Tamar Thesis TheoryChapt

The Standard Model

Matter is composed of two types of elementary particles, quarks and leptons, which form composite particles by exchanging bosons, yet another elementary particle. The Standard Model of particle physics, a Quantum Field Theory, was developed between 1970 and 1973. The Standard Model describes all of the known elementary particle interactions except gravity. It is the collection of the following related theories: quantum electrodynamics, the Glashow-Weinberg-Salam theory of electroweak processes and quantum chromodynamics. The Standard Model describes a nucleon, a neutron or proton, as a particle composed of 3 constituent quarks having a flavor of either up or down. Quarks are spin 1/2 particles with fractional charge([math]e_{q}[/math]) and come in the flavors of strangeness(S), charm(C), beauty(B) and truth(T) in addition to up (u) and down(d). Quarks have Baryon quantum number ([math]B^{\prime}[/math]) of 1/3. The quantum numbers of quarks with their antiparticles are given in Table 1.

THE QUARK CLASSIFICATION

Quark	Spin	[math]e_{q}[/math](electric charge)	[math]I_{3}[/math](Isospin)	[math]B^{\prime}[/math](Baryon Number)	C(Charmness)	S(Strangeness)	T(Topness)	B(Bottomness)	Antiquark
[math]u[/math](up)	1/2	+2/3	+1/2	+1/3	0	0	0	0	[math]\bar{u}[/math]
[math]d[/math](down)	1/2	-1/3	-1/2	+1/3	0	0	0	0	[math]\bar{d}[/math]
[math]c[/math](charm)	1/2	+2/3	0	+1/3	+1	0	0	0	[math]\bar{c}[/math]
[math]s[/math](strange)	1/2	-1/3	0	+1/3	0	-1	0	0	[math]\bar{s}[/math]
[math]t[/math](top)	1/2	+2/3	0	+1/3	0	0	+1	0	[math]\bar{t}[/math]
[math]b[/math](bottom)	1/2	-1/3	0	+1/3	0	0	0	-1	[math]\bar{b}[/math]

Table 1. Quarks in the Quark Model with their quantum numbers and electric charge in units of electron

The Quark Parton Model

In 1964 Gell-Mann and Zweig suggested that a proton was composed of point like particles in an effort to explain the resonance spectra observed by experiments in the 1950s. These point like particles, referred to as partons and later quarks, are the building blocks of baryons and mesons and have not been observed as free particles. The model assumes that the partons are identified according to a quantum number called flavor which contains three values: up([math]u[/math]), down([math]d[/math]) and strange([math]s[/math]) and their antiparticles. This set of flavor quantum numbers can be used within the context of group theory's SU(3) representation to construct isospin wave functions for the nucleon. The quarks carry electric charges [math]\pm \frac{2}{3}[/math] and [math]\pm \frac{1}{3}[/math] of the electron charge, which has never been observed before.

Baryons are obtained by as a combination of three quarks([math]qqq[/math]) and mesons by combining a quark and an antiquark ([math]q\bar{q}[/math]). From the rules for combining representation of SU(3) one can show the patterns of baryons and mesons <ref name="Close">Close, F.E. (1979). An Introduction to Quarks and Patrons. London, UK: Academic Press Inc. LTD.</ref>:

[math]q\bar{q} = \bold{3} \otimes \bold{3} = 1 \oplus 8[/math]

[math]qqq = 3 \otimes 3 \otimes 3 = 1 \oplus 8 \oplus 8 \oplus 10[/math]

The constituent quark model describes a nucleon as a combination of three quarks. According to the quark model, two of the three quarks in a proton are labeled as having a flavor ``up" and the remaining quark a flavor ``down". The two up quarks have fractional charge [math]+\frac{2}{3}e[/math] while the down quark has a charge [math]-\frac{1}{3}e[/math]. All quarks are spin [math]\frac{1}{2}[/math] particles. In the quark model each quark carries one third of the nucleon mass.

Since late 1960, inelastic scattering experiments were used to probe a nucleon's excited states. Performed experiments suggested that the charge of the nucleon is distributed on a pointlike constituents of the nucleon. The experiments at the SLAC used high energy electrons scattered by nucleons, where virtual photon is the mediator between the target nucleon and coulomb scattering of an electron. The four-momentum, Q, of the virtual photon serves as a measure of the resolution of the scattering and may be formulated as:

[math]d = \frac{\hbar c}{Q} = \frac{0.2 \;\mbox {GeV} \cdot \mbox{ fm}}{Q}[/math] .

The electron scattering data taken during the SLAC experiments revealed a scaling behavior, which was later defined as Bjorken scaling. The inelastic cross section was anticipated to fall sharply with $Q^2$ like the elastic cross section. However, the observed limited dependence on [math]Q^2[/math] suggested that the nucleons constituents are pointlike dimensionless scattering centers. Independently, Richard Feynman introduced the quark parton model where the nucleons are constructed by three point like constituents, called partons.

Shortly afterwards, it was discovered that partons and quarks are the same particles. In the QPM the mass of the quark is much smaller than in the naive quark model. In the parton model the inelastic electron nucleon interaction via the virtual photon is understood as an incoherent elastic scattering processes between the electron and the constituents of the target nucleon. ``In other words, one assumes that a single interaction does not happen with the nucleon as a whole, but with exactly one of its constituents."<ref name="QCDHighEnergyExperimentsandTheory">Dissertori, G., Knowles, I.K., & Schmelling, M. (2003). Quantum Chromodynamics: High Energy Experiments and Theory. Oxford, UK: Oxford University Press.</ref> In addition, two categories of quarks were introduced, ``sea" and ``valence" quarks. The macroscopic properties of the particle are determined by its valence quarks. On the other hand, the so called sea quarks, virtual quarks and antiquarks, are constantly emitted and absorbed by the vacuum.

The inelastic scattering between the electron and the nucleon can be described by the two structure function, which only depend on [math]x_{B}[/math] Bjorken scaling variable - the fraction of nucleon four-momentum carried by the partons.

It was experimentally shown, that the measured croos section of inelastic lepton-nucleon scattering depends only on $x_{B}$, as it was mention above it is reffered as scaling. If there where additional objects inside the nucleon beside the main building partons, it would introduce new energy scale. The experimental observation of scaling phenomenon was the first evidence of the statement that the quarks are the constituents of the hadron. The results which were obtained from MIT-SLAC Collaboration(1970)are presented below on Figure 1 and 2 <ref name="QCDHighEnergyExperimentsandTheory">Dissertori, G., Knowles, I.K., & Schmelling, M. (2003). Quantum Chromodynamics: High Energy Experiments and Theory. Oxford, UK: Oxford University Press.</ref> <ref name="RobertsSpinStructure">Roberts, R. G. (1990). The structure of the proton. Cambridge Monographs on Mathematical Physics. Cambridge, UK: Cambridge University Press.</ref> . It clearly shows the structure function dependence on [math]x_{B}[/math] variable and independence of the four-momentum transfer squared.

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Figure 1. Scaling behavior of [math]\nu W_2(1/x_{B})=F_2(1/x_{B})[/math] for various [math]Q^{2}[/math] ranges.

Figure 2.Value of [math]\nu W_2(Q^{2})=F_2(Q^{2})[/math] for [math]x_B=0.25[/math] .

The quark parton model predictions are in agreement with the experimental results. One of those predictions is the magnet moments of baryons. For example, the magnet moment of the proton should be the sum of the magnetic moments of the constituent quarks according to the naive quark model <ref name="Anisovich">Anisovich, V.V., Kobrinsky, M.N., Nyiri, J., & Shabelski, Yu. M. (2004). Quark Model and High Energy Collisions. World Scientific Publishing Co. Pte. Ltd.</ref> :

[math]\frac{e}{2m_p} \mu_p= \Sigma_{i=1,2,3} \lt P_{\frac{1}{2}}|\frac{e_q(i)\sigma_z(i)}{2m_p(i)}|P_{\frac{1}{2}}\gt [/math]

Assuming that the masses of light non-strange quarks are just one third of the total nucleon mass [math]m_d=m_u=\frac{m_p}{3}=\frac{m_n}{3}[/math] and expressing the magnetic moment in units of [math]\frac{e}{2m_p}[/math] we get the following result [math]\mu_p=3[/math], which agrees with the findings of experiment. In addition, the quark parton model predictions of magnetic moments of the other baryons are compared with the experimental results below in Table 2. As it can be observed, it is in agreement with the experiment within the accuracy of 20 - 25 [math]%[/math].

Particle	The Quark Model Prediction	Experimental Result
p	3	2.79
n	-2	-1.91
[math]\Lambda[/math]	-0.5	-0.61
[math]\Sigma^+[/math]	2.84	2.46
[math]\Sigma^-[/math]	-1.16	-1.16 [math]\pm[/math] 0.03
[math]\Xi^0[/math]	-1.33	-1.25[math] \pm[/math] 0.01
[math]\Xi^-[/math]	-0.33	-0.65 [math]\pm[/math] 0.04

Table 2. Magnetic moment of baryons in units of nuclear magnetons ([math]\frac{e}{2m_p}[/math]). <ref name="Anisovich">Anisovich, V.V., Kobrinsky, M.N., Nyiri, J., & Shabelski, Yu. M. (2004). Quark Model and High Energy Collisions. World Scientific Publishing Co. Pte. Ltd.</ref>

The Quark Parton Model was succesful explaining the mass of baryons. The baryon masses can be expressed in the quark model using the de Rujula-Georgi-Glashow approach:

[math]m_B = \Sigma_i m_q(i)+ b \Sigma_{i\neq j}\frac{\sigma(i)\sigma(j)}{m_q(i)m_q(j)}[/math]

The difference between the actual experimental results and the predictions is in order of 5 -6 MeV. On the other hand, the similar formula for meson masses fails. The difference in meson mass case, between the experiment and calculation is approximately 100 MeV. This can be explained, by calculating the average mass of the quark in a baryon and meson <ref name="Anisovich">Anisovich, V.V., Kobrinsky, M.N., Nyiri, J., & Shabelski, Yu. M. (2004). Quark Model and High Energy Collisions. World Scientific Publishing Co. Pte. Ltd.</ref> :

[math]\lt m_q\gt _M = \frac{1}{2}(\frac{1}{4}m_\pi + \frac{3}{4}m_p)=303 MeV[/math]

[math]\lt m_q\gt _B = \frac{1}{3}(\frac{1}{2}m_N + \frac{1}{2}m_{\Delta})=363 MeV[/math]

Particle	Prediction ([math]MeV/c^{2}[/math])	Experiment ([math]MeV/c^{2}[/math])
N	930	940 [math]\pm[/math] 2
[math]\Delta[/math]	1230	1232 [math]\pm[/math] 2
[math]\Sigma[/math]	1178	1193 [math]\pm[/math] 5
[math]\Lambda[/math]	1110	1116 [math]\pm[/math] 1
[math]\Sigma^*[/math]	1377	1385 [math]\pm[/math] 4
[math]\Xi[/math]	1329	1318 [math]\pm[/math] 4
[math]\Xi^*[/math]	1529	1533 [math]\pm[/math] 4
[math]\Omega[/math]	1675	1672 [math]\pm[/math] 1

Table 3. Baryon mass predictions compared with experimental findings.<ref name="Anisovich">Anisovich, V.V., Kobrinsky, M.N., Nyiri, J., & Shabelski, Yu. M. (2004). Quark Model and High Energy Collisions. World Scientific Publishing Co. Pte. Ltd.</ref> <ref name="Camalich"> Camalich, J.M., Geng, L.S., & Vicente Vacas, M.J. (2010). The lowest-lying baryon masses in covariant SU(3)-flavor chiral perturbation theory. arXiv:1003.1929v1 [hep-lat]</ref>

Lattice QCD

Although the Quark Model successfully described several nucleon properties, it was not a fundamental theory opening the doorway for the development of new field theory called Quantum Chromodynamics. In the Quark Model, the particles of the baryon decuplet are symmetric in spin and flavor, so that the wave function that describes the fermions are fully symmetric and identical, which is a violation of the Pauli principle. As a solution the Quantum Chromodynamics suggested that quarks carry additional degree of freedom "color". Quarks have three degrees of freedom: spin, flavour and color. There are three states of color: red, green and blue.

Deep inelastic lepton nucleon scattering experiments gave us opportunity to measure the momentum weighted probability density function of partons in the proton and neutron. The fraction of the nucleon momentum carried by the quarks can be calculated by integrating the probability density function:

[math]\frac{18}{5}{\int_0}^1 dx {F_2}^{eN}(x) = {\int_0}^1 dx [u(x) + d(x) + \overline{d}(x) + \overline{u}(x)][/math]

The last expression shows that the quarks inside the nucleon carry about 50 % of the total momentum. It leads to the question, are quarks the only particles inside the nucleon? In conclusion, in addition to the quarks and antiquarks, there are other components and they cant be seen by using electromagnetic (electron) and weak (neutrino) probe, because the do not carry weak or electric charge.

As it was mentioned above scaling behavior was given by assumption that the nucleon is built by non-interacting pointlike quarks and antiquarks. However, by increasing the four-momentum transferred squared [math]Q^2[/math] one can see that inside the nucleon there are more components then just three charged quarks.

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It was concluded that a nucleon consists of three main quarks so called "valence" quarks which carry the quantum numbers of the nucleon and a "sea" of quark-antiquark pairs. The interaction between the quark-antiquark are mediated by the gluons. Unlike QED, where photon doesn't carry the charge, in QCD, gluon has a color charge and they can interact with each other. In other words, QCD is a theory where a field quanta is at the same time a field source. That makes QCD a non-Abelian field theory.

QCD allowes the following interactions

[math]q \rightarrow q + g[/math]

[math]g \rightarrow q + \bar{q}[/math]

[math]g \rightarrow g + g[/math]

The colors carried by the eight gluons are following: [math]R\bar{B}[/math], [math]R\bar{G}[/math], [math]B\bar{R}[/math], [math]G\bar{R}[/math], [math]B\bar{G}[/math], [math]G\bar{B}[/math], [math](R\bar{R} - G\bar{G})/\sqrt{2}[/math], [math](R\bar{R} + G\bar{G} - 2B\bar{B})/\sqrt{6}[/math].

The color is not experimentally observable, only "colorless" quark antiquark systems are observed: baryons(qqq), mesons([math]q\bar{q}[/math]) and antibaryons([math]\bar{q}\bar{q}\bar{q}[/math]).

The confinement of the quark antiquark system can be explained by the fact that color force increases with the separation increase. As separation decreases the force becomes, so that the quarks no longer interact. This phenomenon is referred as an asymptotic freedom. The strong coupling in QCD is defined to first order the following way:

[math]\alpha_s(Q^2) = \frac{1}{\beta_0 ln(Q^2/\Lambda^2_{QCD})}[/math],

[math]\beta_0 = \frac{33 - 2n_f}{12\pi}[/math]

where [math]\Lambda_{QCD}[/math] is found experimentally and [math]n_f[/math] is the number of active quark flavors. At [math]Q^2 \sim \Lambda_{QCD}[/math], [math]\alpha_s \rightarrow \infty[/math] the quark confinement takes place.

The perturbative QCD is used to describe?? the deep inelastic scattering, because of incapacity to calculate more than a few non-perturbative quantities within the QCD.

"The two most striking features of QCD are confinement and asymptotic freedom, and both are somehow related to the running of the coupling constant, a feature of all quantum field theories.

Confinement. All observed particles are colourless: as two colour charges move apart, their interaction grows strong enough to create colour-anticolour pairs from the vacuum.These colour charges recombine with the original charges to form colourless objects in a process called hadronization. Thus, confinement is related to the rising of the coupling constant as the distance between charges becomes large, or equivalently as the energy scale Q2 goes to zero.

Asymptotic freedom. The interaction between quarks asymptotically tends to zero as the distance between quarks goes to zero. As a consequence, quarks in the nucleon can be considered free particles. Thus, asymptotic freedom is related to the falling of the coupling constant as the distance between charges becomes small, or equivalently as the energy scale Q2 goes to infinity."

Semi Inclusive Deep Inelastic Scattering

Deep inelastic scattering (DIS) of leptons on nucleons is the most powerful experimental tool for the investigation of the structure of nucleons. In experiments both the charged (electrons, muons) and neutral (neutrinos) leptons are used with their antiparticles. In deep inelastic scattering the scattering occurs on a single nucleon or on a bound protons and neutrons inside the nucleus. At large momentum transfer the inelastic scattering is the incoherent sum of elastic scattering off the nucleon constituents, which are assumed to be dimensionless pointlike quarks. In the Constituent quark model (CQM) the constituents of the hadron are up and down quarks, whereas in the Quantum Chromodynamics the nucleon is a composition of quarks, antiquarks and gluons.

In inclusive deep inelastic scattering, only the electron is detected in the final state while in the case of semi inclusive deep inelatic scattering, a hadron is detected in coincidence with the scattered electron. Both physics processes can be characterized by the differential cross section. The cross section is proportional to the detection rate. The differential cross section for inclusive deep inelastic scattering can be written in terms of a lepton and a hadronic tensor <ref name="RobertsSpinStructure">Roberts, R. G. (1990). The structure of the proton. Cambridge Monographs on Mathematical Physics. Cambridge, UK: Cambridge University Press.</ref> :

[math]\frac{d^2\sigma}{dxdQ^2} \propto L_{\mu \nu} W^{\mu \nu}[/math]

where

[math]L_{\mu \nu} (k, k^') = 2 (k_\mu k^'_\nu + k^'_\mu k_\nu - \frac{1}{2} Q^2 g_{\mu \nu})[/math]

and

[math]W^{\mu \nu} = -W_1(g_{\nu \mu} +\frac{1}{Q^2} q_\mu q_\nu) + \frac{1}{M^2} W_2 (p_\mu +\frac{p \cdot q}{Q^2} q_mu)(p_\nu +\frac{p \cdot q}{Q^2} q_nu)[/math]

the leptonic tensor [math]L_{\mu \nu}[/math] describes the coupling between the scattering lepton and the virtual photon. The hadronic tensor [math]W^{\mu \nu}[/math] describes the absorption of the virtual photon by the target nucleon. The hadronic tensor contains information about the nucleon structure. It can be written in terms of structure functions using symmetry arguments and conservation laws. However, the information about the spin distribution inside the nucleon is contained in the asymmetric part of the hadronic tensor, which can be obtained by taking the difference of the cross sections with opposite spin states of the initial electron beam.

The polarized quark distribution functions can be extracted from SIDIS measurements using the quark flavor tagging method and exclude assumptions used in inclusive DIS measurements. In SIDIS the double spin asymmetry can be expressed in terms of the cross sections of final state hadrons produced in the experiment <ref name="Airapetian"> Airapetian, A., et al. (The HERMES Collaboration). (2005). Quark helicity distributions in the nucleon for up, down, and strange quarks from semi-inclusive deep inelastic scattering. Phys. Rev., D(71), 012003.</ref>:

[math]A_1^h = \frac{\sigma_{1/2}^h - \sigma_{3/2}^h}{\sigma_{1/2}^h + \sigma_{3/2}^h}[/math]

where [math]\sigma_{1/2}^h[/math] ([math]\sigma_{3/2}^h[/math]) represents the semi inclusive cross section of type $h$ hadrons produced in the final state when the spin of the initial electron beam was antiparallel(parallel) to the target nucleon spin.

The semi-inclusive cross section can be expressed in terms of quark distribution functions and fragmentation functions:

[math] \frac{d^3 \sigma^h_{1/2(3/2)}}{dxdQ^2 dz}\approx \Sigma_q e_q^2 q^{+(-)}(x,Q^2)D_q^h(z,Q^2)[/math]

The measured structure function in inclusive deep inelastic scattering experiments contains the contribution from all the different quark flavors to the total nucleon momentum and spin, without distinguishing the contribution from the individual quark flavors. Semi inclusive deep inelastic scattering experiments provide an opportunity to determine the struck quark flavor by detecting the hadron in the final state in coincidence with an electron.

The kinematics of single pion electroproduction in SIDIS can be described by five variables: the virtual photon four-momentum transfered squared [math]Q^2[/math], invariant mass of the photon-nucleon system [math]W[/math], the polar [math]{\theta_{\pi}}^*[/math] and the azimuthal angle [math]{\varphi_{\pi}}^*[/math] of the outgoing pion in the center of mass frame, and the scattered electron azimuthal angle [math]{\varphi}_e[/math].

Diagram of The Semi Inclusive Deep Inelastic Scattering<ref name="Airapetian"> Airapetian, A., et al. (The HERMES Collaboration). (2005). Quark helicity distributions in the nucleon for up, down, and strange quarks from semi-inclusive deep inelastic scattering. Phys. Rev., D(71), 012003.</ref>

The incoming electron with four momentum [math]k = (E[/math], [math]\vec{k}[/math]) is scattered from the target of four momentum ([math]M[/math], [math]\vec{0}[/math]), where [math]M[/math] represents the rest mass of the target nucleon. The four momentum of the scattered electron and hadron are respectively [math]k^{'}[/math] = ([math]E^{'}[/math], [math]\vec{k^{'}}[/math]) and [math]p_h[/math] = ([math]E_h[/math], [math]\vec{p_h}[/math]). Semi inclusive deep inelastic scattering is depicted in Figure. 1. The four momentum of the exchanged virtual photon, through which the SIDIS occurs, is the four momentum lost by the initial electron [math]q = k - k^'[/math]. The negative square of the four momenta can be written as [math]Q^2 = - q^2|_{lab} = 4EE^{'}\sin^{2} \frac{\theta}{2}[/math], where [math]Q^2[/math] is greater then zero. The energy transferred from the scattering electron to the target nucleon, which is also the energy of the virtual photon, is given by

[math]\nu = \frac {p \cdot q}{M} = E - E^{'}|_{lab}[/math]

The Bjorken scaling variable x is defined as

[math]x = \frac {Q^2}{2 p \cdot q} = \frac {Q^2}{2M \nu}[/math]

The fraction of the virtual photon energy transferred to a hadron, that is detected in the final state in coincidence with the scattered electron, is

[math]z = \frac{p\cdot p_h}{p\cdot q} =^{lab} \frac{E_h}{\nu}[/math]

where the last kinematical variable is the invariant mass of the scattering process available to produce the final hadronic state

[math]W^2 = (q + p_h)^2 = M^2 + 2 M \nu -Q^2[/math]

Kinematic variables in deep inelastic scattering

Kinematic variable	Description
[math]k = (E, k)[/math], [math]k = (E^', k^')[/math]	4 - momenta of the initial and final state leptons
[math]\theta[/math], [math]\phi[/math]	Polar and azimuthal angle of the scattered lepton
[math]P^{lab} = (M, 0)[/math]	4 - momentum of the initial target nucleon
[math]q = k - k^'[/math]	4 - momentum of the virtual photon
[math]Q^2 = - {q^2} ^{lab} = 4EE^'\sin^2 \frac{\theta}{2}[/math]	Negative squared 4 - momentum transfer
[math]\nu = \frac {p \cdot q}{M} =^{lab} E - E^'[/math]	Energy of the virtual photon
[math]x = \frac {Q^2}{2 p \cdot q} = \frac {Q^2}{2M \nu}[/math]	Bjorken scaling variable
[math]y = \frac{p \cdot q}{Pk} =^{lab} \frac{\nu}{E}[/math]	Fractional energy of the virtual photon
[math]W^2 = (p + q)^2 = M^2 + 2M\nu - Q^2[/math]	Squared invariant mass of the photon-nucleon system
[math]p = (E_h, p)[/math]	4 - momentum of a hadron in the final state
[math]z = \frac{p\cdot p_h}{p\cdot q} =^{lab} \frac{E_h}{\nu}[/math]	Fractional energy of the observed final state hadron

The electron scattering cross section off a nucleon can be written as <ref name="RobertsSpinStructure">Roberts, R. G. (1990). The structure of the proton. Cambridge Monographs on Mathematical Physics. Cambridge, UK: Cambridge University Press.</ref> :

[math]\frac{d^2 \sigma}{dQ^{2}dW^{2}} = \frac{2 \pi \alpha^2 M}{(s-M^2)^2Q^2} [2W_1 (W^2,Q^2) + W_2(W^2,Q^2)(\frac{(s-M^2)(s-W^2-Q^2)}{M^2Q^2}-1)][/math]

where

[math]s=(p + k)^2[/math]

and in the target rest frame it can be expressed in terms of the initial and final energies of the electron and the electron scattering angle [math]\theta[/math]:

[math]\frac{d^2 \sigma}{d\Omega d E^{'}} = \frac{\alpha^{2} M}{8E^{2}E_p \sin^4\frac{\theta}{2}}[2W_1\sin^2\frac{\theta}{2} + W_2 \frac{4E^2_p}{M^2}\cos^2\frac{\theta}{2}][/math]

where [math]W_1[/math] and [math]W_2[/math] are so called structure functions, [math]E_p[/math] and [math]E[/math] the energy of the initial proton and electron respectively, [math]\theta[/math] the polar angle of the scattered electron. [math]M[/math] is the mass of the target, in our case the proton.

As it was mentioned above, the DIS interaction doesn't happen with the hadron as a whole, but with one of its constituents. Each quark(constituent) carries the fraction four-momentum [math]x[/math] of the nucleon with probability density [math]q(x)[/math]. [math]q(x)[/math] is the probability of finding the [math]q[/math]th quark with fraction [math]x[/math] of the nucleon four-momentum. Under these assumptions, the structure functions can be written as a sum of the elastic structure functions weighted by [math]q(x)[/math]. Taking into consideration that the mass of the [math]i[/math]th quark is also the fraction [math]x[/math] of the nucleon mass [math]M_q = x M_h[/math]:

[math]W_1(Q^2, \nu ) =\Sigma_q \int_0^1 dx q(x) e_q^2 \frac{Q^2}{4x^2 M_h^2} \delta (\nu - \frac{Q^2}{2M_hx}) = \Sigma_q e_q^2 q(x_B)\frac{1}{2M_h}[/math]

and

[math]W_2(Q^2, \nu ) =\Sigma_q \int_0^1 dx q(x) e_q^2 \delta (\nu - \frac{Q^2}{2M_hx}) = \Sigma_q e_q^2 q(x_B)\frac{x_B}{\nu}.[/math]

The DIS of the unpolarized electron by a nucleon can be described in terms of two structure functions, [math]F_1(x)[/math] and [math]F_2(x)[/math] where:

[math]F_1(x) = M_h W_1 = \frac{1}{2}\Sigma_q e_q^2q(x)[/math]

and

[math]F_2(x) = \nu W_2 = \frac{1}{2}\Sigma_q x e_q^2 q(x)[/math]

The relation between the structure functions [math]F_1(x)[/math] and [math]F_2(x)[/math] is given by the following equation:

[math]F_2(x) \frac{1+\gamma^2}{1+R} = 2 x F_1(x)[/math]

where [math]R(x,Q^2)[/math] is the ratio of longitudinal to transverse deep inelastic scattering cross sections and [math]\gamma = \sqrt{\frac{Q^2}{\nu^2}}[/math]. In the naive quark parton model the longitudinal-transverse interference is neglected. In the Bjorken limit it can be reduced to the Callan-Gross relation:

[math]F_2(x) = 2 x F_1(x)[/math]

The structure function [math]F_1[/math] measures the parton density, while [math]F_2[/math] describes the momentum density.

The distributions of up and down quarks in the nucleon are defined as [math]u(x)[/math] and [math]d(x)[/math]. There are two categories of quarks: valence and sea quarks [math]u(x) = u_v(x) + u_s(x)[/math], assuming that [math]u_s(x)=\bar{u}(x)[/math]. The constituent quark model (CQM or QPM) states that the proton(neutron) contains two up(down) quarks and one down(up) quark. Summing over all the constituents of a proton should result in the following sum rule:

[math]\int_0^1 dx u_v(x) = 2[/math]

and

[math]\int_0^1 dx d_v(x) = 1[/math]

The electromagnetic structure function for the proton and neutron can be expressed in terms of quark distribution functions:

[math]F_2^{ep} = \frac{4}{9}[xu(x) + x\bar{u}(x) + xc(x) + x\bar{c}(x)] + \frac{1}{9}[xd(x) + x\bar{d}(x) + xs(x) + x\bar{s}(x)][/math]

[math]F_2^{en}[/math] can be obtained from [math]F_2^{ep}[/math] by replacing [math]u[/math] [math]\rightarrow[/math] [math]d[/math] and vice versa. From the last two equations the structure functions for the proton and neutron can be written in terms of valence quark distribution functions:

[math]F_2^{ep} = x [ \frac{4}{9} u_v(x) + \frac{1}{9} d_v(x) ][/math]

and

[math]F_2^{en} = x [ \frac{4}{9} d_v(x) + \frac{1}{9} u_v(x) ][/math]

For most fixed-target experiments like EG1, the spin asymmetry is given by the ratio of the polarized structure function to the unpolarized: [math]A(x, Q^2) = \frac{g_1(x)}{F_1(x)}[/math], where the polarized structure function [math]g_1(x)[/math] represents the helicity difference of quark number densities. The spin asymmetry [math]A[/math] and the unpolarized structure function [math]F_1[/math] are measurable quantities and through them one can determine [math]g_1(x)[/math], which maybe expressed as :

[math]g_1(x) = \frac{1}{2} \Sigma_q e_q^2 (q^+(x) - q^-(x)) \equiv \frac{1}{2}\Sigma_q e_q^2 \Delta q(x)[/math]

where [math]q^{+(-)}(x)[/math] is the quark distribution function with spin oriented parallel(antiparallel) to the spin of nucleon.

Fragmentation Independence

The asymmetries from semi inclusive pion electroproduction using proton or deuteron targets can be written in terms of the difference of the yield from oppositely charged pions <ref name="Christova"> Christova, E., & Leader, E. (1999). Semi-inclusive production-tests for independent fragmentation and for polarized quark densities. hep-ph/9907265.</ref>:

[math]A_{1,p}^{\pi^+ \pm \pi^-} = \frac{\Delta \sigma_p^{\pi^+ \pm \pi^-}}{\sigma_p^{\pi^+ \pm \pi^-}} = \frac{[({\sigma_p}^{\pi^+})_{1/2}-({\sigma_p}^{\pi^+})_{3/2}] \pm [({\sigma_p}^{\pi^-})_{1/2}-({\sigma_p}^{\pi^-})_{3/2}]}{[({\sigma_p}^{\pi^+})_{1/2}+({\sigma_p}^{\pi^+})_{3/2}] \pm [({\sigma_p}^{\pi^-})_{1/2}+({\sigma_p}^{\pi^-})_{3/2}]}[/math]

[math]A_{1,2H}^{\pi^+ \pm \pi^-} = \frac{\Delta \sigma_{2H}^{\pi^+ \pm \pi^-}}{\sigma_{2H}^{\pi^+ \pm \pi^-}} = \frac{[({\sigma_{2H}}^{\pi^+})_{1/2}-({\sigma_{2H}}^{\pi^+})_{3/2}] \pm [({\sigma_{2H}}^{\pi^-})_{1/2}-({\sigma_{2H}}^{\pi^-})_{3/2}]}{[({\sigma_{2H}}^{\pi^+})_{1/2}+({\sigma_{2H}}^{\pi^+})_{3/2}] \pm [({\sigma_{2H}}^{\pi^-})_{1/2}+({\sigma_{2H}}^{\pi^-})_{3/2}]}[/math]

Independent fragmentation identifies the process in which quarks fragment into hadrons, independent of the photon-quark scattering process. In other words, the fragmentation process is independent of the initial quark environment which initiates the hadronization process. Assuming independent fragmentation and using isospin ([math]D_u^{\pi^+} = D_{\overline{u}}^{\pi^-}[/math] and [math]D_d^{\pi^-} = D_{\overline{d}}^{\pi^+}[/math] ) and charge ([math]D_u^{\pi^+} = D_d^{\pi^-}[/math]) conjugation invariance for the fragmentation functions, the following equality holds:

[math]D_u^{\pi^+ \pm \pi^-} = D_u^{\pi^+} \pm D_u^{\pi^-} = D_d^{\pi^+ \pm \pi^-}[/math]

The polarized and unpolarized cross sections for pion electroproduction can be written in terms of valence quark distribution functions in the valence region as:

[math]\Delta \sigma_p^{\pi^+ \pm \pi^-} = \frac{1}{9}[4(\Delta u + \Delta \bar{u}) \pm (\Delta d + \Delta \bar{d})]D_u^{\pi^+ \pm \pi^-}[/math]

[math]\Delta \sigma_n^{\pi^+ \pm \pi^-} = \frac{1}{9}[4(\Delta d + \Delta d^-) \pm (\Delta u + \Delta u^-)]D_u^{\pi^+ \pm \pi^-}[/math]

[math]\Delta \sigma_{2H}^{\pi^+ \pm \pi^-} = \frac{5}{9}[(\Delta u + \Delta \bar{u}) \pm (\Delta d + \Delta \bar{d})]D_u^{\pi^+ \pm \pi^-}[/math]

and unpolarized:

[math]\sigma_p^{\pi^+ \pm \pi^-} = \frac{1}{9}[4( u + \bar{u}) \pm ( d + \bar{d})]D_u^{\pi^+ \pm \pi^-}[/math]

[math]\sigma_n^{\pi^+ \pm \pi^-} = \frac{1}{9}[4(d + \bar{d}) \pm (u + \bar{u})]D_u^{\pi^+ \pm \pi^-}[/math]

[math]\sigma_{2H}^{\pi^+ \pm \pi^-} = \frac{5}{9}[( u + \bar{u}) \pm ( d + \bar{d})]D_u^{\pi^+ \pm \pi^-}[/math]

In the valence region ([math]x_{B}\gt 0.3[/math]), where the sea quark contribution is minimized, the above asymmetries can be expressed in terms of polarized and unpolarized valence quark distributions:

[math]A_{1,p}^{\pi^+ \pm \pi^-} = \frac{4 \Delta u_v(x) \pm \Delta d_v(x)}{4u_v(x) \pm d_v(x)}[/math]

[math]A_{1,2H}^{\pi^+ \pm \pi^-} = \frac{\Delta u_v(x) + \Delta d_v(x)}{u_v(x) + d_v(x)}[/math]

The ratio of polarized to unpolarized valence up and down quark distributions may then be written as

[math]\frac{\Delta u_v}{u_v}(x,Q^2) = \frac{\Delta \sigma_p^{\pi^+ \pm \pi^-} + \Delta \sigma_{2H}^{\pi^+ \pm \pi^-}}{\sigma_p^{\pi^+ \pm \pi^-} + \sigma_{2H}^{\pi^+ \pm \pi^-}} (x,Q^2)[/math]

and

[math]\frac{\Delta d_v}{d_v}(x,Q^2) = \frac{\Delta \sigma_p^{\pi^+ \pm \pi^-} - 4\Delta \sigma_{2H}^{\pi^+ \pm \pi^-}}{\sigma_p^{\pi^+ \pm \pi^-} - 4\sigma_{2H}^{\pi^+ \pm \pi^-}} (x,Q^2)[/math]

The ratio of polarized to unpolarized valence quark distribution functions can be extracted using the last two equations.

Independent Fragmentation Function Test

A test of independent fragmentation can be performed with polarized proton and neutron targets. The ratio of the difference of polarized to unpolarized cross sections for proton and neutron targets [math]\Delta R_{np}^{\pi^+ + \pi^-}[/math] can be written in terms of the structure functions:

[math]\Delta R_{np}^{\pi^+ + \pi^-} = \frac{\Delta \sigma_p^{\pi^+ + \pi^-} - \Delta \sigma_{n}^{\pi^+ + \pi^-}}{\sigma_p^{\pi^+ + \pi^-} - \sigma_{n}^{\pi^+ + \pi^-}}=[/math]

[math]=\frac{(\Delta u +\Delta \bar{u}) - (\Delta d + \Delta \bar{d})}{(u+\bar{u}) - (d+\bar{d})}(x,Q^2)=[/math]

[math]= \frac{g_1^p - g_1^n}{F_1^p - F_1^n}(x,Q^2)[/math]

The last expression of the asymmetry [math]\Delta R_{np}^{\pi^+ + \pi^-}[/math] was obtained from the following equations:

[math]g_1^p - g_1^n = \frac{1}{6}[(\Delta u +\Delta \bar{u}) - (\Delta d + \Delta \bar{d})][/math]

and

[math]F_1^p - F_1^n = \frac{1}{6}[(u+\bar{u}) - (d+\bar{d})][/math]

Independent fragmentation holds if the ratio of the difference of polarized to unpolarized cross sections for proton and neutron targets [math]\Delta R_{np}^{\pi^+ + \pi^-}[/math] depends only on [math]x[/math] and [math]Q^2[/math] of the quantities [math]g_1[/math] and [math]F_1[/math] measured in deep inelastic scattering and is independent of [math]z[/math].

Notes

<references/>

Delta_D_over_D