c entral e xclusive m eson pair production in perturbative regime

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Central Exclusive Meson Pair Production in Perturbative Regime. (based on works by V.Khoze, M. RYskin and W.J. STirling and L. HArland-Lang) (KRYSTHAL collaboration) V.A. Khoze (IPPP, Durham & PNPI) For more details see: ArXiV: 1105.1626

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C entral E xclusive M eson Pair Production in Perturbative Regime. (KRYSTHAL collaboration). V.A. Khoze ( IPPP, Durham & PNPI ). (based on works by V. K h oze, M. RY sk in and W.J. ST irling and L. HA rland -L ang ). For more details see: ArXiV:. 1105.1626. CEP-spin-parity filter - PowerPoint PPT Presentation

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Page 1: C entral  E xclusive  M eson Pair Production in Perturbative Regime

Central Exclusive Meson Pair Production in Perturbative Regime.

(based on works by V.Khoze, M. RYskin and W.J. STirling and L.

HArland-Lang)

(KRYSTHAL collaboration)

V.A. Khoze (IPPP, Durham & PNPI)

For more details see: ArXiV:1105.1626

Page 2: C entral  E xclusive  M eson Pair Production in Perturbative Regime

CEP is reported by LHCb (DIS-11)

new CDF CEP results (Erik, low x-11)All measurements in agreement with Durham group (pre)dictions.

CEP-spin-parity filter (KMR-00,KKMR-03)

Page 3: C entral  E xclusive  M eson Pair Production in Perturbative Regime

Prio

r to

thi

s W

orks

hop

Now 43 events

(now proved to be small)

(KMRS-04)(LKRS-10)

Page 4: C entral  E xclusive  M eson Pair Production in Perturbative Regime
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(M.Benayoun,V.Chernyak,-1990)

40 diagrams (4 basic)

(Mariola’s talk)

Page 8: C entral  E xclusive  M eson Pair Production in Perturbative Regime

(explicit calculation)

is this easy to understand ?

Page 9: C entral  E xclusive  M eson Pair Production in Perturbative Regime

is this easy to understand ?

currently popular (among the more formal community) MHV- technique

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g

g

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(KRYSTHAL coll.- 09-11)

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New CDF data nicely confirm this ! (Erik’s talk)

(K-factor,..)

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New CDF data confirm both Durham predictions for CEPand strong suppression of the

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PT expectations if no proton tagging

Violation of

-momentum transfer through the ‘digluon Pomeron’

In the low mass region: is small.

Non-relativistic effects for spin 2.

Non-PT contribution ( for spin 1, still ~ ).

Spin-2 quarkonium suppression is easier to violate!

for CEP (KMRS-04)

ppY+X+Z

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