Lepton Scattering Cross Section and Nuclear Structure Function of 4 He and 12 C Nuclei

This paper is an effort to extract the structure function, the EMC ratio, and the lepton scattering cross section in the convolution nuclear theory framework for He and C nuclei. We suppose that, in conventional approach, based on harmonic oscillator model, one could consider for a nucleus shell different parameters which are associated with the square root of the mean radius of the nucleus shells. We use GRV free nucleon structure function, which has good agreement with the proton and neutron structure function, extracted from experimental results. In addition, the lepton scattering cross sections of He and C nuclei are calculated in energy higher than 1 GeV. The extracted results show good agreement with experimental data. ω 


Introduction
One of the best methods of acquiring information about the structure of the bound nucleons inside the nuclei is the studying of the leptons scattering from the nuclei.This kind of scattering is due to weak electromagnetic interactions of quarks inside nuclei which gain a great deal of momentum from transferred momentum of virtual photon.In this process, the change of the whole structure of the nuclei is small and ignorable.The weak interacttions do not change the structure of the nuclei, so lepton scattering can be utilized to determine the structure of the nuclei [1].The experimental data, obtained from the deep inelastic leptons scattering from free and bound nucleons, have been get considerable information about the structure function of the free and bound nucleons.This accomplishment was published in 1983 by EMC group under Aubert supervision [2].The EMC group found out that the bound nucleons inside the nuclei have different momentum distribution in comparison with the free nucleons [2] there is a lot of explained theory about this difference such as Fermi motion [3,4] and the binding energy [5,6], quark exchange effect [7], pionic contribution [8,9], shadowing effect [10] and presence of the ∆ particles [11].In this paper, with considering Fermi motion and binding energy effects, which have major roles in difference between the structure function of the free and bound nucleons, the structure function and EMC ratio in the conventional nuclear theory for 4 He and 12 C nuclei are calculated by using harmonic oscillator model with considering different parameters for different shells inside the nucleus have been investigated.For calculating the structure function and the EMC effect, we imply the GRV structure function of free nucleon [12].Finally, we calculate the differential cross section leptons scattering from 4 He and 12 C nuclei.It is shown that the obtained results have good agreement with experimental data.ω 

Convoluted Nuclear Structure Function
The structure function of nucleus in convolution model can be obtained by using the following equation [5]: where the first sum is over proton and neutron cases.The second sum is over the quantum number of states.The The momentum distribution function of the nucleons inside the nucleus is given by [5]: where is the bjorken variable for the free nucleon.The effects of the momentum and energy distribution of the nucleon in the nucleus are included in Equation ( 2) through and nl , respectively.The magnitude of the nuclear binding energy nl mainly affects the structure function in the intermediate x region.The momentum and energy distribution of a nucleon inside a nucleus is expressed by f z that satisfies the normalization rule as below [3]: When the gluons and sea quark are considered, sum rule becomes as: Equation ( 2) describes the momentum and energy distribution of nucleons inside nuclei.In order to calculate ( ) ϕ the harmonic-oscillator nuclear wave function is used.Since in the nucleus the deeper closed shells have different root mean square radius, each shell of a nucleus has different root mean square radius from others as [13]: Where 2 n m ω α =  and in the natural unite, we have: where m n = 938.905MeV is a nucleon mass, The calculated data for 2 2 1 r and ħ are expressed in Table 1 for 2 H, 4 He and 12 C nuclei.2) we use the below expression to describe the momentum distribution and energy of the nucleons in a nucleus as [5]: n l n l n t n t t t For ( ) F x z we use the GRV free proton and neutro un showed that the structure func-n str ctions [12], and we ignore the contribution of strange quark, the structure function of 2 H, 4 He and 12 C nuclei are plotted in Figure 1 based on Ref. [12].

The EMC Ratio ucture f
The experimental results tion of a nucleus could not be obtained by summing all of the structure function of the nucleons inside the nucleus [2].Since there are some factors like Fermi motion [3,4], binding energy [5,6], quark exchange [7], pionic contribution [8][9], and the shadowing effect [10], presence of ∆ particle [11], that cause to this difference.One of the main reasons to this difference is the Fermi motion effect that impresses the structure function of nucleus in x→1.The nuclear structure function is incoherent sum of the structure function of constituted nucleons, therefore the Fermi motion has effect on the nuclear structure function.In addition, the nuclear wave function is the convolution of the free nucleon wave function by momentum distribution of nucleon, therefore the binding energy also has effect on nuclear structure function.
To show the difference between the free nucleon with the bound nucleon inside the nucleus, the EMC ratio could be expressed as follows [2,5]: Figure 2 shows the EMC ratio, R(x), when Fer tio mi mon and binding energy are considered.When x arise to 1, it is seen that x > .In this region, one can see that the structure fun f 4 He and 12 C are very small, however the structure function of free nucleon vanishes, so when x arise to 1 the ( ) x goes to above 1.Because of the structure function ucleus vanishes when x approach to A (A > 1), which is atomic number of nucleus.We should remark that x is the fraction of momentum that is carried by nucleons inside the nucleus.x > 0.8 is the Fermi motion region, and in this region nucleons have Fermi-like motions [17,18].

Deep Inelastic Scattering
Particle collision in low energy is the other word this kind of collision particles.Otherwise, if particles have enough energy when they collide to each other they create new particles.This kind of collision is called inelastic scattering.In deep inelastic scattering, the number of scattered particles with large angles demonstrates that the protons have inner structures.When leptons incident on nuclei and produce new particles, this deep inelastic scattering could be seen as the elastic scattering of leptons from nuclei constituted particles i.e. partons [20].
The differential cross section could be expressed by [21]:

Results and Discussion
These f mention that, in o paring our results with that nuclear interactions Based on the calculations and com the previous works, we conclude specially binding energy effects and the new assumptions considered in this paper can clarify both qualitatively and quantitatively the deep inelastic lepton-nuclear scattering without considering the nucleon's quark structure changes.
the structure function of nucleons which we have used the GRV structure function of neutron and proton.
ħ are expressed in Fermi and MeV unit, respectively.

Figure 1 .
Figure 1.The structure function of 2 H, 4 He and 12 C nuclei.In order to obtain the nucleus structure function we have used the GRV structure function of the free proton.The experimental data are taken from [15,16].

Figure 2
Figure 2. The on GRV nucleon structure function of free proton and neutron [12] i.e. dashed and the other have been taken from Ref. [5] i.e. dashdouble dotted.The experimental data have been taken from Ref. [19].

2 ν
the fine structure constant, mentum transfer s four-mo quared is Q .Initial and scattered lepton energies are E and E′ , respectively.Energy of the virtual photon is E E

Figure 3
shows the scattering differential cross section of leptons from the4 He nucleus, fo are plotted with dashdouble-dotted, also, for θ = 29˚, with d These curves show our main results.Of course we should der to obtain the results of Figure3(a) we have used the GRV free nucleon structure function[12], and to obtain the results of Figure3(b) we have used the nucleon structure function used in Ref.[5].Also Figure4demonstrates the scattering differential cross section of leptons from the 12 C nucleus, for E = 5.86 GeV, θ = 30˚, and ash-dotted as well.with dash-dotted as well.igures show our main results.Of course we should rder to obtain the results of Figure4(a) we have used the GRV free nucleon structure function[12], and to obtain the results of Figure4(b) we have used the nucleon structure function used in Ref.[5].

Figure 3 .
Figure 3.The (a) and (b) diagrams 4 He nuclei.We have u d the GRV nucleon structure funct in (a) and nucleon structure show the deep inelast of electron beam from ion [12] for calculation of nucleus structure function that plotted ic cross section se function from [5] for calculating of nucleus structure function that plotted in (b) diagram.The dash-double-dotted and dot and dash-dotted cures shows our calculation.The CGA, CGA + CT, PWIA curves, and experimental data have been taken from [22].

Figure 4 .
Figure 4.The (a) and (b) diagrams show the 12 C nuclei.We have used the GRV nucleon structure functio n (a) and nucleon structure