Exotic matter
In physics, exotic matter is matter that somehow deviates from normal matter and has "exotic" properties. A broader definition of exotic matter is any kind of non-baryonic matter—that is not made of baryons, the subatomic particles (such as protons and neutrons) of which ordinary matter is composed.[1] Exotic mass has been considered a colloquial term for matters such as dark matter, negative mass, or complex mass.[2][3][4][5][6][7]
Contents
1 Types
2 Negative mass
3 Complex mass
4 Materials at high pressure
5 See also
6 References
7 External links
Types
There are several types of exotic matter:
- Hypothetical particles and states of matter that have "exotic" physical properties that would violate known laws of physics, such as a particle having a negative mass.
Hypothetical particles and states of matter that have not yet been encountered, but whose properties would be within the realm of mainstream physics if found to exist.- Several particles whose existence has been experimentally confirmed that are conjectured to be exotic hadrons and within the Standard Model.
States of matter that are not commonly encountered, such as Bose–Einstein condensates, fermionic condensates, quantum spin liquid, string-net liquid, supercritical fluid, color-glass condensate, quark–gluon plasma, Rydberg matter, Rydberg polaron and photonic matter but whose properties are entirely within the realm of mainstream physics.- States of matter that are poorly understood, such as dark matter and mirror matter.
- Ordinary matter placed under high pressure, which may result in dramatic changes in its physical or chemical properties.
- Degenerate matter
- Exotic atoms
Negative mass
Negative mass would possess some strange properties, such as accelerating in the direction opposite of applied force. Despite being inconsistent with the expected behavior of "normal" matter, negative mass is mathematically consistent and introduces no violation of conservation of momentum or energy. It is used in certain speculative theories, such as on the construction of artificial wormholes and the Alcubierre drive. The closest known real representative of such exotic matter is the region of pseudo-negative-pressure density produced by the Casimir effect.
According to mass–energy equivalence, mass m{displaystyle m} is in proportion to energy E{displaystyle E}
and the coefficient of proportionality is c2{displaystyle c^{2}}
. Actually, m{displaystyle m}
is still equivalent to E{displaystyle E}
although the coefficient is another constant[8] such as −c2{displaystyle -c^{2}}
.[9] In this case, it is unnecessary to introduce a negative energy because the mass can be negative although the energy is positive. That is to say,
- E=−mc2>0{displaystyle E=-mc^{2}>0}
- m=−Ec2<0{displaystyle m=-{frac {E}{c^{2}}}<0}
Under the circumstances,
- dE=Fds=dpdtds=dsdtdp=vdp=vd(mv){displaystyle dE=Fds={frac {dp}{dt}}ds={frac {ds}{dt}}dp=vdp=vd(mv)}
- −c2dm=vd(mv){displaystyle -c^{2}dm=vd(mv)}
- −c2(2m)dm=2mvd(mv){displaystyle -c^{2}(2m)dm=2mvd(mv)}
- −c2d(m2)=d(m2v2){displaystyle -c^{2}d(m^{2})=d(m^{2}v^{2})}
- −m2c2=m2v2+C{displaystyle -m^{2}c^{2}=m^{2}v^{2}+C}
When v=0{displaystyle v=0},
- C=−m02c2{displaystyle C=-m_{0}^{2}c^{2}}
Consequently,
- −m2c2=m2v2−m02c2{displaystyle -m^{2}c^{2}=m^{2}v^{2}-m_{0}^{2}c^{2}}
- m=m01+v2c2{displaystyle m={m_{0} over {sqrt {1+displaystyle {v^{2} over c^{2}}}}}}
where m0<0{displaystyle m_{0}<0} is invariant mass and invariant energy equals E0=−m0c2>0{displaystyle E_{0}=-m_{0}c^{2}>0}
. The squared mass is still positive and the particle can be stable.
Since m=m01+v2c2<0{displaystyle m={m_{0} over {sqrt {1+displaystyle {v^{2} over c^{2}}}}}<0},
- p=mv=m0v1+v2c2<0{displaystyle p=mv={m_{0}v over {sqrt {1+displaystyle {v^{2} over c^{2}}}}}<0}
The negative momentum is applied to explain negative refraction, inverse Doppler effect and reverse Cherenkov effect observed in a negative index metamaterial. The radiation pressure in the metamaterial is also negative[10] because the force is defined as F=dpdt{displaystyle F={frac {dp}{dt}}}. Negative pressure exists in dark energy too. Using these above equations, the energy-momentum relation should be
- E2=−p2c2+m02c4{displaystyle E^{2}=-p^{2}c^{2}+m_{0}^{2}c^{4}}
Substituting the Planck-Einstein relation E=ℏω{displaystyle E=hbar omega } and de Broglie's p=ℏk{displaystyle p=hbar k}
, we obtain the following dispersion relation
ω2=−k2c2+ωp2{displaystyle omega ^{2}=-k^{2}c^{2}+omega _{p}^{2}}, (E0=ℏωp=−m0c2>0){displaystyle (E_{0}=hbar omega _{p}=-m_{0}c^{2}>0)}
of the wave consists of a stream of particles whose energy-momentum relation is E2=−p2c2+m02c4{displaystyle E^{2}=-p^{2}c^{2}+m_{0}^{2}c^{4}}(wave–particle duality) can be excited in a negative index metamaterial.The velocity of such a particle is equal to
- v=cE02E2−1=cωp2ω2−1{displaystyle v=c{sqrt {{frac {E_{0}^{2}}{E^{2}}}-1}}=c{sqrt {{frac {omega _{p}^{2}}{omega ^{2}}}-1}}}
and range is from zero to infinity
ωp2ω2<2{displaystyle {frac {omega _{p}^{2}}{omega ^{2}}}<2}, v<c{displaystyle v<c}
ωp2ω2>2{displaystyle {frac {omega _{p}^{2}}{omega ^{2}}}>2}, v>c{displaystyle v>c}
Moreover, the kinetic energy is also negative
Ek=E−E0=−mc2−(−m0c2)=−m0c21+v2c2+m0c2=m0c2(1−11+v2c2)<0{displaystyle E_{k}=E-E_{0}=-mc^{2}-(-m_{0}c^{2})=-{m_{0}c^{2} over {sqrt {1+displaystyle {v^{2} over c^{2}}}}}+m_{0}c^{2}=m_{0}c^{2}(1-{1 over {sqrt {1+displaystyle {v^{2} over c^{2}}}}})<0}, (m0<0){displaystyle (m_{0}<0)}
In fact, the negative kinetic energy exists in some models[11] to describe dark energy (phantom energy) whose pressure is negative. In this way, the negative mass of exotic matter is now associated with negative momentum, negative pressure, negative kinetic energy and FTL (faster-than-light).
Complex mass
A hypothetical particle with complex rest mass would always travel faster than the speed of light. Such particles are called tachyons. There is no confirmed existence of tachyons.
- E=m⋅c21−|v|2c2{displaystyle E={frac {mcdot c^{2}}{sqrt {1-{frac {left|mathbf {v} right|^{2}}{c^{2}}}}}}}
If the rest mass m{displaystyle m} is complex this implies that the denominator is complex because the total energy is observable and thus must be real. Therefore, the quantity under the square root must be negative, which can only happen if v is greater than c. As noted by Gregory Benford et al., special relativity implies that tachyons, if they existed, could be used to communicate backwards in time[12] (see tachyonic antitelephone). Because time travel is considered to be non-physical, tachyons are believed by physicists either not to exist, or else to be incapable of interacting with normal matter.
In quantum field theory, complex mass would induce tachyon condensation.
Materials at high pressure
At high pressure, materials such as sodium chloride (NaCl) in the presence of an excess of either chlorine or sodium were transformed into compounds "forbidden" by classical chemistry, such as Na
3Cl and NaCl
3. Quantum mechanical calculations predict the possibility of other compounds, such as NaCl
7, Na
3Cl
2 and Na
2Cl. The materials are thermodynamically stable at high pressures. Such compounds may exist in natural environments that exist at high pressure, such as the deep ocean or inside planetary cores. The materials have potentially useful properties. For instance, Na
3Cl is a two-dimensional metal, made of layers of pure sodium and salt that can conduct electricity. The salt layers act as insulators while the sodium layers act as conductors.[13][14]
See also
Antimatter – Material composed of the antiparticles of the corresponding particles of ordinary matter
Dark energy – unknown property in cosmology that causes the expansion of the universe to accelerate.
Dark matter – Hypothetical form of matter comprising most of the matter in the universe
Gravitational interaction of antimatter – Theory of gravity on antimatter
Mirror matter – A hypothetical counterpart to ordinary matter- Negative energy
Negative mass – Concept in physical models- Strange matter
QCD matter – Theorized phases of matter whose degrees of freedom include quarks and gluons
References
^ "Exotic matter". daviddarling.info. Retrieved 2015-06-24..mw-parser-output cite.citation{font-style:inherit}.mw-parser-output .citation q{quotes:"""""""'""'"}.mw-parser-output .citation .cs1-lock-free a{background:url("//upload.wikimedia.org/wikipedia/commons/thumb/6/65/Lock-green.svg/9px-Lock-green.svg.png")no-repeat;background-position:right .1em center}.mw-parser-output .citation .cs1-lock-limited a,.mw-parser-output .citation .cs1-lock-registration a{background:url("//upload.wikimedia.org/wikipedia/commons/thumb/d/d6/Lock-gray-alt-2.svg/9px-Lock-gray-alt-2.svg.png")no-repeat;background-position:right .1em center}.mw-parser-output .citation .cs1-lock-subscription a{background:url("//upload.wikimedia.org/wikipedia/commons/thumb/a/aa/Lock-red-alt-2.svg/9px-Lock-red-alt-2.svg.png")no-repeat;background-position:right .1em center}.mw-parser-output .cs1-subscription,.mw-parser-output .cs1-registration{color:#555}.mw-parser-output .cs1-subscription span,.mw-parser-output .cs1-registration span{border-bottom:1px dotted;cursor:help}.mw-parser-output .cs1-ws-icon a{background:url("//upload.wikimedia.org/wikipedia/commons/thumb/4/4c/Wikisource-logo.svg/12px-Wikisource-logo.svg.png")no-repeat;background-position:right .1em center}.mw-parser-output code.cs1-code{color:inherit;background:inherit;border:inherit;padding:inherit}.mw-parser-output .cs1-hidden-error{display:none;font-size:100%}.mw-parser-output .cs1-visible-error{font-size:100%}.mw-parser-output .cs1-maint{display:none;color:#33aa33;margin-left:0.3em}.mw-parser-output .cs1-subscription,.mw-parser-output .cs1-registration,.mw-parser-output .cs1-format{font-size:95%}.mw-parser-output .cs1-kern-left,.mw-parser-output .cs1-kern-wl-left{padding-left:0.2em}.mw-parser-output .cs1-kern-right,.mw-parser-output .cs1-kern-wl-right{padding-right:0.2em}
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^ Wang, Z.Y; Wang P.Y; Xu Y.R (2011). "Crucial experiment to resolve Abraham-Minkowski Controversy". Optik. 122 (22): 1994–1996. arXiv:1103.3559. Bibcode:2011Optik.122.1994W. doi:10.1016/j.ijleo.2010.12.018.
^ Wang, Z.Y. (2016). "Modern Theory for Electromagnetic Metamaterials". Plasmonics. 11 (2): 503–508. doi:10.1007/s11468-015-0071-7.
^ Veselago, V. G. (1968). "The electrodynamics of substances with simultaneously negative values of permittivity and permeability". Soviet Physics Uspekhi. 10 (4): 509–514. Bibcode:1968SvPhU..10..509V. doi:10.1070/PU1968v010n04ABEH003699.
^ Caldwell, R.R. (2002). "A phantom menace? Cosmological consequences of a dark energy component with super-negative equation of state". Physics Letters B. 545 (1–2): 23–29. arXiv:astro-ph/9908168. Bibcode:2002PhLB..545...23C. doi:10.1016/S0370-2693(02)02589-3.
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^ Zhang, W.; Oganov, A. R.; Goncharov, A. F.; Zhu, Q.; Boulfelfel, S. E.; Lyakhov, A. O.; Stavrou, E.; Somayazulu, M.; Prakapenka, V. B.; Konôpková, Z. (2013). "Unexpected Stable Stoichiometries of Sodium Chlorides". Science. 342 (6165): 1502–1505. arXiv:1310.7674. Bibcode:2013Sci...342.1502Z. doi:10.1126/science.1244989. PMID 24357316.
External links
Exotic Matter and Negative Energy on YouTube
The Riddle of AntiMatter on YouTube