The quantum tricriticality of d-dimensional transverse Ising-like systems is
studied by means of a perturbative renormalization group approach focusing on
static susceptibility. This allows us to obtain the phase diagram for 3<d<4,
with a clear location of the critical lines ending in the conventional quantum
critical points and in the quantum tricritical one, and of the tricritical line
for temperature T \geq 0. We determine also the critical and the tricritical
shift exponents close to the corresponding ground state instabilities.
Remarkably, we find a tricritical shift exponent identical to that found in the
conventional quantum criticality and, by approaching the quantum tricritical
point increasing the non-thermal control parameter r, a crossover of the
quantum critical shift exponents from the conventional value \phi = 1/(d-1) to
the new one \phi = 1/2(d-1). Besides, the projection in the (r,T)-plane of the
phase boundary ending in the quantum tricritical point and crossovers in the
quantum tricritical region appear quite similar to those found close to an
usual quantum critical point. Another feature of experimental interest is that
the amplitude of the Wilsonian classical critical region around this peculiar
critical line is sensibly smaller than that expected in the quantum critical
scenario. This suggests that the quantum tricriticality is essentially governed
by mean-field critical exponents, renormalized by the shift exponent \phi =
1/2(d-1) in the quantum tricritical region.Comment: 9 pages, 2 figures; to be published on EPJ