PDF format

Backup Slides
Relations with Previous Notation, Partial Waves
D |0,0〉
1
D |1,0〉
1
D |1,±1〉
1
D |2,0〉
1
D |2,±1〉
1
D |2,±2〉
1
„ 1
= D 1,OO =
4 Ds 1,OO + 3 4
1,OO«
Dp ,
= D 1,OL ,
= D 1,OT ∓ |k T | |R|
M
h
2 G ⊥ 1,OT ,
= 1 2 D 1,LL,
= 1 2
D 1,LT ∓ |k !
T | |R|
M
h
2 G ⊥ 1,LT ,
= D 1,TT ∓ 1 |k T | |R|
2 M
h
2 G ⊥ 1,TT ,
H ⊥|0,0〉
1
H ⊥|1,1〉
1
H ⊥|1,0〉
1
H ⊥|1,−1〉
1
H ⊥|2,2〉
1
H ⊥|2,1〉
1
H ⊥|2,0〉
1
H ⊥|2,−1〉
1
H ⊥|2,−2〉
1
= H ⊥ 1,OO = 1 4 H⊥s 1,OO + 3 4 H⊥p 1,OO ,
= H ⊥ 1,OT + |R| ¯H 1,OT
|k T |
=
|R|
|k T | H 1,OT
= H ⊥ 1,OL ,
= H ⊥ 1,OT ,
= H ⊥ 1,TT + |R| ¯H 1,TT
|k T |
=
|R|
|k T | H 1,TT
= 1 2 H⊥ 1,LT + 1 |R|
¯H 1,LT
2 |k T | = 1 |R|
2 |k T | H 1,LT
= 1 2 H⊥ 1,LL ,
= 1 2 H⊥ 1,LT ,
= H ⊥ 1,TT .
Gliske (HERMES / Michigan) SIDIS Vector Mesons at Hermes 11 April, 2011 63 / 66