Free fermions in d dimensions have a hole probability that scales as exp[-(k_F R)^{d+1} Φ_d(u)] with a transition of order 3/2(d+1) in Φ_d at the universal point u_c=2/π, computed exactly via Coulomb gas mapping.
T^ d/2 A_d(t)= V_d (p( =- ,T)-p( ,T)) where p( ,T) is the pressure of the Fermi gas, see Eq
1 Pith paper cite this work. Polarity classification is still indexing.
1
Pith paper citing it
fields
cond-mat.stat-mech 1years
2026 1verdicts
CONDITIONAL 1representative citing papers
citing papers explorer
-
A transition in the hole probability at finite temperature for free fermions in $d$ dimensions
Free fermions in d dimensions have a hole probability that scales as exp[-(k_F R)^{d+1} Φ_d(u)] with a transition of order 3/2(d+1) in Φ_d at the universal point u_c=2/π, computed exactly via Coulomb gas mapping.