Wikipedia

Faster-than-light

(Redirected from Causality problem)
For other uses, see Faster-than-light (disambiguation).

Faster-than-light (superluminal or supercausal) travel and communication are the conjectural propagation of matter or information faster than the speed of light (c). The special theory of relativity implies that only particles with zero rest mass (i.e., photons) may travel at the speed of light, and that nothing may travel faster.

Because the sphere travels faster than light, the observer sees nothing until it has already passed. Then, two images appear: one of the sphere arriving (on the right) and one of it departing (on the left).

Particles whose speed exceeds that of light (tachyons) have been hypothesized, but their existence would violate causality and would imply time travel. The scientific consensus is that they do not exist.

According to all observations and current scientific theories, matter travels at slower-than-light (subluminal) speed with respect to the locally distorted spacetime region. Speculative faster-than-light concepts include the Alcubierre drive, Krasnikov tubes, traversable wormholes, and quantum tunneling.[1][2] Some of these proposals find loopholes around general relativity, such as by expanding or contracting space to make the object appear to be travelling greater than c. Such proposals are still widely believed to be impossible as they still violate current understandings of causality, and they all require fanciful mechanisms to work (such as requiring exotic matter).

Superluminal travel of non-information

edit
Main article: Superluminal motion

In the context of this article, "faster-than-light" means the transmission of information or matter faster than c, a constant equal to the speed of light in vacuum, which is 299,792,458 m/s (by definition of the metre)[3] or about 186,282.397 miles per second. This is not quite the same as traveling faster than light, since:

  • Some processes propagate faster than c, but cannot carry information (see examples in the sections immediately following).
  • In some materials where light travels at speed c/n (where n is the refractive index) other particles can travel faster than c/n (but still slower than c), leading to Cherenkov radiation (see phase velocity below).

Neither of these phenomena violates special relativity or creates problems with causality, and thus neither qualifies as faster-than-light as described here.

In the following examples, certain influences may appear to travel faster than light, but they do not convey energy or information faster than light, so they do not violate special relativity.

Daily sky motion

edit

For an earth-bound observer, objects in the sky complete one revolution around the Earth in one day. Proxima Centauri, the nearest star outside the Solar System, is about four and a half light-years away.[4] In this frame of reference, in which Proxima Centauri is perceived to be moving in a circular trajectory with a radius of four light years, it could be described as having a speed many times greater than c as the rim speed of an object moving in a circle is a product of the radius and angular speed.[4] It is also possible on a geostatic view, for objects such as comets to vary their speed from subluminal to superluminal and vice versa simply because the distance from the Earth varies. Comets may have orbits which take them out to more than 1000 AU.[5] The circumference of a circle with a radius of 1000 AU is greater than one light day. In other words, a comet at such a distance is superluminal in a geostatic, and therefore non-inertial, frame.

Light spots and shadows

edit

If a laser beam is swept across a distant object, the spot of laser light can seem to move across the object at a speed greater than c.[6] Similarly, a shadow projected onto a distant object seems to move across the object faster than c.[6] In neither case does the light travel from the source to the object faster than c, nor does any information travel faster than light. No object is moving in these examples. For comparison, consider water squirting out of a garden hose as it is swung side to side: water does not instantly follow the direction of the hose.[6][7][8]

Closing speeds

edit

The rate at which two objects in motion in a single frame of reference get closer together is called the mutual or closing speed. This may approach twice the speed of light, as in the case of two particles travelling at close to the speed of light in opposite directions with respect to the reference frame.

Imagine two fast-moving particles approaching each other from opposite sides of a particle accelerator of the collider type. The closing speed would be the rate at which the distance between the two particles is decreasing. From the point of view of an observer standing at rest relative to the accelerator, this rate will be slightly less than twice the speed of light.

Special relativity does not prohibit this. It tells us that it is wrong to use Galilean relativity to compute the velocity of one of the particles, as would be measured by an observer traveling alongside the other particle. That is, special relativity gives the correct velocity-addition formula for computing such relative velocity.

It is instructive to compute the relative velocity of particles moving at v and −v in accelerator frame, which corresponds to the closing speed of 2v > c. Expressing the speeds in units of c, β = v/c:

 

Proper speeds

edit

If a spaceship travels to a planet one light-year (as measured in the Earth's rest frame) away from Earth at high speed, the time taken to reach that planet could be less than one year as measured by the traveller's clock (although it will always be more than one year as measured by a clock on Earth). The value obtained by dividing the distance traveled, as determined in the Earth's frame, by the time taken, measured by the traveller's clock, is known as a proper speed or a proper velocity. There is no limit on the value of a proper speed as a proper speed does not represent a speed measured in a single inertial frame. A light signal that left the Earth at the same time as the traveller would always get to the destination before the traveller would.

Phase velocities above c

edit

The phase velocity of an electromagnetic wave, when traveling through a medium, can routinely exceed c, the vacuum velocity of light. For example, this occurs in most glasses at X-ray frequencies.[9] However, the phase velocity of a wave corresponds to the propagation speed of a theoretical single-frequency (purely monochromatic) component of the wave at that frequency. Such a wave component must be infinite in extent and of constant amplitude (otherwise it is not truly monochromatic), and so cannot convey any information.[10] Thus a phase velocity above c does not imply the propagation of signals with a velocity above c.[11]

Group velocities above c

edit

The group velocity of a wave may also exceed c in some circumstances.[12][13] In such cases, which typically at the same time involve rapid attenuation of the intensity, the maximum of the envelope of a pulse may travel with a velocity above c. However, even this situation does not imply the propagation of signals with a velocity above c,[14] even though one may be tempted to associate pulse maxima with signals. The latter association has been shown to be misleading, because the information on the arrival of a pulse can be obtained before the pulse maximum arrives. For example, if some mechanism allows the full transmission of the leading part of a pulse while strongly attenuating the pulse maximum and everything behind (distortion), the pulse maximum is effectively shifted forward in time, while the information on the pulse does not come faster than c without this effect.[15] However, group velocity can exceed c in some parts of a Gaussian beam in vacuum (without attenuation). The diffraction causes the peak of the pulse to propagate faster, while overall power does not.[16]

Cosmic expansion

edit

According to Hubble's law, the expansion of the universe causes distant galaxies to recede from us faster than the speed of light. However, the recession speed associated with Hubble's law, defined as the rate of increase in proper distance per interval of cosmological time, is not a velocity in a relativistic sense. Moreover, in general relativity, velocity is a local notion, and there is not even a unique definition for the relative velocity of a cosmologically distant object.[17] Faster-than-light cosmological recession speeds are entirely a coordinate effect.

There are many galaxies visible in telescopes with redshift numbers of 1.4 or higher. All of these have cosmological recession speeds greater than the speed of light. Because the Hubble parameter is decreasing with time, there can actually be cases where a galaxy that is receding from us faster than light does manage to emit a signal which reaches us eventually.[18][19][20]

However, because the expansion of the universe is accelerating, it is projected that most galaxies will eventually cross a type of cosmological event horizon where any light they emit past that point will never be able to reach us at any time in the infinite future,[21] because the light never reaches a point where its "peculiar velocity" towards us exceeds the expansion velocity away from us (these two notions of velocity are also discussed in Comoving and proper distances#Uses of the proper distance). The current distance to this cosmological event horizon is about 16 billion light-years, meaning that a signal from an event happening at present would eventually be able to reach us in the future if the event was less than 16 billion light-years away, but the signal would never reach us if the event was more than 16 billion light-years away.[19]

Astronomical observations

edit

Apparent superluminal motion is observed in many radio galaxies, blazars, quasars, and recently also in microquasars. The effect was predicted before it was observed by Martin Rees[clarification needed] and can be explained as an optical illusion caused by the object partly moving in the direction of the observer,[22] when the speed calculations assume it does not. The phenomenon does not contradict the theory of special relativity. Corrected calculations show these objects have velocities close to the speed of light (relative to our reference frame). They are the first examples of large amounts of mass moving at close to the speed of light.[23] Earth-bound laboratories have only been able to accelerate small numbers of elementary particles to such speeds.

Quantum mechanics

edit

Certain phenomena in quantum mechanics, such as quantum entanglement, might give the superficial impression of allowing communication of information faster than light. According to the no-communication theorem these phenomena do not allow true communication; they only let two observers in different locations see the same system simultaneously, without any way of controlling what either sees. Wavefunction collapse can be viewed as an epiphenomenon of quantum decoherence, which in turn is nothing more than an effect of the underlying local time evolution of the wavefunction of a system and all of its environment. Since the underlying behavior does not violate local causality or allow FTL communication, it follows that neither does the additional effect of wavefunction collapse, whether real or apparent.

The uncertainty principle implies that individual photons may travel for short distances at speeds somewhat faster (or slower) than c, even in vacuum; this possibility must be taken into account when enumerating Feynman diagrams for a particle interaction.[24] However, it was shown in 2011 that a single photon may not travel faster than c.[25]

There have been various reports in the popular press of experiments on faster-than-light transmission in optics — most often in the context of a kind of quantum tunnelling phenomenon. Usually, such reports deal with a phase velocity or group velocity faster than the vacuum velocity of light.[26][27] However, as stated above, a superluminal phase velocity cannot be used for faster-than-light transmission of information[28][29]

Hartman effect

edit
Main article: Hartman effect

The Hartman effect is the tunneling effect through a barrier where the tunneling time tends to a constant for large barriers.[30][31] This could, for instance, be the gap between two prisms. When the prisms are in contact, the light passes straight through, but when there is a gap, the light is refracted. There is a non-zero probability that the photon will tunnel across the gap rather than follow the refracted path.

However, it has been claimed that the Hartman effect cannot actually be used to violate relativity by transmitting signals faster than c, also because the tunnelling time "should not be linked to a velocity since evanescent waves do not propagate".[32] The evanescent waves in the Hartman effect are due to virtual particles and a non-propagating static field, as mentioned in the sections above for gravity and electromagnetism.

Casimir effect

edit
Main article: Casimir effect

In physics, the Casimir–Polder force is a physical force exerted between separate objects due to resonance of vacuum energy in the intervening space between the objects. This is sometimes described in terms of virtual particles interacting with the objects, owing to the mathematical form of one possible way of calculating the strength of the effect. Because the strength of the force falls off rapidly with distance, it is only measurable when the distance between the objects is extremely small. Because the effect is due to virtual particles mediating a static field effect, it is subject to the comments about static fields discussed above.

EPR paradox

edit
Main article: EPR paradox

The EPR paradox refers to a famous thought experiment of Albert Einstein, Boris Podolsky and Nathan Rosen that was realized experimentally for the first time by Alain Aspect in 1981 and 1982 in the Aspect experiment. In this experiment, the two measurements of an entangled state are correlated even when the measurements are distant from the source and each other. However, no information can be transmitted this way; the answer to whether or not the measurement actually affects the other quantum system comes down to which interpretation of quantum mechanics one subscribes to.

An experiment performed in 1997 by Nicolas Gisin has demonstrated quantum correlations between particles separated by over 10 kilometers.[33] But as noted earlier, the non-local correlations seen in entanglement cannot actually be used to transmit classical information faster than light, so that relativistic causality is preserved. The situation is akin to sharing a synchronized coin flip, where the second person to flip their coin will always see the opposite of what the first person sees, but neither has any way of knowing whether they were the first or second flipper, without communicating classically. See No-communication theorem for further information. A 2008 quantum physics experiment also performed by Nicolas Gisin and his colleagues has determined that in any hypothetical non-local hidden-variable theory, the speed of the quantum non-local connection (what Einstein called "spooky action at a distance") is at least 10,000 times the speed of light.[34]

Delayed choice quantum eraser

edit
Main article: Delayed-choice quantum eraser

The delayed-choice quantum eraser is a version of the EPR paradox in which the observation (or not) of interference after the passage of a photon through a double slit experiment depends on the conditions of observation of a second photon entangled with the first. The characteristic of this experiment is that the observation of the second photon can take place at a later time than the observation of the first photon,[35] which may give the impression that the measurement of the later photons "retroactively" determines whether the earlier photons show interference or not, although the interference pattern can only be seen by correlating the measurements of both members of every pair and so it cannot be observed until both photons have been measured, ensuring that an experimenter watching only the photons going through the slit does not obtain information about the other photons in an faster-than-light or backwards-in-time manner.[36][37]

Superluminal communication

edit
Main article: Superluminal communication

Faster-than-light communication is, according to relativity, equivalent to time travel. What we measure as the speed of light in vacuum (or near vacuum) is actually the fundamental physical constant c. This means that all inertial and, for the coordinate speed of light, non-inertial observers, regardless of their relative velocity, will always measure zero-mass particles such as photons traveling at c in vacuum. This result means that measurements of time and velocity in different frames are no longer related simply by constant shifts, but are instead related by Poincaré transformations. These transformations have important implications:

  • The relativistic momentum of a massive particle would increase with speed in such a way that at the speed of light an object would have infinite momentum.
  • To accelerate an object of non-zero rest mass to c would require infinite time with any finite acceleration, or infinite acceleration for a finite amount of time.
  • Either way, such acceleration requires infinite energy.
  • Some observers with sub-light relative motion will disagree about which occurs first of any two events that are separated by a space-like interval.[38] In other words, any travel that is faster-than-light will be seen as traveling backwards in time in some other, equally valid, frames of reference,[39] or need to assume the speculative hypothesis of possible Lorentz violations at a presently unobserved scale (for instance the Planck scale).[citation needed] Therefore, any theory which permits "true" FTL also has to cope with time travel and all its associated paradoxes,[40] or else to assume the Lorentz invariance to be a symmetry of thermodynamical statistical nature (hence a symmetry broken at some presently unobserved scale).
  • In special relativity the coordinate speed of light is only guaranteed to be c in an inertial frame; in a non-inertial frame the coordinate speed may be different from c.[41] In general relativity no coordinate system on a large region of curved spacetime is "inertial", so it is permissible to use a global coordinate system where objects travel faster than c, but in the local neighborhood of any point in curved spacetime we can define a "local inertial frame" and the local speed of light will be c in this frame,[42] with massive objects moving through this local neighborhood always having a speed less than c in the local inertial frame.

Justifications

edit

Casimir vacuum and quantum tunnelling

edit

Special relativity postulates that the speed of light in vacuum is invariant in inertial frames. That is, it will be the same from any frame of reference moving at a constant speed. The equations do not specify any particular value for the speed of light, which is an experimentally determined quantity for a fixed unit of length. Since 1983, the SI unit of length (the meter) has been defined using the speed of light.

The experimental determination has been made in vacuum. However, the vacuum we know is not the only possible vacuum which can exist. The vacuum has energy associated with it, called simply the vacuum energy, which could perhaps be altered in certain cases.[43] When vacuum energy is lowered, light itself has been predicted to go faster than the standard value c. This is known as the Scharnhorst effect. Such a vacuum can be produced by bringing two perfectly smooth metal plates together at near atomic diameter spacing. It is called a Casimir vacuum. Calculations imply that light will go faster in such a vacuum by a minuscule amount: a photon traveling between two plates that are 1 micrometer apart would increase the photon's speed by only about one part in 1036.[44] Accordingly, there has as yet been no experimental verification of the prediction. A recent analysis[45] argued that the Scharnhorst effect cannot be used to send information backwards in time with a single set of plates since the plates' rest frame would define a "preferred frame" for FTL signaling. However, with multiple pairs of plates in motion relative to one another the authors noted that they had no arguments that could "guarantee the total absence of causality violations", and invoked Hawking's speculative chronology protection conjecture which suggests that feedback loops of virtual particles would create "uncontrollable singularities in the renormalized quantum stress-energy" on the boundary of any potential time machine, and thus would require a theory of quantum gravity to fully analyze. Other authors argue that Scharnhorst's original analysis, which seemed to show the possibility of faster-than-c signals, involved approximations which may be incorrect, so that it is not clear whether this effect could actually increase signal speed at all.[46]

It was later claimed by Eckle et al. that particle tunneling does indeed occur in zero real time.[47] Their tests involved tunneling electrons, where the group argued a relativistic prediction for tunneling time should be 500–600 attoseconds (an attosecond is one quintillionth (10−18) of a second). All that could be measured was 24 attoseconds, which is the limit of the test accuracy. Again, though, other physicists believe that tunneling experiments in which particles appear to spend anomalously short times inside the barrier are in fact fully compatible with relativity, although there is disagreement about whether the explanation involves reshaping of the wave packet or other effects.[48][49][50]

Give up (absolute) relativity

edit

Because of the strong empirical support for special relativity, any modifications to it must necessarily be quite subtle and difficult to measure. The best-known attempt is doubly special relativity, which posits that the Planck length is also the same in all reference frames, and is associated with the work of Giovanni Amelino-Camelia and João Magueijo.[51][52] There are speculative theories that claim inertia is produced by the combined mass of the universe (e.g., Mach's principle), which implies that the rest frame of the universe might be preferred by conventional measurements of natural law. If confirmed, this would imply special relativity is an approximation to a more general theory, but since the relevant comparison would (by definition) be outside the observable universe, it is difficult to imagine (much less construct) experiments to test this hypothesis. Despite this difficulty, such experiments have been proposed.[53]

Spacetime distortion

edit

Although the theory of special relativity forbids objects to have a relative velocity greater than light speed, and general relativity reduces to special relativity in a local sense (in small regions of spacetime where curvature is negligible), general relativity does allow the space between distant objects to expand in such a way that they have a "recession velocity" which exceeds the speed of light, and it is thought that galaxies which are at a distance of more than about 14 billion light-years from us today have a recession velocity which is faster than light.[19] Miguel Alcubierre theorized that it would be possible to create a warp drive, in which a ship would be enclosed in a "warp bubble" where the space at the front of the bubble is rapidly contracting and the space at the back is rapidly expanding, with the result that the bubble can reach a distant destination much faster than a light beam moving outside the bubble, but without objects inside the bubble locally traveling faster than light.[54] However, several objections raised against the Alcubierre drive appear to rule out the possibility of actually using it in any practical fashion. Another possibility predicted by general relativity is the traversable wormhole, which could create a shortcut between arbitrarily distant points in space. As with the Alcubierre drive, travelers moving through the wormhole would not locally move faster than light travelling through the wormhole alongside them, but they would be able to reach their destination (and return to their starting location) faster than light traveling outside the wormhole.

Gerald Cleaver and Richard Obousy, a professor and student of Baylor University, theorized that manipulating the extra spatial dimensions of string theory around a spaceship with an extremely large amount of energy would create a "bubble" that could cause the ship to travel faster than the speed of light. To create this bubble, the physicists believe manipulating the 10th spatial dimension would alter the dark energy in three large spatial dimensions: height, width and length. Cleaver said positive dark energy is currently responsible for speeding up the expansion rate of our universe as time moves on.[55]

Lorentz symmetry violation

edit
Main articles: Modern searches for Lorentz violation and Standard-Model Extension

The possibility that Lorentz symmetry may be violated has been seriously considered in the last two decades, particularly after the development of a realistic effective field theory that describes this possible violation, the so-called Standard-Model Extension.[56][57][58] This general framework has allowed experimental searches by ultra-high energy cosmic-ray experiments[59] and a wide variety of experiments in gravity, electrons, protons, neutrons, neutrinos, mesons, and photons.[60] The breaking of rotation and boost invariance causes direction dependence in the theory as well as unconventional energy dependence that introduces novel effects, including Lorentz-violating neutrino oscillations and modifications to the dispersion relations of different particle species, which naturally could make particles move faster than light.

In some models of broken Lorentz symmetry, it is postulated that the symmetry is still built into the most fundamental laws of physics, but that spontaneous symmetry breaking of Lorentz invariance[61] shortly after the Big Bang could have left a "relic field" throughout the universe which causes particles to behave differently depending on their velocity relative to the field;[62] however, there are also some models where Lorentz symmetry is broken in a more fundamental way. If Lorentz symmetry can cease to be a fundamental symmetry at the Planck scale or at some other fundamental scale, it is conceivable that particles with a critical speed different from the speed of light be the ultimate constituents of matter.

In current models of Lorentz symmetry violation, the phenomenological parameters are expected to be energy-dependent. Therefore, as widely recognized,[63][64] existing low-energy bounds cannot be applied to high-energy phenomena; however, many searches for Lorentz violation at high energies have been carried out using the Standard-Model Extension.[60] Lorentz symmetry violation is expected to become stronger as one gets closer to the fundamental scale.

Superfluid theories of physical vacuum

edit
Main article: Superfluid vacuum theory

In this approach, the physical vacuum is viewed as a quantum superfluid which is essentially non-relativistic, whereas Lorentz symmetry is not an exact symmetry of nature but rather the approximate description valid only for the small fluctuations of the superfluid background.[65] Within the framework of the approach, a theory was proposed in which the physical vacuum is conjectured to be a quantum Bose liquid whose ground-state wavefunction is described by the logarithmic Schrödinger equation. It was shown that the relativistic gravitational interaction arises as the small-amplitude collective excitation mode[66] whereas relativistic elementary particles can be described by the particle-like modes in the limit of low momenta.[67] The important fact is that at very high velocities the behavior of the particle-like modes becomes distinct from the relativistic one – they can reach the speed of light limit at finite energy; also, faster-than-light propagation is possible without requiring moving objects to have imaginary mass.[68][69]

FTL neutrino flight results

edit

MINOS experiment

edit
Main article: MINOS

In 2007 the MINOS collaboration reported results measuring the flight-time of 3 GeV neutrinos yielding a speed exceeding that of light by 1.8-sigma significance.[70] However, those measurements were considered to be statistically consistent with neutrinos traveling at the speed of light.[71] After the detectors for the project were upgraded in 2012, MINOS corrected their initial result and found agreement with the speed of light. Further measurements are going to be conducted.[72]

OPERA neutrino anomaly

edit
Main article: Faster-than-light neutrino anomaly

On September 22, 2011, a preprint[73] from the OPERA Collaboration indicated detection of 17 and 28 GeV muon neutrinos, sent 730 kilometers (454 miles) from CERN near Geneva, Switzerland to the Gran Sasso National Laboratory in Italy, traveling faster than light by a relative amount of 2.48×10−5 (approximately 1 in 40,000), a statistic with 6.0-sigma significance.[74] On 17 November 2011, a second follow-up experiment by OPERA scientists confirmed their initial results.[75][76] However, scientists were skeptical about the results of these experiments, the significance of which was disputed.[77] In March 2012, the ICARUS collaboration failed to reproduce the OPERA results with their equipment, detecting neutrino travel time from CERN to the Gran Sasso National Laboratory indistinguishable from the speed of light.[78] Later the OPERA team reported two flaws in their equipment set-up that had caused errors far outside their original confidence interval: a fiber-optic cable attached improperly, which caused the apparently faster-than-light measurements, and a clock oscillator ticking too fast.[79]

Tachyons

edit
Main article: Tachyon

In special relativity, it is impossible to accelerate an object to the speed of light, or for a massive object to move at the speed of light. However, it might be possible for an object to exist which always moves faster than light. The hypothetical elementary particles with this property are called tachyons or tachyonic particles. Attempts to quantize them failed to produce faster-than-light particles, and instead illustrated that their presence leads to an instability.[80][81]

Various theorists have suggested that the neutrino might have a tachyonic nature,[82][83][84][85] while others have disputed the possibility.[86]

General relativity

edit

General relativity was developed after special relativity to include concepts like gravity. It maintains the principle that no object can accelerate to the speed of light in the reference frame of any coincident observer.[citation needed] However, it permits distortions in spacetime that allow an object to move faster than light from the point of view of a distant observer.[citation needed] One such distortion is the Alcubierre drive, which can be thought of as producing a ripple in spacetime that carries an object along with it. Another possible system is the wormhole, which connects two distant locations as though by a shortcut. Both distortions would need to create a very strong curvature in a highly localized region of space-time and their gravity fields would be immense. To counteract the unstable nature, and prevent the distortions from collapsing under their own 'weight', one would need to introduce hypothetical exotic matter or negative energy.

General relativity also recognizes that any means of faster-than-light travel could also be used for time travel. This raises problems with causality. Many physicists believe that the above phenomena are impossible and that future theories of gravity will prohibit them. One theory states that stable wormholes are possible, but that any attempt to use a network of wormholes to violate causality would result in their decay.[citation needed] In string theory, Eric G. Gimon and Petr Hořava have argued[87] that in a supersymmetric five-dimensional Gödel universe, quantum corrections to general relativity effectively cut off regions of spacetime with causality-violating closed timelike curves. In particular, in the quantum theory a smeared supertube is present that cuts the spacetime in such a way that, although in the full spacetime a closed timelike curve passed through every point, no complete curves exist on the interior region bounded by the tube.

edit
See also: Space travel in science fiction

FTL travel is a common plot device in science fiction.[88]

See also

edit

Notes

edit
  1. ^ "Quantum-tunnelling time is measured using ultracold atoms". Physics World. 22 July 2020.
  2. ^ "Quanta Magazine". 20 October 2020.
  3. ^ "The 17th Conférence Générale des Poids et Mesures (CGPM) : Definition of the metre". bipm.org. Archived from the original on May 27, 2020. Retrieved July 5, 2020.
  4. ^ a b University of York Science Education Group (2001). Salter Horners Advanced Physics A2 Student Book. Heinemann. pp. 302–303. ISBN 978-0435628925.
  5. ^ "The Furthest Object in the Solar System". Information Leaflet No. 55. Royal Greenwich Observatory. 15 April 1996.
  6. ^ a b c Gibbs, P. (1997). "Is Faster-Than-Light Travel or Communication Possible?". The Original Usenet Physics FAQ. Retrieved 20 August 2008.
  7. ^ Salmon, W. C. (2006). Four Decades of Scientific Explanation. University of Pittsburgh Press. p. 107. ISBN 978-0-8229-5926-7.
  8. ^ Steane, A. (2012). The Wonderful World of Relativity: A Precise Guide for the General Reader. Oxford University Press. p. 180. ISBN 978-0-19-969461-7.
  9. ^ Hecht, E. (1987). Optics (2nd ed.). Addison Wesley. p. 62. ISBN 978-0-201-11609-0.
  10. ^ Sommerfeld, A. (1907). "An Objection Against the Theory of Relativity and its Removal" . Physikalische Zeitschrift. 8 (23): 841–842.
  11. ^ Weber, J. (1954). "Phase, Group, and Signal Velocity". American Journal of Physics. 22 (9): 618. Bibcode:1954AmJPh..22..618W. doi:10.1119/1.1933858. Retrieved 2007-04-30.
  12. ^ Wang, L. J.; Kuzmich, A.; Dogariu, A. (2000). "Gain-assisted superluminal light propagation". Nature. 406 (6793): 277–279. Bibcode:2000Natur.406..277W. doi:10.1038/35018520. PMID 10917523. S2CID 4358601.
  13. ^ Bowlan, P.; Valtna-Lukner, H.; Lõhmus, M.; Piksarv, P.; Saari, P.; Trebino, R. (2009). "Measurement of the spatiotemporal electric field of ultrashort superluminal Bessel-X pulses". Optics and Photonics News. 20 (12): 42. Bibcode:2009OptPN..20...42M. doi:10.1364/OPN.20.12.000042. S2CID 122056218.
  14. ^ Brillouin, L. (1960). Wave Propagation and Group Velocity. Academic Press.
  15. ^ Withayachumnankul, W.; Fischer, B. M.; Ferguson, B.; Davis, B. R.; Abbott, D. (2010). "A Systemized View of Superluminal Wave Propagation" (PDF). Proceedings of the IEEE. 98 (10): 1775–1786. doi:10.1109/JPROC.2010.2052910. S2CID 15100571.
  16. ^ Horváth, Z. L.; Vinkó, J.; Bor, Zs.; von der Linde, D. (1996). "Acceleration of femtosecond pulses to superluminal velocities by Gouy phase shift" (PDF). Applied Physics B. 63 (5): 481–484. Bibcode:1996ApPhB..63..481H. doi:10.1007/BF01828944. S2CID 54757568. Archived (PDF) from the original on 2003-04-03.
  17. ^ Wright, E. L. (12 June 2009). "Cosmology Tutorial – Part 2". Ned Wright's Cosmology Tutorial. UCLA. Retrieved 2011-09-26.
  18. ^ See the last two paragraphs in Rothstein, D. (10 September 2003). "Is the universe expanding faster than the speed of light?". Ask an Astronomer.
  19. ^ a b c Lineweaver, C.; Davis, T. M. (March 2005). "Misconceptions about the Big Bang" (PDF). Scientific American. pp. 36–45. Archived (PDF) from the original on 2006-05-27. Retrieved 2008-11-06.
  20. ^ Davis, T. M.; Lineweaver, C. H. (2004). "Expanding Confusion: common misconceptions of cosmological horizons and the superluminal expansion of the universe". Publications of the Astronomical Society of Australia. 21 (1): 97–109. arXiv:astro-ph/0310808. Bibcode:2004PASA...21...97D. doi:10.1071/AS03040. S2CID 13068122.
  21. ^ Loeb, A. (2002). "The Long-Term Future of Extragalactic Astronomy". Physical Review D. 65 (4): 047301. arXiv:astro-ph/0107568. Bibcode:2002PhRvD..65d7301L. doi:10.1103/PhysRevD.65.047301. S2CID 1791226.
  22. ^ Rees, M. J. (1966). "Appearance of relativistically expanding radio sources". Nature. 211 (5048): 468–470. Bibcode:1966Natur.211..468R. doi:10.1038/211468a0. S2CID 41065207.
  23. ^ Blandford, R. D.; McKee, C. F.; Rees, M. J. (1977). "Super-luminal expansion in extragalactic radio sources". Nature. 267 (5608): 211–216. Bibcode:1977Natur.267..211B. doi:10.1038/267211a0. S2CID 4260167.
  24. ^ Grozin, A. (2007). Lectures on QED and QCD. World Scientific. p. 89. ISBN 978-981-256-914-1.
  25. ^ Zhang, S.; Chen, J. F.; Liu, C.; Loy, M. M. T.; Wong, G. K. L.; Du, S. (2011). "Optical Precursor of a Single Photon" (PDF). Physical Review Letters. 106 (24): 243602. Bibcode:2011PhRvL.106x3602Z. doi:10.1103/PhysRevLett.106.243602. PMID 21770570. Archived (PDF) from the original on 2019-12-05.
  26. ^ Kåhre, J. (2012). The Mathematical Theory of Information (Illustrated ed.). Springer Science & Business Media. p. 425. ISBN 978-1-4615-0975-2.
  27. ^ Steinberg, A. M. (1994). When Can Light Go Faster Than Light? (Thesis). University of California, Berkeley. p. 100. Bibcode:1994PhDT.......314S.
  28. ^ Chubb, J.; Eskandarian, A.; Harizanov, V. (2016). Logic and Algebraic Structures in Quantum Computing (Illustrated ed.). Cambridge University Press. p. 61. ISBN 978-1-107-03339-9.
  29. ^ Ehlers, J.; Lämmerzahl, C. (2006). Special Relativity: Will it Survive the Next 101 Years? (Illustrated ed.). Springer. p. 506. ISBN 978-3-540-34523-7.
  30. ^ Martinez, J. C.; Polatdemir, E. (2006). "Origin of the Hartman effect". Physics Letters A. 351 (1–2): 31–36. Bibcode:2006PhLA..351...31M. doi:10.1016/j.physleta.2005.10.076.
  31. ^ Hartman, T. E. (1962). "Tunneling of a Wave Packet". Journal of Applied Physics. 33 (12): 3427–3433. Bibcode:1962JAP....33.3427H. doi:10.1063/1.1702424.
  32. ^ Winful, H. G. (2006). "Tunneling time, the Hartman effect, and superluminality: A proposed resolution of an old paradox". Physics Reports. 436 (1–2): 1–69. Bibcode:2006PhR...436....1W. doi:10.1016/j.physrep.2006.09.002.
  33. ^ Suarez, A. (26 February 2015). "History". Center for Quantum Philosophy. Retrieved 2017-06-07.
  34. ^ Salart, D.; Baas, A.; Branciard, C.; Gisin, N.; Zbinden, H. (2008). "Testing spooky action at a distance". Nature. 454 (7206): 861–864. arXiv:0808.3316. Bibcode:2008Natur.454..861S. doi:10.1038/nature07121. PMID 18704081. S2CID 4401216.
  35. ^ Kim, Yoon-Ho; Yu, Rong; Kulik, Sergei P.; Shih, Yanhua; Scully, Marlan O. (2000). "Delayed "Choice" Quantum Eraser". Physical Review Letters. 84 (1): 1–5. arXiv:quant-ph/9903047. Bibcode:2000PhRvL..84....1K. doi:10.1103/PhysRevLett.84.1. PMID 11015820. S2CID 5099293.
  36. ^ Hillmer, R.; Kwiat, P. (16 April 2017). "Delayed-Choice Experiments". Scientific American.
  37. ^ Motl, L. (November 2010). "Delayed choice quantum eraser". The Reference Frame.
  38. ^ Einstein, A. (1927). Relativity:the special and the general theory. Methuen & Co. pp. 25–27.
  39. ^ Odenwald, S. "If we could travel faster than light, could we go back in time?". NASA Astronomy Café. Retrieved 7 April 2014.
  40. ^ Gott, J. R. (2002). Time Travel in Einstein's Universe. Mariner Books. pp. 82–83. ISBN 978-0618257355.
  41. ^ Petkov, V. (2009). Relativity and the Nature of Spacetime. Springer Science & Business Media. p. 219. ISBN 978-3642019623.
  42. ^ Raine, D. J.; Thomas, E. G. (2001). An Introduction to the Science of Cosmology. CRC Press. p. 94. ISBN 978-0750304054.
  43. ^ "What is the 'zero-point energy' (or 'vacuum energy') in quantum physics? Is it really possible that we could harness this energy?". Scientific American. 1997-08-18. Retrieved 2009-05-27.
  44. ^ Scharnhorst, Klaus (1990-05-12). "Secret of the vacuum: Speedier light". Vrije Universiteit Amsterdam. Retrieved 2009-05-27.
  45. ^ Liberati, Stefano; Sonego, Sebastiano; Visser, Matt (2002). "Faster-than-c Signals, Special Relativity, and Causality". Annals of Physics. 298 (1): 167–185. arXiv:gr-qc/0107091. Bibcode:2002AnPhy.298..167L. doi:10.1006/aphy.2002.6233. S2CID 48166.
  46. ^ Fearn, H. (2007). "Can light signals travel faster than c in nontrivial vacua in flat space-time? Relativistic causality II". Laser Physics. 17 (5): 695–699. arXiv:0706.0553. Bibcode:2007LaPhy..17..695F. doi:10.1134/S1054660X07050155. ISSN 1054-660X. S2CID 61962.
  47. ^ Eckle, P.; Pfeiffer, A. N.; Cirelli, C.; Staudte, A.; Dorner, R.; Muller, H. G.; Buttiker, M.; Keller, U. (5 December 2008). "Attosecond Ionization and Tunneling Delay Time Measurements in Helium". Science. 322 (5907): 1525–1529. Bibcode:2008Sci...322.1525E. doi:10.1126/science.1163439. PMID 19056981. S2CID 206515239.
  48. ^ Winful, Herbert G. (December 2006). "Tunneling time, the Hartman effect, and superluminality: A proposed resolution of an old paradox" (PDF). Physics Reports. 436 (1–2): 1–69. Bibcode:2006PhR...436....1W. doi:10.1016/j.physrep.2006.09.002. Archived from the original (PDF) on 2011-12-18. Retrieved 2010-06-08.
  49. ^ For a summary of Herbert G. Winful's explanation for apparently superluminal tunneling time which does not involve reshaping, see Winful, Herbert (2007). "New paradigm resolves old paradox of faster-than-light tunneling". SPIE Newsroom. doi:10.1117/2.1200711.0927.
  50. ^ Sokolovski, D. (8 February 2004). "Why does relativity allow quantum tunneling to 'take no time'?". Proceedings of the Royal Society A. 460 (2042): 499–506. Bibcode:2004RSPSA.460..499S. doi:10.1098/rspa.2003.1222. S2CID 122620657.
  51. ^ Amelino-Camelia, Giovanni (1 November 2009). "Doubly-Special Relativity: Facts, Myths and Some Key Open Issues". Recent Developments in Theoretical Physics. Statistical Science and Interdisciplinary Research. Vol. 9. pp. 123–170. arXiv:1003.3942. doi:10.1142/9789814287333_0006. ISBN 978-981-4287-32-6. S2CID 118855372.
  52. ^ Amelino-Camelia, Giovanni (1 July 2002). "Doubly Special Relativity". Nature. 418 (6893): 34–35. arXiv:gr-qc/0207049. Bibcode:2002Natur.418...34A. doi:10.1038/418034a. PMID 12097897. S2CID 16844423.
  53. ^ Chang, Donald C. (March 22, 2017). "Is there a resting frame in the universe? A proposed experimental test based on a precise measurement of particle mass". The European Physical Journal Plus. 132 (3): 140. arXiv:1706.05252. Bibcode:2017EPJP..132..140C. doi:10.1140/epjp/i2017-11402-4.
  54. ^ Alcubierre, Miguel (1 May 1994). "The warp drive: hyper-fast travel within general relativity". Classical and Quantum Gravity. 11 (5): L73–L77. arXiv:gr-qc/0009013. Bibcode:1994CQGra..11L..73A. CiteSeerX 10.1.1.338.8690. doi:10.1088/0264-9381/11/5/001. S2CID 4797900.
  55. ^ "Traveling Faster Than the Speed of Light: A New Idea That Could Make It Happen". www.newswise.com. Retrieved 2023-08-24.
  56. ^ Colladay, Don; Kostelecký, V. Alan (1997). "CPT violation and the standard model". Physical Review D. 55 (11): 6760–6774. arXiv:hep-ph/9703464. Bibcode:1997PhRvD..55.6760C. doi:10.1103/PhysRevD.55.6760. S2CID 7651433.
  57. ^ Colladay, Don; Kostelecký, V. Alan (1998). "Lorentz-violating extension of the standard model". Physical Review D. 58 (11): 116002. arXiv:hep-ph/9809521. Bibcode:1998PhRvD..58k6002C. doi:10.1103/PhysRevD.58.116002. S2CID 4013391.
  58. ^ Kostelecký, V. Alan (2004). "Gravity, Lorentz violation, and the standard model". Physical Review D. 69 (10): 105009. arXiv:hep-th/0312310. Bibcode:2004PhRvD..69j5009K. doi:10.1103/PhysRevD.69.105009. S2CID 55185765.
  59. ^ Gonzalez-Mestres, Luis (2009). "AUGER-HiRes results and models of Lorentz symmetry violation". Nuclear Physics B - Proceedings Supplements. 190: 191–197. arXiv:0902.0994. Bibcode:2009NuPhS.190..191G. doi:10.1016/j.nuclphysbps.2009.03.088. S2CID 14848782.
  60. ^ a b Kostelecký, V. Alan; Russell, Neil (2011). "Data tables for Lorentz and CPT violation". Reviews of Modern Physics. 83 (1): 11–31. arXiv:0801.0287. Bibcode:2011RvMP...83...11K. doi:10.1103/RevModPhys.83.11. S2CID 3236027.
  61. ^ Kostelecký, V. A.; Samuel, S. (15 January 1989). "Spontaneous breaking of Lorentz symmetry in string theory" (PDF). Physical Review D. 39 (2): 683–685. Bibcode:1989PhRvD..39..683K. doi:10.1103/PhysRevD.39.683. hdl:2022/18649. PMID 9959689. Archived (PDF) from the original on 2021-07-13.
  62. ^ "PhysicsWeb – Breaking Lorentz symmetry". PhysicsWeb. 2004-04-05. Archived from the original on 2004-04-05. Retrieved 2011-09-26.
  63. ^ Mavromatos, Nick E. (15 August 2002). "Testing models for quantum gravity". CERN Courier.
  64. ^ Overbye, Dennis (2002-12-31). "Interpreting the Cosmic Rays". The New York Times. ISSN 0362-4331. Retrieved 2023-08-24.
  65. ^ Volovik, G. E. (2003). "The Universe in a helium droplet". International Series of Monographs on Physics. 117: 1–507.
  66. ^ Zloshchastiev, Konstantin G. (2011). "Spontaneous symmetry breaking and mass generation as built-in phenomena in logarithmic nonlinear quantum theory". Acta Physica Polonica B. 42 (2): 261–292. arXiv:0912.4139. Bibcode:2011AcPPB..42..261Z. doi:10.5506/APhysPolB.42.261. S2CID 118152708.
  67. ^ Avdeenkov, Alexander V.; Zloshchastiev, Konstantin G. (2011). "Quantum Bose liquids with logarithmic nonlinearity: Self-sustainability and emergence of spatial extent". Journal of Physics B: Atomic, Molecular and Optical Physics. 44 (19): 195303. arXiv:1108.0847. Bibcode:2011JPhB...44s5303A. doi:10.1088/0953-4075/44/19/195303. S2CID 119248001.
  68. ^ Zloshchastiev, Konstantin G.; Chakrabarti, Sandip K.; Zhuk, Alexander I.; Bisnovatyi-Kogan, Gennady S. (2010). "Logarithmic nonlinearity in theories of quantum gravity: Origin of time and observational consequences". American Institute of Physics Conference Series. AIP Conference Proceedings. 1206: 288–297. arXiv:0906.4282. Bibcode:2010AIPC.1206..112Z. doi:10.1063/1.3292518.
  69. ^ Zloshchastiev, Konstantin G. (2011). "Vacuum Cherenkov effect in logarithmic nonlinear quantum theory". Physics Letters A. 375 (24): 2305–2308. arXiv:1003.0657. Bibcode:2011PhLA..375.2305Z. doi:10.1016/j.physleta.2011.05.012. S2CID 118152360.
  70. ^ Adamson, P.; Andreopoulos, C.; Arms, K.; Armstrong, R.; Auty, D.; Avvakumov, S.; Ayres, D.; Baller, B.; et al. (2007). "Measurement of neutrino velocity with the MINOS detectors and NuMI neutrino beam". Physical Review D. 76 (7): 072005. arXiv:0706.0437. Bibcode:2007PhRvD..76g2005A. doi:10.1103/PhysRevD.76.072005. S2CID 14358300.
  71. ^ Overbye, Dennis (22 September 2011). "Tiny neutrinos may have broken cosmic speed limit". The New York Times. Archived from the original on 2022-01-02. That group found, although with less precision, that the neutrino speeds were consistent with the speed of light.
  72. ^ "MINOS reports new measurement of neutrino velocity". Fermilab today. June 8, 2012. Retrieved June 8, 2012.
  73. ^ Adam, T.; et al. (OPERA Collaboration) (22 September 2011). "Measurement of the neutrino velocity with the OPERA detector in the CNGS beam". arXiv:1109.4897v1 [hep-ex].
  74. ^ Cho, Adrian; Neutrinos Travel Faster Than Light, According to One Experiment, Science NOW, 22 September 2011
  75. ^ Overbye, Dennis (18 November 2011). "Scientists Report Second Sighting of Faster-Than-Light Neutrinos". The New York Times. Archived from the original on 2022-01-02. Retrieved 2011-11-18.
  76. ^ Adam, T.; et al. (OPERA Collaboration) (17 November 2011). "Measurement of the neutrino velocity with the OPERA detector in the CNGS beam". arXiv:1109.4897v2 [hep-ex].
  77. ^ "Study rejects "faster than light" particle finding". Reuters. 2011-11-20. Retrieved 2023-08-24.
  78. ^ Antonello, M.; et al. (ICARUS Collaboration) (15 March 2012). "Measurement of the neutrino velocity with the ICARUS detector at the CNGS beam". Physics Letters B. 713 (1): 17–22. arXiv:1203.3433. Bibcode:2012PhLB..713...17A. doi:10.1016/j.physletb.2012.05.033. S2CID 55397067.
  79. ^ Strassler, M. (2012-04-02). "OPERA: What Went Wrong". Of Particular Significance. Retrieved 2023-08-24.
  80. ^ Randall, Lisa; Warped Passages: Unraveling the Mysteries of the Universe's Hidden Dimensions, p. 286: "People initially thought of tachyons as particles travelling faster than the speed of light...But we now know that a tachyon indicates an instability in a theory that contains it. Regrettably for science fiction fans, tachyons are not real physical particles that appear in nature."
  81. ^ Gates, S.James; Nishino, Hitoshi (October 2000). "Will the real 4D, N=1 SG limit of superstring/M-theory please stand up?". Physics Letters B. 492 (1–2): 178–186. arXiv:hep-th/0008206. Bibcode:2000PhLB..492..178G. doi:10.1016/S0370-2693(00)01073-X.
  82. ^ Chodos, A.; Hauser, A. I.; Alan Kostelecký, V. (1985). "The neutrino as a tachyon". Physics Letters B. 150 (6): 431–435. Bibcode:1985PhLB..150..431C. doi:10.1016/0370-2693(85)90460-5. hdl:2022/20737.
  83. ^ Chodos, Alan; Alan Kostelecký, V.; IUHET 280 (1994). "Nuclear null tests for spacelike neutrinos". Physics Letters B. 336 (3–4): 295–302. arXiv:hep-ph/9409404. Bibcode:1994PhLB..336..295C. doi:10.1016/0370-2693(94)90535-5. S2CID 16496246.{{cite journal}}: CS1 maint: numeric names: authors list (link)
  84. ^ Chodos, A.; Kostelecký, V. A.; Potting, R.; Gates, Evalyn (1992). "Null experiments for neutrino masses". Modern Physics Letters A. 7 (6): 467–476. Bibcode:1992MPLA....7..467C. doi:10.1142/S0217732392000422.
  85. ^ Chang, Tsao (2002). "Parity Violation and Neutrino Mass". Nuclear Science and Techniques. 13: 129–133. arXiv:hep-ph/0208239. Bibcode:2002hep.ph....8239C.
  86. ^ Hughes, R. J.; Stephenson, G. J. (1990). "Against tachyonic neutrinos". Physics Letters B. 244 (1): 95–100. Bibcode:1990PhLB..244...95H. doi:10.1016/0370-2693(90)90275-B.
  87. ^ Gimon, Eric G.; Hořava, Petr (2004). "Over-rotating black holes, Gödel holography and the hypertube". arXiv:hep-th/0405019.
  88. ^ "Themes : Faster Than Light : SFE : Science Fiction Encyclopedia". www.sf-encyclopedia.com. Retrieved 2021-09-01.

Further reading

edit
edit
 
Wikimedia Commons has media related to Faster-than-light travel.
Retrieved from "https://en.wikipedia.org/w/index.php?title=Faster-than-light&oldid=1252645133"