|
| 1 | +import torch |
| 2 | +import torch_geometric as pyg |
| 3 | +import torch_geometric.utils as pyg_utils |
| 4 | +from ParticleGraph.utils import to_numpy |
| 5 | + |
| 6 | +class PDE_D_DualFieldCTC(pyg.nn.MessagePassing): |
| 7 | + """ |
| 8 | + Dual-field CTC: C2 modulates the CTC response strength based on C1. |
| 9 | +
|
| 10 | + Extends DampedCTC by adding a second morphogen channel to the CTC decision. |
| 11 | + Instead of sign_factor = -tanh(s*(C1-T)/A), uses: |
| 12 | + sign_factor = -tanh(s*(C1-T)/A) * (1 + beta * tanh(s2*(C2-T2)/A)) |
| 13 | +
|
| 14 | + When C2 is near its own threshold T2, the C1-based CTC response is amplified |
| 15 | + (or attenuated if beta < 0). This provides a second channel of positional |
| 16 | + information for particle sorting, inspired by morphogen gradient intersection |
| 17 | + in developmental biology. |
| 18 | +
|
| 19 | + The key difference from all prior CTC variants: the core tanh(C1-T) mechanism |
| 20 | + is PRESERVED (not replaced). C2 acts as a MODULATOR, not an alternative signal. |
| 21 | + This avoids the anti-convergence problem of deadzone, ratio, and gradient-based |
| 22 | + CTC modifications. |
| 23 | +
|
| 24 | + Physics: |
| 25 | + 1. fp: Durotaxis gradient-amplified mobility + dual-field CTC coupling |
| 26 | + v = M * (1 + alpha * |gradC1|) * (-tanh(s*(C1-T)/A)) * (1+beta*tanh(s2*(C2-T2)/A)) * grad * dir |
| 27 | + 2. pf: Standard consumption/production coupling |
| 28 | + 3. pp: Field-damped attraction-repulsion (same as DampedCTC) |
| 29 | +
|
| 30 | + Literature: |
| 31 | + - Wolpert, L. (1969) J Theor Biol 25:1-47 |
| 32 | + "Positional information and the spatial pattern of cellular differentiation" |
| 33 | + (Intersecting morphogen gradients for 2D positional specification) |
| 34 | + - Green, J.B.A. & Sharpe, J. (2015) Development 142:1203-1211 |
| 35 | + "Positional information and reaction-diffusion: two big ideas in developmental |
| 36 | + biology combine" (Multi-morphogen positional encoding) |
| 37 | + - Painter, K.J. & Hillen, T. (2002) CAMQ 10(4):501-543 |
| 38 | +
|
| 39 | + Per-type params layout: [M1, M2, consumption, production, ar_p1, ar_p2, ar_p3, ar_p4] |
| 40 | + """ |
| 41 | + |
| 42 | + PARAMS_DOC = { |
| 43 | + "model_name": "DualFieldCTC", |
| 44 | + "literature": "Wolpert (1969) J Theor Biol 25:1; Green & Sharpe (2015) Development 142:1203", |
| 45 | + "description": "Dual-field CTC: C2 modulates C1-based CTC response strength for 2D positional encoding", |
| 46 | + "equations": { |
| 47 | + "field_to_particle": "v = M * (1+alpha*|gradC1|) * (-tanh(s*(C1-T1)/A)) * (1+beta*tanh(s2*(C2-T2)/A)) * grad * dir", |
| 48 | + "particle_to_field": "dC1 = -consumption * w(r), dC2 = production * w(r)", |
| 49 | + "particle_to_particle": "f = f_AR * (1 - damping * exp(-(C1_i - T)^2 / (2*width^2)))" |
| 50 | + }, |
| 51 | + "params_mesh": [ |
| 52 | + { |
| 53 | + "row": 0, "description": "C1 field parameters + CTC threshold", |
| 54 | + "slots": [ |
| 55 | + {"index": 0, "name": "D1", "description": "Diffusion coeff for C1 (mesh model)", "typical_range": [0.01, 0.5]}, |
| 56 | + {"index": 1, "name": "Da_c", "description": "Damkohler number (mesh model)", "typical_range": [1.0, 50.0]}, |
| 57 | + {"index": 2, "name": "A", "description": "Brusselator param A (mesh model, also CTC reference)", "typical_range": [0.5, 5.0]}, |
| 58 | + {"index": 3, "name": "B", "description": "Brusselator param B (mesh model)", "typical_range": [1.0, 10.0]}, |
| 59 | + {"index": 4, "name": "mu", "description": "Morphological parameter (mesh model)", "typical_range": [0.01, 0.1]}, |
| 60 | + {"index": 5, "name": "M1", "description": "Mobility coefficient for C1 gradients", "typical_range": [-16, 16]}, |
| 61 | + {"index": 6, "name": "grad_amp_alpha", "description": "Durotaxis gradient amplification (0=off)", "typical_range": [0.0, 2.0]}, |
| 62 | + {"index": 7, "name": "ctc_threshold", "description": "CTC threshold for C1 (T1=ctc*A)", "typical_range": [0.5, 3.0]} |
| 63 | + ] |
| 64 | + }, |
| 65 | + { |
| 66 | + "row": 1, "description": "C2 field parameters + pp damping + C2 modulation", |
| 67 | + "slots": [ |
| 68 | + {"index": 0, "name": "D2", "description": "Diffusion coeff for C2 (mesh model)", "typical_range": [0.1, 1.0]}, |
| 69 | + {"index": 1, "name": "M2", "description": "Mobility coefficient for C2 gradients", "typical_range": [-16, 16]}, |
| 70 | + {"index": 2, "name": "pp_damping", "description": "pp damping strength at CTC threshold", "typical_range": [0.0, 0.95]}, |
| 71 | + {"index": 3, "name": "pp_damping_width", "description": "Width of Gaussian damping zone", "typical_range": [0.1, 1.0]}, |
| 72 | + {"index": 4, "name": "c2_beta", "description": "C2 modulation strength (0=off, >0 amplifies, <0 attenuates)", "typical_range": [-0.5, 0.5]}, |
| 73 | + {"index": 5, "name": "c2_threshold", "description": "C2 threshold factor (T2=c2_thresh*A for Brusselator equilibrium B/A)", "typical_range": [0.5, 3.0]}, |
| 74 | + {"index": 6, "name": "c2_steepness", "description": "Steepness of C2 modulation tanh", "typical_range": [1.0, 5.0]}, |
| 75 | + {"index": 7, "name": "unused", "description": "Pad", "typical_range": [0.0, 0.0]} |
| 76 | + ] |
| 77 | + }, |
| 78 | + { |
| 79 | + "row": 2, "description": "Particle-field coupling + per-type threshold spread", |
| 80 | + "slots": [ |
| 81 | + {"index": 0, "name": "Pe", "description": "Peclet number", "typical_range": [0.5, 2.0]}, |
| 82 | + {"index": 1, "name": "consumption", "description": "Particle consumption rate of C1", "typical_range": [10, 200]}, |
| 83 | + {"index": 2, "name": "production", "description": "Particle production rate of C2", "typical_range": [-200, -10]}, |
| 84 | + {"index": 3, "name": "influence_radius", "description": "Gaussian influence radius for pf coupling", "typical_range": [0.01, 0.1]}, |
| 85 | + {"index": 4, "name": "fp_drag", "description": "Velocity-dependent drag (0=off)", "typical_range": [0.0, 0.3]}, |
| 86 | + {"index": 5, "name": "cross_type_factor", "description": "Per-type CTC threshold spread", "typical_range": [0.0, 0.5]}, |
| 87 | + {"index": 6, "name": "unused2", "description": "Pad", "typical_range": [0.0, 0.0]}, |
| 88 | + {"index": 7, "name": "unused3", "description": "Pad", "typical_range": [0.0, 0.0]} |
| 89 | + ] |
| 90 | + } |
| 91 | + ], |
| 92 | + "width_constraint": "ALL rows of params_mesh MUST have same number of columns (8). Pad shorter rows.", |
| 93 | + "particle_params": { |
| 94 | + "description": "Per-type params from simulation.params (one row per n_particle_types)", |
| 95 | + "slots": [ |
| 96 | + {"index": 0, "name": "M1", "description": "Per-type mobility for C1"}, |
| 97 | + {"index": 1, "name": "M2", "description": "Per-type mobility for C2"}, |
| 98 | + {"index": 2, "name": "consumption", "description": "Per-type consumption rate"}, |
| 99 | + {"index": 3, "name": "production", "description": "Per-type production rate"}, |
| 100 | + {"index": 4, "name": "ar_p1", "description": "Attraction strength"}, |
| 101 | + {"index": 5, "name": "ar_p2", "description": "Attraction exponent"}, |
| 102 | + {"index": 6, "name": "ar_p3", "description": "Repulsion strength"}, |
| 103 | + {"index": 7, "name": "ar_p4", "description": "Repulsion exponent"} |
| 104 | + ] |
| 105 | + } |
| 106 | + } |
| 107 | + |
| 108 | + def __init__(self, aggr_type='mean', p=None, particle_params=None, bc_dpos=None, dimension=2, sigma=0.005): |
| 109 | + super(PDE_D_DualFieldCTC, self).__init__(aggr=aggr_type) |
| 110 | + |
| 111 | + self.p = p |
| 112 | + self.particle_params = particle_params |
| 113 | + self.bc_dpos = bc_dpos |
| 114 | + self.dimension = dimension |
| 115 | + self.sigma = sigma |
| 116 | + |
| 117 | + self.M1 = p[0, 5] |
| 118 | + self.M2 = p[1, 1] |
| 119 | + self.consumption_rate = p[2, 1] |
| 120 | + self.production_rate = p[2, 2] |
| 121 | + self.influence_radius = p[2, 3] |
| 122 | + self.Pe = p[2, 0] |
| 123 | + self.repulsion_strength = 50 |
| 124 | + self.repulsion_range = 0.04 |
| 125 | + |
| 126 | + # Durotaxis gradient amplification |
| 127 | + self.grad_amp_alpha = p[0, 6] if p.shape[1] > 6 else 0.0 |
| 128 | + |
| 129 | + # CTC threshold for C1 |
| 130 | + self.ctc_threshold = p[0, 7] if p.shape[1] > 7 else 0.0 |
| 131 | + self.A_ref = p[0, 2] |
| 132 | + |
| 133 | + # Per-type threshold spread |
| 134 | + self.cross_type_factor = p[2, 5] if p.shape[1] > 5 else 0.0 |
| 135 | + |
| 136 | + # pp damping parameters (Painter & Hillen 2002) |
| 137 | + self.pp_damping = p[1, 2] if p.shape[1] > 2 else 0.0 |
| 138 | + self.pp_damping_width = p[1, 3] if p.shape[1] > 3 else 0.5 |
| 139 | + |
| 140 | + # C2 modulation parameters (Wolpert 1969; Green & Sharpe 2015) |
| 141 | + self.c2_beta = p[1, 4] if p.shape[1] > 4 else 0.0 |
| 142 | + self.c2_threshold = p[1, 5] if p.shape[1] > 5 else 1.0 |
| 143 | + self.c2_steepness = p[1, 6] if p.shape[1] > 6 else 3.0 |
| 144 | + |
| 145 | + # fp drag |
| 146 | + self.fp_drag = p[2, 4] if p.shape[1] > 4 else 0.0 |
| 147 | + |
| 148 | + print(f"initialized PDE_D_DualFieldCTC with parameters:") |
| 149 | + print(f" mobility: M1={self.M1.item()}, M2={self.M2.item()}") |
| 150 | + ga_val = self.grad_amp_alpha.item() if hasattr(self.grad_amp_alpha, 'item') else self.grad_amp_alpha |
| 151 | + print(f" grad_amp_alpha={ga_val:.3f} (durotaxis, Lo 2000)") |
| 152 | + ctc_val = self.ctc_threshold.item() if hasattr(self.ctc_threshold, 'item') else self.ctc_threshold |
| 153 | + T_val = ctc_val * self.A_ref.item() |
| 154 | + print(f" ctc_threshold={ctc_val:.3f} (T1={T_val:.2f}, Wolpert 1969)") |
| 155 | + c2b = self.c2_beta.item() if hasattr(self.c2_beta, 'item') else self.c2_beta |
| 156 | + c2t = self.c2_threshold.item() if hasattr(self.c2_threshold, 'item') else self.c2_threshold |
| 157 | + c2s = self.c2_steepness.item() if hasattr(self.c2_steepness, 'item') else self.c2_steepness |
| 158 | + T2_val = c2t * self.A_ref.item() |
| 159 | + print(f" C2 modulation: beta={c2b:.3f}, T2={T2_val:.2f} (c2_thresh={c2t:.2f}), steepness={c2s:.1f} (Green & Sharpe 2015)") |
| 160 | + damp_val = self.pp_damping.item() if hasattr(self.pp_damping, 'item') else self.pp_damping |
| 161 | + damp_w = self.pp_damping_width.item() if hasattr(self.pp_damping_width, 'item') else self.pp_damping_width |
| 162 | + print(f" pp_damping={damp_val:.3f}, pp_damping_width={damp_w:.3f}") |
| 163 | + fp_d = self.fp_drag.item() if hasattr(self.fp_drag, 'item') else self.fp_drag |
| 164 | + print(f" fp_drag={fp_d:.3f}") |
| 165 | + ctf_val = self.cross_type_factor.item() if hasattr(self.cross_type_factor, 'item') else self.cross_type_factor |
| 166 | + if ctf_val > 0 and particle_params is not None: |
| 167 | + n_types = particle_params.shape[0] |
| 168 | + mean_idx = (n_types - 1) / 2.0 |
| 169 | + for t in range(n_types): |
| 170 | + t_offset = ctf_val * (t - mean_idx) |
| 171 | + t_val = T_val * (1.0 + t_offset) |
| 172 | + print(f" Type {t}: CTC threshold = {t_val:.2f} (offset={t_offset:+.2f})") |
| 173 | + print(f" Pe={self.Pe.item():.3f}, sigma={self.sigma}") |
| 174 | + print(f" particle->field: consumption={self.consumption_rate.item()}, production={self.production_rate.item()}, influence_radius={self.influence_radius.item():.3f}") |
| 175 | + if particle_params is not None: |
| 176 | + print(f" multi-type support: {particle_params.shape[0]} particle types") |
| 177 | + |
| 178 | + def forward(self, data, direction='fp'): |
| 179 | + x, edge_index = data.x, data.edge_index |
| 180 | + edge_index, _ = pyg_utils.remove_self_loops(edge_index) |
| 181 | + |
| 182 | + if self.particle_params is not None: |
| 183 | + particle_type = x[:, 1 + 2*self.dimension].long() |
| 184 | + max_type = particle_type.max().item() |
| 185 | + n_param_rows = self.particle_params.shape[0] |
| 186 | + if max_type >= n_param_rows: |
| 187 | + raise ValueError( |
| 188 | + f"PDE_D_DualFieldCTC: particle_params has {n_param_rows} rows but found " |
| 189 | + f"particle type {max_type}. Need {max_type + 1} rows in simulation.params." |
| 190 | + ) |
| 191 | + parameters = self.particle_params[to_numpy(particle_type), :] |
| 192 | + else: |
| 193 | + parameters = None |
| 194 | + |
| 195 | + if direction == 'interpolate': |
| 196 | + result = self.propagate(edge_index, x=x, mode='interpolate', parameters=parameters) |
| 197 | + pos = x[:, 1:self.dimension+1] |
| 198 | + in_box = ((pos >= 0) & (pos <= 1)).all(dim=1, keepdim=True) |
| 199 | + result = result * in_box.float() |
| 200 | + return result |
| 201 | + elif direction == 'fp': |
| 202 | + result = self.propagate(edge_index, x=x, mode='fp', parameters=parameters) |
| 203 | + pos = x[:, 1:self.dimension+1] |
| 204 | + in_box = ((pos >= 0) & (pos <= 1)).all(dim=1, keepdim=True) |
| 205 | + result = result * in_box.float() |
| 206 | + return result |
| 207 | + elif direction == 'pf': |
| 208 | + result = self.propagate(edge_index, x=x, mode='pf', parameters=parameters) |
| 209 | + return result |
| 210 | + else: |
| 211 | + result = self.propagate(edge_index, x=x, mode='pp', parameters=parameters) |
| 212 | + return result |
| 213 | + |
| 214 | + def message(self, edge_index_i, edge_index_j, x_i, x_j, mode=None, parameters_i=None): |
| 215 | + pos_i = x_i[:, 1:self.dimension+1] |
| 216 | + pos_j = x_j[:, 1:self.dimension+1] |
| 217 | + |
| 218 | + d_pos = self.bc_dpos(pos_j - pos_i) |
| 219 | + dist = torch.sqrt(torch.sum(d_pos**2, dim=1)) |
| 220 | + dist_safe = torch.clamp(dist, min=1e-6) |
| 221 | + |
| 222 | + if mode == 'interpolate': |
| 223 | + C1_mesh = x_j[:, 6:7] |
| 224 | + C2_mesh = x_j[:, 7:8] |
| 225 | + weight = torch.exp(-dist / 0.01).unsqueeze(1) |
| 226 | + return torch.cat([C1_mesh * weight, C2_mesh * weight, weight], dim=1) |
| 227 | + |
| 228 | + elif mode == 'fp': |
| 229 | + fields_i = x_i[:, 6:8] |
| 230 | + fields_j = x_j[:, 6:8] |
| 231 | + |
| 232 | + dC1 = fields_j[:, 0:1] - fields_i[:, 0:1] |
| 233 | + dC2 = fields_j[:, 1:2] - fields_i[:, 1:2] |
| 234 | + |
| 235 | + kernel = torch.exp(-dist / 0.05) |
| 236 | + dir_norm = d_pos / dist_safe.unsqueeze(1) |
| 237 | + domain_scale = 32.0 |
| 238 | + grad_C1 = (dC1 * kernel.unsqueeze(1)) / (dist_safe.unsqueeze(1) * domain_scale) |
| 239 | + grad_C2 = (dC2 * kernel.unsqueeze(1)) / (dist_safe.unsqueeze(1) * domain_scale) |
| 240 | + |
| 241 | + if parameters_i is not None: |
| 242 | + M1 = parameters_i[:, 0:1] |
| 243 | + M2 = parameters_i[:, 1:2] |
| 244 | + else: |
| 245 | + M1 = self.M1 |
| 246 | + M2 = self.M2 |
| 247 | + |
| 248 | + velocity_raw = (M1 * grad_C1 + M2 * grad_C2) * dir_norm |
| 249 | + |
| 250 | + # 1. Durotaxis: amplify velocity at steep gradients (Lo et al. 2000) |
| 251 | + if self.grad_amp_alpha > 0: |
| 252 | + grad_mag = torch.abs(grad_C1) |
| 253 | + grad_mag_clamped = torch.clamp(grad_mag, max=1.0) |
| 254 | + amp_factor = 1.0 + self.grad_amp_alpha * grad_mag_clamped |
| 255 | + velocity_raw = velocity_raw * amp_factor |
| 256 | + |
| 257 | + # 2. Concentration-threshold coupling on C1 (Wolpert 1969) |
| 258 | + if self.ctc_threshold > 0: |
| 259 | + C1_local = fields_i[:, 0:1] |
| 260 | + C2_local = fields_i[:, 1:2] |
| 261 | + A_ref = self.A_ref |
| 262 | + base_T = self.ctc_threshold * A_ref |
| 263 | + steepness = 3.0 |
| 264 | + |
| 265 | + # Per-type thresholds when multi-type + cross_type_factor > 0 |
| 266 | + if (parameters_i is not None and self.cross_type_factor > 0 |
| 267 | + and x_i.numel() > 0): |
| 268 | + type_i = x_i[:, 1 + 2*self.dimension].long() |
| 269 | + n_types = type_i.max().item() + 1 if type_i.numel() > 0 else 1 |
| 270 | + mean_idx = (n_types - 1) / 2.0 |
| 271 | + type_offset = self.cross_type_factor * (type_i.float() - mean_idx) |
| 272 | + T = base_T * (1.0 + type_offset.unsqueeze(1)) |
| 273 | + else: |
| 274 | + T = base_T |
| 275 | + |
| 276 | + # Core CTC on C1 — PRESERVED exactly as DampedCTC |
| 277 | + sign_factor = -torch.tanh(steepness * (C1_local - T) / (A_ref + 1e-6)) |
| 278 | + |
| 279 | + # 3. C2 modulation (Green & Sharpe 2015) |
| 280 | + # C2 provides a second channel of positional information |
| 281 | + # When beta > 0: C2 near T2 amplifies CTC response |
| 282 | + # When beta < 0: C2 near T2 attenuates CTC response |
| 283 | + c2_beta_val = self.c2_beta |
| 284 | + if hasattr(c2_beta_val, 'item'): |
| 285 | + c2_beta_check = c2_beta_val.item() |
| 286 | + else: |
| 287 | + c2_beta_check = float(c2_beta_val) |
| 288 | + |
| 289 | + if abs(c2_beta_check) > 1e-6: |
| 290 | + T2 = self.c2_threshold * A_ref |
| 291 | + c2_steep = self.c2_steepness |
| 292 | + if hasattr(c2_steep, 'item'): |
| 293 | + c2_steep = c2_steep |
| 294 | + c2_mod = 1.0 + c2_beta_val * torch.tanh(c2_steep * (C2_local - T2) / (A_ref + 1e-6)) |
| 295 | + sign_factor = sign_factor * c2_mod |
| 296 | + |
| 297 | + velocity_raw = velocity_raw * sign_factor |
| 298 | + |
| 299 | + # 4. Velocity-dependent drag (Tranquillo 1987) |
| 300 | + fp_drag_val = self.fp_drag |
| 301 | + if hasattr(fp_drag_val, 'item'): |
| 302 | + fp_drag_check = fp_drag_val.item() |
| 303 | + else: |
| 304 | + fp_drag_check = float(fp_drag_val) |
| 305 | + |
| 306 | + if fp_drag_check > 0: |
| 307 | + vel_i = x_i[:, self.dimension+1:2*self.dimension+1] |
| 308 | + speed = torch.sqrt(torch.sum(vel_i**2, dim=1, keepdim=True) + 1e-10) |
| 309 | + drag = 1.0 / (1.0 + fp_drag_check * speed) |
| 310 | + velocity_raw = velocity_raw * drag |
| 311 | + |
| 312 | + return velocity_raw |
| 313 | + |
| 314 | + elif mode == 'pf': |
| 315 | + weights = torch.exp(-dist**2 / (2 * (self.influence_radius/3)**2)) |
| 316 | + |
| 317 | + if parameters_i is not None: |
| 318 | + consumption = parameters_i[:, 2] |
| 319 | + production = parameters_i[:, 3] |
| 320 | + else: |
| 321 | + consumption = self.consumption_rate |
| 322 | + production = self.production_rate |
| 323 | + |
| 324 | + field_updates = torch.zeros((pos_i.size(0), 2), device=pos_i.device) |
| 325 | + field_updates[:, 0] = -consumption * weights |
| 326 | + field_updates[:, 1] = production * weights |
| 327 | + return field_updates |
| 328 | + |
| 329 | + else: # mode == 'pp' |
| 330 | + if parameters_i is not None: |
| 331 | + p1 = parameters_i[:, 4] |
| 332 | + p2 = parameters_i[:, 5] |
| 333 | + p3 = parameters_i[:, 6] |
| 334 | + p4 = parameters_i[:, 7] |
| 335 | + |
| 336 | + f = (p1 * torch.exp(-dist ** (2 * p2) / (2 * self.sigma ** 2)) |
| 337 | + - p3 * torch.exp(-dist ** (2 * p4) / (2 * self.sigma ** 2))) |
| 338 | + |
| 339 | + forces = f[:, None] * d_pos / dist_safe.unsqueeze(1) |
| 340 | + else: |
| 341 | + forces = torch.zeros_like(pos_i) |
| 342 | + in_range = dist < self.repulsion_range |
| 343 | + if in_range.any(): |
| 344 | + dir_norm = d_pos / dist_safe.unsqueeze(1) |
| 345 | + repulsion_mag = self.repulsion_strength * torch.exp( |
| 346 | + -5.0 * dist[in_range] / self.repulsion_range |
| 347 | + ) |
| 348 | + forces[in_range] = -dir_norm[in_range] * repulsion_mag.unsqueeze(1) |
| 349 | + |
| 350 | + # Field-dependent pp damping (Painter & Hillen 2002) |
| 351 | + if self.pp_damping > 0 and self.ctc_threshold > 0: |
| 352 | + C1_local = x_i[:, 6:7].squeeze(1) |
| 353 | + A_ref = self.A_ref |
| 354 | + base_T = self.ctc_threshold * A_ref |
| 355 | + |
| 356 | + if (parameters_i is not None and self.cross_type_factor > 0 |
| 357 | + and x_i.numel() > 0): |
| 358 | + type_i = x_i[:, 1 + 2*self.dimension].long() |
| 359 | + n_types = type_i.max().item() + 1 if type_i.numel() > 0 else 1 |
| 360 | + mean_idx = (n_types - 1) / 2.0 |
| 361 | + type_offset = self.cross_type_factor * (type_i.float() - mean_idx) |
| 362 | + T_local = base_T * (1.0 + type_offset) |
| 363 | + else: |
| 364 | + T_local = base_T |
| 365 | + |
| 366 | + width = self.pp_damping_width * A_ref |
| 367 | + deviation = (C1_local - T_local) |
| 368 | + damping_factor = 1.0 - self.pp_damping * torch.exp(-deviation**2 / (2 * width**2 + 1e-8)) |
| 369 | + forces = forces * damping_factor.unsqueeze(1) |
| 370 | + |
| 371 | + return forces |
| 372 | + |
| 373 | + def update(self, aggr_out, mode=None): |
| 374 | + if mode == 'interpolate': |
| 375 | + C1_weighted = aggr_out[:, 0:1] |
| 376 | + C2_weighted = aggr_out[:, 1:2] |
| 377 | + weight_sum = aggr_out[:, 2:3] |
| 378 | + weight_sum = torch.clamp(weight_sum, min=1e-10) |
| 379 | + return torch.cat([C1_weighted / weight_sum, C2_weighted / weight_sum], dim=1) |
| 380 | + else: |
| 381 | + return aggr_out |
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