The measurements of the top-quark transverse momentum distribution have been performed at the Fermilab Tevatron collider at 
= 1800 and 1960 GeV by the CDF [
collider in 1995 by the CDF and DØ Collaborations [3,4] at a mass of around 170 GeV. It is expected [5-12] that the top physics is extremely important for scientific search for new phenomena.
In the given paper we have analyzed the DØ data using the method known as z-scaling [13,14]. Main features of the approach in pp and 
interactions at FNAL, CERN, and BNL (RHIC) energies were presented and discussed in [15,16]. Some results of analysis of the LHC data on the charged hadron [
-meson [
and scaling variable z are expressed via experimentally measurable quantities: inclusive and total inelastic cross sections, multiplicity density, momenta and masses of colliding and produced particles and using some physical parameters. The shape of the scaling function was found to be independent of the collision energy, multiplicity density of particles, detection angle and hadron type. The power behavior of function 
was established in high-z (high-pT) range. At low z (lowpT), saturation of the scaling function was found down to a value of 
10−3 [16,22]. It has been concluded that z-scaling reflects self-similarity of the hadron structure, constituent interactions and hadronization process. The analyzed experimental data cover a wide range of the collision energies, transverse momenta and angles of the produced particles. The energy, angular and multiplicity independence of scaling function 
gives strong constraints on the values of parameters δ, c, and ε entering in definition of z. The parameter c which controls the behavior of 
at low z has analogy with the “specific heat” of the produced medium associated with the inclusive particle production. The scaling in pp and 
collisions is consistent with the constant value of c = 0.25. A possible change of this parameter could be assumed to be an indication of the phase transition of the matter produced in high energy collisions. The structure of the interacting objects produced at high momenta is characterized by parameter 
interpreted as a nucleon fractal dimension. The scaling is consistent with the constant value of δ = 0.5 for all types of the analyzed inclusive hadrons. The fragmentation process is parameterized in terms of dimension 
which increases together with the hadron mass.
In this paper we have analyzed the data [
collisions at energy 
= 1960 GeV in the middle rapidity range obtained by the DØ Collaboration at the Tevatron. The measurements select the events with an isolated lepton having transverse momentum pT of at least 20 GeV/c and a pseudo-rapidity of 
1.1 (e + jets) or 
2.0 (μ + jets). A cut on the missing transverse energy of 20 GeV was applied. Furthermore at least four jets were required with pT > 20 GeV/c and 
2.5, an additional cut of pT > 40 GeV/c was applied for the leading jet. Finally at least one jet needs to be identified as a b-jet. Additional constraints are used to reconstruct the event kinematics: the masses of two W bosons are constrained to 80.4 GeV. The masses of the two reconstructed top quarks are assumed to be equal.
The results of analysis of the top inclusive cross sections are compared with Tevatron data [24-26] on J/ψ, D0B, and Υ particle spectra at 
= 1960 and 1800 GeV in the z-presentation. We have verified the flavor independence of 
including the inclusive top-quark measurements in this region. A microscopic scenario of hadron production in the z-scaling approach is used to estimate the energy loss and recoil mass at a constituent level in the dependence on transverse momentum of an inclusive particle. This gives the specific dependence of the momentum fraction x1 characteristic for different types of produced hadrons. The pT-behavior of the fraction x1 for the top-quark production is compared with other particles.
We expect that systematic measurements of the inclusive differential spectra of the top-quark as a function of the transverse momentum at LHC energies could give new information on self-similarity of the heavy flavor production in the super high energy domain.
and
. The constituents of the incoming objects (hadrons or nuclei) with masses M1, M2 carry away fractions x1, x2 of their momenta P1, P2. The inclusive particle has a fraction (denoted by
) of the momentum of the object produced in the constituent collision in the observed direction. Its fragmentation is characterized by parameter
. The fragmentation in the recoil direction is described by parameter 
and momentum fraction
. Multiple interactions of the constituents are considered to be similar. This property reflects the self-similarity of the hadron interactions at the constituent level.
and 
in the final state. The produced secondary objects transform into real particles after the constituent collisions. The registered particle with mass m1 and 4-momentum p is produced with its hadron counterpart with mass m2 carrying the momentum fractions of the produced recoil. The momentum conservation law of the constituent sub-process is written in the following form:
.
, and 
which determine the underlying elementary sub-process.
, and
, respectively. The parameters are related with the corresponding momentum fractions by function
and
. The Ω is interpreted as a relative volume which occupies these configurations in the space of the momentum fractions. Parameters
, and 
are taken as fractal dimensions in the parts of the space of the momentum fractions which correspond to the colliding objects and fragmentation processes, respectively. For the given values of
, and 
the fractions 
and 
are determined in such a way to maximize the function Ω, simultaneously fulfilling condition (1).
) interactions we have 
and set
. It is assumed that the fragmentation of the objects moving in the scattered and recoil directions can be described by the same parameter 
which depends on the type of the inclusive particle. The values of parameters 
and 
are determined according to the self-similarity requirements of experimental data in z-presentation. They were found to have constant values in pp and 
collisions at high energies.
, and 
is the maximal value of (2) with condition (1). For the above inclusive reaction the quantity z is proportional to the transverse kinetic energy 
of the constituent subprocess consumed for the production of the inclusive particle and its counterpart with masses m1 and m2, respectively. The quantity 
is the corresponding multiplicity density of charged particles produced in the central region of the reaction at the pseudo-rapidity
. Parameter c characterizes properties of the produced medium. It is interpreted as “specific heat”. The constant mN is taken to be a nucleon mass.
is expressed in terms of the experimentally measured inclusive cross section
, the multiplicity density
, and the total inelastic cross section 
as follows [
in (4) depends on the center-of-mass energy, centrality, and on the production angles at which the inclusive spectra were measured. The above expression can be rewritten in the central interaction region into the following form:
as a probability density of the production of the inclusive particle with the corresponding value of variable z.
in z-presentation [15,16]. Our previous analysis is based on the observation that simultaneous energy, angular and multiplicity independence of the z-scaling for negative pions, kaons, and anti-protons produced in proton-proton collisions gives the same shape of the scaling function. The flavor independence of 
was also confirmed for other inclusive particles including the heavy quarkonia, J/ψ [
= 1960 and 1800 GeV. The property of 
was observed at very small values of 
10−3. In the region 
0.1 we observe a saturation of scaling function 
which can be approximated by a constant.
for different hadron species. Parameter 
is the scale independent quantity. The transformation does not destroy the shape of
. It preserves the normalization Equation (6) and the energy, angular and multiplicity independences of the z-presentation of particle spectra.
collisions at the Tevatron energies 
= 1960 and 1800 GeV in the central rapidity region. The experimental data are shown by symbols. The data include measurements up to small transverse momenta (pT ≈ 125 MeV/c for charmonia, pT ≈ 290 MeV/c for bottomia, and pT ≈ 500 MeV/c for B-mesons). The data on the 
-meson spectra at 
= 53 GeV [
collisions in the range z = 0.001 - 4. This is indicated by the solid line. One can see that distributions of different hadrons are sufficiently well described with a single curve over a wide z-range (0.001 - 10). Function 
changes more than by six orders of magnitude in this region. The values of parameters 
and 
shown in this 
, pT, and
). The scale factors 
are constants. It allows us to describe z-presentation of the spectra for different hadron species with a single function. The collapse of data points onto a single curve corresponds to the estimated errors of 
at the level of 20%.
collisions at the energy 
= 1960 GeV and the central rapidity range in zpresentation. The solid line is the same curve as depicted in 
for the topquark distribution was calculated according to Equation (5). The vertical errors are given by a quadratic sum of the statistical uncertainties and the systematic uncertainties on the shape of the cross section in each pT-bin. The
and n = 2. This corresponds to two entries per event with the total normalization to the 
production cross section 
= 8.31 pb [
= 0.5 and “specific heat” c = 0.25 are the same as used in the previous analyses of the inclusive spectra [15,16,21]. We have set 
in the case of the top-quark since no energy loss is assumed in the elementary 
production process. This choice corresponds to 
in the whole pT-range. The value of 
in the transformation (7) is found to be 
0.0045. No additional parameters were used.
) collisions for other particles sufficiently well. Note that the top-spectrum is in the limited kinematic region and the error bars of the data are large enough. We would like to stress that existing analyses were performed with pT-distributions of the inclusive cross sections 
which reveal strong dependence on the energy, angle, multiplicity and type of the produced particles. Based on the above comparison we have concluded that the Tevatron data on inclusive spectra of the top-quark production measured by the DØ Collaboration support the flavor independence of scaling function 
over the range of z = 0.02 - 2. This result gives us an indication on self-similarity of top-quark production in 
collisions at 
= 1960 GeV.
and by the value of recoil mass MX which is practically equal to the mass of the top-quark. The kinematics of the underlying sub-process is fully determined by momentum fractions x1 and x2 in this case. The fractions characterize the amount of the energy (momentum) of the incoming protons (antiprotons) carried by the interacting constituents which cause the inclusive particle production. In the general case of other particles, x1 and x2 are functions of ya and yb [
. One can see the x1 growth with
. The value of x1 is larger for the production of heavy particles as compared with the light ones. The exception for J/ψ meson was observed (see discussed in [
related
the fraction x1 decreases while increasing collision energy
. The kinematic limit of the reaction 
corresponds to 
at any collision energy and for any type of the inclusive particle.
collisions at the energy 
= 1960 GeV measured by the DØ Collaboration at the Tevatron. The transverse momentum spectra in z-presentation are compared with the data obtained for the heavy mesons J/ψ, D0, B, and Υ at the Tevatron energies 
= 1960 and 1800 GeV in the central rapidity range. Based on the results presented here we conclude that the data on the transverse momentum distribution of the top-quark production in 
collision are in good agreement with flavor independence of the z-scaling. The result also supports the energy independence of the scaling function in the middle rapidity region. A tendency to 
saturation at low z for the top-quark production is confirmed as well. The momentum fraction x1 of the incoming protons for the top-quark was compared with the corresponding values for the heavy mesons measured at the Tevatron. Though production of the top-quark is characterized by no energy loss and constant recoil mass
, the fraction x1 reveal similar dependences on the scaled transverse momentum 
as for the heavy mesons.
at the Tevatron and LHC could be of interest to verify the flavor independence of z-scaling and self-similarity of top-quark production.