# Landau quantization and mass-radius relation of magnetized White Dwarfs in general relativity

###### Abstract

Recently, several white dwarfs have been proposed with masses significantly above the Chandrasekhar limit, known as Super-Chandrasekhar White Dwarfs, to account for the overluminous Type Ia supernovae. In the present work, Equation of State of a completely degenerate relativistic electron gas in magnetic field based on Landau quantization of charged particles in a magnetic field is developed. The mass-radius relations for magnetized White Dwarfs are obtained by solving the Tolman-Oppenheimer-Volkoff equations. The effects of the magnetic energy density and pressure contributed by a density-dependent magnetic field are treated properly to find the stability configurations of realistic magnetic White Dwarf stars. Keywords: White Dwarf; Mass-Radius relation; Electrons in Magnetic field; Landau Quantization.

###### pacs:

97.20.-w, 97.20.Rp, 97.60.Bw, 71.70.Di, 04.40.Dg## I Introduction

Ultrahigh magnetic fields in nature are known to be associated with compact astrophysical objects namely white dwarfs, neutron stars and black holes. Of these, the largest magnetic fields are found on the surfaces of magnetars, Anomalous X-ray Pulsars (AXPs) and Soft Gamma Repeaters (SGRs), certain classes of neutron stars, with an order of magnitude of gauss. Recently, a strong magnetic field of the same order of magnitude as that of a magnetar has been found at the jet base of a supermassive black hole PKS 1830-211 Vi15 (). These strong magnetic fields drastically modify the Equation of State (EoS) of a compact star and its stability. Hence, studying the EoS and equilibria of compact stars in presence of high magnetic fields is an important and rapidly growing field of research in theoretical astrophysics. Magnitudes of magnetic fields of white dwarfs are constrained by the virial theorem:

(1) |

which gives

(2) |

Here, are the magnetic field, mass and radius of the white dwarf and sun respectively. Using gauss, 1.4 and 0.0086 , we get the order of magnitude as gauss.

The recently observed peculiar Type Ia supernovae, e.g. SN2006gz, SN2007if, SN2009dc, SN2003fg, Ho06 (); Sc10 (); Hi07 (); Ya09 (); Si11 () with exceptionally high luminosities do not fit with the explosion of a Chandrasekhar mass white dwarf. Moreover, it has been seen that there is a correlation between the surface magnetic field and the mass of white dwarfs. The magnetic white dwarfs seem to be more massive than their nonmagnetic counterparts Fe15 (). Lastly, predictions from the luminosities reveal that the progenitor white dwarfs had masses significantly higher than the Chandrasekhar limit. It seems that the Chandrasekhar limit may be violated by highly magnetized white dwarfs. To account for these facts, we have calculated theoretically the masses of white dwarfs in presence of such high magnetic fields in the general relativistic formalism.

## Ii Completely degenerate ideal Fermi gas and EoS for non-magnetic White Dwarfs

We consider a relativistic, completely degenerate Fermi gas at zero temperature and neglect any form of interactions between the fermions. By the Pauli exclusion principle, no quantum state can be occupied by more than one fermion with an identical set of quantum numbers. Thus a noninteracting Fermi gas, unlike a Bose gas, is prohibited from condensing into a Bose-Einstein condensate. The total energy of the Fermi gas at absolute zero is larger than the sum of the single-particle ground states because the Pauli principle implies a degeneracy pressure that keeps fermions separated and moving. For this reason, the pressure of a Fermi gas is non-zero even at zero temperature, in contrast to that of a classical ideal gas. This so-called degeneracy pressure stabilizes a white dwarf (a Fermi gas of electrons) against the inward pull of gravity, which would ostensibly collapse the star into a Black Hole. However if a star is sufficiently massive to overcome the degeneracy pressure, it collapse into a singularity due to gravity. While the pressure inside a white dwarf is entirely due to electrons, its mass comes mostly from the atomic nuclei.

### ii.1 Completely degenerate free Fermi gas

The non-interacting assembly of fermions at zero temperature exerts pressure because of kinetic energy from different states filled up to Fermi level. Since pressure is force per unit area which means rate of momentum transfer per unit area, it is given by

(3) |

where is the rest mass, is the velocity of the particles with momentum and is the number of particles per unit volume having momenta between and . The factor accounts for the fact that, on average, only rd of total particles are moving in a particular direction. For fermions having spin , degeneracy = 2, and hence number density is given by

(4) |

where is the Fermi momentum which is maximum momentum possible at zero temperature, is a dimensionless quantity and is the Compton wavelength. The energy density is given by

(5) |

which along with Eq.(3) turns out upon integration to be

(6) |

where

(7) |

and

(8) |

### ii.2 EoS for non-magnetic White Dwarfs

For the EoS for non-magnetic White Dwarfs, the pressure is provided by the relativistic electrons only and therefore, pressure is given by

(9) |

whereas for energy density both electrons (with its kinetic energy) and atomic nuclei contribute, so that

(10) |

where and are the masses of neutron and proton, respectively and is the number of neutrons per electron. Commonly, electron-degenerate stars consist of helium, carbon, oxygen, etc., for which . To be precise, one should in fact also subtract times binding energy per nucleon from the second term on the right hand side of the above equation. Obviously, this correction is composition dependent and its contribution being quite small, e.g. in case of helium star it is about 0.7 to the second term, it is not considered in calculations. Since the kinetic energy of electrons in the above equation contributes negligibly, the mass density for white dwarfs can be expressed in units of 2 gms/cc by multiplying number density of electrons expressed in units of fm by the factor 1.6717305.

## Iii Landau quantization and EoS for magnetized White Dwarfs

Like the former case, here also we consider a completely degenerate relativistic electron gas at zero temperature but embedded in a strong magnetic field. We do not consider any form of interactions with the electrons. Electrons, being charged particles, occupy Landau quantized states in a magnetic field. This changes the EoS, which, in turn, changes the pressure and energy density of the white dwarf. In addition to the matter energy density and pressure, the energy density and pressure due to magnetic field are also taken into account. It is the combined pressure and energy density of matter and magnetic field that determines the mass-radius relation of strongly magnetized white dwarfs. It should be emphasized that protons also, being charged particles, are Landau quantized. But since the proton mass is times the electron mass their cyclotron energy is times smaller than that of the electron for the same magnetic field, and hence we neglect it.

### iii.1 Landau quantization and EoS for free electron gas in magnetic field

In order to calculate the thermodynamic quantities like the energy density and pressure of an electron gas in a magnetic field, we need to know the density of states and the dispersion relation. The quantum mechanics of a charged particle in a magnetic field is presented in many texts (e.g. Sokolov and Ternov (1968) ST68 (), Landau and Lifshitz (1977) LL77 (), Canuto and Ventura (1977) CV77 () Mészáros (1992) Me92 ()). Here we summarize the basics needed for our later discussion. Let us first consider the motion of a charged particle (charge and mass ) in a uniform magnetic field assumed to be along the z-axis. In classical physics, the particle gyrates in a circular orbit with radius and angular frequency (cyclotron frequency) given by

(11) |

where is the velocity perpendicular to the magnetic field. The hamiltonian of the system is given by

(12) |

where with being the electromagnetic vector potential. To have magnetic field in z-direction with magnitude one must have

(13) |

and therefore

(14) |

The operator commutes with this hamiltonian since the operator is absent. Thus operator can be replaced by its eigenvalue .Using cyclotron frequency one obtains

(15) |

the first two terms of which is exactly the quantum harmonic oscillator with the minimum of the potential shifted in co-ordinate space by . Noting that translating harmonic oscillator potential does not affect the energies, energy eigenvalues can be given by

(16) |

The energy does not depend on the quantum number , so there will be degeneracies. Each set of wave functions with same value of is called a Landau Level. Each Landau level is degenerate due to the second quantum number . If periodic boundary condition is assumed can take values where is another integer and being the dimensions of the system. The allowed values of are further restricted by the condition that the centre of the force of the oscillator must physically lie within the system, which implies . Hence for electrons with spin and charge , the maximum number of particles per Landau level per unit area is . On solving Schrödinger’s equation for electrons with spin in an external magnetic field in z-direction which is uniform and static, Eq.(16) modifies to

(17) |

Clearly for the lowest Landau level () the spin degeneracy (since only , is allowed) and for all other higher Landau levels (), (for ).

For extremely strong magnetic fields such that the motion perpendicular to the magnetic field still remains quantized but becomes relativistic. The solution of the Dirac equation in a constant magnetic field Lai91 () is given by the energy eigenvalues

(18) |

where the dimensionless magnetic field defined as is introduced with given by gauss. Obviously, the density of states in presence of magnetic field gets modified to

(19) |

where the sum is on all Landau levels . At zero temperature the number density of electrons is given by

(20) |

where is the Fermi momentum in the th Landau level and is the upper limit of the Landau level summation. The Fermi energy of the th Landau level is given by

(21) |

and can be found from the condition or

(22) |

where is the dimensionless Fermi energy and the dimensionless maximum Fermi energy of a system for a given and . Obviously, very small corresponds to large number of Landau levels leading to the familiar non-magnetic EoS. is taken to be the nearest lowest integer. Like the former case, if we define a dimensionless Fermi momentum then Eqns.(20) and (21) may be written as

(23) |

and

(24) |

or

(25) |

The electron energy density is given by

where

(27) |

The pressure of the electron gas is given by

where

(29) |

### iii.2 Magnetized White Dwarfs

In the present case of magnetic White Dwarfs, the explicit contributions from the energy density and pressure arising due to magnetic field need to be added to the matter energy density and pressure as

(30) | |||||

and

(31) | |||||

## Iv Tolman-Oppenheimer-Volkoff Equation and theoretical calculations of mass-radius relation for White Dwarfs

If rapidly rotating compact stars were non-axisymmetric, they would emit gravitational waves in a very short time scale and settle down to axisymmetric configurations. Therefore, we need to solve for rotating and axisymmetric configurations in the framework of general relativity. For the matter and the spacetime the following assumptions are made. The matter distribution and the spacetime are axisymmetric, the matter and the spacetime are in a stationary state, the matter has no meridional motions, the only motion of the matter is a circular one that is represented by the angular velocity, the angular velocity is constant as seen by a distant observer at rest and the matter can be described as a perfect fluid. To study the rotating stars the following metric is used

(32) |

where the gravitational potentials , , and are functions of polar coordinates and only. The Einstein’s field equations for the three potentials , and can be solved using the Green’s-function technique Ko89 () and the fourth potential can be determined from other potentials. All the physical quantities may then be determined from these potentials. Rotational frequency of stars is limited by Kepler’s frequency which is the mass shedding limit. For very compact stars such as neutron stars the Kepler’s frequency is very high and can go up to millisecond order Ch10 (); Mi12 () whereas white dwarfs being about thousand times bigger in size and much less dense, Kepler’s frequency is very small and one may safely use the zero frequency limit Ba14 () to the Einstein’s field equations. Obviously, at the zero frequency limit corresponding to the static solutions of the Einstein’s field equations for spheres of fluid, the present formalism yields the results for the solution of the Tolman-Oppenheimer-Volkoff (TOV) equation TOV39a (); TOV39b () given by

(33) | |||

which can be easily solved numerically using Runge-Kutta method for masses and radii. The quantities and are the energy density and pressure at a radial distance from the centre, and are given by the equation of state. The mass of the star contained within a distance is given by . The size of the star is determined by the boundary condition and the total mass of the star integrated up to the surface is given by Um97 (). The single integration constant needed to solve the TOV equation is , the pressure at the center of the star calculated at a given central density .

## V Results and discussion

Recently, there are some important calculations for masses and radii of magnetized white dwarfs using non-relativistic Lane-Emden equation assuming a constant magnetic field throughout which provided masses up to 2.3-2.6 Das12 (), a mass significantly greater than the Chandrasekhar limit. However, because of the structure of the Lane-Emden equation, pressure arising due to constant magnetic field do not contribute while for the general relativistic TOV equation case is not the same. Moreover, the EoS needed to be fitted to a polytropic form. In order to derive a mass limit for magnetized white dwarfs (similar to the mass limit of 1.4 obtained by Chandrasekhar Ch35 () for non-magnetic white dwarfs), the same authors, under certain approximations, have been able to reduce the EoS to a polytropic form with index for which analytic solution of Lane-Emden equation exists ( where with and being density and central density, respectively) and avoiding the energy density and pressure arising due to magnetic field by assuming it to be constant throughout, they were able to set a mass limit of 2.58 Das13 (); Do14 (). In the present work, we have calculated masses and radii of white dwarfs by solving the general relativistic TOV equation both for non-magnetic and magnetized white dwarfs using the exact EoS without resorting to fit it to a polytropic form.

### v.1 Chandrasekhar limit for White Dwarfs

We verify Chandrasekhar limit Ch35 () for masses of white dwarfs by actually solving TOV equation for non-magnetic white dwarfs. The masses and radii of such white dwarfs are listed in Table-I. It is interesting to note that considering a very high central density of 3.343 gms/cc for white dwarfs, one can asymptotically reach the Chandrasekhar mass limit. It is important to mention that beyond this density at 4.3 gms/cc, the neutron drip point Ch15 (), the nuclei become so neutron rich that with increasing density the continuum neutron states begin to be filled, and the lattice of neutron-rich nuclei becomes permeated by a sea of neutrons. In Table-I, masses and radii of non-magnetic white dwarfs as a function of central density are provided. In Fig.-1 plot for masses of non-magnetic white dwarfs is shown as a function of central density whereas in Fig.-2 mass-radius relationship of non-magnetic white dwarfs is provided. These results for non-magnetic white dwarfs do conform to the traditional Chandrasekhar mass-limit.

(r=0) | Radius | Mass |
---|---|---|

fm | Kms | |

1.010 | 917.87 | 1.3904 |

5.010 | 1126.83 | 1.3905 |

4.010 | 1202.53 | 1.3896 |

3.810 | 1220.55 | 1.3893 |

3.610 | 1239.80 | 1.3890 |

3.410 | 1260.43 | 1.3887 |

3.210 | 1282.65 | 1.3883 |

3.010 | 1306.67 | 1.3878 |

2.810 | 1332.78 | 1.3873 |

2.610 | 1361.33 | 1.3866 |

2.410 | 1392.75 | 1.3859 |

2.210 | 1427.62 | 1.3850 |

2.010 | 1466.67 | 1.3839 |

1.810 | 1510.90 | 1.3825 |

1.610 | 1561.69 | 1.3809 |

1.410 | 1621.01 | 1.3788 |

1.210 | 1691.86 | 1.3761 |

1.010 | 1779.00 | 1.3724 |

8.010 | 1890.72 | 1.3673 |

6.010 | 2043.29 | 1.3594 |

4.010 | 2275.36 | 1.3457 |

2.010 | 2721.16 | 1.3138 |

1.010 | 3233.63 | 1.2692 |

1.010 | 5482.58 | 1.0051 |

1.010 | 8721.75 | 0.5949 |

### v.2 Super-Chandrasekhar White Dwarfs

As mentioned in the beginning of this section that unlike non-relativistic Lane-Emden equation, pressure arising due to constant magnetic field does contribute to the general relativistic TOV equation. Presence of high constant magnetic field do not provide valid solutions to the TOV equations. Hence, we present stable solutions of magnetostatic equilibrium models for super-Chandrasekhar white dwarfs with varying magnetic field profiles which is maximum at the centre and goes to 10 gauss at the surface of the star. This has been obtained by self-consistently including the effects of the magnetic pressure gradient and total magnetic density in a general relativistic framework. Nevertheless, we have also performed calculations corresponding to very high (single Landau level) and high (multi Landau levels) magnetic field which is constant throughout the star in order to compare with the results from solutions of Lane-Emden equation described above, but for these cases we have to ignore the explicit contributions from energy density and pressure arising due to magnetic field. Results of such calculations are provided in Tables-II III for magnetized white dwarfs with single and multiple Landau levels, respectively.

(r=0) | Radius | Mass | |
---|---|---|---|

fm | Kms | in units of | |

5.010 | 592.28 | 2.4521 | 253 |

4.010 | 636.54 | 2.4508 | 218 |

3.010 | 698.11 | 2.4461 | 180 |

2.010 | 792.71 | 2.4204 | 138 |

1.010 | 989.84 | 2.4149 | 86.5 |

(r=0) | Radius | Mass | |
---|---|---|---|

fm | Kms | in units of | |

4.673610 | 1149.77 | 1.3925 | 1.5 |

3.514710 | 663.58 | 2.4491 | 200 |

Now we perform the actual calculations with varying magnetic field including the effects of energy density and pressure arising due to magnetic field in a general relativistic framework. The variation of magnetic field Ba97 () inside white dwarf is taken to be of the form

(34) |

where (in units of ) is the magnetic field at electronic number density , (in units of ) is the surface magnetic field and is taken as (r=0)/10 and , are constants. Once central magnetic field is fixed, can be determined from above equation. We choose constants and , rather arbitrarily by using unequal non-unity values, which provides stable solutions of magnetostatic equilibrium models for super-Chandrasekhar white dwarfs. Nevertheless, the magnetic field is not taken completely in ad hoc manner, because central and surface magnetic fields once fixed the variations of its profile do not alter the gross results. Moreover, we have kept maximum central magnetic field strength at 10 which is gauss, near to the lower of the maximum limit suggested by N. Chamel et al. Ch13 () and surface magnetic field gauss estimated by observations. In Table-IV the results of these realistic calculations are listed. In Figs.-3,4 plots for masses and radii of magnetized white dwarfs are shown as functions of central magnetic field. Present calculations estimate that the maximum stable mass of magnetized white dwarfs could be 3 . These results are quite useful in explaining the peculiar, overluminous type Ia supernovae that do not conform to the traditional Chandrasekhar mass-limit.

## Vi Summary and conclusion

In summary, we have considered a relativistic, degenerate electron gas at zero temperature under the influence of a density dependent magnetic field. Since the electrons are Landau quantized, the density of states gets modified due to the presence of the magnetic field. This, in turn, modifies the EoS of the white dwarf matter. The presence of magnetic field also gives rise to magnetic energy density and pressure which is added to those due to degenerate matter. We find that the masses of such white dwarfs increase with the magnitude of the central magnetic field. Hence we obtain a conclusive result that it is possible to have electron-degenerate magnetized white dwarfs, with masses significantly greater than the Chandrasekhar limit in the range of 3 , provided it has an appropriate magnetic field profile with high magnitude at the centre as well as high central density.

(r=0) | Radius | Mass | |
---|---|---|---|

fm | Kms | in units of | |

4.67401710 | 1285.91 | 1.4146 | 1.5 |

4.67384610 | 1344.46 | 1.4236 | 1.75 |

4.67420910 | 1349.45 | 1.4339 | 2.0 |

4.67537410 | 1388.04 | 1.4906 | 3.0 |

4.67218810 | 1438.94 | 1.5731 | 4.0 |

4.67083010 | 1503.64 | 1.6863 | 5.0 |

4.67811810 | 1581.27 | 1.8353 | 6.0 |

4.67767710 | 1663.86 | 2.0217 | 7.0 |

4.66574110 | 1758.40 | 2.2601 | 8.0 |

4.66165710 | 1954.44 | 2.8997 | 10. |

To date there are about 250 magnetized white dwarfs with well determined fields Fe15 () and over 600 if objects with no or uncertain field determination Ke13 (); Ke15 () are also included. Surveys such as the SDSS, HQS and the Cape Survey have discovered these magnetized white dwarfs. The complete samples show that the field distribution of magnetized white dwarfs is in the range 10-10 gauss which basically provides the surface magnetic fields. However, the central magnetic field strength, which is presumably unobserved by the above observations, could be several orders of magnitude higher than the surface field. In fact, it is the central magnetic field which is crucial for super-Chandrasekhar magnetized white dwarfs. However, the softening of the EoS accompanying the onset of electron captures and pycnonuclear reactions in the core of these stars can lead to local instabilities which set an upper limit to the magnetic field strength at the center of the star, ranging from 10-10 gauss depending on the core Ch13 () composition.

## References

- (1) Ivan Marti-Vidal, Sebastien Muller, Wouter Vlemmings, Cathy Horellou, Susanne Aalto, Science 348, 6232 (2015).
- (2) D. Andrew Howell et al., Nature 443, 308 (2006).
- (3) R. A. Scalzo et al., Astrophys. J. 713, 1073 (2010).
- (4) M. Hicken et al., Astrophys. J. 669, L17 (2007).
- (5) M. Yamanaka et al., Astrophys. J. 707, L118 (2009).
- (6) Jeffrey M. Silverman et al., Mon. Not. R. Astron. Soc., 410, 1 (2011).
- (7) Lilia Ferrario, Domitilla deMartino, Boris T. Gansicke, arXiv: 1504.08072v1 (2015).
- (8) A. A. Sokolov and I. M. Ternov, Synchrotron Radiation (Pergamon, Oxford) (1968).
- (9) L. D. Landau and E. M. Lifshitz, Quantum Mechanics (3rd. ed.; Oxford: Pergamon) (1977).
- (10) V. Canuto and J. Ventura, Fundam. Cosm. Phys. 2, 203 (1977).
- (11) P. Mészáros, High Energy Radiation from Magnetized Neutron Stars (University of Chicago, Chicago) (1992).
- (12) Dong Lai and Stuart L. Shapiro, Astrophys. J. 383, 745 (1991).
- (13) H. Komatsu, Y. Eriguchi, I. Hachisu, Mon. Not. R. Astron. Soc. 237, 355 (1989).
- (14) P. R. Chowdhury, A. Bhattacharyya, D. N. Basu, Phys. Rev. C 81, 062801(R) (2010).
- (15) Abhishek Mishra, P. R. Chowdhury and D. N. Basu, Astropart. Phys. 36, 42 (2012).
- (16) D. N. Basu, Partha Roy Chowdhury and Abhishek Mishra, Eur. Phys. J. Plus 129, 62 (2014).
- (17) R. C. Tolman, Phys. Rev. 55, 364 (1939).
- (18) J. R. Oppenheimer and G. M. Volkoff Phys. Rev. 55, 374 (1939).
- (19) V. S. Uma Maheswari, D. N. Basu, J. N. De and S. K. Samaddar, Nucl. Phys. A 615, 516 (1997).
- (20) U. Das and B. Mukhopadhyay, Phys. Rev. D 86, 042001 (2012).
- (21) S. Chandrasekhar, Mon. Not. R. Astron. Soc. 95, 207 (1935).
- (22) U. Das and B. Mukhopadhyay, Phys. Rev. Lett. 110, 071102 (2013).
- (23) J. M. Dong, W. Zuo, P. Yin and J. Z. Gu, Phys. Rev. Lett. 112, 039001 (2014).
- (24) N. Chamel, Zh. K. Stoyanov, L. M. Mihailov, Y. D. Mutafchieva, R. L. Pavlov and Ch. J. Velchev, Phys. Rev. C 91, 065801 (2015).
- (25) D. Bandyopadhyay, S. Chakrabarty and S. Pal, Phys. Rev. Lett. 79, 2176 (1997).
- (26) N. Chamel, A. F. Fantina and P. J. Davis, Phys. Rev. D 88, 081301(R) (2013).
- (27) S. O. Kepler, I. Pelisoli, S. Jordan, S. J. Kleinman, D. Koester, B. Külebi, V. Pecanha, B. G. Castanheira, A. Nitta, J. E. S. Costa, D. E. Winget, A Kanaan, and L. Fraga, Mon. Not. R. Astron. Soc. 429, 2934 (2013).
- (28) S. O. Kepler, I. Pelisoli, D. Koester, G. Ourique, S. J. Kleinman, A. D. Romero, A. Nitta, D. J. Eisenstein, J. E. S. Costa, B. Külebi, S. Jordan, P. Dufour, P. Giommi and A. Rebassa-Mansergas, Mon. Not. R. Astron. Soc. 446, 4078 (2015).