|
| 1 | +{ |
| 2 | + "cells": [ |
| 3 | + { |
| 4 | + "cell_type": "code", |
| 5 | + "execution_count": null, |
| 6 | + "metadata": {}, |
| 7 | + "outputs": [], |
| 8 | + "source": [ |
| 9 | + "!pip install numpy==1.26.4 matplotlib==3.9.2 mpmath==1.3.0 scipy==1.14.1 plotly==5.24.1 sympy==1.13.3" |
| 10 | + ] |
| 11 | + }, |
| 12 | + { |
| 13 | + "cell_type": "code", |
| 14 | + "execution_count": null, |
| 15 | + "metadata": {}, |
| 16 | + "outputs": [], |
| 17 | + "source": [ |
| 18 | + "import numpy as np\n", |
| 19 | + "import plotly.graph_objects as go\n", |
| 20 | + "from mpmath import mp, chi\n", |
| 21 | + "from sympy import zeta as sympy_zeta\n", |
| 22 | + "from functools import lru_cache\n", |
| 23 | + "from scipy.interpolate import interp1d\n", |
| 24 | + "\n", |
| 25 | + "# Настройки mpmath\n", |
| 26 | + "mp.dps = 30\n", |
| 27 | + "\n", |
| 28 | + "# Параметры\n", |
| 29 | + "T = 50\n", |
| 30 | + "t = np.linspace(-T, T, 300)\n", |
| 31 | + "gamma_n = [14.1347, 21.0220, 25.0108]\n", |
| 32 | + "k = 1.0\n", |
| 33 | + "epsilon = 1e-8\n", |
| 34 | + "omega = 1e12\n", |
| 35 | + "hbar = 6.582e-16\n", |
| 36 | + "dt_avg = 2 * T / len(t)\n", |
| 37 | + "\n", |
| 38 | + "# Кэширование zeta и chi\n", |
| 39 | + "@lru_cache(maxsize=1000)\n", |
| 40 | + "def cached_zeta(s_real, s_imag):\n", |
| 41 | + " try:\n", |
| 42 | + " return complex(sympy_zeta(complex(s_real, s_imag)))\n", |
| 43 | + " except:\n", |
| 44 | + " return 0.0\n", |
| 45 | + "\n", |
| 46 | + "@lru_cache(maxsize=1000)\n", |
| 47 | + "def cached_chi(s_real, s_imag):\n", |
| 48 | + " try:\n", |
| 49 | + " return complex(chi(complex(s_real, s_imag)))\n", |
| 50 | + " except:\n", |
| 51 | + " return 0.0\n", |
| 52 | + "\n", |
| 53 | + "# Модуль |zeta(1/2 + it)|^2\n", |
| 54 | + "def zeta_squared(u):\n", |
| 55 | + " z = cached_zeta(0.5, u)\n", |
| 56 | + " result = z * z.conjugate()\n", |
| 57 | + " return float(result.real) if not np.isnan(result) and not np.isinf(result) else 0.0\n", |
| 58 | + "\n", |
| 59 | + "# Функция psi\n", |
| 60 | + "def psi(s, u, epsilon):\n", |
| 61 | + " denom = (s - 0.5 - 1j*u)**2 * (1 - s - 0.5 - 1j*u)**2 + epsilon**2\n", |
| 62 | + " result = 1 / denom\n", |
| 63 | + " zeta_s = cached_zeta(s.real, s.imag)\n", |
| 64 | + " chi_s = cached_chi(s.real, s.imag)\n", |
| 65 | + " chi_zeta = abs(chi_s * zeta_s)**2\n", |
| 66 | + " if chi_zeta > 1e10:\n", |
| 67 | + " chi_zeta = 1e10\n", |
| 68 | + " result *= chi_zeta\n", |
| 69 | + " return result if not np.isnan(result) and not np.isinf(result) else 0.0\n", |
| 70 | + "\n", |
| 71 | + "# Вычисление ядра K_sym\n", |
| 72 | + "def compute_kernel(epsilon):\n", |
| 73 | + " N = len(t)\n", |
| 74 | + " K = np.zeros((N, N), dtype=complex)\n", |
| 75 | + " for i in range(N):\n", |
| 76 | + " for j in range(N):\n", |
| 77 | + " s = 0.5 + 1j * t[i]\n", |
| 78 | + " u = t[j]\n", |
| 79 | + " psi_val = psi(s, u, epsilon)\n", |
| 80 | + " zeta_val = zeta_squared(u)\n", |
| 81 | + " K[i, j] = psi_val * zeta_val\n", |
| 82 | + " K = (K + K.conj().T) / 2\n", |
| 83 | + " return K\n", |
| 84 | + "\n", |
| 85 | + "# Потенциал\n", |
| 86 | + "V_eff = -k * np.array([zeta_squared(ti) for ti in t])\n", |
| 87 | + "\n", |
| 88 | + "# Вычисление собственных функций\n", |
| 89 | + "K_sym = compute_kernel(epsilon) * dt_avg\n", |
| 90 | + "eigvals, eigvecs = np.linalg.eigh(K_sym)\n", |
| 91 | + "idx = np.argsort(eigvals)[::-1]\n", |
| 92 | + "eigvals = eigvals[idx]\n", |
| 93 | + "eigvecs = eigvecs[:, idx]\n", |
| 94 | + "\n", |
| 95 | + "# Выбор трёх собственных функций\n", |
| 96 | + "selected_indices = [np.argmin(np.abs(eigvals - gamma)) for gamma in gamma_n]\n", |
| 97 | + "fn_data = [np.abs(eigvecs[:, idx])**2 for idx in selected_indices]\n", |
| 98 | + "\n", |
| 99 | + "# Интерполяция\n", |
| 100 | + "fn_interps = [interp1d(t, fn, kind='cubic') for fn in fn_data]\n", |
| 101 | + "\n", |
| 102 | + "# Плотности вероятности с фазой\n", |
| 103 | + "psi_data = []\n", |
| 104 | + "for i, gamma in enumerate(gamma_n):\n", |
| 105 | + " frames = []\n", |
| 106 | + " for time in np.linspace(0, 1e-12, 20):\n", |
| 107 | + " phase = omega * gamma * time\n", |
| 108 | + " psi = fn_interps[i](t) * np.exp(1j * phase)\n", |
| 109 | + " psi_squared = np.abs(psi)**2\n", |
| 110 | + " frames.append(psi_squared)\n", |
| 111 | + " psi_data.append(frames)\n", |
| 112 | + "\n", |
| 113 | + "# Описание в виде цитаты\n", |
| 114 | + "print(\"\"\"\n", |
| 115 | + "> * Любо́н (Lub): Описание и цвета графика *\n", |
| 116 | + "> ----------------------------------------\n", |
| 117 | + "> @ Тип: Скалярный бозон (спин-0)\n", |
| 118 | + "> # Масса: ~10^-3 эВ/c^2 (легче нейтрино)\n", |
| 119 | + "> ~ Энергия: E_n = ℏωγ_n, где γ_n — нули ζ(1/2 + iγ_n)\n", |
| 120 | + "> & Природа: Резонанс квантовой системы с хаотической динамикой\n", |
| 121 | + "> = Связь: Дзета-функция Римана ζ(s)\n", |
| 122 | + "> ? Где искать: Квантовые точки, фотонные кристаллы, космос\n", |
| 123 | + "> % Тёмная материя?: Возможный кандидат\n", |
| 124 | + "> $ Статистика: GUE (хаотический спектр)\n", |
| 125 | + "> ! Значение: Мост между математикой и физикой\n", |
| 126 | + ">\n", |
| 127 | + "> + Цвета линий на графике:\n", |
| 128 | + "> - # Синий: |lub_1(t)|^2 (γ_1 = 14.1347)\n", |
| 129 | + "> - # Зелёный: |lub_2(t)|^2 (γ_2 = 21.0220)\n", |
| 130 | + "> - # Фиолетовый: |lub_3(t)|^2 (γ_3 = 25.0108)\n", |
| 131 | + "> - # Красный (пунктир): Потенциал V_eff(t) = -|ζ(1/2 + it)|^2\n", |
| 132 | + "> - # Полупрозрачная красная поверхность: Потенциал V_eff(t)\n", |
| 133 | + "> ----------------------------------------\n", |
| 134 | + "\"\"\")\n", |
| 135 | + "\n", |
| 136 | + "# Создание графика\n", |
| 137 | + "fig = go.Figure()\n", |
| 138 | + "\n", |
| 139 | + "# Волновые функции\n", |
| 140 | + "colors = ['blue', 'green', 'purple']\n", |
| 141 | + "for i, gamma in enumerate(gamma_n):\n", |
| 142 | + " fig.add_trace(go.Scatter3d(\n", |
| 143 | + " x=t,\n", |
| 144 | + " y=psi_data[i][0],\n", |
| 145 | + " z=V_eff,\n", |
| 146 | + " mode='lines',\n", |
| 147 | + " line=dict(width=5, color=colors[i]),\n", |
| 148 | + " name=f'|lub_{i+1}(t)|^2 (γ_{i+1} = {gamma})',\n", |
| 149 | + " visible=(i == 0)\n", |
| 150 | + " ))\n", |
| 151 | + "\n", |
| 152 | + "# Потенциал\n", |
| 153 | + "fig.add_trace(go.Scatter3d(\n", |
| 154 | + " x=t,\n", |
| 155 | + " y=np.zeros_like(t),\n", |
| 156 | + " z=V_eff,\n", |
| 157 | + " mode='lines',\n", |
| 158 | + " line=dict(width=4, color='red', dash='dash'),\n", |
| 159 | + " name='V_eff(t)'\n", |
| 160 | + "))\n", |
| 161 | + "\n", |
| 162 | + "# Поверхностный график\n", |
| 163 | + "X, Y = np.meshgrid(t, np.linspace(0, max(psi_data[0][0]) * 1.1, 20))\n", |
| 164 | + "Z = np.tile(V_eff, (20, 1))\n", |
| 165 | + "fig.add_trace(go.Surface(\n", |
| 166 | + " x=X,\n", |
| 167 | + " y=Y,\n", |
| 168 | + " z=Z,\n", |
| 169 | + " opacity=0.3,\n", |
| 170 | + " colorscale='Reds',\n", |
| 171 | + " showscale=False,\n", |
| 172 | + " name='Потенциал (поверхность)'\n", |
| 173 | + "))\n", |
| 174 | + "\n", |
| 175 | + "# Аннотации\n", |
| 176 | + "for gamma in gamma_n:\n", |
| 177 | + " fig.add_trace(go.Scatter3d(\n", |
| 178 | + " x=[gamma],\n", |
| 179 | + " y=[max(psi_data[0][0]) * 0.5],\n", |
| 180 | + " z=[min(V_eff)],\n", |
| 181 | + " mode='text',\n", |
| 182 | + " text=[f'γ_{gamma}'],\n", |
| 183 | + " textposition='top center',\n", |
| 184 | + " showlegend=False\n", |
| 185 | + " ))\n", |
| 186 | + "\n", |
| 187 | + "# Анимация\n", |
| 188 | + "frames = []\n", |
| 189 | + "for f in range(20):\n", |
| 190 | + " frame_data = []\n", |
| 191 | + " for i, gamma in enumerate(gamma_n):\n", |
| 192 | + " frame_data.append(go.Scatter3d(\n", |
| 193 | + " x=t,\n", |
| 194 | + " y=psi_data[i][f],\n", |
| 195 | + " z=V_eff,\n", |
| 196 | + " mode='lines',\n", |
| 197 | + " line=dict(width=5, color=colors[i]),\n", |
| 198 | + " name=f'|lub_{i+1}(t)|^2',\n", |
| 199 | + " visible=(i == 0)\n", |
| 200 | + " ))\n", |
| 201 | + " frame_data.append(fig.data[len(gamma_n)])\n", |
| 202 | + " frame_data.append(fig.data[len(gamma_n) + 1])\n", |
| 203 | + " for j in range(len(gamma_n)):\n", |
| 204 | + " frame_data.append(fig.data[len(gamma_n) + 2 + j])\n", |
| 205 | + " frames.append(go.Frame(data=frame_data, name=f'frame{f}'))\n", |
| 206 | + "\n", |
| 207 | + "fig.frames = frames\n", |
| 208 | + "\n", |
| 209 | + "# Слайдеры\n", |
| 210 | + "sliders = [\n", |
| 211 | + " dict(\n", |
| 212 | + " steps=[\n", |
| 213 | + " dict(\n", |
| 214 | + " method='update',\n", |
| 215 | + " args=[{'visible': [k == i for k in range(len(gamma_n))] + [True, True] + [True]*len(gamma_n)},\n", |
| 216 | + " {'title': f'Любо́н: |lub_{i+1}(t)|^2 (γ_{i+1} = {gamma_n[i]})'}],\n", |
| 217 | + " label=f'γ_{i+1}'\n", |
| 218 | + " ) for i in range(len(gamma_n))\n", |
| 219 | + " ],\n", |
| 220 | + " active=0,\n", |
| 221 | + " currentvalue={'prefix': 'Выбор нуля: '},\n", |
| 222 | + " pad={'t': 50}\n", |
| 223 | + " )\n", |
| 224 | + "]\n", |
| 225 | + "\n", |
| 226 | + "# Кнопки анимации\n", |
| 227 | + "fig.update_layout(\n", |
| 228 | + " updatemenus=[\n", |
| 229 | + " dict(\n", |
| 230 | + " type='buttons',\n", |
| 231 | + " showactive=True,\n", |
| 232 | + " buttons=[\n", |
| 233 | + " dict(\n", |
| 234 | + " label='Играть',\n", |
| 235 | + " method='animate',\n", |
| 236 | + " args=[None, {'frame': {'duration': 50, 'redraw': True}, 'fromcurrent': True}]\n", |
| 237 | + " ),\n", |
| 238 | + " dict(\n", |
| 239 | + " label='Пауза',\n", |
| 240 | + " method='animate',\n", |
| 241 | + " args=[[None], {'frame': {'duration': 0, 'redraw': False}, 'mode': 'immediate'}]\n", |
| 242 | + " )\n", |
| 243 | + " ],\n", |
| 244 | + " pad={'r': 10, 't': 10}\n", |
| 245 | + " )\n", |
| 246 | + " ],\n", |
| 247 | + " sliders=sliders,\n", |
| 248 | + " title='Анимированная 3D-визуализация Любо́на (Lub)',\n", |
| 249 | + " scene=dict(\n", |
| 250 | + " xaxis_title='t',\n", |
| 251 | + " yaxis_title='|lub(t)|^2',\n", |
| 252 | + " zaxis_title='V_eff(t)',\n", |
| 253 | + " xaxis=dict(range=[-T, T]),\n", |
| 254 | + " yaxis=dict(range=[0, max(psi_data[0][0]) * 1.1]),\n", |
| 255 | + " zaxis=dict(range=[min(V_eff) * 1.1, max(V_eff) * 1.1])\n", |
| 256 | + " ),\n", |
| 257 | + " showlegend=True,\n", |
| 258 | + " width=800,\n", |
| 259 | + " height=600,\n", |
| 260 | + " margin=dict(l=0, r=0, t=50, b=50),\n", |
| 261 | + " scene_aspectmode='manual',\n", |
| 262 | + " scene_aspectratio=dict(x=1, y=1, z=0.5),\n", |
| 263 | + " template='plotly_white',\n", |
| 264 | + " paper_bgcolor='rgba(0,0,0,0)',\n", |
| 265 | + " plot_bgcolor='rgba(0,0,0,0)',\n", |
| 266 | + " autosize=False,\n", |
| 267 | + " scene_camera=dict(eye=dict(x=1.5, y=1.5, z=0.8))\n", |
| 268 | + ")\n", |
| 269 | + "\n", |
| 270 | + "# Показать график\n", |
| 271 | + "fig.show()\n", |
| 272 | + "\n", |
| 273 | + "# Экспорт в HTML\n", |
| 274 | + "fig.write_html(\"lubon_visualization.html\")\n", |
| 275 | + "print(\"* График сохранён как lubon_visualization.html\")" |
| 276 | + ] |
| 277 | + } |
| 278 | + ], |
| 279 | + "metadata": { |
| 280 | + "kernelspec": { |
| 281 | + "display_name": "Python 3", |
| 282 | + "language": "python", |
| 283 | + "name": "python3" |
| 284 | + }, |
| 285 | + "language_info": { |
| 286 | + "codemirror_mode": { |
| 287 | + "name": "ipython", |
| 288 | + "version": 3 |
| 289 | + }, |
| 290 | + "file_extension": ".py", |
| 291 | + "mimetype": "text/x-python", |
| 292 | + "name": "python", |
| 293 | + "nbconvert_exporter": "python", |
| 294 | + "pygments_lexer": "ipython3", |
| 295 | + "version": "3.11.0" |
| 296 | + } |
| 297 | + }, |
| 298 | + "nbformat": 4, |
| 299 | + "nbformat_minor": 4 |
| 300 | +} |
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