|
The MAGIC telescope has been built with the
clear goal to lower the energy threshold for gamma rays.
For many unanswered physics questions,
a low energy threshold holds the key.
As the MAGIC telescope reaches its design performance,
it is likely that, beyond the physics that has been predicted,
new avenues will open.
The general argument is the absolute necessity to explore the electromagnetic
spectrum at all wavelengths, and the absence, at the present time, of
any instrument exploring the energy region between some tens of GeV and several
hundred GeV with adequate sensitivity. At lower energies,
satellite experiments, in particular EGRET, have contributed
substantial knowledge. Their energy range and sensitivity will be
much improved by the EGRET successor, GLAST,
(launch foreseen in 2007), but even that will have the limit of detector size,
and will have to be supplemented by complementary terrestrial observations.
Pre-MAGIC gamma-ray telescopes, on the other hand, have typically an energy
threshold of several hundred GeV.
The Gamma Ray Horizon is commonly defined as that energy for
each redshift, for which the
photon flux is reduced by a factor of e. Gamma rays from
distant sources interact in the
intergalactic space with infrared
photons and other low-energy photon fields,
and are substantially attenuated.
Observations at lower energy threshold give access to
gamma-ray sources with higher redshifts,
hence a larger sensitivity for tests of light propagation effects.
Cosmology provides strong arguments for some 25% of the energy in the
Universe to be in the form of Dark Matter; most of it should be 'cold',
non-baryonic, and weakly interacting, Weakly Interacting Massive
Particles or WIMPs. The Standard Model of Particle Physics has
no candidate for WIMPs, and the nature of Dark Matter
can only be explained by going beyond the Standard Model.
Supersymmetry assumes symmetry between the fermionic
and bosonic degrees of freedom, and thus provides a quite natural
candidate for the WIMP, the neutralino.
The neutralino could be the Lightest Supersymmetric Particle
and should, therefore, be stable. Neutralinos might be
indirectly detected by their annihilation through different
channels, producing high energy gammas; in particular, gamma/gamma or p
Z/gamma pairs provide ideal observational results (monochromatic annihilation lines).
Another possible reaction is through hadronic jets producing several gammas;
in this reaction, neutralinos could be observed as
an energy distribution in gammas different from the power laws
characteristic for the cosmic acceleration mechanisms.
In any case, lowering the gamma energy threshold to
identify the continuum signature extends the sensitivity to
many competing theoretical neutralino production models.
Models of Quantum Gravity naturally contain quantum fluctuations of
the gravitational vacuum, and lead to predictions of an
energy-dependent velocity for electromagnetic
waves. In other words, gammas of different energy produced simultaneously in an
extragalactic object, arrive on Earth at different times due to their propagation through
the gravitational vacuum.
Gamma telescopes could be suitable instruments.
Their figure of merit, in order to be sensitive to such an effect, is to
provide sensitivity to large expected time delays between gammas
in a wide range of energies.
Also, any time delay effect must be studied over a wide range
of redshifts, in order to disentangle any Quantum Gravity effect from
source-dependent time delay emission effects.
For this reason, a large number of
sources at different redshifts and different characteristics must be
detected and measured
with precision. A low-energy threshold and high-sensitivity detector
has clear advantages.
Nearly 3000 Gamma Ray Bursts (GRBs) have been observed by BATSE, but
the phenomena at their origin are not fully understood.
GRBs seen in the gamma ray domain last between a
fractions of a second and minutes; the X-ray emission
typically runs on a scale of days, and the optical one
even on a scale of weeks.
Multiwavelength observations of GRBs have been made made possible by fast
distribution of the information coming mainly from satellites, in real time.
Some BATSE observations (less than a percent)
were complemented by EGRET, at ~1 GeV of energy;
however, both the field of view (FOV) and
the sensitivity of EGRET sets severe limits. Encouraging is the fact that
two of the EGRET-detected GRBs (GRB930131 and GRB940217)
lasted longer inside the EGRET energy window than the observation in BATSE, so that
an afterglow at higher energies can not be excluded, at least for some GRBs. The
existence of exceptionally long GRBs, with the gamma ray emission lasting
clearly longer than emisssion in the hard X-ray range, is particularly challenging
for theoretical models, that have to deal with a continuous acceleration process
at a substantially higher energy than that of the prompt emission.
The successful
simultaneous observation of some GRBs at different wavelengths has
favored, at least for longer lasting bursts, among the existing theoretical
models that of a collapsing supermassive star. The emission mechanism, however,
is still under discussion. While the "fireball shock model" is commonly
accepted for the prompt emission, the origin of the longer-lived
afterglow is explained by various models,
differing substantially in their predictions for high-energy gamma emission.
Experimental data for higher-energy gamma-rays are not available;
MAGIC has been constructed (light weight = fast slewing) to provide
this information, for the moment a totally new territory.
Shell-type supernova remnants have long been suggested to be sites
for cosmic ray acceleration below 100~TeV,
mainly on the basis of general energetics
arguments. We know from their synchrotron,
radio and X-ray emission that electrons
are accelerated to TeV energies.
There is, however, no solid evidence for proton
acceleration. A possible signature of proton
acceleration would be the spectrum of
neutral pi decay from collisions
of cosmic ray protons and nearby matter
like high density molecular clouds. A number of shells have
been observed by EGRET at 0.1-10~GeV energies
and by gamma ray telescopes at TeV energies; the energy region in
between still has to be pinned down experimentally.
Also, the origin of this radiation
remains uncertain, due to the contamination
of gamma-rays produced by leptonic
processes (Bremsstrahlung or Inverse-Compton).
A low threshold and high sensitivity will allow spectral
studies in the range above 10 GeV, where the different
mechanisms are expected to show different
spectral shapes; it also will allow
to pin down the exact positions of possible
spectral cutoffs.
Plerions or Pulsar-Wind Nebulae are SNRs
in which a pulsar wind injects energy into
its surroundings. A bubble is inflated
out to a radius where it is confined by the
expanding shell, as already suggested for the Crab Nebula.
Particle acceleration is expected in the
wind termination shock.
A precise measurement
of the spectrum in the energy range below 100 GeV
is crucial to constrain the model parameters
and to ascertain if another source of photons
is necessary, possibly Bremsstrahlung
from dense regions of gas.
The observation of gamma-ray pulsars in the GeV domain is of special
interest: in this range, the EGRET pulsar spectra cut off due to
limited sensitivity; observations of the differential spectra of
gamma-ray pulsars in this energy domain
will give us clues about the different proposed models
( Galaxy formation and evolution in the early universe are among
the main open questions of extragalactic astronomy.
The conventional understanding is based on a co-evolution
of galaxies and super-massive black holes, which power the AGN phenomenon. Recent
observations, however, seem to challenge this understanding, by showing early star and
galaxy formation, compared to a later evolution of AGNs.
Gamma ray observations of AGNs at different redshifts (i.e.with
a low energy threshold) will
help in understanding the evolution
of AGNs and their central engines, super-massive black holes.
A low threshold will enable us to study the gamma ray emission
of a large population of AGNs, up to
redshifts above z~2, as the lower-energy gammas can reach us largely unabsorbed by
the meta-galactic radiation field.
The diffuse photon background may be classified according to its origin:
The Extragalactic Background Radiation (EBR) and the Diffuse Galactic Emission
(DGE). EBR is essentially isotropic, and is well established
up to energies of some 50 GeV. In the energy range
from 30 GeV to 100 TeV, a large part of the EBR may be due to the direct
emission from Active Galactic Nuclei, which have not yet been resolved.
Direct measurements of the DGE exist up to energies of ~70 GeV. The data
are explained by the interaction of cosmic-ray electrons and hadrons with
the interstellar radiation fields and with the interstellar matter.
The production mechanisms are synchrotron radiation
of electrons, high-energy
electron bremsstrahlung, inverse Compton scattering with low-energy photons,
and pi-0 production by nucleon-nucleon interactions. More recently,
measurements by INTEGRAL seem to show that rather than diffuse, galactic emission
is associated to multiple point sources.
New measurements of the gamma radiation (either diffuse or from point-like
or extended sources)
in the energy region below 300 GeV will help to better understand the
different sources of the diffuse gamma ray background :
this is an enormously rich field of activity for
detailed studies, possible with modest observation times on nearly
half of the observable EGRET sources.
their expected steep energy spectrum makes
observations at low
energy a particularly good argument, as they allow enough flux to be
detected in the gamma ray domain.
|
||||||||||||||||||
This page was created by Rudolf Bock. Last modification 20.07.2008 by Robert Wagner. The MAGIC Telescope web pages are hosted at MPI für Physik, Munich. Imprint | |||||||||||||||||||