dafne upgrades - lnf.infn.it · dafne experience not critical • feedbacks: challenging but ok •...
TRANSCRIPT
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DAFNE upgrades
C. Biscari
15 novembre 2002
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present next future
• Lmax = 0.8 10 32 cm-2 sec-1 1.5 10 32
• Lint/day = 4.5 pbarn-1 8
• I+ = 1.2 A 2• I- = 0.9, 1.4 A 2• N bunches = 50 , 100 100
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Upgrades – future future
• Higher E ~ 1031 @ 1 + 1 GeV
• Higher L > 1033 @ 510 + 510 MeV
• BOTH with the same machine ?
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Higher E ~ 1031 @ 1 + 1 GeV
Rinaldo Baldini will give us a talk (december 2002)on Fenice2 and other measurements at this energy
Riunione alla SIF (fine settembre 02)Bini, Zallo, Filippi Files pdf disponibili
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FENICE experiment @ ADONE
<L> = 5 1028 cm-2 sec -1
Lp = 1029 cm-2 sec -1
L int = 0.48 pb-1
With ~ 100 pb-1 answers to open questions on FF
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Higher L > 1033 @ 510 + 510 MeV
Fabio Bossi and Gino Isidoriwill gave us a talk before before the end of the yearon the physics motivation for this request
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• High currents• 120 bunches - feedbacks• Impedance• Vacuum• Crossing angle - parasitic crossings• Coupling - beam sizes
Concerns @ DAFNE design
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DAFNE experienceNot critical• Feedbacks: challenging but ok• Crossing angle• Coupling• IP �*
Critical• Damping time still long• Non linearities• 2 IPs • Beam lifetime and background: Touschek
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1) Higher E
2) Higher L
3) 1) + 2)
1) Easy accelerator physicsHardwareCostsInjection/ramping
Challengingflat/roundhigh currentmore damping…
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Possible scenarios
• Minimum modifications to increase the energy
• Change as much as needed to increase the luminosity
• and include whatneeded to increase the energy
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Higher Energy : 2 GeV (1+1)
Easier luminosityNaturally increase radiation damping and
lifetime
But
hardware, costs, injection
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0
50
100
150
200
250
PL105 PL106 PL107 PS101 PS104 PS105 PS106 PS204 PS205 PS206 PL204 PL205 PL206
large quadrupolesI (510)I (1000)
I (A)
saturation
510 MeV1 GeV
QUADRUPOLES
0
100
200
300
400
500
600
700
PL101PL102PL103PL104PL108PL109PL110PS102PS103PS107PS108PS109PS110PS201PS202PS203PS207PS208PS209PL207PL208PL209PL210
small quadsI (510)
I (1000) lin
saturation
I (A)
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510 MeV1 GeV
SEXTUPOLES
0
50
100
150
200
250
300
PL102 PL103 PS101 PS102 PS103 PS202 PS203 PL202 PL203
LARGE SEXTS
I (510)I (1000)
I (A)
saturation
0
50
100
150
200
250
300
350
400
PL101 PL104 PS104 PS201 PS204 PL201 PL204
SMALL SEXTS
I (510)I (1000)
I (A)
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DIPOLES
Long: L =1.21mShort: L = 0.99 m
� = 1.4 mLT = 8.8 mB = 1.2 T
B = 1.76 T @ 1 GeV� = 245 °
Missing 115 ° = 2.8m
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Substitute with SC dipoles, same total dimension
saving vacuum chamber
Add adyacent dipoles (pm, sc, …) simmetrically around each dipole, needed > 3 T to fit in the spaces
Modify layout, substitute with normal conducting dipoles, change arc vacuum chamber
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SPLITTERS Maximum current : 750 ANow 420 - 460
Compensators o.k. - Compensate the detector field
Others: correctors, skews, octupoles,….Can be adapted…
Low beta: control if combinations of KLOE + FINUDA quadscan be used to design a new low-beta
Wigglers o.k. – larger �, but still more radiation
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Uo = 1.88 10-15 �3 E I2 (m-1)
Uo (keV) ~ I2 (m-1) @ 510 MeV
Uo (keV) ~ 15 I2 (m-1) @ 1 GeV
Now : I2 = 9.8 m-1 -> Uo = 9.4 keV
1GeV same �d, same wigglers:I2 = 7.2 m-1 Uo = 108 keV
increasing �d, same wigglers: I2 = 5.6 m-1 Uo = 85 keV
Energy lost per turn
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Luminosity 5 1031 cm-2 sec-1
I = 1ANb = 50
fcoll = 153 MHzIb = 20 mA = 4 1010 part/bunch
�x �y = 4 10-8 m2
�x = 2 mm�y = 20 �
… easyRf …
Feedbacks …
Vacuum …
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L estimation at 2 GeV
Peak L should not decrease asthe energy increases
Now: Lav = 0.7 Lpeak ~ 5 1031
Injection at lower energy ~ factor 2 below:Lav = 0.35 Lpeak
Feasible to achievethe request of1pb-1/day = 1031 average
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Higher luminosity at the � energy
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“Conservative” L upgrade
• Add damping: sc wigglers and/or sc dipoles• Increase crossing angle: increase rf frequency
and n. of buckets -> bunches• Increase V for lifetime • Eliminate 2nd IP• Minimize �* and bunch length• Background estimation and shielding• 2 independent injection chains
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Damping
Radiated energy per turn Uo � E4 I2 I2 �
ds�
2�
Damping time:few tens of ms
1�
�
E3 I2
To
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Wigglers
NOW
4 wigglers/ring ��= 0.94 mB = 1.8 TLTOT = 8mI2 ~ 5.7 m-1
--->
4 SC wigglers/ring ��= 0.34 mB = 5 TLTOT = 10mI2 ~ 60 m-1
Damping increased by a factor 10...
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Wigglers added to optimize L at lower energies
For example:
LEPP, Cornell University (Laboratory for Elementary-Particle Physics)
Optimization of luminosity performance of the 768 m circumference e+e- collider CESR at 1.9 GeV is a critical objective of the CESR-c conversion project. In order to achieve a reasonable damping rate at the low energy approximately 18 m of 2.1 Tesla peak field wigglers will be installed. 90% of the synchrotron radiation power in the ring will be produced in the wigglers. The non-linear properties of the wigglers are a concern for high luminosity operation.
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AbstractThe superconducting 3.5 T wiggler was designed and fabricated for the ELETTRA storage ring (Italy) forthegeneration of synchrotron radiation with critical energy of9.3 keV. The presented wiggler is a 49 polesuperconducting magnet with maximum field of 3.5 Teslainserted into a special liquid helium cryostat. The wigglerdesign and main parameters are presentedin this article.Results of magnetic field measurements and wiggler testing in different modes of operation are discussed.. The general view of the magnet isshown in Fig.1.The main goal of the wiggler design was to obtain a magnetic field of 3.5 Tesla while keeping the periodof the magnet structure as short as possible. The wiggler period is 64 mm. The shape of the central pole is elliptical with axes 140 mm and 7 mm. The 45 central coils consist of two different sections which are wound one over another. Each section is energised by different currents in order to obtain the optimal field-current characteristics
A SUPERCONDUCTING 3.5 T MULTIPOLE WIGGLER FOR THEELETTRA STORAGE RINGA.Batrakov, V.Jurba, S.Khrushchev, G.Kulipanov, E.Kuper, M.Kuzin, A.Medvedko, N.Mezentsev,V.Shkaruba, BINP, Novosibirsk,Russia;D.Zangrando, B.Diviacco, R.P.Walker1 , Sincrotrone Trieste, Trieste, ItalyProceedings of EPAC 2002, Paris, France
Abstract
A SUPERCONDUCTI NG 3.5 T MULTIPOLE WIGGLER FOR THEELETTRA STORAGE RI NGA.Batrakov, V.Jurba, S.Khrushchev, G.Kulipanov, E.Kuper, M.Kuzin, A.Medvedko, N.Mezentsev,V.Shkaruba, BINP, Novosibirsk ,Russia;D.Zangrando, B.Div iacco, R.P.Walker1 , Sincrotrone Trieste, Trieste, ItalyProceedings of EPAC 2002, Paris, France
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ELETTRA wiggler – 3.5T
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A SUPERCONDUCTING 7T MULTIPOLE WIGGLER FOR BESSY II: MAIN CHALLENGES AND FIRST FIELD MEASUREMENTS�
D. Berger, Hahn-Meitner-Institut, Glienicker Str. 100, 14109 Berlin, Germany E. Weihreter, BESSY, Einsteinstraße 15, 12489 Berlin, Germany
N. Mezentsev, V. Shkaruba, BINP, Acad. Lavrentiev prospect 11, 630090 Novosibirsk, Russia Proceedings of EPAC 2002, Paris, France
Abstract To provide high flux hard X-ray beams with a critical energy of 16.8
keV for material research, a 17 pole superconducting 7T wigglerhas been built for the BESSY II ring. The scope of this paper is to describe the magnetic layout and the main technological challenges of this unique insertion device. Secondly we will report on first tests of the magnet at high fields including the quenching behaviour. Magnetic fields were measured using Hall-probes to determine the on-axis field distribution as well as the lifetime in the persistent current mode and the remanent field strength. A first evaluation of the measured fields including a comparison with 3D-field calculations indicates that the specified field quality could be met.
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BESSY wiggler – 7T
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Increase rf frequency
Present: 369 MHzC = 98 m h = nmax = 120
Going to 500 MHzC = 100 m h = nmax = 160
Decrease bunch length
Distance between bunches:D = 0.8 m
D = 0.6 m
Increase fcoll
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2 independent injection chains
Ratio between integrated and peak luminosity depends
on:
•Beam lifetime •Injection efficiency
KLOE runs
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Luminosity 1033 cm-2 sec-1
I = 5ANb = 140
fcoll = 467 MHzIb = 36 mA = 7 1010 part/bunch
�x �y = 1.8 10-8 m2
�x = 1 mm�y = 18 �
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Ring for two energies
1�
�
E3 I2
To
16 UoD -4UoWUoD - UoWEnergy lost per turn
�oD / 8 - �ow / 2 �oD - �owDampingtime
2 �w�wWigglers
�o�oDipoles
3.31.7B� (T m)
1.00.5Energy(GeV)
� constantB ramping
B constant
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… ideas for higher L
• Round beam (Novosibirsk style)• Round beam + 2 IPs (H / V)
• AWM
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Round beam (Novosibirsk style)
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From a seminar by Valishev @ KEK, march 2002
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Hadron’s colliders:working point near the main coupling resonance
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Ruggiero – Zimmermann (CERN) 2 Ips – H/V
The beam-beam effect between the horizontal and the vertical crossing is compensated
The luminosity increases with crossing angle and bunch length
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AWM: All Wiggler Machine
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Starting point
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Two rings, multibunchOnly 1 IP, 1 detector
Add SC wigglers / dipoles
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Round beam = no coupling
90° 90°
D � Mode
1
2
D �
D �
One turn
detector
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Interaction Region for flat and round beam
Ld
IP
d = Bd Ld/2B�����
C1 C2
FLAT beam: C1 = C2 = - 22.5°
ROUND beam: C1 = C2 = 22.5°
tot = 0
tot = 90°
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Ld = 3m -> Bd ��������
(90° = 5.3 Tm @ 510 MeV)
Detector: 45°
Compensators: 45°/2 Lc = 20 cm -> Bc �������
Example:
Superconducting compensators inside the detector(Bassetti, Biscari, Milardi, 1993, L-11Alternative Interaction Region Design)
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Flat�x* = 1m�y* = 2cm
Round�x* = 4cm�y* = 4cm
Betatron functions inside the detector
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Ld
IP
C1 C2
Add focusing with ‘wiggling sc solenoids’
Positive Bs + Negative Bs = 0
C1 + C2 + Bd = 0 FLATC1 + C2 + Bd = 90° ROUND
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Betatron functions inside the detector
Flat�x* = 1m�y* = 2cm
Round�x* = 2cm�y* = 2cm
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Can we make an experiment on DAFNE?
Round beam with Finuda?
Finuda detector: BL = 2.6 Tm => 44 °
+ Compensators: 22° + 22 °
Almost 90°
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FINUDA IR - now
compensator
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FINUDA IR with equal �*
� *1 = � *2 = 20cm
� *1 = � *2 = 30cm
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But trajectory off-axis + rotation of 90° transform the horizontal separation into vertical
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Off-axis + 90 °:
Two equal rings vertically separated
Round beam
Multibunch
Only 1 crossing point
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When?Present schedule:
2002 : KLOE + DEAR2003 : shutdown for FINUDA, KLOE, ...
FINUDA + KLOE runs2004: FINUDA + KLOE runs2005 - on
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Some of the items to be studied
Higher energy• Ring structure (����, rf, bunch length,….)• Interaction region• New magnets design• Magnet Ramping with injection @ 510• Diagnostics• Cost estimation
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Higher luminosity… everything
Flat/round beam => Ring structure• Wigglers• Rf• IR• Background• Injection system• …
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Next appointments
• Seminar bossi/isidori• Seminar baldini• Workshop @ Thuile (march 2003) – to
be organized• Workshop @ Alghero (june 2003) – to
be organized