Abstract
This technical specification details the software architecture, algorithmic translation, and mathematical mapping required to execute scalar universe interactions (Ξ-scalar dynamics) on modern quantum hardware backends. By mapping continuous scalar field parameters and inter-system coupling into discrete Hamiltonian matrix representations, we establish a two-qubit unitary time-evolution protocol U(t) = exp(-i * H_Ξ * t). Furthermore, we provide a complete, modular, and deployable Python software architecture equipped with both a Streamlit graphical user interface (GUI) and direct integration with IBM Quantum Cloud execution services.
1. Theoretical & Mathematical Foundations
To execute scalar simulations on Quantum Processing Units (QPUs), continuous field variables must be mapped onto a discrete Hilbert space defined by N qubits.
1.1 State Mapping & Encoding
For a 2-qubit system (N = 2), the composite state vector |ψ> spans a 4-dimensional complex Hilbert space:
|ψ(t)> = c0 |00> + c1 |01> + c2 |10> + c3 |11>
Where: Σ |c_i|² = 1 (for i = 0 to 3)
1.2 Hamiltonian Formulation (H_Ξ)
The parameterized scalar Hamiltonian H_Ξ is constructed using Pauli spin matrices (σ_z, σ_x) and identity matrices (I):
H_Ξ = Ξ • (σ_z ⊗ I) + g • (σ_x ⊗ σ_x)
- Ξ: Primary scalar parameter (e.g., Ξ = 1.618).
- g: Inter-system coupling coefficient.
- (σ_z ⊗ I): Localized field dynamics operator.
- (σ_x ⊗ σ_x): Cross-system interaction term.
1.3 Unitary Time-Evolution
U(Δt) = exp(-i • H_Ξ • Δt)
|ψ(t + Δt)> = U(Δt) |ψ(t)>
2. Software Architecture
scalar_quantum_sim/
├── core/
│ ├── __init__.py
│ ├── hamiltonian.py (Construct scalar operators and matrices)
│ └── engine.py (Quantum state evolution & IBM QPU driver)
└── app.py (Streamlit Web GUI & interactive dashboard)
3. Production Code Base
3.1 Scalar Hamiltonian Builder (core/hamiltonian.py)
import numpy as np
class ScalarHamiltonianBuilder:
"""Constructs parameterized Hamiltonian operators from scalar field metrics."""
def __init__(self):
self.I = np.array([[1, 0], [0, 1]], dtype=complex)
self.X = np.array([[0, 1], [1, 0]], dtype=complex)
self.Z = np.array([[1, 0], [0, -1]], dtype=complex)
def build_custom_operator(self, xi_scalar: float, coupling: float) -> np.ndarray:
"""
Generates the 4x4 matrix representation of H_Xi.
H_Xi = Xi * (Z x I) + g * (X x X)
"""
H_field = xi_scalar * np.kron(self.Z, self.I)
H_interaction = coupling * np.kron(self.X, self.X)
return H_field + H_interaction
3.2 Quantum Execution Engine (core/engine.py)
import numpy as np
from scipy.linalg import expm
from qiskit import QuantumCircuit
from qiskit.quantum_info import Operator, Statevector
from qiskit_ibm_runtime import QiskitRuntimeService, SamplerV2 as Sampler
class QuantumSimulationEngine:
"""Handles time evolution compilation and dispatch to ideal simulators or IBM QPUs."""
def __init__(self, hamiltonian: np.ndarray, num_qubits: int = 2):
self.H = hamiltonian
self.num_qubits = num_qubits
def generate_evolution_circuit(self, time_delta: float) -> QuantumCircuit:
"""Synthesizes the continuous operator into a Qiskit QuantumCircuit."""
U = expm(-1j * self.H * time_delta)
qc = QuantumCircuit(self.num_qubits)
qc.h(0) # Initial state preparation
qc.append(Operator(U), range(self.num_qubits))
qc.measure_all()
return qc
def run_local_ideal(self, time_delta: float) -> dict:
"""Executes exact statevector evolution locally."""
U = expm(-1j * self.H * time_delta)
qc = QuantumCircuit(self.num_qubits)
qc.h(0)
qc.append(Operator(U), range(self.num_qubits))
state = Statevector.from_label('00').evolve(qc)
return {
"mode": "Local Statevector (Ideal)",
"probabilities": state.probabilities_dict(),
"statevector": state.data,
"circuit": qc
}
def run_ibm_quantum(self, time_delta: float, api_token: str, backend_name: str = "ibm_brisbane", shots: int = 1024) -> dict:
"""Submits synthesized circuits to remote IBM Quantum processing units."""
qc = self.generate_evolution_circuit(time_delta)
service = QiskitRuntimeService(channel="ibm_quantum", token=api_token)
backend = service.backend(backend_name)
sampler = Sampler(mode=backend)
job = sampler.run([qc], shots=shots)
result = job.result()
pub_result = result[0]
counts = pub_result.data.meas.get_counts()
total_shots = sum(counts.values())
probs = {state: count / total_shots for state, count in counts.items()}
return {
"mode": f"IBM Quantum ({backend_name})",
"probabilities": probs,
"counts": counts,
"job_id": job.job_id(),
"circuit": qc
}
3.3 Streamlit GUI Dashboard (app.py)
import streamlit as st
import pandas as pd
from core.hamiltonian import ScalarHamiltonianBuilder
from core.engine import QuantumSimulationEngine
st.set_page_config(page_title="Scalar Quantum Simulator", page_icon="⚛️", layout="wide")
st.title("⚛️ Scalar Quantum Simulator Dashboard")
st.markdown("Bridge abstract scalar frameworks into executable quantum algorithms.")
# Sidebar Controls
st.sidebar.header("🎛️ System Control Panel")
xi_val = st.sidebar.slider("Xi Parameter (Xi)", min_value=0.0, max_value=5.0, value=1.618, step=0.01)
coupling_val = st.sidebar.slider("Coupling Coefficient (g)", min_value=0.0, max_value=2.0, value=0.50, step=0.05)
time_val = st.sidebar.slider("Evolution Delta (t)", min_value=0.1, max_value=10.0, value=1.0, step=0.1)
backend_mode = st.sidebar.radio("Backend Mode:", ["Local Simulator (Ideal)", "Real IBM Quantum QPU"])
ibm_api_token = ""
ibm_backend_choice = "ibm_brisbane"
if backend_mode == "Real IBM Quantum QPU":
ibm_api_token = st.sidebar.text_input("IBM Quantum API Token", type="password")
ibm_backend_choice = st.sidebar.selectbox("Target Hardware Backend", ["ibm_brisbane", "ibm_kyoto", "ibm_osaka"])
run_button = st.sidebar.button("🚀 Execute Simulation", type="primary")
if run_button:
builder = ScalarHamiltonianBuilder()
H_matrix = builder.build_custom_operator(xi_scalar=xi_val, coupling=coupling_val)
engine = QuantumSimulationEngine(H_matrix)
with st.spinner("Executing simulation pipeline..."):
try:
if backend_mode == "Local Simulator (Ideal)":
results = engine.run_local_ideal(time_delta=time_val)
else:
if not ibm_api_token:
st.error("Authentication Error: An IBM Quantum API Token is required.")
st.stop()
results = engine.run_ibm_quantum(
time_delta=time_val,
api_token=ibm_api_token,
backend_name=ibm_backend_choice
)
col1, col2 = st.columns([1, 1])
with col1:
st.subheader("📊 Basis State Measurement Probabilities")
df_probs = pd.DataFrame(
list(results["probabilities"].items()),
columns=["Basis State |q1 q0>", "Probability"]
).sort_values(by="Basis State |q1 q0>")
st.bar_chart(df_probs.set_index("Basis State |q1 q0>"))
st.dataframe(df_probs, use_container_width=True)
with col2:
st.subheader("⚙️ Quantum Circuit Assembly")
st.markdown(f"**Execution Engine:** `{results['mode']}`")
if "job_id" in results:
st.success(f"**Hardware Job ID:** `{results['job_id']}`")
st.code(str(results["circuit"].draw(output="text")), language="text")
except Exception as e:
st.error(f"Runtime Execution Failure: {str(e)}")
4. Launch Instructions
# Install required packages
pip install qiskit qiskit-ibm-runtime scipy numpy pandas streamlit
# Launch the Dashboard
streamlit run app.py
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