This article has been updated


Earth’s nearest candidate supermassive black hole lies at the centre of the Milky Way1. Its electromagnetic emission is thought to be powered by radiatively inefficient accretion of gas from its environment2, which is a standard mode of energy supply for most galactic nuclei. X-ray measurements have already resolved a tenuous hot gas component from which the black hole can be fed3. The magnetization of the gas, however, which is a crucial parameter determining the structure of the accretion flow, remains unknown. Strong magnetic fields can influence the dynamics of accretion, remove angular momentum from the infalling gas4, expel matter through relativistic jets5 and lead to synchrotron emission such as that previously observed6,7,8. Here we report multi-frequency radio measurements of a newly discovered pulsar close to the Galactic Centre9,10,11,12 and show that the pulsar’s unusually large Faraday rotation (the rotation of the plane of polarization of the emission in the presence of an external magnetic field) indicates that there is a dynamically important magnetic field near the black hole. If this field is accreted down to the event horizon it provides enough magnetic flux to explain the observed emission—from radio to X-ray wavelengths—from the black hole.


Linearly polarized radio waves that pass through a magnetized medium experience Faraday rotation. The resulting rotation of the polarization vector is given by Δϕ = RMλ2, where the rotation measure, , depends on the line-of-sight magnetic field, B; the free-electron density, n; the path length, s; the electron charge, e, and mass, me; and the speed of light, c. The radio emission associated with the Galactic Centre black hole, Sagittarius A* (Sgr A*), has RM = −5 × 105 rad m−2, which is the highest known RM of any source in the Galaxy, and is believed to be due to a column of hot, magnetized gas from the accretion flow onto the black hole13,14.

The radio emission from Sgr A*, however, probes only the innermost scales of accretion. For most accretion models14, the term B(r)n(r) decays much faster than r−1, where r is the radial distance from the black hole. Consequently, the Faraday rotation imprinted onto the radio emission from Sgr A*, which has to pass through the entire column of accreting gas, is dominated by the smallest scales. To measure the magnetization of the accretion flow on the outermost scales, other polarized radio sources, such as pulsars, are needed. A pulsar closely orbiting Sgr A* would also be an unparalleled tool for testing the space-time structure around the black hole15. Despite predictions that there are more than a thousand pulsars in the central parsec of the Galaxy16, there has been a surprising lack of detections17, potentially owing to severe interstellar dispersion and scattering in the inner Galaxy18.

Recently, the NASA Swift X-ray Telescope detected a bright X-ray flare9 near Sgr A* (projected offset of 3″ = 0.12 pc (ref. 19) at a Galactic Centre distance of d = 8.3 kpc). Subsequent X-ray observations by the NASA NuSTAR telescope resulted in the detection of pulsations with a period of 3.76 s (ref. 10). This behaviour is indicative of a magnetar, a highly magnetized pulsar, in outburst. During radio follow-up observations at the MPIfR Effelsberg Radio Observatory on 28 April 2013, the first weak detection of pulsations, with spin parameters matching those reported by NuSTAR, was made. Since then, the pulsar, PSR J1745–2900, has been consistently detected at Effelsberg, at the Paris Observatory-Nançay Radio Astronomy Facility, at the NRAO Karl G. Jansky Very Large Array (VLA), tentatively at The University of Manchester Jodrell Bank Observatory (Fig. 1) and with the CSIRO Australia Telescope Compact Array12. Measurements of the delay in the arrival times of pulses at lower frequencies (2.5 GHz) with respect to those at higher frequencies (8.35 GHz) yield an integrated column density of free electrons, the dispersion measure, of DM = 1,778 ± 3 cm−3 pc, which is the highest value measured for any known pulsar. This is consistent with a source located within <10 pc of the Galactic Centre, in the framework of the NE2001 free-electron density model of the Galaxy20. Including this source, only four radio-emitting magnetars are known21 in the Milky Way, making a chance alignment unlikely. If we consider a uniform source distribution occupying a cylinder of radius 10 kpc and height 1 kpc, then the fraction of sources present within an angular distance of 3″ around Sgr A* is 3 × 10−9. Given the current population of radio pulsars (2,000) and radio magnetars, the numbers present within the same region by chance will be 6 × 10−6 and 1 × 10−8, respectively.

Figure 1: Average pulse profiles of PSR J1745–2900 at each of the radio frequencies where detections have been made.
Figure 1

All observations have been centred on the X-ray position measured with NASA’s Chandra X-ray Observatory19. The telescope used, the total observation time required to generate the profile and the average flux density are indicated in brackets after the frequency label. In each case, the profile has been down-sampled from the original sampling interval to 256 phase bins (64 for the Jodrell Bank data), and the peak flux density has been normalized to unity. The profiles have been aligned on the peak of the main pulse detected. By measuring accurate pulse arrival times, we have constructed a coherent timing solution, that is, a model that tracks every single rotation of the pulsar. Between modified Julian dates 56414 and 56426, this model has given a value for the spin period of P = 3.76354676(2) s and a value for the time derivative of the period (spin-down) of ; uncertainties in the last digit, given in brackets, are derived from the 1σ error of the timing model fit. Absolute timing from 1.5 to 8.35 GHz has established that the main pulse in each profile is indeed aligned at each frequency.

The emission from the pulsar is highly linearly polarized12,22 (Fig. 2). Using the RM synthesis method23 and measuring the Faraday rotation in three frequency bands and at three different telescope sites, we derive a RM of (−6.696 ± 0.005) × 104 rad m−2 (Fig. 3). This measurement is consistent with that reported elsewhere12. The RM is the largest measured for any Galactic object other than Sgr A*13,14, and is more than an order of magnitude larger than all the other RMs measured to within tens of parsecs of Sgr A*24. The RM is also more than what can be optimistically expected as foreground25. This constrains the magnetized plasma causing the Faraday rotation (the Faraday screen) to be within some ten parsecs from the Galactic Centre.

Figure 2: Pulse profile of PSR J1745–2900 at 8.35 GHz.
Figure 2

After correcting for the Faraday rotation of (−6.696 ± 0.005) × 104 rad m−2, we can measure the intrinsic polarization across the pulse profile, together with the polarization position angle (PA). The degree of linear polarization (red dashed line) is nearly 100%, and a significant amount (15%) of circular polarization (blue dotted line) is also detected. A consistent ‘S’-shaped PA swing is measured at each frequency.

Figure 3: RM synthesis analysis for the radio polarization of PSR J1745–2900.
Figure 3

The red points, with 1σ error bars given by the off-pulse, baseline root mean squared value of the polarization profile, show the observed polarized flux density in the Stokes parameters Q and U. We note that polarization measurements were not possible at all frequencies, owing to hardware limitations. RM is measured by a two-step method. First we perform the Fourier transformation of the polarization intensity to get the RM Faraday spectrum, the peak of which is used to find a rough estimate of RM. Using this initial value, we then perform a least-squares fit to the Q and U curves to find RM and its error. The black curves are the model values based on the best-fit RM. The sinusoidal variation in Q and U due to Faraday rotation is seen across the frequency bands centred at 4.85 GHz (a and b) and 8.35 GHz (c and d). At 2.5 GHz (not shown), the variation is so severe that this signature is more easily seen in the RM spectrum. The RM values derived for each frequency band are independently consistent: at 2.5 GHz, RM = (−6.70 ± 0.01) × 104 rad m−2; at 4.85 GHz, RM = (−6.694 ± 0.006) × 104 rad m−2; and at 8.35 GHz, RM = (−6.68 ± 0.04) × 104 rad m−2. RM has also been measured with the VLA at 8.67 GHz, giving (−6.70 ± 0.04) × 104 rad m−2. The combined and appropriately weighted average is (−6.696 ± 0.005) × 104 rad m−2.

A frequently used estimate of the magnetic field is B ≥ RM/0.81DM μG, which gives B ≥ 50 μG (ref. 12). However, this is not a stringent limit, because DM and RM are dominated by very different scales. Hence, the extra information about the gas in the central 10 pc must be used for a more robust estimate of the magnetic field.

Two ionized gas phases in the Galactic Centre interstellar medium towards the line of sight of the pulsar could be associated with the Faraday screen: a warm component from the northern arm of the gas streamer Sgr A West26, which passes behind Sgr A*, and a diffuse hot component seen in the X-ray emission3 with T = 2.2 × 107 K. The warm gas in the northern arm has a width of >0.1 pc, electron densities of 105 cm−3 measured from radio recombination lines26, and a magnetic field of 2 mG (ref. 27). The inferred RM and DM values for a source in or behind the northern arm are RM ≈ 2 × 107 rad m−2 (for an ordered magnetic field) and DM ≈ 104 pc cm−3. The measured DM and RM values therefore place the pulsar and the screen in front of the northern arm26.

Consequently, the Faraday screen must be associated with the hot gas component, for which no magnetic field estimates yet exist. The density in the hot gas shows a radial fall-off as a function of r. At 0.4 pc (10″) we find that n ≈ 26 cm−3, whereas at 0.06 pc (1.5″) it can be inferred that , using the optically thin thermal plasma model3. Farther away, on the 40-pc scale28 (17′), the density has decreased to 0.1–0.5 cm−3 and we can roughly describe the density within the central parsecs with a profile of the form . The contribution of this hot gas component to DM is of order 102 cm−3 pc. This is consistent with the modest increase in DM with respect to the hitherto closest known pulsars to the Galactic Centre.

For a simple one-zone Faraday screen, where RM B(r)n(r)r, we have RM = 8.1 × 105B(r)n(r)r rad m−2, where B(r) is in units of Gauss, n(r) is expressed in units of cm−3 and r is expressed in parsecs. Using the density prescription above with an r1 scaling, we find that . This is a lower limit, because possible turbulent field components or field reversals reduce RM. We note again that this RM value is indeed dominated by the smallest distance scale, that is, by the gas on scales of the de-projected distance, r > 0.12 pc, of the pulsar from Sgr A*.

This B value is higher than the magnetic field in the northern arm and is also higher than the equipartition field in the hot phase at this scale. To bring thermal and magnetic energy into equipartition, the gas density at r ≈ 0.12 pc would need to increase by a factor of three, to 260 cm−3, yielding B ≈ 2.6 mG. If there were many field reversals within the Faraday screen, the magnetic field would be driven to values much greater than the equipartition field, suggesting that a relatively ordered magnetic field is pervading the hot gas close to the supermassive black hole.

Because Sgr A* accretes from this magnetized hot phase, density and magnetic field will further increase at smaller radii. Emission models of Sgr A* require magnetic fields of about 30–100 G to explain the synchrotron radiation from near the event horizon6,7,8. Hence, if the gas falls from 3 × 105 Schwarzschild radii (0.12 pc) down to a few Schwarzschild radii, a simple Br−1 scaling would be enough to provide a magnetic field of several hundred gauss. This is well within the range of most accretion models, where equipartition between magnetic, kinetic and gravitational energy in the accreting gas is assumed14,29.

The field at large radius in the accretion flow onto Sgr A* is therefore sufficient to provide the necessary field at small radius, via simple accretion. Moreover, the availability of ordered magnetic fields would make the proposed formation of a jet-like outflow in Sgr A*30 viable. Super-equipartition magnetic fields could also suppress accretion and help to explain the low accretion rate of Sgr A*.

At its projected distance, PSR J1745–2900 could move (owing to orbital motion) through the hot gas surrounding Sgr A* at several milliarcseconds per year and reveal RM variations as well as proper motion. Continued pulsar polarimetry and very-long-baseline interferometry astrometry can readily measure these effects. Also, given that magnetars constitute only a small fraction of the pulsar population and the excess DM towards the Galactic Centre is not too large, we expect there to be additional observable radio pulsars in the same region. Such pulsars could be used to map out the accretion region around the black hole in more detail, and even to test its space-time properties.

Online Content Any additional Methods, Extended Data display items and Source Data are available in the online version of the paper; references unique to these sections appear only in the online paper.

Change history

  • 20 August 2013

    Source Data files for Figs 1–3 were added.


  1. 1.

    , & The Galactic Center massive black hole and nuclear star cluster. Rev. Mod. Phys. 82, 3121–3195 (2010)

  2. 2.

    & Advection-dominated accretion: a self-similar solution. Astrophys. J. 428, L13–L16 (1994)

  3. 3.

    et al. Chandra X-ray spectroscopic imaging of Sagittarius A* and the central parsec of the Galaxy. Astrophys. J. 591, 891–915 (2003)

  4. 4.

    & A powerful local shear instability in weakly magnetized disks. I - Linear analysis. II - Nonlinear evolution. Astrophys. J. 376, 214–233 (1991)

  5. 5.

    , & The influence of magnetic field geometry on the evolution of black hole accretion flows: similar disks, drastically different jets. Astrophys. J. 678, 1180–1199 (2008)

  6. 6.

    & The jet model for Sgr A*: radio and X-ray spectrum. Astron. Astrophys. 362, 113–118 (2000)

  7. 7.

    , , , & Radiative Models of Sgr A* from GRMHD simulations. Astrophys. J. 706, 497–507 (2009)

  8. 8.

    , , & The submillimeter bump in Sgr A* from relativistic MHD simulations. Astrophys. J. 717, 1092–1104 (2010)

  9. 9.

    et al. Swift Discovery of a new soft gamma repeater, SGR J1745–29, near Sagittarius A*. Astrophys. J. 770, L24 (2013)

  10. 10.

    et al. NuSTAR discovery of a 3.76 s transient magnetar near Sagittarius A*. Astrophys. J. 770, L23 (2013)

  11. 11.

    et al. Detection of radio pulsations from the direction of the NuSTAR 3.76 second X-ray pulsar at 8.35 GHz. Astron. Telegr. 5040, 1 (2013)

  12. 12.

    & Radio properties of the magnetar near Sagittarius A* from observations with the Australia Telescope Compact Array. Preprint at (2013)

  13. 13.

    , , & Variable linear polarization from Sagittarius A*: evidence of a hot turbulent accretion flow. Astrophys. J. 618, L29–L32 (2005)

  14. 14.

    , , & An unambiguous detection of Faraday rotation in Sagittarius A*. Astrophys. J. 654, L57–L60 (2007)

  15. 15.

    , , , & Prospects for probing the spacetime of Sgr A* with pulsars. Astrophys. J. 747, 1 (2012)

  16. 16.

    , , , & Multiwavelength constraints on pulsar populations in the Galactic Center. Astrophys. J. 753, 108 (2012)

  17. 17.

    et al. in Neutron Stars and Pulsars: Challenges and Opportunities After 80 Years (ed. ) 382–384 (Cambridge Univ. Press, 2013)

  18. 18.

    & Hyperstrong radio-wave scattering in the Galactic Center. II. A likelihood analysis of free electrons in the Galactic Center. Astrophys. J. 505, 715–731 (1998)

  19. 19.

    et al. Chandra localization of the soft gamma repeater in the Galactic Center region. Astron. Telegr. 5032, 1 (2013)

  20. 20.

    & NE2001.I. A new model for the galactic distribution of free electrons and its fluctuations. Preprint at (2002)

  21. 21.

    , , , & Constraining radio emission from magnetars. Astrophys. J. 744, 97 (2012)

  22. 22.

    et al. Polarisation profiles and rotation measure of PSR J1745–2900 measured at Effelsberg. Astron. Telegr. 5064, 1 (2013)

  23. 23.

    & Faraday rotation measure synthesis. Astron. Astrophys. 441, 1217–1228 (2005)

  24. 24.

    , & A constraint on the organization of the Galactic Center magnetic field using Faraday rotation. Astrophys. J. 731, 36 (2011)

  25. 25.

    , , , & The linear polarization of Sagittarius A*. I. VLA spectropolarimetry at 4.8 and 8.4 GHz. Astrophys. J. 521, 582–586 (1999)

  26. 26.

    et al. The high-density ionized gas in the central parsec of the Galaxy. Astrophys. J. 723, 1097–1109 (2010)

  27. 27.

    , & The magnetic fields in the galactic center: detection of H1 Zeeman splitting. Astrophys. J. 445, L113–L116 (1995)

  28. 28.

    et al. Diffuse X-ray emission in a deep Chandra image of the Galactic Center. Astrophys. J. 613, 326–342 (2004)

  29. 29.

    , , , & The rotation measure and 3.5 millimeter polarization of Sagittarius A*. Astrophys. J. 646, L111–L114 (2006)

  30. 30.

    , & The galactic center radio jet. Astron. Astrophys. 278, L1–L4 (1993)

Download references


We wish to thank D. D. Xu., P. Lazarus and L. Guillemot for discussions. We also thank O. Wucknitz and R. Beck for reading the manuscript. R.K., L.G.S. and P.C.C.F. gratefully acknowledge financial support from the European Research Council for the ERC Starting Grant BEACON under contract no. 279702. K.J.L. was funded by ERC Advanced Grant LEAP under contract no. 227947. H.F. acknowledges funding from an Advanced Grant of the European Research Council under the European Union’s Seventh Framework Programme (FP/2007-2013)/ERC Grant Agreement no. 227610. This work was based on observations with the 100-m telescope of the MPIfR (Max-Planck-Institut für Radioastronomie) at Effelsberg. The Nançay radio telescope is part of the Paris Observatory, associated with the Centre National de la Recherche Scientifique (CNRS), and partly supported by the Région Centre in France. The National Radio Astronomy Observatory (NRAO) is a facility of the National Science Foundation operated under cooperative agreement by Associated Universities, Inc.

Author information


  1. Max-Planck-Institut für Radioastronomie, Auf dem Hügel 69, D-53121 Bonn, Germany

    • R. P. Eatough
    • , H. Falcke
    • , R. Karuppusamy
    • , K. J. Lee
    • , D. J. Champion
    • , G. Desvignes
    • , D. H. F. M. Schnitzeler
    • , L. G. Spitler
    • , M. Kramer
    • , B. Klein
    • , A. Brunthaler
    • , P. C. C. Freire
    • , A. Kraus
    • , A. Noutsos
    •  & N. Wex
  2. Department of Astrophysics, Institute for Mathematics, Astrophysics and Particle Physics, Radboud University, PO Box 9010, 6500 GL Nijmegen, The Netherlands

    • H. Falcke
  3. ASTRON, PO Box 2, 7990 AA Dwingeloo, The Netherlands

    • H. Falcke
    •  & A. T. Deller
  4. Jodrell Bank Centre for Astrophysics, School of Physics and Astronomy, The University of Manchester, Manchester M13 9PL, UK

    • E. F. Keane
    • , M. Kramer
    • , C. Bassa
    • , A. G. Lyne
    •  & B. Stappers
  5. Bonn-Rhein-Sieg University of Applied Sciences, Grantham-Allee 20, D-53757 Sankt Augustin, Germany

    • B. Klein
  6. Astronomy Department, B-20 Hearst Field Annex, University of California, Berkeley, California 94720-3411, USA

    • G. C. Bower
  7. LPC2E/CNRS - Université d’Orléans, 45071 Orléans, France

    • I. Cognard
  8. Nançay/Paris Observatory, 18330 Nançay, France

    • I. Cognard
  9. National Radio Astronomy Observatory, 520 Edgemont Road, Charlottesville, Virginia 22903, USA

    • P. B. Demorest


  1. Search for R. P. Eatough in:

  2. Search for H. Falcke in:

  3. Search for R. Karuppusamy in:

  4. Search for K. J. Lee in:

  5. Search for D. J. Champion in:

  6. Search for E. F. Keane in:

  7. Search for G. Desvignes in:

  8. Search for D. H. F. M. Schnitzeler in:

  9. Search for L. G. Spitler in:

  10. Search for M. Kramer in:

  11. Search for B. Klein in:

  12. Search for C. Bassa in:

  13. Search for G. C. Bower in:

  14. Search for A. Brunthaler in:

  15. Search for I. Cognard in:

  16. Search for A. T. Deller in:

  17. Search for P. B. Demorest in:

  18. Search for P. C. C. Freire in:

  19. Search for A. Kraus in:

  20. Search for A. G. Lyne in:

  21. Search for A. Noutsos in:

  22. Search for B. Stappers in:

  23. Search for N. Wex in:


R.P.E.: initial detections, observations performed at Effelsberg and data processing; H.F.: observational and theoretical background and paper formulation; R.K.: observational technical assistance and pulsar timing; K.J.L.: polarization and RM measurements; D.J.C.: pulsar timing solution; E.F.K.: flux density calculations, observational assistance and observations at Jodrell Bank; G.D.: observations at Nançay; D.H.F.M.S.: observational background and RM interpretation; L.G.S.: observational background and data processing and analysis; M.K.: observational background and RM interpretation; B.K.: technical observational assistance at Effelsberg; C.B.: observations at Jodrell Bank; G.C.B.: observations at the VLA and RM interpretation; A.B.: observations at the VLA; I.C.: observations at Nançay; A.T.D.: observations at the VLA; P.B.D.: observations at the VLA; P.C.C.F.: observational background and pulsar timing; A.K.: technical observational assistance at Effelsberg; A.G.L.: observations at Jodrell Bank and help with initial detections; A.N.: observational background and RM interpretation; B.S.: observations at Jodrell Bank; N.W.: theoretical background and orbital characteristics.

Competing interests

The authors declare no competing financial interests.

Corresponding author

Correspondence to R. P. Eatough.

About this article

Publication history






By submitting a comment you agree to abide by our Terms and Community Guidelines. If you find something abusive or that does not comply with our terms or guidelines please flag it as inappropriate.