giant flares and magnetars - trinity college dublintrussn/projects/magnetar_poster_1.pdf ·...

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Giant Flares Giant flares are enormous emissions of electromagnetic energy, far larger than ordinary observed bursts. These events are extremely rare, but also spectacular. The three largest were observed in 1979 [1] , 1998 [6] and 2004 [7] . These events are powerful enough to saturate every gamma radiation detector in space. Existing theoretical models had difficulty explaining the magnitudes of some of these outbursts. Currently there are several competing models explaining the mechanism behind giant flares. SGR 1806-20 The event in 2004 [7] was the largest ever observed, it saturated satellite instruments for up to 0.5 s. [9] This magnetar is the most highly magnetized object ever observed [9] , with magnetic field of over 10 11 T. It unleashed energy at a rate of about 10 40 watts for 0.2s. The total energy produced was more than the Sun emits in 150,000 years [9] . Thankfully it is located approximately 40,000 light years away [4] and so did not pose a significant danger. The magnitude of the flare observed led to the development of the Lyutikov model to allow for the larger flare energies. Open Questions Research is being done into 3D magnetic reconnection, and relativistic models for reconnection. Theoretical models for giant flare mechanisms need to be improved upon, as none of the current proposed models are entirely satisfactory. Can a method be developed to detect inactive magnetars? Can magnetars be used to detect gravitational wavebursts? References 1. E.P. Mazets et al. 1979 Nature 282, 587 - 589 2. C. Thompson and R. C. Duncan 1992 ApJ 392, L9 3. A. I. Ibrahim et al. 2001 ApJ 558 237 4. McGill Online SGR/AXP Catalogue http://www.physics.mcgill.ca/~pulsar/magnetar/main.html 5. R.C. Duncan, 2003 6. C. Thompson,R. and C. Duncan 2001 ApJ 561, 980 7. K. Hurley et al. 2005 Nature 434, 1098-1103 8. M. Lyutikov 2006 MNRAS 367, 1602 9. S. E. Boggs et al. 2007 ApJ 661, 458 Flux Freezing In a perfectly conducting fluid, a phenomenon occurs whereby the magnetic field lines move with the material, i.e they are "frozen" into the plasma. Motions along the field lines do not change the field, but motion transverse to the field lines carry the field with them. If field lines in a star pass through the surface, the field is anchored to surface. This means that for huge magnetic fields, there are huge forces acting on the surface. This leads to "winding up" of field lines in the interior of a magnetar, giving rise to enormous internal magnetic stresses. GIANT FLARES AND MAGNETARS Mark Allen and Nikki Truss Trinity College Dublin Supervisor: Professor Tristan McLoughlin Comparison of Two Giant Flare Models Crust Failure Model Thompson, Duncan (2001) [6] Magnetic stresses in core become too great, exceeding the elastic stresses in the crust Quick and brittle fracture of the crust occurs, i.e starquake Due to the relaxation of internal magnetic stresses, energy is released via giant flares Energy limited by tensile strength of crust Created after the 1998 event, which reached a peak luminosity of 10 6 L Edd [6] Magnetospheric Model Lyutikov (2006) [8] Slow untwisting of the internal magnetic field leads to twisting of magnetospheric field lines Flux injection leads to increase in magnetospheric energy held in flux ropes Unstable flux ropes rupture and release energy via giant flares Energy limited by total external magnetic field Created to explain magnitude of 2004 event which reached a peak luminosity of 10 9 L Edd [7] Magnetic Reconnection Magnetic reconnection is at the heart of many magnetar phenomena. The magnetic field stores energy, and when the topology of the magnetic field changes, this energy is released as EM radiation. There are various models describing magnetic reconnection in two dimensions, such as the Sweet-Parker, Petschek, and almost uniform models. Meanwhile, 3D reconnection is still a very new field where progress is driven by computational models. Introduction In 1979 [1] , a large burst of gamma rays was detected from the Large Magellanic Cloud. The object that produced this burst was monitored over a period of time and was eventually dubbed a ‘Soft Gamma Repeater’ (SGR) due to its periodic bursts of energy in the soft-gamma region of the spectrum. In 1992, Robert Duncan and Christopher Thompson proposed the magnetar model [2] to explain these large emissions of energy. These proposed magnetars were neutrons stars with extraordinarily large magnetic fields and a short but active lifetime. Along with the repeated smaller bursts, occasionally magnetars have been observed to release enormous bursts of electromagnetic radiation, known as giant flares. Magnetar Formation Magnetars are hypothesised to be a type of neutron star, and like other neutron stars, are believed to be the result of supernova collapse. They are thought to have diameters in the range of 10 - 20 km and masses greater than that of the Sun. The large magnetic fields of magnetars are thought to result from dynamo action during their formation. In magnetars, dynamo action increases their magnetic field from 10 8 T to 10 11 T. [3] There are currently 20 confirmed magnetars [4] , along with 3 proposed candidates. They are located between 10,000 - 50,000 light years away, and are only active for approximately 10,000 years. There are an estimated 30 million inactive magnetars [5] in the Milky Way, however these are almost impossible to detect. Location of 1979 SGR inside N49 supernova remnant (X ray image inset) (Image Hubble/ROSAT) When the flux is frozen in, the flux moves with the plasma and vice versa (Priest 2000) Magnetic reconnection (Priest 2000) Radio image of the location of SGR1806-20 (Image University of Hawaii) Gamma ray intensity from 1979 burst [1] Magnetohydrodynamics Here are some of the central equations describing MHD: An important quantity is the magnetic Reynold’s number R m which is the ratio of the advection term to the diffusion term in the induction equation. Ideal MHD is the case in the limit where R m >>1, here many interesting phenomena emerge, such as flux “freezing”. Energy equation Momentum equation Continuity equation Induction equation B B v B 2 ) ( t 0 ) ( V t L p Dt D 1 B j p v v v ) ( t Magnetic Reconnection is the cause of phenomena like CME’s (Image NASA) Twisted magnetic field inside a magnetar [6]

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Page 1: GIANT FLARES AND MAGNETARS - Trinity College Dublintrussn/Projects/Magnetar_Poster_1.pdf · magnetar is the most highly magnetized object ever observed[9], with magnetic field of

Giant Flares Giant flares are enormous emissions of electromagnetic energy, far larger than

ordinary observed bursts. These events are extremely rare, but also spectacular. The three largest were observed in 1979[1] , 1998[6] and 2004[7].

These events are powerful enough to saturate every gamma radiation detector in space. Existing theoretical models had difficulty explaining the magnitudes of some of these outbursts. Currently there are several competing models explaining the mechanism behind giant flares.

SGR 1806-20 The event in 2004[7] was the largest ever observed,

it saturated satellite instruments for up to 0.5 s.[9] This magnetar is the most highly magnetized object ever observed[9], with magnetic field of over 1011 T. It unleashed energy at a rate of about 1040 watts for 0.2s.

The total energy produced was more than the Sun emits in 150,000 years[9]. Thankfully it is located approximately 40,000 light years away[4] and so did not pose a significant danger. The magnitude of the flare observed led to the development of the Lyutikov model to allow for the larger flare energies.

Open Questions • Research is being done into 3D magnetic reconnection, and relativistic models for

reconnection.

• Theoretical models for giant flare mechanisms need to be improved upon, as none of the current proposed models are entirely satisfactory.

• Can a method be developed to detect inactive magnetars?

• Can magnetars be used to detect gravitational wavebursts?

References

1. E.P. Mazets et al. 1979 Nature 282, 587 - 589 2. C. Thompson and R. C. Duncan 1992 ApJ 392, L9 3. A. I. Ibrahim et al. 2001 ApJ 558 237 4. McGill Online SGR/AXP Catalogue

http://www.physics.mcgill.ca/~pulsar/magnetar/main.html 5. R.C. Duncan, 2003 6. C. Thompson,R. and C. Duncan 2001 ApJ 561, 980 7. K. Hurley et al. 2005 Nature 434, 1098-1103 8. M. Lyutikov 2006 MNRAS 367, 1602 9. S. E. Boggs et al. 2007 ApJ 661, 458

Flux Freezing In a perfectly conducting fluid, a phenomenon

occurs whereby the magnetic field lines move with the material, i.e they are "frozen" into the plasma. Motions along the field lines do not change the field, but motion transverse to the field lines carry the field with them. If field lines in a star pass through the surface, the field is anchored to surface. This means that for huge magnetic fields, there are huge forces acting on the surface. This leads to "winding up" of field lines in the interior of a magnetar, giving rise to enormous internal magnetic stresses.

GIANT FLARES AND MAGNETARS Mark Allen and Nikki Truss

Trinity College Dublin Supervisor: Professor Tristan McLoughlin

Comparison of Two Giant Flare Models Crust Failure Model

• Thompson, Duncan (2001)[6]

• Magnetic stresses in core become too great, exceeding the elastic stresses in the crust

• Quick and brittle fracture of the crust occurs, i.e starquake

• Due to the relaxation of internal magnetic stresses, energy is released via giant flares

• Energy limited by tensile strength of crust

• Created after the 1998 event, which reached a peak luminosity of 106 LEdd [6]

Magnetospheric Model • Lyutikov (2006)[8]

• Slow untwisting of the internal magnetic field leads to twisting of magnetospheric field lines

• Flux injection leads to increase in magnetospheric energy held in flux ropes

• Unstable flux ropes rupture and release energy via giant flares

• Energy limited by total external magnetic field

• Created to explain magnitude of 2004 event which reached a peak luminosity of 109 LEdd [7]

Magnetic Reconnection Magnetic reconnection is at the heart of many magnetar phenomena. The magnetic

field stores energy, and when the topology of the magnetic field changes, this energy is released as EM radiation. There are various models describing magnetic reconnection in two dimensions, such as the Sweet-Parker, Petschek, and almost uniform models. Meanwhile, 3D reconnection is still a very new field where progress is driven by computational models.

Introduction

In 1979[1], a large burst of gamma rays was detected from the Large Magellanic Cloud. The object that produced this burst was monitored over a period of time and was eventually dubbed a ‘Soft Gamma Repeater’ (SGR) due to its periodic bursts of energy in the soft-gamma region of the spectrum. In 1992, Robert Duncan and Christopher Thompson proposed the magnetar model[2] to explain these large emissions of energy. These proposed magnetars were neutrons stars with extraordinarily large magnetic fields and a short but active lifetime. Along with the repeated smaller bursts, occasionally magnetars have been observed to release enormous bursts of electromagnetic radiation, known as giant flares.

Magnetar Formation Magnetars are hypothesised to be a type of neutron star, and like

other neutron stars, are believed to be the result of supernova collapse. They are thought to have diameters in the range of 10 - 20 km and masses greater than that of the Sun. The large magnetic fields of magnetars are thought to result from dynamo action during their formation. In magnetars, dynamo action increases their magnetic field from 108 T to 1011 T.[3] There are currently 20 confirmed magnetars[4], along with 3 proposed candidates. They are located between 10,000 - 50,000 light years away, and are only active for approximately 10,000 years. There are an estimated 30 million inactive magnetars[5] in the Milky Way, however these are almost impossible to detect.

Location of 1979 SGR inside N49 supernova

remnant (X ray image inset) (Image Hubble/ROSAT)

When the flux is frozen in, the flux moves with the plasma and vice

versa (Priest 2000)

Magnetic reconnection (Priest 2000)

Radio image of the location of

SGR1806-20 (Image University of Hawaii)

Gamma ray intensity from 1979 burst [1]

Magnetohydrodynamics Here are some of the central equations describing MHD:

An important quantity is the magnetic Reynold’s number Rm which is the

ratio of the advection term to the diffusion term in the induction equation. Ideal MHD is the case in the limit where Rm >>1, here many interesting phenomena emerge, such as flux “freezing”.

• Energy equation

• Momentum equation

• Continuity equation

• Induction equation BBv

B 2)(

t

0)(

V

tL

p

Dt

D

1

Bjpvvv

)(

t

Magnetic Reconnection is the cause of phenomena like CME’s (Image NASA)

Twisted magnetic field inside a magnetar[6]