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CROSSWORD
ANSWER

hermitic

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The answer HERMITIC has 2 possible clue(s) in existing crosswords.

Searching in Word Games ...

The word HERMITIC is VALID in some board games. Check HERMITIC in word games in Scrabble, Words With Friends, see scores, anagrams etc.

Searching in Dictionaries ...

Definitions of hermitic in various dictionaries:

adj - characterized by ascetic solitude

noun - one who lives in solitude and seclusion

Word Research / Anagrams and more ...

Keep reading for additional results and analysis below.

Possible Crossword Clues
Living as a recluse
I met rich crook shunning company

Last Seen in these Crosswords & Puzzles
Apr 4 2017 The Guardian - Cryptic crossword
May 1 2005 Premier Sunday - King Feature Syndicate

Possible Dictionary Clues
Of, pertaining to, or typical of a hermit
bDefinitionb of bHERMITICb. : of, relating to, or suited for a hermit. hermitically-tk()l adverb.
characterized by ascetic solitude

Hermitic might refer to
In mathematics, a Self-adjoint operator on a finite-dimensional complex vector space V with inner product * * * * ⟨ * ⋅ * , * ⋅ * ⟩ * * * {\displaystyle \langle \cdot ,\cdot \rangle } * is a linear map A (from V to itself) that is its own adjoint: * * * * ⟨ * A * v * , * w * ⟩ * = * ⟨ * v * , * A * w * ⟩ * * * {\displaystyle \langle Av,w\rangle =\langle v,Aw\rangle } * for all vectors v and w. If V is finite-dimensional with a given orthonormal basis, this is equivalent to the condition that the matrix of A is Hermitian, i.e., equal to its conjugate transpose A∗. By the finite-dimensional spectral theorem, V has an orthonormal basis such that the matrix of A relative to this basis is a diagonal matrix with entries in the real numbers. In this article, we consider generalizations of this concept to operators on Hilbert spaces of arbitrary dimension. * Self-adjoint operators are used in functional analysis and quantum mechanics. In quantum mechanics their importance lies in the Dirac–von Neumann formulation of quantum mechanics, in which physical observables such as position, momentum, angular momentum and spin are represented by self-adjoint operators on a Hilbert space. Of particular significance is the Hamiltonian operator * * * * * * * H * ^ * * * * * * {\displaystyle {\hat {H}}} * defined by* * * * * * * H * ^ * * * * ψ * = * − * * * * ℏ * * 2 * * * * 2 * m * * * * * ∇ * * 2 * * * ψ * + * V * ψ * , * * * {\displaystyle {\hat {H}}\psi =-{\frac {\hbar ^{2}}{2m}}\nabla ^{2}\psi +V\psi ,} * which as an observable corresponds to the total energy of a particle of mass m in a real potential field V. Differential operators are an important class of unbounded operators. * The structure of self-adjoint operators on infinite-dimensional Hilbert spaces essentially resembles the * finite-dimensional case. That is to say, operators are self-adjoint if and only if they are unitarily equivalent to real-valued multiplication operators. With suitable modifications, this result can be extended to possibly unbounded operators on infinite-dimensional spaces. Since an everywhere-defined self-adjoint operator is necessarily bounded, one needs be more attentive to the domain issue in the unbounded case. This is explained below in more detail. * *

Hermitic might refer to

In mathematics, a Self-adjoint operator on a finite-dimensional complex vector space V with inner product
*
*
*
* ⟨
* ⋅
* ,
* ⋅
* ⟩
*
*
* {\displaystyle \langle \cdot ,\cdot \rangle }
* is a linear map A (from V to itself) that is its own adjoint:
*
*
*
* ⟨
* A
* v
* ,
* w
* ⟩
* =
* ⟨
* v
* ,
* A
* w
* ⟩
*
*
* {\displaystyle \langle Av,w\rangle =\langle v,Aw\rangle }
* for all vectors v and w. If V is finite-dimensional with a given orthonormal basis, this is equivalent to the condition that the matrix of A is Hermitian, i.e., equal to its conjugate transpose A∗. By the finite-dimensional spectral theorem, V has an orthonormal basis such that the matrix of A relative to this basis is a diagonal matrix with entries in the real numbers. In this article, we consider generalizations of this concept to operators on Hilbert spaces of arbitrary dimension.
* Self-adjoint operators are used in functional analysis and quantum mechanics. In quantum mechanics their importance lies in the Dirac–von Neumann formulation of quantum mechanics, in which physical observables such as position, momentum, angular momentum and spin are represented by self-adjoint operators on a Hilbert space. Of particular significance is the Hamiltonian operator
*
*
*
*
*
*
* H
* ^
*
*
*
*
*
* {\displaystyle {\hat {H}}}
* defined by*
*
*
*
*
*
* H
* ^
*
*
*
* ψ
* =
* −
*
*
*
* ℏ
*
* 2
*
*
*
* 2
* m
*
*
*
*
* ∇
*
* 2
*
*
* ψ
* +
* V
* ψ
* ,
*
*
* {\displaystyle {\hat {H}}\psi =-{\frac {\hbar ^{2}}{2m}}\nabla ^{2}\psi +V\psi ,}
* which as an observable corresponds to the total energy of a particle of mass m in a real potential field V. Differential operators are an important class of unbounded operators.
* The structure of self-adjoint operators on infinite-dimensional Hilbert spaces essentially resembles the
* finite-dimensional case. That is to say, operators are self-adjoint if and only if they are unitarily equivalent to real-valued multiplication operators. With suitable modifications, this result can be extended to possibly unbounded operators on infinite-dimensional spaces. Since an everywhere-defined self-adjoint operator is necessarily bounded, one needs be more attentive to the domain issue in the unbounded case. This is explained below in more detail.
*
*

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