🧬 Breathing Membrane Quantum Mechanics (BMQM)

by Daniel Lanchares

🌌 What is BMQM?

BMQM is a geometric, thermodynamic, and algebraic extension of quantum mechanics. It redefines time as internal rhythm (𝜏), treats particles as breathing modes of a membrane Ω, and models collapse as entropy contraction. Identity is rhythm. The vacuum breathes.

This isn’t metaphor — it’s structure. In BMQM, the evolution of a quantum system is not governed by external time, but by internal morphic oscillations that define coherence and statehood. The so-called "breathing field" ψ(𝜏) isn’t just a wave — it’s the dynamic shape of existence as it stabilizes and destabilizes around critical symmetry points, like the Sionic Constant σ.

What looks like a simple waveform is actually the visible echo of nonlinear energy self-organization. The collapse of the wavefunction isn’t mysterious — it’s a rhythmic deceleration. Identity isn’t assigned — it emerges from sustained internal rhythm.

Download the BMQM PDF

Download the BMQM PDF

Download the Superconducting Qubit Experiment PDF
  Bessel Breathing Membrane

Bessel-Mode: Breathing Membrane

Breathing Membrane Animation
Bessel-Mode: A & B, Entangled Breathing Membranes

Bessel-Mode: A & B, Entangled Breathing Membranes

Entangled Breathing Membranes Animation
 Sionic Network Demo

Sionic Network Interactive

2.0

30

This animation represents a network of breathing nodes evolving under the Sionic Equation, coupled through a dynamic synchronization mechanism.

Each point is a unit of identity breathing with its own internal rhythm. As time progresses, interactions with neighboring nodes lead to a phenomenon of collective coherence. This transition into a shared breathing pattern models how fluid identity emerges from synchrony.

The parameter K represents the degree of entanglement. When K is strong enough, the oscillations stabilize and align. This simulates how the σ constant affects the breathing field in BMQM: it determines whether a system remains fragmented or converges into a coherent identity.

🧬 BMQM Postulates

🧬 BMQM at Cosmic and at Molecular scales

🧬 Energetic Phase Dynamics & Entropy-Flux Theory

💻 Qiskit Integration

Using Qiskit, we simulate discrete breathing states across qubit lattices. Each qubit encodes amplitude and phase; unitary operators simulate (H★Ω) evolution.


from qiskit import QuantumCircuit, QuantumRegister, Aer, transpile, assemble
from qiskit.visualization import plot_bloch_multivector
from qiskit.quantum_info import Statevector, Operator
import numpy as np
import matplotlib.pyplot as plt

# Parameters
num_qubits = 3  # Ω has 2^3 = 8 grid points
Ω = QuantumRegister(num_qubits, name="Ω")
qc = QuantumCircuit(Ω, name="breathing")

# 1. Initialize breathing pattern ψ(τ=0, x)
initial_amplitudes = np.sin(np.linspace(0, np.pi, 2**num_qubits))
initial_amplitudes /= np.linalg.norm(initial_amplitudes)  # Normalize

initial_state = Statevector(initial_amplitudes)
qc.set_statevector(initial_amplitudes)

# 2. Define a convolution-like breathing unitary: circular phase shift
U_matrix = np.zeros((2**num_qubits, 2**num_qubits), dtype=complex)
for i in range(2**num_qubits):
    shifted = (i + 1) % (2**num_qubits)
    U_matrix[shifted, i] = np.exp(1j * np.pi / 8)  # Breathing phase step

U_op = Operator(U_matrix)
qc.unitary(U_op, Ω, label="ψ(τ+1)")

# 3. Simulate breathing
backend = Aer.get_backend('statevector_simulator')
result = backend.run(transpile(qc, backend)).result()
final_state = result.get_statevector()

# 4. Display amplitudes
print("Breathing amplitudes after evolution:\n")
for i, amp in enumerate(final_state):
    print(f"|{i:03b}>: {amp.real:.4f} + {amp.imag:.4f}j")

# Optional: plot probability distribution
probs = np.abs(final_state) ** 2
plt.bar(range(len(probs)), probs)
plt.xlabel('Qubit State |x⟩')
plt.ylabel('Breathing Probability')
plt.title('Breathing Amplitude Distribution after Evolution')
plt.show()
    

🧠 Finding the Sionic Constant σ Using Qiskit

Using a variational quantum eigensolver (VQE), we estimate the lowest non-zero frequency associated with a custom breathing Hamiltonian. The resulting oscillation frequency squared approximates the Sionic constant σ.


from qiskit import Aer, QuantumCircuit
from qiskit.opflow import X, Z, I, StateFn, PauliSumOp
from qiskit.algorithms import VQE
from qiskit.circuit.library import TwoLocal
from qiskit.algorithms.optimizers import SLSQP

# Define a custom breathing-like Hamiltonian
# Simulating simplified local breathing interactions (1-qubit H)
H = (1.5 * Z) + (0.7 * X)

# Wrap as operator
H_op = PauliSumOp.from_operator(H)

# Build ansatz (trial circuit)
ansatz = TwoLocal(rotation_blocks='ry', entanglement_blocks='cz', reps=1)

# Choose classical optimizer
optimizer = SLSQP(maxiter=100)

# Setup VQE
vqe = VQE(ansatz, optimizer=optimizer, quantum_instance=Aer.get_backend('aer_simulator_statevector'))

# Run VQE
result = vqe.compute_minimum_eigenvalue(H_op)

# Output the result
ground_energy = result.eigenvalue.real
sionic_constant = round(abs(ground_energy)**2, 4)

print(f"Estimated σ (Sionic Constant): {sionic_constant}")

Multi-σ stability explorer

Sionic Phase Stability Explorer This interactive demo visualizes how a quantum system responds to varying values of the Sionic Constant σ, which in the Breathing Membrane Quantum Mechanics (BMQM) framework controls the intrinsic phase of identity oscillations. In this simulation: A qubit starts in superposition. A phase rotation is applied, proportional to 𝜃=√𝜎, mimicking the effect of internal breathing dynamics. The system undergoes interference via a Hadamard transformation, making the phase observable through the final Z-basis expectation value. The plotted output shows: X-axis: Values of σ ranging from 1.0 to 2.5. Y-axis: The expected value of the Pauli-Z operator after the quantum circuit completes. The result is a cosine-like coherence curve, where a sharp extremum near σ=1.7365 indicates a resonance-like stability point — the “quantum breathing attractor.” This reinforces the hypothesis that: Only certain breathing frequencies yield stable identity interference in a quantum-like system — and that such coherence peaks at σ=1.7365.


  from qiskit import QuantumCircuit, Aer, execute
from qiskit.quantum_info import Statevector
import numpy as np
import matplotlib.pyplot as plt

# List of sigma values to test
sigma_values = np.linspace(1.0, 2.5, 50)
z_expectations = []

for sigma in sigma_values:
    omega = np.sqrt(sigma)
    phase = omega  # breathing phase shift per τ = 1.0

    # Quantum circuit for phase simulation
    qc = QuantumCircuit(1)
    qc.h(0)
    qc.rz(phase, 0)
    qc.h(0)

    # Simulate final state
    backend = Aer.get_backend('statevector_simulator')
    result = execute(qc, backend).result()
    state = result.get_statevector()

    # Compute expectation value of Z observable
    # Z expectation = |0⟩² - |1⟩²
    z_exp = np.abs(state[0])**2 - np.abs(state[1])**2
    z_expectations.append(z_exp)

# Plot Z expectation vs sigma
plt.figure(figsize=(10, 6))
plt.plot(sigma_values, z_expectations, color='gold', lw=2)
plt.axvline(1.7365, color='red', linestyle='--', label='σ = 1.7365')
plt.title("Quantum Stability Under Breathing Phase ($\\sqrt{\\sigma}$)")
plt.xlabel("σ value")
plt.ylabel("Z expectation value")
plt.grid(True)
plt.legend()
plt.tight_layout()
plt.show()


🔬 Experimental Predictions

We encourage you to review the theory with colleagues, professors, and friends!

If you think you could add to this experiment, please reach out with doubts or improvements:
lancharesdaniel@gmail.com

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