

The Radio Ice Cerenkov Experiment (RICE) is an astrophysics
neutrino experiment, co-deployed with AMANDA, and based at
the South Pole. The experiment uses an array of 16 radio
receivers, deployed at depths up to 200 m., to detect
showers in the ice initiated by electron neutrinos. We
summarize the deployments to date, over the last 3 austral
summers, and testing and calibration of the transmitters and
receivers used in the experiment, both on-site and at the
home institutions.
[B16.002] STATUS OF THE RICE EXPERIMENT - ANALYSIS AND RESULTS
Dave Schmitz (U. of Kansas), RICE Collaboration
The Radio Ice Cerenkov Experiment (RICE) is an astrophysics
neutrino experiment, co-deployed with AMANDA, and based at
the South Pole. The experiment uses an array of 16 radio
receivers, deployed at depths up to 200 m., to detect
showers in the ice initiated by electron neutrinos. We
discuss analysis of the 1999 data, including an estimated
upper limit on the neutrino flux above 1 PeV from that
dataset.
[B16.003] New Population of Unidentified High Energy Gamma Ray Sources
Neil Gehrels (NASA's Goddard Space Flight Center), Daryl Macomb (Universities Space Research Association), David Bertsch, David Thompson, Robert Hartman (NASA's Goddard Space Flight Center)
One of the great mysteries of the high energy gamma-ray sky
is the existence of a large number of unidentified point
sources. They account for more than half of the sources
detected by the EGRET instrument on CGRO, numbering 171 out
of 270 total sources in the recent 3rd EGRET catalog. No
clear counterparts have been found at other wavelengths
despite 20 years of effort. In this presentation, we will
show evidence for a new population of these sources in the
3rd EGRET catalog. A cluster of ~20 faint sources appears
concentrated near the galactic center, extending to ~30š
galactic latitude and with more sources toward positive
latitudes than negative. They are part of a broader class of
faint sources sprinkled around the sky at mid-latitudes.
Several tests show that they are real point sources and that
they are distinct from the population of bright unidentified
sources that lie along the galactic plane. Candidates for
the counterparts include massive stars (gamma rays generated
in the stellar wind), radio quiet gamma-ray pulsars and jets
from accreting black holes.
[B16.004] Rapid Variability of TeV Blazars
Michael Catanese (Harvard-Smithsonian Center for Astrophysics)
Observations of blazars have revealed hour-scale or shorter
flux variations on several occasions, from radio to
gamma-ray wavelengths. These very fast flares provide a
means of investigating the flaring mechanisms and
acceleration processes in these objects and, when observed
simultaneously at several wavelengths, provide a means of
investigating the environment of the blazar jet and the
mechanism which produces the gamma-ray emission. In this
talk, I will review recent observations of hour-scale
variability at X-ray and TeV energies from the TeV-emitting
blazars, Markarian 421 and Markarian 501, and discuss what
we have learned about these objects from these observations.
[B16.005] Extragalactic Background Light and \gamma-ray observations of AGN.
Vladimir Vassiliev (Whipple Observatory, Harvard-Smithsonian CfA, P.O. Box 97, Amado, AZ 85645, USA)
The spectral density of the Extragalactic Background Light
(EBL) (0.1-100 \mum) contains extensive information on
the early history of the Universe: cosmology, galaxy and
star formation, metal and dust production, and the rate of
re-processing of starlight to infrared wavelengths by the
dust. In spite of great interest, EBL has so far escaped
direct detection due to strong backgrounds from
interplanetary dust scattering and emission, stars and
galactic foregrounds, and interstellar dust emission. In the
late sixties Gould and Schréder pointed out that
observations of extragalactic photons in the region 0.1 to
100 TeV can be used for indirect detection of EBL because
the two photons are coupled via pair production. Recent
detections of AGN which indeed emit such energetic photons
provide the data necessary to utilize this technique. We
will review recent experimental results and uncertainties
associated with theoretical predictions of EBL as well as
the contribution and potential of the ground based
\gamma-ray observatories, such as Whipple and VERITAS, to
measure the EBL field.
[B16.006] Fast Timing Bi-Directional CCD for Use in Gamma-Ray Astronomy
P.P. Altice, M.L. Cherry, T.G. Guzik, S.C. Kappadath (LSU), J.G. Stacy (LSU, Southern U.)
A CCD coupled with a pixellated inorganic scintillator (such
as segmented CsI) can provide high position resolution
(\sim300 \mum). However, standard CCDs are integrating
devices typically operating no faster than video rates. For
a balloon-borne \gamma-ray telescope capable of measuring
the energy of individual photons, the CCD must have a time
resolution better than the average time interval between
cosmic ray hits on the veto shield (\sim10 kHz). A Fast
Timing Bi-Directional CCD has better than 10 \mus time
resolution and 50 \mum position resolution. We describe
the CCD readout architecture, the ASIC readout design, the
present status of the development, and the application to a
\gamma-ray astronomy telescope suitable for a 100-day
Ultra Long Duration Balloon mission.
[B16.007] High x-ray yields in CO2 laser driven relativistic Thomson scattering
Igor Pogorelsky, Ilan Ben-Zvi (BNL), Tachishige Hirose (Tokyo Metropolitan University), Shigeru Kashiwagi (Waseda University (Japan)), Vitali Yakimenko, Karl Kusche, Peter Siddons (BNL), Tsunehiko Omori (KEK (Japan)), JLC polarized positron source US-Japan Collaboration
We report results of the first stage proof-of-principle
demonstration of the ultra-high intensity laser synchrotron
source (LSS) that combines a photocathode RF linac and a
picosecond CO2 laser. Selection of such components is based
on a systematic approach to optimize the LSS towards the
maximum photon yield. Simultaneously, this approach opens a
prospect to ultra-high peak intensity femtosecond x-ray and
gamma sources. The 600 MW CO2 laser interacted in a head-on
collision with the 60 MeV, 140 A, 3.5 ps electron beam. Both
beams were focused to the r(rms)=32 um spot. 6.4*10^6 of the
1.8-2.3 Å x-ray photons per 3.5 ps pulse are detected in
agreement with simulations that model the experimental
conditions. Our next plan is to demonstrate 10^10 x-ray
photons per pulse using a CO2 laser of the ~1 TW peak power.
The next stage of the ATF LSS experiment will also open an
opportunity for detailed study of Thomson harmonics
generated on relativistic electron beams at the normalized
laser strength of a~1.
[B16.008] Inherently Bursting Accretion
B. Coppi (MIT), P.S. Coppi (Yale University)
Magnetized accretion disks are shown to be subject to collective processes, that can induce the needed outward transport of angular momentum, whose growth rates, as in the case of laboratory plasmas depend on the finiteness of the plasma temperature(B. Coppi and P.S. Coppi, \itPhys. Lett. A)239\rm, 261 (1998) and on the gradient of the rotation frequency(E. Velikhov, \itSoviet Phys.) JETP36\rm, 1938 (1959); S.A. Balbus and J.F. Hawley, \itAp. J. \bf376\rm, 214 (1991) combined. Therefore accretion is envisioned to occur as a sequence of two stages: i) a preheating phase of accumulated plasmas at the outer edge of the disk and ii) a rapid infalling phase following the excitation of the relevant modes. The proposed scenario is similar to that of the so called ``monster sawtooth oscillations'' occuring in magnetically confined laboratory plasmas where the central temperature is observed to rise, as a result of the injection of a high energy particle population and then to crash periodically. The crash leads to a spatial redistribution of the thermal energy and is caused by the excitation of internal modes driven by the plasma pressure gradient when this is raised above a characteristic threshold by the energy transferred from the injected particles to the thermal plasma.
Sponsored in part by the U.S. Department of Energy
[B16.009] Flash Heating of Circumstellar Clouds by Gamma-Ray Bursts
Charles Dermer (Naval Research Laboratory), Markus Boettcher (Rice University)
The identification of flaring and fading X-ray, optical and
radio counterparts to gamma-ray burst (GRB) sources, and the
large energy releases implied by redshift measurements, find
a consistent explanation in an expanding relativistic
blast-wave model. This model has been called into question
by observations of spectra from GRBs that are harder than
can be produced through the synchrotron process. If GRBs
originate from the collapse of massive stars, then
circumstellar clouds near burst sources will be illuminated
by intense gamma radiation, and the electrons in these
clouds will be rapidly scattered to energies as large as
several hundred keV. Low-energy photons that subsequently
pass through the hot plasma will be scattered to higher
energies, and this effect resolves the line-of-death
objection to the synchrotron shock model. Illuminated clouds
near GRBs will form relativistic plasmas containing large
numbers of electron-positron pairs that can be detected
within ~ 1-2 days of the explosion before expanding and
dissipating. Localized regions of pair annihilation
radiation in the Galaxy would reveal past GRB explosions.
[B16.010] The Rapid Gamma-ray Burst Response Campaign with ROTSE
R. Balsano, J. Bloch, D. Casperson, S. Fletcher, G. Gisler, J. Hills, W. Priedhorsky, J. Szymanski, J. Wren (Los Alamos National Laboratory), C. Akerlof, R. Kehoe, T. McKay, A. Pawl (University of Michigan), S. Marshall (Lawrence Livermore National Laboratory), B. Lee (Fermi National Accelerator Laboratory, University of Michigan), S. Barthelmy, P. Butterworth, T. Cline (NASA/Goddard Space Flight Center)
The main goal of the Robotic Optical Transient Search Experiment (ROTSE) is to detect optical emission from Gamma-ray Bursts (GRBs) during and immediately following GRBs. The instruments comprising ROTSE consist of wide-field optics on rapidly slewing mounts optimized for quick response to GRBs localized to several degree regions. Thus far, only one prompt optical counterpart to a GRB has been discovered although simple scaling arguments suggest more should be easily detected. This talk will cover ROTSE responses to GRBs detected by the Burst and Transient Source Experiment and the soon-to-be-launched High Energy Transient Experiment. The expansion of ROTSE to a global network of identical telescopes will also be briefly discussed.
[B16.011] Search for a TeV Component of GRBs Using the Milagrito Detector
Isabel Leonor (University of California at Irvine), Milagro Collaboration
Observing gamma-ray bursts (GRBs) in the TeV energy range
can be extremely valuable in providing insight into GRB
radiation mechanisms and in constraining source distances.
The Milagrito detector was an air shower array which used
the water Cherenkov technique to search for TeV sources.
Unlike other detectors which have attempted to search for
GRBs at TeV energies, Milagrito combined the characteristics
of a low energy threshold, a large field of view, and a high
duty cycle, making it a practical instrument for detecting
gammay ray events which lasted but fleetingly and which were
unpredictable in both time and position of occurrence. Data
from this detector was analyzed to look for TeV emission
from 54 BATSE GRBs which were in the field of view of the
Milagrito detector during its lifetime (January 1997 to May
1998). Results from this analysis, including evidence for
TeV emission from GRB 970417a, will be presented.
[B16.012] Considerations for a Next Generation GRB Observatory
Gerald J. Fishman (NASA-MSFC)
A framework will be described for the planning of a Next
Generation Burst Observatory. This Observatory, using Swift
as a pathfinder mission, would study early star formation
and early galaxy formation at very high redshifts through
observations of thousands of GRBs, their afterglows and
environments. It is suggested that the international GRB
community should begin some initial studies for such an
observatory.
[B16.013] Gamma-Ray Bursts Cannot Produce the Observed Cosmic Rays above ~10 EeV
F.W. Stecker, Sean Scully (NASA Goddard Space Flight Center)
It has been suggested that cosmological \gamma-ray bursts
can produce the observed flux of cosmic rays at the highest
energies. However, recent observations indicate that the
redshift distribution of \gamma-ray bursts most likely
follows the redshift distribution of the average star
formation rate in the universe, a rate which was much higher
at redshifts between 1.5 and 2 than it is today. We show
that as a consequence, energy losses suffered by ultrahigh
energy cosmic rays caused by meson-producing interactions
with photons of the big-bang relic background radiation
would have a profound effect on both the flux and energy
spectrum of these cosmic rays which would be observed at
Earth during the present epoch. The cosmic rays with
energies above 10 EeV from \gamma-ray bursts which we
predict would have a much lower flux than that observed and
would have a sharp cutoff in their spectrum at an energies
above \sim 30 EeV, an order of magnitude lower in energy
than the highest energy cosmic ray event reported by the
Fly's Eye detector array.
[B16.014]
This abstract not available.