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    1

    Projection and Some of Its Applications

    Mohammed Nasser

    Professor, Dept. of Statistics, RU,BangladeshEmail: [email protected]

    1

    The use of matrix theory is now widespread .- - - -- areessential in ----------modern treatment of univeriate andmultivariate statistical methods. ----------C. . ao

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    !

    "#li$ue and "rtho%onal Projection in !

    "rtho%onal Projection into a &ine n

    Inner product SpaceProjection into a Su#space'ram-Schmidt "rtho%onali(ationProjection and )atricesProjection in Infinite-dimensional SpaceProjection in )ultivariate )ethods

    Contents

    !

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    *

    M a t h em

    a t i c al

    C on

    c e p t s

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    +

    Mathematical Concepts

    Covariance

    VarianceProjection

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    ,

    1

    0 and

    1

    1

    1."#li$ue and "rtho%onalProjection in !

    are two independent vectors in!

    1 2

    1 0{ | } and { | }

    1 1V l l R V m m R⇒ ∈ ∈

    are two one-dimensional su#spaces in !

    ! 1 / !1 0 ! 23

    ! 1 !

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    4

    1."#li$ue and "rtho%onalProjection in !

    51617 1

    52617

    !

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    8

    1

    0 and

    1

    1

    1."#li$ue and "rtho%onalProjection in !

    are two independent vectors in!

    =⇔=⇔+=⇒−

    2

    1

    2

    11

    2

    1

    2

    121

    2

    1

    1 1

    0 1

    1 1

    0 1

    1

    0

    1

    1

    a

    a

    x

    x

    a

    a

    x

    xaa

    x

    x

    −=⇒ 121

    2

    1

    x x x

    aa

    −+=⇒1

    0)(

    1

    1121

    2

    1 x x x x

    x

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    9

    1."#li$ue and "rtho%onalProjection in !

    :e define;&; ! as → 11

    t =1

    11

    2

    1 x

    x

    x L

    :e can easily show that it is a linear mapThis linear map is called projection 5o#li$ue

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    =

    1."#li$ue and "rtho%onalProjection in !

    51617 1

    !

    5-1617

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    12

    1."#li$ue and "rtho%onalProjection in !

    1

    1- and

    1

    1 are two ortho%onal5>independent7 vectors in !

    &et us consider −

    += 11

    1

    121

    2

    1

    aa x

    x

    In this case we can find values of ?a@ withoutinverse

    [ ] [ ]

    [ ]

    [ ]2

    2

    1

    1

    1

    2

    1

    111 1

    1 1

    111 11 1

    v

    v x x

    x

    a

    a x x

    T

    ==

    =

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    11

    1."#li$ue and "rtho%onalProjection in !

    :e define;&; ! as → 11

    t = 11

    1

    1

    1

    1

    2

    2

    1

    T

    x

    x

    x L

    This linear map is called ortho%onalprojection.

    The vector is projected on the space %enerated #yalon% the space %enerated #y 1

    1

    −1

    1

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    1!

    Projections

    =

    2

    2

    2

    000

    010

    001

    0

    2

    2

    5262617

    5261627

    5162627

    5!6!6!7

    a 51627

    # 5!6!7

    ==0

    2a

    aaba

    c T T

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    1*

    1."rtho%onal Projection Into a &ine

    Definition 1.1 : Orthogonal Projection

    The orthogonal projection of v into the line spanned by a non ero s is the!ector.

    ( ) ( )"" proj = ×s v v s s

    ×= ×v s

    ss s

    " = =×

    s ss

    s s s

    #$a%ple 1.1 : Orthogonal projection of the !ector ( 2 & ) T into the line y '2 x.

    ( )2 11 1

    2 & 2

    proj = + ÷ ÷

    s

    2 x x = ÷

    s 2 2* x x x= + =s 11"2 = ÷

    s

    1+2 = ÷ 1*

    If S has unit len%th6 then 5v.s7s and its len%th is 5v.s7

    ( ) ( )"" proj = ×s v v s s

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    1+

    #$a%ple 1.2 : Orthogonal projection of a general !ector in , & into the y-a$is

    2

    0

    10

    ÷

    = ÷ ÷ e 2

    0 0

    1 10 0

    x x

    proj y y z z

    ÷ ÷ ÷ ÷

    = × ÷ ÷ ÷ ÷ ÷ ÷ ÷ ÷ e

    0

    10

    y

    ÷

    = ÷ ÷

    0

    0 y

    ÷

    = ÷ ÷

    #$a%ple 1.& : Project ' Discard orthogonal co%ponents railroad car left on an east- est trac/ itho t its bra/e is p shed by a ind

    blo ing to ard the northeast at fifteen %iles per ho r hat speed ill the car reach

    1 proj= ev w 11 02 = ÷

    1112

    = ÷ w

    12

    speed = =v

    1+

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    1,

    #$a%ple 1.* : 3earest Point

    1,

    5a6#7 A

    C

    5c6d7

    &et A 5a6#7 and 5c6d7 #etwo vectors. :e have tofind the nearest vector to Aon

    That means we have to find the value of B for which5B7 55a6#7- B5c6d77T55a6#7- B5c6d77 is minimum 6 i.e. 6 len%th

    of AC is minimum.

    D5c6d7

    Easy application of derivative shows that

    5A. 7F . 3

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    14

    Exercises 1

    1. Consider the function mappin% a plane to itself thattaBes a vector to its

    projection into the line y x .5a7Produce a matrix that descri#es the functionGs action.5#7Show also that this map can #e o#tained #y first

    rotatin% everythin% in the plane HF+ radians clocBwise6then projectin% into the x -axis6 and then rotatin% HF+radians counterclocBwise.

    !. Show that

    14

    0))().(( =− v projvv proj s s

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    18

    2.1Definition

    n inner product on a real spaces V is a f nction that associatesa n %ber4 denoted u4v 4 ith each pair of !ectors u and v of V . This f nction has to satisfy the follo ing conditions for

    !ectors u4v4 and w4 and scalar c.

    1. u4v ' v4u (sy%%etry a$io%)2. u + v 4w ' u4w 5 v4w (additi!e a$io%)&. cu4v ' c u4v (ho%ogeneity a$io%)*. u4u ≥ 04 and u4u ' 0 if and only if u ' 0

    (position definite a$io%)

    2.Inner product pace

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    19

    vector space on which an inner product is defined iscalled an inner product space .Any function on a vectorspace that satisfies the axioms of an inner product defines

    an inner product on the space. .

    There can #e many inner products on a %iven vectorspace

    2.Inner product pace

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    1=

    Example !.16et u ' ( x14 x2)4v ' ( y14 y2)4 and w ' ( z 14 z 2) be arbitrary !ectors in

    R 2

    . Pro!e that u4v 4 defined as follo s4 is an inner prod cton R 2.

    u4v ' x1 y1 5 * x2 y2Deter%ine the inner prod ct of the !ectors ( −24 )4 (&4 1) nder

    this inner prod ct.olution

    $io% 1: u4v ' x1 y1 5 * x2 y2 ' y1 x1 5 * y2 x2 ' v4u

    $io% 2: u + v 4w ' ( x14 x2) 5 ( y14 y2) 4 ( z 14 z 2)

    ' ( x1 5 y14 x2 5 y2)4 ( z 14 z 2)' ( x1 5 y1) z 1 5 *( x2 5 y2) z 2' x1 z 1 5 * x2 z 2 5 y1 z 1 5 * y2 z 2

    ' ( x14 x2)4 ( z 14 z 2) 5 ( y14 y2)4 ( z 14 z 2)'

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    !2

    $io% &: cu4v ' c( x14 x2)4 ( y14 y2)

    ' (cx14cx2)4 ( y14 y2) ' cx1 y1 5 * cx2 y2 ' c( x1 y1 5 * x2 y2)

    ' c u4v $io% *: u4u ' ( x14 x2)4 ( x14 x2) ' 0*

    22

    21 ≥+ x x

    7 rther4 if and only if x1 ' 0 and x2 ' 0. That is u '0. Th s u4u ≥ 04 and u4u ' 0 if and only if u ' 0.The fo r inner prod ct a$io%s are satisfied4

    u4v ' x1 y1 5 * x2 y2 is an inner prod ct on R 2.

    0*22

    21 =+ x x

    The inner prod ct of the !ectors ( −24 )4 (&4 1) is(−24 )4 (&4 1) ' ( −2 × &) 5 *( × 1) ' 1*

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    !1

    Example !.!8onsider the !ector space M 22 of 2 × 2 %atrices. 6et u and v defined as follo s be arbitrary 2 × 2 %atrices.

    Pro!e that the follo ing f nction is an inner prod ct on M 22.

    u4v ' ae 5 bf 5 cg 5 dh Deter%ine the inner prod ct of the %atrices .

    ==h g

    f e

    d c

    bavu 4

    olution$io% 1: u4v ' ae 5 bf 5 cg 5 dh ' ea 5 fb 5 gc 5 hd = v4

    u

    $io% &: 6et k be a scalar. Thenk u4v ' kae 5 kbf 5 kcg 5 kdh ' k (ae 5 bf 5 cg 5 dh) ' k u4

    v *)01()90()2&()2(409

    2

    10

    &2 =×+×+×−+×= −

    −092

    and10&2

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    !!

    Example !.*8onsider the !ector space P n of polyno%ials of degree ≤ n. 6et f

    and g be ele%ents of P n. Pro!e that the follo ing f nctiondefines an inner prod ct of P n.

    Deter%ine the inner prod ct of polyno%ials

    f ( x) ' x2 5 2 x 1 and g ( x) ' * x 5 1

    ∫ =1

    0)()(g4 dx x g x f f

    olution$io% 1: f g dx x f x g dx x g x f g f 4)()()()(4

    1

    0

    1

    0=== ∫ ∫

    h g h f

    dx xh x g dx xh x f

    dx xh x g xh x f

    dx xh x g x f h g f

    44

    )()();()(<

    );()()()(<

    )();()(

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    !+

    orm of a ector

    Definition 2.26et V be an inner prod ct space. The norm of a !ector v isdenoted >>v>> and it defined by

    vv,v =

    The nor% of a !ector in R n

    can be e$pressed in ter%s of the dot prod ct as follo s

    )444()444()()444(

    2121

    22121

    nn

    nn

    x x x x x x x x x x x⋅=

    ++=

    ?enerali e this definition:The nor%s in general !ector space do not necessary ha!e geo%etricinterpretations4 b t are often i%portant in n %erical or/.

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    !,

    Example !.+8onsider the !ector space P n of polyno%ials ith inner prod ct

    The nor% of the f nction f generated by this inner prod ct is

    Deter%ine the nor% of the f nction f ( x) ' x2 5 1.

    ∫ =1

    0 )()(4 dx x g x f g f

    ∫ ==1

    0

    2);(

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    !4

    Example !., 8onsider the !ector space M 22 of 2 × 2 %atrices. 6et u and v

    defined as follo s be arbitrary 2 × 2 %atrices.

    At is /no n that the f nction u4v ' ae 5 bf 5 cg 5 dh is aninner prod ct on M 22 by #$a%ple 2.

    The nor% of the %atri$ is

    ==h g

    f e

    d c

    bavu 4

    22224 d cba +++== uuu

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    !8

    Definition 2.!6et V be an inner prod ct space. The angle θ bet een t onon ero !ectors u and v in V is gi!en by

    vuvu,=θ cos

    The dot prod ct in R n as sed to define angle bet een !ectors.The angle θ bet een !ectors u and v in R n is defined by

    ( )cosvuvu ⋅=θ

    An%le #etween two vectors

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    !9

    An%le #etween two vectors

    In " n #e first prove C$ ine%ualit&

    ' then define cos(

    In " 2 #e first define cos(' then prove C$ine%ualit&

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    !=

    Example !.48onsider the inner prod ct space P n of polyno%ials ith inner

    prod ctThe angle bet een t o non ero f nctions f and g is gi!en by

    Deter%ine the cosine of the angle bet een the f nctions f ( x) ' x2 and g ( x) ' & x

    ∫ =1

    0 )()(4 dx x g x f g f

    g f

    dx x g x f

    g f

    g f

    )()(

    4cos

    1

    0∫ ==θ

    olution =e first co%p te >> f >> and >> g >>.

    &;&

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    *2

    Example !.8 8onsider the !ector space M 22 of 2 × 2 %atrices. 6et u and v

    defined as follo s be arbitrary 2 × 2 %atrices.

    At is /no n that the f nction u4v ' ae 5 bf 5 cg 5 dh is aninner prod ct on M 22 by #$a%ple 2.

    The nor% of the %atri$ is

    The angle bet een u and v is

    ==h g

    f e

    d c

    bavu 4

    22224 d cba +++== uuu

    22222222

    4cos

    h g f ed cba

    dhcg bf ae

    +++++++++==

    vu

    vuθ

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    *1

    "rtho%onal ectorsDef 2.4. 6et V be an inner prod ct space. T o non ero !ectors u and v in V are said to be orthogonal if

    04 =vu

    Example 2.8

    Bho that the f nctions f ( x) ' & x 2 and g ( x) ' x are orthogonal

    in P n ith inner prod ct .)()(41

    0∫ = dx x g x f g f olution

    0;

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    *!

    Jistance

    Definition 2.)6et V be an inner prod ct space ith !ector nor% defined by

    The distance bet een t o !ectors (points) u and v is definedd (u4v) and is defined by

    vv,v =

    )4( )4( vuvuvuvu −−=−=d

    s for nor%4 the concept of distance ill not ha!e direct

    geo%etrical interpretation. At is ho e!er4 sef l in n %erical%athe%atics to be able to disc ss ho far apart !ario sf nctions are .

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    **

    Example !.98onsider the inner prod ct space P n of polyno%ials disc ssed

    earlier. Deter%ine hich of the f nctions g ( x) ' x2

    & x 5 or h( x)' x2 5 * is closed to f ( x) ' x2.olution

    1&)&(&4&4);4(<1

    0

    22 =−=−−=−−= ∫ dx x x x g f g f g f d 1)*(*4*4);4(<

    1

    0

    22 =−=−−=−−= ∫ dxh f h f h f d Th sThe distance bet een f and h is *4 as e %ight s spect4 g is closer

    than h to f.

    .*)4(and1&)4( == h f d g f d

    * ' S h idt " th % li( ti

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    *+

    *.'ram-Schmidt "rtho%onali(ation'iven a vector s 6 any vector v in an inner product space V can #e decomposed as

    ( ) proj proj= + −s sv v v v CC ⊥= +v v CC 0⊥× =v vwhereJefinition *.1 ; )utually "rtho%onal ectors

    ectors v 16 K6 v k ∈ are mutually ortho%onal if v i Lv j 2

    i≠

    j Theorem *.1 ;

    A set of mutually ortho%onal non-(ero vectors islinearly independent.Proof ;

    i ii

    c =∑ v 0 0 j i i j j ji

    c c=× =×∑v v v v

    c j ' 0 ∀ j*+

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    *,

    8orollary .&.1 :

    set of k % t ally orthogonal non ero !ectors in Vk

    is a basis forthe space.

    Definition &.&: Orthonor%al Easis n orthonor%al basis for a !ector space is a basis of % t ally

    orthogonal !ectors of nit length.

    Definition &.2 : Orthogonal Easis n orthogonal basis for a !ector space is a basis of % t ally

    orthogonal !ectors.

    *.'ram-Schmidt "rtho%onali(ation

    Definition &.* : Orthogonal 8o%ple%ent

    The orthogonal co%ple%ent of a s bspace M of * is M ⊥ ' F v ∈ * >

    v is perpendic lar to all !ectors in M G ( read H M perpI ).

    The orthogonal projection proj M (v ) of a !ector is its projection into

    M alon M ⊥ .

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    *4

    6e%%a &.1 :

    6et M be a s bspace of n. Then M ⊥ is also a s bspace and n. ' M ⊕ M ⊥ .

    Jence4 ∀ v∈ n.4 v − proj M (v) is perpendic lar to all !ectors in M .

    Proof : 8onstr ct bases sing ?-B orthogonali ation.

    Theore% &.2 :

    6et v be a !ector inn

    and let M be a s bspace ofn.

    ith basis β1 4 K4 βk .AfA is the %atri$ hose col %ns are the βLs then

    proj M (v ) ' c1β1 5 K5 ck βk

    here the coefficients ci are the entries of the !ector (A T A)-1 AT v. That is4

    proj M (v ) ' A (A T A)−1 AT v.

    Proof : ( ) M proj M ∈v

    T T =A A c A v

    here c is a col %n !ector

    ( )T = −0 A v Ac

    ( ) M proj =v A c

    Ey le%%a&.M4

    ( ) 1T T −=c A A A v*4

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    *8

    Anterpretation of Theore% &.2:

    Af ' β1 4 K4 βk is an orthonor%al basis4 then A T A ' .

    An hich case4 proj M (v ) ' A (A T A)−1 AT v ' A A T v.

    ( ) ( )1

    1

    T

    M k T

    k

    proj

    ÷= × ÷ ÷

    β

    vββv

    β

    L M ( )1

    1

    T

    k T

    k

    × ÷= ÷ ÷×

    βv

    ββ

    βv

    L M ( )1

    1 k

    k

    v

    v

    ÷= ÷ ÷

    ββ L M

    B

    1

    k

    j j j

    v=

    =∑

    βith j jv = ×βv

    An partic lar4 if ' k 4 then A ' A T ' .

    An case is not orthonor%al4 the tas/ is to find ! s.t. " ' A! and B T B ' .

    ( ) ( )T = A! A! T T = ! A A! ( )1 1T T − −=A A ! ! ( )1T −= !!

    Jence

    ( )1T T −=!! A A

    ( ) T M proj =v "" v ( ) T = A! A! v T T = A!! A v ( )

    1T T −= A A A A v

    *8

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    *9

    #$a%ple &.1 :

    To orthogonally project1

    1

    1

    ÷= − ÷ ÷

    v 0

    x

    P y x z

    z

    ÷= + = ÷ ÷

    1 0

    0 1

    1 0

    ÷= ÷ ÷−

    A

    into s bspace

    7ro%1 0

    0 1 4

    1 0

    P x y x y ÷ ÷= + ∈ ÷ ÷ ÷ ÷ −

    R e get

    ( )1

    1 01C 2 0 1 0 1

    0 10 1 0 1 0

    1 0

    T T − − ÷= ÷ ÷ ÷ ÷−

    A A A A

    1 01 0 1

    0 10 1 01 0

    T

    − ÷= ÷ ÷ ÷−

    A A2 0

    0 1

    = ÷ ( )1 1C 2 0

    0 1T −

    = ÷ A A

    1 01C 2 0 1C 2

    0 10 1 0

    1 0

    − ÷= ÷ ÷ ÷−

    1C 2 0 1C 2

    0 1 0

    1C 2 0 1C 2

    − ÷= ÷ ÷−

    ( )1C 2 0 1C 2 1

    0 1 0 1

    1C 2 0 1C 2 1 P proj

    − ÷ ÷= − ÷ ÷ ÷ ÷−

    v

    0

    1

    0

    ÷= − ÷ ÷

    *9

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    *=

    Exercises *.

    1. Perform the 'ram-Schmidt process on this #asis for , & 4

    2 1 0

    2 4 0 4 &

    2 1 1

    ÷ ÷ ÷ ÷ ÷ ÷ ÷ ÷ ÷−

    2. Show that the columns of an n×n matrix form anorthonormal set if and only if the inverse of the matrix is itstranspose. Produce such a matrix.

    *=

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    +2

    + Projection Into a Su#spaceJefinition *.1 ; or any direct sum V M⊕ N and any v ∈ V

    such that v m / n with m ∈ M and n ∈ N .The projection of v into M alon% N is defined as E5v7 proj M 6N 5v 7 m

    eminder ; M M N need not #e ortho%onal.There need not

    even #e an inner product defined.

    +2

    Theorem*.1; Show that 5i7 E is linear and 5ii7 E ! E.

    Theorem*.!; &et E; > is linear and E! E then65i7 E5u7 u for any u N ImE. 5ii7 is the direct sum of the

    ima%e and Bernel of E. i.e.6 ImE DerE. 5iii7 E is theprojection of into ImE6 its ima%e alon% DerE.

    Theorem*.!; &et E; > is linear and E! E then65i7 E5u7 u for any u N ImE. 5ii7 is the direct sum of the

    ima%e and Bernel of E. i.e.6 ImE DerE. 5iii7 E is theprojection of into ImE6 its ima%e alon% DerE.

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    +1

    Projection and )atrices

    O &et &5 7 & & is a linear map #etween and itself3. &5 7is a vector space under function addition and scalarmultiplication.

    O dim5&7 n! if d5 7 n.O If we fix a #asis in 6 there arises a one to one

    correspondence #etween & and set of all matrices oforder n 5the last set is also a vector space withdimension n ! 7. The result implies that matrices identifylinear operators.

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    +!

    "rtho%onal Projection

    "

    Q 516!7

    5!617R

    two vector spaces 16 ! #y multiplyin% the vectors and#y B where B .

    1 B and ! B

    2

    1

    1

    2

    +!

    2

    1

    1

    2

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    +*

    *rthogonal +ro,ection

    ow6 we can find the vector space ! as 1 !&et #e any vector of ! and B 16 B! then we can

    write B

    1 /B

    !

    Therefore6

    2

    1

    x

    x

    2

    1

    x

    x

    2

    1

    1

    2

    +*

    2

    1

    x

    x

    12

    21

    2

    1

    k

    k

    2

    1

    k

    k 1

    12

    21 −

    2

    1

    k

    k

    +−

    21

    21

    &1

    &2

    &2

    &1

    x x

    x x

    2

    1

    x

    x

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    ++

    "rtho%onal Projectionow6 let P #e a projection matrix and x #e a vector in ! 6

    then a projection from ! to 1 is %iven #y6

    Px B 1

    ++

    2

    1-1F* x1 /!F* x ! U 2

    1-

    &

    *

    &

    2&

    2

    &

    1

    2

    1

    x

    x

    Ex. 17 ChecB that P is idempotent #ut not symmetric. :hy<

    !7 Prove that if the second vector is 6 P will #e then

    idempotent as well as symmetric

    −12

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    +,

    )eanin% of P nVn xnV1O Case 1; P nVn is sin%ular #ut not idempotent

    ≠21 1

    , ( ) 1,2 2

    P rank P P P

    1 13

    2 2

    The whole space6 n is mapped to the column space ofPnVn 6 an improper su#space of n .

    An vector of the su#space may mapped to another vector ofthe Su#space.6

    1 12 21 1

    1 2

    2 2

    1 1 1( )

    2 2 2

    P x x x x

    x x

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    +4

    )eanin% of P nVn xnV1

    O Case !; PnVn

    is sin%ular and idempotent5 asymmetric7

    21 0

    , ( ) 11 0

    P rank P and P P

    ¬11

    2

    1

    1Px

    x x

    x 3 1

    32 1

    Px is not ortho%onal to x-Px

    2 2

    2 2P

    The whole space6 n

    is mapped to the columnspace of PnVn 6 an improper su#space of n .

    An vector of the su#space is mapped to the samevector of the Su#space.6

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    +8

    )eanin% of P nVn xnV1

    O Case *; P nVn is sin%ular and idempotent5 symmetric7

    )eanin%; The whole space6 n is mapped to the column space ofP nVn 6 an improper su#space of n . An vector of the su#space ismapped to the same vector of the Su#space. It is ortho%onal

    projection6 That is6 the su#space is to its complement. or example6

    2

    1

    2

    1

    2

    1

    2

    1

    Px 5x1/x ! 7 1/ 2

    1/ 2 Px is ortho%onal to x-Px

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    +9

    )eanin% of P nVn xnV1

    O Case +; P nVn is non-sin%ular and non-ortho%onal )eanin%; The whole space6 n is mapped to the column space of

    P nVn 6 same as n . The mappin% is one-to-one and onto.:e havenow columns of P nVn as a new 5o#li$ue7 #asis in place of standard#asis. An%les #etween vectors and len%th of vectors are notpreserved. or example6

    1 22 1

    1, x y Px y x P y → →

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    +=

    )eanin% of P nVn xnV1O Case ; P nVn is non-sin%ular and ortho%onal

    )eanin%; The whole space6 n is mapped to the column space ofP nVn 6 same as n . The mappin% is one-to-one and onto.:ehave now columns of P nVn as a new 5ortho%onal7 #asis in place

    of standard #asis. An%les #etween vectors and len%th of vectorsare preserved. :e have only a rotation of axes. or example6

    2

    1-

    2

    1

    2

    1

    2

    1 rom a symmetricmatrix we havealways such a Pof its nindependentei%en vectors

    rom a symmetricmatrix we have alwaya symmetricidempotent P of itsr5Wn 7independentei%en vectors

    P j i Th I Xil# S

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    ,2

    Projection Theorem In a Xil#ert Space

    &et #e a closed su#space of a Xil#ert space6 . Thereexists a uni$ue pair of mappin%s P;X → and Y; → suchthat x Px/Yx for all xN . P and Y have the followin%properties;

    i7 x N x x6 Yx 2

    ii7 x N T Px 26 Yx x

    ii7 Px is closest vector in to x.

    iv7 Yx is closest vector in to x

    v7 Px! / Yx ! x!

    vi7 P and Y are linear maps and P ! P6 Y ! Y

    inite dimensional spaces are always closed

    1

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    ,1

    The common characteristic 5structure7 amon% thefollowin% statistical methods<

    1. Principal Components Analysis!. 5 id%e 7 re%ression*. isher discriminant analysis+. Canonical correlation analysis,.Sin%ular value decomposition4. Independent component analysis

    Applications

    We consider linear co binations of inp!t vector" ( ) T f x # x=:e maBe use concepts of len%th and dot productavaila#le in Euclidean space.

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    ,!

    :hat is feature reduction<

    d $ ℜ∈ pd T % ×ℜ∈

    p & ℜ∈

    d T d p

    & %$ & % ℜ∈=→ℜ∈ ×

    :

    &inear transformation

    "ri%inal data reduced data

    Ji i li d i

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    ,*

    Jimensionality eduction

    O "ne approach to deal with hi%h dimensional data is #yreducin% their dimensionality.

    O Project hi%h dimensional data onto a lower dimensionalsu#-space usin% linear or non-linear transformations.

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    ,+

    Principal Component Analysis 5PCA7

    1 1 2 2

    1 2

    " ...here 4 4...4 isa basein the -di%ensionals b-space (NO3)

    ' '

    '

    x b ! b ! b !! ! ! ' = + + +

    " x x=

    1 1 2 2

    1 2

    ...here 4 4...4 isa basein the original 3-di%ensionalspace

    ( (

    n

    x a v a v a vv v v

    = + + +

    O ind a #asis in a low dimensional su#-space;

    Z Approximate vectors #y projectin% them in a low dimensional su#-space;

    517 "ri%inal space representation;

    5!7 &ower-dimensional su#-space representation;

    O Note if D 6 then

    P i i l C t A l i 5PCA7

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    ,,

    Principal Component Analysis 5PCA7O Information loss

    ZJimensionality reduction implies information loss [[ Z PCA preserves as much information as possi#le;

    O :hat is the ?#est@ lower dimensional su#-space< The ?#est@ low-dimensional space is centered at the sample mean and has directions determined #y the ?#est@ ei%envectors of the covariance matrix of the data x.

    Z y ?#est@ ei%envectors we mean those correspondin% to the largest ei%envalues 5 i.e.6 principal components/ 7.

    Z Since the covariance matrix is real and symmetric6 these ei%envectors are ortho%onal and form a set of #asis vectors.

    "%in >> >> (reconstr ction error) x x−

    ZSin%ular alue

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    ,4

    Principal Component Analysis 5PCA7O )ethodolo%y

    Z Suppose x 16 x ! 6 ...6 x M are N x 1 vectors

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    ,8

    Principal Component Analysis 5PCA7O )ethodolo%y Z cont.

    ( )T i ib ! x x= −

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    ,9

    Principal Component Analysis 5PCA7O &inear transformation implied #y PCA

    Z The linear transformation R N

    → R !

    that performs the dimensionality reduction is;

    P i i l C t A l i

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    ,=

    Principal Component Analysis5PCA7

    O Ei%envalue spectrum

    # i$ # %

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    42

    Principal Com(ponent Analysis 5PCA7O :hat is the error due to dimensionality reduction<

    O It can #e shown that error due to dimensionality reduction is e$ual to;

    (

    k ii

    (

    iie

    11

    2

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    41

    Principal Component Analysis 5PCA7O Standardi(ation

    Z The principal components are dependent on the "nits used tomeasure the ori%inal varia#les as well as on the range of values theyassume.

    Z :e should always standardi(e the data prior to usin% PCA. Z A common standardi(ation method is to transform all the data to

    have (ero mean and unit standard deviation;

    Principal Component Analysis 5PCA7

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    4!

    Principal Component Analysis 5PCA7

    O Case Study ; Ei%enfaces for ace JetectionF eco%nition

    Z ). TurB6 A. Pentland6 \Ei%enfaces for eco%nition\6 #o"rnal of $ogniti%eNe"roscience 6 vol. *6 no. 16 pp. 81-946 1==1.

    O 0ace "ecognition

    Z The simplest approach is to thinB of it as a templatematchin% pro#lem

    Z Pro#lems arise when performin% reco%nition in ahi%h-dimensional space.

    Z Si%nificant improvements can #e achieved #y firstmappin% the data into a lo&er di'ensionalityspace.

    Z Xow to find this lower-dimensional space<

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    4*

    Principal Component Analysis 5PCA7O )ain idea #ehind ei%enfaces

    a!erage face

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    4+

    Principal Component Analysis 5PCA7O Computation of the ei%enfaces Z cont.

    i

    )

    i n d t h a t t h i s i s n

    or m

    al i (

    e d ..

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    4,

    Principal Component Analysis 5PCA7O Computation of the ei%enfaces Z cont.

    P i i l C t A l i 5PCA7

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    44

    Principal Component Analysis 5PCA7O epresentin% faces onto this #asis

    Principal Component Analysis 5PCA7

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    48

    Principal Component Analysis 5PCA7

    O epresentin% faces onto this #asis Z cont.

    P i i l C t A l i 5PCA7

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    49

    Principal Component Analysis 5PCA7O ace eco%nition ]sin% Ei%enfaces

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    4=

    Principal Component Analysis 5PCA7O ace eco%nition ]sin% Ei%enfaces Z cont.

    Z The distance e r is called distance &ithin the face space 5difs 7

    Z Comment; we can use the common Euclidean distance to compute e r 6however6 it has #een reported that the Mahalano(is distance performs #etter;

    P i i l C t A l i 5PCA7

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    82

    Principal Component Analysis 5PCA7O ace Jetection ]sin% Ei%enfaces

    l l

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    81

    Principal Component Analysis 5PCA7O ace Jetection ]sin% Ei%enfaces Z cont.

    Principal Component Analysis

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    8!

    Principal Component Analysis5PCA7O econstruction

    of faces and non-faces

    Principal Component Analysis

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    8*

    Principal Component Analysis5PCA7

    O Applications

    Z ace detection6 tracBin%6 and reco%nitiondffs

    Principal Components

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    8+

    Principal Components Analysis

    So6 principal components are %iven #y;

    ( 1 " 11 x 1 / " 1! x ! / ... / " 1 x

    ( ! " !1 x 1 / " !! x ! / ... / " ! x ...( a 1 x 1 / a ! x ! / ... / a x

    x j Gs are standardi(ed if correlation 'atrix is used5mean 2.26 SJ 1.27

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    8,

    Principal Components Analysis

    core of i th unit on j th principalcomponent

    ( i,j " j 1 x i 1 / " j ! x i ! / ... / " jN x iN

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    84

    PCA Scores

    +.2 +., ,.2 ,., 4.2!

    *

    +

    ,

    xi)

    xi*

    bi+* bi+)

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    88

    Principal Components Analysis

    Amount of variance accounted for #y;1st principal component6 ^16 1st eigenvalue

    !nd principal component6 ^!6 !nd eigenvalue

    ...

    ^1 _ ^ ! _ ^* _ ^ + _ ...

    Avera%e ̂j 1 5correlation matrix7

    Principal Components Analysis;

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    89

    Principal Components Analysis;Ei%envalues

    +.2 +., ,.2 ,., 4.2!

    *

    +

    ,

    1 2

    1

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    han3 &ou