Bunch compression at the SPring-8 linac for successive generation - - PowerPoint PPT Presentation

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Bunch compression at the SPring-8 linac for successive generation - - PowerPoint PPT Presentation

Bunch compression at the SPring-8 linac for successive generation of THz pulse train in the isochronous ring T. Asaka, H. Hanaki, Y. Shoji, H. Dewa, T. Kobayashi, T. Matsubara, A. Mizuno, T. Taniuchi, Y. Hisaoka, S. Suzuki, H. Tomizawa,


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SLIDE 1

Bunch compression at the SPring-8 linac for successive generation of THz pulse train in the isochronous ring

  • T. Asaka, H. Hanaki,
  • H. Dewa, T. Kobayashi,
  • A. Mizuno, T. Taniuchi,
  • S. Suzuki, H. Tomizawa,
  • K. Yanagida

SPring-8, JASRI

  • Y. Shoji,
  • T. Matsubara,
  • Y. Hisaoka,
  • T. Mitsui,

NewSUBARU, LASTI, University of Hyogo

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SLIDE 2

Contents

・ Introduction to CSR ・ Basic Idea ・ Demonstration Experiment ・ Upgrading plan

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SLIDE 3

Introduction

Applications of Short Electron Bunch ・Coheremt synchrotron radiation (CSR) ・Short Pulsed X-Ray

For time resolving experiments → Sub-ps (femto-second) pulse → Intense ps pulse is still valuable → extremely strong THz radiation → stable radiation

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SLIDE 4

z beam Bunch length

Coherent Synchrotron Radiation (CSR)

P

tot(ω) = p(ω) N +( N 2 − N ) f(ω) 2

[ ]

f(ω) = ρ(z)exp(iωz /c)dz ∫

p(ω) : power from an electron f(ω) : form factor

ρ(z)dz = 1 ∫ Form factor

( ρ(z) : charge density, )

Radiation power from N electrons in a bunch

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SLIDE 5
  • 1. Make short and intense bunch in a linac
  • 2. Let the bunch circulate in an isochronous ring
  • 3. Use short pulsed X-ray train or THz CSR

The Concept

P u l s e d X

  • r

a y t r a i n T H z C S R

N

  • s

t

  • r

a g e ! !

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SLIDE 6

Merits

(iii) Existing acceleratiors are enough for a few ps pulse.

  • -> No special expense is required

(i) Short and intense pulse is obtained at ring BL.

  • -> Light for many BLs at the same time

(ii) Short pulse train with fixed period

  • -> It helps to confirm the synchronization.
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SLIDE 7

Demonstration Experiment

1. ECS cavity --> energy gradient 2. Linac-NS BT--> magnetic compression 3. Streak camera --> measure bunch length

NewSUBARU

Linac-NS BT

Energy Compression System (ECS)

Booster synchrotron SPring-8 Linac

Electron Gun

20 40 (m)

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SLIDE 8

Simulation of bunch compression

  • 1

1 2 3 4 5

  • 5

5 10 15 20 25 20 40 60 80 100 120

Dispersion η(m) Bunch length (ps) Location in Linac-NS transport line (m) (a) normal; ∆E/E=+0.3% (b) our choice; ∆E/E=+0.5% (c) too much compression; ∆E/E=+1.2%

Magnetic compression along the Li-NS transport

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SLIDE 9

Bunch Length Measurement

10 20 30 40 50

Intensity (arb. unit) Time (ps) σ = 5.1 ps Data Gaussian fit

1σ = 5.1 ps

10 20 30 40 50 50 100 150 200 250 300

Intensity (arb. unit) Time (ps) σ = 2.2 ps Data Gaussian fit

BW < 10ps

1σ = 2.2 ps

Normal Operation Parameters ECS parameters Optimized

  • 0.4
  • 0.2

0.2 0.4

Intensity(arb. unit) ∆E/E (%)

Time profile at the initial turn in the ring

BW = 0.75%

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SLIDE 10

Multi-turn Circulation

∆L/L = α1δ + α2δ2 + α3δ3 + ...

δ = ∆E E

(here )

αn : n-th momentum compaction factor

Energy dependence of path-length NewSUBARU storage ring Invert Bend →control α1 Modified DBA BM IB ・α1 =1.3×10-3 → ≈ 0 ・α2 = 0 (setting accuracy ≈ 10-3) ・α3 no control knob (α3 ≈ 0.5 ) Modified DBA

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SLIDE 11

Tracking simulation in the non-linear rf bucket

Initial state; just after injection ∆E/E = ±0.5% ∆τ = ± 4ps

∆τ (ps) ∆E/E (%)

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SLIDE 12

Tracking simulation in the non-linear rf bucket

Initial state; just after injection ∆E/E = ±0.5% ∆τ = ± 4ps

∆τ (ps) ∆E/E (%)

α2 = 0 α3 = 0.5 α4 = -20 α1 = 0 After 100 turns α1 = -1 X10-5 After 100 turns

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SLIDE 13

Quasi-isochronous ring 50 turns with σ < 3ps

2 3 4 5 6 7 10 20 30

Turn number Time(µs)

Bunch length : σ (ps)

25 50

α 1=0 α 1=-0.02×10

  • 3

α 1=-0.06×10-3 α 1=1.3×10-3 α 1=-0.06×10-3 3 ps injection 2 ps injection

Optimum α1 was larger than the expected Bunch elongation was faster than the expected

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SLIDE 14

CSR detection

Set-up of micro-wave detector (90-140GHz)

Signal waveform

  • 0.05
  • 0.025

0.025 0.05 0.075 0.1 0.05 0.1 0.15

Voltage (V)

Time (µs)

Revolution period=0.4µs

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SLIDE 15

Turn by turn CSR power

24 pC/bunch 20 pC X 3 bunches

Stronger CSR at the injection It lasted longer than the normal condition

0.05 0.1 0.15 0.2 0.25 0.3 5 10 15 20 25 30

Power (mW)

Time from injection (µs) Turn number

25 50 75

Normal Operation Compressed, Single bunch, QI ring

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SLIDE 16

Bunch length & CSR power

24 pC/bunch 20 pC X 3 bunches

0.05 0.1 0.15 0.2 0.25 0.3 5 10 15 20 25 30

Power (mW)

Time from injection (µs) Turn number

25 50 75

Normal Operation Compressed, Single bunch, QI ring 2 3 4 5 6 7 10 20 30

Turn number Time(µs)

Bunch length : σ (ps)

25 50

α 1=0 α 1=-0.02×10

  • 3

α 1=-0.06×10-3 α 1=1.3×10-3 α 1=-0.06×10-3 3 ps injection 2 ps injection

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SLIDE 17

0.01 0.1 1 10 100 1 10

f (ω)

2

Frequency (GHz)

90GHz 140GHz 3 cm-1

Wave number (cm

  • 1)

10 20 30 40 50 10 15 20 25 30 35 Time from injection point ( µs)

Time (ps)

2.4ps (1σ) 2.3ps 2.9ps 4.1ps 5.3ps Data Gaussian fit

Reduction of CSR

Sensitive to a small change of the bunch length

Evolution of time profile after injection

Gaussian σ = 2.9ps Triangle L = 7.6ps

contribution of form factor f(ω)

1st 50th

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SLIDE 18

Summary of Experiment

Short Bunch Circulation ・succeeded to keep 1σ < 3ps for 50 turns ・larger CSR lasted longer

Of course, still there are many problems …

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SLIDE 19

Future Improvement

Ring (magnet system) ・improve stability ; temperature control ; magnetic field ; better tuning = improvements for the daily operation Linac (electron gun) ・thermionic gun --> photo-cathode RF gun

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SLIDE 20

Photo-cathode RF gun

Thermionic Gun

20 40 (m)

RF gun R&D room

Rf gun Acceleration structure

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SLIDE 21

Photo-cathode rf gun

Electron Gun Thermionic Photo-Cath Energy Spread + 0.5% + 0.1% Bunch Length 2.2 ps < 1 ps Bunch Charge < 0.1 nC > 1 nC

∆E/E (%) ∆τ (ps)

Initial state ∆E/E = ±0.5%; ∆τ = ± 2.2ps

α1 = -1.5 X10-6; after 500 turns

Initial state ∆E/E = ±0.1%; ∆τ = ± 1ps

α1 = -0.5 X10-6; after 500 turns

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SLIDE 22

~ 50 >100 ? 1 quasi-dc Pulses per shot 24 1000 ~ 10 ~ 1 charge (pC/bunch) 3 (1σ) <1.0 0.16 (1σ) 1.0 (1σ) bunch length (ps) Short Bunch Circulation (SPring-8 Linac & NewSUBARU) Demonstration Photo-cathode gun Laser Slicing (ALS) QI operation (BESSY-II) Beam Parameters

Comparison with other methods

stable short strong

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SLIDE 23

Beam physics study

  • 1. Stable operation of quasi-isochronous ring
  • 2. Circulation of an extreme beam

Similarity with ERL’s arc Problem would be enhanced with multi-turn circulation Ring parameter can be tuned using stored beam

  • 3. Future project at Tohoku Univ.

Circulation of sub-mm pulse [ H. Hama, 27th International FEL Conference (2005)].