Sentence examples for definite properties of from inspiring English sources

Einstein believed that particles have definite properties of their own, independent of what we choose to measure, and that local actions produce only local effects — that what Toby orders has no bearing on what Ellie orders.

Since D is non-negative, combining the negative definite properties of (mathcal{M}) and Lemma 4, we obtain that sigma(A)=sigma(Dmathcal{M} subseteqmathcal{W}(D mathcal {W}( mathcal{M} subseteqbigl{ deltainmathbb{C}|operatorname{Re}(delta)< 0bigr}.

By the positive definite property of A, the first eigenvalue (mu _{1}>0).

However, this estimate does not preserve the positive definite property of the difference.

By the positive definite property of A, the first eigenvalue λ1 > 0. From [16, 17], we know that -A generates an analytic operator semigroup T (t)(t ≥ 0) on H, which is exponentially stable and satisfies | | T ( t ) | | ≤ e - λ 1 t, ∀ t ≥ 0. (6).

Moreover, the symmetric positive-definite property of the coefficient matrix on an (N−1 -dimensional hyperplaN−1 -dimensional fundamental importance to thyperplanesedness of the models — can be proved equivalent to some physical condition for pairwhichsurface tensisns.

Based on the positive-definite property of the matrix resulting from the multiplication of the MIMO channel matrix H by its Hermitian H H, β j values and the matrices determinants (Δ E ), (Δ A ), and ((phantom {dot {i}!}Delta _{mathbf {D - CA^{-1}B}})) are proved to be positive real numbers.

Accordingly, one cannot get away with simply specifying the definite properties at each instant of time.

For on the one hand, by applying mathematical induction – i.e. the principle that for all definite properties \(P x)\) of natural numbers, we may infer \(\forall x P x)\) from \(P 0)\) and \(\forall x(P x) \rightarrow P(x+1))\) – to the predicate \(F x)\), we may conclude that \(\forall x F x)\) from (i) and (ii).

The theory envisions that a string undergoing a particular mode of vibration corresponds to a particle with definite properties such as mass and charge.

Anticipating the work of the Phenomenologists, Meinong maintained that objects remain objects and have a definite character and definite properties (Sosein) even if they have no being (Sein).