Introduction
Shanghai Synchrotron Radiation Facility (SSRF) is one of the advanced third-generation synchrotron radiation facilities in the world [1]. Since its official start of operation in May 2009, SSRF has provided user beam time of about 522,820 hours and served more than 40000 users coming from universities, institutes, hospitals, and high-tech companies from home and abroad. Over 10,000 papers have been published based on the experiments conducted at the SSRF.
However, even though a number of beamlines were built in Phase I [2], and even with the addition of dedicated beamlines built subsequently, the SSRF still could not meet the huge user demand. In this context, the SSRF Phase-II Beamline Project proposed building 16 state-of-the-art beamlines, realizing nearly 60 new experimental methods, and equipping them with offline user experimental assistance support [3, 4]. The latest beamline layout of the SSRF is shown in Fig. 1. This new experimental ability is mainly reflected in the following aspects:
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● Energy range: Many enhanced photon energy options such as high-brightness infrared for molecular structure analysis, tender X-rays for elemental analysis of P, S, and Cl in environmental science, ultrahard X-rays for structural analysis of aircraft engine materials, and γ-rays for photonuclear physics.
● Spatial resolution from micrometers to nanometers: Enriched beam-size options, such as sub-micrometer X-ray beams for membrane protein structure analysis; spatial resolution of tens of nanometers by X-ray nano-probe or X-ray nano-CT for analysis of elemental mapping, chemical state, and nano-structures in environmental science, material science, and industry applications. Striking examples are lithium-ion batteries or nanoscale semiconductor devices.
● Time resolution from milliseconds, microseconds to picoseconds: Many enriched time resolution options for observing electron/atomic/molecular structures on picosecond, nanosecond, microsecond, or millisecond time scales in the rapid reaction process of a catalytic system to recognize the catalytic active site and selectivity, clarify the catalytic reaction process, and reveal the catalytic mechanism; to observe the microstructural evolution of polymer materials on a millisecond time scale during the impact process; and to investigate the deformation and failure behavior of materials under impact loading and high-speed fuel spray processes of automotive engines by picosecond X-ray single pulse imaging.
● Industry applications: Long beamlines for in situ monitoring of the structural evolution process of polymers in pilot-scale experiments and in situ characterization of engineering materials of large sizes in a serving environment.
● High sensitivity: chemical sensitivity (1ppb) and single-atom-level detection capability for environmental and geological sciences.
● Techniques combining multiple regions of the spectrum: To observe the same dynamic process from different viewpoints by combining complementary synchrotron radiation techniques, for example, the combination of X-rays and infrared (IR) can simultaneously detect the atomic, electronic, and molecular structures, and the combination of hard and soft X-rays can detect the electronic and chemical structures of a film layer by layer.
● Hazardous and radioactive samples: Biosafety P2 protection facilities dedicated to the macromolecular crystal structure analysis of moderate-risk infectious viruses; radioactive protection facilities dedicated to the composition and structure characterization of radioactive materials.
● User data center: for mass user data storage, real-time data analysis, deep data mining, artificial intelligence, and automation.
Accelerator upgrades
To meet the requirements of these new beamlines in the project, the storage ring has been upgraded accordingly, including the replacement of dipoles with super-bends in two cells, the construction of a 650-W helium cryogenic system, the development of a bunch-length control system, and an upgrade of the beam diagnostics and control systems.
The SSRF lattice was modified with two super-bend-based DBA cells and two straight sections (ID11, ID16) were inserted in a quadrupole triplet so that each creates double mini-βy optics for accommodating dual canted undulators.
A 3rd harmonic superconducting cavity system was developed and installed to lengthen the bunch in the passive operation mode. A 650-W helium cryogenic system was built to support the 3rd harmonic superconducting cavity and the superconducting wiggler, which can be switched to support the main RF cavities as backup when the phase-I cryogenic system fails. The hybrid filling pattern of the storage ring allows a single bunch current of up to 24.5 mA and a bunch train of 200 mA in the ring with the help of a transverse feedback system and a 3rd harmonic cavity, which can suppress instabilities and stretch the bunch length. This hybrid filling mode provides powerful support for single-pulse imaging and pump-probe transient structure research. The main parameters of the storage ring are listed in Table 1.
Parameters | Before Phase II | After Phase II |
---|---|---|
Beam energy (GeV) | 3.5 | 3.5 |
Circumference (m) | 432 | 432 |
Emittance (nm·rad) | 3.89 | 4.22(with superconducting wiggler) |
Energy spread | 9.8×10-4 | 11.1×10-4 |
Straight section (numbers × length (m)) | 4×12, 16×6.5 | 4×12, 16×6.5, 2×1.9 |
Beam length (mm) | 3.8 | 4-8 |
Beam current, multi-bunch/single-bunch (mA) | 200-300/5 | 200-300/20 |
Critical energy of normal/super bend magnet radiation (keV) | 10.3/- | 10.3/18.7 |
New Beamlines
Sixteen beamlines (including one RIXS station) were built in this project, the main specifications of which are listed in Table 2. The photon energy extends to previously uncovered regions, such as the tender X-ray region, super-hard X-ray region, and low-energy gamma-ray region. Beamline design has strengthened support for the industry. In practice, the design and construction of beamlines are extremely difficult. For example, one straight section usually has to consider supporting two beamlines to allow as many beamlines as possible for use, one beamline usually connects multiple end-stations to provide more methodology choices for users, and several experimental end-stations will realize state-of-the-art techniques that combine multiple regions of the spectrum with challenging technical difficulties that need to be solved.
Beamlines | Source | Specifications | Scientific goals | Methods |
---|---|---|---|---|
E-line: Hard X-ray Soft X-ray | IVU EPU | Soft X-ray station: Energy range: 118–1560 eV. Energy resolution: 1.3×10-4 @ 244 eV. Beam size: 23.0 µm ×7.9 µm. Flux: 3.0×1012 phs/s@244 eV@0.1%BW | Energy conversion and control, Electron-hole excitation/charge order, Solid/liquid, interface | Resonant Inelastic X-ray Scattering (RIXS), Resonant X-ray Elastic Scattering (RXES) |
Hard X-ray station: Energy range: 2800–19,000 eV. Energy resolution: 1.9×10-4@ 5000 eV. Beam size: 63.1.0 µm ×17.7 µm. Flux: 2.1×1012 phs/s @5000 eV@0.1%BW | Chemical and electronic structure in-situ. | X-ray Emission Spectroscopy (XES), High-energy Resolution Fluorescence Detection (HERFD), X-ray Raman Spectroscopy (XRS) | ||
The combined station: Energy range: 128.7–11,900 eV Energy resolution: 1.8×10-4@ 244 eV; 1.9×10-4@ 5000 eV. Beam size: 92.7 µm ×42.2 µm@244 eV, 56.6 µm ×39.3 µm@5000 eV. Flux: 3.3×1012 phs/s@300 mA@244 eV@0.1%BW, 3.0×1012 phs/s @5000 eV@0.1%BW | Solid/gas, solid/solution interface, Layer-by-layer profile detection, Electronic structures, microscopy | Ambient-pressure X-ray photoelectron Spectroscopy (APXPS), Hard X-ray photoelectron Spectroscopy (HAXPES), X-ray fine structure spectroscopy(XAFS) | ||
D-Line: X-ray IR | IVU BM | Energy dispersive XAS station: Energy range: 4.96-25.5 keV. Energy resolution: 2×10-4@ Cu K-edge. Beamsize (FWHM): 3.6 µm ×21.6 µm. Flux: 2.5×1012 phs/s·300 eV BW@7.2 keV. Time resolution: ~25 μs | Chemistry/catalysis, Condensed matter physics, Ultrafast transient structure | Time-resolved Energy -Dispersive XAS (ED-XAS), Extreme conditions, Pump-probe ED-XAS |
IR station: Spectral range: 10–10000 cm-1. Spectral resolution: 0.1cm-1. Flux: 3.2×1013phs/s/0.1% BW@ 4200 cm-1 @300 mA. Beamsize: 23 μ mμ ×24 μ m@1000 cm-1(Full width, Diffraction limit) | Chemistry, materials, biology, medicine | IR spectroscopy; IR microspectroscopy; Nano-IR spectroscopy | ||
The combined station: Energy range: 5-25 keV; Spectral range: 50–10000 cm-1. Energy resolution: 2×10-4@ CuK K-edge; Spectral resolution: 13.1 cm-1(FTIR rapid scan) Beamsiz (FWHM): 3.6 µm ×21.6 µm, 15.1 µm (H)×25.8 µm(V) m@1000 cm-1. Fluxs: 2.5×1012 phs/s@300 eV BW@7.2 keV; 2.8×1013 (phs/s/0.1%b.w.) @4200 cm-1 @300 mA. Time resolution: 8.7 ms (FTIR); ~25 µs (ED-XAS) | Time resolved atomic, electronic and molecular structures in non-equilibrium systems | Energy -Dispersive XAS+IR microspectroscopy. Energy -Dispersive XAS+DRIFTS | ||
Radioactive Materials | W | Beamline: Energy Range: 4.97-50.24 keV. Energy resolution: 2.2×10-4 @20 keV. Beamsize: 384 µm ×315 µm; 10.5 µm ×14.4 µm. Flux: 3.3×1012 phs/s@300 mA; 5.8×1010 phs/s@300 mA, micro-focus. End-station: Sample Radioactive Activity: ≤1.85 GBq/Sample (α/β emitter); ≤185 MBq/Sample (γ emitter). HRXRD angle resolution: 0.009°@20 keV,HRXES energy resolution: 2.8 eV@13.618 keV | Detection of radioactive materials of sample activity up to 185 MBq/sample (γ emitter) and 1.85 GBq/sample (α/β emitter), Physics & chemistry related to radioactive materials. Nuclear fuels & waste, radioactive contaminations, radiation chemistry. | XAFS, XES, XRD, XRF, and Imaging |
Hard X-Ray Spectroscopy | BM | Energy range: 4.9-31.6 keV. Energy resolution: 1.31×10-4 @10 keV. Beam size: 214 µm ×244 µm. Flux: 4.98×1011 phs/s @10 keV | Catalysis | X-ray absorption fine structure (XAFS). Quick-scanning XAFS. Combined XAFS and XRD. In-situ XAFS |
Hard X-ray Nanoprobe | IVU | High flux mode: Energy range: 10 keV. Energy resolution: 0.76×10-2@ 10 keV. Beamsize: 27.53 nm ×23.31 nm@10 keV. Flux:5.2×109 phs/s @10 keV. High-energy resolution mode: Energy range: 4.95–25.65 keV. Energy resolution: 2×10-4@10 keV. Beamsize: 50 nm ×50 nm@10 keV. Flux:1×109 phs/s @10 keV | Nano technology, material science, life science, environment science., components | X-ray fluorescence, X-ray nanodiffraction, X-ray near edge absorption spectroscopy and coherent diffraction imaging |
Medium-energy Spectroscopy | IVU | Energy range: 2.08-16.20 keV. Energy resolution: 1.76×10-4@ 2.5keV. Beam size: 3.1 µm ×1.1 µm @10 keV(K-B),0.32 μm ×0.23 μ m@2.5 keV(sK-B). Flux: 3.74×1012 phs/s @2.5 keV(K-B),3.69×1012 phs/s @10 keV(K-B). Detection Limit: 4.1 ppb@Cu K-edge | Environmental pollutants, Environmental Catalysis, Energy material, Biological element analysis | XAFS、XRF、TEYμ XAFSμ XRFTXRF |
3D Nano Imaging | BM | Energy range: 4.97–14.35 keV. Energy resolution (ΔE/E): 1.83×10-4. Flux: 1.84×1010 phs/s@8 keV@300 mA. Spatial resolution: 19.9 nm@TXM@8 keV | Nano imaging | TXM Nano CT Nano-Spectral imaging |
S2-Line: Spatial and Spin resolution ARPES and Magnetism | Twin EPU | Energy range: 48.2~2007 eV. Energy resolution: 11500@867 eV; 16308@91 eV; Beamsize: 69.3 µm ×48.3 µm@Spin-ARPES; 200 nm ×200 nm@Nano-ARPES; Flux:2.89×1011 phs/s/0.01%BW@867 eV, 300 mA, 9.48×109 phs/s/0.01%BW@91 eV, 300 mA | Magnetic and electronic properties | Nano-ARPES; Spin-ARPES; XMCD/XMLD |
RIXS Station | EPU | RIXS station: Energy range: 244.5-1845 eV. Energy resolution: 59.3 meV@930 eV. Beamsize: 40 µm ×10 µm (H×V). Flux: ≥1.52×1010 phs/s/0.01%BW@930 eV@ 300mA. Sample temperature: 10.7~300 K | Collective excitations in quantum materials. Charge transfer in Energy materials | Resonant Inelastic X-ray ScatteringX-ray emission spectroscopy |
Laue Microdiffraction | Super B | Materiel Station: Energy range: 7-30 keV (white beam). Energy resolution: 0.96×10-4@10 keV. Beamsize: 0.9 µm ×1.3 µm. Flux: 4×1013 phs/s@300 mA (white beam). Protein Station: Energy range: 7-20 keV (white beam). Energy resolution: 0.96×10-4@10 keV. Beamsize: 4.2 µm ×4.3 µm. Flux: 6×1014 phs/s@300 mA (white beam) | Local microstructure and defects Laue Crystallography | Laue diffraction Fluorescence Serial protein X-ray crystallography, in-site data collection |
Surface Diffraction | CPMU | Energy range: 4.7-28 keV. Energy resolution: 1.3×10-4 @10 ke. VFlux: 6.3×1012 phs/s@10 keV. Beam divergence: 42 µrad ×17 µrad. Beamsize: 102 µm ×73 µm | Surface and interface of low-dimensional thin films Solid-liquid, liquid-liquid interfaces. Biomembrane structure, self-assembly in soft matte | Grazing Incident X-ray Diffraction X-ray Reflectivity Crystal truncation rods. Liquid X-ray scattering |
Shanghai Laser Electron Gamma Source | ID | Energy range: 0.25–21.7 MeV. Flux: 2.14×104@20°–7.99×106 phs/s@180˚. Energy resolution 4.26% @180˚ with collimator. Angle divergence: 0.38 mrad | Nuclear Physics/Nuclear astrophysics/Gamma Source Application | Photonuclear Reaction |
P2 Protein Crystallography | IVU | Energy range: 6.5~18.1 keV. Energy resolution: 1.78×10-4. Beamsize: 16.8 μ m ×9.4 μ m. Flux:2.52×1012 phs/s(@12.7 keV, 300 mA)Biosafety: Level-2. Sample changer: Swordfish | Moderate-risk infectious viruses | Shutterless data collection, MR, MAD/SAD, In-situ Data collection |
Membrane Protein Crystallography | CPMU | Energy Range: 4.97-25.51 keV; Energy resolution: 1.75×10-4@ 12 keV& DCM Flux: 3.07 × 1011 phs/s (DCM@300 mA@12 keV @ 0.75 µm × 0.65 µm); 3.23× 1012 phs/s (DMM@300 mA@12 keV @0.70 µm ×0.68 µm). Beamsize: 0.7–20 µm. Data collection time: 32 s (360o). Sample measuring speed: 49 crystals/h | Membrane protein | Macromolecular crystallography; Micro- protein crystallography (μ-MX); Quasi serial protein x-ray crystallography (SF); The multi- and single wavelength anomalous dispersion (MAD/SAD) |
Ultra-Hard X-ray Applications | SCW | Energy range: 29.7–162 keV. Beamsize: 300 µm–100 mm. Energy resolution: 5×10-3. Flux: 2.3×1011phs/s@100 keV@25 μrad | Engineering materials and geological science | High energy EDXRD, XRD, Imaging, PDF |
Time-resolved USAXS | IVU | Beamline: Energy range: 8~15 keV. Energy resolution: 5.8×10-3@10 keV. Flux:1.1×1013 phs/s@10 keV @300 mA. Beamsize: 379 µm ×341µm @10 keV (H×V) | ||
USAXS endstation: Time resolution: ~1.3 ms. qmin=0.0030 nm-1 | In-situ monitoring of structural evolution process in polymer processing and fiber-spinningat nm~μm scale | Time-resolved USAXS | ||
Micro-SAXS end-station: Flux: 3.2×1012 phs/s@10 keV @300 mA. Beamsize: 7.6 µm ×4.3 µm @10 keV(H×V). qmin=0.049 nm-1 | Local microstructure study by microfocus X-ray scattering | Microfocus SAXS/WAXS | ||
Industrial application endstation. Flux: 1.1×1013 phs/s@10 keV. @300 mATensile range of in-situ stretching device: 0-4300 N. Temperature range of in-situ stretching device: RT-520 °C | Industrial application | Time-resolved SAXS/WAXS | ||
Fast X-ray Imaging | CPMU | Energy range: 8.3~30.5 keV. Energy resolution: 1.6×10-4@ 10 keV. Beamsize: 2.64 mm×1.87 mm. Flux: 2.39 × 1013 phs/s @10 keV; 1.31 ×1016 phs/s (white beam); 1.5 × 109 phs (single pulse). Spatial resolution: 0.7 μm. Temporal resolution of single-pulse ultrafast X-ray imaging: 60 ps; Temporal resolution of X-ray dynamic imaging: 2 μs; Temporal resolution of X-ray dynamic micro-CT: 50 ms | Fast process imaging | Single-pulse ultrafast X-ray imaging. Microsecond resolved X-ray dynamic imaging. Milisecond resolved X-ray dynamic micro-CT. High-resolution quantitative micro-CT |
In this paper, a brief description of the new beamlines is introduced, and a detailed description of this special issue can be found.
User Experimental Support
The experimental support for users includes materials laboratories, chemical laboratories, biomedical laboratories, in situ instrumentation pools, and user data centers. They are another essential part of the SSRF Phase II beamline project with the goals of serving users in various aspects and effectively improving the comprehensive experimental capabilities at the SSRF.
(1) The material preparation laboratory satisfies the user requirements for material sample preparation. It provides sample preparation and auxiliary measurements for high-pressure materials, micro-and nanomaterials, etc.
● Powder sample pressing: 5–8 mm
● High temperature treating: 25–1900 K
● Thin film cutting: 0.1–25 mm
● SEM / TEM: 3nm /0.1nm
(2) Chemical and environmental laboratory: Chemical sample preparation and on-site treatment, such as auxiliary component testing and auxiliary structure analysis
● Operating environment: H2O <1 ppm, O2< 1 ppm
● Sample storage: – 85 °C ~ –10 °C
● Particle crushing: 40 – 150 µm
(3) Biology and medicine laboratory: provides the basic experimental conditions for biomedical sample preparation on site, auxiliary testing of biomacromolecules and sample preparation, tissue sample preparation, and treatment.
● Slice thickness: 1–100 µm
● Slice temperature: –35 – 0 °C, 5 K
● Freezing rate: 18000 °C /s
(4) In situ instrumentation pool: This provides in situ equipment for the experimental station, such as for changing the temperature, pressure, vacuum, and magnetic field.
● Temperature: 4.5–2600 K
● Magnetic field: 0~8000 Gs
● Vacuum transmission device: 1.0×10-9 Torr
● Tensile loading: 5 kN
(5) User data center: With 23 PB storage, 11000 CPU cores, 28 GPUs, and 19 edge clusters for beamlines, it provides mass data storage, real-time data analysis, deep data mining, and artificial intelligence and automation. A schematic view of the big data framework in the user datacenter is shown in Fig. 2.
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● CPU+GPU: Rpeak 967 Tflops
● Store capacity: 23 PB HDD + 100 TB SSD
● Bandwidth to beamline: 40 GB/s
Beamline Technique Support
The beamline technique support supports the construction of optics, mechanical engineering, control and electronics, engineering analysis, and test beamlines. The primary specifications of the X-ray test beamline are listed in Table 3. As an essential part of the SSRF Phase-II Beamline Project, beamline technique support will provide solutions for various key technical issues regarding the development, installation, tuning, and testing of the equipment used at beamlines. In the future, they will ensure the highly efficient operation of the beamlines.
Beamlines | Source | Specifications | Scientific goals | Methods |
---|---|---|---|---|
X-ray test beamline | BM | Energy range: 4~30 keV. Energy resolution: 5×10-4 @10 keV. Beam size: 500 µm ×400 µm@10 keV. Flux: 3×1011 phs/s @10 keV | High performance beamline instrument and optics | XRD/XRF/XAFS Imaging |
High-performance X-ray optics are the basis and prerequisites for the construction of advanced synchrotron radiation beamlines and experimental stations. Highly brilliant and coherent X-rays are deflected, collimated, changed to be monochromatic, and focused by a series of optical components before being delivered to the sample for scientific experimental research. Therefore, the full utilization of the coherent wavefront and ultrahigh brightness of advanced X-ray light sources depends on the performance of the optical components. Through domestic cooperation and taking advantage of the high-precision optical metrology technology developed by the SSRF, a 1000-mm-long plane mirror with a 0.2-μrad slope error and a multilayer monochromator have been successfully developed.
High-performance key equipment guarantees the construction of advanced beamlines for the project. A series of core equipment was developed to meet the requirements of the beamlines in the SSRF Phase-II Beamline project. For example, the high energy sagittal-focusing Laue monochromator can achieve small radius dynamic bending of ultra-thin crystals, the size of the focusing spot reached 260 µm. The cryo-cooled meridian bent Laue monochromator was first domestically developed and has passed the test acceptance. The plane-grating monochromator realized cryo-cooling of high heat load plane mirrors for the first time. Meanwhile, a number of general key equipment, such as a sub-microradian mirror bender system, a cryo-cooled double crystal monochromator and a precision monochromatic slit have also been developed. The slope error of the mirror bender was less than 0.4 μrad (RMS), and the bending curve resolution and repeatability of the bender was less than 0.5%(∆R/R). The relative stabilities of the first and second DCM crystals were 63 nrad (RMS). The performance of this general key equipment meets the requirements of most beamlines in the project.
The control systems were designed using the EPICS (Experimental Physics and Industrial Control System) [5] and the Bluesky Data Collection Framework. The system supports motion control, detector control, and equipment protection at the beamlines. Hardware for stepper motor control was developed. The synchronization accuracy of the hardware for fly scanning reaches 20 ns, which can meet most requirements for fly scanning experiments. A beam position monitor (BPM) and its current front-end amplifier have been developed successfully with precisions of 1 mm and 1pA, which can play important roles in nanometer positioning feedback control. The control system is equipped with single-pulse timing synchronization control and measurement instruments, such as an event timing system and a streak camera, which can support the timing control of picosecond time-resolved pump-probe experiments. EPICSv7, the most cutting-edge EPICS technology, has been researched and used in a control lab to overcome the bottlenecks of big data communication and enhance the overall performance of the control system.
Conclusion and Perspectives
Since its first operation in 2009, the SSRF has greatly accelerated the development of photon science in mainland China. The completion of the SSRF Phase-II Beamline Project is believed to bring the experimental capability of the SSRF to a new level, with rich and diverse choices in photon energies, methodologies, and in situ conditions, mutual promotion of offline and online experiments, rapid data processing and analysis, and various resolution abilities close to the limit of the third-generation light source. Figure 3 shows the latest bird’s-eye view of the SSRF.
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The construction of the SSRF Phase II Project has been conducted while the SSRF is still in operation, which brought great challenges to project management, installation, and testing. The first beamline, the hard X-ray spectroscopy beamline, was completed and began commissioning at the end of 2018, whereas the last two beamlines, the hard X-ray nanoprobe beamline and the medium-energy spectroscopy beamline, were completed at the end of July of that year. Till the end of 2023, SSRF Phase II beamlines have provided 45,741 h of beamtime and executed a total of 1152 research proposals from 678 research teams, with 368 user papers published, including seven CNS papers [6-12]. The next step is to optimize machine performance for stable operation and to organize and promote large scientific research projects.
To date, 34 beamlines in the SSRF are in operation, and nearly 100 types of advanced experimental methods have been realized. This systematic and state-of-the-art experimental facility for third-generation synchrotron radiation, particularly the SSRF Phase II Beamline Project, is anticipated to contribute significantly to cutting-edge science and technology.
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