  Experiments are conducted in a two-dimensional mono-layer vibrofluidized bed
of glass beads, with a goal to understand the transition scenario and the
underlying microstructure and dynamics in different patterned-states. At small
shaking accelerations ($\Gamma=A\omega^2/g <1$), the particles remain attached
with the base of the vibrating container -- this is known as the solid bed
(SB). With increasing $\Gamma$ (at large enough shaking amplitude $A/d$) and/or
with increasing $A/d$ (at large enough $\Gamma$), the sequence of
transitions/bifurcations unfolds as follows: SB to BB ("bouncing bed") to LS
("Leidenfrost state") to "2-roll Convection" to "1-roll Convection" and finally
to a gas-like state. For a given length of the container, the coarsening of
multiple convection rolls leading to the genesis of a "single-roll" structure
(dubbed the {\it multi-roll transition}), and its subsequent transition to a
granular-gas are two novel findings of this work. We show that the critical
shaking intensity ($\Gamma_{BB}^{LS}$) for "$BB\to LS$"-transition has a
power-law dependence on the particle loading ($F=h_0/d$, where $h_0$ is the
number of particle layers at rest and $d$ is the particle diameter) and the
shaking amplitude ($A/d$). The characteristics of $BB$ and $LS$ states are
studied by calculating (i) the coarse-grained density and temperature profiles
and (ii) the pair correlation function. It is shown that while the contact
network of particles in the BB represents a hexagonal-packed structure, the
contact network within the LS resembles a liquid-like state. An unsteadiness of
the LS has been uncovered wherein the interface (between the floating-cluster
and the dilute gas underneath) and the top of the bed are found to oscillate
sinusoidally, with its oscillation frequency closely matching with the
frequency of external shaking.
