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It has been suggested that this article or section be merged with 1 E-25 s, 1 E-24 s, 1 E-21 s, 1 E-18 s, 1 E-15 s, 1 E-12 s, 1 E-11 s, 1 E-10 s, 1 E-9 s, 1 E-8 s, 1 E-7 s, 1 E-6 s, 1 E-5 s, 1 E-4 s, Millisecond, 1 E-2 s, 1 E-1 s, 1 E0 s and 1 E1 s to form Time. (Discuss)

It has been suggested that this article or section be merged with 1 E2 s, Kilosecond, 1 E4 s, 1 E5 s, 1 E6 s, 1 E7 s, 1 E8 s, 1 E9 s, 1 E10 s, 1 E11 s, 1 E12 s, 1 E13 s, 1 E14 s, 1 E15 s, 1 E16 s, 1 E17 s, 1 E18 s, 1 E19 s and more, Orders of magnitude (time) and second to form Time. (Discuss)

Main article: Orders of magnitude (time)

To help compare orders of magnitude of different times, this page lists times longer than 10¹⁹ seconds (317 billion years). See also Ultimate fate of the Universe.

• 3.3 × 10¹² years – According to the traditional Vedic time of Hinduism, this is the lifetime of Brahma.^{[citation needed]}

Some radioisotopes have extremely long half-lives:

• (1.4 ± 0.4) × 10¹⁷ years – vanadium-50
• (1.9 ± 0.2) × 10¹⁹ years – bismuth-209
• (3.1 ± 0.4) × 10¹⁹ years – cadmium-116
• (2.2 ± 0.3) × 10²⁴ years – tellurium-128

The following times all assume that the Universe is "open"; that is to say that it will continue indefinitely and not collapse in upon itself within a finite timescale.

• 3 trillion years -- point at which the nearest galaxies will recede beyond the cosmic light horizon.
• 200 trillion years – the estimated time until low-mass stars cool off. The smallest red dwarf stars are the longest-lived stars, and are believed to have a lifetime of up to 14 trillion years (1.4 x 10¹³ years). Star formation is expected to cease in galaxies in about 10¹³ to 10¹⁴ years as galaxies are depleted of the gas clouds they need to form stars. The longest-lived stars formed from the last gas clouds will therefore cool off after about 2 x 10¹⁴ years.
• 10¹⁵ years – the estimated time until planets detach from stars. Whenever two stars pass close to each other, the orbits of the planets can be disrupted and the planets can be ejected from orbit around their parent star. Planets that orbit closer to their stars take longer to be ejected in this manner on average because a passing star must make a closer pass to the planet's star to eject the planet.
• 10¹⁹ years – the estimated time until stars detach from galaxies. When two stars pass close enough to each other, the stars exchange orbital energy with lower-mass stars tending to gain energy. The lower-mass stars can gain enough energy in this manner through repeated encounters to be ejected from the galaxy. This process can cause the galaxy to eject the majority of its stars.
• 10²⁰ years – the estimated time until orbits decay by gravitational radiation
• 10³⁰ years – the estimated time until galaxies disappear due to black holes
• 10³⁶ years – the estimated half-life for proton decay, if GUT is right
• 10⁴⁰ years – the estimated expiration of all protons in the universe due to proton decay, if GUT is right (probability dictates only less than one proton in the universe will survive its half-life if its true value is close to the theoretical lower bound)
• 10⁴⁵ years – the estimated half-life of theorized radioactive decay of protons by virtual black holes, if they exist ^[1]
• 10⁶⁴ years – the estimated time until black holes decay by the Hawking process
• 10⁶⁵ years – the estimated timescale at which all matter is liquid at zero temperature due to tunneling effects
• 10¹⁰⁰ years (a googol year) – the estimated time until supermassive black holes decay by the Hawking process
• 10¹⁵⁰⁰ years – the estimated time until all matter decays to iron (if the proton does not decay). See isotopes of iron.

An alternative could be the following also according to Freeman Dyson's "Time without end: physics and biology in an open universe"

• 10¹⁰²⁶ years – low estimate for the time until all matter collapses into black holes, assuming no proton decay
• 10¹⁰⁷⁶ years – high estimate for the time until all matter collapses into neutron stars or black holes, again assuming no proton decay.^[2]

This time assumes a statistical model subject to Poincaré recurrence. A much simplified way of thinking about this time is in a model where our universe's history repeats itself arbitrarily many times due to properties of statistical mechanics, this is the time scale when it will first be somewhat similar (for a reasonable choice of "similar") to its current state again.

• 10¹⁰¹¹⁰⁰ years – scale of an estimated Poincaré recurrence time for the quantum state of a hypothetical box containing a black hole with the estimated mass of our entire universe.

1. ^ Adams, Fred C.; Kane, Gordon L.; Mbonye, Manasse; Perry, Malcolm J. (2000). "Proton Decay, Black Holes, and Large Extra Dimensions" (PDF). Int.J.Mod.Phys. A16 (2001) 2399-2410. Retrieved on 2006-12-27.
2. ^ Dyson, Freeman: Reviews of Modern Physics, Vol. 51, No. 3, July 1979(c) 1979 American Physical Society

• Dyson, Freeman. Time without End: Physics and Biology in an Open Universe. Reviews of Modern Physics, Vol. 51, No. 3, July 1979
• Poincaré recurrence and large numbers