This image is a composite of several types of radiation astronomy: radio, infrared, visual, ultraviolet, soft and hard X-ray. Credit: NASA.
 Completion status: this resource has reached a high level of completion.

Radiation astronomy is astronomy applied to the various extraterrestrial sources of radiation, especially at night. It is also conducted above the Earth's atmosphere and at locations away from the Earth, by satellites and space probes, as a part of explorational (or exploratory) radiation astronomy.

 Educational level: this is a secondary education resource.

Seeing the Sun and feeling the warmth of its rays is probably a student's first encounter with an astronomical radiation source. This will happen from a very early age, but a first understanding of the concepts of radiation may occur at a secondary educational level.

 Educational level: this is a tertiary (university) resource.

Radiation is all around us on top of the Earth's crust, regolith, and soil, where we live. The study of radiation, including radiation astronomy, usually intensifies at the university undergraduate level.

 Educational level: this is a research resource.

And, generally, radiation becomes hazardous, when a student embarks on graduate study.

 Resource type: this resource is an article.

Cautionary speculation may be introduced unexpectedly to stimulate the imagination and open a small crack in a few doors that may appear closed at present. As such, this learning resource is part lecture and part article as it incorporates some state-of-the-art results from the scholarly literature.

 Resource type: this resource contains a lecture or lecture notes.

The laboratories of radiation astronomy are limited to the radiation observatories themselves and the computers and other instruments (sometimes off site) used to analyse the results.

 Subject classification: this is an astronomy resource.

# Notation

Notation: let the symbol Def. indicate that a definition is following.

Notation: let the symbols between [ and ] be replacement for that portion of a quoted text.

# Universals

Radiation astronomy consists of three fundamental parts:

1. derivation of logical laws with respect to incoming radiation,
2. natural radiation sources outside the Earth, and
3. the sky and associated realms with respect to radiation.

To help with definitions, their meanings and intents, there is the learning resource theory of definition.

Def. a spontaneous emission of an α ray, β ray, or γ ray by the disintegration of an atomic nucleus is called radioactivity.[1]

# Astronomy

This ultraviolet-wavelength image mosaic, taken by NASA's GALEX, shows a comet-like "tail" stretching 13 light year across space. Credit: NASA.

A nomy (Latin nomia) is a "system of laws governing or [the] sum of knowledge regarding a (specified) field."[1] Nomology is the "science of physical and logical laws."[1] When any effort to acquire a system of laws or knowledge focusing on an astr, aster, or astro, that is, any natural body in the sky especially at night,[1] succeeds even in its smallest measurement, astronomy is the name of the result.

# Planetary science

This is a true-color image of Io taken by the Galileo probe. Credit: NASA.

"Planetary science ... is the scientific study of planets (including Earth), moons, and planetary systems, in particular those of the solar system and the processes that form them [using the radiation they emit, reflect, fluoresce, or absorb]. It studies objects ranging in size from micrometeoroids to gas giants, aiming to determine their composition, dynamics, formation, interrelations and history. It is a strongly interdisciplinary field, originally growing from astronomy and earth science,[2] but which now incorporates many disciplines, including planetary astronomy, planetary geology (together with geochemistry and geophysics), atmospheric science, oceanography, hydrology, theoretical planetary science, glaciology, and the study of extrasolar planets.[2]"[3]

# Theoretical astronomy

This image is a theory for the interior of the Sun. Credit: Pbroks13.

Theoretical astronomy at its simplest is the definition of terms to be applied to astronomical entities, sources, and objects.

Def. an "expanse of space that seems to be [overhead] like a dome"[1] is called a sky.

Computer simulations are usually used to represent astronomical phenomena.

Part of the fun of theory is extending the known to what may be known to see if knowing is really occurring, or is it something else.

The laboratories of astronomy are limited to the observatories themselves. The phenomena observed are located in the heavens, far beyond the reach, let alone control, of the astronomical observer.[4] “So how can one be sure that what one sees out there is subject to the same rules and disciplines of science that govern the local laboratory experiments of physics and chemistry?”[4] “The most incomprehensible thing about the universe is that it is comprehensible.” - Albert Einstein.[4]

# Source astronomy

Volcanic bombs are thrown into the sky and travel some distance before returning to the ground. This bomb is in the Craters of the Moon National Monument and Preserve, Idaho, USA. Credit: National Park Service.

In source astronomy, the question is "Where did it come from?"

Source astronomy has its origins in the actions of intelligent life on Earth when they noticed things or entities falling from above and became aware of the sky. Sometimes what they noticed is an acorn or walnut being dropped on them or thrown at them by a squirrel in a tree. Other events coupled with keen intellect allowed these life forms to deduce that some entities falling from the sky are coming down from locations higher than the tops of local trees.

Def. a source or apparent source detected or “created at or near the time of the [ event or] events” is called a primary source.

Direct observation and tracking of the origination and trajectories of falling entities such as volcanic bombs presented early intelligent life with vital albeit sometimes dangerous opportunities to compose the science that led to source astronomy.

# The Electron Volt

This is a unit that will be useful later.

The eV is the energy gained by an electron in passing through a potential difference of one volt. Since the charge on an electron is 1.60218 x 10-19 Coulombs, an eV is 1.60218 x 10-19 J. A keV is 1000 eV and a MeV is 1000 keV).

A photon with an energy of 1eV has a frequency of 1 eV/h = 2.41799 x 1014 Hz or about 242 THz and a wavelength of c.h/1 eV = 1.23984 x 10-6 m or about 1,240nm or 12,400Å. That would put the photon in the infrared range. In practice, photon energies are seldom stated for such long wavelengths.

A lead castle is built to shield a radioactive sample. Credit: Changlc.

“In physics, radiation is a process in which energetic particles or energetic waves travel through a medium or space.”[5]

Def. an action or process of throwing or sending out a traveling ray of energy in a line, beam, or stream of small cross section is called radiation.

Def. “[t]he shooting forth of anything from a point or surface, like the diverging rays of light; as, the radiation of heat”, from wiktionary radiation, is called radiation.

The term radiation is often used to refer to the ray itself.

“Different types of ionizing radiation behave in different ways, so different shielding techniques are used.

1. Particle radiation consists of a stream of charged or neutral particles, both charged ions and subatomic elementary particles. This includes solar wind, cosmic radiation, and neutron flux in nuclear reactors.
2. Alpha particles (helium nuclei) are the least penetrating. Even very energetic alpha particles can be stopped by a single sheet of paper.
3. Beta particles (electrons) are more penetrating, but still can be absorbed by a few millimeters of aluminum. However, in cases where high energy beta particles are emitted shielding must be accomplished with low density materials, e.g. plastic, wood, water or acrylic glass (Plexiglas, Lucite). This is to reduce generation of Bremsstrahlung X-rays. In the case of beta+ radiation (positrons), the gamma radiation from the electron-positron annihilation reaction poses additional concern.
4. Neutron radiation is not as readily absorbed as charged particle radiation, which makes this type highly penetrating. Neutrons are absorbed by nuclei of atoms in a nuclear reaction. This most-often creates a secondary radiation hazard, as the absorbing nuclei transmute to the next-heavier isotope, many of which are unstable.
5. Cosmic radiation is not a common concern, as the Earth's atmosphere absorbs it and the magnetosphere acts as a shield, but it poses a problem for satellites and astronauts and frequent fliers are also at a slight risk. Cosmic radiation is extremely high energy, and is very penetrating.
6. Electromagnetic radiation consists of emissions of electromagnetic waves, the properties of which depend on the wavelength.
7. X-ray and gamma radiation are best absorbed by atoms with heavy nuclei; the heavier the nucleus, the better the absorption. In some special applications, depleted uranium is used, but lead is much more common; several centimeters are often required. Barium sulfate is used in some applications too. However, when cost is important, almost any material can be used, but it must be far thicker. Most nuclear reactors use thick concrete shields to create a bioshield with a thin water cooled layer of lead on the inside to protect the porous concrete from the coolant inside. The concrete is also made with heavy aggregates, such as Baryte, to aid in the shielding properties of the concrete.
8. Ultraviolet (UV) radiation is ionizing but it is not penetrating, so it can be shielded by thin opaque layers such as sunscreen, clothing, and protective eyewear. Protection from UV is simpler than for the other forms of radiation above, so it is often considered separately.

At the bottom of this visible emission model is a visual intensity curve. Credit: Stanlekub.

At its simplest theoretical radiation astronomy is the definition of terms to be applied to astronomical radiation phenomena.

Def. a theory of the science of the biological, chemical, physical, and logical laws (or principles) with respect to any natural radiation source in the sky especially at night is called theoretical radiation astronomy.

Exploratory theory is the playtime activity that leads to discoveries which better our world. In the radiation physics laboratories here on Earth, the emission, reflection, transmission, absorption, and fluorescence of radiation is studied and laws relative to sources are proven.

"A principle is a law or rule that has to be, or usually is to be followed, or can be desirably followed, or is an inevitable consequence of something, such as the laws observed in nature or the way that a system is constructed. The principles of such a system are understood by its users as the essential characteristics of the system, or reflecting system's designed purpose, and the effective operation or use of which would be impossible if any one of the principles was to be ignored.[6]"[7]

# Meteor astronomy

This meteor image of October 17, 2012, is prior to the meteorite fall on the same day. Credit: Paola-Castillo; and Petrus M. Jenniskens, SETI Institute/NASA ARC.

"A meteor is the visible path of a meteoroid that has entered the Earth's atmosphere."[8]

Although there are many definitions of a meteor ranging from "[a]ny atmospheric phenomenon"[9] to "[a] fast-moving streak of light in the night sky caused by the entry of extraterrestrial matter into the earth's atmosphere: A shooting star or falling star"[9], for radiation astronomy, an alternative definition is used.

Def. any natural object radiating through a portion or all of the Earth's or another natural object's atmosphere is called a meteor.

A hypervelocity star "snow-plowing" through the interstellar medium of a galaxy is a meteor and the subject of meteor astronomy.

A meteor may be as small as an electron. Astronomical objects that are atoms, nuclei, or subatomic particles are part of cosmic-ray astronomy.

# Cosmic-ray astronomy

The flux of cosmic-ray particles is a function of their energy. Credit: Sven Lafebre, after Swordy.[10]

At right is an image indicating the range of cosmic-ray energies. The flux for the lowest energies (yellow zone) is mainly attributed to solar cosmic rays, intermediate energies (blue) to galactic cosmic rays, and highest energies (purple) to extragalactic cosmic rays.[10]

There is "a correlation between the arrival directions of cosmic rays with energy above 6 x 1019 electron volts and the positions of active galactic nuclei (AGN) lying within ~75 megaparsecs."[11]

"[T]he Oh-My-God particle [was] observed on the evening of 15 October 1991 over Dugway Proving Ground, Utah. Its observation was a shock to astrophysicists, who estimated its energy to be approximately 3×1020
eV
[12](50 joules)—in other words, a subatomic particle with kinetic energy equal to that of a baseball (142 g or 5 oz) traveling at 100 km/h (60 mph)."[13]

"It was most probably a proton with a speed very close to the speed of light, so close, in fact, [(1 − 5×10−24
) × c], that in a year-long race between light and the cosmic ray, the ray would fall behind only 46 nanometers (5×10−24
light-years), or 0.15 femtoseconds (1.5×10−16
s
).[14]"[13]

# Neutron astronomy

The image shows the hydrogen concentrations on the Moon detected by the Lunar Prospector. Credit: NASA.

Around EeV (1018 eV) energies, there may be associated ultra high energy neutrons "observed in anisotropic clustering ... because of the relativistic neutrons boosted lifetime."[15] “[A]t En = 1020 eV, [these neutrons] are flying a Mpc, with their directional arrival (or late decayed proton arrival) ... more on-line toward the source.”[15] From “neutron (and anti-neutron) life-lengths (while being marginal or meaningless at tens of Mpcs)", the growth of their half-lives with energy may naturally explain an associated, showering neutrino halo.[15]

Fairly large fluxes of neutrons have been observed during solar flares such as that of November 12, 1960, with a flux of 30-70 neutrons per cm-2 s-1.[16]

At right is the result of an all Moon survey by the Lunar Prospector using an onboard neutron spectrometer (NS). Cosmic rays impacting the lunar surface generate neutrons which in turn lose much of their energy in collisions with hydrogen atoms trapped within the Moon's surface.[17] Some of these thermal neutrons collide with the helium atoms within the NS to yield an energy signature which is detected and counted.[17] The NS aboard the Lunar Prospector has a surface resolution of 150 km.[17]

# Proton astronomy

The diagram shows a possible proton collision with an atmosphere molecule. Credit: Magnus Manske.

"Proton astronomy should be possible; it may also provide indirect information on inter-galactic magnetic fields."[18]

Proton astronomy per se often consists of directly or indirectly detecting the protons and deconvoluting a spatial, temporal, and spectral distribution.

“[A]t the high end of the proton energy spectrum (above ≈ 1018 eV) [the Larmor radius] deflection becomes small enough that proton astronomy becomes possible.”[19]

"The third largest solar proton event in the past thirty years took place during July 14-16, 2000, and had a significant impact on the earth's atmosphere."[20]

# Beta particle astronomy

"Beta particles are high-energy, high-speed electrons or positrons"[21].

Beta particles may be the key to fusion. "If the exterior of the capsule is maintained at a uniform temperature of about 19.5 K, the natural beta decay energy of the tritium will accomplish this through a process known as "beta layering." The very low energy beta particles from tritium decay deposit their energy very close to the location of the original tritium atoms."[22]

"Beta-particles leaving the upper surface of the lunar sample could trigger the upper beta detector, while the lower beta-detector was triggered by beta particles from the lower surface of the sample."[23]

Notation: let the symbol β designate an unbound electron in motion.

Notation: let β+ designate an unbound positron in motion.

## Electron astronomy

Aurorae are mostly caused by energetic electrons precipitating into the atmosphere.[24] Credit: Samuel Blanc[2].

Although electron astronomy is usually not recognized as a formal branch of astronomy, the measurement of electron fluxes help to understand a variety of natural phenomena.

Particles such as electrons are used as tracers of cosmic magnetic fields.[25] "From a plasma-physics point of view, the particles represent the correct way to identify magnetic field lines."[25] "The suprathermal electrons in the solar wind and in solar particle events have excellent properties for this application: they move rapidly, they remain tightly bound to their field lines, and they may arrive "scatter-free" even at low energies, and from deep in the solar atmosphere (Lin 1985)."[25] These electrons "provide remote-sensing observations of distant targets in the heliosphere - the Sun, the Moon, Jupiter, and various heliospheric structures."[25] ""[E]lectron astronomy" has an interesting future".[25]

"A delta ray is characterized by very fast electrons produced in quantity by alpha particles or other fast energetic charged particles knocking orbiting electrons out of atoms. Collectively, these electrons are defined as delta radiation when they have sufficient energy to ionize further atoms through subsequent interactions on their own."[26]

"The conventional procedure of delta-ray counting to measure charge (Powell, Fowler, and Perkins 1959), which was limited to resolution σz = 1-2 because of uncertainties of the criterion of delta-ray ranges, has been significantly improved by the application of delta-ray range distribution measurements for 16O and 32S data of 200 GeV per nucleon (Takahashi 1988; Parnell et al. 1989)."[27] Here, the delta-ray tracks in emulsion chambers have been used for "[d]irect measurements of cosmic-ray nuclei above 1 TeV/nucleon ... in a series of balloon-borne experiments".[27]

## Positron astronomy

Observation of positrons from a terrestrial gamma ray flash is performed by the Fermi gamma ray telescope. Credit: NASA Goddard Space Flight Center.

"Positron astronomy is 30 years old but remains in its infancy."[28]

"[P]ositron astronomy results ... have been obtained using the INTEGRAL spectrometer SPI".[29] The positrons are not directly observed by the INTEGRAL space telescope, but "the 511 keV positron annihilation emission is".[29]

During solar flares “[s]everal radioactive nuclei that emit positrons are also produced; [which] slow down and annihilate in flight with the emission of two 511 keV photons or form positronium with the emission of either a three gamma continuum (each photon < 511 keV) or two 511 keV photons."[30]

# Neutrino astronomy

This "neutrino image" of the Sun is by using the Super-Kamiokande to detect the neutrinos from nuclear fusion in the solar interior. Credit: R. Svoboda and K. Gordan (LSU), and NASA.

“The field of neutrino astronomy is still very much in its infancy – the only confirmed extraterrestrial sources so far are the Sun and supernova SN1987A.”[31] Neutrino astronomy “observes astronomical objects with neutrino detectors in special observatories.”[32]

“Because neutrinos are only weakly interacting with other particles of matter, neutrino detectors must be very large in order to detect a significant number of neutrinos. Neutrino detectors are often built underground to isolate the detector from cosmic rays and other background radiation.[33][31]

The Super-Kamiokande, or "Super-K" is a large-scale experiment constructed in an unused mine in Japan to detect and study neutrinos. The image at right required 500 days worth of data to produce the "neutrino image" of the Sun. The image is centered on the Sun's position. This image covers a 90° x 90° octant of the sky (in right ascension and declination). The higher the brightness of the color, the larger is the neutrino flux.

# Gamma-ray astronomy

This photograph shows Vela 5A/B satellites in their cleanroom. Credit: Los Alamos National Laboratory and NASA.

"Most astronomical gamma-rays are thought to be produced not from radioactive decay, however, but from the same type of accelerations of electrons, and electron-photon interactions, that produce X-rays in astronomy (but occurring at a higher energy in the production of gamma-rays)."[34]

For gamma-ray astronomy, "the Vela satellites were the first devices ever to detect cosmic gamma ray bursts."[35]

"Gamma-ray bursts (GRBs) are flashes of gamma rays associated with extremely energetic explosions that have been observed in distant galaxies. They are the most luminous electromagnetic events known to occur in the universe. Bursts can last from ten milliseconds to several minutes, although a typical burst lasts 20–40 seconds. The initial burst is usually followed by a longer-lived "afterglow" emitted at longer wavelengths (X-ray, ultraviolet, optical, infrared, microwave and radio).[36]"[37]

# X-ray astronomy

This image captures the core of Messier 31 (M31) in X-rays using the Chandra X-ray Observatory. Credit: S. Murray, M. Garcia, et al., Authors & editors: Robert Nemiroff (MTU) & Jerry Bonnell (USRA) NASA.

X-rays are electromagnetic radiation from a portion of the wavelength spectrum of about 5 to 8 nanometers (nm)s down to approximately 5 to 8 picometers (pm)s (ranging over three orders of magnitude).

An astronomical X-ray source may have one or more positional locations, plus associated error circles or boxes, from which incoming X-radiation (X-rays) has been detected.

Generally, a coronal cloud, a cloud composed of plasma, is usually associated with a star or other celestial or astronomical body, extending sometimes millions of kilometers into space, or thousands of light-years, depending on the associated body. The high temperature of the coronal cloud gives it unusual spectral features. These features have been traced to highly ionized atoms of elements such as iron which indicate a plasma's temperature in excess of 106 K (MK) and associated emission of X-rays.

The importance of X-ray astronomy is exemplified in the use of an X-ray imager such as the one on GOES 14 for the early detection of solar flares, coronal mass ejections (CME)s and other X-ray generating phenomena that impact the Earth.

# Ultraviolet astronomy

A GALEX image of the spiral galaxy Messier 81 in ultraviolet light. Credit: NASA/JPL-Caltech/J. Huchra (Harvard-Smithsonian CfA).

"Ultraviolet astronomy is generally used to refer to observations of electromagnetic radiation at ultraviolet wavelengths between approximately 10 and 320 nanometres"[38].

There are many important spectral lines in these wavelengths. Among the most important are the Lyman lines, which are emitted or absorbed when an electron jumps to or from the innermost electron shell in a hydrogen atom. The first three (known as alpha, beta and gamma) have wavelengths of 121.52, 102.53 and 97.22 nm respectively.[39]

Since the Earth's atmosphere strongly absorbs ultraviolet light, especially the shorter wavelengths, ultraviolet astronomy is mostly conducted by satellites. Longer wavelengths can be detected from baloons launched into the stratosphere.

Like the English astronomer William Fox, "In the summer of 1980, reflecting his age, Walter Scott Houston finally underwent surgery to remove a cataract from his right eye. Now to just about anyone else, a cataract would spell the end of a sky gazing career. But not Houston. With his lens removed and a plastic UV-transparent replacement implanted, Scotty reported that a whole new world of star gazing was opened up. The flood of ultraviolet light onto his retina allowed him to see faint blue stars previously invisible by at least one magnitude above the visual limit (to normally sighted observers)."[40]

# Optical astronomy

Actuators are part of the active optics of the Gran Telescopio Canarias. Credit: Vesta.

Optical astronomy includes those portions of ultraviolet, visual, and infrared astronomy that benefit from the use of quartz crystal or silica glass telescope components.

"Observations at these wavelengths generally use optical components (mirrors, lenses and solid state digital detectors)."[41]

"In popular culture optical astronomy encompasses a wide variety of observations via telescopes that are sensitive in the range of visible light. Scientists would call this visible-light astronomy. It includes imaging, where a picture of some sort is made of the object; photometry, where the amount of light coming from an object is measured, spectroscopy, where the distribution of that light with respect to its wavelength is measured, and polarimetry where the polarisation state of that light is measured."[41]

Def. "[a]stronomy using infrared, visible and/or ultraviolet wavelengths"[42] is called optical astronomy.

Def. "[a]n optical system in telescopes that reduces atmospheric distortion by dynamically measuring and correcting wavefront aberrations in real time, often by using a deformable mirror"[43] is called adaptive optics.

"Already it has allowed ground-based telescopes to produce images with sharpness rivalling those from the Hubble Space Telescope. The technique is expected to revolutionize the future of ground-based optical astronomy."[44]

"[T]he color index is a simple numerical expression that determines the color of an object, which in the case of a star gives its temperature. To measure the index, one observes the magnitude of an object successively through two different filters, such as U and B, or B and V, where U is sensitive to ultraviolet rays, B is sensitive to blue light, and V is sensitive to visible (green-yellow) light (see also: UBV system). The set of passbands or filters is called a photometric system. The difference in magnitudes found with these filters is called the U-B or B–V color index, respectively. The smaller the color index, the more blue (or hotter) the object is. Conversely, the larger the color index, the more red (or cooler) the object is. This is a consequence of the logarithmic magnitude scale, in which brighter objects have smaller (more negative) magnitudes than dimmer ones. For comparison, the yellowish Sun has a B–V index of 0.656 ± 0.005,[45] while the bluish Rigel has B–V –0.03 (its B magnitude is 0.09 and its V magnitude is 0.12, B–V = –0.03).[46] The passbands most optical astronomers use are the UBVRI filters, where the U, B, and V filters are as mentioned above, the R filter passes red light, and the I filter passes infrared light. ... These filters were specified as particular combinations of glass filters and photomultiplier tubes."[47]

"An optical telescope gathers and focuses light mainly from the visible part of the electromagnetic spectrum (although some work in the infrared and ultraviolet).[48]"[49]

# Visual astronomy

“I think everyone can conjure up a mental image of astronomers at every level and place in history, gazing through the eyepieces of their telescopes at sights far away - true visual astronomy.”[50]

Color Frequency Wavelength
violet 668–789 THz 380–450 nm
blue 631–668 THz 450–475 nm
cyan 606–630 THz 476–495 nm
green 526–606 THz 495–570 nm
yellow 508–526 THz 570–590 nm
orange 484–508 THz 590–620 nm
red 400–484 THz 620–750 nm

"The visible spectrum is the portion of the electromagnetic spectrum that is visible to (can be detected by) the human eye. Electromagnetic radiation in this range of wavelengths is called visible light or simply light. A typical human eye will respond to wavelengths from about 390 to 750 nm.[51] In terms of frequency, this corresponds to a band in the vicinity of 400–790 THz. A light-adapted eye generally has its maximum sensitivity at around 555 nm (540 THz), in the green region of the optical spectrum (see: luminosity function)."[52]

There are several cases of astronomers who claimed that following a cataract operation, they could see shorter wavelengths than other people, slightly into the ultraviolet.

# Violet astronomy

This image of Venus is taken through a violet filter by the Galileo spacecraft on February 14, 1990. Credit: NASA/JPL-Caltech.

"The aluminium abundance was derived from the resonance line at 394.4nm, and Al is underabundant by ∼ −0.7 dex with respect to iron."[53] "These abundances are the LTE values; no NLTE corrections, as prescribed by Baum ̈uller and Gehren (1997) and Baumüller et al. (1998), have been applied. The prescribed NLTE corrections for Teff = 6500K, log g = 4.0, [Fe/H] = –3.0 are –0.11 ... for ... Al .... If we assume these values to apply for our lower-gravity star [CS 29497-030], then Al follows iron"[53]. The elemental abundance ratios for CS 29497-030 of aluminum are [Al/H] = -3.37, [Al/Fe] = -0.67.[53]

A discovery in violet astronomy is that "carbon stars are enormously fainter in the violet region than expected from appropriate blackbody spectra."[54]

Violet photographs of the planet Venus taken in 1927 “recorded two nebulous bright streaks, or bands, running ... approximately at right angles to the terminator” that may be from the upper atmosphere.[55]

"The “Purple Haze” is a diffuse blueish/purple glow within a few arcseconds of the central star in HST images of the Homunculus (Morse et al. 1998; Smith et al. 2000, 2004). This emission is seen in excess of violet starlight scattered by dust, and the strength of the excess increases into the far UV (Smith et al. 2004; hereafter Paper I)."[56]

# Blue astronomy

This picture from the Voyager 2 sequence shows two of the four cloud features which have been tracked by the Voyager cameras during the past two months. Credit: NASA.

Blue astronomy is focused on the wavelength range 450-475 nm.

Stars are often referred to by their predominant color. For example, blue stragglers are found among the galactic halo globular clusters.[57] Blue main sequence stars that are metal poor ([Fe/H] ≤ -1.0) are most likely very different in origin from blue stragglers.[57]

"[G]round-based UV [and blue astronomy] is a powerful facility for [the] study of [the] chemical evolution of [the] early Galaxy."[58] UV and B astronomy use radiation over the wavelength range 355.0-500.0 nm.[58]

“To date, all of the reported hypervelocity stars (HVSs), which are believed to be ejected from the Galactic center, are blue and therefore almost certainly young.”[59]

"A trace amount of methane is also present. Prominent absorption bands of methane occur at wavelengths above 600 nm, in the red and infrared portion of the spectrum. As with Uranus, this absorption of red light by the atmospheric methane is part of what gives Neptune its blue hue,[60] although Neptune's vivid azure differs from Uranus's milder cyan. Since Neptune's atmospheric methane content is similar to that of Uranus, some unknown atmospheric constituent is thought to contribute to Neptune's colour.[61]"[62]

# Cyan astronomy

Recent changes in Comet Lulin's greenish coma and tails are shown in these two panels taken on January 31st (top) and February 4th (bottom) 2009. In both views the comet has an apparent antitail to the left of the coma of dust. Credit: Joseph Brimacombe, Cairns, Australia.

Perhaps the most prominent cyan planetary source is Uranus, which has only been visited by the space probe Voyager 2. More recent images come from the Hubble Space Telescope in orbit around Earth.

"Methane possesses prominent absorption bands in the visible and near-infrared (IR) making Uranus aquamarine or cyan in color.[63]"[64]

“During the Halley Monitoring Program at La Silla from Feb.17 to Apr.17,1986 ... In the light of the neutral CN-radical a continuous formation and expansion of [cyan] gas-shells could be observed.”[65] “The gas-expansion velocity decreases with increasing heliocentric distance from 1 km/s in early March to 0.8 km/s in April.”[65]

Shown at right, "Lulin's green color comes from the gases that make up its Jupiter-sized atmosphere. Jets spewing from the comet's nucleus contain cyanogen (CN: a poisonous gas found in many comets) and diatomic carbon (C2). Both substances glow green when illuminated by sunlight"[66]

“The electric blue glow of electricity results from the spectral emission of the excited ionized atoms (or excited molecules) of air (mostly oxygen and nitrogen) falling back to unexcited states, which happens to produce an abundance of electric blue light. This is the reason electrical sparks in air, including lightning, appear electric blue. It is a coincidence that the color of Cherenkov radiation and light emitted by ionized air are a very similar blue despite their very different methods of production.”[67]

# Green astronomy

A picture of the solar corona taken with the LASCO C1 coronagraph. The image is color coded for the doppler shift of the FeXIV 530.8 nm line. Credit: NASA and NRL.

Green objects or emission lines in the green portion of the visible spectrum are the subject of green astronomy.

In the image at right the iron (Fe XIV) green line is followed by doppler imaging to show associated relative coronal plasma velocity towards (-7 km/s side) and away from (+7 km/s side) the large angle spectrometric coronagraph LASCO satellite camera.

"Carroll and McCormack (1972) in Dublin reported complex spectra in the blue and green wavelength regions of both FeH and FeD".[66]

For elongated dust particles in cometary comas an investigation is performed at 535.0 nm (green) and 627.4 nm (red) peak transmission wavelengths of the Rosetta spacecraft's OSIRIS Wide Angle Camera broadband green and red filters, respectively.[68] "In the green, the polarization of the pure silicate composition qualitatively appears a better fit to the shape of the observed polarization curves".[68] "[B]ut they are characterized by a high albedo."[68] The silicates used to model the cometary coma dust are olivene (Mg-rich is green) and the pyroxene, enstatite.[68]

"In December 2006, seven papers were published in the scientific journal, Science, discussing initial details of the sample analysis. Among the findings are: a wide range of organic compounds, including two that contain biologically usable nitrogen; indigenous aliphatic hydrocarbons with longer chain lengths than those observed in the diffuse interstellar medium; abundant amorphous silicates in addition to crystalline silicates such as olivine and pyroxene, proving consistency with the mixing of solar system and interstellar matter, previously deduced spectroscopically from ground observations;[69] hydrous silicates and carbonate minerals were found to be absent, suggesting a lack of aqueous processing of the cometary dust; limited pure carbon (CHON) was also found in the samples returned; methylamine and ethylamine was found in the aerogel but was not associated with specific particles."[70]

# Yellow astronomy

This is a visual image of the Sun with some sunspots visible. The two small spots in the middle have about the same diameter as our planet Earth. Credit: NASA.

During the limb flares of December 18, 1956, a coronal line at 569.4 nm, a yellow line, occurred at 1822 UTC, 1900 UTC, undiminished up to 20,000 km above the solar limb, and at 2226 UTC, is identified as Ca XV.[71] "The coronal temperature was 4000000°."[71] "The December 18, 1956, flare appears to have been a violent condensation of material from a dense coronal cloud above an active region."[71]

Sodium produces two spectral lines known as D1 and D2, or the "sodium doublet". Their average wavelength, 589.3 nm, is often just called "D".

Io "is the innermost of the four Galilean moons of the planet Jupiter and, with a diameter of 3,642 kilometres (2,263 mi), the fourth-largest moon in the Solar System. ... With over 400 active volcanoes, Io is the most geologically active object in the Solar System.[72][73] ... Most of Io's surface is characterized by extensive plains coated with sulfur and sulfur dioxide frost. ... Io's volcanism is responsible for many of the satellite's unique features. Its volcanic plumes and lava flows produce large surface changes and paint the surface in various shades of yellow, red, white, black, and green, largely due to allotropes and compounds of sulfur."[74]

# Orange astronomy

Cloud bands are clearly visible on Jupiter. Credit: NASA/JPL/USGS.

"[O]range [is] the color of Jupiter"[75].

"The orange and brown coloration in the clouds of Jupiter are caused by upwelling compounds that change color when they are exposed to ultraviolet light from the Sun. The exact makeup remains uncertain, but the substances are believed to be phosphorus, sulfur or possibly hydrocarbons.[76][77] These colorful compounds, known as chromophores, mix with the warmer, lower deck of clouds. The zones are formed when rising convection cells form crystallizing ammonia that masks out these lower clouds from view.[78]"[79].

The orange system [in orange astronomy] is a number of emission lines very close together forming a band in the orange portion of the visible spectrum. These lines are usually associated with particular molecular species, including ScO, YO, and TiO.[80]

The orange band from molecular CaCl is "observed in the spectra of many carbon stars."[81]

The Fe VII emission line at 608.7 nm, "frequently observed in the spectra of astrophysical plasmas", has been detected in planetary nebulae, Seyfert galaxies, and quasars.[82]

# Red astronomy

AZ Cancri. Credit: SDSS Data Release 6.

With respect to the color 'red', there are studies of the redness of objects such as the red dwarf AZ Cancri shown in the visual image at right. Cool stars of spectral class M appear red; they are (depending on their size) referred to as "red giants" or "red dwarfs".

"Ideally all intrinsic colours should be found from unreddened stars. This is possible for dwarf and giant stars later than about A0 (Johnson, 1964) ... However, it cannot be used for stars of other spectral classes since they are all relatively infrequent in space, and generally reddened."[83]

A very important wavelength in this region is the Balmer alpha line, 656.28 nm. It is emitted or absorbed by hydrogen atoms when electrons move between the second and third electron shells. Other Balmer lines, known as beta, gamma and delta, have wavelengths of 486.13, 434.05 and 410.17 nm respectively;[3] these are also in the visual range but are less important than the alpha line.

# Infrared astronomy

This is a plot of Earth atmosphere transmittance in the infrared region of the electromagnetic spectrum. Credit: US Navy.

"The wavelength of infrared light ranges from 0.75 to 300 micrometers. Infrared falls in between visible radiation, which ranges from 380 to 750 nanometers, and submillimeter waves."[84]

"Infrared and optical astronomy are often practiced using the same telescopes, as the same mirrors or lenses are usually effective over a wavelength range that includes both visible and infrared light."[84]

"Far-infrared astronomy ... deals with objects visible in far-infrared radiation (extending from 30 µm towards submillimeter wavelengths around 450 µm)."[85]

"Huge, cold clouds of gas and dust in our own galaxy, as well as in nearby galaxies, glow in far-infrared light. This is due to thermal radiation of interstellar dust contained in molecular clouds."[85]

Visually dark infrared sources can be radiative cosmic dust, hydrogen gas such as an H II region (e.g. the Orion Nebula), an H I region of hydrogen, a molecular cloud, or a coronal cloud.

There are about 1,892,100 infrared (IR) objects in the SIMBAD database. Some of these like IRAS 20542+3631 are only IR objects. 1RXS J205444.6+361116 is an IR and an X-ray object only. These objects are visibly dark infrared sources. As is 2MASS J21074764+3802561, which is an IR and UV object only.

# Submillimeter astronomy

BLAST is hanging from the launch vehicle in Esrange near Kiruna, Sweden before launch June 2005. Credit: Mtruch.

"Submillimetre astronomy or submillimeter astronomy (see spelling differences) is the branch of observational astronomy that is conducted at submillimetre wavelengths of the electromagnetic spectrum. Astronomers place the submillimetre waveband between the far-infrared and microwave wavebands, typically taken to be between a few hundred micrometres and a millimetre." and "Using submillimetre observations, astronomers examine molecular clouds and dark cloud cores with a goal of clarifying the process of star formation from earliest collapse to stellar birth."[86]

These wavelengths are sometimes called Terahertz radiation, since they have frequencies of the order of 1 THz.

“The Balloon-borne Large Aperture Submillimeter Telescope (BLAST) is a submillimeter telescope that hangs from a high altitude balloon. It has a 2 meter primary mirror that directs light into bolometer arrays operating at 250, 350, and 500 µm. ... BLAST's primary science goals are:[87]

• Measure photometric redshifts, rest-frame FIR luminosities and star formation rates of high-redshift starburst galaxies, thereby constraining the evolutionary history of those galaxies that produce the FIR/submillimeter background.
• Measure cold pre-stellar sources associated with the earliest stages of star and planet formation.
• Make high-resolution maps of diffuse galactic emission over a wide range of galactic latitudes.”[88]

This image has the radio image of Greg Taylor, NRAO, overlain on the X-ray image from Chandra. The radio source Hydra A originates in a galaxy near the center of the cluster. Optical observations show a few hundred galaxies in the cluster. Credit: NASA/CXC/SAO; Radio: NRAO.

"Radio waves are a type of electromagnetic radiation with wavelengths in the electromagnetic spectrum longer than infrared light. Radio waves have frequencies from 300 GHz to as low as 3 kHz, and corresponding wavelengths from 1 millimeter to 100 kilometers."[89]

"Microwaves, a subset of radio waves, have wavelengths ranging from as long as one meter to as short as one millimeter, or equivalently, with frequencies between 300 MHz (0.3 GHz) and 300 GHz.[90] This broad definition includes both UHF and EHF (millimeter waves), and various sources use different boundaries.[91] In all cases, microwave includes the entire SHF band (3 to 30 GHz, or 10 to 1 cm) at minimum, with RF engineering often putting the lower boundary at 1 GHz (30 cm), and the upper around 100 GHz (3 mm)."[92]

Several satellites have served as observatories for radio waves and specifically for microwaves. The Radio Astronomy Explorer (RAE) 1 is launched into orbit on July 4, 1968, around Earth, while the RAE 2 is launched on June 10, 1973, around the Moon.

The COBE is launched into Earth orbit on November 18, 1989. The WMAP is launched on June 30, 2001, into orbit at the Lagrange 2 location. Both satellites have aboard detectors designed to perform microwave astronomy, as these are limited to only the microwave band.

# Superluminal astronomy

Because a tachyon always moves faster than light, we cannot see it approaching. After a tachyon has passed nearby, we would be able to see two images of it, appearing and departing in opposite directions. Credit: TxAlien.

In the diagram at right, the black line is the shock wave of Cherenkov radiation, shown only in one moment of time. This double image effect is most prominent for an observer located directly in the path of a superluminal object (in this example a sphere, shown in grey). The right hand bluish shape is the image formed by the blue-doppler shifted light arriving at the observer—who is located at the apex of the black Cherenkov lines—from the sphere as it approaches. The left-hand reddish image is formed from red-shifted light that leaves the sphere after it passes the observer. Because the object arrives before the light, the observer sees nothing until the sphere starts to pass the observer, after which the image-as-seen-by-the-observer splits into two—one of the arriving sphere (to the right) and one of the departing sphere (to the left).

Superluminal refers "to the propagation of information or matter faster than the speed of light. Under the special theory of relativity, a particle (that has rest mass) with subluminal velocity needs infinite energy to accelerate to the speed of light, although special relativity does not forbid the existence of particles that travel faster than light at all times (tachyons)."[93]

"On the other hand, what some physicists refer to as "apparent" or "effective" FTL[94][95][96][97] depends on the hypothesis that unusually distorted regions of spacetime might permit matter to reach distant locations in less time than light could in normal or undistorted spacetime. Although according to current theories matter is still required to travel subluminally with respect to the locally distorted spacetime region, apparent FTL is not excluded by general relativity."[93]

Tachyonic γ rays have not been observed directly as of 2007.[98] "The tachyonic spectral densities generated by ultra-relativistic electrons in uniform motion are fitted to the high-energy spectra of Galactic supernova remnants, such as RX J0852.0−4622 and the pulsar wind nebulae in G0.9+0.1 and MSH 15-52. ... Tachyonic cascade spectra are quite capable of generating the spectral curvature seen ... Estimates on the electron/proton populations generating the tachyon flux are obtained from the spectral fits"[98]

"Tachyonic radiation implies superluminal signal transfer [1-7], the energy quanta propagating faster than light in vacuum, in contrast to rotating superluminal light sources emitting vacuum Cherenkov radiation [8, 9]."[99] "The existence of superluminal energy transfer has not been established so far, and one may ask why. There is the possibility that superluminal quanta just do not exist, the vacuum speed of light being the definitive upper bound. There is another explanation, the interaction of superluminal radiation with matter is very small, the quotient of tachyonic and electric fine-structure constants being q2/e2 ≈ 1.4 x 10-11 [5], and therefore superluminal quanta are hard to detect."[99]

“Observed variations concerning the brightness distributions in four extragalactic radio sources were so rapid that the apparent transverse velocity of expansion is greater than the velocity of light.”[100]

# Chemistry

This image is a cross-section of the Laguna Manantiales meteorite showing Widmanstätten patterns. Credit: Aram Dulyan.

“[T]he study of the abundance and reactions of chemical elements and molecules in the universe, [as can be assessed by] their interaction with radiation” is part of astronomical radiation chemistry"[101].

Each of the different forms of radiation often interact with chemicals in novel and sometimes surprising ways.

"Ultraviolet line spectrum measurements are used to discern the chemical composition, densities, and temperatures of the interstellar medium, and the temperature and composition of hot young stars."[102]

Def. "[a] metallic or stony object that is the remains of a meteor", from Wiktionary meteorite, is called a meteorite.

"Widmanstätten patterns, also called Thomson structures, are unique figures of long nickel-iron crystals, found in the octahedrite iron meteorites and some pallasites. They consist of a fine interleaving of kamacite and taenite bands or ribbons called lamellæ. Commonly, in gaps between the lamellæ, a fine-grained mixture of kamacite and taenite called plessite can be found."[103]

# Geography

All four of the HESS telescope array in Namibia are in operation at night. Credit: H.E.S.S. collaboration.

"High Energy Stereoscopic System or H.E.S.S. is a next-generation system of Imaging Atmospheric Cherenkov Telescopes (IACT) for the investigation of cosmic gamma rays in the 100 GeV and TeV energy range. The acronym was chosen in honour of Victor Hess, who was the first to observe cosmic rays."[104]

"The name also emphasizes two main features of the currently-operating installation, namely the simultaneous observation of air showers with several telescopes, under different viewing angles, and the combination of telescopes to a large system to increase the effective detection area for gamma rays. H.E.S.S. permits the exploration of gamma-ray sources with intensities at a level of a few thousandth parts of the flux of the Crab Nebula."[104]

"H.E.S.S. is located on the Cranz family farm, Göllschau, in Namibia, near the Gamsberg, an area well known for its excellent optical quality. The first of the four telescopes of Phase I of the H.E.S.S. project went into operation in Summer 2002; all four were operational in December 2003."[104]

"The ideal submillimetre observing site is dry, cool, has stable weather conditions and is away from urban population centres. There are only a handful of such sites identified, they include Mauna Kea (Hawaii, USA), the Llano de Chajnantor Observatory on the Atacama Plateau (Chile), the South Pole, and Hanla (India). Comparisons show that all four sites are excellent for submillimetre astronomy, and of these sites Mauna Kea is the most established and arguably the most accessible. The Llano de Chajnantor Observatory site hosts the Atacama Pathfinder Experiment (APEX), the largest submillimetre telescope operating in the southern hemisphere, and the world's largest ground based astronomy project, the Atacama Large Millimeter Array (ALMA), an interferometer for submillimetre wavelength observations made of 54 12-metre and 12 7-metre radio telescopes. The Submillimeter Array (SMA) is another interferometer, located at Mauna Kea, consisting of eight 6-metre diameter radio telescopes. The largest existing submillimetre telescope, the James Clerk Maxwell Telescope, is also located on Mauna Kea."[105]

# History

The NRL Ionosphere 1 solar X-ray, ionosphere, and meteorite mission launches on a V-2 on September 29, 1949, from White Sands at 16:58 GMT and reached 151.1 km. Credit: Naval Research Laboratory.

The Hominidae have apparently been on Earth for around seven million years, at least somewhere in Africa and possibly elsewhere. Fortunately and deliberately, many of these have worked out ways to record knowledge about the objects or entities in the sky observed by the radiation they produce.

"Mere "star ordering" is not "astronomy", so far as the modern usage of the term implies, regardless of the word's etymology".[106]

The modern scientific discipline of astronomy focuses on reproducibility and physical theory to explain and describe observations. Many ancient observers produced remarkably reproducible calendars such as the Mesoamerican Long Count calendar which apparently goes from August 11, 3114 BCE, to October 13, 4772, and beyond.

From X-ray astronomy: "The beginning of the search for X-ray sources above the Earth's atmosphere is August 5, 1948, at 12:07 GMT (Greenwich Mean Time).[107][108] As part of Project Hermes a US Army (formerly German) V-2 rocket number 43 is launched from White Sands Proving Grounds, launch complex (LC) 33, to an altitude of 166 km.[108] This is "the first detection of solar X-rays."[109]"

"Infrared astronomy began in the 1830s, a few decades after the discovery of infrared light by William Herschel in 1800."[110]

"The initial detection of radio waves from an astronomical object was made in the 1930s, when Karl Jansky observed radiation coming from the Milky Way."[111]

# Mathematics

First synchrotron function, F(x)

In astrophysics, x is usually a ratio of frequencies, that is, the frequency over a critical frequency (critical frequency is the frequency at which most synchrotron radiation is radiated). This is needed when calculating the spectra for different types of synchrotron emission. It takes a spectrum of electrons (or any charged particle) generated by a separate process (such as a power law distribution of electrons and positrons from a constant injection spectrum) and converts this to the spectrum of photons generated by the input electrons/positrons.”[112]

Mathematics is involved in many ways to help describe the entities or objects used to model radiation astronomy results.

Usually, in mathematical astronomy, a number is associated with a dimension or aspect of an entity. For example, the Earth is 1.50 x 108 km on average from the Sun. Kilometer (km) is a dimension and 1.50 x 108 is a number.

Def. "[t]he study of the dimensions of ... quantities; used to obtain information about large complex systems, and as a means of checking ... equations", after Wiktionary dimensional analysis, is called dimensional analysis.

"Olivines are described by Mg2yFe2-2ySiO4, with y ∈ [0, 1]."[68] Substituting values for y from 0 to 1 produce ideal compositions from forsterite Mg2SiO4 to fayalite Fe2SiO4. "Amorphous olivine with y = 0.5 and crystalline olivine with y = 0.95 were taken into account for the olivine component." as best fits to observed data.[68]

# Physics

The physics of radiation astronomy consists of the emission of radiation by a source and the detection of this radiation by devices available to the astronomer. Astrophysics at its simplest is the application of laboratory physics, i.e., physics demonstrated in a laboratory and described with logical laws, to natural astronomical entities. This is done to understand these astronomical entities, their origin, history, and current constitution.

## Detection

From astronomy: radiation "[a]stronomy likely started with visual astronomy. Visual refers to that portion of the electromagnetic spectrum called the visible spectrum. Probing the sky with additional portions of this spectrum is difficult as the atmosphere absorbs over many portions." This absorption is illustrated by the diagram below.

The electromagnetic transmittance, or opacity, of the Earth's atmosphere is indicated on the right vertical scale. Credit: NASA and Mysid.

"To overcome the limitations of observing in portions on either side of the visual, telescopes and spectrometers are lofted above the atmosphere for short times on board sounding rockets and balloons. Longer observing times are available with satellites placed into orbit around the Earth, the Sun, or other solar system bodies." per astronomy.

## Emission

"Alpha decay is characterized by the emission of an alpha particle, a 4He nucleus. The mode of this decay causes the parent nucleus to decrease by two protons and two neutrons. This type of decay follows the relation:

${}_Z^A\!X\to {}_{Z-2}^{A-4}\!Y+ {}_4^2\alpha$ [113]"[114]

"Neutron activation is the process in which neutron radiation induces radioactivity in materials, and occurs when atomic nuclei capture free neutrons, becoming heavier and entering excited states. The excited nucleus often decays immediately by emitting particles such as neutrons, protons, or alpha particles. The neutron capture, even after any intermediate decay, often results in the formation of an unstable activation product. Such radioactive nuclei can exhibit half-lives ranging from small fractions of a second to many years."[115]

"Proton emission (also known as proton radioactivity) is a type of radioactive decay in which a proton is ejected from a nucleus. Proton emission can occur from high-lying excited states in a nucleus following a beta decay, in which case the process is known as beta-delayed proton emission, or can occur from the ground state (or a low-lying isomer) of very proton-rich nuclei, in which case the process is very similar to alpha decay."[116]

"Beta decay is characterized by the emission of a neutrino and a negatron which is equivalent to an electron. This process occurs when a nucleus has an excess of neutrons with respect to protons, as compared to the stable isobar. This type of transition converts a neutron into a proton; similarly, a positron is released when a proton is converted into a neutron. These decays follows the relation:

${}_Z^A\!X\to {}_{Z+1}^A\!Y+ \bar{\nu} + \beta^-$
${}_Z^A\!X\to {}_{Z-1}^A\!Y+ \nu + \beta^+$ [117]"[114]

This diagram illustrates part of the concept behind Bremsstrahlung electromagnetic radiation. Credit: Trex2001.

"Gamma ray emission is follows the previously discussed modes of decay when the decay leaves a daughter nucleus in an excited state. This nucleus is capable of further de-excitation to a lower energy state by the release of a photon. This decay follows the relation:

${}^A\!X^* \to {}^A\!Y + \gamma$ [118]"[114]

Generation of electromagnetic radiation can occur whenever charged particles pass within certain distances of each other without being in fixed orbits, the accelerations (or decelerations) may give off the radiation. This is partly illustrated by the diagram at right where an electron has its course altered by near passage by a positive particle. Bremsstrahlung radiation also occurs when two electrons or other similarly charged particles pass close enough to deflect, slow down, or speed up at least one of the particles.

Bremsstrahlung includes synchrotron and cyclotron radiation.

When high-energy radiation bombards materials, the excited atoms within emit characteristic "secondary" (or fluorescent) radiation.

# Planetary astronomy

This view of the rising Earth greeted the Apollo 8 astronauts as they came from behind the Moon after the lunar orbit insertion burn. Credit: NASA.

"Energetic photons, ions and electrons from the solar wind, together with galactic and extragalactic cosmic rays, constantly bombard surfaces of planets, planetary satellites, dust particles, comets and asteroids."[119] "[I]nterplanetary space ... is a stormy and sometimes very violent environment permeated by energetic particles and radation constantly emanating from the Sun."[119]

Each of the astronomical objects that constitute planetary science emits, reflects, or fluoresces radiation that is observed and analyzed.

"The spectrum of gaseous methane at 77 K in the 1.1-2.6 µm region [is] a benchmark for planetary astronomy".[120]

"The advantages of radar in planetary astronomy result from (1) the observer's control of all the attributes of the coherent signal used to illuminate the target, especially the wave form's time/frequency modulation and polarization; (2) the ability of radar to resolve objects spatially via measurements of the distribution of echo power in time delay and Doppler frequency; (3) the pronounced degree to which delay-Doppler measurements constrain orbits and spin vectors; and (4) centimeter-to-meter wavelengths, which easily penetrate optically opaque planetary clouds and cometary comae, permit investigation of near-surface macrostructure and bulk density, and are sensitive to high concentrations of metal or, in certain situations, ice."[121]

# Science

First Public Image is from GOES 14 taken with the Solar X-ray Imager (SXI). Credit: NWS Internet Services Team of the NOAA/Space Weather Prediction Center.

The image at right is the first public image taken by the solar X-ray imager (SXI) aboard the GOES 14 satellite. These geostationary operational environmental satellites (GOES) monitor the Sun’s X-rays for the early detection of solar flares, coronal mass ejections (CMEs), and other phenomena that impact the geospace environment. This early warning is important because travelling solar disturbances affect not only the safety of humans in high-altitude missions, such as human spaceflight, but also military and commercial satellite communications. In addition, CMEs can damage long-distance electric power grids, causing extensive power blackouts.

From X-ray astronomy: "An astronomical X-ray source catalog or catalogue is a list or tabulation of astronomical objects that are X-ray sources, typically grouped together because they share a common type, morphology, origin, means of detection, or method of discovery. Astronomical X-ray source catalogs are usually the result of an astronomical survey of some kind, often performed using an X-ray astronomical observatory in orbit around Earth."

• "Distribution and Variability of Cosmic X-Ray Sources", published on April 1, 1967, describes 35 astronomical X-ray sources detected by sounding rocket launched with an X-ray detector on board by the X-ray astronomy group at the Naval Research Laboratory in the United States.[122]
• "The fourth Uhuru catalog of X-ray sources", contains 339 sources observed over the entire active period of the satellite, but not necessarily the earlier designation.[123] It does not contain actual dates of observation for any sources. Sources detected during the final observation period from August 27, 1973, to January 12, 1974, are prefixed with "4U".
• "The Ariel V /3 A/ catalogue of X-ray sources. II - Sources at high galactic latitude |b| > 10°", contains sources with high galactic latitudes and includes some sources observed by HEAO 1, Einstein, OSO 7, SAS 3, Uhuru, and earlier, mainly rocket, observations.[124]

# Technology

This diagram illustrates a special version of a "black body" (instrument), used for defining the luminous intensity unit, before its current scientific International Standard (SI) definition. Credit: Lex Tollenaar.
This spectrum of X-rays is emitted by an X-ray tube with a rhodium target, operated at 60 kV. The continuous curve is due to bremsstrahlung, and the spikes are characteristic K lines for rhodium. Credit: LinguisticDemographer.
Beam of electrons are moving in a circle in a magnetic field (cyclotron motion). Lighting is caused by excitation of atoms of gas in a bulb. Credit: Marcin Białek.

Black-body radiation is the type of electromagnetic radiation within or surrounding a body in thermodynamic equilibrium with its environment, or emitted by a black body (an opaque and non-reflective body) held at constant, uniform temperature. The radiation has a specific spectrum and intensity that depends only on the temperature of the body.[125][126][127][128][129]

“In an X-ray tube, electrons are accelerated in a vacuum by an electric field and shot into a piece of metal called the "target". X-rays are emitted as the electrons slow down (decelerate) in the metal. The output spectrum consists of a continuous spectrum of X-rays, with additional sharp peaks at certain energies (see graph on right). The continuous spectrum is due to bremsstrahlung, while the sharp peaks are characteristic X-rays associated with the atoms in the target. For this reason, bremsstrahlung in this context is also called continuous X-rays.[130][131]

“A cyclotron is a compact type of particle accelerator in which charged particles in a static magnetic field are travelling outwards from the center along a spiral path and get accelerated by radio frequency electromagnetic fields. ... Cyclotrons accelerate charged particle beams using a high frequency alternating voltage which is applied between two "D"-shaped electrodes (also called "dees"). An additional static magnetic field $B$ is applied in perpendicular direction to the electrode plane, enabling particles to re-encounter the accelerating voltage many times at the same phase. To achieve this, the voltage frequency must match the particle's cyclotron resonance frequency

$f = \frac{q B}{2\pi m}$,

with the relativistic mass m and its charge q. This frequency is given by equality of centripetal force and magnetic Lorentz force. The particles, injected near the center of the magnetic field, increase their kinetic energy only when recirculating through the gap between the electrodes; thus they travel outwards along a spiral path.”[132]

Cyclotron radiation is electromagnetic radiation emitted by moving charged particles deflected by a magnetic field. The Lorentz force on the particles acts perpendicular to both the magnetic field lines and the particles' motion through them, creating an acceleration of charged particles that causes them to emit radiation (and to spiral around the magnetic field lines). ... Cyclotron radiation is emitted by all charged particles travelling through magnetic fields, however, not just those in cyclotrons. Cyclotron radiation from plasma in the interstellar medium or around black holes and other astronomical phenomena is an important source of information about distant magnetic fields. The power (energy per unit time) of the emission of each electron can be calculated using:

${-dE \over dt}={\sigma_t B^2 V^2 \over c \mu_o}$

where E is energy, t is time, $\sigma_t$ is the Thomson cross section (total, not differential), B is the magnetic field strength, V is the velocity perpendicular to the magnetic field, c is the speed of light and $\mu_o$ is the permeability of free space.”[133]

“A synchrotron is a particular type of cyclic particle accelerator originating from the cyclotron in which the guiding magnetic field (bending the particles into a closed path) is time-dependent, being synchronized to a particle beam of increasing kinetic energy. The synchrotron is one of the first accelerator concepts that enable the construction of large-scale facilities, since bending, beam focusing and acceleration can be separated into different components. ... Unlike in a cyclotron, synchrotrons are unable to accelerate particles from zero kinetic energy; one of the obvious reasons for this is that its closed particle path would be cut by a device that emits particles. Thus, schemes were developed to inject pre-accelerated particle beams into a synchrotron. The pre-acceleration can be realized by a chain of other accelerator structures like a linac, a microtron or another synchrotron; all of these in turn need to be fed by a particle source comprising a simple high voltage power supply, typically a Cockcroft-Walton generator.”[112]

# References

1. Philip B. Gove, ed (1963). Webster's Seventh New Collegiate Dictionary. Springfield, Massachusetts: G. & C. Merriam Company. pp. 1221.
2. Stuart Ross Taylor (29 July 2004). "Why can't planets be like stars?". Nature 430 (6999): 509. doi:10.1038/430509a. PMID 15282586. Bibcode2004Natur.430..509T.
3. (May 16, 2012) "Planetary science". Wikipedia. San Francisco, California: Wikimedia Foundation, Inc. Retrieved on 2012-06-06.
4. Narlikar JV (1990). Pasachoff JM, Percy JR. ed. Curriculum for the Training of Astronomers ‘’In: The Teaching of astronomy. Cambridge, England: Cambridge University Press.
5. (May 31, 2012) "Radiation". Wikipedia. San Francisco, California: Wikimedia Foundation, Inc. Retrieved on 2012-06-02.
6. Guido Alpa (1994). "General Principles of Law". Annual Survey of International & Comparative Law 1: 1. Retrieved on 2012-04-29.
7. (May 13, 2012) "Principle". Wikipedia. San Francisco, California: Wikimedia Foundation, Inc. Retrieved on 2012-06-07.
8. (September 26, 2012) "Meteoroid". Wikipedia. San Francisco, California: Wikimedia Foundation, Inc. Retrieved on 2012-09-30.
9. (October 5, 2012) "meteor". Wiktionary. San Francisco, California: Wikimedia Foundation, Inc. Retrieved on 2012-10-13.
10. S. Swordy (2001). "The energy spectra and anisotropies of cosmic rays". Space Science Reviews 99: 85–94.
11. The Pierre Auger Collaboration (November 2007). "Correlation of the Highest-Energy Cosmic Rays with Nearby Extragalactic Objects". Science 318 (5852): 938-43. doi:10.1126/science.1151124. Bibcode2007Sci...318..938T. Retrieved on 2011-11-24.
12. Open Questions in Physics. German Electron-Synchrotron. A Research Centre of the Helmholtz Association. Updated March 2006 by JCB. Original by John Baez.
13. (June 6, 2012) "Ultra-high-energy cosmic ray". Wikipedia. San Francisco, California: Wikimedia Foundation, Inc. Retrieved on 2012-06-07.
14. J. Walker (January 4, 1994). "The Oh-My-God Particle". Fourmilab.
15. Fargion D, Khlopov M, Konoplich R, De Sanctis Lucentini PG, De Santis M, Mele B (March 2003). "Ultra High Energy Particle Astronomy, Neutrino Masses and Tau Airshowers". Recent Research and Development in Astrophysics 1 (3): 395-454. Bibcode2003astro.ph..3233F.
16. Lingenfelter RE, Flamm EJ, Canfield EH, Kellman S (September 1965). "High-Energy Solar Neutrons 2. Flux at the Earth". Journal of Geophysical Research 70 (17): 4087–95. doi:10.1029/JZ070i017p04087. Bibcode1965JGR....70.4087L. Retrieved on 2011-11-25.
17. David R. Williams (November 2011). "Lunar Prospector Neutron Spectrometer (NS)". Goddard Space Flight Laboratory: National Aeronautics and Space Administration. Retrieved 2012-01-11.
18. Francis Halzen and Dan Hooper (July 2002). "High-energy neutrino astronomy: the cosmic ray connection". Reports on Progress in Physics 65 (7): 1025-78. doi:10.1088/0034-4885/65/7/201. Bibcode2002RPPh...65.1025H. Retrieved on 2011-11-24.
19. K. D. Hoffman (May 12, 2009). "High energy neutrino telescopes". New Journal of Physics 11 (5): 055006. doi:10.1088/1367-2630/11/5/055006. Retrieved on 2012-03-28.
20. Charles H. Jackman, Richard D. McPeters, Gordon J. Labow, Eric L.Fleming, Cid J. Praderas, James M. Russell (August 2001). "Northern Hemisphere atmospheric effects due to the July 2000 solar proton event". Geophysical Research Letters 28 (15): 2883-6. Retrieved on 2011-11-24.
21. (May 28, 2012) "Beta particle". Wikipedia. San Francisco, California: Wikimedia Foundation, Inc. Retrieved on 2012-06-08.
22. K. R. Schultz (September 1998). "Cost Effective Steps to Fusion power: IFE target fabrication, injection and tracking". Journal of Fusion Energy 17 (3): 237-46. doi:10.1023/A:1021814514091. Retrieved on 2012-06-08.
23. L. A. Rancitelli, R. W. Perkins, W. D. Felix, and N. A. Wogman (1971). "Erosion and mixing of the lunar surface from cosmogenic and primordial radio-nuclide measurements in Apollo 12 lunar samples". Proceedings of the Lunar Science Conference 2: 1757-72. Bibcode1971LPSC....2.1757R. Retrieved on 2012-06-08.
24. S. Wolpert (July 24, 2008). "Scientists solve 30-year-old aurora borealis mystery". University of California. Retrieved 2008-10-11.
25. H. S. Hudson and A. B. Galvin (September 1997). "Correlated Studies at Activity Maximum: the Sun and the Solar Wind, In: Correlated Phenomena at the Sun, in the Heliosphere and in Geospace": 275-82. Noordwijk, The Netherlands: European Space Agency. Bibcode1997ESASP.415..275H. Retrieved on 2011-11-25.
26. (July 26, 2012) "Delta ray". Wikipedia. San Francisco, California: Wikimedia Foundation, Inc. Retrieved on 2012-09-17.
27. T. H. Burnett et al.; The JACEE Collaboration (January 1990). "Energy spectra of cosmic rays above 1 TeV per nucleon". The Astrophysical Journal 349 (1): L25-8. doi:10.1086/185642. Bibcode1990ApJ...349L..25B. Retrieved on 2011-11-25.
28. P.A.Milne, J.D.Kurfess, R.L.Kinzer, M.D.Leising, D.D.Dixon (April 2000). "Investigations of positron annihilation radiation, In: Proceedings of the 5th COMPTON Symposium" 510 (4): 21-30. Washington, DC: American Institute of Physics. doi:10.1063/1.1303167. Bibcode2000AIPC..510...21M. Retrieved on 2011-11-25.
29. G. Weidenspointner, G.K. Skinner, P. Jean, J. Knödlseder, P. von Ballmoos, R. Diehl, A. Strong, B. Cordier, S. Schanne, C. Winkler (October 2008). "Positron astronomy with SPI/INTEGRAL". New Astronomy Reviews 52 (7-10): 454-6. doi:10.1016/j.newar.2008.06.019. Retrieved on 2011-11-25.
30. Gerald H. Share and Ronald J. Murphy (January 2004). Andrea K. Dupree, A. O. Benz. ed. Solar Gamma-Ray Line Spectroscopy – Physics of a Flaring Star, In: Stars as Suns: Activity, Evolution and Planets. San Francisco, CA: Astronomical Society of the Pacific. pp. 133-44. ISBN 158381163X. Bibcode: 2004IAUS..219..133S.
31. (May 23, 2012) "Neutrino detector". Wikipedia. San Francisco, California: Wikimedia Foundation, Inc. Retrieved on 2012-06-08.
32. (March 5, 2012) "Neutrino astronomy". Wikipedia. San Francisco, California: Wikimedia Foundation, Inc. Retrieved on 2012-06-08.
33. KENNETH CHANG (April 26, 2005). "Tiny, Plentiful and Really Hard to Catch". The New York Times. Retrieved 2011-06-16. "In 1987, astronomers counted 19 neutrinos from an explosion of a star in the nearby Large Magellanic Cloud, 19 out of the billion trillion trillion trillion trillion neutrinos that flew from the supernova."
34. (May 15, 2012) "Gamma-ray astronomy". Wikipedia. San Francisco, California: Wikimedia Foundation, Inc. Retrieved on 2012-09-17.
35. (June 27, 2012) "Vela (satellite)". Wikipedia. San Francisco, California: Wikimedia Foundation, Inc. Retrieved on 2012-09-17.
36. Vedrenne, G and Atteia, J.-L. (2009). Gamma-Ray Bursts: The brightest explosions in the Universe. Springer/Praxis Books. ISBN 978-3-540-39085-5.
37. (September 3, 2012) "Gamma-ray burst". Wikipedia. San Francisco, California: Wikimedia Foundation, Inc. Retrieved on 2012-09-17.
38. (June 2, 20102) "Ultraviolet astronomy". Wikipedia. San Francisco, California: Wikimedia Foundation, Inc. Retrieved on 2012-06-06.
39. Chung Chieh (December 1997). "Hydrogen Spectra". Waterloo, Ontario, Canada: University of Waterloo. Retrieved 2012-06-06.
40. Eric Hilbert (May 28, 2012). "Deep-Sky Wonders". State College, Pennsylvania: Starlight Astronomy Club. Retrieved 2012-06-06.
41. (June 29, 2009) "Optical astronomy". Wikipedia. San Francisco, California: Wikimedia Foundation, Inc. Retrieved on 2012-06-08.
42. (December 6, 2009) "optical astronomy". Wiktionary. San Francisco, California: Wikimedia Foundation, Inc. Retrieved on 2012-09-17.
43. "adaptive optics". Wiktionary. San Francisco, California: Wikimedia Foundation, Inc. Retrieved on 2012-09-17.
44. François Roddier, ed (1999). Adaptive Optics in Astronomy. Cambridge, United Kingdom: Cambridge University Press. pp. 411. ISBN 0 521 55375 X. Retrieved 2012-02-15.
45. David F. Gray (1992), The Inferred Color Index of the Sun, Publications of the Astronomical Society of the Pacific, vol. 104, no. 681, pp. 1035-1038 (November 1992)
46. (August 22, 2012) "Color index". Wikipedia. San Francisco, California: Wikimedia Foundation, Inc. Retrieved on 2012-09-17.
47. (September 14, 2012) "Telescope". Wikipedia. San Francisco, California: Wikimedia Foundation, Inc. Retrieved on 2012-09-17.
48. Antony Cooke (2005). Visual Astronomy Under Dark Skies: A New Approach to Observing Deep Space. London: Springer-Verlag. pp. 180. ISBN 1852339012. Retrieved 2011-11-06.
49. Cecie Starr (2005). Biology: Concepts and Applications. Thomson Brooks/Cole. ISBN 053446226X.
50. (September 15, 2012) "Visible spectrum". Wikipedia. San Francisco, California: Wikimedia Foundation, Inc. Retrieved on 2012-09-17.
51. T. Sivarani, P. Bonifacio, P. Molaro, R. Cayrel, M. Spite, F. Spite, B. Plez, J. Andersen, B. Barbuy, T. C. Beers, E. Depagne, V. Hill, P. François, B. Nordström, and F. Primas (January 2004). "First stars IV. CS 29497-030: Evidence for operation of the s-process at very low metallicity". Astronomy and Astrophysics 413 (1): 1073-85. doi:10.1051/0004-6361:20031590. Bibcode2004A&A...413.1073S. Retrieved on 2012-06-02.
52. Jesse D. Bregman and Joel N. Bregman (May 15, 1978). "The violet opacity of carbon stars". The Astrophysical Journal 222 (5): L41-3. doi:10.1086/182688. Bibcode1978ApJ...222L..41B. Retrieved on 2012-02-27.
53. W. H. Wright (August 1927). "Photographs of Venus made by Infra-red and by Violet Light". Publications of the Astronomical Society of the Pacific 39 (230): 220-1. doi:10.1086/123718. Bibcode1927PASP...39..220W. Retrieved on 2011-11-24.
54. Nathan Smith, Jon A. Morse, Nicholas R. Collins, and Theodore R. Gull (August 2004). "The Purple Haze of η Carinae: Binary-induced Variability?". The Astrophysical Journal 610 (2): L105-8. doi:10.1086/423341. Bibcode2004ApJ...610L.105S. Retrieved on 2012-01-08.
55. Preston, G. W.; Beers, T. C.; Shectman, S. A. (December 1993). "The Space Density and Kinematics of Metal-Poor Blue Main Sequence Stars Near the Solar Circle". Bulletin of the American Astronomical Society 25 (12): 1415. Bibcode1993BAAS...25Q1415P. Retrieved on 2011-11-24.
56. Klochkova, Valentina; Ermakov, Sergey; Panchuk, Vladimir; Zhao, Gang (July 2007). Ana I. Gómez de Castro and Martin A. Barstow. ed. High resolution spectroscopy of halo stars within the spectral region 3550-5000 °A°A, In: UV Astronomy: Stars from Birth to Death. Proceedings of the Joint Discussion n.4 during the IAU general Assembly of 2006. International Astronomical Union. pp. 161. ISBN 978-84-7491-852-6. Bibcode: 2007uasb.conf..161K.
57. Juna A. Kollmeier and Andrew Gould (July 20, 2007). "Where Are the Old-Population Hypervelocity Stars?". The Astrophysical Journal 664 (1): 343-8. doi:10.1086/518405. Retrieved on 2012-03-05.
58. Crisp, D.; Hammel, H. B. (June 14, 1995). "Hubble Space Telescope Observations of Neptune". Hubble News Center. Retrieved April 22, 2007.
59. Munsell, Kirk; Smith, Harman; Harvey, Samantha (November 13, 2007). "Neptune overview". Solar System Exploration. NASA. Retrieved February 20, 2008.
60. (June 1, 2012) "Neptune". Wikipedia. San Francisco, California: Wikimedia Foundation, Inc. Retrieved on 2012-06-08.
61. Jonathan I. Lunine (1993). "The Atmospheres of Uranus and Neptune". Annual Review of Astronomy and Astrophysics 31: 217–263. doi:10.1146/annurev.aa.31.090193.001245. Bibcode1993ARA&A..31..217L.
62. (June 5, 2012) "Uranus". Wikipedia. San Francisco, California: Wikimedia Foundation, Inc. Retrieved on 2012-06-08.
63. Wolfhard Schlosser, Rita Schulz, Paul Koczet (1986). The cyan shells of Comet P/Halley, In: Proceedings of the 20th ESLAB Symposium on the Exploration of Halley's Comet. 3. European Space Agency. pp. 495-8. Bibcode: 1986ESASP.250c.495S.
64. James A. Phillips (2009). "Green Comet Approaches Earth". National Aeronautics and Space Administration Science News. Retrieved 2012-05-05.
65. (May 4, 2012) "Electric blue (color)". Wikipedia. San Francisco, California: Wikimedia Foundation, Inc. Retrieved on 2012-06-08.
66. I. Bertini, N. Thomas, and C. Barbieri (January 2007). "Modeling of the light scattering properties of cometary dust using fractal aggregates". Astronomy & Astrophysics 461 (1): 351-64. doi:10.1051/0004-6361:20065461. Bibcode2007A&A...461..351B. Retrieved on 2011-12-08.
67. "The building blocks of planets within the `terrestrial' region of protoplanetary disks". nottingham.ac.uk. Retrieved 2008-03-04.
68. (August 28, 2012) "Stardust (spacecraft)". Wikipedia. San Francisco, California: Wikimedia Foundation, Inc. Retrieved on 2012-09-17.
69. Harold Zirin (March 1959). "Physical Conditions in Limb Flares and Active Prominences. II. a Remarkable Limb Flare, December 18, 1956". Astrophysical Journal 129 (3): 414-23. doi:10.1086/146633. Bibcode1959ApJ...129..414Z. Retrieved on 2011-08-01.
70. Rosaly MC Lopes (2006). "Io: The Volcanic Moon". In Lucy-Ann McFadden, Paul R. Weissman, Torrence V. Johnson. Encyclopedia of the Solar System. Academic Press. pp. 419–431. ISBN 978-0-12-088589-3.
71. Lopes, R. M. C.; et al. (2004). "Lava lakes on Io: Observations of Io’s volcanic activity from Galileo NIMS during the 2001 fly-bys". Icarus 169 (1): 140–174. doi:10.1016/j.icarus.2003.11.013. Bibcode2004Icar..169..140L.
72. (June 7, 2012) "Io (moon)". Wikipedia. San Francisco, California: Wikimedia Foundation, Inc. Retrieved on 2012-06-08.
73. Faber Birren (Summer 1983). "Color and human response". Color Research and Application 8 (2): 75-81. doi:10.1002/col.5080080204. Retrieved on 2012-04-23.
74. Elkins-Tanton, Linda T. (2006). Jupiter and Saturn. New York: Chelsea House. ISBN 0-8160-5196-8.
75. Strycker, P. D.; Chanover, N.; Sussman, M.; Simon-Miller, A. (2006). A Spectroscopic Search for Jupiter's Chromophores. American Astronomical Society. Bibcode: 2006DPS....38.1115S.
76. Gierasch, Peter J.; Nicholson, Philip D. (2004). "Jupiter". World Book @ NASA. Retrieved 2006-08-10.
77. (June 7, 2012) "Jupiter". Wikipedia. San Francisco, California: Wikimedia Foundation, Inc. Retrieved on 2012-06-08.
78. G. H. Herbig (March 1974). "VY Canis Majoris. IV. The emission bands of ScO". The Astrophysical Journal 188 (3): 533-8. doi:10.1086/152744. Bibcode1974ApJ...188..533H. Retrieved on 2012-02-01.
79. J. E. Littleton and Sumner P. Davis (October 1988). "Transition strength data for the orange and red bands of CaCl". The Astrophysical Journal 333 (10): 1026-34. doi:10.1086/166809. Bibcode1988ApJ...333.1026L. Retrieved on 2012-02-01.
80. F. P. Keenan and P. H. Norrington (July 1987). "Relative emission line strengths for Fe VII in astrophysical plasmas". Astronomy and Astrophysics 181 (2): 370-2. Bibcode1987A&A...181..370K. Retrieved on 2012-01-17.
81. M. Pim FitzGerald (February 1970). "The Intrinsic Colours of Stars and Two-Colour Reddening Lines". Astronomy and Astrophysics 4 (2): 234-43. Bibcode1970A&A.....4..234F. Retrieved on 2011-11-24.
82. (September 17, 2012) "Infrared astronomy". Wikipedia. San Francisco, California: Wikimedia Foundation, Inc. Retrieved on 2012-09-17.
83. (May 24, 2012) "Far-infrared astronomy". Wikipedia. San Francisco, California: Wikimedia Foundation, Inc. Retrieved on 2012-09-17.
84. (June 2, 2012) "Submillimetre astronomy". Wikipedia. San Francisco, California: Wikimedia Foundation, Inc. Retrieved on 2012-06-08.
85. BLAST Public Webpage
86. (February 4, 2012) "BLAST (telescope)". Wikipedia. San Francisco, California: Wikimedia Foundation, Inc. Retrieved on 2012-06-08.
87. (September 14, 2012) "Radio waves". Wikipedia. San Francisco, California: Wikimedia Foundation, Inc. Retrieved on 2012-09-17.
88. Pozar, David M. (1993). Microwave Engineering Addison-Wesley Publishing Company. ISBN 0-201-50418-9.
90. (September 10, 2012) "Microwave". Wikipedia. San Francisco, California: Wikimedia Foundation, Inc. Retrieved on 2012-09-17.
91. (May 29, 2012) "Faster-than-light". Wikipedia. San Francisco, California: Wikimedia Foundation, Inc. Retrieved on 2012-06-08.
92. Gonzalez-Diaz, P. F. (2000). "Warp drive space-time". Physical Review D 62 (4). doi:10.1103/PhysRevD.62.044005. Bibcode2000PhRvD..62d4005G.
93. F. Loup, David Waite, E. Halerewicz Jr. (2001). [ttp://arxiv.org/abs/gr-qc/0107097 "Reduced Total Energy Requirements for a Modified Alcubierre Warp Drive Spacetime"]. arXiv:gr-qc/0107097. Bibcode:2001gr.qc.....7097L.
94. (2000) "Superluminal censorship". Nuclear Physics B: Proceedings Supplement 88: 267–270. doi:10.1016/S0920-5632(00)00782-9. Bibcode2000NuPhS..88..267V.
95. (1999) "Perturbative superluminal censorship and the null energy condition". AIP Conference Proceedings 493: 301–305. doi:10.1063/1.1301601.
96. Roman Tomaschitz (March 2007). "Superluminal cascade spectra of TeV [gamma-ray sources]". Annals of Physics 322 (3): 677-700. doi:10.1016/j.aop.2006.11.005. Retrieved on 2011-11-24.
97. R Tomaschitz (October 2010). "Superluminal spectral densities of ultra-relativistic electrons in intense electromagnetic wave fields". Applied Physics B Lasers and Optics 101 (1-2): 143-64. doi:10.1007/s00340-010-4182-8. Retrieved on 2012-03-21.
98. M. H. Cohen, K. I. Kellermann, D. B. Shaffer, R. P. Linfield, A. T. Moffet, J. D. Romney, G. A. Seielstad, I. I. K. Pauliny-Toth, E. Preuss, A. Witzel, R. T. Schilizzi & B. J. Geldzahler (August 1977). "Radio sources with superluminal velocities". Nature 268: 405-9. doi:10.1038/268405a0. Bibcode1977Natur.268..405C. Retrieved on 2012-02-19.
99. (April 6, 2012) "Astrochemistry". Wikipedia. San Francisco, California: Wikimedia Foundation, Inc. Retrieved on 2012-06-08.
100. (June 2, 2012) "Ultraviolet astronomy". Wikipedia. San Francisco, California: Wikimedia Foundation, Inc. Retrieved on 2012-06-08.
101. (May 9, 2012) "Widmanstätten pattern". Wikipedia. San Francisco, California: Wikimedia Foundation, Inc. Retrieved on 2012-06-08.
102. (August 1, 2012) "High Energy Stereoscopic System". Wikipedia. San Francisco, California: Wikimedia Foundation, Inc. Retrieved on 2012-09-17.
103. (August 8, 2012) "Submillimetre astronomy". Wikipedia. San Francisco, California: Wikimedia Foundation, Inc. Retrieved on 2012-09-17.
104. David Brown (2000). Cuneiform Monographs 18: Mesopotamian Planetary Astronomy-Astrology. Groningen: Styx Publications. pp. 113-20.
105. Rolf Mewe (December 1996). "X-ray Spectroscopy of Stellar Coronae: History - Present - Future". Solar Physics 169 (2): 335-48. doi:10.1007/BF00190610. Bibcode1996SoPh..169..335M. Retrieved on 2011-10-16.
106. T. R. Burnight (1949). "Soft X-radiation in the upper atmosphere". Physical Review A 76: 165. Retrieved on 2011-10-16.
107. Pounds (1962). "A simple rocket-borne X-radiation monitor-its scope and results of an early flight". Monthly Notices of the Royal Astronomical Society 123: 347-57. Bibcode1962MNRAS.123..347P. Retrieved on 2011-10-16.
108. (May 10, 2012) "Infrared astronomy". Wikipedia. San Francisco, California: Wikimedia Foundation, Inc. Retrieved on 2012-06-08.
109. (June 3, 2012) "Radio astronomy". Wikipedia. San Francisco, California: Wikimedia Foundation, Inc. Retrieved on 2012-06-08.
110. (December 5, 2011) "Synchrotron function". Wikipedia. San Francisco, California: Wikimedia Foundation, Inc. Retrieved on 2012-05-14.
111. http://library.thinkquest.org/27954/dequ.htm
112. (June 19, 2012) "Radioanalytical chemistry". Wikipedia. San Francisco, California: Wikimedia Foundation, Inc. Retrieved on 2012-09-17.
113. (September 8, 2012) "Neutron activation". Wikipedia. San Francisco, California: Wikimedia Foundation, Inc. Retrieved on 2012-09-17.
114. (September 15, 2012) "Proton emission". Wikipedia. San Francisco, California: Wikimedia Foundation, Inc. Retrieved on 2012-09-17.
116. Loveland, W., Morrissey, D. J., Seaborg, G. T., Modern Nuclear Chemistry, 2006, John Wiley & Sons, 221.
117. Theodore E. Madey, Robert E. Johnson, Thom M. Orlando (March 2002). "Far-out surface science: radiation-induced surface processes in the solar system". Surface Science 500 (1-3): 838-58. doi:10.1016/S0039-6028(01)01556-4. Retrieved on 2012-02-09.
118. A. R. W. McKellar (November 1989). "The spectrum of gaseous methane at 77 K in the 1.1-2.6 μm region: a benchmark for planetary astronomy". Canadian Journal of Physics 67 (11): 1027-35. doi:10.1139/p89-180. Retrieved on 2012-02-09.
119. Steven J. Ostro (October-December 1993). "Planetary radar astronomy". Reviews of Modern Physics 65 (4): 1235-79. doi:10.1103/RevModPhys.65.1235. Retrieved on 2012-02-09.
120. Friedman H, Byram ET, Chubb TA (April 1967). "Distribution and Variability of Cosmic X-Ray Sources". Science 156 (3773): 374-8. doi:10.1126/science.156.3773.374. PMID 17812381. Retrieved on 2009-11-25.
121. Forman W, Jones C, Cominsky L, Julien P, Murray S, Peters G (December 1978). "The fourth Uhuru catalog of X-ray sources". The Astrophysical Journal Supplemental Series 38 (12): 357-412. doi:0.1086/190561. Bibcode1978ApJS...38..357F. Retrieved on 2009-10-11.
122. McHardy IM, Lawrence A, Pye JP, Pounds KA (December 1981). "The Ariel V /3 A/ catalogue of X-ray sources. II - Sources at high galactic latitude /absolute value of B greater than 10 deg/". Monthly Notices of the Royal Astronomical Society (MNRAS) 197: 893-919. Bibcode1981MNRAS.197..893M. Retrieved on 2010-01-10.
123. Loudon 2000, Chapter 1.
124. Mandel & Wolf 1995, Chapter 13.
125. Kondepudi & Prigogine 1998, Chapter 11.
126. Peter Theodore Landsberg (1990). "Chapter 13: Bosons: black-body radiation". Thermodynamics and statistical mechanics (Reprint of Oxford University Press 1978 ed.). Courier Dover Publications. pp. 208 ff. ISBN 0486664937.
127. (September 17, 2012) "Black-body radiation". Wikipedia. San Francisco, California: Wikimedia Foundation, Inc. Retrieved on 2012-09-17.
128. Electron microprobe analysis and scanning electron microscopy in geology, by S. J. B. Reed, 2005, page 12 [1]
129. (August 26, 2012) "Bremsstrahlung". Wikipedia. San Francisco, California: Wikimedia Foundation, Inc. Retrieved on 2012-09-17.
130. (August 30, 2012) "Cyclotron". Wikipedia. San Francisco, California: Wikimedia Foundation, Inc. Retrieved on 2012-09-17.
131. (May 28, 2012) "Cyclotron radiation". Wikipedia. San Francisco, California: Wikimedia Foundation, Inc. Retrieved on 2012-09-17.