~1m undulator IP Pol. e + source based on Compton scattering with FEL & 4 mirror cavity Low energy electron beam Gamma-ray FEL photon beam LCWS2014 in.

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~1m undulator IP Pol. e + source based on Compton scattering with FEL & 4 mirror cavity Low energy electron beam Gamma-ray FEL photon beam LCWS2014 in Belgrade, 8 Oct KEK, Junji Urakawa and TPU, Alexander Potylitsyn Super conducting electron linear accelerator Energy range from 0.8 to 4.33 GeV Super conducting electron linear accelerator for FEL We assume super radiant mode to generate photon beam. Energy range from 31 to 200 MeV We survey the possibility of ILC positron source based on inverse Compton scattering with super conducting linear accelerator including advanced technologies which will be confirmed within 3 or 4 years. Consider LCLS-II and recent EUV project.

2 FEL photon beam ~2m undulator Low energy electron beam Gamma-ray IP Wavelength [um]12 Both beam size in sigma at IP [um]1016 Enhancement factor FEL electron beam energy [MeV]5030 High energy electron beam energy [GeV] Energy of Fundamental Compton Edge [MeV]36 Collimated Gamma yield on target [x 10 7 ] Super conducting electron linear accelerator Energy range from 1.4 to 1.96 GeV (2.3MW or 3.1MW beam) Super conducting electron linear accelerator for FEL We assume super radiant mode to generate photon beam. Energy range from 30 to 50 MeV (473kW or 788kW beam)

3 “Pol. Positron source based on inverse Compton scattering with super-radiant FEL and 4 mirror optical cavity” We assume 50mA 5Hz-63msec super-conducting linear accelerator to generate high intensity FEL photon beam and gamma-ray based on inverse Compton scattering. I am also assuming 100% beam injection efficiency to accumulate positron beam into 5GeV damping ring. 63msec and 5Hz super-conducting linear accelerator has 162.5MHz bunch repetition rate which means 63 x 162.5k bunches with bunch spacing 6.15nsec per beam pulse. So, we will accelerate 307.5pC/bunch with 6.15ns bunch spacing to generate the gamma-ray beam and to stack positron beam 7802 times for each bunch into the 5GeV damping ring. The conversion efficiency from gamma-ray to accumulated positron is assumed to be 10%. Necessary yield of the gamma-ray from single Compton collision is 3.7 x 10 7 gamma-ray. Wavelength [um] 12 Laser pulse energy from ~2.0m wiggler [mJ] FEL efficiency from beam energy to photon energy, k eff [%] FEL photon number per bunch [ x ] Resulting photon number per pulse (with taking into account the enhancement factor) [ x ] Pulse energy in the cavity [J] Stored laser average power [MW] 6166 Rayleigh length [mm] Number of Pol. Positron/bunch in DR [x ]

4 What is super radiant mode? Ideal micro-bunch train with same micro-bunch spacing as main radiation wavelength can radiate coherently,which is narrow bandwidth radiation. We are seriously considering the generation of micro-bunch train in single RF acceleration period, say in 10ps. How to generate it and keep time structure of such micro-bunch train during acceleration? Use fs laser (Ti-Sa laser) and photo-cathode gun or phase rotation from transverse to longitudinal direction. Micro-bunch spacing : 500fs 25pC/micro-bunch at cathode

5 Simulation result by ASTRA with 1.6 cell photo-cathode RF gun

6 One example of measurement result using zero cross acceleration technique to convert time structure to energy. Generation of two micro-bunch train was confirmed using Ti-Sa laser and photo-cathode RF gun. 4 micro-bunch train generation is not difficult. We will generate THz and confirm the super radiation using appropriate Smith-Purcell gratings. Next step; we will install 30cm wiggler to confirm the super radiation also.

7 For shorter wavelength radiation, we use phase-space rotation. I copy parts of the slide from M. Kuriki’s talk at PFWS 2013.

8 Simulation result from Kuriki’s slide. We have to demonstrate this method using existing accelerator in the range from 150  m to 1  m as wavelength. For more shorter wavelength, Grave of MIT gave an idea and the simulation results in Precise beam instrumentation and new cathode idea are necessary for this study.

9 Bunch repetition rate is 162.5MHz and 1312 bunches are needed in 3238 m damping ring. In the damping ring, we can expect the stacking by factor 7802 based on top-up injection using non-linear kicker or very fast kicker. If we assume 10% conversion efficiency from gamma-ray to positron and 100% positron injection efficiency into the damping ring, 3.0 x positron/bunch is obtainable during 63msec every 5Hz. In this case single FEL target system is enough in order to obtain ILC pol. positron beam in the damping ring. Wavelength [um] 12 Rayleigh length [mm] Pulse energy in the cavity [J] Stored laser average power [MW] 6166 No. of Gamma photons on rotating target per beam pulse in the period of 63ms [x ] No. of generated Pol. positron just after the target in the period of 63ms [x ] Number of Pol. Positron/bunch in DR [x ] Bunch charge is 307.5pC/bunch. Pre-Summary: 50mA beam acceleration and 63msec RF source are relatively difficult at present. However, ERL should be establish following technologies: 100mA, CW operation with 15MV/m accelerating gradient in the future. ILC target problem requests longer gamma-ray pulse and 63msec for the generation of gamma-ray is attractive, so we are considering 15MV/m acceleration gradient operation with 63msec RF pulse length. Therefore, precise FEL radiation evaluation is necessary including the effect of super-radiation with normalized emittance 1  rad.

10 Cooling system for cryogenic undulator should be applied to optical cavity because heating due to circulating laser power is very high. Concept of new scheme 1.5Hz long electron pulse acceleration technology using super conducting linear accelerator like ILC and ERL. 2. Positron beam stacking into main damping ring within 63msec period. 3. FEL coherent radiation photons are coherently accumulated in 4 mirror planar optical cavity. 4. High energy gamma-ray is generated based on inverse Compton scattering with 5Hz super conducting linear accelerator. 5. Efficiency of positron injection into damping ring is 100% using fast kicker into longitudinal & transverse phase space. From IPAC14 I thought 148k Cryogenic undulator was good candidate for FEL because of cooling ability. The period of permanent magnet at 148k will be 5cm with gap more than 2cm and we can reduce the beam energy, also we can increase the stored energy in the optical cavity using 148k cooling system.

11 Ceramic tube for High voltage isolation cathode anode 500kV-DC Gun 500kV high voltage electron gun technology From Negative Electron Affinity (NEA)-GaAs Photocathode to Multi- Alkali photocathode Development From DC gun to Cryogenic RF gun Development Reason: to long lifetime and Compact Compact semi-conductor amplifier is commercial available.. 4K 325MHz super Conducting Spoke cavity 500keV-1.8mA Beam generation Time (min) current (mA) Time (min) current (mA) Pressure (Pa) High Voltage (kV) Radiation (cps)

12 JAEA almost established the specification which we requested. Laser system will be installed in this year at KEK-cERL. Total system will be tested in this year. X-ray generation will start on March 2015.

13 Compact X-ray Source (Peak Brightness ) ~keV-100keV tunable X-ray generation ICS (Inverse Compton Scattering) Optical cavity for pulse laser accumulation, collision point Super conducting cavity cERL ~35MeV Application of X-ray: Imaging etc. Development of Basic Technologies 1. Multi-alkali photocathode for high average current 2. 20k Cryogenic rf-gun 3. ERL ~1MW electron beam 4. ~1MW high-average power laser 5. ~10  m precise collision technique 6. X-ray imaging 7. 4K 325MHz spoke cavity New QB Program (Fundamental Technology Development for High Brightness X-ray Source and the Imaging by Compact Accelerator under Photon and Quantum Basic Research Coordinated Development Program) 2013 – 2017 research program

14 Summary 1. The technologies for electron beam generation are almost mature mA beam acceleration is relatively challenging. (CW 1.3GHz RF source : 80kW and 300kW exist. 650MHz or 325MHz SRF technologies should be developed for future ILC beam source.) 3. Control of 4 mirror optical cavity is almost mature with enhancement of ~ Stable collision is almost OK with timing accuracy of 1psec. 5. Generation of micro-bunch train with wavelength 2  m as micro-bunch spacing which is corresponding 6.64fs. It is relatively challenging. 6. Problem which should be solved is only heating due to power loss on mirrors. Stored laser power with about 50 times higher comparing usual case is serious problem. Hopeful solution : Cryogenic optical cavity is necessary like 148k Cryogenic permanent magnet undulators. There are many interesting and bright research items for many young researchers.

15 X-ray Lasers Synchrotron Radiation X-ray Tubes Relativity Coherent Emission ICS Super-radiant ICS Key-tech. for stimulated and super radiation Efficient pre-bunched FEL and micro-bunch train generation Energy or velocity modulation to make intensity modulation by laser field or intensity modulation by other tech.. and coherent radiation 2D 4-mirror optical cavity ~2m Thank you for your attention! Copy of presentation by W.S. Graves, MIT, March, 2012 Presented at the ICFA Future Light Sources Workshop

High Finesse 4 mirror optical cavity development Transmitted light Applied voltage to PZT Resonance of 0-order mode PD High Finesse cavity CW laser MirrorCo.Reflectivity(spec.) [%]Transmission(meas. ) [ppm] M1(flat)REO ±7 M2(flat)LMA ±3 M3(concave)LMA ±3 M4(concave)LMA ±3 M1 M2 M3 M4

Evaluation of high finesse cavity Transmitted light Applied voltage to PZT Finesse ∝ lifetime of photon in the cavity 200us attenuation rate within one turn in the optical cavity:140ppm =transmission of 4 mirrors(100ppm)+scattering rate + absorption rate ⇒ total scattering of 4 mirrors + total absorption =40ppm Old optical cavity had 600ppm ↔ new optical cavity has 40ppm

18 Nitrogen doping

19 Nb 3 Sn SRF possibility To higher gradient (100MV/m?)