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GZK III: A Visit to the Zoo

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'Something' (1) penetrates CMB,(2) arrives in air showers, (3) ... it's not Science. Top-Down people need ... Very weird and singular as xT - 0. In other words, ... – PowerPoint PPT presentation

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Title: GZK III: A Visit to the Zoo


1
GZK III A Visit to the Zoo
  • How I protect my independence from various
    proposals

2
recall
  • Something (1) penetrates CMB,(2) arrives in air
    showers, (3) reported E gt 1019 eV, (4) shows
    angular correlations
  • YOUR probability
  • of something is for YOU to decide with help
    from statistics.

?????
P(GZK new physics) P(new physics)
P(new physics GZK)P(GZK)
3
The Physicists Gambit
  • P(new physics GZK)
  • P(GZK new physics) P(new physics)

P(GZK)
?????
????????
4
What do we want ?
  • We want to discover stuff!
  • Plenty of people have discovered nothing
  • Do you think 50 is good odds?
    . ... Is 10 good odds?

5
If you Are in Physics, You Already Paid the
Priceof Assuming New Physics Could Be
Found.P(new) finite.Right?
6
??????????
?
7
try to get morethings explainedthanthe number
of newassumptionsyou made
8
Nuclei
ANIMAL 1
  • 3o

Stecker
9
Nuclei
  • They exist
  • Even harder to accelerate up
  • Fall apart quickly in 30
  • Super-GZK, angular correlations ? no way.
  • Its something to do. Does it turn you on?

10
Strangelets?
?dsudsuds
  • They dont exist --
  • so I thought.
  • Why accelerate chunks?
  • Decay to neutral
  • Stranglet CMB
  • Testable show me the strangelet

11
Everything Else, (e. e.) Animal 2 Top Down Models
  • Cosmic strings, defects, etc.
  • Freedom to use fields unconstrained by particle
    physics
  • Put them all over, invisibly, and decay at any
    rate you want.
  • And any mass wanted

Bondi déjà vu all over again

12
Historical Fact
  • Heavy things can over-close the Universe
  • They ought to annihilate away
  • But s lt 1/M2, from unitarity.
  • Then if too heavy, they freeze out excess
    density. hence bounds lt TeV were long accepted
  • Herald Tribune
  • TOP DOWN MODELS GET SPECIAL VARIANCE

13
well-cited, incredibly incredibly detailed
  • If no particle physics in final decay products,
    then nothing to do
  • If particle physics in decay products, then
  • ???????????g/P gtgt1, which was not planned
  • Angular auto-correlations, correlations with
    AGN?
  • A neutrino source?

14
My RuleIf it cant be ruled out,its not
Science
  • Top-Down people need
  • to develop ways to rule out their own models
    model independently

15
e.e. topic 3 Z-bursts
  • Annihilate to Z0

n n n
n
n
n
n n
n
n
v
n
n
50/cm3
Weiler Fargione
16
Z0 exists !
  • mn????eV will suffice.
  • MZ2 2 mn? En?
  • En?????????????eV /(mn????? eV)
  • Many gs a prediction
  • Resonance tall but narrow,
  • overall rate low
  • Fix with flux
  • Needs about 1000-100000 more neutrinos than
    conventional in flux, in target clustering, or
    both.

17
I personally think theflux calculations are not
a basis of decision.( P(correct social
accepted ) is not one of my terms. )Plus,
neutrinosCANcluster
18
Z-burstseem to be a good model,just lacking
asecond testable signal
19
e.e. topic 3 black holes
?
  • s? p rs2 is conventional
  • rs Schwartzchild radius for M2 s
    . cm energy2
  • much work remains to be done

BH
Extra dims, Mgt TeV
20
a healthybusiness in setting limits
  • But read Voloshin. The quantum amplitude
  • to form a coherent black hole cannot possibly be
    as big as the classical calculations imposing
    coherence.

21
e. e. animal Lorentz Violation
  • Fast free charge makes Cherenkov radiation
  • in vacuum, vgtcm

22
.and fast gs spontaneously convert to pairs
?????????? ?????????????
tMIN
23
Early excitement
  • ...continued excitement
  • maybe somebody knows what else there is to do
  • and not-so-much crisp predictability for the
    GZK problem, e.g. angular stuff

24
Magnetic Monopoles
  • Everyones favorite particle
  • .eg/hc nh/2, mod t
  • Strongly interacting
  • Strongly steered and accelerated
  • Mass unknown, large
  • unseen

25
e.e. M. M. ?
  • Bremsstrahlung losses small, heavy
  • Observable large signal, AMANDA, RICE (in
    progress)
  • Progressive

Wick, Weiler, Biermann
26
e.e. Neutrinos ? Already did that. How to
MEASURE them?
27
RICE
????????? Cherenkov Experiment
Kansas University, Bartol Research
Institute, University of Canturbury, Christchurch
NZ, MIT
??3
???
28
RICE background sheet
  • Cold ice is 1 km transparent to radio waves
  • There is plenty of ice at South Pole
  • n -gt e shower makes lots of radio
  • E field \sim energy, power \sim energy2
  • Best method known, E gt PeV
  • Not just planned, running

29
Coherent Cherenkov Radiation
????
ANTENNAS! 200 MHz
ICE
?????
??
Method is a new technology, very well suited
to EgtgtPeV
??????
30
(No Transcript)
31
Beautifully REDUNDANTdetection scheme
  • Each event detected by 4, 5, 6 antennas
  • 4 suffice to get vertex in 3 DIMS !
  • OVERdetermined events are real events
  • ALSO fit Cherenkov cone SEPARATELY

32
and we are using matched filter correlations of
our own
  • imaginary parts (blue) and real part (red) of
    antenna impedance

33
RICE...Limits
  • ???? Limit

?????????
34
And Now, for something really different
35
Photon torpedoes
36
Exercise solved
Bessels equation !
37
What this thing is.
  • In other words,
  • THESE ARE THE FIELDS of a UNIFORMLY MOVING CHARGE
  • Cherenkov radiation,
  • boosted back into the frame vlt c
  • Improper boost turns J0 into K0 Bessel
  • Very weird and singular as xT -gt0

38
What LPM Forgot
Q
E
Actually, Ter-Mikaelian did not forget e??, but
used the atomic physics regime e?? 1 - wp2/w2.

We need sTOT (g p) at UHE
39
e. e. LPM?
P
  • Literature of Landau, Pomeranchuk, Migdal
  • Concept of coherence length.

R1
R2
l v Dt
40
Coherenceadd in phase
41
What is not really explained
42
Coherence length
43
Result UHE bremss emissions are coherent over
many many interactions
  • even if you might think that the wavelength of a
    gamma ray is far too small for interference

44
Multiple scattering jitter during the
bremsstrahlung
45
Yielding a factor w1/2
46
???? changes thespectrum to a new power
47
Radiative vs direct losses
  • Radiative losses bremsstrahlung, need an
    acceleration.
  • LPM damps them.
  • Direct losses exist at constant velocity. LPM
    overlooked.
  • Direct losses gt gt radiative losses
  • LPM quenched

..WE claim
48
LPM in AIRES code for air showers
Everyone accepts LPMsomeone ought to check it
out
  • Cillis et al (AIRES) PRD 1999

49
There is anerror inhigh energyelectromagnetic
showercodes
50
Size of effect depends on sTOT(gA)for
E????????????
sTOT Donnachi Landshoff
51
While still in progress, weve wondered about
AGASAshower evolution and energy calibration
  • Hadronic photoproduction produces larger
    transverse momenta than usually considered, a
    pause for doubt on their calibration method

52
Lets not complain about AGASA,lets find
somethingto do!
53
Does fixing a mistake in relativistic
electrodynamicsdone for 50 years countas new
physics?
  • yes

54
Energy, SchmenergyAre there angular
correlations?
???????????????????????
55
Its the ??????? variable!
56
GZK and UHE Neutrinos have room for new physics,
one way or the other
The tremendous scope of the problem of the
highest energy cosmic rays has hardly been
appreciated.
57
e.e. GRB Connection, do we really need a model?
HETE
58
(No Transcript)
59
GRB seen in downtown Tokyo
60
CAN YOU IMAGINEthe excitement of GRB
Razzaque, Meszaros, Waxman astro-ph 2003
61
g-normalized Flux
  • Kalashev, Kuzmin, Semikoz, Sigl
  • PRD 2002

62
Exercise
63
So what is RELIABLY known about n flux?
  • upper limits
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