High-energy cosmic ra ys and w eak-scale string theo ries - - PDF document

high energy cosmic ra ys and w eak scale string theo ries
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High-energy cosmic ra ys and w eak-scale string theo ries - - PDF document

High-energy cosmic ra ys and w eak-scale string theo ries Michael Pl umacher Universit y of Oxfo rd M. Kachelrie, M. P .: Phys. Rev. D 62, 103006; astro-ph/0005309 Outline Intro duction La rge extra


slide-1
SLIDE 1 High-energy cosmic ra ys and w eak-scale string theo ries Michael Pl umacher Universit y
  • f
Oxfo rd M. Kachelrie, M. P .: Phys. Rev. D 62, 103006; astro-ph/0005309 Outline
  • Intro
duction
  • La
rge extra dimension s
  • Neutrino-Nucleon
scattering
  • Conclusions
slide-2
SLIDE 2 Intro duction Detection
  • f
cosmic ra ys:
  • Energy
sp ectrum: p
  • w
er la w b ehaviour
  • ver
a wide range
  • f
energies
  • p
rima ries a re shielded b y the atmosphere
  • fo
r energies less than
  • 100
T eV the cosmic ra y ux is high enough to allo w direct detection
  • f
p rima ries from space
  • ab
  • ve
  • 100
T eV sho w ers
  • f
seconda ry pa rticles can b e detected from the ground Comp
  • sition:
  • muon
content and depth
  • f
sho w er maximum p rovide info rmation
  • n
the chemical comp
  • sition
  • rule
  • f
thumb: heavy nuclei p ro duce air sho w ers with a higher muon content and a sho w er maximum higher up in the atmosphere than light
  • nes
slide-3
SLIDE 3
slide-4
SLIDE 4 Greisen-Zatsepin
  • Kuzm
in (GZK) cuto at energies E > 6
  • 10
19 eV p rotons lose energy due to pion photop ro duc tion p +
  • CMB
  • !
  • +
  • !
p +
  • fo
r nuclei at E
  • >
10 19 eV: photo disint egra tion in the CMB and IR background 56 F e +
  • CMB
  • !
55 F e + n photons interact with the CMB and the geomagnetic eld ) pair p ro duction ab
  • ve
  • 200
T eV Events ab
  • ve
10 20 eV have b een
  • bserved:
events a re consistent with nucleon p rima ries:
  • longitudin
al sho w er p role
  • f
the Fly's Ey e event b est tted b y a p roton
  • lateral
electron and muon distribut ion s measured b y A GASA indicate that the p rima ries a re nucleons isotropic a rrival directions ) extragalactic
  • rigin
no plausibl e astrophysical sources within
  • 100
Mp c Could neutrinos b e the p rima ries?
slide-5
SLIDE 5

0.01 0.1 1 10 1017 1018 1019 1020 1021 E2.7dN/dE (cm-2sr-1s-1GeV1.7) E (eV / nucleus) All-particle spectrum α=2.25 α=2.0 Super-GZK Akeno [16] MSU [17] AGASA [18] Haverah Park [19] Yakutsk [20] Fly’s Eye (mono) [21] Fly’s Eye (stereo) [6]

slide-6
SLIDE 6

100 200 300 250 500 750 1000 Depth in g/cm2 Number of particles/109

500 550 600 650 700 750 800 850 900 16.5 17 17.5 18 18.5 19 19.5 20

Xmax (g/cm2)

log10 ( E(eV) ) Fly’s Eye [6] HiRes-MIA [7] Haverah Park [8] Yakutsk [9] SIBYLL 2.1 [11] QGSJET [12]

slide-7
SLIDE 7 La rge Extra Dimension s Consider a w
  • rld
with
  • extra
dimensions Compacticati
  • n
radius R Standa rd mo del elds live
  • n
a 3-b rane ) they do not feel the extra dimensions
  • nly
gravit y p ropagates in the higher dimensional space ) Gravit y is w eak due to the la rge compacticatio n radius G 1 N = 8 R
  • M
  • +2
D F undamental mass scale M D
  • 1
T eV ) R
  • 1
mm fo r
  • =
2 Solution to the hiera rchy p roblem? 4-d Planck scale
  • electro
w eak scale new hiera rchy p roblem: M D
  • 1
T eV
  • R
1
  • 10
3 eV
slide-8
SLIDE 8 Astrophysical b
  • unds
Sup ernova b
  • unds:
SN 1987a (Hanha rt et al., astro-ph/0102063) energy loss due to KK emission ) sho rtening
  • f
the neutrino signal
  • =
2 ) M D > 60 T eV
  • =
3 ) M D > 5 T eV SN contributi
  • ns
to
  • ra
y background: (S. Hannestad et al., hep-ph/0103201) deca ys
  • f
KK gravitons emitted b y all SNe
  • ver
the age
  • f
the universe K K ! 2 ; e + e
  • ;
  • )
contribution to the diuse
  • ra
y background
  • =
2 ) M D > 84 T eV
  • =
3 ) M D > 7 T eV
slide-9
SLIDE 9 Cosmol
  • gi
cal Bounds KK gravitons a re p ro duced in the ea rly universe at high temp eratur es: pair annihilat ion : 2 ; e + e
  • ;
  • !
K K gravi-b remsstrahl un g gravi-Compton scattering contributio ns to
  • ra
y background : (S. Hannestad, hep-ph/0102290) T M AX during reheating 1 GeV
  • =
2 ) M D > 170 T eV
  • =
3 ) M D > 20 T eV
  • =
4 ) M D > 5 T eV
  • =
5 ) M D > 2 T eV contribution to the energy densit y
  • f
matter (M. F airbairn, hep-ph/0101131) ) ea rlier matter-radia tion equalit y ) lo w age
  • f
the universe T RE H = 170 MeV and t > 12:8 Gyrs
  • =
2 ) M D > 10 3 T eV
  • =
3 ) M D > 60 T eV
  • =
4 ) M D > 9 T eV
slide-10
SLIDE 10 Naturally realized in T yp e I string theo ries:
  • SM
elds co rresp
  • nd
to
  • p
en strings b eginnin g and ending
  • n
D-b ranes
  • gravitons
co rresp
  • nd
to closed strings which can p ropagate in the higher dimensiona l space ) from
  • ur
4-dimensiona l p
  • int
  • f
view the graviton is an innite to w er
  • f
Kaluza-Klein excitations with masses m 2 ~ n = ~ n 2 R 2 assume g ~ n = p 8 M Pl in p ro cesses mediated b y a virtual graviton
  • ne
has to sum
  • ver
all KK-mo des X ~ n 1 p 2
  • m
2 ~ n diverges fo r
  • >
1 ! intro duce cuto b y hand j ~ nj < M st R
slide-11
SLIDE 11 ) Neutrino-Nucl eon cross section at high energies
  • tot
  • E
10 20 eV
  • 2
  • 1
T eV M D
  • 4
ba rn 4-dim eld theo ry result not valid fo r E > M D eld theo retical unita rizati
  • n:
  • tot
  • 4
s M 4 D
  • E
10 20 eV
  • 1
T eV M D
  • 4
mba rn Right
  • rder
  • f
magnitude to explain the ultrahig h energy cosmic ra y events! Ho w ever, lo w energy eective theo ry not valid fo r E
  • 10
20 eV nite width
  • f
the b ranes b ecomes imp
  • rtant
b rane tension supp resses the couplings
  • f
higher KK mo des g n = g e c(n=R) 2 = M 2 D ; where c = 1 2
  • M
D f
  • 4
slide-12
SLIDE 12 Neutrino-Nucleon Scattering mediated b y graviton in the t-channel Sum
  • ver
all KK mo des: exp
  • nential
supp resion
  • f
couplings
  • f
higher KK mo des p rovides a dynamical cuto P ( ^ t ) = R
  • P
~ n exp ( cm 2 ~ n = M 2 D ) ^ tm 2 ~ n =
  • =2
( ^ t )
  • =21
exp
  • c
^ t M 2 D
  • 1
  • 2
;
  • c
^ t M 2 D
  • Cross-section
in the lo w-energy limit, s
  • M
2 D Neutrino-qua rk scattering: d d xd ^ t = 1 512 ^ s 2 P 2 ( ^ t ) M 4+2 D
  • 32
^ s 4 + 64 ^ s 3 ^ t + 42 ^ s 2 ^ t 2 + 10 ^ s ^ t 3 + ^ t 4
  • gluon-neutrin
  • scattering
d
  • dxd
^ t = 1 32 ^ s 2 P 2 ( ^ t) M 4+2 D
  • 2
^ s 4 + 4 ^ s 3 ^ t + 3 ^ s 2 ^ t 2 + ^ s ^ t 3
slide-13
SLIDE 13 T
  • tal
cross section:

1e-09 1e-08 1e-07 1e-06 1e-05 1e-04 0.001 0.01 0.1 1 10 17 17.5 18 18.5 19 19.5 20 20.5 21

log(Eν/eV) σνN/mbarn CC 6 TeV 15 TeV 30 TeV

) M D
  • 1
T eV needed fo r
  • KK
N
  • =
1
  • 10
mba rn energy-loss in SN 1987a due to KK graviton p ro duction M D
  • >
60 T eV Age
  • f
the universe
  • >
12 Gyrs ) M D
  • >
10 3 T eV
slide-14
SLIDE 14 Energy transfer: y = (E
  • E
  • )=E
  • nucleon-nuc
leon collisions: y
  • 0:6

0.05 0.1 0.15 0.2 0.25 0.3 0.35 0.4 0.45 0.5 3 4 5 6 7 8 9 10 11 12

log(Eν/GeV) y CC g q

) neutrinos a re deeply p enetrati ng pa rticles
slide-15
SLIDE 15 Cross section in the high-energy limit s
  • M
2 D 1. e. 4-dim. theo ry not valid fo r s > M 2 D 2. and
  • KK
N
  • violates
unita rit y ) calculation
  • f
  • KK
N
  • in
string theo ry needed Conservative upp er b
  • und:
Unita rize the cross section:
  • Regge
Amplitude
  • eik
  • nal
metho d xes the energy dep enden ce
  • f
the cross section:
  • tot
/ ln 2 (s=s ) cho
  • se
constant as
  • KK
N
  • (s
), where s
  • M
D is the scale where s-w ave unita rit y is violated
  • tot
(s) =
  • KK
N
  • (M
2 D ) ln 2
  • s=
M 2 D
  • s=
M 2 D
  • 0:363
slide-16
SLIDE 16 String theo ry calculati
  • n:
(Co rnet, Illana and Masip, hep-ph/0102065) T yp e I IB
  • rbifold
6 la rge extra dimension s SM elds conned to N D3 b ranes V eneziano Amplitude S (s; t) = (1
  • s)(1
  • t)
(1
  • s
  • t)
gives a series
  • f
p
  • les
and zero es ) string amplitude can b e app ro ximated as a sum
  • ver
s-channel resonances (lepto qua rks) Neutrino-Nucle
  • n
total cross section: M S = 2:0 T eV M S = 0:5 T eV SM (i) (ii) (i) (ii) E
  • [GeV℄
  • N
[ m 2 ℄ 10 13 10 12 10 11 10 10 10 9 10 8 10 7 10 6 10 5 10 4 10 3 10 2 10 29 10 30 10 31 10 32 10 33 10 34 10 35 10 36 10 37
slide-17
SLIDE 17 Conclusions Neutrino-nucl eon interaction s via KK gravitons in mo dels with la rge extra dimension s cannot explain the ultrahigh energy cosmic ra ys:
  • supp
ression
  • f
KK couplings due to b rane uctuations )
  • KK
N
  • is
small
  • energy
transfer p er interaction is small neutrinos a re deeply p enetrati ng pa rticles ) sho w ers initiated b y p rotons and neutrinos a re clea rly distinguish ab le Outlo
  • k:
neutrino induced ho rizontal air sho w ers ma y give interesting b
  • unds
  • n
the string scale