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Update app.py
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app.py
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import os
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import math
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import tempfile
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import gradio as gr
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import cudaq
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import numpy as np
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import cupy as cp
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from pathlib import Path
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import plotly.graph_objects as go
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import plotly.io as pio
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from scipy.spatial import Delaunay
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# Set Plotly engine for image export
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try:
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except AttributeError:
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pass
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def simulate_qlbm_and_animate(num_reg_qubits: int, T: int, distribution_type: str, ux_input: float, uy_input: float, velocity_field_type: str):
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"""
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Simulates a 2D advection-diffusion problem using a Quantum Lattice Boltzmann Method (QLBM)
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and generates an interactive Plotly figure with a slider for selected time steps.
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"""
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# GIF related variables removed as GIF generation is no longer needed
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# video_length = T
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# simulation_fps = 0.1
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# frames = int(simulation_fps * video_length)
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# if frames == 0:
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# frames = 1
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num_anc = 3
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num_qubits_total = 2 * num_reg_qubits + num_anc
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current_N = 2**num_reg_qubits
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N_tot_state_vector = 2**num_qubits_total
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num_ranks = 1
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rank = 0
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N_sub_per_rank = int(N_tot_state_vector // num_ranks)
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# timesteps_per_frame logic removed as it was for GIF
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# timesteps_per_frame = 1
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# if frames < T and frames > 0:
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# timesteps_per_frame = int(T / frames)
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# if timesteps_per_frame == 0:
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# timesteps_per_frame = 1
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# Initial state setup
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if distribution_type == "Sine Wave (Original)":
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selected_initial_state_function_raw = lambda x, y, N_val_func: \
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np.sin(x * 2 * np.pi / N_val_func) * (1 - 0.5 * x / N_val_func) * \
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np.sin(y * 4 * np.pi / N_val_func) * (1 - 0.5 * y / N_val_func) + 1
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elif distribution_type == "Gaussian":
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selected_initial_state_function_raw = lambda x, y, N_val_func: \
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np.exp(-((x - N_val_func / 2)**2 / (2 * (N_val_func / 5)**2) +
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(y - N_val_func / 2)**2 / (2 * (N_val_func / 5)**2))) * 1.8 + 0.2
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elif distribution_type == "Random":
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selected_initial_state_function_raw = lambda x, y, N_val_func: \
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np.random.rand(N_val_func, N_val_func) * 1.5 + 0.2 if isinstance(x, int) else \
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np.random.rand(x.shape, x.shape[3]) * 1.5 + 0.2
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else:
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print(f"Warning: Unknown distribution type '{distribution_type}'. Defaulting to Sine Wave.")
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selected_initial_state_function_raw = lambda x, y, N_val_func: \
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np.sin(x * 2 * np.pi / N_val_func) * (1 - 0.5 * x / N_val_func) * \
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np.sin(y * 4 * np.pi / N_val_func) * (1 - 0.5 * y / N_val_func) + 1
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initial_state_func_eval = lambda x_coords, y_coords: \
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selected_initial_state_function_raw(x_coords, y_coords, current_N) * \
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(y_coords < current_N).astype(int)
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with tempfile.TemporaryDirectory() as tmp_npy_dir:
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intermediate_folder_path = Path(tmp_npy_dir)
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cudaq.set_target('nvidia', option='fp64')
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@cudaq.kernel
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def alloc_kernel(num_qubits_alloc: int):
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qubits = cudaq.qvector(num_qubits_alloc)
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from cupy.cuda.memory import MemoryPointer, UnownedMemory
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def to_cupy_array(state):
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tensor = state.getTensor()
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pDevice = tensor.data()
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sizeByte = tensor.get_num_elements() * tensor.get_element_size()
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mem = UnownedMemory(pDevice, sizeByte, owner=state)
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memptr_obj = MemoryPointer(mem, 0)
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cupy_array_val = cp.ndarray(tensor.get_num_elements(),
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dtype=cp.complex128,
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memptr=memptr_obj)
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return cupy_array_val
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class QLBMAdvecDiffD2Q5_new:
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def __init__(self, ux=0.2, uy=0.15) -> None:
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self.dim = 2
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self.ndir = 5
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self.nq_dir = math.ceil(np.log2(self.ndir))
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self.dirs =
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for dir_int in range(self.ndir):
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dir_bin = f"{dir_int:b}".zfill(self.nq_dir)
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self.dirs.append(dir_bin)
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self.e_unitvec = np.array([0, 1, -1, 1, -1])
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self.wts = np.array([2/6, 1/6, 1/6, 1/6, 1/6])
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self.cs = 1 / np.sqrt(3)
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self.ux = ux
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self.uy = uy
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self.u = np.array([0, self.ux, self.ux, self.uy, self.uy])
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self.wtcoeffs = np.multiply(self.wts, 1 + self.e_unitvec * self.u / self.cs**2)
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self.create_circuit()
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def create_circuit(self):
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v = np.pad(self.wtcoeffs, (0, 2**num_anc - self.ndir))
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v = v**0.5
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v += 1 # Original line was v += 1, not v += 1
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v = v / np.linalg.norm(v)
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U_prep = 2 * np.outer(v, v) - np.eye(len(v))
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cudaq.register_operation("prep_op", U_prep)
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def collisionOp(dirs_list):
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dirs_i_list_val =
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for dir_str in dirs_list:
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dirs_i = [(int(c)) for c in dir_str]
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dirs_i_list_val += dirs_i[::-1]
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return dirs_i_list_val
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self.dirs_i_list = collisionOp(self.dirs)
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@cudaq.kernel
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def rshift(q: cudaq.qview, n: int):
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for i in range(n):
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if i == n - 1:
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x(q[n - 1 - i])
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elif i == n - 2:
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x.ctrl(q[n - 1 - (i + 1)], q[n - 1 - i])
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else:
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x.ctrl(q[0:n - 1 - i], q[n - 1 - i])
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@cudaq.kernel
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def lshift(q: cudaq.qview, n: int):
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for i in range(n):
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if i == 0:
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x(q) # Corrected from x(q)
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elif i == 1:
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x.ctrl(q, q[3])
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else:
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x.ctrl(q[0:i], q[i])
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@cudaq.kernel
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def d2q5_tstep(q: cudaq.qview, nqx: int, nqy: int, nq_dir_val: int, dirs_i_val: list[int]):
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qx = q[0:nqx]
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qy = q[nqx:nqx + nqy]
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qdir = q[nqx + nqy:nqx + nqy + nq_dir_val]
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idx_lqx = 2
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b_list = dirs_i_val[idx_lqx * nq_dir_val:(idx_lqx + 1) * nq_dir_val]
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for j in range(nq_dir_val):
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if b_list[j] == 0: x(qdir[j])
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cudaq.control(lshift, qdir, qx, nqx)
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for j in range(nq_dir_val):
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if b_list[j] == 0: x(qdir[j])
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idx_rqx = 1
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b_list = dirs_i_val[idx_rqx * nq_dir_val:(idx_rqx + 1) * nq_dir_val]
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for j in range(nq_dir_val):
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if b_list[j] == 0: x(qdir[j])
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cudaq.control(rshift, qdir, qx, nqx)
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for j in range(nq_dir_val):
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if b_list[j] == 0: x(qdir[j])
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idx_lqy = 4
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b_list = dirs_i_val[idx_lqy * nq_dir_val:(idx_lqy + 1) * nq_dir_val]
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for j in range(nq_dir_val):
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if b_list[j] == 0: x(qdir[j])
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cudaq.control(lshift, qdir, qy, nqy)
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for j in range(nq_dir_val):
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if b_list[j] == 0: x(qdir[j])
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idx_rqy = 3
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b_list = dirs_i_val[idx_rqy * nq_dir_val:(idx_rqy + 1) * nq_dir_val]
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for j in range(nq_dir_val):
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if b_list[j] == 0: x(qdir[j])
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cudaq.control(rshift, qdir, qy, nqy)
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for j in range(nq_dir_val):
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if b_list[j] == 0: x(qdir[j])
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@cudaq.kernel
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def d2q5_tstep_wrapper(state_arg: cudaq.State, nqx: int, nqy: int, nq_dir_val: int, dirs_i_val: list[int]):
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q = cudaq.qvector(state_arg)
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qdir = q[nqx + nqy:nqx + nqy + nq_dir_val]
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prep_op(qdir[4], qdir[3], qdir) # Corrected from qdir
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d2q5_tstep(q, nqx, nqy, nq_dir_val, dirs_i_val)
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prep_op(qdir[4], qdir[3], qdir) # Corrected from qdir
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@cudaq.kernel
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def d2q5_tstep_wrapper_hadamard(vec_arg: list[complex], nqx: int, nqy: int, nq_dir_val: int, dirs_i_val: list[int]):
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q = cudaq.qvector(vec_arg)
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qdir = q[nqx + nqy:nqx + nqy + nq_dir_val]
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qy = q[nqx:nqx + nqy]
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prep_op(qdir[4], qdir[3], qdir) # Corrected from qdir
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d2q5_tstep(q, nqx, nqy, nq_dir_val, dirs_i_val)
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prep_op(qdir[4], qdir[3], qdir) # Corrected from qdir
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for i in range(nqy):
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h(qy[i])
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def run_timestep_func(vec_arg, hadamard=False):
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if hadamard:
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result = cudaq.get_state(d2q5_tstep_wrapper_hadamard, vec_arg, num_reg_qubits, num_reg_qubits, self.nq_dir, self.dirs_i_list)
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else:
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result = cudaq.get_state(d2q5_tstep_wrapper, vec_arg, num_reg_qubits, num_reg_qubits, self.nq_dir, self.dirs_i_list)
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num_nonzero_ranks = num_ranks / (2**num_anc)
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rank_slice_cupy = to_cupy_array(result)
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if rank >= num_nonzero_ranks and num_nonzero_ranks > 0:
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sub_sv_zeros = np.zeros(N_sub_per_rank, dtype=np.complex128)
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cp.cuda.runtime.memcpy(rank_slice_cupy.data.ptr, sub_sv_zeros.ctypes.data, sub_sv_zeros.nbytes, cp.cuda.runtime.memcpyHostToDevice)
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if rank == 0 and num_nonzero_ranks < 1 and N_sub_per_rank > 0:
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limit_idx = int(N_tot_state_vector / (2**num_anc))
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if limit_idx < rank_slice_cupy.size:
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rank_slice_cupy[limit_idx:] = 0
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return result
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self.run_timestep = run_timestep_func
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def write_state(self, state_to_write, t_step_str_val):
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rank_slice_cupy = to_cupy_array(state_to_write)
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num_nonzero_ranks = num_ranks / (2**num_anc)
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if rank < num_nonzero_ranks or (rank == 0 and num_nonzero_ranks <= 0):
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save_path = intermediate_folder_path / f"{t_step_str_val}_{rank}.npy"
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with open(save_path, 'wb') as f:
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arr_to_save = None
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data_limit = N_sub_per_rank
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if num_nonzero_ranks < 1 and rank == 0:
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data_limit = int(N_tot_state_vector / (2**num_anc))
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if data_limit > 0:
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relevant_part_cupy = cp.real(rank_slice_cupy[:data_limit])
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else:
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relevant_part_cupy = cp.array(, dtype=cp.float64)
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if relevant_part_cupy.size >= current_N * current_N:
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arr_flat = relevant_part_cupy[:current_N * current_N]
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if downsampling_factor > 1 and current_N > 0:
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arr_reshaped = arr_flat.reshape((current_N, current_N))
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arr_downsampled = arr_reshaped[::downsampling_factor, ::downsampling_factor]
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arr_to_save = arr_downsampled.flatten()
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else:
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arr_to_save = arr_flat
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elif relevant_part_cupy.size > 0:
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if downsampling_factor > 1:
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arr_to_save = relevant_part_cupy[::downsampling_factor]
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else:
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arr_to_save = relevant_part_cupy
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if arr_to_save is not None and arr_to_save.size > 0:
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np.save(f, arr_to_save.get() if isinstance(arr_to_save, cp.ndarray) else arr_to_save)
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def run_evolution(self, initial_state_arg, total_timesteps, observable=False, timesteps_to_save=None):
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current_state_val = initial_state_arg
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for t_iter in range(total_timesteps):
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next_state_val = None
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if t_iter == total_timesteps - 1 and observable:
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next_state_val = self.run_timestep(current_state_val, True)
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self.write_state(next_state_val, str(t_iter)) # Save final state
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else:
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next_state_val = self.run_timestep(current_state_val)
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# Save data only for specific intervals for the slider
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if timesteps_to_save and t_iter in timesteps_to_save:
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self.write_state(next_state_val, str(t_iter))
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if rank == 0 and t_iter % 10 == 0: # Print progress less frequently
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print(f"Timestep: {t_iter}/{total_timesteps}")
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cp.get_default_memory_pool().free_all_blocks()
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current_state_val = next_state_val
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if rank == 0:
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print(f"Timestep: {total_timesteps}/{total_timesteps} (Evolution complete)")
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cp.get_default_memory_pool().free_all_blocks()
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self.final_state = current_state_val
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downsampling_factor = 2**5
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if current_N == 0:
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print("Error: current_N is zero. num_reg_qubits likely too small.")
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return None, None
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if current_N < downsampling_factor:
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downsampling_factor = current_N if current_N > 0 else 1
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qlbm_obj = QLBMAdvecDiffD2Q5_new(ux=ux_input, uy=uy_input)
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initial_state_val = cudaq.get_state(alloc_kernel, num_qubits_total)
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xv_init = np.arange(current_N)
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yv_init = np.arange(current_N)
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initial_grid_2d_X, initial_grid_2d_Y = np.meshgrid(xv_init, yv_init)
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if distribution_type == "Random":
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initial_grid_2d = selected_initial_state_function_raw(current_N, current_N, current_N)
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else:
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initial_grid_2d = initial_state_func_eval(initial_grid_2d_X, initial_grid_2d_Y)
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sub_sv_init_flat = initial_grid_2d.flatten().astype(np.complex128)
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full_initial_sv_host = np.zeros(N_sub_per_rank, dtype=np.complex128)
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num_computational_states = current_N * current_N
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if len(sub_sv_init_flat) == num_computational_states:
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if num_computational_states <= N_sub_per_rank:
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full_initial_sv_host[:num_computational_states] = sub_sv_init_flat
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else:
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| 299 |
-
print(f"Error: Grid data {num_computational_states} > N_sub_per_rank {N_sub_per_rank}")
|
| 300 |
-
return None, None
|
| 301 |
-
else:
|
| 302 |
-
print(f"Warning: Initial state size {len(sub_sv_init_flat)}!= expected {num_computational_states}")
|
| 303 |
-
fill_len = min(len(sub_sv_init_flat), num_computational_states, N_sub_per_rank)
|
| 304 |
-
full_initial_sv_host[:fill_len] = sub_sv_init_flat[:fill_len]
|
| 305 |
-
|
| 306 |
-
rank_slice_init = to_cupy_array(initial_state_val)
|
| 307 |
-
print(f'Rank {rank}: Initializing state with {distribution_type} (ux={ux_input}, uy={uy_input})...')
|
| 308 |
-
cp.cuda.runtime.memcpy(rank_slice_init.data.ptr, full_initial_sv_host.ctypes.data, full_initial_sv_host.nbytes, cp.cuda.runtime.memcpyHostToDevice)
|
| 309 |
-
print(f'Rank {rank}: Initial state copied. Size: {len(sub_sv_init_flat)}. N_sub_per_rank: {N_sub_per_rank}')
|
| 310 |
-
|
| 311 |
-
# Explicitly save initial state (t=0)
|
| 312 |
-
qlbm_obj.write_state(initial_state_val, "0")
|
| 313 |
-
|
| 314 |
-
print("Starting QLBM evolution...")
|
| 315 |
-
# Define specific timesteps to save for the slider
|
| 316 |
-
timesteps_for_slider = # T-1 is the last t_iter
|
| 317 |
-
qlbm_obj.run_evolution(initial_state_val, T, timesteps_to_save=timesteps_for_slider)
|
| 318 |
-
print("QLBM evolution complete.")
|
| 319 |
-
|
| 320 |
-
print("Generating plots with Plotly...")
|
| 321 |
-
downsampled_N = current_N // downsampling_factor
|
| 322 |
-
if downsampled_N == 0 and current_N > 0:
|
| 323 |
-
downsampled_N = 1
|
| 324 |
-
elif current_N == 0:
|
| 325 |
-
print("Error: current_N is zero before Plotly stage.")
|
| 326 |
-
return None, None
|
| 327 |
-
|
| 328 |
-
# Load data for specific time steps for interactive plot
|
| 329 |
-
# These correspond to the filenames saved: 0, T//4, 3*T//4, T-1
|
| 330 |
-
time_steps_to_load =
|
| 331 |
-
data_frames =
|
| 332 |
-
actual_timesteps_loaded =
|
| 333 |
-
for t in time_steps_to_load:
|
| 334 |
-
file_path = intermediate_folder_path / f"{t}_{rank}.npy"
|
| 335 |
-
if file_path.exists():
|
| 336 |
-
sol_loaded = np.load(file_path)
|
| 337 |
-
if sol_loaded.size == downsampled_N * downsampled_N:
|
| 338 |
-
Z_data = np.reshape(sol_loaded, (downsampled_N, downsampled_N))
|
| 339 |
-
data_frames.append(Z_data)
|
| 340 |
-
actual_timesteps_loaded.append(t)
|
| 341 |
-
else:
|
| 342 |
-
print(f"Warning: File {file_path} size {sol_loaded.size}!= expected {downsampled_N*downsampled_N}. Skipping.")
|
| 343 |
-
else:
|
| 344 |
-
print(f"Warning: File {file_path} not found. Skipping.")
|
| 345 |
-
|
| 346 |
-
if not data_frames:
|
| 347 |
-
print("Error: No data frames loaded for interactive plot.")
|
| 348 |
-
return None, None
|
| 349 |
-
|
| 350 |
-
x_coords_plot = np.linspace(-10, 10, downsampled_N)
|
| 351 |
-
y_coords_plot = np.linspace(-10, 10, downsampled_N)
|
| 352 |
-
|
| 353 |
-
# Calculate global min/max for consistent scaling
|
| 354 |
-
z_min = min([np.min(Z) for Z in data_frames])
|
| 355 |
-
z_max = max([np.max(Z) for Z in data_frames])
|
| 356 |
-
if z_max == z_min:
|
| 357 |
-
z_max += 1e-9
|
| 358 |
-
|
| 359 |
-
# Create interactive Plotly figure with slider
|
| 360 |
-
fig = go.Figure()
|
| 361 |
-
|
| 362 |
-
for i, Z in enumerate(data_frames):
|
| 363 |
-
fig.add_trace(
|
| 364 |
-
go.Surface(
|
| 365 |
-
z=Z, x=x_coords_plot, y=y_coords_plot,
|
| 366 |
-
colorscale='Viridis',
|
| 367 |
-
cmin=z_min, cmax=z_max,
|
| 368 |
-
name=f'Time: {actual_timesteps_loaded[i]}',
|
| 369 |
-
showscale=(i == 0) # Show color scale only for the first trace
|
| 370 |
-
)
|
| 371 |
-
)
|
| 372 |
-
|
| 373 |
-
steps =
|
| 374 |
-
for i in range(len(data_frames)):
|
| 375 |
-
step = dict(
|
| 376 |
-
method="update",
|
| 377 |
-
args=[{"visible": [False] * len(data_frames)}],
|
| 378 |
-
label=f"Time: {actual_timesteps_loaded[i]}"
|
| 379 |
-
)
|
| 380 |
-
step["args"]["visible"][i] = True
|
| 381 |
-
steps.append(step)
|
| 382 |
-
|
| 383 |
-
sliders =
|
| 384 |
-
|
| 385 |
-
fig.update_layout(
|
| 386 |
-
title='QLBM Simulation - Density Evolution',
|
| 387 |
-
scene=dict(
|
| 388 |
-
xaxis_title='X',
|
| 389 |
-
yaxis_title='Y',
|
| 390 |
-
zaxis_title='Density',
|
| 391 |
-
xaxis=dict(range=[x_coords_plot, x_coords_plot[-1]]),
|
| 392 |
-
yaxis=dict(range=[y_coords_plot, y_coords_plot[-1]]),
|
| 393 |
-
zaxis=dict(range=[z_min, z_max]),
|
| 394 |
-
),
|
| 395 |
-
sliders=sliders,
|
| 396 |
-
width=1000, # Increased width
|
| 397 |
-
height=900 # Increased height
|
| 398 |
-
)
|
| 399 |
-
|
| 400 |
-
# GIF generation logic removed as per request
|
| 401 |
-
#... (removed all GIF related code)...
|
| 402 |
-
|
| 403 |
-
return fig # Return only the interactive Plotly figure
|
| 404 |
|
| 405 |
-
|
| 406 |
-
def qlbm_gradio_interface(num_reg_qubits_input: int, timescale_input: int, distribution_type_param: str, ux_param: float, uy_param: float, velocity_field_type_param: str):
|
| 407 |
-
num_reg_qubits_val = int(num_reg_qubits_input)
|
| 408 |
-
timescale_val = int(timescale_input)
|
| 409 |
-
ux_val = float(ux_param)
|
| 410 |
-
uy_val = float(uy_param)
|
| 411 |
-
|
| 412 |
-
print(f"Gradio Interface: num_reg_qubits={num_reg_qubits_val}, T={timescale_val}, Distribution={distribution_type_param}, ux={ux_val}, uy={uy_val}, VelocityFieldType={velocity_field_type_param}")
|
| 413 |
-
|
| 414 |
-
plot_fig = simulate_qlbm_and_animate( # Only expecting plot_fig now
|
| 415 |
-
num_reg_qubits=num_reg_qubits_val,
|
| 416 |
-
T=timescale_val,
|
| 417 |
-
distribution_type=distribution_type_param,
|
| 418 |
-
ux_input=ux_val,
|
| 419 |
-
uy_input=uy_val,
|
| 420 |
-
velocity_field_type=velocity_field_type_param # Pass the new dummy parameter
|
| 421 |
-
)
|
| 422 |
-
|
| 423 |
-
if plot_fig is None:
|
| 424 |
-
gr.Warning("Simulation or plotting failed. Please check console for errors.")
|
| 425 |
-
return None
|
| 426 |
-
return plot_fig # Return only the interactive Plotly figure
|
| 427 |
|
| 428 |
-
with gr.Blocks(theme=gr.themes.Soft(), title="QLBM Simulation with Plotly") as qlbm_demo:
|
| 429 |
-
gr.Markdown(
|
| 430 |
-
"""
|
| 431 |
-
# ⚛️ Quantum Lattice Boltzmann Method (QLBM) Simulator (Plotly Animation)
|
| 432 |
-
Welcome to the Quantum Lattice Boltzmann Method (QLBM) simulator! This version uses Plotly for 3D animation and interactive plots.
|
| 433 |
-
|
| 434 |
-
**How this Simulator Works:**
|
| 435 |
-
This simulator implements a D2Q5 model on a quantum computer simulator (CUDA-Q).
|
| 436 |
-
- Control grid size (via Number of Register Qubits: $N=2^{\text{num_reg_qubits}}$).
|
| 437 |
-
- Set total simulation time (Timescale T).
|
| 438 |
-
- Choose initial distribution.
|
| 439 |
-
- Set advection velocities `ux` and `uy`.
|
| 440 |
-
The simulation generates an interactive Plotly figure with a slider for selected time steps.
|
| 441 |
-
|
| 442 |
-
**Note:** Higher qubit counts and longer timescales are computationally intensive. Advection velocities should be small (e.g., < 0.3).
|
| 443 |
-
The Plotly figure allows interactive exploration of specific time steps.
|
| 444 |
-
"""
|
| 445 |
-
)
|
| 446 |
-
with gr.Row():
|
| 447 |
-
with gr.Column(scale=1):
|
| 448 |
-
gr.Markdown("## Simulation Parameters")
|
| 449 |
-
num_reg_qubits_slider = gr.Slider(
|
| 450 |
-
minimum=2, maximum=10, value=8, step=1,
|
| 451 |
-
label="Number of Register Qubits (num_reg_qubits)",
|
| 452 |
-
info="Grid N = 2^num_reg_qubits. Max 10 (Note: >8 slow; >9 may hit simulator/memory limits on free tiers)."
|
| 453 |
-
)
|
| 454 |
-
timescale_slider = gr.Slider(
|
| 455 |
-
minimum=0, maximum=2000, value=100, step=10,
|
| 456 |
-
label="Timescale (T)", info="Total number of timesteps. Max 2000."
|
| 457 |
-
)
|
| 458 |
-
|
| 459 |
-
# Group 1: Initial Conditions
|
| 460 |
-
with gr.Accordion("Initial Conditions", open=True):
|
| 461 |
-
distribution_options =
|
| 462 |
-
distribution_type_input = gr.Radio(
|
| 463 |
-
choices=distribution_options, value="Sine Wave (Original)",
|
| 464 |
-
label="Initial Distribution Type", info="Select the initial pattern of the substance."
|
| 465 |
-
)
|
| 466 |
-
|
| 467 |
-
# Group 2: Velocity Fields
|
| 468 |
-
with gr.Accordion("Velocity Fields", open=True):
|
| 469 |
-
velocity_field_options = # Dummy options
|
| 470 |
-
velocity_field_type_input = gr.Radio(
|
| 471 |
-
choices=velocity_field_options, value="Uniform",
|
| 472 |
-
label="Velocity Field Type", info="Select the type of background velocity field."
|
| 473 |
-
)
|
| 474 |
-
ux_slider = gr.Slider(
|
| 475 |
-
minimum=-0.4, maximum=0.4, value=0.2, step=0.01,
|
| 476 |
-
label="Advection Velocity ux", info="x-component of background advection."
|
| 477 |
-
)
|
| 478 |
-
uy_slider = gr.Slider(
|
| 479 |
-
minimum=-0.4, maximum=0.4, value=0.15, step=0.01,
|
| 480 |
-
label="Advection Velocity uy", info="y-component of background advection."
|
| 481 |
-
)
|
| 482 |
-
|
| 483 |
-
run_qlbm_btn = gr.Button("Run QLBM Simulation", variant="primary")
|
| 484 |
-
|
| 485 |
-
with gr.Column(scale=2):
|
| 486 |
-
# Removed gr.Image for GIF
|
| 487 |
-
# qlbm_plot_output = gr.Image(label="QLBM Simulation Animation (GIF)", type="filepath", height=900)
|
| 488 |
-
qlbm_interactive_plot = gr.Plot(label="Interactive Density Plot with Slider")
|
| 489 |
-
|
| 490 |
-
qlbm_inputs_list = [num_reg_qubits_slider, timescale_slider, distribution_type_input, ux_slider, uy_slider, velocity_field_type_input]
|
| 491 |
-
run_qlbm_btn.click(
|
| 492 |
-
fn=qlbm_gradio_interface,
|
| 493 |
-
inputs=qlbm_inputs_list,
|
| 494 |
-
outputs=[qlbm_interactive_plot] # Only interactive plot
|
| 495 |
-
)
|
| 496 |
-
gr.Examples(
|
| 497 |
-
examples=,
|
| 498 |
-
[6, 50, "Gaussian", 0.1, 0.05, "Uniform"],
|
| 499 |
-
,
|
| 500 |
-
inputs=qlbm_inputs_list,
|
| 501 |
-
outputs=[qlbm_interactive_plot], # Only interactive plot
|
| 502 |
-
fn=qlbm_gradio_interface,
|
| 503 |
-
cache_examples=False
|
| 504 |
-
)
|
| 505 |
|
| 506 |
-
|
| 507 |
-
|
| 508 |
-
|
| 509 |
-
|
| 510 |
-
|
| 511 |
-
|
| 512 |
-
|
| 513 |
-
|
| 514 |
-
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|
| 1 |
import math
|
| 2 |
+
|
| 3 |
import tempfile
|
| 4 |
+
|
| 5 |
import gradio as gr
|
| 6 |
+
|
| 7 |
import cudaq
|
| 8 |
+
|
| 9 |
import numpy as np
|
| 10 |
+
|
| 11 |
import cupy as cp
|
| 12 |
+
|
| 13 |
from pathlib import Path
|
| 14 |
+
|
| 15 |
import plotly.graph_objects as go
|
| 16 |
+
|
| 17 |
import plotly.io as pio
|
| 18 |
+
|
| 19 |
+
import imageio
|
| 20 |
+
|
| 21 |
from scipy.spatial import Delaunay
|
| 22 |
|
| 23 |
+
|
| 24 |
+
|
| 25 |
# Set Plotly engine for image export
|
| 26 |
+
|
| 27 |
try:
|
| 28 |
+
|
| 29 |
+
pio.kaleido.scope.mathjax = None
|
| 30 |
+
|
| 31 |
except AttributeError:
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| 32 |
|
| 33 |
+
pass
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|
| 35 |
|
| 36 |
+
|
| 37 |
+
def simulate_qlbm_and_animate(num_reg_qubits: int, T: int, distribution_type: str, ux_input: float, uy_input: float):
|
| 38 |
+
|
| 39 |
+
"""
|
| 40 |
+
|
| 41 |
+
Simulates a 2D advection-diffusion problem using a Quantum Lattice Boltzmann Method (QLBM)
|
| 42 |
+
|
| 43 |
+
and generates a GIF animation and an interactive Plotly figure with a slider for selected time steps.
|
| 44 |
+
|
| 45 |
+
"""
|
| 46 |
+
|
| 47 |
+
video_length = T
|
| 48 |
+
|
| 49 |
+
simulation_fps = 0.1
|
| 50 |
+
|
| 51 |
+
frames = int(simulation_fps * video_length)
|
| 52 |
+
|
| 53 |
+
if frames == 0:
|
| 54 |
+
|
| 55 |
+
frames = 1
|
| 56 |
+
|
| 57 |
+
|
| 58 |
+
|
| 59 |
+
num_anc = 3
|
| 60 |
+
|
| 61 |
+
num_qubits_total = 2 * num_reg_qubits + num_anc
|
| 62 |
+
|
| 63 |
+
current_N = 2**num_reg_qubits
|
| 64 |
+
|
| 65 |
+
N_tot_state_vector = 2**num_qubits_total
|
| 66 |
+
|
| 67 |
+
num_ranks = 1
|
| 68 |
+
|
| 69 |
+
rank = 0
|
| 70 |
+
|
| 71 |
+
N_sub_per_rank = int(N_tot_state_vector // num_ranks)
|
| 72 |
+
|
| 73 |
+
|
| 74 |
+
|
| 75 |
+
timesteps_per_frame = 1
|
| 76 |
+
|
| 77 |
+
if frames < T and frames > 0:
|
| 78 |
+
|
| 79 |
+
timesteps_per_frame = int(T / frames)
|
| 80 |
+
|
| 81 |
+
if timesteps_per_frame == 0:
|
| 82 |
+
|
| 83 |
+
timesteps_per_frame = 1
|
| 84 |
+
|
| 85 |
+
|
| 86 |
+
|
| 87 |
+
# Initial state setup
|
| 88 |
+
|
| 89 |
+
if distribution_type == "Sine Wave (Original)":
|
| 90 |
+
|
| 91 |
+
selected_initial_state_function_raw = lambda x, y, N_val_func: \
|
| 92 |
+
|
| 93 |
+
np.sin(x * 2 * np.pi / N_val_func) * (1 - 0.5 * x / N_val_func) * \
|
| 94 |
+
|
| 95 |
+
np.sin(y * 4 * np.pi / N_val_func) * (1 - 0.5 * y / N_val_func) + 1
|
| 96 |
+
|
| 97 |
+
elif distribution_type == "Gaussian":
|
| 98 |
+
|
| 99 |
+
selected_initial_state_function_raw = lambda x, y, N_val_func: \
|
| 100 |
+
|
| 101 |
+
np.exp(-((x - N_val_func / 2)**2 / (2 * (N_val_func / 5)**2) +
|
| 102 |
+
|
| 103 |
+
(y - N_val_func / 2)**2 / (2 * (N_val_func / 5)**2))) * 1.8 + 0.2
|
| 104 |
+
|
| 105 |
+
elif distribution_type == "Random":
|
| 106 |
+
|
| 107 |
+
selected_initial_state_function_raw = lambda x, y, N_val_func: \
|
| 108 |
+
|
| 109 |
+
np.random.rand(N_val_func, N_val_func) * 1.5 + 0.2 if isinstance(x, int) else \
|
| 110 |
+
|
| 111 |
+
np.random.rand(x.shape[0], x.shape[1]) * 1.5 + 0.2
|
| 112 |
+
|
| 113 |
+
else:
|
| 114 |
+
|
| 115 |
+
print(f"Warning: Unknown distribution type '{distribution_type}'. Defaulting to Sine Wave.")
|
| 116 |
+
|
| 117 |
+
selected_initial_state_function_raw = lambda x, y, N_val_func: \
|
| 118 |
+
|
| 119 |
+
np.sin(x * 2 * np.pi / N_val_func) * (1 - 0.5 * x / N_val_func) * \
|
| 120 |
+
|
| 121 |
+
np.sin(y * 4 * np.pi / N_val_func) * (1 - 0.5 * y / N_val_func) + 1
|
| 122 |
+
|
| 123 |
+
|
| 124 |
+
|
| 125 |
+
initial_state_func_eval = lambda x_coords, y_coords: \
|
| 126 |
+
|
| 127 |
+
selected_initial_state_function_raw(x_coords, y_coords, current_N) * \
|
| 128 |
+
|
| 129 |
+
(y_coords < current_N).astype(int)
|
| 130 |
+
|
| 131 |
+
|
| 132 |
+
|
| 133 |
+
with tempfile.TemporaryDirectory() as tmp_npy_dir:
|
| 134 |
+
|
| 135 |
+
intermediate_folder_path = Path(tmp_npy_dir)
|
| 136 |
+
|
| 137 |
+
|
| 138 |
+
|
| 139 |
+
cudaq.set_target('nvidia', option='fp64')
|
| 140 |
+
|
| 141 |
+
|
| 142 |
+
|
| 143 |
+
@cudaq.kernel
|
| 144 |
+
|
| 145 |
+
def alloc_kernel(num_qubits_alloc: int):
|
| 146 |
+
|
| 147 |
+
qubits = cudaq.qvector(num_qubits_alloc)
|
| 148 |
+
|
| 149 |
+
|
| 150 |
+
|
| 151 |
+
from cupy.cuda.memory import MemoryPointer, UnownedMemory
|
| 152 |
+
|
| 153 |
+
|
| 154 |
+
|
| 155 |
+
def to_cupy_array(state):
|
| 156 |
+
|
| 157 |
+
tensor = state.getTensor()
|
| 158 |
+
|
| 159 |
+
pDevice = tensor.data()
|
| 160 |
+
|
| 161 |
+
sizeByte = tensor.get_num_elements() * tensor.get_element_size()
|
| 162 |
+
|
| 163 |
+
mem = UnownedMemory(pDevice, sizeByte, owner=state)
|
| 164 |
+
|
| 165 |
+
memptr_obj = MemoryPointer(mem, 0)
|
| 166 |
+
|
| 167 |
+
cupy_array_val = cp.ndarray(tensor.get_num_elements(),
|
| 168 |
+
|
| 169 |
+
dtype=cp.complex128,
|
| 170 |
+
|
| 171 |
+
memptr=memptr_obj)
|
| 172 |
+
|
| 173 |
+
return cupy_array_val
|
| 174 |
+
|
| 175 |
+
|
| 176 |
+
|
| 177 |
+
class QLBMAdvecDiffD2Q5_new:
|
| 178 |
+
|
| 179 |
+
def __init__(self, ux=0.2, uy=0.15) -> None:
|
| 180 |
+
|
| 181 |
+
self.dim = 2
|
| 182 |
+
|
| 183 |
+
self.ndir = 5
|
| 184 |
+
|
| 185 |
+
self.nq_dir = math.ceil(np.log2(self.ndir))
|
| 186 |
+
|
| 187 |
+
self.dirs = []
|
| 188 |
+
|
| 189 |
+
for dir_int in range(self.ndir):
|
| 190 |
+
|
| 191 |
+
dir_bin = f"{dir_int:b}".zfill(self.nq_dir)
|
| 192 |
+
|
| 193 |
+
self.dirs.append(dir_bin)
|
| 194 |
+
|
| 195 |
+
self.e_unitvec = np.array([0, 1, -1, 1, -1])
|
| 196 |
+
|
| 197 |
+
self.wts = np.array([2/6, 1/6, 1/6, 1/6, 1/6])
|
| 198 |
+
|
| 199 |
+
self.cs = 1 / np.sqrt(3)
|
| 200 |
+
|
| 201 |
+
self.ux = ux
|
| 202 |
+
|
| 203 |
+
self.uy = uy
|
| 204 |
+
|
| 205 |
+
self.u = np.array([0, self.ux, self.ux, self.uy, self.uy])
|
| 206 |
+
|
| 207 |
+
self.wtcoeffs = np.multiply(self.wts, 1 + self.e_unitvec * self.u / self.cs**2)
|
| 208 |
+
|
| 209 |
+
self.create_circuit()
|
| 210 |
+
|
| 211 |
+
|
| 212 |
+
|
| 213 |
+
def create_circuit(self):
|
| 214 |
+
|
| 215 |
+
v = np.pad(self.wtcoeffs, (0, 2**num_anc - self.ndir))
|
| 216 |
+
|
| 217 |
+
v = v**0.5
|
| 218 |
+
|
| 219 |
+
v[0] += 1
|
| 220 |
+
|
| 221 |
+
v = v / np.linalg.norm(v)
|
| 222 |
+
|
| 223 |
+
U_prep = 2 * np.outer(v, v) - np.eye(len(v))
|
| 224 |
+
|
| 225 |
+
cudaq.register_operation("prep_op", U_prep)
|
| 226 |
+
|
| 227 |
+
|
| 228 |
+
|
| 229 |
+
def collisionOp(dirs_list):
|
| 230 |
+
|
| 231 |
+
dirs_i_list_val = []
|
| 232 |
+
|
| 233 |
+
for dir_str in dirs_list:
|
| 234 |
+
|
| 235 |
+
dirs_i = [(int(c)) for c in dir_str]
|
| 236 |
+
|
| 237 |
+
dirs_i_list_val += dirs_i[::-1]
|
| 238 |
+
|
| 239 |
+
return dirs_i_list_val
|
| 240 |
+
|
| 241 |
+
|
| 242 |
+
|
| 243 |
+
self.dirs_i_list = collisionOp(self.dirs)
|
| 244 |
+
|
| 245 |
+
|
| 246 |
+
|
| 247 |
+
@cudaq.kernel
|
| 248 |
+
|
| 249 |
+
def rshift(q: cudaq.qview, n: int):
|
| 250 |
+
|
| 251 |
+
for i in range(n):
|
| 252 |
+
|
| 253 |
+
if i == n - 1:
|
| 254 |
+
|
| 255 |
+
x(q[n - 1 - i])
|
| 256 |
+
|
| 257 |
+
elif i == n - 2:
|
| 258 |
+
|
| 259 |
+
x.ctrl(q[n - 1 - (i + 1)], q[n - 1 - i])
|
| 260 |
+
|
| 261 |
+
else:
|
| 262 |
+
|
| 263 |
+
x.ctrl(q[0:n - 1 - i], q[n - 1 - i])
|
| 264 |
+
|
| 265 |
+
|
| 266 |
+
|
| 267 |
+
@cudaq.kernel
|
| 268 |
+
|
| 269 |
+
def lshift(q: cudaq.qview, n: int):
|
| 270 |
+
|
| 271 |
+
for i in range(n):
|
| 272 |
+
|
| 273 |
+
if i == 0:
|
| 274 |
+
|
| 275 |
+
x(q[0])
|
| 276 |
+
|
| 277 |
+
elif i == 1:
|
| 278 |
+
|
| 279 |
+
x.ctrl(q[0], q[1])
|
| 280 |
+
|
| 281 |
+
else:
|
| 282 |
+
|
| 283 |
+
x.ctrl(q[0:i], q[i])
|
| 284 |
+
|
| 285 |
+
|
| 286 |
+
|
| 287 |
+
@cudaq.kernel
|
| 288 |
+
|
| 289 |
+
def d2q5_tstep(q: cudaq.qview, nqx: int, nqy: int, nq_dir_val: int, dirs_i_val: list[int]):
|
| 290 |
+
|
| 291 |
+
qx = q[0:nqx]
|
| 292 |
+
|
| 293 |
+
qy = q[nqx:nqx + nqy]
|
| 294 |
+
|
| 295 |
+
qdir = q[nqx + nqy:nqx + nqy + nq_dir_val]
|
| 296 |
+
|
| 297 |
+
|
| 298 |
+
|
| 299 |
+
idx_lqx = 2
|
| 300 |
+
|
| 301 |
+
b_list = dirs_i_val[idx_lqx * nq_dir_val:(idx_lqx + 1) * nq_dir_val]
|
| 302 |
+
|
| 303 |
+
for j in range(nq_dir_val):
|
| 304 |
+
|
| 305 |
+
if b_list[j] == 0: x(qdir[j])
|
| 306 |
+
|
| 307 |
+
cudaq.control(lshift, qdir, qx, nqx)
|
| 308 |
+
|
| 309 |
+
for j in range(nq_dir_val):
|
| 310 |
+
|
| 311 |
+
if b_list[j] == 0: x(qdir[j])
|
| 312 |
+
|
| 313 |
+
|
| 314 |
+
|
| 315 |
+
idx_rqx = 1
|
| 316 |
+
|
| 317 |
+
b_list = dirs_i_val[idx_rqx * nq_dir_val:(idx_rqx + 1) * nq_dir_val]
|
| 318 |
+
|
| 319 |
+
for j in range(nq_dir_val):
|
| 320 |
+
|
| 321 |
+
if b_list[j] == 0: x(qdir[j])
|
| 322 |
+
|
| 323 |
+
cudaq.control(rshift, qdir, qx, nqx)
|
| 324 |
+
|
| 325 |
+
for j in range(nq_dir_val):
|
| 326 |
+
|
| 327 |
+
if b_list[j] == 0: x(qdir[j])
|
| 328 |
+
|
| 329 |
+
|
| 330 |
+
|
| 331 |
+
idx_lqy = 4
|
| 332 |
+
|
| 333 |
+
b_list = dirs_i_val[idx_lqy * nq_dir_val:(idx_lqy + 1) * nq_dir_val]
|
| 334 |
+
|
| 335 |
+
for j in range(nq_dir_val):
|
| 336 |
+
|
| 337 |
+
if b_list[j] == 0: x(qdir[j])
|
| 338 |
+
|
| 339 |
+
cudaq.control(lshift, qdir, qy, nqy)
|
| 340 |
+
|
| 341 |
+
for j in range(nq_dir_val):
|
| 342 |
+
|
| 343 |
+
if b_list[j] == 0: x(qdir[j])
|
| 344 |
+
|
| 345 |
+
|
| 346 |
+
|
| 347 |
+
idx_rqy = 3
|
| 348 |
+
|
| 349 |
+
b_list = dirs_i_val[idx_rqy * nq_dir_val:(idx_rqy + 1) * nq_dir_val]
|
| 350 |
+
|
| 351 |
+
for j in range(nq_dir_val):
|
| 352 |
+
|
| 353 |
+
if b_list[j] == 0: x(qdir[j])
|
| 354 |
+
|
| 355 |
+
cudaq.control(rshift, qdir, qy, nqy)
|
| 356 |
+
|
| 357 |
+
for j in range(nq_dir_val):
|
| 358 |
+
|
| 359 |
+
if b_list[j] == 0: x(qdir[j])
|
| 360 |
+
|
| 361 |
+
|
| 362 |
+
|
| 363 |
+
@cudaq.kernel
|
| 364 |
+
|
| 365 |
+
def d2q5_tstep_wrapper(state_arg: cudaq.State, nqx: int, nqy: int, nq_dir_val: int, dirs_i_val: list[int]):
|
| 366 |
+
|
| 367 |
+
q = cudaq.qvector(state_arg)
|
| 368 |
+
|
| 369 |
+
qdir = q[nqx + nqy:nqx + nqy + nq_dir_val]
|
| 370 |
+
|
| 371 |
+
prep_op(qdir[2], qdir[1], qdir[0])
|
| 372 |
+
|
| 373 |
+
d2q5_tstep(q, nqx, nqy, nq_dir_val, dirs_i_val)
|
| 374 |
+
|
| 375 |
+
prep_op(qdir[2], qdir[1], qdir[0])
|
| 376 |
+
|
| 377 |
+
|
| 378 |
+
|
| 379 |
+
@cudaq.kernel
|
| 380 |
+
|
| 381 |
+
def d2q5_tstep_wrapper_hadamard(vec_arg: list[complex], nqx: int, nqy: int, nq_dir_val: int, dirs_i_val: list[int]):
|
| 382 |
+
|
| 383 |
+
q = cudaq.qvector(vec_arg)
|
| 384 |
+
|
| 385 |
+
qdir = q[nqx + nqy:nqx + nqy + nq_dir_val]
|
| 386 |
+
|
| 387 |
+
qy = q[nqx:nqx + nqy]
|
| 388 |
+
|
| 389 |
+
prep_op(qdir[2], qdir[1], qdir[0])
|
| 390 |
+
|
| 391 |
+
d2q5_tstep(q, nqx, nqy, nq_dir_val, dirs_i_val)
|
| 392 |
+
|
| 393 |
+
prep_op(qdir[2], qdir[1], qdir[0])
|
| 394 |
+
|
| 395 |
+
for i in range(nqy):
|
| 396 |
+
|
| 397 |
+
h(qy[i])
|
| 398 |
+
|
| 399 |
+
|
| 400 |
+
|
| 401 |
+
def run_timestep_func(vec_arg, hadamard=False):
|
| 402 |
+
|
| 403 |
+
if hadamard:
|
| 404 |
+
|
| 405 |
+
result = cudaq.get_state(d2q5_tstep_wrapper_hadamard, vec_arg, num_reg_qubits, num_reg_qubits, self.nq_dir, self.dirs_i_list)
|
| 406 |
+
|
| 407 |
+
else:
|
| 408 |
+
|
| 409 |
+
result = cudaq.get_state(d2q5_tstep_wrapper, vec_arg, num_reg_qubits, num_reg_qubits, self.nq_dir, self.dirs_i_list)
|
| 410 |
+
|
| 411 |
+
num_nonzero_ranks = num_ranks / (2**num_anc)
|
| 412 |
+
|
| 413 |
+
rank_slice_cupy = to_cupy_array(result)
|
| 414 |
+
|
| 415 |
+
if rank >= num_nonzero_ranks and num_nonzero_ranks > 0:
|
| 416 |
+
|
| 417 |
+
sub_sv_zeros = np.zeros(N_sub_per_rank, dtype=np.complex128)
|
| 418 |
+
|
| 419 |
+
cp.cuda.runtime.memcpy(rank_slice_cupy.data.ptr, sub_sv_zeros.ctypes.data, sub_sv_zeros.nbytes, cp.cuda.runtime.memcpyHostToDevice)
|
| 420 |
+
|
| 421 |
+
if rank == 0 and num_nonzero_ranks < 1 and N_sub_per_rank > 0:
|
| 422 |
+
|
| 423 |
+
limit_idx = int(N_tot_state_vector / (2**num_anc))
|
| 424 |
+
|
| 425 |
+
if limit_idx < rank_slice_cupy.size:
|
| 426 |
+
|
| 427 |
+
rank_slice_cupy[limit_idx:] = 0
|
| 428 |
+
|
| 429 |
+
return result
|
| 430 |
+
|
| 431 |
+
self.run_timestep = run_timestep_func
|
| 432 |
+
|
| 433 |
+
|
| 434 |
+
|
| 435 |
+
def write_state(self, state_to_write, t_step_str_val):
|
| 436 |
+
|
| 437 |
+
rank_slice_cupy = to_cupy_array(state_to_write)
|
| 438 |
+
|
| 439 |
+
num_nonzero_ranks = num_ranks / (2**num_anc)
|
| 440 |
+
|
| 441 |
+
if rank < num_nonzero_ranks or (rank == 0 and num_nonzero_ranks <= 0):
|
| 442 |
+
|
| 443 |
+
save_path = intermediate_folder_path / f"{t_step_str_val}_{rank}.npy"
|
| 444 |
+
|
| 445 |
+
with open(save_path, 'wb') as f:
|
| 446 |
+
|
| 447 |
+
arr_to_save = None
|
| 448 |
+
|
| 449 |
+
data_limit = N_sub_per_rank
|
| 450 |
+
|
| 451 |
+
if num_nonzero_ranks < 1 and rank == 0:
|
| 452 |
+
|
| 453 |
+
data_limit = int(N_tot_state_vector / (2**num_anc))
|
| 454 |
+
|
| 455 |
+
if data_limit > 0:
|
| 456 |
+
|
| 457 |
+
relevant_part_cupy = cp.real(rank_slice_cupy[:data_limit])
|
| 458 |
+
|
| 459 |
+
else:
|
| 460 |
+
|
| 461 |
+
relevant_part_cupy = cp.array([], dtype=cp.float64)
|
| 462 |
+
|
| 463 |
+
if relevant_part_cupy.size >= current_N * current_N:
|
| 464 |
+
|
| 465 |
+
arr_flat = relevant_part_cupy[:current_N * current_N]
|
| 466 |
+
|
| 467 |
+
if downsampling_factor > 1 and current_N > 0:
|
| 468 |
+
|
| 469 |
+
arr_reshaped = arr_flat.reshape((current_N, current_N))
|
| 470 |
+
|
| 471 |
+
arr_downsampled = arr_reshaped[::downsampling_factor, ::downsampling_factor]
|
| 472 |
+
|
| 473 |
+
arr_to_save = arr_downsampled.flatten()
|
| 474 |
+
|
| 475 |
+
else:
|
| 476 |
+
|
| 477 |
+
arr_to_save = arr_flat
|
| 478 |
+
|
| 479 |
+
elif relevant_part_cupy.size > 0:
|
| 480 |
+
|
| 481 |
+
if downsampling_factor > 1:
|
| 482 |
+
|
| 483 |
+
arr_to_save = relevant_part_cupy[::downsampling_factor]
|
| 484 |
+
|
| 485 |
+
else:
|
| 486 |
+
|
| 487 |
+
arr_to_save = relevant_part_cupy
|
| 488 |
+
|
| 489 |
+
if arr_to_save is not None and arr_to_save.size > 0:
|
| 490 |
+
|
| 491 |
+
np.save(f, arr_to_save.get() if isinstance(arr_to_save, cp.ndarray) else arr_to_save)
|
| 492 |
+
|
| 493 |
+
|
| 494 |
+
|
| 495 |
+
def run_evolution(self, initial_state_arg, total_timesteps, observable=False):
|
| 496 |
+
|
| 497 |
+
current_state_val = initial_state_arg
|
| 498 |
+
|
| 499 |
+
for t_iter in range(total_timesteps):
|
| 500 |
+
|
| 501 |
+
next_state_val = None
|
| 502 |
+
|
| 503 |
+
if t_iter == total_timesteps - 1 and observable:
|
| 504 |
+
|
| 505 |
+
next_state_val = self.run_timestep(current_state_val, True)
|
| 506 |
+
|
| 507 |
+
self.write_state(next_state_val, str(t_iter + 1) + "_h")
|
| 508 |
+
|
| 509 |
+
else:
|
| 510 |
+
|
| 511 |
+
next_state_val = self.run_timestep(current_state_val)
|
| 512 |
+
|
| 513 |
+
# Save data at specific intervals for static plots
|
| 514 |
+
|
| 515 |
+
if t_iter == 0 or t_iter == total_timesteps // 4 or t_iter == 3 * total_timesteps // 4 or t_iter == total_timesteps - 1 or (t_iter + 1) % timesteps_per_frame == 0:
|
| 516 |
+
|
| 517 |
+
self.write_state(next_state_val, str(t_iter + 1))
|
| 518 |
+
|
| 519 |
+
if rank == 0:
|
| 520 |
+
|
| 521 |
+
print(f"Timestep: {t_iter + 1}/{total_timesteps}")
|
| 522 |
+
|
| 523 |
+
cp.get_default_memory_pool().free_all_blocks()
|
| 524 |
+
|
| 525 |
+
current_state_val = next_state_val
|
| 526 |
+
|
| 527 |
+
if rank == 0:
|
| 528 |
+
|
| 529 |
+
print(f"Timestep: {total_timesteps}/{total_timesteps} (Evolution complete)")
|
| 530 |
+
|
| 531 |
+
cp.get_default_memory_pool().free_all_blocks()
|
| 532 |
+
|
| 533 |
+
self.final_state = current_state_val
|
| 534 |
+
|
| 535 |
+
|
| 536 |
+
|
| 537 |
+
downsampling_factor = 2**5
|
| 538 |
+
|
| 539 |
+
if current_N == 0:
|
| 540 |
+
|
| 541 |
+
print("Error: current_N is zero. num_reg_qubits likely too small.")
|
| 542 |
+
|
| 543 |
+
return None, None
|
| 544 |
+
|
| 545 |
+
if current_N < downsampling_factor:
|
| 546 |
+
|
| 547 |
+
downsampling_factor = current_N if current_N > 0 else 1
|
| 548 |
+
|
| 549 |
+
|
| 550 |
+
|
| 551 |
+
qlbm_obj = QLBMAdvecDiffD2Q5_new(ux=ux_input, uy=uy_input)
|
| 552 |
+
|
| 553 |
+
initial_state_val = cudaq.get_state(alloc_kernel, num_qubits_total)
|
| 554 |
+
|
| 555 |
+
|
| 556 |
+
|
| 557 |
+
xv_init = np.arange(current_N)
|
| 558 |
+
|
| 559 |
+
yv_init = np.arange(current_N)
|
| 560 |
+
|
| 561 |
+
initial_grid_2d_X, initial_grid_2d_Y = np.meshgrid(xv_init, yv_init)
|
| 562 |
+
|
| 563 |
+
|
| 564 |
+
|
| 565 |
+
if distribution_type == "Random":
|
| 566 |
+
|
| 567 |
+
initial_grid_2d = selected_initial_state_function_raw(current_N, current_N, current_N)
|
| 568 |
+
|
| 569 |
+
else:
|
| 570 |
+
|
| 571 |
+
initial_grid_2d = initial_state_func_eval(initial_grid_2d_X, initial_grid_2d_Y)
|
| 572 |
+
|
| 573 |
+
|
| 574 |
+
|
| 575 |
+
sub_sv_init_flat = initial_grid_2d.flatten().astype(np.complex128)
|
| 576 |
+
|
| 577 |
+
full_initial_sv_host = np.zeros(N_sub_per_rank, dtype=np.complex128)
|
| 578 |
+
|
| 579 |
+
num_computational_states = current_N * current_N
|
| 580 |
+
|
| 581 |
+
|
| 582 |
+
|
| 583 |
+
if len(sub_sv_init_flat) == num_computational_states:
|
| 584 |
+
|
| 585 |
+
if num_computational_states <= N_sub_per_rank:
|
| 586 |
+
|
| 587 |
+
full_initial_sv_host[:num_computational_states] = sub_sv_init_flat
|
| 588 |
+
|
| 589 |
+
else:
|
| 590 |
+
|
| 591 |
+
print(f"Error: Grid data {num_computational_states} > N_sub_per_rank {N_sub_per_rank}")
|
| 592 |
+
|
| 593 |
+
return None, None
|
| 594 |
+
|
| 595 |
+
else:
|
| 596 |
+
|
| 597 |
+
print(f"Warning: Initial state size {len(sub_sv_init_flat)} != expected {num_computational_states}")
|
| 598 |
+
|
| 599 |
+
fill_len = min(len(sub_sv_init_flat), num_computational_states, N_sub_per_rank)
|
| 600 |
+
|
| 601 |
+
full_initial_sv_host[:fill_len] = sub_sv_init_flat[:fill_len]
|
| 602 |
+
|
| 603 |
+
|
| 604 |
+
|
| 605 |
+
rank_slice_init = to_cupy_array(initial_state_val)
|
| 606 |
+
|
| 607 |
+
print(f'Rank {rank}: Initializing state with {distribution_type} (ux={ux_input}, uy={uy_input})...')
|
| 608 |
+
|
| 609 |
+
cp.cuda.runtime.memcpy(rank_slice_init.data.ptr, full_initial_sv_host.ctypes.data, full_initial_sv_host.nbytes, cp.cuda.runtime.memcpyHostToDevice)
|
| 610 |
+
|
| 611 |
+
print(f'Rank {rank}: Initial state copied. Size: {len(sub_sv_init_flat)}. N_sub_per_rank: {N_sub_per_rank}')
|
| 612 |
+
|
| 613 |
+
|
| 614 |
+
|
| 615 |
+
print("Starting QLBM evolution...")
|
| 616 |
+
|
| 617 |
+
qlbm_obj.run_evolution(initial_state_val, T)
|
| 618 |
+
|
| 619 |
+
print("QLBM evolution complete.")
|
| 620 |
+
|
| 621 |
+
|
| 622 |
+
|
| 623 |
+
print("Generating animation and plots with Plotly...")
|
| 624 |
+
|
| 625 |
+
downsampled_N = current_N // downsampling_factor
|
| 626 |
+
|
| 627 |
+
if downsampled_N == 0 and current_N > 0:
|
| 628 |
+
|
| 629 |
+
downsampled_N = 1
|
| 630 |
+
|
| 631 |
+
elif current_N == 0:
|
| 632 |
+
|
| 633 |
+
print("Error: current_N is zero before Plotly stage.")
|
| 634 |
+
|
| 635 |
+
return None, None
|
| 636 |
+
|
| 637 |
+
|
| 638 |
+
|
| 639 |
+
# Load data for specific time steps for static plots
|
| 640 |
+
|
| 641 |
+
time_steps = [0, T//4, 3*T//4, T]
|
| 642 |
+
|
| 643 |
+
data_frames = []
|
| 644 |
+
|
| 645 |
+
actual_timesteps = []
|
| 646 |
+
|
| 647 |
+
for t in time_steps:
|
| 648 |
+
|
| 649 |
+
file_path = intermediate_folder_path / f"{t}_{rank}.npy"
|
| 650 |
+
|
| 651 |
+
if file_path.exists():
|
| 652 |
+
|
| 653 |
+
sol_loaded = np.load(file_path)
|
| 654 |
+
|
| 655 |
+
if sol_loaded.size == downsampled_N * downsampled_N:
|
| 656 |
+
|
| 657 |
+
Z_data = np.reshape(sol_loaded, (downsampled_N, downsampled_N))
|
| 658 |
+
|
| 659 |
+
data_frames.append(Z_data)
|
| 660 |
+
|
| 661 |
+
actual_timesteps.append(t)
|
| 662 |
+
|
| 663 |
+
else:
|
| 664 |
+
|
| 665 |
+
print(f"Warning: File {file_path} size {sol_loaded.size} != expected {downsampled_N*downsampled_N}. Skipping.")
|
| 666 |
+
|
| 667 |
+
else:
|
| 668 |
+
|
| 669 |
+
print(f"Warning: File {file_path} not found. Skipping.")
|
| 670 |
+
|
| 671 |
+
|
| 672 |
+
|
| 673 |
+
if not data_frames:
|
| 674 |
+
|
| 675 |
+
print("Error: No data frames loaded for static plots.")
|
| 676 |
+
|
| 677 |
+
return None, None
|
| 678 |
+
|
| 679 |
+
|
| 680 |
+
|
| 681 |
+
x_coords_plot = np.linspace(-10, 10, downsampled_N)
|
| 682 |
+
|
| 683 |
+
y_coords_plot = np.linspace(-10, 10, downsampled_N)
|
| 684 |
+
|
| 685 |
+
|
| 686 |
+
|
| 687 |
+
# Calculate global min/max for consistent scaling
|
| 688 |
+
|
| 689 |
+
z_min = min([np.min(Z) for Z in data_frames])
|
| 690 |
+
|
| 691 |
+
z_max = max([np.max(Z) for Z in data_frames])
|
| 692 |
+
|
| 693 |
+
if z_max == z_min:
|
| 694 |
+
|
| 695 |
+
z_max += 1e-9
|
| 696 |
+
|
| 697 |
+
|
| 698 |
+
|
| 699 |
+
# Create interactive Plotly figure with slider
|
| 700 |
+
|
| 701 |
+
fig = go.Figure()
|
| 702 |
+
|
| 703 |
+
|
| 704 |
+
|
| 705 |
+
for i, Z in enumerate(data_frames):
|
| 706 |
+
|
| 707 |
+
fig.add_trace(
|
| 708 |
+
|
| 709 |
+
go.Surface(
|
| 710 |
+
|
| 711 |
+
z=Z, x=x_coords_plot, y=y_coords_plot,
|
| 712 |
+
|
| 713 |
+
colorscale='Viridis',
|
| 714 |
+
|
| 715 |
+
cmin=z_min, cmax=z_max,
|
| 716 |
+
|
| 717 |
+
name=f'Time: {actual_timesteps[i]}',
|
| 718 |
+
|
| 719 |
+
showscale=(i == 0)
|
| 720 |
+
|
| 721 |
+
)
|
| 722 |
+
|
| 723 |
+
)
|
| 724 |
+
|
| 725 |
+
|
| 726 |
+
|
| 727 |
+
steps = []
|
| 728 |
+
|
| 729 |
+
for i in range(len(data_frames)):
|
| 730 |
+
|
| 731 |
+
step = dict(
|
| 732 |
+
|
| 733 |
+
method="update",
|
| 734 |
+
|
| 735 |
+
args=[{"visible": [False] * len(data_frames)}],
|
| 736 |
+
|
| 737 |
+
label=f"Time: {actual_timesteps[i]}"
|
| 738 |
+
|
| 739 |
+
)
|
| 740 |
+
|
| 741 |
+
step["args"][0]["visible"][i] = True
|
| 742 |
+
|
| 743 |
+
steps.append(step)
|
| 744 |
+
|
| 745 |
+
|
| 746 |
+
|
| 747 |
+
sliders = [dict(active=0, currentvalue={"prefix": "Time: "}, pad={"t": 50}, steps=steps)]
|
| 748 |
+
|
| 749 |
+
|
| 750 |
+
|
| 751 |
+
fig.update_layout(
|
| 752 |
+
|
| 753 |
+
title='QLBM Simulation - Density Evolution',
|
| 754 |
+
|
| 755 |
+
scene=dict(
|
| 756 |
+
|
| 757 |
+
xaxis_title='X',
|
| 758 |
+
|
| 759 |
+
yaxis_title='Y',
|
| 760 |
+
|
| 761 |
+
zaxis_title='Density',
|
| 762 |
+
|
| 763 |
+
xaxis=dict(range=[x_coords_plot[0], x_coords_plot[-1]]),
|
| 764 |
+
|
| 765 |
+
yaxis=dict(range=[y_coords_plot[0], y_coords_plot[-1]]),
|
| 766 |
+
|
| 767 |
+
zaxis=dict(range=[z_min, z_max]),
|
| 768 |
+
|
| 769 |
+
),
|
| 770 |
+
|
| 771 |
+
sliders=sliders,
|
| 772 |
+
|
| 773 |
+
width=800,
|
| 774 |
+
|
| 775 |
+
height=700
|
| 776 |
+
|
| 777 |
+
)
|
| 778 |
+
|
| 779 |
+
|
| 780 |
+
|
| 781 |
+
# Generate GIF (unchanged from original)
|
| 782 |
+
|
| 783 |
+
plotted_timesteps_str = sorted(list(set([str(t) for t in range(0, T + 1, timesteps_per_frame) if (intermediate_folder_path / f"{t}_{rank}.npy").exists()] + ['0'] if T == 0 else [])), key=lambda k_str: int(k_str))
|
| 784 |
+
|
| 785 |
+
data_frames_list = []
|
| 786 |
+
|
| 787 |
+
actual_timesteps_for_title = []
|
| 788 |
+
|
| 789 |
+
for i_str_val in plotted_timesteps_str:
|
| 790 |
+
|
| 791 |
+
file_path_load = intermediate_folder_path / f"{i_str_val}_{rank}.npy"
|
| 792 |
+
|
| 793 |
+
if file_path_load.exists():
|
| 794 |
+
|
| 795 |
+
sol_loaded = np.load(file_path_load)
|
| 796 |
+
|
| 797 |
+
if sol_loaded.size == downsampled_N * downsampled_N:
|
| 798 |
+
|
| 799 |
+
Z_data = np.reshape(sol_loaded, (downsampled_N, downsampled_N))
|
| 800 |
+
|
| 801 |
+
data_frames_list.append(Z_data)
|
| 802 |
+
|
| 803 |
+
actual_timesteps_for_title.append(i_str_val)
|
| 804 |
+
|
| 805 |
+
|
| 806 |
+
|
| 807 |
+
if not data_frames_list:
|
| 808 |
+
|
| 809 |
+
print("Error: No data frames loaded for GIF.")
|
| 810 |
+
|
| 811 |
+
return None, None
|
| 812 |
+
|
| 813 |
+
|
| 814 |
+
|
| 815 |
+
norm_factor_plotly = np.max(np.abs(data_frames_list[0])) if data_frames_list[0].size > 0 else 1.0
|
| 816 |
+
|
| 817 |
+
all_data_max_val = max([np.max(np.abs(d_frame)) for d_frame in data_frames_list]) if data_frames_list else norm_factor_plotly
|
| 818 |
+
|
| 819 |
+
clim_upper_plotly = (all_data_max_val / norm_factor_plotly) * 1.0 or 0.6
|
| 820 |
+
|
| 821 |
+
|
| 822 |
+
|
| 823 |
+
results_base_dir = "Results"
|
| 824 |
+
|
| 825 |
+
gif_frames_for_naming = int(simulation_fps * T) or 1
|
| 826 |
+
|
| 827 |
+
dist_name_part = distribution_type.replace(' ','').replace('(Original)','').replace('(','').replace(')','')
|
| 828 |
+
|
| 829 |
+
specific_folder_name = f"d2q5_plotly_N{current_N}_T{T}_fr{gif_frames_for_naming}_dist{dist_name_part}_ux{ux_input:.2f}_uy{uy_input:.2f}"
|
| 830 |
+
|
| 831 |
+
final_output_dir = Path(results_base_dir) / specific_folder_name
|
| 832 |
+
|
| 833 |
+
os.makedirs(final_output_dir, exist_ok=True)
|
| 834 |
+
|
| 835 |
+
gif_path_to_return = final_output_dir / "animation_plotly.gif"
|
| 836 |
+
|
| 837 |
+
|
| 838 |
+
|
| 839 |
+
Z_initial_placeholder = np.zeros((downsampled_N, downsampled_N))
|
| 840 |
+
|
| 841 |
+
gif_fig = go.Figure(data=[go.Surface(
|
| 842 |
+
|
| 843 |
+
z=Z_initial_placeholder, x=x_coords_plot, y=y_coords_plot,
|
| 844 |
+
|
| 845 |
+
colorscale='Viridis', cmin=0, cmax=clim_upper_plotly,
|
| 846 |
+
|
| 847 |
+
colorbar=dict(title=dict(text='Density', side='right', font=dict(color='white')),
|
| 848 |
+
|
| 849 |
+
tickfont=dict(size=10, color='white'), bgcolor='rgba(0,0,0,0.4)',
|
| 850 |
+
|
| 851 |
+
bordercolor='gray', outlinewidth=1, thickness=20, len=0.8, x=0.85, y=0.5))])
|
| 852 |
+
|
| 853 |
+
|
| 854 |
+
|
| 855 |
+
gif_fig.update_layout(
|
| 856 |
+
|
| 857 |
+
paper_bgcolor='black', plot_bgcolor='black', font=dict(color='white'),
|
| 858 |
+
|
| 859 |
+
scene=dict(
|
| 860 |
+
|
| 861 |
+
bgcolor='black',
|
| 862 |
+
|
| 863 |
+
xaxis=dict(title=dict(text='X Axis', font=dict(color='white')), tickfont=dict(color='white'),
|
| 864 |
+
|
| 865 |
+
gridcolor='rgba(128,128,128,0.3)', zerolinecolor='rgba(128,128,128,0.5)', linecolor='rgba(128,128,128,0.5)'),
|
| 866 |
+
|
| 867 |
+
yaxis=dict(title=dict(text='Y Axis', font=dict(color='white')), tickfont=dict(color='white'),
|
| 868 |
+
|
| 869 |
+
gridcolor='rgba(128,128,128,0.3)', zerolinecolor='rgba(128,128,128,0.5)', linecolor='rgba(128,128,128,0.5)'),
|
| 870 |
+
|
| 871 |
+
zaxis=dict(title=dict(text='Density', font=dict(color='white')), tickfont=dict(color='white'),
|
| 872 |
+
|
| 873 |
+
range=[0, clim_upper_plotly], gridcolor='rgba(128,128,128,0.3)',
|
| 874 |
+
|
| 875 |
+
zerolinecolor='rgba(128,128,128,0.5)', linecolor='rgba(128,128,128,0.5)'),
|
| 876 |
+
|
| 877 |
+
aspectratio=dict(x=1, y=1, z=0.7),
|
| 878 |
+
|
| 879 |
+
camera=dict(eye=dict(x=1.5, y=1.5, z=1.0), center=dict(x=0, y=0, z=-0.1), up=dict(x=0,y=0,z=1))
|
| 880 |
+
|
| 881 |
+
),
|
| 882 |
+
|
| 883 |
+
margin=dict(l=10, r=10, b=10, t=60), width=800, height=700
|
| 884 |
+
|
| 885 |
+
)
|
| 886 |
+
|
| 887 |
+
|
| 888 |
+
|
| 889 |
+
temp_image_files = []
|
| 890 |
+
|
| 891 |
+
gif_fps_val = 10
|
| 892 |
+
|
| 893 |
+
|
| 894 |
+
|
| 895 |
+
for k, Z_frame_data in enumerate(data_frames_list):
|
| 896 |
+
|
| 897 |
+
Z_plotly_frame = Z_frame_data / norm_factor_plotly
|
| 898 |
+
|
| 899 |
+
gif_fig.data[0].z = Z_plotly_frame
|
| 900 |
+
|
| 901 |
+
current_ts_title = actual_timesteps_for_title[k] if k < len(actual_timesteps_for_title) else "Unknown"
|
| 902 |
+
|
| 903 |
+
gif_fig.update_layout(
|
| 904 |
+
|
| 905 |
+
title_text=f'QLBM Simulation (Plotly) - Timestep: {current_ts_title}',
|
| 906 |
+
|
| 907 |
+
title_x=0.5, title_font_size=16
|
| 908 |
+
|
| 909 |
+
)
|
| 910 |
+
|
| 911 |
+
temp_image_path = intermediate_folder_path / f"plotly_frame_{k:04d}.png"
|
| 912 |
+
|
| 913 |
+
gif_fig.write_image(str(temp_image_path), engine="kaleido")
|
| 914 |
+
|
| 915 |
+
temp_image_files.append(str(temp_image_path))
|
| 916 |
+
|
| 917 |
+
|
| 918 |
+
|
| 919 |
+
if temp_image_files:
|
| 920 |
+
|
| 921 |
+
with imageio.get_writer(str(gif_path_to_return), mode='I', fps=gif_fps_val, loop=0) as writer:
|
| 922 |
+
|
| 923 |
+
for filename in temp_image_files:
|
| 924 |
+
|
| 925 |
+
image = imageio.imread(filename)
|
| 926 |
+
|
| 927 |
+
writer.append_data(image)
|
| 928 |
+
|
| 929 |
+
print(f"Plotly animation saved to {gif_path_to_return}")
|
| 930 |
+
|
| 931 |
+
else:
|
| 932 |
+
|
| 933 |
+
print("Error: No Plotly frames generated for GIF.")
|
| 934 |
+
|
| 935 |
+
return None, None
|
| 936 |
+
|
| 937 |
+
|
| 938 |
+
|
| 939 |
+
return str(gif_path_to_return), fig
|
| 940 |
+
|
| 941 |
+
|
| 942 |
+
|
| 943 |
+
# Gradio Interface Definition
|
| 944 |
+
|
| 945 |
+
def qlbm_gradio_interface(num_reg_qubits_input: int, timescale_input: int, distribution_type_param: str, ux_param: float, uy_param: float):
|
| 946 |
+
|
| 947 |
+
num_reg_qubits_val = int(num_reg_qubits_input)
|
| 948 |
+
|
| 949 |
+
timescale_val = int(timescale_input)
|
| 950 |
+
|
| 951 |
+
ux_val = float(ux_param)
|
| 952 |
+
|
| 953 |
+
uy_val = float(uy_param)
|
| 954 |
+
|
| 955 |
+
|
| 956 |
+
|
| 957 |
+
print(f"Gradio Interface: num_reg_qubits={num_reg_qubits_val}, T={timescale_val}, Distribution={distribution_type_param}, ux={ux_val}, uy={uy_val}")
|
| 958 |
+
|
| 959 |
+
|
| 960 |
+
|
| 961 |
+
gif_path, plot_fig = simulate_qlbm_and_animate(
|
| 962 |
+
|
| 963 |
+
num_reg_qubits=num_reg_qubits_val,
|
| 964 |
+
|
| 965 |
+
T=timescale_val,
|
| 966 |
+
|
| 967 |
+
distribution_type=distribution_type_param,
|
| 968 |
+
|
| 969 |
+
ux_input=ux_val,
|
| 970 |
+
|
| 971 |
+
uy_input=uy_val
|
| 972 |
+
|
| 973 |
+
)
|
| 974 |
+
|
| 975 |
+
|
| 976 |
+
|
| 977 |
+
if gif_path is None or plot_fig is None:
|
| 978 |
+
|
| 979 |
+
gr.Warning("Simulation or plotting failed. Please check console for errors.")
|
| 980 |
+
|
| 981 |
+
return None, None
|
| 982 |
+
|
| 983 |
+
return gif_path, plot_fig
|
| 984 |
+
|
| 985 |
+
|
| 986 |
+
|
| 987 |
+
with gr.Blocks(theme=gr.themes.Soft(), title="QLBM Simulation with Plotly") as qlbm_demo:
|
| 988 |
+
|
| 989 |
+
gr.Markdown(
|
| 990 |
+
|
| 991 |
+
"""
|
| 992 |
+
|
| 993 |
+
# ⚛️ Quantum Lattice Boltzmann Method (QLBM) Simulator (Plotly Animation)
|
| 994 |
+
|
| 995 |
+
Welcome to the Quantum Lattice Boltzmann Method (QLBM) simulator! This version uses Plotly for 3D animation and interactive plots.
|
| 996 |
+
|
| 997 |
+
|
| 998 |
+
|
| 999 |
+
**How this Simulator Works:**
|
| 1000 |
+
|
| 1001 |
+
This simulator implements a D2Q5 model on a quantum computer simulator (CUDA-Q).
|
| 1002 |
+
|
| 1003 |
+
- Control grid size (via Number of Register Qubits: $N=2^{\text{num_reg_qubits}}$).
|
| 1004 |
+
|
| 1005 |
+
- Set total simulation time (Timescale T).
|
| 1006 |
+
|
| 1007 |
+
- Choose initial distribution.
|
| 1008 |
+
|
| 1009 |
+
- Set advection velocities `ux` and `uy`.
|
| 1010 |
+
|
| 1011 |
+
The simulation generates a GIF animation and an interactive Plotly figure with a slider for selected time steps.
|
| 1012 |
+
|
| 1013 |
+
|
| 1014 |
+
|
| 1015 |
+
**Note:** Higher qubit counts and longer timescales are computationally intensive. Advection velocities should be small (e.g., < 0.3).
|
| 1016 |
+
|
| 1017 |
+
The output GIF loops indefinitely, and the Plotly figure allows interactive exploration of specific time steps.
|
| 1018 |
+
|
| 1019 |
+
"""
|
| 1020 |
+
|
| 1021 |
+
)
|
| 1022 |
+
|
| 1023 |
+
with gr.Row():
|
| 1024 |
+
|
| 1025 |
+
with gr.Column(scale=1):
|
| 1026 |
+
|
| 1027 |
+
gr.Markdown("## Simulation Parameters")
|
| 1028 |
+
|
| 1029 |
+
num_reg_qubits_slider = gr.Slider(
|
| 1030 |
+
|
| 1031 |
+
minimum=2, maximum=10, value=8, step=1,
|
| 1032 |
+
|
| 1033 |
+
label="Number of Register Qubits (num_reg_qubits)",
|
| 1034 |
+
|
| 1035 |
+
info="Grid N = 2^num_reg_qubits. Max 10 (Note: >8 slow; >9 may hit simulator/memory limits on free tiers)."
|
| 1036 |
+
|
| 1037 |
+
)
|
| 1038 |
+
|
| 1039 |
+
timescale_slider = gr.Slider(
|
| 1040 |
+
|
| 1041 |
+
minimum=0, maximum=2000, value=100, step=10,
|
| 1042 |
+
|
| 1043 |
+
label="Timescale (T)", info="Total number of timesteps. Max 2000."
|
| 1044 |
+
|
| 1045 |
+
)
|
| 1046 |
+
|
| 1047 |
+
distribution_options = ["Sine Wave (Original)", "Gaussian", "Random"]
|
| 1048 |
+
|
| 1049 |
+
distribution_type_input = gr.Radio(
|
| 1050 |
+
|
| 1051 |
+
choices=distribution_options, value="Sine Wave (Original)",
|
| 1052 |
+
|
| 1053 |
+
label="Initial Distribution Type", info="Select the initial pattern of the substance."
|
| 1054 |
+
|
| 1055 |
+
)
|
| 1056 |
+
|
| 1057 |
+
ux_slider = gr.Slider(
|
| 1058 |
+
|
| 1059 |
+
minimum=-0.4, maximum=0.4, value=0.2, step=0.01,
|
| 1060 |
+
|
| 1061 |
+
label="Advection Velocity ux", info="x-component of background advection."
|
| 1062 |
+
|
| 1063 |
+
)
|
| 1064 |
+
|
| 1065 |
+
uy_slider = gr.Slider(
|
| 1066 |
+
|
| 1067 |
+
�� minimum=-0.4, maximum=0.4, value=0.15, step=0.01,
|
| 1068 |
+
|
| 1069 |
+
label="Advection Velocity uy", info="y-component of background advection."
|
| 1070 |
+
|
| 1071 |
+
)
|
| 1072 |
+
|
| 1073 |
+
run_qlbm_btn = gr.Button("Run QLBM Simulation", variant="primary")
|
| 1074 |
+
|
| 1075 |
+
|
| 1076 |
+
|
| 1077 |
+
with gr.Column(scale=2):
|
| 1078 |
+
|
| 1079 |
+
qlbm_plot_output = gr.Image(label="QLBM Simulation Animation (GIF)", type="filepath", height=600)
|
| 1080 |
+
|
| 1081 |
+
qlbm_interactive_plot = gr.Plot(label="Interactive Density Plot with Slider")
|
| 1082 |
+
|
| 1083 |
+
|
| 1084 |
+
|
| 1085 |
+
qlbm_inputs_list = [num_reg_qubits_slider, timescale_slider, distribution_type_input, ux_slider, uy_slider]
|
| 1086 |
+
|
| 1087 |
+
run_qlbm_btn.click(
|
| 1088 |
+
|
| 1089 |
+
fn=qlbm_gradio_interface,
|
| 1090 |
+
|
| 1091 |
+
inputs=qlbm_inputs_list,
|
| 1092 |
+
|
| 1093 |
+
outputs=[qlbm_plot_output, qlbm_interactive_plot]
|
| 1094 |
+
|
| 1095 |
+
)
|
| 1096 |
+
|
| 1097 |
+
gr.Examples(
|
| 1098 |
+
|
| 1099 |
+
examples=[
|
| 1100 |
+
|
| 1101 |
+
[8, 100, "Sine Wave (Original)", 0.2, 0.15],
|
| 1102 |
+
|
| 1103 |
+
[6, 50, "Gaussian", 0.1, 0.05],
|
| 1104 |
+
|
| 1105 |
+
[4, 30, "Random", -0.05, 0.1],
|
| 1106 |
+
|
| 1107 |
+
],
|
| 1108 |
+
|
| 1109 |
+
inputs=qlbm_inputs_list,
|
| 1110 |
+
|
| 1111 |
+
outputs=[qlbm_plot_output, qlbm_interactive_plot],
|
| 1112 |
+
|
| 1113 |
+
fn=qlbm_gradio_interface,
|
| 1114 |
+
|
| 1115 |
+
cache_examples=False
|
| 1116 |
+
|
| 1117 |
+
)
|
| 1118 |
+
|
| 1119 |
+
|
| 1120 |
+
|
| 1121 |
+
if __name__ == "__main__":
|
| 1122 |
+
|
| 1123 |
+
try:
|
| 1124 |
+
|
| 1125 |
+
cudaq.set_target('nvidia', option='fp64')
|
| 1126 |
+
|
| 1127 |
+
print(f"CUDA-Q Target successfully set to: {cudaq.get_target().name}")
|
| 1128 |
+
|
| 1129 |
+
except Exception as e_target:
|
| 1130 |
+
|
| 1131 |
+
print(f"Warning: Could not set CUDA-Q target to 'nvidia'. Error: {e_target}")
|
| 1132 |
+
|
| 1133 |
+
print(f"Current CUDA-Q Target: {cudaq.get_target().name}. Performance may be affected.")
|
| 1134 |
+
|
| 1135 |
+
|
| 1136 |
+
|
| 1137 |
+
qlbm_demo.launch()
|