Spaces:
Sleeping
Sleeping
Upload 2 files
Browse files- app.py +731 -0
- requirements.txt +3 -0
app.py
ADDED
|
@@ -0,0 +1,731 @@
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
| 1 |
+
"""
|
| 2 |
+
Quantum Paradox Lab
|
| 3 |
+
Interactive demos proving quantum's future is architecture over qubit counts.
|
| 4 |
+
|
| 5 |
+
Explores: Barren Plateaus, QSVT Unification, Photonic Blueprints, AI Circuit Design
|
| 6 |
+
"""
|
| 7 |
+
|
| 8 |
+
import gradio as gr
|
| 9 |
+
import numpy as np
|
| 10 |
+
import plotly.graph_objects as go
|
| 11 |
+
import plotly.express as px
|
| 12 |
+
from plotly.subplots import make_subplots
|
| 13 |
+
import math
|
| 14 |
+
|
| 15 |
+
# Quantum algorithm data for QSVT unification
|
| 16 |
+
QSVT_ALGORITHMS = {
|
| 17 |
+
"Grover's Search": {
|
| 18 |
+
"year": 1996,
|
| 19 |
+
"speedup": "Quadratic",
|
| 20 |
+
"problem": "Unstructured search",
|
| 21 |
+
"classical": "O(N)",
|
| 22 |
+
"quantum": "O(鈭歂)",
|
| 23 |
+
"unified_by_qsvt": True,
|
| 24 |
+
"polynomial": "Sign function approximation"
|
| 25 |
+
},
|
| 26 |
+
"Quantum Phase Estimation": {
|
| 27 |
+
"year": 1995,
|
| 28 |
+
"speedup": "Exponential",
|
| 29 |
+
"problem": "Eigenvalue extraction",
|
| 30 |
+
"classical": "O(N鲁)",
|
| 31 |
+
"quantum": "O(log N)",
|
| 32 |
+
"unified_by_qsvt": True,
|
| 33 |
+
"polynomial": "Window function"
|
| 34 |
+
},
|
| 35 |
+
"HHL (Linear Systems)": {
|
| 36 |
+
"year": 2009,
|
| 37 |
+
"speedup": "Exponential",
|
| 38 |
+
"problem": "Solve Ax = b",
|
| 39 |
+
"classical": "O(N鲁)",
|
| 40 |
+
"quantum": "O(log N)",
|
| 41 |
+
"unified_by_qsvt": True,
|
| 42 |
+
"polynomial": "1/x inversion"
|
| 43 |
+
},
|
| 44 |
+
"Hamiltonian Simulation": {
|
| 45 |
+
"year": 1982,
|
| 46 |
+
"speedup": "Exponential",
|
| 47 |
+
"problem": "Time evolution",
|
| 48 |
+
"classical": "O(2^N)",
|
| 49 |
+
"quantum": "O(poly(N))",
|
| 50 |
+
"unified_by_qsvt": True,
|
| 51 |
+
"polynomial": "Jacobi-Anger expansion"
|
| 52 |
+
},
|
| 53 |
+
"Amplitude Amplification": {
|
| 54 |
+
"year": 2000,
|
| 55 |
+
"speedup": "Quadratic",
|
| 56 |
+
"problem": "Probability boost",
|
| 57 |
+
"classical": "O(1/p)",
|
| 58 |
+
"quantum": "O(1/鈭歱)",
|
| 59 |
+
"unified_by_qsvt": True,
|
| 60 |
+
"polynomial": "Chebyshev iteration"
|
| 61 |
+
},
|
| 62 |
+
"Eigenvalue Threshold": {
|
| 63 |
+
"year": 2019,
|
| 64 |
+
"speedup": "Polynomial",
|
| 65 |
+
"problem": "Spectral filtering",
|
| 66 |
+
"classical": "O(N鲁)",
|
| 67 |
+
"quantum": "O(N路polylog)",
|
| 68 |
+
"unified_by_qsvt": True,
|
| 69 |
+
"polynomial": "Step function"
|
| 70 |
+
}
|
| 71 |
+
}
|
| 72 |
+
|
| 73 |
+
# Quantum hardware comparison
|
| 74 |
+
QUANTUM_HARDWARE = {
|
| 75 |
+
"Superconducting (IBM)": {
|
| 76 |
+
"temp_kelvin": 0.015,
|
| 77 |
+
"qubits_2024": 1121,
|
| 78 |
+
"coherence_us": 300,
|
| 79 |
+
"gate_fidelity": 0.999,
|
| 80 |
+
"color": "#0066cc",
|
| 81 |
+
"pros": "Fast gates, high connectivity",
|
| 82 |
+
"cons": "Cryogenic cooling required"
|
| 83 |
+
},
|
| 84 |
+
"Superconducting (Google)": {
|
| 85 |
+
"temp_kelvin": 0.015,
|
| 86 |
+
"qubits_2024": 105,
|
| 87 |
+
"coherence_us": 100,
|
| 88 |
+
"gate_fidelity": 0.9995,
|
| 89 |
+
"color": "#4285f4",
|
| 90 |
+
"pros": "Highest 2-qubit fidelity",
|
| 91 |
+
"cons": "Expensive infrastructure"
|
| 92 |
+
},
|
| 93 |
+
"Trapped Ions (IonQ)": {
|
| 94 |
+
"temp_kelvin": 0.001,
|
| 95 |
+
"qubits_2024": 35,
|
| 96 |
+
"coherence_us": 10000000,
|
| 97 |
+
"gate_fidelity": 0.999,
|
| 98 |
+
"color": "#ff6b35",
|
| 99 |
+
"pros": "Long coherence, all-to-all connectivity",
|
| 100 |
+
"cons": "Slow gates, scaling challenges"
|
| 101 |
+
},
|
| 102 |
+
"Photonic (Xanadu)": {
|
| 103 |
+
"temp_kelvin": 293,
|
| 104 |
+
"qubits_2024": 216,
|
| 105 |
+
"coherence_us": float('inf'),
|
| 106 |
+
"gate_fidelity": 0.99,
|
| 107 |
+
"color": "#00ff88",
|
| 108 |
+
"pros": "Room temperature, natural networking",
|
| 109 |
+
"cons": "Probabilistic gates, photon loss"
|
| 110 |
+
},
|
| 111 |
+
"Neutral Atoms (QuEra)": {
|
| 112 |
+
"temp_kelvin": 0.00001,
|
| 113 |
+
"qubits_2024": 256,
|
| 114 |
+
"coherence_us": 1000,
|
| 115 |
+
"gate_fidelity": 0.995,
|
| 116 |
+
"color": "#9b59b6",
|
| 117 |
+
"pros": "Large arrays, reconfigurable",
|
| 118 |
+
"cons": "Laser complexity"
|
| 119 |
+
}
|
| 120 |
+
}
|
| 121 |
+
|
| 122 |
+
# Energy costs
|
| 123 |
+
ENERGY_COSTS = {
|
| 124 |
+
"Classical GPU (A100)": {"watts": 400, "ops_per_sec": 1e15, "cost_per_kwh": 0.12},
|
| 125 |
+
"Classical TPU (v4)": {"watts": 200, "ops_per_sec": 2.7e15, "cost_per_kwh": 0.12},
|
| 126 |
+
"Superconducting QC": {"watts": 25000, "qubits": 1000, "cost_per_kwh": 0.12},
|
| 127 |
+
"Photonic QC": {"watts": 500, "qubits": 200, "cost_per_kwh": 0.12},
|
| 128 |
+
}
|
| 129 |
+
|
| 130 |
+
def simulate_barren_plateau(num_qubits, num_layers, num_samples=100):
|
| 131 |
+
"""
|
| 132 |
+
Simulate gradient variance decay in variational quantum circuits.
|
| 133 |
+
Demonstrates barren plateau phenomenon.
|
| 134 |
+
"""
|
| 135 |
+
np.random.seed(42)
|
| 136 |
+
|
| 137 |
+
qubit_range = range(2, num_qubits + 1)
|
| 138 |
+
layer_configs = [1, num_layers // 2, num_layers]
|
| 139 |
+
|
| 140 |
+
results = []
|
| 141 |
+
for n_qubits in qubit_range:
|
| 142 |
+
for n_layers in layer_configs:
|
| 143 |
+
gradients = []
|
| 144 |
+
for _ in range(num_samples):
|
| 145 |
+
grad = np.random.randn() * np.exp(-n_qubits * n_layers / 10)
|
| 146 |
+
noise = np.random.randn() * 0.01
|
| 147 |
+
gradients.append(grad + noise)
|
| 148 |
+
|
| 149 |
+
variance = np.var(gradients)
|
| 150 |
+
results.append({
|
| 151 |
+
"qubits": n_qubits,
|
| 152 |
+
"layers": n_layers,
|
| 153 |
+
"variance": variance,
|
| 154 |
+
"vanishing": variance < 1e-6
|
| 155 |
+
})
|
| 156 |
+
|
| 157 |
+
return results
|
| 158 |
+
|
| 159 |
+
def create_barren_plateau_chart(num_qubits, num_layers):
|
| 160 |
+
"""Create interactive barren plateau visualization."""
|
| 161 |
+
results = simulate_barren_plateau(num_qubits, num_layers)
|
| 162 |
+
|
| 163 |
+
fig = make_subplots(
|
| 164 |
+
rows=1, cols=2,
|
| 165 |
+
subplot_titles=("Gradient Variance vs Qubits", "The Paradox Zone"),
|
| 166 |
+
specs=[[{"type": "scatter"}, {"type": "heatmap"}]]
|
| 167 |
+
)
|
| 168 |
+
|
| 169 |
+
for n_layers in [1, num_layers // 2, num_layers]:
|
| 170 |
+
layer_data = [r for r in results if r["layers"] == n_layers]
|
| 171 |
+
fig.add_trace(
|
| 172 |
+
go.Scatter(
|
| 173 |
+
x=[r["qubits"] for r in layer_data],
|
| 174 |
+
y=[r["variance"] for r in layer_data],
|
| 175 |
+
mode='lines+markers',
|
| 176 |
+
name=f'{n_layers} layers',
|
| 177 |
+
line=dict(width=2),
|
| 178 |
+
marker=dict(size=8)
|
| 179 |
+
),
|
| 180 |
+
row=1, col=1
|
| 181 |
+
)
|
| 182 |
+
|
| 183 |
+
fig.add_hline(y=1e-6, line_dash="dash", line_color="red",
|
| 184 |
+
annotation_text="Vanishing threshold", row=1, col=1)
|
| 185 |
+
|
| 186 |
+
qubits_list = list(range(2, num_qubits + 1))
|
| 187 |
+
layers_list = list(range(1, num_layers + 1))
|
| 188 |
+
z_matrix = np.zeros((len(layers_list), len(qubits_list)))
|
| 189 |
+
|
| 190 |
+
for i, n_layers in enumerate(layers_list):
|
| 191 |
+
for j, n_qubits in enumerate(qubits_list):
|
| 192 |
+
z_matrix[i, j] = np.exp(-n_qubits * n_layers / 10)
|
| 193 |
+
|
| 194 |
+
fig.add_trace(
|
| 195 |
+
go.Heatmap(
|
| 196 |
+
z=np.log10(z_matrix + 1e-10),
|
| 197 |
+
x=qubits_list,
|
| 198 |
+
y=layers_list,
|
| 199 |
+
colorscale=[
|
| 200 |
+
[0, "#00ff88"],
|
| 201 |
+
[0.5, "#ffcc00"],
|
| 202 |
+
[1, "#ff0000"]
|
| 203 |
+
],
|
| 204 |
+
showscale=True,
|
| 205 |
+
colorbar=dict(title="log鈧佲個(variance)")
|
| 206 |
+
),
|
| 207 |
+
row=1, col=2
|
| 208 |
+
)
|
| 209 |
+
|
| 210 |
+
fig.update_layout(
|
| 211 |
+
title=dict(
|
| 212 |
+
text="Barren Plateaus: The Trainability Paradox",
|
| 213 |
+
font=dict(size=20, color="#00ff88")
|
| 214 |
+
),
|
| 215 |
+
paper_bgcolor='#0d0d1a',
|
| 216 |
+
plot_bgcolor='#0d0d1a',
|
| 217 |
+
font=dict(color='white'),
|
| 218 |
+
height=450,
|
| 219 |
+
showlegend=True
|
| 220 |
+
)
|
| 221 |
+
|
| 222 |
+
fig.update_xaxes(title_text="Number of Qubits", gridcolor='#333355', row=1, col=1)
|
| 223 |
+
fig.update_yaxes(title_text="Gradient Variance", type="log", gridcolor='#333355', row=1, col=1)
|
| 224 |
+
fig.update_xaxes(title_text="Qubits", row=1, col=2)
|
| 225 |
+
fig.update_yaxes(title_text="Layers", row=1, col=2)
|
| 226 |
+
|
| 227 |
+
return fig
|
| 228 |
+
|
| 229 |
+
def create_qsvt_unification_chart():
|
| 230 |
+
"""Create visualization of QSVT unifying quantum algorithms."""
|
| 231 |
+
fig = go.Figure()
|
| 232 |
+
|
| 233 |
+
algorithms = list(QSVT_ALGORITHMS.keys())
|
| 234 |
+
years = [QSVT_ALGORITHMS[a]["year"] for a in algorithms]
|
| 235 |
+
colors = ['#0074D9', '#FF4136', '#2ECC40', '#FFDC00', '#F012BE', '#FF851B']
|
| 236 |
+
|
| 237 |
+
for i, (algo, data) in enumerate(QSVT_ALGORITHMS.items()):
|
| 238 |
+
fig.add_trace(go.Scatter(
|
| 239 |
+
x=[data["year"]],
|
| 240 |
+
y=[i],
|
| 241 |
+
mode='markers+text',
|
| 242 |
+
marker=dict(size=30, color=colors[i], symbol='circle'),
|
| 243 |
+
text=[algo.split()[0]],
|
| 244 |
+
textposition="middle right",
|
| 245 |
+
textfont=dict(color='white', size=11),
|
| 246 |
+
hovertemplate=f"<b>{algo}</b><br>Year: {data['year']}<br>Speedup: {data['speedup']}<br>Problem: {data['problem']}<extra></extra>"
|
| 247 |
+
))
|
| 248 |
+
|
| 249 |
+
fig.add_shape(
|
| 250 |
+
type="rect",
|
| 251 |
+
x0=2015, x1=2025, y0=-0.5, y1=5.5,
|
| 252 |
+
fillcolor="rgba(0, 255, 136, 0.1)",
|
| 253 |
+
line=dict(color="#00ff88", width=2)
|
| 254 |
+
)
|
| 255 |
+
|
| 256 |
+
fig.add_annotation(
|
| 257 |
+
x=2020, y=5.8,
|
| 258 |
+
text="QSVT Unification (2019+)",
|
| 259 |
+
showarrow=False,
|
| 260 |
+
font=dict(color="#00ff88", size=14)
|
| 261 |
+
)
|
| 262 |
+
|
| 263 |
+
for i in range(len(algorithms)):
|
| 264 |
+
fig.add_shape(
|
| 265 |
+
type="line",
|
| 266 |
+
x0=years[i], y0=i,
|
| 267 |
+
x1=2019, y1=2.5,
|
| 268 |
+
line=dict(color=colors[i], width=1, dash="dot")
|
| 269 |
+
)
|
| 270 |
+
|
| 271 |
+
fig.update_layout(
|
| 272 |
+
title="QSVT: One Framework to Rule Them All",
|
| 273 |
+
xaxis=dict(title="Year Discovered", range=[1980, 2026], gridcolor='#333355'),
|
| 274 |
+
yaxis=dict(visible=False, range=[-1, 7]),
|
| 275 |
+
paper_bgcolor='#0d0d1a',
|
| 276 |
+
plot_bgcolor='#0d0d1a',
|
| 277 |
+
font=dict(color='white'),
|
| 278 |
+
height=400,
|
| 279 |
+
showlegend=False
|
| 280 |
+
)
|
| 281 |
+
|
| 282 |
+
return fig
|
| 283 |
+
|
| 284 |
+
def create_hardware_comparison():
|
| 285 |
+
"""Create quantum hardware comparison chart."""
|
| 286 |
+
fig = make_subplots(
|
| 287 |
+
rows=1, cols=2,
|
| 288 |
+
subplot_titles=("Operating Temperature (log scale)", "Qubit Count vs Coherence"),
|
| 289 |
+
specs=[[{"type": "bar"}, {"type": "scatter"}]]
|
| 290 |
+
)
|
| 291 |
+
|
| 292 |
+
names = list(QUANTUM_HARDWARE.keys())
|
| 293 |
+
temps = [QUANTUM_HARDWARE[n]["temp_kelvin"] for n in names]
|
| 294 |
+
colors = [QUANTUM_HARDWARE[n]["color"] for n in names]
|
| 295 |
+
|
| 296 |
+
fig.add_trace(
|
| 297 |
+
go.Bar(
|
| 298 |
+
x=names,
|
| 299 |
+
y=temps,
|
| 300 |
+
marker_color=colors,
|
| 301 |
+
text=[f"{t:.3f}K" if t < 1 else f"{t}K" for t in temps],
|
| 302 |
+
textposition='outside'
|
| 303 |
+
),
|
| 304 |
+
row=1, col=1
|
| 305 |
+
)
|
| 306 |
+
|
| 307 |
+
qubits = [QUANTUM_HARDWARE[n]["qubits_2024"] for n in names]
|
| 308 |
+
coherence = [min(QUANTUM_HARDWARE[n]["coherence_us"], 1e7) for n in names]
|
| 309 |
+
|
| 310 |
+
fig.add_trace(
|
| 311 |
+
go.Scatter(
|
| 312 |
+
x=qubits,
|
| 313 |
+
y=coherence,
|
| 314 |
+
mode='markers+text',
|
| 315 |
+
marker=dict(size=20, color=colors),
|
| 316 |
+
text=[n.split()[0] for n in names],
|
| 317 |
+
textposition="top center",
|
| 318 |
+
textfont=dict(size=10)
|
| 319 |
+
),
|
| 320 |
+
row=1, col=2
|
| 321 |
+
)
|
| 322 |
+
|
| 323 |
+
fig.add_annotation(
|
| 324 |
+
x=216, y=1e7,
|
| 325 |
+
text="Photonic:<br>Room temp!",
|
| 326 |
+
showarrow=True,
|
| 327 |
+
arrowhead=2,
|
| 328 |
+
arrowcolor="#00ff88",
|
| 329 |
+
font=dict(color="#00ff88"),
|
| 330 |
+
row=1, col=2
|
| 331 |
+
)
|
| 332 |
+
|
| 333 |
+
fig.update_layout(
|
| 334 |
+
paper_bgcolor='#0d0d1a',
|
| 335 |
+
plot_bgcolor='#0d0d1a',
|
| 336 |
+
font=dict(color='white'),
|
| 337 |
+
height=400,
|
| 338 |
+
showlegend=False
|
| 339 |
+
)
|
| 340 |
+
|
| 341 |
+
fig.update_yaxes(type="log", title="Temperature (K)", gridcolor='#333355', row=1, col=1)
|
| 342 |
+
fig.update_xaxes(tickangle=45, row=1, col=1)
|
| 343 |
+
fig.update_xaxes(title="Qubits (2024)", gridcolor='#333355', row=1, col=2)
|
| 344 |
+
fig.update_yaxes(type="log", title="Coherence (渭s)", gridcolor='#333355', row=1, col=2)
|
| 345 |
+
|
| 346 |
+
return fig
|
| 347 |
+
|
| 348 |
+
def create_energy_comparison(problem_size):
|
| 349 |
+
"""Compare energy costs for quantum vs classical."""
|
| 350 |
+
classical_ops = problem_size ** 3
|
| 351 |
+
quantum_advantage_threshold = 1000
|
| 352 |
+
|
| 353 |
+
classical_gpu_time = classical_ops / ENERGY_COSTS["Classical GPU (A100)"]["ops_per_sec"]
|
| 354 |
+
classical_gpu_energy = classical_gpu_time * ENERGY_COSTS["Classical GPU (A100)"]["watts"] / 3600000
|
| 355 |
+
|
| 356 |
+
quantum_ops = problem_size * np.log2(problem_size) if problem_size > 1 else 1
|
| 357 |
+
quantum_time = quantum_ops / 1e6
|
| 358 |
+
|
| 359 |
+
sc_energy = quantum_time * ENERGY_COSTS["Superconducting QC"]["watts"] / 3600000
|
| 360 |
+
photonic_energy = quantum_time * ENERGY_COSTS["Photonic QC"]["watts"] / 3600000
|
| 361 |
+
|
| 362 |
+
fig = go.Figure()
|
| 363 |
+
|
| 364 |
+
categories = ["Classical GPU", "Superconducting QC", "Photonic QC"]
|
| 365 |
+
energies = [classical_gpu_energy * 1000, sc_energy * 1000, photonic_energy * 1000]
|
| 366 |
+
colors = ["#ff6b6b", "#0066cc", "#00ff88"]
|
| 367 |
+
|
| 368 |
+
fig.add_trace(go.Bar(
|
| 369 |
+
x=categories,
|
| 370 |
+
y=energies,
|
| 371 |
+
marker_color=colors,
|
| 372 |
+
text=[f"{e:.4f} Wh" for e in energies],
|
| 373 |
+
textposition='outside'
|
| 374 |
+
))
|
| 375 |
+
|
| 376 |
+
fig.update_layout(
|
| 377 |
+
title=f"Energy per Query (Problem Size: {problem_size})",
|
| 378 |
+
yaxis=dict(title="Energy (mWh)", type="log", gridcolor='#333355'),
|
| 379 |
+
paper_bgcolor='#0d0d1a',
|
| 380 |
+
plot_bgcolor='#0d0d1a',
|
| 381 |
+
font=dict(color='white'),
|
| 382 |
+
height=350
|
| 383 |
+
)
|
| 384 |
+
|
| 385 |
+
return fig
|
| 386 |
+
|
| 387 |
+
def generate_circuit_description(problem_type, num_qubits):
|
| 388 |
+
"""Generate a description of a quantum circuit for the given problem."""
|
| 389 |
+
circuits = {
|
| 390 |
+
"QAOA (Max-Cut)": f"""
|
| 391 |
+
# QAOA Circuit for {num_qubits}-qubit Max-Cut
|
| 392 |
+
# Layers: 2, Parameters: {num_qubits * 4}
|
| 393 |
+
|
| 394 |
+
OPENQASM 3.0;
|
| 395 |
+
include "stdgates.inc";
|
| 396 |
+
|
| 397 |
+
qubit[{num_qubits}] q;
|
| 398 |
+
bit[{num_qubits}] c;
|
| 399 |
+
|
| 400 |
+
// Initial superposition
|
| 401 |
+
for int i in [0:{num_qubits-1}] {{ h q[i]; }}
|
| 402 |
+
|
| 403 |
+
// Cost layer (problem-dependent ZZ interactions)
|
| 404 |
+
for int i in [0:{num_qubits-2}] {{
|
| 405 |
+
cx q[i], q[i+1];
|
| 406 |
+
rz(gamma) q[i+1];
|
| 407 |
+
cx q[i], q[i+1];
|
| 408 |
+
}}
|
| 409 |
+
|
| 410 |
+
// Mixer layer
|
| 411 |
+
for int i in [0:{num_qubits-1}] {{ rx(beta) q[i]; }}
|
| 412 |
+
|
| 413 |
+
// Measurement
|
| 414 |
+
c = measure q;
|
| 415 |
+
""",
|
| 416 |
+
"VQE (H2 Molecule)": f"""
|
| 417 |
+
# VQE Ansatz for Molecular Simulation
|
| 418 |
+
# Qubits: {num_qubits}, Parameters: {num_qubits * 2}
|
| 419 |
+
|
| 420 |
+
OPENQASM 3.0;
|
| 421 |
+
include "stdgates.inc";
|
| 422 |
+
|
| 423 |
+
qubit[{num_qubits}] q;
|
| 424 |
+
|
| 425 |
+
// Hardware-efficient ansatz
|
| 426 |
+
for int i in [0:{num_qubits-1}] {{
|
| 427 |
+
ry(theta[i]) q[i];
|
| 428 |
+
rz(phi[i]) q[i];
|
| 429 |
+
}}
|
| 430 |
+
|
| 431 |
+
// Entangling layer
|
| 432 |
+
for int i in [0:{num_qubits-2}] {{
|
| 433 |
+
cx q[i], q[i+1];
|
| 434 |
+
}}
|
| 435 |
+
|
| 436 |
+
// Second rotation layer
|
| 437 |
+
for int i in [0:{num_qubits-1}] {{
|
| 438 |
+
ry(theta2[i]) q[i];
|
| 439 |
+
}}
|
| 440 |
+
""",
|
| 441 |
+
"Grover's Search": f"""
|
| 442 |
+
# Grover's Algorithm for {num_qubits}-qubit search
|
| 443 |
+
# Iterations: {int(np.pi/4 * np.sqrt(2**num_qubits))}
|
| 444 |
+
|
| 445 |
+
OPENQASM 3.0;
|
| 446 |
+
include "stdgates.inc";
|
| 447 |
+
|
| 448 |
+
qubit[{num_qubits}] q;
|
| 449 |
+
qubit ancilla;
|
| 450 |
+
|
| 451 |
+
// Initialize
|
| 452 |
+
for int i in [0:{num_qubits-1}] {{ h q[i]; }}
|
| 453 |
+
x ancilla;
|
| 454 |
+
h ancilla;
|
| 455 |
+
|
| 456 |
+
// Grover iterations
|
| 457 |
+
for int iter in [0:{int(np.pi/4 * np.sqrt(2**num_qubits))-1}] {{
|
| 458 |
+
// Oracle (problem-specific)
|
| 459 |
+
// ... mark target state ...
|
| 460 |
+
|
| 461 |
+
// Diffusion operator
|
| 462 |
+
for int i in [0:{num_qubits-1}] {{ h q[i]; x q[i]; }}
|
| 463 |
+
// Multi-controlled Z
|
| 464 |
+
for int i in [0:{num_qubits-1}] {{ h q[i]; x q[i]; }}
|
| 465 |
+
}}
|
| 466 |
+
"""
|
| 467 |
+
}
|
| 468 |
+
|
| 469 |
+
return circuits.get(problem_type, "Select a problem type")
|
| 470 |
+
|
| 471 |
+
def get_algorithm_details(algo_name):
|
| 472 |
+
"""Get detailed information about a QSVT-unified algorithm."""
|
| 473 |
+
if algo_name not in QSVT_ALGORITHMS:
|
| 474 |
+
return "Select an algorithm"
|
| 475 |
+
|
| 476 |
+
data = QSVT_ALGORITHMS[algo_name]
|
| 477 |
+
return f"""
|
| 478 |
+
Algorithm: {algo_name}
|
| 479 |
+
Year Discovered: {data['year']}
|
| 480 |
+
Speedup Type: {data['speedup']}
|
| 481 |
+
|
| 482 |
+
Problem Solved: {data['problem']}
|
| 483 |
+
Classical Complexity: {data['classical']}
|
| 484 |
+
Quantum Complexity: {data['quantum']}
|
| 485 |
+
|
| 486 |
+
QSVT Polynomial: {data['polynomial']}
|
| 487 |
+
|
| 488 |
+
How QSVT Unifies This:
|
| 489 |
+
QSVT represents this algorithm as a polynomial transformation
|
| 490 |
+
of singular values. The specific polynomial ({data['polynomial']})
|
| 491 |
+
is implemented via a sequence of signal processing rotations.
|
| 492 |
+
|
| 493 |
+
This means: ONE framework, ONE circuit template, MANY algorithms.
|
| 494 |
+
"""
|
| 495 |
+
|
| 496 |
+
CSS = """
|
| 497 |
+
@import url('https://fonts.googleapis.com/css2?family=JetBrains+Mono:wght@400;700&family=Orbitron:wght@400;700&display=swap');
|
| 498 |
+
|
| 499 |
+
.gradio-container {
|
| 500 |
+
background: linear-gradient(135deg, #0a0a1a 0%, #1a0a2e 50%, #0a1a1a 100%) !important;
|
| 501 |
+
}
|
| 502 |
+
|
| 503 |
+
h1, h2, h3 {
|
| 504 |
+
font-family: 'Orbitron', sans-serif !important;
|
| 505 |
+
color: #00ffcc !important;
|
| 506 |
+
text-shadow: 0 0 30px rgba(0, 255, 204, 0.4);
|
| 507 |
+
}
|
| 508 |
+
|
| 509 |
+
.tab-nav button.selected {
|
| 510 |
+
background: linear-gradient(135deg, #00ffcc, #00cc99) !important;
|
| 511 |
+
color: #0a0a1a !important;
|
| 512 |
+
}
|
| 513 |
+
|
| 514 |
+
button.primary {
|
| 515 |
+
background: linear-gradient(135deg, #00ffcc, #00cc99) !important;
|
| 516 |
+
color: #0a0a1a !important;
|
| 517 |
+
}
|
| 518 |
+
|
| 519 |
+
.prose code {
|
| 520 |
+
background: #1a1a2e !important;
|
| 521 |
+
color: #00ffcc !important;
|
| 522 |
+
}
|
| 523 |
+
"""
|
| 524 |
+
|
| 525 |
+
with gr.Blocks(title="Quantum Paradox Lab") as demo:
|
| 526 |
+
|
| 527 |
+
gr.Markdown("""
|
| 528 |
+
# Quantum Paradox Lab
|
| 529 |
+
|
| 530 |
+
**Interactive proof that quantum's future is architecture over qubit counts.**
|
| 531 |
+
|
| 532 |
+
Explore the counter-intuitive truths reshaping quantum computing: barren plateaus as features,
|
| 533 |
+
QSVT unifying all algorithms, and photonics enabling room-temperature quantum.
|
| 534 |
+
""")
|
| 535 |
+
|
| 536 |
+
with gr.Tabs():
|
| 537 |
+
|
| 538 |
+
# Tab 1: Barren Plateaus
|
| 539 |
+
with gr.TabItem("Barren Plateaus"):
|
| 540 |
+
gr.Markdown("""
|
| 541 |
+
## The Trainability Paradox
|
| 542 |
+
|
| 543 |
+
**Conventional wisdom:** Deeper circuits = more expressive power = better results.
|
| 544 |
+
|
| 545 |
+
**Reality:** Deep random circuits have vanishing gradients. Training becomes impossible.
|
| 546 |
+
|
| 547 |
+
**The twist:** This is actually a FEATURE. If gradients vanished easily, classical computers
|
| 548 |
+
could simulate the circuit. Barren plateaus signal genuine quantum behavior.
|
| 549 |
+
""")
|
| 550 |
+
|
| 551 |
+
with gr.Row():
|
| 552 |
+
qubits_slider = gr.Slider(4, 20, 12, step=1, label="Max Qubits")
|
| 553 |
+
layers_slider = gr.Slider(2, 20, 10, step=1, label="Max Layers")
|
| 554 |
+
|
| 555 |
+
bp_chart = gr.Plot(value=create_barren_plateau_chart(12, 10))
|
| 556 |
+
|
| 557 |
+
qubits_slider.change(create_barren_plateau_chart, [qubits_slider, layers_slider], bp_chart)
|
| 558 |
+
layers_slider.change(create_barren_plateau_chart, [qubits_slider, layers_slider], bp_chart)
|
| 559 |
+
|
| 560 |
+
gr.Markdown("""
|
| 561 |
+
**Key insight:** The green zone (high variance) is trainable but classically simulable.
|
| 562 |
+
The red zone (low variance) has quantum advantage but cannot be trained naively.
|
| 563 |
+
|
| 564 |
+
**Solutions being explored:**
|
| 565 |
+
1. Layer-wise training
|
| 566 |
+
2. Problem-specific ansatze
|
| 567 |
+
3. Tensor network initialization
|
| 568 |
+
4. Parameter correlation structures
|
| 569 |
+
""")
|
| 570 |
+
|
| 571 |
+
# Tab 2: QSVT Unification
|
| 572 |
+
with gr.TabItem("QSVT Unification"):
|
| 573 |
+
gr.Markdown("""
|
| 574 |
+
## One Framework to Rule Them All
|
| 575 |
+
|
| 576 |
+
Quantum Singular Value Transformation (QSVT) unifies the major quantum algorithms
|
| 577 |
+
under a single mathematical framework: polynomial transformations of singular values.
|
| 578 |
+
""")
|
| 579 |
+
|
| 580 |
+
qsvt_chart = gr.Plot(value=create_qsvt_unification_chart())
|
| 581 |
+
|
| 582 |
+
with gr.Row():
|
| 583 |
+
algo_dropdown = gr.Dropdown(
|
| 584 |
+
choices=list(QSVT_ALGORITHMS.keys()),
|
| 585 |
+
label="Select Algorithm",
|
| 586 |
+
value="Grover's Search"
|
| 587 |
+
)
|
| 588 |
+
algo_details = gr.Textbox(label="Algorithm Details", lines=15, interactive=False)
|
| 589 |
+
|
| 590 |
+
algo_dropdown.change(get_algorithm_details, [algo_dropdown], algo_details)
|
| 591 |
+
|
| 592 |
+
gr.Markdown("""
|
| 593 |
+
**Why this matters:**
|
| 594 |
+
|
| 595 |
+
Before QSVT, each algorithm was discovered separately, with unique proofs and implementations.
|
| 596 |
+
Now we understand they are all special cases of one technique.
|
| 597 |
+
|
| 598 |
+
This is like discovering that addition, multiplication, and exponentiation
|
| 599 |
+
are all just repeated applications of the successor function.
|
| 600 |
+
""")
|
| 601 |
+
|
| 602 |
+
# Tab 3: Hardware Comparison
|
| 603 |
+
with gr.TabItem("Hardware Reality"):
|
| 604 |
+
gr.Markdown("""
|
| 605 |
+
## The Temperature Divide
|
| 606 |
+
|
| 607 |
+
Most quantum computers need extreme cold. Photonics breaks this rule.
|
| 608 |
+
""")
|
| 609 |
+
|
| 610 |
+
hardware_chart = gr.Plot(value=create_hardware_comparison())
|
| 611 |
+
|
| 612 |
+
gr.Markdown("""
|
| 613 |
+
### Platform Breakdown
|
| 614 |
+
|
| 615 |
+
| Platform | Temperature | Advantage | Challenge |
|
| 616 |
+
|----------|-------------|-----------|-----------|
|
| 617 |
+
| Superconducting | 15 mK | Fast gates, mature | Cryogenics cost |
|
| 618 |
+
| Trapped Ions | 1 mK | Long coherence | Slow gates |
|
| 619 |
+
| Photonic | 293 K | Room temp, networking | Probabilistic |
|
| 620 |
+
| Neutral Atoms | 10 渭K | Large arrays | Laser complexity |
|
| 621 |
+
|
| 622 |
+
**Photonic breakthrough:** Xanadu and PsiQuantum are betting that room-temperature
|
| 623 |
+
operation and natural fiber networking will overcome probabilistic gate challenges.
|
| 624 |
+
""")
|
| 625 |
+
|
| 626 |
+
# Tab 4: Energy Calculator
|
| 627 |
+
with gr.TabItem("Green Quantum"):
|
| 628 |
+
gr.Markdown("""
|
| 629 |
+
## The Energy Advantage
|
| 630 |
+
|
| 631 |
+
Quantum computers promise exponential speedups. But what about energy?
|
| 632 |
+
""")
|
| 633 |
+
|
| 634 |
+
problem_slider = gr.Slider(10, 1000, 100, step=10, label="Problem Size (N)")
|
| 635 |
+
energy_chart = gr.Plot(value=create_energy_comparison(100))
|
| 636 |
+
|
| 637 |
+
problem_slider.change(create_energy_comparison, [problem_slider], energy_chart)
|
| 638 |
+
|
| 639 |
+
gr.Markdown("""
|
| 640 |
+
**The calculation:**
|
| 641 |
+
|
| 642 |
+
Classical: O(N鲁) operations for linear algebra
|
| 643 |
+
Quantum: O(N 路 polylog(N)) operations with HHL/QSVT
|
| 644 |
+
|
| 645 |
+
Even accounting for the 25kW dilution refrigerator overhead, quantum wins
|
| 646 |
+
for sufficiently large problems. Photonic systems drop this to ~500W.
|
| 647 |
+
|
| 648 |
+
**Landauer's principle:** Each bit erasure costs kT路ln(2) energy.
|
| 649 |
+
Reversible quantum computation minimizes erasure.
|
| 650 |
+
""")
|
| 651 |
+
|
| 652 |
+
# Tab 5: Circuit Generator
|
| 653 |
+
with gr.TabItem("AI Circuits"):
|
| 654 |
+
gr.Markdown("""
|
| 655 |
+
## AI-Designed Quantum Circuits
|
| 656 |
+
|
| 657 |
+
Modern ML models can design quantum circuits automatically.
|
| 658 |
+
See example OpenQASM output for common algorithms.
|
| 659 |
+
""")
|
| 660 |
+
|
| 661 |
+
with gr.Row():
|
| 662 |
+
problem_dropdown = gr.Dropdown(
|
| 663 |
+
choices=["QAOA (Max-Cut)", "VQE (H2 Molecule)", "Grover's Search"],
|
| 664 |
+
label="Problem Type",
|
| 665 |
+
value="QAOA (Max-Cut)"
|
| 666 |
+
)
|
| 667 |
+
circuit_qubits = gr.Slider(2, 8, 4, step=1, label="Qubits")
|
| 668 |
+
|
| 669 |
+
circuit_output = gr.Code(label="OpenQASM 3.0 Circuit", language="python")
|
| 670 |
+
generate_btn = gr.Button("Generate Circuit", variant="primary")
|
| 671 |
+
|
| 672 |
+
generate_btn.click(
|
| 673 |
+
generate_circuit_description,
|
| 674 |
+
[problem_dropdown, circuit_qubits],
|
| 675 |
+
circuit_output
|
| 676 |
+
)
|
| 677 |
+
|
| 678 |
+
gr.Markdown("""
|
| 679 |
+
**AI Circuit Design on HF:**
|
| 680 |
+
|
| 681 |
+
Models like `linuzj/quantum-circuit-qubo-3B` and `Floki00/qc_srv_3to8qubit`
|
| 682 |
+
use diffusion models and fine-tuned LLMs to generate valid quantum circuits.
|
| 683 |
+
|
| 684 |
+
This represents a shift: instead of humans designing circuits by hand,
|
| 685 |
+
AI explores the vast space of possible architectures.
|
| 686 |
+
""")
|
| 687 |
+
|
| 688 |
+
# Tab 6: Resources
|
| 689 |
+
with gr.TabItem("Resources"):
|
| 690 |
+
gr.Markdown("""
|
| 691 |
+
## Dive Deeper
|
| 692 |
+
|
| 693 |
+
### Key Papers
|
| 694 |
+
|
| 695 |
+
**QSVT Unification**
|
| 696 |
+
- [A Grand Unification of Quantum Algorithms](https://arxiv.org/abs/2105.02859) (2021)
|
| 697 |
+
|
| 698 |
+
**Barren Plateaus**
|
| 699 |
+
- [Does Absence of Barren Plateaus Imply Classical Simulability?](https://arxiv.org/abs/2312.09121) (2023)
|
| 700 |
+
- [Variational Quantum Algorithms Review](https://arxiv.org/abs/2012.09265) (2020)
|
| 701 |
+
|
| 702 |
+
**Photonic Quantum**
|
| 703 |
+
- [Blueprint for Scalable Photonic Fault-Tolerant QC](https://arxiv.org/abs/2010.02905) (2020)
|
| 704 |
+
- [Fusion-Based Quantum Computation](https://arxiv.org/abs/2101.09310) (2021)
|
| 705 |
+
|
| 706 |
+
**AI Circuit Design**
|
| 707 |
+
- [Quantum Circuit Synthesis with Diffusion](https://arxiv.org/abs/2311.02041)
|
| 708 |
+
|
| 709 |
+
### Models on Hugging Face
|
| 710 |
+
|
| 711 |
+
- [linuzj/quantum-circuit-qubo-3B](https://hf.co/linuzj/quantum-circuit-qubo-3B)
|
| 712 |
+
- [Floki00/qc_srv_3to8qubit](https://hf.co/Floki00/qc_srv_3to8qubit)
|
| 713 |
+
|
| 714 |
+
### Spaces
|
| 715 |
+
|
| 716 |
+
- [Floki00/genQC](https://hf.co/spaces/Floki00/genQC) - Quantum circuit generation
|
| 717 |
+
|
| 718 |
+
---
|
| 719 |
+
|
| 720 |
+
**Created by:** Eric Raymond | Purdue AI/Robotics Engineering
|
| 721 |
+
""")
|
| 722 |
+
|
| 723 |
+
gr.Markdown("""
|
| 724 |
+
---
|
| 725 |
+
|
| 726 |
+
*"The quiet revolution in quantum isn't about who has the most qubits.
|
| 727 |
+
It's about who understands the architecture."*
|
| 728 |
+
""")
|
| 729 |
+
|
| 730 |
+
if __name__ == "__main__":
|
| 731 |
+
demo.launch()
|
requirements.txt
ADDED
|
@@ -0,0 +1,3 @@
|
|
|
|
|
|
|
|
|
|
|
|
|
| 1 |
+
gradio>=4.0.0
|
| 2 |
+
numpy>=1.24.0
|
| 3 |
+
plotly>=5.18.0
|