superconducting rf for storage rings, erls, and linac-based fels … · 2017. 2. 22. · june 26,...

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S. Belomestnykh S. Belomestnykh USPAS 2009, Albuquerque, NM June 26, 2009 Superconducting RF for storage rings, Superconducting RF for storage rings, ERLs ERLs , , and linac and linac - - based based FELs FELs : : Lecture 14 Lecture 14 Overview of remaining challenges

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Page 1: Superconducting RF for storage rings, ERLs, and linac-based FELs … · 2017. 2. 22. · June 26, 2009 USPAS 2009, S. Belomestnykh, Lecture 14: Remaining challenges 2 Short list of

S. BelomestnykhS. Belomestnykh

USPAS 2009, Albuquerque, NM June 26, 2009

Superconducting RF for storage rings, Superconducting RF for storage rings, ERLsERLs, ,

and linacand linac--based based FELsFELs::

● Lecture 14 Lecture 14 Overview of remaining challenges

Page 2: Superconducting RF for storage rings, ERLs, and linac-based FELs … · 2017. 2. 22. · June 26, 2009 USPAS 2009, S. Belomestnykh, Lecture 14: Remaining challenges 2 Short list of

June 26, 2009 USPAS 2009, S. Belomestnykh, Lecture 14: Remaining challenges 2

Short list of most important challenges (personal view)

� Basic SRF studies:

� Nature of residual resistivity and how to consistently achieve

low Rres in cavities.

� Nature of Q-slopes.

� Theory & experimental studies of weak Type II RF

superconductors (Nb): what is the RF critical magnetic field?

� Alternative materials to bulk Nb.

� Cavity development:

� New & alternative cavity geometries;

� New ways to fabricate cavities.

� Other SRF technology challenges

� SRF guns

Page 3: Superconducting RF for storage rings, ERLs, and linac-based FELs … · 2017. 2. 22. · June 26, 2009 USPAS 2009, S. Belomestnykh, Lecture 14: Remaining challenges 2 Short list of

June 26, 2009 USPAS 2009, S. Belomestnykh, Lecture 14: Remaining challenges 3

What causes Rres?

� Record Q reached so far, 2××××1011 corresponds to Rs = 1.5 nOhm and Rres < 0.5 nOhm!� What is the physics behind the residual resistivity?

� Why cannot all cavities be like this?

Page 4: Superconducting RF for storage rings, ERLs, and linac-based FELs … · 2017. 2. 22. · June 26, 2009 USPAS 2009, S. Belomestnykh, Lecture 14: Remaining challenges 2 Short list of

June 26, 2009 USPAS 2009, S. Belomestnykh, Lecture 14: Remaining challenges 4

What is the nature of Q-slopes?

Page 5: Superconducting RF for storage rings, ERLs, and linac-based FELs … · 2017. 2. 22. · June 26, 2009 USPAS 2009, S. Belomestnykh, Lecture 14: Remaining challenges 2 Short list of

June 26, 2009 USPAS 2009, S. Belomestnykh, Lecture 14: Remaining challenges 5

What is the critical RF magnetic field?

� Is it Hc, Hsh, Hc3 or something else?

� We need advances in both theory

and experiments to answer this question

0

500

1000

1500

2000

2500

3000

0 0.2 0.4 0.6 0.8 1

(T/Tc)^2

H [

Oe]

T. Hays (BCP cavity)

New data (EP cavity)

Hsh from GL-theory

Page 6: Superconducting RF for storage rings, ERLs, and linac-based FELs … · 2017. 2. 22. · June 26, 2009 USPAS 2009, S. Belomestnykh, Lecture 14: Remaining challenges 2 Short list of

June 26, 2009 USPAS 2009, S. Belomestnykh, Lecture 14: Remaining challenges 6

Can we make other materials to work better than Nb?

� Nb results are consistent with Hsh

� Nb3Sn results fall short: Can we improve the quality of Nb3Sn film and reach Hsh?

RE cavity

Page 7: Superconducting RF for storage rings, ERLs, and linac-based FELs … · 2017. 2. 22. · June 26, 2009 USPAS 2009, S. Belomestnykh, Lecture 14: Remaining challenges 2 Short list of

June 26, 2009 USPAS 2009, S. Belomestnykh, Lecture 14: Remaining challenges 7

Recent theoretical advances

GL

Page 8: Superconducting RF for storage rings, ERLs, and linac-based FELs … · 2017. 2. 22. · June 26, 2009 USPAS 2009, S. Belomestnykh, Lecture 14: Remaining challenges 2 Short list of

June 26, 2009 USPAS 2009, S. Belomestnykh, Lecture 14: Remaining challenges 8

Can we reach these gradients in multicellcavities? Are there better geometries?

� Eacc = 59 MV/m corresponds to Epk = 125 MV/m and Hpk = 2065 Oe at 2 K

Page 9: Superconducting RF for storage rings, ERLs, and linac-based FELs … · 2017. 2. 22. · June 26, 2009 USPAS 2009, S. Belomestnykh, Lecture 14: Remaining challenges 2 Short list of

June 26, 2009 USPAS 2009, S. Belomestnykh, Lecture 14: Remaining challenges 9

Can we develop better (cheaper) fabrication techniques?

� Can we prove that this techniques produce cavities with good performance?

� Are they cheaper for mass-production?

� Are there other (better) techniques?

9-cell cavity welded from three 3-cell

hydroformed sections

Spinning an entire cavity from a tube

Page 10: Superconducting RF for storage rings, ERLs, and linac-based FELs … · 2017. 2. 22. · June 26, 2009 USPAS 2009, S. Belomestnykh, Lecture 14: Remaining challenges 2 Short list of

June 26, 2009 USPAS 2009, S. Belomestnykh, Lecture 14: Remaining challenges 10

Other SRF technology challenges

►Thin film technology & surface studies.

►Cavity treatment: new acid mixtures w/o HF?

►Input couplers for high average power.

►Alternative materials and coatings for RF windows.

►HOM couplers and new absorbing materials.

Page 11: Superconducting RF for storage rings, ERLs, and linac-based FELs … · 2017. 2. 22. · June 26, 2009 USPAS 2009, S. Belomestnykh, Lecture 14: Remaining challenges 2 Short list of

June 26, 2009 USPAS 2009, S. Belomestnykh, Lecture 14: Remaining challenges 11

SRF guns

LASER

NC Cs2Tephoto cathode

Heliumport

SC Nb3½ -cell cavity

e-

Liquid HeVessel

Cathode cooling (77 K)& support system

Photo cathodealignmentCavity

tuners

RF powercoupler

ELBE SRF Gun Cryomodule

Page 12: Superconducting RF for storage rings, ERLs, and linac-based FELs … · 2017. 2. 22. · June 26, 2009 USPAS 2009, S. Belomestnykh, Lecture 14: Remaining challenges 2 Short list of

June 26, 2009 USPAS 2009, S. Belomestnykh, Lecture 14: Remaining challenges 12

SRF: hard work and a lot of fun

Page 13: Superconducting RF for storage rings, ERLs, and linac-based FELs … · 2017. 2. 22. · June 26, 2009 USPAS 2009, S. Belomestnykh, Lecture 14: Remaining challenges 2 Short list of

June 26, 2009 USPAS 2009, S. Belomestnykh, Lecture 14: Remaining challenges 13

SRF around the world

CLS

CESR-CHESS

NSLS-II

DIAMOND

SOLEILSLS

ELETTRABEPC-II

SSRF TLS/TPS

Superconducting RF in StorageSuperconducting RF in Storage--RingRing--Based Light Sources Based Light Sources

Page 14: Superconducting RF for storage rings, ERLs, and linac-based FELs … · 2017. 2. 22. · June 26, 2009 USPAS 2009, S. Belomestnykh, Lecture 14: Remaining challenges 2 Short list of

June 26, 2009 USPAS 2009, S. Belomestnykh, Lecture 14: Remaining challenges 14

SRF2009 conference

SRF 2009 conference

held at Helmholtz-ZentrumBerlin (formerly BESSY)

Sept 20th – 25th

Tutorials at FZ-DresdenSept 17th – 19th

srf2009.helmholtz-berlin.de

Page 15: Superconducting RF for storage rings, ERLs, and linac-based FELs … · 2017. 2. 22. · June 26, 2009 USPAS 2009, S. Belomestnykh, Lecture 14: Remaining challenges 2 Short list of

June 26, 2009 USPAS 2009, S. Belomestnykh, Lecture 14: Remaining challenges 15

Concluding remarks

� The field of RF superconductivity is very active.

� The technology is mature and became the

technology of choice for many accelerator types.

� BUT: there are still many problems that need

attention and careful investigation.

� This will require better understanding of

fundamentals and technological advances.

� The design process will never be reduced to just

a few simple rules or recipes.

� There will always be ample opportunities for

imagination, originality, and common sense.

Page 16: Superconducting RF for storage rings, ERLs, and linac-based FELs … · 2017. 2. 22. · June 26, 2009 USPAS 2009, S. Belomestnykh, Lecture 14: Remaining challenges 2 Short list of

June 26, 2009 USPAS 2009, S. Belomestnykh, Lecture 14: Remaining challenges 16

See you next time at a conference or a workshop related to RF superconductivity!