Title: GZK III: A Visit to the Zoo
1GZK III A Visit to the Zoo
- How I protect my independence from various
proposals
2recall
- 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)
3The Physicists Gambit
- P(new physics GZK)
- P(GZK new physics) P(new physics)
-
P(GZK)
?????
????????
4What 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?
5If you Are in Physics, You Already Paid the
Priceof Assuming New Physics Could Be
Found.P(new) finite.Right?
6??????????
?
7try to get morethings explainedthanthe number
of newassumptionsyou made
8Nuclei
ANIMAL 1
Stecker
9Nuclei
- 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?
10Strangelets?
?dsudsuds
- They dont exist --
- so I thought.
- Why accelerate chunks?
- Decay to neutral
- Stranglet CMB
- Testable show me the strangelet
11Everything 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
12Historical 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
13well-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?
14My RuleIf it cant be ruled out,its not
Science
- Top-Down people need
- to develop ways to rule out their own models
model independently
15e.e. topic 3 Z-bursts
n n n
n
n
n
n n
n
n
v
n
n
50/cm3
Weiler Fargione
16Z0 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.
17I personally think theflux calculations are not
a basis of decision.( P(correct social
accepted ) is not one of my terms. )Plus,
neutrinosCANcluster
18Z-burstseem to be a good model,just lacking
asecond testable signal
19e.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
20a 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.
21e. e. animal Lorentz Violation
- Fast free charge makes Cherenkov radiation
- in vacuum, vgtcm
22.and fast gs spontaneously convert to pairs
?????????? ?????????????
tMIN
23Early 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
24Magnetic Monopoles
- Everyones favorite particle
- .eg/hc nh/2, mod t
- Strongly interacting
- Strongly steered and accelerated
- Mass unknown, large
- unseen
25e.e. M. M. ?
- Bremsstrahlung losses small, heavy
- Observable large signal, AMANDA, RICE (in
progress) - Progressive
Wick, Weiler, Biermann
26e.e. Neutrinos ? Already did that. How to
MEASURE them?
27RICE
????????? Cherenkov Experiment
Kansas University, Bartol Research
Institute, University of Canturbury, Christchurch
NZ, MIT
??3
???
28RICE 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
29Coherent Cherenkov Radiation
????
ANTENNAS! 200 MHz
ICE
?????
??
Method is a new technology, very well suited
to EgtgtPeV
??????
30(No Transcript)
31Beautifully 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
32and we are using matched filter correlations of
our own
- imaginary parts (blue) and real part (red) of
antenna impedance
33RICE...Limits
?????????
34And Now, for something really different
35Photon torpedoes
36Exercise solved
Bessels equation !
37What 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
-
38What 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
40Coherenceadd in phase
41What is not really explained
42Coherence length
43Result 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
44Multiple scattering jitter during the
bremsstrahlung
45Yielding a factor w1/2
46???? changes thespectrum to a new power
47Radiative 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
..WE claim
48LPM in AIRES code for air showers
Everyone accepts LPMsomeone ought to check it
out
- Cillis et al (AIRES) PRD 1999
49There is anerror inhigh energyelectromagnetic
showercodes
50Size of effect depends on sTOT(gA)for
E????????????
sTOT Donnachi Landshoff
51While 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
52Lets not complain about AGASA,lets find
somethingto do!
53Does fixing a mistake in relativistic
electrodynamicsdone for 50 years countas new
physics?
54Energy, SchmenergyAre there angular
correlations?
???????????????????????
55Its the ??????? variable!
56GZK 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.
57e.e. GRB Connection, do we really need a model?
HETE
58(No Transcript)
59GRB seen in downtown Tokyo
60CAN YOU IMAGINEthe excitement of GRB
Razzaque, Meszaros, Waxman astro-ph 2003
61 g-normalized Flux
- Kalashev, Kuzmin, Semikoz, Sigl
- PRD 2002
62Exercise
63So what is RELIABLY known about n flux?