  It is shown that de-confinement can be achieved in high multiplicity non jet
$\bar{p}$p collisions at $\sqrt{s}$= 1.8 TeV Fermi National Accelerator
Laboratory(FNAL- E735) experiment. Previously the evidence for de-confinement
was the demonstrated by the constant freeze out energy density in high
multiplicity events. In this paper we use the same data but analyze the
transverse momentum spectrum in the framework of the clustering of color
sources. The charged particle pseudorapidities densities in the range 7.0 $\leq
\langle dN_{c}/d\eta \rangle \leq$26.0 are considered. Results are presented
for both thermodynamic and transport properties. The initial temperature and
energy density are obtained and compared with the Lattice Quantum Chromo
Dynamics(LQCD) simulations. The energy density ($\varepsilon/T^{4}$) $\sim$
11.5 for $ \langle dN_{c}/d\eta \rangle \sim $ 25.0 is close to the value for
0-10\% central events in Au+Au collisions at $\sqrt{s_{NN}}$= 200 GeV. The
shear viscosity to entropy density ratio($\eta/s$) is $\sim$ 0.2 at the
transition temperature. The result for the trace anomaly $\Delta$ is in
excellent agreement with LQCD simulations. These results confirm our earlier
observation that the de-confined state of matter was created in high
multiplicity events in $\bar{p}$p collisions at $\sqrt{s}$=1.8 TeV.
