# Kira integral family for the dissipative crossed family PX2 (pm5_2SF_PX2_diss): four loop momenta,
# 22 propagators in the order D_1..D_22 of Eq. (6) of the paper, the first four cut (delta(2 k_i.u)).
# Source of the propagator list: arXiv:2601.16256, supplemental material, Eqs. (16)-(20) (PX2 = {D1,D3,D4,D6} there).
# Linearized worldline propagators use Kira's general-propagator syntax.  No i0 assignment is part of
# the family definition.  This is the configuration used for the first-stage reduction of Table 2
# (non-comment lines identical to the run configuration; see README.md).
integralfamilies:
  - name: "pm5_2SF_PX2_diss"
    loop_momenta: [k1, k2, k3, k4]
    top_level_sectors: [340479, 1077759, 599551, 1091071]
    propagators:
      - [ "2*k1*u1", 0 ]
      - [ "2*k2*u1", 0 ]
      - [ "2*k3*u2", 0 ]
      - [ "2*k4*u2", 0 ]
      - [ "2*k1*u2", 0 ]
      - [ "2*k1*u2-2*k2*u2", 0 ]
      - [ "2*k3*u1", 0 ]
      - [ "2*k3*u1-2*k4*u1", 0 ]
      - [ "k1-k2", 0 ]
      - [ "k1-k3", 0 ]
      - [ "k1-k4", 0 ]
      - [ "k2-k3", 0 ]
      - [ "k2-k4", 0 ]
      - [ "k3-k4", 0 ]
      - [ "k1+q", 0 ]
      - [ "k2+q", 0 ]
      - [ "k3+q", 0 ]
      - [ "k4+q", 0 ]
      - [ "k1", 0 ]
      - [ "k2", 0 ]
      - [ "k3", 0 ]
      - [ "k4", 0 ]
    cut_propagators: [1, 2, 3, 4]