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Electron Cooling in the Recycler Electron Cooling in the Recycler Ring Ring Alexander Shemyakin (Fermilab/AD) May 31, 2005
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Electron Cooling in the Recycler Ring Alexander Shemyakin (Fermilab/AD) May 31, 2005.

Jan 20, 2016

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  • Electron Cooling in the Recycler RingAlexander Shemyakin (Fermilab/AD)May 31, 2005

  • Tevatron luminosity and antiprotonsThe Tevatron luminosity is linear with the total number of antiprotons available for the Tevatron store. The antiproton beam quality is characterized by the phase-space density. To achieve higher luminosity this density needs to be increased.

  • Fermilabs antiproton production chainInconel targetDebuncher (stochastic cooling)Accumulator (stochastic cooling)

    8 GeV8 GeVUntil 2005Electron cooling in the Recycler Ring eliminates one of the bottlenecks in the long chain of the antiproton production. is the relative phase-space density

  • Idea of Electron coolingThe idea of electron cooling is a heat exchange through Coulomb scattering between hot heavy particles (antiprotons) and cold electrons while the beams are mixed in a cooling section.Was invented in 1967 by G.I. Budker (INP, Novosibirsk) as a way to increase luminosity of p-p and p-pbar colliders.

    First tested in 1974 with 68 MeV protons at NAP-M storage ring at INP (Novosibirsk).CERN- ICE 1977 1979Fermilab 1979 - 1982

  • Low energy coolersWell established techniques for electron energies below 300 keV.A strong, continuous longitudinal magnetic field from the gun to the collectorAn electrostatic accelerator working in the energy- recovery modeExample of a 300 keV, 3 A cooler produced by Budker INP for IMP, Lanzhou (China). The voltage difference between the gun and collector ~ 3 kV.

  • Difficulties of implementing at relativistic energiesHigh electron beam power:4 MeV * 0.5 A = 2 MW DC!

    Beam quality:The electron beam temperature (in the rest frame) should be comparable with the cathode temperature of 1200K (only a factor of ~10 increase is allowed for the transverse degree of freedom)

    Design parameters of the RR ECool beam

    Energy4.34 MeVBeam current0.5 Amps DC Angular spread0.2 mrad Effective energy spread 300 eV

  • History of relativistic electron coolingFermilab, 1983: D. Cline et al., Intermediate energy electron cooling for antiproton sources using a Pelletron acceleratorFor a pulsed electron beam in a Pelletron the beam quality is adequate for electron coolingNovosibirsk, 1987: successfully tested a prototype 1-MV, 1-A electron beam system.Continuous magnetic fieldAcceleration tubes are not sensitive to vacuum UVFermilab, UCLA, NEC, 1989: tested a 2-MV, 0.1-A DC recirculation system with a Pelletron.Poor stabilityFermilab, IUCF, NEC, 1995: started to work on a 2-MV Pelletron again- beginning of the RR ECool project

  • PremiseSolution for a high-power beam generator: use of a standard electrostatic accelerator (Pelletron) and non-standard focusing scheme Recirculation (energy/charge recovery) schemeNo continuous magnetic fieldA low-magnitude longitudinal magnetic field in the cooling section and at the cathode, but a lumped focusing in the remaining part of the beam line

    Failure of the previous attempt was recognized to be caused by high losses in the acceleration tubesCurrent losses needs to be decreased below 0.01%

    New solutions for the gun and collector were found. A gun with a negatively biased control electrode to suppress the beam halo and provide the beam transport at all currentsEffective suppressing of secondary electrons in the collector can be done by applying a transverse field in the collector cavity

  • Stage I - Test at NEC (Middleton, WI)GOALTo demonstrate a stable (~1 hour) generation of a 0.2 A relativistic beam using an existing 2 MV Pelletron at NEC

    Nov. 95:project startedJan. 97:first recirculated current (10 A)Dec. 97:Max. recirculated current of 0.2 AMay. 98:0.2 A for 1 hours at 1.3 MeVDec. 98:Max. current of 0.7 AJan. 99:Gun solenoid (200 G) installedFeb. 99: 5 MeV Pelletron orderedMay.99:0.9 A with 200 G at the cathodeHow to scale the result for 1.3 MeV beam in a 2-MV tubes to a 4.3 MeV beam in a 5-MV accelerator ?

  • Stage II short line at WideBand Building (Fermilab)New means to improve stability: ion stoppers, crash scraper, closing the gun in 1 msDiagnostics: BPMs, scrapers, flying wireOperation was stable only at 3.5 MV. The tubes clearly needed to be extended. Now the main question was the beam quality.GOAL : To demonstrate a stable generation of a 0.5 A, 4.34 MeV beam in a short beam line

    Feb 99: 5 MV Pelletron ordered.May 01: First beam of 30 A in the collector.Dec 01: 0.5 A at 3.5 MV Apr 02: NEC replaced acceleration tubesOct 02: 0.5 A at 4.34 MeVNov 02: Imax = 1.7 A at 3.5 MV Shut down to install the full beamline

  • Stage III full- length line at WideBandThe beam line was very similar to the final one at MI-31A novel type of the beam optics, angular momentum dominated Developed a technique of precise measurements of the solenoid field qualityBeam envelope measurements with movable orificesFinal version of BPM electronics

    Jul- 03 - first DC beam in the full- scale lineDec-03- 0.5 A DC beamMay-04- 0.1 A beam with required properties in the cooling section

  • Final stage- Cooler in the RecyclerJun. 2004 Jan. 2005- assembling the cooler in MI-31/30Oct 2004- magnetic measurements in cooling sectionApr 2005- first DC beam in the collector passed through the cooling section

  • Difficulties (some of them) and solutionsFull dischargesImprovements in the protection system (closing the gun in 1 s)Minimizing current losses to acceleration tubes (dI/I
  • CoolingOne of the first indications of interaction between antiprotons and electrons. The plot shows evolution of antiproton energy distribution (log scale) after turning on an electron beam. Initially antiprotons occupy the entire momentum aperture of the Recycler.First interaction - July 9, 2005

    First cooling- July 11, 2005

    First electron cooling-assisted shot to Tevatron- July 12, 2005

  • Drag Force as a function of the antiproton momentum deviation100 mA, nominal cooling settings

  • First cooling rate measurements published

  • Electron cooling between transfers/extractionElectron beam is moved inStochastic coolingafter injectionElectron beam out (5 mm offset)Electron beam current 0.1 A/divTransverse emittance 1.5 p mm mrad/divElectron beam position 2 mm/divLongitudinal emittance (circle) 25 eVs/divPbar intensity (circle) 16e10/div~1 hour100 mA195e10~60 eVs254e10

  • Evolution of the number of antiprotons available from the RecyclerMixed mode operationEcool implementationRecycler only shots01/10/05 02/18/06

    Chart1

    42

    47

    85

    90

    91

    54

    56

    78

    67

    74

    89

    37

    37

    45

    45

    49

    49

    91

    91

    72

    71

    71

    69

    70

    71

    71

    86

    86

    81

    81

    68

    16

    57

    48

    78

    64

    85

    92

    98

    91

    43

    76

    65

    70

    63

    56

    124.1

    113

    166

    51

    74

    58

    39

    108

    60

    116

    90

    138

    124

    121

    143

    144

    44

    66

    138

    94

    56

    69

    58

    14

    16

    59

    7

    33

    32

    42

    45

    49

    47

    65

    52

    128

    85

    51

    59

    74

    43

    71

    95

    30

    90

    32

    62

    106

    83

    53

    100

    81

    58

    61

    60

    94

    109

    51

    46

    92

    137

    116

    111

    Ecooling

    59.5

    90.7

    30.6

    85

    48

    100

    60

    100

    143

    126

    59

    59

    89

    85

    92

    81

    97

    116

    112

    137

    111

    182

    46

    41

    98

    110.5

    143

    60

    109

    64

    70

    136

    70

    113

    165

    129

    134

    141

    142

    216

    241

    90

    55

    69

    77

    225

    280

    235

    257

    183

    153

    209

    117

    197

    228

    111

    168

    191

    219.57

    223

    285

    247

    266

    320

    220

    256

    89

    171

    248

    204

    200

    300

    248

    252

    174

    99

    132

    77

    181

    72

    55

    163

    219

    288

    236

    137

    270

    255

    273

    260

    354

    326

    323

    289.7

    284

    198

    154

    115

    127

    182

    30

    107

    176

    201

    139

    209

    181

    334

    258

    258

    418

    197

    131

    150

    283

    166

    243

    Number of antiprotons (x 1010)

    Sheet1

    data

    DateIntensityLong emittance 90%Long emittance 95%RMS mom spread90% mom spreadBucket lengthTrans emittanceNotes

    2/14/041.88E+0114.018.215linear ramp, two bunches

    4/7/041.60E+017.09.13.36linear ramp,single bunch

    2/20/041.20E+0263.081.95.37Barrier bucket

    3/12/043.50E+0121.027.32.37Barrier bucket

    3/14/047.80E+0151.061.23.110.54.87Barrier bucket

    3/25/043.57E+0131.938.32.89.23.33Barrier bucket

    4/7/041.60E+017.09.23.511.70.36Barrier bucket

    4/8/043.10E+0111.314.33.70.67Barrier bucket

    4/12/045.20E+0120.625.6413.21.26Barrier bucket

    4/23/049.70E+0149.058.83.110.34.64Barrier bucket

    4/21/047.50E+0140.752.9

    4/24/048.70E+0151.066.35.4

    4/26/041.26E+0264.083.26

    4/27/041.23E+0254.164.93105.33Before instability

    4/30/041.17E+0250.060.03.110.34.74.2Barrier bucket

    4/30/041.30E+0258.169.6310.25.73.6

    5/3/041.45E+0263.876.53.210.65.854.3

    5/28/044.33E+0116.319.72.58.41.855

    6/9/046.70E+0130.837.23.311.12.65before mining for mixed mode

    6/29/047.78E+0123.428.43.210.925Barrier bucket, before mining, after linear rf

    7/6/047.50E+0123.028.03.411.61.85Barrier bucket, before mining, after linear rf

    7/16/049.10E+0129.135.33.511.72.265Barrier bucket, before mining, after linear rf

    7/20/046.04E+0122.327.23.310.81.825.4Barrier bucket, before mining, after linear rf

    7/20/04626234.5

    7/21/04505023.1

    8/5/04424220.9

    8/11/04303018.8

    8/12/04404020.3

    From This Time on we started

    12/29/046.62E+0118.928.02.9101.85Barrier bucket, before mining, after linear rf

    1/7/052.63E+0111.113.83.310.90.774.2Barrier bucket, before mining, after linear rf

    1/10/054.23E+0114.717.72.68.61.574Barrier bucket, before mining, after linear rf

    1/11/053.11E+0111.614.53.411.30.775Barrier bucket, before mining, after linear rf

    1/15/05331414

    1/17/058.57E+0125.931.32.99.72.545.3Barrier bucket, before mining, after linear rf

    1/18/059.02E+0131.738.22.99.73.154Barrier bucket, before mining, after linear rf

    1/25/055.40E+0118.322.02.79.31.94.3Barrier bucket, before mining, after linear rf

    1/27/054016.0

    1/26/054.04E+0112.416.24.2140.454.5Barrier bucket, before mining, after linear rf

    1/28/055.61E+0118.022.13.511.91.294.1Barrier bucket, before mining, after linear rf

    1/29/057.79E+0125.030.63.612.31.834.4Barrier bucket, before mining, after linear rf

    1/31/057.01E+0122.427.33.411.51.754Barrier bucket, before mining, after linear rf

    2/1/056.72E+0121.626.231024.2Barrier bucket, before mining, after linear rf

    2/3/057.45E+0124.429.63.3511.11.974Barrier bucket, before mining, after linear rf

    2/5/055.81E+0122.827.93.4411.51.763.3Barrier bucket, before mining, after linear rf

    2/6/054.34E+0116.219.62.79.141.6663.7Barrier bucket, before mining, after linear rf

    2/8/058.93E+0134.241.63.7612.42.464.5

    TDR2.60E+0254.070.25538.547.75

    6.50E+0254.070.25538.5125

    1.80E+0254.070.25538.536.855

    2.00E+016.07.85.854.0954.095

    2.00E+010.00.0000

    0.00E+000.0

    1.80E+0296.0

    6/30/047932

    7/6/047728

    7/16/049235.3

    12/23/044120.9

    12/29/046628

    1/10/054220

    1/12/054722

    1/17/058536

    1/18/059040

    1/20/059143

    1/24/055422.1

    1/28/055627

    1/30/057829

    2/1/056726

    2/3/057428

    2/8/058941

    2/13/053719

    2/13/053718

    2/17/0545

    2/17/054522

    2/22/054932

    2/22/054932

    2/23/059148

    2/23/059144

    2/24/057236

    2/26/057130

    2/26/057129

    2/27/056939

    2/27/057038

    3/4/057135

    3/4/057135

    3/5/058640

    3/5/058640

    3/7/058140

    3/7/058140

    3/8/056837

    3/9/05168.5

    3/10/055728

    3/12/0548

    3/14/0578

    3/15/056430

    3/17/058543

    3/18/059248

    3/20/059847

    3/21/059148

    3/25/054323

    3/26/057641

    3/27/056530

    3/29/057033

    3/30/056328Started using ibs to help cool

    4/2/055628

    4/4/05124.147

    4/7/05113.046.0

    4/8/05166.059.3

    4/10/0551.025.0

    4/14/0574.031.0

    4/17/0558.027.0

    18-Apr39.019.0

    4/20/05108.040.0

    4/23/0560.028.0

    4/24/05116.054.0

    4/25/0590.035.0

    4/27/05138.052.0

    4/29/05124.045.0

    4/30/05121.045.0

    5/2/05143.052.0

    5/4/05144.051.0

    5/7/0544.020.0

    5/9/0566.028.0

    5/12/05138.051.0

    5/13/0594.037.0

    5/17/0556.022.0

    5/18/0569.026.0

    5/19/0558.024.0

    5/19/0514.09.0

    5/21/0516.010.0

    5/23/0559.025.0

    5/23/057.06.3

    5/24/0533.014.0

    5/26/0532.013.0

    5/27/0542.018.0

    5/28/0545.020.0

    5/29/0549.024.0

    5/31/0547.021.0

    6/2/0565.028.0

    6/4/0552.025.0

    6/6/05128.051.0

    6/7/0585.032.0

    6/8/0551.035

    6/10/0559.031.0

    6/11/0574.030.0

    6/17/0543.020.0

    6/18/0571.030.0

    6/19/0595.042.0

    6/20/0530.014.0

    6/22/0590.041.0

    6/23/0532.014.0

    6/24/0562.024.0

    6/26/05106.045.0

    6/28/0583.033.0

    7/1/0553.023.0

    7/5/05100.040.0

    7/23/0581.026.0

    7/26/0558.041.0

    7/30/0561.025.0

    7/31/0560.026.0

    8/2/0594.041.0

    8/7/05109.040.0

    8/16/0551.025.0

    8/18/0546.022.0

    8/22/0592.044.0

    8/26/05137.078.0

    8/27/05116.078.5

    8/29/05111.076.0

    Ecooling

    7/16/0559.515.9

    7/18/0590.727.0

    7/19/0530.68.5

    7/21/0585.028.0

    7/22/0548.019.0

    7/25/05100.028.0

    7/28/0560.020.0

    8/1/05100.034.0

    8/4/05143.051.0

    8/6/05126.040.0

    8/8/0559.018.0

    8/10/0559.018.0

    8/12/0589.024.0

    8/13/0585.024.0

    8/14/0592.028.0

    8/18/0581.025.0

    8/19/0597.035.0

    8/23/05116.035.0

    8/24/05112.031.0

    8/26/05137.054.0

    8/30/05111.037.0

    9/1/05182.062.0

    9/2/0546.018.0

    9/3/0541.016.0

    9/5/0598.030.0

    9/6/05110.522.9

    9/8/05143.036.0

    9/9/0560.016.0

    9/12/05109.028.0

    9/13/0564.021.0

    9/14/0570.021.0

    9/16/05136.051.0

    9/17/0570.027.0

    9/18/05113.027.0

    9/20/05165.067.0

    9/22/05129.050.0

    9/22/05134.047.5

    9/24/05141.055.0

    9/25/05142.049.0

    9/26/05216.064.0

    9/28/05241.065.0

    9/28/0590.035.0

    9/30/0555.020.0

    10/1/0569.023.0

    10/2/0577.028.0

    10/4/05225.062.0

    10/5/05280.060.0

    10/8/05235.065.0

    10/10/05257.066.0

    10/12/05183.078.0

    10/13/05153.051.0

    10/15/05209.065.0

    10/15/05117.032.0

    10/16/05197.066.0

    10/17/05228.066.0

    10/19/05111.035.0

    10/21/05168.057.0

    10/22/05191.068.0

    10/23/05219.657.0

    10/25/05223.067.0

    10/27/05285.067.0

    10/29/05247.078.0

    10/28/05266.066.0

    10/31/05320.072.0

    11/2/05220.071.0

    11/3/05256.080.0

    11/4/0589.045.0

    11/5/05171.051.0

    11/6/05248.065.0

    11/7/05204.070.0

    11/9/05200.070.0

    11/10/05300.068.0

    11/12/05248.065.0

    11/13/05252.067.0

    11/15/05174.055.0

    12/12/0599.040.0

    12/13/05132.060.0

    12/14/0577.035.0

    12/16/05181.058.0

    12/17/0572.037.0

    12/18/0555.028.0

    12/19/05163.065.0

    12/21/05219.063.0

    12/22/05288.066.0

    12/23/05236.064.0

    12/25/05137.040.0

    12/27/05270.065.0

    12/28/05255.059.0

    12/30/05273.065.0

    1/2/06260.067.0

    1/6/06354.072.0

    1/7/06326.076.0

    1/8/06323.070.0

    1/10/06289.766.0

    1/11/06284.068.0

    1/14/06198.055.0

    1/19/06154.061.0

    1/23/06115.069.0

    1/27/06127.074.0

    1/28/06182.069.0

    1/30/0630.049.0

    2/2/06107.041.0

    2/3/06176.041.0

    2/4/06201.061.0

    2/5/06139.040.0

    2/6/06209.059.0

    2/7/06181.090.0

    2/9/06334.075.0

    2/10/06258.055.0

    2/12/06258.067.0

    2/14/06418.066.0

    2/17/06197.066.0

    2/18/06131.054.0

    2/19/06150.055.0

    2/20/06283.058.0

    2/21/06166.054.0

    2/22/06243.059.0

    2/1/06274.062.0

    2/1/06240.043.0

    Damper Test

    8/23/0558.09.8

    8/24/05112.024.0

    now110.522.9

    2.2222222222

    7.5

    data

    00000

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    Cons data

    Pbar intensity, xE10

    Long emittance (95%), eV-s

    Recycler's best long. emittance as of 04/10/05

    Plot

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    Pink Line

    Post IBS Cooling (3/05 - 8/05)

    blue Line

    Ecool (7/05 - present)

    'Feb/04 - Dec/04'

    Last 5 to Tev

    Pbar intensity, xE10

    Long emittance (95%), eV-s

    Recycler's Long. Emittance with Electron Cooling

    Sheet3

    000

    000

    000

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    0

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    blue Line

    Pink Line

    'Feb/04 - Dec/04'

    Pbar intensity, xE10

    Long emittance (95%), eV-s

    Recycler's Long. Emittance Pre IBS Cooling

    0000000

    0000000

    0000000

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    Pink Line

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    last 5

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    Recycler's Long. Emittance as of 2/28/06

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    Pink Line

    Post IBS Cooling (3/05 - 8/05)

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    'Feb/04 - Dec/04'

    Pbar intensity, xE10

    Long emittance (95%), eV-s

    Recycler's Long. Emittance Post IBS Cooling

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    Mixed Mode Operations

    EcoolImplementation

    Recycler OnlyShots

    Number of antiprotons (x 1010)

    Long emittance

    14

    63

    21

    50.9913654065

    31.908509866

    7.0404649281

    11.2891480685

    48.9543515619

    40.7

    51

    64

    54.1471258502

    50

    49.9728362532

    58.0912629581

    63.8191827374

    16.3045085162

    30.7541904285

    20.6061774981

    7

  • Remaining questionsLife timeThe antiproton life time suffers at strong electron coolingEffect is not dramatic, but its removal will add additional percents to the number of antiprotons in Tevatron

    Ultimate strength of coolingECool works at 3001010 , but additional work may be needed to cool effectively 6001010.

  • SummaryThe relativistic, non- magnetized electron cooling has been demonstratedAllows other laboratories to proceed with further developments:BNL- electron cooling at RHIC, Ee= 54 MeVGSI & TSL- fast cooling of antiprotons, Ee= 4 - 8 MeV

    Fermilab has a world record electron cooling system that has allowed recent advances in luminosity

    A hard limit on the maximum number of antiprotons in the Recycler has been removed. The road to higher luminosities is open.

  • The team (at the final stages)Beam studiesA.BurovK.CarlsonD.BroemmelsiekC.GattusoM.HuG.Kazakevich (BINP, guest scientist)T.KrocS.NagaitsevL.ProstS.PrussS.Seletskiy (U.of Rochester)A.ShemyakinC.SchmidtM.SutherlandV.TupikovA.Warner

    Engineering supportB. KramperJ. LeibfritzL. NobregaG. SaewertK. Williams

    Technical supportM. FrettR. KellettJ. NelsonJ. Simmons

    International collaborationBINP (Novosibirsk, Russia)V. ParkhomchukV. RevaCOSY (Juelich, Germany)D. PrashunBNLA. FedotovPhysics discussions and modelingV. Lebedev

    JINR(Dubna, Russia)I.N. MeshkovA. SidorinANLW. Gai