LCLS CDR 2/17/16 9.3 Facility requirements (access, personal protection, radiation shielding and beam containment, toxic materials) 9.3.1 Requirements and calculations The radiation concerns related to the LCLS project fall into three distinct areas: • radiation safety • radiation background in experiments • machine protection In each of these areas one or more of the following radiation sources needs to be considered: 1) bremsstrahlung from beam/halo interactions with beamline components 2) gas bremsstrahlung 3) synchrotron radiation 4) neutrons 5) muons 6) induced activity 7) secondary electrons and positrons 9.3.1.1 Photons We are concerned with radiation effects in the areas downstream of the undulator, taking into account any relevant radiation source, located upstream, inside, or downstream of the undulator. Potentially all sources, 1 through 7 above, can contribute to the radiation background in experiments. Machine protection mainly concerns possible radiation damage to mirrors and collimators which will intercept the spontaneous synchrotron radiation from source number 3, accompanying the laser beam proper. The radiation safety items include shielding, beam containment system (BCS) and personnel protection system (PPS). Since the LCLS electron beam power will be comparable to that of the FFTB, the existing enclosure and dump shielding as well as PPS and BCS should be adequate without major modifications. New designs of the three safety items are only required for the optics enclosure and experimental hutch downstream of the electron beam dump, taking into account radiation sources 1 through 6. The ultimate goal is to have sufficiently accurate estimates of radiation sources 1 through 7 and their effects. Initial modeling of some of the dominant sources has been completed and the status of the calculations is summarized in the text below. More comprehensive calculations, as described below, will be continued in the future. -1- LCLS CDR 2/17/16 9.3.1.1.1 Bremsstrahlung from collimators Two copper collimators, each 10 cm long and with an internal diameter of 0.2 cm, will be placed between the dog-leg and the undulator. The purpose of the first collimator is to reduce the electron beam halo, while the second should intercept any mis-steered beam which could hit and damage the undulator. The first collimator, continuously intercepting about 1% of the beam, will be a constant source of forward-directed bremsstrahlung and muon radiation. The second one should interact with the beam only in exceptional cases and is not expected to contribute substantially to the radiation field under normal operating conditions. Bremsstrahlung radiation produced in the first collimator will hit the PPS photon stoppers which must be inserted into any beamlines when access is allowed in any downstream enclosure. Two calculations have been made with the FLUKA code [1] for the first of such photon stoppers, assumed located 20 m downstream of the undulator: electrons in the beam halo were assumed to hit the collimator on its front edge in one case, and inside the aperture in the second case. The first case was found to generate the higher energy deposition. For a 1% loss of a 14.35 GeV electron beam of 1.722 kW (1 nC/pulse at 120 pps) the calculated energy deposition rate in the stopper was less than 0.02 mW. The shielding requirements for Giant Resonance photo-neutrons generated in the stoppers located in the on-line hutches of the Near-Field Hall are being evaluated by means of the SHIELD11 code considering an equivalent electron beam depositing the same power in the stoppers. However, bremsstrahlung from collimators is neither the only nor the main source of radiation to be considered for shielding design: other radiation components (bremsstrahlung from profile monitors, muons, X-rays) must also be taken into account. 9.3.1.1.2 Bremsstrahlung from profile and intensity monitors A Profile Monitor will be inserted into the electron beam upstream of the undulator for diagnostic purposes. It consists of a wire scanner with tungsten wires of 20 m diameter. During a scan, 20% of the electron beam will be intercepted on average. A FLUKA simulation was made assuming electrons hitting an equivalent wire of square cross section 17.72 m m thick 3 m upstream of the undulator. For a 14.35 GeV beam of 1.722 kW at 120 Hz and 20% interception, the absorbed power in a photon stopper is 0.46 mW. This would cause unacceptable radiation levels in hutches downstream of the stopper when access is allowed. Therefore, it has been decided to allow use of the profile monitor only with a 10 Hz beam, thus reducing the power absorption to 0.04 mW. This condition will be part of the PPS interlock logic for access. The calculated radiation level, together with that due to collimator-halo interaction, will be used to evaluate shielding requirements for on-line hutches. -2- LCLS CDR 2/17/16 X-ray Intensity Monitors will be used at several locations along the undulator as diagnostic devices for the photon beam. However, the electron beam will also be intercepted. There will be 10 or 12 of them, but calculations have been made for the one located in the last 10 m section of the undulator. The material is diamond, 0.5 mm thick: but because the beam strikes it at an angle of 45˚, the effective thickness traversed is 0.707 mm. The 5 W deposited in the photon stopper result in radiation levels which are too high to allow access downstream of these devices. Therefore, they will be interlocked with the PPS system. Scattered bremsstrahlung and photo-neutrons produced in the stoppers must be taken into account in the stopper shielding design. 9.3.1.1.3 Gas bremsstrahlung Interaction of the electron beam with residual low-pressure gas molecules in the vacuum pipe will give rise to forward-directed gas bremsstrahlung. This type of radiation has been thoroughly investigated at circular storage rings, where the beam current is much more intense. However, at LCLS the straight length over which bremsstrahlung is produced will be much longer (120 m between the dog-leg and the first bending magnet before the electron dump). The residual gas pressure and the electron energy will also be higher. A preliminary estimation of gas bremsstrahlung dose rate, made by an empirical formula reported by Ferrari et al. [2], gives 60 mrem/h at a 20 m distance from the end of the undulator, in absence of any shielding. The dose rate behind the photon stopper shielding would be much smaller and would represent a negligible contribution compared with that of bremsstrahlung due to collimators and to beam diagnostic devices, but since the formula was derived for very different conditions (lower energies and much smaller straight lengths), it is planned to get a more accurate estimate by carrying out more a detailed Monte Carlo calculation. Bremsstrahlung, will co-propagate with any insertion device radiation until it hits a medium with an adequately short extinction depth. This will be either a mirror or a crystal. The impact will, in general, impulsively excite an intense thermal neutron field which will decay with a time constant on the order of milliseconds. To suppress any possible interference with LCLS experiments operating over similar time intervals, the layout includes a lead/polyethylene shield wall between the crystal and specular take-off optics tanks and the experimental end stations. Since both beam lines pass through this wall at off-axis angles and via small apertures, the suppression of this source of interference by the wall is expected to be very effective. -3- LCLS CDR 2/17/16 9.3.1.2 Muons Muons produced by electron interactions in the Beam Switchyard and upstream of it are already ranged out at present by 55 feet of iron and cannot constitute a concern. Muons can be created in the diagnostic area (by losses upstream of and inside the dogleg, in the collimators and in the profile monitors); there will be other possible muon sources inside the undulator (X-ray intensity monitors) and the electron dump. These muons will be either bent away by magnets downstream of the undulator or shielded by iron shielding located on the top of the electron dump. However, persons accessing the on-line hutches and the research yard downstream of the Near-Field Hall and possibly the Far-Field Hall could be exposed to several other muon sources, which are produced when high-energy bremsstrahlung hits the photon stoppers. Muons can also constitute an important radiation background for experiments. The presently available calculation tools (programs MUCARLO [3] and MUON89 [4] can only address muon production in thick targets and have been applied to estimate the contribution of the electron dump. The FLUKA code can simulate with great accuracy muon transport, but not yet muon production by photons. Work is in progress to include this effect and it is planned to use this code for a detailed simulation as soon as the upgrade will take place. It is expected that not more than 3 m of iron will be needed to shield any of the known muon sources. 9.3.1.3 Neutrons Photo-neutrons can be generated on the zero-degree line in any object hit by electrons and by bremsstrahlung (and, to a much lesser degree, by muons). Such objects include the electron dump, the transport line to the dump, photon stoppers outside and inside the experimental Halls, and any optical device in the X-ray line. Neutrons generated outside the Near-Field Hall can penetrate to the Hall through the concrete shielding or streaming through the X-ray beam pipe. Neutron shielding design must consider both personnel protection and reduction of experimental background. For the latter, time-dependent calculations may be necessary in order to take advantage of the slowing down time which could allow to gate out thermal neutron contribution. Preliminary estimations can be easily made for the Giant Resonance neutron component, which is practically isotropic and whose yield is known to be proportional to deposited power. Higher energy components require a more detailed study which can be carried out by the FLUKA code. 9.3.1.4 Toxic materials Both Li and Be are materials under consideration for optical components, Add section on how to deal with Be -4- LCLS CDR 2/17/16 9.3.2 Personnel protection system (PPS) and access In light of the above sections, the access and personnel protection system (PPS) is designed to prevent access to experimental areas where beams are present and to prevent beams from entering an area during personnel access. The experimental hall shielding will consist of fixed and moveable parts. The experimental hall perimeter walls and central beamline walls are planned to be fixed shielding consisting of appropriate material for the energy spectra of expected radiation. The experimenter hutches may have movable walls to adjust for experimental requirements. The moveable wall configuration will activate the current radiological configuration control system when changing the hutch shielding. The experimental walls will have the capability of adjusting to the different angles of any hutch branch lines. The access control system will be capable of retaining integrity and reliability, while compensating for wall placement. The PPS functions as an access control system to the central beamline and each experimenter hutch. The PPS access control components consist of entry modules (from the experimental control area into the hutch, and entry points from the experimenter hutch to the central beamline), interlocks for photon stopper and electrical hazards, logic for access, and status and control both locally and remotely. The hutch will be designed to contain all radiation background so that the dose rates outside the hutch are acceptable when photons from the FEL are inside the hutch. Access to the hutch will be controlled by a Hutch Protection System (HPS) modeled after existing SSRL hutches. The key parts of the HPS are a keyed access door, photon stopper interlocks, and area security system. The HPS allows either permission for personnel access or for beam to enter the hutch. It contains the logic interlock circuits that govern the sequence of access operations centered on the status of the stoppers. It also captures or releases the hutch door keys, acknowledges completion of a personnel security search, and keys the experiment enclosure on-line or off-line. Access to the hutch is permitted only if all photon stoppers are closed. Access to the front end enclosure requires the FFTB stoppers inside the FFTB tunnel to be in. The LCLS HPS will control the operation of photon stoppers per other areas or hutches, which are required to be in. Each stopper is protected by two ion chambers and a burn-through monitor. A list of possible PPS violations and system responses is contained in Table 9.3.21. Table 9.3.2.1 PPS violation and response. 1. FFTB tunnel security fault -5- Any FFTB tunnel security fault, while dump D2 and stoppers ST60 and ST61 are not closed, will shut-off the LCLS beam, close FFTB stoppers, turn off the electrical hazards. LCLS CDR 2/17/16 2. Inside tunnel BSOICs trip These BSOICs continuously monitor the radiation inside the tunnel. If the detected radiation level exceeds the preset limit, the PPS will shut-off the LCLS and any other beams in the Linac. The BSOIC interlocks are by-passed when the FFTB tunnel is in the No Access state. 3. Outside tunnel BSOICs trip These BSOICs continuously monitor the radiation outside the tunnel. If the detected radiation level exceeds the preset limit, the PPS will shut-off the LCLS beam and close the beam stoppers. 4. HPS security fault Any HPS security fault while the hutch photon stoppers and the FFTB beam stoppers are not closed will shut-off the LCLS beam and close the hutch and FFTB stoppers. References [1] A. Fassò, A. Ferrari, J. Ranft, P. R. Sala, “New developments in FLUKA modeling hadronic and EM interactions”, SARE3 Workshop, KEK 7-9 May 1997. Ed. H. Hirayama, KEK Proceedings 97-5 (1997), p. 32-43 [2] A. Ferrari, M. Pelliccioni, P. R. Sala, “Estimation of fluence rate and absorbed dose rate due to gas bremsstrahlung from electron storage rings”, Nucl. Instr. Meth. B83, 518 (1993) [3] L. P. Keller, “Muon background in a 1.0 TeV Linear Colider”, SLAC-PUB 6385, 1993 [4] W. R. Nelson and Y. Namito, Computer Code MUON89, SLAC Radiation Physics Dept., 1989 9.3.3 PPS beam stoppers Two Personnel Protection System (PPS) beam stoppers will be required to allow entry into the experimental hutches while the e- beam is being delivered to the undulator and deflected into the dump. The function of these stoppers is to block and absorb any coherent or incoherent or X-radiation from the undulator, as well as bremsstrahlung from anywhere in the beam transport system. These stoppers are patterned after an SLC design used in Sector 10 of the SLAC linac and in the PEP-II extraction lines [1]. The design energy is 12-15 GeV and the assumed power for continuous exposure is Pav ~5 kW. The absorbing element in each stopper is a Cu/W block assembly with an overall length of 20.32 cm [~22 radiation lengths (Xo)]. The beam first encounters the 3.7 Xo long Cu section. The remaining 12.3 Xo are provided by a block of free-machining tungsten (W~90%, ~17 g/cm3) which is brazed to the Cu. The shower maximum of the electromagnetic cascade for 12-15 GeV occurs at a depth of 5.5-5.7 Xo. A built-in burnthrough monitor is located at that z-depth. It consists of a pair of cavities separated by a Cu diaphragm. The first cavity is pressurized with dry N2. Its return line contains a pressure switch with the trip level set to 15 psig. Should excessive beam power be deposited in the stopper block, the diaphragm will perforate, allowing the N2 to escape into the second cavity, which is open to atmospheric conditions on the outside. The pressure switch will interrupt beam delivery within 2-3 linac pulses. The transverse dimensions of the stopper block are 3.16 cm wide x 2.9 cm high. The minimum radial attenuation distances are then, respectively, 3.5 Xo and 3.1 Xo in the Cu section and 3.5 -6- LCLS CDR 2/17/16 Xo and 3.1 Xo in the free-machining W. This is more than adequate to attenuate the radial shower. The absorber block can be vertically inserted or removed from the beam channel by means of a remotely controlled air cylinder. The block has a water-cooled heat sink attached to the top surface which allows continuous and safe dissipation of up to 5 kW of beam power. A third stopper will be installed which is essentially an ordinary pneumatic valve with no special heat-removal provisions. It is intended for protective insertion when the linac is running in an ultra-low peak or average current mode, for which the average radiation power is on the order of mW or less. References [1] D. Walz, "Beam Stopper for PEP II Injection," SLAC Memorandum, Sept. 28, 1994. 9.3.4 Burn through monitors A built-in burn-through monitor is located in the PPS stoppers, and described as part of that system. It consists of a pair of cavities separated by a Cu diaphragm. The first cavity is pressurized with dry N2. Its return line contains a pressure switch with the trip level set to 15 psig. Should excessive beam power be deposited in the stopper block, the diaphragm will perforate, allowing the N2 to escape into the second cavity, which is open to atmospheric conditions on the outside. The pressure switch will interrupt beam delivery within 2-3 linac pulses. 9.3.5 Shielding 9.3.6 Beam containment system (BCS) 9.3.7 Lead end stops 9.3.8 Muon stops -7-