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Spin, Mass and SizeCharacteristics of Hyperons Which Contain a Strange Quark |
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This material stems from a model of quarks being spherical shells of charge and hadrons being concentric spheres of quarks. A previous study established estimates of densities, volumes and masses for Up and Down quarks in their three different varieties of small, medium and large. These estimates are based upon the characteristics of nucleons and pi mesons. It is presumed that these characteristics are intrinsic properties of the quarks and carry over to quarks in other particles.

This material is to investigate the characteristics of quarks in relation to those of hadrons which include a
Strange quark along with an Up or Down quark. These are called *hyperons*. There are also mesons
containing Strange quarks. These are called *kaons* or k-mesons.
They include a Strange quark
and an anti-version of an Up quark or a Down quark.

A positive sigma particle is composed of two *up* quarks and one *strange* quark. Another sigma
particle is composed
of two *down* quarks and one *Strange* quark. The neutralS sigma particle is composed of one up quark, one down quark
and a strange quark. The Up quark has an electrostatic charge of
+2/3 and a Strange quark an electrostatic charge of −1/3. Therefore a positive sigma particle has an electrostatic charge
of +1. A neutral sigma particle has a charge of zero. A sigma particle with two Down quarks and a Strange quark has a charge of −1.
But a particle consisting of a Down quark and two Strange quarks would also have a charge of −1.

As mentioned above there are also mesons which contain a strange quark. The negative kaon consists of a strange quark and an anti-Up quark. An anti-Up quark has the same characteristics as an Up quark exept its charge is the opposite. Thus a negative kaon has a charge of −1.

A meson consisting of a strange quark and an anti-Down quark would have a charge of −2/3. A meson consisting of an Up quark and an anti-Strange quark would have a charge of +1. It would be properly called a positive kaon.

Charge in the Nucleons

The radial distributions of electrostatic charge are found by sending electrons as probes against collections of positi and analyzing the deviations from a straight path. Here are the results of such experiments.

The conventional model of the quarkic structure of nucleons is of quarks as point particles in a plane rotating about their center of mass. The model being considered here is an alternative to that conventional model. In this model a quark is spherical shell of charge(s). A nucleon is three concentric shells.

According to this concentric shell model there should be such radial distributions and they should appear the same in any radial direction. According to the conventional model there should be no such radial distribution. The peceived charge would depend upon the angle between the radial direction and the plane of point quarks.

The experimental radial charge distribution for a neutron, shown above, could not occur unless there is a radial separation of the Up quark and the Down quarks.

The radial distribution of charge for neutrons is entirely in keeping with the concentric shells model. However according to this alternative model there should also be radial range of negative charge for the proton. It may well be that the experimentalists who developed the above distribution for protons overlooked such negative charge density because they were not expecting it.

In the *concentric shells*
model of the quarkic structure of hadons a quark is a spherical shell of electrostatic charges.

A hyperon in this model consists of three concentric rotating quarkic shells. There is thus three versions of each quark: The small, medium and large versions. It is impossible to separate them because any action taken againt the outer quark equally affects the other quarks in a nucleon.

Conventionally each quark has another attribute that is callled *color* although it
has nothing to do with visual color. A nucleon has quarks of each color so it is said to be *color neutral white*.

The attribute corresponding to *color* is the outer radius
of the quark shell. It is obvious in this model why
there must be quarks of three different attributes in each nucleon.

The force of attraction is zero between shells of opposite charge if one is located within another but becomes large positive if they are not concentric. However, if separated the force of attraction decreases with separation distance.

In the conventional model of hadreon structure there is no mechanism that would account for the radial distributions of charge and their boundedness if quarks were point particles. On the other hand if quarks are bounded symmmetrical distributions of charge their effects outside their boundaries is the same as if their charges were concentrated at their centers.

An actual charged point particle would have infinite energy. There is not enough energy in the entire Universe to create even one charged point quark. That is to say, in attempting to create one point particle quark the the effort would fail even after all of the energy of the billions of stars in every one the billions of galaxies is used up. And there would be nothing left over for creating a second quark or any of the zillions upon zillions of other quarks in the Universe.

The mass of a positive or negative kaon is 966.1 electron masses. It is uncertain as to whether the Strange quark is the center quark or whether the anti-Up quark is. From the previous study the mass of a small Up quark is 50.2382 electron masses. This means the mass of a medium sized Strange quark would be 915.8616 electron masses. With the mass density of a Strange quark being the same as that of a Down quark the volume occupied by the medium Strange quark would be 2.9264 cubic fermi (f³). This added to the volume occupied by a small Up quark gives the volume occupied by the two inner quarks in a sigma hyperon; i.e., 2.9264+0.0654=2.9918 f³. Dividing this figure by (4/3)π gives the cube of radius of the medium Strange quark; i.e., 0.7142 fermi. This would mean the radius of a Strange quark would be 0.8939 fermi.

If the Strange quark is at the center of the hyperon its mass would be 966.1 electron masses less the mass the mass of a medium
anti-Up quark; i.e., 966.1 − 224.7953 = 741.55027 electron masses. Dividing this mass by the density of a Down quark gives
the volume of a Strange quark; i.e., 2.3693 f³. Dividing this volume by (4/3)π gives the cube of the radius of the Strange quark; i.e.,
0.5656 f³. This means the radius of a Strange quark would be 0.8270 fermi. This seems to be the more plausible alternative
especially since the arrangement S__U____U__ obey the rule of no particle being linked to more thatn one of its own kind and no
more than one of its opposite kind,

The mass of a positive sigma hyperon is 2327.53 electron masses. Subtractin the mass of a charged kaon from this gives the mass of a large anti-Up quark; i.e., a large Up quark as 1361.4342 electron masses, whereas the value from the previous study is 1565.5525 electron masses. These are the same order of magnitude and close enough to provise some confirmation of the concentric spheres model of haron structure..

A magnetic moment is generated by spinning charged particles or charged particles in shells if flowing in a circular path. For some of the details of the technicalities of magnetic moments see Studies.

A magnetic moment of a system composed of charged particles rotating about a center can arise in part from that rotation of
charges. This is usually called a *dipole moment*. But it is thought that the magnet moment of a rotating particle structure can also
come from the intrinsic magnetic moments of
the particles. This latter phenomenon is usually deemed as being due to the *spin* of the particles. In 1922 the physicists
Otto Stern and Walther Gerlach
ejected a beam of silver atoms into a sharply varying magnetic field. The beam separated into two parts. This separation
could be explained by the outer unpaired electrons of these atoms having a spin that is oriented in either of two directions. It has been long
asserted that this so-called *spin* is not necessarily literally physial particle spin.
However there is no evidence that it is not.
Here it is accepted that the
magnet moment of any particle is due to its actual spinning.

The magnetic moments of the sigma hyperons derive from the intrinsic moments of their quarks and any dipole moment of the quarks within them. The magnetic moment of a positive sigma particle, measured in nuclear magneton units, is +2.458. The nuclear magneton is defined

and

e(½

where e is the unit of electrical charge,
~~h~~ is the reduced Planck's constant,
m_{P} is the rest mass of a proton and c is the speed of light. It has the dimensions of energy per unit time.

No measured magnetic moment for the neutral sigma particle is available at present but it is likely to be nonzero just as is that of the neutron.

The magnetic moment of a negative sigma particle is −1.160. The ratio of these two magnetic moments is −0.47193, intriguingly close to −1/2. This suggests that the ratio of the intrinsic magnetic moments of the negative and positive sigma particles is precisely −1/2.

If the ratio of the intrinsic magnetic moments of the negative and positive sigma particles is −1/2 then any dipole moment of the rotating quarks would result in a deviation of the overall magnetic moments from that value. The question is what spatial structure of nucleons would tend to have a negligible dipole moment. In the concentric shells model the concentricity of three spheres forces a closeness of their centers. Also if the spheresare subject to a force that drops off faster than distance squared then concentric spheres will line up their centers exactly. See Quarks for the details.

of the Quarks

As noted previously a positive sigma particle is composed of two Up quarks and one Strange quark. For a negative sigma particle
its composition is two Strange quarks and one Up quark. Let μ_{U} and μ_{S} be the magnetic moments of
the Up and Strange quarks, respectively.
Then

and

μ

Dividing the second equation by 2 gives

Subtracting this equation from the first gives

and hence

μ

The magnetic moment of the Strange quark is then

Note the ratio |μ_{S}|/μ_{U} = −0.7864 ≅ (3/4)
This is the ratio of magnetic moments but not necessarily the ratio of quark sizes.

The magnetic moment of a particle is of the form

where Q is charge and k is a constant determined by the spatial distribution of the charge. For a spherical suface k=2/3. For a spherical ball of charge k=2/5. For a spherical charge distributed over a spherical shell of some thickness 2/5<k<2/3. R is the average charge radius and ω is the rate of rotation.

As noted previously the charge of the Up quark is +2/3 and that of the Strange quark is −1/3. Let the average charge radii of
the Up and Strange quarks be denoted by R_{U} and R_{S}, repectively .
Likewise let ω_{U} and ω_{S} be their spin rates and k_{U}
and k_{D} are the coefficients for the nature of their charge distributions.

Then

and

(−1/3)k

Equivalently these are

and

k

Note that the ratio of the RHS of these equations is

If k_{U}=k_{S} and ω_{U}=ω_{S} then

and hence

R

Notably the analysis indicates that the Strange quark is essentially same size as the Up quark.

What this means is that an Up quark and a Strange quark are roughly the same size and in particular an Up quark is not a point particle, as in the conventional model. As noted before, there is a good reason a spherical shell quark would be mistakenly thought to be a point particle. Outside of the spherical shell its physical effects are the same as if its charge were concentrated at its center. In other words at points outside of its shell the effects of a spherically distributed quark cannot be distinguished from that of a point particle. Thus any evidence for a point quark is not evidence for an impossible infinite energy charged point particle, but instead evidence for spherically distributed charged particle.