Linear Vector Spaces and Operators

Quantum Mechanics A

Schrödinger Equation The most fundamental equation of quantum mechanics; given a Hamiltonian Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle \mathcal{H}} , it describes how a state Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle |\Psi\rangle} evolves in time.

Physical Basis of Quantum Mechanics

Basic Concepts and Theory of Motion UV Catastrophe (Black-Body Radiation) Photoelectric Effect Stability of Matter Double Slit Experiment Stern-Gerlach Experiment The Principle of Complementarity The Correspondence Principle The Philosophy of Quantum Theory

Schrödinger Equation

Brief Derivation of Schrödinger Equation Relation Between the Wave Function and Probability Density Stationary States Heisenberg Uncertainty Principle Some Consequences of the Uncertainty Principle

Operators, Eigenfunctions, and Symmetry

Linear Vector Spaces and Operators Commutation Relations and Simultaneous Eigenvalues The Schrödinger Equation in Dirac Notation Transformations of Operators and Symmetry Time Evolution of Expectation Values and Ehrenfest's Theorem

Motion in One Dimension

One-Dimensional Bound States Oscillation Theorem The Dirac Delta Function Potential Scattering States, Transmission and Reflection Motion in a Periodic Potential Summary of One-Dimensional Systems

Discrete Eigenvalues and Bound States

Harmonic Oscillator Spectrum and Eigenstates Analytical Method for Solving the Simple Harmonic Oscillator Coherent States Charged Particles in an Electromagnetic Field WKB Approximation

Time Evolution and the Pictures of Quantum Mechanics

The Heisenberg Picture: Equations of Motion for Operators The Interaction Picture The Virial Theorem

Angular Momentum

Commutation Relations Angular Momentum as a Generator of Rotations in 3D Spherical Coordinates Eigenvalue Quantization Orbital Angular Momentum Eigenfunctions

Central Forces

General Formalism Free Particle in Spherical Coordinates Spherical Well Isotropic Harmonic Oscillator Hydrogen Atom WKB in Spherical Coordinates

The Path Integral Formulation of Quantum Mechanics

Feynman Path Integrals The Free-Particle Propagator Propagator for the Harmonic Oscillator

Continuous Eigenvalues and Collision Theory

Differential Cross Section and the Green's Function Formulation of Scattering Central Potential Scattering and Phase Shifts Coulomb Potential Scattering

Quantum Mechanics can be conveniently formulated in the language of abstract state vectors, from which the various representations (wave mechanics, matrix mechanics, Schrödinger, Heisenberg and interaction pictures, etc.) can be derived. A formulation of quantum mechanics in terms of linear vector spaces hinges on the fact that the Schrödinger equation is linear. An operator is a mathematical operation performed on a vector belonging to a linear vector space, the result of which is another vector belonging to the same linear vector space.

The Vector (Ket) Space

In quantum mechanics a physical state is represented by a state vector in a complex vector space and have all the properties described above. Following Dirac, we call such a vector a "ket", denoted by Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle |\alpha\rangle} . This state ket is postulated to contain complete information about the physical state (i.e. everything we are allowed to ask about the state is contained in the ket). The complex linear vector spaces that we work with in quantum mechanics are usually infinite dimensional. In this case, the vector space in question is known as a Hilbert space after D. Hilbert, who studied vector spaces in infinite dimensions.

One of the postulates of quantum mechanics is that Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle |\alpha\rangle} and Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle c|\alpha\rangle,} with Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle c\neq 0,} represent the same physical state. In other words, only the ”direction” in vector space is of significance.

The Dual (Bra) Space

The vector space we have been dealing with is a ket space. We now introduce the notion of a "bra" space, a vector space ”dual to” the ket space. We postulate that corresponding to every ket Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle |\alpha\rangle} there exists a bra denoted by Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle \langle\alpha |} in this dual or bra space. The bra space is spanned by a set of bra vectors Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle \left \{\langle\alpha |\right \}} which correspond to the set of kets Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle \left \{|\alpha\rangle\right \}.} Mathematically, the dual space is a set of linear functions Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle \langle\beta|: V \rightarrow C } that act on the members of the corresponding vector space (kets) where Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle V} is the vector space and Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle C} is the set of complex numbers.

There is a one to one correspondence between the members of a ket space and those of the corresponding bra space, Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle |\alpha\rangle\leftrightarrow\langle\alpha |,} where Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle \leftrightarrow} stands for dual correspondence. Roughly speaking, we can regard the bra space as some kind of "mirror image" of the ket space.

The bra dual to Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle c|\alpha\rangle} is postulated to be Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle c^{\ast}\langle\alpha |} , not Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle c\langle\alpha |,} which is a very important point to note. More generally, we have

Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle c_{\alpha}|\alpha\rangle+c_{\beta}|\beta\rangle+\cdots\leftrightarrow c^{\ast}_{\alpha}\langle\alpha |+c^{\ast}_{\beta}\langle\beta |+\cdots}

Linear Independence and Bases

Consider Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle N\!} vectors (ket states) Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle |1\rangle } ,Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle |2\rangle,\ldots,|N\rangle.} They are linearly independent if the relation Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle \sum_{i=1}^{N}c_i|i\rangle=0 } necessarily implies Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle c_i=0 \!} for Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle i = 1,2,...,N\!} . They can be used as basis in a vector space, and decomposition of any vector in terms of basis vectors in unique.

While any set of linearly independent vectors can be used as a basis, normally the discussion is greatly simplified if the basis is orthonormal, i.e Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle \langle i|j \rangle=\delta_{ij}} . The action of an operator is completely known once its action on each of the basis vectors of Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle \mathit{V}} is given.

The Hilbert Space

A Hilbert space Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle H\!} consisting of a set of vectors Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle \psi,\phi,\chi,\ldots\!} and a set of scalars Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle a,b,c,\ldots\!} obeys the following properties.

(a) Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle H\!} is a linear vector space. It obeys all the properties of a linear vector space as mentioned in the previous section.

(b) The scalar product defined in Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle H\!} is strictly positive. The scalar product of one element Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle \phi\!} with another element Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle \psi\!} is a complex number, denoted by Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle \langle\phi|\psi\rangle} . This scalar satisfies the following properties.

1. The scalar product of Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle \phi\!} with Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle \psi\!} is same as the complex conjugate of the scalar product of Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle \psi\!} with Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle \phi\!} .

             Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle \langle\phi|\psi\rangle}
=Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle \langle\psi|\phi\rangle^{\ast}}

2. The scalar product of Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle \psi\!} with Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle \phi\!} is linear with respect to Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle \phi\!} .

            Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle \langle\psi|a\psi_{1} + b\psi_{2}\rangle}
 = Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle a\langle\psi|\phi_{1}\rangle + b\langle\psi|\phi_{2}\rangle}

3. The scalar product of a state vector Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle \psi\!} with itself is a positive real number.

              Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle \langle\psi|\psi\rangle=|\psi|^2\geq 0 }

Schwartz Inequality

For two states Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle |\psi\rangle} and Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle |\phi\rangle} belonging to a linear vector space, the following theorem, known as the Schwartz inequality, holds:

                          $|\langle \psi |\phi \rangle |^{2}\leq \langle \psi |\psi \rangle \langle \phi |\phi \rangle$

If the vectors $|\psi \rangle$and $|\phi \rangle$are linearly dependent, i.e. $|\psi \rangle$=$\alpha |\phi \rangle ,$ then the above relation becomes an equality.

Proof: Let $|\psi \rangle$ and $|\phi \rangle$ be arbitrary vectors in the vector space $V.$ The inequality is trivial in the case that at least one of $|\psi \rangle$ and $|\phi \rangle =0,$ so we will consider the case that both are nonzero. Let $\lambda$ be a complex number. Then

$0\leq \langle \psi -\lambda \phi |\psi -\lambda \phi \rangle =\langle \psi |\psi \rangle -\lambda ^{\ast }\langle \psi |\phi \rangle -\lambda \langle \phi |\psi \rangle +|\lambda |^{2}\langle \phi |\phi \rangle .$

The above expression is valid for any number $\lambda$. The right-hand side of the above expression is minimized if we choose

$\lambda ={\frac {\langle \psi |\phi \rangle }{\langle \phi |\phi \rangle }}.$

Using this value of $\lambda ,$ we obtain

$0\leq \langle \psi |\psi \rangle -{\frac {|\langle \psi |\phi \rangle |^{2}}{\langle \phi |\phi \rangle }},$

or

$|\langle \psi |\phi \rangle |^{2}\leq \langle \psi |\psi \rangle \langle \phi |\phi \rangle .$

Dual Spaces and Adjoint Operators

Let ${\mathit {V}}$ be a Linear Vector Space. From ${\mathit {V}}\!$, we can construct another Linear Vector Space ${\mathit {V^{'}}}$ by the following rule: For each element in ${\mathit {V}}$ of the form $|z\rangle \equiv [\alpha |x\rangle +\beta |y\rangle ]\in {\mathit {V}}$, we associate it with $\langle z|\in [\alpha ^{*}\langle x|+\beta ^{*}\langle y|\in {\mathit {V}}$. ${\mathit {V^{*}}}\!$ is called the dual of ${\mathit {V}}\!$ (the bra space). together, they form a bracket. Let ${\mathit {A}}$ be an operator.It is completely known if $\langle y|A|x\rangle$ is known for all $|x\rangle$ and $|y\rangle$ $\in V$. We define a new operator $A^{\dagger }$ (the adjoint) such that $\langle x|A^{\dagger }|y\rangle =\langle y|A|x\rangle$ for all $|x\rangle$ and $|y\rangle$ $\in V$.

Special Linear Operators in Quantum Mechanics

Hermitian Operator: An operator $H\!$is called hermitian if $H=H^{\dagger }$. all physical observables in quantum mechanics are represented by hermitian operators.

Unitary Operator: An operator $U\!$is called unitary if there exits an unique $U^{-1}\!$ and is equal to $U^{\dagger }$, i.e., $UU^{\dagger }=U^{\dagger }U=1$. An important property of unitary operators is that it preserves the norm of a vector,which in quantum mechanics refers to the conservation of probability under physical operations.

Antihermitian operator: An operator $A\!$ is called antihermitian if $A^{\dagger }=-A$. Every operator $C\!$ can be decomposed uniquely in terms of a hermitian and an antihermitian part: $B={\frac {B+B^{\dagger }}{2}}+{\frac {B-B^{\dagger }}{2}}\equiv H+A$.

Antilinear operator: An operator $A\!$ is called antilinear if for all $|x\rangle$ and $|y\rangle$ $\in V$ and for every complex numbers $\alpha$ and $\beta$, $A[\alpha |x\rangle +\beta |y\rangle ]=[\alpha ^{*}|x\rangle +\beta ^{*}|y\rangle ]$. In quantum mechanics, we need only linear operators but for one important exception: The operator $T\!$ that represents time reversal of states is an "antilinear operator".

Theorem on Hermitian Operator

Eigenvalues of a hermitian operators are real and eigenvectors of a hermitian operator and corresponding to different eigenvalues are orthogonal.

Proof: Consider the eigenvalue equation:

$H|x\rangle =\lambda |x\rangle$ where $|x\rangle$ is an eigenvector corresponding to an eigenvalue $\lambda \!$ of $H\!$. Taking the dual of the equation, and using the fact that $H^{\dagger }=H$, we get

$\langle x|H=\lambda \langle x|$

Taking the scalar product of the first equation with $\langle x|$ and of the second with $|x\rangle$, we get

$\langle x|H|x\rangle =\lambda \langle x|x\rangle =\lambda ^{*}\langle x|x\rangle$

As $|x\rangle$ is not a null vector, $\lambda ^{*}=\lambda \!$,i.e, $\lambda$ is real. To prove the second part of the theorem, consider another eigenstate $|y\rangle$ with a distinct (real)eigenvalue $\lambda ^{'}\neq \lambda$. Taking scalar product of the first equation with $\langle y|$ and of the second equation withn $\langle x|$, we get

$\langle |H|x\rangle =\lambda \langle y|x\rangle =\lambda ^{'}\langle y|x\rangle$.

As $\lambda \neq \lambda ^{'}$, $\langle y|x\rangle =0$, i.e., $|x\rangle$ and $|y\rangle$ are mutually orthogonal.

Hermitian adjoint

Suppose that there exists an operator ${\hat {A}}^{\dagger }$, for which $\langle {\hat {A}}^{\dagger }\psi _{1}|\psi _{2}\rangle =\langle \psi _{1}|{\hat {A}}|\psi _{2}\rangle$. If this holds for all wavefunction, then we construct a Hermitian adjoint.

An operator is called Hermitian if: ${\hat {O}}^{\dagger }={\hat {O}}$.

Relations of Hermitian adjoint

$({\hat {F}}^{\dagger })^{\dagger }={\hat {F}}$
$(c{\hat {F}})^{\dagger }=c^{*}{\hat {F}}^{\dagger }$
$({\hat {F}}+{\hat {G}})^{\dagger }={\hat {F}}^{\dagger }+{\hat {G}}^{\dagger }$
$({\hat {F}}{\hat {G}})^{\dagger }={\hat {G}}^{\dagger }{\hat {F}}^{\dagger }$
$c^{\dagger }=c^{*}$
$|a\rangle ^{\dagger }=\langle a|$
$\langle a|b\rangle ^{\dagger }=\langle b|a\rangle$
$(|a\rangle \langle b|)^{\dagger }=|b\rangle \langle a|$

The Law of Calculation for Operators

(1) If ${\hat {F}}|\psi \rangle ={\hat {G}}|\psi \rangle$ for every $|\psi \rangle$, then ${\hat {F}}$ is equal to ${\hat {G}}$.

(2) Commutative Law: ${\hat {F}}+{\hat {G}}={\hat {G}}+{\hat {F}}\!$

(3) Associative Law: $({\hat {F}}+{\hat {G}})+{\hat {H}}={\hat {F}}+({\hat {G}}+{\hat {H}})\!$

(4) Multiply: ${\hat {F}}{\hat {G}}|\psi \rangle ={\hat {F}}({\hat {G}}|\psi \rangle )$

(5) Identity operator: ${\hat {I}}|\psi \rangle =|\psi \rangle$

(6) Zero operator: ${\hat {0}}|\psi \rangle =|0\rangle$

Projection Operator

An operator${\hat {P}}$ is said to be a Projection operator , if it is Hermitian and equal to its own square. Thus,${\hat {P}}$= ${\hat {P}}^{\dagger }$ and ${\hat {P}}$ = ${\hat {P}}^{2}$ Properties of Projection operator:

1. The Product of two commuting projection operators ${\hat {P}}_{1}$ and ${\hat {P}}_{2}$ is also a projection operator.

    $({\hat {P}}_{1}{\hat {P}}_{2})^{\dagger }={\hat {P}}_{2}^{\dagger }{\hat {P}}_{1}^{\dagger }={\hat {P}}_{2}{\hat {P}}_{1}={\hat {P}}_{1}{\hat {P}}_{2}$

and $({\hat {P}}_{1}{\hat {P}}_{2})^{2}={\hat {P}}_{1}{\hat {P}}_{2}{\hat {P}}_{1}{\hat {P}}_{2}={\hat {P}}_{1}^{2}{\hat {P}}_{2}^{2}={\hat {P}}_{1}{\hat {P}}_{2}$

2. The sum of two or more Projection operators is not a Projection operator in general.The sum is a Projection operator iff the operators are mutually orthogonal.

3. Two Projection operators are said to be orthogonal if the product of the two operators is zero.

The Projection operator corresponding to the ket $|x\rangle$ can be written as ${\hat {P}}=|x\rangle \langle x|$. The completion relation is given by $\Sigma |x\rangle \langle x|=I$ or, $\Sigma P_{x}\!=I$

For any vector V,

 $P_{x}|V\rangle =|x\rangle \langle x|V\rangle =|x\rangle v_{x}$

The Projection operator selects the component of $|V\rangle$ in the direction of $|x\rangle$