Grice on hypostasis versus hypothesis

--- "The hunting of the quark"
------ Refs: "Constructing quarks"

--- by JLS
------ for the GC

"The sound came to me first: 'quork' (as from a duck) and as such could be pronounced in Joyce -- if meant as a parody on 'quart'], from "The Quark and the Jaguar".

GRICE SPEAKS OF QUARKS.

"Actions and Events", Pacific Philosophical Quarterly, vol. 67, p. 2ff

---

He is referring to "the universe".

"It is a widely (if not universally) held view,
that at least one part of the business of
metaphysics is to determine an ontology; or,
if you prefer, to settle on an answer to the
questoion what, in general or particular terms,
the 'universe' ... contains." (page 1).

----


"Thus far,

a. people
b. tables
c. chairs
d. atoms
e. electrons and
f. quarks

have escaped exclusion". (p. 2)

[to that ontological question.]

-----

Grice proposes a representation of a "Scentific realist", for whom,

"metaphysical hypotheses wll be judicious
to the extent to which, if true, they would
provide backing or justification for
the content and methodology of scientific
theory."

---- but cfr. his qualms against what he elsewhere calls "The devil of Scientism" -- cited by Grandy/Warner in their "Grice" entry for the Stanford Encyclopedia.

Grice continues again in the "Actions and events" piece:

--- Having delivered the motto of the constructivist (he identifies with): 'hypostasise rather than hypothesise', Grice continues with the implicatures of the scientific realist:

"The diagnostic realist wishes to regard the
optimal metaphysical posture as being one
which accepts the general accoutn of Reality
which maximally justifies and supports
the deliverances of science."

----

"But WHAT science?"

----

(He is echoing Davidson, and other philosophers, including Quine (he just quotes these two) who would appeal to science -- Quine to wavicles explicitly in Word and object -- without much detail about those appeals).

Grice goes on:

"WHAT science? Palmistry? Phlogiston Theory?"

--- recall the previous reference to 'atom', 'electron', and 'quark'.

----

"It seems that we need at least a restriction to
REPUTABLE deliverances of REPUTABLE sciences"

----

SECOND problem:

"And how are these [reputable deliverances now of reputable sciences]
to be selected EXCEPT ON THE BASIS of likelihood
of truth, and how is THAT to be optimised in advance
of ANY CLUE about the nature of Reality?"

----- Here it may be that the clash between

b. and c. 'table' and 'chair' -- and d (atom), e (electron) and f (quark) may fit in, if you are in clash mode.

Grice continues:

"It seems that there is an initial need
for SOME GROUNDS of acceptability of
the findings of science which are
INDEPENDENT of those which, it is hoped, will
be provided by a correct and adequate
account of Reality."

----

In "Method in philosophical psychology", he elaborates on this -- the whole essay repr. in "Conception of Value" (his second book, of 1991) -- especially in the final section, where he considers the various claims of "PHYSICALISM". He preferred to see himself as a 'functionalist' rather than a physicalist. In the later "Actionsa and Events" he does distinguish between a functionalist who would see an unconstructed segment of reality ('physical reality') from a thorough constructivist who would deny that there is such unconstructed segment.

----

So, we all know about an atom and an electron. But why the need by Grice to add the quark?

Let's see what we learn from wiki:

"A quark is an elementary particle and a fundamental constituent of matter."

"Quarks combine to form composite particles called hadrons, the most stable of which are protons and neutrons, the components of atomic nuclei[1]."

"Due to a phenomenon known as color confinement, quarks are never found in isolation."

"They can only be found within hadrons.[2][3]."

For this reason, much of what is known about quarks has
been drawn from observations of the hadrons themselves."

"There are six types of quarks, known as flavors."

1. up,
2. down,
3. charm,
4. strange,
5. top, and
6. bottom.[4]"

"Up and down quarks have the lowest masses of all quarks."

"The heavier quarks rapidly change into up and down quarks through a process of particle decay."

"This is the transformation from a higher mass state to a lower mass state."

"Because of this, up and down quarks are generally stable and the most common in the universe, whereas charm, strange, top, and bottom quarks can only be produced in high energy collisions (such as those involving cosmic rays and in particle accelerators)."

"Quarks have various intrinsic properties, including electric charge, color charge, spin, and mass."

"Quarks are the only elementary particles in the Standard Model of particle physics to experience all four fundamental interactions, also known as fundamental forces (electromagnetism, gravitation, strong interaction, and weak interaction), as well as the only known particles whose electric charges are not integer multiples of the elementary charge."

THE ANTI-QUARK:

"For every quark flavor there is a corresponding type of antiparticle, known as antiquark, that differs from the quark only in that some of its properties have equal magnitude but opposite sign."

"The quark model was independently proposed by physicists

a. Murray Gell-Mann and
b. George Zweig

in 1964.[5]"

"Quarks were introduced as parts of an ordering scheme for hadrons, and there was little evidence for their physical existence until 1968.[6][7]"

"All six flavors of quark have since been observed in accelerator experiments."

"The top quark, first observed at Fermilab in 1995, was the
last to be discovered.[5]"

"Six of the particles in the Standard Model are quarks. Each of
the first three columns forms a generation of matter."

"The Standard Model is the theoretical framework describing all the currently known elementary particles,

as well as the unobserved

[nb 1] Higgs boson.[8]"

"This model contains six flavors of quarks (q), named up (u), down (d), charm (c), strange (s), top (t), and bottom (b).[4]"

"Antiparticles of quarks are called antiquarks, and are denoted by a bar over the symbol for the corresponding quark, such as u for an up antiquark."

"As with antimatter in general, antiquarks have the same mass, mean lifetime, and spin as their respective quarks, but the electric charge and other charges have the opposite sign.[9]"

"Quarks are spin-1⁄2 particles, implying that they are fermions according to the spin-statistics theorem."

"They are subject to the Pauli exclusion principle, which states that no two identical fermions can simultaneously occupy the same quantum state."

"This is in contrast to bosons (particles with integer spin), of which any number can be in the same state.[10]"

"Unlike leptons, quarks possess color charge, which causes them to engage in the strong interaction."

"The resulting attraction between different quarks causes the formation of composite particles known as hadrons."

"The quarks which determine the quantum numbers of hadrons are called valence quarks."

"Apart from these, any hadron may contain an indefinite number of virtual (or sea) quarks, antiquarks, and gluons which do not influence its quantum numbers.[11]"

"There are two families of hadrons."

"Baryons, with three valence quarks, and mesons, with a valence quark and an antiquark.[12]"

"The most common baryons are the proton and the neutron, the building blocks of the atomic nucleus.[13]"

"A great number of hadrons are known, most of them differentiated by their quark content and the properties these constituent quarks confer."

********************* important point below vis a vis Grice's point above:

"The existence of "exotic" hadrons with more valence quarks, such as tetraquarks (qqqq) and pentaquarks (qqqqq), has been conjectured[14]"


"but not proven.[nb 2][14][15]"

"Elementary fermions are grouped into three generations, each
comprising two leptons and two quarks."

"The first generation includes up and down quarks, the
second charm and strange quarks, and the third top
and bottom quarks."

"All searches for a fourth generation of quarks and other elementary fermions have failed,[16]"

"and there is strong indirect evidence that no more than three generations exist.[nb 3][17]"

"Particles in higher generations generally have greater mass and lesser stability, causing them to decay into lower-generation particles by means of weak interactions."

"Only first-generation (up and down) quarks occur commonly in nature."

"Heavier quarks can only be created in high-energy collisions (such as in those involving cosmic rays), and decay quickly."

"owever, they are thought to have been present during the first fractions of a second after the Big Bang, when the universe was in an extremely hot and dense phase (the quark epoch)."

"Studies of heavier quarks are conducted in artificially created conditions, such as in particle accelerators.[18]"

"Having electric charge, mass, color charge, and flavor, quarks are the only known elementary particles that engage in all four fundamental interactions of contemporary physics: electromagnetism, gravitation, strong interaction, and weak interaction.[13]"

"Gravitation is too weak to be relevant to individual particle interactions except at extremes of energy (Planck energy) and distance scales (Planck distance)."

"However, since no successful quantum theory of gravity exists, gravitation is not described by the Standard Model."

"Gell-Mann and George Zweig proposed the quark model in 1964."

"The quark model was independently proposed by physicists Murray Gell-Mann[19] and George Zweig[20][21] in 1964.[5]"

"The proposal came shortly after Gell-Mann's 1961 formulation of a particle classification system known as the Eightfold Way—or, in more technical terms, SU(3) flavor symmetry.[22]"

"Physicist Yuval Ne'eman had independently developed a scheme similar to the Eightfold Way in the same year.[23][24]"

"At the time of the quark theory's inception, the "particle zoo" included, amongst other particles, a multitude of hadrons."

----------------------- HYPOSTASIS vs. HYPOTHESIS?

"Gell-Mann and Zweig posited that they were not elementary particles, but were instead composed of combinations of quarks and antiquarks."

"Their model involved three flavors of quarks—up, down, and strange—to which they ascribed properties such as spin and electric charge.[19][20][21]"

"The initial reaction of the physics community to the proposal was mixed."

------------------ abstract entity? Not allowed. Cfr. Grice's paragraph opening
--------------------- discussion about 'ontological scheme'.

"There was particular contention about whether the quark was a physical entity or an abstraction used to explain concepts that were not properly understood at the time.[25]"

----- On 'abstraction': cfr. Grice, on the question on what there is: "In recent times there has been a STRONG tendency to restrict recognition to INDIVIDUAL entities, ecluding of course, all ABSTRACT entities except sets, and excuding above all "intentional" entities like universals and propositions" (p. 2).

The wiki on quarks continues:

"In less than a year, extensions to the Gell-Mann–Zweig model were proposed."

"Sheldon Lee Glashow and James Bjorken

predicted the existence

of a fourth flavor of quark, which they called charm."

----------------- hypothesis, not hypostasis.

"The addition was proposed because it allowed for a better description of the weak interaction (the mechanism that allows quarks to decay), equalized the number of known quarks with the number of known leptons, and implied a mass formula that correctly reproduced the masses of the known mesons.[26]"

---- deconstructing the proton:

"In 1968, deep inelastic scattering experiments at the
Stanford Linear Accelerator Center (SLAC) showed that
the proton contained much smaller, point-like objects and
was therefore not an elementary particle.[6][7][27]"

Dolly Parton -- quarky?

"Physicists were reluctant to identify these objects with quarks at the time, instead calling them "partons"—a term coined by Richard Feynman.[28][29][30]".

"The objects that were observed at the SLAC would later be identified as up and down quarks as the other flavors were discovered.[31]"

"Nevertheless, "parton" remains in use as a collective term for the constituents of hadrons (quarks, antiquarks, and gluons)."

"The strange quark's existence was indirectly
validated by the SLAC's scattering experiments: not only was it a necessary component of Gell-Mann and Zweig's three-quark model, but it provided an explanation for the kaon (K) and pion (π) hadrons discovered in cosmic rays in 1947.[32]"

"In a 1970 paper, Glashow, John Iliopoulos and Luciano Maiani presented further reasoning for the existence of the as-yet undiscovered charm quark.[33][34]"

"The number of supposed quark flavors grew to the current six in 1973, when Makoto Kobayashi and Toshihide Maskawa noted that the experimental observation of CP violation[nb 4][35] could be explained if there were another pair of quarks."

The wiki includes a photograph of "the event that led to the discovery of the Σ++c baryon, at the Brookhaven National Laboratory in 1974."

"Charm quarks were produced almost simultaneously by two teams in November 1974 (see November Revolution)—one at the SLAC under Burton Richter, and one at Brookhaven National Laboratory under Samuel Ting."

"The charm quarks were observed bound with charm antiquarks in mesons."

"The two parties had assigned the discovered meson two different symbols, J and ψ; thus, it became formally known as the J/ψ meson."

"The discovery finally convinced the physics community of the quark model's validity.[30]."

"In the following years a number of suggestions appeared for extending the quark model to six quarks."

"Of these, the 1975 paper by Haim Harari[36] was the first to coin the terms top and bottom for the additional quarks.[37]"

---- He found inspiration in an old English folksong.

"In 1977, the bottom quark was observed by a team at Fermilab led
by Leon Lederman.[38][39]"

"This was a strong indicator of the top quark's existence: without the top quark, the bottom quark would have been without a partner."

TOP SEEN.

"However, it was not until 1995 that the top quark was finally observed, also by the CDF[40] and DØ[41] teams at Fermilab.[5]"

"It had a mass much greater than had been previously expected[42]—almost as great as a gold atom.[43]"

"Gell-Mann originally named the quark after the sound made
by ducks.[44]"

"For some time, he was undecided on an actual spelling for the
term he intended to coin, until he found the word quark in James Joyce's book Finnegans Wake."

"Three quarks for Muster Mark!
Sure he has not got much of a bark
And sure any he has it's all beside the mark."
-----—James Joyce, Finnegans Wake[45]

--

THE QUARK AND THE JAGUAR.

"Gell-Mann went into further detail regarding the name of the quark in his book, The Quark and the Jaguar:[46]"

"In 1963, when I assigned the

name "quark" to the fundamental

constituents of the nucleon, I had the

sound first, without the spelling, which

could have been "kwork". Then, in one

of my occasional perusals of Finnegans

Wake, by James Joyce, I came across the

word "quark" in the phrase "Three quarks

for Muster Mark". Since "quark" (meaning, for

one thing, the cry of the gull) was clearly

intended to rhyme with "Mark", as well

as "bark" and other such words, I had to

find an excuse to pronounce it as "kwork". But

the book represents the dream of a publican named Humphrey

Chimpden Earwicker. Words in the text are typically

drawn from several sources at once, like

the "portmanteau" words in "Through the

Looking-Glass". From time to time, phrases

occur in the book that are partially

determined by calls for drinks at the bar. I argued,

therefore, that perhaps one of the multiple

sources of the cry "Three quarks for Muster Mark" might

be

"Three quarts for Mister Mark", in which case

the pronunciation "kwork" would not be totally unjustified. In

any case, the number three fitted perfectly the way

quarks occur in nature."

----

"Zweig preferred the name "ace" for the particle he had
theorized, but Gell-Mann's terminology came to
prominence once the quark model had been commonly accepted.[47]"

"The quark flavors were given their names for a number of
reasons."

"The up and down quarks are named after the up and down components of isospin, which they carry.[48]"

"Strange quarks were given their name because they were discovered to be components of the strange particles discovered in cosmic rays years before the quark model was proposed."

"These particles were deemed "strange" because they had unusually long lifetimes.[49]"

"Glashow, who coproposed charm quark with Bjorken, is quoted as saying, "We called our construct the 'charmed quark', for we were fascinated and pleased by the symmetry it brought to the subnuclear world."[50]"

"The names "top" and "bottom", coined by Harari, were chosen because they are "logical partners for up and down quarks".[36][37][49]"

"In the past, top and bottom quarks were sometimes referred to as "truth" and "beauty" respectively, but these names have mostly fallen out of use.[51]"

"Quarks have fractional electric charge values—either −1⁄3 or +2⁄3 times the elementary charge, depending on flavor."

"Up, charm, and top quarks (collectively referred to as up-type quarks) have a charge of +2⁄3, while down, strange, and bottom quarks (down-type quarks) have −1⁄3."

"Antiquarks have the opposite charge to their corresponding quarks; up-type antiquarks have charges of −2⁄3 and down-type antiquarks have charges of +1⁄3."

"Since the electric charge of a hadron is the sum of the charges of the constituent quarks, all hadrons have integer charges: the combination of three quarks (baryons), three antiquarks (antibaryons), or a quark and an antiquark (mesons) always results in integer charges.[52]"

"For example, the hadron constituents of atomic nuclei, neutrons and protons, have charges of 0 and +1 respectively; the neutron is composed of two down quarks and one up quark, and the proton of two up quarks and one down quark.[13]"

"Spin is an intrinsic property of elementary particles, and its direction is an important degree of freedom. It is sometimes visualized as the rotation of an object around its own axis (hence the name "spin"), though this notion is somewhat misguided at subatomic scales because elementary particles are believed to be point-like.[53]"

"Spin can be represented by a vector whose length is measured in units of the reduced Planck constant ħ (pronounced "h bar"). For quarks, a measurement of the spin vector component along any axis can only yield the values +ħ/2 or −ħ/2; for this reason quarks are classified as spin-1⁄2 particles.[54] The component of spin along a given axis—by convention the z axis—is often denoted by an up arrow ↑ for the value +1⁄2 and down arrow ↓ for the value −1⁄2, placed after the symbol for flavor. For example, an up quark with a spin of +1⁄2 along the z axis is denoted by u↑.[55]"

"Feynman diagram of beta decay with time flowing upwards. The CKM matrix (discussed below) encodes the probability of this and other quark decays.A quark of one flavor can transform into a quark of another flavor only through the weak interaction, one of the four fundamental interactions in particle physics. By absorbing or emitting a W boson, any up-type quark (up, charm, and top quarks) can change into any down-type quark (down, strange, and bottom quarks) and vice versa. This flavor transformation mechanism causes the radioactive process of beta decay, in which a neutron (n) "splits" into a proton (p), an electron (e⁻) and an electron antineutrino (νe)."

"This occurs when one of the down quarks in the neutron (udd) decays into an up quark by emitting a virtual W⁻ boson, transforming the neutron into a proton (uud). The W⁻ boson then decays into an electron and an electron antineutrino.[56]"

n → p + e⁻ + νe (Beta decay, hadron notation)
udd → uud + e⁻ + νe (Beta decay, quark notation)

"Both beta decay and the inverse process of inverse beta decay are routinely used in medical applications such as positron emission tomography (PET) and in high-energy experiments such as neutrino detection."

"The strengths of the weak interactions between the six quarks. The "intensities" of the lines are determined by the elements of the CKM matrix.While the process of flavor transformation is the same for all quarks, each quark has a preference to transform into the quark of its own generation. The relative tendencies of all flavor transformations are described by a mathematical table, called the Cabibbo–Kobayashi–Maskawa matrix (CKM matrix). The approximate magnitudes of the entries of the CKM matrix are:[57] such, where Vij represents the tendency of a quark of flavor i to change into a quark of flavor j (or vice versa).[nb 5]"

"There exists an equivalent weak interaction matrix for leptons (right side of the W boson on the above beta decay diagram), called the Pontecorvo–Maki–Nakagawa–Sakata matrix (PMNS matrix).[58] Together, the CKM and PMNS matrices describe all flavor transformations, but the links between the two are not yet clear.[59]"

"All types of hadrons have zero total color charge."

"Quarks possess a property called color charge."

"There are three types of color charge, arbitrarily labeled blue, green, and red.[nb 6]"

"Each of them is complemented by an anticolor—antiblue, antigreen, and antired."

"Every quark carries a color, while every antiquark carries an anticolor.[60]"

"The system of attraction and repulsion between quarks charged with different combinations of the three colors is called strong interaction, which is mediated by force carrying particles known as gluons."

"The theory that describes strong interactions is called quantum chromodynamics (QCD)."

"A quark charged with one color value can form a bound system with an antiquark carrying the corresponding anticolor; three (anti)quarks, one of each (anti)color, will similarly be bound together."

"The result of two attracting quarks will be color neutrality: a quark with color charge ξ plus an antiquark with color charge −ξ will result in a color charge of 0 (or "white" color) and the formation of a meson."

"Analogous to the additive color model in basic optics, the combination of three quarks or three antiquarks, each with different color charges, will result in the same "white" color charge and the formation of a baryon or antibaryon.[61]"

"In modern particle physics, gauge symmetries—a kind of symmetry group—relate interactions between particles (see gauge theories)."

"Color SU(3) (commonly abbreviated to SU(3)c) is the gauge symmetry that relates the color charge in quarks and is the defining symmetry for quantum chromodynamics.[62] Just as the laws of physics are independent of which directions in space are designated x, y, and z, and remain unchanged if the coordinate axes are rotated to a new orientation, the physics of quantum chromodynamics is independent of which directions in three-dimensional color space are identified as blue, red, and green."

"SU(3)c color transformations correspond to "rotations" in color space (which, mathematically speaking, is a complex space). Every quark flavor f, each with subtypes fB, fG, fR corresponding to the quark colors,[63] forms a triplet: a three-component quantum field which transforms under the fundamental representation of SU(3)c.[64]"

"The requirement that SU(3)c should be local—that is, that its transformations be allowed to vary with space and time—determines the properties of the strong interaction, in particular the existence of eight gluon types to act as its force carriers.[62][65]"

"Two terms are used in referring to a quark's mass: current quark mass refers to the mass of a quark by itself, while constituent quark mass refers to the current quark mass plus the mass of the gluon particle field surrounding the quark.[66] These masses typically have very different values. Most of a hadron's mass comes from the gluons that bind the constituent quarks together, rather than from the quarks themselves. While gluons are inherently massless, they possess energy—more specifically, quantum chromodynamics binding energy (QCBE)—and it is this that contributes so greatly to the overall mass of the hadron (see mass in special relativity). For example, a proton has a mass of approximately 938 MeV/c2, of which the rest mass of its three valence quarks only contributes about 11 MeV/c2; much of the remainder can be attributed to the gluons' QCBE.[67][68]"

"The Standard Model posits that elementary particles derive their masses from the Higgs mechanism, which is related to the unobserved Higgs boson. Physicists hope that further research into the reasons for the top quark's large mass, which was found to be approximately equal to that of a gold nucleus (~171 GeV/c2),[67][69] might reveal more about the origin of the mass of quarks and other elementary particles.[70]"

"The following table summarizes the key properties of the six quarks. Flavor quantum numbers (isospin (I3), charm (C), strangeness (S, not to be confused with spin), topness (T), and bottomness (B′)) are assigned to certain quark flavors, and denote qualities of quark-based systems and hadrons. The baryon number (B) is +1⁄3 for all quarks, as baryons are made of three quarks. For antiquarks, the electric charge (Q) and all flavor quantum numbers (B, I3, C, S, T, and B′) are of opposite sign. Mass and total angular momentum (J; equal to spin for point particles) do not change sign for the antiquarks."

Quark flavor properties[67] Name Symbol Mass (MeV/c2)* J B Q I3 C S T B′ Antiparticle Antiparticle symbol
First generation
Up u 1.5 to 3.3 1⁄2 +1⁄3 +2⁄3 +1⁄2 0 0 0 0 Antiup u
Down d 3.5 to 6.0 1⁄2 +1⁄3 −1⁄3 −1⁄2 0 0 0 0 Antidown d
Second generation
Charm c 1,270+70−110 1⁄2 +1⁄3 +2⁄3 0 +1 0 0 0 Anticharm c
Strange s 92.4+2.5−2.5[71] 1⁄2 +1⁄3 −1⁄3 0 0 −1 0 0 Antistrange s
Third generation
Top t 171,200±2,100 1⁄2 +1⁄3 +2⁄3 0 0 0 +1 0 Antitop t
Bottom b 4,200+170−70 1⁄2 +1⁄3 −1⁄3 0 0 0 0 −1 Antibottom b
J = total angular momentum, B = baryon number, Q = electric charge, I3 = isospin, C = charm, S = strangeness, T = topness, B′ = bottomness.
* Notation such as 4,200+170−70 denotes measurement uncertainty.
[edit] Interacting quarks
See also: Color confinement and Gluon

"As described by quantum chromodynamics, the strong interaction between quarks is mediated by gluons, massless vector gauge bosons. Each gluon carries one color charge and one anticolor charge. In the standard framework of particle interactions (part of a more general formulation known as perturbation theory), gluons are constantly exchanged between quarks through a virtual emission and absorption process. When a gluon is transferred between quarks, a color change occurs in both; for example, if a red quark emits a red–antigreen gluon, it becomes green, and if a green quark absorbs a red–antigreen gluon, it becomes red. Therefore, while each quark's color constantly changes, their strong interaction is preserved.[72][73][74]"

"Since gluons carry color charge, they themselves are able to emit and absorb other gluons. This causes asymptotic freedom: as quarks come closer to each other, the chromodynamic binding force between them weakens.[75] Conversely, as the distance between quarks increases, the binding force strengthens. The color field becomes stressed, much as an elastic band is stressed when stretched, and more gluons of appropriate color are spontaneously created to strengthen the field. Above a certain energy threshold, pairs of quarks and antiquarks are created. These pairs bind with the quarks being separated, causing new hadrons to form. This phenomenon is known as color confinement: quarks never appear in isolation.[73][76] This process of hadronization occurs before quarks formed in a high energy collision are able to interact in any other way. The only exception is the top quark, which may decay before it hadronizes.[77]"

"Hadrons, along with the valence quarks (qv) that contribute to their quantum numbers, contain virtual quark–antiquark (qq) pairs known as sea quarks (qs). Sea quarks form when a gluon of the hadron's color field splits; this process also works in reverse in that the annihilation of two sea quarks produces a gluon."

"The result is a constant flux of gluon splits and creation colloquially known as "the sea".[78]"

"Sea quarks are much less stable than their valence counterparts, and they typically annihilate each other within the interior of the hadron. Despite this, sea quarks can hadronize into baryonic or mesonic particles under certain circumstances.[79]"

"A qualitative rendering of the phase diagram of quark matter. The precise details of the diagram are the subject of ongoing research.[80][81]Under sufficiently extreme conditions, quarks may become deconfined and exist as free particles. In the course of asymptotic freedom, the strong interaction becomes weaker at higher temperatures. Eventually, color confinement would be lost and an extremely hot plasma of freely moving quarks and gluons would be formed. This theoretical phase of matter is called quark–gluon plasma.[82] The exact conditions needed to give rise to this state are unknown and have been the subject of a great deal of speculation and experimentation. A recent estimate puts the needed temperature at 1.90±0.02×1012 kelvins.[83] While a state of entirely free quarks and gluons has never been achieved (despite numerous attempts by CERN in the 1980s and 1990s),[84] recent experiments at the Relativistic Heavy Ion Collider have yielded evidence for liquid-like quark matter exhibiting "nearly perfect" fluid motion.[85]"

"The quark–gluon plasma would be characterized by a great increase in the number of heavier quark pairs in relation to the number of up and down quark pairs. It is believed that in the period prior to 10−6 seconds after the Big Bang (the quark epoch), the universe was filled with quark–gluon plasma, as the temperature was too high for hadrons to be stable.[86]"

"Given sufficiently high baryon densities and relatively low temperatures—possibly comparable to those found in neutron stars—quark matter is expected to degenerate into a Fermi liquid of weakly interacting quarks. This liquid would be characterized by a condensation of colored quark Cooper pairs, thereby breaking the local SU(3)c symmetry. Because quark Cooper pairs harbor color charge, such a phase of quark matter would be color superconductive; that is, color charge would be able to pass through it with no resistance.[87]"

"See also, Physics portal, Book:Particles of the Standard Model, Book:Hadronic Matter

Books are collections of articles that can be downloaded or ordered in print.
Color–flavor locking Quarkonium – Mesons made of a quark and antiquark of the same flavor Preons – Hypothetical particles which were once postulated to be subcomponents of quarks and leptons Quark–lepton complementarity – Possible fundamental relation between quarks and leptons
Quark star – A hypothetical degenerate neutron star with extreme density

Notes
^ As of July 2009[update].

^

"Several research groups claimed to have proven the existence of tetraquarks and
pentaquarks in the early 2000s."

----- PROVING A NEGATIVE:

"While the status of tetraquarks is still under debate, all known pentaquark candidates have since been established as non-existent."


^ The main evidence is based on the resonance width of the Z⁰ boson, which constrains the 4th generation neutrino to have a mass greater than ~45 GeV/c2. This would be highly contrasting with the other three generations' neutrinos, whose masses cannot exceed 2 MeV/c2.

^ "CP violation is a phenomenon which causes weak interactions to behave differently when left and right are swapped (P symmetry) and particles are replaced with their corresponding antiparticles (C symmetry)."

---- NOT to be confused with violations to Grice's cooperative principle.

^ "The actual probability of decay of one quark to another is a complicated function of (amongst other variables) the decaying quark's mass, the masses of the decay products, and the corresponding element of the CKM matrix. This probability is directly proportional (but not equal) to the magnitude squared of the corresponding CKM entry."

^ "Despite its name, color charge is not related to the color spectrum of visible light."

References
^ "Quark (subatomic particle)". Encyclopedia Britannica. http://www.britannica.com/EBchecked/topic/486323/quark. Retrieved 2008-06-29.

^ R. Nave. "Confinement of Quarks". HyperPhysics. Georgia State University, Department of Physics and Astronomy. http://hyperphysics.phy-astr.gsu.edu/hbase/Particles/quark.html#c6. Retrieved 2008-06-29.

^ R. Nave.
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[edit] Further reading
D.J. Griffiths (2008). Introduction to Elementary Particles (2nd ed.). Wiley–VCH. ISBN 3527406018.
I.S. Hughes (1985). Elementary particles (2nd ed.). Cambridge University Press. ISBN 0-521-26092-2.
R. Oerter (2005). The Theory of Almost Everything: The Standard Model, the Unsung Triumph of Modern Physics. Pi Press. ISBN 0132366789.
A. Pickering (1984). Constructing Quarks: A Sociological History of Particle Physics. The University of Chicago Press. ISBN 0-226-66799-5.
B. Povh (1995). Particles and Nuclei: An Introduction to the Physical Concepts. Springer–Verlag. ISBN 0-387-59439-6.
M. Riordan (1987). The Hunting of the Quark: A true story of modern physics. Simon & Schuster. ISBN 0-671-64884-5.
B.A. Schumm (2004). Deep Down Things: The Breathtaking Beauty of Particle Physics. Johns Hopkins University Press. ISBN 0-8018-7971-X.
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