User:Marshallsumter/Sources/Astronomy
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. It may have taken awhile to realize that the sky is penetrable.
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.
"Where did it come from?" is the question.
Answering this fundamental question is at the heart of source astronomy. Radiation incoming to the detector may have been altered just after it left the source, just before it arrived at the detector, or anywhere in between. Occasionally, contamination occurs within the detector that can produce spurious conclusions.
"What is the source?"
Minerals
edit"A time-dependent model of the solar nebula is used to describe the outward transport of hot mineral aggregates from locations in the warm inner regions of the nebula under the influence of photophoresis."[1]
Theoretical source astronomy
editDef. an entity from which something comes or is acquired is called a source.
Def. a source or apparent source detected or created at or near the time of the event or events is called a primary source.
Def. a source or apparent source that transforms or transduces anything originating from a primary source is called a secondary source.
Def. a source or apparent source that selects (such as through selective absorption), distills, scatters, or reflects anything from a primary or secondary source is called a tertiary source.
Def. the point of origin of a ray, beam, or stream of small cross section traveling in a line is called a radiation source.
"Def. a natural source in the sky especially at night is called an astronomical source.", after the definition of astronomical source in theoretical astronomy.
Early observations of origination, tracking, and recovery of entities are the proof of concept that entities falling from the sky have an origin or source.
Entities
editDef.
- 1.a: an "independent, separate, or self-contained [astronomical] existence",
- 1.b: "the [astronomical] existence of a thing as contrasted with its attributes", or
- 2. "some [astronomical] thing that has separate and distinct existence and objective or conceptual reality",[2]
is called an astronomical entity.
Skies
editDef. an "expanse of space that seems to be [overhead] like a dome"[2] is called the sky, or sometimes the heavens.
This definition applies especially well to an individual on top of the Earth's solid crust looking around at what lies above and off to the horizon in all directions. Similarly, it applies to an individual's visual view while floating on a large body of water, where off on the horizon is still water.
A more general definition of 'sky' allows for skies as seen on other worlds.
Is the sky a source or an obstruction between the observer and a source?
The same question may be asked when looking downward at the Earth's crust, regolith, or water below the observer.
The sky may have been thought of at one time as impenetrable. The same assumption may have occurred regarding the Earth below.
Is the sky a mirror?
The sky, also known as the celestial dome, commonly refers to everything that lies a certain distance above the surface of Earth, including the atmosphere and the rest of outer space. In the field of astronomy, the sky is also called the celestial sphere. This is an imaginary dome where the sun, stars, planets, and the moon are seen to be traveling. The celestial sphere is divided into regions called constellations. Usually, the term sky is used from the point of view of the Earth's surface. However, the exact meaning of the term can vary; in some cases, the sky is defined as only the denser portions of the atmosphere, for example.
Celestial spheres
editIn astronomy and navigation, the celestial sphere is an imaginary sphere of arbitrarily large radius, concentric with the Earth and rotating upon the same axis. All objects in the sky can be thought of as projected upon the celestial sphere. Projected upward from Earth's equator and poles are the celestial equator and the celestial poles. The celestial sphere is a very practical tool for positional astronomy.
The celestial sphere is divided into 89 areas. These are the International Astronomical Union (IAU) 88 modern constellations of astronomy. Although there are only 88 IAU constellations, the sky is actually divided into 89 irregularly shaped boxes as the constellation Serpens is split into two separate sections, Serpens Caput (the snake's head) to the west and Serpens Cauda (the snake's tail) to the east. From each of these areas of the celestial sphere, incoming radiation have been detected above the Earth's atmosphere and occasionally through it.
Celestial equators
editThe celestial equator (in hours of longitude) passes through these constellations (RA): Pisces (1), Cetus (~2), Taurus (4+), Eridanus (3-), Orion (5), Monoceros (7), Canis Minor (8), Hydra (8 to 15), Sextans (10), Leo (11), Virgo (13), Serpens (16,18), Ophiuchus (17), Aquila (20), and Aquarius (23).
Celestial poles
editIn the first diagram at right, the Earth is shown as seen from the Sun. The north and south celestial poles, their relation to the Earth's axis of rotation, the plane of the Earth's orbit around the Sun, and Earth's axial tilt are shown.
The second diagram at right shows the path of the celestial north pole around the ecliptic north pole. The beginning of the four "astrological ages" of the historical period are marked with their zodiacal symbols: the Age of Taurus from the Chalcolithic to the Early Bronze Age, the Age of Aries from the Middle Bronze Age to Classical Antiquity, the Age of Pisces from Late Antiquity to the present, and the Age of Aquarius beginning in the mid 3rd millennium.
The first image at left shows that over the course of an evening, stars appear to rotate about the north celestial pole when viewing in the northern hemisphere of Earth. Polaris, within a degree of the pole, is the single nearly-stationary star just to the right of the centre of this image.
The second image at left shows the star trails during the course of an evening around the south celestial pole as viewed from the southern hemisphere of Earth. The image shows these star rotations around the celestial South Pole over the Very Large Telescope.[3]
The third diagram at right shows how to locate the south celestial pole. Sigma Octantis is currently designated as the south celestial polar star.
Autumnal equinoxes
editThe vernal equinox is the point of equal Sun light and darkness (no Sun visible). Twelve hours occurs for each. The date is about March 22nd.
Ecliptics
editThe Earth in its orbit around the Sun causes the Sun to appear on the celestial sphere as moving along the ecliptic (red, in the diagram at right), which is tilted with respect to the celestial equator (blue-white).
The International Astronomical Union's constellations are shown at left in a equirectangular plot of declination vs right ascension of the modern constellations with a dotted line denoting the ecliptic. Constellations are colour-coded by family and year established. Note that the right ascension axis increases from right to left to approximate the view of the night sky.
Zodiacs
editThe Sun travels through the 13 constellations along the ecliptic, the 12 of the Zodiac and Ophiuchus.
№ | Symbol | Long. | Latin name | English translation | Greek name | Sanskrit name | Sumero-Babylonian name[4] |
---|---|---|---|---|---|---|---|
1 | ♈ | 0° | Aries | The Ram | Κριός (Krios) | Meṣha (मेष) | MUL LU.ḪUŊ.GA "The Agrarian Worker", Dumuzi |
2 | ♉ | 30° | Taurus | The Bull | Ταῦρος (Tavros) | Vṛiṣhabha (वृषभ) | MULGU4.AN.NA "The Steer of Heaven" |
3 | ♊ | 60° | Gemini | The Twins | Δίδυμοι (Didymoi) | Mithuna (मिथुन) | MULMAŠ.TAB.BA.GAL.GAL "The Great Twins" (Castor and Pollux) |
4 | ♋ | 90° | Cancer | The Crab | Καρκῖνος (Karkinos) | Karkaṭa (कर्कट) | MULAL.LUL "The Crayfish" |
5 | ♌ | 120° | Leo | The Lion | Λέων (Leōn) | Siṃha (सिंह) | MULUR.GU.LA "The Lion" |
6 | ♍ | 150° | Virgo | The Maiden | Παρθένος (Parthenos) | Kanyā (कन्या) | MULAB.SIN "The Furrow"; "The Furrow, the goddess Shala's ear of corn" |
7 | ♎ | 180° | Libra | The Scales | Ζυγός (Zygos) | Tulā (तुला) | MULZIB.BA.AN.NA "The Scales" |
8 | ♏ | 210° | Scorpio | The Scorpion | Σκoρπιός (Skorpios) | Vṛśhchika (वृश्चिक) | MULGIR.TAB "The Scorpion" |
9 | ♐ | 240° | Sagittarius | The (Centaur) Archer | Τοξότης (Toxotēs) | Dhanuṣha (धनुष) | MULPA.BIL.SAG, Nedu "soldier" |
10 | ♑ | 270° | Capricorn | "Goat-horned" (The Sea-Goat) | Αἰγόκερως (Aigokerōs) | Makara (मकर) | MULSUḪUR.MAŠ "The Goat-Fish" of Enki |
11 | ♒ | 300° | Aquarius | The Water-Bearer | Ὑδροχόος (Hydrokhoos) | Kumbha (कुम्भ) | MULGU.LA "The Great One", later qâ "pitcher" |
12 | ♓ | 330° | Pisces | The Fishes | Ἰχθύες (Ikhthyes) | Mīna (मीन) | MULSIM.MAḪ "The Tail of the Swallow", later DU.NU.NU "fish-cord" |
Constellations
editThe International Astronomical Union provides figures of each constellation and coordinates for the boundaries which can be used to determine the constellational location of a celestial object using its right ascension (RA) and declination (Dec). As the position of these constellations has shifted due to Earth orbit precessions, there is an approximate four minute increase between the right ascension boundaries of epoch 1950 B1950.0 and the most recent calibration of epoch 2000 J2000.0 and a few minutes of change in many declinations.
Milky Way
editThe center of the galaxy is in the direction of Sagittarius, and the Milky Way "passes" (going westward, Earthview, to the right) through Scorpius, Ara, Norma, Triangulum Australe, Circinus, Centaurus, Musca, Crux, Carina, Vela, Puppis, Canis Major, Monoceros, Orion & Gemini, Taurus, Auriga, Perseus, Andromeda, Cassiopeia, Cepheus & Lacerta, Cygnus, Vulpecula, Sagitta, Aquila, Ophiuchus, Scutum, and back to Sagittarius.
In the diagram at right, spherical triangles are shown for deriving the relationship between equatorial and galactic coordinate systems. The yellow plane is the celestial equator, P and P' are its celestial poles. The green plane is the galactic plane, G and G' are its galactic poles. B is the direction towards the galactic center, which is now used as a starting point for measuring galactic longitude. Prior to 1959, the starting point was the intersection of the galactic and equatorial planes (point C).
Quadrants
editIn the table of locations by quadrants that follows, ranges of RA, Dec are included, e.g. (23-02, +23 to +52), to help make a fast assessment whether a particular source is in or borders a specific constellation. Questionable locations near a border require consulting the IAU website.
Quadrant | Total Number of Constellations | Constellation | Right ascension range | Declination range |
---|---|---|---|---|
NQ1 | 08 | Pisces | 23 to 02 | -26 to +30 |
--- | --- | Andromeda | 23 to 02 | +23 to +52 |
--- | --- | Cassiopeia | 23 to 03 | +47 to +75 |
--- | --- | Triangulum | 01 to 02 | +27 to +36 |
--- | --- | Aries | 01 to 03 | +10 to +31 |
--- | --- | Perseus | 01.5 to 04.8 | +31 to +59 |
--- | --- | Taurus | 23 to 02 | +23 to +52 |
--- | --- | Orion | 04 to 06 | -9 to +20 |
NQ2 | 10 | Auriga | 04 to 07 | +28 to +55 |
--- | --- | Monoceras | 05.9 to 08.3 | -11 to +12 |
--- | --- | Gemini | 06 to 07 | +12 to +35 |
--- | --- | Canis Minor | 07 to 08 | +00 to +12 |
--- | --- | Lynx | 06 to 09 | +34 to +61 |
--- | --- | Cancer | 07 to 09 | +07 to +32 |
--- | --- | Camelopardalis | 03 to 14.5 | +53 to +87 |
--- | --- | Leo Minor | 09 to 11 | +23 to +41 |
--- | --- | Leo | 09 to 11 | -04 to +29 |
--- | --- | Ursa Major | 08 to 13 | +31 to +70 |
NQ3 | 08 | Coma Berenices | 12 to 13.6 | +12 to +34 |
--- | --- | Canes Venatici | 12 to 14 | +31 to +51 |
--- | --- | Boötes | 13 to 15 | +07 to +54 |
--- | --- | Ursa Minor | 00 to 23 | +65 to +90 |
--- | --- | Draco | 09 to 21 | +48 to +86 |
--- | --- | Corona Borealis | 15 to 16 | +26 to +39 |
--- | --- | Serpens cauda | 17.2 to 19 | -16 to +07 |
--- | --- | Serpens caput | 15.2 to 16.4 | -4 to +25 |
--- | --- | Hercules | 15.8 to 19 | +4 to +52 |
NQ4 | 10 | Lyra | 18h 13m to 19h 27m | +25.66 to +47.70 |
--- | --- | Sagitta | 18.9 to 20.5 | +16 to +22 |
--- | --- | Aquila | 18h 41m to 20h 38m | -11.86 to +16.49 |
--- | --- | Vulpecula | 18.9 to 21.5 | +19 to +30 |
--- | --- | Cygnus | 19.1 to 22.1 | +28 to +62 |
--- | --- | Delphinus | 20h 19m to 21h 07m | +02 to +20 |
--- | --- | Equuleus | 20h 59m to 21h 25m | +02 to +11 |
--- | --- | Cepheus | 20 to 09 | +53 to +88 |
--- | --- | Lacerta | 21.9 to 23 | +35 to +57 |
--- | --- | Pegasus | 21 to 00 | +02 to +35 |
SQ1 | 14 | Sculptor | 23 to 01 | -25 to -38 |
--- | --- | Phoenix | 23.5 to 02.5 | -39 to -58 |
--- | --- | Cetus | 23.9 to 03.4 | -24 to +11 |
--- | --- | Hydrus | 0.08 to 04.66 | -58 to -82 |
--- | --- | Fornax | 01 to 03 | -23 to -38 |
--- | --- | Horologium | 02 to 04 | -40 to -66 |
--- | --- | Eridanus | 01 to 05 | -57 to +00 |
--- | --- | Reticulum | 03 to 04 | -25 to -66 |
--- | --- | Caelum | 04 to 05 | -30 to -46 |
--- | --- | Dorado | 3.8 to 6.6 | -48 to -70 |
--- | --- | Mensa | 03 to 07.5 | -70 to -85.5 |
--- | --- | Lepus | 05 to 06 | -11 to -27 |
--- | --- | Pictor | 4.6 to 7.9 | -43 to -64 |
--- | --- | Columba | 05 to 06 | -27 to -42 |
SQ2 | 11 | Canis Major | 6 to 7 | -11 to -32 |
--- | --- | Puppis | 06 to 08.4 | -11 to -51 |
--- | --- | Volans | 06.5 to 09 | -64 to -75 |
--- | --- | Carina | 06 to 11 | -51 to -74 |
--- | --- | Pyxis | 08 to 09 | -19 to -37 |
--- | --- | Vela | 8.1 to 11.1 | -37 to -56 |
--- | --- | Sextans | 9.7 to 10.8 | -8 to +06 |
--- | --- | Antlia | 09 to 11 | -25 to -40 |
--- | --- | Chamaeleon | 07 to 13 | -75 to -82 |
--- | --- | Crater | 10 to 11 | -7 to -24 |
--- | --- | Hydra | 08 to 15 | -35 to +06 |
SQ3 | 14 | Corvus | 11 to 12 | -11 to -24 |
--- | --- | Crux | 11 to 12 | -55 to -64 |
--- | --- | Musca | 11 to 13 | -64 to -75 |
--- | --- | Centaurus | 11h 05m to 15h 03m | -30.19 to -64.70 |
--- | --- | Virgo | 11h 37m to 15h 11m | -22.68 to +14.36 |
--- | --- | Circinus | 13h 38m to 15h 30m | -55.43 to -70.62 |
--- | --- | Libra | 14h 21m to 16h 02m | -0.47 to -29.99 |
--- | --- | Lupus | 14h 17m to 16h 08m | -29.83 to -55.58 |
--- | --- | Norma | 15h 12m to 16h 36m | -42.27 to -60.44 |
--- | --- | Triangulum Australe | 14h 56m to 17h 13m | -60.26 to -70.51 |
--- | --- | Apus | 14 to 18 | -67 to -82 |
--- | --- | Scorpius | 15h 47m to 17h 59m | -8.29 to -45.77 |
--- | --- | Ara | 16h 36m to 18h 10m | -45.48 to -67.69 |
--- | --- | Ophiuchus | 16 to 18.8 | -30 to +14 |
SQ4 | 13 | Corona Australis | 18 to 19 | -36 to -45 |
--- | --- | Scutum | 18.3 to 19 | -15 to -04 |
--- | --- | Sagittarius | 17.8 to 20.5 | -45 to -12 |
--- | --- | Telescopium | 18 to 20 | -45 to -56 |
--- | --- | Pavo | 17 to 21 | -56 to -73 |
--- | --- | Microscopium | 20.5 to 21.5 | -45 to -27 |
--- | --- | Capricornus | 20 to 21 | -9 to -26 |
--- | --- | Indus | 20 to 23 | -45 to -70 |
--- | --- | Piscis Austrinus | 21 to 23 | -25 to -34 |
--- | --- | Aquarius | 20 to 23 | -24 to +02 |
--- | --- | Grus | 21 to 23 | -36 to -53 |
--- | --- | Octans | 23 to 00 | -75 to -90 |
--- | --- | Tucana | 22 to 01 | -56 to -79 |
Andromeda
editThe figure at right shows the sky map of Andromeda. Around the edges of the map are coordinates related to longitude and latitude.
Antlia
editThe figure at right shows the sky map of Antlia. Around the edges of the map are coordinates related to longitude and latitude.
Right ascension in hours (h) minutes (m) seconds (s) | Declination in degrees |
---|---|
09 27 37.0404 | -24.5425186 |
09 27 05.1837 | -37.2920151 |
09 26 56.1747 | -40.2918739 |
11 05 49.5611 | -40.4246216 |
11 05 55.0471 | -35.6746559 |
10 55 50.0437 | -35.6664963 |
10 55 54.6924 | -31.8332005 |
10 40 48.3309 | -31.8185863 |
10 40 51.0945 | -29.8186131 |
10 20 43.5185 | -29.7947845 |
10 20 47.8410 | -27.1281624 |
09 50 38.2279 | -27.0835037 |
09 50 43.1235 | -24.5835705 |
Apus
editThe figure at right shows the sky map of Apus. Around the edges of the map are coordinates related to longitude and latitude.
Aquarius
editThe figure at right shows the sky map of Aquarius. Around the edges of the map are coordinates related to longitude and latitude.
Aquila
editThe figure at right shows the sky map of Aquila. Around the edges of the map are coordinates related to longitude and latitude.
Ara
editThe diagram at right is the International Astronomical Union's official sky chart for the constellation Ara with notable sources marked and located.
At left is a three-colors image of NGC 6193 and NGC 6188 obtained with the Curtis-Schmidt telescope at Cerro Tololo Inter-American Observatory (Chile). The red channel is ionized Sulfur, green channel ionized Hydrogen, and the blue channel is double ionized Oxygen.
Aries
editAt left is the sky chart of the constellation Aries from the IAU.
Auriga
editAt right is a map of the constellation Auriga, with the surrounding constellations shaded in gray. Vertical coordinates are in declination while horizontal coordinates are right ascension. The green lines outline the constellation's conventional asterism, while the black dots show the location and apparent magnitude of the visible naked eye stars. The heavy blue line bisecting the constellation represents the Galactic Plane of the Milky Way. The lighter blue line to the south of the constellation is the ecliptic.
At left in the near infrared is the planetary nebula IC 2419 in Auriga.
Boötes
editThe figure at right shows the sky map of Boötes. Around the edges of the map are coordinates related to longitude and latitude.
Caelum
editThe figure at right shows the sky map of Caelum. Around the edges of the map are coordinates related to longitude and latitude.
Camelopardalis
editThe official IAU sky chart for the constellation Camelopardalis is at right with notable sources marked and located.
"A bright star [in the image at left] is surrounded by a tenuous shell of gas in this unusual image from the NASA/ESA Hubble Space Telescope. U Camelopardalis, or U Cam for short, is a star nearing the end of its life. As it begins to run low on fuel, it is becoming unstable. Every few thousand years, it coughs out a nearly spherical shell of gas as a layer of helium around its core begins to fuse. The gas ejected in the star’s latest eruption is clearly visible in this picture as a faint bubble of gas surrounding the star."[5]
"U Cam is an example of a carbon star. This is a rare type of star whose atmosphere contains more carbon than oxygen. Due to its low surface gravity, typically as much as half of the total mass of a carbon star may be lost by way of powerful stellar winds."[5]
"Located in the constellation of Camelopardalis (The Giraffe), near the North Celestial Pole, U Cam itself is actually much smaller than it appears in Hubble’s picture. In fact, the star would easily fit within a single pixel at the centre of the image. Its brightness, however, is enough to overwhelm the capability of Hubble’s Advanced Camera for Surveys making the star look much bigger than it really is. The shell of gas, which is both much larger and much fainter than its parent star, is visible in intricate detail in Hubble’s portrait. While phenomena that occur at the ends of stars’ lives are often quite irregular and unstable (see for example Hubble’s images of Eta Carinae, potw1208a), the shell of gas expelled from U Cam is almost perfectly spherical."[5]
"The image was produced with the High Resolution Channel of the Advanced Camera for Surveys [using the 606 nm and 814 nm filters]."[5]
Cancer
editThe figure at right shows the sky map of Cancer. Around the edges of the map are coordinates related to longitude and latitude.
Canes Venatici
editAt right is the IAU official sky chart for the constellation Canes Venatici with notable sources marked and located.
The left image is of the Whale galaxy [NGC 4631] in Canes Venatici. The image is a visual record using a backyard telescope. For comparison an ultraviolet image is just below it from the GALEX satellite.
Canis Major
editThe figure at right shows the sky map of Canis Major. Around the edges of the map are coordinates related to longitude and latitude.
Canis Major [...] is one of the 88 modern constellations, and was included in the 2nd-century astronomer Ptolemy's 48 constellations. [...] Canis Major is a constellation in the southern hemisphere's summer (or northern hemisphere's winter) sky [...] The three-letter abbreviation for the constellation, as adopted by the International Astronomical Union in 1922, is 'CMa'.[6] The official constellation boundaries, as set by Eugène Delporte in 1930, are defined by a polygon of 4 sides. In the equatorial coordinate system, the right ascension coordinates of these borders lie between 06h 12.5m and 07h 27.5m, while the declination coordinates are between -11.03° and −33.25°.[7] Covering 380 square degrees, it ranks 43rd of the 88 constellations in size.
At left is a visual image of Sirius, the brightest star as seen from Earth, apart from the Sun.
Around 150 AD, the Hellenistic astronomer Claudius Ptolemy described Sirius as reddish, along with five other stars, Betelgeuse, Antares, Aldebaran, Arcturus and Pollux, all of which are clearly of orange or red hue.[8] The discrepancy was first noted by amateur astronomer Thomas Barker, ... who prepared a paper and spoke at a meeting of the Royal Society in London in 1760.[9] The existence of other stars changing in brightness gave credence to the idea that some may change in colour too; Sir John Herschel noted this in 1839, possibly influenced by witnessing Eta Carinae two years earlier.[8] Thomas Jefferson Jackson See resurrected discussion on red Sirius with the publication of several papers in 1892, and a final summary in 1926.[8] He cited not only Ptolemy but also the poet Aratus, the orator Cicero, and general Germanicus as colouring the star red, though acknowledging that none of the latter three authors were astronomers, the last two merely translating Aratus' poem Phaenomena.[8] Seneca, too, had described Sirius as being of a deeper red colour than Mars.[10] However, not all ancient observers saw Sirius as red. The 1st century AD poet Marcus Manilius described it as "sea-blue", as did the 4th century Avienus.[8] It is the standard star for the color white in ancient China, and multiple records from the 2nd century BC up to the 7th century AD all describe Sirius as white in hue.[11][12]
In 1985, German astronomers Wolfhard Schlosser and Werner Bergmann published an account of an 8th century Lombardic manuscript, which contains De cursu stellarum ratio by St. Gregory of Tours. The Latin text taught readers how to determine the times of nighttime prayers from positions of the stars, and Sirius is described within as rubeola — "reddish". The authors proposed this was further evidence Sirius B had been a red giant at the time.[13]
Canis Minor
editAt left is the International Astronomical Union official sky chart for the constellation Canis Minor with notable sources marked and located.
The right image is from the Hubble Space Telescope of a region that includes Orion at the right, Monoceras, Canis Major, and Canis Minor. Located within this region is the Cone Nebula.
Capricornus
editAt right is the IAU sky chart for Capricornus with the notable sources marked and located.
The left image is of the solar twin HIP 102152, "a star located 250 light-years from Earth in the constellation of Capricornus (The Sea Goat)."[14]
"HIP 102152 is more like the Sun than any other solar twin — apart from the fact that it is nearly four billion years older, giving us an unprecedented chance to study how the Sun will look when it ages. It is the oldest solar twin identified to date, and was studied by an international team using ESO’s Very Large Telescope, led by astronomers in Brazil."[14]
"The different colours of the star are caused by the star moving slightly between the two exposures, many years apart."[14]
Carina
editAt left is the IAU sky chart for the constellation Carina with notable sources located.
"NGC 3199, in the constellation Carina, [...] is the wind-blown partial "ring" around the Wolf-Rayet (W-R) star WR 18 (aka HD 89358), the easternmost (leftmost) of the three bright blue stars near the center of the 2MASS image. NGC 3199 and WR 18 are at a distance of about 3.6 kpc (11,736 light years) from us. W-R stars represent the final evolutionary stages of very massive stars (with ~30 solar masses or greater). The nebula shows an asymmetric appearance, i.e., only one side (the western one) of the shell is bright, both in the optical and the near-infrared. The fainter, eastern side is there, but is much fainter. Some W-R ring nebulae can be seen in 2MASS images, such as the more complete ring around M1-67. But, NGC 3199 is particularly bright in the 2MASS data. Dyson & Ghanbari (1989, A&A, 226, 270) provided an explanation for the ring's appearance through a model where a moving WR 18 is blowing a strong stellar wind into a surrounding uniform interstellar medium. Vigorous mass loss of 10-5 to 10-4 solar masses per year is characteristic of W-R stars, as the star approaches the end of its short life, although not all are surrounded by ring nebulae."[15]
Cassiopeia
editAt right is a sky chart for the constellation Cassiopeia from the IAU where notable sources are indicated and located.
"This spectacular image [at left] of the supernova remnant Cassiopeia A is the most detailed image ever made of the remains of an exploded star. The one-million-second image shows a bright outer ring (green) ten light years in diameter that marks the location of a shock wave generated by the supernova explosion. A large jet-like structure that protrudes beyond the shock wave can be seen in the upper left. In the accompanying image, specially processed to highlight silicon ions, a counter-jet can be seen on the lower right."[16]
"Surprisingly, the X-ray spectra show that the jet and counter-jet are rich in silicon atoms and relatively poor in iron atoms. This indicates that the jets formed soon after the initial explosion of the star; otherwise, the jets should have contained large quantities of iron from the star's central regions."[16]
"The bright blue fingers located near the shock wave on the lower left are composed almost purely of iron gas. This iron was produced in the central, hottest regions of the star and somehow ejected in a direction almost perpendicular to the jets."[16]
"The bright source at the center of the image is presumed to be a neutron star created during the supernova. Unlike the rapidly rotating neutron stars in the Crab Nebula and Vela supernova remnants that are surrounded by dynamic magnetized clouds of electrons called pulsar wind nebulas, this neutron star is quiet, faint, and so far shows no evidence for pulsed radiation."[16]
"A working hypothesis is that the explosion that created Cassiopeia A produced high-speed jets similar to but less energetic than the hypernova jets thought to produce gamma-ray bursts. During the explosion, the neutron star may have developed an extremely strong magnetic field that helped to accelerate the jets. This strong magnetic field later stifled any pulsar wind activity, so the neutron star today resembles other strong-field neutron stars (a.k.a. "magnetars") in lacking a pulsar wind nebula."[16]
Centaurus
editThe sky chart for the constellation Centaurus is at right with notable sources indicated and located.
"This image [at left] of the planetary nebula SuWt 2 reveals a bright ring-like structure encircling a bright central star. The central star is actually a close binary system where two stars completely circle each other every five days. The interaction of these stars and the more massive star that sheds material to create the nebula formed the ring structure. The burned out core of the massive companion has yet to be found inside the nebula. The nebula is located 6,500 light-years from Earth in the direction of the constellation Centaurus. This color image was taken on Jan. 31, 1995 with the National Optical Astronomy Observatory's 1.5-meter telescope at the Cerro Tololo Inter-American Observatory in Chile."[17]
The second lower image at left is the Boomerang nebula.
"The Boomerang Nebula is a young planetary nebula and the coldest object found in the Universe so far. The NASA/ESA Hubble Space Telescope image is yet another example of how Hubble's sharp eye reveals surprising details in celestial objects."[18]
"This NASA/ESA Hubble Space Telescope image shows a young planetary nebula known (rather curiously) as the Boomerang Nebula. It is in the constellation of Centaurus, 5000 light-years from Earth. Planetary nebulae form around a bright, central star when it expels gas in the last stages of its life."[18]
"The Boomerang Nebula is one of the Universe's peculiar places. In 1995, using the 15-metre Swedish ESO Submillimetre Telescope in Chile, astronomers Sahai and Nyman revealed that it is the coldest place in the Universe found so far. With a temperature of -272C, it is only 1 degree warmer than absolute zero (the lowest limit for all temperatures). Even the -270C background glow from the Big Bang is warmer than this nebula. It is the only object found so far that has a temperature lower than the background radiation."[18]
"Keith Taylor and Mike Scarrott called it the Boomerang Nebula in 1980 after observing it with a large ground-based telescope in Australia. Unable to see the detail that only Hubble can reveal, the astronomers saw merely a slight asymmetry in the nebula's lobes suggesting a curved shape like a boomerang. The high-resolution Hubble images indicate that 'the Bow tie Nebula' would perhaps have been a better name."[18]
"The Hubble telescope took this image in 1998. It shows faint arcs and ghostly filaments embedded within the diffuse gas of the nebula's smooth 'bow tie' lobes. The diffuse bow-tie shape of this nebula makes it quite different from other observed planetary nebulae, which normally have lobes that look more like 'bubbles' blown in the gas. However, the Boomerang Nebula is so young that it may not have had time to develop these structures. Why planetary nebulae have so many different shapes is still a mystery."[18]
"The general bow-tie shape of the Boomerang appears to have been created by a very fierce 500 000 kilometre-per-hour wind blowing ultracold gas away from the dying central star. The star has been losing as much as one-thousandth of a solar mass of material per year for 1500 years. This is 10-100 times more than in other similar objects. The rapid expansion of the nebula has enabled it to become the coldest known region in the Universe."[18]
"The image was exposed for 1000 seconds through a green-yellow filter. The light in the image comes from starlight from the central star reflected by dust particles."[18]
Cepheus
editStarting at the right is the IAU sky chart for the constellation Cepheus.
Two astronomical entities are shown in the images at left: the supernova remnant CTA 1 and the Natal Microcosm, the latter is an image from the Spitzer space telescope.
Cetus
editThe constellation Cetus is charted by the IAU in the diagram at left.
At right the Chandra X-ray Observatory has confirmed that β Ceti is an X-ray source.
Chamaeleon
editThe IAU sky chart for the constellation Chamaeleon is at right with notable sources indicated and located.
At left is a ROSAT PSPC false-color image of the Chamaeleon I dark cloud, a well-known site of star formation. The contours show the 100 micron emission from dust in this cloud as measured by the infrared IRAS satellite. This image was made from X-rays with energies between 500 eV and 1100 eV. Since these soft (low energy) X-rays are absorbed by interstellar dust and gas, the observation of a "shadow" provides an indication of the intensity of X-rays coming from behind the absorbing cloud. X-ray "shadows" like this are the X-ray analog of well-known optical dark nebulae such as the Horsehead Nebula, produced by absorption in a dark cloud of optical photons emitted in a bright nebula behind the cloud. In the X-ray case, the entire sky is bright with a diffuse glow known as the diffuse X-ray background (somewhat like the night sky as seen from a modern city, where scattered light from street lamps produces a bright glow in the sky and washes out all but the brightest stars). Observations like this will help us understand the source of the diffuse X-ray background at these energies.
Circinus
editMano de Dios is shown at right in the constellation Circinus, sky chart at left.
Columba
editThe center of NGC 1808 is imaged at left with the Hubble Space Telescope. The galaxy occurs in the constellation Columba whose sky chart is at right.
Coma Berenices
editThe GALEX ultraviolet observatory has imaged the NGC 4793 galaxy (at right) in Coma Berenices. The IAU chart for the constellation Coma Berenices is at left.
Corona Australis
edit"The star R Coronae Australis [in the image at right] lies in one of the nearest and most spectacular star-forming regions. This portrait was taken by the Wide Field Imager (WFI) on the MPG/ESO 2.2-metre telescope at the La Silla Observatory in Chile. The image is a combination of twelve separate pictures taken through red, green and blue filters."[19]
Corona Australis is the constellation charted in the diagram at left.
Corona Borealis
editThe IAU chart for the constellation Corona Borealis is at left. Abell 2142 is an object in Corona Borealis.
Corvus
editThe IAU sky chart for the constellation Corvus is at right.
“This NASA Hubble Space Telescope image of the Antennae galaxies (NGC 4038 & 4039) is the sharpest yet of this merging pair of galaxies. During the course of the collision, billions of stars will be formed. The brightest and most compact of these star birth regions are called super star clusters.”[20]
Crater
editThe International Astronomical Union sky chart for the constellation Crater is at left. Notable sources are located and identified.
Crux
editThe constellation Crux has borders determined by the IAU and embodied at right in their sky chart.
Cygnus
editThe IAU sky chart for the constellation Cygnus is at left and includes the currently accepted boundaries.
Delphinus
editThe IAU has included the currently accepted boundaries for the constellation Delphinus in their sky chart.
Dorado
editAt left is the IAU sky chart for the constellation Dorado.
Draco
editThe IAU sky chart for the constellation Draco is at right. Notable sources are identified and located.
Equuleus
editAt left is the IAU sky chart for the constellation Equuleus. Notable sources are located and named.
Eridanus
editThe sky chart for the constellation Eridanus is at right.
Fornax
editThe sky chart for the constellation Fornax from the IAU is on the left.
Gemini
editAt right is the IAU sky chart for the constellation Gemini with notable sources marked.
At left is a multiwavelength composite that shows the supernova remnant IC 443, also known as the Jellyfish Nebula. Fermi GeV gamma-ray emission is shown in magenta, optical wavelengths as yellow, and infrared data from NASA's Wide-field Infrared Survey Explorer (WISE) mission is shown as blue (3.4 microns), cyan (4.6 microns), green (12 microns) and red (22 microns). Cyan loops indicate where the remnant is interacting with a dense cloud of interstellar gas.
Grus
editGrus is a constellation that has notable sources as shown on the sky chart of the IAU at right.
Hercules
editAt left is the IAU sky chart for the constellation Hercules.
Horologium
editAt right is the IAU sky chart for the constellation Horologium.
Hydra
editThe constellation Hydra is close to the ecliptic as shown on the IAU sky chart at right.
Hydrus
editThe notable sources in the constellation Hydrus are shown in the image at left.
Indus
editThe IAU sky chart for the constellation Indus is at left.
Lacerta
editThe sky chart for the constellation Lacerta is shown at right.
Leo
editAt left is the sky chart for the constellation Leo.
Leo Minor
editThe sky chart for the constellation Leo Minor is at the right.
Lepus
editThe constellation Lepus is at left with its notable sources located and indicated.
Libra
editAt right is the IAU sky chart for the constellation Libra.
Lupus
editLynx
editLyra
editMensa
editMicroscopium
editMonoceros
editMusca
editNorma
editOctans
editOphiuchus
editOrion
editAt right is the IAU sky chart for Orion with notable sources indicated.
At left is Abell 520, the "Train Wreck" cluster. The composite view shows inferred mass, visible light and X-ray.
Pavo
editPegasus
editPerseus
editAt right is the IAU Perseus chart.
At left, baby stars are forming near the eastern rim of the cosmic cloud Perseus, in this infrared image from NASA's Spitzer Space Telescope.
The baby stars are approximately three million years old and are shown as reddish-pink dots to the right of the image. The pinkish color indicates that these infant stars are still shrouded by the cosmic dust and gas that collapsed to form them. These stars are part of the IC348 star cluster, which consists of over 300 known member stars.
The Perseus Nebula can be seen as the large green cloud at the center of the image. Wisps of green are organic molecules called Polycyclic Aromatic Hydrocarbons (PAHs) that have been illuminated by the nearby star formation. Meanwhile, wisps of orange-red are dust particles warmed by the newly forming stars.
The Perseus Nebula is located about 1,043 light-years away in the Perseus constellation.
The image is a three channel false color composite, where emission at 4.5 microns is blue, emission at 8.0 microns is green, and 24-micron emission is red.
Phoenix
editPictor
editPisces
editPiscis Austrinus
editPuppis
editPyxis
editReticulum
editSagitta
editSagittarius
editScorpius
editSculptor
editAt left is the International Astronomical Union sky chart for the constellation Sculptor.
On the right is a visual image of the Sculptor Dwarf Galaxy.
Scutum
editSerpens Caput
editAt right is the IAU sky chart for the constellation Serpens Caput with notable sources marked.
At left is a Hubble Space Telescope image of Seyfert's Sextet in Serpens Caput. "The NASA/ESA Hubble Space Telescope is witnessing a grouping of galaxies engaging in a slow dance of destruction that will last for billions of years. The galaxies are so tightly packed together that gravitational forces are beginning to rip stars from them and distort their shapes. Those same gravitational forces eventually could bring the galaxies together to form one large galaxy."[21]
"The name of this grouping, Seyfert's Sextet, implies that six galaxies are participating in the action. But only four galaxies are on the dance card. The small face-on spiral with the prominent arms [center] of gas and stars is a background galaxy almost five times farther away than the other four. Only a chance alignment makes it appear as if it is part of the group. The sixth member of the sextet isn't a galaxy at all but a long 'tidal tail' of stars [below, right] torn from one of the galaxies."[21]
Serpens Cauda
editThe constellation Serpens is split into two separate sections, Serpens Caput (the snake's head) to the west and Serpens Cauda (the snake's tail) to the east. The constellation Ophiuchus is between them.
Sextans
editTaurus
editAt right is the IAU sky chart for the constellation Taurus. Legend: red oval - Galaxy, yellow circle - Open star cluster, yellow circle with vertical cross-hairs - Globular cluster, green circle inside cross-hairs - Planetary nebula, green square - Bright nebula, black circle - Star, open circle - Variable star.
At left is an APEX telescope image of part of the Taurus Molecular Cloud. It shows a sinuous filament of cosmic dust more than ten light-years long. In it, newborn stars are hidden, and dense clouds of gas are on the verge of collapsing to form yet more stars. The cosmic dust grains are so cold that observations at submillimetre wavelengths, such as these made by the LABOCA camera on APEX, are needed to detect their faint glow. This image shows two regions in the cloud: the upper-right part of the filament shown here is Barnard 211, while the lower-left part is Barnard 213. The submillimetre-wavelength observations from the LABOCA camera on APEX, which reveal the heat glow of the cosmic dust grains, are shown here in orange tones. They are superimposed on a visible-light image of the region, which shows the rich background of stars. The bright star above the filament is φ Tauri.
Telescopium
editTriangulum
editTriangulum Australe
editThe figure at right shows the sky map of Triangulum Australe. Around the edges of the map are coordinates related to longitude and latitude, but with the Earth rotating on its axis every 24 hours the celestial coordinates must remain fixed relative to the background light sources in the sky.
"The galaxies of this beautiful interacting pair [on the left] bear some resemblance to musical notes on a stave. Long tidal tails sweep out from the two galaxies: gas and stars were stripped out and torn away from the outer regions of the galaxies. The presence of these tails is the unique signature of an interaction. ESO 69-6 is located in the constellation of Triangulum Australe, the Southern Triangle, about 650 million light-years away from Earth."[22]
Tucana
editUrsa Major
editUrsa Minor
editVela
editVirgo
editThe Virgo Supercluster is on the left.
Volans
editVolans is one of the 12 constellations that were introduced by the Dutch navigators Pieter Dirkszoon Keyser and Frederick de Houtman in the late 16th century. It was first depicted on Petrus Plancius’ globe in 1598. Plancius called the constellation Vliegendenvis (flying fish).[23]
Vulpecula
editAbout 4000 years old and at 1200 ly distant, the Dumbbell nebula on the left is brightened by a very hot star (85,000 K).
Weather
editWeather is the state of the atmosphere, to the degree that it is hot or cold, wet or dry, calm or stormy, clear or cloudy.[24] Most weather phenomena occur in the troposphere,[25][26] just below the stratosphere. Weather refers, generally, to day-to-day temperature and precipitation activity, whereas climate is the term for the average atmospheric conditions over longer periods of time.[27]
On Earth, common weather phenomena include wind, cloud, rain, snow, fog and dust storms. Less common events include natural disasters such as tornadoes, hurricanes, typhoons and ice storms.
Air pollution
editAir pollution is the release of chemicals and particulates into the atmosphere. Common gaseous pollutants include carbon monoxide, sulfur dioxide, chlorofluorocarbons (CFCs) and nitrogen oxides produced by industry and motor vehicles. Photochemical ozone and smog are created as nitrogen oxides and hydrocarbons react to sunlight. Particulate matter (PM), or fine dust is characterized by their micrometre size PM10 to PM2.5. Particulate pollution is observed around the globe in varying sizes and compositions and is the focus of many epidemiological studies. PM is generally classified into two main size categories: PM10 and PM2.5. PM10, also known as coarse particulate matter, consists of particles 10 micrometers (μm) and smaller, while PM2.5, also called fine particulate matter, consists of particles 2.5 μm and smaller.[28] Particles 2.5 μm or smaller in size are especially notable as they can be inhaled into the lower respiratory system, and with enough exposure, absorbed into the bloodstream. Particulate pollution can occur directly or indirectly from a number of sources including, but not limited to: agriculture, automobiles, construction, forest fires, chemical pollutants, and power plants.[29]
Telluric sources
editMost astronomical observations are conducted by measuring photons (electromagnetic waves) which originate beyond the sky. The molecules in the Earth's atmosphere, however, absorb and emit their own light, especially in the visible and near-IR portion of the spectrum, and any ground-based observation is subject to contamination from these telluric (earth-originating) sources. Water vapor, oxygen, and OH are some of the more important molecules in telluric contamination. Water contamination was particularly pronounced in the Mount Wilson solar Doppler measurements.
It is possible to correct for the effects of telluric contamination in an astronomical spectrum. This is done by preparing a telluric correction function, made by dividing a model spectrum of a star by an observation of an astronomical photometric standard stars. This function can then be multiplied by an astronomical observation at each wavelength point.
While this method can restore the original shape of the spectrum, the regions affected can be prone to high levels of noise due to the low number of counts in that area of the spectrum.
Light pollution
editScientific definitions of light pollution include the following:
- Degradation of photic habitat by artificial light.[30]
- Alteration of natural light levels in the outdoor environment owing to artificial light sources.[31]
- Light pollution is the alteration of light levels in the outdoor environment (from those present naturally) due to man-made sources of light. Indoor light pollution is such alteration of light levels in the indoor environment due to sources of light, which compromises human health.[32]
- Light pollution is the introduction by humans, directly or indirectly, of artificial light into the environment.[33]
Light pollution obscures the stars in the night sky for city dwellers [and] interferes with astronomical observatories ... Light is particularly problematic for amateur astronomers, whose ability to observe the night sky from their property is likely to be inhibited by any stray light from nearby. Most major optical astronomical observatories are surrounded by zones of strictly enforced restrictions on light emissions.
Sky glow is of particular irritation to astronomers, because it reduces contrast in the night sky to the extent where it may even become impossible to see any but the brightest stars.
To precisely measure how bright the sky gets, night time satellite imagery of the earth is used as raw input for the number and intensity of light sources. These are put into a physical model[34] of scattering due to air molecules and aerosoles to calculate cumulative sky brightness. Maps that show the enhanced sky brightness have been prepared for the entire world.[35]
Some astronomers use narrow-band "nebula filters" which only allow specific wavelengths of light commonly seen in nebulae, or broad-band "light pollution filters" which are designed to reduce (but not eliminate) the effects of light pollution by filtering out spectral lines commonly emitted by sodium- and mercury-vapor lamps, thus enhancing contrast and improving the view of dim objects such as galaxies and nebulae.[36] Unfortunately these light pollution reduction (LPR) filters are not a cure for light pollution. LPR filters reduce the brightness of the object under study and this limits the use of higher magnifications. LPR filters work by blocking light of certain wavelengths, which alters the color of the object, often creating a pronounced green cast. Furthermore, LPR filters only work on certain object types (mainly emission nebulae) and are of little use on galaxies and stars. No filter can match the effectiveness of a dark sky for visual or photographic purposes. Due to their low surface brightness, the visibility of diffuse sky objects such as nebulae and galaxies is affected by light pollution more than are stars. Most such objects are rendered invisible in heavily light polluted skies around major cities. A simple method for estimating the darkness of a location is to look for the Milky Way, which from truly dark skies appears bright enough to cast a shadow.[37]
In addition to skyglow, light trespass can impact observations when artificial light directly enters the tube of the telescope and is reflected from non-optical surfaces until it eventually reaches the eyepiece. This direct form of light pollution causes a glow across the field of view which reduces contrast. Light trespass also makes it hard for a visual observer to become sufficiently dark adapted. The usual measures to reduce this glare, if reducing the light directly is not an option, include flocking the telescope tube and accessories to reduce reflection, and putting a light shield (also usable as a dew shield) on the telescope to reduce light entering from angles other than those near the target. Under these conditions, some astronomers prefer to observe under a black cloth to ensure maximum dark adaptation.
Space weather
editSpace weather is the concept of changing environmental conditions in near-Earth space or the space from the Sun's atmosphere to the Earth's atmosphere.
Near-earth space is defined as the region from the interface between the solar wind and the Earth into the magnetosphere and down to the ionosphere and thermosphere.
The sun's corona is constantly being lost to space, creating what is essentially a very thin atmosphere throughout the Solar System. The movement of mass ejected from the Sun is known as the solar wind. Inconsistencies in this wind and larger events on the surface of the star, such as coronal mass ejections, form a system that has features analogous to conventional weather systems (such as pressure and wind) and is generally known as space weather. Coronal mass ejections have been tracked as far out in the solar system as Saturn.[38] The activity of this system can affect planetary atmospheres and occasionally surfaces. The interaction of the solar wind with the terrestrial atmosphere can produce spectacular aurorae,[39] and can play havoc with electrically sensitive systems such as electricity grids and radio signals.
Point sources
editDef. "[a]n idealized discrete source of radiation that subtends an infinitesimally small angle"[40] is called a point source.
It is "[a] source whose angular extent cannot be measured (< 0".05)."[40]
Absorptions
edit"[W]hen the medium [behaves] like an amplifier to the incident radiation" it is "possible for negative absorption to arise at radio wavelengths".[41]
Negative absorptions
editThe necessary and sufficient conditions for negative absorption to occur at radio wavelengths are
- "the kinetic energy distribution F(η) of the radiating electrons [is] markedly non-thermal with an appreciable excess of high energy electrons such that ∂F/∂η is positive over a finite range of the kinetic energy η" and
- "the stimulated transition probability [has] a maximum at some finite value of the kinetic energy, the most favorable case occurring when this maximum is a sharp one at the value of η at which ∂F/∂η has a positive maximum."[41]
"These conditions can both be met in principle for the cases in which the dominant radiation process is due [to]
- [the] Cerenkov effect,
- gyro radiation by non-relativistic electrons, [and]
- synchrotron-type radiation by highly relativistic electrons".[41]
Def. "radiation at the fundamental or at the first few harmonics of the gyro frequency by weakly relativistic electrons rotating in a magnetic field" is called gyro radiation.[41]
Def. "radiation by strongly relativistic electrons at high harmonics of the gyro frequency" is called synchrotron radiation.[41]
Def. the frequency of the circular motion of a charged particle in the presence of a uniform magnetic field is called the gyro frequency, here also it is the first or fundamental frequency.
Def. the emission of light (Cerenkov radiation) that occurs when a charged particle passes through an insulator at a speed greater than the speed of light in that medium is called the Cerenkov effect.
Def. the electromagnetic radiation emitted by the accelerating charged particles in a synchrotron that are moving at near the speed of light is called synchrotron radiation.
Def. a component frequency of the signal that is an integer multiple of the fundamental frequency is called a harmonic of the wave.
At right is a diagram which shows the higher harmonics of the fundamental frequency (ff) at the top. Each higher harmonic is an integral multiple of the first: 2ff, 3ff, 4ff, 5ff, 6ff, 7ff, from top to bottom.
Positive absorptions
editA rotational transition is an abrupt change in angular momentum in quantum physics. Like all other properties of a quantum particle, angular momentum is quantized, meaning it can only equal certain discrete values, which correspond to different rotational energy states. When a particle loses angular momentum, it is said to have transitioned to a lower rotational energy state. Likewise, when a particle gains angular momentum, a positive rotational transition is said to have occurred. ... [U]nique spectral lines ... result. [For] a net gain or loss of energy during a transition, electromagnetic radiation of a particular frequency must be absorbed or emitted.
"The 111 → 110 rotational transition of formaldehyde (H2CO) [occurs] in absorption in the direction of four dark nebulae. The radiation ... being absorbed appears to be the isotropic microwave background".[42] One of the dark nebulae sampled, per SIMBAD is TGU H1211 P5.
Accelerations
editFor proton astronomy, “at the high end of the proton energy spectrum (above ≈ 1018 eV) [the Larmor radius] deflection becomes small enough that proton astronomy becomes possible.”[43]
The Larmor radius is the radius of the circular motion of a charged particle in the presence of a uniform magnetic field.
“[F]or a particle of energy E in EeV and charge Z in a magnetic field B in µG [the Larmor radius (RL)] is roughly”[44]
where
- is the Larmor radius,
- is the energy of the particle in EeV
- is the charge of the particle, and
- is the constant magnetic field.
Diffractions
editDef. the "breaking up of an electromagnetic wave as it passes a geometric structure (e.g. a slit), followed by reconstruction of the wave by interference"[45] is called diffraction.
Distillations
editDef. the "separation of the volatile parts of a substance from the more fixed; specifically, the operation of driving off gas or vapor from volatile liquids or solids, by heat in a retort or still, and the condensation of the products as far as possible by a cool receiver, alembic, or condenser; rectification; vaporization; condensation"[46] is called distillation.
Emissions
editDef. the act of sending or throwing out; the act of putting into circulation is called an emission.
Def. origination by some process, [biological], chemical, or [physical], is called generation.
Holes
editDef. a hollow spot in a surface is called a hole.
Def. an opening in a solid, liquid, gas, or plasma is called a hole.
Def. a round or irregular patch on [or apparently on] the surface of [an entity] having a different color, texture etc. and generally round in shape is called a spot.
Def. an opening through which entities such as gases can pass is called a vent.
Lensings
editThe image at right shows several blue, loop-shaped objects that are multiple images of the same galaxy, duplicated by the gravitational lens effect of the cluster of yellow galaxies near the middle of the photograph. The lens is produced by the cluster's gravitational field that bends light to magnify and distort the image of a more distant object.
Reflections
editDef. the property of a propagated wave being thrown back from a surface (such as a mirror) is called reflection.
Def.
Refractions
editDef. the turning or bending of any wave, such as a light or sound wave, when it passes from one medium into another of different optical density is called refraction.
Scatterings
editSpallations
editDef. a reaction in which an entity fragments into many due to stress or impact is called spallation.
Transductions
editDef. the process to convert energy from one form to another is called transduction.
Transformations
editTransmutations
editSuper soft X-ray sources
editA super soft X-ray source (SSXS, or SSS) is an astronomical source of very low energy X-rays. Soft X-rays have energies in the 0.09 to 2.5 keV range, whereas hard X-rays are in the 1-20 keV range.[47]
SSXSs are in most cases only detected below 0.5 keV, so that within our own galaxy they are usually hidden by interstellar absorption in the galactic disk.[48] They are readily evident in external galaxies, with ~10 found in the Magellanic Clouds and at least 15 seen in M31.[48]
As of early 2005, more than 100 SSSs have been reported in ~20 external galaxies, the Large Magellanic Cloud (LMC), Small Magellanic Cloud (SMC), and the Milky Way (MW).[49] Those with luminosities below ~3 x 1038 erg/s are consistent with steady nuclear burning in accreting white dwarfs (WD)s or post-novae.[49] There are a few SSS with luminosities ≥1039 erg/s.[49]
Super soft X-rays are believed to be produced by steady nuclear fusion on a white dwarf's surface of material pulled from a binary companion,[50] the so-called close-binary supersoft source (CBSS).[51]
This requires a flow of material sufficiently high to sustain the fusion. Contrast this with the nova, where less flow causes the material to only fuse sporadically. Super soft X-ray sources can evolve into type Ia supernova, where a sudden fusion of material destroys the white dwarf, and neutron stars, through collapse[52].
Super soft X-ray sources were first discovered by the Einstein Observatory. Further discoveries were made by ROSAT.[53]
Many different classes of objects emit supersoft X-radiation (emission dominantly below 0.5 keV).[51]
Luminous supersoft X-ray sources
editLuminous super soft X-ray sources have a characteristic blackbody temperature of a few tens of eV (~20-100 eV)[49] and a bolometric luminosity of ~1038 erg/s (below ~ 3 x 1038 erg/s).[48][49]
Apparently, luminous SSSs can have equivalent blackbody temperatures as low as ~15 eV and luminosities ranging from 1036 to 1038 erg/s.[54] The numbers of luminous SSSs in the disks of ordinary spiral galaxies such as the MW and M31 are estimated to be on the order of 103.[54]
Milky Way SSXSs
editSSXSs have now been discovered in our galaxy and in globular cluster M3.[48] MR Velorum (RX J0925.7-4758) is one of the rare MW super soft X-ray binaries.[51] "The source is heavily reddened by interstellar material, making it difficult to observe in the blue and ultraviolet."[55] The period determined for MR Velorum at ~4.03 d is considerably longer than that of other supersoft systems, which is usually less than a day.[55]
Close-binary supersoft sources
editThe close-binary supersoft source CBSS model invokes steady nuclear burning on the surface of an accreting white dwarf (WD) as the generator of the prodigious super soft X-ray flux.[51] As of 1999, eight SSXSs have orbital periods between ~4 hr and 1.35 d: RX J0019.8+2156 (MW), RX J0439.8-6809 (LMC), RX J0513.9-6951 (LMC), RX J0527.8-6954 (LMC), RX J0537.7-7034 (LMC), CAL 83 (LMC), CAL 87 LMC), and 1E 0035.4-7230 (SMC).[51]
Symbiotic binaries
editA symbiotic binary star is a variable binary star system in which a red giant has expanded its outer envelope and is shedding mass quickly, and another hot star (often a white dwarf) is ionizing the gas.[56] Three symbiotic binaries as of 1999 are SSXSs: AG Dra (BB, MW), RR Tel (WD, MW), and RX J0048.4-7332 (WD, SMC).[51]
Noninteracting white dwarfs
editThe youngest, hottest WD is very close to 100,000 K, of type DO and is the first single WD recorded as an X-ray source with ROSAT.[57][58]
Cataclysmic variables
edit"Cataclysmic variables (CVs) are close binary systems consisting of a white dwarf and a red-dwarf secondary transferring matter via the Roche lobe overflow."[59]
Both fusion- and accretion-powered cataclysmic variables have been observed to be X-ray sources.[60] The accretion disk may be prone to instability leading to dwarf nova outbursts: a portion of the disk material falls onto the white dwarf, the cataclysmic outbursts occur when the density and temperature at the bottom of the accumulated hydrogen layer rise high enough to ignite nuclear fusion reactions, which rapidly burn the hydrogen layer to helium.
Apparently the only SSXS nonmagnetic cataclysmic variable is V Sge: bolometric luminosity of (1 - 10) x 1037, a binary including a blackbody (BB) accretor at T < 80 eV, and an orbital period of 0.514195 d.[51]"
The accretion disk can become thermally stable in systems with high mass-transfer rates (Ṁ).[59] Such systems are called nova-like (NL) stars, because they lack outbursts characteristic of dwarf novae.[61]
VY Scl cataclysmic variables
editAmong the NL stars is a small group which shows a temporary reduction or cessation of Ṁ from the secondary. These are the VY Scl-type stars or anti-dwarf novae.[62]
V751 Cygni
editV751 Cyg (BB, MW) is a VY Scl CV, has a bolometric luminosity of 6.5 x 1036 erg/s,[51] and emits soft X-rays at quiescence.[63] The discovery of a weak soft X-ray source of V751 Cyg at minimum presents a challenge as this is unusual for CVs which commonly display weak hard X-ray emission at quiescence.[63]
The high luminosity (6.5 x 1036 erg/s) is particularly hard to understand in the context of VY Scl stars generally, because observations suggest that the binaries become simple red dwarf + white dwarf pairs at quiescence (the disk mostly disappears).[63] "A high luminosity in soft X-rays poses an additional problem of understanding why the spectrum is of only modest excitation."[63] The ratio He II λ4686/Hβ did not exceed ~0.5 in any of the spectra recorded up to 2001, which is typical for accretion-powered CVs and does not approach the ratio of 2 commonly seen in supersoft binaries (CBSS).[63]
Pushing the edge of acceptable X-ray fits toward lower luminosity suggests that the luminosity should not exceed ~2 x 1033 ergs/s, which gives only ~4 x 1031 ergs/s of reprocessed light in the WD about equal to the secondary's expected nuclear luminosity.[63]
Magnetic cataclysmic variables
editX-rays from magnetic cataclysmic variables are common because accretion provides a continuous supply of coronal gas.[64] A plot of number of systems vs. orbit period shows a statistically significant minimum for periods between 2 and 3 hr which can probably be understood in terms of the effects of magnetic braking when the companion star becomes completely convective and the usual dynamo (which operates at the base of the convective envelope) can no longer give the companion a magnetic wind to carry off angular momentum.[64] The rotation has been blamed on asymmetric ejection of planetary nubulae and winds[65] and the fields on in situ dynamos.[66] Orbit and rotation periods are synchronized in strongly magnetized WDs.[64] Those with no detectable field never are synchronized.
With temperatures in the range 11,000 to 15,000 K, all the WDs with the most extreme fields are far too cool to be detectable EUV/X-ray sources, e.g., Grw +70°8247, LB 11146, SBS 1349+5434, PG 1031+234 and GD 229.[67]
Most highly magnetic WDs appear to be isolated objects, although G 23-46 (7.4 MG) and LB 1116 (670 MG) are in unresolved binary systems.[68]
RE J0317-853 is the hottest magnetic WD at 49,250 K, with an exceptionally intense magnetic field of ~340 MG, and implied rotation period of 725.4 s.[68] Between 0.1 and 0.4 keV, RE J0317-853 was detectable by ROSAT, but not in the higher energy band from 0.4 to 2.4 keV.[69] RE J0317-853 is associated with a blue star 16 arcsec from LB 9802 (also a blue WD) but not physically associated.[68] A centered dipole field is not able to reproduce the observations, but an off-center dipole 664 MG at the south pole and 197 MG at the north pole does.[68]
Until recently (1995) only PG 1658+441 possessed an effective temperature > 30,000 K.[68] Its polar field strength is only 3 MG.[68]
The ROSAT Wide Field Camera (WFC) source RE J0616-649 has an ~20 MG field.[70]
PG 1031+234 has a surface field that spans the range from ~200 MG to nearly 1000 MG and rotates with a period of 3h24m.[71]
The magnetic fields in CVs are confined to a narrow range of strengths, with a maximum of 7080 MG for RX J1938.4-4623.[72]
None of the single magnetic stars has been seen as of 1999 as an X-ray source, although fields are of direct relevance to the maintenance of coronae in main sequence stars.[64]
PG 1159 stars
editPG 1159 stars are a group of very hot, often pulsating WDs for which the prototype is PG 1159 dominated by carbon and oxygen in their atmospheres.[64]
PG 1159 stars reach luminosities of ~1038 erg/s but form a rather distinct class.[73] RX J0122.9-7521 has been identified as a galactic PG 1159 star.[74][75]
Novas
editThere are three SSXSs with bolometric luminosity of ~1038 erg/s that are novae: GQ Mus (BB, MW), V1974 Cyg (WD, MW), and Nova LMC 1995 (WD).[51] Apparently, as of 1999 the orbital period of Nova LMC 1995 if a binary was not known.
U Sco, a recurrent nova as of 1999 unobserved by ROSAT, is a WD (74-76 eV), Lbol ~ (8-60) x 1036 erg/s, with an orbital period of 1.2306 d.[51]
Planetary nebulas
editIn the SMC, 1E 0056.8-7154 is a WD with bolometric luminosity of 2 x 1037 that has a planetary nebula associated with it.[51]
Super soft active galactic nuclei
editSupersoft active galactic nuclei reach luminosities up to 1045 erg/s.[51]
Large amplitude outbursts
editLarge amplitude outbursts of super soft X-ray emission have been interpreted as tidal disruption events.[76]
Greens
editChlorophyll is a common source of green on Earth's surface by reflection of sunlight. Malachite is a green mineral also by reflection of sunlight that occurs in rocks at or near the interface between Earth's atmosphere and crust.
There is a green emission continuum.
Hypotheses
edit- Some intervening material between the detector and the alleged source may turn out to be the source.
References
edit- ↑ O. Mousis; J.-M. Petit; G. Wurm; O. Krauss; Y. Alibert; J. Horner (2007). "Photophoresis as a source of hot minerals in comets". Astronomy and Astrophysics 466 (2): L9-12. doi:10.1051/0004-6361:20077170. http://oro.open.ac.uk/19419/. Retrieved 2013-12-28.
- ↑ 2.0 2.1 Philip B. Gove, ed (1963). Webster's Seventh New Collegiate Dictionary. Springfield, Massachusetts: G. & C. Merriam Company. pp. 1221.
- ↑ Swirling Star Trails Over Yepun, In: Picture of the Week. ESO. https://www.eso.org/public/images/potw1301a/. Retrieved 11 January 2013.
- ↑ MUL.APIN; Peter Whitfield, History of Astrology (2001); W. Muss-Arnolt, The Names of the Assyro-Babylonian Months and Their Regents, Journal of Biblical Literature (1892).
- ↑ 5.0 5.1 5.2 5.3 H. Olofsson (July 2, 2012). Red giant blows a bubble. Maryland USA: SpaceTelescope Organization. http://www.spacetelescope.org/images/potw1227a/. Retrieved 2013-12-24.
- ↑ Russell, Henry Norris (1922). "The New International Symbols for the Constellations". Popular Astronomy 30: 469–71.
- ↑ "Canis Major, Constellation Boundary". The Constellations (International Astronomical Union). http://www.iau.org/public/constellations/#cma. Retrieved 15 November 2012.
- ↑ 8.0 8.1 8.2 8.3 8.4 J.B. Holberg (2007). Sirius: Brightest Diamond in the Night Sky. Chichester, UK: Praxis Publishing. ISBN 0-387-48941-X.
- ↑ R. C. Ceragioli (1995). "The Debate Concerning 'Red' Sirius". Journal for the History of Astronomy 26 (3): 187–226.
- ↑ Whittet, D. C. B. (1999). "A physical interpretation of the 'red Sirius' anomaly". Monthly Notices of the Royal Astronomical Society 310 (2): 355–359. doi:10.1046/j.1365-8711.1999.02975.x.
- ↑ 江晓原 (1992). "中国古籍中天狼星颜色之记载". Ť文学报 33 (4).
- ↑ Jiang, Xiao-Yuan (April 1993). "The colour of Sirius as recorded in ancient Chinese texts". Chinese Astronomy and Astrophysics 17 (2): 223–8. doi:10.1016/0275-1062(93)90073-X.
- ↑ Schlosser, W.; Bergmann, W. (November 1985). "An early-medieval account on the red colour of Sirius and its astrophysical implications". Nature 318 (318): 45–6. doi:10.1038/318045a0.
- ↑ 14.0 14.1 14.2 Davide De Martin (August 28, 2013). Image of HIP 102152. ESO’s Very Large Telescope in Brazil: European Southern Observatory. http://www.eso.org/public/images/eso1337b/. Retrieved 2013-12-24.
- ↑ S. Van Dyk (May 22, 2003). 2MASS Atlas Image Gallery: Miscellaneous Objects. California USA: IPAC, California Institute of Technology. http://www.ipac.caltech.edu/2mass/gallery/images_misc.html. Retrieved 2013-12-24.
- ↑ 16.0 16.1 16.2 16.3 16.4 U. Hwang (August 23, 2004). Cassiopeia A: Deepest Image of Exploded Star Uncovers Bipolar Jets. Cambridge, Massachusetts, USA: Harvard-Smithsonian Center for Astrophysics. http://chandra.harvard.edu/photo/2004/casa/. Retrieved 2013-12-24.
- ↑ H. Bond; K. Exter (June 3, 2008). White Dwarf Lost in Planetary Nebula. Maryland USA: Hubblesite Organization. http://hubblesite.org/newscenter/archive/releases/2008/21/image/a/. Retrieved 2013-12-24.
- ↑ 18.0 18.1 18.2 18.3 18.4 18.5 18.6 Keith Taylor; Mike Scarrott (February 20, 2003). The Boomerang Nebula - the coolest place in the Universe?. Maryland USA: SpaceTelescope Organization. http://www.spacetelescope.org/images/heic0301a/. Retrieved 2013-12-24.
- ↑ Richard Hook (June 30, 2010). R Coronae Australis: A Cosmic Watercolour. Garching, Germany: European Southern Obsrvatory. http://www.eso.org/public/news/eso1027/. Retrieved 2013-12-25.
- ↑ Heritage Team (October 16, 2006). Colliding galaxies make love, not war. Maryland USA: Space Telescope Organization. http://www.spacetelescope.org/images/heic0615a/. Retrieved 2013-12-25.
- ↑ 21.0 21.1 J. English (December 12, 2002). Cosmic Dance of Destruction. Maryland USA: Space Telescope Organization. http://www.spacetelescope.org/images/opo0222a/. Retrieved 2013-12-23.
- ↑ A. Evans (8 April 2002). Hubble Interacting Galaxy ESO 69-6. Baltimore, Maryland USA: Hubblesite. http://hubblesite.org/image/2288/news_release/2008-16. Retrieved 2017-06-16.
- ↑ Constellations: A Guide to the Night Sky. 2013. http://www.constellation-guide.com/constellation-list/volans-constellation/.
- ↑ Merriam-Webster Dictionary. Weather. Retrieved on 27 June 2008.
- ↑ Glossary of Meteorology. Hydrosphere. Retrieved on 27 June 2008.
- ↑ Glossary of Meteorology. Troposphere. Retrieved on 27 June 2008.
- ↑ Glossary of Meteorology. American Meteorological Society. http://amsglossary.allenpress.com/glossary/search?id=climate1. Retrieved 14 May 2008.
- ↑ WHO Air quality guidelines for particulate matter, ozone, nitrogen dioxide, and sulfur dioxide. https://www.epa.gov/pm-pollution/health-and-environmental-effects-particulate-matter-pm.
- ↑ Particulate Matter (PM) Basics. https://www.epa.gov/pm-pollution/particulate-matter-pm-basics.
- ↑ . PMID 3896840.
- ↑ Cinzano, P.; Falchi, F.; Elvidge, C. D.; Baugh, K. E. (2000). "The artificial night sky brightness mapped from DMSP Operational Linescan System measurements". Monthly Notices of the Royal Astronomical Society 318 (3): 641. doi:10.1046/j.1365-8711.2000.03562.x. http://www.lightpollution.it/cinzano/download/mnras_paper.pdf.
- ↑ Hollan, J: What is light pollution, and how do we quantify it?. Darksky2008 conference paper, Vienna, August 2008. Updated April 2009.
- ↑ Marín, C. and Orlando, G. (eds.): Starlight Reserves and World Heritage. Starlight Initiative, IAC and the UNESCO World Heritage Centre. Fuerteventura, Spain, June 2009.
- ↑ P. Cinzano; F. Falchi; C. D. Elvidge (2001). "The first world atlas of the artificial night sky brightness". Mon.Not.Roy.Astron.Soc. 328 (3): 689–707. doi:10.1046/j.1365-8711.2001.04882.x. http://debora.pd.astro.it/cinzano/download/0108052.pdf.
- ↑ The World Atlas of the Artificial Night Sky Brightness. Lightpollution.it. Retrieved on 2011-12-03.
- ↑ www.astronexus.com, Use of light pollution filters in astronomy. Astronexus.com. Retrieved on 2011-12-03.
- ↑ NASA Astronomy Picture of the Day, 2010 August 23. Apod.nasa.gov. Retrieved on 2011-12-03.
- ↑ Bill Christensen. Shock to the (Solar) System: Coronal Mass Ejection Tracked to Saturn. Retrieved on 28 June 2008.
- ↑ AlaskaReport. What Causes the Aurora Borealis? Retrieved on 28 June 2008.
- ↑ 40.0 40.1 MiMi.hu. Point source. Hungary: DOMIX Studio. http://en.mimi.hu/astronomy/point_source.html. Retrieved 2012-04-18.
- ↑ 41.0 41.1 41.2 41.3 41.4 R. Q. Twiss (December 1958). "Radiation Transfer and the Possibility of Negative Absorption in Radio Astronomy". Australian Journal of Physics 11 (12): 564.
- ↑ Patrick Palmer; B. Zuckerman; David Buhl; Lewis E. Snyder (June 1969). "Formaldehyde Absorption in Dark Nebulae". The Astrophysical Journal 156 (6): L147-50. doi:10.1086/180368.
- ↑ 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. http://arxiv.org/pdf/0812.3809. Retrieved 2012-03-28.
- ↑ P Sommers; S Westerhoff (May 12, 2009). "Cosmic ray astronomy". New Journal of Physics 11 (5): 055004. doi:10.1088/1367-2630/11/5/055004. http://arxiv.org/pdf/0802.1267. Retrieved 2012-03-28.
- ↑ SemperBlotto (7 April 2005). diffraction. San Francisco, California: Wikimedia Foundation, Inc. https://en.wiktionary.org/wiki/diffraction. Retrieved 19 June 2021.
- ↑ Poccil (20 October 2004). distillation. San Francisco, California: Wikimedia Foundation, Inc. https://en.wiktionary.org/wiki/distillation. Retrieved 19 June 2021.
- ↑ Supersoft X-Ray Sources. http://library.thinkquest.org/27930/supersoft.htm.
- ↑ 48.0 48.1 48.2 48.3 White NE; Giommi P; Heise J; Angelini L; Fantasia S. "RX J0045.4+4154: A Recurrent Supersoft X-ray Transient in M31". The Astrophysical Journal Letters 445: L125. http://lheawww.gsfc.nasa.gov/users/white/wgacat/apjl.html.
- ↑ 49.0 49.1 49.2 49.3 49.4 Kahabka P (Dec 2006). "Supersoft X-ray sources". Adv Space Res. 38 (12): 2836–9. doi:10.1016/j.asr.2005.10.058. http://www.sciencedirect.com/science?_ob=ArticleURL&_udi=B6V3S-4MBT29S-2&_user=10&_origUdi=B6V3S-3YN948T-5&_fmt=high&_coverDate=12%2F31%2F2006&_rdoc=1&_orig=article&_acct=C000050221&_version=1&_urlVersion=0&_userid=10&md5=3a3d0440365be046b322ab561aae9230.
- ↑ Super Soft X-ray Sources - Discovered with ROSAT (Max Planck Institute for Extraterrestrial Physics)
- ↑ 51.00 51.01 51.02 51.03 51.04 51.05 51.06 51.07 51.08 51.09 51.10 51.11 Greiner J (2000). "Catalog of supersoft X-ray sources". New Astron. 5 (3): 137–41. doi:10.1016/S1384-1076(00)00018-X. http://www.mpe.mpg.de/~jcg/sss/ssscat.html.
- ↑ Proceedings of the Workshop on Supersoft X-ray Sources held at the Max Planck Institute for Extraterrestrial Physics
- ↑ Catalog of Supersoft X-ray Sources. http://www.aip.de/~jcg/sss/ssscat.html.
- ↑ 54.0 54.1 Kahabka P, van den Heuvel EPJ (1997). "Luminous Supersoft X-Ray Sources". Ann Rev Astron Astrophys. 35 (1): 69–100. doi:10.1146/annurev.astro.35.1.69.
- ↑ 55.0 55.1 Schmidtke PC, Cowley AP (Sep 2001). "SYNOPTIC OBSERVATIONS OF THE SUPERSOFT BINARY MR VELORUM (RX J0925.7-4758): DETERMINATION OF THE ORBITAL PERIOD". Astron J. 122 (3): 1569–71. doi:10.1086/322155. http://www.iop.org/EJ/article/1538-3881/122/3/1569/201190.text.html.
- ↑ David Darling site symbiotic star description. http://www.daviddarling.info/encyclopedia/S/symbiotic_star.html.
- ↑ Fleming TA "et al." (1994). Ap J. 411: L79.
- ↑ Werner (1994). Astron Astrophys. 284: 907.
- ↑ 59.0 59.1 Kato T; Ishioka R; Uemura M (Dec 2002). "Photometric Study of KR Aurigae during the High State in 2001". Publ Astron Soc Japan 54 (6): 1033–9. http://pasj.asj.or.jp/v54/n6/540624/540624-frame.html.
- ↑ Introduction to Cataclysmic Variables (CVs). http://heasarc.gsfc.nasa.gov/docs/objects/cvs/cvstext.html.
- ↑ Osaki, Yoji (1996). "Dwarf-Nova Outbursts". PASP 108: 39. doi:10.1086/133689.
- ↑ Warner B (1995). Cataclysmic Variable Stars. Cambridge: Cambridge University Press. http://adsabs.harvard.edu/cgi-bin/bib_query?1995cvs..book.....W.
- ↑ 63.0 63.1 63.2 63.3 63.4 63.5 Patterson J; Thorstensen JR; Fried R; Skillman DR; Cook LM; Jensen L (Jan 2001). "Superhumps in Cataclysmic Binaries. XX. V751 Cygni". Publ Astron Soc Pacific (PASP) 113 (779): 72–81. doi:10.1086/317973.
- ↑ 64.0 64.1 64.2 64.3 64.4 Trimble V (1999). "White dwarfs in the 1990's". Bull Astron Soc India. 27: 549–66.
- ↑ Spruit HC (1998). Astron Astrophys. 333: 603.
- ↑ Schmidt GD, Grauer AD (1997). "Upper Limits for Magnetic Fields on Pulsating White Dwarfs". Ap J. 488 (2): 827. doi:10.1086/304746.
- ↑ Schmidt GD, Smith PS (1995). "A Search for Magnetic Fields among DA White Dwarfs". Ap J. 448: 305. doi:10.1086/175962.
- ↑ 68.0 68.1 68.2 68.3 68.4 68.5 Barstow MA; Jordan S; O'Donoghue D; Burleigh MR; Napiwotzki R; Harrop-Allin MK (1995). "RE J0317-853: the hottest known highly magnetic DA white dwarf". MNRAS 277 (3): 931–85.
- ↑ Fleming TA (1995). Astron Astrophys..
- ↑ Jordan, Finley.
- ↑ Latter WB; Schmidt GD; Green RF (1987). "The rotationally modulated Zeeman spectrum at nearly 10 to the 9th Gauss of the white dwarf PG 1031 + 234". Ap J. 320: 308. doi:10.1086/165543.
- ↑ Schwope AD, "et al." (1995). Astron Astrophys. 293: 764.
- ↑ Dreizler S; Werner K; Heber U (1995). Kӧster D, Werner K. ed. "White Dwarfs". Lect Notes Phys. (Berlin: Springer) 443: 160.
- ↑ Cowley AP; Schmidtke PC; Hutchings JB; Crampton D (1995). "X-Ray Discovery of a Hot PG1159 Star, RX J0122.9-7521". PASP 107: 927. doi:10.1086/133640.
- ↑ Werner K; Wolff B; Cowley AP; Schmidtke PC; Hutchings JB; Crampton D (1996). Greiner. ed. "Supersoft X-ray Sources". Lect Notes Phys. (Berlin: Springer) 472: 131.
- ↑ Komossa S, Greiner J (1999). Astron Astrophys. 349: L45.
Further reading
edit- Eberhard Haug; Werner Nakel (2004). The elementary process of Bremsstrahlung. River Edge NJ: World Scientific. p. Scientific lecture notes in physics, vol. 73. ISBN 9812385789. http://books.google.com/books?hl=en&id=v4FMtIwTri8C&printsec=frontcover&source=web&ots=THjay1eeFA&sig=aHe-xMFwT8jxhpAGJHDnxKC6Jjc#PPA29,M1.
- Vedrenne G; Atteia J.-L. (2009). Gamma-Ray Bursts: The brightest explosions in the Universe. Springer. ISBN 978-3540390855. http://books.google.com/books?id=jZHSdrvzz0gC&printsec=frontcover&source=gbs_v2_summary_r&cad=0#v=onepage&q&f=false.
External links
edit- Google scholar Advanced Scholar Search
- International Astronomical Union
- NASA/IPAC Extragalactic Database - NED
- NASA's National Space Science Data Center
- NCBI All Databases Search
- Office of Scientific & Technical Information
- PubChem Public Chemical Database
- The SAO/NASA Astrophysics Data System
- Scirus for scientific information only advanced search
- SDSS Quick Look tool: SkyServer
- SIMBAD Astronomical Database
- Spacecraft Query at NASA
- Universal coordinate converter
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