J. Hansen’s research while affiliated with CERN and other places

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Publications (37)


Figure 4: Schematic of the spectrometer vacuum chamber. Electrons enter from the left hand side and are spread out by the magnetic field of the magnet. The vacuum window comprises the upper right side of the triangular chamber and the scintillator is fixed to its exterior surface. The high energy protons propagate through the chamber and exit through the beam pipe on the right hand side, continuing to a beam dump.
A magnetic spectrometer to measure electron bunches accelerated at AWAKE
  • Preprint
  • File available

February 2019

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95 Reads

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11 Citations

Nuclear Instruments and Methods in Physics Research Section A Accelerators Spectrometers Detectors and Associated Equipment

J. Bauche

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M. Wing

A magnetic spectrometer has been developed for the AWAKE experiment at CERN in order to measure the energy distribution of bunches of electrons accelerated in wakefields generated by proton bunches in plasma. AWAKE is a proof-of-principle experiment for proton-driven plasma wakefield acceleration, using proton bunches from the SPS. Electron bunches are accelerated to O\mathcal{O}(1 GeV) in a rubidium plasma cell and then separated from the proton bunches via a dipole magnet. The dipole magnet also induces an energy-dependent spatial horizontal spread on the electron bunch which then impacts on a scintillator screen. The scintillation photons emitted are transported via three highly-reflective mirrors to an intensified CCD camera, housed in a dark room, which passes the images to the CERN controls system for storage and further analysis. Given the known magnetic field and determination of the efficiencies of the system, the spatial spread of the scintillation photons can be converted to an electron energy distribution. A lamp attached on a rail in front of the scintillator is used to calibrate the optical system, with calibration of the scintillator screen's response to electrons carried out at the CLEAR facility at CERN. In this article, the design of the AWAKE spectrometer is presented, along with the calibrations carried out and expected performance such that the energy distribution of accelerated electrons can be measured.

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FIG. 1. (a) Schematic location of the imaging stations (IS1 and IS2) and of the OTR streak camera screen with respect to the plasma. The proton bunch moves from left to right. (b) Schematic drawing of the optical setup of the imaging stations.
FIG. 2. Streak camera image showing the transverse distribution of the self-modulated proton bunch as a function of time. The image is obtained by summing ten individual measurements. The bunch moves down along the time axis. The timescale is set to show only 34 ps of the ∼73 ps image. The white line indicates the observed increase of the maximum defocusing of the protons along the bunch.
Experimental Observation of Plasma Wakefield Growth Driven by the Seeded Self-Modulation of a Proton Bunch

February 2019

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369 Reads

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83 Citations

Physical Review Letters

We measure the effects of transverse wakefields driven by a relativistic proton bunch in plasma with densities of 2.1×1014 and 7.7×1014 electrons/cm3. We show that these wakefields periodically defocus the proton bunch itself, consistently with the development of the seeded self-modulation process. We show that the defocusing increases both along the bunch and along the plasma by using time resolved and time-integrated measurements of the proton bunch transverse distribution. We evaluate the transverse wakefield amplitudes and show that they exceed their seed value (<15 MV/m) and reach over 300 MV/m. All these results confirm the development of the seeded self-modulation process, a necessary condition for external injection of low energy and acceleration of electrons to multi-GeV energy levels.


FIG. 2. (a) Streak camera image of the proton bunch without plasma. The bunch is on the right hand side of the image and the short laser pulse on the left hand side (see text). The green temporal profile is fitted with a Gaussian function (dotted black line, σ t ¼ 437 ps, 1.5 × 10 11 protons). The laser timing is marked by the red line (t ¼ 0). (b) Image with plasma (n Rb ¼ 2.092 × 10 14 cm −3 , 3 × 10 11 protons) and ionizing laser pulse (blocked, not visible) placed as in (a). The effect of the plasma (t > 0) is visible in the image and on the bunch profile (green line). (c) Image as in (b), but with n Rb ¼ 2.558 × 10 14 cm −3 and the ionizing laser pulse in the front of the bunch at −390 ps. The SSM effect and streak camera setting are such that the bunch charge behind the laser pulse is not visible. The spatial dimension displayed is that at the OTR wafer.
FIG. 3. Streak camera images on the fast (73 ps) timescale (a) at low (n Rb ¼ 2.457 × 10 14 cm −3 ) and (c) at high (n Rb ¼ 6.994 × 10 14 cm −3 ) plasma densities. Profiles obtained by summing the images along the spatial axis from −0.4 to 0.6 mm are displayed on the left-hand side of each image. The profile of image (a) shows the defocusing effect of SSM starting at the laser pulse time (∼10 ps). Image (c) is obtained ∼10 ps behind the ionizing laser pulse that is placed in the middle of the bunch as in Fig. 2. It is also obtained with a narrower band-pass filter (25 nm) than for image (a) and (e) (50 nm) to reduce the intensity of the light and decrease time resolution limitations originating from a broad OTR spectrum reaching the streak photocathode [26]. Figures (b) and (d) show the DFT power spectrum for the two profiles (black diamonds, no padding) as well as for background images (orange lines). The green lines depict the interpolated power spectrum (with padding). The blue lines show a noise threshold used for automatically detecting frequencies. Image (e) shows a low density case (n Rb ¼ 2.190 × 10 14 cm −3 ) where the full train of microbunches is shown. The Rubidium (and thus plasma) density for image (e) has an upwards density gradient of 3.4%=10 m.
Experimental Observation of Proton Bunch Modulation in a Plasma at Varying Plasma Densities

February 2019

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441 Reads

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87 Citations

Physical Review Letters

We give direct experimental evidence for the observation of the full transverse self-modulation of a long, relativistic proton bunch propagating through a dense plasma. The bunch exits the plasma with a periodic density modulation resulting from radial wakefield effects. We show that the modulation is seeded by a relativistic ionization front created using an intense laser pulse copropagating with the proton bunch. The modulation extends over the length of the proton bunch following the seed point. By varying the plasma density over one order of magnitude, we show that the modulation frequency scales with the expected dependence on the plasma density, i.e., it is equal to the plasma frequency, as expected from theory.


Generation and delivery of an ultraviolet laser beam for the RF-photoinjector of the AWAKE electron beam

January 2019

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25 Reads

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5 Citations

In the AWAKE experiment, the electron beam is used to probe the proton-driven wakefield acceleration in plasma. Electron bunches are produced using an RF-gun equipped with a Cs2Te photocathode illuminated by an ultraviolet (UV) laser pulse. To generate the UV laser beam a fraction of the infrared (IR) laser beam used for production of rubidium plasma is extracted from the laser system, time-compressed to a picosecond scale and frequency tripled using nonlinear crystals. The optical line for transporting the laser beam over the 24 m distance was built using rigid supports for mirrors and air-evacuated tube to minimize beam-pointing instabilities. Construction of the UV beam optical system enables appropriate beam shaping and control of its size and position on the cathode, as well as time delay with respect to the IR pulse seeding the plasma wakefield.


Experimental observation of proton bunch modulation in a plasma, at varying plasma densities

September 2018

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167 Reads

We give direct experimental evidence for the observation of the full transverse self-modulation of a relativistic proton bunch propagating through a dense plasma. The bunch exits the plasma with a density modulation resulting from radial wakefield effects with a period reciprocal to the plasma frequency. We show that the modulation is seeded by using an intense laser pulse co-propagating with the proton bunch which creates a relativistic ionization front within the bunch. We show by varying the plasma density over one order of magnitude that the modulation period scales with the expected dependence on the plasma density.


Layout of the AWAKE experiment
The proton bunch and laser pulse propagate from left to right across the image, through a 10-m column of rubidium (Rb) vapour. This laser pulse (green, bottom images) singly ionizes the rubidium to form a plasma (yellow), which then interacts with the proton bunch (red, bottom left image). This interaction modulates the long proton bunch into a series of microbunches (bottom right image), which drive a strong wakefield in the plasma. These microbunches are millimetre-scale in the longitudinal direction (ξ) and submillimetre-scale in the transverse (x) direction. The self-modulation of the proton bunch is measured in imaging stations 1 and 2 and the optical and coherent transition radiation (OTR, CTR) diagnostics. The rubidium (pink) is supplied by two flasks at each end of the vapour source. The density is controlled by changing the temperature in these flasks and a gradient may be introduced by changing their relative temperature. Electrons (blue), generated using a radio-frequency source, propagate a short distance behind the laser pulse and are injected into the wakefield by crossing at an angle. Some of these electrons are captured in the wakefield and accelerated to high energies. The accelerated electron bunches are focused and separated from the protons by the quadrupoles and dipole magnet of the spectrometer (grey, right). These electrons interact with a scintillating screen, creating a bright intensity spot (top right image), allowing them to be imaged and their energy inferred from their position.
Signal of accelerated electrons
a, An image of the scintillator (with horizontal distance x and vertical distance y) with background subtraction and geometric corrections applied is shown, with an electron signal clearly visible. The intensity of the image is given in charge Q per unit area (d²Q/dxdy), calculated using the central value from the calibration of the scintillator. b, A projection of the image in a is obtained by integrating vertically over the charge observed in the central region of the image. A 1σ uncertainty band from the background subtraction is shown in orange around zero. Both the image (a) and the projection (b) are binned in space, as shown on the top axis, but the central value from the position–energy conversion is indicated at various points on the bottom axis. The electron signal is clearly visible above the noise, with a peak intensity at an energy of E ≈ 800 MeV.
Background-subtracted projections of consecutive electron-injection events
Each projection (event) is a vertical integration over the central region of a background-subtracted spectrometer camera image. Brighter colours indicate regions of high charge density dQ/dx, corresponding to accelerated electrons. The quadrupoles of the spectrometer were varied to focus at energies of 460–620 MeV over the duration of the dataset. No other parameters were varied deliberately. The consistent peak around energy E ≈ 600 MeV demonstrates the stability and reliability of the electron acceleration.
Measurement of the highest peak energies μE achieved at different plasma densities npe, with and without a gradient in the plasma density
The error bars arise from the position–energy conversion. The gradients chosen are those that were observed to maximize the energy gain. Acceleration to 2.0 ± 0.1 GeV is achieved with a plasma density of 6.6 × 10¹⁴ cm⁻³ with a density difference of +2.2% ± 0.1% over 10 m.
Acceleration of electrons in the plasma wakefield of a proton bunch

August 2018

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619 Reads

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265 Citations

Nature

High-energy particle accelerators have been crucial in providing a deeper understanding of fundamental particles and the forces that govern their interactions. To increase the energy of the particles or to reduce the size of the accelerator, new acceleration schemes need to be developed. Plasma wakefield acceleration1–5, in which the electrons in a plasma are excited, leading to strong electric fields (so called ‘wakefields’), is one such promising acceleration technique. Experiments have shown that an intense laser pulse6–9 or electron bunch10,11 traversing a plasma can drive electric fields of tens of gigavolts per metre and above—well beyond those achieved in conventional radio-frequency accelerators (about 0.1 gigavolt per metre). However, the low stored energy of laser pulses and electron bunches means that multiple acceleration stages are needed to reach very high particle energies5,12. The use of proton bunches is compelling because they have the potential to drive wakefields and to accelerate electrons to high energy in a single acceleration stage¹³. Long, thin proton bunches can be used because they undergo a process called self-modulation14–16, a particle–plasma interaction that splits the bunch longitudinally into a series of high-density microbunches, which then act resonantly to create large wakefields. The Advanced Wakefield (AWAKE) experiment at CERN17–19 uses high-intensity proton bunches—in which each proton has an energy of 400 gigaelectronvolts, resulting in a total bunch energy of 19 kilojoules—to drive a wakefield in a ten-metre-long plasma. Electron bunches are then injected into this wakefield. Here we present measurements of electrons accelerated up to two gigaelectronvolts at the AWAKE experiment, in a demonstration of proton-driven plasma wakefield acceleration. Measurements were conducted under various plasma conditions and the acceleration was found to be consistent and reliable. The potential for this scheme to produce very high-energy electron bunches in a single accelerating stage²⁰ means that our results are an important step towards the development of future high-energy particle accelerators21,22.


FIG. 1. The layout of the AWAKE experiment. The proton bunch and laser pulse propagate from left to right across the image, through a 10 m column of rubidium vapour. This laser pulse (green, bottom images) singly ionises the rubidium (Rb) to form a plasma (yellow) which then interacts with the proton bunch (red, bottom left image). This interaction modulates the long proton bunch into a series of microbunches (bottom right image) which drive a strong wakefield in the plasma. The self-modulation of the proton bunch is measured in imaging stations 1 and 2 and the optical and coherent transition radiation (OTR, CTR) diagnostics. The rubidium is supplied by two flasks (pink) at each end of the vapour source. The density is controlled by changing the temperature in these flasks and a gradient may be introduced by changing their relative temperature. Electrons (blue), generated using a radio frequency (RF) source, propagate a short distance behind the laser pulse and are injected into the wakefield by crossing at an angle. Some of these electrons are captured in the wakefield and accelerated to high energies. The accelerated electron bunches are focused and separated from the protons by the spectrometer's quadrupoles and dipole magnet (grey, right). These electrons interact with a scintillating screen (top right image), allowing them to be imaged and their energy inferred from their position.
FIG. 2. Signal of accelerated electrons. An image of the scintillator (horizontal distance, x, and vertical distance, y) with an electron signal clearly visible (top) and a vertical integration over the observed charge in the central region of the image (bottom), with background subtraction and geometric corrections applied, is shown. The intensity of the image is given in charge, Q, per unit area, calculated using the central value from the calibration of the scintillator. A 1 ? uncertainty band from the background subtraction is shown in orange around zero on the bottom plot. Both the image and the projection are binned in space, as shown on the top axis, but the central value from the position-energy conversion is indicated at various points on the bottom axis. The electron signal is clearly visible above the noise, with a peak intensity at energy, E ? 800 MeV.
Acceleration of electrons in the plasma wakefield of a proton bunch

August 2018

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279 Reads

High energy particle accelerators have been crucial in providing a deeper understanding of fundamental particles and the forces that govern their interactions. In order to increase the energy or reduce the size of the accelerator, new acceleration schemes need to be developed. Plasma wakefield acceleration, in which the electrons in a plasma are excited, leading to strong electric fields, is one such promising novel acceleration technique. Pioneering experiments have shown that an intense laser pulse or electron bunch traversing a plasma, drives electric fields of 10s GV/m and above. These values are well beyond those achieved in conventional RF accelerators which are limited to ~0.1 GV/m. A limitation of laser pulses and electron bunches is their low stored energy, which motivates the use of multiple stages to reach very high energies. The use of proton bunches is compelling, as they have the potential to drive wakefields and accelerate electrons to high energy in a single accelerating stage. The long proton bunches currently available can be used, as they undergo self-modulation, a particle-plasma interaction which longitudinally splits the bunch into a series of high density microbunches, which then act resonantly to create large wakefields. The AWAKE experiment at CERN uses intense bunches of protons, each of energy 400 GeV, with a total bunch energy of 19 kJ, to drive a wakefield in a 10 m long plasma. Bunches of electrons are injected into the wakefield formed by the proton microbunches. This paper presents measurements of electrons accelerated up to 2 GeV at AWAKE. This constitutes the first demonstration of proton-driven plasma wakefield acceleration. The potential for this scheme to produce very high energy electron bunches in a single accelerating stage means that the results shown here are a significant step towards the development of future high energy particle accelerators.


Table 1 : Awake electron beam parameters for the RUN1 and RUN2 of the AWAKE experiment
Figure 2: Spectrometer and light path layout to measure the plasma wake-field accelerated electrons. 
The electron accelerators for the AWAKE experiment at CERN-Baseline and Future Developments

February 2018

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355 Reads

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29 Citations

Nuclear Instruments and Methods in Physics Research Section A Accelerators Spectrometers Detectors and Associated Equipment

The AWAKE collaboration prepares a proton driven plasma wakefield acceleration experiment using the SPS beam at CERN. A long proton bunch extracted from the SPS interacts with a high power laser and a 10 m long rubidium vapor plasma cell to create strong wakefields allowing sustained electron acceleration. The electron beam to probe these wakefields is created by an electron accelerator consisting of an rf-gun and a booster structure. This electron source should provide beams with intensities between 0.1 and 1 nC, bunch lengths between 0.3 and 3 ps and an emittance of the order of 2 mm mrad. The booster structure should accelerate the electrons to 16 MeV. The electron line includes a series of diagnostics (pepper-pot, BPMs, spectrometer, Faraday cup and screens) and an optical transfer line merges the electron beam with the proton beam on the same axis. The installation of the electron line started in early 2017 and the commissioning will take place at the end of 2017. The first phase of operation is called RUN1. After the long shutdown of LHC a second phase for AWAKE is planned starting 2021 called RUN2. In this phase the aim is to demonstrate the acceleration of high quality electron beams therefore a bunch length of the order of 100 fs rms is required corresponding to a fraction of the plasma wavelength. The AWAKE collaboration is studying the design of such an injector either based on classical rf-gun injectors or on laser wake-field acceleration. The focus for the RF accelerator is on a hybrid design using an S-band rf-gun and x-band bunching and acceleration cavities. The layout of the current and the future electron accelerator and transfer line, including the diagnostics will be presented.


AWAKE readiness for the study of the seeded self-modulation of a 400GeV proton bunch

November 2017

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158 Reads

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2 Citations

AWAKE is a proton-driven plasma wakefield acceleration experiment. We show that the experimental setup briefly described here is ready for systematic study of the seeded self-modulation of the 400 GeV proton bunch in the 10 m long rubidium plasma with density adjustable from 1 to 10×101410\times {10}^{14} cm−3. We show that the short laser pulse used for ionization of the rubidium vapor propagates all the way along the column, suggesting full ionization of the vapor. We show that ionization occurs along the proton bunch, at the laser time and that the plasma that follows affects the proton bunch.


CERN’s Linac4 cesiated surface H− source

August 2017

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352 Reads

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11 Citations

AIP Conference Proceedings

Linac4 cesiated surface H⁻ sources are routinely operated for the commissioning of the CERN’s Linac4 and on an ion source test stand. Stable current of 40-50 mA are achieved but the transmission through the LEBT of 80% was below expectations and triggered additional beam simulation and characterization. The H⁻ beam profile is not Gaussian and emittance measurements are larger than simulation. The status of ongoing development work is described; 36 mA H⁻ and 20 mA D⁻ beams were produced with a 5.5 mm aperture cesiated surface ion source. The emittances measured at the test stand are presented. During a preliminary test, the Linac4 proton source delivered a total beam intensity of 70 mA (p, H2⁺, H3⁺).


Citations (32)


... In that matter, Radiofrequency (RF) photoinjectors have become the workhorse when low emittance and high peak current are required. Some of these applications at CERN include the production of witness electron bunches for plasma wake field acceleration in 10 m plasma columns [1,2,3], or irradiation experiments at GHz repetition rates in the CLEAR facility [4,5]. Beyond CERN, free electron lasers (FEL), electron diffraction microscopy, or high photon energy sources in the X-ray and γ-ray regimes [6], are examples of machines that require ultrafast and well synchronized high peak current electron bunches. ...

Reference:

Copper Surface Treatment with deep UV Ultrafast Laser for Improved Photocathode Photoemissive Properties
Generation and delivery of an ultraviolet laser beam for the RF-photoinjector of the AWAKE electron beam
  • Citing Conference Paper
  • January 2019

... The resulting time-resolved images are used for studying a variety of features of the modulation of the proton bunch in the plasma [1,[12][13][14][15]. An important component of the setup is a high-power laser [16]. This laser produces a high-intensity pulse that ionizes a 10-m-long column of Rb vapor, generating the plasma, -1 -and a timing reference signal that is sent to the streak camera. ...

Integration of a terawatt laser at the CERN SPS beam for the AWAKE experiment on proton-driven plasma wake acceleration
  • Citing Conference Paper
  • January 2016

... The delay t seed between the e − and the p þ bunch centers can be adjusted using a delay stage. We use a magnetic spectrometer [33] to measure the FIG. 1. Schematic of the experimental setup: the ionizing laser pulse enters the vapor source t p ahead of the p þ bunch center and ionizes the rubidium atoms, creating the plasma. The seed e − bunch follows, t seed ahead of the p þ bunch. ...

A magnetic spectrometer to measure electron bunches accelerated at AWAKE

Nuclear Instruments and Methods in Physics Research Section A Accelerators Spectrometers Detectors and Associated Equipment

... 11,12,[40][41][42]50 Nevertheless, at short interaction distances, uniform plasmas can demonstrate high acceleration rates and serve as a proof of the self-modulation concept. 20,51,52 While perspective applications of multi-bunch wakefield excitation require as stable bunches as possible, 11,13,53 near-future experiments 11 may have a different target function and aim to obtain the highest witness energy within a limited acceleration distance. In this paper, we show that if the acceleration distance is limited and much shorter than the beam dephasing length, the witness energy gain can be increased with a negative gradient of the plasma density. ...

Experimental Observation of Plasma Wakefield Growth Driven by the Seeded Self-Modulation of a Proton Bunch

Physical Review Letters

... 11,12,[40][41][42]50 Nevertheless, at short interaction distances, uniform plasmas can demonstrate high acceleration rates and serve as a proof of the self-modulation concept. 20,51,52 While perspective applications of multi-bunch wakefield excitation require as stable bunches as possible, 11,13,53 near-future experiments 11 may have a different target function and aim to obtain the highest witness energy within a limited acceleration distance. In this paper, we show that if the acceleration distance is limited and much shorter than the beam dephasing length, the witness energy gain can be increased with a negative gradient of the plasma density. ...

Experimental Observation of Proton Bunch Modulation in a Plasma at Varying Plasma Densities

Physical Review Letters

... [15][16][17] Therefore, it is more practical to convert a proton beam into a bunch train either in the plasma 9 or before entering the plasma. 18 Wave excitation by trains of particle bunches has been and is being studied in the AWAKE experiment 11,[19][20][21] at CERN and in several experiments with electron beams around the world. [22][23][24][25][26][27][28][29] The measurements are in good agreement with numerical simulations, 30-33 despite the fact that multi-bunch drivers are far away from other plasma wakefield accelerators in parameter space. ...

Acceleration of electrons in the plasma wakefield of a proton bunch

Nature

... The laser pulse propagates 620 ps (∼2.8σ t ) ahead of the proton bunch longitudinal center and is aligned on its axis; thus, it does not seed SM [23] or induce hosing. A 18.9 MeV, ∼225 pC, ∼4 ps-long electron bunch [31,32] placed 600 ps ahead of the proton bunch center, i.e., in plasma, 20 ps behind the laser pulse, drives seed wakefields. ...

The electron accelerators for the AWAKE experiment at CERN-Baseline and Future Developments

Nuclear Instruments and Methods in Physics Research Section A Accelerators Spectrometers Detectors and Associated Equipment

... Fabrication of the five Spiral2 1-meter modules is close to completion, with tuning operations starting in 2014 Q3. Linac4 RFQ is now operational [2], while ESS RFQ [3] is still under development. 60 0 0 2 0 62 Specified resonance frequencies and inter-vane voltage functions of these RFQs are obtained via the careful adjustment of tuning devices, which may be slugs, thickness plates, rods, active RF ports or dummy RF ports, and generally a combination of these. ...

COMMISSIONING AND OPERATIONAL EXPERIENCE GAINED WITH THE LINAC4 RFQ AT CERN

... The 3D Particle-in-cell (PIC) Monte Carlo (MC) code ONIX (Orsay Negative Ion eXtraction [1]), written to study H − beam formation processes in neutral-beam injectors for fusion, has been adapted to single aperture accelerator H − sources. The code was modified to match the conditions of the beam formation and extraction regions of the Linac4 H − source [2]. A set of parameters was chosen to characterize the plasma and to match the specific volume and surface production modes. ...

CERN’s Linac4 cesiated surface H− source

AIP Conference Proceedings

... Plasma acceleration occurs in an electron density wave generated by an intense laser pulse [7] or by a charged particle bunch [8] and can potentially sustain electric fields 1000 times larger than conventional radio frequency particle acceleration cavities [7]. The Advanced Proton Driven Plasma Wakefield Acceleration Experiment (AWAKE) [6], [9] uses proton bunches to generate a wakefield able to accelerate electrons with an energy gain of up to 0.2 GeV/m [10]. ...

AWAKE readiness for the study of the seeded self-modulation of a 400\,GeV proton bunch