development of room temperature and superconducting ch … · 2007. 5. 21. · institut für...

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Institut für Angewandte Physik LINAC AG H. Podlech, IAP 1 HPPA 2007 HPPA 2007 Mol, Belgium, May 6.-9. 2007 Holger J. Podlech Institut für Angewandte Physik (IAP) J.W.-Goethe-Universität, Frankfurt am Main, Germany Development of Room Temperature and Superconducting CH-Structures for High Power Applications

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Page 1: Development of Room Temperature and Superconducting CH … · 2007. 5. 21. · Institut für Angewandte Physik LINAC AG H. Podlech, IAP 4 HPPA 2007 High efficiency (Z) for low and

Institut für Angewandte PhysikLINAC AG

H. Podlech, IAP 1 HPPA 2007

HPPA 2007

Mol, Belgium, May 6.-9. 2007

Holger J. Podlech

Institut für Angewandte Physik (IAP)

J.W.-Goethe-Universität, Frankfurt am Main, Germany

Development of Room Temperature and SuperconductingCH-Structures for High Power Applications

Page 2: Development of Room Temperature and Superconducting CH … · 2007. 5. 21. · Institut für Angewandte Physik LINAC AG H. Podlech, IAP 4 HPPA 2007 High efficiency (Z) for low and

Institut für Angewandte PhysikLINAC AG

H. Podlech, IAP 2 HPPA 2007

• H-mode cavities – CH-structure

• room temperature (rt) CH-structure (FAIR p-linac)

• superconducting (sc) CH-structure

• Projects (EUROTRANS, IFMIF)

Overview

Page 3: Development of Room Temperature and Superconducting CH … · 2007. 5. 21. · Institut für Angewandte Physik LINAC AG H. Podlech, IAP 4 HPPA 2007 High efficiency (Z) for low and

Institut für Angewandte PhysikLINAC AG

H. Podlech, IAP 3 HPPA 2007

IH-Structure

4-Vane RFQIH-RFQ

CH-Structure

Interdigital H-Mode (IH)B E

++

-- Interdigital H-Mode (IH)BBB E

++

-- B E

++

++

--

--

Crossbar H-Mode (CH)BBB E

++

++

--

--

Crossbar H-Mode (CH)

The Family of H-mode cavities (H11, H21)

Page 4: Development of Room Temperature and Superconducting CH … · 2007. 5. 21. · Institut für Angewandte Physik LINAC AG H. Podlech, IAP 4 HPPA 2007 High efficiency (Z) for low and

Institut für Angewandte PhysikLINAC AG

H. Podlech, IAP 4 HPPA 2007

High efficiency (Z) for low and medium energies (3-100 AMeV)

• Homogeneous distribution of lossesGood cooling possibilities

• Possible cw operation

• Use of KONUS Less rf defocusinglong lensfree sections

• High real estate gradients

• High mechanical stability

• Room temperature- and superconducting operation

H - CavityH - Mode211

RF Frequency 432 MHz

The CH-StructureCross-Bar H-Mode-Structure

Page 5: Development of Room Temperature and Superconducting CH … · 2007. 5. 21. · Institut für Angewandte Physik LINAC AG H. Podlech, IAP 4 HPPA 2007 High efficiency (Z) for low and

Institut für Angewandte PhysikLINAC AG

H. Podlech, IAP 5 HPPA 2007

rt IHE< 30 AMeV

30<f<250 MHz

rt CH E< 100 AMeV

150<f<700 MHz

sc CH E< 100 AMeV

150<f<700 MHz

H-mode DTL- cavities

Page 6: Development of Room Temperature and Superconducting CH … · 2007. 5. 21. · Institut für Angewandte Physik LINAC AG H. Podlech, IAP 4 HPPA 2007 High efficiency (Z) for low and

Institut für Angewandte PhysikLINAC AG

H. Podlech, IAP 6 HPPA 2007

p-bar target

p-linac

Super- FRS

SIS100SIS300

HESR

CRRESR

Unilac

The FAIR Accelerator ComplexSIS 100

NESR

HESR Antiproton Prod. Target

SIS18

CR

GSI Today

RESR

p-linac SIS 300

UNILAC

FAIR 100 m

FAIR: Facility for Antiproton and Ion Research

7⋅1010 cooled / hour

2⋅1016 p / hour

Requirement: 7*1012 p/pulseUNILAC: Factor 500 too low

New dedicated p-injector

p

Page 7: Development of Room Temperature and Superconducting CH … · 2007. 5. 21. · Institut für Angewandte Physik LINAC AG H. Podlech, IAP 4 HPPA 2007 High efficiency (Z) for low and

Institut für Angewandte PhysikLINAC AG

H. Podlech, IAP 7 HPPA 2007

95 keV 3 MeV 70 MeV

Source LEBT RFQ CH-DTLRe-Buncher

to Dump

to SIS18

Particles Protons RF drivers (6x) 2.5 MW KlystronsCurrent (mA) 70 Pulse power (MW) 4.9Energy (MeV) 70 Beam pulse length (μs) 36Frequency (MHz) 325.224 Repetition rate (Hz) 4RF structures (6x) r.t. CCH Linac length (m) 25

FAIR proton-linac

High gradients (3-7 MV/m), low duty cycle r.t. CH-structures

Page 8: Development of Room Temperature and Superconducting CH … · 2007. 5. 21. · Institut für Angewandte Physik LINAC AG H. Podlech, IAP 4 HPPA 2007 High efficiency (Z) for low and

Institut für Angewandte PhysikLINAC AG

H. Podlech, IAP 8 HPPA 2007

The Coupled CH (CCH)

Coupling Cavity (E010)

Coupling of two CH-sections (H21-mode) via a resonant oscillating coupling cell (E010-mode)

Page 9: Development of Room Temperature and Superconducting CH … · 2007. 5. 21. · Institut für Angewandte Physik LINAC AG H. Podlech, IAP 4 HPPA 2007 High efficiency (Z) for low and

Institut für Angewandte PhysikLINAC AG

H. Podlech, IAP 9 HPPA 2007

The 2 kW level (4kW/m, ~ 310 kV) has been reached within 20 minutes

Measured Q0: 13000 (95 % Ideal MWS Value)

r.t. CH-prototype Test Setup

Page 10: Development of Room Temperature and Superconducting CH … · 2007. 5. 21. · Institut für Angewandte Physik LINAC AG H. Podlech, IAP 4 HPPA 2007 High efficiency (Z) for low and

Institut für Angewandte PhysikLINAC AG

H. Podlech, IAP 10 HPPA 2007

Motivation for the Development of the Superconducting CH-Structure

Several fixed velocity accelerators with cw operation areunder discussion

(i.e. Spallation neutron sources, IFMIF, Transmuter, isotope production...)

Superconducting operation

lack of efficient superconducting low β cavities,whereas efficient means large energy gain per cavity

Page 11: Development of Room Temperature and Superconducting CH … · 2007. 5. 21. · Institut für Angewandte Physik LINAC AG H. Podlech, IAP 4 HPPA 2007 High efficiency (Z) for low and

Institut für Angewandte PhysikLINAC AG

H. Podlech, IAP 11 HPPA 2007

SuperconductingCH-Prototype

The first low energy s.c.multi cell cavity

140 mm

Gap number 19

Length (mm) 1048

Frequency (MHz) 350

(Ra/Q)G (Ω2) 178000

W (mJ/(MV/m)2) 155

β 0.1

Ep/Ea (βλ-definition) 5.2

G=RsQ0 (Ω) 56

Ra/Q (Ω) (T incl.) 3180

Bp/Ea (mT/(MV/m)) 5.7

Q0 (BCS, 4.4K, 352 MHz) 1.5x109

Page 12: Development of Room Temperature and Superconducting CH … · 2007. 5. 21. · Institut für Angewandte Physik LINAC AG H. Podlech, IAP 4 HPPA 2007 High efficiency (Z) for low and

Institut für Angewandte PhysikLINAC AG

H. Podlech, IAP 12 HPPA 2007

Cryogenic Test of the sc CH-cavity

tP

rP

fP

fon PP =rP

eoff PP =

Page 13: Development of Room Temperature and Superconducting CH … · 2007. 5. 21. · Institut für Angewandte Physik LINAC AG H. Podlech, IAP 4 HPPA 2007 High efficiency (Z) for low and

Institut für Angewandte PhysikLINAC AG

H. Podlech, IAP 13 HPPA 2007

Q0 versus Gradient and Voltage

L=n/2βλ=9.5βλGradient Voltage

Page 14: Development of Room Temperature and Superconducting CH … · 2007. 5. 21. · Institut für Angewandte Physik LINAC AG H. Podlech, IAP 4 HPPA 2007 High efficiency (Z) for low and

Institut für Angewandte PhysikLINAC AG

H. Podlech, IAP 14 HPPA 2007

Projects and possible applications (sc CH)

EUROTRANS (Nuclear waste transmutation)

IFMIF (Fusion material research)

Page 15: Development of Room Temperature and Superconducting CH … · 2007. 5. 21. · Institut für Angewandte Physik LINAC AG H. Podlech, IAP 4 HPPA 2007 High efficiency (Z) for low and

Institut für Angewandte PhysikLINAC AG

H. Podlech, IAP 15 HPPA 2007

A CH-Injector for XADS/EUROTRANS

Page 16: Development of Room Temperature and Superconducting CH … · 2007. 5. 21. · Institut für Angewandte Physik LINAC AG H. Podlech, IAP 4 HPPA 2007 High efficiency (Z) for low and

Institut für Angewandte PhysikLINAC AG

H. Podlech, IAP 16 HPPA 2007

• High flux source of fast neutrons

• Development of new material for fusion reactors

• Up to 100 dpa/fpy

• Liquid Li target

• Beam: 40 MeV Deuterons

• Beam current 2x125 mA

• Beam power: 10 MW

• Duty cycle 100%

• RFQ/CH combination with 175 MHz

IFMIF

International Fusion Material Irradiation Facility

Reference design: Alvarez!

Page 17: Development of Room Temperature and Superconducting CH … · 2007. 5. 21. · Institut für Angewandte Physik LINAC AG H. Podlech, IAP 4 HPPA 2007 High efficiency (Z) for low and

Institut für Angewandte PhysikLINAC AG

H. Podlech, IAP 17 HPPA 2007

r.t./s.c. CH-linac for IFMIF

s.c. cavity doublet with tuner

• One room temperature H-mode cavity (2.5-4.5 AMeV)• 8 superconducting CH-cavities (per linac)• Sc cavity RF power: 30 W• Static losses: 20 W per cavity

800 W@4K • 3 Cryo plants (500 W each) for IFMIF, 2 in operation ,1 stand by• Beam loading per cavity 400-500 kW• Power couplers: 2 coaxial-couplers per cavity with 250 kW

Main advantages

Stable cw operation without thermal problems

Significant operational cost savings: 5 MW 45 Mio kWh/a

Page 18: Development of Room Temperature and Superconducting CH … · 2007. 5. 21. · Institut für Angewandte Physik LINAC AG H. Podlech, IAP 4 HPPA 2007 High efficiency (Z) for low and

Institut für Angewandte PhysikLINAC AG

H. Podlech, IAP 18 HPPA 2007

IFMIF IAP Proposal: sc CH-Linac

Page 19: Development of Room Temperature and Superconducting CH … · 2007. 5. 21. · Institut für Angewandte Physik LINAC AG H. Podlech, IAP 4 HPPA 2007 High efficiency (Z) for low and

Institut für Angewandte PhysikLINAC AG

H. Podlech, IAP 19 HPPA 2007

People

U. RatzingerH. KleinH. PodlechH. LiebermannC. ZhangA. Bechtold

C. ClementeR. TiedeM. BuschF. DziubaD. BänschI. Müller

Page 20: Development of Room Temperature and Superconducting CH … · 2007. 5. 21. · Institut für Angewandte Physik LINAC AG H. Podlech, IAP 4 HPPA 2007 High efficiency (Z) for low and

Institut für Angewandte PhysikLINAC AG

H. Podlech, IAP 20 HPPA 2007

Conclusion

• The CH-structure is a very efficient DTL-Structure

larger real estate gradient, smaller number of sub-systems

reliability, cost reduction

• Suitable for room temperature and superconducting operation

• Prototypes have been developed and tested successfully

• Projects: FAIR p-linac, EUROTRANS, IFMIF

Page 21: Development of Room Temperature and Superconducting CH … · 2007. 5. 21. · Institut für Angewandte Physik LINAC AG H. Podlech, IAP 4 HPPA 2007 High efficiency (Z) for low and

Institut für Angewandte PhysikLINAC AG

H. Podlech, IAP 21 HPPA 2007

Thank you for your attention

Page 22: Development of Room Temperature and Superconducting CH … · 2007. 5. 21. · Institut für Angewandte Physik LINAC AG H. Podlech, IAP 4 HPPA 2007 High efficiency (Z) for low and

Institut für Angewandte PhysikLINAC AG

H. Podlech, IAP 22 HPPA 2007

Effective Shunt Impedance of DTL-Cavities

Page 23: Development of Room Temperature and Superconducting CH … · 2007. 5. 21. · Institut für Angewandte Physik LINAC AG H. Podlech, IAP 4 HPPA 2007 High efficiency (Z) for low and

Institut für Angewandte PhysikLINAC AG

H. Podlech, IAP 23 HPPA 2007

r.t. CH-cavity and MEBT for EUROTRANS

Steerer diagnostic

~ 215 cm

~ 175 cm

Page 24: Development of Room Temperature and Superconducting CH … · 2007. 5. 21. · Institut für Angewandte Physik LINAC AG H. Podlech, IAP 4 HPPA 2007 High efficiency (Z) for low and

Institut für Angewandte PhysikLINAC AG

H. Podlech, IAP 24 HPPA 2007

QuadsTubes

Envelopes r.t. CH-cavity

Page 25: Development of Room Temperature and Superconducting CH … · 2007. 5. 21. · Institut für Angewandte Physik LINAC AG H. Podlech, IAP 4 HPPA 2007 High efficiency (Z) for low and

Institut für Angewandte PhysikLINAC AG

H. Podlech, IAP 25 HPPA 2007

Beam Dynamics (KONUS)Code: LORASR

KONUS (Combined Zero Degree Structure)

0-degree-sections reduce rf defocusingLess focusing elements requiredlong lens free sectionsslim drift tubeshigh shunt impedance

Strong triplet-channel