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Future of an expanding universe

Current observations suggest that the expansion of the universe will continue forever. The prevailing theory is that the universe will cool as it expands, eventually becoming too cold to sustain life. For this reason, this future scenario popularly called "Heat Death" is also known as the "Big Chill" or "Big Freeze". Some of the other popular theories include the Big Rip, the Big Crunch, the Big Bounce, and the Big Slurp.

Cosmology
Infinite expansion does not constrain the overall spatial curvature of the universe. It can be open (with negative spatial curvature), flat, or closed (positive spatial curvature), although if it is closed, sufficient dark energy must be present to counteract the gravitational forces or else the universe will end in a Big Crunch. Observations of the Cosmic microwave background by the Wilkinson Microwave Anisotropy Probe and the Planck mission suggest that the universe is spatially flat and has a significant amount of dark energy. In this case, the universe might continue to expand at an accelerating rate. The acceleration of the universe's expansion has also been confirmed by observations of distant supernovae. If, as in the concordance model of physical cosmology (Lambda-cold dark matter or ΛCDM), dark energy is in the form of a cosmological constant, the expansion will eventually become exponential, with the size of the universe doubling at a constant rate. If the theory of inflation is correct, the universe went through an episode dominated by a different form of dark energy in the first moments of the Big Bang; but inflation ended, indicating an equation of state much more complicated than those assumed so far for present-day dark energy. It is possible that the dark energy equation of state could change again resulting in an event that would have consequences which are extremely difficult to parametrize or predict. == Future history ==
Future history
In the 1970s, the future of an expanding universe was studied by the astrophysicist Jamal Islam and the physicist Freeman Dyson. Then, in their 1999 book The Five Ages of the Universe, the astrophysicists Fred Adams and Gregory Laughlin divided the past and future history of an expanding universe into five eras. The first, the Primordial Era, is the time in the past just after the Big Bang when stars had not yet formed. The second, the Stelliferous Era, includes the present day and all of the stars and galaxies now seen. It is the time during which stars form from collapsing clouds of gas. In the subsequent Degenerate Era, the stars will have burnt out, leaving all stellar-mass objects as stellar remnantswhite dwarfs, neutron stars, and black holes. In the Black Hole Era, white dwarfs, neutron stars, and other smaller astronomical objects have been destroyed by proton decay, leaving only black holes. Finally, in the Dark Era, even black holes have disappeared, leaving only a dilute gas of photons and leptons. == Timeline ==
Timeline
The Stelliferous Era : From the present to about (100 trillion) years after the Big Bang s. LH 95 star forming region of the Large Magellanic Cloud. The image was taken using the Hubble Space Telescope. Source: European Space Agency (ESA/Hubble) The observable universe is currently 1.38 (13.8 billion) years old. This time lies within the Stelliferous Era. About 155 million years after the Big Bang, the first star formed. Since then, stars have formed by the collapse of small, dense core regions in large, cold molecular clouds of hydrogen gas. At first, this produces a protostar, which is hot and bright because of energy generated by gravitational contraction. After the protostar contracts for a while, its core could become hot enough to fuse hydrogen, if it exceeds critical mass, a process called 'stellar ignition' occurs, and its lifetime as a star will properly begin. Stars of low to medium mass, such as our own sun, will expel some of their mass as a planetary nebula and eventually become white dwarfs; more massive stars will explode in a core-collapse supernova, leaving behind neutron stars or black holes. In any case, although some of the star's matter may be returned to the interstellar medium, a degenerate remnant will be left behind whose mass is not returned to the interstellar medium. Therefore, the supply of gas available for star formation is steadily being exhausted. Milky Way Galaxy and the Andromeda Galaxy merge into one : 4–8 billion years from now (17.8–21.8 billion years after the Big Bang) during the Milky way-Andromeda galaxy collision event The Andromeda Galaxy is approximately 2.5 million light years away from our galaxy, the Milky Way galaxy, and they are moving towards each other at approximately 300 kilometres (186 miles) per second. Approximately five billion years from now, or 19 billion years after the Big Bang, the Milky Way and the Andromeda galaxy will collide with one another and merge into one large galaxy based on current evidence. Up until 2012, there was no way to confirm whether the possible collision was going to happen. In 2012, researchers came to the conclusion that the collision is definite after using the Hubble Space Telescope between 2002 and 2010 to track the motion of Andromeda. This results in the formation of Milkdromeda (also known as Milkomeda). 22 billion years in the future is the earliest possible end of the Universe in the Big Rip scenario, assuming a model of dark energy with = −1.5. False vacuum decay may occur in 20 to 30 billion years if the Higgs field is metastable. Coalescence of Local Group and galaxies outside the Local Supercluster are no longer accessible : (100 billion) to (1 trillion) years The galaxies in the Local Group, the cluster of galaxies which includes the Milky Way and the Andromeda Galaxy, are gravitationally bound to each other. It is expected that between (100 billion) and (1 trillion) years from now, their orbits will decay and the entire Local Group will merge into one large galaxy. of galaxies Galaxies outside the Local Supercluster are no longer detectable : (2 trillion) years 2 (2 trillion) years from now, all galaxies outside the Local Supercluster will be redshifted to such an extent that even gamma rays they emit will have wavelengths longer than the size of the observable universe of the time. Therefore, these galaxies will no longer be detectable in any way. Degenerate Era : From (100 trillion) to (10 duodecillion) years By (100 trillion) years from now, star formation will end, The least-massive stars take the longest to exhaust their hydrogen fuel (see stellar evolution). Thus, the longest living stars in the universe are low-mass red dwarfs, with a mass of about 0.08 solar masses (), which have a lifetime of over (10 trillion) years. Coincidentally, this is comparable to the length of time over which star formation takes place. If the combined mass is not above the Chandrasekhar limit but is larger than the minimum mass to fuse carbon (about ), a carbon star could be produced, with a lifetime of around (1 million) years. Planets fall or are flung from orbits by a close encounter with another star : (1 quadrillion) years Over time, the orbits of planets will decay due to gravitational radiation, or planets will be ejected from their local systems by gravitational perturbations caused by encounters with another stellar remnant. Stellar remnants escape galaxies or fall into black holes : to (10 to 100 quintillion) years Over time, objects in a galaxy exchange kinetic energy in a process called dynamical relaxation, making their velocity distribution approach the Maxwell–Boltzmann distribution. Dynamical relaxation can proceed either by close encounters of two stars or by less violent but more frequent distant encounters. In the case of a close encounter, two brown dwarfs or stellar remnants will pass close to each other. When this happens, the trajectories of the objects involved in the close encounter change slightly, in such a way that their kinetic energies are more nearly equal than before. After a large number of encounters, then, lighter objects tend to gain speed while the heavier objects lose it. Because of dynamical relaxation, some objects will gain just enough energy to reach galactic escape velocity and depart the galaxy, leaving behind a smaller, denser galaxy. Since encounters are more frequent in this denser galaxy, the process then accelerates. The result is that most objects (90% to 99%) are ejected from the galaxy, leaving a small fraction (maybe 1% to 10%) which fall into the central supermassive black hole. Possible ionization of matter : > years from now In an expanding universe with decreasing density and non-zero cosmological constant, matter density would reach zero, resulting in most matter except black dwarfs, neutron stars, black holes, and planets ionizing and dissipating at thermal equilibrium. == Future with proton decay ==
Future with proton decay
The following timeline assumes that protons do decay. : Chance: (100 nonillion) – years (1 tredecillion) The subsequent evolution of the universe depends on the possibility and rate of proton decay. Experimental evidence shows that if the proton is unstable, it has a half-life of at least years. Some of the Grand Unified theories (GUTs) predict long-term proton instability between and years, with the upper bound on standard (non-supersymmetry) proton decay at 1.4 years and an overall upper limit maximum for any proton decay (including supersymmetry models) at 6 years. Recent research showing proton lifetime (if unstable) at or exceeding – year range rules out simpler GUTs and most non-supersymmetry models. Nucleons start to decay Neutrons bound into nuclei are also suspected to decay with a half-life comparable to that of protons. Planets (substellar objects) would decay in a simple cascade process from heavier elements to hydrogen and finally to photons and leptons while radiating energy. If the proton does not decay at all, then stellar objects would still disappear, but more slowly. See below. Shorter or longer proton half-lives will accelerate or decelerate the process. This means that after years (the maximum proton half-life used by Adams & Laughlin (1997)), one-half of all baryonic matter will have been converted into gamma ray photons and leptons through proton decay. All nucleons decay : (10 tredecillion) years Given our assumed half-life of the proton, nucleons (protons and bound neutrons) will have undergone roughly 1,000 half-lives by the time the universe is years old. This means that there will be roughly 0.51,000 (approximately ) as many nucleons; as there are an estimated protons currently in the universe, none will remain at the end of the Degenerate Age. Effectively, all baryonic matter will have been changed into photons and leptons. Some models predict the formation of stable positronium atoms with diameters greater than the observable universe's current diameter (roughly 6 metres) in years, and that these will in turn decay to gamma radiation in years. :> years from now Although protons are stable in standard model physics, a quantum anomaly may exist on the electroweak level, which can cause groups of baryons (protons and neutrons) to annihilate into antileptons via the sphaleron transition. Such baryon/lepton violations have a number of 3 and can only occur in multiples or groups of three baryons, which can restrict or prohibit such events. No experimental evidence of sphalerons has yet been observed at low energy levels, though they are believed to occur regularly at high energies and temperatures. s, electrons, positrons, and neutrinos are all that remain after the last supermassive black holes evaporate. Black Hole Era : (10 tredecillion) years to approximately (1 googol) years, up to years for the largest supermassive black holes After  years, black holes will dominate the universe. They will slowly evaporate via Hawking radiation. The largest black holes in the universe are predicted to continue to grow. Larger black holes of up to (100 trillion) may form during the collapse of superclusters of galaxies. Even these would evaporate over a timescale of to years. Hawking radiation has a thermal spectrum. During most of a black hole's lifetime, the radiation has a low temperature and is mainly in the form of massless particles such as photons and hypothetical gravitons. As the black hole's mass decreases, its temperature increases, becoming comparable to the Sun's by the time the black hole mass has decreased to kilograms. The hole then provides a temporary source of light during the general darkness of the Black Hole Era. During the last stages of its evaporation, a black hole will emit not only massless particles, but also heavier particles, such as electrons, positrons, protons, and antiprotons. By this era, with only very diffuse matter remaining, activity in the universe will eventually tail off dramatically (compared with previous eras), with very low energy levels and very large time scales, with events taking a very long time to happen if they ever happen at all. Electrons and positrons drifting through space will encounter one another and occasionally form positronium atoms. These structures are unstable, however, and their constituent particles must eventually annihilate. However, most electrons and positrons will remain unbound. Other low-level annihilation events will also take place, albeit extremely slowly. The universe now gradually tends towards its lowest energy state. ==Future without proton decay ==
Future without proton decay
If protons do not decay, stellar-mass objects will still become black holes, although even more slowly. The following timeline that assumes proton decay does not take place. : years from now 2018 estimate of Standard Model lifetime before collapse of a false vacuum; 95% confidence interval is 1065 to 101383 years due in part to uncertainty about the top quark mass. Degenerate Era Matter decays into iron : to years from now will slowly decay into iron, which will take from to years. In years, pycnonuclear fusion occurring via quantum tunnelling should make the light nuclei in stellar-mass objects fuse into iron-56 nuclei (see isotopes of iron). Fission and alpha particle emission should make heavy nuclei also decay to iron, leaving stellar-mass objects as cold spheres of iron, called iron stars. Black Hole Era Collapse of iron stars to black holes : to years from now Quantum tunneling should also turn large objects into black holes, which (on these timescales) will instantaneously evaporate into subatomic particles. Depending on the assumptions made, the time this takes to happen can be calculated as from years to years. Quantum tunneling may also make iron stars collapse into neutron stars in around years. == Beyond ==
Beyond
: Beyond years if proton decay occurs, or years without proton decay Whatever event happens beyond this era is highly speculative. It is possible that a Big Rip event may occur far off into the future. This singularity would take place at a finite scale factor. If the current vacuum state is a false vacuum, the vacuum may decay into an even lower-energy state. Presumably, extreme low-energy states imply that localized quantum events become major macroscopic phenomena rather than negligible microscopic events because even the smallest perturbations make the biggest difference in this era, so there is no telling what will or might happen to space or time. It is perceived that the laws of "macro-physics" will break down, and the laws of quantum physics will prevail. Through this, the universe could possibly avoid an eternal heat death through random quantum tunneling and quantum fluctuations, given the non-zero probability of producing a new Big Bang creating a new universe in roughly years, according to physicists Sean M. Carroll and Jennifer Chen. == Graphical timelines ==
Graphical timelines
If protons decay: • ImageSize = width:1100 height:370 # too wide ImageSize = width:1000 height:370 PlotArea = left:40 right:235 bottom:50 top:50 Colors = id:period1 value:rgb(1,1,0.7) # light yellow id:period2 value:rgb(0.7,0.7,1) # light blue id:events value:rgb(1,0.7,1) # light purple id:era2 value:lightorange id:era1 Value:yellowgreen DateFormat = yyyy Period = from:-51 till:1000 TimeAxis = format:yyyy orientation:horizontal ScaleMajor = unit:year increment:100 start:0 ScaleMinor = unit:year increment:10 start:-50 AlignBars = justify BarData = bar:Era bar:Events TextData = fontsize:M pos:(0,260) text:"Big" text:"Bang" • pos:(880,260) pos:(780,260) text:"Heat" text:"Death" • pos:(880,90) pos:(780,90) text:"log" text:"year" PlotData= textcolor:black fontsize:M width:110 bar:Era mark:(line,white) align:left shift:(0,0) from:-51 till:8 shift:(0,35) color:era1 text:"Primordial Era" from:8 till:14 shift:(0,15) color:era2 text:"Stelliferous Era" from:14 till:40 shift:(0,-5) color:era1 text:"Degenerate Era" from:40 till:100 shift:(0,-25) color:era2 text:"Black Hole Era" from:100 till:1000 shift:(0,-45) color:era1 text:"Dark Era" width:110 bar:Events color:events align:left shift:(43,3) mark:(line,teal) at:-8 shift:(0,35) text:"One second" at:8 shift:(-2,15) text:"First star began to shine" at:10 shift:(-2,-5) text:"13.8 billion years, the present day" at:14 shift:(0,-25) text:"The last star has died" at:40 shift:(0,-35) text:"The last proton has decayed" at:100 shift:(0,-45) text:"The last supermassive black holes have evaporated" If protons do not decay:# ImageSize = width:1100 height:370 # too wide ImageSize = width:1000 height:370 PlotArea = left:40 right:235 bottom:50 top:50 Colors = id:period1 value:rgb(1,1,0.7) # light yellow id:period2 value:rgb(0.7,0.7,1) # light blue id:events value:rgb(1,0.7,1) # light purple id:era2 value:lightorange id:era1 Value:yellowgreen DateFormat = yyyy Period = from:-170 till:5500 TimeAxis = format:yyyy orientation:horizontal ScaleMajor = unit:year increment:1000 start:0 ScaleMinor = unit:year increment:100 start:-100 AlignBars = justify BarData = bar:Era bar:Events TextData = fontsize:M pos:(0,260) text:"Big" text:"Bang" • pos:(880,260) pos:(780,260) text:"Heat" text:"Death" • pos:(880,90) pos:(780,90) text:"log log" text:"year" PlotData= textcolor:black fontsize:M width:110 bar:Era mark:(line,white) align:left shift:(0,0) from:-170 till:90 shift:(0,35) color:era1 text:"Primordial Era" from:90 till:115 shift:(0,15) color:era2 text:"Stelliferous Era" from:115 till:317 shift:(0,-5) color:era1 text:"Degenerate Era" from:317 till:5000 shift:(0,-25) color:era2 text:"Ferrostelliferous Era" from:5000 till:5500 shift:(0,-45) color:era1 text:"Dark Era" width:110 bar:Events color:events align:left shift:(43,3) mark:(line,teal) at:-87 shift:(0,35) text:"One second" at:90 shift:(-2,15) text:"First star began to shine" at:101 shift:(-2,-5) text:"13.8 billion years, the present day" at:115 shift:(0,-25) text:"The last star has died" at:200 shift:(0,-45) text:"The last supermassive black holes have evaporated" at:317 shift:(0,40) text:"The first iron stars form" at:5000 shift:(0,0) text:"The last iron stars collapse into black holes" == See also ==
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