ΣΠΑΣΙΜΟ ΣΥΜΜΕΤΡΙΑΣ Garamond.pdf

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    TO SU(2)XU(1) .

    SU(2)WXU(1)Y

    MSc.

    2011

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    TO SU(2)XU(1) .

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    TO SU(2)XU(1) .

    ,

    (electroweak) (Standard

    Model).

    Lagrangian:

    2 2 ( )( ) ( )

    4

    L

    (1)

    , SU(2) (SU(2) douplet) :

    1 2

    0

    3 4

    1 ( )

    2

    1 ( )

    2

    i

    i

    (2)

    , 0

    . ( (1)

    SU(2) , U(1) : SU(2)

    U(1) ).

    + 2 Lagrangian

    2 . (

    2 , + 2 - 2 , ( 2 0 ), free ( 0 )

    Lagrangian (1) 4 ,

    m).

    (1) , ( 2 0 ),

    :

    2 2

    min

    2 ( )

    2

    (3)

    http://en.wikipedia.org/wiki/Lagrangianhttp://en.wikipedia.org/wiki/Lagrangianhttp://en.wikipedia.org/wiki/Lagrangianhttp://en.wikipedia.org/wiki/Lagrangian
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    TO SU(2)XU(1) .

    U(1) , (3) vacuum

    expectation value (vev) :

    2

    0 02

    (4),

    0 (ground state).

    H Lagrangian (1):

    i) glbal :

    . exp( )

    2

    ai

    (5)

    ii) U(1) glbal :

    exp( )ia (6)

    SU(2) U(1) .

    (local version), 3 SU(2) gauge ,

    ( ),iW x 1,2,3i U(1) ( )B x .

    :

    0

    ,

    (covariant) :

    .2

    WD ig

    ,

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    TO SU(2)XU(1) .

    U(1) :

    2

    B

    ig

    :

    2 2 1 1 ( ) ( ) ( )4 4 4

    GL D D F F G G

    (7),

    :

    ( . )2 2

    W BD ig ig

    (8)

    F W W gW W (9)

    G B B (10)

    .

    (

    0, ,W W Z ) ( ).

    ()

    vev .

    Weinberg(1967) :

    0

    0 0

    2

    (11),

    :2

    2

    (11) :

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    TO SU(2)XU(1) .

    1( )

    23

    1( ) 0 0 0

    2t (12),

    U(1)

    SU(2) isospin.

    Steven Weinberg

    :

    1( )

    2

    3

    1 0 0 ( 0 0 ) exp[ ( ) 0 0 0 0

    2ia t (13),

    1

    (32

    3)2

    t

    , (weak) isospin.

    (12) ,

    :

    http://en.wikipedia.org/wiki/Steven_Weinberghttp://en.wikipedia.org/wiki/Steven_Weinberghttp://en.wikipedia.org/wiki/Steven_Weinberg
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    TO SU(2)XU(1) .

    0

    exp( ( ). ) 1( ( ))2

    2

    i xH x

    (14)

    ,

    (14) (

    ):

    0

    1( ( ))

    2H x

    (15)

    (15) Lagrangian

    ( ), :

    2 21 2

    Free

    GL H H H

    2 2

    1 1 1 1 1 1

    1 1 ( )( )

    4 8W W W W g W W

    2 2

    2 2 2 2 2 2

    1 1 ( )( )

    4 8W W W W g W W

    3 3 3 3

    1 1 ( )( )

    4 4W W W W G G

    2

    3 3

    1 ( )( ).

    8gW g B gW g B

    (16),

    ( ),

    : H H , 2 2H .

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    TO SU(2)XU(1) .

    ,

    .

    :

    0

    1( ( ))

    2H x

    , :

    1 2

    3

    1 ( ) ( ( )) 2 2

    ( . )12 2

    ( ( )) ( ( ))2 22

    ig W iW H xW B

    ig ig ig ig

    W H x B H x

    , :

    1 1 1 2 1 3 .W W W W

    1 2 3

    0 1 0 1 0

    1 0 0 0 1

    iW W W

    i

    3 1 2

    1 2 3

    W W iW

    W iW W

    , :

    ( . ) .2 2 2 2

    W B ig ig ig ig W B

    =

    3 1 2

    1 2 3

    0

    1 ( ( ))2

    2

    W W iW ig

    H xW iW W

    0

    1( ( ))2

    2

    igB

    H x

    1 2

    3

    1 ( ) ( ( )

    2 2

    1 1 ( ( ) ( ( ))

    2 22 2

    igW iW H x

    ig ig W H x B H x

    (17)

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    TO SU(2)XU(1) .

    (17) ,

    , :

    2 2 2 2 2

    1 2 3 3

    1 1 ( ) ( )( )

    8 8g W W gW g B gW g B

    ,

    (16).

    (16) :

    2Hm ( Higgs)

    1W

    2W

    (1 2 3

    , ,W W W) , :

    1 2

    2

    W

    gM M M

    , 3W B .

    :

    2

    3 3

    1 ( )( )

    8gW g B gW g B

    ,

    3

    gW g B .

    :

    3 cos sinW WZ W B

    (18),

    :

    1

    2 2 2

    cos

    ( )

    W

    g

    g g

    1

    2 2 2

    sin

    ( )

    W

    g

    g g

    (19),

    http://en.wikipedia.org/wiki/Higgs_bosonhttp://en.wikipedia.org/wiki/Higgs_bosonhttp://en.wikipedia.org/wiki/Higgs_bosonhttp://en.wikipedia.org/wiki/Higgs_bosonhttp://en.wikipedia.org/wiki/Higgs_boson
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    TO SU(2)XU(1) .

    :

    3 sin cos

    W WA W B (20)

    (16), :

    3 3 3 3

    1 ( )( )

    4W W W W

    2

    3 3

    1 1 ( )( )

    4 8G G gW g B gW g B

    =

    =1

    ( )( )4

    Z Z Z Z

    2 2 21 1 ( )8 4

    g g Z Z F F

    (21),

    : F A A (22)

    W , :

    tanW

    g

    g

    ,

    g g Weinberg (

    Glashow)

    , :

    3

    3

    cos sin

    sin cos

    W W

    W W

    Z W B

    A W B

    (23)

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    TO SU(2)XU(1) .

    , 3

    W

    B , ( )WR ,

    :

    3

    ( )

    W

    BAR

    WZ

    ,

    3

    cos sin sin cos

    W W

    W W

    BAWZ

    (24)

    (

    ).

    (24), :

    3

    ( ) W

    B A

    RW Z

    3

    cos sin

    sin cos

    W W

    W W

    B A

    W Z

    (25)

    3

    cos sin

    sin cos

    W W

    W W

    B A Z

    W A Z

    (26)

    (26) (21),

    (21).

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    TO SU(2)XU(1) .

    :

    2 2 21 1 1 ( )( ) ( ) ( )( )4 8 4

    Z Z Z Z g g Z Z A A A A

    :

    i) A A

    , 0A

    M . A

    , .

    ii) Z :

    1

    2 2 21

    ( )2 cos

    WZ

    W

    MM g g

    (27),

    ( 0Z ( 0, ,W W Z ).

    . (7) 12

    :

    3 Ws , 8 (=42) , 4

    4 ( vector 2

    , ).

    :

    3 :1 2

    ,W W Z , : 33=9 ,

    A 2

    H (1 ).

    :

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    TO SU(2)XU(1) .

    0

    1( ( ))

    2H x

    ,

    Ws 0Z , :2

    2 2

    .[ ]i gM

    M i

    A ,

    D(

    A

    Z

    ),

    :

    23 3 31 1

    { sin ( ) [ sin ( )] }2 cos 2 2

    W W

    W

    igD ig A Z

    (28)

    , 31

    0 0 (

    (12))

    A

    ,

    0 0 0 .

    3

    1

    ( ).

    D

    :

    sinW

    e g (29)

    (16)

    . (

    ).

    :

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    TO SU(2)XU(1) .

    2 1

    3

    0

    12

    2

    ii

    ,

    t Hooft:

    2 2 2

    3

    1,2

    1 { ( ) ( ) ( ) }

    2i W i Z

    i

    W M Z M A

    (30)

    :

    2 2 1

    2 2

    (1 )[ ]( )i g M

    M

    (31)

    ( ).

    ( , (31)

    , - 21

    ,

    QED Lorentz).

    WeinbergW :

    cos WW

    Z

    M

    M (32),

    Q, .

    -

    Q=91,2GeV/c, Z

    M -boson. :

    2sin 0, 23W , : 28,7W

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    TO SU(2)XU(1) .

    Higgs (Higgs, Englert,

    Brout) 3 .

    Higgs ( Standard Model) .

    Higgs .

    , .

    Higgs ().

    Higgs . (

    ).

    Higgs LHC

    CERN ( 2011-

    ...).

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    TO SU(2)XU(1) .

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    TO SU(2)XU(1) .

    Glashow-Salam-Weinberg

    :Sheldon Lee Glashow, USA,Abdus Salam, Pakistan,

    and Steven Weinberg, USA, Nobel 1979

    ().

    http://en.wikipedia.org/wiki/Sheldon_Lee_Glashowhttp://en.wikipedia.org/wiki/Sheldon_Lee_Glashowhttp://en.wikipedia.org/wiki/Sheldon_Lee_Glashowhttp://en.wikipedia.org/wiki/Abdus_Salamhttp://en.wikipedia.org/wiki/Abdus_Salamhttp://en.wikipedia.org/wiki/Steven_Weinberghttp://en.wikipedia.org/wiki/Steven_Weinberghttp://www.nobelprize.org/nobel_prizes/physics/laureates/1979/http://www.nobelprize.org/nobel_prizes/physics/laureates/1979/http://www.nobelprize.org/nobel_prizes/physics/laureates/1979/http://www.nobelprize.org/nobel_prizes/physics/laureates/1979/http://www.nobelprize.org/nobel_prizes/physics/laureates/1979/http://www.nobelprize.org/nobel_prizes/physics/laureates/1979/http://www.nobelprize.org/nobel_prizes/physics/laureates/1979/http://en.wikipedia.org/wiki/Steven_Weinberghttp://en.wikipedia.org/wiki/Abdus_Salamhttp://en.wikipedia.org/wiki/Sheldon_Lee_Glashow
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    TO SU(2)XU(1) .

    = vector bosons

    Higgs ?

    = quarks

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    TO SU(2)XU(1) .

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    TO SU(2)XU(1) .

    1. Gauge Theories in Particle Physics, I J R Aitchison-A J G Hey, volume (II): QCD and theElectroweak Theory, Taylor & Francis 2004.

    2.A Modern Introduction to Quantum Field Theory, Michele Maggiore, Oxford University Press

    2005

    3.An Introduction to Quantum Field Theory, M E Peskin-D V Schroeder,Reading MA: Addison

    Wesley, 1995.

    4. The Quantum Theory of Fields, volume (II) Modern Applications, Steven Weinberg, CambridgeUniversity Press, 1996.

    5.Quantum Field Theory in a Nutshell,A.Zee, Princeton University Press, 2003

    6. Field Quantization, W. Greiner-J. Reinhardt, Springer 1996.