stochastic acceleration of cosmic rays in anisotropic plasma turbulence

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STOCHASTIC ACCELERATION OF COSMIC RAYS IN STOCHASTIC ACCELERATION OF COSMIC RAYS IN ANISOTROPIC PLASMA TURBULENCE ANISOTROPIC PLASMA TURBULENCE Yurij Fedorov Yurij Fedorov 1 , and Milan Stehlik , and Milan Stehlik 2 1 Main Astronomical Observatory NASU, Kiev, Ukraine 2 Institute of Experimental Physics SAS, Košice, Slovakia

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STOCHASTIC ACCELERATION OF COSMIC RAYS IN ANISOTROPIC PLASMA TURBULENCE. Yurij Fedorov 1 , and Milan Stehlik 2 1 Main Astronomical Observatory NASU, Kiev, Ukraine 2 Institute of Experimental Physics SAS, Ko š ice, Slovakia. The diffusion coefficient in momentum space. Conclusions. - PowerPoint PPT Presentation

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Page 1: STOCHASTIC ACCELERATION OF COSMIC RAYS IN ANISOTROPIC PLASMA TURBULENCE

STOCHASTIC ACCELERATION OF COSMIC RAYS IN STOCHASTIC ACCELERATION OF COSMIC RAYS IN ANISOTROPIC PLASMA TURBULENCEANISOTROPIC PLASMA TURBULENCE

Yurij FedorovYurij Fedorov11, and Milan Stehlik, and Milan Stehlik22

1Main Astronomical Observatory NASU, Kiev, Ukraine2Institute of Experimental Physics SAS, Košice, Slovakia

Page 2: STOCHASTIC ACCELERATION OF COSMIC RAYS IN ANISOTROPIC PLASMA TURBULENCE

K i c h a t i n o v , 1 9 8 3 .

;0v

p

fF

r

f

t

f

( 1 )

;Hu1

;Hv

cE

c

eEeF

;10 HHH

;10 uuu

;0v

p

fD

pp

fF

r

f

t

f

( 2 )

;),,(),,(),,;,,( 11111111 tprFtprFtprtprD

0

);,,v;,,( tprtprDdD

Page 3: STOCHASTIC ACCELERATION OF COSMIC RAYS IN ANISOTROPIC PLASMA TURBULENCE

; v 000 Hc

eEeF

;

11000 c

Hu

c

HuE

; 011 HHu ( 3 )

K r a u s e , R a d l e r , 1 9 8 0

;22

1Q

p

NpDp

ppt

N

( 4 )

;KDFDpD

;v3

21

2

up

FD ( 5 )

F e r m i , 1 9 4 9 ; T o p t y g i n , 1 9 8 5 .

;2v3

22

R

pKD

( 6 )

K i c h a t i n o v , 1 9 8 3 ; F e d o r o v , K a t z , K i c h a t i n o v , S t e h l i k , 1 9 9 2 .

Page 4: STOCHASTIC ACCELERATION OF COSMIC RAYS IN ANISOTROPIC PLASMA TURBULENCE

;2

21

2

RuFD

KD

;; mc

p

;2

0

02

1

2

Ru

;1 21 FD ;1 21

KD

U n r e l a t i v i s t i c : ;1;1 KDFD

U l t r a r e l a t i v i s t i c : ;;2 KDFD

;)1(22

0

02

1

2

RuFD

KD

Page 5: STOCHASTIC ACCELERATION OF COSMIC RAYS IN ANISOTROPIC PLASMA TURBULENCE

11

The diffusion coefficient in momentum spaceThe diffusion coefficient in momentum space

Page 6: STOCHASTIC ACCELERATION OF COSMIC RAYS IN ANISOTROPIC PLASMA TURBULENCE

11

Page 7: STOCHASTIC ACCELERATION OF COSMIC RAYS IN ANISOTROPIC PLASMA TURBULENCE

;)()(

20

p

tppQ

;0

DD p

;)()(1

2302

2

mc

NN

( 7 )

; ; 0

2

0

0 D

mct

t

t

Page 8: STOCHASTIC ACCELERATION OF COSMIC RAYS IN ANISOTROPIC PLASMA TURBULENCE

:0

; 2

2),( 2

2

2

2

02

1

03

sIsKmc

sN

:0

; 2

2),( 2

2

02

2

2

1

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sIsKmc

sN

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2

2exp

)2(

)(),( 2

2

2

02

2

0

2

3

2

1

0

Imc

N (8)

;2

1

Page 9: STOCHASTIC ACCELERATION OF COSMIC RAYS IN ANISOTROPIC PLASMA TURBULENCE

11

Page 10: STOCHASTIC ACCELERATION OF COSMIC RAYS IN ANISOTROPIC PLASMA TURBULENCE

;)(1

2

02

2 p

ppq

t

N

p

NDp

ppt

N

e

p

( 9 )

B e c k e r e t a l . , 2 0 0 6 ; D e r m e r e t a l . , 1 9 9 6 ; D r o e g e , S c h l i c k e i s e r , 1 9 8 6 ; M i l l e r e t

a l . , 1 9 9 0 ; S t e i n a c k e r , S c h l i c k e i s e r , 1 9 8 9 .

;)()(1

23002

2

mc

qtNNN

e

( 1 0 )

;0t

t ee

:0

;2

2

)2(

222

0)2(

22

1

03)2(

02)(

e

Ie

Kmc

q tN ( 1 1 )

:0

;)2(

2

)2(

2

)2(

2)( 2

2

2

2

02

1

030

ee

KImc

qtN ( 1 2 )

Page 11: STOCHASTIC ACCELERATION OF COSMIC RAYS IN ANISOTROPIC PLASMA TURBULENCE

11

F ig .4 . T h e e n e rg e t ic s p e c tra c o r re s p o n d in g to th e s te a d y s ta te s o lu t io n (1 1 ) ,(1 2 ) .

N u m b e rs n e a r c u rv e s c o r re s p o n d to d im e n s io n le s s p a ra m e te r e = t e / t 0 .

T h e m o m e n tu m d if fu s io n c o e f f ic ie n t is g iv e n b y e q u a t io n (5 ) ; = 0 .5 .

1 0 -1 1 0 0 1 0 1 1 0 2 1 0 3 1 0 4

1 0 -8

1 0 -7

1 0 -6

1 0 -5

1 0 -4

1 0 -3

1 0 -2

1 0 -1

1 0 0

1 0 1

0 .0 1

0 .1

1

N m c 2 /q t0

Ek, M e V

Page 12: STOCHASTIC ACCELERATION OF COSMIC RAYS IN ANISOTROPIC PLASMA TURBULENCE

11

F ig .5 . T h e e n e r g e t ic s p e c t r a c o r r e s p o n d in g to th e s te a d y s ta te s o lu t io n ( 1 1 ) ,( 1 2 ) .

N u m b e r s n e a r c u r v e s c o r r e s p o n d to d im e n s io n le s s p a r a m e te r e = t e / t 0 .

T h e m o m e n tu m d i f f u s io n c o e f f ic ie n t i s g iv e n b y e q u a t io n ( 6 ) ; = 0 .5 .

1 0-1

1 00

1 01

1 02

1 03

1 04

1 0-8

1 0-7

1 0-6

1 0-5

1 0-4

1 0-3

1 0-2

1 0-1

1 00

1 01

0 .0 1

0 .1

1

N m c2/q t

0

Ek, M e V

Page 13: STOCHASTIC ACCELERATION OF COSMIC RAYS IN ANISOTROPIC PLASMA TURBULENCE

11

;

2

2

2

2

2

2

22

1

2

2

2

2

1

2

2

1

2

2

e

ee

e

K

KK

Page 14: STOCHASTIC ACCELERATION OF COSMIC RAYS IN ANISOTROPIC PLASMA TURBULENCE

11

Fig.7. The differential proton spectra on June 15, 1991 GLE

(Belov, Eroshenko, 1996).

Page 15: STOCHASTIC ACCELERATION OF COSMIC RAYS IN ANISOTROPIC PLASMA TURBULENCE

11

;

242

2exp

)2(),(

2

2

0

2

0

22

0

2

1

030

1

Id

mc

qtN

e;

2

22

1

Page 16: STOCHASTIC ACCELERATION OF COSMIC RAYS IN ANISOTROPIC PLASMA TURBULENCE

11

F ig .9 . T h e sp ec tra o f en erg e tic p a rtic les u n d er m o n o en erg e tic in jec tio n .

N u m b er n ea r cu rv es d en o te d im en sio n less tim e; D p = D F ; = 0 .5 .

10-1

100

101

102

103

10-5

10-4

10-3

10-2

10-1

100

101

S tead y s ta te so lu tion

0 .20 .050 .010 .001

N m c2/q t

0

Ek, M eV

Page 17: STOCHASTIC ACCELERATION OF COSMIC RAYS IN ANISOTROPIC PLASMA TURBULENCE

11

F ig .1 0 . T h e s p e c tra o f e n e rg e t ic p a r t ic le s u n d e r m o n o e n e rg e t ic in je c t io n .

N u m b e r n e a r c u rv e s d e n o te d im e n s io n le s s t im e ; D p = D k ; = 0 .5 .

1 0-1

1 00

1 01

1 02

1 03

1 0-6

1 0-5

1 0-4

1 0-3

1 0-2

1 0-1

1 00

S te a d y s ta te s o lu t io n

0 .20 .0 50 .0 10 .0 0 1N m c2/q t

0

Ek, M e V

Page 18: STOCHASTIC ACCELERATION OF COSMIC RAYS IN ANISOTROPIC PLASMA TURBULENCE

ConclusionsConclusions

Particle acceleration by large scale EF can Particle acceleration by large scale EF can be efficient for a medium of sufficiently be efficient for a medium of sufficiently high magnetic helicityhigh magnetic helicity

The results can be useful for description of The results can be useful for description of particle acceleration in astrophysical particle acceleration in astrophysical objects ( solar flares, supernova remnants, objects ( solar flares, supernova remnants, galactic nuclei, … )galactic nuclei, … )

Page 19: STOCHASTIC ACCELERATION OF COSMIC RAYS IN ANISOTROPIC PLASMA TURBULENCE

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