Genuine restrictions between any two finite cylinder Sobolev orders.
The same derivative word at a larger Sobolev order.
Instances For
@[simp]
theorem
EulerCylinderSobolevSpace.restrictOperator_apply
(period : ℝ)
[Fact (0 < period)]
{p q : ℕ}
(h : q ≤ p)
(u : ↥(SobolevSpace period p))
(w : SobolevWord q)
:
@[simp]
theorem
EulerCylinderSobolevSpace.value_restrictOperator
(period : ℝ)
[Fact (0 < period)]
{p q : ℕ}
(h : q ≤ p)
(u : ↥(SobolevSpace period p))
:
theorem
EulerCylinderSobolevSpace.restrictOperator_bound
(period : ℝ)
[Fact (0 < period)]
{p q : ℕ}
(h : q ≤ p)
(u : ↥(SobolevSpace period p))
:
@[simp]
theorem
EulerCylinderSobolevSpace.restrictOperator_self
(period : ℝ)
[Fact (0 < period)]
{q : ℕ}
(u : ↥(SobolevSpace period q))
:
@[simp]
theorem
EulerCylinderSobolevSpace.restrictOperator_comp
(period : ℝ)
[Fact (0 < period)]
{p q r : ℕ}
(hqp : q ≤ p)
(hrq : r ≤ q)
(u : ↥(SobolevSpace period p))
:
@[simp]
theorem
EulerCylinderSobolevSpace.restrictOperator_truncate
(period : ℝ)
[Fact (0 < period)]
{p q : ℕ}
(h : q ≤ p)
(u : ↥(SobolevSpace period (p + 1)))
:
@[simp]
theorem
EulerCylinderSobolevSpace.truncate_restrictOperator
(period : ℝ)
[Fact (0 < period)]
{p q : ℕ}
(h : q + 1 ≤ p)
(u : ↥(SobolevSpace period p))
:
theorem
EulerCylinderSobolevSpace.restrictOperator_derivative
(period : ℝ)
[Fact (0 < period)]
{p q : ℕ}
(h : q ≤ p)
(i : Fin 4)
(u : ↥(SobolevSpace period (p + 1)))
:
(restrictOperator period h) ((derivativeOperator period p i) u) = (derivativeOperator period q i) ((restrictOperator period ⋯) u)
Actual restriction and spatial differentiation commute.
theorem
EulerCylinderSobolevSpace.restrictOperator_translation
(period : ℝ)
[Fact (0 < period)]
{p q : ℕ}
(h : q ≤ p)
(a : EulerLiftedGradientSpace.LiftDomain period)
(u : ↥(SobolevSpace period p))
:
(restrictOperator period h) ((sobolevTranslation period p a) u) = (sobolevTranslation period q a) ((restrictOperator period h) u)
Restriction commutes with every genuine cylinder translation.