Skip to main content

Thank you for visiting nature.com. You are using a browser version with limited support for CSS. To obtain the best experience, we recommend you use a more up to date browser (or turn off compatibility mode in Internet Explorer). In the meantime, to ensure continued support, we are displaying the site without styles and JavaScript.

  • Letter
  • Published:

Core crystallization and pile-up in the cooling sequence of evolving white dwarfs

Abstract

White dwarfs are stellar embers depleted of nuclear energy sources that cool over billions of years1. These stars, which are supported by electron degeneracy pressure, reach densities of 107 grams per cubic centimetre in their cores2. It has been predicted that a first-order phase transition occurs during white-dwarf cooling, leading to the crystallization of the non-degenerate carbon and oxygen ions in the core, which releases a considerable amount of latent heat and delays the cooling process by about one billion years3. However, no direct observational evidence of this effect has been reported so far. Here we report the presence of a pile-up in the cooling sequence of evolving white dwarfs within 100 parsecs of the Sun, determined using photometry and parallax data from the Gaia satellite4. Using modelling, we infer that this pile-up arises from the release of latent heat as the cores of the white dwarfs crystallize. In addition to the release of latent heat, we find strong evidence that cooling is further slowed by the liberation of gravitational energy from element sedimentation in the crystallizing cores5,6,7. Our results describe the energy released by crystallization in strongly coupled Coulomb plasmas8,9, and the measured cooling delays could help to improve the accuracy of methods used to determine the age of stellar populations from white dwarfs10.

This is a preview of subscription content, access via your institution

Access options

Buy this article

Prices may be subject to local taxes which are calculated during checkout

Fig. 1: Effects of crystallization on the cooling of white dwarfs.
Fig. 2: Observational Gaia colour–magnitude Hertzsprung–Russell diagram for white dwarfs within 100 pc of the Sun.
Fig. 3: Observational Gaia Hertzsprung–Russell diagram for white dwarfs with SDSS spectra.
Fig. 4: Luminosity function for massive white dwarfs within 100 pc of the Sun.

Similar content being viewed by others

Data availability

The Gaia DR2 catalogue of white dwarfs used in this study is available from the University of Warwick astronomy catalogues repository, https://warwick.ac.uk/fac/sci/physics/research/astro/research/catalogues/gaia_dr2_white_dwarf_candidates_v2.csv. All modelling was performed with our extensive white-dwarf evolution code. We have opted not to make this multi-purpose code available, but the cooling sequences calculated for this work are available on request.

References

  1. Mestel, L. On the theory of white dwarf stars. I. The energy sources of white dwarfs. Mon. Not. R. Astron. Soc. 112, 583–597 (1952).

    Article  ADS  Google Scholar 

  2. Tassoul, M., Fontaine, G. & Winget, D. E. Evolutionary models for pulsation studies of white dwarfs. Astrophys. J. Suppl. Ser. 72, 335–386 (1990).

    Article  ADS  CAS  Google Scholar 

  3. van Horn, H. M. Crystallization of white dwarfs. Astrophys. J. 151, 227–238 (1968).

    Article  ADS  Google Scholar 

  4. Gaia Collaboration. Gaia Data Release 2. Summary of the contents and survey properties. Astron. Astrophys. 616, A1 (2018).

    Article  Google Scholar 

  5. Garcia-Berro, E., Hernanz, M., Mochkovitch, R. & Isern, J. Theoretical white-dwarf luminosity functions for two phase diagrams of the carbon-oxygen dense plasma. Astron. Astrophys. 193, 141–147 (1988).

    ADS  CAS  Google Scholar 

  6. Segretain, L. et al. Cooling theory of crystallized white dwarfs. Astrophys. J. 434, 641–651 (1994).

    Article  ADS  CAS  Google Scholar 

  7. Althaus, L. G., García-Berro, E., Isern, J., Córsico, A. H. & Miller Bertolami, M. M. New phase diagrams for dense carbon-oxygen mixtures and white dwarf evolution. Astron. Astrophys. 537, A33 (2012).

    Article  ADS  Google Scholar 

  8. Horowitz, C. J., Schneider, A. S. & Berry, D. K. Crystallization of carbon–oxygen mixtures in white dwarf stars. Phys. Rev. Lett. 104, 231101 (2010).

    Article  ADS  CAS  Google Scholar 

  9. Hughto, J. et al. Direct molecular dynamics simulation of liquid-solid phase equilibria for a three-component plasma. Phys. Rev. E 86, 066413 (2012).

    Article  ADS  CAS  Google Scholar 

  10. Winget, D. E., et al. An independent method for determining the age of the universe. Astrophys. J. 315, 77–81 (1987).

    Article  ADS  Google Scholar 

  11. Fontaine, G., Brassard, P. & Bergerson, P. The potential of white dwarf cosmochronology. Publ. Astron. Soc. Pacif. 113, 409–435 (2001).

    Article  ADS  Google Scholar 

  12. Obertas, A. et al. The onset of convective coupling and freezing in the white dwarfs of 47 Tucanae. Mon. Not. R. Astron. Soc. 474, 677–682 (2018).

    Article  ADS  Google Scholar 

  13. García-Berro, E. et al. A white dwarf cooling age of 8 Gyr for NGC 6791 from physical separation processes. Nature 465, 194–196 (2010).

    Article  ADS  Google Scholar 

  14. Bédard, A., Bergeron, P. & Fontaine, G. Measurements of physical parameters of white dwarfs: a test of the mass-radius relation. Astrophys. J. 848, 11 (2017).

    Article  ADS  Google Scholar 

  15. Gaia Collaboration. Gaia Data Release 2: observational Hertzsprung–Russell diagrams. Astron. Astrophys. 616, A10 (2018).

    Article  Google Scholar 

  16. Hansen, B. M. S. et al. The white dwarf cooling sequence of the globular cluster Messier 4. Astrophys. J. 574, L155–L158 (2002).

    Article  ADS  Google Scholar 

  17. Tremblay, P.-E., Kalirai, J. S., Soderblom, D. R., Cignoni, M. & Cummings, J. White dwarf cosmochronology in the solar neighborhood. Astrophys. J. 791, 92 (2014).

    Article  ADS  Google Scholar 

  18. Gentile Fusillo, N. P. et al. A Gaia Data Release 2 catalogue of white dwarfs and a comparison with SDSS. Mon. Not. R. Astron. Soc. 482, 4570–4591 (2019).

  19. Tremblay, P.-E., Ludwig, H.-G., Steffen, M. & Freytag, B. Spectroscopic analysis of DA white dwarfs with 3D model atmospheres. Astron. Astrophys. 559, A104 (2013).

    Article  Google Scholar 

  20. El-Badry, K., Rix, H.-W. & Weisz, D. R. An empirical measurement of the initial–final mass relation with Gaia white dwarfs. Astrophys. J. 860, L17 (2018).

    Article  ADS  Google Scholar 

  21. Chandrasekhar, S. The highly collapsed configurations of a stellar mass. (Second paper.) Mon. Not. R. Astron. Soc. 95, 207–225 (1935).

    Article  ADS  Google Scholar 

  22. Kleinman, S. J. et al. SDSS DR7 white dwarf catalog. Astrophys. J. Suppl. Ser. 204, 5 (2013).

    Article  ADS  Google Scholar 

  23. Bergeron, P., Saffer, R. A. & Liebert, J. A spectroscopic determination of the mass distribution of DA white dwarfs. Astrophys. J. 394, 228–247 (1992).

    Article  ADS  Google Scholar 

  24. Kalirai, J. S., Richer, H. B., Hansen, B. M. S., Reitzel, D. & Rich, R. M. The dearth of massive, helium-rich white dwarfs in young open star clusters. Astrophys. J. 618, L129–L132 (2005).

    Article  ADS  CAS  Google Scholar 

  25. Tremblay, P.-E. et al. On the evolution of magnetic white dwarfs. Astrophys. J. 812, 19 (2015).

    Article  ADS  Google Scholar 

  26. Kalirai, J. S. et al. Ultra-deep Hubble Space Telescope imaging of the small Magellanic cloud: the initial mass function of stars with M 1M . Astrophys. J. 763, 110 (2013).

    Article  ADS  Google Scholar 

  27. Bertelli, G., Nasi, E., Girardi, L. & Marigo, P. Scaled solar tracks and isochrones in a large region of the ZY plane. II. From 2.5 to 20 M stars. Astron. Astrophys. 508, 355–369 (2009).

    Article  ADS  Google Scholar 

  28. Potekhin, A. Y. & Chabrier, G. Equation of state of fully ionized electron–ion plasmas. II. Extension to relativistic densities and to the solid phase. Phys. Rev. E 62, 8554–8563 (2000).

    CAS  PubMed  Google Scholar 

  29. Marigo, P. Chemical yields from low- and intermediate-mass stars: model predictions and basic observational constraints. Astron. Astrophys. 370, 194–217 (2001).

    Article  ADS  CAS  Google Scholar 

  30. Mestel, L. & Ruderman, M. A. The energy content of a white dwarf and its rate of cooling. Mon. Not. R. Astron. Soc. 136, 27–38 (1967).

    Article  ADS  Google Scholar 

Download references

Acknowledgements

This research received funding from the European Research Council under the European Union’s Horizon 2020 research and innovation programme number 677706 (WD3D) and under the European Union’s Seventh Framework Programme (FP/2007- 2013)/ERC Grant Agreement number 320964 (WDTracer). This work made use of data from the European Space Agency (ESA) mission Gaia (https://www.cosmos.esa.int/gaia), processed by the Gaia Data Processing and Analysis Consortium (DPAC, https://www.cosmos.esa.int/web/gaia/dpac/consortium). Funding for the DPAC was provided by national institutions, in particular the institutions participating in the Gaia Multilateral Agreement. Support for J.J.H. was provided by NASA through Hubble Fellowship grant #HST-HF2-51357.001-A, awarded by the Space Telescope Science Institute, which is operated by the Association of Universities for Research in Astronomy, Inc., under NASA contract NAS5-26555.

Author information

Authors and Affiliations

Authors

Contributions

P.-E.T. and B.H.D. identified and characterized the empirical crystallization sequence. G.F. made the evolutionary white-dwarf models used in this work. N.P.G.F., M.A.H. and T.C. constructed the Gaia white-dwarf sample employed in this study and performed the cross-match with other photometric and spectroscopic surveys. P.-E.T., B.T.G., T.R.M., J.J.H. and G.F. wrote the text and developed the argument for a crystallization sequence. E.C. and T.C. characterized the accuracy of Gaia measurements and derived parameters for white dwarfs.

Corresponding author

Correspondence to Pier-Emmanuel Tremblay.

Ethics declarations

Competing interests

The authors declare no competing interests.

Additional information

Publisher’s note: Springer Nature remains neutral with regard to jurisdictional claims in published maps and institutional affiliations.

Source data

Rights and permissions

Reprints and permissions

About this article

Check for updates. Verify currency and authenticity via CrossMark

Cite this article

Tremblay, PE., Fontaine, G., Fusillo, N.P.G. et al. Core crystallization and pile-up in the cooling sequence of evolving white dwarfs. Nature 565, 202–205 (2019). https://doi.org/10.1038/s41586-018-0791-x

Download citation

  • Received:

  • Accepted:

  • Published:

  • Issue date:

  • DOI: https://doi.org/10.1038/s41586-018-0791-x

This article is cited by

Comments

Commenting on this article is now closed.

  1. The conclusions and observations seem plausible, and evidentiary.

    The underlying assumptions do not conform to physical observations.

    Very outdated assumptions, by the astronomy profession ... IMHPO

  2. The standard solar model is incorrect.

    Gravity will NOT COMPACT the core.

    Please see this article - http://www.teqnicraft.com/i...

  3. 20 years ago, a Nobel Prize was awarded for use of the Hubble Telescope,
    to measure the meteoric volume hitting the earth’s atmosphere. An immense
    volume of ICE is added to the earth each year, also stone meteors. It had
    previously been assumed that most meteors were metallic. However, the evidence indicates that the greatest meteoric mass is ice crystals, followed by stone meteors, and metallic meteors are the least mass which are added to the earth. Metal & stone meteors produced light flashes, and ripples, upon entering the earth's atmosphere. Ice crystals produced atmospheric ripples upon impact, but no light flashes from friction/heat.

    Ergo: Our Sun is receiving vast quantities of additional mass as it moves through the galaxy.

  4. Reportably (and plausibly) Our Solar System travels at an average velocity of 828,000 km/h (230 km/s) or 514,000 mph (143 mi/s) within its trajectory around the Milky Way galactic center, a speed at which an object could circumnavigate the Earth’s equator in 2 minutes and 54 seconds; that speed corresponds to approximately 1/1300 of the speed of light.

    And, I posit … The Sun is being refueled with VAST volumes/mass in the forms of ice, stone & metal meteors along the way. The Perseid meteor shower each August is our easiest vantage point to observe the solar refueling process. The solar output responds to this fueling, in presently undetermined ways.

  5. To properly study and predict the energy production of the Sun and the effect on Earth’s climate, we would need satellites on the leading edge of the Solar System, i.e. in front of the Sun. These satellites could monitor the matter being swept into the Sun, which presumably become its fuel. Leading and trailing solar satellites in the outer reaches of the Sun’s gravitational field, would give us a clearer ‘before and after picture of the mass added to the Sun each day, year, century.

    I posit that the Sun and other stars are dependent upon this continuing mass accretion process for fuel, and their: form, size, mass, thermal output, and color are quickly affected thereby.

  6. In the 1st order analysis, the refueling of the Sun seems to be critical to aging calculations.

    So, if the refueling is neglected, it is difficult to consider the analysis and projections to represent a serious effort.

  7. https://s22380.pcdn.co/wp-c...

  8. The sun (1 solar mass) has no mechanism to introduce new hydrogen into the core, where the fusion takes place. That is why it's lifetime is on the order of 10 billion years. In fact, the sun will only consume a tiny fraction of it's hydrogen during its lifetime.
    Contrast this to a red dwarf star of only 0.5 solar mass. This star is totally convective, which means it can supply the core with new H as it's used up. Because of this, not a single red dwarf start has ever died yet! Most will take hundreds of billions of year to exhaust their hydrogen. Stars with a mass of 0.4 solar mass will live to be something like 800 billions years or more!
    Also, the sun may accumulate mass as it orbits the center of the galaxy, but that accumulated material will never reach the core of the sun, so that process won't help to extend the life of the sun at all.

  9. Robert Potter,

    The penetration depth of the circulation into the solar core is possibly
    dependent upon tachocline turbulence, rather than absent entirely. The
    available observation & modeling are inadequate to establish your
    contention, to a high degree of reliability. IMHPO

  10. Same Robert Potter? Subaru Observation System Associate at Subaru Telescope, Location: 650 North A'ohoku Pl., Hilo, Hawaii, United States, Subaru Telescope: Ph: (808) 934-5900, Updated:12/11/2018, https://subarutelescope.org/

    The Subaru telescope is Japan's premier optical-infrared telescope operated by the National Astronomical Observatory of Japan. Located on Maunakea on the island of Hawaii, the telescope, with an effective aperture of 8.2 m, is also one of the world's largest and most technologically advanced telescopes. Through the open use program astronomers throughout the world have access to Subaru's excellent image quality.

    Thanks for contributing.

  11. http://www.aip.de/en/resear...

  12. http://www.aip.de/en/resear...

Search

Quick links

Nature Briefing

Sign up for the Nature Briefing newsletter — what matters in science, free to your inbox daily.

Get the most important science stories of the day, free in your inbox. Sign up for Nature Briefing