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  1. # -*- coding: utf-8 -*-
  2. """
  3. .bin 波形文件 -> 时频曲线查看/出图工具(PLSR 项目用)
  4. 数据格式: 逻辑分析仪导出的单通道数字采样,每字节 1 个采样点;
  5. 电平 >= 阈值(默认128) 判为高(脉冲),否则为低。
  6. 频率定义: 用连续 N 个脉冲的上升沿间隔估计频率;
  7. 频率点放在 N 周期测量窗口中间;
  8. 频率 = N * 采样率 /(第 N 个后续上升沿 - 当前上升沿);
  9. 时间定义: 频率点时间为测量窗口中点;高电平宽度取中心脉冲。
  10. 用法:
  11. python bin_to_time_freq.py <bin文件> [采样率Hz] [选项]
  12. 未填写采样率时默认使用 3125000 Hz。
  13. 示例:
  14. python bin_to_time_freq.py "Document/PLSR_document/波形/10段.bin" 3125000
  15. python bin_to_time_freq.py xxx.bin 3125000 --ymax=12000
  16. python bin_to_time_freq.py xxx.bin 3125000 --save=out.png
  17. python bin_to_time_freq.py xxx.bin 3125000 --selftest
  18. python bin_to_time_freq.py xxx.bin 3125000 --reverse --cycles=8
  19. python bin_to_time_freq.py xxx.bin 3125000 --d1 --d2
  20. python bin_to_time_freq.py xxx.bin 3125000 --d1 --dwindow-ms=10
  21. python bin_to_time_freq.py xxx.bin 3125000 --d1 --d2 --d1-window-ms=5 --d2-window-ms=15
  22. 选项:
  23. --thresh=128 电平阈值(默认128)
  24. --cycles=8 用连续多少个周期估计频率(默认8;1为逐周期)
  25. --reverse 反相电平后再检测脉冲(低电平作为脉冲高电平)
  26. --ymax=12000 频率轴上限(默认自适应)
  27. --d1 另开一张图:频率对时间的一阶导数 df/dt(红)
  28. --d2 另开一张图:频率对时间的二阶导数 d²f/dt²(黑)
  29. --dwindow-ms=5 一、二阶导数的公共拟合窗口,单位 ms(默认5)
  30. --d1-window-ms 原函数 -> 一阶导数的拟合窗口(默认继承 --dwindow-ms)
  31. --d2-window-ms 一阶导数 -> 二阶导数的拟合窗口(默认继承 --dwindow-ms)
  32. --save=路径 保存 PNG 后退出(不弹窗)
  33. --selftest 仅打印统计,不画图
  34. --help, -h 显示这份中文帮助后退出
  35. 交互(弹窗模式):
  36. 滚轮 缩放 X 轴(向上放大/向下缩小,以鼠标位置为中心)
  37. Ctrl+滚轮 缩放 Y 轴(以鼠标 Y 位置为中心)
  38. 左键拖拽 双向平移(上下左右跟随鼠标)
  39. 双击 复位到全图
  40. 鼠标悬停 高亮最近的点并显示其测量点序号、时间与频率
  41. 依赖: pip install numpy matplotlib
  42. """
  43. import sys
  44. import os
  45. import numpy as np
  46. try:
  47. import matplotlib
  48. matplotlib.rcParams['font.sans-serif'] = ['Microsoft YaHei', 'SimHei']
  49. matplotlib.rcParams['axes.unicode_minus'] = False
  50. except Exception:
  51. pass
  52. def load_time_freq(path, fs, threshold=128, cycles=8, reverse=False):
  53. """读取 bin,返回 (t_sec, freq_hz, hi_width_sec, meta)。
  54. t_sec 以第一个脉冲高电平中点为 0 时刻;hi_width 为中心脉冲高电平宽度。"""
  55. data = np.fromfile(path, dtype=np.uint8)
  56. if data.size == 0:
  57. raise ValueError("文件为空: %s" % path)
  58. if not 0 <= threshold <= 255:
  59. raise ValueError("阈值必须在0到255之间")
  60. samples = (data >= threshold).astype(np.int8)
  61. if reverse:
  62. samples = 1 - samples
  63. # run 级压缩
  64. changes = np.flatnonzero(np.diff(samples) != 0) + 1
  65. starts = np.concatenate(([0], changes))
  66. ends = np.concatenate((changes, [len(samples)]))
  67. runs = np.column_stack((starts, ends, samples[starts]))
  68. # 每个高电平 run 的起点都是一个可用于测周期的上升沿。
  69. # 若采集从高电平开始,第一个高电平起点不是被观测到的上升沿,丢弃它。
  70. hi = np.flatnonzero(runs[:, 2] == 1)
  71. if hi.size and runs[hi[0], 0] == 0:
  72. hi = hi[1:]
  73. if hi.size == 0:
  74. raise ValueError("未检测到上升沿脉冲: %s" % path)
  75. # 保留浮点上升沿位置:在原始电平相邻采样点之间线性插值,
  76. # 再配合多周期测量,显著降低整数采样点带来的量化抖动。
  77. rise_idx = runs[hi, 0].astype(np.int64)
  78. t_start = rise_idx.astype(np.float64)
  79. valid = rise_idx > 0
  80. if np.any(valid):
  81. y0 = data[rise_idx[valid] - 1].astype(np.float64)
  82. y1 = data[rise_idx[valid]].astype(np.float64)
  83. delta = y1 - y0
  84. frac = np.zeros_like(y0)
  85. np.divide(float(threshold) - y0, delta, out=frac, where=delta != 0)
  86. t_start[valid] = rise_idx[valid] - 1.0 + np.clip(frac, 0.0, 1.0)
  87. hi_width = (runs[hi, 1] - runs[hi, 0]).astype(np.float64)
  88. if fs <= 0:
  89. raise ValueError("采样率必须大于0")
  90. try:
  91. cycles = int(cycles)
  92. except (TypeError, ValueError):
  93. raise ValueError("cycles 必须是正整数")
  94. if cycles < 1:
  95. raise ValueError("cycles 必须是正整数")
  96. if len(t_start) < 2:
  97. raise ValueError("脉冲不足两个,无法计算频率")
  98. # 用下降沿的阈值 crossing 计算高电平宽度,时间单位仍为采样点。
  99. # 文件末尾若停在高电平,频率仍可用该上升沿作为前一窗口终点;
  100. # 该脉冲的宽度只取到文件末尾,不用于猜测频率。
  101. has_fall = np.zeros(len(hi), dtype=bool)
  102. adjacent = (hi + 1) < len(runs)
  103. has_fall[adjacent] = runs[hi[adjacent] + 1, 2] == 0
  104. fall_idx = np.where(has_fall, runs[hi, 1], len(data)).astype(np.int64)
  105. fall_edge = fall_idx.astype(np.float64)
  106. valid = has_fall & (fall_idx > 0) & (fall_idx < len(data))
  107. if np.any(valid):
  108. y0 = data[fall_idx[valid] - 1].astype(np.float64)
  109. y1 = data[fall_idx[valid]].astype(np.float64)
  110. delta = y1 - y0
  111. frac = np.zeros_like(y0)
  112. np.divide(float(threshold) - y0, delta, out=frac, where=delta != 0)
  113. fall_edge[valid] = fall_idx[valid] - 1.0 + np.clip(frac, 0.0, 1.0)
  114. hi_width = np.maximum(fall_edge - t_start, 0.0)
  115. pulse_mid = t_start + hi_width / 2.0
  116. # 单周期只看到整数采样点,周期接近半个采样点时会严重跳变。
  117. # 跨 cycles 个周期计算总时长,再换算回单周期频率,可显著抑制量化抖动。
  118. cycles = min(cycles, len(t_start) - 1)
  119. left = np.arange(len(t_start) - cycles, dtype=np.int64)
  120. right = left + cycles
  121. period = t_start[right] - t_start[left]
  122. freq = cycles * float(fs) / np.maximum(period, np.finfo(np.float64).eps)
  123. # 频率点放在测量窗口的时间中心;宽度取中心附近脉冲,仅用于兼容绘图接口。
  124. t_center = (t_start[left] + t_start[right]) / 2.0
  125. center_idx = np.minimum(left + cycles // 2, len(hi_width) - 1)
  126. hi_width_out = hi_width[center_idx]
  127. # 时间原点仍为第一个脉冲的高电平中点;多周期测量点自然位于窗口中心。
  128. t_sec = (t_center - pulse_mid[0]) / fs
  129. meta = {
  130. 'total_samples': int(len(samples)),
  131. 'duration': len(samples) / fs,
  132. 'pulses': int(len(freq)),
  133. 'detected_pulses': int(len(t_start)),
  134. 'cycles': int(cycles),
  135. 'offset_ms': t_start[0] / fs * 1000,
  136. 'activity_duration': max(0.0, (fall_edge[-1] - pulse_mid[0]) / fs),
  137. }
  138. return t_sec, freq, hi_width_out / fs, meta
  139. def selftest(path, fs, thresh, cycles, reverse=False):
  140. import statistics
  141. t, freq, hi_w, meta = load_time_freq(path, fs, thresh, cycles, reverse)
  142. print("文件: %s" % path)
  143. print("总采样: %d (%.3f s @ %.2f MS/s)" % (meta['total_samples'], meta['duration'], fs / 1e6))
  144. print("起始采集偏移: %.1f ms" % meta['offset_ms'])
  145. print("检测到脉冲: %d,频率测量点: %d" % (
  146. meta['detected_pulses'], meta['pulses']))
  147. if meta['pulses']:
  148. print("频率 min=%.0f max=%.0f 中位=%.0f Hz" % (
  149. freq.min(), freq.max(), statistics.median(freq)))
  150. print("末测量点: t=%.3f ms, 高电平 %.3f ms, %.0f Hz" % (
  151. t[-1] * 1000, hi_w[-1] * 1000, freq[-1]))
  152. print("估计周期窗口: %d 个周期" % meta['cycles'])
  153. print("波形活动时长: %.1f ms" % (meta['activity_duration'] * 1000))
  154. def local_linear_derivative(t_sec, values, window_s=5e-3, min_points=7):
  155. """对非等间隔时间点做局部线性拟合,返回 d(values)/dt。
  156. 直接对相邻频率点差分会放大采样量化抖动;局部最小二乘斜率
  157. 使用真实时间间隔,并对这种抖动做平均。
  158. """
  159. t = np.asarray(t_sec, dtype=np.float64)
  160. y = np.asarray(values, dtype=np.float64)
  161. if t.ndim != 1 or y.ndim != 1 or len(t) != len(y):
  162. raise ValueError("t_sec 和 values 必须是等长一维数组")
  163. if len(t) < 2:
  164. raise ValueError("至少需要两个点才能计算导数")
  165. if window_s <= 0:
  166. raise ValueError("导数拟合窗口必须大于0")
  167. if np.any(np.diff(t) <= 0):
  168. raise ValueError("时间点必须严格递增")
  169. n = len(t)
  170. min_points = min(n, max(2, int(min_points)))
  171. half_window = window_s / 2.0
  172. left = np.searchsorted(t, t - half_window, side='left')
  173. right = np.searchsorted(t, t + half_window, side='right')
  174. # 低频段在固定时间窗口内可能点数太少,至少补足 min_points 个点。
  175. idx = np.arange(n)
  176. fallback_left = np.clip(idx - min_points // 2, 0, n - min_points)
  177. fallback_right = fallback_left + min_points
  178. too_few = (right - left) < min_points
  179. left[too_few] = fallback_left[too_few]
  180. right[too_few] = fallback_right[too_few]
  181. # 移动时间原点减少长时采集时前缀和相减的精度损失。
  182. x = t - (t[0] + t[-1]) / 2.0
  183. sx = np.concatenate(([0.0], np.cumsum(x)))
  184. sy = np.concatenate(([0.0], np.cumsum(y)))
  185. sxx = np.concatenate(([0.0], np.cumsum(x * x)))
  186. sxy = np.concatenate(([0.0], np.cumsum(x * y)))
  187. count = (right - left).astype(np.float64)
  188. sum_x = sx[right] - sx[left]
  189. sum_y = sy[right] - sy[left]
  190. sum_xx = sxx[right] - sxx[left]
  191. sum_xy = sxy[right] - sxy[left]
  192. denominator = count * sum_xx - sum_x * sum_x
  193. numerator = count * sum_xy - sum_x * sum_y
  194. derivative = np.empty(n, dtype=np.float64)
  195. good = np.abs(denominator) > np.finfo(np.float64).eps
  196. derivative[good] = numerator[good] / denominator[good]
  197. derivative[~good] = np.gradient(y, t)[~good]
  198. return derivative
  199. def plot_show(path, fs, thresh, ymax, cycles, reverse, save_path=None,
  200. draw_d1=False, draw_d2=False, d1_window_ms=5.0,
  201. d2_window_ms=None):
  202. t, freq, hi_w, meta = load_time_freq(path, fs, thresh, cycles, reverse)
  203. import matplotlib.pyplot as plt
  204. from matplotlib.ticker import MaxNLocator
  205. fig, ax = plt.subplots(figsize=(15, 7))
  206. fig.subplots_adjust(bottom=0.10, top=0.92)
  207. # 全脉冲散点:复用 artist,重绘时按可见范围抽稀(大文件流畅)
  208. MAX_VISIBLE_POINTS = 5000 # 可见范围内最多绘制的点数,超过则等间隔抽稀
  209. (scatter,) = ax.plot([], [], '.', ms=1.5, color='C0', alpha=0.5, zorder=1)
  210. tx_ms = t * 1000
  211. x_full = tx_ms
  212. y_full = freq
  213. ax.set_xlim(0.0, meta['activity_duration'] * 1000 * 1.02)
  214. ax.set_ylim(0, ymax if ymax > 0 else freq.max() * 1.08)
  215. ax.set_title("%s 时频曲线(检测到脉冲 %d,频率测量点 %d,%d 周期平均,活动时长 %.0f ms)" % (
  216. os.path.basename(path), meta['detected_pulses'], meta['pulses'], meta['cycles'],
  217. meta['activity_duration'] * 1000))
  218. ax.set_xlabel("时间 (ms)")
  219. ax.set_ylabel("频率 (Hz)")
  220. # 更密的刻度
  221. ax.xaxis.set_major_locator(MaxNLocator(nbins=20))
  222. ax.yaxis.set_major_locator(MaxNLocator(nbins=15))
  223. ax.grid(True, which='major', alpha=0.35)
  224. ax.grid(True, which='minor', alpha=0.15)
  225. ax.minorticks_on()
  226. fig_der = None
  227. draw_d1 = draw_d1 and (len(freq) >= 2)
  228. draw_d2 = draw_d2 and (len(freq) >= 3)
  229. if draw_d1 or draw_d2:
  230. f64 = freq.astype(np.float64)
  231. if d2_window_ms is None:
  232. d2_window_ms = d1_window_ms
  233. d1_full = local_linear_derivative(t, f64, d1_window_ms * 1e-3)
  234. d2_full = (local_linear_derivative(t, d1_full, d2_window_ms * 1e-3)
  235. if draw_d2 else None)
  236. plot_count = int(draw_d1) + int(draw_d2)
  237. fig_der, axes_der = plt.subplots(plot_count, 1, figsize=(15, 4.5 * plot_count),
  238. sharex=True, squeeze=False)
  239. fig_der.subplots_adjust(bottom=0.14, top=0.90)
  240. row = 0
  241. if draw_d1:
  242. ax_der = axes_der[row, 0]
  243. ax_der.plot(x_full, d1_full, '-', lw=0.9, color='red', label='df/dt')
  244. ax_der.set_ylabel("一阶导数 (Hz/s)")
  245. ax_der.legend(loc='upper right')
  246. row += 1
  247. if draw_d2:
  248. ax_der = axes_der[row, 0]
  249. ax_der.plot(x_full, d2_full, '-', lw=0.9, color='black', label='d²f/dt²')
  250. ax_der.set_ylabel("二阶导数 (Hz/s²)")
  251. ax_der.legend(loc='upper right')
  252. for ax_der in axes_der[:, 0]:
  253. ax_der.set_xlim(0.0, meta['activity_duration'] * 1000 * 1.02)
  254. ax_der.grid(True, which='major', alpha=0.35)
  255. ax_der.minorticks_on()
  256. axes_der[-1, 0].set_xlabel("时间 (ms)")
  257. axes_der[0, 0].set_title(
  258. "时频曲线导数(一阶窗口 %.3g ms / 二阶窗口 %.3g ms)" %
  259. (d1_window_ms, d2_window_ms))
  260. if save_path:
  261. scatter.set_data(x_full, y_full)
  262. root, ext = os.path.splitext(save_path)
  263. fig.savefig(save_path, dpi=130)
  264. print("已保存: %s" % save_path)
  265. if fig_der is not None:
  266. der_path = root + "_d" + ext
  267. fig_der.savefig(der_path, dpi=130)
  268. print("已保存: %s" % der_path)
  269. plt.close(fig)
  270. if fig_der is not None:
  271. plt.close(fig_der)
  272. return
  273. # 交互:滚轮缩放 X(Ctrl+滚轮缩放 Y)/ 左键双向拖拽平移 / 双击复位 / 悬停高亮
  274. state = {'press_x': None, 'press_y': None,
  275. 'press_xlim': None, 'press_ylim': None}
  276. # 悬停高亮:一个红点标记 + 一个带框文本
  277. (hl_marker,) = ax.plot([], [], 'o', ms=9, mfc='red', mec='white',
  278. mew=1.0, zorder=5, visible=False)
  279. hl_text = ax.text(0, 0, '', fontsize=10, color='black',
  280. bbox=dict(boxstyle='round,pad=0.3', fc='yellow', ec='red', alpha=0.9),
  281. zorder=6, visible=False)
  282. hover_last = {'idx': -1, 'visible': False}
  283. # 可见范围内抽稀绘制散点(大文件性能优化)
  284. def update_scatter():
  285. x0, x1 = ax.get_xlim()
  286. mask = (x_full >= x0) & (x_full <= x1)
  287. n_vis = int(np.count_nonzero(mask))
  288. if n_vis > MAX_VISIBLE_POINTS:
  289. # 等间隔抽稀:取 n_vis 中的 MAX_VISIBLE_POINTS 个
  290. step = (n_vis + MAX_VISIBLE_POINTS - 1) // MAX_VISIBLE_POINTS
  291. idx = np.flatnonzero(mask)[::step]
  292. else:
  293. idx = np.flatnonzero(mask)
  294. scatter.set_data(x_full[idx], y_full[idx])
  295. def on_scroll(event):
  296. if event.inaxes is not ax or event.xdata is None:
  297. return
  298. zoom_in = event.button == 'up'
  299. factor = 1.0 / 1.5 if zoom_in else 1.5
  300. if event.key in ('control', 'ctrl'):
  301. # Ctrl+滚轮:缩放 Y 轴,以鼠标 Y 位置为锚点(锚点数据点不动)
  302. y0, y1 = ax.get_ylim()
  303. cy = event.ydata
  304. n0 = cy - (cy - y0) * factor
  305. n1 = cy + (y1 - cy) * factor
  306. if n1 - n0 < 1.0:
  307. return
  308. ax.set_ylim(n0, n1)
  309. else:
  310. # 普通滚轮:缩放 X 轴,以鼠标 X 位置为锚点(锚点数据点不动)
  311. x0, x1 = ax.get_xlim()
  312. n0 = event.xdata - (event.xdata - x0) * factor
  313. n1 = event.xdata + (x1 - event.xdata) * factor
  314. if n1 - n0 < 1e-6:
  315. return
  316. ax.set_xlim(n0, n1)
  317. update_scatter()
  318. fig.canvas.draw_idle()
  319. def on_press(event):
  320. if event.inaxes is ax and event.button == 1:
  321. state['press_x'] = event.xdata
  322. state['press_y'] = event.ydata
  323. state['press_xlim'] = ax.get_xlim()
  324. state['press_ylim'] = ax.get_ylim()
  325. def on_motion(event):
  326. if event.inaxes is not ax or event.xdata is None:
  327. return
  328. if state['press_x'] is not None:
  329. # 拖拽平移:X/Y 双向跟随鼠标
  330. x0, x1 = state['press_xlim']
  331. y0, y1 = state['press_ylim']
  332. dx = event.xdata - state['press_x']
  333. dy = event.ydata - state['press_y']
  334. ax.set_xlim(x0 - dx, x1 - dx)
  335. ax.set_ylim(y0 - dy, y1 - dy)
  336. update_scatter()
  337. fig.canvas.draw_idle()
  338. return
  339. # 悬停:找可见范围内距鼠标最近的脉冲点(屏幕像素距离 < 20px 才高亮)
  340. x0, x1 = ax.get_xlim()
  341. mask = (x_full >= x0) & (x_full <= x1)
  342. if not np.any(mask):
  343. if hover_last['visible']:
  344. hl_marker.set_visible(False)
  345. hl_text.set_visible(False)
  346. fig.canvas.draw_idle()
  347. hover_last['visible'] = False
  348. return
  349. px, py = ax.transData.transform(np.column_stack([x_full[mask], y_full[mask]])).T
  350. dist = np.hypot(px - event.x, py - event.y)
  351. k = int(np.argmin(dist))
  352. if dist[k] <= 20.0:
  353. idx = int(np.flatnonzero(mask)[k])
  354. hl_marker.set_data([x_full[idx]], [y_full[idx]])
  355. hl_text.set_text("测量点 #%d\nt = %.3f ms\nf = %.0f Hz"
  356. % (idx + 1, x_full[idx], y_full[idx]))
  357. hl_text.set_position((x_full[idx] + (x1 - x0) * 0.01,
  358. y_full[idx] + (ax.get_ylim()[1] - ax.get_ylim()[0]) * 0.02))
  359. hl_marker.set_visible(True)
  360. hl_text.set_visible(True)
  361. if hover_last['idx'] != idx or not hover_last['visible']:
  362. fig.canvas.draw_idle()
  363. hover_last['idx'] = idx
  364. hover_last['visible'] = True
  365. else:
  366. if hover_last['visible']:
  367. hl_marker.set_visible(False)
  368. hl_text.set_visible(False)
  369. fig.canvas.draw_idle()
  370. hover_last['visible'] = False
  371. def on_release(event):
  372. state['press_x'] = None
  373. def on_double(event):
  374. if event.dblclick:
  375. ax.set_xlim(0.0, meta['activity_duration'] * 1000 * 1.02)
  376. ax.set_ylim(0, ymax if ymax > 0 else freq.max() * 1.08)
  377. update_scatter()
  378. fig.canvas.draw_idle()
  379. update_scatter()
  380. fig.canvas.mpl_connect('scroll_event', on_scroll)
  381. fig.canvas.mpl_connect('button_press_event', on_press)
  382. fig.canvas.mpl_connect('button_release_event', on_release)
  383. fig.canvas.mpl_connect('motion_notify_event', on_motion)
  384. fig.canvas.mpl_connect('button_press_event', on_double)
  385. print("打开窗口:滚轮缩放X / Ctrl+滚轮缩放Y / 左键双向拖拽平移 / 双击复位")
  386. print("检测到脉冲 %d,频率测量点 %d,使用 %d 周期平均,活动时长 %.1f ms" % (
  387. meta['detected_pulses'], meta['pulses'], meta['cycles'],
  388. meta['activity_duration'] * 1000))
  389. plt.show()
  390. def main():
  391. args = [a for a in sys.argv[1:] if not a.startswith('--')]
  392. opts = {a.split('=', 1)[0]: (a.split('=', 1)[1] if '=' in a else True)
  393. for a in sys.argv[1:] if a.startswith('--')}
  394. if len(args) < 1 or '--help' in opts or '-h' in sys.argv[1:]:
  395. print(__doc__)
  396. sys.exit(0)
  397. path = args[0]
  398. fs = float(args[1]) if len(args) > 1 else 3.125e6
  399. thresh = int(opts.get('--thresh', 128))
  400. cycles = int(opts.get('--cycles', 8))
  401. reverse = '--reverse' in opts
  402. ymax = float(opts.get('--ymax', 0))
  403. save_path = opts.get('--save', '')
  404. draw_d1 = '--d1' in opts
  405. draw_d2 = '--d2' in opts
  406. derivative_window_ms = float(opts.get('--dwindow-ms', 5.0))
  407. d1_window_ms = float(opts.get('--d1-window-ms', derivative_window_ms))
  408. d2_window_ms = float(opts.get('--d2-window-ms', derivative_window_ms))
  409. if not os.path.isfile(path):
  410. print("错误:文件不存在 - %s" % path)
  411. sys.exit(1)
  412. if '--selftest' in opts:
  413. selftest(path, fs, thresh, cycles, reverse)
  414. else:
  415. plot_show(path, fs, thresh, ymax, cycles, reverse, save_path or None,
  416. draw_d1, draw_d2, d1_window_ms, d2_window_ms)
  417. if __name__ == '__main__':
  418. main()