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Codex 또는 Claude로 설치 이 Prompt를 복사해 Codex, Claude 또는 다른 어시스턴트에 붙여 넣으면 Skill 페이지를 검토하고 설치를 진행할 수 있습니다.
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npx skills add https://github.com/majiayu000/claude-skill-registry --skill qutip명령은 한 줄로 유지됩니다. 복사하기 전에 가로로 스크롤해 전체 내용을 확인하세요.
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SKILL.md 표시 중
| category | Research |
| id | qutip |
| name | Qutip |
| description | Quantum mechanics simulations and analysis using QuTiP (Quantum Toolbox in Python). |
QuTiP provides comprehensive tools for simulating and analyzing quantum mechanical systems. It handles both closed (unitary) and open (dissipative) quantum systems with multiple solvers optimized for different scenarios.
uv pip install qutip
Optional packages for additional functionality:
# Quantum information processing (circuits, gates)
uv pip install qutip-qip
# Quantum trajectory viewer
uv pip install qutip-qtrl
from qutip import *
import numpy as np
import matplotlib.pyplot as plt
# Create quantum state
psi = basis(2, 0) # |0⟩ state
# Create operator
H = sigmaz() # Hamiltonian
# Time evolution
tlist = np.linspace(0, 10, 100)
result = sesolve(H, psi, tlist, e_ops=[sigmaz()])
# Plot results
plt.plot(tlist, result.expect[0])
plt.xlabel('Time')
plt.ylabel('⟨σz⟩')
plt.show()
Create and manipulate quantum states and operators:
# States
psi = basis(N, n) # Fock state |n⟩
psi = coherent(N, alpha) # Coherent state |α⟩
rho = thermal_dm(N, n_avg) # Thermal density matrix
# Operators
a = destroy(N) # Annihilation operator
H = num(N) # Number operator
sx, sy, sz = sigmax(), sigmay(), sigmaz() # Pauli matrices
# Composite systems
psi_AB = tensor(psi_A, psi_B) # Tensor product
See references/core_concepts.md for comprehensive coverage of quantum objects, states, operators, and tensor products.
Multiple solvers for different scenarios:
# Closed systems (unitary evolution)
result = sesolve(H, psi0, tlist, e_ops=[num(N)])
# Open systems (dissipation)
c_ops = [np.sqrt(0.1) * destroy(N)] # Collapse operators
result = mesolve(H, psi0, tlist, c_ops, e_ops=[num(N)])
# Quantum trajectories (Monte Carlo)
result = mcsolve(H, psi0, tlist, c_ops, ntraj=500, e_ops=[num(N)])
Solver selection guide:
sesolve: Pure states, unitary evolutionmesolve: Mixed states, dissipation, general open systemsmcsolve: Quantum jumps, photon counting, individual trajectoriesbrmesolve: Weak system-bath couplingfmmesolve: Time-periodic Hamiltonians (Floquet)See references/time_evolution.md for detailed solver documentation, time-dependent Hamiltonians, and advanced options.
Compute physical quantities:
# Expectation values
n_avg = expect(num(N), psi)
# Entropy measures
S = entropy_vn(rho) # Von Neumann entropy
C = concurrence(rho) # Entanglement (two qubits)
# Fidelity and distance
F = fidelity(psi1, psi2)
D = tracedist(rho1, rho2)
# Correlation functions
corr = correlation_2op_1t(H, rho0, taulist, c_ops, A, B)
w, S = spectrum_correlation_fft(taulist, corr)
# Steady states
rho_ss = steadystate(H, c_ops)
See references/analysis.md for entropy, fidelity, measurements, correlation functions, and steady state calculations.
Visualize quantum states and dynamics:
# Bloch sphere
b = Bloch()
b.add_states(psi)
b.show()
# Wigner function (phase space)
xvec = np.linspace(-5, 5, 200)
W = wigner(psi, xvec, xvec)
plt.contourf(xvec, xvec, W, 100, cmap='RdBu')
# Fock distribution
plot_fock_distribution(psi)
# Matrix visualization
hinton(rho) # Hinton diagram
matrix_histogram(H.full()) # 3D bars
See references/visualization.md for Bloch sphere animations, Wigner functions, Q-functions, and matrix visualizations.
Specialized techniques for complex scenarios:
# Floquet theory (periodic Hamiltonians)
T = 2 * np.pi / w_drive
f_modes, f_energies = floquet_modes(H, T, args)
result = fmmesolve(H, psi0, tlist, c_ops, T=T, args=args)
# HEOM (non-Markovian, strong coupling)
from qutip.nonmarkov.heom import HEOMSolver, BosonicBath
bath = BosonicBath(Q, ck_real, vk_real)
hsolver = HEOMSolver(H_sys, [bath], max_depth=5)
result = hsolver.run(rho0, tlist)
# Permutational invariance (identical particles)
psi = dicke(N, j, m) # Dicke states
Jz = jspin(N, 'z') # Collective operators
See references/advanced.md for Floquet theory, HEOM, permutational invariance, stochastic solvers, superoperators, and performance optimization.
# System parameters
N = 20 # Hilbert space dimension
omega = 1.0 # Oscillator frequency
kappa = 0.1 # Decay rate
# Hamiltonian and collapse operators
H = omega * num(N)
c_ops = [np.sqrt(kappa) * destroy(N)]
# Initial state
psi0 = coherent(N, 3.0)
# Time evolution
tlist = np.linspace(0, 50, 200)
result = mesolve(H, psi0, tlist, c_ops, e_ops=[num(N)])
# Visualize
plt.plot(tlist, result.expect[0])
plt.xlabel('Time')
plt.ylabel('⟨n⟩')
plt.title('Photon Number Decay')
plt.show()
# Create Bell state
psi0 = bell_state('00')
# Local dephasing on each qubit
gamma = 0.1
c_ops = [
np.sqrt(gamma) * tensor(sigmaz(), qeye(2)),
np.sqrt(gamma) * tensor(qeye(2), sigmaz())
]
# Track entanglement
def compute_concurrence(t, psi):
rho = ket2dm(psi) if psi.isket else psi
return concurrence(rho)
tlist = np.linspace(0, 10, 100)
result = mesolve(qeye([2, 2]), psi0, tlist, c_ops)
# Compute concurrence for each state
C_t = [concurrence(state.proj()) for state in result.states]
plt.plot(tlist, C_t)
plt.xlabel('Time')
plt.ylabel('Concurrence')
plt.title('Entanglement Decay')
plt.show()
# System parameters
N = 10 # Cavity Fock space
wc = 1.0 # Cavity frequency
wa = 1.0 # Atom frequency
g = 0.05 # Coupling strength
# Operators
a = tensor(destroy(N), qeye(2)) # Cavity
sm = tensor(qeye(N), sigmam()) # Atom
# Hamiltonian (RWA)
H = wc * a.dag() * a + wa * sm.dag() * sm + g * (a.dag() * sm + a * sm.dag())
# Initial state: cavity in coherent state, atom in ground state
psi0 = tensor(coherent(N, 2), basis(2, 0))
# Dissipation
kappa = 0.1 # Cavity decay
gamma = 0.05 # Atomic decay
c_ops = [np.sqrt(kappa) * a, np.sqrt(gamma) * sm]
# Observables
n_cav = a.dag() * a
n_atom = sm.dag() * sm
# Evolve
tlist = np.linspace(0, 50, 200)
result = mesolve(H, psi0, tlist, c_ops, e_ops=[n_cav, n_atom])
# Plot
fig, axes = plt.subplots(2, 1, figsize=(8, 6), sharex=True)
axes[0].plot(tlist, result.expect[0])
axes[0].set_ylabel('⟨n_cavity⟩')
axes[1].plot(tlist, result.expect[1])
axes[1].set_ylabel('⟨n_atom⟩')
axes[1].set_xlabel('Time')
plt.tight_layout()
plt.show()
sesolve for pure states is faster than mesolve'cos(w*t)') is fasteste_ops instead of storing all statesOptionsmcsolve automatically uses multiple CPUsntraj, Hilbert space size, and tolerancesMemory issues: Reduce Hilbert space dimension, use store_final_state option, or consider Krylov methods
Slow simulations: Use string-based time-dependence, increase tolerances slightly, or try method='bdf' for stiff problems
Numerical instabilities: Decrease time steps (nsteps option), increase tolerances, or check Hamiltonian/operators are properly defined
Import errors: Ensure QuTiP is installed correctly; quantum gates require qutip-qip package
This skill includes detailed reference documentation:
references/core_concepts.md: Quantum objects, states, operators, tensor products, composite systemsreferences/time_evolution.md: All solvers (sesolve, mesolve, mcsolve, brmesolve, etc.), time-dependent Hamiltonians, solver optionsreferences/visualization.md: Bloch sphere, Wigner functions, Q-functions, Fock distributions, matrix plotsreferences/analysis.md: Expectation values, entropy, fidelity, entanglement measures, correlation functions, steady statesreferences/advanced.md: Floquet theory, HEOM, permutational invariance, stochastic methods, superoperators, performance tipsLLM token logprobs and calibration. Per-decision confidence, ECE, Brier, reliability diagrams, low-confidence triage.
Analyze LLM token logprobs and calibration. Use for per-decision confidence, ECE, Brier scores, reliability diagrams, and low-confidence triage.
回顾最近 N 天的 Claude Code 使用记录——扫描原始会话数据,按主题分组汇总"我都做了什么",并从个人操作系统视角输出模式、风险与增删建议。当用户说 /recap、"看看我这几天做了什么"、"回顾一下我最近的会话"、"这两天我用 claude 干了啥"、"活动回顾" 时使用。
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