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pdn, ωn, K+-, K0 reactions at PANDA facility
Yu. Rogov, First seminar of FRRC Fellows
FAIR – Russia Research Center,
Moscow June, 9 - 10, 2009
OZI rule*
NN→φπ is forbidden, NN→ωπ is allowed• φ production is possible only via mixing,
because φ and ω are mixture of ω0 and ω8: = cos 8 - sin 0
= sin 8 + cos 0
*Okubo S. // Phys. Rev. 1977. V.16. P.2336
0)()(
)(2
ddCBAMuuCBAM
ssCBAMZ
)(3
10 ssdduu
)2(6
18 ssdduu
OZI rule
• Introducing ideal mixing angle Θi, cosΘi=(2/3)1/2, sinΘi=(1/3)1/2, Θi=35.5°
• Θ(mφ,mω,mω8), mω8=m(K*,ρ), Θ=39°
• If Z=0, then
• R(φ/ω)=tan2(Θ-Θi)f = 4.2·10-3
)cos()sin()(2
1 ii ssdduu
)tan()(
)(iCBAM
CBAM
OZI rule
• Okubo: production of ss states in the non-strange hadrons interactions is forbidden
• - production in pp (pp) interaction is possible either due to admixture of light quarks in the wave function or due to strange quarks admixture in the nucleon.
0)()(
)(2
ddCBAMuuCBAM
ssCBAMZ
32 102.4)(tan)(
)(
iCBA
CBA
)cos()sin()(2
1 ii ssdduu
= -i =3.70
OZI rule predicitions
32 104)(tan)(
)(
iCBA
CBA
• Universal, does not depend on energy or other properties of the initial state.
• Depends on the masses of the meson in the nonet
3
2
2 1016))1270((
))1525((
fCBA
fCBA
25.1)(
)(
CBA
CBA
Comparison with experiment
R(/)=tg2(-I)=4.2 10-3
Weighted average of all experimental data
N
R(/)=(3.300.34)10-3
• NN
R(/)=(12.780.34)10-
3
NN
R(/)=(14.551.92)10-
3
The OZI rule is always correct, its violation is only apparent
Violation indicates on non-trivial physics:
• Strange degrees of freedom in the nucleon
• Role of gluon degrees of freedom
About hydrogen target
• Proton annihilation at rest• Slow antiproton capture on an orbit of
ppbar atom with large principal quantum number n~30.
• Low pressure gas (~mbar): cascade to lower level, annihilation from P levels with n=2
• Liquid H: Stark mixing between various angular momentum states, annihilation from large n and L=0, i.e. S states.
• Crystal Barrel, 1995, LQ hydrogen targetp + p → + p + p → +
• R() = (29497) 10-3
• R()OZI = 4.2 10-3
• L=0, S=0 1S0 spin singlet
• OBELIX, 1995, LQ, NTP, 5 mbp + p → + p + p → +
• R() = (11410) 10-3
• R()OZI = 4.2 10-3
• L=0, S=1 3S1
• spin triplet
• Different situation for annihilation from S- and P-waves
• R() = (12012) 10-
3 3S1
• R() < 7.2 10-3 1 P1
• spin triplet – enhanced• spin singlet – suppressed
f2’(1525)/f2(1270)
• Tensor mesons:
L=1, S=1, J=2
f2(1270) normal qq
f2’ (1525) ss
• R(f2’f2) = (4714) 10-3 3S1
• R(f2’f2) = (14920) 10-3 1
P1
• spin triplet – suppressed• spin singlet – enhanced
• OBELIX, 1995, NTP,
5 mb p + p → + + + -
p + p → + + + -
For all events:• R() = (5-6) 10-3
• R()OZI = 4.2 10-3
For events with M=300-500 MeV
• R() = (16-30) 10-
3
nn
• OBELIX, Crystal Barrelp + d → + np + d → + nB.Pontecorvo, 1956One-meson annihilation• R() = (15629)
10-3
• R()OZI = 4.2 10-3
/
p
p
s
s
s
s
pp
• If it were a normal quark reaction
()exp ~ 4 b• why is it so large?() was not
measured
nbtg i 10)()()( 4
At LEAR experiemts
Strong violation of the OZI rule was found in
pp pp, pp (3S1)
pdn
Does it depend on – spin– orbital angular
momentum– momentum transfer– isospin?
Pontecorvo reactions
• Largest momentum transfer:q2=-0.782 GeV2/c2 inpdn, compared toq2=-0.360 GeV2/c2 inpp0
• Interesting physics*:two-step modelpp0, nnR() = (15629) 10-3
Rth() = (9227) 10-3
R() decreases with energy
*Kondratyuk L.A., Sapozhnikov M.G., Phys.Lett., 1989, B220, 333.
*Kondratyuk L.A. et al., Yad.Fiz., 1998, 61, 1670.
Pontecorvo reactions
• Reactions p + d+K0, 0+K0
R=Y(K)/Y(K) = 0.920.15two-step model R=0.012 because σ(KNX) > σ(KN X)
• Is two-step model correct?
Pontecorvo reactions at PANDA
• Energy region never measured before
• High statistics expected
• Noone really knows why OZI rule is violated in such selective manner
• Assuming that OZI rule is precisely correct, we have a hint to non-trivial physics