search for the h 0 dibaryon at ktev
DESCRIPTION
Search for the H 0 Dibaryon at KTeV. Overview KTeV Detector Analysis Signal Mode Normalization Mode Transmission Effects Lifetime and Branching Ratio Results and Future Plans KTeV Collaboration : - PowerPoint PPT PresentationTRANSCRIPT
Search for the H0 Dibaryon at KTeV
• Overview• KTeV Detector• Analysis
– Signal Mode
– Normalization Mode
– Transmission Effects
– Lifetime and Branching Ratio
• Results and Future Plans
KTeV Collaboration:Arizona, UCLA, UCSD, Chicago, Colorado, Elmhurst, Fermilab, Osaka, Rice, Rutgers, Virginia, Wisconsin
Ram Ben-DavidFermilab
Rencontres de Moriond /QCDMarch 21-27, 1999
Moriond QCD99 Ram Ben-David
What is the H0 Dibaryon?
• It’s a 6q color singlet hadron:
H0 = (B = 2, S = -2)
• Schematic deuteron wave function:
• Additional flavor possibly lowers the system’s energy through the color-hyperfine interaction:
pnqd 6
2x3q color singlets(long distance, bound by 2.2 MeV)
6q color singlet(short distance repulsion)
NqH 6
Is it stable against strong decays?
uuddss
Moriond QCD99 Ram Ben-David
Theoretical Predictions for MH
MH
Moriond QCD99 Ram Ben-David
So What?
• It would be a new form of matter, analogous to mesons and baryons.
• Increase knowledge of strong interactions.
• First of many (?) of multiquark states.
• Astrophysical implications.
M a s s R a n g e L i f e t i m e
2H MM U n s t a b l e
2Hn MMM M e t a s t a b l e : 1S sec1010 -7-10
nHnn MMM M e t a s t a b l e : 2S
days 10
nnH MM C o m p l e t e l y S t a b l e
Moriond QCD99 Ram Ben-David
KTeV Search Region
Recent Experimental Searches
From D. Ashery, Proceedings of Hadron Spectroscopy: 7th Int. Conf. (1997)
Moriond QCD99 Ram Ben-David
The H0 at KTeV
• Fully reconstruct the final state.
• First analysis to normalize to ’s (S = -2)
– Test coalescense portion of the production model.
• Sensitive to the remaining mass window in
Donoghue et al. model. (PRD34, 3434, 1986)
• Test production at high energies: Rotondo’s model (PRD47, 3871, 1993)
Signal
Mode
Normal
Mode
Moriond QCD99 Ram Ben-David
Highlights:– 800 GeV/c p on BeO target
– clean and intense beams
– long decay volume
– hermetic detector
– high resolution CsI EM calorimeter
– new DAQ system w/online event filtering
KTeV Spectrometer (Rare Decay Configuration)
GeV 15 E @ % 1 E/E
Moriond QCD99 Ram Ben-David
Final H0 Cuts
Pt of H0 vs. MH
MH = 2.21 GeV/c2
= 5.28 nsec
Moriond QCD99 Ram Ben-David
Mass and Momentum Distributions
N
0 0D
Moriond QCD99 Ram Ben-David
Result
Moriond QCD99 Ram Ben-David
Test of Donoghue et al. Model
Moriond QCD99 Ram Ben-David
Sensitivity to Lifetime
Assume BR(H0N) = 100 %
then BR(H0ppp
Moriond QCD99 Ram Ben-David
Future Plans
• To probe for shorter lifetimes, we need to close the distance between the target and the spectrometer
look for H0’s produced in the regenerator.
• Based on production rate in the regenerator, estimate sensitivity of 100 H0’s per day.
Moriond QCD99 Ram Ben-David
Conclusions
• Ruled out the remaining mass window for long lived H0’s as proposed by Donoghue et al. – Sensitive to the range: nsec <H < 107 nsec
• First test of Rotondo’s production model (at high energies).– Normalizing to ’s is a sensitive probe
of coalescence.
• In KTeV99, we have the ability to search down to 0.5 nsec).
… in addition to the H0, there are some interesting Kaon results.