Yongseok Oh Kyungpook National University" sss ! baryon number = 1, isospin = 0 " Named Ω P. 4...
Transcript of Yongseok Oh Kyungpook National University" sss ! baryon number = 1, isospin = 0 " Named Ω P. 4...
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Yongseok Oh Kyungpook National University
Dense 2011, YITP, Kyoto Apr. 19, 2011
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Contents
1. Introduction 2. Models for hyperon spectrum 3. Bound state approach to the Skyrme model 4. Heavy quark baryons 5. Production process 6. Outlook
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! p! K +K +"#
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INTRODUCTION
I
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Introduction
¤ Baryons with S = -2 ¥ qss (q: light u/d quark) è baryon number = 1, isospin = ½ ¥ Named Ξ
¤ Baryons with S = -3 ¥ sss è baryon number = 1, isospin = 0 ¥ Named Ω
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SU(3) baryons
4/19/2011 P. 5
Baryon octet Baryon decuplet
Baryons: made of three quarks (!!!)
10881333 ⊕⊕⊕=⊗⊗ :flavor 23
21
21
21
21 ,:spin =⊕⊕ ⨁ "
J P =1 2+ J P = 3 2+
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Ξ spectrum
¤ Ξ spectrum ¥ If flavor SU(3) symmetry is good for the classification of hyperon
resonances, then we have ¥ Currently, only a dozen of Ξ baryons have been identified so far.
(cf. more than 20 N* and more than 20 Δ*)
¤ In PDG
4/19/2011 P. 6
N(!*) = N(N*)+ N(!*)
P is not directly measured
Cf. Spin of Ω- (=3/2) was confirmed only recently
by BaBar Collab. PRL 97 (2006)
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Ξ spectrum
¤ Only Ξ(1318) and Ξ(1530) are four-star rated. ¤ Only three states with known spin-parity
¥ The quantum numbers of the other states should be identified.
4/19/2011 P. 7
Advantages
Difficulties
• Small decay widths • Identifiable in missing mass plots • Isospin is 1/2.
(↔ nonstrange sector: #=1/2 and 3/2) • No flavor singlet state (unlike Λ hyperons)
• In most cases, initial state has been used à no hadron beams for Ξ physics
• With initial state, § 3-body final states at least § cross section is very small ~ § other technical difficulties PDG 2010
nb
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Ξ spectrum
¤ No meaningful information for Ξ resonances since 1990s ¥ It can open a new window for studying hadron structure.
¦ Baryon structure from Ξ spectroscopy ¦ Properties of S=-1 hyperons (in production mechanisms) ¦ New particles
¤ Recent experiments
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WA89 (CERN-SPS) EPJC, 11 (1999), hep-ex/0406077
1690 Σ--nucleus collisions
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CLAS @ JLab
4/19/2011 P. 9
PRC 71 (2005) PRC 76 (2007)
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Questions
4/19/2011 P. 10
PDG 2008
The 3rd lowest state
1. Does Ξ(1620) really exist? 2. Ξ(1620) or Ξ(1690)?
Most recent report on Ξ(1620): NPB 189 (1981) 3. What are their spin-parity quantum numbers?
↔ comparison with theoretical predictions
Ξ(1530)
CLAS: PRC 76 (2007)
1690 ?
BaBar: JP of Ξ(1690) is ½- PRD 78 (2008)
1620 ?
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MODELS FOR HYPERON SPECTRUM
II
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Models
4/19/2011 P. 12
• Classify the states as members of octet or decuplet • Use spin-parity (if known) and Gell-Mann—Okubo mass relation
• Works before 1975: reviewed by Samlos, Goldberg, Meadows RMP 46 (1974)
• Recent work along this line Guzey & Polyakov, hep-ph/0512355 (2005)
• No dynamics
Direct extension of the classification in the quark model
• Most parameters of models are fixed by the $=0 and $=−1 sector à in principle, no free parameter for the $=−2, −3
• Most models give (almost) correct masses for %(1318) and %(1530) ü Requirement to survive ü SU(3) group structure
• But they give very different spectrum for the excited % states!
Hadron models for Ξ baryons
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Nonrelativistic quark model
4/19/2011 P. 13
Chao, Isgur, Karl PRD 23 (1981)
from S. Capstick
The 3rd lowest state at 1695 MeV?
• Ξ(1690)*** has JP = 1/2+? • The first negative parity state
appears at ~1800 MeV • Decay widths are not fully calculated
because of the limited final states (but indicates narrow widths)
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Relativistic quark model
4/19/2011 P. 14
Capstick, Isgur PRD 34 (1986)
from S. Capstick
The 3rd lowest state at 1750 MeV?
NRQM
• Negative parity states have lower masses
• The third lowest state has JP = 1/2- at ~1750 MeV
• Where is Ξ(1690)?
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One-boson exchange model
4/19/2011 P. 15
Glozman, Riska Phys. Rep 268 (1996)
from S. Capstick
Negative states have lower mass
• Degeneracy pattern appears
• No clear separation between (+) and (–) parity states
• Where is %(1690)?
The 3rd lowest state at 1760 MeV ?
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Large NC (constituent quark model)
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• Based on quark model • Expand the mass operator by expansion • Mass formula (e.g. 70-plet)
• Fit the coefficients to the known masses and predict.
Large NC quark model
M = cnOnn=0
11
! + dnBnn=1
3
!
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4/19/2011 P. 17
The 3rd lowest state at 1780 MeV?
from J.L. Goity
• Where is %(1690)?
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Model dependence (mass spectrum)
4/19/2011 P. 18
QM (Pervin, Roberts)
1325 1891 2014
PRC 75
1520 1934 2020 1725 1811 1759 1826
1820 (expt.)
1320 (expt.)
1530 (expt.)
: the 3rd lowest state
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Summary
4/19/2011 P. 19
• The predicted masses for the third lowest state are higher than 1690 MeV (except NRQM)
• How to describe %(1690)?
• The presence of %(1620) is puzzling, if it exits.
Highly model-dependent !
Cf. similar problem in QM: Λ(1405)
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BOUND STATE APPROACH TO THE SKYRME MODEL
III
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Skyrme model
4/19/2011 P. 21
bound kaon
SU(3) is badly broken
Treat light flavors and strangeness on the different footing
L = LSU(2) + LK/K*
Soliton provides background potential which traps K/K* (or heavy) meson
Bound state approach (Callan, Klebanov)
Anomaly terms (i) Push up the state
to the continuum } no bound state
(ii) Pull down the state below the threshold } bound state } give hyperons
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Bound state model
4/19/2011 P. 22
• Renders two bound states with negative strangeness Ø p-wave: lowest state Ø s-wave: excited state
• After quantization
Ø p-wave: positive parity hyperons Λ(1116) Ø s-wave: negative parity hyperons Λ(1405)
270 MeV energy difference
• Includes parameters • They should be computed with a given Lagrangian (dynamics). • Or fix them to known masses and then predict.
Mass formula
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Hyperon spectrum (expt.)
4/19/2011 P. 23
289 MeV
290 MeV
285 MeV positive parity
negative parity
parity undetermined
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Mass formula
4/19/2011 P. 24
M (i, j, jm ) =Msol + n1!1 + n2!2 +12I{i(i+1)+ c1c2 jm ( jm +1)+ (c1 ! c1c2 ) j1( j1 +1)+ (c2 ! c1c2 ) j2 ( j2 +1)
!!!!!!!!!!!!!!!!!!!!!+ c1 + c22
j( j +1)! jm ( jm +1)! i(i+1)[ ]+ c1 ! c22!R ! (!J1 !!J2 )}
8 parameters: fit to the available data g give predictions to the other resonances The last term gives a mixing between the states which have same i, j, jm but different R, J1, J2
Fitted valuesMsol = 866 MeV, I =1.01 fm!1 = 211 MeV, c1 = 0.754,!!!!!!!!!c1 = 0.532!2 = 479 MeV, c2 = 0.641,!!!!!!!!!c2 = 0.821
cf. c1 = c12,!!!c2 = c2
2 in Kaplan, Klebanov, NPB 335 (1990)
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Hyperon spectrum (Skyrme model)
4/19/2011 P. 25
YO, PRD 75 (2007) spin-parity
Recently confirmed by COSY PRL 96 (2006)
Unique prediction of this model. The Ξ(1620) should be there.
still one-star resonance
High precision experiments are required!
Ω’s would be discovered in future.
BaBar: the spin-parity of Ξ(1690) is 1/2- PRD 78 (2008)
NRQM predicts 1/2+
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More comments
4/19/2011 P. 26
Two Ξ states
Other approaches
Unitary extension of chiral perturbation theoryRamos, Oset, Bennhold, PRL 89 (2002): 1 / 2!state at 1606 MeVGarcia-Recio, Lutz, Nieves, PLB 582 (2004): claim tht the "(1620) and "(1690) are 1 / 2!states
Kaons: one in p-wave and one in s-wave!!!!!
!J =!Jsol +
!Jm !!!!!!!(
!Jm =
!J1 +!J2 )
!!!!!!!!!!Jsol : soliton spin (=1/ 2),!!!!!
!J1(!J2 ) : spin of the p(s)-wave kaon !(=1/ 2)
!!!!!!!!!Jm = 0 or 1: both of them can lead to J P =1/ 2" !#!states Therefore, two J P =1/ 2" !#!states and one J P = 3 / 2" !#!statesIn this model, it is natural to have two J P =1/ 2" !#!states at 1616 MeV & 1658 MeVClearly, different from quark models
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Sum rules
¤ Mass sum rules ¥ Modified GMO and equal spacing rules
¥ The hyperfine relation
¥ The same relations hold for
¤ Magnetic moments
4/19/2011 P. 27
3! +"# 2(N +$) = "*#%# (&#$*)(&#$*)# ($*#"*) = ($*#"*)# ("*#%)
!*"!+ 32(!"#) = $" N
!(1 / 2" ),!!#(1 / 2" ),!!#(3 / 2" ),!!$(1 / 2+ ),!!!$(3 / 2+ ),!!!%(3 / 2" )
µ(!,1 / 2" ) = 43µ(#1116 )"
13µ(#1405 ),
µ(!,3 / 2" ) = 2µ(#1116 )+µ(#1405 ),!!!etc YO, PRD 75 (2007)
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HEAVY QUARK BARYONS
IV
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Heavy quark baryons
¤ A dog wagging a tail? ¥ Large NC vs. Large M
4/19/2011 P. 29
Large NC: Y.O. & B.Y. Park, PRD 51 (1995)
Large M: Y.O. & B.Y. Park, ZPA 359 (1997) Fewer bound states
300 MeV
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Charm baryon spectrum
Λc Σc Ξc Ωc Ξcc
1/2+ 2287 1/2+ 2454 1/2+ 2470 1/2+ 2695 ?? 3519 1/2- 2595 3/2+ 2518 1/2+ 2577 3/2+ 2766 3/2- 2628 ?? 2800 3/2+ 2646 5/2+ 2882 1/2- 2790 ?? 2939 3/2- 2817
?? 2931 ?? 2971 ?? 3054 ?? 3077 ?? 3123
4/19/2011 P. 30
in MeV Under analysis in the Skyrme model
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PRODUCTION PROCESSES
V
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Ξ photoproduction
4/19/2011 P. 32
!
"N #KK$Dominance of the intermediate S=-1 hyperon states
M1/2±
2, M
5/2±2! EN !M N( ) E"
!M"( )
M3/2±
2, M
7/2±2! EN ±M N( ) E"
±M"( )
Nakayama, YO, Haberzettl, PRC 74
Man, YO, Nakayama, arXiv:1103.1699
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Ξ photoproduction
4/19/2011 P. 33
If we include spin-1/2 and 3/2 hyperon resonances in the intermediate state, then we fail.
Nakayama, YO, Haberzettl, PRC 74
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4/19/2011 P. 34
p2 +m2( )!!1!2!!s= 0
! !"+m( )#!1!2!!n$1= 0
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Propagator
¤ propagators
¤ General expressions
4/19/2011 P. 35
S(p) = ip2 !M 2 " for a boson
S(p) = ip2 !M 2 p #! +M( )" for a fermion
For integer spin n
!!1!!n"1!!n (n, p) = 1
n!"
#$
%
&'
2
"#i!i + a1"#1#2
" !1!2 "#i!i
i=3
n
( +!i=1
n
()
*+
,
-.
P(! ),P(" )/
for even nwith
ar(n) = 0
12
"
#$
%
&'r n!r!(n0 2r)!
1(2n01)(2n03)!(2n0 2r +1)
,
etc
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RNπ Lagrangian
4/19/2011 P. 36
!
JP =12
±
case
L1/ 2 = g"NR N i#$(±)" !1% #
MR ± MN
$µ(±)& µ"
'
( )
*
+ , R + H.c.
JP =32
±
case
L3 / 2 =g"NRM"
N$(! )& µ"Rµ + H.c.
JP =52
±
case
L5 / 2 = i g"NRM"
2 N$(±)& µ&-"Rµ- + H.c.
JP =72
±
case
L7 / 2 =g"NRM"
3 N$(! )& µ&-&."Rµ-. + H.c.
!± =!51
"
#$$
%
&'',!!!!!!!µ
± =!µ!5!µ
"
#
$$
%
&
''
!
"(R#N$) =3g$NR
2
4$2n (n!)2
n(2n)!k$
2n%1
MRM$2(n%1) EN ± MN( )
for (%1)n Ps = ±1 with Ps being the parity of the spin - s resonance R
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Ξ photoproduction
¤ inclusion of spin-7/2 Σ(2030)
4/19/2011 P. 37
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4/19/2011 P. 38
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OUTLOOK
VI
4/19/2011 39
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Outlook
4/19/2011 P. 40
¤ Study on the spectrum of Ξ hyperons ¥ Opens a new window for understanding baryon structure
¤ Theoretical models for Ξ spectrum ¥ Different and even contradictory predictions ¥ What is the third lowest Ξ resonance?
And the quantum numbers? ¥ Soliton model: Ξ(1620) and Ξ(1690): analogue to Λ(1405)
¤ Experimentally, more data are required! ¥ Does Ξ(1620) exist? ¥ Should confirm other poorly established Ξ resonances in PDG as well as th
eir quantum numbers ¥ Almost no information on the Ω baryon resonances
¤ Role of Λ and Σ resonances in Ξ photoproduction. ¥ Offers a chance to study those hyperons. ¥ Higher mass and high spin resonances