820 research outputs found
Difference in multiplicity distributions in proton-proton and proton-antiproton collisions at high energies
Secondary charged hadrons multiplicity distributions in proton-proton and
proton-antiproton collisions differ on principle. There are three types of
inelastic processes in proton-antiproton scattering. The first type is
production of secondary hadrons shower at gluon string decay. The second type
is shower produced from two quark strings decay, the third type is shower
produced from three quark strings decay. At the same time there are only two
types of inelastic processes for proton-proton scattering - gluon string shower
and two quark strings shower. Theoretical description of multiplicity
distributions is obtained for proton-proton collisions at energies from 44.5
GeV to 200 GeV and for proton-antiproton collisions at energies from 200 GeV to
1800 GeV. The difference between proton-proton and proton-antiproton
multiplicity distributions is discussed. The predictions of multiplicity
distribution and mean multiplicity at LHC energy are given.Comment: Talk given at ISMD 2009 conference 5 pages, 9 figure
About agreement of PYTHIA and the experimental results in annihilation to hadrons
The experimental charged particles multiplicity distributions in
annihilation to hadrons are compared with the distributions obtained by PYTHIA.
The ratio /degrees of freedom is calculated for 6 energies at
14 -- 206.2 GeV. The necessity of more subtle tuning of PYTHIA at
the energy of peak is discussed.Comment: 17 pages, 9 figure
Total cross section of neutron-proton scattering at low energies in quark-gluon model
We show that analysis of nonrelativistic neutron-proton scattering in a
framework of relativistic QCD based quark model can give important information
about QCD vacuum structure. In this model we describe total cross section of
neutron-proton scattering at kinetic energies of projectile neutron from 1 eV
up to 1 MeV.Comment: 8 pages, 4 figure
Possible difference between multiplicity distributions and inclusive spectra of secondary hadrons in proton-proton and proton-antiproton collisions at energy sqrt(s)=900 GeV
We consider QCD based model of hadrons interaction in which gluons density in
wave function of initial state is low in rapidity space and real hadrons are
produced by decay of color field strings. Hadrons production processes in pp
and p antip interactions differ on principle. There are three types of
inelastic processes in p antip collision. The first type is production of
secondary hadrons shower from decay of gluon string. The second type is shower
produced from decay of two quark strings and the third one -- from decay of
three quark strings. At the same time there are only two types of inelastic
processes for pp collision, they are shower from gluon string and shower from
two quark strings. Therefore multiplicity distributions and inclusive spectra
of secondary hadrons are different in pp and p antip interactions, and this
difference may be observed at energy sqrt(s)=900 GeV.Comment: 12 pages, 13 figure
KNO scaling in processes of electron-positron annihilation to hadrons
The charged particles multiplicity distribution in the KNO form is discussed
in processes of annihilation at energies 14 -- 206.2 GeV.
The experimental data are compared to data, obtained with Monte Carlo
simulation in PYTHIA in the Lund quark string model. It is shown, that both
experimental and simulated data are described by the same distribution function
in the KNO form. It is shown, that the KNO scaling is consequence of quark
string hadronization dynamics in the Lund string model.Comment: 11 pages, 5 figure
Color Diagrams for Non Vacuum Reggeons in Hadron-Hadron Interactions
One-to-one correspondence between dual diagrams of dual resonance model and
QCD based color diagrams describing non vacuum exchanges in pi+ pi-, pi+- p, p
anti p interactions is discussed. Both for dual and color diagrams there are
state with quark-antiquark in t channel and state, in which only coherent quark
string exists, in s channel. There are no such dual diagrams in pp interaction.
Color diagram for pp interaction was found basing on principle of conformity.
Secondary hadrons spectrum, obtained from this diagram, has nucleon in its
central region. This effect may lead to increase of baryon chemical potential
in nucleus-nucleus collisions in facilities NICA and FAIR.Comment: 9 pages, 13 figure
Inclusive cross sections of proton-proton and proton-antiproton scattering
We have predicted the difference in inclusive cross sections on
pseudorapidity in and interactions at ~GeV. Their ratio
in the whole pseudorapidity range.
On the basis of AGK theorem we show that the ratio of inclusive cross sections
of and at ~GeV in the region of low transverse
momenta up to 2~GeV . Experimental
measurements by the ATLAS Coll. give value for interval
.
The difference in inclusive cross sections results from presence of
additional subprocess in -- hadrons production from decay of three
quark strings, which is absent in scattering.Comment: Talk presented at the ISMD 2010, Antwerp (Belgium). Some typos are
correcte
Experimental evidences of difference in and interactions at high energies
Hadrons production is different in and interactions at high
energies. There is process of hadrons production from three quark strings in
which is absent in . This process grows as and
becomes significant when energy of collision increases. Inclusive cross
sections of interaction exceed inclusive cross sections of .
Theoretical estimation of the ratio of to at energy
GeV gives . The UA1 data on transverse
momentum distribution are about 1.2 -- 1.3 times higher than the CMS, ATLAS and
ALICE data on at energy GeV.Comment: 16 pages, 4 figures, preprint submitted to Physics Letters
Nucleus-Nucleus Collisions at Low Energies. The Effects from Non Vacuum Exchange
Experimental data on total and differential elastic cross sections for
, , , , starting from
energy 3.5 GeV in CMS are used to determine parameters of vacuum contribution
and parameters of basic non vacuum reggeons: , , and .
It is argued that non vacuum contributions to proton-proton and proton-neutron
collisions correspond to spectrum in which baryon number is moved from the
fragmentation region to central region in rapidity space. In this case it is
possible that chemical potential is increased in central region of spectrum of
nucleus-nucleus interaction at low energies. This effect might be important for
facilities FAIR and NICA
Multiplicity Distribution of Secondary Hadrons at LHC Energy and Total Cross Sections of Hadron-Hadron Interactions
The multiple production processes of secondary hadrons in proton-antiproton
scattering are divided into three types. The first type is a shower of
secondary hadrons produced from gluon string decay, the second type is a shower
of secondary hadrons produced from two quark strings decay and the third is a
shower produced from three quark strings decay. At the same time there are only
two types for proton-proton scattering - shower from gluon string and shower
from two quark strings. These showers do not correspond to pomeron showers
originating from cuts of one, two, three, ... pomerons. Multiplicity
distribution in gluon string is Gaussian, in two and three quark strings it is
negative binomial. Gluon string weight in the multiplicity distribution is
determined by the constant contribution to total cross sections, the quark
strings weights - by the growing with energy contributions. The expected value
of proton-proton scattering total cross section and the multiplicity
distribution at energy 14 TeV are givenComment: 17 pages, 26 figure
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