i.savin @ prague in 2011 i 1 - fyzikální ústav · pdf filek0-long decay...
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I.SAVIN @ PRAGUE IN 20111I
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I.Savin@Prague in 2011 2
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MY LIFE TIME COLLABORATION WITH CZECH PHYSICISTSIN HIGH ENERGY PHYSICS EXPERIMENTS
I.Savin, JINR, Dubna, ,
OUTLINE 1. Introduction.2. Experiments @ 10 GeV JINR synchrophasotron (1955-1965):
-detector development,-elastic scattering of positive and negative pions.
3. Experiments @ 70 GeV IHEP proton synchrotron (1968-1974):-neutral kaon regeneration,-neutral kaon decays.
4 E i t @ 450 G V CERN t h t4. Experiments @ 450 GeV CERN proton synchrotron:-NA-4 (1974-1991),-COMPASS (from 1995).
5 Conclusions5. Conclusions.
Prague, 26 May, 2011
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10 GeV proton synchrophasotpon, largest in the world at the time, putin operation in 1957in operation in 1957
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1960-s were Gold years of detector development for high energy experiments at LHE:
-nuclear emulsions-cloud, diffusion, bubble chambers (propane, xenon, hydrogen)-electronic detectors (scintillation and Cherenkov (solid & gas) counters, sparkchambers (optical & on-line), MWPC, DC ) and associated electronics
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Special agreement on collaboration betweenSpecial agreement on collaboration betweenIHEP and JINR in high energy experiments
at 76 GeV proton synchrotron14I.Savin@Prague in 2011
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Experiments at U-70 at Serpukhovp p
19671967Significant break-through in High Energy PhysicsPhysicsCommissioning of 70 GeV proton Synchrotron in ProtvinoS b t ti l d t i thSynchrotron in ProtvinoSubstantial advantage in energy over the world
A.LogunovA.LogunovU 70 t 76 G V l t i th ldU 70 t 76 G V l t i th ld Director of IHEP Director of IHEP U-70 parameters: 76 GeV, largest in the world,
put in operations in 1967
U-70 parameters: 76 GeV, largest in the world,
put in operations in 1967 15I.Savin@Prague in 2011
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The collaboration, extended later by the new members, has performed a number, y , pof experiments - BIS, CHARM, EXCHARM
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BIS experiment at U-70 One of the first experiments at U-70 –One of the first experiments at U-70 –
p
Study of K0L – K0
S regeneration in Hydrogen, Deuterium and CarbonStudy of K0
L – K0S regeneration in
Hydrogen, Deuterium and Carbon
The goal of experiments:The goal of experiments:study of energy dependence of the transmission regeneration amplitude in thestudy of energy dependence of the transmission regeneration amplitude in thetransmission regeneration amplitude in the momentum range 10 – 50 GeV/c, that is an equivalent to measurement of the difference of
transmission regeneration amplitude in the momentum range 10 – 50 GeV/c, that is an equivalent to measurement of the difference ofequivalent to measurement of the difference of total cross-sections of K0 and K0 interaction with a matter
equivalent to measurement of the difference of total cross-sections of K0 and K0 interaction with a matterwith a matter.with a matter.
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BIS lay outBIS lay out
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BIS properties
00
BIS properties
• crossing geometry for selections of ,
• 3 m long H2 and D2 targets, C-target with d~1 g/cm3,
00 , SL KK
• He filled decay volume,
• e – and - detectors for registration of and decays,03eK 0
3K• Si- hodoscopes for decay pattern oriented triggers,
• hadron calorimeter for beam monitoring,
t f 18 k h b ith t t i ti d t• set of 18 spark chambers with magnetostrictive read out,
• BESM-3M on line, optimized soft ware,
• world class apparatus at the time of executions• world class apparatus at the time of executions.
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Experiment on K0L – K0
S regenerationp L S g
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BIS data analysis in Prague
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Contributions of Czech physicists to BIS:
-participation in the setting up of the experiment and on-line software,
-data taking and analysis ondata taking and analysis on K0-long-K0-short regeneration from Carbon (full Prague
responsibility),D and H,K0-long decay form factors,searches for new vector mesons and charm particles,
-preparations of new experiments with upgraded BIS –preparations of new experiments with upgraded BIS CHARM,EXCHARM
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-Interference between and 0LK 0
sK
BIS main results
regenerated in H2, D2 and C has been observed at high energies for the first time.The modulus and phase of the regeneration amplitudes have been
L s
-The modulus and phase of the regeneration amplitudes have been measured in the energy range 10 – 50 GeV.
-The modulus and differential cross section of the transmission
regeneration as a function of momentum follow the power low
predicted by the CAM model and Pomeranchuk theorem -
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BIS main results
-The phase of the regenerationamplitude is energy independent, itsvalue is in agreement with predictiong p
from the crossing symmetry andanalytic properties of scatteringamplitudeamplitude.
-The and total crosssection difference has a power low
pK 0 pK 0
section difference has a power low~Ap-n. Rising of the K+n total crosssection was predicted and confirmedat IHEP by direct measurementsat IHEP by direct measurements
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Members of the Berlin, Budapest, Dubna, Moscow, Prague, Sofia ,Tbilisi Collaboration
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Collaboration at CERN 450 GeV SPS...
1976Commissioning of the 400 GeV ….In the first common CERN-JINR experiment NA-4 under special agreement between the CERN and JINR Directors General – N N Bogolubov and W Jentschke duringg
Superconductive Proton Synchrotron at CERN
Directors General N.N.Bogolubov and W. Jentschke during the NNB visit in 1974
SPS
John AdamsJohn AdamsJohn AdamsDirector of the SPS
project – Super Proto
John AdamsDirector of the SPS
project – Super ProtoSPS CERN M i
NA4p j p
Synchrotron,
later CERN Director
p j pSynchrotron,
later CERN Director
SPS Meyrin
CERN 27I.Savin@Prague in 2011
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JINR @ the NA4 experiment:the success story of an early CERN JINRthe success story of an early CERN-JINR
collaboration
R.Voss,Symposium in honour of Igor Savin’s 80th, Dubna, 7 December 2010 29I.Savin@Prague in 2011
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Original proposal SPSC/P19: CERN-Munich-Rome!Original proposal SPSC/P19: CERN Munich Rome!
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Addendum by Dubna,CERN,Munich,Roma
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Co-operation with CERN at SPS1975
A Proposal is approved to build an apparatus and study inclusive deep inelastic muon scattering on nucleons and nuclei to the highest
1975deep inelastic muon scattering on nucleons and nuclei to the highest energies and four-momentum transfers available at the SPS - the NA4 experiment by the BCDMS collaboration:NA4 experiment by the BCDMS collaboration:
B Bologna, INFN, ItalyC CERND Dubna, JINR M Munich University, GermanyS Saclay CEN France
The first JINR – CERN (USSR – CERN) experiment at CERN
S Saclay, CEN, France
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JINR=USSR , Bulgaria, Czechoslovakia, DDR, Hungary
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NA4 – the First JINR-CERN Experimentp
DIS muon trajectory in the toroidal magnetic fieldDIS muon trajectory in the toroidal magnetic field
M/0.3 B ~ 1.5 m33I.Savin@Prague in 2011
A1
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Слайд 33
A1 Admin; 04.03.2011
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NA4 – the First JINR-CERN Experimentp
High Luminosity spectrometer for deep inelasticHigh Luminosity spectrometer for deep inelastic muon scattering
JINR contributions (~30% of total costs): 10 supermodules of iron yoke,
80 halfplanes of MWPC,
7 planes of hexagonal MWPS
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The iron yoke modules production at the JINR workshop( originally at Prague?), weight of each module is about 20 t.( originally at Prague?), weight of each module is about 20 t.
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Arrival of first iron modules at CERN (1977),80 modules in total80 modules in total
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Modules areare assembled to 10 Super-pmodules …
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… the magnet coils are installed …… the magnet coils are installed …
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… and dundergo a
stringentquality control!!!
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MWPC production at Dubnap
MWPC are designed by I.Golutvin et al….
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…….produced…..
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…..tested……
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…inspected by the important visitors…
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….. transported to Geneva by air …
(First commercial(First commercial flight ever of IL-76 to the West,,February,1978)
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...unloaded nder theunder the
eyes of an important delegation g…
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… installed in the SpectrometerSpectrometer ….
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… and with a little help from somehelp from some good old friends …,
NA4 is getting… NA4 is getting ready for physics!47I.Savin@Prague in 2011
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The NA4 technical run, 1978
The veryThe very first muon
track,track, recorded by
the JINR MWPC
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Data taking: 1979 – 1985, analysis up to 1991
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Contributions of Czech physicists to NA-4:
ti i ti i d t t ki d l i f i lt-participation in data taking and analysis of main results:nucleon structure functions F2(x,Q2) and QCD test,observation of the electro-weak interferenceobservation of the electro-weak interference,observation of nuclear effects in SF, including at x>1;
-studies of special aspects of the experiment:map of the solenoid magnetic field,muon energy losses,Fermi motion corrections to DIS,d l t f th d f th QCD l idevelopment of new method of the QCD analysis,on-line monitoring , ectect.
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The NA4 heritage: the structure function F2(x,Q2) of protons.The EMC and SLAC data corrected after the NA4 publication.
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Still a pillar ofStill a pillar of today’s world set of d t l
NA4 data on nucleon structure functions! corner
(RPP 2010)
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Scaling violations: test of perturbative QCD andg pmeasurementof the strong coupling constant
s(MZ2) = 0.113 ± 0.003 (exp)
± 0.004 (th)
Still a competitive measurement today!measurement today!
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Week-electromagnetic interference has been observed for the first time in the muon-quarkobserved for the first time in the muon quark Interactions….(20 years before HERA):
WS/GIM mixing angle and InterferenceStructure function xF3 have been derived fromthe measured B-asymmetries….
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Other highlights:g gNuclear effects…
Qualitatively the EMC effect isconfirmed and corrected: the structure of freenucleons is different from the t t f l b d istructure of nucleons bound in
nuclei
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SF at x>1, kinematically forbidden for a muon-nucleon interaction
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COMPASS: COMPASS: THETHE new fixed target facility at CERN !new fixed target facility at CERN !
COMPASS - History
• 1996 COMPASS proposal• 1997 conditional approval
26. June 19981997 conditional approval
• 1998 MoU
• 1999 – 2001 construction & installation
• 2001 technical run
• 2002 - 2011 data taking• COMPASS II @CERN at least until 2015
8. April 1999
• COMPASS-II @CERN at least until 2015
I.Savin @ International practice 57I.Savin@Prague in 2011
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The COMPASS Collaboration(230 Physicists from 12 Countries)
• Bielefeld, Bochum, Bonn (ISKP & PI), Erlangen, Freiburg, Heidelberg,
• Dubna (LPP and LNP), Moscow (INR, LPI, State University) Protvino
g gMainz, München (LMU & TU)CERN
University), Protvino
Helsinki• Warsaw (SINS),
Warsaw (TU) Prague
SaclayNagoya Saclay
Lisboa
• Burdwan, • Calcutta
Torino(University,INFN),Trieste(University,INFN)
Tel AvivTel Aviv
Czech physicists participate in the Dubna & Prague teams58I.Savin@Prague in 2011
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COMPASS Physics Goals
With muon beam: With hadron beam:
nucleon spin structure hadron spectroscopy
• Gluon Polarization G/GT s s s i st t f ti
• Primakoff-Reactions-polarizability of and K• Transverse spin structure function
h1(x)
Fl d d t l i d k
polarizability of and K
• Glueballs and hybrids• Flavor dependent polarized quark
helicity densities q(x)• Charmed mesons and
baryons
• Spin dependent fragmentation
functions
-semi-leptonic decays-double-charmed baryons
f
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COMPASS
Beam: 160 GeV µ+, pol. 80%f d Hodoscopesfrom π decay
Two‐stage spectrometer60 m long
SME/HCAL1 M W ll 2SM1 2RICH1
E/HCAL1 Muon Wall 2MWPC
E/HCAL2Polarized Target
Muon Wall 1160 GeV
MWPC, Gems, Scifi, W45 (not shown)
Muon Wall 1, Rich Wall
160 GeVµ beam
Straws, GemsI f t t
Micromegas, SDC, ScifiScifi, SiliconInfrastructure
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Parton Distribution Functions
Three twist‐2 PDFs
q(x)f q ( )
unpolarised PDFquark with momentum xP in a nucleon
f1q (x) well known – unpolarized DIS
helicity PDFq(x) g1
q(x)
helicity PDFquark with spin parallel to the nucleon spin in a longitudinally polarised nucleon
known – polarized DIS
q(x)transversity PDF
k i h i ll l h l i iTq(x)h1
q(x)hi l dd l k
quark with spin parallel to the nucleon spin in a transversely polarised nucleon
chiral odd, poorly known
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Factorization & x‐sect. asymmetriesy
• Inclusive scattering• Inclusive scattering
Semi‐inclusive scattering
long. double spin asymmetry
transverse single asymmetry
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HILIGHTS of COMPASS RESULTS on NUCLEON SPIN STRUCTUREHILIGHTS of COMPASS RESULTS on NUCLEON SPIN STRUCTURE
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Proton asymmetriesy• incl. & semi‐incl. asymmetries,
• similar data for deuteron
K+π+incl.
KK−π –
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Q2 evolution of g1(x,Q2)1
• Q2 dependence of g1 data related to gluon polarization (DGLAP)
• Limited kinematic range (c.f. unpol. HERA)
dp dp
CLAS
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The role of quark flavours
• LO semi-inclusive data analysisO se c us e data a a ys s
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Bjorken sum ruleBjorken sum rule
from neutron β decay
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TMD parton distributions
• 8 intrinsic transverse‐momentum dependent PDFs at LO
• Azimuthal asymmetries with different angular modulations in the hadron and spin azimuthal angles, Φh and Φs
aka
Sivers
Boer–Mulders
Transversity
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Proton Collins asymmetry
• Fit to COMPASS d, HERMES, BELLE (Collins FF, e+e-)• in good agreement with new proton data
pp
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Proton Collins asymmetry
• Fit to COMPASS d, HERMES, BELLE (Collins FF, e+e-)• in good agreement with new proton data
pp
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ConclusionsConclusions• BIS and NA4 have been the landmark experiments
th t d i i l d l ti t ib ti t ththat made original and lasting contributions to the particle physicsC h ti i t f th i t J C h• Czech participants of these experiments – J.Cvach, J.Hladky, R.Lednicky, S.Nemechek, M.Nowak, A.Prokesh, PReimer J Strachota J Votruba J Zhachek PZavada canP.Reimer, J.Strachota, J.Votruba, J.Zhachek, P.Zavada ‐ can be proud of their contributions
• Experience gained was very important for further• Experience gained was very important for further participation of Czech physicists in experiments at JINR, DESY, CERN, BNL, , ,
• Prague team in COMPASS and annual Prague workshops on spin physics promote the field in the p p p y pworld
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Thank you my dear friends and colleagues
Special thanks to Czechoslovakian AcademySpecial thanks to Czechoslovakian Academyof Science for awarding me with Gold medal
and to Czech Physics Society for the present valuable awardvaluable award
THANKS TO ALL OF YOUTHANKS TO ALL OF YOU73I.Savin@Prague in 2011