• Nenhum resultado encontrado

Braz. J. Phys. vol.30 número3

N/A
N/A
Protected

Academic year: 2018

Share "Braz. J. Phys. vol.30 número3"

Copied!
4
0
0

Texto

(1)

On Positron Radiation Belt in the

Earth's Magnetosphere

A.A. Gusev 1

,U.B. Jayanthi 2

, I.M. Martin 1

, G.I.Pugaheva 1

, and W.N. Spjeldik 3

1

UniversityofCampinas, InstitutodeFsia/DRCC,13083-970, Campinas,SP,Brazil

2

InstitutoNaionaldasPesquisas Espaiais,INPE,S~aoJosedosCampos,SP, Brazil

3

Department ofPhysis,WeberStateUniversity,Ogden, Utah84408-2508,USA

Reeived28February,2000

Theratioofpositron/eletronuxesoriginatedinnulearspallationreationsintheEarth`s

magne-tosphereisonsidered.Itissupposedthatpositronsaswellaseletronsareproduedinthedeayof

hargedpions(

!

!e

)borninnulearollisionsoftrappedrelativistiinnerzoneprotons

withthe residual atmosphere. These positronsand eletrons are aptured inthe magnetosphere

andreatepositronand eletronradiationbeltsofnulear origin. Thepositron/eletron trapped

magnetospheriuxesformedwiththismehanismaresimulatedandtheresultingomputede +

=e

uxratio4appearsinagreementwiththereentobservations. Thisratioissigniantlydierent

fromtheratio1obtainedfromtheprimaryosmiraysourethroughthesamemehanism.

I Introdution

In our reent papers [1,2℄ we showed that signiant

uxes of trapped anti-partiles must exist in the

in-nermost magnetosphere of the Earth. However they

are not of that primordial nature of origin, whih

at-trats the generalinterest of astrophysis ommunity,

but are born in a more trivialproess, as seondaries

from nulear spallation reations of energeti trapped

protons andprimaryosmi rays(CR) withthe

resid-ual terrestrial (or other planet's,for example, Jovian)

atmosphere. These seondary partiles being trapped

bytheEarth'smagnetieldanbeaumulatedthere

andformmoreradiationbelts,forexample,anti-proton

andpositronradiationbelts,inadditiontoalready

ex-istingones i.e. thoseofprotons, eletronsand

anoma-lous CR nulei. These trapped uxes of anti-protons

andpositronsouldbeevengreaterthantheseondary

interstellaruxeswhiharegeneratedbyCRononly5

- 7g.m 2

of interstellarmatter. These uxes are

pro-dued on the 2-3 radiation lengthsof eletronsin the

air[3℄,thatis363=108g/m 2

. Thus,theyould

beabout 15-20 timesgreater than interstellarones at

ertainenergies. Duringgeomagnetiunstableperiods

theyouldpossiblypreipitateinto theatmosphereor

ouldleavethemagnetosphereandappearinthe

inter-planetarymedium,ausingnewpuzzles.

In the same spallation reations the trapped

en-ergeti protons also produe the isotopesof light

ele-3

and 3

He isotopes were atually observed reently by

SAMPEX and CRRES satellites [6,7℄. This disovery

supportstheideathatsigniantuxesoftrapped

se-ondarypositronsouldbeproduedbythetrapped

pro-tonsontherareeddensityoftheresidualatmosphere

at thealtitudesof300{1000km.

Signianttrapped energeti positron uxes ould

beobservedaordingtothis ideaintheinnerestpart

ofthegeomagnetospherewhereatmosphereisrare,but

still existsand whereasuÆientux ofenergeti

pro-tonsexiststosustainthepositronpopulation.

However,until last yearthere wasnolear

experi-mentalonrmationoftheexisteneofapositron

radi-ation belt. Inthepreviousexperimentswithmagneti

spetrometerperformedonboardoftheCOSMOS-1669

and MIR station ontraditoryresults were obtained.

It seems that the new generation of experiments

-nallymanagedtoprovetheidea: InJuly's1999issueof

CERN Courieritwasommuniatedthat Alpha

Mag-neti Spetrometer(AMS)[8℄observedhigh energy(>

200MeV)positronux in theequatorialregionat the

altitude of 400 km with the intensity about 4 times

higherthan theeletronux ofthe sameenergv. The

authorsharaterizedtheresultasverysurprisingand

puzzling. However,wethink thatthis observation isa

onrmationoftheaboveformulatedmehanismwhih

hasbeendevelopedsine1982[3,9℄.

Inthis paperit will be demonstrated that the

(2)

II The soure of positrons

Fromatheoretialpointofview,thepositronradiation

beltgenerationisabitmoreompliatedthanthe

for-mationoftheisotoperadiationbelts. The

geomagneti-allyonnedpositronsdonotappearasanimmediate

diret produtofanulearreation. Rather,thebasi

mehanism of positron and eletron nulear ollision

generation isthemuon-positron deayof harged

pos-itivepions andkaons, resultingfrom thesamenulear

reationswheredeuterium,tritiumand 3

Heseondary

nulei are born. The other dierene is that for pion

prodution,thereexistsanimportantminimumenergy

threshold of 290 MeV per inident proton on an

ex-ospheri neutral. This largeinident proton energyis

neessaryforaprotontoprodueapioninthereation

withtheatmospheritargetnuleus.

To be spei, in nulearspallation reationsboth

negativeandpositivepionsandkaonswillbeprodued

alongwiththeseondarynulei. Onetheseshort-lived

partilesareborntheydeayinto:

;K ) + )e

+~+ (1)

Infat,theyaresoshort-livedthattheydeay

pra-tially at the sameplae in the magnetospherewhere

theyareborn. Theirshort lifetime

0

isof26

nanose-onds for harged pionsand 2.197 sfor muons. They

ould travelfrom thepoint of generation for only the

distaneofabout:

0

v,herev-pion's,muon'sveloity,

is a partile Lorentz fator. For example, for 1000

MeVpionthistraveldistaneis: 1000/139.57*2.610 8

s*310 5

km/s=56m. Fora1000MeVmuonthetravel

distane is: 1000/105.66*2.19710 6

s *3.10 5

km/s=

6.25 km. Thus, from the point of view of

magneto-spheri partile apture, it means that the positrons

are born and trapped in the same region of

magne-tosphere, where energeti trapped protons exist. The

onnement areaat L<1:2 isonentrated in avery

restritedanglenearthegeomagnetiequatorialplane.

Duetothatonlythepositronsbornwithveloity

dire-tionwithinthisangle(i.e. neartheplaneoftheparent

proton Larmourrotation)an beaptured andwillbe

takenintoaountinthefollowingonsideration.

In Fig.1 we depit the loation of > 400 MeV

trappedproton uxat thealtitudeof 400km over

at-mosphere based on the AP-8 magnetospheri proton

model[10℄.

Reognizing, however, the strong dynamis of the

eletron radiation belt observed reently [11℄, the

positron belt spatial loation may sometimes be

dif-ferentfromthatoftheparentprotonsandthepositron

uxes ould even disappearfrom the areaand appear

intheinterplanetarymediumastheresultofhigh

geo-magnetiativity.

Figure1.Thespaedistributionofthe>400MeVtrapped

protonsatthealtitudesof400kmaordingtoAP-8model

(Vette,1991).

III The positron beltformation

ToalulatethepositronuxF

e +

(E)wemustintegrate

thepositron dierentialprodution spetrumP

e (E

0

)

(i.e. uxes generated in 1g/m 2

of the air) alongthe

positrontrajetorytakingintoaountthatapositron

ofenergyE wasbornwithenergyE 0

atthedistaneof

X 0

g/m 2

fromthepointofobservation. Ifthepositron

energy losses are (dE=dX); it results in the

relation-ship: F e (E) = R 1 0 P e (E 0 )(dE 0 =dE)dX 0 = P e (>

E)=(dE=dX) [2℄, i.e. the e +

=e ux ratio is

propor-tionaltotheratiooftheirintegralprodutionspetra.

Themeanfrationofenergyarriedawaybyamuon

inapion'sdeayandbyaneletroninamuondeayis

typiallyequaltoq

1

=0:80and q

2

=0:33respetively.

With this simpliation, we an relate the positron

(eletron) P

e

and pion produtionspetraQ

with

thefollowingrathersimpleexpression:

P e (E)= 1 q 1 q 2 Q (E=q 1 q 2 ):

Fromthissetofphysial ideasandamodest

math-ematialonstrutiononeanrathertransparentlysee

that positron/eletron ux ratioat equalenergies per

partileisproportionaltotheratioofpositiveand

neg-ativeintegralpionprodutionspetraQ

(>E)atthe

l=q

l q

2

greaterenergiesthaneletronones:

F e +(E)=F e (E)= Q +(>E=q 1 q 2 )

Q (>E=q

1 q

2 )

(3)

Thepionprodutionspetrafor

pionswere

ear-lieromputed[1℄fortrappedprotonuxesat L=1:2.

These arepresentedin Table1. Fromthis oneansee

thatthissouremehanismprovidesfourtimesgreater

positivepionuxesthannegativepionuxesatpion

en-ergiesofmorethan600-800MeV.Consequently,these

produtionspetraofseondarypartileuxesan

sup-ply four times greater positron uxes than eletron

uxes at energies morethan 150- 200 MeV on these

geomagnetiL-shells.Indeed,thisispreiselythesame

positron-to-eletronuxratiothatwasobservedinthe

AMSexperimentnotedaboveforpositron/eletronux

ratio at energies of more than 200 MeV per partile.

Wethusonludethatthepuzzleappearsresolved,and

thatthereexistsasimplephysialexplanationbasedon

the knowledge of the nulear ollision reations from

whihmostpositivepionsareborn.

Table1. Thepionprodutionspetra.

The geomagnetially trapped protons have

rela-tivelylowenergies(fromanulearinterationpointof

view) and less than 1 seondary pion per reation is

generated. Certainlytheyhavepositive(!) hargedue

to thehargeonservation law. Inomparison, in the

aseofpositronsbornbyprimaryCR,havingtensGeV

energies,agreatermultipliity ofpionsgenerated,and

thepositronux exessis negligible.

TotheoretiallysearhapositronuxfromtheCR

soure,weusedaversionofanulearreationomputer

ode SHIELD for Monte Carlo simulation of hadron

asades in matter[12℄. Usingthis ode weomputed

positiveandnegativepionprodutionspetrafrom

pro-tonswith variousenergiesorrespondingto the

upper-most range of trapped proton energies (500 MeV - 2

GeV)intheinnermostpartsofthemagnetosphereand

toCRprotonomponent(morethan8-10GeVforthe

magnetospheri equatorial region). The ratios of the

integralprodutionspetraofpositiveandnegative

pi-ons for various parent proton energies are plotted in

Fig. 2. Aswementionedabovethis ratio isthe same

ase +

=e ux ratio. Fromthis gureonean

immedi-soureislessthanfromthetrappedprotonsoureand

equal1formorethan100MeV positron energies.

Figure2.Curve1: Thedependeneofthee +

=e -uxratio

ontheparentprotonenergy;urves2-7: Thedependene

ofthe +

= integralprodutionuxratioande +

=e ux

ratioontheande

energies,orrespondingly.

Intheinnermostpartof magnetosphere,at low

L-shells of L 1:2 it is diÆult to expet an existene

of hundredsMeVtrappedeletronsof diusiveorigin.

As it was shown in [13,14℄ the eletrons an not

dif-fuse there from the boundary of magnetosphere

be-ausetheylossitsenergyduetosynhrotronradiation

andundergostrongpith-anglesatteringwithplasma

wavesattheregionofL3onthewayintoinner

mag-netosphere. Thus, a diusive eletron omponent at

those energiesdoesnotdereaseomputede +

=e ux

ratioobtainedfrom nulearsoureandinobservations

in theinnermostpartofmagnetosphereexatlye +

=e

ux ratio equalto 4 is expeted to be registeredin

the ase of nulear reationsoure of magnetospheri

positrons.

IV Conlusion

A mehanismforgeneration oftheterrestrial positron

radiationbeltduetonulearreationsoftrapped

radi-ationbeltprotonswiththenuleioftheneutralatoms

in the upper atmosphere/exosphere region is

onsid-ered. The ratio of positron/eletron uxes omputed

(4)

four times the ambient eletronux in theequatorial

region for partilesof morethan 200MeV.That is in

exellentagreementwiththeAMS-instrument

observa-tions reported in the literature. In ontrast, the CR

soure in this region providesa positron/eletron ux

ratioaboutequal1. TheCRuxesarethusnot

respon-siblefortheobservedinnermostradiationbeltpositrons

and eletrons. We believethat this physial

onsider-ation will help to solvethepuzzle of theuniqueAMS

positronbeltobservation.

Aknowledgements

TheworkwassupportedbyFAPESP-SP

(93/4978-0) andCNPq(300015/99-2).

Referenes

[1℄ A.A. Gusev, I.M.Martin,G.I. Pugaheva,A. Turtelli

Jr., W.N. Spjeldvik, Il Nuovo Cimento, Set. C, 19,

461(1996).

[2℄ G.I. Pugaheva, W.N. Spjeldvik, A.A. Gusev, I.M.

Martin,J.Atm.Sol.-Terr.Phys.59,363(1997).

[3℄ R.N. Basilova, A.A. Gusev, G.I. Pugaheva, A.F.

Titenkov, Geomagnetism and Aeronomia, 22, 671

(1982).

[4℄ W.N. Spjeldvik, G.I. Pugaheva, I.M. Martin, A.A.

Gusev,N.M.Sobolevsky,AdvanesinSpaeResearh,

[5℄ W.N. Spjeldvik, G.I. Pugaheva, A.A. Gusev, I.M.

Martin, and N.M. Sobolevsky, Annales Geophysiae,

16,931(1998)b.

[6℄ J.Chen, T.G.Guzik,J.P.Wefel, K.R.Pyle, and J.F.

Cooper,J.Geophys.Res.101,24(1996).

[7℄ R.S. Selesnik, and R.A. Mewaldt, J. Geophys. Res.

101,19745(1996).

[8℄ Cern Courier, Magneti detetor sees osmi-ray

anomalies,39,6(1999).

[9℄ I.M.Martin,A.A. Gusev, G.I.Pugaheva,A. Turtelli

Jr.,Yu.V.Mineev,J.Atmosph.and Terr.Phys.57.2,

201(1995).

[10℄ J.I.Vette,Rep.NSSDC 91-24,NASAGoddardSpae

FlightCenter,Greenbelt,Md.November,(1991).

[11℄ A.A.Gusev, T. Kohno,I.M. Martin,G.I. Pugaheva,

A. Turtelli Jr., A. Tylka, K. Kudela. Planetary and

SpaeSiene,43,1131 (1995).

[12℄ N.M. Sobolevsky, G.I. Pugaheva, A.A. Gusev, and

I.M.Martin,The-Proeedingsofthe8thInternational

ConfereneonRadiationShielding,April24-28,1994:

Arlington,TX,publishedbytheAmerianNulear

So-iety,619(1994).

[13℄ G.I.Pugaheva,D.M.Bosher,A.A.Gusev,I.M.

Mar-tin,W.N.Spjeldvik,Geoph.Res.Let.25,1519(1998)a.

[14℄ G.I.Pugaheva,D.M.Bosher,A.A.Gusev,I.M.

Mar-tin,WN.Spjeldvik,J.Atm.Sol.-Terr.Phys.60,1159

Imagem

Figure 1. The spae distribution of the &gt; 400 MeV trapped
Table 1. The pion prodution spetra.

Referências

Documentos relacionados

higher arbon ontent the density of Si-C bonds should. derease and the C-C bonds

lms were grown on &lt; 100 &gt; silion using the neutral luster beam deposition tehnique). These lms were highly rystalline and

the tree level) of Fierz-Pauli higher derivative theory. T o begin with we analyze the poles to

The observed harateristis are explained using small signal a iruit analysis.. It is shown that the theoretial urve generated using the a iruit analysis gives

oupied moleular orbital (H), the next lower oupied level (H-1), their energy dierene value () and their relative. ontribution dierene to the LDOS ()

The stati and spherially symmetri solution of the eld of a harged point.. partile

the present higher-derivative model the magneti eld restores hiral symmetry broken initially on.. the

The expliit form of the multipliative and onformal anomalies in losed oriented hyperboli.. manifolds