Cosmic Ray and Neutrino Astrophysics

The last two subjects I want to briefly cover  are  also usually classified as high-energy astrophysics, and that is cosmic ray and neutrino astrophysics. First, cosmic rays (liberally borrowed from this site):

"Cosmic rays are high energy charged particles, originating in outer space, that travel at nearly the speed of light and strike the Earth from all directions. Most cosmic rays are the nuclei of atoms, ranging from the lightest to the heaviest elements in the periodic table. Cosmic rays also include high energy electrons, positrons, and other subatomic particles. The term "cosmic rays" usually refers to galactic cosmic rays, which originate in sources outside the solar system, distributed throughout our Milky Way galaxy. However, this term has also come to include other classes of energetic particles in space, including nuclei and electrons accelerated in association with energetic events on the Sun (called solar energetic particles), and particles accelerated in interplanetary space."

Discovery and Early Research: Cosmic rays were discovered in 1912 by Victor Hess, when he found that an electroscope discharged more rapidly as he ascended in a balloon. He attributed this to a source of radiation entering the atmosphere from above, and in 1936 was awarded the Nobel prize for his discovery.

For some time it was believed that the radiation was electromagnetic in nature (hence the name cosmic "rays"), and some textbooks still incorrectly include cosmic rays as part of the electromagnetic spectrum. However, during the 1930's it was found that cosmic rays must be electrically charged because they are affected by the Earth's magnetic field.

From the 1930s to the 1950s, before man-made particle accelerators reached very high energies, cosmic rays served as a source of particles for high energy physics investigations, and led to the discovery of subatomic particles that included the positron and muon. Although these applications continue, since the dawn of the space age the main focus of cosmic ray research has been directed towards astrophysical investigations of where cosmic rays originate, how they get accelerated to such high velocities, what role they play in the dynamics of the Galaxy, and what their composition tells us about matter from outside the solar system. To measure cosmic rays directly, before they have been slowed down and broken up by the atmosphere, research is carried out by instruments carried on spacecraft and high altitude balloons, using particle detectors similar to those used in nuclear and high energy physics experiments.


Cosmic Ray Energies and Acceleration: The energy of cosmic rays is usually measured in units of MeV, for mega-electron volts, or GeV, for giga-electron volts. (One electron volt is the energy gained when an electron is accelerated through a potential difference of 1 volt). Most galactic cosmic rays have energies between 100 MeV (corresponding to a velocity for protons of 43% of the speed of light) and 10 GeV (corresponding to 99.6% of the speed of light). The number of cosmic rays with energies beyond 1 GeV decreases by about a factor of 50 for every factor of 10 increase in energy. Over a wide energy range the number of particles per m2 per steradian per second with energy greater than E (measured in GeV) is given approximately by N(>E) = k(E + 1)-a, where k ~ 5000 per m2 per steradian per second and a ~1.6. The highest energy cosmic rays measured to date have had more than 1020 eV, equivalent to the kinetic energy of a baseball traveling at approximately 100 mph!

It is believed that most galactic cosmic rays derive their energy from supernova explosions, which occur approximately once every 50 years in our Galaxy. To maintain the observed intensity of cosmic rays over millions of years requires that a few percent of the more than 1051 ergs released in a typical supernova explosion be converted to cosmic rays. There is considerable evidence that cosmic rays are accelerated as the shock waves from these explosions travel through the surrounding interstellar gas. The energy contributed to the Galaxy by cosmic rays (about 1 eV per cm3) is about equal to that contained in galactic magnetic fields, and in the thermal energy of the gas that pervades the space between the stars.

Acceleration mechanisms:

Cosmic Ray Composition: Cosmic rays include essentially all of the elements in the periodic table; about 89% of the nuclei are hydrogen (protons), 10% helium, and about 1% heavier elements. The common heavier elements (such as carbon, oxygen, magnesium, silicon, and iron) are present in about the same relative abundances as in the solar system, but there are important differences in elemental and isotopic composition that provide information on the origin and history of galactic cosmic rays. For example there is a significant overabundance of the rare elements Li, Be, and B produced when heavier cosmic rays such as carbon, nitrogen, and oxygen fragment into lighter nuclei during collisions with the interstellar gas. The isotope 22Ne is also overabundant, showing that the nucleosynthesis of cosmic rays and solar system material have differed. Electrons constitute about 1% of galactic cosmic rays. It is not known why electrons are apparently less efficiently accelerated than nuclei.



Cosmic Rays in the Galaxy: Because cosmic rays are electrically charged they are deflected by magnetic fields, and their directions have been randomized, making it impossible to tell where they originated. However, cosmic rays in other regions of the Galaxy can be traced by the electromagnetic radiation they produce. Supernova remnants such as the Crab Nebula are known to be a source of cosmic rays from the radio synchrotron radiation emitted by cosmic ray electrons spiraling in the magnetic fields of the remnant. In addition, observations of high energy (10 MeV - 1000 MeV) gamma rays resulting from cosmic ray collisions with interstellar gas show that most cosmic rays are confined to the disk of the Galaxy, presumably by its (micro-Gauss) magnetic field. Similar collisions of cosmic ray nuclei produce lighter nuclear fragments, including radioactive isotopes such as 10Be, which has a half-life of 1.6 million years. The measured amount of 10Be in cosmic rays implies that, on average, cosmic rays spend about 10 million years in the Galaxy before escaping into inter-galactic space.


Very High Energy Cosmic Rays: When high energy cosmic rays undergo collisions with atoms of the upper atmosphere, they produce a cascade of "secondary" particles that shower down through the atmosphere to the Earth's surface. Secondary cosmic rays include pions (which quickly decay to produce muons, neutrinos and gamma rays), as well as electrons and positrons produced by muon decay and gamma ray interactions with atmospheric atoms. The number of particles reaching the Earth's surface is related to the energy of the cosmic ray that struck the upper atmosphere. Cosmic rays with energies beyond 1014 eV are studied with large "air shower" arrays of detectors distributed over many square kilometers that sample the particles produced. The frequency of air showers ranges from about 100 per m2 per year for energies >1015 eV to only about 1 per km2 per century for energies beyond 1020 eV. Cosmic ray interaction products such as neutrinos are also studied by large detectors placed deep in underground mines or under water.



Most secondary cosmic rays reaching the Earth's surface are muons, with an average intensity of about 100 per m2 per second. Although thousands of cosmic rays pass through our bodies every minute, the resulting radiation levels are relatively low, corresponding, at sea level, to only a few percent of the natural background radiation. However, the greater intensity of cosmic rays in outer space is a potential radiation hazard for astronauts, especially when the Sun is active, and interplanetary space may suddenly be filled with solar energetic particles. Cosmic rays are also a hazard to electronic instrumentation in space; impacts of heavily-ionizing cosmic ray nuclei can cause computer memory bits to "flip" or small microcircuits to fail.

One big goal of future missions (e.g., Pamela) is to find anti-matter CRs which could be produced using rather exotic means:


Detection systems: These share a lot with EGRET/GLAST type gamma-ray detectors.



Neutrino Astrophysics

Why high-energy neutrino astronomy?

The reason for high-energy neutrino astronomy is to open up all wavelengths for astronomy and to peer into sources that would be opaque to photons and protons.

At high energies photons (gamma-rays) and protons are not viable probes.

With a high-energy neutrino detector we can open up a new window on the Universe. New windows have usually meant new discoveries.

The fundamental scientific motivation for high-energy neutrino astronomy is that of transparency, as compared to photons and CRs:


Thus neutrinos will allow us to observe what we cannot with other detectors. In particular we will be able to observe sources at cosmological distances. This includes both diffuse and nearly point-like sources. Based upon the GRO (Compton Gamma-Ray Observatory) full sky survey one would anticipate that there are of the order of one hundred ultra-high-energy particle sources, probably Active Galaxies that should be detectable with a sufficiently large detector. It is also quite likely that Gamma-Ray Bursters (GRBs) are sources of high-energy neutrinos. There is roughly one GRB per day detectable by GRO type instruments. (Over 1000 observed todate.)

A measurement of the flux, energy spectrum, angular distribution, and timing of high-energy neutrinos is a fundamental observation of the Universe.

Estimated fluxes:


Potential sources:

AGN: Active Galactic Nuclei (AGN) is one of the possible, and likely, acceleration sites to produce EHE cosmic rays, and the accelerated proton energy loss due to proton-proton and/or proton-gamma interactions in the AGN accretion disk or with UV photons in the associated jets are dominant mechanism for neutrino (and photon) production.

GRBs:  GRBs are expected to produce significant fluxes of neutrinos from the approximately 100 MeV thermal spectrum and from accelerated protons producing pions by photoproduction on the radiations fields present. These radiation fields include, the thermal radiation, synchrotron radiation for accelerated electrons, Compton-up-converted versions of these original fields.



Diffuse sources:

CR-CMB: EHE neutrinos above 1019 eV are produced by photopion production of the 2.7 K cosmic background radiation photons and the ultra-high energy cosmic ray nucleons during propagation in intergalactic space.

Annihilation or collapse of topological defects (TDs): Decay of topological defects such as monopoles, cosmic strings would release their trapped energy in the form of supermassive gauge bosons and Higgs bosons. Further decay of these "X-particles" can give rise into quarks, gluons, leptons, etc., which materialize into EHE nucleons, photons, and neutrinos with energies up to the GUT scale (1014 - 1016 GeV = 1023 - 1025 eV). The figure, below, shows the fluxes of the cosmic neutrinos produced by this mechanism. Neutrinos resulting from such decays reach energies of the grand unification (GUT) scale, and collisions of superhigh energy neutrinos with the cosmic background neutrinos initiate neutrino cascading which enhances the EHE neutrino flux at Earth.

Detection Schemes

Once upon a time, chemical detectors were used (Homestake goldmine, etc.):

But those were too difficult. Nowadays it is the detection of the interaction and interaction products. When a neutrino interacts with a proton or neutron (or an electron) it will produce a cascade of particles. This cascade of particles will generally build up to a substantial number of particles and then die out on the scale of 10 meters. If it is a charged-current reaction,


These particles and particle cascades, when in water (or ice), will produce a lot of light primarily through the Cerenkov effect. This Cherenkov light comes out as a cone-shaped shock wave at about 40-degrees from the particles' trajectory.

The detector concept is an array of optical modules (OMs) which detects the time of arrival (to roughly one nanosecond) and intensity of the Cherenkov light. By comparing the arrival timing and intensity of this light one can attempt to reconstruct the event geometry and energy deposition. Amanda:

IceCube is the follow-on experiment:


(80 strings of 60 detectors each)

Super-Kamiokande is another effort:

Large PMTs:

The detection of something (besides the Sun!), SN1987A:

You can even look at the "spectrum" (19 events!):