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Definitions are deliberately short. Each lesson defines its terms again in context, with the assumptions that apply.

Amplitude
A complex number attached to a possible outcome of a quantum state. The probability of the outcome in an ideal measurement is the squared magnitude of its amplitude (the Born rule).
Average treatment effect (ATE)
The mean difference between the outcomes a population would have under treatment and under no treatment, E[Y(1)−Y(0)]E[Y(1) - Y(0)].
Back-door criterion
A graphical condition on a set of variables ZZ: no member of ZZ is a descendant of XX, and ZZ blocks every path from XX to YY that starts with an arrow into XX. If it holds, adjusting for ZZ identifies the effect of XX on YY.
Barren plateau
A region of a variational circuit’s parameter space where gradients are exponentially small in the number of qubits, which makes training by gradient descent impractical.
Bayes’ rule
P(H∣E)=P(E∣H) P(H)/P(E)P(H\mid E) = P(E\mid H)\,P(H) / P(E). It updates the probability of a hypothesis HH after seeing evidence EE.
Bell inequality
A bound on correlations that every local hidden-variable model satisfies. Some measurements on entangled quantum states violate it.
Bloch sphere
A geometric picture of single-qubit states: pure states lie on the surface of a unit sphere, mixed states inside it.
Causal discovery
Inferring a causal graph, or a set of graphs that fit equally well, from data plus explicit assumptions such as the causal Markov condition and faithfulness.
Causal graph (DAG)
A directed acyclic graph whose arrows represent direct causal influences among variables.
CHSH inequality
The Clauser–Horne–Shimony–Holt form of a Bell inequality, ∣S∣≤2|S| \le 2 for local hidden-variable models. Quantum mechanics allows up to 222\sqrt{2} (Tsirelson’s bound).
Choi matrix
A matrix that represents a quantum channel completely. The channel is completely positive exactly when its Choi matrix is positive semidefinite.
Classical shadow
A compact classical description of a quantum state built from randomized measurements. It can estimate many properties of the state from relatively few measurements.
Collider
A variable with two arrows pointing into it on a path, as X→C←YX \to C \leftarrow Y. Conditioning on a collider can create an association between XX and YY that is not causal.
Common cause
A variable that influences two others. An unmeasured common cause (a confounder) can create correlation without direct causation between the two.
Complete positivity
The property that a map stays positive when it acts on part of a larger system. Physical quantum channels are completely positive and trace preserving (CPTP).
Concurrence
A measure of entanglement for two qubits, from 0 (not entangled) to 1 (maximally entangled).
Confounding
Bias in an estimated causal effect caused by a common cause of treatment and outcome that the analysis does not account for.
Counterfactual
A statement about what would have happened to the same unit under a different action, given what actually happened.
Density matrix
A positive semidefinite matrix with trace one. It describes pure and mixed quantum states.
do-operator
Pearl’s notation do(X=x)do(X = x) for an intervention that sets XX to xx by an external action, cutting the arrows into XX in the causal graph.
Entanglement
A joint quantum state is entangled when it cannot be written as a probabilistic mixture of product states.
Entropy
A measure of uncertainty. Shannon entropy applies to probability distributions; von Neumann entropy, −Tr⁡ρlog⁡ρ-\operatorname{Tr}\rho\log\rho, applies to density matrices.
Expectation value
The probability-weighted average of measurement outcomes, ⟨A⟩=Tr⁡(ρA)\langle A \rangle = \operatorname{Tr}(\rho A) for a quantum observable AA.
Faithfulness
The assumption that every conditional independence in the data follows from the causal graph and is not due to an exact cancellation of effects.
Front-door criterion
A graphical condition that identifies a causal effect through a fully observed mediator even when the treatment and outcome share an unmeasured common cause.
Hermitian matrix
A matrix equal to its conjugate transpose. Its eigenvalues are real; quantum observables are represented by Hermitian operators.
Identification
Showing that a causal quantity can be computed from the distribution of observed data under stated assumptions.
Indefinite causal order
A situation, described by process matrices, in which the operations cannot be assigned a definite order, nor any probabilistic mixture of definite orders (causal nonseparability). A random but classical choice of order is not indefinite; the quantum switch with its control in superposition is the standard example.
Interference
The effect produced when amplitudes for different paths add, so that outcome probabilities depend on relative phase.
Intervention
An action that sets or changes a variable from outside the system, as opposed to passively observing it.
Kraus operators
Matrices KkK_k that represent a quantum channel as ρ↦∑kKkρKk†\rho \mapsto \sum_k K_k \rho K_k^\dagger, with ∑kKk†Kk=I\sum_k K_k^\dagger K_k = I for trace preservation.
Parameter-shift rule
A rule that computes exact gradients of many variational quantum circuits from the circuit’s outputs at two shifted parameter values.
Partial trace
The operation that gives the state of a subsystem from the state of a larger joint system.
Process matrix
An operator that describes how local quantum operations in several laboratories are connected, without assuming a fixed causal order between them.
Quantum causal model
A causal model in which the nodes are quantum systems or quantum operations and the mechanisms are quantum channels, generalizing classical structural causal models.
Quantum channel
A completely positive, trace-preserving linear map that describes how a quantum state can change, including noise.
Quantum switch
A process in which a control qubit determines the order in which two operations act on a target; with the control in superposition, the order is indefinite.
Qubit
A two-level quantum system, the quantum counterpart of a bit.
Randomized controlled trial
An experiment in which treatment is assigned by a random mechanism, which balances measured and unmeasured characteristics between groups on average.
Structural causal model (SCM)
A set of equations, one per variable, that determine each variable from its direct causes and an exogenous noise term, together with a distribution over the noise terms.
Superposition
A quantum state that is a linear combination of other states, such as α∣0⟩+β∣1⟩\alpha|0\rangle + \beta|1\rangle.
Variational quantum algorithm
A hybrid method in which a classical optimizer tunes the parameters of a quantum circuit to minimize a cost estimated from measurements.