OverWhelmingly Large Simulations project indicating that the average line-of-sight metal-filling fraction within the absorbing gas is low (c(L) similar to 0.1). Most of the Ne viii in our model is produced in low-density, collisionally ionized gas (n(H) = 10(-6)-10(-4) cm(-3), T = 10 (5)-10 (6) K). Strong Ne viii absorbers (log(10)(N-NeVIII/cm(-2))14), like those recently detected by Hubble Space Telescope/Cosmic Origins Spectrograph, are found to arise in higher density gas (n(H) greater than or similar to 10(-4) cm(-3), T approximate to 5 x 10 (5) K). Ne viii cloudlets harbour only 1 per cent of the cosmic baryon budget. The baryon content of the surrounding gas (which has similar densities and temperatures as the Ne viii cloudlets) is a factor c(-1)L higher. We conclude that Ne viii absorbers are robust probes of shock-heated diffuse gas, but that spectra with signal-to-noise ratios S/N > 100 would be required to detect the bulk of the baryons in warm-hot gas. KW - methods: analytical KW - methods: numerical KW - galaxies: formation KW - intergalactic medium KW - quasars: absorption lines KW - cosmology: theory Y1 - 2013 U6 - https://doi.org/10.1093/mnras/stt1712 SN - 0035-8711 SN - 1365-2966 VL - 436 IS - 3 SP - 2063 EP - 2081 PB - Oxford Univ. Press CY - Oxford ER -